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19,800 | 1511.08008 | V\'ictor Navas | V\'ictor Navas-Portella and Eduard Vives | Influence of the aspect ratio and boundary conditions on universal
finite size scaling functions in the athermal metastable 2d Random Field
Ising Model | 10 pages, 12 figures | Phys. Rev. E 93, 022129 (2016) | 10.1103/PhysRevE.93.022129 | null | cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This work studies universal finite size scaling functions for the number of
1d spanning avalanches in a two-dimensional disordered system with boundary
conditions of different nature and different aspect ratios. For this purpose,
we consider the 2d Random Field Ising Model at T = 0 driven by the external
field H with athermal dynamics implemented with periodic and forced boundary
conditions. We choose a convenient scaling variable z that accounts for the
deformation of the distance to the critical point caused by the aspect ratio.
Moreover, assuming that the dependence of the finite size scaling functions on
the aspect ratio can be accounted by an additional multiplicative factor, we
have been able to collapse data for different system sizes, different aspect
ratios and different nature of the boundary conditions into a single scaling
function Q.
| [{'version': 'v1', 'created': 'Wed, 25 Nov 2015 10:10:49 GMT'}
{'version': 'v2', 'created': 'Thu, 26 Nov 2015 13:44:49 GMT'}
{'version': 'v3', 'created': 'Fri, 15 Jan 2016 10:07:59 GMT'}] | 2016-02-24 | [array(['Navas-Portella', 'Víctor', ''], dtype=object)
array(['Vives', 'Eduard', ''], dtype=object)] |
19,801 | hep-th/0408064 | Ashoke Sen | Ashoke Sen | Symmetries, Conserved Charges and (Black) Holes in Two Dimensional
String Theory | LaTeX file, 60 pages | JHEP 0412:053,2004 | 10.1088/1126-6708/2004/12/053 | null | hep-th | null | Two dimensional string theory is known to have an infinite dimensional
symmetry, both in the continuum formalism as well as in the matrix model
formalism. We develop a systematic procedure for computing the conserved
charges associated with these symmetries for any configuration of D-branes in
the continuum description. We express these conserved charges in terms of the
boundary state associated with the D-brane, and also in terms of the asymptotic
field configurations produced by this D-brane. Comparison of the conserved
charges computed in the continuum description with those computed in the matrix
model description facilitates identification of the states between these two
formalisms. Using this we put constraints on the continuum description of the
hole states in the matrix model, and matrix model description of the black
holes solutions of the continuum theory. We also discuss possible
generalization of the construction of the conserved charges to the case of
D-branes in critical string theory.
| [{'version': 'v1', 'created': 'Mon, 9 Aug 2004 06:53:00 GMT'}] | 2009-09-15 | [array(['Sen', 'Ashoke', ''], dtype=object)] |
19,802 | 1608.08130 | Olaf Hartig | Magnus Knuth and Olaf Hartig and Harald Sack | Scheduling Refresh Queries for Keeping Results from a SPARQL Endpoint
Up-to-Date (Extended Version) | This document is an extended version of a paper published in ODBASE
2016 | null | null | null | cs.DB | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Many datasets change over time. As a consequence, long-running applications
that cache and repeatedly use query results obtained from a SPARQL endpoint may
resubmit the queries regularly to ensure up-to-dateness of the results. While
this approach may be feasible if the number of such regular refresh queries is
manageable, with an increasing number of applications adopting this approach,
the SPARQL endpoint may become overloaded with such refresh queries. A more
scalable approach would be to use a middle-ware component at which the
applications register their queries and get notified with updated query results
once the results have changed. Then, this middle-ware can schedule the repeated
execution of the refresh queries without overloading the endpoint. In this
paper, we study the problem of scheduling refresh queries for a large number of
registered queries by assuming an overload-avoiding upper bound on the length
of a regular time slot available for testing refresh queries. We investigate a
variety of scheduling strategies and compare them experimentally in terms of
time slots needed before they recognize changes and number of changes that they
miss.
| [{'version': 'v1', 'created': 'Mon, 29 Aug 2016 16:16:36 GMT'}] | 2016-08-30 | [array(['Knuth', 'Magnus', ''], dtype=object)
array(['Hartig', 'Olaf', ''], dtype=object)
array(['Sack', 'Harald', ''], dtype=object)] |
19,803 | 1108.5115 | Alessandro La Rosa | A. La Rosa, M. Boscardin, M. Cobal, C. Da Vi\'a, G. F. Dalla Betta, G.
Darbo, C. Gallrapp, C. Gemme, F. Huegging, J. Janssen, A. Micelli, H.
Pernegger, M. Povoli, N. Wermes, N. Zorzi | Functional characterization of irradiated 3D-DDTC pixel sensor
prototypes fabricated at FBK | This paper has been withdrawn by the author due to an update of some
results | null | null | null | physics.ins-det | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we discuss results relevant to 3D Double-Side Double Type
Column (3D-DDTC) pixel sensors fabricated at FBK (Trento, Italy) and oriented
to the ATLAS upgrade.
| [{'version': 'v1', 'created': 'Thu, 25 Aug 2011 15:11:16 GMT'}
{'version': 'v2', 'created': 'Fri, 7 Oct 2011 07:47:43 GMT'}
{'version': 'v3', 'created': 'Sat, 10 Dec 2011 01:37:43 GMT'}] | 2011-12-13 | [array(['La Rosa', 'A.', ''], dtype=object)
array(['Boscardin', 'M.', ''], dtype=object)
array(['Cobal', 'M.', ''], dtype=object)
array(['Da Viá', 'C.', ''], dtype=object)
array(['Betta', 'G. F. Dalla', ''], dtype=object)
array(['Darbo', 'G.', ''], dtype=object)
array(['Gallrapp', 'C.', ''], dtype=object)
array(['Gemme', 'C.', ''], dtype=object)
array(['Huegging', 'F.', ''], dtype=object)
array(['Janssen', 'J.', ''], dtype=object)
array(['Micelli', 'A.', ''], dtype=object)
array(['Pernegger', 'H.', ''], dtype=object)
array(['Povoli', 'M.', ''], dtype=object)
array(['Wermes', 'N.', ''], dtype=object)
array(['Zorzi', 'N.', ''], dtype=object)] |
19,804 | 1403.3209 | Vicente Botella-Soler | V. Botella-Soler, P. Glendinning | Hierarchy and Polysynchrony in an adaptive network | 13 pages, 17 figures | null | 10.1103/PhysRevE.89.062809 | null | nlin.AO nlin.CD | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We describe a simple adaptive network of coupled chaotic maps. The network
reaches a stationary state (frozen topology) for all values of the coupling
parameter, although the dynamics of the maps at the nodes of the network can be
non-trivial. The structure of the network shows interesting hierarchical
properties and in certain parameter regions the dynamics is polysynchronous:
nodes can be divided in differently synchronized classes but contrary to
cluster synchronization, nodes in the same class need not be connected to each
other. These complicated synchrony patterns have been conjectured to play roles
in systems biology and circuits. The adaptive system we study describes ways
whereby this behaviour can evolve from undifferentiated nodes.
| [{'version': 'v1', 'created': 'Thu, 13 Mar 2014 09:21:04 GMT'}] | 2015-06-19 | [array(['Botella-Soler', 'V.', ''], dtype=object)
array(['Glendinning', 'P.', ''], dtype=object)] |
19,805 | hep-ph/9802317 | Thomas Gasenzer | D. Bruss (1), T. Gasenzer (2) and O. Nachtmann (2), ((1) ISI, Torino,
Italy; (2) Univ. Heidelberg, Germany) | Parity Violating Energy Shifts and Berry Phases in Atoms, I | 62 pages, 1 table, 17 figures, LaTeX, submitted to Ann. Phys. (NY),
Rev. ver.: some calculations shifted into appendices, only minor changes in
content, more refs. added | Eur.Phys.J.direct D1 (1999) 2 | null | HD-THEP-97-36 | hep-ph nucl-th physics.atom-ph | null | We present a study of parity (P) violating contributions to the eigenenergies
of stationary systems containing atoms in spatially inhomogeneous external
electric fields. In this context the subtle interplay of P-violation and time
reversal (T) invariance plays an important role. If the entire field
configuration is chosen to exhibit chirality the energies are in general
shifted by pseudoscalar contributions which change sign under a planar
reflection of the field. To calculate the effects we use the standard model of
elementary particle physics where the P-odd interaction arises through the
exchange of Z-bosons between the quarks in the nucleus and the atomic
electrons. We consider in detail hydrogen-like systems in unstable levels of
principal quantum number n=2. The nominal order of P-violating effects is
10^-5...10^-9 Hz which is determined by the mixing of the 2S_1/2 and 2P_1/2
states. However we point out that it is possible to enhance the P-violating
energy shifts dramatically! Instead of energy shifts linear in the P-violation
parameters we get then shifts proportional to the square root of these
parameters. Numerically we find such energy shifts to be of order 10^-5...1 Hz.
Application of our technique to hydrogen-like atoms with a nucleus of spin
I=1/2 yields P-violating energy shifts which are very sensitive to the nuclear
spin dependent P-odd force, which receives a rather large contribution from the
polarized strange quark density in polarized nuclei. Thus, a measurement of
these energy shifts could provide an important tool to elucidate nuclear
properties connected to the so called ``spin crisis''. We also present a method
for treating degenerate perturbation theory which combines advantages of both,
Kato's and Bloch's methods.
| [{'version': 'v1', 'created': 'Fri, 13 Feb 1998 15:30:59 GMT'}
{'version': 'v2', 'created': 'Tue, 8 Sep 1998 10:45:49 GMT'}] | 2007-05-23 | [array(['Bruss', 'D.', ''], dtype=object)
array(['Gasenzer', 'T.', ''], dtype=object)
array(['Nachtmann', 'O.', ''], dtype=object)] |
19,806 | 2303.10515 | Hanliang Zhang | Hanliang Zhang, Cristina David, Yijun Yu, Meng Wang | Ownership guided C to Rust translation | null | null | null | null | cs.PL cs.SE | http://creativecommons.org/licenses/by/4.0/ | Dubbed a safer C, Rust is a modern programming language that combines memory
safety and low-level control. This interesting combination has made Rust very
popular among developers and there is a growing trend of migrating legacy
codebases (very often in C) to Rust. In this paper, we present a C to Rust
translation approach centred around static ownership analysis. We design a
suite of analyses that infer ownership models of C pointers and automatically
translate the pointers into safe Rust equivalents. The resulting tool, Crown,
scales to real-world codebases (half a million lines of code in less than 10
seconds) and achieves a high conversion rate.
| [{'version': 'v1', 'created': 'Sat, 18 Mar 2023 23:14:04 GMT'}] | 2023-03-21 | [array(['Zhang', 'Hanliang', ''], dtype=object)
array(['David', 'Cristina', ''], dtype=object)
array(['Yu', 'Yijun', ''], dtype=object)
array(['Wang', 'Meng', ''], dtype=object)] |
19,807 | 1603.08873 | Gilberto Fabbris | G. Fabbris, D. Meyers, J. Okamoto, J. Pelliciari, A. S. Disa, Y.
Huang, Z.-Y. Chen, W. B. Wu, C. T. Chen, S. Ismail-Beigi, C. H. Ahn, F. J.
Walker, D. J. Huang, T. Schmitt, M. P. M. Dean | Orbital engineering in nickelate heterostructures driven by anisotropic
oxygen hybridization rather than orbital energy levels | Accepted for publication in Physical Review Letters. 6 pages, 4
figures | Phys. Rev. Lett. 117, 147401 (2016) | 10.1103/PhysRevLett.117.147401 | null | cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Resonant inelastic x-ray scattering is used to investigate the electronic
origin of orbital polarization in nickelate heterostructures taking
$\mathrm{LaTiO_3-LaNiO_3-3x(LaAlO_3)}$, a system with exceptionally large
polarization, as a model system. We find that heterostructuring generates only
minor changes in the Ni $3d$ orbital energy levels, contradicting the
often-invoked picture in which changes in orbital energy levels generate
orbital polarization. Instead, O $K$-edge x-ray absorption spectroscopy
demonstrates that orbital polarization is caused by an anisotropic
reconstruction of the oxygen ligand hole states. This provides an explanation
for the limited success of theoretical predictions based on tuning orbital
energy levels and implies that future theories should focus on anisotropic
hybridization as the most effective means to drive large changes in electronic
structure and realize novel emergent phenomena.
| [{'version': 'v1', 'created': 'Tue, 29 Mar 2016 18:31:15 GMT'}
{'version': 'v2', 'created': 'Thu, 2 Jun 2016 13:38:50 GMT'}
{'version': 'v3', 'created': 'Thu, 8 Sep 2016 13:47:07 GMT'}] | 2016-10-05 | [array(['Fabbris', 'G.', ''], dtype=object)
array(['Meyers', 'D.', ''], dtype=object)
array(['Okamoto', 'J.', ''], dtype=object)
array(['Pelliciari', 'J.', ''], dtype=object)
array(['Disa', 'A. S.', ''], dtype=object)
array(['Huang', 'Y.', ''], dtype=object)
array(['Chen', 'Z. -Y.', ''], dtype=object)
array(['Wu', 'W. B.', ''], dtype=object)
array(['Chen', 'C. T.', ''], dtype=object)
array(['Ismail-Beigi', 'S.', ''], dtype=object)
array(['Ahn', 'C. H.', ''], dtype=object)
array(['Walker', 'F. J.', ''], dtype=object)
array(['Huang', 'D. J.', ''], dtype=object)
array(['Schmitt', 'T.', ''], dtype=object)
array(['Dean', 'M. P. M.', ''], dtype=object)] |
19,808 | 1408.6711 | Ilya Kossovskiy | Ilya Kossovskiy and Bernhard Lamel | On the analyticity of CR-diffeomorphisms | arXiv admin note: text overlap with arXiv:1309.6799 | null | null | null | math.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In any positive CR-dimension and CR-codimension we provide a construction of
real-analytic holomorphically nondegenerate CR-submanifolds, which are
$C^\infty$ CR-equivalent, but are inequivalent holomorphically. As a corollary,
we provide the negative answer to the conjecture of Ebenfelt and Huang
\cite{eh} on the analyticity of CR-equivalences between real-analytic Levi
nonflat hypersurfaces in dimension 2.
| [{'version': 'v1', 'created': 'Thu, 28 Aug 2014 13:33:29 GMT'}] | 2014-08-29 | [array(['Kossovskiy', 'Ilya', ''], dtype=object)
array(['Lamel', 'Bernhard', ''], dtype=object)] |
19,809 | 1206.3196 | Nils Ackermann | Nils Ackermann and Andrzej Szulkin | A concentration phenomenon for semilinear elliptic equations | null | null | 10.1007/s00205-012-0589-1 | null | math.AP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For a domain $\Omega\subset\dR^N$ we consider the equation $ -\Delta u +
V(x)u = Q_n(x)\abs{u}^{p-2}u$ with zero Dirichlet boundary conditions and
$p\in(2,2^*)$. Here $V\ge 0$ and $Q_n$ are bounded functions that are positive
in a region contained in $\Omega$ and negative outside, and such that the sets
$\{Q_n>0\}$ shrink to a point $x_0\in\Omega$ as $n\to\infty$. We show that if
$u_n$ is a nontrivial solution corresponding to $Q_n$, then the sequence
$(u_n)$ concentrates at $x_0$ with respect to the $H^1$ and certain
$L^q$-norms. We also show that if the sets $\{Q_n>0\}$ shrink to two points and
$u_n$ are ground state solutions, then they concentrate at one of these points.
| [{'version': 'v1', 'created': 'Thu, 14 Jun 2012 17:50:09 GMT'}
{'version': 'v2', 'created': 'Mon, 18 Jun 2012 19:55:49 GMT'}] | 2015-06-05 | [array(['Ackermann', 'Nils', ''], dtype=object)
array(['Szulkin', 'Andrzej', ''], dtype=object)] |
19,810 | 2101.05421 | Sayaka Kamei | Sayaka Kamei, Anissa Lamani, Fukuhito Ooshita, Sebastien Tixeuil,
Koichi Wada | Asynchronous Gathering in a Torus | 41 pages | null | null | null | cs.DC | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We consider the gathering problem for asynchronous and oblivious robots that
cannot communicate explicitly with each other, but are endowed with visibility
sensors that allow them to see the positions of the other robots. Most of the
investigations on the gathering problem on the discrete universe are done on
ring shaped networks due to the number of symmetric configuration. We extend in
this paper the study of the gathering problem on torus shaped networks assuming
robots endowed with local weak multiplicity detection. That is, robots cannot
make the difference between nodes occupied by only one robot from those
occupied by more than one robots unless it is their current node. As a
consequence, solutions based on creating a single multiplicity node as a
landmark for the gathering cannot be used. We present in this paper a
deterministic algorithm that solves the gathering problem starting from any
rigid configuration on an asymmetric unoriented torus shaped network.
| [{'version': 'v1', 'created': 'Thu, 14 Jan 2021 02:06:28 GMT'}] | 2021-01-15 | [array(['Kamei', 'Sayaka', ''], dtype=object)
array(['Lamani', 'Anissa', ''], dtype=object)
array(['Ooshita', 'Fukuhito', ''], dtype=object)
array(['Tixeuil', 'Sebastien', ''], dtype=object)
array(['Wada', 'Koichi', ''], dtype=object)] |
19,811 | 2110.02000 | Qi Wang | Toshitaka Aoki and Qi Wang | On $\tau$-tilting finiteness of blocks of Schur algebras | 28 pages | null | null | null | math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, we determine the $\tau$-tilting finiteness for some blocks of
(classical) Schur algebras. Combining with the results in arXiv:2010.05206, we
get a complete classification of $\tau$-tilting finite Schur algebras. As a
refinement, we also give a complete classification of $\tau$-tilting finite
blocks of the Schur algebra $S(2,r)$.
| [{'version': 'v1', 'created': 'Tue, 5 Oct 2021 12:44:11 GMT'}] | 2021-10-06 | [array(['Aoki', 'Toshitaka', ''], dtype=object)
array(['Wang', 'Qi', ''], dtype=object)] |
19,812 | 2104.11086 | Bulat Nurmievich Khabibullin | B. N. Khabibullin | Meromorphic functions and differences of subharmonic functions in
integrals and the difference characteristic of Nevanlinna. II. Explicit
estimates of the integral of the radial maximum growth characteristic | 7 pages, in Russian | null | null | null | math.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Let $U\not\equiv \pm\infty$ be the difference of subharmonic functions, i.e.,
a $\delta$-subharmonic function, on a closed disc of radius $R$ centered at
zero. In the preceding first part of our paper, we obtained general estimates
for the integral of the positive part of the radial maximum growth
characteristic ${\mathsf M}_U(t):=\sup\bigl\{U(z)\bigm| |z|=r\bigr\}$ over the
increasing integration function $m$ on the segment $[0, r]$ via the Nevanlinna
difference characteristic and the modulus of continuity of the function $m$.
The second part of the work gives an explicit view for such estimates, provided
that the modulus of continuity of the function $m$ does not exceed some
differentiable function $h$ on the open interval $(0,r)$ with the only
condition $\sup\limits_{t\in (0,r)}\dfrac{h(t)}{th'(t)}<+\infty$. This
condition is satisfied by any power functions $t\mapsto t^d$ of degree $d>0$.
The estimates are optimal in a certain sense.
| [{'version': 'v1', 'created': 'Fri, 16 Apr 2021 15:35:47 GMT'}] | 2021-04-23 | [array(['Khabibullin', 'B. N.', ''], dtype=object)] |
19,813 | 1602.08817 | Junping Wang | Lin Mu, Junping Wang, and Xiu Ye | Effective Implementation of the Weak Galerkin Finite Element Methods for
the Biharmonic Equation | 10 pages | null | null | null | math.NA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The weak Galerkin (WG) methods have been introduced in the references [11,
16] for solving the biharmonic equation. The purpose of this paper is to
develop an algorithm to implement the WG methods effectively. This can be
achieved by eliminating local unknowns to obtain a global system with
significant reduction of size. In fact, this reduced global system is
equivalent to the Schur complements of the WG methods. The unknowns of the
Schur complement of the WG method are those defined on the element boundaries.
The equivalence of the WG method and its Schur complement is established. The
numerical results demonstrate the effectiveness of this new implementation
technique.
| [{'version': 'v1', 'created': 'Mon, 29 Feb 2016 04:07:13 GMT'}] | 2016-03-01 | [array(['Mu', 'Lin', ''], dtype=object)
array(['Wang', 'Junping', ''], dtype=object)
array(['Ye', 'Xiu', ''], dtype=object)] |
19,814 | 2206.08449 | Yunpeng Zhao | Yunpeng Zhao, Haiyan Wang, Kuai Xu, Yue Wang, Ji Zhu, and Feng Wang | Adaptive Algorithm for Quantum Amplitude Estimation | null | null | null | null | quant-ph stat.ME | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Quantum amplitude estimation is a key sub-routine of a number of quantum
algorithms with various applications. We propose an adaptive algorithm for
interval estimation of amplitudes. The quantum part of the algorithm is based
only on Grover's algorithm. The key ingredient is the introduction of an
adjustment factor, which adjusts the amplitude of good states such that the
amplitude after the adjustment, and the original amplitude, can be estimated
without ambiguity in the subsequent step. We show with numerical studies that
the proposed algorithm uses a similar number of quantum queries to achieve the
same level of precision $\epsilon$ compared to state-of-the-art algorithms, but
the classical part, i.e., the non-quantum part, has substantially lower
computational complexity. We rigorously prove that the number of oracle queries
achieves $O(1/\epsilon)$, i.e., a quadratic speedup over classical Monte Carlo
sampling, and the computational complexity of the classical part achieves
$O(\log(1/\epsilon))$, both up to a double-logarithmic factor.
| [{'version': 'v1', 'created': 'Thu, 16 Jun 2022 21:11:15 GMT'}] | 2022-06-20 | [array(['Zhao', 'Yunpeng', ''], dtype=object)
array(['Wang', 'Haiyan', ''], dtype=object)
array(['Xu', 'Kuai', ''], dtype=object)
array(['Wang', 'Yue', ''], dtype=object)
array(['Zhu', 'Ji', ''], dtype=object)
array(['Wang', 'Feng', ''], dtype=object)] |
19,815 | 0904.3488 | Alexander Schekochihin | S. V. Nazarenko (Warwick) and A. A. Schekochihin (Oxford) | Critical balance in magnetohydrodynamic, rotating and stratified
turbulence: towards a universal scaling conjecture | JFM-style tex, 16 pages, 1 figure; replaced with final published
version (minor edits) | J.Fluid Mech.677:134,2011 | 10.1017/S002211201100067X | null | physics.flu-dyn astro-ph.GA astro-ph.SR nlin.CD physics.ao-ph physics.space-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is proposed that critical balance - a scale-by-scale balance between the
linear propagation and nonlinear interaction time scales - can be used as a
universal scaling conjecture for determining the spectra of strong turbulence
in anisotropic wave systems. Magnetohydrodynamic (MHD), rotating and stratified
turbulence are considered under this assumption and, in particular, a novel and
experimentally testable energy cascade scenario and a set of scalings of the
spectra are proposed for low-Rossby-number rotating turbulence. It is argued
that in neutral fluids, the critically balanced anisotropic cascade provides a
natural path from strong anisotropy at large scales to isotropic Kolmogorov
turbulence at very small scales. It is also argued that the kperp^{-2} spectra
seen in recent numerical simulations of low-Rossby-number rotating turbulence
may be analogous to the kperp^{-3/2} spectra of the numerical MHD turbulence in
the sense that they could be explained by assuming that fluctuations are
polarised (aligned) approximately as inertial waves (Alfven waves for MHD).
| [{'version': 'v1', 'created': 'Wed, 22 Apr 2009 16:13:46 GMT'}
{'version': 'v2', 'created': 'Mon, 28 Dec 2009 14:56:22 GMT'}
{'version': 'v3', 'created': 'Sat, 4 Jun 2011 11:21:12 GMT'}] | 2011-07-26 | [array(['Nazarenko', 'S. V.', '', 'Warwick'], dtype=object)
array(['Schekochihin', 'A. A.', '', 'Oxford'], dtype=object)] |
19,816 | cond-mat/0306569 | G. Baskaran | G. Baskaran (Matscience, Madras) | How Ice enables Superconductivity in Na_xCoO_2.yH_2O by melting charge
order: Possibility of novel Electric Field Effects | 5 pages of LaTex file, 4 figures in eps files; Invited Talk presented
at the 7th International Conference on Materials and Mechanisms of
Superconductivity and High Temperature Superconductors (M2S-Rio 2003),
Brazil, 26-30 May 2003. Typos and few sentences corrected | null | null | IMSc\2003\06\16 | cond-mat.str-el cond-mat.mtrl-sci | null | Charge ordering in doped \cob planes near the commensurate fillings $x =
{1/4}$ and 1/3 are considered for $Na_x CoO_2.yH_2O$ and suggested to be
competitors to superconductivity, leading to the experimentally seen narrow
superconducting dome bounded by commensurate doping: ${1/4}<x< {1/3}$.
Intercalated hydrogen bonded $H_2O$ network, by its enhanced dielectric
constant, screen and frustrate local {\em charge order condensation energy} and
replace a generic `charge glass order' by superconductivity in the dome. An
access to superconductivity and charge order, available through the new water
channel, is used to predict novel effects such as `Electrical Modulation of
Superconductivity' and `Electroresistance Effect'.
| [{'version': 'v1', 'created': 'Mon, 23 Jun 2003 15:22:02 GMT'}
{'version': 'v2', 'created': 'Tue, 24 Jun 2003 17:13:23 GMT'}] | 2007-05-23 | [array(['Baskaran', 'G.', '', 'Matscience, Madras'], dtype=object)] |
19,817 | 1907.08275 | Rachel Karpman | Rachel Karpman | The Purity Conjecture in Type $C$ | 14 pages, 2 figures | null | null | null | math.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A collection $\mathcal{C}$ of $k$-element subsets of $\{1,2,\ldots,m\}$ is
weakly separated if for each $I, J \in \mathcal{C}$, when the integers
$1,2,\ldots,m$ are arranged around in a circle, there is a chord separating $I
\backslash J$ from $J \backslash I$. Oh, Postnikov and Speyer constructed a
correspondence between weakly separated collections which are maximal by
inclusion and reduced plabic graphs, a class of networks defined by Postnikov
which give coordinate charts on the Grassmannian of $k$-planes in m-space. As a
corollary, they proved Scott's Purity Conjecture, which states that a weakly
separated collection is maximal by inclusion if and only if it is maximal by
size. In this note, we describe maximal weakly separated collections
corresponding to symmetric plabic graphs, which give coordinate charts on the
Lagrangian Grassmannian, and prove a symmetric version of the Purity
Conjecture.
| [{'version': 'v1', 'created': 'Thu, 18 Jul 2019 20:34:38 GMT'}] | 2019-07-22 | [array(['Karpman', 'Rachel', ''], dtype=object)] |
19,818 | math/0110292 | B. J. van der Steeg | K. P. Hart and B. J. van der Steeg | On the Ma\'{c}kowiak-Tymchatyn theorem | 16 pages | null | null | null | math.GN | null | In this paper we give new proofs of the theorem of Ma\'{c}kowiak and
Tymchatyn that every metric continuum is a weakly-confluent image of some
one-dimensional hereditarily indecomposable continuum of countable weight. The
first is a model-theoretic argument; the second is a topological proof inspired
by the first.
| [{'version': 'v1', 'created': 'Fri, 26 Oct 2001 13:07:40 GMT'}] | 2007-05-23 | [array(['Hart', 'K. P.', ''], dtype=object)
array(['van der Steeg', 'B. J.', ''], dtype=object)] |
19,819 | 1808.04505 | Tianshui Chen | Tianshui Chen, Wenxi Wu, Yuefang Gao, Le Dong, Xiaonan Luo, Liang Lin | Fine-Grained Representation Learning and Recognition by Exploiting
Hierarchical Semantic Embedding | Accepted at ACM MM 2018 as oral presentation | null | null | null | cs.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Object categories inherently form a hierarchy with different levels of
concept abstraction, especially for fine-grained categories. For example, birds
(Aves) can be categorized according to a four-level hierarchy of order, family,
genus, and species. This hierarchy encodes rich correlations among various
categories across different levels, which can effectively regularize the
semantic space and thus make prediction less ambiguous. However, previous
studies of fine-grained image recognition primarily focus on categories of one
certain level and usually overlook this correlation information. In this work,
we investigate simultaneously predicting categories of different levels in the
hierarchy and integrating this structured correlation information into the deep
neural network by developing a novel Hierarchical Semantic Embedding (HSE)
framework. Specifically, the HSE framework sequentially predicts the category
score vector of each level in the hierarchy, from highest to lowest. At each
level, it incorporates the predicted score vector of the higher level as prior
knowledge to learn finer-grained feature representation. During training, the
predicted score vector of the higher level is also employed to regularize label
prediction by using it as soft targets of corresponding sub-categories. To
evaluate the proposed framework, we organize the 200 bird species of the
Caltech-UCSD birds dataset with the four-level category hierarchy and construct
a large-scale butterfly dataset that also covers four level categories.
Extensive experiments on these two and the newly-released VegFru datasets
demonstrate the superiority of our HSE framework over the baseline methods and
existing competitors.
| [{'version': 'v1', 'created': 'Tue, 14 Aug 2018 02:09:34 GMT'}] | 2018-08-15 | [array(['Chen', 'Tianshui', ''], dtype=object)
array(['Wu', 'Wenxi', ''], dtype=object)
array(['Gao', 'Yuefang', ''], dtype=object)
array(['Dong', 'Le', ''], dtype=object)
array(['Luo', 'Xiaonan', ''], dtype=object)
array(['Lin', 'Liang', ''], dtype=object)] |
19,820 | 1003.5765 | Alexander Holevo | A. S. Holevo | The entropy gain of infinite-dimensional quantum channels | 10 pages | Doklady Mathematics, 82:2 (2010), 730-731 | 10.1134/S1064562410050133 | null | math-ph math.MP quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the present paper we study the entropy gain $H(\Phi [\rho])-H(\rho)$ for
infinite-dimensional channels $\Phi$. We show that unlike finite-dimensional
case where the minimal entropy gain is always nonpositive \cite{al}, there is a
plenty of channels with positive minimal entropy gain. We obtain the new lower
bound and compute the minimal entropy gain for a broad class of Bosonic
Gaussian channels by proving that the infimum is attained on the Gaussian
states.
| [{'version': 'v1', 'created': 'Tue, 30 Mar 2010 08:56:06 GMT'}] | 2010-11-23 | [array(['Holevo', 'A. S.', ''], dtype=object)] |
19,821 | 1202.0465 | Guido Montagna Prof | L. Barze', G. Montagna, P. Nason, O. Nicrosini and F. Piccinini | Implementation of electroweak corrections in the POWHEG BOX: single W
production | 31 pages, 7 figures. Minor corrections, references added and updated.
Final version to appear in JHEP | JHEP 1204 (2012) 037 | 10.1007/JHEP04(2012)037 | CERN-PH-TH-2012-025; FNT/2012/01; LPN12-031 | hep-ph hep-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present a fully consistent implementation of electroweak and strong
radiative corrections to single W hadroproduction in the POWHEG BOX framework,
treating soft and collinear photon emissions on the same ground as coloured
parton emissions. This framework can be easily extended to more complex
electroweak processes. We describe how next-to-leading order (NLO) electroweak
corrections are combined with the NLO QCD calculation, and show how they are
interfaced to QCD and QED shower Monte Carlo. The resulting tool fills a gap in
the literature and allows to study comprehensively the interplay of QCD and
electroweak effects to W production using a single computational framework.
Numerical comparisons with the predictions of the electroweak generator HORACE,
as well as with existing results on the combination of electroweak and QCD
corrections to W production, are shown for the LHC energies, to validate the
reliability and accuracy of the approach
| [{'version': 'v1', 'created': 'Thu, 2 Feb 2012 15:37:50 GMT'}
{'version': 'v2', 'created': 'Fri, 23 Mar 2012 11:23:57 GMT'}] | 2014-11-14 | [array(["Barze'", 'L.', ''], dtype=object)
array(['Montagna', 'G.', ''], dtype=object)
array(['Nason', 'P.', ''], dtype=object)
array(['Nicrosini', 'O.', ''], dtype=object)
array(['Piccinini', 'F.', ''], dtype=object)] |
19,822 | math/0504220 | Kui-hua Yan | Zhi-guang Hu and Kui-hua Yan | The Weyl Integration Model for KAK decomposition of Reductive Lie Group | 10 pages | null | null | null | math.GR | null | The Weyl integration model presented by An and Wang can be effectively used
to reduce the integration over $G$-space. In this paper, we construct an
especial Weyl integration model for KAK decomposition of Reductive Lie Group
and obtain an integration formula which implies that the integration of
$L^1$-integrable function over reductive Lie group $G$ can be carried out by
first integrating over each conjugacy class and then integrating over the set
of conjugacy classes.
| [{'version': 'v1', 'created': 'Mon, 11 Apr 2005 13:35:46 GMT'}] | 2007-05-23 | [array(['Hu', 'Zhi-guang', ''], dtype=object)
array(['Yan', 'Kui-hua', ''], dtype=object)] |
19,823 | hep-th/9703090 | Connie Jones | C. R. Hagen (University of Rochester) | Perturbative Expansion in the Galilean Invariant Spin One-Half
Chern-Simons Field Theory | 14 pages LaTeX, including 2 figures using epsf | Phys.Rev. D56 (1997) 2250-2256 | 10.1103/PhysRevD.56.2250 | null | hep-th quant-ph | null | A Galilean Chern-Simons field theory is formulated for the case of two
interacting spin-1/2 fields of distinct masses M and M'. A method for the
construction of states containing N particles of mass M and N' particles of
mass M' is given which is subsequently used to display equivalence to the
spin-1/2 Aharonov-Bohm effect in the N = N' =1 sector of the model. The latter
is then studied in perturbation theory to determine whether there are
divergences in the fourth order (one loop) diagram. It is found that the
contribution of that order is finite (and vanishing) for the case of parallel
spin projections while the antiparallel case displays divergences which are
known to characterize the spin zero case in field theory as well as in quantum
mechanics.
| [{'version': 'v1', 'created': 'Wed, 12 Mar 1997 19:14:05 GMT'}] | 2009-10-30 | [array(['Hagen', 'C. R.', '', 'University of Rochester'], dtype=object)] |
19,824 | 1806.02404 | Anders Sandberg | Anders Sandberg, Eric Drexler and Toby Ord | Dissolving the Fermi Paradox | Submitted to Proceedings of the Royal Society of London A; 4
supplements | null | null | null | physics.pop-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Fermi paradox is the conflict between an expectation of a high {\em ex
ante} probability of intelligent life elsewhere in the universe and the
apparently lifeless universe we in fact observe. The expectation that the
universe should be teeming with intelligent life is linked to models like the
Drake equation, which suggest that even if the probability of intelligent life
developing at a given site is small, the sheer multitude of possible sites
should nonetheless yield a large number of potentially observable
civilizations. We show that this conflict arises from the use of Drake-like
equations, which implicitly assume certainty regarding highly uncertain
parameters. We examine these parameters, incorporating models of chemical and
genetic transitions on paths to the origin of life, and show that extant
scientific knowledge corresponds to uncertainties that span multiple orders of
magnitude. This makes a stark difference. When the model is recast to represent
realistic distributions of uncertainty, we find a substantial {\em ex ante}
probability of there being no other intelligent life in our observable
universe, and thus that there should be little surprise when we fail to detect
any signs of it. This result dissolves the Fermi paradox, and in doing so
removes any need to invoke speculative mechanisms by which civilizations would
inevitably fail to have observable effects upon the universe.
| [{'version': 'v1', 'created': 'Wed, 6 Jun 2018 19:51:21 GMT'}] | 2018-06-08 | [array(['Sandberg', 'Anders', ''], dtype=object)
array(['Drexler', 'Eric', ''], dtype=object)
array(['Ord', 'Toby', ''], dtype=object)] |
19,825 | 2304.13688 | Tobias M\"uller | Tobias M\"uller, Milena Zahn and Florian Matthes | Unlocking the Potential of Collaborative AI -- On the Socio-technical
Challenges of Federated Machine Learning | Accepted for Publication at the 31st European Conference on
Information Systems (ECIS 2023) | null | null | null | cs.AI | http://creativecommons.org/licenses/by/4.0/ | The disruptive potential of AI systems roots in the emergence of big data.
Yet, a significant portion is scattered and locked in data silos, leaving its
potential untapped. Federated Machine Learning is a novel AI paradigm enabling
the creation of AI models from decentralized, potentially siloed data. Hence,
Federated Machine Learning could technically open data silos and therefore
unlock economic potential. However, this requires collaboration between
multiple parties owning data silos. Setting up collaborative business models is
complex and often a reason for failure. Current literature lacks guidelines on
which aspects must be considered to successfully realize collaborative AI
projects. This research investigates the challenges of prevailing collaborative
business models and distinct aspects of Federated Machine Learning. Through a
systematic literature review, focus group, and expert interviews, we provide a
systemized collection of socio-technical challenges and an extended Business
Model Canvas for the initial viability assessment of collaborative AI projects.
| [{'version': 'v1', 'created': 'Wed, 26 Apr 2023 17:14:44 GMT'}
{'version': 'v2', 'created': 'Thu, 27 Apr 2023 07:47:17 GMT'}
{'version': 'v3', 'created': 'Sat, 29 Apr 2023 00:15:47 GMT'}] | 2023-05-02 | [array(['Müller', 'Tobias', ''], dtype=object)
array(['Zahn', 'Milena', ''], dtype=object)
array(['Matthes', 'Florian', ''], dtype=object)] |
19,826 | cond-mat/0204013 | Igor Mazin | I. I. Mazin, O. K. Andersen, O. Jepsen, O. V. Dolgov, J. Kortus, A. A.
Golubov, A. B. Kuz'menko, D. van der Marel | Two-gap superconductivity in MgB$_{2}$: clean or dirty? | null | Phys. Rev. Lett 89, 107002 (2002) | 10.1103/PhysRevLett.89.107002 | null | cond-mat.supr-con | null | A large number of experimental facts and theoretical arguments favor a
two-gap model for superconductivity in MgB$_{2}$. However, this model predicts
strong suppression of the critical temperature by interband impurity scattering
and, presumably, a strong correlation between the critical temperature and the
residual resistivity. No such correlation has been observed. We argue that this
fact can be understood if the band disparity of the electronic structure is
taken into account, not only in the superconducting state, but also in normal
transport.
| [{'version': 'v1', 'created': 'Mon, 1 Apr 2002 16:50:37 GMT'}] | 2009-11-07 | [array(['Mazin', 'I. I.', ''], dtype=object)
array(['Andersen', 'O. K.', ''], dtype=object)
array(['Jepsen', 'O.', ''], dtype=object)
array(['Dolgov', 'O. V.', ''], dtype=object)
array(['Kortus', 'J.', ''], dtype=object)
array(['Golubov', 'A. A.', ''], dtype=object)
array(["Kuz'menko", 'A. B.', ''], dtype=object)
array(['van der Marel', 'D.', ''], dtype=object)] |
19,827 | 1510.05000 | Gregory Ngirmang | Gregory K. Ngirmang, Chris Orban, Scott Feister, John T. Morrison,
Kyle Frische, Enam A. Chowdhury and W. M. Roquemore | 3D PIC simulations of electron beams created via reflection of intense
laser light from a water target | version 3, with a few updates. Submitted to PoP. 10 pages, Comments
welcome! | null | 10.1063/1.4945739 | null | physics.plasm-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present 3D Particle-in-Cell (PIC) modeling of an ultra-intense laser
experiment by the Extreme Light group at the Air Force Research Laboratory
(AFRL) using the PIC code LSP. This is the first time PIC simulations have been
performed in 3D for this experiment which involves an ultra-intense,
short-pulse (30 fs) laser interacting with a water jet target at normal
incidence. These 3D PIC simulation results are compared to results from
2D(3$v$) PIC simulations for both $5.4~\cdot~10^{17}$ W cm$^{-2}$ and
$3~\cdot~10^{17}$ W cm$^{-2}$ intensities. Comparing the 2D(3$v$) and 3D
simulation results, the laser-energy-to-ejected-electron-energy conversion
efficiencies were comparable, but the angular distribution of ejected electrons
show interesting differences with qualitative differences at higher intensity.
An analytic plane-wave model is discussed which provides some explanation for
the angular distribution and energies of ejected electrons in the 2D(3$v$)
simulations. We also performed a 3D simulation with circularly polarized light
and found a significantly higher conversion efficiency and peak electron
energy, which is promising for future experiments.
| [{'version': 'v1', 'created': 'Fri, 16 Oct 2015 19:58:58 GMT'}
{'version': 'v2', 'created': 'Tue, 1 Dec 2015 22:21:19 GMT'}
{'version': 'v3', 'created': 'Wed, 6 Jan 2016 04:11:53 GMT'}] | 2016-05-25 | [array(['Ngirmang', 'Gregory K.', ''], dtype=object)
array(['Orban', 'Chris', ''], dtype=object)
array(['Feister', 'Scott', ''], dtype=object)
array(['Morrison', 'John T.', ''], dtype=object)
array(['Frische', 'Kyle', ''], dtype=object)
array(['Chowdhury', 'Enam A.', ''], dtype=object)
array(['Roquemore', 'W. M.', ''], dtype=object)] |
19,828 | 1401.4953 | Han Jingjun | Jingjun Han, Liyun Dai, Bican Xia | Constructing Fewer Open Cells by GCD Computation in CAD Projection | Accepted by ISSAC 2014 (July 23--25, 2014, Kobe, Japan) | null | 10.1145/2608628.2608676 | null | cs.SC | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | A new projection operator based on cylindrical algebraic decomposition (CAD)
is proposed. The new operator computes the intersection of projection factor
sets produced by different CAD projection orders. In other words, it computes
the gcd of projection polynomials in the same variables produced by different
CAD projection orders. We prove that the new operator still guarantees
obtaining at least one sample point from every connected component of the
highest dimension, and therefore, can be used for testing semi-definiteness of
polynomials. Although the complexity of the new method is still doubly
exponential, in many cases, the new operator does produce smaller projection
factor sets and fewer open cells. Some examples of testing semi-definiteness of
polynomials, which are difficult to be solved by existing tools, have been
worked out efficiently by our program based on the new method.
| [{'version': 'v1', 'created': 'Mon, 20 Jan 2014 15:55:33 GMT'}
{'version': 'v2', 'created': 'Sat, 17 May 2014 15:20:27 GMT'}] | 2014-05-20 | [array(['Han', 'Jingjun', ''], dtype=object)
array(['Dai', 'Liyun', ''], dtype=object)
array(['Xia', 'Bican', ''], dtype=object)] |
19,829 | 1605.03640 | Amine Ahriche | Dounia Cherigui, Chahrazed Guella (Oran, Sci. Tech. U.), Amine Ahriche
(Jijel U. and ICTP, Trieste and NCTS, Taipei), Salah Nasri (United Arab
Emirates U.) | Probing Radiative Neutrino Mass Models Using Trilepton Channel at the
LHC | 10 pages, 6 figures & 4 tables | Phys. Lett. B762 (2016) 225-231 | 10.1016/j.physletb.2016.09.031 | null | hep-ph hep-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work, we probe a class of neutrino mass models through the lepton
flavor violating interactions of a singlet charged scalar, $S^{\pm}$ at the LHC
proton-proton collisions with 8 TeV and 14 TeV energies. This scalar couples to
the leptons and induces many processes such as
$pp\rightarrow\ell^{\pm}\ell^{\pm}\ell^{\mp}+\slashed{E}_{T}$. In our analysis
we discuss the opposite sign same flavor leptons signal, as well as the
background free channel with the tau contribution which can enhance the
signal/background ratio for center of mass energies $\sqrt{s}$= 8 TeV and
$\sqrt{s}$ = 14 TeV.
| [{'version': 'v1', 'created': 'Wed, 11 May 2016 23:45:12 GMT'}
{'version': 'v2', 'created': 'Wed, 30 Nov 2016 20:08:26 GMT'}] | 2016-12-01 | [array(['Cherigui', 'Dounia', '', 'Oran, Sci. Tech. U.'], dtype=object)
array(['Guella', 'Chahrazed', '', 'Oran, Sci. Tech. U.'], dtype=object)
array(['Ahriche', 'Amine', '',
'Jijel U. and ICTP, Trieste and NCTS, Taipei'], dtype=object)
array(['Nasri', 'Salah', '', 'United Arab\n Emirates U.'], dtype=object)] |
19,830 | 2003.02373 | Sizheng Ma | Sizheng Ma, Hang Yu, Yanbei Chen | Excitation of f-modes during mergers of spinning binary neutron star | null | Phys. Rev. D 101, 123020 (2020) | 10.1103/PhysRevD.101.123020 | null | gr-qc astro-ph.HE | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Tidal effects have important imprints on gravitational waves (GWs) emitted
during the final stage of the coalescence of binaries that involve neutron
stars (NSs). Dynamical tides can be significant when NS oscillations become
resonant with orbital motion; understanding this process is important for
accurately modeling GW emission from these binaries, and for extracting NS
information from GW data. In this paper, we carry out a systematic study on the
tidal excitation of fundamental modes of spinning NSs in coalescencing
binaries, focusing on the case when the NS spin is anti-aligned with the
orbital angular momentum-where the tidal resonance is most likely to take
place. We first expand NS oscillations into stellar eigen-modes, and then
obtain a Hamiltonian that governs the tidally coupled orbit-mode evolution. We
next find a new approximation that can lead to analytic expressions of tidal
excitations to a high accuracy, and are valid in all regimes of the binary
evolution: adiabatic, resonant, and post-resonance. Using the method of
osculating orbits, we obtain semi-analytic approximations to the orbital
evolution and GW emission; their agreements with numerical results give us
confidence in on our understanding of the system's dynamics. In particular, we
recover both the averaged post-resonance evolution, which differs from the
pre-resonance point-particle orbit by shifts in orbital energy and angular
momentum, as well as instantaneous perturbations driven by the tidal motion.
Finally, we use the Fisher matrix technique to study the effect of dynamical
tides on parameter estimation. We find that the dynamical tides may potentially
provide an additional channel to study the physics of NSs. The method presented
in this paper is generic and not restricted to f mode; it can also be applied
to other types of tide.
| [{'version': 'v1', 'created': 'Wed, 4 Mar 2020 23:55:04 GMT'}
{'version': 'v2', 'created': 'Thu, 4 Jun 2020 03:41:46 GMT'}] | 2020-06-19 | [array(['Ma', 'Sizheng', ''], dtype=object)
array(['Yu', 'Hang', ''], dtype=object)
array(['Chen', 'Yanbei', ''], dtype=object)] |
19,831 | 2111.06801 | Igor Melnyk | Igor Melnyk, Payel Das, Vijil Chenthamarakshan, Aurelie Lozano | Benchmarking deep generative models for diverse antibody sequence design | Learning Meaningful Representations of Life Workshop paper at NeurIPS
2021 | null | null | null | q-bio.BM cs.CL | http://creativecommons.org/licenses/by/4.0/ | Computational protein design, i.e. inferring novel and diverse protein
sequences consistent with a given structure, remains a major unsolved
challenge. Recently, deep generative models that learn from sequences alone or
from sequences and structures jointly have shown impressive performance on this
task. However, those models appear limited in terms of modeling structural
constraints, capturing enough sequence diversity, or both. Here we consider
three recently proposed deep generative frameworks for protein design: (AR) the
sequence-based autoregressive generative model, (GVP) the precise
structure-based graph neural network, and Fold2Seq that leverages a fuzzy and
scale-free representation of a three-dimensional fold, while enforcing
structure-to-sequence (and vice versa) consistency. We benchmark these models
on the task of computational design of antibody sequences, which demand
designing sequences with high diversity for functional implication. The
Fold2Seq framework outperforms the two other baselines in terms of diversity of
the designed sequences, while maintaining the typical fold.
| [{'version': 'v1', 'created': 'Fri, 12 Nov 2021 16:23:32 GMT'}] | 2021-11-15 | [array(['Melnyk', 'Igor', ''], dtype=object)
array(['Das', 'Payel', ''], dtype=object)
array(['Chenthamarakshan', 'Vijil', ''], dtype=object)
array(['Lozano', 'Aurelie', ''], dtype=object)] |
19,832 | 2011.10135 | Ge He | Ge He, Dong Li, Daniel Jost, Andi Baum, Peipei Shen, Xiaoli Dong,
Zhongxian Zhao, and Rudi Hackl | Raman Study of Cooper Pairing Instabilities in (Li$_{1-x}$Fe$_x$)OHFeSe | 9 pages, 12 figures | Phys. Rev. Lett. 125, 217002(2020) | 10.1103/PhysRevLett.125.217002 | null | cond-mat.supr-con cond-mat.str-el | http://creativecommons.org/publicdomain/zero/1.0/ | We studied the electronic Raman spectra of (Li$_{1-x}$Fe$_x$)OHFeSe as a
function of light polarization and temperature. In the B$_{1g}$ spectra alone
we observe the redistribution of spectral weight expected for a superconductor
and two well-resolved peaks below T$_c$. The nearly resolution-limited peak at
110 cm$^{-1}$ (13.6 meV) is identified as a collective mode. The peak at 190
cm$^{-1}$ (23.6 meV) is presumably another collective mode since the line is
symmetric and its energy is significantly below the gap energy observed by
single-particle spectroscopies. Given the experimental band structure of
(Li$_{1-x}$Fe$_x$)OHFeSe, the most plausible explanations include conventional
spin-fluctuation pairing between the electron bands and the incipient hole band
and pairing between the hybridized electron bands. The absence of gap features
in A$_{1g}$ and B$_{2g}$ symmetry favors the second case. Thus, in spite of
various differences between the pnictides and chalcogenides, this Letter
demonstrates the proximity of pairing states and the importance of band
structure effects in the Fe-based compounds.
| [{'version': 'v1', 'created': 'Thu, 19 Nov 2020 22:44:45 GMT'}] | 2020-11-23 | [array(['He', 'Ge', ''], dtype=object)
array(['Li', 'Dong', ''], dtype=object)
array(['Jost', 'Daniel', ''], dtype=object)
array(['Baum', 'Andi', ''], dtype=object)
array(['Shen', 'Peipei', ''], dtype=object)
array(['Dong', 'Xiaoli', ''], dtype=object)
array(['Zhao', 'Zhongxian', ''], dtype=object)
array(['Hackl', 'Rudi', ''], dtype=object)] |
19,833 | astro-ph/0403525 | Ata Sarajedini | Glenn P. Tiede, Ata Sarajedini, and Michael K. Barker | The Stellar Populations in the Outer Regions of M33. I. Metallicity
Distribution Function | 34 pages, 13 figures, accepted to The Astronomical Journal, July
2004, high resolution version available at
ftp://www.astro.ufl.edu/pub/ata/sarajedini_m33.pdf | null | 10.1086/421369 | null | astro-ph | null | We present deep CCD photometry in the VI passbands using the WIYN 3.5m
telescope of a field located approximately 20' southeast of the center of M33;
this field includes the region studied by Mould & Kristian in their 1986 paper.
The color-magnitude diagram (CMD) extends to I~25 and shows a prominent red
giant branch (RGB), along with significant numbers of asymptotic giant branch
and young main sequence stars. The red clump of core helium burning stars is
also discernable near the limit of our CMD. The I-band apparent magnitude of
the red giant branch tip implies a distance modulus of (m-M)_I = 24.77 +/-
0.06, which combined with an adopted reddening of E(V-I)=0.06 +/- 0.02 yields
an absolute modulus of (m-M)_0 = 24.69 +/- 0.07 (867 +/- 28 kpc) for M33. Over
the range of deprojected radii covered by our field (~8.5 to ~12.5 kpc), we
find a significant age gradient with an upper limit of ~1 Gyr (~0.25 Gyr/kpc).
Comparison of the RGB photometry to empirical giant branch sequences for
Galactic globulars allows us to use the dereddened color of these stars to
construct a metallicity distribution function (MDF). The primary peak in the
MDF is at a metallicity of [Fe/H] ~ -1.0 with a tail to lower abundances. The
peak does show radial variation with a slope of d[Fe/H]/dR_{deproj} = -0.06 +/-
0.01 dex/kpc. This gradient is consistent with the variation seen in the inner
disk regions of M33. As such, we conclude that the vast majority of stars in
this field belong to the disk of M33, not the halo as previously thought.
| [{'version': 'v1', 'created': 'Mon, 22 Mar 2004 17:01:39 GMT'}] | 2009-11-10 | [array(['Tiede', 'Glenn P.', ''], dtype=object)
array(['Sarajedini', 'Ata', ''], dtype=object)
array(['Barker', 'Michael K.', ''], dtype=object)] |
19,834 | 1708.03682 | Johanna Palmstrom | Johanna C. Palmstrom and Alexander T. Hristov and Steven A. Kivelson
and Jiun-Haw Chu and Ian R. Fisher | Critical divergence of the symmetric ($A_{1g}$) nonlinear
elastoresistance near the nematic transition in an iron-based superconductor | null | Phys. Rev. B 96, 205133 (2017) | 10.1103/PhysRevB.96.205133 | null | cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We report the observation of a nonlinear elastoresistivity response for the
prototypical underdoped iron pnictide Ba(Fe$_{0.975}$Co$_{0.025}$)$_2$As$_2$.
Our measurements reveal a large quadratic term in the isotropic ($A_{1g}$)
electronic response that was produced by a purely shear ($B_{2g}$) strain. The
divergence of this quantity upon cooling towards the structural phase
transition reflects the temperature dependence of the nematic susceptibility.
This observation shows that nematic fluctuations play a significant role in
determining even the isotropic properties of this family of compounds.
| [{'version': 'v1', 'created': 'Fri, 11 Aug 2017 19:49:45 GMT'}] | 2017-11-22 | [array(['Palmstrom', 'Johanna C.', ''], dtype=object)
array(['Hristov', 'Alexander T.', ''], dtype=object)
array(['Kivelson', 'Steven A.', ''], dtype=object)
array(['Chu', 'Jiun-Haw', ''], dtype=object)
array(['Fisher', 'Ian R.', ''], dtype=object)] |
19,835 | 1908.06544 | Yudhik Agrawal | Abbhinav Venkat, Chaitanya Patel, Yudhik Agrawal, Avinash Sharma | HumanMeshNet: Polygonal Mesh Recovery of Humans | to appear in ICCV-W, 2019. Project:
https://github.com/yudhik11/HumanMeshNet | null | null | null | cs.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | 3D Human Body Reconstruction from a monocular image is an important problem
in computer vision with applications in virtual and augmented reality
platforms, animation industry, en-commerce domain, etc. While several of the
existing works formulate it as a volumetric or parametric learning with complex
and indirect reliance on re-projections of the mesh, we would like to focus on
implicitly learning the mesh representation. To that end, we propose a novel
model, HumanMeshNet, that regresses a template mesh's vertices, as well as
receives a regularization by the 3D skeletal locations in a multi-branch,
multi-task setup. The image to mesh vertex regression is further regularized by
the neighborhood constraint imposed by mesh topology ensuring smooth surface
reconstruction. The proposed paradigm can theoretically learn local surface
deformations induced by body shape variations and can therefore learn
high-resolution meshes going ahead. We show comparable performance with SoA (in
terms of surface and joint error) with far lesser computational complexity,
modeling cost and therefore real-time reconstructions on three publicly
available datasets. We also show the generalizability of the proposed paradigm
for a similar task of predicting hand mesh models. Given these initial results,
we would like to exploit the mesh topology in an explicit manner going ahead.
| [{'version': 'v1', 'created': 'Mon, 19 Aug 2019 00:27:24 GMT'}] | 2019-08-20 | [array(['Venkat', 'Abbhinav', ''], dtype=object)
array(['Patel', 'Chaitanya', ''], dtype=object)
array(['Agrawal', 'Yudhik', ''], dtype=object)
array(['Sharma', 'Avinash', ''], dtype=object)] |
19,836 | 1803.02870 | Md Tauhidul Islam | Md Tauhidul Islam, Udoy Saha, K.T. Shahid, Ahmed Bin Hussain, Celia
Shahnaz | Speech Enhancement Based on Non-stationary Noise-driven Geometric
Spectral Subtraction and Phase Spectrum Compensation | 13 pages, 10 figures, 8 tables. arXiv admin note: substantial text
overlap with arXiv:1803.00396; text overlap with arXiv:1802.02665,
arXiv:1802.05125, arXiv:1803.01841 | null | null | null | eess.AS cs.SD | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, a speech enhancement method based on noise compensation
performed on short time magnitude as well phase spectra is presented. Unlike
the conventional geometric approach (GA) to spectral subtraction (SS), here the
noise estimate to be subtracted from the noisy speech spectrum is proposed to
be determined by exploiting the low frequency regions of current frame of noisy
speech rather than depending only on the initial silence frames. This approach
gives the capability of tracking non-stationary noise thus resulting in a
non-stationary noise-driven geometric approach of spectral subtraction for
speech enhancement. The noise compensated magnitude spectrum from the GA step
is then recombined with unchanged phase of noisy speech spectrum and used in
phase compensation to obtain an enhanced complex spectrum, which is used to
produce an enhanced speech frame. Extensive simulations are carried out using
speech files available in the NOIZEUS database shows that the proposed method
consistently outperforms some of the recent methods of speech enhancement when
employed on the noisy speeches corrupted by street or babble noise at different
levels of SNR in terms of objective measures, spectrogram analysis and formal
subjective listening tests.
| [{'version': 'v1', 'created': 'Sat, 3 Mar 2018 05:57:11 GMT'}] | 2018-03-09 | [array(['Islam', 'Md Tauhidul', ''], dtype=object)
array(['Saha', 'Udoy', ''], dtype=object)
array(['Shahid', 'K. T.', ''], dtype=object)
array(['Hussain', 'Ahmed Bin', ''], dtype=object)
array(['Shahnaz', 'Celia', ''], dtype=object)] |
19,837 | 1601.00076 | Roldao da Rocha | R. A. C. Correa, D. M. Dantas, C. A. S. Almeida, Roldao da Rocha | Bounds on topological Abelian string-vortex and string-cigar from
information-entropic measure | 6 pages, 7 figures, final version to appear in Phys. Lett. B | Phys. Lett. B 755 (2016) 358 | 10.1016/j.physletb.2016.02.038 | null | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this work we obtain bounds on the topological Abelian string-vortex and on
the string-cigar, by using a new measure of configurational complexity, known
as configurational entropy. In this way, the information-theoretical measure of
six-dimensional braneworlds scenarios are capable to probe situations where the
parameters responsible for the brane thickness are arbitrary. The so-called
configurational entropy (CE) selects the best value of the parameter in the
model. This is accomplished by minimizing the CE, namely, by selecting the most
appropriate parameters in the model that correspond to the most organized
system, based upon the Shannon information theory. This information-theoretical
measure of complexity provides a complementary perspective to situations where
strictly energy-based arguments are inconclusive. We show that the higher the
energy the higher the CE, what shows an important correlation between the
energy of the a localized field configuration and its associated entropic
measure.
| [{'version': 'v1', 'created': 'Fri, 1 Jan 2016 12:22:22 GMT'}
{'version': 'v2', 'created': 'Wed, 17 Feb 2016 17:36:53 GMT'}] | 2016-08-02 | [array(['Correa', 'R. A. C.', ''], dtype=object)
array(['Dantas', 'D. M.', ''], dtype=object)
array(['Almeida', 'C. A. S.', ''], dtype=object)
array(['da Rocha', 'Roldao', ''], dtype=object)] |
19,838 | 2111.08662 | Braden Crimmins | Braden L. Crimmins, Marshall Rhea, J. Alex Halderman | RemoteVote and SAFE Vote: Towards Usable End-to-End Verification for
Vote-by-Mail | null | null | null | null | cs.CR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Postal voting is growing rapidly in the U.S., with 43% of voters casting
ballots by mail in 2020, yet until recently there has been little research
about extending the protections of end-to-end verifiable (E2E-V) election
schemes to vote-by-mail contexts. The first - and to date, only - framework to
focus on this setting is STROBE, which has important usability limitations. In
this work, we present two approaches, RemoteVote and SAFE Vote, that allow
mail-in voters to benefit from E2E-V without changing the voter experience for
those who choose not to participate in verification. To evaluate these systems
and compare them with STROBE, we consider an expansive set of properties,
including novel attributes of usability and verifiability, several of which
have applicability beyond vote-by-mail contexts. We hope that our work will
help catalyze further progress towards universal applicability of E2E-V for
real-world elections.
| [{'version': 'v1', 'created': 'Tue, 16 Nov 2021 17:49:54 GMT'}
{'version': 'v2', 'created': 'Wed, 17 Nov 2021 06:19:36 GMT'}
{'version': 'v3', 'created': 'Sun, 16 Jan 2022 21:19:49 GMT'}] | 2022-01-19 | [array(['Crimmins', 'Braden L.', ''], dtype=object)
array(['Rhea', 'Marshall', ''], dtype=object)
array(['Halderman', 'J. Alex', ''], dtype=object)] |
19,839 | 1907.06391 | Anke Arentsen | Anke Arentsen, Philippe Prugniel, Anais Gonneau, Ariane Lan\c{c}on,
Scott Trager, Reynier Peletier, Mariya Lyubenova, Yan-Ping Chen, Jes\'us
Falc\'on Barroso, Patricia S\'anchez Bl\'azquez, and Alejandro Vazdekis | Stellar atmospheric parameters for 754 spectra from the X-shooter
Spectral Library | 15 pages, 12 figures, 3 tables, published in A&A | 2019, A&A, 627, A138 | 10.1051/0004-6361/201834273 | null | astro-ph.SR astro-ph.GA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The X-shooter Spectral Library (XSL) is an empirical stellar library at
medium spectral resolution covering the wavelength range from 3000 \AA to 24
800 \AA. This library aims to provide a benchmark for stellar population
studies. In this work, we present a uniform set of stellar atmospheric
parameters, effective temperatures, surface gravities, and iron abundances for
754 spectra of 616 XSL stars. We used the full-spectrum fitting package ULySS
with the empirical MILES library as reference to fit the ultraviolet-blue (UVB)
and visible (VIS) spectra. We tested the internal consistency and we compared
our results with compilations from the literature. The stars cover a range of
effective temperature 2900 < Teff < 38 000 K, surface gravity 0 < log g < 5.7,
and iron abundance -2.5 < [Fe/H] < +1.0, with a couple of stars extending down
to [Fe/H] = -3.9. The precisions of the measurements for the G- and K-type
stars are 0.9%, 0.14, and 0.06 in Teff, log g, and [Fe/H], respectively. For
the cool giants with log g < 1, the precisions are 2.1%, 0.21, and 0.22, and
for the other cool stars these values are 1%, 0.14, and 0.10. For the hotter
stars (Teff > 6500 K), these values are 2.6%, 0.20, and 0.10 for the three
parameters.
| [{'version': 'v1', 'created': 'Mon, 15 Jul 2019 09:39:31 GMT'}] | 2019-07-24 | [array(['Arentsen', 'Anke', ''], dtype=object)
array(['Prugniel', 'Philippe', ''], dtype=object)
array(['Gonneau', 'Anais', ''], dtype=object)
array(['Lançon', 'Ariane', ''], dtype=object)
array(['Trager', 'Scott', ''], dtype=object)
array(['Peletier', 'Reynier', ''], dtype=object)
array(['Lyubenova', 'Mariya', ''], dtype=object)
array(['Chen', 'Yan-Ping', ''], dtype=object)
array(['Barroso', 'Jesús Falcón', ''], dtype=object)
array(['Blázquez', 'Patricia Sánchez', ''], dtype=object)
array(['Vazdekis', 'Alejandro', ''], dtype=object)] |
19,840 | hep-ph/0211436 | Gerasyuta S. M. | S.M. Gerasyuta, V.I. Kochkin | Relativistic quark model and pentaquark spectroscopy | 22 pages, pdf | Int.J.Mod.Phys. E12 (2003) 793-808 | 10.1142/S0218301303001582 | null | hep-ph | null | The relativistic five-quark equations are found in the framework of the
dispersion relation technique. The solutions of these equations using the
method based on the extraction of leading singularities of the amplitudes are
obtained. The five-quark amplitudes for the low-lying pentaquarks are
calculated under the condition that flavor SU(3) symmetry holds. The poles of
five-quark amplitudes determine the masses of the lowest pentaquarks. The mass
spectra of pentaquarks which contain only light quarks are calculated. The
calculation of pentaquark amplitudes estimates the contributions of three
subamplitudes. The main contributions to the pentaquark amplitude are
determined by the subamplitudes, which include the meson states.
| [{'version': 'v1', 'created': 'Wed, 27 Nov 2002 18:49:21 GMT'}] | 2009-11-07 | [array(['Gerasyuta', 'S. M.', ''], dtype=object)
array(['Kochkin', 'V. I.', ''], dtype=object)] |
19,841 | hep-ph/0103051 | Jun Yan | Guang-jiong Ni and Tsao Chang | Is Neutrino a Superluminal Particle? | 10 pages, No figures | null | null | null | hep-ph | null | Based on the experimental discovery that the mass-square of neutrino is
negative, a quantum theory for superluminal neutrino is proposed. Two Weyl
equations coupled together via a mass term respecting the maximum parity
violation lead to a new equation which describes the superluminal motion of
neutrino with permanent helicity. Various strange features of subluminal and
superluminal particles can be ascribed to the relative variation of two
contradictory fields superposing coherently inside the particle with the change
of its speed u in the whole range ($0<u<\infty$). Being compatible with the
theory of special relativity, this theory may have various applications.
| [{'version': 'v1', 'created': 'Mon, 5 Mar 2001 16:54:53 GMT'}] | 2007-05-23 | [array(['Ni', 'Guang-jiong', ''], dtype=object)
array(['Chang', 'Tsao', ''], dtype=object)] |
19,842 | 2212.13915 | Deguang Kong | Deguang Kong, Konstantin Shmakov and Jian Yang | Demystifying Advertising Campaign Bid Recommendation: A Constraint
target CPA Goal Optimization | null | null | null | null | cs.IR cs.AI cs.LG | http://creativecommons.org/licenses/by/4.0/ | In cost-per-click (CPC) or cost-per-impression (CPM) advertising campaigns,
advertisers always run the risk of spending the budget without getting enough
conversions. Moreover, the bidding on advertising inventory has few connections
with propensity one that can reach to target cost-per-acquisition (tCPA) goals.
To address this problem, this paper presents a bid optimization scenario to
achieve the desired tCPA goals for advertisers. In particular, we build the
optimization engine to make a decision by solving the rigorously formalized
constrained optimization problem, which leverages the bid landscape model
learned from rich historical auction data using non-parametric learning. The
proposed model can naturally recommend the bid that meets the advertisers'
expectations by making inference over advertisers' historical auction
behaviors, which essentially deals with the data challenges commonly faced by
bid landscape modeling: incomplete logs in auctions, and uncertainty due to the
variation and fluctuations in advertising bidding behaviors. The bid
optimization model outperforms the baseline methods on real-world campaigns,
and has been applied into a wide range of scenarios for performance improvement
and revenue liftup.
| [{'version': 'v1', 'created': 'Mon, 26 Dec 2022 07:43:26 GMT'}] | 2022-12-29 | [array(['Kong', 'Deguang', ''], dtype=object)
array(['Shmakov', 'Konstantin', ''], dtype=object)
array(['Yang', 'Jian', ''], dtype=object)] |
19,843 | 2305.00183 | Kiyoshi Shiraishi | Nahomi Kan, Kiyoshi Shiraishi | Dynamical mass generation of spin-2 fields in de Sitter space for an
$O(N)$ symmetric model at large $N$ | 15 pages, 7 figures | null | null | null | hep-th | http://creativecommons.org/licenses/by/4.0/ | We consider the strong-coupling phase in a model of $O(N)$ spin-2 field
theory in de Sitter spacetime and the effective mass of spin-2 fields therein.
In the strong-coupling phase, the Higuchi bound limits the parameters included
in the theory. The analysis using the large $N$ approximation finds the
critical value of the parameters with numerical calculation.
| [{'version': 'v1', 'created': 'Sat, 29 Apr 2023 06:27:28 GMT'}] | 2023-05-02 | [array(['Kan', 'Nahomi', ''], dtype=object)
array(['Shiraishi', 'Kiyoshi', ''], dtype=object)] |
19,844 | 2306.05185 | Constantin Christof | Constantin Christof and Julia Kowalczyk | On the Identification and Optimization of Nonsmooth Superposition
Operators in Semilinear Elliptic PDEs | null | null | null | null | math.OC cs.LG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study an infinite-dimensional optimization problem that aims to identify
the Nemytskii operator in the nonlinear part of a prototypical semilinear
elliptic partial differential equation (PDE) which minimizes the distance
between the PDE-solution and a given desired state. In contrast to previous
works, we consider this identification problem in a low-regularity regime in
which the function inducing the Nemytskii operator is a-priori only known to be
an element of $H^1_{loc}(\mathbb{R})$. This makes the studied problem class a
suitable point of departure for the rigorous analysis of training problems for
learning-informed PDEs in which an unknown superposition operator is
approximated by means of a neural network with nonsmooth activation functions
(ReLU, leaky-ReLU, etc.). We establish that, despite the low regularity of the
controls, it is possible to derive a classical stationarity system for local
minimizers and to solve the considered problem by means of a gradient
projection method. The convergence of the resulting algorithm is proven in the
function space setting. It is also shown that the established first-order
necessary optimality conditions imply that locally optimal superposition
operators share various characteristic properties with commonly used activation
functions: They are always sigmoidal, continuously differentiable away from the
origin, and typically possess a distinct kink at zero. The paper concludes with
numerical experiments which confirm the theoretical findings.
| [{'version': 'v1', 'created': 'Thu, 8 Jun 2023 13:33:20 GMT'}] | 2023-06-09 | [array(['Christof', 'Constantin', ''], dtype=object)
array(['Kowalczyk', 'Julia', ''], dtype=object)] |
19,845 | 1611.06621 | Shilpak Banerjee | Shilpak Banerjee and Philipp Kunde | Real-analytic AbC constructions on the torus | 48 pages, 7 figures | Ergod. Th. Dynam. Sys. 39 (2019) 2643-2688 | 10.1017/etds.2017.132 | null | math.DS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this article we demonstrate a way to extend the AbC (approximation by
conjugation) method invented by Anosov and Katok from the smooth category to
the category of real-analytic diffeomorphisms on the torus. We present a
general framework for such constructions and prove several results. In
particular, we construct minimal but not uniquely ergodic diffeomorphisms and
nonstandard real-analytic realizations of toral translations.
| [{'version': 'v1', 'created': 'Mon, 21 Nov 2016 00:56:48 GMT'}] | 2019-09-11 | [array(['Banerjee', 'Shilpak', ''], dtype=object)
array(['Kunde', 'Philipp', ''], dtype=object)] |
19,846 | 1905.04434 | Jingjin Yu | Si Wei Feng and Shuai D. Han and Kai Gao and Jingjin Yu | Efficient Algorithms for Optimal Perimeter Guarding | null | 2019 Robotics: Science and Systems | null | null | cs.RO cs.CG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We investigate the problem of optimally assigning a large number of robots
(or other types of autonomous agents) to guard the perimeters of closed 2D
regions, where the perimeter of each region to be guarded may contain multiple
disjoint polygonal chains. Each robot is responsible for guarding a subset of a
perimeter and any point on a perimeter must be guarded by some robot. In
allocating the robots, the main objective is to minimize the maximum 1D
distance to be covered by any robot along the boundary of the regions. For this
optimization problem which we call optimal perimeter guarding (OPG), thorough
structural analysis is performed, which is then exploited to develop fast exact
algorithms that run in guaranteed low polynomial time. In addition to formal
analysis and proofs, experimental evaluations and simulations are performed
that further validate the correctness and effectiveness of our algorithmic
results.
| [{'version': 'v1', 'created': 'Sat, 11 May 2019 03:06:40 GMT'}] | 2019-05-14 | [array(['Feng', 'Si Wei', ''], dtype=object)
array(['Han', 'Shuai D.', ''], dtype=object)
array(['Gao', 'Kai', ''], dtype=object)
array(['Yu', 'Jingjin', ''], dtype=object)] |
19,847 | 0910.1351 | Max Tegmark | Andy Lutomirski (MIT), Max Tegmark (MIT), Nevada Sanchez (MIT), Leo
Stein (MIT), Lynn Urry (Berkeley), Matias Zaldarriaga (IAS) | Solving the Corner-Turning Problem for Large Interferometers | Revised to match accepted MNRAS version. 7 pages, 4 figs | null | 10.1111/j.1365-2966.2010.17587.x | null | astro-ph.IM astro-ph.CO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The so-called corner turning problem is a major bottleneck for radio
telescopes with large numbers of antennas. The problem is essentially that of
rapidly transposing a matrix that is too large to store on one single device;
in radio interferometry, it occurs because data from each antenna needs to be
routed to an array of processors that will each handle a limited portion of the
data (a frequency range, say) but requires input from each antenna. We present
a low-cost solution allowing the correlator to transpose its data in real time,
without contending for bandwidth, via a butterfly network requiring neither
additional RAM memory nor expensive general-purpose switching hardware. We
discuss possible implementations of this using FPGA, CMOS, analog logic and
optical technology, and conclude that the corner turner cost can be small even
for upcoming massive radio arrays.
| [{'version': 'v1', 'created': 'Thu, 8 Oct 2009 19:16:10 GMT'}
{'version': 'v2', 'created': 'Wed, 25 Aug 2010 03:57:48 GMT'}] | 2010-12-14 | [array(['Lutomirski', 'Andy', '', 'MIT'], dtype=object)
array(['Tegmark', 'Max', '', 'MIT'], dtype=object)
array(['Sanchez', 'Nevada', '', 'MIT'], dtype=object)
array(['Stein', 'Leo', '', 'MIT'], dtype=object)
array(['Urry', 'Lynn', '', 'Berkeley'], dtype=object)
array(['Zaldarriaga', 'Matias', '', 'IAS'], dtype=object)] |
19,848 | 0810.5444 | Paul Sutcliffe | Paul Sutcliffe | Multi-Skyrmions with Vector Mesons | Version to appear in Phys. Rev. D | Phys.Rev.D79:085014,2009 | 10.1103/PhysRevD.79.085014 | DCPT-08/59 | hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | It is known that including vector mesons stabilizes the size of a Skyrmion
without the need for a Skyrme term. This paper provides the first results for
static multi-Skyrmions in such a theory. The rational map ansatz is used to
investigate multi-Skyrmions in a theory which includes the omega vector meson
and has no Skyrme term. Bound states with baryon numbers two, three and four
are found, which have axial, tetrahedral and cubic symmetries, respectively.
The results reveal a qualitative similarity with the standard Skyrme model with
a Skyrme term and no vector mesons, suggesting that some features are universal
and do not depend on the details of the theory. Setting the pion decay constant
and meson masses to their experimental values leaves only a single free
parameter in the model. Fixing this parameter, by equating the energy of the
baryon number four Skyrmion to the Helium-4 mass, yields reasonable results for
other baryon numbers.
| [{'version': 'v1', 'created': 'Thu, 30 Oct 2008 08:49:18 GMT'}
{'version': 'v2', 'created': 'Mon, 20 Apr 2009 11:51:42 GMT'}] | 2009-11-06 | [array(['Sutcliffe', 'Paul', ''], dtype=object)] |
19,849 | 2008.01277 | ShaoPeng Hong | Hong Shaopeng | Generalized Autoregressive Score asymmetric Laplace Distribution and
Extreme Downward Risk Prediction | 13 pages, 12 figures | null | null | null | q-fin.RM | http://creativecommons.org/licenses/by/4.0/ | Due to the skessed distribution, high peak and thick tail and asymmetry of
financial return data, it is difficult to describe the traditional
distribution. In recent years, generalized autoregressive score (GAS) has been
used in many fields and achieved good results. In this paper, under the
framework of generalized autoregressive score (GAS), the asymmetric Laplace
distribution (ALD) is improved, and the GAS-ALD model is proposed, which has
the characteristics of time-varying parameters, can describe the peak thick
tail, biased and asymmetric distribution. The model is used to study the
Shanghai index, Shenzhen index and SME board index. It is found that: 1) the
distribution parameters and moments of the three indexes have obvious
time-varying characteristics and aggregation characteristics. 2) Compared with
the commonly used models for calculating VaR and ES, the GAS-ALD model has a
high prediction effect.
| [{'version': 'v1', 'created': 'Tue, 4 Aug 2020 02:11:57 GMT'}
{'version': 'v2', 'created': 'Tue, 11 Aug 2020 08:36:03 GMT'}
{'version': 'v3', 'created': 'Tue, 13 Oct 2020 05:41:29 GMT'}] | 2020-10-14 | [array(['Shaopeng', 'Hong', ''], dtype=object)] |
19,850 | 2302.12201 | Lukas Hintze | Petra Berenbrink, Lukas Hintze, Hamed Hosseinpour, Dominik Kaaser,
Malin Rau | Dynamic Averaging Load Balancing on Arbitrary Graphs | null | null | null | null | cs.DC cs.DS math.PR | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper we study dynamic averaging load balancing on general graphs. We
consider infinite time and dynamic processes, where in every step new load
items are assigned to randomly chosen nodes. A matching is chosen, and the load
is averaged over the edges of that matching. We analyze the discrete case where
load items are indivisible, moreover our results also carry over to the
continuous case where load items can be split arbitrarily. For the choice of
the matchings we consider three different models, random matchings of linear
size, random matchings containing only single edges, and deterministic
sequences of matchings covering the whole graph. We bound the discrepancy,
which is defined as the difference between the maximum and the minimum load.
Our results cover a broad range of graph classes and, to the best of our
knowledge, our analysis is the first result for discrete and dynamic averaging
load balancing processes. As our main technical contribution we develop a drift
result that allows us to apply techniques based on the effective resistance in
an electrical network to the setting of dynamic load balancing.
| [{'version': 'v1', 'created': 'Thu, 23 Feb 2023 17:51:37 GMT'}] | 2023-02-24 | [array(['Berenbrink', 'Petra', ''], dtype=object)
array(['Hintze', 'Lukas', ''], dtype=object)
array(['Hosseinpour', 'Hamed', ''], dtype=object)
array(['Kaaser', 'Dominik', ''], dtype=object)
array(['Rau', 'Malin', ''], dtype=object)] |
19,851 | 1610.05586 | Mu Li | Mu Li and Wangmeng Zuo and David Zhang | Deep Identity-aware Transfer of Facial Attributes | null | null | null | null | cs.CV | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This paper presents a Deep convolutional network model for Identity-Aware
Transfer (DIAT) of facial attributes. Given the source input image and the
reference attribute, DIAT aims to generate a facial image that owns the
reference attribute as well as keeps the same or similar identity to the input
image. In general, our model consists of a mask network and an attribute
transform network which work in synergy to generate a photo-realistic facial
image with the reference attribute. Considering that the reference attribute
may be only related to some parts of the image, the mask network is introduced
to avoid the incorrect editing on attribute irrelevant region. Then the
estimated mask is adopted to combine the input and transformed image for
producing the transfer result. For joint training of transform network and mask
network, we incorporate the adversarial attribute loss, identity-aware adaptive
perceptual loss, and VGG-FACE based identity loss. Furthermore, a denoising
network is presented to serve for perceptual regularization to suppress the
artifacts in transfer result, while an attribute ratio regularization is
introduced to constrain the size of attribute relevant region. Our DIAT can
provide a unified solution for several representative facial attribute transfer
tasks, e.g., expression transfer, accessory removal, age progression, and
gender transfer, and can be extended for other face enhancement tasks such as
face hallucination. The experimental results validate the effectiveness of the
proposed method. Even for the identity-related attribute (e.g., gender), our
DIAT can obtain visually impressive results by changing the attribute while
retaining most identity-aware features.
| [{'version': 'v1', 'created': 'Tue, 18 Oct 2016 12:56:47 GMT'}
{'version': 'v2', 'created': 'Thu, 6 Dec 2018 13:36:08 GMT'}] | 2018-12-07 | [array(['Li', 'Mu', ''], dtype=object)
array(['Zuo', 'Wangmeng', ''], dtype=object)
array(['Zhang', 'David', ''], dtype=object)] |
19,852 | 1801.06088 | Wei Cheng | Kai Zhao, Wei Cheng | On the vanishing contact structure for viscosity solutions of contact
type Hamilton-Jacobi equations I: Cauchy problem | null | null | null | null | math.AP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the representation formulae for the fundamental solutions and
viscosity solutions of the Hamilton-Jacobi equations of contact type. We also
obtain a vanishing contact structure result for relevant Cauchy problems which
can be regarded as an extension to the vanishing discount problem.
| [{'version': 'v1', 'created': 'Thu, 18 Jan 2018 15:07:59 GMT'}
{'version': 'v2', 'created': 'Fri, 19 Jan 2018 14:55:03 GMT'}
{'version': 'v3', 'created': 'Thu, 1 Feb 2018 17:48:58 GMT'}
{'version': 'v4', 'created': 'Fri, 13 Apr 2018 20:42:04 GMT'}] | 2018-04-17 | [array(['Zhao', 'Kai', ''], dtype=object)
array(['Cheng', 'Wei', ''], dtype=object)] |
19,853 | 2006.12985 | Wilfredo Urbina-Romero | Eduard Navas, Ebner Pineda and Wilfredo Urbina | The Boundedness of General Alternative Gaussian Singular Integrals on
variable Lebesgue spaces with Gaussian measure | arXiv admin note: text overlap with arXiv:1911.06375 | null | null | null | math.CA | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In a previous paper, we introduced a new class of Gaussian singular
integrals, that we called the general alternative Gaussian singular integrals
and study the boundedness of them on $L^p(\gamma_d)$, $ 1 < p < \infty.$ In
this paper, we study the boundedness of those operators on Gaussian variable
Lebesgue spaces under a certain additional condition of regularity on
$p(\cdot)$ following a paper by E. Dalmasso and R. Scotto.
| [{'version': 'v1', 'created': 'Sat, 20 Jun 2020 06:23:36 GMT'}
{'version': 'v2', 'created': 'Mon, 5 Oct 2020 18:23:24 GMT'}
{'version': 'v3', 'created': 'Mon, 22 Mar 2021 15:46:57 GMT'}] | 2021-03-23 | [array(['Navas', 'Eduard', ''], dtype=object)
array(['Pineda', 'Ebner', ''], dtype=object)
array(['Urbina', 'Wilfredo', ''], dtype=object)] |
19,854 | 2204.09512 | Xiaoquan Xu | Xiaoquan Xu | On $\mathbf{K}$-reflections of Scott spaces | 16 pages, 24 references. arXiv admin note: text overlap with
arXiv:1911.11618 | null | null | null | math.GM | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper, for a full subcategory $\mathbf{K}$ of the category of all
$T_0$ spaces with continuous mappings, we investigate the questions under what
conditions the $\mathbf{K}$-reflection of a Scott space is still a Scott space
and under what conditions the Scott $\mathbf{K}$-completion of a poset exists.
Some necessary and sufficient conditions for the $\mathbf{K}$-reflection of a
Scott space to be a Scott space and for the existence of Scott
$\mathbf{K}$-completion of a poset are established, respectively. It is shown
that neither the sobrification nor the well-filtered reflection of the
Johnstone space is a Scott space. The $\mathbf{K}$-reflections of Alexandroff
spaces and the $\mathbf{K}$-completions of posets are also discussed.
| [{'version': 'v1', 'created': 'Wed, 20 Apr 2022 16:39:27 GMT'}] | 2022-04-21 | [array(['Xu', 'Xiaoquan', ''], dtype=object)] |
19,855 | 1602.06473 | William Banks | William D. Banks and Igor E. Shparlinski | On the number of distinct quadratic fields generated by the Shanks
sequence | 17 pages | null | null | null | math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Let $g>1$ be an integer and $f(X)\in{\mathbb Z}[X]$ a polynomial of positive
degree with no multiple roots, and put $u(n)=f(g^n)$. In this note, we study
the sequence of quadratic fields ${\mathbb Q}(\sqrt{u(n)}\,)$ as $n$ varies
over the consecutive integers $M+1,\ldots,M+N$. Fields of this type include
Shanks fields and their generalizations. Using the square sieve together with
new bounds on character sums, we improve an upper bound of Luca and Shparlinski
(2009) on the number of $n \in \{M+1,\ldots,M+N\}$ with ${\mathbb
Q}(\sqrt{u(n)}\,) = {\mathbb Q}(\sqrt{s}\,)$ for a given squarefree integer
$s$.
| [{'version': 'v1', 'created': 'Sat, 20 Feb 2016 22:58:21 GMT'}] | 2016-02-23 | [array(['Banks', 'William D.', ''], dtype=object)
array(['Shparlinski', 'Igor E.', ''], dtype=object)] |
19,856 | 2209.12158 | Chenglong Li | Chenglong Li, Emmeric Tanghe, Sofie Pollin, Wout Joseph | Ubiquitous Indoor Positioning and Tracking for Industrial
Internet-of-Things: A Channel Response Perspective | null | null | null | null | eess.SP | http://creativecommons.org/licenses/by-nc-nd/4.0/ | The future of industrial location-aided applications is shaped by the
ubiquity of Internet-of-Things (IoT) devices. As an increasing amount of
commercial off-the-shelf radio devices support channel response collection, it
is possible to achieve fine-grained position estimation at a relatively low
cost. In this article, we focus on channel response-based positioning and
tracking for industrial IoT applications. We first give an overview of the
state of the art (SOTA) of channel response-enabled localization, which is
further classified into two categories, \textit{i.e.}, device-based and
contact-free schemes. Then we propose a taxonomy for these complementary
approaches concerning the involved techniques. Finally, we discuss the
practical issues of the SOTA methods for real-world applications and point out
future research opportunities for channel response-based positioning and
tracking.
| [{'version': 'v1', 'created': 'Sun, 25 Sep 2022 06:07:02 GMT'}] | 2022-09-27 | [array(['Li', 'Chenglong', ''], dtype=object)
array(['Tanghe', 'Emmeric', ''], dtype=object)
array(['Pollin', 'Sofie', ''], dtype=object)
array(['Joseph', 'Wout', ''], dtype=object)] |
19,857 | 0912.1513 | Patricia L. Alireza | Patricia L. Alireza, Fumihiko Nakamura, Swee K. Goh, Yoshiteru Maeno,
Satoru Nakatsuji, Y. T. Chris Ko, Michael Sutherland, Stephen Julian and
Gilbert G. Lonzarich | Evidence of superconductivity on the border of quasi-2D ferromagnetism
in Ca2RuO4 at high pressure | 6 pages | null | null | null | cond-mat.supr-con cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The layered perovskite Ca2RuO4 is a spin-one Mott insulator at ambient
pressure and exhibits metallic ferromagnetism at least up to ~ 80 kbar with a
maximum Curie temperature of 28 K. Above ~ 90 kbar and up to 140 kbar, the
highest pressure reached, the resistivity and ac susceptibility show pronounced
downturns below ~ 0.4 K in applied magnetic fields of up to ~10 mT. This
indicates that our specimens of Ca2RuO4 are weakly superconducting on the
border of a quasi-2D ferromagnetic state.
| [{'version': 'v1', 'created': 'Tue, 8 Dec 2009 14:59:50 GMT'}] | 2009-12-09 | [array(['Alireza', 'Patricia L.', ''], dtype=object)
array(['Nakamura', 'Fumihiko', ''], dtype=object)
array(['Goh', 'Swee K.', ''], dtype=object)
array(['Maeno', 'Yoshiteru', ''], dtype=object)
array(['Nakatsuji', 'Satoru', ''], dtype=object)
array(['Ko', 'Y. T. Chris', ''], dtype=object)
array(['Sutherland', 'Michael', ''], dtype=object)
array(['Julian', 'Stephen', ''], dtype=object)
array(['Lonzarich', 'Gilbert G.', ''], dtype=object)] |
19,858 | 2106.14512 | Jacques Fattaccioli | Olivier Mesdjian, Nicolas Ruyssen, Marie-Caroline Jullien, Rachele
Allena, Jacques Fattaccioli | Enhancing the capture efficiency and homogeneity of single-layer
flow-through trapping microfluidic devices using oblique hydrodynamic streams | Post-reviewing revised version | null | null | null | physics.flu-dyn | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | With the aim to parallelize and monitor biological or biochemical phenomena,
trapping and immobilization of objects such as particles, droplets or cells in
microfluidic devices has been an intense area of research and engineering so
far. Either being passive or active, these microfluidic devices are usually
composed of arrays of elementary traps with various levels of sophistication.
For a given array, it is important to have an efficient and fast immobilization
of the highest number of objects, while optimizing the spatial homogeneity of
the trapping over the whole chip. For passive devices, this has been achieved
with two-layers structures, making the fabrication process more complex. In
this work, we designed small microfluidic traps by single-layer direct laser
writing into a photoresist, and we show that even in this simplest case, the
orientation of the main flow of particles with respect to the traps have a
drastic effect on the trapping efficiency and homogeneity. To better understand
this phenomenon, we have considered two different flow geometries: parallel and
oblique with respect to the traps array, and compared quantitatively the
immobilization of particles with various sizes and densities. Using image
analysis, we show that diagonal flows gives a spatial distribution of the trap
loading that is more homogeneous over the whole chip as compared to the
straight ones, and by performing FEM and trapping simulation, we propose a
qualitative explanation of this phenomenon.
| [{'version': 'v1', 'created': 'Mon, 28 Jun 2021 09:58:24 GMT'}
{'version': 'v2', 'created': 'Thu, 16 Sep 2021 14:41:19 GMT'}] | 2021-09-17 | [array(['Mesdjian', 'Olivier', ''], dtype=object)
array(['Ruyssen', 'Nicolas', ''], dtype=object)
array(['Jullien', 'Marie-Caroline', ''], dtype=object)
array(['Allena', 'Rachele', ''], dtype=object)
array(['Fattaccioli', 'Jacques', ''], dtype=object)] |
19,859 | hep-th/0605237 | Dafni Marchioro | A. L. Gadelha, Dafni Z. Marchioro, Daniel L. Nedel | Entanglement and entropy operator for strings in pp-wave time dependent
background | revtex4, 15 pages, revised version to appear in Physics Letters B | Phys.Lett. B639 (2006) 383-388 | 10.1016/j.physletb.2006.06.044 | null | hep-th | null | In this letter new aspects of string theory propagating in a pp-wave time
dependent background with a null singularity are explored. It is shown the
appearance of a 2d entanglement entropy dynamically generated by the
background. For asymptotically flat observers, the vacuum close to the
singularity is unitarily inequivalent to the vacuum at $\tau = -\infty$ and it
is shown that the 2d entanglement entropy diverges close to this point. As a
consequence, the positive time region is inaccessible for observers in $\tau
=-\infty$. For a stationary measure, the vacuum at finite time is seen by those
observers as a thermal state and the information loss is encoded as a heat bath
of string states.
| [{'version': 'v1', 'created': 'Tue, 23 May 2006 19:11:13 GMT'}
{'version': 'v2', 'created': 'Wed, 21 Jun 2006 18:10:35 GMT'}] | 2009-11-11 | [array(['Gadelha', 'A. L.', ''], dtype=object)
array(['Marchioro', 'Dafni Z.', ''], dtype=object)
array(['Nedel', 'Daniel L.', ''], dtype=object)] |
19,860 | math/0702589 | Peter Constantin | Peter Constantin and Nader Masmoudi | Global well-posedness for a Smoluchowski equation coupled with
Navier-Stokes equations in 2D | null | null | 10.1007/s00220-007-0384-2 | null | math.AP | null | We prove global existence for a nonlinear Smoluchowski equation (a nonlinear
Fokker-Planck equation) coupled with Navier-Stokes equations in two dimensions.
The proof uses a deteriorating regularity estimate and the tensorial structure
of the main nonlinear terms.
| [{'version': 'v1', 'created': 'Tue, 20 Feb 2007 19:35:30 GMT'}] | 2009-11-13 | [array(['Constantin', 'Peter', ''], dtype=object)
array(['Masmoudi', 'Nader', ''], dtype=object)] |
19,861 | 1704.02443 | Mugurel Tolea C | F. Tolea, M. Tolea, M. Valeanu | Thermal memory fading by heating to a lower temperature: experimental
data on polycrystalline NiFeGa ribbons and 2D statistical model predictions | 6 pages, 4 figures | Solid State Communications 257 (2017), 36 | 10.1016/j.ssc.2017.04.003 | null | cond-mat.mtrl-sci | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Shape memory alloys are known to memorise one -or several- temperatures at
which the martensite-austenite transformation was stopped before completion in
the past, the memory manifesting as specific dips in subsequent calorimetric
scans. Previous studies have shown that this memory can be erased by heating to
higher temperatures than the ones previously recorded. In this paper, we study
a distinct memory fading effect which takes place by heating to a lower
temperature. This effect is reported in NiFeGa as polycrystalline ribbons, the
alloy being initially studied as bulk for which the thermal memory effect was
not found. If, after an initial incomplete heating up to T1 one performs a
second incomplete heating up to T2<T1, a new calorimetric dip appears at T2, as
expected, while less expected was that the dip corresponding to T1 reduces in
amplitude or even vanishes (if the arrest at T2 is repeated). The memory fading
effect is more clear for small differences T1-T2 and less obvious or absent for
large ones. The second part of the paper employs a statistical 2D model, which
associates the memorized temperatures with a depletion of certain martensite
plates sizes, and also supports the memory fading effect.
| [{'version': 'v1', 'created': 'Sat, 8 Apr 2017 05:48:37 GMT'}] | 2017-04-11 | [array(['Tolea', 'F.', ''], dtype=object)
array(['Tolea', 'M.', ''], dtype=object)
array(['Valeanu', 'M.', ''], dtype=object)] |
19,862 | 1603.01525 | Malin Klintefjord | M. Klintefjord and K. Hady\'nska-Kl\c{e}k and A. G\"orgen and C. Bauer
and F.L. Bello Garrote and S. B\"onig and B. Bounthong and A. Damyanova and
J.-P. Delaroche and V. Fedosseev and D.A. Fink and F. Giacoppo and M. Girod
and P. Hoff and N. Imai and W. Korten and A.C. Larsen and J. Libert and R.
Lutter and B.A. Marsh and P.L. Molkanov and H. Na\"idja and P. Napiorkowski
and F. Nowacki and J. Pakarinen and E. Rapisarda and P. Reiter and T.
Renstr{\o}m and S. Rothe and M.D. Seliverstov and B. Siebeck and S. Siem and
J. Srebrny and T. Stora and P. Th\"ole and T.G. Tornyi and G.M. Tveten and P.
Van Duppen and M.J Vermeulen and D. Voulot and N. Warr and F. Wenander and H.
De Witte and M. Zieli\'nska | The structure of low-lying states in ${}^{140}$Sm studied by Coulomb
excitation | 15 pages, 12 figures | Phys. Rev. C 93, 054303 (2016) | 10.1103/PhysRevC.93.054303 | null | nucl-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The electromagnetic structure of $^{140}$Sm was studied in a low-energy
Coulomb excitation experiment with a radioactive ion beam from the REX-ISOLDE
facility at CERN. The $2^+$ and $4^+$ states of the ground-state band and a
second $2^+$ state were populated by multi-step excitation. The analysis of the
differential Coulomb excitation cross sections yielded reduced transition
probabilities between all observed states and the spectroscopic quadrupole
moment for the $2_1^+$ state. The experimental results are compared to
large-scale shell model calculations and beyond-mean-field calculations based
on the Gogny D1S interaction with a five-dimensional collective Hamiltonian
formalism. Simpler geometric and algebraic models are also employed to
interpret the experimental data. The results indicate that $^{140}$Sm shows
considerable $\gamma$ softness, but in contrast to earlier speculation no signs
of shape coexistence at low excitation energy. This work sheds more light on
the onset of deformation and collectivity in this mass region.
| [{'version': 'v1', 'created': 'Fri, 4 Mar 2016 16:34:10 GMT'}] | 2016-05-09 | [array(['Klintefjord', 'M.', ''], dtype=object)
array(['Hadyńska-Klȩk', 'K.', ''], dtype=object)
array(['Görgen', 'A.', ''], dtype=object)
array(['Bauer', 'C.', ''], dtype=object)
array(['Garrote', 'F. L. Bello', ''], dtype=object)
array(['Bönig', 'S.', ''], dtype=object)
array(['Bounthong', 'B.', ''], dtype=object)
array(['Damyanova', 'A.', ''], dtype=object)
array(['Delaroche', 'J. -P.', ''], dtype=object)
array(['Fedosseev', 'V.', ''], dtype=object)
array(['Fink', 'D. A.', ''], dtype=object)
array(['Giacoppo', 'F.', ''], dtype=object)
array(['Girod', 'M.', ''], dtype=object)
array(['Hoff', 'P.', ''], dtype=object)
array(['Imai', 'N.', ''], dtype=object)
array(['Korten', 'W.', ''], dtype=object)
array(['Larsen', 'A. C.', ''], dtype=object)
array(['Libert', 'J.', ''], dtype=object)
array(['Lutter', 'R.', ''], dtype=object)
array(['Marsh', 'B. A.', ''], dtype=object)
array(['Molkanov', 'P. L.', ''], dtype=object)
array(['Naïdja', 'H.', ''], dtype=object)
array(['Napiorkowski', 'P.', ''], dtype=object)
array(['Nowacki', 'F.', ''], dtype=object)
array(['Pakarinen', 'J.', ''], dtype=object)
array(['Rapisarda', 'E.', ''], dtype=object)
array(['Reiter', 'P.', ''], dtype=object)
array(['Renstrøm', 'T.', ''], dtype=object)
array(['Rothe', 'S.', ''], dtype=object)
array(['Seliverstov', 'M. D.', ''], dtype=object)
array(['Siebeck', 'B.', ''], dtype=object)
array(['Siem', 'S.', ''], dtype=object)
array(['Srebrny', 'J.', ''], dtype=object)
array(['Stora', 'T.', ''], dtype=object)
array(['Thöle', 'P.', ''], dtype=object)
array(['Tornyi', 'T. G.', ''], dtype=object)
array(['Tveten', 'G. M.', ''], dtype=object)
array(['Van Duppen', 'P.', ''], dtype=object)
array(['Vermeulen', 'M. J', ''], dtype=object)
array(['Voulot', 'D.', ''], dtype=object)
array(['Warr', 'N.', ''], dtype=object)
array(['Wenander', 'F.', ''], dtype=object)
array(['De Witte', 'H.', ''], dtype=object)
array(['Zielińska', 'M.', ''], dtype=object)] |
19,863 | 1204.1823 | Masatoshi Suzuki | Masatoshi Suzuki | On monotonicity of certain weighted summatory functions associated with
L-functions | 13 pages | Comment. Math. Univ. St. Pauli 60 (2011), no. 1 & no. 2, 211-225 | null | null | math.NT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We state some sufficient or equivalent conditions to GRH of general
L-functions in terms of monotonicity of certain weighted summatory functions.
| [{'version': 'v1', 'created': 'Mon, 9 Apr 2012 08:21:27 GMT'}] | 2012-04-10 | [array(['Suzuki', 'Masatoshi', ''], dtype=object)] |
19,864 | 0808.2016 | Thomas Schwetz | Thomas Schwetz, Mariam Tortola, Jose W.F. Valle | Three-flavour neutrino oscillation update | 17 pages, 7 figures. An appendix is added providing three-neutrino
parameter determinations as of February 2010. We include all oscillation
data, such as the first MINOS electron neutrino appearance data, the low
energy threshold analysis given by the SNO Collaboration, as well as recently
updated Standard Solar Models | New J.Phys.10:113011,2008 | 10.1088/1367-2630/10/11/113011 | CERN-PH-TH/2008-177 | hep-ph astro-ph hep-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We review the present status of three-flavour neutrino oscillations, taking
into account the latest available neutrino oscillation data presented at the
Neutrino 2008 Conference. This includes the data released this summer by the
MINOS collaboration, the data of the neutral current counter phase of the SNO
solar neutrino experiment, as well as the latest KamLAND and Borexino data. We
give the updated determinations of the leading 'solar' and 'atmospheric'
oscillation parameters. We find from global data that the mixing angle
$\theta_{13}$ is consistent with zero within $0.9\sigma$ and we derive an upper
bound of $\sin^2\theta_{13} < 0.035 (0.056)$ at 90% CL (3$\sigma$).
| [{'version': 'v1', 'created': 'Thu, 14 Aug 2008 15:55:31 GMT'}
{'version': 'v2', 'created': 'Mon, 1 Dec 2008 10:21:49 GMT'}
{'version': 'v3', 'created': 'Thu, 11 Feb 2010 18:48:12 GMT'}] | 2010-02-11 | [array(['Schwetz', 'Thomas', ''], dtype=object)
array(['Tortola', 'Mariam', ''], dtype=object)
array(['Valle', 'Jose W. F.', ''], dtype=object)] |
19,865 | 2205.13481 | Vincent Jeanselme | Vincent Jeanselme, Glen Martin, Niels Peek, Matthew Sperrin, Brian Tom
and Jessica Barrett | DeepJoint: Robust Survival Modelling Under Clinical Presence Shift | null | null | null | null | cs.LG | http://creativecommons.org/licenses/by/4.0/ | Observational data in medicine arise as a result of the complex interaction
between patients and the healthcare system. The sampling process is often
highly irregular and itself constitutes an informative process. When using such
data to develop prediction models, this phenomenon is often ignored, leading to
sub-optimal performance and generalisability of models when practices evolve.
We propose a multi-task recurrent neural network which models three clinical
presence dimensions -- namely the longitudinal, the inter-observation and the
missingness processes -- in parallel to the survival outcome. On a prediction
task using MIMIC III laboratory tests, explicit modelling of these three
processes showed improved performance in comparison to state-of-the-art
predictive models (C-index at 1 day horizon: 0.878). More importantly, the
proposed approach was more robust to change in the clinical presence setting,
demonstrated by performance comparison between patients admitted on weekdays
and weekends. This analysis demonstrates the importance of studying and
leveraging clinical presence to improve performance and create more
transportable clinical models.
| [{'version': 'v1', 'created': 'Thu, 26 May 2022 16:42:38 GMT'}] | 2022-05-27 | [array(['Jeanselme', 'Vincent', ''], dtype=object)
array(['Martin', 'Glen', ''], dtype=object)
array(['Peek', 'Niels', ''], dtype=object)
array(['Sperrin', 'Matthew', ''], dtype=object)
array(['Tom', 'Brian', ''], dtype=object)
array(['Barrett', 'Jessica', ''], dtype=object)] |
19,866 | 1405.2540 | Dmitry Gourevitch | Avraham Aizenbud, Dmitry Gourevitch, Eitan Sayag, and Alexander
Kemarsky | z-Finite distributions on p-adic groups | 27 pages. v2:version to appear in Advances in Mathematics | Advances in Mathematics 285 (2015) 1376-1414 | 10.1016/j.aim.2015.07.033 | null | math.RT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | For a real reductive group G, the center
$\mathfrak{z}(\mathcal{U}(\mathfrak{g}))$ of the universal enveloping algebra
of the Lie algebra $\mathfrak{g}$ of G acts on the space of distributions on G.
This action proved to be very useful (see e.g. [HC63, HC65, Sha74, Bar03]).
Over non-Archimedean local fields, one can replace this action by the action
of the Bernstein center z of G, i.e. the center of the category of smooth
representations. However, this action is not well studied. In this paper we
provide some tools to work with this action and prove the following results.
1) The wave-front set of any z-finite distribution on G over any point $g\in
G$ lies inside the nilpotent cone of $T_g^*G \cong \mathfrak{g}$.
2) Let $H_1,H_2 \subset G$ be symmetric subgroups. Consider the space J of
$H_1\times H_2$-invariant distributions on G. We prove that the z-finite
distributions in J form a dense subspace. In fact we prove this result in wider
generality, where the groups $H_i$ are spherical groups of certain type and the
invariance condition is replaced by equivariance. Further we apply those
results to density and regularity of spherical characters.
The first result can be viewed as a version of Howe's expansion of
characters. The second result can be viewed as a spherical space analog of a
classical theorem on density of characters of admissible representations. It
can also be viewed as a spectral version of Bernstein's localization principle.
In the Archimedean case, the first result is well-known and the second
remains open.
| [{'version': 'v1', 'created': 'Sun, 11 May 2014 15:41:51 GMT'}
{'version': 'v2', 'created': 'Fri, 4 Sep 2015 07:55:28 GMT'}] | 2016-05-06 | [array(['Aizenbud', 'Avraham', ''], dtype=object)
array(['Gourevitch', 'Dmitry', ''], dtype=object)
array(['Sayag', 'Eitan', ''], dtype=object)
array(['Kemarsky', 'Alexander', ''], dtype=object)] |
19,867 | math/0603132 | Hans-Georg M\"{u}ller | Fang Yao, Hans-Georg M\"uller, Jane-Ling Wang | Functional linear regression analysis for longitudinal data | Published at http://dx.doi.org/10.1214/009053605000000660 in the
Annals of Statistics (http://www.imstat.org/aos/) by the Institute of
Mathematical Statistics (http://www.imstat.org) | Annals of Statistics 2005, Vol. 33, No. 6, 2873-2903 | 10.1214/009053605000000660 | IMS-AOS-AOS0040 | math.ST stat.TH | null | We propose nonparametric methods for functional linear regression which are
designed for sparse longitudinal data, where both the predictor and response
are functions of a covariate such as time. Predictor and response processes
have smooth random trajectories, and the data consist of a small number of
noisy repeated measurements made at irregular times for a sample of subjects.
In longitudinal studies, the number of repeated measurements per subject is
often small and may be modeled as a discrete random number and, accordingly,
only a finite and asymptotically nonincreasing number of measurements are
available for each subject or experimental unit. We propose a functional
regression approach for this situation, using functional principal component
analysis, where we estimate the functional principal component scores through
conditional expectations. This allows the prediction of an unobserved response
trajectory from sparse measurements of a predictor trajectory. The resulting
technique is flexible and allows for different patterns regarding the timing of
the measurements obtained for predictor and response trajectories. Asymptotic
properties for a sample of $n$ subjects are investigated under mild conditions,
as $n\to \infty$, and we obtain consistent estimation for the regression
function. Besides convergence results for the components of functional linear
regression, such as the regression parameter function, we construct asymptotic
pointwise confidence bands for the predicted trajectories. A functional
coefficient of determination as a measure of the variance explained by the
functional regression model is introduced, extending the standard $R^2$ to the
functional case. The proposed methods are illustrated with a simulation study,
longitudinal primary biliary liver cirrhosis data and an analysis of the
longitudinal relationship between blood pressure and body mass index.
| [{'version': 'v1', 'created': 'Mon, 6 Mar 2006 08:09:42 GMT'}] | 2016-08-16 | [array(['Yao', 'Fang', ''], dtype=object)
array(['Müller', 'Hans-Georg', ''], dtype=object)
array(['Wang', 'Jane-Ling', ''], dtype=object)] |
19,868 | 1711.10992 | Aurya Javeed | Aurya Javeed | An Uncertainty Principle for Estimates of Floquet Multipliers | null | null | null | null | math.DS stat.AP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We derive a Cram\'er-Rao lower bound for the variance of Floquet multiplier
estimates that have been constructed from stable limit cycles perturbed by
noise. To do so, we consider perturbed periodic orbits in the plane. We use a
periodic autoregressive process to model the intersections of these orbits with
cross sections, then passing to the limit of a continuum of sections to obtain
a bound that depends on the continuous flow restricted to the (nontrivial)
Floquet mode. We compare our bound against the empirical variance of estimates
constructed using several cross sections. The section-based estimates are close
to being optimal. We posit that the utility of our bound persists in higher
dimensions when computed along Floquet modes for real and distinct multipliers.
Our bound elucidates some of the empirical observations noted in the
literature; e.g., (a) it is the number of cycles (as opposed to the frequency
of observations) that drives the variance of estimates to zero, and (b) the
estimator variance has a positive lower bound as the noise amplitude tends to
zero.
| [{'version': 'v1', 'created': 'Wed, 29 Nov 2017 18:16:10 GMT'}] | 2017-11-30 | [array(['Javeed', 'Aurya', ''], dtype=object)] |
19,869 | 1111.4510 | Carl Sabottke | Carl F. Sabottke, Chris D. Richardson, Petr M. Anisimov, Ulvi
Yurtsever, Antia Lamas-Linares, Jonathan P. Dowling | Thwarting the Photon Number Splitting Attack with Entanglement Enhanced
BB84 Quantum Key Distribution | 10 pages, 4 figures | New J. Phys. 14, 043003 (2012) | 10.1088/1367-2630/14/4/043003 | null | quant-ph physics.optics | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We develop an improvement to the weak laser pulse BB84 scheme for quantum key
distribution, which utilizes entanglement to improve the security of the scheme
and enhance its resilience to the photon-number-splitting attack. This protocol
relies on the non-commutation of photon phase and number to detect an
eavesdropper performing quantum non-demolition measurement on number. The
potential advantages and disadvantages of this scheme are compared to the
coherent decoy state protocol.
| [{'version': 'v1', 'created': 'Fri, 18 Nov 2011 22:46:21 GMT'}
{'version': 'v2', 'created': 'Wed, 1 Feb 2012 22:57:41 GMT'}] | 2015-03-19 | [array(['Sabottke', 'Carl F.', ''], dtype=object)
array(['Richardson', 'Chris D.', ''], dtype=object)
array(['Anisimov', 'Petr M.', ''], dtype=object)
array(['Yurtsever', 'Ulvi', ''], dtype=object)
array(['Lamas-Linares', 'Antia', ''], dtype=object)
array(['Dowling', 'Jonathan P.', ''], dtype=object)] |
19,870 | 0803.1418 | S{\o}ren Gammelmark | Soren Gammelmark, Klaus Molmer | Quantum learning by measurement and feedback | 6 pages, 5 figures | 2009 New J. Phys. 11 033017 | 10.1088/1367-2630/11/3/033017 | null | quant-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We propose an approach to quantum computing in which quantum gate strengths
are parametrized by quantum degrees of freedom, and the capability of the
quantum computer to perform desired tasks is monitored and gradually improved
by successive feedback modifications of the coupling strength parameters. Our
proposal aims at experimental implementation, scalable to computational
problems too large to be simulated theoretically, and we demonstrate
feasibility of our proposal with simulations on search and factoring
algorithms.
| [{'version': 'v1', 'created': 'Mon, 10 Mar 2008 14:01:38 GMT'}
{'version': 'v2', 'created': 'Wed, 25 Jun 2008 13:02:41 GMT'}
{'version': 'v3', 'created': 'Thu, 12 Feb 2009 13:32:56 GMT'}] | 2009-11-25 | [array(['Gammelmark', 'Soren', ''], dtype=object)
array(['Molmer', 'Klaus', ''], dtype=object)] |
19,871 | 2004.13832 | Luca Mariot | Luca Manzoni, Domagoj Jakobovic, Luca Mariot, Stjepan Picek, Mauro
Castelli | Towards an evolutionary-based approach for natural language processing | 18 pages, 7 figures, 2 tables. Accepted for publication at the
Genetic and Evolutionary Computation Conference (GECCO 2020) | null | null | null | cs.CL cs.AI cs.NE | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Tasks related to Natural Language Processing (NLP) have recently been the
focus of a large research endeavor by the machine learning community. The
increased interest in this area is mainly due to the success of deep learning
methods. Genetic Programming (GP), however, was not under the spotlight with
respect to NLP tasks. Here, we propose a first proof-of-concept that combines
GP with the well established NLP tool word2vec for the next word prediction
task. The main idea is that, once words have been moved into a vector space,
traditional GP operators can successfully work on vectors, thus producing
meaningful words as the output. To assess the suitability of this approach, we
perform an experimental evaluation on a set of existing newspaper headlines.
Individuals resulting from this (pre-)training phase can be employed as the
initial population in other NLP tasks, like sentence generation, which will be
the focus of future investigations, possibly employing adversarial
co-evolutionary approaches.
| [{'version': 'v1', 'created': 'Thu, 23 Apr 2020 18:44:12 GMT'}] | 2020-04-30 | [array(['Manzoni', 'Luca', ''], dtype=object)
array(['Jakobovic', 'Domagoj', ''], dtype=object)
array(['Mariot', 'Luca', ''], dtype=object)
array(['Picek', 'Stjepan', ''], dtype=object)
array(['Castelli', 'Mauro', ''], dtype=object)] |
19,872 | 1401.7340 | Marco Zaro | R. Frederix, S. Frixione, V. Hirschi, F. Maltoni, O. Mattelaer, P.
Torrielli, E. Vryonidou, M. Zaro | Higgs pair production at the LHC with NLO and parton-shower effects | 11 pages, 7 figures, version accepted for publication on PLB | Phys.Lett. B732 (2014) 142-149 | 10.1016/j.physletb.2014.03.026 | CERN-PH-TH/2014-014, CP3-14-07, ZU-TH03/14, LPN14-055 | hep-ph | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We present predictions for the SM-Higgs-pair production channels of relevance
at the LHC: gluon-gluon fusion, VBF, and top-pair, W, Z and single-top
associated production. All these results are at the NLO accuracy in QCD, and
matched to parton showers by means of the MC@NLO method; hence, they are fully
differential. With the exception of the gluon-gluon fusion process, for which a
special treatment is needed in order to improve upon the infinite-top-mass
limit, our predictions are obtained in a fully automatic way within the
publicly available MadGraph5_aMC@NLO framework. We show that for all channels
in general, and for gluon-gluon fusion and top-pair associated production in
particular, NLO corrections reduce the theoretical uncertainties, and are
needed in order to arrive at reliable predictions for total rates as well as
for distributions.
| [{'version': 'v1', 'created': 'Tue, 28 Jan 2014 21:05:23 GMT'}
{'version': 'v2', 'created': 'Thu, 20 Mar 2014 16:48:43 GMT'}] | 2014-05-16 | [array(['Frederix', 'R.', ''], dtype=object)
array(['Frixione', 'S.', ''], dtype=object)
array(['Hirschi', 'V.', ''], dtype=object)
array(['Maltoni', 'F.', ''], dtype=object)
array(['Mattelaer', 'O.', ''], dtype=object)
array(['Torrielli', 'P.', ''], dtype=object)
array(['Vryonidou', 'E.', ''], dtype=object)
array(['Zaro', 'M.', ''], dtype=object)] |
19,873 | 1704.04768 | He Jiang | Jifeng Xuan, He Jiang, Zhilei Ren, Zhongxuan Luo | Solving the Large Scale Next Release Problem with a Backbone Based
Multilevel Algorithm | 18 pages, 7 figures | null | null | null | cs.SE | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The Next Release Problem (NRP) aims to optimize customer profits and
requirements selection for the software releases. The research on the NRP is
restricted by the growing scale of requirements. In this paper, we propose a
Backbone based Multilevel Algorithm (BMA) to address the large scale NRP. In
contrast to direct solving approaches, BMA employs multilevel reductions to
downgrade the problem scale and multilevel refinements to construct the final
optimal set of customers. In both reductions and refinements, the backbone is
built to fix the common part of the optimal customers. Since it is intractable
to extract the backbone in practice, the approximate backbone is employed for
the instance reduction while the soft backbone is proposed to augment the
backbone application. In the experiments, to cope with the lack of open large
requirements databases, we propose a method to extract instances from open bug
repositories. Experimental results on 15 classic instances and 24 realistic
instances demonstrate that BMA can achieve better solutions on the large scale
NRP instances than direct solving approaches. Our work provides a reduction
approach for solving large scale problems in search based requirements
engineering.
| [{'version': 'v1', 'created': 'Sun, 16 Apr 2017 12:53:33 GMT'}] | 2017-04-18 | [array(['Xuan', 'Jifeng', ''], dtype=object)
array(['Jiang', 'He', ''], dtype=object)
array(['Ren', 'Zhilei', ''], dtype=object)
array(['Luo', 'Zhongxuan', ''], dtype=object)] |
19,874 | 1510.02810 | Alberto Escalante | Alberto Escalante (Puebla U., Mexico), Omar Rodr\'iguez-Tzompantzi
(Puebla U., Mexico) | Dirac's and Generalized Faddeev-Jackiw brackets for Einstein's theory in
G $\rightarrow 0$ limit | null | null | 10.1016/j.aop.2015.10.021 | null | gr-qc hep-th | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this paper the Dirac and Faddeev-Jackiw formulation for Einstein's theory
in the $G \rightarrow 0$ limit is performed; the fundamental Dirac's and
Faddeev-Jackiw brackets for the theory are obtained. First, the Dirac brackets
are constructed by eliminating the second class constraints remaining the first
class ones, then we fix the gauge and we convert the first class constraints
into second class constraints and the new fundamental Dirac's brackets are
computed. Alternatively, we reproduce all relevant Dirac's results by means of
the symplectic method. We identify the Faddeev-Jackiw constraints and we prove
that the Dirac and the Faddeev-Jackiw brackets coincide to each other. .
| [{'version': 'v1', 'created': 'Tue, 4 Aug 2015 05:58:00 GMT'}
{'version': 'v2', 'created': 'Tue, 13 Oct 2015 15:43:06 GMT'}
{'version': 'v3', 'created': 'Tue, 27 Oct 2015 02:48:35 GMT'}] | 2016-01-20 | [array(['Escalante', 'Alberto', '', 'Puebla U., Mexico'], dtype=object)
array(['Rodríguez-Tzompantzi', 'Omar', '', 'Puebla U., Mexico'],
dtype=object) ] |
19,875 | 1404.2111 | Giorgio Audrito | Giorgio Audrito and Matteo Viale | Absoluteness via Resurrection | 34 pages | null | null | null | math.LO | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The resurrection axioms are forcing axioms introduced recently by Hamkins and
Johnstone, developing on ideas of Chalons and Velickovi\'c. We introduce a
stronger form of resurrection axioms (the \emph{iterated} resurrection axioms
$\textrm{RA}_\alpha(\Gamma)$ for a class of forcings $\Gamma$ and a given
ordinal $\alpha$), and show that $\textrm{RA}_\omega(\Gamma)$ implies generic
absoluteness for the first-order theory of $H_{\gamma^+}$ with respect to
forcings in $\Gamma$ preserving the axiom, where $\gamma=\gamma_\Gamma$ is a
cardinal which depends on $\Gamma$ ($\gamma_\Gamma=\omega_1$ if $\Gamma$ is any
among the classes of countably closed, proper, semiproper, stationary set
preserving forcings).
We also prove that the consistency strength of these axioms is below that of
a Mahlo cardinal for most forcing classes, and below that of a stationary limit
of supercompact cardinals for the class of stationary set preserving posets.
Moreover we outline that simultaneous generic absoluteness for $H_{\gamma_0^+}$
with respect to $\Gamma_0$ and for $H_{\gamma_1^+}$ with respect to $\Gamma_1$
with $\gamma_0=\gamma_{\Gamma_0}\neq\gamma_{\Gamma_1}=\gamma_1$ is in principle
possible, and we present several natural models of the Morse Kelley set theory
where this phenomenon occurs (even for all $H_\gamma$ simultaneously). Finally,
we compare the iterated resurrection axioms (and the generic absoluteness
results we can draw from them) with a variety of other forcing axioms, and also
with the generic absoluteness results by Woodin and the second author.
| [{'version': 'v1', 'created': 'Tue, 8 Apr 2014 12:59:10 GMT'}
{'version': 'v2', 'created': 'Tue, 1 Jul 2014 10:29:36 GMT'}
{'version': 'v3', 'created': 'Wed, 3 Jun 2015 12:41:27 GMT'}
{'version': 'v4', 'created': 'Wed, 5 Apr 2017 13:10:02 GMT'}] | 2017-04-06 | [array(['Audrito', 'Giorgio', ''], dtype=object)
array(['Viale', 'Matteo', ''], dtype=object)] |
19,876 | 1910.14546 | Ajay Rajan | Bharath Honnesara Sreenivasa, Ajay Rajan | Debian Package usage profiler for Debian based Systems | null | null | null | null | cs.PF cs.OS | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The embedded devices of today due to their CPU, RAM capabilities can run
various Linux distributions but in most cases they are different from general
purpose distributions as they are usually lighter and specific to the needs of
that particular system. In this project, we share the problems associated in
adopting a fully heavy-weight Debian based system like Ubuntu in
embedded/automotive platforms and provide solutions to optimize them to
identify unused/redundant content in the system. This helps developer to reduce
the hefty general purpose distribution to an application specific distribution.
The solution involves collecting usage data in the system in a non-invasive
manner (to avoid any drop in performance) to suggest users the redundant,
unused parts of the system that can be safely removed without impacting the
system functionality.
| [{'version': 'v1', 'created': 'Thu, 31 Oct 2019 15:47:35 GMT'}] | 2019-11-01 | [array(['Sreenivasa', 'Bharath Honnesara', ''], dtype=object)
array(['Rajan', 'Ajay', ''], dtype=object)] |
19,877 | astro-ph/0510471 | Ashish Mahabal | A. Mahabal (1), D. Stern (2), M. Bogosavljevic (1), S. G. Djorgovski
(1) and D. Thompson (1) ((1) Caltech, (2) JPL) | Discovery of an Optically-Faint Quasar at z=5.70 and Implications for
the Faint End of the Quasar Luminosity Function | 10 pages, 3 eps figures; Accepted for publication in ApJ Letters | Astrophys.J.634:L9-L12,2005 | 10.1086/498847 | null | astro-ph | null | We present observations of an optically-faint quasar, RD J114816.2+525339,
discovered from deep multi-color observations of the field around the z = 6.42
quasar SDSS J1148+5251. The two quasars have a projected separation of 109
arcsec and both are outliers in r-z versus z-J color-color space. Keck
spectroscopy reveals RD J114816.2+525339 to be a broad-absorption line quasar
at z = 5.70. With z_AB = 23.0, RD J114816.2+525339 is 3.3 mag fainter than SDSS
J1148+5251, making it the faintest quasar known at z>5.5. This object was
identified in a survey of ~2.5 square degrees. The implied surface density of
quasars at these redshifts and luminosities is broadly consistent with previous
extrapolations of the faint end of the quasar luminosity function and supports
the idea that active galaxies provide only a minor component of the reionizing
ultraviolet flux at these redshifts.
| [{'version': 'v1', 'created': 'Mon, 17 Oct 2005 03:36:35 GMT'}] | 2009-11-13 | [array(['Mahabal', 'A.', '', 'Caltech'], dtype=object)
array(['Stern', 'D.', '', 'JPL'], dtype=object)
array(['Bogosavljevic', 'M.', '', 'Caltech'], dtype=object)
array(['Djorgovski', 'S. G.', '', 'Caltech'], dtype=object)
array(['Thompson', 'D.', '', 'Caltech'], dtype=object)] |
19,878 | 0808.3332 | Martin Weides | A. A. Bannykh, J. Pfeiffer, V. S. Stolyarov, I. E. Batov, V. V.
Ryazanov, and M. Weides | Josephson tunnel junctions with strong ferromagnetic interlayer | 8 pages, 5 pictures v2: major conceptual changes | Phys. Rev. B 79, 054501 (2009) | 10.1103/PhysRevB.79.054501 | null | cond-mat.supr-con | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The dependence of the critical current density j_c on the ferromagnetic
interlayer thickness d_F was determined for Nb/Al_2O_3/Cu/Ni/Nb Josephson
tunnel junctions with ferromagnetic \Ni interlayer from very thin film
thicknesses (\sim 1 nm) upwards and classified into F-layer thickness regimes
showing a dead magnetic layer, exchange, exchange + anisotropy and total
suppression of j_c. The Josephson coupling changes from 0 to pi as function of
d_F, and -very close to the crossover thickness- as function of temperature.
The strong suppression of the supercurrent in comparison to non-magnetic
\Nb/Al_2O_3/Cu/Nb junctions indicated that the insertion of a F-layer leads to
additional interface scattering. The transport inside the dead magnetic layer
was in dirty limit. For the magnetically active regime fitting with both the
clean and the dirty limit theory were carried out, indicating dirty limit
condition, too. The results were discussed in the framework of literature
| [{'version': 'v1', 'created': 'Mon, 25 Aug 2008 11:07:37 GMT'}
{'version': 'v2', 'created': 'Mon, 10 Nov 2008 11:17:32 GMT'}] | 2009-02-03 | [array(['Bannykh', 'A. A.', ''], dtype=object)
array(['Pfeiffer', 'J.', ''], dtype=object)
array(['Stolyarov', 'V. S.', ''], dtype=object)
array(['Batov', 'I. E.', ''], dtype=object)
array(['Ryazanov', 'V. V.', ''], dtype=object)
array(['Weides', 'M.', ''], dtype=object)] |
19,879 | 1502.07309 | Alhun Aydin | Alhun Aydin and Altug Sisman | Dimensional transitions in thermodynamic properties of ideal
Maxwell-Boltzmann gases | 9 pages, 2 figures | Phys. Scr. 90, 045208, (2015) | 10.1088/0031-8949/90/4/045208 | null | cond-mat.stat-mech cond-mat.quant-gas | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | An ideal Maxwell-Boltzmann gas confined in various rectangular nano domains
is considered under quantum size effects. Thermodynamic quantities are
calculated from their relations with partition function which consists of
triple infinite summations over momentum states in each direction. To get
analytical expressions, summations are converted to integrals for macro systems
by continuum approximation which fails at nanoscales. To avoid both from the
numerical calculation of summations and the failure of their integral
approximations at nanoscale, a method which gives an analytical expression for
single particle partition function (SPPF) is proposed. It's shown that
dimensional transition in momentum space occurs at certain magnitude of
confinement. Therefore, to represent SPPF by lower-dimensional analytical
expressions becomes possible rather than numerical calculation of summations.
Considering rectangular domains with different aspect ratios, comparison of the
results of derived expressions with those of summation forms of SPPF is done.
It's shown that analytical expressions for SPPF give very precise results with
maximum relative errors of around 1%, 2% and 3% at just the transition point
for single, double and triple transitions respectively. Based on dimensional
transitions, expressions for free energy, entropy, internal energy, chemical
potential, heat capacity and pressure are given analytically valid for any
scale.
| [{'version': 'v1', 'created': 'Tue, 24 Feb 2015 15:40:57 GMT'}
{'version': 'v2', 'created': 'Wed, 1 Apr 2015 09:45:49 GMT'}] | 2016-02-24 | [array(['Aydin', 'Alhun', ''], dtype=object)
array(['Sisman', 'Altug', ''], dtype=object)] |
19,880 | hep-th/0308048 | Shevchenko O. Yu. | A.N. Sissakian, O.Yu. Shevchenko, V.N. Samoilov | Possibility of the new type phase transition | null | null | null | null | hep-th | null | The scalar field theory and the scalar electrodynamics quantized in the flat
gap are considered. The dynamical effects arising due to the boundary presence
with two types of boundary conditions (BC) satisfied by scalar fields are
studied. It is shown that while the Neumann BC lead to the usual scalar field
mass generation, the Dirichlet BC give rise to the dynamical mechanism of
spontaneous symmetry breaking. Due to the later, there arises the possibility
of the new type phase transition from the normal to spontaneously broken phase.
The decreasing in the characteristic size of the quantization region (the gap
size here) and increasing in the temperature compete with each other, tending
to transport the system in the spontaneously broken and in the normal phase,
respectively. The system evolves with a combined parameter, simultaneously
reflecting the change in temperature and in the size. As a result, at the
critical value of this parameter there occurs the phase transition from the
normal phase to the spontaneously broken one. In particular, the usual massless
scalar electrodynamics transforms to the Higgs model.
| [{'version': 'v1', 'created': 'Wed, 6 Aug 2003 19:49:25 GMT'}
{'version': 'v2', 'created': 'Mon, 11 Aug 2003 15:50:15 GMT'}
{'version': 'v3', 'created': 'Mon, 15 Dec 2003 12:21:40 GMT'}] | 2015-07-27 | [array(['Sissakian', 'A. N.', ''], dtype=object)
array(['Shevchenko', 'O. Yu.', ''], dtype=object)
array(['Samoilov', 'V. N.', ''], dtype=object)] |
19,881 | 2207.08517 | Eric Ricardo Carreon Ruiz | E. R. Carre\'on Ruiz, J. Lee, J. I. M\'arquez Dami\'an, M. Strobl, G.
Burca, R. Woracek, M. Cochet, M.-O. Ebert, L. H\"oltschi, P. M. Kadletz, A.
S. Tremsin, E. Winter, M. Zlobinski, L. Gubler, and P. Boillat | Spectroscopic Neutron Imaging for Resolving Hydrogen Dynamics Changes in
Battery Electrolytes | null | null | null | null | cond-mat.mtrl-sci physics.chem-ph | http://creativecommons.org/licenses/by/4.0/ | We present spectroscopic neutron imaging (SNI), a bridge between imaging and
scattering techniques, for the analysis of hydrogenated molecules in
lithium-ion cells. The scattering information of CHn-based organic solvents and
electrolytes was mapped in two-dimensional space by investigating the
wavelength-dependent property of hydrogen atoms through time-of-flight imaging.
Our investigation demonstrates a novel approach to detect physical and chemical
changes in hydrogenated liquids, which extends, but not limits, the use of SNI
to relevant applications in electrochemical devices, e.g., the study of
electrolytes in Li-ion batteries.
| [{'version': 'v1', 'created': 'Mon, 18 Jul 2022 11:26:00 GMT'}] | 2022-07-19 | [array(['Ruiz', 'E. R. Carreón', ''], dtype=object)
array(['Lee', 'J.', ''], dtype=object)
array(['Damián', 'J. I. Márquez', ''], dtype=object)
array(['Strobl', 'M.', ''], dtype=object)
array(['Burca', 'G.', ''], dtype=object)
array(['Woracek', 'R.', ''], dtype=object)
array(['Cochet', 'M.', ''], dtype=object)
array(['Ebert', 'M. -O.', ''], dtype=object)
array(['Höltschi', 'L.', ''], dtype=object)
array(['Kadletz', 'P. M.', ''], dtype=object)
array(['Tremsin', 'A. S.', ''], dtype=object)
array(['Winter', 'E.', ''], dtype=object)
array(['Zlobinski', 'M.', ''], dtype=object)
array(['Gubler', 'L.', ''], dtype=object)
array(['Boillat', 'P.', ''], dtype=object)] |
19,882 | 1312.4727 | Reema Al-Aifari | Reema Al-Aifari, Michel Defrise and Alexander Katsevich | Asymptotic analysis of the SVD for the truncated Hilbert transform with
overlap | 25 pages | null | null | null | math.CA math.SP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The truncated Hilbert transform with overlap $H_T$ is an operator that arises
in tomographic reconstruction from limited data, more precisely in the method
of Differentiated Back-Projection (DBP). Recent work [1] has shown that the
singular values of this operator accumulate at both zero and one. To better
understand the properties of the operator and, in particular, the ill-posedness
of the inverse problem associated with it, it is of interest to know the rates
at which the singular values approach zero and one. In this paper, we exploit
the property that $H_T$ commutes with a second-order differential operator
$L_S$ and the global asymptotic behavior of its eigenfunctions to find the
asymptotics of the singular values and singular functions of $H_T$.
| [{'version': 'v1', 'created': 'Tue, 17 Dec 2013 11:45:14 GMT'}] | 2013-12-18 | [array(['Al-Aifari', 'Reema', ''], dtype=object)
array(['Defrise', 'Michel', ''], dtype=object)
array(['Katsevich', 'Alexander', ''], dtype=object)] |
19,883 | 2206.06324 | Mukesh Kumar | Ashok Goyal, Mohammed Omer Khojali, Mukesh Kumar and Alan S. Cornell | Neutrino specific spin-3/2 dark matter | 10 pages, 1 table, 4 figures, published version in EPJC | Eur. Phys. J. C (2022) 82:1002 | 10.1140/epjc/s10052-022-10975-w | null | hep-ph | http://creativecommons.org/publicdomain/zero/1.0/ | In this paper we consider a spin-$\frac{3}{2}$ dark matter (DM) particle
coupled to neutrinos as a viable candidate to produce the observed DM relic
density through the thermal freeze-out mechanism. The couplings of DM to
neutrinos is considered first in a most general dimension six effective field
theory framework. We then consider two specific neutrino-portal models
discussed in the literature. In the first model DM couples to the standard
model neutrinos through mixing generated by a sterile pseudo-Dirac massive
neutrino and the second model we consider is the widely studied $U(1)_{L_\mu -
L_\tau}$ gauge symmetric model. For each of these models we explore the
parameter space required to generate the observed relic density. The
constraints on the parameters of these models from the existing and proposed
neutrino experiments as well as from existing cosmological and astrophysical
bounds are considered in the context of the relic density calculations.
| [{'version': 'v1', 'created': 'Mon, 13 Jun 2022 17:10:22 GMT'}
{'version': 'v2', 'created': 'Sat, 29 Oct 2022 19:15:25 GMT'}
{'version': 'v3', 'created': 'Tue, 8 Nov 2022 17:13:15 GMT'}] | 2022-11-09 | [array(['Goyal', 'Ashok', ''], dtype=object)
array(['Khojali', 'Mohammed Omer', ''], dtype=object)
array(['Kumar', 'Mukesh', ''], dtype=object)
array(['Cornell', 'Alan S.', ''], dtype=object)] |
19,884 | 2204.05403 | Sergey Nadtochiy | Guillermo Alonso Alvarez, Sergey Nadtochiy, and Kevin Webster | Optimal brokerage contracts in Almgren-Chriss model with multiple
clients | null | null | null | null | q-fin.TR q-fin.MF | http://creativecommons.org/licenses/by/4.0/ | This paper constructs optimal brokerage contracts for multiple
(heterogeneous) clients trading a single asset whose price follows the
Almgren-Chriss model. The distinctive features of this work are as follows: (i)
the reservation values of the clients are determined endogenously, and (ii) the
broker is allowed to not offer a contract to some of the potential clients,
thus choosing her portfolio of clients strategically. We find a computationally
tractable characterization of the optimal portfolios of clients (up to a
digital optimization problem, which can be solved efficiently if the number of
potential clients is small) and conduct numerical experiments which illustrate
how these portfolios, as well as the equilibrium profits of all market
participants, depend on the price impact coefficients.
| [{'version': 'v1', 'created': 'Mon, 11 Apr 2022 20:50:04 GMT'}] | 2022-04-13 | [array(['Alvarez', 'Guillermo Alonso', ''], dtype=object)
array(['Nadtochiy', 'Sergey', ''], dtype=object)
array(['Webster', 'Kevin', ''], dtype=object)] |
19,885 | 1512.06403 | Louis Funar | Karim A. Adiprasito and Louis Funar | CAT(0) metrics on contractible manifolds | 26p., 6 figures | null | null | null | math.GT | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We prove that an open manifold $M$ of dimension at least $5$ which admits a
complete CAT(0) polyhedral metric is pseudo-collarable, its fundamental group
at infinity is strongly perfectly semistable and has vanishing
Chapman-Siebenmann obstruction $\tau_{\infty}(M)$. Moreover, this implies that
$M$ is topologically collapsible, when $n\geq 6$. Conversely, any finite
dimensional collapsible polyhedron is PL homeomorphic to a CAT(0) cubical
complex.
| [{'version': 'v1', 'created': 'Sun, 20 Dec 2015 17:13:28 GMT'}
{'version': 'v2', 'created': 'Sun, 3 Jan 2016 20:57:34 GMT'}
{'version': 'v3', 'created': 'Thu, 29 Sep 2016 11:28:49 GMT'}
{'version': 'v4', 'created': 'Sun, 26 Dec 2021 21:02:00 GMT'}] | 2021-12-28 | [array(['Adiprasito', 'Karim A.', ''], dtype=object)
array(['Funar', 'Louis', ''], dtype=object)] |
19,886 | 2202.07161 | Yizhuang Song | Yizhuang Song, Rosalind Sadleir and Jijun Liu | Convergence analysis of the harmonic $B_z$ algorithm with single
injection current in MREIT | null | null | null | null | math.AP | http://creativecommons.org/licenses/by/4.0/ | Magnetic resonance electrical impedance tomography (MREIT) aims to recover
the electrical conductivity distribution of an object using partial information
of magnetic flux densities inside the tissue which can be measured using an MRI
scanner, with the advantage that a higher spatial resolution of conductivity
image can be provided than existing EIT techniques involving surface
measurements. Traditional MREIT reconstruction algorithms use two data sets
obtained with two linearly independent injected currents. However, injection of
two currents is often not possible in applications such as transcranial
electrical stimulation. Recently, we proposed an iterative conductivity
reconstruction algorithm called the single current harmonic $B_z$ algorithm
that demonstrated satisfactory performance in numerical and phantom tests. In
this paper, we provide a rigorous mathematical analysis of the convergence of
the iterative sequence for realizing this algorithm. We prove that, applying
some mild conditions on the exact conductivity, the iterative sequence
converges to the true solution within an explicit error bound. Such theoretical
results substantiate the reasonability and efficiency of the proposed
algorithm. We also provide more numerical evidence to validate these
theoretical results.
| [{'version': 'v1', 'created': 'Tue, 15 Feb 2022 03:15:50 GMT'}] | 2022-02-16 | [array(['Song', 'Yizhuang', ''], dtype=object)
array(['Sadleir', 'Rosalind', ''], dtype=object)
array(['Liu', 'Jijun', ''], dtype=object)] |
19,887 | 1212.0508 | Semyon Konstein | S. E. Konstein and R. Stekolshchik | Klein operator and the Numbers of independent Traces and Supertraces on
the Superalgebra of Observables of Rational Calogero Model based on the Root
System | Latex 2e, 12 pages., arXiv admin note: text overlap with
arXiv:1211.6600, text corresponds to the published version | Journal of Nonlinear Mathematical Physics, 20:2, 295-308 (2013) | 10.1080/14029251.2013.820410 | null | math.RT hep-th math-ph math.MP | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In the Coxeter group W(R) generated by the root system R, let T(R) be the
number of conjugacy classes having no eigenvalue 1 and let S(R) be the number
of conjugacy classes having no eigenvalue -1. The algebra H{R) of observables
of the rational Calogero model based on the root system R possesses T(R)
independent traces, the same algebra considered as an associative superalgebra
with respect to a certain natural parity possesses S(R) even independent
supertraces and no odd trace or supertrace. The numbers T(R) and S(R) are
determined for all irreducible root systems (hence for all root systems). It is
shown that T(R) =< S(R), and T(R) = S(R) if and only if superalgebra H(R)
contains a Klein operator (or, equivalently, W(R) containes -1).
| [{'version': 'v1', 'created': 'Mon, 3 Dec 2012 19:46:56 GMT'}
{'version': 'v2', 'created': 'Sun, 26 Nov 2017 13:48:49 GMT'}] | 2018-08-07 | [array(['Konstein', 'S. E.', ''], dtype=object)
array(['Stekolshchik', 'R.', ''], dtype=object)] |
19,888 | 1510.01943 | Paolo Francavilla | Paolo Francavilla | Measurements of inclusive jet and dijet cross sections at the Large
Hadron Collider | Contribution to "Jet Measurements at the LHC", G. Dissertori ed. To
appear in International Journal of Modern Physics A (IJMPA) | null | null | null | hep-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | This review discusses the measurements of the inclusive jet and dijet cross
section performed by the experimental collaborations at the LHC during what is
now being called LHC Run 1 (2009 - 2013). It summarises some of the
experimental challenges and the techniques used in the measurements of jets
cross sections during the LHC Run 1.
| [{'version': 'v1', 'created': 'Wed, 7 Oct 2015 13:48:35 GMT'}] | 2015-10-08 | [array(['Francavilla', 'Paolo', ''], dtype=object)] |
19,889 | 2008.00558 | Barbara Benato | Barbara Caroline Benato and Jancarlo Ferreira Gomes and Alexandru
Cristian Telea and Alexandre Xavier Falc\~ao | Semi-supervised deep learning based on label propagation in a 2D
embedded space | 7 pages, 5 figures | null | null | null | cs.CV cs.LG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | While convolutional neural networks need large labeled sets for training
images, expert human supervision of such datasets can be very laborious.
Proposed solutions propagate labels from a small set of supervised images to a
large set of unsupervised ones to obtain sufficient truly-and-artificially
labeled samples to train a deep neural network model. Yet, such solutions need
many supervised images for validation. We present a loop in which a deep neural
network (VGG-16) is trained from a set with more correctly labeled samples
along iterations, created by using t-SNE to project the features of its last
max-pooling layer into a 2D embedded space in which labels are propagated using
the Optimum-Path Forest semi-supervised classifier. As the labeled set improves
along iterations, it improves the features of the neural network. We show that
this can significantly improve classification results on test data (using only
1\% to 5\% of supervised samples) of three private challenging datasets and two
public ones.
| [{'version': 'v1', 'created': 'Sun, 2 Aug 2020 20:08:54 GMT'}
{'version': 'v2', 'created': 'Fri, 15 Jan 2021 14:30:27 GMT'}] | 2021-01-18 | [array(['Benato', 'Barbara Caroline', ''], dtype=object)
array(['Gomes', 'Jancarlo Ferreira', ''], dtype=object)
array(['Telea', 'Alexandru Cristian', ''], dtype=object)
array(['Falcão', 'Alexandre Xavier', ''], dtype=object)] |
19,890 | 1706.01775 | David Emin | David Emin, Massoud Akhtari, Aria Fallah, Harry V. Vinters and Gary W.
Mathern | Anomalous frequency-dependent ionic conductivity of lesion-laden
human-brain tissue | 14 pages, 5 figures | Journal of Applied Physics 122,154701 (2017) | 10.1063/1.4986358 | null | physics.med-ph cond-mat.soft | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | We study the effect of lesions on our four-electrode measurements of the
ionic conductivity of (1 cm3) samples of human brain excised from patients
undergoing pediatric epilepsy surgery. For most (about 94 %) samples the
low-frequency ionic conductivity rises upon increasing the applied frequency.
We attributed this behavior to the long-range (0.4 mm) diffusion of solvated
sodium cations before encountering impenetrable blockages such as cell
membranes, blood vessels and cell walls. By contrast, the low-frequency ionic
conductivity of some (6 %) brain tissue samples falls with increasing applied
frequency. We attribute this unusual frequency-dependence to the electric-field
induced liberation of sodium cations from traps introduced by the unusually
severe pathology observed in samples from these patients. Thus, the anomalous
frequency-dependence of the ionic conductivity indicates trap-producing brain
lesions.
| [{'version': 'v1', 'created': 'Mon, 5 Jun 2017 01:57:05 GMT'}] | 2017-12-19 | [array(['Emin', 'David', ''], dtype=object)
array(['Akhtari', 'Massoud', ''], dtype=object)
array(['Fallah', 'Aria', ''], dtype=object)
array(['Vinters', 'Harry V.', ''], dtype=object)
array(['Mathern', 'Gary W.', ''], dtype=object)] |
19,891 | cmp-lg/9409002 | null | Mark Lauer (Microsoft Institute, Sydney) | Conceptual Association for Compound Noun Analysis | 3 pages, postscript only, replaced because original postscript
version incompatible with some printers | Proceedings of the Student Session, 32nd Annual Meeting of the
Association for Computational Linguistics, Las Cruces, NM., 1994 pp337-339 | null | null | cmp-lg cs.CL | null | This paper describes research toward the automatic interpretation of compound
nouns using corpus statistics. An initial study aimed at syntactic
disambiguation is presented. The approach presented bases associations upon
thesaurus categories. Association data is gathered from unambiguous cases
extracted from a corpus and is then applied to the analysis of ambiguous
compound nouns. While the work presented is still in progress, a first attempt
to syntactically analyse a test set of 244 examples shows 75% correctness.
Future work is aimed at improving this accuracy and extending the technique to
assign semantic role information, thus producing a complete interpretation.
| [{'version': 'v1', 'created': 'Tue, 6 Sep 1994 18:59:21 GMT'}
{'version': 'v2', 'created': 'Wed, 11 Sep 1996 02:26:42 GMT'}] | 2008-02-03 | [array(['Lauer', 'Mark', '', 'Microsoft Institute, Sydney'], dtype=object)] |
19,892 | astro-ph/9602002 | Uta Fritze-v. Alvensleben | Uta Fritze - von Alvensleben | Interacting and Merging Galaxies | 14 pages, LaTeX, no figures, to appear in: ''From Stars to
Galaxies'', eds. C. Leitherer, U. Fritze - von Alvensleben, J. Huchra, Minor
revisions: NGC 3597 (not 3596), 2nd nucleus in M31: 2pc (not 2 kpc) | null | null | null | astro-ph | null | I will present a review of some of the many recent developments within the
exciting and rapidly evolving field of Interacting and Merging Galaxies. I will
touch both on observations and on theory, focussing on those aspects where
galaxy evolution modelling may possibly contribute to our understanding.
After briefly outlining the basic concepts and a few specific results of
stellar- and gasdynamical modelling of galaxy -- galaxy mergers (Sect. 1) I
choose three examples of interacting/merged galaxy pairs to discuss different
aspects of mergers: tracing back the star formation history of the old merger
remnant NGC 7252 (Sect. 2), the formation of young star clusters (Sect. 3) and
dwarf galaxies (Sect. 4) in Antennae, and the molecular gas content of IR-UL
galaxies on the example of Arp 220 (Sect. 5). I'll touch the interaction --
activity connection in Sect. 6 and report attempts to identify merger remnants
among today's galaxies in Sect. 7. After few words on merger rates at present
and in the past (Sect. 8), I'll close with a brief outlook.
| [{'version': 'v1', 'created': 'Thu, 1 Feb 1996 10:47:07 GMT'}
{'version': 'v2', 'created': 'Mon, 5 Feb 1996 10:09:25 GMT'}] | 2016-08-30 | [array(['von Alvensleben', 'Uta Fritze -', ''], dtype=object)] |
19,893 | 2201.08893 | Maximilian Wolff | Max Wolff and Stuart Wolff | Signal Strength and Noise Drive Feature Preference in CNN Image
Classifiers | Accepted at SVRHM 2021 | null | null | null | cs.CV cs.LG | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | Feature preference in Convolutional Neural Network (CNN) image classifiers is
integral to their decision making process, and while the topic has been well
studied, it is still not understood at a fundamental level. We test a range of
task relevant feature attributes (including shape, texture, and color) with
varying degrees of signal and noise in highly controlled CNN image
classification experiments using synthetic datasets to determine feature
preferences. We find that CNNs will prefer features with stronger signal
strength and lower noise irrespective of whether the feature is texture, shape,
or color. This provides guidance for a predictive model for task relevant
feature preferences, demonstrates pathways for bias in machine models that can
be avoided with careful controls on experimental setup, and suggests that
comparisons between how humans and machines prefer task relevant features in
vision classification tasks should be revisited. Code to reproduce experiments
in this paper can be found at
\url{https://github.com/mwolff31/signal_preference}.
| [{'version': 'v1', 'created': 'Wed, 19 Jan 2022 11:32:19 GMT'}] | 2022-01-25 | [array(['Wolff', 'Max', ''], dtype=object)
array(['Wolff', 'Stuart', ''], dtype=object)] |
19,894 | 1810.00288 | Govind Paneru | John A.C. Albay, Govind Paneru, Hyuk Kyu Pak, and Yonggun Jun | Optical tweezers as a mathematically driven spatio-temporal potential
generator | null | Opt. Express 26, 29906-29915 (2018) | 10.1364/OE.26.029906 | null | cond-mat.stat-mech | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | The ability to create and manipulate the spatio-temporal potentials is
essential in the diverse fields of science and technology. Here, we introduce
an optical feedback trap system based on a high precision position detection
and an ultrafast feedback control of a Brownian particle in the optical
tweezers to generate spatio-temporal virtual potentials of the desired shape in
a controlled manner. As an application, we study nonequilibrium fluctuation
dynamics of the particle in a time-varying virtual harmonic potential and
validate the Crooks fluctuation theorem in highly nonequilibrium condition.
| [{'version': 'v1', 'created': 'Sun, 30 Sep 2018 01:09:09 GMT'}] | 2018-11-06 | [array(['Albay', 'John A. C.', ''], dtype=object)
array(['Paneru', 'Govind', ''], dtype=object)
array(['Pak', 'Hyuk Kyu', ''], dtype=object)
array(['Jun', 'Yonggun', ''], dtype=object)] |
19,895 | 1310.7723 | Yuval Vinkler | Yuval Vinkler-Aviv, Avraham Schiller and Natan Andrei | Single-molecule-mediated heat current between an electronic and a
bosonic bath | null | Phys. Rev. B 89, 024307 (2014) | 10.1103/PhysRevB.89.024307 | null | cond-mat.str-el | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In molecular devices electronic degrees of freedom are coupled to vibrational
modes of the molecule, offering an opportunity to study fundamental aspects of
this coupling between at the nanoscale. To this end we consider the
nonequilibrium heat exchange between a conduction band and a bosonic bath
mediated by a single molecule. For molecules large enough so that on-site
interactions can be dropped we carry out an asymptotically exact calculation of
the heat current, governed by the smallness of the electron-phonon coupling,
and obtain the steady state heat current driven by a finite temperature drop.
At low temperatures the heat current is found to have a power-law behavior with
respect to the temperature difference with the power depending on the nature of
the bosonic bath. At high temperatures, on the other hand, the current is
linear in the temperature difference for all types of bosonic baths. The
crossover between these behaviors is described. Some of the results are given a
physical explanation by comparing to a perturbative Master equation calculation
(whose limitation we examine).
| [{'version': 'v1', 'created': 'Tue, 29 Oct 2013 09:32:24 GMT'}
{'version': 'v2', 'created': 'Tue, 14 Jan 2014 08:31:44 GMT'}] | 2014-01-29 | [array(['Vinkler-Aviv', 'Yuval', ''], dtype=object)
array(['Schiller', 'Avraham', ''], dtype=object)
array(['Andrei', 'Natan', ''], dtype=object)] |
19,896 | 2211.03576 | Zihan Zang | Zihan Zang, Haoqiang Wang, Yunpeng Xu | DAD vision: opto-electronic co-designed computer vision with division
adjoint method | null | null | null | null | cs.CV eess.IV physics.optics | http://creativecommons.org/licenses/by-nc-nd/4.0/ | The miniaturization and mobility of computer vision systems are limited by
the heavy computational burden and the size of optical lenses. Here, we propose
to use a ultra-thin diffractive optical element to implement passive optical
convolution. A division adjoint opto-electronic co-design method is also
proposed. In our simulation experiments, the first few convolutional layers of
the neural network can be replaced by optical convolution in a classification
task on the CIFAR-10 dataset with no power consumption, while similar
performance can be obtained.
| [{'version': 'v1', 'created': 'Fri, 4 Nov 2022 07:31:44 GMT'}] | 2022-11-08 | [array(['Zang', 'Zihan', ''], dtype=object)
array(['Wang', 'Haoqiang', ''], dtype=object)
array(['Xu', 'Yunpeng', ''], dtype=object)] |
19,897 | 2205.15315 | Giorgio Sonnino | Giorgio Sonnino | Thermodynamic Flux-Force Closure Relations for Systems out of the
Onsager Region | 45 Pages and 12 Figures. Manuscript accepted for publication in
Springer Nature | null | 10.1007/978-3-031-04458-8_5 | null | physics.plasm-ph | http://creativecommons.org/publicdomain/zero/1.0/ | The objective of this work is to determine the nonlinear flux-force relations
for systems out of Onsager's region that respect the existing thermodynamic
theorems for systems far from equilibrium. To this aim, a thermodynamic theory
for irreversible processes [referred to as the Thermodynamical Field Theory
(TFT)] has been developed. The TFT rests upon the concept of equivalence
between thermodynamic systems: "The equivalent character of two alternative
descriptions of a thermodynamic system is ensured if, and only if, the entropy
production and the Glansdorff-Prigogine dissipative quantity remain unaltered
under the thermodynamic forces transformation". The TCT leads naturally to the
"Thermodynamic Covariance Principle" (TCP) stating that "The nonlinear closure
equations, i.e., the flux-force relations, must be covariant under TCT". In
this work, we provide the explicit expression of the nonlinear PDEs, subjected
to the appropriate boundary conditions, which have to be satisfied by transport
coefficients when the skew-symmetric piece is absent. The solution of these
equations allows to determine the flux-force closure relations for systems out
of the Onsager region. Since the proposed PDEs are obtained without neglecting
any term present in the balance equations (i.e., the mass, momentum, and energy
balance equations), we propose them as a good candidate for describing
transport in thermodynamic systems also in turbulent regime. A preliminary test
is carried out by analysing a concrete example where Onsager's relations
manifestly disagree with experience: losses in magnetically confined
Tokamak-plasmas in fully collisional and in turbulent regimes. We show the good
agreement between the theoretical predictions and the experimental data. The
aim is to apply our approach to the "Divertor Tokamak Test facility" (DTT), to
be built in Italy, and to ITER.
| [{'version': 'v1', 'created': 'Sun, 29 May 2022 19:25:27 GMT'}] | 2022-12-07 | [array(['Sonnino', 'Giorgio', ''], dtype=object)] |
19,898 | 1110.2560 | Liangliang Wang | Liangliang Wang (for the BESIII Collaboration) | Study of charmonium spectroscopy at BESIII | 4 pages, 3 figures, hadron2011 proceeding v2 | null | null | null | hep-ex | http://arxiv.org/licenses/nonexclusive-distrib/1.0/ | In this talk, we will present the results on the charmonium spin singlet
states below the open charm threshold, including h_c, \eta_c, and \eta_c(2S).
The masses, widthes, and production rates of these states will be reported. The
results are based on a data sample of 106 million \psi' events collected with
the BESIII experiments at the BEPCII collider.
| [{'version': 'v1', 'created': 'Wed, 12 Oct 2011 03:30:54 GMT'}
{'version': 'v2', 'created': 'Mon, 17 Oct 2011 03:06:30 GMT'}] | 2019-08-13 | [array(['Wang', 'Liangliang', '', 'for the BESIII Collaboration'],
dtype=object) ] |
19,899 | math/0312218 | Mihail N. Kolountzakis | Mihail N. Kolountzakis and Szilard Gy. Revesz | Tur\'an's extremal problem for positive definite functions on groups | 18 pages, 1 figure | null | null | null | math.CA math.NT | null | We study the following question: Given an open set $\Omega$, symmetric about
0, and a continuous, integrable, positive definite function $f$, supported in
$\Omega$ and with $f(0)=1$, how large can $\int f$ be? This problem has been
studied so far mostly for convex domains $\Omega$ in Euclidean space. In this
paper we study the question in arbitrary locally compact abelian groups and for
more general domains. Our emphasis is on finite groups as well as Euclidean
spaces and $\ZZ^d$. We exhibit upper bounds for $\int f$ assuming geometric
properties of $\Omega$ of two types: (a) packing properties of $\Omega$ and (b)
spectral properties of $\Omega$. Several examples and applications of the main
theorems are shown. In particular we recover and extend several known results
concerning convex domains in Euclidean space. Also, we investigate the question
of estimating $\int_{\Omega}f$ over possibly dispersed sets solely in
dependence of the given measure $m:=|\Omega|$ of $\Omega$. In this respect we
show that in $\RR$ and $\ZZ$ the integral is maximal for intervals.
| [{'version': 'v1', 'created': 'Wed, 10 Dec 2003 18:03:33 GMT'}] | 2007-05-23 | [array(['Kolountzakis', 'Mihail N.', ''], dtype=object)
array(['Revesz', 'Szilard Gy.', ''], dtype=object)] |