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1,314,259,996,263 | arxiv | \section{Introduction}
\noindent Transferring knowledge from a labeled source domain to an unlabeled target domain is desirable in many real-world applications. However, deep learning models do not perform well in the presence of such domain shifts. For example, a model trained on synthetic data may fail to generalize... |
1,314,259,996,264 | arxiv | \section{Introduction}
The strong field approximation (SFA) \cite{ref_KFR_amplitude} is {\em the} underlying theory describing the interaction of intense laser light with atoms \cite{ref_JPB_review} or molecules \cite{milo_molecules}. It allows to calculate photoelectron \cite{ref_JPB_review} or high-harmonic spectra \... |
1,314,259,996,265 | arxiv | \section{Acknowledgements}
We thank A.~H\"ogele, M.~Munsch, and J.-V. Kim for fruitful discussions and valuable feedback on the manuscript and A. Ferreira for technical help.
We gratefully acknowledge financial support from the SNI; NCCR QSIT; SNF grants 143697, 155845, 169016 and 178891 the EU Graphene Flagship. N.U.... |
1,314,259,996,266 | arxiv | \section{\label{Introduction}Introduction}
The physics of turbulent flows, which are ubiquitous in real-world applications, is a widely addressed, yet not fully understood, research topic, so that turbulence is often considered as the last unsolved problem of classical physics~\cite{frisch1995turbulence}.
Examples w... |
1,314,259,996,267 | arxiv | \section{Introduction}
In this paper we consider a finite dimensional vector space $X$ over a field $\mathbb K$ of characteristic 0 and
the associative algebras with zero differentials $A=\mathrm S(X^*)$ resp. $B=\wedge(X)$
i.e. the symmetric algebra over $X^*$, resp. the exterior algebra over $X$.
For simplic... |
1,314,259,996,268 | arxiv | \section{Introduction}
For many years the existence of a bound state of two $^4$He atoms
was an open problem. Some potential models predicted such a state
\cite{BruchMcGee1970,Aziz79,UangStwalley} while the others did not
\cite{DeBoer1958,Beck1968}. However practically all more or less
realistic helium-helium p... |
1,314,259,996,269 | arxiv |
\section{Lower bounds for randomized algorithms}
When constructing hard instances for randomized algorithms, one does not have the luxury of reacting to the algorithms queries, because we cannot anticipate the random seed $\xi$. The approach taken here, and in prior work, is to draw orthogonal vectors from some h... |
1,314,259,996,270 | arxiv | \section{Introduction}
\begin{figure}[t]
\centering
\includegraphics[width=0.8\linewidth]{figs/action-comparison.pdf}
\caption{The comparison among common actions in our daily life, actions in individual sports and actions in team sports. Top: common actions in UCF101 \cite{soomro2012ucf101}, which i... |
1,314,259,996,271 | arxiv | \section{More discussion on EMMP}
\section{Hyper-parameters}
For the baselines, we leverage the codebase maintained by~\citep{satorras2021en}. We tune the hyper-parameters around the suggested hyper-parameters as specified in~\citep{huang2022constrained} for the baselines. Specifically, for GNN, RF and EGNN, we tu... |
1,314,259,996,272 | arxiv | \section{Introduction}
\subsection{Totally nonnegative flag varieties of reductive groups}
The theory of total positivity on the reductive groups $G$ and their partial flag varieties $\ensuremath{\mathcal {P}}\xspace_K$ was introduced by Lusztig in the seminal work \cite{Lu94}. The totally nonnegative partial flag va... |
1,314,259,996,273 | arxiv | \section{The model}\label{sec:model}
We focus our attention on a modified version of the $p$-spin
Hamiltonian, the so-called multi-$p$-spin model, in which spins do
interact in $r$-uples with $r$ taking more than one value:
\begin{equation}
\mathcal{H}\{\underline\sigma\} = -\sum_r c_r \sum_{1 \le i_1 < \ldots <
i_r... |
1,314,259,996,274 | arxiv | \section{Introduction and motivation}
\label{intro}Common, even simple, mathematical problems usually involve
nonlinear maps, sometimes acting on sets with little (or none) algebraic
structure; so the extension of linear techniques to the nonlinear setting,
besides its intrinsic mathematical interest, is an impor... |
1,314,259,996,275 | arxiv | \section{Introduction}
In the study of infinite dimensional algebras, the notion of dimension of course has not much sense. However, instead of the dimension, one can categorize an algebra by the growth of the dimension of finitely generated subalgebras, if the algebra is filtered or graded. For commutative algebras, t... |
1,314,259,996,276 | arxiv | \section{Invariant mass spectroscopy in RI-beam experiments}
Rare isotope beams available at in-flight separators, at
RIKEN (RIBF), MSU, GSI, and GANIL, have
expanded physics opportunities to a wider range of $N-Z$.
Accordingly, more experiments have been
performed for nuclei near the drip line or even beyond~\cite{T... |
1,314,259,996,277 | arxiv | \section{Introduction}
For a bipartite graph $G$, we write $G=(V_1\cup V_2, E)$ to indicate that $V_1$ and $V_2$ are the stable sets of $V(G)$. Define a {\it mirror bipartite graph} of order $2n$ to be a bipartite graph $G=(V_1\cup V_2,E)$ for which there exists a bijective function $\varphi : V_1\rightarrow V_2$ ... |
1,314,259,996,278 | arxiv | \section{Introduction}
The history of the theory and practice of quantization dates back to 1948. Since then quantization has become an important field in electrical engineering in connection with signal processing and data compression. Broadly speaking, quantization consists in replacing an actual large data set of... |
1,314,259,996,279 | arxiv | \section{Introduction}
Over the last decades double perovskite manganites have been of great interest in many fields such as cathodes of solid oxide fuel cells (SOFC) for high temperature applications \cite{Navickas2015}, magnetic storage and magnetic field sensing functions at room temperature \cite{Haghiri-Gosnet2000... |
1,314,259,996,280 | arxiv | \section*{Abstract}
The recent increase in public and academic interest in preserving biodiversity has led to the growth of the field of conservation technology. This field involves designing and constructing tools that utilize technology to aid in the conservation of wildlife. In this article, we will use case studies... |
1,314,259,996,281 | arxiv | \section{Introduction}
\label{S1}
Graphene-based electronics has been the subject of an intensive theoretical and experimental research since the discovery of
this striking two-dimensional material in 2004 \cite{NG2004}.
Particularly promising are device architectures that mimic the ordinary semiconductor heterojuncti... |
1,314,259,996,282 | arxiv | \section{Introduction}\label{sec:introduction}}
\else
\section{Introduction}
\label{section:introduction}
\fi
\IEEEPARstart{I}{n} today's world, with tremendous amounts of sensitive data becoming digitized, protecting private user data is paramount. Passwords or other single-sign-on (SSO) security measures are typical... |
1,314,259,996,283 | arxiv | \section{Introduction}
The action we consider in $D=2n$ dimensions reads
\begin{eqnarray}
S = \int d^Dx \left( \sqrt{|g|} g^{ab} R_{ab}(\Gamma) +{\textstyle\frac 1 n} \theta\epsilon^{a_1a_2 \dots a_{D}}
R^{i_1}{}_{i_2 a_1 a_2} R^{i_2}{}_{i_3 a_3 a_4} \dots R^{i_n}{}_{i_1 a_{D-1} a_D}(\Gamma) \right) \,.
\eer{act1}
In... |
1,314,259,996,284 | arxiv | \section{Introduction}
Deeply virtual Compton scattering (DVCS) is considered as the
theoretically cleanest process to investigate generalized parton
distributions (GPDs) \cite{MueRobGeyDitHor94,Ji96,Rad96}. These
distributions are a hybrid of parton densities, form-factors, and
distribution amplitudes and might be re... |
1,314,259,996,285 | arxiv | \section{Introduction}\label{introduction}
Quantum statistical mechanics has many similarities to the classical version, and also some differences. Two facts true in the quantum but not in the classical case, \emph{canonical typicality} and (what we call) \emph{normal typicality}, follow from just the general mathemat... |
1,314,259,996,286 | arxiv | \section{Introduction}
The charmonium spectrum consists of eight narrow states below the open charm threshold (3.73~GeV) and several tens of states above that.
Below the threshold almost all states are well-established. In contrast very little is known at higher masses where there have been discoveries~\cite{qr} of se... |
1,314,259,996,287 | arxiv | \section{Preliminaries}
\subsection{Introduction}
In this paper we are concerned with the existence of the ground state of the so-called semi-relativistic Pauli-Fierz (it is shorthand as "SRPF" in this paper) model in quantum electrodynamics.
This model describes a minimal interaction between a semi-relativistic quan... |
1,314,259,996,288 | arxiv | \section{Introduction}\label{sec:introduction}
Naturally, most verbal communication occurs in context when the listener can see the speaker as well as hear them. Although speech perception is normally regarded as a purely auditory process, visual cues can enhance the level of speech understanding~\cite{OuluVS} and McGu... |
1,314,259,996,289 | arxiv | \subsection*{Acknowledgements} We thank Arend Bayer, Luis Garcia, Chunyi Li, Jan Manschot, Davesh Maulik and Rahul Pandharipande for their generous help with this paper. Our intellectual debt to Yukinobu Toda is described in Section \ref{related}.
We acknowledge the support of an EPSRC postdoctoral fellowship EP/T0186... |
1,314,259,996,290 | arxiv | \section{Supersymmetric Kramers equation}
We consider a system of $n$ interacting particles in the 3-dimensional space,
defined by the Hamiltonian
\begin{equation}
\mathcal{H}=\frac{\mathbf{p}^2}{2m}+V(\mathbf{q}) \,,
\end{equation}
where the vectors $\mathbf{q} = (\vec{q}_{1}, \dots, \vec{q}_{n})$ and $\mathbf{p} ... |
1,314,259,996,291 | arxiv |
\section{Introduction}
\label{sec:intro}
\input{sections/introduction}
\section{Decoupling Using Language-Neutral Protocols}
\label{sec:decoupling}
\input{sections/decoupling}
\section{Specification Language Server Protocol}
\label{sec:slsp}
\input{sections/slsp}
\section{Pilot Study}
\label{sec:pilotStudy}
\i... |
1,314,259,996,292 | arxiv | \subsubsection{\@startsection{subsubsection}{3}{\z@
{0.5\@bls plus .3\@bls minus .1\@bls
{0.5em\@afterindentfalse
{\sagesf\normalsize\itshape}}
\makeatother
\begin{document}
\runninghead{A. Lindmark et al.}
\title{Sensitivity analysis for unobserved confounding of direct and indirect effects using uncertainty ... |
1,314,259,996,293 | arxiv | \section{Preliminaries in Teichm\"uller theory}\label{sec:prelim}
\subsection*{Teichm\"uller space}~\cite{Gardiner:Lakic:book},~\cite{Hubbard:book:T1}
Let $\Sigma_{g,n}$ be a connected, oriented surface of genus $g$ and
$n$ punctures and ${\mathcal T}_{g,n}$ denote the Teichm\"uller space of Riemann
surfaces marked by ... |
1,314,259,996,294 | arxiv | \section{Introduction}
Black $p$-brane solutions of type II supergravity carrying
Ramond-Ramond (RR) charges have been known since the early 90's
\cite{Horowitz-strominger,Duff-Lu}. The string frame metric and dilaton
backgrounds in such solutions may be expressed in the following simple
form:
\begin{equation}
\labe... |
1,314,259,996,295 | arxiv | \section{Introduction and the model}
The spin excitations in isotropic Heisenberg models with long-range N\'eel order are well understood within the framework of the spin-wave theory, even in the extreme quantum spin-1/2 case on the square lattice, as exemplified by La$_2$CuO$_4$.\cite{INS_LaCu2O4_2001,INS_LaCu2O4_201... |
1,314,259,996,296 | arxiv | \section{Introduction}
A wireless channel is open to inputs from anybody operating on the same frequency. Therefore communication has to be protected against deliberate jamming. This means that communication protocols have to be devised whose application enables reliable data transmission even if attacked by a jammer.... |
1,314,259,996,297 | arxiv | \section{Introduction}
\begin{center}
\begin{figure}
\includegraphics[scale=0.82]{porta.png}
\caption{Front cover. 1512 edition.}
\vspace*{1cm}
\end{figure}
\begin{figure}
\includegraphics[scale=0.7]{contra.png}
\caption{Table of Contents. 1512 edition.}
\end{figure}
\end{center}
The first edition of Fray Juan de ... |
1,314,259,996,298 | arxiv | \section{Introduction}
In~\cite{EscardoSimpson:UniCCEI}, Escard\'{o} and Simpson prove a universal property for
the real interval $[-1,1]$, using a theory they develop of \emph{midpoint algebras}:
sets equipped with a binary operation that, abstractly, provides the midpoint of any two elements.
In an \emph{iterativ... |
1,314,259,996,299 | arxiv | \section{Introduction}
In this article we review the literature on lattice simulations for few- and
many-body systems. \ We discuss methods which combine effective field theory
with lattice methods and which can be applied to both cold atomic systems and
low-energy nuclear physics. \ Several recent reviews have alread... |
1,314,259,996,300 | arxiv | \section{Introduction}
The {\small EINSTEIN}, {\small EXOSAT} and {\small ROSAT}
observatories measured surface temperatures of certain neutron
stars and put upper limits on the surface temperatures of others (
cf. Ref.~\cite{steuk} and further references therein). Data on the
supernova remnants in 3C58, the Crab, and... |
1,314,259,996,301 | arxiv | \section{Introduction and preliminaries}
Let $\A$ denote the family of analytic functions $f$ of the form
\beq\label{inteq0}
f(z)= z+\sum_{n=2}^{\infty}\, a_n\,z^n
\eeq with $f(0)=0$ and $f^{\prime}(0)=1$ in the open unit disc $\D =\{z:\, |z|<1\}$ of the complex plane.\\
Let us denote by $\es,$ the class of al... |
1,314,259,996,302 | arxiv | \section{Introduction}
One of the most fundamental discoveries in observational cosmology showed that the universe is not only expanding but it does at an accelerated rate \cite{nature}. As the source of this expanded acceleration remains unknown, several candidates have been proposed to account for it. They include,... |
1,314,259,996,303 | arxiv | \section{Introduction}
The effective field theory approach, {\em i.e.}~the description of a system through the lowest dimension operators compatible with the underlying symmetries, has been very fruitful in many areas, from particle physics to condensed matter. The purpose of this paper is to apply this methodology to ... |
1,314,259,996,304 | arxiv | \section{Introduction}
Given a group $G$ and a symmetric generating set $S \subseteq G\setminus\{1\}$, the Cayley graph $\unCayley{G}{S}$ is the simple unoriented graph with vertex set $G$ and an edge between $g$ and $h$ precisely when $g^{-1}h \in S$. By construction, the action by left-multiplication of $G$ on itself... |
1,314,259,996,305 | arxiv | \section{Introduction}
Suppose a matrix $D\in\mathbb{R}^{m\times n}$ is of the form $D = L^0 + S^0$,
where $L^0$ is a low-rank matrix, i.e. $\mathop{\bf rank}(L^0)\ll\min\{m,n\}$, and
$S^0$ is a sparse matrix. The matrix $S^0$ is interpreted as
gross errors in the measurement of the low rank matrix $L^0$. Wright et al... |
1,314,259,996,306 | arxiv | \section{Introduction}
Critical gravity was introduced in \cite{PopeLu1} where the following four-dimensional action was considered:
\beq
S=\dfrac{1}{2\kappa^2}\int \sqrt{-g}\,d^4x \,(R-2\Lambda + b_1\, R_{\mu\nu}R^{\mu\nu} + b_2\,R^2)
\eeq{S1}
where $R$ is the Ricci scalar, $\Lambda$ the cosmological constant,... |
1,314,259,996,307 | arxiv | \section{Introduction}
\label{introduction}
Natural Language Inference (NLI) is the problem of categorizing a hypothesis into entailment, contradiction, or neutral based on the given premise \cite{DBLP:series/synthesis/2013Dagan}. Large language models such as BERT \cite{devlin-etal-2019-bert}, RoBERTa \cite{DBLP:jour... |
1,314,259,996,308 | arxiv | \section{Our Model}
In this section, we will describe our proposed Influence Self-embedding for Heterogeneous Network Embedding framework.
The basic idea of ISHNE is to project every node into different meta-path based embedding space.
To achieve this, local proximities and individual influence of each node are calc... |
1,314,259,996,309 | arxiv | \section{Introduction}
Sustainable Development (SD)
is an interdisciplinary field which studies the integration and balancing of economic, environmental and social concerns to tackle the broad goal of achieving inclusive and sustainable growth~\cite{brundtland1987our,keeble1988brundtland,sachs2015age}.
As a collective... |
1,314,259,996,310 | arxiv | \section{Introduction}
\label{sec:intro}
This paper considers \emph{Imitation Learning from Observation Alone (ILFO)}. In ILFO, the learner is presented with sequences of states encountered by the expert, {\em without} access to the actions taken by the expert, meaning approaches based on a reduction to supervised lea... |
1,314,259,996,311 | arxiv |
\section{Introduction}
\label{sec:intro}
Granular materials have been paid more and more attention recently, such as sand, grains, snow, et al. Compared to the molecular particles modeled with elastic collision, the granular gases behave quite differently due to the energy dissipation during collisions. Therefore, mo... |
1,314,259,996,312 | arxiv | \section{Introduction}
Active matter refers to a class of non-equilibrium systems in which individual particles are self-propelled due to an irreversible consumption of energy. Their physics is relevant to systems ranging from biological to man-made materials~\cite{vicsek2012collective,romanczuk2012active,marchetti_hy... |
1,314,259,996,313 | arxiv | \section{Introduction}
Radio polarisation observations of gravitational lenses provide
important information about the properties of the lens as well as the
background radio source. Such observations give two measurable
quantities -- the degree and position angle (PA) of polarisation. Both
are unaffected by the gravi... |
1,314,259,996,314 | arxiv |
\subsection{Higgs boson mass spectrum}
\label{subsec:MHiggsCalc}
One of the main purposes of \FH is to provide predictions for the Higgs-boson
masses in the~MSSM. The most direct approach is to calculate
higher-order corrections to the propagators of the Higgs bosons
performing a fixed-order Feynman-diagrammatic ca... |
1,314,259,996,315 | arxiv | \section{INTRODUCTION}
The spectrum of excited nucleon states reflects the dynamics of QCD in the non-perturbative regime. It has been studied for many years using $\pi$ beams. However, the spectrum of known nucleon resonances is in conflict with predictions from quark models \cite{isgur77,loring01}. Most obvious is th... |
1,314,259,996,316 | arxiv | \section{Introduction}\label{sec_intro}
Hydro power plants generate electricity from potential energy and
kinetic energy of natural water, and often a number of power plants
are placed along a long river or a water body system to generate the
power at different stages. Currently, hydro power is one of the most
importa... |
1,314,259,996,317 | arxiv | \section{Introduction}
The LMC has a rich star cluster system spanning a wide range of ages and masses.
One striking feature of the LMC cluster system is the existence of an age gap
between 3-10 Gyrs. Four LMC clusters whose integrated colours are consistent with
those of intermediate age simple stellar populations... |
1,314,259,996,318 | arxiv |
\section{Analyzing Image Quality Factors}
\label{sec:quality_analysis}
\subsection{Experiment Setup}
\label{sec:experiment_setup}
\modified{\textbf{Base Dataset}. Our base dataset consists of three real-world driving datasets: Audi~\citep{geyer2020a2d2}, Honda~\citep{ramanishka2018toward}, and SullyChen~\citep{... |
1,314,259,996,319 | arxiv | \section*{Introduction}
Let an algebraic torus $T$
act on a normal, algebraic
variety $X$.
It is an open problem in Geometric
Invariant Theory to describe
the collection of all $T$-invariant
open subsets $U \subseteq X$ admitting
a geometric quotient $U \to U/T$
with a complete orbit variety $U/T$.
Several construc... |
1,314,259,996,320 | arxiv | \section*{}
\vspace{-1cm}
\footnotetext{\emph{$^{a}$ Center for Free-Electron Laser Science, Deutsches Elektronen-Synchrotron
DESY, 22607 Hamburg, Germany}}%
\footnotetext{\emph{$^{b}$ Center for Ultrafast Imaging, Universität Hamburg, 22761 Hamburg,
Germany}}%
\footnotetext{\emph{$^{c}$ Department of Phys... |
1,314,259,996,321 | arxiv | \section{Introduction}
Turbulence is the most common fluid state of motion
and is inherent in a large number of natural and physical
phenomena. The physics of turbulence can be modelled
mathematically by the Navier-Stokes (NS) equations under the
continuum limit. These equations are highly non-local and
non-linear and ... |
1,314,259,996,322 | arxiv | \section{Introduction}
\label{sec:intro}
The Clifford group and the closely associated stabilizer formalism \cite{Gottesman97:thesis,Gottesman98} are a central notion in quantum computation and many related areas.
The Clifford group on $n$ qubits is defined as the normalizer of the $n$-qubit Pauli (aka discrete Weyl) ... |
1,314,259,996,323 | arxiv | \section{Introduction}
Bone is a complex tissue that is being repaired and rebuilt continuously throughout an individual's life. The process of bone remodeling consists of two subprocesses: the resorption of old bone and the formation of new bone.
In the past decades it has become clear that, at the cellular level, bon... |
1,314,259,996,324 | arxiv | \section{Introduction}
In 1986, Celis {\it{et al}} \cite{CelisT,Celis} introduced the Robin Hood collision resolution strategy for open addressing hash tables. Under this discipline, collisions are decided in favor of the element that is farthest from its home location.
While this does not change the expected search c... |
1,314,259,996,325 | arxiv | \section*{Methods}
\noindent\textbf{Sample Selection}
The {\it low-resolution sample} is selected from a comprehensive sample of common sources of LAMOST and KIC. The total amount of common giant stars between this two datasets is $\sim 42,000$. Among those common sources, about $80\,\%$ are observed in an intense ... |
1,314,259,996,326 | arxiv | \section{Introduction}
Constrained learning is ubiquitous in statistical tasks when seeking to impose desired structure on solutions. Concretely, consider the task of estimating a parameter $\bx\in\bbR^d$ by minimizing some loss function $f(\bx)$ where $\bx$ needs to satisfy a set of constraints encoded by a set $\cal... |
1,314,259,996,327 | arxiv | \section{Introduction}
\label{Int}
\onehalfspacing
The Consistent Histories (CH) framework provides a formulation of quantum mechanics that assigns probabilities to histories of all kinds of systems, microscopic and macroscopic, using a single universal machinery and without ``Heisenberg cuts'' or references to measure... |
1,314,259,996,328 | arxiv | \subsection{Data}
We train our model using high-fidelity DNS data of a three-dimensional, statistically stationary, isotropic turbulent flow with Taylor-Reynolds number $R_\lambda = 90$, solved on a cubic domain with $128$ grid points in each direction. More details on the DNS can be found in our previous works (\ci... |
1,314,259,996,329 | arxiv | \section{Introduction}
Many Dark Matter direct detection experiments aim to observe Dark Matter (DM) through an excess of nuclear recoils (NRs) caused by Weakly Interacting Massive Particles (WIMPs) scattering off nuclei from a target material~\citep{Drukier:1984vhf, Goodman:1984dc, Drukier:1986tm,Billard:2021uyg}... |
1,314,259,996,330 | arxiv | \section{Introduction}
Hamilton decomposability of line graphs has been studied extensively. The {\em line graph} of a graph $G$, denoted by $L(G)$, is the graph with a vertex corresponding to each edge of $G$, and in which two vertices are adjacent if and only if their corresponding edges are adjacent in $G$. A {\em ... |
1,314,259,996,331 | arxiv | \section{Introduction}
Palatini formalism is causing great interest in the study of
non-perturbative quantum gravity\cite{Ash}\cite{romano}\cite{AL},
modified gravity theories\cite{Fla}\cite{Vol} and their
cosmological applications\cite{MW}\cite{Kre}. Also, spacetime
reduction is very important in any high dimensional ... |
1,314,259,996,332 | arxiv | \section{Introduction}
Within the past twenty years, many different declarative semantics for logic
programs with negation have been developed. Different perspectives on the
question what properties a semantics should foremost satisfy, have led to a
variety of diverse proposals. From a knowledge representation and rea... |
1,314,259,996,333 | arxiv | \section{Introduction}
We are currently witnessing the beginning of a new era in gravitational physics ignited by the consolidation of multimessenger astronomy, namely, astronomy with different carriers: electromagnetic radiation (now including shadows), gravitational waves, neutrinos and cosmic rays. The fields of gr... |
1,314,259,996,334 | arxiv | \section*{Introduction}
There is assuredly a long tradition of scholarship in the description of sex roles on mass media of various types: already in her seminal review, Linda \cite{busby1975sex} described how instructional material, TV, films, advertising, newspaper, cartoons and literature have been used since the l... |
1,314,259,996,335 | arxiv | \section{Introduction}
\IEEEPARstart{M}{odern} distribution grids are characterized by the rapidly increasing penetration of DERs, especially photovoltaics (PVs) and battery storage systems. Reverse power flows and a greater ratio of fluctuating generation at the local level require the real-time efficient and secure ... |
1,314,259,996,336 | arxiv | \section{Introduction}
The study of the equilibrium shapes and the corresponding excitation
spectra of atomic nuclei is one of the recurrent themes in nuclear
structure physics. Most of the deformed medium-heavy and heavy nuclei
exhibit reflection-symmetric ground states. However, in some regions
of the nuclear ... |
1,314,259,996,337 | arxiv | \section{Introduction}\label{sec:INTRODUCTION}
\subsection{Background and motivation}
A canonical setup for parallel-server systems consists of $N$ identical servers, each with a dedicated queue.
Tasks arrive into the system as a Poisson process of rate $\lambda(N)$ and must be assigned to one of the queues instantan... |
1,314,259,996,338 | arxiv | \section{ Definitions. Notations. Previous results. Statement of problem.}
\vspace{4mm}
\ Let $ \ (\Omega, \ B, \ {\bf P} ) \ $ be certain probability space with non - trivial probability measure $ \ {\bf P} \ $ and
correspondent expectation $ \ {\bf E}, \ $ and let $ \ \xi = \xi(\omega), \ \omega \in ... |
1,314,259,996,339 | arxiv |
\section{Introduction} \label{sec:intro}
Due to their ability to represent complex functions, neural networks are well-suited to perform control tasks in complicated and high-dimensional problem settings \cite{mnih2015human, pan2017agile}. Proposed autonomous aviation systems, for instance, use neural netw... |
1,314,259,996,340 | arxiv | \section{Introduction}\label{sec:s1}
High quality denoising is one of the main challenges in image processing. It tries to achieve suppression of noise while capturing and preserving edges and fine structures in the image. A huge number of publications related to a variety of denoising\ methods (see, for example the r... |
1,314,259,996,341 | arxiv | \section{Introduction}
Deep convolutional neural networks (ConvNets)~\citep{He2015a,Xie2016c,Redmon2016,He2017} have demonstrated excellent performance across a broad spectrum of computer vision tasks, such as image classification~\citep{He2015a}, semantic segmentation~\citep{Ronneberger2015,Chen2014}, image restorati... |
1,314,259,996,342 | arxiv | \section{Introduction}
Electron and photon triggers play an essential role at the LHC. They select, for example, events containing $W \rightarrow e\nu$ and $Z \rightarrow ee$ decays, processes that are important on their own right to test the Standard Model and to calibrate the experimental apparatus but can also be p... |
1,314,259,996,343 | arxiv |
\section{Introduction}
Quantitative assessment of brain tumors provides valuable information and therefore constitutes an essential part of diagnostic procedures. Automatic segmentation is attractive in this context, as it allows for faster, more objective and potentially more accurate description of relevant tumor p... |
1,314,259,996,344 | arxiv | \section{Introduction}
\label{intro}
Searching for DAMA with WIMP is an interesting question from both theoretical \cite{jung}
and experimental sides.
A considerable experimental work are in progress to measure DAMA-nucleus interaction
in differe... |
1,314,259,996,345 | arxiv | \section{Introduction}
The interaction of the $\Sigma$ hyperon with nuclear matter may be
represented by the complex single particle (s.p.) optical model
potential $U_\Sigma=V_\Sigma-iW_\Sigma$. In this paper we present
our attempts to determine $V_\Sigma$ and $W_\Sigma$. We also point
out the most realistic two-body ... |
1,314,259,996,346 | arxiv | \section{\textbf{Introduction}}
All rings considered in this paper will be commutative and
Noetherian and will have non-zero identities; $R$ will always
denote such a ring. The Cousin complex is an effective tool in
commutative algebra and algebraic geometry. The commutative
algebra analogue of the Cousin complex of \... |
1,314,259,996,347 | arxiv | \section{Introduction}
The equations of motion of a nonspinning test particle around a Kerr black hole are fully integrable because of the existence of four conserved quantities: rest mass, energy, angular momentum and the Carter constant \cite{carter68}. The axisymmetry of spacetime drives the geodesic orbits to fill... |
1,314,259,996,348 | arxiv | \section{Motivation}
Interests in machine learning (ML) and deep learning (DL) have been increasing in recent years. Similarly, the number of learning resources, including textbooks, blogs, online courses, and video tutorials, is growing rapidly as well. This is a great development, and one might say that getting into... |
1,314,259,996,349 | arxiv |
\section{Introduction}
\subsection{A class of continuous optimization problems}
Many tasks particularly in low-level computer vision can be formulated as optimization problems over mappings $u : \Omega \to \Gamma$ between sets $\Omega$ and $\Gamma$.
The energy functional is usually designed in such a way that the mi... |
1,314,259,996,350 | arxiv | \section{Introduction}
The project which we initiated eighteen months ago to study
the gluon excitations of the QCD vacuum in the presence
of a static quark-antiquark source has two distinct goals.
Our first objective
was to determine the spectrum of hybrid $\mathrm c\bar c g$
and $\mathrm b\bar b g$ states with
resul... |
1,314,259,996,351 | arxiv | \subsection{0pt}{12pt plus 4pt minus 2pt}{4pt plus 2pt minus 2pt}
\begin{document}
\maketitle
\begin{abstract}
How we choose to represent our data has a fundamental impact on our ability to subsequently extract information from them. Machine learning promises to automatically determine efficient representations from ... |
1,314,259,996,352 | arxiv | \section{Conclusion}\label{sec:conclusion}
In this paper, we have studied the problem of finding similar documents with respect to technical content. To do that, we proposed a hybrid approach which employs the graph representation techniques and sentence embedding. Using the graph-of-words representation of a document ... |
1,314,259,996,353 | arxiv | \section{Supplementary Information}
The supporting information contains all tabulated results, \gls{ML} model and compute details, \gls{DFT} calculation details, details on the relaxation constraints, inflated \gls{ML} success rates, model constraint counts, and additional results on configuration analysis and random b... |
1,314,259,996,354 | arxiv | \section{Introduction}
A {\em proper $k$-coloring}, or simply $k$-{\em coloring}, of a graph $G = (V, E)$ is a function $f:V \rightarrow \{1,2,\dots,k\}$
such that for each $uv \in E$, $f(u) \neq f(v)$.
A graph $G$ is $k$-{\em colorable} if there exists a $k$-coloring of $G$.
The {\em chromatic number}, $\chi(G)$, of ... |
1,314,259,996,355 | arxiv | \section{Hyperparameters in Algorithm~\ref{alg:vomps}}
Hyper-parameters are presented below in the order of four main components--- updating the critic, the density ratio, the emphatic weights, and the actor. $\alpha_{\nu} \in [0,1]$ is the stepsize in the critic update; $\alpha_{\psi} \in [0,1]$ is the stepsize in the... |
1,314,259,996,356 | arxiv | \section{Introduction}
Capacities (non-additive measures, fuzzy measures) were introduced by Choquet in \cite{Ch} as a natural generalization of additive measures. They found numerous applications (see for example \cite{EK},\cite{Gil},\cite{Sch}). Capacities on compacta were considered in \cite{Lin} where the importan... |
1,314,259,996,357 | arxiv | \section{Introduction}
Quantum algorithms for optimization are of general interest. On the one hand, optimization algorithms have wide applications in machine learning, signal processing, combinatorial optimization, and many other areas. On the other hand, it is crucial in quantum computing research to figure out the ... |
1,314,259,996,358 | arxiv | \section{Introduction}
\label{S:1}
The triboelectric effect or contact electrification is an experimentally proven phenomenon \cite{Sow2012}. Its occurrence in conducting materials can be explained by electron transfer resulting from the difference in work functions or Fermi levels of the contacting metals. That is, el... |
1,314,259,996,359 | arxiv | \section{Introduction}\label{sec:intro}
The idea that reaction-diffusion phenomena is essential to the growth of living organisms seems quite intuitive. Indeed, it would be rather hard to envision how any organism could grow and operate without moving its constituents around and using them in various bio-chemical reac... |
1,314,259,996,360 | arxiv | \section{Introduction} \label{S1}
In contrast to young open clusters and star-forming regions, which have been proved to be simple stellar populations \citep[SSPs. e.g.,][]{deSi09a,Brag12a,Brag14a,Ting12a,Kos21a}, most globular clusters (GCs) and some intermediate-age clusters (older than $\geq$2 Gyr) are multiple stel... |
1,314,259,996,361 | arxiv | \section{Introduction}
With the constantly growing mobile data demand for future wireless communication systems, i.e., 5th Generation (5G), it becomes more and more difficult to allocate a wide and contiguous frequency band to each user equipment (UE) and base station (BS). This has brought about increasing scarcity i... |
1,314,259,996,362 | arxiv | \section{Introduction }
\setcounter{equation}{0}
Modern harmonic analysis was introduced in the '50s, with the
Calder\'on--Zygmund theory at the heart of it. This theory
established criteria for singular integral operators to be
bounded on different scales of function spaces, especially the
Lebesgue spaces $L^p$, $1 ... |
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