uuid int64 541B 3,299B | dataset stringclasses 1
value | text stringlengths 1 4.29M |
|---|---|---|
541,165,882,956 | arxiv | \section{Introduction}
We denote by $\mathbb{C}^{+}=\{x+iy:y>0\}$ the upper half of the
complex plane $\mathbb{C}$, and by $H_{\mathbb{C}^{+}}^{2}$ the
corresponding Hardy space. Thus, an analytic function $u:\mathbb{C}^{+}\to\mathbb{C}$
belongs to $H_{\mathbb{C}^{+}}^{2}$ when\[
\|u\|_{2}^{2}=\sup_{y>0}\int_{-\infty}... |
541,165,882,957 | arxiv | \section{Introduction}
In a number of modern scenarios (e.g., social network analysis, online
finance, online transaction processing, etc.), data are produced as a
continuous stream, and at such a high rate that on-the-fly processing
can only afford to maintain a small portion of the data in memory,
together with a lim... |
541,165,882,958 | arxiv | \section{Proofs for Section \ref{sec:binary-attack}}
\label{apdx:binary-attack}
In this section, we prove the key technical claim from Section \ref{sec:binary-attack}. Let $p(m,n)=\half + \frac{m}{2n} + \sqrt{\frac{1}{2n} \ln 6}$
\begin{clm}[Claim \ref{clm:similar-binomials}, restated]
\label{clm:similar-binomials-apd... |
541,165,882,959 | arxiv | \section{Introduction}
The construction of bipartite graphs with prescribed degrees is a well-studied algorithmic problem with various applications in science.
Whereas the classical problem asks for a bipartite graph whose degrees must \emph{exactly} match prescribed integers, we study the problem of constructing a bi... |
541,165,882,960 | arxiv | \section{Introduction}
Since the Diffusion Limited Aggregation (DLA) was introduced in 1981
by Witten and Sander~\cite{ws}, an enormous literature has been
devoted to it. Its paradigmatic role, concerning a variety of pattern
formations in far-from equilibrium processes, such as DBM~\cite{np},
viscous fingering~\cite... |
541,165,882,961 | arxiv | \section{Introduction}
Recent decades have witnessed the sucess of applying deep learning techniques in many domains given that deep learning strategies could effectively extract the latent information from data and efficiently capture the hidden patterns of data, no matter it is textual data or image data \cite{brons... |
541,165,882,962 | arxiv | \section{Introduction}
\IEEEPARstart{G}{oppa} constructed error-correcting linear codes by using tools from Algebraic Geometry: a non-singular, projective, geometrically irreducible, algebraic curve $\mathcal{X}$ of genus $g$ defined over $\mathbb{F}_{q}$, the finite field with $q$ elements, and two rational divisors ... |
541,165,882,963 | arxiv | \section{Introduction}
Ge/GeSi multiple quantum wells (MQWs) have attracted great interest for Si-based photonic devices since the demonstration of quantum confined Stark effect (QCSE) at room temperature (RT)\cite{kuo}. Optical modulators \cite{paul,schaevitz,morini,chaisakulsse,lever}, photodetectors\cite{fidaner,ona... |
541,165,882,964 | arxiv | \section{0pt}{12pt plus 4pt minus 2pt}{0pt plus 2pt minus 2pt}
\titlespacing\subsection{0pt}{12pt plus 4pt minus 2pt}{0pt plus 2pt minus 2pt}
\titlespacing\subsubsection{0pt}{12pt plus 4pt minus 2pt}{0pt plus 2pt minus 2pt}
\begin{document}
\title{Blockchain Interoperability Landscape
}
\author{\IEEEauthorblockN{In... |
541,165,882,965 | arxiv | \section{} \fancyhead[ER]{\large{\thesection. \textsc{}}}
\theoremstyle{definition}
\newtheorem{mydef}{Definition}[subsection]
\newtheorem{rem1}[mydef]{Remark}
\theoremstyle{plain}
\newtheorem{prop}[mydef]{Proposition}
\newtheorem{lem}[mydef]{Lemma}
\newtheorem{cor}[mydef]{Corollary}
\newtheorem{thm}[myde... |
541,165,882,966 | arxiv |
\subsection{A Study Inspired by ``Don't Replicate the Real World''}
\label{sec:Konstanz}
In May 2018, as part of literature research for a PhD project, \textbf{matthias.kraus} initiated a new thread ``(Don't / Do) Replicate the Real World in VR?'' \cite{kraus:2018:VisGuides}. The discussion focused on the visualizatio... |
541,165,882,967 | arxiv | \section{Introduction}
Analyzing the raw data, which comes pouring out of the $LHC$,
presents a challenge of considerable proportions, given that the
dynamics of the true players in the hadronic inelastic collisions,
i.e. partons, are shadowed bye the laws of strong interactions.
However, to understand the nature of ou... |
541,165,882,968 | arxiv | \section{Introduction}
Recently, much interest is devoted to the question of a possible
enhancement of direct CP-violation effects in \(K^\pm \to 3\pi\){} decays first
proposed in \cite{pl2}. In this paper from chiral Lagrangians with
fourth-order derivative terms, including meson loop rescattering
effects, the CP-... |
541,165,882,969 | arxiv | \section{Introduction}
\begin{figure*}[tbh]
\centerline{\psfig{file=f1.ps,width=6.0in,angle=270}}
\caption{\small
Six different views of the SMM\,J14011 system. The top row comprises
(starting at the left): a true-color image of the galaxy produced from
the R$_{702}$JK imaging; the WFPC2 R$_{702}$ image with the var... |
541,165,882,970 | arxiv | \section*{Acknowledgments}
The author is thankful to the anonymous referee whose advices helped to improve the overall presentation of the work.
\section*{Funding}
The reported study was funded by RFBR according to the research project \textnumero~20-31-90008; by a grant in the subsidies form from the federal budget ... |
541,165,882,971 | arxiv | \section{Introduction}
Interface phenomena related to the superconductivity constitute a rich field of condensed matter physics. When superconductor is attached to normal metal, Cooper pairs penetrate into the normal metal which acquires superconducting correlation. This is called the proximity effect. As a result, fo... |
541,165,882,972 | arxiv |
\section{Introduction}
Understanding charmonium production in hadronic collisions is a
challenge for quantum chromodynamics (QCD). The \JPsi production cross section
measurements at the Tevatron~\cite{cdf:jpsi,cdf:jpsi2} were found to
disagree by about a factor of 50 with theoretical color-singlet calculations~\cite{... |
541,165,882,973 | arxiv | \section{Introduction}
Light from distant galaxies is gravitationally lensed as a result of
mass perturbations along the line of sight. In the weak-field regime, away from the critical curve of the lensing mass,
the effect is to change the observed projected ellipticity
of light bundles, called shear, caused by the
t... |
541,165,882,974 | arxiv | \section{Summary}\label{sec:conclusions}
\edit{We investigated 11 binary star systems with detected planets in circumstellar (S-type) motion, and we calculated the location and extent of the habitable zone for these systems.} In most cases the presence of yet undetected Earth-mass planets cannot be ruled out. Using th... |
541,165,882,975 | arxiv | \section{Related Work}
\label{related_work}
Traditional lossy image compression techniques (JPEG, JPEG2000 (JP2)) combine fixed transformation entropy-based encodings with optimized bit allocation in order to achieve better compression at low bit rates \cite{takamura1994coding}. As a result, these approaches are often ... |
541,165,882,976 | arxiv | \section{Introduction}
\label{sec:intro}
Ultra High Energy Cosmic Rays (UHECR), namely Cosmic Rays with energies larger than $10^{17}\div 10^{18}$ eV, are the most energetic particles observed in nature, with energies exceeding $10^{20}$ eV. The first observation of particles with such extreme energies dates back to t... |
541,165,882,977 | arxiv | \section{Introduction}
Symbiotic stars (SySt) are interacting binaries with the longest orbital periods. In these systems an evolved, cool star is transferring mass to a much hotter, and more luminous compact companion. The mass accretor is typically a white dwarf (WD), but in some cases a neutron star (NS) is observed... |
541,165,882,978 | arxiv | \section{Introduction}\label{intro}
Idempotent states on locally compact quantum groups have been investigated in a number of papers, e.g.~\cite{Pal,FrSk09-1,FrSk09-2,BFS,SaSk12,FST,Salmi,SaSk,KK,FK}. The main idea behind these investigations was based on the classical result of Kawada and It\^o which establishes a bi... |
541,165,882,979 | arxiv | \section{Introduction}
\input{Files/intro}
\section{Preliminaries}
\input{Files/prelims}
\section{Main Approach}
To recover the underlying graph, we will show how to reconstruct the neighborhood of each vertex by solving a convex constrained minimization problem. We will first describe the optimization problem and th... |
541,165,882,980 | arxiv | \section{Introduction}
In this paper is considered the following {\sc Cusa}-{\sc Huygens} inequality
\begin{equation}
\label{Cusa-Huygens}
\frac{3\sin x}{2+\cos x}
<
x
<
\displaystyle\frac{2}{3} \sin x + \displaystyle\frac{1}{3} \tan x,
\end{equation}
for $x \!\in\! \left( 0, \nfrac{\pi}{2} \right)$, as sho... |
541,165,882,981 | arxiv | \section{Introduction}
The imaging of systems of nanometer size is of great importance for many
branches in biological, chemical and physical sciences. The laws of wave optics
demand the usage of wavelengths in the x-ray regime. However, the large energy
carried by each photon rapidly damages such delicate
samples ... |
541,165,882,982 | arxiv | \section*{Introduction}
In this paper we give an account of some results on \emph{topological
Andr\'e-Quillen homology} and \emph{cohomology} for CW commutative
$A$-algebras, where $A$ is a commutative $S$-algebra. The main goal
is to develop arguments based on skeletal filtrations with a view
to continuing the work b... |
541,165,882,983 | arxiv | \section*{Acknowledgement}
This work was partly supported by the EFree, an Energy Frontier Research Center funded by the U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences under Award Number DE-SC0001057 and partly by the Office of Naval Research No. N00014-07-1-0451.
|
541,165,882,984 | arxiv | \section{Introduction}
It has been proposed that an isolated quantum many-body system with a few local conservation laws can still thermalize, in the sense that local observables approach their thermal
equilibrium values \cite{Deutsch:1991,Srednicki:1994,Rigol:2008} set by conserved quantities. Quantum many-body system... |
541,165,882,985 | arxiv | \section{Introduction}
Direct numerical calculations of non-integrable quantum many-body problems become exponentially difficult for large number of particles. The developing of approximate statistical description of such models has been and remain thus of great importance.
For macroscopic bodies the number of inte... |
541,165,882,986 | arxiv | \section{Introduction}
In the analysis of superselection sectors, the localisability
properties of charges are crucial for defining notions as charge
composition and conjugation, statistics or a (global) gauge group. In
a classical work \cite{DHR}, Doplicher, Haag and Roberts carried
through such a programme for charge... |
541,165,882,987 | arxiv | \section{Introduction}
Video stabilization methods aim at removing unwanted shaky motions of a video caused by unsteady moving capture~\cite{guilluy2021video}. There are three main steps: 1) camera motion estimating for trajectory recovery; 2) camera path smoothing; and 3) steady frame synthesize. For the first step, a... |
541,165,882,988 | arxiv | \section{Introduction}
\vspace{-1mm}
Convolutional architectures (CNNs) \cite{he2016deep, tan2019efficientnet} have been dominant in computer vision for a while now. When they were first introduced for large-scale training in image domain, their benefits were quickly realized over Multi-layer Perceptrons (MLPs). In ad... |
541,165,882,989 | arxiv | \section{Introduction.}
In a previous paper \cite{Simple} the BRST quantization on inner product spaces
was considered for
gauge theories with a general Lie group gauge invariance. It
was shown that provided dynamical Lagrange multipliers are introduced the BRST
charge $Q$ may
always be written in the form
\begin{eqna... |
541,165,882,990 | arxiv | \section*{Introduction}
Two (linear) product operations of a certain kind defined on the same vector space are said to be compatible if their linear combinations are still of the same kind. In recent years a lot of studies have been done on various types of compatible algebraic structures, for example, compatible assoc... |
541,165,882,991 | arxiv | \section{INTRODUCTION}\label{intro}
NGC~5506 is a nearby ($z$=0.0062; $\sim 24$\,Mpc) edge-on Sa galaxy within the local Virgo supercluster, hosting an active galactic nucleus (AGN) classified as radio-quiet narrow-line Seyfert I \citep[NLSy1; ][]{2002A&A...391L..21N}. The NLSy1 galaxies generally have lower SMBH ma... |
541,165,882,992 | arxiv | \section{Introduction}
Supernova remnants (SNRs) are among the most exciting astrophysical objects, because they may shed light on a major question of physics: the
origin of cosmic rays. An interesting object in this respect is the remnant of the historical Type Ia event SN~1572, first described by Tycho Brahe.
Due to... |
541,165,882,993 | arxiv | \section*{Highlights}
\begin{itemize}
\item Transforming distribution of synthetic and image data to reference distributions
\item Embedding classes of digit, facial, and histopathology data to desired distributions
\item Manifold embedding of toy and real data to any desired distributions chosen by user
\item Distrib... |
541,165,882,994 | arxiv | \section{Introduction}
In a distributed storage system, we encode and distribute a data file of size $B$ to $n$ storage nodes, with two properties that (i)
any $k$ nodes are sufficient in rebuilding the original file, and (ii) upon the failure of one or more storage nodes, we can recover the lost information efficientl... |
541,165,882,995 | arxiv | \section{Introduction}\label{sec:intro}
Black holes in general relativity never vanish and are eternal. The formalism of quantum field theory in curved spacetime implies however that black holes are complicated entities which emit thermal radiation and have an entropy proportional to the horizon area (Bekenstein-Hawkin... |
541,165,882,996 | arxiv | \section{Introduction}
Missing data are a frequent problem in randomized trials. If the
reasons for outcome missingness and the outcome itself are correlated,
unadjusted estimators of the treatment effect are biased, thus
invalidating the conclusions of the trial. Most methods to mitigate
the bias rely on baseline var... |
541,165,882,997 | arxiv | \section{Introduction}
Ensemble learning has been proven to be theoretically and empirically superior to single models by state-of-the-art literature as a method of combining pre-trained models in a certain way to obtain final predictions \citep[e.g. ][]{brown2005diversity,chandra2006evolving,mendes2012ensemble}.
Typic... |
541,165,882,998 | arxiv | \section{Introduction}
The evolution of wireless communication technology has led to advances in many areas.
Today, 5G has become a key enabler for applications such as virtual reality, vehicle-to-everything communications, massive machine-type communications, etc. The growth in the demand of data rate, reliability... |
541,165,882,999 | arxiv |
\section{Derivation of the formula $\aformula_{\dag}$}
\label{appendix-dag-formula}
\noindent
In this appendix, we explain how to derive the formula $\aformula_{\dag}$
introduced in the proof of Lemma~\ref{lemma:starPSLelim}. As the derivation is rather
complex, we provide it in the appendix with intermediate deriva... |
541,165,883,000 | arxiv | \section{Introduction}
Transition metal based oxide systems with heavier (4$d$ or 5$d$) elements possess strong spin orbit coupling (SOC) and crystal field splitting energy (${\Delta}$) with moderate Coulomb repulsion $U$, and have been at the centerstage of condensed matter physics research for more than a decade now.... |
541,165,883,001 | arxiv | \section{Introduction}
This brief article concerns local approximation results for radial basis function (RBF) approximation with the goal of effectively placing centers at varying resolutions.
We consider RBF approximants of the form
$x\mapsto \sum_{\xi\in\Xi} \phi(x-\xi)$,
where the arrangement of centers, $\Xi$, m... |
541,165,883,002 | arxiv | \section{Introduction}
\bigskip
Cube diagrams are $3$-dimensional representations of knots or links (c.f. \cite{Adam}). A cube diagram is a cubic lattice knot embedded in an $n \times n \times n$ cube in $\mathbb{R}^3$ where each projection to an axis plane ($x = 0$, $y = 0$, and $z = 0$) is a grid diagram. The inte... |
541,165,883,003 | arxiv | \section{Introduction and main results}
\subsection*{Fisher-KPP traveling fronts in homogeneous media}
Traveling front solutions of the reaction-diffusion equation
\begin{equation}\label{apr2801}
u_t=u_{xx}+f(u)
\end{equation}
are used to model phenomena
in a range of applications from biology to social sciences, and... |
541,165,883,004 | arxiv | \section{Introduction}
The main goal of our work is to understand the baryon structure
up to a momentum transfer of $Q^2\approx 1-2$ GeV.
This momentum regime is
particulary interesting because of the interplay between hadronic
degrees of freedom on the one side and their intrinsic quark structure
on the other si... |
541,165,883,005 | arxiv | \section{Introduction}
With advancements in imaging and hardware, machine learning techniques have been well adopted in the medical domain for analysis of highly complex data, however one of the remaining bottlenecks is the task of gathering large volumes of annotated training data.
This is largely due to costs of exp... |
541,165,883,006 | arxiv | \section{Introduction}
The transit and secondary eclipse of an extrasolar planet allow us to
deduce its physical properties to a degree that is not possible in
other observing geometries \citep{charb_ppv}. GJ\,436b \citep{butler}
was recently discovered to be the first transiting Neptune-sized
planet \citep{gillon}, o... |
541,165,883,007 | arxiv | \section{Introduction}
It is a well known fact that the binary encoding is on average optimal for representing integers.
However if we think of a binary string as a computer program, it follows that such a program
implicitly describes a circuit which evaluates to the corresponding integer. When literaly interpreted,
... |
541,165,883,008 | arxiv | \section{Introduction}\label{introduction}
Let $k$ be a field of characteristic zero. Let $R$ be the polynomial ring in $n$ variables over $k$, and let $\widehat{R}$ be the formal power series ring in $n$ variables over $k$. Consider the rings $\mathscr{D} = \mathscr{D}(R,k)$ (resp. $\widehat{\mathscr{D}} = \mathscr{D... |
541,165,883,009 | arxiv | \section{Introduction}
\label{intro}
The astonishing increase of positively diagnosed cases due to COVID-19 has called the
attention of the whole World, including researchers of many areas and governments. It
urges \cite{puevo20} to find explanations for the already known data and models which may
allow us to bette... |
541,165,883,010 | arxiv |
\subsection{Object-level Complexity Factors}
As to a specific object, all its information can be described by appearance and geometry. Therefore we define the below two factors to measure the complexity of appearance and geometry respectively. Notably, both factors are nicely invariant to the object scale.
\begin{it... |
541,165,883,011 | arxiv | \section{Introduction} \label{sec-intro}
\begin{figure}[h]
\begin{center}
\includegraphics[width=2.0in]{what-is.jpg}
\end{center}
\caption{A benzel tiled by (tri)bones.}
\label{fig:what-is}
\end{figure}
This article treats tilings such as the one shown in Figure~\ref{fig:what-is}
in which the tiles are {\em tribones... |
541,165,883,012 | arxiv | \section{Introduction}
Cells can generate temporal patterns of activity by means of genetic oscillations~\cite{goldbeter,mackey}.
Genetic oscillations are biochemical oscillations in the levels of gene products~\cite{liu95,nagoshi04,mihalcescu04,goldbeter12,palmeirim97,aulehla08,masamizu06,krol11,shimojo08,geva06,elow... |
541,165,883,013 | arxiv | \section{Introduction}\label{section1}
In the past years the study of {\it separable systems} (whose Hamilton--Jacobi equations can be integrated by separation of variables) has shown a remarkable development, also in relation with other kinds of integrable systems (bi-Hamiltonian systems, Lax systems). I~think that a... |
541,165,883,014 | arxiv | \section{Introduction}
\approvals{
Daniel & yes \\
Stefan & yes \\
Thomas & yes
}
Given an $n$-dimensional, complex, projective manifold $X$, the notion of
\emph{stability} is arguably the single most important concept in the discussion
of sheaves of $\scr{O}_X$-modules and their moduli. A widely-used stabilit... |
541,165,883,015 | arxiv | \section{Introduction}
Osteoarthritis (OA) is a highly prevalent, degenerative joint disease with a considerable societal and economic impact, in addition to the physical and psychological sequelae it causes in affected individuals.
The pathophysiology of OA involves several tissues and is primarily associated with a ... |
541,165,883,016 | arxiv | \section{Introduction}
Only a small part of the information in natural visual scenes is
consciously accessible following a brief presentation
\cite{Simons2000,Rensink2000}. The information that is retained
depends on what is attended \cite{CognNeuroBook}. The neural
correlates of selective attention have been stud... |
541,165,883,017 | arxiv | \section*{INTRODUCTION}
Inclusive and Semi-Inclusive Deep Inelastic Scattering (DIS and SIDIS) processes
are important tools to
understand the structure of nucleons and nuclei. Spin asymmetries in polarized
SIDIS are directly
related to Transverse Momentum Dependent (TMD) parton distribution and
fragmentation function... |
541,165,883,018 | arxiv | \section{Introduction}
It is well known that when a liquid is disturbed suddenly from its equilibrium
state by changing the temperature or pressure of the surrounding medium, or
both, then the liquid undergoes a rapid, solidlike change, followed by a
slower, liquidlike change towards the new equilibrium state. These c... |
541,165,883,019 | arxiv | \section{Introduction}
The main goal of the ultra-relativistic nucleus-nucleus (AA) collisions programme
is to create in terrestrial laboratories a new state of matter, the Quark-Gluon
Plasma (QGP). The existence of this phase, where quarks and gluons are deconfined,
i.e. can freely move over several hadronic dista... |
541,165,883,020 | arxiv | \section{Introduction}
\label{sec:intro}
In the scenario of emergent spacetime \cite{ref:emergent1,ref:emergent2,ref:emergent3,ref:emergent4,ref:emergent5,ref:emergent6,Ambjorn:2010rx},
the notions of spacetime and distance are not fundamental, but they are just infrared phenomena which appear only after
underlyin... |
541,165,883,021 | arxiv | \section{Introduction}
One of the most important questions in condensed matter is how the strong
interaction between quasiparticles modify their properties and influence
observable quantities. Non-Fermi-liquid behavior was found in many different
substances, but a class of high-$T_c$ copper oxides attracts special att... |
541,165,883,022 | arxiv | \subsection{Acknowledgments}
Y. M. and Y.-Z. Z. especially thank Prof. Francesco Buscemi for numerous advice and encouragement throughout the project.
We thank Jun Zhang, Wen-Yuan Wang, Yan-Lin Tang, Ping Xu, Leonardo Guerini, and Qinghe Mao for valuable and illuminating discussions.
After submission, we became aware... |
541,165,883,023 | arxiv | \section{Introduction}
\label{sec:intro}
Combinatorial discrepancy theory aims to quantify the following phenomenon: if a hypergraph $\mathcal{H}$ is ``sufficiently rich'', then in every $2$-colouring of the vertices of $\mathcal{H}$ there will be some hyperedge which is unbalanced, namely, has significantly more vert... |
541,165,883,024 | arxiv | \section{Introduction}
A central problem in statistical mechanics and the thermodynamic formalism, is the study of phase transitions.
Here we focus on ``zero-temperature'' phase transitions, or the chaotic dependence of Gibbs states on the temperature parameter as it drops to zero.
In good situations, as in the case o... |
541,165,883,025 | arxiv | \section{Introduction}
\vspace{-3mm}
\label{sec:1}
Video Super-Resolution (VSR) aims to reconstruct a high-resolution visual-pleasing video from a low-resolution one.
Recent years have witnessed significant advances due to the use of deep convolutional neural networks (CNNs).
As more frames are used, VSR methods achi... |
541,165,883,026 | arxiv | \section{Introduction}
\rem{%
\newcounter{thm}
\newcounter{remark}
\newcounter{dfn}
\setcounter{thm}{0}
\setcounter{remark}{0}
\setcounter{dfn}{0}
\refstepcounter{thm}
\refstepcounter{remark}
\refstepcounter{dfn}
}%
\noindent
Hamilton's principle for ideal fluid flow might be summarized by saying that \emph{water... |
541,165,883,027 | arxiv | \section{Introduction}
Rotational evolution of young radio pulsars is usually described in a simplistic way using so-called magneto-dipole formula \citep{magnetodipole}. This description is a zeroth-order approximation at best because it lacks multiple physical effects: (1) a radio pulsar is not a point source (see \c... |
541,165,883,028 | arxiv | \section{Introduction}
Coupling between lattice vibrations and electrons in solids produces a great variety of experimentally observable
effects, usually described as ``the physics of polarons''. Different regimes of this coupling build
weak and strong-coupling polarons influencing carriers mobility, effective masses... |
541,165,883,029 | arxiv | \section{Introduction}
We classify irreducible plane curve singularities $f\in K[[x,y]]$ which are simple with respect to parametrization equivalence, where $K$ is an algebraically closed field of arbitrary characteristic. That is, the irreducible plane singularities whose parametrizations have modality 0 up to the cha... |
541,165,883,030 | arxiv | \section{Introduction}\label{S:intro}
Modern imaging surveys such as the Cosmic Evolution Survey (COSMOS) \citep{Scoville07}) and the Great Observatories Origins Deep Survey (GOODS) \citep{Giavalisco04} contain a wealth of galaxy information in the form of stamp images and multiwavelength photometry across the electr... |
541,165,883,031 | arxiv | \section{Introduction}
Let $\S$ be a genus $g$ surface with $n$ boundary components, and let $X$ be a negatively curved metric on $\S$. Closed geodesics on surfaces have been studied extensively over the years. In this paper, we give upper and lower bounds on the number of closed geodesics on $\S$ given upper bounds o... |
541,165,883,032 | arxiv | \section{Introduction}
Economic entities (EE), being individuals, organizations or countries, need resources (natural resources, services, etc.) in order to sustain their existence and normal activity. Their needs are expressed in terms of requests of a certain amount of a given resource (demands) that are generated a... |
541,165,883,033 | arxiv | \section{Introduction}
\label{sec_intro}
The magnetorotational instability
\citep[MRI;][]{1991ApJ...376..214B,1998RvMP...70....1B}, which
occurs in differentially rotating plasmas threaded by a weak magnetic field, is
believed to explain the long-standing puzzle of the origin of turbulence and angular
momentum transpo... |
541,165,883,034 | arxiv | \section{Introduction}
Defeasible reasoning is a nonmonotonic reasoning \cite{MT93}
approach in which the gaps due to incomplete information are
closed through the use of defeasible rules that are usually
appropriate. Defeasible logics were introduced and developed by
Nute \citeyear{Nute94} over several years. These ... |
541,165,883,035 | arxiv | \section{Introduction}\label{sec:int}
Suppose that $A \in \mathbb{C}^{p\times q}$, then it is well known that
the (ordinary) singular values of $A$ can be obtained from the
eigenvalues of either of the products
\begin{equation}\label{eq:sqSVD}
\mathcal A = A^*\!A
\quad\text{or}\quad
\mathcal A = AA^*,
\end{equa... |
541,165,883,036 | arxiv | \section{Introduction}
\label{sec_introduction}
The investigation of neutron-rich $\Lambda$-hypernuclei is an important subject in hypernuclear physics, because it facilitates the understanding of both the structure of neutron-rich nuclei flavored by the $\Lambda$ hyperon and the $\Lambda N$-$\Sigma N$ mixing effect in... |
541,165,883,037 | arxiv | \section{Introduction}
Recently much attention has been devoted to atomic impurities
embedded in ultra-cold atomic media
because of experimental accessibility of such systems in controlled ways
and of observations of various kinds of quasi-particle properties of the impurities
: bosonic \cite{Catani1,Scelle1,Hohmann1... |
541,165,883,038 | arxiv |
\section*{Acknowledgments}
\label{sec:ack}
\update{Special thanks go to the entire ConFlux team and CloudLab team for making Oort\xspace experiments possible. We would also like to
thank the anonymous reviewers, our shepherd, Gennady Pekhimenko, and SymbioticLab members for their insightful feedback. This work was sup... |
541,165,883,039 | arxiv | \section{Introduction}
Finding a quantum state in agreement with a set of expected values of observables is a common task in quantum information processing. If the set of observables is complete, i.e. forms a basis in the space of density matrices, then the problem reduces to quantum state tomography and it is known t... |
541,165,883,040 | arxiv | \section*{Introduction}
The purpose of this paper is to complete the characterization of irreducible Heegaard splittings of orientable Seifert fibered spaces which was given by Moriah and Schultens in \cite{moriahschultens-seifert} for the totally orientable case to the case of orientable Seifert fibered spaces whose ... |
541,165,883,041 | arxiv | \section{Introduction}
A number of proton-rich nuclei between Se and Hg, the so-called p-nuclei, cannot be produced in the s- and r-processes. The majority of p-nuclei are made in photodisintegration processes
in outer shells of massive stars in the course of the final supernova explosion, the $\gamma$-process. Whethe... |
541,165,883,042 | arxiv | \section{Nos\'e and Nos\'e-Hoover Canonical Dynamics Lack Ergodicity}
In 1984 Shuichi Nos\'e used ``time scaling''\cite{b1,b2} to relate his novel
Hamiltonian ${\cal H}$ to an extended version of Gibbs' canonical phase-space
distribution $f$ , proportional to $e^{-{\cal H}/kT}$ . Hoover's simpler
``Nos\'e-Hoover'' moti... |
541,165,883,043 | arxiv | \section*{Author biographies}
\begin{IEEEbiography}[{\includegraphics[width=1in,height=1.25in,clip,keepaspectratio]{figs/authors/yujisaito_gray.pdf}}]{Yuji Saito} received the B.S. degree in mechanical engineering, and the Ph.D. degree in mechanical space engineering from Hokkaido University, Sapporo, Japan in 2014 an... |
541,165,883,044 | arxiv | \section{Introduction}
\xdef\@thefnmark{}\@footnotetext{\noindent G. Yang and J. Schlemper/D. Rueckert and A. Maier share second/last coauthorship.}
Compressed sensing-based Magnetic Resonance Imaging (CS-MRI) is a promising paradigm allowing to accelerate MRI acquisition by reconstructing images from only a fraction... |
541,165,883,045 | arxiv | \section{Introduction}
As usual, let $(F_n)_{n\ge 0}$ and $(L_n)_{n\ge 0}$ denote the
sequences of Fibonacci and Lucas numbers, respectively, given by
the initial values $F_0=0,~F_1=1,~L_0=2,~L_1=1$, and by the recurrence relations
\begin{equation}\label{erra}
F_{n+2}=F_{n+1}+F_n\qquad {\text{\rm and}}\qquad
L_{n+2}=... |
541,165,883,046 | arxiv | \section{Introduction}
The study of the mechanical properties of nanoscale systems presents new theoretical and experimental challenges \cite{ray,book}. The arrangements of atoms at nano and macro scales can be quite different and affect electronic and mechanical properties. Of particular interest are the structure... |
541,165,883,047 | arxiv | \section{Introduction}
The quantum chromodynamics (QCD) predicts that at high temperature and/or density there is a phase transition from hadron
to quark gluon plasma (QGP). The QGP is generally believed to be produced during the relativistic heavy ion collisions.
In statistical QCD, deconfinement and the properties of... |
541,165,883,048 | arxiv | \section{Introduction}
\label{sec:introduction}
Observations of distant quasars over the past two decades have shown
that supermassive black holes (SMBHs) with masses $\gtrsim10^9\,{\rm M}_{\odot}$
exist at redshift $z\gtrsim 6$
\citep[e.g.,][]{Fan+2001,Mortlock2011,Wu2015,Matsuoka2016,Banados2018,Reed2019,Onoue2019,Y... |
541,165,883,049 | arxiv | \subsection{String Commitment}
Here we take a different approach
and look at the task of committing to a string of $n$ bits at once in the setting
where Alice and Bob have unbounded resources. Since perfect bit commitment is impossible, perfect
string commitment is impossible, too. However, is it
possible to design mea... |
541,165,883,050 | arxiv |
\section{Introduction}
\label{sec-intro}
Relations between topological phases can be established via phase transitions\cite{Bais2009a,Barkeshli2010,Burnell2012,schulz2013,Barkeshli2013a,Eliens2013,Chen2013,Gu2014a,HungWan2015a,Ji2019,Hu2021} and via domain walls\cite{Bais2009,Kitaev2012,Gaiotto2012,HungWan2014,Lan201... |
541,165,883,051 | arxiv | \section{Introduction}
\begin{figure}[ht]
\includegraphics[width=\columnwidth]{joins}
\caption{Sampling strategies for joins: \emph{(Left)} Random Sampling after the join execution provides correct semantics, but the entire relations have to participate in the join. \emph{(Middle)} Works by Chaudhari et al.~... |
541,165,883,052 | arxiv | \section{Introduction}
The direct methanol fuel cell (DMFC) has been proposed as an alternative clean and safe power source, due to the easy transportation and storing of liquid methanol and the corresponding low carbon dioxide emissions of the cell. However, the DMFC has performance inconveniences attributed to the me... |
541,165,883,053 | arxiv | \section{INTRODUCTION}
The top quark, the W-boson and the Higg boson form an
interesting triptych of elementary particles.
In the Standard Model knowing the mass of two of these particles,
usually the top quark and W-boson, we can
predict the mass of the third, the Higgs boson.
Therefore in this proceedings I will pri... |
541,165,883,054 | arxiv | \section{Introduction}
Many problems in astrophysics and space physics require the use of numerical methods -- especially for cases where a direct comparison to observations is desired. This applies particularly to environments that can be described with the help of fluid dynamics. The \textsc{Cronos} code that is desc... |
541,165,883,055 | arxiv | \section{Introduction}\label{intros}
The {\em covering radius} of a subset $C$ of the Hamming cube $\{0,1\}^n$ is the minimum $R$ such that any vector in $\{0,1\}^n$ is within Hamming distance at most $R$
from $C$.
Studying the relation between the covering radius of a binary linear code and its dual co... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.