uuid int64 541B 3,299B | dataset stringclasses 1
value | text stringlengths 1 4.29M |
|---|---|---|
1,116,691,497,515 | arxiv | \section{Introduction}
One of the main ingredients of the direct method of the Calculus of Variations (\cite{DacorognaH}) to show existence of minimizers for an integral functional of the kind
$$
I(\mathbf{u})=\int_\Omega\psi(\nabla \mathbf{u}(\mathbf{x}))\,d\mathbf{x}
$$
is its weak lower semicontinuity. Here $\Omega\... |
1,116,691,497,516 | arxiv | \section{Introduction}
The paper is dedicated to the problem of the existence of
universal acting objects - actors in the category of alternative algebras (see Section \ref{def}
for the definitions). Actions in algebraic categories were
studied in \cite{Ho}, \cite{Mc}, \cite{LS}, \cite{Lu}, \cite{No},
\cite{Lo}, \ci... |
1,116,691,497,517 | arxiv | \section{Introduction}\label{intro}}
\IEEEPARstart{F}ederated learning (FL) \cite{DBLP:conf/aistats/McMahanMRHA17,DBLP:journals/tist/YangLCT19,DBLP:conf/aistats/McMahanMRHA17,DBLP:journals/spm/LiSTS20,DBLP:journals/ftml/KairouzMABBBBCC21,li2021personalized} facilitates collaborative training among a set of clients ... |
1,116,691,497,518 | arxiv | \section*{Acknowledgments}
This research was partially funded by NSF IIS 1910733, DBI 1661375, and IIS-1513616.
We would like to thank Vivek Srikumar for his extremely valuable feedbacks regarding applying {\topoact} to the BERT neural networks.
We also would like to thank Jeff Phillips who forwarded a Twitter me... |
1,116,691,497,519 | arxiv | \section{Introduction}\label{intro}
One of the important task in nuclear and particle physics is
the nonperturbative understanding of
the phase structure of Quantum Chromodynamics (QCD) at
finite temperature ($T$) and real chemical potential $(\mur)$.
However, the confinement-deconfinement transition
has no... |
1,116,691,497,520 | arxiv | \section{Introduction}
Lorentz invariance is one of the pillars of the current theories of fundamental physics. It implements the physical equivalence of inertial
observers in absence of gravity, together with the presence of an invariant scale, the speed of light in vacuum. In particular, Lorentz
symmetry is an impor... |
1,116,691,497,521 | arxiv |
\section{Introduction}
\textit{Online} (also known as \textit{simultaneous}) machine translation refers to automatic translation systems which start generating an output hypothesis before the entire input sequence has been consumed \cite{bangalore2012real,sridhar2013segmentation}. Emerging recently a... |
1,116,691,497,522 | arxiv | \section{Introduction}
\label{I}
Relevance of structural disorder for the critical behaviour remains
to be an important problem of modern condensed matter physics.
Even a weak disorder may change drastically the behaviour near the
critical point and in this respect may be related to the global
characteristics of a phy... |
1,116,691,497,523 | arxiv | \section{Introduction}
A fundamental challenge faced by the particle physics community is to determine the Majorana or Dirac nature of the
neutrino. In order to assess this question, experimentalists are exploring different reactions where the Majorana nature
may be manifested (for a review see e.g. \cite{Zralek:1997... |
1,116,691,497,524 | arxiv | \section{Weak solutions}
In this section, we extend the
weak solution theory in \cite{DG2} to cover the case that the initial population range $\Omega_0 $ is
unbounded. To our knowledge, little is known for problem \eqref{eqfrfisher} with a general unbounded $\Omega_0$.
For future applications, we consider the fol... |
1,116,691,497,525 | arxiv | \section{INTRODUCTION}
\setcounter{equation}{0}
The electroweak phase transition is at present the
object of extensive investigations \cite{Sin}. If the
phase transition is first order, which is possibly the case
if the mass of the Higgs boson is not too large,
the phase transition occurs via bubble nucleation. Bubble ... |
1,116,691,497,526 | arxiv | \section{Introduction}
We consider the two-machine flow shop problem with ordered machines in which each job has its smaller processing time
on the first machine and with the objective of determining simultaneously
a minimal common due date $d$ and a minimal number of tardy jobs $n_T$.
More precisely, there is a se... |
1,116,691,497,527 | arxiv | \section{Introduction}
Transmission of a quantum state from one place to another during specific time interval (quantum state transfer) is an important problem in development of quantum communication systems. The simplest model of such transfer is the quantum state transfer in an open 1/2-spin chain. In this case the... |
1,116,691,497,528 | arxiv | \section{Introduction}
Recently, interest has
increased the interpretation of Core Collapse
Supernovae (CCSNe) data, both spectra and photometry (Richardson et al. 2006;
Elmhamdi et al. 2006; Taubenberger et al. 2009; Maurer et al. 2010;
Elmhamdi et al. 2011).
In particular special
attention has been ... |
1,116,691,497,529 | arxiv | \section{Introduction} \label{intro}
A two-way contingency table gives the joint distribution of two
random variables with a finite number of outcomes. If we denote by
$\{0, \ldots, I-1\}$ and $\{0, \ldots, J-1\}$ the outcomes of
$X_1$ and $X_2$ respectively, the contingency table is represented
by a matrix $P=(p_{ij}... |
1,116,691,497,530 | arxiv | \section{Introduction}
The holographic principle has a concrete and well-understood realization in anti-deSitter space (AdS) \cite{Maldacena:1997re}. One hopes that the principle extends in some form to (nearly) flat spacetimes like the one we inhabit. The basic fact that the ratio of the boundary to bulk volume goes ... |
1,116,691,497,531 | arxiv | \section{Introduction}
The letter $G$ will denote a Hausdorff topological group with unit element $e \in G$.
All spaces are assumed to be completely regular and Hausdorff.
By an action of $G$ on a space $X$ we mean a
continuous map $(g, x)\mapsto gx$ of the product $G\times X$ into
$X$ such that $ex=x$ and $(gh... |
1,116,691,497,532 | arxiv | \section{Introduction}
NA60+, a successor of NA60, is a new dimuon experiment that aims to study hard and electromagnetic processes at CERN-SPS energies. It extends and improves the physics program of its predecessor by performing measurements of dileptons and heavy-quark production over the entire SPS energy range and... |
1,116,691,497,533 | arxiv | |
1,116,691,497,534 | arxiv | \section{Introduction}
Let $M$ be an $n$-dimensional, compact, connected, oriented Riemannian
manifold without boundary. The heat kernel is the fundamental solution to
the associated heat equation. That is, it is the unique function $%
K:(0,\infty )\times M\times M$ that satisfies
\begin{eqnarray*}
\left( \frac{\par... |
1,116,691,497,535 | arxiv | \section{Introduction}
\par Recently, device-to-device (D2D) communication has been envisioned as a promising technology to provide a better user experience. Specifically, proximity D2D users can communicate with each other directly without going through the base station (BS). Taking the advantages of the physical p... |
1,116,691,497,536 | arxiv | \section{Introduction}
\label{intro}
Absorption of the 21-cm electron spin-flip transition of neutral hydrogen (\HI) is a powerful probe of the reservoir of
star-forming material in the early Universe. At high redshift, 21-cm absorption can provide important insight into star
formation rates and galaxy evolution at... |
1,116,691,497,537 | arxiv | \section{Introduction}
Among the achievements of HERA, one of the major results was the experimental evidence \cite{Derrick:1993xh,Ahmed:1994nw}
that
among the whole set of $\gamma^* p \to X$ deep inelastic scattering events, almost 10\% are diffractive (DDIS), of the form $\gamma^* p \to X Y$ with a rapidity gap be... |
1,116,691,497,538 | arxiv | \chapter{Audience}
\label{chapter_1}
\large This document is intended to explain the Wireless Backhaul Links Clustering between point to point ethernet transmission links.
With the word clustering the first thing comes to
mind is bundling bunch of physical links to make a single
logical link. While this definition hol... |
1,116,691,497,539 | arxiv | \section{Introduction}
The first solar neutrino experiment, the Cl-Ar radiochemical detector \cite{ClAr} built by Ray Davis, Jr. and his colleagues, provided the only direct information about solar neutrinos in the seemingly endless interval between 1968 and 1988. Towards the end of that period the Kamiokande proton-d... |
1,116,691,497,540 | arxiv | \section{Introduction}
\label{Sect:intro}
\subsection{Maldacena holography, fixed-background holography and the Arnsdorf-Smolin puzzle}
The remarkable conjectured `holographic' correspondence \cite{Aharony:1999ti} due originally to Maldacena
\cite{Maldacena:1997re}, between certain superstring theories in the b... |
1,116,691,497,541 | arxiv | \section{Introduction}
The classification of associative algebras was instituted by Benjamin Peirce
in the 1870's \cite{pie}, who gave a partial classification of the complex
associative algebras of dimension up to 6, although in some sense, one can
deduce the complete classification from his results, with some additi... |
1,116,691,497,542 | arxiv | \section{Details for Section \ref{sec:dec}}
In this section, we give details of lemmas from
Section \ref{sec:dec}.
\subsection{Equivalence of $\textsf{PS 2.0-rlx}$ and ${\mathsf{LoHoW}}$}
To prove Theorem \ref{thm:eqv},
we show the following: Given a program $\prog$,
starting from the initial machine state $\... |
1,116,691,497,543 | arxiv | \section{#1}}
\renewcommand{\theequation}{\thesection.\arabic{equation}}
\textwidth 160mm \textheight 220mm
\begin{document}
\topmargin 0pt \oddsidemargin 0mm
\renewcommand{\thefootnote}{\fnsymbol{footnote}}
\begin{titlepage}
\begin{flushright}
\end{flushright}
\vspace{1mm}
\begin{center}
{\Large \bf Holographic Con... |
1,116,691,497,544 | arxiv | \section{Introduction}
Elastic strips and rods are fundamental physical structures that can be found in many contexts on many different length-scales. Often, they appear in the theoretical description of physical phenomena where the interplay between physics and geometry plays a key role. The collapse of an elastic s... |
1,116,691,497,545 | arxiv | \section{Introduction}
Let $f: \{0,1\}^n \to \{0,1\}$ be a total Boolean function. The \emph{conflict complexity} of $f$, denoted by $\chi(f)$, is a complexity measure of $f$ that is recently defined in \cite{random2} and appears implicitly in \cite{random1}. Using this notion, \cite{random2} and \cite{random1} indep... |
1,116,691,497,546 | arxiv | \section{Introduction}\label{sec_intro}
Let $N$ be a positive integer, $\mathbb{N}^+:=\{1,2,\ldots\}$ and $\mathbb{R}^+:=(0,+\infty)$. Consider the linear diffusion equation over $\mathbb{R}^N$:
\begin{equation}\label{yu-6-24-1}
\left\{
\begin{array}{lll}
\partial_t u(x,t)-\sum\limits_{j,k=1}^N\partial_j\left(a_{jk}(... |
1,116,691,497,547 | arxiv |
\section{Introduction}
Speaking rate control is a speech processing task of changing the speaking rate of a given speech~\cite{src_4,src_0,src_1,src_2,mpm}.
This technology has been widely applied in many real-world applications.
Since speaking rate changes speech intelligibility and accessibility, users may need dif... |
1,116,691,497,548 | arxiv | \section{Introduction}
In recent years significant progress has been made towards understanding the excitation spectrum of strings moving in five-dimensional anti-de Sitter space-time and, accordingly,
the spectrum of scaling dimensions of composite operators in planar ${\cal N} = 4$ supersymmetric gauge theory. This p... |
1,116,691,497,549 | arxiv | \section{Cross-metric Correlation Analysis}\label{sec:cross_metrics_corelation}
\paragraph{Correlations across meaning preservation metrics} Figure~\ref{fig:cross_metric_meaning} presents a cross-metric correlation-based analysis of the different approaches for measuring meaning preservation. We observe consistent tren... |
1,116,691,497,550 | arxiv | \section{Introduction}
Let $W$ be a finite subgroup of $ O(n)$ generated by reflections.
The algebra of $W$-invariant polynomials is generated by $n$
algebraically independent $W$-invariant homogeneous polynomials and
the degrees of these basic invariants are uniquely determined. This
theorem and its converse were firs... |
1,116,691,497,551 | arxiv | \section*{Abstract}
Understanding tumor invasion and metastasis is of crucial importance
for both fundamental cancer research and clinical practice.
\textit{In vitro} experiments have established that the invasive growth
of malignant tumors is characterized by the dendritic invasive branches composed of chains
of tumor... |
1,116,691,497,552 | arxiv | \section{Introduction}
\vspace{0in}The representation-valued equivariant index of a transversally
elliptic operator is an important invariant in $K$-theory (see \cite{A}).
There are few known nontrivial examples in the literature where this
invariant is explicitly computed. Part of the motivation of this paper is to
p... |
1,116,691,497,553 | arxiv | \section{Introduction}
\begin{figure*}[t!]
\centering
\setlength{\tabcolsep}{1pt}
\resizebox{\linewidth}{!}
{
\begin{tabular}{cccccc}
Bicubic Upscaling & Team ZTE VIP & Team Noah\_TerminalVision & Team Rainbow & Team Diggers & High-Resolution Target \\
\\
\includegraphics[width=0.3\linewidth]{Figures/scene_3/5.png}&
\... |
1,116,691,497,554 | arxiv | \section{Introduction}
The mass loss mechanism of AGB stars and red supergiants is a
long-standing astrophysical problem. In the carbon-rich case, an
extraordinary condensate exists (amorphous carbon) which is very
stable, i.\,e.\ it can exist already close the star, and is very opaque in
the optical and near IR spe... |
1,116,691,497,555 | arxiv | \section{Introduction}
Tidal disruption events (TDEs) occur when stars in the center of a galaxy that orbit close to the supermassive black hole (SMBH) get close enough that the tidal forces acting on them exceed their own self gravity, causing the star to be disrupted. In this case a large fraction of the star's mass... |
1,116,691,497,556 | arxiv | \section{Introduction}
The nuclear Equation of State (EoS) around the saturation density of symmetric matter ($n_{sat}$) can be accurately characterized by the so-called empirical parameters, defined as the set of successive derivatives of the energy functional~\cite{Myers1969}. Since the density of atomic nuclei is n... |
1,116,691,497,557 | arxiv | \section{Introduction}
\label{Sect:Intro}
The hadronic contribution to the muon anomalous magnetic moment
$a_{\mu} = (g_{\mu}-2)/2$ represents one of the long--standing
challenging issues of elementary particle physics, which engages
the entire pattern of interactions within the Standard Model.
The~experimental mea... |
1,116,691,497,558 | arxiv | \section{Introduction}
By using a large-scale antenna array at the base station (BS), massive multiple-input multiple-output (MIMO) can serve multiple users at the same frequency band simultaneously and thus boost the system spectral efficiency \cite{Marzetta10noncooperative,Larsson14massive,Sun15Beam,Wang18spatia... |
1,116,691,497,559 | arxiv | \section{Basic definitions}
A {\it tournament} $T=(V(T),A(T))$ or $(V,A)$ consists of a finite
{\it vertex} set $V$ with an {\it arc} set $A$ of ordered pairs of
distinct vertices satisfying: for $x, y \in V$, with $x \neq y$,
$(x, y) \in A$ if and only if $(y, x) \notin A$. The {\it
cardinality} of T is that ... |
1,116,691,497,560 | arxiv | \section{Introduction}
There has been a growing interest in green wireless communications to reduce the power consumption of wireless networks over the past decade \cite{8014295}. Various technologies for green communications have been proposed including cloud radio access networks (C-RANs), energy harvesting, and cogn... |
1,116,691,497,561 | arxiv |
\chapter{A Novel Construction Algorithm\label{ch:algo}}
In this chapter, we propose a novel method for the construction of orthogonal arrays using existing orthogonal arrays and unit column vectors with the help of the Kronecker Product operator. The method proposed herein serves towards forming orthogonal array... |
1,116,691,497,562 | arxiv | \section{Introduction}
A fundamental question in discrete tomography is whether a binary
image can be reconstructed from a small number of projections. As a
special case, one might restrict attention to permutation matrices,
and try to determine which vectors of antidiagonal sums appear only
once. This problem, consi... |
1,116,691,497,563 | arxiv | \section{Introduction}
In this paper we deal with the problem of comparing the lifetimes of $k$-out-of-$n$ systems with respect to ageing properties, by relying on the theory of \textit{stochastic orders}, Shaked and Shanthikumar~\cite{shaked2007}. We recall that the lifetime of a $k$-out-of-$n$ system is represented b... |
1,116,691,497,564 | arxiv | \section{Introduction}
\label{sec.Introduction}
The Peccei-Quinn (PQ) mechanism~\cite{Peccei:1977hh,Peccei:1977ur} represents the most elegant solution to the strong CP problem in Quantum Chromodynamics~\cite{Baker:2006ts,Pendlebury:2015lrz,Abel:2020pzs}. The key ingredient consists of a new dynamical pseudo-scalar fi... |
1,116,691,497,565 | arxiv | \section{Introduction}
The following parabolic initial-boundary value problem is considered
for a singularly perturbed linear system of second order
differential equations
\begin{equation}\label{BVP}
\frac{\partial\vec{u}}{\partial t}
-E\frac{\partial^2\vec{u}}{\partial
x^2}+A\vec{u}=\vec{f},\;\;\mathrm{on}\;\... |
1,116,691,497,566 | arxiv | \section{Introduction}
\label{sec:introduction}}
\begin{CJK}{UTF8}{gbsn}
\IEEEPARstart{R}{ecent} years have witnessed a tremendous progress in computer-aided detection/diagnosis (CAD) in medical imaging and diagnostic radiology, primarily thanks to the advancement of deep learning techniques. Having achieved great su... |
1,116,691,497,567 | arxiv | \section{Introduction}
It is well known that negative refraction takes place at an interface
between a usual isotropic medium (vacuum, for example) and a
material with negative permittivity and permeability (called Veselago medium,
double-negative material, or backward-wave medium).
Recently, a lot of efforts have bee... |
1,116,691,497,568 | arxiv | \section{\bf Introduction}
Higher spin fields in AdS space-time are known to be a crucial ingredient of $AdS/CFT$ correspondence,
as most of the composite operators on the conforml field theory (CFT) side are holographically dual to
the higher spin modes. Perhaps the best known example of such a correspondence i... |
1,116,691,497,569 | arxiv | \section{Introduction}
\label{I}
We consider the \emph{Euler system} describing the time evolution of the mass density $\varrho = \varrho(t,x)$ and the momentum $\vc{v}_m = \vc{v}_m(t,x)$ of
a barotropic inviscid fluid:
\begin{equation} \label{i1}
\begin{split}
\partial_t \varrho + {\rm div}_x \vc{v}_m &= 0,\\
\part... |
1,116,691,497,570 | arxiv | \section{Introduction}\label{sec:1
Pulsars are rapidly rotating neutron stars that emit radio wave pulses via their strong magnetic fields. They serve as extraordinary astrophysical laboratories for studying both nuclear physics and strong gravitation. Thus far, less than 2,700 pulsars have been discovered throughout t... |
1,116,691,497,571 | arxiv | \section{Introduction}
Buildings account for a quarter of total energy consumption globally and up to $40 \%$ in developed countries; the majority of which is used for heating (including hot water), cooling and ventilation. Electric heating with heat pumps is slowly displacing the use of oil and natural gas \cite{pere... |
1,116,691,497,572 | arxiv | \section*{Introduction}
In this small note we introduce a notion of self-stresses on the set
functions in two variables with generic critical points.
The notion naturally comes from a rather exotic representation of classical Maxwell frameworks
in terms of differential forms.
For the sake of clarity we work ... |
1,116,691,497,573 | arxiv | \section{Introduction}
Astronomical and cosmological probes of dark matter not only exist, but indicate that dark matter is five
times as prevalent in the universe than the conventional forms of matter described by the Standard Model \cite{Ade:2013zuv}.
Despite this abundance however, knowledge of dark matter remain... |
1,116,691,497,574 | arxiv | \section{introduction}
Let $\mathcal{X}$ be a Banach space and $r>0$ a real. A subset $\mathcal{Y}\subseteq \mathcal{X}$ is called $r$-equilateral if
$\|x-y\|=r$ for any two distinct $x, y\in \mathcal{Y}$; it is called equilateral if it is $r$-equilateral
for some real $r>0$.
As shown by Brass and by Dekster (\cite{... |
1,116,691,497,575 | arxiv | \section{Introduction}
The presence or absence of broad optical emission lines has been historically used to separate Seyfert galaxies into two classes: Seyfert 1 galaxies
with broad permitted and narrow forbidden lines and Seyfert 2 galaxies with only narrow permitted and forbidden line emission \citep{1974ApJ...... |
1,116,691,497,576 | arxiv | \section{Introduction and statement of the result}
A real random variable $X$ is said to be unimodal if there exists $a\in{\mathbb{R}}$ such that its distribution function ${\mathbb{P}}[X\le x]$ is convex on $(-\infty, a)$ and concave on $(a, +\infty)$. When $X$ is absolutely continuous, this means that its density is... |
1,116,691,497,577 | arxiv | \section{\bf Introduction}
\subsection{(Hereditary) cotorsion pairs in Morita rings} For a ring $R$, let $R$-Mod be the category of left $R$-modules.
For a class $\mathcal C$ of objects in abelian category $\mathcal A$, and $X\in \mathcal A$, by \ $\Ext^1_\mathcal A(X, \mathcal C)=0$ we mean
\ $\Ext^1_\mathcal A(... |
1,116,691,497,578 | arxiv | \section{\bf Introduction}\label{section1}
In this paper, we study the Ricci flow on K\"ahler manifolds defined by
$$X_{n,k} = \mathbb{P}(\mathcal{O}_{\mathbb{C}\mathbb{P}^{n-1}}\oplus \mathcal{O}_{\mathbb{C}\mathbb{P}^{n-1}}(-k))$$ for $k, n \in \mathbb{N}^+$. Such manifolds are holomorphic $\mathbb{C}\mathbb{P}^1$ ... |
1,116,691,497,579 | arxiv | \section{Discussion}
The current standard for the evaluation of an unsupervised method involves the use of an AlexNet architecture trained on ImageNet and tested on class-level tasks.
To understand and measure the various biases introduced by this pipeline on DeepCluster\xspace, we consider a different training set, a... |
1,116,691,497,580 | arxiv | \section{Introduction}
The Standard ($\Lambda$-CDM) Model in cosmology gives a phenomenological description of
the observed {\it Dark Energy} (DE) and {\it Dark Matter} (DM). It is based on the
use of a small positive cosmological constant $\Lambda$ and a {\it Cold Dark Matter} (CDM),
and is consistent with all obser... |
1,116,691,497,581 | arxiv | \section{Introduction}\label{sec:intro}
A surface is one of the central subjects in condensed matter physics.
An open surface changes the spatial symmetry of the system and perturbs the bulk electronic states, which sometimes brings about novel surface states qualitatively different from the bulk one~\cite{PhysRev.11... |
1,116,691,497,582 | arxiv | \section{Introduction}
A scalable quantum computer is expected solve difficult problems that are intractable with classical computing technology. Scaling such a machine to a useful size will necessarily require fault-tolerant components that protect quantum information as the data is processed~\cite{Calderbank96, Ste... |
1,116,691,497,583 | arxiv | \section{Background}
\label{sec:background}
This section summarizes the essential aspects of blockchain technology and discusses initial research efforts at the intersection of BPM and blockchains.
\subsection{Blockchain Technology}
In its original form, Blockchain is a distributed database technology that builds on a ... |
1,116,691,497,584 | arxiv |
\subsection{Analysis of Algorithm~\ref{algo:wam2}}
For a fixed scaling $s: E\to [0,1]$, let $\ell$ be the number of eigenvalues
of the normalized Laplacian $N^{s}$ of $G^{s}$ that are in the range $(0,\zeta]$.
Let $\ell_0 = \ceil{ \frac{\gamma_2 k^2}{(1-\zeta)^2} }$, which, by Theorem~\ref{thm:fewsmall},
is a... |
1,116,691,497,585 | arxiv | \section{Introduction}
The goal of this paper is to understand diffeomorphism symmetries
in the canonical formalism at the classical level. The putative
generators of infinitesimal general coordinate transformations feature
in all canonical quantization approaches, but debate persists in the
literature as to what ... |
1,116,691,497,586 | arxiv | \section{Introduction}
There has been spectacular technological advances in the use of
high-quality optomechanical oscillators for force sensing, enabling
ultra-sensitive force measurements of single spin, charge,
acceleration, magnetic field and mass~\cite{Rugar04_Nat,
Cleland98_Nat, Krause12_NatPhot, Forstner12_P... |
1,116,691,497,587 | arxiv | \section{Introduction}
In human-robot collaboration, it is crucial for a cooperative robot (``co-robot'') to have the abilities of perception of human activities and corresponding appropriate decision-making to understand and interact with human peers. In order to provide these important capabilities, an artificial c... |
1,116,691,497,588 | arxiv | \section{Introduction}\label{sec:s1}
Since the introduction in Kingsbury \cite{king1,king2} of complex wavelet\ transform s implemented by the dual-tree scheme, the complex wavelet s (DT\_CW), wavelet\ frames and wavelet packet s (WPs) have become a field of active research that appears in multiple applications (\ci... |
1,116,691,497,589 | arxiv | \section{Introduction}
The motion of electrons in the periodic potential of ionic crystals is addressable by the celebrated Bloch solutions which give rise to band structure \cite{bloc28, ashc76}. Periodic potentials are also common in the arena of ultracold atoms where gases trapped in optical lattices can serve as... |
1,116,691,497,590 | arxiv | \section*{Informational Fourth Page}
|
1,116,691,497,591 | arxiv | \section{Introduction}
Given the similarity between neutrons and protons, that gets ramified in the concepts of charge symmetry and charge invariance for nuclear interactions, the natural expectation is that there is little difference in how neutrons and protons distribute themselves across a~nucleus. In fact, it has ... |
1,116,691,497,592 | arxiv | \section{Introduction}
Magnetic random access memories are believed to be among the most promising candidates to deliver the future of scalable,
non-volatile, rapidly accessible data storage. At the heart of these devices are magnetic tunnel junctions (MTJs), which
store data on the relative orientation of the magne... |
1,116,691,497,593 | arxiv | \section{Introduction}
Let $C\subset\C$ be a compact infinite set in the complex plane and let $\P_n$ be the set of all polynomials with complex coefficients of degree $n$. Then $L_n(C)$, defined by
\begin{equation}
L_n(C)\equiv\max_{z\in{C}}|z^n+\sum_{k=0}^{n-1}c_{k}^{*}z^{k}|:=
\min_{c_{k}\in\C}\max_{z\in{C}}... |
1,116,691,497,594 | arxiv | \section{\large{\bf Introduction}}
SUSY hybrid inflation \cite{Dvali:1994ms,Copeland:1994vg,Linde:1993cn,Dvali:1997uq} provides fascinating framework to realize inflation within the grand unified theories (GUTs) of particle physics. Several GUT models such as, $SU(5)$ \cite{Georgi:1974sy}, Flipped $SU(5)$ \cite{Barr:1... |
1,116,691,497,595 | arxiv | \section{Acknowledgements}
The authors acknowledge discussions with
A. Macdonald, D. Ralph, Kelly Luo, Vishakha Gupta, Rakshit Jain, Nai Chao Hu, Bowen Shen, and Zui Tao.
Work at UCSB was primarily supported by the Army Research Office under award W911NF-20-2-0166 and by the Gordon and Betty Moore Foundation EPIQS pr... |
1,116,691,497,596 | arxiv | \section{Introduction}
\label{sec:intro}
The $\Lambda$ cold dark matter ($\Lambda$CDM) model has become
well established as the standard model of cosmology,
due to its very impressive fit
to a variety of cosmological observations, including
CMB anisotropy \citep{wmap9h,planck-xvi}, large-scale
galaxy c... |
1,116,691,497,597 | arxiv | \section{Introduction}
\label{sec:intro}
Convolutional neural networks have led to significant progress in object detection by learning with a large number of training images with annotations~\cite{ren2015faster,redmon2017yolo9000,cai2018cascade,carion2020end}. However, humans can easily localize and recognize new obj... |
1,116,691,497,598 | arxiv | \section{Introduction}
Reionization was the last major phase transition of the intergalactic medium (IGM), and scrutinizing the detailed evolution of the IGM is a key frontier in observational cosmology. High-redshift star-forming galaxies are thought to be the primary sources of ionizing photons \citep[e.g.,][]{Rober... |
1,116,691,497,599 | arxiv | \section{Introduction and Conclusions}
Supersymmetry breaking string vacua (including 10d non-supersymmetric strings) are generically affected by tadpole sources for dynamical fields, unstabilizing the vacuum \cite{Fischler:1986ci,Fischler:1986tb}. We refer to them as {\em dynamical tadpoles} to distinguish them from... |
1,116,691,497,600 | arxiv | \section{Introduction}
\IEEEPARstart{T}{he} interplay between social networks and complex human behavioral dynamics has been the subject of extensive research. Social ties, a.k.a. friendships and/or acquaintanceships, have been connected to various complex human phenomena. Some studies, for example, demonstrated the s... |
1,116,691,497,601 | arxiv | \section{Introduction}
Machine learning models are increasingly deployed for critical decision-making tasks (e.g., Bail decision\cite{angwin2016machine} ). It is important to verify that they do not contain gender or racial biases picked up from training data.
Typical approaches to achieve fairness revolve around e... |
1,116,691,497,602 | arxiv | \section{Introduction}
\label{intro}
The goal of this study is three-fold:
\begin{enumerate}
\item Construct an algorithm to approximate a solution to a system of congruence equations pertaining to the zeta function.
\item Use the approximations in item (1) to locate regions along the line $\sigma=1$ where the real par... |
1,116,691,497,603 | arxiv | \section{Introduction}
\label{sec1} |
1,116,691,497,604 | arxiv | \section{Introduction}
Consider the following problem faced by a group of $n$ manufacturers of some good. Each manufacturer produces the same undifferentiated product, which sells for some exogenously given price. The manufacturers are constrained by the production process into producing goods of the same given aver... |
1,116,691,497,605 | arxiv | \section{Introduction}
Topological phases have been the subject of extensive studies over the past few decades~\cite{Thouless1982,Thouless1983,Kane_and_Mele2005, ExperimentalRealization2007,chen2009experimental,chang2013experimental,Khanikaev2013,Gao2013,lv2015experimental,xu2015discovery,yang2015weyl,Chiu2016,he2017c... |
1,116,691,497,606 | arxiv | \section*{Acknowledgments}
I would like to warmly thank my collaborator and friend Fran\c cois Englert with whom almost all the original results
presented here have been derived. I am also grateful to Sophie de Buyl, Marc Henneaux and Nassiba Tabti for enjoyable collaborations.
|
1,116,691,497,607 | arxiv | \section{Introduction}
The theory of the (eigenvalue) matrix models (MAMO) occupies more and more space in the
context of modern theoretical physics,
what could seem unexpected and even unjustified.
However, this impression is basically wrong:
MAMO are indeed crucially significant, because they appear to capture
the m... |
1,116,691,497,608 | arxiv | \section{Introduction}
It is well known that for an absolutely irreducible polynomial
$f\in\Z[x,y]$ the reduction $f\bmod p$ is also absolutely irreducible
if the prime $p$ is large enough. For small $p$ the polynomial $f\bmod
p$ may be reducible.
E.g. $f=x^9y-9x^9-2x+9y+2$ is absolutely irreducible over
$\Q$ but red... |
1,116,691,497,609 | arxiv | \section{Introduction}
Plasma diagnostics using $K_{\alpha}$ fluorescence spectra allows to investigate properties of warm dense matter.
This work focuses on the bulk temperature distribution of plasmas created from Ar droplets irradiated by high energy laser pulses
with a power of 10$^{19}$ W/cm$^2$ \cite{Ar}. Due ... |
1,116,691,497,610 | arxiv | \section{Introduction}
Our aim was to obtain for categorical groups an analogous description in terms of certain crossed module type objects as we have it for $\mathcal{G}$-groupoids obtained by Brown and Spencer \cite{BS1}, which are strict categorical groups, or equivalently, group-groupoids or internal categorie... |
1,116,691,497,611 | arxiv | \section*{Acknowledgments}
E.~L.~Berger is supported
by the United States Department of Energy, Division of High Energy
Physics, under Contract W-31-109-ENG-38. J.~W.~Qiu is supported in part by
the United States Department of Energy under Grant No. DE-FG02-87ER40371.
Y.~Wang is supported in part by the United S... |
1,116,691,497,612 | arxiv | \section{Introduction}
Pluto, Titan and Triton all have a nitrogen-based atmosphere containing a significant fraction of methane, an efficient recipe known to lead to the formation of organic haze in the atmosphere, as confirmed by observations \citep{Toma:05,RagePoll:92,HerbSand:91,Ster:15} and laboratory experiments... |
1,116,691,497,613 | arxiv | \section*{Notes}}
\newcommand{\Exer}{
\bigskip\markright{EXERCISES}
\section*{Exercises}}
\newcommand{D_G}{D_G}
\newcommand{{\rm S5}_m}{{\rm S5}_m}
\newcommand{{\rm S5C}_m}{{\rm S5C}_m}
\newcommand{{\rm S5I}_m}{{\rm S5I}_m}
\newcommand{{\rm S5CI}_m}{{\rm S5CI}_m}
\newcommand{Mart\'\i n\ }{Mart\'\i n\ }
\newcommand{\set... |
1,116,691,497,614 | arxiv | \section*{Main Text}
\subsection*{Introduction}
Breath analysis examines the hundreds or thousands of low-concentration molecular species present in exhaled human breath and correlates them with particular health conditions or diseases. Some examples include formaldehyde being correlated with breast cancer, ammonia w... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.