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1,116,691,501,115 | arxiv | \section{Introduction}
In this paper, we first construct nonholonomic systems of $n$ homogeneous balls $\mathbf B_1,\dots,\mathbf B_n$ with centers $O_1,...,O_n$ and with the same radius $r$ that are rolling without slipping around a fixed sphere $\mathbf S_0$ with center $O$ and radius $R$.
We assume that a dynamical... |
1,116,691,501,116 | arxiv | \section{introduction}
Generically, many-body quantum systems have two robust distinct fates after a quantum quench: thermalization and localization (see Ref.~\onlinecite{Nandkishore2015} and the references therein). In the former case, the system effectively serves as a heat bath for small enough subsystems, resulti... |
1,116,691,501,117 | arxiv | \section{Introduction}
In numerical weather prediction (NWP) a data assimilation procedure is used to combine observations of the atmosphere with a model description of the system in order to obtain initial conditions for forecasts. The contribution of each component is weighted by its respective error statistics.
In ... |
1,116,691,501,118 | arxiv | \section{Introduction}
\label{sec:intro}
For the decades, dark matter searches have been taken place by many experiments although nature is yet to be cleared.
A direct dark matter search, which detect nuclear recoil by the dark matter, is one of the useful methods to explore its nature.
Especially, assuming that a dar... |
1,116,691,501,119 | arxiv | \section{Introduction}
The discovery of over twenty quasars at
redshift $z \gtapprox 5.7$ (e.g. \citealt{Fan00,Fan01a,Fan03,Fan04,Fan06a,Goto06}), with
masses estimated to be $ \gtapprox 10^9 \ensuremath{M_\odot}$
\citep{Barth03, Vestergaard04, Jiang06a, Kurk07},
challenges our current understanding of the early u... |
1,116,691,501,120 | arxiv | \section{Introduction}
The cosmic Dark Ages ended with the formation of the first stars in
$10^5 - 10^6\, {\rm M_\odot}$ cosmological haloes at $z \sim 20 - 30$.
Primordial (or Pop III) stars are the key to understanding primeval
galaxies, the onset of early cosmological reionization and chemical
enrichment, and the o... |
1,116,691,501,121 | arxiv |
\subsection{Introduction}
Each of the usual cohomology theories $X\rightsquigarrow H^{j}(X,r)$ on
algebraic varieties arises from a functor $R\Gamma$ taking values in a
triangulated category $\mathsf{D}$ equipped with a $t$-structure and a Tate
twist $N\rightsquigarrow N(r)$. The heart of $\mathsf{D}$ has a ten... |
1,116,691,501,122 | arxiv | \section{Introduction}
The topic of the in-medium properties of strange hadrons is
a subject of intense research in the context of the heavy
ion collision experiments as well as in the study
of the bulk matter in nuclear astrophysical objects, e.g.,
(proto) neutron stars \cite{Tolos_Prog_Part_Nucl_Phys_112_103770_20... |
1,116,691,501,123 | arxiv | \section{Introduction}
\label{sec:intro}
\vspace{-1mm}
Consider a conventional neural network trained to predict whether a random person would classify a drawing as either a `rabbit' or a `duck'.
As illustrated in Figure \ref{fig:nn_example}, given a single drawing, the network generates a marginal prediction that ass... |
1,116,691,501,124 | arxiv | \section{INTRODUCTION}
In MIMO (multiple-input multiple-output) systems, channel capacity grows linearly with the number of spatial degrees of freedom (DoF), which is relative to both the scattering environment and antenna array geometries. Recently, the concept of \textit{holographic MIMO} has drawn increasing attenti... |
1,116,691,501,125 | arxiv | \section{...}
Violation of the combined Charge-conjugation and Parity symmetries
($CP$) in the standard model (SM) is produced by a non-vanishing phase
in the Cabibbo-Kobayashi-Maskawa flavor-mixing matrix~\cite{CKM},
where the violation may be observed as a non-zero $CP$ asymmetry
defined as
\begin{equation}
A^{D\r... |
1,116,691,501,126 | arxiv | \section{Mean Field analysis}\label{A}
If the field $\Phi_\perp =0$, the GP functional (\ref{HH},\ref{grad}) becomes (at $\vec{\eta}=0$):
\begin{widetext}
\begin{eqnarray}
H=\int dxdy\left[i(\Phi^*\dot{\Phi}-c.c.) - \frac{1}{2m}|\vec{\nabla} \Phi|^2 + \left(\frac{ (\vec{\nabla}\theta)^2}{2m} -\mu - n_0d^2_0\right) |... |
1,116,691,501,127 | arxiv | \section{Introduction
A quasitoric manifold $M$ over a simple polytope $P$, which was introduced by Davis and Januszkiewicz \cite{DJ91},
is a $2n$-dimensional smooth manifold with a locally standard $T^n=(S^1)^n$-action for which the orbit space is identified with $P$.
Quasitoric manifolds are defined as a topological... |
1,116,691,501,128 | arxiv | \chapter*{Abstract}
This dissertation concerns the classification of groupoid and higher-rank graph $C^*$-algebras and has two main components. Firstly,
for a groupoid it is shown that the notions of strength of convergence in the orbit space and measure-theoretic accumulation along the orbits are equivalent ways of r... |
1,116,691,501,129 | arxiv | \section{\label{sec:level1}INTRODUCTION}
Based on the principle of quantum mechanism, quantum key distribution (QKD) can share unconditional security keys between two communication parties under insecure channels \cite{r1,r2}. According to the modulation methods adopted in quantum state exchanges, QKD protocols are us... |
1,116,691,501,130 | arxiv |
\section{Analysis of the hyperbolicity in the closed curves }
In this section we prove that an open and dense subset of the vector fields having a robustly chain transitive chain recurrence class $C$ has a dominated splitting over $B(C)$. A dominated splitting over $\widetilde{\La(C)}$, from\cite{BdL}, and since for a... |
1,116,691,501,131 | arxiv | \section{Introduction}
Magnetic fields play an important role in determining the evolution of the matter in many astrophysical objects. In highly conducting plasma, the magnetic field can be amplified by gas contraction or shear motion. Even when the magnetic field is weak initially, the magnetic field can grow rapidl... |
1,116,691,501,132 | arxiv | \section{\bf Introduction:}
Two-dimensional string theory can be viewed as one dimensional-matter
(time) coupled to two-dimensional gravity [\DNW,\POLONE,\BL].
Since the latter has a nonperturbative formulation in terms of a
one-dimensional matrix model [\BKZ] (nonrelativistic fermions) we have an
opportunity to study... |
1,116,691,501,133 | arxiv |
\section*{Appendix}
\subsection{More Details about Data Collection}
The dance videos are collected from YouTube by crowd workers, which are all solo dance videos with 30FPS.
We trim the beginning and ending several seconds for each of collected videos to remove the silence parts, and split them into one-minute video ... |
1,116,691,501,134 | arxiv | \section{Symmetries and band structure for different $t_2/t$}
The tight binding part of our Hamiltonian has the following form
\begin{equation}
\label{Seq:tb}
H_{0} = -t\sum_{\langle ij \rangle l \sigma}\left(c^{\dagger}_{il\sigma}c_{jl\sigma}+h.c. \right)-t_2\sum_{\langle ij \rangle' l\sigma} \left( i^{2l-1}c^{\dagge... |
1,116,691,501,135 | arxiv | \section{Five Zones of Debris Dust}
Great advances are being made in the observations of debris disks
using all available platforms, revealing enduring patterns in the
behavior of debris disk structure and its evolution that point toward
general aspects of planetary system information and development that
are no... |
1,116,691,501,136 | arxiv | \section{Introduction}
Quantum computation is one based on the principle of quantum mechanics.
Compared with classical computation, it provides the advantage on
calculation speed {[}1{]}. For example, quantum computer can simulate
the property of quantum mechanics, and it is very difficult for classical
computer... |
1,116,691,501,137 | arxiv | \section{Introduction}
The recent discovery of superconductivity in iron-pnictides \cite{kamihara} has generated an intense research activity, in part because they provide an unexpected and very interesting scenario to study the interplay between magnetism and superconductivity.\cite{reviews} The interest for these co... |
1,116,691,501,138 | arxiv |
\section{Introduction}
The train and test distributions are often not identically distributed. Such train-test mismatches occur because evaluation datasets rarely characterize the entire distribution~\cite{Torralba2011UnbiasedLA}, and the test distribution typically drifts over time~\cite{QuioneroCandela2009DatasetSI... |
1,116,691,501,139 | arxiv | \section{Introduction}
Non-linear stochastic flows are at the heart of thermally driven
processes in systems whose potential energy surfaces are characterized
by multiple local energy minima. Pioneered by the seminal work of Kramers
\cite{kramers_brownian_1940} the concept of thermally activated
barrier-crossing has ev... |
1,116,691,501,140 | arxiv | \section{Introduction}
\IEEEPARstart{G}{eant4} \cite{g4nim,g4tns} is an object oriented toolkit for the
simulation of particle interactions with matter. It provides advanced
functionality for all the domains typical of detector simulation:
geometry and material modelling, description of particle properties,
physics pro... |
1,116,691,501,141 | arxiv | \section{Introduction}
One-counter automata (OCAs) are a fundamental model of infinite-state systems. Their expressive power resides between finite automata and pushdown automata. Unlike finite automata, however, OCAs are not robust: They lack closure under complementation and have an undecidable universality, equival... |
1,116,691,501,142 | arxiv | \section{Introduction}
\vspace{0.3cm}
With the consideration that the Quantum Chromodynamics (QCD) is
the underlying theory of the strong interaction,
the hadronic systems are assumed to be composed of quarks and gluons, and
most of descriptions of baryons are associated with some effective degrees of
freedom of no... |
1,116,691,501,143 | arxiv | \section{Introduction}
Prosodic phrasing is the division of fluent speech into \emph{prosodic} (or \emph{intonation}~\cite{beckman1997guidelines}) \emph{phrases} -- groups of words in a spoken sentence, typically featuring an intonation peak and often separated by pauses.
Prosodic phrasing not only plays an important... |
1,116,691,501,144 | arxiv | \section{Introduction}
We study simultaneous tilings of $\mathbb{R}^n$ by two actions which, on their face, do not have any relationship. The first action is via translation by a full rank lattice $\Gamma \subset \mathbb{R}^n$. There always exists a set $V \subset \mathbb{R}^n$ of finite measure such that $\{V + \gamm... |
1,116,691,501,145 | arxiv | \section{Introduction}\Label{int}
The remarkable result of Forstreni\v{c} \cite{Fo} on the classification problem of proper holomorphic mappings between unit balls states that if $f$ is proper, holomorphic map from a ball in $\mathbb C^n$ to a ball in $\mathbb C^N$ and smooth of class $C^{N-n+1}$ on the closure then $... |
1,116,691,501,146 | arxiv | \section{Acknowledgements}
MT would like to acknowledge suport from the Open Partnership Joint Projects of JSPS Bilateral Joint
Research Projects and the ImPACT Program of Council
for Science, Technology and Innovation, Japan.
KPS, and JPD would like to acknowledge support from the
Air Force Office of Scientific Rese... |
1,116,691,501,147 | arxiv | \section{Parallelization as Information Exchange}
\label{sec:communication-graph}
We observe that our parallelization approach implicitly defines a certain type of informational dependencies.
In both \eqref{def:greedy-algorithm} and \eqref{def:parallel-greedy}, each agent uses the choices of prior agents to make its o... |
1,116,691,501,148 | arxiv | \section{\label{sec:level1}Introduction:\protect\\ }
\section{Introduction}
In the near-wall region of turbulent shear flows, there exists a universal logarithmic velocity profile \citep{karman1930mechanische,millikan1938critical}, characterized by a constant slope between mean velocity and the logarithm of the distan... |
1,116,691,501,149 | arxiv | \section{Introduction}
Most stars in the galactic disk are formed in dense molecular gas within
giant molecular clouds (GMCs) as members of clusters (Lada \& Lada 2003).
Thus, clusters must play a critical role in the origins of some of
the most fundamental properties of the galactic stellar population.
In additio... |
1,116,691,501,150 | arxiv | \section{Analytic treatment of the periodically modulated double well}
\label{ap:analytic}
In the following we provide an analytic description of the periodically modulated double well system. First, the static Hamiltonian and its properties are discussed. Afterwards, the driven system is treated with a high frequency... |
1,116,691,501,151 | arxiv | \section{Introduction}
\label{sec:intro}
The thermodynamic limit, i.\,e.\ taking averages over larger and larger volumes,
performs the transition from microscopic to macroscopic models.
In the context of this paper, thermodynamic limits are used to define
the integrated density of states (IDS) of discrete Schr\"odinge... |
1,116,691,501,152 | arxiv | \section{Introduction}
Quantifying biochemical processes at the cellular level is becoming
increasingly central to modern molecular biology \cite{Elowitz2002,
Pedraza2005}. Much of this attention can be attributed to the development
of new methodologies for measuring biochemical events. In particular,
the use of g... |
1,116,691,501,153 | arxiv | \section{Introduction}\label{sec:pre}
Many notions of topology and combinatorics of the reals have been reformulated and investigated in terms of ideals on the natural numbers (always assuming that an ideal contains all the finite sets of natural numbers). For instance, the usual notion of convergence on a topological... |
1,116,691,501,154 | arxiv | \section{Introduction}
A basic task in Fractal Geometry is to determine or estimate the various dimensions of fractal sets. Fractal dimensions are introduced to measure the sizes of fractal sets and are used in many different disciplines. Many results on fractal dimensions and measures are obtained, among which the st... |
1,116,691,501,155 | arxiv |
\subsection{Shapes3D}
\begin{table*}[h]
{
\begin{center}
\small
\begin{tabular}{ccccc}
Layer & Units & Kernel size & Activation & Stride \\
\hline \\
Conv2D & 32 & 3x3 & ReLU & 1 \\
Conv2D & 32 & 3x3 & ReLU & 1 \\
Conv2D & 64 & 3x3 & ReLU & 2 \\
Conv2D & 64 & 3x3 & ReLU & 1 \\
Conv2D & 128 & 3x3 & ReLU & 1 \\... |
1,116,691,501,156 | arxiv | \section{Introduction}
\subsection{}
The present paper is a companion to \cite{arXiv:1703.05599} and is similarly inspired by the classification results of \cite{MR3600042}; however it can be read independently.
We recall the setting. We have a non-archimedean locally compact field $F$ of residue characteristic $p... |
1,116,691,501,157 | arxiv | \section{Introduction}
\label{sec:introduction}
Molecular dynamics simulation is a powerful method allowing to simulate at the particle scale different materials such as colloidal systems \citep{boattini_unsupervised_2019}, glassy materials \citep{barbot_rejuvenation_2020,barbot_characterization_2020} or metallic... |
1,116,691,501,158 | arxiv | \section{Introduction}\label{s-intro}
{In this talk two different but related subjects are considered:}\\
{\it I. A mechanism of massive PBH formation, which is much different from the caninocal ones.}
{According to this mechanism the fundament of PBH creation is build at inflation by making large isocurvature
fluctu... |
1,116,691,501,159 | arxiv | \section{Introduction}
The reaction $K^-p\rightarrow \Sigma^0\pi^0$ is of particular
interest in the study of baryon resonances and $\bar{K}N$
interaction since there are no isospin-1 baryons contributing here
and it gives us a rather clean channel to study the $\Lambda$
resonances, such as $\Lambda(1405)S_{01}$, $\... |
1,116,691,501,160 | arxiv | \section{Introduction}
Finsler geometry is a natural generalization of the Riemannian one. Roughly speaking, it is based on the notion of an interval without the quadratic restriction, i.e. on the interval that locally does not look like the one given by the Pythagoras theorem. In fact, this possibility was already di... |
1,116,691,501,161 | arxiv | \part*{Commentaire mathématique}
\addcontentsline{toc}{part}{Commentaire mathématique}
\label{comm_debut}
\paragraph{Théorème d'Apollonius, lemme de `Ur\d{d}{\=\i} et couple de
\d{T}\=us{\=\i}} On démontre ici trois propositions concernant les rotations
affines du plan. Elles nous seront utiles pour comparer entre e... |
1,116,691,501,162 | arxiv | \section{#1} \setcounter{equation}{0}}
\newtheorem{theo}{Theorem}[section]
\begin{document}
\newtheorem{lem}[theo]{Lemma}
\newtheorem{prop}[theo]{Proposition}
\newtheorem{coro}[theo]{Corollary}
\title{Controlled Geometry via Smoothing \footnote{ 1991 {\em Mathematics
Subject Classification}. Primary 53C20.}}
\auth... |
1,116,691,501,163 | arxiv | \section{Introduction and summary}
One of the many surprises during the second superstring revolution was the realization that the construction of $\mathrm{SU}(N)$ instantons on $\mathbb{R}^4$ by Aityah-Drinfeld-Hitchin-Manin \cite{Atiyah:1978ri} and on asymptotically locally Euclidean (ALE) spaces by Kronheimer-Na... |
1,116,691,501,164 | arxiv | \section{Introduction}
What is the probability that an extensive observable in a physical system has a value far from its average?
Such questions are the subject of large-deviation theory~\cite{Touchette}, which provides a mathematical foundation for
classical thermodynamics~\cite{Ruelle}, and has more recently been... |
1,116,691,501,165 | arxiv | \section{Introduction}\label{sec:introduction}
Be/X-ray transients harbour high-magnetic field (B$\sim$10$^{12-13}$ G) neutron stars (NSs) that move around Be-type stars in eccentric orbits. Typically, these binaries can exhibit two types of transient activity: more common, short-lived (i.e., small fraction of the orbi... |
1,116,691,501,166 | arxiv | \section{Introduction}
The persistent global consistency of the Standard Model (SM) predictions against the data collected so far at the CERN Large Hadron Collider (LHC) is radically changing our perspective on the origin of possible new physics beyond the SM, and on its characteristic energy scale. This is also suppo... |
1,116,691,501,167 | arxiv | \section{Introduction}\label{sec:intro}
Casimir and related effects, where quantum effects depend upon the
existence of boundary conditions for a quantum field, have been extensively
studied~\cite{rev}. Many different points of view and approaches to this
kind of problem have been followed, under quite different sets o... |
1,116,691,501,168 | arxiv | \section{\@startsection{section}{1}%
\usepackage{amssymb,amsthm, amsmath, amsfonts, url, graphicx,verbatim,scrextend}
\usepackage{amscd}
\usepackage{enumitem}
\hyphenation{res-pec-tiv}
\oddsidemargin20mm
\evensidemargin4mm
\headsep25mm
\theoremstyle{plain}
\newtheorem*{thm*}{Theorem}
\theoremstyle{plain}
\newtheorem{... |
1,116,691,501,169 | arxiv | \section{Introduction}
In this paper we are interested to the zygodactyly phenomenon in birds, and in particolar in parrots.
This arrangement, common in species living on trees, is a distribution of the foot with two toes facing forward and two back.
We give a model for the foot, and thanks to the methods of... |
1,116,691,501,170 | arxiv | \section{Introduction}
One of the principal objectives in modern cosmology is a
good description of
the physics that govern the formation of structure
from the galactic through to the supercluster scale.
Recent theoretical and observational work in this area has concentrated on understanding the relationship between t... |
1,116,691,501,171 | arxiv | \section{Introduction}
Multiphase flows of two immiscible fluids are encountered in many industrial applications ranging from small scale droplet interactions \cite{Khatavkar}, phase separation and microstructural evolution in materials \cite{Fried}, bubbly and slug flows in oil and natural gas pipelines to free-surf... |
1,116,691,501,172 | arxiv | \section{Introduction}
Among assessment methods, the job interview remains the most common way to evaluate candidates. The interview can be done via phone, live video, face to face, or more recently asynchronous video interview.
For the latter, candidates connect to a platform, and record themselves while answering a... |
1,116,691,501,173 | arxiv | \section{Introduction} \label{sect:1}
\hspace*{0.5cm} Hadron decays of the tau lepton provide a prime scenario
to study the hadronization of QCD currents in an energy region settled by
many resonances. This task has a twofold significance. First, the study of
branching fractions and spectra of those decays is a major ... |
1,116,691,501,174 | arxiv | \section{Proof of the First Zonklar Equation}
\section*{Acknowledgment}
This material is based on research sponsored by DARPA and Air Force Research Laboratory (AFRL) under agreement number FA8750-16-2-0173.
Hardware support was generously provided by the NVIDIA Corporation.
We also thank the financial support of FAPE... |
1,116,691,501,175 | arxiv | \chapter[IMB, Kamiokande and Super-K]{Neutrino Astronomy with IMB, Kamiokande and Super Kamiokande\footnotemark}\footnotetext{To be published in Neutrino Physics and
Astrophysics, edited by F. W. Stecker, in the Encyclopedia of Cosmology II,
edited by G. G. Fazio, World Scientific Publishing Company, Singapore, 2022.}
... |
1,116,691,501,176 | arxiv | \section{Introduction}
\medskip
Given a group or semi-group $\Gamma$ generated (in the sense of
semi-groups) by some subset $S\subset \Gamma$, the
{\it Cayley graph} of $\Gamma$ with respect to $S$ is the
oriented graph having vertices $\gamma\in \Gamma$ and oriented
edges $(\gamma,\gamma s)_{s\in S}$.
In this pape... |
1,116,691,501,177 | arxiv | \section{Introduction}
When Onsager solved in \cite{44Onsager} the square-lattice Ising model,
the basic structure of his derivation is an algebraic structure
which is now called the Onsager algebra.
He showed that
the representation of the original Hamiltonian can be reduced into
direct products of two-dimensi... |
1,116,691,501,178 | arxiv | \section{Introduction}
The atomic pair distribution function (PDF) analysis of x-ray and neutron powder
diffraction is growing in popularity with the advent of nanoscience and
nanotechnology. The technique is more than 70 years
old~\cite{debye;pz30,warre;b;xd90,egami;b;utbp03} and was originally applied almost
exclus... |
1,116,691,501,179 | arxiv | \section{Introduction}
Quantum key distribution (QKD) is a technology that allows establishing provably secure keys between legitimate parties~\cite{BB84,Gisin2002,Scarani2009,Lo2014,Lo2016}.
The QKD security is based on the fundamental laws of quantum physics, so QKD remains secure against any unforeseen developments... |
1,116,691,501,180 | arxiv | \section{Introduction}\label{sec:intro}
Long-duration ($t\gtrsim 2~\mathrm{s}$) Gamma Ray Bursts, simply
indicated as GRBs throughout this paper, are widely considered
powerful tracers of the star formation history of the Universe
\citep{bloom2002,chary2007,savaglio09,robertson12}. In fact, their
progenitors are estab... |
1,116,691,501,181 | arxiv |
\section{Introduction} \label{Sec.1}
To explain the observed cosmological matter-antimatter asymmetry, the baryon number $B$ violation is one of three basic ingredients for an initially symmetrical Universe \cite{Sakharov:1967dj}.
The baryon number is necessarily violated in the Grand Unified Theories (GUTs) \cite{Ge... |
1,116,691,501,182 | arxiv |
\section{Introduction}
Consider the initial value problem
\begin{equation}
\label{sys}
y''(t) = f(t,y(t)),\quad
y(0) = y_0,\quad y'(0) = y'_0,\quad
t\in [t_0,\, t_0+T]
\end{equation}
where $f:[t_0,t_0+T]\times \mbox{\rm I\hspace{-.15em}R}\to \mbox{\rm I\hspace{-.15em}R}$ and $f(t,y)$ is continuous with respect to $t$... |
1,116,691,501,183 | arxiv | \section{Introduction}
\label{intro}
One of the popular scenarios of baryogenesis is the spontaneous baryogenesis (SBG) proposed in
papers~\cite{spont-BG-1,spont-BG-2,spont-BG-3}, for reviews see e.g. Refs.~\cite{BG-rev,AD-30}.
It is assumed that in the unbroken phase the theory is
invariant with respect to the glob... |
1,116,691,501,184 | arxiv | \section{Introduction}
\label{intro}
Multi-label learning deals with the problem where each sample is represented by a feature vector and is associated with multiple concepts or semantic labels. For example, in image annotation, an image may be annotated with different scenes; or in text categorization, a document may ... |
1,116,691,501,185 | arxiv | \section{Introduction}
\label{sec:intro}
Topological defects arise in a wide variety of systems ranging from table-top experiments in condensed matter systems\cite{Chuang:1991zz, Hendry:1994,Ruutu:1996,Bauerle:1996,Dodd:1998aan,Carmi:2000zz,Digal:1998ak} to theories of the early Universe,
extremely dense stars e... |
1,116,691,501,186 | arxiv | \section{Introduction}
Microgels are colloid-size particles made by crosslinked polymer networks generally organized into a dense core and a softer, loose corona~\cite{vlassopoulos2014tunable}. They can be synthesized in a range of diameters going from approximately 50 nm to a few microns~\cite{pelton2004unresolved} an... |
1,116,691,501,187 | arxiv | \section{\bf Introduction }
Resonant scattering amplitudes near inelastic thresholds cannot be accurately
described
by the Breit-Wigner formula. About 30 years ago S. M. Flatt\'e proposed the
following parameterization of the $S$-wave $\pi\eta$ and the $\rm K \overline{K}$ production
amplitudes which are dominated... |
1,116,691,501,188 | arxiv | \section{Introduction, Definitions and Notations}
\bigskip Recently, $q$-analysis has served as a structure between
mathematics and physics. Therefore, there is a significant increase of
activity in the area of the $q$-analysis due to applications of the $q
-analysis in mathematics, statistics and physics.
$p$-... |
1,116,691,501,189 | arxiv |
\section{Introduction}
Top quarks are produced in pairs via the strong interaction either from the fusion of two incoming gluons or from the annihilation of an incoming quark and anti-quark at leading order (LO). The interference effects between the Born diagram and the box diagram at next-to-leading order (NLO), as w... |
1,116,691,501,190 | arxiv | \section{Introduction}\label{introduction}
The unprecedented adoption of mobile handhelds has created a host of new services that require accurate localization, even in GPS-denied environments. How to accurately localize without satellite positioning has been an active research topic. Various cooperative localization m... |
1,116,691,501,191 | arxiv | \section{\@ifstar{\starsection}{\nostarsection}}
\newcommand\nostarsection[1]
{\sectionprelude\origsection{#1}\sectionpostlude}
\newcommand\starsection[1]
{\sectionprelude\origsection*{#1}\sectionpostlude}
\newcommand\sectionprelude{%
\vspace{1em}
}
\newcommand\sectionpostlude{}
\makeatother
\newcommand{\mathbb{Q}}{... |
1,116,691,501,192 | arxiv | \section{Introduction \& Context}\label{sec1}
Set covering is a well-known problem in combinatorial optimization. The objective is to cover a set of elements, called the universe, using a minimum number of available covers. The theoretical problem is known to be generally NP-difficult to solve \cite{Vazirani2001}, and... |
1,116,691,501,193 | arxiv | |
1,116,691,501,194 | arxiv | \section{Introduction}
The complexity of the orbital problems that aerospace engineers commonly confront makes that analytical solutions to them remain generally unknown. Because of that, simplified models that may capture the bulk of the dynamics of concern for a particular mission are customarily used in the prelimi... |
1,116,691,501,195 | arxiv | \section{Introduction}
\label{sec:intro}
There is considerable progress in calculations of various cross sections
for deep inelastic lepton scattering in the Lipatov limit ($\nu\to\infty$
and $Q^2$ fixed at a large value \cite{FKL75}). In particular a
picture has been proposed \cite{NZ91,M94} which reproduces the b... |
1,116,691,501,196 | arxiv | \section{DFT Embedding}
Density Functional Theory (DFT) is one of the most powerful tools for the \emph{ab initio} calculation of the physical and chemical properties of materials, being both efficient and accurate.
Many implementations of DFT exist, which differ in the approach taken to approximating the unknown densi... |
1,116,691,501,197 | arxiv | \section{Introduction}\label{sec:intro}
The investigation of super-Poissonian and sub-Poissonian light sources plays a significant role in the history of quantum optics~\cite{hbt1956interferometer,short1983observation}. The photon-number distributions of these sources display variances that are, respectively, wider or... |
1,116,691,501,198 | arxiv | \section{Introduction}
The data-driven modeling of complex systems is currently undergoing a revolution.
There is unprecedented availability of high-fidelity measurements from historical records, numerical simulations, and experimental data, and recent developments in machine learning and compressed sensing make it pos... |
1,116,691,501,199 | arxiv | \section{Introduction}
Globular clusters (GCs) are ubiquitous and apparently obey a universal
formation mechanism \cite{1994ApJ...429..117H} as evidence by the constancy of
the globlar cluster luminosity function (GCLF)
\cite{1991ARA&A..29..543H}. However, this constancy of formation
appears juxtaposed against the env... |
1,116,691,501,200 | arxiv | \section{INTRODUCTION}
\label{sec:Introduction}
High-velocity clouds (HVCs) are clouds in the Galactic halo traveling at high speed relative to the
local standard of rest ($\ga$90~\ensuremath{\mathrm{km}\ \mathrm{s}^{-1}}; \citealt{wakker97}). HVCs play an important role in the
Galaxy, by supplying material to fuel st... |
1,116,691,501,201 | arxiv |
\section{Introduction} \label{intro}
Pillars and globules are probes of the dramatic physical and structural changes
produced as a result of the erosion of the neutral gas at the interface between
\hii-regions and molecular clouds by the ionising radiation from OB-stars.
Expanding ionisation fronts encounter pre... |
1,116,691,501,202 | arxiv | \section{Introduction}
\label{intro}
Generally speaking, a complex system can be understood as a large number of interacting elements whose global behaviour cannot be derived from the local laws that characterize each of its components. The global response of the system can be observed at different scales and the vas... |
1,116,691,501,203 | arxiv | \section{Introduction}
Let $C \subset \PP^2$ be a projective curve of degree $d > 2$ such that all
its singularities are nodes, and let $\nu\colon \hatC \to C$ be the
normalization mapping. For a point $p \notin C$ consider the projection
$\pr_p: C \to \PP^1 = p^\perp$ from $p$; here $p^\perp \subset \mathbb P... |
1,116,691,501,204 | arxiv | \section{Introduction}
On November 8, 2017, ``Drone Integration Pilot Program'' \cite{USprogramm_UAV} was launched under a presidential memorandum from the White House, which aimed at further exploring expanded use of unmanned aerial vehicles (UAVs) including beyond-visual-line-of-sight flights, night-time operatio... |
1,116,691,501,205 | arxiv | \section{Introduction}
\label{sec:intro}
The ongoing experiments at the Large Hadron Collider (LHC) allow us to
enter new terrain at the ${\rm Te\kern -1pt V}$ scale and to search for new physics in
an unprecedented way. In fact, due to the remarkable properties of
supersymmetric (SUSY) extensions of the Standard Mode... |
1,116,691,501,206 | arxiv | \section{Introduction}
With the progress of computers, microscopic simulation methods
have become popular in the heavy-ion reaction studies.
The benefit of microscopic simulation method is
that one can investigate nuclear reactions without making
any specific assumption on the reaction mechanism.
There are many kind... |
1,116,691,501,207 | arxiv | \section{Introduction}
Time-delayed feedback was originally proposed in the context of chaos control \citep{PYR92} as an alternative to the famous OGY method developed earlier by \citet{OTT90}. The idea was to achieve stabilization of unstable periodic orbits (UPOs) by adding, to a chaotic system, a control force in th... |
1,116,691,501,208 | arxiv | \section{A-Posteriori Error Estimator}
\label{sec:a_posteriori}
The model reduction error in the ArbiLoMod has to be controlled.
To this end, an a posteriori error estimator is used
which should have the following properties:
\begin{enumerate}[topsep=0pt,itemsep=-1ex,partopsep=1ex,parsep=1ex]
\item It is robust and ef... |
1,116,691,501,209 | arxiv | \section{Introduction}
Recently, various authors \cite{KLT,KKLR,GKKLR} considered pure $R^2$ theories of gravity coupled to matter.
These theories are particularly interesting also in regard to cosmology because they naturally accommodate for de Sitter universes. While demanding conformal
invariance (Weyl local g... |
1,116,691,501,210 | arxiv |
\section{Introduction}
\label{introduction}
\noindent Malware attacks pose a massive threat to the security of companies and individuals. The average annual cost of malware attacks has increased to \$2.6 million per mid-sized company worldwide \cite{bissell2019}. Anti-malware engines are essential to proactively p... |
1,116,691,501,211 | arxiv | \section{Introduction}
The discovery that the rate of expansion of the Universe is apparently
accelerating was one of the key advances in physical cosmology in
the 1990s (\citealt{Riess1998, Perlmutter1999}). Understanding
the nature of the dynamically dominant dark energy, which is believed
to be responsible for ... |
1,116,691,501,212 | arxiv | \section{Introduction}
\IEEEPARstart{I}{n} recent years, as a kind of optical remote sensing image with high spectral resolution, hyperspectral images (HSIs) have attracted much attention because of their unique properties and the massive information they contain \cite{Li2019}. HSIs have been widely used in mineral ex... |
1,116,691,501,213 | arxiv | \section{Introduction and main results}
\label{s1}
Let $\alpha_1< \cdots <\alpha_p$ be any $p$ distinct real numbers, and let $\rho_1,\dots ,\rho_p$ be positive
numbers. The \textit{generalized Lam\'e equation}\footnote{Usually the term generalized Lam\'e equation refers to such equations in which the $\alpha_j$'s are... |
1,116,691,501,214 | arxiv | \section{\label{sec:introduction}Introduction}
Increasing the channel capacity of wireless systems is an essential demand in the implementation of new generations of telecommunication networks. An attractive way to meet this need without increasing the frequency bandwidth is to utilize photon orbital angular momentum (... |
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