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541,165,882,756 | arxiv | \section{Introduction}
The continuous development of the experimental techniques for measuring the nuclear $\beta$ decay spectra has recently increased the interest in calculating the atomic corrections for the process. Precise investigations of the $\beta$ spectra are currently used for getting information on some fu... |
541,165,882,757 | arxiv | \section{Introduction}
\bigskip The nuclear many--body problem has been extensively investigated since
several decades. One of the challenges, at a very fundamental level, is the
development of the
nucleon-nucleon (NN) interaction. Several versions of phenomenological and recently
developed chiral effective--field-... |
541,165,882,758 | arxiv | \section{Introduction}
\label{sec:1}
Certain spin chains have been known to model advantageously devices that effect perfectly the transfer of quantum states between locations [1, 2, 3]. Calling upon their dynamics to realize the transport has the merit of minimizing the need for external interventions and of protectin... |
541,165,882,759 | arxiv | \section{Introduction}
Magnetic gradiometry, as a powerful tool for magnetic anomaly
mapping, have been discussed in literature in conjunction with
future planetary and deep space missions (see for example Alves and
Madeira\cite{alves}\cite{acuna}). Although conventional
magnetometers are more commonly deployed on sat... |
541,165,882,760 | arxiv | \section{Introduction}
In this work, we propose kernel density estimators for estimating the invariant density associated to a stochastic differential equation. More precisely, we study the inference for the d-dimensional process
\begin{equation}
X_t= X_0 + \int_0^t b( X_s)ds + \int_0^t a(X_s)dW_s, \quad t \in [0,T], ... |
541,165,882,761 | arxiv | \section{Introduction}
Holographic duality\cite{Witten:1998ty,Gubser:1998fe,Maldacena:1999fk} is a duality proposed between a quantum field theory (the boundary theory) and a gravitational theory (the bulk theory) in one higher dimension.
In 2006, S. Ryu and T. Takayanagi proposed the Ryu-Takayanagi (RT) formula\cite... |
541,165,882,762 | arxiv | \section{Introduction}
The unique extraction of partial-wave scattering amplitudes
and universal baryon-resonance parameters
from experimental data as well as their precise interpretation
in QCD ranks among the most challenging tasks
in modern hadron physics.
During the last decades, an enormous effort
to study b... |
541,165,882,763 | arxiv | \@ifstar{\origsection*}{\@startsection{section}{1}\z@{.7\linespacing\@plus\linespacing}{.5\linespacing}{\normalfont\scshape\centering\S}}{\@ifstar{\origsection*}{\@startsection{section}{1}\z@{.7\linespacing\@plus\linespacing}{.5\linespacing}{\normalfont\scshape\centering\S}}}
\def\@startsection{section}{1}\z@{.7\linesp... |
541,165,882,764 | arxiv | \section{Introduction}
\subsection{Background of wave equations with scale-invariant damping}
In the last two decades, the wave equations with scale-invariant damping have caught a lot of attention. Let us begin with the corresponding linear Cauchy problem with vanishing right-hand side as follows:
\begin{align}\labe... |
541,165,882,765 | arxiv | \section{Introduction}
Multi-label learning is widely used to serve our real life\cite{Montanari2016Selectivity,Mercan2017Multi,Wan2016Mem,Guo2016Human,Wan2017Transductive,Zhang2018Ontological}.
In the field of music classification\cite{Oramas2017Multi}, traditional classification algorithms will classify music into p... |
541,165,882,766 | arxiv | \section{Introduction}
With expanding of new computational technologies and needs of industry
it is vital importance to use efficient computational methods for
simulation of partial differential equations in two and
three-dimensions when computational domains are very large. Domain
decomposition methods attracted a... |
541,165,882,767 | arxiv | \section*{Data availability}
The data that support the findings of this study are available from the corresponding author upon reasonable request.
|
541,165,882,768 | arxiv | \section{Introduction}
The literature is replete with techniques which attempt to estimate
a non-observable probability density function using observed data
believed to be sampled from an underlying distribution. Density estimation
techniques have a long history and run the gamut of histogramming,
Parzen windows \cite... |
541,165,882,769 | arxiv | \section{Introduction}
Convolutional Neural Networks (CNNs) have recently become the par
excellence base approach to deal with many computer vision tasks~\cite{2016_arXiv_Homography,2018_arXiv_descriptors,2018_CVPR_ImClassif,2016_CVPR_YOLO,2017_CVPR_PSPNet,2017_ICCV_EventCaptioning}.
Their widespread use is attributab... |
541,165,882,770 | arxiv | \section*{Introduction}
In the high energy limit of hadron scattering, in the regime where the center
of mass energy is larger than any other available scale, perturbative approach
to processes with high momentum transfer allows factorization
of the cross section into a hard matrix element with initial off-shell glu... |
541,165,882,771 | arxiv | \section*{Introduction}
Our aim is to explore the connection between {\em Ammann tilings}
and symplectic geometry. Ammann tilings are $3D$ analogues of
Penrose rhombus tilings, made of two kinds of tiles: an {\em oblate}
and a {\em prolate} rhombohedron having same edge lengths. The basic
idea underlying this connectio... |
541,165,882,772 | arxiv | \section{Introduction}\label{Intro}
Battery technology development has progressed much more slowly compared to other areas of electronics, and, as a result, batteries are often considered the least green and the most design- and performance-limiting components of any electronic device \cite{armand2008,1251172}. Radica... |
541,165,882,773 | arxiv | \section{Introduction}
When a transition takes place between two distinct phases, the change of heat capacity and other thermodynamic quantities is
consistently understood in a theory of phase transitions \cite{landau}. Often a disordered system such as a liquid forms a
similarly disordered solid glass without a t... |
541,165,882,774 | arxiv | \section{Introduction}
The last few years have changed our view on the evolution of galaxies:
the most distant galaxies (i.e. systems having stellar population)
have been found at $z$=6.68 (Chen et al., 1999)
and radio galaxies at $z$=5.2 (van Breugel et al., 1999).
Some of models suggests that galaxies can start the... |
541,165,882,775 | arxiv | \section{Introduction}
The contributions of this paper are twofold. First, results concerning the asymptotic behavior of a large class of reinforced random walks (RRW) are proved. Second, we present a strongly reinforced random walk, useful to model the path formation phenomenon.
By formation of a path, we mean that... |
541,165,882,776 | arxiv | \section{Introduction and motivation}
Experiments of the heavy-ion collisions have provided a magnificent opportunity to study strongly coupled systems
\cite{experiments}.
An important part of this study is to understand the physics of the thermalization in which the fascinating
state of matter ``quark-gluon plasma''... |
541,165,882,777 | arxiv | \section{Introduction}
\IEEEPARstart{I}{n wireless} communication networks, multiple nodes often
share a common channel and contend for access. To resolve
contention among nodes, many different MAC protocols have been devised and are currently used in international standards
(e.g., IEEE 802.11a/b/g protocols) \cite{WL... |
541,165,882,778 | arxiv | \section{Introduction}
Recently, stochastic noise is not at all a new phenomenon to the scientific and engineering communities.
The representation of the uncertainties by multiplicative noise has attracted a huge amount of research interests in practical systems.
Study in \cite{Elia2005Remote} also shown that stochast... |
541,165,882,779 | arxiv | \section{I. Introduction}
It has been widely accepted that the standard cosmological model ($\Lambda$CDM model) \cite{Book by Dodelson}
is the paradigm of the modern cosmology.
This model makes several observable predictions
which have withstood large quantities of tests by the cosmological observations during th... |
541,165,882,780 | arxiv | \section*{Acknowledgments}
The authors thank Xiao-Liu Chu for fruitful discussions at the beginning of the project.
We gratefully acknowledge financial support from Danmarks Grundforskningsfond (DNRF 139, Hy-Q Center for Hybrid Quantum Networks).
BS acknowledges financial support from Deutsche Forschungsgemeinschaft ... |
541,165,882,781 | arxiv | \section{Introduction}
Generative modeling of images \cite{van2016conditional, goodfellow_generative_2014, gregor2016towards, kingma2016improved, dinh2016density}, audio \cite{oord2016wavenet, mehri2016samplernn}, and videos \cite{kalchbrenner2017video, finn2016unsupervised} has advanced remarkably in the past few ye... |
541,165,882,782 | arxiv | \section{Introduction}
Quantum technology is a class of technology that works by using quantum effects, such as quantum coherence, squeezing, and entanglement, to develop revolutionary techniques. Including quantum computation and algorithm \cite{Feynman1982,Ekert1996,Law2001,DiVincenzo2000}, quantum metrology and sens... |
541,165,882,783 | arxiv | \section{PixLoc Details}
\label{sec:pixloc}
Given an initial pose estimate, a set of database images, and a set of 3D points potentially visible in it, PixLoc~\cite{Sarlin2021CVPR} refines the initial estimate by minimizing a feature-metric error:
PixLoc computes feature maps for the images, projects the 3D points int... |
541,165,882,784 | arxiv | \section{Introduction}
\label{sec:intro}
The Imaging Atmospheric Cherenkov Technique (IACT) uses one or several telescopes to record the Cherenkov light flashes produced by extensive air showers initiated by Very High Energy (VHE, E $>$ 50 GeV) gamma rays in the upper atmosphere. These telescopes typically feature 1-3... |
541,165,882,785 | arxiv | \section{Introduction}
Hardy-Orlicz spaces are a natural generalization of the Hardy spaces. Holomorphic functions on the unit disk in $\mathbb{C}$ belonging to Hardy-Orlicz spaces have been studied in \cite{stoll1}, \cite{khalil}, \cite{deeb1}, and \cite{deeb2}. For the higher dimensional case of holomorphic maps on ... |
541,165,882,786 | arxiv | \section{Introduction. Main result}
Throughout the paper we will work in the following geometric context ---
details may be found in \cite{JarPfl2007}, see also \cite{JarPfl2003a}, \cite{JarPfl2003b}.
We fix an integer $N\geq2$ and let $D_j$ be a (connected) \textit{Riemann domain of holomorphy}
over $\mathbb C^{n_j}$... |
541,165,882,787 | arxiv | \section{Introduction}\label{Sec:Intro}
A fundamental challenge to the broader application of quantum information science is the management of error in fragile quantum hardware~\cite{NC, oskin2002practical}. The need for higher-fidelity performance motivates research at all architectural levels~\cite{JonesPRX2012}, fro... |
541,165,882,788 | arxiv | \section{Related work}
\subsection{Physics-based interaction}
An increasing number of mixed reality applications are using \mbox{realistic} physics, to enhance the user experience and support natural interaction with virtual content. Buchanan~et~al.~\cite{buchanan08} presented an educational augmented reality game, w... |
541,165,882,789 | arxiv | \section{Introduction}
Accurate video segmentation is an important step in many high-level computer vision tasks. It can provide for example window proposals for object detection \cite{girshick15fastrcnn,ren2015faster} or action tubes for action recognition \cite{actiontubes,gkioxari2015wholesandparts}. One of the key... |
541,165,882,790 | arxiv | \section{Introduction}
The fate of the chiral anomaly of quantum chromodynamics (QCD) at finite temperature remains to be understood theoretically. It is well established that at high enough temperature, due to the exponential damping of the instanton density, the anomalous breaking of the $U_A(1)$ subgroup of chiral ... |
541,165,882,791 | arxiv | \section{Introduction}
We consider the transport properties of a two-dimensional (2D)
disordered strip connected to two disorder-free leads, as shown in figure 1.
In the transverse direction, the
system is restricted to a finite width of $W$ by confinement potentials.
The entire system
is subject to a perpendicular... |
541,165,882,792 | arxiv | \section{INTRODUCTION}
IC342 is a nearby (1.8Mpc; see~\citealt{Buta1999} for a review) late-type Sc/Scd galaxy in the Maffei Group which is one of the closest groups to our Galaxy. Its spiral arms are well developed and are almost face-on ($i = 25^{\circ}\pm3^{\circ}$;~\citealt{Newton1980}). Its active star formation a... |
541,165,882,793 | arxiv | \section{Introduction}
Let $k$ be an arbitrary field, and $G$ a $k$-group which is pseudo-reductive; that is, the largest connected smooth normal unipotent $k$-subgroup $\mathscr{R}_{u,k}(G)$ of $G$ is trivial. The classification of $G$ up to isomorphism in \cite{CGP15} and \cite{CP17} becomes exceedingly intricate whe... |
541,165,882,794 | arxiv |
\section{Empirical Evaluation}
\label{sec:experiments}
This section aims to empirically answer three main questions:
\begin{enumerate}
\item How does weighted training affect the latent space of \glspl{dgm}? (\cref{subsec:expt-weighting})
\item How do the parameters of weighted retraining influence optimizatio... |
541,165,882,795 | arxiv |
\section{Proof of Lemma XXX}
\section{Algorithm Details}
\subsection{Pessimistic Value Iteration (PEVI,\citep{jin2021pessimism})}
In this section, we describe the details of PEVI algorithm.
\label{algo_describ}
In linear MDPs, we can construct $\hat\BB \hat{V}$ and $\Gamma$ based on $\cD$ as follows, where $\... |
541,165,882,796 | arxiv | \section{Introduction}
Consider the stochastic differential equation
\begin{equation}\label{main_equation}
X(t) = x_0 +\int_{0}^{t}b(X(s))ds +\sigma B(t)
\textrm{ $;$ }t\in [0,T],
\end{equation}
where $\sigma,T > 0$, $B$ is a fractional Brownian motion of Hurst index $H\in ]1/2,1[$, $b :\mathbb R\rightarrow\mathbb R$ i... |
541,165,882,797 | arxiv | \section{Introduction}
Following our first article \cite{Onay2017}, we extend our definition of valued modules over non-commutative rings of twisted polynomials and study their model theory.
Model theory of valued fields (including additional structures, such as endowed with an automorphism or a derivation) is muc... |
541,165,882,798 | arxiv | \section{INTRODUCTION}
\label{sec:intro}
Using information entirely based on the Solar System obtained by Brahe and Kepler and on Earth experiments by Galilei, in 1687, Newton\cite{Newton1687} suggested an empirically-derived classical law of universal gravitation which is today interpreted to be an effective mathemati... |
541,165,882,799 | arxiv | \section{Introduction} \label{sec:introduction}
The issue of mass segregation in globular and open clusters has been
discussed in the literature for over 20 years. Historically, the first
indicator of mass segregation was simply that the brightest, most
massive cluster members lay closest to the cluster core, whereas ... |
541,165,882,800 | arxiv | \section{Introduction}
\label{intro}
Let $Y$ be a symplectic Calabi-Yau manifold with symplectic form $\omega$, $L\subset Y$ a Lagrangian submanifold and and $\rho$ a symplectomorphism. Using these data, Seidel proposed a method to explicitly construct a complex Calabi-Yau manifold $X$ mirror to $Y$, provided that $X$... |
541,165,882,801 | arxiv | \section{Introduction}
Argumentation is one of the major fields in non-monotonic reasoning (NMR) which has been shown to be very relevant for decision making and for explanation \cite{Toni2019}.
The relationships between preferential semantics of commonsense reasoning \cite{Pearl90,whatdoes,GeffnerAIJ1992,BenferhatIJC... |
541,165,882,802 | arxiv | \section{INTRODUCTION}
\label{sec:intro}
In recent years, there has been considerable work on approaches to task allocation for a large number of homogeneous robots that switch stochastically between tasks at tunable transition rates \cite{berman2009optimized,martinoli2004modeling,mather2014synthesis}. In these approa... |
541,165,882,803 | arxiv | \section{Introduction} \label{sec-intro}
Our understanding of theories of interacting spin-2 fields has experienced significant progress in the past few years. In a development mimicking the way in which interacting spin-1 theories were discovered and explored in the past -- leading from massless Maxwell-like and Yang... |
541,165,882,804 | arxiv | \section{Introduction}
It has been known since Gauss that every complex polynomial $p$ in a single complex variable splits into linear factors, and since Ruffini and Abel that there is no method based on finite concatenation of $n$-th roots to find these factors algebraically in general. Therefore, numerical approxim... |
541,165,882,805 | arxiv | \section{Introduction}
The understanding of the dynamics of supercooled liquids is still
far from being complete
\cite{Debenedetti01,Binder:2005,Dyre:2006,Lubchenko:2006}. A lot of
insight has been gained from simulations . For example, in real
space the microscopic nature of dynamic heterogeneities has been
clarified... |
541,165,882,806 | arxiv | \section*{Introduction}
Parallel convective heat exchangers are relevant in many applicative contexts
such as heating/cooling systems \cite{shah_Dusan_Sekulic_book}, haemodialysis \cite{gostoli_80},
as well as convective heat exchangers \cite{kragh_07}.
A number of works devoted to parallel convective heat ... |
541,165,882,807 | arxiv | \section{Introduction}
There are several notions of exact categories given by Barr, Buchsbaum or Quillen. We study in this article Quillen's \cite{Qu} notion of exact category, which is formulated in the context of an additive category $\mathcal{A}$. One specifies a distinguished class $\mathcal{E}$ of short exact se... |
541,165,882,808 | arxiv | \section{Introduction}
\label{sec1}
Machine learning and data science have entered many domains of human effort in modern times. The number of self-reported data scientists has doubled in recent years \cite{harrison1995validity}. They have entered various domains including academia, industry and business among others.... |
541,165,882,809 | arxiv | \section{Introduction}
The Standard Model (SM) of particle physics involves very minimalistic idea of electroweak symmetry breaking scenario. Consequently SM results with the single real scalar field representing the last experimentally unobserved particle of SM - the Higgs boson. However, being inspired by the famil... |
541,165,882,810 | arxiv | \section{Introduction}
Bannai and Bannai \cite{BB} showed that the association scheme of the complete graph on four vertices is the only primitive symmetric association scheme with a multiplicity equal to three. They also posed the problem of determining all such imprimitive symmetric association schemes. As many prod... |
541,165,882,811 | arxiv | \section{Introduction}
The shell-model or independent particle model (IPM) has been very successful
in describing basic features of nuclear systems. This means that nuclei are
considered as a system of nucleons moving independently in a mean field and
the residual interaction between these particle or quasiparticles i... |
541,165,882,812 | arxiv | \section{Introduction}
Channel capacity is the maximal rate at which communication with vanishing error probability is possible, provided that the length of each codeword is allowed to grow without limit.
Owing to the celebrated Shannon theory \cite{SHA49}, this asymptotic regime of communication is well understood. Si... |
541,165,882,813 | arxiv | \section{Introduction}
\label{sec:level1}
The dynamics of phase transformation by nucleation and subsequent growth of a nucleus of a stable phase is a very old problem, which has been studied for more than half a century~\cite{Christian,Kolmogorov,Johnson,Avrami,Price} from a fundamental point of view as well as from ... |
541,165,882,814 | arxiv | \section{Introduction}
The nuclear reaction of unstable nuclei is of high interest in the
contemporary fundamental physics as well as applied nuclear physics.
The corresponding information from experimental data is always too
sparse or totally lacking. Therefore, during the past few decades,
considerable effort ... |
541,165,882,815 | arxiv | \section{Introduction}
\label{sec:introduction}
The bright evolved star $\gamma$~Cephei ($V = 3.21$, SpT =
K1~III--IV, $\alpha = 23^{\rm h} 39^{\rm m} 21\fs01$, $\delta =
+77\arcdeg 37\arcmin 55\farcs2$, J2000; also known as HD~222404,
HR~8974, HIP~116727) is among the first objects to be subjected to
high-precision r... |
541,165,882,816 | arxiv | \section{Introduction}
Along with substantial progress made recently in designing near-optimal mechanisms for multi-item auctions, interesting structural questions have also been raised and studied. In particular, is it true that the seller can always extract more revenue from a market where the buyers value the ite... |
541,165,882,817 | arxiv | \section{On the hypothesis}
\begin{context}
\label{3.0}
${{\mathscr U}},{\bf F}$ is as in Definition \ref{0.2}.
\end{context}
\begin{notation}
1) $S_\kappa (A)= \{B \subseteq A :|B|<\kappa\}$.
\noindent
2) $A/B$ is free mean $(A,B)\in {\bf F}$.
\noindent
3) $A,B,D$ denote subsets of ${{\mathscr U}}$.
\noindent
... |
541,165,882,818 | arxiv |
\subsection{Properties of the Past-Discounted Payoff}
In \cite{Gimbert07} Gimbert provides a convenient sufficient condition on objectives that ensures positional determinacy in some situations.
If an objective function is both prefix-independent and submixing, as defined below, then there are optimal positional... |
541,165,882,819 | arxiv | \section{Angular Power Spectrum}
\onecolumn
\section{Quadratic estimator}
\label{appendix}
In Section \ref{mlhood}, we reasoned that we would apply the
Newton-Raphson root-finding algorithm (Eq. \ref{eq:newton}) to locate
the peak of the likelihood function (Eq. \ref{eq:like}). We now
continue and evaluate the d... |
541,165,882,820 | arxiv | \section{Introduction}
\label{sec:intro}
In molecular electronics,\cite{Galperin07} many-body correlations are expected to play an important role at low temperatures.\cite{Hewson97,Paaske05}
Transport measurements in such systems can reveal the direct consequences of the local Coulomb interaction or the local electron... |
541,165,882,821 | arxiv | \section{INTRODUCTION}
\subsection{Background}
Recently, robots are used in order to complete tasks instead of humans
in the place where a human cannot enter.
Some of them are full autonomous,
but even in the case of an autonomous robot,
teleoperation is often necessary when the robot is applied to real missi... |
541,165,882,822 | arxiv | \section{Introduction}
\label{sec:Introduction}
Radio galaxies are an important class of extragalactic objects: they represent one of the most
energetic astrophysical phenomena; they may be used as probes of their environments; and they
are unique probes of the early Universe \citep{McCarthy93}.
As the 3CR sample ... |
541,165,882,823 | arxiv | \section{INTRODUCTION}
\label{sec:intro}
Low-mass star-forming galaxies with metallicties of Z$_{\odot}$/10 and
lower\footnote[1]{Throughout this paper, we use the new scale for solar
metallicity, viz., Z$_{\odot}$\ corresponds to 12~+~$\log$~(O/H)~=~8.66 (\citet{Solar04}).}
(i.e., 12~+~$\log$~(O/H)$~\leq~$7.65... |
541,165,882,824 | arxiv | \section{Introduction}
High-temperature (high-$T_{c}$) cuprate super\-conductors \cite{mueller,nagaosa,np} rank
among the most complex materials ever discovered. Despite the rich diversity
within the cuprate family, all compounds share common features such as
the antiferromagnetic Mott insulator phase at zero or small... |
541,165,882,825 | arxiv | \section{#1}}
\newcommand{\be}[1]{\begin{equation}\label{#1}}
\newcommand{\end{equation}}{\end{equation}}
\newcommand{\begin{eqnarray}}{\begin{eqnarray}}
\newcommand{\end{eqnarray}}{\end{eqnarray}}
\def\displaystyle{\displaystyle}
\def \lower .75ex \hbox{$\sim$} \llap{\raise .27ex \hbox{$>$}} { \lower .75ex \h... |
541,165,882,826 | arxiv | \section{Introduction}
\label{sec:intro}
Formulation of discretized supersymmetric Yang--Mills (SYM) theories in a way ensuring compatibility with the lattice is an old problem in lattice field theory. Recent developments based on the ideas taken from topological field theories and also orbifold/deconstruction techni... |
541,165,882,827 | arxiv | \section{Appendix}
\subsection{Simulation of adsorption/desorption isotherms}
To simulate the 3D distribution of water inside the porous network, we setup a lattice gas model\citep{kierlik2001capillary, kierlik2002adsorption,coasne2013adsorption} based on a solid distribution of Ioannidou's \textit{et al.} mesoscale C... |
541,165,882,828 | arxiv | \section{Introduction}
Forecasting financial markets is a tempting challenge for both researchers and investors. It is an intricate task, due to the dynamic, nonlinear and noisy behavior of the markets. In past decades, data mining techniques have been widely used for technical and fundamental analysis in market predic... |
541,165,882,829 | arxiv |
\section{Simulations}
\textbf{Protocol} We implemented a Grand Canonical Monte Carlo Scheme \cite{Frenkel2001}, in which the number of particles $N$ is allowed to vary according to a fixed chemical potential $\mu$.
\textbf{Parameters} Each simulation was carried out in a two-dimensional square box of length $50$ wit... |
541,165,882,830 | arxiv | \section{Introduction}
Alzheimer’s disease (AD) is the main cause of dementia in the elderly. It is symptomatically characterized by loss of memory and other intellectual abilities to such an extent that it affects daily life. Long before memory problems occur, microscopic changes related to cell death take place and s... |
541,165,882,831 | arxiv |
\section{#1}\label{sec:#2}}
\newcommand{\mysubsection}[2]{\subsection{#1}\label{sec:#2}}
\newcommand{\mysubsubsection}[2]{\subsubsection{#1}\label{sec:#2}}
\usepackage{pifont}
\newcommand{\cmark}{\multicolumn{1}{c}{\checkmark}}%
\newcommand{\xmark}{\multicolumn{1}{c}{\scalebox{0.8}{\ding{53}}}}%
\usepackage{adjustb... |
541,165,882,832 | arxiv | \section{Introduction}
Much progress has been made in understanding the black hole solutions of supergravity. This line of enquiry has fed into many important insights, perhaps most notably the microscopic derivation of the Bekenstein-Hawking entropy in string theory \cite{Strominger:1996sh}.
A ubiquitous feature... |
541,165,882,833 | arxiv | \section{Introduction} All spaces considered in this paper are
Tychonoff, i.e., $T_{3\frac{1}{2}}$-spaces. Let $\tau\geq\omega$ denote an infinite cardinal number,
and $\mathbb R^\tau$ the product of $\tau$ copies of the real line with the product topology.
J. F. Kennison defined a space $X$ to be {\em $\tau$-pseud... |
541,165,882,834 | arxiv | \section{Introduction}
Particle mixing and oscillations play a relevant role in high energy physics.
In particular,
in recent years a growing interest in neutrino mixing and
oscillations\cite{BP78}
has been developed which manifests itself both in a strong experimental
effort and in a renewed theoretical research act... |
541,165,882,835 | arxiv |
\section*{Appendix: The Running Example Implementation}
\label{sec:appA}
\subsection*{The SystemC Source Code}
\begin{lstlisting}[caption=The fifo\_if.h,label=lst:fifointerfaces,mathescape]
#ifndef FIFO_IF
#define FIFO_IF
#include <systemc.h>
class fifo_write_if : virtual public sc_interface {
public:
virtual void... |
541,165,882,836 | arxiv | \section{Introduction} \label{introduction}
Liquid metal batteries (LMBs) are among the systems currently discussed for
electrochemical energy storage on the grid level. With growing share
of renewable and volatile sources, as wind and solar, demand for economic
large-scale storage rises. Future energy systems based p... |
541,165,882,837 | arxiv | \section{\label{sec-intro} Introduction}
\begin{figure*}
\centering
\includegraphics[width=0.99\linewidth]{Picture1.pdf}
\caption{\label{fig:hysteresis-loops}
(a) Cross-section schematic of the sample and coordinate system.
(b) Image of the device consisting of 8 converging racetracks.
(c) Hysteresis loop measured by... |
541,165,882,838 | arxiv | \section{Introduction}
\begin{figure}[t]
\begin{center}
\includegraphics[width=3.1in]{plots/module_real_sim2.png}
\caption{\textbf{The EMeRGE module}. The left image is an example of a real EMeRGE module, and the right is our Unity simplification.}
\label{module}
\end{center}
\end{figure}
When co-optimizing morpholog... |
541,165,882,839 | arxiv | \section{Introduction}\label{intro}
Kubert dans son article \cite {Ku79} a introduit le formalisme
des distributions sur $\mathbb{Q}$. Il y d\'emontre aussi
que la distribution ordinaire universelle sur $\mathbb{Q}$
est sans $\mathbb{Z}$-torsion.
La question de l'existence de torsion dans
la distribution ordinaire ... |
541,165,882,840 | arxiv | \section{Introduction}
Many problems in computational science and engineering require
repeated evaluation of an expensive nonlinear parametric map for
numerous instances of input parameters drawn from a probability
distribution $\nu$. These {\em many-query problems} arise in such
problems as Bayesian inference, forward... |
541,165,882,841 | arxiv | \section{Introduction}
\label{s:intro}
A Riemannian manifold $(M,g)$ is called a \emph{geodesic orbit manifold} (or a manifold with homogeneous geodesics, or a GO-manifold) if any geodesic of $M$ is an orbit of a one-parameter subgroup of the full isometry group of $(M,g)$ \cite{KV} (one loses no generality by repl... |
541,165,882,842 | arxiv | \section{Introduction}
Thermal emission measurements taken during secondary eclipse have the potential to reveal information on both the compositions and thermal structures of hot Jupiter atmospheres. The compositions of hot Jupiter atmospheres can be used to track their formation and migration conditions \citep{Ventu... |
541,165,882,843 | arxiv | \subsection{Please Capitalize the First Letter of Each Notional Word in Subsection Title}
\section{Introduction}
\label{sect:intro}
Type Ia supernovae (SNe Ia) represent a kind of high-energy astrophysical phenomena with similar light curves
in the universe. Typically, the peak luminosity of SN Ia, the colo... |
541,165,882,844 | arxiv | \section{Introduction}
One of the main challenges of building practical quantum computing architectures is the implementation of high-fidelity entangling gates at scale. When increasing the quantum processor size, issues such as parasitic couplings from neighboring qubits and frequency crowding can limit two-qubit gate... |
541,165,882,845 | arxiv | \section{Introduction}\label{sec:intro}
IEEE 802.11 Wireless Local Area Networks (WLANs) is becoming an indispensable part of our life, at homes and working places. Due to the problems, such as frame collisions and protocol overheads, the throughput of WLANs is significantly lower than the raw data rate of what the Ph... |
541,165,882,846 | arxiv | \section{Appendix}\label{Appendix}
\subsection{Sketch of the proof of Theorem 1:} According to Picard-Lindelof theorem (see chapter 13, sections 1 and 2 of \cite{nagle1996fundamentals}), to prove uniqueness of solutions, we need to have $\bm{F}$ in (\ref{eqn: ydot}) continuous in $t$ (obtained from A1-A3) and Lipschit... |
541,165,882,847 | arxiv | \section{Introduction}
Let $R$ be a root system, ${\mathscr K}$ a field and $q\in{\mathscr K}$ an invertible element. We denote by $U_{\mathscr K}=U_{({\mathscr K},q)}(R)$ the corresponding quantum group that is obtained via base change from Lusztig's integral form $U_{{\mathbb Z}[v,v^{-1}]}$. This is a triangularized... |
541,165,882,848 | arxiv | \section{Introduction}
Given a set of waypoints to visit and a car-like robot, this article considers two variants of a path planning problem where each waypoint must be visited by the robot and the length of the path traveled by the robot is minimized. Field of view constraints are also placed when the robot arrives ... |
541,165,882,849 | arxiv | \section{Introduction}
The observation of gravitational waves radiated by binary systems of massive astrophysical objects has
opened a new and exciting astrophysical avenue for testing Einstein's
theory of gravity. To unlock the full discovery potential of
gravitational-wave astrophysics, and to keep abreast with mode... |
541,165,882,850 | arxiv | \section{Introduction}
After the discovery of nuclear fission by Hahn and Strassmann~\cite{hahn1939nachweis} in 1939, nuclear fission has become one of the most challenging topics in physics since it is a key ingredient for modeling nucleosynthesis~\cite{Baran2015}, energy production~\cite{Fermi1934}, medicine~\cite{We... |
541,165,882,851 | arxiv | \section{Introduction}
All graphs considered in this paper are simple, finite and
undirected. We follow the terminology and notation of Bondy and
Murty \cite{Bondy}. Let $G$ be a nontrivial connected graph with an
edge-coloring $c: E(G)\rightarrow \{1,2,\ldots,q\}$, $q\in
\mathbb{N}$, where adjacent edges may be c... |
541,165,882,852 | arxiv | \section{Introduction}\label{sec:1}
Random band matrices were introduced many years ago by E.Wigner
\cite{Wigner} as a model Hamiltonian for complicated quantum
systems. In the last few years statistical properties of random band
matrices have become again the subject of intensive analytical and
numerical investigatio... |
541,165,882,853 | arxiv | \section{Introduction}
\label{sect:intro}
Over the past 23 years, the Five-hundred-meter Aperture Spherical radio Telescope (FAST) has been conceived, designed, optimized and constructed to provide a powerful radio tool at low frequencies for the astronomical community (Nan 2006). The active main reflecto... |
541,165,882,854 | arxiv |
\section{Introduction}
By 8 months of age, human infants learn to recognize not only the names of their caregivers and common objects, but also the contrast between the different vowels and consonants which comprise these words~\citep{dupoux18}. Nearly all toddlers learn to carry a conversation long before they ca... |
541,165,882,855 | arxiv | \section{Introduction}
Creating a model of a computer system that can be used for tasks such as predicting future resource usage and detecting anomalies is a challenging problem.
Most current systems rely on heuristics and overly simplistic assumptions about the workloads and system statistics.
These heuristics are ty... |
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