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1,108,101,565,615 | arxiv |
\section{Method}
\label{sec:method}
At every step of active learning, we divide the entire training data by three pools.
At first, the \textit{unlabeled pool} ($\mathcal{P}^o$) contains all the samples that are not labeled yet.
The \textit{labeled pool} ($\mathcal{P}$) consists of the other sa... |
1,108,101,565,616 | arxiv | \section{Introduction}
Numerous astrophysical observations, such as galaxy rotational curves \cite{1980ApJ...238..471R,1982ApJ...261..439R}, velocity dispersions \citep{1976ApJ...204..668F}, and gravitational lensing \citep{Massey:2010hh} reveal the existence of invisible matter, the so-called dark matter. In combinat... |
1,108,101,565,617 | arxiv | \section*{Introduction}
Semiconductor avalanche photodiodes (APD's) are versatile for weak light detection, with applications from remote ranging\cite{Wehr1999,Schreiber1999}, quantum communication \cite{yuan2018} and fluorescence lifetime imaging\cite{Damalakiene2016} to optical time-domain reflectometry \cite{Healey... |
1,108,101,565,618 | arxiv | \section{Introduction}
Perturbation theory for gauge theories at finite temperature suffers from
infrared singularities and gauge dependent results for physical quantities.
These problems are avoided by using an effective perturbation theory
(Braaten-Pisarski method \cite{ref1}) which is based on the resummation
of ha... |
1,108,101,565,619 | arxiv | \section{Introduction}
The discovery of the Higgs boson with a mass of about 125~GeV \cite{Atlas:2012gk,CMS:2012gu} has a strong impact on the parameter range of supersymmetric models. In particular in the Constrained Minimal Supersymmetric Standard Model (CMSSM) large regions of the parameter space are not consistent ... |
1,108,101,565,620 | arxiv | \section{Introduction}\label{s1}
\hskip\parindent John and Nirenberg \cite{jn61} introduced the {\it
space ${\mathrm {BMO}\,}(\rn)$}, which is defined to be the space of
all $f\in L_{\rm loc}^1(\rn)$ such that
$$\|f\|_{\rm BMO\,(\rn)}\ev\sup_{{\rm ball}\ B\st\rn}\frac1{|B|}
\int_B|f(x)-f_B|\,dx<\fz,$$
where and... |
1,108,101,565,621 | arxiv | \section*{Theory of cascaded-mode resonances}
The functionality of electromagnetic resonators can be understood from the constructive interference of waves---creating resonant modes. A crucial parameter that determines these modes is the round-trip phase $\Delta \phi$, accumulated by the field after completing one roun... |
1,108,101,565,622 | arxiv | \section{Introduction}\label{introduction}
Let $f = \sum_{j = 0}^d a_j X^j\in \mathbb{R}[X]$ be a univariate polynomial
of degree $d \in \mathbb{Z}^+$. It is a classical result due to
Newton (see \cite{HLP}, \S2.22 and \S4.3 for two proofs) that
whenever all the roots of $f$ are real, then the coefficients of $f$
s... |
1,108,101,565,623 | arxiv | \section{Introduction}
\label{sec:introduction}
The COVID-19 pandemic is an ongoing epidemic of the coronavirus disease~\cite{cao2020covid}. The epidemic was declared a public health emergency of international concern by the World Health Organization (WHO) and it is impacting all aspects of life. At the same time, the ... |
1,108,101,565,624 | arxiv | \section{Preliminaries}
The configuration space $\Ga :=\Ga _{\R^d}$ over $\R^d$,
$d\in\N$, is defined as the set of all locally finite subsets of
$\R^d$,
\begin{equation}
\Ga :=\left\{ \ga \subset \R^d:\left| \ga_\La\right|
<\infty \text{ for every compact }\La\subset \R^d\right\} ,
\end{equation}
where $\left| \cdot \... |
1,108,101,565,625 | arxiv | \section{Introduction}
\input{text/1.introduction}
\section{Materials and Methods}
\input{text/2.method}
\section{Results}
\input{text/3.results}
\section{Analysis and Discussion}
\input{text/4.discussion}
\section{Conclusion}
\input{text/5.conclusion}
\section{Acknowledgements}
This study was supported in pa... |
1,108,101,565,626 | arxiv | \section{Introduction}
For time to event outcomes, hazard models are convenient because they allow for straightforward regressions on covariates. Nevertheless, it is well-known that estimates on the hazard scale, e.g.\ hazard ratios (HRs), are hard to interpret causally \citep{robins1989probability, greenland1996absenc... |
1,108,101,565,627 | arxiv | \section{Introduction}\label{s1}
\IEEEPARstart{G}raph-based representations have been widely employed to model and analyze data that lies on high-dimensional non-Euclidean domains and that is naturally described in terms of pairwise relationships between its parts~\cite{DBLP:conf/nips/DefferrardBV16,DBLP:journals/tnn/Z... |
1,108,101,565,628 | arxiv | \section*{Executive Summary}
The document at hand describes the physics case, the key
experiments proposed and the technical solution for the project ``WASA at
COSY'', which concerns the transfer of the WASA pellet-target and
detector system from CELSIUS (TSL, Uppsala, Sweden) to COSY (FZJ,
J\"ulich, Germany) and its ... |
1,108,101,565,629 | arxiv | \section{Analytical Insights from $2 \times 2$ MIMO}
In this section, we provide detailed insight regarding quantization via the $2 \times 2$ system. By analysis of a limiting noiseless regime, we prove that phase-only quantization cannot yield unique decodability, while amplitude-phase quantization can.
\subsection... |
1,108,101,565,630 | arxiv | \section{Introduction}
\label{sec:introduction}
Let $\Gr = (\Gr,+)$ be an abelian group.
For two sets $A,B\subseteq \Gr$ define the {\it sumset} as
$$A+B := \{ x\in \Gr ~:~ x=a+b \,,a\in A\,,b\in B \}$$
and, similarly, the {\it difference} set
$$A-B := \{ x\in \Gr ~:~ x=a-b \,,a\in A\,,b\in B \} \,.$$
Also... |
1,108,101,565,631 | arxiv | \section{Introduction}
The classical Ericksen-Leslie
theory (\cite {Er}, \cite
{Le}) successfully describes the dynamic
flow of uniaxial nematic liquid crystals. In \cite{BE94}, Beris-Edwards pointed out that the Ericksen-Leslie
flow theory has a limited domain of applications to liquid crystals. Therefore, base... |
1,108,101,565,632 | arxiv | \section{Introduction}
\label{intro}
The investigation of the physical mechanisms for the generation of ocean waves by wind has a long history which starts at the beginning of the 20th century~\cite{1925RSPSA.107..189J}
and is still ongoing. The problem is highly
nonlinear~\cite{JanssenBook} and the feedback at the ... |
1,108,101,565,633 | arxiv |
\section{Case study: Toy bars data}
To understand how different training objectives impact both predictive
performance and interpretability of topic-word parameters, we consider
a version of the toy bars dataset inspired by
\cite{griffiths:2004:fst}, but changed so the optimal $\phi$ parameters are distinct for unsupe... |
1,108,101,565,634 | arxiv | \section{Introduction}
Continuing theoretical advances in lattice gauge theory, especially in chiral fermion formulations and fermion simulation algorithms, and increasing computational resources are making systematic continuum extrapolation
of many QCD quantities without uncontrolled systematic error a reality.
RBC ... |
1,108,101,565,635 | arxiv |
\section*{Acknowledgements}
The research leading to these results is supported by the SmartData@PoliTO center for data analysis and Big Data technologies.
\biboptions{sort&compress}
\small
\bibliographystyle{ieeetr}
\section{Introduction}
\label{sec:intro}
Year by year, new services are born as the Internet connec... |
1,108,101,565,636 | arxiv | \section{Motivation and Examples}
If ${\mathbf{C}}$ is a category then a functor $$F : {\mathbf{C}}^{\mathrm{op}} \to {\mathbf{Set}}$$
also called a ``presheaf over ${\mathbf{C}}$'' is most naturally considered as a ``set
varying over ${\mathbf{C}}$''. Of course, one may consider also contravariant functors
on ${\mat... |
1,108,101,565,637 | arxiv | \section*{APPENDIX}
\bibliographystyle{./IEEEtranBST/IEEEtran}
\section{Methods}
\label{sec:methods}
Our proposed shape estimation method is a learned multi-view shape estimation from grayscale images.
First, different views of the desired object are captured by two cameras.
Then, unnecessary information in the i... |
1,108,101,565,638 | arxiv | \subsubsection{The Model}
As mentioned earlier, several candidates for pairing of unequal Fermi surfaces have been proposed in the literature. The Sarma phase~\cite{Sarma} and the prior version of the BP phase~\cite{Wilczek1}, are unstable~\cite{Heron1,Heron2,Wilczek3}, and will not be considered. Regarding the LOFF s... |
1,108,101,565,639 | arxiv | \section{Introduction}
\PARstart{S}{hape} decomposition is a fundamental problem in geometry processing where an arbitrary object is regarded as an arrangement of simple primitives \cite{Kaick2015ShapeAnalysis, Zhou2015GeneralizedDecomposition} or semantic components \cite{Au2008SkeletonContraction, Berretti20093DGraph... |
1,108,101,565,640 | arxiv | \section{Introduction}
In a 1990 paper \cite{Knuth90} Knuth introduced the class of nested
CNF formulas and showed that their satisfiability can be decided in
polynomial time. A CNF formula is \emph{nested} if its variables can
be linearly ordered such that there is no pair of clauses that
\emph{straddle} each other;... |
1,108,101,565,641 | arxiv | \section{Introduction}
\label{sec:1}
The self-gravitating collisionless fluid dynamics (SG-CFD) is the study of motion of collisionless matter under the influence of its own gravity. A typical example is the large-scale gravitational collapse of collisionless system \citep{Lukic:2007-The-halo-mass-function--High-r}. Th... |
1,108,101,565,642 | arxiv | \section{Introduction}
The electromagnetic signature of core-collapse supernovae has been
exploited comprehensively and thoroughly by countless observations
during the past decades, providing only indirect information about the
explosion mechanism, however. The up to now only recorded neutrino
signal of a core-collaps... |
1,108,101,565,643 | arxiv | \section{\label{intr}Introduction}
Recently, a new Eddington-inspired theory of gravity with a Born-Infeld like structure \cite{Born:1934gh} has been proposed by Banados and Ferreira \cite{Banados:2010ix} (see also \cite{Deser:1998rj,Vollick:2003qp,Wohlfarth:2003ss,Nieto:2004qj,Comelli:2005tn,Vollick:2005gc,Zinoviev:2... |
1,108,101,565,644 | arxiv | \section{Introduction}
Frustrated magnetic systems are characterized by competing magnetic interactions, which allow for a number of different, yet energetically nearly degenerate, magnetic states.
As a result, already a subtle perturbation, e.g., a weak additional interaction or anisotropy, can completely change the ... |
1,108,101,565,645 | arxiv | \section{\bf Introduction}
\label{sec:intro-jja}
The physics of Josephson junctions arrays (JJA) has been a subject of
significant interest in the last ten years \cite{mooij-schon}. A large
number of studies, both experimental
\cite{mooij_van-wees_geerligs_peters_fazio_schon,van-der-zant_geerling_mooij-92,tighe-tuom... |
1,108,101,565,646 | arxiv | \section{Introduction}
The ability to focus, trap, and guide the propagation of waves on subwavelength scales is of fundamental importance in physics. Systems of subwavelength resonators have, in particular, been shown to have desirable and sometimes remarkable properties thanks to their tendency to interact very str... |
1,108,101,565,647 | arxiv |
\section{Centralised Sparse Representation}\label{sec:csr}
\vsp
A different approach to take into account self similarities in sparse models is
the CSR approach of \cite{dong2012nonlocally}. This approach
is easier to turn into a differentiable algorithm than the LSSC method, but we have
empirically observed that it ... |
1,108,101,565,648 | arxiv | \section*{Introduction}
\ssec{} Let $G$ be a simple complex algebraic group and $B$ its Borel
subgroup. Consider the category $\on{D}(G/B)\mod$ of left D-modules on
the flag variety $G/B$. The Lie algebra $\fg$ of $G$, and hence its
universal enveloping algebra $U(\fg)$, acts on the space
$\Gamma(G/B,{\mc F})$ of glob... |
1,108,101,565,649 | arxiv | \section{Introduction}
Masses of thin actinide samples, often a mix of several isotopes, are routinely inferred by counting spontaneously emitted $\alpha$-particles with silicon detectors or gas-based 2$\pi$ or 4$\pi$ counters \cite{Pomme2007}. Traditionally,
when measurements of actinide sample mass have been used to... |
1,108,101,565,650 | arxiv | \section{Introduction}
\label{intro}
Formation and evolutionary processes of stellar and planetary
systems are
expected to leave their imprint on the present-day systems. One
such imprint is the stellar obliquity, the angle between the
stellar spin axis and the orbital angular momentum axis, also
referred to as the sp... |
1,108,101,565,651 | arxiv | \section{introduction}
The exploration of the connection between statistical mechanics and
quantum information has been extensive in recent years since the
work \cite{preskill}. Especially the research of entanglement in
many-body systems has contributed to the comprehensive crossover
between the two hot areas \cite{af... |
1,108,101,565,652 | arxiv | \section{Introduction}
The most well-known theory for describing the mechanism behind
superconductivity from microscopic perspective is the BCS theory proposed by
Bardeen, Cooper and Schrieffer. According to BCS theory, the condensation of
Cooper pairs into a boson-like state, at low temperature, is responsible for
in... |
1,108,101,565,653 | arxiv | \section{Introduction}
Liouville type theorems for several kinds of nonlinear elliptic equations in half space have already been extensively studied. For the semilinear elliptic equation $-\Delta u=|u|^{p-2}u$ in $\mathbf R_+^n$ with zero-Dirichlet boundary condition when $n\geq3$ and $2<p<2n/(n-2),$ Gidas and Spruck ... |
1,108,101,565,654 | arxiv | \section{Introduction}
Hypergeometric series with noncommutative parameters and argument,
in the special case involving square matrices, have been the subject
of recent study, see e.g.\ the papers by Duval and Ovsienko~\cite{DO},
Gr\"unbaum~\cite{G}, Tirao~\cite{T}, and some of the references
mentioned therein. Of cou... |
1,108,101,565,655 | arxiv | \section{Conclusion}
In this paper, we proposed $\mu$-cuDNN, a wrapper library for cuDNN , which divides the mini-batch to utilize high-performance convolution algorithms with limited amount of memory for workspace.
We have shown that $\mu$-cuDNN \ works well even with recent CNNs, which are composed of many convolutio... |
1,108,101,565,656 | arxiv | \section{Introduction}
\label{sec:intro}
The flavor changing processes in the ${s}-{b}$ sector are sensitive probe
of new physics (NP) beyond the standard model (SM) because they are experimentally the
least constrained.
In the minimal supersymmetric standard model (MSSM), however, the
flavor mixing in the chirality f... |
1,108,101,565,657 | arxiv | \section{Introduction}
The mass metallicity relationship (MZR) is an important galaxy scaling relation that describes the coevolution of galaxies and their metal content~\citep[e.g.][]{Tremonti2004}.
Over the past several years, observational results have begun to indicate that the scatter in the MZR may be correlated ... |
1,108,101,565,658 | arxiv |
\section{Introduction}
\label{sec:intro}
Rapid shifts in technology and business models have led to a mismatch between the skills needed by employers and the skills possessed by the labor force. It has been estimated that this mismatch will seriously hinder progress on climate change and reduce manufacturing output by... |
1,108,101,565,659 | arxiv | \section{Introduction}\label{sec:intro}
Classification of phases of matter has been one of the most fundamental
problems in the physics of many-body systems.
Different phases of matter have been classified by their symmetries,
which led to the theory of spontaneously
symmetry breaking~\cite{landau1937theory, ginzbur... |
1,108,101,565,660 | arxiv | \section*{1 Introduction}
Problems associated with large order behaviour of perturbation series
coefficients were examined in many papers. It was F.Dyson \cite{D} who
argued in 1952 that perturbation series in quantum field theory diverges.
Asymptotics of coefficients at high orders which is useful, for example,
for ... |
1,108,101,565,661 | arxiv | \section{Introduction}
\IEEEPARstart{I}{n} recent years, we can observe an increase in the global facial recognition market size, mainly due to the growth of importance of the surveillance industry, investment by the government and defense sector and increasing technological advancement across industry verticals~\cite... |
1,108,101,565,662 | arxiv | \section{Introduction}
The 6.4 keV Fe K$\alpha$ emission line has long been known to
be an important diagnostic of the material accreting onto supermassive black holes.
The Compton reflection hump, frequently seen in Seyfert spectra above
$\sim$7~keV and peaking near 20--30 keV (Pounds et al.\ 1990), indicates that ... |
1,108,101,565,663 | arxiv | \section{Introduction}
The quest for quantum computer with intrinsic fault tolerance spurs
recent interest in searching for exotic fractional quantum Hall (FQH)
states that support non-Abelian anyons~\cite{nayak08}. While it is
easy to write down a trial wave function with highly nontrivial
statistics, the realization... |
1,108,101,565,664 | arxiv | \section{Introduction}
In this contribution I would like to discuss some of the conceptual
and physical issues surrounding the approach to noncommutative
geometry coming out of quantum groups and braided groups, in
somewhat greater depth than I had time for in my lecture in Goslar.
The discussion is intended to be int... |
1,108,101,565,665 | arxiv | \section*{Acknowledgements}
The authors wish to acknowledge the support of the grant DEC-2012/06/A/ST2/00389 from the National Science Centre Poland.
\bibliographystyle{unsrt}
|
1,108,101,565,666 | arxiv | \section{Introduction}
Figure \ref{fig:teaser} shows a high scoring detection from an object detector
with HOG features and a linear SVM classifier trained on a large database of
images. \changed{\emph{Why} does this detector think that sea water looks like a car?}
\begin{figure}
\centering
\includegraphics[width=\l... |
1,108,101,565,667 | arxiv | \section{Introduction}\label{Sec1}
We define ${\mathcal Q} _n(w)$ (where $n \ge 1$ and $-1 <w < \frac{1}{n-1}$)
as in the Abstract, and let
${\mathcal O} _n := {\mathcal Q} _n(0)$,
${\mathcal P} _n := {\mathcal Q} _n(\frac{1}{n})$.
Hadwiger~\cite{Hadw1951} showed in 1951
(see also Hertel~\cite{Hert2003})
that ${\m... |
1,108,101,565,668 | arxiv | \section{Introduction}
This paper is devoted to a study of conservation laws and symmetries
for a class of time-dependent generalized Korteweg-de Vries equations
\begin{equation}\label{gkdv}
u_t +f(t,u)u_x + u_{xxx} =0
\end{equation}
with
\begin{equation}\label{conds}
f|_{u=0}=0,
\quad
f_{u}\neq 0 .
\... |
1,108,101,565,669 | arxiv | \section{Introduction}
The rise of antiferromagnetic spintronics~\cite{Baltz2018} brought about renewed interest in 'old' materials where aspects previously disregarded have now become important.
One of the those materials, which has been known~\cite{Bronger1986} to be an antiferromagnet (AFM) since 1980's and has onl... |
1,108,101,565,670 | arxiv |
\section{Method}
\label{sec:approach}
We propose a novel end-to-end framework for cross-domain label-adaptive stance detection. Our architecture (see Figure~\ref{fig:approach:moe}) is based on input representations from a pre-trained language model, adapted to source domains using Mixture-of-Experts and domain adve... |
1,108,101,565,671 | arxiv | \section{Introduction}
\label{sec:intro}
The present 3\% experimental precision on $\mathcal{B}(\pi^0_\text{D})$\footnote{%
We use the shorthand notation $\pi_f^0\coloneqq\pi^0\to f$, with $\text{D}\coloneqq e^+e^-\gamma$ and $\text{DD}\coloneqq e^+e^-e^+e^-$.
}~\cite{Tanabashi:2018oca} represents a limitation for rar... |
1,108,101,565,672 | arxiv | \section{introduction}
In this work, we consider the problem of Quantitative Group Testing (QGT). Consider a set of $N$ items among which $K$ items are defective. The QGT problem is to identify (all or a sufficiently large fraction of) the defective items, where the result of a test reveals the number of defective item... |
1,108,101,565,673 | arxiv | \section{Introduction}
Magnetism and superconductivity appear nearby in typical phase diagrams of transition-metal and heavy-fermion compounds.
Magnetism is related to the Mott insulating state and heavy-fermion formation, which can be described in terms of local correlations.
On the other hand, unconventional super... |
1,108,101,565,674 | arxiv | \section{Introduction}
\label{section:introduction}
Radio relics appear as diffuse synchrotron radio sources in the peripheral regions of some merging or cool-core clusters, typically showing an elongated morphology with a linear extent and strong polarization up to the 30\% level in integrated linear measurement \cite... |
1,108,101,565,675 | arxiv | \section{#1}}
\newcommand{\sect}[1]{{\bf{#1.} }}
\begin{document}
\title{Categorization of two-loop Feynman diagrams in the $\mathcal O(\alpha^2)$ correction to $e^+e^- \rightarrow ZH$
\thanks{This work was supported by the National Natural Science Foundation of China under Grant No. 11675185 and 12075251.}
}
\autho... |
1,108,101,565,676 | arxiv | \section{Introduction}
The following theorem is one of the main results of this paper.
Our proof of Theorem \ref{f-thm1.1}
uses the framework of the toric Mori theory developed by
\cite{reid}, \cite{fujino-notes},
\cite{fujino-equiv}, \cite{fujino-osaka}, \cite{fujino-sato}, and so on.
\begin{thm-a}[Theorem \ref... |
1,108,101,565,677 | arxiv | \section{#1}}
\newcommand{\newsubsection}[1]{\setcounter{equation}{0}
\setcounter{dfn}{0}
\subsection{#1}}
\renewcommand{\theequation}{\thesection.\arabic{equation}}
\newtheorem{dfn}{Definition}[section]
\newtheorem{thm}[dfn]{Theorem}
\newtheorem{lmma}[dfn]{Lemma}
\newtheorem{ppsn}[dfn]{Proposition}
\newtheorem{crlre... |
1,108,101,565,678 | arxiv | \section{Introduction}
We introduce a random graph $\ensuremath{\mathcal G}$, called \emph{Poisson $h$--generalized Boolean model}, with vertexes in ${\ensuremath{\mathbb R}} ^d$ where
$d\geq 2$,
whose construction depends on a structural symmetric function $h(\cdot, \cdot)$ with real entries, a parameter $\l>0$... |
1,108,101,565,679 | arxiv | \section{Introduction}
Point processes serve as canonical models for dealing with support estimation. Poisson point processes (PPP) appear in the continuous limit of nonparametric regression models with one-sided or irregular error variables, cf. Meister and Rei\ss\ \cite{Meister13}, and thus form counterparts of the ... |
1,108,101,565,680 | arxiv | \section{Introduction}
In the NLP literature, neural networks generally conduct a fixed number of computations over all words in a sentence, regardless of whether they are easy or difficult.
In terms of both efficiency and ease of learning, it is preferable to dynamically vary the numbers of computations according to t... |
1,108,101,565,681 | arxiv | \section{Introduction}
Methods for prediction of instability and transition have evolved considerably during the past several decades. Advances, driven by increases in computer speed and memory, include the availability of high-fidelity DNS and LES solutions for canonical wall-bounded flows \citep{sayadi2013direct}, ... |
1,108,101,565,682 | arxiv | \section{Discussion}
\label{sec:conclusion}
In this paper, we propose a novel self-supervised prior with a joint-level spatial-temporal layer for recovering human motions from monocular occluded videos. For better generalization ability, we represent the human motion in 2D maps, and thus we can employ a lot of non-oc... |
1,108,101,565,683 | arxiv |
\subsection{Authentication in Disk Drive}
\vspace{-0.15in}
\subsection{Disk-level Access-Control}
\label{sec:auth_disk}
{\textsc{Key-SSD}}
implements a disk-level access-control mechanism where unauthorized requests are denied by the disk drive.
Access authentication is performed using
such computational resources ... |
1,108,101,565,684 | arxiv | \section{Introduction} \label{SEC:intro}
Charles Babbage was an English mathematician, philosopher, inventor, mechanical engineer, and ``irascible genius'' who pioneered computing machines \cite{babbagebio,beyer,grabiner,moseley,mactutor,odonnell}.
Although he held the Lucasian Chair of Mathematics at Cambridge Univer... |
1,108,101,565,685 | arxiv | \section{Security Analysis}
\subsection{Outline}
We begin our security analysis by describing how we model the honest and dishonest scenarios, i.e.~what assumptions are made on the devices used to execute the protocol. In Section~\ref{sec:fault-tolerant-rbc} we describe a generalized protocol, in which the states emi... |
1,108,101,565,686 | arxiv | \section{Introduction}\label{Intro}
Normal polytopes show up in various contexts, including algebraic geometry (via toric varieties), integer programming (integral Carath\'eodory property), combinatorial commutative
algebra (quadratic Gr\"ob\-ner bases of binomial ideals), and geometric combinatorics (Ehr\-hart theory... |
1,108,101,565,687 | arxiv | \section{Introduction}
Ever since Black, Merton, and Scholes introduced their celebrated option valuation formula~\cite{black:scholes:paper,merton:bspaper} a great deal of effort has been dedicated to reproduce that result using more realistic stochastic models for the underlying asset. In the discrete time modeling ... |
1,108,101,565,688 | arxiv | \section{\qquad Introduction}
This work was originally motived by mathematical proofs that a positive
frequency field cannot be confined to a finite region of space. According to
the Hegerfeldt theorem a positive frequency field localized in a finite region
for an instant spreads immediately throughout space \cit... |
1,108,101,565,689 | arxiv | \section{ALGORITHM}\label{sec:algo}
The key assumption that motivates RNM is a smoothness condition
that goes beyond the standard assumptions in the optimization literature, where smoothness would be characterized by a symmetric quadratic with the radius $L$. Instead, Assumption \ref{ass:smooth} below is... |
1,108,101,565,690 | arxiv | \section{Introduction}
Two-player games on finite graphs which admit infinite plays are of fundamental importance in many areas of logic and computer science, especially in the
formal analysis of reactive systems, where they model the non-terminating interaction between a system and its environment.
In such a game, t... |
1,108,101,565,691 | arxiv | \section*{Introduction: a new tool for nanotechnology}
Although based on physical principles it should be possible to assemble matter atom-by-atom, only few attempts at such manipulation have been successful. The first and so far only methods to truly achieve this goal are scanning probe microscopies (SPM), scanning t... |
1,108,101,565,692 | arxiv | \section{Introduction}
Active galactic nuclei (AGNs) are classified as type-1 or type-2, depending on the presence or absence of broad optical emission lines. The existence of different classes of AGNs can be explained by the unified model \citep{Antonucci1993}, which is based on the orientation of the optically thick ... |
1,108,101,565,693 | arxiv | \section{Introduction}
\label{sec:intro}
More and more research institutes and scientists consider attaching camera to Autonomous Underwater Vehicles (AUVs) and Remotely Operated Vehicles (ROVs) in order to perform different underwater tasks, such as marine organism capturing, ecological surveillance and biodiversity... |
1,108,101,565,694 | arxiv | \section{Introduction}
We describe FAR (Forward Abstracted Reachability), an algorithm for
fully automatic verification of parameterized software systems. A
parameterized system describes a family of programs such as cache
coherence protocols where the number of processes involved can change
but the algorithm handling ... |
1,108,101,565,695 | arxiv |
\section{Introduction}
Parity games are games played on a directed graph without leaves by
two players, Even (0) and Odd (1). A node has an owner (a player) and an integer
priority. A play is an infinite path in the graph where the owner of a node
chooses which outgoing edge to follow. A play and its nodes is
won by ... |
1,108,101,565,696 | arxiv |
\section{Introduction}
\label{sec:introduction}
Trajectory prediction is a fundamental and challenging task, which needs to forecast the future path of the agents in autonomous applications, such as autonomous vehicles, socially compliant robots, agents in simulators, to navigate in a shared environment.
With multi... |
1,108,101,565,697 | arxiv | \section{Introduction}
One of the possible ways for building completely integrable quantum systems
is the {\it inverse method of separation of variables} based on
the use of the
so-called {\it multi-parameter spectral equations}. The idea is to
interpret these equations as the result of separating variables in ... |
1,108,101,565,698 | arxiv | \section*{List of Accepted Publications}
\begin{itemize}
\item {\em Shai Bagon}, {\bf Boundary Driven Interactive Segmentation}.
Published in the proceedings of the 3$^{rd}$ International Conference on Information Science and Applications (ICISA), 2012.
\item {\em Sebastian Nowozin, Carsten Rother, Shai Bagon, Toby Sh... |
1,108,101,565,699 | arxiv | \section*{Executive Summary}
\section*{Executive Summary}
We propose the development of a muon-proton and muon-nucleus
collider, referred to as a ``muon-ion collider'' (MuIC),
that utilizes the existing hadron accelerator facilities at Brookhaven National Laboratory (BNL), Fermilab, or CERN while seeding, or lev... |
1,108,101,565,700 | arxiv | \section*{Introduction}
\paragraph{}
Observational and numerical data (\citet{ros}) stress the dynamical consideration of spiral arms as for stars have been observed to migrate radially through the spiral arms leaving significant distances between their observed positions and birthregions. It is well known that spiral ... |
1,108,101,565,701 | arxiv | \section{Introduction} \label{sec:intro}
Solar filaments/prominences are one of the most common structures in the corona, which may lead to energetic coronal mass ejections (CMEs) and flares when they erupt \citep{che00,for00,lin00,yan13,xue16,yang17}. They appear at the limb as bright features called prominences. In c... |
1,108,101,565,702 | arxiv | \section{Introduction}
Consider the space $\ensuremath{\mathbb{F}}^n_2$ of dimension $n$ over
the Galois field $\mathbb{F}_2 = \{0,1\}$. A binary \emph{code} of length $n$ is
a subset of $\ensuremath{\mathbb{F}}^n_2$.
The \emph{(Hamming) distance} $d({\bf x}, {\bf y})$ between two codewords
${\bf x}$, ${\bf y}$ is the... |
1,108,101,565,703 | arxiv | \section{Introduction}
Each irreducible representation of a simple Lie algebra is defined by a set of weights which, for rank two algebras, can be conveniently arranged in a two-dimensional weight diagram. These weights result from successive applications of the lowering operators $E_{-\alpha}$ corresponding to the ... |
1,108,101,565,704 | arxiv | \section*{Introduction}
\noindent
Let $G$ be a simple algebraic group with Lie algebra $\g$, $\EuScript U(\g)$ the enveloping algebra, and
$\Phi$ the Killing form on $\g$. If $\h\subset\g$ is a reductive subalgebra, then $\Phi\vert_\h$ is
non-degenerate and $\me:=\h^\perp$ is a complementary $\h$-submodule of $\g$, ... |
1,108,101,565,705 | arxiv | \section{Introduction}
Shape coexistence is a unique phenomenon of the atomic core in which the nucleus displays intrinsically different shapes within a small energy range. Manifestation of this behaviour has been observed all across the nuclear chart, but the neutron-deficient Pb region (\textit{Z}$\leq$82, $N$<126) ... |
1,108,101,565,706 | arxiv | \section{Introduction}
The modelling of financial markets and other social systems by means
of individual-based simulations has attracted a significant amount of
attention in recent years, both in the economics and socio-economics
community, as well as among statistical physicists
\cite{Axelrod,Gilbert&Troitzsch,LLS, C... |
1,108,101,565,707 | arxiv | \section{Introduction}
\label{secct:intro}
Let $X$ be a geometrically integral smooth projective Fano variety over a number field $F$ and let $\mathcal{L} = \mathcal{O}_{X}(L)$ be an adelically metrized big and nef line bundle on $X$. Manin's Conjecture, first formulated in \cite{FMT89} and \cite{BM}, predicts that t... |
1,108,101,565,708 | arxiv |
\section{Introduction}
The neutrino flavor eigenstates are linear combination of the mass eigenstates with the unitary matrix, Pontecorvo-Maki-Nakagawa-Sakata (PMNS) matrix. In the PMNS matrix, the three mixing angles ($\theta_{12}$, $\theta_{23}$, $\theta_{13}$ ) can be measured experimentally. The Daya Bay collabora... |
1,108,101,565,709 | arxiv | \section{Introduction}
Cortical morphology is a useful imaging-based biomarker for a range of applications, including aging and disease. Measures that describe the shape and folding of a brain, such as gyrification and cortical thickness, are being used both over the entire cortex and locally to identify differences i... |
1,108,101,565,710 | arxiv | \section*{Abstract}
It is shown that for any $W$ weakly compact set of a real
Banach space $X$, the set $L_{\infty }(\mu ,W)$ is $N$-simultaneously
proximinal in $L_{\infty }(\mu ,X)$ for arbitrary monotonous norm $N$ in
${\R}^n$.
\section{Introduction}
Throughout this paper, $(X,\|\cdot\|)$ is... |
1,108,101,565,711 | arxiv | \section{Introduction}
{The merging galaxy \object{NGC 6240} has a large
far-infrared (FIR) luminosity of L$_{\rm FIR}$ = 3.5 $\times$
10$^{11}$ \mbox{L$_{\sun}$}\,\citep{yun02} and belongs to the category of luminous
infrared galaxies (LIRGs; L$_{\rm IR}$ = 10$^{11}$$-$10$^{12}$ \mbox{L$_{\sun}$})
\citep[see][for a ... |
1,108,101,565,712 | arxiv | \section{Introduction}
\label{sec:intro}
Mechanism design studies how to achieve a social goal in the presence of
decentralized decision making, and one important subfield is Nash
implementation.\footnote
There are two paradigms in mechanism design: full implementation (e.g., Nash
implementation) and partial i... |
1,108,101,565,713 | arxiv | \section{Introduction}
{Recent years have witnessed a spurt of progress in modern machine learning technology, more effective and complex machine learning models can be trained through large-scale distributed training. However, in each iteration of the distributed optimization, information exchange among distributed ... |
1,108,101,565,714 | arxiv | \section{Introduction}\label{sec: intro}
Optical fibre technology based on silica glass has revolutionised application fields as diverse as telecommunications and manufacturing (e.g. laser cutting and welding) by providing a robust and efficient integrated platform for the generation of visible and near-infrared light... |
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