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1,108,101,566,415 | arxiv | \section{Introduction}
FU Ori objects were originally identified as systems in star-forming regions that exhibit large outbursts at optical wavelengths \citep{Ambart1971, Herbig1977, Hartmann1996, Audard2014}. These outbursts have been explained by the onset of rapid mass accretion, rising from quiescent states of 10$... |
1,108,101,566,416 | arxiv | \section{The Kontsevich Integral}
The Kontsevich integral \cite{K} is a functional on knots that can be seen as a generalization of the Gauss integral. It is a graded sum of chord diagrams times some coefficients that are essentially integrals of powers of log differentials. Chord diagrams are the knots used as an arg... |
1,108,101,566,417 | arxiv | \section{Introduction}
Human translators exhibit remarkable generalization capabilities and are able to translate even rare inflections they may have never seen before. Indeed, this skill is necessary for translation since language follows a Zipfian distribution \cite{zipf1949human}: a large number of the tokens in a ... |
1,108,101,566,418 | arxiv |
\section{Prefetcher architecture}
\label{sec:arch}
\begin{figure}[t!]
\centering
\fbox{\includegraphics[width=0.95\columnwidth]{block_diagram.PNG}}
\caption{Semantic prefetcher block diagram (existing core blocks in gray).}
\label{fig:block_diagram}
\vspace{3mm}
\centering
\fbox{\includegraphics[width=0.95\c... |
1,108,101,566,419 | arxiv | \section{Introduction}\label{sec:introduction}}
\else
\section{Introduction}
\label{sec:introduction}
\fi
\IEEEPARstart{T}{his} demo file is intended to serve as a ``starter file''
for IEEE Computer Society journal papers produced under \LaTeX\ using
IEEEtran.cls version 1.8b and later.
I wish you the best of succe... |
1,108,101,566,420 | arxiv | \section{Introduction} \label{s1}
It is well established on theoretical grounds that close
binary stars can have a significant impact on dynamical
evolution of globular clusters (Hut et al. 1992). At the same
time, the theory predicts that large numbers of white/red dwarf
binaries should form in the cores of globular ... |
1,108,101,566,421 | arxiv | \section{Introduction}
The long-term orbital evolution of debris in geosynchronous earth orbit (GEO) has been studied extensively over the past 50 years \cite{allan1964, schildknecht2007, rosengren2019}. Lacking atmospheric drag and other natural de-orbit mechanisms, GEO debris will remain on orbit indefinitely \cite... |
1,108,101,566,422 | arxiv |
\section{Introduction}
The number density of galaxy clusters as a function of mass and
redshift can be used to constrain cosmological parameters and probe
the growth of structure
\citep[e.g.,][]{Henry00,Borgani01,Gladders07,Henry09,Mantz10,Vikhlinin09}.
This approach is conceptually straightforward, but the actual
im... |
1,108,101,566,423 | arxiv | \section{Introduction}
Galaxies have long been seen as islands distantly scattered and stable in the
universe. We now know that galaxies are not randomly distributed in
space. They are in groups that are subject to the expansion of the universe
and mutual gravitational interaction. The interaction between galaxies has... |
1,108,101,566,424 | arxiv | \section{Introduction}
\section{Introduction} \label{sec:INTRO}
One of the bedrock principles of physics is that there is just one
time. Indeed, entertaining multiple timelike directions is
tantamount to jeopardizing the whole edifice of causality.\footnote{With
two timelike directions one automatically has
closed... |
1,108,101,566,425 | arxiv | \section{Introduction}
A kervolutional neural network (KNN) is like a traditional convolutional neural network (CNN) except it uses a 'kervolution' operation instead of a convolution operation\cite{b1}. Kervolution is like convolution, the only difference being that kernel functions are applied to filters and receptive... |
1,108,101,566,426 | arxiv | \section[Introduction]{Introduction}
\label{sec:intro}
In 1950 van~Roosbroeck \cite{roosbroeck50} established a system of
partial differential equations describing the motion of electrons and
holes in a semiconductor device due to drift and diffusion within a
self-consistent electrical field. In 1964 Gummel \cite{gumm... |
1,108,101,566,427 | arxiv | \section{#1}}
\newcommand{\col}[2]{\left(\begin{array}{c} #1 \\ #2 \end{array}\right)}
\newcommand{\fl}[1]{ \lfloor #1 \rfloor }
\newcommand{\ket}[1]{\vert #1 \rangle}
\renewcommand{\mod}[1]{\ (\mathrm{mod}\ #1)}
\newcommand{\new}[1]{{\em #1}}
\newcommand{\rep}[1]{{\bf #1}}
\newcommand{\set}[1]{\{#1\}}
\def \begin{eq... |
1,108,101,566,428 | arxiv | \section{Introduction}
\vspace{-0.5 em}
Relativistic electron-positron (\emph{$e^-e^+$}) pair plasma represents a unique state of matter, which is believed to exist in many extreme astrophysical environments, such as Active Galactic Nuclei (AGN), Pulsar Wind Nebulae (PWN), Gamma Ray Bursts (GRBs), and Black Holes (BHs)... |
1,108,101,566,429 | arxiv | \section{Introduction}
Consider autonomous dynamical system
\begin{equation}
\frac{dy}{dt}=f(y,p)
\end{equation}
where $f:\mathbb{R}^n\times\mathbb{R}^q\to\mathbb{R}^n$ and non-autonomous system
\begin{equation}
\frac{dy}{dt}=f(t,y,p)
\end{equation}
where $f:\mathbb{R}\times\mathbb{R}^n\times\mathbb{R}^q\to\mat... |
1,108,101,566,430 | arxiv | \section{Introduction}
\label{sec:intro}
Magnetic reconnection is a commonly observed fundamental process in
plasmas. It allows topological change of magnetic field lines, and
rapidly converts the free energy stored in the magnetic field into
various forms of energy.
Amongst other poorly understood aspects of magnetic... |
1,108,101,566,431 | arxiv | \section{Introduction}
Traditionally, power distribution systems have been engineered as radial networks that carry power from the utility feeder to the end consumers of electricity. These consumers are seen as a set of passive loads, and generally, the utility has no control of their electricity demand, and does not ... |
1,108,101,566,432 | arxiv | \section{Introduction}
In the context of conventional (classical) error correction,
deletion correction, which was introduced by Levenshtein in 1966
\cite{levenshtein66}, has attracted much attention recently
(see, for example, \cite{sima21} and the references therein).
In the correction of erasures,
the receiver is a... |
1,108,101,566,433 | arxiv | \section{Introduction}
Describing chemical reactions which take place on more than just one electronic potential-energy surface
poses one of the primary open challenges in the field of
chemical reaction dynamics. \cite{Althorpe_2016,Lawrence2019rates}
These processes are relevant to many phenomena which we encounter ... |
1,108,101,566,434 | arxiv | \section{Introduction}
From the very beginning of the invention of Galois theory, one problem has emerged. For a given finite group $G$, find a Galois extension $K/\Q$ such that ${\rm Gal}(K/\Q)\simeq G$. This is still an open problem in spite of the great efforts of a number of mathematicians and substantial progres... |
1,108,101,566,435 | arxiv | \section{Introduction}\label{sec:Introduction}
Multi-agents prediction has been attracting great attention from both industry and academia researchers, due to the practical desire to deal with complex problems. In most of the real-world scenarios, multiple agents are coordinated in different roles but aim at achievin... |
1,108,101,566,436 | arxiv | \section{Introduction}
The spin symmetry energy of neutron matter, defined as the difference between
the energy per particle of spin polarized and unpolarized neutron matter,
is the main ingredient to understand the spin susceptibility of
neutron matter, which is basically proportional to the invers of this quant... |
1,108,101,566,437 | arxiv | \section{Rashba-Anderson Hamiltonian}
The complete Hamiltonian $H=H_c+H_d+H_h$, as described in the main text is given by,
\begin{equation}{\mylabel{eqn:Hamiltonian}}
\begin{split}
H = \sum_{\bk \alpha} \varepsilon_\alpha(\bk) c^\dagger_{\bk \alpha} c_{\bk \alpha} + \sum_{\sigma}{\tilde{\varepsilon}_{d}d_{\sigma}^{\d... |
1,108,101,566,438 | arxiv | \section{Introduction} \label{intro}
Most young stars are surrounded by circumstellar disks, the natural by-product of star formation.
After a protostar has formed, its disk plays a crucial role in the evolution of the system,
first by serving as reservoir for mass accretion, and later by becoming the birthplace of t... |
1,108,101,566,439 | arxiv | \section{Introduction}
Stellar interiors are obvious sites for interesting dynamical phenomena,
with strong potential effects of convection and other forms of instabilities,
rotation and its evolution, as well as magnetic fields,
forming a fascinating playing field for theoretical investigations.
However, `class... |
1,108,101,566,440 | arxiv | \section{INTRODUCTION}
A topological insulator (TI) is a material with the insulating bulk, but with topologically protected gapless surface or edge states
\cite{PhysRevLett.95.146802,PhysRevLett.95.226801,bernevig2006quantum,PhysRevLett.98.106803,PhysRevB.76.045302,PhysRevB.78.045426,PhysRevB.78.195424,RevModPhys.82.3... |
1,108,101,566,441 | arxiv | \section{Introduction}\label{introduction}
\subsection{Anosov maps} Anosov maps are fundamental objects
in the field of dynamical systems. A $C^1$ diffeomorphism $f$ of a
compact Riemannian manifold $M$ is called \textit{Anosov} if there
exist constants $\lambda$ in $(0,1)$ and $c > 0$ along with a
$df$-invariant s... |
1,108,101,566,442 | arxiv | \section{Introduction}
\label{section:intro}
\subsection{Jordan property}
The \textit{Cremona group of rank $n$} is the group $\Cr_n(\Bbbk)$ of birational transformations of
the projective space $\mathbb P^n$ over a field $\Bbbk$.
It has been actively studied from various points of view for many years
(see~\c... |
1,108,101,566,443 | arxiv | \section*{Acknowledgement}
We appreciate the feedback from anonymous reviewers.
MZ is supported in part by the Office of the Director of National Intelligence (\abr{odni}), Intelligence Advanced Research Projects Activity (\abr{iarpa}), via the \abr{better} Program contract \#2019-19051600005. The views and conclusion... |
1,108,101,566,444 | arxiv | \section{Introduction}
A lot of work is being done in recent times to find a suitable system to physically implement qubits, which are the fundamental building blocks of quantum computation. Some of the leading candidates are superconducting qubits, trapped ion qubits, NV$^{-}$ center based qubits etc. One of the leadi... |
1,108,101,566,445 | arxiv | \section{Introduction}
In \cite{ArCa}, the first and third author investigated the $k$-\emph{universal transversal
property}, or $k$-ut property for short, of a permutation group $G$ on
$\Omega$. We say that $G$ has this property if, given any $k$-subset $S$ of
$\Omega$ (subset with $k$ elements), and any $k$-partitio... |
1,108,101,566,446 | arxiv | \section{Problem Definition}
After introducing the general program synthesis paradigm in the previous section, we are now in a position to define the DSL-based program synthesis problem formally. Given a DSL $L$, we aim to learn a synthesis algorithm $A$ such that given a set of text description and its corresponding ... |
1,108,101,566,447 | arxiv | \section{Introduction}
Molecular spectroscopy is a well established discipline and the increasing precision of measurements has provided the capacity to test fundamental physics. Recently, a set of several ``forbidden'' $\Delta k\!=\!\pm 3$ transitions between the rotation-inversion energy levels of $^{14}$NH$_3$ in t... |
1,108,101,566,448 | arxiv | \section{Introduction}
It is by now clear that
$p$--branes are fated to play a central role in the duality relations
occurring in string theories and $M$--theory. Among these dualities an
interesting one is the heterotic string/heterotic five--brane
strong--weak--coupling duality \cite{DUAL}.
Unfortunately until now... |
1,108,101,566,449 | arxiv | \section{Introduction}
Experiments using radioactive beams have brought the development of physics of unstable nuclei.
Neutron halo structure is one of new phenomena of nuclear structures appearing in the drip-line nuclei, such as $^6$He, $^{11}$Li, and $^{11}$Be \cite{tanihata85,tanihata13}.
One of the characteri... |
1,108,101,566,450 | arxiv |
\section{Conclusion}
\label{sec:conclusion}
This paper studied the time required for a random walk to reach one or more nodes in a target set. We demonstrated that the problem of selecting a set of nodes in order to minimize random walk times including commute, cover, and hitting times has an inherent submodular struc... |
1,108,101,566,451 | arxiv | \section{Introduction}
Generative Adversarial Networks (GANs) have shown great promise for the generation of photo-realistic synthetic images ~\citep{goodfellow2014generative, radford2015unsupervised, denton2015deep, salimans2016improved}, and the highly-compelling nature of images generated by GANs has driven research... |
1,108,101,566,452 | arxiv | \section{}
Over the past few years, Spiking Neural Networks (SNNs) have become popular as a possible pathway to enable low-power event-driven neuromorphic hardware. However, their application in machine learning have largely been limited to very shallow neural network architectures for simple problems. In this paper, w... |
1,108,101,566,453 | arxiv | \section{introduction}
Kaluza-Klein black holes, which have compact extra dimensions, are
interesting spacetimes in a class of higher-dimensional black holes.
In particular, there exist a variety of exact solutions of
five-dimensional squashed Kaluza-Klein black holes, which have
squashed S$^3$ horizons
\... |
1,108,101,566,454 | arxiv | \section{Conclusion}
We presented a deep learning technique for estimating 3D human body shape and pose from a single color image. To that end, we propose an iterative training approach that alternates between deformable surface registration and training of deep ConvNets, which gradually improves accuracy of predict... |
1,108,101,566,455 | arxiv | \section*{Introduction}
In a recent paper~\cite{Hetyei-EKP} the present author introduced a
class of progressively finite games played on ranked posets,
where each move of the winning strategy is unique and the positions
satisfy the following uniformity criterion: each
position of a given rank may be reached from the... |
1,108,101,566,456 | arxiv | \section{Introduction}
\label{sec:intro}
The dwarf spheroidal galaxy (dSph) companions of the Milky Way (MW)
are excellent laboratories for investigating the chemical evolution
and star formation histories of dwarf galaxies. These galaxies have
undergone at most a few star formation episodes \citep{hol06} and are
dyn... |
1,108,101,566,457 | arxiv | \section{Introduction}
We assume everywhere $X$ to be a connected, compact polyhedron and $f:X\rightarrow X$ to be a continuous map. Let $p:\tilde{X}\rightarrow X$ be the universal cover of $X$ and $\tilde{f}:\tilde{X}\rightarrow \tilde{X}$ a lifting
of $f$, {i.e.,} $p\circ\tilde{f}=f\circ p$. Two lifts $\tilde{f}$ an... |
1,108,101,566,458 | arxiv | \section{Introduction}
\label{sec:introduction}
Since the late eighteenth century, there have been increased movements toward
equality (\cite{piketty_2022}).
%
{\em Political equality} is one of the most important types of equality.
%
As a core element of political equality,
{\em proportionality in representati... |
1,108,101,566,459 | arxiv | \section{Introduction}%
\label{sec:intro
In models of warm inflation~\cite{Berera:1995wh,Berera:1995ie}, the inflaton interacts with a thermal bath of relativistic particles with a slowly evolving temperature $T$. In order to prevent the temperature from redshifting away, the thermal bath must be continuously replenis... |
1,108,101,566,460 | arxiv | \section{Overview of term structure modeling}
The purpose of this paper is to study the generalized Fong--Vasicek two-factor interest rate model with stochastic volatility. In this model the dispersion of the stochastic short rate (square of volatility) is assumed to be stochastic as well and it follows a non-negativ... |
1,108,101,566,461 | arxiv | \section{Introduction}
Propylene oxide, CH$_3$C$_2$H$_3$O (\textit{alias} methyloxirane or propene oxide), is a stable chiral molecule whose microwave spectrum up to 40 GHz was first reported by Herschbach \& Swalen in 1957 \citep{Swalen.1957,Herschbach.1958}. Its high vapor pressure at room temperature and its comm... |
1,108,101,566,462 | arxiv | \section{Introduction}
\label{sec:intro}
The memristor is the first (and possibly the only) non-linear fundamental circuit element, and, as such, has a lot to offer to those interested in non-linear dynamics. By virtue of being a fundamental element, we can be reasonably certain that it's the simplest non-linear ... |
1,108,101,566,463 | arxiv |
\section{Introduction}
\label{sect:intro}
Gravitationally lensed quasars offer unique insights into a number of cosmological and astrophysical questions \citep[e.g.,][and references therein]{CSS02}. For example, they can be used to infer properties of the quasar host galaxy \citep{Peng:2006p236}, measure the gravitat... |
1,108,101,566,464 | arxiv |
\section{Introduction}
\label{sec:introduction}
The initial discovery of the astrophysical neutrino flux around PeV energies \citep{Aartsen2013} a few years ago marked the beginning of high-energy neutrino astronomy. Since then, its properties have been measured with increasing accuracy \citep{Aartsen2015}. The most ... |
1,108,101,566,465 | arxiv | \section{Introduction}
\begin{center}
\small {Ripple in still water}\\
\small {When there is no pebble tossed}\\
\small {Nor wind to blow}\\
\small {\it -The Grateful Dead}\\
\end{center}
Originally \cite{HarHaw83}, the No-Boundary Proposal was an
attempt to eliminate the initial and final singularities (which are
`b... |
1,108,101,566,466 | arxiv | \section{Introduction}
Conic optimization problems arise frequently when modeling
parametric value-at-risk (VaR) minimization, portfolio optimization, and robust optimization with ellipsoidal objective uncertainty. Although convex versions of these models are solved efficiently by polynomial interior-point algorithms... |
1,108,101,566,467 | arxiv | \section{Introduction}
The classical Enestr\"om-Kakeya Theorem states the following
\begin{thma}
Let $p(z)=\displaystyle{\sum_{j=0}^{n}a_jz^j}$ be a polynomial with real coefficients satisfying $$0<a_0\leq a_1\leq a_2\leq a_3\ldots\leq a_n.$$ Then all the zeros of $p(z)$ lie in $|z|\leq 1.$
\end{thma}
By putting a... |
1,108,101,566,468 | arxiv | \section{Introduction}
Phase transitions in the early Universe may give rise to topological defects \cite{Vilenkin:2000jqa},
which are predicted in a wide range of high-energy physics models of the early Universe \cite{Vilenkin:2000jqa,Jeannerot:2003qv,Sarangi:2002yt,Jones:2003da}.
Defects from symmetry breaking at ... |
1,108,101,566,469 | arxiv | \section{Introduction}
Optimally allocating limited resources is a central problem in economics \citep{samuelson2010economics} and operations research \citep{ward1957optimal, everett1963generalized}. It is often complicated further by uncertainty inherent to the considered problem. On the one hand, future resource cap... |
1,108,101,566,470 | arxiv | \section{Introduction}
It is quite clear that our understanding of the molecular complexity of interstellar and circumstellar environments is rapidly growing. It is also apparent that our understanding of interstellar molecular synthesis is presently incomplete; observations of new interstellar molecules are currently ... |
1,108,101,566,471 | arxiv | \section{2011 Nobel Prize Winners in Physics}
"The Nobel Prize in Physics 2011 was divided, one half awarded to
Saul Perlmutter, the other half jointly to Brian P. Schmidt and
Adam G. Riess for the discovery of the accelerating expansion of
the Universe through observations of distant supernovae." the
nobelpr... |
1,108,101,566,472 | arxiv | \section{Introduction}
\label{sec::introduction}
Inverse differential problems, where given a set of measurements one seeks a set of optimal parameters in a governing differential equation, arise in numerous scientific and technological domains. Some well-known applications include X-ray tomography \cite{epstein2007int... |
1,108,101,566,473 | arxiv | \section{INTRODUCTION}
\label{sec:intro}
The \textit{Lite (Light) satellite for the studies of B-mode polarization and Inflation from cosmic background Radiation Detection} (LiteBIRD) mission\cite{Sugai:article} is the successor of the CMB space missions COBE\cite{COBE:ARTICLE}, WMAP\cite{WMAP:article}, and Planck\ci... |
1,108,101,566,474 | arxiv | \section{Introduction}
Actuator shape is an important design variable for feedback synthesis in control of distributed parameter systems. Optimizing actuator shape can improve performance of the controller and significantly reduces the cost of control. Numerical simulations in \cite{kalise2017optimal} show significant ... |
1,108,101,566,475 | arxiv | \section{Introduction and main results}
\label{sec:intro}
Let $G$ be one of the classical Lie groups
\[
{\mathrm{GL}}_{n}(\mathbb R),\,{\mathrm{GL}}_{n}(\mathbb{C}),\,\operatorname{O}(p,q),\, \operatorname{O}_{n}(\mathbb{C}),\, \operatorname{U}(p,q),
\]
and let $G'$ be respectively the subgroup
\[
{\mathrm{GL}}_{n... |
1,108,101,566,476 | arxiv | \subsection{#1}}
\theoremstyle{remark}
\newtheorem*{remark}{Remark}
\newcommand{\comma}{{},\,}
\newcommand{\col}{\colon}
\newcommand{\bbZ}{\mathbb Z}
\newcommand\Z{\bbZ}
\newcommand{\bbR}{\mathbb R}
\newcommand{\mcA}{\mathcal A}
\newcommand{\mcB}{\mathcal B}
\newcommand{\mcC}{\mathcal C}
\newcomman... |
1,108,101,566,477 | arxiv | \subsection{System partition}
\indent Fluctuations of power flow distribution can be attributed as fluctuation of power injections. Hence in this paper, fluctuation sources are modeled as injections. For fluctuation source $i$, we know its connecting node $k_{i}$, standard error for fluctuation of active and reactive p... |
1,108,101,566,478 | arxiv | \section{Introduction}
\label{sec:intro}
Computer systems are distressingly insecure.
Visiting a website, opening an email, or serving a client request is often
all it takes to be subjected to a control-hijacking attack.
These devastating low-level attacks typically exploit memory-safety
vulnerabilities such as buffer... |
1,108,101,566,479 | arxiv | \section{CCQE event selection in MiniBooNE}
The MiniBooNE\footnote{The mini-Booster neutrino experiment (MiniBooNE)
at Fermi National Accelerator Laboratory (Fermilab)
is designed to search for
$\nu_\mu \rightarrow \nu_e$
appearance neutrino oscillations~\cite{MB_osc}.} detector, a spherical tank filled with mineral ... |
1,108,101,566,480 | arxiv | \section{Introduction}
Cosmological perturbation theory plays a central role in confronting theories
of the early universe with observations. The increasing
accuracy of the observations, however,
has made it necessary to extend the theory from linear to
second order (\emph{i.e.\,}nonlinear)
perturbations, which presen... |
1,108,101,566,481 | arxiv | \section{Introduction}
\label{sec:intro}
The discovery of the relationship between the masses of nuclear
supermassive black holes (SMBH) and the luminosity, velocity
dispersion, or mass of their host galactic spheroids
\citep{dressler:89,kormendy_review:95,magorrian:98,ferrarese:00,gebhardt:00,marconi:03,haering:04}
i... |
1,108,101,566,482 | arxiv | \section{Introduction}
\setcounter{equation}{0}
In this paper, we study the dynamical behavior of the
non-autonomous Reaction-Diffusion equation defined on $I \kern -.3em R^n$:
\begin{equation}
\label{intr1}
\frac {\partial u}{\partial t}
- \Delta u + \lambda u = f(x, u) + g(x,t),
\end{equation}
where $... |
1,108,101,566,483 | arxiv | \section{Memo}
\section{Introduction}
\subsection{Background}
Let $G$ be a group and $N$ be a normal subgroup of $G$. An element of the form $[g,x] = gxg^{-1}x^{-1}$ with $g\in G$ and $x\in N$ is called a \emph{$(G,N)$-commutator} or a \emph{mixed commutator}; $[G,N]$ is the subgroup generated by mixed ... |
1,108,101,566,484 | arxiv | \section{Introduction}
\label{intro}
The low-lying structure of $^{12}$C is still one of the most fascinating open problems in nuclear physics. Alpha-clusterization and the nature of the so-called Hoyle state, which plays a crucial role in nucleosynthesis, have attracted special interest. Microscopic theories (e.g., \c... |
1,108,101,566,485 | arxiv | \section{Introduction}
Unstable $r$-modes \cite{A97,FM98} may limit the angular velocity of
old neutron stars spun up by accretion and may contribute to the spin-down of
nascent neutron stars (see \cite{Lindblom98b,fsbook,Bondarescu07,Bondarescu09}
for references and reviews). Spruit \cite{Spruit99} argued that ... |
1,108,101,566,486 | arxiv | \section{Introduction}
The past two years have seen several experimental observations of new
heavy and light quark states. Most of
those states contain a charm quark, so their observation rekindled
interest in heavy-flavor spectroscopy~\cite{Petrov:2003un}. The unusual
properties of those states invited some speculati... |
1,108,101,566,487 | arxiv | \section{Introduction}
Due to the importance of convexity and its generalisations in the study of optimality to resolve mathematical issues, researchers have concentrated a lot of their efforts on generalised convex functions for this purpose. As an illustration, Hudzik and Maligranda (1994) \cite{Hudzik}, investigat... |
1,108,101,566,488 | arxiv | \section{Introduction}
The steady state radio sky is considerably well studied and modeled (e.g. \citet{Be95, Co98}) but dynamic radio sky is not studied in detail due to one or more reasons including lack of telescopes with large field of view, observational
constraints, band width and poor time resolution etc. The... |
1,108,101,566,489 | arxiv | \section{Introduction}
The flexoelectric (FxE) effect, where polarization is induced by a
strain gradient, is universal in all insulators. As devices shrink to
the micro and nano scale, large strain gradients can occur, and
therefore the FxE effect can play a significant role in the properties
of such devices, influen... |
1,108,101,566,490 | arxiv | \section{Introduction}
\label{sec:intro}
In data centers, applictions are replicated on multiple instances running \textit{e.g.}, \ in containers or virtual machines (VMs) to provide scalable services~\cite{dragoni2017microservices}.
One of the main components in such data centers for optimal resource utilization is ... |
1,108,101,566,491 | arxiv | \section*{IEEE Copyright Notice}
© IEEE. Personal use of this material is permitted. However, permission to reprint/republish this material for advertising or promotional purposes or for creating new collective works for resale or redistribution to servers or lists, or to reuse any copyrighted component of this work in... |
1,108,101,566,492 | arxiv |
\section{Guiding principles}
\label{sec:principles}
This section elaborates on the main design goals, which are portability, versatility, safety and autonomy, and on the implications that they entail for a RPC-based detection setup. This section also summarizes the main technical choices of our current prototype; fo... |
1,108,101,566,493 | arxiv | \section{\label{sec:intro}Introduction}
Magnetic materials on lattices comprised of equilateral triangles continue to attract attention from both the experimental and theoretical viewpoint due to the richness of physical properties provided by geometric frustration~\cite{sadoc_mosseri_frustration_1999,diep_frustration... |
1,108,101,566,494 | arxiv |
\section
An atlas of the Richelot isogeny graph
\label{sec:atlas}
We are now ready to compute the neighbourhoods of each type of vertex
and edge in the Richelot isogeny graph.
We begin with general (\textsf{Type-A}\xspace) vertices,
before considering each type with an involution,
in order of increasing speciali... |
1,108,101,566,495 | arxiv | \section{Introduction}
The {\it IJCAI--23 Proceedings} will be printed from electronic
manuscripts submitted by the authors. These must be PDF ({\em Portable
Document Format}) files formatted for 8-1/2$''$ $\times$ 11$''$ paper.
\subsection{Length of Papers}
All paper {\em submissions} to the main track mus... |
1,108,101,566,496 | arxiv | \section{Introduction}
\label{sn:introduction}
In 1965 Intel's co-founder Gorden Moore presented the now famous \emph{Moore's
law} stating that: \emph{The number of transistors on a chip will roughly
double every 18 months}. Later in 2000 the 18 months were changed to two years
but the law is still followed by electri... |
1,108,101,566,497 | arxiv | \section{Introduction}
The dimensional reduction of ten-dimensional IIB supergravity on Calabi-Yau orientifolds yields four-dimensional $\mathcal{N}=1$ supergravity theories \cite{Grimm:2004uq}, which are of particular phenomenological interest. The resulting couplings are given by topological quantities of the int... |
1,108,101,566,498 | arxiv | \section{INTRODUCTION}
\noindent
Recent experimental discovery of the $\Theta (1540)$ as a narrow KN bound state in $\gamma$-nucleon and
$\gamma$-nucleus processes, $e^+e^-$ and hadronic machines \cite{NICOLAI}\footnote{However, this narrow state has
not been confirmed by several experiments with high statistics and v... |
1,108,101,566,499 | arxiv | \section{Introduction}
In the recent years, there has been an increasing interest on Deep Learning for supervised classification \citep{lecun}. It is very difficult to give an exact definition of what it is due to its wide applicability in different contexts and formulations, but it can be thought of as a set of algori... |
1,108,101,566,500 | arxiv | \section{Introduction and main result}
In this note we study the effective behavior at low energy of a non relativistic quantum particle in $\mathbb{R}^3$ interacting with a system of $N$ randomly distributed obstacles in the limit $N \rightarrow \infty$. In order to formulate such Lorentz gas model, we introduce the ... |
1,108,101,566,501 | arxiv | \section{Introduction}
The NA60 experiment was approved in the year 2000 to study a number of
physics topics accessible through the measurement of muon pairs. All
topics were studied by previous experiments, but were left with major
open questions: (i)~the excess emission of lepton pairs for masses
below the $\rho$-res... |
1,108,101,566,502 | arxiv | \section{Introduction}
Observations indicate that a significant fraction of spiral galaxies are barred (e.g. Cheung et al. 2013
and references therein). While precise measurements of the
bar fraction vary (between 20 and 70 percent, depending on the sample) there is no doubt that the phenomenon is a
rather common... |
1,108,101,566,503 | arxiv | \section{Introduction}
{Cyber-physical systems (CPSs) refer to a class of engineering systems that integrate the cyber aspects of computation and communication with physical entities \cite{c1}.} Integrating communication and computation with sensing and control elements has made CPSs a key enabler in designing emerging... |
1,108,101,566,504 | arxiv | \section{Introduction}
As overhead imagery captured via remote sensing becomes more abundant,
it is increasingly relied upon as an important source of information
for understanding locations and how they change over time. For
example, methods have been proposed for extracting
roads~\cite{batra2019improved}, detecting
... |
1,108,101,566,505 | arxiv | \section{Introduction}
Recent advances in the field of machine learning have provided many opportunities for researching applications in the sciences. Fundamentally, the machine learning approach is motivated by the use of pattern recognition and statistical inference in a manner capable of isolating statistically sig... |
1,108,101,566,506 | arxiv | \section*{Methods}
\textbf{NMR experiments} were performed using variable temperature $^4$He cryostats and superconducting magnets. At $T\geq 4$~K magnetic field and frequency were fixed according to the $^1$H resonance condition $\nu_0=^1\gamma B$, with $^1\gamma=42.5774$~MHz/T, as the proton NMR spectrum was resolve... |
1,108,101,566,507 | arxiv | \section{Introduction}
\IEEEPARstart{I}{nternet} of Things (IoT) is bound to explode with huge business requirements in the beyond fifth generation (B5G) era. With the increasing demand for wireless connection in IoT deployment, teraherhz (THz) is expected to become an attractive candidate spectrum for B5G networks du... |
1,108,101,566,508 | arxiv | \section{Introduction}
\label{sec:introduction}
In the global market capitalization, 5G technologies are projected to be worth over USD 12.3 trillion by 2035 \cite{kim2018network}, and network slicing is seen as the key enabling technology that can bring up to 150\% increased revenues for the operators, in comparison w... |
1,108,101,566,509 | arxiv | \section{Introduction \label{s-intro}}
Astronomical observations demonstrate the general trend, indicating that many objects in the universe were formed much
earlier than expected by theory and possibly so old objects are even not allowed by the standard theory.
Among them there are stars in the Milky Way, ol... |
1,108,101,566,510 | arxiv | \section{Introduction}
The DP control system can continuously activate the vessel’s propellers to balance the external disturbances (wind, waves and currents, etc.), and automatically control the position/heading of vessel in horizontal plane. Recently, with the deepening of marine development, the development of marin... |
1,108,101,566,511 | arxiv | \section{Introduction}
The main goal of this monograph is to further the point of view that many
beautiful geometrical and analytical results valid on differentiable manifolds
hold on general metric spaces. Besides the wider relevance gained by
generalization, the foundations of the subject are clarified when the limi... |
1,108,101,566,512 | arxiv | \section{Introduction}
From contact tracing devices preventing the epidemic spread to vehicular networks and smart cities, \emph{cyber-physical systems} (CPS) are pervasive information and communication technologies augmenting the human perception and control over the physical world. CPS consist of engineering, phys... |
1,108,101,566,513 | arxiv | \section{Introduction}
\noindent
In this work we consider the problem of the existence of commutative $C^*$-algebras that are generated by families of Toeplitz operators on weighted Bergman spaces over irreducible bounded symmetric domains. More precisely, we are interested in the case where the Toeplitz operators are ... |
1,108,101,566,514 | arxiv | \section{Introduction}
\label{sec:intro}
The four 8.2m telescopes of the Very Large Telescope (VLT) at the European Southern Observatory (ESO)
form the world’s most scientifically productive ground-based observatory in the visible and infrared. However, looking at the future of the VLT, there is a long-standing need ... |
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