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3,212,635,537,806 | arxiv | \section{Introduction}
Massive multiple-input multiple-output (MIMO) has been regarded as one
of the enabling technologies in next generation wireless
communications\cite{marzetta10twc, resek13spmag,larsson14commag,lu14jstsp}. Considering the large
number of antennas at the base station (BS), it becomes almost im... |
3,212,635,537,807 | arxiv | |
3,212,635,537,808 | arxiv | \section{Introduction}
The interplay of strong correlation physics and magnetic behavior in itinerant
electronic systems has been a fascinating subject for many years. At low
temperature it is often possible to describe the response of such systems in
terms of the low energy
excitations and quasiparticle properties su... |
3,212,635,537,809 | arxiv | \section{Introduction}
\label{sec:introduction}
Many well-studied problems in combinatorics concern characterising discrete structures that~satisfy certain `local' constraints. For example, the~celebrated theorem of~Szemer\'edi~\cite{Sz75} gives an~upper bound on the~maximum size of~a~subset of~the~first $n$ integers ... |
3,212,635,537,810 | arxiv | \section{Boundary entropy of topological loop-gasses}\label{sec:boundaryentropy}
We now turn to the computation of the boundary diagnostics from \cref{sec:entropydiagnostics}. As before, we begin with Levin-Wen models.
\subsection{Levin-Wen models}
\begin{thm}[Topological entropy of (2+1)D Levin-Wen models at a boun... |
3,212,635,537,811 | arxiv | \section{Introduction}\label{intro}
This article presents an experimental study of HD$^+$ in the vicinity of the H$^+$ + D(1s) and H(1s) + D$^+$ dissociation thresholds by pulsed-field-ionisation zero-kinetic-energy (PFI-ZEKE) photoelectron spectroscopy. We used a resonant multiphoton excitation sequence via the $v=1... |
3,212,635,537,812 | arxiv | \section{Introduction}
The FCC-hh project, defined by the target of 100 TeV proton-proton collisions with a total integrated luminosity of 30 ab$^{-1}$,
will allow to extend the searches for flavour-changing neutral currents (FCNC, figure \ref{fcnc_decays})
forbidden in Standard Model (SM) at tree level and are strongl... |
3,212,635,537,813 | arxiv | \section{Introduction}
\begin{figure*}
\includegraphics[width=0.49\textwidth]{LC_Ground_SM.png}
\hfill
\includegraphics[width=0.49\textwidth]{LC_Space.png}
\caption{Photometric observations of ASASSN-18tb. Ground-based $BVgri$ photometry obtained with LCOGT, ASAS-SN, and SMARTS is shown on the left, and space-based \... |
3,212,635,537,814 | arxiv | \section{Abstract}
An extensive program for the calculation of galactic cosmic-ray
propagation has been developed. Primary and secondary nucleons,
primary and secondary electrons, secondary positrons and antiprotons
are included. Fragmentation and energy losses are computed using
realistic distributions for the inter... |
3,212,635,537,815 | arxiv | \section{Introduction}
The search for the QCD critical point has attracted considerable
theoretical and experimental attention recently. The existence of such a
point -- an ending point of the first order chiral transition in QCD --
was suggested a long time ago \cite{Asakawa,Barducci},
and the properties were studied... |
3,212,635,537,816 | arxiv | \section{Introduction}
For its own sake, it is interesting to understand how the so far most fundamental theory of quantum fields is related to kinetic theory - a description of physics in terms of momentum distributions that is closer to the physics of classical particles. The relation of quantum field theory and kine... |
3,212,635,537,817 | arxiv | \section{\@startsection {section}{1}{\zeta@}%
{-3.5ex \@plus -1ex \@minus -.2ex}%
{2.3ex \@plus.2ex}%
{\normalfont\large\bfseries}}
\renewcommand\subsection{\@startsection{subsection}{2}{\zeta@}%
... |
3,212,635,537,818 | arxiv | \section{Introduction}
Fix positive integers $m$ and $n$.
In \cite{KT21,KST21}, the first and third author introduced a family of $S_{mn}$ modules of cardinality $n^{mn-2}$ with the property that in the case $m=1$, the resulting representation restricted to $S_{n-1}$ is Haiman's well-known parking function representat... |
3,212,635,537,819 | arxiv | \section{Introduction
\label{sec:Intr}
Gravitating matter tends to clusterise and form objects on different scales. It is suspected that, similar to stars, star clusters may form groups \citep{1996ApJ...466..802E, 1997AJ....113..249F, 2010MNRAS.403..996B, 2013MNRAS.434..313G} and physical pairs. The fraction of these... |
3,212,635,537,820 | arxiv | \section{Introduction}
The covariant open superstring description of D-branes
\cite{Lambert:1999id,Bain:2002tq} has been a useful way
in classifying supersymmetric D-branes, especially 1/2-BPS D-branes,
in a given supersymmetric background.
It has been successfully applied to some important backgrounds
in superstring ... |
3,212,635,537,821 | arxiv | \section{Introduction}
\label{sec:intro}
Voice-only, spoken conversational systems such as Google Home, Amazon Echo, or Apple Homepod, are becoming widely used. These systems can answer factoid questions. However, they are yet not able to engage in complex information seeking tasks where multiple turns are needed to ex... |
3,212,635,537,822 | arxiv |
\section{Introduction}\label{sec:introduction}
One of the challenging aspects in the design of autonomous vehicles is their communication with other, non-autonomous
participants in traffic. Specifically the interaction with pedestrians requires clear communication of intent to allow
for safe interactions \citep{rasou... |
3,212,635,537,823 | arxiv | \section{Introduction}
The Boltzmann equation describes the underlying microscopic dynamics of
dilute classical gases \cite{cercignanibook}. It is widely employed to model
a variety of nonequilibrium phenomena in several areas of physics such as
the dynamics of the hot hadronic matter produced in the late stages of
ul... |
3,212,635,537,824 | arxiv | \section{Introduction}
The tunneling phenomenon is a salient feature of quantum physics that even physicists sometimes find peculiar. One such example of it is resonant tunneling. The tunneling effect is usually characterized by an exponential suppression by a potential barrier; however, if a pair of potential barriers... |
3,212,635,537,825 | arxiv | \section{Introduction}
This document is a model and instructions for \LaTeX.
Please observe the conference page limits.
\section{Ease of Use}
\subsection{Maintaining the Integrity of the Specifications}
The IEEEtran class file is used to format your paper and style the text. All margins,
column widths, line spaces... |
3,212,635,537,826 | arxiv |
\section*{Bigger Picture}
The genome contains instructions for building the function and structure, and guiding the evolution of molecules and organisms. Recent high-throughput techniques allow the generation of a vast amount of genomics data. However, the path of transforming genomics data into tangible therapeutics... |
3,212,635,537,827 | arxiv | \section{Introduction}
The Hardy inequality, introduced in \cite{Hardy20}, is one of the well known mathematical manifestations of the Uncertainty Principle in Quantum Mechanics. It affirms that
\begin{equation}\label{eq:Hardy-classical}
\int_{\mathbb{R}^d} |\nabla\psi(x)|^2\,dx
\geq \frac{(d-2)^2}{4}
\int_{\mathbb{R}... |
3,212,635,537,828 | arxiv | \section{Introduction}\label{Sec:Intro}
For an affine real smooth algebraic hypersurface $X \subset {\mathbb C}^{n+1}$ with real part ${\mathbb R} X \subset {\mathbb R}^{n+1}$ there is an universal inequality between the total curvatures of the real part ${\mathbb R} X$ and the one of ${\mathbb C} X$ (\cite{Ris03}), s... |
3,212,635,537,829 | arxiv | \section{Introduction}
Transition metals with nearly half-filled bands, such as
Cr,~\cite{Faw88} Mn,~\cite{Yam70,Yam71,Men57} $\gamma$-Fe,~\cite{Tsu89,Qia01} and
their alloys,~\cite{Bac57,Huc70,End71,Yam00,Akb98,Fis99} show
complex magnetic structures due to competing magnetic interactions.
The determination of their ... |
3,212,635,537,830 | arxiv | \section{Introduction}
Recently,
organic semiconductors have been attracting considerable attention for their use in
electronic devices like organic light-emitting diodes and organic solar cells. \cite{Brutting}
Carrier transport in molecular solids can be described by hopping transitions between neighboring molecul... |
3,212,635,537,831 | arxiv | \section{Introduction}
\label{sec:introduction}
In this paper an extensive treatment of type-2 fuzzy sets and membership functions is presented
that is more general than the ones that can be found in literature.
Moreover, the potentials of fuzzy logic and probability theory are discussed,
as well as how real-li... |
3,212,635,537,832 | arxiv | \section{Introduction}
\begin{figure*}[!ht]
\centering
\includegraphics[width=0.99\linewidth]{images/Novel_views.pdf}
\caption{Visualization of novel view rendering in the proposed method on two samples of Structured3D and Replica360.
A plausible viewpoint image with 3D consistency is synthesized at position... |
3,212,635,537,833 | arxiv | \section{Introduction}
\label{sec:introduction}
Neural word embeddings \cite{bengio2006,collobert2008,mikolov2013efficient} have
received much attention in the distributional semantics community, and have
shown state-of-the-art performance in many natural language processing
tasks. While they have been compared with c... |
3,212,635,537,834 | arxiv | \section{Introduction and Summary}
\label{s1}
In this volume there is an introduction to cosmology and CMB physics by Sourdeep, and on the inflationary paradigm by Wands. They summarize the synergy between theory and observations that has produced spectacular advances in our understanding of the universe in the last d... |
3,212,635,537,835 | arxiv | \section{Introduction}
Bagger, Lambert \cite{Bagger:2006sk,Bagger:2007jr,Bagger:2007vi}
and Gustavsson \cite{Gustavsson:2007vu,Gustavsson:2008dy}
discovered an interesting model
for multiple M2-branes
(which we will call BLG model in the following)
based on an algebraic structure
called Lie 3-algebra.
Since membran... |
3,212,635,537,836 | arxiv | \section{Introduction}
Explaining the
fermion mass hierarchy and mixing pattern is an outstanding
challenge of particle physics \cite{Froggatt:1978nt}\cite{attempts}\cite{Nandi:2008zw}.
The fermion masses are parameterized by the Standard Model
Yukawa interactions of chiral fermions with a single Higgs doublet.
It is ... |
3,212,635,537,837 | arxiv | \section{Introduction}
The compact (scale sizes of $\sim 0.1-1$ pc) and ultracompact (UC;
scale sizes $\;\lower4pt\hbox{${\buildrel\displaystyle <\over\sim}$}\; 0.15$ pc) H \Rmnum{2} regions are associated with
massive OB stars \citep[e.g.,][]{Habing}.
The UC H \Rmnum{2} region stage ($\;\lower4pt\hbox{${\buildrel\di... |
3,212,635,537,838 | arxiv |
\subsubsection*{Achievability} \label{achievability}
We now propose an online scheduling policy $\pi^{\textsf{MMW}}$ which approximately minimizes the average AoI \eqref{objective} for mobile UEs (the abbreviation \textsf{MMW} stands for ``Multi-cell Max-Weight"). Our policy is a multi-cell generalization of the $4$-a... |
3,212,635,537,839 | arxiv | \section{Introduction} \label{Sec_1}
Let us consider the one-dimensional stochastic differential equation (SDE)
\begin{align}\label{SDE_1}
X_t=
x_0
+\int_0^t b(X_s)ds
+\int_0^t \sigma(X_s)dW_s,
~x_0 \in \mathbb{R},
~t \in [0,T],
\end{align}
where $W:=(W_t)_{0\leq t \leq T}$ is a standard Brownian motion defined on a p... |
3,212,635,537,840 | arxiv |
\section{Conclusion} \label{sec:Conclusion}
In this paper, we proposed a novel machine learning-based self-compensating approximate accelerators for enhancing the efficiency of approximate computing applications. In contrast to the state-of-the-art error reduction methodologies, the proposed generic self-compensatin... |
3,212,635,537,841 | arxiv | \section{Introduction}
\setcounter{equation}{0}\hspace{0.25in}In an instrumental variable (IV)
model, researchers often rely on asymptotic approximations when making
inference on the structural coefficients. These approximations, however, can
be poor when instruments are weakly correlated with the endogenous
regressor... |
3,212,635,537,842 | arxiv | \section{Introduction}
Phase-field approximations provide a convenient way of treating curvature energies numerically. Typically, the phase-field problem is more stable numerically than the potentially highly non-linear original problem. A classical example of a curvature energy is the Willmore functional
\[
{\mathca... |
3,212,635,537,843 | arxiv | \section{Introduction.}
A recent account of the baryon distribution in the local Universe
concluded that about half the baryons synthesized in the Big-Bang
have yet to be identified (Shull, Smith \& Danforth 2012)
confirming an earlier deficit of baryons found by
Fukugita, Hogan \& Peebles (1998).
Numerical simulatio... |
3,212,635,537,844 | arxiv | \section{Introduction}
\label{s:intro}
This paper has to do with determining information about the internal structure of a finite group $\Gamma$ from the knowledge of the universal deformation rings $R(\Gamma,V)$ associated to absolutely irreducible $\mathbb{F}_p\Gamma$-modules $V$. The kind of internal structure we ... |
3,212,635,537,845 | arxiv | \section{Introduction}
Symmetry considerations make it seem obvious that an ideal cubical die lands on all six faces with an identical probability of $\frac{1}{6}$. However, what happens when non-fair
dice are tossed? In particular, what are the face-probabilities of a homogeneous \emph{cuboid}, i.e.\ a six-sided polyh... |
3,212,635,537,846 | arxiv | \section{Introduction}
Light transport simulation can be notoriously hard. The main problem is that forming an image requires evaluating millions of infinite dimensional integrals, whose integrands, while correlated, may contain an infinity of singularities and different modes at disparate frequencies.
Many approaches... |
3,212,635,537,847 | arxiv | \section{INTRODUCTION}
Extremely low-mass ($\la 0.3$ M$_\odot$) white dwarfs (ELM WDs) are the remnants of stars that cannot burn helium (He) in
their cores. Because the Universe does not have enough time to produce them by single-star evolution, the He-core ELM WDs
are thought to be formed by considerable mass ... |
3,212,635,537,848 | arxiv | \section{Introduction}
\label{sec:intro}
The development of reinforcement learning (RL) methods has achieved much success over the last decade, since together with advances in computer vision \citep{krizhevsky2012imagenet,he2016deep}, it became possible to teach agents to solve various tasks, play computer games \cit... |
3,212,635,537,849 | arxiv | \subsection{
\refstepcounter{equation}
\noindent {\bf \arabic{section}.\arabic{equation}.}
}
\newcommand{\mathbb{Z}}{\mathbb{Z}}
\newcommand{\mathbb{C}}{\mathbb{C}}
\newcommand{\mathbb{A}}{\mathbb{A}}
\newcommand{\mathbb{Q}}{\mathbb{Q}}
\newcommand{\mathbb{R}}{\mathbb{R}}
\renewcommand{\P}{\mathbb{P}}
\newcommand{{\... |
3,212,635,537,850 | arxiv | \section{Introduction}
Compact objects, such as black holes, neutron stars, etc. are identified by electromagnetic radiations
emitted from the accreting matter. Understanding the spectral and timing properties of this radiation is
essential for model builders and theorists alike. In a binary system, matter from ... |
3,212,635,537,851 | arxiv | \section{LIST OF SYMBOLS}
\begin{abstract}
Sleep staging is of great importance in the diagnosis and treatment of sleep disorders. Recently, numerous data driven deep learning models have been proposed for automatic sleep staging. They mainly rely on the assumption that training and testing data are drawn from the sa... |
3,212,635,537,852 | arxiv | \section{Introduction}
In 1924 T. Rad\'o proved the following remarkable theorem \cite{Ra}:
\begin{theorem}
Let $\Omega\subseteq \mathbb{C}$, be an open set and $f$ be a continuous function in $\Omega$ which is holomorphic on $\Omega\setminus\lbrace f^{-1}(0)\rbrace$. Then $f$ is holomorphic in $\Omega$.
\end{theorem... |
3,212,635,537,853 | arxiv | \section{Jet vetoing: gaps between jets}
We consider dijet production with transverse momentum $Q$ and a veto on the emission of additional radiation in the inter-jet rapidity region, $Y$, harder than $Q_0$.
We shall refer generically to the ``gaps between jets'' process, although the veto scale is chosen to be large,... |
3,212,635,537,854 | arxiv | \section{Introduction}
\label{sec:intro}
Accurate high-resolution information of precipitation data is essential to effective prediction and management of water resources \citep{clark2015}. Dramatic improvements in modeling physical processes driving precipitation have resulted in more realistic simulations from globa... |
3,212,635,537,855 | arxiv | \section{Introduction}
The birth of massive stars is inextricably linked to that of cluster formation, as most massive stars form at the centre of dense molecular clouds. The structure of such regions is dense and filamentary, far removed from simple spherical models. In \citet{Smith12a}, hereafter Paper I, we investig... |
3,212,635,537,856 | arxiv | \section{\sf Introduction}
In this paper, a \emph{smooth} finite dimensional algebra over a field $k$ is a finite dimensional algebra of finite global dimension. The word "smooth" is originated in commutative algebra and is convenient for brevity. Observe that in \cite{CUNTZQUILLEN}, for finite dimensional algebras, ... |
3,212,635,537,857 | arxiv | \section{Introduction}
In the 1960s, Douglas Richard Hofstadter introduced the $Q$-sequence~\cite{18}, which is defined by the nested recurrence relation $Q\p{n}=Q\p{n-Q\p{n-1}}+Q\p{n-Q\p{n-2}}$ with initial conditions $Q\p{1}=Q\p{2}=1$. The resulting sequence appears to grow approximately like $\frac{n}{2}$, but with... |
3,212,635,537,858 | arxiv | \section{Continuous transition between doubled semion and toric code models}
\label{dstcSec}
Here we note that it is possible to understand a continuous transition between two kinds of
$SU(2)$ invariant $Z_2$ spin liquids, corresponding to the doubled semion and toric code models, respectively.
Specifically, the dou... |
3,212,635,537,859 | arxiv | \section{Acknowledgments}
The authors gratefully acknowledge stimulating discussions with Mario Italo Trioni.
This work was supported by the Deutsche Forschungsgemeinschaft within SPP 1666 (Grant No. BO1468/21-1).
K.A.K. and O.E.T. acknowledge the financial support by the RFBR (Grant nos. 13-02-92105 and 14-08-31110).... |
3,212,635,537,860 | arxiv | \section{\label{s1}Introduction}
Digital receivers are a class of electronic systems where operations like amplification, filtering, integration etc. are performed as a series of mathematical operation on embedded components like FPGAs, Microprocessors or GPUs. Compared to their analog counterparts, digital receivers ... |
3,212,635,537,861 | arxiv | \section{Introduction}
The Resonating Valence Bond (RVB) state, defined as an equal weight superposition of (non-orthogonal) nearest neighbor (NN) singlet (or dimer) coverings, was
first proposed by Anderson~\cite{Anderson1973} to describe a possible spin liquid ground
state (GS) of the $S=1/2$ antiferromagnetic Heise... |
3,212,635,537,862 | arxiv | \section{Introduction}
\label{sec:intro}
One of the mysteries of nature is the origin of mass scales.
At least in QCD, we have an answer: the hadronic mass scale can arise when
the gauge coupling evolves to large values such that the fundamental
constituents, the quarks, condense to bound states.
From dimensional t... |
3,212,635,537,863 | arxiv | \section{Introduction}
The non local character of Quantum Mechanics (\textit{QM}) has been
object of a great debate starting from the famous Einstein-Podolsky-Rosen
(\textit{EPR}) paper \cite{EPR}. Consider, for instance, a quantum
system made by two photons \emph{a} and \emph{b} that are in the polarization
entangled... |
3,212,635,537,864 | arxiv | \section{Introduction}
The $T\bar{T}$ deformation, introduced in \cite{Smirnov:2016lqw},\cite{Cavaglia:2016oda}, is a solvable irrelevant operator deformation of quantum field theories in two dimensions. The deforming operator is defined by the coincidence limit of the following bi-local operator formed from the energy... |
3,212,635,537,865 | arxiv | \section*{Abstract}
In the present paper, an asymptotic model is constructed for the short-time deformation of an articular cartilage layer modeled as transversely isotropic, transversely homogeneous (TITH) biphasic material. It is assumed that the layer thickness is relatively small compared with the characteristic s... |
3,212,635,537,866 | arxiv | \section{Introduction}
To understand the emergence of cooperative behavior among selfish
individuals, researchers have considered various mechanisms, such as
network reciprocity~\cite{1,2}, voluntary participation~\cite{3,4},
aspiration~\cite{5,6,7}, social diversity~\cite{9,10},
migration~\cite{11,12,13}, chaot... |
3,212,635,537,867 | arxiv | \section{Introduction}
\IEEEPARstart{L}{oad} forecasting plays a key role in the management and dispatching of power systems. Load forecasting involves forecasting the load demand of a future time span. Load forecasting within an interval of an hour to a week is often referred to as short-term load forecasting (STLF). ... |
3,212,635,537,868 | arxiv | \section{Introduction}
Cosmic strings are among the most important class of linear topological
defects with the conical geometry outside the core \cite{Vile94}. The
formation of these type of topologically stable structures during the
cosmological expansion is predicted in most interesting models of high
energy physics... |
3,212,635,537,869 | arxiv |
\section{Introduction} \label{sec:introduction}
Globally, nearly a third of women report experiencing violence perpetrated by an intimate partner \cite{devries_global_2013} with far-reaching consequences for their health, their families, their opportunities, and their livelihoods \cite{ellsberg_intimate_2008}. This h... |
3,212,635,537,870 | arxiv | \section{Introduction}\label{Introduction}
\subsection{Coboundaries} Let $T$ be a bounded linear operator acting on a complex Banach space $\mathcal X$. An element $x$ of $\mathcal X$ is called a \emph{coboundary for} $T$ if there is $y\in \mathcal X$ such that $x = y - Ty$. Coboundaries are related to the behavior of ... |
3,212,635,537,871 | arxiv |
\section*{Introduction} The aim of this paper is to prove several new results on elliptic curves with complex multiplication, most of which are generalisations of previous ones. Let $K$ be an imaginary quadratic field, $L$ an extension of $K$ and $E/L$ an elliptic curve with complex multiplication. In \S\S 1--2 we ana... |
3,212,635,537,872 | arxiv | \section{Introduction}
The Garden of Eden theorem,
originally established by Moore~\cite{moore} and Myhill~\cite{myhill} in the early 1960s, is an important result in symbolic dynamics and coding theory.
It provides a necessary and sufficient condition for a cellular automaton to be surjective.
More specifica... |
3,212,635,537,873 | arxiv | \section{Introduction}
Semantic representation is an essential part of NLP. For this reason, several semantic representation paradigms have been proposed. Among them we find PropBank \cite{palmer2005proposition} and FrameNet Semantics \cite{baker1998berkeley}, Abstract Meaning Representation (AMR) \cite{banarescu2013a... |
3,212,635,537,874 | arxiv |
\section{Introduction} \label{sec:intro}
In the last twenty years large and systematic digital imaging surveys of the sky have revolutionized astronomical exploration. Beginning with the Sloan Digital Sky Survey \citep[SDSS;][]{York2000}, ground-based surveys like the PS1 \citep[Pan-STARRS1][]{Chambers2016}, Dark En... |
3,212,635,537,875 | arxiv | \section{Introduction}
Social behaviors often provide useful insights in determining the way problems are solved in computer science. For instance, matters of security in decision making or in collaborative content filtering/production are enforced by implementing reputation and trust strategies \cite{JosangQ09,schill... |
3,212,635,537,876 | arxiv | \section{Introduction\label{ss:theory_r}}
The two predominant astrophysical mechanisms for production of heavy elements in the universe are the slow neutron-capture process (s-process) and the rapid neutron-capture process (r-process) \cite{RevModPhys.29.547}. The r-process occurs in high neutron-density areas in the ... |
3,212,635,537,877 | arxiv | \section{Introduction}
\setcounter{equation}{0}
Consider the classical Lane-Emden system
\begin{align}\label{1.1}
-\Delta u = v^p, \quad-\Delta v= u^\theta,\quad u,v>0\quad\mbox{in }\; \mathbb{R}^N, \quad\mbox{where }\; p,\theta >0.
\end{align}
There is a famous conjecture who states that: {\sl Let $p, \theta > 0$. If... |
3,212,635,537,878 | arxiv | \section{INTRODUCTION}
Under the influence of the high pressure, the elemental calcium undergoes a series of structural phase transitions. In particular, one can distinguish seven phases in the range of pressure ($p$) from $0$ to $241$ GPa \cite{Olijnyk}, \cite{Yabuuchi}, \cite{Sakata} (please see Figure \fig{fig1} (A... |
3,212,635,537,879 | arxiv | \section{Introduction}
Since the earliest “artificial neuron” model proposed based on studies of the human brain and nervous system, neural networks have achieved a series of developments and even notable successes in some commercially essential areas, such as image captioning, machine translation and video games. How... |
3,212,635,537,880 | arxiv | \section{Introduction}
Massive multiple input multiple output (MIMO) is a key component of 5G since this technology can improve ergodic spectral efficiency (SE) with the orders of magnitude compared to single-antenna systems. It is achieved by equipping each base station (BS) with a large number of antennas such that... |
3,212,635,537,881 | arxiv | \section{Introduction\label{sec:1}}
Vortical structures are ubiquitously observed in hydrodynamic and
magnetohydrodynamic phenomena. The genesis of cyclones (typhoon,
hurricane, tornado, etc.) is one of the open problems in
atmospheric science. Small-scale vortical structures in turbulence are
considered to be the caus... |
3,212,635,537,882 | arxiv | \section{Introduction}
Neutron stars (NS) are gravitationally bound, therefore the precise measurement of mass and radius
of a NS should provide a very fine probe for the equation of state (EOS) of dense matter.
The first reasonable ideas about the composition of compact stars argued that matter are under extreme
den... |
3,212,635,537,883 | arxiv | \section{Introduction}
Despite the tremendous progress made in communication, we are still in its infancy. As first envisioned in Claude E. Shannon's seminal work \cite{Shannon1948}, the current goal of communication is about how to accurately transfer and reconstruct information bits, while ignoring the \emph{meaning ... |
3,212,635,537,884 | arxiv | \section{Acoustic Levitation}\label{sec:acoustic-levitation}
\begin{figure}[b]
\centering
\includegraphics[width=1\textwidth]{figures/Acoustic_Levitation.png}
\caption{(A) A user performing a pointing task on the real prototype (left), and in the \textit{Levitation Simulator}~\cite{Paneva20} (middle, right... |
3,212,635,537,885 | arxiv | \section{Introduction}\label{sec:intro}
The discovery of the SM-like Higgs boson and nothing else presents a serious challenge to particle phenomenology. On one hand, the SM is incomplete, as it fails to explain properties such as the hierarchy problem, neutrino masses, cosmological inflation and dark matter. On the ot... |
3,212,635,537,886 | arxiv | \section{Introduction}\label{c:sec1}
In a recent work we parameterized the fully unintegrated, off-diagonal quark-quark
correlator for a spin-0 hadron in terms of so-called generalized parton
correlation functions (GPCFs)~\cite{Meissner:2008ay}.
The GPCFs depend on the full 4-momentum of the quark and, in addition, o... |
3,212,635,537,887 | arxiv | \section{Introduction}\label{sect:introduction}
In this paper we consider the nonlinear scalar field equation with an $L^2$ constraint:
\begin{linenomath*}
\begin{equation*}\tag{$P_m$}\label{problem}
\left\{
\begin{aligned}
-\Delta u&=f(u)-\mu u\quad\text{in}~\mathbb{R}^N,\... |
3,212,635,537,888 | arxiv | \section{Introduction}
It has long been known that particles with non-zero spin can have
``toroidal'' electromagnetic form factors that are odd under charge
conjugation $C$, which implies that they violate either parity ($P$)
or time reversal ($T$), but not both symmetries simultaneously~\cite{Khr97}.
The toroidal dip... |
3,212,635,537,889 | arxiv |
\section{Sequential Fully Dynamic Triangle Counting of~\cite{KNNOZ19}}\label{app:triangle}
Here, we present the sequential fully dynamic triangle counting
algorithm of Kara et al.~\cite{KNNOZ19} that operates in $O(m)$ space,
$O(\sqrt{m})$ amortized work per edge update, and $O(m^{3/2})$ work
for preprocessing. This ... |
3,212,635,537,890 | arxiv | \section{Introduction}
Flux distributions in type-II superconductors are commonly inferred from
magnetization and critical current measurements\cite{reviews}
and interpreted in the context of the Bean model\cite{bean} or its variations.
The Bean model, which has been widely used for over three decades,
{\it postulates... |
3,212,635,537,891 | arxiv | \section*{Introduction}\label{introduction}
Groups in which all elements belong to the conjugacy class of their inverses are called {\it real groups}.
It is well known that all entries in the character tables of finite real groups are real \cite{SerreRepnBook}.
However real groups may admit complex representations whic... |
3,212,635,537,892 | arxiv | \section{Introduction}
Complex systems are ubiquitous phenomenon in natural and scientific disciplines, and how relationships between parts give rise to global behaviours of a system is a central theme in many areas of study such as system biology \cite{biology}, neural science \cite{brain}, and drug and mat... |
3,212,635,537,893 | arxiv | \section{Introduction}
\IEEEPARstart{W}{ith} the rapid development of the Internet of Things (IoT), more and more IoT devices access wireless networks to support diverse applications, e.g., smart city, intelligent transportation, smart industry and healthcare (eHealth) [1], [2]. It can be predicted that the number of ... |
3,212,635,537,894 | arxiv | \section{Introduction}
\label{section:intro}
In a planetary system, the stellar obliquity is defined as the angle between the stellar spin axis and the net orbital angular momentum vector of the system. While the true stellar obliquity is not currently possible to pinpoint in most exoplanet systems due to incomplete... |
3,212,635,537,895 | arxiv | \section{Introduction}
The issue of a possible loss of quantum coherence in processes in which a black hole is produced and then evaporates has been the subject of much debate since Hawking's claim \cite{Haw} that black holes should emit an exactly thermal spectrum of light quanta (see e.g. \cite{Mathur} for a recen... |
3,212,635,537,896 | arxiv | \section{Introduction}
The realization of new coherent radiation sources in the THz frequencies boosts dramatically the development of innovative spectroscopic techniques~\cite{Lee_09}. These spectroscopies are non-invasive methods that provide complementary information to traditional analytical tools. THz radiation i... |
3,212,635,537,897 | arxiv | \section{introduction}
In a recent paper\cite{wulee12}, we presented predictions of
photo-production of bound states $[^3He]_{J/\Psi}$ on $^4He$ target and
$[q^6]_{J/\Psi}$ on $^3He$ target. In this work we apply the
same approach to
predict the production cross sections for these bound states with pion beams.
Our pr... |
3,212,635,537,898 | arxiv |
\section{Introduction}
In computer vision and robotics, \acf{hoi}~\cite{liao2020ppdm,liao2022gen,zhang2021mining,yuan2022detecting} is the crux of modern fine-grained human activity understanding. In this work, we tackle a challenging problem of \acf{fahoi}, which requires (i) building on kinematic-agnostic object re... |
3,212,635,537,899 | arxiv | \section{Introduction}
Ikeda--Mihalcea--Naruse \cite{IkedaMihalceaNaruse} introduced the {\it double Schubert polynomials} of type $C$ (also $B$ and $D$) by extending Billey--Haiman \cite{BilleyHaiman}'s construction for the single case. These polynomials represent the equivariant cohomology classes of Schubert variet... |
3,212,635,537,900 | arxiv | \section{Conclusion}
\label{sec:conclusion}
We developed a dynamic mapping algorithm based on Bayesian kernel inference that models the motion of dynamic objects with scene flow. Our map may be built from any 3D sensor and uses deep neural networks to obtain semantic labels and scene flow from raw point cloud data. We ... |
3,212,635,537,901 | arxiv | \section{Introduction} \label{sec:intro}
Whether thermalization occurs in isolated quantum many-body systems has attracted much attention since the birth of quantum mechanics~\cite{Neumann_29}. A recent impetus for exploring this question comes from experimental advances in ultracold quantum gases, in which nearly iso... |
3,212,635,537,902 | arxiv | \section{Introduction}\label{sec:intro}
Chemical vapour deposition (CVD) has become one of the most popular methods for epitaxial growth of single crystal diamond (SCD) and polycrystalline diamond (PCD) for a wide variety of applications. The basis of this technique requires dissociation of a gaseous hydrocarbon pre-c... |
3,212,635,537,903 | arxiv | \section{Introduction}
The continuous miniaturization of the field-effect transistor (FET) has enabled the fabrication of increasingly powerful circuits on a single microchip. The performance of traditional planar FETs drops significantly as the source-drain separation is pushed below 50~nm due to short channel effect... |
3,212,635,537,904 | arxiv | \section{Introduction}
In this paper we consider optimization problems where the objective is a sum of
two terms: The first term is separable in the variable blocks, and the second
term is separable in the difference between consecutive variable blocks. One
example is the Fused Lasso method in statistical learning,
\... |
3,212,635,537,905 | arxiv | \section{Introduction}
Increase in fault currents in power grids is due to the ongoing expansion in energy generation and demand, as well as the trend to parallelize the network sections. As a result, there is a global effort underway to find solutions to the fault currents problem in order to prevent having to replace... |
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