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2,869,038,156,928 | arxiv | \section{Introduction}
Considerable progress has been recently achieved in the spectroscopy of hydrogen molecular ions. Several rovibrational transitions in HD$^+$ have been measured with relative uncertainties in the 10$^{-11}$--10$^{-12}$ range through Doppler-free spectroscopy of ultracold trapped ions in the Lam... |
2,869,038,156,929 | arxiv | \section{INTRODUCTION}
Recently the field of autonomous driving has witnessed rapid development. A number of novel behavior planning algorithms have been proposed, many of which are awesome achievements. However, it is almost impossible for a single behavior planner to drive through so many different real and complex s... |
2,869,038,156,930 | arxiv | \section{\label{sec:intro}Introduction}
Numerous geophysical and astrophysical flows present a two-layer configuration, with a turbulent convective layer standing above or below a stably stratified one. Examples include planetary atmospheres, stars interiors, and possibly the outermost layer of the Earth liquid core \c... |
2,869,038,156,931 | arxiv | \section*{ Introduction}
The classical Myers's theorem (\cite{M}) and Cheng's maximum diam theorem (\cite{Ch}) in Riemannian geometry are well known.
As for their generalizations, we can refer to \cite{BL}, \cite{Q} and \cite{R}.
In Finsler geometry, the Myers type theorem (\cite{Sh1}) states that if $(M,F,d\mu)... |
2,869,038,156,932 | arxiv | \section*{Acknowledgments}\end{small}}
\newcommand\altaffilmark[1]{$^{#1}$}
\newcommand\altaffiltext[1]{$^{#1}$}
\voffset=-0.6in
\title[The Acoustic RDI]{The Resonant Drag Instability (RDI): Acoustic Modes
\vspace{-0.5cm}}
\vspace{-0.2cm}
\author[Hopkins \&\ Squire]{
\parbox[t]{\textwidth}{
Philip F.~Hopkins\altaffi... |
2,869,038,156,933 | arxiv | \section{Introduction}
In this paper, we assume that $\Omega$ is a simply connected bounded domain in $\RR^3$ with smooth boundary and investigate the following system in $\Omega$,
\begin{equation}\label{equation1.1}
\begin{cases}
\rho_t+\dive (\rho u)=0,\,\,\rho\geq 0,\\
(\rho u)_t+\dive(\rho u\otimes u)-\dive[2\... |
2,869,038,156,934 | arxiv | \section{Introduction}
\label{intro}
We assume throughout that $\Omega $ is a bounded domain in ${\mathbb{C}}^n$. Let ${\mathbb{D}}$ stand for the unit disk in
${\mathbb{C}}$.
The classical Lempert function with pole at $a \in \Omega $
\cite{Lempert} is defined by
$$
\ell_a (z):=\inf \big\{ \log|\zeta|:\exists \varphi... |
2,869,038,156,935 | arxiv |
\section{Introduction}
Many machine learning models can be formulated as the following empirical risk minimization problem:
\begin{align}\label{equation:object}
\min_{{\bf w}\in {\mathbb R}^d} F({\bf w}) := \frac{1}{n}\sum_{i=1}^n f({\bf w};\xi_i),
\end{align}
where ${\bf w}$ denotes the model parameter, $\xi_i$ deno... |
2,869,038,156,936 | arxiv | \section{Introduction}
Video Object Segmentation (VOS) is a fundamental task in computer vision with many potential applications, including augmented reality~\cite{ngan2011video} and self-driving cars~\cite{zhang2016instance}. In this paper, we focus on semi-supervised VOS, which targets on segmenting a particular obj... |
2,869,038,156,937 | arxiv | \section{Introduction}
Low-dimensional systems have been very popular among theorists for a number of decades now \cite{Mattis,Cazalilla}, not without a reason. On one hand, many of these allow for an exact treatment. The Bethe {\it ansatz} solves a number of one-dimensional problems exactly, such as the Lieb-Liniger ... |
2,869,038,156,938 | arxiv | \section{Introduction and main results}
Cluster algebras were introduced by Fomin and Zelevinsky~\cite{FZ} in an effort to describe dual canonical bases in the universal enveloping algebras of Borel subalgebras of simple complex Lie algebras. {A cluster algebra possesses the distinguished set of generators, \emph{clus... |
2,869,038,156,939 | arxiv | \section{Introduction}
\label{sec:intro}
Cataclysmic Variables (CVs) are a class of close binary system, with a
typical orbital period of a few hours, where a
white dwarf primary accretes material from its companion via Roche lobe
overflow.
The secondary is normally a late-type main sequence star although examples
... |
2,869,038,156,940 | arxiv | \section*{Introdução}
Sabemos que quando as dimensões de uma fonte luminosa são pequenas quando comparadas à distância entre essa fonte e um receptor dessa luz, podemos considerar que a fonte luminosa em questão é pontual. Uma maneira de confirmar os limites de validade dessa aproximação é medindo a queda da intensida... |
2,869,038,156,941 | arxiv | \section{Introduction}
\label{sec:introduction}
Large optical surveys demonstrated that galaxies evolve through mergers from star-forming spirals, through a transition region, to massive elliptical galaxies \citep[e.g.][]{bell04,faber07,schawinski14}. Outflows and the energetic feedback from active galactic nuclei (AGN... |
2,869,038,156,942 | arxiv | \section*{Highlights}
\begin{itemize}
\item Complexity characteristics of the scientific collaboration networks of several world renown scholars are studied.
\item Scientific collaboration community of H. Eugene Stanley self-organizes into a scale-free hierarchy but this is seen exclusively in the weighted network r... |
2,869,038,156,943 | arxiv | \section*{Architecture}
Figure \ref{architecture} shows how this PIC architecture allows us to realize a fully integrated coherent optical neural network (FICONN) through the following stages: (i) the \textit{transmitter} (TX) maps input vectors $\mathbf{x}_{(j)}$ to an optical field vector $\mathbf{a}_{(j)}^{(1)}$ b... |
2,869,038,156,944 | arxiv | \section{Introduction}\label{sec1
Throughout this paper, by $\rho(M)$ we mean the usual spectral radius of a real square matrix $M\in\mathbb{R}^{d\times d}$, where $2\le d<+\infty$. For an arbitrary finite family of real matrices
\bean
\bA=\{A_1,\dotsc,A_K\}\subset\mathbb{R}^{d\times d},
\eean
its \textit{general... |
2,869,038,156,945 | arxiv | \section{}
\robbert{no shadowing}\\
We want a UE to be served by approximately $L_{u}$ O-RUs. Thus we need to
define a circle around the UE which contains the $L_{u}$ closest O-RUs.
The O-RUs are distributed as a poisson point process. For this, we can
use Campbell's theorem. If we define the Borel set $\mathcal{B}$... |
2,869,038,156,946 | arxiv | \section{Introduction}
This paper studies finite difference schemes for nonlinear fractional order Klein-Gordon type equations.
Fractional differential equations have applications in physics, biology and petroleum industry.
Interested reader can refer to \cite{Kilbas2006,EBarkai_Phy,Meerschaert2001_Phy,Meerschaert2... |
2,869,038,156,947 | arxiv | \section{\label{Sec.intro}Introduction}
Precise estimation of parameters is desired for realizing upcoming quantum technologies such as quantum information processing.
Quantum metrology is a promising method that offers higher precision sensing of target parameters than classical counterparts by exploiting enta... |
2,869,038,156,948 | arxiv | \section{INTRODUCTION}
Solid particles of refractory substances are formed at high temperature in the outer shells and in the cooling outflows of evolved stars \citep[e.g.,][]{Ferrarotti06}, and in supernova ejecta \citep[e.g.,][]{Sugerman06,Matsuura11}. They are eventually injected into the interstellar medium (ISM... |
2,869,038,156,949 | arxiv |
\section{Introduction}
\label{sec:Intro}
It is possible for new phenomena (NP) beyond the standard model (SM) of particle physics to be
observed either directly or indirectly, \ie, through their influence on other physics processes.
Indirect searches for NP generally proceed by comparing experimental results with the... |
2,869,038,156,950 | arxiv | \section{Introduction}
Markov-modulated Brownian motion~\cite{asmussen95,kk95}
is a popular tool to model continuous-time phenomena in a stochastic context. An MMBM can be described as the pair $\{Y(t), \phi(t)\}_{t \geq 0}$, where $\phi(t)$ is a continuous-time Markov chain on a state space $\mathcal{S} = \{1,2,\dots... |
2,869,038,156,951 | arxiv | \section{The Model}
\label{sect_model}
The model \cite{Knochel:2008ks} is based on Higgsless models proposed in \cite{Csaki:2003dt,Cacciapaglia:2004rb}. They are constructed in 5D using a warped background inspired by the RSI scenario \cite{Randall:1999ee},
$ g_{\mu\nu}=\eta_{\mu\nu}e^{-2 R k y}\quad g_{55}=-R^2\quad y... |
2,869,038,156,952 | arxiv | \section{1. Introduction}
It is well known that Maxwell equations can be generalized in a non-linear way, adding to the Lagrangian
higher powers of the invariants constructed from the electromagnetic field. Well-known examples are the corrections due to
quantum electrodynamics that were proposed by Heisenberg and Euler... |
2,869,038,156,953 | arxiv | \section{Algorithm}
In this section, we describe a decision procedure for a local theory
extension, say $({\Theory_0}, \axioms_e, {\Theory_1})$, which
can be easily implemented in most SMT solvers with quantifier
instantiation support. We describe our procedure
$\mathfrak{D}_{{\Theory_1}}$ as a theory module in a typi... |
2,869,038,156,954 | arxiv | \section{Introduction}
This paper was motivated by problems posed by Ie.~Lutsenko and I.V.~Protasov in a preliminary version of the paper \cite{LP2} devoted to relatively thin sets in groups.
Following \cite{LP1}, we say that a subset $A$ of a group $G$ is {\em thin} if for any distinct points $x,y\in G$ the interse... |
2,869,038,156,955 | arxiv | \section{Introduction}
The Los Alamos National Laboratory (LANL) designed and built Mars Odyssey Neutron Spectrometer (MONS) has been continuously measuring the leakage flux of neutrons from a Mars polar orbit since February 2002. These data have been used to map the hydrogen content of Mars up through July 2009 \ci... |
2,869,038,156,956 | arxiv | \section{Introduction}
In hierarchical clustering theories of structure formation,
like the cold dark matter (CDM) models,
small mass clumps of dark matter form first and gather into larger
and larger masses subsequently. The structure of these dark matter
"halos", is likely to be related to how the halos formed,
... |
2,869,038,156,957 | arxiv | \chapter{Generalized event structures and probabilities}
\begin{center}
{Karl Svozil}\\
{\it Institute for Theoretical Physics, Vienna University of Technology}\\
{\it Wiedner Hauptstra\ss e 8-10/136, A-1040 Vienna, Austria}\\
{\it email: {svozil@tuwien.ac.at} homepage: {http://tph.tuwien.ac.at/\char`\~svozil} ... |
2,869,038,156,958 | arxiv | \section{Preliminaries}\label{appen:pre}
We use ${\mathcal{F}}_r$ to denote the filtration generated by
\begin{align*}
\{\xi_t^i:t\in {\mathcal{I}}_l,i=1,...N\}_{l=1}^{r-1} \cup \{\widetilde{\xi}_l^i:i=1,...N\}_{l=1}^{r-1}.
\end{align*}
It means that given ${\mathcal{F}}_r$, the global solution $\bar{\vx}_r$ is fix... |
2,869,038,156,959 | arxiv | \section{Introduction}
Supersymmetry (SUSY) \cite{SUSY_refs} is a promising extension of the
Standard Model of particle physics (SM) \cite{SM_refs}; the simplest
form is denoted the supersymmetric SM (SSM). It should be imminently
testable at the LHC \cite{LHC_refs}. Supersymmetric particles, if they
exist, typically d... |
2,869,038,156,960 | arxiv | \section{Introduction}
\label{Sec:Introduction}
The nature of matter has long been a source of philosophical debate:
Around 400BC, Democritus and Leucippus postulated an indivisible unit which they called the atom \citep{Coveney_highfield}.
With no evidence for the existence of atoms and the apparent continuous natu... |
2,869,038,156,961 | arxiv | \section{Introduction}
In \cite{pseudo-split}, Loughran-Skorobogatov-Smeets develop, building upon work of Denef \cite{denef}, a necessary and sufficient criterion to say when a morphism of varieties over a number field $k$ is surjective on $k_v$-points for almost all finite places $v$. This property is called \emph{ar... |
2,869,038,156,962 | arxiv | \section{Introduction}\label{section1}
Throughout this text all functions we consider are real-valued. Let $\Omega$ be a Lipschitz bounded domain of $\mathbb{R}^n$ ($n\ge 3$), with boundary $\Gamma$, and set
\[
C_+(\overline{\Omega})=\{ \sigma \in C(\overline{\Omega});\; \sigma >0\; \mbox{in}\; \overline{\Omega}\}.
... |
2,869,038,156,963 | arxiv | \section{Introduction}
Structurally or magnetically disordered glassy systems show special characteristics like memory effects or replica symmetry breaking as a result of a complex energy landscape. A large number of local minima or metastable states exist and can trap the system at low temperatures. Therefore, these... |
2,869,038,156,964 | arxiv | \section{Introduction}
The properties of physical, biological and many other systems
can be described by differential and recursive equations; the
latter are also called discrete dynamical system (see e.g.
\cite{De}, \cite{GR}, \cite{Sh}). Also systems of non-linear, higher dimensional
recursive equations arise in sol... |
2,869,038,156,965 | arxiv | \section{Introduction}
Homological quantum codes \cite{Martin,PHD} are an important class of stabilizer codes, each of them is constructed by selecting a special basis for each vector space in a short chain complex. The most common types of homological quantum codes are surface codes and color codes. In surface code's ... |
2,869,038,156,966 | arxiv | \section{Introduction}
There is evidence for solar or super-solar metallicities in the circumnuclear environments
of quasars out to redshifts $z$$>$4 (e.g., Hamann \& Ferland 1999; Kurk et al. 2007;
Jiang et al. 2007; Juarez et al. 2009; Matsuoka et al. 2009). This evidence, mainly
from optical lines, is supported ... |
2,869,038,156,967 | arxiv | \section{Introduction}
Event cameras, also known as neuromorphic cameras, have successfully opened their path to the computer vision and robotics society for its low cost and high dynamic sensing range with low latency and low power consumption.
It represents the changes of intensity for a pixel location $(x,y)$ as a... |
2,869,038,156,968 | arxiv | \section{Introduction}
Modern optical time-domain surveys, unbiased with respect to host galaxy environment, have discovered superluminous supernovae (SLSNe) with luminosities exceeding those of normal supernovae (SNe) by at least an order of magnitude \citep{Quimby2011,Chomiuk2011,Gal-Yam2012}. This has dramatically... |
2,869,038,156,969 | arxiv | \section{Introduction} The origin of associated absorption systems (AAS) in the
spectra of QSOs with \ensuremath{\beta}~$<$ 0.01\footnote{\ensuremath{\beta}~ is the relative velocity of
the absorption systems with respect to the systemic redshift of the QSO in
units of velocity of light} (the relative velocity of the A... |
2,869,038,156,970 | arxiv |
\section{Introduction}\label{sec:intro}
ESA's {\it Gaia}\ mission \citep{GaiaMission} is an enormous project that is revolutionising Milky Way astronomy. {\it Gaia}\ will provide a wide range of data about the stars of the Milky Way, including photometry and spectroscopy. However it is the astrometry -- and in particu... |
2,869,038,156,971 | arxiv | \section{Introduction}
In \cite{Dvlag} we found differential equations of spectral type
satisfied by the generalized Laguerre polynomials
$\left\{L_n^{\alpha,M}(x)\right\}_{n=0}^{\infty}$ which are
orthogonal on the interval $[0,\infty)$ with respect to the
weight function
$$\frac{1}{\Gamma(\alpha+1)}x^{\alpha}e^{-x}+M... |
2,869,038,156,972 | arxiv | \section*{Acknowledgments}
\noindent
We thank the ICHEP2022 organizers and convenors for the conference and the invitation.
The work of J.~Fiaschi has been supported by STFC under the Consolidated Grant ST/T000988/1.
S.~Moretti is supported in part through the NExT Institute and acknowledges funding from the STFC Conso... |
2,869,038,156,973 | arxiv | \section{Introduction}
One of the main problems in understanding galaxy formation is that star formation is extremely complex. The gas out of which stars form is a turbulent mix of forces in which gravitational collapse, thermal pressure, magnetic fields, cosmic ray pressure and energy from supernovae all fight for do... |
2,869,038,156,974 | arxiv | \subsection{Paper length}
Papers must be 9~pages in length, {\em excluding} the bibliography.
{\bf Papers which are
clearly overlength will not be reviewed}. This includes papers where the
margins and formatting are deemed to have been significantly altered from
those laid down by this style guide. The reason such pa... |
2,869,038,156,975 | arxiv | \section{Cubic B\'{e}zier Splines\label{sec:bezier}}
SVG can produce graceful curves by graphing quadratic and cubic equations.
As mentioned before, in jQuery.Feyn we use cubic B\'{e}zier segments to
approximate the photon and gluon propagators (for the line type, gluon
propagators are drawn as elliptical arc paths su... |
2,869,038,156,976 | arxiv | \section{Introduction}
Machine learning methods \cite{haykin:08,goodfellow:16,bishop:06} have
found applications in condensed matter physics detecting phases of
matter and transitions between these on both quantum and classical
systems (see, for example,
Refs.~\cite{ronhovde:11,nussinov:16,carrasquilla:17,chng:17,tana... |
2,869,038,156,977 | arxiv |
\section{Hyperbolic anti-concentration bound}\label{sec:anticon}
\subsection{Our result}
In this section, we will prove an anti-concentration bound for random vectors with respect to the hyperbolic norm, which generalizes the result for PSD matrices in \cite{ay21}. In particular, an important tool we use is the hyper... |
2,869,038,156,978 | arxiv | \section{Introduction}
The combinatorial definition of a \emph{Magidor cardinal} $\lambda$ is given by $\lambda\rightarrow[\lambda]^{\aleph_0\text{-bd}}_\lambda$.
Recall that $[\lambda]^{\aleph_0\text{-bd}}$ is the family of all countable bounded subsets of $\lambda$. It contains subsets of any countable order type. ... |
2,869,038,156,979 | arxiv | \section{Introduction}
\section{Motivation}
F. B. Jones \cite{jones} proved in 1942, in a famous paper,
the existence of additive discontinuous functions
$f:\mathbb{R}\to\mathbb{R}$ whose graph
$G(f)=\{(x,f(x)):x\in\mathbb{R}\}$ is connected, and characterized them.
These functions are extraordinary since
their graph... |
2,869,038,156,980 | arxiv | \section{Introduction}
The search for Higgs bosons is among the prime tasks of the CERN Large Hadron
Collider (LHC) \cite{Kunszt:1991qe}.
While the standard model (SM) of elementary-particle physics contains one
complex Higgs doublet, from which one neutral $CP$-even Higgs boson $H$
emerges in the physical particle sp... |
2,869,038,156,981 | arxiv | \section{Introduction}
In this paper, we consider the following one-dimensional nonlocal boundary value problem,
\begin{equation}\label{1}
\left\{
\begin{array}{ll}
\epsilon v''+(a_2-\frac{b_2 \lambda}{1+v}-c_2v)v=0,&x \in (0,L), \\
v'(0)=v'(L)=0,\\
\int_0^L \frac{a_1-c_1v}{1+v}-\frac{b_1 \lambda}{(1+v)^2} dx=0,
\... |
2,869,038,156,982 | arxiv | \section{Introduction}
Dust scattering of starlight by UV bright stars in our own Milky Way is now known to explain the majority of the diffuse far ultraviolet (FUV, $\sim$1300-1800 \AA) background. However, interest in the diffuse FUV background began not with a focus on Galactic dust, but with a search for a cosmol... |
2,869,038,156,983 | arxiv | \section{\label{sec:Sec1}Introduction}
A systematic measurement of energy dependence of the elastic scattering of positive pions from $^{12}C$ presented in Ref.\cite{Alex98} showed oscillations in the excitation function at energies around 35 MeV. The differential cross sections were measured at six scattering angle... |
2,869,038,156,984 | arxiv | \section{Introduction}
Understanding the mechanism of unconventional superconductivity, where the structure lacks an inversion symmetry has been a tough challenge ever since the discovery of the heavy fermion noncentrosymmetric (NCS) superconductor CePt$_{3}$Si \cite{Bauer2004,EBA}. The lack of an inversion center in ... |
2,869,038,156,985 | arxiv | \section{Introduction}
\label{Intro}
The paradigm example of a topological complexity invariant for dynamical systems
is topological entropy.
It measures the exponential growth, in time, of orbits distinguishable at finite
precision and can be used to compare the complexity of dynamical systems defined
on arbit... |
2,869,038,156,986 | arxiv | \section{Introduction}
\label{s:intro}
Recommender systems suffer from the well-known cold-start problem~\cite{schein2002methods} that arises when users have rated no or only few items. The cold-start problem is particularly problematic in neighborhood-based recommendation approaches such as collaborative filtering (... |
2,869,038,156,987 | arxiv | \section{Introduction}
Gradings for cluster algebras have been introduced in various ways by a number of authors and for a number of purposes. The evolution of the notion started with the foundational work of Fomin and Zelevinsky \cite{FZ-CA1}, who consider $\ensuremath{\mathbb{Z}}^{n}$-gradings where $n$ is precisel... |
2,869,038,156,988 | arxiv |
\subsection{\em ...}; the following
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\setlen... |
2,869,038,156,989 | arxiv | \section{Introduction}
In this article we study the regularization of the
minimization problem
\begin{equation}\label{OCPl}\tag{$\mathbb P_0$}
\min_{u\in\Uad} J_0(u)\quad\text{with}\quad
J_0(u):= \frac{1}{2} \norm{Tu-z}^2_{H}
\end{equation}
for $T:U \to H$ a given linear and continuous operator be... |
2,869,038,156,990 | arxiv | \section{Introduction}\setcounter{equation}{0}\quad
Kinks are examples of topological solitons (for a review see \cite{MS})
in one space dimension, which interpolate between distinct vacua.
A kink can be trivially embedded into three-dimensional Euclidean space as
a solution which is independent of all but one spatial ... |
2,869,038,156,991 | arxiv | \section{Staying in the Lorentz sector}
In the context of the attempts to provide a quantum theory of gravity
or to describe spacetime quantum-mechanically,
some works \cite{KotE, KotF, StaA}
have lately proved it quite useful to introduce
a peculiar sort of effective or quantum metric $q_{ab}$,
also called qmetric,
... |
2,869,038,156,992 | arxiv | \section{Price competition and breaking the ``Bertrand curse''}
\label{s:bertrand-single}
The results of Appendix~\ref{s:cournot} were for the Cournot notion of
competition by offered capacity. Each SP decides to serve demand $q_i$ and
then the price is determined by the total capacity $q_1+q_2$. The main
alternative n... |
2,869,038,156,993 | arxiv | \section{Future Work}
We are interested in making the circuit design system more intelligent by incorporating a circuit simulator (e.g., SPICE), a physics engine (e.g., Open Dynamics Engine) to simulate printed characters' dynamics, a schematic image recognition system~\cite{Arvo:2000:FSC:354401.354413}, or an intera... |
2,869,038,156,994 | arxiv | \section*{Methods}
\textbf{Material growth.} Multiple Bi$_2$Se$_3$/EuSe\ heterostructures are grown using molecular beam epitaxy (MBE), details of the growth, structural and magnetic characterization of EuSe films grown on different substrates can be found in Ref.~\onlinecite{Wang2022a}. For this study we use EuSe(001... |
2,869,038,156,995 | arxiv | \section{Introduction}
The region-based object detectors~\cite{rcnn,fastrcnn,fasterrcnn,fpn,cascade,ecr} popularized by R-CNN framework~\cite{rcnn} are conceptually intuitive and flexible, and have achieved top accuracies on challenging benchmarks like MS-COCO~\cite{coco}. Region-based detectors first generate a spars... |
2,869,038,156,996 | arxiv | \section{Introduction}
Chiral magnets have attracted a great deal of attention for a long time \cite{dzyaloshinskii1964,bak1980theory,muhlbauer2009skyrmion}. The absence of inversion symmetry in the atomic lattice gives rise to twists of magnetization $\mathbf M(\mathbf r)$ in magnetically ordered states, which range ... |
2,869,038,156,997 | arxiv | \section*{References}}
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\textcolor{red}{\sf\underline{JA:}\ #1}
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\usepackage{lineno}
\begin{document}
\nolinenumbers
\title{SMIXS: Novel efficient algorithm for non-parametric mixture regression-based clustering}
\author{Peter Ml... |
2,869,038,156,998 | arxiv | \section{Introduction} \label{Introduction}
The interaction between atoms and surfaces is of fundamental importance in the fields of physics, chemistry and biology. For example, atom-surface interactions play an important role in atomic force microscopy \cite{Binnig} and they also affect the dynamical properties of an ... |
2,869,038,156,999 | arxiv |
\section{Home-grown Efficiency Maps \label{EMcreation}}
While most efficiency maps included in the {SModelS\,v1.1}\ database were directly provided by the experimental collaborations as auxiliary material for their publications, we also produced a number of them ourselves in order to improve the coverage of simplif... |
2,869,038,157,000 | arxiv | \section*{References}
|
2,869,038,157,001 | arxiv | \section{Introduction}
Ever since the proposition, in 1988, by Tsallis \cite{tsallis0}, \cite
{tsallis1} of a nonextensive generalization of the canonical formalism of
statistical mechanics a spirited discussion \cite{cho1}, \cite{latora1} has
grown on the foundations of this branch of physics. But, only until recentl... |
2,869,038,157,002 | arxiv | \section{Introduction}
A large body of observational evidence from the scale of dwarf galaxies to cosmological scales indicates that 27\% of the mass-energy content of the Universe is in the form of dark matter (DM)~\cite{Ade:2015xua,Bertone:2010zza}. Galaxies like our own are believed to be embedded in a DM halo whi... |
2,869,038,157,003 | arxiv | \section*{Introduction}
In \cite{Sim1} and \cite{Sim2}, Simpson defined the coarse Betti, de Rham and Dolbeault moduli spaces of a smooth projective complex variety. These are all algebraic spaces, with a complex analytic isomorphism between the Betti and de Rham moduli spaces.
The non-abelian Hodge Theorem of \ci... |
2,869,038,157,004 | arxiv |
\section{Introduction}
Current cellular networks are expected to evolve towards heterogeneous networks (HetNets) to cope with the explosive demand for wireless data \cite{HetNet1-Qualcomm11,HetNet2-Ghosh12}. This requires service providers (SPs) to deploy small-cells in addition to traditional macro-cells. While typic... |
2,869,038,157,005 | arxiv | \section{Introduction}
\label{S0}
In the coevolving voter model, an actor placed at a node of a social network either copies the state of his/her neighbor, or rewires the link as to connect another node in the same state as him/herself \cite{vzqz}. In the related Monte Carlo scheme, this decision is taken by randomly s... |
2,869,038,157,006 | arxiv | \section{Introduction}
In multi-agent emergent communication research, one of the long-term goals is to develop machines that can successfully communicate between themselves but also with humans. Visual communication in the form of sketching and drawing, which has long preceded written language communication, can direc... |
2,869,038,157,007 | arxiv | \section{Introduction}
\label{sec:intro}
Rogue waves threaten safety and survivability of marine structures. The mechanisms leading to the formation of such extreme waves have been investigated and probabilistic descriptions derived to provide improved design criteria (e.g. \cite{perlin2013breaking,bitner2014occurrenc... |
2,869,038,157,008 | arxiv | \section{Introduction}
The most valuable characteristics of quantum systems are quantum correlations such as entanglement, which represents a useful resource for applications unattainable in the framework of classical theory, such as quantum teleportation, quantum cryptography and dense coding \cite{hor, brus}. In the... |
2,869,038,157,009 | arxiv | \section{}
{\bf Abstract.}
We
define the twisted de Rham cohomology and show how to use it
to define the notion of an integral of the form
$\int g(x) e^{f(x)}dx$ over an arbitrary ring. We discuss also a definition of a family of integrals and some properties of the homological definition of integral.
We show how to... |
2,869,038,157,010 | arxiv | \section{Introduction}
\label{sec:introduction}
\vspace{-6pt}
Recent years have witnessed exciting achievements in the development of highly capable deep neural networks (DNNs), to the extent that new state-of-the-art (SOTA) results are being published frequently.
However, achieving this level of performance requires ... |
2,869,038,157,011 | arxiv | \section{Introducción}
Sir Isaac Newton (1642-1727) cuando concibió el principio de inercia imaginó la
existencia de un objeto masivo que mantenía su estado en movimiento rectilíneo
uniforme. De hecho, Newton suponía que los objetos físicos pueden existir por
sí mismos, de manera que podemos abstraer su existencia d... |
2,869,038,157,012 | arxiv | \section{Introduction}
Although the MSSM is the leading candidate for new physics beyond
the Standard Model and sensible explains electroweak symmetry
breaking by stabilizing the energy scale, it still leaves with no
answer the open problems of the SM, among them the flavor
problem \cite{FN}\cite{Diaz-Cruz:2001gf}. Fur... |
2,869,038,157,013 | arxiv | \section{Introduction}
One system that has long been a
paradigm of the quantum optics community is a single-atom coupled
to a single mode of the electromagnetic field, the Jaynes-Cummings
model\cite{JC}. In practice the creation of a preferred
field mode is accomplished by the use of an optical resonator.
This resona... |
2,869,038,157,014 | arxiv | \section{Introduction}
\label{sec:intro}
In gravitational and gauge theories, asymptotic symmetries (AS) are a global remnant of large diffeomorphisms and gauge transformations which act non-trivially on physical data at spacetime infinity. The classic example of infinite-dimensional AS, and in many ways the best unde... |
2,869,038,157,015 | arxiv | \section{Introduction}
For non interacting systems, the appearance of non dissipative Hall-like currents is due to the existence of topological structures present in the electronic spectrum\cite{TKN82,KM05}. In the case of the quantum Hall effect (QHE) the physical ingredient allowing for such structure is the presenc... |
2,869,038,157,016 | arxiv | \section{Introduction}
\label{sec:intro}
It has been more than a century since astrophysical jets were first observed \citep{Curtis1918PLicO..13....9C}. Astrophysical jets are collimated relativistic magnetized plasma outflows launched from compact accreting objects. They are found in stellar-mass black holes (BH; \ci... |
2,869,038,157,017 | arxiv | \section{Introduction}
Elliptic fibrations are a versatile tool for studying algebraic surfaces.
One of their key advantages is that one can often compute the N\'eron-Severi\ lattice,
and in particular the Picard number, in a systematic way.
This has been carried out with great success in the study of K3 surfaces.
The... |
2,869,038,157,018 | arxiv | \section{Approach}
\label{sec:approach}
We are interested in using echoes for predicting depth map of a scene. There is a spatio-temporal relationship between the received echoes and the depth of the scene, i.e\onedot the echoes received at different instant of time directly relate to the different depths in the scene.... |
2,869,038,157,019 | arxiv | \section{\label{sec:intro} Introduction}
Bennett~{\em et~al.}~\cite{Bennett93} showed that an unknown quantum state (a qubit) could be {\em teleported} via two classical bits with the use of a maximally entangled Bell state shared between the sender and receiver. The significance of teleportation as a tool for quantu... |
2,869,038,157,020 | arxiv | \section{Introduction}
In this paper, we consider the feedback interconnection shown in Figure \ref{fig:StableNegativefeedback}, where a linear system $G$ is in feedback with a sector-bounded nonlinearity $\Phi$, and we are interested in conditions that guarantee closed-loop stability.
Different forms of this problem... |
2,869,038,157,021 | arxiv | \section{Introduction}
In this article we apply Deift-Zhou's non-linear steepest descent method to the 5th order MKdV equation:
\begin{equation}\label{eq:5th mkdv}
q_t=30q^4q_x-10q^2q_{xxx}-40qq_{xx}q_x-10q_x^3+q_{xxxxx}
\end{equation}
which belongs to the AKNS hierarchy~\cite{AKNS1974}. As is well known in the in... |
2,869,038,157,022 | arxiv | \section{Introduction}
\begin{quote}
\emph{How do geometric constraints restrict the combinatorics of polytopes?}
\end{quote}
One instance of this question asks for the combinatorial types of $d$-polytopes
that are \emph{inscribable}, that is, that have realizations with all vertices
on a sphere. This question was r... |
2,869,038,157,023 | arxiv | \section{Introduction}
\label{sec-intro}
\subsection{Overview}
We study a family of probability measures on spanning-tree-decorated rooted planar maps, which we
define in Section~\ref{sec-burger}, using a generalization of the Sheffield hamburger-cheeseburger model~\cite{shef-burger}.
This family includes as special c... |
2,869,038,157,024 | arxiv | \section{Introduction}
All realistic quantum systems interact with an environment and a proper description of their dynamics calls for the toolbox of open quantum systems theory \cite{bp, weiss}. In this framework the simplest type of noise is described by a Markovian master equation in the Lindblad form, corresponding... |
2,869,038,157,025 | arxiv | \section{Frequency-Dependent Cable Parameters}
\label{app:cable-parameters}
\subsection{Impact on the Branch Admittance of the Line Model}
\begin{figure}[ht]
\centering
\includegraphics[width=0.8\linewidth]{Figures/FreqDepParams_LineAdmittance.pdf}
\caption{%
Comparison of line branch admittances... |
2,869,038,157,026 | arxiv |
\section{Proof of Lemma~\ref{lemma:clique_sunflower}}
Let $\mb U_{n,q} \subseteq [n]$ be a $q$-random subset of $[n]$
(independent of $\mb G(n,p)$).
Let $c_1 \defeq \ln(1/\eps)$ and for $\ell \ge 2$,
let $c_\ell \defeq 2\ln(1/\eps)\sum_{j=1}^{\ell-1}\binom{\ell}{j}c_j$.
\begin{lemma}
$c_\ell \le \ell!(2\log(1/\ep... |
2,869,038,157,027 | arxiv | \section{Probability distributions at longer times}
As discussed in the main text, all states in the quasienergy
spectrum contribute to the probability distribution of the walker. Since most of the states are non-critical, the probability distribution for static binary disorder thus follows $|\psi(q)|^2\sim e^{-|q|/\... |
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