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3,212,635,537,606 | arxiv | \chapter{\bf Acknowledgements} I would like to thank Ramy Brustein, Gary
Horowitz, and Joe Polchinski, for discussions. This work is partially
supported by Department of Energy contract No.
DE-AC02-86ER40253.
\refout
\end
|
3,212,635,537,607 | arxiv | \subsection{Please Capitalize the First Letter of Each Notional Word in Subsection Title}
\section{Introduction}
\label{sect:intro}
Now it is a golden era to study galaxy formation and evolution.
Fortunately, elliptical galaxies supply us a good chance to carry
out this work because they seem to be homogeneo... |
3,212,635,537,608 | arxiv |
\section*{Acknowledgement} We would like to thank Huy Ha, Zeyi Liu, and Mandi Zhao for their helpful feedback and fruitful discussions. This work was supported in part by NSF Awards 2037101, 2132519, 2037101, and Toyota Research Institute. Dr. Gan was supported by the DARPA MCS program and gift funding from MERL, Ci... |
3,212,635,537,609 | arxiv | \section{Introduction}
The recent years in gravitational physics were exciting for experimental physics as well as theoretical physics. The first detection of gravitational waves of a binary black hole merger \cite{Abbot:2016} and of a binary neutron star merger \cite{Abbot:2017} by LIGO/VIRGO mark the starting point o... |
3,212,635,537,610 | arxiv | \section{Introduction}
A diffraction grating, defined as a periodic optical structure with infinite extent in one direction diffracts waves incident on its surface~\cite{1}.
Being imposed by the periodicity of a grating, which can be of the order of a free-space wavelength or greater, an incident wave is scattered as... |
3,212,635,537,611 | arxiv | \section{Introduction}
Spin-orbitronics\cite{spin-orbitronics1,spin-orbitronics2} has attracted a lot of attention recently as a new subfield of spintronics\cite{Spintronics review1,Spintronics review2} in which the relativistic spin-orbit interaction (SOI) plays a central role. Spin-orbitronics includes generation and... |
3,212,635,537,612 | arxiv | \section{Introduction}
\label{Introduction}
Relativistic jet outflows from radio galaxies are a primary mechanism for
energy extraction from supermassive black holes in active galactic nuclei
(AGN) and an important source of
energy input to the intergalactic medium (IGM) in groups and clusters
(e.g. \citealt[and refer... |
3,212,635,537,613 | arxiv | \section{Introduction}
In this paper will consider the expansion properties of a random binomial simplicial complex past the threshold
for the cohomological connectivity.
This model was introduced by Linial and Meshulam~\cite{ar:LinMesh2006} and it is
a generalisation of the binomial random graph $G(n,p)$.
Let $Y(... |
3,212,635,537,614 | arxiv | \section{Introduction
The $N$th singular value~\cite{Watson-sing,B-C-Z}
is the algebraic number $k_N\in[0,1]$ for which
\begin{equation}
{\rm AGM}\left(1,\sqrt{1-k_N^2}\right)=\sqrt{N}\,{\rm AGM}(1,k_N)
\label{k-N}
\end{equation}
where the arithmetic-geometric mean (AGM) is obtained by
iterating the rapidly convergent... |
3,212,635,537,615 | arxiv | \section{Introduction}
\label{sec:intro}
Publishing new research in journals/conferences is a common practice in the scientific community. It is noticed that papers of few authors consistently get accepted in journals whereas papers of certain other authors get rarely accepted\footnote{https://www.sciencemag.org/career... |
3,212,635,537,616 | arxiv | \section{acknowledgments}
We gratefully acknowledge financial support by the Deutsche Forschungsgemeinschaft through the research unit FOR 1162 (projects Ge1855/10-2 and Fa222/5-2) as well as experimental support by R. H{\"{o}}lldobler.
\providecommand{\noopsort}[1]{}\providecommand{\singleletter}[1]{#1}%
|
3,212,635,537,617 | arxiv | \section{Introduction}
Let $\Omega\subset \mathbb{R}^n$ be a bounded domain with the boundary $\partial\Omega$ of
$C^2$ class. We set $Q=\Omega \times (0,T)$, where $T>0$. We use notations
$\partial_t= \frac{\partial}{\partial t}$, $\partial_i=\frac{\partial}{\partial x_i}$ ($i=1,2,\ldots, n$).
We also use the mul... |
3,212,635,537,618 | arxiv | \section{Introduction}
For statistical hypothesis testing, one of the widely-used conventional methods
is using the Student $t$-test statistic,
\[
T= \frac{\bar{X}-\mu}{S/\sqrt{n}},
\]
where $\bar{X}$ is the sample mean and $S$ is the sample standard deviation.
However, a statistical inference using this Studen... |
3,212,635,537,619 | arxiv | \section{Force-Extension Relation}
As a first step towards an understanding of the macroscopic viscoelastic
properties of an entangled network of wormlike chains one has to understand the
elastic properties of a single wormlike chain. The linear force-extension
relation of a wormlike chain is obtained by the following ... |
3,212,635,537,620 | arxiv | \section{Introduction} \label{sec:intro}
In many real world problems, optimization decisions have to be made with limited information. Whether it is a static optimization or dynamic control problem, obtaining detailed and accurate information about the problem or system can often be a costly and time consuming process... |
3,212,635,537,621 | arxiv | \section{Introduction}
\section{Introduction}
Expressions involving products of Dirac spinors are among the most common objects appearing in the problems of high energy physics. For example, any Feynmann diagram involving fermions includes Dirac bilinears (e.g. as in FIG. I). Various conventions for spinors are prese... |
3,212,635,537,622 | arxiv |
\section{Deep Impact Framework}
\boldparagraph{Document Expansion.}
In our approach, we leverage \textsf{DocT5Query}\ document expansion to enrich the original document collection with expansion terms. As noted by \citet{doc2query}, document expansion can be seen as a two-fold approach. By adding terms that are alr... |
3,212,635,537,623 | arxiv | \section{Introduction}
In most challenging real-world supervised machine learning tasks in model serving such as sentiment analysis of Twitter users and weather forecasting, data evolve and change over time, causing the machine learning models built on historical data to become increasingly unreliable. One reason is u... |
3,212,635,537,624 | arxiv |
\section{Introduction}
\vspace{-0.08in}
\LetLtxMacro{\section}{\oldsection}
\vspace{-0.06in}
{
\bibliographystyle{style/IEEEtran}
\section{Introduction}
\setlength{\epigraphwidth}{0.9\columnwidth}
\renewcommand{\epigraphflush}{center}
\epigraph{All simulations are wrong, but so... |
3,212,635,537,625 | arxiv | \section{Introduction}
Black hole binaries (BHB) transit through different ``spectral states'' during their outbursts. The two canonical ones are the soft state (also known as ``high'' state, hereafter HSS) and the hard state (also known as ``low'' state, hereafter LHS).
In the HSS, the emission
is dominated by a bri... |
3,212,635,537,626 | arxiv | \section{Introduction} \label{sec:introduction}
Observations of local Milky Way clouds show that the bulk of molecular
gas is inert with star formation concentrated in the small fraction of
the cloud at high surface density
\citep[][]{2010ApJ...723.1019H,2010ApJ...724..687L,2012ApJ...745..190L}. This
observation lead... |
3,212,635,537,627 | arxiv | \section{Introduction and motivation}
\label{introduction}
\flo{- Why generative models are cool}
Generative models have interesting properties, as shown in \cite{ng2002discriminative} where the conditional distribution $P( Y | X )$(X represents the samples and Y the classes) learned by a generative model is compare... |
3,212,635,537,628 | arxiv | \section{Splitting of a cotangent bundle}
\medskip \par
For the dynamical systems with a high degree of symmetry it is natural to
try to parametrize as much of the phase space, as possible by the global
constants of motion. \par
In the case of geodesic motion on a semisimple group manifold (with the
Hamiltonian being ... |
3,212,635,537,629 | arxiv | \section*{Some comments and Open Problems}
In contrast to Theorem~\ref{main}, Theorem~\ref{main2} is true for the Euclidean plane $E^2$ even in a stronger form: for any subset $C\subset E^2$ not lying on a line and any partition $E^2=A_1\cup A_2$ one of the cells of the partition contains an unbounded subset symmetric... |
3,212,635,537,630 | arxiv | \section{Detection Method}\seclab{method}
Cosmic $\nu_{\tau}$ can produce taus\footnote{Other neutrino flavors can be neglected, as the electron range in matter at these energies is too short and the muon decay length too large.} under the Earth surface through charged-current interactions. Taus may then exit and deca... |
3,212,635,537,631 | arxiv | \section{Introduction} \label{sec:intro}
Over the duration of its operation, from 2009--2013, the Herschel Space Observatory (HSO) enabled observations of the fundamental rotational transitions of a variety of molecular hydrides and hydride ions, several of them being newly discovered. Many of these transitions cannot ... |
3,212,635,537,632 | arxiv | \section{Introduction}
\label{introduction}
Count data are random variables that assume non-negative integer values
and represent the number of times an event occurs in the observation
period. This kind of data is common in crop sciences, such as the number
of grains produced by a plant, number of fruits produced by a... |
3,212,635,537,633 | arxiv | \section{Introduction}
One of the major goals of evolutionary genomics is the identification of genomic changes that underpin phenotypic differences between species \cite{anisimova2012detecting}.
To identify such changes it is important to identify regions or even individual sites in molecular sequences that have be... |
3,212,635,537,634 | arxiv | \section{Introduction}
\setcounter{equation}{0}
Let $f$ be a rational or a transcendental entire function. For $n \in \mathbb{N} $, let $ f^{n}$ denote the $n^{th}$ iterate of $f$. The set \\
$ F(f) = \{ z : (f^n) $ is normal in some neighbourhood of $ z \}$ is called Fatou set of $f$ and its complement denoted ... |
3,212,635,537,635 | arxiv | \section{Introduction}
PKS\,1510--089\ is a bright flat spectrum radio quasar (FSRQ) located at a redshift of $z=0.36$ \citep{ta96}.
It was the second FSRQ to be detected in the very-high-energy (VHE, $>100$\,GeV) range \citep{ab13}.
The source is monitored by various instruments spanning the full range from radio up... |
3,212,635,537,636 | arxiv | \section{Introduction}
Let $k$ be a field. The Grothendieck ring of varieties $K_0(\mathbf{Var}_{/k})$ is as a group defined to have generators the isomorphism classes $[X]$ where $X$ is a variety over $K$, and relations $[X-Y] + [Y] = [X]$ where $Y \hookrightarrow X$ is a closed inclusion. The multiplication is indu... |
3,212,635,537,637 | arxiv | \section{Introduction}
We study programs with {\em monotone} constraints \cite{mt04,mnt03,mnt06}
and introduce a related class of programs with {\em convex} constraints.
These formalisms allow constraints to appear in the heads of program
rules, which sets them apart from other recent proposals for integrating
con... |
3,212,635,537,638 | arxiv | \section{Introduction\newline}
Polarons emerge naturally from cold atom mixtures with an extreme population
imbalance where minority atoms are so outnumbered by majority atoms that they may be considered impurities submerged in a host medium. Polaron studies have undergone an exciting revival in recent years, spark... |
3,212,635,537,639 | arxiv | \section{Introduction}
Submodularity is an important property that models a diminishing return phenomenon, i.e., the marginal value of adding an element to a set decreases as the set expands. It has been extensively studied in the literature, mainly accompanied with maximization or minimization problems of set function... |
3,212,635,537,640 | arxiv | \section{}
\section{\label{sec:level1}Introduction}
This study investigates the localization in the time-average of the absolute squares of the time-evolving wave function on the desymmetrized stadium billiard that occurs after the Gaussian wavepacket is launched as the initial state.
In chaotic billiards like... |
3,212,635,537,641 | arxiv | \section{Introduction}
Massive type IIA supergravity \cite{Romans:1985tz} admits a consistent truncation on the six-sphere to maximal supergravity in four dimensions with gauge group $\textrm{ISO}(7) = \textrm{SO}(7) \ltimes \mathbb{R}^7$ \cite{Guarino:2015jca,Guarino:2015vca}. The gauging is dyonic, in the sense of \... |
3,212,635,537,642 | arxiv | \section{Introduction}
Multidimensional continued fractions (MCFs) were introduced by Jacobi \cite{Jac} in order to answer to a question posed by Hermite \cite{Her}, namely the existence of an algorithm defined over the real numbers that becomes eventually periodic when it processes algebraic irrationalities. In oth... |
3,212,635,537,643 | arxiv | \section*{ABSTRACT}
\begin{quote}
\begin{small}
We have found provably optimal algorithms for full-domain discrete-ordinate
transport sweeps on a class of grids in 2D and 3D Cartesian geometry that
are regular at a coarse level but arbitrary within the coarse blocks. We describe these algorithms and show that they alw... |
3,212,635,537,644 | arxiv | \section*{Non-equilibrium condensation}
The optical mode in our system is provided by a 2D array of silver nanorods (NRs) where the LSPs of the individual nanoparticles are coherently coupled with each other through the diffraction orders propagating in the plane of the array, thus sustaining SLRs. The NRs array, whos... |
3,212,635,537,645 | arxiv | \section{Introduction}
\iffalse
Things to write about.
Comparisons to
\begin{enumerate}
\item Sums of products of univariates.
\item Ankit Gupta's PIT paper...need to read it slightly
\item Any other non-multilinear PIT of larger than depth 3....Shubhangi might know
\item Can handle polylog top fan-in for depth three... |
3,212,635,537,646 | arxiv | \section{Introduction}
\label{intro}
Observations of the Cosmic Microwave Background (CMB) radiation are one of the most powerful tools to study the early Universe, also they can provide precise measurement of the cosmological parameters. Starting with COBE's groundbreaking detection, in the past two decades there has... |
3,212,635,537,647 | arxiv | \section{Introduction}
Let $V$ be finite-dimensional $\mathbbm{C}$-vector space,
$W \subset \GL(V)$ be a finite (pseudo-)reflection group
with corresponding hyperplane arrangement $\mathcal{A}$.
We assume that $\mathcal{A}$ is essential, meaning
that $\bigcap \mathcal{A} = \{ 0 \}$ and denote $n = \dim V$ the
rank of ... |
3,212,635,537,648 | arxiv | \section{Introduction}
Information in the brain is mainly represented in the form of neural impulses.
All those impulses are roughly identical in their height and width and called
spikes, see Fig. \ref{spikes}.
The only thing which matters is the time when such an impulse
has been generated or received.
If neural impul... |
3,212,635,537,649 | arxiv | \section*{Abstract}
We solve the local and global structural identifiability problems for viscoelastic mechanical models represented by networks of springs and dashpots. We propose a very simple characterization of both local and global structural identifiability based on \emph{identifiability tables}, with the purp... |
3,212,635,537,650 | arxiv | \section{Introduction}
There is a considerable recent interest in two directions of classical and
quantum gravity and possible implications in cosmology and astrophysics:\
The first one is related to gravity models with anisotropic scaling between
space and time at short distances which is usually referred to as ... |
3,212,635,537,651 | arxiv | \section{Introduction}
One-dimensional (1D) quantum wires and the junctions of several 1D
quantum wires are expected to be important
for potential applications as components in future nano-electronic devices.
Such 1D quantum wires with interacting electrons are described by
the Tomonaga-Luttinger liquid (TLL) theor... |
3,212,635,537,652 | arxiv | \section{Introduction}
The two-term Machin-like formula for pi is given by
\begin{equation}\label{eq_1}
\frac{\pi }{4} = {\alpha _1}\arctan \left( {\frac{1}{{{\beta _1}}}} \right) + {\alpha _2}\arctan \left( {\frac{1}{{{\beta _2}}}} \right),
\end{equation}
where ${\alpha _1}$, ${\alpha _2}$, ${\beta _1}$ and ${\beta _... |
3,212,635,537,653 | arxiv | \section{Introduction}
It has been a longstanding challenge to predict accurately the
equation of state and in particular the phase diagrams of fluids
and fluid mixtures from atomistic models via computer
simulation.\cite{1,2,3,4,5} Such applications have required a widespread
development of computer simulation method... |
3,212,635,537,654 | arxiv | \section{Introduction}\label{sec1}
In the study of population genetics models, it is of great importance
to identify their stationary distributions. Such identifications
provide us with basic information of possible equilibria of the models
and are needed prior to quantitative discussions on statistical
inference.... |
3,212,635,537,655 | arxiv | \section{Introduction}
High-$P_T$ processes taking place in the background of the medium produced in ultrarelativistic heavy-ion (A-A) collisions are a cornerstone of the experimental A-A program at the LHC. The aim is to use these processes to do
``jet tomography'', i.e. to study both the short-distance physics of ... |
3,212,635,537,656 | arxiv | \section{INTRODUCTION}
In the recent paper~\cite{anos},
Adler, Nemenman, Overduin and
Santiago criticize a limit on the measurability
of distances which was originally
derived by Salecker and Wigner in the 1950s~\cite{wign}.
If correct, this criticism would have implications for all the recent
papers which have used ... |
3,212,635,537,657 | arxiv | \section{Introduction}\label{sec1}
In \cite{ambro}, the notion of quasi-log structures was introduced
in order to prove the cone and contraction theorem for $(X, \Delta)$ where
$X$ is a normal variety and $\Delta$ is an effective $\mathbb R$-divisor
such that $K_X+\Delta$ is $\mathbb R$-Cartier. Although the theory... |
3,212,635,537,658 | arxiv | \section{The HEGRA IACT Array}
The HEGRA IACT system is located on the Canary Island of La Palma,
at the Observatorio del Roque de los Muchachos
of the Instituto Astrofisico de Canarias,
at a height of about 2200~m asl.
In its final form, the HEGRA IACT array will consist of
five identical telescopes with 8.5~m$^2$ ... |
3,212,635,537,659 | arxiv | \section{Introduction}
The pragmatically applied rules of quantum mechanics involve two distinct laws of
evolution for the state of the system: these are the Schr\"odinger equation and quantum state reduction.
A long-standing problem is how to make sense of this since there is no underlying theory stating when one o... |
3,212,635,537,660 | arxiv | \section{Introduction}
In many industrial processes, one frequently faces a measured data that is composed of the true value of a signal and some random noise. One central problem in signal processing is to find the characteristics of noise, which is critical to many important tasks such as signal filtering, estimatio... |
3,212,635,537,661 | arxiv | \section*{Introduction}
\addcontentsline{toc}{section}{Introduction}
Localization in commutative algebra means a universal construction
where a set of chosen elements in a given commutative
ring is made invertible (they will become denominators):
the outcome is called a ring of fractions.
The classical exa... |
3,212,635,537,662 | arxiv | \section{Introduction}
In the preceeding paper, A. Shiryaev, Z. Xu and X.Y. Zhou \cite{SXZ} ask about the optimal time to sell a
stock
over a certain time interval $[0,T]$, knowing that the price is a geometrical Brownian motion with
a certain average return over the risk-free rate $a-r$ and a certain volatility $\s... |
3,212,635,537,663 | arxiv | \section{Introduction}
\setcounter{equation}{0}
The Jacobian conjecture was first formulated in 1939 by Keller \cite{K} which states that a polynomial
map $P:\bfF^n\to \bfF^n$ where $\bfF$ is a field of characteristic zero and $n\geq2$ has a polynomial inverse if the Jacobian
$J(P)$ of $P$ is a nonzero constant. This ... |
3,212,635,537,664 | arxiv | \section{Introduction and Main Results}\label{section1}
Over the last decade, significant progress has been made concerning the quenched invariance principle on random conductance models. A typical and important
example is random walk on the infinite cluster of supercritical
bond percolation on $\mathbb Z^d$. It is sho... |
3,212,635,537,665 | arxiv | \section{Introduction}
Entanglement plays a very important role in quantum information
processes \cite{yu1, wbps, AFOV, FLWDR} (see also references
therein). Even if different parts of the quantum system (quantum
register) are initially disentangled, entanglement naturally appears
in the process of quantum protocols... |
3,212,635,537,666 | arxiv | \section{Introduction}
Research in natural language processing (NLP) has traditionally focused on developing models for English and a small set of other languages with
large amounts of data (see~Figure \ref{fig:stats}, bottom right).
While the lack of data is generally cited as the key reason for the lack of progres... |
3,212,635,537,667 | arxiv | \section{Introduction}
In this note using non-smooth critical point theory together with classical
local invertibility results we consider locally invertible locally Lipschitz
functions $f
\mathbb{R}
^{n}\rightarrow
\mathbb{R}
^{n}$. We provide conditions for global invertibility of $f$. This note aims
at ans... |
3,212,635,537,668 | arxiv | \section{Introduction}
Triboelectric nanogenerators (TENGs) have received
considerable attention recently as potential candidates for energy
scavenging~\cite{envsci17, id1, id2, id4}. These devices have been
shown to convert mechanical energy into electricity in
applications such as energy harvesting and self-powered s... |
3,212,635,537,669 | arxiv | \section*{Introduction}
The use of discounting in optimal control and Hamilton--Jacobi equations theory is both motivated by the models used and very useful from a theoretical point of view. In the models, the discount accounts for the lesser influence of events far away in time. From the theoretical point of view, the... |
3,212,635,537,670 | arxiv | \section{Introduction}
Molecules are often used as tracers of the physical conditions of many astrophysical environments. Their presence and abundance, as well as their internal states, give strong constraints on the temperature, density, and also dynamics of the observed media. Observations are almost always supporte... |
3,212,635,537,671 | arxiv | \section{Introduction}
In recent years impressive progress has been achieved in fabricating,
functionalizing and controlling molecular junctions for charge transfer
[\onlinecite{reviews,cuniberti,scheer}] and as nano-machines
[\onlinecite{browne}].
This includes advanced techniques to link molecular structures to meta... |
3,212,635,537,672 | arxiv |
\section{Appendix}
\begin{table}[htb]
\renewcommand\thetable{A}
\centering
\caption{The performance (Agreement and test accuracy) of previous methods under the soft-label and the hard-label settings.
And the average performance reduction of each dataset under hard label is reported in the last row.}
\resizebox{\tex... |
3,212,635,537,673 | arxiv | \section{Introduction}
Integrable systems are widely investigated in $(1+1)$ dimensions,
where one of the dimensions stands for the time evolution variable
and the other one stands for the space variable. The space
variable is usually considered on continuous intervals, or both on
integer values and on $\mathbb{R}$ \c... |
3,212,635,537,674 | arxiv | \section{Introduction}
Recognizing actions and activities in videos is a long studied problem in computer vision \cite{bobick2001recognition,haritaoglu2000w,bregler1997learning}. An action is defined as a short duration movement such as jumping, throwing, kicking. In contrast, activities are more complex. An activity h... |
3,212,635,537,675 | arxiv | \section{Introduction}
\setcounter{equation}{0}
Shape optimization has started its development especially in the last quarter of the previous century and we just quote several
monographs devoted to this subject Pironneau
\cite{Pironneau1984},
Haslinger and Neittaanm\"aki \cite{Haslinger1996},
Sokolowski and Zolesio ... |
3,212,635,537,676 | arxiv | \section{Introduction}
In this note, we are interested in four theorems on spherical point configurations.
The first of these theorems is concerned with orthonormal representation of graphs.
The notion of orthonormal representation of a graph was introduced by Lov\'{a}sz in his study of Shannon capacity of graphs \cit... |
3,212,635,537,677 | arxiv | \section{Introduction}
In the Skyrme model of nuclear physics, both pions and nucleons are
represented by a single scalar SU(2) group valued field, $U(x)$.
Pions occur as field quanta, while baryons are instead represented as
topological solitons. The classical Skyrme theory, with a simple
quantisation of the spin and... |
3,212,635,537,678 | arxiv | \section{Introduction}
The quasinormal modes (QNMs) and quasinormal frequencies (QNFs)
\cite{Regge:1957td,Zerilli:1971wd, Kokkotas:1999bd, Nollert:1999ji, Konoplya:2011qq}
have recently acquired great interest due
to the detection of gravitational waves \cite{Abbott:2016blz}.
Despite the detected signal is consistent ... |
3,212,635,537,679 | arxiv |
\section{#2\protect\margine{#1}
\else\section{#2}
\fi
\paragrafonew{#2}
\global\advance\nparagrafo by 1 \setcounter{ES}{0} \setcounter{AS}{0}
\scrivi{#1}{p}{PARAGRAFO}{\nparagrafo}
}
\def\undefinedpagestyle{\relax}
\nofiles
\begin{document}
\bozzefalse
\REPORT
LABEL:sp%
DRIVEFIG:./SP/... |
3,212,635,537,680 | arxiv | \section{Quantum fluctuations of the gravitational field}
\indent
Gravity deals with the frame in which everything takes place,
i.e., with spacetime. We are used to putting everything into
spacetime, so that we can name and handle events. General
relativity made spacetime dynamical but the relations between
different ... |
3,212,635,537,681 | arxiv | \section{Introduction}
Two broad questions often occur in problems related to condensed matter systems: What sort of gapless phases can arise from finite density or charge density states? What kind of physics can emerge at a quantum critical point? In the absence of sharp quasiparticles or weakly coupled effective deg... |
3,212,635,537,682 | arxiv | \section{Introduction}
Since an international electron-positron ($e^-e^+$) linear collider (ILC)
can measure particle masses very accurately,
there is a growing consensus that the next high energy machine to be built
after the Large Hadron Collider (LHC) should be an ILC.
Such a machine is technically feasible an... |
3,212,635,537,683 | arxiv | \section{\bf Introduction}
Poisson cohomology, a way of parametrizing the deformations of a Poisson structure, is an important invariant in Poisson geometry. However, the computation of Poisson cohomology is quite difficult in general and few explicit results are known (\cite{Dufour}, p.43). One class of manifolds wher... |
3,212,635,537,684 | arxiv | \section{Introduction}
Nowadays, consumer demand for more functionalities, low power consumption and compact systems. Memory is an important part of many electronics gadgets. The major concern for memories is soft errors which are caused by radiation \cite{Dixit2011}, \cite{Ibe2010}. These soft errors corrupt the digit... |
3,212,635,537,685 | arxiv | \section{Introduction}
Language technologies have become important tools for content moderation on several platforms. Offensive content is either flagged or deleted completely. Some of these language technologies are trained on data that are labeled by annotators who provide ground-truth labels for the data samples. Ho... |
3,212,635,537,686 | arxiv | \section*{Acknowledgements}
We thank Adam Jermyn for useful discussions on typical stellar parameters and Liam O'Connor, Ben Hyatt, Adrian Fraser, Kyle Augustson, and Whitney Powers for their valuable feedback and discussions.
DL is supported in part by NASA HTMS grant 80NSSC20K1280.
EHA is funded as a CIERA Postdo... |
3,212,635,537,687 | arxiv | \section{Introduction}
Diagrams are a common feature of many everyday media from newspapers to school textbooks, and not surprisingly, different forms of \emph{diagrammatic representation} have been studied from various perspectives. To name just a few examples, recent work has examined patterns in diagram design \cit... |
3,212,635,537,688 | arxiv | \section{Introduction}
\label{sec:intro}
The tight-binding model on a honeycomb lattice with broken time-reversal
symmetry proposed by Haldane \cite{haldane1988model} is an interesting
example of a Chern band insulator \cite{kane13,rpp-rachel18}.
At half-filling, it can exhibit a quantized Hall conductance in the
a... |
3,212,635,537,689 | arxiv | \section{introduction}
Propagation of optical waves in waveguide arrays has become an important and
effective means to investigate various optical phenomena which have analogues
in many fields of physics \cite{Longhi}. Special attention has been paid to
nonlinear surface waves and nonlinear guided waves in planar... |
3,212,635,537,690 | arxiv | \section{Introduction}
The quark-gluon plasma produced in heavy-ion collisions at RHIC is very opaque to energetic partons as shown by the observed
strong jet quenching \cite{Adler:2003qi,Adler:2002tq} due to multiple scattering and induced parton energy loss \cite{Wang:1991xy}.
The energy and momentum lost by a propa... |
3,212,635,537,691 | arxiv | \section{Introduction}
\label{sec:introduction}
A time-honored possibility to study the low-energy regime of the theory of strong interactions,
Quan\-tum Chromo\-dy\-na\-mics (QCD), is given by Effective Field Theories (EFTs).
In this approach, one investigates QCD-inspired effective models that describe the interac... |
3,212,635,537,692 | arxiv | \section{Introduction}\label{sec:introduction}
\subsection{Dark Patterns}
Dark patterns are user interface designs on online services that make users behave in unintended ways. Dark patterns have been called into question in recent years.
In 2010, Harry \cite{darkpattern.org} defined dark patterns as “tricks used in w... |
3,212,635,537,693 | arxiv | \section{Introduction} \label{sec:intro}
In the recent work~\cite{kh-vwtriang}, we have shown how, after a
separation of variables, the radial mode equations of the vector wave
equation $\square v_\mu = 0$ on the Schwarzschild black hole spacetime
may be significantly simplified by systematically decoupling them into ... |
3,212,635,537,694 | arxiv | \section{Introduction} \label{sec:1}
Personalized decision-making is an emerging artificial intelligence paradigm tailored to an individual's characteristics, with wide real-world applications such as
precision medicine \citep{chakraborty2013statistical},
customized economics \citep{turvey2017optimal},
and personaliz... |
3,212,635,537,695 | arxiv | \section{Introduction and main results}
We are interested in a model of alignment of unit vectors. Our interest comes from the mechanism of alignment of self-propelled particles presented by Degond and Motsch in~\cite{degond2008continuum}, which is a time-continuous model inspired from the Vicsek model~\cite{vicsek199... |
3,212,635,537,696 | arxiv | \section{Introduction}
The GW170817 event~\cite{abbott17a,abbott17b} was arguably one of the most important astrophysical findings of the last decade for several reasons. First, it demonstrated that binary neutron star (BNS) mergers can produce strong gravitational wave (GW) signals and power bright electromagnetic emi... |
3,212,635,537,697 | arxiv | \section{Introduction and Summary}
Symmetry has always been a guiding principle in characterizing physical systems. While weakly coupled field theories are known to be tractable in terms of perturbation theory in coupling, often the strongly coupled ones can only be constrained by symmetry arguments. For example, the ... |
3,212,635,537,698 | arxiv | \section{Introduction}\label{introduction}
Fano manifolds, i.e., smooth complex projective varieties with ample anticanonical class,
play an important role in the classification of complex projective varieties.
In \cite{mori79}, Mori showed that Fano manifolds are uniruled, i.e.,
they contain rational curves through... |
3,212,635,537,699 | arxiv | \section{Introduction}
\object{PSR B0656+14} is one of three nearby pulsars in the middle-age range in
which pulsed high-energy emission has been detected. These are
commonly known as ``The Three Musketeers'' \citep{bt97}, the other two
being Geminga and PSR B1055--52. PSR B0656+14 was included in a recent
extensive s... |
3,212,635,537,700 | arxiv | \section{Introduction}
Direct simulations of star clusters have a long history.
As algorithms and hardware have improved, larger numbers of stars could be simulated, allowing a more realistic representation of the dynamical evolution of globular star clusters.
\nbody \citep{Aarseth2003} is a state-of-the-art dir... |
3,212,635,537,701 | arxiv | \section{Introduction}
The Fr\'echet distance and its variants provide a versatile class of distance measures for parametrized curves as they occur in application areas such as trajectories of moving objects (e.g., vehicles, animals, or robots), outlines of shapes, signatures, gestures, and other types of time series ... |
3,212,635,537,702 | arxiv | \section{Introduction}
In this paper, we aim attention at a family of linear singularly perturbed equations that involve linear fractional
transforms and partial derivatives of the form
\begin{equation}
\mathcal{P}(t,z,\epsilon,\{m_{k,t,\epsilon}\}_{k \in I},\partial_{t},\partial_{z})y(t,z,\epsilon)=0 \label{SPEm_int... |
3,212,635,537,703 | arxiv | \section{Introduction and Summary}
The relevant degrees of freedom in QCD at large distances are still poorly understood.
A perturbative approach in this domain is rendered impossible by the lack of convergence and by the existence of multiple solutions to the gauge fixing condition (Gribov copies) \cite{Gribov:1977w... |
3,212,635,537,704 | arxiv |
\section*{S1. Landauer+DFT calculations}
We model the QPC as a set of three electrostatically coupled strictly two-dimensional systems: the electrodes, the donor layer and the 2DEG. The structure of the simulation closely models the one used in the experiment, with small modifications in simulated charge density to m... |
3,212,635,537,705 | arxiv | \section{Introduction}
The traditional concept of globular clusters (GCs) as simple stellar populations, where all stars share the same age and abundances within some small tolerance, is now a view of the past, as it has become clear that (nearly) all GCs host significant abundance spreads within them. While all GCs ... |
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