arxiv_id stringlengths 0 16 | text stringlengths 10 1.65M |
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2004.01355 | \section{How to learn fair models?} At a high level, the optimization problem that we seek to solve is written as,\begin{align}
\min_{h\in\mathcal{H}} \mathbb{E}_{z:(x,y,s)\sim \mathcal{D}} \mathcal{L}(h;(x,y)) ~~\text{subject to}~~ h \in \mathcal{F}_{d_h}, \label{eq:fairopt}
\end{align}
where $\mathcal{L}$ denotes t... |
1404.7321 | \section{Introduction}
The present contribution focuses on the dynamics of particles and
their accumulation in electro-osmotic flow through micro-channel junctions
which are a basic element of microfluidic systems. This work thus
extends previous studies \cite{takhistov_electrokinetic_2003,thamida_nonlinear_2002,yossi... |
2105.00282 | \section{Introduction}
\label{sec:intro}
Various ML pipeline composition and optimisation methods have been proposed in recent years to find valid and well-performing pipelines given both a problem (i.e., a dataset) and a set of ML components with tunable hyperparameters \cite{sabu18,zohu19,ngma20,kemu20}.
One of th... |
2105.00324 | \section{Introduction}
Deep learning is the prevailing paradigm for machine learning.
Over the course of its meteoric rise, its many differences from human learning have become increasingly clear.
Chief among these are gaps in data efficiency, robustness, generalizability, and energy efficiency --- all unlikely to narr... |
1912.11583 | \section{Introduction} \label{Sec1}
Matrix data have been popularly encountered in various big data applications. For example, many science and social applications consist of individuals with complicated interaction systems. Such system can often be modeled using a network with the nodes representing the $n$ individ... |
1409.0274 | \section{Introduction}
Let $\mathfrak{g}$ be a~f\/inite-dimensional complex simple Lie algebra with highest root $\theta$. The current algebra
$\mathfrak{g}[t]$ associated to $\mathfrak{g}$ is equal to $\mathfrak{g}\otimes \mathbb{C}[t]$, where $\mathbb{C}[t]$ is
the polynomial ring in one variable.
The degree grading... |
1409.0479 | \section{Introduction}
In recent years dynamical systems with delays have evolved as a major topic in nonlinear sciences \cite{bookThomas,E}. Time delays arise naturally, and might play a role in many areas of physics, biology and technology, such as nonlinear optics \cite{RMPIngo,Nix12}, gene regulatory circuits \cite... |
2006.15557 | \section{Introduction}
The Casimir effect was discovered \cite{1} as an attractive force which arises
between two parallel uncharged ideal metal planes in vacuum and depends only
on the Planck constant $\hbar$, speed of light $c$, and interplane distance
$a$. At zero temperature of the planes this effect is entir... |
2006.15435 | \section{Introduction}
Summarization is the task of generating a shorter text that contains the key information from source text, and the task is a good measure for natural language understanding and generation. Broadly, there are two approaches in summarization: extractive and abstractive. Extractive approaches simply... |
1811.10371 | \section{Important theorems and lemmas}
\label{chap:RMT}
In the derivation of large system analysis, we use well-known lemmas including
trace lemma~\cite[Lemma 2.6]{bai1998no},\cite[Theorem 3.4]{RMT} along with rank-1 perturbation lemma~\cite[Lemma 2.6]{silverstein1995empirical},\cite[Theorem 3.9]{RMT}. The former one... |
1412.3674 | \section{Introduction}
In-line holography relates to the original holographic scheme proposed by Gabor \cite{Gabor:1947,Gabor:1948,Gabor:1949}. It is of conceptually simple design, does not include optical elements between sample and detector and has been employed since its invention in numerous experiments using ... |
1412.3596 | \section{Introduction}
With the increasing popularity of GoPro \cite{gopro} and the introduction of Google Glass \cite{glass} the use of head worn egocentric cameras is on the rise. These cameras are typically operated in a hands-free, always-on manner, allowing the wearers to concentrate on their activities. While mo... |
1003.4213 | \section{Introduction}
Recent efforts to produce atomic clocks in the optical domain have proven so successful that they are now surpassing the performance of the best frequency standards in the microwave domain~\cite{Rosenband2008,Boyd2007,Ludlow2008,Schneider2005}.
However, one limitation to further improvements of... |
2012.02854 | \section{Introduction}
Streamflow prediction is one of the key tasks for effective water resource management. A number of physics based models have been developed over the decade to model different aspects of the hydrological cycle using physical equations. A major drawback of these models is that they require extensiv... |
2004.06952 | \section{Introduction}
Complex Hessian equations are important examples of fully non-linear PDE's of second order on complex manifolds. They interpolate between (linear) complex Poisson equations ($m = 1$) and (non linear) complex Monge-Amp\`ere equations $(m=n$).
They appear in many geometric problems, including t... |
1610.02991 | \section{Discussion}
Most social psychology data lie in the bounding box of language, culture, ethnicity, and even environment.
Social media sites like Facebook and Twitter, however, are useful places for behavioral data mining wherein people without the care of language, ethnicity, and boundaries are free to speak th... |
1610.02734 | \section{Introduction}\label{s.Introduction}
\subsection{Main result}
In this paper we study the
existence of non-trivial wandering domains in nonhyperbolic dynamics.
Here a \emph{non-trivial wandering domain} for a given map $f$ on a manifold $M$ means a
non-empty connected open set $D\subset M$ which satisfies t... |
1011.3447 | \section{Introduction}
\subsection{Representations of $\operatorname{Gal}(\overline{\mathbf{Q}}/\mathbf{Q})$}
\label{rpgqgl}
The starting point for this survey is that one can attach representations of the group $\operatorname{Gal}(\overline{\mathbf{Q}}/\mathbf{Q})$ to some objects which occur in arithmetic geometry,... |
1011.3651 | \section{Introduction}
Recent years have witnessed a great deal of interest
in the possible existence of mass dimension
two condensates in gauge theories, see for example
\cite{Gubarev:2000eu,Gubarev:2000nz,Verschelde:2001ia,Dudal:2002pq,Dudal:2003vv,Vercauteren:2007gx,Dudal:2005na,Boucaud:2001st,Furui:2005he,Gubarev:2... |
2203.13088 | \section{Introduction}
\label{sec:intro}
Traditional retrieval systems have long relied on bag-of-words representations to search within unstructured text collections. This has led to mature architectures that are known to support highly-efficient search. The compact inverted indexes enable fast top-$k$ retrieval stra... |
2203.12993 | \section{Introduction}
According to the physical theory, if an incompressible viscous Newtonian fluid occupies the whole space $\mathbb{R}^{n}$ in the absence of external forces, then the velocity $U(\tau,x)$ and kinematic pressure $\varPi(\tau,x)$ of the fluid at time $\tau>0$ and position $x\in\mathbb{R}^{n}$ satisf... |
2206.11691 | \section{Introduction}
\begin{figure}[ht!]
\begin{center}
\subfigure[]{\includegraphics[scale=0.30]{Fig1a_new.eps}}
\subfigure[]{\includegraphics[scale=0.20]{Fig1b.eps}}
\end{center}
\caption{(a) The room temperature x-ray diffraction patterns for bulk and nanoscale samples and their refinement by Ful... |
2212.10996 | \section{Renewal theory}
\label{sec:renewaltheory}
\begin{figure}[tp]
\centering
\includegraphics[width=\linewidth]{fig_1.pdf}
\caption{Schematic of the run-and-tumble motion of a particle with mean run and tumbling times, $\tau_R$ and $\tau_T$, respectively. The particle moves at velocity $v$ during the run phase.
$P... |
2005.11351 | \section{Introduction}
This paper is devoted to show the existence and uniqueness of logarithmic models for any holomorphic foliation on $({\mathbb C}^n,0)$ of generalized hypersurface type. In the case of $n=2$, this result has been obtained by N. Corral in \cite{Cor}. The main result is Theorem \ref{teo:main} in th... |
1410.2206 | \section{Introduction}
An intriguing relation between entanglement entropy and partition functions holds in quantum field theories \cite{Calabrese:2004eu}.
The R{\'e}nyi entropy $S_n$, one parameter generalization of entanglement entropy $S=S_1$, can be written as
\begin{align}\label{REdef}
S_n = \frac{1}{1-n} \log \l... |
1001.4405 | \section{Introduction}
\label{sec:intro}
The basic definition of Virtual Organisation (VO) is simple enough: organisations and individuals who bind themselves dynamically to one another
in order to share resources within temporary alliances~\cite{FosterKessel01}.
Several issues arise at various levels of abstraction w... |
1001.4679 | \section{Introduction}
\label{introduction}
The idea of Kaluza and Klein~\cite{kk} of obtaining the electromagnetism
- and under the influence of their idea nowadays also the weak and colour
fields~\cite{geogla,chofre,zee,salstr,mec,dufnilspop,daess,wet} -
from purely gravitational degrees of freedom connected ... |
1001.4458 | \section{Transverse gravity and scale invariance}
The hope that scale invariance could shed some light on the fact that the observed value of the cosmological constant scale is much lower than expected from the wilsonian viewpoint is certainly an old and cherished one. Let us mention just a couple of recent works \c... |
1001.3921 | \section{Introduction}
Recently, quantum gravity at a Lifshitz point, which is
power-counting renormalizable and hence potentially UV complete, was
proposed by Ho\v{r}ava~\cite{ho1,ho2,ho3}. This theory for quantum
gravity is not intended to be a unified theory like string theory.
A hot issue of the Ho\v{r}ava-Lifshi... |
1001.4522 | \section{Introduction}
The author was pleased and honored to have a part in a symposium honoring Eyring that was part of an American Chemical Society Meeting in Salt Lake City in March, 2009. This article is based on the author's talk in this symposium. A portion of this article together with two additional figures ... |
2110.08014 | \section{Introduction}
Between April and September 2017, after spending 13 years exploring the Kronian system, the Cassini spacecraft performed 23 proximal orbits passing within Saturn's D ring, allowing us to directly probe the upper atmosphere of a gas giant planet. This ``Grand Finale'' phase of the mission culmina... |
0801.2921 | \section{SUPPLEMENTARY INFORMATION}
\subsection{Nomenclature}
ARPES: angular resolved photoemission spectroscopy,
Bi-2212: Bi$_2$Sr$_2$CaCu$_2$O$_{8+\delta}$,
Bi(Y)-2212: Y-doped Bi-2212,
DoS: density of states,
$\Delta$: energy gap,
$\Delta T$: self-heating,
$\Gamma$: depairing factor, reciprocal quasiparticle... |
0801.2134 | \section{Introduction}
The proper theory of the motion of a spinning mass in a gravitational field is due to Mathisson~\cite{1}, Papapetrou~\cite{2}, and Dixon~\cite{3}. A main aspect of this theory, which already appears in the work of Mathisson~\cite{1}, is the existence of a spin-curvature force
\begin{equation}\la... |
0801.3314 | \section{Introduction}
Local times for semimartingales have been widely studied. See for example the monograph \cite{RY} and the references therein.
On the other hand, local times of Gaussian processes have also been the object of a rich probabilistic literature; see for
example the recent paper \cite{MR} by Marcus an... |
1306.4386 | \section{Introduction}
The arithmetic properties of Fourier coefficients of modular forms are involved in many areas of number theory, and they
have formed the topic of a vast amount of research. A prototypical modular form is the Dedekind eta function
\[\eta(z): = q^{1/24} \prod_{n=1}^{\infty} (1-q^n),\qquad q:=e^{... |
1602.05750 | \section{Introduction}
\noindent
Differentiable extensions of functions were considered already in
the
1920's.
In \cite{J}, V.~Jarn\'ik proved that every real-valued differentiable function defined on a~perfect subset of~$\R$
can be extended to an everywhere differentiable function on~$\R$
(he even proved a~stronger fo... |
1705.09272 | \section{Introduction}
Recently, Bose-Einstein condensates (BEC) with dipole-dipole interactions (DDI) have received considerable attention both experimentally and theoretically
\cite{Baranov, Pfau,Carr, Pupillo2012}.
Dipolar quantum gases, in stark contrast to dilute gases of isotropic interparticle interactions, o... |
1801.07011 | \section{Introduction}
\label{sec:introduction}
In case of events concerning several communities, event-centric information available in different languages can reflect community-specific bias \cite{Rogers:2013}.
As events unfold, it therefore becomes particularly important to analyze language-specific differences a... |
2107.01948 | \section{Introduction}
The dynamic mode decomposition (DMD) algorithm, is a powerful and versatile data-driven approach proposed by \cite{Schmid2010}, ideally suited to analyze complex high-dimensional geophysical flows in terms of recurrent or quasi-periodic modes. The DMD is indeed related to the Koopman theory \cite... |
2107.02050 | \section{Some examples and best-practices}
\end{document}
\section{Acknowledgement \label{sec:acknowledgement}}
We thank Jade Powell for pointing us the supernova repository.
The authors gratefully acknowledge the support of the NSF for the provision of computational resources. Th... |
2107.01950 | \section{Introduction}
Yu. Manin~\cite[\S 14]{Manin} introduced the notion of $R$-equivalence for points of algebraic varieties over a field.
This notion has been used extensively in the study of reductive algebraic groups, e.g.~\cite{CTS1,CTS2,Gi2,ACP}.
In the present paper, we propose
a generalized definition of $R... |
gr-qc/9611030 | \section{Introduction}
The recent progress in non-perturbative quantum gravity using
Ashtekar's formulation of general relativity is due, in part, to
the application to gravity of techniques used for studying
Yang-Mills theory non-perturbatively \cite{Ash}. The constraints
of Euclidean or Lorenzian general relativity ... |
cond-mat/9611158 | \section{Introduction}
\footnotetext{Dedicated to Prof.~W.~G\"otze on the occasion of his
60th birthday.} As is well known, superconductivity only exists
at sufficiently low temperatures $T$ and small external magnetic
fields $H$. The resulting $H-T$ boundary for the normal to superconducting transition is
determined b... |
1712.07080 | \section{Introduction}
Prototype quantum processors based on superconducting qubits \cite{blais_quantum-information_2007,devoret_superconducting_2013}, and in particular transmon-related qubits, have become a leading platform for experimentally testing ideas in quantum information processing. The creation of a 10-qubi... |
1712.01151 | \section{Introduction}
The Interstellar Boundary Explorer (IBEX) has been continually observing the interaction
of the heliosphere with the surrounding interstellar medium since 2009 January \citep{mcc09}. The scientific payload
consists of two energetic neutral atom (ENA) imagers, IBEX-Lo \citep{fus09} and IBEX-Hi \c... |
1712.01277 | \section{Introduction}
\input{./Introduction.tex}
\section{Materials and Methods}
One FHD patient and one healthy subject (HS) were involved in this pilot study.
The EEG was recorded from one monopolar EEG channel placed on C3, the standard location of the International 10-20 System over the left hemisphere correspo... |
1912.08713 | \section{Introduction}
Quanto CDS is a flavor of a credit default swap. It has a special feature that in case of default
all payments including the swap premium and/or the cashflows are done not in a currency of the reference asset, but in another one.
As mentioned in \cite{Brigo}, a typical example would be a CDS t... |
1406.4248 | \section{Introduction}
The aim of this article is to study two-player zero-sum general
repeated games with signals (sometimes called ``stochastic
games with partial observation''). At each stage, each player chooses
some action in a finite set. This generates a stage reward then a new
state and new signals are r... |
2002.11946 | \section{Proof of the main theorem}\label{app:average-hardness}
In this section, we provide a detailed proof of the main theorem of the main text, which reads:
\bigskip
\begin{m_thm}\label{thm:main}
Assuming conjecture 1 and 2, the ability to classically sample from $p_M(\mathbf z)$ up to an additive error $\beta=1/(8... |
math/9805127 | \section{#2}\label{S:#1}%
\ifShowLabels \TeXref{{S:#1}} \fi}
\newcommand{\ssec}[2]{\subsection{#2}\label{SS:#1}%
\ifShowLabels \TeXref{{SS:#1}} \fi}
\newcommand{\refs}[1]{Section ~\ref{S:#1}}
\newcommand{\refss}[1]{Subsection ~\ref{SS:#1}}
\newcommand{\reft}[1]{Theorem ~\ref{T:#1}}
\newcommand{\refl}[1... |
2011.13936 | \section{Introduction}
\label{sec:Introduction}
Vacuum decay may be the cause of both the beginning and end of our universe. It is also one of the very few systems in which the quantum aspects of gravity are crucial in order to have a proper description of the physical process. Euclidean methods, developed mostly... |
1905.00048 | \section*{Abstract}
We derive the properties and demonstrate the desirability of a model-based method for estimating the spatially-varying effects of covariates on the quantile function. By modeling the quantile function as a combination of I-spline basis functions and Pareto tail distributions, we allow for flexible p... |
2205.07322 | \section{introduction}\label{intro}
\noindent
The interplay between the hook lengths of a partition $\lambda$ and the contents of its cells appears in Stanley's formula for the dimension of the irreducible polynomial representation of the general linear group, $GL(n, \mathbb C)$, indexed by $\lambda$ \cite[(7.106)... |
2207.01200 | \section{Introduction}
\IEEEPARstart{H}{umans} have shown great enthusiasm for Mars. The history of human research on Mars can date back to the 1960s. So far, more than 30 rovers have been dispatched to the red planet, and the increasing amount of available data promotes the application and development of deep learning... |
1407.6854 | \section*{Metastability implies no criticality}
\subsection*{Time scales and length scales}
A metastable state lifetime, $\tau_\mathrm{MS}$, is a property of an irreversible system. Unlike equilibrium properties, $\tau_\mathrm{MS}$ can depend upon system size and preparation protocols. For example, upon ordinary coo... |
1407.6449 | \section{Introduction}
In the paper, we consider the Cauchy problem on
the following linear symmetric hyperbolic system with relaxation (cf.~\cite{Da}):
\begin{gather}
u_t + A_m u_{x} + L_m u = 0 \label{sys1}
\end{gather}
with
\begin{equation}\label{ID}
u|_{t=0}=u_0.
\end{equation}
Here
$u=u(t,x) = (u_1, \cdots, ... |
2003.06470 | \section{Introduction}
In this paper we present the framework to construct ${\mathbb Z}_2\times {\mathbb Z}_2$-graded mechanics as a one-dimensional classical theory. We extend to the ${\mathbb Z}_2\times {\mathbb Z}_2$-graded setting the results and approach employed for ordinary worldline supersymmetric \textcolor{b... |
cond-mat/9706088 | \section{Introduction}
Bose-Einstein condensation is central to much of our
understanding of phenomena in condensed matter physics \cite{Huang}. It is
one of the simplest processes where quantum effects manifest themselves on
the macroscopic level when a finite fraction of the non-interacting bosons
in a system sta... |
hep-ph/9706312 | \section{Introduction}
Early in the next decade two heavy-ion accelerators, the
Relativistic Heavy Ion Collider (RHIC) and the Large Hadron
Collider (LHC), will create highly excited regions, similar
to heavy-ion in size and with temperatures exceeding $200
MeV $. Among the most interesting speculations regarding ... |
1212.3028 | \section{Introduction}\label{sec:1}
In two dimensional quantum field theory, two elegant theorems are known.
Zamolodchikov showed~\cite{Zamolodchikov:1986gt} that there exists a function $c(r)$ of a length scale $r$ which monotonically decreases
as $r$ is increased, and becomes constant only on conformal fixed points.... |
1212.3179 | \section{Introduction}
The Hosoya polynomial of a graph was introduced in the Hosoya's seminal
paper~\cite{hosoya-1988} back in 1988 and received a lot of attention afterwards.
The polynomial was later independently introduced and considered by
Sagan, Yeh, and Zhang~\cite{sagan-1996} under the name {\em Wiener polyn... |
1212.3238 | \section{Introduction}
\label{intr}
The LMG model was introduced in nuclear physics to mimic the behavior of closed shell nuclei \cite{LMG}. It is a simple model with one quantum degree of freedom. The dimension of the Hamiltonian matrix increase linearly with the size of the systems allowing its exact diagonalization... |
2107.13038 | \section{Introduction}
An over-arching goal of cosmology is the reconstruction of how the minuscule cosmic microwave background (CMB) anisotropies grow to the intricate cosmic web that we observe from galaxy surveys. The key challenge in this process is the deeper understanding of the elusive dark energy component in ... |
gr-qc/9304016 | \section{Introduction}
Since the famous work of von Neumann [1], the statistical operator
$\rho$ has been used to represent
the general quantum state of a given
quantum system. The statistical interpretation of $\rho$ is
given in frames of the quantum measurement theory.
For the recent years, serious efforts have bee... |
hep-ph/9304239 | \section{#1}}
\def\firstsubsec#1{\obsolete\firstsubsec \subsection{#1}}
\def\thispage#1{\obsolete\thispage \global\pagenumber=#1\frontpagefalse}
\def\thischapter#1{\obsolete\thischapter \global\chapternumber=#1}
\def\nextequation#1{\obsolete\nextequation \global\equanumber=#1
\ifnum\the\equanumber>0 \global\advance\... |
1707.02962 | \section{Introduction}
The formulation of a string theory for hadrons has been an attractive proposal induced by the phenomenological success in explaining Venziano formula~\cite{Veneziano:1968yb} and even before the formulation of quantum chromodynamics (QCD). Despite the difficulties encountered in the quantizatio... |
2204.13048 | \section{Introduction}
The goal of computational protein design is to identify a protein sequence that has a specified structure and, thereby, function \cite{Frappier2021}. Protein design has been used to design enzymes that catalyze important organic reactions \citep{Siegel2010} and to identify miniproteins that bind... |
2003.09851 | \section{Introduction}
A very large orbital angular momentum (OAM) can be generated in peripheral heavy ion collisions
in the direction perpendicular to the reaction plane. Such a large OAM in the system
can be converted into the spin polarization of hadrons along the direction of the OAM through
spin-orbit couplings \... |
1906.08877 | \section{Introduction}
In previous decades, several correlations between the mass of supermassive black holes (SMBH) and the properties of their host spheroids (spheroidal mass, luminosity, stellar velocity dispersion) point towards the co-evolution between SMBHs and host galaxies \citep[see][and references therein]{1... |
1906.09048 | \section{Introduction}
Reaction-diffusion systems are universally invoked as a reference modeling tool, owing to their inherent ability to sustain the spontaneous generation of -- spatially extended -- patterned motifs. The theory of pattern formation was laid down by A. Turing~\cite{Turing52} and later on fertilized ... |
1906.09181 | \section{Results}
We present the results of our evaluation using the two discussed approaches. For each dataset collected during the two data collection sessions, we used the first 80\% of the ECG trace across 49 subjects as the training data and the remaining 20\% of the signal as the test data. Thus, we obtained two ... |
2002.01956 | \section{Introduction}
Galaxy clusters emerged from the largest overdensities in the primordial universe. Their evolution is sensitive to both the growth rate of structure and the expansion history of the universe. For this reason, they are a useful probe to test cosmological theories. The observed size, mass, and abun... |
0903.0533 | \section{Introduction}
The motion of a general barotropic compressible fluid is described by the following system:
\begin{equation}
\begin{cases}
\begin{aligned}
&\partial_{t}\rho+{\rm div}(\rho u)=0,\\
&\partial_{t}(\rho u)+{\rm div}(\rho u\otimes u)-{\rm div}(\mu(\rho)D(u))-\nabla(\lambda(\rho){\rm div} u)+\nabla P(\... |
0903.0815 | \section{Introduction}
For almost 50 years since Casimir's discovery [1], theory existed
independent of rare experiments [2,3]. A lot of theoretical work has been
done during this period. However, the relationship to reality of some
theoretical
models, such as an ideal metal spherical shell, an ideal metal
rectangular... |
0903.1220 | \section{Introduction}
In the standard model (SM), the purely leptonic $B$ meson decays
\ensuremath{\Bp \to \ellp \nul}\xspace~\cite{charge}
proceed at lowest order through the annihilation diagram
shown in Fig.~\ref{fig:diagram}.
The SM branching fraction can be calculated as~\cite{Silverman:1988gc}
\begin{equa... |
2003.04699 | \section{Introduction}
In order for autonomous vehicles to travel safely at higher speeds or operate in wide-open spaces where there is a dearth of distinct features, a new level of robust sensing is required.
\gls{fmcw} radar satisfies these requirements, thriving in all environmental conditions (rain, snow, dust, fo... |
2003.04597 | \section{Introduction}
Let $(M,g)$ be a smooth, compact, Riemannian manifold of dimension $n$ and consider normalized Laplace eigenfunctions: solutions to
$$
(-\Delta_g-\lambda^2)\phi_\lambda=0,\qquad \|\phi_\lambda\|_{L^2(M)}=1.
$$
This article studies the growth of $L^p$ norms of the eigenfunctions, $\phi_\lambda$, ... |
1911.12811 | \section*{Abstract}
{\bf
We give a detailed description of the nested algebraic Bethe ansatz. We consider integrable models
with a $\mathfrak{gl}_3$-invariant $R$-matrix as
the basic example, however, we also describe possible generalizations.
We give recursions and explicit formulas for the Bethe vectors. We also give... |
1911.12950 | \section{Introduction}
\hspace*{1em}
As a special case of image object segmentation, object co-segmentation refers to the task of jointly discovering and segmenting the objects shared in a group of images.
It has been widely used to support various computer vision applications, such as interactive image segmentation~\c... |
1411.4143 | \section{Introduction}
QCD at finite baryon density and low temperatures is one of the
least understood regions of the QCD phase diagram. The reason is that
the baryon chemical potential introduces a sign problem which invalidates standard stochastic methods to
evaluate the path integral for the QCD
partition functi... |
2109.02290 | \section{Introduction}
Logistics systems are becoming increasingly complex and interrelated, from the operational level to the strategic level, due to economic globalization, offshoring of production, increasing product complexity, and fast-changing trends, among others. \citep{Harland2003-ez, Dolgui2020-yf, Choi2001-p... |
1911.03407 | \section{Credits}
\section{Introduction}
Question Generation (QG) from text has gained significant popularity in recent years in both academia and industry, owing to its wide applicability in a range of scenarios including conversational agents, automating reading comprehension assessment, and improving question answ... |
1905.03110 | \section{Introduction}
Gaussian mixture models provide accurate estimates of free energy landscapes~\cite{westerlund_inference_2018}. Determining metastable core states within a protein's free energy landscape is key to obtaining important biological insights. However, extracting such states from molecular dynamics (MD... |
1905.02967 | \section{}
\unskip
\subsection{}
The appendix is an optional section that can contain details and data supplemental to the main text. For example, explanations of experimental details that would disrupt the flow of the main text, but nonetheless remain crucial to understanding and reproducing the research shown; figure... |
2012.03956 | \section{Introduction}\label{sec:intro}
Since their first observations over 100 years ago~\cite{Hess:1912srp} much has been learned in the study of
cosmic rays. Modern experiments (both direct and air-shower observations) provide invaluable information about the composition and energy spectra
of cosmic rays over a hu... |
2012.04021 | \section{Introduction}
Two-dimensional nanostructured materials are promising cost-efficiency solutions for developing novel flat optoelectronic applications \cite{sun2016optical,gupta2015recent,zhang2016van,yu2020two}. Their controllable size allows for electronic wave function confinement, which is desirable for des... |
1706.01341 | \chapter{Hardware}
\label{app:hardware}
This appendix gives an overview of the processors used throughout this work and
their relevant properties.
Note that, while the single-threaded peak performance is, where appropriate,
based on the processors' maximum turbo frequency, the multi-threaded peak
performance is inste... |
1412.0576 | \section{Introduction}
We study a 2D problem of diffraction by a segment bearing im\-pe\-dan\-ce boundary conditions
on both sides. This problem can be considered as a cross-section of a 3D problem of diffraction by an infinitely long strip with finite width and zero thickness.
The governing equation is the Helmhotz o... |
2205.06194 | \section{Introduction}
Quantum electrodynamics (QED) can be regarded as the oldest and possibly most accurate and successful quantum field theory (QFT) there is. The renormalisation of QED,
by the pioneers Dyson, Feynman, Schwinger, Tomonaga and others \cite{Schweber:1994qa}, gave birth
to the successful applicat... |
1711.08180 | \section{Introduction}
Semantic segmentation assigns all pixels in an image to semantic classes; it gives finely-detailed pixel-level information to visual data and can build a valuable module for higher-level applications such as image answering, event detection, and autonomous driving. Conventional semantic segmenta... |
1711.08225 | \section{Introduction}
\label{sec:1}
Research on pedestrian dynamics has systematically analysed the influence of group behaviour only in the last years (see, e.g.,~\cite{TheraulazGroup,DBLP:journals/prl/BandiniGV14,VonKruchten2017}): although observations and experiments agree on some aggregated and microscopic effect... |
1711.08394 | \section{Introduction}
The advent of high-precision space-based broadband optical photometry with satellites (or ensembles of satellites) such as the \textit{Microvariability and Oscillations of STars} (MOST; \citealt{2003PASP..115.1023W}) and \textit{BRIght Target Explorer} (BRITE; \citealt{2014PASP..126..573W}) miss... |
1602.02794 | \section*{~}
As one of the three clock-synchronization algorithms studied for wireless sensor
networks (WSNs) under unknown delay \cite{leng10}, Leng and Wu proposed the
generalization of the maximum-likelihood-like estimator (MLLE) proposed by Noh
\textit{et al}. \cite{noh07:_novel}. To overcome the drawback of th... |
2108.01515 | \section{INTRODUCTION}
Characterizing the mechanical properties of materials has many applications in industrial testing and bioengineering. These can be inferred by tracking the deformation of a specimen under known loads. Optical coherence tomography (OCT) is a powerful modality for the role of displacement tracking,... |
1806.09006 | \section{Introduction}
\label{sec:into}
The axial, scalar and tensor charges of the nucleon are needed to
interpret the results of many experiments and probe new physics. In
this paper, we extend the calculations presented in
Refs.~\cite{Bhattacharya:2015wna,Bhattacharya:2015esa,Bhattacharya:2016zcn}
by analyzing elev... |
1910.12941 | \section{Credits}
This document has been adapted from the instructions
for earlier ACL and NAACL proceedings,
including
those for
NAACL 2019 by Stephanie Lukin and Alla Roskovskaya,
ACL 2018 by Shay Cohen, Kevin Gimpel, and Wei Lu,
NAACL 2018 by Margaret Michell and Stephanie Lukin,
2017/2018 (NA)ACL bibtex sugges... |
0903.1462 | \section{Introduction}
Recently, there has been considerable interest in studying correlations between separated systems in `no signaling' theories, which include subquantum (e.g., classical), quantum, and superquantum theories. The primary foundational aim is to characterize quantum mechanics, i.e., to identify physi... |
0903.2272 | \section{Introduction}
\label{sec:intro} \vspace{0.0cm} \PARstart{D}{igital} cameras use
image-processing tools, e.g., interpolation techniques, such as
those used in analog camcorders, in order to achieve good quality
images. One big difference between digital cameras and analog
camcorders is that digital cameras stor... |
0903.2606 | \section{Introduction}
The characterization of variability timescales can provide information on the sizes
and locations of the emission regions in active galactic nuclei. Although Doppler
boosted emission from a relativistic jet provides a very reasonable explanation
for the non-thermal spectra and small-scale rad... |
0903.2223 | \section{Introduction}
A component of particle motion in magnetized plasmas is the stochastic
electric drift produced by the electric field of the turbulence and by the
confining magnetic field. This drift determines a trapping effect or eddy
motion in turbulence with slow time variation \cite{kraichnan}. Typical
part... |
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