meta stringlengths 97 612 | red_pajama_subset stringclasses 4
values | prompt stringlengths 1 200 | answer stringlengths 0 518k |
|---|---|---|---|
{'timestamp': '2021-01-08T02:12:33', 'yymm': '2005', 'arxiv_id': '2005.14484', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14484'} | arxiv | \section{Introduction}
In this work we bring forward the study of the normalized Laplacian that has been established for \textsl{chemical hypergraphs}: hypergraphs with the additional structure that e | ach vertex in a hyperedge is either an input, an output or both (in which case we say that it is a catalyst for that hyperedge). Chemical hypergraphs have been introduced in \cite{Hypergraphs} with the idea of modelling chemical reaction networks and related ones, such as metabolic networks. In this model, each vertex ... |
{'timestamp': '2020-06-01T02:09:11', 'yymm': '2005', 'arxiv_id': '2005.14463', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14463'} | arxiv | \section{Grids}
\begin{table}[ht]
\centering
\begin{tabular}[t]{cccccc}
\hline
\hline
$E_{\text{trans}}$ [eV]&$v$&$j$&$E_{\text{trans}}'$ [eV]&$v'$&$j'$\\
\hline
0.0&0&0&0.1&0&0\\
0.2&2&15&0.3&2&20\\ |
0.4&4&30&0.5&4&40\\
0.6&6&45&1.0&6&60\\
1.0&9&60&1.5&9&80\\
1.5&12&90&2.0&12&100\\
2.0&15&120&2.5&15&125\\
2.5&18&150&3.0&18&150\\
3.0&21&180&3.5&21&175\\
3.5&24&210&4.5&24&200\\
4.5&27&240&5.5&27&220\\
5.5&30&-&6.5&30&240\\
6.5&33&-&7.5&33&-\\
7.5&36&-&8.5&36&-\\
8.5&-&-&9.5&42&-\\
9.5&-&-&10.5&47&-\\
10.5&-&-&-&-&-\... |
{'timestamp': '2021-03-29T02:17:49', 'yymm': '2005', 'arxiv_id': '2005.14471', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14471'} | arxiv | \section{Introduction}
\label{sec:Introduction}
Diffractive hadron interactions at high scattering energies are characterised by final states consisting of two systems well separated in rapidity, whi | ch carry the quantum numbers of the initial state hadrons. Most diffractive phenomena are governed by \text{soft}, large distance processes. Despite being dominated by the strong interaction, they remain largely inaccessible to the description by Quantum Chromodynamics (QCD) in terms of quark and gluon interactions. In... |
{'timestamp': '2020-06-01T02:06:38', 'yymm': '2005', 'arxiv_id': '2005.14388', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14388'} | arxiv | \section{Conclusions}
\bibliographystyle{IEEEtran}
\subsection{Dynamic program to compute $\mathbf F(\cdot)$}
\label{app:F_compute}
We here describe how to compute $\mathbf F(p,v)$ in $O(mn)$ time | and space complexity, where $p=(p_1,...,p_n)$ and $v=v_1...v_m$, via a dynamic programming approach.
We first define
\begin{align*}
&\mathbf G^{for}(k,j)\triangleq \mathbf F(p_{[1:k]},v_{[1:j]}).
\numberthis
\label{eq:G}
\end{align*}
Using Lemma~\ref{lemma:F_decomposition} with $i=n$, we get
\begin{align*}
\m... |
{'timestamp': '2020-06-01T02:09:46', 'yymm': '2005', 'arxiv_id': '2005.14480', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14480'} | arxiv | \section{Introduction}
Computer-aided thoracic disease diagnosis based on chest X-ray has been
significantly advanced by deep convolutional neural networks (DCNNs) in recent
years~\cite{wang2017chestx | ,tang2018attention,sedai2018deep,wang2018chestnet}.
Most of these approaches are formulated as a multi-task binary classification
problem, where a CNN is trained to predict the risk probabilities of different
thoracic diseases. In clinical practices, visual localization of the
lesions on chest X-ray, such as heatmaps ... |
{'timestamp': '2020-06-25T02:04:28', 'yymm': '2005', 'arxiv_id': '2005.14278', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14278'} | arxiv | \section{Introduction}
The space of diffeomorphisms splits into two classes:
those with zero entropy and those with positive entropy (by which we always mean topological entropy). The former contains | Morse-Smale diffeomorphisms: their nonwandering set is formed by finitely many periodic points.
The latter contains the systems exhibiting a transverse homoclinic orbit, \emph{i.e.} an orbit which accumulates on the past and on the future
on a same periodic orbit and which persists under small perturbations: the nonwa... |
{'timestamp': '2020-09-01T02:16:22', 'yymm': '2005', 'arxiv_id': '2005.14418', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14418'} | arxiv | \section{Introduction}
\label{sec:introduction}
Collective excitations are simple and informative probes of various physical properties in solids. Among them, excitations related to the interaction | of light and matter are, perhaps, among the most numerous. In particular, polaritons are quasiparticles related to the coupling of electromagnetic waves with any resonance in material. The paradigmatic example of polaritons is realized by coupled states of electromagnetic waves with phonons in ionic crystals~\cite{Tolp... |
{'timestamp': '2020-06-01T02:05:22', 'yymm': '2005', 'arxiv_id': '2005.14365', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14365'} | arxiv | \section{Introduction}
\label{S:intro}
In this paper we consider the problem of estimating the number of isomorphism
classes of principally polarized abelian varieties $(A,\lambda)$ such that $A$
lie | s in a given isogeny class of simple ordinary abelian varieties over a finite
field. We approach this problem by subdividing isogeny classes into their
\emph{strata}, which are the subsets of an isogeny class consisting of abelian
varieties sharing the same endomorphism ring. (To avoid awkward locutions,
we will say ... |
{'timestamp': '2020-09-15T02:19:26', 'yymm': '2005', 'arxiv_id': '2005.14274', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14274'} | arxiv | \section{Introduction}
The uncertainty principle states that a non-zero function and its Fourier transform cannot be simultaneously sharply localized. There are various ways of measuring localizatio | n of a function and depending on it one can formulate different forms of the uncertainty principle. Uncertainty principles can be subdivided into quantitative and qualitative uncertainty principles. Quantitative uncertainty principles are some special inequalities which give us information about how a function and its ... |
{'timestamp': '2020-06-01T02:06:36', 'yymm': '2005', 'arxiv_id': '2005.14386', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14386'} | arxiv | \section{Introduction}
Most existing captioning models learn an autoregressive model, either
LSTM or transformer, in which explicit control of generation process
is difficult. In particular, the leng | th of the caption is determined
only after the End Of Sentence ($<$eos$>$) is generated. It is hard to
know and control the length beforehand. However, length can be an
important property of a caption. A model that allows control of output
length would provide more options for the end users of the captioning
model. By ... |
{'timestamp': '2020-06-01T02:04:28', 'yymm': '2005', 'arxiv_id': '2005.14339', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14339'} | arxiv | \section{Introduction}
\label{intro}
A \textit{degenerate parabolic equation} \cite[Chapter III]{showalter} (also called \textit{parabolic-elliptic equation} \cite{pluschke})
is an abstract evolution |
equation of the form
\begin{equation}\label{deg-1}
\dfrac{d}{dt}(Ru(t))+ A(t)u(t)=f(t),
\end{equation}
where $R$ is a linear, bounded and monotone operator
and $(A(t))_{t\in[0,T]}$ is a family of linear and bounded operators.
They arise in several applications, for instance
in the study of eddy currents in electro... |
{'timestamp': '2021-06-04T02:04:45', 'yymm': '2005', 'arxiv_id': '2005.14356', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14356'} | arxiv | \section{Introduction \label{sec:intro}}
Centrality measures are prescriptions for assigning importance values to nodes in complex networks, and the power of the concept stems from the flexibility | of characterizing importance in different ways. As such, centralities can be applied everywhere from Internet search results (Google's PageRank \cite{page1999pagerank}) to identifying important structures in neuron networks \cite{joyce2010new}. Centrality is one of the most basic and widely studied concepts in network ... |
{'timestamp': '2022-02-23T02:15:21', 'yymm': '2005', 'arxiv_id': '2005.14373', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14373'} | arxiv |
\subsection{IR-Based Code Search}\label{back_ir}
Traditional code search models (e.g., CodeHow \cite{lv2015codehow}) mainly depend on IR techniques. Generally, the IR-based model builds an index for | terms (i.e., each word token) in code methods, so that the keywords generated from search query can match the expected code methods quickly by checking the index. Afterward, the model recommends the top-n relevant code methods according to a designed keywords-terms matching degree. During the indexing, the method name... |
{'timestamp': '2020-06-01T02:10:19', 'yymm': '2005', 'arxiv_id': '2005.14499', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14499'} | arxiv | \section{Introduction}\label{sec:intro}
A vast number of todays technological advancements is due to the ever advancing improvement in modeling and solving of partial differential equation (PDE) probl | ems. One class of especially challenging problems is PDE-constrained optimization which has a broad number of applications, reaching from engineering design and control problems to medical applications like cancer treatment \cite{schenk2009,biegler2003large,fisher2009data}.
We consider a typical PDE-constrained optimi... |
{'timestamp': '2021-05-06T02:13:27', 'yymm': '2005', 'arxiv_id': '2005.14445', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14445'} | arxiv | \section{Introduction}
In \cite{Hit.1}, Nigel Hitchin describes, for a Riemann surface $S$, a connected component of the character variety
$$\Rep(\pi_1(S), \PSL_n(\R)) = \Hom(\pi_1(S), \PSL_n(\R | ))/\PSL_n(\R)$$
which he parametrizes by holomorphic differentials. These components are called \textbf{Hitchin components} and their study \emph{higher Teichmüller theory}.
His approach uses Higgs bundle theory, more precisely the hyperkähler structure of the moduli space of polystable Higgs bundles. These componen... |
{'timestamp': '2020-09-21T02:09:49', 'yymm': '2005', 'arxiv_id': '2005.14483', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14483'} | arxiv | \section{Introduction}
The solar atmosphere is full of energetic particles. They are produced when ambient plasma particles are accelerated out of thermal equilibrium by a strong electric field or by | rebounding off moving magnetic elements. Upon leaving the site of acceleration, their available trajectories are limited by the Lorentz force, which compels charged particles to follow the direction of the magnetic field. Consequently, the accelerated particles form coherent beams. The interactions of these beams with ... |
{'timestamp': '2020-06-01T02:09:36', 'yymm': '2005', 'arxiv_id': '2005.14473', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14473'} | arxiv | \section*{\large\refname}
\small\@mkboth{\MakeUppercase\refname}{\MakeUppercase\refname}
\list{\@biblabel{\@arabic\c@enumiv}}
{\settowidth\labelwidth{\@biblabel{#1}}
| \leftmargin\labelwidth
\advance\leftmargin\labelsep
\@openbib@code
\usecounter{enumiv}%
\let\p@enumiv\@empty
\renewcommand\theenumiv{\@arabic\c@enumiv}}
\sloppy
\clubpenalty4000
\@clubpenalty \clubpenalty
\widowpenalty4000%
\sfco... |
{'timestamp': '2021-01-22T02:13:02', 'yymm': '2005', 'arxiv_id': '2005.14503', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14503'} | arxiv | \section{Introduction}
We consider parabolic control systems on $L_p(\R^d)$, $p\in [1,\infty)$, of the form
\begin{equation}
\label{eq:system-intro}
\dot{x}(t) = -A_p x(t) + \1_\thickset u(t | ),\quad t\in (0,T],\quad x(0) = x_0\in L_p(\R^d),
\end{equation}
where $-A_p$ is a strongly elliptic differential operator of order $m \in \N$ with constant coefficients, $\1_\thickset \from L_p (\thickset)\to L_p(\R^d)$ is the embedding from a measurable set $\thickset \subset \R^d$ to $\R^d$, $T>0$, and where $u \... |
{'timestamp': '2020-09-01T02:36:50', 'yymm': '2005', 'arxiv_id': '2005.14426', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14426'} | arxiv | \section{Introduction}
We study learning the best possible single neuron that captures the relationship between the input $x\in \mathbb{R}^d$ and the output label $y\in \mathbb{R}$ as measured by the | expected square loss over some unknown but fixed distribution $(x,y)\sim \mathcal{D}$. In particular, for a given activation function $\sigma:\mathbb{R}\to \mathbb{R}$, we define the population risk $F(w)$ associated with a set of weights $w$ as
\begin{equation} F(w) := (1/2) \mathbb{E}_{(x,y) \sim \mathcal{D}} \l[ \l... |
{'timestamp': '2020-06-01T02:09:08', 'yymm': '2005', 'arxiv_id': '2005.14460', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14460'} | arxiv | \section{Introduction}
Volterra processes appear naturally in models with non-local features.
In this article, we will investigate the analytic and probabilistic properties of Volterra processes cons | tructed as pathwise integrals of a kernel $K$ against a Gaussian process $W$. For generality, we will assume that the Gaussian process $W$ takes values in a Hilbert space $H$ with a covariance operator $Q_W$, and that the kernel $(t,s)\mapsto K(t,s)$ for $t>s$ is a linear operator on the same Hilbert space. In parti... |
{'timestamp': '2020-06-01T02:11:28', 'yymm': '2005', 'arxiv_id': '2005.14541', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14541'} | arxiv | \section{Introduction}
One way to arrive at the Bogoliubov axioms of perturbative quantum field theory (pQFT) is by
analogy with non-relativistic quantum mechanics \cite{Gl}, \cite{H}; a discussion o | n this point can also be found in \cite{third order}.
We give the main ideas. Suppose that we have a time-dependent interaction potential
$V$. Then one goes to the interaction picture and the time evolution is governed by the evolution equation:
\begin{equation}
{d \over dt}U(t,s) = - i V_{\rm int}(t) U(t,s); \qquad U(... |
{'timestamp': '2020-06-01T02:10:19', 'yymm': '2005', 'arxiv_id': '2005.14500', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14500'} | arxiv | \section{Supplemental Materials for ``Topological second-order spin-$\frac{3}{2}$ liquids with hinge Fermi arcs"}
\section{Symmetric and traceless quadratic forms}
The five independent symmetric | and traceless $3\times 3$ quadratic forms are explicitly given by
\begin{equation}
Q^1=\frac{1}{\sqrt{3}}\begin{pmatrix}
0 & 0 & 0\\
0 & 0 & 1\\
0 & 1 & 0
\end{pmatrix},~~Q^2=\frac{1}{\sqrt{3}}\begin{pmatrix}
0 & 0 & 1\\
0 & 0 & 0\\
1 & 0 & 0
\end{pmatrix},~~Q^3=\frac{1}{\sqrt{3}}\begin{pmatrix}
0 & 1 & 0\\
1 & 0 & 0\... |
{'timestamp': '2020-06-01T02:09:24', 'yymm': '2005', 'arxiv_id': '2005.14468', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14468'} | arxiv | \section{Introduction}
Evaluating the performance of a power deliver network (PDN) has become a critical issue in very large-scale integration (VLSI) designs.
The power supply from the package do | wn to on-chip integrated circuits is distributed through metal layers and vias, which could be modeled as a linear network consisting of resistors, capacitors and inductors \cite{nassif2008power}. The on-chip circuit modules are simplified as time-varying current sources in PDN analysis. Due to the shrinking feature si... |
{'timestamp': '2020-06-01T02:08:46', 'yymm': '2005', 'arxiv_id': '2005.14451', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14451'} | arxiv | \section*{Robot HSR Hardware Description}
\section*{Appendix 1: Competition results}
\begin{table}[t]
\begin{center}
\caption{Results of recent competitions. [DSPL, domestic standard-platform lea | gue; JSAI, Japanese Society for Artificial Intelligence; METI, Ministry of Economy, Trade and Industry (Japan); OPL, open-platform league; RSJ, Robotics Society of Japan]}
\label{tab:result}
\begin{tabular}{l|l|l} \hline
\multicolumn{1}{c|}{Country} & \multicolumn{1}{c|}{Competition} & \multicolumn{1}{c}{Result} \\ \h... |
{'timestamp': '2020-06-01T02:10:14', 'yymm': '2005', 'arxiv_id': '2005.14496', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14496'} | arxiv | \section{Introducntion}
The present COVID-19 pandemic is a dynamic and volatile process with often unpredictable ups and downs in the infected populations that make it difficult to predict its future | course. In the absence of any vaccine or definitive drug in the immediate future \cite{Chen2020} the fight against COVID-19 is a hard and long drawn bitter battle, with two strategies being put forward. The first is the widely enforced lockdown, quarantine, and social distancing where the spread of the disease is cont... |
{'timestamp': '2020-06-01T02:09:36', 'yymm': '2005', 'arxiv_id': '2005.14474', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14474'} | arxiv | \section{Introduction}\label{secintroduction}
Einstein's general theory of relativity may not be the final word on gravity. As beautiful and successful as it is, it seems to have serious problems bot | h on very small and on very large length scales. A problem on small length scales is signaled by $90$ years of unwavering resistance of general relativity to quantization. A problem on the largest length scales is indicated by the present search for ``dark energy'' to explain the accelerated expansion of the universe w... |
{'timestamp': '2021-02-04T02:16:38', 'yymm': '2005', 'arxiv_id': '2005.14495', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14495'} | arxiv | \section{Introduction}
\label{section:into}
Compelling evidence for the existence of non-baryonic dark matter
particles is provided by the temperature structure of the cosmic
microwave background ra | diation \citep{planck2016} and supported by
observations of gravitational lensing \citep[see][for a
review]{massey2010}. Measurements of the cosmic large-scale structure
set constraints on the properties of the particles.
Thus, the observed large-scale distribution of galaxies rules out hot
dark matter, that is, parti... |
{'timestamp': '2020-06-01T02:05:06', 'yymm': '2005', 'arxiv_id': '2005.14355', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14355'} | arxiv |
\section{Introduction}
\Blindtext[5][2]
\midlacknowledgments{\blindtext}
\end{document}
\section{Introduction}
In last decade, the automated or semi-automated segmentation approaches have been wid | ely developed to identify and parse organs, bones, tumors, and other regions-of-interest (ROI).
However, most of the segmentation approaches tend to have difficulty in producing high quality prediction at the foreground boundary areas where appearance contrast of medical images is intrinsically fuzzy, which is usually ... |
{'timestamp': '2020-06-01T02:08:05', 'yymm': '2005', 'arxiv_id': '2005.14433', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14433'} | arxiv |
\section{Introduction}
Recently, deployments of \glspl{mav} are gaining increasing attention, especially in the mining industry~\cite{mansouri2020deploying}. The autonomous navigation of the \gls{ma | v}, equipped with a sensor suite has the ability to collect information, such as images, gas level, dust level, monitor the personnel, explore unknown and production areas, and minimize service times. At the same time, the deployments of \glspl{mav} increase the production and the overall safety in the mining industry,... |
{'timestamp': '2020-06-01T02:04:20', 'yymm': '2005', 'arxiv_id': '2005.14334', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14334'} | arxiv | \section{Introduction and main results}
Consider the following semilinear elliptic equation, which has been extensively studied:
$$
\left\{
\begin{array}{ll}
-\Delta u=\lambda f(u)\ \ \ \ | \ \ \ & \mbox{ in } \Omega \, ,\\
u>0 & \mbox{ in } \Omega \, ,\\
u=0 & \mbox{ on } \partial\Omega \, ,\\
\end{array}
\right. \eqno{(P_\lambda)}
$$
\
\noindent where $\Omega\subset\real^N$ is a smooth bounded domain,
$N\geq 1$, $\lambda\geq 0$ is a real parameter and the
nonlinearity $f:[0,\infty)\rightar... |
{'timestamp': '2020-11-30T02:04:55', 'yymm': '2005', 'arxiv_id': '2005.14314', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14314'} | arxiv | \section{Introduction}
Consider the system constituted by a hollow rigid body $\mathcal B_1$ whose cavity contains a homogeneous rigid ball $\mathcal B_2$. Let the gap between $\mathcal B_1$ and $\mat | hcal B_2$ be entirely filled by a viscous incompressible fluid $\mathscr{L}$ (simply called {\em liquid}). Let $G$ be the center of mass of the system $\mathscr S_C$ constituted by the outer rigid body $\mathcal{B}_1$ and the liquid. Suppose that $G$ is a fixed point in space and time with respect to an inertial frame ... |
{'timestamp': '2021-05-19T02:19:55', 'yymm': '2005', 'arxiv_id': '2005.14478', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14478'} | arxiv | \subsection{Methods}
\subsubsection{Sample Fabrication}
The plasmonic nanoantennas are fabricated using a top-down approach, based on the method outlined by \citet{horrer2013}. Au(80 nm) films were de | posited using electron-beam evaporation onto glass substrates. Later, Al$_{2}$O$_{3}$(3.5 nm)/Tb$_{18}$Co$_{82}$(15 nm)/Al$_{2}$O$_{3}$(2 nm) films were sputter deposited onto these films, with the complete structure being Au(80 nm)/Al$_{2}$O$_{3}$(3.5 nm)/Tb$_{18}$Co$_{82}$(15 nm)/Al$_{2}$O$_{3}$(2 nm). The Tb$_{18}$C... |
{'timestamp': '2020-06-01T02:11:20', 'yymm': '2005', 'arxiv_id': '2005.14534', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14534'} | arxiv | \section{Introduction}
Understanding galaxy formation is a major goal of current astrophysical research. Detailed studies of the stellar components of the Milky Way galaxy play a fundamental role in | building this understanding
because they provide direct and robust tests of and constraints on theories of galaxy formation. The latter are presently formulated within the framework of hierarchical formation
in a $\Lambda$CDM Universe (e.g., \citealt{1991ApJ...379...52W,1998MNRAS.295..319M}), and the past few decades ... |
{'timestamp': '2020-06-01T02:07:53', 'yymm': '2005', 'arxiv_id': '2005.14430', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14430'} | arxiv | \section{Introduction}
With 5G mobile systems being commercially rolling out gradually, research discussions into next-generation mobile systems, i.e., 6G, have started \cite{Latva-Aho2019}. 5G will | incur 10 times energy consumption of 4G due to increased density of cells and that of antennas, though energy efficiency per bit has increased. With 6G going towards higher spectrum (such as Tera-Hertz or THz) and thus resulting in even denser networks and smaller cells, energy consumption will become a big hurdle on t... |
{'timestamp': '2020-06-01T02:09:29', 'yymm': '2005', 'arxiv_id': '2005.14470', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14470'} | arxiv | \section{Introduction}
Heavy quarks (HQs), namely charm and bottom, are considered as a solid probe
to characterize the matter created in the QGP phase
~\cite{Svetitsky:1987gq,Moore:2004tg,Dong:2019 | unq,Prino:2016cni,Andronic:2015wma,Aarts:2016hap,Cao:2018ews,Rapp:2018qla}.
The large mass of heavy quarks has several implications in this context.
They are produced in the early stage of the collisions by pQCD process and being
$M_{HQ}>> T$ also the thermal pair production and annihilation processes are negligible.
F... |
{'timestamp': '2020-06-01T02:05:14', 'yymm': '2005', 'arxiv_id': '2005.14359', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14359'} | arxiv | \section{Introduction}
\IEEEPARstart{I}{n} machine learning, computer vision, data mining, and other fields, with the increase of the difficulty of research objects, we have to deal with some high-dim | ensional data, such as text data, image data, and various gene expression data. When processing high-dimensional data, we are confronted with the curse of dimensionality and some other difficulties caused by too many features, which not only makes the prediction results inaccurate, but also consumes the calculation tim... |
{'timestamp': '2020-06-01T02:04:21', 'yymm': '2005', 'arxiv_id': '2005.14335', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14335'} | arxiv | \section{Introduction}
\emph{Quantum computing} \cite{nc2010,a2017,aazksw2019part1} is one of the hot topics in computer science of last decades.
There are many problems where quantum algorithms outpe | rform the best known classical algorithms \cite{dw2001,quantumzoo,ks2019,kks2019}.
One of such problems are problems for strings. Researchers show the power of quantum algorithms for such problems in \cite{m2017,bbbv1997,rv2003,ki2019}.
In this paper, we consider the problem of constructing text from dictionary stri... |
{'timestamp': '2020-11-17T02:31:18', 'yymm': '2005', 'arxiv_id': '2005.14494', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14494'} | arxiv | \section{Introduction}
Magnetoresistance is one of the fundamental phenomena in the research field of spintronics.
Giant magnetoresistance\cite{Baibich1988,Binasch1989,Fert2008} and tunneling magneto | resistance\cite{Julliere1975,Miyazaki1995,Moodera1995,Yuasa2004,Parkin2004} are now essential ingredients in spintronics technology for sensors, memories, and data storage.
Recently, a novel type of magnetoresistance called spin Hall magnetoresistance (SMR) has been observed in a bilayer system composed of a normal met... |
{'timestamp': '2020-09-15T02:14:20', 'yymm': '2005', 'arxiv_id': '2005.14420', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14420'} | arxiv | \section{ Introduction}
In this paper, we consider the Dirichlet problem for the Lagrangian mean curvature equation on a uniformly convex, bounded domain $\Omega\subset\mathbb{R}^n$, given by
\begin | {align}
\begin{cases}
F(D^{2}u)=\sum _{i=1}^{n}\arctan \lambda_{i}=\psi(x) \text{ in } \Omega\\
u=\phi \text{ on }
\partial \Omega
\end{cases}\label{lab}
\end{align}
where $\lambda_i$'s are the eigenvalues of the Hessian matrix $D^2u$, $\psi$ is the potential for the mean curvature of the Lagrangian subma... |
{'timestamp': '2020-06-01T02:08:26', 'yymm': '2005', 'arxiv_id': '2005.14443', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14443'} | arxiv | \section{Introduction}
\label{intro}
Neutron star is a compact stellar object which can provide valuable information on the physics of dense nuclear matter because the density of the central part o | f a neutron star can reach several times of the normal nuclear matter density. In this dense environment, the quantum degeneracy pressure of hadrons dominates and the microscopic calculation based on QCD is almost impossible due to the highly non-perturbative nature of the strong interaction. Hence many effective appro... |
{'timestamp': '2020-06-01T02:03:32', 'yymm': '2005', 'arxiv_id': '2005.14299', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14299'} | arxiv | \section{Introduction}
A large portion of the empirical methods in Natural Language Processing (NLP) are defined over canonical text interpretation tasks such as Named Entity Recognition (NER), Seman | tic Role Labeling (SRL), Sentiment Analysis (SA), among others. The systematic creation of benchmarks and the comparative performance analysis of resources, representations and algorithms is instrumental for moving the boundaries of natural language interpretation. SemEval \cite{semeval-2019-international,semeval-2018-... |
{'timestamp': '2021-01-01T02:05:40', 'yymm': '2005', 'arxiv_id': '2005.14462', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14462'} | arxiv | \section{Introduction \label{section intro}}
In biostatistics, many models for survival and reliability analysis are two-state stochastic processes which lead to a particular event such as death, or | the outcome of a particular drug treatment. However, applying a multi-state stochastic process allows the modeller to provide a richer and more accurate model by adding more details. These details allow to capture alternative paths to the event of interest, specify all the intermediate events, and also allow to unde... |
{'timestamp': '2021-09-03T02:19:20', 'yymm': '2005', 'arxiv_id': '2005.14298', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14298'} | arxiv | \section*{Introduction}
A Josephson junction (JJ) consists of a localized discontinuity (weak link) in the order parameter of two superconducting electrodes \cite{tinkham_introduction_2004}, where the | dissipation-less current ruled by the Cooper pairs transport is controlled by the macroscopic quantum phase difference ($\varphi$) across the junction.
Weak links are typically realized in the form of a thin insulator, a semiconductor or metallic wire, or a narrow superconducting constriction~\cite{tinkham_introducti... |
{'timestamp': '2020-06-01T02:11:20', 'yymm': '2005', 'arxiv_id': '2005.14535', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14535'} | arxiv | \section{Introduction}\label{sec:introduction}
The equation of state (EoS) of strongly interacting matter is one of the key observables characterizing properties of matter under extreme conditions. I | t encodes information on the phase structure of Quantum Chromodynamics (QCD). One way of delineating the EoS is through the speed of sound, $c_s^2 \equiv \mathrm{d} P /\mathrm{d} \epsilon$. It has been conjectured that the speed of sound is bounded by $c_s^2 < 1/3$ (conformal bound). This conjecture was in fact confirm... |
{'timestamp': '2020-06-01T02:05:17', 'yymm': '2005', 'arxiv_id': '2005.14364', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14364'} | arxiv | \section{Introduction}
\begin{figure}[htb]
\includegraphics[scale=0.5]{Fig1.png}
\caption{(a) Schematics of $\alpha$-(BEDT-TTF)$_2$I$_3$ irradiated with circularly polarized light. (b) Unit cell (dash | ed rectangle) with four nonequivalent BEDT-TTF molecules (A, A$^\prime$, B, C) and transfer integrals in the BEDT-TTF layer.}
\label{Fig1}
\end{figure}
Photo-induced phase transitions are one of the central topics in recent condensed-matter physics~\cite{Tokura06,Bukov15,Basov17,Aoki14,Yonemitsu06}. A theoretical study... |
{'timestamp': '2020-12-08T02:10:00', 'yymm': '2005', 'arxiv_id': '2005.14411', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14411'} | arxiv | \section{Introduction}
\IEEEPARstart{T}{he} rapid development of the worldwide mobile communication technologies has been witnessed in recent years. After the 4th generation (4G) mobile communications | became universal around the world, the initial 5th generation (5G) standard was completed in 2018 and the 5G commercial networks were already employed in part in the first quarter of 2020. For supporting huge mobile data traffic and high-speed communications required by a growing number of {\color{black}the} mobile de... |
{'timestamp': '2020-11-19T02:23:35', 'yymm': '2005', 'arxiv_id': '2005.14454', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14454'} | arxiv | \section{\label{intr}Introduction}
Cosmic strings and other topological defects are a generic prediction of many theories beyond the Standard Model of particle physics, being formed by means of the Ki | bble mechanism \citep{Kibble:1976sj}. Since the properties of these objects and their astrophysical consequences are intrinsically linked to the symmetry breaking patterns which produce them, one can think of them as fossil relics of the physical conditions in the early Universe. As such, hunting for defects in the ear... |
{'timestamp': '2021-05-18T02:14:25', 'yymm': '2005', 'arxiv_id': '2005.14369', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14369'} | arxiv | \section{Introduction}
\label{sec:intro}
Recently, quantum computing (QC) has been gaining increased attention as a potential way to significantly speed up simulations of physical systems \cite{ref:m | ontanaro16}. The focus is usually made on modeling many-body quantum systems, whose enormous configuration space is often straightforward to map on reasonably sized quantum circuits, at least in principle. But it is also of interest to explore whether QC can be useful for modeling classical systems such as plasmas. In ... |
{'timestamp': '2020-06-01T02:10:40', 'yymm': '2005', 'arxiv_id': '2005.14508', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14508'} | arxiv | \section{Introduction}
Estimating the average treatment effect (ATE) is an important issue in many fields including social science and health science. See \cite{pspara}. There are two basic methodolo | gies: inverse propensity score-based estimation (PS) and outcome regression-based estimation (OR). But the former requires correctly postulated propensity model and the latter needs correctly postulated regression model. To avoid these misspecifications, as a very promising method, the doubly robust estimation (DR) has... |
{'timestamp': '2020-08-19T02:09:37', 'yymm': '2005', 'arxiv_id': '2005.14381', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14381'} | arxiv | \section{Introduction and related works}
A Bayesian Network (BN) is a type of a probabilistic graphical model that can be viewed as a Directed Acyclic Graph (DAG), where nodes represent uncertain vari | ables and arcs represent dependency or causal relationship between variables. The structure of a BN can be learned from data, and there are three main classes of structure learning: constraint-based, score-based and hybrid learning. The first type relies on conditional independence tests to construct the skeleton and o... |
{'timestamp': '2021-07-14T02:26:12', 'yymm': '2005', 'arxiv_id': '2005.14319', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14319'} | arxiv | \section{Introduction\label{sec:introduction}}
Recently the TOTEM experiment measured differential cross-sections of elastic proton-proton collisions in the TeV energy range, from $\sqrt{s} = 2.76$ | through 7 and 8 to 13 TeV, together with the total, elastic and inelastic cross-sections and the real to imaginary ratio of the scattering amplitude at vanishing four-momentum transfer. These measurements provided surprizes and unexpected results. First of all, the shape of the differential cross-section of elastic sca... |
{'timestamp': '2020-06-01T02:11:23', 'yymm': '2005', 'arxiv_id': '2005.14538', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14538'} | arxiv | \section{Introduction and results}
Diophantine approximation has been widely studied by mathematicians. In 1842, Dirichlet \cite{D1842} proved an illustrious theorem as follows.\\
{\bf Dirichl | et Theorem} For any two real numbers $\theta,~Q$ with $Q\geq 1$, there is an integer $n\in[1, Q]$ such that $$\lVert n \theta\rVert<Q^{-1},$$ where $\lVert\xi\rVert$ denotes the distance from $\xi$ to the nearest integer.
Dirichlet Theorem is called a \emph{uniform approximation theorem} in \cite[p.p. 2]{W12}.... |
{'timestamp': '2020-10-13T02:33:48', 'yymm': '2005', 'arxiv_id': '2005.14277', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14277'} | arxiv | \section{Introduction} \label{sec_introduction}
A recent area of research in inverse problems has been the development and study of new eigenvalue problems arising from scattering theory (cf. \cite{a | udibert_cakoni_haddar,audibert_chesnel_haddar,audibert_chesnel_haddar2019,cakoni_colton_meng_monk,camano_lackner_monk,cogar,cogar2019,cogar2020,cogar_colton_meng_monk,cogar_colton_monk,cogar_colton_monk2019}). In addition to generating mathematically interesting problems, the study of the resulting eigenvalues may find... |
{'timestamp': '2020-06-01T02:07:24', 'yymm': '2005', 'arxiv_id': '2005.14413', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14413'} | arxiv | \section{Introduction}
Miniaturization and advances in WiFi technologies have led to the emergence of Web-enabled devices. Interconnected devices are typically referred to as the \emph{Internet of Thi | ngs (IoT)}. More formally, IoT represents the network of \emph{things} that exchange data, essentially enabling a wide variety of applications such as smart homes and smart cities \cite{gubbi2013internet}. A potential application is a crowdsourcing platform whereby IoT devices \emph{crowdsource} services for the benefi... |
{'timestamp': '2020-06-16T02:06:48', 'yymm': '2005', 'arxiv_id': '2005.14419', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14419'} | arxiv | \subsection{Model-Free Policy Search}
In model-free policy search, sampled trajectories are used directly to
update the policy parameters.
The discussion will follow the three main steps followed by | the
algorithms: %
(i) how they {\em explore} the space of policies, %
(ii) how they {\em evaluate} policies, and %
(iii) how policies are {\em updated}.
\subsubsection{Policy Exploration}
Exploring the space of policies implies either sampling the parameter
vector the policy depends on, or perturbing the action choic... |
{'timestamp': '2020-10-30T01:18:05', 'yymm': '2005', 'arxiv_id': '2005.14435', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14435'} | arxiv | \section{Introduction}
In recent years, single-channel speech enhancement methods based on deep learning have been proposed in large numbers, and they can be divided into time domain and frequency | domain methods. Time-domain methods~\cite{segan}~\cite{Hao2019}~\cite{tcnn}~\cite{wavenet_d} typically use the time-domain signal of noisy speech as a direct input to a neural network, and the learning target is the clean speech signal. Frequency-domain methods~\cite{phase_sensitive_bilstm}~\cite{regression_approch}~\c... |
{'timestamp': '2020-11-06T02:20:50', 'yymm': '2005', 'arxiv_id': '2005.14475', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14475'} | arxiv | \section{ Introduction}\label{Intro}
It is anticipated that quantum computers will be able to simulate quantum systems exponentially faster than classical computers \cite{QC_gen_1, QC_gen_2, uni_q_s | im}.
A promising method to perform this task on emerging noisy intermediate-scale quantum (NISQ) computers \cite{NISQ,google_supreme} is the variational-quantum-eigensolver (VQE) algorithm \cite{UCCSD_0, vqe_2, VQE_accelerated, vqe_google_hf}.
The VQE is a hybrid classical-quantum variational algorithm that determine... |
{'timestamp': '2020-06-01T02:06:57', 'yymm': '2005', 'arxiv_id': '2005.14396', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14396'} | arxiv | \section{Introduction}\label{sec1}
Publication bias is one of the most important concerns in systematic reviews and meta-analyses. Part of the issue is that authors and scientific journals are likel | y to publish studies with statistically significant results than inconclusive studies\cite{thornton2000}. To be statistically significant, the studies with small sample size need to show larger treatment effects, which is known as the small-study effect\cite{sterne2000}. Thus, this may force us to analyze selective sa... |
{'timestamp': '2020-08-28T02:13:38', 'yymm': '2005', 'arxiv_id': '2005.14362', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14362'} | arxiv | \section{Introduction}
Galactic modeling requires considering evolution and an asymmetric potential, as pointed out by \citet{antoja2018}, who have revealed in our Galaxy many intriguing signals suc | h as snail shells, arches and ridges, etc. The so called Galactoseismology \citep{Widrow12, Widrow14} concludes the non-equilibrium and non-stationary potential of the Milky Way, observed in many density or velocity asymmetries in \citet{liuchao2017, wang2018a, wang2018b, wang2018c, wang2019, wang2020a, wang2020b, wang... |
{'timestamp': '2020-06-01T02:07:19', 'yymm': '2005', 'arxiv_id': '2005.14406', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14406'} | arxiv | \section{Appendix}\label{s:appendix}
For writing compactness we use the following shorthand notations for the transition and observation functions thoughout the next two subsections: $\ensuremath{T}\x | space = \ensuremath{T(s, a, s')}\xspace$, $\ensuremath{\widehat{T}}\xspace = \ensuremath{\widehat{T}(s, a, s')}\xspace$ and $\ensuremath{Z}\xspace = \ensuremath{Z(s, a, o)}\xspace$, $\ensuremath{\widehat{Z}}\xspace = \ensuremath{\widehat{Z}(s, a, o)}\xspace$. Additionally in section Section~\ref{ssec:proofLem4} we use ... |
{'timestamp': '2021-04-01T02:08:04', 'yymm': '2005', 'arxiv_id': '2005.14427', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14427'} | arxiv | \section{Introduction}\label{sec:bsu-intro}
Spatial structures and spatial algorithms are sometimes overshadowed by geostatistics and geochemical analysis in geology and stratigraphic modelling despit | e playing a no-less important role. In this paper, \textit{surface warping} is concerned with computational methods for mesh surface manipulation that automatically increase spatial fidelity \cite{guglielmino20133d}.\footnote{This should not be confused with alternative meanings in geomorphology for instance where \tex... |
{'timestamp': '2020-07-08T02:21:28', 'yymm': '2005', 'arxiv_id': '2005.14511', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14511'} | arxiv | \section{Introduction}
\blfootnote{* First authors contributed equally.}
Automated analysis of microscopic images heavily relies on classification or segmentation of objects in the image. Starting fro | m a robust and precise segmentation algorithm, downstream analysis subsequently will be more accurate and reliable.
Deep learning (DL) approaches nowadays have state-of-the-art performance in nearly all computer vision tasks (\cite{russakovsky2015imagenet}). In medical images or more specifically in computational path... |
{'timestamp': '2020-06-01T02:07:13', 'yymm': '2005', 'arxiv_id': '2005.14403', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14403'} | arxiv | \section{Introduction}
Graph ($G(V,E)$, in which $V$ is vertex set for describing dataset and $E$ is edge set for representing the relationship set between data) can capture the relationship of data d | istribution based on metric method (For example, Euclidean distance,Cosine distance or Kullback-Leibler divergence etc). As a metric representation, graph plays a vital role in pattern recognition. Especially, the recent graph convolutional networks (GCN) have the promising results for many application, for example, hu... |
{'timestamp': '2020-06-01T02:03:46', 'yymm': '2005', 'arxiv_id': '2005.14309', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14309'} | arxiv | \section{INTRODUCTION}
\label{s:intro}
The discovery of gravitational waves (GWs) from the coalescence of binary black holes (BHs) by the LIGO ground-based laser interferometers (Abbott et al.
2016b | ) was one of the biggest scientific discoveries at the beginning of the 21st century and gave powerful impetus to the development of
multi-wavelength observations of cosmic transients. Multi-wavelength observations of the first binary neutron star (NS) coalescence GW170817 (Abbott et al. 2016a) ushered in a new era of... |
{'timestamp': '2020-06-01T02:04:20', 'yymm': '2005', 'arxiv_id': '2005.14332', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14332'} | arxiv | \section{Introduction} \label{sec:intro}
Due to the high plasma $\beta$ in the photosphere and chromosphere, non-magnetic forces should be taken into account when we study these layers. If we neglect | dynamics and plasma flow, then the resulting static state of the system can be described by the so-called magnetohydrostatic (MHS) assumption, which is determined by the balance of Lorentz force, pressure gradient and gravity force, together with the solenoidal condition of the magnetic field.
The 3D MHS equations c... |
{'timestamp': '2020-06-01T02:08:40', 'yymm': '2005', 'arxiv_id': '2005.14448', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14448'} | arxiv | \section{Introduction}
The Sun is a magnetically active star, filling the interplanetary space with a stream of charged particles called the solar wind \citep[see e.g. a recent review by][]{Verschare | n2019}. The solar wind properties are far from being homogeneous, with strong variations in temperature, density, or interplanetary magnetic field observed in connection with various phenomena of solar activity. The main drivers of strong disturbances of the solar wind are coronal mass ejections (CMEs), the fast--slow ... |
{'timestamp': '2020-06-01T02:05:15', 'yymm': '2005', 'arxiv_id': '2005.14361', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14361'} | arxiv | \section{Introduction}
A main goal of the paper is to develop a methodology to price European option's contracts on electricity and future oil prices. The approach is based on Fourier expansions and | implements models that capture specific stylized features of the underlying assets such as stochastic volatility and random jumps. In particular, we consider a switching time-changed Levy process as an alternative to the BSM model and implement a pricing algorithm based on the expansion of its characteristic function ... |
{'timestamp': '2020-06-04T02:09:42', 'yymm': '2005', 'arxiv_id': '2005.14328', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14328'} | arxiv | \section{Introduction}
The weakly beyond-mean-field description of a Bose quantum fluid, initially introduced by Bogoliubov, relies on small collective excitations on top of a time-independent conden | sate \cite{Bogoliubov1947, Pitaevskii2016}.
These excitations are described as non-interacting quasi-particles with a specific energy spectrum: sound-like at low momenta and free-particle-like at large momenta.
Due to these linear then parabolic dependences at respectively low and large momenta, a system exhibiting thi... |
{'timestamp': '2020-06-01T02:03:58', 'yymm': '2005', 'arxiv_id': '2005.14316', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14316'} | arxiv | \section*{Summary}
\begin{enumerate}
\item Ecologists use distance sampling to estimate the abundance of plants
and animals while correcting for undetected individuals. By design,
data collection is s | implified by requiring only the distances from
a transect to the detected individuals be recorded. Compared to traditional
design-based methods that require restrictive assumption and limit
the use of distance sampling data, model-based approaches enable broader
applications such as spatial prediction, inferring specie... |
{'timestamp': '2020-06-01T02:03:53', 'yymm': '2005', 'arxiv_id': '2005.14313', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14313'} | arxiv |
\section{Introduction}
\label{sec:intro}
Several prior works for depth estimation from monocular images doesn't work with raw images straight out of the camera, which would be distorted and unre | ctified. Instead, these raw images are corrected with image processing techniques before being fed into the network to predict an undistorted rectified depth map. We propose a novel fully differentiable architecture which allows estimating the distorted unrectified depth directly from a raw image without the need for a... |
{'timestamp': '2021-02-23T02:19:09', 'yymm': '2005', 'arxiv_id': '2005.14358', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14358'} | arxiv | \subsection*{Acknowledgments}
We wish to thank Ping Xi for many helpful comments, especially his
suggestion on the presentation of the proof of \eqref{e.M2}. We are grateful
to Nick Katz and Zhiyon | g Zheng for encouragement. We thank the referee for
useful comments. We acknowledge the support of Princeton University, where
part of this work was done during a visit.
\begin{bibdiv}
\begin{biblist}
\bib{dSSV}{article}{
author={de la Bret\`eche, R\'{e}gis},
author={Sha, Min},
author={Shparlinski, I... |
{'timestamp': '2020-06-01T02:05:16', 'yymm': '2005', 'arxiv_id': '2005.14363', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14363'} | arxiv | \section{Introduction}
Judging similarity between any pair of stimuli is an ambiguous problem: deciding what counts as similar is subjective and sensitive to context \cite{Medin1993}.
Nevertheless, pe | ople are relatively consistent in making similarity judgments, which is perhaps explained in part by the biases they develop towards emphasizing some stimulus features over others (\textit{e.g.,} shape over size, color, or material; \citeNP{Diesendruck2003}). Understanding the features (and the weights upon them) that ... |
{'timestamp': '2020-06-01T02:05:27', 'yymm': '2005', 'arxiv_id': '2005.14366', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14366'} | arxiv | \section{INTRODUCTION}
\label{sec:intro}
In the standard model, radio pulsars are highly-magnetised rapidly rotating neutron stars that emit a coherent light-house beam of often highly polarised rad | io emission directed by
their magnetospheres \citep{2004hpa..book.....L}.
The weak braking torques caused by their rapidly rotating magnetic fields and their high moments of inertia make them extremely stable flywheels, and it is often possible to predict the pulsar spin period and indeed pulse phase years in advance ... |
{'timestamp': '2020-06-01T02:05:33', 'yymm': '2005', 'arxiv_id': '2005.14368', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14368'} | arxiv | \section{Introduction}
Apart from the conventional microelectronic application, manganese silicide alloy of nominal composition Mn$_5$Si$_3$ has attracted renewed interest among researchers due to the | recent discovery of different interesting magnetic and magnetofunctional properties, which includes magnetocaloric effect, anomalous Hall effect, inverted hysteresis behavior, thermomagnetic irreversibility, and spin fluctuation~\cite{lander, menshikov, silva, gottschilch, brown, kanani, surgers, biniskos,prb-scd}. At... |
{'timestamp': '2020-06-01T02:11:09', 'yymm': '2005', 'arxiv_id': '2005.14520', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14520'} | arxiv |
\section{Introduction}
In response to climate change concerns, the decarbonization and digitization of the electricity sector have been accelerated in recent years. The path to decarbonization is as | sociated with the high penetration of Distributed Energy Resources (DERs), such as rooftop solar, home batteries and electric vehicles with the potential to support a reliable, affordable and lower-emissions electricity grid. Increase in the deployment of DERs raises several opportunities and challenges in the electric... |
{'timestamp': '2020-06-01T02:08:47', 'yymm': '2005', 'arxiv_id': '2005.14452', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14452'} | arxiv | \subsubsection{\@startsection{subsubsection}{3}%
\newcommand{\mathbb{Z}}{\mathbb{Z}}
\newcommand{\mathbb{F}}{\mathbb{F}}
\newcommand{\mathbb{F}_p}{\mathbb{F}_p}
\newcommand{\mathbb{Z}_p}{\mathbb{Z}_ | p}
\newcommand{\mathfrak{p}}{\mathfrak{p}}
\DeclareMathOperator{\rk}{rk}
\newcommand{\rk_p}{\rk_p}
\newcommand{\mathcal{H}}{\mathcal{H}}
\newcommand{\operatorname{H}^{*}}{\operatorname{H}^{*}}
\DeclareMathOperator{\Ker}{Ker}
\DeclareMathOperator{\Image}{Im}
\DeclareMathOperator{\id}{id}
\DeclareMathOperator{\Hom}{Hom}... |
{'timestamp': '2020-06-01T02:07:09', 'yymm': '2005', 'arxiv_id': '2005.14400', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14400'} | arxiv | \section{Introduction}
\label{sec:intro}
Traditional multispectral images (MSIs, \textit{e}.\textit{g}. RGB images) usually contain a reduced number of spectral bands providing a limited spectral inf | ormation. It is well-known that, the more spectral bands we have, the better we would understand the latent spectral structure. Since hyperspectral imaging can obtain more spectral bands, it has become a non-negligible technology that is able to capture the intrinsic properties of different materials.
However, due to t... |
{'timestamp': '2020-06-01T02:11:17', 'yymm': '2005', 'arxiv_id': '2005.14532', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14532'} | arxiv | \section{Introduction}
The epidemic of SARS-CoV-2 infection triggered an unprecedented public health response.
Given the lack of effective vaccine and treatment in 2020, this
response included a var | iety of travel restrictions and social distancing measures \cite{Tian}.
While these measures help to slow down the epidemic they come at significant economical and societal
cost \cite{ECDCRRA}.
As an alternative an approach focusing on rapid diagnosis is increasingly recommended \cite{WHO.S} and prior to lifting soci... |
{'timestamp': '2020-06-01T02:07:22', 'yymm': '2005', 'arxiv_id': '2005.14412', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14412'} | arxiv | \section{Introduction and Summary}
It is well known that effective action for Dp-brane is
Dirac-Born-Infeld (DBI) action
\cite{Polchinski:1995mt,Leigh:1989jq}(For review, see for example
\cite{Sim | on:2011rw}). The problem with this action is that it is
non-polynomial in world-volume coordinates and in world-volume gauge
field that makes its analysis rather complicated. Similar situation
occurs with fundamental string whose dynamics is governed by
Nambu-Gotto form of the action which is again non-polynomial i... |
{'timestamp': '2020-10-28T01:02:10', 'yymm': '2005', 'arxiv_id': '2005.14331', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14331'} | arxiv | \section{Introduction}
The M5-brane is an interesting and important object in M-Theory for a variety of reasons. Its dynamics are described by a six-dimensional field theory with $(2,0)$ supersymmetr | y. For multiple M5-branes this is an interacting, strongly coupled superconformal field theory. However, we currently lack a satisfactory understanding of this theory.
Nevertheless, a particularly fruitful application of M5-branes involves compactifying them on a manifold to obtain lower dimensional field theories. In ... |
{'timestamp': '2020-10-30T01:18:04', 'yymm': '2005', 'arxiv_id': '2005.14441', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14441'} | arxiv | \section{Introduction}
\label{sec:intro}
Speech enhancement is to separate clean speech from noisy speech~\cite{se_book}. It is an essential branch of speech signal processing and has been widely stu | died in the past few decades. It can be used in hearing aids, voice recorders, and smart speakers, as well as the front end of tasks such as speech recognition~\cite{speech_se} and speaker recognition~\cite{speaker_se}. In recent years, a large number of speech enhancement methods based on deep learning have been propo... |
{'timestamp': '2020-11-17T02:15:07', 'yymm': '2005', 'arxiv_id': '2005.14506', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14506'} | arxiv |
\section{Introduction}
\label{sec:introduction}
\input{introduction}
\section{Notation}
\input{notation}
\section{DCTN's description}
\subsection{Input preprocessing}
\label{sec:input_preprocessing | }
\input{input_preprocessing}
\subsection{Entangled plaquette states}
\label{sec:entangled_plaquette_states}
\input{entangled_plaquette_states}
\subsection{Description of the whole model}
\label{sec:description_of_the_whole_model}
\input{description_of_the_whole_model}
\subsection{Optimization}
\input{optimization}
... |
{'timestamp': '2021-03-23T01:34:37', 'yymm': '2005', 'arxiv_id': '2005.14282', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14282'} | arxiv |
\section{Introduction}
Blockchain technology is maturing at a fast pace. The development of real-world applications shows real interest from both industry and academia \cite{zohar2015,UlHassan2019}. | For instance, applications have been developed in the areas of public administration \cite{Belchior2019, Belchior2019_Audits}, access control \cite{rouhani2019,ssibac}, and others \cite{casino2019}. Additionally, blockchain is progressing towards the performance of centralized systems: for example, the Hyperledger Fab... |
{'timestamp': '2020-06-01T02:04:50', 'yymm': '2005', 'arxiv_id': '2005.14348', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14348'} | arxiv |
\section{Introduction}
\begin{figure}
\centering
\includegraphics[width=0.4\textwidth]{Picture1_v3ga.png}
\caption{\small D0$_3$ (space group Fm$\bar3$m no. 225, prototype BiF$_3$) and $\beta$-W A1 | 5 (space group Pm$\bar3$n no. 223, prototype Cr$_3$Si) crystal structures of V$_3$Ga.}
\label{fig1}
\end{figure}
Combining superconductivity and antiferromagnetism could find useful applications in quantum spintronic devices. Superconductivity and magnetism were once thought to be mutually exclusive, as magnetic field... |
{'timestamp': '2020-06-23T02:29:50', 'yymm': '2005', 'arxiv_id': '2005.14521', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14521'} | arxiv | \section{Introduction}
Tensors, as a generalization of vectors and matrices, arise in many data processing applications and have attracted great interests.
For instance, video inpainting \cite{tens | or_video},
magnetic resonance imaging (MRI) data recovery \cite{tensor_MRI, MRI_tensor},
3D image reconstruction \cite{tensor_3dimage, tensor_3DReconstruction},
high-order web link analysis [16],
hyperspectral image (HSI) or multispectral image recovery \cite{tensor_HSI, chen2018tensor},
personalized web search \cite{t... |
{'timestamp': '2020-06-16T02:10:27', 'yymm': '2005', 'arxiv_id': '2005.14346', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14346'} | arxiv | \section{Introduction}
A Bayesian network (BN) is a probabilistic graphical model consisting of a labeled directed acyclic graph (DAG) $\mathcal{G} = (V, E)$, in which the vertex set $V = \{V_1, \dot | s, V_m\}$ corresponds to $m$ random variables, and the edge set $E$ prescribes a decomposition of the joint probability distribution of the random variables based on their parents in $\mathcal{G}$. The edge set $E$ encodes Markov relations on the nodes in the sense that each node is conditionally independent of its non... |
{'timestamp': '2020-06-01T02:03:57', 'yymm': '2005', 'arxiv_id': '2005.14315', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14315'} | arxiv | \section{Introduction}
Neural conversation systems which treat dialogue response generation as a sequence generation task \cite{neural_conversation_model} often produce generic and incoherent response | s \cite{shao-etal-2017-generating}. The primary reason for this is that, unlike humans, such systems do not have any access to background knowledge about the topic of conversation. For example, while chatting about movies, we use our background knowledge about the movie in the form of plot details, reviews and comments... |
{'timestamp': '2020-06-01T02:09:57', 'yymm': '2005', 'arxiv_id': '2005.14491', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14491'} | arxiv | \section{Introduction}
Throughout this article, we shall assume that all schemes have an ample family of line bundles. For example, every quasi-projective scheme over a commutative ring has an ample f | amily of line bundles. Usually, $K$-theory of vector bundles behaves well under this assumption. By a quasi-projective scheme will always mean a scheme which is quasi-projective over some commutative ring.
Let $\mathcal{E}$ be a vector bundle of rank $r+1$ over a quasi-projective scheme $X,$ and $\mathbb{P}(\mathcal{E... |
{'timestamp': '2020-06-01T02:09:21', 'yymm': '2005', 'arxiv_id': '2005.14467', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14467'} | arxiv | \section{Introduction}
Intracranial aneurysms (IAs) are abnormal vessel wall dilatations in the cerebral vasculature and, according to a study that included $94,912$ subjects~\cite{vlak2011prevalence | }, have a high 3.2\% prevalence in the general population. Most IAs are small and it is estimated that 50-80\% do not rupture during a person's lifetime. Still, rupture of IA is one of the most common causes of subarachnoid hemorrhage (SAH) \cite{van2007subarachnoid}, a condition with 50\% mortality rate~\cite{etminan2... |
{'timestamp': '2020-06-01T02:04:16', 'yymm': '2005', 'arxiv_id': '2005.14329', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14329'} | arxiv |
\section{Comparison with experimental quantities}
Figure \ref{f:experiment} illustrates the main experimental spectroscopic
results on the superlattices (SL) \cite{gu2018,laverock2017}, in which
tran | sport measurements established that
the 2:7 and 3:6 SLs were insulating, whereas the 13:4 SL was metallic. The 6:5
SL was found to be
metallic at room temperature, with an metal-insulator transition (MIT)
at low temperature. The experimental
results (performed at room temperature) show the evolution in correlated
elect... |
{'timestamp': '2020-06-01T02:10:17', 'yymm': '2005', 'arxiv_id': '2005.14497', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14497'} | arxiv | \section{Introduction}
Engineering of local magnetic properties of continuous thin films has long been an important topic in design and fabrication of future spintronic devices, high-density magnetic | data-storage devices, and magnetologic devices. Since Chappert \textit{et al.}~first reported the ability of ion irradiation to induce modification of local magnetic properties without altering topographic features,\cite{Chappert1998} ion-induced magnetic patterning has been investigated intensively and demonstrated t... |
{'timestamp': '2020-06-01T02:07:01', 'yymm': '2005', 'arxiv_id': '2005.14398', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14398'} | arxiv | \section{Introduction}
The following set of features are derived from other packages with
slight modifications to make them compatible with the \verb"gji"
documentclass. They can be accessed by inc | luding the \verb"extra"
option to the \verb"gji" document class e.g.
\begin{verbatim}
\documentclass[extra,mreferee]{gji}
\end{verbatim}
\section{Reserved Space and Boxed Figures }
It is possible to reserve space for a figure (or to draw a box of
a specified size) using the \verb!\figbox! command.
The \... |
{'timestamp': '2021-11-29T02:27:10', 'yymm': '2005', 'arxiv_id': '2005.14289', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14289'} | arxiv | \section{Introduction}
Determinantal ideals and their generalizations have been explored extensively both in the context of commutative algebra and also in the study of Schubert varieties in flag var | ieties. This overlap is to be expected because, for example,
\begin{itemize}
\item each ideal generated by the $k\times k$ minors of a generic matrix is the defining ideal of an open patch of a Schubert variety in a Grassmannian;
\item each one-sided ladder determinantal ideal is a Schubert determinantal ideal for a v... |
{'timestamp': '2020-06-01T02:03:23', 'yymm': '2005', 'arxiv_id': '2005.14293', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14293'} | arxiv | \section{High-harmonic generation in spin-orbit coupled systems - Supplementary material}
\section{Selection rules -- a simple example}
To illustrate the formalism introduced in the paper on a sim | ple example, we derive the well known result that inversion symmetry implies only odd order harmonics. We consider the Hamiltonian
\begin{equation}
\hat{H}(t) = \sum_{{k}} \cos({k} + A_0 \cos(\Omega t)) \hat{c}^{\dagger}_{{k}} \hat{c}_{{k}},
\end{equation}
and, since we are interested in HHG, choose as operator $\mat... |
{'timestamp': '2020-06-01T02:08:55', 'yymm': '2005', 'arxiv_id': '2005.14455', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14455'} | arxiv | \section{Introduction}
Multiple unmanned aerial vehicles (UAVs) have attracted considerable interest these years, of which prospective applications include disaster area or maritime surveillance, bor | der patrol, environmental sensing, delivery service, etc (\cite{jenie2016taxonomy}). This determines that the UAVs would fly in an integrated airspace with a variety of possible conflict objects therein (See in Fig. \ref{fig:environment}).
However, one key issue that limits the extensive application and the integratio... |
{'timestamp': '2020-06-01T02:04:34', 'yymm': '2005', 'arxiv_id': '2005.14340', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14340'} | arxiv | \section{Introduction}
This work is concerned with the numerical resolution of the stationary Dirac equation with periodic coefficients. The Dirac equation is historically associated with relativistic | quantum mechanics, and is central in condensed matter physics in the study of graphene, topological insulators, and Weyl/Dirac semimetals, etc. This is the main application we consider here. The two-dimensional expression of the (linear) Dirac Hamiltonian reads, with all physical constants set to one,
\mathbf e} \newc... |
{'timestamp': '2020-06-01T02:04:51', 'yymm': '2005', 'arxiv_id': '2005.14349', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14349'} | arxiv | \section{Introduction}
\IEEEPARstart{L}{et} $\mathbb{F}_{q}$ be a finite field with $q$ elements, in which $q$ is prime or a prime power. $\mathbb{F}_{q^n}$ denotes a finite extension field of $\mathb | b{F}_{q}$, which may be seen as a $n-$dimensional vector space over $\mathbb{F}_q$.
A polynomial $f(x) \in \mathbb{F}_{q^n} [x]$ is called a \emph{permutation polynomial} of $\mathbb{F}_{q^n}$ if the induced mapping by it
\begin{equation}
\begin{array}{cccc}
\phi_f:&\mathbb{F}_{q^n} &\rightarrow& \mathbb{F}_{q^n}\\
&... |
{'timestamp': '2020-06-01T02:07:29', 'yymm': '2005', 'arxiv_id': '2005.14416', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14416'} | arxiv | \section{Introduction}
The holographic approach based on the string/gauge duality
is a powerful method to study various thermo-dynamical
and non-perturbative properties of the Yang-Mills theory |
especially when the chemical potential ($\mu$) of the fundamental fermions plays an important role.
Various results have been
obtained in such cases and they could give us many kinds of insight into the phase diagram of QCD. (See for example
\cite{mateos2,Horigome,GKTT,GKTTT}.)
On the other hand, many non-p... |
{'timestamp': '2020-10-28T01:29:44', 'yymm': '2005', 'arxiv_id': '2005.14276', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14276'} | arxiv | \section{Introduction}
\label{Sec:intro}
The bottom-quark production in hadron-hadron collisions is an important
test of perturbative quantum chromodynamics (pQCD) calculations. Because
of its larg | e mass, $m_b \gg \Lambda_{QCD}$, the $b$-quark production
cross section can be reliably calculated by including next-to-leading
order (NLO) processes, especially at high center of mass
energies~\cite{Mangano1992295}. The measurement of the $b\bar{b}$\xspace production
cross section over a wide range of colliding e... |
{'timestamp': '2020-07-31T02:07:30', 'yymm': '2005', 'arxiv_id': '2005.14327', 'language': 'en', 'url': 'https://arxiv.org/abs/2005.14327'} | arxiv | \section{Introduction}
Recently, the speech community is seeing a significant trend of moving from deep neural network based hybrid modeling \cite{DNN4ASR-hinton2012} to end-to-end (E2E) modeling \cit | e{miao2015eesen, chan2016listen, prabhavalkar2017comparison, battenberg2017exploring, rao2017exploring, chiu2018state, Li18CTCnoOOV, he2019streaming, Li2020Developing} for automatic speech recognition (ASR). While hybrid models require disjoint optimization of separate constituent models such as acoustic and language ... |
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