id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
1,803.01967 | Learning Scene Gist with Convolutional Neural Networks to Improve Object
Recognition | Advancements in convolutional neural networks (CNNs) have made significant
strides toward achieving high performance levels on multiple object recognition
tasks. While some approaches utilize information from the entire scene to
propose regions of interest, the task of interpreting a particular region or
object is st... | cs.CV | advancements in convolutional neural networks cnns have made significant strides toward achieving high performance levels on multiple object recognition tasks while some approaches utilize information from the entire scene to propose regions of interest the task of interpreting a particular region or object is still pe... | [['advancements', 'in', 'convolutional', 'neural', 'networks', 'cnns', 'have', 'made', 'significant', 'strides', 'toward', 'achieving', 'high', 'performance', 'levels', 'on', 'multiple', 'object', 'recognition', 'tasks', 'while', 'some', 'approaches', 'utilize', 'information', 'from', 'the', 'entire', 'scene', 'to', 'p... | [-0.0189553362911163, 0.009345596112392808, -0.06689779713833656, 0.03891187780918603, -0.12041369403303458, -0.16080308677480806, 0.024683183221708215, 0.445851089225875, -0.25568461042666246, -0.3832612448918914, 0.05490633307108606, -0.2598097141925738, -0.2161149825619302, 0.19496516740471914, -0.2083611030329319, ... |
1,803.01968 | An Online Algorithm for Learning Buyer Behavior under Realistic Pricing
Restrictions | We propose a new efficient online algorithm to learn the parameters governing
the purchasing behavior of a utility maximizing buyer, who responds to prices,
in a repeated interaction setting. The key feature of our algorithm is that it
can learn even non-linear buyer utility while working with arbitrary price
constra... | stat.ML cs.LG econ.EM math.OC | we propose a new efficient online algorithm to learn the parameters governing the purchasing behavior of a utility maximizing buyer who responds to prices in a repeated interaction setting the key feature of our algorithm is that it can learn even nonlinear buyer utility while working with arbitrary price constraints t... | [['we', 'propose', 'a', 'new', 'efficient', 'online', 'algorithm', 'to', 'learn', 'the', 'parameters', 'governing', 'the', 'purchasing', 'behavior', 'of', 'a', 'utility', 'maximizing', 'buyer', 'who', 'responds', 'to', 'prices', 'in', 'a', 'repeated', 'interaction', 'setting', 'the', 'key', 'feature', 'of', 'our', 'alg... | [-0.08899003139844067, 0.01315888845802922, -0.1007627729498046, 0.10037657725440927, -0.24062916825182343, -0.258400303863087, 0.146748886566217, 0.4582055227242802, -0.32011539284384954, -0.31533053123367655, 0.06586580660108379, -0.25712639822220235, -0.17852505725367288, 0.12299378172151353, -0.15766008663922548, 0... |
1,803.01969 | Moment-Based Quantile Sketches for Efficient High Cardinality
Aggregation Queries | Interactive analytics increasingly involves querying for quantiles over
sub-populations of high cardinality datasets. Data processing engines such as
Druid and Spark use mergeable summaries to estimate quantiles, but summary
merge times can be a bottleneck during aggregation. We show how a compact and
efficiently mer... | cs.DB | interactive analytics increasingly involves querying for quantiles over subpopulations of high cardinality datasets data processing engines such as druid and spark use mergeable summaries to estimate quantiles but summary merge times can be a bottleneck during aggregation we show how a compact and efficiently mergeable... | [['interactive', 'analytics', 'increasingly', 'involves', 'querying', 'for', 'quantiles', 'over', 'subpopulations', 'of', 'high', 'cardinality', 'datasets', 'data', 'processing', 'engines', 'such', 'as', 'druid', 'and', 'spark', 'use', 'mergeable', 'summaries', 'to', 'estimate', 'quantiles', 'but', 'summary', 'merge', ... | [-0.05156790950362954, 0.06715301465695067, -0.06415339882266434, 0.11823421696077703, -0.08320432841830873, -0.11685105231042732, 0.12632750628023026, 0.4102531720363699, -0.23980836375233006, -0.3920013166197083, 0.12376973707817823, -0.3207143796388717, -0.04656020695795579, 0.23453951865872916, -0.0813457792487872,... |
1,803.0197 | Existence Results for the Nonlinear Hodge Minimal Surface Energy | Given a compact Riemannian manifold $(M^n,g)$ and a fixed cohomology class,
$[\alpha^*] \in H^k(M)$, we consider the existence of a minimizer $\alpha \in
[\alpha^*]$ of the generalized minimal surface energy $\int_M
\sqrt{1+|\alpha|^2} dV_g$. When $k = 1$, we prove the existence of unique
minimizers for every cohomol... | math.DG | given a compact riemannian manifold mng and a fixed cohomology class alpha in hkm we consider the existence of a minimizer alpha in alpha of the generalized minimal surface energy int_m sqrt1alpha2 dv_g when k 1 we prove the existence of unique minimizers for every cohomology class alpha next when k 1 we construct exam... | [['given', 'a', 'compact', 'riemannian', 'manifold', 'mng', 'and', 'a', 'fixed', 'cohomology', 'class', 'alpha', 'in', 'hkm', 'we', 'consider', 'the', 'existence', 'of', 'a', 'minimizer', 'alpha', 'in', 'alpha', 'of', 'the', 'generalized', 'minimal', 'surface', 'energy', 'int_m', 'sqrt1alpha2', 'dv_g', 'when', 'k', '1'... | [-0.186308307318311, 0.09730550456350963, -0.03535579074860403, 0.10009536990822342, -0.06307309702970088, -0.1935258087113892, -0.005602585739995304, 0.30804108375879496, -0.27777886067173985, -0.19519739566664945, 0.10527541009329358, -0.32775325501631747, -0.14331592737059845, 0.15568538029972268, -0.054100889722375... |
1,803.01971 | Exoplanets Torqued by the Combined Tides of a Moon and Parent Star | In recent years, there has been interest in Earth-like exoplanets in the
habitable zones of low mass stars ($\sim0.1-0.6\,M_\odot$). Furthermore, it has
been argued that a large moon may be important for stabilizing conditions on a
planet for life. If these two features are combined, then an exoplanet can feel
a simi... | astro-ph.EP | in recent years there has been interest in earthlike exoplanets in the habitable zones of low mass stars sim0106m_odot furthermore it has been argued that a large moon may be important for stabilizing conditions on a planet for life if these two features are combined then an exoplanet can feel a similar tidal influence... | [['in', 'recent', 'years', 'there', 'has', 'been', 'interest', 'in', 'earthlike', 'exoplanets', 'in', 'the', 'habitable', 'zones', 'of', 'low', 'mass', 'stars', 'sim0106m_odot', 'furthermore', 'it', 'has', 'been', 'argued', 'that', 'a', 'large', 'moon', 'may', 'be', 'important', 'for', 'stabilizing', 'conditions', 'on'... | [-0.11784252431622244, 0.23714621746927977, -0.10192448578938668, 0.09128685972447, -0.1694285184858609, -0.03260821216300554, 0.031137040627900722, 0.3282012653639313, -0.24478273884756718, -0.331147132514516, 0.10710344109939775, -0.2786444347111387, -0.11271971176526077, 0.23559767284858366, -0.10617793154546885, -0... |
1,803.01972 | SysML/KAOS Domain Models and B System Specifications | In this paper, we use a combination of the SysML/KAOS requirements
engineering method, an extension of SysML, with concepts of the KAOS goal
model, and of the B System formal method. Translation rules from a SysML/KAOS
goal model to a B System specification have been defined. They allow to obtain
a skeleton of the B ... | cs.SE | in this paper we use a combination of the sysmlkaos requirements engineering method an extension of sysml with concepts of the kaos goal model and of the b system formal method translation rules from a sysmlkaos goal model to a b system specification have been defined they allow to obtain a skeleton of the b system spe... | [['in', 'this', 'paper', 'we', 'use', 'a', 'combination', 'of', 'the', 'sysmlkaos', 'requirements', 'engineering', 'method', 'an', 'extension', 'of', 'sysml', 'with', 'concepts', 'of', 'the', 'kaos', 'goal', 'model', 'and', 'of', 'the', 'b', 'system', 'formal', 'method', 'translation', 'rules', 'from', 'a', 'sysmlkaos'... | [-0.10284045426454688, -0.02385817078486196, -0.1017630450579824, 0.02792767476991153, -0.09195411645766324, -0.09982961895963494, 0.08508613767723243, 0.3569931565262612, -0.2944571399657091, -0.30056921322976454, 0.10331892653781358, -0.23284580834127916, -0.1447017018700827, 0.17095210425315555, -0.08077901345238371... |
1,803.01973 | The enzyme-like catalytic activity of cerium oxide nanoparticles and its
dependency on Ce3+ surface area concentration | Cerium oxide nanoparticles are known to catalyze the decomposition of
reactive oxygen species such as superoxide radical and hydrogen peroxide.
Herein, we examine the superoxide dismutase (SOD) and catalase (CAT) mimetic
catalytic activities of nanoceria and demonstrate the existence of generic
behaviors. For particl... | cond-mat.mtrl-sci | cerium oxide nanoparticles are known to catalyze the decomposition of reactive oxygen species such as superoxide radical and hydrogen peroxide herein we examine the superoxide dismutase sod and catalase cat mimetic catalytic activities of nanoceria and demonstrate the existence of generic behaviors for particles of siz... | [['cerium', 'oxide', 'nanoparticles', 'are', 'known', 'to', 'catalyze', 'the', 'decomposition', 'of', 'reactive', 'oxygen', 'species', 'such', 'as', 'superoxide', 'radical', 'and', 'hydrogen', 'peroxide', 'herein', 'we', 'examine', 'the', 'superoxide', 'dismutase', 'sod', 'and', 'catalase', 'cat', 'mimetic', 'catalytic... | [-0.03354230272008828, 0.18886047217870436, -0.023066236575147468, 0.016811424459465603, 0.04132332290304406, -0.143492474615057, 0.06851563457417431, 0.37655174350321435, -0.2302822816334932, -0.3064342031086033, 0.023378810628429256, -0.3211012009629293, -0.10447036386935406, 0.15253435239991237, -0.00792139993855756... |
1,803.01974 | Pro-arrhythmogenic effects of heterogeneous tissue curvature: A
suggestion for role of left atrial appendage in atrial fibrillation | Background: The arrhythmogenic role of atrial complex morphology has not yet
been clearly elucidated. We hypothesized that bumpy tissue geometry can induce
action potential duration (APD) dispersion and wavebreak in atrial fibrillation
(AF).
Methods and Results: We simulated 2D-bumpy atrial model by varying the deg... | q-bio.TO physics.bio-ph | background the arrhythmogenic role of atrial complex morphology has not yet been clearly elucidated we hypothesized that bumpy tissue geometry can induce action potential duration apd dispersion and wavebreak in atrial fibrillation af methods and results we simulated 2dbumpy atrial model by varying the degree of bumpin... | [['background', 'the', 'arrhythmogenic', 'role', 'of', 'atrial', 'complex', 'morphology', 'has', 'not', 'yet', 'been', 'clearly', 'elucidated', 'we', 'hypothesized', 'that', 'bumpy', 'tissue', 'geometry', 'can', 'induce', 'action', 'potential', 'duration', 'apd', 'dispersion', 'and', 'wavebreak', 'in', 'atrial', 'fibri... | [-0.105170457071348, 0.11425630881109135, -0.05504836674761657, 0.06720409216865411, -0.016345919427070497, -0.17544681056974015, -0.009211782303049369, 0.4216649202260994, -0.18386573198246928, -0.2541416958694297, 0.07505282295636095, -0.3037969562931409, -0.20008739218979643, 0.18058371029744727, -0.1144872545827054... |
1,803.01975 | Exponential Riordan arrays and generalized Narayana polynomials | Generalized Euler polynomials ${{\alpha }_{n}}\left( x \right)={{\left( 1-x
\right)}^{n+1}}\sum\nolimits_{m=0}^{\infty }{{{p}_{n}}}\left( m
\right){{x}^{m}}$, where ${{p}_{n}}\left( x \right)$ is the polynomial of
degree $n$, are the numerator polynomials of the generating functions of
diagonals of the ordinary Riord... | math.NT | generalized euler polynomials alpha _nleft x rightleft 1x rightn1sumnolimits_m0infty p_nleft m rightxm where p_nleft x right is the polynomial of degree n are the numerator polynomials of the generating functions of diagonals of the ordinary riordan arrays generalized narayana polynomials varphi _nleft x rightleft 1x r... | [['generalized', 'euler', 'polynomials', 'alpha', '_nleft', 'x', 'rightleft', '1x', 'rightn1sumnolimits_m0infty', 'p_nleft', 'm', 'rightxm', 'where', 'p_nleft', 'x', 'right', 'is', 'the', 'polynomial', 'of', 'degree', 'n', 'are', 'the', 'numerator', 'polynomials', 'of', 'the', 'generating', 'functions', 'of', 'diagonal... | [-0.3079312262066369, 0.1508828739523652, 0.04211531534696682, 0.04618424934753559, -0.042049937759219565, -0.16901016495886106, -0.040736696407305005, 0.2992372874146964, -0.3466585162036781, -0.1591927215966832, 0.004101410488998871, -0.3402436789614443, -0.17385519990001957, 0.1005410549077618, -0.024234732565811917... |
1,803.01976 | An infinite family of congruences arising from a second order mock theta
function | Let $\beta(q)=\sum_{n\ge 0} \mathfrak{b}(n)q^n$ be a second order mock theta
function defined by $$\sum_{n\ge
0}\frac{q^{n(n+1)}(-q^2;q^2)_n}{(q;q^2)_{n+1}^2}.$$ In this paper, we obtain an
infinite family of congruences modulo powers of $3$ for $\mathfrak{b}(n)$.
| math.NT | let betaqsum_nge 0 mathfrakbnqn be a second order mock theta function defined by sum_nge 0fracqnn1q2q2_nqq2_n12 in this paper we obtain an infinite family of congruences modulo powers of 3 for mathfrakbn | [['let', 'betaqsum_nge', '0', 'mathfrakbnqn', 'be', 'a', 'second', 'order', 'mock', 'theta', 'function', 'defined', 'by', 'sum_nge', '0fracqnn1q2q2_nqq2_n12', 'in', 'this', 'paper', 'we', 'obtain', 'an', 'infinite', 'family', 'of', 'congruences', 'modulo', 'powers', 'of', '3', 'for', 'mathfrakbn']] | [-0.21851147049003178, 0.1166145694835534, -0.06663097537778041, 0.0061316510653813125, -0.07940888497978449, -0.06431229562602109, -0.029562591950202152, 0.28207864001807237, -0.33122010639420263, -0.27293451213174397, 0.0657647748745081, -0.28930852589783845, -0.13394569177008062, 0.21043150226964993, -0.017934561293... |
1,803.01977 | Advances in Synthetic Gauge Fields for Light Through Dynamic Modulation | Photons are weak particles that do not directly couple to magnetic fields.
However, it is possible to generate a photonic gauge field by breaking
reciprocity such that the phase of light depends on its direction of
propagation. This non-reciprocal phase indicates the presence of an effective
magnetic field for the li... | physics.optics | photons are weak particles that do not directly couple to magnetic fields however it is possible to generate a photonic gauge field by breaking reciprocity such that the phase of light depends on its direction of propagation this nonreciprocal phase indicates the presence of an effective magnetic field for the light it... | [['photons', 'are', 'weak', 'particles', 'that', 'do', 'not', 'directly', 'couple', 'to', 'magnetic', 'fields', 'however', 'it', 'is', 'possible', 'to', 'generate', 'a', 'photonic', 'gauge', 'field', 'by', 'breaking', 'reciprocity', 'such', 'that', 'the', 'phase', 'of', 'light', 'depends', 'on', 'its', 'direction', 'of... | [-0.1648558979378625, 0.24725497245975323, -0.056288544721125315, 0.037390249072708076, -0.13141795098781586, -0.11697110239571581, 0.0011989975881685191, 0.4093362015672028, -0.2615253715387856, -0.31252947013296456, 0.07275985204323661, -0.23523072768002748, -0.20761423589040837, 0.20442941853252705, -0.0267582137195... |
1,803.01978 | Learning Task-Specific Dynamics to Improve Whole-Body Control | In task-based inverse dynamics control, reference accelerations used to
follow a desired plan can be broken down into feedforward and feedback
trajectories. The feedback term accounts for tracking errors that are caused
from inaccurate dynamic models or external disturbances. On underactuated,
free-floating robots, s... | cs.RO | in taskbased inverse dynamics control reference accelerations used to follow a desired plan can be broken down into feedforward and feedback trajectories the feedback term accounts for tracking errors that are caused from inaccurate dynamic models or external disturbances on underactuated freefloating robots such as hu... | [['in', 'taskbased', 'inverse', 'dynamics', 'control', 'reference', 'accelerations', 'used', 'to', 'follow', 'a', 'desired', 'plan', 'can', 'be', 'broken', 'down', 'into', 'feedforward', 'and', 'feedback', 'trajectories', 'the', 'feedback', 'term', 'accounts', 'for', 'tracking', 'errors', 'that', 'are', 'caused', 'from... | [-0.08785207351648774, 0.059252162786343925, -0.06612062547594691, 0.037085245037600634, -0.15193669995149742, -0.1543956810226425, 0.06755496926534062, 0.40278876677919656, -0.2623517405814849, -0.396655247379572, 0.06657462409661653, -0.21816562607120246, -0.15921441879099568, 0.2218656027307495, -0.16100566066467228... |
1,803.01979 | A Virtual Element Method for the Transmission Eigenvalue Problem | In this paper, we analyze a virtual element method (VEM) for solving a
non-selfadjoint fourth-order eigenvalue problem derived from the transmission
eigenvalue problem. We write a variational formulation and propose a
$C^1$-conforming discretization by means of the VEM. We use the classical
approximation theory for c... | math.NA | in this paper we analyze a virtual element method vem for solving a nonselfadjoint fourthorder eigenvalue problem derived from the transmission eigenvalue problem we write a variational formulation and propose a c1conforming discretization by means of the vem we use the classical approximation theory for compact nonsel... | [['in', 'this', 'paper', 'we', 'analyze', 'a', 'virtual', 'element', 'method', 'vem', 'for', 'solving', 'a', 'nonselfadjoint', 'fourthorder', 'eigenvalue', 'problem', 'derived', 'from', 'the', 'transmission', 'eigenvalue', 'problem', 'we', 'write', 'a', 'variational', 'formulation', 'and', 'propose', 'a', 'c1conforming... | [-0.12009610392528379, -0.0022165806113201895, -0.09838506913410476, 0.09281266581146391, -0.06991789106532563, -0.09978020264203717, 0.04900806674296841, 0.34522850488105583, -0.29088080973352914, -0.2563171135146677, 0.1225621522070817, -0.28644346358415523, -0.19229646756336738, 0.19467042839545526, -0.0615438198998... |
1,803.0198 | Learning Filter Bank Sparsifying Transforms | Data is said to follow the transform (or analysis) sparsity model if it
becomes sparse when acted on by a linear operator called a sparsifying
transform. Several algorithms have been designed to learn such a transform
directly from data, and data-adaptive sparsifying transforms have demonstrated
excellent performance... | stat.ML cs.LG eess.SP | data is said to follow the transform or analysis sparsity model if it becomes sparse when acted on by a linear operator called a sparsifying transform several algorithms have been designed to learn such a transform directly from data and dataadaptive sparsifying transforms have demonstrated excellent performance in sig... | [['data', 'is', 'said', 'to', 'follow', 'the', 'transform', 'or', 'analysis', 'sparsity', 'model', 'if', 'it', 'becomes', 'sparse', 'when', 'acted', 'on', 'by', 'a', 'linear', 'operator', 'called', 'a', 'sparsifying', 'transform', 'several', 'algorithms', 'have', 'been', 'designed', 'to', 'learn', 'such', 'a', 'transfo... | [-0.012152295172755456, -0.01475621308651432, -0.13667106789029287, 0.0671891017101586, -0.15410508348433646, -0.19675088367385868, -0.031299430059971746, 0.4931602900078197, -0.3667405927902322, -0.26382393930888104, 0.1518819494560517, -0.26169326802169135, -0.2331491183060149, 0.15493825265948108, -0.109207645585637... |
1,803.01981 | An explicit form of the canonical submodule of a Drinfeld module | We define the canonical submodule of a Drinfeld module of rank greater than
one over the affine line over a finite field. (This extends the definition of
the level 1 canonical subgroup of Hattori for rank 2 with ordinary reduction.)
We give a criterion for the existence of the canonical submodule in terms of a
lift o... | math.NT | we define the canonical submodule of a drinfeld module of rank greater than one over the affine line over a finite field this extends the definition of the level 1 canonical subgroup of hattori for rank 2 with ordinary reduction we give a criterion for the existence of the canonical submodule in terms of a lift of the ... | [['we', 'define', 'the', 'canonical', 'submodule', 'of', 'a', 'drinfeld', 'module', 'of', 'rank', 'greater', 'than', 'one', 'over', 'the', 'affine', 'line', 'over', 'a', 'finite', 'field', 'this', 'extends', 'the', 'definition', 'of', 'the', 'level', '1', 'canonical', 'subgroup', 'of', 'hattori', 'for', 'rank', '2', 'w... | [-0.18578334200060648, 0.026759129077789143, -0.13862922320015028, 0.06176056968880037, -0.0725769463321592, -0.09456031635387713, -0.03003781853327289, 0.26299457519482344, -0.304870056370512, -0.22070933278236124, 0.05056391844752794, -0.20981255338057622, -0.17019225279681194, 0.21582909242815188, -0.145200384677284... |
1,803.01982 | Low-Rank Matrix Approximations with Flip-Flop Spectrum-Revealing QR
Factorization | We present Flip-Flop Spectrum-Revealing QR (Flip-Flop SRQR) factorization, a
significantly faster and more reliable variant of the QLP factorization of
Stewart, for low-rank matrix approximations. Flip-Flop SRQR uses SRQR
factorization to initialize a partial column pivoted QR factorization and then
compute a partial... | math.NA cs.NA | we present flipflop spectrumrevealing qr flipflop srqr factorization a significantly faster and more reliable variant of the qlp factorization of stewart for lowrank matrix approximations flipflop srqr uses srqr factorization to initialize a partial column pivoted qr factorization and then compute a partial lq factoriz... | [['we', 'present', 'flipflop', 'spectrumrevealing', 'qr', 'flipflop', 'srqr', 'factorization', 'a', 'significantly', 'faster', 'and', 'more', 'reliable', 'variant', 'of', 'the', 'qlp', 'factorization', 'of', 'stewart', 'for', 'lowrank', 'matrix', 'approximations', 'flipflop', 'srqr', 'uses', 'srqr', 'factorization', 't... | [-0.049320209385994934, 0.017210374714630244, -0.08343648509233062, 0.10791982377673968, -0.06555542440633781, -0.19203652629790746, 0.022749241058257704, 0.37005523127729295, -0.26897795304875843, -0.21015116154731062, 0.1551056047200127, -0.2145442241768104, -0.18067549116423595, 0.1446888049491768, -0.05343693035498... |
1,803.01983 | Surface reconstruction and charge modulation in BaFe2As2 superconducting
film | Whether or not epitaxially grown superconducting films have the same
bulk-like superconducting properties is an important concern. We report the
structure and the electronic properties of epitaxially grown Ba(Fe1-xCox)2As2
films using scanning tunneling microscopy and scanning tunneling spectroscopy
(STS). This film ... | cond-mat.supr-con | whether or not epitaxially grown superconducting films have the same bulklike superconducting properties is an important concern we report the structure and the electronic properties of epitaxially grown bafe1xcox2as2 films using scanning tunneling microscopy and scanning tunneling spectroscopy sts this film showed a d... | [['whether', 'or', 'not', 'epitaxially', 'grown', 'superconducting', 'films', 'have', 'the', 'same', 'bulklike', 'superconducting', 'properties', 'is', 'an', 'important', 'concern', 'we', 'report', 'the', 'structure', 'and', 'the', 'electronic', 'properties', 'of', 'epitaxially', 'grown', 'bafe1xcox2as2', 'films', 'usi... | [-0.14215760229398375, 0.1777474907653295, -0.10831596299439021, -0.04789617494173834, 0.011307424857564594, -0.13202567259659587, 0.08179779247046731, 0.43252743767655416, -0.2803707796837325, -0.3288629078508719, -0.018105391344136516, -0.3822042267931544, -0.12055611822389714, 0.2116022872839771, 0.04579323038620793... |
1,803.01984 | Bayesian Predictive Synthesis with Outcome-Dependent Pools | This paper reviews background and examples of Bayesian predictive synthesis
(BPS), and develops details in a subset of BPS mixture models. BPS expands on
standard Bayesian model uncertainty analysis for model mixing to provide a
broader foundation for calibrating and combining predictive densities from
multiple model... | stat.ME | this paper reviews background and examples of bayesian predictive synthesis bps and develops details in a subset of bps mixture models bps expands on standard bayesian model uncertainty analysis for model mixing to provide a broader foundation for calibrating and combining predictive densities from multiple models or o... | [['this', 'paper', 'reviews', 'background', 'and', 'examples', 'of', 'bayesian', 'predictive', 'synthesis', 'bps', 'and', 'develops', 'details', 'in', 'a', 'subset', 'of', 'bps', 'mixture', 'models', 'bps', 'expands', 'on', 'standard', 'bayesian', 'model', 'uncertainty', 'analysis', 'for', 'model', 'mixing', 'to', 'pro... | [-0.016294327596797192, 0.03463264327396005, -0.06798668467637477, 0.11949513095195394, -0.08780062177038965, -0.15044397973358709, 0.06132682066912909, 0.36885018294385397, -0.23051753598658076, -0.31577840334376744, 0.1006437129301092, -0.2494398019674896, -0.11163479908431195, 0.18537810203164862, -0.095058807223075... |
1,803.01985 | Evidence of Gate-Tunable Mott Insulator in Trilayer Graphene-Boron
Nitride Moir\'e Superlattice | Mott insulator plays a central role in strongly correlated physics, where the
repulsive Coulomb interaction dominates over the electron kinetic energy and
leads to insulating states with one electron occupying each unit cell. Doped
Mott insulator is often described by the Hubbard model3, which can give rise to
other ... | cond-mat.mes-hall cond-mat.mtrl-sci cond-mat.str-el | mott insulator plays a central role in strongly correlated physics where the repulsive coulomb interaction dominates over the electron kinetic energy and leads to insulating states with one electron occupying each unit cell doped mott insulator is often described by the hubbard model3 which can give rise to other corre... | [['mott', 'insulator', 'plays', 'a', 'central', 'role', 'in', 'strongly', 'correlated', 'physics', 'where', 'the', 'repulsive', 'coulomb', 'interaction', 'dominates', 'over', 'the', 'electron', 'kinetic', 'energy', 'and', 'leads', 'to', 'insulating', 'states', 'with', 'one', 'electron', 'occupying', 'each', 'unit', 'ce... | [-0.18683362532187295, 0.27064153191849133, 0.003830849166439797, 0.05532891252941421, -0.005335254859779212, -0.26996587721407694, 0.1099332950220963, 0.4123999093509234, -0.2824023123307342, -0.31368086701921755, -0.0781981908142469, -0.3527408970157138, -0.1516373034079179, 0.14802639477202592, 0.046403943095356226,... |
1,803.01986 | Reservoir-engineered entanglement in a hybrid modulated three-mode
optomechanical system | We propose an effective approach for generating highly pure and strong
cavity-mechanical entanglement (or optical-microwave entanglement) in a hybrid
modulated three-mode optomechanical system. By applying two-tone driving to the
cavity and modulating the coupling strength between two mechanical oscillators
(or betwe... | quant-ph | we propose an effective approach for generating highly pure and strong cavitymechanical entanglement or opticalmicrowave entanglement in a hybrid modulated threemode optomechanical system by applying twotone driving to the cavity and modulating the coupling strength between two mechanical oscillators or between a mecha... | [['we', 'propose', 'an', 'effective', 'approach', 'for', 'generating', 'highly', 'pure', 'and', 'strong', 'cavitymechanical', 'entanglement', 'or', 'opticalmicrowave', 'entanglement', 'in', 'a', 'hybrid', 'modulated', 'threemode', 'optomechanical', 'system', 'by', 'applying', 'twotone', 'driving', 'to', 'the', 'cavity'... | [-0.20125420326803578, 0.26408318661242447, -0.057563215052596206, -0.013060236083902055, 0.01841006550603197, -0.1985145835824369, 0.05186246736502653, 0.38384129364567343, -0.2429698397318134, -0.24330342128814664, 0.0188573292680303, -0.2682548260563635, -0.13065153119168826, 0.2141236998977547, 0.01880829883430124,... |
1,803.01987 | Odoni's conjecture for number fields | Let $K$ be a number field, and let $d\geq 2$. A conjecture of Odoni (stated
more generally for characteristic zero Hilbertian fields $K$) posits that there
is a monic polynomial $f\in K[x]$ of degree $d$, and a point $x_0\in K$, such
that for every $n\geq 0$, the so-called arboreal Galois group
$Gal(K(f^{-n}(x_0))/K)... | math.NT math.DS | let k be a number field and let dgeq 2 a conjecture of odoni stated more generally for characteristic zero hilbertian fields k posits that there is a monic polynomial fin kx of degree d and a point x_0in k such that for every ngeq 0 the socalled arboreal galois group galkfnx_0k is an nfold wreath product of the symmetr... | [['let', 'k', 'be', 'a', 'number', 'field', 'and', 'let', 'dgeq', '2', 'a', 'conjecture', 'of', 'odoni', 'stated', 'more', 'generally', 'for', 'characteristic', 'zero', 'hilbertian', 'fields', 'k', 'posits', 'that', 'there', 'is', 'a', 'monic', 'polynomial', 'fin', 'kx', 'of', 'degree', 'd', 'and', 'a', 'point', 'x_0in... | [-0.27754030037730204, 0.17837638209136364, -0.09485969915129673, -0.019820523674428547, -0.05170015240323612, -0.2252127626889396, -0.053917964084084606, 0.32610346916420707, -0.31790763709223135, -0.1972636060692884, 0.06080039853267586, -0.25528728827598623, -0.13354369972821797, 0.17454724979383507, -0.067356337766... |
1,803.01988 | Global weak solutions for the three-dimensional chemotaxis-Navier-Stokes
system with slow $p$-Laplacian diffusion | This paper investigates an incompressible chemotaxis-Navier-Stokes system
with slow $p$-Laplacian diffusion \begin{eqnarray} \left\{\begin{array}{lll}
n_t+u\cdot\nabla n=\nabla\cdot(|\nabla n|^{p-2}\nabla
n)-\nabla\cdot(n\chi(c)\nabla c),& x\in\Omega,\ t>0, c_t+u\cdot\nabla c=\Delta
c-nf(c),& x\in\Omega,\ t>0, u_t+(u... | math.AP | this paper investigates an incompressible chemotaxisnavierstokes system with slow plaplacian diffusion begineqnarray leftbeginarraylll n_tucdotnabla nnablacdotnabla np2nabla nnablacdotnchicnabla c xinomega t0 c_tucdotnabla cdelta cnfc xinomega t0 u_tucdotnabla udelta unabla pnnablaphi xinomega t0 nablacdot u0 xinomega ... | [['this', 'paper', 'investigates', 'an', 'incompressible', 'chemotaxisnavierstokes', 'system', 'with', 'slow', 'plaplacian', 'diffusion', 'begineqnarray', 'leftbeginarraylll', 'n_tucdotnabla', 'nnablacdotnabla', 'np2nabla', 'nnablacdotnchicnabla', 'c', 'xinomega', 't0', 'c_tucdotnabla', 'cdelta', 'cnfc', 'xinomega', 't... | [-0.24442851980395539, 0.07019069641396389, 0.013452979016371748, -0.057186989257149774, -0.07245203581693901, -0.3301188232132582, -0.10457221777860376, 0.35471592435020616, -0.3281677174428948, -0.0020890835616173167, 0.19461713471059508, -0.4146589278196446, -0.006220102695291956, 0.12392678921995214, -0.05313374909... |
1,803.01989 | Relaxed highest-weight modules I: rank $1$ cases | Relaxed highest-weight modules play a central role in the study of many
important vertex operator (super)algebras and their associated (logarithmic)
conformal field theories, including the admissible-level affine models. Indeed,
their structure and their (super)characters together form the crucial input
data for the ... | math.RT hep-th math-ph math.MP math.QA | relaxed highestweight modules play a central role in the study of many important vertex operator superalgebras and their associated logarithmic conformal field theories including the admissiblelevel affine models indeed their structure and their supercharacters together form the crucial input data for the standard modu... | [['relaxed', 'highestweight', 'modules', 'play', 'a', 'central', 'role', 'in', 'the', 'study', 'of', 'many', 'important', 'vertex', 'operator', 'superalgebras', 'and', 'their', 'associated', 'logarithmic', 'conformal', 'field', 'theories', 'including', 'the', 'admissiblelevel', 'affine', 'models', 'indeed', 'their', 's... | [-0.14743932804558427, 0.08344695535615756, -0.0540199280968712, 0.11815033049982351, -0.1056597916292958, -0.17313466265720004, -0.049789604372684454, 0.358172656254222, -0.33206014716997745, -0.21581897409632803, 0.09563432730210479, -0.20896093980409206, -0.16881579610441502, 0.19492205984036748, -0.0954796920258862... |
1,803.0199 | The distance sum rule from strong lensing systems and quasars - test of
cosmic curvature and beyond | Testing the distance-sum-rule in strong lensing systems provides an
interesting method to determine the curvature parameter $\Omega_k$ using more
local objects. In this paper, we apply this method to a quite recent data set
of strong lensing systems in combination with intermediate-luminosity quasars
calibrated as st... | astro-ph.CO gr-qc | testing the distancesumrule in strong lensing systems provides an interesting method to determine the curvature parameter omega_k using more local objects in this paper we apply this method to a quite recent data set of strong lensing systems in combination with intermediateluminosity quasars calibrated as standard rul... | [['testing', 'the', 'distancesumrule', 'in', 'strong', 'lensing', 'systems', 'provides', 'an', 'interesting', 'method', 'to', 'determine', 'the', 'curvature', 'parameter', 'omega_k', 'using', 'more', 'local', 'objects', 'in', 'this', 'paper', 'we', 'apply', 'this', 'method', 'to', 'a', 'quite', 'recent', 'data', 'set',... | [-0.09056323330710117, 0.044401534667414484, -0.09727290991335846, 0.11397041105329746, -0.11743230260522247, -0.1270254977084554, -0.008556177322630766, 0.4103741833541591, -0.19203887903843253, -0.34693668563962066, 0.07050724100122252, -0.28430483686660446, -0.09496560011884629, 0.2516683208131878, -0.03491219714122... |
1,803.01991 | Breaking the spectral degeneracies in black hole binaries with fast
timing data | The spectra of black hole binaries in the low/hard state are complex, with
evidence for multiple different Comptonisation regions contributing to the hard
X-rays in addition to a cool disc component. We show this explicitly for some
of the best RXTE data from Cyg X-1, where the spectrum strongly requires (at
least) t... | astro-ph.HE | the spectra of black hole binaries in the lowhard state are complex with evidence for multiple different comptonisation regions contributing to the hard xrays in addition to a cool disc component we show this explicitly for some of the best rxte data from cyg x1 where the spectrum strongly requires at least two differe... | [['the', 'spectra', 'of', 'black', 'hole', 'binaries', 'in', 'the', 'lowhard', 'state', 'are', 'complex', 'with', 'evidence', 'for', 'multiple', 'different', 'comptonisation', 'regions', 'contributing', 'to', 'the', 'hard', 'xrays', 'in', 'addition', 'to', 'a', 'cool', 'disc', 'component', 'we', 'show', 'this', 'explic... | [-0.03651115300377742, 0.14809409806593543, -0.08020032870228447, 0.11710804964448991, -0.09620615415984676, -0.09903897739547704, 0.007266557997181302, 0.4367462691363125, -0.2544370982441164, -0.3300057658792606, 0.09561887971469246, -0.3157310178896989, 0.001931421443199118, 0.19394393876150606, -0.03183609714795325... |
1,803.01992 | All-dielectric active photonics driven by bound states in the continuum | Recently emerged dielectric resonators and metasurfaces offer a low-loss
platform for efficient manipulation of electromagnetic waves from microwave to
visible. Such flat meta-optics can focus electromagnetic waves, generate
structured beams and vortices, enhance local fields for sensing as well as
provide additional... | physics.optics | recently emerged dielectric resonators and metasurfaces offer a lowloss platform for efficient manipulation of electromagnetic waves from microwave to visible such flat metaoptics can focus electromagnetic waves generate structured beams and vortices enhance local fields for sensing as well as provide additional functi... | [['recently', 'emerged', 'dielectric', 'resonators', 'and', 'metasurfaces', 'offer', 'a', 'lowloss', 'platform', 'for', 'efficient', 'manipulation', 'of', 'electromagnetic', 'waves', 'from', 'microwave', 'to', 'visible', 'such', 'flat', 'metaoptics', 'can', 'focus', 'electromagnetic', 'waves', 'generate', 'structured',... | [-0.1459390817918353, 0.2195108412353355, -0.05780901330984941, 0.006409529559392513, -0.134747384879112, -0.20146079970124578, -0.0002244701687277866, 0.4981614031492412, -0.21742008067667484, -0.3092790906104267, 0.0903752795518415, -0.23527253101415493, -0.19724242004151105, 0.2773779498241028, -0.000711317755234967... |
1,803.01993 | Inconsistencies in the Electronic Properties of Phosphorene Nanotubes:
New Insights from Large-Scale DFT Calculations | Contrary to recent reports, we show that the electronic properties of
phosphorene nanotubes are surprisingly rich and much more complex than
previously assumed. We find that all phosphorene nanotubes exhibit an intricate
direct-to-indirect bandgap transition as the nanotube diameter decreases - a
unique property not ... | cond-mat.mes-hall cond-mat.mtrl-sci physics.chem-ph | contrary to recent reports we show that the electronic properties of phosphorene nanotubes are surprisingly rich and much more complex than previously assumed we find that all phosphorene nanotubes exhibit an intricate directtoindirect bandgap transition as the nanotube diameter decreases a unique property not identifi... | [['contrary', 'to', 'recent', 'reports', 'we', 'show', 'that', 'the', 'electronic', 'properties', 'of', 'phosphorene', 'nanotubes', 'are', 'surprisingly', 'rich', 'and', 'much', 'more', 'complex', 'than', 'previously', 'assumed', 'we', 'find', 'that', 'all', 'phosphorene', 'nanotubes', 'exhibit', 'an', 'intricate', 'di... | [-0.12502848027817284, 0.07857444383145776, -0.05870336363906972, 0.02886076203081757, -0.0665118618371586, -0.12660108348354698, 0.11612908202533921, 0.4816410630941391, -0.23951165519111478, -0.31691112304416796, 0.02195282079046592, -0.33167859217268414, -0.210784432447205, 0.1858217266186451, 0.01808150946162641, 0... |
1,803.01994 | Halogen Bonding Interactions: Revised Benchmarks and a New Assessment of
Exchange vs. Dispersion | We present a new analysis of exchange and dispersion effects for calculating
halogen-bonding interactions in a wide variety of complex dimers (69 total)
within the XB18 and XB51 benchmark sets. Contrary to previous work on these
systems, we find that dispersion plays a more significant role than exact
exchange in acc... | physics.chem-ph physics.atm-clus | we present a new analysis of exchange and dispersion effects for calculating halogenbonding interactions in a wide variety of complex dimers 69 total within the xb18 and xb51 benchmark sets contrary to previous work on these systems we find that dispersion plays a more significant role than exact exchange in accurately... | [['we', 'present', 'a', 'new', 'analysis', 'of', 'exchange', 'and', 'dispersion', 'effects', 'for', 'calculating', 'halogenbonding', 'interactions', 'in', 'a', 'wide', 'variety', 'of', 'complex', 'dimers', '69', 'total', 'within', 'the', 'xb18', 'and', 'xb51', 'benchmark', 'sets', 'contrary', 'to', 'previous', 'work', ... | [-0.08242202078269974, 0.060270273145684464, -0.06644011769339958, 0.1155481187203136, -0.034314194304240216, -0.09888682174440248, 0.06048833132729899, 0.39568041607243826, -0.19417821258833878, -0.3748082423397531, 0.019774889072728712, -0.3031373118521668, -0.15094660177647348, 0.22890550532540957, -0.00673979174216... |
1,803.01995 | Unusual Bandgap Oscillations in Template-Directed {\pi}-Conjugated
Porphyrin Nanotubes | Using large-scale DFT calculations (up to 1,476 atoms and 18,432 orbitals),
we present the first detailed analysis on the unusual electronic properties of
recently synthesized porphyrin nanotubes. We surprisingly observe extremely
large oscillations in the bandgap of these nanostructures as a function of
size, in con... | cond-mat.mes-hall cond-mat.mtrl-sci physics.chem-ph | using largescale dft calculations up to 1476 atoms and 18432 orbitals we present the first detailed analysis on the unusual electronic properties of recently synthesized porphyrin nanotubes we surprisingly observe extremely large oscillations in the bandgap of these nanostructures as a function of size in contradiction... | [['using', 'largescale', 'dft', 'calculations', 'up', 'to', '1476', 'atoms', 'and', '18432', 'orbitals', 'we', 'present', 'the', 'first', 'detailed', 'analysis', 'on', 'the', 'unusual', 'electronic', 'properties', 'of', 'recently', 'synthesized', 'porphyrin', 'nanotubes', 'we', 'surprisingly', 'observe', 'extremely', '... | [-0.12046035754457607, 0.15026919993473903, -0.03750514918570652, 0.03372427935698254, -0.006154179266702972, -0.1320853137907474, 0.10131959149332129, 0.4952781726851275, -0.2599427139142982, -0.3049879919072785, -0.00391373495796487, -0.3085740243745692, -0.18439547395897343, 0.17309794008983054, 0.022784343939795355... |
1,803.01996 | The Importance of Short- and Long-Range Exchange on Various Excited
State Properties of DNA Monomers, Stacked Complexes, and Watson-Crick Pairs | We present a detailed analysis of several time-dependent DFT (TD-DFT)
methods, including conventional hybrid functionals and two types of
non-empirically tuned range-separated functionals, for predicting a diverse set
of electronic excitations in DNA nucleobase monomers and dimers. This large and
extensive set of exc... | physics.chem-ph physics.atm-clus physics.bio-ph | we present a detailed analysis of several timedependent dft tddft methods including conventional hybrid functionals and two types of nonempirically tuned rangeseparated functionals for predicting a diverse set of electronic excitations in dna nucleobase monomers and dimers this large and extensive set of excitations co... | [['we', 'present', 'a', 'detailed', 'analysis', 'of', 'several', 'timedependent', 'dft', 'tddft', 'methods', 'including', 'conventional', 'hybrid', 'functionals', 'and', 'two', 'types', 'of', 'nonempirically', 'tuned', 'rangeseparated', 'functionals', 'for', 'predicting', 'a', 'diverse', 'set', 'of', 'electronic', 'exc... | [-0.12509517315284988, 0.14047163981625713, -0.026135471273262642, 0.13357808442286975, 0.017144096963793824, -0.14098934502536922, 0.06294536468768983, 0.3753036920177309, -0.23079173316456084, -0.30934968138799857, -0.050991230166370145, -0.35984602808396293, -0.13309475532610363, 0.13495127396890894, 0.0672070324091... |
1,803.01997 | Mathematical modeling and analysis of the pathway network consisting of
symmetrical complexes with N monomers, like the activation of MMP2 | The activation of matrix metalloproteinase 2 (MMP2) is a crucial event during
tumor metastasis and invasion, and this pathway network consists of 3 monomers.
The pathway network of the activation obeys to a set of specified reaction
rules. According to the rules, the individual molecules localize in a
particular orde... | q-bio.BM q-bio.MN | the activation of matrix metalloproteinase 2 mmp2 is a crucial event during tumor metastasis and invasion and this pathway network consists of 3 monomers the pathway network of the activation obeys to a set of specified reaction rules according to the rules the individual molecules localize in a particular order and sy... | [['the', 'activation', 'of', 'matrix', 'metalloproteinase', '2', 'mmp2', 'is', 'a', 'crucial', 'event', 'during', 'tumor', 'metastasis', 'and', 'invasion', 'and', 'this', 'pathway', 'network', 'consists', 'of', '3', 'monomers', 'the', 'pathway', 'network', 'of', 'the', 'activation', 'obeys', 'to', 'a', 'set', 'of', 'sp... | [-0.09578389634392509, 0.08370184243362093, -0.05739291458154853, 0.025837367102361227, -0.03654102796013942, -0.14493630041976516, 0.11094917190185159, 0.3560187361887371, -0.28503376448096956, -0.2741285828956372, 0.017217429024547492, -0.25092272058471426, -0.20697570615091684, 0.09649471104102285, -0.01687460747186... |
1,803.01998 | Dwarf irregular galaxies with extended HI gas disks: Suppression of
small-scale spiral structure by dark matter halo | Dwarf irregular galaxies with extended HI disk distributions, such as DDO
154, allow measurement of rotation curves, hence deduction of dark matter halo
properties to large radial distances, up to several times the optical radius.
These galaxies contain a huge reservoir of dark matter halo, which dominates
over most ... | astro-ph.GA | dwarf irregular galaxies with extended hi disk distributions such as ddo 154 allow measurement of rotation curves hence deduction of dark matter halo properties to large radial distances up to several times the optical radius these galaxies contain a huge reservoir of dark matter halo which dominates over most of disk ... | [['dwarf', 'irregular', 'galaxies', 'with', 'extended', 'hi', 'disk', 'distributions', 'such', 'as', 'ddo', '154', 'allow', 'measurement', 'of', 'rotation', 'curves', 'hence', 'deduction', 'of', 'dark', 'matter', 'halo', 'properties', 'to', 'large', 'radial', 'distances', 'up', 'to', 'several', 'times', 'the', 'optical... | [-0.12411474792148977, 0.07363429008406339, -0.12711532213276577, 0.10547506985085837, -0.12658238893699483, -0.03135563411168891, -0.03274471034646171, 0.3910089000170931, -0.1577866824857523, -0.3568970119461007, 0.02654527169823168, -0.2359969182925351, -0.05011831029583145, 0.18524081165552003, -0.00727237156942623... |
1,803.01999 | ABC and Indirect Inference | This chapter will appear in the forthcoming Handbook of Approximate Bayesian
Computation (2018).
Indirect inference (II) is a classical likelihood-free approach that
pre-dates the main developments of ABC and relies on simulation from a
parametric model of interest to determine point estimates of the parameters. It... | stat.CO stat.ME | this chapter will appear in the forthcoming handbook of approximate bayesian computation 2018 indirect inference ii is a classical likelihoodfree approach that predates the main developments of abc and relies on simulation from a parametric model of interest to determine point estimates of the parameters it is not surp... | [['this', 'chapter', 'will', 'appear', 'in', 'the', 'forthcoming', 'handbook', 'of', 'approximate', 'bayesian', 'computation', '2018', 'indirect', 'inference', 'ii', 'is', 'a', 'classical', 'likelihoodfree', 'approach', 'that', 'predates', 'the', 'main', 'developments', 'of', 'abc', 'and', 'relies', 'on', 'simulation',... | [-0.02311931569350972, -0.025660080986701705, -0.084326178802266, 0.0863972779951014, -0.14064416246754782, -0.15515131940788013, 0.06633793468631449, 0.3598084717988968, -0.26118104480916543, -0.32788122840935274, 0.12685089395048896, -0.21956448803345363, -0.19602910212817645, 0.18715074493860204, -0.0910334142676133... |
1,803.02 | Indirect strong coupling regime between a quantum dot and a nanocavity
mediated by a mechanical resonator | Achieving strong coupling between light and matter is usually a challenge in
Cavity Quantum Electrodynamics (cQED), especially in solid state systems. For
this reason is useful taking advantage of alternative approaches to reach this
regime, and then, generate reliable quantum polaritons. In this work we study a
syst... | cond-mat.mes-hall quant-ph | achieving strong coupling between light and matter is usually a challenge in cavity quantum electrodynamics cqed especially in solid state systems for this reason is useful taking advantage of alternative approaches to reach this regime and then generate reliable quantum polaritons in this work we study a system compos... | [['achieving', 'strong', 'coupling', 'between', 'light', 'and', 'matter', 'is', 'usually', 'a', 'challenge', 'in', 'cavity', 'quantum', 'electrodynamics', 'cqed', 'especially', 'in', 'solid', 'state', 'systems', 'for', 'this', 'reason', 'is', 'useful', 'taking', 'advantage', 'of', 'alternative', 'approaches', 'to', 're... | [-0.1570304477767598, 0.15815978521050544, -0.06340827308194612, 0.015445295651192946, -0.01855173446012721, -0.21162146143114535, 0.05550528833797822, 0.3707410409265468, -0.23162857845916301, -0.2940207632403741, -0.01138605293379696, -0.2877827031658061, -0.13364567808551533, 0.2193669365125618, 0.022656453508002463... |
1,803.02001 | Quantum criticality in the metal-superconductor transition of
interacting Dirac fermions on a triangular lattice | We investigate a semimetal-superconductor phase transition of two-dimensional
Dirac electrons at zero temperature by large-scale and essentially unbiased
quantum Monte Carlo simulations for the half-filled attractive Hubbard model on
the triangular lattice, in the presence of alternating magnetic $\pi$-flux,
that is ... | cond-mat.str-el hep-lat | we investigate a semimetalsuperconductor phase transition of twodimensional dirac electrons at zero temperature by largescale and essentially unbiased quantum monte carlo simulations for the halffilled attractive hubbard model on the triangular lattice in the presence of alternating magnetic piflux that is introduced t... | [['we', 'investigate', 'a', 'semimetalsuperconductor', 'phase', 'transition', 'of', 'twodimensional', 'dirac', 'electrons', 'at', 'zero', 'temperature', 'by', 'largescale', 'and', 'essentially', 'unbiased', 'quantum', 'monte', 'carlo', 'simulations', 'for', 'the', 'halffilled', 'attractive', 'hubbard', 'model', 'on', '... | [-0.14987306390888988, 0.2109233545213439, -0.05601193540197398, 0.0618988777929917, -0.018042932434805804, -0.13744985778416907, 0.09385560180725797, 0.34234490160032044, -0.20781597123082196, -0.2773065027062382, -0.0070621403073892, -0.33257050492501417, -0.13523699254462762, 0.08788936259624149, 0.05782886767493827... |
1,803.02002 | Refrigeration beyond weak internal coupling | We investigate the performance of a three-spin quantum absorption
refrigerator using a refined open quantum system model valid across all
inter-spin coupling strengths. It describes the transition between previous
approximate models for the weak and the ultrastrong coupling limit, and it
predicts optimal refrigeratio... | quant-ph | we investigate the performance of a threespin quantum absorption refrigerator using a refined open quantum system model valid across all interspin coupling strengths it describes the transition between previous approximate models for the weak and the ultrastrong coupling limit and it predicts optimal refrigeration for ... | [['we', 'investigate', 'the', 'performance', 'of', 'a', 'threespin', 'quantum', 'absorption', 'refrigerator', 'using', 'a', 'refined', 'open', 'quantum', 'system', 'model', 'valid', 'across', 'all', 'interspin', 'coupling', 'strengths', 'it', 'describes', 'the', 'transition', 'between', 'previous', 'approximate', 'mode... | [-0.1990543368816922, 0.1829476164779941, -0.01810912422781558, 0.101188914962393, -0.04562980708091947, -0.21581987071698322, 0.11504949929885902, 0.3560201276681925, -0.2550473611178647, -0.28691710144477456, 0.010858057836189698, -0.2813329595260154, -0.0811161263040582, 0.20512696581584564, 0.08370189941173098, -0.... |
1,803.02003 | Towards high-capacity quantum communications by combining wavelength-
and time-division multiplexing technologies | Optical communication systems are able to send the information from one user
to another in light beams that travel through the free space or optical fibers,
therefore how to send larger amounts of information in smaller periods of time
is a long term concern, one promising way is to use multiplexing of photon's
diffe... | quant-ph physics.optics | optical communication systems are able to send the information from one user to another in light beams that travel through the free space or optical fibers therefore how to send larger amounts of information in smaller periods of time is a long term concern one promising way is to use multiplexing of photons different ... | [['optical', 'communication', 'systems', 'are', 'able', 'to', 'send', 'the', 'information', 'from', 'one', 'user', 'to', 'another', 'in', 'light', 'beams', 'that', 'travel', 'through', 'the', 'free', 'space', 'or', 'optical', 'fibers', 'therefore', 'how', 'to', 'send', 'larger', 'amounts', 'of', 'information', 'in', 's... | [-0.16707488868658424, 0.19560361219048025, -0.06336651220146543, -0.008548153641449797, -0.05203052365612595, -0.23204706913856848, 0.09667589961236735, 0.4115362909094543, -0.2892551840383821, -0.30938898938097015, 0.05531420013392759, -0.2871678477684466, -0.021604244184982815, 0.22168342121817455, -0.05111060418473... |
1,803.02004 | Enhancement of steady-state bosonic squeezing and entanglement in a
dissipative optomechanical system | We systematically study the influence of amplitude modulation on the
steady-state bosonic squeezing and entanglement in a dissipative three-mode
optomechanical system, where a vibrational mode of the membrane is coupled to
the left and right cavity modes via the radiation pressure. Numerical
simulation results show t... | quant-ph | we systematically study the influence of amplitude modulation on the steadystate bosonic squeezing and entanglement in a dissipative threemode optomechanical system where a vibrational mode of the membrane is coupled to the left and right cavity modes via the radiation pressure numerical simulation results show that th... | [['we', 'systematically', 'study', 'the', 'influence', 'of', 'amplitude', 'modulation', 'on', 'the', 'steadystate', 'bosonic', 'squeezing', 'and', 'entanglement', 'in', 'a', 'dissipative', 'threemode', 'optomechanical', 'system', 'where', 'a', 'vibrational', 'mode', 'of', 'the', 'membrane', 'is', 'coupled', 'to', 'the'... | [-0.19835504988529437, 0.2276687258845689, -0.047335836090055775, 0.008037026079943065, -0.013577864216076154, -0.19412953520165474, 0.05764929081091064, 0.401132799917832, -0.2593643107437388, -0.24750839137105327, 0.10194036785855354, -0.2331353095042604, -0.13649214377492722, 0.25040615143811784, -0.0092281686198530... |
1,803.02005 | On the Early In Situ Formation of Pluto's Small Satellites | The formation of Pluto's small satellites - Styx, Nix, Keberos and Hydra -
remains a mystery. Their orbits are nearly circular and are near mean-motion
resonances and nearly coplanar with Charon's orbit. One scenario suggests that
they all formed close to their current locations from a disk of debris that was
ejected... | astro-ph.EP | the formation of plutos small satellites styx nix keberos and hydra remains a mystery their orbits are nearly circular and are near meanmotion resonances and nearly coplanar with charons orbit one scenario suggests that they all formed close to their current locations from a disk of debris that was ejected from the cha... | [['the', 'formation', 'of', 'plutos', 'small', 'satellites', 'styx', 'nix', 'keberos', 'and', 'hydra', 'remains', 'a', 'mystery', 'their', 'orbits', 'are', 'nearly', 'circular', 'and', 'are', 'near', 'meanmotion', 'resonances', 'and', 'nearly', 'coplanar', 'with', 'charons', 'orbit', 'one', 'scenario', 'suggests', 'tha... | [-0.14879035007721636, 0.19041945179995196, -0.07133365811499874, 0.07807556635224203, -0.030286201302670932, -0.07263449905131145, 0.007052040368368009, 0.33076524108945005, -0.20704644004633008, -0.3860813651699573, 0.0708278993400127, -0.2914046048046609, -0.03966934819689301, 0.1899978894739313, -0.0358981063725443... |
1,803.02006 | Galois covers of graphs and embedded topology of plane curves | The splitting number is effective to distinguish the embedded topology of
plane curves, and it is not determined by the fundamental group of the
complement of the plane curve. In this paper, we give a generalization of the
splitting number, called the splitting graph. By using the splitting graph, we
classify the emb... | math.AG math.GT | the splitting number is effective to distinguish the embedded topology of plane curves and it is not determined by the fundamental group of the complement of the plane curve in this paper we give a generalization of the splitting number called the splitting graph by using the splitting graph we classify the embedded to... | [['the', 'splitting', 'number', 'is', 'effective', 'to', 'distinguish', 'the', 'embedded', 'topology', 'of', 'plane', 'curves', 'and', 'it', 'is', 'not', 'determined', 'by', 'the', 'fundamental', 'group', 'of', 'the', 'complement', 'of', 'the', 'plane', 'curve', 'in', 'this', 'paper', 'we', 'give', 'a', 'generalization... | [-0.2462270202898029, 0.05665278683106104, -0.07940023916139119, 0.05198090410946558, -0.1086280770815801, -0.08659924282624885, 0.043763900163880404, 0.3487704841123111, -0.2906052960973719, -0.30818295705577603, 0.0875891687169644, -0.2476511460499487, -0.1531824651511683, 0.21316676923627223, -0.07153778367986281, -... |
1,803.02007 | Occupancy Map Prediction Using Generative and Fully Convolutional
Networks for Vehicle Navigation | Fast, collision-free motion through unknown environments remains a
challenging problem for robotic systems. In these situations, the robot's
ability to reason about its future motion is often severely limited by sensor
field of view (FOV). By contrast, biological systems routinely make decisions
by taking into consid... | cs.LG cs.CV cs.RO | fast collisionfree motion through unknown environments remains a challenging problem for robotic systems in these situations the robots ability to reason about its future motion is often severely limited by sensor field of view fov by contrast biological systems routinely make decisions by taking into consideration wha... | [['fast', 'collisionfree', 'motion', 'through', 'unknown', 'environments', 'remains', 'a', 'challenging', 'problem', 'for', 'robotic', 'systems', 'in', 'these', 'situations', 'the', 'robots', 'ability', 'to', 'reason', 'about', 'its', 'future', 'motion', 'is', 'often', 'severely', 'limited', 'by', 'sensor', 'field', 'o... | [-0.08817122742805063, 0.03877158322156059, -0.056435272603338915, 0.05690122672991938, -0.11058975035472718, -0.1535497636484932, 0.06074173524374426, 0.5107982261044695, -0.2543811264354581, -0.36872602489450024, 0.07717502664848669, -0.2354939974463215, -0.21243608584750864, 0.22686101477099768, -0.14481242301732006... |
1,803.02008 | Planetary Spectrum Generator: an accurate online radiative transfer
suite for atmospheres, comets, small bodies and exoplanets | We have developed an online radiative-transfer suite
(https://psg.gsfc.nasa.gov) applicable to a broad range of planetary objects
(e.g., planets, moons, comets, asteroids, TNOs, KBOs, exoplanets). The
Planetary Spectrum Generator (PSG) can synthesize planetary spectra
(atmospheres and surfaces) for a broad range of w... | astro-ph.EP | we have developed an online radiativetransfer suite httpspsggsfcnasagov applicable to a broad range of planetary objects eg planets moons comets asteroids tnos kbos exoplanets the planetary spectrum generator psg can synthesize planetary spectra atmospheres and surfaces for a broad range of wavelengths uvvisnearirirfar... | [['we', 'have', 'developed', 'an', 'online', 'radiativetransfer', 'suite', 'httpspsggsfcnasagov', 'applicable', 'to', 'a', 'broad', 'range', 'of', 'planetary', 'objects', 'eg', 'planets', 'moons', 'comets', 'asteroids', 'tnos', 'kbos', 'exoplanets', 'the', 'planetary', 'spectrum', 'generator', 'psg', 'can', 'synthesize... | [-0.05100425848442163, 0.09239884073414421, -0.06488253660271377, 0.06192172145737069, -0.10543112776784776, -0.12647804310381616, 0.007043359526765666, 0.39065608092226156, -0.18763265640726395, -0.39529126122943126, 0.10837135968488708, -0.3058124048257014, -0.08450138979294154, 0.28824806425317157, -0.06790168756898... |
1,803.02009 | MIS-SLAM: Real-time Large Scale Dense Deformable SLAM System in Minimal
Invasive Surgery Based on Heterogeneous Computing | Real-time simultaneously localization and dense mapping is very helpful for
providing Virtual Reality and Augmented Reality for surgeons or even surgical
robots. In this paper, we propose MIS-SLAM: a complete real-time large scale
dense deformable SLAM system with stereoscope in Minimal Invasive Surgery based
on hete... | cs.CV | realtime simultaneously localization and dense mapping is very helpful for providing virtual reality and augmented reality for surgeons or even surgical robots in this paper we propose misslam a complete realtime large scale dense deformable slam system with stereoscope in minimal invasive surgery based on heterogeneou... | [['realtime', 'simultaneously', 'localization', 'and', 'dense', 'mapping', 'is', 'very', 'helpful', 'for', 'providing', 'virtual', 'reality', 'and', 'augmented', 'reality', 'for', 'surgeons', 'or', 'even', 'surgical', 'robots', 'in', 'this', 'paper', 'we', 'propose', 'misslam', 'a', 'complete', 'realtime', 'large', 'sc... | [-0.0862451905444745, 0.010880626215329094, -0.03057852177129638, 0.028297355163827417, -0.10739130698925545, -0.1983010417000661, 0.01722402201680046, 0.4507530984048161, -0.24181527301609035, -0.339156519964097, 0.13261521091429337, -0.214563369282311, -0.1411324530794856, 0.22516596857007712, -0.15795018658522636, 0... |
1,803.0201 | Strain-tunable charge carrier mobility of atomically thin phosphorus
allotropes | We explore the impact of strain on charge carrier mobility of monolayer
$\alpha$, $\beta$, $\gamma$ and $\delta$-P, the four well known atomically thin
allotropes of phosphorus, using density functional theory. Owing to the highly
anisotropic band dispersion, the charge carrier mobility of the pristine
allotropes is ... | cond-mat.mtrl-sci | we explore the impact of strain on charge carrier mobility of monolayer alpha beta gamma and deltap the four well known atomically thin allotropes of phosphorus using density functional theory owing to the highly anisotropic band dispersion the charge carrier mobility of the pristine allotropes is significantly higher ... | [['we', 'explore', 'the', 'impact', 'of', 'strain', 'on', 'charge', 'carrier', 'mobility', 'of', 'monolayer', 'alpha', 'beta', 'gamma', 'and', 'deltap', 'the', 'four', 'well', 'known', 'atomically', 'thin', 'allotropes', 'of', 'phosphorus', 'using', 'density', 'functional', 'theory', 'owing', 'to', 'the', 'highly', 'an... | [-0.1540396274009254, 0.17767776208218292, 0.010513072773917682, -0.031665011677089044, -0.004123411102530857, -0.15212672144795458, 0.09249055507178935, 0.472167771609707, -0.28072590673497566, -0.27285491182572313, -0.004685283553812446, -0.3108089560228917, -0.11855952571948163, 0.177973044774909, 0.0348815426282170... |
1,803.02011 | A Lower Bound for the Cardinality of Function Basis of Tensor Invariants | In this article, we give a proof for that the cardinality of a function basis
of the invariants for a finite dimensional real vector space by a compact group
is lower bounded by the intuitive difference of the dimensions of the vector
space and the group. An application is given to the space of third order three
dime... | math.AG | in this article we give a proof for that the cardinality of a function basis of the invariants for a finite dimensional real vector space by a compact group is lower bounded by the intuitive difference of the dimensions of the vector space and the group an application is given to the space of third order three dimensio... | [['in', 'this', 'article', 'we', 'give', 'a', 'proof', 'for', 'that', 'the', 'cardinality', 'of', 'a', 'function', 'basis', 'of', 'the', 'invariants', 'for', 'a', 'finite', 'dimensional', 'real', 'vector', 'space', 'by', 'a', 'compact', 'group', 'is', 'lower', 'bounded', 'by', 'the', 'intuitive', 'difference', 'of', 't... | [-0.15555673474445939, 0.12412382058428192, -0.07811119117832277, 0.029050201587961056, -0.1045368649996817, -0.05278148459619843, -0.006084950920194387, 0.3082084070891142, -0.267993348557502, -0.2100293662631884, 0.12394961510144639, -0.2213495655101724, -0.1709231231827289, 0.1688816758192843, -0.04589799704262987, ... |
1,803.02012 | A Dynamic Model of Central Counterparty Risk | We introduce a dynamic model of the default waterfall of derivatives CCPs and
propose a risk sensitive method for sizing the initial margin (IM), and the
default fund (DF) and its allocation among clearing members. Using a Markovian
structure model of joint credit migrations, our evaluation of DF takes into
account t... | q-fin.RM | we introduce a dynamic model of the default waterfall of derivatives ccps and propose a risk sensitive method for sizing the initial margin im and the default fund df and its allocation among clearing members using a markovian structure model of joint credit migrations our evaluation of df takes into account the joint ... | [['we', 'introduce', 'a', 'dynamic', 'model', 'of', 'the', 'default', 'waterfall', 'of', 'derivatives', 'ccps', 'and', 'propose', 'a', 'risk', 'sensitive', 'method', 'for', 'sizing', 'the', 'initial', 'margin', 'im', 'and', 'the', 'default', 'fund', 'df', 'and', 'its', 'allocation', 'among', 'clearing', 'members', 'usi... | [-0.1166494897890674, -0.04326791701352467, -0.12088959221525684, 0.08817689977282578, -0.05243836610132585, -0.14074557319121517, 0.13833708208175782, 0.3914069597487864, -0.23280375133390013, -0.23957835089253343, 0.11131407729673969, -0.22306206822395325, -0.12997801640759343, 0.1631560405999746, -0.0866220955673666... |
1,803.02013 | Modulational instability, rogue waves, and envelope solitons in opposite
polarity dusty plasmas | Dust-acoustic (DA) waves (DAWs) and their modulational instability (MI) have
been investigated theoretically in a plasma system consisting of inertial
opposite polarity (positively and negatively) warm adiabatic charged dust
particles as well as inertialess non-extensive $q$-distributed electrons and
non-thermal ions... | physics.plasm-ph | dustacoustic da waves daws and their modulational instability mi have been investigated theoretically in a plasma system consisting of inertial opposite polarity positively and negatively warm adiabatic charged dust particles as well as inertialess nonextensive qdistributed electrons and nonthermal ions a nonlinear sch... | [['dustacoustic', 'da', 'waves', 'daws', 'and', 'their', 'modulational', 'instability', 'mi', 'have', 'been', 'investigated', 'theoretically', 'in', 'a', 'plasma', 'system', 'consisting', 'of', 'inertial', 'opposite', 'polarity', 'positively', 'and', 'negatively', 'warm', 'adiabatic', 'charged', 'dust', 'particles', 'a... | [-0.13231095173370586, 0.22624955055365278, -0.08371767636572758, 0.10628562243425052, -0.06107319798320532, -0.13374718760170942, -0.07156942278955254, 0.33781488576729957, -0.20430535733556518, -0.21872935246594333, 0.07134130415071703, -0.2560035445200341, -0.09944494047258459, 0.20450692389104105, 0.032967008970125... |
1,803.02014 | Properties of solutions to some weighted $p$-Laplacian equation | In this paper, we prove some qualitative properties for the positive
solutions to some degenerate elliptic equation given by
\[-\operatorname{div}(w|\nabla u|^{p-2}\nabla u)=f(x,u);\;\;w\in
\mathcal{A}_p\] on smooth domain and for varying nonlinearity $f$.
| math.AP | in this paper we prove some qualitative properties for the positive solutions to some degenerate elliptic equation given by operatornamedivwnabla up2nabla ufxuwin mathcala_p on smooth domain and for varying nonlinearity f | [['in', 'this', 'paper', 'we', 'prove', 'some', 'qualitative', 'properties', 'for', 'the', 'positive', 'solutions', 'to', 'some', 'degenerate', 'elliptic', 'equation', 'given', 'by', 'operatornamedivwnabla', 'up2nabla', 'ufxuwin', 'mathcala_p', 'on', 'smooth', 'domain', 'and', 'for', 'varying', 'nonlinearity', 'f']] | [-0.16743159061297774, 0.012192098290792533, -0.0380237527258162, 0.04389845960291235, -0.12980228130306518, -0.1795413888591741, -0.03435212310120862, 0.34061049909463953, -0.33037286823881523, -0.19569419956366932, 0.12177997680763449, -0.34049266669899225, -0.1462415632392679, 0.23601712313081538, -0.122687221770840... |
1,803.02015 | Generative Modeling of Multimodal Multi-Human Behavior | This work presents a methodology for modeling and predicting human behavior
in settings with N humans interacting in highly multimodal scenarios (i.e.
where there are many possible highly-distinct futures). A motivating example
includes robots interacting with humans in crowded environments, such as
self-driving cars... | cs.RO cs.HC | this work presents a methodology for modeling and predicting human behavior in settings with n humans interacting in highly multimodal scenarios ie where there are many possible highlydistinct futures a motivating example includes robots interacting with humans in crowded environments such as selfdriving cars operating... | [['this', 'work', 'presents', 'a', 'methodology', 'for', 'modeling', 'and', 'predicting', 'human', 'behavior', 'in', 'settings', 'with', 'n', 'humans', 'interacting', 'in', 'highly', 'multimodal', 'scenarios', 'ie', 'where', 'there', 'are', 'many', 'possible', 'highlydistinct', 'futures', 'a', 'motivating', 'example', ... | [-0.06977380952451837, 0.06680479064562966, -0.09831401893729864, 0.07480919247495749, -0.11414762954461757, -0.19358547957738934, 0.02878431237612294, 0.4781660955066288, -0.24901492464032243, -0.34577061990067864, 0.007283114561194543, -0.30830521263863747, -0.23172742084407524, 0.1645818821105107, -0.132745752838835... |
1,803.02016 | LAMOST DR1: Stellar parameters and chemical abundances with SP_Ace | We present a new analysis of the LAMOST DR1 survey spectral database
performed with the code SP_Ace, which provides the derived stellar parameters
T$_{\rm eff}$, log (g), [Fe/H], and [$\alpha$/Fe] for 1,097,231 stellar
objects. We tested the reliability of our results by comparing them to
reference results from high ... | astro-ph.GA astro-ph.SR | we present a new analysis of the lamost dr1 survey spectral database performed with the code sp_ace which provides the derived stellar parameters t_rm eff log g feh and alphafe for 1097231 stellar objects we tested the reliability of our results by comparing them to reference results from high spectral resolution surve... | [['we', 'present', 'a', 'new', 'analysis', 'of', 'the', 'lamost', 'dr1', 'survey', 'spectral', 'database', 'performed', 'with', 'the', 'code', 'sp_ace', 'which', 'provides', 'the', 'derived', 'stellar', 'parameters', 't_rm', 'eff', 'log', 'g', 'feh', 'and', 'alphafe', 'for', '1097231', 'stellar', 'objects', 'we', 'test... | [-0.045317669568414036, 0.08225120831481066, -0.055298337784080095, 0.10473221977345246, -0.06629123604492754, -0.08290956392191536, 0.10765872281891378, 0.44151619652455504, -0.1558705812458657, -0.4593043651524161, 0.016262311630782265, -0.34538215933721667, 0.020510599956162705, 0.2562134859675526, -0.11380948023177... |
1,803.02017 | Depth and regularity of monomial ideals via polarization and
combinatorial optimization | In this paper we use polarization to study the behavior of the depth and
regularity of a monomial ideal $I$, locally at a variable $x_i$, when we lower
the degree of all the highest powers of the variable $x_i$ occurring in the
minimal generating set of $I$, and examine the depth and regularity of powers
of edge idea... | math.AC math.CO | in this paper we use polarization to study the behavior of the depth and regularity of a monomial ideal i locally at a variable x_i when we lower the degree of all the highest powers of the variable x_i occurring in the minimal generating set of i and examine the depth and regularity of powers of edge ideals of clutter... | [['in', 'this', 'paper', 'we', 'use', 'polarization', 'to', 'study', 'the', 'behavior', 'of', 'the', 'depth', 'and', 'regularity', 'of', 'a', 'monomial', 'ideal', 'i', 'locally', 'at', 'a', 'variable', 'x_i', 'when', 'we', 'lower', 'the', 'degree', 'of', 'all', 'the', 'highest', 'powers', 'of', 'the', 'variable', 'x_i'... | [-0.15167812373280734, 0.07768911614753973, -0.03139237334326535, -0.010376280232274031, -0.060951607865183714, -0.1234649091900385, -0.011460599928306272, 0.38363743663628724, -0.34676617113026703, -0.1954072991832179, 0.11367983528057934, -0.28080689509796514, -0.10703425292557404, 0.10624579493431831, -0.11896339227... |
1,803.02018 | Intent-aware Multi-agent Reinforcement Learning | This paper proposes an intent-aware multi-agent planning framework as well as
a learning algorithm. Under this framework, an agent plans in the goal space to
maximize the expected utility. The planning process takes the belief of other
agents' intents into consideration. Instead of formulating the learning problem
as... | cs.AI | this paper proposes an intentaware multiagent planning framework as well as a learning algorithm under this framework an agent plans in the goal space to maximize the expected utility the planning process takes the belief of other agents intents into consideration instead of formulating the learning problem as a partia... | [['this', 'paper', 'proposes', 'an', 'intentaware', 'multiagent', 'planning', 'framework', 'as', 'well', 'as', 'a', 'learning', 'algorithm', 'under', 'this', 'framework', 'an', 'agent', 'plans', 'in', 'the', 'goal', 'space', 'to', 'maximize', 'the', 'expected', 'utility', 'the', 'planning', 'process', 'takes', 'the', '... | [-0.0640745067599316, 0.03343812539204703, -0.10513853813766397, 0.061033817824685796, -0.1492311841683443, -0.14077526236855492, 0.06059733057123388, 0.47404296204601365, -0.2867539518119134, -0.32787821171133175, 0.0735037028057424, -0.23349048396360642, -0.2225119031080016, 0.17528403122410102, -0.15235634469763212,... |
1,803.02019 | Modelling stock correlations with expected returns from investors | Stock correlations is crucial to asset pricing, investor decision-making, and
financial risk regulations. However, microscopic explanation based on
agent-based modeling is still lacking. We here propose a model derived from
minority game for modeling stock correlations, in which an agent's expected
return for one sto... | q-fin.CP q-fin.ST | stock correlations is crucial to asset pricing investor decisionmaking and financial risk regulations however microscopic explanation based on agentbased modeling is still lacking we here propose a model derived from minority game for modeling stock correlations in which an agents expected return for one stock is influ... | [['stock', 'correlations', 'is', 'crucial', 'to', 'asset', 'pricing', 'investor', 'decisionmaking', 'and', 'financial', 'risk', 'regulations', 'however', 'microscopic', 'explanation', 'based', 'on', 'agentbased', 'modeling', 'is', 'still', 'lacking', 'we', 'here', 'propose', 'a', 'model', 'derived', 'from', 'minority',... | [-0.05416699037436516, 0.09462060202898893, -0.08696774802501163, 0.17366740330452882, -0.07983064212378174, -0.19468948962467333, 0.11933258446684528, 0.44417482633744515, -0.24978873764254875, -0.2701383086503483, 0.1355060663006659, -0.36724373724672105, -0.14026338181818926, 0.1717215557838039, -0.1060114195630435,... |
1,803.0202 | Light-Matter Interactions via the Exact Factorization Approach | The exact factorization approach, originally developed for electron-nuclear
dynamics, is extended to light-matter interactions within the dipole
approximation. This allows for a Schrodinger equation for the photonic
wavefunction, in which the potential contains exactly the effects on the photon
field of its coupling ... | quant-ph | the exact factorization approach originally developed for electronnuclear dynamics is extended to lightmatter interactions within the dipole approximation this allows for a schrodinger equation for the photonic wavefunction in which the potential contains exactly the effects on the photon field of its coupling to matte... | [['the', 'exact', 'factorization', 'approach', 'originally', 'developed', 'for', 'electronnuclear', 'dynamics', 'is', 'extended', 'to', 'lightmatter', 'interactions', 'within', 'the', 'dipole', 'approximation', 'this', 'allows', 'for', 'a', 'schrodinger', 'equation', 'for', 'the', 'photonic', 'wavefunction', 'in', 'whi... | [-0.10786457683059796, 0.10570758974339817, -0.11099973202525246, 0.09981682797324312, -0.044133274263725424, -0.1555489939714451, 0.0037456413515466304, 0.36788137929036846, -0.23680105685325695, -0.302184337442202, -0.0034401735150416898, -0.2557484228723184, -0.14600627210514605, 0.1875790451183792, 0.06613664000202... |
1,803.02021 | Understanding Short-Horizon Bias in Stochastic Meta-Optimization | Careful tuning of the learning rate, or even schedules thereof, can be
crucial to effective neural net training. There has been much recent interest
in gradient-based meta-optimization, where one tunes hyperparameters, or even
learns an optimizer, in order to minimize the expected loss when the training
procedure is ... | cs.LG stat.ML | careful tuning of the learning rate or even schedules thereof can be crucial to effective neural net training there has been much recent interest in gradientbased metaoptimization where one tunes hyperparameters or even learns an optimizer in order to minimize the expected loss when the training procedure is unrolled b... | [['careful', 'tuning', 'of', 'the', 'learning', 'rate', 'or', 'even', 'schedules', 'thereof', 'can', 'be', 'crucial', 'to', 'effective', 'neural', 'net', 'training', 'there', 'has', 'been', 'much', 'recent', 'interest', 'in', 'gradientbased', 'metaoptimization', 'where', 'one', 'tunes', 'hyperparameters', 'or', 'even',... | [-0.09153307562119718, 0.08850307975389929, -0.043707282383747666, 0.10171146004176047, -0.11022697918483784, -0.1926185034198561, 0.05705613499975382, 0.4421507914603683, -0.2964212322014099, -0.35017707593102065, 0.1325945504488655, -0.23215753088073102, -0.127375020299932, 0.21550028811937555, -0.1293031458590027, 0... |
1,803.02022 | Modular linear differential equations of fourth order and minimal
$\mathcal{W}$-algebras | A characterization of the minimal $\mathcal{W}$-algebras associated with the
Deligne exceptional series at level $-h^\vee/6$ is obtained by using
one-parameter family of modular linear differential equations of order $4$. In
particular, the characters of the Ramond-twisted modules of minimal
$\mathcal{W}$-algebras re... | math.QA math.NT | a characterization of the minimal mathcalwalgebras associated with the deligne exceptional series at level hvee6 is obtained by using oneparameter family of modular linear differential equations of order 4 in particular the characters of the ramondtwisted modules of minimal mathcalwalgebras related to the deligne excep... | [['a', 'characterization', 'of', 'the', 'minimal', 'mathcalwalgebras', 'associated', 'with', 'the', 'deligne', 'exceptional', 'series', 'at', 'level', 'hvee6', 'is', 'obtained', 'by', 'using', 'oneparameter', 'family', 'of', 'modular', 'linear', 'differential', 'equations', 'of', 'order', '4', 'in', 'particular', 'the'... | [-0.16936798237311917, 0.03312430290549319, -0.04189470290946655, 0.03642684125299685, -0.08901304761186624, -0.12631812778253776, -0.060561755210913434, 0.2337726422642262, -0.3104053512812616, -0.2825492777598974, 0.14886107144262403, -0.2955349910264023, -0.13925849333501014, 0.21923004460628503, -0.0761248959491077... |
1,803.02023 | Accumulate Then Transmit: Multi-user Scheduling in Full-Duplex
Wireless-Powered IoT Systems | This paper develops and evaluates an accumulate-then-transmit framework for
multi-user scheduling in a full-duplex (FD) wireless-powered Internet-of-Things
system, consisting of multiple energy harvesting (EH) IoT devices (IoDs) and
one FD hybrid access point (HAP). All IoDs have no embedded energy supply and
thus ne... | cs.IT math.IT | this paper develops and evaluates an accumulatethentransmit framework for multiuser scheduling in a fullduplex fd wirelesspowered internetofthings system consisting of multiple energy harvesting eh iot devices iods and one fd hybrid access point hap all iods have no embedded energy supply and thus need to perform eh be... | [['this', 'paper', 'develops', 'and', 'evaluates', 'an', 'accumulatethentransmit', 'framework', 'for', 'multiuser', 'scheduling', 'in', 'a', 'fullduplex', 'fd', 'wirelesspowered', 'internetofthings', 'system', 'consisting', 'of', 'multiple', 'energy', 'harvesting', 'eh', 'iot', 'devices', 'iods', 'and', 'one', 'fd', 'h... | [-0.24543888516930856, -0.011114922588286802, -0.051337905052307356, -0.005469366045706399, -0.07303468317094866, -0.24775401098823707, 0.1402703020523623, 0.40294897091030085, -0.2741668594685186, -0.27473047037156784, 0.0608486889048066, -0.27489186617781514, -0.14174753616668315, 0.15214056143038654, -0.119506742312... |
1,803.02024 | Using Survival Information in Truncation by Death Problems Without the
Monotonicity Assumption | In some randomized clinical trials, patients may die before the measurements
of their outcomes. Even though randomization generates comparable treatment and
control groups, the remaining survivors often differ significantly in
background variables that are prognostic to the outcomes. This is called the
truncation by ... | stat.AP stat.ME | in some randomized clinical trials patients may die before the measurements of their outcomes even though randomization generates comparable treatment and control groups the remaining survivors often differ significantly in background variables that are prognostic to the outcomes this is called the truncation by death ... | [['in', 'some', 'randomized', 'clinical', 'trials', 'patients', 'may', 'die', 'before', 'the', 'measurements', 'of', 'their', 'outcomes', 'even', 'though', 'randomization', 'generates', 'comparable', 'treatment', 'and', 'control', 'groups', 'the', 'remaining', 'survivors', 'often', 'differ', 'significantly', 'in', 'bac... | [-0.05938197261110959, 0.10761566162951777, -0.11807833856612855, 0.11408279861508396, -0.14207526368917384, -0.15953771811886575, 0.1284294205544582, 0.3761391156544937, -0.22170992472194997, -0.30593264086789745, 0.15205543654989545, -0.23433076729997993, -0.09978775717037257, 0.19725831060660956, -0.1467460698223480... |
1,803.02025 | Excitation mechanism of OI lines in Herbig Ae/Be stars | We have investigated the role of a few prominent excitation mechanisms viz.
collisional excitation, recombination, continuum fluorescence and Lyman beta
fluorescence on the OI line spectra in Herbig Ae/Be stars. The aim is to
understand which of them is the central mechanism that explains the observed OI
line strengt... | astro-ph.SR | we have investigated the role of a few prominent excitation mechanisms viz collisional excitation recombination continuum fluorescence and lyman beta fluorescence on the oi line spectra in herbig aebe stars the aim is to understand which of them is the central mechanism that explains the observed oi line strengths the ... | [['we', 'have', 'investigated', 'the', 'role', 'of', 'a', 'few', 'prominent', 'excitation', 'mechanisms', 'viz', 'collisional', 'excitation', 'recombination', 'continuum', 'fluorescence', 'and', 'lyman', 'beta', 'fluorescence', 'on', 'the', 'oi', 'line', 'spectra', 'in', 'herbig', 'aebe', 'stars', 'the', 'aim', 'is', '... | [-0.0038881995592277892, 0.060868285930612824, 0.062498317962014896, 0.10197885604343893, -0.03257008145060043, -0.09857163392585812, 0.039220849458440586, 0.5119479717628926, -0.12020335648417102, -0.2960375463271872, -0.03776499228653214, -0.3159063032463841, 0.008524197361993124, 0.12211721390485764, 0.0454584145976... |
1,803.02026 | Spectral Analysis of GFDM Modulated Signal under Nonlinear Behavior of
Power Amplifier | General frequency division multiplexing (GFDM) is a flexible non-orthogonal
waveform candidate for 5G which can offer some advantages such as low
out-of-band (OOB) emission and high spectral efficiency. In this paper, the
effects of nonlinear behavior of practical PAs on GFDM signal are studied. In
the first step, a ... | eess.SP | general frequency division multiplexing gfdm is a flexible nonorthogonal waveform candidate for 5g which can offer some advantages such as low outofband oob emission and high spectral efficiency in this paper the effects of nonlinear behavior of practical pas on gfdm signal are studied in the first step a closed form e... | [['general', 'frequency', 'division', 'multiplexing', 'gfdm', 'is', 'a', 'flexible', 'nonorthogonal', 'waveform', 'candidate', 'for', '5g', 'which', 'can', 'offer', 'some', 'advantages', 'such', 'as', 'low', 'outofband', 'oob', 'emission', 'and', 'high', 'spectral', 'efficiency', 'in', 'this', 'paper', 'the', 'effects'... | [-0.1615565952200156, 0.0032111224790032093, -0.05608555862250236, 0.027904723768229955, -0.06435387580691335, -0.18175476506137503, 0.0007187115610577166, 0.4027293521624345, -0.24958033787373166, -0.2312607820969648, 0.09457158081394691, -0.21709541497895352, -0.19569843482190313, 0.21300616776391576, -0.058942072498... |
1,803.02027 | DNA Base Pair Mismatches Induce Structural Changes and Alter the Free
Energy Landscape of Base Flip | Double-stranded DNA may contain mismatched base pairs beyond the Watson-Crick
pairs guanine-cytosine and adenine-thymine. Such mismatches bear adverse
consequences for human health. We utilize molecular dynamics and metadynamics
computer simulations to study the equilibrium structure and dynamics for both
matched and... | physics.bio-ph q-bio.BM | doublestranded dna may contain mismatched base pairs beyond the watsoncrick pairs guaninecytosine and adeninethymine such mismatches bear adverse consequences for human health we utilize molecular dynamics and metadynamics computer simulations to study the equilibrium structure and dynamics for both matched and mismatc... | [['doublestranded', 'dna', 'may', 'contain', 'mismatched', 'base', 'pairs', 'beyond', 'the', 'watsoncrick', 'pairs', 'guaninecytosine', 'and', 'adeninethymine', 'such', 'mismatches', 'bear', 'adverse', 'consequences', 'for', 'human', 'health', 'we', 'utilize', 'molecular', 'dynamics', 'and', 'metadynamics', 'computer',... | [-0.16870132877738797, 0.10349523930926807, -0.0017887998837977648, 0.1440682347965776, -0.07147750060539693, -0.15601713558013822, 0.11983418990469848, 0.42896907186756533, -0.2945947674355314, -0.28480498417047784, -0.023808310201881493, -0.3092518497972681, -0.2088138191126442, 0.12682543996682702, -0.05088919811593... |
1,803.02028 | Heavy-element yields and abundances of Asymptotic Giant Branch models
with a Small Magellanic Cloud metallicity | We present new theoretical stellar yields and surface abundances for
asymptotic giant branch (AGB) models with a metallicity appropriate for stars
in the Small Magellanic Cloud (SMC, $Z= 0.0028$, [Fe/H] $\approx -0.7$). New
evolutionary sequences and post-processing nucleosynthesis results are
presented for initial m... | astro-ph.SR | we present new theoretical stellar yields and surface abundances for asymptotic giant branch agb models with a metallicity appropriate for stars in the small magellanic cloud smc z 00028 feh approx 07 new evolutionary sequences and postprocessing nucleosynthesis results are presented for initial masses between 1m_odot ... | [['we', 'present', 'new', 'theoretical', 'stellar', 'yields', 'and', 'surface', 'abundances', 'for', 'asymptotic', 'giant', 'branch', 'agb', 'models', 'with', 'a', 'metallicity', 'appropriate', 'for', 'stars', 'in', 'the', 'small', 'magellanic', 'cloud', 'smc', 'z', '00028', 'feh', 'approx', '07', 'new', 'evolutionary'... | [0.0017287258398593277, 0.16087044656566693, -0.030891011066332057, 0.08229008248455504, -0.027413114480598754, -0.059989179323033034, 0.09840467994768373, 0.4362412437393859, -0.1358049123950181, -0.3556954775441874, -0.019964574142422125, -0.2943371178315919, 0.02893421394951843, 0.179347759437053, -0.081343289661097... |
1,803.02029 | Enhanced Superconducting Transition Temperature in Electroplated Rhenium | We show that electroplated Re films in multilayers with noble metals such as
Cu, Au, and Pd have an enhanced superconducting critical temperature relative
to previous methods of preparing Re. The dc resistance and magnetic
susceptibility indicate a critical temperature of approximately 6 K. Magnetic
response as a fun... | cond-mat.supr-con | we show that electroplated re films in multilayers with noble metals such as cu au and pd have an enhanced superconducting critical temperature relative to previous methods of preparing re the dc resistance and magnetic susceptibility indicate a critical temperature of approximately 6 k magnetic response as a function ... | [['we', 'show', 'that', 'electroplated', 're', 'films', 'in', 'multilayers', 'with', 'noble', 'metals', 'such', 'as', 'cu', 'au', 'and', 'pd', 'have', 'an', 'enhanced', 'superconducting', 'critical', 'temperature', 'relative', 'to', 'previous', 'methods', 'of', 'preparing', 're', 'the', 'dc', 'resistance', 'and', 'magn... | [-0.14240123156196205, 0.21972215313022994, 0.051367949853496006, -0.07482475148669133, 0.025942760185959438, -0.16539913411640253, 0.09343281893137222, 0.42307464509115866, -0.1815828373345236, -0.36421171681334574, 0.031373822381525925, -0.36092528867690515, -0.012409891568434734, 0.28897910021866363, 0.0575685490951... |
1,803.0203 | Exact partial information decompositions for Gaussian systems based on
dependency constraints | The Partial Information Decomposition (PID) [arXiv:1004.2515] provides a
theoretical framework to characterize and quantify the structure of
multivariate information sharing. A new method (Idep) has recently been
proposed for computing a two-predictor PID over discrete spaces.
[arXiv:1709.06653] A lattice of maximum ... | cond-mat.stat-mech cs.IT math.IT physics.data-an q-bio.QM stat.ML | the partial information decomposition pid arxiv10042515 provides a theoretical framework to characterize and quantify the structure of multivariate information sharing a new method idep has recently been proposed for computing a twopredictor pid over discrete spaces arxiv170906653 a lattice of maximum entropy probabili... | [['the', 'partial', 'information', 'decomposition', 'pid', 'arxiv10042515', 'provides', 'a', 'theoretical', 'framework', 'to', 'characterize', 'and', 'quantify', 'the', 'structure', 'of', 'multivariate', 'information', 'sharing', 'a', 'new', 'method', 'idep', 'has', 'recently', 'been', 'proposed', 'for', 'computing', '... | [-0.06218571429253443, 0.02187419722271203, -0.12972820481889277, 0.09470254189211998, -0.09647131838150076, -0.19563780918174967, 0.02660909029245786, 0.36776456687916687, -0.24767980134437004, -0.27692859336109527, 0.13214341224366952, -0.2794302739765864, -0.14662811503704679, 0.2123462109785568, -0.0987016926084614... |
1,803.02031 | Pressure strain correlation modeling for turbulent flows | Almost all investigations of turbulent flows in academia and in the industry
utilize some degree of turbulence modeling. Of the available approaches to
turbulence modeling Reynolds Stress Models have the highest potential to
replicate complex flow phenomena. Due to its complexity and its importance in
flow evolution ... | physics.flu-dyn | almost all investigations of turbulent flows in academia and in the industry utilize some degree of turbulence modeling of the available approaches to turbulence modeling reynolds stress models have the highest potential to replicate complex flow phenomena due to its complexity and its importance in flow evolution mode... | [['almost', 'all', 'investigations', 'of', 'turbulent', 'flows', 'in', 'academia', 'and', 'in', 'the', 'industry', 'utilize', 'some', 'degree', 'of', 'turbulence', 'modeling', 'of', 'the', 'available', 'approaches', 'to', 'turbulence', 'modeling', 'reynolds', 'stress', 'models', 'have', 'the', 'highest', 'potential', '... | [-0.11387462167638457, 0.11350358204514373, -0.06282670254167778, 0.062171737947257756, -0.03217902595445124, -0.08305277868350541, -0.04116591739276534, 0.3839203514937871, -0.2910799576560023, -0.2924112111628299, 0.11754126972488425, -0.26172359510525767, -0.17791790120741902, 0.23456665819961262, -0.025294476975473... |
1,803.02032 | John's Walk | We present an affine-invariant random walk for drawing uniform random samples
from a convex body $\mathcal{K} \subset \mathbb{R}^n$ that uses maximum volume
inscribed ellipsoids, known as John's ellipsoids, for the proposal
distribution. Our algorithm makes steps using uniform sampling from the John's
ellipsoid of th... | stat.ML cs.CG cs.DS stat.CO | we present an affineinvariant random walk for drawing uniform random samples from a convex body mathcalk subset mathbbrn that uses maximum volume inscribed ellipsoids known as johns ellipsoids for the proposal distribution our algorithm makes steps using uniform sampling from the johns ellipsoid of the symmetrization o... | [['we', 'present', 'an', 'affineinvariant', 'random', 'walk', 'for', 'drawing', 'uniform', 'random', 'samples', 'from', 'a', 'convex', 'body', 'mathcalk', 'subset', 'mathbbrn', 'that', 'uses', 'maximum', 'volume', 'inscribed', 'ellipsoids', 'known', 'as', 'johns', 'ellipsoids', 'for', 'the', 'proposal', 'distribution',... | [-0.10075747631971949, 0.1525565801111325, -0.07387559031184505, 0.002565115257688188, -0.06040597911362119, -0.1306301089814575, 0.09752765055223979, 0.3760439715958361, -0.2945515467415981, -0.228092896346613, 0.09536261953501801, -0.29878755626750403, -0.09754213822226779, 0.15611939678964173, -0.09919772035008746, ... |
1,803.02033 | Atomic Visualization of Copper Oxide Structure in Infinite-Layer Cuprate
SrCuO2 | We report on atomic-scale visualization of the structure of infinite-layer
cuprate SrCuO2 thin films grown on Nb-doped SrTiO3 substrates by molecular beam
epitaxy. In-situ scanning tunneling microscopy study reveals stoichiometric
copper oxide (CuO2) plane with a 2 x 2 surface reconstruction, prompted by
preferential... | cond-mat.supr-con cond-mat.str-el | we report on atomicscale visualization of the structure of infinitelayer cuprate srcuo2 thin films grown on nbdoped srtio3 substrates by molecular beam epitaxy insitu scanning tunneling microscopy study reveals stoichiometric copper oxide cuo2 plane with a 2 x 2 surface reconstruction prompted by preferential clusterin... | [['we', 'report', 'on', 'atomicscale', 'visualization', 'of', 'the', 'structure', 'of', 'infinitelayer', 'cuprate', 'srcuo2', 'thin', 'films', 'grown', 'on', 'nbdoped', 'srtio3', 'substrates', 'by', 'molecular', 'beam', 'epitaxy', 'insitu', 'scanning', 'tunneling', 'microscopy', 'study', 'reveals', 'stoichiometric', 'c... | [-0.1972729041409053, 0.2151331189480948, 0.023390918695291536, -0.003927139134993624, -0.028219827496614613, -0.1444287764473406, 0.13286267400224938, 0.4452134701499685, -0.25863016752495627, -0.3028534366672889, -0.033569962233801175, -0.3468365580965688, -0.11484313788289419, 0.13736474134464993, 0.0658259744313163... |
1,803.02034 | Effective multi-scale approach to the Schr\"odinger cocycle over a skew
shift base | We prove a conditional theorem on the positivity of the Lyapunov exponent for
a Schr\"odinger cocycle over a skew shift base with a cosine potential and the
golden ratio as frequency. For coupling below 1, which is the threshold for
Herman's subharmonicity trick, we formulate three conditions on the Lyapunov
exponent... | math-ph math.AP math.DS math.MP | we prove a conditional theorem on the positivity of the lyapunov exponent for a schrodinger cocycle over a skew shift base with a cosine potential and the golden ratio as frequency for coupling below 1 which is the threshold for hermans subharmonicity trick we formulate three conditions on the lyapunov exponent in a fi... | [['we', 'prove', 'a', 'conditional', 'theorem', 'on', 'the', 'positivity', 'of', 'the', 'lyapunov', 'exponent', 'for', 'a', 'schrodinger', 'cocycle', 'over', 'a', 'skew', 'shift', 'base', 'with', 'a', 'cosine', 'potential', 'and', 'the', 'golden', 'ratio', 'as', 'frequency', 'for', 'coupling', 'below', '1', 'which', 'i... | [-0.1274485578497305, 0.11093108628512077, -0.11402904670280607, 0.10544981445469286, -0.03757508677865743, -0.14375309167308328, 0.07597296638110572, 0.2973975101890771, -0.2601067144423723, -0.21223357110891652, 0.15125570866461518, -0.2617068904006611, -0.17453001921834504, 0.2510370838881025, -0.04912010665335085, ... |
1,803.02035 | Large deviation estimates and H\"older regularity of the Lyapunov
exponents for quasi-periodic Schr\"odinger cocycles | We consider one-dimensional quasi-periodic Schr\"odinger operators with
analytic potentials. In the positive Lyapunov exponent regime, we prove large
deviation estimates which lead to optimal H\"older continuity of the Lyapunov
exponents and the integrated density of states, in both small Lyapunov exponent
and large ... | math-ph math.DS math.MP math.SP | we consider onedimensional quasiperiodic schrodinger operators with analytic potentials in the positive lyapunov exponent regime we prove large deviation estimates which lead to optimal holder continuity of the lyapunov exponents and the integrated density of states in both small lyapunov exponent and large coupling re... | [['we', 'consider', 'onedimensional', 'quasiperiodic', 'schrodinger', 'operators', 'with', 'analytic', 'potentials', 'in', 'the', 'positive', 'lyapunov', 'exponent', 'regime', 'we', 'prove', 'large', 'deviation', 'estimates', 'which', 'lead', 'to', 'optimal', 'holder', 'continuity', 'of', 'the', 'lyapunov', 'exponents'... | [-0.21936435678175517, 0.1345928657184621, -0.07729634414759598, 0.11056450266291254, -0.034020286891193664, -0.1957184027414769, 0.045917493773491254, 0.27379010430844836, -0.28084535968290375, -0.13963885282698488, 0.11994245238851622, -0.31130330357700586, -0.15849793412988739, 0.24826794375465916, -0.00620674538160... |
1,803.02036 | Hot fusion reactions with deformed nuclei for synthesis of superheavy
nuclei: an extension of the fusion-by-diffusion model | The fusion-by-diffusion model proposed by Swiatecki {\it et al.} [Phys. Rev.
C71, 014602 (2005)] has provided a simple and convenient tool to estimate
evaporation residue cross sections for superheavy nuclei. I extend this model
by taking into account deformation of the target nucleus, and discuss the role
of orienta... | nucl-th nucl-ex | the fusionbydiffusion model proposed by swiatecki it et al phys rev c71 014602 2005 has provided a simple and convenient tool to estimate evaporation residue cross sections for superheavy nuclei i extend this model by taking into account deformation of the target nucleus and discuss the role of orientation of deformed ... | [['the', 'fusionbydiffusion', 'model', 'proposed', 'by', 'swiatecki', 'it', 'et', 'al', 'phys', 'rev', 'c71', '014602', '2005', 'has', 'provided', 'a', 'simple', 'and', 'convenient', 'tool', 'to', 'estimate', 'evaporation', 'residue', 'cross', 'sections', 'for', 'superheavy', 'nuclei', 'i', 'extend', 'this', 'model', '... | [-0.034233915870187474, 0.10686688844400444, -0.09753245715041617, 0.06375131508758547, -0.009921600067001931, -0.09454255084616735, 0.04081413410877918, 0.3362006235812955, -0.2620026093770695, -0.30095982783446634, -0.013076242696329513, -0.25520468000596497, -0.06677191269974334, 0.16864047467516846, -0.024850040218... |
1,803.02037 | Matter effects on the flavor conversions of solar neutrinos and
high-energy astrophysical neutrinos | Can we observe the solar eclipses in the neutrino light? In principle, this
is possible by identifying the lunar matter effects on the flavor conversions
of solar neutrinos when they traverse the Moon before reaching the detectors at
the Earth. Unfortunately, we show that the lunar matter effects on the survival
prob... | hep-ph | can we observe the solar eclipses in the neutrino light in principle this is possible by identifying the lunar matter effects on the flavor conversions of solar neutrinos when they traverse the moon before reaching the detectors at the earth unfortunately we show that the lunar matter effects on the survival probabilit... | [['can', 'we', 'observe', 'the', 'solar', 'eclipses', 'in', 'the', 'neutrino', 'light', 'in', 'principle', 'this', 'is', 'possible', 'by', 'identifying', 'the', 'lunar', 'matter', 'effects', 'on', 'the', 'flavor', 'conversions', 'of', 'solar', 'neutrinos', 'when', 'they', 'traverse', 'the', 'moon', 'before', 'reaching'... | [-0.07750710161510578, 0.33091412469745163, -0.06309925099367696, 0.19056079432479883, -0.041978597271540935, -0.05720865997785995, 0.06159316253856071, 0.3472661987901473, -0.2408533763786978, -0.3582865854355791, 0.05135155314952905, -0.31098133652309373, -0.0740463760766116, 0.205169469395206, -0.02869212639341054, ... |
1,803.02038 | Gate-tunable Room-temperature Ferromagnetism in Two-dimensional
Fe$_3$GeTe$_2$ | Material research has been a major driving force in the development of modern
nano-electronic devices. In particular, research in magnetic thin films has
revolutionized the development of spintronic devices; identifying new magnetic
materials is key to better device performance and new device paradigm. The
advent of ... | cond-mat.mtrl-sci | material research has been a major driving force in the development of modern nanoelectronic devices in particular research in magnetic thin films has revolutionized the development of spintronic devices identifying new magnetic materials is key to better device performance and new device paradigm the advent of twodime... | [['material', 'research', 'has', 'been', 'a', 'major', 'driving', 'force', 'in', 'the', 'development', 'of', 'modern', 'nanoelectronic', 'devices', 'in', 'particular', 'research', 'in', 'magnetic', 'thin', 'films', 'has', 'revolutionized', 'the', 'development', 'of', 'spintronic', 'devices', 'identifying', 'new', 'magn... | [-0.166451612348217, 0.18236795277229736, 0.0038064794960556573, -0.0879495103409053, -0.059980189970204816, -0.2141834512621779, 0.07780251387517524, 0.42789540694277617, -0.26457825223507225, -0.31770383049109857, -0.0381727945941654, -0.32966955404995085, -0.14139731769562824, 0.27467515784647006, 0.0261321748203607... |
1,803.02039 | Observation of $\psi(3686) \to n\bar{n}$ and improved measurement of
$\psi(3686) \to p \bar{p}$ | We observe the decay $\psi(3686) \to n \bar{n}$ for the first time and
measure $\psi(3686) \to p \bar{p}$ with improved accuracy by using $1.07\times
10^8$ $\psi(3686)$ events collected with the BESIII detector. The measured
branching fractions are $\mathcal{B}(\psi(3686) \to n \bar{n}) = (3.06 \pm 0.06
\pm 0.14)\tim... | hep-ex | we observe the decay psi3686 to n barn for the first time and measure psi3686 to p barp with improved accuracy by using 107times 108 psi3686 events collected with the besiii detector the measured branching fractions are mathcalbpsi3686 to n barn 306 pm 006 pm 014times 104 and mathcalbpsi3686 to p barp 305 pm 002 pm 012... | [['we', 'observe', 'the', 'decay', 'psi3686', 'to', 'n', 'barn', 'for', 'the', 'first', 'time', 'and', 'measure', 'psi3686', 'to', 'p', 'barp', 'with', 'improved', 'accuracy', 'by', 'using', '107times', '108', 'psi3686', 'events', 'collected', 'with', 'the', 'besiii', 'detector', 'the', 'measured', 'branching', 'fracti... | [-0.10693073821628628, 0.2404152386902791, -0.044701721442296456, 0.022639596628268126, 0.07993816424809072, -0.0791641113525459, 0.11092283644956415, 0.31370723727766586, -0.12563345853401267, -0.4023361097049454, -0.007545846541736113, -0.4583027655339759, 0.1481604646526925, 0.17510479107377647, -0.00083708207770858... |
1,803.0204 | Principal eigenvalues of a class of nonlinear integro-differential
operators | We consider a class of nonlinear integro-differential operators and prove
existence of two principal (half) eigenvalues in bounded smooth domains with
exterior Dirichlet condition. We then establish simplicity of the principal
eigenfunctions in viscosity sense, maximum principles, continuity property of
the principal... | math.AP | we consider a class of nonlinear integrodifferential operators and prove existence of two principal half eigenvalues in bounded smooth domains with exterior dirichlet condition we then establish simplicity of the principal eigenfunctions in viscosity sense maximum principles continuity property of the principal eigenva... | [['we', 'consider', 'a', 'class', 'of', 'nonlinear', 'integrodifferential', 'operators', 'and', 'prove', 'existence', 'of', 'two', 'principal', 'half', 'eigenvalues', 'in', 'bounded', 'smooth', 'domains', 'with', 'exterior', 'dirichlet', 'condition', 'we', 'then', 'establish', 'simplicity', 'of', 'the', 'principal', 'e... | [-0.17079281052010079, 0.02716268883567395, -0.07021818719239849, 0.03701963634089087, -0.1441237676049103, -0.10183599624415916, -0.039372052672798884, 0.3154185444511699, -0.35003319943577726, -0.17478576755225236, 0.16230107642089328, -0.27720579019550123, -0.16830563525824496, 0.1558946721312223, -0.097138118930161... |
1,803.02041 | Numerical Investigations of SO(4) Emergent Extended Symmetry in Spin-1/2
Heisenberg Antiferromagnetic Chains | The antiferromagnetic Heisenberg chain is expected to have an extended
symmetry, [SU(2)xSU(2)]/Z 2 , in the infrared limit, whose physical
interpretation is that the spin and dimer order parameters form the components
of a common 4-dimensional vector. Here we numerically in- vestigate this
emergent symmetry using qua... | cond-mat.str-el | the antiferromagnetic heisenberg chain is expected to have an extended symmetry su2xsu2z 2 in the infrared limit whose physical interpretation is that the spin and dimer order parameters form the components of a common 4dimensional vector here we numerically in vestigate this emergent symmetry using quantum monte carlo... | [['the', 'antiferromagnetic', 'heisenberg', 'chain', 'is', 'expected', 'to', 'have', 'an', 'extended', 'symmetry', 'su2xsu2z', '2', 'in', 'the', 'infrared', 'limit', 'whose', 'physical', 'interpretation', 'is', 'that', 'the', 'spin', 'and', 'dimer', 'order', 'parameters', 'form', 'the', 'components', 'of', 'a', 'common... | [-0.13415235101922668, 0.18283990010399562, -0.08153114069083875, 0.1282770362947221, -0.04003414539673196, -0.09738755818795074, -0.01630049337796994, 0.37492213435471056, -0.2613923327573998, -0.2519792289134454, 0.09770494824677536, -0.283674339001829, -0.15922344344329428, 0.13014877950349316, 0.08816778564994986, ... |
1,803.02042 | Accelerated Gradient Boosting | Gradient tree boosting is a prediction algorithm that sequentially produces a
model in the form of linear combinations of decision trees, by solving an
infinite-dimensional optimization problem. We combine gradient boosting and
Nesterov's accelerated descent to design a new algorithm, which we call AGB
(for Accelerat... | stat.ML cs.LG | gradient tree boosting is a prediction algorithm that sequentially produces a model in the form of linear combinations of decision trees by solving an infinitedimensional optimization problem we combine gradient boosting and nesterovs accelerated descent to design a new algorithm which we call agb for accelerated gradi... | [['gradient', 'tree', 'boosting', 'is', 'a', 'prediction', 'algorithm', 'that', 'sequentially', 'produces', 'a', 'model', 'in', 'the', 'form', 'of', 'linear', 'combinations', 'of', 'decision', 'trees', 'by', 'solving', 'an', 'infinitedimensional', 'optimization', 'problem', 'we', 'combine', 'gradient', 'boosting', 'and... | [-0.04822755602230741, 0.05885904541527535, -0.10299461958294903, 0.09103224724531174, -0.12352441816844724, -0.14390480785672977, 0.0507450974101878, 0.4551482620141046, -0.29591574441980234, -0.30532060019587254, 0.10728685752255843, -0.256541768478399, -0.16973554171113805, 0.23694254740522327, -0.10616865587971089,... |
1,803.02043 | Online Deep Learning: Growing RBM on the fly | We propose a novel online learning algorithm for Restricted Boltzmann
Machines (RBM), namely, the Online Generative Discriminative Restricted
Boltzmann Machine (OGD-RBM), that provides the ability to build and adapt the
network architecture of RBM according to the statistics of streaming data. The
OGD-RBM is trained ... | cs.NE cs.LG stat.ML | we propose a novel online learning algorithm for restricted boltzmann machines rbm namely the online generative discriminative restricted boltzmann machine ogdrbm that provides the ability to build and adapt the network architecture of rbm according to the statistics of streaming data the ogdrbm is trained in two phase... | [['we', 'propose', 'a', 'novel', 'online', 'learning', 'algorithm', 'for', 'restricted', 'boltzmann', 'machines', 'rbm', 'namely', 'the', 'online', 'generative', 'discriminative', 'restricted', 'boltzmann', 'machine', 'ogdrbm', 'that', 'provides', 'the', 'ability', 'to', 'build', 'and', 'adapt', 'the', 'network', 'arch... | [-0.028559060293103095, 0.019555529455908903, -0.05743922364229384, 0.06556090496987063, -0.16195322547172752, -0.22027908783617528, 0.08245039274472565, 0.4687186557895098, -0.306486174699615, -0.3092264267871832, 0.0457028326379722, -0.27277276883304336, -0.17858806223823473, 0.14762273816657917, -0.1411790253761678,... |
1,803.02044 | Halo structure of $^8$B determined from intermediate energy proton
elastic scattering in inverse kinematics | The absolute differential cross section for small-angle proton elastic
scattering on the proton-rich $^8$B nucleus has been measured in inverse
kinematics for the first time. The experiment was performed using a secondary
radioactive beam with an energy of 0.7 GeV/u at GSI, Darmstadt. The active
target, namely hydrog... | nucl-ex nucl-th | the absolute differential cross section for smallangle proton elastic scattering on the protonrich 8b nucleus has been measured in inverse kinematics for the first time the experiment was performed using a secondary radioactive beam with an energy of 07 gevu at gsi darmstadt the active target namely hydrogenfilled time... | [['the', 'absolute', 'differential', 'cross', 'section', 'for', 'smallangle', 'proton', 'elastic', 'scattering', 'on', 'the', 'protonrich', '8b', 'nucleus', 'has', 'been', 'measured', 'in', 'inverse', 'kinematics', 'for', 'the', 'first', 'time', 'the', 'experiment', 'was', 'performed', 'using', 'a', 'secondary', 'radio... | [-0.03903464935856926, 0.16616723712829887, -0.11498966240050161, 0.10797328309272416, 0.028382951475899008, -0.08813315430923147, -0.004283550587784061, 0.3831319738508147, -0.18469869150739054, -0.34931812055052863, -0.01406551045981948, -0.3712566651732606, 0.067549259136157, 0.19342325033811741, 0.05128050473902156... |
1,803.02045 | Requiem for an ideal clock | The `problem of time' remains an unresolved issue in all known physical
descriptions of the Universe. One aspect of this problem is the conspicuous
absence of time in the Wheeler-Dewitt equation, which is the analogue of the
Schrodinger equation for the Universal wavefunction. Page and Wootters famously
addressed thi... | quant-ph hep-th | the problem of time remains an unresolved issue in all known physical descriptions of the universe one aspect of this problem is the conspicuous absence of time in the wheelerdewitt equation which is the analogue of the schrodinger equation for the universal wavefunction page and wootters famously addressed this proble... | [['the', 'problem', 'of', 'time', 'remains', 'an', 'unresolved', 'issue', 'in', 'all', 'known', 'physical', 'descriptions', 'of', 'the', 'universe', 'one', 'aspect', 'of', 'this', 'problem', 'is', 'the', 'conspicuous', 'absence', 'of', 'time', 'in', 'the', 'wheelerdewitt', 'equation', 'which', 'is', 'the', 'analogue', ... | [-0.14517170450322292, 0.1314676916742298, -0.1129404779282465, 0.05700439152602411, -0.051498111700449066, -0.11594881709208903, 0.040193662962553146, 0.3207615172395445, -0.2587331675434941, -0.2944697998806226, 0.09777723163252278, -0.21847866500480748, -0.10870366960155721, 0.1717271093630745, -0.04168689482636294,... |
1,803.02046 | Characterizations of $(m,n)$-Jordan derivations on some algebras | Let $\mathcal R$ be a ring, $\mathcal{M}$ be a $\mathcal R$-bimodule and
$m,n$ be two fixed nonnegative integers with $m+n\neq0$. An additive mapping
$\delta$ from $\mathcal R$ into $\mathcal{M}$ is called an \emph{$(m,n)$-Jordan
derivation} if $(m+n)\delta(A^{2})=2mA\delta(A)+2n\delta(A)A$ for every $A$ in
$\mathcal... | math.OA | let mathcal r be a ring mathcalm be a mathcal rbimodule and mn be two fixed nonnegative integers with mnneq0 an additive mapping delta from mathcal r into mathcalm is called an emphmnjordan derivation if mndeltaa22madeltaa2ndeltaaa for every a in mathcal r in this paper we prove that every mnjordan derivation from a ca... | [['let', 'mathcal', 'r', 'be', 'a', 'ring', 'mathcalm', 'be', 'a', 'mathcal', 'rbimodule', 'and', 'mn', 'be', 'two', 'fixed', 'nonnegative', 'integers', 'with', 'mnneq0', 'an', 'additive', 'mapping', 'delta', 'from', 'mathcal', 'r', 'into', 'mathcalm', 'is', 'called', 'an', 'emphmnjordan', 'derivation', 'if', 'mndeltaa... | [-0.1564477550350791, 0.14258635042952691, -0.0649061598759916, -0.04627580607665383, -0.05207703281717496, -0.2668839210517616, -0.059906395318223574, 0.3464697282430688, -0.40742184294486894, -0.03337914642696021, 0.07735369857001125, -0.34116121519015297, -0.07135103514539243, 0.14532535158637802, -0.119303829422407... |
1,803.02047 | Observation of topological phenomena in a programmable lattice of 1,800
qubits | The celebrated work of Berezinskii, Kosterlitz and Thouless in the 1970s
revealed exotic phases of matter governed by topological properties of
low-dimensional materials such as thin films of superfluids and
superconductors. Key to this phenomenon is the appearance and interaction of
vortices and antivortices in an a... | quant-ph cond-mat.stat-mech | the celebrated work of berezinskii kosterlitz and thouless in the 1970s revealed exotic phases of matter governed by topological properties of lowdimensional materials such as thin films of superfluids and superconductors key to this phenomenon is the appearance and interaction of vortices and antivortices in an angula... | [['the', 'celebrated', 'work', 'of', 'berezinskii', 'kosterlitz', 'and', 'thouless', 'in', 'the', '1970s', 'revealed', 'exotic', 'phases', 'of', 'matter', 'governed', 'by', 'topological', 'properties', 'of', 'lowdimensional', 'materials', 'such', 'as', 'thin', 'films', 'of', 'superfluids', 'and', 'superconductors', 'ke... | [-0.16633696861908864, 0.2113346860759298, -0.09237681294414932, 0.021856369145910052, -0.023433732036740994, -0.13991138150379892, 0.045002987030234046, 0.35304410515808754, -0.2536535198248667, -0.30793109757809745, 0.04291488111764592, -0.2731208022663374, -0.16767065080176027, 0.1835196755272876, 0.0073694889253812... |
1,803.02048 | Spatially dependent atom-photon entanglement | The atom-photon entanglement using the Laguerre-Gaussian beams is studied in
the closed-loop three-level $V$-type quantum systems. We consider two schemes
with degenerated and non-degenerated upper levels: in the first, the effect of
the quantum interference due to the spontaneous emission is taken into account
and i... | physics.optics quant-ph | the atomphoton entanglement using the laguerregaussian beams is studied in the closedloop threelevel vtype quantum systems we consider two schemes with degenerated and nondegenerated upper levels in the first the effect of the quantum interference due to the spontaneous emission is taken into account and in the second ... | [['the', 'atomphoton', 'entanglement', 'using', 'the', 'laguerregaussian', 'beams', 'is', 'studied', 'in', 'the', 'closedloop', 'threelevel', 'vtype', 'quantum', 'systems', 'we', 'consider', 'two', 'schemes', 'with', 'degenerated', 'and', 'nondegenerated', 'upper', 'levels', 'in', 'the', 'first', 'the', 'effect', 'of',... | [-0.16182334063929799, 0.20399814036514874, -0.0794142317262036, 0.04131738628928709, 0.007272761465624125, -0.12102617110558456, 0.017561951068916705, 0.38330978823759865, -0.25915970688102524, -0.2729537275836173, 0.043774380304526087, -0.23557682228133534, -0.08973937846409778, 0.23087430772644402, -0.00242712698180... |
1,803.02049 | Dynamical Phase Transition of two-component Bose-Einstein condensate
with nonlinear tunneling in an optomechanical cavity-mediated double-well
system | We investigate the dynamical phase transition of two-component Bose-Einstein
condensate with nonlinear tunneling, which is trapped inside a double-well and
dispersively coupled to a single mode of a high-finesse optical cavity with one
moving end mirror driven by a single mode standing field. The nonlinear
tunneling ... | quant-ph cond-mat.quant-gas | we investigate the dynamical phase transition of twocomponent boseeinstein condensate with nonlinear tunneling which is trapped inside a doublewell and dispersively coupled to a single mode of a highfinesse optical cavity with one moving end mirror driven by a single mode standing field the nonlinear tunneling interact... | [['we', 'investigate', 'the', 'dynamical', 'phase', 'transition', 'of', 'twocomponent', 'boseeinstein', 'condensate', 'with', 'nonlinear', 'tunneling', 'which', 'is', 'trapped', 'inside', 'a', 'doublewell', 'and', 'dispersively', 'coupled', 'to', 'a', 'single', 'mode', 'of', 'a', 'highfinesse', 'optical', 'cavity', 'wi... | [-0.21950006978087394, 0.2127903947401471, -0.07585661152556523, -0.034207035865805736, -0.006013670375532642, -0.19492924396466577, 0.06510615815368138, 0.33201224582117733, -0.2586155885792508, -0.2695226484947667, 0.028862554361397515, -0.2923103554022251, -0.10930237763238196, 0.1527240960098499, 0.0094961989754145... |
1,803.0205 | Characterizations of Jordan derivations on algebras of locally
measurable operators | We prove that if $\mathcal M$ is a properly infinite von Neumann algebra and
$LS(\mathcal M)$ is the local measurable operator algebra affiliated with
$\mathcal M$, then every Jordan derivation from $LS(\mathcal M)$ into itself is
continuous with respect to the local measure topology $t(\mathcal M)$. We
construct an ... | math.OA | we prove that if mathcal m is a properly infinite von neumann algebra and lsmathcal m is the local measurable operator algebra affiliated with mathcal m then every jordan derivation from lsmathcal m into itself is continuous with respect to the local measure topology tmathcal m we construct an extension of a jordan der... | [['we', 'prove', 'that', 'if', 'mathcal', 'm', 'is', 'a', 'properly', 'infinite', 'von', 'neumann', 'algebra', 'and', 'lsmathcal', 'm', 'is', 'the', 'local', 'measurable', 'operator', 'algebra', 'affiliated', 'with', 'mathcal', 'm', 'then', 'every', 'jordan', 'derivation', 'from', 'lsmathcal', 'm', 'into', 'itself', 'i... | [-0.15467521263302392, 0.09980384945487862, -0.10714477986001815, -0.05338565314499041, -0.10870609797027886, -0.1929393118709071, -0.0332500369896969, 0.3074568589934363, -0.33087109596046627, -0.1399614681642996, 0.09600480494256584, -0.3041041843019999, -0.09877991397729796, 0.15078671095080864, -0.1546364094938637,... |
1,803.02051 | Efficient Decentralized LTL Monitoring Framework Using Tableau Technique | This paper presents a novel framework for decentralized monitoring of Linear
Temporal Logic (LTL), under the situation where processes are synchronous,
uniform (i.e. all processes are peers), and the formula is represented as a
tableau. The tableau technique allows one to construct a semantic tree for the
input formu... | cs.LO | this paper presents a novel framework for decentralized monitoring of linear temporal logic ltl under the situation where processes are synchronous uniform ie all processes are peers and the formula is represented as a tableau the tableau technique allows one to construct a semantic tree for the input formula which can... | [['this', 'paper', 'presents', 'a', 'novel', 'framework', 'for', 'decentralized', 'monitoring', 'of', 'linear', 'temporal', 'logic', 'ltl', 'under', 'the', 'situation', 'where', 'processes', 'are', 'synchronous', 'uniform', 'ie', 'all', 'processes', 'are', 'peers', 'and', 'the', 'formula', 'is', 'represented', 'as', 'a... | [-0.10968773696698587, 0.06634850850510482, -0.10901246911309885, 0.08919475506708929, -0.14939800567191208, -0.18572385579234724, 0.10272963828844667, 0.42563565039273465, -0.2983352340644959, -0.28676662378605794, 0.0892559381152475, -0.21399379018561873, -0.10270067595904975, 0.214130762383116, -0.092350604411331, 0... |
1,803.02052 | A shrinking projection approximant for the split equilibrium problems
and fixed point problems in Hilbert spaces | This work is devoted to establish the strong convergence results of an
iterative algorithm generated by the shrinking projection method in Hilbert
spaces. The proposed approximation sequence is used to find a common element in
the set of solutions of a finite family of split equilibrium problems and the
set of common... | math.FA | this work is devoted to establish the strong convergence results of an iterative algorithm generated by the shrinking projection method in hilbert spaces the proposed approximation sequence is used to find a common element in the set of solutions of a finite family of split equilibrium problems and the set of common fi... | [['this', 'work', 'is', 'devoted', 'to', 'establish', 'the', 'strong', 'convergence', 'results', 'of', 'an', 'iterative', 'algorithm', 'generated', 'by', 'the', 'shrinking', 'projection', 'method', 'in', 'hilbert', 'spaces', 'the', 'proposed', 'approximation', 'sequence', 'is', 'used', 'to', 'find', 'a', 'common', 'ele... | [-0.09817409770091973, 0.026073648229820643, -0.08465398217450423, 0.0441328706556415, -0.03553211506938629, -0.04955475885667894, 0.05844771134083619, 0.3328317145715995, -0.2942555075432791, -0.23139562298465205, 0.11863375579551176, -0.2589681620249547, -0.14750842261969685, 0.1924772568450994, -0.11308161464957409,... |
1,803.02053 | Beam energy dependence of squeeze-out effect on the directed and
elliptic flow in Au+Au collisions at high baryon density region | We present a detailed analysis of the beam energy dependence of the
mechanisms for the generation of directed and elliptic flows in Au+Au
collisions focusing on the role of hadronic rescattering and spectator
shadowing within a microscopic transport model JAM with different equation of
state. A systematic study of th... | nucl-ex hep-ex hep-ph nucl-th | we present a detailed analysis of the beam energy dependence of the mechanisms for the generation of directed and elliptic flows in auau collisions focusing on the role of hadronic rescattering and spectator shadowing within a microscopic transport model jam with different equation of state a systematic study of the be... | [['we', 'present', 'a', 'detailed', 'analysis', 'of', 'the', 'beam', 'energy', 'dependence', 'of', 'the', 'mechanisms', 'for', 'the', 'generation', 'of', 'directed', 'and', 'elliptic', 'flows', 'in', 'auau', 'collisions', 'focusing', 'on', 'the', 'role', 'of', 'hadronic', 'rescattering', 'and', 'spectator', 'shadowing'... | [-0.11389436377870404, 0.29612363539636133, -0.15773779551179715, 0.11705864729035807, -0.008710264172607465, -0.09294869508138737, -0.07835586050616415, 0.3524030931941841, -0.23994357956107706, -0.30044178036851404, -0.08099699551188995, -0.3665742052779735, 0.05614184810699004, 0.12591127228832033, 0.074833059191334... |
1,803.02054 | Countable Markov Partitions Suitable for Thermodynamic Formalism | We study hyperbolic attractors of some dynamical systems with apriori given
countable Markov partitions. Assuming that contraction is stronger than
expansion we construct new Markov rectangles such that their crossections by
unstable manifolds are Cantor sets of positive Lebesgue measure. Using new
Markov partitions ... | math.DS | we study hyperbolic attractors of some dynamical systems with apriori given countable markov partitions assuming that contraction is stronger than expansion we construct new markov rectangles such that their crossections by unstable manifolds are cantor sets of positive lebesgue measure using new markov partitions we d... | [['we', 'study', 'hyperbolic', 'attractors', 'of', 'some', 'dynamical', 'systems', 'with', 'apriori', 'given', 'countable', 'markov', 'partitions', 'assuming', 'that', 'contraction', 'is', 'stronger', 'than', 'expansion', 'we', 'construct', 'new', 'markov', 'rectangles', 'such', 'that', 'their', 'crossections', 'by', '... | [-0.12406573323926455, 0.1768610197919565, -0.10732873460986245, 0.16638467158682801, -0.07994376244941648, -0.1329236381808558, 0.03522022424633024, 0.36105778530030186, -0.2716519077780696, -0.15785298089195096, 0.1367610921053557, -0.2908803781979835, -0.1274250836872404, 0.19080957579574037, -0.0543243998045128, 0.... |
1,803.02055 | Multi-scale simulations of black hole accretion in barred galaxies:
Numerical methods and tests | Due to the non-axisymmetric potential of the central bar, barred spiral
galaxies form, in addition to their characteristic arms and bar, a variety of
structures within the thin gas disk, like nuclear rings, inner spirals and
dust-lanes. In this first of two papers, we present a method to accurately
simulate the gas f... | astro-ph.GA physics.comp-ph | due to the nonaxisymmetric potential of the central bar barred spiral galaxies form in addition to their characteristic arms and bar a variety of structures within the thin gas disk like nuclear rings inner spirals and dustlanes in this first of two papers we present a method to accurately simulate the gas flow within ... | [['due', 'to', 'the', 'nonaxisymmetric', 'potential', 'of', 'the', 'central', 'bar', 'barred', 'spiral', 'galaxies', 'form', 'in', 'addition', 'to', 'their', 'characteristic', 'arms', 'and', 'bar', 'a', 'variety', 'of', 'structures', 'within', 'the', 'thin', 'gas', 'disk', 'like', 'nuclear', 'rings', 'inner', 'spirals'... | [-0.094610162749925, 0.030882643599232488, -0.11300314373090432, 0.08646841448912597, -0.07721776350532189, -0.06559661402913534, -0.004949933989743187, 0.36591446615201384, -0.2707008912482045, -0.2890380541870971, 0.03654362168740327, -0.19865888903833434, -0.0877304283290147, 0.20143585180679013, -0.0238846544414943... |
1,803.02056 | Imaginary quadratic number fields with class groups of small exponent | Let $D<0$ be a fundamental discriminant and denote by $E(D)$ the exponent of
the ideal class group $\text{Cl}(D)$ of $K={\mathbb Q}(\sqrt{D})$. Under the
assumption that no Siegel zeros exist we compute all such $D$ with $E(D)$ is a
divisor of $8$. We compute all $D$ with $|D|\leq 3.1\cdot 10^{20}$ such that
$E(D)\le... | math.NT | let d0 be a fundamental discriminant and denote by ed the exponent of the ideal class group textcld of kmathbb qsqrtd under the assumption that no siegel zeros exist we compute all such d with ed is a divisor of 8 we compute all d with dleq 31cdot 1020 such that edleq 8 | [['let', 'd0', 'be', 'a', 'fundamental', 'discriminant', 'and', 'denote', 'by', 'ed', 'the', 'exponent', 'of', 'the', 'ideal', 'class', 'group', 'textcld', 'of', 'kmathbb', 'qsqrtd', 'under', 'the', 'assumption', 'that', 'no', 'siegel', 'zeros', 'exist', 'we', 'compute', 'all', 'such', 'd', 'with', 'ed', 'is', 'a', 'di... | [-0.214015108384192, 0.11797596460208297, -0.07137705953791737, 0.004324259136337787, -0.03401262386818416, -0.17921023512259127, 0.0066570165543816985, 0.2709650640003383, -0.25771069768816235, -0.2486859583109617, 0.09610430303611793, -0.33971362303942443, -0.15231519553810358, 0.17923978311009706, 0.0126986725814640... |
1,803.02057 | The Earth ain't Flat: Monocular Reconstruction of Vehicles on Steep and
Graded Roads from a Moving Camera | Accurate localization of other traffic participants is a vital task in
autonomous driving systems. State-of-the-art systems employ a combination of
sensing modalities such as RGB cameras and LiDARs for localizing traffic
participants, but most such demonstrations have been confined to plain roads.
We demonstrate, to ... | cs.RO cs.CV cs.LG | accurate localization of other traffic participants is a vital task in autonomous driving systems stateoftheart systems employ a combination of sensing modalities such as rgb cameras and lidars for localizing traffic participants but most such demonstrations have been confined to plain roads we demonstrate to the best ... | [['accurate', 'localization', 'of', 'other', 'traffic', 'participants', 'is', 'a', 'vital', 'task', 'in', 'autonomous', 'driving', 'systems', 'stateoftheart', 'systems', 'employ', 'a', 'combination', 'of', 'sensing', 'modalities', 'such', 'as', 'rgb', 'cameras', 'and', 'lidars', 'for', 'localizing', 'traffic', 'partici... | [-0.09195367734631207, -0.003772312034152789, -0.06400423004973704, 0.00614281882702379, -0.08977190078939219, -0.14328112417612882, 0.01451680182347689, 0.45311207450877605, -0.2069506744703497, -0.3656537919700925, 0.07996887350272314, -0.2899360142136906, -0.1670501281726448, 0.23157548149697654, -0.1797380494349484... |
1,803.02058 | First-order optical spatial differentiator based on a guided-mode
resonant grating | We present an experimental demonstration of a subwavelength diffraction
grating performing first-order differentiation of the transverse profile of an
incident optical beam with respect to a spatial variable. The experimental
results are in a good agreement with the presented analytical model suggesting
that the diff... | physics.optics | we present an experimental demonstration of a subwavelength diffraction grating performing firstorder differentiation of the transverse profile of an incident optical beam with respect to a spatial variable the experimental results are in a good agreement with the presented analytical model suggesting that the differen... | [['we', 'present', 'an', 'experimental', 'demonstration', 'of', 'a', 'subwavelength', 'diffraction', 'grating', 'performing', 'firstorder', 'differentiation', 'of', 'the', 'transverse', 'profile', 'of', 'an', 'incident', 'optical', 'beam', 'with', 'respect', 'to', 'a', 'spatial', 'variable', 'the', 'experimental', 'res... | [-0.14073118806289345, 0.07020945192658366, -0.08887655020568191, -0.0036401572861530654, -0.03655343934866216, -0.10515819874468862, 0.024031921551795676, 0.4568544893837123, -0.2530569372123436, -0.3104365765761673, 0.0685011789045187, -0.2775250580641167, -0.1333226433420992, 0.21606215611031718, 0.00644551134695682... |
1,803.02059 | Ergodicity properties of $p$ -adic $(2,1)$-rational dynamical systems
with unique fixed point | We consider a family of $(2,1)$-rational functions given on the set of
$p$-adic field $Q_p$. Each such function has a unique fixed point. We study
ergodicity properties of the dynamical systems generated by $(2,1)$-rational
functions. For each such function we describe all possible invariant spheres.
We characterize ... | math.DS | we consider a family of 21rational functions given on the set of padic field q_p each such function has a unique fixed point we study ergodicity properties of the dynamical systems generated by 21rational functions for each such function we describe all possible invariant spheres we characterize ergodicity of each padi... | [['we', 'consider', 'a', 'family', 'of', '21rational', 'functions', 'given', 'on', 'the', 'set', 'of', 'padic', 'field', 'q_p', 'each', 'such', 'function', 'has', 'a', 'unique', 'fixed', 'point', 'we', 'study', 'ergodicity', 'properties', 'of', 'the', 'dynamical', 'systems', 'generated', 'by', '21rational', 'functions'... | [-0.2085723312090287, 0.12433453440666853, -0.1288712021549431, 0.07403329451793407, -0.0006083403007661024, -0.10864021588807528, -0.0028534313726626087, 0.3642751320024555, -0.3073191884591171, -0.1663881861114236, 0.09845636016754643, -0.2850983235357183, -0.17638263100590768, 0.18481899093669119, -0.078446003775834... |
1,803.0206 | A Dynamical Approach to the Perron-Frobenius Theory and Generalized
Krein-Rutman Type Theorems | We present a dynamical approach to the classical Perron-Frobenius theory by
using some elementary knowledge on linear ODEs. It is completely self-contained
and significantly different from those in the literature. As a result, we
develop a complex version of the Perron-Frobenius theory and prove some
generalized Krei... | math.FA | we present a dynamical approach to the classical perronfrobenius theory by using some elementary knowledge on linear odes it is completely selfcontained and significantly different from those in the literature as a result we develop a complex version of the perronfrobenius theory and prove some generalized kreinrutman ... | [['we', 'present', 'a', 'dynamical', 'approach', 'to', 'the', 'classical', 'perronfrobenius', 'theory', 'by', 'using', 'some', 'elementary', 'knowledge', 'on', 'linear', 'odes', 'it', 'is', 'completely', 'selfcontained', 'and', 'significantly', 'different', 'from', 'those', 'in', 'the', 'literature', 'as', 'a', 'result... | [-0.050696692163390775, 0.06398569826720929, -0.15668310988124232, 0.13811797971067455, -0.10801794163274522, -0.13440909474489413, 0.022627578734667326, 0.27102246515604916, -0.31443697913568847, -0.24214445005113983, 0.15404158138803073, -0.24325878615966257, -0.25461626516735864, 0.20433116734636073, -0.098309173134... |
1,803.02061 | Schr\"{o}dinger Equations on normal real form Symmetric Spaces | We prove dispersive and Strichartz estimates for Schr\"{o}dinger equations on
normal real form symmetric spaces. These estimates apply to the well-posedness
and scattering for the nonlinear Schr\"{o}dinger equations.
| math.AP | we prove dispersive and strichartz estimates for schrodinger equations on normal real form symmetric spaces these estimates apply to the wellposedness and scattering for the nonlinear schrodinger equations | [['we', 'prove', 'dispersive', 'and', 'strichartz', 'estimates', 'for', 'schrodinger', 'equations', 'on', 'normal', 'real', 'form', 'symmetric', 'spaces', 'these', 'estimates', 'apply', 'to', 'the', 'wellposedness', 'and', 'scattering', 'for', 'the', 'nonlinear', 'schrodinger', 'equations']] | [-0.0828766703738698, 0.032449836343792934, -0.04880947353584426, 0.16976650874961965, -0.1550155857777489, -0.1255880389695189, -0.10529459387596164, 0.31223925575613976, -0.27122080844960045, -0.11438887927215546, 0.16712067853326776, -0.3819949387772275, -0.15232737844676844, 0.26033825394032256, 0.01716257152812821... |
1,803.02062 | Intelligent Identification of Two-Dimensional Structure by
Machine-Learning Optical Microscopy | Two-dimensional (2D) materials and their heterostructures, with wafer-scale
synthesis methods and fascinating properties, have attracted numerous interest
and triggered revolutions of corresponding device applications. However, facile
methods to realize accurate, intelligent and large-area characterizations of
these ... | cond-mat.mtrl-sci | twodimensional 2d materials and their heterostructures with waferscale synthesis methods and fascinating properties have attracted numerous interest and triggered revolutions of corresponding device applications however facile methods to realize accurate intelligent and largearea characterizations of these 2d structure... | [['twodimensional', '2d', 'materials', 'and', 'their', 'heterostructures', 'with', 'waferscale', 'synthesis', 'methods', 'and', 'fascinating', 'properties', 'have', 'attracted', 'numerous', 'interest', 'and', 'triggered', 'revolutions', 'of', 'corresponding', 'device', 'applications', 'however', 'facile', 'methods', 't... | [-0.08124632506254822, 0.04894977918634495, -0.05946910528611418, -0.03742696775258882, -0.09174980518758191, -0.18295321687527583, 0.037429850323518726, 0.48792313209715044, -0.2543309896471018, -0.3443484863807969, 0.07529195312555906, -0.2749991003417324, -0.24658161246445665, 0.2860382731990717, -0.0352148631594229... |
1,803.02063 | Connection between zero-energy Yu-Shiba-Rusinov states and 0-$\pi$
transitions in magnetic Josephson junctions | We study the bound state spectrum and 0-$\pi$ transitions in ballistic
quasi-1D superconductor/ferromagnetic insulator/superconductor (S/FI/S)
Josephson junctions. In addition to the Andreev bound states, stemming from the
phase coherence, the magnetic barrier gives rise to qualitatively different
Yu-Shiba-Rusinov (Y... | cond-mat.supr-con | we study the bound state spectrum and 0pi transitions in ballistic quasi1d superconductorferromagnetic insulatorsuperconductor sfis josephson junctions in addition to the andreev bound states stemming from the phase coherence the magnetic barrier gives rise to qualitatively different yushibarusinov ysr bound states wit... | [['we', 'study', 'the', 'bound', 'state', 'spectrum', 'and', '0pi', 'transitions', 'in', 'ballistic', 'quasi1d', 'superconductorferromagnetic', 'insulatorsuperconductor', 'sfis', 'josephson', 'junctions', 'in', 'addition', 'to', 'the', 'andreev', 'bound', 'states', 'stemming', 'from', 'the', 'phase', 'coherence', 'the'... | [-0.28935305989407334, 0.22899564312273027, -0.08866152650501469, 0.08452369313627149, -0.032909017093110796, -0.21989553151560007, 0.10615884583434182, 0.3477020917810721, -0.2203407670823064, -0.2699040356922046, -0.08578718193497804, -0.33925122293726645, -0.12737131977481492, 0.1728825939975974, 0.03988520198012933... |
1,803.02064 | Comparative study on magnetoresistance of carbon-cobalt nanocomposite
thin films grown by pulsed laser deposition | We present a comparative study on the influence of applied magnetic field on
the resistance of $C_{1-x}Co_x$ thin films (with $x=0.1$, $0.15$ and $0.2$)
grown on $Si$ substrate by pulsed laser deposition technique. It is found that
the behavior of magnetoresistance (MR) drastically depends on the temperature.
Namely,... | cond-mat.mtrl-sci | we present a comparative study on the influence of applied magnetic field on the resistance of c_1xco_x thin films with x01 015 and 02 grown on si substrate by pulsed laser deposition technique it is found that the behavior of magnetoresistance mr drastically depends on the temperature namely at low temperatures mr is ... | [['we', 'present', 'a', 'comparative', 'study', 'on', 'the', 'influence', 'of', 'applied', 'magnetic', 'field', 'on', 'the', 'resistance', 'of', 'c_1xco_x', 'thin', 'films', 'with', 'x01', '015', 'and', '02', 'grown', 'on', 'si', 'substrate', 'by', 'pulsed', 'laser', 'deposition', 'technique', 'it', 'is', 'found', 'tha... | [-0.14327782614245302, 0.22927175117434845, -0.029745260830081645, -0.028568356700513203, 0.013243554916698486, -0.18711568024342082, 0.06583621488451692, 0.40428316679650117, -0.23053927907589933, -0.31538296052964315, 0.03188101161781344, -0.32896729319223333, -0.08870451486048599, 0.2487862944891233, 0.0456036114732... |
1,803.02065 | "So, Tell Me What Users Want, What They Really, Really Want!" | Equating users' true needs and desires with behavioural measures of
'engagement' is problematic. However, good metrics of 'true preferences' are
difficult to define, as cognitive biases make people's preferences change with
context and exhibit inconsistencies over time. Yet, HCI research often glosses
over the philos... | cs.CY | equating users true needs and desires with behavioural measures of engagement is problematic however good metrics of true preferences are difficult to define as cognitive biases make peoples preferences change with context and exhibit inconsistencies over time yet hci research often glosses over the philosophical and t... | [['equating', 'users', 'true', 'needs', 'and', 'desires', 'with', 'behavioural', 'measures', 'of', 'engagement', 'is', 'problematic', 'however', 'good', 'metrics', 'of', 'true', 'preferences', 'are', 'difficult', 'to', 'define', 'as', 'cognitive', 'biases', 'make', 'peoples', 'preferences', 'change', 'with', 'context',... | [-0.06329328557438674, 0.06875437363905129, -0.1190369127197536, 0.16043036202016217, -0.22164687729889043, -0.18948012927150423, 0.13473447128436183, 0.44765527459309884, -0.23901178404964782, -0.36620166720132585, 0.08091489926058178, -0.2779132057912648, -0.17015480779594294, 0.13810677965240623, -0.2021113374373979... |
1,803.02066 | Kinetics of island growth in the framework of planar diffusion zones and
3D nucleation and growth models for electrodeposition | In the electrochemical deposition of thin films the measurement of the
current-time curve does not allow for a direct determination of the nucleus
growth law, electrode surface coverage and mean film thickness. In this work we
present a theoretical approach suitable to gain insight into these quantities
from the know... | cond-mat.soft cond-mat.mtrl-sci | in the electrochemical deposition of thin films the measurement of the currenttime curve does not allow for a direct determination of the nucleus growth law electrode surface coverage and mean film thickness in this work we present a theoretical approach suitable to gain insight into these quantities from the knowledge... | [['in', 'the', 'electrochemical', 'deposition', 'of', 'thin', 'films', 'the', 'measurement', 'of', 'the', 'currenttime', 'curve', 'does', 'not', 'allow', 'for', 'a', 'direct', 'determination', 'of', 'the', 'nucleus', 'growth', 'law', 'electrode', 'surface', 'coverage', 'and', 'mean', 'film', 'thickness', 'in', 'this', ... | [-0.047836759021634805, 0.07120109933640549, -0.12424168009674039, 0.008218084489650066, -0.033759227036360175, -0.0856500547794201, 0.07431896216245276, 0.3860288233136629, -0.22818110112820078, -0.30028705291523794, 0.0652594563913172, -0.2621121908270634, -0.11423456011164823, 0.21928869630210102, -0.023249839506305... |
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