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 |
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1,801.08469 | Joint and Conditional Local Limit Theorems for Lattice Random Walks and
Their Occupation Measures | Let $S_n$ be a lattice random walk with mean zero and finite variance, and
let $\Lambda^a_n$ be its occupation measure at level $a$. In this note, we
prove local limit theorems for $\Pr[S_n=x,\Lambda^a_n=\ell]$ and
$\Pr[S_n=x|\Lambda^a_n=\ell]$ in the cases where $a$, $|x-a|$ and $\ell$ are
either zero or at least of... | math.PR | let s_n be a lattice random walk with mean zero and finite variance and let lambdaa_n be its occupation measure at level a in this note we prove local limit theorems for prs_nxlambdaa_nell and prs_nxlambdaa_nell in the cases where a xa and ell are either zero or at least of order sqrt n the asymptotic description of th... | [['let', 's_n', 'be', 'a', 'lattice', 'random', 'walk', 'with', 'mean', 'zero', 'and', 'finite', 'variance', 'and', 'let', 'lambdaa_n', 'be', 'its', 'occupation', 'measure', 'at', 'level', 'a', 'in', 'this', 'note', 'we', 'prove', 'local', 'limit', 'theorems', 'for', 'prs_nxlambdaa_nell', 'and', 'prs_nxlambdaa_nell', '... | [-0.07391250056865732, 0.15143804300465183, -0.13624374296895303, 0.009293998534504898, -0.016733758052629708, -0.1143969181900333, 0.07762709868540246, 0.3430474963764438, -0.26637479335696035, -0.2680481041789846, 0.12960522068536684, -0.30319112242586843, -0.10685617876222638, 0.1869121582877814, -0.0839372555626375... |
1,801.0847 | Scattering of electromagnetic waves from a cone with conformal mapping:
application to scanning near-field optical microscope | We study the response of a conical metallic surface to an external
electromagnetic (EM) field by representing the fields in basis functions
containing integrable singularities at the tip of the cone. A fast analytical
solution is obtained by the conformal mapping between the cone and a round
disk. We apply our calcul... | cond-mat.mes-hall | we study the response of a conical metallic surface to an external electromagnetic em field by representing the fields in basis functions containing integrable singularities at the tip of the cone a fast analytical solution is obtained by the conformal mapping between the cone and a round disk we apply our calculation ... | [['we', 'study', 'the', 'response', 'of', 'a', 'conical', 'metallic', 'surface', 'to', 'an', 'external', 'electromagnetic', 'em', 'field', 'by', 'representing', 'the', 'fields', 'in', 'basis', 'functions', 'containing', 'integrable', 'singularities', 'at', 'the', 'tip', 'of', 'the', 'cone', 'a', 'fast', 'analytical', '... | [-0.11258982032031027, 0.12358039666431546, -0.07959691975652004, 0.02727901429680395, -0.056625436532229595, -0.07692701295061115, 0.029236222067976603, 0.3651009508610321, -0.26117011567380294, -0.26656664255040824, 0.04377015067955419, -0.31871380217690964, -0.13239475597910721, 0.21375717413032316, 0.02117772218191... |
1,801.08471 | Affine Grassmannians in A^1-algebraic topology | Let k be a field. Denote by Spc(k)_* the unstable, pointed motivic homotopy
category and by Omega_Gm: Spc(k)_* \to Spc(k)_* the Gm-loops functor. For a
k-group G, denote by Gr_G the affine Grassmannian of G. If G is isotropic
reductive, we provide a canonical motivic equivalence Omega_Gm G = Gr_G. If k
is perfect, we... | math.AG math.AT math.KT | let k be a field denote by spck_ the unstable pointed motivic homotopy category and by omega_gm spck_ to spck_ the gmloops functor for a kgroup g denote by gr_g the affine grassmannian of g if g is isotropic reductive we provide a canonical motivic equivalence omega_gm g gr_g if k is perfect we use this to compute the ... | [['let', 'k', 'be', 'a', 'field', 'denote', 'by', 'spck_', 'the', 'unstable', 'pointed', 'motivic', 'homotopy', 'category', 'and', 'by', 'omega_gm', 'spck_', 'to', 'spck_', 'the', 'gmloops', 'functor', 'for', 'a', 'kgroup', 'g', 'denote', 'by', 'gr_g', 'the', 'affine', 'grassmannian', 'of', 'g', 'if', 'g', 'is', 'isotr... | [-0.26938455753394813, 0.10475010351567972, -0.1484451174552812, -0.0049723656294623116, -0.15567539143757742, -0.1680912523622029, 0.004066536813730099, 0.34688127004220837, -0.39329804370149235, -0.16276692588370842, -0.014879278600078504, -0.18359753963648204, -0.10548231210635944, 0.14665583145545155, -0.1777744300... |
1,801.08472 | $L_\infty$-resolutions and twisting in the curved context | In this short note we describe an alternative global version of the twisting
procedure used by Dolgushev to prove formality theorems. This allows us to
describe the maps of Fedosov resolutions, which are key factors of the
formality morphisms, in terms of a twist of the fiberwise quasi-isomorphisms
induced by the loc... | math.QA | in this short note we describe an alternative global version of the twisting procedure used by dolgushev to prove formality theorems this allows us to describe the maps of fedosov resolutions which are key factors of the formality morphisms in terms of a twist of the fiberwise quasiisomorphisms induced by the local for... | [['in', 'this', 'short', 'note', 'we', 'describe', 'an', 'alternative', 'global', 'version', 'of', 'the', 'twisting', 'procedure', 'used', 'by', 'dolgushev', 'to', 'prove', 'formality', 'theorems', 'this', 'allows', 'us', 'to', 'describe', 'the', 'maps', 'of', 'fedosov', 'resolutions', 'which', 'are', 'key', 'factors',... | [-0.1582936478337567, 0.011664147547899599, -0.12168594354665593, 0.10193952194684626, -0.07251582176571614, -0.0865797734280166, -0.010145312175154686, 0.3336277821738469, -0.3568640182677068, -0.25038540647610236, 0.053942884441073, -0.14048868377086413, -0.1742747040955644, 0.17252308082227644, -0.21445774590078814,... |
1,801.08473 | Black hole quasibound states from a draining bathtub vortex flow | Quasinormal modes are a set of damped resonances that describe how an excited
open system is driven back to equilibrium. In gravitational physics these modes
characterise the ringdown of a perturbed black hole, e.g. following a binary
black hole merger. A careful analysis of the ringdown spectrum reveals the
properti... | gr-qc | quasinormal modes are a set of damped resonances that describe how an excited open system is driven back to equilibrium in gravitational physics these modes characterise the ringdown of a perturbed black hole eg following a binary black hole merger a careful analysis of the ringdown spectrum reveals the properties of t... | [['quasinormal', 'modes', 'are', 'a', 'set', 'of', 'damped', 'resonances', 'that', 'describe', 'how', 'an', 'excited', 'open', 'system', 'is', 'driven', 'back', 'to', 'equilibrium', 'in', 'gravitational', 'physics', 'these', 'modes', 'characterise', 'the', 'ringdown', 'of', 'a', 'perturbed', 'black', 'hole', 'eg', 'fol... | [-0.1806681287199992, 0.1427298601987051, -0.10503727814895993, 0.0904566677110121, -0.09900966010358621, -0.10087655524802493, -0.0024107923784461665, 0.2888467729319521, -0.18643276255696695, -0.2593450947748893, 0.07351165872371875, -0.2889647334579538, -0.12728555181479834, 0.23573046255772537, -0.00852684451309230... |
1,801.08474 | Adaptive covariance inflation in the ensemble Kalman filter by Gaussian
scale mixtures | This paper studies multiplicative inflation: the complementary scaling of the
state covariance in the ensemble Kalman filter (EnKF). Firstly, error sources
in the EnKF are catalogued and discussed in relation to inflation; nonlinearity
is given particular attention as a source of sampling error. In response, the
"fin... | physics.data-an nlin.CD stat.AP | this paper studies multiplicative inflation the complementary scaling of the state covariance in the ensemble kalman filter enkf firstly error sources in the enkf are catalogued and discussed in relation to inflation nonlinearity is given particular attention as a source of sampling error in response the finitesize ref... | [['this', 'paper', 'studies', 'multiplicative', 'inflation', 'the', 'complementary', 'scaling', 'of', 'the', 'state', 'covariance', 'in', 'the', 'ensemble', 'kalman', 'filter', 'enkf', 'firstly', 'error', 'sources', 'in', 'the', 'enkf', 'are', 'catalogued', 'and', 'discussed', 'in', 'relation', 'to', 'inflation', 'nonl... | [-0.0640536922458806, 0.04528714161341554, -0.13185834348670497, 0.09254685191850838, -0.059737955090521974, -0.18337793127843333, 0.013348642498445975, 0.39897008797782935, -0.249592769453117, -0.2938741181995596, 0.13831067302292027, -0.24898863018225162, -0.16531068676256186, 0.20234760216788839, -0.1156732801761206... |
1,801.08475 | Explicit formula for the average of Goldbach and prime tuples
representations | Let $\Lambda\left(n\right)$ be the Von Mangoldt function, let \[
r_{G}\left(n\right)=\underset{{\scriptstyle
m_{1}+m_{2}=n}}{\sum_{m_{1},m_{2}\leq
n}}\Lambda\left(m_{1}\right)\Lambda\left(m_{2}\right), \] \[
r_{PT}\left(N,h\right)=\sum_{n=0}^{N}\Lambda\left(n\right)\Lambda\left(n+h\right),\,h\in\mathbb{N}
\] be the c... | math.NT | let lambdaleftnright be the von mangoldt function let r_gleftnrightundersetscriptstyle m_1m_2nsum_m_1m_2leq nlambdaleftm_1rightlambdaleftm_2right r_ptleftnhrightsum_n0nlambdaleftnrightlambdaleftnhrighthinmathbbn be the counting function of the goldbach numbers and the counting function of the prime tuples respectively ... | [['let', 'lambdaleftnright', 'be', 'the', 'von', 'mangoldt', 'function', 'let', 'r_gleftnrightundersetscriptstyle', 'm_1m_2nsum_m_1m_2leq', 'nlambdaleftm_1rightlambdaleftm_2right', 'r_ptleftnhrightsum_n0nlambdaleftnrightlambdaleftnhrighthinmathbbn', 'be', 'the', 'counting', 'function', 'of', 'the', 'goldbach', 'numbers... | [-0.1611921598625211, 0.10405148164047102, -0.12853109444720004, 0.0843412945626901, -0.037055013499240265, -0.0809972899403634, 0.03984474963596407, 0.2916555486988487, -0.2655615005817897, -0.26406429345139637, 0.08822795070206993, -0.29922934943142365, -0.13655160295058763, 0.22038458733828212, -0.03887843511963509,... |
1,801.08476 | A note on the Bloch representation of absolutely maximally entangled
states | The absolutely maximally entangled (AME) states play key roles in quantum
information processing. We provide an explicit expression of the generalized
Bloch representation of AME states for general dimension $d$ of individual
subsystems and arbitrary number of partite $n$. Based on this analytic formula,
we prove tha... | quant-ph | the absolutely maximally entangled ame states play key roles in quantum information processing we provide an explicit expression of the generalized bloch representation of ame states for general dimension d of individual subsystems and arbitrary number of partite n based on this analytic formula we prove that the trace... | [['the', 'absolutely', 'maximally', 'entangled', 'ame', 'states', 'play', 'key', 'roles', 'in', 'quantum', 'information', 'processing', 'we', 'provide', 'an', 'explicit', 'expression', 'of', 'the', 'generalized', 'bloch', 'representation', 'of', 'ame', 'states', 'for', 'general', 'dimension', 'd', 'of', 'individual', '... | [-0.16387782445304938, 0.14687145019239065, -0.0884951710117353, 0.0635363064578823, -0.0007543209593720912, -0.14932586418442606, 0.03893636229969118, 0.29280181696993257, -0.20338432723656297, -0.2261841273423107, 0.06442684434503983, -0.2703623430348844, -0.14251287449761071, 0.1712032069585153, -0.01950214347536010... |
1,801.08477 | A Theory of Traffic Regulators for Deterministic Networks with
Application to Interleaved Regulators | We define the minimal interleaved regulator, which generalizes the Urgency
Based Shaper that was recently proposed by Specht and Samii as a simpler
alternative to per-flow reshaping in deterministic networks with aggregate
scheduling. With this regulator, packets of multiple flows are processed in one
FIFO queue; the... | cs.NI | we define the minimal interleaved regulator which generalizes the urgency based shaper that was recently proposed by specht and samii as a simpler alternative to perflow reshaping in deterministic networks with aggregate scheduling with this regulator packets of multiple flows are processed in one fifo queue the packet... | [['we', 'define', 'the', 'minimal', 'interleaved', 'regulator', 'which', 'generalizes', 'the', 'urgency', 'based', 'shaper', 'that', 'was', 'recently', 'proposed', 'by', 'specht', 'and', 'samii', 'as', 'a', 'simpler', 'alternative', 'to', 'perflow', 'reshaping', 'in', 'deterministic', 'networks', 'with', 'aggregate', '... | [-0.17343071056449408, 0.07767970300198282, -0.10028737687939254, 0.05169904195598417, -0.08374472817165717, -0.19127310531815805, 0.10254334509887729, 0.3674894726710729, -0.3045121939597471, -0.25444382699506896, 0.13344334093059845, -0.2400204383055701, -0.13415181967494194, 0.17654833256820654, -0.12347396779462078... |
1,801.08478 | Small-amplitude static periodic patterns at a fluid-ferrofluid interface | We establish the existence of static doubly periodic patterns (in particular
rolls, rectangles and hexagons) on the free surface of a ferrofluid near onset
of the Rosensweig instability, assuming a general (nonlinear) magnetisation
law. A novel formulation of the ferrohydrostatic equations in terms of
Dirichlet- Neum... | math.AP | we establish the existence of static doubly periodic patterns in particular rolls rectangles and hexagons on the free surface of a ferrofluid near onset of the rosensweig instability assuming a general nonlinear magnetisation law a novel formulation of the ferrohydrostatic equations in terms of dirichlet neumann operat... | [['we', 'establish', 'the', 'existence', 'of', 'static', 'doubly', 'periodic', 'patterns', 'in', 'particular', 'rolls', 'rectangles', 'and', 'hexagons', 'on', 'the', 'free', 'surface', 'of', 'a', 'ferrofluid', 'near', 'onset', 'of', 'the', 'rosensweig', 'instability', 'assuming', 'a', 'general', 'nonlinear', 'magnetisa... | [-0.17254394399604261, 0.0934976265412071, -0.07822134736643145, 0.07314637382491257, -0.10463771672750061, -0.11932066085776596, 0.006538770676618724, 0.2635015851860358, -0.3050854404202916, -0.2072545083579513, 0.16468526502586714, -0.2639523922663295, -0.14961086543549718, 0.19666555263995747, -0.05996019979280354,... |
1,801.08479 | An axially-variant kernel imaging model applied to ultrasound image
reconstruction | Existing ultrasound deconvolution approaches unrealistically assume,
primarily for computational reasons, that the convolution model relies on a
spatially invariant kernel and circulant boundary conditions. We discard both
restrictions and introduce an image formation model applicable to ultrasound
imaging and deconv... | eess.SP | existing ultrasound deconvolution approaches unrealistically assume primarily for computational reasons that the convolution model relies on a spatially invariant kernel and circulant boundary conditions we discard both restrictions and introduce an image formation model applicable to ultrasound imaging and deconvoluti... | [['existing', 'ultrasound', 'deconvolution', 'approaches', 'unrealistically', 'assume', 'primarily', 'for', 'computational', 'reasons', 'that', 'the', 'convolution', 'model', 'relies', 'on', 'a', 'spatially', 'invariant', 'kernel', 'and', 'circulant', 'boundary', 'conditions', 'we', 'discard', 'both', 'restrictions', '... | [-0.032267694306508526, -0.012708899308950274, -0.09862106653502373, 0.08212826556918454, -0.0879181517970081, -0.18101857125201798, -0.02514784876486345, 0.42944208186442456, -0.2668851686744239, -0.2951872011148884, 0.1504177665447919, -0.20328719413465285, -0.15758475247590883, 0.19500351429588755, -0.10310319070814... |
1,801.0848 | An Integrated Soft Computing Approach to a Multi-biometric Security
Model | The abstract of the thesis consists of three sections, videlicet,
Motivation
Chapter Organization
Salient Contributions.
The complete abstract is included with the thesis. The final section on
Salient Contributions is reproduced below.
Salient Contributions
The research presents the following salient cont... | cs.CV cs.CY | the abstract of the thesis consists of three sections videlicet motivation chapter organization salient contributions the complete abstract is included with the thesis the final section on salient contributions is reproduced below salient contributions the research presents the following salient contributions i a novel... | [['the', 'abstract', 'of', 'the', 'thesis', 'consists', 'of', 'three', 'sections', 'videlicet', 'motivation', 'chapter', 'organization', 'salient', 'contributions', 'the', 'complete', 'abstract', 'is', 'included', 'with', 'the', 'thesis', 'the', 'final', 'section', 'on', 'salient', 'contributions', 'is', 'reproduced', ... | [-0.07861946783796475, 0.051090752650787566, -0.0742055516314219, 0.07901426542268478, -0.0798209320749728, -0.15873089312726893, 0.07246679078117156, 0.35500677867808883, -0.26415162200206205, -0.3538266257709709, 0.08279978091422092, -0.2974094567653721, -0.10664531701497668, 0.15938236757197924, -0.08618586310854369... |
1,801.08481 | A Gravitationally Lensed Quasar Discovered in OGLE | We report the discovery of a new gravitationally lensed quasar (double) from
the Optical Gravitational Lensing Experiment (OGLE) identified inside the
$\sim$670 sq. deg area encompassing the Magellanic Clouds. The source was
selected as one of $\sim$60 "red W1-W2" mid-IR objects from WISE and having a
significant amo... | astro-ph.GA | we report the discovery of a new gravitationally lensed quasar double from the optical gravitational lensing experiment ogle identified inside the sim670 sq deg area encompassing the magellanic clouds the source was selected as one of sim60 red w1w2 midir objects from wise and having a significant amount of variability... | [['we', 'report', 'the', 'discovery', 'of', 'a', 'new', 'gravitationally', 'lensed', 'quasar', 'double', 'from', 'the', 'optical', 'gravitational', 'lensing', 'experiment', 'ogle', 'identified', 'inside', 'the', 'sim670', 'sq', 'deg', 'area', 'encompassing', 'the', 'magellanic', 'clouds', 'the', 'source', 'was', 'selec... | [-0.06448272567464632, 0.055939440805972976, -0.05344481139565522, 0.06546373355720954, -0.09848780423000625, -0.1093871553322639, 0.047558275424870025, 0.43554874496026474, -0.13179266465158435, -0.3513293240134689, 0.04821867901112207, -0.37210944713601335, -0.01195076295539779, 0.20700011566831647, -0.02932425367603... |
1,801.08482 | Dust in brown dwarfs and extra-solar planets VI. Assessing seed
formation across the brown dwarf and exoplanet regimes | The cloud formation process starts with the formation of seed particles,
after which, surface chemical reactions grow or erode the cloud particles. We
investigate which materials may form cloud condensation seeds in the gas
temperature and pressure regimes (T$_{\rm gas}$ = 100-2000 K, p$_{\rm gas}$ =
10$^{-8}$-100 ba... | astro-ph.EP astro-ph.SR | the cloud formation process starts with the formation of seed particles after which surface chemical reactions grow or erode the cloud particles we investigate which materials may form cloud condensation seeds in the gas temperature and pressure regimes t_rm gas 1002000 k p_rm gas 108100 bar expected to occur in planet... | [['the', 'cloud', 'formation', 'process', 'starts', 'with', 'the', 'formation', 'of', 'seed', 'particles', 'after', 'which', 'surface', 'chemical', 'reactions', 'grow', 'or', 'erode', 'the', 'cloud', 'particles', 'we', 'investigate', 'which', 'materials', 'may', 'form', 'cloud', 'condensation', 'seeds', 'in', 'the', 'g... | [-0.07192633573556252, 0.23894742901295882, -0.046644212135496285, 0.05980212762555733, -0.00862261757824204, -0.09223313053475327, 0.10898812647324771, 0.34637309672793243, -0.2355156369573836, -0.33079699119636125, 0.04666857777920086, -0.2616409043475869, 0.009379668346809922, 0.1606440012240325, 0.03423306730525967... |
1,801.08483 | Field Theory of Disordered Elastic Interfaces at 3-Loop Order: The
$\beta$-Function | We calculate the effective action for disordered elastic manifolds in the
ground state (equilibrium) up to 3-loop order. This yields the
renormalization-group $\beta$-function to third order in $\epsilon=4-d$, in an
expansion in the dimension $d$ around the upper critical dimension $d=4$. The
calculations are perform... | cond-mat.dis-nn | we calculate the effective action for disordered elastic manifolds in the ground state equilibrium up to 3loop order this yields the renormalizationgroup betafunction to third order in epsilon4d in an expansion in the dimension d around the upper critical dimension d4 the calculations are performed using exact rg and s... | [['we', 'calculate', 'the', 'effective', 'action', 'for', 'disordered', 'elastic', 'manifolds', 'in', 'the', 'ground', 'state', 'equilibrium', 'up', 'to', '3loop', 'order', 'this', 'yields', 'the', 'renormalizationgroup', 'betafunction', 'to', 'third', 'order', 'in', 'epsilon4d', 'in', 'an', 'expansion', 'in', 'the', '... | [-0.1370274507687153, 0.13037297045593732, -0.09646082530825344, 0.06901238290832706, -0.02542566620361279, -0.10856615283581264, 0.04136866928242585, 0.3028091617503806, -0.21356137618696427, -0.2700966716853573, 0.08200642424772549, -0.3384773933931309, -0.11087528379935332, 0.1364615858936518, 0.05020578128888326, 0... |
1,801.08484 | Arbitrary-order functionally fitted energy-diminishing methods for
gradient systems | It is well known that for gradient systems in Euclidean space or on a
Riemannian manifold, the energy decreases monotonically along solutions. In
this letter we derive and analyse functionally fitted energy-diminishing
methods to preserve this key property of gradient systems. It is proved that
the novel methods are ... | math.NA | it is well known that for gradient systems in euclidean space or on a riemannian manifold the energy decreases monotonically along solutions in this letter we derive and analyse functionally fitted energydiminishing methods to preserve this key property of gradient systems it is proved that the novel methods are uncond... | [['it', 'is', 'well', 'known', 'that', 'for', 'gradient', 'systems', 'in', 'euclidean', 'space', 'or', 'on', 'a', 'riemannian', 'manifold', 'the', 'energy', 'decreases', 'monotonically', 'along', 'solutions', 'in', 'this', 'letter', 'we', 'derive', 'and', 'analyse', 'functionally', 'fitted', 'energydiminishing', 'metho... | [-0.113841973941284, 0.03927732176250882, -0.0847842265673057, 0.08042006610982082, -0.03778901193855387, -0.14524151993482703, -0.012127956549514724, 0.4326517918720992, -0.27248670322340773, -0.29203917567778115, 0.14118264875000794, -0.2692098930064175, -0.16541887284726883, 0.24903398878740693, -0.10398799281231025... |
1,801.08485 | Sine Cosine Crow Search Algorithm: A powerful hybrid meta heuristic for
global optimization | This paper presents a novel hybrid algorithm named Since Cosine Crow Search
Algorithm. To propose the SCCSA, two novel algorithms are considered including
Crow Search Algorithm (CSA) and Since Cosine Algorithm (SCA). The advantages of
the two algorithms are considered and utilize to design an efficient hybrid
algorit... | cs.NE | this paper presents a novel hybrid algorithm named since cosine crow search algorithm to propose the sccsa two novel algorithms are considered including crow search algorithm csa and since cosine algorithm sca the advantages of the two algorithms are considered and utilize to design an efficient hybrid algorithm which ... | [['this', 'paper', 'presents', 'a', 'novel', 'hybrid', 'algorithm', 'named', 'since', 'cosine', 'crow', 'search', 'algorithm', 'to', 'propose', 'the', 'sccsa', 'two', 'novel', 'algorithms', 'are', 'considered', 'including', 'crow', 'search', 'algorithm', 'csa', 'and', 'since', 'cosine', 'algorithm', 'sca', 'the', 'adva... | [-0.07947301552423781, -0.04483642029133034, -0.12628262869271814, 0.07219142852902562, -0.11177682089106322, -0.19741343977758502, 0.045945316591592095, 0.4407334385471324, -0.25041239647100033, -0.3724268982344765, 0.05783993362595122, -0.21244134479281257, -0.24514254984461656, 0.24879003829575316, -0.05547370857922... |
1,801.08486 | Self-Learning to Detect and Segment Cysts in Lung CT Images without
Manual Annotation | Image segmentation is a fundamental problem in medical image analysis. In
recent years, deep neural networks achieve impressive performances on many
medical image segmentation tasks by supervised learning on large manually
annotated data. However, expert annotations on big medical datasets are
tedious, expensive or s... | cs.CV | image segmentation is a fundamental problem in medical image analysis in recent years deep neural networks achieve impressive performances on many medical image segmentation tasks by supervised learning on large manually annotated data however expert annotations on big medical datasets are tedious expensive or sometime... | [['image', 'segmentation', 'is', 'a', 'fundamental', 'problem', 'in', 'medical', 'image', 'analysis', 'in', 'recent', 'years', 'deep', 'neural', 'networks', 'achieve', 'impressive', 'performances', 'on', 'many', 'medical', 'image', 'segmentation', 'tasks', 'by', 'supervised', 'learning', 'on', 'large', 'manually', 'ann... | [0.05599926275497211, -0.018658540415704066, -0.015752175696378136, 0.09628162879488189, -0.1437623817531139, -0.20496508688091036, 0.03722707423048071, 0.48672260503273135, -0.19432263576460104, -0.364009914799007, 0.08592400535866389, -0.2717850512572001, -0.1660338870061412, 0.20972120076458164, -0.22827612558655716... |
1,801.08487 | Coarse-grained patterns in multiplex networks | A new class of patterns for multiplex networks is studied, which consists in
a collection of different homogeneous states each referred to a distinct layer.
The associated stability diagram exhibits a tricritical point, as a function of
the inter-layer diffusion coefficients. The coarse-grained patterns made of
alter... | cond-mat.stat-mech | a new class of patterns for multiplex networks is studied which consists in a collection of different homogeneous states each referred to a distinct layer the associated stability diagram exhibits a tricritical point as a function of the interlayer diffusion coefficients the coarsegrained patterns made of alternating h... | [['a', 'new', 'class', 'of', 'patterns', 'for', 'multiplex', 'networks', 'is', 'studied', 'which', 'consists', 'in', 'a', 'collection', 'of', 'different', 'homogeneous', 'states', 'each', 'referred', 'to', 'a', 'distinct', 'layer', 'the', 'associated', 'stability', 'diagram', 'exhibits', 'a', 'tricritical', 'point', 'a... | [-0.20139736593277616, 0.17689933810086753, -0.05596570800143209, 0.023540227610448546, -0.059400572421410204, -0.15481442920122804, 0.08428521276536313, 0.32373920807784257, -0.3444728860123591, -0.23034283204258166, 0.041326860036827964, -0.24566256535366515, -0.19924365217712792, 0.12716032257303594, 0.0334927462528... |
1,801.08488 | Statistical overview of BRITE targets observed so far | We characterize BRITE data obtained between 2013 and 2017 in the first 21
BRITE observing fields. Then, we overview the sample of 426 stars observed so
far by the BRITE satellites. The review shows that BRITEs provide unique and
precise space photometry, which allows to obtain outstanding scientific results
in many a... | astro-ph.SR | we characterize brite data obtained between 2013 and 2017 in the first 21 brite observing fields then we overview the sample of 426 stars observed so far by the brite satellites the review shows that brites provide unique and precise space photometry which allows to obtain outstanding scientific results in many areas o... | [['we', 'characterize', 'brite', 'data', 'obtained', 'between', '2013', 'and', '2017', 'in', 'the', 'first', '21', 'brite', 'observing', 'fields', 'then', 'we', 'overview', 'the', 'sample', 'of', '426', 'stars', 'observed', 'so', 'far', 'by', 'the', 'brite', 'satellites', 'the', 'review', 'shows', 'that', 'brites', 'pr... | [-0.04663198927624358, 0.08019192283973098, -0.09441090675277843, 0.08942830317688209, -0.1397460774578913, -0.012282588415675692, 0.06281867885479221, 0.3754718655858327, -0.1825651184534999, -0.43725489050632826, 0.1069359471277696, -0.29364524459648506, -0.13197629070944256, 0.2759594741725811, -0.09653949747896856,... |
1,801.08489 | Microstructural control of the transport properties of $\beta$-FeSe
films grown by sputtering | We have investigated the correlation between structural and transport
properties in sputtered $\beta$-FeSe films grown onto SrTiO$_3$ (100). The
growth parameters, such as substrate temperature and thickness, have been
varied in order to explore different regimes. In the limit of textured thick
films, we found promis... | cond-mat.supr-con | we have investigated the correlation between structural and transport properties in sputtered betafese films grown onto srtio_3 100 the growth parameters such as substrate temperature and thickness have been varied in order to explore different regimes in the limit of textured thick films we found promising features li... | [['we', 'have', 'investigated', 'the', 'correlation', 'between', 'structural', 'and', 'transport', 'properties', 'in', 'sputtered', 'betafese', 'films', 'grown', 'onto', 'srtio_3', '100', 'the', 'growth', 'parameters', 'such', 'as', 'substrate', 'temperature', 'and', 'thickness', 'have', 'been', 'varied', 'in', 'order'... | [-0.14759353789637183, 0.17647002989835484, -0.0456624646960735, -0.0019950267916301083, -0.027199277059436297, -0.10349247082265764, 0.05219955916982144, 0.43044409363121705, -0.2822496960416618, -0.2957927535696909, 0.07051386039777909, -0.29664621540208963, -0.14890197866664426, 0.183707153776706, 0.0305453781932933... |
1,801.0849 | Tempered distributions with discrete support and spectrum | We investigate properties of tempered distributions with discrete or
countable supports such that their Fourier transforms are distributions with
discrete or countable supports as well. We find sufficient conditions for
support of the distribution to be a finite union of translations of a full-rank
lattice.
| math.CA | we investigate properties of tempered distributions with discrete or countable supports such that their fourier transforms are distributions with discrete or countable supports as well we find sufficient conditions for support of the distribution to be a finite union of translations of a fullrank lattice | [['we', 'investigate', 'properties', 'of', 'tempered', 'distributions', 'with', 'discrete', 'or', 'countable', 'supports', 'such', 'that', 'their', 'fourier', 'transforms', 'are', 'distributions', 'with', 'discrete', 'or', 'countable', 'supports', 'as', 'well', 'we', 'find', 'sufficient', 'conditions', 'for', 'support'... | [-0.10222206881476772, 0.18021678208476968, -0.1457130511601766, 0.08299663048237563, -0.10809666157907082, -0.05981731269922522, 0.04507872479864293, 0.4592761018209987, -0.29682104852464464, -0.17403525859117508, 0.16217631734907628, -0.24135799552831386, -0.03701633379484216, 0.15366810369046613, -0.0571978714213603... |
1,801.08491 | Time-reversal of rank-one quantum strategy functions | The quantum strategy (or quantum combs) framework is a useful tool for
reasoning about interactions among entities that process and exchange quantum
information over the course of multiple turns. We prove a time-reversal
property for a class of linear functions, defined on quantum strategy
representations within this... | quant-ph | the quantum strategy or quantum combs framework is a useful tool for reasoning about interactions among entities that process and exchange quantum information over the course of multiple turns we prove a timereversal property for a class of linear functions defined on quantum strategy representations within this framew... | [['the', 'quantum', 'strategy', 'or', 'quantum', 'combs', 'framework', 'is', 'a', 'useful', 'tool', 'for', 'reasoning', 'about', 'interactions', 'among', 'entities', 'that', 'process', 'and', 'exchange', 'quantum', 'information', 'over', 'the', 'course', 'of', 'multiple', 'turns', 'we', 'prove', 'a', 'timereversal', 'p... | [-0.13244334888755718, 0.14551558522981028, -0.10140093507934987, 0.07579191556466067, -0.05747534398427372, -0.144682091222937, 0.07142745721876732, 0.3688821199058152, -0.31587616654474343, -0.24025906995633867, 0.07812547349933979, -0.24888351659373895, -0.1858871484109298, 0.22286236180868277, -0.0429622147930786, ... |
1,801.08492 | Bounds on special values of L-functions of elliptic curves in an
Artin-Schreier family | In this paper, we study a certain Artin--Schreier family of elliptic curves
over the function field $\mathbb{F}_q(t)$. We prove an asymptotic estimate on
the size of the special value of their $L$-function in terms of the degree of
their conductor; loosely speaking, we show that the special values are
"asymptotically... | math.NT | in this paper we study a certain artinschreier family of elliptic curves over the function field mathbbf_qt we prove an asymptotic estimate on the size of the special value of their lfunction in terms of the degree of their conductor loosely speaking we show that the special values are asymptotically as large as possib... | [['in', 'this', 'paper', 'we', 'study', 'a', 'certain', 'artinschreier', 'family', 'of', 'elliptic', 'curves', 'over', 'the', 'function', 'field', 'mathbbf_qt', 'we', 'prove', 'an', 'asymptotic', 'estimate', 'on', 'the', 'size', 'of', 'the', 'special', 'value', 'of', 'their', 'lfunction', 'in', 'terms', 'of', 'the', 'd... | [-0.19715310464637864, 0.011532704160827937, -0.1533195192604202, 0.07778922429893463, -0.05484680389672254, -0.05835085366316865, 0.00872341464417863, 0.27635603020198446, -0.27981768268267665, -0.26363928143380094, 0.09572795570098622, -0.25015707181115526, -0.15425690669675596, 0.2893365492582717, -0.127879876832980... |
1,801.08493 | The $l$ dependence of the helion optical model potential and the
undularity of the $l$-independent equivalent | The relationship between $l$-dependence and undularity of the optical model
potential (OMP) is studied for the case of the elastic scattering of 33 MeV
\nuc{3}{He} on $^{58}$Ni. The relationship that emerges follows the general
features of the same relationship found for the proton OMP presented in
arXiv:1705.07003. ... | nucl-th | the relationship between ldependence and undularity of the optical model potential omp is studied for the case of the elastic scattering of 33 mev nuc3he on 58ni the relationship that emerges follows the general features of the same relationship found for the proton omp presented in arxiv170507003 the general backgroun... | [['the', 'relationship', 'between', 'ldependence', 'and', 'undularity', 'of', 'the', 'optical', 'model', 'potential', 'omp', 'is', 'studied', 'for', 'the', 'case', 'of', 'the', 'elastic', 'scattering', 'of', '33', 'mev', 'nuc3he', 'on', '58ni', 'the', 'relationship', 'that', 'emerges', 'follows', 'the', 'general', 'fea... | [-0.07820806247009723, 0.10840949251023294, -0.08564507520619642, 0.1230256892438909, 0.002099384339763438, -0.10179840620171658, 0.021292125530264997, 0.3742844506546303, -0.24321095500555304, -0.248637311126071, -0.004287235494875522, -0.3137357833760756, -0.15784107748832968, 0.15999625772410245, 0.02703207770914391... |
1,801.08494 | Evaluating Predictive Models of Student Success: Closing the
Methodological Gap | Model evaluation -- the process of making inferences about the performance of
predictive models -- is a critical component of predictive modeling research in
learning analytics. We survey the state of the practice with respect to model
evaluation in learning analytics, which overwhelmingly uses only naive methods
for... | stat.AP cs.CY | model evaluation the process of making inferences about the performance of predictive models is a critical component of predictive modeling research in learning analytics we survey the state of the practice with respect to model evaluation in learning analytics which overwhelmingly uses only naive methods for model eva... | [['model', 'evaluation', 'the', 'process', 'of', 'making', 'inferences', 'about', 'the', 'performance', 'of', 'predictive', 'models', 'is', 'a', 'critical', 'component', 'of', 'predictive', 'modeling', 'research', 'in', 'learning', 'analytics', 'we', 'survey', 'the', 'state', 'of', 'the', 'practice', 'with', 'respect',... | [-0.00024095639626649644, -0.04349575224064505, -0.11976073562040282, 0.10862061718574119, -0.09210498232340855, -0.17926744611853426, 0.09062792250899959, 0.42348655912247923, -0.18840701698841486, -0.3499324961331767, 0.10083501086842098, -0.28816611239378404, -0.142261298969656, 0.23512819149739128, -0.0491641426556... |
1,801.08495 | Limiting behaviour of the stationary search cost distribution driven by
a generalized gamma process | Consider a list of labeled objects that are organized in a heap. At each
time, object $j$ is selected with probability $p_j$ and moved to the top of the
heap. This procedure defines a Markov chain on the set of permutations which is
referred to in the literature as Move-to-Front rule. The present contribution
focuses... | stat.ME math.PR | consider a list of labeled objects that are organized in a heap at each time object j is selected with probability p_j and moved to the top of the heap this procedure defines a markov chain on the set of permutations which is referred to in the literature as movetofront rule the present contribution focuses on the stat... | [['consider', 'a', 'list', 'of', 'labeled', 'objects', 'that', 'are', 'organized', 'in', 'a', 'heap', 'at', 'each', 'time', 'object', 'j', 'is', 'selected', 'with', 'probability', 'p_j', 'and', 'moved', 'to', 'the', 'top', 'of', 'the', 'heap', 'this', 'procedure', 'defines', 'a', 'markov', 'chain', 'on', 'the', 'set', ... | [-0.10318649861196809, 0.12068749905200768, -0.07597557711569185, 0.06890548734216113, -0.07007366391392239, -0.1123522832921848, 0.10876682440639282, 0.35774853438237647, -0.29123434095661965, -0.27242547795423216, 0.10598475398143174, -0.2665137189273901, -0.0788071889504297, 0.12956465003913306, -0.0804615971055622,... |
1,801.08496 | BRITE Cookbook 2.0 | The raw BRITE photometry is affected by the presence of many outliers and
instrumental effects. We present and discuss possible ways to correct the
photometry for instrumental effects. Special attention is paid to the procedure
of decorrelation which enables removal of most of the instrumental effects and
considerabl... | astro-ph.IM astro-ph.SR | the raw brite photometry is affected by the presence of many outliers and instrumental effects we present and discuss possible ways to correct the photometry for instrumental effects special attention is paid to the procedure of decorrelation which enables removal of most of the instrumental effects and considerably im... | [['the', 'raw', 'brite', 'photometry', 'is', 'affected', 'by', 'the', 'presence', 'of', 'many', 'outliers', 'and', 'instrumental', 'effects', 'we', 'present', 'and', 'discuss', 'possible', 'ways', 'to', 'correct', 'the', 'photometry', 'for', 'instrumental', 'effects', 'special', 'attention', 'is', 'paid', 'to', 'the', ... | [-0.03610371352935379, 0.07999064225534147, -0.10303741642697291, 0.09689857921224426, -0.13563456477766686, -0.09583856632763689, 0.0820303028237752, 0.35830562846227126, -0.20319426682227376, -0.34905558743260123, 0.10577876284210519, -0.29263576569289645, -0.13055781640789726, 0.20465462705628437, -0.159590465046296... |
1,801.08497 | BRITE view of $\sigma$ Scorpii, $\beta$ Cephei-type star studied for
over a century | Preliminary results of the analysis of the combined space-based BRITE and
SMEI, and ground-based Stroemgren photometry are presented. The BRITE data
allowed to find seven p and three g modes in the frequency spectrum of this
star; only four p modes were known in this star prior to this study. The first
results of sei... | astro-ph.SR | preliminary results of the analysis of the combined spacebased brite and smei and groundbased stroemgren photometry are presented the brite data allowed to find seven p and three g modes in the frequency spectrum of this star only four p modes were known in this star prior to this study the first results of seismic mod... | [['preliminary', 'results', 'of', 'the', 'analysis', 'of', 'the', 'combined', 'spacebased', 'brite', 'and', 'smei', 'and', 'groundbased', 'stroemgren', 'photometry', 'are', 'presented', 'the', 'brite', 'data', 'allowed', 'to', 'find', 'seven', 'p', 'and', 'three', 'g', 'modes', 'in', 'the', 'frequency', 'spectrum', 'of... | [-0.12000022380281303, 0.11538183867489382, -0.09838242989854287, 0.03585161497792766, -0.1297968790187674, -0.045894615859251024, 0.05623372287442118, 0.3869107467895847, -0.16891315923530167, -0.3533330487750344, 0.1257227166374293, -0.3272747376586421, -0.10823812316787446, 0.25033608145254144, -0.04800176579442065,... |
1,801.08498 | Simulation studies of CZT(S,Se) single and tandem junction solar cells
towards possibilities for higher efficiencies up to 22% | We simulated photovoltaic characteristics of single heterojunction solar cell
with Cu2ZnSnS4 and Cu2ZnSnSe4 absorber layer numerically using one dimensional
solar cell capacitance simulator (SCAPS-1D). n-CdS/ZnO double buffer layer is
used for hetrostructure interfaces with the absorber layer. The cell
performance is... | physics.app-ph | we simulated photovoltaic characteristics of single heterojunction solar cell with cu2znsns4 and cu2znsnse4 absorber layer numerically using one dimensional solar cell capacitance simulator scaps1d ncdszno double buffer layer is used for hetrostructure interfaces with the absorber layer the cell performance is investig... | [['we', 'simulated', 'photovoltaic', 'characteristics', 'of', 'single', 'heterojunction', 'solar', 'cell', 'with', 'cu2znsns4', 'and', 'cu2znsnse4', 'absorber', 'layer', 'numerically', 'using', 'one', 'dimensional', 'solar', 'cell', 'capacitance', 'simulator', 'scaps1d', 'ncdszno', 'double', 'buffer', 'layer', 'is', 'u... | [-0.11605713184967283, 0.1090510147956333, 0.08013462193221563, -0.04165825793530703, 0.019784291657353088, -0.21148490453647573, 0.10745508225850894, 0.4361065394422483, -0.2599039858754016, -0.3416715302945314, 0.048444256521872286, -0.26257134697932216, -0.08950938407187572, 0.20034909378903518, -0.06777893355216033... |
1,801.08499 | Learning general sparse additive models from point queries in high
dimensions | We consider the problem of learning a $d$-variate function $f$ defined on the
cube $[-1,1]^d\subset {\mathbb R}^d$, where the algorithm is assumed to have
black box access to samples of $f$ within this domain. Denote ${\mathcal S}_r
\subset {[d] \choose r}; r=1,\dots,r_0$ to be sets consisting of unknown
$r$-wise int... | math.NA | we consider the problem of learning a dvariate function f defined on the cube 11dsubset mathbb rd where the algorithm is assumed to have black box access to samples of f within this domain denote mathcal s_r subset d choose r r1dotsr_0 to be sets consisting of unknown rwise interactions amongst the coordinate variables... | [['we', 'consider', 'the', 'problem', 'of', 'learning', 'a', 'dvariate', 'function', 'f', 'defined', 'on', 'the', 'cube', '11dsubset', 'mathbb', 'rd', 'where', 'the', 'algorithm', 'is', 'assumed', 'to', 'have', 'black', 'box', 'access', 'to', 'samples', 'of', 'f', 'within', 'this', 'domain', 'denote', 'mathcal', 's_r',... | [-0.15251045855448433, 0.06838106967313108, 0.008962162468187193, -0.05208785884851271, -0.02901039430320165, -0.18700343004954784, 0.027638936807450495, 0.3563190180636746, -0.28034744436751535, -0.22303555387770757, 0.05537120346209696, -0.31671480583884803, -0.05366228499425281, 0.11383050405359092, -0.0887695883521... |
1,801.085 | The fate of $U_A(1)$ and topological features of QCD at finite
temperature | The nature of chiral phase transition for QCD with two light quark flavors is
not yet completely resolved. This is primarily because one has to understand
whether or not the anomalous U(1) symmetry in the flavor sector is effectively
restored along with the chiral symmetry. Since the physics near the chiral
phase tra... | hep-lat hep-ph | the nature of chiral phase transition for qcd with two light quark flavors is not yet completely resolved this is primarily because one has to understand whether or not the anomalous u1 symmetry in the flavor sector is effectively restored along with the chiral symmetry since the physics near the chiral phase transitio... | [['the', 'nature', 'of', 'chiral', 'phase', 'transition', 'for', 'qcd', 'with', 'two', 'light', 'quark', 'flavors', 'is', 'not', 'yet', 'completely', 'resolved', 'this', 'is', 'primarily', 'because', 'one', 'has', 'to', 'understand', 'whether', 'or', 'not', 'the', 'anomalous', 'u1', 'symmetry', 'in', 'the', 'flavor', '... | [-0.11557496142047066, 0.27658011924658216, -0.12273898943453575, 0.08120883193256542, -0.11088028412190414, -0.11440768274837652, 0.06962525993819506, 0.37059746346671446, -0.20592993764406958, -0.2371006574063936, 0.08529493848414586, -0.2758680459059705, -0.10443426892770646, 0.03617995853860053, 0.04456993403817879... |
1,801.08501 | Density perturbations for running vacuum: a successful approach to
structure formation and to the $\sigma_8$-tension | Recent studies suggest that dynamical dark energy (DDE) provides a better fit
to the rising affluence of modern cosmological observations than the
concordance model ($\Lambda$CDM) with a rigid cosmological constant, $\Lambda$.
Such is the case with the running vacuum models (RVMs) and to some extent also
with a simpl... | astro-ph.CO gr-qc hep-ph hep-th | recent studies suggest that dynamical dark energy dde provides a better fit to the rising affluence of modern cosmological observations than the concordance model lambdacdm with a rigid cosmological constant lambda such is the case with the running vacuum models rvms and to some extent also with a simple xcdm parametri... | [['recent', 'studies', 'suggest', 'that', 'dynamical', 'dark', 'energy', 'dde', 'provides', 'a', 'better', 'fit', 'to', 'the', 'rising', 'affluence', 'of', 'modern', 'cosmological', 'observations', 'than', 'the', 'concordance', 'model', 'lambdacdm', 'with', 'a', 'rigid', 'cosmological', 'constant', 'lambda', 'such', 'i... | [-0.0874004998738272, 0.074219048417982, -0.08722608680491922, 0.1179195129980406, -0.14494974082795742, -0.12262716140826098, -0.01257998766013471, 0.3186164727288877, -0.20664264735863486, -0.3446691181518352, 0.09254328930154519, -0.288673226443242, -0.08078862976478297, 0.19610557061238712, 0.015664030845208024, 0.... |
1,801.08502 | Non-volatile bipolar resistive switching in sol-gel derived BiFeO3 thin
films | BiFeO3 thin films are deposited on FTO coated glass substrates using a simple
sol-gel deposition technique, limiting thickness about 70 nm and Ag/BiFeO3/FTO
RRAM devices are prepared. The devices showed low-voltage bipolar switching
with the maximum Ion/Ioff ~ 450, and low set and reset voltages ~ 1.1 V and
-1.5 V, r... | cond-mat.mtrl-sci | bifeo3 thin films are deposited on fto coated glass substrates using a simple solgel deposition technique limiting thickness about 70 nm and agbifeo3fto rram devices are prepared the devices showed lowvoltage bipolar switching with the maximum ionioff 450 and low set and reset voltages 11 v and 15 v respectively the de... | [['bifeo3', 'thin', 'films', 'are', 'deposited', 'on', 'fto', 'coated', 'glass', 'substrates', 'using', 'a', 'simple', 'solgel', 'deposition', 'technique', 'limiting', 'thickness', 'about', '70', 'nm', 'and', 'agbifeo3fto', 'rram', 'devices', 'are', 'prepared', 'the', 'devices', 'showed', 'lowvoltage', 'bipolar', 'swit... | [-0.14796534824867066, 0.21745299167315088, 0.05070808900916201, -0.0565200238479448, 0.029948484544884267, -0.22227939529579102, 0.13521707188851367, 0.45837589246257554, -0.21662340294129737, -0.35148017448703134, 0.07797014167418659, -0.3161723921882121, -0.041273056815459036, 0.21352328540845297, -0.053761839840055... |
1,801.08503 | Convex Integration Arising in the Modelling of Shape-Memory Alloys: Some
Remarks on Rigidity, Flexibility and Some Numerical Implementations | We study convex integration solutions in the context of the modelling of
shape-memory alloys. The purpose of the article is two-fold, treating both
rigidity and flexibility properties: Firstly, we relate the maximal regularity
of convex integration solutions to the presence of lower bounds in variational
models with ... | math.AP | we study convex integration solutions in the context of the modelling of shapememory alloys the purpose of the article is twofold treating both rigidity and flexibility properties firstly we relate the maximal regularity of convex integration solutions to the presence of lower bounds in variational models with surface ... | [['we', 'study', 'convex', 'integration', 'solutions', 'in', 'the', 'context', 'of', 'the', 'modelling', 'of', 'shapememory', 'alloys', 'the', 'purpose', 'of', 'the', 'article', 'is', 'twofold', 'treating', 'both', 'rigidity', 'and', 'flexibility', 'properties', 'firstly', 'we', 'relate', 'the', 'maximal', 'regularity'... | [-0.11803242268206754, 0.027909913229396437, -0.06415909244033444, 0.061032008505334134, -0.0692049741081082, -0.11025598469549919, 0.027513376799052452, 0.3694271497096461, -0.29205504067168375, -0.26732982689570084, 0.15422421551106663, -0.24565251358775514, -0.1650693200477906, 0.19566190763754715, -0.06381064089531... |
1,801.08504 | Finite momentum Cooper pairing in 3D topological insulator Josephson
junctions | Unconventional superconductivity arising from the interplay between strong
spin-orbit coupling and magnetism is an intensive area of research. One form of
unconventional superconductivity arises when Cooper pairs subjected to a
magnetic exchange coupling acquire a finite momentum. Here, we report on a
signature of fi... | cond-mat.mes-hall | unconventional superconductivity arising from the interplay between strong spinorbit coupling and magnetism is an intensive area of research one form of unconventional superconductivity arises when cooper pairs subjected to a magnetic exchange coupling acquire a finite momentum here we report on a signature of finite m... | [['unconventional', 'superconductivity', 'arising', 'from', 'the', 'interplay', 'between', 'strong', 'spinorbit', 'coupling', 'and', 'magnetism', 'is', 'an', 'intensive', 'area', 'of', 'research', 'one', 'form', 'of', 'unconventional', 'superconductivity', 'arises', 'when', 'cooper', 'pairs', 'subjected', 'to', 'a', 'm... | [-0.2620413798264208, 0.22741114247961017, -0.06408420656411414, 0.08676445827297602, -0.11058737352450794, -0.1313795540812062, 0.07086601785337883, 0.34809254350286, -0.2657546897960417, -0.3074602246092936, -0.07282965427680695, -0.30143100993562466, -0.14254415466562442, 0.18411525464385536, 0.057769583415979826, -... |
1,801.08505 | LYCORIS - A Large Area Strip Telescope | The LYCORIS Large Area Silicon Strip Telescope for the DESY II Test Beam
Facility is presented. The DESY II Test Beam Facility provides elec- tron and
positron beams for beam tests of up to 6 GeV. A new telescope with a large
10x20 cm$^2$ coverage area based on a 25 {\mu}m pitch strip sensor is to be
installed within... | physics.ins-det | the lycoris large area silicon strip telescope for the desy ii test beam facility is presented the desy ii test beam facility provides elec tron and positron beams for beam tests of up to 6 gev a new telescope with a large 10x20 cm2 coverage area based on a 25 mum pitch strip sensor is to be installed within the pcmag ... | [['the', 'lycoris', 'large', 'area', 'silicon', 'strip', 'telescope', 'for', 'the', 'desy', 'ii', 'test', 'beam', 'facility', 'is', 'presented', 'the', 'desy', 'ii', 'test', 'beam', 'facility', 'provides', 'elec', 'tron', 'and', 'positron', 'beams', 'for', 'beam', 'tests', 'of', 'up', 'to', '6', 'gev', 'a', 'new', 'tel... | [-0.08825113059221101, 0.14545415093057923, -0.013882130570709705, 0.012677666676297251, -0.02723752817671214, -0.22408339522912035, 0.012407575627522809, 0.394778057939506, -0.1194740497640201, -0.3722794247525079, 0.09946792898699641, -0.32526097167283297, 0.12748955855412142, 0.26874750607780046, -0.0228138101985678... |
1,801.08506 | Stable 3D FDTD Method for arbitrary Fully Electric and Magnetic
Anisotropic Maxwell Equations | We have developed a new fully anisotropic 3D FDTD Maxwell solver for
arbitrary electrically and magnetically anisotropic media for piecewise
constant electric and magnetic materials that are co-located over the primary
computational cells. Two numerical methods were developed that are called
non-averaged and averaged... | math.NA | we have developed a new fully anisotropic 3d fdtd maxwell solver for arbitrary electrically and magnetically anisotropic media for piecewise constant electric and magnetic materials that are colocated over the primary computational cells two numerical methods were developed that are called nonaveraged and averaged meth... | [['we', 'have', 'developed', 'a', 'new', 'fully', 'anisotropic', '3d', 'fdtd', 'maxwell', 'solver', 'for', 'arbitrary', 'electrically', 'and', 'magnetically', 'anisotropic', 'media', 'for', 'piecewise', 'constant', 'electric', 'and', 'magnetic', 'materials', 'that', 'are', 'colocated', 'over', 'the', 'primary', 'comput... | [-0.11236909059675243, 0.08744844495959114, -0.03708376989907351, 0.02124319287453959, -0.07148851634122395, -0.1205090714102143, -0.009187004464938883, 0.4242093992415127, -0.21548198598935778, -0.34746321538348474, 0.10415066857557409, -0.24891209978195375, -0.13109044487239413, 0.22287859599507676, 0.010607545437308... |
1,801.08507 | On $\ell_4 : \ell_2$ ratio of functions with restricted Fourier support | Given a subset $A \subseteq \{0,1\}^n$, let $\mu(A)$ be the maximal ratio
between $\ell_4$ and $\ell_2$ norms of a function whose Fourier support is a
subset of $A$. We make some simple observations about the connections between
$\mu(A)$ and the additive properties of $A$ on one hand, and between $\mu(A)$
and the unc... | math.CO | given a subset a subseteq 01n let mua be the maximal ratio between ell_4 and ell_2 norms of a function whose fourier support is a subset of a we make some simple observations about the connections between mua and the additive properties of a on one hand and between mua and the uncertainty principle for a on the other h... | [['given', 'a', 'subset', 'a', 'subseteq', '01n', 'let', 'mua', 'be', 'the', 'maximal', 'ratio', 'between', 'ell_4', 'and', 'ell_2', 'norms', 'of', 'a', 'function', 'whose', 'fourier', 'support', 'is', 'a', 'subset', 'of', 'a', 'we', 'make', 'some', 'simple', 'observations', 'about', 'the', 'connections', 'between', 'm... | [-0.13813625437722765, 0.09895649141442307, -0.07491622150754901, 0.05329233877516041, -0.06727386519950987, -0.13602464731472233, 0.10517953037008367, 0.3461986540954698, -0.2752381494372255, -0.2609057024259258, 0.12359575005312864, -0.32694484752223446, -0.09874580462282109, 0.24046901014366154, -0.05571526917628944... |
1,801.08508 | Measuring the masses of Intermediate Polars with NuSTAR: V709 Cas, NY
Lup and V1223 Sgr | The X-ray spectra of intermediate polars can be modelled to give a direct
measurement of white dwarf mass. Here we fit accretion column models to NuSTAR
spectra of three intermediate polars; V709 Cas, NY Lup and V1223 Sgr in order
to determine their masses. From fits to 3-78 keV spectra, we find masses of
$M_{\rm WD}... | astro-ph.HE | the xray spectra of intermediate polars can be modelled to give a direct measurement of white dwarf mass here we fit accretion column models to nustar spectra of three intermediate polars v709 cas ny lup and v1223 sgr in order to determine their masses from fits to 378 kev spectra we find masses of m_rm wd088005_004m_o... | [['the', 'xray', 'spectra', 'of', 'intermediate', 'polars', 'can', 'be', 'modelled', 'to', 'give', 'a', 'direct', 'measurement', 'of', 'white', 'dwarf', 'mass', 'here', 'we', 'fit', 'accretion', 'column', 'models', 'to', 'nustar', 'spectra', 'of', 'three', 'intermediate', 'polars', 'v709', 'cas', 'ny', 'lup', 'and', 'v... | [-0.06336760208810205, 0.1254548813439609, -0.06797966694037588, 0.08675597524951335, -0.11727494025989524, -0.13139816626185938, 0.10148504856130425, 0.43140176919130785, -0.1413864474370197, -0.3843256910419408, 0.057837904818610834, -0.3320036553338451, 0.008092968904782297, 0.22563150463590645, -0.06395851168781519... |
1,801.08509 | Fluorographene with Impurities as a Biomimetic Light-Harvesting Medium | We investigate the prospect of using a two-dimensional material,
fluorographene, to mimic light-harvesting function of natural photosynthetic
antennae. We show by quantum chemical calculations that isles of graphene in a
fluorographene sheet can act as quasi-molecules similar to natural pigments
from which structures... | physics.chem-ph quant-ph | we investigate the prospect of using a twodimensional material fluorographene to mimic lightharvesting function of natural photosynthetic antennae we show by quantum chemical calculations that isles of graphene in a fluorographene sheet can act as quasimolecules similar to natural pigments from which structures similar... | [['we', 'investigate', 'the', 'prospect', 'of', 'using', 'a', 'twodimensional', 'material', 'fluorographene', 'to', 'mimic', 'lightharvesting', 'function', 'of', 'natural', 'photosynthetic', 'antennae', 'we', 'show', 'by', 'quantum', 'chemical', 'calculations', 'that', 'isles', 'of', 'graphene', 'in', 'a', 'fluorograph... | [-0.12888967092075046, 0.1391477277508577, -0.051064957466984175, 0.07727444028511407, -0.0335225651728078, -0.1046237242605202, 0.013981179745680599, 0.4211864889101692, -0.28357469849288464, -0.3337766932836049, 0.031420856896571064, -0.2317257244928331, -0.16606228273834975, 0.19608502560812566, -0.00464967807764729... |
1,801.0851 | NLO radiative corrections for Forward-Backward and Left-Right
Asymmetries at a B-Factory | This paper presents the first calculations of the parity-violating
polarization asymmetry and forward-backward asymmetry of the $e^- e^+
\rightarrow \mu^+ \mu^- (\gamma)$ process at a center-of-mass energy of 10.58
GeV with up to one-loop electroweak radiative corrections. The calculations are
relevant for future pre... | hep-ph | this paper presents the first calculations of the parityviolating polarization asymmetry and forwardbackward asymmetry of the e e rightarrow mu mu gamma process at a centerofmass energy of 1058 gev with up to oneloop electroweak radiative corrections the calculations are relevant for future precision electroweak measur... | [['this', 'paper', 'presents', 'the', 'first', 'calculations', 'of', 'the', 'parityviolating', 'polarization', 'asymmetry', 'and', 'forwardbackward', 'asymmetry', 'of', 'the', 'e', 'e', 'rightarrow', 'mu', 'mu', 'gamma', 'process', 'at', 'a', 'centerofmass', 'energy', 'of', '1058', 'gev', 'with', 'up', 'to', 'oneloop',... | [-0.09215786572674226, 0.16575827835436813, -0.08318467916406948, 0.09582934611055956, -0.03167371902582718, -0.09219637780193368, 0.02226973819899662, 0.33022173743309646, -0.24327863661636567, -0.30079137425034724, -0.009086064661146495, -0.3765848131416815, 0.04667455875154199, 0.18532231180639616, 0.092489425234239... |
1,801.08511 | Heusler compounds -- how to tune the magnetocrystalline anisotropy | Tailoring and controlling magnetic properties is an important factor for
materials design. Here, we present a case study for Ni-based Heusler compounds
of the type Ni$_2$YZ with Y = Mn, Fe, Co and Z = B, Al, Ga, In, Si, Ge, Sn
based on first principles electronic structure calculations. These compounds
are interestin... | cond-mat.mtrl-sci | tailoring and controlling magnetic properties is an important factor for materials design here we present a case study for nibased heusler compounds of the type ni_2yz with y mn fe co and z b al ga in si ge sn based on first principles electronic structure calculations these compounds are interesting since the material... | [['tailoring', 'and', 'controlling', 'magnetic', 'properties', 'is', 'an', 'important', 'factor', 'for', 'materials', 'design', 'here', 'we', 'present', 'a', 'case', 'study', 'for', 'nibased', 'heusler', 'compounds', 'of', 'the', 'type', 'ni_2yz', 'with', 'y', 'mn', 'fe', 'co', 'and', 'z', 'b', 'al', 'ga', 'in', 'si', ... | [-0.1152839645409049, 0.14010943429296813, -0.0031776532387504212, 0.028516987415078358, -0.016001814508285278, -0.09751902469792045, 0.10414988732305713, 0.4313210207491349, -0.2846149957476136, -0.31640357682779907, 0.03789687676844784, -0.3050113554327534, -0.12973435790492938, 0.20053745296974787, 0.009779551345854... |
1,801.08512 | Inference in high-dimensional graphical models | We provide a selected overview of methodology and theory for estimation and
inference on the edge weights in high-dimensional directed and undirected
Gaussian graphical models. For undirected graphical models, two main explicit
constructions are provided: one based on a global method that maximizes the
joint likeliho... | math.ST stat.ME stat.TH | we provide a selected overview of methodology and theory for estimation and inference on the edge weights in highdimensional directed and undirected gaussian graphical models for undirected graphical models two main explicit constructions are provided one based on a global method that maximizes the joint likelihood the... | [['we', 'provide', 'a', 'selected', 'overview', 'of', 'methodology', 'and', 'theory', 'for', 'estimation', 'and', 'inference', 'on', 'the', 'edge', 'weights', 'in', 'highdimensional', 'directed', 'and', 'undirected', 'gaussian', 'graphical', 'models', 'for', 'undirected', 'graphical', 'models', 'two', 'main', 'explicit... | [-0.07113698757777032, 0.005785601268914174, -0.09961059234397364, 0.10064039825305451, -0.13015097420642247, -0.18138434722285418, 0.0773635029828475, 0.4704165024560516, -0.2563745545590446, -0.2900745329535464, 0.12002773218733823, -0.23953441270103637, -0.15879288578132358, 0.1402544039369554, -0.10457972020767357,... |
1,801.08513 | Unmixing urban hyperspectral imagery with a Gaussian mixture model on
endmember variability | In this paper, we model a pixel as a linear combination of endmembers sampled
from probability distributions of Gaussian mixture models (GMM). The parameters
of the GMM distributions are estimated using spectral libraries. Abundances are
estimated based on the distribution parameters. The advantage of this algorithm
... | cs.CV | in this paper we model a pixel as a linear combination of endmembers sampled from probability distributions of gaussian mixture models gmm the parameters of the gmm distributions are estimated using spectral libraries abundances are estimated based on the distribution parameters the advantage of this algorithm is that ... | [['in', 'this', 'paper', 'we', 'model', 'a', 'pixel', 'as', 'a', 'linear', 'combination', 'of', 'endmembers', 'sampled', 'from', 'probability', 'distributions', 'of', 'gaussian', 'mixture', 'models', 'gmm', 'the', 'parameters', 'of', 'the', 'gmm', 'distributions', 'are', 'estimated', 'using', 'spectral', 'libraries', '... | [0.005213729031785086, 0.027593309885407445, -0.06631823250815515, 0.0684989032173185, -0.008018320807874077, -0.15364793614100883, 0.030008174240796538, 0.4304286030144626, -0.21187797716907775, -0.4088796716105284, 0.10514699576125175, -0.2797758017701856, -0.060943841015843735, 0.17672997825004222, -0.07595150555132... |
1,801.08514 | Study of the Angular Spectrum of a Bianisotropic Refractive Metasurface
at a Dielectric Interface | We present an initial study of the angular spectrum of a bianisotropic
refractive metasurface at an interface between two dielectric media. In this
study, we report on the existence of three distinct angular regions: a)~a
rotated transmission cone, b)~a modified total internal reflection region, and
c)~a new total re... | physics.optics | we present an initial study of the angular spectrum of a bianisotropic refractive metasurface at an interface between two dielectric media in this study we report on the existence of three distinct angular regions aa rotated transmission cone ba modified total internal reflection region and ca new total retroreflection... | [['we', 'present', 'an', 'initial', 'study', 'of', 'the', 'angular', 'spectrum', 'of', 'a', 'bianisotropic', 'refractive', 'metasurface', 'at', 'an', 'interface', 'between', 'two', 'dielectric', 'media', 'in', 'this', 'study', 'we', 'report', 'on', 'the', 'existence', 'of', 'three', 'distinct', 'angular', 'regions', 'a... | [-0.23300937378779055, 0.12139159747923259, -0.013810262819752096, -0.0437256729719229, -0.057348283007740974, -0.11830385751090944, 0.01928828233387321, 0.48954598121345044, -0.2545542937517166, -0.2915583441220224, -0.014983159576077014, -0.29140120558440685, -0.11474071064032615, 0.11665980238467455, 0.0177567397139... |
1,801.08515 | Deciphering noise amplification and reduction in open chemical reaction
networks | The impact of random fluctuations on the dynamical behavior a complex
biological systems is a longstanding issue, whose understanding would shed
light on the evolutionary pressure that nature imposes on the intrinsic noise
levels and would allow rationally designing synthetic networks with controlled
noise. Using the... | q-bio.MN | the impact of random fluctuations on the dynamical behavior a complex biological systems is a longstanding issue whose understanding would shed light on the evolutionary pressure that nature imposes on the intrinsic noise levels and would allow rationally designing synthetic networks with controlled noise using the ito... | [['the', 'impact', 'of', 'random', 'fluctuations', 'on', 'the', 'dynamical', 'behavior', 'a', 'complex', 'biological', 'systems', 'is', 'a', 'longstanding', 'issue', 'whose', 'understanding', 'would', 'shed', 'light', 'on', 'the', 'evolutionary', 'pressure', 'that', 'nature', 'imposes', 'on', 'the', 'intrinsic', 'noise... | [-0.15059298127224402, 0.15675624945924937, -0.04948918420489333, 0.05723897316264421, -0.0016535803536368934, -0.1661715940626891, 0.04007657763525328, 0.35621472677615074, -0.2557401844366853, -0.28599877092970666, 0.04634232285077035, -0.2883508822550149, -0.15168783262613164, 0.1632411325452787, -0.0166289153525472... |
1,801.08516 | Multiplicity of positive solutions for a quasilinear Schr\"odinger
equation with an almost critical nonlinearity | In this paper we prove an existence result of multiple positive solutions for
the following quasilinear problem \begin{equation*} \left\{
\begin{array}[c]{ll} -\Delta u - \Delta (u^2)u = |u|^{p-2}u & \mbox{ in }
\Omega u= 0 &\mbox{ on } \partial\Omega, \end{array} \right. \end{equation*}
where $\Omega$ is a smooth an... | math.AP | in this paper we prove an existence result of multiple positive solutions for the following quasilinear problem beginequation left beginarraycll delta u delta u2u up2u mbox in omega u 0 mbox on partialomega endarray right endequation where omega is a smooth and bounded domain in mathbb rnngeq3 more specifically we prov... | [['in', 'this', 'paper', 'we', 'prove', 'an', 'existence', 'result', 'of', 'multiple', 'positive', 'solutions', 'for', 'the', 'following', 'quasilinear', 'problem', 'beginequation', 'left', 'beginarraycll', 'delta', 'u', 'delta', 'u2u', 'up2u', 'mbox', 'in', 'omega', 'u', '0', 'mbox', 'on', 'partialomega', 'endarray', ... | [-0.25551401247724276, 0.04622693866940032, 0.033529554782553185, -0.012710319494510281, -0.07042765211611632, -0.19068766007482818, -0.021321149341042945, 0.279853374921257, -0.38333512022148203, -0.12660898695570194, 0.10790171428389046, -0.4058046190987659, -0.05912553837310664, 0.1708675155996734, -0.07677162673230... |
1,801.08517 | Extending the Brewster Effect to Arbitrary Angle and Polarization using
Bianisotropic Metasurfaces | A bianisotropic metasurface design is proposed for extending the Brewster
effect to arbitrary angles and polarizations. The metasurface is synthesized
using the surface susceptibility tensor and Generalized Sheet Transition
Conditions (GSTCs) synthesis method, and is demonstrated by GSTC-FDFD
simulation. It is found ... | physics.optics | a bianisotropic metasurface design is proposed for extending the brewster effect to arbitrary angles and polarizations the metasurface is synthesized using the surface susceptibility tensor and generalized sheet transition conditions gstcs synthesis method and is demonstrated by gstcfdfd simulation it is found that an ... | [['a', 'bianisotropic', 'metasurface', 'design', 'is', 'proposed', 'for', 'extending', 'the', 'brewster', 'effect', 'to', 'arbitrary', 'angles', 'and', 'polarizations', 'the', 'metasurface', 'is', 'synthesized', 'using', 'the', 'surface', 'susceptibility', 'tensor', 'and', 'generalized', 'sheet', 'transition', 'conditi... | [-0.1315078885326116, 0.18199448652704173, -0.056638933427525504, -0.018275259567114215, -0.139396904228991, -0.16587808776508878, -0.05359116434637043, 0.4738141204471941, -0.24362100458439487, -0.30197864759391474, 0.05956500626950996, -0.22814175042749188, -0.15904954836968285, 0.2523568612695844, -0.000680241906256... |
1,801.08518 | Monotonicity results for the first Steklov eigenvalue on compact
surfaces | We show several results comparing sharp eigenvalue bounds for the first
Steklov eigenvalue on surfaces under change of the topology. Among others, we
obtain strict monotonicity in the genus. Combined with results of the second
named author \cite{petrides_2} this implies the existence of free boundary
minimal immersio... | math.DG math.AP | we show several results comparing sharp eigenvalue bounds for the first steklov eigenvalue on surfaces under change of the topology among others we obtain strict monotonicity in the genus combined with results of the second named author citepetrides_2 this implies the existence of free boundary minimal immersions from ... | [['we', 'show', 'several', 'results', 'comparing', 'sharp', 'eigenvalue', 'bounds', 'for', 'the', 'first', 'steklov', 'eigenvalue', 'on', 'surfaces', 'under', 'change', 'of', 'the', 'topology', 'among', 'others', 'we', 'obtain', 'strict', 'monotonicity', 'in', 'the', 'genus', 'combined', 'with', 'results', 'of', 'the',... | [-0.16681776417407218, 0.057119328377453926, -0.11452420115736979, 0.07333533804978595, -0.08392778725980164, -0.11761756018771753, 0.04182114886035296, 0.2901210256053933, -0.21906668346907412, -0.2969202639704401, 0.1085503151089969, -0.2920910864100828, -0.15101791938839407, 0.22258614056876727, -0.17709957174472996... |
1,801.08519 | Quantification of Ion Migration in CH3NH3PbI3 Perovskite Solar Cells by
Transient Capacitance Measurements | Solar cells based on organic-inorganic metal halide perovskites show
efficiencies close to highly-optimized silicon solar cells. However, ion
migration in the perovskite films leads to device degradation and impedes large
scale commercial applications. We use transient ion-drift measurements to
quantify activation en... | cond-mat.mtrl-sci | solar cells based on organicinorganic metal halide perovskites show efficiencies close to highlyoptimized silicon solar cells however ion migration in the perovskite films leads to device degradation and impedes large scale commercial applications we use transient iondrift measurements to quantify activation energy dif... | [['solar', 'cells', 'based', 'on', 'organicinorganic', 'metal', 'halide', 'perovskites', 'show', 'efficiencies', 'close', 'to', 'highlyoptimized', 'silicon', 'solar', 'cells', 'however', 'ion', 'migration', 'in', 'the', 'perovskite', 'films', 'leads', 'to', 'device', 'degradation', 'and', 'impedes', 'large', 'scale', '... | [-0.11828264746834677, 0.1980113210452218, 0.08733890787821519, -0.028769170344319372, 0.018123558249383692, -0.18341096284769712, 0.09495978200717006, 0.42101547370354336, -0.22921763397950343, -0.3264883559051822, -0.0012185237119122156, -0.33041911447795214, -0.10890129404684538, 0.18575279041816772, -0.077041825358... |
1,801.0852 | Self-testing quantum states and measurements in the prepare-and-measure
scenario | The goal of self-testing is to characterize an a priori unknown quantum
system based solely on measurement statistics, i.e. using an uncharacterized
measurement device. Here we develop self-testing methods for quantum
prepare-and-measure experiments, thus not necessarily relying on entanglement
and/or violation of a ... | quant-ph | the goal of selftesting is to characterize an a priori unknown quantum system based solely on measurement statistics ie using an uncharacterized measurement device here we develop selftesting methods for quantum prepareandmeasure experiments thus not necessarily relying on entanglement andor violation of a bell inequal... | [['the', 'goal', 'of', 'selftesting', 'is', 'to', 'characterize', 'an', 'a', 'priori', 'unknown', 'quantum', 'system', 'based', 'solely', 'on', 'measurement', 'statistics', 'ie', 'using', 'an', 'uncharacterized', 'measurement', 'device', 'here', 'we', 'develop', 'selftesting', 'methods', 'for', 'quantum', 'prepareandme... | [-0.11318873311392963, 0.10496603363445992, -0.06847615695397298, 0.060137147183503166, -0.03247783055457358, -0.2214631475194787, 0.1148927967565564, 0.34043294391057527, -0.21298314749380481, -0.2737771909227237, 0.11064806862962612, -0.25195020763539316, -0.10778983915224671, 0.2480917940668475, -0.09250662565262666... |
1,801.08521 | OB Stars and Cepheids From the Gaia TGAS Catalogue: Test of their
Distances and Proper Motions | We consider young distant stars from the Gaia TGAS catalog. These are 250
classical Cepheids and 244 OB stars located at distances up to 4 kpc from the
Sun. These stars are used to determine the Galactic rotation parameters using
both trigonometric parallaxes and proper motions of the TGAS stars. In this
case the con... | astro-ph.GA | we consider young distant stars from the gaia tgas catalog these are 250 classical cepheids and 244 ob stars located at distances up to 4 kpc from the sun these stars are used to determine the galactic rotation parameters using both trigonometric parallaxes and proper motions of the tgas stars in this case the consider... | [['we', 'consider', 'young', 'distant', 'stars', 'from', 'the', 'gaia', 'tgas', 'catalog', 'these', 'are', '250', 'classical', 'cepheids', 'and', '244', 'ob', 'stars', 'located', 'at', 'distances', 'up', 'to', '4', 'kpc', 'from', 'the', 'sun', 'these', 'stars', 'are', 'used', 'to', 'determine', 'the', 'galactic', 'rota... | [-0.06172891818331899, 0.15832536902140687, -0.08226336175936956, 0.059937096244000176, -0.11905675232525409, -0.01770072956037719, 0.0870260211472388, 0.3859104234725237, -0.23737330116722502, -0.35176284292735804, 0.03781564220395169, -0.2996356772419847, 0.0395952154290115, 0.25641790933958775, -0.041042507263935275... |
1,801.08522 | Floating Forests: Quantitative Validation of Citizen Science Data
Generated From Consensus Classifications | Large-scale research endeavors can be hindered by logistical constraints
limiting the amount of available data. For example, global ecological questions
require a global dataset, and traditional sampling protocols are often too
inefficient for a small research team to collect an adequate amount of data.
Citizen scien... | physics.soc-ph q-bio.QM | largescale research endeavors can be hindered by logistical constraints limiting the amount of available data for example global ecological questions require a global dataset and traditional sampling protocols are often too inefficient for a small research team to collect an adequate amount of data citizen science offe... | [['largescale', 'research', 'endeavors', 'can', 'be', 'hindered', 'by', 'logistical', 'constraints', 'limiting', 'the', 'amount', 'of', 'available', 'data', 'for', 'example', 'global', 'ecological', 'questions', 'require', 'a', 'global', 'dataset', 'and', 'traditional', 'sampling', 'protocols', 'are', 'often', 'too', '... | [-0.06327981682351003, 0.022683283057715296, -0.04088143844049997, 0.04967866679205774, -0.13442339955005222, -0.11944416554179042, 0.09342510133283213, 0.42803303420693667, -0.2102856745853877, -0.44520924956752705, 0.14208852324025847, -0.33836523724715406, -0.09251955233182974, 0.23024933587473173, -0.14185069997687... |
1,801.08523 | Extracting Particle Physics Information from Direct Detection of Dark
Matter with Minimal Assumptions | In the absence of direct accelerator data to constrain particle models, and
given existing astrophysical uncertainties associated with the phase space
distribution of WIMP dark matter in our galactic halo, extracting information
on fundamental particle microphysics from possible signals in underground
direct detector... | hep-ph astro-ph.CO astro-ph.GA hep-ex nucl-ex | in the absence of direct accelerator data to constrain particle models and given existing astrophysical uncertainties associated with the phase space distribution of wimp dark matter in our galactic halo extracting information on fundamental particle microphysics from possible signals in underground direct detectors wi... | [['in', 'the', 'absence', 'of', 'direct', 'accelerator', 'data', 'to', 'constrain', 'particle', 'models', 'and', 'given', 'existing', 'astrophysical', 'uncertainties', 'associated', 'with', 'the', 'phase', 'space', 'distribution', 'of', 'wimp', 'dark', 'matter', 'in', 'our', 'galactic', 'halo', 'extracting', 'informati... | [-0.09814399260041469, 0.17334918332943583, -0.09330907510935932, 0.173020120695069, -0.11860083559911479, -0.10261205235112678, 0.016909466101787986, 0.3183233533081982, -0.23410151189138345, -0.39041143189020017, 0.022744946803568918, -0.29721797823029406, -0.046094208572279007, 0.1898757245781941, 0.0191219748079995... |
1,801.08524 | On a class of immersions of spheres into space forms of nonpositive
curvature | Let $ M^{n+1} $ ($ n \ge 2 $) be a simply-connected space form of sectional
curvature $ -\kappa^2 $ for some $ \kappa \geq 0 $, and $ I $ an interval not
containing $ [-\kappa,\kappa] $ in its interior. It is known that the domain of
a closed immersed hypersurface of $ M $ whose principal curvatures lie in $ I $
must... | math.GT math.DG | let mn1 n ge 2 be a simplyconnected space form of sectional curvature kappa2 for some kappa geq 0 and i an interval not containing kappakappa in its interior it is known that the domain of a closed immersed hypersurface of m whose principal curvatures lie in i must be diffeomorphic to the sphere sn these hypersurfaces ... | [['let', 'mn1', 'n', 'ge', '2', 'be', 'a', 'simplyconnected', 'space', 'form', 'of', 'sectional', 'curvature', 'kappa2', 'for', 'some', 'kappa', 'geq', '0', 'and', 'i', 'an', 'interval', 'not', 'containing', 'kappakappa', 'in', 'its', 'interior', 'it', 'is', 'known', 'that', 'the', 'domain', 'of', 'a', 'closed', 'immer... | [-0.2100327599568603, 0.1283496909380968, -0.057794627159213026, 0.021346533840987832, -0.10510992816028496, -0.17295091627165676, -0.03446584570997705, 0.3891772846505046, -0.2889569789827025, -0.2008099687565118, 0.10096403898205608, -0.27727023712669807, -0.09464459784949819, 0.15903664311238874, -0.1367936017643660... |
1,801.08525 | Kinetic Mixing, Dark Photons and an Extra Dimension: I | Extra dimensions (ED) can provide a useful tool for model-building. In this
paper we introduce a single, flat ED extension of the kinetic-mixing/dark
photon (DP) portal for dark matter (DM) interactions with the Standard Model
(SM) assuming a compactification `radius' of order $R^{-1}\sim10-1000$ MeV and
examine the ... | hep-ph | extra dimensions ed can provide a useful tool for modelbuilding in this paper we introduce a single flat ed extension of the kineticmixingdark photon dp portal for dark matter dm interactions with the standard model sm assuming a compactification radius of order r1sim101000 mev and examine the resulting modifications t... | [['extra', 'dimensions', 'ed', 'can', 'provide', 'a', 'useful', 'tool', 'for', 'modelbuilding', 'in', 'this', 'paper', 'we', 'introduce', 'a', 'single', 'flat', 'ed', 'extension', 'of', 'the', 'kineticmixingdark', 'photon', 'dp', 'portal', 'for', 'dark', 'matter', 'dm', 'interactions', 'with', 'the', 'standard', 'model... | [-0.1262294427704414, 0.16863417743257478, -0.061392249700018754, 0.14146057245237786, -0.11364201778514958, -0.154308570118679, 0.00442160136359631, 0.2966200583864158, -0.23870719473520585, -0.344018878286727, 0.04421934205756738, -0.22563990581761337, -0.08256082993184433, 0.12600064107175002, 0.012629062170162797, ... |
1,801.08526 | Nonlinear Beam Propagation in a Class of Complex Non-PT -Symmetric
Potentials | The subject of PT-symmetry and its areas of application have been blossoming
over the past decade. Here, we consider a nonlinear Schr\"odinger model with a
complex potential that can be tuned controllably away from being PT-symmetric,
as it might be the case in realistic applications. We utilize two parameters:
the f... | nlin.PS | the subject of ptsymmetry and its areas of application have been blossoming over the past decade here we consider a nonlinear schrodinger model with a complex potential that can be tuned controllably away from being ptsymmetric as it might be the case in realistic applications we utilize two parameters the first one br... | [['the', 'subject', 'of', 'ptsymmetry', 'and', 'its', 'areas', 'of', 'application', 'have', 'been', 'blossoming', 'over', 'the', 'past', 'decade', 'here', 'we', 'consider', 'a', 'nonlinear', 'schrodinger', 'model', 'with', 'a', 'complex', 'potential', 'that', 'can', 'be', 'tuned', 'controllably', 'away', 'from', 'being... | [-0.10301200031723916, 0.09442544782612317, -0.08545804737013078, 0.046546629545680375, -0.06896767188644337, -0.16647721825426856, 0.002595268990175274, 0.3784099104033482, -0.26968927913719043, -0.25932908403369304, 0.12263956429885733, -0.24984597400232347, -0.17366463194802, 0.19739914865966351, -0.0038775195992233... |
1,801.08527 | Price of Asymptotic Safety | All known examples of four dimensional quantum field theories with asymptotic
freedom or asymptotic safety at weak coupling involve non-abelian gauge
interactions. We demonstrate that this is not a coincidence: no weakly coupled
fixed points, ultraviolet or otherwise, can be reliably generated in theories
lacking gau... | hep-th hep-ph | all known examples of four dimensional quantum field theories with asymptotic freedom or asymptotic safety at weak coupling involve nonabelian gauge interactions we demonstrate that this is not a coincidence no weakly coupled fixed points ultraviolet or otherwise can be reliably generated in theories lacking gauge inte... | [['all', 'known', 'examples', 'of', 'four', 'dimensional', 'quantum', 'field', 'theories', 'with', 'asymptotic', 'freedom', 'or', 'asymptotic', 'safety', 'at', 'weak', 'coupling', 'involve', 'nonabelian', 'gauge', 'interactions', 'we', 'demonstrate', 'that', 'this', 'is', 'not', 'a', 'coincidence', 'no', 'weakly', 'cou... | [-0.17885002161581384, 0.26803524070814, -0.05896353573435759, 0.1202099969989415, -0.08490642653857121, -0.21532712474670576, -0.013854975679936677, 0.3399152479971112, -0.18488531142978346, -0.2872036499271201, 0.0738562142330427, -0.28827838236623904, -0.18237279076918456, 0.1321192095865164, 0.00830431381966603, 0.... |
1,801.08528 | Formulating Categorical Concepts using Classes | We examine the use of classes to formulate several categorical notions. This
leads to two proposals: an explicit structure for working with subobjects, and
a hierarchy of $k$-classes. We apply the latter to both ordinary and higher
categories.
| math.CT | we examine the use of classes to formulate several categorical notions this leads to two proposals an explicit structure for working with subobjects and a hierarchy of kclasses we apply the latter to both ordinary and higher categories | [['we', 'examine', 'the', 'use', 'of', 'classes', 'to', 'formulate', 'several', 'categorical', 'notions', 'this', 'leads', 'to', 'two', 'proposals', 'an', 'explicit', 'structure', 'for', 'working', 'with', 'subobjects', 'and', 'a', 'hierarchy', 'of', 'kclasses', 'we', 'apply', 'the', 'latter', 'to', 'both', 'ordinary',... | [-0.0916487236360186, 0.0263553208240314, -0.0636228347491277, 0.14570999575325436, -0.11211949356488492, -0.11065738494998138, 0.022355890554057335, 0.3690951348919618, -0.3021621877621663, -0.30771673275893063, 0.0858379113120272, -0.22310539310312474, -0.12832151823922208, 0.1524735084783874, -0.12645574352753006, -... |
1,801.08529 | Fuchsian Equations with Three Non-Apparent Singularities | We show that for every second order Fuchsian linear differential equation $E$
with $n$ singularities of which $n-3$ are apparent there exists a
hypergeometric equation $H$ and a linear differential operator with polynomial
coefficients which maps the space of solutions of $H$ into the space of
solutions of $E$. This ... | math.CA math-ph math.MP | we show that for every second order fuchsian linear differential equation e with n singularities of which n3 are apparent there exists a hypergeometric equation h and a linear differential operator with polynomial coefficients which maps the space of solutions of h into the space of solutions of e this map is surjectiv... | [['we', 'show', 'that', 'for', 'every', 'second', 'order', 'fuchsian', 'linear', 'differential', 'equation', 'e', 'with', 'n', 'singularities', 'of', 'which', 'n3', 'are', 'apparent', 'there', 'exists', 'a', 'hypergeometric', 'equation', 'h', 'and', 'a', 'linear', 'differential', 'operator', 'with', 'polynomial', 'coef... | [-0.1948482500367044, 0.05697708588004822, -0.07082211600527877, 0.03290336877440236, -0.10231148813008553, -0.18956499954774267, -0.033753706967192036, 0.29639265620304894, -0.28418328464474707, -0.24148555534581342, 0.0880833920313134, -0.3441648975990358, -0.17492972424564263, 0.19177906960248947, -0.051106723899110... |
1,801.0853 | A classification of 3+1D bosonic topological orders (II): the case when
some point-like excitations are fermions | In this paper, we classify EF topological orders for 3+1D bosonic systems
where some emergent pointlike excitations are fermions. (1) We argue that all
3+1D bosonic topological orders have gappable boundary. (2) All the pointlike
excitations in EF topological orders are described by the representations of
$G_f=Z_2^f\... | cond-mat.str-el | in this paper we classify ef topological orders for 31d bosonic systems where some emergent pointlike excitations are fermions 1 we argue that all 31d bosonic topological orders have gappable boundary 2 all the pointlike excitations in ef topological orders are described by the representations of g_fz_2fleftthreetimes_... | [['in', 'this', 'paper', 'we', 'classify', 'ef', 'topological', 'orders', 'for', '31d', 'bosonic', 'systems', 'where', 'some', 'emergent', 'pointlike', 'excitations', 'are', 'fermions', '1', 'we', 'argue', 'that', 'all', '31d', 'bosonic', 'topological', 'orders', 'have', 'gappable', 'boundary', '2', 'all', 'the', 'poin... | [-0.21400418782705496, 0.2862449887307417, -0.06550375490703365, 0.04533229176895199, -0.06658152363525005, -0.17732061355050202, -0.01695970884413162, 0.34186510170217266, -0.23758010438177735, -0.25847914093879587, 0.06835768621297603, -0.3264210226726859, -0.12487095992687638, 0.10160099754064118, -0.030746886280019... |
1,801.08531 | A randomized and fully discrete Galerkin finite element method for
semilinear stochastic evolution equations | In this paper the numerical solution of non-autonomous semilinear stochastic
evolution equations driven by an additive Wiener noise is investigated. We
introduce a novel fully discrete numerical approximation that combines a
standard Galerkin finite element method with a randomized Runge-Kutta scheme.
Convergence of ... | math.NA math.PR | in this paper the numerical solution of nonautonomous semilinear stochastic evolution equations driven by an additive wiener noise is investigated we introduce a novel fully discrete numerical approximation that combines a standard galerkin finite element method with a randomized rungekutta scheme convergence of the me... | [['in', 'this', 'paper', 'the', 'numerical', 'solution', 'of', 'nonautonomous', 'semilinear', 'stochastic', 'evolution', 'equations', 'driven', 'by', 'an', 'additive', 'wiener', 'noise', 'is', 'investigated', 'we', 'introduce', 'a', 'novel', 'fully', 'discrete', 'numerical', 'approximation', 'that', 'combines', 'a', 's... | [-0.10378161033788548, 0.009020753985989954, -0.12414582920120618, 0.057677504182688244, -0.09302367010376358, -0.12239284982360833, 0.008926145119419469, 0.36691096751431446, -0.3265317134822892, -0.20833246325672217, 0.13937884219510036, -0.24922006681099929, -0.15574851915635893, 0.1846076735229421, -0.0970439594321... |
1,801.08532 | SQR: Balancing Speed, Quality and Risk in Online Experiments | Controlled experimentation, also called A/B testing, is widely adopted to
accelerate product innovations in the online world. However, how fast we
innovate can be limited by how we run experiments. Most experiments go through
a "ramp up" process where we gradually increase the traffic to the new
treatment to 100%. We... | stat.AP | controlled experimentation also called ab testing is widely adopted to accelerate product innovations in the online world however how fast we innovate can be limited by how we run experiments most experiments go through a ramp up process where we gradually increase the traffic to the new treatment to 100 we have seen h... | [['controlled', 'experimentation', 'also', 'called', 'ab', 'testing', 'is', 'widely', 'adopted', 'to', 'accelerate', 'product', 'innovations', 'in', 'the', 'online', 'world', 'however', 'how', 'fast', 'we', 'innovate', 'can', 'be', 'limited', 'by', 'how', 'we', 'run', 'experiments', 'most', 'experiments', 'go', 'throug... | [-0.08093867968820688, 0.13811572719632093, -0.09358472849083968, 0.0729184955732692, -0.11734189734774585, -0.16046192385520325, 0.13545251436490738, 0.44297683602390986, -0.3017225257023814, -0.3266070182243189, 0.14286617596859363, -0.27144004832281127, -0.13932834268480385, 0.1933545121747866, -0.07615120781071906,... |
1,801.08533 | How long does it take for Internal DLA to forget its initial profile? | Internal DLA is a discrete model of a moving interface. On the cylinder graph
$\mathbb{Z}_N \times \mathbb{Z}$, a particle starts uniformly on $\mathbb{Z}_N
\times \{0\}$ and performs simple random walk on the cylinder until reaching an
unoccupied site in $\mathbb{Z}_N \times \mathbb{Z}_{\geq 0}$, which it occupies
f... | math.PR | internal dla is a discrete model of a moving interface on the cylinder graph mathbbz_n times mathbbz a particle starts uniformly on mathbbz_n times 0 and performs simple random walk on the cylinder until reaching an unoccupied site in mathbbz_n times mathbbz_geq 0 which it occupies forever this operation defines a mark... | [['internal', 'dla', 'is', 'a', 'discrete', 'model', 'of', 'a', 'moving', 'interface', 'on', 'the', 'cylinder', 'graph', 'mathbbz_n', 'times', 'mathbbz', 'a', 'particle', 'starts', 'uniformly', 'on', 'mathbbz_n', 'times', '0', 'and', 'performs', 'simple', 'random', 'walk', 'on', 'the', 'cylinder', 'until', 'reaching', ... | [-0.12906021230839312, 0.22688877800332163, -0.03137146426542174, 0.00024874049240535234, -0.017798451825030266, -0.18680390623205947, 0.05455933137434638, 0.404174150196865, -0.2291035576536882, -0.25086884128875914, 0.11212390401799764, -0.32373561843165327, -0.04400831307764978, 0.1070554326611778, -0.03582209836514... |
1,801.08534 | Electrical generation and detection of spin waves in a quantum Hall
ferromagnet | Spin waves are collective excitations of magnetic systems. An attractive
setting for studying long-lived spin-wave physics is the quantum Hall (QH)
ferromagnet, which forms spontaneously in clean two-dimensional electron
systems at low temperature and in a perpendicular magnetic field. We used
out-of-equilibrium occu... | cond-mat.mes-hall | spin waves are collective excitations of magnetic systems an attractive setting for studying longlived spinwave physics is the quantum hall qh ferromagnet which forms spontaneously in clean twodimensional electron systems at low temperature and in a perpendicular magnetic field we used outofequilibrium occupation of qh... | [['spin', 'waves', 'are', 'collective', 'excitations', 'of', 'magnetic', 'systems', 'an', 'attractive', 'setting', 'for', 'studying', 'longlived', 'spinwave', 'physics', 'is', 'the', 'quantum', 'hall', 'qh', 'ferromagnet', 'which', 'forms', 'spontaneously', 'in', 'clean', 'twodimensional', 'electron', 'systems', 'at', ... | [-0.22362768174097478, 0.31169998079205025, -0.02570623911934782, 0.06986752522885273, -0.022859212259305112, -0.15300214957041702, 0.029929475030721218, 0.36755355914949245, -0.2669551126957643, -0.25936241145685035, -0.004904698700213559, -0.2947099175971915, -0.11053881279405926, 0.19503291115551344, 0.1393141659429... |
1,801.08535 | CommanderSong: A Systematic Approach for Practical Adversarial Voice
Recognition | The popularity of ASR (automatic speech recognition) systems, like Google
Voice, Cortana, brings in security concerns, as demonstrated by recent attacks.
The impacts of such threats, however, are less clear, since they are either
less stealthy (producing noise-like voice commands) or requiring the physical
presence o... | cs.CR cs.LG cs.SD eess.AS | the popularity of asr automatic speech recognition systems like google voice cortana brings in security concerns as demonstrated by recent attacks the impacts of such threats however are less clear since they are either less stealthy producing noiselike voice commands or requiring the physical presence of an attack dev... | [['the', 'popularity', 'of', 'asr', 'automatic', 'speech', 'recognition', 'systems', 'like', 'google', 'voice', 'cortana', 'brings', 'in', 'security', 'concerns', 'as', 'demonstrated', 'by', 'recent', 'attacks', 'the', 'impacts', 'of', 'such', 'threats', 'however', 'are', 'less', 'clear', 'since', 'they', 'are', 'eithe... | [-0.12640695465565294, 0.08740066585482369, -0.05790978790070686, 0.055817877164315334, -0.11620053015551798, -0.20681398974107432, 0.04335280076212966, 0.40785479115527024, -0.2521420363176807, -0.32993622966682423, 0.11636967691032128, -0.28987695941584507, -0.23327153655078692, 0.2796107389639907, -0.165058264362562... |
1,801.08536 | Cavity enhanced DUV laser for two-photon cooling of atomic hydrogen | We demonstrate a \SI{650}{\mW} \SI{243}{\nm} continuous-wave laser coupled to
a linear optical enhancement cavity. The enhancement cavity can maintain
$>$\SI{30}{\W} of intracavity power for \SI{1}{\hour} of continuous operation
without degradation. This system has sufficient power for a demonstration of
two-photon l... | physics.ins-det physics.atom-ph physics.optics | we demonstrate a si650mw si243nm continuouswave laser coupled to a linear optical enhancement cavity the enhancement cavity can maintain si30w of intracavity power for si1hour of continuous operation without degradation this system has sufficient power for a demonstration of twophoton laser cooling of hydrogen and may ... | [['we', 'demonstrate', 'a', 'si650mw', 'si243nm', 'continuouswave', 'laser', 'coupled', 'to', 'a', 'linear', 'optical', 'enhancement', 'cavity', 'the', 'enhancement', 'cavity', 'can', 'maintain', 'si30w', 'of', 'intracavity', 'power', 'for', 'si1hour', 'of', 'continuous', 'operation', 'without', 'degradation', 'this', ... | [-0.15433583250985697, 0.16426879027858377, -0.04270380354361036, -0.057512856556478746, -0.014793511820383944, -0.20843679222385758, 0.06867911822001378, 0.46331574572608447, -0.23384131738342917, -0.271741772392908, 0.03668318247386756, -0.22852024695692727, -0.07575386399045013, 0.3170499358899318, -0.02518434641667... |
1,801.08537 | A No-go Theorem for Superposed Actions (Making Schr\"odinger's Cat
Quantum Nonlocal) | The Extended Wigner's Friend thought experiment, which involves a quantum
system with an agent who draws conclusions based on the results of a
measurement of a quantum state provided in two nonorthogonal versions by
another agent, led its designers to the conclusion that quantum theory cannot
consistently explain the... | quant-ph | the extended wigners friend thought experiment which involves a quantum system with an agent who draws conclusions based on the results of a measurement of a quantum state provided in two nonorthogonal versions by another agent led its designers to the conclusion that quantum theory cannot consistently explain the use ... | [['the', 'extended', 'wigners', 'friend', 'thought', 'experiment', 'which', 'involves', 'a', 'quantum', 'system', 'with', 'an', 'agent', 'who', 'draws', 'conclusions', 'based', 'on', 'the', 'results', 'of', 'a', 'measurement', 'of', 'a', 'quantum', 'state', 'provided', 'in', 'two', 'nonorthogonal', 'versions', 'by', 'a... | [-0.0942087785607054, 0.14532720568922422, -0.16931362397369595, 0.09438230067742272, -0.0626796239692314, -0.2111729509718195, 0.06929649956201991, 0.317301403340343, -0.2103798337853872, -0.26308826647920314, 0.042125500704428845, -0.26056517598095474, -0.1651428728608636, 0.17681717487716384, -0.09551259014556848, 0... |
1,801.08538 | A Radiation Tolerant Light Pulser for Particle Physics Applications | A light emitting diode (LED) pulser has been developed that can be used for
tests or calibration of timing and amplitude sensitivity of particle physics
detectors. A comparative study is performed on the components and pulser output
characteristics before and after application of 800 MeV protons and cobalt-60
gammas.... | physics.ins-det hep-ex | a light emitting diode led pulser has been developed that can be used for tests or calibration of timing and amplitude sensitivity of particle physics detectors a comparative study is performed on the components and pulser output characteristics before and after application of 800 mev protons and cobalt60 gammas this d... | [['a', 'light', 'emitting', 'diode', 'led', 'pulser', 'has', 'been', 'developed', 'that', 'can', 'be', 'used', 'for', 'tests', 'or', 'calibration', 'of', 'timing', 'and', 'amplitude', 'sensitivity', 'of', 'particle', 'physics', 'detectors', 'a', 'comparative', 'study', 'is', 'performed', 'on', 'the', 'components', 'and... | [-0.010681597801989743, 0.20488265825967703, -0.07203903844846146, 0.019965223835814477, -0.002628678667575254, -0.1596707566375179, 0.05536822185219665, 0.45430651903152464, -0.14724760938967976, -0.41443572651062693, 0.08140352714274611, -0.315654651501349, 0.03143345908195313, 0.2878182568770301, -0.0450467104225286... |
1,801.08539 | Self-bound droplets of light with orbital angular momentum | Systems with competing attractive and repulsive interactions have a tendency
to condense into droplets. This is the case for water in a sink, liquid helium
and dipolar atomic gases. Here, we consider a photon fluid which is formed in
the transverse plane of a monochromatic laser beam propagating in an attractive
(foc... | cond-mat.quant-gas cond-mat.other physics.flu-dyn physics.optics quant-ph | systems with competing attractive and repulsive interactions have a tendency to condense into droplets this is the case for water in a sink liquid helium and dipolar atomic gases here we consider a photon fluid which is formed in the transverse plane of a monochromatic laser beam propagating in an attractive focusing n... | [['systems', 'with', 'competing', 'attractive', 'and', 'repulsive', 'interactions', 'have', 'a', 'tendency', 'to', 'condense', 'into', 'droplets', 'this', 'is', 'the', 'case', 'for', 'water', 'in', 'a', 'sink', 'liquid', 'helium', 'and', 'dipolar', 'atomic', 'gases', 'here', 'we', 'consider', 'a', 'photon', 'fluid', 'w... | [-0.18593043398112058, 0.24806076088279952, -0.09251164015103132, 0.058270055199041965, -0.033725941218435765, -0.12840083076804876, 0.009403714023530484, 0.3719840994402766, -0.23819969280064107, -0.2801718411371112, -0.004409858349710703, -0.3426669135093689, -0.09699981500394643, 0.11412012315541506, 0.0792418196126... |
1,801.0854 | The Kinematics of the Scorpius-Centaurus OB Association from Gaia DR1 | We present a kinematic study of the Scorpius-Centaurus (Sco-Cen) OB
association (Sco OB2) using Gaia DR1 parallaxes and proper motions. Our goal is
to test the classical theory that OB associations are the expanded remnants of
dense and compact star clusters disrupted by processes such as residual gas
expulsion. Gaia... | astro-ph.SR astro-ph.GA | we present a kinematic study of the scorpiuscentaurus scocen ob association sco ob2 using gaia dr1 parallaxes and proper motions our goal is to test the classical theory that ob associations are the expanded remnants of dense and compact star clusters disrupted by processes such as residual gas expulsion gaia astrometr... | [['we', 'present', 'a', 'kinematic', 'study', 'of', 'the', 'scorpiuscentaurus', 'scocen', 'ob', 'association', 'sco', 'ob2', 'using', 'gaia', 'dr1', 'parallaxes', 'and', 'proper', 'motions', 'our', 'goal', 'is', 'to', 'test', 'the', 'classical', 'theory', 'that', 'ob', 'associations', 'are', 'the', 'expanded', 'remnant... | [-0.09496769659780534, 0.09288788063891044, -0.1294473436456628, 0.11264462115070821, -0.12422455643773139, -0.011252485014539878, 0.10798940081972765, 0.4375696012133172, -0.2004859955864012, -0.30231790821545007, 0.06979923751167347, -0.26234398226109823, -0.033236843458569906, 0.18551196300754005, -0.026966080933665... |
1,801.08541 | Galaxy Zoo: Morphological classification of galaxy images from the
Illustris simulation | Modern cosmological simulations model the universe with increasing
sophistication and at higher spatial and temporal resolutions. These
enhancements permit detailed comparisons between the simulation outputs and
real observational data. Recent projects such as Illustris are capable of
producing simulated images that ... | astro-ph.GA astro-ph.CO astro-ph.IM | modern cosmological simulations model the universe with increasing sophistication and at higher spatial and temporal resolutions these enhancements permit detailed comparisons between the simulation outputs and real observational data recent projects such as illustris are capable of producing simulated images that are ... | [['modern', 'cosmological', 'simulations', 'model', 'the', 'universe', 'with', 'increasing', 'sophistication', 'and', 'at', 'higher', 'spatial', 'and', 'temporal', 'resolutions', 'these', 'enhancements', 'permit', 'detailed', 'comparisons', 'between', 'the', 'simulation', 'outputs', 'and', 'real', 'observational', 'dat... | [-0.023905953471548856, 0.04127224773797206, -0.09288489270210266, 0.14059316609241068, -0.09556127383932471, -0.07357171219075098, 0.0019746897565200926, 0.44696935057640075, -0.14978286863025278, -0.4090586187392473, 0.039064308504574, -0.3177960399761796, -0.11224254042375832, 0.25022576936613766, -0.063955520011484... |
1,801.08542 | Fourier domain gravitational waveforms for precessing eccentric binaries | We build two families of inspiral waveforms for precessing binaries on
eccentric orbits in the Fourier domain. To achieve this, we use a small
eccentricity expansion of the waveform amplitudes in order to separate the
periastron precession timescale from the orbital timescale, and use a shifted
uniform asymptotics tr... | gr-qc astro-ph.CO | we build two families of inspiral waveforms for precessing binaries on eccentric orbits in the fourier domain to achieve this we use a small eccentricity expansion of the waveform amplitudes in order to separate the periastron precession timescale from the orbital timescale and use a shifted uniform asymptotics transfo... | [['we', 'build', 'two', 'families', 'of', 'inspiral', 'waveforms', 'for', 'precessing', 'binaries', 'on', 'eccentric', 'orbits', 'in', 'the', 'fourier', 'domain', 'to', 'achieve', 'this', 'we', 'use', 'a', 'small', 'eccentricity', 'expansion', 'of', 'the', 'waveform', 'amplitudes', 'in', 'order', 'to', 'separate', 'the... | [-0.18865044695611288, 0.1430945310042981, -0.09208764750632195, 0.03813544966986561, -0.08675220440707955, -0.024801038126491644, 0.005680360860233895, 0.37631579157987644, -0.24233149889296565, -0.28026882930220487, 0.09222303196145648, -0.24666875875037578, -0.08727272891506456, 0.24735325830532054, -0.0805075923467... |
1,801.08543 | Planet Occurrence: Doppler and Transit Surveys | Prior to the 1990s, speculations about the occurrence of planets around other
stars were based only on planet formation theory, observations of circumstellar
disks, and the knowledge that at least one seemingly ordinary star had managed
to make a variety of different planets. Since then, Doppler and transit surveys
h... | astro-ph.EP | prior to the 1990s speculations about the occurrence of planets around other stars were based only on planet formation theory observations of circumstellar disks and the knowledge that at least one seemingly ordinary star had managed to make a variety of different planets since then doppler and transit surveys have rev... | [['prior', 'to', 'the', '1990s', 'speculations', 'about', 'the', 'occurrence', 'of', 'planets', 'around', 'other', 'stars', 'were', 'based', 'only', 'on', 'planet', 'formation', 'theory', 'observations', 'of', 'circumstellar', 'disks', 'and', 'the', 'knowledge', 'that', 'at', 'least', 'one', 'seemingly', 'ordinary', 's... | [-0.09861344154219792, 0.15165581658263416, -0.08856933830626809, 0.04816617263567109, -0.18063959931884305, -0.07665915837307938, 0.04695312132835858, 0.3721953656195718, -0.14613571082155744, -0.39008717751521776, 0.12548662785503292, -0.3072469769558818, -0.08472694847106683, 0.24731108178423733, -0.0910328338157479... |
1,801.08544 | New Constraints on the Geometry and Kinematics of Matter Surrounding the
Accretion Flow in X-ray Binaries from $Chandra$ HETG X-ray Spectroscopy | The narrow, neutral Fe K{\alpha} fluorescence emission line in X-ray binaries
(XRBs) is a powerful probe of the geometry, kinematics and Fe abundance of
matter around the accretion flow. In a recent study it has been claimed, using
$Chandra$ High-Energy Transmission Grating (HETG) spectra for a sample of XRBs,
that t... | astro-ph.HE astro-ph.SR | the narrow neutral fe kalpha fluorescence emission line in xray binaries xrbs is a powerful probe of the geometry kinematics and fe abundance of matter around the accretion flow in a recent study it has been claimed using chandra highenergy transmission grating hetg spectra for a sample of xrbs that the circumnuclear m... | [['the', 'narrow', 'neutral', 'fe', 'kalpha', 'fluorescence', 'emission', 'line', 'in', 'xray', 'binaries', 'xrbs', 'is', 'a', 'powerful', 'probe', 'of', 'the', 'geometry', 'kinematics', 'and', 'fe', 'abundance', 'of', 'matter', 'around', 'the', 'accretion', 'flow', 'in', 'a', 'recent', 'study', 'it', 'has', 'been', 'c... | [-0.019192868588067104, 0.06341275184354542, -0.03278827953111866, 0.11555533547450424, -0.08506983410232984, -0.15981236811443839, 0.04496711418640031, 0.5091901214793324, -0.13571986668216793, -0.3332635080057156, 0.0461675277830142, -0.3286535947462139, 0.008595813922179134, 0.16366556039707655, 0.003596320506387754... |
1,801.08545 | Direct Collapse to Supermassive Black Hole Seeds with Radiative
Transfer: Isolated Halos | Direct collapse within dark matter (DM) halos is a promising path to form
supermassive black hole (SMBH) seeds at high redshifts. The outer part of this
collapse remains optically thin, and has been studied intensively using
numerical simulations. However, the innermost region of the collapse is
expected to become op... | astro-ph.GA | direct collapse within dark matter dm halos is a promising path to form supermassive black hole smbh seeds at high redshifts the outer part of this collapse remains optically thin and has been studied intensively using numerical simulations however the innermost region of the collapse is expected to become optically th... | [['direct', 'collapse', 'within', 'dark', 'matter', 'dm', 'halos', 'is', 'a', 'promising', 'path', 'to', 'form', 'supermassive', 'black', 'hole', 'smbh', 'seeds', 'at', 'high', 'redshifts', 'the', 'outer', 'part', 'of', 'this', 'collapse', 'remains', 'optically', 'thin', 'and', 'has', 'been', 'studied', 'intensively', ... | [-0.07909436617349759, 0.1342138410065369, -0.05026972782151359, 0.10433581723945433, -0.06538596386720504, -0.05399286109766561, -0.005181323175848875, 0.3908083981052389, -0.22761909147892664, -0.32752197862848537, 0.09907852995254668, -0.27751039995281546, 0.0032960458205100926, 0.17577831548987888, 0.03555173034520... |
1,801.08546 | Proof of the Weak Gravity Conjecture from Black Hole Entropy | We prove that higher-dimension operators contribute positively to the entropy
of a thermodynamically stable black hole at fixed mass and charge. Our results
apply whenever the dominant corrections originate at tree level from quantum
field theoretic dynamics. More generally, positivity of the entropy shift is
equival... | hep-th gr-qc hep-ph | we prove that higherdimension operators contribute positively to the entropy of a thermodynamically stable black hole at fixed mass and charge our results apply whenever the dominant corrections originate at tree level from quantum field theoretic dynamics more generally positivity of the entropy shift is equivalent to... | [['we', 'prove', 'that', 'higherdimension', 'operators', 'contribute', 'positively', 'to', 'the', 'entropy', 'of', 'a', 'thermodynamically', 'stable', 'black', 'hole', 'at', 'fixed', 'mass', 'and', 'charge', 'our', 'results', 'apply', 'whenever', 'the', 'dominant', 'corrections', 'originate', 'at', 'tree', 'level', 'fr... | [-0.14072012997405858, 0.20135676256448312, -0.047447165087766315, 0.16721263236907963, -0.04385660174820158, -0.19077438874675412, 0.0360674832698743, 0.2506280893374697, -0.20979810254404846, -0.27349261274816944, 0.08617436306496315, -0.3161757485286692, -0.06284239830059651, 0.20448939056665288, -0.0674120448955815... |
1,801.08547 | Inferring binary and trinary stellar populations in photometric and
astrometric surveys | Multiple stellar systems are ubiquitous in the Milky Way, but are often
unresolved and seen as single objects in spectroscopic, photometric, and
astrometric surveys. Yet, modeling them is essential for developing a full
understanding of large surveys such as Gaia, and connecting them to stellar and
Galactic models. I... | astro-ph.SR astro-ph.GA | multiple stellar systems are ubiquitous in the milky way but are often unresolved and seen as single objects in spectroscopic photometric and astrometric surveys yet modeling them is essential for developing a full understanding of large surveys such as gaia and connecting them to stellar and galactic models in this pa... | [['multiple', 'stellar', 'systems', 'are', 'ubiquitous', 'in', 'the', 'milky', 'way', 'but', 'are', 'often', 'unresolved', 'and', 'seen', 'as', 'single', 'objects', 'in', 'spectroscopic', 'photometric', 'and', 'astrometric', 'surveys', 'yet', 'modeling', 'them', 'is', 'essential', 'for', 'developing', 'a', 'full', 'und... | [-0.0647622395322883, 0.03947976965071826, -0.08280946863494043, 0.1219076492518572, -0.15568448803548154, -0.11115938901644329, 0.06710926586007378, 0.4302200018075006, -0.23670147786816131, -0.38205366586816725, 0.1048065273789689, -0.3068334949476813, -0.10362522058060457, 0.23868115182709077, -0.088542128354311, 0.... |
1,801.08548 | Non-topological parafermions in a one-dimensional fermionic model with
even multiplet pairing | We discuss a one-dimensional fermionic model with a generalized
$\mathbb{Z}_{N}$ even multiplet pairing extending Kitaev $\mathbb{Z}_{2}$
chain. The system shares many features with models believed to host localized
edge parafermions, the most prominent being a similar bosonized Hamiltonian and
a $\mathbb{Z}_{N}$ sym... | cond-mat.str-el | we discuss a onedimensional fermionic model with a generalized mathbbz_n even multiplet pairing extending kitaev mathbbz_2 chain the system shares many features with models believed to host localized edge parafermions the most prominent being a similar bosonized hamiltonian and a mathbbz_n symmetry enforcing an nfold d... | [['we', 'discuss', 'a', 'onedimensional', 'fermionic', 'model', 'with', 'a', 'generalized', 'mathbbz_n', 'even', 'multiplet', 'pairing', 'extending', 'kitaev', 'mathbbz_2', 'chain', 'the', 'system', 'shares', 'many', 'features', 'with', 'models', 'believed', 'to', 'host', 'localized', 'edge', 'parafermions', 'the', 'mo... | [-0.2640513143311525, 0.23782681721533425, -0.02938235384425607, 0.08470471039164704, -0.06353420012232348, -0.24749517416500527, 0.0014296527445802221, 0.32348799648816173, -0.24646115391869503, -0.24574046269518093, 0.06353007368591573, -0.31568180837843945, -0.1304547803854381, 0.05770260880134352, 0.012387665126985... |
1,801.08549 | Conformal blocks from Wilson lines with loop corrections | We compute the conformal blocks of the Virasoro minimal model or its W$_N$
extension with large central charge from Wilson line networks in a Chern-Simons
theory including loop corrections. In our previous work, we offered a
prescription to regularize divergences from loops attached to Wilson lines. In
this paper, we... | hep-th | we compute the conformal blocks of the virasoro minimal model or its w_n extension with large central charge from wilson line networks in a chernsimons theory including loop corrections in our previous work we offered a prescription to regularize divergences from loops attached to wilson lines in this paper we generali... | [['we', 'compute', 'the', 'conformal', 'blocks', 'of', 'the', 'virasoro', 'minimal', 'model', 'or', 'its', 'w_n', 'extension', 'with', 'large', 'central', 'charge', 'from', 'wilson', 'line', 'networks', 'in', 'a', 'chernsimons', 'theory', 'including', 'loop', 'corrections', 'in', 'our', 'previous', 'work', 'we', 'offer... | [-0.08151556267556823, 0.08753101562395832, -0.03676911345068014, 0.07083091072909499, -0.030983590797679324, -0.1917751075629637, 0.017077967757359147, 0.36254156054489595, -0.1625788185244672, -0.23046104884530716, 0.09579870354863024, -0.29946967144057435, -0.20061778522289866, 0.13718645125715379, -0.06857515053322... |
1,801.0855 | Two-Player Pebbling on Diameter 2 Graphs | A pebbling move refers to the act of removing two pebbles from one vertex and
placing one pebble on an adjacent vertex. The goal of graph pebbling is: Given
an initial distribution of pebbles, use pebbling moves to reach a specified
goal vertex called the root. The pebbling number of a graph $\pi(G)$ is the
minimum n... | math.CO | a pebbling move refers to the act of removing two pebbles from one vertex and placing one pebble on an adjacent vertex the goal of graph pebbling is given an initial distribution of pebbles use pebbling moves to reach a specified goal vertex called the root the pebbling number of a graph pig is the minimum number of pe... | [['a', 'pebbling', 'move', 'refers', 'to', 'the', 'act', 'of', 'removing', 'two', 'pebbles', 'from', 'one', 'vertex', 'and', 'placing', 'one', 'pebble', 'on', 'an', 'adjacent', 'vertex', 'the', 'goal', 'of', 'graph', 'pebbling', 'is', 'given', 'an', 'initial', 'distribution', 'of', 'pebbles', 'use', 'pebbling', 'moves'... | [-0.10283910904302081, 0.12046507230821699, -0.09865075342336309, 0.009306837635205142, -0.14204436668486736, -0.2022639336064458, 0.11874268554262261, 0.329997346811205, -0.3113485956008532, -0.3328274160123138, 0.03904427181574891, -0.33092204439662287, -0.08157410576883982, 0.04451897011986419, -0.18242104744900073,... |
1,801.08551 | Power Corrections to the Universal Heavy WIMP-Nucleon Cross Section | WIMP-nucleon scattering is analyzed at order $1/M$ in Heavy WIMP Effective
Theory. The $1/M$ power corrections, where $M\gg m_W$ is the WIMP mass,
distinguish between different underlying UV models with the same universal
limit and their impact on direct detection rates can be enhanced relative to
naive expectations ... | hep-ph astro-ph.CO | wimpnucleon scattering is analyzed at order 1m in heavy wimp effective theory the 1m power corrections where mgg m_w is the wimp mass distinguish between different underlying uv models with the same universal limit and their impact on direct detection rates can be enhanced relative to naive expectations due to generic ... | [['wimpnucleon', 'scattering', 'is', 'analyzed', 'at', 'order', '1m', 'in', 'heavy', 'wimp', 'effective', 'theory', 'the', '1m', 'power', 'corrections', 'where', 'mgg', 'm_w', 'is', 'the', 'wimp', 'mass', 'distinguish', 'between', 'different', 'underlying', 'uv', 'models', 'with', 'the', 'same', 'universal', 'limit', '... | [-0.09971260141464881, 0.2065321613690685, -0.016875135691225295, 0.15775720800641768, -0.03306756266586793, -0.12635812589724082, 0.019535487277122836, 0.312886378436815, -0.15883594379653612, -0.32772001245757565, 0.029701520402159075, -0.33983009492512795, -0.03249824216303144, 0.18664003678034835, 0.061269274945758... |
1,801.08552 | Correlating nonlinear properties with spectral states of RXTE data:
Possible observational evidences for four different accretion modes around
compact objects | By analyzing the time series of RXTE/PCA data, the nonlinear variabilities of
compact sources have been repeatedly established. Depending on the variation in
temporal classes, compact sources exhibit different nonlinear features.
Sometimes they show low correlation/fractal dimension, but in other classes or
intervals... | astro-ph.HE | by analyzing the time series of rxtepca data the nonlinear variabilities of compact sources have been repeatedly established depending on the variation in temporal classes compact sources exhibit different nonlinear features sometimes they show low correlationfractal dimension but in other classes or intervals of time ... | [['by', 'analyzing', 'the', 'time', 'series', 'of', 'rxtepca', 'data', 'the', 'nonlinear', 'variabilities', 'of', 'compact', 'sources', 'have', 'been', 'repeatedly', 'established', 'depending', 'on', 'the', 'variation', 'in', 'temporal', 'classes', 'compact', 'sources', 'exhibit', 'different', 'nonlinear', 'features', ... | [-0.12755404935857326, 0.10066105880900449, -0.08716912228224236, 0.10813399066682905, -0.11250849481737024, -0.11473965031679632, -0.020747428979767963, 0.3899572732576797, -0.28609205689497813, -0.2950421068817377, 0.13743009712698676, -0.2699080766552279, -0.09146963726014419, 0.23011186147476873, -0.042408740322706... |
1,801.08553 | Constraints on the sum of the neutrino masses in dynamical dark energy
models with $w(z) \geq -1$ are tighter than those obtained in $\Lambda$CDM | We explore cosmological constraints on the sum of the three active neutrino
masses $M_{\nu}$ in the context of dynamical dark energy (DDE) models with
equation of state (EoS) parametrized as a function of redshift $z$ by
$w(z)=w_0+w_a\,z/(1+z)$, and satisfying $w(z)\geq-1$ for all $z$. We perform a
Bayesian analysis ... | astro-ph.CO gr-qc hep-ph | we explore cosmological constraints on the sum of the three active neutrino masses m_nu in the context of dynamical dark energy dde models with equation of state eos parametrized as a function of redshift z by wzw_0w_az1z and satisfying wzgeq1 for all z we perform a bayesian analysis and show that within these models t... | [['we', 'explore', 'cosmological', 'constraints', 'on', 'the', 'sum', 'of', 'the', 'three', 'active', 'neutrino', 'masses', 'm_nu', 'in', 'the', 'context', 'of', 'dynamical', 'dark', 'energy', 'dde', 'models', 'with', 'equation', 'of', 'state', 'eos', 'parametrized', 'as', 'a', 'function', 'of', 'redshift', 'z', 'by', ... | [-0.08256743467063643, 0.11883267129605608, -0.07025992582643856, 0.099201298403469, -0.08482555303789648, -0.13799317849131484, 0.09552559917298795, 0.31244632851148985, -0.17149006534777017, -0.3437355075300068, 0.07600903980456872, -0.2642313601303282, -0.03827205605127595, 0.23715966722793932, 0.03903560813738626, ... |
1,801.08554 | Precise extrapolation of the correlation function asymptotics in uniform
tensor network states with application to the Bose-Hubbard and XXZ models | We analyze the problem of extracting the correlation length from infinite
matrix product states (MPS) and corner transfer matrix (CTM) simulations. When
the correlation length is calculated directly from the transfer matrix, it is
typically significantly underestimated for finite bond dimensions used in
numerical sim... | cond-mat.str-el quant-ph | we analyze the problem of extracting the correlation length from infinite matrix product states mps and corner transfer matrix ctm simulations when the correlation length is calculated directly from the transfer matrix it is typically significantly underestimated for finite bond dimensions used in numerical simulation ... | [['we', 'analyze', 'the', 'problem', 'of', 'extracting', 'the', 'correlation', 'length', 'from', 'infinite', 'matrix', 'product', 'states', 'mps', 'and', 'corner', 'transfer', 'matrix', 'ctm', 'simulations', 'when', 'the', 'correlation', 'length', 'is', 'calculated', 'directly', 'from', 'the', 'transfer', 'matrix', 'it... | [-0.06605975670947865, 0.09669719612662543, -0.08032293824583489, 0.10271796398441133, -0.009860950705776661, -0.1299262640186318, 0.05628629774162577, 0.3493834094484621, -0.2739454321071456, -0.27989501978667214, 0.09592324749585057, -0.3009265990798721, -0.14132358153925428, 0.19188292353051306, 0.02619501146435639,... |
1,801.08555 | A Model for Protostellar Cluster Luminosities and the Impact on the
CO-H$_2$ Conversion Factor | We construct a semi-analytic model to study the effect of far-ultraviolet
(FUV) radiation on gas chemistry from embedded protostars. We use the
Protostellar Luminosity Function (PLF) formalism of Offner & McKee (2011) to
calculate the total, FUV, and ionizing cluster luminosity for various
protostellar accretion hist... | astro-ph.GA astro-ph.SR | we construct a semianalytic model to study the effect of farultraviolet fuv radiation on gas chemistry from embedded protostars we use the protostellar luminosity function plf formalism of offner mckee 2011 to calculate the total fuv and ionizing cluster luminosity for various protostellar accretion histories and clust... | [['we', 'construct', 'a', 'semianalytic', 'model', 'to', 'study', 'the', 'effect', 'of', 'farultraviolet', 'fuv', 'radiation', 'on', 'gas', 'chemistry', 'from', 'embedded', 'protostars', 'we', 'use', 'the', 'protostellar', 'luminosity', 'function', 'plf', 'formalism', 'of', 'offner', 'mckee', '2011', 'to', 'calculate',... | [0.0013018280793076907, 0.08570736848080579, -0.005475783634644288, 0.10704212208779959, -0.03601182489775312, 0.013738975423173263, 0.04604446850478267, 0.46171427942239324, -0.17281291611397115, -0.3601177034708552, -0.01805453265014176, -0.2782200118717857, 0.006651424703737482, 0.15033443439274263, 0.01479511191361... |
1,801.08556 | Thermalization of plastic flow versus stationarity of thermomechanical
equilibrium in SGR theory | We discuss issues related to thermalization of plastic flow in the context of
soft glassy rheology (SGR) theory. An apparent problem with the theory in its
current form is that the stationarity of thermomechanical equilibrium obtained
by requiring that its flow rule satisfy detailed balance in the absence of
applied ... | cond-mat.soft | we discuss issues related to thermalization of plastic flow in the context of soft glassy rheology sgr theory an apparent problem with the theory in its current form is that the stationarity of thermomechanical equilibrium obtained by requiring that its flow rule satisfy detailed balance in the absence of applied defor... | [['we', 'discuss', 'issues', 'related', 'to', 'thermalization', 'of', 'plastic', 'flow', 'in', 'the', 'context', 'of', 'soft', 'glassy', 'rheology', 'sgr', 'theory', 'an', 'apparent', 'problem', 'with', 'the', 'theory', 'in', 'its', 'current', 'form', 'is', 'that', 'the', 'stationarity', 'of', 'thermomechanical', 'equi... | [-0.0968316571795315, 0.16330794144297606, -0.15962323067443712, 0.04584322028780922, -0.09884981128769661, -0.1440539506480231, -0.008060087865617658, 0.36295068216402016, -0.30645558076711105, -0.24568908621690103, 0.12050674032902212, -0.245229345979169, -0.15847837803552725, 0.12893769594510168, -0.1224865167459938... |
1,801.08557 | Fracturing of topological Maxwell lattices | We present fracturing analysis of topological Maxwell lattices when they are
stretched by applied stress. Maxwell lattices are mechanical structures
containing equal numbers of degrees of freedom and constraints in the bulk and
are thus on the verge of mechanical instability. Recent progress in topological
mechanics ... | cond-mat.soft cond-mat.mes-hall cond-mat.mtrl-sci | we present fracturing analysis of topological maxwell lattices when they are stretched by applied stress maxwell lattices are mechanical structures containing equal numbers of degrees of freedom and constraints in the bulk and are thus on the verge of mechanical instability recent progress in topological mechanics led ... | [['we', 'present', 'fracturing', 'analysis', 'of', 'topological', 'maxwell', 'lattices', 'when', 'they', 'are', 'stretched', 'by', 'applied', 'stress', 'maxwell', 'lattices', 'are', 'mechanical', 'structures', 'containing', 'equal', 'numbers', 'of', 'degrees', 'of', 'freedom', 'and', 'constraints', 'in', 'the', 'bulk',... | [-0.168931867682905, 0.22884741218925264, -0.05694113090603473, -0.011789163578978131, -0.09331676291072875, -0.12114204325615455, 0.016372926308109697, 0.3883660978004748, -0.2729506104546522, -0.2398480678090404, 0.10715645914691506, -0.2813129674267662, -0.1924442774037321, 0.1439142741336235, -0.03376753450222108, ... |
1,801.08558 | Deep Learning for End-to-End Automatic Target Recognition from Synthetic
Aperture Radar Imagery | The standard architecture of synthetic aperture radar (SAR) automatic target
recognition (ATR) consists of three stages: detection, discrimination, and
classification. In recent years, convolutional neural networks (CNNs) for SAR
ATR have been proposed, but most of them classify target classes from a target
chip extr... | cs.CV | the standard architecture of synthetic aperture radar sar automatic target recognition atr consists of three stages detection discrimination and classification in recent years convolutional neural networks cnns for sar atr have been proposed but most of them classify target classes from a target chip extracted from sar... | [['the', 'standard', 'architecture', 'of', 'synthetic', 'aperture', 'radar', 'sar', 'automatic', 'target', 'recognition', 'atr', 'consists', 'of', 'three', 'stages', 'detection', 'discrimination', 'and', 'classification', 'in', 'recent', 'years', 'convolutional', 'neural', 'networks', 'cnns', 'for', 'sar', 'atr', 'have... | [-0.02530800618842477, -0.031974887850810776, -0.0013681414031452733, -0.008400386334687936, -0.03782000262872316, -0.2147692073864164, -0.02345457725259621, 0.4595636080252007, -0.20286752607571543, -0.3574343209620565, 0.10221664621931267, -0.2639404757588636, -0.17219489409453673, 0.2142586255504284, -0.159995380547... |
1,801.08559 | The impact of baryons on the matter power spectrum from the Horizon-AGN
cosmological hydrodynamical simulation | Accurate cosmology from upcoming weak lensing surveys relies on knowledge of
the total matter power spectrum at percent level at scales $k < 10$ $h$/Mpc,
for which modelling the impact of baryonic physics is crucial. We compare
measurements of the total matter power spectrum from the Horizon cosmological
hydrodynamic... | astro-ph.CO | accurate cosmology from upcoming weak lensing surveys relies on knowledge of the total matter power spectrum at percent level at scales k 10 hmpc for which modelling the impact of baryonic physics is crucial we compare measurements of the total matter power spectrum from the horizon cosmological hydrodynamical simulati... | [['accurate', 'cosmology', 'from', 'upcoming', 'weak', 'lensing', 'surveys', 'relies', 'on', 'knowledge', 'of', 'the', 'total', 'matter', 'power', 'spectrum', 'at', 'percent', 'level', 'at', 'scales', 'k', '10', 'hmpc', 'for', 'which', 'modelling', 'the', 'impact', 'of', 'baryonic', 'physics', 'is', 'crucial', 'we', 'c... | [-0.07177678225537723, 0.1124691806018139, -0.08808355208699746, 0.10151593851430031, -0.08407125141626845, -0.048736124821395305, 0.006943872793150755, 0.3431904114802213, -0.20220568449003623, -0.38608315096159157, 0.035685084937237356, -0.32539885144215075, -0.012760434802233551, 0.2216084763679343, 0.04957630192608... |
1,801.0856 | A Tractable Analysis of the Blind-spot Probability in Localization
Networks under Correlated Blocking | In localization applications, the line-of-sight between anchors and targets
may be blocked by obstacles in the environment. A target that is invisible
(i.e., without line-of-sight) to a sufficient number of anchors cannot be
unambiguously localized and is, therefore, said to be in a blind spot. In this
paper, we anal... | cs.NI | in localization applications the lineofsight between anchors and targets may be blocked by obstacles in the environment a target that is invisible ie without lineofsight to a sufficient number of anchors cannot be unambiguously localized and is therefore said to be in a blind spot in this paper we analyze the blind spo... | [['in', 'localization', 'applications', 'the', 'lineofsight', 'between', 'anchors', 'and', 'targets', 'may', 'be', 'blocked', 'by', 'obstacles', 'in', 'the', 'environment', 'a', 'target', 'that', 'is', 'invisible', 'ie', 'without', 'lineofsight', 'to', 'a', 'sufficient', 'number', 'of', 'anchors', 'can', 'not', 'be', '... | [-0.09766876088563824, 0.09936518309638187, -0.06027458629399104, 0.09025180784508459, -0.06345042847187339, -0.148959503981547, 0.13339579341316016, 0.3929409575784235, -0.27052642073814565, -0.31371902025449405, 0.10147216973783339, -0.24811742246915017, -0.11357896642994533, 0.12638010864950788, -0.10403680729903551... |
1,801.08561 | Exotic components of $\mathrm{SO}(p,q)$ surface group representations,
and their Higgs bundle avatars | For semisimple Lie groups, moduli spaces of Higgs bundles on a Riemann
surface correspond to representation varieties for the surface fundamental
group. In many cases, natural topological invariants label connected components
of the moduli spaces. Hitchin representations into split real forms, and
maximal representat... | math.AG | for semisimple lie groups moduli spaces of higgs bundles on a riemann surface correspond to representation varieties for the surface fundamental group in many cases natural topological invariants label connected components of the moduli spaces hitchin representations into split real forms and maximal representations in... | [['for', 'semisimple', 'lie', 'groups', 'moduli', 'spaces', 'of', 'higgs', 'bundles', 'on', 'a', 'riemann', 'surface', 'correspond', 'to', 'representation', 'varieties', 'for', 'the', 'surface', 'fundamental', 'group', 'in', 'many', 'cases', 'natural', 'topological', 'invariants', 'label', 'connected', 'components', 'o... | [-0.1957304605415889, 0.13330875136782605, -0.08210192820323366, 0.12386055872656823, -0.17910131919958003, -0.13508394134839122, -0.030006445298085407, 0.3619105215469489, -0.3165921482818239, -0.23129942051458116, 0.10856238881967087, -0.22655698084937675, -0.16964718515507174, 0.22761692558724092, -0.134721633070623... |
1,801.08562 | N* Structure and Strong QCD | In attempting to match QCD with Nature, it is necessary to confront the many
complexities of strong, nonlinear dynamics in relativistic quantum field
theory, e.g. the loss of particle number conservation, the frame and scale
dependence of the explanations and interpretations of observable processes, and
the evolving ... | nucl-th hep-lat hep-ph nucl-ex | in attempting to match qcd with nature it is necessary to confront the many complexities of strong nonlinear dynamics in relativistic quantum field theory eg the loss of particle number conservation the frame and scale dependence of the explanations and interpretations of observable processes and the evolving character... | [['in', 'attempting', 'to', 'match', 'qcd', 'with', 'nature', 'it', 'is', 'necessary', 'to', 'confront', 'the', 'many', 'complexities', 'of', 'strong', 'nonlinear', 'dynamics', 'in', 'relativistic', 'quantum', 'field', 'theory', 'eg', 'the', 'loss', 'of', 'particle', 'number', 'conservation', 'the', 'frame', 'and', 'sc... | [-0.057911505677351136, 0.22326726801239136, -0.13105645373525254, 0.1293021865285615, -0.09805614999836175, -0.116627693141061, 0.030994214672913276, 0.3518428617293333, -0.24165348187316119, -0.31282153797404066, 0.052348991900273575, -0.2980151737972004, -0.07908795224076773, 0.11929308864935415, -0.0116149684187115... |
1,801.08563 | Flow and Thermal Fields Investigation in Divergent Micro/Nano Channels | The present work is related to the study of the nitrogen gas flow through
diverging micro and nano-channels. The direct simulation Monte-Carlo (DSMC)
method has been used to study the flow. The Simplified Bernoulli Trials (SBT)
collision scheme has been employed to reduce the computational costs and
required amounts ... | physics.flu-dyn | the present work is related to the study of the nitrogen gas flow through diverging micro and nanochannels the direct simulation montecarlo dsmc method has been used to study the flow the simplified bernoulli trials sbt collision scheme has been employed to reduce the computational costs and required amounts of the com... | [['the', 'present', 'work', 'is', 'related', 'to', 'the', 'study', 'of', 'the', 'nitrogen', 'gas', 'flow', 'through', 'diverging', 'micro', 'and', 'nanochannels', 'the', 'direct', 'simulation', 'montecarlo', 'dsmc', 'method', 'has', 'been', 'used', 'to', 'study', 'the', 'flow', 'the', 'simplified', 'bernoulli', 'trials... | [-0.1252576757169855, 0.16555898979832792, -0.10547879032342683, -0.0010073942678512904, -0.040433506495103175, -0.10321355700681481, -0.002874936490960199, 0.3531304913246808, -0.2860701413891958, -0.3092947196547445, 0.10371677871726705, -0.30356409233299236, -0.07014477217200563, 0.1968746793707872, -0.0133481311291... |
1,801.08564 | An Asymptotically Tight Bound on the Number of Relevant Variables in a
Bounded Degree Boolean Function | We prove that there is a constant $C\leq 6.614$ such that every Boolean
function of degree at most $d$ (as a polynomial over $\mathbb{R}$) is a $C\cdot
2^d$-junta, i.e. it depends on at most $C\cdot 2^d$ variables. This improves
the $d\cdot 2^{d-1}$ upper bound of Nisan and Szegedy [Computational Complexity
4 (1994)]... | math.CO cs.CC | we prove that there is a constant cleq 6614 such that every boolean function of degree at most d as a polynomial over mathbbr is a ccdot 2djunta ie it depends on at most ccdot 2d variables this improves the dcdot 2d1 upper bound of nisan and szegedy computational complexity 4 1994 our proof uses a new weighting scheme ... | [['we', 'prove', 'that', 'there', 'is', 'a', 'constant', 'cleq', '6614', 'such', 'that', 'every', 'boolean', 'function', 'of', 'degree', 'at', 'most', 'd', 'as', 'a', 'polynomial', 'over', 'mathbbr', 'is', 'a', 'ccdot', '2djunta', 'ie', 'it', 'depends', 'on', 'at', 'most', 'ccdot', '2d', 'variables', 'this', 'improves'... | [-0.15128256367700202, 0.1270440167064584, -0.039800153193828555, 0.02126554811786888, -0.049701134260716054, -0.22312699204811187, 0.10157134493729517, 0.309521938472597, -0.24103183125722596, -0.3013933697374843, 0.07658493601883859, -0.254274235204307, -0.14723643612415432, 0.1988737924031413, -0.06769245357249182, ... |
1,801.08565 | Rollercoasters and Caterpillars | A rollercoaster is a sequence of real numbers for which every maximal
contiguous subsequence, that is increasing or decreasing, has length at least
three. By translating this sequence to a set of points in the plane, a
rollercoaster can be defined as a polygonal path for which every maximal
sub-path, with positive- o... | cs.CG cs.DM cs.DS | a rollercoaster is a sequence of real numbers for which every maximal contiguous subsequence that is increasing or decreasing has length at least three by translating this sequence to a set of points in the plane a rollercoaster can be defined as a polygonal path for which every maximal subpath with positive or negativ... | [['a', 'rollercoaster', 'is', 'a', 'sequence', 'of', 'real', 'numbers', 'for', 'which', 'every', 'maximal', 'contiguous', 'subsequence', 'that', 'is', 'increasing', 'or', 'decreasing', 'has', 'length', 'at', 'least', 'three', 'by', 'translating', 'this', 'sequence', 'to', 'a', 'set', 'of', 'points', 'in', 'the', 'plane... | [-0.19195320200646834, 0.13522837280537428, -0.06895872395130266, 0.013929198289253307, -0.05833071407457618, -0.1368345131677894, 0.07651476192289633, 0.35925030888756737, -0.261634539347142, -0.2843467009891021, 0.10090354242435608, -0.3242589632764544, -0.14949419696993, 0.181483941975258, -0.08268913484062068, 0.01... |
1,801.08566 | The integrated Sachs-Wolfe effect in the AvERA cosmology | The recent AvERA cosmological simulation of R\'acz et al. (2017) has a
$\Lambda \mathrm{CDM}$-like expansion history and removes the tension between
local and Planck (cosmic microwave background) Hubble constants. We contrast
the AvERA prediction of the integrated Sachs--Wolfe (ISW) effect with that of
$\Lambda \math... | astro-ph.CO | the recent avera cosmological simulation of racz et al 2017 has a lambda mathrmcdmlike expansion history and removes the tension between local and planck cosmic microwave background hubble constants we contrast the avera prediction of the integrated sachswolfe isw effect with that of lambda mathrmcdm the linear isw eff... | [['the', 'recent', 'avera', 'cosmological', 'simulation', 'of', 'racz', 'et', 'al', '2017', 'has', 'a', 'lambda', 'mathrmcdmlike', 'expansion', 'history', 'and', 'removes', 'the', 'tension', 'between', 'local', 'and', 'planck', 'cosmic', 'microwave', 'background', 'hubble', 'constants', 'we', 'contrast', 'the', 'avera'... | [-0.07620580518166967, 0.07199376381907585, -0.11173251939555823, 0.09885290189593378, -0.11212911788547009, -0.06162157401768971, -0.04155989418516761, 0.3528933872147127, -0.22593653291933713, -0.334832149829005, 0.03748791612871951, -0.3297317564804299, -0.08784360396219705, 0.18914013050290152, 0.022445803240227234... |
1,801.08567 | Novel Two-Dimensional Silicon Dioxide with in-plane Negative Poisson's
Ratio | Silicon dioxide or silica, normally existing in various bulk crystalline and
amorphous forms, is recently found to possess a two-dimensional structure. In
this work, we use ab initio calculation and evolutionary algorithm to unveil
three new 2D silica structures whose themal, dynamical and mechanical
stabilities are ... | cond-mat.mtrl-sci cond-mat.mes-hall | silicon dioxide or silica normally existing in various bulk crystalline and amorphous forms is recently found to possess a twodimensional structure in this work we use ab initio calculation and evolutionary algorithm to unveil three new 2d silica structures whose themal dynamical and mechanical stabilities are compared... | [['silicon', 'dioxide', 'or', 'silica', 'normally', 'existing', 'in', 'various', 'bulk', 'crystalline', 'and', 'amorphous', 'forms', 'is', 'recently', 'found', 'to', 'possess', 'a', 'twodimensional', 'structure', 'in', 'this', 'work', 'we', 'use', 'ab', 'initio', 'calculation', 'and', 'evolutionary', 'algorithm', 'to',... | [-0.10568335745483637, 0.15001053560003388, -0.012819056498951145, -0.05294112851760084, -0.0401887449070013, -0.17425226666382515, -0.030847612454921805, 0.49335981000747, -0.24061326061575009, -0.3202809798398188, 0.04166451337930214, -0.3387781408349318, -0.19121592023709258, 0.14116159539303874, 0.05973237492144108... |
1,801.08568 | Resolving the Inner Arcsecond of the RY Tau Jet With HST | Faint X-ray emission from hot plasma (T > 1 MK) has been detected extending
outward a few arcseconds along the optically-delineated jets of some classical
T Tauri stars including RY Tau. The mechanism and location where the jet is
heated to X-ray temperatures is unknown. We present high spatial resolution HST
far-ult... | astro-ph.SR astro-ph.GA | faint xray emission from hot plasma t 1 mk has been detected extending outward a few arcseconds along the opticallydelineated jets of some classical t tauri stars including ry tau the mechanism and location where the jet is heated to xray temperatures is unknown we present high spatial resolution hst farultraviolet lon... | [['faint', 'xray', 'emission', 'from', 'hot', 'plasma', 't', '1', 'mk', 'has', 'been', 'detected', 'extending', 'outward', 'a', 'few', 'arcseconds', 'along', 'the', 'opticallydelineated', 'jets', 'of', 'some', 'classical', 't', 'tauri', 'stars', 'including', 'ry', 'tau', 'the', 'mechanism', 'and', 'location', 'where', ... | [-0.06704969752682098, 0.14058022472119835, -0.02829296862164253, 0.034440989905018385, -0.12447740442712914, -0.1365296920537477, 0.004142059522134719, 0.505807250284026, -0.2134354436320139, -0.3268972372435788, 0.04572899546228616, -0.31135336733285635, 0.12124120571084698, 0.1816103816777075, -0.012180756721527705,... |
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