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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1,803.02367 | Evidence for a Variable Ultrafast Outflow in the Newly Discovered
Ultraluminous Pulsar NGC 300 ULX-1 | Ultraluminous pulsars are a definite proof that persistent super-Eddington
accretion occurs in nature. They support the scenario according to which most
Ultraluminous X-ray Sources (ULXs) are super-Eddington accretors of stellar
mass rather than sub-Eddington intermediate mass black holes. An important
prediction of ... | astro-ph.HE | ultraluminous pulsars are a definite proof that persistent supereddington accretion occurs in nature they support the scenario according to which most ultraluminous xray sources ulxs are supereddington accretors of stellar mass rather than subeddington intermediate mass black holes an important prediction of theories o... | [['ultraluminous', 'pulsars', 'are', 'a', 'definite', 'proof', 'that', 'persistent', 'supereddington', 'accretion', 'occurs', 'in', 'nature', 'they', 'support', 'the', 'scenario', 'according', 'to', 'which', 'most', 'ultraluminous', 'xray', 'sources', 'ulxs', 'are', 'supereddington', 'accretors', 'of', 'stellar', 'mass... | [-0.0979496227544939, 0.09744415443586354, -0.07646517739762672, 0.11701034945097842, -0.12713599722501973, -0.10542591135374331, 0.03832169034848771, 0.45099179714992305, -0.14538864790923864, -0.3544908612440791, 0.12051912918761973, -0.30367029679097957, -0.0032257500204122473, 0.24227038002103538, -0.03704388148241... |
1,803.02368 | Likelihood for Detection of Sub-parsec Supermassive Black Hole Binaries
in Spectroscopic Surveys | Motivated by observational searches for sub-parsec supermassive black hole
binaries (SBHBs) we develop a modular analytic model to determine the
likelihood for detection of SBHBs by ongoing spectroscopic surveys. The model
combines the parametrized rate of orbital evolution of SBHBs in circumbinary
disks with the sel... | astro-ph.HE astro-ph.GA gr-qc | motivated by observational searches for subparsec supermassive black hole binaries sbhbs we develop a modular analytic model to determine the likelihood for detection of sbhbs by ongoing spectroscopic surveys the model combines the parametrized rate of orbital evolution of sbhbs in circumbinary disks with the selection... | [['motivated', 'by', 'observational', 'searches', 'for', 'subparsec', 'supermassive', 'black', 'hole', 'binaries', 'sbhbs', 'we', 'develop', 'a', 'modular', 'analytic', 'model', 'to', 'determine', 'the', 'likelihood', 'for', 'detection', 'of', 'sbhbs', 'by', 'ongoing', 'spectroscopic', 'surveys', 'the', 'model', 'combi... | [-0.12582379185615872, 0.13599228191274484, -0.05889818715646523, 0.107653791211445, -0.09815940571585631, -0.11812248016819667, 0.049189600893547486, 0.36397043868311957, -0.16317878330476135, -0.3662593120042934, 0.08954993544215978, -0.2985942590850332, -0.011381646902281096, 0.257482752701484, 0.013746023932143397,... |
1,803.02369 | Subsystem symmetry protected topological order | In this work, we introduce a new type of topological order which is protected
by subsystem symmetries which act on lower dimensional subsets of lattice
many-body system, e.g. along lines or planes in a three dimensional system. The
symmetry groups for such systems exhibit a macroscopic number of generators in
the inf... | cond-mat.str-el | in this work we introduce a new type of topological order which is protected by subsystem symmetries which act on lower dimensional subsets of lattice manybody system eg along lines or planes in a three dimensional system the symmetry groups for such systems exhibit a macroscopic number of generators in the infinite vo... | [['in', 'this', 'work', 'we', 'introduce', 'a', 'new', 'type', 'of', 'topological', 'order', 'which', 'is', 'protected', 'by', 'subsystem', 'symmetries', 'which', 'act', 'on', 'lower', 'dimensional', 'subsets', 'of', 'lattice', 'manybody', 'system', 'eg', 'along', 'lines', 'or', 'planes', 'in', 'a', 'three', 'dimension... | [-0.19507391725253678, 0.21149957149212523, -0.03448384402571876, 0.020990115121231043, -0.017981687031994414, -0.17013266058708715, 0.03832920610859178, 0.3248403768678357, -0.2592487786896527, -0.29770516018782345, 0.1251394503235229, -0.2964883787991633, -0.1476233405799822, 0.11426414650010604, -0.00641290074970601... |
1,803.0237 | On the need for soft dressing | In order to deal with IR divergences arising in QED or perturbative quantum
gravity scattering processes, one can either calculate inclusive quantities or
use dressed asymptotic states. We consider incoming superpositions of momentum
eigenstates and show that in calculations of cross-sections these two
approaches yie... | hep-th gr-qc quant-ph | in order to deal with ir divergences arising in qed or perturbative quantum gravity scattering processes one can either calculate inclusive quantities or use dressed asymptotic states we consider incoming superpositions of momentum eigenstates and show that in calculations of crosssections these two approaches yield di... | [['in', 'order', 'to', 'deal', 'with', 'ir', 'divergences', 'arising', 'in', 'qed', 'or', 'perturbative', 'quantum', 'gravity', 'scattering', 'processes', 'one', 'can', 'either', 'calculate', 'inclusive', 'quantities', 'or', 'use', 'dressed', 'asymptotic', 'states', 'we', 'consider', 'incoming', 'superpositions', 'of',... | [-0.132719362154603, 0.24857402808473644, -0.09217130532903996, 0.1658511903307434, -0.04416191283131151, -0.1217971122615771, 0.038032936844891604, 0.37136602335210356, -0.19384744199591555, -0.25880322549866314, -0.04231789244659012, -0.3284811909127581, -0.0751845893495816, 0.0963269023122848, -0.025171284106493528,... |
1,803.02371 | Merger types forming the Virgo cluster in recent gigayears | As our closest cluster-neighbor, the Virgo cluster of galaxies is intensely
studied by observers to unravel the mysteries of galaxy evolution within
clusters. At this stage, cosmological numerical simulations of the cluster are
useful to efficiently test theories and calibrate model. However, it is not
trivial to sel... | astro-ph.CO astro-ph.GA | as our closest clusterneighbor the virgo cluster of galaxies is intensely studied by observers to unravel the mysteries of galaxy evolution within clusters at this stage cosmological numerical simulations of the cluster are useful to efficiently test theories and calibrate model however it is not trivial to select the ... | [['as', 'our', 'closest', 'clusterneighbor', 'the', 'virgo', 'cluster', 'of', 'galaxies', 'is', 'intensely', 'studied', 'by', 'observers', 'to', 'unravel', 'the', 'mysteries', 'of', 'galaxy', 'evolution', 'within', 'clusters', 'at', 'this', 'stage', 'cosmological', 'numerical', 'simulations', 'of', 'the', 'cluster', 'a... | [-0.07141968004752196, 0.09068904812005858, -0.12307767526894114, 0.08655284573073349, -0.08775291372817962, -0.008577806167270526, 0.018636913929749824, 0.39932629482032067, -0.19771906114971508, -0.3426358517816793, 0.08829187433554853, -0.23901284176407614, -0.07826668792659158, 0.20134338909967456, 0.00777920922026... |
1,803.02372 | Soft evolution after a hard scattering process | The dynamical cascade of momentum, spin, charge, and other quantum numbers
from an ultra-violet process into the infra-red is a fundamental concern for
asymptotically free or conformal gauge field theories. It is also a practical
concern for any high energy scattering experiment with energies above tens of
GeV. We pr... | hep-ph hep-th | the dynamical cascade of momentum spin charge and other quantum numbers from an ultraviolet process into the infrared is a fundamental concern for asymptotically free or conformal gauge field theories it is also a practical concern for any high energy scattering experiment with energies above tens of gev we present a f... | [['the', 'dynamical', 'cascade', 'of', 'momentum', 'spin', 'charge', 'and', 'other', 'quantum', 'numbers', 'from', 'an', 'ultraviolet', 'process', 'into', 'the', 'infrared', 'is', 'a', 'fundamental', 'concern', 'for', 'asymptotically', 'free', 'or', 'conformal', 'gauge', 'field', 'theories', 'it', 'is', 'also', 'a', 'p... | [-0.10631788128557673, 0.2309743575279981, -0.10081031041409005, 0.11451409234840781, -0.0723159033450429, -0.09950690012328778, 0.01582221968055819, 0.3374252683215673, -0.2662468447433639, -0.29244117400594405, 0.04934547357242991, -0.2806277148047229, -0.10531292488030886, 0.11998598639729607, 0.04483459872687945, 0... |
1,803.02373 | The SLUGGS Survey: A comparison of total-mass profiles of early-type
galaxies from observations and cosmological simulations, to $\sim$4 effective
radii | We apply the Jeans Anisotropic MGE (JAM) dynamical modelling method to SAGES
Legacy Unifying Globulars and GalaxieS (SLUGGS) survey data of early-type
galaxies in the stellar mass range $10^{10}<M_*/{\rm M}_{\odot}<10^{11.6}$ that
cover a large radial range of $0.1-4.0$ effective radii. We combine SLUGGS and
ATLAS$^{... | astro-ph.GA | we apply the jeans anisotropic mge jam dynamical modelling method to sages legacy unifying globulars and galaxies sluggs survey data of earlytype galaxies in the stellar mass range 1010m_rm m_odot10116 that cover a large radial range of 0140 effective radii we combine sluggs and atlasrm 3d datasets to model the totalma... | [['we', 'apply', 'the', 'jeans', 'anisotropic', 'mge', 'jam', 'dynamical', 'modelling', 'method', 'to', 'sages', 'legacy', 'unifying', 'globulars', 'and', 'galaxies', 'sluggs', 'survey', 'data', 'of', 'earlytype', 'galaxies', 'in', 'the', 'stellar', 'mass', 'range', '1010m_rm', 'm_odot10116', 'that', 'cover', 'a', 'lar... | [-0.05468487246041624, 0.11785693529205503, -0.09676095845404631, 0.12974261415825805, -0.05322219071408304, -0.045977570120997444, -0.01115039561708004, 0.4288603072293485, -0.10308553358444418, -0.41080806793000263, -0.0019494386625667221, -0.2906688833052022, -0.004770277184434235, 0.21588444904748622, 0.00199137385... |
1,803.02374 | Identifying Mergers Using Quantitative Morphologies in Zoom Simulations
of High-Redshift Galaxies | Non-parametric morphology measures are a powerful tool for identifying galaxy
mergers at low redshifts. We employ cosmological zoom simulations using Gizmo
with the Mufasa feedback scheme, post-processed using 3D dust radiative
transfer into mock observations, to study whether common morphological measures
Gini G, M2... | astro-ph.GA | nonparametric morphology measures are a powerful tool for identifying galaxy mergers at low redshifts we employ cosmological zoom simulations using gizmo with the mufasa feedback scheme postprocessed using 3d dust radiative transfer into mock observations to study whether common morphological measures gini g m20 concen... | [['nonparametric', 'morphology', 'measures', 'are', 'a', 'powerful', 'tool', 'for', 'identifying', 'galaxy', 'mergers', 'at', 'low', 'redshifts', 'we', 'employ', 'cosmological', 'zoom', 'simulations', 'using', 'gizmo', 'with', 'the', 'mufasa', 'feedback', 'scheme', 'postprocessed', 'using', '3d', 'dust', 'radiative', '... | [-0.06675222422647774, 0.12340823470346479, -0.07752187094481017, 0.12628704057323586, -0.06073243325338878, -0.09288474328171176, -0.005881649785526231, 0.45746687437909156, -0.1225370101036298, -0.35022825681908915, 0.02507748454585313, -0.2880230425485374, -0.042651134522972055, 0.21109383488566472, 0.00492259859022... |
1,803.02375 | The Kormendy Relation of Galaxies in the Frontier Fields Clusters: Abell
S1063 and MACS J1149.5+2223 | We analyse the Kormendy relations (KRs) of the two Frontier Fields clusters,
Abell S1063, at z = 0.348, and MACS J1149.5+2223, at z = 0.542, exploiting very
deep Hubble Space Telescope photometry and VLT/MUSE integral field
spectroscopy. With this novel dataset, we are able to investigate how the KR
parameters depend... | astro-ph.GA | we analyse the kormendy relations krs of the two frontier fields clusters abell s1063 at z 0348 and macs j114952223 at z 0542 exploiting very deep hubble space telescope photometry and vltmuse integral field spectroscopy with this novel dataset we are able to investigate how the kr parameters depend on the cluster gala... | [['we', 'analyse', 'the', 'kormendy', 'relations', 'krs', 'of', 'the', 'two', 'frontier', 'fields', 'clusters', 'abell', 's1063', 'at', 'z', '0348', 'and', 'macs', 'j114952223', 'at', 'z', '0542', 'exploiting', 'very', 'deep', 'hubble', 'space', 'telescope', 'photometry', 'and', 'vltmuse', 'integral', 'field', 'spectro... | [-0.027068204428329103, 0.06290676539056572, -0.09328362658311855, 0.06954223552944594, -0.1066523161167159, -0.09308832065080384, 0.040807798871562655, 0.4366214179110118, -0.13465685098304098, -0.360260535631121, 0.0317591121949879, -0.3172333046370246, -0.04158193984442658, 0.19456481644079338, -0.02753697917696744,... |
1,803.02376 | Magnetic field strength of a neutron-star-powered ultraluminous X-ray
source | Ultraluminous X-ray sources (ULXs) are bright X-ray sources in nearby
galaxies not associated with the central supermassive black hole. Their
luminosities imply they are powered by either an extreme accretion rate onto a
compact stellar remnant, or an intermediate mass ($\sim100-10^5$ M$_{\odot}$)
black hole. The rec... | astro-ph.HE | ultraluminous xray sources ulxs are bright xray sources in nearby galaxies not associated with the central supermassive black hole their luminosities imply they are powered by either an extreme accretion rate onto a compact stellar remnant or an intermediate mass sim100105 m_odot black hole the recent detection of cohe... | [['ultraluminous', 'xray', 'sources', 'ulxs', 'are', 'bright', 'xray', 'sources', 'in', 'nearby', 'galaxies', 'not', 'associated', 'with', 'the', 'central', 'supermassive', 'black', 'hole', 'their', 'luminosities', 'imply', 'they', 'are', 'powered', 'by', 'either', 'an', 'extreme', 'accretion', 'rate', 'onto', 'a', 'co... | [-0.0986111053337889, 0.18364734572994698, -0.03021078759178134, 0.12732338184563058, -0.10441506215339078, -0.08710416447238772, 0.04506447026104634, 0.43074341052179704, -0.16461923899337777, -0.33328004972688086, 0.05049190883412315, -0.3214876796696977, 0.02925645879646442, 0.24316538686599132, -0.01204910304011969... |
1,803.02377 | The equivariant volumes of the permutahedron | We consider the action of the symmetric group $S_n$ on the permutahedron
$\Pi_n$. We prove that if $\sigma$ is a permutation of $S_n$ which has $m$
cycles of lengths $l_1, \ldots, l_m$, then the subpolytope of $\Pi_n$ fixed by
$\sigma$ has normalized volume $n^{m-2} \gcd(l_1, \ldots, l_m)$.
| math.CO | we consider the action of the symmetric group s_n on the permutahedron pi_n we prove that if sigma is a permutation of s_n which has m cycles of lengths l_1 ldots l_m then the subpolytope of pi_n fixed by sigma has normalized volume nm2 gcdl_1 ldots l_m | [['we', 'consider', 'the', 'action', 'of', 'the', 'symmetric', 'group', 's_n', 'on', 'the', 'permutahedron', 'pi_n', 'we', 'prove', 'that', 'if', 'sigma', 'is', 'a', 'permutation', 'of', 's_n', 'which', 'has', 'm', 'cycles', 'of', 'lengths', 'l_1', 'ldots', 'l_m', 'then', 'the', 'subpolytope', 'of', 'pi_n', 'fixed', 'b... | [-0.2419212843536946, 0.21944783769709908, -0.08952283466477758, -0.0042237039812354615, 0.009438679447276112, -0.12436975590358286, 0.004716428077739218, 0.364491060335675, -0.32641621419916983, -0.1427374602429589, 0.08543097814949958, -0.33997805157433386, -0.09085834018238213, 0.06837735830745457, -0.13441884961060... |
1,803.02378 | Linearized Flux Evolution (LiFE): A Technique for Rapidly Adapting
Fluxes from Full-Physics Radiative Transfer Models | Solar and thermal radiation are critical aspects of planetary climate, with
gradients in radiative energy fluxes driving heating and cooling. Climate
models require that radiative transfer tools be versatile, computationally
efficient, and accurate. Here, we describe a technique that uses an accurate
full-physics rad... | astro-ph.EP | solar and thermal radiation are critical aspects of planetary climate with gradients in radiative energy fluxes driving heating and cooling climate models require that radiative transfer tools be versatile computationally efficient and accurate here we describe a technique that uses an accurate fullphysics radiative tr... | [['solar', 'and', 'thermal', 'radiation', 'are', 'critical', 'aspects', 'of', 'planetary', 'climate', 'with', 'gradients', 'in', 'radiative', 'energy', 'fluxes', 'driving', 'heating', 'and', 'cooling', 'climate', 'models', 'require', 'that', 'radiative', 'transfer', 'tools', 'be', 'versatile', 'computationally', 'effic... | [0.011136075884882194, 0.18354381017790314, -0.042478805890918445, 0.11448353684370624, -0.06294291915223743, -0.08200204312402885, 0.03955160060420224, 0.40302067338975506, -0.28627498762969356, -0.37079753766481566, 0.09218210873335358, -0.250432222210501, -0.12432096744030344, 0.2065881024478513, -0.0165257870221964... |
1,803.02379 | Clues about the scarcity of stripped-envelope stars from the
evolutionary state of the sdO+Be binary system phi Persei | Stripped-envelope stars (SESs) form in binary systems after losing mass
through Roche-lobe overflow. They bear astrophysical significance as sources of
UV and ionizing radiation in older stellar populations and, if sufficiently
massive, as stripped supernova progenitors. Binary evolutionary models predict
them to be ... | astro-ph.SR | strippedenvelope stars sess form in binary systems after losing mass through rochelobe overflow they bear astrophysical significance as sources of uv and ionizing radiation in older stellar populations and if sufficiently massive as stripped supernova progenitors binary evolutionary models predict them to be common but... | [['strippedenvelope', 'stars', 'sess', 'form', 'in', 'binary', 'systems', 'after', 'losing', 'mass', 'through', 'rochelobe', 'overflow', 'they', 'bear', 'astrophysical', 'significance', 'as', 'sources', 'of', 'uv', 'and', 'ionizing', 'radiation', 'in', 'older', 'stellar', 'populations', 'and', 'if', 'sufficiently', 'ma... | [-0.063861868038417, 0.15288697030711665, -0.0697878961214679, 0.12048522409408202, -0.11600558363091779, -0.10250111969753412, 0.10649018477119825, 0.3970890329480663, -0.14824004337520463, -0.36021298459629614, 0.09296415911729236, -0.2848223583738584, -0.03382614338324826, 0.1960502187415985, -0.08071891245126368, -... |
1,803.0238 | Fast Cylinder and Plane Extraction from Depth Cameras for Visual
Odometry | This paper presents CAPE, a method to extract planes and cylinder segments
from organized point clouds, which processes 640x480 depth images on a single
CPU core at an average of 300 Hz, by operating on a grid of planar cells.
While, compared to state-of-the-art plane extraction, the latency of CAPE is
more consisten... | cs.CV cs.RO | this paper presents cape a method to extract planes and cylinder segments from organized point clouds which processes 640x480 depth images on a single cpu core at an average of 300 hz by operating on a grid of planar cells while compared to stateoftheart plane extraction the latency of cape is more consistent and 410 t... | [['this', 'paper', 'presents', 'cape', 'a', 'method', 'to', 'extract', 'planes', 'and', 'cylinder', 'segments', 'from', 'organized', 'point', 'clouds', 'which', 'processes', '640x480', 'depth', 'images', 'on', 'a', 'single', 'cpu', 'core', 'at', 'an', 'average', 'of', '300', 'hz', 'by', 'operating', 'on', 'a', 'grid', ... | [-0.1051753329571026, 0.027055469525609322, -0.0719889287557453, -0.0012098286091350018, -0.07927840038513144, -0.11975661526899785, 0.06474314314701284, 0.451986389371256, -0.23412158963580926, -0.3251135443150997, 0.10705160568390662, -0.28744522848476967, -0.10858491473598406, 0.23604009031201711, -0.183529008089875... |
1,803.02381 | Evolution of the Stellar Mass Function in Multiple-Population Globular
Clusters | We present the results of a survey of N-body simulations aimed at studying
the effects of the long-term dynamical evolution on the stellar mass function
(MF) of multiple stellar populations in globular clusters. Our simulations show
that if first-(1G) and second-generation (2G) stars have the same initial MF
(IMF), t... | astro-ph.GA | we present the results of a survey of nbody simulations aimed at studying the effects of the longterm dynamical evolution on the stellar mass function mf of multiple stellar populations in globular clusters our simulations show that if first1g and secondgeneration 2g stars have the same initial mf imf the global mfs of... | [['we', 'present', 'the', 'results', 'of', 'a', 'survey', 'of', 'nbody', 'simulations', 'aimed', 'at', 'studying', 'the', 'effects', 'of', 'the', 'longterm', 'dynamical', 'evolution', 'on', 'the', 'stellar', 'mass', 'function', 'mf', 'of', 'multiple', 'stellar', 'populations', 'in', 'globular', 'clusters', 'our', 'simu... | [-0.14832277299348176, 0.18833796458363714, -0.11672428298936072, 0.16555774323463568, 0.018981772833073653, -0.024443632202133178, 0.03356246221679671, 0.3633220572338765, -0.24581539113239112, -0.3775872074882967, 0.03320545720471346, -0.26011393907859576, -0.1112053988091872, 0.16129146796982197, 0.02038216942838995... |
1,803.02382 | Quantum oscillations and criticality in a fermionic and bosonic dimer
model for the cuprates | We study quantum oscillations for a system of fermionic and bosonic dimers
and compare the results to those experimentally observed in the cuprate
superconductors in their underdoped regime. Based on gauge invariance, we argue
that the charge carriers obey the Onsager quantization condition and quantum
oscillations t... | cond-mat.str-el | we study quantum oscillations for a system of fermionic and bosonic dimers and compare the results to those experimentally observed in the cuprate superconductors in their underdoped regime based on gauge invariance we argue that the charge carriers obey the onsager quantization condition and quantum oscillations take ... | [['we', 'study', 'quantum', 'oscillations', 'for', 'a', 'system', 'of', 'fermionic', 'and', 'bosonic', 'dimers', 'and', 'compare', 'the', 'results', 'to', 'those', 'experimentally', 'observed', 'in', 'the', 'cuprate', 'superconductors', 'in', 'their', 'underdoped', 'regime', 'based', 'on', 'gauge', 'invariance', 'we', ... | [-0.1870627474104128, 0.16935951710605113, -0.09592504967440618, 0.09844047444609091, -0.036639948672688515, -0.19305003160843626, 0.1312629012015685, 0.30278274952434003, -0.2085560290510521, -0.21820935839787126, -0.0440042579070187, -0.39323234868597384, -0.15606064845709816, 0.16665404656822302, 0.01454065974777270... |
1,803.02383 | Constraining Density Fluctuations with Big Bang Nucleosynthesis in the
Era of Precision Cosmology | We reexamine big bang nucleosynthesis with large-scale baryon density
inhomogeneities when the length scale of the density fluctuations exceeds the
neutron diffusion length ($\sim 10^7-10^8$ cm at BBN), and the amplitude of the
fluctuations is sufficiently small to prevent gravitational collapse. In this
limit, the f... | astro-ph.CO gr-qc hep-ph | we reexamine big bang nucleosynthesis with largescale baryon density inhomogeneities when the length scale of the density fluctuations exceeds the neutron diffusion length sim 107108 cm at bbn and the amplitude of the fluctuations is sufficiently small to prevent gravitational collapse in this limit the final light ele... | [['we', 'reexamine', 'big', 'bang', 'nucleosynthesis', 'with', 'largescale', 'baryon', 'density', 'inhomogeneities', 'when', 'the', 'length', 'scale', 'of', 'the', 'density', 'fluctuations', 'exceeds', 'the', 'neutron', 'diffusion', 'length', 'sim', '107108', 'cm', 'at', 'bbn', 'and', 'the', 'amplitude', 'of', 'the', '... | [-0.07667661700343266, 0.24467273112059684, -0.07883280261480304, 0.11571350420160731, 0.01573076496807564, -0.03286117099753815, 0.05346180779086045, 0.28083721070403334, -0.21625361847418922, -0.33368649626183405, 0.02679964878980332, -0.31723256373869213, 0.009855841584667041, 0.17158936794264493, -0.007112132269638... |
1,803.02384 | Fractional uncertainty | We use techniques of dyadic analysis in order to prove that, for every
$0<s<\tfrac{1}{2}$, there exists a positive constant $\gamma(s)$ such that the
inequality $$\left(\iint_{\mathbb{R}^2}|x-y|^{2s-1}|\varphi(x)||\varphi(y)|dx
dy\right)\left(\iint_{\mathbb{R}^2}|x-y|^{-2s-1}|\varphi(x)-\varphi(y)|^2 dx
dy\right)\geq... | math.FA | we use techniques of dyadic analysis in order to prove that for every 0stfrac12 there exists a positive constant gammas such that the inequality leftiint_mathbbr2xy2s1varphixvarphiydx dyrightleftiint_mathbbr2xy2s1varphixvarphiy2 dx dyrightgeq gammas holds for every varphi with varphi_l2mathbbr1 the second integral on t... | [['we', 'use', 'techniques', 'of', 'dyadic', 'analysis', 'in', 'order', 'to', 'prove', 'that', 'for', 'every', '0stfrac12', 'there', 'exists', 'a', 'positive', 'constant', 'gammas', 'such', 'that', 'the', 'inequality', 'leftiint_mathbbr2xy2s1varphixvarphiydx', 'dyrightleftiint_mathbbr2xy2s1varphixvarphiy2', 'dx', 'dyri... | [-0.16044613395970833, 0.07441574651040608, -0.08185315558309608, 0.04776877345505489, -0.042438325755109516, -0.11983633379723076, 0.016315439692403698, 0.3048696337220601, -0.2894882070890899, -0.1906146717646831, 0.09138049526564494, -0.33886550116953973, -0.10978723422600593, 0.2191287616674517, -0.0109372386956422... |
1,803.02385 | Packing Plane Spanning Trees into a Point Set | Let $P$ be a set of $n$ points in the plane in general position. We show that
at least $\lfloor n/3\rfloor$ plane spanning trees can be packed into the
complete geometric graph on $P$. This improves the previous best known lower
bound $\Omega\left(\sqrt{n}\right)$. Towards our proof of this lower bound we
show that t... | cs.CG cs.DM | let p be a set of n points in the plane in general position we show that at least lfloor n3rfloor plane spanning trees can be packed into the complete geometric graph on p this improves the previous best known lower bound omegaleftsqrtnright towards our proof of this lower bound we show that the center of a set of poin... | [['let', 'p', 'be', 'a', 'set', 'of', 'n', 'points', 'in', 'the', 'plane', 'in', 'general', 'position', 'we', 'show', 'that', 'at', 'least', 'lfloor', 'n3rfloor', 'plane', 'spanning', 'trees', 'can', 'be', 'packed', 'into', 'the', 'complete', 'geometric', 'graph', 'on', 'p', 'this', 'improves', 'the', 'previous', 'best... | [-0.1694474800885336, 0.11817855278208647, -0.08386511735981712, -0.009601375810508553, -0.054297804277492305, -0.1126122993021591, 0.10336023464492738, 0.3141867782831294, -0.24663038388507008, -0.2922181567713006, 0.058274365291764885, -0.2985038348945649, -0.10797131677119903, 0.1850216561156542, -0.0827464261147313... |
1,803.02386 | Study of a chemo-repulsion model with quadratic production. Part I:
Analysis of the continuous problem and time-discrete numerical schemes | We consider a chemo-repulsion model with quadratic production in a bounded
domain. Firstly, we obtain global in time weak solutions, and give a regularity
criterion (which is satisfied for $1D$ and $2D$ domains) to deduce uniqueness
and global regularity. After, we study two cell-conservative and
unconditionally ener... | math.NA cs.NA | we consider a chemorepulsion model with quadratic production in a bounded domain firstly we obtain global in time weak solutions and give a regularity criterion which is satisfied for 1d and 2d domains to deduce uniqueness and global regularity after we study two cellconservative and unconditionally energystable firsto... | [['we', 'consider', 'a', 'chemorepulsion', 'model', 'with', 'quadratic', 'production', 'in', 'a', 'bounded', 'domain', 'firstly', 'we', 'obtain', 'global', 'in', 'time', 'weak', 'solutions', 'and', 'give', 'a', 'regularity', 'criterion', 'which', 'is', 'satisfied', 'for', '1d', 'and', '2d', 'domains', 'to', 'deduce', '... | [-0.1648418536461476, 0.012881120004587703, -0.08066677053963454, 0.08290141129486815, -0.0392544506152195, -0.17662437918975396, 0.02063848241749737, 0.34619262550302127, -0.32301506849902645, -0.21790784706266736, 0.16316711235774198, -0.2253368185608889, -0.10514339268966405, 0.17368999590096926, -0.0485728288219871... |
1,803.02387 | Lower bounds for Waldschmidt constants of generic lines in
$\mathbb{P}^3$ and a Chudnovsky-type theorem | The Waldschmidt constant $\alphahat(I)$ of a radical ideal $I$ in the
coordinate ring of $\PP^N$ measures (asymptotically) the degree of a
hypersurface passing through the set defined by $I$ in $\PP^N$. Nagata's
approach to the 14th Hilbert Problem was based on computing such constant for
the set of points in $\PP^2$... | math.AG math.AC | the waldschmidt constant alphahati of a radical ideal i in the coordinate ring of ppn measures asymptotically the degree of a hypersurface passing through the set defined by i in ppn nagatas approach to the 14th hilbert problem was based on computing such constant for the set of points in pp2 since then these constants... | [['the', 'waldschmidt', 'constant', 'alphahati', 'of', 'a', 'radical', 'ideal', 'i', 'in', 'the', 'coordinate', 'ring', 'of', 'ppn', 'measures', 'asymptotically', 'the', 'degree', 'of', 'a', 'hypersurface', 'passing', 'through', 'the', 'set', 'defined', 'by', 'i', 'in', 'ppn', 'nagatas', 'approach', 'to', 'the', '14th'... | [-0.14790608590517781, 0.08054453870183927, -0.028150780956677505, 0.08057017883249118, -0.05411174676479086, -0.21878466649152534, 0.04582818205495929, 0.3303942549973726, -0.2069409047406608, -0.2647737407395126, 0.10624251741912878, -0.2609081086304382, -0.10029906380958364, 0.251704984994017, -0.06327948477548107, ... |
1,803.02388 | Learning SMaLL Predictors | We present a new machine learning technique for training small
resource-constrained predictors. Our algorithm, the Sparse Multiprototype
Linear Learner (SMaLL), is inspired by the classic machine learning problem of
learning $k$-DNF Boolean formulae. We present a formal derivation of our
algorithm and demonstrate the... | cs.LG | we present a new machine learning technique for training small resourceconstrained predictors our algorithm the sparse multiprototype linear learner small is inspired by the classic machine learning problem of learning kdnf boolean formulae we present a formal derivation of our algorithm and demonstrate the benefits of... | [['we', 'present', 'a', 'new', 'machine', 'learning', 'technique', 'for', 'training', 'small', 'resourceconstrained', 'predictors', 'our', 'algorithm', 'the', 'sparse', 'multiprototype', 'linear', 'learner', 'small', 'is', 'inspired', 'by', 'the', 'classic', 'machine', 'learning', 'problem', 'of', 'learning', 'kdnf', '... | [-0.027042657883732387, -0.04436050776877102, -0.09472958234859244, 0.05826996640469176, -0.17053359540460525, -0.19073966492564892, 0.10332496922665257, 0.3811132187058903, -0.2906405943322857, -0.30905355850480637, 0.03866176312473023, -0.19599991390165292, -0.27526587764468957, 0.22508444426194676, -0.14196801468519... |
1,803.02389 | Unconventional multi-band superconductivity in bulk SrTiO$_{3}$ and
LaAlO$_{3}$/SrTiO$_{3}$ interfaces | Although discovered many decades ago, superconductivity in doped SrTiO$_{3}$
remains a topic of intense research. Recent experiments revealed that, upon
increasing the carrier concentration, multiple bands cross the Fermi level,
signaling the onset of Lifshitz transitions. Interestingly, $T_{c}$ was
observed to be su... | cond-mat.supr-con | although discovered many decades ago superconductivity in doped srtio_3 remains a topic of intense research recent experiments revealed that upon increasing the carrier concentration multiple bands cross the fermi level signaling the onset of lifshitz transitions interestingly t_c was observed to be suppressed across t... | [['although', 'discovered', 'many', 'decades', 'ago', 'superconductivity', 'in', 'doped', 'srtio_3', 'remains', 'a', 'topic', 'of', 'intense', 'research', 'recent', 'experiments', 'revealed', 'that', 'upon', 'increasing', 'the', 'carrier', 'concentration', 'multiple', 'bands', 'cross', 'the', 'fermi', 'level', 'signali... | [-0.17490713978776526, 0.24515881882341, -0.061010962335760116, 0.09436172483124915, -0.05161452906626001, -0.19549768361669612, 0.1330810884178967, 0.3757138686372676, -0.24965646502260172, -0.2760637661599567, -0.04282059258630525, -0.36372312314441085, -0.17012880208679068, 0.1311901368817288, 0.012114502063257173, ... |
1,803.0239 | Lecture Notes on Noncommutative Lp-Spaces | These lecture notes were written during a mini-course on noncommutative
Lp-spaces at the Basque Center of Applied Mathematics. It starts presenting the
theory of weights and traces in von Neumann algebra, followed by the theory of
noncommutative measure. After that, it presents a construction of these spaces
in all d... | math.OA math.FA | these lecture notes were written during a minicourse on noncommutative lpspaces at the basque center of applied mathematics it starts presenting the theory of weights and traces in von neumann algebra followed by the theory of noncommutative measure after that it presents a construction of these spaces in all detail an... | [['these', 'lecture', 'notes', 'were', 'written', 'during', 'a', 'minicourse', 'on', 'noncommutative', 'lpspaces', 'at', 'the', 'basque', 'center', 'of', 'applied', 'mathematics', 'it', 'starts', 'presenting', 'the', 'theory', 'of', 'weights', 'and', 'traces', 'in', 'von', 'neumann', 'algebra', 'followed', 'by', 'the',... | [-0.05490117499915262, 0.12300552108790726, -0.13585304516212393, 0.08922660280950367, -0.04305282908026129, -0.1301574818363103, -0.03204907134252911, 0.3200353466866848, -0.27592672038202487, -0.23817678003882367, 0.1889175320471016, -0.26726115072766937, -0.1527906091262897, 0.2132535638908545, -0.18167826163892944,... |
1,803.02391 | Study of a chemo-repulsion model with quadratic production. Part II:
Analysis of an unconditional energy-stable fully discrete scheme | This work is devoted to the study of a fully discrete scheme for a repulsive
chemotaxis with quadratic production model. By following the ideas presented in
[Guilen-Gonzalez et al], we introduce an auxiliary variable (the gradient of
the chemical concentration), and prove that the corresponding Finite Element
(FE) ba... | math.NA cs.NA | this work is devoted to the study of a fully discrete scheme for a repulsive chemotaxis with quadratic production model by following the ideas presented in guilengonzalez et al we introduce an auxiliary variable the gradient of the chemical concentration and prove that the corresponding finite element fe backward euler... | [['this', 'work', 'is', 'devoted', 'to', 'the', 'study', 'of', 'a', 'fully', 'discrete', 'scheme', 'for', 'a', 'repulsive', 'chemotaxis', 'with', 'quadratic', 'production', 'model', 'by', 'following', 'the', 'ideas', 'presented', 'in', 'guilengonzalez', 'et', 'al', 'we', 'introduce', 'an', 'auxiliary', 'variable', 'the... | [-0.08945039740763605, -0.013370098209707066, -0.11728400395065545, 0.05536908739525825, -0.07747601566091179, -0.16890158389136195, 0.05274143387377262, 0.38475748144090177, -0.29051127075776456, -0.24418704251060264, 0.11343683634884655, -0.26205110740475357, -0.1580943765975535, 0.22701019988767804, -0.0831851468094... |
1,803.02392 | Multimodal Emoji Prediction | Emojis are small images that are commonly included in social media text
messages. The combination of visual and textual content in the same message
builds up a modern way of communication, that automatic systems are not used to
deal with. In this paper we extend recent advances in emoji prediction by
putting forward ... | cs.CL | emojis are small images that are commonly included in social media text messages the combination of visual and textual content in the same message builds up a modern way of communication that automatic systems are not used to deal with in this paper we extend recent advances in emoji prediction by putting forward a mul... | [['emojis', 'are', 'small', 'images', 'that', 'are', 'commonly', 'included', 'in', 'social', 'media', 'text', 'messages', 'the', 'combination', 'of', 'visual', 'and', 'textual', 'content', 'in', 'the', 'same', 'message', 'builds', 'up', 'a', 'modern', 'way', 'of', 'communication', 'that', 'automatic', 'systems', 'are',... | [-0.059579927351608476, 0.04050624054185131, -0.07847789071092848, 0.08306914674051638, -0.1512790200832699, -0.14901232663209418, 0.0289624946499576, 0.4652804306841322, -0.26869174085025277, -0.32063745414572103, 0.03949170791560651, -0.3858503895146506, -0.18928367142964686, 0.18066878470292846, -0.13237260105420967... |
1,803.02393 | Game Theoretic Analysis of Road User Safety Scenarios Involving
Autonomous Vehicles | Interactions between pedestrians, bikers, and human-driven vehicles have been
a major concern in traffic safety over the years. The upcoming age of
autonomous vehicles will further raise major problems on whether self-driving
cars can accurately avoid accidents; on the other hand, usability issues arise
on whether hu... | cs.GT cs.LO | interactions between pedestrians bikers and humandriven vehicles have been a major concern in traffic safety over the years the upcoming age of autonomous vehicles will further raise major problems on whether selfdriving cars can accurately avoid accidents on the other hand usability issues arise on whether humandriven... | [['interactions', 'between', 'pedestrians', 'bikers', 'and', 'humandriven', 'vehicles', 'have', 'been', 'a', 'major', 'concern', 'in', 'traffic', 'safety', 'over', 'the', 'years', 'the', 'upcoming', 'age', 'of', 'autonomous', 'vehicles', 'will', 'further', 'raise', 'major', 'problems', 'on', 'whether', 'selfdriving', '... | [-0.19137324085516602, 0.1002745974800308, -0.091718019456617, 0.07560365528461487, -0.09607904295172588, -0.17277988548861978, 0.08921165429817421, 0.3800540930465048, -0.2244173723214053, -0.33499769845770466, 0.13434513304224469, -0.2937259113209115, -0.16267036358728132, 0.21003865090308044, -0.20918790019335753, 0... |
1,803.02394 | Impact of disorder on the superconducting transition temperature near a
Lifshitz transition | Multi-band superconductivity is realized in a plethora of systems, from
high-temperature superconductors to very diluted superconductors. While several
properties of multi-band superconductors can be understood as straightforward
generalizations of their single-band counterparts, recent works have unveiled
rather unu... | cond-mat.supr-con | multiband superconductivity is realized in a plethora of systems from hightemperature superconductors to very diluted superconductors while several properties of multiband superconductors can be understood as straightforward generalizations of their singleband counterparts recent works have unveiled rather unusual beha... | [['multiband', 'superconductivity', 'is', 'realized', 'in', 'a', 'plethora', 'of', 'systems', 'from', 'hightemperature', 'superconductors', 'to', 'very', 'diluted', 'superconductors', 'while', 'several', 'properties', 'of', 'multiband', 'superconductors', 'can', 'be', 'understood', 'as', 'straightforward', 'generalizat... | [-0.182441117009148, 0.2022869439495742, -0.06375561990133752, 0.10921370944801849, -0.0718046608181663, -0.19527735249846015, 0.12424657659166663, 0.3557170539703003, -0.22244537502716583, -0.23917980310380285, -0.012014348079597193, -0.3474800716614503, -0.15668646449038345, 0.16180878908782, 0.018696912185138123, -0... |
1,803.02395 | Arbitrary Discrete Sequence Anomaly Detection with Zero Boundary LSTM | We propose a simple mathematical definition and new neural architecture for
finding anomalies within discrete sequence datasets. Our model comprises of a
modified LSTM autoencoder and an array of One-Class SVMs. The LSTM takes in
elements from a sequence and creates context vectors that are used to predict
the probab... | cs.LG | we propose a simple mathematical definition and new neural architecture for finding anomalies within discrete sequence datasets our model comprises of a modified lstm autoencoder and an array of oneclass svms the lstm takes in elements from a sequence and creates context vectors that are used to predict the probability... | [['we', 'propose', 'a', 'simple', 'mathematical', 'definition', 'and', 'new', 'neural', 'architecture', 'for', 'finding', 'anomalies', 'within', 'discrete', 'sequence', 'datasets', 'our', 'model', 'comprises', 'of', 'a', 'modified', 'lstm', 'autoencoder', 'and', 'an', 'array', 'of', 'oneclass', 'svms', 'the', 'lstm', '... | [-0.06191442535570778, 0.03568623814371853, -0.07729263605439167, 0.07615633617331573, -0.10202942792217708, -0.17616382114322476, 0.016908368975086845, 0.46150371771378135, -0.2951483123176234, -0.2696438506516872, 0.07237587361234846, -0.2702044020316482, -0.205958639904495, 0.18567788650426398, -0.10205248418463014,... |
1,803.02396 | A toy model for time evolving QFT on a lattice with controllable chaos | A class of models with a dynamics of generalized quantum cat maps on a
product of quantum tori is described. These tori are defined by an algebra of
clock-shift matrices of dimension $N$. The dynamics is such that the Lyapunov
exponents can be computed analytically at large $N$. Some of these systems can
be thought o... | hep-th quant-ph | a class of models with a dynamics of generalized quantum cat maps on a product of quantum tori is described these tori are defined by an algebra of clockshift matrices of dimension n the dynamics is such that the lyapunov exponents can be computed analytically at large n some of these systems can be thought of as a toy... | [['a', 'class', 'of', 'models', 'with', 'a', 'dynamics', 'of', 'generalized', 'quantum', 'cat', 'maps', 'on', 'a', 'product', 'of', 'quantum', 'tori', 'is', 'described', 'these', 'tori', 'are', 'defined', 'by', 'an', 'algebra', 'of', 'clockshift', 'matrices', 'of', 'dimension', 'n', 'the', 'dynamics', 'is', 'such', 'th... | [-0.17176653529582084, 0.19900764060736853, -0.0756375974574596, 0.052776048162145185, 0.03523720097994022, -0.19811644622502078, 0.03439794676900231, 0.35408576850574625, -0.28279516664494214, -0.245414783594054, 0.12092771801840642, -0.2639111268609072, -0.13755101023807897, 0.22709500364826768, -0.01914430562728426,... |
1,803.02397 | Markov chain Monte Carlo population synthesis of single radio pulsars in
the Galaxy | We present a model of evolution of solitary neutron stars, including spin
parameters, magnetic field decay, motion in the Galactic potential and birth
inside spiral arms. We use two parametrizations of the radio-luminosity law and
model the radio selection effects. Dispersion measure is estimated from the
recent mode... | astro-ph.IM astro-ph.HE | we present a model of evolution of solitary neutron stars including spin parameters magnetic field decay motion in the galactic potential and birth inside spiral arms we use two parametrizations of the radioluminosity law and model the radio selection effects dispersion measure is estimated from the recent model of fre... | [['we', 'present', 'a', 'model', 'of', 'evolution', 'of', 'solitary', 'neutron', 'stars', 'including', 'spin', 'parameters', 'magnetic', 'field', 'decay', 'motion', 'in', 'the', 'galactic', 'potential', 'and', 'birth', 'inside', 'spiral', 'arms', 'we', 'use', 'two', 'parametrizations', 'of', 'the', 'radioluminosity', '... | [-0.08125999591180257, 0.14166661929422325, -0.04130234728800133, 0.1149628111759999, -0.10361775158505354, -0.09703650394554383, 0.03716456225374713, 0.4265353593310075, -0.21288147481058592, -0.37024507556177144, 0.06785517980377855, -0.29218549566077334, -0.04005815422694598, 0.22076009022005436, 0.06935493074540448... |
1,803.02398 | Visualizing Convolutional Neural Network Protein-Ligand Scoring | Protein-ligand scoring is an important step in a structure-based drug design
pipeline. Selecting a correct binding pose and predicting the binding affinity
of a protein-ligand complex enables effective virtual screening. Machine
learning techniques can make use of the increasing amounts of structural data
that are be... | stat.ML cs.LG q-bio.BM | proteinligand scoring is an important step in a structurebased drug design pipeline selecting a correct binding pose and predicting the binding affinity of a proteinligand complex enables effective virtual screening machine learning techniques can make use of the increasing amounts of structural data that are becoming ... | [['proteinligand', 'scoring', 'is', 'an', 'important', 'step', 'in', 'a', 'structurebased', 'drug', 'design', 'pipeline', 'selecting', 'a', 'correct', 'binding', 'pose', 'and', 'predicting', 'the', 'binding', 'affinity', 'of', 'a', 'proteinligand', 'complex', 'enables', 'effective', 'virtual', 'screening', 'machine', '... | [-0.03799775787629187, 0.033253458428530835, -0.04819254618168117, 0.13757369375652484, -0.1234403763356949, -0.22107429482463387, 0.00899097503373219, 0.5229373199805136, -0.27065689885808575, -0.31153683173319985, 0.006180283395693668, -0.2506153127328763, -0.2919444846830541, 0.17756555107452215, -0.0949236528662544... |
1,803.02399 | Multi-Dimensional Item Response Theory and the Force Concept Inventory | Research on the test structure of the Force Concept Inventory (FCI) has
largely been performed with exploratory methods such as factor analysis and
cluster analysis. Multi-Dimensional Item Response Theory (MIRT) provides an
alternative to traditional Exploratory Factor Analysis which allows statistical
testing to ide... | physics.ed-ph | research on the test structure of the force concept inventory fci has largely been performed with exploratory methods such as factor analysis and cluster analysis multidimensional item response theory mirt provides an alternative to traditional exploratory factor analysis which allows statistical testing to identify th... | [['research', 'on', 'the', 'test', 'structure', 'of', 'the', 'force', 'concept', 'inventory', 'fci', 'has', 'largely', 'been', 'performed', 'with', 'exploratory', 'methods', 'such', 'as', 'factor', 'analysis', 'and', 'cluster', 'analysis', 'multidimensional', 'item', 'response', 'theory', 'mirt', 'provides', 'an', 'alt... | [-0.03854521037448323, 0.019483034950169252, -0.10833269016871201, 0.07132613650806573, -0.09460651904686494, -0.11735077368563428, 0.11633072011026549, 0.3239656988945272, -0.2602547135728227, -0.36020373089091656, 0.08036261610751806, -0.2776165284759254, -0.13891046802661772, 0.16125103502291377, -0.0229069935405347... |
1,803.024 | Natural Language to Structured Query Generation via Meta-Learning | In conventional supervised training, a model is trained to fit all the
training examples. However, having a monolithic model may not always be the
best strategy, as examples could vary widely. In this work, we explore a
different learning protocol that treats each example as a unique pseudo-task,
by reducing the orig... | cs.CL cs.LG | in conventional supervised training a model is trained to fit all the training examples however having a monolithic model may not always be the best strategy as examples could vary widely in this work we explore a different learning protocol that treats each example as a unique pseudotask by reducing the original learn... | [['in', 'conventional', 'supervised', 'training', 'a', 'model', 'is', 'trained', 'to', 'fit', 'all', 'the', 'training', 'examples', 'however', 'having', 'a', 'monolithic', 'model', 'may', 'not', 'always', 'be', 'the', 'best', 'strategy', 'as', 'examples', 'could', 'vary', 'widely', 'in', 'this', 'work', 'we', 'explore'... | [-0.017261872184462845, -0.0063692094990983605, -0.07161650827831843, 0.0679234631348994, -0.11639260600680824, -0.20293110036502846, 0.06848756928361995, 0.4322512708604336, -0.2401951223622415, -0.3505239203699272, 0.06704208178284303, -0.2520715564447032, -0.15416402105157348, 0.22622866769300096, -0.140745991946790... |
1,803.02401 | Low-noise heralded single photons from cascaded downconversion | Heralded single photon sources are often implemented using spontaneous
parametric downconversion, but their quality can be restricted by optical loss,
double pair emission and detector dark counts. Here, we show that the
performance of such sources can be improved using cascaded downconversion, by
providing a second ... | quant-ph | heralded single photon sources are often implemented using spontaneous parametric downconversion but their quality can be restricted by optical loss double pair emission and detector dark counts here we show that the performance of such sources can be improved using cascaded downconversion by providing a second trigger... | [['heralded', 'single', 'photon', 'sources', 'are', 'often', 'implemented', 'using', 'spontaneous', 'parametric', 'downconversion', 'but', 'their', 'quality', 'can', 'be', 'restricted', 'by', 'optical', 'loss', 'double', 'pair', 'emission', 'and', 'detector', 'dark', 'counts', 'here', 'we', 'show', 'that', 'the', 'perf... | [-0.09152398401320996, 0.17820218755525385, -0.016149079363623805, 0.06520897865641129, -0.0374132180039658, -0.1918225957038389, 0.0479040554774022, 0.4521274165934742, -0.20491948173289667, -0.3280270942063494, 0.05877497281339443, -0.2809415930656321, -0.03071563567430007, 0.2730594928919648, -0.028824788744025158, ... |
1,803.02402 | Self-reporting and screening: Data with current-status and censored
observations | We consider survival data that combine three types of observations:
uncensored, right-censored, and left-censored. Such data arises from screening
a medical condition, in situations where self-detection arises naturally. Our
goal is to estimate the failure-time distribution, based on these three
observation types. We... | math.ST stat.AP stat.TH | we consider survival data that combine three types of observations uncensored rightcensored and leftcensored such data arises from screening a medical condition in situations where selfdetection arises naturally our goal is to estimate the failuretime distribution based on these three observation types we propose a nov... | [['we', 'consider', 'survival', 'data', 'that', 'combine', 'three', 'types', 'of', 'observations', 'uncensored', 'rightcensored', 'and', 'leftcensored', 'such', 'data', 'arises', 'from', 'screening', 'a', 'medical', 'condition', 'in', 'situations', 'where', 'selfdetection', 'arises', 'naturally', 'our', 'goal', 'is', '... | [-0.06327511719154084, 0.0752149948008831, -0.10710233628256795, 0.09839976131710608, -0.07368001909652615, -0.17705031982075203, 0.07831733431119253, 0.4074490468250588, -0.22331087607890368, -0.32710569250972615, 0.17720945918699726, -0.3082817249438342, -0.11707146591164501, 0.19846177125240075, -0.12310509113320971... |
1,803.02403 | Trifo-VIO: Robust and Efficient Stereo Visual Inertial Odometry using
Points and Lines | In this paper, we present the Trifo Visual Inertial Odometry (Trifo-VIO), a
tightly-coupled filtering-based stereo VIO system using both points and lines.
Line features help improve system robustness in challenging scenarios when
point features cannot be reliably detected or tracked, e.g. low-texture
environment or l... | cs.CV | in this paper we present the trifo visual inertial odometry trifovio a tightlycoupled filteringbased stereo vio system using both points and lines line features help improve system robustness in challenging scenarios when point features cannot be reliably detected or tracked eg lowtexture environment or lighting change... | [['in', 'this', 'paper', 'we', 'present', 'the', 'trifo', 'visual', 'inertial', 'odometry', 'trifovio', 'a', 'tightlycoupled', 'filteringbased', 'stereo', 'vio', 'system', 'using', 'both', 'points', 'and', 'lines', 'line', 'features', 'help', 'improve', 'system', 'robustness', 'in', 'challenging', 'scenarios', 'when', ... | [-0.1049673390562499, -0.004096426435832032, -0.05699086648727596, -0.0030143918181573482, -0.10612234640652068, -0.19974998239807687, 0.047270692159623935, 0.4547318228471436, -0.25559475232148543, -0.37507070163509953, 0.12691339204090918, -0.27478196504403296, -0.14357013740166286, 0.1687758475048835, -0.17720508148... |
1,803.02404 | Effective electronic-only Kohn-Sham equations for the muonic molecules | A set of effective electronic-only Kohn-Sham (EKS) equations are derived for
the muonic molecules (containing a positively charged muon), which are
completely equivalent to the coupled electronic-muonic Kohn-Sham equations
derived previously within the framework of the Nuclear-Electronic Orbital
density functional th... | physics.atm-clus cond-mat.other physics.atom-ph physics.chem-ph | a set of effective electroniconly kohnsham eks equations are derived for the muonic molecules containing a positively charged muon which are completely equivalent to the coupled electronicmuonic kohnsham equations derived previously within the framework of the nuclearelectronic orbital density functional theory neodft ... | [['a', 'set', 'of', 'effective', 'electroniconly', 'kohnsham', 'eks', 'equations', 'are', 'derived', 'for', 'the', 'muonic', 'molecules', 'containing', 'a', 'positively', 'charged', 'muon', 'which', 'are', 'completely', 'equivalent', 'to', 'the', 'coupled', 'electronicmuonic', 'kohnsham', 'equations', 'derived', 'previ... | [-0.08325336201450051, 0.13566301227033206, -0.05042232266587868, 0.07787178033054691, -0.04717275911400011, -0.1575026695584109, 0.012005113229150908, 0.32931496626905987, -0.23190057764944172, -0.29284821270700934, 0.028372362622671496, -0.2922112997945639, -0.07951851500735725, 0.17990500762880854, 0.025727611205387... |
1,803.02405 | Gravitational radiation from the classical spinning double copy | We establish a correspondence between perturbative classical gluon and
gravitational radiation emitted by spinning sources, to linear order in spin.
This is an extension of the non-spinning classical perturbative double copy and
uses the same color-to-kinematic replacements. The gravitational theory has a
scalar (dil... | hep-th gr-qc hep-ph | we establish a correspondence between perturbative classical gluon and gravitational radiation emitted by spinning sources to linear order in spin this is an extension of the nonspinning classical perturbative double copy and uses the same colortokinematic replacements the gravitational theory has a scalar dilaton and ... | [['we', 'establish', 'a', 'correspondence', 'between', 'perturbative', 'classical', 'gluon', 'and', 'gravitational', 'radiation', 'emitted', 'by', 'spinning', 'sources', 'to', 'linear', 'order', 'in', 'spin', 'this', 'is', 'an', 'extension', 'of', 'the', 'nonspinning', 'classical', 'perturbative', 'double', 'copy', 'an... | [-0.14564122111358516, 0.13483479673563767, -0.11370795101666932, 0.12070547000856845, -0.10739896240342847, -0.0809517100582632, 0.03135059325979776, 0.29759480571374297, -0.19554764411740883, -0.2688912873512463, 0.0017441490002538024, -0.275540645371246, -0.14811623190625517, 0.16786979168639793, -0.0385076623692036... |
1,803.02406 | Tip of the red giant branch distances to the dwarf galaxies dw1335-29
and dw1340-30 in the Centaurus group | The abundance and spatial distribution of dwarf galaxies are excellent
empirical benchmarks to test models of structure formation on small scales. The
nearby Centaurus group, with its two subgroups centered on CenA and M83, stands
out as an important alternative to the Local Group for scrutinizing
cosmological model ... | astro-ph.GA | the abundance and spatial distribution of dwarf galaxies are excellent empirical benchmarks to test models of structure formation on small scales the nearby centaurus group with its two subgroups centered on cena and m83 stands out as an important alternative to the local group for scrutinizing cosmological model predi... | [['the', 'abundance', 'and', 'spatial', 'distribution', 'of', 'dwarf', 'galaxies', 'are', 'excellent', 'empirical', 'benchmarks', 'to', 'test', 'models', 'of', 'structure', 'formation', 'on', 'small', 'scales', 'the', 'nearby', 'centaurus', 'group', 'with', 'its', 'two', 'subgroups', 'centered', 'on', 'cena', 'and', 'm... | [-0.03995970178388585, 0.02653658193789057, -0.1323537573367219, 0.10541931273836337, -0.12546928874762264, -0.06337797573722594, 0.09269652679410233, 0.4656517858475059, -0.14543132823435365, -0.39906929193071494, 0.054947399573667205, -0.3079577693854178, -0.013517480460644724, 0.18903567131152585, -0.072741134292151... |
1,803.02407 | On the accuracy of simulating mixing by random-walk particle-based
mass-transfer algorithms | Several algorithms have been used for mass transfer between particles
undergoing advective and macro-dispersive random walks. The mass transfer
between particles is required for general reactions on, and among, particles.
The mass transfer is shown to be diffusive, and may be simulated using
implicit, explicit, or mi... | physics.comp-ph | several algorithms have been used for mass transfer between particles undergoing advective and macrodispersive random walks the mass transfer between particles is required for general reactions on and among particles the mass transfer is shown to be diffusive and may be simulated using implicit explicit or mixed method... | [['several', 'algorithms', 'have', 'been', 'used', 'for', 'mass', 'transfer', 'between', 'particles', 'undergoing', 'advective', 'and', 'macrodispersive', 'random', 'walks', 'the', 'mass', 'transfer', 'between', 'particles', 'is', 'required', 'for', 'general', 'reactions', 'on', 'and', 'among', 'particles', 'the', 'mas... | [-0.021660697509360033, 0.1364404254266992, -0.06804167212918401, 0.12970123322331348, -0.04651859573554248, -0.19977022647857667, 0.010271122106350958, 0.43869793843477967, -0.2057583590131253, -0.35807261830195786, 0.08788638267084024, -0.2745824573142454, -0.0776750519638881, 0.22952538362937047, 0.02242282613180577... |
1,803.02408 | ALMA Multiple-Transition Observations of High Density Molecular Tracers
in Ultraluminous Infrared Galaxies | We present the results of our ALMA observations of eleven (ultra)luminous
infrared galaxies ((U)LIRGs) at J=4-3 of HCN, HCO+, HNC and J=3-2 of HNC. This
is an extension of our previously published HCN and HCO+ J=3-2 observations to
multiple rotational J-transitions of multiple molecules, to investigate how
molecular ... | astro-ph.GA | we present the results of our alma observations of eleven ultraluminous infrared galaxies ulirgs at j43 of hcn hco hnc and j32 of hnc this is an extension of our previously published hcn and hco j32 observations to multiple rotational jtransitions of multiple molecules to investigate how molecular emission line flux ra... | [['we', 'present', 'the', 'results', 'of', 'our', 'alma', 'observations', 'of', 'eleven', 'ultraluminous', 'infrared', 'galaxies', 'ulirgs', 'at', 'j43', 'of', 'hcn', 'hco', 'hnc', 'and', 'j32', 'of', 'hnc', 'this', 'is', 'an', 'extension', 'of', 'our', 'previously', 'published', 'hcn', 'and', 'hco', 'j32', 'observatio... | [-0.03843395583603564, 0.023199300837123033, 0.059157507786675625, 0.09437494748581068, 0.0026006641467019452, -0.10455100528022225, 0.00674174182952497, 0.5493007939951742, -0.048989378822456416, -0.2682603305938192, -0.010792186431199379, -0.28084300008429364, 0.027236747344238765, 0.0859895232662684, 0.0513061582660... |
1,803.02409 | On the parameterized complexity of manipulating Top Trading Cycles | We study the problem of exchange when 1) agents are endowed with
heterogeneous indivisible objects, and 2) there is no money. In general, no
rule satisfies the three central properties Pareto-efficiency, individual
rationality, and strategy-proofness \cite{Sonmez1999}. Recently, it was shown
that Top Trading Cycles i... | cs.GT cs.CC | we study the problem of exchange when 1 agents are endowed with heterogeneous indivisible objects and 2 there is no money in general no rule satisfies the three central properties paretoefficiency individual rationality and strategyproofness citesonmez1999 recently it was shown that top trading cycles is nphard to mani... | [['we', 'study', 'the', 'problem', 'of', 'exchange', 'when', '1', 'agents', 'are', 'endowed', 'with', 'heterogeneous', 'indivisible', 'objects', 'and', '2', 'there', 'is', 'no', 'money', 'in', 'general', 'no', 'rule', 'satisfies', 'the', 'three', 'central', 'properties', 'paretoefficiency', 'individual', 'rationality',... | [-0.1546112230627618, 0.08844071811915045, -0.07592979163933568, 0.09826154105177377, -0.1347583751684349, -0.19277451144346194, 0.1113595476834245, 0.3908515801661435, -0.299513541243709, -0.3246692545325305, 0.08619062569842004, -0.278593058059297, -0.12326667452508812, 0.1776897836774751, -0.10853618162831194, 0.018... |
1,803.0241 | Quantum algorithm for energy matching in hard optimization problems | We consider the ability of local quantum dynamics to solve the energy
matching problem: given an instance of a classical optimization problem and a
low energy state, find another macroscopically distinct low energy state.
Energy matching is difficult in rugged optimization landscapes, as the given
state provides litt... | cond-mat.dis-nn cond-mat.stat-mech quant-ph | we consider the ability of local quantum dynamics to solve the energy matching problem given an instance of a classical optimization problem and a low energy state find another macroscopically distinct low energy state energy matching is difficult in rugged optimization landscapes as the given state provides little inf... | [['we', 'consider', 'the', 'ability', 'of', 'local', 'quantum', 'dynamics', 'to', 'solve', 'the', 'energy', 'matching', 'problem', 'given', 'an', 'instance', 'of', 'a', 'classical', 'optimization', 'problem', 'and', 'a', 'low', 'energy', 'state', 'find', 'another', 'macroscopically', 'distinct', 'low', 'energy', 'state... | [-0.14995859374435858, 0.16409814903528697, -0.09854353273961138, 0.12198071244192567, -0.012192290481378106, -0.15890174217750022, 0.043474144741714474, 0.3347953102452324, -0.2938425897600803, -0.3513339915055227, 0.07329349664059726, -0.24729428087129565, -0.10936111046120207, 0.14492101519011913, -0.014452101314499... |
1,803.02411 | The Deconfinement Phase Transition in Proto-Neutron-Star Matter | In this work, we study in detail the deconfinement phase transition that
takes place in hot/dense nuclear matter in the context of neutron stars and
proto-neutron stars (in which lepton fraction is fixed). The possibility of
different mixtures of phases with different locally and globally conserved
quantities is cons... | nucl-th astro-ph.HE astro-ph.SR | in this work we study in detail the deconfinement phase transition that takes place in hotdense nuclear matter in the context of neutron stars and protoneutron stars in which lepton fraction is fixed the possibility of different mixtures of phases with different locally and globally conserved quantities is considered i... | [['in', 'this', 'work', 'we', 'study', 'in', 'detail', 'the', 'deconfinement', 'phase', 'transition', 'that', 'takes', 'place', 'in', 'hotdense', 'nuclear', 'matter', 'in', 'the', 'context', 'of', 'neutron', 'stars', 'and', 'protoneutron', 'stars', 'in', 'which', 'lepton', 'fraction', 'is', 'fixed', 'the', 'possibility... | [-0.07702060973131529, 0.24868942358701926, -0.10912181677356843, 0.08567710278520702, -0.0347867562280347, -0.060421761245496815, 0.03227040076488128, 0.3707005020271065, -0.1418504506644983, -0.2626563240924189, 0.005785956886166366, -0.25194003641284923, -0.068811741539888, 0.09331940867066864, 0.009075535518888345,... |
1,803.02412 | Securing Untrusted Full-Duplex Relay Channels in the Presence of
Multiple External Cluster-Based Eavesdroppers | This letter investigates the physical layer security in a wireless
cooperative network where communication is assisted by a full-duplex (FD)
untrusted relay in the presence of multiple external eavesdroppers. A
cluster-based colluding eavesdropping setting is considered, where illegitimate
nodes with common interests... | cs.IT cs.NI math.IT | this letter investigates the physical layer security in a wireless cooperative network where communication is assisted by a fullduplex fd untrusted relay in the presence of multiple external eavesdroppers a clusterbased colluding eavesdropping setting is considered where illegitimate nodes with common interests are gro... | [['this', 'letter', 'investigates', 'the', 'physical', 'layer', 'security', 'in', 'a', 'wireless', 'cooperative', 'network', 'where', 'communication', 'is', 'assisted', 'by', 'a', 'fullduplex', 'fd', 'untrusted', 'relay', 'in', 'the', 'presence', 'of', 'multiple', 'external', 'eavesdroppers', 'a', 'clusterbased', 'coll... | [-0.35204936082376853, 0.0030093718262361293, -0.00877060299333101, -0.013585397129864396, -0.07720953969790817, -0.36396338199300315, 0.18933983469255886, 0.36188471796257154, -0.265310567558596, -0.2496156975555362, 0.04032937777088605, -0.29027782699891497, -0.16660332735767938, 0.05710430344290107, -0.1344227170417... |
1,803.02413 | The weak type $(1,p)$ for convolution operators on locally compact
groups | In this paper we provide necessary and sufficient conditions for the
$\textnormal{weak}(1,p)$ boundedness, $1< p<\infty,$ of convolution operators
on locally compact (Hausdorff) topological groups. So, we generalize a
classical result due to Sobolev-Hardy-Littlewood and Stepanov. Applications to
Fourier multipliers o... | math.FA | in this paper we provide necessary and sufficient conditions for the textnormalweak1p boundedness 1 pinfty of convolution operators on locally compact hausdorff topological groups so we generalize a classical result due to sobolevhardylittlewood and stepanov applications to fourier multipliers on lie groups also are gi... | [['in', 'this', 'paper', 'we', 'provide', 'necessary', 'and', 'sufficient', 'conditions', 'for', 'the', 'textnormalweak1p', 'boundedness', '1', 'pinfty', 'of', 'convolution', 'operators', 'on', 'locally', 'compact', 'hausdorff', 'topological', 'groups', 'so', 'we', 'generalize', 'a', 'classical', 'result', 'due', 'to',... | [-0.1224847257050664, 0.08630779446210972, -0.08502366805319177, 0.12285905563933125, -0.13588458399266698, -0.08886972155292021, 0.022321922626064788, 0.42701386729645174, -0.2725567857539931, -0.1616524212755436, 0.18910939426183007, -0.2133793407228104, -0.1623489625838607, 0.24607434722616575, -0.21722711507924075,... |
1,803.02414 | A gradient method in a Hilbert space with an optimized inner product:
achieving a Newton-like convergence | In this paper we introduce a new gradient method which attains quadratic
convergence in a certain sense. Applicable to infinite-dimensional
unconstrained minimization problems posed in a Hilbert space $H$, the approach
consists in finding the energy gradient $g(\lambda)$ defined with respect to an
optimal inner produ... | math.NA | in this paper we introduce a new gradient method which attains quadratic convergence in a certain sense applicable to infinitedimensional unconstrained minimization problems posed in a hilbert space h the approach consists in finding the energy gradient glambda defined with respect to an optimal inner product selected ... | [['in', 'this', 'paper', 'we', 'introduce', 'a', 'new', 'gradient', 'method', 'which', 'attains', 'quadratic', 'convergence', 'in', 'a', 'certain', 'sense', 'applicable', 'to', 'infinitedimensional', 'unconstrained', 'minimization', 'problems', 'posed', 'in', 'a', 'hilbert', 'space', 'h', 'the', 'approach', 'consists',... | [-0.08736744526715025, 0.025634969272006827, -0.0835684692848283, 0.03181135795614499, -0.045295063103961676, -0.11485122417019109, 0.029681683023456543, 0.3682042412445184, -0.32130746299943586, -0.23508782447687, 0.09892919925948987, -0.23533175597114003, -0.1437085162102076, 0.21016527963417223, -0.07889193173967243... |
1,803.02415 | Almost Sure Uniqueness of a Global Minimum Without Convexity | This paper establishes the argmin of a random objective function to be unique
almost surely. This paper first formulates a general result that proves almost
sure uniqueness without convexity of the objective function. The general result
is then applied to a variety of applications in statistics. Four applications
are... | econ.EM math.ST stat.TH | this paper establishes the argmin of a random objective function to be unique almost surely this paper first formulates a general result that proves almost sure uniqueness without convexity of the objective function the general result is then applied to a variety of applications in statistics four applications are disc... | [['this', 'paper', 'establishes', 'the', 'argmin', 'of', 'a', 'random', 'objective', 'function', 'to', 'be', 'unique', 'almost', 'surely', 'this', 'paper', 'first', 'formulates', 'a', 'general', 'result', 'that', 'proves', 'almost', 'sure', 'uniqueness', 'without', 'convexity', 'of', 'the', 'objective', 'function', 'th... | [-0.09632904819940051, -0.049470713081425186, -0.10148228826128865, 0.12006301314518979, -0.0611484318474078, -0.14430890291648574, 0.03765414880065579, 0.35851736795412353, -0.29489634908123374, -0.23866212739902612, 0.1573757667545778, -0.23534557343243737, -0.20803530017960153, 0.19416343936160818, -0.13451676459804... |
1,803.02416 | Examination of the observability of a chiral magnetically-driven
charge-separation difference in collisions of the $\mathrm{^{96}_{44}Ru +\,
^{96}_{44}Ru}$ and $\mathrm{^{96}_{40}Zr +\, ^{96}_{40}Zr}$ isobars at
energies available at RHIC | Anomalous Viscous Fluid Dynamics (AVFD) model calculations for
$\mathrm{^{96}_{44}Ru +\, ^{96}_{44}Ru}$ and $\mathrm{^{96}_{40}Zr +\,
^{96}_{40}Zr}$ collisions ($\sqrt{s_{\rm NN}} = 200$ GeV) are used in concert
with a charge-sensitive correlator, to test its ability to detect and
characterize the charge separation d... | nucl-ex | anomalous viscous fluid dynamics avfd model calculations for mathrm96_44ru 96_44ru and mathrm96_40zr 96_40zr collisions sqrts_rm nn 200 gev are used in concert with a chargesensitive correlator to test its ability to detect and characterize the charge separation difference expected from the chiral magnetic effect cme i... | [['anomalous', 'viscous', 'fluid', 'dynamics', 'avfd', 'model', 'calculations', 'for', 'mathrm96_44ru', '96_44ru', 'and', 'mathrm96_40zr', '96_40zr', 'collisions', 'sqrts_rm', 'nn', '200', 'gev', 'are', 'used', 'in', 'concert', 'with', 'a', 'chargesensitive', 'correlator', 'to', 'test', 'its', 'ability', 'to', 'detect'... | [-0.08522535362766771, 0.1828182079167344, -0.12134492288782331, 0.14314892779543134, 0.017088079113082206, -0.11338363439691337, -0.03609571488735782, 0.33964672920194044, -0.16759258729967574, -0.3459737643999748, -0.0034488006571908136, -0.34022338611404757, -0.0038663892244750805, 0.1833548037121688, 0.070849550202... |
1,803.02417 | Room temperature deposition of superconducting Niobium Nitride films by
ion beam assisted sputtering | We use room temperature ion beam assisted sputtering (IBAS) to deposit
niobium nitride thin films. Electrical and structural characterizations were
performed by electric transport and magnetization measurements at variable
temperatures, X-ray diffraction and atomic force microscopy. Compared to
reactive sputtering of... | cond-mat.supr-con | we use room temperature ion beam assisted sputtering ibas to deposit niobium nitride thin films electrical and structural characterizations were performed by electric transport and magnetization measurements at variable temperatures xray diffraction and atomic force microscopy compared to reactive sputtering of nbn fil... | [['we', 'use', 'room', 'temperature', 'ion', 'beam', 'assisted', 'sputtering', 'ibas', 'to', 'deposit', 'niobium', 'nitride', 'thin', 'films', 'electrical', 'and', 'structural', 'characterizations', 'were', 'performed', 'by', 'electric', 'transport', 'and', 'magnetization', 'measurements', 'at', 'variable', 'temperatur... | [-0.07489494448527693, 0.2822959412321506, -0.0059179853275418285, -0.08028492202749477, 0.029269128012820146, -0.20085112502798438, 0.09887050742923748, 0.48367164984345434, -0.23140310306102038, -0.3364944994356483, 0.008121293194126338, -0.3770656671375036, 0.047518772080074996, 0.2533896312559955, 0.010179327819496... |
1,803.02418 | Anisotropic swim stress in active matter with nematic order | Active Brownian Particles (ABPs) transmit a swim pressure $\Pi^{swim}=n\zeta
D^{swim}$ to the container boundaries, where $\zeta$ is the drag coefficient,
$D^{swim}$ is the swim diffusivity and $n$ is the uniform bulk number density
far from the container walls. In this work we extend the notion of the
isotropic swim... | cond-mat.soft | active brownian particles abps transmit a swim pressure piswimnzeta dswim to the container boundaries where zeta is the drag coefficient dswim is the swim diffusivity and n is the uniform bulk number density far from the container walls in this work we extend the notion of the isotropic swim pressure to the anisotropic... | [['active', 'brownian', 'particles', 'abps', 'transmit', 'a', 'swim', 'pressure', 'piswimnzeta', 'dswim', 'to', 'the', 'container', 'boundaries', 'where', 'zeta', 'is', 'the', 'drag', 'coefficient', 'dswim', 'is', 'the', 'swim', 'diffusivity', 'and', 'n', 'is', 'the', 'uniform', 'bulk', 'number', 'density', 'far', 'fro... | [-0.1802138638626589, 0.25358478038532767, -0.09749316908809215, -0.04822977718772825, -0.08985391452284383, -0.1047582045631454, -0.02615101977266098, 0.358202246856432, -0.30436688691075325, -0.25258045856955497, 0.03119526241408632, -0.276025851410131, -0.13851965074451805, 0.13319832649988889, -0.000669315656042457... |
1,803.02419 | A multi-instrument and multi-wavelength high angular resolution study of
MWC614: quantum heated particles inside the disk cavity | High angular resolution observations of young stellar objects are required to
study the inner astronomical units of protoplanetary disks in which the
majority of planets form. As they evolve, gaps open up in the inner disk
regions and the disks are fully dispersed within ~10 Myrs. MWC 614 is a
pre-transitional object... | astro-ph.SR | high angular resolution observations of young stellar objects are required to study the inner astronomical units of protoplanetary disks in which the majority of planets form as they evolve gaps open up in the inner disk regions and the disks are fully dispersed within 10 myrs mwc 614 is a pretransitional object with a... | [['high', 'angular', 'resolution', 'observations', 'of', 'young', 'stellar', 'objects', 'are', 'required', 'to', 'study', 'the', 'inner', 'astronomical', 'units', 'of', 'protoplanetary', 'disks', 'in', 'which', 'the', 'majority', 'of', 'planets', 'form', 'as', 'they', 'evolve', 'gaps', 'open', 'up', 'in', 'the', 'inner... | [-0.06685945904873153, 0.13234732741690636, -0.06542838472608871, 0.019283114259745528, -0.09481012710330493, -0.0724867602671556, 0.0033126537182784463, 0.4518710493446982, -0.1915158926628213, -0.35289211744601107, 0.10791677622647183, -0.2696003863285791, 0.017276265004530868, 0.15040434341149483, -0.084718336116527... |
1,803.0242 | Classification of Groups according to the number of end vertices in the
coprime graph | In this paper we characterize groups according to the number of end vertices
in the associated coprime graphs. An upper bound on the order of the group that
depends on the number of end vertices is obtained. We also prove that
$2-$groups are the only groups whose coprime graphs have odd number of end
vertices. Classi... | math.GR | in this paper we characterize groups according to the number of end vertices in the associated coprime graphs an upper bound on the order of the group that depends on the number of end vertices is obtained we also prove that 2groups are the only groups whose coprime graphs have odd number of end vertices classification... | [['in', 'this', 'paper', 'we', 'characterize', 'groups', 'according', 'to', 'the', 'number', 'of', 'end', 'vertices', 'in', 'the', 'associated', 'coprime', 'graphs', 'an', 'upper', 'bound', 'on', 'the', 'order', 'of', 'the', 'group', 'that', 'depends', 'on', 'the', 'number', 'of', 'end', 'vertices', 'is', 'obtained', '... | [-0.23753455680106644, 0.17038136742058155, -0.03884032041178611, -0.0005635166662218778, -0.09179325458978344, -0.13703175569358078, 0.028516954963814223, 0.3856265922785615, -0.2127004955571307, -0.3376609560345178, 0.08617514904472046, -0.34696205948357994, -0.15543188992887735, 0.11182355506183661, -0.1011130629998... |
1,803.02421 | Masked Conditional Neural Networks for Audio Classification | We present the ConditionaL Neural Network (CLNN) and the Masked ConditionaL
Neural Network (MCLNN) designed for temporal signal recognition. The CLNN takes
into consideration the temporal nature of the sound signal and the MCLNN
extends upon the CLNN through a binary mask to preserve the spatial locality of
the featu... | stat.ML cs.LG cs.SD eess.AS | we present the conditional neural network clnn and the masked conditional neural network mclnn designed for temporal signal recognition the clnn takes into consideration the temporal nature of the sound signal and the mclnn extends upon the clnn through a binary mask to preserve the spatial locality of the features and... | [['we', 'present', 'the', 'conditional', 'neural', 'network', 'clnn', 'and', 'the', 'masked', 'conditional', 'neural', 'network', 'mclnn', 'designed', 'for', 'temporal', 'signal', 'recognition', 'the', 'clnn', 'takes', 'into', 'consideration', 'the', 'temporal', 'nature', 'of', 'the', 'sound', 'signal', 'and', 'the', '... | [-0.06166622716261131, -0.04109398113924188, -0.0715232659701486, 0.07095643286878357, -0.11468724175641427, -0.15628972334540164, -0.007892983663846187, 0.4390483860078515, -0.25311129700454255, -0.2909836215537269, 0.08406277191682662, -0.2592956837056126, -0.2073537701056624, 0.19671840910153576, -0.1038266587717344... |
1,803.02422 | Towards Quantifying Sampling Bias in Network Inference | Relational inference leverages relationships between entities and links in a
network to infer information about the network from a small sample. This method
is often used when global information about the network is not available or
difficult to obtain. However, how reliable is inference from a small labelled
sample?... | cs.SI physics.soc-ph | relational inference leverages relationships between entities and links in a network to infer information about the network from a small sample this method is often used when global information about the network is not available or difficult to obtain however how reliable is inference from a small labelled sample how s... | [['relational', 'inference', 'leverages', 'relationships', 'between', 'entities', 'and', 'links', 'in', 'a', 'network', 'to', 'infer', 'information', 'about', 'the', 'network', 'from', 'a', 'small', 'sample', 'this', 'method', 'is', 'often', 'used', 'when', 'global', 'information', 'about', 'the', 'network', 'is', 'not... | [-0.0767742029016459, 0.04795296493180614, -0.06732374299965042, 0.12599151201152745, -0.1044485491627633, -0.14706089414835455, 0.11620737601290732, 0.4519807132170162, -0.27939530777530797, -0.3705789184865148, 0.09508057193890374, -0.23856026749002104, -0.21393649508793125, 0.15032124608371625, -0.1131587941822083, ... |
1,803.02423 | Matched Filters for Noisy Induced Subgraph Detection | The problem of finding the vertex correspondence between two noisy graphs
with different number of vertices where the smaller graph is still large has
many applications in social networks, neuroscience, and computer vision. We
propose a solution to this problem via a graph matching matched filter:
centering and paddi... | stat.ML cs.DS | the problem of finding the vertex correspondence between two noisy graphs with different number of vertices where the smaller graph is still large has many applications in social networks neuroscience and computer vision we propose a solution to this problem via a graph matching matched filter centering and padding the... | [['the', 'problem', 'of', 'finding', 'the', 'vertex', 'correspondence', 'between', 'two', 'noisy', 'graphs', 'with', 'different', 'number', 'of', 'vertices', 'where', 'the', 'smaller', 'graph', 'is', 'still', 'large', 'has', 'many', 'applications', 'in', 'social', 'networks', 'neuroscience', 'and', 'computer', 'vision'... | [-0.08048826984732467, 0.03163600001451628, -0.05069509910981116, 0.07971967226579128, -0.10084284742034096, -0.16580501934890088, 0.02836930709754062, 0.4404895111863666, -0.32358294845942187, -0.3517848932376022, 0.1063606898594812, -0.27317091222195067, -0.22806883209439763, 0.16056325336343005, -0.11928347170435111... |
1,803.02424 | Universal image systems for non-periodic and periodic Stokes flows above
a no-slip wall | It is well-known that by placing judiciously chosen image point forces and
doublets to the Stokeslet above a flat wall, the no-slip boundary condition can
be conveniently imposed on the wall [Blake, J. R. Math. Proc. Camb. Philos.
Soc. 70(2), 1971: 303.]. However, to further impose periodic boundary
conditions on dir... | math.NA physics.flu-dyn | it is wellknown that by placing judiciously chosen image point forces and doublets to the stokeslet above a flat wall the noslip boundary condition can be conveniently imposed on the wall blake j r math proc camb philos soc 702 1971 303 however to further impose periodic boundary conditions on directions parallel to th... | [['it', 'is', 'wellknown', 'that', 'by', 'placing', 'judiciously', 'chosen', 'image', 'point', 'forces', 'and', 'doublets', 'to', 'the', 'stokeslet', 'above', 'a', 'flat', 'wall', 'the', 'noslip', 'boundary', 'condition', 'can', 'be', 'conveniently', 'imposed', 'on', 'the', 'wall', 'blake', 'j', 'r', 'math', 'proc', 'c... | [-0.1275144280117591, 0.04321413248348353, -0.050587186066622145, 0.009775309808410997, -0.11958313938308758, -0.18255945307390994, 0.02910738087683037, 0.3900377233774307, -0.2903556114875612, -0.27251032936279507, 0.11505600382257358, -0.20393243123487154, -0.1270948114891254, 0.18258210000963987, -0.1184662578639239... |
1,803.02425 | Product SCFTs for the $E_7$ Theory | We present a simple criterion for when an N=2 SCFT must be a product SCFT.
Applied to the class-S theories of type $E_7$, we find 29 (out of 11,000)
3-punctured spheres which are product SCFTs.
| hep-th | we present a simple criterion for when an n2 scft must be a product scft applied to the classs theories of type e_7 we find 29 out of 11000 3punctured spheres which are product scfts | [['we', 'present', 'a', 'simple', 'criterion', 'for', 'when', 'an', 'n2', 'scft', 'must', 'be', 'a', 'product', 'scft', 'applied', 'to', 'the', 'classs', 'theories', 'of', 'type', 'e_7', 'we', 'find', '29', 'out', 'of', '11000', '3punctured', 'spheres', 'which', 'are', 'product', 'scfts']] | [-0.10271978878549166, 0.10855613222187717, -0.06391869437481676, 0.05210172810724804, -0.0253581409342587, -0.19091693173561777, 0.006985766833115901, 0.36607462944728986, -0.1558320796649371, -0.2671356536980186, 0.12550833245207157, -0.2796583794057369, -0.16853222698305867, 0.09907328209706716, -0.06251679733395576... |
1,803.02426 | Local available quantum correlations for Bell Diagonal states and
markovian decoherence | Local available quantum correlations (LAQCs), as defined by Mundarain et al.
[19], are analytically determined for Bell Diagonal states. Using the Kraus
operators formalism [10], we analyze the dissipative dynamics of 2-qubit LAQCs
under markovian decoherence. This is done for Werner states under the
depolarizing [20... | quant-ph | local available quantum correlations laqcs as defined by mundarain et al 19 are analytically determined for bell diagonal states using the kraus operators formalism 10 we analyze the dissipative dynamics of 2qubit laqcs under markovian decoherence this is done for werner states under the depolarizing 20 and phase dampi... | [['local', 'available', 'quantum', 'correlations', 'laqcs', 'as', 'defined', 'by', 'mundarain', 'et', 'al', '19', 'are', 'analytically', 'determined', 'for', 'bell', 'diagonal', 'states', 'using', 'the', 'kraus', 'operators', 'formalism', '10', 'we', 'analyze', 'the', 'dissipative', 'dynamics', 'of', '2qubit', 'laqcs',... | [-0.11222882062687119, 0.22838178149679988, -0.007205304079812712, 0.07949856765963863, 0.08374063584302445, -0.22808995354195347, 0.039172272117544725, 0.3072343516962982, -0.1745684172118374, -0.30054209246176533, 0.08233255559766038, -0.28888768059370495, -0.12728615966419468, 0.21453392809767902, -0.059167706313341... |
1,803.02427 | Estimating network structure from unreliable measurements | Most empirical studies of networks assume that the network data we are given
represent a complete and accurate picture of the nodes and edges in the system
of interest, but in real-world situations this is rarely the case. More often
the data only specify the network structure imperfectly -- like data in
essentially ... | cs.SI physics.soc-ph | most empirical studies of networks assume that the network data we are given represent a complete and accurate picture of the nodes and edges in the system of interest but in realworld situations this is rarely the case more often the data only specify the network structure imperfectly like data in essentially every ot... | [['most', 'empirical', 'studies', 'of', 'networks', 'assume', 'that', 'the', 'network', 'data', 'we', 'are', 'given', 'represent', 'a', 'complete', 'and', 'accurate', 'picture', 'of', 'the', 'nodes', 'and', 'edges', 'in', 'the', 'system', 'of', 'interest', 'but', 'in', 'realworld', 'situations', 'this', 'is', 'rarely',... | [-0.12705659020803464, 0.03291776252107398, -0.027753118894643325, 0.07271522550803164, -0.10556500477284408, -0.16822666683963136, 0.07192555231892545, 0.4318933458863825, -0.25980537970283785, -0.32557836996842315, 0.12314907572842945, -0.30892734210668266, -0.18444690106949513, 0.17927596989371206, -0.06136268122033... |
1,803.02428 | Strongly correlated photon transport in waveguide QED with weakly
coupled emitters | We show that strongly correlated photon transport can be observed in
waveguides containing optically dense ensembles of emitters. Remarkably, this
occurs even for weak coupling efficiencies. Specifically, we compute the photon
transport properties through a chirally coupled system of $N$ two-level systems
driven by a... | quant-ph physics.optics | we show that strongly correlated photon transport can be observed in waveguides containing optically dense ensembles of emitters remarkably this occurs even for weak coupling efficiencies specifically we compute the photon transport properties through a chirally coupled system of n twolevel systems driven by a weak coh... | [['we', 'show', 'that', 'strongly', 'correlated', 'photon', 'transport', 'can', 'be', 'observed', 'in', 'waveguides', 'containing', 'optically', 'dense', 'ensembles', 'of', 'emitters', 'remarkably', 'this', 'occurs', 'even', 'for', 'weak', 'coupling', 'efficiencies', 'specifically', 'we', 'compute', 'the', 'photon', 't... | [-0.1712389704140444, 0.2546794462056207, -0.03737565038665648, 0.05059057440113036, 0.018526666854778606, -0.24313196573827056, 0.03661062727952676, 0.44314771581200824, -0.23611759296468188, -0.28529069153291564, -0.013501402018441548, -0.32781545944331636, -0.08748230566420863, 0.20495239693310954, 0.024697255850168... |
1,803.02429 | Testing Gravitational Memory Generation with Compact Binary Mergers | Gravitational memory is an important prediction of classical General
Relativity, which is intimately related to asymptotic symmetries at null
infinity and the so-called soft graviton theorem first shown by Weinberg. For a
given transient astronomical event, the angular distributions of energy and
angular momentum flu... | gr-qc hep-th | gravitational memory is an important prediction of classical general relativity which is intimately related to asymptotic symmetries at null infinity and the socalled soft graviton theorem first shown by weinberg for a given transient astronomical event the angular distributions of energy and angular momentum flux uniq... | [['gravitational', 'memory', 'is', 'an', 'important', 'prediction', 'of', 'classical', 'general', 'relativity', 'which', 'is', 'intimately', 'related', 'to', 'asymptotic', 'symmetries', 'at', 'null', 'infinity', 'and', 'the', 'socalled', 'soft', 'graviton', 'theorem', 'first', 'shown', 'by', 'weinberg', 'for', 'a', 'gi... | [-0.1292451424624546, 0.1551183247919517, -0.06963952615102433, 0.17373754788757484, -0.125739396795973, -0.08969626261788452, 0.03297316224913745, 0.33473163116830346, -0.20964352561203742, -0.33802284863536597, 0.07355728278862549, -0.2985587292083207, -0.09918330380179245, 0.20260683660818285, 0.004549649059665443, ... |
1,803.0243 | Quantum Distillation of Hilbert Spaces, Semi-classics and Anomaly
Matching | A symmetry-twisted boundary condition of the path integral provides a
suitable framework for the semi-classical analysis of nonperturbative quantum
field theories (QFTs), and we reinterpret it from the viewpoint of the Hilbert
space. An appropriate twist with the unbroken symmetry can potentially produce
huge cancell... | hep-th | a symmetrytwisted boundary condition of the path integral provides a suitable framework for the semiclassical analysis of nonperturbative quantum field theories qfts and we reinterpret it from the viewpoint of the hilbert space an appropriate twist with the unbroken symmetry can potentially produce huge cancellations a... | [['a', 'symmetrytwisted', 'boundary', 'condition', 'of', 'the', 'path', 'integral', 'provides', 'a', 'suitable', 'framework', 'for', 'the', 'semiclassical', 'analysis', 'of', 'nonperturbative', 'quantum', 'field', 'theories', 'qfts', 'and', 'we', 'reinterpret', 'it', 'from', 'the', 'viewpoint', 'of', 'the', 'hilbert', ... | [-0.14083392383272333, 0.19311298397539595, -0.12133534023244838, 0.09681010106511177, -0.06078020972872659, -0.12811905557069, 0.08546636749369851, 0.3246393063390961, -0.2525047172706122, -0.2457018819182702, 0.0882501238748442, -0.234316285128969, -0.16936267170593455, 0.13730057252899372, -0.07013883881869448, 0.07... |
1,803.02431 | Convexity of Self-Similar Transonic Shocks and Free Boundaries for the
Euler Equations for Potential Flow | We are concerned with geometric properties of transonic shocks as free
boundaries in two-dimensional self-similar coordinates for compressible fluid
flows, which are not only important for the understanding of geometric
structure and stability of fluid motions in continuum mechanics but also
fundamental in the mathem... | math.AP math-ph math.MP | we are concerned with geometric properties of transonic shocks as free boundaries in twodimensional selfsimilar coordinates for compressible fluid flows which are not only important for the understanding of geometric structure and stability of fluid motions in continuum mechanics but also fundamental in the mathematica... | [['we', 'are', 'concerned', 'with', 'geometric', 'properties', 'of', 'transonic', 'shocks', 'as', 'free', 'boundaries', 'in', 'twodimensional', 'selfsimilar', 'coordinates', 'for', 'compressible', 'fluid', 'flows', 'which', 'are', 'not', 'only', 'important', 'for', 'the', 'understanding', 'of', 'geometric', 'structure'... | [-0.13268970937812646, 0.08977530946930859, -0.13028601160531358, 0.06264632030907007, -0.10858225303222936, -0.1212761622659776, -0.04249034677780195, 0.32925311506677396, -0.34787852321401497, -0.22120332846692575, 0.1254842921248987, -0.22358030947769797, -0.08213051224687282, 0.18822124774831567, -0.042500520313449... |
1,803.02432 | On Nonlinear Dimensionality Reduction, Linear Smoothing and Autoencoding | We develop theory for nonlinear dimensionality reduction (NLDR). A number of
NLDR methods have been developed, but there is limited understanding of how
these methods work and the relationships between them. There is limited basis
for using existing NLDR theory for deriving new algorithms. We provide a novel
framewor... | stat.ML | we develop theory for nonlinear dimensionality reduction nldr a number of nldr methods have been developed but there is limited understanding of how these methods work and the relationships between them there is limited basis for using existing nldr theory for deriving new algorithms we provide a novel framework for an... | [['we', 'develop', 'theory', 'for', 'nonlinear', 'dimensionality', 'reduction', 'nldr', 'a', 'number', 'of', 'nldr', 'methods', 'have', 'been', 'developed', 'but', 'there', 'is', 'limited', 'understanding', 'of', 'how', 'these', 'methods', 'work', 'and', 'the', 'relationships', 'between', 'them', 'there', 'is', 'limite... | [-0.0784545846777319, -0.015289474279305784, -0.13727699624600284, 0.09205471237726284, -0.11338013231782525, -0.14185347948505572, 0.031433659924589324, 0.3811045521362261, -0.27480800629480545, -0.2746844408373969, 0.10012734765469125, -0.2411946893656436, -0.2017288494460059, 0.21363300243815916, -0.1068431039834677... |
1,803.02433 | Extracting useful information from connected vehicle data: An empirical
study of driving volatility measures and crash frequency at intersections | With the emergence of high-frequency connected and automated vehicle data,
analysts have become able to extract useful information from them. To this end,
the concept of "driving volatility" is defined and explored as deviation from
the norm. Several measures of dispersion and variation can be computed in
different w... | stat.AP | with the emergence of highfrequency connected and automated vehicle data analysts have become able to extract useful information from them to this end the concept of driving volatility is defined and explored as deviation from the norm several measures of dispersion and variation can be computed in different ways using... | [['with', 'the', 'emergence', 'of', 'highfrequency', 'connected', 'and', 'automated', 'vehicle', 'data', 'analysts', 'have', 'become', 'able', 'to', 'extract', 'useful', 'information', 'from', 'them', 'to', 'this', 'end', 'the', 'concept', 'of', 'driving', 'volatility', 'is', 'defined', 'and', 'explored', 'as', 'deviat... | [-0.10796465861366082, 0.10981463851416755, -0.06449946984248965, 0.12071890521226039, -0.05628386060482856, -0.1709318905058934, 0.07586209122166337, 0.3943525329307021, -0.2518505500610843, -0.31813502027447443, 0.1618840928034236, -0.3173596349032409, -0.0778465837387024, 0.2126708420921102, -0.13351737225734925, 0.... |
1,803.02434 | Impact of the reduced speed of light approximation on the post-overlap
neutral hydrogen fraction in numerical simulations of the epoch of
reionization | The reduced speed of light approximation is used in a variety of simulations
of the epoch of reionization and galaxy formation. Its popularity stems from
its ability to drastically reduce the computing cost of a simulation, by
allowing the use of larger, and therefore fewer timesteps to reach a solution.
It is physic... | astro-ph.CO astro-ph.GA | the reduced speed of light approximation is used in a variety of simulations of the epoch of reionization and galaxy formation its popularity stems from its ability to drastically reduce the computing cost of a simulation by allowing the use of larger and therefore fewer timesteps to reach a solution it is physically m... | [['the', 'reduced', 'speed', 'of', 'light', 'approximation', 'is', 'used', 'in', 'a', 'variety', 'of', 'simulations', 'of', 'the', 'epoch', 'of', 'reionization', 'and', 'galaxy', 'formation', 'its', 'popularity', 'stems', 'from', 'its', 'ability', 'to', 'drastically', 'reduce', 'the', 'computing', 'cost', 'of', 'a', 's... | [-0.06633131636612284, 0.12480530524639376, -0.06383070828166272, 0.030226929856166627, -0.051498222888905, -0.07502484229662139, 0.09450698514985836, 0.3721001722827503, -0.2479775044330975, -0.34774228835040766, 0.07172385216058516, -0.24080195874487823, -0.058408972810428984, 0.19521538061857915, -0.0306982317286514... |
1,803.02435 | On the symmetrized arithmetic-geometric mean inequality for opertors | We study the symmetrized noncommutative arithmetic geometric mean inequality
introduced(AGM) by Recht and R\'{e} $$
\|\frac{(n-d)!}{n!}\sum\limits_{{ j_1,...,j_d \mbox{ different}}
}A_{j_{1}}^*A_{j_{2}}^*...A_{j_{d}}^*A_{j_{d}}...A_{j_{2}}A_{j_{1}} \| \leq
C(d,n) \|\frac{1}{n} \sum_{j=1}^n A_j^*A_j\|^d .$$
Comple... | math.OA math.FA | we study the symmetrized noncommutative arithmetic geometric mean inequality introducedagm by recht and re fracndnsumlimits_ j_1j_d mbox different a_j_1a_j_2a_j_da_j_da_j_2a_j_1 leq cdn frac1n sum_j1n a_ja_jd complementing the results from recht and re we find upper bounds for cdn under additional assumptions moreover ... | [['we', 'study', 'the', 'symmetrized', 'noncommutative', 'arithmetic', 'geometric', 'mean', 'inequality', 'introducedagm', 'by', 'recht', 'and', 're', 'fracndnsumlimits_', 'j_1j_d', 'mbox', 'different', 'a_j_1a_j_2a_j_da_j_da_j_2a_j_1', 'leq', 'cdn', 'frac1n', 'sum_j1n', 'a_ja_jd', 'complementing', 'the', 'results', 'f... | [-0.10333410746910993, 0.07627829133587725, -0.06515009334201322, 0.08444548009292167, -0.010281732448321932, -0.1758707656415508, 0.07940198174294304, 0.329751482112881, -0.262639676600092, -0.2700290389139863, 0.10614290569415864, -0.3028198287849698, -0.15319549741826075, 0.2482449137879645, -0.10089748221559121, 0.... |
1,803.02436 | Impact Factors and the Central Limit Theorem: Why Citation Averages Are
Scale Dependent | Citation averages, and Impact Factors (IFs) in particular, are sensitive to
sample size. We apply the Central Limit Theorem (CLT) to IFs to understand
their scale-dependent behavior. For a journal of $n$ randomly selected papers
from a population of all papers, we expect from the CLT that its IF fluctuates
around the... | physics.soc-ph cs.DL | citation averages and impact factors ifs in particular are sensitive to sample size we apply the central limit theorem clt to ifs to understand their scaledependent behavior for a journal of n randomly selected papers from a population of all papers we expect from the clt that its if fluctuates around the population av... | [['citation', 'averages', 'and', 'impact', 'factors', 'ifs', 'in', 'particular', 'are', 'sensitive', 'to', 'sample', 'size', 'we', 'apply', 'the', 'central', 'limit', 'theorem', 'clt', 'to', 'ifs', 'to', 'understand', 'their', 'scaledependent', 'behavior', 'for', 'a', 'journal', 'of', 'n', 'randomly', 'selected', 'pape... | [-0.042250521724563186, 0.13380934882593545, -0.0887163400110318, 0.12003589371571403, -0.07352850679390448, -0.11821929900331074, 0.11562254552831445, 0.36351779323110733, -0.20831542291806834, -0.32139659654381997, 0.006695943076226057, -0.33809720628397943, -0.08661839547698705, 0.18979779878703634, -0.1015573450058... |
1,803.02437 | Metallic nanolayers -- a sub-visible wonderland of optical properties | It was predicted long ago that ultra-thin metallic films must exhibit unusual
optical properties for radiation frequencies from rf to infrared domain. A film
would remain highly reflective even when it is orders of magnitude thinner than
a skin depth at any frequency. Only when it is a few nanometers thick
(depending... | physics.optics | it was predicted long ago that ultrathin metallic films must exhibit unusual optical properties for radiation frequencies from rf to infrared domain a film would remain highly reflective even when it is orders of magnitude thinner than a skin depth at any frequency only when it is a few nanometers thick depending on ma... | [['it', 'was', 'predicted', 'long', 'ago', 'that', 'ultrathin', 'metallic', 'films', 'must', 'exhibit', 'unusual', 'optical', 'properties', 'for', 'radiation', 'frequencies', 'from', 'rf', 'to', 'infrared', 'domain', 'a', 'film', 'would', 'remain', 'highly', 'reflective', 'even', 'when', 'it', 'is', 'orders', 'of', 'ma... | [-0.07952227808909454, 0.172209851539639, -0.06104679648563558, -0.00035792932270423453, -0.09516026258842983, -0.14868616782512298, 0.03907988511377434, 0.48822823785902825, -0.22401486524362482, -0.3018140158542961, 0.13733347428633885, -0.30368922541246696, -0.11919539045158993, 0.26110182869403314, -0.0258370187937... |
1,803.02438 | Quantum Process Identification: A Method for Characterizing
Non-Markovian Quantum Dynamics | Established methods for characterizing quantum information processes do not
capture non-Markovian (history-dependent) behaviors that occur in real systems.
These methods model a quantum process as a fixed map on the state space of a
predefined system of interest. Such a map averages over the system's
environment, whi... | quant-ph | established methods for characterizing quantum information processes do not capture nonmarkovian historydependent behaviors that occur in real systems these methods model a quantum process as a fixed map on the state space of a predefined system of interest such a map averages over the systems environment which may ret... | [['established', 'methods', 'for', 'characterizing', 'quantum', 'information', 'processes', 'do', 'not', 'capture', 'nonmarkovian', 'historydependent', 'behaviors', 'that', 'occur', 'in', 'real', 'systems', 'these', 'methods', 'model', 'a', 'quantum', 'process', 'as', 'a', 'fixed', 'map', 'on', 'the', 'state', 'space',... | [-0.12823000672107485, 0.0937250093787512, -0.1362833714638369, 0.05710120025750793, -0.013298612097533394, -0.1360048586002989, 0.04774022933901564, 0.3635941496433597, -0.29325172330622806, -0.26033936994635076, 0.08940600095684618, -0.24424691619372768, -0.1971308139330438, 0.25426848413322767, -0.04816278804850565,... |
1,803.02439 | Microscopic dynamical Casimir effect | We consider an atom in its ground state undergoing a non-relativistic
oscillation in free space. The interaction with the electromagnetic quantum
vacuum leads to two effects to leading order in perturbation theory. When the
mechanical frequency is larger than the atomic transition frequency, the
dominant effect is th... | quant-ph physics.atom-ph | we consider an atom in its ground state undergoing a nonrelativistic oscillation in free space the interaction with the electromagnetic quantum vacuum leads to two effects to leading order in perturbation theory when the mechanical frequency is larger than the atomic transition frequency the dominant effect is the moti... | [['we', 'consider', 'an', 'atom', 'in', 'its', 'ground', 'state', 'undergoing', 'a', 'nonrelativistic', 'oscillation', 'in', 'free', 'space', 'the', 'interaction', 'with', 'the', 'electromagnetic', 'quantum', 'vacuum', 'leads', 'to', 'two', 'effects', 'to', 'leading', 'order', 'in', 'perturbation', 'theory', 'when', 't... | [-0.14822593486499486, 0.24839142751617188, -0.08738064840296979, 0.04967896927234112, -0.059545959287571525, -0.0716947212540753, 0.017041390426387425, 0.3413509582377859, -0.2256452700665304, -0.27270428292842497, 0.006029148107401526, -0.33261464570940874, -0.05565857142210007, 0.16661802712661117, 0.059504387594425... |
1,803.0244 | A shift map with a discontinuous entropy function | Let $f:X\to X$ be a continuous map on a compact metric space with finite
topological entropy. Further, we assume that the entropy map $\mu\mapsto
h_\mu(f)$ is upper semi-continuous. It is well-known that this implies the
continuity of the localized entropy function of a given continuous potential
$\phi:X\to R$. In th... | math.DS | let fxto x be a continuous map on a compact metric space with finite topological entropy further we assume that the entropy map mumapsto h_muf is upper semicontinuous it is wellknown that this implies the continuity of the localized entropy function of a given continuous potential phixto r in this note we show that thi... | [['let', 'fxto', 'x', 'be', 'a', 'continuous', 'map', 'on', 'a', 'compact', 'metric', 'space', 'with', 'finite', 'topological', 'entropy', 'further', 'we', 'assume', 'that', 'the', 'entropy', 'map', 'mumapsto', 'h_muf', 'is', 'upper', 'semicontinuous', 'it', 'is', 'wellknown', 'that', 'this', 'implies', 'the', 'continu... | [-0.16124920755497774, 0.1141429326407061, -0.12789692439731548, 0.04759754934506914, -0.048535824118351396, -0.125312643813562, 0.04916679652788761, 0.36834730149712414, -0.32466781355271285, -0.11352965465365825, 0.06765674504276831, -0.2766015082068572, -0.15669120657681065, 0.18855210352392698, -0.11486873346042227... |
1,803.02441 | Optimal Placement of Relay Nodes in Wireless Sensor Network Using
Artificial Bee Colony Algorithm | Deploying sensor nodes randomly most of the time generates initial
communication hole even in highly dense networks. These communication holes
cannot be totally eliminated even when the deployment is done in a structured
manner. In either case, the resulting inter-node distances may degrade the
performance of the net... | cs.NI | deploying sensor nodes randomly most of the time generates initial communication hole even in highly dense networks these communication holes cannot be totally eliminated even when the deployment is done in a structured manner in either case the resulting internode distances may degrade the performance of the network t... | [['deploying', 'sensor', 'nodes', 'randomly', 'most', 'of', 'the', 'time', 'generates', 'initial', 'communication', 'hole', 'even', 'in', 'highly', 'dense', 'networks', 'these', 'communication', 'holes', 'can', 'not', 'be', 'totally', 'eliminated', 'even', 'when', 'the', 'deployment', 'is', 'done', 'in', 'a', 'structur... | [-0.2465849928298559, 0.040475185632320027, 0.023693173682378933, -0.0031833810156864507, -0.10232538390260243, -0.22858504730086968, 0.11572639950743095, 0.43027353110078775, -0.29417376498560976, -0.332166036348172, 0.060914880062025306, -0.23274080163326943, -0.21209694217378494, 0.08697054666297077, -0.102309335403... |
1,803.02442 | Underwater Optical Wireless Communications, Networking, and
Localization: A Survey | Underwater wireless communications can be carried out through acoustic, radio
frequency (RF), and optical waves. Compared to its bandwidth limited acoustic
and RF counterparts, underwater optical wireless communications (UOWCs) can
support higher data rates at low latency levels. However, severe aquatic
channel condi... | cs.NI | underwater wireless communications can be carried out through acoustic radio frequency rf and optical waves compared to its bandwidth limited acoustic and rf counterparts underwater optical wireless communications uowcs can support higher data rates at low latency levels however severe aquatic channel conditions eg abs... | [['underwater', 'wireless', 'communications', 'can', 'be', 'carried', 'out', 'through', 'acoustic', 'radio', 'frequency', 'rf', 'and', 'optical', 'waves', 'compared', 'to', 'its', 'bandwidth', 'limited', 'acoustic', 'and', 'rf', 'counterparts', 'underwater', 'optical', 'wireless', 'communications', 'uowcs', 'can', 'sup... | [-0.22918051448369214, 0.04202088309902247, 0.05772147481048295, 0.012231085081021864, -0.08230268964825382, -0.23031682718627072, 0.1070278999344497, 0.4594307959611927, -0.28974395421343846, -0.3186817560882236, 0.1623870091273572, -0.27778336026828615, -0.20349319475948566, 0.2228562535556893, -0.08238417889979147, ... |
1,803.02443 | The N-Player Trust Game and its Replicator Dynamics | Trust is a fundamental concept that underpins the coherence and resilience of
social systems and shapes human behavior. Despite the importance of trust as a
social and psychological concept, the concept has not gained much attention
from evolutionary game theorists. In this paper, an N-player trust-based social
dilem... | physics.soc-ph | trust is a fundamental concept that underpins the coherence and resilience of social systems and shapes human behavior despite the importance of trust as a social and psychological concept the concept has not gained much attention from evolutionary game theorists in this paper an nplayer trustbased social dilemma game ... | [['trust', 'is', 'a', 'fundamental', 'concept', 'that', 'underpins', 'the', 'coherence', 'and', 'resilience', 'of', 'social', 'systems', 'and', 'shapes', 'human', 'behavior', 'despite', 'the', 'importance', 'of', 'trust', 'as', 'a', 'social', 'and', 'psychological', 'concept', 'the', 'concept', 'has', 'not', 'gained', ... | [-0.13028669227894638, 0.08178268260724374, -0.11766557163548377, 0.0893095636873185, -0.10224317879768582, -0.156128023027595, 0.10089884395119182, 0.3610655297183216, -0.2397171795495791, -0.28904209808199166, 0.06234640384284979, -0.28361160023069526, -0.22026755812178014, 0.1069905728017543, -0.1513345079854299, -0... |
1,803.02444 | Analytical Modeling of Wi-Fi and LTE-LAA Coexistence: Throughput and
Impact of Energy Detection Threshold | With both small-cell LTE and Wi-Fi networks available as alternatives for
deployment in unlicensed bands (notably 5 GHz), the investigation into their
coexistence is a topic of active interest, primarily driven by industry groups.
3GPP has recently standardized LTE Licensed Assisted Access (LTE-LAA) that
seeks to mak... | cs.NI | with both smallcell lte and wifi networks available as alternatives for deployment in unlicensed bands notably 5 ghz the investigation into their coexistence is a topic of active interest primarily driven by industry groups 3gpp has recently standardized lte licensed assisted access ltelaa that seeks to make lte more c... | [['with', 'both', 'smallcell', 'lte', 'and', 'wifi', 'networks', 'available', 'as', 'alternatives', 'for', 'deployment', 'in', 'unlicensed', 'bands', 'notably', '5', 'ghz', 'the', 'investigation', 'into', 'their', 'coexistence', 'is', 'a', 'topic', 'of', 'active', 'interest', 'primarily', 'driven', 'by', 'industry', 'g... | [-0.1667415406073003, 0.009028478588793748, -0.010741783190839073, 0.04461813250040856, -0.07015995931672683, -0.241961816949169, 0.14389197098095, 0.4065454556776952, -0.2003663110106142, -0.2970971587284278, 0.11911523815617465, -0.24131111766246738, -0.1612378191653519, 0.1803997214820977, -0.06592165988679695, 0.04... |
1,803.02445 | Linear networks based speaker adaptation for speech synthesis | Speaker adaptation methods aim to create fair quality synthesis speech voice
font for target speakers while only limited resources available. Recently, as
deep neural networks based statistical parametric speech synthesis (SPSS)
methods become dominant in SPSS TTS back-end modeling, speaker adaptation under
the neura... | eess.AS cs.SD | speaker adaptation methods aim to create fair quality synthesis speech voice font for target speakers while only limited resources available recently as deep neural networks based statistical parametric speech synthesis spss methods become dominant in spss tts backend modeling speaker adaptation under the neural networ... | [['speaker', 'adaptation', 'methods', 'aim', 'to', 'create', 'fair', 'quality', 'synthesis', 'speech', 'voice', 'font', 'for', 'target', 'speakers', 'while', 'only', 'limited', 'resources', 'available', 'recently', 'as', 'deep', 'neural', 'networks', 'based', 'statistical', 'parametric', 'speech', 'synthesis', 'spss', ... | [-0.005841665537847793, 0.01552863498625168, -0.038754000269308767, 0.06668433169281182, -0.15522778634553086, -0.3070635563302888, 0.03027555359416842, 0.5035652465583211, -0.2044177660339085, -0.31684892882724186, 0.033433150335405414, -0.2569775720440798, -0.1476747367623679, 0.18137776072893436, -0.1660293262935557... |
1,803.02446 | Categorical Mixture Models on VGGNet activations | In this project, I use unsupervised learning techniques in order to cluster a
set of yelp restaurant photos under meaningful topics. In order to do this, I
extract layer activations from a pre-trained implementation of the popular
VGGNet convolutional neural network. First, I explore using LDA with the
activations of... | cs.CV | in this project i use unsupervised learning techniques in order to cluster a set of yelp restaurant photos under meaningful topics in order to do this i extract layer activations from a pretrained implementation of the popular vggnet convolutional neural network first i explore using lda with the activations of convolu... | [['in', 'this', 'project', 'i', 'use', 'unsupervised', 'learning', 'techniques', 'in', 'order', 'to', 'cluster', 'a', 'set', 'of', 'yelp', 'restaurant', 'photos', 'under', 'meaningful', 'topics', 'in', 'order', 'to', 'do', 'this', 'i', 'extract', 'layer', 'activations', 'from', 'a', 'pretrained', 'implementation', 'of'... | [0.050545769958842954, -0.00809143137327638, -0.044244580299538726, 0.08207165303996161, -0.14006849589827078, -0.16651453049618656, 0.06270103611271172, 0.4633814262914933, -0.30427277435650346, -0.33775079485905524, 0.03685916649537677, -0.35769855531574296, -0.19619664158955796, 0.10885857250404489, -0.0909853103818... |
1,803.02447 | Triangulation Tracking of a Radially Propagating MHD Wave in the AIA
1600 Acoustic Power Maps in Active Region 12193 | For decades it has been established that the amount of energy released by
solar flares excites the acoustic oscillations propagating on the surface of
the Sun (Wolff 1972). It is believed that these flares can excite velocity
oscillations in active regions, especially those regions where a higher class
solar flare ha... | astro-ph.SR | for decades it has been established that the amount of energy released by solar flares excites the acoustic oscillations propagating on the surface of the sun wolff 1972 it is believed that these flares can excite velocity oscillations in active regions especially those regions where a higher class solar flare has take... | [['for', 'decades', 'it', 'has', 'been', 'established', 'that', 'the', 'amount', 'of', 'energy', 'released', 'by', 'solar', 'flares', 'excites', 'the', 'acoustic', 'oscillations', 'propagating', 'on', 'the', 'surface', 'of', 'the', 'sun', 'wolff', '1972', 'it', 'is', 'believed', 'that', 'these', 'flares', 'can', 'excit... | [-0.1432794069849132, 0.26297191494432764, -0.03369621734548543, 0.14401397004257888, -0.09478782082719374, -0.07142591929905825, -0.008232361534499518, 0.3292606891620727, -0.2370263336162593, -0.3627598358850394, 0.09393798016494007, -0.29713165495611193, -0.1386425398578424, 0.270033789266433, -0.04622577592298122, ... |
1,803.02448 | Stable solutions of symmetric systems involving hypoelliptic operators | Please see the article for the abstract.
| math.AP math.DG math.FA | please see the article for the abstract | [['please', 'see', 'the', 'article', 'for', 'the', 'abstract']] | [0.010289429287825311, -0.04269717527287347, -0.149080658497821, 0.1898058663521494, -0.2114703401124903, -0.08125704420464379, 0.03760846810681479, 0.26571789596761974, -0.26465263377342907, -0.32290709231581005, 0.11635005314435277, -0.273463994796787, -0.176402587177498, 0.10834350782845702, -0.17535660522324698, -0... |
1,803.02449 | Coupled-cluster treatment of molecular strong-field ionization | Ionization rates and Stark shifts of H$_2$, CO, O$_2$, H$_2$O, and CH$_4$ in
static electric fields have been computed with coupled-cluster methods in a
basis set of atom-centered Gaussian functions with complex-scaled exponent.
Consideration of electron correlation is found to be of great importance even
for a quali... | physics.chem-ph | ionization rates and stark shifts of h_2 co o_2 h_2o and ch_4 in static electric fields have been computed with coupledcluster methods in a basis set of atomcentered gaussian functions with complexscaled exponent consideration of electron correlation is found to be of great importance even for a qualitatively correct d... | [['ionization', 'rates', 'and', 'stark', 'shifts', 'of', 'h_2', 'co', 'o_2', 'h_2o', 'and', 'ch_4', 'in', 'static', 'electric', 'fields', 'have', 'been', 'computed', 'with', 'coupledcluster', 'methods', 'in', 'a', 'basis', 'set', 'of', 'atomcentered', 'gaussian', 'functions', 'with', 'complexscaled', 'exponent', 'consi... | [-0.09718188512269207, 0.10455691470183752, -0.03834100652446029, 0.07448563865581227, 0.06346183213823405, -0.10271381882366083, 0.06170774170107419, 0.40975292938290747, -0.19563272288939115, -0.2935255752170398, -0.049487617207310534, -0.24498962339292962, -0.046304184873338025, 0.17461358521494172, 0.06392828398133... |
1,803.0245 | Semiclassical resolvent estimates for bounded potentials | We study the cut-off resolvent of semiclassical Schr{\"o}dinger operators on
$\mathbb{R}^d$ with bounded compactly supported potentials $V$. We prove that
for real energies $\lambda^2$ in a compact interval in $\mathbb{R}_+$ and for
any smooth cut-off function $\chi$ supported in a ball near the support of the
potent... | math.AP math-ph math.MP math.SP | we study the cutoff resolvent of semiclassical schrodinger operators on mathbbrd with bounded compactly supported potentials v we prove that for real energies lambda2 in a compact interval in mathbbr_ and for any smooth cutoff function chi supported in a ball near the support of the potential v for some constant c0 one... | [['we', 'study', 'the', 'cutoff', 'resolvent', 'of', 'semiclassical', 'schrodinger', 'operators', 'on', 'mathbbrd', 'with', 'bounded', 'compactly', 'supported', 'potentials', 'v', 'we', 'prove', 'that', 'for', 'real', 'energies', 'lambda2', 'in', 'a', 'compact', 'interval', 'in', 'mathbbr_', 'and', 'for', 'any', 'smoot... | [-0.20582003282206185, 0.07185587638552696, -0.03264869790258895, 0.03612556101626836, -0.05910893976714399, -0.1748282846880234, 0.00015624657314915896, 0.32521381717716347, -0.24664970814684853, -0.15415588155513701, 0.08579320007383658, -0.37305455136518695, -0.06790747139089111, 0.20161402209885626, -0.010159123444... |
1,803.02451 | Probing the $N = 14$ subshell closure: $g$ factor of the
$^{26}$Mg(2$^+_1$) state | The first-excited state $g$~factor of $^{26}$Mg has been measured relative to
the $g$ factor of the $^{24}$Mg($2^+_1$) state using the high-velocity
transient-field technique, giving $g=+0.86\pm0.10$. This new measurement is in
strong disagreement with the currently adopted value, but in agreement with the
$sd$-shell... | nucl-ex | the firstexcited state gfactor of 26mg has been measured relative to the g factor of the 24mg2_1 state using the highvelocity transientfield technique giving g086pm010 this new measurement is in strong disagreement with the currently adopted value but in agreement with the sdshell model using the usdb interaction the n... | [['the', 'firstexcited', 'state', 'gfactor', 'of', '26mg', 'has', 'been', 'measured', 'relative', 'to', 'the', 'g', 'factor', 'of', 'the', '24mg2_1', 'state', 'using', 'the', 'highvelocity', 'transientfield', 'technique', 'giving', 'g086pm010', 'this', 'new', 'measurement', 'is', 'in', 'strong', 'disagreement', 'with',... | [-0.07624543810615668, 0.1800358571481329, -0.022990707362590877, 0.06594289106165839, 0.024145328548845945, -0.11881335470657628, 0.07056714340767546, 0.37133418768644333, -0.14861541415086468, -0.32022794701058316, -0.08259371058021144, -0.33782328906057923, 0.038978074534653545, 0.15757096961333608, 0.06890340525287... |
1,803.02452 | Additional clock transitions in neutral ytterbium bring new
possibilities for testing physics beyond the Standard Model | We study the prospects of using transitions from the ytterbium ground state
to metastable states $^3{\rm P}^{\rm o}_2$ at $E=19\,710.388~$cm$^{-1}$ and
$4f^{13}5d6s^2\,(J=2)$ at $E=23\,188.518~$cm$^{-1}$ as clock transitions in an
optical lattice clock. Having more than one clock transition in Yb could
benefit the se... | physics.atom-ph | we study the prospects of using transitions from the ytterbium ground state to metastable states 3rm prm o_2 at e19710388cm1 and 4f135d6s2j2 at e23188518cm1 as clock transitions in an optical lattice clock having more than one clock transition in yb could benefit the search for new physics beyond the standard model via... | [['we', 'study', 'the', 'prospects', 'of', 'using', 'transitions', 'from', 'the', 'ytterbium', 'ground', 'state', 'to', 'metastable', 'states', '3rm', 'prm', 'o_2', 'at', 'e19710388cm1', 'and', '4f135d6s2j2', 'at', 'e23188518cm1', 'as', 'clock', 'transitions', 'in', 'an', 'optical', 'lattice', 'clock', 'having', 'more'... | [-0.11314286430256547, 0.21558332181740572, -0.010920929063747569, 0.048759784955508645, 0.019253839905245033, -0.12814323747591153, 0.13791991099885598, 0.3700851501851547, -0.2406114223753897, -0.2816348983111178, 0.06784410457263088, -0.28523525007530987, -0.05195616874503108, 0.13521949551068246, 0.0592295813442366... |
1,803.02453 | A Reductions Approach to Fair Classification | We present a systematic approach for achieving fairness in a binary
classification setting. While we focus on two well-known quantitative
definitions of fairness, our approach encompasses many other previously studied
definitions as special cases. The key idea is to reduce fair classification to
a sequence of cost-se... | cs.LG | we present a systematic approach for achieving fairness in a binary classification setting while we focus on two wellknown quantitative definitions of fairness our approach encompasses many other previously studied definitions as special cases the key idea is to reduce fair classification to a sequence of costsensitive... | [['we', 'present', 'a', 'systematic', 'approach', 'for', 'achieving', 'fairness', 'in', 'a', 'binary', 'classification', 'setting', 'while', 'we', 'focus', 'on', 'two', 'wellknown', 'quantitative', 'definitions', 'of', 'fairness', 'our', 'approach', 'encompasses', 'many', 'other', 'previously', 'studied', 'definitions'... | [-0.08078907779417932, -0.05354116981228193, -0.06824933327152394, 0.08983902802598702, -0.09116174504257894, -0.18241039893958563, 0.10913877093116753, 0.41484873885444057, -0.24951327890933803, -0.32110431956728763, 0.09011411457201272, -0.27156619504724705, -0.125531660412283, 0.2410626171461748, -0.1506949287771325... |
1,803.02454 | Energy Harvesting with a Liquid-Metal Microfluidic Influence Machine | We describe and demonstrate a new energy harvesting technology based on a
microfluidic realization of a Wimshurst influence machine. The prototype device
converts the mechanical energy of a pressure-driven flow into electrical
energy, using a multiphase system composed of droplets of liquid mercury
surrounded by insu... | physics.app-ph | we describe and demonstrate a new energy harvesting technology based on a microfluidic realization of a wimshurst influence machine the prototype device converts the mechanical energy of a pressuredriven flow into electrical energy using a multiphase system composed of droplets of liquid mercury surrounded by insulatin... | [['we', 'describe', 'and', 'demonstrate', 'a', 'new', 'energy', 'harvesting', 'technology', 'based', 'on', 'a', 'microfluidic', 'realization', 'of', 'a', 'wimshurst', 'influence', 'machine', 'the', 'prototype', 'device', 'converts', 'the', 'mechanical', 'energy', 'of', 'a', 'pressuredriven', 'flow', 'into', 'electrical... | [-0.13394981951901822, 0.16259475497229556, -0.0369377848991592, -0.03007529758698573, -0.05183489970596773, -0.149853889579286, 0.07135787160701251, 0.3603395156362759, -0.26915211528207045, -0.36774146970627564, 0.03807652749653374, -0.2522665636547442, -0.11096309339295009, 0.2547153926321438, -0.05155304280841457, ... |
1,803.02455 | Exciton-polaron spectral structures in two dimensional hybrid
lead-halide perovskites | Owing to both electronic and dielectric confinement effects, two-dimensional
organic-inorganic hybrid perovskites sustain strongly bound excitons at room
temperature. Here, we demonstrate that there are non-negligible contributions
to the excitonic correlations that are specific to the lattice structure and
its polar... | cond-mat.mtrl-sci physics.chem-ph | owing to both electronic and dielectric confinement effects twodimensional organicinorganic hybrid perovskites sustain strongly bound excitons at room temperature here we demonstrate that there are nonnegligible contributions to the excitonic correlations that are specific to the lattice structure and its polar fluctua... | [['owing', 'to', 'both', 'electronic', 'and', 'dielectric', 'confinement', 'effects', 'twodimensional', 'organicinorganic', 'hybrid', 'perovskites', 'sustain', 'strongly', 'bound', 'excitons', 'at', 'room', 'temperature', 'here', 'we', 'demonstrate', 'that', 'there', 'are', 'nonnegligible', 'contributions', 'to', 'the'... | [-0.1376741646756799, 0.18357977549598184, -0.04418770483044802, 0.05422086162919489, -0.017446665488675517, -0.13388970896086227, 0.08848171813249495, 0.4236361408992758, -0.2525497666800266, -0.2762999364684494, -0.04803587515024269, -0.29665233932857243, -0.2011963148592567, 0.1439668173439004, 0.048244171172567886,... |
1,803.02456 | Observation and uses of position-space Bloch oscillations in an
ultracold gas | We report the direct observation and characterization of position-space Bloch
oscillations using an ultracold gas in a tilted optical lattice. While Bloch
oscillations in momentum space are a common feature of optical lattice
experiments, the real-space center-of-mass dynamics are typically too small to
resolve. Tuni... | cond-mat.quant-gas physics.atom-ph | we report the direct observation and characterization of positionspace bloch oscillations using an ultracold gas in a tilted optical lattice while bloch oscillations in momentum space are a common feature of optical lattice experiments the realspace centerofmass dynamics are typically too small to resolve tuning into t... | [['we', 'report', 'the', 'direct', 'observation', 'and', 'characterization', 'of', 'positionspace', 'bloch', 'oscillations', 'using', 'an', 'ultracold', 'gas', 'in', 'a', 'tilted', 'optical', 'lattice', 'while', 'bloch', 'oscillations', 'in', 'momentum', 'space', 'are', 'a', 'common', 'feature', 'of', 'optical', 'latti... | [-0.1929616515135142, 0.22292034913116368, -0.0569676629303453, 0.01459230065990526, -0.06642959068457667, -0.115737363577892, 0.09430054412223399, 0.41904482698211304, -0.30253000045911627, -0.26330138846802026, 0.05284306752593973, -0.2380017823754595, -0.1014621187825329, 0.23904661290311757, 0.038839552755682516, 0... |
1,803.02457 | Characterization and Performance of the Cananea Near-infrared Camera
(CANICA) | We present details of characterization and imaging performance of the Cananea
Near-infrared camera (CANICA) at the 2.1m telescope of the Guillermo Haro
Astrophysical Observatory (OAGH) located in Cananea, Sonora, Mexico. CANICA has
a HAWAII array with a HgCdTe detector of 1024 x 1024 pixels covering a field of
view o... | astro-ph.IM | we present details of characterization and imaging performance of the cananea nearinfrared camera canica at the 21m telescope of the guillermo haro astrophysical observatory oagh located in cananea sonora mexico canica has a hawaii array with a hgcdte detector of 1024 x 1024 pixels covering a field of view of 55 x 55 a... | [['we', 'present', 'details', 'of', 'characterization', 'and', 'imaging', 'performance', 'of', 'the', 'cananea', 'nearinfrared', 'camera', 'canica', 'at', 'the', '21m', 'telescope', 'of', 'the', 'guillermo', 'haro', 'astrophysical', 'observatory', 'oagh', 'located', 'in', 'cananea', 'sonora', 'mexico', 'canica', 'has',... | [-0.1134263968431971, 0.09047161151918874, -0.04681521566378234, 0.010654533015045707, -0.010371915435963223, -0.12728136654625832, 0.02409027156174042, 0.3857742603692525, -0.14877088032091773, -0.43141953371913294, 0.11811455045683959, -0.3525768775879493, -0.005022451402355899, 0.2018894954334136, -0.060372519257416... |
1,803.02458 | Robust Multiple Kernel k-means Clustering using Min-Max Optimization | Multiple kernel learning is a type of multiview learning that combines
different data modalities by capturing view-specific patterns using kernels.
Although supervised multiple kernel learning has been extensively studied,
until recently, only a few unsupervised approaches have been proposed. In the
meanwhile, advers... | cs.LG | multiple kernel learning is a type of multiview learning that combines different data modalities by capturing viewspecific patterns using kernels although supervised multiple kernel learning has been extensively studied until recently only a few unsupervised approaches have been proposed in the meanwhile adversarial le... | [['multiple', 'kernel', 'learning', 'is', 'a', 'type', 'of', 'multiview', 'learning', 'that', 'combines', 'different', 'data', 'modalities', 'by', 'capturing', 'viewspecific', 'patterns', 'using', 'kernels', 'although', 'supervised', 'multiple', 'kernel', 'learning', 'has', 'been', 'extensively', 'studied', 'until', 'r... | [-0.026986578618089764, -0.03844613692585806, -0.10472564124425904, 0.09271231062119939, -0.10799488388485393, -0.18588368694140203, -0.005662170040314315, 0.46292302146798275, -0.25195413905251873, -0.32239168509840965, 0.07122995118964259, -0.2850047389421958, -0.24925862383122857, 0.1913902238113144, -0.169286677047... |
1,803.02459 | Complex Hyperbolic Geometry and Hilbert Spaces with the Complete Pick
Property | Suppose $H$ is a finite dimensional reproducing kernel Hilbert space of
functions on $X.$ If $H$ has the complete Pick property then there is an
isometric map, $\Phi,$ from $X,$ with the metric induced by $H,$ into complex
hyperbolic space, $\mathbb{CH}^{n},$ with its pseudohyperbolic metric. We
investigate the relat... | math.FA | suppose h is a finite dimensional reproducing kernel hilbert space of functions on x if h has the complete pick property then there is an isometric map phi from x with the metric induced by h into complex hyperbolic space mathbbchn with its pseudohyperbolic metric we investigate the relationships between the geometry o... | [['suppose', 'h', 'is', 'a', 'finite', 'dimensional', 'reproducing', 'kernel', 'hilbert', 'space', 'of', 'functions', 'on', 'x', 'if', 'h', 'has', 'the', 'complete', 'pick', 'property', 'then', 'there', 'is', 'an', 'isometric', 'map', 'phi', 'from', 'x', 'with', 'the', 'metric', 'induced', 'by', 'h', 'into', 'complex',... | [-0.09710388070743647, 0.1188977113799865, -0.08758045492868405, 0.02993267649799236, -0.0793536486744415, -0.12367903335689334, -0.01662243902501359, 0.4143764766922686, -0.3435979574569501, -0.1627023511537118, 0.06764648625539849, -0.311573392158607, -0.1607581978169037, 0.1398376179568004, -0.05443280354666058, -0.... |
1,803.0246 | Quantum Circuit Design for Objective Function Maximization in Gate-Model
Quantum Computers | Gate-model quantum computers provide an experimentally implementable
architecture for near term quantum computations. To design a reduced quantum
circuit that can simulate a high complexity reference quantum circuit, an
optimization should be taken on the number of input quantum states, on the
unitary operations of t... | quant-ph cs.IT math.IT | gatemodel quantum computers provide an experimentally implementable architecture for near term quantum computations to design a reduced quantum circuit that can simulate a high complexity reference quantum circuit an optimization should be taken on the number of input quantum states on the unitary operations of the qua... | [['gatemodel', 'quantum', 'computers', 'provide', 'an', 'experimentally', 'implementable', 'architecture', 'for', 'near', 'term', 'quantum', 'computations', 'to', 'design', 'a', 'reduced', 'quantum', 'circuit', 'that', 'can', 'simulate', 'a', 'high', 'complexity', 'reference', 'quantum', 'circuit', 'an', 'optimization'... | [-0.1456210682634264, 0.0901196789439483, -0.07585624531946249, 0.05467948888027523, -0.0444292769042982, -0.21532815448784579, 0.05091387698582063, 0.36706582800381715, -0.3357462565932009, -0.338626643953224, 0.07505073931469168, -0.20554079938059053, -0.16495486193000236, 0.2511574810474283, -0.08832505957689137, 0.... |
1,803.02461 | Subgradient methods for sharp weakly convex functions | Subgradient methods converge linearly on a convex function that grows sharply
away from its solution set. In this work, we show that the same is true for
sharp functions that are only weakly convex, provided that the subgradient
methods are initialized within a fixed tube around the solution set. A variety
of statist... | math.OC | subgradient methods converge linearly on a convex function that grows sharply away from its solution set in this work we show that the same is true for sharp functions that are only weakly convex provided that the subgradient methods are initialized within a fixed tube around the solution set a variety of statistical a... | [['subgradient', 'methods', 'converge', 'linearly', 'on', 'a', 'convex', 'function', 'that', 'grows', 'sharply', 'away', 'from', 'its', 'solution', 'set', 'in', 'this', 'work', 'we', 'show', 'that', 'the', 'same', 'is', 'true', 'for', 'sharp', 'functions', 'that', 'are', 'only', 'weakly', 'convex', 'provided', 'that', ... | [-0.05358532493030935, 0.030733442686573423, -0.09495905483367317, 0.05316434689030766, -0.057142950569731045, -0.2092166877718586, 0.04933305861277863, 0.4518179339591903, -0.3100592639212581, -0.23539258977586422, 0.1558993983745688, -0.2871905793294762, -0.16842548823162837, 0.2417561662256379, -0.12093920981972431,... |
1,803.02462 | Wavefunctions for a Class of Branes in Three-space | Wavefunctions are proposed for a class of Lagrangian branes in three
complex-dimensional space. The branes are asymptotic to Legendrian surfaces of
genus g. The expansion of these wavefunctions in appropriate coordinates
conjecturally encodes all-genus open Gromov-Witten invariants, i.e. the free
energy of the topolo... | hep-th math.AG math.SG | wavefunctions are proposed for a class of lagrangian branes in three complexdimensional space the branes are asymptotic to legendrian surfaces of genus g the expansion of these wavefunctions in appropriate coordinates conjecturally encodes allgenus open gromovwitten invariants ie the free energy of the topological open... | [['wavefunctions', 'are', 'proposed', 'for', 'a', 'class', 'of', 'lagrangian', 'branes', 'in', 'three', 'complexdimensional', 'space', 'the', 'branes', 'are', 'asymptotic', 'to', 'legendrian', 'surfaces', 'of', 'genus', 'g', 'the', 'expansion', 'of', 'these', 'wavefunctions', 'in', 'appropriate', 'coordinates', 'conjec... | [-0.1715582425805873, 0.10343078226516289, -0.12188915595678347, 0.1347043431497046, -0.14278236259706317, -0.18074769283910946, -0.017200824503587293, 0.269049896539322, -0.2434458558796905, -0.2993652133271098, 0.019316945595866334, -0.2948086651108627, -0.14019837259714094, 0.1628555128350854, -0.18598638702283746, ... |
1,803.02463 | Higgs boson pair production at NNLO with top quark mass effects | We consider QCD radiative corrections to Higgs boson pair production through
gluon fusion in proton collisions. We combine the exact next-to-leading order
(NLO) contribution, which features two-loop virtual amplitudes with the full
dependence on the top quark mass $M_t$, with the next-to-next-to-leading order
(NNLO) ... | hep-ph | we consider qcd radiative corrections to higgs boson pair production through gluon fusion in proton collisions we combine the exact nexttoleading order nlo contribution which features twoloop virtual amplitudes with the full dependence on the top quark mass m_t with the nexttonexttoleading order nnlo corrections comput... | [['we', 'consider', 'qcd', 'radiative', 'corrections', 'to', 'higgs', 'boson', 'pair', 'production', 'through', 'gluon', 'fusion', 'in', 'proton', 'collisions', 'we', 'combine', 'the', 'exact', 'nexttoleading', 'order', 'nlo', 'contribution', 'which', 'features', 'twoloop', 'virtual', 'amplitudes', 'with', 'the', 'full... | [-0.01844105544043895, 0.14049584896380038, -0.08940114043486704, 0.1675338128879679, -0.025934787307941944, -0.05625646494475089, 0.020249156117420262, 0.3683770021426073, -0.181071346205759, -0.3113166608096918, 0.012212309465973462, -0.386044583535202, 0.035378825842469395, 0.12710513433023374, 0.061120605611774535,... |
1,803.02464 | The first obstructions to enhancing a triangulated category | In this paper we relate triangulated category structures to the cohomology of
small categories and define initial obstructions to the existence of an
algebraic or topological enhancement. We show that these obstructions do not
vanish in an example of triangulated category without models. We also obtain
cohomological ... | math.KT math.AT math.CT | in this paper we relate triangulated category structures to the cohomology of small categories and define initial obstructions to the existence of an algebraic or topological enhancement we show that these obstructions do not vanish in an example of triangulated category without models we also obtain cohomological char... | [['in', 'this', 'paper', 'we', 'relate', 'triangulated', 'category', 'structures', 'to', 'the', 'cohomology', 'of', 'small', 'categories', 'and', 'define', 'initial', 'obstructions', 'to', 'the', 'existence', 'of', 'an', 'algebraic', 'or', 'topological', 'enhancement', 'we', 'show', 'that', 'these', 'obstructions', 'do... | [-0.18146550873802467, 0.00029426406359892677, -0.10785349128259854, 0.14011614860077812, -0.11601073989136652, -0.12011756742881104, -0.05255064260510897, 0.40442093949426305, -0.4170463282614946, -0.2706066890683195, 0.06293051260184836, -0.15872508695518428, -0.18150710071945056, 0.11360892018260942, -0.285895450616... |
1,803.02465 | Anomalous DC Hall response in noncentrosymmetric tilted Weyl semimetals | Weyl nodes come in pairs of opposite chirality. For broken time reversal
symmetry (TR) they are displaced in momentum space by $\bf{Q}$ and the
anomalous DC Hall conductivity $\sigma_{xy}$ is proportional to $\bf{Q}$ at
charge neutrality. For finite doping there are additive corrections to
$\sigma_{xy}$ which depend ... | cond-mat.str-el cond-mat.mes-hall | weyl nodes come in pairs of opposite chirality for broken time reversal symmetry tr they are displaced in momentum space by bfq and the anomalous dc hall conductivity sigma_xy is proportional to bfq at charge neutrality for finite doping there are additive corrections to sigma_xy which depend on the chemical potential ... | [['weyl', 'nodes', 'come', 'in', 'pairs', 'of', 'opposite', 'chirality', 'for', 'broken', 'time', 'reversal', 'symmetry', 'tr', 'they', 'are', 'displaced', 'in', 'momentum', 'space', 'by', 'bfq', 'and', 'the', 'anomalous', 'dc', 'hall', 'conductivity', 'sigma_xy', 'is', 'proportional', 'to', 'bfq', 'at', 'charge', 'neu... | [-0.17525082006885886, 0.2149564217926136, -0.024759080950076683, 0.021720177425786552, -0.09865236241897249, -0.18600931416519664, 0.06175967858342284, 0.377866639652186, -0.30042813815214114, -0.24486102149445527, 0.0334852153307175, -0.31432329195862013, -0.08352560815260265, 0.13577981501573114, -0.0263848797052321... |
1,803.02466 | Improved implementation of reflection operators | Quantum algorithms for diverse problems, including search and optimization
problems, require the implementation of a reflection operator over a target
state. Commonly, such reflections are approximately implemented using phase
estimation. Here we use a linear combination of unitaries and a version of
amplitude amplif... | quant-ph | quantum algorithms for diverse problems including search and optimization problems require the implementation of a reflection operator over a target state commonly such reflections are approximately implemented using phase estimation here we use a linear combination of unitaries and a version of amplitude amplification... | [['quantum', 'algorithms', 'for', 'diverse', 'problems', 'including', 'search', 'and', 'optimization', 'problems', 'require', 'the', 'implementation', 'of', 'a', 'reflection', 'operator', 'over', 'a', 'target', 'state', 'commonly', 'such', 'reflections', 'are', 'approximately', 'implemented', 'using', 'phase', 'estimat... | [-0.09404481415028679, 0.11732933667371981, -0.0883115786178638, 0.024164588474973915, -0.050820132510105524, -0.13508233661086508, 0.08493439050307344, 0.384774421021098, -0.24747930838639945, -0.3006600640711624, 0.13941928815819282, -0.2416480076728297, -0.15513732248937578, 0.25940575072404426, -0.06688680285791475... |
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