id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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1,801.03069 | Open-Access Full-Duplex Wireless in the ORBIT Testbed | In order to support experimentation with full-duplex (FD) wireless, we
recently integrated an open-access FD transceiver in the ORBIT testbed. In this
report, we present the design and implementation of the FD transceiver and
interfaces, and provide examples and guidelines for experimentation. In
particular, an ORBIT... | cs.NI eess.SP | in order to support experimentation with fullduplex fd wireless we recently integrated an openaccess fd transceiver in the orbit testbed in this report we present the design and implementation of the fd transceiver and interfaces and provide examples and guidelines for experimentation in particular an orbit node with a... | [['in', 'order', 'to', 'support', 'experimentation', 'with', 'fullduplex', 'fd', 'wireless', 'we', 'recently', 'integrated', 'an', 'openaccess', 'fd', 'transceiver', 'in', 'the', 'orbit', 'testbed', 'in', 'this', 'report', 'we', 'present', 'the', 'design', 'and', 'implementation', 'of', 'the', 'fd', 'transceiver', 'and... | [-0.23790575451821036, -0.010315192812873946, 0.02898803490060794, -0.05318900222722087, -0.08126574010541072, -0.27858949944530204, 0.05484857640370632, 0.47979888303464724, -0.16551825071130938, -0.25187139793688174, 0.09896210938562415, -0.2392263433194566, -0.20469748386170103, 0.2526747993240722, -0.07002089992224... |
1,801.0307 | On Frobenius semisimplicity in Hida families | Let $p\geq 5$ be a prime and $\ell\neq p$ be a prime not dividing the tame
level of a $p$-ordinary Hida family. We prove that the actions of the Frobenius
element at $\ell$ on the Galois representations attached to almost all
arithmetic specializations are semisimple and non-scalar. If $k_f$ denotes the
weight of a c... | math.NT | let pgeq 5 be a prime and ellneq p be a prime not dividing the tame level of a pordinary hida family we prove that the actions of the frobenius element at ell on the galois representations attached to almost all arithmetic specializations are semisimple and nonscalar if k_f denotes the weight of a cusp form fz sum_ngeq... | [['let', 'pgeq', '5', 'be', 'a', 'prime', 'and', 'ellneq', 'p', 'be', 'a', 'prime', 'not', 'dividing', 'the', 'tame', 'level', 'of', 'a', 'pordinary', 'hida', 'family', 'we', 'prove', 'that', 'the', 'actions', 'of', 'the', 'frobenius', 'element', 'at', 'ell', 'on', 'the', 'galois', 'representations', 'attached', 'to', ... | [-0.24901361435870914, 0.1342883438584121, -0.09612861677237293, 0.06242392177775721, -0.05972955409327851, -0.21369962899890893, -0.01950521879719899, 0.2700276953770834, -0.3466506952091175, -0.21240057615453706, 0.029510691252482287, -0.3278026533888324, -0.10688971552778692, 0.19410544569220614, -0.0547264270922716... |
1,801.03071 | Bell monogamy relations in arbitrary qubit networks | Characterizing trade-offs between simultaneous violations of multiple Bell
inequalities in a large network of qubits is computationally demanding. We
propose a graph-theoretic approach to efficiently produce Bell monogamy
relations in arbitrary arrangements of qubits. All the relations obtained for
bipartite Bell ine... | quant-ph | characterizing tradeoffs between simultaneous violations of multiple bell inequalities in a large network of qubits is computationally demanding we propose a graphtheoretic approach to efficiently produce bell monogamy relations in arbitrary arrangements of qubits all the relations obtained for bipartite bell inequalit... | [['characterizing', 'tradeoffs', 'between', 'simultaneous', 'violations', 'of', 'multiple', 'bell', 'inequalities', 'in', 'a', 'large', 'network', 'of', 'qubits', 'is', 'computationally', 'demanding', 'we', 'propose', 'a', 'graphtheoretic', 'approach', 'to', 'efficiently', 'produce', 'bell', 'monogamy', 'relations', 'i... | [-0.16936939787774463, 0.12775724057185775, -0.05148816839209758, 0.17608194842614466, -0.05972030710836407, -0.3006457276690829, 0.06749684772027346, 0.350588072091341, -0.23871692824036472, -0.32246284299374867, 0.01037278044350387, -0.2906899567800186, -0.16000126365846276, 0.2511700655547126, -0.08286184363047748, ... |
1,801.03072 | A one-phase interior point method for nonconvex optimization | The work of Wachter and Biegler suggests that infeasible-start interior point
methods (IPMs) developed for linear programming cannot be adapted to nonlinear
optimization without significant modification, i.e., using a two-phase or
penalty method. We propose an IPM that, by careful initialization and updates
of the sl... | math.OC | the work of wachter and biegler suggests that infeasiblestart interior point methods ipms developed for linear programming cannot be adapted to nonlinear optimization without significant modification ie using a twophase or penalty method we propose an ipm that by careful initialization and updates of the slack variable... | [['the', 'work', 'of', 'wachter', 'and', 'biegler', 'suggests', 'that', 'infeasiblestart', 'interior', 'point', 'methods', 'ipms', 'developed', 'for', 'linear', 'programming', 'can', 'not', 'be', 'adapted', 'to', 'nonlinear', 'optimization', 'without', 'significant', 'modification', 'ie', 'using', 'a', 'twophase', 'or'... | [-0.06047550363098664, -0.0608908190419659, -0.09142327224279975, 0.06746322048003281, -0.1032544436404504, -0.1960559296814433, 0.08195367805008967, 0.37247671831556295, -0.2897467058023448, -0.3304027782473292, 0.14770744721046145, -0.2336438572067902, -0.14570252331400133, 0.24330503163517014, -0.1038888465980957, 0... |
1,801.03073 | XYZ - SU3 Breakings from Laplace Sum Rule at Higher Orders: Summary | This talk reviews and summarizes some of our results in [1] on XYZ- SU3
Breakings obtained from QCD Laplace Sum Rules (LSR) at next-to-next-leading
order (N2LO) of perturbative (PT) theory and including next-to-leading order
(NLO) SU3 breaking corrections and leading order (LO) contributions of
dimensions d< (6 - 8) ... | hep-ph hep-ex hep-lat | this talk reviews and summarizes some of our results in 1 on xyz su3 breakings obtained from qcd laplace sum rules lsr at nexttonextleading order n2lo of perturbative pt theory and including nexttoleading order nlo su3 breaking corrections and leading order lo contributions of dimensions d 6 8 nonperturbative condensat... | [['this', 'talk', 'reviews', 'and', 'summarizes', 'some', 'of', 'our', 'results', 'in', '1', 'on', 'xyz', 'su3', 'breakings', 'obtained', 'from', 'qcd', 'laplace', 'sum', 'rules', 'lsr', 'at', 'nexttonextleading', 'order', 'n2lo', 'of', 'perturbative', 'pt', 'theory', 'and', 'including', 'nexttoleading', 'order', 'nlo'... | [-0.11316428213523558, 0.2249792796326801, -0.03507885491618743, 0.0999326609639236, -0.005477996421261476, -0.11790048439915364, 0.0607983546770321, 0.35527187806482496, -0.15171779447163528, -0.2710874209753596, 0.0569776220085959, -0.38599746159922615, -0.027575543687607233, 0.0798280651251284, 0.06868099604840748, ... |
1,801.03074 | Game of Drones - Detecting Streamed POI from Encrypted FPV Channel | Drones have created a new threat to people's privacy. We are now in an era in
which anyone with a drone equipped with a video camera can use it to invade a
subject's privacy by streaming the subject in his/her private space over an
encrypted first person view (FPV) channel. Although many methods have been
suggested t... | cs.CR | drones have created a new threat to peoples privacy we are now in an era in which anyone with a drone equipped with a video camera can use it to invade a subjects privacy by streaming the subject in hisher private space over an encrypted first person view fpv channel although many methods have been suggested to detect ... | [['drones', 'have', 'created', 'a', 'new', 'threat', 'to', 'peoples', 'privacy', 'we', 'are', 'now', 'in', 'an', 'era', 'in', 'which', 'anyone', 'with', 'a', 'drone', 'equipped', 'with', 'a', 'video', 'camera', 'can', 'use', 'it', 'to', 'invade', 'a', 'subjects', 'privacy', 'by', 'streaming', 'the', 'subject', 'in', 'h... | [-0.12319250073735237, 0.054316029124452346, -0.1062549106918324, 0.050689656766558955, -0.1230620687789242, -0.19383060089451498, 0.06927185692979064, 0.39817397789195624, -0.2761918405199479, -0.2889186809640447, 0.1184268530506863, -0.317618956361939, -0.14219080880214807, 0.18264637899119407, -0.18296897581601806, ... |
1,801.03075 | Rayleigh fractionation in high-Rayleigh-number solutal convection in
porous media | We study the fractionation of two components between a well-mixed gas and a
saturated convecting porous layer. Motivated by geological carbon dioxide
(CO$_2$) storage we assume that convection is driven only by the dissolved
concentration of the first component, while the second acts as a tracer with
increased diffus... | physics.flu-dyn | we study the fractionation of two components between a wellmixed gas and a saturated convecting porous layer motivated by geological carbon dioxide co_2 storage we assume that convection is driven only by the dissolved concentration of the first component while the second acts as a tracer with increased diffusivity dir... | [['we', 'study', 'the', 'fractionation', 'of', 'two', 'components', 'between', 'a', 'wellmixed', 'gas', 'and', 'a', 'saturated', 'convecting', 'porous', 'layer', 'motivated', 'by', 'geological', 'carbon', 'dioxide', 'co_2', 'storage', 'we', 'assume', 'that', 'convection', 'is', 'driven', 'only', 'by', 'the', 'dissolved... | [-0.10292466948665077, 0.22265964808212893, 0.009873111840457685, -0.0049480390104074635, 0.0514490416829264, -0.10465254124794757, 0.0303971043532534, 0.36197534089968086, -0.2777076448644361, -0.2765329479363807, 0.06580032290019576, -0.2728144287221855, -0.06315666359038122, 0.13698505274951459, -0.00825530953645225... |
1,801.03076 | Unidirectional spin density wave state in metallic (Sr1-xLax)2IrO4 | Materials that exhibit both strong spin orbit coupling and electron
correlation effects are predicted to host numerous new electronic states. One
prominent example is the Jeff =1/2 Mott state in Sr2IrO4, where introducing
carriers is predicted to manifest high temperature superconductivity analogous
to the S=1/2 Mott... | cond-mat.mtrl-sci cond-mat.str-el | materials that exhibit both strong spin orbit coupling and electron correlation effects are predicted to host numerous new electronic states one prominent example is the jeff 12 mott state in sr2iro4 where introducing carriers is predicted to manifest high temperature superconductivity analogous to the s12 mott state o... | [['materials', 'that', 'exhibit', 'both', 'strong', 'spin', 'orbit', 'coupling', 'and', 'electron', 'correlation', 'effects', 'are', 'predicted', 'to', 'host', 'numerous', 'new', 'electronic', 'states', 'one', 'prominent', 'example', 'is', 'the', 'jeff', '12', 'mott', 'state', 'in', 'sr2iro4', 'where', 'introducing', '... | [-0.23755504900352067, 0.2583771659852976, -0.00499433910805457, 0.11342046923400997, -0.05805203143894772, -0.17738440488121354, 0.11386093344139372, 0.3761584366540481, -0.22010585130036078, -0.2518800831393608, -0.05253393917841424, -0.3844477510276632, -0.1348669106631396, 0.1048971555467645, 0.10457214655279613, 0... |
1,801.03077 | The clustering of the SDSS-IV extended Baryon Oscillation Spectroscopic
Survey DR14 quasar sample: Anisotropic Baryon Acoustic Oscillations
measurements in Fourier-space with optimal redshift weights | We present a measurement of the anisotropic and isotropic Baryon Acoustic
Oscillations (BAO) from the extended Baryon Oscillation Spectroscopic Survey
Data Release 14 quasar sample with optimal redshift weights. Applying the
redshift weights improves the constraint on the BAO dilation parameter
$\alpha(z_{\rm eff})$ ... | astro-ph.CO | we present a measurement of the anisotropic and isotropic baryon acoustic oscillations bao from the extended baryon oscillation spectroscopic survey data release 14 quasar sample with optimal redshift weights applying the redshift weights improves the constraint on the bao dilation parameter alphaz_rm eff by 17 we reco... | [['we', 'present', 'a', 'measurement', 'of', 'the', 'anisotropic', 'and', 'isotropic', 'baryon', 'acoustic', 'oscillations', 'bao', 'from', 'the', 'extended', 'baryon', 'oscillation', 'spectroscopic', 'survey', 'data', 'release', '14', 'quasar', 'sample', 'with', 'optimal', 'redshift', 'weights', 'applying', 'the', 're... | [-0.06865569644582432, 0.10239226831676992, -0.02721748487218409, 0.06168505916925701, -0.18920914603497935, -0.025975907460559864, 0.10666859947692452, 0.32719161520032464, -0.1887634326577992, -0.31451680891316486, 0.05046894002982692, -0.37187498132068963, 0.006828682673339908, 0.1977954784760604, 0.0440600981205903... |
1,801.03078 | A converse to Schreier's index-rank formula | In "Subgroups of free profinite groups and large subfields of Q" (Israel J.
Math. 39 (1981), no. 1-2, pages 25-45; MR 617288) A. Lubotzky and L. van den
Dries raise the question whether a finitely generated, residually finite group
is necessarily free if the rank function on its subgroups of finite index
satisfies Sc... | math.GR | in subgroups of free profinite groups and large subfields of q israel j math 39 1981 no 12 pages 2545 mr 617288 a lubotzky and l van den dries raise the question whether a finitely generated residually finite group is necessarily free if the rank function on its subgroups of finite index satisfies schreiers wellknown i... | [['in', 'subgroups', 'of', 'free', 'profinite', 'groups', 'and', 'large', 'subfields', 'of', 'q', 'israel', 'j', 'math', '39', '1981', 'no', '12', 'pages', '2545', 'mr', '617288', 'a', 'lubotzky', 'and', 'l', 'van', 'den', 'dries', 'raise', 'the', 'question', 'whether', 'a', 'finitely', 'generated', 'residually', 'fini... | [-0.11404140563830337, 0.09312603513334328, -0.09385637252373581, 0.10471720562905985, -0.10905723366886377, -0.17374696713832624, 0.0748297224054113, 0.31106004742794036, -0.27726922895848516, -0.3255288807397827, 0.05877941589866904, -0.30037254669723357, -0.09250749849734154, 0.1646372997301056, -0.2144451316822558,... |
1,801.03079 | Asymmetry Hurts: Private Information Retrieval Under Asymmetric Traffic
Constraints | We consider the classical setting of private information retrieval (PIR) of a
single message (file) out of $M$ messages from $N$ distributed databases under
the new constraint of \emph{asymmetric traffic} from databases. In this
problem, the \emph{ratios between the traffic} from the databases are
constrained, i.e., ... | cs.IT cs.CR math.IT | we consider the classical setting of private information retrieval pir of a single message file out of m messages from n distributed databases under the new constraint of emphasymmetric traffic from databases in this problem the emphratios between the traffic from the databases are constrained ie the ratio of the lengt... | [['we', 'consider', 'the', 'classical', 'setting', 'of', 'private', 'information', 'retrieval', 'pir', 'of', 'a', 'single', 'message', 'file', 'out', 'of', 'm', 'messages', 'from', 'n', 'distributed', 'databases', 'under', 'the', 'new', 'constraint', 'of', 'emphasymmetric', 'traffic', 'from', 'databases', 'in', 'this',... | [-0.18851452481415537, 0.0516608032077137, -0.041853841113754446, 0.04957690647648027, -0.05573042768933293, -0.1887113999722836, 0.1342736508987016, 0.29158459464708963, -0.29221166819954913, -0.3057736300527015, 0.10476841152283467, -0.3072541184557809, -0.09430102965794504, 0.1807067611735935, -0.09518559037345566, ... |
1,801.0308 | Quadrature Compound: An approximating family of distributions | Compound distributions allow construction of a rich set of distributions.
Typically they involve an intractable integral. Here we use a quadrature
approximation to that integral to define the quadrature compound family.
Special care is taken that this approximation is suitable for computation of
gradients with respec... | stat.CO | compound distributions allow construction of a rich set of distributions typically they involve an intractable integral here we use a quadrature approximation to that integral to define the quadrature compound family special care is taken that this approximation is suitable for computation of gradients with respect to ... | [['compound', 'distributions', 'allow', 'construction', 'of', 'a', 'rich', 'set', 'of', 'distributions', 'typically', 'they', 'involve', 'an', 'intractable', 'integral', 'here', 'we', 'use', 'a', 'quadrature', 'approximation', 'to', 'that', 'integral', 'to', 'define', 'the', 'quadrature', 'compound', 'family', 'special... | [-0.07397397565232082, 0.09024686100165127, -0.1690825930203904, 0.09747939809881659, -0.1218831826361235, -0.08822383947924457, 0.06305164463225413, 0.43096064057582145, -0.30396620709533717, -0.2676994106293106, 0.07179778817914087, -0.2323133143532852, -0.12059865292500366, 0.17481813644990324, -0.09075373823897363,... |
1,801.03081 | A proof of Bertrand's theorem using the theory of isochronous potentials | We give an alternative proof for the celebrated Bertrand's theorem as a
corollary of the isochronicity of a certain family of centers.
| math.DS | we give an alternative proof for the celebrated bertrands theorem as a corollary of the isochronicity of a certain family of centers | [['we', 'give', 'an', 'alternative', 'proof', 'for', 'the', 'celebrated', 'bertrands', 'theorem', 'as', 'a', 'corollary', 'of', 'the', 'isochronicity', 'of', 'a', 'certain', 'family', 'of', 'centers']] | [-0.1519583266503601, -0.012765653065633325, -0.17598327875814654, 0.10845198431475596, -0.06936039445413784, -0.10086305028843609, 0.07978497648780997, 0.20644379915161568, -0.2778983603824269, -0.2595296632498503, 0.11747783208689229, -0.21249053271656687, -0.1443870980504223, 0.2892819395796819, -0.15511748609556394... |
1,801.03082 | Rational points and prime values of polynomials in moderately many
variables | We derive the Hasse principle and weak approximation for pencils of certain
varieties in the spirit of work by Colliot-Th\'el\`ene,Sansuc and
Harpaz-Skorobogatov-Wittenberg. Our varieties are defined through polynomials
in many variables and part of our work is devoted to establishing Schinzel's
hypothesis for polyno... | math.NT | we derive the hasse principle and weak approximation for pencils of certain varieties in the spirit of work by colliotthelenesansuc and harpazskorobogatovwittenberg our varieties are defined through polynomials in many variables and part of our work is devoted to establishing schinzels hypothesis for polynomials of thi... | [['we', 'derive', 'the', 'hasse', 'principle', 'and', 'weak', 'approximation', 'for', 'pencils', 'of', 'certain', 'varieties', 'in', 'the', 'spirit', 'of', 'work', 'by', 'colliotthelenesansuc', 'and', 'harpazskorobogatovwittenberg', 'our', 'varieties', 'are', 'defined', 'through', 'polynomials', 'in', 'many', 'variable... | [-0.16001386207838852, 0.02024591065003603, -0.08635195178822393, 0.08516483466540065, -0.0671955425380951, -0.09494836165436676, 0.05877166220120021, 0.26320352055841967, -0.28831213063205635, -0.3026117860516977, 0.09622413743553417, -0.22223893820884683, -0.1684569115262656, 0.23058486795718117, -0.14642482412358124... |
1,801.03083 | Smoluchowski's discrete coagulation equation with forcing | In this article we study an extension of Smoluchowski's discrete coagulation
equation, where particle in- and output takes place. This model is frequently
used to describe aggregation processes in combination with sedimentation of
clusters. More precisely, we show that the evolution equation is well-posed for
a large... | math-ph math.AP math.MP | in this article we study an extension of smoluchowskis discrete coagulation equation where particle in and output takes place this model is frequently used to describe aggregation processes in combination with sedimentation of clusters more precisely we show that the evolution equation is wellposed for a large class of... | [['in', 'this', 'article', 'we', 'study', 'an', 'extension', 'of', 'smoluchowskis', 'discrete', 'coagulation', 'equation', 'where', 'particle', 'in', 'and', 'output', 'takes', 'place', 'this', 'model', 'is', 'frequently', 'used', 'to', 'describe', 'aggregation', 'processes', 'in', 'combination', 'with', 'sedimentation'... | [-0.07450937188475075, 0.0880465851346977, -0.11359130038549722, 0.08607610850300215, -0.04265912679094774, -0.09517047156379381, 0.0031757219458776937, 0.33696569466986986, -0.3058457050849743, -0.2060681018813313, 0.12265871252637663, -0.22773209899145214, -0.1288558438544079, 0.15737839772136103, -0.0514294853982150... |
1,801.03084 | A Langevin approach to multi-scale modeling | In plasmas, distribution functions often demonstrate long anisotropic tails
or otherwise significant deviations from local Maxwellians. The tails,
especially if they are pulled out from the bulk, pose a serious challenge for
numerical simulations as resolving both the bulk and the tail on the same mesh
is often chall... | physics.plasm-ph | in plasmas distribution functions often demonstrate long anisotropic tails or otherwise significant deviations from local maxwellians the tails especially if they are pulled out from the bulk pose a serious challenge for numerical simulations as resolving both the bulk and the tail on the same mesh is often challenging... | [['in', 'plasmas', 'distribution', 'functions', 'often', 'demonstrate', 'long', 'anisotropic', 'tails', 'or', 'otherwise', 'significant', 'deviations', 'from', 'local', 'maxwellians', 'the', 'tails', 'especially', 'if', 'they', 'are', 'pulled', 'out', 'from', 'the', 'bulk', 'pose', 'a', 'serious', 'challenge', 'for', '... | [-0.07458790984565587, 0.08616807521521873, -0.18058085055296305, 0.0947762699694841, -0.058891118556847644, -0.11737539452495496, 0.013913050479157854, 0.36196947416794895, -0.287816452721741, -0.30920216793101796, 0.07015524996002076, -0.2624860804025354, -0.10349356987158567, 0.15540311850918695, -0.0338344252385322... |
1,801.03085 | The Mean Ultraviolet Spectrum of a Representative Sample of Faint z~3
Lyman Alpha Emitters | We discuss the rest-frame ultraviolet emission line spectra of a large (~100)
sample of low luminosity redshift z~3.1 Lyman alpha emitters (LAEs) drawn from
a Subaru imaging survey in the SSA22 survey field. Our earlier work based on
smaller samples indicated that such sources have high [OIII]/[OII] line ratios
possi... | astro-ph.GA | we discuss the restframe ultraviolet emission line spectra of a large 100 sample of low luminosity redshift z31 lyman alpha emitters laes drawn from a subaru imaging survey in the ssa22 survey field our earlier work based on smaller samples indicated that such sources have high oiiioii line ratios possibly arising from... | [['we', 'discuss', 'the', 'restframe', 'ultraviolet', 'emission', 'line', 'spectra', 'of', 'a', 'large', '100', 'sample', 'of', 'low', 'luminosity', 'redshift', 'z31', 'lyman', 'alpha', 'emitters', 'laes', 'drawn', 'from', 'a', 'subaru', 'imaging', 'survey', 'in', 'the', 'ssa22', 'survey', 'field', 'our', 'earlier', 'w... | [0.010404462168603582, 0.09929127701944127, -0.008227579732454877, 0.14159210938131772, -0.047310495154453895, -0.07645713692207963, 0.043855855734347624, 0.5265584545428151, -0.053447018396361054, -0.36033806390221323, -0.01152464360426608, -0.3373624043149018, 0.01118359360361455, 0.20902508382710652, 0.0193346720209... |
1,801.03086 | Precision determination of absolute neutron flux | A technique for establishing the total neutron rate of a highly-collimated
monochromatic cold neutron beam was demonstrated using a method of an
alpha-gamma counter. The method involves only the counting of measured rates
and is independent of neutron cross sections, decay chain branching ratios, and
neutron beam ene... | physics.ins-det nucl-ex | a technique for establishing the total neutron rate of a highlycollimated monochromatic cold neutron beam was demonstrated using a method of an alphagamma counter the method involves only the counting of measured rates and is independent of neutron cross sections decay chain branching ratios and neutron beam energy for... | [['a', 'technique', 'for', 'establishing', 'the', 'total', 'neutron', 'rate', 'of', 'a', 'highlycollimated', 'monochromatic', 'cold', 'neutron', 'beam', 'was', 'demonstrated', 'using', 'a', 'method', 'of', 'an', 'alphagamma', 'counter', 'the', 'method', 'involves', 'only', 'the', 'counting', 'of', 'measured', 'rates', ... | [-0.03912001288446608, 0.19307454154240195, -0.10672309225439043, 0.05156174317285742, -0.023368545400444418, -0.08420472357101971, 0.09614135088960883, 0.36974297773153725, -0.19428526714656744, -0.3262468064710012, 0.012549489906118453, -0.33941831766708713, 0.03211892511488101, 0.27820173663127684, 0.001206708963170... |
1,801.03087 | Design Studies for a TPC Readout Plane Using Zigzag Patterns with
Multistage GEM Detectors | A new Time Projection Chamber (TPC) is currently under development for the
sPHENIX experiment at RHIC. The TPC will be read out using multistage GEM
detectors on each end and will be divided into approximately 40 pad layers in
radius. Each pad layer is required to provide a spatial resolution of ~250
microns, which m... | physics.ins-det | a new time projection chamber tpc is currently under development for the sphenix experiment at rhic the tpc will be read out using multistage gem detectors on each end and will be divided into approximately 40 pad layers in radius each pad layer is required to provide a spatial resolution of 250 microns which must be a... | [['a', 'new', 'time', 'projection', 'chamber', 'tpc', 'is', 'currently', 'under', 'development', 'for', 'the', 'sphenix', 'experiment', 'at', 'rhic', 'the', 'tpc', 'will', 'be', 'read', 'out', 'using', 'multistage', 'gem', 'detectors', 'on', 'each', 'end', 'and', 'will', 'be', 'divided', 'into', 'approximately', '40', ... | [-0.07746625719038526, 0.09445922931941236, -0.06842344441410418, -0.018969937519658905, -0.02834927666705875, -0.17576422380815296, 0.0022153010638939633, 0.4289301718900723, -0.23610524263721508, -0.3393583385161852, 0.10843372017544659, -0.3081489309816128, -0.008219610576522969, 0.2096698708282631, -0.0610797772631... |
1,801.03088 | Construction and Performance of the Barrel Electromagnetic Calorimeter
for the GlueX Experiment | The barrel calorimeter is part of the new spectrometer installed in Hall D at
Jefferson Lab for the GlueX experiment. The calorimeter was installed in 2013,
commissioned in 2014 and has been operating routinely since early 2015. The
detector configuration, associated Monte Carlo simulations, calibration and
operation... | physics.ins-det nucl-ex | the barrel calorimeter is part of the new spectrometer installed in hall d at jefferson lab for the gluex experiment the calorimeter was installed in 2013 commissioned in 2014 and has been operating routinely since early 2015 the detector configuration associated monte carlo simulations calibration and operational perf... | [['the', 'barrel', 'calorimeter', 'is', 'part', 'of', 'the', 'new', 'spectrometer', 'installed', 'in', 'hall', 'd', 'at', 'jefferson', 'lab', 'for', 'the', 'gluex', 'experiment', 'the', 'calorimeter', 'was', 'installed', 'in', '2013', 'commissioned', 'in', '2014', 'and', 'has', 'been', 'operating', 'routinely', 'since'... | [-0.06779650881274625, 0.21741764370871838, -0.09338146013608419, -0.004393998599140147, 0.002033567240158486, -0.12240206023006765, -0.017260444297747642, 0.3922547994907079, -0.16257561865597042, -0.41266990072895277, 0.0550371556042634, -0.3526657715948775, 0.039834272787841254, 0.2113184978113358, 0.027334556232618... |
1,801.03089 | Prospects for indirect detection of frozen-in dark matter | We study observational consequences arising from dark matter (DM) of
non-thermal origin, produced by dark freeze-out from a hidden sector heat bath.
We assume this heat bath was populated by feebly-coupled mediator particles,
produced via a Higgs portal interaction with the Standard Model (SM). The dark
sector then a... | hep-ph astro-ph.CO astro-ph.HE | we study observational consequences arising from dark matter dm of nonthermal origin produced by dark freezeout from a hidden sector heat bath we assume this heat bath was populated by feeblycoupled mediator particles produced via a higgs portal interaction with the standard model sm the dark sector then attained inter... | [['we', 'study', 'observational', 'consequences', 'arising', 'from', 'dark', 'matter', 'dm', 'of', 'nonthermal', 'origin', 'produced', 'by', 'dark', 'freezeout', 'from', 'a', 'hidden', 'sector', 'heat', 'bath', 'we', 'assume', 'this', 'heat', 'bath', 'was', 'populated', 'by', 'feeblycoupled', 'mediator', 'particles', '... | [-0.11964707967574494, 0.2803807918501731, -0.10899710374472377, 0.14765108185999382, -0.1001805598095346, -0.1687041486461217, 0.051448084852801494, 0.2927393155315748, -0.27153577836893067, -0.3391965612804947, -0.020512171215019546, -0.3027510637477043, -0.004935547852745423, 0.1294822116951064, 0.1107717781739596, ... |
1,801.0309 | Measurement-based universal blind quantum computation with minor
resources | Blind quantum computation (BQC) enables a client with less quantum
computational ability to delegate her quantum computation to a server with
strong quantum computational power while preserving the client's privacy.
Generally, many-qubit entangled states are often used to complete BQC tasks.
But for a large-scale ent... | quant-ph | blind quantum computation bqc enables a client with less quantum computational ability to delegate her quantum computation to a server with strong quantum computational power while preserving the clients privacy generally manyqubit entangled states are often used to complete bqc tasks but for a largescale entangled sta... | [['blind', 'quantum', 'computation', 'bqc', 'enables', 'a', 'client', 'with', 'less', 'quantum', 'computational', 'ability', 'to', 'delegate', 'her', 'quantum', 'computation', 'to', 'a', 'server', 'with', 'strong', 'quantum', 'computational', 'power', 'while', 'preserving', 'the', 'clients', 'privacy', 'generally', 'ma... | [-0.16203261654092266, 0.11439537243837103, -0.08255528457693243, 0.019739847792755668, -0.06931721486569363, -0.3245760931524125, 0.1357765137900988, 0.3578852214375321, -0.2432949854867785, -0.31483919921388126, 0.07282395739012103, -0.256480223062978, -0.05587610368716663, 0.18441953314159407, -0.1451267959337387, 0... |
1,801.03091 | A time-dependent Schr\"odinger equation for molecular core-hole dynamics | X-ray spectroscopy is an important tool for the investigation of matter. X
rays primarily interact with inner-shell electrons creating core (inner-shell)
holes that will decay on the time scale of attoseconds to few femtoseconds
through electron relaxations involving the emission of a photon or an electron.
The adven... | physics.atom-ph quant-ph | xray spectroscopy is an important tool for the investigation of matter x rays primarily interact with innershell electrons creating core innershell holes that will decay on the time scale of attoseconds to few femtoseconds through electron relaxations involving the emission of a photon or an electron the advent of femt... | [['xray', 'spectroscopy', 'is', 'an', 'important', 'tool', 'for', 'the', 'investigation', 'of', 'matter', 'x', 'rays', 'primarily', 'interact', 'with', 'innershell', 'electrons', 'creating', 'core', 'innershell', 'holes', 'that', 'will', 'decay', 'on', 'the', 'time', 'scale', 'of', 'attoseconds', 'to', 'few', 'femtosec... | [-0.06704389694917562, 0.20418751333134674, -0.06948904946831794, 0.12002932355269501, -0.04641253827139735, -0.11446335364398065, 0.042701978049269104, 0.4357764278458239, -0.2598419299109333, -0.3046319794867204, 0.048518991700959684, -0.3313670436899852, -0.017499019004452717, 0.26612924377971875, 0.0903386853972514... |
1,801.03092 | Ultrafast x-ray-induced nuclear dynamics in diatomic molecules using
femtosecond x-ray/x-ray pump-probe spectroscopy | The capability of generating two intense, femtosecond x-ray pulses with
controlled time delay opens the possibility of performing time-resolved
experiments for x-ray induced phenomena. We have applied this capability to
study the photoinduced dynamics in diatomic molecules. In molecules composed of
low-Z elements, \t... | physics.atom-ph quant-ph | the capability of generating two intense femtosecond xray pulses with controlled time delay opens the possibility of performing timeresolved experiments for xray induced phenomena we have applied this capability to study the photoinduced dynamics in diatomic molecules in molecules composed of lowz elements textitkshell... | [['the', 'capability', 'of', 'generating', 'two', 'intense', 'femtosecond', 'xray', 'pulses', 'with', 'controlled', 'time', 'delay', 'opens', 'the', 'possibility', 'of', 'performing', 'timeresolved', 'experiments', 'for', 'xray', 'induced', 'phenomena', 'we', 'have', 'applied', 'this', 'capability', 'to', 'study', 'the... | [-0.07507058999475998, 0.2412312615910589, -0.05297473506574091, 0.08417878339380361, 0.06717733898879709, -0.09578168035258312, 0.055292260970265884, 0.42538860660247707, -0.25810242078795625, -0.2880710038243214, -0.04172404601326766, -0.3243582979360646, -0.006484890315757209, 0.1812723469190501, 0.10516807189009883... |
1,801.03093 | End-of-Use Core Triage in Extreme Scenarios Based on a Threshold
Approach | Remanufacturing is a significant factor in securing sustainability through a
circular economy. Sorting plays a significant role in remanufacturing
pre-processing inspections. Its significance can increase when remanufacturing
facilities encounter extreme situations, such as abnormally huge core arrivals.
Our main obj... | stat.AP | remanufacturing is a significant factor in securing sustainability through a circular economy sorting plays a significant role in remanufacturing preprocessing inspections its significance can increase when remanufacturing facilities encounter extreme situations such as abnormally huge core arrivals our main objective ... | [['remanufacturing', 'is', 'a', 'significant', 'factor', 'in', 'securing', 'sustainability', 'through', 'a', 'circular', 'economy', 'sorting', 'plays', 'a', 'significant', 'role', 'in', 'remanufacturing', 'preprocessing', 'inspections', 'its', 'significance', 'can', 'increase', 'when', 'remanufacturing', 'facilities', ... | [-0.05724513127676679, 0.0685812957404602, -0.09236929501371441, 0.11818087102592094, -0.08562322584096738, -0.15802440575156618, 0.07970533829851909, 0.4018228851679352, -0.21991687845347518, -0.32740103895454087, 0.13956024816414248, -0.27280414932137054, -0.12283639919789602, 0.1873475651595793, -0.13687928021061427... |
1,801.03094 | Long-term radio and X-ray evolution of the tidal disruption event
ASASSN-14li | We report on late time radio and X-ray observations of the tidal disruption
event candidate ASASSN-14li, covering the first 1000 days of the decay phase.
For the first $\sim200$ days the radio and X-ray emission fade in concert. This
phase is better fit by an exponential decay at X-ray wavelengths, while the
radio em... | astro-ph.HE | we report on late time radio and xray observations of the tidal disruption event candidate asassn14li covering the first 1000 days of the decay phase for the first sim200 days the radio and xray emission fade in concert this phase is better fit by an exponential decay at xray wavelengths while the radio emission is wel... | [['we', 'report', 'on', 'late', 'time', 'radio', 'and', 'xray', 'observations', 'of', 'the', 'tidal', 'disruption', 'event', 'candidate', 'asassn14li', 'covering', 'the', 'first', '1000', 'days', 'of', 'the', 'decay', 'phase', 'for', 'the', 'first', 'sim200', 'days', 'the', 'radio', 'and', 'xray', 'emission', 'fade', '... | [-0.06564495670507946, 0.16492095791229233, -0.06985962966396271, 0.12357124369705359, -0.10263013199690486, -0.10453640411952106, 0.05868540098384509, 0.4511894723349858, -0.2115223534011697, -0.30822350189555436, 0.14560534678584308, -0.3132129380904624, -0.026032792602959293, 0.19774302167681287, 0.03159259222530122... |
1,801.03095 | Evidence for feedback and stellar-dynamically regulated bursty star
cluster formation: the case of the Orion Nebula Cluster | (abridged) A scenario for the formation of multiple co-eval populations
separated in age by about 1 Myr in very young clusters (VYCs, ages less than 10
Myr) and with masses in the range 600-20000 Msun is outlined. It rests upon a
converging inflow of molecular gas building up a first population of pre-main
sequence s... | astro-ph.GA | abridged a scenario for the formation of multiple coeval populations separated in age by about 1 myr in very young clusters vycs ages less than 10 myr and with masses in the range 60020000 msun is outlined it rests upon a converging inflow of molecular gas building up a first population of premain sequence stars the as... | [['abridged', 'a', 'scenario', 'for', 'the', 'formation', 'of', 'multiple', 'coeval', 'populations', 'separated', 'in', 'age', 'by', 'about', '1', 'myr', 'in', 'very', 'young', 'clusters', 'vycs', 'ages', 'less', 'than', '10', 'myr', 'and', 'with', 'masses', 'in', 'the', 'range', '60020000', 'msun', 'is', 'outlined', '... | [-0.06373682907866954, 0.15957668678396764, -0.06381313864817369, 0.09008886165718329, -0.06103713723132387, -0.04563789275776157, 0.07792617641868727, 0.4090984882102074, -0.20192719391528882, -0.34468338577140706, 0.0663935386937559, -0.22820553632781787, -0.0087151538646853, 0.17020902214868577, -0.04775172875459105... |
1,801.03096 | Accretion of satellites onto central galaxies in clusters: merger mass
ratios and orbital parameters | We study the statistical properties of mergers between central and satellite
galaxies in galaxy clusters in the redshift range $0<z<1$, using a sample of
dark-matter only cosmological N-body simulations from Le SBARBINE dataset.
Using a spherical overdensity algorithm to identify dark-matter haloes, we
construct halo... | astro-ph.GA | we study the statistical properties of mergers between central and satellite galaxies in galaxy clusters in the redshift range 0z1 using a sample of darkmatter only cosmological nbody simulations from le sbarbine dataset using a spherical overdensity algorithm to identify darkmatter haloes we construct halo merger tree... | [['we', 'study', 'the', 'statistical', 'properties', 'of', 'mergers', 'between', 'central', 'and', 'satellite', 'galaxies', 'in', 'galaxy', 'clusters', 'in', 'the', 'redshift', 'range', '0z1', 'using', 'a', 'sample', 'of', 'darkmatter', 'only', 'cosmological', 'nbody', 'simulations', 'from', 'le', 'sbarbine', 'dataset'... | [-0.09895884991722899, 0.09769798812825077, -0.11951659974996194, 0.140719908575799, -0.09935484568268294, 0.00046357372533141944, 0.0147239848835549, 0.36832761362408445, -0.1122754993023894, -0.3814627026343563, 0.0017014276121093037, -0.3007578879103221, 0.05192956696798016, 0.22528834038894274, 0.030001815132739768... |
1,801.03097 | Stellar Streams Discovered in the Dark Energy Survey | We perform a search for stellar streams around the Milky Way using the first
three years of multi-band optical imaging data from the Dark Energy Survey
(DES). We use DES data covering $\sim 5000$ sq. deg. to a depth of $g > 23.5$
with a relative photometric calibration uncertainty of $< 1 \%$. This data set
yields un... | astro-ph.GA astro-ph.CO | we perform a search for stellar streams around the milky way using the first three years of multiband optical imaging data from the dark energy survey des we use des data covering sim 5000 sq deg to a depth of g 235 with a relative photometric calibration uncertainty of 1 this data set yields unprecedented sensitivity ... | [['we', 'perform', 'a', 'search', 'for', 'stellar', 'streams', 'around', 'the', 'milky', 'way', 'using', 'the', 'first', 'three', 'years', 'of', 'multiband', 'optical', 'imaging', 'data', 'from', 'the', 'dark', 'energy', 'survey', 'des', 'we', 'use', 'des', 'data', 'covering', 'sim', '5000', 'sq', 'deg', 'to', 'a', 'de... | [-0.06328653710826292, 0.03766856632105011, -0.12171683715763543, 0.1142793260076891, -0.1513842215433931, -0.0015892983513134244, 0.04625645856603782, 0.39182658218242955, -0.17060532822145924, -0.44749350155975703, 0.022084401089562087, -0.3034112550966252, -0.03470432804691383, 0.2647389622633881, -0.046718767707120... |
1,801.03098 | $\mathcal{N}=2$ supersymmetry and anisotropic scale invariance | We find a class of scale-anomaly-free $\mathcal{N}=2$ supersymmetric quantum
systems with non-vanishing potential terms where space and time scale with
distinct exponents. Our results generalise the known case of the supersymmetric
inverse square potential to a larger class of scaling symmetries.
| hep-th math-ph math.MP quant-ph | we find a class of scaleanomalyfree mathcaln2 supersymmetric quantum systems with nonvanishing potential terms where space and time scale with distinct exponents our results generalise the known case of the supersymmetric inverse square potential to a larger class of scaling symmetries | [['we', 'find', 'a', 'class', 'of', 'scaleanomalyfree', 'mathcaln2', 'supersymmetric', 'quantum', 'systems', 'with', 'nonvanishing', 'potential', 'terms', 'where', 'space', 'and', 'time', 'scale', 'with', 'distinct', 'exponents', 'our', 'results', 'generalise', 'the', 'known', 'case', 'of', 'the', 'supersymmetric', 'in... | [-0.11035177176818252, 0.16277913477970288, 0.01599284140393138, 0.07120093069970608, -0.053964164096396414, -0.16333588886191136, -0.04112531950813718, 0.26056422194524204, -0.21161434887908398, -0.28833169012796134, 0.08563263303367422, -0.2893074280349538, -0.20462127411738038, 0.17614246609155088, -0.00654302479233... |
1,801.03099 | Predicting the binary black hole population of the Milky Way with
cosmological simulations | Binary black holes are the primary endpoint of massive stellar evolution.
Their properties provide a unique opportunity to constrain binary evolution,
which is still poorly understood. In this paper, we predict the inventory of
binary black holes and their merger products in/around the Milky Way, and
detail their mai... | astro-ph.GA | binary black holes are the primary endpoint of massive stellar evolution their properties provide a unique opportunity to constrain binary evolution which is still poorly understood in this paper we predict the inventory of binary black holes and their merger products inaround the milky way and detail their main proper... | [['binary', 'black', 'holes', 'are', 'the', 'primary', 'endpoint', 'of', 'massive', 'stellar', 'evolution', 'their', 'properties', 'provide', 'a', 'unique', 'opportunity', 'to', 'constrain', 'binary', 'evolution', 'which', 'is', 'still', 'poorly', 'understood', 'in', 'this', 'paper', 'we', 'predict', 'the', 'inventory'... | [-0.09325956824119203, 0.09499670129508013, -0.05417708569765091, 0.15384238367900252, -0.11226409729290754, -0.038940864351112395, 0.037081572447437795, 0.37695543592795727, -0.13350256839953362, -0.389848217042163, 0.05349084991426207, -0.32131969306990504, -0.040352120181778445, 0.21052971230703407, -0.0216222677004... |
1,801.031 | Multi-timescale X-ray reverberation mapping of accreting black holes | Accreting black holes show characteristic reflection features in their X-ray
spectrum, including an iron K$\alpha$ line, resulting from hard X-ray continuum
photons illuminating the accretion disk. The reverberation lag resulting from
the path length difference between direct and reflected emission provides a
powerfu... | astro-ph.HE | accreting black holes show characteristic reflection features in their xray spectrum including an iron kalpha line resulting from hard xray continuum photons illuminating the accretion disk the reverberation lag resulting from the path length difference between direct and reflected emission provides a powerful tool to ... | [['accreting', 'black', 'holes', 'show', 'characteristic', 'reflection', 'features', 'in', 'their', 'xray', 'spectrum', 'including', 'an', 'iron', 'kalpha', 'line', 'resulting', 'from', 'hard', 'xray', 'continuum', 'photons', 'illuminating', 'the', 'accretion', 'disk', 'the', 'reverberation', 'lag', 'resulting', 'from'... | [-0.05391762221232057, 0.06627534969101867, -0.09634758579027322, 0.1366559822133018, -0.12741496878158715, -0.09511403045824005, 0.05214731544566651, 0.45503334127883943, -0.22848309125751257, -0.31164634289013016, 0.08913846611252262, -0.2911424964355926, -0.06507567411288619, 0.248123211014188, -0.008733149032211967... |
1,801.03101 | Many-Body Spectral Reflection Symmetry and Protected
Infinite-Temperature Degeneracy | Protected zero modes in quantum physics traditionally arise in the context of
ground states of many-body Hamiltonians. Here we study the case where zero
modes exist in the center of a reflection-symmetric many-body spectrum, giving
rise to the notion of a protected "infinite-temperature" degeneracy. For a
certain cla... | cond-mat.str-el cond-mat.quant-gas cond-mat.stat-mech quant-ph | protected zero modes in quantum physics traditionally arise in the context of ground states of manybody hamiltonians here we study the case where zero modes exist in the center of a reflectionsymmetric manybody spectrum giving rise to the notion of a protected infinitetemperature degeneracy for a certain class of nonin... | [['protected', 'zero', 'modes', 'in', 'quantum', 'physics', 'traditionally', 'arise', 'in', 'the', 'context', 'of', 'ground', 'states', 'of', 'manybody', 'hamiltonians', 'here', 'we', 'study', 'the', 'case', 'where', 'zero', 'modes', 'exist', 'in', 'the', 'center', 'of', 'a', 'reflectionsymmetric', 'manybody', 'spectru... | [-0.2118314598659529, 0.2637806729295514, -0.095886123550295, 0.08533018764639667, 0.014362851528345908, -0.17691355094421837, 0.04403589124927415, 0.31565040179436477, -0.26106477896092645, -0.2524036529513312, 0.040386512392679305, -0.3143068791931154, -0.09706143316366828, 0.12824616494299976, 0.016439698972660576, ... |
1,801.03102 | Advanced Environmentally Resistant Lithium Fluoride Mirror Coatings for
the Next-Generation of Broadband Space Observatories | Recent advances in the physical vapor deposition (PVD) of protective fluoride
films have raised the far-ultraviolet (FUV: 912-1600 {\AA}) reflectivity of
aluminum-based mirrors closer to the theoretical limit. The greatest gains, at
more than 20%, have come for lithium fluoride-protected aluminum, which has the
short... | astro-ph.IM | recent advances in the physical vapor deposition pvd of protective fluoride films have raised the farultraviolet fuv 9121600 aa reflectivity of aluminumbased mirrors closer to the theoretical limit the greatest gains at more than 20 have come for lithium fluorideprotected aluminum which has the shortest wavelength cuto... | [['recent', 'advances', 'in', 'the', 'physical', 'vapor', 'deposition', 'pvd', 'of', 'protective', 'fluoride', 'films', 'have', 'raised', 'the', 'farultraviolet', 'fuv', '9121600', 'aa', 'reflectivity', 'of', 'aluminumbased', 'mirrors', 'closer', 'to', 'the', 'theoretical', 'limit', 'the', 'greatest', 'gains', 'at', 'm... | [-0.043264617784805, 0.1545676064424208, -0.04766726795513864, -0.012430562589552895, -0.07572726266688957, -0.13696248300113184, 0.023824989516538397, 0.43589843365974645, -0.2014480865240017, -0.34888104254990737, 0.10774791572726161, -0.32684482426272443, -0.08077348912289987, 0.22092547575863059, -0.126670578589803... |
1,801.03103 | A Candidate $z\sim10$ Galaxy Strongly Lensed into a Spatially Resolved
Arc | The most distant galaxies known are at z~10-11, observed 400-500 Myr after
the Big Bang. The few z~10-11 candidates discovered to date have been
exceptionally small- barely resolved, if at all, by the Hubble Space Telescope.
Here we present the discovery of SPT0615-JD, a fortuitous z~10
(z_phot=9.9+/-0.6) galaxy cand... | astro-ph.GA | the most distant galaxies known are at z1011 observed 400500 myr after the big bang the few z1011 candidates discovered to date have been exceptionally small barely resolved if at all by the hubble space telescope here we present the discovery of spt0615jd a fortuitous z10 z_phot9906 galaxy candidate stretched into an ... | [['the', 'most', 'distant', 'galaxies', 'known', 'are', 'at', 'z1011', 'observed', '400500', 'myr', 'after', 'the', 'big', 'bang', 'the', 'few', 'z1011', 'candidates', 'discovered', 'to', 'date', 'have', 'been', 'exceptionally', 'small', 'barely', 'resolved', 'if', 'at', 'all', 'by', 'the', 'hubble', 'space', 'telescop... | [-0.06143553596145163, 0.09912751905170201, -0.09975263159334039, 0.11086420872015879, -0.14341207550023682, -0.09251647874480114, 0.037089864918380046, 0.42135961557893703, -0.15708206406222114, -0.37672006379095063, 0.07000516431022939, -0.30864641127021364, -0.03041142241563648, 0.20540728798199173, 0.00457953220466... |
1,801.03104 | Physical properties and scaling relations of molecular clouds: the
effect of stellar feedback | Using hydrodynamical simulations of entire galactic discs similar to the
Milky Way, reaching 4.6pc resolution, we study the origins of observed physical
properties of giant molecular clouds (GMCs). We find that efficient stellar
feedback is a necessary ingredient in order to develop a realistic interstellar
medium (I... | astro-ph.GA | using hydrodynamical simulations of entire galactic discs similar to the milky way reaching 46pc resolution we study the origins of observed physical properties of giant molecular clouds gmcs we find that efficient stellar feedback is a necessary ingredient in order to develop a realistic interstellar medium ism leadin... | [['using', 'hydrodynamical', 'simulations', 'of', 'entire', 'galactic', 'discs', 'similar', 'to', 'the', 'milky', 'way', 'reaching', '46pc', 'resolution', 'we', 'study', 'the', 'origins', 'of', 'observed', 'physical', 'properties', 'of', 'giant', 'molecular', 'clouds', 'gmcs', 'we', 'find', 'that', 'efficient', 'stella... | [-0.09884299910857577, 0.1027274172507472, -0.09464258170087955, 0.09926113469723183, -0.04578512329812888, -0.016750591899176222, 0.04000179592269258, 0.42101367168988174, -0.2108187527436722, -0.3569389183872512, -0.013816267472006136, -0.22669399681419217, -0.07929856637057818, 0.16820566721163321, 0.031185760916272... |
1,801.03105 | Full-disc $^{13}$CO(1-0) mapping across nearby galaxies of the EMPIRE
survey and the CO-to-H$_2$ conversion factor | Carbon monoxide (CO) provides crucial information about the molecular gas
properties of galaxies. While $^{12}$CO has been targeted extensively,
isotopologues such as $^{13}$CO have the advantage of being less optically
thick and observations have recently become accessible across full galaxy
discs. We present a comp... | astro-ph.GA | carbon monoxide co provides crucial information about the molecular gas properties of galaxies while 12co has been targeted extensively isotopologues such as 13co have the advantage of being less optically thick and observations have recently become accessible across full galaxy discs we present a comprehensive new dat... | [['carbon', 'monoxide', 'co', 'provides', 'crucial', 'information', 'about', 'the', 'molecular', 'gas', 'properties', 'of', 'galaxies', 'while', '12co', 'has', 'been', 'targeted', 'extensively', 'isotopologues', 'such', 'as', '13co', 'have', 'the', 'advantage', 'of', 'being', 'less', 'optically', 'thick', 'and', 'obser... | [-0.0479246899937349, 0.06378318496451778, -0.027460352180581262, 0.05423339891487232, -0.026423740852711056, -0.033518679007862213, 0.03390449798429635, 0.4332890247842714, -0.15994540888750092, -0.34784685497505785, 0.07563514573240666, -0.28190695404756205, -0.03724823387447439, 0.17153973487959898, 0.00883307368338... |
1,801.03106 | Why informatics and general science need a conjoint basic definition of
information | First the basic definition of information as a selection from a set of
possibilities resp. domain is recalled. This also applies to digital
information. The bits of digital information are parts of number sequences
which represent a selection from a set of possibilities resp. domain. For
faultless conversation sender... | cs.DL | first the basic definition of information as a selection from a set of possibilities resp domain is recalled this also applies to digital information the bits of digital information are parts of number sequences which represent a selection from a set of possibilities resp domain for faultless conversation sender and re... | [['first', 'the', 'basic', 'definition', 'of', 'information', 'as', 'a', 'selection', 'from', 'a', 'set', 'of', 'possibilities', 'resp', 'domain', 'is', 'recalled', 'this', 'also', 'applies', 'to', 'digital', 'information', 'the', 'bits', 'of', 'digital', 'information', 'are', 'parts', 'of', 'number', 'sequences', 'whi... | [-0.12246855025989048, 0.053618627814888846, -0.08942024730586251, 0.06671147955384353, -0.1797788950240835, -0.15609183515973238, 0.08220806343482528, 0.3673344619230044, -0.325950824447312, -0.2953075307918725, 0.13911546921523027, -0.26053423584732077, -0.10201165528705051, 0.16828630618801732, -0.10468486747641091,... |
1,801.03107 | An excess of massive stars in the local 30 Doradus starburst | The 30 Doradus star-forming region in the Large Magellanic Cloud is a nearby
analogue of large star-formation events in the distant Universe. We determine
the recent formation history and the initial mass function (IMF) of massive
stars in 30 Doradus based on spectroscopic observations of 247 stars more
massive than ... | astro-ph.SR astro-ph.GA | the 30 doradus starforming region in the large magellanic cloud is a nearby analogue of large starformation events in the distant universe we determine the recent formation history and the initial mass function imf of massive stars in 30 doradus based on spectroscopic observations of 247 stars more massive than 15 sola... | [['the', '30', 'doradus', 'starforming', 'region', 'in', 'the', 'large', 'magellanic', 'cloud', 'is', 'a', 'nearby', 'analogue', 'of', 'large', 'starformation', 'events', 'in', 'the', 'distant', 'universe', 'we', 'determine', 'the', 'recent', 'formation', 'history', 'and', 'the', 'initial', 'mass', 'function', 'imf', '... | [-0.0675747253647717, 0.15854572565078456, -0.05608458549146895, 0.15032305459252895, -0.08118484179598519, -0.008325183805309038, 0.09476244146317507, 0.37677506027759705, -0.07929981645790085, -0.39478440895116174, 0.001801557890427983, -0.2675732702132216, 0.03193859239644577, 0.210971191855131, -0.06102253323801035... |
1,801.03108 | Enforcing the Courant-Friedrichs-Lewy Condition in Explicitly
Conservative Local Time Stepping Schemes | An optimally efficient explicit numerical scheme for solving fluid dynamics
equations, or any other parabolic or hyperbolic system of partial differential
equations, should allow local regions to advance in time with their own,
locally constrained time steps. However, such a scheme can result in violation
of the Cour... | physics.comp-ph astro-ph.CO astro-ph.GA | an optimally efficient explicit numerical scheme for solving fluid dynamics equations or any other parabolic or hyperbolic system of partial differential equations should allow local regions to advance in time with their own locally constrained time steps however such a scheme can result in violation of the courantfrie... | [['an', 'optimally', 'efficient', 'explicit', 'numerical', 'scheme', 'for', 'solving', 'fluid', 'dynamics', 'equations', 'or', 'any', 'other', 'parabolic', 'or', 'hyperbolic', 'system', 'of', 'partial', 'differential', 'equations', 'should', 'allow', 'local', 'regions', 'to', 'advance', 'in', 'time', 'with', 'their', '... | [-0.17639580121958406, 0.10776979587054654, -0.09909021276138764, 0.05668619168346148, -0.12443843843299622, -0.16842629865737957, 0.09375285452999975, 0.3352845084858732, -0.2849459119120055, -0.3151799186243344, 0.14075124634648173, -0.1836224116193753, -0.08281492298313727, 0.1648269163771522, -0.09661487276576418, ... |
1,801.03109 | An operator-valued Lyapunov theorem | We generalize Lyapunov's convexity theorem for classical (scalar-valued)
measures to quantum (operator-valued) measures. In particular, we show that the
range of a nonatomic quantum probability measure is a weak*-closed convex set
of quantum effects (positive operators bounded above by the identity operator)
under a ... | math.FA quant-ph | we generalize lyapunovs convexity theorem for classical scalarvalued measures to quantum operatorvalued measures in particular we show that the range of a nonatomic quantum probability measure is a weakclosed convex set of quantum effects positive operators bounded above by the identity operator under a sufficient cond... | [['we', 'generalize', 'lyapunovs', 'convexity', 'theorem', 'for', 'classical', 'scalarvalued', 'measures', 'to', 'quantum', 'operatorvalued', 'measures', 'in', 'particular', 'we', 'show', 'that', 'the', 'range', 'of', 'a', 'nonatomic', 'quantum', 'probability', 'measure', 'is', 'a', 'weakclosed', 'convex', 'set', 'of',... | [-0.13109897306409254, 0.13587014690562282, -0.09744247128706306, 0.12314363824008333, -0.07092734337634136, -0.1204731638783649, 0.06124972833460698, 0.30684710982986674, -0.3139820424138859, -0.13229892978204355, 0.1114805955665126, -0.2656823003424271, -0.14078777748089966, 0.2174244472576726, -0.1500372264173723, 0... |
1,801.0311 | QCD thermodynamics from lattice calculations with non-equilibrium
methods: The SU(3) equation of state | A precise lattice determination of the equation of state in SU(3) Yang-Mills
theory is carried out by means of a simulation algorithm, based on Jarzynski's
theorem, that allows one to compute physical quantities in thermodynamic
equilibrium, by driving the field configurations of the system out of
equilibrium. The ph... | hep-lat hep-ph hep-th nucl-th | a precise lattice determination of the equation of state in su3 yangmills theory is carried out by means of a simulation algorithm based on jarzynskis theorem that allows one to compute physical quantities in thermodynamic equilibrium by driving the field configurations of the system out of equilibrium the physical res... | [['a', 'precise', 'lattice', 'determination', 'of', 'the', 'equation', 'of', 'state', 'in', 'su3', 'yangmills', 'theory', 'is', 'carried', 'out', 'by', 'means', 'of', 'a', 'simulation', 'algorithm', 'based', 'on', 'jarzynskis', 'theorem', 'that', 'allows', 'one', 'to', 'compute', 'physical', 'quantities', 'in', 'thermo... | [-0.1078457540255541, 0.10482122304648915, -0.1614787804310599, 0.033074952393793794, -0.021584818045361134, -0.10982949645818459, 0.08866224011636185, 0.33701060460055177, -0.2045011364006072, -0.2887433308966552, 0.08398155026031728, -0.27542928037181336, -0.09352703023218562, 0.19405159682825301, 0.0385910231484501,... |
1,801.03111 | Lambert function methods for laser dynamics with time-delayed feedback | Time-delayed differential equations arise frequently in the study of
nonlinear dynamics of lasers with optical feedback. Traditionally, one has
resorted to numerical methods because the analytical solution of such equations
are intractable. In this manuscript, we show that under some conditions, the
rate equations mo... | physics.optics quant-ph | timedelayed differential equations arise frequently in the study of nonlinear dynamics of lasers with optical feedback traditionally one has resorted to numerical methods because the analytical solution of such equations are intractable in this manuscript we show that under some conditions the rate equations model that... | [['timedelayed', 'differential', 'equations', 'arise', 'frequently', 'in', 'the', 'study', 'of', 'nonlinear', 'dynamics', 'of', 'lasers', 'with', 'optical', 'feedback', 'traditionally', 'one', 'has', 'resorted', 'to', 'numerical', 'methods', 'because', 'the', 'analytical', 'solution', 'of', 'such', 'equations', 'are', ... | [-0.10733825140597678, 0.106262552005736, -0.07694306634226464, 0.03196887930512036, -0.058459183001624684, -0.16614045308118588, 0.009366045083633546, 0.3867863708672891, -0.30871161815703363, -0.25835450327626075, 0.12096725576522208, -0.24371897646565607, -0.18717132857125393, 0.23784023730252357, -0.044815629367065... |
1,801.03112 | Fundamental Solutions and Decay of Fully Non-local Problems | In this paper, we study a fully non-local reaction-diffusion equation which
is non-local both in time and space. We apply subordination principles to
construct the fundamental solutions of this problem, which we use to find a
representation of the mild solutions. Moreover, using techniques of Harmonic
Analysis and Fo... | math.AP | in this paper we study a fully nonlocal reactiondiffusion equation which is nonlocal both in time and space we apply subordination principles to construct the fundamental solutions of this problem which we use to find a representation of the mild solutions moreover using techniques of harmonic analysis and fourier mult... | [['in', 'this', 'paper', 'we', 'study', 'a', 'fully', 'nonlocal', 'reactiondiffusion', 'equation', 'which', 'is', 'nonlocal', 'both', 'in', 'time', 'and', 'space', 'we', 'apply', 'subordination', 'principles', 'to', 'construct', 'the', 'fundamental', 'solutions', 'of', 'this', 'problem', 'which', 'we', 'use', 'to', 'fi... | [-0.09625637972882638, 0.0129392733797431, -0.1337900486153861, 0.08749324156863926, -0.09168433058075606, -0.09164449834885696, 0.02075872938342703, 0.3520037055636446, -0.3250522455200553, -0.20438584235962481, 0.15338240925533075, -0.23407628804755706, -0.20203705417613188, 0.17791419823964436, -0.04745841395730774,... |
1,801.03113 | Influence of image forces on the interlayer exchange interaction in
magnetic tunnel junctions with ferroelectric barrier | We study interlayer exchange interaction in magnetic tunnel junctions with
ferroelectric barrier. We focus on the influence of image forces on the voltage
dependence of the interlayer magnetic interaction (magneto-electric effect).
The influence of the image forces is twofold: 1) they significantly enforce
magneto-el... | cond-mat.mes-hall | we study interlayer exchange interaction in magnetic tunnel junctions with ferroelectric barrier we focus on the influence of image forces on the voltage dependence of the interlayer magnetic interaction magnetoelectric effect the influence of the image forces is twofold 1 they significantly enforce magnetoelectric eff... | [['we', 'study', 'interlayer', 'exchange', 'interaction', 'in', 'magnetic', 'tunnel', 'junctions', 'with', 'ferroelectric', 'barrier', 'we', 'focus', 'on', 'the', 'influence', 'of', 'image', 'forces', 'on', 'the', 'voltage', 'dependence', 'of', 'the', 'interlayer', 'magnetic', 'interaction', 'magnetoelectric', 'effect'... | [-0.26139850232310774, 0.15959822815500246, 0.0028908550214106427, 0.023993803941840797, -0.09718839485282288, -0.14837368472682355, 0.06545190747715253, 0.42558426482785017, -0.31820753202038377, -0.3405032992166908, -0.07756972458927815, -0.3130577926460962, -0.1252788495748563, 0.17400369309309058, 0.064446777248881... |
1,801.03114 | Magneto-electric effect in doped magnetic ferroelectrics | We propose a model of magneto-electric effect in doped magnetic
ferroelectrics. This magneto-electric effect does not involve the spin-orbit
coupling and is based purely on the Coulomb interaction. We calculate magnetic
phase diagram of doped magnetic ferroelectrics. We show that magneto-electric
coupling is pronounc... | cond-mat.mtrl-sci | we propose a model of magnetoelectric effect in doped magnetic ferroelectrics this magnetoelectric effect does not involve the spinorbit coupling and is based purely on the coulomb interaction we calculate magnetic phase diagram of doped magnetic ferroelectrics we show that magnetoelectric coupling is pronounced only f... | [['we', 'propose', 'a', 'model', 'of', 'magnetoelectric', 'effect', 'in', 'doped', 'magnetic', 'ferroelectrics', 'this', 'magnetoelectric', 'effect', 'does', 'not', 'involve', 'the', 'spinorbit', 'coupling', 'and', 'is', 'based', 'purely', 'on', 'the', 'coulomb', 'interaction', 'we', 'calculate', 'magnetic', 'phase', '... | [-0.2555637283020475, 0.22616654388499288, -0.01082902249953385, -0.013040499043588139, -0.17337340931931322, -0.1525513870390446, 0.0679472219787559, 0.47057979106065934, -0.20741597073299162, -0.26202988406915345, -0.08881969164711621, -0.28760630742050286, -0.20054430059377062, 0.16704716442121464, 0.051795635445650... |
1,801.03115 | Topological Aspect of Graphene Patchwork with Regular Arrays of Nano
Holes | Triangular and honeycomb lattices are dual to each other -- if we puncture
holes into a featureless plane in a regular triangular alignment, the remaining
body looks like a honeycomb lattice, and vice versa, if the holes are in a
regular honeycomb alignment, the remaining body has a feature of triangular
lattice. In ... | cond-mat.mes-hall | triangular and honeycomb lattices are dual to each other if we puncture holes into a featureless plane in a regular triangular alignment the remaining body looks like a honeycomb lattice and vice versa if the holes are in a regular honeycomb alignment the remaining body has a feature of triangular lattice in this work ... | [['triangular', 'and', 'honeycomb', 'lattices', 'are', 'dual', 'to', 'each', 'other', 'if', 'we', 'puncture', 'holes', 'into', 'a', 'featureless', 'plane', 'in', 'a', 'regular', 'triangular', 'alignment', 'the', 'remaining', 'body', 'looks', 'like', 'a', 'honeycomb', 'lattice', 'and', 'vice', 'versa', 'if', 'the', 'hol... | [-0.19718121239750447, 0.19295056759677473, -0.018878213306771047, 0.011439465694394716, -0.06656855544888804, -0.18471159103998466, 0.029090203069256547, 0.4349015559058023, -0.2688415076412685, -0.21408821508300171, 0.06164845536666321, -0.35347664923866906, -0.13909671778637397, 0.1254597421841625, -0.00078279266275... |
1,801.03116 | Existence and continuity of solution trajectories of generalized
equations with application in electronics | We consider a special form of parametric generalized equations arising from
electronic circuits with AC sources and study the effect of perturbing the
input signal on solution trajectories. Using methods of variational analysis
and strong metric regularity property of an auxiliary map, we are able to prove
the regula... | math.OC | we consider a special form of parametric generalized equations arising from electronic circuits with ac sources and study the effect of perturbing the input signal on solution trajectories using methods of variational analysis and strong metric regularity property of an auxiliary map we are able to prove the regularity... | [['we', 'consider', 'a', 'special', 'form', 'of', 'parametric', 'generalized', 'equations', 'arising', 'from', 'electronic', 'circuits', 'with', 'ac', 'sources', 'and', 'study', 'the', 'effect', 'of', 'perturbing', 'the', 'input', 'signal', 'on', 'solution', 'trajectories', 'using', 'methods', 'of', 'variational', 'ana... | [-0.15696287411265075, 0.037285544525730074, -0.08060501085576387, 0.09920437600297961, -0.09501883649052335, -0.10478031118579495, 0.028789777881824054, 0.33298637869078307, -0.353235669577351, -0.24393194392681694, 0.10324194100058566, -0.286816746374825, -0.1727371275326452, 0.17692034042388863, -0.06513676290901807... |
1,801.03117 | Magnetic Monopole Supercurrent through a Quantum Spin Ice Tunnel
Junction | Magnetic monopoles are hypothetical particles that may exist as quantized
sources and sinks of the magnetic field. In materials, they may appear in an
emergent quantum electrodynamics described by a U(1) lattice gauge theory.
Particularly, quantum spin ice hosts monopoles as bosonic spinons coupled to
emergent gauge ... | cond-mat.str-el | magnetic monopoles are hypothetical particles that may exist as quantized sources and sinks of the magnetic field in materials they may appear in an emergent quantum electrodynamics described by a u1 lattice gauge theory particularly quantum spin ice hosts monopoles as bosonic spinons coupled to emergent gauge fields i... | [['magnetic', 'monopoles', 'are', 'hypothetical', 'particles', 'that', 'may', 'exist', 'as', 'quantized', 'sources', 'and', 'sinks', 'of', 'the', 'magnetic', 'field', 'in', 'materials', 'they', 'may', 'appear', 'in', 'an', 'emergent', 'quantum', 'electrodynamics', 'described', 'by', 'a', 'u1', 'lattice', 'gauge', 'theo... | [-0.23532595911382378, 0.3543869359209121, -0.04861230291816947, 0.0769529831823665, -0.06330562242912455, -0.16094380730463492, 0.025684208958409727, 0.3672718682319864, -0.2011856670862624, -0.2776434783322307, -0.005897225430267831, -0.2898098932110242, -0.13766530362752402, 0.1365020152529819, 0.024197313560081736,... |
1,801.03118 | Nonperturbative renormalization-group approach preserving the momentum
dependence of correlation functions | We present an approximation scheme of the nonperturbative renormalization
group that preserves the momentum dependence of correlation functions. This
approximation scheme can be seen as a simple improvement of the local potential
approximation (LPA) where the derivative terms in the effective action are
promoted to a... | cond-mat.stat-mech cond-mat.quant-gas cond-mat.str-el hep-th | we present an approximation scheme of the nonperturbative renormalization group that preserves the momentum dependence of correlation functions this approximation scheme can be seen as a simple improvement of the local potential approximation lpa where the derivative terms in the effective action are promoted to arbitr... | [['we', 'present', 'an', 'approximation', 'scheme', 'of', 'the', 'nonperturbative', 'renormalization', 'group', 'that', 'preserves', 'the', 'momentum', 'dependence', 'of', 'correlation', 'functions', 'this', 'approximation', 'scheme', 'can', 'be', 'seen', 'as', 'a', 'simple', 'improvement', 'of', 'the', 'local', 'poten... | [-0.12227938853757223, 0.06827164337164504, -0.14500277198603725, 0.10722287210737705, -0.07305245566822123, -0.09267237905878574, 0.03799063114274759, 0.3621530349249952, -0.26413898201135455, -0.2518958204658702, 0.05920233945653308, -0.26247164656833777, -0.1743735176656628, 0.18720349218783666, 0.05192646256473381,... |
1,801.03119 | Giulio Fermi's contributions to biophysics and molecular biology | This paper presents a comprehensive list of the scientific articles of Giulio
Fermi (1936-1997), son of the Italian-American physicist Enrico Fermi,
published between 1962 and 1997. The initial research activity of Giulio was
concerned with virology and biological cybernetics while, from 1975 onward, his
work was com... | physics.hist-ph physics.bio-ph q-bio.BM | this paper presents a comprehensive list of the scientific articles of giulio fermi 19361997 son of the italianamerican physicist enrico fermi published between 1962 and 1997 the initial research activity of giulio was concerned with virology and biological cybernetics while from 1975 onward his work was completely dev... | [['this', 'paper', 'presents', 'a', 'comprehensive', 'list', 'of', 'the', 'scientific', 'articles', 'of', 'giulio', 'fermi', '19361997', 'son', 'of', 'the', 'italianamerican', 'physicist', 'enrico', 'fermi', 'published', 'between', '1962', 'and', '1997', 'the', 'initial', 'research', 'activity', 'of', 'giulio', 'was', ... | [-0.07947563482448458, 0.0867506727237593, -0.07917037674395198, 0.018058448200198737, -0.11541033470579846, -0.09837249492041089, 0.09482585237975318, 0.26183448785238644, -0.16221368364905092, -0.35207891201769764, 0.03274950935738161, -0.34156276343644343, -0.15714075861668045, 0.21881011368452824, -0.14204662975601... |
1,801.0312 | Limiting curves for the dyadic odometer and the generalized
Trollope-Delange formula | We study limiting curves resulting from deviations in partial sums in the
ergodic theorem for the dyadic odometer and non-cylindric functions. In
particular, we generalize the Trollope-Delange formula for the case of the
weighted sum-of-binary-digits function and show that the Takagi-Landsberg curve
arises.
| math.DS | we study limiting curves resulting from deviations in partial sums in the ergodic theorem for the dyadic odometer and noncylindric functions in particular we generalize the trollopedelange formula for the case of the weighted sumofbinarydigits function and show that the takagilandsberg curve arises | [['we', 'study', 'limiting', 'curves', 'resulting', 'from', 'deviations', 'in', 'partial', 'sums', 'in', 'the', 'ergodic', 'theorem', 'for', 'the', 'dyadic', 'odometer', 'and', 'noncylindric', 'functions', 'in', 'particular', 'we', 'generalize', 'the', 'trollopedelange', 'formula', 'for', 'the', 'case', 'of', 'the', 'w... | [-0.1042941881576553, 0.04471004970837385, -0.10845481171272695, 0.13345137145370245, 0.008511237474158407, -0.035980661679059264, 0.09006945791188628, 0.31927446089684963, -0.31461320775561036, -0.17560487983282655, 0.09604311433795373, -0.3122293752618134, -0.2143462859094143, 0.2723552424926311, -0.13499485661741345... |
1,801.03121 | Merging massive black holes: the right place and the right time | The LIGO/Virgo detections of gravitational waves from merging black holes of
$\simeq$ 30 solar mass suggest progenitor stars of low metallicity
(Z/Z$_{\odot} \lesssim 0.3$). In this talk I will provide constrains on where
the progenitors of GW150914 and GW170104 may have formed, based on advanced
models of galaxy for... | astro-ph.GA | the ligovirgo detections of gravitational waves from merging black holes of simeq 30 solar mass suggest progenitor stars of low metallicity zz_odot lesssim 03 in this talk i will provide constrains on where the progenitors of gw150914 and gw170104 may have formed based on advanced models of galaxy formation and evoluti... | [['the', 'ligovirgo', 'detections', 'of', 'gravitational', 'waves', 'from', 'merging', 'black', 'holes', 'of', 'simeq', '30', 'solar', 'mass', 'suggest', 'progenitor', 'stars', 'of', 'low', 'metallicity', 'zz_odot', 'lesssim', '03', 'in', 'this', 'talk', 'i', 'will', 'provide', 'constrains', 'on', 'where', 'the', 'prog... | [-0.09628528791711086, 0.12969082928007142, -0.04673374857596279, 0.13369056941070534, -0.12651738046529376, -0.05124196625774267, 0.02475262288754056, 0.40413214718052126, -0.09133487272941108, -0.3560213595084459, 0.01923418203262951, -0.2905934986646299, -0.018972660927404347, 0.1983103718753759, -0.0196021458847665... |
1,801.03122 | A detailed treatment of Doob's theorem | Doob's theorem provides guarantees of consistent estimation and posterior
consistency under very general conditions. Despite the limitation that it only
guarantees consistency on a set with prior probability 1, for many models
arising in practice, Doob's theorem is an easy way of showing that consistency
will hold al... | math.ST stat.TH | doobs theorem provides guarantees of consistent estimation and posterior consistency under very general conditions despite the limitation that it only guarantees consistency on a set with prior probability 1 for many models arising in practice doobs theorem is an easy way of showing that consistency will hold almost ev... | [['doobs', 'theorem', 'provides', 'guarantees', 'of', 'consistent', 'estimation', 'and', 'posterior', 'consistency', 'under', 'very', 'general', 'conditions', 'despite', 'the', 'limitation', 'that', 'it', 'only', 'guarantees', 'consistency', 'on', 'a', 'set', 'with', 'prior', 'probability', '1', 'for', 'many', 'models'... | [-0.10873864694343259, -0.008194744503271068, -0.18308760126819834, 0.14418648261538086, -0.08768228377448395, -0.132974577586477, 0.09661831489453714, 0.38089258000254633, -0.2167953602038324, -0.2700891320904096, 0.1547655777190812, -0.19612370952963828, -0.11603161554861192, 0.24854938086743156, -0.22180613569604854... |
1,801.03123 | Level-dependent interpolatory Hermite subdivision schemes and wavelets | We study many properties of level-dependent Hermite subdivision, focusing on
schemes preserving polynomial and exponential data. We specifically consider
interpolatory schemes, which give rise to level-dependent multiresolution
analyses through a prediction-correction approach. A result on the decay of the
associated... | math.NA | we study many properties of leveldependent hermite subdivision focusing on schemes preserving polynomial and exponential data we specifically consider interpolatory schemes which give rise to leveldependent multiresolution analyses through a predictioncorrection approach a result on the decay of the associated multiwav... | [['we', 'study', 'many', 'properties', 'of', 'leveldependent', 'hermite', 'subdivision', 'focusing', 'on', 'schemes', 'preserving', 'polynomial', 'and', 'exponential', 'data', 'we', 'specifically', 'consider', 'interpolatory', 'schemes', 'which', 'give', 'rise', 'to', 'leveldependent', 'multiresolution', 'analyses', 't... | [-0.1205833319675278, 0.015343248811109949, -0.12090960596184674, 0.07810596981859841, -0.08162723700012509, -0.10523087676060763, 0.03303399622893414, 0.34332923874309335, -0.3067371197598609, -0.18164710110884058, 0.12251084663659788, -0.2268134078555237, -0.19662294561999874, 0.21930707768360908, -0.0478034975397325... |
1,801.03124 | Is 4C+29.48 a gamma-ray source? | The Fermi Large Area Telescope revealed that the extragalactic gamma-ray sky
is dominated by blazars, active galactic nuclei (AGN) whose jet is seen at very
small angle to the line of sight. To associate and then classify the gamma-ray
sources, data have been collected from lower frequency surveys and
observations. T... | astro-ph.GA astro-ph.HE | the fermi large area telescope revealed that the extragalactic gammaray sky is dominated by blazars active galactic nuclei agn whose jet is seen at very small angle to the line of sight to associate and then classify the gammaray sources data have been collected from lower frequency surveys and observations the gammara... | [['the', 'fermi', 'large', 'area', 'telescope', 'revealed', 'that', 'the', 'extragalactic', 'gammaray', 'sky', 'is', 'dominated', 'by', 'blazars', 'active', 'galactic', 'nuclei', 'agn', 'whose', 'jet', 'is', 'seen', 'at', 'very', 'small', 'angle', 'to', 'the', 'line', 'of', 'sight', 'to', 'associate', 'and', 'then', 'c... | [-0.08861237911790504, 0.08831710967116178, -0.06187464696003039, 0.1291294648960338, -0.1891862146429678, -0.11606881418841308, 0.04147648786041596, 0.5177521594658546, -0.1499799970424711, -0.3147295728241926, 0.09902045456962533, -0.32467638933208404, -0.012437935692320707, 0.22504090872558669, -0.020507600988580618... |
1,801.03125 | Mathematical modeling of cholera epidemics in South Sudan | In this work, we analyze and model the cholera epidemics that affected South
Sudan, the newest country in the world, during 2014 and 2015. South Sudan
possibly represents one of the most difficult context in which adapt the
deterministic mathematical cholera model, due to the unstable social and
political situation t... | q-bio.PE | in this work we analyze and model the cholera epidemics that affected south sudan the newest country in the world during 2014 and 2015 south sudan possibly represents one of the most difficult context in which adapt the deterministic mathematical cholera model due to the unstable social and political situation that cle... | [['in', 'this', 'work', 'we', 'analyze', 'and', 'model', 'the', 'cholera', 'epidemics', 'that', 'affected', 'south', 'sudan', 'the', 'newest', 'country', 'in', 'the', 'world', 'during', '2014', 'and', '2015', 'south', 'sudan', 'possibly', 'represents', 'one', 'of', 'the', 'most', 'difficult', 'context', 'in', 'which', ... | [-0.06679168017385449, 0.08742026824645009, -0.0716627747869166, 0.09998806610903037, -0.041109527044483465, -0.13216565123430507, 0.053714856888879746, 0.2935277748336436, -0.20922622603986474, -0.317835031769888, 0.14675923239463204, -0.31651089628062706, -0.2380438675172627, 0.1585674805746672, -0.14971362761840099,... |
1,801.03126 | Schramm's formula for multiple loop-erased random walks | We revisit the computation of the discrete version of Schramm's formula for
the loop-erased random walk derived by Kenyon. The explicit formula in terms of
the Green function relies on the use of a complex connection on a graph, for
which a line bundle Laplacian is defined. We give explicit results in the
scaling lim... | cond-mat.stat-mech math-ph math.MP | we revisit the computation of the discrete version of schramms formula for the looperased random walk derived by kenyon the explicit formula in terms of the green function relies on the use of a complex connection on a graph for which a line bundle laplacian is defined we give explicit results in the scaling limit for ... | [['we', 'revisit', 'the', 'computation', 'of', 'the', 'discrete', 'version', 'of', 'schramms', 'formula', 'for', 'the', 'looperased', 'random', 'walk', 'derived', 'by', 'kenyon', 'the', 'explicit', 'formula', 'in', 'terms', 'of', 'the', 'green', 'function', 'relies', 'on', 'the', 'use', 'of', 'a', 'complex', 'connectio... | [-0.14899856676657994, 0.06420173675753177, -0.10808888895437122, 0.0884560122123609, -0.10546258450485765, -0.1121428953918318, 0.09940227677424748, 0.3391078541303674, -0.19500161000837882, -0.20475103719780843, 0.16300870882657667, -0.23411522955944142, -0.19601705320179463, 0.22997840251773596, -0.07234415559680202... |
1,801.03127 | Recognizing Material Properties from Images | Humans rely on properties of the materials that make up objects to guide our
interactions with them. Grasping smooth materials, for example, requires care,
and softness is an ideal property for fabric used in bedding. Even when these
properties are not visual (e.g. softness is a physical property), we may still
infer... | cs.CV | humans rely on properties of the materials that make up objects to guide our interactions with them grasping smooth materials for example requires care and softness is an ideal property for fabric used in bedding even when these properties are not visual eg softness is a physical property we may still infer their prese... | [['humans', 'rely', 'on', 'properties', 'of', 'the', 'materials', 'that', 'make', 'up', 'objects', 'to', 'guide', 'our', 'interactions', 'with', 'them', 'grasping', 'smooth', 'materials', 'for', 'example', 'requires', 'care', 'and', 'softness', 'is', 'an', 'ideal', 'property', 'for', 'fabric', 'used', 'in', 'bedding', ... | [-0.048635601817308624, 0.029509820603137827, -0.08223742753767288, 0.08573402329758413, -0.1871019270314614, -0.17487608346495134, 0.04059868603701897, 0.46752657465931535, -0.2932788393788522, -0.3796341323977162, 0.05262629442895166, -0.2806266005580831, -0.18759882973051437, 0.17087684641927212, -0.1500602203133187... |
1,801.03128 | Dust arcs in the region of Jupiter's Trojan asteroids | Aims. The surfaces of the Trojan asteroids are steadily bombarded by
interplanetary micrometeoroids, which releases ejecta of small dust particles.
These particles form the faint dust arcs that are associated with asteroid
clouds. Here we analyze the particle dynamics and structure of the arc in the
region of the $L_... | astro-ph.EP | aims the surfaces of the trojan asteroids are steadily bombarded by interplanetary micrometeoroids which releases ejecta of small dust particles these particles form the faint dust arcs that are associated with asteroid clouds here we analyze the particle dynamics and structure of the arc in the region of the l_4 troja... | [['aims', 'the', 'surfaces', 'of', 'the', 'trojan', 'asteroids', 'are', 'steadily', 'bombarded', 'by', 'interplanetary', 'micrometeoroids', 'which', 'releases', 'ejecta', 'of', 'small', 'dust', 'particles', 'these', 'particles', 'form', 'the', 'faint', 'dust', 'arcs', 'that', 'are', 'associated', 'with', 'asteroid', 'c... | [-0.11751226285831576, 0.2063985902964031, -0.11301603766175054, 0.05733966903623575, 0.01001006097207407, -0.011431853329701102, -0.01370297486792846, 0.34339369669646386, -0.2212354907014194, -0.3201235835496561, 0.034467007976771526, -0.3383457223794995, -0.05583204069113112, 0.11584854839265862, -0.0700275639048567... |
1,801.03129 | Phases of superclimbing dislocation with long-range interaction between
jogs | The main candidate for the superfluid pathways in solid Helium-4 are
dislocations with Burgers vector along the hcp symmetry axis. Here we focus on
quantum behavior of a generic edge dislocation which can perform superclimb --
climb supported by the superflow along its core. The role of the long range
elastic interac... | cond-mat.other | the main candidate for the superfluid pathways in solid helium4 are dislocations with burgers vector along the hcp symmetry axis here we focus on quantum behavior of a generic edge dislocation which can perform superclimb climb supported by the superflow along its core the role of the long range elastic interactions be... | [['the', 'main', 'candidate', 'for', 'the', 'superfluid', 'pathways', 'in', 'solid', 'helium4', 'are', 'dislocations', 'with', 'burgers', 'vector', 'along', 'the', 'hcp', 'symmetry', 'axis', 'here', 'we', 'focus', 'on', 'quantum', 'behavior', 'of', 'a', 'generic', 'edge', 'dislocation', 'which', 'can', 'perform', 'supe... | [-0.1528946882835064, 0.24378948666407427, -0.07024933007822365, 0.04324541573458232, -0.04412049359004749, -0.08656615659216405, 0.01843948046417725, 0.3841805914416909, -0.27896986838738275, -0.2726456097264151, 0.05401035500567799, -0.2619233920792104, -0.14185691903226247, 0.11671221473068699, 0.0748592462369654, 0... |
1,801.0313 | Isovector and flavor-diagonal charges of the nucleon | We present an update on the status of the calculations of isovector and
flavor-diagonal charges of the nucleon. The calculations of the isovector
charges are being done using ten $2+1+1$-flavor HISQ ensembles generated by the
MILC collaboration covering the range of lattice spacings $a \approx$ 0.12,
0.09, 0.06 fm an... | hep-lat | we present an update on the status of the calculations of isovector and flavordiagonal charges of the nucleon the calculations of the isovector charges are being done using ten 211flavor hisq ensembles generated by the milc collaboration covering the range of lattice spacings a approx 012 009 006 fm and pion masses m_p... | [['we', 'present', 'an', 'update', 'on', 'the', 'status', 'of', 'the', 'calculations', 'of', 'isovector', 'and', 'flavordiagonal', 'charges', 'of', 'the', 'nucleon', 'the', 'calculations', 'of', 'the', 'isovector', 'charges', 'are', 'being', 'done', 'using', 'ten', '211flavor', 'hisq', 'ensembles', 'generated', 'by', '... | [-0.11484864591730862, 0.26424650883581213, -0.05865811362613257, 0.08048481304715498, 0.014912067803207741, -0.059906236988704974, 0.13004896927470944, 0.38887473516987536, -0.08502547181849404, -0.294118476446762, 0.046329746164902166, -0.35665694780383755, 0.038641256024954676, 0.11224248454774048, 0.092521693495168... |
1,801.03131 | Lifted graphene nanoribbons on gold: from smooth sliding to multiple
stick-slip regimes | Graphene nanoribbons (GNRs) physisorbed on a Au(111) surface can be picked
up, lifted at one end, and made slide by means of the tip of an atomic-force
microscope. The dynamical transition from smooth sliding to multiple stick-slip
regimes, the pushing/pulling force asymmetry, the presence of pinning, and its
origin ... | cond-mat.mes-hall | graphene nanoribbons gnrs physisorbed on a au111 surface can be picked up lifted at one end and made slide by means of the tip of an atomicforce microscope the dynamical transition from smooth sliding to multiple stickslip regimes the pushingpulling force asymmetry the presence of pinning and its origin are real fricti... | [['graphene', 'nanoribbons', 'gnrs', 'physisorbed', 'on', 'a', 'au111', 'surface', 'can', 'be', 'picked', 'up', 'lifted', 'at', 'one', 'end', 'and', 'made', 'slide', 'by', 'means', 'of', 'the', 'tip', 'of', 'an', 'atomicforce', 'microscope', 'the', 'dynamical', 'transition', 'from', 'smooth', 'sliding', 'to', 'multiple... | [-0.1358930860528505, 0.15504634264241185, -0.08610287339788077, -0.008688541284707179, -0.0402412637685254, -0.17444741017702894, 0.06208877883679969, 0.3848569331886737, -0.3158364501830779, -0.29075538652863253, 0.02001007208233013, -0.2671690423648167, -0.14162945076761962, 0.19656729088072958, -0.00629831049713845... |
1,801.03132 | Robust Propensity Score Computation Method based on Machine Learning
with Label-corrupted Data | In biostatistics, propensity score is a common approach to analyze the
imbalance of covariate and process confounding covariates to eliminate
differences between groups. While there are an abundant amount of methods to
compute propensity score, a common issue of them is the corrupted labels in the
dataset. For exampl... | stat.ME cs.AI stat.ML | in biostatistics propensity score is a common approach to analyze the imbalance of covariate and process confounding covariates to eliminate differences between groups while there are an abundant amount of methods to compute propensity score a common issue of them is the corrupted labels in the dataset for example the ... | [['in', 'biostatistics', 'propensity', 'score', 'is', 'a', 'common', 'approach', 'to', 'analyze', 'the', 'imbalance', 'of', 'covariate', 'and', 'process', 'confounding', 'covariates', 'to', 'eliminate', 'differences', 'between', 'groups', 'while', 'there', 'are', 'an', 'abundant', 'amount', 'of', 'methods', 'to', 'comp... | [-0.008702579197303679, 0.013130103554850883, -0.11414550852406627, 0.07229924666147816, -0.11326959962025285, -0.12890820804302797, 0.09572216671501967, 0.4187450322832984, -0.256164995069132, -0.3531516404204572, 0.08670966680410157, -0.332631408492139, -0.15241725314207052, 0.16818003609380236, -0.1259962401818484, ... |
1,801.03133 | Dynamics and distribution of Jovian dust ejected from the Galilean
satellites | In this paper, the dynamical analysis of the Jovian dust originating from the
four Galilean moons is presented. High accuracy orbital integrations of dust
particles are used to determine their dynamical evolution. A variety of forces
are taken into account, including the Lorentz force, solar radiation pressure,
Poynt... | astro-ph.EP | in this paper the dynamical analysis of the jovian dust originating from the four galilean moons is presented high accuracy orbital integrations of dust particles are used to determine their dynamical evolution a variety of forces are taken into account including the lorentz force solar radiation pressure poyntingrober... | [['in', 'this', 'paper', 'the', 'dynamical', 'analysis', 'of', 'the', 'jovian', 'dust', 'originating', 'from', 'the', 'four', 'galilean', 'moons', 'is', 'presented', 'high', 'accuracy', 'orbital', 'integrations', 'of', 'dust', 'particles', 'are', 'used', 'to', 'determine', 'their', 'dynamical', 'evolution', 'a', 'varie... | [-0.10101963053225574, 0.23193262024353647, -0.07670261912018639, 0.07615266236644702, -0.02970898358530029, -0.052790906677347184, -0.0313462934053901, 0.34307712744689584, -0.21298535742470415, -0.34540195094954795, 0.0519160795314392, -0.292904315755946, -0.026546909596531408, 0.1933954908817821, -0.0737706964593289... |
1,801.03134 | A $q$-analog of Jacobi's two squares formula and its applications | We consider a $q$-analog $r_2(n, q)$ of the number of representations of an
integer as a sum of two squares $r_2(n)$. This $q$-analog is generated by the
expansion of a product that was studied by Kronecker and Jordan. We generalize
Jacobi's two squares formula from $r_2(n)$ to $r_2(n, q)$. We characterize the
signs ... | math.NT | we consider a qanalog r_2n q of the number of representations of an integer as a sum of two squares r_2n this qanalog is generated by the expansion of a product that was studied by kronecker and jordan we generalize jacobis two squares formula from r_2n to r_2n q we characterize the signs in the coefficients of r_2n q ... | [['we', 'consider', 'a', 'qanalog', 'r_2n', 'q', 'of', 'the', 'number', 'of', 'representations', 'of', 'an', 'integer', 'as', 'a', 'sum', 'of', 'two', 'squares', 'r_2n', 'this', 'qanalog', 'is', 'generated', 'by', 'the', 'expansion', 'of', 'a', 'product', 'that', 'was', 'studied', 'by', 'kronecker', 'and', 'jordan', 'w... | [-0.22624807167140876, 0.10829385823231218, -0.07205144065048764, 0.019564515930216977, -0.05366100361570716, -0.11067143184516359, 0.003581345588078394, 0.290431180705919, -0.3226397703675663, -0.20875899833353126, 0.06708698520738193, -0.3170051760971546, -0.17121773955193073, 0.16426006020868525, -0.0695927959812038... |
1,801.03135 | Mass-deformed ABJM and Black Holes in AdS$_4$ | We find a class of new supersymmetric dyonic black holes in four-dimensional
maximal gauged supergravity which are asymptotic to the ${\rm SU(3)}\times {\rm
U(1)}$ invariant AdS$_4$ Warner vacuum. These black holes can be embedded in
eleven-dimensional supergravity where they describe the backreaction of
M2-branes wr... | hep-th | we find a class of new supersymmetric dyonic black holes in fourdimensional maximal gauged supergravity which are asymptotic to the rm su3times rm u1 invariant ads_4 warner vacuum these black holes can be embedded in elevendimensional supergravity where they describe the backreaction of m2branes wrapped on a riemann su... | [['we', 'find', 'a', 'class', 'of', 'new', 'supersymmetric', 'dyonic', 'black', 'holes', 'in', 'fourdimensional', 'maximal', 'gauged', 'supergravity', 'which', 'are', 'asymptotic', 'to', 'the', 'rm', 'su3times', 'rm', 'u1', 'invariant', 'ads_4', 'warner', 'vacuum', 'these', 'black', 'holes', 'can', 'be', 'embedded', 'i... | [-0.17575513574605187, 0.16993388459086417, -0.04874472586615455, 0.14677035761221002, -0.07493383980666597, -0.13819961315464405, -0.06044904255818221, 0.2642855004496163, -0.07941413889417336, -0.24045171441421623, 0.10046546125474075, -0.30004855798823493, -0.19892998312910398, 0.09704300487591397, -0.12026997574180... |
1,801.03136 | Numerical simulations of ICME-ICME interactions | We present hydrodynamical simulations of interacting Coronal Mass Ejections
in the Interplanetary medium (ICMEs). In these events, two consecutive CMEs are
launched from the Sun in similar directions within an interval of time of a few
hours. In our numerical model, we assume that the ambient solar wind is
characteri... | astro-ph.SR | we present hydrodynamical simulations of interacting coronal mass ejections in the interplanetary medium icmes in these events two consecutive cmes are launched from the sun in similar directions within an interval of time of a few hours in our numerical model we assume that the ambient solar wind is characterized by i... | [['we', 'present', 'hydrodynamical', 'simulations', 'of', 'interacting', 'coronal', 'mass', 'ejections', 'in', 'the', 'interplanetary', 'medium', 'icmes', 'in', 'these', 'events', 'two', 'consecutive', 'cmes', 'are', 'launched', 'from', 'the', 'sun', 'in', 'similar', 'directions', 'within', 'an', 'interval', 'of', 'tim... | [-0.09231950786504825, 0.16477299206436838, -0.07278518301165848, 0.09056491554553749, -0.03135791621309424, -0.03351548381260558, 0.01374103698955648, 0.4219592580031673, -0.20243616074887988, -0.3795461357481601, 0.08331564897117395, -0.24151392175719058, -0.08793339763014348, 0.18553695527704253, -0.0326049857009912... |
1,801.03137 | Convergence Analysis of Gradient Descent Algorithms with Proportional
Updates | The rise of deep learning in recent years has brought with it increasingly
clever optimization methods to deal with complex, non-linear loss functions.
These methods are often designed with convex optimization in mind, but have
been shown to work well in practice even for the highly non-convex optimization
associated... | cs.LG cs.AI stat.ML | the rise of deep learning in recent years has brought with it increasingly clever optimization methods to deal with complex nonlinear loss functions these methods are often designed with convex optimization in mind but have been shown to work well in practice even for the highly nonconvex optimization associated with n... | [['the', 'rise', 'of', 'deep', 'learning', 'in', 'recent', 'years', 'has', 'brought', 'with', 'it', 'increasingly', 'clever', 'optimization', 'methods', 'to', 'deal', 'with', 'complex', 'nonlinear', 'loss', 'functions', 'these', 'methods', 'are', 'often', 'designed', 'with', 'convex', 'optimization', 'in', 'mind', 'but... | [-0.035465766304995455, 0.0453638773135325, -0.09519927456599424, 0.07874191242105914, -0.11693786735780384, -0.18353356289428543, 0.010843282533579902, 0.4459492362739059, -0.31508892152696844, -0.33739198587535024, 0.1421145194226857, -0.2480850537747706, -0.19476549333513216, 0.1790636765143885, -0.13662863681762646... |
1,801.03138 | Deep In-GPU Experience Replay | Experience replay allows a reinforcement learning agent to train on samples
from a large amount of the most recent experiences. A simple in-RAM experience
replay stores these most recent experiences in a list in RAM, and then copies
sampled batches to the GPU for training. I moved this list to the GPU, thus
creating ... | cs.AI | experience replay allows a reinforcement learning agent to train on samples from a large amount of the most recent experiences a simple inram experience replay stores these most recent experiences in a list in ram and then copies sampled batches to the gpu for training i moved this list to the gpu thus creating an ingp... | [['experience', 'replay', 'allows', 'a', 'reinforcement', 'learning', 'agent', 'to', 'train', 'on', 'samples', 'from', 'a', 'large', 'amount', 'of', 'the', 'most', 'recent', 'experiences', 'a', 'simple', 'inram', 'experience', 'replay', 'stores', 'these', 'most', 'recent', 'experiences', 'in', 'a', 'list', 'in', 'ram',... | [-0.06480870011234374, 0.09282021411098398, -0.07869307465823085, 0.009453191293516393, -0.13964677445138945, -0.21021197287252907, 0.12328810002654791, 0.4442403556496808, -0.24864634496837176, -0.3525454489740007, 0.09932017765769904, -0.2969685503268424, -0.0854298152382288, 0.17378184604387956, -0.1447092269448507,... |
1,801.03139 | Experimental Observation of Strong Coupling Between an Epsilon-Near-Zero
Mode in a Deep Subwavelength Nanofilm and a Gap Plasmon Mode | Strong coupling is a phenomenon which occurs when the interaction between two
resonance systems is so strong that the oscillatory energy exchange between
them exceeds all dissipative loss channels. Each resonance can then no longer
be described individually but only as a part of the coupled, hybrid system.
Here, we s... | physics.optics cond-mat.mes-hall | strong coupling is a phenomenon which occurs when the interaction between two resonance systems is so strong that the oscillatory energy exchange between them exceeds all dissipative loss channels each resonance can then no longer be described individually but only as a part of the coupled hybrid system here we show th... | [['strong', 'coupling', 'is', 'a', 'phenomenon', 'which', 'occurs', 'when', 'the', 'interaction', 'between', 'two', 'resonance', 'systems', 'is', 'so', 'strong', 'that', 'the', 'oscillatory', 'energy', 'exchange', 'between', 'them', 'exceeds', 'all', 'dissipative', 'loss', 'channels', 'each', 'resonance', 'can', 'then'... | [-0.19584290582758807, 0.18233035927141186, -0.03328984806438724, 0.048763216480745566, -0.04098332697250159, -0.17182093007411336, 0.039896134280560304, 0.4220483640248192, -0.2755350395118896, -0.27008840699785086, 0.033475424577875564, -0.28672005394211325, -0.1249626924687157, 0.2070105531118469, 0.0498205999133396... |
1,801.0314 | Detailed abundance analysis of globular clusters in the Local Group: NGC
147, NGC 6822, and Messier 33 | We present new abundance measurements for eleven GCs in the Local Group
galaxies NGC 147, NGC 6822, and Messier 33. These are combined with previously
published observations of four GCs in the Fornax and WLM galaxies. The
abundances were determined from analysis of integrated-light spectra, obtained
with HIRES on the... | astro-ph.GA | we present new abundance measurements for eleven gcs in the local group galaxies ngc 147 ngc 6822 and messier 33 these are combined with previously published observations of four gcs in the fornax and wlm galaxies the abundances were determined from analysis of integratedlight spectra obtained with hires on the keck i ... | [['we', 'present', 'new', 'abundance', 'measurements', 'for', 'eleven', 'gcs', 'in', 'the', 'local', 'group', 'galaxies', 'ngc', '147', 'ngc', '6822', 'and', 'messier', '33', 'these', 'are', 'combined', 'with', 'previously', 'published', 'observations', 'of', 'four', 'gcs', 'in', 'the', 'fornax', 'and', 'wlm', 'galaxie... | [0.017135268578819373, 0.08027878778586252, -0.08339523114198731, 0.12118679419743054, -0.11678062644558654, -0.011200924166782854, 0.04712472868121499, 0.4853537502028396, -0.0371016814998282, -0.443069750094943, -0.08647751354745145, -0.3412821514218628, 0.02612011089363945, 0.21897823342687078, -0.0791517499688508, ... |
1,801.03141 | Anatomy of triply-periodic network assemblies: Characterizing skeletal
and inter-domain surface geometry of block copolymer gyroids | Triply-periodic networks (TPNs), like the well-known gyroid and diamond
network phases, abound in soft matter assemblies, from block copolymers (BCPs),
lyotropic liquid crystals and surfactants to functional architectures in
biology. While TPNs are, in reality, volume-filling patterns of
spatially-varying molecular c... | cond-mat.soft cond-mat.mtrl-sci | triplyperiodic networks tpns like the wellknown gyroid and diamond network phases abound in soft matter assemblies from block copolymers bcps lyotropic liquid crystals and surfactants to functional architectures in biology while tpns are in reality volumefilling patterns of spatiallyvarying molecular composition physic... | [['triplyperiodic', 'networks', 'tpns', 'like', 'the', 'wellknown', 'gyroid', 'and', 'diamond', 'network', 'phases', 'abound', 'in', 'soft', 'matter', 'assemblies', 'from', 'block', 'copolymers', 'bcps', 'lyotropic', 'liquid', 'crystals', 'and', 'surfactants', 'to', 'functional', 'architectures', 'in', 'biology', 'whil... | [-0.07834851044056894, 0.09619840168953213, -0.07972178375348449, 0.05788586102155319, -0.051300309653675484, -0.15503901819763488, 0.018987671123969173, 0.4397697078908772, -0.2951716570730516, -0.2875784307263445, 0.06937764841023572, -0.24505801797346322, -0.23235240698532136, 0.14594913171658422, -0.015495261069127... |
1,801.03142 | Topological freeness for $C^*$-correspondences | We study conditions that ensure uniqueness theorems of Cuntz-Krieger type for
relative Cuntz-Pimsner algebras $\mathcal{O}(J,X)$ associated to a
$C^*$-correspondence $X$ over a $C^*$-algebra $A$. We give general sufficient
conditions phrased in terms of a multivalued map $\widehat{X}$ acting on the
spectrum $\widehat... | math.OA | we study conditions that ensure uniqueness theorems of cuntzkrieger type for relative cuntzpimsner algebras mathcalojx associated to a ccorrespondence x over a calgebra a we give general sufficient conditions phrased in terms of a multivalued map widehatx acting on the spectrum widehata of a when xj is of type i we con... | [['we', 'study', 'conditions', 'that', 'ensure', 'uniqueness', 'theorems', 'of', 'cuntzkrieger', 'type', 'for', 'relative', 'cuntzpimsner', 'algebras', 'mathcalojx', 'associated', 'to', 'a', 'ccorrespondence', 'x', 'over', 'a', 'calgebra', 'a', 'we', 'give', 'general', 'sufficient', 'conditions', 'phrased', 'in', 'term... | [-0.1299828080621233, 0.03440531554904921, -0.08054304769825485, 0.09045631062363362, -0.11318470656590389, -0.1275042356326908, 0.01119150689354153, 0.3797169525792702, -0.337370482816113, -0.15829874125892202, 0.15079671516260734, -0.21634688653829073, -0.15713309981732917, 0.18216949846032712, -0.21446402649656474, ... |
1,801.03143 | Comparing heterogeneous entities using artificial neural networks of
trainable weighted structural components and machine-learned activation
functions | To compare entities of differing types and structural components, the
artificial neural network paradigm was used to cross-compare structural
components between heterogeneous documents. Trainable weighted structural
components were input into machine-learned activation functions of the neurons.
The model was used for... | stat.ML cs.AI cs.IR cs.LG cs.NE | to compare entities of differing types and structural components the artificial neural network paradigm was used to crosscompare structural components between heterogeneous documents trainable weighted structural components were input into machinelearned activation functions of the neurons the model was used for matchi... | [['to', 'compare', 'entities', 'of', 'differing', 'types', 'and', 'structural', 'components', 'the', 'artificial', 'neural', 'network', 'paradigm', 'was', 'used', 'to', 'crosscompare', 'structural', 'components', 'between', 'heterogeneous', 'documents', 'trainable', 'weighted', 'structural', 'components', 'were', 'inpu... | [-0.05596774625259319, 0.04053905093210882, -0.003418324498592743, 0.07675177094383148, -0.13262578257542504, -0.14711497022290132, 0.044797852778823914, 0.46314131441925255, -0.2648283234365018, -0.34890583656462176, 0.019442359324394993, -0.3704548523029579, -0.17092946475687704, 0.16302583704444779, -0.0713520000904... |
1,801.03144 | Reconstruction of piecewise smooth wave speeds using multiple scattering | Let $c$ be a piecewise smooth wave speed on $\mathbb R^n$, unknown inside a
domain $\Omega$. We are given the solution operator for the scalar wave
equation $(\partial_t^2-c^2\Delta)u=0$, but only outside $\Omega$ and only for
initial data supported outside $\Omega$. Using our recently developed
scattering control me... | math.AP | let c be a piecewise smooth wave speed on mathbb rn unknown inside a domain omega we are given the solution operator for the scalar wave equation partial_t2c2deltau0 but only outside omega and only for initial data supported outside omega using our recently developed scattering control method we prove that piecewise sm... | [['let', 'c', 'be', 'a', 'piecewise', 'smooth', 'wave', 'speed', 'on', 'mathbb', 'rn', 'unknown', 'inside', 'a', 'domain', 'omega', 'we', 'are', 'given', 'the', 'solution', 'operator', 'for', 'the', 'scalar', 'wave', 'equation', 'partial_t2c2deltau0', 'but', 'only', 'outside', 'omega', 'and', 'only', 'for', 'initial', ... | [-0.16411519314397524, 0.0761106618933235, -0.06957260343399875, 0.03115863989568451, -0.12422765179953167, -0.1779812818971797, 0.00966150205112198, 0.39393714932923757, -0.3209889920301808, -0.1750944890217512, 0.1299955601254659, -0.23900738122502288, -0.1401442224973614, 0.2373965129643923, -0.03850798572874763, 0.... |
1,801.03145 | Visual and Semantic Knowledge Transfer for Large Scale Semi-supervised
Object Detection | Deep CNN-based object detection systems have achieved remarkable success on
several large-scale object detection benchmarks. However, training such
detectors requires a large number of labeled bounding boxes, which are more
difficult to obtain than image-level annotations. Previous work addresses this
issue by transf... | cs.CV | deep cnnbased object detection systems have achieved remarkable success on several largescale object detection benchmarks however training such detectors requires a large number of labeled bounding boxes which are more difficult to obtain than imagelevel annotations previous work addresses this issue by transforming im... | [['deep', 'cnnbased', 'object', 'detection', 'systems', 'have', 'achieved', 'remarkable', 'success', 'on', 'several', 'largescale', 'object', 'detection', 'benchmarks', 'however', 'training', 'such', 'detectors', 'requires', 'a', 'large', 'number', 'of', 'labeled', 'bounding', 'boxes', 'which', 'are', 'more', 'difficul... | [-0.000732096999766674, -0.02562460745797281, -0.043664360909322325, 0.09239600109169155, -0.13342340515503562, -0.1938637833353942, 0.033206128735761134, 0.45644221954713554, -0.19439380881174104, -0.40677083620648596, 0.0405187837679416, -0.33206205317555987, -0.13372120109121294, 0.2077801899996711, -0.1580843337528... |
1,801.03146 | Venus: The Making of an Uninhabitable World | The goals of the astrobiology community are focussed on developing a
framework for the detection of biosignatures, or evidence thereof, on objects
inside and outside of our solar system. A fundamental aspect of understanding
the limits of habitable environments and detectable signatures is the study of
where the boun... | astro-ph.EP | the goals of the astrobiology community are focussed on developing a framework for the detection of biosignatures or evidence thereof on objects inside and outside of our solar system a fundamental aspect of understanding the limits of habitable environments and detectable signatures is the study of where the boundarie... | [['the', 'goals', 'of', 'the', 'astrobiology', 'community', 'are', 'focussed', 'on', 'developing', 'a', 'framework', 'for', 'the', 'detection', 'of', 'biosignatures', 'or', 'evidence', 'thereof', 'on', 'objects', 'inside', 'and', 'outside', 'of', 'our', 'solar', 'system', 'a', 'fundamental', 'aspect', 'of', 'understand... | [-0.12042780706613529, 0.11329902729905769, -0.0966275949882934, 0.07405502851285813, -0.13994695189005762, -0.037054128149842346, 0.10716018442876592, 0.3287261499591717, -0.21167001562340684, -0.3296651208756219, 0.14167348413817618, -0.24826371567267017, -0.16256449967424, 0.21170761924742426, -0.06682186626272685, ... |
1,801.03147 | "Robust-squared" Imputation Models Using BART | Examples of "doubly robust" estimator for missing data include augmented inverse probability weighting (AIPWT) models (Robins et al., 1994) and penalized splines of propensity prediction (PSPP) models (Zhang and Little, 2009). Doubly-robust estimators have the property that, if either the response propensity or the mea... | stat.AP | examples of doubly robust estimator for missing data include augmented inverse probability weighting aipwt models robins et al 1994 and penalized splines of propensity prediction pspp models zhang and little 2009 doublyrobust estimators have the property that if either the response propensity or the mean is modeled cor... | [['examples', 'of', 'doubly', 'robust', 'estimator', 'for', 'missing', 'data', 'include', 'augmented', 'inverse', 'probability', 'weighting', 'aipwt', 'models', 'robins', 'et', 'al', '1994', 'and', 'penalized', 'splines', 'of', 'propensity', 'prediction', 'pspp', 'models', 'zhang', 'and', 'little', '2009', 'doublyrobus... | [0.004845729283856186, 0.01661392585374415, -0.08518392373066903, 0.11958857669008219, -0.09130036843178624, -0.19875763572583144, 0.07053607009584084, 0.4124646922298284, -0.2161703550537244, -0.34613904191435063, 0.12301024776057932, -0.2926223112989894, -0.16548787432812703, 0.13687827249523252, -0.15431048605083064... |
1,801.03148 | $\tau \to f_1 (1285)\pi^{-} \nu_{\tau}$ decay in the extended Nambu --
Jona-Lasinio model | Within the framework of the extended Nambu -- Jona-Lasinio model, we
calculate the matrix element of the $\tau \to f_1(1285) \pi^{-} \nu_{\tau}$
decay, obtain the invariant mass distribution of the $f_1\pi$ -system and
estimate the branching ratio Br$(\tau \to f_1 \pi^{-}\nu_{\tau})=4.0\times
10^{-4}$. The two types ... | hep-ph | within the framework of the extended nambu jonalasinio model we calculate the matrix element of the tau to f_11285 pi nu_tau decay obtain the invariant mass distribution of the f_1pi system and estimate the branching ratio brtau to f_1 pinu_tau40times 104 the two types of contributions are considered the contact intera... | [['within', 'the', 'framework', 'of', 'the', 'extended', 'nambu', 'jonalasinio', 'model', 'we', 'calculate', 'the', 'matrix', 'element', 'of', 'the', 'tau', 'to', 'f_11285', 'pi', 'nu_tau', 'decay', 'obtain', 'the', 'invariant', 'mass', 'distribution', 'of', 'the', 'f_1pi', 'system', 'and', 'estimate', 'the', 'branchin... | [-0.11521512481908266, 0.18359979706407664, -0.07879671467159935, 0.13045830736958536, -0.02145002926733318, -0.12427144507348216, 0.07359914610952996, 0.2978843728469001, -0.22355169640906764, -0.22993376910378285, -0.0072112994146258606, -0.3437502122879457, -0.012980626071485014, 0.11794102797452226, 0.1048658239063... |
1,801.03149 | An overview of deep learning based methods for unsupervised and
semi-supervised anomaly detection in videos | Videos represent the primary source of information for surveillance
applications and are available in large amounts but in most cases contain
little or no annotation for supervised learning. This article reviews the
state-of-the-art deep learning based methods for video anomaly detection and
categorizes them based on... | cs.CV | videos represent the primary source of information for surveillance applications and are available in large amounts but in most cases contain little or no annotation for supervised learning this article reviews the stateoftheart deep learning based methods for video anomaly detection and categorizes them based on the t... | [['videos', 'represent', 'the', 'primary', 'source', 'of', 'information', 'for', 'surveillance', 'applications', 'and', 'are', 'available', 'in', 'large', 'amounts', 'but', 'in', 'most', 'cases', 'contain', 'little', 'or', 'no', 'annotation', 'for', 'supervised', 'learning', 'this', 'article', 'reviews', 'the', 'stateo... | [-0.04279537793450259, -0.049176458451846566, -0.04876990298067245, 0.08169264606093182, -0.1316099990209615, -0.1808762903879019, 0.020149858454494057, 0.4222949658696716, -0.17807710272215962, -0.34782311237240965, 0.14496352478572344, -0.308508964280623, -0.16460763994365227, 0.23213441445290842, -0.1132011564662428... |
1,801.0315 | Moments in Time Dataset: one million videos for event understanding | We present the Moments in Time Dataset, a large-scale human-annotated
collection of one million short videos corresponding to dynamic events
unfolding within three seconds. Modeling the spatial-audio-temporal dynamics
even for actions occurring in 3 second videos poses many challenges: meaningful
events do not includ... | cs.CV cs.AI | we present the moments in time dataset a largescale humanannotated collection of one million short videos corresponding to dynamic events unfolding within three seconds modeling the spatialaudiotemporal dynamics even for actions occurring in 3 second videos poses many challenges meaningful events do not include only pe... | [['we', 'present', 'the', 'moments', 'in', 'time', 'dataset', 'a', 'largescale', 'humanannotated', 'collection', 'of', 'one', 'million', 'short', 'videos', 'corresponding', 'to', 'dynamic', 'events', 'unfolding', 'within', 'three', 'seconds', 'modeling', 'the', 'spatialaudiotemporal', 'dynamics', 'even', 'for', 'action... | [-0.08751990719337684, 0.09976036571749523, -0.045231031218942015, 0.10628963270764187, -0.11087816728903466, -0.13051120745491862, 0.01760582562476784, 0.4479341612525844, -0.26179469225529817, -0.3637853177288558, 0.10120589419932917, -0.30241637750369943, -0.13910755183752302, 0.1852943559286233, -0.1185132369757064... |
1,801.03151 | Domain-dependent stability analysis and parameter classification of a
reaction-diffusion model on spherical geometries | In this work an activator-depleted reaction-diffusion system is investigated
on polar coordinates with the aim of exploring the relationship and the
corresponding influence of domain size on the types of possible
diffusion-driven instabilities. Quantitative relationships are found in the
form of necessary conditions ... | math.DS | in this work an activatordepleted reactiondiffusion system is investigated on polar coordinates with the aim of exploring the relationship and the corresponding influence of domain size on the types of possible diffusiondriven instabilities quantitative relationships are found in the form of necessary conditions on the... | [['in', 'this', 'work', 'an', 'activatordepleted', 'reactiondiffusion', 'system', 'is', 'investigated', 'on', 'polar', 'coordinates', 'with', 'the', 'aim', 'of', 'exploring', 'the', 'relationship', 'and', 'the', 'corresponding', 'influence', 'of', 'domain', 'size', 'on', 'the', 'types', 'of', 'possible', 'diffusiondriv... | [-0.12946824398472312, 0.04472114457338326, -0.07526463501810657, 0.05067821884147546, -0.04692088875118399, -0.10515796698784399, 0.03311994106800592, 0.3524981807143627, -0.23806583995861713, -0.2517417585164589, 0.15264656423544307, -0.24918371647612628, -0.13672511104807486, 0.2487305415276739, -0.03415430387416977... |
1,801.03152 | Invariant measures for the periodic derivative nonlinear Schr\"odinger
equation | We construct invariant measures associated to the integrals of motion of the
periodic derivative nonlinear Schr\"odinger equation (DNLS) for small data in
$L^2$ and we show these measures to be absolutely continuous with respect to
the Gaussian measure. The key ingredient of the proof is the analysis of the
gauge gro... | math-ph math.AP math.MP | we construct invariant measures associated to the integrals of motion of the periodic derivative nonlinear schrodinger equation dnls for small data in l2 and we show these measures to be absolutely continuous with respect to the gaussian measure the key ingredient of the proof is the analysis of the gauge group of tran... | [['we', 'construct', 'invariant', 'measures', 'associated', 'to', 'the', 'integrals', 'of', 'motion', 'of', 'the', 'periodic', 'derivative', 'nonlinear', 'schrodinger', 'equation', 'dnls', 'for', 'small', 'data', 'in', 'l2', 'and', 'we', 'show', 'these', 'measures', 'to', 'be', 'absolutely', 'continuous', 'with', 'resp... | [-0.11877983568522793, 0.06886986246237752, -0.11111169336930825, 0.08261936045556258, -0.0572566620957775, -0.08387869185744187, -0.020878131743162297, 0.37394097714852065, -0.29885195224330974, -0.19950770743889734, 0.13490161790888613, -0.296757486075736, -0.13583852919952896, 0.18370855825308424, -0.099432287976527... |
1,801.03153 | A New Coding Paradigm for the Primitive Relay Channel | We consider the primitive relay channel, where the source sends a message to
the relay and to the destination, and the relay helps the communication by
transmitting an additional message to the destination via a separate channel.
Two well-known coding techniques have been introduced for this setting:
decode-and-forwa... | cs.IT math.IT | we consider the primitive relay channel where the source sends a message to the relay and to the destination and the relay helps the communication by transmitting an additional message to the destination via a separate channel two wellknown coding techniques have been introduced for this setting decodeandforward and co... | [['we', 'consider', 'the', 'primitive', 'relay', 'channel', 'where', 'the', 'source', 'sends', 'a', 'message', 'to', 'the', 'relay', 'and', 'to', 'the', 'destination', 'and', 'the', 'relay', 'helps', 'the', 'communication', 'by', 'transmitting', 'an', 'additional', 'message', 'to', 'the', 'destination', 'via', 'a', 'se... | [-0.21570291236537642, -0.003970567663792347, -0.07566168640214938, 0.005942404542076418, -0.10104438795540546, -0.3469001670290674, 0.16013296080147363, 0.38943260127942764, -0.3450898445665733, -0.16121474025403648, 0.11522371787940407, -0.2726757298610383, -0.1656197719896296, 0.10824066272914204, -0.106316534926386... |
1,801.03154 | Holographic Lifshitz superconductors: Analytic solution | We construct an analytic solution for a one-parameter family of holographic
superconductors in asymptotically Lifshitz spacetimes. We utilize this solution
to explore various properties of the systems such as (1) the superfluid phase
background and the grand canonical potential, (2) the order parameter response
funct... | hep-th gr-qc | we construct an analytic solution for a oneparameter family of holographic superconductors in asymptotically lifshitz spacetimes we utilize this solution to explore various properties of the systems such as 1 the superfluid phase background and the grand canonical potential 2 the order parameter response function or th... | [['we', 'construct', 'an', 'analytic', 'solution', 'for', 'a', 'oneparameter', 'family', 'of', 'holographic', 'superconductors', 'in', 'asymptotically', 'lifshitz', 'spacetimes', 'we', 'utilize', 'this', 'solution', 'to', 'explore', 'various', 'properties', 'of', 'the', 'systems', 'such', 'as', '1', 'the', 'superfluid'... | [-0.16301375668857018, 0.13922512482947372, -0.07788442713398562, 0.06289640805512971, -0.050193697400628685, -0.12662402536168846, 0.0432711033737382, 0.2825462549962864, -0.23714553065864102, -0.2505677794961601, 0.08982034663940609, -0.330956075131437, -0.17517427064725483, 0.15485632867903962, 0.029787272029575342,... |
1,801.03155 | Morphology and Kinematics of Filaments in the Serpens and Perseus
Molecular Clouds | We present H13CO+ (J=1-0) and HNC (J=1-0) maps of regions in Serpens South,
Serpens Main and NGC 1333 containing filaments. We also observe the Serpens
regions using H13CN (J=1-0). These dense gas tracer molecular line observations
carried out with CARMA have an angular resolution of ~7", a spectral resolution
of ~0.... | astro-ph.GA astro-ph.SR | we present h13co j10 and hnc j10 maps of regions in serpens south serpens main and ngc 1333 containing filaments we also observe the serpens regions using h13cn j10 these dense gas tracer molecular line observations carried out with carma have an angular resolution of 7 a spectral resolution of 016 kms and a sensitivit... | [['we', 'present', 'h13co', 'j10', 'and', 'hnc', 'j10', 'maps', 'of', 'regions', 'in', 'serpens', 'south', 'serpens', 'main', 'and', 'ngc', '1333', 'containing', 'filaments', 'we', 'also', 'observe', 'the', 'serpens', 'regions', 'using', 'h13cn', 'j10', 'these', 'dense', 'gas', 'tracer', 'molecular', 'line', 'observati... | [-0.09363288312690037, 0.08787010591748351, -0.008404589700512588, 0.04700218639971519, -0.02017686176642945, -0.013753897590901364, -0.03803245800187473, 0.5339829397980462, -0.208910887950862, -0.3131454557349736, 0.05569872198552316, -0.2517311012996784, -0.02878873922692781, 0.108655336297604, 0.07046164316894978, ... |
1,801.03156 | Asymmetric information capacities of reciprocal pairs of quantum
channels | Reciprocal pairs of quantum channels are defined as completely positive
transformations which admit a rigid, distance-preserving, yet not
completely-positive transformation that allows to reproduce the outcome of one
from the corresponding outcome of the other. From a classical perspective these
transmission lines sh... | quant-ph | reciprocal pairs of quantum channels are defined as completely positive transformations which admit a rigid distancepreserving yet not completelypositive transformation that allows to reproduce the outcome of one from the corresponding outcome of the other from a classical perspective these transmission lines should ex... | [['reciprocal', 'pairs', 'of', 'quantum', 'channels', 'are', 'defined', 'as', 'completely', 'positive', 'transformations', 'which', 'admit', 'a', 'rigid', 'distancepreserving', 'yet', 'not', 'completelypositive', 'transformation', 'that', 'allows', 'to', 'reproduce', 'the', 'outcome', 'of', 'one', 'from', 'the', 'corre... | [-0.19236081743331038, 0.14023721696484195, -0.0837176612357756, 0.06619495255137353, -0.0663238621108528, -0.22147346941117002, 0.06826979576879622, 0.3680238560528347, -0.28749182129180745, -0.2430495361576935, 0.053041658227907885, -0.2543547734785534, -0.15975614150001524, 0.20498273835370415, -0.05608750702078013,... |
1,801.03157 | The massive Dirac equation in the Kerr-Newman-de Sitter and Kerr-Newman
black hole spacetimes | Exact solutions of the Dirac general relativistic equation (DE) that describe
the dynamics of a massive, electrically charged particle with half-integer spin
in the curved spacetime geometry of an electrically charged, rotating
Kerr-Newman-(anti) de Sitter black hole (BH) are investigated. We first, derive
the DE in ... | gr-qc astro-ph.GA hep-th math-ph math.MP | exact solutions of the dirac general relativistic equation de that describe the dynamics of a massive electrically charged particle with halfinteger spin in the curved spacetime geometry of an electrically charged rotating kerrnewmananti de sitter black hole bh are investigated we first derive the de in the kerrnewmand... | [['exact', 'solutions', 'of', 'the', 'dirac', 'general', 'relativistic', 'equation', 'de', 'that', 'describe', 'the', 'dynamics', 'of', 'a', 'massive', 'electrically', 'charged', 'particle', 'with', 'halfinteger', 'spin', 'in', 'the', 'curved', 'spacetime', 'geometry', 'of', 'an', 'electrically', 'charged', 'rotating',... | [-0.16590421997317847, 0.10078433258155549, -0.10697806961830303, 0.10791189729480456, -0.08318857092027229, -0.12820245410110934, -0.037561581524151726, 0.2562123480589783, -0.20619119694357382, -0.2585488614487521, 0.06978410335566439, -0.3025006181395329, -0.09230628762565923, 0.1736089178808496, -0.0060858224214761... |
1,801.03158 | Stabbing Pairwise Intersecting Disks by Five Points | Suppose we are given a set $\mathcal{D}$ of $n$ pairwise intersecting disks
in the plane. A planar point set $P$ stabs $\mathcal{D}$ if and only if each
disk in $\mathcal{D}$ contains at least one point from $P$. We present a
deterministic algorithm that takes $O(n)$ time to find five points that stab
$\mathcal{D}$. ... | cs.CG | suppose we are given a set mathcald of n pairwise intersecting disks in the plane a planar point set p stabs mathcald if and only if each disk in mathcald contains at least one point from p we present a deterministic algorithm that takes on time to find five points that stab mathcald furthermore we give a simple exampl... | [['suppose', 'we', 'are', 'given', 'a', 'set', 'mathcald', 'of', 'n', 'pairwise', 'intersecting', 'disks', 'in', 'the', 'plane', 'a', 'planar', 'point', 'set', 'p', 'stabs', 'mathcald', 'if', 'and', 'only', 'if', 'each', 'disk', 'in', 'mathcald', 'contains', 'at', 'least', 'one', 'point', 'from', 'p', 'we', 'present', ... | [-0.1651015006051094, 0.07896234463195655, -0.09079979958457757, 0.015459201219326825, -0.04399500169123696, -0.17270868388622734, 0.08004735598126345, 0.3798993949869038, -0.25865192081371274, -0.22699466618025196, 0.07701180598274104, -0.3136162236827401, -0.14958523721145714, 0.18593418151469884, -0.0640105847310505... |
1,801.03159 | Design, status and perspective of the Mu2e crystal calorimeter | The Mu2e experiment at Fermilab will search for the charged lepton flavor
violating process of neutrino-less $\mu \to e$ coherent conversion in the field
of an aluminum nucleus. Mu2e will reach a single event sensitivity of about
$2.5\cdot 10^{-17}$ that corresponds to four orders of magnitude improvements
with respe... | physics.ins-det hep-ex | the mu2e experiment at fermilab will search for the charged lepton flavor violating process of neutrinoless mu to e coherent conversion in the field of an aluminum nucleus mu2e will reach a single event sensitivity of about 25cdot 1017 that corresponds to four orders of magnitude improvements with respect to the curren... | [['the', 'mu2e', 'experiment', 'at', 'fermilab', 'will', 'search', 'for', 'the', 'charged', 'lepton', 'flavor', 'violating', 'process', 'of', 'neutrinoless', 'mu', 'to', 'e', 'coherent', 'conversion', 'in', 'the', 'field', 'of', 'an', 'aluminum', 'nucleus', 'mu2e', 'will', 'reach', 'a', 'single', 'event', 'sensitivity'... | [-0.07417326291775977, 0.19030875424455715, -0.012944410035551406, -0.003335258542089529, -0.030329740444692423, -0.11866263525725222, 0.021644211004386803, 0.3558008161216632, -0.17315088677834592, -0.3750752503876764, 0.055625522209863575, -0.35524597093716365, 0.02712619240351376, 0.14406039825716646, -0.00599043187... |
1,801.0316 | A Formalization of Kant's Second Formulation of the Categorical
Imperative | We present a formalization and computational implementation of the second
formulation of Kant's categorical imperative. This ethical principle requires
an agent to never treat someone merely as a means but always also as an end.
Here we interpret this principle in terms of how persons are causally affected
by actions... | cs.AI | we present a formalization and computational implementation of the second formulation of kants categorical imperative this ethical principle requires an agent to never treat someone merely as a means but always also as an end here we interpret this principle in terms of how persons are causally affected by actions we i... | [['we', 'present', 'a', 'formalization', 'and', 'computational', 'implementation', 'of', 'the', 'second', 'formulation', 'of', 'kants', 'categorical', 'imperative', 'this', 'ethical', 'principle', 'requires', 'an', 'agent', 'to', 'never', 'treat', 'someone', 'merely', 'as', 'a', 'means', 'but', 'always', 'also', 'as', ... | [-0.06452184057915811, 0.0839230941834052, -0.09573252396853445, 0.11209288827254327, -0.17725399991992366, -0.1642225110427952, 0.08809528960781238, 0.370225000533868, -0.2921377293361755, -0.3078023062081083, 0.10228109658431991, -0.2387941303079658, -0.1808470389199235, 0.14604774344927415, -0.22610497515656186, -0.... |
1,801.03161 | Resolving zero-divisors using Hensel lifting | Algorithms which compute modulo triangular sets must respect the presence of
zero-divisors. We present Hensel lifting as a tool for dealing with them. We
give an application: a modular algorithm for computing GCDs of univariate
polynomials with coefficients modulo a radical triangular set over the
rationals. Our modu... | cs.SC | algorithms which compute modulo triangular sets must respect the presence of zerodivisors we present hensel lifting as a tool for dealing with them we give an application a modular algorithm for computing gcds of univariate polynomials with coefficients modulo a radical triangular set over the rationals our modular alg... | [['algorithms', 'which', 'compute', 'modulo', 'triangular', 'sets', 'must', 'respect', 'the', 'presence', 'of', 'zerodivisors', 'we', 'present', 'hensel', 'lifting', 'as', 'a', 'tool', 'for', 'dealing', 'with', 'them', 'we', 'give', 'an', 'application', 'a', 'modular', 'algorithm', 'for', 'computing', 'gcds', 'of', 'un... | [-0.12400733762249154, -0.0462796313220583, -0.11933520321097028, 0.009235858984634672, -0.0794195100591567, -0.15294533382831632, -0.01800131267641279, 0.3618646552081612, -0.31480102210403665, -0.28143927049715883, 0.08757641048654669, -0.22259139934383138, -0.17825363347870543, 0.2767064062094218, -0.078440628186064... |
1,801.03162 | NP-Completeness and Inapproximability of the Virtual Network Embedding
Problem and Its Variants | Many resource allocation problems in the cloud can be described as a basic
Virtual Network Embedding Problem (VNEP): the problem of finding a mapping of a
request graph (describing a workload) onto a substrate graph (describing the
physical infrastructure). Applications range from mapping testbeds (from where
the pro... | cs.NI cs.CC | many resource allocation problems in the cloud can be described as a basic virtual network embedding problem vnep the problem of finding a mapping of a request graph describing a workload onto a substrate graph describing the physical infrastructure applications range from mapping testbeds from where the problem origin... | [['many', 'resource', 'allocation', 'problems', 'in', 'the', 'cloud', 'can', 'be', 'described', 'as', 'a', 'basic', 'virtual', 'network', 'embedding', 'problem', 'vnep', 'the', 'problem', 'of', 'finding', 'a', 'mapping', 'of', 'a', 'request', 'graph', 'describing', 'a', 'workload', 'onto', 'a', 'substrate', 'graph', 'd... | [-0.1337431631827106, 0.012645063905178435, -0.06417285782905917, 0.06413100013465044, -0.10837522002957052, -0.15556748666179676, 0.12281977420595164, 0.38525663027096363, -0.31146324710765233, -0.3470759802719667, 0.12740578254673718, -0.22692560560203023, -0.14901205390203923, 0.2064611259531895, -0.1023595531737165... |
1,801.03163 | Sufficient Conditions for the Tightness of Shannon's Capacity Bounds for
Two-Way Channels | New sufficient conditions for determining in closed form the capacity region
of point-to-point memoryless two-way channels (TWCs) are derived. The proposed
conditions not only relax Shannon's condition which can identify only TWCs with
a certain symmetry property but also generalize other existing results.
Examples a... | cs.IT math.IT | new sufficient conditions for determining in closed form the capacity region of pointtopoint memoryless twoway channels twcs are derived the proposed conditions not only relax shannons condition which can identify only twcs with a certain symmetry property but also generalize other existing results examples are given t... | [['new', 'sufficient', 'conditions', 'for', 'determining', 'in', 'closed', 'form', 'the', 'capacity', 'region', 'of', 'pointtopoint', 'memoryless', 'twoway', 'channels', 'twcs', 'are', 'derived', 'the', 'proposed', 'conditions', 'not', 'only', 'relax', 'shannons', 'condition', 'which', 'can', 'identify', 'only', 'twcs'... | [-0.19625800292231832, 0.07419248355587048, -0.03292874867717425, 0.06202465820091742, -0.11037832247179553, -0.2656629397965002, 0.06643271012473162, 0.3617662461129604, -0.27955349658926326, -0.2305581117807715, 0.12091853866931396, -0.15728838928043842, -0.12440386477909568, 0.2317656679768805, -0.1356061875040824, ... |
1,801.03164 | Paranom: A Parallel Anomaly Dataset Generator | In this paper, we present Paranom, a parallel anomaly dataset generator. We
discuss its design and provide brief experimental results demonstrating its
usefulness in improving the classification correctness of LSTM-AD, a
state-of-the-art anomaly detection model.
| cs.LG cs.AI stat.ML | in this paper we present paranom a parallel anomaly dataset generator we discuss its design and provide brief experimental results demonstrating its usefulness in improving the classification correctness of lstmad a stateoftheart anomaly detection model | [['in', 'this', 'paper', 'we', 'present', 'paranom', 'a', 'parallel', 'anomaly', 'dataset', 'generator', 'we', 'discuss', 'its', 'design', 'and', 'provide', 'brief', 'experimental', 'results', 'demonstrating', 'its', 'usefulness', 'in', 'improving', 'the', 'classification', 'correctness', 'of', 'lstmad', 'a', 'stateoft... | [-0.14802001042743074, -0.09341262911700389, -0.04220442016340905, 0.0004294495288790627, -0.12362077736267538, -0.10463811214448827, 0.056159931062156276, 0.4160819550919713, -0.17519279079737538, -0.34696455186966696, 0.14933699583211404, -0.27343903112253454, -0.2227634373262073, 0.19842772964021246, -0.128727257971... |
1,801.03165 | Algebraic differential formulas for the shuffle, stuffle and duality
relations of iterated integrals | In this paper we prove certain algebraic identities, which correspond to
differentiations of the shuffle relation, the stuffle relation, and the
relations which arise from M\"obius transformations of iterated integrals.
These formulas provide fundamental and useful tools in the study of iterated
integrals on a punctu... | math.NT math.CO | in this paper we prove certain algebraic identities which correspond to differentiations of the shuffle relation the stuffle relation and the relations which arise from mobius transformations of iterated integrals these formulas provide fundamental and useful tools in the study of iterated integrals on a punctured proj... | [['in', 'this', 'paper', 'we', 'prove', 'certain', 'algebraic', 'identities', 'which', 'correspond', 'to', 'differentiations', 'of', 'the', 'shuffle', 'relation', 'the', 'stuffle', 'relation', 'and', 'the', 'relations', 'which', 'arise', 'from', 'mobius', 'transformations', 'of', 'iterated', 'integrals', 'these', 'form... | [-0.18889403296634555, 0.04491184569390801, -0.13244991450725743, 0.15039984360676803, -0.1159511834460621, -0.09389872507502635, 0.0726058624010572, 0.29492740959782776, -0.3684527240693569, -0.23024450595645854, 0.107456724823957, -0.22930560578242876, -0.2522882304037921, 0.2500431240381052, -0.0942971882841448, 0.0... |
1,801.03166 | Compton thick AGN in the NuSTAR era | We present the 2-100 keV spectral analysis of 30 candidate Compton thick
(CT-) active galactic nuclei (AGN) selected in the Swift-BAT 100-month survey.
The average redshift of these objects is $\langle z\rangle\sim$0.03 and they
all lie within $\sim$500 Mpc. We used the MyTorus (Murphy et al. 2009) model to
perform X... | astro-ph.HE | we present the 2100 kev spectral analysis of 30 candidate compton thick ct active galactic nuclei agn selected in the swiftbat 100month survey the average redshift of these objects is langle zranglesim003 and they all lie within sim500 mpc we used the mytorus murphy et al 2009 model to perform xray spectral fitting bot... | [['we', 'present', 'the', '2100', 'kev', 'spectral', 'analysis', 'of', '30', 'candidate', 'compton', 'thick', 'ct', 'active', 'galactic', 'nuclei', 'agn', 'selected', 'in', 'the', 'swiftbat', '100month', 'survey', 'the', 'average', 'redshift', 'of', 'these', 'objects', 'is', 'langle', 'zranglesim003', 'and', 'they', 'a... | [-0.008068613250575521, 0.09348514784702702, -0.02115889984073446, 0.11158777131657938, -0.07238291298477527, -0.05935357229181511, 0.09932333590764114, 0.45778938382864, -0.1536614477086593, -0.4392414471014704, 0.06312376389978454, -0.3679464301231372, 0.05542877869105295, 0.18919646818026462, -0.021326105320579648, ... |
1,801.03167 | SN 2016X: A Type II-P Supernova with A Signature of Shock Breakout from
Explosion of A Massive Red Supergiant | We present extensive ultraviolet (UV) and optical photometry, as well as
dense optical spectroscopy for type II Plateau (IIP) supernova SN 2016X that
exploded in the nearby ($\sim$ 15 Mpc) spiral galaxy UGC 08041. The
observations span the period from 2 to 180 days after the explosion; in
particular, the Swift UV dat... | astro-ph.HE astro-ph.SR | we present extensive ultraviolet uv and optical photometry as well as dense optical spectroscopy for type ii plateau iip supernova sn 2016x that exploded in the nearby sim 15 mpc spiral galaxy ugc 08041 the observations span the period from 2 to 180 days after the explosion in particular the swift uv data probably capt... | [['we', 'present', 'extensive', 'ultraviolet', 'uv', 'and', 'optical', 'photometry', 'as', 'well', 'as', 'dense', 'optical', 'spectroscopy', 'for', 'type', 'ii', 'plateau', 'iip', 'supernova', 'sn', '2016x', 'that', 'exploded', 'in', 'the', 'nearby', 'sim', '15', 'mpc', 'spiral', 'galaxy', 'ugc', '08041', 'the', 'obser... | [-0.017168457786440206, 0.09069848601349553, -0.05292188537012031, 0.10932923210503791, -0.11574772136097228, -0.12296642876302438, 0.06789335325522879, 0.4607549573712308, -0.12430477584862744, -0.3378240741982028, 0.09532157125368972, -0.33619271695063396, 0.0007628956889926359, 0.22710554193050986, -0.05663096497301... |
1,801.03168 | Greenhouse: A Zero-Positive Machine Learning System for Time-Series
Anomaly Detection | This short paper describes our ongoing research on Greenhouse - a
zero-positive machine learning system for time-series anomaly detection.
| cs.AI | this short paper describes our ongoing research on greenhouse a zeropositive machine learning system for timeseries anomaly detection | [['this', 'short', 'paper', 'describes', 'our', 'ongoing', 'research', 'on', 'greenhouse', 'a', 'zeropositive', 'machine', 'learning', 'system', 'for', 'timeseries', 'anomaly', 'detection']] | [-0.16116209202172124, 0.030822432545178077, -0.05861886984819327, 0.029764955062145257, -0.13520430926890933, -0.13078499494997017, 0.05510374986539211, 0.35146753588581786, -0.23131502844283686, -0.2815121217247318, 0.1612047406242174, -0.3231681718984071, -0.2558176517486572, 0.27004503809353886, -0.2022071293664767... |
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