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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709.1535 | Comments on "The Coronal Heating Paradox" by M.J. Aschwanden, A.
Winebarger, D. Tsiklauri and H. Peter [2007, Astrophys J., 659, 1673] | We point out the priority of our paper (Mahajan et al. 2001, Phys. Plasmas,
8, 1340) over (Aschwanden et al. 2007, Astrophys J., 659, 1673) in introducing
the term "Formation and primary heating of the solar corona" working out
explicit models (theory as well as simulation) for coronal structure formation
and heating... | astro-ph | we point out the priority of our paper mahajan et al 2001 phys plasmas 8 1340 over aschwanden et al 2007 astrophys j 659 1673 in introducing the term formation and primary heating of the solar corona working out explicit models theory as well as simulation for coronal structure formation and heating on analyzing the as... | [['we', 'point', 'out', 'the', 'priority', 'of', 'our', 'paper', 'mahajan', 'et', 'al', '2001', 'phys', 'plasmas', '8', '1340', 'over', 'aschwanden', 'et', 'al', '2007', 'astrophys', 'j', '659', '1673', 'in', 'introducing', 'the', 'term', 'formation', 'and', 'primary', 'heating', 'of', 'the', 'solar', 'corona', 'workin... | [-0.10253467036405417, 0.20452586866133374, -0.00509669125241078, 0.08235714813047336, -0.07804615069525661, -0.049260503559640643, 0.0542700678271092, 0.36846580168370296, -0.1947922784616642, -0.3594962950496946, 0.08070504734146029, -0.23026021474679173, -0.10540533123859837, 0.19972674222663045, -0.0811118926196488... |
709.1536 | Influence of deterministic trend on the estimated parameters of
GARCH(1,1) model | The log returns of financial time series are usually modeled by means of the
stationary GARCH(1,1) stochastic process or its generalizations which can not
properly describe the nonstationary deterministic components of the original
series. We analyze the influence of deterministic trends on the GARCH(1,1)
parameters ... | q-fin.ST physics.data-an | the log returns of financial time series are usually modeled by means of the stationary garch11 stochastic process or its generalizations which can not properly describe the nonstationary deterministic components of the original series we analyze the influence of deterministic trends on the garch11 parameters using mon... | [['the', 'log', 'returns', 'of', 'financial', 'time', 'series', 'are', 'usually', 'modeled', 'by', 'means', 'of', 'the', 'stationary', 'garch11', 'stochastic', 'process', 'or', 'its', 'generalizations', 'which', 'can', 'not', 'properly', 'describe', 'the', 'nonstationary', 'deterministic', 'components', 'of', 'the', 'o... | [-0.06788432254806169, 0.12651384141175978, -0.07645250570720001, 0.12051195069176585, -0.020313364731508396, -0.10635067462815993, 0.030751901727560305, 0.3983241781862753, -0.29274254359094604, -0.26663984527723156, 0.14127658197145548, -0.2854846733351869, -0.15452327766087687, 0.23438757163615176, -0.03278342937119... |
709.1537 | Asymptotic Behaviour of Parameter Ideals in Generalized Cohen-Macaulay
Modules | The purpose of this paper is to give affirmative answers to two open
questions as follows. Let $(R, \m)$ be a generalized Cohen-Macaulay Noetherian
local ring. Both questions, the first question was raised by M. Rogers \cite
{R} and the second one is due to S. Goto and H. Sakurai \cite {GS1}, ask
whether for every pa... | math.AC | the purpose of this paper is to give affirmative answers to two open questions as follows let r m be a generalized cohenmacaulay noetherian local ring both questions the first question was raised by m rogers cite r and the second one is due to s goto and h sakurai cite gs1 ask whether for every parameter ideal q contai... | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'give', 'affirmative', 'answers', 'to', 'two', 'open', 'questions', 'as', 'follows', 'let', 'r', 'm', 'be', 'a', 'generalized', 'cohenmacaulay', 'noetherian', 'local', 'ring', 'both', 'questions', 'the', 'first', 'question', 'was', 'raised', 'by', 'm', 'rogers', 'c... | [-0.1472501000108013, 0.0954786609975969, -0.029333997630401627, 0.056434568378480744, -0.08091960215408887, -0.23895834848939718, 0.012353438772721687, 0.27210912598644965, -0.3150872841968641, -0.26873651830540907, 0.11728562872503771, -0.2566870476456953, -0.0590728512332854, 0.16612867724692837, -0.1396820926527073... |
709.1538 | Representing complex data using localized principal components with
application to astronomical data | Often the relation between the variables constituting a multivariate data
space might be characterized by one or more of the terms: ``nonlinear'',
``branched'', ``disconnected'', ``bended'', ``curved'', ``heterogeneous'', or,
more general, ``complex''. In these cases, simple principal component analysis
(PCA) as a to... | astro-ph | often the relation between the variables constituting a multivariate data space might be characterized by one or more of the terms nonlinear branched disconnected bended curved heterogeneous or more general complex in these cases simple principal component analysis pca as a tool for dimension reduction can fail badly o... | [['often', 'the', 'relation', 'between', 'the', 'variables', 'constituting', 'a', 'multivariate', 'data', 'space', 'might', 'be', 'characterized', 'by', 'one', 'or', 'more', 'of', 'the', 'terms', 'nonlinear', 'branched', 'disconnected', 'bended', 'curved', 'heterogeneous', 'or', 'more', 'general', 'complex', 'in', 'the... | [-0.10044411074909601, 0.028894567360310774, -0.08460305859156646, 0.11173507812161945, -0.10274274257530809, -0.1683311216975944, 0.002744015722912151, 0.37882102810131396, -0.29711494924655807, -0.25272438769315275, 0.1565204143251898, -0.28443087713507925, -0.17019952372953173, 0.22479243699812376, -0.05395120680790... |
709.1539 | The Set of Prime Numbers | In this work we show that the prime distribution is deterministic. Indeed the
set of prime numbers P can be expressed in terms of two subsets of N using
three specific selection rules, acting on two sets of prime candidates. The
prime candidates are obtained in terms of the first perfect number. The
asymptotic behavi... | math.GM | in this work we show that the prime distribution is deterministic indeed the set of prime numbers p can be expressed in terms of two subsets of n using three specific selection rules acting on two sets of prime candidates the prime candidates are obtained in terms of the first perfect number the asymptotic behaviour is... | [['in', 'this', 'work', 'we', 'show', 'that', 'the', 'prime', 'distribution', 'is', 'deterministic', 'indeed', 'the', 'set', 'of', 'prime', 'numbers', 'p', 'can', 'be', 'expressed', 'in', 'terms', 'of', 'two', 'subsets', 'of', 'n', 'using', 'three', 'specific', 'selection', 'rules', 'acting', 'on', 'two', 'sets', 'of',... | [-0.2180371607866991, 0.11882093956806916, -0.06183409756498344, 0.07221928596389984, -0.04728179890101394, -0.10176730594676302, 0.03322122416582452, 0.294201171653996, -0.24097218408799134, -0.33481374779626366, 0.036414692056342866, -0.27717712834051034, -0.08717821443352444, 0.23948077139085586, -0.0101297402709542... |
709.154 | A dynamic density functional theory for particles in a flowing solvent | We present a dynamic density functional theory (dDFT) which takes into accou
nt the advection of the particles by a flowing solvent. For potential flows we
can use the same closure as in the absence of solvent flow. The structure of
the resulting advected dDFT suggests that it could be used for non-potential
flows as... | cond-mat.soft cond-mat.stat-mech | we present a dynamic density functional theory ddft which takes into accou nt the advection of the particles by a flowing solvent for potential flows we can use the same closure as in the absence of solvent flow the structure of the resulting advected ddft suggests that it could be used for nonpotential flows as well w... | [['we', 'present', 'a', 'dynamic', 'density', 'functional', 'theory', 'ddft', 'which', 'takes', 'into', 'accou', 'nt', 'the', 'advection', 'of', 'the', 'particles', 'by', 'a', 'flowing', 'solvent', 'for', 'potential', 'flows', 'we', 'can', 'use', 'the', 'same', 'closure', 'as', 'in', 'the', 'absence', 'of', 'solvent', ... | [-0.09369941913090381, 0.15438241700836183, -0.1389537494341355, 0.033557623931777754, -0.015404126207743372, -0.0713764111999245, -0.015122128677571059, 0.3430616613532904, -0.2786410462964947, -0.30031430604036097, 0.053867822495660564, -0.24838988359815198, -0.157815090059081, 0.16265408046768112, -0.032317908212245... |
709.1541 | Propagation of high-energy cosmic rays in extragalactic turbulent
magnetic fields: resulting energy spectrum and composition | We extend previous studies of mixed-composition extragalactic cosmic-ray
source models, by investigating the influence of a non-negligible extragalactic
magnetic field on the propagated cosmic-ray spectrum and composition. We study
the transport of charged particles in turbulent fields and the transition from
a balli... | astro-ph | we extend previous studies of mixedcomposition extragalactic cosmicray source models by investigating the influence of a nonnegligible extragalactic magnetic field on the propagated cosmicray spectrum and composition we study the transport of charged particles in turbulent fields and the transition from a ballistic to ... | [['we', 'extend', 'previous', 'studies', 'of', 'mixedcomposition', 'extragalactic', 'cosmicray', 'source', 'models', 'by', 'investigating', 'the', 'influence', 'of', 'a', 'nonnegligible', 'extragalactic', 'magnetic', 'field', 'on', 'the', 'propagated', 'cosmicray', 'spectrum', 'and', 'composition', 'we', 'study', 'the'... | [-0.11001364540759108, 0.18818384593306872, -0.07492600291295619, 0.10645976980583223, -0.05824935724042722, -0.05494565186930484, 0.02656964410752913, 0.3669694655681731, -0.24457329301713188, -0.32749608015549964, -0.0017083889182626468, -0.2656867058403059, -0.059132435366456, 0.20080692356272953, 0.0313896524422176... |
709.1542 | Coherent single atom shuttle between two Bose-Einstein condensates | We study an atomic quantum dot representing a single hyperfine "impurity"
atom which is coherently coupled to two well-separated Bose-Einstein
condensates, in the limit when the coupling between the dot and the condensates
dominates the inter-condensate tunneling coupling. It is demonstrated that the
quantum dot by i... | cond-mat.other quant-ph | we study an atomic quantum dot representing a single hyperfine impurity atom which is coherently coupled to two wellseparated boseeinstein condensates in the limit when the coupling between the dot and the condensates dominates the intercondensate tunneling coupling it is demonstrated that the quantum dot by itself can... | [['we', 'study', 'an', 'atomic', 'quantum', 'dot', 'representing', 'a', 'single', 'hyperfine', 'impurity', 'atom', 'which', 'is', 'coherently', 'coupled', 'to', 'two', 'wellseparated', 'boseeinstein', 'condensates', 'in', 'the', 'limit', 'when', 'the', 'coupling', 'between', 'the', 'dot', 'and', 'the', 'condensates', '... | [-0.18412983313673872, 0.23879353144646345, -0.04809465469128784, 0.041688543128855955, 0.007998706023583466, -0.20627617756782593, 0.011848242980181828, 0.34071919409793683, -0.2588810494347561, -0.2664282577588683, -0.0369537419267534, -0.29291928378734156, -0.09505174002856359, 0.17587623072001313, 0.072701379280616... |
709.1543 | Kinetic Exchange Models for Income and Wealth Distributions | Increasingly, a huge amount of statistics have been gathered which clearly
indicates that income and wealth distributions in various countries or
societies follow a robust pattern, close to the Gibbs distribution of energy in
an ideal gas in equilibrium. However, it also deviates in the low income and
more significan... | q-fin.GN cond-mat.stat-mech nlin.AO physics.soc-ph | increasingly a huge amount of statistics have been gathered which clearly indicates that income and wealth distributions in various countries or societies follow a robust pattern close to the gibbs distribution of energy in an ideal gas in equilibrium however it also deviates in the low income and more significantly fo... | [['increasingly', 'a', 'huge', 'amount', 'of', 'statistics', 'have', 'been', 'gathered', 'which', 'clearly', 'indicates', 'that', 'income', 'and', 'wealth', 'distributions', 'in', 'various', 'countries', 'or', 'societies', 'follow', 'a', 'robust', 'pattern', 'close', 'to', 'the', 'gibbs', 'distribution', 'of', 'energy'... | [-0.01039547445304664, 0.12754292564953976, -0.1803041159786951, 0.15639197489997345, -0.05463344637485249, -0.11382263707719854, 0.07368588282678054, 0.34950881907299386, -0.24190088070984653, -0.3532204267971996, 0.07903040870468118, -0.31971372401953413, -0.07252201831677178, 0.22976520144269427, -0.0994912754716490... |
709.1544 | A radiative transfer scheme for cosmological reionization based on a
local Eddington tensor | A radiative transfer scheme is presented, based on a moment description of
the equation of radiative transfer and the so-called ``M1 closure model'' for
the Eddington tensor. This model features a strictly hyperbolic transport step
for radiation: it has been implemented using standard Godunov--like techniques
in a ne... | astro-ph | a radiative transfer scheme is presented based on a moment description of the equation of radiative transfer and the socalled m1 closure model for the eddington tensor this model features a strictly hyperbolic transport step for radiation it has been implemented using standard godunovlike techniques in a new code calle... | [['a', 'radiative', 'transfer', 'scheme', 'is', 'presented', 'based', 'on', 'a', 'moment', 'description', 'of', 'the', 'equation', 'of', 'radiative', 'transfer', 'and', 'the', 'socalled', 'm1', 'closure', 'model', 'for', 'the', 'eddington', 'tensor', 'this', 'model', 'features', 'a', 'strictly', 'hyperbolic', 'transpor... | [-0.04961841224329704, 0.06285911068414986, -0.07131480205393696, 0.09102467957576263, -0.06859547217076613, -0.14061626868117286, 0.00014195400852536373, 0.36300969029326874, -0.23790533348554904, -0.2846351319892427, 0.07904579508378785, -0.2298787756649367, -0.06910482330142444, 0.22496726039907564, 0.00402053070458... |
709.1545 | A non-linear dynamical systems approach to source compression for
constrained sources | We have recently established a strong connection between the Tent map (also
known as Generalized Luroth Series or GLS which is a chaotic, ergodic and
lebesgue measure preserving non-linear dynamical system) and Arithmetic coding
which is a popular source compression algorithm used in international
compression standar... | nlin.CD | we have recently established a strong connection between the tent map also known as generalized luroth series or gls which is a chaotic ergodic and lebesgue measure preserving nonlinear dynamical system and arithmetic coding which is a popular source compression algorithm used in international compression standards suc... | [['we', 'have', 'recently', 'established', 'a', 'strong', 'connection', 'between', 'the', 'tent', 'map', 'also', 'known', 'as', 'generalized', 'luroth', 'series', 'or', 'gls', 'which', 'is', 'a', 'chaotic', 'ergodic', 'and', 'lebesgue', 'measure', 'preserving', 'nonlinear', 'dynamical', 'system', 'and', 'arithmetic', '... | [-0.1272567668271185, 0.10914171935821121, -0.0802549451796545, 0.09893029402574581, -0.04026193635343019, -0.17264859112228897, 0.09211513210167976, 0.4023373025949254, -0.3655124876384783, -0.18817522590791788, 0.158631607958332, -0.2876197283551323, -0.17335058364433922, 0.20084091719778518, -0.14424270840662748, 0.... |
709.1546 | Combinatorics of the Dimer Model on a Strip | In this note, we give a closed formula for the partition function of the
dimer model living on a (2 x n) strip of squares or hexagons on the torus for
arbitrary even n. The result is derived in two ways, by using a Potts model
like description for the dimers, and via a recursion relation that was obtained
from a map ... | math.CO cond-mat.stat-mech hep-th | in this note we give a closed formula for the partition function of the dimer model living on a 2 x n strip of squares or hexagons on the torus for arbitrary even n the result is derived in two ways by using a potts model like description for the dimers and via a recursion relation that was obtained from a map to a 1d ... | [['in', 'this', 'note', 'we', 'give', 'a', 'closed', 'formula', 'for', 'the', 'partition', 'function', 'of', 'the', 'dimer', 'model', 'living', 'on', 'a', '2', 'x', 'n', 'strip', 'of', 'squares', 'or', 'hexagons', 'on', 'the', 'torus', 'for', 'arbitrary', 'even', 'n', 'the', 'result', 'is', 'derived', 'in', 'two', 'way... | [-0.13540268617667137, 0.07445508095696168, -0.06875034565887143, 0.05163074975773212, -0.0369202492818717, -0.1378598565696388, 0.07664224693691858, 0.323854216925239, -0.25327074119660964, -0.30908906127336205, 0.10930942583538752, -0.2870534532002464, -0.15307338900303327, 0.1904547394188221, -0.012970244521976159, ... |
709.1547 | Finite Temperature Large N Gauge Theory with Quarks in an External
Magnetic Field | Using a ten dimensional dual string background, we study aspects of the
physics of finite temperature large N four dimensional SU(N) gauge theory,
focusing on the dynamics of fundamental quarks in the presence of a background
magnetic field. At vanishing temperature and magnetic field, the theory has N=2
supersymmetr... | hep-th | using a ten dimensional dual string background we study aspects of the physics of finite temperature large n four dimensional sun gauge theory focusing on the dynamics of fundamental quarks in the presence of a background magnetic field at vanishing temperature and magnetic field the theory has n2 supersymmetry and the... | [['using', 'a', 'ten', 'dimensional', 'dual', 'string', 'background', 'we', 'study', 'aspects', 'of', 'the', 'physics', 'of', 'finite', 'temperature', 'large', 'n', 'four', 'dimensional', 'sun', 'gauge', 'theory', 'focusing', 'on', 'the', 'dynamics', 'of', 'fundamental', 'quarks', 'in', 'the', 'presence', 'of', 'a', 'b... | [-0.1334021145064356, 0.27389039492943507, -0.0864968541589324, 0.061403773700707216, -0.03232031339195682, -0.09060298605238212, 0.03217423123953892, 0.3410408393160176, -0.18929196588013933, -0.24732547504966385, 0.0640581051589671, -0.2754922716377942, -0.1174356731492331, 0.10282450053257061, 0.042352501951060745, ... |
709.1548 | Conductance enhancement due to the resonant tunneling into the subgap
vortex core states in normal metal/superconductor ballistic junctions | We investigate the low-energy quantum transport in the ballistic normal
metal-insulator -superconductor junction in the presence of magnetic field
creating Abrikosov vortices in the superconductor. Within the Bogolubov- de
Gennes theory we show that the presence of the subgap quasiparticle states
localized within the... | cond-mat.supr-con | we investigate the lowenergy quantum transport in the ballistic normal metalinsulator superconductor junction in the presence of magnetic field creating abrikosov vortices in the superconductor within the bogolubov de gennes theory we show that the presence of the subgap quasiparticle states localized within the vortex... | [['we', 'investigate', 'the', 'lowenergy', 'quantum', 'transport', 'in', 'the', 'ballistic', 'normal', 'metalinsulator', 'superconductor', 'junction', 'in', 'the', 'presence', 'of', 'magnetic', 'field', 'creating', 'abrikosov', 'vortices', 'in', 'the', 'superconductor', 'within', 'the', 'bogolubov', 'de', 'gennes', 'th... | [-0.24769479873376427, 0.1825627983103079, -0.06452376641272033, 0.0425002838792203, -0.01890304659065775, -0.11177498179671096, 0.07530421773391607, 0.3071076408272884, -0.2579790205526792, -0.29886865446374555, -0.036712207918276736, -0.25553963941399804, -0.08795034115920301, 0.16201249896319675, 0.05126688474804529... |
709.1549 | On the Origin of Rapid Flares in TeV Blazars | The rapid variability of the VHE emission reported for some TeV blazars
implies Doppler factors well in excess of those inferred from superluminal
motions and unification schemes. We propose that those extreme flares may
result from radiative deceleration of blobs on scales where local dissipation
occurs. The minimum... | astro-ph | the rapid variability of the vhe emission reported for some tev blazars implies doppler factors well in excess of those inferred from superluminal motions and unification schemes we propose that those extreme flares may result from radiative deceleration of blobs on scales where local dissipation occurs the minimum jet... | [['the', 'rapid', 'variability', 'of', 'the', 'vhe', 'emission', 'reported', 'for', 'some', 'tev', 'blazars', 'implies', 'doppler', 'factors', 'well', 'in', 'excess', 'of', 'those', 'inferred', 'from', 'superluminal', 'motions', 'and', 'unification', 'schemes', 'we', 'propose', 'that', 'those', 'extreme', 'flares', 'ma... | [-0.06327747142035514, 0.2010676867328584, -0.0771125527434051, 0.16787014500517397, -0.10690030651539564, -0.10906400296837092, -0.009430273988458793, 0.45472892773710194, -0.23203274351358413, -0.33908925313036886, 0.024256576699204745, -0.24383495271205902, 0.04649216280132532, 0.24467268137307838, -0.02632601499930... |
709.155 | A particle mechanism for the index of refraction | We propose to go away from the electromagnetic wave description of light and
to explain through a purely corpuscular and neutral approach, the phenomenon of
the slowing down of light in a transparent medium. The quantum predictions and
ours are compared against experimental refractive indices. In our framework the
op... | physics.optics | we propose to go away from the electromagnetic wave description of light and to explain through a purely corpuscular and neutral approach the phenomenon of the slowing down of light in a transparent medium the quantum predictions and ours are compared against experimental refractive indices in our framework the optical... | [['we', 'propose', 'to', 'go', 'away', 'from', 'the', 'electromagnetic', 'wave', 'description', 'of', 'light', 'and', 'to', 'explain', 'through', 'a', 'purely', 'corpuscular', 'and', 'neutral', 'approach', 'the', 'phenomenon', 'of', 'the', 'slowing', 'down', 'of', 'light', 'in', 'a', 'transparent', 'medium', 'the', 'qu... | [-0.0661073773226235, 0.11554072513536084, -0.140016518846096, 0.07321645867341431, -0.09594134663348086, -0.13180140350596048, 0.07886466226409539, 0.39204348891507834, -0.22813413035328267, -0.31282529776581214, 0.06147672214501654, -0.3047650962253101, -0.16672790086158784, 0.24557719479980733, -0.027975951568805613... |
709.1551 | AdS/CFT with Flavour in Electric and Magnetic Kalb-Ramond Fields | We investigate gauge/gravity duals with flavour for which pure-gauge
Kalb-Ramond B fields are turned on in the background, into which a D7 brane
probe is embedded. First we consider the case of a magnetic field in two of the
spatial boundary directions. We show that at finite temperature, i.e. in the
AdS-Schwarzschil... | hep-th | we investigate gaugegravity duals with flavour for which puregauge kalbramond b fields are turned on in the background into which a d7 brane probe is embedded first we consider the case of a magnetic field in two of the spatial boundary directions we show that at finite temperature ie in the adsschwarzschild background... | [['we', 'investigate', 'gaugegravity', 'duals', 'with', 'flavour', 'for', 'which', 'puregauge', 'kalbramond', 'b', 'fields', 'are', 'turned', 'on', 'in', 'the', 'background', 'into', 'which', 'a', 'd7', 'brane', 'probe', 'is', 'embedded', 'first', 'we', 'consider', 'the', 'case', 'of', 'a', 'magnetic', 'field', 'in', '... | [-0.16826933948044293, 0.16785480387503293, -0.0575680700019225, 0.05126921893557545, -0.07357046955047611, -0.10648191125204641, 0.017062659524548465, 0.3696608432975715, -0.2188502691775382, -0.22843574268553785, 0.07599249370898048, -0.2519002158451312, -0.08173959760251873, 0.11523488943303327, -0.02530428939889553... |
709.1552 | Some aspects of infinite range models of spin glasses: theory and
numerical simulations | These notes give an introduction to the physics of the infinite range version
of the Edwards--Anderson model, the so-called Sherrington--Kirkpatrick model.
In a first part, I motivate and introduce the Edwards--Anderson and
Sherrington--Kirkpatrick models. In the second part, I explain the analytical
solution of the ... | cond-mat.dis-nn | these notes give an introduction to the physics of the infinite range version of the edwardsanderson model the socalled sherringtonkirkpatrick model in a first part i motivate and introduce the edwardsanderson and sherringtonkirkpatrick models in the second part i explain the analytical solution of the sherringtonkirkp... | [['these', 'notes', 'give', 'an', 'introduction', 'to', 'the', 'physics', 'of', 'the', 'infinite', 'range', 'version', 'of', 'the', 'edwardsanderson', 'model', 'the', 'socalled', 'sherringtonkirkpatrick', 'model', 'in', 'a', 'first', 'part', 'i', 'motivate', 'and', 'introduce', 'the', 'edwardsanderson', 'and', 'sherrin... | [-0.08278543269174188, 0.0968007225013921, -0.08031196646826495, 0.07205591809365171, -0.056525854414847115, -0.09005483935711402, 0.025041082110676103, 0.25353627977892756, -0.2139359674262429, -0.3084846592851375, 0.09895867751946294, -0.28342977680503983, -0.09925168739365679, 0.12731320960657264, -0.015808873501767... |
709.1553 | Probing Transversity GPDs in Photo and Electroproduction of Two Vector
Mesons | Electroproduction of two mesons well separated in rapidity allows the first
feasible selective access to chiral-odd transversity GPDs provided one of these
mesons is a transversely polarized vector meson rho_T.
| hep-ph nucl-th | electroproduction of two mesons well separated in rapidity allows the first feasible selective access to chiralodd transversity gpds provided one of these mesons is a transversely polarized vector meson rho_t | [['electroproduction', 'of', 'two', 'mesons', 'well', 'separated', 'in', 'rapidity', 'allows', 'the', 'first', 'feasible', 'selective', 'access', 'to', 'chiralodd', 'transversity', 'gpds', 'provided', 'one', 'of', 'these', 'mesons', 'is', 'a', 'transversely', 'polarized', 'vector', 'meson', 'rho_t']] | [-0.14272124947359163, 0.3691952617838979, -0.2059011415888866, 0.20201684070828682, -0.14859486613422632, -0.1479823448540022, 0.04735634090999762, 0.43519739179561534, -0.2109061767657598, 0.03289694550136725, -0.21448453657406694, -0.3211260285310952, 0.09646255411207676, 0.054272500798106194, 0.14319531933094065, 0... |
709.1554 | Quarks in an External Electric Field in Finite Temperature Large N Gauge
Theory | We use a ten dimensional dual string background to aspects of the physics
large N four dimensional SU(N) gauge theory, where its fundamental quarks are
charged under a background electric field. The theory is N=2 supersymmetric for
vanishing temperature and electric field. At zero temperature, we observe that
the ele... | hep-th | we use a ten dimensional dual string background to aspects of the physics large n four dimensional sun gauge theory where its fundamental quarks are charged under a background electric field the theory is n2 supersymmetric for vanishing temperature and electric field at zero temperature we observe that the electric fie... | [['we', 'use', 'a', 'ten', 'dimensional', 'dual', 'string', 'background', 'to', 'aspects', 'of', 'the', 'physics', 'large', 'n', 'four', 'dimensional', 'sun', 'gauge', 'theory', 'where', 'its', 'fundamental', 'quarks', 'are', 'charged', 'under', 'a', 'background', 'electric', 'field', 'the', 'theory', 'is', 'n2', 'supe... | [-0.10975279515731104, 0.31811042645119686, -0.08010076718104149, 0.05198230763660774, -0.01082104560919106, -0.13688262890181727, 0.05264830355724645, 0.31553290133911466, -0.2203634955572881, -0.22378005745214602, 0.004376690913294811, -0.32430703896615243, -0.06528060808814766, 0.08109566235973958, 0.024556024550711... |
709.1555 | Turing structures in dc gas discharges | Self-organized spatial plasma structures exhibit many similarities with
Turing structures obtained in biology and chemistry. Using an analytical
mesoscopic approach it is shown that plasma balls of fire belong to the same
class of Turing structures like the Brusselator. It is also mathematically
proved that the exist... | physics.plasm-ph nlin.AO | selforganized spatial plasma structures exhibit many similarities with turing structures obtained in biology and chemistry using an analytical mesoscopic approach it is shown that plasma balls of fire belong to the same class of turing structures like the brusselator it is also mathematically proved that the existence ... | [['selforganized', 'spatial', 'plasma', 'structures', 'exhibit', 'many', 'similarities', 'with', 'turing', 'structures', 'obtained', 'in', 'biology', 'and', 'chemistry', 'using', 'an', 'analytical', 'mesoscopic', 'approach', 'it', 'is', 'shown', 'that', 'plasma', 'balls', 'of', 'fire', 'belong', 'to', 'the', 'same', 'c... | [-0.09583148639515342, 0.14005473056080853, -0.09928340065003984, 0.07477827511872326, -0.05023232573140198, -0.19016503811888824, -0.04115097201696929, 0.3526545614967572, -0.269229296980233, -0.2594652394496504, 0.06250371461354154, -0.2548484046857847, -0.1945552730012214, 0.22409938511320915, -0.05200483205717528, ... |
709.1556 | Approximation of complex algebraic numbers by algebraic numbers of
bounded degree | We investigate how well complex algebraic numbers can be approximated by
algebraic numbers of degree at most n. We also investigate how well complex
algebraic numbers can be approximated by algebraic integers of degree at most
n+1. It follows from our investigations that for every positive integer n there
are complex... | math.NT | we investigate how well complex algebraic numbers can be approximated by algebraic numbers of degree at most n we also investigate how well complex algebraic numbers can be approximated by algebraic integers of degree at most n1 it follows from our investigations that for every positive integer n there are complex alge... | [['we', 'investigate', 'how', 'well', 'complex', 'algebraic', 'numbers', 'can', 'be', 'approximated', 'by', 'algebraic', 'numbers', 'of', 'degree', 'at', 'most', 'n', 'we', 'also', 'investigate', 'how', 'well', 'complex', 'algebraic', 'numbers', 'can', 'be', 'approximated', 'by', 'algebraic', 'integers', 'of', 'degree'... | [-0.22895789099263256, 0.2071270614824429, -0.03139714204839298, 0.1255170694096204, -0.06274673902448646, -0.19820311406095112, -0.017205485893527463, 0.3022253402337736, -0.2998569583643836, -0.32348820966863245, 0.06921900624447332, -0.2878999225605203, -0.19459130558926535, 0.26478283660372304, -0.00275302063483668... |
709.1557 | The Szemeredi property in ergodic W*-dynamical systems | We study weak mixing of all orders for asymptotically abelian weakly mixing
state preserving C*-dynamical systems, where the dynamics is given by the
action of an abelian second countable locally compact group which contains a
Folner sequence satisfying the Tempelman condition. For a smaller class of
groups (which in... | math.OA | we study weak mixing of all orders for asymptotically abelian weakly mixing state preserving cdynamical systems where the dynamics is given by the action of an abelian second countable locally compact group which contains a folner sequence satisfying the tempelman condition for a smaller class of groups which include z... | [['we', 'study', 'weak', 'mixing', 'of', 'all', 'orders', 'for', 'asymptotically', 'abelian', 'weakly', 'mixing', 'state', 'preserving', 'cdynamical', 'systems', 'where', 'the', 'dynamics', 'is', 'given', 'by', 'the', 'action', 'of', 'an', 'abelian', 'second', 'countable', 'locally', 'compact', 'group', 'which', 'conta... | [-0.1907575588033657, 0.16299613064414858, -0.09263979864654819, 0.07197874721675886, -0.08457686245968246, -0.1442799469023341, 0.013988499427355375, 0.31969176053135384, -0.2787914014035704, -0.15996311580517678, 0.11798115779476409, -0.2666068569253754, -0.10681441091612508, 0.21991974849434984, -0.10409533762081404... |
709.1558 | Global phase-locking in finite populations of phase-coupled oscillators | We present new necessary and sufficient conditions for the existence of fixed
points in a finite system of coupled phase oscillators on a complete graph. We
use these conditions to derive bounds on the critical coupling.
| math.DS math.CA | we present new necessary and sufficient conditions for the existence of fixed points in a finite system of coupled phase oscillators on a complete graph we use these conditions to derive bounds on the critical coupling | [['we', 'present', 'new', 'necessary', 'and', 'sufficient', 'conditions', 'for', 'the', 'existence', 'of', 'fixed', 'points', 'in', 'a', 'finite', 'system', 'of', 'coupled', 'phase', 'oscillators', 'on', 'a', 'complete', 'graph', 'we', 'use', 'these', 'conditions', 'to', 'derive', 'bounds', 'on', 'the', 'critical', 'co... | [-0.22241017400907973, 0.10848471226118919, -0.07633476854405469, 0.026614495190895267, -0.05973730142512876, -0.1398411594952146, 0.13542374753807154, 0.32753536940759254, -0.15797280291897348, -0.24706935613519615, 0.1568179333213872, -0.20816285618477398, -0.16438466023343304, 0.17877816820853493, -0.057002164733906... |
709.1559 | Koppelman formulas on Grassmannians | We construct Koppelman formulas on Grassmannians for forms with values in any
holomorphic line bundle as well as in the tautological vector bundle and its
dual. As a consequence we obtain some vanishing theorems of the Bott-Borel-Weil
type. We also relate the projection part of our formulas to the Bergman kernels
ass... | math.CV math.RT | we construct koppelman formulas on grassmannians for forms with values in any holomorphic line bundle as well as in the tautological vector bundle and its dual as a consequence we obtain some vanishing theorems of the bottborelweil type we also relate the projection part of our formulas to the bergman kernels associate... | [['we', 'construct', 'koppelman', 'formulas', 'on', 'grassmannians', 'for', 'forms', 'with', 'values', 'in', 'any', 'holomorphic', 'line', 'bundle', 'as', 'well', 'as', 'in', 'the', 'tautological', 'vector', 'bundle', 'and', 'its', 'dual', 'as', 'a', 'consequence', 'we', 'obtain', 'some', 'vanishing', 'theorems', 'of',... | [-0.14614173269364983, -0.02343278558380137, -0.024364914246169583, 0.10188399285211094, -0.14820228407292493, -0.09929407549290252, 0.01386084086594305, 0.36877017953832236, -0.2609722299966961, -0.13911254649117058, 0.16434712676813693, -0.23268942042653049, -0.1894534708532904, 0.22888659822222376, -0.11103938406605... |
709.156 | On two notions of complexity of algebraic numbers | we derive new, improved lower bounds for the block complexity of an
irrational algebraic number and for the number of digit changes in the b-ary
expansion of an irrational algebraic number. To this end, we apply a
quantitative version of the Subspace Theorem due to Evertse and Schlickewei
(2002).
| math.NT | we derive new improved lower bounds for the block complexity of an irrational algebraic number and for the number of digit changes in the bary expansion of an irrational algebraic number to this end we apply a quantitative version of the subspace theorem due to evertse and schlickewei 2002 | [['we', 'derive', 'new', 'improved', 'lower', 'bounds', 'for', 'the', 'block', 'complexity', 'of', 'an', 'irrational', 'algebraic', 'number', 'and', 'for', 'the', 'number', 'of', 'digit', 'changes', 'in', 'the', 'bary', 'expansion', 'of', 'an', 'irrational', 'algebraic', 'number', 'to', 'this', 'end', 'we', 'apply', 'a... | [-0.16804597952536174, 0.057404061661182657, -0.10064501999592294, 0.09114707727697963, -0.08718910569572175, -0.07776227022274113, 0.12278311968096817, 0.23888415290156798, -0.2741822417521355, -0.2988934027677288, 0.12242187609734508, -0.24003417183626063, -0.12306058868689805, 0.24499998135701279, -0.174779737995443... |
709.1561 | Calibration of the galaxy cluster M_500-Y_X relation with XMM-Newton | The quantity Y_ X, the product of the X-ray temperature T_ X and gas mass M_
g, has recently been proposed as a robust low-scatter mass indicator for galaxy
clusters. Using precise measurements from XMM-Newton data of a sample of 10
relaxed nearby clusters, spanning a Y_ X range of 10^13 -10^15 M_sun keV, we
investig... | astro-ph | the quantity y_ x the product of the xray temperature t_ x and gas mass m_ g has recently been proposed as a robust lowscatter mass indicator for galaxy clusters using precise measurements from xmmnewton data of a sample of 10 relaxed nearby clusters spanning a y_ x range of 1013 1015 m_sun kev we investigate the m_500... | [['the', 'quantity', 'y_', 'x', 'the', 'product', 'of', 'the', 'xray', 'temperature', 't_', 'x', 'and', 'gas', 'mass', 'm_', 'g', 'has', 'recently', 'been', 'proposed', 'as', 'a', 'robust', 'lowscatter', 'mass', 'indicator', 'for', 'galaxy', 'clusters', 'using', 'precise', 'measurements', 'from', 'xmmnewton', 'data', '... | [-0.08335718887259386, 0.13299648622732743, -0.06941693675571255, 0.11462024683731475, -0.022420205878359932, -0.054842128248087, 0.0984188464869346, 0.3877996086009911, -0.1852086357852178, -0.3948048711887428, 0.0725364005711994, -0.3301737236923405, 0.03767991843633354, 0.22751930353763913, -0.028558686577848026, 0.... |
709.1562 | Transport of interacting electrons through a potential barrier:
nonperturbative RG approach | We calculate the linear response conductance of electrons in a Luttinger
liquid with arbitrary interaction g_2, and subject to a potential barrier of
arbitrary strength, as a function of temperature. We first map the Hamiltonian
in the basis of scattering states into an effective low energy Hamiltonian in
current alg... | cond-mat.str-el cond-mat.mes-hall | we calculate the linear response conductance of electrons in a luttinger liquid with arbitrary interaction g_2 and subject to a potential barrier of arbitrary strength as a function of temperature we first map the hamiltonian in the basis of scattering states into an effective low energy hamiltonian in current algebra ... | [['we', 'calculate', 'the', 'linear', 'response', 'conductance', 'of', 'electrons', 'in', 'a', 'luttinger', 'liquid', 'with', 'arbitrary', 'interaction', 'g_2', 'and', 'subject', 'to', 'a', 'potential', 'barrier', 'of', 'arbitrary', 'strength', 'as', 'a', 'function', 'of', 'temperature', 'we', 'first', 'map', 'the', 'h... | [-0.17806783337146043, 0.15074791388862016, -0.07763182851688369, 0.071971431846285, -0.02822953914292157, -0.11566809587504552, 0.020580811562704974, 0.3230208373264126, -0.2514501712527936, -0.2588159124893339, 0.031965906763165866, -0.3072564744542393, -0.13372758013479735, 0.16282120458781718, 0.03772613854835863, ... |
709.1563 | Blind Multi-Band Signal Reconstruction: Compressed Sensing for Analog
Signals | We address the problem of reconstructing a multi-band signal from its
sub-Nyquist point-wise samples. To date, all reconstruction methods proposed
for this class of signals assumed knowledge of the band locations. In this
paper, we develop a non-linear blind perfect reconstruction scheme for
multi-band signals which ... | nlin.CG nlin.SI | we address the problem of reconstructing a multiband signal from its subnyquist pointwise samples to date all reconstruction methods proposed for this class of signals assumed knowledge of the band locations in this paper we develop a nonlinear blind perfect reconstruction scheme for multiband signals which does not re... | [['we', 'address', 'the', 'problem', 'of', 'reconstructing', 'a', 'multiband', 'signal', 'from', 'its', 'subnyquist', 'pointwise', 'samples', 'to', 'date', 'all', 'reconstruction', 'methods', 'proposed', 'for', 'this', 'class', 'of', 'signals', 'assumed', 'knowledge', 'of', 'the', 'band', 'locations', 'in', 'this', 'pa... | [-0.07937005515045979, 0.03385539161501904, -0.06411428645746235, 0.04321669716839952, -0.08531854431117501, -0.13936222770306117, 0.08883375041666167, 0.39065518690108814, -0.32227000445127485, -0.3239697408478926, 0.1562655976103783, -0.20003622671150986, -0.14339681163649348, 0.2059277333538322, -0.09401844963568318... |
709.1564 | Ab-initio self-energy corrections in systems with metallic screening | The calculation of self-energy corrections to the electron bands of a metal
requires the evaluation of the intraband contribution to the polarizability in
the small-q limit. When neglected, as in standard GW codes for semiconductors
and insulators, a spurious gap opens at the Fermi energy. Systematic methods to
inclu... | cond-mat.mtrl-sci | the calculation of selfenergy corrections to the electron bands of a metal requires the evaluation of the intraband contribution to the polarizability in the smallq limit when neglected as in standard gw codes for semiconductors and insulators a spurious gap opens at the fermi energy systematic methods to include intra... | [['the', 'calculation', 'of', 'selfenergy', 'corrections', 'to', 'the', 'electron', 'bands', 'of', 'a', 'metal', 'requires', 'the', 'evaluation', 'of', 'the', 'intraband', 'contribution', 'to', 'the', 'polarizability', 'in', 'the', 'smallq', 'limit', 'when', 'neglected', 'as', 'in', 'standard', 'gw', 'codes', 'for', 's... | [-0.11058382666042056, 0.08384700475361052, -0.04602885976269403, 0.09505856400081779, -0.016091211881561606, -0.09418940384799213, 0.1187468054613062, 0.3725163787466419, -0.2026596504044445, -0.26906395013279777, 0.008990365771038056, -0.34324781671531646, -0.10934322810955528, 0.20975783182417646, 0.0399404158881367... |
709.1565 | Overpartition pairs and two classes of basic hypergeometric series | We study the combinatorics of two classes of basic hypergeometric series. We
first show that these series are the generating functions for certain
overpartition pairs defined by frequency conditions on the parts. We then show
that when specialized these series are also the generating functions for
overpartition pairs... | math.CO math.NT | we study the combinatorics of two classes of basic hypergeometric series we first show that these series are the generating functions for certain overpartition pairs defined by frequency conditions on the parts we then show that when specialized these series are also the generating functions for overpartition pairs wit... | [['we', 'study', 'the', 'combinatorics', 'of', 'two', 'classes', 'of', 'basic', 'hypergeometric', 'series', 'we', 'first', 'show', 'that', 'these', 'series', 'are', 'the', 'generating', 'functions', 'for', 'certain', 'overpartition', 'pairs', 'defined', 'by', 'frequency', 'conditions', 'on', 'the', 'parts', 'we', 'then... | [-0.16851901410180808, 0.11518638961327572, -0.04571545629629067, 0.12686828272195444, -0.06401503584458537, -0.07057580868491814, 0.012858192436397076, 0.37533884598607464, -0.30529210281868774, -0.25925479282713715, 0.11370390223982256, -0.2957787858322263, -0.1916864785654027, 0.2642271888575384, -0.0336958716313044... |
709.1566 | Spin polarized current in a junction of zigzag carbon nanotube | We investigated spin-resolved electronic transport through a junction
composed of a nonmagnetic metal electrode and a zigzag carbon nanotube by means
of self-consistent Green's function method in the tight binding approximation
and the unrestricted Hartree-Fock approximation. Our results show that the
electric curren... | cond-mat.mes-hall | we investigated spinresolved electronic transport through a junction composed of a nonmagnetic metal electrode and a zigzag carbon nanotube by means of selfconsistent greens function method in the tight binding approximation and the unrestricted hartreefock approximation our results show that the electric current can b... | [['we', 'investigated', 'spinresolved', 'electronic', 'transport', 'through', 'a', 'junction', 'composed', 'of', 'a', 'nonmagnetic', 'metal', 'electrode', 'and', 'a', 'zigzag', 'carbon', 'nanotube', 'by', 'means', 'of', 'selfconsistent', 'greens', 'function', 'method', 'in', 'the', 'tight', 'binding', 'approximation', ... | [-0.20916890915801575, 0.14782188371219465, -0.01644963664785687, 0.04879347223631906, 0.03250725630905677, -0.14549877356111476, 0.11761621127432559, 0.4330661952561509, -0.26614723503754467, -0.2821970783685029, -0.06440253658178963, -0.2756146128264676, -0.12126611928204156, 0.1542780346595641, 0.12781086089954902, ... |
709.1567 | Quantum graphs and the integer quantum Hall effect | We study the spectral properties of infinite rectangular quantum graphs in
the presence of a magnetic field. We study how these properties are affected
when three-dimensionality is considered, in particular, the chaological
properties. We then establish the quantization of the Hall transverse
conductivity for these s... | cond-mat.mes-hall cond-mat.stat-mech | we study the spectral properties of infinite rectangular quantum graphs in the presence of a magnetic field we study how these properties are affected when threedimensionality is considered in particular the chaological properties we then establish the quantization of the hall transverse conductivity for these systems ... | [['we', 'study', 'the', 'spectral', 'properties', 'of', 'infinite', 'rectangular', 'quantum', 'graphs', 'in', 'the', 'presence', 'of', 'a', 'magnetic', 'field', 'we', 'study', 'how', 'these', 'properties', 'are', 'affected', 'when', 'threedimensionality', 'is', 'considered', 'in', 'particular', 'the', 'chaological', 'p... | [-0.18879292185618718, 0.20291129183307838, -0.07210490008509612, 0.03801627192333859, -0.052818630456547194, -0.0926933255270595, -0.03059476966707366, 0.36711732477326936, -0.30383909239339396, -0.2515123187434636, 0.0771018361843698, -0.2607883421727751, -0.18748792161858535, 0.19122623857346516, -0.0425745170280525... |
709.1568 | Automated Calculation Scheme for alpha^n Contributions of QED to Lepton
g-2: New Treatment of Infrared Divergence for Diagrams without Lepton Loops | We have developed an efficient algorithm for the subtraction of infrared
divergences that arise in the evaluation of QED corrections to the anomalous
magnetic moment of lepton (g-2). By incorporating this new algorithm, we have
extended the automated code-generating system developed previously to deal with
diagrams w... | hep-ph hep-th | we have developed an efficient algorithm for the subtraction of infrared divergences that arise in the evaluation of qed corrections to the anomalous magnetic moment of lepton g2 by incorporating this new algorithm we have extended the automated codegenerating system developed previously to deal with diagrams without i... | [['we', 'have', 'developed', 'an', 'efficient', 'algorithm', 'for', 'the', 'subtraction', 'of', 'infrared', 'divergences', 'that', 'arise', 'in', 'the', 'evaluation', 'of', 'qed', 'corrections', 'to', 'the', 'anomalous', 'magnetic', 'moment', 'of', 'lepton', 'g2', 'by', 'incorporating', 'this', 'new', 'algorithm', 'we'... | [-0.1097659055554008, 0.14721508860556998, -0.07997309114247309, 0.1306143720442887, -0.09177921863146506, -0.12773693440150533, 0.04601795091532995, 0.3557489865727849, -0.16817270970303502, -0.2945703466647794, 0.04400733289589032, -0.30153969685562837, -0.13180177242858176, 0.2023503952245307, -0.03552765390535785, ... |
709.1569 | Tridiagonal PT-symmetric N by N Hamiltonians and a fine-tuning of their
observability domains in the strongly non-Hermitian regime | A generic PT-symmetric Hamiltonian is assumed tridiagonalized and truncated
to N dimensions, and its up-down symmetrized special cases with J=[N/2] real
couplings are considered. In the strongly non-Hermitian regime the secular
equation gets partially factorized at all N. This enables us to reveal a
fine-tuned alignm... | math-ph math.MP | a generic ptsymmetric hamiltonian is assumed tridiagonalized and truncated to n dimensions and its updown symmetrized special cases with jn2 real couplings are considered in the strongly nonhermitian regime the secular equation gets partially factorized at all n this enables us to reveal a finetuned alignment of the do... | [['a', 'generic', 'ptsymmetric', 'hamiltonian', 'is', 'assumed', 'tridiagonalized', 'and', 'truncated', 'to', 'n', 'dimensions', 'and', 'its', 'updown', 'symmetrized', 'special', 'cases', 'with', 'jn2', 'real', 'couplings', 'are', 'considered', 'in', 'the', 'strongly', 'nonhermitian', 'regime', 'the', 'secular', 'equat... | [-0.16049791930394397, 0.19123717311418117, -0.03497619657601054, 0.04769583067202286, -0.04155000813881162, -0.18050886489878837, -0.03839268584458812, 0.3553010406148796, -0.23225584802393978, -0.2301005459315068, 0.05871748658387947, -0.26513397548586837, -0.14126232122322796, 0.10580344823176495, -0.001877840897823... |
709.157 | Reciprocal cyclotomic polynomials | Let $\Psi_n(x)$ be the monic polynomial having precisely all non-primitive
$n$th roots of unity as its simple zeros. One has
$\Psi_n(x)=(x^n-1)/\Phi_n(x)$, with $\Phi_n(x)$ the $n$th cyclotomic
polynomial. The coefficients of $\Psi_n(x)$ are integers that like the
coefficients of $\Phi_n(x)$ tend to be surprisingly s... | math.NT | let psi_nx be the monic polynomial having precisely all nonprimitive nth roots of unity as its simple zeros one has psi_nxxn1phi_nx with phi_nx the nth cyclotomic polynomial the coefficients of psi_nx are integers that like the coefficients of phi_nx tend to be surprisingly small in absolute value eg for n561 all coeff... | [['let', 'psi_nx', 'be', 'the', 'monic', 'polynomial', 'having', 'precisely', 'all', 'nonprimitive', 'nth', 'roots', 'of', 'unity', 'as', 'its', 'simple', 'zeros', 'one', 'has', 'psi_nxxn1phi_nx', 'with', 'phi_nx', 'the', 'nth', 'cyclotomic', 'polynomial', 'the', 'coefficients', 'of', 'psi_nx', 'are', 'integers', 'that... | [-0.21525842212696575, 0.12572007403889698, -0.060476982955640156, -0.011540404548729533, -0.07498070348832589, -0.15557532831887477, -0.07062256804653513, 0.28501301068367796, -0.35589127224494715, -0.1987852345067841, 0.11371182341392694, -0.33449456885234635, -0.10802475135050603, 0.21764281545696196, -0.03884671843... |
709.1571 | High-redshift microlensing and the spatial distribution of dark matter
in the form of MACHOs | A substantial part of the dark matter of the Universe could be in the form of
compact objects (MACHOs), detectable through gravitational microlensing effects
as they pass through the line of sight to background light sources. So far,
most attempts to model the effects of high-redshift microlensing by a
cosmologically... | astro-ph | a substantial part of the dark matter of the universe could be in the form of compact objects machos detectable through gravitational microlensing effects as they pass through the line of sight to background light sources so far most attempts to model the effects of highredshift microlensing by a cosmologically distrib... | [['a', 'substantial', 'part', 'of', 'the', 'dark', 'matter', 'of', 'the', 'universe', 'could', 'be', 'in', 'the', 'form', 'of', 'compact', 'objects', 'machos', 'detectable', 'through', 'gravitational', 'microlensing', 'effects', 'as', 'they', 'pass', 'through', 'the', 'line', 'of', 'sight', 'to', 'background', 'light',... | [-0.09732726920859903, 0.11176297865763661, -0.11361908854358638, 0.0955713871808257, -0.11617730584897337, -0.0744737023395294, 0.05528766769566573, 0.39933435883491286, -0.20499193421260098, -0.35487837091897656, 0.06307968981000447, -0.2652093343358646, -0.053065934687823293, 0.20035071332665486, -0.0530748914165924... |
709.1572 | Is mass loss along the red giant branch of globular clusters sharply
peaked? The case of M3 | There is a growing evidence that several globular clusters must contain
multiple stellar generations, differing in helium content. This hypothesis has
helped to interpret peculiar unexplained features in their horizontal branches.
In this framework we model the peaked distribution of the RR Lyr periods in M3,
that ha... | astro-ph | there is a growing evidence that several globular clusters must contain multiple stellar generations differing in helium content this hypothesis has helped to interpret peculiar unexplained features in their horizontal branches in this framework we model the peaked distribution of the rr lyr periods in m3 that has defi... | [['there', 'is', 'a', 'growing', 'evidence', 'that', 'several', 'globular', 'clusters', 'must', 'contain', 'multiple', 'stellar', 'generations', 'differing', 'in', 'helium', 'content', 'this', 'hypothesis', 'has', 'helped', 'to', 'interpret', 'peculiar', 'unexplained', 'features', 'in', 'their', 'horizontal', 'branches... | [-0.09117406064569089, 0.14123476015382333, -0.13793792013574196, 0.10669114043353384, -0.09855872536794083, -0.07088519883142903, 0.08511703190759815, 0.41368852904173437, -0.17262525328689368, -0.36751028626209736, 0.015707455228238954, -0.2897182167839122, -0.049128732339608905, 0.15116371168227424, -0.1195743549224... |
709.1573 | Quantum simulation of Anderson and Kondo lattices with superconducting
qubits | We introduce a mapping between a variety of superconducting circuits and a
family of Hamiltonians describing localized magnetic impurities interacting
with conduction bands. This includes the Anderson model, the single impurity
one- and two-channel Kondo problem, as well as the 1D Kondo lattice. We compare
the requir... | cond-mat.mes-hall quant-ph | we introduce a mapping between a variety of superconducting circuits and a family of hamiltonians describing localized magnetic impurities interacting with conduction bands this includes the anderson model the single impurity one and twochannel kondo problem as well as the 1d kondo lattice we compare the requirements f... | [['we', 'introduce', 'a', 'mapping', 'between', 'a', 'variety', 'of', 'superconducting', 'circuits', 'and', 'a', 'family', 'of', 'hamiltonians', 'describing', 'localized', 'magnetic', 'impurities', 'interacting', 'with', 'conduction', 'bands', 'this', 'includes', 'the', 'anderson', 'model', 'the', 'single', 'impurity',... | [-0.1556030831237634, 0.15237488120328635, -0.001975378692150116, 0.054849996658352516, -0.016440114192664623, -0.27498959688469765, 0.07130598288650314, 0.3624539573552708, -0.24314597440262636, -0.2871917579074701, 0.016618891457716625, -0.31472461665670076, -0.1278316105467578, 0.21892609033423166, 0.026480938637396... |
709.1574 | The Active Mirror Control of the MAGIC Telescope | One of the main design goals of the MAGIC telescopes is the very fast
repositioning in case of Gamma Ray Burst (GRB) alarms, implying a low weight of
the telescope dish. This is accomplished by using a space frame made of carbon
fiber epoxy tubes, resulting in a strong but not very rigid support structure.
Therefore ... | astro-ph | one of the main design goals of the magic telescopes is the very fast repositioning in case of gamma ray burst grb alarms implying a low weight of the telescope dish this is accomplished by using a space frame made of carbon fiber epoxy tubes resulting in a strong but not very rigid support structure therefore it is ne... | [['one', 'of', 'the', 'main', 'design', 'goals', 'of', 'the', 'magic', 'telescopes', 'is', 'the', 'very', 'fast', 'repositioning', 'in', 'case', 'of', 'gamma', 'ray', 'burst', 'grb', 'alarms', 'implying', 'a', 'low', 'weight', 'of', 'the', 'telescope', 'dish', 'this', 'is', 'accomplished', 'by', 'using', 'a', 'space', ... | [-0.1270312674037125, 0.132334976777699, -0.06040521177938845, 0.039516321720722586, -0.08136045184726708, -0.1610082671778579, 0.06354457191311014, 0.4577378287083573, -0.22949389474959964, -0.32000846875847405, 0.12536989437499776, -0.21000567168936643, -0.1295372621418956, 0.20892675374992764, -0.10226510229926461, ... |
709.1575 | Configurational Temperature Control for Atomic and Molecular Systems | A new configurational temperature thermostat suitable for molecules with
holonomic constraints is derived. This thermostat has a simple set of motion
equations, can generate the canonical ensemble in both position and momentum
space, acts homogeneously through the spatial coordinates, and does not
intrinsically viola... | cond-mat.stat-mech | a new configurational temperature thermostat suitable for molecules with holonomic constraints is derived this thermostat has a simple set of motion equations can generate the canonical ensemble in both position and momentum space acts homogeneously through the spatial coordinates and does not intrinsically violate the... | [['a', 'new', 'configurational', 'temperature', 'thermostat', 'suitable', 'for', 'molecules', 'with', 'holonomic', 'constraints', 'is', 'derived', 'this', 'thermostat', 'has', 'a', 'simple', 'set', 'of', 'motion', 'equations', 'can', 'generate', 'the', 'canonical', 'ensemble', 'in', 'both', 'position', 'and', 'momentum... | [-0.1393785828061528, 0.1708021627865353, -0.11270306489942891, 0.01310513585794054, -0.06936113724200907, -0.1723728897326263, 0.044789957768536344, 0.3306348815449845, -0.29371570349055326, -0.26580848060232604, 0.023714083718467442, -0.24906827254078778, -0.08762968138010258, 0.17931315879006002, -0.0501029160568269... |
709.1576 | Groups which are not properly 3-realizable | A group is properly 3-realizable if it is the fundamental group of a compact
polyhedron whose universal covering is proper homotopically equivalent to some
3-manifold. We prove that when such a group is also quasi-simply filtered then
it has {\em pro-(finitely generated free) fundamental group at infinity} and
{\em s... | math.GT math.GR | a group is properly 3realizable if it is the fundamental group of a compact polyhedron whose universal covering is proper homotopically equivalent to some 3manifold we prove that when such a group is also quasisimply filtered then it has em profinitely generated free fundamental group at infinity and em semistable ends... | [['a', 'group', 'is', 'properly', '3realizable', 'if', 'it', 'is', 'the', 'fundamental', 'group', 'of', 'a', 'compact', 'polyhedron', 'whose', 'universal', 'covering', 'is', 'proper', 'homotopically', 'equivalent', 'to', 'some', '3manifold', 'we', 'prove', 'that', 'when', 'such', 'a', 'group', 'is', 'also', 'quasisimpl... | [-0.15160732626880905, 0.16277910268115925, -0.15316955117145326, 0.07554267712715422, -0.16249832271870862, -0.17249760137893622, -0.007450421904384091, 0.4225925836235103, -0.34470048596764485, -0.2088731815342837, 0.14206195798725252, -0.23947085720123495, -0.13318119771642292, 0.20702454246716892, -0.17128783768247... |
709.1577 | Analytic Extension of a maximal surface in $\Bbb L^3$ along its boudary | We prove that a maximal surface in Lorentz-Minkowski space $\Bbb L^3$ can be
extended analytically along its boundary if the boundary lies in a plane
meeting the surface at a constant angle.
| math.DG math.CV | we prove that a maximal surface in lorentzminkowski space bbb l3 can be extended analytically along its boundary if the boundary lies in a plane meeting the surface at a constant angle | [['we', 'prove', 'that', 'a', 'maximal', 'surface', 'in', 'lorentzminkowski', 'space', 'bbb', 'l3', 'can', 'be', 'extended', 'analytically', 'along', 'its', 'boundary', 'if', 'the', 'boundary', 'lies', 'in', 'a', 'plane', 'meeting', 'the', 'surface', 'at', 'a', 'constant', 'angle']] | [-0.25569162447936833, 0.15775979743921198, -0.0942054685583571, 0.01979692408349365, -0.08157096669310704, -0.11257678910624236, 0.016919862071517855, 0.37153080210555345, -0.2892010420328006, -0.1603109634888824, 0.1728403435627115, -0.27305400457044016, -0.12140342622296885, 0.19247310422360897, -0.09877565645729192... |
709.1578 | Intersection homology D-Modules and Bernstein polynomials associated
with a complete intersection | Let X be a complex analytic manifold. Given a closed subspace $Y\subset X$ of
pure codimension p>0, we consider the sheaf of local algebraic cohomology
$H^p_{[Y]}({\cal O}_X)$, and ${\cal L}(Y,X)\subset H^p_{[Y]}({\cal O}_X)$ the
intersection homology D_X-Module of Brylinski-Kashiwara. We give here an
algebraic chara... | math.AG | let x be a complex analytic manifold given a closed subspace ysubset x of pure codimension p0 we consider the sheaf of local algebraic cohomology hp_ycal o_x and cal lyxsubset hp_ycal o_x the intersection homology d_xmodule of brylinskikashiwara we give here an algebraic characterization of the spaces y such that lyx c... | [['let', 'x', 'be', 'a', 'complex', 'analytic', 'manifold', 'given', 'a', 'closed', 'subspace', 'ysubset', 'x', 'of', 'pure', 'codimension', 'p0', 'we', 'consider', 'the', 'sheaf', 'of', 'local', 'algebraic', 'cohomology', 'hp_ycal', 'o_x', 'and', 'cal', 'lyxsubset', 'hp_ycal', 'o_x', 'the', 'intersection', 'homology',... | [-0.2937111217149739, 0.015103907693597741, -0.10524614676201748, 0.05928400907886483, -0.07065160515702378, -0.14913443925837844, -0.037440036960198715, 0.288434496307272, -0.3632450596571474, -0.07489793583498162, 0.03879724111273822, -0.25138802400206106, -0.12330939490505952, 0.12382626492466967, -0.196136263514853... |
709.1579 | Dislocation formation from a surface step in semiconductors: an ab
initio study | The role of a simple surface defect, such as a step, for relaxing the stress
applied to a semiconductor, has been investigated by means of large scale first
principles calculations. Our results indicate that the step is the privileged
site for initiating plasticity, with the formation and glide of 60$^\circ$
dislocat... | cond-mat.mtrl-sci | the role of a simple surface defect such as a step for relaxing the stress applied to a semiconductor has been investigated by means of large scale first principles calculations our results indicate that the step is the privileged site for initiating plasticity with the formation and glide of 60circ dislocations for bo... | [['the', 'role', 'of', 'a', 'simple', 'surface', 'defect', 'such', 'as', 'a', 'step', 'for', 'relaxing', 'the', 'stress', 'applied', 'to', 'a', 'semiconductor', 'has', 'been', 'investigated', 'by', 'means', 'of', 'large', 'scale', 'first', 'principles', 'calculations', 'our', 'results', 'indicate', 'that', 'the', 'step... | [-0.10659529030615683, 0.14789314645006219, -0.07906506382601543, 0.0004459766447932149, -0.031018361294021208, -0.07925458615581091, 0.03925801021331507, 0.4178114002053108, -0.2821802270546969, -0.26711768351702225, 0.1128114299240729, -0.2083487843370272, -0.183834101206028, 0.17226428091978757, 0.03618070949515742,... |
709.158 | Suzaku Detection of Extended/Diffuse Hard X-Ray Emission from the
Galactic Center | Five on-plane regions within +/- 0.8deg of the Galactic center were observed
with the Hard X-ray Detector (HXD) and the X-ray Imaging Spectrometer (XIS)
onboard Suzaku. From all regions, significant hard X-ray emission was detected
with HXD-PIN up to 40 keV, in addition to the extended plasma emission which is
domina... | astro-ph | five onplane regions within 08deg of the galactic center were observed with the hard xray detector hxd and the xray imaging spectrometer xis onboard suzaku from all regions significant hard xray emission was detected with hxdpin up to 40 kev in addition to the extended plasma emission which is dominant in the xis band ... | [['five', 'onplane', 'regions', 'within', '08deg', 'of', 'the', 'galactic', 'center', 'were', 'observed', 'with', 'the', 'hard', 'xray', 'detector', 'hxd', 'and', 'the', 'xray', 'imaging', 'spectrometer', 'xis', 'onboard', 'suzaku', 'from', 'all', 'regions', 'significant', 'hard', 'xray', 'emission', 'was', 'detected',... | [-0.004957902876045463, 0.11881570002463247, -0.07565685848618302, 0.1245648449119364, -0.07971751787860332, -0.12016969677026434, 0.04303419244047851, 0.5005589778090052, -0.17902191688210287, -0.39538126616862607, 0.09307840171618745, -0.401641598558558, 0.04188331442293275, 0.2279792105437261, -0.01702347357546351, ... |
709.1581 | Stability of undissociated screw dislocations in zinc-blende covalent
materials from first principle simulations | The properties of perfect screw dislocations have been investigated for
several zinc-blende materials such as diamond, Si, $\beta$-SiC, Ge and GaAs, by
performing first principles calculations. For almost all elements, a core
configuration belonging to shuffle set planes is favored, in agreement with low
temperature ... | cond-mat.mtrl-sci | the properties of perfect screw dislocations have been investigated for several zincblende materials such as diamond si betasic ge and gaas by performing first principles calculations for almost all elements a core configuration belonging to shuffle set planes is favored in agreement with low temperature experiments on... | [['the', 'properties', 'of', 'perfect', 'screw', 'dislocations', 'have', 'been', 'investigated', 'for', 'several', 'zincblende', 'materials', 'such', 'as', 'diamond', 'si', 'betasic', 'ge', 'and', 'gaas', 'by', 'performing', 'first', 'principles', 'calculations', 'for', 'almost', 'all', 'elements', 'a', 'core', 'config... | [-0.10529195163398981, 0.1542864102962015, 0.045136311299239215, -0.021355992718599736, 0.013253796061214346, -0.13724682879849123, 0.06505272992004534, 0.47770297091740827, -0.22705084751718319, -0.293806638296407, 0.04813728083569843, -0.3028001130128709, -0.07412931004610772, 0.1364599897705305, 0.05466298557674656,... |
709.1582 | Energy dependence of nuclear effects in hadron-nucleus collisions | The energy dependence of light and heavy particle production in
hadron-nucleus collisions is discussed. Whereas the production mechanism at
lower energies can be understood in the Glauber rescattering picture,
experimental data at RHIC indicate that particles are mostly produced in
coherent processes. The importance ... | hep-ph | the energy dependence of light and heavy particle production in hadronnucleus collisions is discussed whereas the production mechanism at lower energies can be understood in the glauber rescattering picture experimental data at rhic indicate that particles are mostly produced in coherent processes the importance of ene... | [['the', 'energy', 'dependence', 'of', 'light', 'and', 'heavy', 'particle', 'production', 'in', 'hadronnucleus', 'collisions', 'is', 'discussed', 'whereas', 'the', 'production', 'mechanism', 'at', 'lower', 'energies', 'can', 'be', 'understood', 'in', 'the', 'glauber', 'rescattering', 'picture', 'experimental', 'data', ... | [-0.05168869829642409, 0.2953993225625406, -0.1640200540894598, 0.1770327103329778, -0.010258483755890103, -0.09679394393294517, -0.03832917238053467, 0.38135127018072773, -0.22692236631909118, -0.27093707520093413, -0.04352187946122805, -0.34173252241730334, 0.050341927546209524, 0.1880145501130582, 0.0722195967128278... |
709.1583 | Surface step effects on Si (100) under uniaxial tensile stress, by
atomistic calculations | This paper reports a study of the influence of the step at a silicon surface
under an uniaxial tensile stress, using an empirical potential. Our aim was to
find conditions leading to nucleation of dislocations from the step. We
obtained that no dislocations could be generated with such conditions. This
behaviour, dif... | cond-mat.mtrl-sci | this paper reports a study of the influence of the step at a silicon surface under an uniaxial tensile stress using an empirical potential our aim was to find conditions leading to nucleation of dislocations from the step we obtained that no dislocations could be generated with such conditions this behaviour different ... | [['this', 'paper', 'reports', 'a', 'study', 'of', 'the', 'influence', 'of', 'the', 'step', 'at', 'a', 'silicon', 'surface', 'under', 'an', 'uniaxial', 'tensile', 'stress', 'using', 'an', 'empirical', 'potential', 'our', 'aim', 'was', 'to', 'find', 'conditions', 'leading', 'to', 'nucleation', 'of', 'dislocations', 'from... | [-0.08258687616843316, 0.12103939153773051, -0.11260707660241881, -0.03233577915428517, -0.03276212345291343, -0.07372758558226956, 0.03627951988568788, 0.41817624910941553, -0.29868137738150025, -0.2700746655076121, 0.062089173349603594, -0.27428465491781634, -0.16644348635842712, 0.14512737199806403, -0.0071584539319... |
709.1584 | Can one control systematic errors of QCD sum rule predictions for bound
states? | We study the possibility to control systematic errors of the ground-state
parameters obtained by Shifman-Vainshtein-Zakharov (SVZ) sum rules, making use
of the harmonic-oscillator potential model as an example. In this case, one
knows the exact solution for the polarization operator, which allows one to
obtain both t... | hep-ph | we study the possibility to control systematic errors of the groundstate parameters obtained by shifmanvainshteinzakharov svz sum rules making use of the harmonicoscillator potential model as an example in this case one knows the exact solution for the polarization operator which allows one to obtain both the ope to an... | [['we', 'study', 'the', 'possibility', 'to', 'control', 'systematic', 'errors', 'of', 'the', 'groundstate', 'parameters', 'obtained', 'by', 'shifmanvainshteinzakharov', 'svz', 'sum', 'rules', 'making', 'use', 'of', 'the', 'harmonicoscillator', 'potential', 'model', 'as', 'an', 'example', 'in', 'this', 'case', 'one', 'k... | [-0.07625821403883122, 0.072121872461651, -0.059848290564561334, 0.06892918243883522, -0.06632196031234883, -0.08567974545337535, 0.12016129414378493, 0.3591606487554532, -0.26114351059551594, -0.27885625271333586, 0.09844217172099484, -0.2618374130327505, -0.0913401880974157, 0.1686450845234234, 0.016164664686140088, ... |
709.1585 | Ab initio Study of Misfit Dislocations at the SiC/Si(001) Interface | The high lattice mismatched SiC/Si(001) interface was investigated by means
of combined classical and ab initio molecular dynamics. Among the several
configurations analyzed, a dislocation network pinned at the interface was
found to be the most efficient mechanism for strain relief. A detailed
description of the dis... | cond-mat.mtrl-sci | the high lattice mismatched sicsi001 interface was investigated by means of combined classical and ab initio molecular dynamics among the several configurations analyzed a dislocation network pinned at the interface was found to be the most efficient mechanism for strain relief a detailed description of the dislocation... | [['the', 'high', 'lattice', 'mismatched', 'sicsi001', 'interface', 'was', 'investigated', 'by', 'means', 'of', 'combined', 'classical', 'and', 'ab', 'initio', 'molecular', 'dynamics', 'among', 'the', 'several', 'configurations', 'analyzed', 'a', 'dislocation', 'network', 'pinned', 'at', 'the', 'interface', 'was', 'foun... | [-0.17667225700445013, 0.13140107327453274, -0.0827753338284932, 0.08723697227372823, -0.03505001066229011, -0.11755363374972079, 0.04967006439154473, 0.4127148556747014, -0.28387882696948, -0.26142550288121913, 0.08043936065315635, -0.26215422607345296, -0.1712508630714839, 0.1671704041854113, 0.04107911815230228, 0.0... |
709.1586 | H\to hh in the Mirror Model at the CERN Large Hadron Collider | The Higgs sector may play an important role in detecting the mirror
particles, which can be the candidates of the dark matter and appear as missing
energy in the detectors at the LHC. In this paper we worked out the Higgs boson
spectrum and the Higgs couplings for the symmetric vacuum, namely $v_1=v_2=v$,
in the mirr... | hep-ph hep-ex | the higgs sector may play an important role in detecting the mirror particles which can be the candidates of the dark matter and appear as missing energy in the detectors at the lhc in this paper we worked out the higgs boson spectrum and the higgs couplings for the symmetric vacuum namely v_1v_2v in the mirror model a... | [['the', 'higgs', 'sector', 'may', 'play', 'an', 'important', 'role', 'in', 'detecting', 'the', 'mirror', 'particles', 'which', 'can', 'be', 'the', 'candidates', 'of', 'the', 'dark', 'matter', 'and', 'appear', 'as', 'missing', 'energy', 'in', 'the', 'detectors', 'at', 'the', 'lhc', 'in', 'this', 'paper', 'we', 'worked'... | [-0.044083460123817385, 0.24130613457153352, -0.06639835593607009, 0.17884635630299886, -0.07937681465298294, -0.1928673440692991, 0.029393544197238483, 0.3397569105866851, -0.20957045778676725, -0.28894996660445155, 0.03793581218835251, -0.2934920683494239, -0.010881011111385515, 0.15985846761324438, 0.067403884136683... |
709.1587 | Theory of single atom manipulation with a scanning probe tip: Force
signatures, constant-height, and constant-force scans | We report theoretical results predicting the atomic manipulation of a silver
atom on a Si(001) surface by a scanning probe tip, and providing insight into
the manipulation phenomena. A molecular mechanics technique has been used, the
system being described by a quantum chemistry method for the short-range
interaction... | cond-mat.mtrl-sci | we report theoretical results predicting the atomic manipulation of a silver atom on a si001 surface by a scanning probe tip and providing insight into the manipulation phenomena a molecular mechanics technique has been used the system being described by a quantum chemistry method for the shortrange interactions and an... | [['we', 'report', 'theoretical', 'results', 'predicting', 'the', 'atomic', 'manipulation', 'of', 'a', 'silver', 'atom', 'on', 'a', 'si001', 'surface', 'by', 'a', 'scanning', 'probe', 'tip', 'and', 'providing', 'insight', 'into', 'the', 'manipulation', 'phenomena', 'a', 'molecular', 'mechanics', 'technique', 'has', 'bee... | [-0.09611709318805213, 0.1390239551406788, -0.128544291937454, 0.03756461528612307, -0.03383114071926329, -0.15367340560854845, 0.04975221274000388, 0.4160751792624956, -0.2663315021001348, -0.3520796237308986, 0.023878749314462766, -0.2819281666221597, -0.13913180434326755, 0.233823683418095, 0.023177929235361064, 0.0... |
709.1588 | Undissociated screw dislocations in silicon: calculations of core
structure and energy | The stability of the perfect screw dislocation in silicon has been
investigated using both classical potentials and first-principles calculations.
Although a recent study by Koizumi et al . stated that the stable screw
dislocation was located in both the 'shuffle' and the 'glide' sets of {111}
planes, it is shown tha... | cond-mat.mtrl-sci | the stability of the perfect screw dislocation in silicon has been investigated using both classical potentials and firstprinciples calculations although a recent study by koizumi et al stated that the stable screw dislocation was located in both the shuffle and the glide sets of 111 planes it is shown that this result... | [['the', 'stability', 'of', 'the', 'perfect', 'screw', 'dislocation', 'in', 'silicon', 'has', 'been', 'investigated', 'using', 'both', 'classical', 'potentials', 'and', 'firstprinciples', 'calculations', 'although', 'a', 'recent', 'study', 'by', 'koizumi', 'et', 'al', 'stated', 'that', 'the', 'stable', 'screw', 'disloc... | [-0.13787422718146006, 0.09422044883843139, -0.053067880123102616, 0.006533502601087093, -0.006783880293369293, -0.056583292812349334, 0.03466351705602363, 0.3699447888159944, -0.27051249742902245, -0.25879156991704216, 0.07637523940854496, -0.25795711504085167, -0.16808346207741828, 0.1484040242616057, -0.012536422674... |
709.1589 | American Options under Proportional Transaction Costs: Pricing, Hedging
and Stopping Algorithms for Long and Short Positions | American options are studied in a general discrete market in the presence of
proportional transaction costs, modelled as bid-ask spreads. Pricing algorithms
and constructions of hedging strategies, stopping times and martingale
representations are presented for short (seller's) and long (buyer's) positions
in an Amer... | q-fin.PR math.PR | american options are studied in a general discrete market in the presence of proportional transaction costs modelled as bidask spreads pricing algorithms and constructions of hedging strategies stopping times and martingale representations are presented for short sellers and long buyers positions in an american option ... | [['american', 'options', 'are', 'studied', 'in', 'a', 'general', 'discrete', 'market', 'in', 'the', 'presence', 'of', 'proportional', 'transaction', 'costs', 'modelled', 'as', 'bidask', 'spreads', 'pricing', 'algorithms', 'and', 'constructions', 'of', 'hedging', 'strategies', 'stopping', 'times', 'and', 'martingale', '... | [-0.12640090971335508, 0.06648627985204156, -0.07480072848803816, 0.14071076815779054, -0.1230362294819097, -0.19870505684017264, 0.16133600740240103, 0.42061282052336485, -0.3095737442466817, -0.22843408396696313, 0.20774435441143135, -0.26204927757039276, -0.043298033495673266, 0.1476982485037297, -0.1680951832592138... |
709.159 | Comparison between classical potentials and ab initio for silicon under
large shear | The homogeneous shear of the {111} planes along the <110> direction of bulk
silicon has been investigated using ab initio techniques, to better understand
the strain properties of both shuffle and glide set planes. Similar
calculations have been done with three empirical potentials, Stillinger-Weber,
Tersoff and EDIP... | cond-mat.mtrl-sci | the homogeneous shear of the 111 planes along the 110 direction of bulk silicon has been investigated using ab initio techniques to better understand the strain properties of both shuffle and glide set planes similar calculations have been done with three empirical potentials stillingerweber tersoff and edip in order t... | [['the', 'homogeneous', 'shear', 'of', 'the', '111', 'planes', 'along', 'the', '110', 'direction', 'of', 'bulk', 'silicon', 'has', 'been', 'investigated', 'using', 'ab', 'initio', 'techniques', 'to', 'better', 'understand', 'the', 'strain', 'properties', 'of', 'both', 'shuffle', 'and', 'glide', 'set', 'planes', 'simila... | [-0.10090993508918898, 0.0557040548296058, -0.0908629948499839, 0.03323607692423671, -0.018397239594812598, -0.08322162348105833, 0.028267190636446077, 0.4305827712287774, -0.26969498987855006, -0.2949355459931466, 0.030558895921703796, -0.27822664689675375, -0.1498591405526223, 0.18213134322541993, 0.05303500757158339... |
709.1591 | Theoretical investigations of a highly mismatched interface: the case of
SiC/Si(001) | Using first principles, classical potentials, and elasticity theory, we
investigated the structure of a semiconductor/semiconductor interface with a
high lattice mismatch, SiC/Si(001). Among several tested possible
configurations, a heterostructure with (i) a misfit dislocation network pinned
at the interface and (ii... | cond-mat.mtrl-sci | using first principles classical potentials and elasticity theory we investigated the structure of a semiconductorsemiconductor interface with a high lattice mismatch sicsi001 among several tested possible configurations a heterostructure with i a misfit dislocation network pinned at the interface and ii reconstructed ... | [['using', 'first', 'principles', 'classical', 'potentials', 'and', 'elasticity', 'theory', 'we', 'investigated', 'the', 'structure', 'of', 'a', 'semiconductorsemiconductor', 'interface', 'with', 'a', 'high', 'lattice', 'mismatch', 'sicsi001', 'among', 'several', 'tested', 'possible', 'configurations', 'a', 'heterostru... | [-0.1486673152201578, 0.11832107256306434, -0.040891721444682054, 0.04737269783265188, -0.0030253535200260645, -0.13514925067862257, 0.0458401802322294, 0.4155344395364961, -0.2782216436950028, -0.2711748625510014, 0.07626941199832334, -0.27100154103185886, -0.16915174063273236, 0.10846980413398108, 0.06480871890591951... |
709.1592 | Combined Electric and Magnetic Aharonov-Bohm Effects | It is well-known that the electric and magnetic Aharonov-Bohm effects may be
formally described on equal footing using the four-vector potential in a
relativistic framework. We propose an illustrative manifestation of both
effects in a single configuration, in which the specific path of the charged
particle determine... | quant-ph | it is wellknown that the electric and magnetic aharonovbohm effects may be formally described on equal footing using the fourvector potential in a relativistic framework we propose an illustrative manifestation of both effects in a single configuration in which the specific path of the charged particle determines the w... | [['it', 'is', 'wellknown', 'that', 'the', 'electric', 'and', 'magnetic', 'aharonovbohm', 'effects', 'may', 'be', 'formally', 'described', 'on', 'equal', 'footing', 'using', 'the', 'fourvector', 'potential', 'in', 'a', 'relativistic', 'framework', 'we', 'propose', 'an', 'illustrative', 'manifestation', 'of', 'both', 'ef... | [-0.1678196003980025, 0.21645424478882952, -0.12537537328898907, 0.06865524077452285, -0.0385205305159785, -0.11538191703906239, -0.003881198351358085, 0.3598795233857493, -0.24750388273427826, -0.30298424908501465, -0.012078857894033887, -0.2440243100444245, -0.14592070536428067, 0.12896022965812104, -0.02732233658736... |
709.1593 | Theoretical study of dislocation nucleation from simple surface defects
in semiconductors | Large-scale atomistic calculations, using empirical potentials for modeling
semiconductors, have been performed on a stressed system with linear surface
defects like steps. Although the elastic limits of systems with surface defects
remain close to the theoretical strength, the results show that these defects
weaken ... | cond-mat.mtrl-sci | largescale atomistic calculations using empirical potentials for modeling semiconductors have been performed on a stressed system with linear surface defects like steps although the elastic limits of systems with surface defects remain close to the theoretical strength the results show that these defects weaken the ato... | [['largescale', 'atomistic', 'calculations', 'using', 'empirical', 'potentials', 'for', 'modeling', 'semiconductors', 'have', 'been', 'performed', 'on', 'a', 'stressed', 'system', 'with', 'linear', 'surface', 'defects', 'like', 'steps', 'although', 'the', 'elastic', 'limits', 'of', 'systems', 'with', 'surface', 'defect... | [-0.1188071140253516, 0.1998824806422622, -0.04478895453579515, 0.04024554607588972, 0.002521918888560662, -0.11062304445359612, 0.02827155758261193, 0.4147603259743931, -0.2909325748577575, -0.2763276026958478, 0.06663344227969994, -0.291536189351888, -0.13410248373152045, 0.16640781705696397, 0.02341315205422204, 0.0... |
709.1594 | Temperature dependent sound velocity in hydrodynamic equations for
relativistic heavy-ion collisions | We analyze the effects of different forms of the sound-velocity function
cs(T) on the hydrodynamic evolution of matter formed in the central region of
relativistic heavy-ion collisions. At high temperatures (above the critical
temperature Tc) the sound velocity is calculated from the recent lattice
simulations of QCD... | nucl-th | we analyze the effects of different forms of the soundvelocity function cst on the hydrodynamic evolution of matter formed in the central region of relativistic heavyion collisions at high temperatures above the critical temperature tc the sound velocity is calculated from the recent lattice simulations of qcd while in... | [['we', 'analyze', 'the', 'effects', 'of', 'different', 'forms', 'of', 'the', 'soundvelocity', 'function', 'cst', 'on', 'the', 'hydrodynamic', 'evolution', 'of', 'matter', 'formed', 'in', 'the', 'central', 'region', 'of', 'relativistic', 'heavyion', 'collisions', 'at', 'high', 'temperatures', 'above', 'the', 'critical'... | [-0.12457820436928511, 0.20848477244757677, -0.11134461782151653, 0.029473482198657728, 0.004608788796680509, -0.08274634744501322, 0.038659832397756236, 0.33046182889055703, -0.2379093480531767, -0.27402887499380496, 0.04679491484765544, -0.29528252391885684, -0.022904599836516763, 0.16535681646106945, 0.0532588365405... |
709.1595 | When will a One Parameter Family of Unimodal Maps Produce Finite Limit
Cycles Monotonically with the Parameter? | In this note we consider a collection $\cal{C}$ of one parameter families of
unimodal maps of $[0,1].$ Each family in the collection has the form $\{\mu
f\}$ where $\mu\in [0,1].$ Denoting the kneading sequence of $\mu f$ by $K(\mu
f)$, we will prove that for each member of $\cal{C}$, the map $\mu\mapsto K(\mu
f)$ is... | math.DS | in this note we consider a collection calc of one parameter families of unimodal maps of 01 each family in the collection has the form mu f where muin 01 denoting the kneading sequence of mu f by kmu f we will prove that for each member of calc the map mumapsto kmu f is monotone it then follows that for each member of ... | [['in', 'this', 'note', 'we', 'consider', 'a', 'collection', 'calc', 'of', 'one', 'parameter', 'families', 'of', 'unimodal', 'maps', 'of', '01', 'each', 'family', 'in', 'the', 'collection', 'has', 'the', 'form', 'mu', 'f', 'where', 'muin', '01', 'denoting', 'the', 'kneading', 'sequence', 'of', 'mu', 'f', 'by', 'kmu', '... | [-0.1488078058787188, 0.10800434755954412, -0.007078194529703348, -0.009494244677733889, -0.005131350110958118, -0.15847637999968806, 0.03154566940865341, 0.3184495617146834, -0.3231258795615101, -0.18303251192711367, 0.051793462128867165, -0.32734511416442325, -0.10068383255955016, 0.16429804011546584, -0.108816841197... |
709.1596 | The Effects of Partial Crop Harvest on Biological Pest Control | In this paper, the effects of periodic partial harvesting of a continuously
grown crop on augmentative biological control are analyzed. Partial harvesting
can remove a proportion of both pests and biological control agents, so its
influence on the control efficiency cannot be a priori neglected. An impulsive
model co... | math.DS | in this paper the effects of periodic partial harvesting of a continuously grown crop on augmentative biological control are analyzed partial harvesting can remove a proportion of both pests and biological control agents so its influence on the control efficiency cannot be a priori neglected an impulsive model consisti... | [['in', 'this', 'paper', 'the', 'effects', 'of', 'periodic', 'partial', 'harvesting', 'of', 'a', 'continuously', 'grown', 'crop', 'on', 'augmentative', 'biological', 'control', 'are', 'analyzed', 'partial', 'harvesting', 'can', 'remove', 'a', 'proportion', 'of', 'both', 'pests', 'and', 'biological', 'control', 'agents'... | [-0.14746932638681856, 0.14116216327969933, -0.021084381712732907, 0.04612043650586748, -0.09631549444461822, -0.15298384100661863, 0.06049283966740156, 0.34743630862667585, -0.30019242448803507, -0.3026945490197309, 0.14654981636421888, -0.2919027372182263, -0.14000293930173124, 0.19846541033116236, -0.110484323617009... |
709.1597 | Analytic continuation of residue currents | Let $X$ be a complex manifold and $f\colon X\to \C^p$ a holomorphic mapping
defining a complete intersection. We prove that the iterated Mellin transform
of the residue integral associated to $f$ has an analytic continuation to a
neighborhood of the origin in $\C^p$.
| math.CV | let x be a complex manifold and fcolon xto cp a holomorphic mapping defining a complete intersection we prove that the iterated mellin transform of the residue integral associated to f has an analytic continuation to a neighborhood of the origin in cp | [['let', 'x', 'be', 'a', 'complex', 'manifold', 'and', 'fcolon', 'xto', 'cp', 'a', 'holomorphic', 'mapping', 'defining', 'a', 'complete', 'intersection', 'we', 'prove', 'that', 'the', 'iterated', 'mellin', 'transform', 'of', 'the', 'residue', 'integral', 'associated', 'to', 'f', 'has', 'an', 'analytic', 'continuation',... | [-0.2572664820567466, -0.025008116033521134, -0.15631808843030487, 0.1014539670892233, -0.13471523226173812, -0.09595173596794349, 0.039795203524273494, 0.3276305954123652, -0.3679781791775726, -0.1009308728714322, 0.07569373067370941, -0.26662174345882134, -0.1567389376591458, 0.14957994694799878, -0.07333890257706475... |
709.1598 | Linear convergence of iterative soft-thresholding | In this article a unified approach to iterative soft-thresholding algorithms
for the solution of linear operator equations in infinite dimensional Hilbert
spaces is presented. We formulate the algorithm in the framework of generalized
gradient methods and present a new convergence analysis. As main result we show
tha... | math.FA math.NA | in this article a unified approach to iterative softthresholding algorithms for the solution of linear operator equations in infinite dimensional hilbert spaces is presented we formulate the algorithm in the framework of generalized gradient methods and present a new convergence analysis as main result we show that the... | [['in', 'this', 'article', 'a', 'unified', 'approach', 'to', 'iterative', 'softthresholding', 'algorithms', 'for', 'the', 'solution', 'of', 'linear', 'operator', 'equations', 'in', 'infinite', 'dimensional', 'hilbert', 'spaces', 'is', 'presented', 'we', 'formulate', 'the', 'algorithm', 'in', 'the', 'framework', 'of', '... | [-0.046841539281275366, 0.016285949913387904, -0.13002136074289009, 0.10822093592991014, -0.07966751540575909, -0.14949734202494508, 0.013240182564257965, 0.3845167529108919, -0.35202186590930845, -0.20405413982168327, 0.16112104460948193, -0.1979927345442387, -0.21980180257938986, 0.18473163535474937, -0.0875692548655... |
709.1599 | Experimental Review on Lepton Universality and Lepton Flavour Violation
tests at the B-factories | Since 1999, the B-factories collaborations BABAR and Belle have accumulated
and studied large samples of tau lepton pairs. The experimental results on
Lepton Universality checks and Lepton Flavour Violation searches are reported.
| hep-ex | since 1999 the bfactories collaborations babar and belle have accumulated and studied large samples of tau lepton pairs the experimental results on lepton universality checks and lepton flavour violation searches are reported | [['since', '1999', 'the', 'bfactories', 'collaborations', 'babar', 'and', 'belle', 'have', 'accumulated', 'and', 'studied', 'large', 'samples', 'of', 'tau', 'lepton', 'pairs', 'the', 'experimental', 'results', 'on', 'lepton', 'universality', 'checks', 'and', 'lepton', 'flavour', 'violation', 'searches', 'are', 'reporte... | [-0.07960391578671988, 0.30972385832865257, -0.008790235533524537, 0.17240302162826993, -0.11995996779296547, -0.2244054182083346, 0.11448323397780769, 0.222154107876122, -0.03222426224965602, -0.3069880632683635, -0.03765276445847121, -0.4581461844500154, 0.08591239471570589, 0.09418124437797815, 0.14165453793248162, ... |
709.16 | Relevance of angular momentum conservation in mesoscale hydrodynamics
simulations | The angular momentum is conserved in fluids with a few exceptions such as
ferrofluids. However it can be violated locally in fluid simulations to reduce
computational costs. The effects of this violation are investigated using a
particle-based simulation method, multi-particle collision dynamics, which can
switch on ... | cond-mat.soft | the angular momentum is conserved in fluids with a few exceptions such as ferrofluids however it can be violated locally in fluid simulations to reduce computational costs the effects of this violation are investigated using a particlebased simulation method multiparticle collision dynamics which can switch on or off a... | [['the', 'angular', 'momentum', 'is', 'conserved', 'in', 'fluids', 'with', 'a', 'few', 'exceptions', 'such', 'as', 'ferrofluids', 'however', 'it', 'can', 'be', 'violated', 'locally', 'in', 'fluid', 'simulations', 'to', 'reduce', 'computational', 'costs', 'the', 'effects', 'of', 'this', 'violation', 'are', 'investigated... | [-0.16160038183244246, 0.18065668920723674, -0.0956616503560645, 0.025206371234395564, -0.05217522977747851, -0.12916600449472412, -0.03967095710512283, 0.3472159227085674, -0.2362377755343914, -0.31488717841700864, 0.036974662439260855, -0.2702264206117799, -0.08298606103938869, 0.15810256209383663, -0.048884581627212... |
709.1601 | Temporal evolution of the Evershed flow in sunspots. II. Physical
properties and nature of Evershed clouds | Context: Evershed clouds (ECs) represent the most conspicuous variation of
the Evershed flow in sunspot penumbrae. Aims: We determine the physical
properties of ECs from high spatial and temporal resolution spectropolarimetric
measurements. Methods: The Stokes profiles of four visible and three infrared
spectral line... | astro-ph | context evershed clouds ecs represent the most conspicuous variation of the evershed flow in sunspot penumbrae aims we determine the physical properties of ecs from high spatial and temporal resolution spectropolarimetric measurements methods the stokes profiles of four visible and three infrared spectral lines are sub... | [['context', 'evershed', 'clouds', 'ecs', 'represent', 'the', 'most', 'conspicuous', 'variation', 'of', 'the', 'evershed', 'flow', 'in', 'sunspot', 'penumbrae', 'aims', 'we', 'determine', 'the', 'physical', 'properties', 'of', 'ecs', 'from', 'high', 'spatial', 'and', 'temporal', 'resolution', 'spectropolarimetric', 'me... | [-0.1356709469885876, 0.1417848131444902, -0.06000849696270585, 0.07699203065560863, -0.06195093431669447, -0.07205822429649096, 0.009193700193406528, 0.42204505735420966, -0.21569380230298643, -0.32861504664745284, 0.09910373115043684, -0.23275513574271253, -0.13517024747288978, 0.17134984985055812, -0.037025058021148... |
709.1602 | Is Communication Complexity Physical? | Recently, Brassard et. al. conjectured that the fact that the maximal
possible correlations between two non-local parties are the quantum-mechanical
ones is linked to a reasonable restriction on communication complexity. We
provide further support for the conjecture in the multipartite case. We show
that any multipar... | quant-ph | recently brassard et al conjectured that the fact that the maximal possible correlations between two nonlocal parties are the quantummechanical ones is linked to a reasonable restriction on communication complexity we provide further support for the conjecture in the multipartite case we show that any multipartite comm... | [['recently', 'brassard', 'et', 'al', 'conjectured', 'that', 'the', 'fact', 'that', 'the', 'maximal', 'possible', 'correlations', 'between', 'two', 'nonlocal', 'parties', 'are', 'the', 'quantummechanical', 'ones', 'is', 'linked', 'to', 'a', 'reasonable', 'restriction', 'on', 'communication', 'complexity', 'we', 'provid... | [-0.15240995394783474, 0.10978855095846503, -0.09809837534035347, 0.1049112041994017, -0.08052601239510945, -0.1931483467746222, 0.04623365812645085, 0.3118664920805212, -0.23192104889394427, -0.3039605590516027, 0.01643780049896438, -0.2679292434251544, -0.16398497923676456, 0.19208405315115742, -0.11961476399316168, ... |
709.1603 | The Nonlinear Essence of Gravitational Waves | A critical review of gravitational wave theory is made. It is pointed out
that the usual linear approach to the gravitational wave theory is neither
conceptually consistent nor mathematically justified. Relying upon that
analysis it is then argued that -- analogously to a Yang-Mills propagating
field, which must be n... | gr-qc hep-th | a critical review of gravitational wave theory is made it is pointed out that the usual linear approach to the gravitational wave theory is neither conceptually consistent nor mathematically justified relying upon that analysis it is then argued that analogously to a yangmills propagating field which must be nonlinear ... | [['a', 'critical', 'review', 'of', 'gravitational', 'wave', 'theory', 'is', 'made', 'it', 'is', 'pointed', 'out', 'that', 'the', 'usual', 'linear', 'approach', 'to', 'the', 'gravitational', 'wave', 'theory', 'is', 'neither', 'conceptually', 'consistent', 'nor', 'mathematically', 'justified', 'relying', 'upon', 'that', ... | [-0.15656395089151204, 0.1780485580742791, -0.1811900307977761, 0.0856010260320255, -0.1957401619495257, -0.13541582914447223, -0.0137369012615333, 0.3489079285359037, -0.22673418421460234, -0.17232096293752175, 0.09105982639543388, -0.25485259019162343, -0.22250626896224593, 0.1615167782554214, 0.010724967656036219, 0... |
709.1604 | First principles determination of the Peierls stress of the shuffle
screw dislocation in silicon | The Peierls stress of the a/2<110> screw dislocation belonging to the shuffle
set is calculated for silicon using density functional theory. We have checked
the effect of boundary conditions by using two models, the supercell method
where one considers a periodic array of dislocations, and the cluster method
where a ... | cond-mat.mtrl-sci | the peierls stress of the a2110 screw dislocation belonging to the shuffle set is calculated for silicon using density functional theory we have checked the effect of boundary conditions by using two models the supercell method where one considers a periodic array of dislocations and the cluster method where a single d... | [['the', 'peierls', 'stress', 'of', 'the', 'a2110', 'screw', 'dislocation', 'belonging', 'to', 'the', 'shuffle', 'set', 'is', 'calculated', 'for', 'silicon', 'using', 'density', 'functional', 'theory', 'we', 'have', 'checked', 'the', 'effect', 'of', 'boundary', 'conditions', 'by', 'using', 'two', 'models', 'the', 'supe... | [-0.12617910742320546, 0.18030189591028342, -0.027858640612443773, 0.01691555205119274, 0.019878481969055607, -0.07429698921694625, 0.06883795534005499, 0.3805496641624022, -0.24743066228381017, -0.31538069046034317, 0.04464773567984017, -0.266401053856816, -0.08284191966692848, 0.12147791526939083, 0.03168595621856383... |
709.1605 | Ab initio molecular dynamics calculations of threshold displacement
energies in silicon carbide | Using first principles molecular dynamics simulations, we have determined the
threshold displacement energies and the associated created defects in cubic
silicon carbide. Contrary to previous studies using classical molecular
dynamics, we found values close to the experimental consensus, and also created
defects in g... | cond-mat.mtrl-sci | using first principles molecular dynamics simulations we have determined the threshold displacement energies and the associated created defects in cubic silicon carbide contrary to previous studies using classical molecular dynamics we found values close to the experimental consensus and also created defects in good ag... | [['using', 'first', 'principles', 'molecular', 'dynamics', 'simulations', 'we', 'have', 'determined', 'the', 'threshold', 'displacement', 'energies', 'and', 'the', 'associated', 'created', 'defects', 'in', 'cubic', 'silicon', 'carbide', 'contrary', 'to', 'previous', 'studies', 'using', 'classical', 'molecular', 'dynami... | [-0.046277896636315895, 0.09695042308510071, -0.060596311825417706, 0.00013971572581638573, 0.03071886429222681, -0.10990187393561486, 0.07168666291881794, 0.48270702586379105, -0.2191853248514235, -0.29191113800130863, 0.020358115270663734, -0.3128178927606793, -0.16927501651388344, 0.18735428456898018, 0.001684855649... |
709.1606 | Local and global methods in arithmetic (in Russian) | Let $p$ be a prime. We discuss methods of solution of congruences modulo
$p^n$ using $p$-adic numbers; these methods are similar to computations with
real numbers (local methods). Examples of relations between local and global
methods are given producing a passage from congruences to solutions in integers
(global met... | math.NT | let p be a prime we discuss methods of solution of congruences modulo pn using padic numbers these methods are similar to computations with real numbers local methods examples of relations between local and global methods are given producing a passage from congruences to solutions in integers global methods the use of ... | [['let', 'p', 'be', 'a', 'prime', 'we', 'discuss', 'methods', 'of', 'solution', 'of', 'congruences', 'modulo', 'pn', 'using', 'padic', 'numbers', 'these', 'methods', 'are', 'similar', 'to', 'computations', 'with', 'real', 'numbers', 'local', 'methods', 'examples', 'of', 'relations', 'between', 'local', 'and', 'global',... | [-0.21009883981605526, 0.008948675313149579, -0.17719827516702935, 0.09887478900236601, -0.06080314530117903, -0.11310439634689828, 0.01202581603138242, 0.30889811101951636, -0.31624847976490855, -0.3088302323012613, 0.06781620185756765, -0.28968174928741064, -0.14096669508944615, 0.3045739179942757, -0.060891140732564... |
709.1607 | The hyperbolic geometric flow on Riemann surfaces | In this paper the authors study the hyperbolic geometric flow on Riemann
surfaces. This new nonlinear geometric evolution equation was recently
introduced by the first two authors motivated by Einstein equation and
Hamilton's Ricci flow. We prove that, for any given initial metric on
${\mathbb{R}}^{2}$ in certain cla... | math.DG math.AP | in this paper the authors study the hyperbolic geometric flow on riemann surfaces this new nonlinear geometric evolution equation was recently introduced by the first two authors motivated by einstein equation and hamiltons ricci flow we prove that for any given initial metric on mathbbr2 in certain class of metrics on... | [['in', 'this', 'paper', 'the', 'authors', 'study', 'the', 'hyperbolic', 'geometric', 'flow', 'on', 'riemann', 'surfaces', 'this', 'new', 'nonlinear', 'geometric', 'evolution', 'equation', 'was', 'recently', 'introduced', 'by', 'the', 'first', 'two', 'authors', 'motivated', 'by', 'einstein', 'equation', 'and', 'hamilto... | [-0.1646426136648261, 0.12153734750550604, -0.12035588995853289, 0.040781646913409915, -0.13910785895215624, -0.17157250360703502, -0.0697484764413662, 0.32943908633642843, -0.2898810900555089, -0.21093335834963398, 0.14594011148571667, -0.26452630749454015, -0.13596819397115587, 0.166144285013835, -0.10041031715909726... |
709.1608 | First results on e^+e^- -> 3 jets at NNLO | Precision studies of QCD at $e^+e^-$ colliders are based on measurements of
event shapes and jet rates. To match the high experimental accuracy,
theoretical predictions to next-to-next-to-leading order (NNLO) in QCD are
needed for a reliable interpretation of the data. We report the first
calculation of NNLO correcti... | hep-ph | precision studies of qcd at ee colliders are based on measurements of event shapes and jet rates to match the high experimental accuracy theoretical predictions to nexttonexttoleading order nnlo in qcd are needed for a reliable interpretation of the data we report the first calculation of nnlo corrections cal oalpha_s3... | [['precision', 'studies', 'of', 'qcd', 'at', 'ee', 'colliders', 'are', 'based', 'on', 'measurements', 'of', 'event', 'shapes', 'and', 'jet', 'rates', 'to', 'match', 'the', 'high', 'experimental', 'accuracy', 'theoretical', 'predictions', 'to', 'nexttonexttoleading', 'order', 'nnlo', 'in', 'qcd', 'are', 'needed', 'for',... | [-0.06996759047145926, 0.06742260285142448, -0.1095223187153498, 0.13545084906171165, -0.08086904372659422, -0.041806015554034424, 0.034483152111211134, 0.4102386150869631, -0.09371381578966975, -0.2930320991924213, 0.05280484662263564, -0.3998640775680542, 0.04327682789505249, 0.150505980656993, 0.043624228422319694, ... |
709.1609 | The surprising external upturn of the Blue Straggler radial distribution
in M55 | By combining high-resolution HST and wide-field ground based observations, in
ultraviolet and optical bands, we study the Blue Straggler Star (BSS)
population of the low density galactic globular cluster M55 (NGC 6809) over its
entire radial extent. The BSS projected radial distribution is found to be
bimodal, with a... | astro-ph | by combining highresolution hst and widefield ground based observations in ultraviolet and optical bands we study the blue straggler star bss population of the low density galactic globular cluster m55 ngc 6809 over its entire radial extent the bss projected radial distribution is found to be bimodal with a central pea... | [['by', 'combining', 'highresolution', 'hst', 'and', 'widefield', 'ground', 'based', 'observations', 'in', 'ultraviolet', 'and', 'optical', 'bands', 'we', 'study', 'the', 'blue', 'straggler', 'star', 'bss', 'population', 'of', 'the', 'low', 'density', 'galactic', 'globular', 'cluster', 'm55', 'ngc', '6809', 'over', 'it... | [-0.08893518730829375, 0.1023451041841126, -0.1153232195051607, 0.09783613029134086, -0.06795055260258455, -0.05042144249919362, 0.07704730639894178, 0.4219706821655048, -0.12382260850799365, -0.3910721994159142, 0.017081434249980595, -0.30311479293337956, -0.028606370835763027, 0.15643610628541765, -0.0777226632871613... |
709.161 | On q-summation and confluence | This paper is divided in two parts. In the first part we consider irregular
singular analytic q-difference equations, with q\in ]0,1[, and we show how the
Borel sum of a divergent solution of a differential equation can be uniformly
approximated on a convenient sector by a meromorphic solution of such a
q-difference ... | math.CA math.QA | this paper is divided in two parts in the first part we consider irregular singular analytic qdifference equations with qin 01 and we show how the borel sum of a divergent solution of a differential equation can be uniformly approximated on a convenient sector by a meromorphic solution of such a qdifference equation in... | [['this', 'paper', 'is', 'divided', 'in', 'two', 'parts', 'in', 'the', 'first', 'part', 'we', 'consider', 'irregular', 'singular', 'analytic', 'qdifference', 'equations', 'with', 'qin', '01', 'and', 'we', 'show', 'how', 'the', 'borel', 'sum', 'of', 'a', 'divergent', 'solution', 'of', 'a', 'differential', 'equation', 'c... | [-0.20389271507096685, 0.00562368220859326, -0.1272297876367906, 0.07895861717525451, -0.08725859700911204, -0.10545554557549101, -0.013623239613869893, 0.309029556392711, -0.3034947839499052, -0.18073330150575054, 0.10154055012746391, -0.323180155629026, -0.18539099127282294, 0.1871563702707692, -0.07103006352138307, ... |
709.1611 | Modular forms and $p$-adic numbers (in Russian) | Let $p$ be a prime. We discuss $p$-adic properties of various arithmetical
functions related to the coefficients of modular form and generating functions.
Modular forms are considered as a tool of solving arithmetical problems.
Examples of congruences between modular forms modulo $p$ and modulo $p^n$ are
given, and t... | math.NT | let p be a prime we discuss padic properties of various arithmetical functions related to the coefficients of modular form and generating functions modular forms are considered as a tool of solving arithmetical problems examples of congruences between modular forms modulo p and modulo pn are given and the use of a comp... | [['let', 'p', 'be', 'a', 'prime', 'we', 'discuss', 'padic', 'properties', 'of', 'various', 'arithmetical', 'functions', 'related', 'to', 'the', 'coefficients', 'of', 'modular', 'form', 'and', 'generating', 'functions', 'modular', 'forms', 'are', 'considered', 'as', 'a', 'tool', 'of', 'solving', 'arithmetical', 'problem... | [-0.2346078020054847, 0.03444429597196479, -0.15078574827251334, 0.09546790165865483, -0.10713576994215449, -0.12991850199953964, -0.05586409536190331, 0.2552954156727841, -0.34802753968785205, -0.2728109237427513, 0.062276375208360456, -0.2676465801506614, -0.2010903758229688, 0.30969575569033625, -0.00746750979063411... |
709.1612 | VLT/SINFONI Integral Field Spectroscopy of The Super-antennae | We present the results of H- and K-band VLT/SINFONI integral field
spectroscopy of the ULIRG IRAS 19254-7245 (The Super-antennae), an interacting
double galaxy system containing an embedded AGN. Deep K-band spectroscopy
reveals PaAlpha arising in a warped disc with position angle of 330 degree and
an inclination i=40... | astro-ph | we present the results of h and kband vltsinfoni integral field spectroscopy of the ulirg iras 192547245 the superantennae an interacting double galaxy system containing an embedded agn deep kband spectroscopy reveals paalpha arising in a warped disc with position angle of 330 degree and an inclination i4055 degree the... | [['we', 'present', 'the', 'results', 'of', 'h', 'and', 'kband', 'vltsinfoni', 'integral', 'field', 'spectroscopy', 'of', 'the', 'ulirg', 'iras', '192547245', 'the', 'superantennae', 'an', 'interacting', 'double', 'galaxy', 'system', 'containing', 'an', 'embedded', 'agn', 'deep', 'kband', 'spectroscopy', 'reveals', 'paa... | [-0.03513547115009995, 0.0693312546932131, 0.021344718750184163, 0.07652345332928981, -0.03748285189832155, -0.11964611714490904, 0.0015835196827538311, 0.5184655736128871, -0.13928731840450126, -0.2864984061855536, 0.043696084714984186, -0.311085052215136, 0.032065200458209105, 0.1416765363403381, 0.006485395112227147... |
709.1613 | WIMP Gamma Rays From the Galactic Center with GLAST and Accelerator
Comparison | We will describe the prospects for detecting gamma-rays from WIMP's
annihilation in the Galactic Center and we compare this search with the
possibilities at LHC and with space antimatter experiments like PAMELA.
| astro-ph hep-ph | we will describe the prospects for detecting gammarays from wimps annihilation in the galactic center and we compare this search with the possibilities at lhc and with space antimatter experiments like pamela | [['we', 'will', 'describe', 'the', 'prospects', 'for', 'detecting', 'gammarays', 'from', 'wimps', 'annihilation', 'in', 'the', 'galactic', 'center', 'and', 'we', 'compare', 'this', 'search', 'with', 'the', 'possibilities', 'at', 'lhc', 'and', 'with', 'space', 'antimatter', 'experiments', 'like', 'pamela']] | [0.014724751323228702, 0.23832856660010293, -0.06307595247926656, 0.14867602391677792, -0.12368046905612573, -0.06351032399106771, 0.0179168488830328, 0.37232498262892477, -0.23578250216087326, -0.35902363242348656, -0.03693067313361098, -0.4060172834142577, -0.0035377967869862914, 0.27694702415465144, 0.07815169310197... |
709.1614 | Cavity losses for the dissipative Jaynes-Cummings Hamiltonian beyond
Rotating Wave Approximation | A microscopic derivation of the master equation for the
Jaynes-Cummings model with cavity losses is given, taking into account the
terms in the dissipator which vary with frequencies of the order of the vacuum
Rabi frequency. Our approach allows to single out physical contexts wherein the
usual phenomenological dis... | quant-ph | a microscopic derivation of the master equation for the jaynescummings model with cavity losses is given taking into account the terms in the dissipator which vary with frequencies of the order of the vacuum rabi frequency our approach allows to single out physical contexts wherein the usual phenomenological dissipator... | [['a', 'microscopic', 'derivation', 'of', 'the', 'master', 'equation', 'for', 'the', 'jaynescummings', 'model', 'with', 'cavity', 'losses', 'is', 'given', 'taking', 'into', 'account', 'the', 'terms', 'in', 'the', 'dissipator', 'which', 'vary', 'with', 'frequencies', 'of', 'the', 'order', 'of', 'the', 'vacuum', 'rabi', ... | [-0.1032969151115553, 0.06837961099005373, -0.07501633498098025, -0.05051960133476479, -0.11004952026467602, -0.10352667422690005, 0.07317729239135091, 0.2762428319229829, -0.18255667441355233, -0.31703277154486964, -0.036840505789520896, -0.22416616269583756, -0.11999992065300996, 0.18698737366834062, -0.0411758731193... |
709.1615 | On permutation polytopes | A permutation polytope is the convex hull of a group of permutation matrices.
In this paper we investigate the combinatorics of permutation polytopes and
their faces. As applications we completely classify permutation polytopes in
dimensions 2,3,4, and the corresponding permutation groups up to a suitable
notion of e... | math.CO math.GR math.RT | a permutation polytope is the convex hull of a group of permutation matrices in this paper we investigate the combinatorics of permutation polytopes and their faces as applications we completely classify permutation polytopes in dimensions 234 and the corresponding permutation groups up to a suitable notion of equivale... | [['a', 'permutation', 'polytope', 'is', 'the', 'convex', 'hull', 'of', 'a', 'group', 'of', 'permutation', 'matrices', 'in', 'this', 'paper', 'we', 'investigate', 'the', 'combinatorics', 'of', 'permutation', 'polytopes', 'and', 'their', 'faces', 'as', 'applications', 'we', 'completely', 'classify', 'permutation', 'polyt... | [-0.13651415003366324, 0.10180863110286031, -0.050225427318642386, 0.04502821242464567, -0.064697237282213, -0.11223234922917032, 0.0945799575315844, 0.3545521557775896, -0.3992610869567786, -0.2546487892699887, 0.15294893308014457, -0.2828003282366849, -0.18177041201504754, 0.10409651406164934, -0.21784179874542933, 0... |
709.1616 | Bandwidth Selection for Weighted Kernel Density Estimation | In the this paper, the authors propose to estimate the density of a targeted
population with a weighted kernel density estimator (wKDE) based on a weighted
sample. Bandwidth selection for wKDE is discussed. Three mean integrated
squared error based bandwidth estimators are introduced and their performance
is illustra... | stat.ME | in the this paper the authors propose to estimate the density of a targeted population with a weighted kernel density estimator wkde based on a weighted sample bandwidth selection for wkde is discussed three mean integrated squared error based bandwidth estimators are introduced and their performance is illustrated via... | [['in', 'the', 'this', 'paper', 'the', 'authors', 'propose', 'to', 'estimate', 'the', 'density', 'of', 'a', 'targeted', 'population', 'with', 'a', 'weighted', 'kernel', 'density', 'estimator', 'wkde', 'based', 'on', 'a', 'weighted', 'sample', 'bandwidth', 'selection', 'for', 'wkde', 'is', 'discussed', 'three', 'mean', ... | [-0.04778663188171981, 0.00017943117097857293, -0.0897579440700539, 0.12375838926527649, -0.07813474804874551, -0.1309750506424167, 0.091953349374287, 0.44804956144496294, -0.24455591375950012, -0.29745708205580207, 0.17242325586920834, -0.2688936225316498, -0.1260784615041803, 0.19139427921912644, -0.10729781638705328... |
709.1617 | Frequency and damping of the Scissors Mode of a Fermi gas | We calculate the frequency and damping of the scissors mode in a classical
gas as a function of temperature and coupling strength. Our results show good
agreement with the main features observed in recent measurements of the
scissors mode in an ultracold gas of $^6$Li atoms. The comparison between
theory and experime... | cond-mat.stat-mech cond-mat.other | we calculate the frequency and damping of the scissors mode in a classical gas as a function of temperature and coupling strength our results show good agreement with the main features observed in recent measurements of the scissors mode in an ultracold gas of 6li atoms the comparison between theory and experiment invo... | [['we', 'calculate', 'the', 'frequency', 'and', 'damping', 'of', 'the', 'scissors', 'mode', 'in', 'a', 'classical', 'gas', 'as', 'a', 'function', 'of', 'temperature', 'and', 'coupling', 'strength', 'our', 'results', 'show', 'good', 'agreement', 'with', 'the', 'main', 'features', 'observed', 'in', 'recent', 'measurement... | [-0.09751047141617164, 0.14667578927349365, -0.07448835133441857, 0.020769314102030225, 0.01707501709461212, -0.10998517180393849, 0.09268512524098955, 0.31667134067309755, -0.21225947280015264, -0.2952336205967835, -0.0012215280431389277, -0.31152135565165995, -0.09219058473993624, 0.23771104320351566, 0.0241478971671... |
709.1618 | Yield scaling, size hierarchy and fluctuations of observables in
fragmentation of excited heavy nuclei | Multifragmentation properties measured with INDRA are studied for single
sources produced in Xe+Sn reactions in the incident energy range 32-50 A MeV
and quasiprojectiles from Au+Au collisions at 80 A MeV. A comparison for both
types of sources is presented concerning Fisher scaling, Zipf law, fragment
size and fluct... | nucl-ex | multifragmentation properties measured with indra are studied for single sources produced in xesn reactions in the incident energy range 3250 a mev and quasiprojectiles from auau collisions at 80 a mev a comparison for both types of sources is presented concerning fisher scaling zipf law fragment size and fluctuation o... | [['multifragmentation', 'properties', 'measured', 'with', 'indra', 'are', 'studied', 'for', 'single', 'sources', 'produced', 'in', 'xesn', 'reactions', 'in', 'the', 'incident', 'energy', 'range', '3250', 'a', 'mev', 'and', 'quasiprojectiles', 'from', 'auau', 'collisions', 'at', '80', 'a', 'mev', 'a', 'comparison', 'for... | [-0.04087222893549888, 0.16962595390483598, -0.13177435826596426, 0.150742190409262, 0.062442304555184416, -0.0983407396900778, 0.024441797027571335, 0.3174595411401242, -0.21155136933170812, -0.3246980358467058, -0.007967604280026906, -0.4337277558752922, 0.04547508400692432, 0.2088594933782049, 0.0602323082337669, 0.... |
709.1619 | Vector modes generated by primordial density fluctuations | While vector modes are usually ignored in cosmology since they are not
produced during inflation they are inevitably produced from the interaction of
density fluctuations of differing wavelengths. This effect may be calculated
via a second-order perturbative expansion. We investigate this effect during
the radiation ... | astro-ph gr-qc | while vector modes are usually ignored in cosmology since they are not produced during inflation they are inevitably produced from the interaction of density fluctuations of differing wavelengths this effect may be calculated via a secondorder perturbative expansion we investigate this effect during the radiation era w... | [['while', 'vector', 'modes', 'are', 'usually', 'ignored', 'in', 'cosmology', 'since', 'they', 'are', 'not', 'produced', 'during', 'inflation', 'they', 'are', 'inevitably', 'produced', 'from', 'the', 'interaction', 'of', 'density', 'fluctuations', 'of', 'differing', 'wavelengths', 'this', 'effect', 'may', 'be', 'calcul... | [-0.18313748335563823, 0.29361440004829903, -0.10697981791178647, 0.09905653697129119, -0.039484042407773236, -0.07653226234680532, -0.059406338492408395, 0.34823590856486636, -0.2655207328130736, -0.28077654172911454, 0.09038515334281041, -0.2908776858515155, -0.0997345241056265, 0.15252223811847598, 0.060516400850917... |
709.162 | Quantum Stephani exact cosmological solutions and the selection of time
variable | We study perfect fluid Stephani quantum cosmological model. In the present
work the Schutz's variational formalism which recovers the notion of time is
applied. This gives rise to Wheeler-DeWitt equation for the scale factor. We
use the eigenfunctions in order to construct wave packets for each case. We
study the tim... | gr-qc | we study perfect fluid stephani quantum cosmological model in the present work the schutzs variational formalism which recovers the notion of time is applied this gives rise to wheelerdewitt equation for the scale factor we use the eigenfunctions in order to construct wave packets for each case we study the timedepende... | [['we', 'study', 'perfect', 'fluid', 'stephani', 'quantum', 'cosmological', 'model', 'in', 'the', 'present', 'work', 'the', 'schutzs', 'variational', 'formalism', 'which', 'recovers', 'the', 'notion', 'of', 'time', 'is', 'applied', 'this', 'gives', 'rise', 'to', 'wheelerdewitt', 'equation', 'for', 'the', 'scale', 'fact... | [-0.1277845750138273, 0.0649031794301289, -0.13505213919287437, 0.07311396830824807, -0.08757396228611469, -0.10616071968038074, -0.014854812388554873, 0.2787034295444541, -0.26123099235358976, -0.2708733191384989, 0.01779846614569097, -0.23596223334179206, -0.14782974161618553, 0.12813466087305536, -0.0275041858857388... |
709.1621 | On the Configuration Spaces of Homogeneous Loop Quantum Cosmology and
Loop Quantum Gravity | The set of homogeneous isotropic connections, as used in loop quantum
cosmology, forms a line $l$ in the space of all connections $\cal A$. This
embedding, however, does not continuously extend to an embedding of the
configuration space $\overline l$ of homogeneous isotropic loop quantum
cosmology into that of loop q... | math-ph gr-qc math.MP | the set of homogeneous isotropic connections as used in loop quantum cosmology forms a line l in the space of all connections cal a this embedding however does not continuously extend to an embedding of the configuration space overline l of homogeneous isotropic loop quantum cosmology into that of loop quantum gravity ... | [['the', 'set', 'of', 'homogeneous', 'isotropic', 'connections', 'as', 'used', 'in', 'loop', 'quantum', 'cosmology', 'forms', 'a', 'line', 'l', 'in', 'the', 'space', 'of', 'all', 'connections', 'cal', 'a', 'this', 'embedding', 'however', 'does', 'not', 'continuously', 'extend', 'to', 'an', 'embedding', 'of', 'the', 'co... | [-0.17215258794901675, 0.1840385601242942, -0.05658993140664385, 0.05959958732290583, -0.1011302427139653, -0.1392306879996647, 0.009612298543499999, 0.35427577763276047, -0.26666226478964955, -0.2019681185592226, 0.06325436028419062, -0.23557596196702055, -0.1361676236224729, 0.22125518213833012, -0.04888081833243717,... |
709.1622 | Dark Energy, scalar-curvature couplings and a critical acceleration
scale | We study the effects of coupling a cosmologically rolling scalar field to
higher order curvature terms. We show that when the strong coupling scale of
the theory is on the 10^{-3}-10^{-1}eV range, the model passes all experimental
bounds on the existence of fifth forces even if the field has a mass of the
order of th... | astro-ph gr-qc hep-ph hep-th | we study the effects of coupling a cosmologically rolling scalar field to higher order curvature terms we show that when the strong coupling scale of the theory is on the 103101ev range the model passes all experimental bounds on the existence of fifth forces even if the field has a mass of the order of the hubble scal... | [['we', 'study', 'the', 'effects', 'of', 'coupling', 'a', 'cosmologically', 'rolling', 'scalar', 'field', 'to', 'higher', 'order', 'curvature', 'terms', 'we', 'show', 'that', 'when', 'the', 'strong', 'coupling', 'scale', 'of', 'the', 'theory', 'is', 'on', 'the', '103101ev', 'range', 'the', 'model', 'passes', 'all', 'ex... | [-0.160079320490412, 0.17009384979877115, -0.09201213479714675, 0.08540920655359514, -0.10085598410288286, -0.09127889116255877, 0.011157900458460466, 0.3160594030386872, -0.25262900979982483, -0.30905787696441017, 0.0959346314432979, -0.2591296544195049, -0.1002223296996413, 0.176999970283618, 0.01863820877754026, -9.... |
709.1623 | Dynamic correlations in an ordered c(2$\times$2) lattice gas | We obtain the dynamic correlation function of two-dimensional lattice gas
with nearest-neighbor repulsion in ordered c(2$\times$2) phase
(antiferromagnetic ordering) under the condition of low concentration of
structural defects. It is shown that displacements of defects of the ordered
state are responsible for the p... | cond-mat.stat-mech | we obtain the dynamic correlation function of twodimensional lattice gas with nearestneighbor repulsion in ordered c2times2 phase antiferromagnetic ordering under the condition of low concentration of structural defects it is shown that displacements of defects of the ordered state are responsible for the particle numb... | [['we', 'obtain', 'the', 'dynamic', 'correlation', 'function', 'of', 'twodimensional', 'lattice', 'gas', 'with', 'nearestneighbor', 'repulsion', 'in', 'ordered', 'c2times2', 'phase', 'antiferromagnetic', 'ordering', 'under', 'the', 'condition', 'of', 'low', 'concentration', 'of', 'structural', 'defects', 'it', 'is', 's... | [-0.12113819120399233, 0.19550774410712501, -0.0565342167572629, 0.10676767264582938, 0.0024901937738421465, -0.11179792135953903, 0.009687800372710392, 0.3515622689598991, -0.2449159997545423, -0.312896445153221, 0.054434433293288516, -0.3315480972129491, -0.09876988344345122, 0.15805381351571168, 0.018292996743994375... |
709.1624 | Black Hole Thermodynamics and the Factor of 2 Problem | We show that the recent tunneling formulas for black hole radiation in
static, spherically symmetric spacetimes follow as a consequence of the first
law of black hole thermodynamics and the area-entropy relation based on the
radiation temperature. A tunneling formula results even if the radiation
temperature is diffe... | gr-qc astro-ph hep-th | we show that the recent tunneling formulas for black hole radiation in static spherically symmetric spacetimes follow as a consequence of the first law of black hole thermodynamics and the areaentropy relation based on the radiation temperature a tunneling formula results even if the radiation temperature is different ... | [['we', 'show', 'that', 'the', 'recent', 'tunneling', 'formulas', 'for', 'black', 'hole', 'radiation', 'in', 'static', 'spherically', 'symmetric', 'spacetimes', 'follow', 'as', 'a', 'consequence', 'of', 'the', 'first', 'law', 'of', 'black', 'hole', 'thermodynamics', 'and', 'the', 'areaentropy', 'relation', 'based', 'on... | [-0.08269584626369006, 0.13917644469809062, -0.11194690122458807, 0.09808370831025834, -0.04267523580023812, -0.145425214095869, 0.00033389004831271314, 0.29377871182643706, -0.20287690496210148, -0.2822835894077326, 0.057306507504243334, -0.3129851520665128, -0.12828888524651388, 0.23085004816487156, -0.04168823654092... |
709.1625 | On the possibility of Dark Energy from corrections to the Wheeler-De
Witt equation | We present a method for approximating the effective consequence of generic
quantum gravity corrections to the Wheeler-DeWitt equation. We show that in
many cases these corrections can produce departures from classical physics at
large scales and that this behaviour can be interpreted as additional matter
components. ... | gr-qc astro-ph hep-ph hep-th | we present a method for approximating the effective consequence of generic quantum gravity corrections to the wheelerdewitt equation we show that in many cases these corrections can produce departures from classical physics at large scales and that this behaviour can be interpreted as additional matter components this ... | [['we', 'present', 'a', 'method', 'for', 'approximating', 'the', 'effective', 'consequence', 'of', 'generic', 'quantum', 'gravity', 'corrections', 'to', 'the', 'wheelerdewitt', 'equation', 'we', 'show', 'that', 'in', 'many', 'cases', 'these', 'corrections', 'can', 'produce', 'departures', 'from', 'classical', 'physics'... | [-0.11874152263798923, 0.15706528343812184, -0.14121672431334714, 0.16643958565287498, -0.09923139671553616, -0.11961155451178827, -0.0256863529017816, 0.2385333114243285, -0.31892345565009034, -0.34761169211749265, 0.05527354049802482, -0.2446123706219994, -0.13451209340645517, 0.19738758733082148, -0.0249205710241329... |
709.1626 | Astrometry of Water Maser Sources in Nearby Molecular Clouds with VERA -
II. SVS 13 in NGC 1333 | We report on the results of multi-epoch VLBI observations with VERA (VLBI
Exploration of Radio Astrometry) of the 22 GHz H2O masers associated with the
young stellar object SVS 13 in the NGC 1333 region. We have carried out
phase-referencing VLBI astrometry and measured an annual parallax of the maser
features in SVS... | astro-ph | we report on the results of multiepoch vlbi observations with vera vlbi exploration of radio astrometry of the 22 ghz h2o masers associated with the young stellar object svs 13 in the ngc 1333 region we have carried out phasereferencing vlbi astrometry and measured an annual parallax of the maser features in svs 13 of ... | [['we', 'report', 'on', 'the', 'results', 'of', 'multiepoch', 'vlbi', 'observations', 'with', 'vera', 'vlbi', 'exploration', 'of', 'radio', 'astrometry', 'of', 'the', '22', 'ghz', 'h2o', 'masers', 'associated', 'with', 'the', 'young', 'stellar', 'object', 'svs', '13', 'in', 'the', 'ngc', '1333', 'region', 'we', 'have',... | [-0.07385179910477231, 0.03988653801252678, -0.05997282747370959, -0.005666220529585179, -0.13093933311208147, -0.08107688412599325, 0.03266282861257528, 0.48423566645820726, -0.15334871851507556, -0.33167361827684244, 0.12048963773373944, -0.2718036163754332, 0.019098784939108018, 0.19656815739465555, -0.0368329462223... |
709.1627 | Formulas of F-thresholds and F-jumping coefficients on toric rings | F-thresholds are defined by Mustata, Takagi and Watanabe in [F-thresholds and
Bernstein-Sato polynomials], which are invariants of the pair of ideals on
rings of characteristic $p$. In their paper, it is proved F-thresholds equal to
jumping numbers for the test ideal on regular local rings. In this note, we
give an f... | math.AC math.AG | fthresholds are defined by mustata takagi and watanabe in fthresholds and bernsteinsato polynomials which are invariants of the pair of ideals on rings of characteristic p in their paper it is proved fthresholds equal to jumping numbers for the test ideal on regular local rings in this note we give an formula of fthres... | [['fthresholds', 'are', 'defined', 'by', 'mustata', 'takagi', 'and', 'watanabe', 'in', 'fthresholds', 'and', 'bernsteinsato', 'polynomials', 'which', 'are', 'invariants', 'of', 'the', 'pair', 'of', 'ideals', 'on', 'rings', 'of', 'characteristic', 'p', 'in', 'their', 'paper', 'it', 'is', 'proved', 'fthresholds', 'equal'... | [-0.22455248323028848, -0.0019160729676631519, -0.08127511413993253, 0.13575915841671127, -0.033441822970240946, -0.1475359894853506, -0.02028508033817484, 0.29881447190118415, -0.3017554461633066, -0.19837441966838895, 0.07986418386609594, -0.26017808067732523, -0.1639746878175966, 0.2382821878268113, -0.1626306496290... |
709.1628 | On the nonextensive character of some magnetic systems | During the past few years, nonextensive statistics has been successfully
applied to explain many different kinds of systems. Through these studies some
interpretations of the entropic parameter q, which has major role in this
statistics, in terms of physical quantities have been obtained. The aim of the
present work ... | cond-mat.stat-mech | during the past few years nonextensive statistics has been successfully applied to explain many different kinds of systems through these studies some interpretations of the entropic parameter q which has major role in this statistics in terms of physical quantities have been obtained the aim of the present work is to y... | [['during', 'the', 'past', 'few', 'years', 'nonextensive', 'statistics', 'has', 'been', 'successfully', 'applied', 'to', 'explain', 'many', 'different', 'kinds', 'of', 'systems', 'through', 'these', 'studies', 'some', 'interpretations', 'of', 'the', 'entropic', 'parameter', 'q', 'which', 'has', 'major', 'role', 'in', '... | [-0.0885980137733414, 0.09950510568095898, -0.12204897666678709, 0.05333632784073844, -0.03754023917238502, -0.05714052175993428, -0.07206963798757095, 0.3409150371547131, -0.2564932618440841, -0.35371655288755016, 0.09881791370057993, -0.2505037441082737, -0.150768895239761, 0.2612571056713076, -0.07772892949801377, 0... |
709.1629 | Disordered pinning models and copolymers: beyond annealed bounds | We consider a general model of a disordered copolymer with adsorption. This
includes, as particular cases, a generalization of the copolymer at a selective
interface introduced by Garel et al. [Europhys. Lett. 8 (1989) 9--13], pinning
and wetting models in various dimensions, and the Poland--Scheraga model of DNA
den... | math.PR cond-mat.soft | we consider a general model of a disordered copolymer with adsorption this includes as particular cases a generalization of the copolymer at a selective interface introduced by garel et al europhys lett 8 1989 913 pinning and wetting models in various dimensions and the polandscheraga model of dna denaturation we prove... | [['we', 'consider', 'a', 'general', 'model', 'of', 'a', 'disordered', 'copolymer', 'with', 'adsorption', 'this', 'includes', 'as', 'particular', 'cases', 'a', 'generalization', 'of', 'the', 'copolymer', 'at', 'a', 'selective', 'interface', 'introduced', 'by', 'garel', 'et', 'al', 'europhys', 'lett', '8', '1989', '913',... | [-0.09974830548377021, 0.13475073706067633, -0.08130674954430249, 0.03340798883429287, -0.007658242249530495, -0.16509170933430525, 0.11259323796257377, 0.3084327943181913, -0.2154319725048385, -0.2641931427593686, 0.0492830904096512, -0.26369226697685294, -0.17412962047138103, 0.157419638445993, -0.052985583343788195,... |
709.163 | Comment on ``Can Black Holes be Torn Up by a Phantom in Cyclic
Cosmology?" by X. Zhang. arXiv:0708.1408 [gr-qc] | In a recently archived paper by Zhang\cite{Zhang}, it is claimed that before
turnaround in a cyclic model two unexpected events happen: (1) black holes
cease to contract and begin to expand; (2) separated causal patches start to
reconnect. We show that both conclusions are erroneous and result from the
author's choic... | gr-qc | in a recently archived paper by zhangcitezhang it is claimed that before turnaround in a cyclic model two unexpected events happen 1 black holes cease to contract and begin to expand 2 separated causal patches start to reconnect we show that both conclusions are erroneous and result from the authors choice of variables | [['in', 'a', 'recently', 'archived', 'paper', 'by', 'zhangcitezhang', 'it', 'is', 'claimed', 'that', 'before', 'turnaround', 'in', 'a', 'cyclic', 'model', 'two', 'unexpected', 'events', 'happen', '1', 'black', 'holes', 'cease', 'to', 'contract', 'and', 'begin', 'to', 'expand', '2', 'separated', 'causal', 'patches', 'st... | [-0.12305037720272174, 0.1533798179544437, -0.11717171567635468, 0.12514507474350886, -0.09426189369808596, -0.14957376714580908, 0.12131415957880493, 0.38558013970032334, -0.23212072610532722, -0.33207727826307887, 0.12941655388119847, -0.3006808710499452, -0.14259002191157868, 0.1308428235934116, -0.10328263617478885... |
709.1631 | Size-dependent Surface States on Strained Cobalt Nanoislands on Cu(111) | Low-temperature scanning tunneling spectroscopy over Co nanoislands on
Cu(111) showed that the surface states of the islands vary with their size.
Occupied states exhibit a sizeable downward energy shift as the island size
decreases. The position of the occupied states also significantly changes
across the islands. A... | cond-mat.mtrl-sci cond-mat.str-el | lowtemperature scanning tunneling spectroscopy over co nanoislands on cu111 showed that the surface states of the islands vary with their size occupied states exhibit a sizeable downward energy shift as the island size decreases the position of the occupied states also significantly changes across the islands atomicsca... | [['lowtemperature', 'scanning', 'tunneling', 'spectroscopy', 'over', 'co', 'nanoislands', 'on', 'cu111', 'showed', 'that', 'the', 'surface', 'states', 'of', 'the', 'islands', 'vary', 'with', 'their', 'size', 'occupied', 'states', 'exhibit', 'a', 'sizeable', 'downward', 'energy', 'shift', 'as', 'the', 'island', 'size', ... | [-0.13086324535044178, 0.23758180843267057, -0.058940528566017746, 0.04295904288966475, 0.05774320921461497, -0.09869692441342133, 0.13384662598171937, 0.40602265085492817, -0.2830659520945379, -0.33290937330041614, -0.06273840215622581, -0.3437532016741378, -0.10192882205259853, 0.17760514766975705, 0.0485288554935583... |
709.1632 | Sterile Neutrinos as the Warm Dark Matter in the Type II Seesaw Model | In the framework of type II seesaw mechanism we discuss the number of sterile
right-handed Majorana neutrinos being the warm dark matter (WDM). When the type
II seesaw mass term $M_\nu ^{II}$ is far less than the type I seesaw mass term
$M_\nu ^{I}$, only one of three sterile neutrinos may be the WDM particle. On
the... | hep-ph | in the framework of type ii seesaw mechanism we discuss the number of sterile righthanded majorana neutrinos being the warm dark matter wdm when the type ii seesaw mass term m_nu ii is far less than the type i seesaw mass term m_nu i only one of three sterile neutrinos may be the wdm particle on the contrary the wdm pa... | [['in', 'the', 'framework', 'of', 'type', 'ii', 'seesaw', 'mechanism', 'we', 'discuss', 'the', 'number', 'of', 'sterile', 'righthanded', 'majorana', 'neutrinos', 'being', 'the', 'warm', 'dark', 'matter', 'wdm', 'when', 'the', 'type', 'ii', 'seesaw', 'mass', 'term', 'm_nu', 'ii', 'is', 'far', 'less', 'than', 'the', 'typ... | [-0.11122160497741009, 0.3491412770984295, 0.10374662205244281, 0.22597038046452717, -0.12404216904542409, -0.3254949556264494, 0.03797104558907449, 0.2984138323725866, -0.16866644517618365, -0.2958100740028645, 0.014020562536773338, -0.32842614041042645, 0.022922334922311296, 0.09998855886702326, 0.03755164014208796, ... |
709.1633 | Three-Particle Azimuthal Correlations | Two-particle azimuthal correlations in central Au+Au collisional at RHIC have
revealed a broadened away-side structure, with respect to perpherial Au+Au, pp,
and d+Au. This could be explained by different physics mechanisms such as:
large angle gluon radiation, deflected jets, Cerenkov gluon radiation, and
conical fl... | nucl-ex | twoparticle azimuthal correlations in central auau collisional at rhic have revealed a broadened awayside structure with respect to perpherial auau pp and dau this could be explained by different physics mechanisms such as large angle gluon radiation deflected jets cerenkov gluon radiation and conical flow generated by... | [['twoparticle', 'azimuthal', 'correlations', 'in', 'central', 'auau', 'collisional', 'at', 'rhic', 'have', 'revealed', 'a', 'broadened', 'awayside', 'structure', 'with', 'respect', 'to', 'perpherial', 'auau', 'pp', 'and', 'dau', 'this', 'could', 'be', 'explained', 'by', 'different', 'physics', 'mechanisms', 'such', 'a... | [-0.04094999355794949, 0.26985952267684393, -0.22405314342353808, 0.19995603892651917, -0.03965122472042235, -0.14551873835430384, -0.17854027001831296, 0.42233425436027905, -0.2539084904139566, -0.2546941367980032, -0.05626337897145651, -0.3452546498259512, 0.04830322511250449, 0.1605460793878796, 0.07467928500497871,... |
709.1634 | GaN:$\delta$-Mg grown by MOVPE: structural properties and their effect
on the electronic and optical behaviour | The effect of Mg $\delta$-doping on the structural, electrical and optical
properties of GaN grown $\textsl{via}$ metalorganic vapor phase epitaxy has
been studied using transmission electron microscopy, secondary ion mass
spectroscopy, atomic force microscopy, x-ray diffraction, Hall effect
measurements and photolum... | cond-mat.mtrl-sci | the effect of mg deltadoping on the structural electrical and optical properties of gan grown textslvia metalorganic vapor phase epitaxy has been studied using transmission electron microscopy secondary ion mass spectroscopy atomic force microscopy xray diffraction hall effect measurements and photoluminescence for an ... | [['the', 'effect', 'of', 'mg', 'deltadoping', 'on', 'the', 'structural', 'electrical', 'and', 'optical', 'properties', 'of', 'gan', 'grown', 'textslvia', 'metalorganic', 'vapor', 'phase', 'epitaxy', 'has', 'been', 'studied', 'using', 'transmission', 'electron', 'microscopy', 'secondary', 'ion', 'mass', 'spectroscopy', ... | [-0.09032097494569402, 0.17767228337040292, -0.01660574801008469, -0.006376615765727119, 0.0521126267919024, -0.09778098259911926, 0.08309809085927646, 0.4362341608858005, -0.23075351745194797, -0.34832579439869094, 0.01016375458720228, -0.31690825125987426, -0.09532330676901547, 0.14400258510367675, -0.005310441428830... |
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