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710.3853 | Hopf modules for autonomous pseudomonoids and the monoidal centre | In this work we develop some aspects of the theory of Hopf algebras to the
context of autonomous map pseudomonoids. We concentrate in the Hopf modules and
the Centre or Drinfel'd double. If $A$ is a map pseudomonoid in a monoidal
bicategory \M, the analogue of the category of Hopf modules for $A$ is an
Eilenberg-Moor... | math.CT math.QA | in this work we develop some aspects of the theory of hopf algebras to the context of autonomous map pseudomonoids we concentrate in the hopf modules and the centre or drinfeld double if a is a map pseudomonoid in a monoidal bicategory m the analogue of the category of hopf modules for a is an eilenbergmoore constructi... | [['in', 'this', 'work', 'we', 'develop', 'some', 'aspects', 'of', 'the', 'theory', 'of', 'hopf', 'algebras', 'to', 'the', 'context', 'of', 'autonomous', 'map', 'pseudomonoids', 'we', 'concentrate', 'in', 'the', 'hopf', 'modules', 'and', 'the', 'centre', 'or', 'drinfeld', 'double', 'if', 'a', 'is', 'a', 'map', 'pseudomo... | [-0.16431957094000946, 0.029307539878371043, -0.07357276535670583, 0.0784307313361852, -0.10493772789508242, -0.10928255332961541, 0.0059918035312202175, 0.33824366845483717, -0.3711275893793855, -0.1751050711932799, 0.12771423603084664, -0.20928700960724167, -0.15824907092718166, 0.1796370179185437, -0.152309528961066... |
710.3854 | Models for the Observable System Parameters of Ultraluminous X-ray
Sources | We investigate the evolution of the properties of model populations of
ultraluminous X-ray sources (ULXs) consisting of a black-hole accretor in a
binary with a donor star. We have computed models corresponding to three
different populations of black-hole binaries; two invoke stellar-mass (~10
Msun) black hole accret... | astro-ph | we investigate the evolution of the properties of model populations of ultraluminous xray sources ulxs consisting of a blackhole accretor in a binary with a donor star we have computed models corresponding to three different populations of blackhole binaries two invoke stellarmass 10 msun black hole accretors and the t... | [['we', 'investigate', 'the', 'evolution', 'of', 'the', 'properties', 'of', 'model', 'populations', 'of', 'ultraluminous', 'xray', 'sources', 'ulxs', 'consisting', 'of', 'a', 'blackhole', 'accretor', 'in', 'a', 'binary', 'with', 'a', 'donor', 'star', 'we', 'have', 'computed', 'models', 'corresponding', 'to', 'three', '... | [-0.06979313424613792, 0.07397914363362361, -0.03556451024538546, 0.1903471822850406, -0.06051124985096976, -0.0934116985136643, 0.07021821975242347, 0.4377767095901072, -0.09482674925588071, -0.384609491978772, 0.07992006657121237, -0.3548349537095055, -0.007460612640716136, 0.25079704716801643, -0.06769036033656448, ... |
710.3855 | Extraction of Singlet States from Noninteracting High-Dimensional Spins | We present a scheme for the extraction of singlet states of two remote
particles of arbitrary quantum spin number. The goal is achieved through
post-selection of the state of interaction mediators sent in succession. A
small number of iterations is sufficient to make the scheme effective. We
propose two suitable expe... | quant-ph | we present a scheme for the extraction of singlet states of two remote particles of arbitrary quantum spin number the goal is achieved through postselection of the state of interaction mediators sent in succession a small number of iterations is sufficient to make the scheme effective we propose two suitable experiment... | [['we', 'present', 'a', 'scheme', 'for', 'the', 'extraction', 'of', 'singlet', 'states', 'of', 'two', 'remote', 'particles', 'of', 'arbitrary', 'quantum', 'spin', 'number', 'the', 'goal', 'is', 'achieved', 'through', 'postselection', 'of', 'the', 'state', 'of', 'interaction', 'mediators', 'sent', 'in', 'succession', 'a... | [-0.22422187517654021, 0.21873521408194613, -0.06639094258947618, 0.020286248623521935, -0.015829662896756982, -0.22381748395554465, 0.08064192771140871, 0.36982648183816463, -0.23548617781589515, -0.32737652636293707, 0.040664884661211924, -0.19594102249288098, -0.08018940952927645, 0.18384645396345778, -0.01443563632... |
710.3856 | The Lattice Free Energy of QCD with Clover Fermions, up to Three-Loops | We calculate the perturbative value of the free energy in Lattice QCD, up to
three loops. Our calculation is performed using Wilson gluons and the
Sheikholeslami - Wolhert (clover) improved action for fermions.
The free energy is directly related to the average plaquette. To carry out
the calculation, we compute al... | hep-lat | we calculate the perturbative value of the free energy in lattice qcd up to three loops our calculation is performed using wilson gluons and the sheikholeslami wolhert clover improved action for fermions the free energy is directly related to the average plaquette to carry out the calculation we compute all relevant fe... | [['we', 'calculate', 'the', 'perturbative', 'value', 'of', 'the', 'free', 'energy', 'in', 'lattice', 'qcd', 'up', 'to', 'three', 'loops', 'our', 'calculation', 'is', 'performed', 'using', 'wilson', 'gluons', 'and', 'the', 'sheikholeslami', 'wolhert', 'clover', 'improved', 'action', 'for', 'fermions', 'the', 'free', 'en... | [-0.12134667975813385, 0.20654410778053975, -0.08627840084588434, 0.06541675091519453, -0.05647648068137584, -0.0640667852776961, 0.10867850739127538, 0.3916500687423184, -0.13100579235057427, -0.30613282067686554, 0.08189407139961556, -0.28785071756661407, -0.044253964673757085, 0.19041661683316013, 0.0346000453853231... |
710.3857 | Generalizations of Sch\"{o}bi's Tetrahedral Dissection | Let v_1, ..., v_n be unit vectors in R^n such that v_i . v_j = -w for i != j,
where -1 <w < 1/(n-1). The points Sum_{i=1..n} lambda_i v_i, where 1 >=
lambda_1 >= ... >= lambda_n >= 0, form a ``Hill-simplex of the first type'',
denoted by Q_n(w). It was shown by Hadwiger in 1951 that Q_n(w) is
equidissectable with a c... | math.MG math.CO | let v_1 v_n be unit vectors in rn such that v_i v_j w for i j where 1 w 1n1 the points sum_i1n lambda_i v_i where 1 lambda_1 lambda_n 0 form a hillsimplex of the first type denoted by q_nw it was shown by hadwiger in 1951 that q_nw is equidissectable with a cube in 1985 schobi gave a threepiece dissection of q_3w into ... | [['let', 'v_1', 'v_n', 'be', 'unit', 'vectors', 'in', 'rn', 'such', 'that', 'v_i', 'v_j', 'w', 'for', 'i', 'j', 'where', '1', 'w', '1n1', 'the', 'points', 'sum_i1n', 'lambda_i', 'v_i', 'where', '1', 'lambda_1', 'lambda_n', '0', 'form', 'a', 'hillsimplex', 'of', 'the', 'first', 'type', 'denoted', 'by', 'q_nw', 'it', 'wa... | [-0.1378939547286925, 0.10388088813659051, -0.03911359128448487, -0.05875963036116397, -0.04341887787371974, -0.20358599352708162, 0.004152563984987119, 0.32630982155592847, -0.30393951969930666, -0.19600017973840636, 0.08063883012341923, -0.33552525295319674, -0.10753651449906847, 0.11717971853736862, -0.0967507693922... |
710.3858 | Tamagawa defect of Euler systems | As remarked in [Kolyvagin systems, by Barry Mazur and Karl Rubin] Proposition
6.2.6 and Buyukboduk[ arXiv:0706.0377v1 ] Remark 3.25 one does not expect the
Kolyvagin system obtained from an Euler system for a p-adic Galois
representation T to be primitive (in the sense of [Kolyvagin systems, by Barry
Mazur and Karl R... | math.NT | as remarked in kolyvagin systems by barry mazur and karl rubin proposition 626 and buyukboduk arxiv07060377v1 remark 325 one does not expect the kolyvagin system obtained from an euler system for a padic galois representation t to be primitive in the sense of kolyvagin systems by barry mazur and karl rubin definition 4... | [['as', 'remarked', 'in', 'kolyvagin', 'systems', 'by', 'barry', 'mazur', 'and', 'karl', 'rubin', 'proposition', '626', 'and', 'buyukboduk', 'arxiv07060377v1', 'remark', '325', 'one', 'does', 'not', 'expect', 'the', 'kolyvagin', 'system', 'obtained', 'from', 'an', 'euler', 'system', 'for', 'a', 'padic', 'galois', 'repr... | [-0.19860411697262106, 0.05643894579164529, -0.144990322432706, 0.06989696669830557, -0.0929810164611957, -0.1517905853293057, 0.05906336409651546, 0.16354355341420065, -0.26662802334047025, -0.33693033432454067, 0.03602210948703311, -0.26792182720546287, -0.14000184807372493, 0.22876038714433758, -0.18816757393282613,... |
710.3859 | Endogenous versus Exogenous Origins of Diseases | Many illnesses are associated with an alteration of the immune system
homeostasis due to any combination of factors, including exogenous bacterial
insult, endogenous breakdown (e.g., development of a disease that results in
immuno suppression), or an exogenous hit like surgery that simultaneously
alters immune respon... | physics.bio-ph physics.med-ph q-bio.CB | many illnesses are associated with an alteration of the immune system homeostasis due to any combination of factors including exogenous bacterial insult endogenous breakdown eg development of a disease that results in immuno suppression or an exogenous hit like surgery that simultaneously alters immune responsiveness a... | [['many', 'illnesses', 'are', 'associated', 'with', 'an', 'alteration', 'of', 'the', 'immune', 'system', 'homeostasis', 'due', 'to', 'any', 'combination', 'of', 'factors', 'including', 'exogenous', 'bacterial', 'insult', 'endogenous', 'breakdown', 'eg', 'development', 'of', 'a', 'disease', 'that', 'results', 'in', 'imm... | [-0.12558969274484824, 0.19211621842602364, 0.009999114631376576, 0.041693227592701165, -0.01739482728518011, -0.24170274748529555, 0.09265179210342467, 0.2806355230574968, -0.22232551170009784, -0.23161780069511168, 0.07928708785959006, -0.30802675177278716, -0.2890378825779954, 0.13806019175167075, -0.151343759038640... |
710.386 | Prime and composite Laurent polynomials | In 1922 Ritt constructed the theory of functional decompositions of
polynomials with complex coefficients. In particular, he described explicitly
indecomposable polynomial solutions of the functional equation f(p(z))=g(q(z)).
In this paper we study the equation above in the case when f,g,p,q are
holomorphic functions... | math.CV math.AG | in 1922 ritt constructed the theory of functional decompositions of polynomials with complex coefficients in particular he described explicitly indecomposable polynomial solutions of the functional equation fpzgqz in this paper we study the equation above in the case when fgpq are holomorphic functions on compact riema... | [['in', '1922', 'ritt', 'constructed', 'the', 'theory', 'of', 'functional', 'decompositions', 'of', 'polynomials', 'with', 'complex', 'coefficients', 'in', 'particular', 'he', 'described', 'explicitly', 'indecomposable', 'polynomial', 'solutions', 'of', 'the', 'functional', 'equation', 'fpzgqz', 'in', 'this', 'paper', ... | [-0.13002829248400624, 0.048223783305900936, -0.13068887817618602, 0.09557646332062124, -0.06108426789150519, -0.09091867328457096, -0.011103226679979879, 0.2668496519655866, -0.27603749834028457, -0.21014666293802506, 0.08169551440882702, -0.28902747052557326, -0.22389675231773734, 0.18860086500644685, -0.095559693478... |
710.3861 | Optimal encoding on discrete lattice with translational invariant
constrains using statistical algorithms | In this paper will be presented methodology of encoding information in
valuations of discrete lattice with some translational invariant constrains in
asymptotically optimal way. The method is based on finding statistical
description of such valuations and changing it into statistical algorithm,
which allows to constr... | cs.IT math.IT | in this paper will be presented methodology of encoding information in valuations of discrete lattice with some translational invariant constrains in asymptotically optimal way the method is based on finding statistical description of such valuations and changing it into statistical algorithm which allows to construct ... | [['in', 'this', 'paper', 'will', 'be', 'presented', 'methodology', 'of', 'encoding', 'information', 'in', 'valuations', 'of', 'discrete', 'lattice', 'with', 'some', 'translational', 'invariant', 'constrains', 'in', 'asymptotically', 'optimal', 'way', 'the', 'method', 'is', 'based', 'on', 'finding', 'statistical', 'desc... | [-0.05353254100234846, 0.08863924753699284, -0.15227676154489614, 0.09707627697663604, -0.09075881870213284, -0.2115342179313302, 0.08165790837470081, 0.41396935292477927, -0.3061430056739265, -0.2970898915933612, 0.11870958102578576, -0.2303696218931243, -0.14581608167960683, 0.21283032045935962, -0.11285882083518403,... |
710.3862 | Large-scale instability in a sheared nonhelical turbulence: formation of
vortical structures | We study a large-scale instability in a sheared nonhelical turbulence that
causes generation of large-scale vorticity. Three types of the background
large-scale flows are considered, i.e., the Couette and Poiseuille flows in a
small-scale homogeneous turbulence, and the "log-linear" velocity shear in an
inhomogeneous... | physics.flu-dyn astro-ph physics.geo-ph | we study a largescale instability in a sheared nonhelical turbulence that causes generation of largescale vorticity three types of the background largescale flows are considered ie the couette and poiseuille flows in a smallscale homogeneous turbulence and the loglinear velocity shear in an inhomogeneous turbulence it ... | [['we', 'study', 'a', 'largescale', 'instability', 'in', 'a', 'sheared', 'nonhelical', 'turbulence', 'that', 'causes', 'generation', 'of', 'largescale', 'vorticity', 'three', 'types', 'of', 'the', 'background', 'largescale', 'flows', 'are', 'considered', 'ie', 'the', 'couette', 'and', 'poiseuille', 'flows', 'in', 'a', ... | [-0.2865597994586084, 0.2567313394841469, -0.0624508718221796, 0.06743930697962557, -0.04631461348912511, -0.017405168539608405, -0.13329574515965814, 0.28253508419869255, -0.3155828753597863, -0.22500032070548862, 0.09593713925915345, -0.2015898767614647, -0.11869252285456568, 0.22265171051918087, 0.023891867332113265... |
710.3863 | Analysis of the convex hull of the attractor of an IFS | In this paper we will introduce the methodology of analysis of the convex
hull of the attractors of iterated functional systems (IFS) - compact fixed
sets of self-similarity mapping. The method is based on a function which for a
direction, gives width in that direction. We can write the self similarity
equation in te... | math.CA | in this paper we will introduce the methodology of analysis of the convex hull of the attractors of iterated functional systems ifs compact fixed sets of selfsimilarity mapping the method is based on a function which for a direction gives width in that direction we can write the self similarity equation in terms of thi... | [['in', 'this', 'paper', 'we', 'will', 'introduce', 'the', 'methodology', 'of', 'analysis', 'of', 'the', 'convex', 'hull', 'of', 'the', 'attractors', 'of', 'iterated', 'functional', 'systems', 'ifs', 'compact', 'fixed', 'sets', 'of', 'selfsimilarity', 'mapping', 'the', 'method', 'is', 'based', 'on', 'a', 'function', 'w... | [-0.14123130626118693, 0.04977836873578398, -0.13408937127280393, 0.059576974803042644, -0.05429711785216473, -0.09159829111916847, 0.06121096486642368, 0.35646070906965943, -0.32501440567797735, -0.23592887754601083, 0.09780780123669262, -0.27539022520160006, -0.17128271397056155, 0.18305698025138362, -0.0613154578365... |
710.3864 | Criteria for the density property of complex manifolds | In this paper we suggest new effective criteria for the density property.
This enables us to give a trivial proof of the original Anders\'en-Lempert
result and to establish (almost free of charge) the algebraic density property
for all linear algebraic groups whose connected components are different from
tori or $\C_... | math.CV | in this paper we suggest new effective criteria for the density property this enables us to give a trivial proof of the original andersenlempert result and to establish almost free of charge the algebraic density property for all linear algebraic groups whose connected components are different from tori or c_ as anothe... | [['in', 'this', 'paper', 'we', 'suggest', 'new', 'effective', 'criteria', 'for', 'the', 'density', 'property', 'this', 'enables', 'us', 'to', 'give', 'a', 'trivial', 'proof', 'of', 'the', 'original', 'andersenlempert', 'result', 'and', 'to', 'establish', 'almost', 'free', 'of', 'charge', 'the', 'algebraic', 'density', ... | [-0.16383859658295788, 0.08267565678078227, -0.10231947667737741, 0.07082299559473673, -0.10522427039061923, -0.12955563120180513, 0.060126712497482755, 0.3043437859543213, -0.2863065680239077, -0.25446373206086276, 0.0857831131675417, -0.23420273366088912, -0.14508686952077124, 0.19024549825287357, -0.1093419481000704... |
710.3865 | Inhomogeneous exclusion processes with extended objects: The effect of
defect locations | We study the effects of local inhomogeneities, i.e., slow sites of hopping
rate $q<1$, in a totally asymmetric simple exclusion process (TASEP) for
particles of size $\ell \geq 1$ (in units of the lattice spacing). We compare
the simulation results of $\ell =1$ and $\ell >1$ and notice that the existence
of local def... | cond-mat.stat-mech | we study the effects of local inhomogeneities ie slow sites of hopping rate q1 in a totally asymmetric simple exclusion process tasep for particles of size ell geq 1 in units of the lattice spacing we compare the simulation results of ell 1 and ell 1 and notice that the existence of local defects has qualitatively simi... | [['we', 'study', 'the', 'effects', 'of', 'local', 'inhomogeneities', 'ie', 'slow', 'sites', 'of', 'hopping', 'rate', 'q1', 'in', 'a', 'totally', 'asymmetric', 'simple', 'exclusion', 'process', 'tasep', 'for', 'particles', 'of', 'size', 'ell', 'geq', '1', 'in', 'units', 'of', 'the', 'lattice', 'spacing', 'we', 'compare'... | [-0.1469691953659224, 0.17208868582045916, -0.045098920934833586, 0.09131376260662753, 0.02141310361080936, -0.14975844197241323, 0.06033803963232674, 0.3571493254054249, -0.2632947693928145, -0.251193608622998, 0.0795261986391519, -0.3035911823667231, -0.13450375491464955, 0.16618473779886872, 0.009881415234607024, -0... |
710.3866 | Constraints on the Velocity and Spatial Distribution of Helium-like Ions
in the Wind of SMC X-1 from Observations with XMM-Newton/RGS | We present here X-ray spectra of the HMXB SMC X-1 obtained in an observation
with the XMM observatory beginning before eclipse and ending near the end of
eclipse. With the Reflection Grating Spectrometers (RGS) on board XMM, we
observe emission lines from hydrogen-like and helium-like ions of nitrogen,
oxygen, neon, ... | astro-ph | we present here xray spectra of the hmxb smc x1 obtained in an observation with the xmm observatory beginning before eclipse and ending near the end of eclipse with the reflection grating spectrometers rgs on board xmm we observe emission lines from hydrogenlike and heliumlike ions of nitrogen oxygen neon magnesium and... | [['we', 'present', 'here', 'xray', 'spectra', 'of', 'the', 'hmxb', 'smc', 'x1', 'obtained', 'in', 'an', 'observation', 'with', 'the', 'xmm', 'observatory', 'beginning', 'before', 'eclipse', 'and', 'ending', 'near', 'the', 'end', 'of', 'eclipse', 'with', 'the', 'reflection', 'grating', 'spectrometers', 'rgs', 'on', 'boa... | [-0.07927257400006056, 0.14196690412825272, -0.0024308892323615704, 0.03273193721778374, -0.015393278522892519, -0.11059047139665865, 0.08819221184270684, 0.431710250449783, -0.18738755638552632, -0.3164932420358379, 0.05113695924309023, -0.35719127420018965, 0.05169936698821789, 0.17094161515619527, -0.001673589353548... |
710.3867 | Tidal debris from high-velocity collisions as fake dark galaxies: A
numerical model of VirgoHI21 | High speed collisions, although current in clusters of galaxies, have long
been neglected, as they are believed to cause little damages to galaxies,
except when they are repeated, a process called harassment. In fact, they are
able to produce faint but extended gaseous tails. Such low-mass, starless,
tidal debris may... | astro-ph | high speed collisions although current in clusters of galaxies have long been neglected as they are believed to cause little damages to galaxies except when they are repeated a process called harassment in fact they are able to produce faint but extended gaseous tails such lowmass starless tidal debris may become detac... | [['high', 'speed', 'collisions', 'although', 'current', 'in', 'clusters', 'of', 'galaxies', 'have', 'long', 'been', 'neglected', 'as', 'they', 'are', 'believed', 'to', 'cause', 'little', 'damages', 'to', 'galaxies', 'except', 'when', 'they', 'are', 'repeated', 'a', 'process', 'called', 'harassment', 'in', 'fact', 'they... | [-0.09636864496554297, 0.11126306424043457, -0.130841706394519, 0.14145296162957965, -0.1332504576627039, -0.07029946229798734, -0.011399046266258912, 0.41544724566707936, -0.17608364163967954, -0.3362414046659842, 0.058254773651960454, -0.2677856384552455, -0.06304879151574092, 0.18452103195241057, -0.0435108107854297... |
710.3868 | Formation, Survival, and Destruction of Vortices in Accretion Disks | Two dimensional hydrodynamical disks are nonlinearly unstable to the
formation of vortices. Once formed, these vortices essentially survive forever.
What happens in three dimensions? We show with pseudospectral simulations that
in 3D a vortex in a short box forms and survives just as in 2D. But a vortex in
a tall box... | astro-ph | two dimensional hydrodynamical disks are nonlinearly unstable to the formation of vortices once formed these vortices essentially survive forever what happens in three dimensions we show with pseudospectral simulations that in 3d a vortex in a short box forms and survives just as in 2d but a vortex in a tall box is uns... | [['two', 'dimensional', 'hydrodynamical', 'disks', 'are', 'nonlinearly', 'unstable', 'to', 'the', 'formation', 'of', 'vortices', 'once', 'formed', 'these', 'vortices', 'essentially', 'survive', 'forever', 'what', 'happens', 'in', 'three', 'dimensions', 'we', 'show', 'with', 'pseudospectral', 'simulations', 'that', 'in'... | [-0.16646360158613457, 0.22348142692155037, -0.07416027392506196, 0.10387450439292331, -0.05986727321206397, -0.11545569340377151, -0.031046350521771886, 0.34980709718309283, -0.24794170712728852, -0.25029662320328977, 0.0834904293138931, -0.23482211930821686, -0.06105634676068732, 0.1818593817315418, 0.001868290748109... |
710.3869 | Khasminskii--Whitham averaging for randomly perturbed KdV equation | We consider the damped-driven KdV equation $$ \dot
u-\nu{u_{xx}}+u_{xxx}-6uu_x=\sqrt\nu \eta(t,x), x\in S^1, \int u dx\equiv
\int\eta dx\equiv0, $$ where $0<\nu\le1$ and the random process $\eta$ is
smooth in $x$ and white in $t$. For any periodic function $u(x)$ let $
I=(I_1,I_2,...) $ be the vector, formed by the K... | math.AP math-ph math.MP | we consider the dampeddriven kdv equation dot unuu_xxu_xxx6uu_xsqrtnu etatx xin s1 int u dxequiv inteta dxequiv0 where 0nule1 and the random process eta is smooth in x and white in t for any periodic function ux let ii_1i_2 be the vector formed by the kdv integrals of motion calculated for the potential ux we prove tha... | [['we', 'consider', 'the', 'dampeddriven', 'kdv', 'equation', 'dot', 'unuu_xxu_xxx6uu_xsqrtnu', 'etatx', 'xin', 's1', 'int', 'u', 'dxequiv', 'inteta', 'dxequiv0', 'where', '0nule1', 'and', 'the', 'random', 'process', 'eta', 'is', 'smooth', 'in', 'x', 'and', 'white', 'in', 't', 'for', 'any', 'periodic', 'function', 'ux'... | [-0.19798903647338, 0.10626967227689817, -0.03774411525433018, 0.02649337994554232, -0.038289183094887665, -0.17688886803561743, -0.019673314191479708, 0.30444917566484025, -0.3415822480398584, -0.11137235903797645, 0.07634483989734779, -0.3661655361278796, -0.1218893152569801, 0.16352753598295466, -0.03638720393679302... |
710.387 | The WKB method for conjugate points in the volumorphism group | In this paper, we are interested in the location of conjugate points along a
geodesic in the volumorphism group of a compact three-dimensional manifold
without boundary (the configuration space of an ideal fluid). As shown in the
author's previous work, these are typically pathological, i.e., they can occur
in cluste... | math.AP math.DG | in this paper we are interested in the location of conjugate points along a geodesic in the volumorphism group of a compact threedimensional manifold without boundary the configuration space of an ideal fluid as shown in the authors previous work these are typically pathological ie they can occur in clusters along a ge... | [['in', 'this', 'paper', 'we', 'are', 'interested', 'in', 'the', 'location', 'of', 'conjugate', 'points', 'along', 'a', 'geodesic', 'in', 'the', 'volumorphism', 'group', 'of', 'a', 'compact', 'threedimensional', 'manifold', 'without', 'boundary', 'the', 'configuration', 'space', 'of', 'an', 'ideal', 'fluid', 'as', 'sho... | [-0.1933155805565266, 0.10743472563995632, -0.08349390348262141, 0.072358064702712, -0.09639601692603245, -0.09500309271724816, 0.01646823081446969, 0.40540111067534335, -0.254944285732025, -0.23101492798034573, 0.12258303677007346, -0.2605760629833217, -0.15703807753169727, 0.21992817020345426, -0.12528012986016185, 0... |
710.3871 | Algebraic Geometry over Free Metabelian Lie Algebra I: U-Algebras and
Universal Classes | This paper is the first in a series of three, the aim of which is to lay the
foundations of algebraic geometry over the free metabelian Lie algebra $F$. In
the current paper we introduce the notion of a metabelian Lie $U$-algebra and
establish connections between metabelian Lie $U$-algebras and special matrix
Lie alg... | math.AG math.LO | this paper is the first in a series of three the aim of which is to lay the foundations of algebraic geometry over the free metabelian lie algebra f in the current paper we introduce the notion of a metabelian lie ualgebra and establish connections between metabelian lie ualgebras and special matrix lie algebras we def... | [['this', 'paper', 'is', 'the', 'first', 'in', 'a', 'series', 'of', 'three', 'the', 'aim', 'of', 'which', 'is', 'to', 'lay', 'the', 'foundations', 'of', 'algebraic', 'geometry', 'over', 'the', 'free', 'metabelian', 'lie', 'algebra', 'f', 'in', 'the', 'current', 'paper', 'we', 'introduce', 'the', 'notion', 'of', 'a', 'm... | [-0.1926019181661746, 0.037158253997126044, -0.0817055483786937, 0.03847803862025852, -0.1449468671618139, -0.09390200816971414, 0.017576835745507304, 0.3623338727828334, -0.36781004101914516, -0.19807801439481623, 0.12188146708341425, -0.1805311526034904, -0.1774393458467196, 0.18474325790782184, -0.11262428771211382,... |
710.3872 | Algebraic Geometry over Free Metabelian Lie Algebra II: Finite Field
Case | This paper is the second in a series of three, the aim of which is to
construct algebraic geometry over a free metabelian Lie algebra $F$. For the
universal closure of free metabelian Lie algebra of finite rank $r \ge 2$ over
a finite field $k$ we find a convenient set of axioms in the language of Lie
algebras $L$ an... | math.AG math.LO | this paper is the second in a series of three the aim of which is to construct algebraic geometry over a free metabelian lie algebra f for the universal closure of free metabelian lie algebra of finite rank r ge 2 over a finite field k we find a convenient set of axioms in the language of lie algebras l and the languag... | [['this', 'paper', 'is', 'the', 'second', 'in', 'a', 'series', 'of', 'three', 'the', 'aim', 'of', 'which', 'is', 'to', 'construct', 'algebraic', 'geometry', 'over', 'a', 'free', 'metabelian', 'lie', 'algebra', 'f', 'for', 'the', 'universal', 'closure', 'of', 'free', 'metabelian', 'lie', 'algebra', 'of', 'finite', 'rank... | [-0.19168727224197, 0.0985889605231463, -0.08288210939480772, 0.04746693119804765, -0.11997964940289216, -0.11112143223609534, -0.006547453899627491, 0.3558741056044856, -0.38530251807758525, -0.18681705621777162, 0.07123440424085505, -0.19799205222197117, -0.08895242001181619, 0.22900393733664626, -0.08141990292877439... |
710.3873 | Semidomains and Metabelian Product of Metabelian Lie Algebras | This paper is the third in a series of papers, the aim of which is to
construct algebraic geometry over metabelian Lie algebras.
| math.AG math.LO | this paper is the third in a series of papers the aim of which is to construct algebraic geometry over metabelian lie algebras | [['this', 'paper', 'is', 'the', 'third', 'in', 'a', 'series', 'of', 'papers', 'the', 'aim', 'of', 'which', 'is', 'to', 'construct', 'algebraic', 'geometry', 'over', 'metabelian', 'lie', 'algebras']] | [-0.1773059072944781, -0.0038761767842199492, -0.11158031581536583, 0.010908679414095113, -0.17559166600846726, -0.05821757891174892, -0.04334886667176919, 0.3252088659159515, -0.346381070173305, -0.23063689356912737, 0.1405690687495972, -0.22464043080158855, -0.17026259993081508, 0.195344770975087, -0.1966834526266092... |
710.3874 | Equilibrium sequences of non rotating and rapidly rotating crystalline
color superconducting hybrid stars | The three-flavor crystalline color-superconducting (CCS) phase of quantum
chromodynamics (QCD) is a candidate phase for the ground state of cold matter
at moderate densities above the density of the deconfinement phase transition.
Apart from being a superfluid, the CCS phase has properties of a solid, such as
a latti... | astro-ph cond-mat.supr-con hep-ph nucl-th | the threeflavor crystalline colorsuperconducting ccs phase of quantum chromodynamics qcd is a candidate phase for the ground state of cold matter at moderate densities above the density of the deconfinement phase transition apart from being a superfluid the ccs phase has properties of a solid such as a lattice structur... | [['the', 'threeflavor', 'crystalline', 'colorsuperconducting', 'ccs', 'phase', 'of', 'quantum', 'chromodynamics', 'qcd', 'is', 'a', 'candidate', 'phase', 'for', 'the', 'ground', 'state', 'of', 'cold', 'matter', 'at', 'moderate', 'densities', 'above', 'the', 'density', 'of', 'the', 'deconfinement', 'phase', 'transition'... | [-0.12639318566154772, 0.24279603380810832, -0.11446207760505982, 0.05288432198650044, -0.03005408204626292, -0.06501487489692187, 0.07514021370291442, 0.3165041909276231, -0.20460643386127436, -0.29184852840865516, 0.07694389560859785, -0.2572134587901166, -0.01344732370391186, 0.11097196677829735, 0.04468368343588883... |
710.3875 | Dielectric loss of 2D metal-insulator composite near the percolation
threshold | The frequency dependence of the dielectric loss angle for a metal-insulator
composite was shown previously to be an efficient method to experimentally
determine the percolation threshold. The statistical properties of this angle
are found here to be similar to those of the critical links (supporting the
total current... | cond-mat.mtrl-sci | the frequency dependence of the dielectric loss angle for a metalinsulator composite was shown previously to be an efficient method to experimentally determine the percolation threshold the statistical properties of this angle are found here to be similar to those of the critical links supporting the total current near... | [['the', 'frequency', 'dependence', 'of', 'the', 'dielectric', 'loss', 'angle', 'for', 'a', 'metalinsulator', 'composite', 'was', 'shown', 'previously', 'to', 'be', 'an', 'efficient', 'method', 'to', 'experimentally', 'determine', 'the', 'percolation', 'threshold', 'the', 'statistical', 'properties', 'of', 'this', 'ang... | [-0.14369154157166739, 0.13273635799942868, -0.06869098142657465, 0.03846251597239193, -0.09173331735203567, -0.10516064631463327, 0.11975453266855872, 0.40153694253197864, -0.2675579814602015, -0.31307893797972247, 0.07394381641812658, -0.27131409212512875, -0.15359537968258327, 0.1951876109606107, -0.0270407803275269... |
710.3876 | Acoustic Kappa-Density Fluctuation Waves in Suprathermal Kappa Function
Fluids | We describe a new wave mode similar to the acoustic wave in which both
density and velocity fluctuate. Unlike the acoustic wave in which the
underlying distribution is Maxwellian, this new wave mode occurs when the
underlying distribution is a suprathermal kappa function and involves
fluctuations in the power law ind... | astro-ph | we describe a new wave mode similar to the acoustic wave in which both density and velocity fluctuate unlike the acoustic wave in which the underlying distribution is maxwellian this new wave mode occurs when the underlying distribution is a suprathermal kappa function and involves fluctuations in the power law index k... | [['we', 'describe', 'a', 'new', 'wave', 'mode', 'similar', 'to', 'the', 'acoustic', 'wave', 'in', 'which', 'both', 'density', 'and', 'velocity', 'fluctuate', 'unlike', 'the', 'acoustic', 'wave', 'in', 'which', 'the', 'underlying', 'distribution', 'is', 'maxwellian', 'this', 'new', 'wave', 'mode', 'occurs', 'when', 'the... | [-0.15279917954754682, 0.24133770946965893, -0.09508257584623349, 0.09146227435795246, -0.11663391181831191, -0.08242626891781886, -0.014277624081314347, 0.3119393264023978, -0.26270205261657176, -0.18310988922660917, 0.04463449425788389, -0.3165958927553377, -0.1021807522593457, 0.17916539260818634, 0.0694479970433921... |
710.3877 | Quasirandom groups | Babai and S\'os have asked whether there exists a constant c>0 such that
every finite group G has a product-free subset of size at least c|G|: that is,
a subset X that does not contain three elements x, y and z with xy=z. In this
paper we show that the answer is no. Moreover, we give a simple sufficient
condition for... | math.CO math.GR | babai and sos have asked whether there exists a constant c0 such that every finite group g has a productfree subset of size at least cg that is a subset x that does not contain three elements x y and z with xyz in this paper we show that the answer is no moreover we give a simple sufficient condition for a group not to... | [['babai', 'and', 'sos', 'have', 'asked', 'whether', 'there', 'exists', 'a', 'constant', 'c0', 'such', 'that', 'every', 'finite', 'group', 'g', 'has', 'a', 'productfree', 'subset', 'of', 'size', 'at', 'least', 'cg', 'that', 'is', 'a', 'subset', 'x', 'that', 'does', 'not', 'contain', 'three', 'elements', 'x', 'y', 'and'... | [-0.1847888221698148, 0.11104541538017136, -0.08976545784223293, 0.00021070447650605015, -0.09514095204483186, -0.20044837965896087, 0.08793933337853689, 0.4359067399320858, -0.23402206309671914, -0.2175022503361106, 0.11653353432692322, -0.2984117003423827, -0.11593342505927597, 0.14020827022780266, -0.095543801684730... |
710.3878 | Fundamental Solutions for Wave Equation in de Sitter Model of Universe | In this article we construct the fundamental solutions for the wave equation
arising in the de Sitter model of the universe. We use the fundamental
solutions to represent solutions of the Cauchy problem and to prove the
$L^p-L^q$-decay estimates for the solutions of the equation with and without a
source term.
| math.AP math-ph math.MP | in this article we construct the fundamental solutions for the wave equation arising in the de sitter model of the universe we use the fundamental solutions to represent solutions of the cauchy problem and to prove the lplqdecay estimates for the solutions of the equation with and without a source term | [['in', 'this', 'article', 'we', 'construct', 'the', 'fundamental', 'solutions', 'for', 'the', 'wave', 'equation', 'arising', 'in', 'the', 'de', 'sitter', 'model', 'of', 'the', 'universe', 'we', 'use', 'the', 'fundamental', 'solutions', 'to', 'represent', 'solutions', 'of', 'the', 'cauchy', 'problem', 'and', 'to', 'pro... | [-0.12840981205925345, -0.004565748013556003, -0.10215375533793121, 0.08523678480414673, -0.08545656327158213, -0.04985133587382734, -0.013181722983717918, 0.22627069361507893, -0.29473083801567557, -0.26060226883739235, 0.1634793608589098, -0.3181401100195944, -0.13684790585190057, 0.17734312202315777, -0.024602895695... |
710.3879 | On Penrose's `before the big bang' ideas | We point out that algebraically special Einstein fields with twisting rays
exhibit the basic properties of conformal Universes considered recently by
Roger Penrose.
| gr-qc math.DG | we point out that algebraically special einstein fields with twisting rays exhibit the basic properties of conformal universes considered recently by roger penrose | [['we', 'point', 'out', 'that', 'algebraically', 'special', 'einstein', 'fields', 'with', 'twisting', 'rays', 'exhibit', 'the', 'basic', 'properties', 'of', 'conformal', 'universes', 'considered', 'recently', 'by', 'roger', 'penrose']] | [-0.18311278214273247, 0.1620495765996368, -0.10043601238209268, 0.13487741986856513, -0.1550206143570983, -0.17823999520877135, -0.07791676842000174, 0.3516744383327339, -0.20850235758268315, -0.17593526548665503, 0.03132834731925117, -0.2217144744531454, -0.17864978621187416, 0.20434851620508276, -0.00483726807262586... |
710.388 | Galileo satellite constellation and extensions to General Relativity | We consider the impact of some known extensions of General Relativity in
observables that will be available with the Galileo positioning systems, and
draw conclusions as to the possibility of measuring them. We specifically
address the effects of the presence of a cosmological constant, a Yukawa-like
addition to the ... | gr-qc | we consider the impact of some known extensions of general relativity in observables that will be available with the galileo positioning systems and draw conclusions as to the possibility of measuring them we specifically address the effects of the presence of a cosmological constant a yukawalike addition to the newton... | [['we', 'consider', 'the', 'impact', 'of', 'some', 'known', 'extensions', 'of', 'general', 'relativity', 'in', 'observables', 'that', 'will', 'be', 'available', 'with', 'the', 'galileo', 'positioning', 'systems', 'and', 'draw', 'conclusions', 'as', 'to', 'the', 'possibility', 'of', 'measuring', 'them', 'we', 'specifica... | [-0.15169574177743475, 0.10072157689370934, -0.07818417894987413, 0.08013088068706387, -0.11399685791521161, -0.1423549056340607, 0.015325780383046762, 0.30774612238998583, -0.25518942402422795, -0.3105172504107525, 0.07434699548851055, -0.24414048256513513, -0.13538091582602557, 0.16538773585731784, -0.038841698922354... |
710.3881 | The relation between the quantum games, communication complexity
problems and Bell inequalities | We study the relation between the quantum games, communication complexity
problems and Bell inequalities. In particular we are interested in answering
the question whether for every element of one of these groups there is a
corresponding element in the other two. We show that there are cases where
there is no such re... | quant-ph | we study the relation between the quantum games communication complexity problems and bell inequalities in particular we are interested in answering the question whether for every element of one of these groups there is a corresponding element in the other two we show that there are cases where there is no such relatio... | [['we', 'study', 'the', 'relation', 'between', 'the', 'quantum', 'games', 'communication', 'complexity', 'problems', 'and', 'bell', 'inequalities', 'in', 'particular', 'we', 'are', 'interested', 'in', 'answering', 'the', 'question', 'whether', 'for', 'every', 'element', 'of', 'one', 'of', 'these', 'groups', 'there', 'i... | [-0.146140161724879, 0.10695371197837204, -0.04691962136215047, 0.11435329924113577, -0.002546824833165996, -0.18772692381274664, 0.04559159811138164, 0.38779591448322126, -0.2823364504167583, -0.26409358342614353, 0.10912254638527814, -0.3097929378995035, -0.176287664486614, 0.26911744442355784, -0.08731531180276335, ... |
710.3882 | Special types of intuitionistic fuzzy left h-ideals of hemirings | Characteristic, normal and completely normal intuitionistic fuzzy left
$h$-ideals of hemirings are described.
| math.RA | characteristic normal and completely normal intuitionistic fuzzy left hideals of hemirings are described | [['characteristic', 'normal', 'and', 'completely', 'normal', 'intuitionistic', 'fuzzy', 'left', 'hideals', 'of', 'hemirings', 'are', 'described']] | [-0.09135754549732575, 0.1716667044048126, -0.020737901473274596, 0.16781873542528886, -0.11736658559395717, -0.26510257388536745, -0.04972008271859242, 0.35386870686824506, -0.4405876942552053, -0.03410921303125528, 0.1103292187774339, -0.33229319693950504, -0.05998116932236231, 0.0866408055791488, -0.2001122002704785... |
710.3883 | Axion Inflation in Type II String Theory | Inflationary models driven by a large number of axion fields are discussed in
the context of type IIB compactifications with N=1 supersymmetry. The inflatons
arise as the scalar modes of the R-R two-forms evaluated on vanishing
two-cycles in the compact geometry. The vanishing cycles are resolved by small
two-volumes... | hep-th astro-ph hep-ph | inflationary models driven by a large number of axion fields are discussed in the context of type iib compactifications with n1 supersymmetry the inflatons arise as the scalar modes of the rr twoforms evaluated on vanishing twocycles in the compact geometry the vanishing cycles are resolved by small twovolumes or nsns ... | [['inflationary', 'models', 'driven', 'by', 'a', 'large', 'number', 'of', 'axion', 'fields', 'are', 'discussed', 'in', 'the', 'context', 'of', 'type', 'iib', 'compactifications', 'with', 'n1', 'supersymmetry', 'the', 'inflatons', 'arise', 'as', 'the', 'scalar', 'modes', 'of', 'the', 'rr', 'twoforms', 'evaluated', 'on',... | [-0.20343453627058558, 0.27771876460883504, -0.0196453856597972, 0.1530768235785548, -0.08577961778395217, -0.15537420433908913, -0.014326984890927137, 0.2802490424417721, -0.17872394988609647, -0.3088376823976763, 0.09915579136445145, -0.24590114399854263, -0.087570354686415, 0.1462016951465392, -0.05496852012054825, ... |
710.3884 | Fuzzy n-ary groups as a generalization of Rosenfeld's fuzzy groups | The notion of an $n$-ary group is a natural generalization of the notion of a
group and has many applications in different branches. In this paper, the
notion of (normal) fuzzy $n$-ary subgroup of an $n$-ary group is introduced and
some related properties are investigated. Characterizations of fuzzy $n$-ary
subgroups... | math.RA | the notion of an nary group is a natural generalization of the notion of a group and has many applications in different branches in this paper the notion of normal fuzzy nary subgroup of an nary group is introduced and some related properties are investigated characterizations of fuzzy nary subgroups are given | [['the', 'notion', 'of', 'an', 'nary', 'group', 'is', 'a', 'natural', 'generalization', 'of', 'the', 'notion', 'of', 'a', 'group', 'and', 'has', 'many', 'applications', 'in', 'different', 'branches', 'in', 'this', 'paper', 'the', 'notion', 'of', 'normal', 'fuzzy', 'nary', 'subgroup', 'of', 'an', 'nary', 'group', 'is', ... | [-0.18381805902418608, 0.11733569047702566, -0.06978496393332115, 0.060731766058149964, -0.14885431821816242, -0.048740966514182776, 0.007721906288329942, 0.3814756621678288, -0.356064617060698, -0.22865065584818905, 0.10850325511105788, -0.2827340681822254, -0.19814014732121274, 0.20407470881652373, -0.244398209946946... |
710.3885 | Differentiating dark energy and modified gravity with galaxy redshift
surveys | The observed cosmic acceleration today could be due to an unknown energy
component (dark energy), or a modification to general relativity (modified
gravity). If dark energy models and modified gravity models are required to
predict the same cosmic expansion history H(z), they will predict different
growth rate for co... | astro-ph gr-qc hep-ph | the observed cosmic acceleration today could be due to an unknown energy component dark energy or a modification to general relativity modified gravity if dark energy models and modified gravity models are required to predict the same cosmic expansion history hz they will predict different growth rate for cosmic large ... | [['the', 'observed', 'cosmic', 'acceleration', 'today', 'could', 'be', 'due', 'to', 'an', 'unknown', 'energy', 'component', 'dark', 'energy', 'or', 'a', 'modification', 'to', 'general', 'relativity', 'modified', 'gravity', 'if', 'dark', 'energy', 'models', 'and', 'modified', 'gravity', 'models', 'are', 'required', 'to'... | [-0.07467324427085004, 0.10435872795449044, -0.10304700219883442, 0.12218598745130965, -0.12661776302478575, -0.09113904297509921, 0.02643824248562646, 0.33399050293930177, -0.2225404039860404, -0.38242428793272903, 0.04900755621110539, -0.27682960983468874, -0.015758757227756826, 0.21985809501892856, -0.00578449443291... |
710.3886 | alpha'^2-corrections to extremal dyonic black holes in heterotic string
theory | We calculate alpha'^2-corrections to the entropy of the 5-dimensional
3-charge and the 4-dimensional 4-charge large extremal black holes using the
low energy effective action of the heterotic string theory. In the
4-dimensional case, our results are in agreement with the microscopic
statistical entropy both for the B... | hep-th | we calculate alpha2corrections to the entropy of the 5dimensional 3charge and the 4dimensional 4charge large extremal black holes using the low energy effective action of the heterotic string theory in the 4dimensional case our results are in agreement with the microscopic statistical entropy both for the bps and the n... | [['we', 'calculate', 'alpha2corrections', 'to', 'the', 'entropy', 'of', 'the', '5dimensional', '3charge', 'and', 'the', '4dimensional', '4charge', 'large', 'extremal', 'black', 'holes', 'using', 'the', 'low', 'energy', 'effective', 'action', 'of', 'the', 'heterotic', 'string', 'theory', 'in', 'the', '4dimensional', 'ca... | [-0.1119252590453942, 0.09439357649190007, -0.0494374965455521, 0.1487963829508603, -0.04606660224186877, -0.1227953189259602, 0.011894905073050823, 0.26355974701819596, -0.11191281962587878, -0.2862586494397234, 0.0806426717710026, -0.32380172074944885, -0.1640086938523584, 0.20787864818272214, -0.07994017130522817, 0... |
710.3887 | Ultra LI-ideals in lattice implication algebras and MTL-algebras | A mistake concerning the ultra \textit{LI}-ideal of a lattice implication
algebra is pointed out, and some new sufficient and necessary conditions for an
\textit{LI}-ideal to be an ultra \textit{LI}-ideal are given. Moreover, the
notion of an \textit{LI}-ideal is extended to MTL-algebras, the notions of a
(prime, ult... | math.LO math.GM | a mistake concerning the ultra textitliideal of a lattice implication algebra is pointed out and some new sufficient and necessary conditions for an textitliideal to be an ultra textitliideal are given moreover the notion of an textitliideal is extended to mtlalgebras the notions of a prime ultra obstinate boolean text... | [['a', 'mistake', 'concerning', 'the', 'ultra', 'textitliideal', 'of', 'a', 'lattice', 'implication', 'algebra', 'is', 'pointed', 'out', 'and', 'some', 'new', 'sufficient', 'and', 'necessary', 'conditions', 'for', 'an', 'textitliideal', 'to', 'be', 'an', 'ultra', 'textitliideal', 'are', 'given', 'moreover', 'the', 'not... | [-0.16154454622174735, 0.11828754073133535, -0.09630565252155066, 0.10856312215986216, -0.07359866895864758, -0.12693204923593643, 0.003682607574813554, 0.4081991870239701, -0.26066835272206884, -0.22799431834795067, 0.14094140732777305, -0.21086638914826122, -0.08418605006907297, 0.21003162003699286, -0.16043388282718... |
710.3888 | Cooperative Multi-Cell Networks: Impact of Limited-Capacity Backhaul and
Inter-Users Links | Cooperative technology is expected to have a great impact on the performance
of cellular or, more generally, infrastructure networks. Both multicell
processing (cooperation among base stations) and relaying (cooperation at the
user level) are currently being investigated. In this presentation, recent
results regardin... | cs.IT math.IT | cooperative technology is expected to have a great impact on the performance of cellular or more generally infrastructure networks both multicell processing cooperation among base stations and relaying cooperation at the user level are currently being investigated in this presentation recent results regarding the perfo... | [['cooperative', 'technology', 'is', 'expected', 'to', 'have', 'a', 'great', 'impact', 'on', 'the', 'performance', 'of', 'cellular', 'or', 'more', 'generally', 'infrastructure', 'networks', 'both', 'multicell', 'processing', 'cooperation', 'among', 'base', 'stations', 'and', 'relaying', 'cooperation', 'at', 'the', 'use... | [-0.2749307295340157, 0.020347633483932814, 0.030224333086407908, 0.017688845893559613, -0.0669384508363241, -0.2351687382602037, 0.16251594876591988, 0.3908382920530912, -0.22053257010389712, -0.24699842099483324, 0.07694926269778929, -0.24326203511070424, -0.22554431168284161, 0.17674431644998073, -0.1227725087839100... |
710.3889 | Epigenetic Chromatin Silencing: Bistability and Front Propagation | The role of post-translational modification of histones in eukaryotic gene
regulation is well recognized. Epigenetic silencing of genes via heritable
chromatin modifications plays a major role in cell fate specification in higher
organisms. We formulate a coarse-grained model of chromatin silencing in yeast
and study... | q-bio.MN | the role of posttranslational modification of histones in eukaryotic gene regulation is well recognized epigenetic silencing of genes via heritable chromatin modifications plays a major role in cell fate specification in higher organisms we formulate a coarsegrained model of chromatin silencing in yeast and study the c... | [['the', 'role', 'of', 'posttranslational', 'modification', 'of', 'histones', 'in', 'eukaryotic', 'gene', 'regulation', 'is', 'well', 'recognized', 'epigenetic', 'silencing', 'of', 'genes', 'via', 'heritable', 'chromatin', 'modifications', 'plays', 'a', 'major', 'role', 'in', 'cell', 'fate', 'specification', 'in', 'hig... | [-0.12896050886974034, 0.1280756409868206, -0.07190909804408684, 0.11224662885498746, -0.040375673247035594, -0.16615117906752092, 0.05983215573268305, 0.3210620088698833, -0.24996419387232316, -0.24584368890837618, 0.005099574733819616, -0.19772698779002224, -0.2835915073703386, 0.17727945395010083, -0.090809934531142... |
710.389 | The genus of a curve of Fermat type | In this paper we begin to study curves on a weighted projective plane with
one trivial weight, ${\mathbb P}(1,m,n)$, by determining the genus of curves of
Fermat type. These are curves defined by a ``homogeneous'' polynomial analagous
to the one from Fermat's last theorem. We begin by finding local coordinates
for th... | math.AG | in this paper we begin to study curves on a weighted projective plane with one trivial weight mathbb p1mn by determining the genus of curves of fermat type these are curves defined by a homogeneous polynomial analagous to the one from fermats last theorem we begin by finding local coordinates for the standard affine co... | [['in', 'this', 'paper', 'we', 'begin', 'to', 'study', 'curves', 'on', 'a', 'weighted', 'projective', 'plane', 'with', 'one', 'trivial', 'weight', 'mathbb', 'p1mn', 'by', 'determining', 'the', 'genus', 'of', 'curves', 'of', 'fermat', 'type', 'these', 'are', 'curves', 'defined', 'by', 'a', 'homogeneous', 'polynomial', '... | [-0.1613445738765681, 0.02496397598846772, -0.13631079441684985, 0.032095606435551614, -0.09139367875373253, -0.14550558722221127, 0.047604319614480105, 0.33199692688116406, -0.3711010937657312, -0.21257420259780277, 0.1106974298001711, -0.253174689694125, -0.1410466545200515, 0.2617264419498148, -0.1674384139391167, 0... |
710.3891 | Analysis of Critical State Response in Thin Films by ac Susceptibility
Measurements | Harmonic analysis of the temperature dependence of the nonlinear ac
susceptibility of Nb thin film gives excellent agreement with the
susceptibility calculated on basis of model of the hysteretic critical state in
2D disk.
| cond-mat.supr-con | harmonic analysis of the temperature dependence of the nonlinear ac susceptibility of nb thin film gives excellent agreement with the susceptibility calculated on basis of model of the hysteretic critical state in 2d disk | [['harmonic', 'analysis', 'of', 'the', 'temperature', 'dependence', 'of', 'the', 'nonlinear', 'ac', 'susceptibility', 'of', 'nb', 'thin', 'film', 'gives', 'excellent', 'agreement', 'with', 'the', 'susceptibility', 'calculated', 'on', 'basis', 'of', 'model', 'of', 'the', 'hysteretic', 'critical', 'state', 'in', '2d', 'd... | [-0.1555675403214991, 0.07855851959217997, -0.03424810267546598, -0.0747168609420495, -0.011392560568364227, -0.12974013497724252, 0.09142840954968158, 0.34841161473270726, -0.17051161935224252, -0.26895576463464427, 0.0028937628924134463, -0.3560958469067426, -0.08142521672005601, 0.26962841931483983, 0.09151812993428... |
710.3892 | Maturity-independent risk measures | The new notion of maturity-independent risk measures is introduced and
contrasted with the existing risk measurement concepts. It is shown, by means
of two examples, one set on a finite probability space and the other in a
diffusion framework, that, surprisingly, some of the widely utilized risk
measures cannot be us... | q-fin.RM math.OC math.PR | the new notion of maturityindependent risk measures is introduced and contrasted with the existing risk measurement concepts it is shown by means of two examples one set on a finite probability space and the other in a diffusion framework that surprisingly some of the widely utilized risk measures cannot be used to bui... | [['the', 'new', 'notion', 'of', 'maturityindependent', 'risk', 'measures', 'is', 'introduced', 'and', 'contrasted', 'with', 'the', 'existing', 'risk', 'measurement', 'concepts', 'it', 'is', 'shown', 'by', 'means', 'of', 'two', 'examples', 'one', 'set', 'on', 'a', 'finite', 'probability', 'space', 'and', 'the', 'other',... | [-0.0396670963845712, 0.07436548949121252, -0.08565792437079117, 0.16083603003095814, -0.04255644058330769, -0.14391677444923276, 0.048356982070560516, 0.38415638033888844, -0.26358460975614817, -0.2281257291692064, 0.15705953609492435, -0.28797827174543944, -0.1859192277893032, 0.24069278190941795, -0.1522176077246274... |
710.3893 | Mass limits for heavy neutrinos | Neutrinos heavier than $M_Z/2\sim 45$ GeV are not excluded by particle
physics data. Stable neutrinos heavier than this might contribute to the cosmic
gamma ray background through annihilation in distant galaxies as well as to the
dark matter content of the universe. We calculate the evolution of the heavy
neutrino d... | astro-ph | neutrinos heavier than m_z2sim 45 gev are not excluded by particle physics data stable neutrinos heavier than this might contribute to the cosmic gamma ray background through annihilation in distant galaxies as well as to the dark matter content of the universe we calculate the evolution of the heavy neutrino density i... | [['neutrinos', 'heavier', 'than', 'm_z2sim', '45', 'gev', 'are', 'not', 'excluded', 'by', 'particle', 'physics', 'data', 'stable', 'neutrinos', 'heavier', 'than', 'this', 'might', 'contribute', 'to', 'the', 'cosmic', 'gamma', 'ray', 'background', 'through', 'annihilation', 'in', 'distant', 'galaxies', 'as', 'well', 'as... | [-0.03209922854633381, 0.23372890139442115, -0.0865050757586557, 0.20950841097025355, -0.05848607514469352, -0.04083462783213084, 0.012143707002646156, 0.33422715986879276, -0.22565908340662386, -0.37209906104752527, -0.00504787159124611, -0.34282382148584084, 0.06717704741943938, 0.19073159561126626, 0.068902430655206... |
710.3894 | Upper and lower bounds on resonances for manifolds hyperbolic near
infinity | For a conformally compact manifold that is hyperbolic near infinity and of
dimension $n+1$, we complete the proof of the optimal $O(r^{n+1})$ upper bound
on the resonance counting function, correcting a mistake in the existing
literature. In the case of a compactly supported perturbation of a hyperbolic
manifold, we ... | math.SP math.DG | for a conformally compact manifold that is hyperbolic near infinity and of dimension n1 we complete the proof of the optimal orn1 upper bound on the resonance counting function correcting a mistake in the existing literature in the case of a compactly supported perturbation of a hyperbolic manifold we establish a poiss... | [['for', 'a', 'conformally', 'compact', 'manifold', 'that', 'is', 'hyperbolic', 'near', 'infinity', 'and', 'of', 'dimension', 'n1', 'we', 'complete', 'the', 'proof', 'of', 'the', 'optimal', 'orn1', 'upper', 'bound', 'on', 'the', 'resonance', 'counting', 'function', 'correcting', 'a', 'mistake', 'in', 'the', 'existing',... | [-0.17452974280027986, 0.05239516609917582, -0.10793624346011452, 0.11497013815134377, -0.09509944759442338, -0.08760589310996138, 0.056129227977475854, 0.28566657119224986, -0.19417713350289828, -0.2218565597114238, 0.09534152986603871, -0.305358956434897, -0.16431382802835146, 0.20172741724928092, -0.0618110301166579... |
710.3895 | Thermal/quantum effects and induced superstring cosmologies | We consider classical superstring theories on flat four dimensional
space-times, and where N=4 or N=2 supersymmetry is spontaneously broken. We
obtain the thermal and quantum corrections at the string one-loop level and
show that the back-reaction on the space-time metric induces a cosmological
evolution. We concentr... | hep-th gr-qc hep-ph | we consider classical superstring theories on flat four dimensional spacetimes and where n4 or n2 supersymmetry is spontaneously broken we obtain the thermal and quantum corrections at the string oneloop level and show that the backreaction on the spacetime metric induces a cosmological evolution we concentrate on hete... | [['we', 'consider', 'classical', 'superstring', 'theories', 'on', 'flat', 'four', 'dimensional', 'spacetimes', 'and', 'where', 'n4', 'or', 'n2', 'supersymmetry', 'is', 'spontaneously', 'broken', 'we', 'obtain', 'the', 'thermal', 'and', 'quantum', 'corrections', 'at', 'the', 'string', 'oneloop', 'level', 'and', 'show', ... | [-0.17418817065379305, 0.21431181905885555, -0.03890210812961733, 0.11452015656914964, -0.06322967241568542, -0.13484792832310336, -0.025269748173603737, 0.3040990821287237, -0.23815482736540003, -0.26956440120293584, 0.12552461658189124, -0.24983245171354831, -0.12283031926993784, 0.11163060061407049, -0.0282054906358... |
710.3896 | Verifying the Cosmological Utility of Type Ia Supernovae: Implications
of a Dispersion in the Ultraviolet Spectra | We analyze the mean rest-frame ultraviolet (UV) spectrum of Type Ia
Supernovae (SNe Ia) and its dispersion using high signal-to-noise Keck-I/LRIS-B
spectroscopy for a sample of 36 events at intermediate redshift (z=0.5)
discovered by the Canada-France-Hawaii Telescope Supernova Legacy Survey
(SNLS). We introduce a ne... | astro-ph | we analyze the mean restframe ultraviolet uv spectrum of type ia supernovae sne ia and its dispersion using high signaltonoise keckilrisb spectroscopy for a sample of 36 events at intermediate redshift z05 discovered by the canadafrancehawaii telescope supernova legacy survey snls we introduce a new method for removing... | [['we', 'analyze', 'the', 'mean', 'restframe', 'ultraviolet', 'uv', 'spectrum', 'of', 'type', 'ia', 'supernovae', 'sne', 'ia', 'and', 'its', 'dispersion', 'using', 'high', 'signaltonoise', 'keckilrisb', 'spectroscopy', 'for', 'a', 'sample', 'of', '36', 'events', 'at', 'intermediate', 'redshift', 'z05', 'discovered', 'b... | [-0.03445426749072316, 0.06467773326734008, -0.07661515585636298, 0.1418784925137157, -0.13034706220139552, -0.09317641538766681, 0.08399542048403545, 0.466265641893838, -0.18553304597633435, -0.3209031656160135, 0.05020475534876863, -0.32195000466720686, -0.05288631712548761, 0.21144532239409572, -0.07275896512117364,... |
710.3897 | Constraining Muon Internal Bremsstrahlung as a Contribution to the
MiniBooNE Low Energy Excess | Using a cleanly tagged data sample of $\nu_\mu$ charged current events, it is
demonstrated that the rate at which such events are mis-identified as $\nu_e$'s
is accurately simulated in the MiniBooNE $\nu_\mu \to \nu_e$ analysis. Such
mis-identification, which could arise from muon internal bremsstrahlung, is
decisive... | hep-ex | using a cleanly tagged data sample of nu_mu charged current events it is demonstrated that the rate at which such events are misidentified as nu_es is accurately simulated in the miniboone nu_mu to nu_e analysis such misidentification which could arise from muon internal bremsstrahlung is decisively ruled out as a sour... | [['using', 'a', 'cleanly', 'tagged', 'data', 'sample', 'of', 'nu_mu', 'charged', 'current', 'events', 'it', 'is', 'demonstrated', 'that', 'the', 'rate', 'at', 'which', 'such', 'events', 'are', 'misidentified', 'as', 'nu_es', 'is', 'accurately', 'simulated', 'in', 'the', 'miniboone', 'nu_mu', 'to', 'nu_e', 'analysis', '... | [-0.030625012648912767, 0.22799751384752906, -0.0549278204018871, 0.21271438657357875, -0.0738766627619043, -0.08245393319262398, 0.10700349798555382, 0.2867232671421435, -0.19496195462221902, -0.34283986940152117, -0.05509327413359036, -0.4244465393738614, -0.03106362010455794, 0.1699123937714224, -0.02059761517577701... |
710.3898 | Around MOND: Lagrangians, Hubble Equations, Perturbations and External
Field Effect | The MOdified Newtonian Dynamics (MOND) is presented here, as well as a theory
that can be linked to it: the theory of the Aether, a four-vector field
breaking Lorentz invariance. The form of its Lagrangian is studied, then basic
equations of the theory are rederived in a detailed way, and calculated for
different met... | astro-ph | the modified newtonian dynamics mond is presented here as well as a theory that can be linked to it the theory of the aether a fourvector field breaking lorentz invariance the form of its lagrangian is studied then basic equations of the theory are rederived in a detailed way and calculated for different metrics explor... | [['the', 'modified', 'newtonian', 'dynamics', 'mond', 'is', 'presented', 'here', 'as', 'well', 'as', 'a', 'theory', 'that', 'can', 'be', 'linked', 'to', 'it', 'the', 'theory', 'of', 'the', 'aether', 'a', 'fourvector', 'field', 'breaking', 'lorentz', 'invariance', 'the', 'form', 'of', 'its', 'lagrangian', 'is', 'studied... | [-0.1819384846215447, 0.1446899400339351, -0.1397172838449478, 0.10077623180778963, -0.14561683370598724, -0.1101792362163819, -0.06492456559734862, 0.30063759288085357, -0.25087200246219127, -0.283941984779778, 0.04146726756201436, -0.19250713520062465, -0.1716837488647018, 0.13867066019835572, -0.006561939679973182, ... |
710.3899 | Possible Enhanced Flux of Glassy Solid Helium in Cylindrical Corrugated
Nanopores | By using the glassy (helium-)fluid model and boundary perturbation method, we
can obtain the velocity fields (as well as the flow rate; up to the second
order) inside the wavy-rough cylindrical nanopores which are of the same size
as those samples prepared by Kim and Chan as well as Day {\it et al.} Our
results show ... | cond-mat.other cond-mat.dis-nn | by using the glassy heliumfluid model and boundary perturbation method we can obtain the velocity fields as well as the flow rate up to the second order inside the wavyrough cylindrical nanopores which are of the same size as those samples prepared by kim and chan as well as day it et al our results show that the veloc... | [['by', 'using', 'the', 'glassy', 'heliumfluid', 'model', 'and', 'boundary', 'perturbation', 'method', 'we', 'can', 'obtain', 'the', 'velocity', 'fields', 'as', 'well', 'as', 'the', 'flow', 'rate', 'up', 'to', 'the', 'second', 'order', 'inside', 'the', 'wavyrough', 'cylindrical', 'nanopores', 'which', 'are', 'of', 'the... | [-0.005382695837761275, 0.1719756765232887, -0.05743467534193769, -0.003006126149557531, -0.025305190007202327, -0.10472783651202917, 0.004005264642182737, 0.4004832183592953, -0.2524102743354888, -0.39117492008954285, 0.1262646266637603, -0.26486807405017315, -0.09963975364807993, 0.20128374313644598, -0.0648061489104... |
710.39 | Law without Law | We consider a model for spacetime in which there is an ubiquitous background
Dark Energy which is the Zero Point Field. This is further modeled in terms of
a Weiner process that leads to a Random or Brownian characterization.
Nevertheless we are able to recover meaningful physics, very much in the spirit
of Wheeler's... | physics.gen-ph | we consider a model for spacetime in which there is an ubiquitous background dark energy which is the zero point field this is further modeled in terms of a weiner process that leads to a random or brownian characterization nevertheless we are able to recover meaningful physics very much in the spirit of wheelers law w... | [['we', 'consider', 'a', 'model', 'for', 'spacetime', 'in', 'which', 'there', 'is', 'an', 'ubiquitous', 'background', 'dark', 'energy', 'which', 'is', 'the', 'zero', 'point', 'field', 'this', 'is', 'further', 'modeled', 'in', 'terms', 'of', 'a', 'weiner', 'process', 'that', 'leads', 'to', 'a', 'random', 'or', 'brownian... | [-0.08867077590107467, 0.13761476606922576, -0.14764338271043292, 0.07785517323306769, -0.08323660151412089, -0.14196192366635482, 0.020424267031943822, 0.3080447350036014, -0.2553971272921472, -0.2841078035364097, 0.07035151754230769, -0.2426521355201575, -0.17188171092703036, 0.19777967025187204, -0.11821046811669614... |
710.3901 | A recursive linear time modular decomposition algorithm via LexBFS | A module of a graph G is a set of vertices that have the same set of
neighbours outside. Modules of a graphs form a so-called partitive family and
thereby can be represented by a unique tree MD(G), called the modular
decomposition tree. Motivated by the central role of modules in numerous
algorithmic graph theory que... | cs.DM | a module of a graph g is a set of vertices that have the same set of neighbours outside modules of a graphs form a socalled partitive family and thereby can be represented by a unique tree mdg called the modular decomposition tree motivated by the central role of modules in numerous algorithmic graph theory questions t... | [['a', 'module', 'of', 'a', 'graph', 'g', 'is', 'a', 'set', 'of', 'vertices', 'that', 'have', 'the', 'same', 'set', 'of', 'neighbours', 'outside', 'modules', 'of', 'a', 'graphs', 'form', 'a', 'socalled', 'partitive', 'family', 'and', 'thereby', 'can', 'be', 'represented', 'by', 'a', 'unique', 'tree', 'mdg', 'called', '... | [-0.1320676376834806, 0.07943279432590332, -0.09978792673434343, 0.07680504745088942, -0.1392097017245792, -0.1295246338520787, 0.05683722365913063, 0.36570035943990215, -0.29171541326662953, -0.30354613395767255, 0.14199668240249402, -0.21388296877736585, -0.16025343164393122, 0.17907633058922856, -0.08099811737785083... |
710.3902 | Strangeness and bulk freeze-out properties at RHIC | Identified charged kaon, pion, and proton spectra and ratios from sqrt(s_NN)
= 200 and 62.4 GeV Cu+Cu collisions are studied with a hydro-motivated
blast-wave and a statistical model framework in order to explore the
strangeness production at RHIC and characterize the bulk freeze-out properties
of the created system.... | nucl-ex | identified charged kaon pion and proton spectra and ratios from sqrts_nn 200 and 624 gev cucu collisions are studied with a hydromotivated blastwave and a statistical model framework in order to explore the strangeness production at rhic and characterize the bulk freezeout properties of the created system the spectra a... | [['identified', 'charged', 'kaon', 'pion', 'and', 'proton', 'spectra', 'and', 'ratios', 'from', 'sqrts_nn', '200', 'and', '624', 'gev', 'cucu', 'collisions', 'are', 'studied', 'with', 'a', 'hydromotivated', 'blastwave', 'and', 'a', 'statistical', 'model', 'framework', 'in', 'order', 'to', 'explore', 'the', 'strangeness... | [-0.05243751833202421, 0.26203147774746566, -0.17968566028543542, 0.12541519827613634, 0.07390463425286321, -0.09705571188492791, -0.06996172570183666, 0.30202993806677925, -0.21373001523574608, -0.32810640877061004, -0.13941886646514629, -0.4040737679072966, 0.190279479583195, 0.12390958822005713, 0.11103460766349195,... |
710.3903 | Lorentzian spacetimes with constant curvature invariants in three
dimensions | In this paper we study Lorentzian spacetimes for which all polynomial scalar
invariants constructed from the Riemann tensor and its covariant derivatives
are constant (CSI spacetimes) in three dimensions. We determine all such CSI
metrics explicitly, and show that for every CSI with particular constant
invariants the... | gr-qc | in this paper we study lorentzian spacetimes for which all polynomial scalar invariants constructed from the riemann tensor and its covariant derivatives are constant csi spacetimes in three dimensions we determine all such csi metrics explicitly and show that for every csi with particular constant invariants there is ... | [['in', 'this', 'paper', 'we', 'study', 'lorentzian', 'spacetimes', 'for', 'which', 'all', 'polynomial', 'scalar', 'invariants', 'constructed', 'from', 'the', 'riemann', 'tensor', 'and', 'its', 'covariant', 'derivatives', 'are', 'constant', 'csi', 'spacetimes', 'in', 'three', 'dimensions', 'we', 'determine', 'all', 'su... | [-0.2110587618431993, 0.14845154612576442, -0.05304292717067126, 0.05068661947549868, -0.12947685261892658, -0.21626962693999446, -0.094785590477783, 0.38842474213904804, -0.22805091253821813, -0.16187165418477167, 0.13174133637406316, -0.26743450338050484, -0.17058629893867802, 0.09074642108420708, -0.0397481552310406... |
710.3904 | Aharanov-Bohm effect for the edge states of zigzag carbon nanotubes | Two delocalized states of metallic zigzag carbon nanotubes near the Dirac
point can be localized by the Aharanov-Bohm magnetic field around 20 Tesla. The
dependence of the localization on the length and diameter of the nanotubes
shows that the localization-delocalization transition can be observed for 2 nm
diameter t... | cond-mat.mes-hall cond-mat.mtrl-sci | two delocalized states of metallic zigzag carbon nanotubes near the dirac point can be localized by the aharanovbohm magnetic field around 20 tesla the dependence of the localization on the length and diameter of the nanotubes shows that the localizationdelocalization transition can be observed for 2 nm diameter tube t... | [['two', 'delocalized', 'states', 'of', 'metallic', 'zigzag', 'carbon', 'nanotubes', 'near', 'the', 'dirac', 'point', 'can', 'be', 'localized', 'by', 'the', 'aharanovbohm', 'magnetic', 'field', 'around', '20', 'tesla', 'the', 'dependence', 'of', 'the', 'localization', 'on', 'the', 'length', 'and', 'diameter', 'of', 'th... | [-0.17312292320032915, 0.26311124678628117, -0.05839857668159347, 0.03034468303096718, 0.04146465402628368, -0.14559987049513295, 0.04072297026583578, 0.38920344793986456, -0.2677538813110076, -0.2921121828623262, 0.01646989912100538, -0.314746694666717, -0.1425015882168915, 0.14602490388970896, 0.03705167596904086, -0... |
710.3905 | The (ir)Relevance of Initial Conditions in Soft Leptogenesis | We explore how the initial conditions affect the final lepton asymmetry in
Soft Leptogenesis. It has been usually assumed that the initial state is a
statistical mixture of sterile sneutrinos and anti-sneutrinos with equal
abundances. We calculate the lepton asymmetry due to the most general initial
mixture. The usua... | hep-ph | we explore how the initial conditions affect the final lepton asymmetry in soft leptogenesis it has been usually assumed that the initial state is a statistical mixture of sterile sneutrinos and antisneutrinos with equal abundances we calculate the lepton asymmetry due to the most general initial mixture the usually as... | [['we', 'explore', 'how', 'the', 'initial', 'conditions', 'affect', 'the', 'final', 'lepton', 'asymmetry', 'in', 'soft', 'leptogenesis', 'it', 'has', 'been', 'usually', 'assumed', 'that', 'the', 'initial', 'state', 'is', 'a', 'statistical', 'mixture', 'of', 'sterile', 'sneutrinos', 'and', 'antisneutrinos', 'with', 'equ... | [-0.088709416162545, 0.29607493741216157, -0.0685908348657764, 0.18795712053811608, -0.06468206396004042, -0.2076282649193532, 0.030363573184093603, 0.2914948730299679, -0.20770512036710548, -0.30456479837079176, 0.043859732887694215, -0.26252560653508855, 0.003008104205274811, 0.03391561708771265, -0.01711938547400328... |
710.3906 | A Parameter Study of the Dust and Gas Temperature in a Field of Young
Stars | We model the thermal effect of young stars on their surrounding environment
in order to understand clustered star formation. We take radiative heating of
dust, dust-gas collisional heating, cosmic-ray heating, and molecular cooling
into account. Using Dusty, a spherical continuum radiative transfer code, we
model the... | astro-ph | we model the thermal effect of young stars on their surrounding environment in order to understand clustered star formation we take radiative heating of dust dustgas collisional heating cosmicray heating and molecular cooling into account using dusty a spherical continuum radiative transfer code we model the dust tempe... | [['we', 'model', 'the', 'thermal', 'effect', 'of', 'young', 'stars', 'on', 'their', 'surrounding', 'environment', 'in', 'order', 'to', 'understand', 'clustered', 'star', 'formation', 'we', 'take', 'radiative', 'heating', 'of', 'dust', 'dustgas', 'collisional', 'heating', 'cosmicray', 'heating', 'and', 'molecular', 'coo... | [-0.005464265946721455, 0.149004961747457, -0.08393629344704584, 0.11357366231743622, -0.06146670478795256, -0.022104175436553082, 0.01770783189151968, 0.46028060275090843, -0.17743907265459039, -0.3586145164914617, 0.01844955881188835, -0.2317590231712743, 0.017387788601908365, 0.15157490400372448, 0.01085268104979142... |
710.3907 | Impacts of preference and geography on epidemic spreading | We investigate the standard susceptible-infected-susceptible model on a
random network to study the effects of preference and geography on diseases
spreading. The network grows by introducing one random node with $m$ links on a
Euclidean space at unit time. The probability of a new node $i$ linking to a
node $j$ with... | physics.soc-ph | we investigate the standard susceptibleinfectedsusceptible model on a random network to study the effects of preference and geography on diseases spreading the network grows by introducing one random node with m links on a euclidean space at unit time the probability of a new node i linking to a node j with degree k_j ... | [['we', 'investigate', 'the', 'standard', 'susceptibleinfectedsusceptible', 'model', 'on', 'a', 'random', 'network', 'to', 'study', 'the', 'effects', 'of', 'preference', 'and', 'geography', 'on', 'diseases', 'spreading', 'the', 'network', 'grows', 'by', 'introducing', 'one', 'random', 'node', 'with', 'm', 'links', 'on'... | [-0.14736999773109952, 0.12978716440160165, -0.0026043641811349626, 0.04316828841745684, -0.05605252571474535, -0.24016781692802341, 0.12175929575283645, 0.32219017652625387, -0.2688638327967827, -0.2136119152286979, 0.07872869135198099, -0.34290182006996917, -0.16033084241842682, 0.09047547740523111, -0.02728826530845... |
710.3908 | Lie Rinehart Bialgebras for Crossed Products | In this paper, we study Lie Rinehart bialgebras, the algebraic generalization
of Lie bialgebroids. More precisely, we analyze the structure of Lie Rinehart
bialgebras for crossed products induced by actions of Lie algebras on K[t].
| math.AC math.RA | in this paper we study lie rinehart bialgebras the algebraic generalization of lie bialgebroids more precisely we analyze the structure of lie rinehart bialgebras for crossed products induced by actions of lie algebras on kt | [['in', 'this', 'paper', 'we', 'study', 'lie', 'rinehart', 'bialgebras', 'the', 'algebraic', 'generalization', 'of', 'lie', 'bialgebroids', 'more', 'precisely', 'we', 'analyze', 'the', 'structure', 'of', 'lie', 'rinehart', 'bialgebras', 'for', 'crossed', 'products', 'induced', 'by', 'actions', 'of', 'lie', 'algebras', ... | [-0.23116947985586844, 0.04764209889939853, -0.026253309500004565, 0.12758130887190677, -0.22816175658788, -0.07780543214508466, -0.005189154852580811, 0.459477345432554, -0.37391135351998467, -0.1681656437260764, 0.09917685701844416, -0.16795343181916644, -0.23304839538676397, 0.18395957499742507, -0.19410756714642047... |
710.3909 | On the Existence of Global Bisections of Lie Groupoids | We show that every source connected Lie groupoid always has global bisections
through any given point. This bisection can be chosen to be the multiplication
of some exponentials as close as possible to a prescribed curve. The existence
of bisections through more than one prescribed points is also discussed. We
give s... | math.DG | we show that every source connected lie groupoid always has global bisections through any given point this bisection can be chosen to be the multiplication of some exponentials as close as possible to a prescribed curve the existence of bisections through more than one prescribed points is also discussed we give some i... | [['we', 'show', 'that', 'every', 'source', 'connected', 'lie', 'groupoid', 'always', 'has', 'global', 'bisections', 'through', 'any', 'given', 'point', 'this', 'bisection', 'can', 'be', 'chosen', 'to', 'be', 'the', 'multiplication', 'of', 'some', 'exponentials', 'as', 'close', 'as', 'possible', 'to', 'a', 'prescribed',... | [-0.16769303566686353, 0.0653416642657759, -0.10313675242165725, 0.06760170715942718, -0.13357564114164888, -0.16615388739298573, 0.05990361445583403, 0.4211975710237758, -0.31371444401641685, -0.2087854588436976, 0.17134154560207798, -0.2506665276777583, -0.18620405365761958, 0.2619847490272501, -0.11880171921496328, ... |
710.391 | On the photoionization of the outer electrons in noble gas endohedral
atoms | We demonstrate the prominent modification of the outer shell photoionization
cross-section in noble gas (NG) endohedral atoms NG@F under the action of the
fullerene F electron shell. This shell leads to two important effects, namely
to strong enhancement of the cross-section due to fullerenes shell polarization
under... | physics.atm-clus physics.atom-ph | we demonstrate the prominent modification of the outer shell photoionization crosssection in noble gas ng endohedral atoms ngf under the action of the fullerene f electron shell this shell leads to two important effects namely to strong enhancement of the crosssection due to fullerenes shell polarization under the acti... | [['we', 'demonstrate', 'the', 'prominent', 'modification', 'of', 'the', 'outer', 'shell', 'photoionization', 'crosssection', 'in', 'noble', 'gas', 'ng', 'endohedral', 'atoms', 'ngf', 'under', 'the', 'action', 'of', 'the', 'fullerene', 'f', 'electron', 'shell', 'this', 'shell', 'leads', 'to', 'two', 'important', 'effect... | [-0.08011042731898972, 0.1149159094687396, -0.03896727025949076, 0.056270731926512475, -0.003127941393662089, -0.07188555261139602, -9.85953192866873e-06, 0.39760006007660803, -0.20543137592297475, -0.2816769127772811, -0.002258983077505642, -0.29270703202928416, -0.057852425878081704, 0.12911929767384814, 0.0230276662... |
710.3911 | Helium stars as supernova progenitors | We follow the evolution of helium stars of initial mass $(2.2 - 2.5)
M_\odot$, and show that they undergo off-center carbon burning, which leaves
behind ${\mathbf \sim 0.01 M_\odot}$ of unburnt carbon in the inner part of the
core. When the carbon-oxygen core grows to Chandrasekhar mass, the amount of
left-over carbo... | astro-ph | we follow the evolution of helium stars of initial mass 22 25 m_odot and show that they undergo offcenter carbon burning which leaves behind mathbf sim 001 m_odot of unburnt carbon in the inner part of the core when the carbonoxygen core grows to chandrasekhar mass the amount of leftover carbon is sufficient to ignite ... | [['we', 'follow', 'the', 'evolution', 'of', 'helium', 'stars', 'of', 'initial', 'mass', '22', '25', 'm_odot', 'and', 'show', 'that', 'they', 'undergo', 'offcenter', 'carbon', 'burning', 'which', 'leaves', 'behind', 'mathbf', 'sim', '001', 'm_odot', 'of', 'unburnt', 'carbon', 'in', 'the', 'inner', 'part', 'of', 'the', '... | [-0.09336884588811867, 0.20146826401529572, -0.0008653314431478991, 0.044029843194937864, -0.020704579401827423, -0.08104680790207706, 0.10097282569884383, 0.36202137523810185, -0.1608486408657069, -0.3608847100993056, 0.08492740547351992, -0.2913771356075738, 0.027668022939152794, 0.18510869373953157, -0.0559122780111... |
710.3912 | The sectional curvature remains positive when taking quotients by
certain nonfree actions | We study some cases when the sectional curvature remains positive under the
taking of quotients by certain nonfree isometric actions of Lie groups. We
consider the actions of the groups $S^1$ and $S^3$ such that the quotient space
can be endowed with a smooth structure using the fibrations
$S^3/S^1{\simeq}S^2$ and $S... | math.DG | we study some cases when the sectional curvature remains positive under the taking of quotients by certain nonfree isometric actions of lie groups we consider the actions of the groups s1 and s3 such that the quotient space can be endowed with a smooth structure using the fibrations s3s1simeqs2 and s7s3simeq s4 we prov... | [['we', 'study', 'some', 'cases', 'when', 'the', 'sectional', 'curvature', 'remains', 'positive', 'under', 'the', 'taking', 'of', 'quotients', 'by', 'certain', 'nonfree', 'isometric', 'actions', 'of', 'lie', 'groups', 'we', 'consider', 'the', 'actions', 'of', 'the', 'groups', 's1', 'and', 's3', 'such', 'that', 'the', '... | [-0.24606501298570416, 0.09388613677583635, -0.08133083694364603, 0.06564574481964838, -0.1172948597033122, -0.12345417437893225, -0.05243729023126567, 0.4209904049227877, -0.2706518414133603, -0.16260830718433347, 0.15760968498624406, -0.2969218223787299, -0.16534421389082038, 0.15765649996834194, -0.15684550492910715... |
710.3913 | Charged fundamental particles in Wesson's IMT | In the framework of the Weyl-Dirac version of Wesson's Induced Matter Theory,
spherically symmetric entities filled with an electrically charged substance
are obtained in the empty 4D space-time, the brane. The substance,
characterized by mass and charge density as well by pressure, is induced by the
5D bulk. The ent... | gr-qc | in the framework of the weyldirac version of wessons induced matter theory spherically symmetric entities filled with an electrically charged substance are obtained in the empty 4d spacetime the brane the substance characterized by mass and charge density as well by pressure is induced by the 5d bulk the entity is sepa... | [['in', 'the', 'framework', 'of', 'the', 'weyldirac', 'version', 'of', 'wessons', 'induced', 'matter', 'theory', 'spherically', 'symmetric', 'entities', 'filled', 'with', 'an', 'electrically', 'charged', 'substance', 'are', 'obtained', 'in', 'the', 'empty', '4d', 'spacetime', 'the', 'brane', 'the', 'substance', 'charac... | [-0.09807355363053553, 0.25258398878166033, -0.028943643930530095, 0.06233028994377136, -0.03510316595376302, -0.1527503633962782, -0.04199744245599267, 0.28319194794470526, -0.20253921404440442, -0.318348115745365, 0.024585796094944944, -0.30846671168894874, -0.060140884595255004, 0.07415462587960064, -0.0445425743844... |
710.3914 | Protecting entanglement via the quantum Zeno effect | We study the exact entanglement dynamics of two atoms in a lossy resonator.
Besides discussing the steady-state entanglement, we show that in the strong
coupling regime the system-reservoir correlations induce entanglement revivals
and oscillations and propose a strategy to fight against the deterioration of
the enta... | quant-ph | we study the exact entanglement dynamics of two atoms in a lossy resonator besides discussing the steadystate entanglement we show that in the strong coupling regime the systemreservoir correlations induce entanglement revivals and oscillations and propose a strategy to fight against the deterioration of the entangleme... | [['we', 'study', 'the', 'exact', 'entanglement', 'dynamics', 'of', 'two', 'atoms', 'in', 'a', 'lossy', 'resonator', 'besides', 'discussing', 'the', 'steadystate', 'entanglement', 'we', 'show', 'that', 'in', 'the', 'strong', 'coupling', 'regime', 'the', 'systemreservoir', 'correlations', 'induce', 'entanglement', 'reviv... | [-0.2307664751458694, 0.2123373505458528, -0.09260035214909151, 0.10752216992242371, 0.0679235229743462, -0.21243143072534426, 0.07667370979199369, 0.3400060369395742, -0.25177286211036, -0.19918613146771402, 0.02327848758603282, -0.2953585149610744, -0.15884835271201297, 0.16843135286049515, -0.0007454671956343102, 0.... |
710.3915 | Inverse spectral results for Schr\"odinger operators on the unit
interval with potentials in L^P spaces | We consider the Schr\"odinger operator on $[0,1]$ with potential in $L^1$. We
prove that two potentials already known on $[a,1]$ ($a\in(0,{1/2}]$) and having
their difference in $L^p$ are equal if the number of their common eigenvalues
is sufficiently large. The result here is to write down explicitly this number
in ... | math.SP | we consider the schrodinger operator on 01 with potential in l1 we prove that two potentials already known on a1 ain012 and having their difference in lp are equal if the number of their common eigenvalues is sufficiently large the result here is to write down explicitly this number in terms of p and a showing the role... | [['we', 'consider', 'the', 'schrodinger', 'operator', 'on', '01', 'with', 'potential', 'in', 'l1', 'we', 'prove', 'that', 'two', 'potentials', 'already', 'known', 'on', 'a1', 'ain012', 'and', 'having', 'their', 'difference', 'in', 'lp', 'are', 'equal', 'if', 'the', 'number', 'of', 'their', 'common', 'eigenvalues', 'is'... | [-0.14372849790379405, 0.13389464508121213, -0.045575870224274694, 0.06749766364422007, -0.02035616251329581, -0.10924366693167636, 0.03158641350455582, 0.35885110252808466, -0.26519940588623286, -0.2958856852725148, 0.1158537225817175, -0.30716703639676174, -0.1323942084175845, 0.15342661986748377, -0.0407607655584191... |
710.3916 | Optimized Design of Survivable MPLS over Optical Transport Networks.
Optical Switching and Networking | In this paper we study different options for the survivability implementation
in MPLS over Optical Transport Networks in terms of network resource usage and
configuration cost. We investigate two approaches to the survivability
deployment: single layer and multilayer survivability and present various
methods for spar... | cs.NI cs.PF | in this paper we study different options for the survivability implementation in mpls over optical transport networks in terms of network resource usage and configuration cost we investigate two approaches to the survivability deployment single layer and multilayer survivability and present various methods for spare ca... | [['in', 'this', 'paper', 'we', 'study', 'different', 'options', 'for', 'the', 'survivability', 'implementation', 'in', 'mpls', 'over', 'optical', 'transport', 'networks', 'in', 'terms', 'of', 'network', 'resource', 'usage', 'and', 'configuration', 'cost', 'we', 'investigate', 'two', 'approaches', 'to', 'the', 'survivab... | [-0.154151496441008, 0.004386758817455326, 0.014583348318074759, 0.005534330604729266, -0.03323384091998331, -0.13764947918363107, 0.16033220616205093, 0.43009688150471986, -0.29593188954182925, -0.34179276038820927, 0.12212114662755853, -0.26625408134303796, -0.10570050011484478, 0.18191322831269832, -0.08740561722944... |
710.3917 | Heuristic Solution to Protect Communications in WDM Networks using
P-cycles | Optical WDM mesh networks are able to transport huge amount of information.
The use of such technology however poses the problem of protection against
failures such as fibre cuts. One of the principal methods for link protection
used in optical WDM networks is pre-configured protection cycle (p-cycle). The
major prob... | cs.NI | optical wdm mesh networks are able to transport huge amount of information the use of such technology however poses the problem of protection against failures such as fibre cuts one of the principal methods for link protection used in optical wdm networks is preconfigured protection cycle pcycle the major problem of th... | [['optical', 'wdm', 'mesh', 'networks', 'are', 'able', 'to', 'transport', 'huge', 'amount', 'of', 'information', 'the', 'use', 'of', 'such', 'technology', 'however', 'poses', 'the', 'problem', 'of', 'protection', 'against', 'failures', 'such', 'as', 'fibre', 'cuts', 'one', 'of', 'the', 'principal', 'methods', 'for', 'l... | [-0.15819174149415313, 0.034048906165006214, -0.06018969979714197, 0.0090530148110069, -0.08172271209364028, -0.14281645341037327, 0.10997223644580631, 0.3402302271038618, -0.31125459806872124, -0.2954948762730371, 0.12665213473424639, -0.2663011868552649, -0.1394734255331771, 0.18515518278866733, -0.11316473264267425,... |
710.3918 | Dependable k-coverage algorithms for sensor networks | Redundant sensing capabilities are often required in sensor network
applications due to various reasons, e.g. robustness, fault tolerance, or
increased accuracy. At the same time high sensor redundancy offers the
possibility of increasing network lifetime by scheduling sleep intervals for
some sensors and still provi... | cs.NI | redundant sensing capabilities are often required in sensor network applications due to various reasons eg robustness fault tolerance or increased accuracy at the same time high sensor redundancy offers the possibility of increasing network lifetime by scheduling sleep intervals for some sensors and still providing con... | [['redundant', 'sensing', 'capabilities', 'are', 'often', 'required', 'in', 'sensor', 'network', 'applications', 'due', 'to', 'various', 'reasons', 'eg', 'robustness', 'fault', 'tolerance', 'or', 'increased', 'accuracy', 'at', 'the', 'same', 'time', 'high', 'sensor', 'redundancy', 'offers', 'the', 'possibility', 'of', ... | [-0.16433758613348534, 0.043817082902136366, 0.013670101564014908, 0.003870768571453812, -0.050867251705675, -0.22931117733808615, 0.12762146184439319, 0.43261702147732795, -0.2809979021549225, -0.362680237789729, 0.13387254874873084, -0.23981101931262333, -0.16868225043120308, 0.16611969017112563, -0.19212595624766782... |
710.3919 | Bounding sectional curvature along a K\"ahler-Ricci flow | If a normalized K\"{a}hler-Ricci flow $g(t),t\in[0,\infty),$ on a compact
K\"{a}hler $n$-manifold, $n\geq 3$, of positive first Chern class satisfies
$g(t)\in 2\pi c_{1}(M)$ and has $L^{n}$ curvature operator uniformly bounded,
then the curvature operator will also uniformly bounded along the flow.
Consequently the f... | math.DG | if a normalized kahlerricci flow gttin0infty on a compact kahler nmanifold ngeq 3 of positive first chern class satisfies gtin 2pi c_1m and has ln curvature operator uniformly bounded then the curvature operator will also uniformly bounded along the flow consequently the flow will converge along a subsequence to a kahl... | [['if', 'a', 'normalized', 'kahlerricci', 'flow', 'gttin0infty', 'on', 'a', 'compact', 'kahler', 'nmanifold', 'ngeq', '3', 'of', 'positive', 'first', 'chern', 'class', 'satisfies', 'gtin', '2pi', 'c_1m', 'and', 'has', 'ln', 'curvature', 'operator', 'uniformly', 'bounded', 'then', 'the', 'curvature', 'operator', 'will',... | [-0.26761243127140344, 0.17699711143459176, -0.11035407257868964, 0.005179657381685341, -0.13256833150836766, -0.2205344659148478, -0.09925212871794607, 0.4000321599408327, -0.3152036255992511, -0.03382741734750715, 0.14290089022788202, -0.3899064743800052, -0.10240793493393735, 0.136798034294271, -0.1480917500733745, ... |
710.392 | An Introduction to Potential Theory in Calibrated Geometry | We introduce and study the notion of plurisubharmonic functions in calibrated
geometry. These functions generalize the classical plurisubharmonic functions
from complex geometry and enjoy their important properties. Moreover, they
exist in abundance whereas the corresponding pluriharmonics are generally quite
scarce.... | math.DG math.CV | we introduce and study the notion of plurisubharmonic functions in calibrated geometry these functions generalize the classical plurisubharmonic functions from complex geometry and enjoy their important properties moreover they exist in abundance whereas the corresponding pluriharmonics are generally quite scarce a num... | [['we', 'introduce', 'and', 'study', 'the', 'notion', 'of', 'plurisubharmonic', 'functions', 'in', 'calibrated', 'geometry', 'these', 'functions', 'generalize', 'the', 'classical', 'plurisubharmonic', 'functions', 'from', 'complex', 'geometry', 'and', 'enjoy', 'their', 'important', 'properties', 'moreover', 'they', 'ex... | [-0.0935062009475327, 0.08790491431663257, -0.07232625668070146, 0.18149437115810413, -0.0674204498008337, -0.13128025917602437, -0.013053269246371374, 0.38790362521651245, -0.23531691976601168, -0.24876188877083005, 0.11707234202241082, -0.24603329449892045, -0.19959428036762844, 0.2468199963504005, -0.138543541782668... |
710.3921 | Duality of Positive Currents and Plurisubharmonic Functions in
Calibrated Geometry | Recently the authors showed that there is a robust potential theory attached
to any calibrated manifold (X,\phi). In particular, on X there exist
\phi-plurisubharmonic functions, \phi-convex domains, \phi-convex boundaries,
etc., all inter-related and having a number of good properties. In this paper
we show that, in... | math.DG math.CV | recently the authors showed that there is a robust potential theory attached to any calibrated manifold xphi in particular on x there exist phiplurisubharmonic functions phiconvex domains phiconvex boundaries etc all interrelated and having a number of good properties in this paper we show that in a strong sense the pl... | [['recently', 'the', 'authors', 'showed', 'that', 'there', 'is', 'a', 'robust', 'potential', 'theory', 'attached', 'to', 'any', 'calibrated', 'manifold', 'xphi', 'in', 'particular', 'on', 'x', 'there', 'exist', 'phiplurisubharmonic', 'functions', 'phiconvex', 'domains', 'phiconvex', 'boundaries', 'etc', 'all', 'interre... | [-0.14840805767529983, 0.06513328185088864, -0.07882799169900574, 0.09266493661516859, -0.0049741926400871704, -0.07724999190965133, 0.03490310766492328, 0.39162496504799804, -0.22774892880819564, -0.21671496320140454, 0.09667890440210584, -0.2706559822955999, -0.19202863642505494, 0.22373722897763113, -0.1520293443644... |
710.3922 | Hysteresis Models of Dynamic Mode Atomic Force Microscopes: Analysis and
Identification | A new class of models based on hysteresis functions is developed to describe
atomic force microscopes operating in dynamic mode. Such models are able to
account for dissipative phenomena in the tip-sample interaction which are
peculiar of this operation mode. The model analysis, which can be pursued using
frequency d... | nlin.CD | a new class of models based on hysteresis functions is developed to describe atomic force microscopes operating in dynamic mode such models are able to account for dissipative phenomena in the tipsample interaction which are peculiar of this operation mode the model analysis which can be pursued using frequency domain ... | [['a', 'new', 'class', 'of', 'models', 'based', 'on', 'hysteresis', 'functions', 'is', 'developed', 'to', 'describe', 'atomic', 'force', 'microscopes', 'operating', 'in', 'dynamic', 'mode', 'such', 'models', 'are', 'able', 'to', 'account', 'for', 'dissipative', 'phenomena', 'in', 'the', 'tipsample', 'interaction', 'whi... | [-0.11148797200798098, 0.09599684604179504, -0.13005047012120485, 0.07173829258475174, -0.1115068868914647, -0.19063652925360114, 0.01719440647692823, 0.38832517426961394, -0.2526572866173315, -0.2959565897263698, 0.0553318351965898, -0.22324905413856258, -0.1711534047082289, 0.28461184060381756, 0.000909994557889095, ... |
710.3923 | Creation of fundamental particles in Wesson's IMT | Fundamental particles, regarded as the constituents of quarks and leptons,
are described classicaly in the framework of the Weyl-Dirac version of Wesson's
Induced Matter Theory. There are neutral particles and particles having charge
Q=+/-(1/3e). The particles appear on the 4D brane, our universe, and are filled
with... | gr-qc | fundamental particles regarded as the constituents of quarks and leptons are described classicaly in the framework of the weyldirac version of wessons induced matter theory there are neutral particles and particles having charge q13e the particles appear on the 4d brane our universe and are filled with a substance indu... | [['fundamental', 'particles', 'regarded', 'as', 'the', 'constituents', 'of', 'quarks', 'and', 'leptons', 'are', 'described', 'classicaly', 'in', 'the', 'framework', 'of', 'the', 'weyldirac', 'version', 'of', 'wessons', 'induced', 'matter', 'theory', 'there', 'are', 'neutral', 'particles', 'and', 'particles', 'having', ... | [-0.12488697461750624, 0.2710834368160379, -0.05200619310406702, 0.04792174882563164, 0.0019434008579212656, -0.11385733247568298, -0.04855749113422852, 0.2762855966388348, -0.17885791713238827, -0.3066965942021592, 0.03715305528852956, -0.32168034800062223, -0.042616942236366286, 0.0691295006524472, -0.034819794985066... |
710.3924 | Convexity properties for generalized moment maps I | We study generalized moment maps for a Hamiltonian action on a connected
compact $H$-twisted generalized complex manifold introduced by Lin and Tolman
and prove the convexity and connectedness properties of the generalized moment
maps for a Hamiltonian torus action.
| math.DG math.SG | we study generalized moment maps for a hamiltonian action on a connected compact htwisted generalized complex manifold introduced by lin and tolman and prove the convexity and connectedness properties of the generalized moment maps for a hamiltonian torus action | [['we', 'study', 'generalized', 'moment', 'maps', 'for', 'a', 'hamiltonian', 'action', 'on', 'a', 'connected', 'compact', 'htwisted', 'generalized', 'complex', 'manifold', 'introduced', 'by', 'lin', 'and', 'tolman', 'and', 'prove', 'the', 'convexity', 'and', 'connectedness', 'properties', 'of', 'the', 'generalized', 'm... | [-0.18292978377296373, 0.07447677547446428, -0.0705405671436053, 0.1275566451681348, -0.10167808654921082, -0.11626655705129871, -0.003722645566225625, 0.32436544180680543, -0.26352537557100636, -0.18399535806085437, 0.1098350380690625, -0.2566608285698562, -0.21060315242562538, 0.15268301772765625, -0.1212008861729349... |
710.3925 | Regge behaviour of structure functions and solution of
Dokshitzer-Gribov-Lipatov-Altarelli-Parisi Evolution equations in
next-to-leading order at low-x | Deuteron and proton structure functions are derived from
Dokshitzer-Gribov-Lipatov-Altarelli-Parisi (DGLAP) evolution equations of
singlet and non-singlet structure functions in next-to-leading order (NLO) at
low-x assuming the Regge behaviour of singlet and non-singlet structure
functions at this limit and results a... | hep-ph | deuteron and proton structure functions are derived from dokshitzergribovlipatovaltarelliparisi dglap evolution equations of singlet and nonsinglet structure functions in nexttoleading order nlo at lowx assuming the regge behaviour of singlet and nonsinglet structure functions at this limit and results are compared wit... | [['deuteron', 'and', 'proton', 'structure', 'functions', 'are', 'derived', 'from', 'dokshitzergribovlipatovaltarelliparisi', 'dglap', 'evolution', 'equations', 'of', 'singlet', 'and', 'nonsinglet', 'structure', 'functions', 'in', 'nexttoleading', 'order', 'nlo', 'at', 'lowx', 'assuming', 'the', 'regge', 'behaviour', 'o... | [-0.03371411448746335, 0.16440890923909404, -0.1304524915530255, 0.20756578920911267, -0.050129403688890094, -0.015359880387846964, -0.0420121386939404, 0.3480338871332945, -0.14872362028223043, -0.25133866509057434, -0.04427333083232025, -0.37319820991479885, 0.0018759614550599864, 0.06874085745463769, 0.1795047593814... |
710.3926 | From an Antiferromagnet to a Valence Bond Solid: Evidence for a First
Order Phase Transition | Using a loop-cluster algorithm we investigate the spin 1/2 Heisenberg
antiferromagnet on a square lattice with exchange coupling $J$ and an
additional four-spin interaction of strength $Q$. We confirm the existence of a
phase transition separating antiferromagnetism at $J/Q > J_c/Q$ from a valence
bond solid (VBS) st... | cond-mat.str-el | using a loopcluster algorithm we investigate the spin 12 heisenberg antiferromagnet on a square lattice with exchange coupling j and an additional fourspin interaction of strength q we confirm the existence of a phase transition separating antiferromagnetism at jq j_cq from a valence bond solid vbs state at jq j_cq alt... | [['using', 'a', 'loopcluster', 'algorithm', 'we', 'investigate', 'the', 'spin', '12', 'heisenberg', 'antiferromagnet', 'on', 'a', 'square', 'lattice', 'with', 'exchange', 'coupling', 'j', 'and', 'an', 'additional', 'fourspin', 'interaction', 'of', 'strength', 'q', 'we', 'confirm', 'the', 'existence', 'of', 'a', 'phase'... | [-0.15230728726918724, 0.21402284498546964, -0.06807356340048665, 0.06805470381496531, -0.03471967828544703, -0.11051466761326248, 0.11267714138410873, 0.41165125260524676, -0.21364995717832988, -0.2472562187492396, 0.07881013150609127, -0.33638920650789234, -0.09182099739237773, 0.13240364265106053, 0.1218655658025068... |
710.3927 | On repulsive gravitational actions | In particular instances and in particular regions the Einsteinian gravity
exerts a repulsive action -- and without any cosmological term. This fact could
have an interest for the explanation of the dark energy, and for the
gravitational collapses.
| physics.gen-ph | in particular instances and in particular regions the einsteinian gravity exerts a repulsive action and without any cosmological term this fact could have an interest for the explanation of the dark energy and for the gravitational collapses | [['in', 'particular', 'instances', 'and', 'in', 'particular', 'regions', 'the', 'einsteinian', 'gravity', 'exerts', 'a', 'repulsive', 'action', 'and', 'without', 'any', 'cosmological', 'term', 'this', 'fact', 'could', 'have', 'an', 'interest', 'for', 'the', 'explanation', 'of', 'the', 'dark', 'energy', 'and', 'for', 't... | [-0.17386582456025723, 0.11263896624685102, -0.10518196344728002, 0.10698803321370301, -0.12021466178467145, -0.10713008618787737, -0.030549979063908796, 0.27232433140680595, -0.20518587831709836, -0.32273932935267285, 0.04781761555932462, -0.25115410920635267, -0.12242594159938194, 0.18487506261649164, -0.048904391785... |
710.3928 | Message passing for the coloring problem: Gallager meets Alon and Kahale | Message passing algorithms are popular in many combinatorial optimization
problems. For example, experimental results show that {\em survey propagation}
(a certain message passing algorithm) is effective in finding proper
$k$-colorings of random graphs in the near-threshold regime. In 1962 Gallager
introduced the con... | math.CO cs.DM math.PR | message passing algorithms are popular in many combinatorial optimization problems for example experimental results show that em survey propagation a certain message passing algorithm is effective in finding proper kcolorings of random graphs in the nearthreshold regime in 1962 gallager introduced the concept of low de... | [['message', 'passing', 'algorithms', 'are', 'popular', 'in', 'many', 'combinatorial', 'optimization', 'problems', 'for', 'example', 'experimental', 'results', 'show', 'that', 'em', 'survey', 'propagation', 'a', 'certain', 'message', 'passing', 'algorithm', 'is', 'effective', 'in', 'finding', 'proper', 'kcolorings', 'o... | [-0.1759768050239497, 0.0011477293833072385, -0.12877517273316058, 0.0819735558714554, -0.10300000825097684, -0.2145229807702472, 0.12112755746253438, 0.4174256796722074, -0.31089790809090956, -0.3532325649583662, 0.07337682603974827, -0.23741102659118338, -0.20803137120438386, 0.1856554931193288, -0.13605802711351095,... |
710.3929 | Supersymmetry, quark confinement and the harmonic oscillator | We study some quantum systems described by noncanonical commutation relations
formally expressed as [q,p]=ihbar(I + chi H), where H is the associated
(harmonic oscillator-like) Hamiltonian of the system, and chi is a Hermitian
(constant) operator, i.e. [H,chi]=0 . In passing, we also consider a simple
(chi=0 canonica... | quant-ph | we study some quantum systems described by noncanonical commutation relations formally expressed as qpihbari chi h where h is the associated harmonic oscillatorlike hamiltonian of the system and chi is a hermitian constant operator ie hchi0 in passing we also consider a simple chi0 canonical model in the framework of a... | [['we', 'study', 'some', 'quantum', 'systems', 'described', 'by', 'noncanonical', 'commutation', 'relations', 'formally', 'expressed', 'as', 'qpihbari', 'chi', 'h', 'where', 'h', 'is', 'the', 'associated', 'harmonic', 'oscillatorlike', 'hamiltonian', 'of', 'the', 'system', 'and', 'chi', 'is', 'a', 'hermitian', 'constan... | [-0.23175605305663818, 0.18220584505712087, -0.03931894265818146, 0.09235300860402859, -0.06644172146740668, -0.1999279883479313, -0.02317043874008616, 0.29365091451953323, -0.2921940521249231, -0.2276114781896742, 0.0025684673400630928, -0.28011119604673024, -0.17906515799322217, 0.16366430180024286, 0.021767305968030... |
710.393 | Interactions of Heavy Hadrons using Regge Phenomenology and the Quark
Gluon String Model | The search for stable heavy exotic hadrons is a promising way to observe new
physics processes at collider experiments. The discovery potential for such
particles can be enhanced or suppressed by their interactions with detector
material. This paper describes a model for the interactions in matter of stable
hadrons c... | hep-ph | the search for stable heavy exotic hadrons is a promising way to observe new physics processes at collider experiments the discovery potential for such particles can be enhanced or suppressed by their interactions with detector material this paper describes a model for the interactions in matter of stable hadrons conta... | [['the', 'search', 'for', 'stable', 'heavy', 'exotic', 'hadrons', 'is', 'a', 'promising', 'way', 'to', 'observe', 'new', 'physics', 'processes', 'at', 'collider', 'experiments', 'the', 'discovery', 'potential', 'for', 'such', 'particles', 'can', 'be', 'enhanced', 'or', 'suppressed', 'by', 'their', 'interactions', 'with... | [-0.08624747723749862, 0.2907177289997912, -0.13548763656190868, 0.12571352880189718, -0.05370081105076412, -0.1645392810630544, 0.021098201644391093, 0.3094521713238664, -0.22839784575626254, -0.303063256756925, -0.005603093649658215, -0.3641134849522354, -0.01956440983680872, 0.11967485433262659, 0.07997936225019214,... |
710.3931 | Geometric phases in semiconductor spin qubits: Manipulations and
decoherence | We describe the effect of geometric phases induced by either classical or
quantum electric fields acting on single electron spins in quantum dots in the
presence of spin-orbit coupling. On one hand, applied electric fields can be
used to control the geometric phases, which allows performing quantum coherent
spin mani... | cond-mat.mes-hall | we describe the effect of geometric phases induced by either classical or quantum electric fields acting on single electron spins in quantum dots in the presence of spinorbit coupling on one hand applied electric fields can be used to control the geometric phases which allows performing quantum coherent spin manipulati... | [['we', 'describe', 'the', 'effect', 'of', 'geometric', 'phases', 'induced', 'by', 'either', 'classical', 'or', 'quantum', 'electric', 'fields', 'acting', 'on', 'single', 'electron', 'spins', 'in', 'quantum', 'dots', 'in', 'the', 'presence', 'of', 'spinorbit', 'coupling', 'on', 'one', 'hand', 'applied', 'electric', 'fi... | [-0.15649899446066015, 0.27246719337216463, -0.024673236451311923, 0.027971498711169565, -0.05576973646078433, -0.17683241458905635, 0.025479654753232533, 0.38327171086011647, -0.2753552329143353, -0.2924217896657848, 0.022895886954442363, -0.26139952998543614, -0.08450849617615987, 0.2538065950181683, 0.01710360021021... |
710.3932 | Complementarity of perturbations driving insulator-to-metal transition
in a charge ordered manganite | Modulation of charge carrier dynamics and hence electrical conductivity of
solids by photoexcitation has been a rich field of research with numerous
applications. Similarly, electric and magnetic field assisted enhancement of
conductivity are of fundamental importance and technological use. Hole doped
manganites of t... | cond-mat.str-el cond-mat.mtrl-sci | modulation of charge carrier dynamics and hence electrical conductivity of solids by photoexcitation has been a rich field of research with numerous applications similarly electric and magnetic field assisted enhancement of conductivity are of fundamental importance and technological use hole doped manganites of the ty... | [['modulation', 'of', 'charge', 'carrier', 'dynamics', 'and', 'hence', 'electrical', 'conductivity', 'of', 'solids', 'by', 'photoexcitation', 'has', 'been', 'a', 'rich', 'field', 'of', 'research', 'with', 'numerous', 'applications', 'similarly', 'electric', 'and', 'magnetic', 'field', 'assisted', 'enhancement', 'of', '... | [-0.17027204304485394, 0.25014890535461937, -0.003976280303826009, -0.016663140195961938, -0.026172975701878647, -0.12610376546075358, 0.06611401004860304, 0.43775515258312225, -0.2453236228653363, -0.3232898120873405, 0.05903664574856849, -0.28487819881367504, -0.13405144026264884, 0.22203936109571418, 0.0215629630799... |
710.3933 | Energy-momentum tensor in thermal strong-field QED with unstable vacuum | The mean value of the one-loop energy-momentum tensor in thermal QED with
electric-like background that creates particles from vacuum is calculated. The
problem differes essentially from calculations of effective actions (similar to
that of Heisenberg--Euler) in backgrounds that do not violate the stability of
vacuum... | hep-th | the mean value of the oneloop energymomentum tensor in thermal qed with electriclike background that creates particles from vacuum is calculated the problem differes essentially from calculations of effective actions similar to that of heisenbergeuler in backgrounds that do not violate the stability of vacuum the role ... | [['the', 'mean', 'value', 'of', 'the', 'oneloop', 'energymomentum', 'tensor', 'in', 'thermal', 'qed', 'with', 'electriclike', 'background', 'that', 'creates', 'particles', 'from', 'vacuum', 'is', 'calculated', 'the', 'problem', 'differes', 'essentially', 'from', 'calculations', 'of', 'effective', 'actions', 'similar', ... | [-0.13234851766754402, 0.21382316022985773, -0.1000488914204029, 0.06332461709376383, -0.027993286530790706, -0.061466208700969645, -0.018621250845784885, 0.30573215766736633, -0.19174316725327392, -0.30399998325823147, 0.0446766847496057, -0.27313466671477543, -0.05822326728467191, 0.14706747290898073, -0.011498921404... |
710.3934 | New mechanism of generation of large-scale magnetic field in a sheared
turbulent plasma | A review of recent studies on a new mechanism of generation of large-scale
magnetic field in a sheared turbulent plasma is presented. This mechanism is
associated with the shear-current effect which is related to the W x J-term in
the mean electromotive force. This effect causes the generation of the
large-scale magn... | astro-ph | a review of recent studies on a new mechanism of generation of largescale magnetic field in a sheared turbulent plasma is presented this mechanism is associated with the shearcurrent effect which is related to the w x jterm in the mean electromotive force this effect causes the generation of the largescale magnetic fie... | [['a', 'review', 'of', 'recent', 'studies', 'on', 'a', 'new', 'mechanism', 'of', 'generation', 'of', 'largescale', 'magnetic', 'field', 'in', 'a', 'sheared', 'turbulent', 'plasma', 'is', 'presented', 'this', 'mechanism', 'is', 'associated', 'with', 'the', 'shearcurrent', 'effect', 'which', 'is', 'related', 'to', 'the',... | [-0.23028166010662648, 0.27744956821227956, -0.021962349348396592, 0.1069728495935349, -0.08570516298512673, -0.0051927134998357004, -0.04179087636448377, 0.2911684791376171, -0.2860873939626051, -0.313739606616112, 0.027988489592587987, -0.18547960296422614, -0.12303362188003628, 0.2052459827916845, 0.0283899000352372... |
710.3935 | Magnetic Reversal Time in Open Long Range Systems | Topological phase space disconnection has been recently found to be a general
phenomenon in isolated anisotropic spin systems. It sets a general framework to
understand the emergence of ferromagnetism in finite magnetic systems starting
from microscopic models without phenomenological on-site barriers. Here we
study ... | cond-mat.stat-mech cond-mat.mes-hall | topological phase space disconnection has been recently found to be a general phenomenon in isolated anisotropic spin systems it sets a general framework to understand the emergence of ferromagnetism in finite magnetic systems starting from microscopic models without phenomenological onsite barriers here we study its r... | [['topological', 'phase', 'space', 'disconnection', 'has', 'been', 'recently', 'found', 'to', 'be', 'a', 'general', 'phenomenon', 'in', 'isolated', 'anisotropic', 'spin', 'systems', 'it', 'sets', 'a', 'general', 'framework', 'to', 'understand', 'the', 'emergence', 'of', 'ferromagnetism', 'in', 'finite', 'magnetic', 'sy... | [-0.16284179787601338, 0.18619019291395333, -0.07062797319479794, 0.08053587908463768, -0.02694034396011864, -0.13440404228587338, 0.050735416308957705, 0.3845937958329308, -0.2520588375699269, -0.31087691831358133, 0.052882275089532846, -0.26814162980711254, -0.13098939986848812, 0.21339414420784736, 0.032937856245355... |
710.3936 | Improved Hardy-Sobolev inequalities | The main result includes features of a Hardy-type inequality and an
inequality of either Sobolev or Gagliardo-Nirenberg type. It is inspired by the
method of proof of a recent improved Sobolev inequality derived by M. Ledoux
which brings out the connection between Sobolev embeddings and heat kernel
bounds. Here Ledou... | math.SP math-ph math.MP | the main result includes features of a hardytype inequality and an inequality of either sobolev or gagliardonirenberg type it is inspired by the method of proof of a recent improved sobolev inequality derived by m ledoux which brings out the connection between sobolev embeddings and heat kernel bounds here ledouxs tech... | [['the', 'main', 'result', 'includes', 'features', 'of', 'a', 'hardytype', 'inequality', 'and', 'an', 'inequality', 'of', 'either', 'sobolev', 'or', 'gagliardonirenberg', 'type', 'it', 'is', 'inspired', 'by', 'the', 'method', 'of', 'proof', 'of', 'a', 'recent', 'improved', 'sobolev', 'inequality', 'derived', 'by', 'm',... | [-0.10498380504089268, 0.017916106263515284, -0.09130458815712227, 0.07631841167003835, -0.11293156864759449, -0.16850644142736923, 0.06147967737920786, 0.2777003034030738, -0.33094087365555436, -0.2698459941869895, 0.14040405040428247, -0.31594104465250283, -0.11466868706876794, 0.24379170294978644, -0.083451965996000... |
710.3937 | An Analytic Proof of the Matrix Spectral Factorization Theorem | An analytic proof is proposed of Wiener's theorem on factorization of
positive definite matrix-functions.
| math.CV | an analytic proof is proposed of wieners theorem on factorization of positive definite matrixfunctions | [['an', 'analytic', 'proof', 'is', 'proposed', 'of', 'wieners', 'theorem', 'on', 'factorization', 'of', 'positive', 'definite', 'matrixfunctions']] | [-0.17724950505154474, -0.07369319325308814, -0.25142951495945454, 0.09261592481717733, -0.15005841252527066, -0.1755420227668115, -0.029090940952301025, 0.2769841293671301, -0.19388012002621377, -0.0969241853537304, 0.10534997031624828, -0.24447938533765928, -0.1644378025084734, 0.23823046178690024, -0.109437410054462... |
710.3938 | Multiplicity Fluctuations in Limited Segments of Momentum Space in
Statistical Models | Multiplicity fluctuations in limited segments of momentum space are
calculated for a classical pion gas within the statistical model. Results for
the grand canonical, canonical, and micro-canonical ensemble are obtained,
compared and discussed. We demonstrate that even in the large volume limit
correlations between m... | nucl-th | multiplicity fluctuations in limited segments of momentum space are calculated for a classical pion gas within the statistical model results for the grand canonical canonical and microcanonical ensemble are obtained compared and discussed we demonstrate that even in the large volume limit correlations between macroscop... | [['multiplicity', 'fluctuations', 'in', 'limited', 'segments', 'of', 'momentum', 'space', 'are', 'calculated', 'for', 'a', 'classical', 'pion', 'gas', 'within', 'the', 'statistical', 'model', 'results', 'for', 'the', 'grand', 'canonical', 'canonical', 'and', 'microcanonical', 'ensemble', 'are', 'obtained', 'compared', ... | [-0.07775220820645909, 0.21114414352847294, -0.14996792047406685, 0.15612841922728743, 0.027077313176676877, -0.07189075013653176, 0.013293992300502589, 0.3109292316281038, -0.1903521418247036, -0.30664175849591124, -0.013555609683132136, -0.3377959613428741, -0.016033123722528946, 0.15778225142371338, 0.00443596878951... |
710.3939 | Rotational symmetry breaking in baby Skyrme models | We consider multisolitons with charges 1 =< B =< 5 in the baby Skyrme model
for the one-parametric family of potentials U=\mu^2 (1-\phi_3)^s with 0<s =< 4.
This class of potentials is a generalization of the `old' (s=1) and
`holomorphic' (s=4) baby Skyrme models. We find that for charge one, stable
solutions exist fo... | hep-th | we consider multisolitons with charges 1 b 5 in the baby skyrme model for the oneparametric family of potentials umu2 1phi_3s with 0s 4 this class of potentials is a generalization of the old s1 and holomorphic s4 baby skyrme models we find that for charge one stable solutions exist for every value of s and they are ro... | [['we', 'consider', 'multisolitons', 'with', 'charges', '1', 'b', '5', 'in', 'the', 'baby', 'skyrme', 'model', 'for', 'the', 'oneparametric', 'family', 'of', 'potentials', 'umu2', '1phi_3s', 'with', '0s', '4', 'this', 'class', 'of', 'potentials', 'is', 'a', 'generalization', 'of', 'the', 'old', 's1', 'and', 'holomorphi... | [-0.16294548787921667, 0.17237720640748738, -0.00854234192892909, 0.10913434591982514, -0.006491115272045135, -0.1919731530211866, 0.011739580884575844, 0.35107786241173744, -0.20086755614727736, -0.2881956641972065, 0.08761607811134309, -0.3181843619579449, -0.06141319442167878, 0.10251055193692446, -0.000958998276153... |
710.394 | A classical picture of the role of vacancies and interstitials in
Helium-4 | Motivated by experimental hints for supersolidity in Helium-4, we perform
Monte Carlo simulations of vacancies and interstitials in a classical two-and
three-dimensional Lennard-Jones solid. We confirm a strong binding energy of
vacancies which is of the order of Lennard-Jones attraction. This is
reminiscent of what ... | cond-mat.other | motivated by experimental hints for supersolidity in helium4 we perform monte carlo simulations of vacancies and interstitials in a classical twoand threedimensional lennardjones solid we confirm a strong binding energy of vacancies which is of the order of lennardjones attraction this is reminiscent of what has been f... | [['motivated', 'by', 'experimental', 'hints', 'for', 'supersolidity', 'in', 'helium4', 'we', 'perform', 'monte', 'carlo', 'simulations', 'of', 'vacancies', 'and', 'interstitials', 'in', 'a', 'classical', 'twoand', 'threedimensional', 'lennardjones', 'solid', 'we', 'confirm', 'a', 'strong', 'binding', 'energy', 'of', 'v... | [-0.103161312174052, 0.1824305651915403, -0.08569575555156916, 0.08401552551591661, 0.04433920914799763, -0.05330557065406957, 0.07040596332696553, 0.38998473337135064, -0.24271262250840664, -0.3017420948286039, -0.037918116590634994, -0.32522507031591463, -0.13534197933264436, 0.10284710241607033, 0.03659160625046262,... |
710.3941 | Solutions of Nuclear Pairing | We give the exact solution of orbit dependent nuclear pairing problem between
two non-degenerate energy levels using the Bethe ansatz technique. Our solution
reduces to previously solved cases in the appropriate limits including
Richardson's treatment of reduced pairing in terms of rational Gaudin algebra
operators.
| nucl-th | we give the exact solution of orbit dependent nuclear pairing problem between two nondegenerate energy levels using the bethe ansatz technique our solution reduces to previously solved cases in the appropriate limits including richardsons treatment of reduced pairing in terms of rational gaudin algebra operators | [['we', 'give', 'the', 'exact', 'solution', 'of', 'orbit', 'dependent', 'nuclear', 'pairing', 'problem', 'between', 'two', 'nondegenerate', 'energy', 'levels', 'using', 'the', 'bethe', 'ansatz', 'technique', 'our', 'solution', 'reduces', 'to', 'previously', 'solved', 'cases', 'in', 'the', 'appropriate', 'limits', 'incl... | [-0.1718714814633131, 0.031956167332828044, -0.07092071259394288, 0.12749627699247665, -0.0877818873617798, -0.16749067692500022, 0.07796616846074661, 0.28453789891468156, -0.2699560054577887, -0.2758057463500235, 0.03909639111306104, -0.221902358573344, -0.10300583983254101, 0.20816219473878542, 0.005711444550090366, ... |
710.3942 | Bottom Baryon Decays in Non-relativistic Quark Model | The reactions $\Sigma_b^* \to \Lambda_b \pi$, $\Sigma_b \to \Lambda_b \pi$,
and $\Xi_b^* \to \Xi_b \pi$ are studied in the $^3P_0$ non-relativistic quark
model with all the model parameters fixed in the sector of light quarks. The
theoretical predictions for the decay widths $\Gamma_{\Sigma_b^* \to \Lambda_b
\pi}$ an... | hep-ph | the reactions sigma_b to lambda_b pi sigma_b to lambda_b pi and xi_b to xi_b pi are studied in the 3p_0 nonrelativistic quark model with all the model parameters fixed in the sector of light quarks the theoretical predictions for the decay widths gamma_sigma_b to lambda_b pi and gamma_sigma_b to lambda_b pi are consist... | [['the', 'reactions', 'sigma_b', 'to', 'lambda_b', 'pi', 'sigma_b', 'to', 'lambda_b', 'pi', 'and', 'xi_b', 'to', 'xi_b', 'pi', 'are', 'studied', 'in', 'the', '3p_0', 'nonrelativistic', 'quark', 'model', 'with', 'all', 'the', 'model', 'parameters', 'fixed', 'in', 'the', 'sector', 'of', 'light', 'quarks', 'the', 'theoret... | [-0.04398266755436596, 0.31046872040812895, -0.09055674750880714, 0.11685815087740163, -0.05549964069908591, -0.1263081625904561, 0.11056410468013941, 0.30721879230910226, -0.19452021293456487, -0.2167225319957524, -0.09484758681266389, -0.3769350864417982, 0.09001204397390482, 0.05932072059684351, 0.1047925602464953, ... |
710.3943 | Change of strength of vortex pinning in YBCO due to BaZrO_3 inclusions | We probe the short-range pinning properties with the application of microwave
currents at very high driving frequencies (47.7 GHz) on
YBa$_2$Cu$_3$O$_{7-\delta}$ films with and without sub-micrometer BaZrO$_3$
inclusions. We explore the temperature and field ranges 60 K$<T<T_c$ and
0$<\mu_0H<$0.8 T, with the field ap... | cond-mat.supr-con cond-mat.mtrl-sci | we probe the shortrange pinning properties with the application of microwave currents at very high driving frequencies 477 ghz on yba_2cu_3o_7delta films with and without submicrometer bazro_3 inclusions we explore the temperature and field ranges 60 ktt_c and 0mu_0h08 t with the field applied along the caxis the magne... | [['we', 'probe', 'the', 'shortrange', 'pinning', 'properties', 'with', 'the', 'application', 'of', 'microwave', 'currents', 'at', 'very', 'high', 'driving', 'frequencies', '477', 'ghz', 'on', 'yba_2cu_3o_7delta', 'films', 'with', 'and', 'without', 'submicrometer', 'bazro_3', 'inclusions', 'we', 'explore', 'the', 'tempe... | [-0.14638659483329816, 0.2134178804544111, -0.002156985051591288, -0.012128406006024417, -0.03911522824994542, -0.12476284634886366, 0.05239526551696613, 0.3912629179374287, -0.24156789365930087, -0.33287433989691745, 0.03678863626476166, -0.3031344617660524, -0.06092606116594239, 0.19404326469044794, 0.021785856664858... |
710.3944 | Crystallographic modelling of protein loops and their heterogeneity with
Rappertk | Background. All-atom crystallographic refinement of proteins is a laborious
manually driven procedure, as a result of which, alternative and multiconformer
interpretations are not routinely investigated.
Results. We describe efficient loop sampling procedures in Rappertk and
demonstrate that single loops in protein... | q-bio.BM | background allatom crystallographic refinement of proteins is a laborious manually driven procedure as a result of which alternative and multiconformer interpretations are not routinely investigated results we describe efficient loop sampling procedures in rappertk and demonstrate that single loops in proteins can be a... | [['background', 'allatom', 'crystallographic', 'refinement', 'of', 'proteins', 'is', 'a', 'laborious', 'manually', 'driven', 'procedure', 'as', 'a', 'result', 'of', 'which', 'alternative', 'and', 'multiconformer', 'interpretations', 'are', 'not', 'routinely', 'investigated', 'results', 'we', 'describe', 'efficient', 'l... | [-0.08057735376035415, 0.11273622797297078, -0.06554081148638481, 0.10156968451747803, -0.05111664650358365, -0.16594527293862382, 0.050576664140106926, 0.46347124161015096, -0.2348969848400218, -0.3536962063484628, 0.0682104461077063, -0.22545712624519118, -0.17460449941662914, 0.189323010014921, -0.06975770666605045,... |
710.3945 | Pinning down the New Minimal Supersymmetric GUT | We show that generic $ {\bf{10\oplus 120\oplus {\bar {126}}}}$ fits of
fermion masses and mixings, using real superpotential couplings but with
complex `Higgs fractions' leading to complex yukawa couplings in the effective
MSSM, \emph{overdetermine}(by one extra constraint) the superpotential
parameters of the New Mi... | hep-ph | we show that generic bf10oplus 120oplus bar 126 fits of fermion masses and mixings using real superpotential couplings but with complex higgs fractions leading to complex yukawa couplings in the effective mssm emphoverdetermineby one extra constraint the superpotential parameters of the new minimal supersymmetric so10 ... | [['we', 'show', 'that', 'generic', 'bf10oplus', '120oplus', 'bar', '126', 'fits', 'of', 'fermion', 'masses', 'and', 'mixings', 'using', 'real', 'superpotential', 'couplings', 'but', 'with', 'complex', 'higgs', 'fractions', 'leading', 'to', 'complex', 'yukawa', 'couplings', 'in', 'the', 'effective', 'mssm', 'emphoverdet... | [-0.1026766045665956, 0.2017436441474152, -0.028571201428996038, 0.16700241862930632, -0.1384555719474068, -0.2075155760976486, 0.06528619817151819, 0.2800140252068089, -0.21646888284856491, -0.35324376158341264, 0.07850602368789807, -0.21986510403041773, -0.0713559713385743, 0.12654776402574108, -0.015276285717748231,... |
710.3946 | Search for Supersymmetry in Di-Photon Final States at sqrt{s} = 1.96 TeV | We report results of a search for supersymmetry (SUSY) with gauge-mediated
symmetry breaking in di-photon events collected by the D0 experiment at the
Fermilab Tevatron Collider in 2002--2006. In 1.1 fb$^{-1}$ of data, we find no
significant excess beyond the background expected from the standard model and
set the mo... | hep-ex | we report results of a search for supersymmetry susy with gaugemediated symmetry breaking in diphoton events collected by the d0 experiment at the fermilab tevatron collider in 20022006 in 11 fb1 of data we find no significant excess beyond the background expected from the standard model and set the most stringent lowe... | [['we', 'report', 'results', 'of', 'a', 'search', 'for', 'supersymmetry', 'susy', 'with', 'gaugemediated', 'symmetry', 'breaking', 'in', 'diphoton', 'events', 'collected', 'by', 'the', 'd0', 'experiment', 'at', 'the', 'fermilab', 'tevatron', 'collider', 'in', '20022006', 'in', '11', 'fb1', 'of', 'data', 'we', 'find', '... | [-0.03705975352846957, 0.18824515794706229, -0.006408920581150171, 0.20185324181983996, -0.06259989003384751, -0.14974325777986994, 0.10679377245341802, 0.3208753942094695, -0.10048726287688577, -0.4201578511916972, 0.048376307842418455, -0.3852915756960774, 0.10311597005718133, 0.18277366487037197, 0.06392027956793424... |
710.3947 | First Eigenvalues of Geometric Operators under the Ricci Flow | In this paper, we prove that the first eigenvalues of $-\Delta + cR$ ($c\geq
\frac14$) is nondecreasing under the Ricci flow. We also prove the monotonicity
under the normalized flow for the case $c=1/4$, and $r\le 0$.
| math.DG | in this paper we prove that the first eigenvalues of delta cr cgeq frac14 is nondecreasing under the ricci flow we also prove the monotonicity under the normalized flow for the case c14 and rle 0 | [['in', 'this', 'paper', 'we', 'prove', 'that', 'the', 'first', 'eigenvalues', 'of', 'delta', 'cr', 'cgeq', 'frac14', 'is', 'nondecreasing', 'under', 'the', 'ricci', 'flow', 'we', 'also', 'prove', 'the', 'monotonicity', 'under', 'the', 'normalized', 'flow', 'for', 'the', 'case', 'c14', 'and', 'rle', '0']] | [-0.21179113945820266, 0.11078626987808901, -0.03774071355453796, 0.04079662263393402, 0.014939539651903842, -0.1731692532905274, -0.03441476606854445, 0.36636973751915825, -0.3168746916991141, -0.12503724643546674, 0.10451844234679204, -0.32271629437390303, -0.1599419779765109, 0.12396816588524315, -0.0849128134755624... |
710.3948 | RNA sampling and crystallographic refinement using Rappertk | Background. Dramatic increases in RNA structural data have made it possible
to recognize its conformational preferences much better than a decade ago. This
has created an opportunity to use discrete restraint-based conformational
sampling for modelling RNA and automating its crystallographic refinement.
Results. All-... | q-bio.BM | background dramatic increases in rna structural data have made it possible to recognize its conformational preferences much better than a decade ago this has created an opportunity to use discrete restraintbased conformational sampling for modelling rna and automating its crystallographic refinement results allatom sam... | [['background', 'dramatic', 'increases', 'in', 'rna', 'structural', 'data', 'have', 'made', 'it', 'possible', 'to', 'recognize', 'its', 'conformational', 'preferences', 'much', 'better', 'than', 'a', 'decade', 'ago', 'this', 'has', 'created', 'an', 'opportunity', 'to', 'use', 'discrete', 'restraintbased', 'conformation... | [-0.093606812763534, 0.11276715731314059, -0.09409538107195302, 0.0640522793932494, -0.0979939867377929, -0.1696332663864545, 0.06638200368894183, 0.4675064566990604, -0.28601587257631444, -0.3169011427656464, 0.006400410860331486, -0.20514374286057832, -0.15062376481339174, 0.18952575331634802, -0.0462184256469102, 0.... |
710.3949 | A note on pairs of metrics in a two-dimensional linear vector space | Pairs of metrics in a two-dimensional linear vector space are considered, one
of which is a Minkowski type metric. Their simultaneous diagonalizability is
studied and canonical presentations for them are suggested.
| math.MG | pairs of metrics in a twodimensional linear vector space are considered one of which is a minkowski type metric their simultaneous diagonalizability is studied and canonical presentations for them are suggested | [['pairs', 'of', 'metrics', 'in', 'a', 'twodimensional', 'linear', 'vector', 'space', 'are', 'considered', 'one', 'of', 'which', 'is', 'a', 'minkowski', 'type', 'metric', 'their', 'simultaneous', 'diagonalizability', 'is', 'studied', 'and', 'canonical', 'presentations', 'for', 'them', 'are', 'suggested']] | [-0.19677008922782638, 0.12168745650729586, -0.0237112574038967, 0.14120152890832433, -0.11015582264911744, -0.15183701014686976, -0.03072259938644786, 0.40434445140342556, -0.23927887913680845, -0.19584244429584471, 0.09140795927059146, -0.29081820585434476, -0.14726487913679692, 0.19968070858909237, -0.04063527992806... |
710.395 | Geometric phase gate on an optical transition for ion trap quantum
computation | We propose a geometric phase gate of two ion qubits that are encoded in two
levels linked by an optical dipole-forbidden transition. Compared to hyperfine
geometric phase gates mediated by electric dipole transitions, the gate has
many interesting properties, such as very low spontaneous emission rates,
applicability... | quant-ph | we propose a geometric phase gate of two ion qubits that are encoded in two levels linked by an optical dipoleforbidden transition compared to hyperfine geometric phase gates mediated by electric dipole transitions the gate has many interesting properties such as very low spontaneous emission rates applicability to mag... | [['we', 'propose', 'a', 'geometric', 'phase', 'gate', 'of', 'two', 'ion', 'qubits', 'that', 'are', 'encoded', 'in', 'two', 'levels', 'linked', 'by', 'an', 'optical', 'dipoleforbidden', 'transition', 'compared', 'to', 'hyperfine', 'geometric', 'phase', 'gates', 'mediated', 'by', 'electric', 'dipole', 'transitions', 'the... | [-0.1648160164362528, 0.25408962609522656, 0.023513811325628152, 0.04214698439595145, 0.02009798980868933, -0.20117057323403342, 0.07447759851708378, 0.45889926880178317, -0.2071129920577604, -0.32070047723155626, 0.014978045864935808, -0.22997663806632823, -0.08590010655666767, 0.22224670117327444, -0.0219210826211385... |
710.3951 | Nonlinear elasticity of composite networks of stiff biopolymers with
flexible linkers | Motivated by recent experiments showing nonlinear elasticity of in vitro
networks of the biopolymer actin cross-linked with filamin, we present an
effective medium theory of flexibly cross-linked stiff polymer networks. We
model such networks by randomly oriented elastic rods connected by flexible
connectors to a sur... | cond-mat.soft | motivated by recent experiments showing nonlinear elasticity of in vitro networks of the biopolymer actin crosslinked with filamin we present an effective medium theory of flexibly crosslinked stiff polymer networks we model such networks by randomly oriented elastic rods connected by flexible connectors to a surroundi... | [['motivated', 'by', 'recent', 'experiments', 'showing', 'nonlinear', 'elasticity', 'of', 'in', 'vitro', 'networks', 'of', 'the', 'biopolymer', 'actin', 'crosslinked', 'with', 'filamin', 'we', 'present', 'an', 'effective', 'medium', 'theory', 'of', 'flexibly', 'crosslinked', 'stiff', 'polymer', 'networks', 'we', 'model... | [-0.13301792198104695, 0.17600413724115546, -0.062100849291753205, -0.059258129415822966, -0.04683350669386398, -0.17017825993908836, -0.0016596685593304713, 0.4287544739698725, -0.3117747563491797, -0.22616429528265836, -0.009332571719174407, -0.27354474736022805, -0.25238759438729, 0.09655109923222058, 0.011268355379... |
710.3952 | The fractional stochastic heat equation on the circle: Time regularity
and potential theory | We consider a system of $d$ linear stochastic heat equations driven by an
additive infinite-dimensional fractional Brownian noise on the unit circle
$S^1$. We obtain sharp results on the H\"older continuity in time of the paths
of the solution $u=\{u(t, x)\}_{t \in \mathbb{R}_+, x \in S^1}$. We then
establish upper a... | math.PR | we consider a system of d linear stochastic heat equations driven by an additive infinitedimensional fractional brownian noise on the unit circle s1 we obtain sharp results on the holder continuity in time of the paths of the solution uut x_t in mathbbr_ x in s1 we then establish upper and lower bounds on hitting proba... | [['we', 'consider', 'a', 'system', 'of', 'd', 'linear', 'stochastic', 'heat', 'equations', 'driven', 'by', 'an', 'additive', 'infinitedimensional', 'fractional', 'brownian', 'noise', 'on', 'the', 'unit', 'circle', 's1', 'we', 'obtain', 'sharp', 'results', 'on', 'the', 'holder', 'continuity', 'in', 'time', 'of', 'the', ... | [-0.16614521844243046, 0.09732650415194326, -0.02507033193164241, 0.0460955956672777, -0.009158265401623141, -0.11200318807291228, 0.11175631762329322, 0.3570150658627277, -0.2959425191242081, -0.18080755922276137, 0.13460186468576318, -0.3207559756267427, -0.07746407626294044, 0.22109956868382089, -0.13313647476372434... |
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