id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
709.4335 | Localization of an impurity particle on a boson Mott insulator
background | We investigate the behavior of a single particle hopping on a three
dimensional cubic optical lattice in the presence of a Mott insulator of bosons
in the same lattice. We calculate the critical interaction strength between the
impurity and background bosons, beyond which there is bound state (polaron)
formation. We ... | cond-mat.other | we investigate the behavior of a single particle hopping on a three dimensional cubic optical lattice in the presence of a mott insulator of bosons in the same lattice we calculate the critical interaction strength between the impurity and background bosons beyond which there is bound state polaron formation we give ex... | [['we', 'investigate', 'the', 'behavior', 'of', 'a', 'single', 'particle', 'hopping', 'on', 'a', 'three', 'dimensional', 'cubic', 'optical', 'lattice', 'in', 'the', 'presence', 'of', 'a', 'mott', 'insulator', 'of', 'bosons', 'in', 'the', 'same', 'lattice', 'we', 'calculate', 'the', 'critical', 'interaction', 'strength'... | [-0.16154593310784549, 0.2323259402462729, -0.051296223140805244, 0.09847094284486957, 0.013332768688157488, -0.18549421323069298, 0.10892270453489171, 0.37594811668476236, -0.20265624723665845, -0.22472503137004635, 0.007298217362124258, -0.32960164231749683, -0.11271899422102322, 0.10052570876723621, 0.06665551255439... |
709.4336 | Universal properties of the confining string in the random percolation
model | Random percolation can be fully interpreted as a confining pure gauge theory.
With numerical high-precision measurements of Polyakov-Polyakov correlators at
finite temperature, we could well observe the presence of shape effects due to
rough fluctuations of the confining string, in complete agreement with the
univers... | hep-lat | random percolation can be fully interpreted as a confining pure gauge theory with numerical highprecision measurements of polyakovpolyakov correlators at finite temperature we could well observe the presence of shape effects due to rough fluctuations of the confining string in complete agreement with the universality p... | [['random', 'percolation', 'can', 'be', 'fully', 'interpreted', 'as', 'a', 'confining', 'pure', 'gauge', 'theory', 'with', 'numerical', 'highprecision', 'measurements', 'of', 'polyakovpolyakov', 'correlators', 'at', 'finite', 'temperature', 'we', 'could', 'well', 'observe', 'the', 'presence', 'of', 'shape', 'effects', ... | [-0.08134580527432263, 0.23790004612877966, -0.11162910032318905, 0.05028661478310823, -0.02696268688887358, -0.10786620625294745, 0.01952986677410081, 0.3492765722051263, -0.21850031981244683, -0.3035252641141415, 0.05412552748573944, -0.31677726870402695, -0.07033172403462232, 0.08685372414067388, -0.0055379860289394... |
709.4337 | Gravitation, Cosmology and Space-Time Torsion | Poincar\'e gauge theory of gravity offers opportunities to solve some
principal problems of general relativity theory and modern cosmology. In the
frame of this theory the gravitational interaction can have the repulsion
character in the case of usual gravitating matter with positive values of
energy density and pres... | gr-qc | poincare gauge theory of gravity offers opportunities to solve some principal problems of general relativity theory and modern cosmology in the frame of this theory the gravitational interaction can have the repulsion character in the case of usual gravitating matter with positive values of energy density and pressure ... | [['poincare', 'gauge', 'theory', 'of', 'gravity', 'offers', 'opportunities', 'to', 'solve', 'some', 'principal', 'problems', 'of', 'general', 'relativity', 'theory', 'and', 'modern', 'cosmology', 'in', 'the', 'frame', 'of', 'this', 'theory', 'the', 'gravitational', 'interaction', 'can', 'have', 'the', 'repulsion', 'cha... | [-0.19317897660309605, 0.11815194809965998, -0.11538370540441736, 0.11766273009799699, -0.09036943191122786, -0.15455070387345748, -0.1008399012759676, 0.27364610429748754, -0.25104042940781773, -0.2931339420099682, 0.03200596672260838, -0.24822445626361905, -0.10297941310313817, 0.12295263368314324, 0.0015259178303112... |
709.4338 | Decay of Scalar Condensation in Quantum Field Theory | We consider decay processes of scalar-field condensation in the framework of
well-established quantum field theory. We postulate that the quantum state
corresponding to the scalar-field condensation is so-called coherent state with
discussing the validity of such a treatment. We show that, by using the
unitarity rela... | hep-ph | we consider decay processes of scalarfield condensation in the framework of wellestablished quantum field theory we postulate that the quantum state corresponding to the scalarfield condensation is socalled coherent state with discussing the validity of such a treatment we show that by using the unitarity relation of t... | [['we', 'consider', 'decay', 'processes', 'of', 'scalarfield', 'condensation', 'in', 'the', 'framework', 'of', 'wellestablished', 'quantum', 'field', 'theory', 'we', 'postulate', 'that', 'the', 'quantum', 'state', 'corresponding', 'to', 'the', 'scalarfield', 'condensation', 'is', 'socalled', 'coherent', 'state', 'with'... | [-0.08047480426000383, 0.17999385474838017, -0.09688697151121341, 0.1144116832019013, -0.004966653113325055, -0.1165324668917391, 0.05603493305229638, 0.30893389805036986, -0.23398580527307195, -0.21298047083899632, 0.050211087950807795, -0.26797305391783005, -0.12685212935918036, 0.1795978393011655, 0.0722318597726969... |
709.4339 | Transference of bilinear multiplier operators on Lorentz spaces | We prove a DeLeeuw type theorem of transference of boundedness for modulation
invariant multiplier operators between the groups defined by the real line and
the torus.
| math.CA | we prove a deleeuw type theorem of transference of boundedness for modulation invariant multiplier operators between the groups defined by the real line and the torus | [['we', 'prove', 'a', 'deleeuw', 'type', 'theorem', 'of', 'transference', 'of', 'boundedness', 'for', 'modulation', 'invariant', 'multiplier', 'operators', 'between', 'the', 'groups', 'defined', 'by', 'the', 'real', 'line', 'and', 'the', 'torus']] | [-0.21256284769624473, 0.07329539928585291, -0.06021445261314511, 0.1160182799398899, -0.04353644453920424, -0.1275697953812778, 0.06269173055887223, 0.30277719736099246, -0.31605941712856295, -0.2188183630257845, 0.1400968643836677, -0.21275386376306415, -0.10989348914474249, 0.24742393324151635, -0.09007642220705747,... |
709.434 | Pyrolysis of secondary raw material from used frying oils | A totally green chemistry alternative that would lead both to energy
production from renewable feedstocks and to solutions of parts of ecological
problems related to waste disposals would be very attractive. Pyrolysis of used
frying oils seems to be one option for this attractive alternative as we
propose to demonstr... | physics.chem-ph | a totally green chemistry alternative that would lead both to energy production from renewable feedstocks and to solutions of parts of ecological problems related to waste disposals would be very attractive pyrolysis of used frying oils seems to be one option for this attractive alternative as we propose to demonstrate... | [['a', 'totally', 'green', 'chemistry', 'alternative', 'that', 'would', 'lead', 'both', 'to', 'energy', 'production', 'from', 'renewable', 'feedstocks', 'and', 'to', 'solutions', 'of', 'parts', 'of', 'ecological', 'problems', 'related', 'to', 'waste', 'disposals', 'would', 'be', 'very', 'attractive', 'pyrolysis', 'of',... | [-0.010482826227054378, 0.14033592224411695, -0.02583516528632989, 0.012908893381332965, -0.012494866165535566, -0.13055789035165513, 0.07861638996361482, 0.36658247608579414, -0.21548010494395448, -0.3189881926138108, 0.0918271181316297, -0.30255675619762196, -0.02737718539512051, 0.15590848719886735, -0.0689953373573... |
709.4341 | On three approaches to conjugacy in semigroups | We compare three approaches to the notion of conjugacy for semigroups, the
first one via the transitive closure of the $uv\sim vu$ relation, the second
one via an action of inverse semigroups on themselves by partial
transformations, and the third one via characters of finite-dimensional
representations.
| math.GR | we compare three approaches to the notion of conjugacy for semigroups the first one via the transitive closure of the uvsim vu relation the second one via an action of inverse semigroups on themselves by partial transformations and the third one via characters of finitedimensional representations | [['we', 'compare', 'three', 'approaches', 'to', 'the', 'notion', 'of', 'conjugacy', 'for', 'semigroups', 'the', 'first', 'one', 'via', 'the', 'transitive', 'closure', 'of', 'the', 'uvsim', 'vu', 'relation', 'the', 'second', 'one', 'via', 'an', 'action', 'of', 'inverse', 'semigroups', 'on', 'themselves', 'by', 'partial'... | [-0.094198913677879, 0.0979372097328609, -0.030364840615378773, 0.0769268505923126, -0.11019564610298561, -0.0655261543781861, 0.04503172702844376, 0.3053067857602044, -0.3893580037452605, -0.19923417816829422, 0.1438549136965657, -0.3448959929949563, -0.13451898146582686, 0.227887740176495, -0.03585082260162934, 0.046... |
709.4342 | A search for various double beta decay modes of tin isotopes | For the first time an extensive search for various double beta decay modes of
124Sn and 112Sn has been performed. A total exposure of 43.29 kg.days has been
accumulated. New half-life limits of 124Sn into excited states of 124Te have
been obtained; the lower half-life limit for the first excited 2+ state at
602.7keV ... | nucl-ex | for the first time an extensive search for various double beta decay modes of 124sn and 112sn has been performed a total exposure of 4329 kgdays has been accumulated new halflife limits of 124sn into excited states of 124te have been obtained the lower halflife limit for the first excited 2 state at 6027kev is t_12 31 ... | [['for', 'the', 'first', 'time', 'an', 'extensive', 'search', 'for', 'various', 'double', 'beta', 'decay', 'modes', 'of', '124sn', 'and', '112sn', 'has', 'been', 'performed', 'a', 'total', 'exposure', 'of', '4329', 'kgdays', 'has', 'been', 'accumulated', 'new', 'halflife', 'limits', 'of', '124sn', 'into', 'excited', 's... | [-0.04813212658309395, 0.2759636830992778, 0.007658624931519746, 0.09923690137506094, 0.08544438429844547, -0.11312954918314475, 0.14454895127586634, 0.30624205269411486, -0.10190096377715785, -0.30880814176689797, 0.1024164425440897, -0.32473362123874844, 0.10795661600807435, 0.21649306588520664, 0.13959758029426975, ... |
709.4343 | D0 - D0bar mixing: theory basics | I discuss how the novel experimental data on D0 - D0bar mixing can be
combined to provide information on the fundamental theoretical quantities
describing the mixing itself. I then discuss the theoretical impact of the new
data, focusing in particular on the MSSM.
| hep-ph | i discuss how the novel experimental data on d0 d0bar mixing can be combined to provide information on the fundamental theoretical quantities describing the mixing itself i then discuss the theoretical impact of the new data focusing in particular on the mssm | [['i', 'discuss', 'how', 'the', 'novel', 'experimental', 'data', 'on', 'd0', 'd0bar', 'mixing', 'can', 'be', 'combined', 'to', 'provide', 'information', 'on', 'the', 'fundamental', 'theoretical', 'quantities', 'describing', 'the', 'mixing', 'itself', 'i', 'then', 'discuss', 'the', 'theoretical', 'impact', 'of', 'the', ... | [-0.06137066872213923, 0.15293344748871668, -0.08428763057149592, 0.1047354438785641, -0.11823729019878167, -0.11383361391545761, 0.0878523116975668, 0.30144331768332494, -0.28629155253015814, -0.23735194888320707, 0.09702673528642793, -0.2977237368689939, -0.09401258904420372, 0.19018319173760356, -0.06266952676343776... |
709.4344 | Emergence of Scale-Free Syntax Networks | The evolution of human language allowed the efficient propagation of
nongenetic information, thus creating a new form of evolutionary change.
Language development in children offers the opportunity of exploring the
emergence of such complex communication system and provides a window to
understanding the transition fr... | q-bio.NC | the evolution of human language allowed the efficient propagation of nongenetic information thus creating a new form of evolutionary change language development in children offers the opportunity of exploring the emergence of such complex communication system and provides a window to understanding the transition from p... | [['the', 'evolution', 'of', 'human', 'language', 'allowed', 'the', 'efficient', 'propagation', 'of', 'nongenetic', 'information', 'thus', 'creating', 'a', 'new', 'form', 'of', 'evolutionary', 'change', 'language', 'development', 'in', 'children', 'offers', 'the', 'opportunity', 'of', 'exploring', 'the', 'emergence', 'o... | [-0.11705915385728023, 0.090631867638561, -0.10687090199026199, 0.09080455320109371, -0.1433813588080034, -0.12374481273212098, 0.062329900062560895, 0.36396383810680727, -0.27049644568105996, -0.3283804386875705, 0.055544727380290586, -0.227055842980118, -0.23869767631108016, 0.15677879398387207, -0.06521487853226031,... |
709.4345 | Three-frame Algorithm of Car Path Reconstruction from Airborne Traffic
Data | The airborne traffic monitoring system forms a novel technology of detecting
vehicle motion. An optical digital camera located on an airborne platform
produces a series of images which then are processed to recognized the fixed
vehicles. In this way the video data are converted into the time sequence of
frames contai... | physics.ins-det physics.data-an | the airborne traffic monitoring system forms a novel technology of detecting vehicle motion an optical digital camera located on an airborne platform produces a series of images which then are processed to recognized the fixed vehicles in this way the video data are converted into the time sequence of frames containing... | [['the', 'airborne', 'traffic', 'monitoring', 'system', 'forms', 'a', 'novel', 'technology', 'of', 'detecting', 'vehicle', 'motion', 'an', 'optical', 'digital', 'camera', 'located', 'on', 'an', 'airborne', 'platform', 'produces', 'a', 'series', 'of', 'images', 'which', 'then', 'are', 'processed', 'to', 'recognized', 't... | [-0.16180330906585555, 0.05194851108549259, -0.10303877075757639, 0.0030183262533342867, -0.048104674381282284, -0.13677060707672456, 0.030800068661762037, 0.4371056069498098, -0.26592502719940286, -0.3515118350683947, 0.10011518230796661, -0.26669156245417264, -0.11906590476788789, 0.22703212287242167, -0.108253583631... |
709.4346 | Flux Distribution in Superconducting Films with Holes | Flux penetration into type-II superconducing films is simulated for
transverse applied magnetic field and flux creep dynamics. The films contain
macroscopic, non-conducting holes and we suggest a new method to introduce the
holes in the simulation formalism. The method implies reconstruction of the
magnetic field cha... | cond-mat.supr-con | flux penetration into typeii superconducing films is simulated for transverse applied magnetic field and flux creep dynamics the films contain macroscopic nonconducting holes and we suggest a new method to introduce the holes in the simulation formalism the method implies reconstruction of the magnetic field change ins... | [['flux', 'penetration', 'into', 'typeii', 'superconducing', 'films', 'is', 'simulated', 'for', 'transverse', 'applied', 'magnetic', 'field', 'and', 'flux', 'creep', 'dynamics', 'the', 'films', 'contain', 'macroscopic', 'nonconducting', 'holes', 'and', 'we', 'suggest', 'a', 'new', 'method', 'to', 'introduce', 'the', 'h... | [-0.136052773418097, 0.17284491577080077, -0.051028800945844235, 0.06036944412290282, 0.00316364471752619, -0.07489275719644022, 0.03333198620947366, 0.39980175138748797, -0.19604599093730302, -0.3436467432100134, 0.030066289209290265, -0.2889189685493247, -0.06656285664594742, 0.2246934243996349, -0.039822938722695135... |
709.4347 | Boundedness from H^1 to L^1 of Riesz transforms on a Lie group of
exponential growth | Let $G$ be the Lie group given by the semidirect product of $R^2$ and $R^+$
endowed with the Riemannian symmetric space structure. Let $X_0, X_1, X_2$ be a
distinguished basis of left-invariant vector fields of the Lie algebra of $G$
and define the Laplacian $\Delta=-(X_0^2+X_1^2+X_2^2)$. In this paper we
consider th... | math.CA | let g be the lie group given by the semidirect product of r2 and r endowed with the riemannian symmetric space structure let x_0 x_1 x_2 be a distinguished basis of leftinvariant vector fields of the lie algebra of g and define the laplacian deltax_02x_12x_22 in this paper we consider the first order riesz transforms r... | [['let', 'g', 'be', 'the', 'lie', 'group', 'given', 'by', 'the', 'semidirect', 'product', 'of', 'r2', 'and', 'r', 'endowed', 'with', 'the', 'riemannian', 'symmetric', 'space', 'structure', 'let', 'x_0', 'x_1', 'x_2', 'be', 'a', 'distinguished', 'basis', 'of', 'leftinvariant', 'vector', 'fields', 'of', 'the', 'lie', 'al... | [-0.1610875861904565, 0.14211655681838795, -0.05568318495678962, 0.018277751123865267, -0.14147065217578214, -0.07884290542130415, -0.06440405994154778, 0.4006174195994984, -0.3639266052644472, -0.1463447626661129, 0.14225598052975588, -0.30191756904657396, -0.0946605559438467, 0.1304274861444244, -0.07441785847007924,... |
709.4348 | The Hall algebra of a cyclic quiver at $q=0$ | We show that the generic Hall algebra of nilpotent representations of an
oriented cycle specialised at $q=0$ is isomorphic to the generic extension
monoid in the sense of Reineke. This continues the work of Reineke.
| math.RT math.RA | we show that the generic hall algebra of nilpotent representations of an oriented cycle specialised at q0 is isomorphic to the generic extension monoid in the sense of reineke this continues the work of reineke | [['we', 'show', 'that', 'the', 'generic', 'hall', 'algebra', 'of', 'nilpotent', 'representations', 'of', 'an', 'oriented', 'cycle', 'specialised', 'at', 'q0', 'is', 'isomorphic', 'to', 'the', 'generic', 'extension', 'monoid', 'in', 'the', 'sense', 'of', 'reineke', 'this', 'continues', 'the', 'work', 'of', 'reineke']] | [-0.17486342000109809, 0.10581258239066561, -0.06492668998294643, -0.007976390639253492, -0.11099253946116992, -0.08224387647850173, -0.07971249861376627, 0.3289916721837861, -0.37877965355291965, -0.1451865378767252, 0.08565596645099244, -0.23310297195400512, -0.19329878709145953, 0.16643369269690345, -0.1969843513132... |
709.4349 | Bose-Einstein condensate in a harmonic trap with an eccentric dimple
potential | We investigate Bose-Einstein condensation of noninteracting gases in a
harmonic trap with an off-center dimple potential. We specifically consider the
case of a tight and deep dimple potential which is modelled by a point
interaction. This point interaction is represented by a Dirac delta function.
The atomic density... | quant-ph cond-mat.other | we investigate boseeinstein condensation of noninteracting gases in a harmonic trap with an offcenter dimple potential we specifically consider the case of a tight and deep dimple potential which is modelled by a point interaction this point interaction is represented by a dirac delta function the atomic density chemic... | [['we', 'investigate', 'boseeinstein', 'condensation', 'of', 'noninteracting', 'gases', 'in', 'a', 'harmonic', 'trap', 'with', 'an', 'offcenter', 'dimple', 'potential', 'we', 'specifically', 'consider', 'the', 'case', 'of', 'a', 'tight', 'and', 'deep', 'dimple', 'potential', 'which', 'is', 'modelled', 'by', 'a', 'point... | [-0.15454273417944442, 0.15735045706753373, -0.0495867953459556, 0.025670740006151736, 0.06494794855196331, -0.15230180834092805, 0.07499475887901075, 0.3866794306684185, -0.2342507149269049, -0.2518083577774264, -0.007168608876511555, -0.3026578922982554, -0.13660065035927235, 0.09900219083096631, 0.06026759434717934,... |
709.435 | Which 3-manifold groups are K\"ahler groups? | The question in the title, first raised by Goldman and Donaldson, was
partially answered by Reznikov. We give a complete answer, as follows: if G can
be realized as both the fundamental group of a closed 3-manifold and of a
compact K\"ahler manifold, then G must be finite, and thus belongs to the
well-known list of f... | math.AG math.GT | the question in the title first raised by goldman and donaldson was partially answered by reznikov we give a complete answer as follows if g can be realized as both the fundamental group of a closed 3manifold and of a compact kahler manifold then g must be finite and thus belongs to the wellknown list of finite subgrou... | [['the', 'question', 'in', 'the', 'title', 'first', 'raised', 'by', 'goldman', 'and', 'donaldson', 'was', 'partially', 'answered', 'by', 'reznikov', 'we', 'give', 'a', 'complete', 'answer', 'as', 'follows', 'if', 'g', 'can', 'be', 'realized', 'as', 'both', 'the', 'fundamental', 'group', 'of', 'a', 'closed', '3manifold'... | [-0.13825173342290023, 0.13295327608163157, -0.09257442779683818, 0.07233262124937027, -0.1593415530708929, -0.16211196177173406, 0.04802536318505493, 0.3323997334887584, -0.2881616017470757, -0.29704253165982664, 0.1279642144974787, -0.22117027764519057, -0.12235337096111228, 0.1812496103423958, -0.17647804470422368, ... |
709.4351 | Dissociation energy of the water dimer from Quantum Monte Carlo
calculations | We report a study of the electronic dissociation energy of the water dimer
using quantum Monte Carlo (QMC) techniques. We have performed variational
quantum Monte Carlo (VMC) and diffusion quantum Monte Carlo (DMC) calculations
of the electronic ground state of the water monomer and dimer using
all-electron and pseud... | cond-mat.other | we report a study of the electronic dissociation energy of the water dimer using quantum monte carlo qmc techniques we have performed variational quantum monte carlo vmc and diffusion quantum monte carlo dmc calculations of the electronic ground state of the water monomer and dimer using allelectron and pseudopotential... | [['we', 'report', 'a', 'study', 'of', 'the', 'electronic', 'dissociation', 'energy', 'of', 'the', 'water', 'dimer', 'using', 'quantum', 'monte', 'carlo', 'qmc', 'techniques', 'we', 'have', 'performed', 'variational', 'quantum', 'monte', 'carlo', 'vmc', 'and', 'diffusion', 'quantum', 'monte', 'carlo', 'dmc', 'calculatio... | [-0.05094653318366526, 0.13280593949010627, -0.05560044270762438, 0.07164347592257209, 0.06887194223032055, -0.1000452855450771, 0.09328450570638668, 0.4149255506294012, -0.1940351048726466, -0.35269792954715196, -0.027325154734538507, -0.32099519354054346, -0.0400644109294374, 0.14509660840543037, 0.09342345611596677,... |
709.4352 | Uniqueness of spacelike hypersurfaces with constant higher order mean
curvature in generalized Robertson-Walker spacetimes | In this paper we study the problem of uniqueness for spacelike hypersurfaces
with constant higher order mean curvature in generalized Robertson-Walker (GRW)
spacetimes. In particular, we consider the following question: Under what
conditions must a compact spacelike hypersurface with constant higher order
mean curvat... | math.DG math-ph math.MP | in this paper we study the problem of uniqueness for spacelike hypersurfaces with constant higher order mean curvature in generalized robertsonwalker grw spacetimes in particular we consider the following question under what conditions must a compact spacelike hypersurface with constant higher order mean curvature in a... | [['in', 'this', 'paper', 'we', 'study', 'the', 'problem', 'of', 'uniqueness', 'for', 'spacelike', 'hypersurfaces', 'with', 'constant', 'higher', 'order', 'mean', 'curvature', 'in', 'generalized', 'robertsonwalker', 'grw', 'spacetimes', 'in', 'particular', 'we', 'consider', 'the', 'following', 'question', 'under', 'what... | [-0.17781644501838456, 0.10829819994365464, -0.10560267146551207, 0.12592163094805994, -0.10012129153219167, -0.13757926062942388, -0.05841348178846908, 0.36101938417872015, -0.19700633533550113, -0.1629227680687824, 0.11425447527298264, -0.23270057188870197, -0.15385338863922973, 0.12264497580236933, -0.14583496589297... |
709.4353 | Bayesian Nash Equilibria and Bell Inequalities | Games with incomplete information are formulated in a multi-sector
probability matrix formalism that can cope with quantum as well as classical
strategies. An analysis of classical and quantum strategy in a multi-sector
extension of the game of Battle of Sexes clarifies the two distinct roles of
nonlocal strategies, ... | quant-ph | games with incomplete information are formulated in a multisector probability matrix formalism that can cope with quantum as well as classical strategies an analysis of classical and quantum strategy in a multisector extension of the game of battle of sexes clarifies the two distinct roles of nonlocal strategies and es... | [['games', 'with', 'incomplete', 'information', 'are', 'formulated', 'in', 'a', 'multisector', 'probability', 'matrix', 'formalism', 'that', 'can', 'cope', 'with', 'quantum', 'as', 'well', 'as', 'classical', 'strategies', 'an', 'analysis', 'of', 'classical', 'and', 'quantum', 'strategy', 'in', 'a', 'multisector', 'exte... | [-0.11138015405844841, 0.0986058334144503, -0.1214428463978554, 0.13005993069052252, -0.01324371627789102, -0.22253346190885154, 0.0849836374626064, 0.32660697700817193, -0.27187799946211694, -0.3004778103847335, 0.07087647267130774, -0.23741252853799222, -0.21787969471970156, 0.11356536463709242, -0.11634810446455741,... |
709.4354 | Two-proton correlation function: a gentle introduction | The recent COSY-11 collaboration measurement of the two-proton correlation
function in the pp -> ppeta reaction, reported at this meeting [1], arouse some
interest in a simple theoretical description of the correlation function. In
these notes we present a pedagogical introduction to the practical methods that
can be... | hep-ph | the recent cosy11 collaboration measurement of the twoproton correlation function in the pp ppeta reaction reported at this meeting 1 arouse some interest in a simple theoretical description of the correlation function in these notes we present a pedagogical introduction to the practical methods that can be used for ca... | [['the', 'recent', 'cosy11', 'collaboration', 'measurement', 'of', 'the', 'twoproton', 'correlation', 'function', 'in', 'the', 'pp', 'ppeta', 'reaction', 'reported', 'at', 'this', 'meeting', '1', 'arouse', 'some', 'interest', 'in', 'a', 'simple', 'theoretical', 'description', 'of', 'the', 'correlation', 'function', 'in... | [-0.059471824751147685, 0.07920568520730396, -0.14097623094391376, 0.11943961090171042, -0.01008207904491222, -0.08861672221067941, 0.008571664811516146, 0.3384609250307856, -0.20212807373653324, -0.28944655033355615, -0.00858723856113359, -0.3351398684295281, -0.13737054613752747, 0.16842017958889594, 0.00994120875619... |
709.4355 | Agent Simulation of Chain Bankruptcy | We have conducted an agent-based simulation of chain bankruptcy. The
propagation of credit risk on a network, i.e., chain bankruptcy, is the key to
nderstanding largesized bankruptcies. In our model, decrease of revenue by the
loss of accounts payable is modeled by an interaction term, and bankruptcy is
defined as a ... | q-fin.GN physics.soc-ph | we have conducted an agentbased simulation of chain bankruptcy the propagation of credit risk on a network ie chain bankruptcy is the key to nderstanding largesized bankruptcies in our model decrease of revenue by the loss of accounts payable is modeled by an interaction term and bankruptcy is defined as a capital defi... | [['we', 'have', 'conducted', 'an', 'agentbased', 'simulation', 'of', 'chain', 'bankruptcy', 'the', 'propagation', 'of', 'credit', 'risk', 'on', 'a', 'network', 'ie', 'chain', 'bankruptcy', 'is', 'the', 'key', 'to', 'nderstanding', 'largesized', 'bankruptcies', 'in', 'our', 'model', 'decrease', 'of', 'revenue', 'by', 't... | [-0.12439425102197246, 0.04067673876373651, -0.01591617268565883, 0.10714440781057963, -0.04982160744615472, -0.14064953051921394, 0.11958417581378394, 0.4023698154741373, -0.2540715655041301, -0.31231993549845666, 0.1614349123237766, -0.35647784444129366, -0.07697337779463229, 0.12745950682263854, -0.09793472603166428... |
709.4356 | City Space Syntax as a Complex Network | The encoding of cities into non-planar dual graphs reveals their complex
structure. We investigate the statistics of the typical space syntax measures
for the five different compact urban patterns. Universal statistical behavior
of space syntax measures uncovers the universality of the city creation
mechanism.
| physics.soc-ph physics.data-an | the encoding of cities into nonplanar dual graphs reveals their complex structure we investigate the statistics of the typical space syntax measures for the five different compact urban patterns universal statistical behavior of space syntax measures uncovers the universality of the city creation mechanism | [['the', 'encoding', 'of', 'cities', 'into', 'nonplanar', 'dual', 'graphs', 'reveals', 'their', 'complex', 'structure', 'we', 'investigate', 'the', 'statistics', 'of', 'the', 'typical', 'space', 'syntax', 'measures', 'for', 'the', 'five', 'different', 'compact', 'urban', 'patterns', 'universal', 'statistical', 'behavio... | [-0.16551043229727921, 0.1413759506434541, -0.12530104035183534, 0.20610792346468026, -0.10529429101469842, -0.06040115392798642, 0.06019951051778414, 0.3417907218364152, -0.26567696331238205, -0.2751710931347175, 0.0025547478792511606, -0.24937928455289116, -0.18830252972177483, 0.17790857846425337, -0.069954987488348... |
709.4357 | Collective excitations of BEC under anharmonic trap position jittering | Collective excitations of a Bose-Einstein condensate under periodic
oscillations of a quadratic plus quartic trap position has been studied. A
coupled set of variational equations is derived for the width and the
condensate wave function center. Analytical expressions for the growth of
oscillation amplitudes in the r... | cond-mat.other | collective excitations of a boseeinstein condensate under periodic oscillations of a quadratic plus quartic trap position has been studied a coupled set of variational equations is derived for the width and the condensate wave function center analytical expressions for the growth of oscillation amplitudes in the resona... | [['collective', 'excitations', 'of', 'a', 'boseeinstein', 'condensate', 'under', 'periodic', 'oscillations', 'of', 'a', 'quadratic', 'plus', 'quartic', 'trap', 'position', 'has', 'been', 'studied', 'a', 'coupled', 'set', 'of', 'variational', 'equations', 'is', 'derived', 'for', 'the', 'width', 'and', 'the', 'condensate... | [-0.170487301272453, 0.1494012880340428, -0.055485039648383555, 0.06251976518383758, -0.03920809496570416, -0.1260876563810414, 0.006850776443671849, 0.31579992638411697, -0.2239473612433431, -0.24638887728103484, 0.033290127024167414, -0.26775808800764456, -0.08449265230541127, 0.22494372840726165, 0.06892887230097043... |
709.4358 | Projective Market Model Approach to AHP Decision-Making | In this paper we describe market in projective geometry language and give
definition of a matrix of market rate, which is related to the matrix rate of
return and the matrix of judgements in the Analytic Hierarchy Process (AHP). We
use these observations to extend the AHP model to projective geometry formalism
and ge... | q-fin.PM physics.data-an physics.soc-ph | in this paper we describe market in projective geometry language and give definition of a matrix of market rate which is related to the matrix rate of return and the matrix of judgements in the analytic hierarchy process ahp we use these observations to extend the ahp model to projective geometry formalism and generali... | [['in', 'this', 'paper', 'we', 'describe', 'market', 'in', 'projective', 'geometry', 'language', 'and', 'give', 'definition', 'of', 'a', 'matrix', 'of', 'market', 'rate', 'which', 'is', 'related', 'to', 'the', 'matrix', 'rate', 'of', 'return', 'and', 'the', 'matrix', 'of', 'judgements', 'in', 'the', 'analytic', 'hierar... | [-0.06735133850926776, -0.005614342276796537, -0.08407486472076373, 0.10945269365554297, -0.11301721929086615, -0.12337750388289113, 0.0650469908926069, 0.35150380244316615, -0.3079869784212307, -0.267786160354381, 0.11597938123083187, -0.21295933104525117, -0.20238098894934292, 0.16229417600223553, -0.1256182580356202... |
709.4359 | On the mechanical quality factors of cryogenic test masses from fused
silica and crystalline quartz | Current interferometric gravitational wave detectors (IGWDs) are operated at
room temperature with test masses made from fused silica. Fused silica shows
very low absorption at the laser wavelength of 1064 nm. It is also well suited
to realize low thermal noise floors in the detector signal band since it offers
low m... | gr-qc | current interferometric gravitational wave detectors igwds are operated at room temperature with test masses made from fused silica fused silica shows very low absorption at the laser wavelength of 1064 nm it is also well suited to realize low thermal noise floors in the detector signal band since it offers low mechani... | [['current', 'interferometric', 'gravitational', 'wave', 'detectors', 'igwds', 'are', 'operated', 'at', 'room', 'temperature', 'with', 'test', 'masses', 'made', 'from', 'fused', 'silica', 'fused', 'silica', 'shows', 'very', 'low', 'absorption', 'at', 'the', 'laser', 'wavelength', 'of', '1064', 'nm', 'it', 'is', 'also',... | [-0.05773779824542414, 0.23598500288436688, -0.05467764880685579, -0.043559751986703345, 0.006510439818902385, -0.1787301375331091, 0.061068237040724074, 0.4506910897436596, -0.18425090381919984, -0.344548818078779, 0.07537146438511887, -0.3081175518843035, -0.0227807047466437, 0.25227957682883634, -0.01246806870968569... |
709.436 | Electrical networks on $n$-simplex fractals | The decimation map $\mathcal{D}$ for a network of admittances on an
$n$-simplex lattice fractal is studied. The asymptotic behaviour of
$\mathcal{D}$ for large-size fractals is examined. It is found that in the
vicinity of the isotropic point the eigenspaces of the linearized map are
always three for $n \geq 4$; they... | cond-mat.dis-nn | the decimation map mathcald for a network of admittances on an nsimplex lattice fractal is studied the asymptotic behaviour of mathcald for largesize fractals is examined it is found that in the vicinity of the isotropic point the eigenspaces of the linearized map are always three for n geq 4 they are given a character... | [['the', 'decimation', 'map', 'mathcald', 'for', 'a', 'network', 'of', 'admittances', 'on', 'an', 'nsimplex', 'lattice', 'fractal', 'is', 'studied', 'the', 'asymptotic', 'behaviour', 'of', 'mathcald', 'for', 'largesize', 'fractals', 'is', 'examined', 'it', 'is', 'found', 'that', 'in', 'the', 'vicinity', 'of', 'the', 'i... | [-0.1678165952267591, 0.09235564352293295, -0.07396019065054134, 0.04298069528886117, -0.008866159935860197, -0.10947229267330841, -0.016414293421257754, 0.3466238347114995, -0.28778590901056306, -0.22169098033336923, 0.11704745270253625, -0.33129839557223023, -0.18278781867411453, 0.17892109430686104, -0.0133150790585... |
709.4361 | Interest rates mapping | The present study deals with the analysis and mapping of Swiss franc interest
rates. Interest rates depend on time and maturity, defining term structure of
the interest rate curves (IRC). In the present study IRC are considered in a
two-dimensional feature space - time and maturity. Geostatistical models and
machine ... | q-fin.ST physics.data-an | the present study deals with the analysis and mapping of swiss franc interest rates interest rates depend on time and maturity defining term structure of the interest rate curves irc in the present study irc are considered in a twodimensional feature space time and maturity geostatistical models and machine learning al... | [['the', 'present', 'study', 'deals', 'with', 'the', 'analysis', 'and', 'mapping', 'of', 'swiss', 'franc', 'interest', 'rates', 'interest', 'rates', 'depend', 'on', 'time', 'and', 'maturity', 'defining', 'term', 'structure', 'of', 'the', 'interest', 'rate', 'curves', 'irc', 'in', 'the', 'present', 'study', 'irc', 'are'... | [-0.06560108014843888, 0.012153248358355323, -0.041213125443539105, 0.10513576044730406, -0.06870135899448583, -0.12384205415156914, 0.05744082465986008, 0.4329137947443906, -0.23667361624203287, -0.25759388145629886, 0.18554976387662594, -0.23176896768445904, -0.16010871977620833, 0.23540052315136334, -0.0938816045217... |
709.4362 | Functional treatment of quantum scattering via the dynamical principle | A careful functional treatment of quantum scattering is given using
Schwinger's dynamical principle which involves a functional differentiation
operation applied to a generating functional written in closed form. For long
range interactions, such as for the Coulomb one, it is shown that this
expression may be used to... | hep-th | a careful functional treatment of quantum scattering is given using schwingers dynamical principle which involves a functional differentiation operation applied to a generating functional written in closed form for long range interactions such as for the coulomb one it is shown that this expression may be used to obtai... | [['a', 'careful', 'functional', 'treatment', 'of', 'quantum', 'scattering', 'is', 'given', 'using', 'schwingers', 'dynamical', 'principle', 'which', 'involves', 'a', 'functional', 'differentiation', 'operation', 'applied', 'to', 'a', 'generating', 'functional', 'written', 'in', 'closed', 'form', 'for', 'long', 'range',... | [-0.11186878513350772, 0.08649416112651427, -0.14314387643729182, 0.1602111938118469, -0.06505390888002391, -0.08931237662715527, 0.028350447968114166, 0.3247586818722387, -0.27237208966786663, -0.26984279543782275, 0.05032059597433545, -0.2050930299020062, -0.18041155675891787, 0.2161590904307862, 0.00657419521206369,... |
709.4363 | Calabi-Bernstein results for maximal surfaces in Lorentzian product
spaces | In this paper we establish new Calabi-Bernstein results for maximal surfaces
immersed into a Lorentzian product space of the form $M^2\times\mathbb{R}_1$,
where $M^2$ is a connected Riemannian surface and $M^2\times\mathbb{R}_1$ is
endowed with the Lorentzian metric $<,>=<,>_{M}-dt^2$. In particular, when $M$
is a Ri... | math.DG math-ph math.MP | in this paper we establish new calabibernstein results for maximal surfaces immersed into a lorentzian product space of the form m2timesmathbbr_1 where m2 is a connected riemannian surface and m2timesmathbbr_1 is endowed with the lorentzian metric _mdt2 in particular when m is a riemannian surface with nonnegative gaus... | [['in', 'this', 'paper', 'we', 'establish', 'new', 'calabibernstein', 'results', 'for', 'maximal', 'surfaces', 'immersed', 'into', 'a', 'lorentzian', 'product', 'space', 'of', 'the', 'form', 'm2timesmathbbr_1', 'where', 'm2', 'is', 'a', 'connected', 'riemannian', 'surface', 'and', 'm2timesmathbbr_1', 'is', 'endowed', '... | [-0.12748183132092047, 0.13200267824713743, -0.09606328818348091, 0.08986800521489899, -0.12365102503896176, -0.14932677513977002, -0.01783985531610546, 0.3907444613735977, -0.2195730915907042, -0.21666735017252045, 0.11601302947448411, -0.26992255657550024, -0.187232353711532, 0.20754007873120173, -0.15104003659288226... |
709.4364 | A topos for algebraic quantum theory | The aim of this paper is to relate algebraic quantum mechanics to topos
theory, so as to construct new foundations for quantum logic and quantum
spaces. Motivated by Bohr's idea that the empirical content of quantum physics
is accessible only through classical physics, we show how a C*-algebra of
observables A induce... | quant-ph math.CT math.OA | the aim of this paper is to relate algebraic quantum mechanics to topos theory so as to construct new foundations for quantum logic and quantum spaces motivated by bohrs idea that the empirical content of quantum physics is accessible only through classical physics we show how a calgebra of observables a induces a topo... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'relate', 'algebraic', 'quantum', 'mechanics', 'to', 'topos', 'theory', 'so', 'as', 'to', 'construct', 'new', 'foundations', 'for', 'quantum', 'logic', 'and', 'quantum', 'spaces', 'motivated', 'by', 'bohrs', 'idea', 'that', 'the', 'empirical', 'content', 'of', 'quantum... | [-0.1049347137021342, 0.10392002446646904, -0.15930508861416265, 0.11280620131098355, -0.09855488600748542, -0.12405484649475272, 0.060617241991087464, 0.30199788516518056, -0.3375093846892317, -0.20343413926801937, 0.03560373843203323, -0.2447020517865256, -0.13196974355939842, 0.17518096446088238, -0.1443396625885119... |
709.4365 | Interplay between Bonding and Magnetism in the Adsorption of NO on Rh
Clusters | We have studied the adsorption of NO on small Rh clusters, containing one to
five atoms, using density functional theory in both spin-polarized and
non-spin-polarized forms. We find that NO bonds more strongly to Rh clusters
than it does to Rh(100) or Rh(111); however, it also quenches the magnetism of
the clusters. ... | cond-mat.mtrl-sci cond-mat.other | we have studied the adsorption of no on small rh clusters containing one to five atoms using density functional theory in both spinpolarized and nonspinpolarized forms we find that no bonds more strongly to rh clusters than it does to rh100 or rh111 however it also quenches the magnetism of the clusters this local effe... | [['we', 'have', 'studied', 'the', 'adsorption', 'of', 'no', 'on', 'small', 'rh', 'clusters', 'containing', 'one', 'to', 'five', 'atoms', 'using', 'density', 'functional', 'theory', 'in', 'both', 'spinpolarized', 'and', 'nonspinpolarized', 'forms', 'we', 'find', 'that', 'no', 'bonds', 'more', 'strongly', 'to', 'rh', 'cl... | [-0.09641994708192911, 0.1464544569261055, -0.057955043519193186, 0.09532070507052691, 0.008705857910830131, -0.09806872872596091, 0.1193330301717419, 0.4073026582321271, -0.23390481969994303, -0.320940846854702, 0.0027934694811305467, -0.358844283849318, -0.13536892208379714, 0.14010533595091088, 0.06390858873566414, ... |
709.4366 | X-Ray Eclipse Time Delays in 4U2129+47 | 4U 2129+47 was discovered in the early 80's and classified as an accretion
disk corona source due to its broad and partial X-ray eclipses. The 5.24 hr
binary orbital period was inferred from the X-ray and optical light curve
modulation, implying a late K or M spectral type companion star.
The source entered a low s... | astro-ph | 4u 212947 was discovered in the early 80s and classified as an accretion disk corona source due to its broad and partial xray eclipses the 524 hr binary orbital period was inferred from the xray and optical light curve modulation implying a late k or m spectral type companion star the source entered a low state in 1983... | [['4u', '212947', 'was', 'discovered', 'in', 'the', 'early', '80s', 'and', 'classified', 'as', 'an', 'accretion', 'disk', 'corona', 'source', 'due', 'to', 'its', 'broad', 'and', 'partial', 'xray', 'eclipses', 'the', '524', 'hr', 'binary', 'orbital', 'period', 'was', 'inferred', 'from', 'the', 'xray', 'and', 'optical', ... | [-0.15218534989818389, 0.10013167194481654, -0.13269640951204068, 0.05648420975665827, -0.11409291474268299, -0.13703681856872482, 0.09783154172047598, 0.40984296900293055, -0.19106778637219907, -0.3505486973129504, 0.15536492995595216, -0.2742866315155722, -0.08135746713004507, 0.21945226913598995, -0.0899599057871994... |
709.4367 | Are biological neurons that vicious ? Or only their models ? | This paper has been withdrawn. Its main conclusions have been published in
"On dynamics of integrate-and-fi re neural networks with conductance based
synapses", arXiv:0709.4370 and
http://www.frontiersin.org/computational_neuroscience/10.3389/neuro.10/002.2008/abstract
| physics.bio-ph nlin.AO physics.comp-ph q-bio.NC | this paper has been withdrawn its main conclusions have been published in on dynamics of integrateandfi re neural networks with conductance based synapses arxiv07094370 and httpwwwfrontiersinorgcomputational_neuroscience103389neuro100022008abstract | [['this', 'paper', 'has', 'been', 'withdrawn', 'its', 'main', 'conclusions', 'have', 'been', 'published', 'in', 'on', 'dynamics', 'of', 'integrateandfi', 're', 'neural', 'networks', 'with', 'conductance', 'based', 'synapses', 'arxiv07094370', 'and', 'httpwwwfrontiersinorgcomputational_neuroscience103389neuro100022008ab... | [-0.11504398375425649, -0.03674933642310941, -0.11579506107322547, -0.08466296289217375, -0.06258764688897392, -0.1632894521943577, -0.010795675658458926, 0.45031566845010157, -0.1898935080870338, -0.3056173395851384, 0.0673621055295529, -0.31615649754910363, -0.2609746184038079, 0.14469169363703416, -0.162936401836898... |
709.4368 | QCD with overlap fermions: Running coupling and the 3-loop beta-function | We calculate the relation between the bare coupling constant g_0 and the
MSbar-renormalized coupling g_MS: g_0 = Z_g(g_0,a \mu) g_MS, to 2 loops in
perturbation theory. We employ the standard Wilson action for gluons and the
overlap action for fermions. For convenience, we have worked with the
background field techni... | hep-lat | we calculate the relation between the bare coupling constant g_0 and the msbarrenormalized coupling g_ms g_0 z_gg_0a mu g_ms to 2 loops in perturbation theory we employ the standard wilson action for gluons and the overlap action for fermions for convenience we have worked with the background field technique which only... | [['we', 'calculate', 'the', 'relation', 'between', 'the', 'bare', 'coupling', 'constant', 'g_0', 'and', 'the', 'msbarrenormalized', 'coupling', 'g_ms', 'g_0', 'z_gg_0a', 'mu', 'g_ms', 'to', '2', 'loops', 'in', 'perturbation', 'theory', 'we', 'employ', 'the', 'standard', 'wilson', 'action', 'for', 'gluons', 'and', 'the'... | [-0.1271222185673593, 0.17848228897215634, -0.08003696558490113, 0.047787651273752035, -0.06622088039175997, -0.11654466916394385, 0.044810564247626056, 0.3639119098823565, -0.13749857225876796, -0.303901580368652, 0.032631151479097155, -0.31096058693514395, -0.10152203293481865, 0.17042577164277103, 0.0515477746972649... |
709.4369 | Fermionic Zero Modes in Gauge and Gravity Backgrounds on a Sphere | In this letter we study fermionic zero modes in gauge and gravity backgrounds
taking a two dimensional compact manifold $S^2$ as extra dimensions. The result
is that there exist massless Dirac fermions which have normalizable zero modes
under quite general assumptions about these backgrounds on the bulk. Several
spec... | hep-th | in this letter we study fermionic zero modes in gauge and gravity backgrounds taking a two dimensional compact manifold s2 as extra dimensions the result is that there exist massless dirac fermions which have normalizable zero modes under quite general assumptions about these backgrounds on the bulk several special cas... | [['in', 'this', 'letter', 'we', 'study', 'fermionic', 'zero', 'modes', 'in', 'gauge', 'and', 'gravity', 'backgrounds', 'taking', 'a', 'two', 'dimensional', 'compact', 'manifold', 's2', 'as', 'extra', 'dimensions', 'the', 'result', 'is', 'that', 'there', 'exist', 'massless', 'dirac', 'fermions', 'which', 'have', 'normal... | [-0.1939687145676351, 0.24879189339381727, -0.06134529770210837, 0.11032246713611213, -0.0774645023047924, -0.21031099653125487, -0.014885772527618841, 0.34517091495746915, -0.10003406608787675, -0.19935425150800834, 0.09612505668844802, -0.2949418456498251, -0.1469116820354071, 0.1557772089162785, -0.03443769344382665... |
709.437 | On Dynamics of Integrate-and-Fire Neural Networks with Conductance Based
Synapses | We present a mathematical analysis of a networks with Integrate-and-Fire
neurons and adaptive conductances. Taking into account the realistic fact that
the spike time is only known within some \textit{finite} precision, we propose
a model where spikes are effective at times multiple of a characteristic time
scale $\d... | physics.bio-ph math.DS nlin.CD q-bio.NC | we present a mathematical analysis of a networks with integrateandfire neurons and adaptive conductances taking into account the realistic fact that the spike time is only known within some textitfinite precision we propose a model where spikes are effective at times multiple of a characteristic time scale delta where ... | [['we', 'present', 'a', 'mathematical', 'analysis', 'of', 'a', 'networks', 'with', 'integrateandfire', 'neurons', 'and', 'adaptive', 'conductances', 'taking', 'into', 'account', 'the', 'realistic', 'fact', 'that', 'the', 'spike', 'time', 'is', 'only', 'known', 'within', 'some', 'textitfinite', 'precision', 'we', 'propo... | [-0.13130928772191205, 0.09686380302902156, -0.07615654885400241, 0.05742058783200466, -0.050853092504872216, -0.15558305096605585, 0.04115456693391833, 0.3616489018913772, -0.27031701639708544, -0.28370252534126245, 0.09707759987200713, -0.23103652732142815, -0.21642613438682423, 0.1803038710076362, -0.071733130659623... |
709.4371 | The Gradient Mechanism in a Communication Network | We study the efficiency of the gradient mechanism of message transfer in a
$2-d$ communication network of regular nodes and randomly distributed hubs.
Each hub on the network is assigned some randomly chosen capacity and hubs with
lower capacities are connected to the hubs with maximum capacity. The average
travel ti... | physics.soc-ph cond-mat.stat-mech nlin.AO | we study the efficiency of the gradient mechanism of message transfer in a 2d communication network of regular nodes and randomly distributed hubs each hub on the network is assigned some randomly chosen capacity and hubs with lower capacities are connected to the hubs with maximum capacity the average travel time of s... | [['we', 'study', 'the', 'efficiency', 'of', 'the', 'gradient', 'mechanism', 'of', 'message', 'transfer', 'in', 'a', '2d', 'communication', 'network', 'of', 'regular', 'nodes', 'and', 'randomly', 'distributed', 'hubs', 'each', 'hub', 'on', 'the', 'network', 'is', 'assigned', 'some', 'randomly', 'chosen', 'capacity', 'an... | [-0.1944003269259107, 0.1269902030096179, -0.04637493005257741, 0.048689298456289394, -0.02772422798318408, -0.16387749219974201, 0.11912272931502191, 0.41567037468125184, -0.30541829959118877, -0.2951948786409752, 0.07502329085267559, -0.29606300568388355, -0.136138522364099, 0.10914189068560479, -0.06268087042942062,... |
709.4372 | Photon lasing in a GaAs microcavity: similarities with a polariton
condensate | We study experimentally the lasing regime of a GaAs based microcavity sample
under strong optical pumping. The very same sample exhibits the strong coupling
regime at low excitation power with a Rabi splitting as large as 15 meV. We
show that some features which may be considered as experimental evidence of
polariton... | cond-mat.mtrl-sci | we study experimentally the lasing regime of a gaas based microcavity sample under strong optical pumping the very same sample exhibits the strong coupling regime at low excitation power with a rabi splitting as large as 15 mev we show that some features which may be considered as experimental evidence of polariton bos... | [['we', 'study', 'experimentally', 'the', 'lasing', 'regime', 'of', 'a', 'gaas', 'based', 'microcavity', 'sample', 'under', 'strong', 'optical', 'pumping', 'the', 'very', 'same', 'sample', 'exhibits', 'the', 'strong', 'coupling', 'regime', 'at', 'low', 'excitation', 'power', 'with', 'a', 'rabi', 'splitting', 'as', 'lar... | [-0.13388186701982074, 0.2185626650717328, -0.05966128321953726, 0.061981938120063244, 0.007486597315006775, -0.19196928219812714, 0.06060142587152861, 0.41768866352385325, -0.20271164718160065, -0.2839837242583079, 0.019010926959133347, -0.2783727845063015, -0.06793098753242165, 0.21613686660076586, 0.0510814701378041... |
709.4373 | The pre-cataclysmic variable, LTT560 | System parameters of the object LTT560 are determined in order to clarify its
nature and evolutionary status. We apply time-series photometry to reveal
orbital modulations of the light curve, time-series spectroscopy to measure
radial velocities of features from both the primary and the secondary star, and
flux-calib... | astro-ph | system parameters of the object ltt560 are determined in order to clarify its nature and evolutionary status we apply timeseries photometry to reveal orbital modulations of the light curve timeseries spectroscopy to measure radial velocities of features from both the primary and the secondary star and fluxcalibrated sp... | [['system', 'parameters', 'of', 'the', 'object', 'ltt560', 'are', 'determined', 'in', 'order', 'to', 'clarify', 'its', 'nature', 'and', 'evolutionary', 'status', 'we', 'apply', 'timeseries', 'photometry', 'to', 'reveal', 'orbital', 'modulations', 'of', 'the', 'light', 'curve', 'timeseries', 'spectroscopy', 'to', 'measu... | [-0.12457523935428652, 0.10853325767794693, -0.1257313927940902, 0.0747401504347971, -0.10153105228444653, -0.06674688438060464, 0.07010129435354324, 0.3953579721025756, -0.23156920846047827, -0.3512534909599201, 0.08975812714817918, -0.3078746330222023, -0.07484240379789463, 0.19741913627405636, -0.08572131448394818, ... |
709.4374 | Lubricated friction between incommensurate substrates | This paper is part of a study of the frictional dynamics of a confined solid
lubricant film - modelled as a one-dimensional chain of interacting particles
confined between two ideally incommensurate substrates, one of which is driven
relative to the other through an attached spring moving at constant velocity.
This m... | cond-mat.mtrl-sci | this paper is part of a study of the frictional dynamics of a confined solid lubricant film modelled as a onedimensional chain of interacting particles confined between two ideally incommensurate substrates one of which is driven relative to the other through an attached spring moving at constant velocity this model sy... | [['this', 'paper', 'is', 'part', 'of', 'a', 'study', 'of', 'the', 'frictional', 'dynamics', 'of', 'a', 'confined', 'solid', 'lubricant', 'film', 'modelled', 'as', 'a', 'onedimensional', 'chain', 'of', 'interacting', 'particles', 'confined', 'between', 'two', 'ideally', 'incommensurate', 'substrates', 'one', 'of', 'whic... | [-0.17028975855835057, 0.1903380303778204, -0.06183969376631725, 0.014007745711650286, -0.057437971993177024, -0.19443386471485374, 0.01655283924404181, 0.35818762198826415, -0.311766935582129, -0.2823180644068706, 0.04810296877913959, -0.2729991649357993, -0.1364788795651776, 0.1867971503129804, 0.022919673119085254, ... |
709.4375 | Scaling and Universality in City Space Syntax: between Zipf and Matthew | We report about universality of rank-integration distributions of open spaces
in city space syntax similar to the famous rank-size distributions of cities
(Zipf's law). We also demonstrate that the degree of choice an open space
represents for other spaces directly linked to it in a city follows a power law
statistic... | physics.soc-ph physics.data-an | we report about universality of rankintegration distributions of open spaces in city space syntax similar to the famous ranksize distributions of cities zipfs law we also demonstrate that the degree of choice an open space represents for other spaces directly linked to it in a city follows a power law statistic univers... | [['we', 'report', 'about', 'universality', 'of', 'rankintegration', 'distributions', 'of', 'open', 'spaces', 'in', 'city', 'space', 'syntax', 'similar', 'to', 'the', 'famous', 'ranksize', 'distributions', 'of', 'cities', 'zipfs', 'law', 'we', 'also', 'demonstrate', 'that', 'the', 'degree', 'of', 'choice', 'an', 'open',... | [-0.09701517545457544, 0.11381405450275901, -0.16936114340908184, 0.18726284187501188, -0.12067444496199317, -0.11527525972917504, 0.1163058019746309, 0.31320447979987354, -0.2867560200286151, -0.3076303756913577, 0.03330769249901775, -0.27117412985869865, -0.16160392399406295, 0.20319044917564968, -0.13642141313945083... |
709.4376 | On Gauss-Bonnet Curvatures | The $(2k)$-th Gauss-Bonnet curvature is a generalization to higher dimensions
of the $(2k)$-dimensional Gauss-Bonnet integrand, it coincides with the usual
scalar curvature for $k=1$. The Gauss-Bonnet curvatures are used in theoretical
physics to describe gravity in higher dimensional space times where they are
known... | math.DG gr-qc math-ph math.MP | the 2kth gaussbonnet curvature is a generalization to higher dimensions of the 2kdimensional gaussbonnet integrand it coincides with the usual scalar curvature for k1 the gaussbonnet curvatures are used in theoretical physics to describe gravity in higher dimensional space times where they are known as the lagrangian o... | [['the', '2kth', 'gaussbonnet', 'curvature', 'is', 'a', 'generalization', 'to', 'higher', 'dimensions', 'of', 'the', '2kdimensional', 'gaussbonnet', 'integrand', 'it', 'coincides', 'with', 'the', 'usual', 'scalar', 'curvature', 'for', 'k1', 'the', 'gaussbonnet', 'curvatures', 'are', 'used', 'in', 'theoretical', 'physic... | [-0.20154789104234688, 0.09199795425804548, -0.051862529706383165, 0.14301069294167465, -0.14762013732065815, -0.17416304541037006, -0.11796279492122012, 0.26640075356916115, -0.19387234841625012, -0.25970885670895494, 0.08805226101973203, -0.29165209938100606, -0.2037503088954403, 0.1321149205918922, -0.15136663415360... |
709.4377 | Importance of hydrodynamic shielding for the dynamic behavior of short
polyelectrolyte chains | The dynamic behavior of polyelectrolyte chains in the oligomer range is
investigated with coarse-grained molecular dynamics simulation and compared to
data obtained by two different experimental methods, namely capillary
electrophoresis and electrophoresis NMR. We find excellent agreement of
experiments and simulatio... | cond-mat.soft | the dynamic behavior of polyelectrolyte chains in the oligomer range is investigated with coarsegrained molecular dynamics simulation and compared to data obtained by two different experimental methods namely capillary electrophoresis and electrophoresis nmr we find excellent agreement of experiments and simulations wh... | [['the', 'dynamic', 'behavior', 'of', 'polyelectrolyte', 'chains', 'in', 'the', 'oligomer', 'range', 'is', 'investigated', 'with', 'coarsegrained', 'molecular', 'dynamics', 'simulation', 'and', 'compared', 'to', 'data', 'obtained', 'by', 'two', 'different', 'experimental', 'methods', 'namely', 'capillary', 'electrophor... | [-0.11804508438400992, 0.12805891973344055, -0.0682306927639303, 0.03986477706925356, 0.046661425393435534, -0.14248065012381286, -0.01005220809649374, 0.42091720653613945, -0.24658530758932937, -0.2995520852808211, 0.03131611405364196, -0.3053912220539542, -0.1571663208977059, 0.167661235284958, 0.06748267738903696, 0... |
709.4378 | Lepton Mass Effects in Single Pion Production by Neutrinos | We reconsider the Feynman-Kislinger-Ravndal model applied to
neutrino-excitation of baryon resonances. The effects of lepton mass are
included, using the formalism of Kuzmin, Lyubushkin and Naumov. In addition we
take account of the pion-pole contribution to the hadronic axial vector
current. Application of this new ... | hep-ph | we reconsider the feynmankislingerravndal model applied to neutrinoexcitation of baryon resonances the effects of lepton mass are included using the formalism of kuzmin lyubushkin and naumov in addition we take account of the pionpole contribution to the hadronic axial vector current application of this new formalism t... | [['we', 'reconsider', 'the', 'feynmankislingerravndal', 'model', 'applied', 'to', 'neutrinoexcitation', 'of', 'baryon', 'resonances', 'the', 'effects', 'of', 'lepton', 'mass', 'are', 'included', 'using', 'the', 'formalism', 'of', 'kuzmin', 'lyubushkin', 'and', 'naumov', 'in', 'addition', 'we', 'take', 'account', 'of', ... | [-0.07665331888165383, 0.18254632771845536, -0.063655225123739, 0.11932199308792235, -0.0327872194829979, -0.12618660716179875, 0.06301607277146104, 0.2973923386671231, -0.17915432010340737, -0.28726704790460644, -0.0846418026203537, -0.3202033727629896, 0.01276381233765278, 0.13574617840458814, 0.04913168555503944, 0.... |
709.4379 | Spin-liquid dynamics of pyrochlore magnets Gd2Ti2O7 and Gd2Sn2O7 | The spin-liquid phase of two highly frustrated pyrochlore magnets Gd2Ti2O7
and Gd2Sn2O7 is probed using electron spin resonance in the temperature range
1.3 - 30 K. The deviation of the absorption line from the paramagnetic position
\nu =\gamma H observed in both compounds below the Curie-Weiss temperature
\Theta_CW ... | cond-mat.str-el cond-mat.mtrl-sci | the spinliquid phase of two highly frustrated pyrochlore magnets gd2ti2o7 and gd2sn2o7 is probed using electron spin resonance in the temperature range 13 30 k the deviation of the absorption line from the paramagnetic position nu gamma h observed in both compounds below the curieweiss temperature theta_cw 10 k suggest... | [['the', 'spinliquid', 'phase', 'of', 'two', 'highly', 'frustrated', 'pyrochlore', 'magnets', 'gd2ti2o7', 'and', 'gd2sn2o7', 'is', 'probed', 'using', 'electron', 'spin', 'resonance', 'in', 'the', 'temperature', 'range', '13', '30', 'k', 'the', 'deviation', 'of', 'the', 'absorption', 'line', 'from', 'the', 'paramagnetic... | [-0.18828818504698575, 0.29157276742185595, 0.0195598244731388, -0.0029179832184270615, -0.019750350976353633, -0.1460421874959904, 0.10170160422460053, 0.39042045010596904, -0.25091703612959365, -0.360509764688016, 0.024688254543243124, -0.35639073123150555, 0.024124490311614386, 0.14779247455360173, 0.132665569149570... |
709.438 | Discovery of the candidate pulsar wind nebula HESS J1718-385 in
very-high-energy gamma-rays | Motivated by recent detections of pulsar wind nebulae in very-high-energy
(VHE) gamma rays, a systematic search for VHE gamma-ray sources associated with
energetic pulsars was performed, using data obtained with the H.E.S.S. (High
Energy Stereoscopic System) instrument. The search for VHE gamma-ray sources
near the p... | astro-ph | motivated by recent detections of pulsar wind nebulae in veryhighenergy vhe gamma rays a systematic search for vhe gammaray sources associated with energetic pulsars was performed using data obtained with the hess high energy stereoscopic system instrument the search for vhe gammaray sources near the pulsar psr j171838... | [['motivated', 'by', 'recent', 'detections', 'of', 'pulsar', 'wind', 'nebulae', 'in', 'veryhighenergy', 'vhe', 'gamma', 'rays', 'a', 'systematic', 'search', 'for', 'vhe', 'gammaray', 'sources', 'associated', 'with', 'energetic', 'pulsars', 'was', 'performed', 'using', 'data', 'obtained', 'with', 'the', 'hess', 'high', ... | [-0.07778783815623332, 0.12382495275281855, -0.04641342897774229, 0.16931233816377098, -0.20536742789843002, -0.07915992558221607, 0.06978796201781566, 0.46069761909575774, -0.19183024790058764, -0.3844566603637293, -0.02876819028937798, -0.35889153487729925, 0.050589346643850334, 0.326323261167541, 0.00901130924369169... |
709.4381 | Un th\'eor\`eme de Helson pour des s\'eries de Walsh | Extension to Walsh series of theorems of Helson and Katznelson on
trigonometric series, saying that a trigonometric series whose partial sums are
positive has its coefficients tend to zero but is not necessarily a
Fourier-Lebesgue series
| math.CA | extension to walsh series of theorems of helson and katznelson on trigonometric series saying that a trigonometric series whose partial sums are positive has its coefficients tend to zero but is not necessarily a fourierlebesgue series | [['extension', 'to', 'walsh', 'series', 'of', 'theorems', 'of', 'helson', 'and', 'katznelson', 'on', 'trigonometric', 'series', 'saying', 'that', 'a', 'trigonometric', 'series', 'whose', 'partial', 'sums', 'are', 'positive', 'has', 'its', 'coefficients', 'tend', 'to', 'zero', 'but', 'is', 'not', 'necessarily', 'a', 'fo... | [-0.18181213655690145, 0.009695869171991944, -0.17202673780007494, 0.022401346323830593, -0.1431007526245796, -0.11875147735958712, 0.024162818176490772, 0.34730215339610976, -0.3255017577515294, -0.1340369371076425, 0.2075811040122062, -0.3374079927388165, -0.13277665649851164, 0.2682624240923259, -0.12786495118376073... |
709.4382 | Hasard et d\'eterminisme chez Laplace | Laplace's views on randomness and determinism. The paper was written for
"Cahiers rationalistes" and addresses a rather wide audience. It contains large
quotations of Laplace, most of them coming from his introduction to the book
"Analytical theory of probabilities".
| math.HO | laplaces views on randomness and determinism the paper was written for cahiers rationalistes and addresses a rather wide audience it contains large quotations of laplace most of them coming from his introduction to the book analytical theory of probabilities | [['laplaces', 'views', 'on', 'randomness', 'and', 'determinism', 'the', 'paper', 'was', 'written', 'for', 'cahiers', 'rationalistes', 'and', 'addresses', 'a', 'rather', 'wide', 'audience', 'it', 'contains', 'large', 'quotations', 'of', 'laplace', 'most', 'of', 'them', 'coming', 'from', 'his', 'introduction', 'to', 'the... | [-0.09251252673321257, 0.03233858509644817, -0.1114665207845208, 0.10709338312000527, -0.17962390297141514, -0.14306289096068786, 0.08111487420913029, 0.26768541654669925, -0.25165112543618307, -0.3121932984182709, 0.09456726371947873, -0.3263223711401224, -0.13724639938261948, 0.19390887426408498, -0.17420779033809117... |
709.4383 | Mailles et ensembles de Sidon | Grid condition and Sidon sets. The grid condition stated by the author in
1957 as a necessary condition for a set of integers to be a Sidon set is
neither improvable nor sufficient ; explanations and stronger statements are
provided.
| math.CA | grid condition and sidon sets the grid condition stated by the author in 1957 as a necessary condition for a set of integers to be a sidon set is neither improvable nor sufficient explanations and stronger statements are provided | [['grid', 'condition', 'and', 'sidon', 'sets', 'the', 'grid', 'condition', 'stated', 'by', 'the', 'author', 'in', '1957', 'as', 'a', 'necessary', 'condition', 'for', 'a', 'set', 'of', 'integers', 'to', 'be', 'a', 'sidon', 'set', 'is', 'neither', 'improvable', 'nor', 'sufficient', 'explanations', 'and', 'stronger', 'sta... | [-0.17379295345968926, 0.09996826903751263, -0.0714320943523676, 0.15425785794818345, -0.12165012759849048, -0.1808838960953439, 0.10300815113199253, 0.3062156275487863, -0.20411826371669006, -0.30236087795585775, 0.1601791124737177, -0.23103745619599253, -0.04439518868159025, 0.15433424724659955, -0.1262338794529056, ... |
709.4384 | Correspondance de Howe: paires duales de type II | In this article, we give a new method for proving Howe correspondence in the
case of dual pairs of type $({\rm GL}_n, {\rm GL}_m)$ over a non-Archimedean
locally compact field $F$. The proof consists in combining a study on Kudla's
filtration with the results of a previous article of the autor about the
irreducibilit... | math.RT | in this article we give a new method for proving howe correspondence in the case of dual pairs of type rm gl_n rm gl_m over a nonarchimedean locally compact field f the proof consists in combining a study on kudlas filtration with the results of a previous article of the autor about the irreducibility of a parabolicall... | [['in', 'this', 'article', 'we', 'give', 'a', 'new', 'method', 'for', 'proving', 'howe', 'correspondence', 'in', 'the', 'case', 'of', 'dual', 'pairs', 'of', 'type', 'rm', 'gl_n', 'rm', 'gl_m', 'over', 'a', 'nonarchimedean', 'locally', 'compact', 'field', 'f', 'the', 'proof', 'consists', 'in', 'combining', 'a', 'study',... | [-0.1842988782711787, 0.015004107354921692, -0.14060246865667494, 0.037599502614250886, -0.10303334522716424, -0.06915604973349858, -0.00026006222254148234, 0.28077753099762365, -0.26458706911423324, -0.22690429874224427, 0.05644433211282263, -0.17900421038103997, -0.1405025581990219, 0.2575184601922462, -0.11662134509... |
709.4385 | Exotic Non-relativistic String | We construct a classical non-relativistic string model in 3+1 dimensions. The
model contains a spurion tensor field that is responsible for the
non-commutative structure of the model. Under double dimensional reduction the
model reduces to the exotic non-relativistic particle in 2+1 dimensions.
| hep-th | we construct a classical nonrelativistic string model in 31 dimensions the model contains a spurion tensor field that is responsible for the noncommutative structure of the model under double dimensional reduction the model reduces to the exotic nonrelativistic particle in 21 dimensions | [['we', 'construct', 'a', 'classical', 'nonrelativistic', 'string', 'model', 'in', '31', 'dimensions', 'the', 'model', 'contains', 'a', 'spurion', 'tensor', 'field', 'that', 'is', 'responsible', 'for', 'the', 'noncommutative', 'structure', 'of', 'the', 'model', 'under', 'double', 'dimensional', 'reduction', 'the', 'mod... | [-0.10365259744936511, 0.17516224033481972, -0.06606127060062829, 0.10559166352807854, -0.013765144738413039, -0.18054497057926797, -0.04930749358165832, 0.2563867270059529, -0.18919314965162248, -0.2724939687177539, 0.008008192379271523, -0.2252315618541269, -0.15050905228902897, 0.1165223905201336, -0.011630358307489... |
709.4386 | Ensembles quasi-ind\'ependants et ensembles de Sidon, th\'eorie de
Bourgain (d'apr\`es Myriam D\'echamps, Li et Queffelec) | Exposition of the relation between quasi-independent and Sidon sets, theorems
of Pisier according to the method of Bourgain
| math.CA | exposition of the relation between quasiindependent and sidon sets theorems of pisier according to the method of bourgain | [['exposition', 'of', 'the', 'relation', 'between', 'quasiindependent', 'and', 'sidon', 'sets', 'theorems', 'of', 'pisier', 'according', 'to', 'the', 'method', 'of', 'bourgain']] | [-0.06092129083764222, 0.08147980129837783, -0.1928693506245812, 0.10291970065898365, -0.056586006863249674, -0.10761853669666582, 0.12863256921344954, 0.23572914416177404, -0.27888185686121386, -0.2932935789382706, 0.08194512047339231, -0.34501803128255737, -0.08099214691254827, 0.22364130409227478, -0.172679198595384... |
709.4387 | Graph-different permutations | We strengthen and put in a broader perspective previous results of the first
two authors on colliding permutations. The key to the present approach is a new
non-asymptotic invariant for graphs.
| math.CO | we strengthen and put in a broader perspective previous results of the first two authors on colliding permutations the key to the present approach is a new nonasymptotic invariant for graphs | [['we', 'strengthen', 'and', 'put', 'in', 'a', 'broader', 'perspective', 'previous', 'results', 'of', 'the', 'first', 'two', 'authors', 'on', 'colliding', 'permutations', 'the', 'key', 'to', 'the', 'present', 'approach', 'is', 'a', 'new', 'nonasymptotic', 'invariant', 'for', 'graphs']] | [-0.12566869038217252, 0.05326036512551288, -0.1383277068455373, 0.08002432063597464, -0.10699096454247352, -0.1174156928074456, 0.08887439662019812, 0.342396869294105, -0.20968671046918438, -0.27544113729269276, 0.04781023569540271, -0.23329125933589473, -0.12661723516160442, 0.2180539277652579, -0.12897257170369547, ... |
709.4388 | One-loop Electroweak and QCD corrections to vector boson scattering into
top pairs and application to ILC | We calculate the electroweak and QCD corrections to W-W+ -> tt and ZZ -> tt.
We also consider the interplay of these corrections with the effect of
anomalous interactions that affect the massive weak bosons and the top. The
results at the VV level fusion are convoluted with the help of the effective
vector boson appr... | hep-ph | we calculate the electroweak and qcd corrections to ww tt and zz tt we also consider the interplay of these corrections with the effect of anomalous interactions that affect the massive weak bosons and the top the results at the vv level fusion are convoluted with the help of the effective vector boson approximation to... | [['we', 'calculate', 'the', 'electroweak', 'and', 'qcd', 'corrections', 'to', 'ww', 'tt', 'and', 'zz', 'tt', 'we', 'also', 'consider', 'the', 'interplay', 'of', 'these', 'corrections', 'with', 'the', 'effect', 'of', 'anomalous', 'interactions', 'that', 'affect', 'the', 'massive', 'weak', 'bosons', 'and', 'the', 'top', ... | [-0.07000778902262922, 0.20728057310990397, -0.07108614285243675, 0.1842117797110289, -0.052563921297116886, -0.1461777339452907, 0.050983619454893325, 0.31449613554610145, -0.2517495345442541, -0.23662355304178265, 0.023522321083065536, -0.3536593316063758, -0.04819123922211547, 0.11111959096576486, 0.1438519502176888... |
709.4389 | Simulation of ratio of old to young people in countries like Poland | Countries like Poland with a recent sharp drop in birth rates still have some
time to prepare for the problems of an ageing society. Ater the year 2030 they
can become increasingly serious.
| physics.soc-ph | countries like poland with a recent sharp drop in birth rates still have some time to prepare for the problems of an ageing society ater the year 2030 they can become increasingly serious | [['countries', 'like', 'poland', 'with', 'a', 'recent', 'sharp', 'drop', 'in', 'birth', 'rates', 'still', 'have', 'some', 'time', 'to', 'prepare', 'for', 'the', 'problems', 'of', 'an', 'ageing', 'society', 'ater', 'the', 'year', '2030', 'they', 'can', 'become', 'increasingly', 'serious']] | [-0.040525148338929284, 0.1887219166860632, -0.10165884002344683, 0.11549451388418674, -0.04072819470820832, -0.15833929988730233, 0.03204996121348813, 0.370863264775835, -0.24827505875146016, -0.3339020672137849, 0.23839452825995977, -0.3316245661408175, -0.07884167047450319, 0.27688123119150987, -0.1806945980351884, ... |
709.439 | A Detailed Analysis of the Dust Formation Zone of IRC+10216 Derived from
Mid-IR Bands of C2H2 and HCN | A spectral survey of IRC+10216 has been carried out in the range 11 to 14 um
with a spectral resolution of about 4 km s^-1. We have identified a forest of
lines in six bands of C2H2 involving the vibrational states from the ground to
3nu5 and in two bands of HCN, involving the vibrational states from the ground
up to... | astro-ph | a spectral survey of irc10216 has been carried out in the range 11 to 14 um with a spectral resolution of about 4 km s1 we have identified a forest of lines in six bands of c2h2 involving the vibrational states from the ground to 3nu5 and in two bands of hcn involving the vibrational states from the ground up to 2nu2 s... | [['a', 'spectral', 'survey', 'of', 'irc10216', 'has', 'been', 'carried', 'out', 'in', 'the', 'range', '11', 'to', '14', 'um', 'with', 'a', 'spectral', 'resolution', 'of', 'about', '4', 'km', 's1', 'we', 'have', 'identified', 'a', 'forest', 'of', 'lines', 'in', 'six', 'bands', 'of', 'c2h2', 'involving', 'the', 'vibratio... | [-0.04877286426224664, 0.14463434761222616, 0.032168488710579514, 0.0094566327160257, 0.03113292734927024, -0.0887020912630026, 0.0575482004706078, 0.4554599606914021, -0.18168565519654453, -0.35694050338127437, 0.09131967875567314, -0.2891288843269362, 0.02767204989479005, 0.12384998282262434, 0.021388192963377947, -0... |
709.4391 | Modified Gravity: living without Birkhoff I. DGP | We consider the consequences of the absence of Birkhoff's theorem in theories
of modified gravity. As an example, we calculate the gravitational force on a
test particle due to a spherical mass shell in the Dvali-Gabadaze-Porrati model
(DGP). We show that unlike in General Relativity, the force depends on the mass
di... | gr-qc astro-ph | we consider the consequences of the absence of birkhoffs theorem in theories of modified gravity as an example we calculate the gravitational force on a test particle due to a spherical mass shell in the dvaligabadazeporrati model dgp we show that unlike in general relativity the force depends on the mass distribution ... | [['we', 'consider', 'the', 'consequences', 'of', 'the', 'absence', 'of', 'birkhoffs', 'theorem', 'in', 'theories', 'of', 'modified', 'gravity', 'as', 'an', 'example', 'we', 'calculate', 'the', 'gravitational', 'force', 'on', 'a', 'test', 'particle', 'due', 'to', 'a', 'spherical', 'mass', 'shell', 'in', 'the', 'dvaligab... | [-0.12941482996668768, 0.11266820572770508, -0.10163779899075225, 0.11268785624368419, -0.06839262642520103, -0.06282287018650488, -0.02652650320826954, 0.2763892869981056, -0.18355875859993534, -0.2774301887162634, 0.029052941053098923, -0.22206310995829268, -0.1436963206364748, 0.17639236340167103, -0.068899898832298... |
709.4392 | Ordinary-derivative formulation of conformal totally symmetric arbitrary
spin bosonic fields | Conformal totally symmetric arbitrary spin bosonic fields in flat space-time
of even dimension greater than or equal to four are studied. Second-derivative
(ordinary-derivative) formulation for such fields is developed. We obtain gauge
invariant Lagrangian and the corresponding gauge transformations. Gauge
symmetries... | hep-th | conformal totally symmetric arbitrary spin bosonic fields in flat spacetime of even dimension greater than or equal to four are studied secondderivative ordinaryderivative formulation for such fields is developed we obtain gauge invariant lagrangian and the corresponding gauge transformations gauge symmetries are reali... | [['conformal', 'totally', 'symmetric', 'arbitrary', 'spin', 'bosonic', 'fields', 'in', 'flat', 'spacetime', 'of', 'even', 'dimension', 'greater', 'than', 'or', 'equal', 'to', 'four', 'are', 'studied', 'secondderivative', 'ordinaryderivative', 'formulation', 'for', 'such', 'fields', 'is', 'developed', 'we', 'obtain', 'g... | [-0.23288640618872966, 0.283092914224068, -0.07295710380259511, 0.11413552414611444, -0.14373067128219347, -0.17180858398679383, -0.1434864580068131, 0.33669690741587055, -0.11110315844416618, -0.2635121571230377, 0.03525765442610682, -0.190248651523865, -0.15869712038146144, 0.06144088896374081, -0.01527675566472864, ... |
709.4393 | Magnus subgroups of one-relator surface groups | A one-relator surface group is the quotient of an orientable surface group by
the normal closure of a single relator. A Magnus subgroup is the fundamental
group of a suitable incompressible sub-surface. A number of results are proved
about the intersections of such subgroups and their conjugates, analogous to
results... | math.GR | a onerelator surface group is the quotient of an orientable surface group by the normal closure of a single relator a magnus subgroup is the fundamental group of a suitable incompressible subsurface a number of results are proved about the intersections of such subgroups and their conjugates analogous to results of bag... | [['a', 'onerelator', 'surface', 'group', 'is', 'the', 'quotient', 'of', 'an', 'orientable', 'surface', 'group', 'by', 'the', 'normal', 'closure', 'of', 'a', 'single', 'relator', 'a', 'magnus', 'subgroup', 'is', 'the', 'fundamental', 'group', 'of', 'a', 'suitable', 'incompressible', 'subsurface', 'a', 'number', 'of', 'r... | [-0.22003068563785275, 0.1478107528671209, -0.15205243062870255, 0.05929364930790175, -0.12248151359180438, -0.06071133859423471, 0.0316241694562105, 0.3283463621768972, -0.33269476235426704, -0.23619665907182055, 0.10373849774197001, -0.27257987195304756, -0.1259289364298356, 0.2539666853202828, -0.17409069730964458, ... |
709.4394 | Effect of internal friction on transformation twin dynamics in
SrxBa1-xSnO3 perovskite | The dynamics of transformation twins in SrxBa1-xSnO3 (x=0.6,0.8) perovskite
has been studied by dynamical mechanical analysis in three-point bend geometry.
This material undergoes phase transitions from orthorhombic to tetragonal and
cubic structures on heating. The mechanical loss signatures of the
transformation tw... | cond-mat.mtrl-sci | the dynamics of transformation twins in srxba1xsno3 x0608 perovskite has been studied by dynamical mechanical analysis in threepoint bend geometry this material undergoes phase transitions from orthorhombic to tetragonal and cubic structures on heating the mechanical loss signatures of the transformation twins include ... | [['the', 'dynamics', 'of', 'transformation', 'twins', 'in', 'srxba1xsno3', 'x0608', 'perovskite', 'has', 'been', 'studied', 'by', 'dynamical', 'mechanical', 'analysis', 'in', 'threepoint', 'bend', 'geometry', 'this', 'material', 'undergoes', 'phase', 'transitions', 'from', 'orthorhombic', 'to', 'tetragonal', 'and', 'cu... | [-0.17170652935339004, 0.22611870841343992, -0.08080834581891132, -0.021298984158064055, -0.07158773715041347, -0.07811713719994944, 0.03299369380722955, 0.45382345287302106, -0.3005794351392416, -0.29690788759245085, 0.03371838988981104, -0.2860362307485385, -0.15063906065188348, 0.11570007361702084, 0.033577203568186... |
709.4395 | The Spatial String Tension in the Deconfined Phase of SU(N) Gauge Theory
and Gauge/String Duality | The spatial string tension of a SU(N) gauge theory without quarks is
calculated using gauge/string duality for 1.2T_c<T<3T_c. The result is
remarkably consistent with the available lattice data for N=2,3. Some evidence
is found that to leading order the large distance physics of a string can be
described by a five-di... | hep-ph hep-lat hep-th nucl-th | the spatial string tension of a sun gauge theory without quarks is calculated using gaugestring duality for 12t_ct3t_c the result is remarkably consistent with the available lattice data for n23 some evidence is found that to leading order the large distance physics of a string can be described by a fivedimensional geo... | [['the', 'spatial', 'string', 'tension', 'of', 'a', 'sun', 'gauge', 'theory', 'without', 'quarks', 'is', 'calculated', 'using', 'gaugestring', 'duality', 'for', '12t_ct3t_c', 'the', 'result', 'is', 'remarkably', 'consistent', 'with', 'the', 'available', 'lattice', 'data', 'for', 'n23', 'some', 'evidence', 'is', 'found'... | [-0.10801437689023542, 0.20521776640917183, -0.09646686951650893, 0.14146400645881058, -0.09300137820236128, -0.11770568055839374, 0.019615362982410168, 0.3395190157381625, -0.20523631388064603, -0.31201801738091584, 0.0946387600370458, -0.24265430051158984, -0.07772396408535283, 0.1502716363375557, -0.0318706434155846... |
709.4396 | Dressing the inflaton with the Standard Model gauge group | In this talk we will discuss how inflation can be embedded within a minimal
extension of the Standard Model where the inflaton carries the Standard Model
charges. There is no need of an ad-hoc scalar field to be introduced in order
to explain the temperature anisotropy of the cosmic microwave background
radiation, al... | hep-ph | in this talk we will discuss how inflation can be embedded within a minimal extension of the standard model where the inflaton carries the standard model charges there is no need of an adhoc scalar field to be introduced in order to explain the temperature anisotropy of the cosmic microwave background radiation all the... | [['in', 'this', 'talk', 'we', 'will', 'discuss', 'how', 'inflation', 'can', 'be', 'embedded', 'within', 'a', 'minimal', 'extension', 'of', 'the', 'standard', 'model', 'where', 'the', 'inflaton', 'carries', 'the', 'standard', 'model', 'charges', 'there', 'is', 'no', 'need', 'of', 'an', 'adhoc', 'scalar', 'field', 'to', ... | [-0.11094871683953664, 0.1987158962553785, -0.13211025259433648, 0.13583547552414715, -0.10838269053472795, -0.1483569740373482, -0.046828391828423, 0.33555809574790746, -0.23254744743562153, -0.2853035494271252, 0.07629639997881335, -0.22948369726092896, -0.12761803733933175, 0.17015763589690447, -0.06843412207622622,... |
709.4397 | The Parallel-Sequential Duality : Matrices and Graphs | Usually, mathematical objects have highly parallel interpretations. In this
paper, we consider them as sequential constructors of other objects. In
particular, we prove that every reflexive directed graph can be interpreted as
a program that builds another and is itself builded by another. That leads to
some optimal ... | math.CO cs.IT math.IT | usually mathematical objects have highly parallel interpretations in this paper we consider them as sequential constructors of other objects in particular we prove that every reflexive directed graph can be interpreted as a program that builds another and is itself builded by another that leads to some optimal memory c... | [['usually', 'mathematical', 'objects', 'have', 'highly', 'parallel', 'interpretations', 'in', 'this', 'paper', 'we', 'consider', 'them', 'as', 'sequential', 'constructors', 'of', 'other', 'objects', 'in', 'particular', 'we', 'prove', 'that', 'every', 'reflexive', 'directed', 'graph', 'can', 'be', 'interpreted', 'as', ... | [-0.13537538959644735, 0.13405765839076292, -0.14720271206460894, 0.10020722585419814, -0.17065580375492573, -0.18480656401758702, 0.03636300855238612, 0.3878285808643947, -0.3437674891203642, -0.2640095718282585, 0.11763352395889039, -0.21757700006322314, -0.19384224262709418, 0.18476612700615078, -0.16754375961609186... |
709.4398 | Spacelike hypersurfaces with constant mean curvature in the steady state
space | We consider complete spacelike hypersurfaces with constant mean curvature in
the open region of de Sitter space known as the steady state space. We prove
that if the hypersurface is bounded away from the infinity of the ambient
space, then the mean curvature must be H=1. Moreover, in the 2-dimensional case
we obtain ... | math.DG math-ph math.MP | we consider complete spacelike hypersurfaces with constant mean curvature in the open region of de sitter space known as the steady state space we prove that if the hypersurface is bounded away from the infinity of the ambient space then the mean curvature must be h1 moreover in the 2dimensional case we obtain that the... | [['we', 'consider', 'complete', 'spacelike', 'hypersurfaces', 'with', 'constant', 'mean', 'curvature', 'in', 'the', 'open', 'region', 'of', 'de', 'sitter', 'space', 'known', 'as', 'the', 'steady', 'state', 'space', 'we', 'prove', 'that', 'if', 'the', 'hypersurface', 'is', 'bounded', 'away', 'from', 'the', 'infinity', '... | [-0.12936907301170636, 0.14617151039381063, -0.08871415794406713, 0.06783965572537608, -0.08808446487626143, -0.13195327298089335, -0.034895165287683494, 0.3586816495300922, -0.2754774820533441, -0.16964214276501793, 0.1538830053543392, -0.2901684750959409, -0.10198469140228972, 0.18453306681682577, -0.0978615248652558... |
709.4399 | Stability of the decagonal quasicrystal in the Lennard-Jones-Gauss
system | Although quasicrystals have been studied for 25 years, there are many open
questions concerning their stability: What is the role of phason fluctuations?
Do quasicrystals transform into periodic crystals at low temperature? If yes,
by what mechanisms? We address these questions here for a simple
two-dimensional model... | cond-mat.other | although quasicrystals have been studied for 25 years there are many open questions concerning their stability what is the role of phason fluctuations do quasicrystals transform into periodic crystals at low temperature if yes by what mechanisms we address these questions here for a simple twodimensional model system a... | [['although', 'quasicrystals', 'have', 'been', 'studied', 'for', '25', 'years', 'there', 'are', 'many', 'open', 'questions', 'concerning', 'their', 'stability', 'what', 'is', 'the', 'role', 'of', 'phason', 'fluctuations', 'do', 'quasicrystals', 'transform', 'into', 'periodic', 'crystals', 'at', 'low', 'temperature', 'i... | [-0.12091390518349056, 0.22606724124565708, -0.08590971849237879, 0.09360687742459081, -0.020799315650947392, -0.15903386731811783, 0.046988463014968784, 0.37666610814630985, -0.30342767369655665, -0.25260985145557735, 0.1361387735835211, -0.3044242875225711, -0.15352757073317966, 0.17069202887400853, 0.004977674317431... |
709.44 | MMT Extremely Metal Poor Galaxy Survey I. An Efficient Technique to
Identify Metal Poor Galaxies | We demonstrate a successful strategy for identifying extremely metal poor
galaxies. Our preliminary survey of 24 candidates contains 10 metal poor
galaxies of which 4 have 12+log(O/H)<7.65, some of the lowest metallicity blue
compact galaxies known to date. Interestingly, our sample of metal poor
galaxies have system... | astro-ph | we demonstrate a successful strategy for identifying extremely metal poor galaxies our preliminary survey of 24 candidates contains 10 metal poor galaxies of which 4 have 12logoh765 some of the lowest metallicity blue compact galaxies known to date interestingly our sample of metal poor galaxies have systematically low... | [['we', 'demonstrate', 'a', 'successful', 'strategy', 'for', 'identifying', 'extremely', 'metal', 'poor', 'galaxies', 'our', 'preliminary', 'survey', 'of', '24', 'candidates', 'contains', '10', 'metal', 'poor', 'galaxies', 'of', 'which', '4', 'have', '12logoh765', 'some', 'of', 'the', 'lowest', 'metallicity', 'blue', '... | [-0.015340392780490219, 0.07070187248796823, -0.037956549140757745, 0.18559812926604147, -0.14897276935101086, -0.0708458099622346, 0.13380974209035879, 0.4840845355231847, 0.0008934303120310817, -0.36436651588550634, -0.02718818350445612, -0.32018778292861366, 0.009319744722701476, 0.24488413466439982, -0.062479750976... |
709.4401 | Classification of interest rate curves using Self-Organising Maps | The present study deals with the analysis and classification of interest rate
curves. Interest rate curves (IRC) are the basic financial curves in many
different fields of economics and finance. They are extremely important tools
in banking and financial risk management problems. Interest rates depend on
time and mat... | physics.data-an | the present study deals with the analysis and classification of interest rate curves interest rate curves irc are the basic financial curves in many different fields of economics and finance they are extremely important tools in banking and financial risk management problems interest rates depend on time and maturity w... | [['the', 'present', 'study', 'deals', 'with', 'the', 'analysis', 'and', 'classification', 'of', 'interest', 'rate', 'curves', 'interest', 'rate', 'curves', 'irc', 'are', 'the', 'basic', 'financial', 'curves', 'in', 'many', 'different', 'fields', 'of', 'economics', 'and', 'finance', 'they', 'are', 'extremely', 'importan... | [-0.12264477258876842, 0.046231561988665196, -0.03614762065219967, 0.10699168282250564, -0.059997898088220286, -0.13386994344638845, 0.04599947509282798, 0.40858444944024086, -0.272820225204615, -0.2623139399231649, 0.18634754060037143, -0.2888486181550166, -0.154153369074943, 0.28601557816214424, -0.14387567019930073,... |
709.4402 | Operators on superspaces and generalizations of the Gelfand-Kolmogorov
theorem | (Write-up of a talk at the Bialowieza meeting, July 2007.)
Gelfand and Kolmogorov in 1939 proved that a compact Hausdorff topological
space $X$ can be canonically embedded into the infinite-dimensional vector
space $C(X)^* $, the dual space of the algebra of continuous functions $C(X)$
as an "algebraic variety" spe... | math-ph math.MP math.RA | writeup of a talk at the bialowieza meeting july 2007 gelfand and kolmogorov in 1939 proved that a compact hausdorff topological space x can be canonically embedded into the infinitedimensional vector space cx the dual space of the algebra of continuous functions cx as an algebraic variety specified by an infinite syst... | [['writeup', 'of', 'a', 'talk', 'at', 'the', 'bialowieza', 'meeting', 'july', '2007', 'gelfand', 'and', 'kolmogorov', 'in', '1939', 'proved', 'that', 'a', 'compact', 'hausdorff', 'topological', 'space', 'x', 'can', 'be', 'canonically', 'embedded', 'into', 'the', 'infinitedimensional', 'vector', 'space', 'cx', 'the', 'd... | [-0.12078607711760748, 0.09858007954154414, -0.13213305155526325, 0.07255590782545868, -0.11966823872118708, -0.09941734970417074, -0.009180230755729461, 0.29656077308520196, -0.31196279311051933, -0.21983628325484772, 0.12471124704461545, -0.2348007010696556, -0.1524306129944581, 0.1910286401899191, -0.115170946141945... |
709.4403 | Minimal Affine Coordinates for SL(3,C) Character Varieties of Free
Groups | Let X be the moduli of SL(3,C) representations of a rank r free group. In
this paper we determine minimal generators of the coordinate ring of X. This at
once gives explicit global coordinates for the moduli and determines the
dimension of the moduli's minimal affine embedding. Along the way, we utilize
results conce... | math.AG math.AC | let x be the moduli of sl3c representations of a rank r free group in this paper we determine minimal generators of the coordinate ring of x this at once gives explicit global coordinates for the moduli and determines the dimension of the modulis minimal affine embedding along the way we utilize results concerning the ... | [['let', 'x', 'be', 'the', 'moduli', 'of', 'sl3c', 'representations', 'of', 'a', 'rank', 'r', 'free', 'group', 'in', 'this', 'paper', 'we', 'determine', 'minimal', 'generators', 'of', 'the', 'coordinate', 'ring', 'of', 'x', 'this', 'at', 'once', 'gives', 'explicit', 'global', 'coordinates', 'for', 'the', 'moduli', 'and... | [-0.21161277175252868, 0.10715206382731192, -0.10749569233658529, 0.008366554214749052, -0.05805832439990238, -0.08967230962264504, 0.01734045833527912, 0.3261403200909669, -0.33964213434346885, -0.18548269422053423, 0.0711468187591256, -0.23644751603823416, -0.137363072593025, 0.13363714433859947, -0.13900746096488695... |
709.4404 | Theory of Relaxation Dynamics in Glass-Forming Hydrogen-Bonded Liquids | We address the relaxation dynamics in hydrogen-bonded super-cooled liquids
near the glass transition, measured via Broad-Band Dielectric Spectroscopy
(BDS). We propose a theory based on decomposing the relaxation of the
macroscopic dipole moment into contributions from hydrogen bonded clusters of
$s$ molecules, with ... | cond-mat.soft cond-mat.stat-mech | we address the relaxation dynamics in hydrogenbonded supercooled liquids near the glass transition measured via broadband dielectric spectroscopy bds we propose a theory based on decomposing the relaxation of the macroscopic dipole moment into contributions from hydrogen bonded clusters of s molecules with s_minle s le... | [['we', 'address', 'the', 'relaxation', 'dynamics', 'in', 'hydrogenbonded', 'supercooled', 'liquids', 'near', 'the', 'glass', 'transition', 'measured', 'via', 'broadband', 'dielectric', 'spectroscopy', 'bds', 'we', 'propose', 'a', 'theory', 'based', 'on', 'decomposing', 'the', 'relaxation', 'of', 'the', 'macroscopic', ... | [-0.06232470755269442, 0.1563249925865424, -0.11858771913650538, 0.036989579466944804, -0.01851326959358865, -0.12320239061525785, 0.07834122620967159, 0.35090152182052686, -0.24555929827527917, -0.2880428608823086, 0.046804019746136925, -0.30808523137163635, -0.11944680659803202, 0.14979455548912507, 0.019921677698281... |
709.4405 | Exciting gauge unstable modes of the quark-gluon plasma by relativistic
jets | We present a study of the properties of the collective modes of a system
composed by a thermalized quark-gluon plasma traversed by a relativistic jet of
partons. We find that when the jet traverses the system unstable gauge field
modes are excited and grow on very short time scales. The aim is to provide a
novel mech... | hep-ph nucl-th | we present a study of the properties of the collective modes of a system composed by a thermalized quarkgluon plasma traversed by a relativistic jet of partons we find that when the jet traverses the system unstable gauge field modes are excited and grow on very short time scales the aim is to provide a novel mechanism... | [['we', 'present', 'a', 'study', 'of', 'the', 'properties', 'of', 'the', 'collective', 'modes', 'of', 'a', 'system', 'composed', 'by', 'a', 'thermalized', 'quarkgluon', 'plasma', 'traversed', 'by', 'a', 'relativistic', 'jet', 'of', 'partons', 'we', 'find', 'that', 'when', 'the', 'jet', 'traverses', 'the', 'system', 'un... | [-0.1514662258651559, 0.19252020766619932, -0.16275973551709091, 0.09183638910692411, -0.043856444850451114, -0.0902330834220982, -0.010366500616355828, 0.3371029221932545, -0.2364204110168485, -0.24713020505327166, 0.01612003523729403, -0.2590483381554033, -0.0656898435543884, 0.14022611223133, 0.04952117438907876, 0.... |
709.4406 | Small x gluon from exclusive J/psi production | Exclusive J/psi production, gamma* p -> J/psi p, offers a unique opportunity
to determine the gluon density of the proton in the small x domain. We use the
available HERA data to determine the gluon distribution in the region 10^{-4}
<~ x <~ 10^{-2} and 2 <~ Q^2 <~ 10 GeV^2, where the uncertainty on the gluon
extract... | hep-ph | exclusive jpsi production gamma p jpsi p offers a unique opportunity to determine the gluon density of the proton in the small x domain we use the available hera data to determine the gluon distribution in the region 104 x 102 and 2 q2 10 gev2 where the uncertainty on the gluon extracted from the global parton analyses... | [['exclusive', 'jpsi', 'production', 'gamma', 'p', 'jpsi', 'p', 'offers', 'a', 'unique', 'opportunity', 'to', 'determine', 'the', 'gluon', 'density', 'of', 'the', 'proton', 'in', 'the', 'small', 'x', 'domain', 'we', 'use', 'the', 'available', 'hera', 'data', 'to', 'determine', 'the', 'gluon', 'distribution', 'in', 'the... | [-0.038360518154194126, 0.18956286672548187, -0.1501263734861845, 0.1369882496286797, -0.031310972910965, -0.0374577126399012, 0.038981242826571914, 0.3384549854459559, -0.2089103128897344, -0.24010869225049847, 0.0043297070781302795, -0.328803480125782, 0.07441895164367629, 0.12190921796576643, 0.05307078130206763, 0.... |
709.4407 | Computing twisted conjugacy classes in free groups using nilpotent
quotients | There currently exists no algebraic algorithm for computing twisted conjugacy
classes in free groups. We propose a new technique for deciding twisted
conjugacy relations using nilpotent quotients. Our technique is generalization
of the common abelianization method, but admits significantly greater rates of
success. W... | math.GR math.GN | there currently exists no algebraic algorithm for computing twisted conjugacy classes in free groups we propose a new technique for deciding twisted conjugacy relations using nilpotent quotients our technique is generalization of the common abelianization method but admits significantly greater rates of success we pres... | [['there', 'currently', 'exists', 'no', 'algebraic', 'algorithm', 'for', 'computing', 'twisted', 'conjugacy', 'classes', 'in', 'free', 'groups', 'we', 'propose', 'a', 'new', 'technique', 'for', 'deciding', 'twisted', 'conjugacy', 'relations', 'using', 'nilpotent', 'quotients', 'our', 'technique', 'is', 'generalization'... | [-0.14445253685449383, 0.08642588604374656, -0.09212869246756392, 0.09859622363832646, -0.0920052002184093, -0.15503617503148104, 0.06501962378554578, 0.4109942489436695, -0.2975773299379008, -0.2803099323064089, 0.10584539043816871, -0.20612526313800897, -0.19230562521676933, 0.29885817273919074, -0.1322971053022359, ... |
709.4408 | SUSY Higgs bosons at the LHC | Recent results on MSSM Higgs physics at the LHC are reviewed. The dependence
of the LHC discovery reach in the b\bar b H/A, H/A \to \tau^+\tau^- channel on
the underlying SUSY scenario is analysed. This is done by combining the latest
results for the prospective CMS experimental sensitivities for an integrated
lumino... | hep-ph | recent results on mssm higgs physics at the lhc are reviewed the dependence of the lhc discovery reach in the bbar b ha ha to tautau channel on the underlying susy scenario is analysed this is done by combining the latest results for the prospective cms experimental sensitivities for an integrated luminosity of 30 or 6... | [['recent', 'results', 'on', 'mssm', 'higgs', 'physics', 'at', 'the', 'lhc', 'are', 'reviewed', 'the', 'dependence', 'of', 'the', 'lhc', 'discovery', 'reach', 'in', 'the', 'bbar', 'b', 'ha', 'ha', 'to', 'tautau', 'channel', 'on', 'the', 'underlying', 'susy', 'scenario', 'is', 'analysed', 'this', 'is', 'done', 'by', 'co... | [-0.06360057754542853, 0.19718861609458385, -0.009720771687856893, 0.121918134394031, -0.07717346945881015, -0.1502484674973969, 0.041709474372345276, 0.33240693700853846, -0.17532516831848008, -0.293257212483158, 0.06204858474768372, -0.2970212547664057, 0.036909812248491665, 0.1741634103924319, 0.037828095095253915, ... |
709.4409 | Comparison between high-energy proton and charged pion induced damage in
Lead Tungstate calorimeter crystals | A Lead Tungstate crystal produced for the electromagnetic calorimeter of the
CMS experiment at the LHC was cut into three equal-length sections. The central
one was irradiated with 290 MeV/c positive pions up to a fluence of (5.67 +-
0.46)x10^13 /cm^2, while the other two were exposed to a 24 GeV/c proton
fluence of ... | physics.ins-det | a lead tungstate crystal produced for the electromagnetic calorimeter of the cms experiment at the lhc was cut into three equallength sections the central one was irradiated with 290 mevc positive pions up to a fluence of 567 046x1013 cm2 while the other two were exposed to a 24 gevc proton fluence of 117 011 x 1013 cm... | [['a', 'lead', 'tungstate', 'crystal', 'produced', 'for', 'the', 'electromagnetic', 'calorimeter', 'of', 'the', 'cms', 'experiment', 'at', 'the', 'lhc', 'was', 'cut', 'into', 'three', 'equallength', 'sections', 'the', 'central', 'one', 'was', 'irradiated', 'with', '290', 'mevc', 'positive', 'pions', 'up', 'to', 'a', 'f... | [-0.04399737693360167, 0.2616886339048938, -0.0594315846533616, 0.0025813251164382195, 0.035405287841832875, -0.09808960240414956, -0.007381022801751843, 0.4150754108582393, -0.15697955019601464, -0.38396754178522835, 0.01579888370049435, -0.4296723855382735, 0.09059118105117048, 0.18405382163675116, 0.0037997420076142... |
709.441 | On the formalism of dark energy accretion onto black- and worm-holes | In this work a general formalism for the accretion of dark energy onto
astronomical objects, black holes and wormholes, is considered. It is shown
that in models with four dimensions or more, any singularity with a divergence
in the Hubble parameter may be avoided by a big trip, if it is assumed that
there is no coup... | astro-ph | in this work a general formalism for the accretion of dark energy onto astronomical objects black holes and wormholes is considered it is shown that in models with four dimensions or more any singularity with a divergence in the hubble parameter may be avoided by a big trip if it is assumed that there is no coupling be... | [['in', 'this', 'work', 'a', 'general', 'formalism', 'for', 'the', 'accretion', 'of', 'dark', 'energy', 'onto', 'astronomical', 'objects', 'black', 'holes', 'and', 'wormholes', 'is', 'considered', 'it', 'is', 'shown', 'that', 'in', 'models', 'with', 'four', 'dimensions', 'or', 'more', 'any', 'singularity', 'with', 'a',... | [-0.10713709960014797, 0.14060531650821484, -0.10664406018656526, 0.09331043921735917, -0.08331978940513245, -0.14753179182298481, -0.03853239703836829, 0.3557202064778742, -0.18152741056347135, -0.2885189293342274, 0.10789029845199007, -0.27259067532628084, -0.12480655273011085, 0.20947484319574786, -0.062305520775966... |
709.4411 | Nested set complexes for posets and the Bier construction | We generalize the concept of combinatorial nested set complexes to posets and
exhibit the topological relationship between the arising nested set complexes
and the order complex of the underlying poset. In particular, a sufficient
condition is given so that this relationship is actually a subdivision. We use
the resu... | math.CO math.AT | we generalize the concept of combinatorial nested set complexes to posets and exhibit the topological relationship between the arising nested set complexes and the order complex of the underlying poset in particular a sufficient condition is given so that this relationship is actually a subdivision we use the results t... | [['we', 'generalize', 'the', 'concept', 'of', 'combinatorial', 'nested', 'set', 'complexes', 'to', 'posets', 'and', 'exhibit', 'the', 'topological', 'relationship', 'between', 'the', 'arising', 'nested', 'set', 'complexes', 'and', 'the', 'order', 'complex', 'of', 'the', 'underlying', 'poset', 'in', 'particular', 'a', '... | [-0.10660095411156745, 0.060713896871005237, -0.06567998387311634, 0.13069128988488382, -0.14014610524387344, -0.05780574448382188, 0.07571117893032926, 0.3553946959344964, -0.33682066535479144, -0.2536900790016118, 0.09397483364476725, -0.23678909622034744, -0.19838069327861854, 0.16474743078364745, -0.159552769306556... |
709.4412 | How long will a bubble be ? | A soap bubble is a metastable object that eventually breaks. Indeed, the
soapy water film thins until rupture, due to drainage and evaporation. In our
experimental investigations, floating bubbles at the surface of a liquid bath
have been considered. Their lifetime has been measured and reported with
respect to their... | physics.flu-dyn | a soap bubble is a metastable object that eventually breaks indeed the soapy water film thins until rupture due to drainage and evaporation in our experimental investigations floating bubbles at the surface of a liquid bath have been considered their lifetime has been measured and reported with respect to their radius ... | [['a', 'soap', 'bubble', 'is', 'a', 'metastable', 'object', 'that', 'eventually', 'breaks', 'indeed', 'the', 'soapy', 'water', 'film', 'thins', 'until', 'rupture', 'due', 'to', 'drainage', 'and', 'evaporation', 'in', 'our', 'experimental', 'investigations', 'floating', 'bubbles', 'at', 'the', 'surface', 'of', 'a', 'liq... | [-0.08440437253907715, 0.22440889761675958, -0.13115247200292193, 0.05686685926425286, -0.03165970008918329, -0.11445001602466953, 0.045175041487489485, 0.3732813110280978, -0.22118936570263223, -0.28535099620624493, 0.1333865644888168, -0.2788889735348915, -0.057518574482712304, 0.18367433060254706, -0.046884574015673... |
709.4413 | Lepton Flavor Violation in the LHT - A Clear Distinction from
Supersymmetry | The Littlest Higgs Model with T-Parity (LHT) contains new sources of flavor
and CP violation both in the quark and lepton sector. These have their origin
in interactions of ordinary fermions with mirror fermions mediated by new heavy
gauge bosons. Large deviations from the Standard Model (SM) are to be expected
in th... | hep-ph | the littlest higgs model with tparity lht contains new sources of flavor and cp violation both in the quark and lepton sector these have their origin in interactions of ordinary fermions with mirror fermions mediated by new heavy gauge bosons large deviations from the standard model sm are to be expected in the lepton ... | [['the', 'littlest', 'higgs', 'model', 'with', 'tparity', 'lht', 'contains', 'new', 'sources', 'of', 'flavor', 'and', 'cp', 'violation', 'both', 'in', 'the', 'quark', 'and', 'lepton', 'sector', 'these', 'have', 'their', 'origin', 'in', 'interactions', 'of', 'ordinary', 'fermions', 'with', 'mirror', 'fermions', 'mediate... | [-0.07377761056728768, 0.33003127168182694, -0.004060110575843938, 0.19836952018582063, -0.07628257053171392, -0.21386081487566355, 0.07478652343814277, 0.2915623758110355, -0.22615485606699814, -0.29717192394643654, -0.007712372121607244, -0.3247140086271235, -0.03893745022245729, 0.12728093818715605, 0.06658197126778... |
709.4414 | The Cauchy problem of f(R) gravity | The initial value problem of metric and Palatini f(R)gravity is studied by
using the dynamical equivalence between these theories and Brans-Dicke gravity.
The Cauchy problem is well-formulated for metric f(R)gravity in the presence of
matter and well-posed in vacuo. For Palatini f(R)gravity, instead, the Cauchy
probl... | gr-qc astro-ph hep-th | the initial value problem of metric and palatini frgravity is studied by using the dynamical equivalence between these theories and bransdicke gravity the cauchy problem is wellformulated for metric frgravity in the presence of matter and wellposed in vacuo for palatini frgravity instead the cauchy problem is not wellf... | [['the', 'initial', 'value', 'problem', 'of', 'metric', 'and', 'palatini', 'frgravity', 'is', 'studied', 'by', 'using', 'the', 'dynamical', 'equivalence', 'between', 'these', 'theories', 'and', 'bransdicke', 'gravity', 'the', 'cauchy', 'problem', 'is', 'wellformulated', 'for', 'metric', 'frgravity', 'in', 'the', 'prese... | [-0.16839676306640006, 0.07378350702893673, -0.09829357834722922, 0.1747269452886884, -0.13572791059102332, -0.15723515983566413, -0.11079787246274705, 0.2665771374250857, -0.2330380804380592, -0.3039510383897898, 0.07493681750944531, -0.24081549223284332, -0.13586462140843578, 0.09459761170936483, -0.12415371314451402... |
709.4415 | Discovering Important Nodes Through Graph Entropy Encoded in Urban Space
Syntax | Potentially influential spaces in the spatial networks of cities can be
detected by means of the entropy participation ratios. Local (connectivity) and
global (centrality) entropies are considered. While the connectivity entropy
has a tendency to increase with the city size, the centrality entropy is
decreasing that ... | physics.soc-ph physics.comp-ph | potentially influential spaces in the spatial networks of cities can be detected by means of the entropy participation ratios local connectivity and global centrality entropies are considered while the connectivity entropy has a tendency to increase with the city size the centrality entropy is decreasing that reflects ... | [['potentially', 'influential', 'spaces', 'in', 'the', 'spatial', 'networks', 'of', 'cities', 'can', 'be', 'detected', 'by', 'means', 'of', 'the', 'entropy', 'participation', 'ratios', 'local', 'connectivity', 'and', 'global', 'centrality', 'entropies', 'are', 'considered', 'while', 'the', 'connectivity', 'entropy', 'h... | [-0.15386456768035053, 0.14908460357268763, -0.08904404163529928, 0.13346284671967046, 0.047321301859814084, -0.09900897437579591, 0.03397569711986845, 0.3637581220298836, -0.2252981850655157, -0.3094627381492914, 0.041962022270044225, -0.3769085221627558, -0.13086178625764494, 0.11365954530298371, -0.11176399202932688... |
709.4416 | The eigenvalue spectrum for dynamical Chirally Improved fermions | We study the eigenvalues of Dirac operators in QCD with two mass degenerate
dynamical fermions. The gauge configurations have been obtained with HMC and
the so-called Chirally Improved fermionic action. We compare eigenvalues
obtained for the overlap Dirac operator on these configurations with those for
the Chirally ... | hep-lat | we study the eigenvalues of dirac operators in qcd with two mass degenerate dynamical fermions the gauge configurations have been obtained with hmc and the socalled chirally improved fermionic action we compare eigenvalues obtained for the overlap dirac operator on these configurations with those for the chirally impro... | [['we', 'study', 'the', 'eigenvalues', 'of', 'dirac', 'operators', 'in', 'qcd', 'with', 'two', 'mass', 'degenerate', 'dynamical', 'fermions', 'the', 'gauge', 'configurations', 'have', 'been', 'obtained', 'with', 'hmc', 'and', 'the', 'socalled', 'chirally', 'improved', 'fermionic', 'action', 'we', 'compare', 'eigenvalue... | [-0.13360174730041763, 0.22083948669751408, -0.08220479661395075, 0.06685636058682576, -0.027234265002334723, -0.12086895210995863, 0.030170138144967495, 0.40086763477302156, -0.09853035068954341, -0.24706888510263525, 0.04527567301374802, -0.3108981692348607, -0.11605927660639281, 0.05738199930055998, 0.04513831619988... |
709.4417 | The New Horizons Pluto Kuiper belt Mission: An Overview with Historical
Context | NASA's New Horizons (NH) Pluto-Kuiper belt (PKB) mission was launched on 19
January 2006 on a Jupiter Gravity Assist (JGA) trajectory toward the Pluto
system for a 14 July 2015 closest approach; Jupiter closest approach occurred
on 28 February 2007. It was competitively selected by NASA for development on
29 November... | astro-ph | nasas new horizons nh plutokuiper belt pkb mission was launched on 19 january 2006 on a jupiter gravity assist jga trajectory toward the pluto system for a 14 july 2015 closest approach jupiter closest approach occurred on 28 february 2007 it was competitively selected by nasa for development on 29 november 2001 new ho... | [['nasas', 'new', 'horizons', 'nh', 'plutokuiper', 'belt', 'pkb', 'mission', 'was', 'launched', 'on', '19', 'january', '2006', 'on', 'a', 'jupiter', 'gravity', 'assist', 'jga', 'trajectory', 'toward', 'the', 'pluto', 'system', 'for', 'a', '14', 'july', '2015', 'closest', 'approach', 'jupiter', 'closest', 'approach', 'o... | [-0.059018648104773606, 0.17793543922876004, -0.1064723449825989, 0.07938807516924659, -0.10409553076301697, -0.06598458118453811, 0.01847222587486674, 0.2980297298842593, -0.1452555966171542, -0.4175173699824367, 0.13059209993812512, -0.33879128192209557, -0.09602376306822469, 0.23575164678797345, -0.14112123293126247... |
709.4418 | Periodic solutions for planar autonomous systems with nonsmooth periodic
perturbations | In this paper we consider a class of planar autonomous systems having an
isolated limit cycle x_0 of smallest period T>0 such that the associated
linearized system around it has only one characteristic multiplier with
absolute value 1. We consider two functions, defined by means of the
eigenfunctions of the adjoint o... | math.CA | in this paper we consider a class of planar autonomous systems having an isolated limit cycle x_0 of smallest period t0 such that the associated linearized system around it has only one characteristic multiplier with absolute value 1 we consider two functions defined by means of the eigenfunctions of the adjoint of the... | [['in', 'this', 'paper', 'we', 'consider', 'a', 'class', 'of', 'planar', 'autonomous', 'systems', 'having', 'an', 'isolated', 'limit', 'cycle', 'x_0', 'of', 'smallest', 'period', 't0', 'such', 'that', 'the', 'associated', 'linearized', 'system', 'around', 'it', 'has', 'only', 'one', 'characteristic', 'multiplier', 'wit... | [-0.16768857489127761, 0.05113436015221296, -0.06662398441581101, 0.029916102540815566, -0.016478076385527212, -0.09063348266091652, -0.0019284816495733473, 0.3276797951789709, -0.2745790024197138, -0.25273829910949597, 0.16620965802931317, -0.2698300822933273, -0.16223735292016234, 0.21248704852627182, -0.065212575537... |
709.4419 | Reply to comment on ``Competing Interactions, the Renormalization Group
and the Isotropic-Nematic Phase Transition'' | The focus of our work is to identify conditions for the presence of an
isotropic-nematic phase transition in the context of a generic system with
isotropic competing interactions. The comment 0709.4205 criticizes our results
by showing that the low temperature fluctuations of a stripe phase in 2d
diverge linearly in ... | cond-mat.soft cond-mat.stat-mech | the focus of our work is to identify conditions for the presence of an isotropicnematic phase transition in the context of a generic system with isotropic competing interactions the comment 07094205 criticizes our results by showing that the low temperature fluctuations of a stripe phase in 2d diverge linearly in the t... | [['the', 'focus', 'of', 'our', 'work', 'is', 'to', 'identify', 'conditions', 'for', 'the', 'presence', 'of', 'an', 'isotropicnematic', 'phase', 'transition', 'in', 'the', 'context', 'of', 'a', 'generic', 'system', 'with', 'isotropic', 'competing', 'interactions', 'the', 'comment', '07094205', 'criticizes', 'our', 'resu... | [-0.14610372202542538, 0.1699464701794988, -0.08930454947123788, 0.0026923930261266204, -0.020802962571346704, -0.09462627483299002, 0.0767446999760488, 0.31194995831734, -0.20512897554838744, -0.2600002886655812, 0.07444017112273006, -0.28341148128339017, -0.17868505510537383, 0.1191673611510151, -0.03695219829499435,... |
709.442 | Confirmation of Shannon's Mistake about Perfect Secrecy of One-time-pad | This paper has been withdrawn
| cs.CR | this paper has been withdrawn | [['this', 'paper', 'has', 'been', 'withdrawn']] | [-0.14966976195573806, -0.11479587350040674, -0.26925536394119265, -0.2174653896363452, -0.24278417900204657, -0.06483052410185337, -0.18645338097121567, 0.4360402226448059, -0.2831330731511116, -0.34362963438034055, 0.12004837393760681, -0.3683081828057766, -0.1602430183440447, -0.10558439195156097, -0.497941048443317... |
709.4421 | Isometry classes of generalized associahedra | Let $(W,S)$ be a finite Coxeter system acting by reflections on an $\mathbb
R$-Euclidean space with simple roots $\Delta=\{\a_s | s\in S\}$ of the same
length and fundamental weights $\Delta^*=\{v_s | s\in S\}$. We set
$M(e)=\sum_{s\in S}\kappa_s v_s$, $\kappa_s>0$, and for $w\in W$ we set
$M(w)=w(M(e))$. The permuta... | math.CO | let ws be a finite coxeter system acting by reflections on an mathbb reuclidean space with simple roots deltaa_s sin s of the same length and fundamental weights deltav_s sin s we set mesum_sin skappa_s v_s kappa_s0 and for win w we set mwwme the permutahedron permw is the convex hull of the set mw win w given a coxete... | [['let', 'ws', 'be', 'a', 'finite', 'coxeter', 'system', 'acting', 'by', 'reflections', 'on', 'an', 'mathbb', 'reuclidean', 'space', 'with', 'simple', 'roots', 'deltaa_s', 'sin', 's', 'of', 'the', 'same', 'length', 'and', 'fundamental', 'weights', 'deltav_s', 'sin', 's', 'we', 'set', 'mesum_sin', 'skappa_s', 'v_s', 'ka... | [-0.11640840777334847, 0.17993813301659264, -0.009465515173141318, -0.04066072720669614, -0.09514621443799641, -0.18071713421426444, 0.07634711679960433, 0.3620537799300559, -0.33508178230980973, -0.19376863668643285, 0.06248643252499267, -0.31375184991812133, -0.10531292667862095, 0.17630960689492928, -0.1329033529548... |
709.4422 | Towards $B \to V \gamma$ Decays at NNLO in SCET | We compute NNLO (${\cal O}(\alpha_s^2)$) corrections to the hard-scattering
kernels entering the QCD factorization formula for $B\to V\gamma$ decays, where
$V$ is a light vector meson. We give complete NNLO results for the dipole
operators $Q_7$ and $Q_8$, and partial results for $Q_1$ valid in the
large-$\beta_0$ li... | hep-ph hep-ex | we compute nnlo cal oalpha_s2 corrections to the hardscattering kernels entering the qcd factorization formula for bto vgamma decays where v is a light vector meson we give complete nnlo results for the dipole operators q_7 and q_8 and partial results for q_1 valid in the largebeta_0 limit and neglecting the nnlo corre... | [['we', 'compute', 'nnlo', 'cal', 'oalpha_s2', 'corrections', 'to', 'the', 'hardscattering', 'kernels', 'entering', 'the', 'qcd', 'factorization', 'formula', 'for', 'bto', 'vgamma', 'decays', 'where', 'v', 'is', 'a', 'light', 'vector', 'meson', 'we', 'give', 'complete', 'nnlo', 'results', 'for', 'the', 'dipole', 'opera... | [-0.057109499799814646, 0.17415410742562795, -0.10036261670994667, 0.16417254088090125, -0.07901484165483211, -0.05425844430015898, 0.054673073472388624, 0.3302702734018771, -0.1731805278615532, -0.11424451568211448, -0.01251050324074696, -0.39670932635056727, -0.009874334290970534, 0.10270115305498546, 0.0980442281745... |
709.4423 | Effects of CMB temperature uncertainties on cosmological parameter
estimation | We estimate the effect of the experimental uncertainty in the measurement of
the temperature of the cosmic microwave background (CMB) on the extraction of
cosmological parameters from future CMB surveys. We find that even for an ideal
experiment limited only by cosmic variance up to l = 2500 for both the
temperature ... | astro-ph | we estimate the effect of the experimental uncertainty in the measurement of the temperature of the cosmic microwave background cmb on the extraction of cosmological parameters from future cmb surveys we find that even for an ideal experiment limited only by cosmic variance up to l 2500 for both the temperature and pol... | [['we', 'estimate', 'the', 'effect', 'of', 'the', 'experimental', 'uncertainty', 'in', 'the', 'measurement', 'of', 'the', 'temperature', 'of', 'the', 'cosmic', 'microwave', 'background', 'cmb', 'on', 'the', 'extraction', 'of', 'cosmological', 'parameters', 'from', 'future', 'cmb', 'surveys', 'we', 'find', 'that', 'even... | [-0.08977728408362184, 0.15285768543311862, -0.024211136932883945, 0.06645134240588439, -0.03685425046299185, -0.05528053103280919, 0.0663304101855361, 0.3298521129148347, -0.23246002869946616, -0.37358509578076854, 0.10420826085776623, -0.3310135985192444, -0.00159358910384721, 0.22008968720478672, -0.0337624945970518... |
709.4424 | Fermi-Fermi Mixtures in the Strong Attraction Limit | The phase diagrams of low density Fermi-Fermi mixtures with equal or unequal
masses and equal or unequal populations are described at zero and finite
temperatures in the strong attraction limit. In this limit, the Fermi-Fermi
mixture can be described by a weakly interacting Bose-Fermi mixture, where the
bosons corres... | cond-mat.supr-con cond-mat.other | the phase diagrams of low density fermifermi mixtures with equal or unequal masses and equal or unequal populations are described at zero and finite temperatures in the strong attraction limit in this limit the fermifermi mixture can be described by a weakly interacting bosefermi mixture where the bosons correspond to ... | [['the', 'phase', 'diagrams', 'of', 'low', 'density', 'fermifermi', 'mixtures', 'with', 'equal', 'or', 'unequal', 'masses', 'and', 'equal', 'or', 'unequal', 'populations', 'are', 'described', 'at', 'zero', 'and', 'finite', 'temperatures', 'in', 'the', 'strong', 'attraction', 'limit', 'in', 'this', 'limit', 'the', 'ferm... | [-0.10760547848459069, 0.3404309776086167, -0.04682904001722326, 0.10052153601659757, 0.05049579960925128, -0.17323750144511949, 0.10446995486571489, 0.36001461677640023, -0.19117503369461156, -0.2564003943106862, -0.004143383388300655, -0.32394792170574266, -0.05660244389411693, 0.055196093965342134, 0.082611406145647... |
709.4425 | Probabilistic annotation of protein sequences based on functional
classifications | BACKGROUND: One of the most evident achievements of bioinformatics is the
development of methods that transfer biological knowledge from characterised
proteins to uncharacterised sequences. This mode of protein function assignment
is mostly based on the detection of sequence similarity and the premise that
functional... | q-bio.QM | background one of the most evident achievements of bioinformatics is the development of methods that transfer biological knowledge from characterised proteins to uncharacterised sequences this mode of protein function assignment is mostly based on the detection of sequence similarity and the premise that functional pro... | [['background', 'one', 'of', 'the', 'most', 'evident', 'achievements', 'of', 'bioinformatics', 'is', 'the', 'development', 'of', 'methods', 'that', 'transfer', 'biological', 'knowledge', 'from', 'characterised', 'proteins', 'to', 'uncharacterised', 'sequences', 'this', 'mode', 'of', 'protein', 'function', 'assignment',... | [-0.06893056088824778, 0.032432198631340725, -0.08914754784530032, 0.0800316612360703, -0.07074960482441384, -0.08928425010071805, 0.10192637691125128, 0.39334979180421215, -0.28163079092428234, -0.3318248852483521, 0.0548189617047683, -0.2638459815881333, -0.1793431203985847, 0.1844290455801456, -0.06662574237270746, ... |
709.4426 | Precision measurements of alphas at HERA | Recent determinations of alphas(Mz) from the H1 and ZEUS Collaborations using
inclusive-jet cross-section measurements in neutral current deep inelastic
scattering at high Q2 are presented. A combined value of alphas(mz)=0.1198 +-
0.0019 (exp.) +- 0.0026 (th.) was obtained from these measurements. The
determinations ... | hep-ex | recent determinations of alphasmz from the h1 and zeus collaborations using inclusivejet crosssection measurements in neutral current deep inelastic scattering at high q2 are presented a combined value of alphasmz01198 00019 exp 00026 th was obtained from these measurements the determinations of alphas at various scale... | [['recent', 'determinations', 'of', 'alphasmz', 'from', 'the', 'h1', 'and', 'zeus', 'collaborations', 'using', 'inclusivejet', 'crosssection', 'measurements', 'in', 'neutral', 'current', 'deep', 'inelastic', 'scattering', 'at', 'high', 'q2', 'are', 'presented', 'a', 'combined', 'value', 'of', 'alphasmz01198', '00019', ... | [-0.04989753129820411, 0.14423135285838865, -0.0820544266106131, 0.05329534958761472, 0.029791356211241623, -0.06741706925050284, 0.0325836337207315, 0.3497828905399029, -0.18895704498371252, -0.3085276203373304, 0.04506145561474394, -0.4324701786614381, 0.06686453018337488, 0.20517545171225302, 0.11004871998268824, 0.... |
709.4427 | Dynamical Electron Mass in a Strong Magnetic Field | Motivated by recent interest in understanding properties of strongly
magnetized matter, we study the dynamical electron mass generated through
approximate chiral symmetry breaking in QED in a strong magnetic field. We
reliably calculate the dynamical electron mass by numerically solving the
nonperturbative Schwinger-... | hep-ph astro-ph | motivated by recent interest in understanding properties of strongly magnetized matter we study the dynamical electron mass generated through approximate chiral symmetry breaking in qed in a strong magnetic field we reliably calculate the dynamical electron mass by numerically solving the nonperturbative schwingerdyson... | [['motivated', 'by', 'recent', 'interest', 'in', 'understanding', 'properties', 'of', 'strongly', 'magnetized', 'matter', 'we', 'study', 'the', 'dynamical', 'electron', 'mass', 'generated', 'through', 'approximate', 'chiral', 'symmetry', 'breaking', 'in', 'qed', 'in', 'a', 'strong', 'magnetic', 'field', 'we', 'reliably... | [-0.1713636918084989, 0.2479383729063393, -0.04394322878607873, 0.11998167670896967, -0.02994594168378396, -0.043373808702924864, 0.008592855561985059, 0.3278491360271412, -0.20048330305667406, -0.3076388526189905, 0.003558722662142991, -0.20923651260418002, -0.10449376348092147, 0.13516082099816773, 0.0530391352518011... |
709.4428 | The Pluto Energetic Particle Spectrometer Science Investigation (PEPSSI)
on the New Horizons Mission | The Pluto Energetic Particle Spectrometer Science Investigation (PEPSSI)
comprises the hardware and accompanying science investigation on the New
Horizons spacecraft to measure pick-up ions from Pluto's outgassing atmosphere.
To the extent that Pluto retains its characteristics similar to those of a
"heavy comet" as ... | astro-ph | the pluto energetic particle spectrometer science investigation pepssi comprises the hardware and accompanying science investigation on the new horizons spacecraft to measure pickup ions from plutos outgassing atmosphere to the extent that pluto retains its characteristics similar to those of a heavy comet as detected ... | [['the', 'pluto', 'energetic', 'particle', 'spectrometer', 'science', 'investigation', 'pepssi', 'comprises', 'the', 'hardware', 'and', 'accompanying', 'science', 'investigation', 'on', 'the', 'new', 'horizons', 'spacecraft', 'to', 'measure', 'pickup', 'ions', 'from', 'plutos', 'outgassing', 'atmosphere', 'to', 'the', ... | [-0.06314913096427364, 0.20052247374650783, -0.06092709324686871, 0.08018590720534084, -0.04532349370647623, -0.10632533915594479, 0.020567155129617393, 0.3357555328564036, -0.19762940285727382, -0.41968170119135983, 0.109665283920603, -0.3223938848177838, -0.01948000577573508, 0.21860812124819265, -0.06096061619487360... |
709.4429 | A converse approach to the calculation of NMR shielding tensors | We introduce an alternative approach to the first-principles calculation of
NMR shielding tensors. These are obtained from the derivative of the orbital
magnetization with respect to the application of a microscopic, localized
magnetic dipole. The approach is simple, general, and can be applied to either
isolated or ... | cond-mat.mtrl-sci | we introduce an alternative approach to the firstprinciples calculation of nmr shielding tensors these are obtained from the derivative of the orbital magnetization with respect to the application of a microscopic localized magnetic dipole the approach is simple general and can be applied to either isolated or periodic... | [['we', 'introduce', 'an', 'alternative', 'approach', 'to', 'the', 'firstprinciples', 'calculation', 'of', 'nmr', 'shielding', 'tensors', 'these', 'are', 'obtained', 'from', 'the', 'derivative', 'of', 'the', 'orbital', 'magnetization', 'with', 'respect', 'to', 'the', 'application', 'of', 'a', 'microscopic', 'localized'... | [-0.08417790098979637, 0.09799382852688196, -0.07065717490437184, 0.04057908178462336, -0.05197562109948932, -0.12859728308124602, 0.023619715735127313, 0.43732451204804407, -0.2299676075361777, -0.2870437179032403, 0.06004499361269932, -0.2798936267423889, -0.13250871708927056, 0.2306239133451026, 0.005013417938481207... |
709.443 | Fast-ion conduction and flexibility of glassy networks | We observe two thresholds in the variations of electrical conductivity of dry
solid electrolyte (AgI)x(AgPO3)1-x glasses, when the AgI additive concentration
x increases to 9.5% and to 37.8%. Raman scattering complemented by calorimetric
measurements confirm that these thresholds are signatures of the rigidity phase
... | cond-mat.soft | we observe two thresholds in the variations of electrical conductivity of dry solid electrolyte agixagpo31x glasses when the agi additive concentration x increases to 95 and to 378 raman scattering complemented by calorimetric measurements confirm that these thresholds are signatures of the rigidity phase transitions a... | [['we', 'observe', 'two', 'thresholds', 'in', 'the', 'variations', 'of', 'electrical', 'conductivity', 'of', 'dry', 'solid', 'electrolyte', 'agixagpo31x', 'glasses', 'when', 'the', 'agi', 'additive', 'concentration', 'x', 'increases', 'to', '95', 'and', 'to', '378', 'raman', 'scattering', 'complemented', 'by', 'calorim... | [-0.1052808689107139, 0.20445456909458032, -0.05571847067925042, -0.04252438408505056, 0.006301344674771901, -0.15282575134668, 0.13176176641328433, 0.4220290503551051, -0.24647625922657473, -0.2556038040706177, 0.07415328744784497, -0.3329329023272106, -0.11473106627938212, 0.1614448797418592, -0.068150098627606, 0.06... |
709.4431 | On the rate of convergence of periodic solutions in perturbed autonomous
systems as the perturbation vanishes | We consider an autonomous system in R^n having a limit cycle x_0 of period
T>0 which is nondegenerate in a suitable sense. We then consider the perturbed
system obtained by adding to the autonomous system a T-periodic, not
necessarily differentiable, term whose amplitude tends to 0 as a small
parameter e>0 tends to 0... | math.CA | we consider an autonomous system in rn having a limit cycle x_0 of period t0 which is nondegenerate in a suitable sense we then consider the perturbed system obtained by adding to the autonomous system a tperiodic not necessarily differentiable term whose amplitude tends to 0 as a small parameter e0 tends to 0 assuming... | [['we', 'consider', 'an', 'autonomous', 'system', 'in', 'rn', 'having', 'a', 'limit', 'cycle', 'x_0', 'of', 'period', 't0', 'which', 'is', 'nondegenerate', 'in', 'a', 'suitable', 'sense', 'we', 'then', 'consider', 'the', 'perturbed', 'system', 'obtained', 'by', 'adding', 'to', 'the', 'autonomous', 'system', 'a', 'tperi... | [-0.2667760412710217, 0.10094479226477183, -0.03440808220305941, -0.0013051119026635865, -0.004871829059793727, -0.18167220677279836, 0.03005971952218685, 0.28762331236522276, -0.2963277633086993, -0.19175103182935124, 0.15617404549873873, -0.27540856773919004, -0.11601629083628183, 0.1448074968961569, -0.0730516744552... |
709.4432 | On the maximal number of three-term arithmetic progressions in subsets
of Z/pZ | Let a be a real number between 0 and 1. Ernie Croot showed that the quantity
\max_A #(3-term arithmetic progressions in A)/p^2, where A ranges over all
subsets of Z/pZ of size at most a*p, tends to a limit as p tends to infinity
through primes. Writing c(a) for this limit, we show that c(a) = a^2/2 provided
that a is... | math.NT math.CO | let a be a real number between 0 and 1 ernie croot showed that the quantity max_a 3term arithmetic progressions in ap2 where a ranges over all subsets of zpz of size at most ap tends to a limit as p tends to infinity through primes writing ca for this limit we show that ca a22 provided that a is smaller than some absol... | [['let', 'a', 'be', 'a', 'real', 'number', 'between', '0', 'and', '1', 'ernie', 'croot', 'showed', 'that', 'the', 'quantity', 'max_a', '3term', 'arithmetic', 'progressions', 'in', 'ap2', 'where', 'a', 'ranges', 'over', 'all', 'subsets', 'of', 'zpz', 'of', 'size', 'at', 'most', 'ap', 'tends', 'to', 'a', 'limit', 'as', '... | [-0.20698298025067505, 0.13142840390240676, -0.0779032550605112, 0.05008802388451601, -0.03215354857966304, -0.1435587338907154, 0.11553516477150352, 0.2890962449882768, -0.2659117352964945, -0.25484414266814526, 0.04960851150956985, -0.3161325705923924, -0.06225697942274182, 0.22252510971830863, -0.09614574589619511, ... |
709.4433 | Isolated Leptons and Missing P_{T} at HERA | The search for events containing isolated leptons (electrons or muons) and
missing transverse momentum produced in e^{\pm}p collisions is performed
individually and in a common phase space with the H1 and ZEUS detectors at HERA
in the period 1994--2007. The analysed H1+ZEUS data sample corresponds to an
integrated lu... | hep-ex | the search for events containing isolated leptons electrons or muons and missing transverse momentum produced in epmp collisions is performed individually and in a common phase space with the h1 and zeus detectors at hera in the period 19942007 the analysed h1zeus data sample corresponds to an integrated luminosity of ... | [['the', 'search', 'for', 'events', 'containing', 'isolated', 'leptons', 'electrons', 'or', 'muons', 'and', 'missing', 'transverse', 'momentum', 'produced', 'in', 'epmp', 'collisions', 'is', 'performed', 'individually', 'and', 'in', 'a', 'common', 'phase', 'space', 'with', 'the', 'h1', 'and', 'zeus', 'detectors', 'at',... | [-0.06297764413207313, 0.18448254994362767, -0.04068257946926712, 0.1563895990342856, 0.0025270795449614525, -0.06740508444087318, 0.014051930760347678, 0.3507953643158901, -0.16043525378996837, -0.39082047760349475, 0.009631386896641067, -0.4359070447679221, 0.14536964848631867, 0.15592177065683563, 0.0881059903571485... |
709.4434 | Stout Smearing for Twisted Mass Fermions | The effect of Stout smearing is investigated in numerical simulations with
twisted mass Wilson quarks. The phase transition near zero quark mass is
studied on 12^3x24, 16^3x32 and 24^3x48 lattices at lattice spacings a = 0.1 -
0.125 fm.
| hep-lat | the effect of stout smearing is investigated in numerical simulations with twisted mass wilson quarks the phase transition near zero quark mass is studied on 123x24 163x32 and 243x48 lattices at lattice spacings a 01 0125 fm | [['the', 'effect', 'of', 'stout', 'smearing', 'is', 'investigated', 'in', 'numerical', 'simulations', 'with', 'twisted', 'mass', 'wilson', 'quarks', 'the', 'phase', 'transition', 'near', 'zero', 'quark', 'mass', 'is', 'studied', 'on', '123x24', '163x32', 'and', '243x48', 'lattices', 'at', 'lattice', 'spacings', 'a', '0... | [-0.1447925060685422, 0.36831475401649605, -0.051973111990436506, 0.07926147474554947, 0.03987839027635149, -0.11615412078822988, 0.13839838224324724, 0.46646444439082535, -0.10190810293361947, -0.21663230952706086, 0.09220437477405712, -0.32546932250261307, 0.03071003223492487, 0.04622947597228041, 0.05208558229276457... |
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