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 |
|---|---|---|---|---|---|---|
706.3214 | Reheating a multi-throat universe by brane motion | We propose a mechanism of reheating after inflation in multi-throat scenarios
of warped extra dimensions. Validity of an effective field theory on the
standard model (SM) brane requires that the position of the SM brane during
inflation be different from the position after inflation. The latter is
supposed to be near... | hep-th astro-ph gr-qc hep-ph | we propose a mechanism of reheating after inflation in multithroat scenarios of warped extra dimensions validity of an effective field theory on the standard model sm brane requires that the position of the sm brane during inflation be different from the position after inflation the latter is supposed to be near the ti... | [['we', 'propose', 'a', 'mechanism', 'of', 'reheating', 'after', 'inflation', 'in', 'multithroat', 'scenarios', 'of', 'warped', 'extra', 'dimensions', 'validity', 'of', 'an', 'effective', 'field', 'theory', 'on', 'the', 'standard', 'model', 'sm', 'brane', 'requires', 'that', 'the', 'position', 'of', 'the', 'sm', 'brane... | [-0.12316871304421746, 0.2661510727326282, -0.1038031598943616, 0.11037817510641029, -0.09658128692535684, -0.18583376905242463, 0.004812582614484258, 0.2846852049471871, -0.2624748004863279, -0.25205398776151633, 0.07405868173772169, -0.24551952867618493, -0.04353100616454838, 0.09471286054242463, -0.03583988365515676... |
706.3215 | Theory of the Nernst effect near quantum phase transitions in condensed
matter, and in dyonic black holes | We present a general hydrodynamic theory of transport in the vicinity of
superfluid-insulator transitions in two spatial dimensions described by
"Lorentz"-invariant quantum critical points. We allow for a weak impurity
scattering rate, a magnetic field B, and a deviation in the density, \rho, from
that of the insulat... | cond-mat.str-el cond-mat.supr-con hep-th | we present a general hydrodynamic theory of transport in the vicinity of superfluidinsulator transitions in two spatial dimensions described by lorentzinvariant quantum critical points we allow for a weak impurity scattering rate a magnetic field b and a deviation in the density rho from that of the insulator we show t... | [['we', 'present', 'a', 'general', 'hydrodynamic', 'theory', 'of', 'transport', 'in', 'the', 'vicinity', 'of', 'superfluidinsulator', 'transitions', 'in', 'two', 'spatial', 'dimensions', 'described', 'by', 'lorentzinvariant', 'quantum', 'critical', 'points', 'we', 'allow', 'for', 'a', 'weak', 'impurity', 'scattering', ... | [-0.14077828329941044, 0.15828018139231287, -0.0860213476645688, 0.0579547569688333, -0.027538858766595252, -0.1289720392624367, 0.0340075610502151, 0.3103208991796731, -0.22210162731793073, -0.24694427181477552, 0.051896296932732, -0.29705668982016303, -0.1393957873763831, 0.18201926091396714, 0.020636266977717616, 0.... |
706.3216 | Bubble-Wrap for Bullets: The Stability Imparted By A Thin Magnetic Layer | There has been significant recent work which examines a situation where a
thin magnetic layer is `draped' over a core merging into a larger cluster; the
same process also appears to be at work at a bubble rising from the cluster
centre. Such a thin magnetic layer could thermally isolate the core from the
cluster medi... | astro-ph physics.flu-dyn physics.plasm-ph | there has been significant recent work which examines a situation where a thin magnetic layer is draped over a core merging into a larger cluster the same process also appears to be at work at a bubble rising from the cluster centre such a thin magnetic layer could thermally isolate the core from the cluster medium but... | [['there', 'has', 'been', 'significant', 'recent', 'work', 'which', 'examines', 'a', 'situation', 'where', 'a', 'thin', 'magnetic', 'layer', 'is', 'draped', 'over', 'a', 'core', 'merging', 'into', 'a', 'larger', 'cluster', 'the', 'same', 'process', 'also', 'appears', 'to', 'be', 'at', 'work', 'at', 'a', 'bubble', 'risi... | [-0.12538322561460252, 0.21187364159916655, -0.0611340034813658, 0.033578849902886856, -0.08812915309090016, -0.09496220498491548, 0.016613851439556092, 0.3655666618407287, -0.28858832839478427, -0.28659881667680737, 0.11260689914319286, -0.2528698310006137, -0.07622024503761782, 0.19809919158403755, 0.0107071602279774... |
706.3217 | Convolution estimates and model surfaces of low codimension | We give examples of measures on certain k-surfaces in R^d. These measures
satisfy convolution estimates which are nearly optimal.
| math.CA | we give examples of measures on certain ksurfaces in rd these measures satisfy convolution estimates which are nearly optimal | [['we', 'give', 'examples', 'of', 'measures', 'on', 'certain', 'ksurfaces', 'in', 'rd', 'these', 'measures', 'satisfy', 'convolution', 'estimates', 'which', 'are', 'nearly', 'optimal']] | [-0.12042222828849365, 0.0964362034574151, -0.07080558050227792, 0.1435493117100314, 0.017941854502025404, -0.1539531593750182, 0.004546484615849822, 0.43005398562864255, -0.21829843962270962, -0.2009214351051732, 0.20082104862299993, -0.3457437632115264, -0.15331252105534077, 0.3069850243628025, -0.17788228186729707, ... |
706.3218 | Computing word length in alternate presentations of Thompson's group F | We introduce a new method for computing the word length of an element of
Thompson's group F with respect to a "consecutive" generating set of the form
X_n={x_0,x_1,...,x_n}, which is a subset of the standard infinite generating
set for F. We use this method to show that (F,X_n) is not almost convex, and
has pockets o... | math.GR | we introduce a new method for computing the word length of an element of thompsons group f with respect to a consecutive generating set of the form x_nx_0x_1x_n which is a subset of the standard infinite generating set for f we use this method to show that fx_n is not almost convex and has pockets of increasing though ... | [['we', 'introduce', 'a', 'new', 'method', 'for', 'computing', 'the', 'word', 'length', 'of', 'an', 'element', 'of', 'thompsons', 'group', 'f', 'with', 'respect', 'to', 'a', 'consecutive', 'generating', 'set', 'of', 'the', 'form', 'x_nx_0x_1x_n', 'which', 'is', 'a', 'subset', 'of', 'the', 'standard', 'infinite', 'gener... | [-0.1399286295918207, 0.11873743730628179, -0.058281870378601934, -0.01282410337702341, -0.07670633115565344, -0.09515523349475716, 0.0587552554019156, 0.38831261461300237, -0.3173529116977607, -0.22683698311166448, 0.06012411360749074, -0.3070787892286335, -0.1196903164475976, 0.23574671409122885, -0.08385289700761918... |
706.3219 | Universal Science of Complexity: Consistent Understanding of Ecological,
Living and Intelligent System Dynamics | A major challenge of interdisciplinary description of complex system
behaviour is whether real systems of higher complexity levels can be understood
with at least the same degree of objective, "scientific" rigour and
universality as "simple" systems of classical, Newtonian science paradigm. The
problem is reduced to ... | physics.gen-ph | a major challenge of interdisciplinary description of complex system behaviour is whether real systems of higher complexity levels can be understood with at least the same degree of objective scientific rigour and universality as simple systems of classical newtonian science paradigm the problem is reduced to that of a... | [['a', 'major', 'challenge', 'of', 'interdisciplinary', 'description', 'of', 'complex', 'system', 'behaviour', 'is', 'whether', 'real', 'systems', 'of', 'higher', 'complexity', 'levels', 'can', 'be', 'understood', 'with', 'at', 'least', 'the', 'same', 'degree', 'of', 'objective', 'scientific', 'rigour', 'and', 'univers... | [-0.16505969983546395, 0.10516318177962411, -0.08455743467883865, 0.10905961919579715, -0.07411753741373134, -0.14261346180143394, 0.022782600844918743, 0.2922357006899528, -0.29726103578913743, -0.3284642365155363, 0.07166817190567584, -0.21352736672719683, -0.2408278938184106, 0.18850008221683887, -0.0885509281907594... |
706.322 | Reionization and the large-scale 21 cm-cosmic microwave background cross
correlation | Of the many probes of reionization, the 21 cm line and the cosmic microwave
background (CMB) are among the most effective. We examine how the
cross-correlation of the 21 cm brightness and the CMB Doppler fluctuations on
large angular scales can be used to study this epoch. We employ a new model of
the growth of large... | astro-ph | of the many probes of reionization the 21 cm line and the cosmic microwave background cmb are among the most effective we examine how the crosscorrelation of the 21 cm brightness and the cmb doppler fluctuations on large angular scales can be used to study this epoch we employ a new model of the growth of large scale f... | [['of', 'the', 'many', 'probes', 'of', 'reionization', 'the', '21', 'cm', 'line', 'and', 'the', 'cosmic', 'microwave', 'background', 'cmb', 'are', 'among', 'the', 'most', 'effective', 'we', 'examine', 'how', 'the', 'crosscorrelation', 'of', 'the', '21', 'cm', 'brightness', 'and', 'the', 'cmb', 'doppler', 'fluctuations'... | [-0.1314781355337792, 0.15569838818417145, -0.08763496748756915, 0.1014273642480942, -0.07253523053605505, -0.0675293014135492, -0.029655656921038553, 0.36328631630208574, -0.23903218040961888, -0.2952107780868501, 0.09319334277219708, -0.3113714093661793, -0.0724684237997023, 0.18776151427764248, 0.04727820635863901, ... |
706.3221 | Curvature line parametrization from circle patterns | We study local and global approximations of smooth nets of curvature lines
and smooth conjugate nets by respective discrete nets (circular nets and planar
quadrilateral nets) with infinitesimal quads. It is shown that choosing the
points of discrete nets on the smooth surface one can obtain second-order
approximation... | math.DG | we study local and global approximations of smooth nets of curvature lines and smooth conjugate nets by respective discrete nets circular nets and planar quadrilateral nets with infinitesimal quads it is shown that choosing the points of discrete nets on the smooth surface one can obtain secondorder approximation globa... | [['we', 'study', 'local', 'and', 'global', 'approximations', 'of', 'smooth', 'nets', 'of', 'curvature', 'lines', 'and', 'smooth', 'conjugate', 'nets', 'by', 'respective', 'discrete', 'nets', 'circular', 'nets', 'and', 'planar', 'quadrilateral', 'nets', 'with', 'infinitesimal', 'quads', 'it', 'is', 'shown', 'that', 'cho... | [-0.11974194051088909, 0.020723845078968083, -0.06018944649169078, 0.07247138982996917, -0.08666060452277843, -0.15644914815202354, 0.0021884677931666373, 0.4264394149184227, -0.31680492277328787, -0.18584008354407092, 0.11386945504122055, -0.24467189595676386, -0.18397710884992893, 0.17078541770863992, -0.135024226542... |
706.3222 | The FIRST-2MASS Red Quasar Survey | Combining radio observations with optical and infrared color selection --
demonstrated in our pilot study to be an efficient selection algorithm for
finding red quasars -- we have obtained optical and infrared spectroscopy for
120 objects in a complete sample of 156 candidates from a sky area of 2716
square degrees. ... | astro-ph | combining radio observations with optical and infrared color selection demonstrated in our pilot study to be an efficient selection algorithm for finding red quasars we have obtained optical and infrared spectroscopy for 120 objects in a complete sample of 156 candidates from a sky area of 2716 square degrees consisten... | [['combining', 'radio', 'observations', 'with', 'optical', 'and', 'infrared', 'color', 'selection', 'demonstrated', 'in', 'our', 'pilot', 'study', 'to', 'be', 'an', 'efficient', 'selection', 'algorithm', 'for', 'finding', 'red', 'quasars', 'we', 'have', 'obtained', 'optical', 'and', 'infrared', 'spectroscopy', 'for', '... | [0.0016494103824918709, 0.06635438179484517, -0.06606301817550206, 0.081970009738602, -0.09985058494782509, -0.08309706641153151, 0.14356859440511788, 0.4968772636911859, -0.11418940182277951, -0.36381891164567, 0.06725050158430235, -0.35204165612654853, -0.023560689132970315, 0.22014999597896234, -0.06989932009154587,... |
706.3223 | Smooth maps of a foliated manifold in a symplectic manifold | The immersions of a smooth manifold $M$ in a symplectic manifold $(N,\sigma)$
inducing a given closed form $\omega$ on $M$ satisfy the $C^0$-dense
$h$-principle in the space of all continuous maps which pull back the deRham
cohomology class of $\sigma$ onto that of $\omega$. In this paper we prove a
foliated version ... | math.DG math.AP | the immersions of a smooth manifold m in a symplectic manifold nsigma inducing a given closed form omega on m satisfy the c0dense hprinciple in the space of all continuous maps which pull back the derham cohomology class of sigma onto that of omega in this paper we prove a foliated version of this result due to gromov | [['the', 'immersions', 'of', 'a', 'smooth', 'manifold', 'm', 'in', 'a', 'symplectic', 'manifold', 'nsigma', 'inducing', 'a', 'given', 'closed', 'form', 'omega', 'on', 'm', 'satisfy', 'the', 'c0dense', 'hprinciple', 'in', 'the', 'space', 'of', 'all', 'continuous', 'maps', 'which', 'pull', 'back', 'the', 'derham', 'cohom... | [-0.23659630097320367, 0.058992216797095945, -0.0882798650839912, 0.056308739140212276, -0.09429643999239237, -0.09759525935454615, 0.024360609303051926, 0.297443936611044, -0.30441571791367283, -0.1917554542165378, 0.05886834335376926, -0.2169302519378734, -0.15884083666003726, 0.15124527956680234, -0.1724399309284214... |
706.3224 | Fermi-Frenet coordinates for space-like curves | We generalize Fermi coordinates, which correspond to an adapted set of
coordinates describing the vicinity of an observer's worldline, to the
worldsheet of an arbitrary spatial curve in a static spacetime. The spatial
coordinate axes are fixed using a covariant Frenet triad so that the metric can
be expressed using t... | gr-qc | we generalize fermi coordinates which correspond to an adapted set of coordinates describing the vicinity of an observers worldline to the worldsheet of an arbitrary spatial curve in a static spacetime the spatial coordinate axes are fixed using a covariant frenet triad so that the metric can be expressed using the cur... | [['we', 'generalize', 'fermi', 'coordinates', 'which', 'correspond', 'to', 'an', 'adapted', 'set', 'of', 'coordinates', 'describing', 'the', 'vicinity', 'of', 'an', 'observers', 'worldline', 'to', 'the', 'worldsheet', 'of', 'an', 'arbitrary', 'spatial', 'curve', 'in', 'a', 'static', 'spacetime', 'the', 'spatial', 'coor... | [-0.18229483865937332, 0.10367897910965652, -0.15249108067817158, 0.04857687297619212, -0.1381082155391068, -0.10274731345405733, -0.06923877392654065, 0.3964306286961576, -0.26660193706414215, -0.2392100999476733, 0.0067365901217002555, -0.2139540262531811, -0.14712070918607492, 0.16177063306253173, -0.103780898495496... |
706.3225 | Seeking the best Internet Model | The models of the Internet reported in the literature are mainly aimed at
reproducing the scale-free structure, the high clustering coefficient and the
small world effects found in the real Internet, while other important
properties (e.g. related to centrality and hierarchical measurements) are not
considered. For a ... | physics.soc-ph | the models of the internet reported in the literature are mainly aimed at reproducing the scalefree structure the high clustering coefficient and the small world effects found in the real internet while other important properties eg related to centrality and hierarchical measurements are not considered for a better cha... | [['the', 'models', 'of', 'the', 'internet', 'reported', 'in', 'the', 'literature', 'are', 'mainly', 'aimed', 'at', 'reproducing', 'the', 'scalefree', 'structure', 'the', 'high', 'clustering', 'coefficient', 'and', 'the', 'small', 'world', 'effects', 'found', 'in', 'the', 'real', 'internet', 'while', 'other', 'important... | [-0.12074153412234138, 0.0460062860700025, -0.03629721173500592, 0.10215260806993733, -0.06395770119962509, -0.1249118178038279, 0.006165415797432935, 0.3739136258215719, -0.24424890002528382, -0.3357377501512953, 0.12085245342333675, -0.2987280751364557, -0.16974117326522853, 0.23631269292201143, -0.03245909837061992,... |
706.3226 | Convex Hull Realizations of the Multiplihedra | We present a simple algorithm for determining the extremal points in
Euclidean space whose convex hull is the nth polytope in the sequence known as
the multiplihedra. This answers the open question of whether the multiplihedra
could be realized as convex polytopes. We use this realization to unite the
approach to A_n... | math.AT math.CO math.CT | we present a simple algorithm for determining the extremal points in euclidean space whose convex hull is the nth polytope in the sequence known as the multiplihedra this answers the open question of whether the multiplihedra could be realized as convex polytopes we use this realization to unite the approach to a_nmaps... | [['we', 'present', 'a', 'simple', 'algorithm', 'for', 'determining', 'the', 'extremal', 'points', 'in', 'euclidean', 'space', 'whose', 'convex', 'hull', 'is', 'the', 'nth', 'polytope', 'in', 'the', 'sequence', 'known', 'as', 'the', 'multiplihedra', 'this', 'answers', 'the', 'open', 'question', 'of', 'whether', 'the', '... | [-0.09217663599430757, 0.06575840923114348, -0.05235620818012587, 0.0910823970818024, -0.06769189042812687, -0.0786862329232617, 0.03316860271112646, 0.344113627196116, -0.31350316476645107, -0.2537550898663447, 0.1319452630172452, -0.26201252963678057, -0.20684662204180546, 0.18422480083812595, -0.15783795434981585, 0... |
706.3227 | Final state interactions and hadron quenching in cold nuclear matter | I examine the role of final state interactions in cold nuclear matter in
modifying hadron production on nuclear targets with leptonic or hadronic beams.
I demonstrate the extent to which available experimental data in
electron-nucleus collisions can give direct information on final state effects
in hadron-nucleus and... | nucl-th hep-ex hep-ph | i examine the role of final state interactions in cold nuclear matter in modifying hadron production on nuclear targets with leptonic or hadronic beams i demonstrate the extent to which available experimental data in electronnucleus collisions can give direct information on final state effects in hadronnucleus and nucl... | [['i', 'examine', 'the', 'role', 'of', 'final', 'state', 'interactions', 'in', 'cold', 'nuclear', 'matter', 'in', 'modifying', 'hadron', 'production', 'on', 'nuclear', 'targets', 'with', 'leptonic', 'or', 'hadronic', 'beams', 'i', 'demonstrate', 'the', 'extent', 'to', 'which', 'available', 'experimental', 'data', 'in',... | [-0.015402446549547755, 0.2404284779306339, -0.21649835214028945, 0.1650269342829352, 0.008005644638172311, -0.10093275083876822, -0.07698403859268065, 0.3500746902888236, -0.18934063785911903, -0.2540533415163341, -0.07935777553458415, -0.3500253729765182, 0.16486078336703308, 0.09905662722480686, 0.08404621894106917,... |
706.3228 | Ohm's Law at strong coupling: S duality and the cyclotron resonance | We calculate the electrical and thermal conductivities and the thermoelectric
coefficient of a class of strongly interacting 2+1 dimensional conformal field
theories with anti-de Sitter space duals. We obtain these transport
coefficients as a function of charge density, background magnetic field,
temperature and freq... | hep-th cond-mat.str-el | we calculate the electrical and thermal conductivities and the thermoelectric coefficient of a class of strongly interacting 21 dimensional conformal field theories with antide sitter space duals we obtain these transport coefficients as a function of charge density background magnetic field temperature and frequency w... | [['we', 'calculate', 'the', 'electrical', 'and', 'thermal', 'conductivities', 'and', 'the', 'thermoelectric', 'coefficient', 'of', 'a', 'class', 'of', 'strongly', 'interacting', '21', 'dimensional', 'conformal', 'field', 'theories', 'with', 'antide', 'sitter', 'space', 'duals', 'we', 'obtain', 'these', 'transport', 'co... | [-0.17915028355838286, 0.18404496908333384, -0.04993987766848434, -0.019622728116588578, -0.08781783578119108, -0.09036652708780907, 0.014507414378403197, 0.3686381934033263, -0.24929814591471638, -0.2195499794646388, 0.05707050937870961, -0.30079190660977645, -0.1553051057559926, 0.220599646715536, 0.03577431627061395... |
706.3229 | Stringy product on twisted orbifold K-theory for abelian quotients | In this paper we present a model to calculate the stringy product on twisted
orbifold K-theory of Adem-Ruan-Zhang for abelian complex orbifolds.
In the first part we consider the non-twisted case on an orbifold presented
as the quotient of a manifold acted by a compact abelian Lie group. We give an
explicit descrip... | math.AT math.AG | in this paper we present a model to calculate the stringy product on twisted orbifold ktheory of ademruanzhang for abelian complex orbifolds in the first part we consider the nontwisted case on an orbifold presented as the quotient of a manifold acted by a compact abelian lie group we give an explicit description of th... | [['in', 'this', 'paper', 'we', 'present', 'a', 'model', 'to', 'calculate', 'the', 'stringy', 'product', 'on', 'twisted', 'orbifold', 'ktheory', 'of', 'ademruanzhang', 'for', 'abelian', 'complex', 'orbifolds', 'in', 'the', 'first', 'part', 'we', 'consider', 'the', 'nontwisted', 'case', 'on', 'an', 'orbifold', 'presented... | [-0.19199458382509907, 0.061891299430160494, -0.10167332712303975, 0.12050025036943884, -0.09974804420409532, -0.10353991168326344, -0.012482398004142631, 0.34407007960795327, -0.28463750413843786, -0.20812372742541904, 0.12826991021584977, -0.2079967224882145, -0.17765546077541236, 0.17768870781432708, -0.152856029043... |
706.323 | Steady states and linear stability analysis of precipitation pattern
formation at geothermal hot springs | A dynamical theory of geophysical precipitation pattern formation is
presented and applied to irreversible calcium carbonate (travertine)
deposition. Specific systems studied here are the terraces and domes observed
at geothermal hot springs, such as those at Yellowstone National Park, and
speleothems, particularly s... | nlin.PS cond-mat.soft physics.geo-ph | a dynamical theory of geophysical precipitation pattern formation is presented and applied to irreversible calcium carbonate travertine deposition specific systems studied here are the terraces and domes observed at geothermal hot springs such as those at yellowstone national park and speleothems particularly stalactit... | [['a', 'dynamical', 'theory', 'of', 'geophysical', 'precipitation', 'pattern', 'formation', 'is', 'presented', 'and', 'applied', 'to', 'irreversible', 'calcium', 'carbonate', 'travertine', 'deposition', 'specific', 'systems', 'studied', 'here', 'are', 'the', 'terraces', 'and', 'domes', 'observed', 'at', 'geothermal', '... | [-0.0958915361193846, 0.1762187788387169, -0.08385145401751454, 0.043607130467379, -0.029458390704045694, -0.10383021242674347, -0.015737783297398975, 0.30713147607207475, -0.2920156613114582, -0.2850605956692662, 0.08749362292174472, -0.32239669514114433, -0.1316488440139125, 0.1626370244864092, -0.014550145456774367,... |
706.3231 | World-sheet dynamics of ZZ branes | We show how non-compact space-time (ZZ branes) emerges as a limit of compact
space-time (FZZT branes) for specific ratios between the square of the boundary
cosmological constant and the bulk cosmological constant in the (2,2m-1)
minimal model coupled to two-dimensional quantum gravity.
| hep-th | we show how noncompact spacetime zz branes emerges as a limit of compact spacetime fzzt branes for specific ratios between the square of the boundary cosmological constant and the bulk cosmological constant in the 22m1 minimal model coupled to twodimensional quantum gravity | [['we', 'show', 'how', 'noncompact', 'spacetime', 'zz', 'branes', 'emerges', 'as', 'a', 'limit', 'of', 'compact', 'spacetime', 'fzzt', 'branes', 'for', 'specific', 'ratios', 'between', 'the', 'square', 'of', 'the', 'boundary', 'cosmological', 'constant', 'and', 'the', 'bulk', 'cosmological', 'constant', 'in', 'the', '2... | [-0.19211606954091362, 0.19156682200818545, -0.0314322876788321, 0.08705541471551571, -0.11013267326745249, -0.23494164857436858, -0.02542023421154313, 0.26703063894196283, -0.18676094852742695, -0.22906494477675074, 0.07190460997489503, -0.25866674436699777, -0.09873791949801325, 0.11684519431132469, -0.05566791736609... |
706.3232 | Asymptotic probability density functions in turbulence | A formalism is presented to obtain closed evolution equations for asymptotic
probability distribution functions of turbulence magnitudes. The formalism is
derived for a generic evolution equation, so that the final result can be
easily applied to rather general problems. Although the approximation involved
cannot be ... | physics.flu-dyn | a formalism is presented to obtain closed evolution equations for asymptotic probability distribution functions of turbulence magnitudes the formalism is derived for a generic evolution equation so that the final result can be easily applied to rather general problems although the approximation involved cannot be ascer... | [['a', 'formalism', 'is', 'presented', 'to', 'obtain', 'closed', 'evolution', 'equations', 'for', 'asymptotic', 'probability', 'distribution', 'functions', 'of', 'turbulence', 'magnitudes', 'the', 'formalism', 'is', 'derived', 'for', 'a', 'generic', 'evolution', 'equation', 'so', 'that', 'the', 'final', 'result', 'can'... | [-0.06667558710614685, 0.07558833403891185, -0.18054403027053922, 0.17125593938180828, -0.09552871307823807, -0.10981455764704151, 0.000873730648891069, 0.31987198944261763, -0.27428345644148067, -0.30483528798504267, 0.07075879598960455, -0.1770263637881726, -0.1741809135346557, 0.23745926952688023, -0.052470121896476... |
706.3233 | Origin of the X-ray Quasi-Periodic Oscillations and Identification of a
Transient Ultraluminous X-Ray Source in M82 | The starburst galaxy M82 contains two ultraluminous X-ray sources (ULXs),
CXOM82 J095550.2+694047 (=X41.4+60) and CXOM82 J095551.1+694045 (=X42.3+59),
which are unresolved by XMM-Newton. We revisited the two XMM-Newton
observations of M82 and analyzed the surface brightness profiles using the
known Chandra source pos... | astro-ph | the starburst galaxy m82 contains two ultraluminous xray sources ulxs cxom82 j0955502694047 x41460 and cxom82 j0955511694045 x42359 which are unresolved by xmmnewton we revisited the two xmmnewton observations of m82 and analyzed the surface brightness profiles using the known chandra source positions we show that the ... | [['the', 'starburst', 'galaxy', 'm82', 'contains', 'two', 'ultraluminous', 'xray', 'sources', 'ulxs', 'cxom82', 'j0955502694047', 'x41460', 'and', 'cxom82', 'j0955511694045', 'x42359', 'which', 'are', 'unresolved', 'by', 'xmmnewton', 'we', 'revisited', 'the', 'two', 'xmmnewton', 'observations', 'of', 'm82', 'and', 'ana... | [-0.09861719027355062, 0.09864191565788318, -0.054892355856229216, 0.14145352824417884, -0.11569874740885076, -0.08883305812695465, 0.05656198719808841, 0.44869958095990375, -0.129002686801416, -0.351737868266882, 0.12396285099040374, -0.3498639962523456, 0.0031058844831290742, 0.27246086020472543, -0.06781298970209731... |
706.3234 | Reverse engineering time discrete finite dynamical systems: A feasible
undertaking? | With the advent of high-throughput profiling methods, interest in reverse
engineering the structure and dynamics of biochemical networks is high.
Recently an algorithm for reverse engineering of biochemical networks was
developed by Laubenbacher and Stigler. It is a top-down approach using time
discrete dynamical sys... | q-bio.QM math.DS q-bio.MN | with the advent of highthroughput profiling methods interest in reverse engineering the structure and dynamics of biochemical networks is high recently an algorithm for reverse engineering of biochemical networks was developed by laubenbacher and stigler it is a topdown approach using time discrete dynamical systems on... | [['with', 'the', 'advent', 'of', 'highthroughput', 'profiling', 'methods', 'interest', 'in', 'reverse', 'engineering', 'the', 'structure', 'and', 'dynamics', 'of', 'biochemical', 'networks', 'is', 'high', 'recently', 'an', 'algorithm', 'for', 'reverse', 'engineering', 'of', 'biochemical', 'networks', 'was', 'developed'... | [-0.11073114160171826, 0.0680672323115914, -0.07026421567570651, 0.08931215973461804, -0.08939599088080286, -0.13165018008885454, 0.07109701777380906, 0.3552588699393482, -0.2852326720533256, -0.3033170688777318, 0.13392168805557958, -0.2544944487672183, -0.1635427007445287, 0.2355877739328207, -0.08471988993557034, 0.... |
706.3235 | Tau and muon pair production cross-sections in electron-positron
annihilations at sqrt{s} = 10.58 GeV | The calculational precision of $\ee\to\tautau$ and $\ee\to\mumu$ production
cross-sections in electron-positron annihilations at \roots = 10.58 \gev are
studied for the \kk Monte Carlo simulation program. We determine
$\sigma(\ee\to\tautau) = (0.919 \pm 0.003) \nb$ and $\sigma(\ee\to\mumu) =
(1.147 \pm 0.005) \nb$, w... | hep-ph | the calculational precision of eetotautau and eetomumu production crosssections in electronpositron annihilations at roots 1058 gev are studied for the kk monte carlo simulation program we determine sigmaeetotautau 0919 pm 0003 nb and sigmaeetomumu 1147 pm 0005 nb where the error represents the precision of the calcula... | [['the', 'calculational', 'precision', 'of', 'eetotautau', 'and', 'eetomumu', 'production', 'crosssections', 'in', 'electronpositron', 'annihilations', 'at', 'roots', '1058', 'gev', 'are', 'studied', 'for', 'the', 'kk', 'monte', 'carlo', 'simulation', 'program', 'we', 'determine', 'sigmaeetotautau', '0919', 'pm', '0003... | [-0.08026074557247656, 0.1432325512340123, -0.06812116671988572, 0.1206732124555856, 0.08506361727433448, -0.09945769849317995, 0.05825745902786201, 0.31422743839026557, -0.1667327325664122, -0.369555534413931, -0.02658825003891252, -0.42245516705919395, 0.1734095850790089, 0.2241201975994045, 0.07352901258590547, 0.09... |
706.3236 | Measurement of Aerosols at the Pierre Auger Observatory | The air fluorescence detectors (FDs) of the Pierre Auger Observatory are
vital for the determination of the air shower energy scale. To compensate for
variations in atmospheric conditions that affect the energy measurement, the
Observatory operates an array of monitoring instruments to record hourly
atmospheric condi... | astro-ph | the air fluorescence detectors fds of the pierre auger observatory are vital for the determination of the air shower energy scale to compensate for variations in atmospheric conditions that affect the energy measurement the observatory operates an array of monitoring instruments to record hourly atmospheric conditions ... | [['the', 'air', 'fluorescence', 'detectors', 'fds', 'of', 'the', 'pierre', 'auger', 'observatory', 'are', 'vital', 'for', 'the', 'determination', 'of', 'the', 'air', 'shower', 'energy', 'scale', 'to', 'compensate', 'for', 'variations', 'in', 'atmospheric', 'conditions', 'that', 'affect', 'the', 'energy', 'measurement',... | [-0.10133747316151857, 0.22269266252801753, -0.06486145921051502, 0.07595671006571501, 0.018830969120375813, -0.07532475574500859, -0.01443245271127671, 0.41993426203727724, -0.23048511351644993, -0.37980522167682645, 0.08907353791873902, -0.33437068843841555, -0.0313624652326107, 0.23753252019174398, -0.01514833047240... |
706.3237 | Blow-up of Electric Fields between Closely Spaced Spherical Perfect
Conductors | The electric field increases toward infinity in the narrow region between
closely adjacent perfect conductors as they approach each other. Much attention
has been devoted to the blow-up estimate, especially in two dimensions, for the
practical relevance to high stress concentration in fiber-reinforced elastic
composi... | math.AP math-ph math.MP | the electric field increases toward infinity in the narrow region between closely adjacent perfect conductors as they approach each other much attention has been devoted to the blowup estimate especially in two dimensions for the practical relevance to high stress concentration in fiberreinforced elastic composites in ... | [['the', 'electric', 'field', 'increases', 'toward', 'infinity', 'in', 'the', 'narrow', 'region', 'between', 'closely', 'adjacent', 'perfect', 'conductors', 'as', 'they', 'approach', 'each', 'other', 'much', 'attention', 'has', 'been', 'devoted', 'to', 'the', 'blowup', 'estimate', 'especially', 'in', 'two', 'dimensions... | [-0.1324991728324676, 0.11425224029032204, -0.025769777936602623, 0.06429715798003599, -0.03305897201304712, -0.13285206674481742, -0.005687348727709225, 0.3970073146629147, -0.24604658762109466, -0.26777952106203884, 0.08219473717690562, -0.2869833778240718, -0.11175047789644547, 0.18464461771266846, -0.06986911337632... |
706.3238 | Perturbation theory of spherically symmetric self-similar black holes | The theory of perturbations of spherically symmetric self-similar black holes
is presented, in the Newman-Penrose formalism. It is shown that the wave
equations for gravitational, electromagnetic, and scalar waves are separable,
though not decoupled. A generalization of the Teukolsky equation is given.
Monopole and d... | gr-qc astro-ph | the theory of perturbations of spherically symmetric selfsimilar black holes is presented in the newmanpenrose formalism it is shown that the wave equations for gravitational electromagnetic and scalar waves are separable though not decoupled a generalization of the teukolsky equation is given monopole and dipole modes... | [['the', 'theory', 'of', 'perturbations', 'of', 'spherically', 'symmetric', 'selfsimilar', 'black', 'holes', 'is', 'presented', 'in', 'the', 'newmanpenrose', 'formalism', 'it', 'is', 'shown', 'that', 'the', 'wave', 'equations', 'for', 'gravitational', 'electromagnetic', 'and', 'scalar', 'waves', 'are', 'separable', 'th... | [-0.23155876018378574, 0.1936465710401535, -0.058618489257059994, 0.14271057620450545, -0.13806604468263686, -0.12835161045659332, -0.17564754934088947, 0.27164278641963996, -0.18122604849437873, -0.18649449093888204, 0.025361197230328494, -0.290717823492984, -0.17386684069254746, 0.15516227410795788, 0.101127318991348... |
706.3239 | Black hole entropy, curved space and monsters | We investigate the microscopic origin of black hole entropy, in particular
the gap between the maximum entropy of ordinary matter and that of black holes.
Using curved space, we construct configurations with entropy greater than their
area in Planck units. These configurations have pathological properties and we
refe... | hep-th gr-qc hep-ph | we investigate the microscopic origin of black hole entropy in particular the gap between the maximum entropy of ordinary matter and that of black holes using curved space we construct configurations with entropy greater than their area in planck units these configurations have pathological properties and we refer to t... | [['we', 'investigate', 'the', 'microscopic', 'origin', 'of', 'black', 'hole', 'entropy', 'in', 'particular', 'the', 'gap', 'between', 'the', 'maximum', 'entropy', 'of', 'ordinary', 'matter', 'and', 'that', 'of', 'black', 'holes', 'using', 'curved', 'space', 'we', 'construct', 'configurations', 'with', 'entropy', 'great... | [-0.13010438436206154, 0.16220504681637132, -0.08614918293323422, 0.1513483474145819, -0.043669700787902097, -0.13407139335860216, 0.05139091763092016, 0.25685130517619353, -0.18526889023411533, -0.33973947369857976, 0.08919704046549168, -0.3708886199603802, -0.08275008400011322, 0.20354395487642699, -0.067060898901705... |
706.324 | Spin current and electrical polarization in GaN double-barrier
structures | Tunnel spin polarization in a piezoelectric AlGaN/GaN double barrier
structure is calculated. It is shown that the piezoelectric field and the
spontaneous electrical polarization increase an efficiency of the tunnel spin
injection. The relation between the electrical polarization and the spin
orientation allows engin... | cond-mat.other | tunnel spin polarization in a piezoelectric algangan double barrier structure is calculated it is shown that the piezoelectric field and the spontaneous electrical polarization increase an efficiency of the tunnel spin injection the relation between the electrical polarization and the spin orientation allows engineerin... | [['tunnel', 'spin', 'polarization', 'in', 'a', 'piezoelectric', 'algangan', 'double', 'barrier', 'structure', 'is', 'calculated', 'it', 'is', 'shown', 'that', 'the', 'piezoelectric', 'field', 'and', 'the', 'spontaneous', 'electrical', 'polarization', 'increase', 'an', 'efficiency', 'of', 'the', 'tunnel', 'spin', 'injec... | [-0.2284412401553709, 0.21146286532408945, 0.0005436286175002654, -0.03700076920213178, -0.052102169999852774, -0.12362483836865673, -0.0014674406047561206, 0.43593518659472463, -0.33721972287942964, -0.30282854263981185, -0.04095531899559622, -0.25014919328605173, -0.08690110913788279, 0.2494403463167449, 0.0923505131... |
706.3241 | Phenomenological features in a model with non-universal gaugino CP
phases | We study phenomenological features in an extended gauge mediation SUSY
breaking model which has non-universal gaugino masses and CP phases. We show
that large CP phases in soft SUSY breaking parameters can be consistent with
the constraints coming from the electric dipole moment (EDM) of an electron, a
neutron, and a... | hep-ph | we study phenomenological features in an extended gauge mediation susy breaking model which has nonuniversal gaugino masses and cp phases we show that large cp phases in soft susy breaking parameters can be consistent with the constraints coming from the electric dipole moment edm of an electron a neutron and also a me... | [['we', 'study', 'phenomenological', 'features', 'in', 'an', 'extended', 'gauge', 'mediation', 'susy', 'breaking', 'model', 'which', 'has', 'nonuniversal', 'gaugino', 'masses', 'and', 'cp', 'phases', 'we', 'show', 'that', 'large', 'cp', 'phases', 'in', 'soft', 'susy', 'breaking', 'parameters', 'can', 'be', 'consistent'... | [-0.11244491292990605, 0.3037490996460879, -0.022476273893474417, 0.15501874046199998, -0.11057988874544607, -0.17386625973490355, 0.021781021294458202, 0.36509820895495815, -0.20022292332027422, -0.317326598600528, 0.05490034764684806, -0.26630473633026963, -0.02238299352961166, 0.12530288905793122, 0.0136620652574662... |
706.3242 | Quantum decay rates in chaotic scattering | In this article we prove that for a large class of operators, including
Schroedinger operators, with hyperbolic classical flows, the smallness of
dimension of the trapped set implies that there is a gap between the resonances
and the real axis. In other words, the quantum decay rate is bounded from below
if the class... | math-ph math.MP math.SP | in this article we prove that for a large class of operators including schroedinger operators with hyperbolic classical flows the smallness of dimension of the trapped set implies that there is a gap between the resonances and the real axis in other words the quantum decay rate is bounded from below if the classical re... | [['in', 'this', 'article', 'we', 'prove', 'that', 'for', 'a', 'large', 'class', 'of', 'operators', 'including', 'schroedinger', 'operators', 'with', 'hyperbolic', 'classical', 'flows', 'the', 'smallness', 'of', 'dimension', 'of', 'the', 'trapped', 'set', 'implies', 'that', 'there', 'is', 'a', 'gap', 'between', 'the', '... | [-0.138781177430329, 0.15270931216681757, -0.053791885594943196, 0.08505372182249134, -0.05228317018852315, -0.10669216524481519, 0.009393528388582954, 0.30530952103435993, -0.2751122096722776, -0.20860359311336651, 0.10011785723856353, -0.30882562868646346, -0.12449955862790706, 0.2126308500731036, -0.0727039668087276... |
706.3243 | Quark deconfinement in neutron star cores and the ground state of
neutral matter | Whether or not deconfined quark phase exists in neutron star cores and
represents the ground state of neutral matter at moderate densities are open
questions. We use two realistic effective quark models, the three-flavor
Nambu-Jona-Lasinio model and the modified quark-meson coupling model, to
describe the neutron sta... | astro-ph | whether or not deconfined quark phase exists in neutron star cores and represents the ground state of neutral matter at moderate densities are open questions we use two realistic effective quark models the threeflavor nambujonalasinio model and the modified quarkmeson coupling model to describe the neutron star matter ... | [['whether', 'or', 'not', 'deconfined', 'quark', 'phase', 'exists', 'in', 'neutron', 'star', 'cores', 'and', 'represents', 'the', 'ground', 'state', 'of', 'neutral', 'matter', 'at', 'moderate', 'densities', 'are', 'open', 'questions', 'we', 'use', 'two', 'realistic', 'effective', 'quark', 'models', 'the', 'threeflavor'... | [-0.08666473749562065, 0.3201527197850664, -0.08525928288612063, 0.12244694316783258, -0.10748988774072142, -0.13029632436359204, 0.12483199470477298, 0.33745100429938363, -0.11996075673690981, -0.317833563501306, 0.009730440703075315, -0.31396808806333065, 0.027608252458834234, 0.07717599091389232, 0.04642312922057388... |
706.3244 | A non-perturbative study of non-commutative U(1) gauge theory | We study U(1) gauge theory on a 4d non-commutative torus, where two
directions are non-commutative. Monte Carlo simulations are performed after
mapping the regularized theory onto a U(N) lattice gauge theory in d=2. At
intermediate coupling strength, we find a phase in which open Wilson lines
acquire non-zero vacuum ... | hep-th hep-lat | we study u1 gauge theory on a 4d noncommutative torus where two directions are noncommutative monte carlo simulations are performed after mapping the regularized theory onto a un lattice gauge theory in d2 at intermediate coupling strength we find a phase in which open wilson lines acquire nonzero vacuum expectation va... | [['we', 'study', 'u1', 'gauge', 'theory', 'on', 'a', '4d', 'noncommutative', 'torus', 'where', 'two', 'directions', 'are', 'noncommutative', 'monte', 'carlo', 'simulations', 'are', 'performed', 'after', 'mapping', 'the', 'regularized', 'theory', 'onto', 'a', 'un', 'lattice', 'gauge', 'theory', 'in', 'd2', 'at', 'interm... | [-0.18921072278344245, 0.23980523256102093, -0.0897304540310331, 0.09218416041241856, -0.04353893339349371, -0.17024965824869773, 0.049716937955020475, 0.36046180151471935, -0.21250635625539063, -0.2417856389225495, 0.05793397730384539, -0.24468512815440557, -0.15447580805091463, 0.0868497804083206, 0.03879039197797990... |
706.3245 | The total energy-momentum of the universe in teleparallel gravity | We investigate the conservation law of energy-momentum in teleparallel
gravity by using general Noether theorem. The energy-momentum current has also
superpotential and is therefore identically conserved. The total
energy-momentum, which includes the contributions of both matter and
gravitational fields, is given by ... | gr-qc | we investigate the conservation law of energymomentum in teleparallel gravity by using general noether theorem the energymomentum current has also superpotential and is therefore identically conserved the total energymomentum which includes the contributions of both matter and gravitational fields is given by the integ... | [['we', 'investigate', 'the', 'conservation', 'law', 'of', 'energymomentum', 'in', 'teleparallel', 'gravity', 'by', 'using', 'general', 'noether', 'theorem', 'the', 'energymomentum', 'current', 'has', 'also', 'superpotential', 'and', 'is', 'therefore', 'identically', 'conserved', 'the', 'total', 'energymomentum', 'whic... | [-0.23461110803764312, 0.1535868096180767, -0.0869285071378245, 0.07953326156472458, -0.12376047551412793, -0.12093167673686848, -0.1409131478942821, 0.24866110686870183, -0.18748792752842694, -0.2751299001495628, -0.0012603063547216794, -0.26512527573196326, -0.10866521055919721, 0.09756897880750544, -0.02210147022543... |
706.3246 | On finite groups whose derived subgroup has bounded rank | Let $G$ be a finite group with derived subgroup of rank $r$. We prove that
$\gzz\leq |G'|^{2r}$. Motivated by the results of I. M. Isaacs in \cite{isa} we
show that if $G$ is capable then $\gz\leq |G'|^{4r}$. This answers a question
of L. Pyber. We prove that if $G$ is a capable $p$-group then the rank of
$G/\mathbf{... | math.GR | let g be a finite group with derived subgroup of rank r we prove that gzzleq g2r motivated by the results of i m isaacs in citeisa we show that if g is capable then gzleq g4r this answers a question of l pyber we prove that if g is a capable pgroup then the rank of gmathbfzg is bounded above in terms of the rank of g | [['let', 'g', 'be', 'a', 'finite', 'group', 'with', 'derived', 'subgroup', 'of', 'rank', 'r', 'we', 'prove', 'that', 'gzzleq', 'g2r', 'motivated', 'by', 'the', 'results', 'of', 'i', 'm', 'isaacs', 'in', 'citeisa', 'we', 'show', 'that', 'if', 'g', 'is', 'capable', 'then', 'gzleq', 'g4r', 'this', 'answers', 'a', 'questio... | [-0.17283372081343143, 0.13471542246314505, -0.07780108837381242, -0.014088483035771383, -0.08120903862817656, -0.15840220768448143, 0.02605679850020106, 0.34019447798057206, -0.3021678585145209, -0.25333319790661335, 0.07551328821979936, -0.23566466933559804, -0.14622713785086358, 0.18520826770598808, -0.1550483595698... |
706.3247 | Relativistic rapidity as change in musical pitch | Relativistic rapidity is usually presented as a computational device. As
Levy-Leblond has shown, it is also the velocity that would be imputed by an
ideal Newtonian inertial guidance system, taking c=1*neper=1. Here, we show
that it can also be interpreted as the change in musical pitch of radiation
fore and aft alon... | physics.gen-ph | relativistic rapidity is usually presented as a computational device as levyleblond has shown it is also the velocity that would be imputed by an ideal newtonian inertial guidance system taking c1neper1 here we show that it can also be interpreted as the change in musical pitch of radiation fore and aft along the direc... | [['relativistic', 'rapidity', 'is', 'usually', 'presented', 'as', 'a', 'computational', 'device', 'as', 'levyleblond', 'has', 'shown', 'it', 'is', 'also', 'the', 'velocity', 'that', 'would', 'be', 'imputed', 'by', 'an', 'ideal', 'newtonian', 'inertial', 'guidance', 'system', 'taking', 'c1neper1', 'here', 'we', 'show', ... | [-0.0784096099076454, 0.16714667700977193, -0.1530227395621213, 0.06338753148659386, -0.11082810092378746, -0.11869603880596431, -0.08624951019883156, 0.42546175921505147, -0.31617165292528543, -0.2883583136580207, 0.06737022220199419, -0.2143056396140971, -0.13442674810913477, 0.244403139738874, -0.11979520020329139, ... |
706.3248 | Compensation of the Crossing Angle with Crab Cavities at KEKB | Crab cavities have been installed in the KEKB B--Factory rings to compensate
the crossing angle at the collision point and thus increase luminosity. The
beam operation with crab crossing has been done since February 2007. This is
the first experience with such cavities in colliders or storage rings. The crab
cavities... | physics.ins-det | crab cavities have been installed in the kekb bfactory rings to compensate the crossing angle at the collision point and thus increase luminosity the beam operation with crab crossing has been done since february 2007 this is the first experience with such cavities in colliders or storage rings the crab cavities have b... | [['crab', 'cavities', 'have', 'been', 'installed', 'in', 'the', 'kekb', 'bfactory', 'rings', 'to', 'compensate', 'the', 'crossing', 'angle', 'at', 'the', 'collision', 'point', 'and', 'thus', 'increase', 'luminosity', 'the', 'beam', 'operation', 'with', 'crab', 'crossing', 'has', 'been', 'done', 'since', 'february', '20... | [-0.10203559237911745, 0.08540711883041593, -0.08445075464457917, 0.02485304110378809, -0.08216185194014768, -0.18301564557362854, -0.016146361474292697, 0.46092625291742106, -0.15793571952316496, -0.38160365474996744, 0.12122527230818422, -0.28694826303291376, 0.023340630457150163, 0.20539331562345686, -0.044809951648... |
706.3249 | Multiplicity free expansions of Schur $P$-functions | After deriving inequalities on coefficients arising in the expansion of a
Schur $P$-function in terms of Schur functions we give criteria for when such
expansions are multiplicity free. From here we study the multiplicity of an
irreducible spin character of the twisted symmetric group in the product of a
basic spin c... | math.CO | after deriving inequalities on coefficients arising in the expansion of a schur pfunction in terms of schur functions we give criteria for when such expansions are multiplicity free from here we study the multiplicity of an irreducible spin character of the twisted symmetric group in the product of a basic spin charact... | [['after', 'deriving', 'inequalities', 'on', 'coefficients', 'arising', 'in', 'the', 'expansion', 'of', 'a', 'schur', 'pfunction', 'in', 'terms', 'of', 'schur', 'functions', 'we', 'give', 'criteria', 'for', 'when', 'such', 'expansions', 'are', 'multiplicity', 'free', 'from', 'here', 'we', 'study', 'the', 'multiplicity'... | [-0.14296901769546874, 0.13474454953892975, -0.13017277974190553, 0.027826839003281027, -0.047532932860637776, -0.049166831994123424, -0.051325583747073786, 0.3404662239351379, -0.302812733506756, -0.1771573031237766, 0.10199468975031832, -0.24321281198245376, -0.12301736477929265, 0.2103611153008333, -0.03290669304499... |
706.325 | Compact symmetric solutions to the postage stamp problem | We derive lower and upper bounds on possible growth rates of certain sets of
positive integers $A_k=\{1= a_1 < a_2 < ... < a_{k}\}$ such that all integers
$n\in \{0, 1, 2, ..., ka_{k}\}$ can be represented as a sum of no more than $k$
elements of $A_k$, with repetition.
| math.NT | we derive lower and upper bounds on possible growth rates of certain sets of positive integers a_k1 a_1 a_2 a_k such that all integers nin 0 1 2 ka_k can be represented as a sum of no more than k elements of a_k with repetition | [['we', 'derive', 'lower', 'and', 'upper', 'bounds', 'on', 'possible', 'growth', 'rates', 'of', 'certain', 'sets', 'of', 'positive', 'integers', 'a_k1', 'a_1', 'a_2', 'a_k', 'such', 'that', 'all', 'integers', 'nin', '0', '1', '2', 'ka_k', 'can', 'be', 'represented', 'as', 'a', 'sum', 'of', 'no', 'more', 'than', 'k', 'e... | [-0.22739835314992393, 0.20190959131683817, 0.023889506394466895, 0.027793067909607835, 0.009004928351549263, -0.22126260077030482, 0.033406734339554205, 0.3508228205080906, -0.26417724118800834, -0.2099422887920148, 0.1069796823959967, -0.3151533366815949, -0.08920918540521101, 0.23565983337837018, 0.00228595769625495... |
706.3251 | On tensor products of polynomial representations | We determine the necessary and sufficient combinatorial conditions for which
the tensor product of two irreducible polynomial representations of
$GL(n,\mathbb{C})$ is isomorphic to another. As a consequence we discover
families of Littlewood-Richardson coefficients that are non-zero, and a
condition on Schur non-nega... | math.CO | we determine the necessary and sufficient combinatorial conditions for which the tensor product of two irreducible polynomial representations of glnmathbbc is isomorphic to another as a consequence we discover families of littlewoodrichardson coefficients that are nonzero and a condition on schur nonnegativity | [['we', 'determine', 'the', 'necessary', 'and', 'sufficient', 'combinatorial', 'conditions', 'for', 'which', 'the', 'tensor', 'product', 'of', 'two', 'irreducible', 'polynomial', 'representations', 'of', 'glnmathbbc', 'is', 'isomorphic', 'to', 'another', 'as', 'a', 'consequence', 'we', 'discover', 'families', 'of', 'li... | [-0.16122544139978431, 0.09977982337364838, -0.09780557427023139, 0.05887504333181174, -0.15697629518607364, -0.15483472365442486, -0.043408421239638256, 0.3233689833432436, -0.3602592745529754, -0.18548838589118705, 0.1570117801228272, -0.1844183752047164, -0.2037042597574847, 0.14683055263456135, -0.08236971331228103... |
706.3252 | Quantum thermal transport from classical molecular dynamics | Using a generalized Langevin equation of motion, quantum ballistic thermal
transport is obtained from classical molecular dynamics. This is possible
because the heat baths are represented by random noises obeying quantum
Bose-Einstein statistics. The numerical method gives asymptotically exact
results in both the low... | cond-mat.stat-mech | using a generalized langevin equation of motion quantum ballistic thermal transport is obtained from classical molecular dynamics this is possible because the heat baths are represented by random noises obeying quantum boseeinstein statistics the numerical method gives asymptotically exact results in both the lowtemper... | [['using', 'a', 'generalized', 'langevin', 'equation', 'of', 'motion', 'quantum', 'ballistic', 'thermal', 'transport', 'is', 'obtained', 'from', 'classical', 'molecular', 'dynamics', 'this', 'is', 'possible', 'because', 'the', 'heat', 'baths', 'are', 'represented', 'by', 'random', 'noises', 'obeying', 'quantum', 'bosee... | [-0.12786393084508532, 0.20480278151328948, -0.1400545093614389, 0.05212048980790902, -0.0353644088451641, -0.20442577353404726, 0.024039964884629145, 0.29638220553888994, -0.347355712270912, -0.20102335666032398, 0.003090474323150428, -0.31034932361148737, -0.1585580658825005, 0.26143637075472403, 0.02041763637543601,... |
706.3253 | Schur positivity of skew Schur function differences and applications to
ribbons and Schubert classes | Some new relations on skew Schur function differences are established both
combinatorially using Sch\"utzenberger's jeu de taquin, and algebraically using
Jacobi-Trudi determinants. These relations lead to the conclusion that certain
differences of skew Schur functions are Schur positive. Applying these results
to a ... | math.CO | some new relations on skew schur function differences are established both combinatorially using schutzenbergers jeu de taquin and algebraically using jacobitrudi determinants these relations lead to the conclusion that certain differences of skew schur functions are schur positive applying these results to a basis of ... | [['some', 'new', 'relations', 'on', 'skew', 'schur', 'function', 'differences', 'are', 'established', 'both', 'combinatorially', 'using', 'schutzenbergers', 'jeu', 'de', 'taquin', 'and', 'algebraically', 'using', 'jacobitrudi', 'determinants', 'these', 'relations', 'lead', 'to', 'the', 'conclusion', 'that', 'certain', ... | [-0.17087009284636248, 0.05980048733219117, -0.12527578567190992, 0.1435327068902552, -0.13151256024063407, -0.13122555684274087, 0.0125027270140973, 0.3439624478266417, -0.32538102339808045, -0.1873450798357462, 0.09694326088866581, -0.20444975505195945, -0.25624772606344964, 0.23145115675477237, -0.10856502007257629,... |
706.3254 | Numerical Linked-Cluster Algorithms. I. Spin systems on square,
triangular, and kagome lattices | We discuss recently introduced numerical linked-cluster (NLC) algorithms that
allow one to obtain temperature-dependent properties of quantum lattice models,
in the thermodynamic limit, from exact diagonalization of finite clusters. We
present studies of thermodynamic observables for spin models on square,
triangular... | cond-mat.stat-mech cond-mat.str-el | we discuss recently introduced numerical linkedcluster nlc algorithms that allow one to obtain temperaturedependent properties of quantum lattice models in the thermodynamic limit from exact diagonalization of finite clusters we present studies of thermodynamic observables for spin models on square triangular and kagom... | [['we', 'discuss', 'recently', 'introduced', 'numerical', 'linkedcluster', 'nlc', 'algorithms', 'that', 'allow', 'one', 'to', 'obtain', 'temperaturedependent', 'properties', 'of', 'quantum', 'lattice', 'models', 'in', 'the', 'thermodynamic', 'limit', 'from', 'exact', 'diagonalization', 'of', 'finite', 'clusters', 'we',... | [-0.08607701679915716, 0.1159853890169201, -0.09054742348028945, 0.0738286514415621, -0.03888165234711091, -0.12867099551466415, 0.07815338732270559, 0.42628267502306766, -0.1826835101435207, -0.24000401053366796, 0.11596827804580999, -0.3400610442106384, -0.13548997701760732, 0.2674591046783256, 0.10040514661825069, 0... |
706.3255 | Numerical Linked-Cluster Algorithms. II. t-J models on the square
lattice | We discuss the application of a recently introduced numerical linked-cluster
(NLC) algorithm to strongly correlated itinerant models. In particular, we
present a study of thermodynamic observables: chemical potential, entropy,
specific heat, and uniform susceptibility for the t-J model on the square
lattice, with J/t... | cond-mat.str-el cond-mat.stat-mech | we discuss the application of a recently introduced numerical linkedcluster nlc algorithm to strongly correlated itinerant models in particular we present a study of thermodynamic observables chemical potential entropy specific heat and uniform susceptibility for the tj model on the square lattice with jt05 and 03 our ... | [['we', 'discuss', 'the', 'application', 'of', 'a', 'recently', 'introduced', 'numerical', 'linkedcluster', 'nlc', 'algorithm', 'to', 'strongly', 'correlated', 'itinerant', 'models', 'in', 'particular', 'we', 'present', 'a', 'study', 'of', 'thermodynamic', 'observables', 'chemical', 'potential', 'entropy', 'specific', ... | [-0.060728506335327705, 0.11832508516137398, -0.07549318412108527, 0.05179774724585455, -0.033289324533524775, -0.144111440445657, 0.1205844250995846, 0.4334328810293828, -0.19306729279173118, -0.27263248585832994, 0.09086326091088384, -0.35521174708922065, -0.11820492861818732, 0.2279282054063984, 0.038887258138387434... |
706.3256 | Dynamics of Alpha-Helix Formation in the CSAW Model | We study the folding dynamics of polyalanine (Ala$_{20}$), a protein fragment
with 20 residues whose native state is a single alpha helix. We use the CSAW
model (conditioned self-avoiding walk), which treats the protein molecule as a
chain in Brownian motion, with interactions that include hydrophobic forces and
inte... | cond-mat.soft | we study the folding dynamics of polyalanine ala_20 a protein fragment with 20 residues whose native state is a single alpha helix we use the csaw model conditioned selfavoiding walk which treats the protein molecule as a chain in brownian motion with interactions that include hydrophobic forces and internal hydrogen b... | [['we', 'study', 'the', 'folding', 'dynamics', 'of', 'polyalanine', 'ala_20', 'a', 'protein', 'fragment', 'with', '20', 'residues', 'whose', 'native', 'state', 'is', 'a', 'single', 'alpha', 'helix', 'we', 'use', 'the', 'csaw', 'model', 'conditioned', 'selfavoiding', 'walk', 'which', 'treats', 'the', 'protein', 'molecul... | [-0.14604197541188638, 0.21773160157157442, -0.060739347196708954, 0.07289198667237187, -0.027492127116864263, -0.12885709126061617, 0.010476842953752473, 0.3638921847874772, -0.3230484285218231, -0.25266326018692964, 0.044419454555698054, -0.24954918401031675, -0.15630193435886908, 0.10622941553237517, 0.0796253982757... |
706.3257 | The Effects of Metallicity and AGN Activity on the Mid-Infrared Dust
Emission of Galaxies | Using a sample of the $Spitzer$ SWIRE-field galaxies whose optical spectra
are taken from the Data Release 4 of the Sloan Digital Sky Survey, we study
possible correlations between the Mid-InfraRed (MIR) dust emission from these
galaxies and both their metallicities and AGN activities. We find that both
metallicity a... | astro-ph | using a sample of the spitzer swirefield galaxies whose optical spectra are taken from the data release 4 of the sloan digital sky survey we study possible correlations between the midinfrared mir dust emission from these galaxies and both their metallicities and agn activities we find that both metallicity and agn act... | [['using', 'a', 'sample', 'of', 'the', 'spitzer', 'swirefield', 'galaxies', 'whose', 'optical', 'spectra', 'are', 'taken', 'from', 'the', 'data', 'release', '4', 'of', 'the', 'sloan', 'digital', 'sky', 'survey', 'we', 'study', 'possible', 'correlations', 'between', 'the', 'midinfrared', 'mir', 'dust', 'emission', 'from... | [-0.04715192966955149, 0.16140509118414464, -0.03023285490614692, 0.12456571646621377, -0.024733900217207398, -0.054364604893778486, 0.0394378517778209, 0.47407779857281623, -0.19881206214075953, -0.33898921195036313, 0.08046345077968371, -0.3130108432213622, -0.031957941764129666, 0.14376967571543778, -0.0289563303300... |
706.3258 | Strangeness in the Nucleon | There are several different experimental indications, such as the strangeness
contribution to the magnetic moment of the proton, sigma_{\pi N} term, strange
spin polarization, ratio of strange and non strange quark flavor distributions
which suggest that the nucleon contains a hidden strangeness component which is
co... | hep-ph | there are several different experimental indications such as the strangeness contribution to the magnetic moment of the proton sigma_pi n term strange spin polarization ratio of strange and non strange quark flavor distributions which suggest that the nucleon contains a hidden strangeness component which is contradicto... | [['there', 'are', 'several', 'different', 'experimental', 'indications', 'such', 'as', 'the', 'strangeness', 'contribution', 'to', 'the', 'magnetic', 'moment', 'of', 'the', 'proton', 'sigma_pi', 'n', 'term', 'strange', 'spin', 'polarization', 'ratio', 'of', 'strange', 'and', 'non', 'strange', 'quark', 'flavor', 'distri... | [-0.093391889284708, 0.252144147738459, -0.0816815283713176, 0.12161986935320065, -0.06693578380846271, -0.09674313719120906, 0.09857888770792143, 0.290916948412594, -0.19305124296806753, -0.2700613430603162, -0.052886084269879285, -0.3499325831175635, -0.005311757610424569, 0.054542103691614774, 0.07533283151048971, 0... |
706.3259 | Searching for a Companion Star of Tycho's Type Ia Supernova with Optical
Spectroscopic Observations | We report our first results of photometric and spectroscopic observations for
Tycho's supernova remnant (SNR Tycho) to search for the companion star of a
type Ia supernova (SN Ia). From photometric observations using Suprime-Cam on
the Subaru Telescope, we have picked up stars brighter than 22 mag (in
$V$-band) for s... | astro-ph | we report our first results of photometric and spectroscopic observations for tychos supernova remnant snr tycho to search for the companion star of a type ia supernova sn ia from photometric observations using suprimecam on the subaru telescope we have picked up stars brighter than 22 mag in vband for spectroscopy whi... | [['we', 'report', 'our', 'first', 'results', 'of', 'photometric', 'and', 'spectroscopic', 'observations', 'for', 'tychos', 'supernova', 'remnant', 'snr', 'tycho', 'to', 'search', 'for', 'the', 'companion', 'star', 'of', 'a', 'type', 'ia', 'supernova', 'sn', 'ia', 'from', 'photometric', 'observations', 'using', 'suprime... | [-0.04257332452127155, 0.0369943205876378, -0.046213974490481084, 0.04260780420178254, -0.12893083767107472, -0.11840844534063227, 0.08532610230868656, 0.48428907313014136, -0.15742282096162194, -0.29980949569120363, 0.03844418406545516, -0.34290394852933004, -0.0055668047135528365, 0.16971593415316782, -0.030119942408... |
706.326 | A comparison of the strong lensing properties of the Sersic and the NFW
profiles | We investigate the strong lensing properties of the Sersic profile as an
alternative to the NFW profile, focusing on applications to lens modelling of
clusters. Given an underlying Sersic dark matter profile, we study whether an
NFW profile can provide an acceptable fit to strong lensing constraints in the
form of si... | astro-ph | we investigate the strong lensing properties of the sersic profile as an alternative to the nfw profile focusing on applications to lens modelling of clusters given an underlying sersic dark matter profile we study whether an nfw profile can provide an acceptable fit to strong lensing constraints in the form of single ... | [['we', 'investigate', 'the', 'strong', 'lensing', 'properties', 'of', 'the', 'sersic', 'profile', 'as', 'an', 'alternative', 'to', 'the', 'nfw', 'profile', 'focusing', 'on', 'applications', 'to', 'lens', 'modelling', 'of', 'clusters', 'given', 'an', 'underlying', 'sersic', 'dark', 'matter', 'profile', 'we', 'study', '... | [-0.06769105979344911, 0.008471508670481853, -0.13747390146125799, 0.1627494450399859, -0.09463768645224196, -0.13154088288407634, -0.03482617777944715, 0.3911855621746293, -0.16964317436364515, -0.393988565966073, 0.05712324723825549, -0.29545353268859564, -0.053232166255582816, 0.18722095011250564, -0.025124642791019... |
706.3261 | Landau thermodynamic potential for BaTiO_3 | In the paper, the description of the dielectric and ferroelectric properties
of BaTiO_3 single crystals using Landau thermodynamic potential is addressed.
Our results suggest that when using the sixth-power free energy expansion of
the thermodynamic potential, remarkably different values of the fourth-power
coefficie... | cond-mat.stat-mech cond-mat.mtrl-sci | in the paper the description of the dielectric and ferroelectric properties of batio_3 single crystals using landau thermodynamic potential is addressed our results suggest that when using the sixthpower free energy expansion of the thermodynamic potential remarkably different values of the fourthpower coefficient beta... | [['in', 'the', 'paper', 'the', 'description', 'of', 'the', 'dielectric', 'and', 'ferroelectric', 'properties', 'of', 'batio_3', 'single', 'crystals', 'using', 'landau', 'thermodynamic', 'potential', 'is', 'addressed', 'our', 'results', 'suggest', 'that', 'when', 'using', 'the', 'sixthpower', 'free', 'energy', 'expansio... | [-0.11717937385008736, 0.14839509496512573, -0.046204632231926696, -0.04388740817601228, -0.04848805175914924, -0.09026319978984704, 0.05188841871073602, 0.3942333850152323, -0.23317180360203696, -0.25220763198563745, 0.029405375397043246, -0.29630445869187494, -0.14408767643418366, 0.1853506696628695, 0.02094247683524... |
706.3262 | Zeta functions and topological entropy of the Markov-Dyck shifts | The Markov-Dyck shifts arise from finite directed graphs. An expression for
the zeta function of a Markov-Dyck shift is given. The derivation of this
expression is based on a formula in Keller (G. Keller, {\it Circular codes,
loop counting, and zeta-functions}, J. Combinatorial Theory {\bf 56} (1991),
pp. 75--83). Fo... | math.DS math.OA | the markovdyck shifts arise from finite directed graphs an expression for the zeta function of a markovdyck shift is given the derivation of this expression is based on a formula in keller g keller it circular codes loop counting and zetafunctions j combinatorial theory bf 56 1991 pp 7583 for a class of examples that i... | [['the', 'markovdyck', 'shifts', 'arise', 'from', 'finite', 'directed', 'graphs', 'an', 'expression', 'for', 'the', 'zeta', 'function', 'of', 'a', 'markovdyck', 'shift', 'is', 'given', 'the', 'derivation', 'of', 'this', 'expression', 'is', 'based', 'on', 'a', 'formula', 'in', 'keller', 'g', 'keller', 'it', 'circular', ... | [-0.16509207501076162, 0.09769769507715176, -0.08694305457174778, 0.0822539821066047, -0.0927785521824703, -0.14011152859805434, 0.05272290008636474, 0.29153721055340476, -0.27195256046781485, -0.24098677058337312, 0.0181290502183732, -0.2823868917131966, -0.19327764746479012, 0.21535962149783067, -0.09037406086413698,... |
706.3263 | A Blass-Sagan bijection on Eulerian equivalence classes | Following the treatment of Blass and Sagan, we present an algorithmic
bijection between the Eulerian equivalence classes of totally cyclic
orientations and the spanning trees without internal activity edges for a given
graph.
| math.CO | following the treatment of blass and sagan we present an algorithmic bijection between the eulerian equivalence classes of totally cyclic orientations and the spanning trees without internal activity edges for a given graph | [['following', 'the', 'treatment', 'of', 'blass', 'and', 'sagan', 'we', 'present', 'an', 'algorithmic', 'bijection', 'between', 'the', 'eulerian', 'equivalence', 'classes', 'of', 'totally', 'cyclic', 'orientations', 'and', 'the', 'spanning', 'trees', 'without', 'internal', 'activity', 'edges', 'for', 'a', 'given', 'gra... | [-0.20299872767293092, 0.1497775975682695, -0.045563772320747375, 0.057718591298907995, -0.13023414680113396, -0.05972267810085958, 0.09438695309147464, 0.404546051540158, -0.3217004294309652, -0.35210515112813673, 0.010687959902552944, -0.2382499057178696, -0.15363896401091057, 0.09886307663030246, -0.1320339388524492... |
706.3264 | Search for New Particles Leading to Z+jets Final States in $p\bar{p}$
Collisions at $\sqrt{s}=1.96$ TeV | We present the results of a search for new particles that lead to a \Z boson
plus jets in $p\bar{p}$ collisions at $\sqrt{s}=1.96$ TeV using the Collider
Detector at Fermilab (CDF II). A data sample with a luminosity of 1.06 \ifb\
collected using \Z boson decays to $ee$ and $\mu\mu$ is used. We describe a
completely ... | hep-ex | we present the results of a search for new particles that lead to a z boson plus jets in pbarp collisions at sqrts196 tev using the collider detector at fermilab cdf ii a data sample with a luminosity of 106 ifb collected using z boson decays to ee and mumu is used we describe a completely databased method to predict t... | [['we', 'present', 'the', 'results', 'of', 'a', 'search', 'for', 'new', 'particles', 'that', 'lead', 'to', 'a', 'z', 'boson', 'plus', 'jets', 'in', 'pbarp', 'collisions', 'at', 'sqrts196', 'tev', 'using', 'the', 'collider', 'detector', 'at', 'fermilab', 'cdf', 'ii', 'a', 'data', 'sample', 'with', 'a', 'luminosity', 'of... | [-0.010401361141309797, 0.1628588855335791, -0.08228367845987196, 0.1585408836474164, -0.024349131303638017, -0.12445067445672042, 0.08730270149032082, 0.32109556226311503, -0.1386962302746503, -0.34234194438652815, -0.015853763742819178, -0.380545796688042, 0.08008531207923551, 0.16696932930593705, 0.06432210720408507... |
706.3265 | Unbounded-error One-way Classical and Quantum Communication Complexity | This paper studies the gap between quantum one-way communication complexity
$Q(f)$ and its classical counterpart $C(f)$, under the {\em unbounded-error}
setting, i.e., it is enough that the success probability is strictly greater
than 1/2. It is proved that for {\em any} (total or partial) Boolean function
$f$, $Q(f)... | quant-ph | this paper studies the gap between quantum oneway communication complexity qf and its classical counterpart cf under the em unboundederror setting ie it is enough that the success probability is strictly greater than 12 it is proved that for em any total or partial boolean function f qflceil cf2 rceil ie the former is ... | [['this', 'paper', 'studies', 'the', 'gap', 'between', 'quantum', 'oneway', 'communication', 'complexity', 'qf', 'and', 'its', 'classical', 'counterpart', 'cf', 'under', 'the', 'em', 'unboundederror', 'setting', 'ie', 'it', 'is', 'enough', 'that', 'the', 'success', 'probability', 'is', 'strictly', 'greater', 'than', '1... | [-0.15777226896061908, 0.11180657152692405, -0.043839917811528434, 0.06128411102301155, -0.03413045734871091, -0.22378300366864548, 0.07457446712014214, 0.3249097171012224, -0.23872529403086545, -0.2763897572666055, 0.11667051960945159, -0.2682971865650061, -0.14843395821141506, 0.18376208065576324, -0.0647192493018760... |
706.3266 | Quantization of the metric diagonal spacetime with Gaussian normal
coordinates | In the analysis of the Wheeler-DeWitt equation, we have simplified the
Hamiltonian constraint of the Wheeler-DeWitt equation using the coordinate
transformation. The coordinate is choose such that metric becomes diagonal and
as Gaussian normal coordinate. Or we treat small universe so that the metric
become diagonal ... | gr-qc | in the analysis of the wheelerdewitt equation we have simplified the hamiltonian constraint of the wheelerdewitt equation using the coordinate transformation the coordinate is choose such that metric becomes diagonal and as gaussian normal coordinate or we treat small universe so that the metric become diagonal and uni... | [['in', 'the', 'analysis', 'of', 'the', 'wheelerdewitt', 'equation', 'we', 'have', 'simplified', 'the', 'hamiltonian', 'constraint', 'of', 'the', 'wheelerdewitt', 'equation', 'using', 'the', 'coordinate', 'transformation', 'the', 'coordinate', 'is', 'choose', 'such', 'that', 'metric', 'becomes', 'diagonal', 'and', 'as'... | [-0.14554691359400748, 0.06176868801858897, -0.12572245116035144, 0.09716674495798847, -0.1308031625673175, -0.17319681664307912, -0.05726266749824087, 0.3209238295753797, -0.25475709676742553, -0.20300329451759655, 0.08849942506446193, -0.29591522460182507, -0.09857661119972666, 0.08838258752599358, -0.011339359960208... |
706.3267 | Affine parts of abelian surfaces as complete intersection of three
quartics | We consider an integrable system in five unknowns having three quartics
invariants. We show that the complex affine variety defined by putting these
invariants equal to generic constants, completes into an abelian surface; the
jacobian of a genus two hyperelliptic curve. This system is algebraic
completely integrable... | nlin.SI | we consider an integrable system in five unknowns having three quartics invariants we show that the complex affine variety defined by putting these invariants equal to generic constants completes into an abelian surface the jacobian of a genus two hyperelliptic curve this system is algebraic completely integrable and i... | [['we', 'consider', 'an', 'integrable', 'system', 'in', 'five', 'unknowns', 'having', 'three', 'quartics', 'invariants', 'we', 'show', 'that', 'the', 'complex', 'affine', 'variety', 'defined', 'by', 'putting', 'these', 'invariants', 'equal', 'to', 'generic', 'constants', 'completes', 'into', 'an', 'abelian', 'surface',... | [-0.2470342989749553, 0.10408650556417885, -0.0847926119897972, 0.05785198143699713, -0.08280354734967675, -0.21623342367411966, -0.09539621204072446, 0.32120433131134823, -0.33227365967213063, -0.2172371756220073, 0.10589109293773379, -0.26477148767005193, -0.19011625918772138, 0.26721731102780294, -0.1296502784580776... |
706.3268 | Detection of Neutron Scattering from Phase IV of Ce0.7La0.3B6: A
Confirmation of the Octupole Order | We have performed a single crystal neutron scattering experiment on
Ce0.7La0.3B6 to investigate the order parameter of phase IV microscopically.
Below the phase transition temperature 1.5 K of phase IV, weak but distinct
superlattice reflections at the scattering vector (h/2,h/2,l/2) (h, l = odd
number) have been obs... | cond-mat.str-el | we have performed a single crystal neutron scattering experiment on ce07la03b6 to investigate the order parameter of phase iv microscopically below the phase transition temperature 15 k of phase iv weak but distinct superlattice reflections at the scattering vector h2h2l2 h l odd number have been observed by neutron sc... | [['we', 'have', 'performed', 'a', 'single', 'crystal', 'neutron', 'scattering', 'experiment', 'on', 'ce07la03b6', 'to', 'investigate', 'the', 'order', 'parameter', 'of', 'phase', 'iv', 'microscopically', 'below', 'the', 'phase', 'transition', 'temperature', '15', 'k', 'of', 'phase', 'iv', 'weak', 'but', 'distinct', 'su... | [-0.16887165608770577, 0.21971963603411698, -0.0488947477602374, 0.03298925255027522, -0.06368749703203018, -0.10048905683450154, 0.059953556706508, 0.3874157189339813, -0.2427442991304108, -0.3040785017850188, 0.016975190889045026, -0.28715757767915623, -0.08647899184466547, 0.16428471867564237, 0.08633617802600686, 0... |
706.3269 | Experimental characterization of Gaussian quantum communication channels | We present a full experimental characterization of continuous variable
quantum communication channels established by shared entanglement together with
local operations and classical communication. The resulting teleportation
channel was fully characterized by measuring all elements of the covariance
matrix of the sha... | quant-ph | we present a full experimental characterization of continuous variable quantum communication channels established by shared entanglement together with local operations and classical communication the resulting teleportation channel was fully characterized by measuring all elements of the covariance matrix of the shared... | [['we', 'present', 'a', 'full', 'experimental', 'characterization', 'of', 'continuous', 'variable', 'quantum', 'communication', 'channels', 'established', 'by', 'shared', 'entanglement', 'together', 'with', 'local', 'operations', 'and', 'classical', 'communication', 'the', 'resulting', 'teleportation', 'channel', 'was'... | [-0.19159186411028106, 0.18151031146860785, -0.06905753592339654, 0.038763227572457655, 0.06305277571599517, -0.23472386833487285, 0.14245971708409746, 0.3339942034333944, -0.298092594390942, -0.24732556273746822, 0.08765015232299143, -0.2387059743102226, -0.0594800640285636, 0.18560243091649478, -0.048166704897044436,... |
706.327 | Theory of Fulde-Ferrell-Larkin-Ovchinnikov state of superconductors with
and without inversion symmetry: Hubbard model approach | We study Fulde-Ferrell-Larkin-Ovchinnikov (FFLO) state of superconductors
with and without inversion symmetry based on the Hubbard model on the square
lattice near half-filling, using the random phase approximation. We show that
center of mass momentum $Q$ tends to be parallel to $x$- or y-axis in the
presence of inv... | cond-mat.supr-con cond-mat.str-el | we study fuldeferrelllarkinovchinnikov fflo state of superconductors with and without inversion symmetry based on the hubbard model on the square lattice near halffilling using the random phase approximation we show that center of mass momentum q tends to be parallel to x or yaxis in the presence of inversion symmetry ... | [['we', 'study', 'fuldeferrelllarkinovchinnikov', 'fflo', 'state', 'of', 'superconductors', 'with', 'and', 'without', 'inversion', 'symmetry', 'based', 'on', 'the', 'hubbard', 'model', 'on', 'the', 'square', 'lattice', 'near', 'halffilling', 'using', 'the', 'random', 'phase', 'approximation', 'we', 'show', 'that', 'cen... | [-0.23945993955626532, 0.21992300463909353, -0.002921189046982262, 0.0409024128474778, -0.0945486787982561, -0.1560665744253331, 0.06450851681573247, 0.37394238749036085, -0.2617534426368635, -0.24205443755620057, 0.027495824995761118, -0.2660785090661159, -0.06907195970588537, 0.07282325988635421, 0.07363097733231606,... |
706.3271 | A cool R Coronae Borealis star Z UMi | The high resolution spectra of a R CrB type star Z UMi are analysed. The
atmospheric parameters of Z UMi are estimated: Teff=5250+/-250K and log
g=0.5+/-0.3. This places Z UMi among the coolest R CrB stars. The hydrogen
deficiency of Z UMi is confirmed. The abundances of other elements resemble
those found for the mi... | astro-ph | the high resolution spectra of a r crb type star z umi are analysed the atmospheric parameters of z umi are estimated teff5250250k and log g0503 this places z umi among the coolest r crb stars the hydrogen deficiency of z umi is confirmed the abundances of other elements resemble those found for the minority group of r... | [['the', 'high', 'resolution', 'spectra', 'of', 'a', 'r', 'crb', 'type', 'star', 'z', 'umi', 'are', 'analysed', 'the', 'atmospheric', 'parameters', 'of', 'z', 'umi', 'are', 'estimated', 'teff5250250k', 'and', 'log', 'g0503', 'this', 'places', 'z', 'umi', 'among', 'the', 'coolest', 'r', 'crb', 'stars', 'the', 'hydrogen'... | [-0.08750976542469815, 0.13132024184059168, -0.0018290428147799728, 0.07880953165358337, -0.04839470933792114, -0.16428364172874801, 0.12154600861063902, 0.3891425957714302, -0.1534811768653816, -0.35157876916607655, 0.04096132491553283, -0.35821276406447095, 0.0007728328928351402, 0.14228331998152577, -0.0874427439833... |
706.3272 | High redshift X-ray galaxy clusters. I. The impact of point sources on
the cluster properties | The current generation of X-ray observatories like Chandra allows studies
with very fine spatial details. It is now possible to resolve X-ray point
sources projected into the cluster diffuse emission and exclude them from the
analysis to estimate the ``correct'' X-ray observables. In order to verify the
incidence of ... | astro-ph | the current generation of xray observatories like chandra allows studies with very fine spatial details it is now possible to resolve xray point sources projected into the cluster diffuse emission and exclude them from the analysis to estimate the correct xray observables in order to verify the incidence of point sourc... | [['the', 'current', 'generation', 'of', 'xray', 'observatories', 'like', 'chandra', 'allows', 'studies', 'with', 'very', 'fine', 'spatial', 'details', 'it', 'is', 'now', 'possible', 'to', 'resolve', 'xray', 'point', 'sources', 'projected', 'into', 'the', 'cluster', 'diffuse', 'emission', 'and', 'exclude', 'them', 'from... | [-0.02892991880428765, 0.09284667287883758, -0.08561186926651812, 0.10774684875688859, -0.07375206529947095, -0.0675147830520393, 0.12965832072567487, 0.4088682635327834, -0.22907528474828914, -0.36478875276812334, 0.10328136960232402, -0.3339657660323147, -0.004231997094170207, 0.20492017813835686, 0.02995959668560157... |
706.3273 | Orientations, lattice polytopes, and group arrangements I: Chromatic and
tension polynomials of graphs | This is the first one of a series of papers on association of orientations,
lattice polytopes, and abelian group arrangements to graphs. The purpose is to
interpret the integral and modular tension polynomials of graphs at zero and
negative integers. The whole exposition is put under the framework of subgroup
arrange... | math.CO | this is the first one of a series of papers on association of orientations lattice polytopes and abelian group arrangements to graphs the purpose is to interpret the integral and modular tension polynomials of graphs at zero and negative integers the whole exposition is put under the framework of subgroup arrangements ... | [['this', 'is', 'the', 'first', 'one', 'of', 'a', 'series', 'of', 'papers', 'on', 'association', 'of', 'orientations', 'lattice', 'polytopes', 'and', 'abelian', 'group', 'arrangements', 'to', 'graphs', 'the', 'purpose', 'is', 'to', 'interpret', 'the', 'integral', 'and', 'modular', 'tension', 'polynomials', 'of', 'graph... | [-0.18633806413303303, 0.05445556147992446, -0.09478996570667136, 0.03622970821756243, -0.14443302666356342, -0.11451299828518413, 0.03330767630863177, 0.3155809531103721, -0.33279646275383706, -0.28300357432737205, 0.09275889477849139, -0.2561122260460284, -0.14791474469517052, 0.1634018971560012, -0.09323342191879597... |
706.3274 | An asteroseismic study of the beta Cephei star theta Ophiuchi:
constraints on global stellar parameters and core overshooting | We present a seismic study of the beta Cephei star theta Ophiuchi. Our
analysis is based on the observation of one radial mode, one rotationally split
l = 1 triplet and three components of a rotationally split l = 2 quintuplet for
which the m-values were well identified by spectroscopy. We identify the radial
mode as... | astro-ph | we present a seismic study of the beta cephei star theta ophiuchi our analysis is based on the observation of one radial mode one rotationally split l 1 triplet and three components of a rotationally split l 2 quintuplet for which the mvalues were well identified by spectroscopy we identify the radial mode as fundament... | [['we', 'present', 'a', 'seismic', 'study', 'of', 'the', 'beta', 'cephei', 'star', 'theta', 'ophiuchi', 'our', 'analysis', 'is', 'based', 'on', 'the', 'observation', 'of', 'one', 'radial', 'mode', 'one', 'rotationally', 'split', 'l', '1', 'triplet', 'and', 'three', 'components', 'of', 'a', 'rotationally', 'split', 'l',... | [-0.08483063339329155, 0.13996233274362205, -0.03488799984672387, 0.037945140200768016, -0.046113453612185724, -0.0989244898994513, 0.0865696041828728, 0.3766628528344147, -0.18270385251586954, -0.36247956195818676, 0.056213421819346215, -0.25660079102642064, -0.041171640864220156, 0.14070428996301013, -0.0321580817282... |
706.3275 | Quantum rattling of molecular hydrogen in clathrate hydrate nanocavities | We have performed high-resolution inelastic neutron scattering studies on
three samples of hydrogenated tetrahydrofuran-water clathrates, containing
either H2 at different para/ortho concentrtion, or HD. By a refined analysis of
the data, we are able to assign the spectral bands to rotational and
center-of-mass trans... | cond-mat.mtrl-sci | we have performed highresolution inelastic neutron scattering studies on three samples of hydrogenated tetrahydrofuranwater clathrates containing either h2 at different paraortho concentrtion or hd by a refined analysis of the data we are able to assign the spectral bands to rotational and centerofmass translational tr... | [['we', 'have', 'performed', 'highresolution', 'inelastic', 'neutron', 'scattering', 'studies', 'on', 'three', 'samples', 'of', 'hydrogenated', 'tetrahydrofuranwater', 'clathrates', 'containing', 'either', 'h2', 'at', 'different', 'paraortho', 'concentrtion', 'or', 'hd', 'by', 'a', 'refined', 'analysis', 'of', 'the', '... | [-0.11307506423966004, 0.14124846701558522, -0.02335244084697035, -0.00022255301634531197, -0.005706282561111105, -0.10698914844308491, 0.04768517064231429, 0.41580784162392886, -0.24575634436432, -0.28908126930090056, 0.0473138205259868, -0.30888349353903677, -0.050007613811630575, 0.10164047117634653, 0.0410079279539... |
706.3276 | The ratchet effect and the transporting islands in the chaotic sea | We study directed transport in a classical deterministic dissipative system.
We consider the generic case of mixed phase space and show that large ratchet
currents can be generated thanks to the presence, in the Hamiltonian limit, of
transporting stability islands embedded in the chaotic sea. Due to the
simultaneous ... | cond-mat.stat-mech | we study directed transport in a classical deterministic dissipative system we consider the generic case of mixed phase space and show that large ratchet currents can be generated thanks to the presence in the hamiltonian limit of transporting stability islands embedded in the chaotic sea due to the simultaneous presen... | [['we', 'study', 'directed', 'transport', 'in', 'a', 'classical', 'deterministic', 'dissipative', 'system', 'we', 'consider', 'the', 'generic', 'case', 'of', 'mixed', 'phase', 'space', 'and', 'show', 'that', 'large', 'ratchet', 'currents', 'can', 'be', 'generated', 'thanks', 'to', 'the', 'presence', 'in', 'the', 'hamil... | [-0.22150142932285186, 0.2124622739749412, -0.04216244635618713, 0.04174360159739903, 0.031801535228063185, -0.10533977450152272, 0.017298582466064045, 0.2816304892225012, -0.28350257102961407, -0.259531931466844, 0.1315773956649873, -0.22042953277848762, -0.11767815940133104, 0.17988003459312532, -0.053961782416405334... |
706.3277 | High redshift X-ray galaxy clusters. II. The L_X-T relationship
revisited | In this paper we re-visit the observational relation between X-ray luminosity
and temperature for high-z galaxy clusters and compare it with the local L_X-T
and with theoretical models. To these ends we use a sample of 17 clusters
extracted from the Chandra archive supplemented with additional clusters from
the liter... | astro-ph | in this paper we revisit the observational relation between xray luminosity and temperature for highz galaxy clusters and compare it with the local l_xt and with theoretical models to these ends we use a sample of 17 clusters extracted from the chandra archive supplemented with additional clusters from the literature e... | [['in', 'this', 'paper', 'we', 'revisit', 'the', 'observational', 'relation', 'between', 'xray', 'luminosity', 'and', 'temperature', 'for', 'highz', 'galaxy', 'clusters', 'and', 'compare', 'it', 'with', 'the', 'local', 'l_xt', 'and', 'with', 'theoretical', 'models', 'to', 'these', 'ends', 'we', 'use', 'a', 'sample', 'o... | [-0.030011836087297242, 0.11580148386120465, -0.10462080514593887, 0.14008291430680858, -0.09077678511281184, -0.10737663252573264, 0.06930852269985702, 0.4015318911674862, -0.19580964329709047, -0.3752285625838848, 0.024844242151928424, -0.31680325565573114, -0.014919539746688868, 0.19247658723086694, 0.01565258193154... |
706.3278 | Simulations on the Heavy Hadron Transport at RHIC | Based on the hadron transport frames, detailed simulations are carried out to
discuss $\phi$, $\Omega$ productions and the significant enhancements in the
very low $p_T$ region for some of the soft spectra in RHIC. Elastic
interactions are introduced in the simulations. The elastic cross sections vary
from different ... | nucl-th hep-ph nucl-ex | based on the hadron transport frames detailed simulations are carried out to discuss phi omega productions and the significant enhancements in the very low p_t region for some of the soft spectra in rhic elastic interactions are introduced in the simulations the elastic cross sections vary from different hadrons and en... | [['based', 'on', 'the', 'hadron', 'transport', 'frames', 'detailed', 'simulations', 'are', 'carried', 'out', 'to', 'discuss', 'phi', 'omega', 'productions', 'and', 'the', 'significant', 'enhancements', 'in', 'the', 'very', 'low', 'p_t', 'region', 'for', 'some', 'of', 'the', 'soft', 'spectra', 'in', 'rhic', 'elastic', '... | [-0.11125378197221647, 0.2281770559456495, -0.16282933675185113, 0.14661826024807634, -0.0011118839250966197, -0.0620504487675452, -0.049046949047358734, 0.3809493508426443, -0.2660544825688241, -0.2737271008451307, -0.046412100488807825, -0.3466821728451621, 0.002296113519973698, 0.17011108766642533, 0.065612843448189... |
706.3279 | Measurement of the Branching Fraction for B^0 --> a1(1260)+-pi-+ with
535 Million BBbar Pairs | We present a measurement of the branching fraction for the decay
B^0->a1+(1260)pi- with a1+->pi+pi+pi- using a data sample containing 535x10^6
BBbar pairs collected with the Belle detector at the KEKB asymmetric-energy
e+e- collider operating at the Upsilon(4S) resonance. We measure the branching
fraction Br(B^0->a1+... | hep-ex | we present a measurement of the branching fraction for the decay b0a11260pi with a1pipipi using a data sample containing 535x106 bbbar pairs collected with the belle detector at the kekb asymmetricenergy ee collider operating at the upsilon4s resonance we measure the branching fraction brb0a1pibra1pipipi 149 16 23x106 ... | [['we', 'present', 'a', 'measurement', 'of', 'the', 'branching', 'fraction', 'for', 'the', 'decay', 'b0a11260pi', 'with', 'a1pipipi', 'using', 'a', 'data', 'sample', 'containing', '535x106', 'bbbar', 'pairs', 'collected', 'with', 'the', 'belle', 'detector', 'at', 'the', 'kekb', 'asymmetricenergy', 'ee', 'collider', 'op... | [-0.08804813883896848, 0.14179363877822956, -0.05365813201017402, 0.00962553826091742, -0.046904893053040186, -0.08985299373873407, 0.11897199969583501, 0.2965335508429066, -0.13440890234024092, -0.3110447372827265, 0.017411069293437456, -0.517282775534248, 0.10979066230356693, 0.17194263621975012, 0.09473035105124668,... |
706.328 | Theoretical background for observing ultra-slow microwaves in a
Bose-Einstein condensate of alkali atoms | We represent a new microscopic approach that allows studying the propagation
properties of microwaves in a Bose-Einstein condensate of alkali atoms. It is
assumed that the frequency of signal is tuned up to the transition between
hyperfine ground state levels of such atoms. Pulse slowing conditions
dependence on the ... | cond-mat.stat-mech cond-mat.other | we represent a new microscopic approach that allows studying the propagation properties of microwaves in a boseeinstein condensate of alkali atoms it is assumed that the frequency of signal is tuned up to the transition between hyperfine ground state levels of such atoms pulse slowing conditions dependence on the syste... | [['we', 'represent', 'a', 'new', 'microscopic', 'approach', 'that', 'allows', 'studying', 'the', 'propagation', 'properties', 'of', 'microwaves', 'in', 'a', 'boseeinstein', 'condensate', 'of', 'alkali', 'atoms', 'it', 'is', 'assumed', 'that', 'the', 'frequency', 'of', 'signal', 'is', 'tuned', 'up', 'to', 'the', 'transi... | [-0.16821998896823773, 0.25386852013504074, -0.04252039185561931, 0.04850805778603655, -0.0076709234314135365, -0.13891751219316856, 0.04981932803009128, 0.43130354398919135, -0.2531528920895353, -0.2847054778555043, -0.029363375325139957, -0.2520643672907363, -0.08190022041233852, 0.18952859900219693, 0.04659895522078... |
706.3281 | Optical and infrared properties of V1647 Orionis during the 2003-2006
outburst. II. Temporal evolution of the eruptive source | The occurrence of new FU Orionis-like objects is fundamental to understand
the outburst mechanism in young stars and their role in star formation and disk
evolution. Our work is aimed at investigating the properties of the recent
outburst of V1647 Ori. Using optical and mid infrared long slit spectroscopy we
monitore... | astro-ph | the occurrence of new fu orionislike objects is fundamental to understand the outburst mechanism in young stars and their role in star formation and disk evolution our work is aimed at investigating the properties of the recent outburst of v1647 ori using optical and mid infrared long slit spectroscopy we monitored v16... | [['the', 'occurrence', 'of', 'new', 'fu', 'orionislike', 'objects', 'is', 'fundamental', 'to', 'understand', 'the', 'outburst', 'mechanism', 'in', 'young', 'stars', 'and', 'their', 'role', 'in', 'star', 'formation', 'and', 'disk', 'evolution', 'our', 'work', 'is', 'aimed', 'at', 'investigating', 'the', 'properties', 'o... | [-0.06956906882931127, 0.09766773229057435, -0.07043662286883631, 0.05992087690604173, -0.08642902981350803, -0.1081258771629617, 0.022970806178145484, 0.4619053806565315, -0.20139808434490894, -0.30573705978148813, 0.0969957308265435, -0.2798520804068388, -0.06966908270713885, 0.1591191257186863, -0.07032312470935768,... |
706.3282 | Braided Hom-Lie bialgebras | We introduce the new concept of braided Hom-Lie bialgebras which is a
generalization of Sommerh\"{a}user-Majid's braided Lie bialgebras and Yau's
Hom-Lie bialgebras. Using this concept we give the unified product construction
for Hom-Lie bialgebras which can be seen as a Hom-Lie version of
Bespalov-Drabant's cocycle ... | math.QA math.RA | we introduce the new concept of braided homlie bialgebras which is a generalization of sommerhausermajids braided lie bialgebras and yaus homlie bialgebras using this concept we give the unified product construction for homlie bialgebras which can be seen as a homlie version of bespalovdrabants cocycle cross product bi... | [['we', 'introduce', 'the', 'new', 'concept', 'of', 'braided', 'homlie', 'bialgebras', 'which', 'is', 'a', 'generalization', 'of', 'sommerhausermajids', 'braided', 'lie', 'bialgebras', 'and', 'yaus', 'homlie', 'bialgebras', 'using', 'this', 'concept', 'we', 'give', 'the', 'unified', 'product', 'construction', 'for', 'h... | [-0.1788875883435236, 0.011808017473277746, -0.014549685562861727, 0.1779302019189964, -0.24262855095204283, -0.16496353624376192, -0.08932173539057096, 0.4497987405456444, -0.43043888923513923, -0.19179452550498413, 0.09122261672994082, -0.16567914459626487, -0.2418998940946891, 0.16383769779287755, -0.239859699534173... |
706.3283 | Novel constraints on light elementary particles and extra-dimensional
physics from the Casimir effect | We present supplementary information on the recent indirect measurement of
the Casimir pressure between two parallel plates using a micromachined
oscillator. The equivalent pressure between the plates is obtained by means of
the proximity force approximation after measuring the force gradient between a
gold coated sp... | hep-ph quant-ph | we present supplementary information on the recent indirect measurement of the casimir pressure between two parallel plates using a micromachined oscillator the equivalent pressure between the plates is obtained by means of the proximity force approximation after measuring the force gradient between a gold coated spher... | [['we', 'present', 'supplementary', 'information', 'on', 'the', 'recent', 'indirect', 'measurement', 'of', 'the', 'casimir', 'pressure', 'between', 'two', 'parallel', 'plates', 'using', 'a', 'micromachined', 'oscillator', 'the', 'equivalent', 'pressure', 'between', 'the', 'plates', 'is', 'obtained', 'by', 'means', 'of'... | [-0.06853158075043805, 0.12147965529734628, -0.07743479336170314, 0.019811097590991693, -0.04510066576931678, -0.13939581708239276, 0.0687391367804329, 0.3724217651315698, -0.21120962345351776, -0.3588509070643272, 0.032039052852841546, -0.30659336951985394, -0.0711577315883112, 0.2211110579962689, 0.025754187675712175... |
706.3284 | The role of string topology in symplectic field theory | We outline a program for incorporating holomorphic curves with Lagrangian
boundary conditions into symplectic field theory, with an emphasis on ideas,
geometric intuition, and a description of the resulting algebraic structures.
| math.SG | we outline a program for incorporating holomorphic curves with lagrangian boundary conditions into symplectic field theory with an emphasis on ideas geometric intuition and a description of the resulting algebraic structures | [['we', 'outline', 'a', 'program', 'for', 'incorporating', 'holomorphic', 'curves', 'with', 'lagrangian', 'boundary', 'conditions', 'into', 'symplectic', 'field', 'theory', 'with', 'an', 'emphasis', 'on', 'ideas', 'geometric', 'intuition', 'and', 'a', 'description', 'of', 'the', 'resulting', 'algebraic', 'structures']] | [-0.16759020184737541, 0.05257462874297128, -0.22127301696567767, 0.08369732714228091, -0.170971236033966, -0.13256518611864698, -0.01878951921413142, 0.33198725906831605, -0.27053280668934027, -0.27559077811817967, 0.10161471425465518, -0.18383252512543433, -0.21488438522623432, 0.20910694552285056, -0.123234359307154... |
706.3285 | Quark Mass in the Sakai-Sugimoto Model of Chiral Symmetry Breaking | We re-analyze D8 brane embeddings in the geometry of a D4 brane wrapped on a
circle that describe chiral symmetry breaking in a strongly coupled
non-supersymmetric gauge theory. We argue that if the holographic fields are
correctly interpreted, the original embeddings describe a complex quark mass
and condensate in t... | hep-th | we reanalyze d8 brane embeddings in the geometry of a d4 brane wrapped on a circle that describe chiral symmetry breaking in a strongly coupled nonsupersymmetric gauge theory we argue that if the holographic fields are correctly interpreted the original embeddings describe a complex quark mass and condensate in the the... | [['we', 'reanalyze', 'd8', 'brane', 'embeddings', 'in', 'the', 'geometry', 'of', 'a', 'd4', 'brane', 'wrapped', 'on', 'a', 'circle', 'that', 'describe', 'chiral', 'symmetry', 'breaking', 'in', 'a', 'strongly', 'coupled', 'nonsupersymmetric', 'gauge', 'theory', 'we', 'argue', 'that', 'if', 'the', 'holographic', 'fields'... | [-0.1386349748648269, 0.24443707687472835, -0.12611566063523003, 0.17276885068649878, -0.07376099573177042, -0.10147997679514359, 0.02834538932668172, 0.31925727131333453, -0.15314597810067018, -0.20430745904162093, 0.03191430202246761, -0.26079236806451694, -0.13637409717730672, 0.06434949769557101, -0.041860768256722... |
706.3286 | Intensity-Based Registration of Freehand 3D Ultrasound and CT-scan
Images of the Kidney | This paper presents a method to register a pre-operative Computed-Tomography
(CT) volume to a sparse set of intra-operative Ultra-Sound (US) slices. In the
context of percutaneous renal puncture, the aim is to transfer planning
information to an intra-operative coordinate system. The spatial position of
the US slices... | physics.med-ph | this paper presents a method to register a preoperative computedtomography ct volume to a sparse set of intraoperative ultrasound us slices in the context of percutaneous renal puncture the aim is to transfer planning information to an intraoperative coordinate system the spatial position of the us slices is measured b... | [['this', 'paper', 'presents', 'a', 'method', 'to', 'register', 'a', 'preoperative', 'computedtomography', 'ct', 'volume', 'to', 'a', 'sparse', 'set', 'of', 'intraoperative', 'ultrasound', 'us', 'slices', 'in', 'the', 'context', 'of', 'percutaneous', 'renal', 'puncture', 'the', 'aim', 'is', 'to', 'transfer', 'planning'... | [-0.05609225794204732, 0.0032359888740636417, -0.07036905545092996, 0.05556981330184338, -0.04605962981042858, -0.12001473481447864, 0.013981582681154472, 0.4168607515362683, -0.2509331916322551, -0.3245729578977955, 0.10885172003869853, -0.2861314808322086, -0.09776043220556943, 0.17554070864603416, -0.116367908848130... |
706.3287 | Evolution of the proton sd states in neutron-rich Ca isotopes | We analyze the evolution with increasing isospin asymmetry of the proton
single-particle states 2s1/2 and 1d3/2 in Ca isotopes, using non-relativistic
and relativistic mean field approaches. Both models give similar trends and it
is shown that this evolution is sensitive to the neutron shell structure, the
two states... | nucl-th | we analyze the evolution with increasing isospin asymmetry of the proton singleparticle states 2s12 and 1d32 in ca isotopes using nonrelativistic and relativistic mean field approaches both models give similar trends and it is shown that this evolution is sensitive to the neutron shell structure the two states becoming... | [['we', 'analyze', 'the', 'evolution', 'with', 'increasing', 'isospin', 'asymmetry', 'of', 'the', 'proton', 'singleparticle', 'states', '2s12', 'and', '1d32', 'in', 'ca', 'isotopes', 'using', 'nonrelativistic', 'and', 'relativistic', 'mean', 'field', 'approaches', 'both', 'models', 'give', 'similar', 'trends', 'and', '... | [-0.06332911695353687, 0.1799600389942167, -0.06823084926176252, 0.14287606336769054, 0.0190319449499701, -0.11600801081072087, 0.026775169467101945, 0.3504034975035624, -0.2193185812793672, -0.27369089534393315, 0.013925761225012441, -0.3195587746516773, -0.08830753150396049, 0.11722365055289684, 0.061914743229069494,... |
706.3288 | Alternative experimental evidence for chiral restoration in excited
baryons | Given existing empirical spectral patterns of excited hadrons it has been
suggested that chiral symmetry is approximately restored in excited hadrons at
zero temperature/density (effective symmetry restoration). If correct, this
implies that mass generation mechanisms and physics in excited hadrons is very
different ... | hep-ph hep-ex nucl-ex nucl-th | given existing empirical spectral patterns of excited hadrons it has been suggested that chiral symmetry is approximately restored in excited hadrons at zero temperaturedensity effective symmetry restoration if correct this implies that mass generation mechanisms and physics in excited hadrons is very different as comp... | [['given', 'existing', 'empirical', 'spectral', 'patterns', 'of', 'excited', 'hadrons', 'it', 'has', 'been', 'suggested', 'that', 'chiral', 'symmetry', 'is', 'approximately', 'restored', 'in', 'excited', 'hadrons', 'at', 'zero', 'temperaturedensity', 'effective', 'symmetry', 'restoration', 'if', 'correct', 'this', 'imp... | [-0.08027841799736563, 0.2765028099372732, -0.09329480442483973, 0.10711119623277421, -0.06397660571989093, -0.1737405865524824, 0.013899310656330165, 0.34990529660388353, -0.20822009762719576, -0.2602239238599745, 0.04457208129937647, -0.3011661760869322, -0.021631392606057866, 0.07661197398898795, 0.06598471572445663... |
706.3289 | Single-qubit operations in the double-donor structure driven by optical
and voltage pulses | We study theoretically the quantum dynamics of an electron in the
singlyionized double-donor structure in the semiconductor host under the
influence of laser pulses whose frequencies are close to structure resonant
frequencies. This system can be used as a charge qubit where the logical states
are defined by the lowe... | cond-mat.mes-hall | we study theoretically the quantum dynamics of an electron in the singlyionized doubledonor structure in the semiconductor host under the influence of laser pulses whose frequencies are close to structure resonant frequencies this system can be used as a charge qubit where the logical states are defined by the lowest t... | [['we', 'study', 'theoretically', 'the', 'quantum', 'dynamics', 'of', 'an', 'electron', 'in', 'the', 'singlyionized', 'doubledonor', 'structure', 'in', 'the', 'semiconductor', 'host', 'under', 'the', 'influence', 'of', 'laser', 'pulses', 'whose', 'frequencies', 'are', 'close', 'to', 'structure', 'resonant', 'frequencie... | [-0.17445266875438392, 0.2880793047080698, -1.4579999346837954e-05, 0.028021686359015467, 0.07862122711742779, -0.1729844738556831, 0.10770521802866521, 0.4167451899567688, -0.2567019510186381, -0.2748482187571763, 0.0008235085363223872, -0.28048890488463696, -0.06670387624762952, 0.19360124905317747, 0.046489734707089... |
706.329 | Multiplicity Distributions in Canonical and Microcanonical Statistical
Ensembles | The aim of this paper is to introduce a new technique for calculation of
observables, in particular multiplicity distributions, in various statistical
ensembles at finite volume. The method is based on Fourier analysis of the
grand canonical partition function. Taylor expansion of the generating function
is used to s... | nucl-th | the aim of this paper is to introduce a new technique for calculation of observables in particular multiplicity distributions in various statistical ensembles at finite volume the method is based on fourier analysis of the grand canonical partition function taylor expansion of the generating function is used to separat... | [['the', 'aim', 'of', 'this', 'paper', 'is', 'to', 'introduce', 'a', 'new', 'technique', 'for', 'calculation', 'of', 'observables', 'in', 'particular', 'multiplicity', 'distributions', 'in', 'various', 'statistical', 'ensembles', 'at', 'finite', 'volume', 'the', 'method', 'is', 'based', 'on', 'fourier', 'analysis', 'of... | [-0.07226377794733987, 0.0831676906064296, -0.17648089640558912, 0.08822183431072447, -0.035543953663168044, -0.021278960537165402, 0.044648984799949595, 0.30215149541886954, -0.22887576467429216, -0.25782568561486324, 0.0415115018402083, -0.284929515967759, -0.08503180138068274, 0.1570014431499518, -0.0170385719844489... |
706.3291 | Continuous Spin Fractionation: A large scale method to improve the
performance of polymers | Most technical polymers and many biopolymers contain very different molecular
species (unlike chain length, molecular architecture and/or chemical
composition) in contrast to pure low molecular weight compounds. This
inconsistent constitution of macromolecules proves very adverse in many cases.
An adequate fractionat... | cond-mat.mtrl-sci | most technical polymers and many biopolymers contain very different molecular species unlike chain length molecular architecture andor chemical composition in contrast to pure low molecular weight compounds this inconsistent constitution of macromolecules proves very adverse in many cases an adequate fractionation of p... | [['most', 'technical', 'polymers', 'and', 'many', 'biopolymers', 'contain', 'very', 'different', 'molecular', 'species', 'unlike', 'chain', 'length', 'molecular', 'architecture', 'andor', 'chemical', 'composition', 'in', 'contrast', 'to', 'pure', 'low', 'molecular', 'weight', 'compounds', 'this', 'inconsistent', 'const... | [-0.0941993708368675, 0.1704998088938686, -0.048285420146713935, 0.030740580846491106, -0.032457864153561805, -0.15954044582803203, 0.04297571334366997, 0.3774754212111095, -0.24617029430548018, -0.28554015862974097, 0.08682560575732463, -0.24650636201102982, -0.07202144709695568, 0.1546056406668654, -0.060738970704831... |
706.3292 | A Differential Model for the Deformation of the Plancherel Growth
Process | In the present paper we construct and solve a differential model for the
q-analog of the Plancherel growth process. The construction is based on a
deformation of the Makrov-Krein correspondence between continual diagrams and
probability distributions.
| math.CO math-ph math.MP | in the present paper we construct and solve a differential model for the qanalog of the plancherel growth process the construction is based on a deformation of the makrovkrein correspondence between continual diagrams and probability distributions | [['in', 'the', 'present', 'paper', 'we', 'construct', 'and', 'solve', 'a', 'differential', 'model', 'for', 'the', 'qanalog', 'of', 'the', 'plancherel', 'growth', 'process', 'the', 'construction', 'is', 'based', 'on', 'a', 'deformation', 'of', 'the', 'makrovkrein', 'correspondence', 'between', 'continual', 'diagrams', '... | [-0.11125368760632617, 0.030697001703083517, -0.16647792437246867, 0.06961528461818359, -0.06541593761316368, -0.042042672048721995, 0.04406529361315604, 0.3241545752622187, -0.26855642944574354, -0.25442841183394194, 0.081588858309468, -0.23719381392002106, -0.22371009566954203, 0.19666935460242843, -0.113118174885000... |
706.3293 | Optimized implementation of the Lanczos method for magnetic systems | Numerically exact investigations of interacting spin systems provide a major
tool for an understanding of their magnetic properties. For medium size systems
the approximate Lanczos diagonalization is the most common method. In this
article we suggest two improvements: efficient basis coding in subspaces and
simple re... | cond-mat.str-el cond-mat.stat-mech | numerically exact investigations of interacting spin systems provide a major tool for an understanding of their magnetic properties for medium size systems the approximate lanczos diagonalization is the most common method in this article we suggest two improvements efficient basis coding in subspaces and simple restruc... | [['numerically', 'exact', 'investigations', 'of', 'interacting', 'spin', 'systems', 'provide', 'a', 'major', 'tool', 'for', 'an', 'understanding', 'of', 'their', 'magnetic', 'properties', 'for', 'medium', 'size', 'systems', 'the', 'approximate', 'lanczos', 'diagonalization', 'is', 'the', 'most', 'common', 'method', 'in... | [-0.17250641186873675, 0.048471796946726, -0.0656375462065774, 0.08847041967876103, -0.05455214438997969, -0.13354053126876148, 0.02152730425705715, 0.4311125631235084, -0.26857689843389526, -0.2743294046317436, 0.09969537295115997, -0.21218907989903676, -0.17275743337576183, 0.23708992734627457, 0.04238262837895249, 0... |
706.3294 | Moriond 07 proceedings:"Extension of the frequency-range of
interferometers for the "magnetic" components of gravitational waves?" | Recently some papers in the literature have shown the presence and importance
of the so-called {}"magnetic" components of gravitational waves (GWs), which
have to be taken into account in the context of the total response functions of
interferometers for GWs propagating from arbitrary directions. In this paper
the re... | gr-qc | recently some papers in the literature have shown the presence and importance of the socalled magnetic components of gravitational waves gws which have to be taken into account in the context of the total response functions of interferometers for gws propagating from arbitrary directions in this paper the response func... | [['recently', 'some', 'papers', 'in', 'the', 'literature', 'have', 'shown', 'the', 'presence', 'and', 'importance', 'of', 'the', 'socalled', 'magnetic', 'components', 'of', 'gravitational', 'waves', 'gws', 'which', 'have', 'to', 'be', 'taken', 'into', 'account', 'in', 'the', 'context', 'of', 'the', 'total', 'response',... | [-0.14436475559897885, 0.14035329256234141, -0.04585505663143361, 0.04555700471973978, -0.07850162302972474, 0.011041487882132916, -0.02544362419661518, 0.3383788523976417, -0.2311905072454144, -0.2890940139289288, 0.08025242906639024, -0.27764083379331755, -0.1337318753152538, 0.21331794993431472, 0.03341226624872755,... |
706.3295 | Lower bounds on the minimum average distance of binary codes | New lower bounds on the minimum average Hamming distance of binary codes are
derived. The bounds are obtained using linear programming approach.
| cs.IT math.CO math.IT | new lower bounds on the minimum average hamming distance of binary codes are derived the bounds are obtained using linear programming approach | [['new', 'lower', 'bounds', 'on', 'the', 'minimum', 'average', 'hamming', 'distance', 'of', 'binary', 'codes', 'are', 'derived', 'the', 'bounds', 'are', 'obtained', 'using', 'linear', 'programming', 'approach']] | [-0.18079702894796024, 0.05275943976911632, -0.07719533966684883, 0.15822567085904832, -0.06323330193250017, -0.22651883223178712, 0.10453380373391238, 0.3207045419628478, -0.3023366250775077, -0.37598480385812844, 0.15445568378676067, -0.3000821503387256, -0.1142652691765265, 0.3282029799778353, -0.05941696862944148, ... |
706.3296 | On the heterogeneous character of water's amorphous polymorphism | In this letter we report {\it in situ} small--angle neutron scattering
results on the high--density (HDA) and low-density amorphous (LDA) ice
structures and on intermediate structures as found during the temperature
induced transformation of HDA into LDA. We show that the small--angle signal is
characterised by two $... | cond-mat.dis-nn cond-mat.soft | in this letter we report it in situ smallangle neutron scattering results on the highdensity hda and lowdensity amorphous lda ice structures and on intermediate structures as found during the temperature induced transformation of hda into lda we show that the smallangle signal is characterised by two q regimes featurin... | [['in', 'this', 'letter', 'we', 'report', 'it', 'in', 'situ', 'smallangle', 'neutron', 'scattering', 'results', 'on', 'the', 'highdensity', 'hda', 'and', 'lowdensity', 'amorphous', 'lda', 'ice', 'structures', 'and', 'on', 'intermediate', 'structures', 'as', 'found', 'during', 'the', 'temperature', 'induced', 'transform... | [-0.1464545426890254, 0.2106293142855803, -0.078999370305069, 0.05302943456980928, -0.008781509713043232, -0.08100980319007224, 0.05784029644737775, 0.40893498447761445, -0.2951753835193813, -0.26043415980828877, 0.052717994622936526, -0.2956606237368809, -0.11689372455600548, 0.1537163862203424, 0.050577384812749114, ... |
706.3297 | Higher Mellin moments for charged current DIS | We report on our recent results for deep-inelastic neutrino-proton
scattering. We have computed the perturbative QCD corrections to three loops
for the harged current structure functions F_2, F_L and F_3 for the combination
nu P - nubar P. In leading twist approximation we have calculated the first six
odd-integer Me... | hep-ph | we report on our recent results for deepinelastic neutrinoproton scattering we have computed the perturbative qcd corrections to three loops for the harged current structure functions f_2 f_l and f_3 for the combination nu p nubar p in leading twist approximation we have calculated the first six oddinteger mellin momen... | [['we', 'report', 'on', 'our', 'recent', 'results', 'for', 'deepinelastic', 'neutrinoproton', 'scattering', 'we', 'have', 'computed', 'the', 'perturbative', 'qcd', 'corrections', 'to', 'three', 'loops', 'for', 'the', 'harged', 'current', 'structure', 'functions', 'f_2', 'f_l', 'and', 'f_3', 'for', 'the', 'combination',... | [-0.12292848869631263, 0.1090888832585494, -0.05605682845374471, 0.08108007327506417, -0.0037741234771123057, -0.023904704361369735, 0.006864482948654577, 0.3810171930217429, -0.1847157923896846, -0.21614862778469135, 0.028422082578273195, -0.3430130087623471, -0.10561449648996227, 0.21734753188334013, 0.09749632776595... |
706.3298 | On geodesics of Berger tangent sphere bundle of Hermitian locally
symmetric manifold | We propose a special deformation of the Sasaki metric on tangent and unit
tangent bundle of a Hermitian locally symmetric manifold. Geodesics of this
deformed metric have different projections on a base manifold for tangent or
unit tangent bundle cases in contrast to usual Sasaki metric. Nevertheless, the
projections... | math.DG math.MG | we propose a special deformation of the sasaki metric on tangent and unit tangent bundle of a hermitian locally symmetric manifold geodesics of this deformed metric have different projections on a base manifold for tangent or unit tangent bundle cases in contrast to usual sasaki metric nevertheless the projections of g... | [['we', 'propose', 'a', 'special', 'deformation', 'of', 'the', 'sasaki', 'metric', 'on', 'tangent', 'and', 'unit', 'tangent', 'bundle', 'of', 'a', 'hermitian', 'locally', 'symmetric', 'manifold', 'geodesics', 'of', 'this', 'deformed', 'metric', 'have', 'different', 'projections', 'on', 'a', 'base', 'manifold', 'for', '... | [-0.23881890583839832, 0.022337141097523272, -0.030952212682953388, 0.045104484805823165, -0.18614794500877685, -0.15226805618625472, -0.03537016854423917, 0.44016988959276315, -0.29013417316177353, -0.10106239882368369, 0.07611472866406213, -0.29263110064097086, -0.19215940736643405, 0.08869964849189714, -0.1685538586... |
706.3299 | Relaxation of the flow of triods by Curve Shortening Flow via the
vector-valued parabolic Allen-Cahn equation | In this paper we find solutions $u_\epsilon$ to a certain class of
vector-valued parabolic Allen-Cahn equation that as $\epsilon \to 0$ develops
as interface a given triod evolving under curve shortening flow.
| math.AP math.DG | in this paper we find solutions u_epsilon to a certain class of vectorvalued parabolic allencahn equation that as epsilon to 0 develops as interface a given triod evolving under curve shortening flow | [['in', 'this', 'paper', 'we', 'find', 'solutions', 'u_epsilon', 'to', 'a', 'certain', 'class', 'of', 'vectorvalued', 'parabolic', 'allencahn', 'equation', 'that', 'as', 'epsilon', 'to', '0', 'develops', 'as', 'interface', 'a', 'given', 'triod', 'evolving', 'under', 'curve', 'shortening', 'flow']] | [-0.238293488600081, 0.03706218851279588, -0.10179575676879575, 0.013028965598242659, -0.11592427707247195, -0.19799955558752821, -0.015325023308246127, 0.3145779865162988, -0.38599181776085206, -0.19263437192045874, 0.1268112290117349, -0.27561881357143003, -0.18810450562065648, 0.19152842329875117, -0.118608728531868... |
706.33 | Trapped Bose gases with large positive scattering length | We calculate the energy and the condensate fraction of a system of trapped
bosons interacting via a short-range two-body potential with positive
scattering length. The potential is attractive and has a two-body bound state.
When the scattering length is small compared to the trap length the system is
model independen... | quant-ph cond-mat.quant-gas | we calculate the energy and the condensate fraction of a system of trapped bosons interacting via a shortrange twobody potential with positive scattering length the potential is attractive and has a twobody bound state when the scattering length is small compared to the trap length the system is model independent all p... | [['we', 'calculate', 'the', 'energy', 'and', 'the', 'condensate', 'fraction', 'of', 'a', 'system', 'of', 'trapped', 'bosons', 'interacting', 'via', 'a', 'shortrange', 'twobody', 'potential', 'with', 'positive', 'scattering', 'length', 'the', 'potential', 'is', 'attractive', 'and', 'has', 'a', 'twobody', 'bound', 'state... | [-0.15446279239524335, 0.24090625265685534, -0.06578470581184023, 0.06963793551255451, 0.033788460862904206, -0.2196507741859888, 0.008918990087198111, 0.31215511114128586, -0.25726136191775206, -0.21099022739720577, -0.019568351975605976, -0.3741001386593268, -0.0838215189931679, 0.14209173574989425, 0.115419634504328... |
706.3301 | On the invariant symmetries of the $\mathcal{D}$-metrics | We analyze the symmetries and other invariant qualities of the
$\mathcal{D}$-metrics (type D aligned Einstein Maxwell solutions with
cosmological constant whose Debever null principal directions determine
shear-free geodesic null congruences). We recover some properties and deduce
new ones about their isometry group ... | gr-qc | we analyze the symmetries and other invariant qualities of the mathcaldmetrics type d aligned einstein maxwell solutions with cosmological constant whose debever null principal directions determine shearfree geodesic null congruences we recover some properties and deduce new ones about their isometry group and about th... | [['we', 'analyze', 'the', 'symmetries', 'and', 'other', 'invariant', 'qualities', 'of', 'the', 'mathcaldmetrics', 'type', 'd', 'aligned', 'einstein', 'maxwell', 'solutions', 'with', 'cosmological', 'constant', 'whose', 'debever', 'null', 'principal', 'directions', 'determine', 'shearfree', 'geodesic', 'null', 'congruen... | [-0.2446402643234974, 0.07927116185022764, -0.05938334295705679, 0.08348977438970862, -0.18840017858668265, -0.15979661003136672, -0.07908246492692102, 0.34467033655887624, -0.2880475930981787, -0.23574379503906492, 0.10867901269840188, -0.3327196480549244, -0.1294862531905388, 0.11627584948283003, -0.01920745403965912... |
706.3302 | Zero-point momentum in Complex media | In this work we apply field regularization techniques to formulate a number
of new phenomena related to momentum induced by electromagnetic zero-point
fluctuations. We discuss the zero-point momentum associated with
magneto-electric media, with moving media, and with magneto-chiral media.
| quant-ph | in this work we apply field regularization techniques to formulate a number of new phenomena related to momentum induced by electromagnetic zeropoint fluctuations we discuss the zeropoint momentum associated with magnetoelectric media with moving media and with magnetochiral media | [['in', 'this', 'work', 'we', 'apply', 'field', 'regularization', 'techniques', 'to', 'formulate', 'a', 'number', 'of', 'new', 'phenomena', 'related', 'to', 'momentum', 'induced', 'by', 'electromagnetic', 'zeropoint', 'fluctuations', 'we', 'discuss', 'the', 'zeropoint', 'momentum', 'associated', 'with', 'magnetoelectri... | [-0.17136752285445347, 0.2246664562381995, -0.07182475088689572, 0.04249237461958845, -0.16214328825187224, -0.05680656966824944, 0.018297668023315523, 0.41800409684387535, -0.30434508754227024, -0.3044632729978707, -0.008037483412175415, -0.3193097392526957, -0.198667175303667, 0.16596963218389413, -0.0556644930337102... |
706.3303 | Soft colour interactions in hadron-hadron hard diffraction | SCI model gives a good and natural description of DDIS cross-sections.
Howevere, this model is pure phenomenological, and does not explain the nature
of soft color rearrangment. In this paper we argue, that the most capabilities
of SCI model can be derived from low constituent model and overview
applicability of low ... | hep-ph | sci model gives a good and natural description of ddis crosssections howevere this model is pure phenomenological and does not explain the nature of soft color rearrangment in this paper we argue that the most capabilities of sci model can be derived from low constituent model and overview applicability of low constitu... | [['sci', 'model', 'gives', 'a', 'good', 'and', 'natural', 'description', 'of', 'ddis', 'crosssections', 'howevere', 'this', 'model', 'is', 'pure', 'phenomenological', 'and', 'does', 'not', 'explain', 'the', 'nature', 'of', 'soft', 'color', 'rearrangment', 'in', 'this', 'paper', 'we', 'argue', 'that', 'the', 'most', 'ca... | [-0.007872281731529669, 0.10428652841259133, -0.08539067178287289, 0.06867226991082796, -0.07573691783472895, -0.1168068812567402, 0.013046335134739902, 0.35958331924947823, -0.21682820306794548, -0.35123314921828835, 0.0044396978527815505, -0.24918126091361045, -0.18654349849305368, 0.12239992138929665, -0.08893808121... |
706.3304 | Standard Model and Gravity from Spinors | We propose to unify the Gravity and Standard Model gauge groups by using
algebraic spinors of the standard four-dimensional Clifford algebra, in
left-right symmetric fashion. This generates exactly a Standard Model family of
fermions, and a Pati-Salam unification group emerges, at the Planck scale,
where (chiral) sel... | hep-th | we propose to unify the gravity and standard model gauge groups by using algebraic spinors of the standard fourdimensional clifford algebra in leftright symmetric fashion this generates exactly a standard model family of fermions and a patisalam unification group emerges at the planck scale where chiral selfdual gravit... | [['we', 'propose', 'to', 'unify', 'the', 'gravity', 'and', 'standard', 'model', 'gauge', 'groups', 'by', 'using', 'algebraic', 'spinors', 'of', 'the', 'standard', 'fourdimensional', 'clifford', 'algebra', 'in', 'leftright', 'symmetric', 'fashion', 'this', 'generates', 'exactly', 'a', 'standard', 'model', 'family', 'of'... | [-0.1560277006208477, 0.22201076329646396, -0.08237295022601603, 0.13077226886361784, -0.1297995259158943, -0.19561405244453903, -0.0478393382353472, 0.27949396021414913, -0.2614442981045011, -0.28632002123172434, 0.03789130285297009, -0.2282743562852413, -0.07773499343622949, 0.06821761446231057, -0.011735749440792372... |
706.3305 | A simple generalization of the ElGamal cryptosystem to non-abelian
groups II | This is a study of the MOR cryptosystem using the special linear group over
finite fields. The automorphism group of the special linear group is analyzed
for this purpose. At our current state of knowledge, I show that the MOR
cryptosystem has better security than the ElGamal cryptosystem over finite
fields.
| cs.CR math.GR | this is a study of the mor cryptosystem using the special linear group over finite fields the automorphism group of the special linear group is analyzed for this purpose at our current state of knowledge i show that the mor cryptosystem has better security than the elgamal cryptosystem over finite fields | [['this', 'is', 'a', 'study', 'of', 'the', 'mor', 'cryptosystem', 'using', 'the', 'special', 'linear', 'group', 'over', 'finite', 'fields', 'the', 'automorphism', 'group', 'of', 'the', 'special', 'linear', 'group', 'is', 'analyzed', 'for', 'this', 'purpose', 'at', 'our', 'current', 'state', 'of', 'knowledge', 'i', 'sho... | [-0.18719695943097273, 0.006778074629312637, -0.15465810771702843, 0.03565517181128848, -0.08638130873441696, -0.1631243097705438, -0.0009997322169296881, 0.3200416874651815, -0.31805067436367856, -0.22214013206608155, 0.15591276385912708, -0.2208396323554802, -0.10913835075117793, 0.23058781597544165, -0.1360275332505... |
706.3306 | Theoretical studies of high-harmonic generation: Effects of symmetry,
degeneracy and orientation | Using a quantum mechanical three-step model we present numerical calculations
on the high-harmonic generation from four polyatomic molecules. Ethylene
(C$_2$H$_4$) serves as an example where orbital symmetry directly affects the
harmonic yield. We treat the case of methane (CH$_4$) to address the
high-harmonic genera... | physics.atom-ph | using a quantum mechanical threestep model we present numerical calculations on the highharmonic generation from four polyatomic molecules ethylene c_2h_4 serves as an example where orbital symmetry directly affects the harmonic yield we treat the case of methane ch_4 to address the highharmonic generation resulting fr... | [['using', 'a', 'quantum', 'mechanical', 'threestep', 'model', 'we', 'present', 'numerical', 'calculations', 'on', 'the', 'highharmonic', 'generation', 'from', 'four', 'polyatomic', 'molecules', 'ethylene', 'c_2h_4', 'serves', 'as', 'an', 'example', 'where', 'orbital', 'symmetry', 'directly', 'affects', 'the', 'harmoni... | [-0.0681287878234049, 0.17534526405217868, -0.031250667388496155, 0.03469527298276422, 0.009481927525484934, -0.08677411212257165, 0.01981218078221633, 0.41832561045885086, -0.26045281551962357, -0.2587207064224297, 0.00799307222426732, -0.31401589779895456, -0.14053495663136026, 0.18603808877592468, 0.0192931804104934... |
706.3307 | Graviweak Unification | The coupling of chiral fermions to gravity makes use only of the selfdual
SU(2) subalgebra of the (complexified) SO(3,1) algebra. It is possible to
identify the antiselfdual subalgebra with the SU(2)_L isospin group that
appears in the Standard Model, or with its right-handed counterpart SU(2)_R
that appears in some ... | hep-th | the coupling of chiral fermions to gravity makes use only of the selfdual su2 subalgebra of the complexified so31 algebra it is possible to identify the antiselfdual subalgebra with the su2_l isospin group that appears in the standard model or with its righthanded counterpart su2_r that appears in some extensions based... | [['the', 'coupling', 'of', 'chiral', 'fermions', 'to', 'gravity', 'makes', 'use', 'only', 'of', 'the', 'selfdual', 'su2', 'subalgebra', 'of', 'the', 'complexified', 'so31', 'algebra', 'it', 'is', 'possible', 'to', 'identify', 'the', 'antiselfdual', 'subalgebra', 'with', 'the', 'su2_l', 'isospin', 'group', 'that', 'appe... | [-0.18839702582252876, 0.15862076526165617, -0.061859131476494994, 0.09750441521197101, -0.15529048803965656, -0.15918350478216092, -0.010698593411670655, 0.3532417371336903, -0.22261778546535238, -0.26346904467981386, 0.0630721639169437, -0.2511124942660788, -0.13299615168231255, 0.0591311137410527, 0.0026567872537642... |
706.3308 | Simulating the formation and evolution of galaxies: Multi-phase
description of the interstellar medium, star formation, and energy feedback | We present a multi-phase representation of the ISM in NB-TSPH simulations of
galaxy formation and evolution with particular attention to the case of
early-type galaxies. Cold gas clouds are described by the so-called sticky
particles algorithm. They can freely move throughout the hot ISM medium; stars
form within the... | astro-ph | we present a multiphase representation of the ism in nbtsph simulations of galaxy formation and evolution with particular attention to the case of earlytype galaxies cold gas clouds are described by the socalled sticky particles algorithm they can freely move throughout the hot ism medium stars form within these clouds... | [['we', 'present', 'a', 'multiphase', 'representation', 'of', 'the', 'ism', 'in', 'nbtsph', 'simulations', 'of', 'galaxy', 'formation', 'and', 'evolution', 'with', 'particular', 'attention', 'to', 'the', 'case', 'of', 'earlytype', 'galaxies', 'cold', 'gas', 'clouds', 'are', 'described', 'by', 'the', 'socalled', 'sticky... | [-0.04576505392936106, 0.13688253535805509, -0.05489521252904804, 0.08663609983789054, -0.09675833856304869, -0.049796454554710254, 0.04715454581235416, 0.43174848857168585, -0.14902492462752912, -0.3156644304951605, 0.012207056917339707, -0.2869525159446475, -0.005822787001633491, 0.18249782907794446, -0.0074466400084... |
706.3309 | Variational methods in relativistic quantum mechanics | This review is devoted to the study of stationary solutions of linear and
nonlinear equations from relativistic quantum mechanics, involving the Dirac
operator. The solutions are found as critical points of an energy functional.
Contrary to the Laplacian appearing in the equations of nonrelativistic quantum
mechanics... | math-ph math.AP math.MP | this review is devoted to the study of stationary solutions of linear and nonlinear equations from relativistic quantum mechanics involving the dirac operator the solutions are found as critical points of an energy functional contrary to the laplacian appearing in the equations of nonrelativistic quantum mechanics the ... | [['this', 'review', 'is', 'devoted', 'to', 'the', 'study', 'of', 'stationary', 'solutions', 'of', 'linear', 'and', 'nonlinear', 'equations', 'from', 'relativistic', 'quantum', 'mechanics', 'involving', 'the', 'dirac', 'operator', 'the', 'solutions', 'are', 'found', 'as', 'critical', 'points', 'of', 'an', 'energy', 'fun... | [-0.10288217060694782, 0.08227816075561956, -0.08317184681072831, 0.08079265755523617, -0.1126390207062165, -0.1373101177904755, -0.03944311803517242, 0.29860183884079256, -0.29125667175937753, -0.27106914229070145, 0.12204225310900559, -0.30317532443751893, -0.18153545733075588, 0.18382530796846064, -0.059545765388756... |
706.331 | Josephson-Like Behaviour of Granular Carbon Films | This work presents the study of some new anomalous electromagnetic effects in
graphite-like thin carbon films. These are: The fast switching (1nanosecond) of
electrical conductivity The detection of microwave radiation and its
temperature dependence The oscillations of film stack magnetization in the
magnetic field o... | cond-mat.supr-con cond-mat.soft | this work presents the study of some new anomalous electromagnetic effects in graphitelike thin carbon films these are the fast switching 1nanosecond of electrical conductivity the detection of microwave radiation and its temperature dependence the oscillations of film stack magnetization in the magnetic field of 15 t ... | [['this', 'work', 'presents', 'the', 'study', 'of', 'some', 'new', 'anomalous', 'electromagnetic', 'effects', 'in', 'graphitelike', 'thin', 'carbon', 'films', 'these', 'are', 'the', 'fast', 'switching', '1nanosecond', 'of', 'electrical', 'conductivity', 'the', 'detection', 'of', 'microwave', 'radiation', 'and', 'its', ... | [-0.23696327200641149, 0.18942223994419963, -0.015792420904698044, -0.0532096975188763, -0.07632100446037306, -0.13444130785024627, 0.09381248661880275, 0.4009219665487094, -0.23188642516796446, -0.321447087057074, 0.023914573189599074, -0.28226929414353663, -0.07342482578235507, 0.27464853617598184, 0.0312063754268590... |
706.3311 | Blue straggler stars in dwarf spheroidal galaxies | Blue straggler star (BSS) candidates have been observed in all old dwarf
spheroidal galaxies (dSphs), however whether or not they are authentic BSSs or
young stars has been a point of debate. To both address this issue and obtain a
better understanding of the formation of BSSs in different environments we have
analys... | astro-ph | blue straggler star bss candidates have been observed in all old dwarf spheroidal galaxies dsphs however whether or not they are authentic bsss or young stars has been a point of debate to both address this issue and obtain a better understanding of the formation of bsss in different environments we have analysed a sam... | [['blue', 'straggler', 'star', 'bss', 'candidates', 'have', 'been', 'observed', 'in', 'all', 'old', 'dwarf', 'spheroidal', 'galaxies', 'dsphs', 'however', 'whether', 'or', 'not', 'they', 'are', 'authentic', 'bsss', 'or', 'young', 'stars', 'has', 'been', 'a', 'point', 'of', 'debate', 'to', 'both', 'address', 'this', 'is... | [-0.06721255282172933, 0.09416202984957231, -0.12255285490925114, 0.12376869050475459, -0.1291298395115882, -0.06650442459930976, 0.07702903860972987, 0.467069622443782, -0.10273459139952643, -0.3698557911042331, 0.022707207142892812, -0.28535005791578444, -0.05167440370346109, 0.1822920887099786, -0.08242657530610611,... |
706.3312 | Two-flow magnetohydrodynamical jets around young stellar objects | We present the first-ever simulations of non-ideal magnetohydrodynamical
(MHD) stellar winds coupled with disc-driven jets where the resistive and
viscous accretion disc is self-consistently described. The transmagnetosonic,
collimated MHD outflows are investigated numerically using the VAC code. Our
simulations show... | astro-ph | we present the firstever simulations of nonideal magnetohydrodynamical mhd stellar winds coupled with discdriven jets where the resistive and viscous accretion disc is selfconsistently described the transmagnetosonic collimated mhd outflows are investigated numerically using the vac code our simulations show that the i... | [['we', 'present', 'the', 'firstever', 'simulations', 'of', 'nonideal', 'magnetohydrodynamical', 'mhd', 'stellar', 'winds', 'coupled', 'with', 'discdriven', 'jets', 'where', 'the', 'resistive', 'and', 'viscous', 'accretion', 'disc', 'is', 'selfconsistently', 'described', 'the', 'transmagnetosonic', 'collimated', 'mhd',... | [-0.126169643659309, 0.18285229876988418, -0.03909300283789087, 0.08101901118712061, -0.08346318884697908, -0.04965376274605446, -0.07629962230772327, 0.38924559331772957, -0.24695744714973605, -0.3074296828359365, 0.0475190107455573, -0.19972544823061017, -0.00045668496407897156, 0.2372545528006466, 0.0039520897505366... |
706.3313 | Parity properties of Costas arrays defined via finite fields | A Costas array of order $n$ is an arrangement of dots and blanks into $n$
rows and $n$ columns, with exactly one dot in each row and each column, the
arrangement satisfying certain specified conditions. A dot occurring in such an
array is even/even if it occurs in the $i$-th row and $j$-th column, where $i$
and $j$ a... | math.CO math.NT | a costas array of order n is an arrangement of dots and blanks into n rows and n columns with exactly one dot in each row and each column the arrangement satisfying certain specified conditions a dot occurring in such an array is eveneven if it occurs in the ith row and jth column where i and j are both even integers a... | [['a', 'costas', 'array', 'of', 'order', 'n', 'is', 'an', 'arrangement', 'of', 'dots', 'and', 'blanks', 'into', 'n', 'rows', 'and', 'n', 'columns', 'with', 'exactly', 'one', 'dot', 'in', 'each', 'row', 'and', 'each', 'column', 'the', 'arrangement', 'satisfying', 'certain', 'specified', 'conditions', 'a', 'dot', 'occurr... | [-0.2062594827943011, 0.22051870054095954, 0.04217164861839465, 0.04303412968593259, 0.030261083026616883, -0.20556877583505645, -0.023955674646722692, 0.36986691409581773, -0.2428794652123445, -0.30589760754818235, 0.07898904671341742, -0.33059882859308876, -0.10935127473015699, 0.15067481480899356, -0.014784016906188... |
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