id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
709.2235 | Bound diquarks and their Bose-Einstein condensation in strongly coupled
quark matter | We explore the formation of diquark molecules and their Bose-Einstein
condensation (BEC) in the phase diagram of three-flavor quark matter at nonzero
temperature, T, and quark chemical potential, mu. Using a quark model with a
four-fermion interaction, we identify possible diquark excitations as poles of
the microsco... | hep-ph | we explore the formation of diquark molecules and their boseeinstein condensation bec in the phase diagram of threeflavor quark matter at nonzero temperature t and quark chemical potential mu using a quark model with a fourfermion interaction we identify possible diquark excitations as poles of the microscopically comp... | [['we', 'explore', 'the', 'formation', 'of', 'diquark', 'molecules', 'and', 'their', 'boseeinstein', 'condensation', 'bec', 'in', 'the', 'phase', 'diagram', 'of', 'threeflavor', 'quark', 'matter', 'at', 'nonzero', 'temperature', 't', 'and', 'quark', 'chemical', 'potential', 'mu', 'using', 'a', 'quark', 'model', 'with',... | [-0.1676589887633565, 0.33003996771627236, -0.09462122754785159, 0.1481999146090525, -0.02005959115922451, -0.15476112951809126, 0.10369301861565974, 0.33223344207490013, -0.14224871805322076, -0.2058587283014305, -0.10930366308959838, -0.2802878182736181, -0.021688524293639357, -0.010735758593202464, 0.172668877405129... |
709.2236 | Jarzynski Relation, Fluctuation Theorems, and Stochastic Thermodynamics
for Non-Markovian Processes | We prove the Jarzynski relation for general stochastic processes including
non-Markovian systems with memory. The only requirement for our proof is the
existence of a stationary state, therefore excluding non-ergodic systems. We
then show how the concepts of stochastic thermodynamics can be used to prove
further exac... | cond-mat.stat-mech | we prove the jarzynski relation for general stochastic processes including nonmarkovian systems with memory the only requirement for our proof is the existence of a stationary state therefore excluding nonergodic systems we then show how the concepts of stochastic thermodynamics can be used to prove further exact noneq... | [['we', 'prove', 'the', 'jarzynski', 'relation', 'for', 'general', 'stochastic', 'processes', 'including', 'nonmarkovian', 'systems', 'with', 'memory', 'the', 'only', 'requirement', 'for', 'our', 'proof', 'is', 'the', 'existence', 'of', 'a', 'stationary', 'state', 'therefore', 'excluding', 'nonergodic', 'systems', 'we'... | [-0.11719955979580325, 0.1286115632983782, -0.1603648905450153, 0.16499998476097566, -0.018493221717930976, -0.16486114250969083, 0.07453612054121636, 0.25679072303076583, -0.3271086309105158, -0.21429893772103012, 0.08130280849420363, -0.27476357891120845, -0.14070051417700827, 0.2565433249350578, -0.0610057164338373,... |
709.2237 | An efficient source of continuous variable polarisation entanglement | We have experimentally demonstrated the efficient creation of highly
entangled bipartite continuous variable polarisation states. Exploiting an
optimised scheme for the production of squeezing using the Kerr non-linearity
of a glass fibre we generated polarisation squeezed pulses with a mean
classical excitation in S... | quant-ph | we have experimentally demonstrated the efficient creation of highly entangled bipartite continuous variable polarisation states exploiting an optimised scheme for the production of squeezing using the kerr nonlinearity of a glass fibre we generated polarisation squeezed pulses with a mean classical excitation in s3 po... | [['we', 'have', 'experimentally', 'demonstrated', 'the', 'efficient', 'creation', 'of', 'highly', 'entangled', 'bipartite', 'continuous', 'variable', 'polarisation', 'states', 'exploiting', 'an', 'optimised', 'scheme', 'for', 'the', 'production', 'of', 'squeezing', 'using', 'the', 'kerr', 'nonlinearity', 'of', 'a', 'gl... | [-0.17360875080149804, 0.21608456687404806, -0.05972992359981973, 0.0509069114543862, 0.041350504940213716, -0.18523043290833416, 0.025717021574762286, 0.41796727707285597, -0.21299894422333202, -0.2956490382810285, 0.03956231840888706, -0.30260820387174253, -0.02184478676898162, 0.20841707484594182, -0.014674061722041... |
709.2238 | Quaternionen and Geometric Algebra (Quaternionen und Geometrische
Algebra) | In the last one and a half centuries, the analysis of quaternions has not
only led to further developments in mathematics but has also been and remains
an important catalyst for the further development of theories in physics. At
the same time, Hestenes geometric algebra provides a didactically promising
instrument to... | physics.ed-ph | in the last one and a half centuries the analysis of quaternions has not only led to further developments in mathematics but has also been and remains an important catalyst for the further development of theories in physics at the same time hestenes geometric algebra provides a didactically promising instrument to mode... | [['in', 'the', 'last', 'one', 'and', 'a', 'half', 'centuries', 'the', 'analysis', 'of', 'quaternions', 'has', 'not', 'only', 'led', 'to', 'further', 'developments', 'in', 'mathematics', 'but', 'has', 'also', 'been', 'and', 'remains', 'an', 'important', 'catalyst', 'for', 'the', 'further', 'development', 'of', 'theories... | [-0.08103676957666482, 0.06760480021215412, -0.1823756929732075, 0.06745417118869036, -0.13528546030191999, -0.1459667299432974, -0.0075124288517001425, 0.35141921782572016, -0.2966683364865419, -0.31504883109346815, 0.13233754359626848, -0.21399475016974304, -0.19231402351471938, 0.22301975583510572, -0.12947906975291... |
709.2239 | Brane Inflation and Fine Tuning | We argue about the importance of embedding the successful mechanism of
Inflation in the context of a fundamental theory. We review some of the
attempts in this direction made in the framework of String Theory. In
particular we report on recent developments in Brane Inflation with emphasis on
the fine tuning issue.
| hep-th | we argue about the importance of embedding the successful mechanism of inflation in the context of a fundamental theory we review some of the attempts in this direction made in the framework of string theory in particular we report on recent developments in brane inflation with emphasis on the fine tuning issue | [['we', 'argue', 'about', 'the', 'importance', 'of', 'embedding', 'the', 'successful', 'mechanism', 'of', 'inflation', 'in', 'the', 'context', 'of', 'a', 'fundamental', 'theory', 'we', 'review', 'some', 'of', 'the', 'attempts', 'in', 'this', 'direction', 'made', 'in', 'the', 'framework', 'of', 'string', 'theory', 'in',... | [-0.1420789801587279, 0.10117311753072919, -0.0777167211053893, 0.059009022695066124, -0.07630261696445254, -0.06494171432971668, 0.0546203613630496, 0.38220617553004277, -0.22297028437829935, -0.2987699922926437, 0.10864591330755502, -0.20159564743964717, -0.21321132141523635, 0.15574544198954335, -0.11070014122658624... |
709.224 | Shifted polynomials in a convection problem | The onset of convection in a horizontal layer of fluid heated from below in
the presence of a gravity field varying across the layer is investigated. The
eigenvalue problem governing the linear stability of the mechanical equilibria
of the fluid layer in the case of free boundaries is solved using a Galerkin
method b... | math-ph math.MP math.SP | the onset of convection in a horizontal layer of fluid heated from below in the presence of a gravity field varying across the layer is investigated the eigenvalue problem governing the linear stability of the mechanical equilibria of the fluid layer in the case of free boundaries is solved using a galerkin method base... | [['the', 'onset', 'of', 'convection', 'in', 'a', 'horizontal', 'layer', 'of', 'fluid', 'heated', 'from', 'below', 'in', 'the', 'presence', 'of', 'a', 'gravity', 'field', 'varying', 'across', 'the', 'layer', 'is', 'investigated', 'the', 'eigenvalue', 'problem', 'governing', 'the', 'linear', 'stability', 'of', 'the', 'me... | [-0.1720506941869122, 0.12158451800341488, -0.08018688943817234, -0.027066911460037847, -0.03928340319544077, -0.09578411845246056, 0.03125918222224859, 0.28294588738411175, -0.35651414664309533, -0.24982535271126716, 0.10754042359061355, -0.2348012963279349, -0.10962456299877557, 0.14821005130156142, -0.03112701178513... |
709.2241 | Influence of particle shape on shear stress in granular media | We analyze the contact and force networks in a dense confined packing of
pentagonal particles simulated by means of the contact dynamics method. The
particle shape effect is evidenced by comparing the data from pentagon packing
and from a packing with identical characteristics except for the circular shape
of the par... | physics.class-ph | we analyze the contact and force networks in a dense confined packing of pentagonal particles simulated by means of the contact dynamics method the particle shape effect is evidenced by comparing the data from pentagon packing and from a packing with identical characteristics except for the circular shape of the partic... | [['we', 'analyze', 'the', 'contact', 'and', 'force', 'networks', 'in', 'a', 'dense', 'confined', 'packing', 'of', 'pentagonal', 'particles', 'simulated', 'by', 'means', 'of', 'the', 'contact', 'dynamics', 'method', 'the', 'particle', 'shape', 'effect', 'is', 'evidenced', 'by', 'comparing', 'the', 'data', 'from', 'penta... | [-0.1708696234882708, 0.17990442165376053, -0.08770440151186093, 0.009058107456961728, -0.019565683459032975, -0.105193776305279, 0.0338343186415327, 0.3755916829990304, -0.2647402849250837, -0.30304832819687283, 0.019909096517316673, -0.31175322497830443, -0.16883384205562912, 0.12272916538742087, -0.01041155685873135... |
709.2242 | XMM-Newton observations of XTE J1817-330 and XTE J1856+053 | The black hole candidate XTE J1817-330 was discovered in outburst on 26
January 2006 with RXTE/ASM. One year later, on 28 February 2007, another X-ray
transient discovered in 1996, XTE J1856+053, was detected by RXTE during a new
outburst. We report on the spectra obtained by XMM-Newton of these two black
hole candid... | astro-ph | the black hole candidate xte j1817330 was discovered in outburst on 26 january 2006 with rxteasm one year later on 28 february 2007 another xray transient discovered in 1996 xte j1856053 was detected by rxte during a new outburst we report on the spectra obtained by xmmnewton of these two black hole candidates | [['the', 'black', 'hole', 'candidate', 'xte', 'j1817330', 'was', 'discovered', 'in', 'outburst', 'on', '26', 'january', '2006', 'with', 'rxteasm', 'one', 'year', 'later', 'on', '28', 'february', '2007', 'another', 'xray', 'transient', 'discovered', 'in', '1996', 'xte', 'j1856053', 'was', 'detected', 'by', 'rxte', 'duri... | [-0.08412658686767209, 0.08694100774438032, -0.08501577263979136, 0.09449897407782527, -0.14310816594592804, -0.1581066683514641, 0.1244449655191516, 0.3966068738614613, -0.05926030505457366, -0.4659232613938105, 0.21231033142550654, -0.45879869197301987, -0.07665768789373478, 0.3084887687890035, -0.09659787966817054, ... |
709.2243 | Rate Determining Factors in Protein Model Structures | Previous research has shown a strong correlation of protein folding rates to
the native state geometry, yet a complete explanation for this dependence is
still lacking. Here we study the rate-geometry relationship with a simple
statistical physics model, and focus on two classes of model geometries,
representing idea... | q-bio.BM cond-mat.stat-mech | previous research has shown a strong correlation of protein folding rates to the native state geometry yet a complete explanation for this dependence is still lacking here we study the rategeometry relationship with a simple statistical physics model and focus on two classes of model geometries representing ideal paral... | [['previous', 'research', 'has', 'shown', 'a', 'strong', 'correlation', 'of', 'protein', 'folding', 'rates', 'to', 'the', 'native', 'state', 'geometry', 'yet', 'a', 'complete', 'explanation', 'for', 'this', 'dependence', 'is', 'still', 'lacking', 'here', 'we', 'study', 'the', 'rategeometry', 'relationship', 'with', 'a'... | [-0.13689243344699942, 0.07220020401438704, -0.07463685722414697, 0.08660337525639641, -0.06146445494207941, -0.12586876742405753, 0.036918028561251884, 0.41772000663233605, -0.24696069980940122, -0.29568189360578073, 0.05059238604473976, -0.25651435876327955, -0.17943687751899692, 0.20495872851984387, -0.0028775647868... |
709.2244 | A numerical finite size scaling approach to many-body localization | We develop a numerical technique to study Anderson localization in
interacting electronic systems. The ground state of the disordered system is
calculated with quantum Monte-Carlo simulations while the localization
properties are extracted from the ``Thouless conductance'' $g$, i.e. the
curvature of the energy with r... | cond-mat.dis-nn cond-mat.str-el | we develop a numerical technique to study anderson localization in interacting electronic systems the ground state of the disordered system is calculated with quantum montecarlo simulations while the localization properties are extracted from the thouless conductance g ie the curvature of the energy with respect to an ... | [['we', 'develop', 'a', 'numerical', 'technique', 'to', 'study', 'anderson', 'localization', 'in', 'interacting', 'electronic', 'systems', 'the', 'ground', 'state', 'of', 'the', 'disordered', 'system', 'is', 'calculated', 'with', 'quantum', 'montecarlo', 'simulations', 'while', 'the', 'localization', 'properties', 'are... | [-0.18776115187506934, 0.16562203340991044, -0.06261638328393573, 0.05634048827568669, 0.02876261958726129, -0.14924045210956768, 0.0421879126954729, 0.37627792718299363, -0.26269821442221686, -0.27749559797309103, 0.014552770220966599, -0.32244149046176573, -0.10851122931009001, 0.17733120397364688, 0.0212365637298562... |
709.2245 | Convergence of weighted averages of relaxed projections | The convergence of the algorithm for solving convex feasibility problem is
studied by the method of sequential averaged and relaxed projections. Some
results of H. H. Bauschke and J. M. Borwein are generalized by introducing new
methods. Examples illustrating these generalizations are given.
| math.MG | the convergence of the algorithm for solving convex feasibility problem is studied by the method of sequential averaged and relaxed projections some results of h h bauschke and j m borwein are generalized by introducing new methods examples illustrating these generalizations are given | [['the', 'convergence', 'of', 'the', 'algorithm', 'for', 'solving', 'convex', 'feasibility', 'problem', 'is', 'studied', 'by', 'the', 'method', 'of', 'sequential', 'averaged', 'and', 'relaxed', 'projections', 'some', 'results', 'of', 'h', 'h', 'bauschke', 'and', 'j', 'm', 'borwein', 'are', 'generalized', 'by', 'introdu... | [-0.08972245970264424, 0.05071058597545638, 8.875499804352605e-05, 0.06993747989073136, -0.04028091411279558, -0.17785286151825688, 0.024635598030980935, 0.37991730931626505, -0.3040182859052059, -0.3261238284149142, 0.16103864101649717, -0.24863779824227095, -0.14836006611585617, 0.23640930084619932, -0.08042626082897... |
709.2246 | Chiral Phase Transition beyond Mean Field Approximation | Based on the analogy between the Nambu--Jona-Lasinio model of chiral symmetry
breaking and the BCS theory of superconductivity, we investigate the effect of
$\bar q q$ pair fluctuations on the chiral phase transition. We include
uncondensed $\bar q q$ pairs at finite temperature and chemical potential in a
self-consi... | hep-ph cond-mat.supr-con nucl-th | based on the analogy between the nambujonalasinio model of chiral symmetry breaking and the bcs theory of superconductivity we investigate the effect of bar q q pair fluctuations on the chiral phase transition we include uncondensed bar q q pairs at finite temperature and chemical potential in a selfconsistent tmatrix ... | [['based', 'on', 'the', 'analogy', 'between', 'the', 'nambujonalasinio', 'model', 'of', 'chiral', 'symmetry', 'breaking', 'and', 'the', 'bcs', 'theory', 'of', 'superconductivity', 'we', 'investigate', 'the', 'effect', 'of', 'bar', 'q', 'q', 'pair', 'fluctuations', 'on', 'the', 'chiral', 'phase', 'transition', 'we', 'in... | [-0.19854771891065562, 0.2527172284252528, -0.09484600514406338, 0.06073171327201029, -0.024432463707247127, -0.1203844187160333, 0.12349640497025878, 0.30606148549769485, -0.21374559751711786, -0.22745741748561463, -0.08483397908437634, -0.3206636082743191, -0.08852848651198049, 0.04728593116871909, 0.0823659865386111... |
709.2247 | Downhill versus two-state protein folding in a statistical mechanical
model | The authors address the problem of downhill protein folding in the framework
of a simple statistical mechanical model, which allows an exact solution for
the equilibrium and a semianalytical treatment of the kinetics. Focusing on
protein 1BBL, a candidate for downhill folding behavior, and comparing it to
the WW doma... | q-bio.BM cond-mat.stat-mech | the authors address the problem of downhill protein folding in the framework of a simple statistical mechanical model which allows an exact solution for the equilibrium and a semianalytical treatment of the kinetics focusing on protein 1bbl a candidate for downhill folding behavior and comparing it to the ww domain of ... | [['the', 'authors', 'address', 'the', 'problem', 'of', 'downhill', 'protein', 'folding', 'in', 'the', 'framework', 'of', 'a', 'simple', 'statistical', 'mechanical', 'model', 'which', 'allows', 'an', 'exact', 'solution', 'for', 'the', 'equilibrium', 'and', 'a', 'semianalytical', 'treatment', 'of', 'the', 'kinetics', 'fo... | [-0.07306072989478707, 0.1029640787061362, -0.1062902014888823, 0.11114294272963889, -0.031531184350606055, -0.1713995107403025, 0.08258976388955488, 0.37038887701928613, -0.2701071550138295, -0.2649757886538282, 0.0484895965247415, -0.2635316677043738, -0.1394270079024136, 0.17596013248665257, 0.002502753371372819, 0.... |
709.2248 | Update on Ion Studies | The effect of ions has received one of the highest priorities in R&D for the
damping rings of the International Linear Collider(ILC). It is detrimental to
the performance of the electron damping ring. In this note, an update
concerning the ion studies for the ILC damping ring is given. We investigate
the gap role and... | physics.acc-ph physics.gen-ph | the effect of ions has received one of the highest priorities in rd for the damping rings of the international linear colliderilc it is detrimental to the performance of the electron damping ring in this note an update concerning the ion studies for the ilc damping ring is given we investigate the gap role and irregula... | [['the', 'effect', 'of', 'ions', 'has', 'received', 'one', 'of', 'the', 'highest', 'priorities', 'in', 'rd', 'for', 'the', 'damping', 'rings', 'of', 'the', 'international', 'linear', 'colliderilc', 'it', 'is', 'detrimental', 'to', 'the', 'performance', 'of', 'the', 'electron', 'damping', 'ring', 'in', 'this', 'note', '... | [-0.16816775052732713, 0.10583186237400279, -0.03778497624129208, 0.052882037619506383, -0.01766099519020802, -0.09227277223977286, -0.03468491903481048, 0.36341169864140654, -0.26438464975689313, -0.241400353421734, 0.08615040223387926, -0.30239067551824644, -0.08723345334717147, 0.18274518062134046, -0.02867800913549... |
709.2249 | Heegaard Splittings of Twisted Torus Knots | Little is known on the classification of Heegaard splittings for hyperbolic
3-manifolds. Although Kobayashi gave a complete classification of Heegaard
splittings for the exteriors of 2-bridge knots, our knowledge of other classes
is extremely limited. In particular, there are very few hyperbolic manifolds
that are kn... | math.GT | little is known on the classification of heegaard splittings for hyperbolic 3manifolds although kobayashi gave a complete classification of heegaard splittings for the exteriors of 2bridge knots our knowledge of other classes is extremely limited in particular there are very few hyperbolic manifolds that are known to h... | [['little', 'is', 'known', 'on', 'the', 'classification', 'of', 'heegaard', 'splittings', 'for', 'hyperbolic', '3manifolds', 'although', 'kobayashi', 'gave', 'a', 'complete', 'classification', 'of', 'heegaard', 'splittings', 'for', 'the', 'exteriors', 'of', '2bridge', 'knots', 'our', 'knowledge', 'of', 'other', 'classe... | [-0.26175313631496727, 0.14576790080289875, -0.07791134567066495, 0.17348635887901764, -0.15268983311086362, -0.23261305888965061, -0.04395514373858792, 0.40329725385527126, -0.21641848104939396, -0.34058305157148944, 0.09063774353957602, -0.24455197088328923, -0.14930208275057208, 0.2523874577267894, -0.18189277550637... |
709.225 | Crystal and magnetic structures of the spin-trimer compounds Ca3 Cu3xNix
(PO4)4 (x=0,1,2) | Crystal and magnetic structures of a series of novel quantum spin trimer
system Ca3Cu3xNix(PO4)4 (x=0,1,2) were studied by neutron powder diffraction at
the temperatures 1.5-290 K. The composition with one Ni per trimer (x=1) has a
monoclinic structure (space group P 21 /a, no. 14) with the unit cell
parameters a = 1... | cond-mat.mtrl-sci cond-mat.str-el | crystal and magnetic structures of a series of novel quantum spin trimer system ca3cu3xnixpo44 x012 were studied by neutron powder diffraction at the temperatures 15290 k the composition with one ni per trimer x1 has a monoclinic structure space group p 21 a no 14 with the unit cell parameters a 1771 a b 489 a c 885 a ... | [['crystal', 'and', 'magnetic', 'structures', 'of', 'a', 'series', 'of', 'novel', 'quantum', 'spin', 'trimer', 'system', 'ca3cu3xnixpo44', 'x012', 'were', 'studied', 'by', 'neutron', 'powder', 'diffraction', 'at', 'the', 'temperatures', '15290', 'k', 'the', 'composition', 'with', 'one', 'ni', 'per', 'trimer', 'x1', 'ha... | [-0.16177153591706883, 0.2053608069783877, 0.01304591328225797, -0.0071514833597272325, -0.019617821480884836, -0.1397504915910152, 0.08507124680666796, 0.424375291079438, -0.25591547977528534, -0.28763678024018496, 0.02783040079715041, -0.36249146721481035, -0.031829422993178015, 0.11939961673827687, 0.092866388046725... |
709.2251 | Multiterminal Nanowire Junctions of Silicon: A Theoretical Prediction of
Atomic Structure and Electronic Properties | Using empirical scheme, atomic structure of a new exotic class of silicon
nanoclusters was elaborated upon the central icosahedral core (Si-IC) and
pentagonal petals (Si-PP) growing from Si-IC vertexes. It was shown that
Si-IC/Si-PP interface formation is energetically preferable. Some experimental
observations of si... | cond-mat.mtrl-sci | using empirical scheme atomic structure of a new exotic class of silicon nanoclusters was elaborated upon the central icosahedral core siic and pentagonal petals sipp growing from siic vertexes it was shown that siicsipp interface formation is energetically preferable some experimental observations of silicon nanostruc... | [['using', 'empirical', 'scheme', 'atomic', 'structure', 'of', 'a', 'new', 'exotic', 'class', 'of', 'silicon', 'nanoclusters', 'was', 'elaborated', 'upon', 'the', 'central', 'icosahedral', 'core', 'siic', 'and', 'pentagonal', 'petals', 'sipp', 'growing', 'from', 'siic', 'vertexes', 'it', 'was', 'shown', 'that', 'siicsi... | [-0.11631743182119926, 0.11340051014767467, -0.06898100913869558, 0.056587293109541734, -0.06098858220502734, -0.14355264299116294, 0.02960694757532853, 0.42654483347211336, -0.22070633571490017, -0.32353916278922223, 0.025187463286450842, -0.273871012451783, -0.1867893712765629, 0.16243682613163452, 0.0017365991780665... |
709.2252 | Otiy: Loactors tracking nodes | We propose Otiy, a node-centric location service that limits the impact of
location updates generate by mobile nodes in IEEE802.11-based wireless mesh
networks. Existing location services use node identifiers to determine the
locator (aka anchor) that is responsible for keeping track of a node's
location. Such a stra... | cs.NI | we propose otiy a nodecentric location service that limits the impact of location updates generate by mobile nodes in ieee80211based wireless mesh networks existing location services use node identifiers to determine the locator aka anchor that is responsible for keeping track of a nodes location such a strategy can be... | [['we', 'propose', 'otiy', 'a', 'nodecentric', 'location', 'service', 'that', 'limits', 'the', 'impact', 'of', 'location', 'updates', 'generate', 'by', 'mobile', 'nodes', 'in', 'ieee80211based', 'wireless', 'mesh', 'networks', 'existing', 'location', 'services', 'use', 'node', 'identifiers', 'to', 'determine', 'the', '... | [-0.18440100118781613, 0.07256156405994454, -0.015575938017428976, 0.02507007858443972, -0.10431489507890249, -0.19783572691896584, 0.16714025889131842, 0.37865094657558784, -0.27587376285212495, -0.3505208358102668, 0.09405953408192134, -0.30924937938982866, -0.1114157694721578, 0.11866390832238295, -0.081131079131675... |
709.2253 | Gravitational waves originated before compactification in Kaluza-Klein
theory | We investigate the propagation of multidimensional gravitational waves
generated before compactification and observes today as 4-dimensional
gravitational waves and gauge fields by generalizing the investigation of
Alesci and Montani(AM) to the case where the internal space is an n-sphere. We
also derive the 4-dimens... | gr-qc | we investigate the propagation of multidimensional gravitational waves generated before compactification and observes today as 4dimensional gravitational waves and gauge fields by generalizing the investigation of alesci and montaniam to the case where the internal space is an nsphere we also derive the 4dimensional fo... | [['we', 'investigate', 'the', 'propagation', 'of', 'multidimensional', 'gravitational', 'waves', 'generated', 'before', 'compactification', 'and', 'observes', 'today', 'as', '4dimensional', 'gravitational', 'waves', 'and', 'gauge', 'fields', 'by', 'generalizing', 'the', 'investigation', 'of', 'alesci', 'and', 'montania... | [-0.14666773937534783, 0.1918206336247547, -0.05656729913661601, 0.08835020506025844, -0.14318675397360628, -0.04338248478490169, -0.03317355277680757, 0.314065821537817, -0.2752315660710102, -0.24141767807089276, 0.106961691606557, -0.24862018613041276, -0.1689120827122005, 0.18049172445898876, -0.0203689639284103, -0... |
709.2254 | High Resolution Cavity BPM for ILC Final Focal System (IP-BPM) | IP-BPM (Interaction Point Beam Position Monitor) is an ultra high resolution
cavity BPM to be used at ATF2, a test facility for ILC final focus system.
Control of beam position in 2 nm precision is required for ATF2. Beam tests at
ATF extraction line proved a 8.7 nm position resolution.
| physics.acc-ph | ipbpm interaction point beam position monitor is an ultra high resolution cavity bpm to be used at atf2 a test facility for ilc final focus system control of beam position in 2 nm precision is required for atf2 beam tests at atf extraction line proved a 87 nm position resolution | [['ipbpm', 'interaction', 'point', 'beam', 'position', 'monitor', 'is', 'an', 'ultra', 'high', 'resolution', 'cavity', 'bpm', 'to', 'be', 'used', 'at', 'atf2', 'a', 'test', 'facility', 'for', 'ilc', 'final', 'focus', 'system', 'control', 'of', 'beam', 'position', 'in', '2', 'nm', 'precision', 'is', 'required', 'for', '... | [-0.08719186173105727, 0.09585383997509038, -0.07668221352279794, -0.007032736963639986, 0.011259840269173895, -0.2943894937064271, 0.011185558049521429, 0.4741558223126494, -0.1837290855390685, -0.3325340245869391, 0.08279116478824645, -0.2737415813156689, 0.18702053240671448, 0.22819406696956376, -0.00731715368943250... |
709.2255 | Non unique solutions to boundary value problems for non symmetric
divergence form equations | We calculate explicitly solutions to the Dirichlet and Neumann boundary value
problems in the upper half plane, for a family of divergence form equations
with non symmetric coefficients with a jump discontinuity. It is shown that the
boundary equation method and the Lax--Milgram method for constructing solutions
may ... | math.AP math.CA | we calculate explicitly solutions to the dirichlet and neumann boundary value problems in the upper half plane for a family of divergence form equations with non symmetric coefficients with a jump discontinuity it is shown that the boundary equation method and the laxmilgram method for constructing solutions may give t... | [['we', 'calculate', 'explicitly', 'solutions', 'to', 'the', 'dirichlet', 'and', 'neumann', 'boundary', 'value', 'problems', 'in', 'the', 'upper', 'half', 'plane', 'for', 'a', 'family', 'of', 'divergence', 'form', 'equations', 'with', 'non', 'symmetric', 'coefficients', 'with', 'a', 'jump', 'discontinuity', 'it', 'is',... | [-0.14856853834708553, 0.06253797031339195, -0.09768805082224435, 0.045408940284070956, -0.12959834289247707, -0.1772120877689982, -0.03419052174914691, 0.2947063627060882, -0.26852996498188475, -0.21191089391960935, 0.19360203586195168, -0.3244601611237405, -0.13426021353925688, 0.19996795369217457, 0.0093334545460292... |
709.2256 | Confinement-induced enhancement of diffusiophoretic forces on
self-propellers | We study the effect of spatial confinement on the strength of propulsive
diffusiophoretic forces acting on a particle that generates density gradients
by exploiting the chemical free energy of its environment. Using a recently
proposed simple model of a self-propelling device driven by chemical reactions
taking place... | cond-mat.stat-mech cond-mat.mtrl-sci | we study the effect of spatial confinement on the strength of propulsive diffusiophoretic forces acting on a particle that generates density gradients by exploiting the chemical free energy of its environment using a recently proposed simple model of a selfpropelling device driven by chemical reactions taking place on ... | [['we', 'study', 'the', 'effect', 'of', 'spatial', 'confinement', 'on', 'the', 'strength', 'of', 'propulsive', 'diffusiophoretic', 'forces', 'acting', 'on', 'a', 'particle', 'that', 'generates', 'density', 'gradients', 'by', 'exploiting', 'the', 'chemical', 'free', 'energy', 'of', 'its', 'environment', 'using', 'a', 'r... | [-0.14787995051798894, 0.1865551143625303, -0.1001952522127783, 0.005086659688113517, -0.014535597667003734, -0.08367836111684955, 0.029813216232895096, 0.3880230317576022, -0.243691635589245, -0.28970696612060826, 0.011751906589687437, -0.24178129369746656, -0.19924158178552798, 0.21180772484734042, -0.000771048752873... |
709.2257 | Uber das Gravitationsfeld eines Massenpunktes nach der Einstenschen
Theorie | Schwarzschild's solution of Einstein's field equations in vacuum can be
written in many different forms. Unfortunately Schwarzschild's own original
form is less nice looking and simple than that latter derived by Droste and
Hilbert. We prove here that we can have both: a nice looking simple form and
the meaning that ... | gr-qc physics.hist-ph | schwarzschilds solution of einsteins field equations in vacuum can be written in many different forms unfortunately schwarzschilds own original form is less nice looking and simple than that latter derived by droste and hilbert we prove here that we can have both a nice looking simple form and the meaning that schwarzs... | [['schwarzschilds', 'solution', 'of', 'einsteins', 'field', 'equations', 'in', 'vacuum', 'can', 'be', 'written', 'in', 'many', 'different', 'forms', 'unfortunately', 'schwarzschilds', 'own', 'original', 'form', 'is', 'less', 'nice', 'looking', 'and', 'simple', 'than', 'that', 'latter', 'derived', 'by', 'droste', 'and',... | [-0.12018107191792556, 0.05632685590535402, -0.16359730901728783, 0.10651607374727194, -0.15626018519646356, -0.17024356330345783, -0.039023699079241074, 0.2996581600180694, -0.2209200675466231, -0.2600635929565345, 0.08576501707346844, -0.23930898210299867, -0.15398768931627274, 0.19195594499220273, -0.098824949767107... |
709.2258 | Quantum memory for squeezed light | We produce a 600-ns pulse of 1.86-dB squeezed vacuum at 795 nm in an optical
parametric amplifier and store it in a rubidium vapor cell for 1 us using
electromagnetically induced transparency. The recovered pulse, analyzed using
time-domain homodyne tomography, exhibits up to 0.21+-0.04 dB of squeezing. We
identify t... | quant-ph | we produce a 600ns pulse of 186db squeezed vacuum at 795 nm in an optical parametric amplifier and store it in a rubidium vapor cell for 1 us using electromagnetically induced transparency the recovered pulse analyzed using timedomain homodyne tomography exhibits up to 021004 db of squeezing we identify the factors lea... | [['we', 'produce', 'a', '600ns', 'pulse', 'of', '186db', 'squeezed', 'vacuum', 'at', '795', 'nm', 'in', 'an', 'optical', 'parametric', 'amplifier', 'and', 'store', 'it', 'in', 'a', 'rubidium', 'vapor', 'cell', 'for', '1', 'us', 'using', 'electromagnetically', 'induced', 'transparency', 'the', 'recovered', 'pulse', 'ana... | [-0.10470885315357116, 0.20319155256648253, -0.05821686581133262, -0.010463935109060806, 0.07495443959145204, -0.12564747364205472, 0.11696393207153853, 0.4847550188081668, -0.25887349423240213, -0.2527973250424325, 0.063527528069886, -0.2498185275026652, -0.024618035634322202, 0.22730419458821416, -0.0422782583764809,... |
709.2259 | Charmonium Polarization in High Energy Collisions | We consider charmonium polarization at high-energy hadron collider Tevatron
in the framework of the nonrelativistic QCD (NRQCD) and the k_T-factorization
approach. The polarization effects are studied for the direct and the prompt
production channels. The obtained predictions can be used to test the Regge
limit of QC... | hep-ph | we consider charmonium polarization at highenergy hadron collider tevatron in the framework of the nonrelativistic qcd nrqcd and the k_tfactorization approach the polarization effects are studied for the direct and the prompt production channels the obtained predictions can be used to test the regge limit of qcd and th... | [['we', 'consider', 'charmonium', 'polarization', 'at', 'highenergy', 'hadron', 'collider', 'tevatron', 'in', 'the', 'framework', 'of', 'the', 'nonrelativistic', 'qcd', 'nrqcd', 'and', 'the', 'k_tfactorization', 'approach', 'the', 'polarization', 'effects', 'are', 'studied', 'for', 'the', 'direct', 'and', 'the', 'promp... | [-0.009662711221323, 0.20377074753609942, -0.19709746129628197, 0.1777314062632036, -0.011012990721592716, -0.08710766309762702, 0.02036105844137423, 0.3566900273675428, -0.178343293202274, -0.16330447391259903, -0.06629504996817559, -0.32699700846683744, 0.09015984863371533, 0.1070973819815645, 0.11556211828856784, 0.... |
709.226 | OVII and OVIII line emission in the diffuse soft X-ray background:
heliospheric and galactic contributions | We study the 0.57 keV (O VII triplet) and 0.65 keV (O VIII) diffuse emission
generated by charge transfer collisions between solar wind (SW) oxygen ions and
interstellar H and He neutral atoms in the inner Heliosphere. These lines which
dominate the 0.3-1.0 keV energy interval are also produced by hot gas in the
gala... | astro-ph | we study the 057 kev o vii triplet and 065 kev o viii diffuse emission generated by charge transfer collisions between solar wind sw oxygen ions and interstellar h and he neutral atoms in the inner heliosphere these lines which dominate the 0310 kev energy interval are also produced by hot gas in the galactic halo gh a... | [['we', 'study', 'the', '057', 'kev', 'o', 'vii', 'triplet', 'and', '065', 'kev', 'o', 'viii', 'diffuse', 'emission', 'generated', 'by', 'charge', 'transfer', 'collisions', 'between', 'solar', 'wind', 'sw', 'oxygen', 'ions', 'and', 'interstellar', 'h', 'and', 'he', 'neutral', 'atoms', 'in', 'the', 'inner', 'heliosphere... | [-0.0047984897037905115, 0.11761727056583769, 0.007844268684149594, 0.14006459219528045, -0.03134206692826607, -0.09643919291897668, 0.03111512670796868, 0.4912717358486072, -0.21167505612106038, -0.3247376650127138, -0.013428329828883277, -0.34905156752027505, 0.022330982969268352, 0.12713137239339417, 0.0340756903935... |
709.2261 | Parabolic Raynaud bundles | Let X be an irreducible smooth projective curve defined over complex numbers,
S= {p_1, p_2,...,p_n} \subset X$ a finite set of closed points and N > 1 a
fixed integer. For any pair (r,d) in Z X Z/N, there exists a parabolic vector
bundle R_{r,d,*} on X, with parabolic structure over S and all parabolic
weights in Z/N... | math.AG | let x be an irreducible smooth projective curve defined over complex numbers s p_1 p_2p_n subset x a finite set of closed points and n 1 a fixed integer for any pair rd in z x zn there exists a parabolic vector bundle r_rd on x with parabolic structure over s and all parabolic weights in zn that has the following prope... | [['let', 'x', 'be', 'an', 'irreducible', 'smooth', 'projective', 'curve', 'defined', 'over', 'complex', 'numbers', 's', 'p_1', 'p_2p_n', 'subset', 'x', 'a', 'finite', 'set', 'of', 'closed', 'points', 'and', 'n', '1', 'a', 'fixed', 'integer', 'for', 'any', 'pair', 'rd', 'in', 'z', 'x', 'zn', 'there', 'exists', 'a', 'par... | [-0.218998240956336, 0.12556637566733717, -0.0026475359267051067, -0.04665932373823, -0.06413149114253872, -0.2485885685950586, 0.019435721514703824, 0.40369727530884086, -0.3574377462062814, -0.0901300827417215, 0.042759739845102535, -0.31560385061231433, -0.05016259429762738, 0.18664200310894383, -0.08118015059500659... |
709.2262 | Plasmons, plasminos and Landau damping in a quasiparticle model of the
quark-gluon plasma | A phenomenological quasiparticle model is surveyed for 2+1 quark flavors and
compared with recent lattice QCD results. Emphasis is devoted to the effects of
plasmons, plasminos and Landau damping. It is shown that thermodynamic bulk
quantities, known at zero chemical potential, can uniquely be mapped towards
nonzero ... | hep-ph | a phenomenological quasiparticle model is surveyed for 21 quark flavors and compared with recent lattice qcd results emphasis is devoted to the effects of plasmons plasminos and landau damping it is shown that thermodynamic bulk quantities known at zero chemical potential can uniquely be mapped towards nonzero chemical... | [['a', 'phenomenological', 'quasiparticle', 'model', 'is', 'surveyed', 'for', '21', 'quark', 'flavors', 'and', 'compared', 'with', 'recent', 'lattice', 'qcd', 'results', 'emphasis', 'is', 'devoted', 'to', 'the', 'effects', 'of', 'plasmons', 'plasminos', 'and', 'landau', 'damping', 'it', 'is', 'shown', 'that', 'thermody... | [-0.11659810638957424, 0.2135909097502008, -0.12245916516985744, 0.06743470782530495, -0.06041540078197916, -0.14680431361775845, 0.10160137919398646, 0.3209321714937687, -0.18077688847358028, -0.23417844528642792, 0.04708331929383955, -0.2955063248984516, -0.10111847866792231, 0.11620481006102637, 0.02270080745326292,... |
709.2263 | Unconventional proximity effects and pairing symmetries in cuprates
caused by conventional phonons | Giant and nil proximity effects and unconventional symmetry of cuprate
superconductors are explained as a result of the strong Froehlich interaction
of holes with c-axis polarised optical phonons acting together with an
anisotropic nonlocal deformation potential.
| cond-mat.supr-con cond-mat.str-el | giant and nil proximity effects and unconventional symmetry of cuprate superconductors are explained as a result of the strong froehlich interaction of holes with caxis polarised optical phonons acting together with an anisotropic nonlocal deformation potential | [['giant', 'and', 'nil', 'proximity', 'effects', 'and', 'unconventional', 'symmetry', 'of', 'cuprate', 'superconductors', 'are', 'explained', 'as', 'a', 'result', 'of', 'the', 'strong', 'froehlich', 'interaction', 'of', 'holes', 'with', 'caxis', 'polarised', 'optical', 'phonons', 'acting', 'together', 'with', 'an', 'an... | [-0.23145379684865475, 0.2315365054241233, -0.023787556565366685, 0.056608371953997344, -0.1462978600627846, -0.1941126683442336, 0.015251056032462252, 0.41005367288986844, -0.24074822860873407, -0.2367544275087615, -0.06595679122902867, -0.3743054423895147, -0.11614020049778952, 0.18232414425195506, 0.0439873993551979... |
709.2264 | Looking for signals of New Physics in the Top quark samples with the CDF
detector | Twelve years after the discovery of the Top quark, the CDF detector has
collected large samples of tt-bar events with integrated luminosities up to
1-1.7 fb^-1, where we are able to probe our knowledge of the Standard Model Top
quark. This article will focuss on those analysis results dedicated to find new
physics in... | hep-ex | twelve years after the discovery of the top quark the cdf detector has collected large samples of ttbar events with integrated luminosities up to 117 fb1 where we are able to probe our knowledge of the standard model top quark this article will focuss on those analysis results dedicated to find new physics in the top q... | [['twelve', 'years', 'after', 'the', 'discovery', 'of', 'the', 'top', 'quark', 'the', 'cdf', 'detector', 'has', 'collected', 'large', 'samples', 'of', 'ttbar', 'events', 'with', 'integrated', 'luminosities', 'up', 'to', '117', 'fb1', 'where', 'we', 'are', 'able', 'to', 'probe', 'our', 'knowledge', 'of', 'the', 'standar... | [-0.006194344257657119, 0.2684359065563692, -0.04772304364822197, 0.12448270636971812, -0.06314118573803226, -0.14734374832513988, 0.11099197655729316, 0.26015492707338866, -0.21121506836284332, -0.34095382582725714, 0.012128519280781958, -0.3534598760306835, 0.07881138251688914, 0.1521029870127182, 0.10369987063249256... |
709.2265 | Discovery of very high-energy gamma-ray emission from the LBL object BL
Lacertae | The low-frequency peaked BL Lac (LBL) object BL Lacertae was observed with
the MAGIC telescope from 2005 August to December (22.2 hr), and from 2006 July
to September (26.0 hr). A very high energy (VHE) gamma-ray signal was
discovered with a 5.1 sigma excess in the 2005 data. Above 200 GeV, an integral
flux of (0.6+-... | astro-ph | the lowfrequency peaked bl lac lbl object bl lacertae was observed with the magic telescope from 2005 august to december 222 hr and from 2006 july to september 260 hr a very high energy vhe gammaray signal was discovered with a 51 sigma excess in the 2005 data above 200 gev an integral flux of 0602x10e11 m2 s1 was meas... | [['the', 'lowfrequency', 'peaked', 'bl', 'lac', 'lbl', 'object', 'bl', 'lacertae', 'was', 'observed', 'with', 'the', 'magic', 'telescope', 'from', '2005', 'august', 'to', 'december', '222', 'hr', 'and', 'from', '2006', 'july', 'to', 'september', '260', 'hr', 'a', 'very', 'high', 'energy', 'vhe', 'gammaray', 'signal', '... | [-0.04200713354463241, 0.14154855815008574, -0.07486888578246909, 0.12135089921253157, -0.10040977955191531, -0.12455241315472046, 0.05053254078277422, 0.4482324576673617, -0.1379339530749001, -0.4827635796413622, 0.057325002541836666, -0.33023845638283567, -0.015601496197965765, 0.23345070040983837, -0.101780111279395... |
709.2266 | Lorentz transformation directly from the invariance of the speed of
light via the addition law of parallel speeds | We show that starting with the addition law of parallel speeds derived as a
consequence of the invariance of the speed of light, the Lorentz
transformations for the space-time coordinates can be derived.
| physics.gen-ph | we show that starting with the addition law of parallel speeds derived as a consequence of the invariance of the speed of light the lorentz transformations for the spacetime coordinates can be derived | [['we', 'show', 'that', 'starting', 'with', 'the', 'addition', 'law', 'of', 'parallel', 'speeds', 'derived', 'as', 'a', 'consequence', 'of', 'the', 'invariance', 'of', 'the', 'speed', 'of', 'light', 'the', 'lorentz', 'transformations', 'for', 'the', 'spacetime', 'coordinates', 'can', 'be', 'derived']] | [-0.15567853207220184, 0.1568805490422881, -0.1241970465828975, 0.015867286164200668, -0.048839686777104034, -0.08188779899060275, 0.02025665311763684, 0.3374058043189121, -0.30744115599064215, -0.29196655784140935, 0.08527463708411563, -0.18166853532646643, -0.11942833633811185, 0.23579169212925163, -0.034969694771324... |
709.2267 | Interpretation of neutrino oscillations based on new physics in the
infrared | An interpretation of neutrino oscillations based on a modification of
relativistic quantum field theory at low energies, without the need to
introduce a neutrino mass, is seen to be compatible with all observations.
| hep-ph hep-th | an interpretation of neutrino oscillations based on a modification of relativistic quantum field theory at low energies without the need to introduce a neutrino mass is seen to be compatible with all observations | [['an', 'interpretation', 'of', 'neutrino', 'oscillations', 'based', 'on', 'a', 'modification', 'of', 'relativistic', 'quantum', 'field', 'theory', 'at', 'low', 'energies', 'without', 'the', 'need', 'to', 'introduce', 'a', 'neutrino', 'mass', 'is', 'seen', 'to', 'be', 'compatible', 'with', 'all', 'observations']] | [-0.09349959373304789, 0.22557844593106754, -0.08404186137980132, 0.12853693481266612, -0.10489975347070757, -0.12976394150631898, 0.007123883591372181, 0.3492107694460587, -0.1835203844574139, -0.33775104198491934, 0.0362258582009059, -0.2296311039421143, -0.0361893494528803, 0.2387420493601398, -0.015907259996641766,... |
709.2268 | Twisting Flux Tubes as a cause of Micro-Flaring Activity | High-cadence optical observations of an H-alpha blue-wing bright point near
solar AR NOAA 10794 are presented. The data were obtained with the Dunn Solar
Telescope at the National Solar Observatory/Sacramento Peak using a newly
developed camera system, the Rapid Dual Imager. Wavelet analysis is undertaken
to search f... | astro-ph | highcadence optical observations of an halpha bluewing bright point near solar ar noaa 10794 are presented the data were obtained with the dunn solar telescope at the national solar observatorysacramento peak using a newly developed camera system the rapid dual imager wavelet analysis is undertaken to search for intens... | [['highcadence', 'optical', 'observations', 'of', 'an', 'halpha', 'bluewing', 'bright', 'point', 'near', 'solar', 'ar', 'noaa', '10794', 'are', 'presented', 'the', 'data', 'were', 'obtained', 'with', 'the', 'dunn', 'solar', 'telescope', 'at', 'the', 'national', 'solar', 'observatorysacramento', 'peak', 'using', 'a', 'n... | [-0.12887978628777355, 0.20713537334997068, -0.01506981655669318, 0.07487464668646301, -0.0635161419971076, -0.10941591752531725, 0.04765969417314595, 0.4006721913909877, -0.18147145005724005, -0.3991379101034694, 0.0826554973307249, -0.3171922281589799, -0.06380298468980967, 0.2322029368255258, -0.008548641449145746, ... |
709.2269 | A Comparison of Mixed-Higgs Scenarios In the NMSSM and the MSSM | We study scenarios in the minimal and next-to minimal supersymmetric models
in which the lightest CP-even Higgs boson can have mass below the 114 GeV
standard model LEP limit by virtue of reduced ZZ coupling due to substantial
mixing among the Higgs bosons. We pay particular attention to the size of
corrections from ... | hep-ph | we study scenarios in the minimal and nextto minimal supersymmetric models in which the lightest cpeven higgs boson can have mass below the 114 gev standard model lep limit by virtue of reduced zz coupling due to substantial mixing among the higgs bosons we pay particular attention to the size of corrections from super... | [['we', 'study', 'scenarios', 'in', 'the', 'minimal', 'and', 'nextto', 'minimal', 'supersymmetric', 'models', 'in', 'which', 'the', 'lightest', 'cpeven', 'higgs', 'boson', 'can', 'have', 'mass', 'below', 'the', '114', 'gev', 'standard', 'model', 'lep', 'limit', 'by', 'virtue', 'of', 'reduced', 'zz', 'coupling', 'due', ... | [-0.06440303947815633, 0.2815214531867394, 0.004555053500966592, 0.1828777500154724, -0.07383821221472292, -0.19538770197122196, 0.06071382930658601, 0.31755369494936164, -0.22850994456728752, -0.3399609710786726, 0.05539372076290184, -0.2537100375076378, 0.01575218861714214, 0.10245195921295537, -0.01534153494541859, ... |
709.227 | Overview of the parametric representation of renormalizable
non-commutative field theory | We review here the parametric representation of Feynman amplitudes of
renormalizable non-commutative quantum field models.
| hep-th | we review here the parametric representation of feynman amplitudes of renormalizable noncommutative quantum field models | [['we', 'review', 'here', 'the', 'parametric', 'representation', 'of', 'feynman', 'amplitudes', 'of', 'renormalizable', 'noncommutative', 'quantum', 'field', 'models']] | [-0.1402367278933525, 0.27238067084302503, -0.13078802054127056, 0.14578142451743284, -0.14076634248097739, -0.12043480314314366, 0.018720528157427908, 0.3505398042500019, -0.19635596026976904, -0.16860297669967014, -0.0545422103566428, -0.18039091527462006, -0.2775216944515705, 0.16821064266065758, -0.0633688019899030... |
709.2271 | First-principles Study of Physisorption of Nucleic Acid Bases on
Small-Diameter Carbon Nanotube | We report the results of our first-principles study based on density
functional theory on the interaction of the nucleic acid base molecules adenine
(A), cytosine (C), guanine (G), thymine (T), and uracil (U), with a
single-walled carbon nanotube (CNT). Specifically, the focus is on the
physisorption of base molecule... | cond-mat.soft cond-mat.mtrl-sci | we report the results of our firstprinciples study based on density functional theory on the interaction of the nucleic acid base molecules adenine a cytosine c guanine g thymine t and uracil u with a singlewalled carbon nanotube cnt specifically the focus is on the physisorption of base molecules on the outer wall of ... | [['we', 'report', 'the', 'results', 'of', 'our', 'firstprinciples', 'study', 'based', 'on', 'density', 'functional', 'theory', 'on', 'the', 'interaction', 'of', 'the', 'nucleic', 'acid', 'base', 'molecules', 'adenine', 'a', 'cytosine', 'c', 'guanine', 'g', 'thymine', 't', 'and', 'uracil', 'u', 'with', 'a', 'singlewalle... | [-0.16294467948569819, 0.14777092462555766, -0.005447965135714896, -0.02194916618112796, 0.015313651339129555, -0.14404836588207331, 0.07594103083662132, 0.4195377982660443, -0.25012842034011135, -0.27569821481753526, -0.04704661606396174, -0.27754473460688667, -0.11806819411784132, 0.11086907010959011, 0.0322910420912... |
709.2272 | Note on distortion and Bourgain $\ell_1$ index | The relation between different notions measuring proximity to $\ell_1$ and
distortability of a Banach space is studied. The main result states that a
Banach space, whose all subspaces have Bourgain $\ell_1$ index greater than
$\omega^\alpha$, $\alpha<\omega_1$, contains either an arbitrary distortable
subspace or an ... | math.FA | the relation between different notions measuring proximity to ell_1 and distortability of a banach space is studied the main result states that a banach space whose all subspaces have bourgain ell_1 index greater than omegaalpha alphaomega_1 contains either an arbitrary distortable subspace or an ell_1alphaasymptotic s... | [['the', 'relation', 'between', 'different', 'notions', 'measuring', 'proximity', 'to', 'ell_1', 'and', 'distortability', 'of', 'a', 'banach', 'space', 'is', 'studied', 'the', 'main', 'result', 'states', 'that', 'a', 'banach', 'space', 'whose', 'all', 'subspaces', 'have', 'bourgain', 'ell_1', 'index', 'greater', 'than'... | [-0.1320259617208395, 0.16603673796296706, -0.0605080229944961, 0.11872118637019899, -0.05671182111295503, -0.14702591137570697, -0.02112956472596717, 0.3930968384063521, -0.34035833526489345, -0.15652623057885226, 0.11270032378000229, -0.3396780220575111, -0.09121587796158395, 0.155707546612681, -0.1307151868592861, -... |
709.2273 | Multi-component strongly attractive Fermi gas: a color superconductor in
a one-dimensional harmonic trap | Recent advances in ultra-cold atomic Fermi gases make it possible to achieve
a fermionic superfluid with multiple spin components. In this context, any
mean-field description is expected to fail, owing to the presence of tightly
bound clusters or molecules that consist of more than two particles. Here we
present a de... | cond-mat.supr-con cond-mat.stat-mech | recent advances in ultracold atomic fermi gases make it possible to achieve a fermionic superfluid with multiple spin components in this context any meanfield description is expected to fail owing to the presence of tightly bound clusters or molecules that consist of more than two particles here we present a detailed s... | [['recent', 'advances', 'in', 'ultracold', 'atomic', 'fermi', 'gases', 'make', 'it', 'possible', 'to', 'achieve', 'a', 'fermionic', 'superfluid', 'with', 'multiple', 'spin', 'components', 'in', 'this', 'context', 'any', 'meanfield', 'description', 'is', 'expected', 'to', 'fail', 'owing', 'to', 'the', 'presence', 'of', ... | [-0.12615058182301112, 0.21688261661217098, -0.09452039849978075, 0.06289256627374071, -0.010695250791845372, -0.12854934505927545, 0.06321702939486243, 0.3468971626877964, -0.19201375544351718, -0.2697120574471283, 0.012197352447182345, -0.29615639908665636, -0.08048335941163375, 0.14995902750068849, 0.057335242566635... |
709.2274 | Quadrupolar Order and Structural Phase Transition in DyB4 with
Geometrical Frustration | Structural phase transition accompanying with quadrupolar ordering in DyB4
with Shastry-Sutherland type geometrical frustration has been studied by X-ray
diffraction. Previous study [D. Okuyama et al.: J. Phys. Soc. Jpn. 74 (2005)
2434.] using resonant X-ray scattering revealed short-range ordering of the
Ozx-type qu... | cond-mat.str-el | structural phase transition accompanying with quadrupolar ordering in dyb4 with shastrysutherland type geometrical frustration has been studied by xray diffraction previous study d okuyama et al j phys soc jpn 74 2005 2434 using resonant xray scattering revealed shortrange ordering of the ozxtype quadrupolar moments an... | [['structural', 'phase', 'transition', 'accompanying', 'with', 'quadrupolar', 'ordering', 'in', 'dyb4', 'with', 'shastrysutherland', 'type', 'geometrical', 'frustration', 'has', 'been', 'studied', 'by', 'xray', 'diffraction', 'previous', 'study', 'd', 'okuyama', 'et', 'al', 'j', 'phys', 'soc', 'jpn', '74', '2005', '243... | [-0.2182108937336724, 0.22886876134173006, 0.008167580242969038, -0.0531605376091302, -0.10318728714690421, -0.09041211336793363, 0.07914402035368216, 0.40886039546033903, -0.2594823921099305, -0.2960770368980345, -0.024111955027752954, -0.3373764938451061, -0.07857746500233116, 0.06722858278513995, 0.1207645117195121,... |
709.2275 | SPINSTARS at low metallicities | The main effect of axial rotation on the evolution of massive PopIII stars is
to trigger internal mixing processes which allow stars to produce significant
amounts of primary nitrogen 14 and carbon 13. Very metal poor massive stars
produce much more primary nitrogen than PopIII stars for a given initial mass
and rota... | astro-ph | the main effect of axial rotation on the evolution of massive popiii stars is to trigger internal mixing processes which allow stars to produce significant amounts of primary nitrogen 14 and carbon 13 very metal poor massive stars produce much more primary nitrogen than popiii stars for a given initial mass and rotatio... | [['the', 'main', 'effect', 'of', 'axial', 'rotation', 'on', 'the', 'evolution', 'of', 'massive', 'popiii', 'stars', 'is', 'to', 'trigger', 'internal', 'mixing', 'processes', 'which', 'allow', 'stars', 'to', 'produce', 'significant', 'amounts', 'of', 'primary', 'nitrogen', '14', 'and', 'carbon', '13', 'very', 'metal', '... | [-0.1079722713549053, 0.2605159571112735, 0.010014032076205655, 0.11572286970530399, -0.05266327355097318, -0.10064236240187313, 0.05463860044860608, 0.3794561368997866, -0.19619459705628875, -0.37209626093297166, 0.043003121419160656, -0.26230497021244203, 0.02953105099454877, 0.20862723328777916, -0.02039936906456528... |
709.2276 | Exact results of the quantum phase transition for the topological order | In this paper a duality between the d=2 Wen-plaquette model in a transverse
field and the d=1 Ising model in a transverse field is used to learn the nature
of the quantum phase transition (QPT) between a spin-polarized phase and a
topological ordered state with the string-net condensation. The QPT is not
induced by s... | quant-ph | in this paper a duality between the d2 wenplaquette model in a transverse field and the d1 ising model in a transverse field is used to learn the nature of the quantum phase transition qpt between a spinpolarized phase and a topological ordered state with the stringnet condensation the qpt is not induced by spontaneous... | [['in', 'this', 'paper', 'a', 'duality', 'between', 'the', 'd2', 'wenplaquette', 'model', 'in', 'a', 'transverse', 'field', 'and', 'the', 'd1', 'ising', 'model', 'in', 'a', 'transverse', 'field', 'is', 'used', 'to', 'learn', 'the', 'nature', 'of', 'the', 'quantum', 'phase', 'transition', 'qpt', 'between', 'a', 'spinpol... | [-0.17198282194898484, 0.2532172209702115, -0.058376461703409536, 0.09246716882657022, -0.056795165487664175, -0.16482050486523261, 0.040761888461890924, 0.3640109569309874, -0.2451093084119419, -0.23442236575833025, 0.034468378643802505, -0.24321800238016913, -0.15730781111608635, 0.06876785043092008, 0.02242097154165... |
709.2277 | Nilpotent symmetry invariance in the non-Abelian 1-form gauge theory:
superfield formalism | We demonstrate that the nilpotent Becchi-Rouet-Stora-Tyutin (BRST) and
anti-BRST symmetry invariance of the Lagrangian density of a four (3 +
1)-dimensional (4D) non-Abelian 1-form gauge theory with Dirac fields can be
captured within the framework of the superfield approach to BRST formalism. The
above 4D theory, wh... | hep-th | we demonstrate that the nilpotent becchirouetstoratyutin brst and antibrst symmetry invariance of the lagrangian density of a four 3 1dimensional 4d nonabelian 1form gauge theory with dirac fields can be captured within the framework of the superfield approach to brst formalism the above 4d theory where there is an exp... | [['we', 'demonstrate', 'that', 'the', 'nilpotent', 'becchirouetstoratyutin', 'brst', 'and', 'antibrst', 'symmetry', 'invariance', 'of', 'the', 'lagrangian', 'density', 'of', 'a', 'four', '3', '1dimensional', '4d', 'nonabelian', '1form', 'gauge', 'theory', 'with', 'dirac', 'fields', 'can', 'be', 'captured', 'within', 't... | [-0.19151163755932116, 0.2045743765565617, -0.06464496604166925, 0.07705020940970983, -0.09357234321590834, -0.11809741993081467, -0.06430182187739711, 0.30894881517401546, -0.19967667357208296, -0.2748905273840827, -0.012179319760842442, -0.2127541683590168, -0.22269783230048829, 0.015780621991043204, -0.0927635830975... |
709.2278 | Observation of Goos-H\"{a}nchen shifts in metallic reflection | We report the first observation of the Goos-H$\rm \ddot{\textbf{a}}$nchen
shift of a light beam incident on a metal surface. This phenomenon is
particularly interesting because the Goos-H$\rm \ddot{\textbf{a}}$nchen shift
for $p$ polarized light in metals is negative and much bigger than the positive
shift for $s$ po... | physics.optics | we report the first observation of the gooshrm ddottextbfanchen shift of a light beam incident on a metal surface this phenomenon is particularly interesting because the gooshrm ddottextbfanchen shift for p polarized light in metals is negative and much bigger than the positive shift for s polarized light the experimen... | [['we', 'report', 'the', 'first', 'observation', 'of', 'the', 'gooshrm', 'ddottextbfanchen', 'shift', 'of', 'a', 'light', 'beam', 'incident', 'on', 'a', 'metal', 'surface', 'this', 'phenomenon', 'is', 'particularly', 'interesting', 'because', 'the', 'gooshrm', 'ddottextbfanchen', 'shift', 'for', 'p', 'polarized', 'ligh... | [-0.12410441563198608, 0.19862501707289734, -0.11870910923890009, 0.058040794078973404, -0.03134974671945888, -0.12880186632522667, 0.07425836925109734, 0.4077670671692004, -0.23375234104768963, -0.2947637709237787, 0.011860823673338686, -0.32829809552343675, -0.08319920054589379, 0.2448923278514448, 0.0043803928800079... |
709.2279 | New symmetric families of silicon quantum dots and their conglomerates
as a tunable source of photoluminescence in nanodevices | We propose a new variety of silicon quantum dots containing fullerene-derived
hollows of nearly arbitrary symmetry. Conglomerate structures are designed by
connecting the quantum dots through two kinds of junctions. The quantum
confinement effect is investigated using semiempirical quantum-mechanical
method. It is sh... | cond-mat.mtrl-sci | we propose a new variety of silicon quantum dots containing fullerenederived hollows of nearly arbitrary symmetry conglomerate structures are designed by connecting the quantum dots through two kinds of junctions the quantum confinement effect is investigated using semiempirical quantummechanical method it is shown tha... | [['we', 'propose', 'a', 'new', 'variety', 'of', 'silicon', 'quantum', 'dots', 'containing', 'fullerenederived', 'hollows', 'of', 'nearly', 'arbitrary', 'symmetry', 'conglomerate', 'structures', 'are', 'designed', 'by', 'connecting', 'the', 'quantum', 'dots', 'through', 'two', 'kinds', 'of', 'junctions', 'the', 'quantum... | [-0.12139139836754426, 0.20853265006083127, -0.02409197537003663, 0.0038603462217624523, -0.016572459771474504, -0.20004707842950853, 0.01652622830467941, 0.42439880928602713, -0.2833648523524532, -0.30631727233914463, -0.011321397968929196, -0.30840193847965064, -0.13651688615109064, 0.1745623184562709, 0.008369212799... |
709.228 | Raman-induced limits to efficient squeezing in optical fibers | We report new experiments on polarization squeezing using ultrashort photonic
pulses in a single pass of a birefringent fiber. We measure what is to our
knowledge a record squeezing of -6.8 +/- 0.3 dB in optical fibers which when
corrected for linear losses is -10.4 +/- 0.8 dB. The measured polarization
squeezing as ... | quant-ph | we report new experiments on polarization squeezing using ultrashort photonic pulses in a single pass of a birefringent fiber we measure what is to our knowledge a record squeezing of 68 03 db in optical fibers which when corrected for linear losses is 104 08 db the measured polarization squeezing as a function of opti... | [['we', 'report', 'new', 'experiments', 'on', 'polarization', 'squeezing', 'using', 'ultrashort', 'photonic', 'pulses', 'in', 'a', 'single', 'pass', 'of', 'a', 'birefringent', 'fiber', 'we', 'measure', 'what', 'is', 'to', 'our', 'knowledge', 'a', 'record', 'squeezing', 'of', '68', '03', 'db', 'in', 'optical', 'fibers',... | [-0.10655439996279459, 0.16282710297270975, -0.07300298607492066, 0.016003500365533253, 0.014328415337157376, -0.13377045514062047, 0.10610719827409992, 0.4551228873439113, -0.23388099539628687, -0.3131477104579198, 0.039689971250481904, -0.28018600956853873, -0.05922163059895343, 0.29407555601024565, -0.03167272884611... |
709.2281 | Groupoid and Inverse Semigroup Presentations of Ultragraph
$C^{*}$-Algebras | Inspired by the work of Paterson on $C^{\ast}$-algebras of directed graphs,
we show how to associate a groupoid $\mathfrak{G}_{\mathcal{G}}$ to an
ultragraph $\mathcal{G}$ in such a way that the $C^*$-algebra of
$\mathfrak{G}_{\mathcal{G}}$ is canonically isomorphic to Tomforde's
$C^*$-algebra $C^*(\mathcal{G})$. The... | math.OA math.DS | inspired by the work of paterson on castalgebras of directed graphs we show how to associate a groupoid mathfrakg_mathcalg to an ultragraph mathcalg in such a way that the calgebra of mathfrakg_mathcalg is canonically isomorphic to tomfordes calgebra cmathcalg the groupoid mathfrakg_mathcalg is built from an inverse se... | [['inspired', 'by', 'the', 'work', 'of', 'paterson', 'on', 'castalgebras', 'of', 'directed', 'graphs', 'we', 'show', 'how', 'to', 'associate', 'a', 'groupoid', 'mathfrakg_mathcalg', 'to', 'an', 'ultragraph', 'mathcalg', 'in', 'such', 'a', 'way', 'that', 'the', 'calgebra', 'of', 'mathfrakg_mathcalg', 'is', 'canonically'... | [-0.10261045951469272, 0.11330257455291062, -0.1114213083158521, 0.041943582122935454, -0.1875942535150577, -0.07979787931795798, -0.035488422594818415, 0.4166597538289851, -0.4730329894752917, -0.17946265385184876, 0.05963000451333309, -0.28636251645637495, -0.15922271825519263, 0.18275113523864717, -0.257370630744844... |
709.2282 | Carleman estimates and inverse problems for Dirac operators | We consider limiting Carleman weights for Dirac operators and prove
corresponding Carleman estimates. In particular, we show that limiting Carleman
weights for the Laplacian also serve as limiting weights for Dirac operators.
As an application we consider the inverse problem of recovering a Lipschitz
continuous magne... | math.AP math-ph math.MP | we consider limiting carleman weights for dirac operators and prove corresponding carleman estimates in particular we show that limiting carleman weights for the laplacian also serve as limiting weights for dirac operators as an application we consider the inverse problem of recovering a lipschitz continuous magnetic f... | [['we', 'consider', 'limiting', 'carleman', 'weights', 'for', 'dirac', 'operators', 'and', 'prove', 'corresponding', 'carleman', 'estimates', 'in', 'particular', 'we', 'show', 'that', 'limiting', 'carleman', 'weights', 'for', 'the', 'laplacian', 'also', 'serve', 'as', 'limiting', 'weights', 'for', 'dirac', 'operators',... | [-0.08198557262597926, 0.07525309692322606, 0.006112216337551844, 0.10303601744616854, -0.13163002259258566, -0.15530509110700724, 0.04276079382618953, 0.3802742837318059, -0.29448529185149175, -0.19424087037171783, 0.12942812984993937, -0.3127352361535204, -0.1769291989119916, 0.1941409844840909, -0.043070175460186495... |
709.2283 | Observations of Very High Energy Gamma-Rays during Moonlight and
Twilight with the MAGIC Telescope | We study the capability of the MAGIC telescope to observe under moderate
moonlight. TeV gamma-ray signals from the Crab nebula were detected with the
MAGIC telescope during periods when the Moon was above the horizon and during
twilight. This was accomplished by increasing the trigger discriminator
thresholds. No cha... | astro-ph | we study the capability of the magic telescope to observe under moderate moonlight tev gammaray signals from the crab nebula were detected with the magic telescope during periods when the moon was above the horizon and during twilight this was accomplished by increasing the trigger discriminator thresholds no change is... | [['we', 'study', 'the', 'capability', 'of', 'the', 'magic', 'telescope', 'to', 'observe', 'under', 'moderate', 'moonlight', 'tev', 'gammaray', 'signals', 'from', 'the', 'crab', 'nebula', 'were', 'detected', 'with', 'the', 'magic', 'telescope', 'during', 'periods', 'when', 'the', 'moon', 'was', 'above', 'the', 'horizon'... | [-0.07751461006550779, 0.18007873958076842, -0.014256268464309234, 0.12172116422324732, -0.07191597499323868, -0.1028998491143988, 0.051610589550647845, 0.42241219022581655, -0.1711154745651349, -0.4401542544765498, 0.1438407337691094, -0.2713662599259111, -0.0789220444757932, 0.23189627869875842, -0.09795072351792647,... |
709.2284 | On convergence of generators of equilibrium dynamics of hopping
particles to generator of a birth-and-death process in continuum | We deal with two following classes of equilibrium stochastic dynamics of
infinite particle systems in continuum: hopping particles (also called Kawasaki
dynamics), i.e., a dynamics where each particle randomly hops over the space,
and birth-and-death process in continuum (or Glauber dynamics), i.e., a
dynamics where ... | math.PR | we deal with two following classes of equilibrium stochastic dynamics of infinite particle systems in continuum hopping particles also called kawasaki dynamics ie a dynamics where each particle randomly hops over the space and birthanddeath process in continuum or glauber dynamics ie a dynamics where there is no motion... | [['we', 'deal', 'with', 'two', 'following', 'classes', 'of', 'equilibrium', 'stochastic', 'dynamics', 'of', 'infinite', 'particle', 'systems', 'in', 'continuum', 'hopping', 'particles', 'also', 'called', 'kawasaki', 'dynamics', 'ie', 'a', 'dynamics', 'where', 'each', 'particle', 'randomly', 'hops', 'over', 'the', 'spac... | [-0.11297223363999959, 0.19371180497094673, -0.11990529135953075, 0.08982941122416545, -0.0050408086416865484, -0.1375294448686094, 0.012538083408977472, 0.3388099763907638, -0.2734088082432601, -0.2265637045580851, 0.06376938016102132, -0.2778352623625835, -0.10642995653381827, 0.13745662193057534, -0.0333809614488915... |
709.2285 | Critically rotating stars in binaries - an unsolved problem - | In close binaries mass and angular momentum can be transferred from one star
to the other during Roche-lobe overflow. The efficiency of this process is not
well understood and constitutes one of the largest uncertainties in binary
evolution.
One of the problems lies in the transfer of angular momentum, which will s... | astro-ph | in close binaries mass and angular momentum can be transferred from one star to the other during rochelobe overflow the efficiency of this process is not well understood and constitutes one of the largest uncertainties in binary evolution one of the problems lies in the transfer of angular momentum which will spin up t... | [['in', 'close', 'binaries', 'mass', 'and', 'angular', 'momentum', 'can', 'be', 'transferred', 'from', 'one', 'star', 'to', 'the', 'other', 'during', 'rochelobe', 'overflow', 'the', 'efficiency', 'of', 'this', 'process', 'is', 'not', 'well', 'understood', 'and', 'constitutes', 'one', 'of', 'the', 'largest', 'uncertaint... | [-0.15668123771378306, 0.20325046886937342, -0.06201516434084624, 0.10460595015935724, -0.12272202390362509, -0.08140849741408601, 0.059049275233410296, 0.36757492295466365, -0.23425684142217507, -0.3678016844717786, 0.06982994990365114, -0.2556084083361202, -0.00753624020377174, 0.24437843327206793, -0.085416037717368... |
709.2286 | A Poincar\'e-Birkhoff-Witt criterion for Koszul operads | The aim of this article is to give a criterion, generalizing the criterion
introduced by Priddy for algebras, to verify that an operad is Koszul. We
define the notion of a Poincare-Birkhoff-Witt basis in the context of operads.
Then we show that an operad having a Poincare-Birkhoff-Witt basis is Koszul.
Besides, we o... | math.AT | the aim of this article is to give a criterion generalizing the criterion introduced by priddy for algebras to verify that an operad is koszul we define the notion of a poincarebirkhoffwitt basis in the context of operads then we show that an operad having a poincarebirkhoffwitt basis is koszul besides we obtain that t... | [['the', 'aim', 'of', 'this', 'article', 'is', 'to', 'give', 'a', 'criterion', 'generalizing', 'the', 'criterion', 'introduced', 'by', 'priddy', 'for', 'algebras', 'to', 'verify', 'that', 'an', 'operad', 'is', 'koszul', 'we', 'define', 'the', 'notion', 'of', 'a', 'poincarebirkhoffwitt', 'basis', 'in', 'the', 'context',... | [-0.1565858502459677, -0.0467841045166914, -0.14200032966011028, 0.14972802523016646, -0.18656585087315947, -0.13931894490401012, -0.056569586225042615, 0.3761260064342354, -0.42986803805997853, -0.14032153868929872, 0.12013504148425558, -0.1484232094091705, -0.23758851088394847, 0.14216731479273567, -0.244907138833799... |
709.2287 | Topological complexity of motion planning and Massey products | We employ Massey products to find sharper lower bounds for the Schwarz genus
of a fibration than those previously known. In particular we give examples of
non-formal spaces $X$ for which the topological complexity $\TC(X)$ (defined to
be the genus of the free path fibration on $X$) is greater than the
zero-divisors c... | math.AT math.OC | we employ massey products to find sharper lower bounds for the schwarz genus of a fibration than those previously known in particular we give examples of nonformal spaces x for which the topological complexity tcx defined to be the genus of the free path fibration on x is greater than the zerodivisors cuplength plus on... | [['we', 'employ', 'massey', 'products', 'to', 'find', 'sharper', 'lower', 'bounds', 'for', 'the', 'schwarz', 'genus', 'of', 'a', 'fibration', 'than', 'those', 'previously', 'known', 'in', 'particular', 'we', 'give', 'examples', 'of', 'nonformal', 'spaces', 'x', 'for', 'which', 'the', 'topological', 'complexity', 'tcx',... | [-0.17410915942693297, 0.0683363313363357, -0.0781460009091957, 0.15495233421679586, -0.08765301719646562, -0.14735556103458458, 0.04486458448015831, 0.31867627386342395, -0.2525677407837727, -0.28611057102680204, 0.08865429393904792, -0.2763982191343199, -0.11869970488954674, 0.2678473665632985, -0.18065386104651474, ... |
709.2288 | Observations of microquasars with the MAGIC telescope | We report on the results from the observations in very high energy band (VHE,
E_gamma > 100GeV) of the black hole X-ray binary (BHXB) Cygnus X-1. The
observations were performed with the MAGIC telescope, for a total of 40 hours
during 26 nights, spanning the period between June and November 2006. We report
on the res... | astro-ph | we report on the results from the observations in very high energy band vhe e_gamma 100gev of the black hole xray binary bhxb cygnus x1 the observations were performed with the magic telescope for a total of 40 hours during 26 nights spanning the period between june and november 2006 we report on the results of the sea... | [['we', 'report', 'on', 'the', 'results', 'from', 'the', 'observations', 'in', 'very', 'high', 'energy', 'band', 'vhe', 'e_gamma', '100gev', 'of', 'the', 'black', 'hole', 'xray', 'binary', 'bhxb', 'cygnus', 'x1', 'the', 'observations', 'were', 'performed', 'with', 'the', 'magic', 'telescope', 'for', 'a', 'total', 'of',... | [-0.0815419660997577, 0.15835026263539476, -0.03706976873218082, 0.07835206256713718, -0.06323654612060636, -0.07002996444498422, 0.1356688694213517, 0.45478576675523075, -0.10913572037388804, -0.4759714539395645, 0.128438866075885, -0.3452108723053243, -0.04000785341486335, 0.30020004101097586, 0.011733295824524249, 0... |
709.2289 | Asymptotic valuations of sequences satisfying first order recurrences | Let t[n] be a sequence that satisfies a first order homogeneous recurrence
t[n] = Q[n]*t[n-1], where Q is a polynomial with integer coefficients. The
asymptotic behavior of the p-adic valuation of t[n] is described under the
assumption that all the roots of Q in Z/pZ have nonvanishing derivative.
| math.NT | let tn be a sequence that satisfies a first order homogeneous recurrence tn qntn1 where q is a polynomial with integer coefficients the asymptotic behavior of the padic valuation of tn is described under the assumption that all the roots of q in zpz have nonvanishing derivative | [['let', 'tn', 'be', 'a', 'sequence', 'that', 'satisfies', 'a', 'first', 'order', 'homogeneous', 'recurrence', 'tn', 'qntn1', 'where', 'q', 'is', 'a', 'polynomial', 'with', 'integer', 'coefficients', 'the', 'asymptotic', 'behavior', 'of', 'the', 'padic', 'valuation', 'of', 'tn', 'is', 'described', 'under', 'the', 'assu... | [-0.28189107795934315, 0.12311321221615958, -0.146871661936925, -0.03360474710453949, -0.10673646298844529, -0.14215672322872863, -0.02075958713312107, 0.2742415192567379, -0.3028947157866281, -0.1350415262454392, 0.08576021935416224, -0.2895567652809879, -0.13167327411634766, 0.1570580449744897, 0.0018017051498527112,... |
709.229 | Mirror Symmetry via Logarithmic Degeneration Data II | This paper continues the authors' program of studying mirror symmetry via log
geometry and toric degenerations, relating affine manifolds with singularities,
log Calabi-Yau spaces, and toric degenerations of Calabi-Yaus. The main focus
of this paper is the calculation of the cohomology of a Calabi-Yau variety
associa... | math.AG | this paper continues the authors program of studying mirror symmetry via log geometry and toric degenerations relating affine manifolds with singularities log calabiyau spaces and toric degenerations of calabiyaus the main focus of this paper is the calculation of the cohomology of a calabiyau variety associated to a g... | [['this', 'paper', 'continues', 'the', 'authors', 'program', 'of', 'studying', 'mirror', 'symmetry', 'via', 'log', 'geometry', 'and', 'toric', 'degenerations', 'relating', 'affine', 'manifolds', 'with', 'singularities', 'log', 'calabiyau', 'spaces', 'and', 'toric', 'degenerations', 'of', 'calabiyaus', 'the', 'main', 'f... | [-0.21199702968603218, 0.004775571540945252, -0.12245564771114618, 0.12573366302107883, -0.0946518217467449, -0.14325395989679285, -0.02527467942401289, 0.27283986379670633, -0.29989246012606696, -0.25944631084703007, 0.11044615095741321, -0.2100805525649823, -0.19149770110228717, 0.1787856583296043, -0.230064691549360... |
709.2291 | Squark Decays in MSSM Under the Cosmological Bounds | We present the numerical investigation of the fermionic two-body decays of
squarks in the Minimal Supersymmetric Standard Model with complex parameters.
In the analysis we particularly take into account the cosmological bounds
imposed by WMAP data. We find that the phase dependences of the decay widths of
the third f... | hep-ph | we present the numerical investigation of the fermionic twobody decays of squarks in the minimal supersymmetric standard model with complex parameters in the analysis we particularly take into account the cosmological bounds imposed by wmap data we find that the phase dependences of the decay widths of the third family... | [['we', 'present', 'the', 'numerical', 'investigation', 'of', 'the', 'fermionic', 'twobody', 'decays', 'of', 'squarks', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'with', 'complex', 'parameters', 'in', 'the', 'analysis', 'we', 'particularly', 'take', 'into', 'account', 'the', 'cosmological', 'bounds... | [-0.1335924719489124, 0.23019672907649144, -0.04150439489005816, 0.12983078672320092, -0.07200002464198388, -0.174062836564856, 0.06847810479097695, 0.3007082128758994, -0.22068685116154133, -0.28286189912348103, 0.040218845837389924, -0.30713398481885174, -0.019944929941972292, 0.15206889348740846, 0.09890063480464834... |
709.2292 | The Formation of Crystalline Dust in AGB Winds from Binary Induced
Spiral Shocks | As stars evolve along the Asymptotic Giant Branch, strong winds are driven
from the outer envelope. These winds form a shell, which may ultimately become
a planetary nebula. Many planetary nebulae are highly asymmetric, hinting at
the presence of a binary companion. Some post-Asymptotic Giant Branch objects
are surro... | astro-ph | as stars evolve along the asymptotic giant branch strong winds are driven from the outer envelope these winds form a shell which may ultimately become a planetary nebula many planetary nebulae are highly asymmetric hinting at the presence of a binary companion some postasymptotic giant branch objects are surrounded by ... | [['as', 'stars', 'evolve', 'along', 'the', 'asymptotic', 'giant', 'branch', 'strong', 'winds', 'are', 'driven', 'from', 'the', 'outer', 'envelope', 'these', 'winds', 'form', 'a', 'shell', 'which', 'may', 'ultimately', 'become', 'a', 'planetary', 'nebula', 'many', 'planetary', 'nebulae', 'are', 'highly', 'asymmetric', '... | [-0.16093605739353858, 0.17130366249859913, -0.1067078623387203, 0.06191857152469275, -0.11381415426007753, -0.048048309849866765, 0.032891864901932986, 0.40132712865772757, -0.20811213287457064, -0.3027260854876446, 0.07931492949307001, -0.24755726803491995, -0.10241428590876964, 0.18548062101042675, -0.06708562217236... |
709.2293 | Titan's rotational state : The effects of a forced "free" resonant
wobble | In Noyelles et al. (2008, Astron. Astrophys., 478, 959-970), a resonance
involving the wobble of Titan is hinted. This paper studies this scenario and
its consequences. The first step is to build an accurate analytical model that
would help to find the likely resonances in the rotation of every synchronous
body. In t... | astro-ph | in noyelles et al 2008 astron astrophys 478 959970 a resonance involving the wobble of titan is hinted this paper studies this scenario and its consequences the first step is to build an accurate analytical model that would help to find the likely resonances in the rotation of every synchronous body in this model i tak... | [['in', 'noyelles', 'et', 'al', '2008', 'astron', 'astrophys', '478', '959970', 'a', 'resonance', 'involving', 'the', 'wobble', 'of', 'titan', 'is', 'hinted', 'this', 'paper', 'studies', 'this', 'scenario', 'and', 'its', 'consequences', 'the', 'first', 'step', 'is', 'to', 'build', 'an', 'accurate', 'analytical', 'model... | [-0.13041437385037347, 0.13760430526496353, -0.06677534173020343, 0.03742723934610423, -0.07414473919806057, -0.09533806822658863, 0.022308556561935138, 0.32555925376615974, -0.2266894591652524, -0.3243303616731445, 0.10345145848531054, -0.2623665529364501, -0.10945841151119362, 0.18671875550852976, -0.1231696077452194... |
709.2294 | Groupoid Methods in Wavelet Analysis | We describe how the Deaconu-Renault groupoid may be used in the study of
wavelets and fractals.
| math.OA | we describe how the deaconurenault groupoid may be used in the study of wavelets and fractals | [['we', 'describe', 'how', 'the', 'deaconurenault', 'groupoid', 'may', 'be', 'used', 'in', 'the', 'study', 'of', 'wavelets', 'and', 'fractals']] | [-0.0411483891075477, 0.10211432870710269, -0.21557529654819518, 0.1904997155070305, -0.10068433859851211, -0.025063789100386202, -0.05755625176243484, 0.42761700600385666, -0.3341032541356981, -0.16679460497107357, 0.13547577603458194, -0.22612051805481315, -0.2826825464144349, 0.22245362075045705, -0.1783490359084680... |
709.2295 | The strong coupling constant $g_{D^* D \pi}$ and final-state
interactions | In this article, we study the contribution from the final-state interactions
to the strong coupling constant $g_{D^* D \pi}$. We take an assumption that the
momentum transfers in the strong decay $D^{*+} \to D^0 \pi^+$ be large to
validate the operator product expansion in the light-cone QCD sum rules. At
large momen... | hep-ph | in this article we study the contribution from the finalstate interactions to the strong coupling constant g_d d pi we take an assumption that the momentum transfers in the strong decay d to d0 pi be large to validate the operator product expansion in the lightcone qcd sum rules at large momentum transfers the finalsta... | [['in', 'this', 'article', 'we', 'study', 'the', 'contribution', 'from', 'the', 'finalstate', 'interactions', 'to', 'the', 'strong', 'coupling', 'constant', 'g_d', 'd', 'pi', 'we', 'take', 'an', 'assumption', 'that', 'the', 'momentum', 'transfers', 'in', 'the', 'strong', 'decay', 'd', 'to', 'd0', 'pi', 'be', 'large', '... | [-0.1708649878543037, 0.20119256084592, -0.11807032338684119, 0.11573737366785254, -0.07867949886886931, -0.04644305509195399, 0.0240324163781618, 0.33867109122116174, -0.2991202631270263, -0.20370091453417025, -0.054839122166454014, -0.31869912119026284, -0.047455474067090164, 0.04008643393085074, 0.08315075113813379,... |
709.2296 | Solitons and Their Arrays: from Quasi One-Dimensional Conductors to
Stripes | We suggest a short review of literature on various solitonic lattices and
individual solitons in quasi one-dimensional conductors. This information seems
to be quite relevant to topics of stripes and their melted phases
correspondingly. We shall quote also the latest experiments, which access
solitons as elementary e... | cond-mat.str-el | we suggest a short review of literature on various solitonic lattices and individual solitons in quasi onedimensional conductors this information seems to be quite relevant to topics of stripes and their melted phases correspondingly we shall quote also the latest experiments which access solitons as elementary excitat... | [['we', 'suggest', 'a', 'short', 'review', 'of', 'literature', 'on', 'various', 'solitonic', 'lattices', 'and', 'individual', 'solitons', 'in', 'quasi', 'onedimensional', 'conductors', 'this', 'information', 'seems', 'to', 'be', 'quite', 'relevant', 'to', 'topics', 'of', 'stripes', 'and', 'their', 'melted', 'phases', '... | [-0.19175789378479952, 0.19740575642014543, -0.12364243771622165, 0.13347462427336723, -0.09560355723628568, -0.11971182552062803, 0.06025768894469365, 0.40605996172461245, -0.2330326909923719, -0.23023427882128292, 0.06415173171941811, -0.3031704511727892, -0.13893367071804177, 0.1435821858105353, -0.01082149291436912... |
709.2297 | New interactions in the dark sector mediated by dark energy | Cosmological observations have revealed the existence of a dark matter
sector, which is commonly assumed to be made up of one particle species only.
However, this sector might be more complicated than we currently believe: there
might be more than one dark matter species (for example two components of cold
dark matte... | astro-ph | cosmological observations have revealed the existence of a dark matter sector which is commonly assumed to be made up of one particle species only however this sector might be more complicated than we currently believe there might be more than one dark matter species for example two components of cold dark matter or a ... | [['cosmological', 'observations', 'have', 'revealed', 'the', 'existence', 'of', 'a', 'dark', 'matter', 'sector', 'which', 'is', 'commonly', 'assumed', 'to', 'be', 'made', 'up', 'of', 'one', 'particle', 'species', 'only', 'however', 'this', 'sector', 'might', 'be', 'more', 'complicated', 'than', 'we', 'currently', 'beli... | [-0.15170346982279242, 0.2193005522039467, -0.1233401462536762, 0.12037098305460955, -0.07300583292501715, -0.13854115361160357, -0.027040824287500726, 0.3231560193095942, -0.22049499535640268, -0.3792308676495867, 0.039011788778534194, -0.2721969294098188, -0.05680872007484003, 0.12161569817082477, 0.06184822944162777... |
709.2298 | Hypernuclei and in-medium chiral dynamics | A recently introduced relativistic nuclear energy density functional,
constrained by features of low-energy QCD, is extended to describe the
structure of hypernuclei. The density-dependent mean field and the spin-orbit
potential of a $\Lambda$-hyperon in a nucleus, are consistently calculated
using the SU(3) extensio... | nucl-th | a recently introduced relativistic nuclear energy density functional constrained by features of lowenergy qcd is extended to describe the structure of hypernuclei the densitydependent mean field and the spinorbit potential of a lambdahyperon in a nucleus are consistently calculated using the su3 extension of inmedium c... | [['a', 'recently', 'introduced', 'relativistic', 'nuclear', 'energy', 'density', 'functional', 'constrained', 'by', 'features', 'of', 'lowenergy', 'qcd', 'is', 'extended', 'to', 'describe', 'the', 'structure', 'of', 'hypernuclei', 'the', 'densitydependent', 'mean', 'field', 'and', 'the', 'spinorbit', 'potential', 'of',... | [-0.1349625232105609, 0.21326427499036527, -0.09656211671608617, 0.14856016663088667, -0.040992704540258273, -0.10369323644044925, -0.0017251958042834303, 0.31587604839296546, -0.23262017167144222, -0.2685462905355962, -0.06602237290462654, -0.2989802030060673, -0.0945265069776724, 0.05988823745428817, 0.10176822033645... |
709.2299 | Gamma-Rays from Decaying Dark Matter | We study the prospects for detecting gamma-rays from decaying Dark Matter
(DM), focusing in particular on gravitino DM in R-parity breaking vacua. Given
the substantially different angular distribution of the predicted gamma-ray
signal with respect to the case of annihilating DM, and the relatively poor (of
order 0.1... | astro-ph hep-ph | we study the prospects for detecting gammarays from decaying dark matter dm focusing in particular on gravitino dm in rparity breaking vacua given the substantially different angular distribution of the predicted gammaray signal with respect to the case of annihilating dm and the relatively poor of order 01circ angular... | [['we', 'study', 'the', 'prospects', 'for', 'detecting', 'gammarays', 'from', 'decaying', 'dark', 'matter', 'dm', 'focusing', 'in', 'particular', 'on', 'gravitino', 'dm', 'in', 'rparity', 'breaking', 'vacua', 'given', 'the', 'substantially', 'different', 'angular', 'distribution', 'of', 'the', 'predicted', 'gammaray', ... | [-0.0860892531145364, 0.19147570211463608, -0.05373122459836304, 0.21844813365768642, -0.13767966011352836, -0.10637542719766498, 0.002006815834029112, 0.3331475101262331, -0.20520446499064565, -0.4103277533077635, -0.004951764012686908, -0.33616578179970386, 0.042090044056996706, 0.2232799731325358, 0.0335283987298607... |
709.23 | Testing the galaxy cluster mass-observable relations at z = 1 with
XMM-Newton and Chandra observations of XLSSJ022403.9-041328 | We present an analysis of deep XMM-Newton and Chandra observations of the
z=1.05 galaxy cluster XLSSJ022403.9-041328 (hereafter XLSSC 029), detected in
the XMM-Newton large scale structure survey. Density and temperature profiles
of the X-ray emitting gas were used to perform a hydrostatic mass analysis of
the system... | astro-ph | we present an analysis of deep xmmnewton and chandra observations of the z105 galaxy cluster xlssj0224039041328 hereafter xlssc 029 detected in the xmmnewton large scale structure survey density and temperature profiles of the xray emitting gas were used to perform a hydrostatic mass analysis of the system this allowed... | [['we', 'present', 'an', 'analysis', 'of', 'deep', 'xmmnewton', 'and', 'chandra', 'observations', 'of', 'the', 'z105', 'galaxy', 'cluster', 'xlssj0224039041328', 'hereafter', 'xlssc', '029', 'detected', 'in', 'the', 'xmmnewton', 'large', 'scale', 'structure', 'survey', 'density', 'and', 'temperature', 'profiles', 'of',... | [-0.07019770792824905, 0.08834682772499036, -0.09616315884018907, 0.08122643966089527, -0.030519117565442382, -0.024331597532485223, 0.0684294831698935, 0.38102297321893275, -0.18554586644071, -0.3910034444464448, 0.056623036286813054, -0.339753529347945, -0.0017242666726815514, 0.15592070047568996, 0.02824778581634746... |
709.2301 | Constraints on decaying Dark Matter from XMM-Newton observations of M31 | We derive constraints on parameters of the radiatively decaying Dark Matter
(DM) particles, using XMM-Newton EPIC spectra of the Andromeda galaxy (M31).
Using the observations of the outer (5'-13') parts of M31 we improve the
existing constraints. For the case of sterile neutrino DM, combining our
constraints with th... | astro-ph hep-ph | we derive constraints on parameters of the radiatively decaying dark matter dm particles using xmmnewton epic spectra of the andromeda galaxy m31 using the observations of the outer 513 parts of m31 we improve the existing constraints for the case of sterile neutrino dm combining our constraints with the latest computa... | [['we', 'derive', 'constraints', 'on', 'parameters', 'of', 'the', 'radiatively', 'decaying', 'dark', 'matter', 'dm', 'particles', 'using', 'xmmnewton', 'epic', 'spectra', 'of', 'the', 'andromeda', 'galaxy', 'm31', 'using', 'the', 'observations', 'of', 'the', 'outer', '513', 'parts', 'of', 'm31', 'we', 'improve', 'the',... | [-0.08632590928007974, 0.16028790168992774, -0.04157582386333898, 0.11068087154401567, -0.11146446375641972, -0.09790308685419527, 0.06790422261661119, 0.30979465216719165, -0.1493844288500416, -0.4071543092487028, 0.028157986521978887, -0.3031078673351707, 0.004300083485243187, 0.21738893785545402, 0.01719652557791984... |
709.2302 | First-principles study of ternary fcc solution phases from special
quasirandom structures | In the present work, ternary Special Quasirandom Structures (SQSs) for a fcc
solid solution phase are generated at different compositions,
$x_A=x_B=x_C=\tfrac{1}{3}$ and $x_A=\tfrac{1}{2}$, $x_B=x_C=\tfrac{1}{4}$,
whose correlation functions are satisfactorily close to those of a random fcc
solution. The generated SQ... | cond-mat.mtrl-sci | in the present work ternary special quasirandom structures sqss for a fcc solid solution phase are generated at different compositions x_ax_bx_ctfrac13 and x_atfrac12 x_bx_ctfrac14 whose correlation functions are satisfactorily close to those of a random fcc solution the generated sqss are used to calculate the mixing ... | [['in', 'the', 'present', 'work', 'ternary', 'special', 'quasirandom', 'structures', 'sqss', 'for', 'a', 'fcc', 'solid', 'solution', 'phase', 'are', 'generated', 'at', 'different', 'compositions', 'x_ax_bx_ctfrac13', 'and', 'x_atfrac12', 'x_bx_ctfrac14', 'whose', 'correlation', 'functions', 'are', 'satisfactorily', 'cl... | [-0.105768102057801, 0.1772353640643128, -0.07715316488113451, 0.073307221409203, -0.021532927096510928, -0.1252208963575724, 0.04524842036066969, 0.38113639957941414, -0.29838850913700043, -0.26036278794013096, 0.09195815409501001, -0.317951087531503, -0.15547259754844403, 0.14944971413882613, 0.06327052698715736, 0.0... |
709.2303 | Phase diagram of hole doped two-leg Cu-O ladders | In the weak coupling limit, we establish the phase diagram of a two-leg
ladder with a unit cell containing both Cu and O atoms, as a function of
doping. We use bosonization and design a specific RG procedure to handle the
additional degrees of freedom. Significant differences are found with the
single orbital case; f... | cond-mat.str-el cond-mat.supr-con | in the weak coupling limit we establish the phase diagram of a twoleg ladder with a unit cell containing both cu and o atoms as a function of doping we use bosonization and design a specific rg procedure to handle the additional degrees of freedom significant differences are found with the single orbital case for purel... | [['in', 'the', 'weak', 'coupling', 'limit', 'we', 'establish', 'the', 'phase', 'diagram', 'of', 'a', 'twoleg', 'ladder', 'with', 'a', 'unit', 'cell', 'containing', 'both', 'cu', 'and', 'o', 'atoms', 'as', 'a', 'function', 'of', 'doping', 'we', 'use', 'bosonization', 'and', 'design', 'a', 'specific', 'rg', 'procedure', ... | [-0.2234834283189748, 0.193406830564478, -0.00608430417086829, 0.03206637580453428, -0.017828391301595876, -0.1447088419640016, 0.11346410331316292, 0.35204318185807554, -0.24159049448026446, -0.2507528320295356, 0.01088176152834128, -0.32495744233971, -0.09814417440824771, 0.08321380491058032, 0.08088974731001672, -0.... |
709.2304 | Pairs of commuting nilpotent matrices, and Hilbert function | Let K be an infinite field and denote by H(n,K) the family of pairs (A,B) of
commuting nilpotent n by n matrices with entries in K. There has been
substantial recent study of the connection between H(n,K) and the fibre H[n] of
the punctual Hilbert scheme of the plane, over an n-fold point of the symmetric
product, by... | math.AC math.AG | let k be an infinite field and denote by hnk the family of pairs ab of commuting nilpotent n by n matrices with entries in k there has been substantial recent study of the connection between hnk and the fibre hn of the punctual hilbert scheme of the plane over an nfold point of the symmetric product by v baranovsky r b... | [['let', 'k', 'be', 'an', 'infinite', 'field', 'and', 'denote', 'by', 'hnk', 'the', 'family', 'of', 'pairs', 'ab', 'of', 'commuting', 'nilpotent', 'n', 'by', 'n', 'matrices', 'with', 'entries', 'in', 'k', 'there', 'has', 'been', 'substantial', 'recent', 'study', 'of', 'the', 'connection', 'between', 'hnk', 'and', 'the'... | [-0.20368409835411092, 0.12978172862517218, -0.06470148004352665, -0.03672952701170475, -0.01421562232530843, -0.1593210104136513, 0.0023892784981468978, 0.32407537477616316, -0.30903342680241436, -0.19306520285466924, 0.05023073435056573, -0.2897758788465021, -0.12691397082705339, 0.14665504157161102, -0.0460539957771... |
709.2305 | The Integrals of Motion for the Deformed W-Algebra $W_{qt}(sl_N^)$ II:
Proof of the commutation relations | We explicitly construct two classes of infinitly many commutative operators
in terms of the deformed W-algebra $W_{qt}(sl_N^)$, and give proofs of the
commutation relations of these operators. We call one of them local integrals
of motion and the other nonlocal one, since they can be regarded as elliptic
deformation ... | math-ph math.MP | we explicitly construct two classes of infinitly many commutative operators in terms of the deformed walgebra w_qtsl_n and give proofs of the commutation relations of these operators we call one of them local integrals of motion and the other nonlocal one since they can be regarded as elliptic deformation of local and ... | [['we', 'explicitly', 'construct', 'two', 'classes', 'of', 'infinitly', 'many', 'commutative', 'operators', 'in', 'terms', 'of', 'the', 'deformed', 'walgebra', 'w_qtsl_n', 'and', 'give', 'proofs', 'of', 'the', 'commutation', 'relations', 'of', 'these', 'operators', 'we', 'call', 'one', 'of', 'them', 'local', 'integrals... | [-0.16303530983701822, 0.09879184504813057, -0.09209646294051307, 0.10474985171803984, -0.09538221899893577, -0.13103016352249405, -0.07395487397088338, 0.3120433387614913, -0.36913471429024713, -0.23940632946520918, 0.09800289134629134, -0.2820775280311956, -0.13053002963000435, 0.2057648016518708, -0.1020917336503833... |
709.2306 | Module d'Alexander et repr\'esentations m\'etab\'eliennes | It is known, since works of Burde and de Rham, that one can detect the roots
of the Alexander polynomial of a knot by the study of the representations of
the knot group into the group of the invertible upper triangular $2x2$
matrices. In this work, we propose to generalize this result by considering the
representatio... | math.GT | it is known since works of burde and de rham that one can detect the roots of the alexander polynomial of a knot by the study of the representations of the knot group into the group of the invertible upper triangular 2x2 matrices in this work we propose to generalize this result by considering the representations of th... | [['it', 'is', 'known', 'since', 'works', 'of', 'burde', 'and', 'de', 'rham', 'that', 'one', 'can', 'detect', 'the', 'roots', 'of', 'the', 'alexander', 'polynomial', 'of', 'a', 'knot', 'by', 'the', 'study', 'of', 'the', 'representations', 'of', 'the', 'knot', 'group', 'into', 'the', 'group', 'of', 'the', 'invertible', '... | [-0.1913954608161558, 0.06876131988511505, -0.12732986167115581, -0.00034433050578544765, -0.0933910118077289, -0.11667373811889609, -0.0018860775638710368, 0.3141184731767597, -0.3169451369427737, -0.2796244403103959, 0.1307335401850816, -0.20704793282361192, -0.21165234299207275, 0.14061732251535763, -0.0834054785611... |
709.2307 | The Generalized Uncertainty Principle in (A)dS Space and the
Modification of Hawking Temperature from the Minimal Length | Recently, the Heisenberg's uncertainty principle has been extended to
incorporate the existence of a large (cut-off) length scale in de Sitter or
anti-de Sitter space, and the Hawking temperatures of the Schwarzshild-(anti)
de Sitter black holes have been reproduced by using the extended uncertainty
principle. I gene... | hep-th gr-qc | recently the heisenbergs uncertainty principle has been extended to incorporate the existence of a large cutoff length scale in de sitter or antide sitter space and the hawking temperatures of the schwarzshildanti de sitter black holes have been reproduced by using the extended uncertainty principle i generalize the ex... | [['recently', 'the', 'heisenbergs', 'uncertainty', 'principle', 'has', 'been', 'extended', 'to', 'incorporate', 'the', 'existence', 'of', 'a', 'large', 'cutoff', 'length', 'scale', 'in', 'de', 'sitter', 'or', 'antide', 'sitter', 'space', 'and', 'the', 'hawking', 'temperatures', 'of', 'the', 'schwarzshildanti', 'de', 's... | [-0.08298517236661197, 0.17132468098432768, -0.12754562677831477, 0.16271621396896455, -0.0861648696864772, -0.10480691731955187, 0.01388736608891915, 0.2963953221288438, -0.20470542240187398, -0.2950321307324239, 0.0998360423080655, -0.2634592991417799, -0.05298867460507422, 0.14896141856900838, -0.09346220945605101, ... |
709.2308 | Albert algebras over curves of genus zero and one | Albert algebras and other Jordan algebras are constructed over curves of
genus zero and one, using a generalization of the Tits process and the first
Tits construction due to Achhammer.
| math.RA math.AG | albert algebras and other jordan algebras are constructed over curves of genus zero and one using a generalization of the tits process and the first tits construction due to achhammer | [['albert', 'algebras', 'and', 'other', 'jordan', 'algebras', 'are', 'constructed', 'over', 'curves', 'of', 'genus', 'zero', 'and', 'one', 'using', 'a', 'generalization', 'of', 'the', 'tits', 'process', 'and', 'the', 'first', 'tits', 'construction', 'due', 'to', 'achhammer']] | [-0.09404332399496744, 0.03310011654835323, -0.1187177339954109, 0.023156971367919547, -0.17507506862025837, -0.2053137652030022, -0.032703472108676516, 0.29041822357424374, -0.34212841498183794, -0.21983871339210148, 0.13762800697365712, -0.2616991797654793, -0.144785708009169, 0.2542225004270159, -0.21076514530156193... |
709.2309 | Evolutionary Catastrophes and the Goldilocks Problem | One of the mainstays of the controversial "rare Earth" hypothesis is the
"Goldilocks problem" regarding various parameters describing a habitable
planet, partially involving the role of mass extinctions and other catastrophic
processes in biological evolution. Usually, this is construed as support for
the uniqueness ... | astro-ph physics.geo-ph physics.soc-ph q-bio.PE | one of the mainstays of the controversial rare earth hypothesis is the goldilocks problem regarding various parameters describing a habitable planet partially involving the role of mass extinctions and other catastrophic processes in biological evolution usually this is construed as support for the uniqueness of the ea... | [['one', 'of', 'the', 'mainstays', 'of', 'the', 'controversial', 'rare', 'earth', 'hypothesis', 'is', 'the', 'goldilocks', 'problem', 'regarding', 'various', 'parameters', 'describing', 'a', 'habitable', 'planet', 'partially', 'involving', 'the', 'role', 'of', 'mass', 'extinctions', 'and', 'other', 'catastrophic', 'pro... | [-0.06239314278271715, 0.14479664198016898, -0.09055312579896833, 0.16566723086205976, -0.12782979308228407, -0.072979720622035, 0.09171285346549536, 0.33230461959194924, -0.2508147412179304, -0.31038715231365394, 0.11596259435505739, -0.2370794260026222, -0.1698820244757891, 0.18160838830517606, -0.10901969007016825, ... |
709.231 | Modelling the SEDs of spiral galaxies | Modelling the UV/optical - infrared/submm SEDs of spiral galaxies observed
with Herschel will be an essential tool to quantitatively interpret these
observations in terms of the present and past star-formation activity of these
systems. In this lecture we describe the SED modelling technique we have
developed, its ap... | astro-ph | modelling the uvoptical infraredsubmm seds of spiral galaxies observed with herschel will be an essential tool to quantitatively interpret these observations in terms of the present and past starformation activity of these systems in this lecture we describe the sed modelling technique we have developed its application... | [['modelling', 'the', 'uvoptical', 'infraredsubmm', 'seds', 'of', 'spiral', 'galaxies', 'observed', 'with', 'herschel', 'will', 'be', 'an', 'essential', 'tool', 'to', 'quantitatively', 'interpret', 'these', 'observations', 'in', 'terms', 'of', 'the', 'present', 'and', 'past', 'starformation', 'activity', 'of', 'these',... | [-0.03493749371828568, 0.0486207515342826, -0.10978771225464615, 0.12003744632326716, -0.06902704538890359, -0.033799269429767846, -0.033720407756680455, 0.5176507900045677, -0.15469449233249621, -0.33706690197471867, 0.059748223136094486, -0.26975200604426913, -0.04514838485258885, 0.18124865401257534, -0.040661338046... |
709.2311 | Two-Loop Electroweak NLL Corrections: from Massless to Massive Fermions | Recently the two-loop next-to-leading logarithmic (NLL) virtual corrections
to arbitrary processes with massless external fermions have been calculated.
Within the spontaneously broken electroweak theory the one- and two-loop mass
singularities have been derived to NLL accuracy and expressed as universal
correction f... | hep-ph | recently the twoloop nexttoleading logarithmic nll virtual corrections to arbitrary processes with massless external fermions have been calculated within the spontaneously broken electroweak theory the one and twoloop mass singularities have been derived to nll accuracy and expressed as universal correction factors dep... | [['recently', 'the', 'twoloop', 'nexttoleading', 'logarithmic', 'nll', 'virtual', 'corrections', 'to', 'arbitrary', 'processes', 'with', 'massless', 'external', 'fermions', 'have', 'been', 'calculated', 'within', 'the', 'spontaneously', 'broken', 'electroweak', 'theory', 'the', 'one', 'and', 'twoloop', 'mass', 'singula... | [-0.15315545730517952, 0.22042592119420418, -0.06312385931672466, 0.12177216998495899, -0.06180987119224373, -0.12943667190783953, 0.0185288351395674, 0.28951223094302875, -0.14176784750524457, -0.3194977828188912, 0.0076977270028482266, -0.30920719109721234, -0.10259983199904417, 0.12215091968415775, 0.023097394900345... |
709.2312 | Asymptotic estimation of some multiple integrals and the electromagnetic
deuteron form factors at high momentum transfer | A theorem about asymptotic estimation of multiple integral of a special type
is proved for the case when the integrand peaks at the integration domain
bound, but not at a point of extremum. Using this theorem the asymptotic
expansion of the electromagnetic deuteron form factors at high momentum
transfers is obtained ... | nucl-th | a theorem about asymptotic estimation of multiple integral of a special type is proved for the case when the integrand peaks at the integration domain bound but not at a point of extremum using this theorem the asymptotic expansion of the electromagnetic deuteron form factors at high momentum transfers is obtained in t... | [['a', 'theorem', 'about', 'asymptotic', 'estimation', 'of', 'multiple', 'integral', 'of', 'a', 'special', 'type', 'is', 'proved', 'for', 'the', 'case', 'when', 'the', 'integrand', 'peaks', 'at', 'the', 'integration', 'domain', 'bound', 'but', 'not', 'at', 'a', 'point', 'of', 'extremum', 'using', 'this', 'theorem', 'th... | [-0.10946426216402762, 0.11065716164246682, -0.140169582580046, 0.12551774894342987, -0.03081060585475737, -0.08345946858346623, 0.055237891417877966, 0.3131375673917993, -0.22181572588861628, -0.27263501316549316, 0.03586529270540522, -0.285243042536901, -0.06375982718021479, 0.18802256078799806, 0.021542432657893625,... |
709.2313 | IGR J17098-3628: an X-ray Nova discovered by INTEGRAL | We report the discovery with INTEGRAL on March 24, 2005, and follow-up
observations of the distant Galactic X-ray nova IGR J17098-3628.
| astro-ph | we report the discovery with integral on march 24 2005 and followup observations of the distant galactic xray nova igr j170983628 | [['we', 'report', 'the', 'discovery', 'with', 'integral', 'on', 'march', '24', '2005', 'and', 'followup', 'observations', 'of', 'the', 'distant', 'galactic', 'xray', 'nova', 'igr', 'j170983628']] | [-0.07777603928531919, 0.05679100153169462, -0.03643018938601017, 0.024998756125569344, -0.2742154642584778, -0.09842875497859149, 0.2054131506454377, 0.46260355909665424, -0.05423796540569691, -0.4310929074597966, 0.20741497332762396, -0.45129934911217007, -0.1103664127488931, 0.25186214077153374, -0.0503616056576859,... |
709.2314 | Bound magnetic polarons in the very dilute regime | We study bound magnetic polarons (BMP) in a very diluted magnetic
semiconductor CdMnTe by means of site selective spectroscopy. In zero magnetic
field we detect a broad and asymmetric band with a characteristic spectral
width of about 5 meV. When external magnetic fields are applied a new line
appears in the emission... | cond-mat.mtrl-sci | we study bound magnetic polarons bmp in a very diluted magnetic semiconductor cdmnte by means of site selective spectroscopy in zero magnetic field we detect a broad and asymmetric band with a characteristic spectral width of about 5 mev when external magnetic fields are applied a new line appears in the emission spect... | [['we', 'study', 'bound', 'magnetic', 'polarons', 'bmp', 'in', 'a', 'very', 'diluted', 'magnetic', 'semiconductor', 'cdmnte', 'by', 'means', 'of', 'site', 'selective', 'spectroscopy', 'in', 'zero', 'magnetic', 'field', 'we', 'detect', 'a', 'broad', 'and', 'asymmetric', 'band', 'with', 'a', 'characteristic', 'spectral',... | [-0.11987785071854098, 0.13710084322256846, -0.01257750546806548, 0.0776763884483904, -0.009413872350705788, -0.12944704524791203, 0.0610565932366593, 0.42666712359536485, -0.2548659478134689, -0.3423219026369323, 0.014293577671415699, -0.28289000518025315, -0.05771496380870062, 0.18513693483209753, 0.0606218995764874,... |
709.2315 | Massless Fermions in multilayer graphitic systems with misoriented
layers | We examine how the misorientation of a few stacked graphene layers affects
the electronic structure of carbon nanosystems. We present {\it ab initio}
calculations on bi- and trilayer systems to demonstrate that the massless
Fermion behavior typical of single layered graphene is also found in
incommensurate multilayer... | cond-mat.mtrl-sci cond-mat.mes-hall | we examine how the misorientation of a few stacked graphene layers affects the electronic structure of carbon nanosystems we present it ab initio calculations on bi and trilayer systems to demonstrate that the massless fermion behavior typical of single layered graphene is also found in incommensurate multilayered grap... | [['we', 'examine', 'how', 'the', 'misorientation', 'of', 'a', 'few', 'stacked', 'graphene', 'layers', 'affects', 'the', 'electronic', 'structure', 'of', 'carbon', 'nanosystems', 'we', 'present', 'it', 'ab', 'initio', 'calculations', 'on', 'bi', 'and', 'trilayer', 'systems', 'to', 'demonstrate', 'that', 'the', 'massless... | [-0.14849454943633236, 0.1166930680244375, -0.033876133253883334, 0.007189263726388096, -0.028062381034016336, -0.1313365900359296, 0.09301585116831654, 0.49756236411972876, -0.3054354851467347, -0.3007307688133159, -0.04479660317323111, -0.37316633571246893, -0.23022663829113366, 0.17373286075078362, 0.051095401505093... |
709.2316 | The pressure of QED from the two-loop 2PI effective action | We compute the pressure of hot quantum electrodynamics from the two-loop
truncation of the 2PI effective action. Since the 2PI resummation guarantees
gauge-fixing independence only up to the order of the truncation, our result
for the pressure presents a gauge dependent contribution of O(e^4). We
numerically characte... | hep-ph | we compute the pressure of hot quantum electrodynamics from the twoloop truncation of the 2pi effective action since the 2pi resummation guarantees gaugefixing independence only up to the order of the truncation our result for the pressure presents a gauge dependent contribution of oe4 we numerically characterize the c... | [['we', 'compute', 'the', 'pressure', 'of', 'hot', 'quantum', 'electrodynamics', 'from', 'the', 'twoloop', 'truncation', 'of', 'the', '2pi', 'effective', 'action', 'since', 'the', '2pi', 'resummation', 'guarantees', 'gaugefixing', 'independence', 'only', 'up', 'to', 'the', 'order', 'of', 'the', 'truncation', 'our', 're... | [-0.15331918848451317, 0.1774290793365231, -0.14805107700025164, 0.0784294122671027, -0.08877000076378264, -0.06370817514976895, 0.08738517548346597, 0.31047117262624385, -0.18483546880505433, -0.2913052932381993, 0.025557934692720087, -0.24498576462473265, -0.12573439341816461, 0.09984897893694479, -0.0514855500901254... |
709.2317 | Adjusted Viterbi training for hidden Markov models | To estimate the emission parameters in hidden Markov models one commonly uses
the EM algorithm or its variation. Our primary motivation, however, is the
Philips speech recognition system wherein the EM algorithm is replaced by the
Viterbi training algorithm. Viterbi training is faster and computationally less
involve... | math.ST math.PR stat.CO stat.TH | to estimate the emission parameters in hidden markov models one commonly uses the em algorithm or its variation our primary motivation however is the philips speech recognition system wherein the em algorithm is replaced by the viterbi training algorithm viterbi training is faster and computationally less involved than... | [['to', 'estimate', 'the', 'emission', 'parameters', 'in', 'hidden', 'markov', 'models', 'one', 'commonly', 'uses', 'the', 'em', 'algorithm', 'or', 'its', 'variation', 'our', 'primary', 'motivation', 'however', 'is', 'the', 'philips', 'speech', 'recognition', 'system', 'wherein', 'the', 'em', 'algorithm', 'is', 'replac... | [-0.030373144591395118, 0.07979777952778767, -0.055618348691734626, 0.15757272683263404, -0.14173094138930567, -0.23289908382461452, 0.04569936564123472, 0.4395726972152708, -0.2612466647091215, -0.34717226388614214, 0.08905587744895277, -0.193666468983226, -0.17273229006420227, 0.17225197682607551, -0.1404802013707698... |
709.2318 | On the relation between the WRT invariant and the Hennings invariant | The purpose of this note is to provide a simple relation between the
Witten-Reshetikhin-Turaev SO(3) invariant and the Hennings invariant of
3-manifolds associated to quantum sl_2.
| math.QA | the purpose of this note is to provide a simple relation between the wittenreshetikhinturaev so3 invariant and the hennings invariant of 3manifolds associated to quantum sl_2 | [['the', 'purpose', 'of', 'this', 'note', 'is', 'to', 'provide', 'a', 'simple', 'relation', 'between', 'the', 'wittenreshetikhinturaev', 'so3', 'invariant', 'and', 'the', 'hennings', 'invariant', 'of', '3manifolds', 'associated', 'to', 'quantum', 'sl_2']] | [-0.2660233311426754, 0.12811134675016198, -0.15218681698808303, 0.14320600620256022, -0.1250585147824425, -0.13564338275374702, -0.040130941492791936, 0.324432814350495, -0.28828615831354487, -0.2696126690134406, 0.05136077406887825, -0.21456221505426443, -0.18884345856405652, 0.18907444093089837, -0.14240802691962856... |
709.2319 | Electroproduction of Soft Pions at Large Momentum Transfers | We consider pion electroproduction on a proton target close to threshold for
Q^2 in the region 1-10 GeV^2. The momentum transfer dependence of the S-wave
multipoles at threshold, E_{0+} and L_{0+}, is calculated using light-cone sum
rules.
| hep-ph nucl-th | we consider pion electroproduction on a proton target close to threshold for q2 in the region 110 gev2 the momentum transfer dependence of the swave multipoles at threshold e_0 and l_0 is calculated using lightcone sum rules | [['we', 'consider', 'pion', 'electroproduction', 'on', 'a', 'proton', 'target', 'close', 'to', 'threshold', 'for', 'q2', 'in', 'the', 'region', '110', 'gev2', 'the', 'momentum', 'transfer', 'dependence', 'of', 'the', 'swave', 'multipoles', 'at', 'threshold', 'e_0', 'and', 'l_0', 'is', 'calculated', 'using', 'lightcone'... | [-0.1089226435177733, 0.21926316810218063, -0.05214504089609191, 0.1683090807070855, -0.03847897797822952, -0.05744515431610666, 0.14091006918130694, 0.41326846101799525, -0.14417785849120165, -0.1798589211964124, -0.13567000064004614, -0.34381767221399256, 0.08892479344865785, 0.13462962441750476, 0.12013815987046582,... |
709.232 | Monte Carlo simulation method for Laughlin-like states in a disk
geometry | We discuss an alternative accurate Monte Carlo method to calculate the
ground-state energy and related quantities for Laughlin states of the
fractional quantum Hall effect in a disk geometry. This alternative approach
allows us to obtain accurate bulk regime (thermodynamic limit) values for
various quantities from Mo... | cond-mat.mes-hall cond-mat.str-el | we discuss an alternative accurate monte carlo method to calculate the groundstate energy and related quantities for laughlin states of the fractional quantum hall effect in a disk geometry this alternative approach allows us to obtain accurate bulk regime thermodynamic limit values for various quantities from monte ca... | [['we', 'discuss', 'an', 'alternative', 'accurate', 'monte', 'carlo', 'method', 'to', 'calculate', 'the', 'groundstate', 'energy', 'and', 'related', 'quantities', 'for', 'laughlin', 'states', 'of', 'the', 'fractional', 'quantum', 'hall', 'effect', 'in', 'a', 'disk', 'geometry', 'this', 'alternative', 'approach', 'allow... | [-0.028812986024870323, 0.16356605613232555, -0.13148627642971966, 0.16575642662803428, -0.030606604396150663, -0.11074100244217194, 0.0594398283220541, 0.3451661193886629, -0.21781571110567222, -0.35832282382135205, 0.019235051149287474, -0.29000104891087036, -0.06578545495151328, 0.272391402707077, 0.0398812334626339... |
709.2321 | An inhomogeneous Josephson phase in thin-film and High-Tc
superconductors | In many cases inhomogeneities are known to exist near the metal (or
superconductor)-insulator transition, as follows from well-known domain-wall
arguments. If the conducting regions are large enough (i.e. when the T=0
superconducting gap is much larger than the single-electron level spacing), and
if they have superco... | cond-mat.supr-con | in many cases inhomogeneities are known to exist near the metal or superconductorinsulator transition as follows from wellknown domainwall arguments if the conducting regions are large enough ie when the t0 superconducting gap is much larger than the singleelectron level spacing and if they have superconducting correla... | [['in', 'many', 'cases', 'inhomogeneities', 'are', 'known', 'to', 'exist', 'near', 'the', 'metal', 'or', 'superconductorinsulator', 'transition', 'as', 'follows', 'from', 'wellknown', 'domainwall', 'arguments', 'if', 'the', 'conducting', 'regions', 'are', 'large', 'enough', 'ie', 'when', 'the', 't0', 'superconducting',... | [-0.136586329018298, 0.20383991823960934, -0.0469708028868795, 0.09938217349306869, -0.03677651507371642, -0.1983965648306084, 0.08238278180039649, 0.36421107382885193, -0.21084292089048168, -0.25615823311556885, 0.0817616360584329, -0.34833692905167346, -0.10959153024599029, 0.19020044529957358, 0.0004123781757254906,... |
709.2322 | Exact enumeration of Hamiltonian circuits, walks, and chains in two and
three dimensions | We present an algorithm for enumerating exactly the number of Hamiltonian
chains on regular lattices in low dimensions. By definition, these are sets of
k disjoint paths whose union visits each lattice vertex exactly once. The
well-known Hamiltonian circuits and walks appear as the special cases k=0 and
k=1 respectiv... | cond-mat.stat-mech | we present an algorithm for enumerating exactly the number of hamiltonian chains on regular lattices in low dimensions by definition these are sets of k disjoint paths whose union visits each lattice vertex exactly once the wellknown hamiltonian circuits and walks appear as the special cases k0 and k1 respectively in t... | [['we', 'present', 'an', 'algorithm', 'for', 'enumerating', 'exactly', 'the', 'number', 'of', 'hamiltonian', 'chains', 'on', 'regular', 'lattices', 'in', 'low', 'dimensions', 'by', 'definition', 'these', 'are', 'sets', 'of', 'k', 'disjoint', 'paths', 'whose', 'union', 'visits', 'each', 'lattice', 'vertex', 'exactly', '... | [-0.17421932693611344, 0.1705313976362168, 0.03234877608433042, 0.010473009181188663, -0.021547376575535567, -0.1811526807166798, 0.07010829249148905, 0.4184148711020775, -0.26113576428337104, -0.2693262536878414, 0.11690223758341745, -0.35410906038621603, -0.10275965720243023, 0.1972104629562439, 0.008428024249556272,... |
709.2323 | Unbiased sampling of globular lattice proteins in three dimensions | We present a Monte Carlo method that allows efficient and unbiased sampling
of Hamiltonian walks on a cubic lattice. Such walks are self-avoiding and visit
each lattice site exactly once. They are often used as simple models of
globular proteins, upon adding suitable local interactions. Our algorithm can
easily be eq... | cond-mat.stat-mech cond-mat.soft | we present a monte carlo method that allows efficient and unbiased sampling of hamiltonian walks on a cubic lattice such walks are selfavoiding and visit each lattice site exactly once they are often used as simple models of globular proteins upon adding suitable local interactions our algorithm can easily be equipped ... | [['we', 'present', 'a', 'monte', 'carlo', 'method', 'that', 'allows', 'efficient', 'and', 'unbiased', 'sampling', 'of', 'hamiltonian', 'walks', 'on', 'a', 'cubic', 'lattice', 'such', 'walks', 'are', 'selfavoiding', 'and', 'visit', 'each', 'lattice', 'site', 'exactly', 'once', 'they', 'are', 'often', 'used', 'as', 'simp... | [-0.10113085079576885, 0.18909071440053782, -0.08251467543545757, 0.0504977442504806, -0.04671828068867085, -0.1894557461843039, 0.06409130071827757, 0.48882915391105003, -0.2572378467383056, -0.2581259937142022, 0.08168490807895132, -0.29552074839927533, -0.17100962611910855, 0.1566105870578181, 0.015439344903229383, ... |
709.2324 | Construction of Fredholm representations and a modification of the
Higson-Roe corona | The Fredholm representation theory is well adapted to construction of
homotopy invariants of non simply connected manifolds on the base of
generalized Hirzebruch formula. Earlier a natural family of the Fredholm
representations was constructed that lead to a symmetric vector bundle on
completion of the fundamental gr... | math.KT | the fredholm representation theory is well adapted to construction of homotopy invariants of non simply connected manifolds on the base of generalized hirzebruch formula earlier a natural family of the fredholm representations was constructed that lead to a symmetric vector bundle on completion of the fundamental group... | [['the', 'fredholm', 'representation', 'theory', 'is', 'well', 'adapted', 'to', 'construction', 'of', 'homotopy', 'invariants', 'of', 'non', 'simply', 'connected', 'manifolds', 'on', 'the', 'base', 'of', 'generalized', 'hirzebruch', 'formula', 'earlier', 'a', 'natural', 'family', 'of', 'the', 'fredholm', 'representatio... | [-0.13859513755177416, 0.07405363972953884, -0.10732229884271904, 0.0524729630333703, -0.12833207417910886, -0.10458977013516588, -0.021659361767795694, 0.32896719425443116, -0.24127529924577576, -0.26076363211781795, 0.15964111689896465, -0.23940822803114453, -0.18250916468500458, 0.16216062658103342, -0.1582101124962... |
709.2325 | Branched Polymers | Building on and from the work of Brydges and Imbrie, we give an elementary
calculation of the volume of the space of branched polymers of order $n$ in the
plane and in 3-space. Our development reveals some more general identities, and
allows exact random sampling. In particular we show that a random 3-dimensional
bra... | math.PR math-ph math.MP | building on and from the work of brydges and imbrie we give an elementary calculation of the volume of the space of branched polymers of order n in the plane and in 3space our development reveals some more general identities and allows exact random sampling in particular we show that a random 3dimensional branched poly... | [['building', 'on', 'and', 'from', 'the', 'work', 'of', 'brydges', 'and', 'imbrie', 'we', 'give', 'an', 'elementary', 'calculation', 'of', 'the', 'volume', 'of', 'the', 'space', 'of', 'branched', 'polymers', 'of', 'order', 'n', 'in', 'the', 'plane', 'and', 'in', '3space', 'our', 'development', 'reveals', 'some', 'more'... | [-0.16438967480863784, 0.14228085429423362, -0.06670593485117905, -0.01820346217099873, -0.048097204357858685, -0.07394657570070454, 0.02362651949275344, 0.350518634084553, -0.20535892432200767, -0.27219508153696853, 0.09074866238220167, -0.2745714422857245, -0.2074622684906769, 0.1708355492483529, -0.05060765249211164... |
709.2326 | Integrable operators and the squares of Hankel operators | Integrable operators arise in random matrix theory, where they describe the
asymptotic eigenvalue distributions of large self-adjoint random matrices from
the generalized unitary ensembles. This paper gives sufficient conditions for
an integrable operator to be the square of a Hankel operator, and applies the
conditi... | math.FA | integrable operators arise in random matrix theory where they describe the asymptotic eigenvalue distributions of large selfadjoint random matrices from the generalized unitary ensembles this paper gives sufficient conditions for an integrable operator to be the square of a hankel operator and applies the condition to ... | [['integrable', 'operators', 'arise', 'in', 'random', 'matrix', 'theory', 'where', 'they', 'describe', 'the', 'asymptotic', 'eigenvalue', 'distributions', 'of', 'large', 'selfadjoint', 'random', 'matrices', 'from', 'the', 'generalized', 'unitary', 'ensembles', 'this', 'paper', 'gives', 'sufficient', 'conditions', 'for'... | [-0.0959783090363172, 0.1708992451537845, -0.07915355928919532, 0.13996457060248677, -0.06339683426882733, -0.16542165639217604, -0.08765540136109022, 0.3085908329622312, -0.31000245728275994, -0.09532674585723064, 0.12427466959396208, -0.2825350898402658, -0.2333041222935373, 0.09873500280082226, -0.091200392303819, 0... |
709.2327 | Spiral Growth and Step Edge Barriers | The growth of spiral mounds containing a screw dislocation is compared to the
growth of wedding cakes by two-dimensional nucleation. Using phase field
simulations and homoepitaxial growth experiments on the Pt(111) surface we show
that both structures attain the same characteristic large scale shape when a
significan... | cond-mat.mtrl-sci cond-mat.stat-mech | the growth of spiral mounds containing a screw dislocation is compared to the growth of wedding cakes by twodimensional nucleation using phase field simulations and homoepitaxial growth experiments on the pt111 surface we show that both structures attain the same characteristic large scale shape when a significant step... | [['the', 'growth', 'of', 'spiral', 'mounds', 'containing', 'a', 'screw', 'dislocation', 'is', 'compared', 'to', 'the', 'growth', 'of', 'wedding', 'cakes', 'by', 'twodimensional', 'nucleation', 'using', 'phase', 'field', 'simulations', 'and', 'homoepitaxial', 'growth', 'experiments', 'on', 'the', 'pt111', 'surface', 'we... | [-0.12564508711114863, 0.15861100979319334, -0.04627402855972336, 0.02062173048695761, -0.014965396334776993, -0.08031893078375353, 0.022306448131613168, 0.39778651265342807, -0.29753980904140254, -0.2933968614617532, 0.05418207508972211, -0.25775100507731125, -0.12787596312542024, 0.16825083406134086, 0.03060642532198... |
709.2328 | Search for X-ray bursts in the INTEGRAL/IBIS data of 2003-2005 and
discovery of the new X-ray burster IGR J17364-2711/17380-3749 | All the observations performed with the IBIS telescope aboard the INTEGRAL
observatory during the first 2.5 years of its in-orbit operation have been
analyzed to find X-ray bursts. There were 1788 statistically confident events
with a duration from 5 to 500 s revealed in time records of the 15-25 keV count
rate of th... | astro-ph | all the observations performed with the ibis telescope aboard the integral observatory during the first 25 years of its inorbit operation have been analyzed to find xray bursts there were 1788 statistically confident events with a duration from 5 to 500 s revealed in time records of the 1525 kev count rate of the ibisi... | [['all', 'the', 'observations', 'performed', 'with', 'the', 'ibis', 'telescope', 'aboard', 'the', 'integral', 'observatory', 'during', 'the', 'first', '25', 'years', 'of', 'its', 'inorbit', 'operation', 'have', 'been', 'analyzed', 'to', 'find', 'xray', 'bursts', 'there', 'were', '1788', 'statistically', 'confident', 'e... | [-0.08797266107831092, 0.1578869925615436, -0.04423972309450619, 0.1375655898664263, -0.10190865357799339, -0.15740314281356405, 0.08570663959835656, 0.4491151826659916, -0.1846123831855948, -0.39741984069632963, 0.16160226728243288, -0.40874151086609345, -0.03608517147040402, 0.26833161172180553, -0.018177410227508517... |
709.2329 | Direct observation of high-speed plasma outflows produced by magnetic
reconnection in solar impulsive events | Spectroscopic observations of a solar limb flare recorded by SUMER on SOHO
reveal, for the first time, hot fast magnetic reconnection outflows in the
corona. As the reconnection site rises across the SUMER spectrometer slit,
significant blue- and red-shift signatures are observed in sequence in the Fe
XIX line, refle... | astro-ph | spectroscopic observations of a solar limb flare recorded by sumer on soho reveal for the first time hot fast magnetic reconnection outflows in the corona as the reconnection site rises across the sumer spectrometer slit significant blue and redshift signatures are observed in sequence in the fe xix line reflecting upf... | [['spectroscopic', 'observations', 'of', 'a', 'solar', 'limb', 'flare', 'recorded', 'by', 'sumer', 'on', 'soho', 'reveal', 'for', 'the', 'first', 'time', 'hot', 'fast', 'magnetic', 'reconnection', 'outflows', 'in', 'the', 'corona', 'as', 'the', 'reconnection', 'site', 'rises', 'across', 'the', 'sumer', 'spectrometer', ... | [-0.10257251044206966, 0.2439991113407394, 0.04777967429254204, 0.13663550705174343, -0.0852705828863411, -0.06815280737618405, 0.0002793925109122378, 0.4873700366230108, -0.16483568127911824, -0.35976954756412083, 0.009808968026146222, -0.2860467090414694, 0.0077597947585253185, 0.2514206847946088, -0.0172577864460226... |
709.233 | Queueing for ergodic arrivals and services | In this paper we revisit the results of Loynes (1962) on stability of queues
for ergodic arrivals and services, and show examples when the arrivals are
bounded and ergodic, the service rate is constant, and under stability the
limit distribution has larger than exponential tail.
| math.PR cs.IT math.IT | in this paper we revisit the results of loynes 1962 on stability of queues for ergodic arrivals and services and show examples when the arrivals are bounded and ergodic the service rate is constant and under stability the limit distribution has larger than exponential tail | [['in', 'this', 'paper', 'we', 'revisit', 'the', 'results', 'of', 'loynes', '1962', 'on', 'stability', 'of', 'queues', 'for', 'ergodic', 'arrivals', 'and', 'services', 'and', 'show', 'examples', 'when', 'the', 'arrivals', 'are', 'bounded', 'and', 'ergodic', 'the', 'service', 'rate', 'is', 'constant', 'and', 'under', 's... | [-0.19111702541510264, 0.1314337867984755, -0.06069106285770734, 0.0833397523396545, 0.015610769763588906, -0.12806687595115768, 0.12157987931795004, 0.35828998924957384, -0.21892927932656472, -0.21241193413734435, 0.1856895464291382, -0.3073743277125888, -0.08258302662935522, 0.18766663372516632, -0.1509039454265601, ... |
709.2331 | Conjugate Points in Length Spaces | In this paper we extend the concept of a conjugate point in a Riemannian
manifold to complete length spaces (also known as geodesic spaces). In
particular, we introduce symmetric conjugate points and ultimate conjugate
points. We then generalize the long homotopy lemma of Klingenberg to this
setting as well as the in... | math.MG | in this paper we extend the concept of a conjugate point in a riemannian manifold to complete length spaces also known as geodesic spaces in particular we introduce symmetric conjugate points and ultimate conjugate points we then generalize the long homotopy lemma of klingenberg to this setting as well as the injectivi... | [['in', 'this', 'paper', 'we', 'extend', 'the', 'concept', 'of', 'a', 'conjugate', 'point', 'in', 'a', 'riemannian', 'manifold', 'to', 'complete', 'length', 'spaces', 'also', 'known', 'as', 'geodesic', 'spaces', 'in', 'particular', 'we', 'introduce', 'symmetric', 'conjugate', 'points', 'and', 'ultimate', 'conjugate', '... | [-0.0950519076465845, 0.06102974384618616, -0.08846074920417606, 0.16070781049969862, -0.1100639564902994, -0.12085198841827072, 0.052753047998218484, 0.368392882315253, -0.2641609616415656, -0.21505595872894037, 0.12328980129340367, -0.2832870274508858, -0.16260118232921872, 0.2337346496414798, -0.1920501358260441, 0.... |
709.2332 | A new method for the numerical evaluation of one-loop amplitudes | We recently presented a new method for the evaluation of one-loop amplitude
of arbitrary scattering processes, in which the reduction to scalar integrals
is performed at the integrand level. In this talk, we review the main features
of the method and briefly summarize the results of the first calculations
performed u... | hep-ph | we recently presented a new method for the evaluation of oneloop amplitude of arbitrary scattering processes in which the reduction to scalar integrals is performed at the integrand level in this talk we review the main features of the method and briefly summarize the results of the first calculations performed using i... | [['we', 'recently', 'presented', 'a', 'new', 'method', 'for', 'the', 'evaluation', 'of', 'oneloop', 'amplitude', 'of', 'arbitrary', 'scattering', 'processes', 'in', 'which', 'the', 'reduction', 'to', 'scalar', 'integrals', 'is', 'performed', 'at', 'the', 'integrand', 'level', 'in', 'this', 'talk', 'we', 'review', 'the'... | [-0.09839435258450416, 0.07756166798599924, -0.1283480505942582, 0.07422666502400087, -0.01420315308496356, -0.03543140817111215, 0.05531313058991845, 0.3327741570269259, -0.19368821246406207, -0.27148591024944413, 0.09227173320071486, -0.26748961593525916, -0.21813329182959235, 0.20167546856772298, 0.02437743145184448... |
709.2333 | Diffusion, super-diffusion and coalescence from single step | From the exact single step evolution equation of the two-point correlation
function of a particle distribution subjected to a stochastic displacement
field $\bu(\bx)$, we derive different dynamical regimes when $\bu(\bx)$ is
iterated to build a velocity field. First we show that spatially uncorrelated
fields $\bu(\bx... | cond-mat.stat-mech cond-mat.dis-nn | from the exact single step evolution equation of the twopoint correlation function of a particle distribution subjected to a stochastic displacement field bubx we derive different dynamical regimes when bubx is iterated to build a velocity field first we show that spatially uncorrelated fields bubx lead to both standar... | [['from', 'the', 'exact', 'single', 'step', 'evolution', 'equation', 'of', 'the', 'twopoint', 'correlation', 'function', 'of', 'a', 'particle', 'distribution', 'subjected', 'to', 'a', 'stochastic', 'displacement', 'field', 'bubx', 'we', 'derive', 'different', 'dynamical', 'regimes', 'when', 'bubx', 'is', 'iterated', 't... | [-0.14286240637062964, 0.16919183914701566, -0.15272864383308493, 0.08782650794956093, -0.03678825086705941, -0.15883553733451436, -0.040009009417357806, 0.35436494079094827, -0.30337505868688913, -0.25903464745439536, 0.022508273837453824, -0.25576511936935975, -0.13528159942233553, 0.16242725511183898, 0.044825577679... |
709.2334 | Noetherian Hopf algebras | This short survey article reviews current understand- ing of the structure of
noetherian Hopf algebras. The focus is on homological properties. A number of
open problems are listed.
| math.RA math.QA | this short survey article reviews current understand ing of the structure of noetherian hopf algebras the focus is on homological properties a number of open problems are listed | [['this', 'short', 'survey', 'article', 'reviews', 'current', 'understand', 'ing', 'of', 'the', 'structure', 'of', 'noetherian', 'hopf', 'algebras', 'the', 'focus', 'is', 'on', 'homological', 'properties', 'a', 'number', 'of', 'open', 'problems', 'are', 'listed']] | [-0.2642283780899431, 0.01583636478920068, -0.04606181101241548, 0.1188285534735769, -0.19263871180425798, -0.10868949813967836, -0.06153908145747015, 0.3374869164877704, -0.37853163986333777, -0.24565693074172096, 0.19340022773082768, -0.2536536194384098, -0.10300454849909459, 0.22248918283730745, -0.15804536229864294... |
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