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 |
|---|---|---|---|---|---|---|
707.383 | On Cosmological Implications of Gravitational Trace Anomaly | We study the infrared effective theory of gravity that stems from the quantum
trace anomaly. Quantum fluctuations of the metric induce running of the
cosmological constant and the Newton constant at cosmological scales. By
imposing the generalized Bianchi identity we obtain a prediction for the scale
dependence of th... | gr-qc astro-ph hep-th | we study the infrared effective theory of gravity that stems from the quantum trace anomaly quantum fluctuations of the metric induce running of the cosmological constant and the newton constant at cosmological scales by imposing the generalized bianchi identity we obtain a prediction for the scale dependence of the da... | [['we', 'study', 'the', 'infrared', 'effective', 'theory', 'of', 'gravity', 'that', 'stems', 'from', 'the', 'quantum', 'trace', 'anomaly', 'quantum', 'fluctuations', 'of', 'the', 'metric', 'induce', 'running', 'of', 'the', 'cosmological', 'constant', 'and', 'the', 'newton', 'constant', 'at', 'cosmological', 'scales', '... | [-0.1500758302964918, 0.1642345284471167, -0.13966554201539585, 0.10585334543746126, -0.0600391057441416, -0.09208578334706229, -0.030469088063514588, 0.249224322564576, -0.2682146511303828, -0.36589273278925405, 0.05786808636216649, -0.23613884778814795, -0.08768511197084318, 0.12074372707359979, 0.037070903714503285,... |
707.3831 | Cobaltocene Encapsulation Into Single-walled Carbon Nanotubes: A
Molecular Dynamics Investigation | Recently (PRL 96, 106804 (2006)) it was suggested that cobaltocene(CC)
molecules encapsulated into (7,7) carbon nanotubes (CNT@(7,7)) could be the
basis for new spintronic devices. We show here based on impact molecular
dynamics and DFT calculations that when dynamical aspects are explicitly
considered the CC encapsu... | cond-mat.mtrl-sci | recently prl 96 106804 2006 it was suggested that cobaltocenecc molecules encapsulated into 77 carbon nanotubes cnt77 could be the basis for new spintronic devices we show here based on impact molecular dynamics and dft calculations that when dynamical aspects are explicitly considered the cc encapsulation into cnt77 d... | [['recently', 'prl', '96', '106804', '2006', 'it', 'was', 'suggested', 'that', 'cobaltocenecc', 'molecules', 'encapsulated', 'into', '77', 'carbon', 'nanotubes', 'cnt77', 'could', 'be', 'the', 'basis', 'for', 'new', 'spintronic', 'devices', 'we', 'show', 'here', 'based', 'on', 'impact', 'molecular', 'dynamics', 'and', ... | [-0.11197666162574339, 0.12270776959358835, -0.08305421865762859, 0.02343698162408343, -0.0740386804808741, -0.1692845385645658, 0.08268842428578468, 0.3938826342295531, -0.22805159918219864, -0.29803624751461344, 0.041206177635341075, -0.23357359846831177, -0.18192549942709182, 0.21033865013210426, -0.0045328321866691... |
707.3832 | Reheating Closed String Inflation | Protecting the inflationary potential from quantum corrections typically
requires symmetries that constrain the form of couplings of the inflaton to
other sectors. We will explore how these restrictions affect reheating in
models with UV completions. In particular, we look at how reheating occurs when
inflation is go... | hep-th astro-ph hep-ph | protecting the inflationary potential from quantum corrections typically requires symmetries that constrain the form of couplings of the inflaton to other sectors we will explore how these restrictions affect reheating in models with uv completions in particular we look at how reheating occurs when inflation is governe... | [['protecting', 'the', 'inflationary', 'potential', 'from', 'quantum', 'corrections', 'typically', 'requires', 'symmetries', 'that', 'constrain', 'the', 'form', 'of', 'couplings', 'of', 'the', 'inflaton', 'to', 'other', 'sectors', 'we', 'will', 'explore', 'how', 'these', 'restrictions', 'affect', 'reheating', 'in', 'mo... | [-0.10054471720442441, 0.2727986878236542, -0.06797146055864037, 0.16324892508107172, -0.12103641791535276, -0.1884554561901106, 0.0030539513328611584, 0.3525320111574339, -0.22041659491203194, -0.3611952131821973, 0.07639376506475466, -0.2787079214945801, -0.04715854047182282, 0.147208561775707, 0.010584655600333852, ... |
707.3833 | Near-Infrared Interferometric, Spectroscopic, and Photometric Monitoring
of T Tauri Inner Disks | We present high angular resolution observations with the Keck Interferometer,
high dispersion spectroscopic observations with Keck/NIRSPEC, and near-IR
photometric observations from PAIRITEL of a sample of 11 solar-type T Tauri
stars in 9 systems. We use these observations to probe the circumstellar
material within 1... | astro-ph | we present high angular resolution observations with the keck interferometer high dispersion spectroscopic observations with kecknirspec and nearir photometric observations from pairitel of a sample of 11 solartype t tauri stars in 9 systems we use these observations to probe the circumstellar material within 1 au of t... | [['we', 'present', 'high', 'angular', 'resolution', 'observations', 'with', 'the', 'keck', 'interferometer', 'high', 'dispersion', 'spectroscopic', 'observations', 'with', 'kecknirspec', 'and', 'nearir', 'photometric', 'observations', 'from', 'pairitel', 'of', 'a', 'sample', 'of', '11', 'solartype', 't', 'tauri', 'star... | [-0.06596172684434765, 0.11924225205352695, -0.054384015265409605, 0.06475389992361796, -0.12712555652654886, -0.04957265345757772, 0.048945477729983686, 0.4669138626149385, -0.15678948725546055, -0.3767522659779775, 0.11371791568160573, -0.2873874377634487, 0.022450110853170183, 0.23451210936706623, -0.044929349512590... |
707.3834 | Spin squeezing in optical lattice clocks via lattice-based QND
measurements | Quantum projection noise will soon limit the best achievable precision of
optical atomic clocks based on lattice-confined neutral atoms. Squeezing the
collective atomic pseudo-spin via measurement of the clock state populations
during Ramsey interrogation suppresses the projection noise. We show here that
the lattice... | quant-ph physics.atom-ph | quantum projection noise will soon limit the best achievable precision of optical atomic clocks based on latticeconfined neutral atoms squeezing the collective atomic pseudospin via measurement of the clock state populations during ramsey interrogation suppresses the projection noise we show here that the lattice laser... | [['quantum', 'projection', 'noise', 'will', 'soon', 'limit', 'the', 'best', 'achievable', 'precision', 'of', 'optical', 'atomic', 'clocks', 'based', 'on', 'latticeconfined', 'neutral', 'atoms', 'squeezing', 'the', 'collective', 'atomic', 'pseudospin', 'via', 'measurement', 'of', 'the', 'clock', 'state', 'populations', ... | [-0.12278557497356991, 0.2702101629502332, -0.030321596139472305, -0.018304923029381383, 0.04797491956574535, -0.14975516960133337, 0.1216601157838985, 0.4099578359571186, -0.2785833828802248, -0.24129027468197553, 0.06099468377956813, -0.23601678242563334, -0.04259130459287864, 0.18143236959009496, -0.0437662831295136... |
707.3835 | Symmetry groups of non-simply-connected four-manifolds | Let $M$ be a closed, connected, orientable topological four-manifold with
$H_1(M)$ nontrivial and free abelian, $b_2(M)\ne 0, 2$, and $\chi(M)\ne 0$. We
show that if $G$ is a finite group of 2-rank $\le 1$ which admits a
homologically trivial, locally linear, effective action on $M$, then $G$ must
be cyclic.
With a... | math.GT math.AT | let m be a closed connected orientable topological fourmanifold with h_1m nontrivial and free abelian b_2mne 0 2 and chimne 0 we show that if g is a finite group of 2rank le 1 which admits a homologically trivial locally linear effective action on m then g must be cyclic with additional assumptions to ensure orientabil... | [['let', 'm', 'be', 'a', 'closed', 'connected', 'orientable', 'topological', 'fourmanifold', 'with', 'h_1m', 'nontrivial', 'and', 'free', 'abelian', 'b_2mne', '0', '2', 'and', 'chimne', '0', 'we', 'show', 'that', 'if', 'g', 'is', 'a', 'finite', 'group', 'of', '2rank', 'le', '1', 'which', 'admits', 'a', 'homologically',... | [-0.24935383499671457, 0.1498916586031123, -0.10212823634017443, 0.01254580662894699, -0.14173484436872572, -0.21179993294345417, 0.02662905615450132, 0.3767664816488724, -0.30569405051519966, -0.2132618534148182, 0.12273053965522068, -0.2568034136317449, -0.13214681218931507, 0.12971397766919512, -0.09889824834126647,... |
707.3836 | The charge and spin sectors of the $t$-$t'$ Hubbard model | The charge and spin sectors, which are intimately coupled to the fermionic
one, of the $t$-$t'$ Hubbard model have been computed self-consistently within
the two-pole approximation. The relevant unknown correlators appearing in the
causal bosonic propagators have been computed by enforcing the constraints
dictated by... | cond-mat.str-el | the charge and spin sectors which are intimately coupled to the fermionic one of the tt hubbard model have been computed selfconsistently within the twopole approximation the relevant unknown correlators appearing in the causal bosonic propagators have been computed by enforcing the constraints dictated by the hydrodyn... | [['the', 'charge', 'and', 'spin', 'sectors', 'which', 'are', 'intimately', 'coupled', 'to', 'the', 'fermionic', 'one', 'of', 'the', 'tt', 'hubbard', 'model', 'have', 'been', 'computed', 'selfconsistently', 'within', 'the', 'twopole', 'approximation', 'the', 'relevant', 'unknown', 'correlators', 'appearing', 'in', 'the'... | [-0.10483084621847849, 0.15945746489214124, -0.061494810282494185, 0.08935459530739873, -0.035291225427365, -0.14929592962963162, 0.018997641642474465, 0.2965212165533255, -0.23992882586187786, -0.2744435029733857, 0.049313411055158615, -0.2954308755557846, -0.08085433612750084, 0.10251405203921928, 0.08346311918312158... |
707.3837 | Effective resistance on random electrical networks | This paper has been withdrawn. See v1 still available to understand the
problem: Proposition 2.2 is false. The error in the proof is in claim (3).
Then, the whole paper collapses. We do not have any correction for now. We
apologize to everyone.
| math.PR math-ph math.MP | this paper has been withdrawn see v1 still available to understand the problem proposition 22 is false the error in the proof is in claim 3 then the whole paper collapses we do not have any correction for now we apologize to everyone | [['this', 'paper', 'has', 'been', 'withdrawn', 'see', 'v1', 'still', 'available', 'to', 'understand', 'the', 'problem', 'proposition', '22', 'is', 'false', 'the', 'error', 'in', 'the', 'proof', 'is', 'in', 'claim', '3', 'then', 'the', 'whole', 'paper', 'collapses', 'we', 'do', 'not', 'have', 'any', 'correction', 'for',... | [-0.0809021012554335, 0.01603969552575849, -0.10695009787437008, 0.082997077937931, -0.11154224824831756, -0.16587841246536997, 0.045046191895380616, 0.3820925095053606, -0.23494733415197494, -0.32514243433251977, 0.1546069692636212, -0.2918504709161298, -0.153698934198812, 0.10994125719907759, -0.22134807887811994, 0.... |
707.3838 | Ergodicity in Strongly Correlated Systems | We present a concise, but systematic, review of the ergodicity issue in
strongly correlated systems. After giving a brief historical overview, we
analyze the issue within the Green's function formalism by means of the
equations of motion approach. By means of this analysis, we are able to
individuate the primary sour... | cond-mat.str-el cond-mat.soft | we present a concise but systematic review of the ergodicity issue in strongly correlated systems after giving a brief historical overview we analyze the issue within the greens function formalism by means of the equations of motion approach by means of this analysis we are able to individuate the primary source of non... | [['we', 'present', 'a', 'concise', 'but', 'systematic', 'review', 'of', 'the', 'ergodicity', 'issue', 'in', 'strongly', 'correlated', 'systems', 'after', 'giving', 'a', 'brief', 'historical', 'overview', 'we', 'analyze', 'the', 'issue', 'within', 'the', 'greens', 'function', 'formalism', 'by', 'means', 'of', 'the', 'eq... | [-0.12056663898616343, 0.10731117833209665, -0.11841440754697512, 0.1014373763856527, -0.058654559969804, -0.1231386626531419, 0.05499664540157506, 0.3526937667966673, -0.2687696879631595, -0.2678955646918008, 0.10151973385731444, -0.26246246281815205, -0.23139754274222804, 0.1887664534151554, -0.05031410065773678, 0.0... |
707.3839 | A class of solvable models in Condensed Matter Physics | In this paper, we show that there is a large class of fermionic systems for
which it is possible to find, for any dimension, a finite closed set of
eigenoperators and eigenvalues of the Hamiltonian. Then, the hierarchy of the
equations of motion closes and analytical expressions for the Green's functions
are obtained... | cond-mat.str-el | in this paper we show that there is a large class of fermionic systems for which it is possible to find for any dimension a finite closed set of eigenoperators and eigenvalues of the hamiltonian then the hierarchy of the equations of motion closes and analytical expressions for the greens functions are obtained in term... | [['in', 'this', 'paper', 'we', 'show', 'that', 'there', 'is', 'a', 'large', 'class', 'of', 'fermionic', 'systems', 'for', 'which', 'it', 'is', 'possible', 'to', 'find', 'for', 'any', 'dimension', 'a', 'finite', 'closed', 'set', 'of', 'eigenoperators', 'and', 'eigenvalues', 'of', 'the', 'hamiltonian', 'then', 'the', 'hi... | [-0.12096112457063124, 0.09172863821994078, -0.05743423112676487, 0.06551440079331498, -0.08027643795536311, -0.09273410503341405, 0.031367228979974786, 0.3137465650299648, -0.2586391217784268, -0.28516272103900575, 0.09793256863171386, -0.25110911173527845, -0.1529017586202302, 0.24156749638024014, -0.0066018766463474... |
707.384 | Green's Function Formalism for Highly Correlated Systems | We present the Composite Operator Method (COM) as a modern approach to the
study of strongly correlated electronic systems, based on the equation of
motion and Green's function method. COM uses propagators of composite operators
as building blocks at the basis of approximate calculations and algebra
constrains to fix... | cond-mat.str-el | we present the composite operator method com as a modern approach to the study of strongly correlated electronic systems based on the equation of motion and greens function method com uses propagators of composite operators as building blocks at the basis of approximate calculations and algebra constrains to fix the re... | [['we', 'present', 'the', 'composite', 'operator', 'method', 'com', 'as', 'a', 'modern', 'approach', 'to', 'the', 'study', 'of', 'strongly', 'correlated', 'electronic', 'systems', 'based', 'on', 'the', 'equation', 'of', 'motion', 'and', 'greens', 'function', 'method', 'com', 'uses', 'propagators', 'of', 'composite', 'o... | [-0.09837246869528105, 0.04367380989863286, -0.1554522152236175, 0.0454085470354628, -0.09298800502992458, -0.07555058683520036, 0.016575454519913782, 0.33815455141048584, -0.2681295777715388, -0.29446999888334957, 0.09147175543180239, -0.2794845564261315, -0.18164847885805463, 0.14933818106776073, 0.023711114929663758... |
707.3841 | Poynting's theorem for planes waves at an interface: a scattering matrix
approach | We apply the Poynting theorem to the scattering of monochromatic
electromagnetic planes waves with normal incidence to the interface of two
different media. We write this energy conservation theorem to introduce a
natural definition of the scattering matrix S. For the dielectric-dielectric
interface the balance equat... | physics.class-ph | we apply the poynting theorem to the scattering of monochromatic electromagnetic planes waves with normal incidence to the interface of two different media we write this energy conservation theorem to introduce a natural definition of the scattering matrix s for the dielectricdielectric interface the balance equation l... | [['we', 'apply', 'the', 'poynting', 'theorem', 'to', 'the', 'scattering', 'of', 'monochromatic', 'electromagnetic', 'planes', 'waves', 'with', 'normal', 'incidence', 'to', 'the', 'interface', 'of', 'two', 'different', 'media', 'we', 'write', 'this', 'energy', 'conservation', 'theorem', 'to', 'introduce', 'a', 'natural'... | [-0.16724800613862922, 0.13669289279283142, -0.07688379411841414, 0.07538530682082432, -0.07881366614494997, -0.11754827600129893, 0.014664326082836365, 0.30846648855039743, -0.28477390897525867, -0.275012725764151, 0.06356273558807336, -0.27804167055144485, -0.08193204204328883, 0.16586625421727993, -0.025663603789133... |
707.3842 | Quenched Dislocation Enhanced Supersolid Ordering | I show using Landau theory that quenched dislocations can facilitate the
supersolid (SS) to normal solid (NS) transition, making it possible for the
transition to occur even if it does not in a dislocation-free crystal. I make
detailed predictions for the dependence of the SS to NS transition temperature
T_c(L), supe... | cond-mat.other cond-mat.stat-mech | i show using landau theory that quenched dislocations can facilitate the supersolid ss to normal solid ns transition making it possible for the transition to occur even if it does not in a dislocationfree crystal i make detailed predictions for the dependence of the ss to ns transition temperature t_cl superfluid densi... | [['i', 'show', 'using', 'landau', 'theory', 'that', 'quenched', 'dislocations', 'can', 'facilitate', 'the', 'supersolid', 'ss', 'to', 'normal', 'solid', 'ns', 'transition', 'making', 'it', 'possible', 'for', 'the', 'transition', 'to', 'occur', 'even', 'if', 'it', 'does', 'not', 'in', 'a', 'dislocationfree', 'crystal', ... | [-0.09725799787726798, 0.22039807181994384, -0.07390372712541832, 0.0534282402669111, -0.08434839560807253, -0.1914121086102272, 0.0962404233934567, 0.39908225641826567, -0.2512818761693125, -0.2617759202408154, 0.07772655225636207, -0.26508980673434357, -0.07562775381976801, 0.18683379061854957, 0.021789703507687937, ... |
707.3843 | Modulator noise suppression in the LISA Time-Delay Interferometric
combinations | We previously showed how the measurements of some eighteen time series of
relative frequency or phase shifts could be combined (1) to cancel the phase
noise of the lasers, (2) to cancel the Doppler fluctuations due to non-inertial
motions of the six optical benches, and (3) to remove the phase noise of the
onboard re... | gr-qc | we previously showed how the measurements of some eighteen time series of relative frequency or phase shifts could be combined 1 to cancel the phase noise of the lasers 2 to cancel the doppler fluctuations due to noninertial motions of the six optical benches and 3 to remove the phase noise of the onboard reference osc... | [['we', 'previously', 'showed', 'how', 'the', 'measurements', 'of', 'some', 'eighteen', 'time', 'series', 'of', 'relative', 'frequency', 'or', 'phase', 'shifts', 'could', 'be', 'combined', '1', 'to', 'cancel', 'the', 'phase', 'noise', 'of', 'the', 'lasers', '2', 'to', 'cancel', 'the', 'doppler', 'fluctuations', 'due', ... | [-0.17817748260986088, 0.19071847054655539, -0.027571606027070903, 0.021973671576966648, -0.04788841176054721, -0.13975624488304975, 0.05063548100404713, 0.4122246775450637, -0.228643109696438, -0.3230704947790692, 0.09749098900972314, -0.28657770167936764, -0.1198195746921238, 0.24178741038076182, -0.08522170714048434... |
707.3844 | Nucleon Structure and Hyperon Form factor from Lattice QCD | In this work, I report the latest lattice QCD calculations of nucleon and
hyperon structure from chiral fermions in 2+1-flavor dynamical simulations. All
calculations are done with a chirally symmetric fermion action, domain-wall
fermions, for valence quarks. % I begin with the latest lattice results on the
nucleon s... | hep-lat | in this work i report the latest lattice qcd calculations of nucleon and hyperon structure from chiral fermions in 21flavor dynamical simulations all calculations are done with a chirally symmetric fermion action domainwall fermions for valence quarks i begin with the latest lattice results on the nucleon structure foc... | [['in', 'this', 'work', 'i', 'report', 'the', 'latest', 'lattice', 'qcd', 'calculations', 'of', 'nucleon', 'and', 'hyperon', 'structure', 'from', 'chiral', 'fermions', 'in', '21flavor', 'dynamical', 'simulations', 'all', 'calculations', 'are', 'done', 'with', 'a', 'chirally', 'symmetric', 'fermion', 'action', 'domainwa... | [-0.08003473073858108, 0.24633025291301897, -0.08487105785675379, 0.04764520202143184, -0.06087310907463914, -0.06722986360700735, 0.06100906719313522, 0.4025710781714755, -0.15515875495121345, -0.2366201602482954, 0.018657440679720645, -0.32311516088656095, -0.05691863247811531, 0.08844958150355492, 0.1063677013436521... |
707.3845 | Modules of constant Jordan type | We introduce the class of modules of constant Jordan type for a finite group
scheme $G$ over a field $k$ of characteristic $p > 0$. This class is closed
under taking direct sums, tensor products, duals, Heller shifts and direct
summands, and includes endotrivial modules. It contains all modules in an
Auslander-Reiten... | math.RT | we introduce the class of modules of constant jordan type for a finite group scheme g over a field k of characteristic p 0 this class is closed under taking direct sums tensor products duals heller shifts and direct summands and includes endotrivial modules it contains all modules in an auslanderreiten component which ... | [['we', 'introduce', 'the', 'class', 'of', 'modules', 'of', 'constant', 'jordan', 'type', 'for', 'a', 'finite', 'group', 'scheme', 'g', 'over', 'a', 'field', 'k', 'of', 'characteristic', 'p', '0', 'this', 'class', 'is', 'closed', 'under', 'taking', 'direct', 'sums', 'tensor', 'products', 'duals', 'heller', 'shifts', 'a... | [-0.2110303346800836, 0.070978624159947, -0.0606188445916756, 0.007157151617030514, -0.112615020224884, -0.19097813207933562, -0.03486029850319028, 0.38603619216604435, -0.3291458086447513, -0.17018203795986606, 0.09256545442374463, -0.2028974231600048, -0.13034630546524645, 0.221280712287556, -0.07054736664360191, -0.... |
707.3846 | Quantum statistical measurements of an atom laser beam | We describe a scheme, operating in a manner analogous to a reversed Raman
output coupler, for measuring the phase-sensitive quadrature statistics of an
atom laser beam. This scheme allows for the transferral of the atomic field
statistics to an optical field, for which the quantum statistics may then be
measured usin... | physics.atom-ph physics.optics | we describe a scheme operating in a manner analogous to a reversed raman output coupler for measuring the phasesensitive quadrature statistics of an atom laser beam this scheme allows for the transferral of the atomic field statistics to an optical field for which the quantum statistics may then be measured using the w... | [['we', 'describe', 'a', 'scheme', 'operating', 'in', 'a', 'manner', 'analogous', 'to', 'a', 'reversed', 'raman', 'output', 'coupler', 'for', 'measuring', 'the', 'phasesensitive', 'quadrature', 'statistics', 'of', 'an', 'atom', 'laser', 'beam', 'this', 'scheme', 'allows', 'for', 'the', 'transferral', 'of', 'the', 'atom... | [-0.12782104653788023, 0.16366521794206446, -0.13072966973714786, -0.008137365604413608, -0.00555244932786144, -0.18347841614439828, 0.07517587075186573, 0.4435500195571061, -0.2707492182480878, -0.23787123756483197, 0.023436960537420136, -0.20009788000933096, -0.07037546846851032, 0.30381761992285994, -0.0354677967181... |
707.3847 | Aspects of Density Fluctuations in Compressible MHD Turbulence | We study scaling relations of compressible isothermal strongly magnetized
turbulence using numerical simulations with resolution 512$^3$. We find a good
correspondence of our results with the Fleck (1996) model of compressible
hydrodynamic turbulence. In particular, we find that the density-weighted
velocity, i.e. $\... | astro-ph | we study scaling relations of compressible isothermal strongly magnetized turbulence using numerical simulations with resolution 5123 we find a good correspondence of our results with the fleck 1996 model of compressible hydrodynamic turbulence in particular we find that the densityweighted velocity ie boldsymbolu equi... | [['we', 'study', 'scaling', 'relations', 'of', 'compressible', 'isothermal', 'strongly', 'magnetized', 'turbulence', 'using', 'numerical', 'simulations', 'with', 'resolution', '5123', 'we', 'find', 'a', 'good', 'correspondence', 'of', 'our', 'results', 'with', 'the', 'fleck', '1996', 'model', 'of', 'compressible', 'hyd... | [-0.14149743824279593, 0.16362928132562396, -0.075097476684265, 0.06474226443634297, -0.03809718946964223, -0.08573989294220723, -0.022715228894194462, 0.31466289593077507, -0.23772579033298594, -0.3217353417087195, 0.0355209434527179, -0.2594139056271827, -0.07602776263153593, 0.16930618722990526, 0.003616281529062541... |
707.3848 | Correlation Inequalities for Generalized Potts Model: General Griffiths'
Inequalities | In this paper, correlation inequalities which have been considered on Ising
model are extended to q-Potts model. It is considered on generalized Potts
model with interaction of any number of spins. We replace the set of spin
values $F=\{1,2,..., q\}$ by the centered set $F=\{-(q-1)/2,-(q-3)/2,...
,(q-3)/2,(q-1)/2\}$.... | math-ph math.MP math.PR | in this paper correlation inequalities which have been considered on ising model are extended to qpotts model it is considered on generalized potts model with interaction of any number of spins we replace the set of spin values f12 q by the centered set fq12q32 q32q12 let n be the subset of onedimensional lattice with ... | [['in', 'this', 'paper', 'correlation', 'inequalities', 'which', 'have', 'been', 'considered', 'on', 'ising', 'model', 'are', 'extended', 'to', 'qpotts', 'model', 'it', 'is', 'considered', 'on', 'generalized', 'potts', 'model', 'with', 'interaction', 'of', 'any', 'number', 'of', 'spins', 'we', 'replace', 'the', 'set', ... | [-0.13682224782597688, 0.15301199598673967, -0.011810855448452963, -0.03024066705811059, -0.016206204710114334, -0.23577147965422934, 0.02012656212946962, 0.38202080090663265, -0.2530234125110188, -0.24678192408164107, 0.07325794938711509, -0.3134460040102048, -0.09068607691017586, 0.1110997972030577, 0.009525408931372... |
707.3849 | The phase structure of a chirally invariant lattice Higgs-Yukawa model -
numerical simulations | The phase diagram of a chirally invariant lattice Higgs-Yukawa model is
explored by means of numerical simulations. The results revealing a rich phase
structure are compared to analytical large Nf calculations which we performed
earlier. The analytical and numerical results are in excellent agreement at
large values ... | hep-lat | the phase diagram of a chirally invariant lattice higgsyukawa model is explored by means of numerical simulations the results revealing a rich phase structure are compared to analytical large nf calculations which we performed earlier the analytical and numerical results are in excellent agreement at large values of nf... | [['the', 'phase', 'diagram', 'of', 'a', 'chirally', 'invariant', 'lattice', 'higgsyukawa', 'model', 'is', 'explored', 'by', 'means', 'of', 'numerical', 'simulations', 'the', 'results', 'revealing', 'a', 'rich', 'phase', 'structure', 'are', 'compared', 'to', 'analytical', 'large', 'nf', 'calculations', 'which', 'we', 'p... | [-0.18426866527668415, 0.16023796965343368, -0.07972164431059386, 0.07303015268984688, -0.03978252669680962, -0.13372980937180398, 0.08618230363601341, 0.36305945173763066, -0.15963682445359573, -0.29103550647871684, 0.07052609071123159, -0.2731458383686511, -0.12626164792253908, 0.14236060447941443, 0.0714549846224490... |
707.385 | Spin wave dispersion based on the quasiparticle self-consistent $GW$
method: NiO, MnO and $\alpha$-MnAs | We present spin wave dispersions in MnO, NiO, and $\alpha$-MnAs based on the
quasiparticle self-consistent $GW$ method (\qsgw), which determines an optimum
quasiparticle picture. For MnO and NiO, \qsgw results are in rather good
agreement with experiments, in contrast to the LDA and LDA+U description. For
$\alpha$-Mn... | cond-mat.mtrl-sci cond-mat.other | we present spin wave dispersions in mno nio and alphamnas based on the quasiparticle selfconsistent gw method qsgw which determines an optimum quasiparticle picture for mno and nio qsgw results are in rather good agreement with experiments in contrast to the lda and ldau description for alphamnas we find a collinear fe... | [['we', 'present', 'spin', 'wave', 'dispersions', 'in', 'mno', 'nio', 'and', 'alphamnas', 'based', 'on', 'the', 'quasiparticle', 'selfconsistent', 'gw', 'method', 'qsgw', 'which', 'determines', 'an', 'optimum', 'quasiparticle', 'picture', 'for', 'mno', 'and', 'nio', 'qsgw', 'results', 'are', 'in', 'rather', 'good', 'ag... | [-0.11758704454968533, 0.07794861423603687, -0.09579063997033142, 0.12500983844661423, -0.010933721453071601, -0.08750623316624231, 0.14527136859138526, 0.4817128335876811, -0.18669214406925735, -0.254962032029946, -0.09524945341118221, -0.3890942050925186, -0.12001392095079345, 0.11863295854099336, 0.09474100765862292... |
707.3851 | The complex Busemann-Petty problem on sections of convex bodies | The complex Busemann-Petty problem asks whether origin symmetric convex
bodies in $\C^n$ with smaller central hyperplane sections necessarily have
smaller volume. We prove that the answer is affirmative if $n\le 3$ and
negative if $n\ge 4.$
| math.FA math.MG | the complex busemannpetty problem asks whether origin symmetric convex bodies in cn with smaller central hyperplane sections necessarily have smaller volume we prove that the answer is affirmative if nle 3 and negative if nge 4 | [['the', 'complex', 'busemannpetty', 'problem', 'asks', 'whether', 'origin', 'symmetric', 'convex', 'bodies', 'in', 'cn', 'with', 'smaller', 'central', 'hyperplane', 'sections', 'necessarily', 'have', 'smaller', 'volume', 'we', 'prove', 'that', 'the', 'answer', 'is', 'affirmative', 'if', 'nle', '3', 'and', 'negative', ... | [-0.12311141745885834, 0.09383855035735501, 0.01601833700098925, 0.11184562977804388, -0.057407766270140805, -0.26703565578079885, -0.07161171863683397, 0.37474265441091525, -0.2347117822048151, -0.22625827406429583, 0.10969621990483978, -0.3212059285077784, -0.14357696633992922, 0.11424273214328827, -0.121304593721611... |
707.3852 | Performance Evaluation of a Multi-Agent Risk-Sensitive Tracking System | In this paper, we consider a simple linear exponential quadratic Gaussian
(LEQG) tracking problem for a multi-agent system. We study the dynamical
behaviors of the group as we vary the risk-sensitivity parameter, comparing in
particular the risk averse case to the LQG case. Then we consider the evolution
of the perfo... | math.OC | in this paper we consider a simple linear exponential quadratic gaussian leqg tracking problem for a multiagent system we study the dynamical behaviors of the group as we vary the risksensitivity parameter comparing in particular the risk averse case to the lqg case then we consider the evolution of the performance per... | [['in', 'this', 'paper', 'we', 'consider', 'a', 'simple', 'linear', 'exponential', 'quadratic', 'gaussian', 'leqg', 'tracking', 'problem', 'for', 'a', 'multiagent', 'system', 'we', 'study', 'the', 'dynamical', 'behaviors', 'of', 'the', 'group', 'as', 'we', 'vary', 'the', 'risksensitivity', 'parameter', 'comparing', 'in... | [-0.1620415286689352, 0.11777919066281846, -0.022344180635319878, 0.056130765839658966, -0.06856061400165064, -0.1568213732026589, 0.08339676703595054, 0.35530384875511606, -0.2772807399384104, -0.29068832652858245, 0.11637237365984429, -0.28659136488388937, -0.1484863737356276, 0.16432385762051965, -0.1007228912105067... |
707.3853 | Semifinite spectral triples associated with graph C*-algebras | We review the recent construction of semifinite spectral triples for graph
C^*-algebras. These examples have inspired many other developments and we
review some of these such as the relation between the semifinite index and the
Kasparov product, examples of noncommutative manifolds, and an index theorem in
twisted cy... | math.OA | we review the recent construction of semifinite spectral triples for graph calgebras these examples have inspired many other developments and we review some of these such as the relation between the semifinite index and the kasparov product examples of noncommutative manifolds and an index theorem in twisted cyclic the... | [['we', 'review', 'the', 'recent', 'construction', 'of', 'semifinite', 'spectral', 'triples', 'for', 'graph', 'calgebras', 'these', 'examples', 'have', 'inspired', 'many', 'other', 'developments', 'and', 'we', 'review', 'some', 'of', 'these', 'such', 'as', 'the', 'relation', 'between', 'the', 'semifinite', 'index', 'an... | [-0.09973088937442538, 0.10805362599428506, -0.07195047833868917, 0.07017124503991513, -0.08581822477983979, -0.106115380504151, -0.020145295919270587, 0.4155124705284834, -0.3024540225852211, -0.28778700017423, 0.144736701787344, -0.2838788508033415, -0.18054725289485365, 0.23000057923765677, -0.19468965406863475, 0.0... |
707.3854 | eta photoproduction and N* resonances | We investigate the eta photoproduction using the effective Lagrangian
approach at the tree level. We focus on the new nucleon resonance N*(1675),
which was reported by the GRAAL, CB-ELSA and Tohoku LNS, testing its possible
spin and parity states theoretically (J^P=1/2^+-,3/2^+-). In addition, we
include six nucleon ... | hep-ph | we investigate the eta photoproduction using the effective lagrangian approach at the tree level we focus on the new nucleon resonance n1675 which was reported by the graal cbelsa and tohoku lns testing its possible spin and parity states theoretically jp1232 in addition we include six nucleon resonances d_131520 s_111... | [['we', 'investigate', 'the', 'eta', 'photoproduction', 'using', 'the', 'effective', 'lagrangian', 'approach', 'at', 'the', 'tree', 'level', 'we', 'focus', 'on', 'the', 'new', 'nucleon', 'resonance', 'n1675', 'which', 'was', 'reported', 'by', 'the', 'graal', 'cbelsa', 'and', 'tohoku', 'lns', 'testing', 'its', 'possible... | [-0.08392443557739884, 0.2160841154422019, -0.06648951318092149, 0.16851847489891034, -0.04381049265127594, -0.09047817163959268, 0.07066293398492804, 0.32785054566077537, -0.13217899831725616, -0.27645294872225723, -0.047539390294995404, -0.3502372967549295, -0.061754498569834455, 0.13845403087717073, 0.09528906182951... |
707.3855 | Special Relativity and Theory of Gravity via Maximum Symmetry and
Localization -- In Honor of the 80th Birthday of Professor Qikeng Lu | Like Euclid, Riemann and Lobachevsky geometries on an almost equal footing,
based on the principle of relativity of maximum symmetry proposed by Lu and the
postulate on invariant universal constants, dS/AdS SR can be set up on an
almost equal footing with Einstein's SR. For dS-case, there is a coin-like
relation: A l... | gr-qc | like euclid riemann and lobachevsky geometries on an almost equal footing based on the principle of relativity of maximum symmetry proposed by lu and the postulate on invariant universal constants dsads sr can be set up on an almost equal footing with einsteins sr for dscase there is a coinlike relation a law of inerti... | [['like', 'euclid', 'riemann', 'and', 'lobachevsky', 'geometries', 'on', 'an', 'almost', 'equal', 'footing', 'based', 'on', 'the', 'principle', 'of', 'relativity', 'of', 'maximum', 'symmetry', 'proposed', 'by', 'lu', 'and', 'the', 'postulate', 'on', 'invariant', 'universal', 'constants', 'dsads', 'sr', 'can', 'be', 'se... | [-0.12995480706237933, 0.13416304695241377, -0.14010340508750893, 0.06118688137767921, -0.09238017180435815, -0.14630803475685586, 0.006036904192825949, 0.29682312115857545, -0.22256542903963816, -0.264329245778605, 0.10222664422630756, -0.27147043876519256, -0.09249753709882498, 0.18618011414232155, -0.068909650274806... |
707.3856 | Stochastic evolution equations for nonlinear filtering of random fields
in the presence of fractional Brownian sheet observation noise | The problem of nonlinear filtering of a random field observed in the presence
of a noise, modeled by a persistent fractional Brownian sheet of Hurst index
$(H_1,H_2)$ with $0.5<H_1,H_2<1$, is studied and a suitable version of the
Bayes' formula for the optimal filter is obtained. Two types of spatial
"fractional" ana... | math.PR | the problem of nonlinear filtering of a random field observed in the presence of a noise modeled by a persistent fractional brownian sheet of hurst index h_1h_2 with 05h_1h_21 is studied and a suitable version of the bayes formula for the optimal filter is obtained two types of spatial fractional analogues of the dunca... | [['the', 'problem', 'of', 'nonlinear', 'filtering', 'of', 'a', 'random', 'field', 'observed', 'in', 'the', 'presence', 'of', 'a', 'noise', 'modeled', 'by', 'a', 'persistent', 'fractional', 'brownian', 'sheet', 'of', 'hurst', 'index', 'h_1h_2', 'with', '05h_1h_21', 'is', 'studied', 'and', 'a', 'suitable', 'version', 'of... | [-0.14449874142642818, 0.11522485626092246, -0.04799900504121603, 0.0384548525999431, -0.043457550939541956, -0.12779862776952833, -0.015966974694304907, 0.372216299053066, -0.2795535553677762, -0.26606294174085965, 0.11629165725567, -0.2767038672531316, -0.1632615421506122, 0.18597674739647133, -0.05941284069221867, 0... |
707.3857 | Exact solution of a model of qubit dephasing due to telegraph noise | We present a general and exact formalism for finding the evolution of a
quantum system subject to external telegraph noise. The various qubit
decoherence rates are determined by the eigenvalues of a transfer matrix. The
formalism can be applied to a qubit subject to an arbitrary combination of
dephasing and relaxatio... | quant-ph | we present a general and exact formalism for finding the evolution of a quantum system subject to external telegraph noise the various qubit decoherence rates are determined by the eigenvalues of a transfer matrix the formalism can be applied to a qubit subject to an arbitrary combination of dephasing and relaxational ... | [['we', 'present', 'a', 'general', 'and', 'exact', 'formalism', 'for', 'finding', 'the', 'evolution', 'of', 'a', 'quantum', 'system', 'subject', 'to', 'external', 'telegraph', 'noise', 'the', 'various', 'qubit', 'decoherence', 'rates', 'are', 'determined', 'by', 'the', 'eigenvalues', 'of', 'a', 'transfer', 'matrix', 't... | [-0.14945117837524993, 0.1243671202659637, -0.052891033013908136, 0.08834685821664645, 0.00667371176010401, -0.16324296359635276, 0.035480387193827706, 0.36301093166406007, -0.2524524941301146, -0.2705952160866912, 0.08929381883143898, -0.2714643389437847, -0.15726262515953252, 0.2229236727040357, -0.05078952124860791,... |
707.3858 | The quantum sinh-Gordon model in noncommutative (1+1) dimensions | Using twisted commutation relations we show that the quantum sinh-Gordon
model on noncommutative space is integrable, and compute the exact two-particle
scattering matrix. The model possesses a strong-weak duality, just like its
commutative counterpart.
| hep-th | using twisted commutation relations we show that the quantum sinhgordon model on noncommutative space is integrable and compute the exact twoparticle scattering matrix the model possesses a strongweak duality just like its commutative counterpart | [['using', 'twisted', 'commutation', 'relations', 'we', 'show', 'that', 'the', 'quantum', 'sinhgordon', 'model', 'on', 'noncommutative', 'space', 'is', 'integrable', 'and', 'compute', 'the', 'exact', 'twoparticle', 'scattering', 'matrix', 'the', 'model', 'possesses', 'a', 'strongweak', 'duality', 'just', 'like', 'its',... | [-0.1331323002848555, 0.10422837671221179, -0.11608703571426518, 0.2178075549309142, -0.11898402157513534, -0.2076190377256888, -0.04926658195087358, 0.34781710217323375, -0.3153170393505955, -0.14954243616803603, 0.06564136355540112, -0.3090189588804017, -0.23412646408028462, 0.16572998939355946, -0.010044260553139098... |
707.3859 | Light-Front Dynamics and AdS/QCD Correspondence: The Pion Form Factor in
the Space- and Time-Like Regions | The AdS/CFT correspondence between string theory in AdS space and conformal
field theories in physical space-time leads to an analytic, semi-classical
model for strongly-coupled QCD which has scale invariance and dimensional
counting at short distances and color confinement at large distances. The
AdS/CFT corresponde... | hep-ph hep-th | the adscft correspondence between string theory in ads space and conformal field theories in physical spacetime leads to an analytic semiclassical model for stronglycoupled qcd which has scale invariance and dimensional counting at short distances and color confinement at large distances the adscft correspondence also ... | [['the', 'adscft', 'correspondence', 'between', 'string', 'theory', 'in', 'ads', 'space', 'and', 'conformal', 'field', 'theories', 'in', 'physical', 'spacetime', 'leads', 'to', 'an', 'analytic', 'semiclassical', 'model', 'for', 'stronglycoupled', 'qcd', 'which', 'has', 'scale', 'invariance', 'and', 'dimensional', 'coun... | [-0.1171166099190155, 0.20164487934053907, -0.15157003928776655, 0.14023157648272186, -0.08581729524765624, -0.09652624309833258, 0.0070231299772292866, 0.3107418812741743, -0.18895055156932256, -0.21051222795324626, -0.019904858622021068, -0.27432545579467504, -0.08475401694114591, 0.09447749912908528, 0.0657929818867... |
707.386 | Cha\^{i}nes de Markov Constructives Index\'{e}es par Z | Nous \'{e}tudions les cha\^{{\i}}nes de Markov $(X_n)_{n\in\mathbf{Z}}$
gouvern\'{e}es par une relation de r\'{e}currence de la forme
$X_{n+1}=f(X_n,V_{n+1})$, o\`{u} $(V_n)_{n\in\mathbf{Z}}$ est une suite de
variables al\'{e}atoires ind\'{e}pendantes et de m\^{e}me loi telle pour tout
$n\in \mathbf{Z}$, $V_{n+1}$ es... | math.PR | nous etudions les chaines de markov x_n_ninmathbfz gouvernees par une relation de recurrence de la forme x_n1fx_nv_n1 ou v_n_ninmathbfz est une suite de variables aleatoires independantes et de meme loi telle pour tout nin mathbfz v_n1 est independante de la suite x_kv_k_kle n lobjet de larticle est de donner une condi... | [['nous', 'etudions', 'les', 'chaines', 'de', 'markov', 'x_n_ninmathbfz', 'gouvernees', 'par', 'une', 'relation', 'de', 'recurrence', 'de', 'la', 'forme', 'x_n1fx_nv_n1', 'ou', 'v_n_ninmathbfz', 'est', 'une', 'suite', 'de', 'variables', 'aleatoires', 'independantes', 'et', 'de', 'meme', 'loi', 'telle', 'pour', 'tout', ... | [-0.26226588457939215, -0.024690979491424514, -0.25148019921107334, 0.054805791362014133, -0.1650657126083388, -0.16108431835164083, -0.3671762817830313, -0.095660913071697, -0.07548902530470514, -0.2856319567490573, -0.013954478687082883, -0.3839437759015709, -0.2543867697895621, 0.13342116952753713, -0.43881810813036... |
707.3861 | The C*-algebras qA\otimes K and S^2A\otimes K are asymptotically
equivalent | Let $A$ be a separable $C^*$-algebra. We prove that its stabilized second
suspension $S^2A\otimes \mathcal K$ and the $C^*$-algebra $qA\otimes \mathcal
K$ constructed by Cuntz in the framework of his picture of KK-theory are
asymptotically equivalent. This means that there exist asymptotic morphisms
from each to the ... | math.OA math.KT | let a be a separable calgebra we prove that its stabilized second suspension s2aotimes mathcal k and the calgebra qaotimes mathcal k constructed by cuntz in the framework of his picture of kktheory are asymptotically equivalent this means that there exist asymptotic morphisms from each to the other whose compositions a... | [['let', 'a', 'be', 'a', 'separable', 'calgebra', 'we', 'prove', 'that', 'its', 'stabilized', 'second', 'suspension', 's2aotimes', 'mathcal', 'k', 'and', 'the', 'calgebra', 'qaotimes', 'mathcal', 'k', 'constructed', 'by', 'cuntz', 'in', 'the', 'framework', 'of', 'his', 'picture', 'of', 'kktheory', 'are', 'asymptoticall... | [-0.11429063314311574, 0.13338539897979404, -0.13984483367714443, 0.03373079639124243, -0.058520487468820395, -0.21401083049070285, 0.004663482764858361, 0.36436513751712546, -0.3772682719169544, -0.17140212617896236, 0.06693321824882571, -0.26140862551370736, -0.1137061375111603, 0.16386197852746895, -0.18051986303180... |
707.3862 | Rational Landen transformations on the real line | The rational Landen transformation is a map on the space of coefficients of a
rational integrand that preserves the value of the integral. We provide a
family of these transformations that apply to rational integrands on the whole
line. Given an integer m, these transformations produce a numerical scheme to
evaluate ... | math.CA | the rational landen transformation is a map on the space of coefficients of a rational integrand that preserves the value of the integral we provide a family of these transformations that apply to rational integrands on the whole line given an integer m these transformations produce a numerical scheme to evaluate the i... | [['the', 'rational', 'landen', 'transformation', 'is', 'a', 'map', 'on', 'the', 'space', 'of', 'coefficients', 'of', 'a', 'rational', 'integrand', 'that', 'preserves', 'the', 'value', 'of', 'the', 'integral', 'we', 'provide', 'a', 'family', 'of', 'these', 'transformations', 'that', 'apply', 'to', 'rational', 'integrand... | [-0.18954511683691164, 0.03462526057109212, -0.1294682322226561, 0.0318286789235948, -0.1226172392930964, -0.07374204785145562, 0.04894973090368098, 0.35868094129295186, -0.28823342598203955, -0.2134778098893705, 0.11394173614199049, -0.26179577609331445, -0.20821683340031524, 0.21430937967520078, -0.06079564205017583,... |
707.3863 | The Jancovici - Lebowitz - Manificat law for large fluctuations of
random complex zeroes | By random complex zeroes we mean the zero set of a random entire function
whose Taylor coefficients are independent complex-valued Gaussian variables,
and the variance of the k-th coefficient is 1/k!. This zero set is distribution
invariant with respect to isometries of the complex plane. We study large
fluctuations ... | math.PR math-ph math.CV math.MP | by random complex zeroes we mean the zero set of a random entire function whose taylor coefficients are independent complexvalued gaussian variables and the variance of the kth coefficient is 1k this zero set is distribution invariant with respect to isometries of the complex plane we study large fluctuations of random... | [['by', 'random', 'complex', 'zeroes', 'we', 'mean', 'the', 'zero', 'set', 'of', 'a', 'random', 'entire', 'function', 'whose', 'taylor', 'coefficients', 'are', 'independent', 'complexvalued', 'gaussian', 'variables', 'and', 'the', 'variance', 'of', 'the', 'kth', 'coefficient', 'is', '1k', 'this', 'zero', 'set', 'is', '... | [-0.18619723637821153, 0.2001074699102901, -0.10162294236652088, 0.04943975745263742, -0.06047771429875866, -0.0867265887442045, 0.02791755343787372, 0.297730911988765, -0.257830690976698, -0.22379141417113715, 0.07620342494774376, -0.3379298781044781, -0.17836597457062453, 0.13172880564816297, -0.0282060896162875, 0.1... |
707.3864 | The equation of state for the nuclear matter and the properties of the
neutron star | The equation of state for the beta stable nuclear matter is calculated
numerically, and then the Tolman-Oppenheimer-Volkov equation for the structure
of the neutron star is solved in the fourth-order Runge-Kutta algorithm. It
shows the mass and radius of the neutron star are functions of the central
density of the ne... | nucl-th | the equation of state for the beta stable nuclear matter is calculated numerically and then the tolmanoppenheimervolkov equation for the structure of the neutron star is solved in the fourthorder rungekutta algorithm it shows the mass and radius of the neutron star are functions of the central density of the neutron st... | [['the', 'equation', 'of', 'state', 'for', 'the', 'beta', 'stable', 'nuclear', 'matter', 'is', 'calculated', 'numerically', 'and', 'then', 'the', 'tolmanoppenheimervolkov', 'equation', 'for', 'the', 'structure', 'of', 'the', 'neutron', 'star', 'is', 'solved', 'in', 'the', 'fourthorder', 'rungekutta', 'algorithm', 'it',... | [-0.09774746313761873, 0.1590361246018364, -0.10331522864643249, 0.08422587914362879, -0.06504905767609141, -0.055112141682589544, 0.02802006761201575, 0.29453300423640166, -0.22115659571688953, -0.31586445940516983, 0.07009544372823844, -0.2859035008586943, -0.0030498431503324756, 0.19715831138612114, 0.02597401545035... |
707.3865 | Distribution of Time-Averaged Observables for Weak Ergodicity Breaking | We find a general formula for the distribution of time-averaged observables
for systems modeled according to the sub-diffusive continuous time random walk.
For Gaussian random walks coupled to a thermal bath we recover ergodicity and
Boltzmann's statistics, while for the anomalous subdiffusive case a weakly
non-ergod... | cond-mat.stat-mech | we find a general formula for the distribution of timeaveraged observables for systems modeled according to the subdiffusive continuous time random walk for gaussian random walks coupled to a thermal bath we recover ergodicity and boltzmanns statistics while for the anomalous subdiffusive case a weakly nonergodic stati... | [['we', 'find', 'a', 'general', 'formula', 'for', 'the', 'distribution', 'of', 'timeaveraged', 'observables', 'for', 'systems', 'modeled', 'according', 'to', 'the', 'subdiffusive', 'continuous', 'time', 'random', 'walk', 'for', 'gaussian', 'random', 'walks', 'coupled', 'to', 'a', 'thermal', 'bath', 'we', 'recover', 'er... | [-0.08859330571266179, 0.19243290979723018, -0.1429357539007882, 0.08748838406526628, 0.02652190542136578, -0.17547099972047756, 0.058803364975358714, 0.34657452575209524, -0.2520086873687573, -0.22247519864479906, 0.07273947501785516, -0.2959392610073243, -0.09848502330174766, 0.18745167053799078, -0.04028288484310981... |
707.3866 | Filtration shrinkage by level-crossings of a diffusion | We develop the mathematics of a filtration shrinkage model that has recently
been considered in the credit risk modeling literature. Given a finite
collection of points $x_1<...<x_N$ in $\mathbb{R}$, the region indicator
function $R(x)$ assumes the value $i$ if $x\in(x_{i-1},x_i]$. We take
$\mathbb{F}$ to be the filt... | math.PR | we develop the mathematics of a filtration shrinkage model that has recently been considered in the credit risk modeling literature given a finite collection of points x_1x_n in mathbbr the region indicator function rx assumes the value i if xinx_i1x_i we take mathbbf to be the filtration generated by rx_t_tgeq0 where ... | [['we', 'develop', 'the', 'mathematics', 'of', 'a', 'filtration', 'shrinkage', 'model', 'that', 'has', 'recently', 'been', 'considered', 'in', 'the', 'credit', 'risk', 'modeling', 'literature', 'given', 'a', 'finite', 'collection', 'of', 'points', 'x_1x_n', 'in', 'mathbbr', 'the', 'region', 'indicator', 'function', 'rx... | [-0.11849195053368884, 0.0759234000381428, -0.10469395823815127, 0.0264588027614044, -0.06773095381609404, -0.13775011167871123, -0.008377408468375732, 0.3730454535905233, -0.3322857384829177, -0.1607825179787151, 0.10758985509404663, -0.28144724458484843, -0.1399796480605782, 0.14749032800258666, -0.14964658855586602,... |
707.3867 | Low/Hard State Spectra of GRO J1655-40 Observed with Suzaku | The Galactic black-hole binary GRO J1655$-$40 was observed with Suzaku on
2005 September 22--23, for a net exposure of 35 ks with the X-ray Imaging
Spectrometer (XIS) and 20 ks with the Hard X-ray Detector (HXD). The source was
detected over a broad and continuous energy range of 0.7--300 keV, with an
intensity of $\... | astro-ph | the galactic blackhole binary gro j165540 was observed with suzaku on 2005 september 2223 for a net exposure of 35 ks with the xray imaging spectrometer xis and 20 ks with the hard xray detector hxd the source was detected over a broad and continuous energy range of 07300 kev with an intensity of sim50 mcrab at 20 kev ... | [['the', 'galactic', 'blackhole', 'binary', 'gro', 'j165540', 'was', 'observed', 'with', 'suzaku', 'on', '2005', 'september', '2223', 'for', 'a', 'net', 'exposure', 'of', '35', 'ks', 'with', 'the', 'xray', 'imaging', 'spectrometer', 'xis', 'and', '20', 'ks', 'with', 'the', 'hard', 'xray', 'detector', 'hxd', 'the', 'sou... | [-0.01097859725842424, 0.18317032692204596, -0.0240190790738885, 0.11449652179716466, -0.01703967879653187, -0.1356954260700646, 0.03599209543365235, 0.4570859269566402, -0.16149255520991548, -0.45244708884532847, 0.05874585686013128, -0.3775358170480706, 0.10111601576018354, 0.2055946348947012, 0.00525867531343074, -0... |
707.3868 | Finite quantum tomography via semidefinite programming | Using the the convex semidefinite programming method and superoperator
formalism we obtain the finite quantum tomography of some mixed quantum states
such as: qudit tomography, N-qubit tomography, phase tomography and coherent
spin state tomography, where that obtained results are in agreement with those
of Reference... | quant-ph | using the the convex semidefinite programming method and superoperator formalism we obtain the finite quantum tomography of some mixed quantum states such as qudit tomography nqubit tomography phase tomography and coherent spin state tomography where that obtained results are in agreement with those of references cites... | [['using', 'the', 'the', 'convex', 'semidefinite', 'programming', 'method', 'and', 'superoperator', 'formalism', 'we', 'obtain', 'the', 'finite', 'quantum', 'tomography', 'of', 'some', 'mixed', 'quantum', 'states', 'such', 'as', 'qudit', 'tomography', 'nqubit', 'tomography', 'phase', 'tomography', 'and', 'coherent', 's... | [0.0007741645392444398, 0.16500566977386674, -0.08151475211294988, 0.03929254538897011, 0.02716531849776705, -0.22401516569985283, -0.005167909018281434, 0.3722115385449595, -0.29663731960786716, -0.2528671121224761, 0.1518198575798629, -0.28987423562341263, -0.1232427488702039, 0.24961523730307816, 0.00108664296567440... |
707.3869 | A flat faint end of the Fornax cluster galaxy luminosity function | We analyse the photometric properties of the early-type Fornax cluster dwarf
galaxy population (M_V>-17 mag), based on a wide field imaging study of the
central cluster area in V and I band-passes with IMACS/Magellan at Las Campanas
Observatory. We create a fiducial sample of ~100 Fornax cluster dwarf
ellipticals (dE... | astro-ph | we analyse the photometric properties of the earlytype fornax cluster dwarf galaxy population m_v17 mag based on a wide field imaging study of the central cluster area in v and i bandpasses with imacsmagellan at las campanas observatory we create a fiducial sample of 100 fornax cluster dwarf ellipticals des with 166m_v... | [['we', 'analyse', 'the', 'photometric', 'properties', 'of', 'the', 'earlytype', 'fornax', 'cluster', 'dwarf', 'galaxy', 'population', 'm_v17', 'mag', 'based', 'on', 'a', 'wide', 'field', 'imaging', 'study', 'of', 'the', 'central', 'cluster', 'area', 'in', 'v', 'and', 'i', 'bandpasses', 'with', 'imacsmagellan', 'at', '... | [-0.06140151836397814, 0.037398792378916385, -0.1508357105134376, 0.13209883116525162, -0.12180212717686821, -0.03342146199400734, 0.03593206270070279, 0.41326920506475595, -0.12721208105175733, -0.39797316641338043, 0.006563734356084554, -0.32161221668821544, -0.05006717773913658, 0.21855086309312305, -0.0969354760181... |
707.387 | Spontaneously induced atom-radiation entanglement in an ensemble of
two-level atoms | Analysis of the spontaneously induced correlation on atom-radiation
entanglement in an ensemble of two-level atoms initially prepared in the upper
level and placed in a cavity containing a squeezed radiation employing the
method of evaluating the coherent-state propagator is presented. It is found
that the cavity rad... | quant-ph | analysis of the spontaneously induced correlation on atomradiation entanglement in an ensemble of twolevel atoms initially prepared in the upper level and placed in a cavity containing a squeezed radiation employing the method of evaluating the coherentstate propagator is presented it is found that the cavity radiation... | [['analysis', 'of', 'the', 'spontaneously', 'induced', 'correlation', 'on', 'atomradiation', 'entanglement', 'in', 'an', 'ensemble', 'of', 'twolevel', 'atoms', 'initially', 'prepared', 'in', 'the', 'upper', 'level', 'and', 'placed', 'in', 'a', 'cavity', 'containing', 'a', 'squeezed', 'radiation', 'employing', 'the', 'm... | [-0.1392847360619935, 0.26078668250880177, -0.09481292194871617, 0.008244100777942333, 0.029735499521761778, -0.15593322941900364, 0.029432627181189934, 0.37693217929659617, -0.2328543806714671, -0.2584794889396382, 0.011252091835356422, -0.28942962119444493, -0.062373047790652704, 0.2008154590481094, 0.018612990643651... |
707.3871 | On the Clausius theorem | We show that for a metastable system there exists a theoretical possibility
of a violation of the Clausius inequality without a violation of the second
law. Possibilities of experimental detection of this hypothetical violation are
pointed out.
| physics.gen-ph | we show that for a metastable system there exists a theoretical possibility of a violation of the clausius inequality without a violation of the second law possibilities of experimental detection of this hypothetical violation are pointed out | [['we', 'show', 'that', 'for', 'a', 'metastable', 'system', 'there', 'exists', 'a', 'theoretical', 'possibility', 'of', 'a', 'violation', 'of', 'the', 'clausius', 'inequality', 'without', 'a', 'violation', 'of', 'the', 'second', 'law', 'possibilities', 'of', 'experimental', 'detection', 'of', 'this', 'hypothetical', 'v... | [-0.1926669757435652, 0.13923158786083395, -0.10686864381706393, 0.06414083802657253, -0.034905638696776854, -0.18822262315331278, 0.205996337900492, 0.21927014262591665, -0.24820019857253175, -0.27459126277952584, 0.049454382885046104, -0.3054932352105105, -0.1058151423679413, 0.21346962089474136, -0.00468188857760381... |
707.3872 | Accuracy matrix in generalized simultaneous measurement of a qubit
system | We formulate the accuracy of quantum measurement for a qubit system in terms
of a 3 by 3 matrix. This matrix, which we refer to as the accuracy matrix, can
be calculated from a positive operator-valued measure (POVM) corresponding to
the quantum measurement. Based on the accuracy matrix, we derive new trade-off
relat... | quant-ph | we formulate the accuracy of quantum measurement for a qubit system in terms of a 3 by 3 matrix this matrix which we refer to as the accuracy matrix can be calculated from a positive operatorvalued measure povm corresponding to the quantum measurement based on the accuracy matrix we derive new tradeoff relations betwee... | [['we', 'formulate', 'the', 'accuracy', 'of', 'quantum', 'measurement', 'for', 'a', 'qubit', 'system', 'in', 'terms', 'of', 'a', '3', 'by', '3', 'matrix', 'this', 'matrix', 'which', 'we', 'refer', 'to', 'as', 'the', 'accuracy', 'matrix', 'can', 'be', 'calculated', 'from', 'a', 'positive', 'operatorvalued', 'measure', '... | [-0.09121440182955072, 0.09477884680764065, -0.11353696418030892, 0.09247170068719034, -0.01639600658227362, -0.14739625167112028, 0.10665524696317298, 0.3313370715402712, -0.2959171388306078, -0.34167394318290095, 0.0888674344630735, -0.30053010728605634, -0.1338561966904054, 0.2016070649319188, -0.10348925956488488, ... |
707.3873 | Alternative parametrizations and reference priors for decomposable
discrete graphical models | For a given discrete decomposable graphical model, we identify several
alternative parametrizations, and construct the corresponding reference priors
for suitable groupings of the parameters. Specifically, assuming that the
cliques of the graph are arranged in a perfect order, the parameters we
consider are condition... | math.ST stat.TH | for a given discrete decomposable graphical model we identify several alternative parametrizations and construct the corresponding reference priors for suitable groupings of the parameters specifically assuming that the cliques of the graph are arranged in a perfect order the parameters we consider are conditional prob... | [['for', 'a', 'given', 'discrete', 'decomposable', 'graphical', 'model', 'we', 'identify', 'several', 'alternative', 'parametrizations', 'and', 'construct', 'the', 'corresponding', 'reference', 'priors', 'for', 'suitable', 'groupings', 'of', 'the', 'parameters', 'specifically', 'assuming', 'that', 'the', 'cliques', 'of... | [-0.09180825763969155, 0.07109012910539446, -0.0673091039162777, 0.10624688627380553, -0.12459394127717646, -0.11644828370164918, 0.05179365475803776, 0.4154767490437497, -0.2696360230911523, -0.3135782905611331, 0.08471375891974237, -0.2502708777927024, -0.10943350737722105, 0.1454349549565687, -0.06685125645067867, 0... |
707.3874 | Binary fluids under steady shear in three dimensions | We simulate by lattice Boltzmann the steady shearing of a binary fluid
mixture with full hydrodynamics in three dimensions. Contrary to some
theoretical scenarios, a dynamical steady state is attained with finite
correlation lengths in all three spatial directions. Using large simulations we
obtain at moderately high... | cond-mat.stat-mech | we simulate by lattice boltzmann the steady shearing of a binary fluid mixture with full hydrodynamics in three dimensions contrary to some theoretical scenarios a dynamical steady state is attained with finite correlation lengths in all three spatial directions using large simulations we obtain at moderately high reyn... | [['we', 'simulate', 'by', 'lattice', 'boltzmann', 'the', 'steady', 'shearing', 'of', 'a', 'binary', 'fluid', 'mixture', 'with', 'full', 'hydrodynamics', 'in', 'three', 'dimensions', 'contrary', 'to', 'some', 'theoretical', 'scenarios', 'a', 'dynamical', 'steady', 'state', 'is', 'attained', 'with', 'finite', 'correlatio... | [-0.12781457660783982, 0.20984693659448075, -0.07874926125052674, 0.058610395619367386, -0.023485574868625438, -0.17880583149996512, 0.015949366442944812, 0.3321687076026681, -0.23572005295119752, -0.3295596170442543, 0.06577685392386783, -0.24571238785725216, -0.0495213617105037, 0.19633001697131958, -0.00092322949384... |
707.3875 | Non-local composite spin-lattice polarons in high temperature
superconductors | The non-local nature of the polaron formation in t-t'-t"-J model is studied
in large lattices up to 64 sites by developing a new numerical method. We show
that the effect of longer-range hoppings t' and t" is a large anisotropy of the
electron-phonon interaction (EPI) leading to a completely different influence
of EP... | cond-mat.str-el cond-mat.supr-con | the nonlocal nature of the polaron formation in tttj model is studied in large lattices up to 64 sites by developing a new numerical method we show that the effect of longerrange hoppings t and t is a large anisotropy of the electronphonon interaction epi leading to a completely different influence of epi on the nodal ... | [['the', 'nonlocal', 'nature', 'of', 'the', 'polaron', 'formation', 'in', 'tttj', 'model', 'is', 'studied', 'in', 'large', 'lattices', 'up', 'to', '64', 'sites', 'by', 'developing', 'a', 'new', 'numerical', 'method', 'we', 'show', 'that', 'the', 'effect', 'of', 'longerrange', 'hoppings', 't', 'and', 't', 'is', 'a', 'la... | [-0.1854362010439534, 0.20176424920234992, -0.024503776160797672, 0.07570327857240994, -0.028053497450183266, -0.17060313402654845, 0.08000614391589213, 0.3454545077566645, -0.2840252596500289, -0.2376923269096195, -0.04254712565275638, -0.35379041759702173, -0.1192344798423026, 0.14260847929045153, 0.07242192714677556... |
707.3876 | Adeles in Mathematical Physics | Application of adeles in modern mathematical physics is briefly reviewed. In
particular, some adelic products are presented.
| math-ph hep-th math.MP | application of adeles in modern mathematical physics is briefly reviewed in particular some adelic products are presented | [['application', 'of', 'adeles', 'in', 'modern', 'mathematical', 'physics', 'is', 'briefly', 'reviewed', 'in', 'particular', 'some', 'adelic', 'products', 'are', 'presented']] | [-0.12800013728658943, 0.12720947008689537, -0.06741003231967196, 0.19474604051570435, -0.10385637051042389, -0.09083423927864608, -0.12675431513172739, 0.3219964634079267, -0.3050358131089631, -0.18610476855846012, 0.21606709812219968, -0.2384636919014156, -0.20058486632564487, 0.3042442820527974, -0.18823623246348956... |
707.3877 | Intrinsic tests for the equality of two correlated proportions | Correlated proportions arise in longitudinal (panel) studies. A typical
example is the ``opinion swing'' problem: ``Has the proportion of people
favoring a politician changed after his recent speech to the nation on TV?''.
Since the same group of individuals is interviewed before and after the speech,
the two proport... | math.ST stat.TH | correlated proportions arise in longitudinal panel studies a typical example is the opinion swing problem has the proportion of people favoring a politician changed after his recent speech to the nation on tv since the same group of individuals is interviewed before and after the speech the two proportions are correlat... | [['correlated', 'proportions', 'arise', 'in', 'longitudinal', 'panel', 'studies', 'a', 'typical', 'example', 'is', 'the', 'opinion', 'swing', 'problem', 'has', 'the', 'proportion', 'of', 'people', 'favoring', 'a', 'politician', 'changed', 'after', 'his', 'recent', 'speech', 'to', 'the', 'nation', 'on', 'tv', 'since', '... | [-0.07207012654892934, 0.05740956681927764, -0.12215834450333903, 0.08848093880593487, -0.10223753496655795, -0.12157114998003697, 0.07714964370944932, 0.4080111124301882, -0.21934972309664777, -0.30224768087622966, 0.12377278105627966, -0.260011125543074, -0.10899665129698438, 0.17696167544363978, -0.08814891114882534... |
707.3878 | Plotkin construction: rank and kernel | Given two binary codes of length n, using Plotkin construction we obtain a
code of length 2n. The construction works for linear and nonlinear codes. For
the linear case, it is straightforward to see that the dimension of the final
code is the sum of the dimensions of the starting codes. For nonlinear codes,
the rank ... | cs.IT math.IT | given two binary codes of length n using plotkin construction we obtain a code of length 2n the construction works for linear and nonlinear codes for the linear case it is straightforward to see that the dimension of the final code is the sum of the dimensions of the starting codes for nonlinear codes the rank and the ... | [['given', 'two', 'binary', 'codes', 'of', 'length', 'n', 'using', 'plotkin', 'construction', 'we', 'obtain', 'a', 'code', 'of', 'length', '2n', 'the', 'construction', 'works', 'for', 'linear', 'and', 'nonlinear', 'codes', 'for', 'the', 'linear', 'case', 'it', 'is', 'straightforward', 'to', 'see', 'that', 'the', 'dimen... | [-0.15016978169823514, 0.0849691942781103, -0.04273692658037247, 0.07546276414108559, 0.0012685197630319103, -0.16702977457115875, -0.021514697902268547, 0.31083575156570853, -0.2911042308156518, -0.23720725876247062, 0.12473206606763147, -0.26705430833430127, -0.14288501090627034, 0.2313153413177907, -0.02654714616893... |
707.3879 | Chemical Equilibrium in Collisions of Small Systems | The system-size dependence of particle production in heavy-ion collisions at
the top SPS energy is analyzed in terms of the statistical model. A systematic
comparison is made of two suppression mechanisms that quantify strange particle
yields in ultra-relativistic heavy-ion collisions: the canonical model with
strang... | hep-ph | the systemsize dependence of particle production in heavyion collisions at the top sps energy is analyzed in terms of the statistical model a systematic comparison is made of two suppression mechanisms that quantify strange particle yields in ultrarelativistic heavyion collisions the canonical model with strangeness co... | [['the', 'systemsize', 'dependence', 'of', 'particle', 'production', 'in', 'heavyion', 'collisions', 'at', 'the', 'top', 'sps', 'energy', 'is', 'analyzed', 'in', 'terms', 'of', 'the', 'statistical', 'model', 'a', 'systematic', 'comparison', 'is', 'made', 'of', 'two', 'suppression', 'mechanisms', 'that', 'quantify', 'st... | [-0.10260350087915096, 0.17044115310647723, -0.18303953324247038, 0.14132212868990432, 0.06977234924367319, -0.0685123548715968, -0.02602930901268723, 0.3212518735178464, -0.21136827915920134, -0.30112029310972005, -0.06886918622397141, -0.3682381785615827, 0.028493225482772246, 0.1361928797940698, 0.08185960518929994,... |
707.388 | Progressive field-state collapse and quantum non-demolition photon
counting | The irreversible evolution of a microscopic system under measurement is a
central feature of quantum theory. From an initial state generally exhibiting
quantum uncertainty in the measured observable, the system is projected into a
state in which this observable becomes precisely known. Its value is random,
with a pro... | quant-ph | the irreversible evolution of a microscopic system under measurement is a central feature of quantum theory from an initial state generally exhibiting quantum uncertainty in the measured observable the system is projected into a state in which this observable becomes precisely known its value is random with a probabili... | [['the', 'irreversible', 'evolution', 'of', 'a', 'microscopic', 'system', 'under', 'measurement', 'is', 'a', 'central', 'feature', 'of', 'quantum', 'theory', 'from', 'an', 'initial', 'state', 'generally', 'exhibiting', 'quantum', 'uncertainty', 'in', 'the', 'measured', 'observable', 'the', 'system', 'is', 'projected', ... | [-0.15368859347100147, 0.24826441503873434, -0.10181119164917618, 0.025044715553078623, 0.013796920113409647, -0.11863755151751407, 0.0642789351383856, 0.3280007276002185, -0.27345710765526055, -0.3140120901599793, 0.062364792151908786, -0.2793737212861223, -0.060762810191330834, 0.17274606493412561, -0.005180998938851... |
707.3881 | Some tensor products | We define the tensor product of 1-motives with motives of weight 0 and we
construct explicitely the 1-motive underlying the quotient M_1 \otimes M_2 /
W_{-3}(M_1 \otimes M_2).
| math.AG math.NT | we define the tensor product of 1motives with motives of weight 0 and we construct explicitely the 1motive underlying the quotient m_1 otimes m_2 w_3m_1 otimes m_2 | [['we', 'define', 'the', 'tensor', 'product', 'of', '1motives', 'with', 'motives', 'of', 'weight', '0', 'and', 'we', 'construct', 'explicitely', 'the', '1motive', 'underlying', 'the', 'quotient', 'm_1', 'otimes', 'm_2', 'w_3m_1', 'otimes', 'm_2']] | [-0.23948029066937473, 0.17209928833807892, -0.0352095879900914, 0.03274930669711186, -0.07237991721082765, -0.172071701918657, -0.08857285990737952, 0.3989148357739815, -0.41598157942868197, -0.10278785318279496, 0.08203747291834308, -0.1760197362074485, -0.12883267254353717, 0.02691376252243152, -0.10430915453113042,... |
707.3882 | Dimensionality induced entanglement in macroscopic dimer systems | We investigate entanglement properties of mixtures of short-range spin-s
dimer coverings in lattices of arbitrary topology and dimension. We show that
in one spacial dimension nearest neighbour entanglement exists for any spin
$s$. Surprisingly, in higher spatial dimensions there is a threshold value of
spin $s$ belo... | quant-ph | we investigate entanglement properties of mixtures of shortrange spins dimer coverings in lattices of arbitrary topology and dimension we show that in one spacial dimension nearest neighbour entanglement exists for any spin s surprisingly in higher spatial dimensions there is a threshold value of spin s below which the... | [['we', 'investigate', 'entanglement', 'properties', 'of', 'mixtures', 'of', 'shortrange', 'spins', 'dimer', 'coverings', 'in', 'lattices', 'of', 'arbitrary', 'topology', 'and', 'dimension', 'we', 'show', 'that', 'in', 'one', 'spacial', 'dimension', 'nearest', 'neighbour', 'entanglement', 'exists', 'for', 'any', 'spin'... | [-0.170051807940409, 0.19218109201992284, 0.026103019953478832, 0.10834172016443885, 0.01752325040414124, -0.19505513431756077, 0.06335530508108236, 0.39094817240697305, -0.23332123043065942, -0.1969061738282845, 0.028971912764088326, -0.32909646532120734, -0.08852854715282651, 0.08062306395102595, 0.07135882455780096,... |
707.3883 | Room temperature Ferromagnetism in Th1-xFexO2-d (x = 0.0, 0.05, 0.10,
0.15, 0.20 and 0.25) nanoparticles | Nanocrystalline (Th1-xFex)O2-d particles with different Fe concentrations (x
= 0.0, 0.05, 0.10, 0.15, 0.20 and 0.25) have been prepared by a gel combustion
method. Rietveld refinement analyses of X-ray diffraction data revealed the
formation of an impurity free cubic type Th1-xFexO2-d structure up to x = 0.20.
This o... | cond-mat.mtrl-sci | nanocrystalline th1xfexo2d particles with different fe concentrations x 00 005 010 015 020 and 025 have been prepared by a gel combustion method rietveld refinement analyses of xray diffraction data revealed the formation of an impurity free cubic type th1xfexo2d structure up to x 020 this observation is further confir... | [['nanocrystalline', 'th1xfexo2d', 'particles', 'with', 'different', 'fe', 'concentrations', 'x', '00', '005', '010', '015', '020', 'and', '025', 'have', 'been', 'prepared', 'by', 'a', 'gel', 'combustion', 'method', 'rietveld', 'refinement', 'analyses', 'of', 'xray', 'diffraction', 'data', 'revealed', 'the', 'formation... | [-0.060262382127499826, 0.19783592689676274, -0.04371270543682234, -0.01153306655275325, 0.006016089745874827, -0.1504903651754527, 0.1424314260554335, 0.4721624900897344, -0.25009224805398844, -0.3539571482494163, 0.0356547019740295, -0.4272155702734987, 0.00491744988054658, 0.19536842894740403, 0.052580408858678616, ... |
707.3884 | Enhanced phase mixing of Alfv\'en waves propagating in stratified and
divergent coronal structures | Corrected analytical solutions describing the enhanced phase mixing of Alfven
waves propagating in divergent stratified coronal structures are presented.
These show that the enhanced phase mixing mechanism can dissipate Alfven waves
at heights less than half that is predicted by the previous analytical
solutions. The... | astro-ph | corrected analytical solutions describing the enhanced phase mixing of alfven waves propagating in divergent stratified coronal structures are presented these show that the enhanced phase mixing mechanism can dissipate alfven waves at heights less than half that is predicted by the previous analytical solutions the enh... | [['corrected', 'analytical', 'solutions', 'describing', 'the', 'enhanced', 'phase', 'mixing', 'of', 'alfven', 'waves', 'propagating', 'in', 'divergent', 'stratified', 'coronal', 'structures', 'are', 'presented', 'these', 'show', 'that', 'the', 'enhanced', 'phase', 'mixing', 'mechanism', 'can', 'dissipate', 'alfven', 'w... | [-0.18892478401897078, 0.3300368706259703, -0.005900843282455464, 0.09907679207453216, -0.04865653768168352, -0.057990028942340066, 0.007152770965323121, 0.3457756067562297, -0.23852191223773017, -0.3174196144428091, 0.08331568017711237, -0.2280591720267996, -0.0731548477781244, 0.2147102955130302, 0.036250155624939426... |
707.3885 | Microscopic quantum superpotential in N=1 gauge theories | We consider the N=1 super Yang-Mills theory with gauge group U(N), adjoint
chiral multiplet X and tree-level superpotential Tr W(X). We compute the
quantum effective superpotential W_mic as a function of arbitrary off-shell
boundary conditions at infinity for the scalar field X. This effective
superpotential has a re... | hep-th | we consider the n1 super yangmills theory with gauge group un adjoint chiral multiplet x and treelevel superpotential tr wx we compute the quantum effective superpotential w_mic as a function of arbitrary offshell boundary conditions at infinity for the scalar field x this effective superpotential has a remarkable prop... | [['we', 'consider', 'the', 'n1', 'super', 'yangmills', 'theory', 'with', 'gauge', 'group', 'un', 'adjoint', 'chiral', 'multiplet', 'x', 'and', 'treelevel', 'superpotential', 'tr', 'wx', 'we', 'compute', 'the', 'quantum', 'effective', 'superpotential', 'w_mic', 'as', 'a', 'function', 'of', 'arbitrary', 'offshell', 'boun... | [-0.15348930719618997, 0.16509595384821296, -0.10054244187350074, 0.10011750004487112, -0.06512004362264028, -0.17260450067619482, 0.004725918531573067, 0.30440202603659905, -0.18224425197268526, -0.25828178265442453, 0.03397106875199825, -0.25664633022621275, -0.1983766228860865, 0.05144330745407691, -0.05152165286242... |
707.3886 | The growth of additive processes | Let $X_t$ be any additive process in $\mathbb{R}^d.$ There are finite indices
$\delta_i, \beta_i, i=1,2$ and a function $u$, all of which are defined in
terms of the characteristics of $X_t$, such that
\liminf_{t\to0}u(t)^{-1/\eta}X_t^*= \cases{0, \quad if $\eta>\delta_1$,
\cr\infty, \quad if $\eta<\delta_2$,}
\l... | math.PR | let x_t be any additive process in mathbbrd there are finite indices delta_i beta_i i12 and a function u all of which are defined in terms of the characteristics of x_t such that liminf_tto0ut1etax_t cases0 quad if etadelta_1 crinfty quad if etadelta_2 limsup_tto0ut1etax_t cases0 quad if etabeta_2 crinfty quad if etabe... | [['let', 'x_t', 'be', 'any', 'additive', 'process', 'in', 'mathbbrd', 'there', 'are', 'finite', 'indices', 'delta_i', 'beta_i', 'i12', 'and', 'a', 'function', 'u', 'all', 'of', 'which', 'are', 'defined', 'in', 'terms', 'of', 'the', 'characteristics', 'of', 'x_t', 'such', 'that', 'liminf_tto0ut1etax_t', 'cases0', 'quad'... | [-0.12214433891768818, 0.1864180747339482, -0.03220947737735446, -0.0035823235937504673, -0.046723591071122915, -0.22954543084607168, -0.04450898748692325, 0.395437816338193, -0.32028978536286024, -0.11042040444394793, 0.15025368025175906, -0.3409501608606348, -0.12695997620692417, 0.19553478250357634, -0.0955080610439... |
707.3887 | Finite-size scaling for the left-current correlator with non-degenerate
quark masses | We study the volume dependence of the left-current correlator with
non-degenerate quark masses to next-to-leading order in the chiral expansion.
We consider three possible regimes: all quark masses are in the
$\epsilon$-regime, all are in the $p$-regime and a mixed-regime where the
lighest quark masses satisfy $m_v \... | hep-lat | we study the volume dependence of the leftcurrent correlator with nondegenerate quark masses to nexttoleading order in the chiral expansion we consider three possible regimes all quark masses are in the epsilonregime all are in the pregime and a mixedregime where the lighest quark masses satisfy m_v sigma v leq 1 while... | [['we', 'study', 'the', 'volume', 'dependence', 'of', 'the', 'leftcurrent', 'correlator', 'with', 'nondegenerate', 'quark', 'masses', 'to', 'nexttoleading', 'order', 'in', 'the', 'chiral', 'expansion', 'we', 'consider', 'three', 'possible', 'regimes', 'all', 'quark', 'masses', 'are', 'in', 'the', 'epsilonregime', 'all'... | [-0.0959573551623639, 0.2628659634552534, -0.03320689075309964, 0.1049056591938512, -0.027666744473164234, -0.07935096224028508, 0.028259680329514578, 0.34062605094869886, -0.1554000139308786, -0.24792085736266617, 0.047707456859163215, -0.3319580851900346, 0.01593336902414132, 0.09308401267360715, 0.056095479255162395... |
707.3888 | Maximal Arithmetic Progressions in Random Subsets | Let U(N) denote the maximal length of arithmetic progressions in a random
uniform subset of {0,1}^N. By an application of the Chen-Stein method, we show
that U(N)- 2 log(N)/log(2) converges in law to an extreme type (asymmetric)
distribution. The same result holds for the maximal length W(N) of arithmetic
progression... | math.PR math.CO | let un denote the maximal length of arithmetic progressions in a random uniform subset of 01n by an application of the chenstein method we show that un 2 lognlog2 converges in law to an extreme type asymmetric distribution the same result holds for the maximal length wn of arithmetic progressions mod n when considered ... | [['let', 'un', 'denote', 'the', 'maximal', 'length', 'of', 'arithmetic', 'progressions', 'in', 'a', 'random', 'uniform', 'subset', 'of', '01n', 'by', 'an', 'application', 'of', 'the', 'chenstein', 'method', 'we', 'show', 'that', 'un', '2', 'lognlog2', 'converges', 'in', 'law', 'to', 'an', 'extreme', 'type', 'asymmetric... | [-0.152485285022455, 0.1492670731446507, -0.10748296881253581, 0.04410880495845226, 0.028815519984629823, -0.1260246581443381, 0.04686867450534298, 0.3493664425786403, -0.27578807508618364, -0.19745083822493964, 0.05573023203192506, -0.31508994224004266, -0.12320000248415987, 0.17133314935944793, -0.16769161976010696, ... |
707.3889 | Analytic application of the mean crossover function to the description
of the isothermal compressibility of xenon | We use the mean crossover functions [Garrabos and Bervillier, Phys Rev. E 74,
021113 (2006)] estimated from the bounded results of the Massive
Renormalization scheme applied to the $\Phi_{d}^{4}(n)$ model in three
dimensions ($d=3$) and scalar order parameter ($n=1$) [Bagnuls and Bervillier,
Phys. Rev. E 65, 066132 (... | cond-mat.stat-mech | we use the mean crossover functions garrabos and bervillier phys rev e 74 021113 2006 estimated from the bounded results of the massive renormalization scheme applied to the phi_d4n model in three dimensions d3 and scalar order parameter n1 bagnuls and bervillier phys rev e 65 066132 2002 to represent the singular beha... | [['we', 'use', 'the', 'mean', 'crossover', 'functions', 'garrabos', 'and', 'bervillier', 'phys', 'rev', 'e', '74', '021113', '2006', 'estimated', 'from', 'the', 'bounded', 'results', 'of', 'the', 'massive', 'renormalization', 'scheme', 'applied', 'to', 'the', 'phi_d4n', 'model', 'in', 'three', 'dimensions', 'd3', 'and'... | [-0.09342732557536479, 0.13700562926068743, -0.02836849604871996, -0.02832619495630423, -0.03950708023609316, -0.10513185363193538, 0.0602287614007203, 0.2784154067073572, -0.18401749728698322, -0.297079651765129, 0.019780769883506397, -0.2805214184026749, -0.1286643791864527, 0.154649131948703, 0.01073808309205986, 0.... |
707.389 | Geometrical dependence of decoherence by electronic interactions in a
GaAs/GaAlAs square network | We investigate weak localization in metallic networks etched in a two
dimensional electron gas between $25\:$mK and $750\:$mK when electron-electron
(e-e) interaction is the dominant phase breaking mechanism. We show that, at
the highest temperatures, the contributions arising from trajectories that wind
around the r... | cond-mat.mes-hall cond-mat.dis-nn | we investigate weak localization in metallic networks etched in a two dimensional electron gas between 25mk and 750mk when electronelectron ee interaction is the dominant phase breaking mechanism we show that at the highest temperatures the contributions arising from trajectories that wind around the rings and trajecto... | [['we', 'investigate', 'weak', 'localization', 'in', 'metallic', 'networks', 'etched', 'in', 'a', 'two', 'dimensional', 'electron', 'gas', 'between', '25mk', 'and', '750mk', 'when', 'electronelectron', 'ee', 'interaction', 'is', 'the', 'dominant', 'phase', 'breaking', 'mechanism', 'we', 'show', 'that', 'at', 'the', 'hi... | [-0.1687452972142843, 0.15050257047427432, -0.05575122676332885, 0.06758185847385628, 0.01687315887060974, -0.12049135488879709, 0.0030381920668384375, 0.37087303681193656, -0.27430151898484184, -0.24909851832737057, 0.03973294535480475, -0.30562824170755326, -0.11073254065517828, 0.19994147411077548, 0.046262592694476... |
707.3891 | Curie temperature of the two band double exchange model for manganites | We consider two-band double exchange model and calculate the critical
temperature in ferromagnetic regime (Curie temperature). The localized spins
are represented in terms of the Schwinger-bosons, and two spin-singlet Fermion
operators are introduced. In terms of the new Fermi fields the on-site Hund's
interactions a... | cond-mat.str-el | we consider twoband double exchange model and calculate the critical temperature in ferromagnetic regime curie temperature the localized spins are represented in terms of the schwingerbosons and two spinsinglet fermion operators are introduced in terms of the new fermi fields the onsite hunds interactions are in a diag... | [['we', 'consider', 'twoband', 'double', 'exchange', 'model', 'and', 'calculate', 'the', 'critical', 'temperature', 'in', 'ferromagnetic', 'regime', 'curie', 'temperature', 'the', 'localized', 'spins', 'are', 'represented', 'in', 'terms', 'of', 'the', 'schwingerbosons', 'and', 'two', 'spinsinglet', 'fermion', 'operator... | [-0.1919120566656246, 0.21160624282650964, -0.029798943841698296, 0.0865849258548553, -0.016133980327825724, -0.14213493404626523, 0.06188865551350476, 0.29847704778438894, -0.22408155426619222, -0.23389777283359697, -0.01278351687748606, -0.3420286707148172, -0.09074341698441708, 0.16178523931159652, 0.073618791700489... |
707.3892 | On elliptic differential operators with shifts: II. The cohomological
index formula | This paper is a continuation of arXiv:0706.3511, where we obtained a local
index formula for matrix elliptic operators with shifts. Here we establish a
cohomological index formula of Atiyah-Singer type for elliptic differential
operators with shifts acting between section spaces of arbitrary vector
bundles. The key s... | math.OA math.AP math.KT | this paper is a continuation of arxiv07063511 where we obtained a local index formula for matrix elliptic operators with shifts here we establish a cohomological index formula of atiyahsinger type for elliptic differential operators with shifts acting between section spaces of arbitrary vector bundles the key step is t... | [['this', 'paper', 'is', 'a', 'continuation', 'of', 'arxiv07063511', 'where', 'we', 'obtained', 'a', 'local', 'index', 'formula', 'for', 'matrix', 'elliptic', 'operators', 'with', 'shifts', 'here', 'we', 'establish', 'a', 'cohomological', 'index', 'formula', 'of', 'atiyahsinger', 'type', 'for', 'elliptic', 'differentia... | [-0.19457774598038557, 0.07549311591322873, -0.08428789341511826, 0.06507188039408489, -0.1212937308397765, -0.13702137006982934, -0.025702813271588337, 0.32492238238002313, -0.32539602707732806, -0.21841941440873075, 0.120669710897897, -0.2597754374993118, -0.17344113896163463, 0.22783064198764888, -0.1301402588812352... |
707.3893 | Jet-induced gauge field instabilities in the quark-gluon plasma: A
kinetic theory approach | We discuss the properties of the collective modes of a system composed by a
thermalized quark-gluon plasma traversed by a relativistic jet of partons. The
transport equations obeyed by the components of the plasma and of the jet are
studied in the Vlasov approximation. Assuming that the partons in the jet can
be desc... | hep-ph | we discuss the properties of the collective modes of a system composed by a thermalized quarkgluon plasma traversed by a relativistic jet of partons the transport equations obeyed by the components of the plasma and of the jet are studied in the vlasov approximation assuming that the partons in the jet can be described... | [['we', 'discuss', 'the', 'properties', 'of', 'the', 'collective', 'modes', 'of', 'a', 'system', 'composed', 'by', 'a', 'thermalized', 'quarkgluon', 'plasma', 'traversed', 'by', 'a', 'relativistic', 'jet', 'of', 'partons', 'the', 'transport', 'equations', 'obeyed', 'by', 'the', 'components', 'of', 'the', 'plasma', 'and... | [-0.15130790610669584, 0.22137814485554205, -0.14596418731860697, 0.0623138097383417, -0.02297400934227481, -0.046001789197030046, -0.018336855584666842, 0.33734395760037594, -0.22674732741951528, -0.25235487010684754, 0.02587586942451597, -0.26847580572954877, -0.03910569985712529, 0.18349421100331242, 0.0578346887477... |
707.3894 | Manifolds with nonnegative isotropic curvature | We prove that if $(M^n,g)$, $n \ge 4$, is a compact, orientable, locally
irreducible Riemannian manifold with nonnegative isotropic curvature, then one
of the following possibilities hold:
(i) $M$ admits a metric with positive isotropic curvature
(ii) $(M,g)$ is isometric to a locally symmetric space
(iii) $(M,... | math.DG | we prove that if mng n ge 4 is a compact orientable locally irreducible riemannian manifold with nonnegative isotropic curvature then one of the following possibilities hold i m admits a metric with positive isotropic curvature ii mg is isometric to a locally symmetric space iii mg is kahler and biholomorphic to c pfra... | [['we', 'prove', 'that', 'if', 'mng', 'n', 'ge', '4', 'is', 'a', 'compact', 'orientable', 'locally', 'irreducible', 'riemannian', 'manifold', 'with', 'nonnegative', 'isotropic', 'curvature', 'then', 'one', 'of', 'the', 'following', 'possibilities', 'hold', 'i', 'm', 'admits', 'a', 'metric', 'with', 'positive', 'isotrop... | [-0.16754327237424327, 0.10726148542584624, -0.026853968442334394, 0.02305532307496552, -0.15155032857101622, -0.27161894575882006, -0.08450574118916582, 0.4025385935858982, -0.21663825329378006, -0.1797772111159151, 0.10553448064142944, -0.28898227421521416, -0.1267502521982462, 0.11242021095931409, -0.134943169397794... |
707.3895 | Knot colouring polynomials | This article introduces a natural extension of colouring numbers of knots,
called colouring polynomials, and studies their relationship to Yang-Baxter
invariants and quandle 2-cocycle invariants.
For a knot K in the 3-sphere let \pi_K be the fundamental group of the knot
complement, and let (m_K,l_K) be a meridian-... | math.GT | this article introduces a natural extension of colouring numbers of knots called colouring polynomials and studies their relationship to yangbaxter invariants and quandle 2cocycle invariants for a knot k in the 3sphere let pi_k be the fundamental group of the knot complement and let m_kl_k be a meridianlongitude pair i... | [['this', 'article', 'introduces', 'a', 'natural', 'extension', 'of', 'colouring', 'numbers', 'of', 'knots', 'called', 'colouring', 'polynomials', 'and', 'studies', 'their', 'relationship', 'to', 'yangbaxter', 'invariants', 'and', 'quandle', '2cocycle', 'invariants', 'for', 'a', 'knot', 'k', 'in', 'the', '3sphere', 'le... | [-0.2576608056416317, 0.0810937647840404, -0.13028994619992265, 0.044114980092894475, -0.1362747074338749, -0.17394233575468446, 0.009020927216222484, 0.3723534782275489, -0.369022477761529, -0.26504841655726685, 0.05901288348121337, -0.2550771417834448, -0.169439687971927, 0.15387681326485553, -0.1602404476363375, -0.... |
707.3896 | A Topological Characterization Of Knots and Links Arising From
Site-Specific Recombination | We develop a topological model of knots and links arising from a single (or
multiple processive) round(s) of recombination starting with an unknot, unlink,
or (2,m)-torus knot or link substrate. We show that all knotted or linked
products fall into a single family, and prove that the size of this family
grows linearl... | math.GT | we develop a topological model of knots and links arising from a single or multiple processive rounds of recombination starting with an unknot unlink or 2mtorus knot or link substrate we show that all knotted or linked products fall into a single family and prove that the size of this family grows linearly with the cub... | [['we', 'develop', 'a', 'topological', 'model', 'of', 'knots', 'and', 'links', 'arising', 'from', 'a', 'single', 'or', 'multiple', 'processive', 'rounds', 'of', 'recombination', 'starting', 'with', 'an', 'unknot', 'unlink', 'or', '2mtorus', 'knot', 'or', 'link', 'substrate', 'we', 'show', 'that', 'all', 'knotted', 'or'... | [-0.2403543069920518, 0.14264958620011295, -0.024831195991700056, 0.032793309155958475, -0.062369929023514514, -0.20316630787002382, 0.08411626961773078, 0.39528021521171647, -0.31116797631514853, -0.3018624529769247, 0.10376905457815155, -0.2766651866010955, -0.1564069511101688, 0.1622205076807896, -0.0648976830769421... |
707.3897 | Josephson effect through a quantum dot array | We analyze the ground state properties of an array of quantum dots connected
in series between superconducting electrodes. This system is represented by a
finite Hubbard chain coupled at both ends to BCS superconductors. The ground
state is obtained using the Lanczos algorithm within a low energy theory in
which the ... | cond-mat.supr-con cond-mat.str-el | we analyze the ground state properties of an array of quantum dots connected in series between superconducting electrodes this system is represented by a finite hubbard chain coupled at both ends to bcs superconductors the ground state is obtained using the lanczos algorithm within a low energy theory in which the bulk... | [['we', 'analyze', 'the', 'ground', 'state', 'properties', 'of', 'an', 'array', 'of', 'quantum', 'dots', 'connected', 'in', 'series', 'between', 'superconducting', 'electrodes', 'this', 'system', 'is', 'represented', 'by', 'a', 'finite', 'hubbard', 'chain', 'coupled', 'at', 'both', 'ends', 'to', 'bcs', 'superconductors... | [-0.1892600643368704, 0.14528793438013443, -0.0768901896529964, 0.044221649759981246, -0.001495202130505017, -0.1273633998153465, 0.07701759786345065, 0.33159202616661787, -0.24331832954393967, -0.282589205631188, 0.053256033273147686, -0.2951936474548919, -0.12809658230016274, 0.17393905897491743, 0.049342970136286954... |
707.3898 | Multivariate normal approximation in geometric probability | Consider a measure $\mu_\lambda = \sum_x \xi_x \delta_x$ where the sum is
over points $x$ of a Poisson point process of intensity $\lambda$ on a bounded
region in $d$-space, and $\xi_x$ is a functional determined by the Poisson
points near to $x$, i.e. satisfying an exponential stabilization condition,
along with a m... | math.PR | consider a measure mu_lambda sum_x xi_x delta_x where the sum is over points x of a poisson point process of intensity lambda on a bounded region in dspace and xi_x is a functional determined by the poisson points near to x ie satisfying an exponential stabilization condition along with a moments condition examples inc... | [['consider', 'a', 'measure', 'mu_lambda', 'sum_x', 'xi_x', 'delta_x', 'where', 'the', 'sum', 'is', 'over', 'points', 'x', 'of', 'a', 'poisson', 'point', 'process', 'of', 'intensity', 'lambda', 'on', 'a', 'bounded', 'region', 'in', 'dspace', 'and', 'xi_x', 'is', 'a', 'functional', 'determined', 'by', 'the', 'poisson', ... | [-0.14343923711473303, 0.09212546961345887, -0.05773350317031145, 0.04895030371072871, -0.0037738068307179118, -0.12674022165893187, 0.099416420144412, 0.34735889777901674, -0.27685050039942705, -0.18417855536550162, 0.09234940951066692, -0.31564824738644903, -0.07180441252046055, 0.18051409626364587, -0.10025430823823... |
707.3899 | Particle propagation in non-trivial backgrounds: a quantum field theory
approach | The basic aim of the thesis is the study of the propagation of particles and
quasiparticles in non-trivial backgrounds from the quantum field theory point
of view. By "non-trivial background" we mean either a non-vacuum state in
Minkowski spacetime or an arbitrary state in a curved spacetime. Starting with
the case o... | hep-ph gr-qc hep-th | the basic aim of the thesis is the study of the propagation of particles and quasiparticles in nontrivial backgrounds from the quantum field theory point of view by nontrivial background we mean either a nonvacuum state in minkowski spacetime or an arbitrary state in a curved spacetime starting with the case of a flat ... | [['the', 'basic', 'aim', 'of', 'the', 'thesis', 'is', 'the', 'study', 'of', 'the', 'propagation', 'of', 'particles', 'and', 'quasiparticles', 'in', 'nontrivial', 'backgrounds', 'from', 'the', 'quantum', 'field', 'theory', 'point', 'of', 'view', 'by', 'nontrivial', 'background', 'we', 'mean', 'either', 'a', 'nonvacuum',... | [-0.10986481042062578, 0.16545708229416922, -0.12934110852390918, 0.09663025638191483, -0.05802527984625168, -0.11001789016816556, -0.010005752824173634, 0.31261555148700204, -0.21414159075793032, -0.2561245837012543, 0.06426248963911797, -0.2935538819950939, -0.09391287971577478, 0.16250948320284192, -0.00618419464422... |
707.39 | Schr\"odinger operators on armchair nanotubes. II | We consider the Schr\"odinger operator with a periodic potential on quasi-1D
models of armchair single-wall nanotubes. The spectrum of this operator
consists of an absolutely continuous part (intervals separated by gaps) plus an
infinite number of eigenvalues with infinite multiplicity. We describe the
absolutely con... | math.SP math-ph math.MP | we consider the schrodinger operator with a periodic potential on quasi1d models of armchair singlewall nanotubes the spectrum of this operator consists of an absolutely continuous part intervals separated by gaps plus an infinite number of eigenvalues with infinite multiplicity we describe the absolutely continuous sp... | [['we', 'consider', 'the', 'schrodinger', 'operator', 'with', 'a', 'periodic', 'potential', 'on', 'quasi1d', 'models', 'of', 'armchair', 'singlewall', 'nanotubes', 'the', 'spectrum', 'of', 'this', 'operator', 'consists', 'of', 'an', 'absolutely', 'continuous', 'part', 'intervals', 'separated', 'by', 'gaps', 'plus', 'an... | [-0.21503106933287394, 0.14983383657427013, -0.07300578657617812, 0.06793357239615533, 0.0029643327047828064, -0.12057618415784291, -0.004518539689841771, 0.36726798555783685, -0.25488115903378156, -0.21520706085908797, 0.09338888132904646, -0.38375776593563377, -0.08253512994676668, 0.09704369655059229, -0.01021539374... |
707.3901 | Laboratory Density Functionals | We compare several definitions of the density of a self-bound system, such as
a nucleus, in relation with its center-of-mass zero-point motion. A trivial
deconvolution relates the internal density to the density defined in the
laboratory frame. This result is useful for the practical definition of density
functionals... | nucl-th | we compare several definitions of the density of a selfbound system such as a nucleus in relation with its centerofmass zeropoint motion a trivial deconvolution relates the internal density to the density defined in the laboratory frame this result is useful for the practical definition of density functionals | [['we', 'compare', 'several', 'definitions', 'of', 'the', 'density', 'of', 'a', 'selfbound', 'system', 'such', 'as', 'a', 'nucleus', 'in', 'relation', 'with', 'its', 'centerofmass', 'zeropoint', 'motion', 'a', 'trivial', 'deconvolution', 'relates', 'the', 'internal', 'density', 'to', 'the', 'density', 'defined', 'in', ... | [-0.1375652152734498, 0.09840165193115051, -0.18015584654616154, 0.07814360871755828, 0.004466549299346904, -0.025891648473285993, 0.007948332155744234, 0.3330051932328691, -0.26555177359841764, -0.3219435829669237, 0.01456235621299129, -0.24543222707385817, -0.09422901678287114, 0.14724993061584732, -0.070619410961323... |
707.3902 | Probing the nuclear EOS with fragment production | We discuss fragmentation mechanisms and isospin transport occurring in
central collisions between neutron rich systems at Fermi energies. In
particular, isospin effects are analyzed looking at the correlations between
fragment isotopic content and kinematical properties. Simulations are based on
an approximate soluti... | nucl-th | we discuss fragmentation mechanisms and isospin transport occurring in central collisions between neutron rich systems at fermi energies in particular isospin effects are analyzed looking at the correlations between fragment isotopic content and kinematical properties simulations are based on an approximate solution of... | [['we', 'discuss', 'fragmentation', 'mechanisms', 'and', 'isospin', 'transport', 'occurring', 'in', 'central', 'collisions', 'between', 'neutron', 'rich', 'systems', 'at', 'fermi', 'energies', 'in', 'particular', 'isospin', 'effects', 'are', 'analyzed', 'looking', 'at', 'the', 'correlations', 'between', 'fragment', 'is... | [-0.11969873214570376, 0.16414229001966305, -0.1226282001258089, 0.16686606363644108, -0.04006365933097326, -0.09108484549304614, 0.017327394916747625, 0.37374671812240895, -0.24425913361259377, -0.2846330701158597, -0.008745399301943298, -0.318323298672644, -0.026084795551231273, 0.10358968081955726, 0.043380816875455... |
707.3903 | Multidimensional cellular automata and generalization of Fekete's lemma | Fekete's lemma is a well known combinatorial result on number sequences: we
extend it to functions defined on $d$-tuples of integers. As an application of
the new variant, we show that nonsurjective $d$-dimensional cellular automata
are characterized by loss of arbitrarily much information on finite supports,
at a gr... | math.GM math.DS | feketes lemma is a well known combinatorial result on number sequences we extend it to functions defined on dtuples of integers as an application of the new variant we show that nonsurjective ddimensional cellular automata are characterized by loss of arbitrarily much information on finite supports at a growth rate gre... | [['feketes', 'lemma', 'is', 'a', 'well', 'known', 'combinatorial', 'result', 'on', 'number', 'sequences', 'we', 'extend', 'it', 'to', 'functions', 'defined', 'on', 'dtuples', 'of', 'integers', 'as', 'an', 'application', 'of', 'the', 'new', 'variant', 'we', 'show', 'that', 'nonsurjective', 'ddimensional', 'cellular', 'a... | [-0.1541074990398354, 0.12164113161524588, -0.039013265853836424, 0.10429648482351608, -0.0390910021240069, -0.11108791862895327, 0.08166877935374421, 0.33973124259639353, -0.2838222822026601, -0.25319594523263356, 0.11680590842540066, -0.23996000782409238, -0.16929210698424232, 0.26270483604203615, -0.1367931105723116... |
707.3904 | Measurement of the Fermi Constant by FAST | An initial measurement of the lifetime of the positive muon to a precision of
16 parts per million (ppm) has been performed with the FAST detector at the
Paul Scherrer Institute. The result is tau_mu = 2.197083 (32) (15) microsec,
where the first error is statistical and the second is systematic. The muon
lifetime de... | hep-ex | an initial measurement of the lifetime of the positive muon to a precision of 16 parts per million ppm has been performed with the fast detector at the paul scherrer institute the result is tau_mu 2197083 32 15 microsec where the first error is statistical and the second is systematic the muon lifetime determines the f... | [['an', 'initial', 'measurement', 'of', 'the', 'lifetime', 'of', 'the', 'positive', 'muon', 'to', 'a', 'precision', 'of', '16', 'parts', 'per', 'million', 'ppm', 'has', 'been', 'performed', 'with', 'the', 'fast', 'detector', 'at', 'the', 'paul', 'scherrer', 'institute', 'the', 'result', 'is', 'tau_mu', '2197083', '32',... | [-0.11946896258889446, 0.22223412320373528, 0.01335426008269664, 0.0043156952356978775, 0.04315179040182441, -0.10673513573165687, 0.07405511042591006, 0.27598763326744713, -0.19751953537620248, -0.40412388153610723, 0.09597843941596765, -0.3634307486788621, 0.10230151903889483, 0.20193199111547852, -0.0246439396610690... |
707.3905 | Spectropolarimetric signatures of Earth-like extrasolar planets | We present results of numerical simulations of the flux (irradiance), F, and
the degree of polarization (i.e. the ratio of polarized to total flux), P, of
light that is reflected by Earth-like extrasolar planets orbiting solar-type
stars, as functions of the wavelength (from 0.3 to 1.0 micron, with 0.001
micron spect... | astro-ph | we present results of numerical simulations of the flux irradiance f and the degree of polarization ie the ratio of polarized to total flux p of light that is reflected by earthlike extrasolar planets orbiting solartype stars as functions of the wavelength from 03 to 10 micron with 0001 micron spectral resolution and a... | [['we', 'present', 'results', 'of', 'numerical', 'simulations', 'of', 'the', 'flux', 'irradiance', 'f', 'and', 'the', 'degree', 'of', 'polarization', 'ie', 'the', 'ratio', 'of', 'polarized', 'to', 'total', 'flux', 'p', 'of', 'light', 'that', 'is', 'reflected', 'by', 'earthlike', 'extrasolar', 'planets', 'orbiting', 'so... | [-0.09698971647026372, 0.1698897568181911, -0.03948743620532609, 0.038482687035797256, -0.06468810589008388, -0.048477955648143375, 0.0527768306467416, 0.4117946782105026, -0.2082886115923646, -0.3374300444942145, 0.046854572515890355, -0.2625102760558504, -0.08612955301401339, 0.2214741564056437, -0.030060642917219195... |
707.3906 | Negative phase velocity in nonlinear oscillatory systems --mechanism and
parameter distributions | Waves propagating inwardly to the wave source are called antiwaves which have
negative phase velocity. In this paper the phenomenon of negative phase
velocity in oscillatory systems is studied on the basis of periodically paced
complex Ginzbug-Laundau equation (CGLE). We figure out a clear physical picture
on the neg... | cond-mat.mtrl-sci | waves propagating inwardly to the wave source are called antiwaves which have negative phase velocity in this paper the phenomenon of negative phase velocity in oscillatory systems is studied on the basis of periodically paced complex ginzbuglaundau equation cgle we figure out a clear physical picture on the negative p... | [['waves', 'propagating', 'inwardly', 'to', 'the', 'wave', 'source', 'are', 'called', 'antiwaves', 'which', 'have', 'negative', 'phase', 'velocity', 'in', 'this', 'paper', 'the', 'phenomenon', 'of', 'negative', 'phase', 'velocity', 'in', 'oscillatory', 'systems', 'is', 'studied', 'on', 'the', 'basis', 'of', 'periodical... | [-0.20556080814317934, 0.21414791700080968, -0.08153930452619014, 0.03473068434478981, -0.106436196525049, -0.10400752296970625, 0.012732776634428384, 0.34590506214382394, -0.25146354329917814, -0.23121507756545076, 0.06351464299701287, -0.25925978125139537, -0.2121596088566418, 0.21201103177985975, 0.02659600510128906... |
707.3907 | Summary of the Heavy Flavor Working Group | During the last year many important results have been achieved in heavy
flavour physics: New measurements of charm and beauty production have been
performed at HERA and the Tevatron. A wealth of new spectroscopy data with
several new, unexpected states in the charmonium and the D_s systems has been
collected and b to... | hep-ph | during the last year many important results have been achieved in heavy flavour physics new measurements of charm and beauty production have been performed at hera and the tevatron a wealth of new spectroscopy data with several new unexpected states in the charmonium and the d_s systems has been collected and b to d ga... | [['during', 'the', 'last', 'year', 'many', 'important', 'results', 'have', 'been', 'achieved', 'in', 'heavy', 'flavour', 'physics', 'new', 'measurements', 'of', 'charm', 'and', 'beauty', 'production', 'have', 'been', 'performed', 'at', 'hera', 'and', 'the', 'tevatron', 'a', 'wealth', 'of', 'new', 'spectroscopy', 'data'... | [-0.039062311441757445, 0.22731004883581313, -0.13539177833106553, 0.06914438997017275, -0.018485948305097546, -0.15255020506620076, 0.04198053682633297, 0.33453647017774013, -0.197550194891225, -0.2803785806927498, 0.052015968053232844, -0.37534361600064403, 0.03424868377681711, 0.17038030066702625, 0.0597917674256876... |
707.3908 | Quasiclassical approach and spin-orbit coupling | We discuss the quasiclassical Green function method for a two-dimensional
electron gas in the presence of spin-orbit coupling, with emphasis on the
meaning of the $\xi$-integration procedure. As an application of our approach,
we demonstrate how the spin-Hall conductivity, in the presence of spin-flip
scattering, can... | cond-mat.mes-hall | we discuss the quasiclassical green function method for a twodimensional electron gas in the presence of spinorbit coupling with emphasis on the meaning of the xiintegration procedure as an application of our approach we demonstrate how the spinhall conductivity in the presence of spinflip scattering can be easily obta... | [['we', 'discuss', 'the', 'quasiclassical', 'green', 'function', 'method', 'for', 'a', 'twodimensional', 'electron', 'gas', 'in', 'the', 'presence', 'of', 'spinorbit', 'coupling', 'with', 'emphasis', 'on', 'the', 'meaning', 'of', 'the', 'xiintegration', 'procedure', 'as', 'an', 'application', 'of', 'our', 'approach', '... | [-0.12450950597259128, 0.07460717330845995, -0.08405530361353226, 0.037148111157189564, -0.035419604455489875, -0.054119423339319114, 0.03118757024969695, 0.37653307419902876, -0.27816600113544826, -0.2586060672787563, 0.03272346536769479, -0.2699593215794215, -0.19285592598454007, 0.23505021130912146, 0.04288881909506... |
707.3909 | Schr\"odinger operators on armchair nanotubes. I | We consider the Schr\"odinger operator with a periodic potential on quasi-1D
models of armchair single-wall nanotubes. The spectrum of this operator
consists of an absolutely continuous part (intervals separated by gaps) plus an
infinite number of eigenvalues with infinite multiplicity. We describe all
eigenfunctions... | math-ph math.MP math.SP | we consider the schrodinger operator with a periodic potential on quasi1d models of armchair singlewall nanotubes the spectrum of this operator consists of an absolutely continuous part intervals separated by gaps plus an infinite number of eigenvalues with infinite multiplicity we describe all eigenfunctions with the ... | [['we', 'consider', 'the', 'schrodinger', 'operator', 'with', 'a', 'periodic', 'potential', 'on', 'quasi1d', 'models', 'of', 'armchair', 'singlewall', 'nanotubes', 'the', 'spectrum', 'of', 'this', 'operator', 'consists', 'of', 'an', 'absolutely', 'continuous', 'part', 'intervals', 'separated', 'by', 'gaps', 'plus', 'an... | [-0.1879522260349018, 0.1023965848182361, -0.08681069238751073, 0.046947321318315735, -0.04105418257772772, -0.11563806095621501, -0.020378113364462148, 0.3764062077935898, -0.22597110497405415, -0.1939658462211038, 0.08627780921277449, -0.3369393397988093, -0.17607164458428143, 0.1573316303288771, -0.01738393632224713... |
707.391 | Landen transformations and the integration of rational functions | We present a rational version of the classical Landen transformation for
elliptic integrals. This is employed to obtain explicit closed-form expressions
for a large class of integrals of even rational functions and to develop an
algorithm for the numerical integration of these functions.
| math.CA | we present a rational version of the classical landen transformation for elliptic integrals this is employed to obtain explicit closedform expressions for a large class of integrals of even rational functions and to develop an algorithm for the numerical integration of these functions | [['we', 'present', 'a', 'rational', 'version', 'of', 'the', 'classical', 'landen', 'transformation', 'for', 'elliptic', 'integrals', 'this', 'is', 'employed', 'to', 'obtain', 'explicit', 'closedform', 'expressions', 'for', 'a', 'large', 'class', 'of', 'integrals', 'of', 'even', 'rational', 'functions', 'and', 'to', 'de... | [-0.1568608986170486, -0.02503383771190149, -0.11795411928188662, 0.11716211582858894, -0.09471219682221323, -0.10844881035560786, 0.04086854374361073, 0.32976004290719363, -0.27287835896361706, -0.24012397935743943, 0.11095196112373107, -0.21909247833672305, -0.21795782576813255, 0.2746327812241953, -0.047013005588290... |
707.3911 | A simple example of a new class of Landen transformation | The rational Landen transformation is a map on the coefficients of a rational
integrand that preserves the value of the integral. This is the rational analog
of the classical Landen transformations for elliptic integrals that leads to
the arithmetic-geometric mean of Legendre and Gauss. We present the effect of
this ... | math.CA | the rational landen transformation is a map on the coefficients of a rational integrand that preserves the value of the integral this is the rational analog of the classical landen transformations for elliptic integrals that leads to the arithmeticgeometric mean of legendre and gauss we present the effect of this trans... | [['the', 'rational', 'landen', 'transformation', 'is', 'a', 'map', 'on', 'the', 'coefficients', 'of', 'a', 'rational', 'integrand', 'that', 'preserves', 'the', 'value', 'of', 'the', 'integral', 'this', 'is', 'the', 'rational', 'analog', 'of', 'the', 'classical', 'landen', 'transformations', 'for', 'elliptic', 'integral... | [-0.190248666331172, 0.032116228893365975, -0.15772845268449082, 0.0641820488630661, -0.1189489514633481, -0.0621903981248449, 0.026908021310061616, 0.27927410462455426, -0.33797375531867146, -0.186706927904327, 0.08811011325867314, -0.2782258874337588, -0.23885297469262565, 0.20804678698602533, -0.096910643125219, 0.0... |
707.3912 | Search for Excited Leptons at HERA | Searches for excited electrons and neutrinos have been performed using the
complete HERA I and II data samples collected by the H1 detector at
$\sqrt{s}=320$ GeV corresponding to an integrated luminosity of up to 435
pb$^{-1}$. In absence of a signal, the limits on the ratio of the coupling to
the compositeness scale... | hep-ex | searches for excited electrons and neutrinos have been performed using the complete hera i and ii data samples collected by the h1 detector at sqrts320 gev corresponding to an integrated luminosity of up to 435 pb1 in absence of a signal the limits on the ratio of the coupling to the compositeness scale derived extend ... | [['searches', 'for', 'excited', 'electrons', 'and', 'neutrinos', 'have', 'been', 'performed', 'using', 'the', 'complete', 'hera', 'i', 'and', 'ii', 'data', 'samples', 'collected', 'by', 'the', 'h1', 'detector', 'at', 'sqrts320', 'gev', 'corresponding', 'to', 'an', 'integrated', 'luminosity', 'of', 'up', 'to', '435', 'p... | [-0.034344370727107595, 0.13042190014892918, -0.027638976371833192, 0.11085703371287282, -0.055473496352058296, -0.06476340832974095, 0.033847195874732824, 0.36547470837831497, -0.13820697875943647, -0.3966722090575677, 0.08008941874227751, -0.35314913347029864, 0.1254488932205114, 0.1745332011487335, 0.098310701336638... |
707.3913 | Deterministic Rendering of BB84 for Practical Quantum Cryptography | We describe how to modify the BB84 protocol for quantum cryptography in order
to make it deterministic. We study both theoretical and experimental aspects of
this issue, showing that the new scheme is as secure as the old one, more
efficient on small-scale distances, and within the range of current technology.
| quant-ph | we describe how to modify the bb84 protocol for quantum cryptography in order to make it deterministic we study both theoretical and experimental aspects of this issue showing that the new scheme is as secure as the old one more efficient on smallscale distances and within the range of current technology | [['we', 'describe', 'how', 'to', 'modify', 'the', 'bb84', 'protocol', 'for', 'quantum', 'cryptography', 'in', 'order', 'to', 'make', 'it', 'deterministic', 'we', 'study', 'both', 'theoretical', 'and', 'experimental', 'aspects', 'of', 'this', 'issue', 'showing', 'that', 'the', 'new', 'scheme', 'is', 'as', 'secure', 'as'... | [-0.10375925556838732, 0.06819934258694012, -0.10729256168226986, 0.09288107698746756, -0.03775110114000592, -0.1858111672906899, 0.0785305750985429, 0.40261198594874026, -0.2791435500862552, -0.3072904024419247, 0.09649550866143887, -0.20362059100229732, -0.15359318605167607, 0.2842639974665408, -0.10155676698366947, ... |
707.3914 | Smooth representations and sheaves | The paper is concerned with `geometrization' of smooth (i.e. with open
stabilizers) representations of the automorphism group of universal domains,
and with the properties of `geometric' representations of such groups. As an
application, we calculate the cohomology groups of several classes of smooth
representations ... | math.AG | the paper is concerned with geometrization of smooth ie with open stabilizers representations of the automorphism group of universal domains and with the properties of geometric representations of such groups as an application we calculate the cohomology groups of several classes of smooth representations of the automo... | [['the', 'paper', 'is', 'concerned', 'with', 'geometrization', 'of', 'smooth', 'ie', 'with', 'open', 'stabilizers', 'representations', 'of', 'the', 'automorphism', 'group', 'of', 'universal', 'domains', 'and', 'with', 'the', 'properties', 'of', 'geometric', 'representations', 'of', 'such', 'groups', 'as', 'an', 'applic... | [-0.24504250969978109, 0.09018048800170354, -0.13129610704979108, 0.009206928247060146, -0.10379813190910124, -0.07033610998863174, -0.0566787994748372, 0.3373644945602263, -0.37422437473170217, -0.2486438416245003, 0.11080980360237581, -0.22391370162668248, -0.13496240371117188, 0.24793168872354493, -0.122413329827043... |
707.3915 | Master crossover functions for the one-component fluid "subclass" | Introducing three well-defined dimensionless numbers, we establish the link
between the scale dilatation method able to estimate master (i.e. unique)
singular behaviors of the one-component fluid "subclass" and the universal
crossover functions recently estimated [Garrabos and Bervillier, Phys. Rev. E
74, 021113 (200... | cond-mat.stat-mech | introducing three welldefined dimensionless numbers we establish the link between the scale dilatation method able to estimate master ie unique singular behaviors of the onecomponent fluid subclass and the universal crossover functions recently estimated garrabos and bervillier phys rev e 74 021113 2006 from the bounde... | [['introducing', 'three', 'welldefined', 'dimensionless', 'numbers', 'we', 'establish', 'the', 'link', 'between', 'the', 'scale', 'dilatation', 'method', 'able', 'to', 'estimate', 'master', 'ie', 'unique', 'singular', 'behaviors', 'of', 'the', 'onecomponent', 'fluid', 'subclass', 'and', 'the', 'universal', 'crossover',... | [-0.12918782169175036, 0.11172554764088313, -0.07779732205957737, 0.00028612513868313917, -0.0665150013804998, -0.16033012163825333, 0.08931164706415795, 0.26270286758201866, -0.24041352021499132, -0.32118367621639987, -0.018713657855152874, -0.24535384138975785, -0.19244891888009524, 0.18574415274702435, -0.0285692341... |
707.3916 | High-fidelity ion-trap quantum computing with hyperfine clock states | We propose the implementation of a geometric-phase gate on
magnetic-field-insensitive qubits with $\hat{\sigma}^z$-dependent forces for
trapped ion quantum computing. The force is exerted by two laser beams in a
Raman configuration. Qubit-state dependency is achieved by a small frequency
detuning from the virtually-e... | quant-ph | we propose the implementation of a geometricphase gate on magneticfieldinsensitive qubits with hatsigmazdependent forces for trapped ion quantum computing the force is exerted by two laser beams in a raman configuration qubitstate dependency is achieved by a small frequency detuning from the virtuallyexcited state ion ... | [['we', 'propose', 'the', 'implementation', 'of', 'a', 'geometricphase', 'gate', 'on', 'magneticfieldinsensitive', 'qubits', 'with', 'hatsigmazdependent', 'forces', 'for', 'trapped', 'ion', 'quantum', 'computing', 'the', 'force', 'is', 'exerted', 'by', 'two', 'laser', 'beams', 'in', 'a', 'raman', 'configuration', 'qubi... | [-0.15736576818550627, 0.22342881391652755, 0.005112268216907978, 0.0042018134172798855, 0.02682717712596059, -0.19825360499736336, 0.11380606711738639, 0.42306450605392454, -0.20164458377597233, -0.32637536072482665, -0.006941698554955009, -0.24899627688444323, 0.002453554615688821, 0.23129088988320695, -0.03166230772... |
707.3917 | Weak Values and Continuous-Variable Entanglement Concentration | We demonstrate a general weak measurement model which allows Gaussian
preserving entanglement concentration of the two mode squeezed vacuum. The
power of this simple and elegant protocol is through the constraints it places
on possible ancilla states and measurement strategies that will allow
entanglement concentrati... | quant-ph | we demonstrate a general weak measurement model which allows gaussian preserving entanglement concentration of the two mode squeezed vacuum the power of this simple and elegant protocol is through the constraints it places on possible ancilla states and measurement strategies that will allow entanglement concentration ... | [['we', 'demonstrate', 'a', 'general', 'weak', 'measurement', 'model', 'which', 'allows', 'gaussian', 'preserving', 'entanglement', 'concentration', 'of', 'the', 'two', 'mode', 'squeezed', 'vacuum', 'the', 'power', 'of', 'this', 'simple', 'and', 'elegant', 'protocol', 'is', 'through', 'the', 'constraints', 'it', 'place... | [-0.11671098219641649, 0.12442294530132238, -0.10982351839980659, 0.06866172609083793, -0.05389174250338007, -0.22583253276808296, 0.08983751802760012, 0.36400566771626475, -0.25393498791929553, -0.27314908144009464, 0.08500367995652863, -0.21722645985856243, -0.19492867475046832, 0.2198564980781692, -0.055813077883794... |
707.3918 | Spin separation in a T ballistic nanojunction due to
lateral-confinement-induced spin-orbit-coupling | We propose a new scheme of spin filtering employing ballistic nanostructures
in two dimensional electron gases (2DEGs). The proposal is essentially based on
the spin-orbit (SO) interaction arising from the lateral confining electric
field. This sets the basic difference with other works employing ballistic
crosses an... | cond-mat.mes-hall | we propose a new scheme of spin filtering employing ballistic nanostructures in two dimensional electron gases 2degs the proposal is essentially based on the spinorbit so interaction arising from the lateral confining electric field this sets the basic difference with other works employing ballistic crosses and t junct... | [['we', 'propose', 'a', 'new', 'scheme', 'of', 'spin', 'filtering', 'employing', 'ballistic', 'nanostructures', 'in', 'two', 'dimensional', 'electron', 'gases', '2degs', 'the', 'proposal', 'is', 'essentially', 'based', 'on', 'the', 'spinorbit', 'so', 'interaction', 'arising', 'from', 'the', 'lateral', 'confining', 'ele... | [-0.16070145525985485, 0.15031705630068073, -0.06623505293113044, 0.002200229347158128, -0.029005561565232072, -0.15736060261201018, 0.030018460570683338, 0.40450241330724496, -0.28776729127151385, -0.2729771903031466, 0.010456361618832264, -0.25509400305967045, -0.12683073214740834, 0.22487455479100218, 0.006919296116... |
707.3919 | A graviton propagator for inflation | We construct the scalar and graviton propagator in quasi de Sitter space up
to first order in the slow roll parameter $\epsilon\equiv -\dot{H}/H^2$. After
a rescaling, the propagators are similar to those in de Sitter space with an
$\epsilon$ correction to the effective mass. The limit $\epsilon\to 0$
corresponds to ... | gr-qc | we construct the scalar and graviton propagator in quasi de sitter space up to first order in the slow roll parameter epsilonequiv dothh2 after a rescaling the propagators are similar to those in de sitter space with an epsilon correction to the effective mass the limit epsilonto 0 corresponds to the e3 vacuum that bre... | [['we', 'construct', 'the', 'scalar', 'and', 'graviton', 'propagator', 'in', 'quasi', 'de', 'sitter', 'space', 'up', 'to', 'first', 'order', 'in', 'the', 'slow', 'roll', 'parameter', 'epsilonequiv', 'dothh2', 'after', 'a', 'rescaling', 'the', 'propagators', 'are', 'similar', 'to', 'those', 'in', 'de', 'sitter', 'space'... | [-0.14424050493107643, 0.22594051036739984, -0.17208900218829512, 0.13739188640611247, -0.12145414935075678, -0.10401624185760738, -0.029762883161311038, 0.2957693092757836, -0.16734461393207312, -0.2674359661992639, 0.05308915080386214, -0.2192163317464292, -0.06743918976862914, 0.08634286874439567, -0.038127435935894... |
707.392 | Higher signal harmonics, LISA's angular resolution, and dark energy | It is generally believed that the angular resolution of the Laser
Interferometer Space Antenna (LISA) for binary supermassive black holes (SMBH)
will not be good enough to identify the host galaxy or galaxy cluster. This
conclusion, based on using only the dominant harmonic of the binary SMBH
signal, changes substant... | astro-ph gr-qc | it is generally believed that the angular resolution of the laser interferometer space antenna lisa for binary supermassive black holes smbh will not be good enough to identify the host galaxy or galaxy cluster this conclusion based on using only the dominant harmonic of the binary smbh signal changes substantially whe... | [['it', 'is', 'generally', 'believed', 'that', 'the', 'angular', 'resolution', 'of', 'the', 'laser', 'interferometer', 'space', 'antenna', 'lisa', 'for', 'binary', 'supermassive', 'black', 'holes', 'smbh', 'will', 'not', 'be', 'good', 'enough', 'to', 'identify', 'the', 'host', 'galaxy', 'or', 'galaxy', 'cluster', 'this... | [-0.1195022152646743, 0.11913502059178427, -0.05286424041696591, 0.14260835101867997, -0.12957991098664934, -0.08292991805501515, 0.04050621800161025, 0.3588603717944352, -0.20073679435881786, -0.3543892707384657, 0.06284638848046598, -0.2791069232953305, -0.05301332702038053, 0.2523405361989717, -0.0075291353787179105... |
707.3921 | Properties of 12Be and 11Be in terms of single-particle motion in
deformed potential | Inspired by the recent measurement of the B(E2;$0_{2}^{+} \to 2_{1}^+$) and
B(E0;$0_{2}^{+} \to 0_{1}^+$) values in $^{12}$Be, we give an interpretation of
available spectroscopic data on both $^{12}$Be and $^{11}$Be, using a simple
model which contains the essential feature of these two nuclei; the presence of
weakl... | nucl-th | inspired by the recent measurement of the be20_2 to 2_1 and be00_2 to 0_1 values in 12be we give an interpretation of available spectroscopic data on both 12be and 11be using a simple model which contains the essential feature of these two nuclei the presence of weaklybound neutrons in deformed potentials the agreement... | [['inspired', 'by', 'the', 'recent', 'measurement', 'of', 'the', 'be20_2', 'to', '2_1', 'and', 'be00_2', 'to', '0_1', 'values', 'in', '12be', 'we', 'give', 'an', 'interpretation', 'of', 'available', 'spectroscopic', 'data', 'on', 'both', '12be', 'and', '11be', 'using', 'a', 'simple', 'model', 'which', 'contains', 'the'... | [-0.05269982219012319, 0.11939443271726106, -0.06587255464029917, 0.0978487901797896, 0.03829219019499378, -0.10027673684627465, 0.04135718535415936, 0.3619715380819811, -0.15477828433116278, -0.3208254212142387, -0.032192974889556455, -0.33947690268573555, -0.04821552203941173, 0.19542659861980466, 0.03642577255495648... |
707.3922 | BRST, anti-BRST and gerbes | We discuss BRST and anti--BRST transformations for an Abelian antisymmetric
gauge field in 4D and find that, in order for them to anticommute, we have to
impose a condition on the auxiliary fields. This condition is similar to the
Curci-Ferrari condition for the 4D non--Abelian 1-form gauge theories and
represents a ... | hep-th | we discuss brst and antibrst transformations for an abelian antisymmetric gauge field in 4d and find that in order for them to anticommute we have to impose a condition on the auxiliary fields this condition is similar to the curciferrari condition for the 4d nonabelian 1form gauge theories and represents a consistency... | [['we', 'discuss', 'brst', 'and', 'antibrst', 'transformations', 'for', 'an', 'abelian', 'antisymmetric', 'gauge', 'field', 'in', '4d', 'and', 'find', 'that', 'in', 'order', 'for', 'them', 'to', 'anticommute', 'we', 'have', 'to', 'impose', 'a', 'condition', 'on', 'the', 'auxiliary', 'fields', 'this', 'condition', 'is',... | [-0.16843659184949913, 0.14908494205665943, -0.08528762671270783, 0.10870089386733844, -0.16043041592713483, -0.11801196744703908, -0.010747480249397227, 0.3806153307944901, -0.18461393172247814, -0.2696149853951077, 0.07525551004320882, -0.19383059688315718, -0.1874133168537285, 0.09488866780644532, -0.100796165338419... |
707.3923 | Filtering of spin currents based on ballistic ring | Quantum interference effects in rings provide suitable means for controlling
spin at mesoscopic scales. Here we apply such a control mechanism to the
spin-dependent transport in a ballistic quasi one dimensional ring patterned in
two dimensional electron gases (2DEGs). The study is essentially based on the
{\it natur... | cond-mat.mes-hall | quantum interference effects in rings provide suitable means for controlling spin at mesoscopic scales here we apply such a control mechanism to the spindependent transport in a ballistic quasi one dimensional ring patterned in two dimensional electron gases 2degs the study is essentially based on the it natural spinor... | [['quantum', 'interference', 'effects', 'in', 'rings', 'provide', 'suitable', 'means', 'for', 'controlling', 'spin', 'at', 'mesoscopic', 'scales', 'here', 'we', 'apply', 'such', 'a', 'control', 'mechanism', 'to', 'the', 'spindependent', 'transport', 'in', 'a', 'ballistic', 'quasi', 'one', 'dimensional', 'ring', 'patter... | [-0.19161933533707495, 0.18181516679941356, -0.014308465233130502, 0.046677886939624096, -0.014016183241981374, -0.139877518944817, -0.010978614116506375, 0.3534562362457168, -0.3074016114280107, -0.24879746360858604, 0.034411803285381896, -0.27551875660711206, -0.1252569810627855, 0.1985003448039095, 0.039756293667579... |
707.3924 | Parking in the city | We show that the spacing distribution between parked cars can be obtained as
a solution of certain linear distributional fixed point equation. The results
are compared with the data measured on the streets of Hradec Kralove. We also
discuss a relation of this results to the random matrix theory.
| nlin.AO nlin.CG | we show that the spacing distribution between parked cars can be obtained as a solution of certain linear distributional fixed point equation the results are compared with the data measured on the streets of hradec kralove we also discuss a relation of this results to the random matrix theory | [['we', 'show', 'that', 'the', 'spacing', 'distribution', 'between', 'parked', 'cars', 'can', 'be', 'obtained', 'as', 'a', 'solution', 'of', 'certain', 'linear', 'distributional', 'fixed', 'point', 'equation', 'the', 'results', 'are', 'compared', 'with', 'the', 'data', 'measured', 'on', 'the', 'streets', 'of', 'hradec'... | [-0.1214400235107763, 0.09775476044717621, -0.13333925121325127, 0.06368146490731692, -0.02589677175645657, -0.0895049425159046, 0.07850782336181704, 0.37874152293389146, -0.29751269440067574, -0.2666869317577716, 0.11145839940117513, -0.3431380723028424, -0.16760729017489134, 0.20490414837494175, -0.05874054767984025,... |
707.3925 | Use of a $d$-Constraint During LDPC Decoding in a Bliss Scheme | Bliss schemes of a run length limited (RLL) codec in combination with an LDPC
codec, generate LDPC parity bits over a systematic sequence of RLL channel bits
that are inherently redundant as they satisfy e.g. a $d=1$ minimum run length
constraint. That is the subsequences consisting of runs of length $d=1$, viz.
$...... | cs.IT math.IT | bliss schemes of a run length limited rll codec in combination with an ldpc codec generate ldpc parity bits over a systematic sequence of rll channel bits that are inherently redundant as they satisfy eg a d1 minimum run length constraint that is the subsequences consisting of runs of length d1 viz 010 and 101 cannot o... | [['bliss', 'schemes', 'of', 'a', 'run', 'length', 'limited', 'rll', 'codec', 'in', 'combination', 'with', 'an', 'ldpc', 'codec', 'generate', 'ldpc', 'parity', 'bits', 'over', 'a', 'systematic', 'sequence', 'of', 'rll', 'channel', 'bits', 'that', 'are', 'inherently', 'redundant', 'as', 'they', 'satisfy', 'eg', 'a', 'd1'... | [-0.2237633794003152, 0.12305213437153058, -0.07158528115664331, 0.037995423801698305, -0.02710100028393719, -0.2842595840036471, 0.13222893783982614, 0.37389231657161454, -0.2900800333991078, -0.2949455927787277, 0.08550565651856107, -0.25827861900036114, -0.11143806625250016, 0.1288542138920912, -0.12953424492836682,... |
707.3926 | Covering spaces and the Kakimizu complex | In 1992, Osamu Kakimizu defined a complex that has become known as the
Kakimizu complex of a knot. Vertices correspond to isotopy classes of minimal
genus Seifert surfaces of the knot. Higher dimensional simplices correspond to
collections of such classes of Seifert surfaces that admit disjoint
representatives. We sh... | math.GT | in 1992 osamu kakimizu defined a complex that has become known as the kakimizu complex of a knot vertices correspond to isotopy classes of minimal genus seifert surfaces of the knot higher dimensional simplices correspond to collections of such classes of seifert surfaces that admit disjoint representatives we show tha... | [['in', '1992', 'osamu', 'kakimizu', 'defined', 'a', 'complex', 'that', 'has', 'become', 'known', 'as', 'the', 'kakimizu', 'complex', 'of', 'a', 'knot', 'vertices', 'correspond', 'to', 'isotopy', 'classes', 'of', 'minimal', 'genus', 'seifert', 'surfaces', 'of', 'the', 'knot', 'higher', 'dimensional', 'simplices', 'corr... | [-0.24703085554594342, 0.11314630931751295, -0.049368300881575455, 0.07965275875546715, -0.12004722258584066, -0.1791671882468191, -0.023748744651675223, 0.3541271808895875, -0.24828567430377008, -0.30574258918111974, 0.04564496439415962, -0.27187169515951115, -0.23275271120735191, 0.19080505763942546, -0.2032527407038... |
707.3927 | Dynamic structure factor of Fermi superfluid in the BEC-BCS crossover | We consider cigar shaped Fermi superfluid in the BEC-BCS crossover. Using
polytropic form of equation of state, we derive low energy multibranch bosonic
excitations and the corresponding density fluctuations in three different
regimes along the crossover, namely weak-coupling BCS, unitarity and molecular
BEC regimes.... | cond-mat.other | we consider cigar shaped fermi superfluid in the becbcs crossover using polytropic form of equation of state we derive low energy multibranch bosonic excitations and the corresponding density fluctuations in three different regimes along the crossover namely weakcoupling bcs unitarity and molecular bec regimes bragg sp... | [['we', 'consider', 'cigar', 'shaped', 'fermi', 'superfluid', 'in', 'the', 'becbcs', 'crossover', 'using', 'polytropic', 'form', 'of', 'equation', 'of', 'state', 'we', 'derive', 'low', 'energy', 'multibranch', 'bosonic', 'excitations', 'and', 'the', 'corresponding', 'density', 'fluctuations', 'in', 'three', 'different'... | [-0.17593726270239463, 0.25637842455299426, -0.13194265991280024, 0.05760818444382907, -0.044049924950708044, -0.13668505490164864, 0.05312612553508106, 0.34871707020158116, -0.27740792722483587, -0.2552014569836584, -0.04497809142974967, -0.2828670645640655, -0.07288473762402481, 0.13060434595470063, 0.044465599852529... |
707.3928 | Asymptotic expansions for functions of the increments of certain
Gaussian processes | Let $G=\{G(x),x\ge 0\}$ be a mean zero Gaussian process with stationary
increments and set $\sigma^2(|x-y|)= E(G(x)-G(y))^2$. Let $f$ be a function
with $Ef^{2}(\eta)<\ff$, where $\eta=N(0,1)$. When $\sigma^2$ is regularly
varying at zero and \[
\lim_{h\to 0}{h^2\over \sigma^2(h)}= 0\qquad {and}\qquad \lim_{h\to
0}... | math.PR | let ggxxge 0 be a mean zero gaussian process with stationary increments and set sigma2xy egxgy2 let f be a function with ef2etaff where etan01 when sigma2 is regularly varying at zero and lim_hto 0h2over sigma2h 0qquad andqquad lim_hto 0sigma2hover h 0 quad but quad d2over ds2sigma2sj_0 is locally integrable for some i... | [['let', 'ggxxge', '0', 'be', 'a', 'mean', 'zero', 'gaussian', 'process', 'with', 'stationary', 'increments', 'and', 'set', 'sigma2xy', 'egxgy2', 'let', 'f', 'be', 'a', 'function', 'with', 'ef2etaff', 'where', 'etan01', 'when', 'sigma2', 'is', 'regularly', 'varying', 'at', 'zero', 'and', 'lim_hto', '0h2over', 'sigma2h'... | [-0.14782629122465163, 0.17721956832891053, -0.02722285895062418, -0.02756971225932213, -0.06339632125367978, -0.25368257505476643, -0.07022688286807174, 0.33747027282089254, -0.3468718059874814, -0.12629122609786433, 0.12476715089983424, -0.3567900977086747, -0.06981093925959163, 0.11193860191637757, -0.07021019338555... |
707.3929 | The sum rules for the spin dependent structure functions corresponding
to the moment at $n=0$ | Sum rules for the spin dependent structure functions corresponding to the
moment at $n=0$ derived from the current algebra based on the canonical
quantization on the null-plane are reviewed.
| hep-ph | sum rules for the spin dependent structure functions corresponding to the moment at n0 derived from the current algebra based on the canonical quantization on the nullplane are reviewed | [['sum', 'rules', 'for', 'the', 'spin', 'dependent', 'structure', 'functions', 'corresponding', 'to', 'the', 'moment', 'at', 'n0', 'derived', 'from', 'the', 'current', 'algebra', 'based', 'on', 'the', 'canonical', 'quantization', 'on', 'the', 'nullplane', 'are', 'reviewed']] | [-0.0805476800506485, 0.10725904029296261, -0.04154733852643905, 0.08265664611525576, -0.09017349880766766, -0.0403651826019431, 0.041072355143741926, 0.3277708798133094, -0.3005661150633261, -0.1938638881105801, 0.10496958080229574, -0.2660147947227133, -0.09259190243379824, 0.1741909767212025, 0.03964580479880859, 0.... |
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