id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
706.3514 | Charge Inversion of Divalent Ionic Solutions in Silica Channels | Recent experiments (F.H.J. Van Der Heyden et al., PRL 96, 224502 (2006)) of
streaming currents in silica nanochannels with divalent ions report charge
inversion, i.e. interfacial charges attracting counterions in excess of their
own nominal charge, in conflict with existing theoretical and simulation
results. We reve... | cond-mat.mtrl-sci | recent experiments fhj van der heyden et al prl 96 224502 2006 of streaming currents in silica nanochannels with divalent ions report charge inversion ie interfacial charges attracting counterions in excess of their own nominal charge in conflict with existing theoretical and simulation results we reveal the mechanism ... | [['recent', 'experiments', 'fhj', 'van', 'der', 'heyden', 'et', 'al', 'prl', '96', '224502', '2006', 'of', 'streaming', 'currents', 'in', 'silica', 'nanochannels', 'with', 'divalent', 'ions', 'report', 'charge', 'inversion', 'ie', 'interfacial', 'charges', 'attracting', 'counterions', 'in', 'excess', 'of', 'their', 'ow... | [-0.08837581232705331, 0.09482793829978463, -0.011797430736825187, 0.0007444482910981837, 0.029183022776975275, -0.10459129528162327, 0.07328115864111943, 0.3719955562871504, -0.19063140296976658, -0.35520975426473517, -0.0044756511639942355, -0.3501925454227293, -0.1823027349235688, 0.17131146698437155, -0.03065240218... |
706.3515 | Wedderburn polynomials over division rings, II | A polynomial $f(t)$ in an Ore extension $K[t;S,D]$ over a division ring $K$
is a Wedderburn polynomial if $f(t)$ is monic and is the minimal polynomial of
an algebraic subset of $K$. These polynomials have been studied in "Wedderburn
polynomials over division rings,I (Journal of Pure and Applied Algebra, Vol.
186, (2... | math.RA | a polynomial ft in an ore extension ktsd over a division ring k is a wedderburn polynomial if ft is monic and is the minimal polynomial of an algebraic subset of k these polynomials have been studied in wedderburn polynomials over division ringsi journal of pure and applied algebra vol 186 2004 4376 in this paper we co... | [['a', 'polynomial', 'ft', 'in', 'an', 'ore', 'extension', 'ktsd', 'over', 'a', 'division', 'ring', 'k', 'is', 'a', 'wedderburn', 'polynomial', 'if', 'ft', 'is', 'monic', 'and', 'is', 'the', 'minimal', 'polynomial', 'of', 'an', 'algebraic', 'subset', 'of', 'k', 'these', 'polynomials', 'have', 'been', 'studied', 'in', '... | [-0.18018316191931566, 0.014790926949353888, -0.12593427473413094, -0.01568334528267206, -0.06158611772670632, -0.08432375064917973, -0.021793707290531268, 0.3088135624703552, -0.33259744991415313, -0.17757266386012946, 0.10239611694899699, -0.20497256397225316, -0.15631473050231026, 0.1822640921920538, -0.142610161376... |
706.3516 | New Developments and Future Perspectives of Gaseous Detectors | Gaseous detectors are fundamental components of all present and planned high
energy physics experiments.
Over the past decade two representatives (GEM, Micromegas) of the
Micro-Pattern Gas Detector (MPGD) concept have become increasingly important;
the high radiation resistance and excellent spatial and time resolu... | physics.ins-det | gaseous detectors are fundamental components of all present and planned high energy physics experiments over the past decade two representatives gem micromegas of the micropattern gas detector mpgd concept have become increasingly important the high radiation resistance and excellent spatial and time resolution make th... | [['gaseous', 'detectors', 'are', 'fundamental', 'components', 'of', 'all', 'present', 'and', 'planned', 'high', 'energy', 'physics', 'experiments', 'over', 'the', 'past', 'decade', 'two', 'representatives', 'gem', 'micromegas', 'of', 'the', 'micropattern', 'gas', 'detector', 'mpgd', 'concept', 'have', 'become', 'increa... | [-0.030424742402930995, 0.136238056302743, -0.04720493248080678, 0.06370134622067491, -0.07591100002282133, -0.19282089471795258, -0.12753222634902694, 0.3497500889020685, -0.22861824776089498, -0.38785457115394073, 0.11066327545852792, -0.3248947098999171, -0.018997626540155334, 0.2556170530521494, 0.01385524193973881... |
706.3517 | Phase structure of matrix quantum mechanics at finite temperature | We study matrix quantum mechanics at finite temperature by Monte Carlo
simulation. The model is obtained by dimensionally reducing 10d U(N) pure
Yang-Mills theory to 1d. Following Aharony et al., one can view the same model
as describing the high temperature regime of (1+1)d U(N) super Yang-Mills
theory on a circle. ... | hep-th hep-lat | we study matrix quantum mechanics at finite temperature by monte carlo simulation the model is obtained by dimensionally reducing 10d un pure yangmills theory to 1d following aharony et al one can view the same model as describing the high temperature regime of 11d un super yangmills theory on a circle in this interpre... | [['we', 'study', 'matrix', 'quantum', 'mechanics', 'at', 'finite', 'temperature', 'by', 'monte', 'carlo', 'simulation', 'the', 'model', 'is', 'obtained', 'by', 'dimensionally', 'reducing', '10d', 'un', 'pure', 'yangmills', 'theory', 'to', '1d', 'following', 'aharony', 'et', 'al', 'one', 'can', 'view', 'the', 'same', 'm... | [-0.13890436217912497, 0.2210104860314459, -0.1029130527560876, 0.030577923533053615, -0.01839111651595984, -0.09121369315638535, 0.04284763813720437, 0.2905608173522696, -0.21580013104185863, -0.3030856730985908, 0.09036503841540448, -0.2904331458203897, -0.15592068803144266, 0.08328242177407988, -0.026671551067281415... |
706.3518 | Towards lattice simulation of the gauge theory duals to black holes and
hot strings | A generalization of the AdS/CFT conjecture postulates a duality between IIA
string theory and 16 supercharge Yang-Mills quantum mechanics in the large N 't
Hooft limit. At low temperatures string theory describes black holes, whose
thermodynamics may hence be studied using the dual quantum mechanics. This
quantum mec... | hep-lat gr-qc hep-th | a generalization of the adscft conjecture postulates a duality between iia string theory and 16 supercharge yangmills quantum mechanics in the large n t hooft limit at low temperatures string theory describes black holes whose thermodynamics may hence be studied using the dual quantum mechanics this quantum mechanics i... | [['a', 'generalization', 'of', 'the', 'adscft', 'conjecture', 'postulates', 'a', 'duality', 'between', 'iia', 'string', 'theory', 'and', '16', 'supercharge', 'yangmills', 'quantum', 'mechanics', 'in', 'the', 'large', 'n', 't', 'hooft', 'limit', 'at', 'low', 'temperatures', 'string', 'theory', 'describes', 'black', 'hol... | [-0.08879286363177623, 0.2085371357686654, -0.10142092659225455, 0.10029995627822548, -0.023711362836669043, -0.17707799807976699, 0.05810465562960113, 0.3232622324867407, -0.20134515406061837, -0.26134355196457665, 0.09559078154537322, -0.2825883664469681, -0.12964173291038605, 0.11631931434506744, -0.0503828518982724... |
706.3519 | Triggering Mechanism for the Filament Eruption on 2005 September 13 in
Active Region NOAA 10808 | On 2005 September 13 a filament eruption accompanied by a halo CME occurred
in the most flare-productive active region NOAA 10808 in Solar Cycle 23. Using
multi-wavelength observations before the filament eruption on Sep. 13th, we
investigate the processes leading to the catastrophic eruption. We find that
the filame... | astro-ph | on 2005 september 13 a filament eruption accompanied by a halo cme occurred in the most flareproductive active region noaa 10808 in solar cycle 23 using multiwavelength observations before the filament eruption on sep 13th we investigate the processes leading to the catastrophic eruption we find that the filament slowl... | [['on', '2005', 'september', '13', 'a', 'filament', 'eruption', 'accompanied', 'by', 'a', 'halo', 'cme', 'occurred', 'in', 'the', 'most', 'flareproductive', 'active', 'region', 'noaa', '10808', 'in', 'solar', 'cycle', '23', 'using', 'multiwavelength', 'observations', 'before', 'the', 'filament', 'eruption', 'on', 'sep'... | [-0.13770906204682137, 0.2095893930403118, -0.018874326451378088, 0.08686042802702523, -0.08385344767178682, -0.0354385588441065, 0.08507264944465748, 0.4274637809159297, -0.20943320131784807, -0.3234981720419496, 0.11908748675872875, -0.24366506759935383, -0.13494357167418752, 0.17474366147417753, -0.05104845145137148... |
706.352 | On probabilities for separating sets of order statistics | Consider a set of order statistics that arise from sorting samples from two
different populations, each with their own, possibly different distribution
function. The probability that these order statistics fall in disjoint, ordered
intervals, and that of the smallest statistics, a certain number come from the
first p... | stat.CO math.PR math.ST stat.TH | consider a set of order statistics that arise from sorting samples from two different populations each with their own possibly different distribution function the probability that these order statistics fall in disjoint ordered intervals and that of the smallest statistics a certain number come from the first populatio... | [['consider', 'a', 'set', 'of', 'order', 'statistics', 'that', 'arise', 'from', 'sorting', 'samples', 'from', 'two', 'different', 'populations', 'each', 'with', 'their', 'own', 'possibly', 'different', 'distribution', 'function', 'the', 'probability', 'that', 'these', 'order', 'statistics', 'fall', 'in', 'disjoint', 'o... | [-0.13168876316575778, 0.1410924225956911, -0.07350585365756637, 0.07391922870634257, -0.01192230834913928, -0.0846777602786287, 0.11150956708782662, 0.300088076852262, -0.27550076512575505, -0.35924802075273227, 0.08505841096519448, -0.2822453584522009, -0.0965227800687509, 0.18389832804955186, -0.07363316030906779, 0... |
706.3521 | Towards the Typology of Elections at Russia | A distinction in reasons and motives for choosing a particular political
leader establishes the key difference between older and young democracy. The
former is based on electoral history, while the latter is based on feelings and
personal attitude. Besides, a comparatively abundant number of political
figures (person... | physics.soc-ph | a distinction in reasons and motives for choosing a particular political leader establishes the key difference between older and young democracy the former is based on electoral history while the latter is based on feelings and personal attitude besides a comparatively abundant number of political figures persons or pa... | [['a', 'distinction', 'in', 'reasons', 'and', 'motives', 'for', 'choosing', 'a', 'particular', 'political', 'leader', 'establishes', 'the', 'key', 'difference', 'between', 'older', 'and', 'young', 'democracy', 'the', 'former', 'is', 'based', 'on', 'electoral', 'history', 'while', 'the', 'latter', 'is', 'based', 'on', '... | [-0.14909893322338472, 0.10013753083870322, -0.1142637720648326, 0.09696197171131668, -0.1498518518780415, -0.15679915580062234, 0.14528004736813785, 0.32645268498786856, -0.20480229571892494, -0.31074023747905377, 0.04922208425566731, -0.3133120066486299, -0.13411003191873025, 0.1506576344064361, -0.14027493022584997,... |
706.3522 | A dynamical law for slow crack growth in polycarbonate films | We study experimentally the slow growth of a single crack in polycarbonate
films submitted to uniaxial and constant imposed stress. For this visco-plastic
material, we uncover a dynamical law that describes the dependence of the
instantaneous crack velocity with experimental parameters. The law involves a
Dugdale-Bar... | physics.class-ph | we study experimentally the slow growth of a single crack in polycarbonate films submitted to uniaxial and constant imposed stress for this viscoplastic material we uncover a dynamical law that describes the dependence of the instantaneous crack velocity with experimental parameters the law involves a dugdalebarenblatt... | [['we', 'study', 'experimentally', 'the', 'slow', 'growth', 'of', 'a', 'single', 'crack', 'in', 'polycarbonate', 'films', 'submitted', 'to', 'uniaxial', 'and', 'constant', 'imposed', 'stress', 'for', 'this', 'viscoplastic', 'material', 'we', 'uncover', 'a', 'dynamical', 'law', 'that', 'describes', 'the', 'dependence', ... | [-0.16695339671285772, 0.1690315226807945, -0.15048631955240224, -0.052028121258371286, -0.10820025081645597, -0.11385327619909485, 0.02677745107133445, 0.3686185330089584, -0.32092775395014195, -0.23242779541760683, 0.03135919575170438, -0.2616370419493398, -0.1534981185104698, 0.1730475768295897, -0.03534181217184743... |
706.3523 | There Exist some Omega-Powers of Any Borel Rank | Omega-powers of finitary languages are languages of infinite words
(omega-languages) in the form V^omega, where V is a finitary language over a
finite alphabet X. They appear very naturally in the characterizaton of regular
or context-free omega-languages. Since the set of infinite words over a finite
alphabet X can ... | cs.LO cs.CC math.LO | omegapowers of finitary languages are languages of infinite words omegalanguages in the form vomega where v is a finitary language over a finite alphabet x they appear very naturally in the characterizaton of regular or contextfree omegalanguages since the set of infinite words over a finite alphabet x can be equipped ... | [['omegapowers', 'of', 'finitary', 'languages', 'are', 'languages', 'of', 'infinite', 'words', 'omegalanguages', 'in', 'the', 'form', 'vomega', 'where', 'v', 'is', 'a', 'finitary', 'language', 'over', 'a', 'finite', 'alphabet', 'x', 'they', 'appear', 'very', 'naturally', 'in', 'the', 'characterizaton', 'of', 'regular',... | [-0.16932909155543396, 0.15924798116588437, -0.0624211945566025, 0.13121472723049954, -0.13556944770130883, -0.18632329553913543, 0.09381456827535667, 0.3675305193245291, -0.3159863341021984, -0.1976715552789921, 0.0923372157500748, -0.2876719372461545, -0.1195748024178111, 0.17530470968437017, -0.1536426059777206, 0.0... |
706.3524 | Relative velocities among accreting planetesimals in binary systems: the
circumbinary case | We numerically investigate the possibility of planetesimal accretion in
circumbinary disks, under the coupled influence of both stars' secular
perturbations and friction due to the gaseous component of the protoplanetary
disk. We focus on one crucial parameter: the distribution of encounter
velocities between planete... | astro-ph | we numerically investigate the possibility of planetesimal accretion in circumbinary disks under the coupled influence of both stars secular perturbations and friction due to the gaseous component of the protoplanetary disk we focus on one crucial parameter the distribution of encounter velocities between planetesimals... | [['we', 'numerically', 'investigate', 'the', 'possibility', 'of', 'planetesimal', 'accretion', 'in', 'circumbinary', 'disks', 'under', 'the', 'coupled', 'influence', 'of', 'both', 'stars', 'secular', 'perturbations', 'and', 'friction', 'due', 'to', 'the', 'gaseous', 'component', 'of', 'the', 'protoplanetary', 'disk', '... | [-0.1693420111554779, 0.18565958406476343, -0.0497301017534674, 0.06484465411593096, -0.06090038750124605, -0.030726134587128303, 0.00680554803540489, 0.3397329154877776, -0.2474313245666532, -0.3053401834270182, 0.04603202807668008, -0.2611012958835712, -0.01997052118071894, 0.19058365762803556, -0.04332622870079879, ... |
706.3525 | Insights into the Evolution of Horizons from Non-Orthogonal Temporal
Coordinates | The introduction of coordinates representing the points of view of various
observers results in the possibility of horizons when acceleration and
gravitation are included. A horizon is a surface of possible light beams in a
region of space of finite distance from the observer, which means that since
nothing travels f... | gr-qc | the introduction of coordinates representing the points of view of various observers results in the possibility of horizons when acceleration and gravitation are included a horizon is a surface of possible light beams in a region of space of finite distance from the observer which means that since nothing travels faste... | [['the', 'introduction', 'of', 'coordinates', 'representing', 'the', 'points', 'of', 'view', 'of', 'various', 'observers', 'results', 'in', 'the', 'possibility', 'of', 'horizons', 'when', 'acceleration', 'and', 'gravitation', 'are', 'included', 'a', 'horizon', 'is', 'a', 'surface', 'of', 'possible', 'light', 'beams', '... | [-0.14771814907489175, 0.1523089530778534, -0.14709955872224217, 0.1123671245877631, -0.10911935740786437, -0.1439175062652858, 0.012698352341370919, 0.35329561319308855, -0.22260027460236972, -0.27916369669032715, 0.12526093804101063, -0.32610562806107957, -0.06914168014909071, 0.1982235974229109, -0.06733297118786333... |
706.3526 | "No Information Without Disturbance": Quantum Limitations of Measurement | In this contribution I review rigorous formulations of a variety of
limitations of measurability in quantum mechanics. To this end I begin with a
brief presentation of the conceptual tools of modern measurement theory. I will
make precise the notion that quantum measurements necessarily alter the system
under investi... | quant-ph | in this contribution i review rigorous formulations of a variety of limitations of measurability in quantum mechanics to this end i begin with a brief presentation of the conceptual tools of modern measurement theory i will make precise the notion that quantum measurements necessarily alter the system under investigati... | [['in', 'this', 'contribution', 'i', 'review', 'rigorous', 'formulations', 'of', 'a', 'variety', 'of', 'limitations', 'of', 'measurability', 'in', 'quantum', 'mechanics', 'to', 'this', 'end', 'i', 'begin', 'with', 'a', 'brief', 'presentation', 'of', 'the', 'conceptual', 'tools', 'of', 'modern', 'measurement', 'theory',... | [-0.09913586491671533, 0.0971705920647009, -0.13684517741834712, 0.04018281349296666, -0.10579791286234129, -0.14803248897226431, 0.06482589434461385, 0.29585006492117705, -0.291696148427298, -0.27734722197055817, 0.08905946732877548, -0.2675098022288185, -0.18118139651556642, 0.1456029549619909, -0.14608947493893615, ... |
706.3527 | Model for monitoring of a charge qubit using a radio-frequency quantum
point contact including experimental imperfections | The extension of quantum trajectory theory to incorporate realistic
imperfections in the measurement of solid-state qubits is important for quantum
computation, particularly for the purposes of state preparation and
error-correction as well as for readout of computations. Previously this has
been achieved for low-fre... | cond-mat.mes-hall quant-ph | the extension of quantum trajectory theory to incorporate realistic imperfections in the measurement of solidstate qubits is important for quantum computation particularly for the purposes of state preparation and errorcorrection as well as for readout of computations previously this has been achieved for lowfrequency ... | [['the', 'extension', 'of', 'quantum', 'trajectory', 'theory', 'to', 'incorporate', 'realistic', 'imperfections', 'in', 'the', 'measurement', 'of', 'solidstate', 'qubits', 'is', 'important', 'for', 'quantum', 'computation', 'particularly', 'for', 'the', 'purposes', 'of', 'state', 'preparation', 'and', 'errorcorrection'... | [-0.1483333644464217, 0.14167023608046514, -0.053918665963591954, 0.015197936736160156, -0.023139464175046393, -0.24627586953962843, 0.05325684545942667, 0.34876110784596565, -0.22966217180770454, -0.2733151393632094, 0.06827079740310596, -0.24434164150928459, -0.12350510300179436, 0.2773867350029336, -0.07532761583199... |
706.3528 | RF Shimming Pulses For Ex-Situ NMR Spectroscopy and Imaging Using B1
Inhomogeneities | I describe a method for generating "shim pulses" for NMR spectroscopy and
imaging (MRI) by taking advantage of the inherent inhomogeneity in the static
and radiofrequency (RF) fields of a one-sided NMR system. The RF inhomogeneity
here is assumed, without loss of generality, to be a linear gradient. General
polynomia... | physics.chem-ph | i describe a method for generating shim pulses for nmr spectroscopy and imaging mri by taking advantage of the inherent inhomogeneity in the static and radiofrequency rf fields of a onesided nmr system the rf inhomogeneity here is assumed without loss of generality to be a linear gradient general polynomials in the spa... | [['i', 'describe', 'a', 'method', 'for', 'generating', 'shim', 'pulses', 'for', 'nmr', 'spectroscopy', 'and', 'imaging', 'mri', 'by', 'taking', 'advantage', 'of', 'the', 'inherent', 'inhomogeneity', 'in', 'the', 'static', 'and', 'radiofrequency', 'rf', 'fields', 'of', 'a', 'onesided', 'nmr', 'system', 'the', 'rf', 'inh... | [-0.14089366744215392, 0.13319041680221502, -0.0587402361122017, 0.03138085537143432, -0.06397440198960962, -0.17164010284183434, 0.009336565816014702, 0.4354163986934843, -0.31656704244336914, -0.2543844519069, 0.05296594679132294, -0.22231111154958075, -0.07688686969613999, 0.21644927171648157, -0.015144215454822597,... |
706.3529 | Mesoscopic fluctuations of spin currents | Spin currents may be generated by applying bias voltages V to the
nanostructures even in the absence of spin-active ferromagnetic interfaces.
Most theoretical proposals concentrate on a concrete spin-orbit interaction and
on the disorder-averaged effect. It remains underappreciated that any
spin-orbit interaction pro... | cond-mat.mes-hall | spin currents may be generated by applying bias voltages v to the nanostructures even in the absence of spinactive ferromagnetic interfaces most theoretical proposals concentrate on a concrete spinorbit interaction and on the disorderaveraged effect it remains underappreciated that any spinorbit interaction produces ra... | [['spin', 'currents', 'may', 'be', 'generated', 'by', 'applying', 'bias', 'voltages', 'v', 'to', 'the', 'nanostructures', 'even', 'in', 'the', 'absence', 'of', 'spinactive', 'ferromagnetic', 'interfaces', 'most', 'theoretical', 'proposals', 'concentrate', 'on', 'a', 'concrete', 'spinorbit', 'interaction', 'and', 'on', ... | [-0.2179807571288294, 0.19770160694328, -0.00898458002310278, 0.03733345445118144, -0.03172494492167209, -0.201104717886346, 0.025127764724585045, 0.3596709194776212, -0.21948544619083563, -0.2728660180209539, -0.008179172267540334, -0.27923495456194264, -0.1437736615920678, 0.22748624253023064, 0.01912258331003225, 0.... |
706.353 | Rescattering effects and the determination of the gluon density for x <<
1 | We consider the possible role of rescattering effects in the determination of
the gluon density for the LHC from DIS data. We discuss a method that uses
results of s-channel calculations to estimate these effects, and comment on
potential applications to diffractive and multi-parton interactions.
| hep-ph | we consider the possible role of rescattering effects in the determination of the gluon density for the lhc from dis data we discuss a method that uses results of schannel calculations to estimate these effects and comment on potential applications to diffractive and multiparton interactions | [['we', 'consider', 'the', 'possible', 'role', 'of', 'rescattering', 'effects', 'in', 'the', 'determination', 'of', 'the', 'gluon', 'density', 'for', 'the', 'lhc', 'from', 'dis', 'data', 'we', 'discuss', 'a', 'method', 'that', 'uses', 'results', 'of', 'schannel', 'calculations', 'to', 'estimate', 'these', 'effects', 'a... | [-0.03894370194110605, 0.14402058378068938, -0.15327099029414562, 0.17016028196861346, -0.0726839969969458, -0.009832575016965469, 0.04768043595055739, 0.35684553649690415, -0.18594516190803714, -0.23941292866236633, -0.0011115405630941191, -0.3264008230012324, -0.12887187875005313, 0.15836940421722828, 0.0646837452012... |
706.3531 | On the Origin of the "Ridge" phenomenon induced by Jets in Heavy Ion
Collisions | We argue that "ridge" in 2-particle correlation function associated with hard
trigger at RHIC heavy ion collisions is naturally explained by an interrelation
of jet quenching and hydrodynamical transverse flow. The excess particles
forming the ridge are produced by QCD bremsstrahlung along the beam (and thus
have wid... | nucl-th | we argue that ridge in 2particle correlation function associated with hard trigger at rhic heavy ion collisions is naturally explained by an interrelation of jet quenching and hydrodynamical transverse flow the excess particles forming the ridge are produced by qcd bremsstrahlung along the beam and thus have wide rapid... | [['we', 'argue', 'that', 'ridge', 'in', '2particle', 'correlation', 'function', 'associated', 'with', 'hard', 'trigger', 'at', 'rhic', 'heavy', 'ion', 'collisions', 'is', 'naturally', 'explained', 'by', 'an', 'interrelation', 'of', 'jet', 'quenching', 'and', 'hydrodynamical', 'transverse', 'flow', 'the', 'excess', 'par... | [-0.06094540926638279, 0.20904051024467407, -0.1630560658673306, 0.12105980094030416, -0.034729541111946774, -0.08978763262981947, -0.10748610568096799, 0.4720095083708718, -0.27090709567530435, -0.272203589391926, -0.01535681981117245, -0.29734836452839414, 0.050214698118385935, 0.1506391902757662, 0.07115726047352458... |
706.3532 | On the Sharpness and Bias of Quantum Effects | The question of quantifying the sharpness (or unsharpness) of a quantum
mechanical effect is investigated. Apart from sharpness, another property,
bias, is found to be relevant for the joint measurability or coexistence of two
effects. Measures of bias will be defined and examples given.
| math-ph math.MP quant-ph | the question of quantifying the sharpness or unsharpness of a quantum mechanical effect is investigated apart from sharpness another property bias is found to be relevant for the joint measurability or coexistence of two effects measures of bias will be defined and examples given | [['the', 'question', 'of', 'quantifying', 'the', 'sharpness', 'or', 'unsharpness', 'of', 'a', 'quantum', 'mechanical', 'effect', 'is', 'investigated', 'apart', 'from', 'sharpness', 'another', 'property', 'bias', 'is', 'found', 'to', 'be', 'relevant', 'for', 'the', 'joint', 'measurability', 'or', 'coexistence', 'of', 't... | [-0.13314751395955682, 0.14666997353461655, -0.0770121044055982, 0.1035536099489863, -0.07448733811774715, -0.1562494210031053, 0.03192493250720541, 0.31853723542934115, -0.30713034996932204, -0.2788336233405227, 0.09514259827450257, -0.27922489045357163, -0.1483596206579188, 0.23194001669021833, -0.11120431952771138, ... |
706.3533 | Rotational dynamics of a superhelix towed in a Stokes fluid | Motivated by the intriguing motility of spirochetes (helically-shaped
bacteria that screw through viscous fluids due to the action of internal
periplasmic flagella), we examine the fundamental fluid dynamics of
superhelices translating and rotating in a Stokes fluid. A superhelical
structure may be thought of as a he... | physics.flu-dyn physics.bio-ph | motivated by the intriguing motility of spirochetes helicallyshaped bacteria that screw through viscous fluids due to the action of internal periplasmic flagella we examine the fundamental fluid dynamics of superhelices translating and rotating in a stokes fluid a superhelical structure may be thought of as a helix who... | [['motivated', 'by', 'the', 'intriguing', 'motility', 'of', 'spirochetes', 'helicallyshaped', 'bacteria', 'that', 'screw', 'through', 'viscous', 'fluids', 'due', 'to', 'the', 'action', 'of', 'internal', 'periplasmic', 'flagella', 'we', 'examine', 'the', 'fundamental', 'fluid', 'dynamics', 'of', 'superhelices', 'transla... | [-0.1809367755151886, 0.16479807880041855, -0.08871526199792112, 0.0031687226173068798, -0.06717960804933681, -0.14619771261832543, 0.009763483550050295, 0.36653508635503906, -0.2515828948521188, -0.26215093614799634, 0.0527058173995465, -0.226726181052093, -0.17864499025845101, 0.19418997976662858, -0.0195366069568055... |
706.3534 | Dynamic metastability in the two-dimensional Potts ferromagnet | We investigate the non-equilibrium dynamics of the 2D Potts model on the
square lattice after a quench below the discontinuous transition point. By
means of numerical simulations of systems with q =12,24 and 48 we observe the
onset of a stationary regime below the temperature-driven transition, in a
temperature inter... | cond-mat.stat-mech | we investigate the nonequilibrium dynamics of the 2d potts model on the square lattice after a quench below the discontinuous transition point by means of numerical simulations of systems with q 1224 and 48 we observe the onset of a stationary regime below the temperaturedriven transition in a temperature interval decr... | [['we', 'investigate', 'the', 'nonequilibrium', 'dynamics', 'of', 'the', '2d', 'potts', 'model', 'on', 'the', 'square', 'lattice', 'after', 'a', 'quench', 'below', 'the', 'discontinuous', 'transition', 'point', 'by', 'means', 'of', 'numerical', 'simulations', 'of', 'systems', 'with', 'q', '1224', 'and', '48', 'we', 'ob... | [-0.10046670123584261, 0.18702224983853546, -0.06000813445512285, 0.0013097229740641854, 0.03194746154142504, -0.1170384000461707, 0.09851805200215746, 0.3324666838954262, -0.24447080144222746, -0.2979230442817541, 0.11492837192441159, -0.30078851958697145, -0.11693193028344119, 0.18292089027075215, 0.04035133248234682... |
706.3535 | Avoidable Sets in The Bicyclic Inverse Semigroup | A subset $U$ of a set $S$ with a binary operation is called {\it avoidable}
if $S$ can be partitioned into two subsets $A$ and $B$ such that no element of
$U$ can be written as a product of two distinct elements of $A$ or as the
product of two distinct elements of $B$. The avoidable sets of the bicyclic
inverse semig... | math.CO math.GR | a subset u of a set s with a binary operation is called it avoidable if s can be partitioned into two subsets a and b such that no element of u can be written as a product of two distinct elements of a or as the product of two distinct elements of b the avoidable sets of the bicyclic inverse semigroup are classified | [['a', 'subset', 'u', 'of', 'a', 'set', 's', 'with', 'a', 'binary', 'operation', 'is', 'called', 'it', 'avoidable', 'if', 's', 'can', 'be', 'partitioned', 'into', 'two', 'subsets', 'a', 'and', 'b', 'such', 'that', 'no', 'element', 'of', 'u', 'can', 'be', 'written', 'as', 'a', 'product', 'of', 'two', 'distinct', 'elemen... | [-0.18806455710728187, 0.17020872065040749, -0.03112496516041574, 0.006396287915777066, -0.020223647530656308, -0.13312939963361714, 0.05321068424382247, 0.33785018051275983, -0.3612173740984872, -0.22432450338237686, 0.14592941261798842, -0.3406518378178589, -0.061800940358807566, 0.17540041417305474, -0.0145142772889... |
706.3536 | Stokes trapping and planet formation | It is believed that planets are formed by aggregation of dust particles
suspended in the turbulent gas forming accretion disks around developing stars.
We describe a mechanism, termed 'Stokes trapping', by which turbulence limits
the growth of aggregates of dust particles, so that their Stokes number
(defined as the ... | astro-ph | it is believed that planets are formed by aggregation of dust particles suspended in the turbulent gas forming accretion disks around developing stars we describe a mechanism termed stokes trapping by which turbulence limits the growth of aggregates of dust particles so that their stokes number defined as the ratio of ... | [['it', 'is', 'believed', 'that', 'planets', 'are', 'formed', 'by', 'aggregation', 'of', 'dust', 'particles', 'suspended', 'in', 'the', 'turbulent', 'gas', 'forming', 'accretion', 'disks', 'around', 'developing', 'stars', 'we', 'describe', 'a', 'mechanism', 'termed', 'stokes', 'trapping', 'by', 'which', 'turbulence', '... | [-0.1237361583755876, 0.22606873440836528, -0.06489636074498441, 0.06738058357042921, -0.04974738734286025, -0.06922420834923543, 0.01951392434731813, 0.3292015492418799, -0.27774212084421257, -0.2860544638129548, 0.05121408614671328, -0.22101721808639835, -0.07781725633184164, 0.16771664833017055, -0.04642589751504434... |
706.3537 | The Yang Mills system and cyclic covering of abelian varieties | In this paper, we consider a dynamical system related to the Yang-Mills
system for a field with gauge group SU(2). We solve this system in terms of
genus two hyperelliptic functions and we show that it is algebraic completely
integrable in the generalized sense.
| math-ph math.DS math.MP | in this paper we consider a dynamical system related to the yangmills system for a field with gauge group su2 we solve this system in terms of genus two hyperelliptic functions and we show that it is algebraic completely integrable in the generalized sense | [['in', 'this', 'paper', 'we', 'consider', 'a', 'dynamical', 'system', 'related', 'to', 'the', 'yangmills', 'system', 'for', 'a', 'field', 'with', 'gauge', 'group', 'su2', 'we', 'solve', 'this', 'system', 'in', 'terms', 'of', 'genus', 'two', 'hyperelliptic', 'functions', 'and', 'we', 'show', 'that', 'it', 'is', 'algebr... | [-0.19673100850460204, 0.11439286064441231, -0.10341869819570672, 0.07968057377464985, -0.042983688075434075, -0.12977497323299758, -0.03425245733921078, 0.3345072926445441, -0.2817904425954277, -0.21510426704348487, 0.10305045866037042, -0.24206098653799432, -0.2734535309401425, 0.16147641651332378, -0.126727770336649... |
706.3538 | Some solutions with torsion in Chern-Simons gravity and observable
effects | It is shown that in all odd dimensional Chern-Simons theories states in which
the torsion is non zero (but it can approach smoothly to zero outside suitable
regions) do exist. Some possible observational effects related to neutrino
oscillations are pointed out. In the theory of continuum media (in which
suitable defe... | gr-qc | it is shown that in all odd dimensional chernsimons theories states in which the torsion is non zero but it can approach smoothly to zero outside suitable regions do exist some possible observational effects related to neutrino oscillations are pointed out in the theory of continuum media in which suitable defects can ... | [['it', 'is', 'shown', 'that', 'in', 'all', 'odd', 'dimensional', 'chernsimons', 'theories', 'states', 'in', 'which', 'the', 'torsion', 'is', 'non', 'zero', 'but', 'it', 'can', 'approach', 'smoothly', 'to', 'zero', 'outside', 'suitable', 'regions', 'do', 'exist', 'some', 'possible', 'observational', 'effects', 'related... | [-0.15470326342761925, 0.22078686402315592, -0.10535852935892052, 0.16534954173172392, -0.10741110774688423, -0.185814302267007, -0.009210603932066389, 0.3292190185180161, -0.2529933858072249, -0.23798629783502803, 0.0801303196789288, -0.25156307489066043, -0.18831673107200825, 0.1837761177093631, -0.04593969241534246,... |
706.3539 | The diameter of random Cayley digraphs of given degree | We consider random Cayley digraphs of order $n$ with uniformly distributed
generating set of size $k$. Specifically, we are interested in the asymptotics
of the probability such a Cayley digraph has diameter two as $n\to\infty$ and
$k=f(n)$. We find a sharp phase transition from 0 to 1 at around $k = \sqrt{n
\log n}$... | math.CO | we consider random cayley digraphs of order n with uniformly distributed generating set of size k specifically we are interested in the asymptotics of the probability such a cayley digraph has diameter two as ntoinfty and kfn we find a sharp phase transition from 0 to 1 at around k sqrtn log n in particular if fn is as... | [['we', 'consider', 'random', 'cayley', 'digraphs', 'of', 'order', 'n', 'with', 'uniformly', 'distributed', 'generating', 'set', 'of', 'size', 'k', 'specifically', 'we', 'are', 'interested', 'in', 'the', 'asymptotics', 'of', 'the', 'probability', 'such', 'a', 'cayley', 'digraph', 'has', 'diameter', 'two', 'as', 'ntoinf... | [-0.17893072998191675, 0.23611482308394666, -0.004298576511496651, 0.018775961613215073, 0.0026024101652960844, -0.19192801306591087, 0.07274346021206482, 0.3933832263978927, -0.26240354502384644, -0.2428676883649567, 0.06870457167784427, -0.38322397418644116, -0.11574089911469407, 0.08280075461590204, -0.0382513202780... |
706.354 | Finite Element Formulation of the Bloch Equations with Dipolar Field
Effects | A Galerkin finite element (FEM) formulation for the Bloch equations with
dipolar field is presented which makes possible the derivation of weak
solutions to the Bloch equations. The FEM formulation has the advantage that
the equations of motion are local in real space, eliminating the global
truncation errors associa... | physics.chem-ph | a galerkin finite element fem formulation for the bloch equations with dipolar field is presented which makes possible the derivation of weak solutions to the bloch equations the fem formulation has the advantage that the equations of motion are local in real space eliminating the global truncation errors associated wi... | [['a', 'galerkin', 'finite', 'element', 'fem', 'formulation', 'for', 'the', 'bloch', 'equations', 'with', 'dipolar', 'field', 'is', 'presented', 'which', 'makes', 'possible', 'the', 'derivation', 'of', 'weak', 'solutions', 'to', 'the', 'bloch', 'equations', 'the', 'fem', 'formulation', 'has', 'the', 'advantage', 'that'... | [-0.14172940074434776, 0.09440806554777553, -0.1016248962737285, 0.028836708784030142, -0.08659041639459267, -0.09118213506122486, -0.03298964272017769, 0.349725960366679, -0.2800662002704117, -0.25922425138355976, 0.11941812126478704, -0.2266019827403714, -0.08159837635035176, 0.2043211911621849, 0.009557065271427122,... |
706.3541 | Beyond Gross-Pitaevskii Mean Field Theory | A large number of effects related to the phenomenon of Bose-Einstein
Condensation (BEC) can be understood in terms of lowest order mean field
theory, whereby the entire system is assumed to be condensed, with thermal and
quantum fluctuations completely ignored. Such a treatment leads to the
Gross-Pitaevskii Equation ... | cond-mat.other | a large number of effects related to the phenomenon of boseeinstein condensation bec can be understood in terms of lowest order mean field theory whereby the entire system is assumed to be condensed with thermal and quantum fluctuations completely ignored such a treatment leads to the grosspitaevskii equation gpe used ... | [['a', 'large', 'number', 'of', 'effects', 'related', 'to', 'the', 'phenomenon', 'of', 'boseeinstein', 'condensation', 'bec', 'can', 'be', 'understood', 'in', 'terms', 'of', 'lowest', 'order', 'mean', 'field', 'theory', 'whereby', 'the', 'entire', 'system', 'is', 'assumed', 'to', 'be', 'condensed', 'with', 'thermal', '... | [-0.10515800595206556, 0.18478269606307782, -0.06174756971018199, 0.07319845685515247, -0.045749647404714405, -0.1385247510412937, -1.7577259884200106e-05, 0.31473742394266113, -0.21313460683844732, -0.27980443222400875, 0.08732102140665875, -0.25583469310293955, -0.13809899066405182, 0.17310045821709613, -0.0228342426... |
706.3542 | Odd-frequency Pairs and Josephson Current through a Strong Ferromagnet | We study Josephson current in superconductor / diffusive ferromagnet
/superconductor junctions by using the recursive Green function method. When
the exchange potential in a ferromagnet is sufficiently large as compared to
the pair potential in a superconductor, an ensemble average of Josephson
current is much smalle... | cond-mat.supr-con | we study josephson current in superconductor diffusive ferromagnet superconductor junctions by using the recursive green function method when the exchange potential in a ferromagnet is sufficiently large as compared to the pair potential in a superconductor an ensemble average of josephson current is much smaller than ... | [['we', 'study', 'josephson', 'current', 'in', 'superconductor', 'diffusive', 'ferromagnet', 'superconductor', 'junctions', 'by', 'using', 'the', 'recursive', 'green', 'function', 'method', 'when', 'the', 'exchange', 'potential', 'in', 'a', 'ferromagnet', 'is', 'sufficiently', 'large', 'as', 'compared', 'to', 'the', 'p... | [-0.26719313228968533, 0.22010714190128056, -0.03756012775702402, 0.11003132350160741, -0.06548347892385209, -0.18264772193215323, 0.10243572542822221, 0.3511244414956309, -0.22276645849051419, -0.24202889275329653, -0.07691499619468231, -0.3793635115027428, -0.06579814921569778, 0.18988139263237827, 0.0892014268232742... |
706.3543 | Study of \pi^{-}p \to \eta n at low energies in a chiral constituent
quark model | A chiral quark model approach is extended to the study of the $\pi N$
scattering at low energies. The process of $\pi^{-}p \to \eta n$ near threshold
is investigated. The model is successful in describing the differential cross
sections and total cross section near the $\eta$ production threshold. The
roles of the re... | nucl-th | a chiral quark model approach is extended to the study of the pi n scattering at low energies the process of pip to eta n near threshold is investigated the model is successful in describing the differential cross sections and total cross section near the eta production threshold the roles of the resonances in nleq 2 s... | [['a', 'chiral', 'quark', 'model', 'approach', 'is', 'extended', 'to', 'the', 'study', 'of', 'the', 'pi', 'n', 'scattering', 'at', 'low', 'energies', 'the', 'process', 'of', 'pip', 'to', 'eta', 'n', 'near', 'threshold', 'is', 'investigated', 'the', 'model', 'is', 'successful', 'in', 'describing', 'the', 'differential',... | [-0.12264396831832669, 0.15746565369506282, -0.05262786194146775, 0.14416564964002146, 0.022311960192049632, -0.07582039813655363, 0.017739369163394605, 0.30756950844079256, -0.19231961263855263, -0.29431309470985556, -0.056045102772079934, -0.36088967578597103, -0.05129291636305271, 0.154451677205146, 0.05918860895059... |
706.3544 | The Origin of Large-scale HI structures in the Magellanic Bridge | We investigate the formation of a number of key large-scale HI features in
the ISM of the Magellanic Bridge using dissipationless numerical simulation
techniques. This study comprises the first direct comparison between detailed
HI maps of the Bridge and numerical simulations. We confirm that the SMC forms
two tidal ... | astro-ph | we investigate the formation of a number of key largescale hi features in the ism of the magellanic bridge using dissipationless numerical simulation techniques this study comprises the first direct comparison between detailed hi maps of the bridge and numerical simulations we confirm that the smc forms two tidal filam... | [['we', 'investigate', 'the', 'formation', 'of', 'a', 'number', 'of', 'key', 'largescale', 'hi', 'features', 'in', 'the', 'ism', 'of', 'the', 'magellanic', 'bridge', 'using', 'dissipationless', 'numerical', 'simulation', 'techniques', 'this', 'study', 'comprises', 'the', 'first', 'direct', 'comparison', 'between', 'det... | [-0.1350912624977589, 0.037817392430658785, -0.09449962949785855, 0.084982425360302, -0.04562812599714004, -0.014099713550099442, 0.059939558672222996, 0.3878222870970926, -0.23581990930195448, -0.2890309800634221, 0.059584615473267474, -0.24796638839958882, -0.12406070031143064, 0.19107621214765635, 0.0377844418004726... |
706.3545 | Cohen-Macaulayness and computation of Newton graded toric rings | Let $H$ be a positive semigroup in $\mathbb{Z}^d$ generated by $A$, and let
$K[H]$ be the associated semigroup ring over a field $K$. We investigate
heredity of the Cohen-Macaulay property from $K[H]$ to both its $A$-Newton
graded ring and to its face rings. We show by example that neither one inherits
in general the... | math.AC math.CO | let h be a positive semigroup in mathbbzd generated by a and let kh be the associated semigroup ring over a field k we investigate heredity of the cohenmacaulay property from kh to both its anewton graded ring and to its face rings we show by example that neither one inherits in general the cohenmacaulay property on th... | [['let', 'h', 'be', 'a', 'positive', 'semigroup', 'in', 'mathbbzd', 'generated', 'by', 'a', 'and', 'let', 'kh', 'be', 'the', 'associated', 'semigroup', 'ring', 'over', 'a', 'field', 'k', 'we', 'investigate', 'heredity', 'of', 'the', 'cohenmacaulay', 'property', 'from', 'kh', 'to', 'both', 'its', 'anewton', 'graded', 'r... | [-0.16152973396720383, 0.03165856778958859, -0.11125959372903044, 0.04947819791813926, -0.06905549149624668, -0.18028967071593077, -0.05919634829367603, 0.35468886827898993, -0.3737262156162713, -0.1260309960181313, 0.1394010401721037, -0.23365021940438194, -0.13796295768524697, 0.22058583898385903, -0.1253363771515118... |
706.3546 | stdchk: A Checkpoint Storage System for Desktop Grid Computing | Checkpointing is an indispensable technique to provide fault tolerance for
long-running high-throughput applications like those running on desktop grids.
This paper argues that a dedicated checkpoint storage system, optimized to
operate in these environments, can offer multiple benefits: reduce the load on
a traditio... | cs.DC | checkpointing is an indispensable technique to provide fault tolerance for longrunning highthroughput applications like those running on desktop grids this paper argues that a dedicated checkpoint storage system optimized to operate in these environments can offer multiple benefits reduce the load on a traditional file... | [['checkpointing', 'is', 'an', 'indispensable', 'technique', 'to', 'provide', 'fault', 'tolerance', 'for', 'longrunning', 'highthroughput', 'applications', 'like', 'those', 'running', 'on', 'desktop', 'grids', 'this', 'paper', 'argues', 'that', 'a', 'dedicated', 'checkpoint', 'storage', 'system', 'optimized', 'to', 'op... | [-0.19269607294117416, -0.002657352334285013, -0.07397371951206508, 0.008566713594636843, -0.09333575657558349, -0.22690881715855946, 0.11734326216467857, 0.39281465042129915, -0.2901894199309376, -0.3403592120308829, 0.13283930662730026, -0.23539753908838676, -0.08859125004113141, 0.2262807569218573, -0.14930307625077... |
706.3547 | Crossed products of k-graph C*-algebras by Z^l | An action of Z^l by automorphisms of a k-graph induces an action of Z^l by
automorphisms of the corresponding k-graph C*-algebra. We show how to construct
a (k+l)-graph whose C*-algebra coincides with the crossed product of the
original k-graph algebra by Z^l. We then investigate the structure of the
crossed-product ... | math.OA | an action of zl by automorphisms of a kgraph induces an action of zl by automorphisms of the corresponding kgraph calgebra we show how to construct a klgraph whose calgebra coincides with the crossed product of the original kgraph algebra by zl we then investigate the structure of the crossedproduct calgebra | [['an', 'action', 'of', 'zl', 'by', 'automorphisms', 'of', 'a', 'kgraph', 'induces', 'an', 'action', 'of', 'zl', 'by', 'automorphisms', 'of', 'the', 'corresponding', 'kgraph', 'calgebra', 'we', 'show', 'how', 'to', 'construct', 'a', 'klgraph', 'whose', 'calgebra', 'coincides', 'with', 'the', 'crossed', 'product', 'of',... | [-0.14985852099955083, 0.13626619384915103, -0.09054424069821834, -0.03932506596669555, -0.08454760416410863, -0.07937368905171752, -0.04808932385174557, 0.42203229188919067, -0.4384100400283933, -0.1859272133372724, 0.07012655714526772, -0.2702200720086694, -0.14341404458973556, 0.09768461234867573, -0.197496922872960... |
706.3548 | The Impact of Stellar Oscillations on Doppler Velocity Planet Searches | We present a quantitative investigation of the effect of stellar oscillations
on Doppler velocity planet searches. Using data from four asteroseismological
observation campaigns, we find a power law relationship between the noise
impact of these oscillations on Doppler velocities and both the
luminosity-to-mass of th... | astro-ph | we present a quantitative investigation of the effect of stellar oscillations on doppler velocity planet searches using data from four asteroseismological observation campaigns we find a power law relationship between the noise impact of these oscillations on doppler velocities and both the luminositytomass of the targ... | [['we', 'present', 'a', 'quantitative', 'investigation', 'of', 'the', 'effect', 'of', 'stellar', 'oscillations', 'on', 'doppler', 'velocity', 'planet', 'searches', 'using', 'data', 'from', 'four', 'asteroseismological', 'observation', 'campaigns', 'we', 'find', 'a', 'power', 'law', 'relationship', 'between', 'the', 'no... | [-0.09160263399756233, 0.1826971992022773, -0.08099363290659904, 0.10435800286814997, -0.13532644932169513, -0.09710871937252716, 0.07756183983011912, 0.3991501040038574, -0.14982948662974052, -0.39310152988028096, 0.12155543160218049, -0.28376803291380875, -0.02587092858009848, 0.28326084174731947, -0.0421817237588419... |
706.3549 | On the existence of the critical point in finite density lattice QCD | We propose a method to probe the nature of phase transitions in lattice QCD
at finite temperature and density, which is based on the investigation of an
effective potential as a function of the average plaquette. We analyze data
obtained in a simulation of two-flavor QCD using p4-improved staggered quarks
with bare q... | hep-lat hep-ph | we propose a method to probe the nature of phase transitions in lattice qcd at finite temperature and density which is based on the investigation of an effective potential as a function of the average plaquette we analyze data obtained in a simulation of twoflavor qcd using p4improved staggered quarks with bare quark m... | [['we', 'propose', 'a', 'method', 'to', 'probe', 'the', 'nature', 'of', 'phase', 'transitions', 'in', 'lattice', 'qcd', 'at', 'finite', 'temperature', 'and', 'density', 'which', 'is', 'based', 'on', 'the', 'investigation', 'of', 'an', 'effective', 'potential', 'as', 'a', 'function', 'of', 'the', 'average', 'plaquette',... | [-0.12264923695329344, 0.24303195001402855, -0.11636321807842857, 0.02919318219574052, -0.0002123621767774845, -0.06412767434570317, 0.14859379967674613, 0.3788152033618341, -0.15853451789007522, -0.27340557891875505, 0.035167949479121795, -0.2833340439538006, -0.07711135369027033, 0.05297335781506263, 0.08819663138516... |
706.355 | The mean curvature flow for isoparametric submanifolds | A submanifold in space forms is isoparametric if the normal bundle is flat
and principal curvatures along any parallel normal fields are constant. We
study the mean curvature flow with initial data an isoparametric submanifold in
Euclidean space and sphere. We show that the mean curvature flow preserves the
isoparame... | math.DG | a submanifold in space forms is isoparametric if the normal bundle is flat and principal curvatures along any parallel normal fields are constant we study the mean curvature flow with initial data an isoparametric submanifold in euclidean space and sphere we show that the mean curvature flow preserves the isoparametric... | [['a', 'submanifold', 'in', 'space', 'forms', 'is', 'isoparametric', 'if', 'the', 'normal', 'bundle', 'is', 'flat', 'and', 'principal', 'curvatures', 'along', 'any', 'parallel', 'normal', 'fields', 'are', 'constant', 'we', 'study', 'the', 'mean', 'curvature', 'flow', 'with', 'initial', 'data', 'an', 'isoparametric', 's... | [-0.25469246770364123, 0.10915331807544655, -0.11942371869967743, 0.05461160078124663, -0.11487768652740044, -0.10660430925063692, -0.1033248437399214, 0.4155850391593072, -0.2474058773126695, -0.14165926763830197, 0.09080703734335574, -0.27464872995367295, -0.13041819857022205, 0.11416115209024835, -0.1416296577202035... |
706.3551 | Supernovae as Probes of Extra Dimensions | Since the dawn of the new millennium, there has been a revived interest in
the concept of extra dimensions.In this scenario all the standard model matter
and gauge fields are confined to the 4 dimensions and only gravity can escape
to higher dimensions of the universe.This idea can be tested using table-top
experimen... | hep-ph | since the dawn of the new millennium there has been a revived interest in the concept of extra dimensionsin this scenario all the standard model matter and gauge fields are confined to the 4 dimensions and only gravity can escape to higher dimensions of the universethis idea can be tested using tabletop experiments col... | [['since', 'the', 'dawn', 'of', 'the', 'new', 'millennium', 'there', 'has', 'been', 'a', 'revived', 'interest', 'in', 'the', 'concept', 'of', 'extra', 'dimensionsin', 'this', 'scenario', 'all', 'the', 'standard', 'model', 'matter', 'and', 'gauge', 'fields', 'are', 'confined', 'to', 'the', '4', 'dimensions', 'and', 'onl... | [-0.07858385259004415, 0.19101250862245853, -0.05996008282749725, 0.0962453417914902, -0.10488590133763007, -0.09303424421056472, 0.021607665529580048, 0.2934202536026824, -0.19825659617605917, -0.35543180664755264, 0.10747854755796, -0.2725385402171117, -0.060404644833157224, 0.2053112471717814, -0.023776628676747555,... |
706.3552 | Strongly enhanced effective mass in dilute two-dimensional electron
systems: System-independent origin | We measure the effective mass in a dilute two-dimensional electron system in
(111)-silicon by analyzing temperature dependence of the Shubnikov-de Haas
oscillations in the low-temperature limit. A strong enhancement of the
effective mass with decreasing electron density is observed. The mass
renormalization as a func... | cond-mat.str-el | we measure the effective mass in a dilute twodimensional electron system in 111silicon by analyzing temperature dependence of the shubnikovde haas oscillations in the lowtemperature limit a strong enhancement of the effective mass with decreasing electron density is observed the mass renormalization as a function of th... | [['we', 'measure', 'the', 'effective', 'mass', 'in', 'a', 'dilute', 'twodimensional', 'electron', 'system', 'in', '111silicon', 'by', 'analyzing', 'temperature', 'dependence', 'of', 'the', 'shubnikovde', 'haas', 'oscillations', 'in', 'the', 'lowtemperature', 'limit', 'a', 'strong', 'enhancement', 'of', 'the', 'effectiv... | [-0.18567618898846008, 0.20798237826926885, -0.06529675718047656, 0.0770364753206613, 0.039127125971119954, -0.09803012689902775, 0.047389318757514294, 0.306181923360438, -0.1726983367792658, -0.3530811779877498, -0.0051403178178982155, -0.3351616463749795, -0.08667366246919374, 0.21451730886474252, 0.03330033840737431... |
706.3553 | L\'evy Statistics and Anomalous Transport: L\'evy flights and
Subdiffusion | Levy flights and subdiffusive processes and their properties are discussed.
We derive the space- and time-fractional transport equations, and consider
their solutions in external potentials. An extensive list of references is
included.
| cond-mat.stat-mech | levy flights and subdiffusive processes and their properties are discussed we derive the space and timefractional transport equations and consider their solutions in external potentials an extensive list of references is included | [['levy', 'flights', 'and', 'subdiffusive', 'processes', 'and', 'their', 'properties', 'are', 'discussed', 'we', 'derive', 'the', 'space', 'and', 'timefractional', 'transport', 'equations', 'and', 'consider', 'their', 'solutions', 'in', 'external', 'potentials', 'an', 'extensive', 'list', 'of', 'references', 'is', 'inc... | [-0.16684712347341701, 0.15299405887026296, -0.01691498013678938, 0.10476554515844327, -0.07223761504792492, -0.11669997486751527, 0.01726971019525081, 0.4590678781969473, -0.26454758084582863, -0.2477787427487783, 0.14023263653143658, -0.35109412303427234, -0.1528815269120969, 0.18078950292692753, -0.02774104016134515... |
706.3554 | Testing gravity with motion of satellites around galaxies: Newtonian
gravity against Modified Newtonian Dynamics | The motion of satellite galaxies around normal galaxies at distances 50-500
kpc provides a sensitive test for the theories. We study the surface density
and the velocities of satellites around isolated galaxies in the Sloan Digital
Sky Survey. We find that the surface number-density of satellites declines with
the pr... | astro-ph | the motion of satellite galaxies around normal galaxies at distances 50500 kpc provides a sensitive test for the theories we study the surface density and the velocities of satellites around isolated galaxies in the sloan digital sky survey we find that the surface numberdensity of satellites declines with the projecte... | [['the', 'motion', 'of', 'satellite', 'galaxies', 'around', 'normal', 'galaxies', 'at', 'distances', '50500', 'kpc', 'provides', 'a', 'sensitive', 'test', 'for', 'the', 'theories', 'we', 'study', 'the', 'surface', 'density', 'and', 'the', 'velocities', 'of', 'satellites', 'around', 'isolated', 'galaxies', 'in', 'the', ... | [-0.09983909842787139, 0.12857856517209512, -0.10423491318480241, 0.12771556616875746, -0.08098519279543272, -0.1114125221862485, 0.008550855666243131, 0.3750329699024371, -0.17140492571471064, -0.38139507618331386, 0.031710093924736754, -0.29447403639188685, -0.012221509151386728, 0.2163834645837608, -0.00934152549452... |
706.3555 | A formula for the hypergeometric function of type $BC_n$ | Formulae of Berezin and Karpelevic for the radial parts of invariant
differential operators and the spherical function on a complex Grassmann
manifold are generalized to the hypergeometric functions associated with root
system of type $BC_n$ under condition that the multiplicity of the middle roots
is zero or one.
| math.RT math.QA | formulae of berezin and karpelevic for the radial parts of invariant differential operators and the spherical function on a complex grassmann manifold are generalized to the hypergeometric functions associated with root system of type bc_n under condition that the multiplicity of the middle roots is zero or one | [['formulae', 'of', 'berezin', 'and', 'karpelevic', 'for', 'the', 'radial', 'parts', 'of', 'invariant', 'differential', 'operators', 'and', 'the', 'spherical', 'function', 'on', 'a', 'complex', 'grassmann', 'manifold', 'are', 'generalized', 'to', 'the', 'hypergeometric', 'functions', 'associated', 'with', 'root', 'syst... | [-0.1790667584443346, 0.07474702591044913, -0.08616526266361804, 0.10217791876230548, -0.10628986374990261, -0.13252739734115435, -0.05787235080943185, 0.2656708718772898, -0.27102069883666774, -0.191462682599717, 0.12469724956107267, -0.28519088744701065, -0.17117155666780123, 0.19945038739651283, -0.07093014101562228... |
706.3556 | Quantum Oscillations in Magnetic Field Induced Antiferromagnetic Phase
of Underdoped Cuprates : Application to Ortho-II YBa2Cu3O6.5 | Magnetic field induced antiferromagnetic phase of the underdoped cuprates is
studied within the t-t'-J model. A magnetic field suppresses the pairing
amplitude, which in turn may induce antiferromagnetism. We apply our theory to
interpret the recently reported quantum oscillations in high magnetic field in
ortho-II Y... | cond-mat.supr-con | magnetic field induced antiferromagnetic phase of the underdoped cuprates is studied within the ttj model a magnetic field suppresses the pairing amplitude which in turn may induce antiferromagnetism we apply our theory to interpret the recently reported quantum oscillations in high magnetic field in orthoii yba2cu3o65... | [['magnetic', 'field', 'induced', 'antiferromagnetic', 'phase', 'of', 'the', 'underdoped', 'cuprates', 'is', 'studied', 'within', 'the', 'ttj', 'model', 'a', 'magnetic', 'field', 'suppresses', 'the', 'pairing', 'amplitude', 'which', 'in', 'turn', 'may', 'induce', 'antiferromagnetism', 'we', 'apply', 'our', 'theory', 't... | [-0.2165998034955313, 0.27803687083845335, -0.015805913163631252, 0.09396309232353374, -0.06023403807458552, -0.07546566770355584, 0.0906019218311871, 0.3078161694222327, -0.25483056509189983, -0.30834863606529933, -0.025358064288880225, -0.2758494586239315, -0.14243966365712835, 0.1546748441778067, 0.00985769018403847... |
706.3557 | Datta-Das type spin-field effect transistor in non-ballistic regime | It is revealed that in spin helix state of (001) quantum well system, strong
suppression of D'yakonov-Perel' spin relaxation process occurs by an interplay
between Rashba and Dresselhaus couplings over a wide range of Rashba coupling
strength. Contrary to common belief in early works, this leads to the finding
that D... | cond-mat.other | it is revealed that in spin helix state of 001 quantum well system strong suppression of dyakonovperel spin relaxation process occurs by an interplay between rashba and dresselhaus couplings over a wide range of rashba coupling strength contrary to common belief in early works this leads to the finding that dattadas ty... | [['it', 'is', 'revealed', 'that', 'in', 'spin', 'helix', 'state', 'of', '001', 'quantum', 'well', 'system', 'strong', 'suppression', 'of', 'dyakonovperel', 'spin', 'relaxation', 'process', 'occurs', 'by', 'an', 'interplay', 'between', 'rashba', 'and', 'dresselhaus', 'couplings', 'over', 'a', 'wide', 'range', 'of', 'ras... | [-0.2527404061111156, 0.18441718018002576, -0.005095091009778636, 0.05511953879875883, -0.06231093036809138, -0.23063898395879992, 0.007976412911167635, 0.3860907208041421, -0.28169071434863974, -0.27667420511133967, -0.08052214706549421, -0.22142910828281726, -0.14625938440273914, 0.24670626164547035, 0.02393456794587... |
706.3558 | A phase transition behavior for Brownian motions interacting through
their ranks | Consider a time-varying collection of n points on the positive real axis,
modeled as exponentials of n Brownian motions whose drift vector at every time
point is determined by the relative ranks of the coordinate processes at that
time. If at each time point we divide the points by their sum, under suitable
assumptio... | math.PR | consider a timevarying collection of n points on the positive real axis modeled as exponentials of n brownian motions whose drift vector at every time point is determined by the relative ranks of the coordinate processes at that time if at each time point we divide the points by their sum under suitable assumptions the... | [['consider', 'a', 'timevarying', 'collection', 'of', 'n', 'points', 'on', 'the', 'positive', 'real', 'axis', 'modeled', 'as', 'exponentials', 'of', 'n', 'brownian', 'motions', 'whose', 'drift', 'vector', 'at', 'every', 'time', 'point', 'is', 'determined', 'by', 'the', 'relative', 'ranks', 'of', 'the', 'coordinate', 'p... | [-0.10928740526371179, 0.1301373772659993, -0.1196530886514588, 0.04645459974429073, -0.011730426644034526, -0.1503174233914135, 0.09664810885417652, 0.3283643070093178, -0.28951381895136324, -0.2389826733321744, 0.11382312359749042, -0.2969567935458048, -0.10545822502054433, 0.13028981685836583, -0.05196346171457875, ... |
706.3559 | Magnetic and Structural Studies of the Quasi-Two-Dimensional Spin-Gap
System (CuCl)LaNb2O7 | We report magnetization, nuclear magnetic resonance (NMR), nuclear quadrupole
resonance (NQR), and transmission electron microscopy (TEM) studies on the
quasi-two-dimensional spin-gap system (CuCl)LaNb2O7, a possible candidate for
the J1-J2 model on a square lattice. A sharp single NQR line is observed at the
Cu and ... | cond-mat.str-el | we report magnetization nuclear magnetic resonance nmr nuclear quadrupole resonance nqr and transmission electron microscopy tem studies on the quasitwodimensional spingap system cucllanb2o7 a possible candidate for the j1j2 model on a square lattice a sharp single nqr line is observed at the cu and cl sites indicating... | [['we', 'report', 'magnetization', 'nuclear', 'magnetic', 'resonance', 'nmr', 'nuclear', 'quadrupole', 'resonance', 'nqr', 'and', 'transmission', 'electron', 'microscopy', 'tem', 'studies', 'on', 'the', 'quasitwodimensional', 'spingap', 'system', 'cucllanb2o7', 'a', 'possible', 'candidate', 'for', 'the', 'j1j2', 'model... | [-0.15900372641481225, 0.19176590267452412, 0.023609364952426402, 0.0005055441099102609, -0.022377936162956757, -0.18825741602340712, 0.09972322686408006, 0.4044090400566347, -0.21142846453294623, -0.26469609985360876, -0.003136776597602875, -0.350796744634863, -0.04469329660059884, 0.14001221470171005, 0.1440655968530... |
706.356 | Reparametrizations of Continuous Paths | A reparametrization (of a continuous path) is given by a surjective weakly
increasing self-map of the unit interval. We show that the monoid of
reparametrizations (with respect to compositions) can be understood via
``stop-maps'' that allow to investigate compositions and factorizations, and we
compare it to the dist... | math.GN | a reparametrization of a continuous path is given by a surjective weakly increasing selfmap of the unit interval we show that the monoid of reparametrizations with respect to compositions can be understood via stopmaps that allow to investigate compositions and factorizations and we compare it to the distributive latti... | [['a', 'reparametrization', 'of', 'a', 'continuous', 'path', 'is', 'given', 'by', 'a', 'surjective', 'weakly', 'increasing', 'selfmap', 'of', 'the', 'unit', 'interval', 'we', 'show', 'that', 'the', 'monoid', 'of', 'reparametrizations', 'with', 'respect', 'to', 'compositions', 'can', 'be', 'understood', 'via', 'stopmaps... | [-0.126871032838244, 0.1738985261964527, -0.0657965092919767, 0.05750951960534704, -0.09254977428354323, -0.06472984143448147, 0.07111840495649217, 0.4470824424008077, -0.3806604271077297, -0.21035810048448514, 0.10720498167105358, -0.2614922226660631, -0.09496964604001154, 0.18584403398192742, -0.11661312058462169, 0.... |
706.3561 | Transport properties of a meson gas | We present recent results on a systematic method to calculate transport
coefficients for a meson gas (in particular, we analyze a pion gas) at low
temperatures in the context of Chiral Perturbation Theory. Our method is based
on the study of Feynman diagrams with a power counting which takes into account
collisions i... | hep-ph | we present recent results on a systematic method to calculate transport coefficients for a meson gas in particular we analyze a pion gas at low temperatures in the context of chiral perturbation theory our method is based on the study of feynman diagrams with a power counting which takes into account collisions in the ... | [['we', 'present', 'recent', 'results', 'on', 'a', 'systematic', 'method', 'to', 'calculate', 'transport', 'coefficients', 'for', 'a', 'meson', 'gas', 'in', 'particular', 'we', 'analyze', 'a', 'pion', 'gas', 'at', 'low', 'temperatures', 'in', 'the', 'context', 'of', 'chiral', 'perturbation', 'theory', 'our', 'method', ... | [-0.11801872454242318, 0.17314681384180272, -0.12884111362224332, 0.029231980798582288, -0.04017665622546813, -0.06363123727227453, 0.04816681002488449, 0.3535063192881897, -0.21208715261447997, -0.2539266624494272, 0.05335703916644969, -0.2972651708516337, -0.12422451253055411, 0.19401254409648555, 0.01280744237584524... |
706.3562 | Subcritical crack growth in fibrous materials | We present experiments on the slow growth of a single crack in a fax paper
sheet submitted to a constant force $F$. We find that statistically averaged
crack growth curves can be described by only two parameters : the mean rupture
time $\tau$ and a characteristic growth length $\zeta$. We propose a model
based on a t... | cond-mat.mtrl-sci physics.class-ph | we present experiments on the slow growth of a single crack in a fax paper sheet submitted to a constant force f we find that statistically averaged crack growth curves can be described by only two parameters the mean rupture time tau and a characteristic growth length zeta we propose a model based on a thermally activ... | [['we', 'present', 'experiments', 'on', 'the', 'slow', 'growth', 'of', 'a', 'single', 'crack', 'in', 'a', 'fax', 'paper', 'sheet', 'submitted', 'to', 'a', 'constant', 'force', 'f', 'we', 'find', 'that', 'statistically', 'averaged', 'crack', 'growth', 'curves', 'can', 'be', 'described', 'by', 'only', 'two', 'parameters'... | [-0.14990713680939127, 0.1521463253768161, -0.1263449622900225, 0.014308274350651119, -0.03347661648100863, -0.10318415902050522, 0.019693830057318944, 0.3828268937921772, -0.30156129983564217, -0.23634978585566083, 0.061946361265533295, -0.2328240279185896, -0.1536122140278773, 0.20250829380432453, -0.0032739785461065... |
706.3563 | Anomaly Analysis of Hawking Radiation from Acoustic Black Hole | The Hawking radiation from the three dimensional rotating acoustic black hole
is considered from the viewpoint of anomaly cancellation method initiated by
Robinson and Wilczek. Quantum field near the horizon is effectively described
by two dimensional charged field with a charge identified as the angular
momentum m. ... | hep-th | the hawking radiation from the three dimensional rotating acoustic black hole is considered from the viewpoint of anomaly cancellation method initiated by robinson and wilczek quantum field near the horizon is effectively described by two dimensional charged field with a charge identified as the angular momentum m the ... | [['the', 'hawking', 'radiation', 'from', 'the', 'three', 'dimensional', 'rotating', 'acoustic', 'black', 'hole', 'is', 'considered', 'from', 'the', 'viewpoint', 'of', 'anomaly', 'cancellation', 'method', 'initiated', 'by', 'robinson', 'and', 'wilczek', 'quantum', 'field', 'near', 'the', 'horizon', 'is', 'effectively', ... | [-0.1238251113212185, 0.16531344377491847, -0.038046474561532845, 0.08155183439389858, -0.02516346841108009, -0.1358503918500101, -0.031432426958176565, 0.29446597511779116, -0.18908609064991574, -0.33305393363607216, 0.09378965416676309, -0.33890531465680485, -0.06518969110336649, 0.1840668480242995, -0.03721649763006... |
706.3564 | Imaging the stick-slip peeling of an adhesive tape under a constant load | Using a high speed camera, we study the peeling dynamics of an adhesive tape
under a constant load with a special focus on the so-called stick-slip regime
of the peeling. It is the first time that the very fast motion of the peeling
point is imaged. The speed of the camera, up to 16000 fps, allows us to observe
and q... | cond-mat.mtrl-sci physics.class-ph | using a high speed camera we study the peeling dynamics of an adhesive tape under a constant load with a special focus on the socalled stickslip regime of the peeling it is the first time that the very fast motion of the peeling point is imaged the speed of the camera up to 16000 fps allows us to observe and quantify t... | [['using', 'a', 'high', 'speed', 'camera', 'we', 'study', 'the', 'peeling', 'dynamics', 'of', 'an', 'adhesive', 'tape', 'under', 'a', 'constant', 'load', 'with', 'a', 'special', 'focus', 'on', 'the', 'socalled', 'stickslip', 'regime', 'of', 'the', 'peeling', 'it', 'is', 'the', 'first', 'time', 'that', 'the', 'very', 'f... | [-0.14385816168052973, 0.20850056219717739, -0.15229313915241854, -0.009139927202206174, -0.10284197857793144, -0.1716023583093947, 0.07807554105508004, 0.377687546648236, -0.29345208634536163, -0.28350635617648046, 0.08713826141320169, -0.19895829608685744, -0.13663841271395707, 0.20273156047591734, -0.082547088813347... |
706.3565 | Experimental Algorithm for the Maximum Independent Set Problem | We develop an experimental algorithm for the exact solving of the maximum
independent set problem. The algorithm consecutively finds the maximal
independent sets of vertices in an arbitrary undirected graph such that the
next such set contains more elements than the preceding one. For this purpose,
we use a technique... | cs.DS | we develop an experimental algorithm for the exact solving of the maximum independent set problem the algorithm consecutively finds the maximal independent sets of vertices in an arbitrary undirected graph such that the next such set contains more elements than the preceding one for this purpose we use a technique deve... | [['we', 'develop', 'an', 'experimental', 'algorithm', 'for', 'the', 'exact', 'solving', 'of', 'the', 'maximum', 'independent', 'set', 'problem', 'the', 'algorithm', 'consecutively', 'finds', 'the', 'maximal', 'independent', 'sets', 'of', 'vertices', 'in', 'an', 'arbitrary', 'undirected', 'graph', 'such', 'that', 'the',... | [-0.14510064734678638, 0.07022520211307581, -0.06970092666986054, 0.020033366477086742, -0.08275844082427658, -0.11841918352659639, 0.08043676283057422, 0.34846324261041894, -0.26377499876671456, -0.3270334402635081, 0.1048464246791124, -0.27788671268294135, -0.13188401018014204, 0.1761768110070939, -0.0568537576066661... |
706.3566 | Algebraic definition of Holonomy on Poisson Manifold | We give an algebraic construction of connection on the symplectic leaves of
Poisson manifold, introduced in \cite{Ginzburg}. This construction is suitable
for the definition of the linearized holonomy on a regular symplectic
foliation.
| math.SG | we give an algebraic construction of connection on the symplectic leaves of poisson manifold introduced in citeginzburg this construction is suitable for the definition of the linearized holonomy on a regular symplectic foliation | [['we', 'give', 'an', 'algebraic', 'construction', 'of', 'connection', 'on', 'the', 'symplectic', 'leaves', 'of', 'poisson', 'manifold', 'introduced', 'in', 'citeginzburg', 'this', 'construction', 'is', 'suitable', 'for', 'the', 'definition', 'of', 'the', 'linearized', 'holonomy', 'on', 'a', 'regular', 'symplectic', 'f... | [-0.26012734399409965, 0.04072968413356648, -0.12491001299349591, 0.07849139312747866, -0.16722567792749032, -0.10853553503693547, -0.04798442752507981, 0.29447401873767376, -0.2752787242643535, -0.17744138301350176, 0.06013644837003085, -0.17642761627212167, -0.2050871461397037, 0.16508228797465563, -0.218936524150194... |
706.3567 | CMB anisotropy power spectrum using linear combinations of WMAP maps | In recent years the goal of estimating different cosmological parameters
precisely has set new challenges in the effort to accurately measure the
angular power spectrum of CMB. This has required removal of foreground
contamination as well as detector noise bias with reliability and precision.
Recently, a novel {\em m... | astro-ph | in recent years the goal of estimating different cosmological parameters precisely has set new challenges in the effort to accurately measure the angular power spectrum of cmb this has required removal of foreground contamination as well as detector noise bias with reliability and precision recently a novel em modelind... | [['in', 'recent', 'years', 'the', 'goal', 'of', 'estimating', 'different', 'cosmological', 'parameters', 'precisely', 'has', 'set', 'new', 'challenges', 'in', 'the', 'effort', 'to', 'accurately', 'measure', 'the', 'angular', 'power', 'spectrum', 'of', 'cmb', 'this', 'has', 'required', 'removal', 'of', 'foreground', 'co... | [-0.022239644824883636, 0.022823729681678943, -0.09273609995301584, 0.023423305479809642, -0.10197608481322265, -0.05723068782956236, 0.03334903693901674, 0.34211058258136484, -0.22772903900010005, -0.39543698033616864, 0.09545830188873856, -0.3321486895840707, -0.08596301924065043, 0.23830964382203226, -0.058775164652... |
706.3568 | Analyzing powers Ayy, Axx, Axz and Ay in the dd->3Hen reaction at 270
MeV | The data on the tensor Ayy, Axx, Axz and vector Ay analyzing powers in the
dd->3Hen obtained at Td= 270 MeV in the angular range 0 - 110 degrees in the
c.m. are presented. The observed negative sign of the tensor analyzing powers
Ayy, Axx and Axz at small angles clearly demonstrate the sensitivity to the
ratio of the... | nucl-ex | the data on the tensor ayy axx axz and vector ay analyzing powers in the dd3hen obtained at td 270 mev in the angular range 0 110 degrees in the cm are presented the observed negative sign of the tensor analyzing powers ayy axx and axz at small angles clearly demonstrate the sensitivity to the ratio of the d and s wave... | [['the', 'data', 'on', 'the', 'tensor', 'ayy', 'axx', 'axz', 'and', 'vector', 'ay', 'analyzing', 'powers', 'in', 'the', 'dd3hen', 'obtained', 'at', 'td', '270', 'mev', 'in', 'the', 'angular', 'range', '0', '110', 'degrees', 'in', 'the', 'cm', 'are', 'presented', 'the', 'observed', 'negative', 'sign', 'of', 'the', 'tens... | [-0.15905580273137823, 0.14791189668939844, -0.002870429178128148, 0.051644803771730696, -0.004952549176246832, -0.045991704250584436, 0.0014861888058557368, 0.32430310994571093, -0.265746600096031, -0.27089265503431903, 0.050552878565717455, -0.3174175168894748, -0.056342695738055795, 0.15184398556570752, 0.1254239498... |
706.3569 | Compact jets as probes for sub-parsec scale regions in AGN | Compact relativistic jets in active galactic nuclei offer an effective tool
for investigating the physics of nuclear regions in galaxies. The emission
properties, dynamics, and evolution of jets in AGN are closely connected to the
characteristics of the central supermassive black hole, accretion disk and
broad-line r... | astro-ph | compact relativistic jets in active galactic nuclei offer an effective tool for investigating the physics of nuclear regions in galaxies the emission properties dynamics and evolution of jets in agn are closely connected to the characteristics of the central supermassive black hole accretion disk and broadline region i... | [['compact', 'relativistic', 'jets', 'in', 'active', 'galactic', 'nuclei', 'offer', 'an', 'effective', 'tool', 'for', 'investigating', 'the', 'physics', 'of', 'nuclear', 'regions', 'in', 'galaxies', 'the', 'emission', 'properties', 'dynamics', 'and', 'evolution', 'of', 'jets', 'in', 'agn', 'are', 'closely', 'connected'... | [-0.04726221588041101, 0.10990461450523331, -0.04657607095993756, 0.18853538390747937, -0.07863156426964062, -0.04245458717590996, -0.04057762995362282, 0.4298954415268132, -0.11567473064309784, -0.29331989833819017, 0.02711369535952274, -0.32926301445945033, 0.0014923158234783581, 0.2259650361857244, -0.00104048965606... |
706.357 | An explicit stationary phase formula for the local formal
Fourier-Laplace transform | We give an explicit formula (i.e., a formal stationary phase formula) for the
local Fourier-Laplace transform of a formal germ of meromorphic connection of
one complex variable with a possibly irregular singularity. This is a complex
analogue of the formulas in the preprint math/0702436v1.
| math.AG math.CV | we give an explicit formula ie a formal stationary phase formula for the local fourierlaplace transform of a formal germ of meromorphic connection of one complex variable with a possibly irregular singularity this is a complex analogue of the formulas in the preprint math0702436v1 | [['we', 'give', 'an', 'explicit', 'formula', 'ie', 'a', 'formal', 'stationary', 'phase', 'formula', 'for', 'the', 'local', 'fourierlaplace', 'transform', 'of', 'a', 'formal', 'germ', 'of', 'meromorphic', 'connection', 'of', 'one', 'complex', 'variable', 'with', 'a', 'possibly', 'irregular', 'singularity', 'this', 'is',... | [-0.2180445786392273, -0.03889095751524004, -0.20672541191844745, 0.10682757883224377, -0.15646882459174755, -0.13134402374542037, 0.027589688294155652, 0.26626370777917463, -0.26649360874191275, -0.15890490423974601, 0.1115640270994803, -0.22190451211577586, -0.22187319826767887, 0.19819605930946593, -0.09675168179531... |
706.3571 | Chern-Simons pre-quantization over four-manifolds | We introduce a pre-symplectic structure on the space of connections in a
G-principal bundle over a four-manifold and a Hamiltonian action on it of the
group of gauge transformations that are trivial on the boundary. The moment map
is given by the square of curvature so that the 0-level set is the space of
flat connec... | math.SG math-ph math.MP | we introduce a presymplectic structure on the space of connections in a gprincipal bundle over a fourmanifold and a hamiltonian action on it of the group of gauge transformations that are trivial on the boundary the moment map is given by the square of curvature so that the 0level set is the space of flat connections t... | [['we', 'introduce', 'a', 'presymplectic', 'structure', 'on', 'the', 'space', 'of', 'connections', 'in', 'a', 'gprincipal', 'bundle', 'over', 'a', 'fourmanifold', 'and', 'a', 'hamiltonian', 'action', 'on', 'it', 'of', 'the', 'group', 'of', 'gauge', 'transformations', 'that', 'are', 'trivial', 'on', 'the', 'boundary', '... | [-0.19744356971990207, 0.07743613779757202, -0.07826696730583058, 0.054087242038948186, -0.15986845423790194, -0.09860132973742589, -0.006493152806473121, 0.38398575753268627, -0.26859697904483887, -0.22816088384635155, 0.10886492035962586, -0.24928960982839218, -0.2193879764250452, 0.12701613572771928, -0.129257518013... |
706.3572 | Quantum-statistical equation-of-state models of dense plasmas:
high-pressure Hugoniot shock adiabats | We present a detailed comparison of two self-consistent equation-of-state
models which differ from their electronic contribution: the atom in a spherical
cell and the atom in a jellium of charges. It is shown that both models are
well suited for the calculation of Hugoniot shock adiabats in the high pressure
range (1... | physics.plasm-ph physics.gen-ph | we present a detailed comparison of two selfconsistent equationofstate models which differ from their electronic contribution the atom in a spherical cell and the atom in a jellium of charges it is shown that both models are well suited for the calculation of hugoniot shock adiabats in the high pressure range 1 mbar10 ... | [['we', 'present', 'a', 'detailed', 'comparison', 'of', 'two', 'selfconsistent', 'equationofstate', 'models', 'which', 'differ', 'from', 'their', 'electronic', 'contribution', 'the', 'atom', 'in', 'a', 'spherical', 'cell', 'and', 'the', 'atom', 'in', 'a', 'jellium', 'of', 'charges', 'it', 'is', 'shown', 'that', 'both',... | [-0.06469769877355336, 0.1410068312449561, -0.0904424053789567, 0.08402030601545478, -0.026435206497779057, -0.11315453912492, 0.027521604396057345, 0.41190514576831655, -0.2192513232509936, -0.3276705983350234, 0.04380331623120113, -0.29816485805467013, -0.06692709674638125, 0.20972715223850233, 0.017553553360255224, ... |
706.3573 | Optical asymptotics via Weniger transformation | Starting from the resurgence equation discovered by Berry and Howls [M. V.
Berry and C. Howls "Hyperasymptotics for integrals with saddles," Proc. R. Soc.
Lond. A 434, 657-675 (1991)], the Weniger transformation is here proposed as a
natural, efficient, and straightforwardly implementable scheme for the
efficient asy... | physics.optics physics.comp-ph | starting from the resurgence equation discovered by berry and howls m v berry and c howls hyperasymptotics for integrals with saddles proc r soc lond a 434 657675 1991 the weniger transformation is here proposed as a natural efficient and straightforwardly implementable scheme for the efficient asymptotics evaluation o... | [['starting', 'from', 'the', 'resurgence', 'equation', 'discovered', 'by', 'berry', 'and', 'howls', 'm', 'v', 'berry', 'and', 'c', 'howls', 'hyperasymptotics', 'for', 'integrals', 'with', 'saddles', 'proc', 'r', 'soc', 'lond', 'a', '434', '657675', '1991', 'the', 'weniger', 'transformation', 'is', 'here', 'proposed', '... | [-0.11873607542120705, 0.03176612639799714, -0.14744351577552917, 0.049473460116260276, -0.07382111250537268, -0.16184858318107823, 0.08866454187470178, 0.3318823956508647, -0.2182481821561069, -0.2947313425931753, 0.10218641380044191, -0.25285062222055305, -0.21129848505778795, 0.26442474138048855, -0.0490958888110247... |
706.3574 | The Characteristic Noise Induced by the Continious Measurements in
Classical Open Systems | We proposed the modified version of quantum-mechanical theory of continuous
measurements for the case of classical open systems. In our approach the
influence of measurement on evolution of distribution function of an open
system is described by the Fokker-Planck equation of a special form. The
diffusion tensor of th... | quant-ph | we proposed the modified version of quantummechanical theory of continuous measurements for the case of classical open systems in our approach the influence of measurement on evolution of distribution function of an open system is described by the fokkerplanck equation of a special form the diffusion tensor of this equ... | [['we', 'proposed', 'the', 'modified', 'version', 'of', 'quantummechanical', 'theory', 'of', 'continuous', 'measurements', 'for', 'the', 'case', 'of', 'classical', 'open', 'systems', 'in', 'our', 'approach', 'the', 'influence', 'of', 'measurement', 'on', 'evolution', 'of', 'distribution', 'function', 'of', 'an', 'open'... | [-0.14825451757811697, 0.09706191603081542, -0.0931113068054014, 0.006398911637432398, 0.014092359658832668, -0.05887995129253002, 0.012714218971623333, 0.28126711848832614, -0.2891720455232347, -0.2988156286986373, 0.07515115181317698, -0.2709672666230761, -0.12754747702191907, 0.21837066280397963, -0.0071848114483481... |
706.3575 | Crossed Andreev reflection at spin-active interfaces | With the aid of the quasiclassical Eilenberger formalism we develop a theory
of non-local electron transport across three-terminal ballistic
normal-superconducting-normal (NSN) devices with spin-active NS interfaces. The
phenomenon of crossed Andreev reflection (CAR) is known to play the key role in
such transport. W... | cond-mat.supr-con | with the aid of the quasiclassical eilenberger formalism we develop a theory of nonlocal electron transport across threeterminal ballistic normalsuperconductingnormal nsn devices with spinactive ns interfaces the phenomenon of crossed andreev reflection car is known to play the key role in such transport we demonstrate... | [['with', 'the', 'aid', 'of', 'the', 'quasiclassical', 'eilenberger', 'formalism', 'we', 'develop', 'a', 'theory', 'of', 'nonlocal', 'electron', 'transport', 'across', 'threeterminal', 'ballistic', 'normalsuperconductingnormal', 'nsn', 'devices', 'with', 'spinactive', 'ns', 'interfaces', 'the', 'phenomenon', 'of', 'cro... | [-0.1822466954169795, 0.14166949009057134, -0.08103617956396192, 0.03198234138690168, -0.07672850903123617, -0.21780161662958564, 0.03311507701990195, 0.4100594058446586, -0.2769527750369161, -0.28867160180583595, -0.04419121063081548, -0.2844655946828425, -0.14085948817431926, 0.24719305181875825, -0.00235121488571166... |
706.3576 | Coulomb effects in polarization transfer in elastic antiproton and
proton electron scattering at low energies | The influence of Coulomb distortion on the polarization transfer in elastic
proton and antiproton electron scattering at low energies is calculated in a
distorted wave Born approximation. For antiproton electron scattering Coulomb
effects reduce substantially the spin transfer cross section compared to the
plane wave... | nucl-th | the influence of coulomb distortion on the polarization transfer in elastic proton and antiproton electron scattering at low energies is calculated in a distorted wave born approximation for antiproton electron scattering coulomb effects reduce substantially the spin transfer cross section compared to the plane wave bo... | [['the', 'influence', 'of', 'coulomb', 'distortion', 'on', 'the', 'polarization', 'transfer', 'in', 'elastic', 'proton', 'and', 'antiproton', 'electron', 'scattering', 'at', 'low', 'energies', 'is', 'calculated', 'in', 'a', 'distorted', 'wave', 'born', 'approximation', 'for', 'antiproton', 'electron', 'scattering', 'co... | [-0.04799805860271427, 0.2510251382699431, -0.02773258982420857, 0.22076761288352922, 0.015852852262306347, -0.07224603006425105, 0.04798887836149157, 0.3711184252665114, -0.21858426304395073, -0.3011717375423481, -0.10625485726632178, -0.3871608220610712, 0.05670975658820191, 0.17107395704057235, 0.15018680210767396, ... |
706.3577 | Parametric Frequency Conversion of Short Optical Pulses Controlled by a
CW Background | We predict that parametric sum-frequency generation of an ultra-short pulse
may result from the mixing of an ultra-short optical pulse with a
quasi-continuous wave control. We analytically show that the intensity, time
duration and group velocity of the generated idler pulse may be controlled in a
stable manner by ad... | physics.optics | we predict that parametric sumfrequency generation of an ultrashort pulse may result from the mixing of an ultrashort optical pulse with a quasicontinuous wave control we analytically show that the intensity time duration and group velocity of the generated idler pulse may be controlled in a stable manner by adjusting ... | [['we', 'predict', 'that', 'parametric', 'sumfrequency', 'generation', 'of', 'an', 'ultrashort', 'pulse', 'may', 'result', 'from', 'the', 'mixing', 'of', 'an', 'ultrashort', 'optical', 'pulse', 'with', 'a', 'quasicontinuous', 'wave', 'control', 'we', 'analytically', 'show', 'that', 'the', 'intensity', 'time', 'duration... | [-0.15417819421150183, 0.27644457552518714, -0.10307684959026805, -0.006225950819881339, -0.012741085109219216, -0.08906587894613806, 0.042233688658789584, 0.5462549232077181, -0.31133238690202697, -0.26692183869645786, 0.03428839257174874, -0.19040012594287922, -0.07713064973716412, 0.27835220222671825, -0.02361625630... |
706.3578 | On the corona of magnetars | Slow dissipation of non-potential magnetic fields in the magnetosphere of the
magnetar is assumed to accelerate particles to hundreds MeV along the magnetic
field lines. We consider interaction of fast particles with the surface of the
magnetar. We argue that the collisionless dissipation does not work in the
atmosph... | astro-ph | slow dissipation of nonpotential magnetic fields in the magnetosphere of the magnetar is assumed to accelerate particles to hundreds mev along the magnetic field lines we consider interaction of fast particles with the surface of the magnetar we argue that the collisionless dissipation does not work in the atmosphere o... | [['slow', 'dissipation', 'of', 'nonpotential', 'magnetic', 'fields', 'in', 'the', 'magnetosphere', 'of', 'the', 'magnetar', 'is', 'assumed', 'to', 'accelerate', 'particles', 'to', 'hundreds', 'mev', 'along', 'the', 'magnetic', 'field', 'lines', 'we', 'consider', 'interaction', 'of', 'fast', 'particles', 'with', 'the', ... | [-0.0915131172011459, 0.26025553857454636, -0.039896571209097946, 0.15174283463469965, -0.08765642945978651, -0.0572519889445101, 0.015313750971530088, 0.3776663049667804, -0.2594203927203364, -0.34679214824075344, 0.0024748826699702246, -0.2809526696716903, -0.010694658741928063, 0.21372015407726136, 0.025055737965803... |
706.3579 | Time-dependent quantum Monte Carlo and the stochastic quantization | We examine the relation between the recently proposed time-dependent quantum
Monte Carlo (TDQMC) method and the principles of stochastic quantization. In
both TDQMC and stochastic quantization particle motion obeys stochastic
guidance equations to preserve quantum equilibrium. In this way the probability
density of t... | physics.atom-ph | we examine the relation between the recently proposed timedependent quantum monte carlo tdqmc method and the principles of stochastic quantization in both tdqmc and stochastic quantization particle motion obeys stochastic guidance equations to preserve quantum equilibrium in this way the probability density of the mont... | [['we', 'examine', 'the', 'relation', 'between', 'the', 'recently', 'proposed', 'timedependent', 'quantum', 'monte', 'carlo', 'tdqmc', 'method', 'and', 'the', 'principles', 'of', 'stochastic', 'quantization', 'in', 'both', 'tdqmc', 'and', 'stochastic', 'quantization', 'particle', 'motion', 'obeys', 'stochastic', 'guida... | [-0.10837433590877352, 0.18497284372330558, -0.08085594029357353, 0.07303367456394835, 0.0019405077323845937, -0.1091159928312644, 0.029605240371583543, 0.36953965450326604, -0.27144280514276936, -0.2836328236756067, 0.03033968147900986, -0.25755560999333277, -0.13230269252989732, 0.14934755879180203, 0.027701972645264... |
706.358 | Cusps of Hilbert modular varieties | Motivated by a question of Hirzebruch on the possible topological types of
cusp cross-sections of Hilbert modular varieties, we give a necessary and
sufficient condition for a manifold M to be diffeomorphic to a cusp
cross-section of a Hilbert modular variety. Specialized to Hilbert modular
surfaces, this proves that... | math.GT math.DG | motivated by a question of hirzebruch on the possible topological types of cusp crosssections of hilbert modular varieties we give a necessary and sufficient condition for a manifold m to be diffeomorphic to a cusp crosssection of a hilbert modular variety specialized to hilbert modular surfaces this proves that every ... | [['motivated', 'by', 'a', 'question', 'of', 'hirzebruch', 'on', 'the', 'possible', 'topological', 'types', 'of', 'cusp', 'crosssections', 'of', 'hilbert', 'modular', 'varieties', 'we', 'give', 'a', 'necessary', 'and', 'sufficient', 'condition', 'for', 'a', 'manifold', 'm', 'to', 'be', 'diffeomorphic', 'to', 'a', 'cusp'... | [-0.2124671906845546, 0.06913150750042404, -0.1690790718519374, 0.12142326533181691, -0.12483122359814221, -0.17197409065832434, -0.045280736241195545, 0.2930849965171594, -0.2802118416336414, -0.20238939902107966, 0.08038219297672376, -0.19545228779806118, -0.20309560405654145, 0.2623652815696244, -0.1808498959302118,... |
706.3581 | The Impact of Type Ia Supernova Explosions on their Companions in Binary
System | Using a simple analytic method, we calculate the impact effect between the
ejecta of a SN Ia and its companion to survey the influence of initial
parameters of the progenitor's system, which is useful for searching the
companion in a explosion remnant. The companion models are obtained from
Eggleton's evolution code.... | astro-ph | using a simple analytic method we calculate the impact effect between the ejecta of a sn ia and its companion to survey the influence of initial parameters of the progenitors system which is useful for searching the companion in a explosion remnant the companion models are obtained from eggletons evolution codethe resu... | [['using', 'a', 'simple', 'analytic', 'method', 'we', 'calculate', 'the', 'impact', 'effect', 'between', 'the', 'ejecta', 'of', 'a', 'sn', 'ia', 'and', 'its', 'companion', 'to', 'survey', 'the', 'influence', 'of', 'initial', 'parameters', 'of', 'the', 'progenitors', 'system', 'which', 'is', 'useful', 'for', 'searching'... | [-0.10586719175908821, 0.11773191948911789, -0.1027985035499196, 0.08196123091832809, -0.1411860720839316, -0.056516609072985384, 0.05042937109511681, 0.3660517490890442, -0.19621745081644912, -0.3174858193632692, 0.06838859680276452, -0.234570989866357, 0.0024844553979263767, 0.21207347102529453, -0.05022832163459493,... |
706.3582 | Bohr and Rogosinski abscissas for ordinary Dirichlet series | We prove that the abscissas of Bohr and Rogosinski for ordinary Dirichlet
series, mapping the right half-plane into the bounded convex domain $G\subset
\mathbb{C} $ are independent of the domain $G$. Furthermore, we obtain new
estimates about these abscissas.
| math.CV math.CA | we prove that the abscissas of bohr and rogosinski for ordinary dirichlet series mapping the right halfplane into the bounded convex domain gsubset mathbbc are independent of the domain g furthermore we obtain new estimates about these abscissas | [['we', 'prove', 'that', 'the', 'abscissas', 'of', 'bohr', 'and', 'rogosinski', 'for', 'ordinary', 'dirichlet', 'series', 'mapping', 'the', 'right', 'halfplane', 'into', 'the', 'bounded', 'convex', 'domain', 'gsubset', 'mathbbc', 'are', 'independent', 'of', 'the', 'domain', 'g', 'furthermore', 'we', 'obtain', 'new', 'e... | [-0.13583364579323176, 0.0238135737442487, -0.061707180446466885, 0.04082498759836764, -0.17755507843921314, -0.09702647187923258, 0.035405257213357334, 0.38812398507788376, -0.3638821563909988, -0.1318880336208118, 0.19321098678267082, -0.3022478717203076, -0.04904197976999992, 0.23273778257488803, -0.1019655462807497... |
706.3583 | Outflow and dense gas emission from massive Infrared Dark Clouds | Infrared Dark Clouds are expected to harbor sources in different, very young
evolutionary stages. To better characterize these differences, we observed a
sample of 43 massive Infrared Dark Clouds, originally selected as candidate
high-mass starless cores, with the IRAM 30m telescope covering spectral line
tracers of ... | astro-ph | infrared dark clouds are expected to harbor sources in different very young evolutionary stages to better characterize these differences we observed a sample of 43 massive infrared dark clouds originally selected as candidate highmass starless cores with the iram 30m telescope covering spectral line tracers of lowdensi... | [['infrared', 'dark', 'clouds', 'are', 'expected', 'to', 'harbor', 'sources', 'in', 'different', 'very', 'young', 'evolutionary', 'stages', 'to', 'better', 'characterize', 'these', 'differences', 'we', 'observed', 'a', 'sample', 'of', '43', 'massive', 'infrared', 'dark', 'clouds', 'originally', 'selected', 'as', 'candi... | [-0.06059137313396252, 0.1265265900841249, -0.024262538793667847, 0.04940517613502714, -0.03899315653691943, -0.05295956887195495, 0.03411983732058078, 0.459494286007723, -0.12001756096391805, -0.36403429760996786, 0.06412689786366359, -0.2615254976425548, 0.006359779793883161, 0.1300425445565916, 0.02657332891142186, ... |
706.3584 | Calorimetric Evidence for a Fulde-Ferrell-Larkin-Ovchinnikov
Superconducting State in the Layered Organic Superconductor
\kappa$-(BEDT-TTF)$_2$Cu(NCS)$_2$ | The specific heat of the layered organic superconductor $\kappa$-%
(BEDT-TTF)$_2$Cu(NCS)$_2$, where BEDT-TTF is bisethylenedithio-%
tetrathiafulvalene, has been studied in magnetic fields up to 28 T applied
perpendicular and parallel to the superconducting layers. In parallel fields
above 21 T, the superconducting tr... | cond-mat.supr-con cond-mat.str-el | the specific heat of the layered organic superconductor kappa bedtttf_2cuncs_2 where bedtttf is bisethylenedithio tetrathiafulvalene has been studied in magnetic fields up to 28 t applied perpendicular and parallel to the superconducting layers in parallel fields above 21 t the superconducting transition becomes first ... | [['the', 'specific', 'heat', 'of', 'the', 'layered', 'organic', 'superconductor', 'kappa', 'bedtttf_2cuncs_2', 'where', 'bedtttf', 'is', 'bisethylenedithio', 'tetrathiafulvalene', 'has', 'been', 'studied', 'in', 'magnetic', 'fields', 'up', 'to', '28', 't', 'applied', 'perpendicular', 'and', 'parallel', 'to', 'the', 'su... | [-0.21123535939492286, 0.24469918688293546, -0.011728835878893734, -0.02509725785581395, -0.06391298558097333, -0.13952683829236776, 0.1033249871712178, 0.3350125411711633, -0.21639098305488005, -0.2711256616562605, 0.04387854736065492, -0.2886121538281441, -0.05048217473551631, 0.16373807228170334, 0.08539336352376267... |
706.3585 | Circular Polarization of Primordial Gravitational Waves in
String-inspired Inflationary Cosmology | We study a mechanism to produce the circular polarization of primordial
gravitational waves.
The circular polarization is generated during the super-inflation driven by
the Gauss-Bonnet term in the string-inspired cosmology. The instability in the
tensor mode caused by the Gauss-Bonnet term and the parity violation... | astro-ph gr-qc hep-th | we study a mechanism to produce the circular polarization of primordial gravitational waves the circular polarization is generated during the superinflation driven by the gaussbonnet term in the stringinspired cosmology the instability in the tensor mode caused by the gaussbonnet term and the parity violation due to th... | [['we', 'study', 'a', 'mechanism', 'to', 'produce', 'the', 'circular', 'polarization', 'of', 'primordial', 'gravitational', 'waves', 'the', 'circular', 'polarization', 'is', 'generated', 'during', 'the', 'superinflation', 'driven', 'by', 'the', 'gaussbonnet', 'term', 'in', 'the', 'stringinspired', 'cosmology', 'the', '... | [-0.20765756541855387, 0.2016091262921691, -0.06639414240051954, 0.11472680040996922, -0.13298291495947306, -0.105456745232771, -0.06515608490868048, 0.27383452807822506, -0.2633819900730178, -0.2589505817202374, 0.04266540825459336, -0.2574720349940202, -0.15917162889853304, 0.16213293343999863, 0.013656640379143156, ... |
706.3586 | Graceful exit via polymerization of pre-big bang cosmology | We consider a phenomenological modification of the Pre Big Bang scenario
using ideas from the resolution of curvature singularities in Loop Quantum
Cosmology. We show that non-perturbative Loop modifications to the dynamics,
arising from the underlying polymer representation, can resolve the graceful
exit problem. Th... | hep-th gr-qc | we consider a phenomenological modification of the pre big bang scenario using ideas from the resolution of curvature singularities in loop quantum cosmology we show that nonperturbative loop modifications to the dynamics arising from the underlying polymer representation can resolve the graceful exit problem the curva... | [['we', 'consider', 'a', 'phenomenological', 'modification', 'of', 'the', 'pre', 'big', 'bang', 'scenario', 'using', 'ideas', 'from', 'the', 'resolution', 'of', 'curvature', 'singularities', 'in', 'loop', 'quantum', 'cosmology', 'we', 'show', 'that', 'nonperturbative', 'loop', 'modifications', 'to', 'the', 'dynamics', ... | [-0.1291115177689191, 0.16069936184094677, -0.13329594428695243, 0.10816522112375573, -0.050746905363954695, -0.16783934311729065, -0.02034926130672139, 0.3275777905637139, -0.28080967870316925, -0.24461350427303888, 0.09689874876779798, -0.2660726496266036, -0.07647231588423063, 0.10185715875623724, -0.081206055947496... |
706.3587 | Dark energy models toward observational tests and data | A huge amount of good quality astrophysical data converges towards the
picture of a spatially flat universe undergoing the today observed phase of
accelerated expansion. This new observational trend is commonly addressed as
Precision Cosmology. Despite of the quality of astrophysical surveys, the
nature of dark energ... | astro-ph | a huge amount of good quality astrophysical data converges towards the picture of a spatially flat universe undergoing the today observed phase of accelerated expansion this new observational trend is commonly addressed as precision cosmology despite of the quality of astrophysical surveys the nature of dark energy dom... | [['a', 'huge', 'amount', 'of', 'good', 'quality', 'astrophysical', 'data', 'converges', 'towards', 'the', 'picture', 'of', 'a', 'spatially', 'flat', 'universe', 'undergoing', 'the', 'today', 'observed', 'phase', 'of', 'accelerated', 'expansion', 'this', 'new', 'observational', 'trend', 'is', 'commonly', 'addressed', 'a... | [-0.10228442792234634, 0.12252382300928127, -0.06378118068033414, 0.1383925440315854, -0.10352030593613766, -0.13252076504269628, 0.023444797230629828, 0.37746121595017346, -0.2399774698821975, -0.3878039738335881, 0.0880851578536919, -0.2653242192237819, 0.019169021391128895, 0.19801510447006432, -0.009544235714018724... |
706.3588 | A new type fit for the CKM matrix elements | The aim of the paper is to propose a new type of fits in terms of invariant
quantities for finding the entries of the CKM matrix from the quark sector, by
using the mathematical solution to the reconstruction problem of 3 x 3 unitary
matrices from experimental data, recently found. The necessity of this type of
fit c... | hep-ph | the aim of the paper is to propose a new type of fits in terms of invariant quantities for finding the entries of the ckm matrix from the quark sector by using the mathematical solution to the reconstruction problem of 3 x 3 unitary matrices from experimental data recently found the necessity of this type of fit comes ... | [['the', 'aim', 'of', 'the', 'paper', 'is', 'to', 'propose', 'a', 'new', 'type', 'of', 'fits', 'in', 'terms', 'of', 'invariant', 'quantities', 'for', 'finding', 'the', 'entries', 'of', 'the', 'ckm', 'matrix', 'from', 'the', 'quark', 'sector', 'by', 'using', 'the', 'mathematical', 'solution', 'to', 'the', 'reconstructio... | [-0.06115989839462073, 0.08300885907129238, -0.07680018863787777, 0.030346953400753832, -0.05069666205856361, -0.10476843734320841, 0.05499705953744093, 0.29093247013852785, -0.2864839454622645, -0.2984071927880378, 0.13348266311529045, -0.2564167215586885, -0.1336957408629946, 0.1524115906905775, -0.05065648635163119,... |
706.3589 | Persistence of direction increases the drift velocity of run and tumble
chemotaxis | Escherichia coli is a motile bacterium that moves up a chemoattractant
gradient by performing a biased random walk composed of alternating runs and
tumbles. Previous models of run and tumble chemotaxis neglect one or more
features of the motion, namely (i) a cell cannot directly detect a
chemoattractant gradient but ... | q-bio.QM | escherichia coli is a motile bacterium that moves up a chemoattractant gradient by performing a biased random walk composed of alternating runs and tumbles previous models of run and tumble chemotaxis neglect one or more features of the motion namely i a cell cannot directly detect a chemoattractant gradient but rather... | [['escherichia', 'coli', 'is', 'a', 'motile', 'bacterium', 'that', 'moves', 'up', 'a', 'chemoattractant', 'gradient', 'by', 'performing', 'a', 'biased', 'random', 'walk', 'composed', 'of', 'alternating', 'runs', 'and', 'tumbles', 'previous', 'models', 'of', 'run', 'and', 'tumble', 'chemotaxis', 'neglect', 'one', 'or', ... | [-0.11359129272425195, 0.17592252144949388, -0.06581882174525942, 0.013599365869369242, -0.10657244630921517, -0.19788781748159054, 0.03245842908668153, 0.41601148298623397, -0.2690591668212636, -0.2296959603543723, 0.03285574617865061, -0.24650565426079382, -0.13581209311186573, 0.1727852381676181, -0.0499997228175771... |
706.359 | Breathers and Raman scattering in a two-leg ladder with staggered
Dzialoshinskii-Moriya interaction | Recent experiments have revealed the role of staggered Dzialoshinskii-Moriya
interaction in the magnetized phase of an antiferromagnetic spin 1/2 two-leg
ladder compound under a uniform magnetic field. We derive a low energy
effective field theory describing a magnetized two-leg ladder with a weak
staggered Dzialoshi... | cond-mat.str-el | recent experiments have revealed the role of staggered dzialoshinskiimoriya interaction in the magnetized phase of an antiferromagnetic spin 12 twoleg ladder compound under a uniform magnetic field we derive a low energy effective field theory describing a magnetized twoleg ladder with a weak staggered dzialoshinskiimo... | [['recent', 'experiments', 'have', 'revealed', 'the', 'role', 'of', 'staggered', 'dzialoshinskiimoriya', 'interaction', 'in', 'the', 'magnetized', 'phase', 'of', 'an', 'antiferromagnetic', 'spin', '12', 'twoleg', 'ladder', 'compound', 'under', 'a', 'uniform', 'magnetic', 'field', 'we', 'derive', 'a', 'low', 'energy', '... | [-0.23154046603788933, 0.27760552756823625, -0.03557485671384105, 0.07079796408045998, -0.01723403729314062, -0.1135593336657621, 0.037671530597435776, 0.400404983452366, -0.21294223715813132, -0.2901019929437704, 0.02275006860024102, -0.3089775881186749, -0.08349377109940785, 0.1156779232963648, 0.13145362551343473, -... |
706.3591 | Probing the electron-phonon coupling in MgB2 through magnetoresistance
measurements in neutron irradiated thin films | We report magnetoresistance (MR) measurements on MgB2 and the corresponding
full account from ab-initio calculations; we suggest that this combination can
be a useful tool to probe electron- phonon coupling. We obtain good
quantitative agreement between high field measurements on neutron irradiated
epitaxial thin fil... | cond-mat.supr-con | we report magnetoresistance mr measurements on mgb2 and the corresponding full account from abinitio calculations we suggest that this combination can be a useful tool to probe electron phonon coupling we obtain good quantitative agreement between high field measurements on neutron irradiated epitaxial thin films and c... | [['we', 'report', 'magnetoresistance', 'mr', 'measurements', 'on', 'mgb2', 'and', 'the', 'corresponding', 'full', 'account', 'from', 'abinitio', 'calculations', 'we', 'suggest', 'that', 'this', 'combination', 'can', 'be', 'a', 'useful', 'tool', 'to', 'probe', 'electron', 'phonon', 'coupling', 'we', 'obtain', 'good', 'q... | [-0.12962515154642806, 0.19265301046959524, -0.06998056827024335, 0.023397729735422347, -0.028456722780884732, -0.1393139743423533, 0.08753144283268956, 0.44059881133337814, -0.24635090859872955, -0.3489546235473383, -0.008680818438352573, -0.30621091314990606, -0.09725334268905932, 0.24704214026929722, 0.0880925596004... |
706.3592 | A model of dense-plasma atomic structure for equation-of-state
calculations | A model of dense plasmas relying on the superconfiguration approximation is
presented. In each superconfiguration the nucleus is totally screened by the
electrons in a Wigner-Seitz sphere (ion-sphere model). Superconfigurations of
the same charge are grouped into ions. It is shown that boundary values of the
wavefunc... | physics.atom-ph physics.plasm-ph | a model of dense plasmas relying on the superconfiguration approximation is presented in each superconfiguration the nucleus is totally screened by the electrons in a wignerseitz sphere ionsphere model superconfigurations of the same charge are grouped into ions it is shown that boundary values of the wavefunctions pla... | [['a', 'model', 'of', 'dense', 'plasmas', 'relying', 'on', 'the', 'superconfiguration', 'approximation', 'is', 'presented', 'in', 'each', 'superconfiguration', 'the', 'nucleus', 'is', 'totally', 'screened', 'by', 'the', 'electrons', 'in', 'a', 'wignerseitz', 'sphere', 'ionsphere', 'model', 'superconfigurations', 'of', ... | [-0.08566100295799003, 0.18038167722052198, -0.10123745800028074, 0.11051066990690199, 0.01193779976717357, -0.14813032626420602, 0.022363341528515535, 0.3283858359630766, -0.20310635295236248, -0.24641354724593545, 0.018615442565000005, -0.27436044450378283, -0.08765129038485987, 0.16223713817963398, 0.015519539276994... |
706.3593 | Evolution of dust and ice features around FU Orionis objects | (abridged) We present spectroscopy data for a sample of 14 FUors and 2 TTauri
stars observed with the Spitzer Space Telescope or with the Infrared Space
Observatory (ISO). Based on the appearance of the 10 micron silicate feature we
define 2 categories of FUors. Objects showing the silicate feature in
absorption (Cat... | astro-ph | abridged we present spectroscopy data for a sample of 14 fuors and 2 ttauri stars observed with the spitzer space telescope or with the infrared space observatory iso based on the appearance of the 10 micron silicate feature we define 2 categories of fuors objects showing the silicate feature in absorption category 1 a... | [['abridged', 'we', 'present', 'spectroscopy', 'data', 'for', 'a', 'sample', 'of', '14', 'fuors', 'and', '2', 'ttauri', 'stars', 'observed', 'with', 'the', 'spitzer', 'space', 'telescope', 'or', 'with', 'the', 'infrared', 'space', 'observatory', 'iso', 'based', 'on', 'the', 'appearance', 'of', 'the', '10', 'micron', 's... | [-0.027862679300792264, 0.0945182333336268, -0.07790002637595334, 0.09645441400227855, -0.06707917720129426, -0.09925535215758688, 0.03545084710220413, 0.4637818611988754, -0.21585509435720227, -0.34067381612468983, 0.08514371940955182, -0.26897822655570397, -0.08057461749768548, 0.13870816314401535, -0.077244443411082... |
706.3594 | 0-pi Transitions in a Superconductor/Chiral Ferromagnet/Superconductor
Junction induced by a Homogeneous Cycloidal Spiral | We study the pi phase in a superconductor-ferromagnet-superconductor
Josephson junction, with a ferromagnet showing a cycloidal spiral spin
modulation with in-plane propagation vector. Our results reveal a high
sensitivity of the junction to the spiral order and indicate the presence of
0-pi quantum phase transitions... | cond-mat.supr-con | we study the pi phase in a superconductorferromagnetsuperconductor josephson junction with a ferromagnet showing a cycloidal spiral spin modulation with inplane propagation vector our results reveal a high sensitivity of the junction to the spiral order and indicate the presence of 0pi quantum phase transitions as func... | [['we', 'study', 'the', 'pi', 'phase', 'in', 'a', 'superconductorferromagnetsuperconductor', 'josephson', 'junction', 'with', 'a', 'ferromagnet', 'showing', 'a', 'cycloidal', 'spiral', 'spin', 'modulation', 'with', 'inplane', 'propagation', 'vector', 'our', 'results', 'reveal', 'a', 'high', 'sensitivity', 'of', 'the', ... | [-0.30258907079696656, 0.18005136733991095, -0.0029933096084278077, -0.007685716365813278, -0.09108070561196654, -0.10629206628073007, 0.04658739022852387, 0.395385083835572, -0.2288396302377805, -0.25445120136719196, -0.044196809070126616, -0.3000213174149394, -0.19436229459824972, 0.16251616459339857, 0.1279307941033... |
706.3595 | Two-dimensional Schroedinger operators with fast decaying potential and
multidimensional $L_2$-kernel | Using Moutard transformations we show how explicit examples of
two-dimensional Schroedinger operators with fast decaying potential and
multidimensional $L_2$-kernel may be constructed
| math-ph math.MP | using moutard transformations we show how explicit examples of twodimensional schroedinger operators with fast decaying potential and multidimensional l_2kernel may be constructed | [['using', 'moutard', 'transformations', 'we', 'show', 'how', 'explicit', 'examples', 'of', 'twodimensional', 'schroedinger', 'operators', 'with', 'fast', 'decaying', 'potential', 'and', 'multidimensional', 'l_2kernel', 'may', 'be', 'constructed']] | [-0.05098981512266965, 0.14050711092672177, -0.06425949616268986, 0.12284911468270279, -0.11199261133913838, -0.20398759336343833, -0.037296545159603865, 0.42702544378560214, -0.2930218344110818, -0.21441093282330603, 0.10351619760816295, -0.27675919325667475, -0.2747233211994171, 0.2592284411103243, 0.0115257015318742... |
706.3596 | Time dependent couplings and crossover length scales in non-equilibrium
surface roughening | We show that time dependent couplings may lead to nontrivial scaling
properties of the surface fluctuations of the asymptotic regime in
non-equilibrium kinetic roughening models . Three typical situations are
studied. In the case of a crossover between two different rough regimes, the
time-dependent coupling may resu... | cond-mat.stat-mech | we show that time dependent couplings may lead to nontrivial scaling properties of the surface fluctuations of the asymptotic regime in nonequilibrium kinetic roughening models three typical situations are studied in the case of a crossover between two different rough regimes the timedependent coupling may result in an... | [['we', 'show', 'that', 'time', 'dependent', 'couplings', 'may', 'lead', 'to', 'nontrivial', 'scaling', 'properties', 'of', 'the', 'surface', 'fluctuations', 'of', 'the', 'asymptotic', 'regime', 'in', 'nonequilibrium', 'kinetic', 'roughening', 'models', 'three', 'typical', 'situations', 'are', 'studied', 'in', 'the', '... | [-0.14668579180609465, 0.22826215653011117, -0.13626083319868185, 0.10328132214317144, -0.05892825812440027, -0.15560997421045072, 0.04060989926561467, 0.3327373348672928, -0.302826290870324, -0.27253083444743087, 0.04550900428569375, -0.29117647359871174, -0.13354896382459494, 0.21892811843070917, -0.00188648327415393... |
706.3597 | Formation of Massive Primordial Stars in a Reionized Gas | We use cosmological hydrodynamic simulations with unprecedented resolution to
study the formation of primordial stars in an ionized gas at high redshifts.
Our approach includes all the relevant atomic and molecular physics to follow
the thermal evolution of a prestellar gas cloud to very high densities of
~10^{18} cm... | astro-ph | we use cosmological hydrodynamic simulations with unprecedented resolution to study the formation of primordial stars in an ionized gas at high redshifts our approach includes all the relevant atomic and molecular physics to follow the thermal evolution of a prestellar gas cloud to very high densities of 1018 cm3 we lo... | [['we', 'use', 'cosmological', 'hydrodynamic', 'simulations', 'with', 'unprecedented', 'resolution', 'to', 'study', 'the', 'formation', 'of', 'primordial', 'stars', 'in', 'an', 'ionized', 'gas', 'at', 'high', 'redshifts', 'our', 'approach', 'includes', 'all', 'the', 'relevant', 'atomic', 'and', 'molecular', 'physics', ... | [-0.0816420654372738, 0.17734172118238908, -0.05838251270505034, 0.10959070581449275, -0.05430720537218353, -0.007576589578062168, 0.04592707513236544, 0.3675759096836878, -0.16363821766124323, -0.3418155949180707, 0.04604517120537627, -0.2622330494515566, 0.008066224144735875, 0.1456669352691955, -0.004401726661301984... |
706.3598 | Jet disc coupling in black hole binaries | In the last decade multi-wavelength observations have demonstrated the
importance of jets in the energy output of accreting black hole binaries. The
observed correlations between the presence of a jet and the state of the
accretion flow provide important information on the coupling between accretion
and ejection proc... | astro-ph | in the last decade multiwavelength observations have demonstrated the importance of jets in the energy output of accreting black hole binaries the observed correlations between the presence of a jet and the state of the accretion flow provide important information on the coupling between accretion and ejection processe... | [['in', 'the', 'last', 'decade', 'multiwavelength', 'observations', 'have', 'demonstrated', 'the', 'importance', 'of', 'jets', 'in', 'the', 'energy', 'output', 'of', 'accreting', 'black', 'hole', 'binaries', 'the', 'observed', 'correlations', 'between', 'the', 'presence', 'of', 'a', 'jet', 'and', 'the', 'state', 'of', ... | [-0.15209025351087685, 0.11324917855497493, -0.05042285337517767, 0.12630971798511303, -0.06051786106241786, -0.08040785328215123, 0.0077710425400215645, 0.4037961968004812, -0.20376707278057068, -0.34428831401780463, 0.09870420323104422, -0.31284171739336697, -0.04756689185202392, 0.23470413672528567, 0.02676631084413... |
706.3599 | Generation of perturbation after multi-field inflation | We explore a new possibility that some inflaton fields in multi-field
inflation models satisfy the observed value of the spectral index so that the
curvature perturbation generated by them through post-inflationary dynamics may
be relevant for the current observations. We illustrate this point using a
simple and reas... | astro-ph gr-qc hep-ph hep-th | we explore a new possibility that some inflaton fields in multifield inflation models satisfy the observed value of the spectral index so that the curvature perturbation generated by them through postinflationary dynamics may be relevant for the current observations we illustrate this point using a simple and reasonabl... | [['we', 'explore', 'a', 'new', 'possibility', 'that', 'some', 'inflaton', 'fields', 'in', 'multifield', 'inflation', 'models', 'satisfy', 'the', 'observed', 'value', 'of', 'the', 'spectral', 'index', 'so', 'that', 'the', 'curvature', 'perturbation', 'generated', 'by', 'them', 'through', 'postinflationary', 'dynamics', ... | [-0.15128761067843208, 0.19478522106431997, -0.10323701330388968, 0.1846898762276396, -0.09892934913245531, -0.17422765605666568, -0.005557943158783019, 0.3285221318212839, -0.2618727151877605, -0.2547649521094102, 0.09311319327949044, -0.1926317814164437, -0.20771302584415444, 0.1865092074749275, -0.054450913002857794... |
706.36 | Experimental search for neutron - mirror neutron oscillations using
storage of ultracold neutrons | The idea of a hidden sector of mirror partners of elementary particles has
attracted considerable interest as a possible candidate for dark matter.
Recently it was pointed out by Berezhiani and Bento that the present
experimental data cannot exclude the possibility of a rapid oscillation of the
neutron n to a mirror ... | nucl-ex | the idea of a hidden sector of mirror partners of elementary particles has attracted considerable interest as a possible candidate for dark matter recently it was pointed out by berezhiani and bento that the present experimental data cannot exclude the possibility of a rapid oscillation of the neutron n to a mirror neu... | [['the', 'idea', 'of', 'a', 'hidden', 'sector', 'of', 'mirror', 'partners', 'of', 'elementary', 'particles', 'has', 'attracted', 'considerable', 'interest', 'as', 'a', 'possible', 'candidate', 'for', 'dark', 'matter', 'recently', 'it', 'was', 'pointed', 'out', 'by', 'berezhiani', 'and', 'bento', 'that', 'the', 'present... | [-0.1326196365509062, 0.24255700896779495, -0.04729923805101745, 0.09555126978760405, -0.034856882715417495, -0.12603851678150316, 0.12929625577864148, 0.29694145815747397, -0.20214655621037367, -0.35409418850416136, 0.06664973825757062, -0.29723295687787954, -0.00019291784922261874, 0.18772849633899186, 0.061944131601... |
706.3601 | Modelling exchange bias in core/shell nanoparticles | We present an atomistic model of a single nanoparticle with core/shell
structure that takes into account its lattice strucutre and spherical geometry,
and in which the values of microscopic parameters such as anisotropy and
exchange constants can be tuned in the core, shell and interfacial regions. By
means of Monte ... | cond-mat.mtrl-sci | we present an atomistic model of a single nanoparticle with coreshell structure that takes into account its lattice strucutre and spherical geometry and in which the values of microscopic parameters such as anisotropy and exchange constants can be tuned in the core shell and interfacial regions by means of monte carlo ... | [['we', 'present', 'an', 'atomistic', 'model', 'of', 'a', 'single', 'nanoparticle', 'with', 'coreshell', 'structure', 'that', 'takes', 'into', 'account', 'its', 'lattice', 'strucutre', 'and', 'spherical', 'geometry', 'and', 'in', 'which', 'the', 'values', 'of', 'microscopic', 'parameters', 'such', 'as', 'anisotropy', '... | [-0.12836246276016078, 0.21456387930668147, -0.06578751838777938, 0.025021948014602433, -0.05147338852050229, -0.08772283412424296, 0.0535993766298675, 0.39355657901614904, -0.26993485971708114, -0.34313562559619754, 0.03957028583702172, -0.24412431134383233, -0.06307116151347913, 0.16237004918151232, 0.081921563411220... |
706.3602 | Twisted noncommutative equivariant cohomology: Weil and Cartan models | We propose Weil and Cartan models for the equivariant cohomology of
noncommutative spaces which carry a covariant action of Drinfel'd twisted
symmetries. The construction is suggested by the noncommutative Weil algebra of
Alekseev and Meinrenken; we show that one can implement a Drinfel'd twist of
their models in ord... | math.QA hep-th math-ph math.MP | we propose weil and cartan models for the equivariant cohomology of noncommutative spaces which carry a covariant action of drinfeld twisted symmetries the construction is suggested by the noncommutative weil algebra of alekseev and meinrenken we show that one can implement a drinfeld twist of their models in order to ... | [['we', 'propose', 'weil', 'and', 'cartan', 'models', 'for', 'the', 'equivariant', 'cohomology', 'of', 'noncommutative', 'spaces', 'which', 'carry', 'a', 'covariant', 'action', 'of', 'drinfeld', 'twisted', 'symmetries', 'the', 'construction', 'is', 'suggested', 'by', 'the', 'noncommutative', 'weil', 'algebra', 'of', 'a... | [-0.18717107927847293, 0.10641116154335079, -0.1441004100150519, 0.12740757626729207, -0.15651353418586716, -0.10353723632532262, -0.05749435284205021, 0.3439015422256724, -0.31701035932787963, -0.22927742700783477, 0.07362746094135687, -0.16578015211533995, -0.16811086168332445, 0.16632132914157643, -0.195714878311499... |
706.3603 | Critical mass of bacterial populations and critical temperature of
self-gravitating Brownian particles in two dimensions | We show that the critical mass M_c=8\pi of bacterial populations in two
dimensions in the chemotactic problem is the counterpart of the critical
temperature T_c=GMm/4k_B of self-gravitating Brownian particles in
two-dimensional gravity. We obtain these critical values by using the Virial
theorem or by considering sta... | physics.bio-ph q-bio.CB | we show that the critical mass m_c8pi of bacterial populations in two dimensions in the chemotactic problem is the counterpart of the critical temperature t_cgmm4k_b of selfgravitating brownian particles in twodimensional gravity we obtain these critical values by using the virial theorem or by considering stationary s... | [['we', 'show', 'that', 'the', 'critical', 'mass', 'm_c8pi', 'of', 'bacterial', 'populations', 'in', 'two', 'dimensions', 'in', 'the', 'chemotactic', 'problem', 'is', 'the', 'counterpart', 'of', 'the', 'critical', 'temperature', 't_cgmm4k_b', 'of', 'selfgravitating', 'brownian', 'particles', 'in', 'twodimensional', 'gr... | [-0.1337464641210092, 0.1351302897111197, -0.044202242369863615, 0.03820684841595405, 0.02206181272602648, -0.13330576709310007, 0.012963756896778634, 0.28985399429586306, -0.24475411059381055, -0.26697617760774767, 0.10223198942128138, -0.29100818529509564, -0.1790204952809621, 0.13921493400380877, -0.0246266700685301... |
706.3604 | An introduction to Seiberg-Witten theory on closed 3-manifolds | This is a version of the author's diploma thesis written at the University of
Cologne in 2002/03. The topic is the construction of Seiberg-Witten invariants
of closed 3-manifolds. In analogy to the four dimensional case, the structure
of the moduli space is investigated. The Seiberg-Witten invariants are defined
and ... | math.GT | this is a version of the authors diploma thesis written at the university of cologne in 200203 the topic is the construction of seibergwitten invariants of closed 3manifolds in analogy to the four dimensional case the structure of the moduli space is investigated the seibergwitten invariants are defined and their behav... | [['this', 'is', 'a', 'version', 'of', 'the', 'authors', 'diploma', 'thesis', 'written', 'at', 'the', 'university', 'of', 'cologne', 'in', '200203', 'the', 'topic', 'is', 'the', 'construction', 'of', 'seibergwitten', 'invariants', 'of', 'closed', '3manifolds', 'in', 'analogy', 'to', 'the', 'four', 'dimensional', 'case',... | [-0.1275591050391974, 0.08408245721750605, -0.12855011725599189, 0.048808501617456895, -0.09898692987972998, -0.07306970377587749, -0.021932586656087112, 0.31556916071940927, -0.2035386521664256, -0.3048162779820557, 0.12887268137979457, -0.2607021523667997, -0.17076557675884851, 0.20005846489576323, -0.141528241155057... |
706.3605 | Form factors in finite volume II:disconnected terms and finite
temperature correlators | Continuing the investigation started in a previous work, we consider form
factors of integrable quantum field theories in finite volume, extending our
investigation to matrix elements with disconnected pieces. Numerical
verification of our results is provided by truncated conformal space approach.
Such matrix element... | hep-th cond-mat.other hep-lat | continuing the investigation started in a previous work we consider form factors of integrable quantum field theories in finite volume extending our investigation to matrix elements with disconnected pieces numerical verification of our results is provided by truncated conformal space approach such matrix elements are ... | [['continuing', 'the', 'investigation', 'started', 'in', 'a', 'previous', 'work', 'we', 'consider', 'form', 'factors', 'of', 'integrable', 'quantum', 'field', 'theories', 'in', 'finite', 'volume', 'extending', 'our', 'investigation', 'to', 'matrix', 'elements', 'with', 'disconnected', 'pieces', 'numerical', 'verificati... | [-0.10184361986815929, 0.13063656110937397, -0.08943119943141938, 0.025195742916936676, -0.05451972525256375, -0.06903793623670935, 0.03342028617548446, 0.3528093895316124, -0.20713350595906377, -0.2268779953196645, 0.111184845288905, -0.27729030766834817, -0.1553981439396739, 0.1866309130191803, 0.00047419751062989236... |
706.3606 | Further progress in ion back-flow reduction with patterned gaseous
hole-multipliers | A new idea on electrostatic deviation and capture of back-drifting
avalanche-ions in cascaded gaseous hole-multipliers is presented. It involves a
flipped reversed-bias Micro-Hole & Strip Plate (F-R-MHSP) element, the strips
of which are facing the drift region of the multiplier. The ions, originating
from successive... | physics.ins-det physics.med-ph | a new idea on electrostatic deviation and capture of backdrifting avalancheions in cascaded gaseous holemultipliers is presented it involves a flipped reversedbias microhole strip plate frmhsp element the strips of which are facing the drift region of the multiplier the ions originating from successive multiplication s... | [['a', 'new', 'idea', 'on', 'electrostatic', 'deviation', 'and', 'capture', 'of', 'backdrifting', 'avalancheions', 'in', 'cascaded', 'gaseous', 'holemultipliers', 'is', 'presented', 'it', 'involves', 'a', 'flipped', 'reversedbias', 'microhole', 'strip', 'plate', 'frmhsp', 'element', 'the', 'strips', 'of', 'which', 'are... | [-0.07396585602775774, 0.14105289429901358, -0.008669446799017134, -0.005525820675546772, 0.013419163267628676, -0.15071146595640247, 0.009799676562412356, 0.36004504020370187, -0.21680753040412554, -0.2828949326079111, 0.10254032756946348, -0.2970118044784885, -0.01898883098160664, 0.23235888688723702, -0.047276637162... |
706.3607 | Boltzmann equation approach to transport in finite modular quantum
systems | We investigate the transport behavior of finite modular quantum systems. Such
systems have recently been analyzed by different methods. These approaches
indicate diffusive behavior even and especially for finite systems. Inspired by
these results we analyze analytically and numerically if and in which sense the
dynam... | cond-mat.stat-mech | we investigate the transport behavior of finite modular quantum systems such systems have recently been analyzed by different methods these approaches indicate diffusive behavior even and especially for finite systems inspired by these results we analyze analytically and numerically if and in which sense the dynamics o... | [['we', 'investigate', 'the', 'transport', 'behavior', 'of', 'finite', 'modular', 'quantum', 'systems', 'such', 'systems', 'have', 'recently', 'been', 'analyzed', 'by', 'different', 'methods', 'these', 'approaches', 'indicate', 'diffusive', 'behavior', 'even', 'and', 'especially', 'for', 'finite', 'systems', 'inspired'... | [-0.13176312777075436, 0.11934960522993796, -0.12094676475234256, 0.08002097227859616, -0.03445992684037895, -0.16381761879374337, 0.0033540692558456766, 0.3285788985540961, -0.3062850293140895, -0.25691038870833593, 0.10438129132138657, -0.26099601338529904, -0.18179594463493565, 0.24585015725777806, -0.02132005709693... |
706.3608 | Projective structures and projective bundles over compact Riemann
surfaces | A projective structure on a compact Riemann surface X of genus g is given by
an atlas with transition functions in PGL(2,C). Equivalently, a projective
structure is given by a projective sl(2,C)-bundle over X equipped with a
section s and a foliation F which is both transversal to the fibers and the
section s. From t... | math.CA math.AG math.DG | a projective structure on a compact riemann surface x of genus g is given by an atlas with transition functions in pgl2c equivalently a projective structure is given by a projective sl2cbundle over x equipped with a section s and a foliation f which is both transversal to the fibers and the section s from this latter g... | [['a', 'projective', 'structure', 'on', 'a', 'compact', 'riemann', 'surface', 'x', 'of', 'genus', 'g', 'is', 'given', 'by', 'an', 'atlas', 'with', 'transition', 'functions', 'in', 'pgl2c', 'equivalently', 'a', 'projective', 'structure', 'is', 'given', 'by', 'a', 'projective', 'sl2cbundle', 'over', 'x', 'equipped', 'wit... | [-0.21979090445877417, 0.04827203411063554, -0.09796425532144697, 0.023868038878350963, -0.10688660733158821, -0.12373402664620105, -0.008866454039335898, 0.3874406045626687, -0.26879956701304764, -0.19024016960200085, 0.07004380269158307, -0.24954942428587895, -0.13062694163628571, 0.23222239210229853, -0.129429959702... |
706.3609 | Electron Spin Dynamics of the Superconductor CaC6 probed by ESR | Conduction Electron Spin Resonance (CESR) was measured on a thick slab of
CaC6 in the normal and superconducting state. A surprising increase of the CESR
intensity below Tc can not be explained by the theoretically predicted change
in spin susceptibility. It is interpreted as a vortex enhanced increase of the
effecti... | cond-mat.supr-con | conduction electron spin resonance cesr was measured on a thick slab of cac6 in the normal and superconducting state a surprising increase of the cesr intensity below tc can not be explained by the theoretically predicted change in spin susceptibility it is interpreted as a vortex enhanced increase of the effective ski... | [['conduction', 'electron', 'spin', 'resonance', 'cesr', 'was', 'measured', 'on', 'a', 'thick', 'slab', 'of', 'cac6', 'in', 'the', 'normal', 'and', 'superconducting', 'state', 'a', 'surprising', 'increase', 'of', 'the', 'cesr', 'intensity', 'below', 'tc', 'can', 'not', 'be', 'explained', 'by', 'the', 'theoretically', '... | [-0.13156693755050322, 0.1959272232564607, -0.035391149343922734, 0.044669295145597844, -0.028547393773416325, -0.12491511852214379, 0.07949418092529023, 0.3160185937636665, -0.23766305026864368, -0.2858641046631549, 0.005081694771070034, -0.331993891431817, -0.07031695001226451, 0.19076357584313622, 0.0233491585107653... |
706.361 | Magnetic friction in Ising spin systems | A new contribution to friction is predicted to occur in systems with magnetic
correlations: Tangential relative motion of two Ising spin systems pumps energy
into the magnetic degrees of freedom. This leads to a friction force
proportional to the area of contact. The velocity and temperature dependence of
this force ... | cond-mat.stat-mech cond-mat.other | a new contribution to friction is predicted to occur in systems with magnetic correlations tangential relative motion of two ising spin systems pumps energy into the magnetic degrees of freedom this leads to a friction force proportional to the area of contact the velocity and temperature dependence of this force are i... | [['a', 'new', 'contribution', 'to', 'friction', 'is', 'predicted', 'to', 'occur', 'in', 'systems', 'with', 'magnetic', 'correlations', 'tangential', 'relative', 'motion', 'of', 'two', 'ising', 'spin', 'systems', 'pumps', 'energy', 'into', 'the', 'magnetic', 'degrees', 'of', 'freedom', 'this', 'leads', 'to', 'a', 'frict... | [-0.2611081813000084, 0.254771550941303, -0.053588258661696406, 0.022483766613359466, -0.07815966772751545, -0.13893404974066836, 0.013874220390488782, 0.3222581350838575, -0.30358496542990676, -0.3095470627945826, -0.0027519100974497247, -0.30076202147046294, -0.06651820748399093, 0.181409650914899, 0.0391410792569123... |
706.3611 | Magnetic and superfluid phases of confined fermions in two-dimensional
optical lattices | We examine antiferromagnetic and d-wave superfluid phases of cold fermionic
atoms with repulsive interactions in a two-dimensional optical lattice combined
with a harmonic trapping potential. For experimentally realistic parameters,
the trapping potential leads to the coexistence of magnetic and superfluid
ordered ph... | cond-mat.str-el cond-mat.supr-con | we examine antiferromagnetic and dwave superfluid phases of cold fermionic atoms with repulsive interactions in a twodimensional optical lattice combined with a harmonic trapping potential for experimentally realistic parameters the trapping potential leads to the coexistence of magnetic and superfluid ordered phases w... | [['we', 'examine', 'antiferromagnetic', 'and', 'dwave', 'superfluid', 'phases', 'of', 'cold', 'fermionic', 'atoms', 'with', 'repulsive', 'interactions', 'in', 'a', 'twodimensional', 'optical', 'lattice', 'combined', 'with', 'a', 'harmonic', 'trapping', 'potential', 'for', 'experimentally', 'realistic', 'parameters', 't... | [-0.20067215531777877, 0.2791390457781605, -0.0543820617676829, 0.08432143848711768, -3.6769510748294683e-06, -0.13584456262805572, 0.08073836538376501, 0.39163840709863085, -0.2595212851436092, -0.25729877249026545, -0.0337657575459721, -0.3279138163376886, -0.14539507147856057, 0.10272414037563767, 0.1212432952060435... |
706.3612 | Chiral entanglement in triangular lattice models | We consider the low energy spectrum of spin-1/2 two-dimensional triangular
lattice models subject to a ferromagnetic Heisenberg interaction and a three
spin chiral interaction of variable strength. Initially, we consider quasi-one
dimensional ladder systems of various geometries. Analytical results are
derived that y... | quant-ph cond-mat.str-el | we consider the low energy spectrum of spin12 twodimensional triangular lattice models subject to a ferromagnetic heisenberg interaction and a three spin chiral interaction of variable strength initially we consider quasione dimensional ladder systems of various geometries analytical results are derived that yield the ... | [['we', 'consider', 'the', 'low', 'energy', 'spectrum', 'of', 'spin12', 'twodimensional', 'triangular', 'lattice', 'models', 'subject', 'to', 'a', 'ferromagnetic', 'heisenberg', 'interaction', 'and', 'a', 'three', 'spin', 'chiral', 'interaction', 'of', 'variable', 'strength', 'initially', 'we', 'consider', 'quasione', ... | [-0.18939854232085626, 0.22603781416088226, -0.04406066207347188, 0.0718415677419123, -0.0054266372453568015, -0.15522144372963648, 0.01694059553996139, 0.37755423121330306, -0.21551160069593178, -0.2459415994111566, 0.08078170462335482, -0.30615789956581874, -0.11710695089317683, 0.13418468982384607, 0.081184291792300... |
706.3613 | Optical and magneto-optical properties of ferromagnetic full-Heusler
films: experiments and first-principles calculations | We report a joint theoretical and experimental study focused on understanding
the optical and magneto-optical properties of Co-based full-Heusler compounds.
We show that magneto-optical spectra calculated within ab-initio density
functional theory are able to uniquely identify the features of the
experimental spectra... | cond-mat.mtrl-sci | we report a joint theoretical and experimental study focused on understanding the optical and magnetooptical properties of cobased fullheusler compounds we show that magnetooptical spectra calculated within abinitio density functional theory are able to uniquely identify the features of the experimental spectra in term... | [['we', 'report', 'a', 'joint', 'theoretical', 'and', 'experimental', 'study', 'focused', 'on', 'understanding', 'the', 'optical', 'and', 'magnetooptical', 'properties', 'of', 'cobased', 'fullheusler', 'compounds', 'we', 'show', 'that', 'magnetooptical', 'spectra', 'calculated', 'within', 'abinitio', 'density', 'functi... | [-0.06757976829026968, 0.07936036915092146, -0.055775226859407404, 0.034225747704513816, -0.04806571469200238, -0.09381110813089852, 0.04464460526873216, 0.44302287049023276, -0.20839422110120875, -0.2982213499371783, 0.031554172572214156, -0.3151293956650958, -0.17082457624028546, 0.2377321014296208, 0.019187429345654... |
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