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 |
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706.3414 | Direct measurement of the intermolecular forces confining a single
molecule in an entangled polymer solution | We use optical tweezers to directly measure the intermolecular forces acting
on a single polymer imposed by surrounding entangled polymers (115 kbp DNA, 1
mg/ml). A tube-like confining field was measured in accord with the key
assumption of reptation models. A time-dependent harmonic potential opposed
transverse disp... | cond-mat.soft | we use optical tweezers to directly measure the intermolecular forces acting on a single polymer imposed by surrounding entangled polymers 115 kbp dna 1 mgml a tubelike confining field was measured in accord with the key assumption of reptation models a timedependent harmonic potential opposed transverse displacement i... | [['we', 'use', 'optical', 'tweezers', 'to', 'directly', 'measure', 'the', 'intermolecular', 'forces', 'acting', 'on', 'a', 'single', 'polymer', 'imposed', 'by', 'surrounding', 'entangled', 'polymers', '115', 'kbp', 'dna', '1', 'mgml', 'a', 'tubelike', 'confining', 'field', 'was', 'measured', 'in', 'accord', 'with', 'th... | [-0.1039682501388259, 0.2316524471416203, -0.042353467820862, 0.0030656957045890566, 0.018290368084752456, -0.2011408744119974, -0.007487914676583091, 0.4189693397993958, -0.22275772609553018, -0.3251540381133118, 0.009437285511223815, -0.3023840192553782, -0.029444544153764497, 0.1505403788381278, -0.00370211377306733... |
706.3415 | Spectral stability of noncharacteristic isentropic Navier-Stokes
boundary layers | Building on work of Barker, Humpherys, Lafitte, Rudd, and Zumbrun in the
shock wave case, we study stability of compressive, or "shock-like", boundary
layers of the isentropic compressible Navier-Stokes equations with gamma-law
pressure by a combination of asymptotic ODE estimates and numerical Evans
function computa... | math.AP | building on work of barker humpherys lafitte rudd and zumbrun in the shock wave case we study stability of compressive or shocklike boundary layers of the isentropic compressible navierstokes equations with gammalaw pressure by a combination of asymptotic ode estimates and numerical evans function computations our resu... | [['building', 'on', 'work', 'of', 'barker', 'humpherys', 'lafitte', 'rudd', 'and', 'zumbrun', 'in', 'the', 'shock', 'wave', 'case', 'we', 'study', 'stability', 'of', 'compressive', 'or', 'shocklike', 'boundary', 'layers', 'of', 'the', 'isentropic', 'compressible', 'navierstokes', 'equations', 'with', 'gammalaw', 'press... | [-0.15670636553528036, 0.09701047768262643, -0.07457069596688298, 0.020662372925943587, -0.05012096150459934, -0.10193860259119279, 0.02483830378756304, 0.3032098817138025, -0.24849867183992144, -0.27549831529702, 0.14981340419919573, -0.21856134123868576, -0.09769597534779931, 0.1954959383738357, -0.02722127071015914,... |
706.3416 | Classical capacity of bosonic broadcast communication and a new minimum
output entropy conjecture | Previous work on the classical information capacities of bosonic channels has
established the capacity of the single-user pure-loss channel, bounded the
capacity of the single-user thermal-noise channel, and bounded the capacity
region of the multiple-access channel. The latter is a multi-user scenario in
which sever... | quant-ph | previous work on the classical information capacities of bosonic channels has established the capacity of the singleuser pureloss channel bounded the capacity of the singleuser thermalnoise channel and bounded the capacity region of the multipleaccess channel the latter is a multiuser scenario in which several transmit... | [['previous', 'work', 'on', 'the', 'classical', 'information', 'capacities', 'of', 'bosonic', 'channels', 'has', 'established', 'the', 'capacity', 'of', 'the', 'singleuser', 'pureloss', 'channel', 'bounded', 'the', 'capacity', 'of', 'the', 'singleuser', 'thermalnoise', 'channel', 'and', 'bounded', 'the', 'capacity', 'r... | [-0.2301760336181315, 0.09985168106245375, -0.0747273692902694, 0.010748149438129103, -0.07338272906219734, -0.28837062010891956, 0.14639358935787775, 0.31661385496949207, -0.2584514006336063, -0.2296130140404226, 0.10127905768164812, -0.25577231995515887, -0.10082650893957971, 0.14214675217903783, -0.12430277130826455... |
706.3417 | Superfuid-insulator transitions at non-integer filling in optical
lattices of fermionic atoms | We determine the superfluid transition temperatures $T_c$ and the ground
states of the attractive Hubbard model and find new insulating phases
associated with non-integer filling at sufficiently strong pairing attraction
$|U|$. These states, distinct from band and Mott insulating phases, derive from
pair localization... | cond-mat.other cond-mat.quant-gas cond-mat.str-el cond-mat.supr-con | we determine the superfluid transition temperatures t_c and the ground states of the attractive hubbard model and find new insulating phases associated with noninteger filling at sufficiently strong pairing attraction u these states distinct from band and mott insulating phases derive from pair localization pair hoppin... | [['we', 'determine', 'the', 'superfluid', 'transition', 'temperatures', 't_c', 'and', 'the', 'ground', 'states', 'of', 'the', 'attractive', 'hubbard', 'model', 'and', 'find', 'new', 'insulating', 'phases', 'associated', 'with', 'noninteger', 'filling', 'at', 'sufficiently', 'strong', 'pairing', 'attraction', 'u', 'thes... | [-0.20440537080833762, 0.28152279288176146, -0.03045600545177793, 0.08901844973590267, -0.013258305993787516, -0.24061590995125728, 0.1332638082148015, 0.35438106649009316, -0.24945364639580506, -0.2583672818995413, -0.0345161663015084, -0.34238757352590904, -0.07857736295367453, 0.03497766927633991, 0.1294427524031750... |
706.3418 | Tunneling Density of States, Pair Correlation, and Josephson Current in
Spin-Incoherent Luttinger Liquid-Superconductor Hybrid Systems | We study a hybrid system consisting of a spin-incoherent Luttinger liquid
adjoined at one or both ends to a superconductor. We find the tunneling density
of states diverges at low energies and exhibits a universal frequency
dependence independent of the strength of the interactions in the system. We
show that in spit... | cond-mat.str-el cond-mat.mes-hall | we study a hybrid system consisting of a spinincoherent luttinger liquid adjoined at one or both ends to a superconductor we find the tunneling density of states diverges at low energies and exhibits a universal frequency dependence independent of the strength of the interactions in the system we show that in spite of ... | [['we', 'study', 'a', 'hybrid', 'system', 'consisting', 'of', 'a', 'spinincoherent', 'luttinger', 'liquid', 'adjoined', 'at', 'one', 'or', 'both', 'ends', 'to', 'a', 'superconductor', 'we', 'find', 'the', 'tunneling', 'density', 'of', 'states', 'diverges', 'at', 'low', 'energies', 'and', 'exhibits', 'a', 'universal', '... | [-0.21978327923376734, 0.20331849542368824, -0.07694469834144305, 0.030905205139667182, 0.035092961753252896, -0.17616395097381124, 0.09018655007821508, 0.28563398067684226, -0.24056505957075083, -0.25001380062506845, 0.03243051175280319, -0.33898590093789, -0.09242647989303805, 0.19379326960188337, 0.03772317564580589... |
706.3419 | New PVLAS results and limits on magnetically induced optical rotation
and ellipticity in vacuum | IIn 2006 the PVLAS collaboration reported the observation of an optical
rotation generated in vacuum by a magnetic field. To further check against
possible instrumental artifacts several upgrades to the PVLAS apparatus have
been made during the last year. Two data taking runs, at the wavelength of 1064
nm, have been ... | hep-ex | iin 2006 the pvlas collaboration reported the observation of an optical rotation generated in vacuum by a magnetic field to further check against possible instrumental artifacts several upgrades to the pvlas apparatus have been made during the last year two data taking runs at the wavelength of 1064 nm have been perfor... | [['iin', '2006', 'the', 'pvlas', 'collaboration', 'reported', 'the', 'observation', 'of', 'an', 'optical', 'rotation', 'generated', 'in', 'vacuum', 'by', 'a', 'magnetic', 'field', 'to', 'further', 'check', 'against', 'possible', 'instrumental', 'artifacts', 'several', 'upgrades', 'to', 'the', 'pvlas', 'apparatus', 'hav... | [-0.11033454251314517, 0.20232462974273568, -0.023836529110302904, 0.035572569577597114, -0.02703787058587913, -0.09540594693957062, 0.07915801112834789, 0.3563044538980798, -0.18826283314923525, -0.40401213175228123, 0.08887091004397751, -0.28017310730382045, 0.01173717643719811, 0.2018615271113145, 0.0036513553330584... |
706.342 | Non-universal dynamics of dimer growing interfaces | A finite temperature version of body-centered solid-on-solid growth models
involving attachment and detachment of dimers is discussed in 1+1 dimensions.
The dynamic exponent of the growing interface is studied numerically via the
spectrum gap of the underlying evolution operator. The finite size scaling of
the latter... | cond-mat.stat-mech cond-mat.soft | a finite temperature version of bodycentered solidonsolid growth models involving attachment and detachment of dimers is discussed in 11 dimensions the dynamic exponent of the growing interface is studied numerically via the spectrum gap of the underlying evolution operator the finite size scaling of the latter is foun... | [['a', 'finite', 'temperature', 'version', 'of', 'bodycentered', 'solidonsolid', 'growth', 'models', 'involving', 'attachment', 'and', 'detachment', 'of', 'dimers', 'is', 'discussed', 'in', '11', 'dimensions', 'the', 'dynamic', 'exponent', 'of', 'the', 'growing', 'interface', 'is', 'studied', 'numerically', 'via', 'the... | [-0.11815395593392046, 0.2193749066811118, -0.05404318261138174, 0.058919337963988856, -0.02669814521619485, -0.13786035105638372, 0.011246375666324342, 0.3156801871716678, -0.28638387679676997, -0.2704967296148619, 0.12094038928168292, -0.24798398349810852, -0.13408476526566435, 0.19161057730697179, 0.0222957607442408... |
706.3421 | The cold neutron star in the soft X-ray transient 1H 1905+000 | We report on our analysis of 300 ks of Chandra observations of the neutron
star soft X-ray transient 1H1905+000 in quiescence. We do not detect the source
down to a 95% confidence unabsorbed flux upper limit of 2E-16 erg cm-2 s-1 in
the 0.5-10 keV energy range for an assumed Gamma=2 power law spectral model. A
limit ... | astro-ph | we report on our analysis of 300 ks of chandra observations of the neutron star soft xray transient 1h1905000 in quiescence we do not detect the source down to a 95 confidence unabsorbed flux upper limit of 2e16 erg cm2 s1 in the 0510 kev energy range for an assumed gamma2 power law spectral model a limit of 14e16 erg ... | [['we', 'report', 'on', 'our', 'analysis', 'of', '300', 'ks', 'of', 'chandra', 'observations', 'of', 'the', 'neutron', 'star', 'soft', 'xray', 'transient', '1h1905000', 'in', 'quiescence', 'we', 'do', 'not', 'detect', 'the', 'source', 'down', 'to', 'a', '95', 'confidence', 'unabsorbed', 'flux', 'upper', 'limit', 'of', ... | [-0.06925942554302952, 0.10101141699001079, -0.06922695347149034, 0.13201831544061218, -0.0756874358664979, -0.06702232407748371, 0.10065200133056565, 0.39944507487063463, -0.12048075150917559, -0.35630426294451084, 0.12917303618322715, -0.34679653824594636, 0.03543735032058869, 0.2351040883205475, -0.05207594081259552... |
706.3422 | Dual representation of Polyakov loop in 3d SU(2) lattice Yang-Mills
theory | We consider the expectation value of a Polyakov loop in 3d SU(2) lattice
Yang--Mills theory and transform it to the dual representation in terms of sums
over spins. The spin dependence of the amplitudes is computed explicitly by a
graphical method. We also determine the asymptotic (large spin) limit of the
amplitude ... | hep-lat | we consider the expectation value of a polyakov loop in 3d su2 lattice yangmills theory and transform it to the dual representation in terms of sums over spins the spin dependence of the amplitudes is computed explicitly by a graphical method we also determine the asymptotic large spin limit of the amplitude factors | [['we', 'consider', 'the', 'expectation', 'value', 'of', 'a', 'polyakov', 'loop', 'in', '3d', 'su2', 'lattice', 'yangmills', 'theory', 'and', 'transform', 'it', 'to', 'the', 'dual', 'representation', 'in', 'terms', 'of', 'sums', 'over', 'spins', 'the', 'spin', 'dependence', 'of', 'the', 'amplitudes', 'is', 'computed', ... | [-0.11866490498079725, 0.18367587852309336, -0.08635660430486754, 0.09270100514536267, -0.036413389275658806, -0.03904839643751675, 0.04004609606553853, 0.36524105764363174, -0.22199679248887202, -0.23195254075217922, 0.08264315662079684, -0.2455705923010718, -0.17505415369984959, 0.12337605876602092, 0.003035558976303... |
706.3423 | An exact string representation of 3d SU(2) lattice Yang--Mills theory | We show that 3d SU(2) lattice Yang--Mills theory can be cast in the form of
an exact string representation. The derivation starts from the exact dual (or
spin foam) representation of the lattice gauge theory. We prove that every dual
configuration (or spin foam) can be equivalently described as a self--avoiding
world... | hep-th hep-lat | we show that 3d su2 lattice yangmills theory can be cast in the form of an exact string representation the derivation starts from the exact dual or spin foam representation of the lattice gauge theory we prove that every dual configuration or spin foam can be equivalently described as a selfavoiding worldsheet of strin... | [['we', 'show', 'that', '3d', 'su2', 'lattice', 'yangmills', 'theory', 'can', 'be', 'cast', 'in', 'the', 'form', 'of', 'an', 'exact', 'string', 'representation', 'the', 'derivation', 'starts', 'from', 'the', 'exact', 'dual', 'or', 'spin', 'foam', 'representation', 'of', 'the', 'lattice', 'gauge', 'theory', 'we', 'prove... | [-0.165967839091111, 0.23511131083340903, -0.08167831140579046, 0.0673496212111786, -0.08041889388027175, -0.10235363802498329, 0.018457952043080754, 0.3803915734289684, -0.24358575750755965, -0.18060522813732935, 0.09072764923635035, -0.26741248115496796, -0.16748992455949155, 0.10762643529032574, -0.02364115227257537... |
706.3424 | Keck/Deimos Spectroscopy of a GALEX UV Selecte Sample from the Medium
Imaging Survey | We report results from a pilot program to obtain spectroscopy for objects
detected in the Galaxy Evolution Explorer (GALEX) Medium Imaging Survey (MIS).
Our study examines the properties of galaxies detected by GALEX fainter than
the Sloan Digital Sky Survey (SDSS) spectroscopic survey. This is the first
study to ext... | astro-ph | we report results from a pilot program to obtain spectroscopy for objects detected in the galaxy evolution explorer galex medium imaging survey mis our study examines the properties of galaxies detected by galex fainter than the sloan digital sky survey sdss spectroscopic survey this is the first study to extend the te... | [['we', 'report', 'results', 'from', 'a', 'pilot', 'program', 'to', 'obtain', 'spectroscopy', 'for', 'objects', 'detected', 'in', 'the', 'galaxy', 'evolution', 'explorer', 'galex', 'medium', 'imaging', 'survey', 'mis', 'our', 'study', 'examines', 'the', 'properties', 'of', 'galaxies', 'detected', 'by', 'galex', 'fainte... | [0.01696145745218857, 0.03876434187863042, -0.04470033570133308, 0.09007588160597449, -0.13664621183754389, 0.009874357385536102, 0.08470546545713466, 0.49850807700253336, -0.03292951736176479, -0.3834769167006016, 0.026728788451853055, -0.36983110996273655, 0.0010650999567897476, 0.20655219316324022, -0.07679511437189... |
706.3425 | Twisted conjugacy classes in nilpotent groups | A group is said to have the $R_\infty$ property if every automorphism has an
infinite number of twisted conjugacy classes. We study the question whether $G$
has the $R_\infty$ property when $G$ is a finitely generated torsion-free
nilpotent group. As a consequence, we show that for every positive integer
$n\ge 5$, th... | math.GR math.AT | a group is said to have the r_infty property if every automorphism has an infinite number of twisted conjugacy classes we study the question whether g has the r_infty property when g is a finitely generated torsionfree nilpotent group as a consequence we show that for every positive integer nge 5 there is a compact nil... | [['a', 'group', 'is', 'said', 'to', 'have', 'the', 'r_infty', 'property', 'if', 'every', 'automorphism', 'has', 'an', 'infinite', 'number', 'of', 'twisted', 'conjugacy', 'classes', 'we', 'study', 'the', 'question', 'whether', 'g', 'has', 'the', 'r_infty', 'property', 'when', 'g', 'is', 'a', 'finitely', 'generated', 'to... | [-0.21819356484514363, 0.17240458064098108, -0.12616082636709763, 0.04072963147213296, -0.10932784362142589, -0.18174183710021372, -0.016242068515703926, 0.41128718998845454, -0.3279154868269304, -0.17483010891614095, 0.11960629365442074, -0.2967388109163434, -0.12084478308350059, 0.2082274303999993, -0.125315544221831... |
706.3426 | Distribution of $^{56}$Ni Yields of Type Ia Supernovae and its
Implication for Progenitors | The amount of $^{56}$Ni produced in type Ia supernova (SN Ia) explosion is
probably the most important physical parameter underlying the observed
correlation of SN Ia luminosities with their light curves. Based on an
empirical relation between the $^{56}$Ni mass and the light curve parameter
$\triangle m_{15}$, we ob... | astro-ph | the amount of 56ni produced in type ia supernova sn ia explosion is probably the most important physical parameter underlying the observed correlation of sn ia luminosities with their light curves based on an empirical relation between the 56ni mass and the light curve parameter triangle m_15 we obtained rough estimate... | [['the', 'amount', 'of', '56ni', 'produced', 'in', 'type', 'ia', 'supernova', 'sn', 'ia', 'explosion', 'is', 'probably', 'the', 'most', 'important', 'physical', 'parameter', 'underlying', 'the', 'observed', 'correlation', 'of', 'sn', 'ia', 'luminosities', 'with', 'their', 'light', 'curves', 'based', 'on', 'an', 'empiri... | [-0.03622592620322257, 0.1167614061610893, -0.0022036056069279076, 0.18581102534128996, -0.12245657104697723, -0.13581853700605662, 0.0784472757355219, 0.42613414329077515, -0.1044919766543461, -0.34041886542104466, -0.0011959515448092461, -0.3301628319532576, 0.02240587767612721, 0.2337369642922075, -0.075778023797591... |
706.3427 | Dose, exposure time, and resolution in Serial X-ray Crystallography | The resolution of X-ray diffraction microscopy is limited by the maximum dose
that can be delivered prior to sample damage. In the proposed Serial
Crystallography method, the damage problem is addressed by distributing the
total dose over many identical hydrated macromolecules running continuously in
a single-file tr... | physics.optics physics.bio-ph | the resolution of xray diffraction microscopy is limited by the maximum dose that can be delivered prior to sample damage in the proposed serial crystallography method the damage problem is addressed by distributing the total dose over many identical hydrated macromolecules running continuously in a singlefile train ac... | [['the', 'resolution', 'of', 'xray', 'diffraction', 'microscopy', 'is', 'limited', 'by', 'the', 'maximum', 'dose', 'that', 'can', 'be', 'delivered', 'prior', 'to', 'sample', 'damage', 'in', 'the', 'proposed', 'serial', 'crystallography', 'method', 'the', 'damage', 'problem', 'is', 'addressed', 'by', 'distributing', 'th... | [-0.07803326258625912, 0.12475520785374102, -0.04309520371524351, 0.05983161262749713, -0.020675890415678827, -0.10730731225933651, 0.04574040726031538, 0.45216557853237477, -0.2783117228890864, -0.3514908585963505, 0.07778161668351719, -0.2807718589768878, -0.06748699092363217, 0.2132119594987634, -0.02962063549143471... |
706.3428 | Aspects of causal viscous hydrodynamics | We investigate the phenomenology of freely expanding fluids, with different
material properties, evolving through the Israel-Stewart (IS) causal viscous
hydrodynamics, and compare our results with those obtained in the relativistic
Eckart-Landau-Navier-Stokes (ELNS) acausal viscous hydrodynamics. Through the
analysis... | nucl-th hep-ph nucl-ex | we investigate the phenomenology of freely expanding fluids with different material properties evolving through the israelstewart is causal viscous hydrodynamics and compare our results with those obtained in the relativistic eckartlandaunavierstokes elns acausal viscous hydrodynamics through the analysis of scaling in... | [['we', 'investigate', 'the', 'phenomenology', 'of', 'freely', 'expanding', 'fluids', 'with', 'different', 'material', 'properties', 'evolving', 'through', 'the', 'israelstewart', 'is', 'causal', 'viscous', 'hydrodynamics', 'and', 'compare', 'our', 'results', 'with', 'those', 'obtained', 'in', 'the', 'relativistic', 'e... | [-0.13588536677083798, 0.1925275806603687, -0.16384424567222594, 0.07623132148158869, -0.02603488309574979, -0.12780934989718454, -0.11679026078964982, 0.3198551883654935, -0.2495547623944003, -0.25666443166722147, 0.0668033613883225, -0.3048573652708105, -0.034405573111559666, 0.16881238694701875, 0.006847465064908777... |
706.3429 | Radio Synchrotron Emission from Secondary Leptons in the Vicinity of Sgr
A* | A point-like source of ~TeV gamma-rays has recently been seen towards the
Galactic center by HESS and other air Cerenkov telescopes. In recent work
(Ballantyne et al. 2007), we demonstrated that these gamma-rays can be
attributed to high-energy protons that (i) are accelerated close to the event
horizon of the centra... | astro-ph | a pointlike source of tev gammarays has recently been seen towards the galactic center by hess and other air cerenkov telescopes in recent work ballantyne et al 2007 we demonstrated that these gammarays can be attributed to highenergy protons that i are accelerated close to the event horizon of the central black hole s... | [['a', 'pointlike', 'source', 'of', 'tev', 'gammarays', 'has', 'recently', 'been', 'seen', 'towards', 'the', 'galactic', 'center', 'by', 'hess', 'and', 'other', 'air', 'cerenkov', 'telescopes', 'in', 'recent', 'work', 'ballantyne', 'et', 'al', '2007', 'we', 'demonstrated', 'that', 'these', 'gammarays', 'can', 'be', 'at... | [-0.027494858057859044, 0.14926308143788672, -0.07846511204520033, 0.09567083733685665, -0.11071145788241082, -0.09555026174634376, 0.020821959434005503, 0.465179822443483, -0.2078488272212796, -0.35038424203665847, 0.019131857454557862, -0.32070354904390425, -0.00846964971990221, 0.19725019184317297, 0.012098695505503... |
706.343 | The Impact of Channel Feedback on Opportunistic Relay Selection for
Hybrid-ARQ in Wireless Networks | This paper presents a decentralized relay selection protocol for a dense
wireless network and describes channel feedback strategies that improve its
performance. The proposed selection protocol supports hybrid
automatic-repeat-request transmission where relays forward parity information
to the destination in the even... | cs.IT math.IT | this paper presents a decentralized relay selection protocol for a dense wireless network and describes channel feedback strategies that improve its performance the proposed selection protocol supports hybrid automaticrepeatrequest transmission where relays forward parity information to the destination in the event of ... | [['this', 'paper', 'presents', 'a', 'decentralized', 'relay', 'selection', 'protocol', 'for', 'a', 'dense', 'wireless', 'network', 'and', 'describes', 'channel', 'feedback', 'strategies', 'that', 'improve', 'its', 'performance', 'the', 'proposed', 'selection', 'protocol', 'supports', 'hybrid', 'automaticrepeatrequest',... | [-0.24077828792786157, -0.03387237477301689, -0.09266816111178033, 0.015616476759856193, -0.0905714069613842, -0.25605167465767376, 0.17245007294695824, 0.42031548351601317, -0.26093473020527097, -0.24442971385325546, 0.09308478595447485, -0.1926851526454643, -0.18910438618450254, 0.12844715338476279, -0.12764657255859... |
706.3431 | Motion of Hexagonal Pencil on an Inclined Plane | This paper has been withdrawn by the author(s), due a crucial sign error in
Eqn. 1.
| physics.class-ph | this paper has been withdrawn by the authors due a crucial sign error in eqn 1 | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'authors', 'due', 'a', 'crucial', 'sign', 'error', 'in', 'eqn', '1']] | [-0.13767500559333712, -0.005415547406300902, -0.061940030194818974, -0.005085243763460312, -0.06042749772313982, -0.11524784224457107, 0.0035364833383937366, 0.30476108007133007, -0.22613738966174424, -0.35564259765669703, 0.1333874656338594, -0.26093209930695593, -0.1833801151951775, 0.049984853831119835, -0.28780148... |
706.3432 | Fluctuation of the Top Location and Avalanches in the Formation Process
of a Sandpile | We investigate the formation processes of a sandpile using numerical
simulation. We find a new relation between the fluctuation of the motion of the
top and the surface state of a sandpile. The top moves frequently as particles
are fed one by one every time interval T. The time series of the top location
has the powe... | cond-mat.soft | we investigate the formation processes of a sandpile using numerical simulation we find a new relation between the fluctuation of the motion of the top and the surface state of a sandpile the top moves frequently as particles are fed one by one every time interval t the time series of the top location has the power spe... | [['we', 'investigate', 'the', 'formation', 'processes', 'of', 'a', 'sandpile', 'using', 'numerical', 'simulation', 'we', 'find', 'a', 'new', 'relation', 'between', 'the', 'fluctuation', 'of', 'the', 'motion', 'of', 'the', 'top', 'and', 'the', 'surface', 'state', 'of', 'a', 'sandpile', 'the', 'top', 'moves', 'frequently... | [-0.13705559759012734, 0.21012658856173705, -0.11970508597635975, 0.015102154361860206, -0.0036319188254613738, -0.10506589624177044, 0.05029616917599924, 0.3316205693641677, -0.29991896320910505, -0.2728634836773078, 0.10173701726113601, -0.2935142168775201, -0.095028896148627, 0.20392719591812541, 0.02583024601141611... |
706.3433 | Unbinding transitions of multicomponent membranes and strings | We present a theory of unbinding transitions for membranes that interact via
short and long receptor/ligand bonds. The detail of unbinding behavior of the
membranes is governed by the binding energies and concentrations of receptors
and ligands. We investigate the unbinding behavior of these membranes with
Monte Carl... | cond-mat.soft | we present a theory of unbinding transitions for membranes that interact via short and long receptorligand bonds the detail of unbinding behavior of the membranes is governed by the binding energies and concentrations of receptors and ligands we investigate the unbinding behavior of these membranes with monte carlo sim... | [['we', 'present', 'a', 'theory', 'of', 'unbinding', 'transitions', 'for', 'membranes', 'that', 'interact', 'via', 'short', 'and', 'long', 'receptorligand', 'bonds', 'the', 'detail', 'of', 'unbinding', 'behavior', 'of', 'the', 'membranes', 'is', 'governed', 'by', 'the', 'binding', 'energies', 'and', 'concentrations', '... | [-0.13187897118704417, 0.1859714510685564, -0.04725674584012809, 0.09035022508005222, 0.053202031180262566, -0.13954536082765348, 0.11208962783647725, 0.38210982473307775, -0.21186528823196982, -0.2558961724390901, 0.024115582042420872, -0.32043777960735736, -0.19107440712823404, 0.1392424059943355, 0.07006906965582431... |
706.3434 | Separating populations with wide data: A spectral analysis | In this paper, we consider the problem of partitioning a small data sample
drawn from a mixture of $k$ product distributions. We are interested in the
case that individual features are of low average quality $\gamma$, and we want
to use as few of them as possible to correctly partition the sample. We analyze
a spectr... | stat.ML stat.AP | in this paper we consider the problem of partitioning a small data sample drawn from a mixture of k product distributions we are interested in the case that individual features are of low average quality gamma and we want to use as few of them as possible to correctly partition the sample we analyze a spectral techniqu... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'problem', 'of', 'partitioning', 'a', 'small', 'data', 'sample', 'drawn', 'from', 'a', 'mixture', 'of', 'k', 'product', 'distributions', 'we', 'are', 'interested', 'in', 'the', 'case', 'that', 'individual', 'features', 'are', 'of', 'low', 'average', 'quality', 'gamma', ... | [-0.08247085165397341, 0.07836320715250622, -0.08137464950947712, 0.06521528899223389, -0.05246256431758714, -0.07421652771687756, 0.10893192684840566, 0.3831143672888478, -0.27168004517012984, -0.36785092460534846, 0.07703813369638131, -0.31851687097999576, -0.11204574424191378, 0.1459400270677482, -0.0637461041954035... |
706.3435 | Undercomplete Blind Subspace Deconvolution via Linear Prediction | We present a novel solution technique for the blind subspace deconvolution
(BSSD) problem, where temporal convolution of multidimensional hidden
independent components is observed and the task is to uncover the hidden
components using the observation only. We carry out this task for the
undercomplete case (uBSSD): we... | stat.ME | we present a novel solution technique for the blind subspace deconvolution bssd problem where temporal convolution of multidimensional hidden independent components is observed and the task is to uncover the hidden components using the observation only we carry out this task for the undercomplete case ubssd we reduce t... | [['we', 'present', 'a', 'novel', 'solution', 'technique', 'for', 'the', 'blind', 'subspace', 'deconvolution', 'bssd', 'problem', 'where', 'temporal', 'convolution', 'of', 'multidimensional', 'hidden', 'independent', 'components', 'is', 'observed', 'and', 'the', 'task', 'is', 'to', 'uncover', 'the', 'hidden', 'component... | [-0.057222419675056604, 0.024292645719496235, -0.08009864487246597, 0.06624080977348638, -0.1180167903620041, -0.12958076601996477, 0.037516839510383274, 0.4088532939499271, -0.298661915531409, -0.3384033774390169, 0.12467846107682672, -0.23864726608862047, -0.16303792057990812, 0.20218462574943577, -0.0877648778057292... |
706.3436 | Rare Kaon Decays Beyond the Standard Model | The rare kaon decays K_L -> pi^0 nu {bar nu}, K^+ -> pi^+ nu {bar nu}, K_L ->
pi^0 e^+ e^- and K_L -> pi^0 mu^+ mu^- are theoretically very clean and, being
strongly CKM suppressed, highly sensitive to New Physics (NP). Recent Flavour
Physics analyses show that they represent unique probes for revealing NP
effects an... | hep-ph | the rare kaon decays k_l pi0 nu bar nu k pi nu bar nu k_l pi0 e e and k_l pi0 mu mu are theoretically very clean and being strongly ckm suppressed highly sensitive to new physics np recent flavour physics analyses show that they represent unique probes for revealing np effects and to provide information on the np flavo... | [['the', 'rare', 'kaon', 'decays', 'k_l', 'pi0', 'nu', 'bar', 'nu', 'k', 'pi', 'nu', 'bar', 'nu', 'k_l', 'pi0', 'e', 'e', 'and', 'k_l', 'pi0', 'mu', 'mu', 'are', 'theoretically', 'very', 'clean', 'and', 'being', 'strongly', 'ckm', 'suppressed', 'highly', 'sensitive', 'to', 'new', 'physics', 'np', 'recent', 'flavour', '... | [-0.07950721403930755, 0.23229070521602455, -0.009900883113851353, 0.16566734347107573, -0.08813488109854563, -0.24053455835816506, 0.12746707162943346, 0.24315671398095332, -0.24549880026488052, -0.23792543726764162, -0.06788036942135124, -0.3273295689592784, -0.01848204770334521, 0.09866460983413367, 0.08268883411620... |
706.3437 | Bell's inequality test with time-delayed two-particle correlations | Adopting the frame of mesoscopic physics, we describe a Bell type experiment
involving time-delayed two-particle correlation measurements. The
indistinguishability of quantum particles results in a specific interference
between different trajectories. We show how the non-locality in the
time-delayed correlations due ... | cond-mat.mes-hall cond-mat.str-el quant-ph | adopting the frame of mesoscopic physics we describe a bell type experiment involving timedelayed twoparticle correlation measurements the indistinguishability of quantum particles results in a specific interference between different trajectories we show how the nonlocality in the timedelayed correlations due to the in... | [['adopting', 'the', 'frame', 'of', 'mesoscopic', 'physics', 'we', 'describe', 'a', 'bell', 'type', 'experiment', 'involving', 'timedelayed', 'twoparticle', 'correlation', 'measurements', 'the', 'indistinguishability', 'of', 'quantum', 'particles', 'results', 'in', 'a', 'specific', 'interference', 'between', 'different... | [-0.17196109549452862, 0.17984518028000215, -0.11157946199515816, 0.07942351684323512, -0.009611355329980142, -0.14049886879123127, 0.05328263855093004, 0.2869496677497712, -0.2861655516552067, -0.3294067265233025, -0.03413230464381437, -0.3056974208448082, -0.11206862318795174, 0.14967961551155895, -0.0191256791780081... |
706.3438 | Dijet correlations in $pp$ collisions at RHIC | We compare results of $k_t$-factorization approach and next-to-leading order
collinear-factorization approach for dijet correlations in proton-proton
collisions at RHIC energies. We discuss correlations in azimuthal angle as well
as correlations in two-dimensional space of transverse momenta of two jets.
Some $k_t$-f... | hep-ph | we compare results of k_tfactorization approach and nexttoleading order collinearfactorization approach for dijet correlations in protonproton collisions at rhic energies we discuss correlations in azimuthal angle as well as correlations in twodimensional space of transverse momenta of two jets some k_tfactorization su... | [['we', 'compare', 'results', 'of', 'k_tfactorization', 'approach', 'and', 'nexttoleading', 'order', 'collinearfactorization', 'approach', 'for', 'dijet', 'correlations', 'in', 'protonproton', 'collisions', 'at', 'rhic', 'energies', 'we', 'discuss', 'correlations', 'in', 'azimuthal', 'angle', 'as', 'well', 'as', 'corre... | [-0.06535868336757024, 0.16678728179385266, -0.15495192960525553, 0.22315860686823727, -0.017567338482864823, -0.03880477750053008, -0.10810707909365495, 0.4507821225374937, -0.15259692780052622, -0.23711570226276915, -0.06105541229403267, -0.3213836495702465, 0.04448311979571978, 0.1709306340292096, 0.0424258791903654... |
706.3439 | Heavy quark correlations in hadronic collisions | We discuss results of the $k_t$ - factorization approach for heavy
quark-heavy antiquark correlations in proton-proton and proton-antiproton
collisions for RHIC, Tevatron and LHC. We consider correlations in the
azimuthal angle as well as in the two-dimensional space of transverse momentum
of heavy quark and heavy an... | hep-ph | we discuss results of the k_t factorization approach for heavy quarkheavy antiquark correlations in protonproton and protonantiproton collisions for rhic tevatron and lhc we consider correlations in the azimuthal angle as well as in the twodimensional space of transverse momentum of heavy quark and heavy antiquark we c... | [['we', 'discuss', 'results', 'of', 'the', 'k_t', 'factorization', 'approach', 'for', 'heavy', 'quarkheavy', 'antiquark', 'correlations', 'in', 'protonproton', 'and', 'protonantiproton', 'collisions', 'for', 'rhic', 'tevatron', 'and', 'lhc', 'we', 'consider', 'correlations', 'in', 'the', 'azimuthal', 'angle', 'as', 'we... | [-0.010591404817876269, 0.2704407924206042, -0.19323001145461544, 0.21328982713128455, -0.006982402753878812, -0.05744860438843731, -0.05850386207343125, 0.4160560561252422, -0.1688767501809558, -0.21831705549457034, -0.11191901513260835, -0.3668276185444633, 0.13408984854573108, 0.11334204899727321, 0.0910102902132956... |
706.344 | The Stellar-Disk Electric (Short) Circuit: Observational Predictions for
a YSO Jet Flow | We discuss the star-disk electric circuit for a young stellar object (YSO)
and calculate the expected torques on the star and the disk. We obtain the same
disk magnetic field and star-disk torques as given by standard
magnetohydrodynamic (MHD) analysis. We show how a short circuit in the
star-disk electric circuit ma... | astro-ph | we discuss the stardisk electric circuit for a young stellar object yso and calculate the expected torques on the star and the disk we obtain the same disk magnetic field and stardisk torques as given by standard magnetohydrodynamic mhd analysis we show how a short circuit in the stardisk electric circuit may produce a... | [['we', 'discuss', 'the', 'stardisk', 'electric', 'circuit', 'for', 'a', 'young', 'stellar', 'object', 'yso', 'and', 'calculate', 'the', 'expected', 'torques', 'on', 'the', 'star', 'and', 'the', 'disk', 'we', 'obtain', 'the', 'same', 'disk', 'magnetic', 'field', 'and', 'stardisk', 'torques', 'as', 'given', 'by', 'stand... | [-0.16320596767727993, 0.11707137837298387, -0.014249078983302452, 0.07844635604665237, -0.13775904458170093, -0.03046170911897928, -0.036564916079817725, 0.4065256190432374, -0.25535136793763186, -0.3149298816950114, 0.06272299071939369, -0.2028209532357075, -0.00194677650497472, 0.2215884596894472, -0.051771752838399... |
706.3441 | Non-archimedean analytification of algebraic spaces | It is now a classical result that an algebraic space locally of finite type
over $\mathbf{C}$ is analytifiable if and only if it is locally separated. In
this paper we study non-archimedean analytifications of algebraic spaces. We
construct a quotient for any etale non-archimedean analytic equivalence
relation whose ... | math.AG | it is now a classical result that an algebraic space locally of finite type over mathbfc is analytifiable if and only if it is locally separated in this paper we study nonarchimedean analytifications of algebraic spaces we construct a quotient for any etale nonarchimedean analytic equivalence relation whose diagonal is... | [['it', 'is', 'now', 'a', 'classical', 'result', 'that', 'an', 'algebraic', 'space', 'locally', 'of', 'finite', 'type', 'over', 'mathbfc', 'is', 'analytifiable', 'if', 'and', 'only', 'if', 'it', 'is', 'locally', 'separated', 'in', 'this', 'paper', 'we', 'study', 'nonarchimedean', 'analytifications', 'of', 'algebraic', ... | [-0.1996539868026351, 0.10296326466401903, -0.12984578974234562, 0.09484877178523068, -0.10209577949717641, -0.12363401274972906, -0.01585053873520034, 0.3854156008145461, -0.37315438928393024, -0.16856630626134575, 0.1119982308805144, -0.17911630827002228, -0.11756416799422974, 0.26778537754435094, -0.1382434165493274... |
706.3442 | Photon-jet correlations in hadronic collisions | We compare results of $k_t$-factorization approach and next-to-leading order
collinear-factorization approach for photon-jet correlations in $pp$ and $p
\bar p$ collisions at RHIC, Tevatron and LHC energies. We discuss correlations
in azimuthal angle as well as in two-dimensional space of transverse momenta of
photon... | hep-ph | we compare results of k_tfactorization approach and nexttoleading order collinearfactorization approach for photonjet correlations in pp and p bar p collisions at rhic tevatron and lhc energies we discuss correlations in azimuthal angle as well as in twodimensional space of transverse momenta of photon and jet differen... | [['we', 'compare', 'results', 'of', 'k_tfactorization', 'approach', 'and', 'nexttoleading', 'order', 'collinearfactorization', 'approach', 'for', 'photonjet', 'correlations', 'in', 'pp', 'and', 'p', 'bar', 'p', 'collisions', 'at', 'rhic', 'tevatron', 'and', 'lhc', 'energies', 'we', 'discuss', 'correlations', 'in', 'azi... | [-0.027637899036764994, 0.17890897183032292, -0.2024837368323157, 0.21198022423130977, 0.013718109024112992, -0.04927775584575203, -0.10412084040257873, 0.4447166114469938, -0.12642671357348767, -0.24308386760660344, -0.13095105112814862, -0.3530275942499025, 0.0790988844819367, 0.1646630699073689, 0.08660601689997646,... |
706.3443 | The SSM Toolbox for Matlab | State Space Models (SSM) is a MATLAB 7.0 software toolbox for doing time
series analysis by state space methods. The software features fully interactive
construction and combination of models, with support for univariate and
multivariate models, complex time-varying (dynamic) models, non-Gaussian
models, and various ... | stat.CO stat.AP | state space models ssm is a matlab 70 software toolbox for doing time series analysis by state space methods the software features fully interactive construction and combination of models with support for univariate and multivariate models complex timevarying dynamic models nongaussian models and various standard model... | [['state', 'space', 'models', 'ssm', 'is', 'a', 'matlab', '70', 'software', 'toolbox', 'for', 'doing', 'time', 'series', 'analysis', 'by', 'state', 'space', 'methods', 'the', 'software', 'features', 'fully', 'interactive', 'construction', 'and', 'combination', 'of', 'models', 'with', 'support', 'for', 'univariate', 'an... | [-0.025920143248992212, -0.032464650558664446, -0.09087873550779219, 0.08010739076169247, -0.10924591634633905, -0.22839366563047606, -0.017988816986904077, 0.43960859367610716, -0.265038710470635, -0.3304417257507642, 0.16958905045101616, -0.23276157308112275, -0.13859548896603974, 0.23647453137409233, -0.002974708376... |
706.3444 | How To Kill a Penguin | Within constrained minimal-flavor-violation the large destructive
flavor-changing Z-penguin managed to survive eradication so far. We give a
incisive description of how to kill it using the precision measurements of the
Z -> b anti-b pseudo observables. The derived stringent range for the
non-standard contribution to... | hep-ph | within constrained minimalflavorviolation the large destructive flavorchanging zpenguin managed to survive eradication so far we give a incisive description of how to kill it using the precision measurements of the z b antib pseudo observables the derived stringent range for the nonstandard contribution to the universa... | [['within', 'constrained', 'minimalflavorviolation', 'the', 'large', 'destructive', 'flavorchanging', 'zpenguin', 'managed', 'to', 'survive', 'eradication', 'so', 'far', 'we', 'give', 'a', 'incisive', 'description', 'of', 'how', 'to', 'kill', 'it', 'using', 'the', 'precision', 'measurements', 'of', 'the', 'z', 'b', 'an... | [-0.10650327092364685, 0.21537546816310196, 0.005167029374702411, 0.14355188279384465, -0.09140336542446731, -0.16545998840592802, 0.16620522944404828, 0.268716494581013, -0.26482189215973695, -0.2668652899958419, 0.0075027626501678515, -0.2717755709097467, -0.004212172737232212, 0.1708794403256792, 0.03634559506705651... |
706.3445 | Analysis of a recent experimental test of Bell inequalities violating
quantum predictions | A recent experiment by Brida et al. (arXiv:0705.0439 [quant-ph]) is analyzed
with the conclusion that is shows a violation of standard quantum predictions.
A simple local hidden variables model is studied which is compatible with the
empirical results and fits fairly well the deviation from the quantum
predictions.
| quant-ph | a recent experiment by brida et al arxiv07050439 quantph is analyzed with the conclusion that is shows a violation of standard quantum predictions a simple local hidden variables model is studied which is compatible with the empirical results and fits fairly well the deviation from the quantum predictions | [['a', 'recent', 'experiment', 'by', 'brida', 'et', 'al', 'arxiv07050439', 'quantph', 'is', 'analyzed', 'with', 'the', 'conclusion', 'that', 'is', 'shows', 'a', 'violation', 'of', 'standard', 'quantum', 'predictions', 'a', 'simple', 'local', 'hidden', 'variables', 'model', 'is', 'studied', 'which', 'is', 'compatible', ... | [-0.04370327118878312, 0.10296923614681718, -0.13580741000143773, 0.06916847967721046, -0.04669546758003058, -0.15188627516692307, 0.07173095604880377, 0.3020656882052092, -0.18449681642604002, -0.34168771844595036, 0.04003161253367967, -0.3075905645147283, -0.16353151366669447, 0.203529855112565, -0.08477396975727157,... |
706.3446 | Estimation of the Birefringence Change in Crystals Induced by
Gravitation Field | The effect of gravitation field of spherically symmetric mass on the
birefringent properties of crystals has been analysed. It has been shown that
the gravitation field with spherical symmetry can lead to a change of
birefringence in anisotropic media.
| physics.optics physics.space-ph | the effect of gravitation field of spherically symmetric mass on the birefringent properties of crystals has been analysed it has been shown that the gravitation field with spherical symmetry can lead to a change of birefringence in anisotropic media | [['the', 'effect', 'of', 'gravitation', 'field', 'of', 'spherically', 'symmetric', 'mass', 'on', 'the', 'birefringent', 'properties', 'of', 'crystals', 'has', 'been', 'analysed', 'it', 'has', 'been', 'shown', 'that', 'the', 'gravitation', 'field', 'with', 'spherical', 'symmetry', 'can', 'lead', 'to', 'a', 'change', 'of... | [-0.14987884757694048, 0.16047474312094542, -0.16773093645819104, -0.029553689062595367, -0.14145184635447386, -0.08707150844379495, -0.1392203542547157, 0.43717736922777617, -0.18077421224174592, -0.27538057266233057, 0.06263637543620112, -0.23518282920122147, -0.13872156855769646, 0.1456818533822512, -0.0194951232466... |
706.3447 | Products of Brauer Severi surfaces | Let $\{P_i\}_{1 \leq i \leq r}$ and $\{Q_i\}_{1 \leq i \leq r}$ be two
collections of Brauer Severi surfaces (resp. conics) over a field $k$. We show
that the subgroup generated by the $P_i's$ in $Br(k)$ is the same as the
subgroup generated by the $Q_i's$ \iff $\Pi P_i $ is birational to $\Pi Q_i$.
Moreover in this ... | math.AG | let p_i_1 leq i leq r and q_i_1 leq i leq r be two collections of brauer severi surfaces resp conics over a field k we show that the subgroup generated by the p_is in brk is the same as the subgroup generated by the q_is iff pi p_i is birational to pi q_i moreover in this case pi p_i and pi q_i represent the same class... | [['let', 'p_i_1', 'leq', 'i', 'leq', 'r', 'and', 'q_i_1', 'leq', 'i', 'leq', 'r', 'be', 'two', 'collections', 'of', 'brauer', 'severi', 'surfaces', 'resp', 'conics', 'over', 'a', 'field', 'k', 'we', 'show', 'that', 'the', 'subgroup', 'generated', 'by', 'the', 'p_is', 'in', 'brk', 'is', 'the', 'same', 'as', 'the', 'subg... | [-0.22487418701524262, 0.1283045515397584, -0.04885990613211806, 0.007305412948551168, -0.030425805833886613, -0.22967209850161613, 0.007924667815421964, 0.3429569275077473, -0.3638317725815616, -0.14521792968018696, 0.016444757860921488, -0.28739337296644735, -0.04697152116632724, 0.19083751198723092, -0.1099258354036... |
706.3448 | Daily Observations of Interstellar Scintillation in PSR B0329+54 | Quasi-continuous observations of PSR B03239+54 over 20 days using the Nanshan
25-m telescope at 1540 MHz have been used to study the effects of refractive
scintillation on the pulsar flux density and diffractive scintillation
properties. Dynamic spectra were obtained from datasets of 90 min duration and
diffractive p... | astro-ph | quasicontinuous observations of psr b0323954 over 20 days using the nanshan 25m telescope at 1540 mhz have been used to study the effects of refractive scintillation on the pulsar flux density and diffractive scintillation properties dynamic spectra were obtained from datasets of 90 min duration and diffractive paramet... | [['quasicontinuous', 'observations', 'of', 'psr', 'b0323954', 'over', '20', 'days', 'using', 'the', 'nanshan', '25m', 'telescope', 'at', '1540', 'mhz', 'have', 'been', 'used', 'to', 'study', 'the', 'effects', 'of', 'refractive', 'scintillation', 'on', 'the', 'pulsar', 'flux', 'density', 'and', 'diffractive', 'scintilla... | [-0.07575346884550527, 0.16820737828482593, -0.09585223348432348, 0.10332789646995746, -0.04700146001927993, -0.12520779030940807, 0.006543822675559889, 0.43664404978135635, -0.19874264643180603, -0.3636117467620209, 0.07611912685587965, -0.3200470542389096, -0.05310389004401205, 0.24220258184890125, -0.003535954742471... |
706.3449 | Incoherent mid-infrared charge excitation and the high energy anomaly in
the photoemission spectra of cuprates | On the basis of a semi-phenomenological model, it is argued that the high
energy anomaly observed in recent photoemission experiments on cuprates is
caused by interaction with an overdamped bosonic mode in the mid-infrared
region of the spectrum. Analysis of optical conductivity allows to connect this
excitation to t... | cond-mat.mtrl-sci | on the basis of a semiphenomenological model it is argued that the high energy anomaly observed in recent photoemission experiments on cuprates is caused by interaction with an overdamped bosonic mode in the midinfrared region of the spectrum analysis of optical conductivity allows to connect this excitation to the inc... | [['on', 'the', 'basis', 'of', 'a', 'semiphenomenological', 'model', 'it', 'is', 'argued', 'that', 'the', 'high', 'energy', 'anomaly', 'observed', 'in', 'recent', 'photoemission', 'experiments', 'on', 'cuprates', 'is', 'caused', 'by', 'interaction', 'with', 'an', 'overdamped', 'bosonic', 'mode', 'in', 'the', 'midinfrare... | [-0.1414644136915312, 0.16023842863608426, -0.0574136974337949, 0.03398391485269017, -0.052630700718830616, -0.12055848340558654, 0.05787714391070254, 0.3958533737808466, -0.2386977784198654, -0.26076692395350515, 0.006513123981901171, -0.3231150415700326, -0.15298848586047398, 0.207316626463195, -0.010120213505990036,... |
706.345 | Ruppeiner Geometry of RN Black Holes: Flat or Curved? | In some recent studies \cite{aman1, aman2, aman3}, Aman {\it et al.} used the
Ruppeiner scalar as a measure of underlying interactions of
Reissner-Nordstr\"{o}m black holes, indicating that it is a non-interacting
statistical system for which classical thermodynamics could be used at any
scale. Here, we show that if ... | hep-th | in some recent studies citeaman1 aman2 aman3 aman it et al used the ruppeiner scalar as a measure of underlying interactions of reissnernordstrom black holes indicating that it is a noninteracting statistical system for which classical thermodynamics could be used at any scale here we show that if we use the complete s... | [['in', 'some', 'recent', 'studies', 'citeaman1', 'aman2', 'aman3', 'aman', 'it', 'et', 'al', 'used', 'the', 'ruppeiner', 'scalar', 'as', 'a', 'measure', 'of', 'underlying', 'interactions', 'of', 'reissnernordstrom', 'black', 'holes', 'indicating', 'that', 'it', 'is', 'a', 'noninteracting', 'statistical', 'system', 'fo... | [-0.10403069331274405, 0.12326061795768026, -0.1144198991105795, 0.13226723170978344, -0.07429079187114711, -0.13475909091641086, 0.017270147606923983, 0.3154041427248097, -0.21124339431475897, -0.2812384626066143, 0.08496434943048985, -0.3489156513801449, -0.14623730679272445, 0.20280289225425427, -0.04635424167522556... |
706.3451 | Complexity test modules | A method is provided for computing an upper bound of the complexity of a
module over a local ring, in terms of vanishing of certain cohomology modules.
We then specialize to complete intersections, which are precisely the rings
over which all modules have finite complexity.
| math.AC | a method is provided for computing an upper bound of the complexity of a module over a local ring in terms of vanishing of certain cohomology modules we then specialize to complete intersections which are precisely the rings over which all modules have finite complexity | [['a', 'method', 'is', 'provided', 'for', 'computing', 'an', 'upper', 'bound', 'of', 'the', 'complexity', 'of', 'a', 'module', 'over', 'a', 'local', 'ring', 'in', 'terms', 'of', 'vanishing', 'of', 'certain', 'cohomology', 'modules', 'we', 'then', 'specialize', 'to', 'complete', 'intersections', 'which', 'are', 'precise... | [-0.20182047889878352, 0.031763418756438316, -0.09765711347055105, 0.026403549078127576, -0.026300639959259166, -0.11608866756368015, -0.012547314529203706, 0.2983064002667864, -0.317655525315139, -0.21625991086992952, 0.1488980202185404, -0.18127409865458807, -0.12968972306698562, 0.2590294123316805, -0.10792549618830... |
706.3452 | Sound Speeds, Cracking and Stability of Self-Gravitating Anisotropic
Compact Objects | Using the the concept of cracking we explore the influence of density
fluctuations and local anisotropy have on the stability of local and non-local
anisotropic matter configurations in general relativity. This concept,
conceived to describe the behaviour of a fluid distribution just after its
departure from equilibr... | gr-qc | using the the concept of cracking we explore the influence of density fluctuations and local anisotropy have on the stability of local and nonlocal anisotropic matter configurations in general relativity this concept conceived to describe the behaviour of a fluid distribution just after its departure from equilibrium p... | [['using', 'the', 'the', 'concept', 'of', 'cracking', 'we', 'explore', 'the', 'influence', 'of', 'density', 'fluctuations', 'and', 'local', 'anisotropy', 'have', 'on', 'the', 'stability', 'of', 'local', 'and', 'nonlocal', 'anisotropic', 'matter', 'configurations', 'in', 'general', 'relativity', 'this', 'concept', 'conc... | [-0.13988953199550774, 0.13460794392578093, -0.16560594788010735, 0.06305949329872476, -0.05120387462388098, -0.05548813168486926, -0.008159059242023963, 0.3399201118453216, -0.27121329226374497, -0.2836282290600702, 0.07163231325154482, -0.23698299646839105, -0.10364445039293671, 0.16811986353281325, -0.01394379916559... |
706.3453 | About agreement of PYTHIA and the experimental results in $e^+e^-$
annihilation to hadrons | The experimental charged particles multiplicity distributions in $e^+e^-$
annihilation to hadrons are compared with the distributions obtained by PYTHIA.
The ratio $\chi^2$/degrees of freedom is calculated for 6 energies at
$\sqrt{s}$ 14 -- 206.2 GeV. The necessity of more subtle tuning of PYTHIA at
the energy of $Z^... | hep-ph | the experimental charged particles multiplicity distributions in ee annihilation to hadrons are compared with the distributions obtained by pythia the ratio chi2degrees of freedom is calculated for 6 energies at sqrts 14 2062 gev the necessity of more subtle tuning of pythia at the energy of z0 peak is discussed | [['the', 'experimental', 'charged', 'particles', 'multiplicity', 'distributions', 'in', 'ee', 'annihilation', 'to', 'hadrons', 'are', 'compared', 'with', 'the', 'distributions', 'obtained', 'by', 'pythia', 'the', 'ratio', 'chi2degrees', 'of', 'freedom', 'is', 'calculated', 'for', '6', 'energies', 'at', 'sqrts', '14', '... | [-0.039690663636548024, 0.23638954340380483, -0.07827749856918746, 0.19081710847759886, 0.04443348067983681, -0.10549123556714277, -0.055631638005641956, 0.40362613070376063, -0.12696503438245582, -0.39370061335515005, -0.11732668733005697, -0.4050437750826989, 0.1595460994986399, 0.14610012278568987, 0.115785758030049... |
706.3454 | Reconstruction of Quantum Well Potentials via the Intertwining Operator
Technique | One of the most important issues of quantum engineering is the construction
of low-dimensional structures possessing desirable properties. For example, in
different areas of possible applications of the structures containing quantum
wells (QW), there is need to have QW energy spectrum, which is predetermined.
Then ... | cond-mat.mes-hall | one of the most important issues of quantum engineering is the construction of lowdimensional structures possessing desirable properties for example in different areas of possible applications of the structures containing quantum wells qw there is need to have qw energy spectrum which is predetermined then the followin... | [['one', 'of', 'the', 'most', 'important', 'issues', 'of', 'quantum', 'engineering', 'is', 'the', 'construction', 'of', 'lowdimensional', 'structures', 'possessing', 'desirable', 'properties', 'for', 'example', 'in', 'different', 'areas', 'of', 'possible', 'applications', 'of', 'the', 'structures', 'containing', 'quant... | [-0.06582048941801781, 0.09652961049163121, -0.08738390576182561, 0.06411630181959395, -0.0906295584275018, -0.18473786916087806, 0.006841345759075598, 0.37965693086738417, -0.2971955638953358, -0.30255853262669324, 0.048823934212360066, -0.24913486432350934, -0.16363313423398024, 0.20776703218053255, -0.03920184920360... |
706.3455 | Thermodynamics of Few-Particle Systems | We consider the wide class of few-particle systems that have some analog of
the thermodynamic laws. These systems are characterized by the distributions
that are determined by the Hamiltonian and satisfy the Liouville equation.
Few-particle systems of this class are described by a non-holonomic constraint:
the power ... | math-ph math.MP | we consider the wide class of fewparticle systems that have some analog of the thermodynamic laws these systems are characterized by the distributions that are determined by the hamiltonian and satisfy the liouville equation fewparticle systems of this class are described by a nonholonomic constraint the power of nonpo... | [['we', 'consider', 'the', 'wide', 'class', 'of', 'fewparticle', 'systems', 'that', 'have', 'some', 'analog', 'of', 'the', 'thermodynamic', 'laws', 'these', 'systems', 'are', 'characterized', 'by', 'the', 'distributions', 'that', 'are', 'determined', 'by', 'the', 'hamiltonian', 'and', 'satisfy', 'the', 'liouville', 'eq... | [-0.1972539185274703, 0.17071148618318452, -0.027727511963651825, 0.04048892143934305, -0.001371098100207746, -0.12804790322843473, -0.02682750066984833, 0.27698847756012884, -0.28725349887584645, -0.29210298680118285, 0.0928740206945804, -0.2571554883616045, -0.15643256893054058, 0.22484497089559832, -0.01872904831543... |
706.3456 | Nonperturbative Scaling Theory of Free Magnetic Moment Phases in
Disordered Metals | The crossover between a free magnetic moment phase and a Kondo phase in low
dimensional disordered metals with dilute magnetic impurities is studied.
We perform a finite size scaling analysis of the distribution of the Kondo
temperature as obtained from a numerical renormalization group calculation of
the local mag... | cond-mat.str-el cond-mat.mes-hall | the crossover between a free magnetic moment phase and a kondo phase in low dimensional disordered metals with dilute magnetic impurities is studied we perform a finite size scaling analysis of the distribution of the kondo temperature as obtained from a numerical renormalization group calculation of the local magnetic... | [['the', 'crossover', 'between', 'a', 'free', 'magnetic', 'moment', 'phase', 'and', 'a', 'kondo', 'phase', 'in', 'low', 'dimensional', 'disordered', 'metals', 'with', 'dilute', 'magnetic', 'impurities', 'is', 'studied', 'we', 'perform', 'a', 'finite', 'size', 'scaling', 'analysis', 'of', 'the', 'distribution', 'of', 't... | [-0.17899926626481688, 0.2427339184205406, -0.04663030875093192, 0.05744013119166574, 0.0058654628568687115, -0.12356125882002883, 0.10762481710407883, 0.31190972614567725, -0.2845421056048228, -0.27783440495035255, 0.013214057944535923, -0.32582624955819206, -0.08293641623324499, 0.13698738019626874, 0.094157992835299... |
706.3457 | Quantum theory for spatial motion of polaritons in inhomogeneous fields | Polaritons are the collective excitations of many atoms dressed by resonant
photons, which can be used to explain the slow light propagation with the
mechanism of electromagnetically induced transparency. As quasi-particles,
these collective excitations possess the typical feature of the matter
particles, which can b... | quant-ph | polaritons are the collective excitations of many atoms dressed by resonant photons which can be used to explain the slow light propagation with the mechanism of electromagnetically induced transparency as quasiparticles these collective excitations possess the typical feature of the matter particles which can be refle... | [['polaritons', 'are', 'the', 'collective', 'excitations', 'of', 'many', 'atoms', 'dressed', 'by', 'resonant', 'photons', 'which', 'can', 'be', 'used', 'to', 'explain', 'the', 'slow', 'light', 'propagation', 'with', 'the', 'mechanism', 'of', 'electromagnetically', 'induced', 'transparency', 'as', 'quasiparticles', 'the... | [-0.1400405210200939, 0.28145006880575757, -0.11694263606090341, 0.060776071410547555, -0.0898724328605579, -0.09442905033031454, -0.016808408087228315, 0.41547815986703357, -0.28252410791911087, -0.3006602341079383, -0.02320967840451094, -0.2638042862224695, -0.12897892938563962, 0.14516210093331341, 0.001176714455684... |
706.3458 | The Thermodynamic Casimir Effect in $^4$He Films near $T_\lambda$: Monte
Carlo Results | The universal finite-size scaling function of the critical Casimir force for
the three dimensional XY universality class with Dirichlet boundary conditions
is determined using Monte Carlo simulations. The results are in excellent
agreement with recent experiments on $^4$He Films at the superfluid transition
and with ... | cond-mat.stat-mech | the universal finitesize scaling function of the critical casimir force for the three dimensional xy universality class with dirichlet boundary conditions is determined using monte carlo simulations the results are in excellent agreement with recent experiments on 4he films at the superfluid transition and with availab... | [['the', 'universal', 'finitesize', 'scaling', 'function', 'of', 'the', 'critical', 'casimir', 'force', 'for', 'the', 'three', 'dimensional', 'xy', 'universality', 'class', 'with', 'dirichlet', 'boundary', 'conditions', 'is', 'determined', 'using', 'monte', 'carlo', 'simulations', 'the', 'results', 'are', 'in', 'excell... | [-0.08256768891199802, 0.18972003491944633, -0.07927145268816578, 0.01993698139024976, 0.007411408708624852, -0.16101257258560508, 0.0011683615545431774, 0.38629708128670853, -0.17232410047048083, -0.2661769314048191, 0.04155574727580339, -0.3826794851338491, -0.062591482468027, 0.25137303257361054, 0.10138982608138274... |
706.3459 | NP by means of lifts and shadows | We show that every NP problem is polynomially equivalent to a simple
combinatorial problem: the membership problem for a special class of digraphs.
These classes are defined by means of shadows (projections) and by finitely
many forbidden colored (lifted) subgraphs. Our characterization is motivated by
the analysis o... | cs.CC math.CO | we show that every np problem is polynomially equivalent to a simple combinatorial problem the membership problem for a special class of digraphs these classes are defined by means of shadows projections and by finitely many forbidden colored lifted subgraphs our characterization is motivated by the analysis of syntact... | [['we', 'show', 'that', 'every', 'np', 'problem', 'is', 'polynomially', 'equivalent', 'to', 'a', 'simple', 'combinatorial', 'problem', 'the', 'membership', 'problem', 'for', 'a', 'special', 'class', 'of', 'digraphs', 'these', 'classes', 'are', 'defined', 'by', 'means', 'of', 'shadows', 'projections', 'and', 'by', 'fini... | [-0.13032780412840178, 0.08719381476157181, -0.021568163504497598, 0.09932875032080625, -0.13860400952158747, -0.1392314128347279, 0.034801732487112436, 0.36484126911796244, -0.3764738351491894, -0.3065483327042888, 0.09032658383264638, -0.24820331681985408, -0.1458976268672298, 0.18855614467573797, -0.1323257526088765... |
706.346 | The AGN nature of 11 out of 12 Swift/RXTE unidentified sources through
optical and X-ray spectroscopy | The Swift Burst Alert Telescope (BAT) is performing a high Galactic latitude
survey in the 14-195 keV band at a flux limit of ~10^{-11} erg cm^{-2} s^{-1},
leading to the discovery of new high energy sources, most of which have not so
far been properly classified. A similar work has also been performed with the
RXTE ... | astro-ph | the swift burst alert telescope bat is performing a high galactic latitude survey in the 14195 kev band at a flux limit of 1011 erg cm2 s1 leading to the discovery of new high energy sources most of which have not so far been properly classified a similar work has also been performed with the rxte slew survey leading t... | [['the', 'swift', 'burst', 'alert', 'telescope', 'bat', 'is', 'performing', 'a', 'high', 'galactic', 'latitude', 'survey', 'in', 'the', '14195', 'kev', 'band', 'at', 'a', 'flux', 'limit', 'of', '1011', 'erg', 'cm2', 's1', 'leading', 'to', 'the', 'discovery', 'of', 'new', 'high', 'energy', 'sources', 'most', 'of', 'whic... | [-0.07159367193457829, 0.09487359215206398, -0.004057625153972784, 0.09212888148655302, -0.10549053201277064, -0.1335384391823158, 0.10020196541642858, 0.457791225422789, -0.12376136598740418, -0.41564228560519995, 0.12948692806312204, -0.36399559127267733, 0.00651826210225855, 0.2515312933248706, -0.011948783168340579... |
706.3461 | Geometrization of quantum formalism | The hypothesis is suggested that the equation for the Dirac free wave field
is, in fact, a group-theoretical relation describing propagation of specific
microscopic deviations of space geometry from the euclidean one (closed
topological manifolds). The Dirac equation for a hydrogen atom can also be
interpreted as a r... | quant-ph | the hypothesis is suggested that the equation for the dirac free wave field is in fact a grouptheoretical relation describing propagation of specific microscopic deviations of space geometry from the euclidean one closed topological manifolds the dirac equation for a hydrogen atom can also be interpreted as a relation ... | [['the', 'hypothesis', 'is', 'suggested', 'that', 'the', 'equation', 'for', 'the', 'dirac', 'free', 'wave', 'field', 'is', 'in', 'fact', 'a', 'grouptheoretical', 'relation', 'describing', 'propagation', 'of', 'specific', 'microscopic', 'deviations', 'of', 'space', 'geometry', 'from', 'the', 'euclidean', 'one', 'closed'... | [-0.13542183555816253, 0.16447693147917383, -0.1118237814270728, 0.11558769909381751, -0.10582966904741586, -0.09142708520107355, 0.010837036482605738, 0.31155881487293957, -0.26882329351777573, -0.2778075287483402, 0.004090337345578237, -0.25401917581936134, -0.15218368022385792, 0.1573945449607581, -0.007449555395593... |
706.3462 | Stability of Hodge bundles and a numerical characterization of Shimura
varieties | Consider a family f:A --> U of g-dimensional abelian varieties over a
quasiprojective manifold U. Suppose that the induced map from U to the moduli
scheme of polarized abelian varieties is generically finite and that there is a
projective manifold Y, containing U as the complement of a normal crossing
divisor S, such... | math.AG math.CV | consider a family fa u of gdimensional abelian varieties over a quasiprojective manifold u suppose that the induced map from u to the moduli scheme of polarized abelian varieties is generically finite and that there is a projective manifold y containing u as the complement of a normal crossing divisor s such that the s... | [['consider', 'a', 'family', 'fa', 'u', 'of', 'gdimensional', 'abelian', 'varieties', 'over', 'a', 'quasiprojective', 'manifold', 'u', 'suppose', 'that', 'the', 'induced', 'map', 'from', 'u', 'to', 'the', 'moduli', 'scheme', 'of', 'polarized', 'abelian', 'varieties', 'is', 'generically', 'finite', 'and', 'that', 'there... | [-0.20453618359341122, 0.06528821814237823, -0.08212987472985518, 0.03661515853021612, -0.09285391272508843, -0.18776876687689778, 0.007585950515931472, 0.3410862510100027, -0.3723480645666785, -0.16495500624903234, 0.07474018888234256, -0.2740781378850122, -0.1328415474070007, 0.1936590707024969, -0.09763642055116953,... |
706.3463 | Classification of hyperfinite factors up to completely bounded
isomorphism of their preduals | In this paper we consider the following problem: When are the preduals of two
hyperfinite (=injective) factors $\M$ and $\N$ (on separable Hilbert spaces)
cb-isomorphic (i.e., isomorphic as operator spaces)? We show that if $\M$ is
semifinite and $\N$ is type III, then their preduals are not cb-isomorphic.
Moreover, ... | math.OA | in this paper we consider the following problem when are the preduals of two hyperfinite injective factors m and n on separable hilbert spaces cbisomorphic ie isomorphic as operator spaces we show that if m is semifinite and n is type iii then their preduals are not cbisomorphic moreover we construct a oneparameter fam... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'following', 'problem', 'when', 'are', 'the', 'preduals', 'of', 'two', 'hyperfinite', 'injective', 'factors', 'm', 'and', 'n', 'on', 'separable', 'hilbert', 'spaces', 'cbisomorphic', 'ie', 'isomorphic', 'as', 'operator', 'spaces', 'we', 'show', 'that', 'if', 'm', 'is', ... | [-0.11647238804508243, 0.1490843564601297, -0.011366356751025935, 0.06436193620027005, -0.08883910186255609, -0.18915890327586635, -0.04018393645964078, 0.4027396029209703, -0.3009414279045976, -0.12930896234645592, 0.14465757882709016, -0.3364814799993556, -0.15009448298714995, 0.16924650012515485, -0.1803652378683152... |
706.3464 | The Disk and Extraplanar Regions of NGC 2403 | Wide field images obtained with WIRCam and MegaCam on the
Canada-France-Hawaii Telescope are used to probe the spatial distribution of
young stars in the Sc galaxy NGC 2403. Bright main sequence stars and blue
supergiants are detected out to projected galactocentric distances of ~14 kpc
(~7 disk scale lengths) along ... | astro-ph | wide field images obtained with wircam and megacam on the canadafrancehawaii telescope are used to probe the spatial distribution of young stars in the sc galaxy ngc 2403 bright main sequence stars and blue supergiants are detected out to projected galactocentric distances of 14 kpc 7 disk scale lengths along the major... | [['wide', 'field', 'images', 'obtained', 'with', 'wircam', 'and', 'megacam', 'on', 'the', 'canadafrancehawaii', 'telescope', 'are', 'used', 'to', 'probe', 'the', 'spatial', 'distribution', 'of', 'young', 'stars', 'in', 'the', 'sc', 'galaxy', 'ngc', '2403', 'bright', 'main', 'sequence', 'stars', 'and', 'blue', 'supergia... | [-0.07222359738374266, 0.10382082304579354, -0.049918708521945236, 0.07303578215189177, -0.06022134138785795, -0.03841150509918757, 0.02765861370624315, 0.4896760206626083, -0.1350525772481693, -0.4002260721872057, 0.04174946267873498, -0.31462381282234236, 0.02932754734799208, 0.20940189152876285, -0.06869946276055149... |
706.3465 | Cosmological Constraint on the Effective Number of Neutrino Species | We discuss constraints on the effective number of neutrino species Nnu from
recent cosmological observations such as CMB, LSS, BBN, including our own
analysis which uses the WMAP and the Luminous Red Galaxy power spectrum data.
We also discuss their implications on some non-standard cosmological scenarios
such as the... | astro-ph | we discuss constraints on the effective number of neutrino species nnu from recent cosmological observations such as cmb lss bbn including our own analysis which uses the wmap and the luminous red galaxy power spectrum data we also discuss their implications on some nonstandard cosmological scenarios such as the low me... | [['we', 'discuss', 'constraints', 'on', 'the', 'effective', 'number', 'of', 'neutrino', 'species', 'nnu', 'from', 'recent', 'cosmological', 'observations', 'such', 'as', 'cmb', 'lss', 'bbn', 'including', 'our', 'own', 'analysis', 'which', 'uses', 'the', 'wmap', 'and', 'the', 'luminous', 'red', 'galaxy', 'power', 'spect... | [-0.06746243969179117, 0.1726131359831645, -0.055470179809400666, 0.14241003525944856, -0.13988566142506897, -0.10993753101390141, 0.012634688071333444, 0.32492708727144276, -0.2078982022877496, -0.3539463192797624, 0.08655955532852273, -0.32655570819400825, -0.05203853895744452, 0.19126797343303154, 0.0610634631978777... |
706.3466 | N=8 supersymmetric mechanics on the sphere S^3 | Starting from quaternionic N=8 supersymmetric mechanics we perform a
reduction over a bosonic radial variable, ending up with a nonlinear off-shell
supermultiplet with three bosonic end eight fermionic physical degrees of
freedom. The geometry of the bosonic sector of the most general sigma-model
type action is descr... | hep-th | starting from quaternionic n8 supersymmetric mechanics we perform a reduction over a bosonic radial variable ending up with a nonlinear offshell supermultiplet with three bosonic end eight fermionic physical degrees of freedom the geometry of the bosonic sector of the most general sigmamodel type action is described by... | [['starting', 'from', 'quaternionic', 'n8', 'supersymmetric', 'mechanics', 'we', 'perform', 'a', 'reduction', 'over', 'a', 'bosonic', 'radial', 'variable', 'ending', 'up', 'with', 'a', 'nonlinear', 'offshell', 'supermultiplet', 'with', 'three', 'bosonic', 'end', 'eight', 'fermionic', 'physical', 'degrees', 'of', 'freed... | [-0.1466262410145386, 0.19453832364953477, -0.04761634645650962, 0.01109654668523165, -0.11051385126691977, -0.20195749125975584, -0.03503460911659723, 0.274624509287865, -0.1866426630346853, -0.24218434916942247, 0.0612419095185552, -0.29044031883157523, -0.17485378277238592, 0.12430314589333388, -0.02023741732617574,... |
706.3467 | Coupled phantom field in loop quantum cosmology | A model of phantom scalar field dark energy under exponential potential
coupling to barotropic dark matter fluid in loop quantum cosmology is addressed
here. We derive a closed-autonomous system for cosmological dynamics in this
scenario. The expansion in loop quantum universe has a bounce even in presence
of the pha... | gr-qc astro-ph hep-th | a model of phantom scalar field dark energy under exponential potential coupling to barotropic dark matter fluid in loop quantum cosmology is addressed here we derive a closedautonomous system for cosmological dynamics in this scenario the expansion in loop quantum universe has a bounce even in presence of the phantom ... | [['a', 'model', 'of', 'phantom', 'scalar', 'field', 'dark', 'energy', 'under', 'exponential', 'potential', 'coupling', 'to', 'barotropic', 'dark', 'matter', 'fluid', 'in', 'loop', 'quantum', 'cosmology', 'is', 'addressed', 'here', 'we', 'derive', 'a', 'closedautonomous', 'system', 'for', 'cosmological', 'dynamics', 'in... | [-0.18995274811544838, 0.19171264774038219, -0.13572808889690421, 0.11182047771267119, -0.058693894650787115, -0.1805307062790163, -0.06418577181266658, 0.2858736067279881, -0.19529623718813574, -0.3367685543774974, -0.004180684071673336, -0.2227856967525155, -0.03584472500883481, 0.15442841577654084, 0.023705932836723... |
706.3468 | Investigating diffractive W production in hadron-hadron collisions at
high energies | We compute the hard diffractive hadroproduction of bosons W at high energies
using Regge factorization and taking into account multiple Pomeron exchange
corrections. The ratio of diffractive to non-diffractive W production agrees
with the current Tevatron data and a prediction for the LHC is presented.
| hep-ph | we compute the hard diffractive hadroproduction of bosons w at high energies using regge factorization and taking into account multiple pomeron exchange corrections the ratio of diffractive to nondiffractive w production agrees with the current tevatron data and a prediction for the lhc is presented | [['we', 'compute', 'the', 'hard', 'diffractive', 'hadroproduction', 'of', 'bosons', 'w', 'at', 'high', 'energies', 'using', 'regge', 'factorization', 'and', 'taking', 'into', 'account', 'multiple', 'pomeron', 'exchange', 'corrections', 'the', 'ratio', 'of', 'diffractive', 'to', 'nondiffractive', 'w', 'production', 'agr... | [-0.04038924553638531, 0.1900450106503235, -0.14656939930282534, 0.20206359944875454, -0.04065969551189078, -0.15534011523963676, 0.020131820626556874, 0.35874091966284644, -0.21464285851559706, -0.21736448568602404, -0.055719945962644284, -0.3675250023603439, 0.10599764031875465, 0.12884000684652064, 0.098653508474429... |
706.3469 | Entanglement and Timing-Based Mechanisms in the Coherent Control of
Scattering Processes | The coherent control of scattering processes is considered, with electron
impact dissociation of H$_2^+$ used as an example. The physical mechanism
underlying coherently controlled stationary state scattering is exposed by
analyzing a control scenario that relies on previously established entanglement
requirements be... | quant-ph physics.atom-ph physics.chem-ph | the coherent control of scattering processes is considered with electron impact dissociation of h_2 used as an example the physical mechanism underlying coherently controlled stationary state scattering is exposed by analyzing a control scenario that relies on previously established entanglement requirements between th... | [['the', 'coherent', 'control', 'of', 'scattering', 'processes', 'is', 'considered', 'with', 'electron', 'impact', 'dissociation', 'of', 'h_2', 'used', 'as', 'an', 'example', 'the', 'physical', 'mechanism', 'underlying', 'coherently', 'controlled', 'stationary', 'state', 'scattering', 'is', 'exposed', 'by', 'analyzing'... | [-0.1399839974137851, 0.16606102461575775, -0.11493623657669458, 0.07255972908331185, -0.03544173259288073, -0.15884715870488436, 0.04751395849291132, 0.3747555690921015, -0.28938276673822355, -0.2650105360300384, 0.033971575619782216, -0.2506570306128803, -0.09769238571041367, 0.1851771918332411, -0.000335878332973354... |
706.347 | Coherent Control and Entanglement in the Attosecond Electron Recollision
Dissociation of D2+ | We examine the attosecond electron recollision dissociation of D2+ recently
demonstrated experimentally [H. Niikura et al., Nature (London) 421, 826
(2003)] from a coherent control perspective. In this process, a strong laser
field incident on D2 ionizes an electron, accelerates the electron in the laser
field to eV ... | quant-ph physics.atom-ph physics.chem-ph | we examine the attosecond electron recollision dissociation of d2 recently demonstrated experimentally h niikura et al nature london 421 826 2003 from a coherent control perspective in this process a strong laser field incident on d2 ionizes an electron accelerates the electron in the laser field to ev energies and the... | [['we', 'examine', 'the', 'attosecond', 'electron', 'recollision', 'dissociation', 'of', 'd2', 'recently', 'demonstrated', 'experimentally', 'h', 'niikura', 'et', 'al', 'nature', 'london', '421', '826', '2003', 'from', 'a', 'coherent', 'control', 'perspective', 'in', 'this', 'process', 'a', 'strong', 'laser', 'field', ... | [-0.10042897111925728, 0.19176809703375594, -0.06385864033585503, 0.08137877643978113, 0.030133675493590244, -0.1514865515241601, 0.02992483985094249, 0.4043664216180836, -0.23500102211998924, -0.2730779679314721, -0.03014379550674648, -0.2792987098002169, -0.07900531201127481, 0.19978733816450195, 0.011991949611871597... |
706.3471 | Radiation- and Phonon-Bottleneck-Induced Tunneling in the Fe8
Single-Molecule Magnet | We measure magnetization changes in a single crystal of the single-molecule
magnet Fe8 when exposed to intense, short (<20 $\mu$s) pulses of microwave
radiation resonant with the m = 10 to 9 transition. We find that radiation
induces a phonon bottleneck in the system with a time scale of ~5 $\mu$s. The
phonon bottlen... | cond-mat.mes-hall cond-mat.mtrl-sci | we measure magnetization changes in a single crystal of the singlemolecule magnet fe8 when exposed to intense short 20 mus pulses of microwave radiation resonant with the m 10 to 9 transition we find that radiation induces a phonon bottleneck in the system with a time scale of 5 mus the phonon bottleneck in turn drives... | [['we', 'measure', 'magnetization', 'changes', 'in', 'a', 'single', 'crystal', 'of', 'the', 'singlemolecule', 'magnet', 'fe8', 'when', 'exposed', 'to', 'intense', 'short', '20', 'mus', 'pulses', 'of', 'microwave', 'radiation', 'resonant', 'with', 'the', 'm', '10', 'to', '9', 'transition', 'we', 'find', 'that', 'radiati... | [-0.1896478029039617, 0.24145521194888994, -0.05498911118503291, 0.009771769252288473, 0.00122863686436296, -0.1459806761154291, 0.09418408914244028, 0.3899771497472302, -0.2899768038519791, -0.35164450031224187, 0.006061708120946455, -0.2978702225737724, -0.012522311358994696, 0.21903096633492508, 0.08535109973604699,... |
706.3472 | Stationarity and Self-similarity Characterization of the Set-indexed
Fractional Brownian Motion | The set-indexed fractional Brownian motion (sifBm) has been defined by
Herbin-Merzbach (2006) for indices that are subsets of a metric measure space.
In this paper, the sifBm is proved to statisfy a strenghtened definition of
increment stationarity. This new definition for stationarity property allows to
get a comple... | math.PR | the setindexed fractional brownian motion sifbm has been defined by herbinmerzbach 2006 for indices that are subsets of a metric measure space in this paper the sifbm is proved to statisfy a strenghtened definition of increment stationarity this new definition for stationarity property allows to get a complete characte... | [['the', 'setindexed', 'fractional', 'brownian', 'motion', 'sifbm', 'has', 'been', 'defined', 'by', 'herbinmerzbach', '2006', 'for', 'indices', 'that', 'are', 'subsets', 'of', 'a', 'metric', 'measure', 'space', 'in', 'this', 'paper', 'the', 'sifbm', 'is', 'proved', 'to', 'statisfy', 'a', 'strenghtened', 'definition', '... | [-0.10296484893396103, 0.1532876417286906, -0.13234215093079985, 0.039921725906816294, -0.10417876287355898, -0.08175915057536184, 0.012389180528726883, 0.3687591636629124, -0.3079800937311512, -0.2111086260481942, 0.14567695278390425, -0.24331256734196388, -0.13525119807374308, 0.1811250531208338, -0.12910181898017967... |
706.3473 | On a class of gauge theories | We give a framework to describe gauge theory in which a nonassociative
Moufang loop takes the place of the structure group. The structure of such
gauge theory has many formal similarities with that of Yang-Mills theory. We
extend the gauge invariance to this theory and construct an on-shell version of
N=1 supersymmet... | hep-th | we give a framework to describe gauge theory in which a nonassociative moufang loop takes the place of the structure group the structure of such gauge theory has many formal similarities with that of yangmills theory we extend the gauge invariance to this theory and construct an onshell version of n1 supersymmetric gau... | [['we', 'give', 'a', 'framework', 'to', 'describe', 'gauge', 'theory', 'in', 'which', 'a', 'nonassociative', 'moufang', 'loop', 'takes', 'the', 'place', 'of', 'the', 'structure', 'group', 'the', 'structure', 'of', 'such', 'gauge', 'theory', 'has', 'many', 'formal', 'similarities', 'with', 'that', 'of', 'yangmills', 'th... | [-0.1341280576652261, 0.15926488721123422, -0.17294107153321858, 0.11842687219959097, -0.10694172802484697, -0.11310852024083336, -0.024910674001417915, 0.3296598009420214, -0.22611553549628566, -0.24388146721240547, 0.024849533666080486, -0.215659046890559, -0.23790117665366442, 0.05524272478565022, -0.068470798010282... |
706.3474 | An exact geometric mass formula | We show an exact geometric mass formula for superspecial points in the
reduction of any quaternionic Shimura variety modulo at a good prime $p$.
| math.NT | we show an exact geometric mass formula for superspecial points in the reduction of any quaternionic shimura variety modulo at a good prime p | [['we', 'show', 'an', 'exact', 'geometric', 'mass', 'formula', 'for', 'superspecial', 'points', 'in', 'the', 'reduction', 'of', 'any', 'quaternionic', 'shimura', 'variety', 'modulo', 'at', 'a', 'good', 'prime', 'p']] | [-0.23261713197765252, -0.030125408481277798, -0.1576334943723244, 0.1349752392464628, -0.056446374976076186, -0.1611391581245698, 0.0419356218772009, 0.25793111658034223, -0.2783037012753387, -0.2813267960057904, -0.028309794535744004, -0.21958620101213455, -0.1223423976431756, 0.3071105781321724, -0.19851719467745474... |
706.3475 | Emergence of time and Observable physics | This is a philosophy paper rather than mathematical physics work. I will
publish it in some other place.
| physics.gen-ph | this is a philosophy paper rather than mathematical physics work i will publish it in some other place | [['this', 'is', 'a', 'philosophy', 'paper', 'rather', 'than', 'mathematical', 'physics', 'work', 'i', 'will', 'publish', 'it', 'in', 'some', 'other', 'place']] | [-0.024563025786644883, 0.08818987249914143, -0.16556341107934713, 0.13316780753019783, -0.2745392271834943, -0.20297373642420602, 0.032596998078386404, 0.30623362958431244, -0.23277096385653648, -0.2868331838399172, 0.09706210610844816, -0.28467574071449536, -0.2093861617354883, 0.20730232385297617, -0.149382908466375... |
706.3476 | Baxter operator and Archimedean Hecke algebra | In this paper we introduce Baxter integral Q-operators for finite-dimensional
Lie algebras gl(n+1) and so(2n+1). Whittaker functions corresponding to these
algebras are eigenfunctions of the Q-operators with the eigenvalues expressed
in terms of Gamma-functions. The appearance of the Gamma-functions is one of
the man... | math.RT | in this paper we introduce baxter integral qoperators for finitedimensional lie algebras gln1 and so2n1 whittaker functions corresponding to these algebras are eigenfunctions of the qoperators with the eigenvalues expressed in terms of gammafunctions the appearance of the gammafunctions is one of the manifestations of ... | [['in', 'this', 'paper', 'we', 'introduce', 'baxter', 'integral', 'qoperators', 'for', 'finitedimensional', 'lie', 'algebras', 'gln1', 'and', 'so2n1', 'whittaker', 'functions', 'corresponding', 'to', 'these', 'algebras', 'are', 'eigenfunctions', 'of', 'the', 'qoperators', 'with', 'the', 'eigenvalues', 'expressed', 'in'... | [-0.15528125751451283, 0.07310994769516958, -0.10211420601182614, 0.09239862001540061, -0.16033187338212382, -0.07220574163881961, -0.05151235828494018, 0.32164337726945647, -0.3134026710811199, -0.2075810683612338, 0.07843562478442191, -0.23444262451999737, -0.2127656053380851, 0.188598613233813, -0.10824782124331533,... |
706.3477 | OrfMapper: A Web-Based Application for Visualizing Gene Clusters on
Metabolic Pathway Maps | Computational analyses of, e.g., genomic, proteomic, or metabolomic data,
commonly result in one or more sets of candidate genes, proteins, or enzymes.
These sets are often the outcome of clustering algorithms. Subsequently, it has
to be tested if, e.g., the candidate gene-products are members of known
metabolic proc... | q-bio.GN | computational analyses of eg genomic proteomic or metabolomic data commonly result in one or more sets of candidate genes proteins or enzymes these sets are often the outcome of clustering algorithms subsequently it has to be tested if eg the candidate geneproducts are members of known metabolic processes with orfmappe... | [['computational', 'analyses', 'of', 'eg', 'genomic', 'proteomic', 'or', 'metabolomic', 'data', 'commonly', 'result', 'in', 'one', 'or', 'more', 'sets', 'of', 'candidate', 'genes', 'proteins', 'or', 'enzymes', 'these', 'sets', 'are', 'often', 'the', 'outcome', 'of', 'clustering', 'algorithms', 'subsequently', 'it', 'ha... | [-0.0640299258419596, 0.0682851411132277, -0.04423758255628248, 0.10559577812049267, -0.08439922399575943, -0.19267497433727418, 0.07718986430731804, 0.41323471015346225, -0.239600187504961, -0.3383832991366153, 0.12882463479974726, -0.33016690139429294, -0.14225086275204693, 0.2570559322948743, -0.019039147972142782, ... |
706.3478 | Relations between tautological cycles on Jacobians | We study tautological cycle classes on the Jacobian of a curve. We prove a
new result about the ring of tautological classes on a general curve that
allows, among other things, easy dimension calculations and leads to some
general results about the structure of this ring. Next we obtain a vanishing
result for some of... | math.AG | we study tautological cycle classes on the jacobian of a curve we prove a new result about the ring of tautological classes on a general curve that allows among other things easy dimension calculations and leads to some general results about the structure of this ring next we obtain a vanishing result for some of the g... | [['we', 'study', 'tautological', 'cycle', 'classes', 'on', 'the', 'jacobian', 'of', 'a', 'curve', 'we', 'prove', 'a', 'new', 'result', 'about', 'the', 'ring', 'of', 'tautological', 'classes', 'on', 'a', 'general', 'curve', 'that', 'allows', 'among', 'other', 'things', 'easy', 'dimension', 'calculations', 'and', 'leads'... | [-0.19146598947280255, -0.013333522686644145, -0.11847800680543066, 0.060508915804303634, -0.10286595925429194, -0.11745497498081112, 0.047769801281812435, 0.2940860288828367, -0.31433868438738294, -0.232523887876238, 0.05179119967763907, -0.22718043882816316, -0.18213959541896999, 0.2658618383136288, -0.14014844352295... |
706.3479 | Hypocomputation | Hypercomputational formal theories will, clearly, be both structurally and
foundationally different from the formal theories underpinning computational
theories. However, many of the maps that might guide us into this strange realm
have been lost. So little work has been done recently in the area of
metamathematics, ... | cs.OH | hypercomputational formal theories will clearly be both structurally and foundationally different from the formal theories underpinning computational theories however many of the maps that might guide us into this strange realm have been lost so little work has been done recently in the area of metamathematics and so m... | [['hypercomputational', 'formal', 'theories', 'will', 'clearly', 'be', 'both', 'structurally', 'and', 'foundationally', 'different', 'from', 'the', 'formal', 'theories', 'underpinning', 'computational', 'theories', 'however', 'many', 'of', 'the', 'maps', 'that', 'might', 'guide', 'us', 'into', 'this', 'strange', 'realm... | [-0.06600747078748971, 0.09204068197397364, -0.15583557603408543, 0.08949981056052116, -0.13127704439553575, -0.11272680856497355, 0.014076256133988172, 0.3668644729818047, -0.24836554645534448, -0.29229287092219775, 0.09990973180917447, -0.2761412192608269, -0.19862792969510798, 0.18146242086880537, -0.124651673007231... |
706.348 | Tight Bounds on the Average Length, Entropy, and Redundancy of
Anti-Uniform Huffman Codes | In this paper we consider the class of anti-uniform Huffman codes and derive
tight lower and upper bounds on the average length, entropy, and redundancy of
such codes in terms of the alphabet size of the source. The Fibonacci
distributions are introduced which play a fundamental role in AUH codes. It is
shown that su... | cs.IT math.IT | in this paper we consider the class of antiuniform huffman codes and derive tight lower and upper bounds on the average length entropy and redundancy of such codes in terms of the alphabet size of the source the fibonacci distributions are introduced which play a fundamental role in auh codes it is shown that such dist... | [['in', 'this', 'paper', 'we', 'consider', 'the', 'class', 'of', 'antiuniform', 'huffman', 'codes', 'and', 'derive', 'tight', 'lower', 'and', 'upper', 'bounds', 'on', 'the', 'average', 'length', 'entropy', 'and', 'redundancy', 'of', 'such', 'codes', 'in', 'terms', 'of', 'the', 'alphabet', 'size', 'of', 'the', 'source',... | [-0.13311486635437428, 0.14391391753786426, -0.05163876770663707, 0.10755211183394509, 0.034984153866682244, -0.1304198109662567, 0.07827259961585246, 0.30880611086927956, -0.28560337355499554, -0.30586551399580364, 0.09303113586140861, -0.2696270099573437, -0.12453453300585007, 0.23254904705742052, -0.0980676432225810... |
706.3481 | Astronomical Image Processing with Array Detectors | We address the question of astronomical image processing from data obtained
with array detectors. We define and analyze the cases of evenly, regularly, and
irregularly sampled maps for idealized (i.e., infinite) and realistic (i.e.,
finite) detectors. We concentrate on the effect of interpolation on the maps,
and the... | astro-ph | we address the question of astronomical image processing from data obtained with array detectors we define and analyze the cases of evenly regularly and irregularly sampled maps for idealized ie infinite and realistic ie finite detectors we concentrate on the effect of interpolation on the maps and the choice of the ke... | [['we', 'address', 'the', 'question', 'of', 'astronomical', 'image', 'processing', 'from', 'data', 'obtained', 'with', 'array', 'detectors', 'we', 'define', 'and', 'analyze', 'the', 'cases', 'of', 'evenly', 'regularly', 'and', 'irregularly', 'sampled', 'maps', 'for', 'idealized', 'ie', 'infinite', 'and', 'realistic', '... | [-0.06403316501904317, 0.09937024970698838, -0.06340707403918107, 0.12860157057320518, -0.03907613634047183, -0.12228248575984528, 0.051264335417818996, 0.4428062310649289, -0.2778185975850757, -0.31762004656848886, 0.19241216636587385, -0.26608277014409654, -0.12060965571524293, 0.1786397357983985, -0.1004958926780017... |
706.3482 | The Assembly History of Massive Galaxies: What Do We Know? | Understanding the formation history of massive galaxies is one of most
popular and longstanding problems in astronomy, with observations and theory
addressing how and when these systems assembled. Since the most massive
galaxies in today's universe, with M_*> 10^11 M_0, are nearly all elliptical
with uniform old stel... | astro-ph | understanding the formation history of massive galaxies is one of most popular and longstanding problems in astronomy with observations and theory addressing how and when these systems assembled since the most massive galaxies in todays universe with m_ 1011 m_0 are nearly all elliptical with uniform old stellar popula... | [['understanding', 'the', 'formation', 'history', 'of', 'massive', 'galaxies', 'is', 'one', 'of', 'most', 'popular', 'and', 'longstanding', 'problems', 'in', 'astronomy', 'with', 'observations', 'and', 'theory', 'addressing', 'how', 'and', 'when', 'these', 'systems', 'assembled', 'since', 'the', 'most', 'massive', 'gal... | [-0.10321014691144229, 0.17436236053084334, -0.011773434386899075, 0.10545704948146724, -0.01583680535821865, -0.06295484826486143, -0.009667185713123116, 0.43332058711805277, -0.07758267105712245, -0.39956148457299506, 0.07648652436573886, -0.29523115180691495, -0.040095507603966525, 0.20140995679319731, 0.01861734379... |
706.3483 | The size of isoperimetric surfaces in 3-manifolds and a rigidity result
for the upper hemisphere | We characterize the standard $\mathbb{S}^3$ as the closed Ricci-positive
3-manifold with scalar curvature at least 6 having isoperimetric surfaces of
largest area: $4\pi$. As a corollary we answer in the affirmative an
interesting special case of a conjecture of Min-Oo's on the scalar curvature
rigidity of the upper ... | math.DG | we characterize the standard mathbbs3 as the closed riccipositive 3manifold with scalar curvature at least 6 having isoperimetric surfaces of largest area 4pi as a corollary we answer in the affirmative an interesting special case of a conjecture of minoos on the scalar curvature rigidity of the upper hemisphere | [['we', 'characterize', 'the', 'standard', 'mathbbs3', 'as', 'the', 'closed', 'riccipositive', '3manifold', 'with', 'scalar', 'curvature', 'at', 'least', '6', 'having', 'isoperimetric', 'surfaces', 'of', 'largest', 'area', '4pi', 'as', 'a', 'corollary', 'we', 'answer', 'in', 'the', 'affirmative', 'an', 'interesting', '... | [-0.22790660943913585, 0.07109307628979877, -0.0345315868811061, 0.10587066338727406, -0.08337882508446152, -0.18576148538462198, -0.025449208177936573, 0.28510192073493573, -0.19764047341110805, -0.3021441391677702, 0.11563465094999022, -0.3182492633738245, -0.16945064008662789, 0.19842482664777586, -0.120245353299348... |
706.3484 | Diffraction at HERA and implications for Tevatron and LHC | We describe new QCD fits to diffractive cross sections measured at HERA and
we use the parton densities derived from these fits to predict the shape of the
dijet mass fraction in double Pomeron exchange at the Tevatron. We discuss the
existence of exclusive events in this dijet channel and some prospects are
given fo... | hep-ph | we describe new qcd fits to diffractive cross sections measured at hera and we use the parton densities derived from these fits to predict the shape of the dijet mass fraction in double pomeron exchange at the tevatron we discuss the existence of exclusive events in this dijet channel and some prospects are given for t... | [['we', 'describe', 'new', 'qcd', 'fits', 'to', 'diffractive', 'cross', 'sections', 'measured', 'at', 'hera', 'and', 'we', 'use', 'the', 'parton', 'densities', 'derived', 'from', 'these', 'fits', 'to', 'predict', 'the', 'shape', 'of', 'the', 'dijet', 'mass', 'fraction', 'in', 'double', 'pomeron', 'exchange', 'at', 'the... | [-0.024002922384329793, 0.15890806524507833, -0.140797103885888, 0.20704490370157974, -0.04844313834614137, -0.051412470718404574, 0.009440668744214793, 0.40162636186077927, -0.19576901017704554, -0.23158764500955217, -0.04539428969534735, -0.34235648719365136, 0.038090081264575325, 0.1364678324183874, 0.06087737311527... |
706.3485 | In which shell-type SNRs should we look for gamma-rays and neutrinos
from p-p collisions? | We present a simple analytic model for the various contributions to the
non-thermal emission from shell type SNRs, and show that this model's results
reproduce well the results of previous detailed calculations. We show that the
\geq 1 TeV gamma ray emission from the shell type SNRs RX J1713.7-3946 and RX
J0852.0-462... | astro-ph | we present a simple analytic model for the various contributions to the nonthermal emission from shell type snrs and show that this models results reproduce well the results of previous detailed calculations we show that the geq 1 tev gamma ray emission from the shell type snrs rx j171373946 and rx j085204622 is domina... | [['we', 'present', 'a', 'simple', 'analytic', 'model', 'for', 'the', 'various', 'contributions', 'to', 'the', 'nonthermal', 'emission', 'from', 'shell', 'type', 'snrs', 'and', 'show', 'that', 'this', 'models', 'results', 'reproduce', 'well', 'the', 'results', 'of', 'previous', 'detailed', 'calculations', 'we', 'show', ... | [-0.04657097667572964, 0.21098526465559694, -0.02505065882806071, 0.1946776172385159, -0.06484223283911333, -0.10202917066241678, 0.0469391904762575, 0.425715723460106, -0.19027800516827606, -0.316554299195094, 0.002919492167350661, -0.3249547641262188, 0.05349649919758361, 0.2327957837325976, 0.059127326948827316, -0.... |
706.3486 | Peak Quasisymmetric Functions and Eulerian Enumeration | Via duality of Hopf algebras, there is a direct association between peak
quasisymmetric functions and enumeration of chains in Eulerian posets. We study
this association explicitly, showing that the notion of $\cd$-index, long
studied in the context of convex polytopes and Eulerian posets, arises as the
dual basis to... | math.CO | via duality of hopf algebras there is a direct association between peak quasisymmetric functions and enumeration of chains in eulerian posets we study this association explicitly showing that the notion of cdindex long studied in the context of convex polytopes and eulerian posets arises as the dual basis to a natural ... | [['via', 'duality', 'of', 'hopf', 'algebras', 'there', 'is', 'a', 'direct', 'association', 'between', 'peak', 'quasisymmetric', 'functions', 'and', 'enumeration', 'of', 'chains', 'in', 'eulerian', 'posets', 'we', 'study', 'this', 'association', 'explicitly', 'showing', 'that', 'the', 'notion', 'of', 'cdindex', 'long', ... | [-0.1349870097876443, 0.05920721979197058, -0.057381689185049475, 0.1243764282671765, -0.11080219249460634, -0.08904496666680022, 0.0007643670286619808, 0.3901796150740569, -0.38826955212810177, -0.16966187439828626, 0.08502872062873519, -0.23739636943834583, -0.17908664837070717, 0.13845496047742484, -0.09959216907287... |
706.3487 | Wronskian solutions to the KdV equation via B\"acklund transformation | In the paper we discuss the B\"acklund transformation of the KdV equation
between solitons and solitons, between negatons and negatons, between positons
and positons, between rational solution and rational solution, and between
complexitons and complexitons. We investigate the conditions that Wronskian
entries satisf... | nlin.SI | in the paper we discuss the backlund transformation of the kdv equation between solitons and solitons between negatons and negatons between positons and positons between rational solution and rational solution and between complexitons and complexitons we investigate the conditions that wronskian entries satisfy for the... | [['in', 'the', 'paper', 'we', 'discuss', 'the', 'backlund', 'transformation', 'of', 'the', 'kdv', 'equation', 'between', 'solitons', 'and', 'solitons', 'between', 'negatons', 'and', 'negatons', 'between', 'positons', 'and', 'positons', 'between', 'rational', 'solution', 'and', 'rational', 'solution', 'and', 'between', ... | [-0.18334951588552292, 0.025986430617942386, -0.04714382478125291, 0.07310548399205077, -0.11712246852263503, -0.18130018101520326, 0.01055543593685972, 0.3363327875299609, -0.32551394203958445, -0.21468166688023366, 0.07720475145360481, -0.32486693322505444, -0.2400947533649941, 0.14459998903745044, -0.009840541072700... |
706.3488 | Generalised parton distributions at HERA and prospects for COMPASS | We present a model of generalised parton distributions based on a forward
ansatz in the DGLAP region. We discuss some aspects of the parametrisations, as
the dependence in t, with factorised and non-factorised approaches, where t is
the square of the four-momentum exchanged at the hadron vertex. The predictions
of th... | hep-ph | we present a model of generalised parton distributions based on a forward ansatz in the dglap region we discuss some aspects of the parametrisations as the dependence in t with factorised and nonfactorised approaches where t is the square of the fourmomentum exchanged at the hadron vertex the predictions of this model ... | [['we', 'present', 'a', 'model', 'of', 'generalised', 'parton', 'distributions', 'based', 'on', 'a', 'forward', 'ansatz', 'in', 'the', 'dglap', 'region', 'we', 'discuss', 'some', 'aspects', 'of', 'the', 'parametrisations', 'as', 'the', 'dependence', 'in', 't', 'with', 'factorised', 'and', 'nonfactorised', 'approaches',... | [-0.07632440575022971, 0.14394109998763943, -0.12481252898672415, 0.12093753173061075, -0.04328997740522027, -0.08687940314412117, 0.008530676268762158, 0.3596556214435447, -0.2392383692342968, -0.22627685254499796, 0.016166905863510987, -0.31553647027861687, -0.05057827296306289, 0.1542536298443954, 0.0574548879786649... |
706.3489 | Information on mean, fluctuation and synchrony conveyed by a population
of firing neurons | A population of firing neurons is expected to carry not only mean firing rate
but also its fluctuation and synchrony among neurons. In order to examine this
possibility, we have studied responses of neuronal ensembles to three kinds of
inputs: mean-, fluctuation- and synchrony-driven inputs. The generalized
rate-code... | cond-mat.dis-nn | a population of firing neurons is expected to carry not only mean firing rate but also its fluctuation and synchrony among neurons in order to examine this possibility we have studied responses of neuronal ensembles to three kinds of inputs mean fluctuation and synchronydriven inputs the generalized ratecode model incl... | [['a', 'population', 'of', 'firing', 'neurons', 'is', 'expected', 'to', 'carry', 'not', 'only', 'mean', 'firing', 'rate', 'but', 'also', 'its', 'fluctuation', 'and', 'synchrony', 'among', 'neurons', 'in', 'order', 'to', 'examine', 'this', 'possibility', 'we', 'have', 'studied', 'responses', 'of', 'neuronal', 'ensembles... | [-0.0900120173622108, 0.1129689044717864, -0.03221412475390658, 0.06529329888566361, -0.007471381206173471, -0.12637099362549614, 0.06371188698013606, 0.3920401012401472, -0.20852282326359775, -0.3029196965328073, 0.05842610461655387, -0.2819449410140926, -0.22097438770521288, 0.1960085233125465, -0.08366068840433344, ... |
706.349 | Maximal planar scale-free Sierpinski networks with small-world effect
and power-law strength-degree correlation | Many real networks share three generic properties: they are scale-free,
display a small-world effect, and show a power-law strength-degree correlation.
In this paper, we propose a type of deterministically growing networks called
Sierpinski networks, which are induced by the famous Sierpinski fractals and
constructed... | physics.soc-ph | many real networks share three generic properties they are scalefree display a smallworld effect and show a powerlaw strengthdegree correlation in this paper we propose a type of deterministically growing networks called sierpinski networks which are induced by the famous sierpinski fractals and constructed in a simple... | [['many', 'real', 'networks', 'share', 'three', 'generic', 'properties', 'they', 'are', 'scalefree', 'display', 'a', 'smallworld', 'effect', 'and', 'show', 'a', 'powerlaw', 'strengthdegree', 'correlation', 'in', 'this', 'paper', 'we', 'propose', 'a', 'type', 'of', 'deterministically', 'growing', 'networks', 'called', '... | [-0.1538554377908654, 0.0831471464213203, -0.0814058472018908, 0.1238635206964853, -0.05901188597028308, -0.17807469431530026, -0.051306203608948955, 0.44669063700712286, -0.2553432585705784, -0.2687416492358727, 0.043156135402729404, -0.3050416269723107, -0.31675269573050385, 0.17602751410894973, -0.01790386716277092,... |
706.3491 | Exact analytical solution of average path length for Apollonian networks | The exact formula for the average path length of Apollonian networks is
found. With the help of recursion relations derived from the self-similar
structure, we obtain the exact solution of average path length, $\bar{d}_t$,
for Apollonian networks. In contrast to the well-known numerical result
$\bar{d}_t \propto (\ln... | cond-mat.stat-mech physics.soc-ph | the exact formula for the average path length of apollonian networks is found with the help of recursion relations derived from the selfsimilar structure we obtain the exact solution of average path length bard_t for apollonian networks in contrast to the wellknown numerical result bard_t propto ln n_t34 phys rev lett ... | [['the', 'exact', 'formula', 'for', 'the', 'average', 'path', 'length', 'of', 'apollonian', 'networks', 'is', 'found', 'with', 'the', 'help', 'of', 'recursion', 'relations', 'derived', 'from', 'the', 'selfsimilar', 'structure', 'we', 'obtain', 'the', 'exact', 'solution', 'of', 'average', 'path', 'length', 'bard_t', 'fo... | [-0.16230352494822836, 0.07761000724102574, -0.05291666302444606, -0.007602058943821353, -0.04807023766140143, -0.11768235110988219, 0.07991072681100889, 0.3370868205574566, -0.18731939738038286, -0.2723727934490675, -0.0001122226333780878, -0.3545596544984086, -0.22345834632736, 0.18374831916432527, -0.045778457808640... |
706.3492 | Multipole State of Heavy Lanthanide Filled Skutterudites | We discuss multipole properties of filled skutterudites containing heavy
lanthanide Ln from a microscopic viewpoint on the basis of a seven-orbital
Anderson model. For Ln=Gd, in contrast to naive expectation, quadrupole moments
remain in addition to main dipole ones. For Ln=Ho, we find an exotic state
governed by oct... | cond-mat.str-el | we discuss multipole properties of filled skutterudites containing heavy lanthanide ln from a microscopic viewpoint on the basis of a sevenorbital anderson model for lngd in contrast to naive expectation quadrupole moments remain in addition to main dipole ones for lnho we find an exotic state governed by octupole mome... | [['we', 'discuss', 'multipole', 'properties', 'of', 'filled', 'skutterudites', 'containing', 'heavy', 'lanthanide', 'ln', 'from', 'a', 'microscopic', 'viewpoint', 'on', 'the', 'basis', 'of', 'a', 'sevenorbital', 'anderson', 'model', 'for', 'lngd', 'in', 'contrast', 'to', 'naive', 'expectation', 'quadrupole', 'moments',... | [-0.09517022400690489, 0.20911544736026624, 0.05228646203920425, 0.09692065134442535, -0.039591726044709064, -0.10016417108386395, 0.032824622173316734, 0.37952820076999894, -0.1836408643649487, -0.24135894667222557, -0.0404522416815835, -0.36432454654251234, -0.07359497117843614, 0.13419361329772117, 0.062710561565157... |
706.3493 | Gabay-Toulouse Phase Transition in Heisenberg Spin-Glasses in Three
Dimensions | We examine three-dimensional $\pm J$ Heisenberg models with and without
random anisotropies in a magnetic field. We calculate both the stiffness
exponent $\theta_s$ at absolute zero temperature and spin-glass correlation
lengths for the longitudinal and transverse spin components at finite
temperatures. We suggest th... | cond-mat.dis-nn | we examine threedimensional pm j heisenberg models with and without random anisotropies in a magnetic field we calculate both the stiffness exponent theta_s at absolute zero temperature and spinglass correlation lengths for the longitudinal and transverse spin components at finite temperatures we suggest that contrary ... | [['we', 'examine', 'threedimensional', 'pm', 'j', 'heisenberg', 'models', 'with', 'and', 'without', 'random', 'anisotropies', 'in', 'a', 'magnetic', 'field', 'we', 'calculate', 'both', 'the', 'stiffness', 'exponent', 'theta_s', 'at', 'absolute', 'zero', 'temperature', 'and', 'spinglass', 'correlation', 'lengths', 'for'... | [-0.17783971167345708, 0.31099207754674796, -0.059126294520054315, 0.06515262513956357, -0.04096686529590295, -0.15579859098746768, 0.037326440123866336, 0.4164000343330003, -0.19078702210272486, -0.24918183412503553, 0.05508884747443419, -0.3096333416052968, -0.09830088328217736, 0.13218723676431723, 0.057950621256856... |
706.3494 | Two-dimensional phase transition models and \lambda \phi^4 field theory | The overview is given of the results obtained recently in the course of
renormalization-group (RG) study of two-dimensional (2D) models. RG functions
of the two-dimensional n-vector \lambda \phi^4 Euclidean field theory are
written down up to the five-loop terms and perturbative series are resummed by
the Pade-Borel-... | cond-mat.stat-mech hep-lat hep-ph hep-th | the overview is given of the results obtained recently in the course of renormalizationgroup rg study of twodimensional 2d models rg functions of the twodimensional nvector lambda phi4 euclidean field theory are written down up to the fiveloop terms and perturbative series are resummed by the padeborelleroy techniques ... | [['the', 'overview', 'is', 'given', 'of', 'the', 'results', 'obtained', 'recently', 'in', 'the', 'course', 'of', 'renormalizationgroup', 'rg', 'study', 'of', 'twodimensional', '2d', 'models', 'rg', 'functions', 'of', 'the', 'twodimensional', 'nvector', 'lambda', 'phi4', 'euclidean', 'field', 'theory', 'are', 'written',... | [-0.1268315677040852, 0.11901272507156736, -0.07748676675568227, 0.059191484606926185, -0.006530206316296442, -0.09416686330659023, 0.013862964477814531, 0.3086397662532332, -0.20530308955380705, -0.24603154834638646, 0.08451094247834744, -0.3396659114011595, -0.16013329373640928, 0.18335830181247878, 0.036319947592556... |
706.3495 | Gravitational Wave Background from Population III Stars | We estimate the gravitational wave (GW) background from Population III (Pop
III) stars using the results from our hydrodynamic simulations (Suwa et al.
2007). We calculate gravitational waveforms from matter motions and anisotropic
neutrino emissions for single Pop III stars. We find that the GW amplitudes
from matte... | astro-ph | we estimate the gravitational wave gw background from population iii pop iii stars using the results from our hydrodynamic simulations suwa et al 2007 we calculate gravitational waveforms from matter motions and anisotropic neutrino emissions for single pop iii stars we find that the gw amplitudes from matter motions a... | [['we', 'estimate', 'the', 'gravitational', 'wave', 'gw', 'background', 'from', 'population', 'iii', 'pop', 'iii', 'stars', 'using', 'the', 'results', 'from', 'our', 'hydrodynamic', 'simulations', 'suwa', 'et', 'al', '2007', 'we', 'calculate', 'gravitational', 'waveforms', 'from', 'matter', 'motions', 'and', 'anisotrop... | [-0.0760373813374847, 0.17360609483957784, -0.028853345479230196, 0.11162974401455623, -0.07136354277831282, -0.0034926111804677194, 0.0868664872858757, 0.3428635008298279, -0.20388442649390925, -0.338425339950416, 0.06030742676007781, -0.3043796584517643, -0.06504341211134641, 0.2468509357945805, 0.040900534318414714,... |
706.3496 | Revised value of the eighth-order electron g-2 | The contribution to the eighth-order anomalous magnetic moment (g-2) of the
electron from a set of diagrams without closed lepton loops is recalculated
using a new FORTRAN code generated by an automatic code generator. Comparing
the contributions of individual diagrams of old and new calculations, we found
an inconsi... | hep-ph | the contribution to the eighthorder anomalous magnetic moment g2 of the electron from a set of diagrams without closed lepton loops is recalculated using a new fortran code generated by an automatic code generator comparing the contributions of individual diagrams of old and new calculations we found an inconsistency i... | [['the', 'contribution', 'to', 'the', 'eighthorder', 'anomalous', 'magnetic', 'moment', 'g2', 'of', 'the', 'electron', 'from', 'a', 'set', 'of', 'diagrams', 'without', 'closed', 'lepton', 'loops', 'is', 'recalculated', 'using', 'a', 'new', 'fortran', 'code', 'generated', 'by', 'an', 'automatic', 'code', 'generator', 'c... | [-0.11339318991398041, 0.11663937472687312, -0.05205793521534442, 0.11080099883478846, -0.04811725521648533, -0.06373417650590117, 0.09638871551488704, 0.3427393761662285, -0.24593988047347645, -0.3482304417915391, 0.029581047968645947, -0.26726114714591437, -0.06913276382439425, 0.1900168716059893, -0.0421939422114846... |
706.3497 | Shell Structure and $\rho$-Tensor Correlations in Density-Dependent
Relativistic Hartree-Fock theory | A new effective interaction PKA1 with $\rho$-tensor couplings for the
density-dependent relativistic Hartree-Fock (DDRHF) theory is presented. It is
obtained by fitting selected empirical ground state and shell structure
properties. It provides satisfactory descriptions of nuclear matter and the
ground state properti... | nucl-th | a new effective interaction pka1 with rhotensor couplings for the densitydependent relativistic hartreefock ddrhf theory is presented it is obtained by fitting selected empirical ground state and shell structure properties it provides satisfactory descriptions of nuclear matter and the ground state properties of finite... | [['a', 'new', 'effective', 'interaction', 'pka1', 'with', 'rhotensor', 'couplings', 'for', 'the', 'densitydependent', 'relativistic', 'hartreefock', 'ddrhf', 'theory', 'is', 'presented', 'it', 'is', 'obtained', 'by', 'fitting', 'selected', 'empirical', 'ground', 'state', 'and', 'shell', 'structure', 'properties', 'it',... | [-0.09840094559795914, 0.1404458056023765, -0.0795699892835992, 0.1573176191931951, -0.035203768616361965, -0.11535603691553396, 0.032750891713095046, 0.3402176875380739, -0.1974385289693131, -0.3452433384894844, -0.02929936685118704, -0.30060321361787856, -0.06313509101784157, 0.1007023825122404, 0.04718232574467097, ... |
706.3498 | Z_{12-I} Orbifold Compactification toward SUSY Standard Model | We explain the orbifold compactification in string models and present a
Z_{12-I} orbifold compactification toward supersymmetric standard models. We
also point out an effective R-parity from this string construction. The VEVs of
gauge singlets are chosen such that phenomenological constraints are satisfied.
| hep-ph | we explain the orbifold compactification in string models and present a z_12i orbifold compactification toward supersymmetric standard models we also point out an effective rparity from this string construction the vevs of gauge singlets are chosen such that phenomenological constraints are satisfied | [['we', 'explain', 'the', 'orbifold', 'compactification', 'in', 'string', 'models', 'and', 'present', 'a', 'z_12i', 'orbifold', 'compactification', 'toward', 'supersymmetric', 'standard', 'models', 'we', 'also', 'point', 'out', 'an', 'effective', 'rparity', 'from', 'this', 'string', 'construction', 'the', 'vevs', 'of',... | [-0.14837441760824904, 0.16870379575751335, -0.08315448520616406, 0.25345368699691745, -0.12353810446248167, -0.215931996071179, 0.03147724005854494, 0.3342047760351783, -0.18599027741168225, -0.25000472906755195, 0.09089043074830745, -0.23429831942277296, -0.09984891897156126, 0.07795719177063022, -0.11251755059874129... |
706.3499 | Metric Embedding for Nearest Neighbor Classification | The distance metric plays an important role in nearest neighbor (NN)
classification. Usually the Euclidean distance metric is assumed or a
Mahalanobis distance metric is optimized to improve the NN performance. In this
paper, we study the problem of embedding arbitrary metric spaces into a
Euclidean space with the go... | stat.ML | the distance metric plays an important role in nearest neighbor nn classification usually the euclidean distance metric is assumed or a mahalanobis distance metric is optimized to improve the nn performance in this paper we study the problem of embedding arbitrary metric spaces into a euclidean space with the goal to i... | [['the', 'distance', 'metric', 'plays', 'an', 'important', 'role', 'in', 'nearest', 'neighbor', 'nn', 'classification', 'usually', 'the', 'euclidean', 'distance', 'metric', 'is', 'assumed', 'or', 'a', 'mahalanobis', 'distance', 'metric', 'is', 'optimized', 'to', 'improve', 'the', 'nn', 'performance', 'in', 'this', 'pap... | [-0.06990127448203429, -0.03742782327726501, -0.10303985587696093, 0.1248026844714446, -0.08462283623539521, -0.15699475940680072, 0.03341257049549816, 0.40617268392523315, -0.26997948846773906, -0.2741110721345311, 0.06363831350576929, -0.28551780976027064, -0.21919907047706158, 0.16095106232286807, -0.102489668890576... |
706.35 | Spin glasses and Stein's method | We introduce some applications of Stein's method in the high temperature
analysis of spin glasses. Stein's method allows the direct analysis of the
Gibbs measure without having to create a cavity. Another advantage is that it
gives limit theorems with total variation error bounds, although the bounds can
be suboptima... | math.PR math-ph math.MP | we introduce some applications of steins method in the high temperature analysis of spin glasses steins method allows the direct analysis of the gibbs measure without having to create a cavity another advantage is that it gives limit theorems with total variation error bounds although the bounds can be suboptimal a sur... | [['we', 'introduce', 'some', 'applications', 'of', 'steins', 'method', 'in', 'the', 'high', 'temperature', 'analysis', 'of', 'spin', 'glasses', 'steins', 'method', 'allows', 'the', 'direct', 'analysis', 'of', 'the', 'gibbs', 'measure', 'without', 'having', 'to', 'create', 'a', 'cavity', 'another', 'advantage', 'is', 't... | [-0.09578918818151579, 0.08106154353590682, -0.2156175401993096, 0.08361675349588041, -0.07865808146307245, -0.13195419156108984, 0.10932569911383325, 0.35732732177712023, -0.21628690329380335, -0.30395654765889046, 0.09264855885849102, -0.25115918686224176, -0.14588718045270072, 0.2382077001966536, -0.0986201474734116... |
706.3501 | The Incidence of Highly-Obscured Star-Forming Regions in SINGS Galaxies | Using the new capabilities of the Spitzer Space Telescope and extensive
multiwavelength data from the Spitzer Infrared Nearby Galaxies Survey (SINGS),
it is now possible to study the infrared properties of star formation in nearby
galaxies down to scales equivalent to large HII regions. We are therefore able
to deter... | astro-ph | using the new capabilities of the spitzer space telescope and extensive multiwavelength data from the spitzer infrared nearby galaxies survey sings it is now possible to study the infrared properties of star formation in nearby galaxies down to scales equivalent to large hii regions we are therefore able to determine w... | [['using', 'the', 'new', 'capabilities', 'of', 'the', 'spitzer', 'space', 'telescope', 'and', 'extensive', 'multiwavelength', 'data', 'from', 'the', 'spitzer', 'infrared', 'nearby', 'galaxies', 'survey', 'sings', 'it', 'is', 'now', 'possible', 'to', 'study', 'the', 'infrared', 'properties', 'of', 'star', 'formation', '... | [-0.06462788599764852, 0.10149989165469561, -0.06215940859189541, 0.11175765906725439, -0.06646759662133223, -0.010362686556469663, 0.0793665959577675, 0.46066529404884377, -0.11977376034968017, -0.3341549595101255, 0.06403047288681439, -0.29518929690635004, -0.03434314584570719, 0.19941426461413642, -0.048152459881525... |
706.3502 | Approximately-Universal Space-Time Codes for the Parallel, Multi-Block
and Cooperative-Dynamic-Decode-and-Forward Channels | Explicit codes are constructed that achieve the diversity-multiplexing gain
tradeoff of the cooperative-relay channel under the dynamic decode-and-forward
protocol for any network size and for all numbers of transmit and receive
antennas at the relays.
A particularly simple code construction that makes use of the A... | cs.IT cs.DM cs.NI math.IT | explicit codes are constructed that achieve the diversitymultiplexing gain tradeoff of the cooperativerelay channel under the dynamic decodeandforward protocol for any network size and for all numbers of transmit and receive antennas at the relays a particularly simple code construction that makes use of the alamouti c... | [['explicit', 'codes', 'are', 'constructed', 'that', 'achieve', 'the', 'diversitymultiplexing', 'gain', 'tradeoff', 'of', 'the', 'cooperativerelay', 'channel', 'under', 'the', 'dynamic', 'decodeandforward', 'protocol', 'for', 'any', 'network', 'size', 'and', 'for', 'all', 'numbers', 'of', 'transmit', 'and', 'receive', ... | [-0.22950105036452942, 0.04162108653583863, -0.04289391293903864, 0.058569979369042256, -0.025642592645754372, -0.30868978939369457, 0.06852982993506818, 0.3971867188811302, -0.2704046815462889, -0.234249896668923, 0.09199814785831531, -0.20683647028315777, -0.16927076788157772, 0.20018608463124946, -0.0765754642347386... |
706.3503 | Largely deformed states of $^{13}$B | The excited states of $^{13}$B were studied with a method of antisymmetrized
molecular dynamics(AMD). The theoretical results suggest that the intruder
states with large deformations construct the rotational bands, $K^\pi=3/2^-$
and $K^\pi=1/2^+$, starting from 5 MeV and 8 MeV, respectively. The neutron
structure of ... | nucl-th | the excited states of 13b were studied with a method of antisymmetrized molecular dynamicsamd the theoretical results suggest that the intruder states with large deformations construct the rotational bands kpi32 and kpi12 starting from 5 mev and 8 mev respectively the neutron structure of the kpi32 is analogous to the ... | [['the', 'excited', 'states', 'of', '13b', 'were', 'studied', 'with', 'a', 'method', 'of', 'antisymmetrized', 'molecular', 'dynamicsamd', 'the', 'theoretical', 'results', 'suggest', 'that', 'the', 'intruder', 'states', 'with', 'large', 'deformations', 'construct', 'the', 'rotational', 'bands', 'kpi32', 'and', 'kpi12', ... | [-0.07982284339723757, 0.21407605795009346, -0.09403844016209782, 0.09309543583328156, 0.0038754570254372215, -0.09899933857744694, 0.07950046370099592, 0.35222530465673757, -0.20122046067656293, -0.32475442303394947, 0.013962821214803838, -0.2887249442975263, -0.012249313844451765, 0.09488279570464615, 0.0756377045081... |
706.3504 | Axiomatic Foundations for the Principle of Entropy Increase | We show that the principle of entropy increase may be exactly founded on a
few axioms valid not only for quantum and classical statistics, but also for a
wide range of statistical processes.
| physics.class-ph | we show that the principle of entropy increase may be exactly founded on a few axioms valid not only for quantum and classical statistics but also for a wide range of statistical processes | [['we', 'show', 'that', 'the', 'principle', 'of', 'entropy', 'increase', 'may', 'be', 'exactly', 'founded', 'on', 'a', 'few', 'axioms', 'valid', 'not', 'only', 'for', 'quantum', 'and', 'classical', 'statistics', 'but', 'also', 'for', 'a', 'wide', 'range', 'of', 'statistical', 'processes']] | [-0.044457795514696925, 0.1629773753441193, -0.11338991276694066, 0.13922971611221632, -0.07079654728824442, -0.15961495880037546, 0.10255842652369404, 0.3082487847317349, -0.29698467954541696, -0.3000747990992033, 0.10026952825049221, -0.21093931272061486, -0.10108770616352558, 0.331083738781286, -0.080126410491313, 0... |
706.3505 | A symmetric Finsler space with Chern connection | We define a symmetry for a Finsler space with Chern connection and
investigate its implementation and properties and find a relation between them
and flag curvature.
| math.DG | we define a symmetry for a finsler space with chern connection and investigate its implementation and properties and find a relation between them and flag curvature | [['we', 'define', 'a', 'symmetry', 'for', 'a', 'finsler', 'space', 'with', 'chern', 'connection', 'and', 'investigate', 'its', 'implementation', 'and', 'properties', 'and', 'find', 'a', 'relation', 'between', 'them', 'and', 'flag', 'curvature']] | [-0.21638523318016759, 0.06003775315072674, -0.08337190023695047, 0.10862110501441818, -0.17039439777055612, -0.16028083291334602, 0.047245263623503536, 0.4226311777646725, -0.27784753769922715, -0.29665231310690826, 0.09659879387786183, -0.24458377826242492, -0.26392063011343664, 0.107584009376856, -0.0219212752193785... |
706.3506 | Experimental Estimates of Dephasing Time in Molecular Magnets | Muon spin relaxation measurements in isotropic molecular magnets (MM) with a
spin value S ranging from 7/2 to 27/2 are used to determine the magnitude and
origin of dephasing time $\tau_\phi$ of molecular magnets. It is found that
$\tau_\phi$ ~ 10 nsec with no S or ligand dependence. This indicates a nuclear
origin f... | cond-mat.str-el | muon spin relaxation measurements in isotropic molecular magnets mm with a spin value s ranging from 72 to 272 are used to determine the magnitude and origin of dephasing time tau_phi of molecular magnets it is found that tau_phi 10 nsec with no s or ligand dependence this indicates a nuclear origin for the stochastic ... | [['muon', 'spin', 'relaxation', 'measurements', 'in', 'isotropic', 'molecular', 'magnets', 'mm', 'with', 'a', 'spin', 'value', 's', 'ranging', 'from', '72', 'to', '272', 'are', 'used', 'to', 'determine', 'the', 'magnitude', 'and', 'origin', 'of', 'dephasing', 'time', 'tau_phi', 'of', 'molecular', 'magnets', 'it', 'is',... | [-0.1122291122862537, 0.21383326582144946, -0.015353774660200412, 0.05897123003316145, -0.005007324553194589, -0.15288055880228058, 0.03617909947206499, 0.37233440453668926, -0.24260852121681506, -0.29522395925596356, 0.06442670019168872, -0.2746103515299702, -0.07276846234058862, 0.22267889993547993, 0.035535788167700... |
706.3507 | Interference in Bohmian Mechanics with Complex Action | In recent years, intensive effort has gone into developing numerical tools
for exact quantum mechanical calculations that are based on Bohmian mechanics.
As part of this effort we have recently developed as alternative formulation of
Bohmian mechanics in which the quantum action, S, is taken to be complex [JCP
{125},... | quant-ph | in recent years intensive effort has gone into developing numerical tools for exact quantum mechanical calculations that are based on bohmian mechanics as part of this effort we have recently developed as alternative formulation of bohmian mechanics in which the quantum action s is taken to be complex jcp 125 231103 20... | [['in', 'recent', 'years', 'intensive', 'effort', 'has', 'gone', 'into', 'developing', 'numerical', 'tools', 'for', 'exact', 'quantum', 'mechanical', 'calculations', 'that', 'are', 'based', 'on', 'bohmian', 'mechanics', 'as', 'part', 'of', 'this', 'effort', 'we', 'have', 'recently', 'developed', 'as', 'alternative', 'f... | [-0.10080599569455401, 0.08326337956163449, -0.1483417203160169, 0.05826645597767417, -0.07617007976752037, -0.14395479115705606, 0.0074204101392282215, 0.34852379500404645, -0.25559615392397494, -0.29644322930288636, 0.012894320679924718, -0.26758492292897523, -0.18277982789301642, 0.20452545921235157, -0.115200649000... |
706.3508 | Unified derivation of Bohmian methods and the incorporation of
interference effects | We present a unified derivation of Bohmian methods that serves as a common
starting point for the derivative propagation method (DPM), Bohmian mechanics
with complex action (BOMCA) and the zero-velocity complex action method
(ZEVCA). The unified derivation begins with the ansatz
$\psi=e^{\frac{iS}{\hbar}}$ where the ... | quant-ph | we present a unified derivation of bohmian methods that serves as a common starting point for the derivative propagation method dpm bohmian mechanics with complex action bomca and the zerovelocity complex action method zevca the unified derivation begins with the ansatz psiefracishbar where the action s is taken to be ... | [['we', 'present', 'a', 'unified', 'derivation', 'of', 'bohmian', 'methods', 'that', 'serves', 'as', 'a', 'common', 'starting', 'point', 'for', 'the', 'derivative', 'propagation', 'method', 'dpm', 'bohmian', 'mechanics', 'with', 'complex', 'action', 'bomca', 'and', 'the', 'zerovelocity', 'complex', 'action', 'method', ... | [-0.10457893801235989, 0.07119568891143369, -0.1420525500309465, 0.05352113029435334, -0.09087355893699486, -0.13158867900699742, 0.003249937698439312, 0.32104154473722, -0.26173865224914683, -0.26577372463031507, 0.018367586641692402, -0.2523947374015315, -0.1778902594754301, 0.18773706095361728, -0.03824503456265237,... |
706.3509 | Two-component model for the axial form factor of the nucleon | The axial form factor of the nucleon is studied in a two-component model
consisting of a three-quark intrinsic structure surrounded by a meson cloud.
The experimental data in the space-like region are well reproduced with a
minimal number of parameters. The results are similar to those obtained from a
dipole fit up t... | nucl-th | the axial form factor of the nucleon is studied in a twocomponent model consisting of a threequark intrinsic structure surrounded by a meson cloud the experimental data in the spacelike region are well reproduced with a minimal number of parameters the results are similar to those obtained from a dipole fit up to 1 gev... | [['the', 'axial', 'form', 'factor', 'of', 'the', 'nucleon', 'is', 'studied', 'in', 'a', 'twocomponent', 'model', 'consisting', 'of', 'a', 'threequark', 'intrinsic', 'structure', 'surrounded', 'by', 'a', 'meson', 'cloud', 'the', 'experimental', 'data', 'in', 'the', 'spacelike', 'region', 'are', 'well', 'reproduced', 'wi... | [-0.09403202459257695, 0.13641164921240748, -0.06498152072474893, 0.0985081353667608, -0.02891830794188926, -0.11639662115235946, 0.04221806194150953, 0.3597054476725004, -0.19398371002171189, -0.29819754661210546, 0.020527823201388986, -0.28472515628319733, -0.07967178770091518, 0.17586634089821018, 0.0441176043046393... |
706.351 | Realistic solution to the tunneling time problem | There remains the old question of how long a quantum particle takes to tunnel
through a potential barrier higher than its incident kinetic energy. In this
article a solution of the question is proposed on the basis of a realistic
explanation of quantum mechanics. The explanation implies that the tunneling
particle ha... | quant-ph | there remains the old question of how long a quantum particle takes to tunnel through a potential barrier higher than its incident kinetic energy in this article a solution of the question is proposed on the basis of a realistic explanation of quantum mechanics the explanation implies that the tunneling particle has a ... | [['there', 'remains', 'the', 'old', 'question', 'of', 'how', 'long', 'a', 'quantum', 'particle', 'takes', 'to', 'tunnel', 'through', 'a', 'potential', 'barrier', 'higher', 'than', 'its', 'incident', 'kinetic', 'energy', 'in', 'this', 'article', 'a', 'solution', 'of', 'the', 'question', 'is', 'proposed', 'on', 'the', 'b... | [-0.16403702230891212, 0.15722219265462628, -0.12442496400180972, 0.1324317418792475, -0.05376587444043253, -0.16559109960799107, 0.06959627351666313, 0.34169186552171593, -0.2449606493479223, -0.3207396197598428, -0.007433925998338964, -0.27018595812332935, -0.10304961149813607, 0.20805775365806767, -0.034029083664063... |
706.3511 | On elliptic differential operators with shifts | We give an index formula for elliptic differential operators whose
coefficients include shifts forming an infinite group.
| math.OA math.AP math.KT | we give an index formula for elliptic differential operators whose coefficients include shifts forming an infinite group | [['we', 'give', 'an', 'index', 'formula', 'for', 'elliptic', 'differential', 'operators', 'whose', 'coefficients', 'include', 'shifts', 'forming', 'an', 'infinite', 'group']] | [-0.2117159629569334, 0.15528778481358826, -0.14687738479936824, 0.049505839014754575, -0.14381295159075627, -0.13528669022900217, -0.06842303053503308, 0.3441312488387613, -0.30394591829356027, -0.22208260109319405, 0.11858781418927453, -0.35121400720056367, -0.11338490872260402, 0.2554553735672551, -0.094078628565458... |
706.3512 | Homogeneous geodesics in homogeneous Finsler spaces | In this paper, we study homogeneous geodesics in homogeneous Finsler spaces.
We first give a simple criterion that characterizes geodesic vectors. We show
that the geodesics on a Lie group, relative to a bi-invariant Finsler metric,
are the cosets of the one-parameter subgroups. The existence of infinitely many
homog... | math.DG | in this paper we study homogeneous geodesics in homogeneous finsler spaces we first give a simple criterion that characterizes geodesic vectors we show that the geodesics on a lie group relative to a biinvariant finsler metric are the cosets of the oneparameter subgroups the existence of infinitely many homogeneous geo... | [['in', 'this', 'paper', 'we', 'study', 'homogeneous', 'geodesics', 'in', 'homogeneous', 'finsler', 'spaces', 'we', 'first', 'give', 'a', 'simple', 'criterion', 'that', 'characterizes', 'geodesic', 'vectors', 'we', 'show', 'that', 'the', 'geodesics', 'on', 'a', 'lie', 'group', 'relative', 'to', 'a', 'biinvariant', 'fin... | [-0.2807632544543594, 0.10785528275417164, -0.09850891354959458, 0.11217046113917604, -0.19844391129910946, -0.07271040702762548, -0.055920996208442375, 0.437794585574884, -0.2822251669690013, -0.09631015427410602, 0.0675286995852366, -0.2617034027655609, -0.20211221002973617, 0.19824939854443074, -0.12917134718270973,... |
706.3513 | Nonlinear elastic stress response in granular packings | We study the nonlinear elastic response of a two-dimensional material to a
localized boundary force, with the particular goal of understanding the
differences observed between isotropic granular materials and those with
hexagonal anisotropy. Corrections to the classical Boussinesq result for the
stresses in an infini... | cond-mat.soft | we study the nonlinear elastic response of a twodimensional material to a localized boundary force with the particular goal of understanding the differences observed between isotropic granular materials and those with hexagonal anisotropy corrections to the classical boussinesq result for the stresses in an infinite ha... | [['we', 'study', 'the', 'nonlinear', 'elastic', 'response', 'of', 'a', 'twodimensional', 'material', 'to', 'a', 'localized', 'boundary', 'force', 'with', 'the', 'particular', 'goal', 'of', 'understanding', 'the', 'differences', 'observed', 'between', 'isotropic', 'granular', 'materials', 'and', 'those', 'with', 'hexago... | [-0.12784028970487812, 0.16333879609513308, -0.04657845675915559, -0.005491271912878221, -0.06066695713200309, -0.05733816662897415, -0.0018300023654406455, 0.38293069617902026, -0.29772002483034465, -0.2795628039958946, 0.04120370829502675, -0.2923610937246617, -0.14785253603080722, 0.1865815044457509, 0.0357911968795... |
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