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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709.2735 | Localization and delocalization in the quantum kicked prime number
rotator | The quantum kicked prime number rotator (QKPR) is defined as the rotator
whose energy levels are prime numbers. The long time behavior is decided by the
kick period $\tau$ and kick strength $k$. When $\frac{\tau}{2\pi}$ is
irrational, QKPR is localized because of the equidistribution theorem. When
$\frac{\tau}{2\pi}$... | nlin.CD | the quantum kicked prime number rotator qkpr is defined as the rotator whose energy levels are prime numbers the long time behavior is decided by the kick period tau and kick strength k when fractau2pi is irrational qkpr is localized because of the equidistribution theorem when fractau2pi is rational qkpr is localized ... | [['the', 'quantum', 'kicked', 'prime', 'number', 'rotator', 'qkpr', 'is', 'defined', 'as', 'the', 'rotator', 'whose', 'energy', 'levels', 'are', 'prime', 'numbers', 'the', 'long', 'time', 'behavior', 'is', 'decided', 'by', 'the', 'kick', 'period', 'tau', 'and', 'kick', 'strength', 'k', 'when', 'fractau2pi', 'is', 'irra... | [-0.25883714695771537, 0.2515295340741674, -0.05695889305944244, 0.09680297511008878, -0.0619647891074419, -0.2516821317312618, 0.014283437243041893, 0.2985417201121648, -0.2709346345315377, -0.25098051376330355, 0.04863243194296956, -0.24538580647359293, -0.07626003991191586, 0.21470123514222603, -0.044236161125202976... |
709.2736 | Comment on "Macroscopic violation of special relativity" by Nimtz and
Stahlhofen [arXiv:0708.0681v1] | A recent paper by G. Nimtz and A. A. Stahlhofen [arXiv:0708.0681v1] makes the
following claims: (1) that the authors have observed a macroscopic violation of
special relativity, (2) that they have demonstrated quantum mechanical behavior
of evanescent modes on a meter-length scale, and (3) that barriers are crossed
i... | quant-ph physics.optics | a recent paper by g nimtz and a a stahlhofen arxiv07080681v1 makes the following claims 1 that the authors have observed a macroscopic violation of special relativity 2 that they have demonstrated quantum mechanical behavior of evanescent modes on a meterlength scale and 3 that barriers are crossed in zero time implyin... | [['a', 'recent', 'paper', 'by', 'g', 'nimtz', 'and', 'a', 'a', 'stahlhofen', 'arxiv07080681v1', 'makes', 'the', 'following', 'claims', '1', 'that', 'the', 'authors', 'have', 'observed', 'a', 'macroscopic', 'violation', 'of', 'special', 'relativity', '2', 'that', 'they', 'have', 'demonstrated', 'quantum', 'mechanical', ... | [-0.15050606461946012, 0.19336432976386986, -0.11950158469787822, 0.05689032709725746, -0.09406568742607062, -0.16875630855367224, 0.038611253726075365, 0.34122755150765, -0.18615061609733213, -0.2909395851694593, 0.08929430900096166, -0.28556860079591323, -0.1676464250038673, 0.22723811689945983, -0.058695141975654334... |
709.2737 | The NuMI Beam at FNAL and its use for Cross Section Measurements | The Neutrinos at the Main Injector (NuMI) facility at Fermilab began
operations in late 2004. NuMI will deliver an intense muon neutrino beam of
variable energy (2-20 GeV). Several aspects of the design and results from runs
of the MINOS experiment are reviewed. I also discuss technique to measure
directly the neutri... | hep-ex | the neutrinos at the main injector numi facility at fermilab began operations in late 2004 numi will deliver an intense muon neutrino beam of variable energy 220 gev several aspects of the design and results from runs of the minos experiment are reviewed i also discuss technique to measure directly the neutrino flux us... | [['the', 'neutrinos', 'at', 'the', 'main', 'injector', 'numi', 'facility', 'at', 'fermilab', 'began', 'operations', 'in', 'late', '2004', 'numi', 'will', 'deliver', 'an', 'intense', 'muon', 'neutrino', 'beam', 'of', 'variable', 'energy', '220', 'gev', 'several', 'aspects', 'of', 'the', 'design', 'and', 'results', 'from... | [-0.04451465219115982, 0.24379977738829509, -0.06281217912641855, 0.13900132634891912, -0.02474102280460871, -0.14089471785924756, 0.014333493090592897, 0.3811416192123523, -0.16933379095907394, -0.34149149280901137, 0.061820795363746586, -0.37715131224921117, 0.0742824029463988, 0.2513675907626748, 0.01296649688424972... |
709.2738 | Impacts of real-time data collection on introductory algebra-based
physics | Including real-time data collection technology is a common practice to
upgrade physics labs, and the assumption is such technology improves student
learning, yet little has been done to demonstrate the effects of technology.
Specific activities have been shown to be enhanced by technology, but the
effects on the clas... | physics.ed-ph | including realtime data collection technology is a common practice to upgrade physics labs and the assumption is such technology improves student learning yet little has been done to demonstrate the effects of technology specific activities have been shown to be enhanced by technology but the effects on the class as a ... | [['including', 'realtime', 'data', 'collection', 'technology', 'is', 'a', 'common', 'practice', 'to', 'upgrade', 'physics', 'labs', 'and', 'the', 'assumption', 'is', 'such', 'technology', 'improves', 'student', 'learning', 'yet', 'little', 'has', 'been', 'done', 'to', 'demonstrate', 'the', 'effects', 'of', 'technology'... | [-0.03541928007422636, 0.06383052249051009, -0.05798952275809521, 0.05575380077352747, -0.12392995100468397, -0.1345031669177115, -0.011274119929876179, 0.4155113501350085, -0.24406149925276016, -0.3665431014200052, 0.11012649118434638, -0.2783643124314646, -0.1527705822388331, 0.24549786186466616, -0.12403701166001459... |
709.2739 | Formation Scenario for Wide and Close Binary Systems | Fragmentation and binary formation processes are studied using
three-dimensional resistive MHD nested grid simulations. Starting with a
Bonnor-Ebert isothermal cloud rotating in a uniform magnetic field, we
calculate the cloud evolution from the molecular cloud core (n=10^4 cm^-3) to
the stellar core (n \simeq 10^22 ... | astro-ph | fragmentation and binary formation processes are studied using threedimensional resistive mhd nested grid simulations starting with a bonnorebert isothermal cloud rotating in a uniform magnetic field we calculate the cloud evolution from the molecular cloud core n104 cm3 to the stellar core n simeq 1022 cm3 we calculat... | [['fragmentation', 'and', 'binary', 'formation', 'processes', 'are', 'studied', 'using', 'threedimensional', 'resistive', 'mhd', 'nested', 'grid', 'simulations', 'starting', 'with', 'a', 'bonnorebert', 'isothermal', 'cloud', 'rotating', 'in', 'a', 'uniform', 'magnetic', 'field', 'we', 'calculate', 'the', 'cloud', 'evol... | [-0.1733157070720579, 0.24885194052449877, -0.049746222059267216, 0.08223708274733531, 0.02756469670290078, -0.031470879250181265, 0.007321707031445245, 0.3900653388308708, -0.19768242434573718, -0.3694971571348877, 0.02716699895181626, -0.22160601299681024, 0.018054810708509086, 0.1361044087934577, 0.03883399484686185... |
709.274 | Transverse Observables and Mass Determination at Hadron Colliders | I consider the two-body decay of a particle at a hadron collider into a
visible and an invisible particle, generalizing $W \to e \nu$, where the masses
of the decaying particle and the invisible decay particle are, {\em a priori},
unknown. I prove that the transverse mass, when maximized over possible
kinematic confi... | hep-ph hep-ex physics.data-an | i consider the twobody decay of a particle at a hadron collider into a visible and an invisible particle generalizing w to e nu where the masses of the decaying particle and the invisible decay particle are em a priori unknown i prove that the transverse mass when maximized over possible kinematic configurations can be... | [['i', 'consider', 'the', 'twobody', 'decay', 'of', 'a', 'particle', 'at', 'a', 'hadron', 'collider', 'into', 'a', 'visible', 'and', 'an', 'invisible', 'particle', 'generalizing', 'w', 'to', 'e', 'nu', 'where', 'the', 'masses', 'of', 'the', 'decaying', 'particle', 'and', 'the', 'invisible', 'decay', 'particle', 'are', ... | [-0.05030438906202714, 0.2982576753182608, -0.08280527329641497, 0.15520832588275274, -0.07140349538272453, -0.21565563616653283, -0.012393497793366098, 0.2782540002449726, -0.26711435264700817, -0.2618290828747882, 0.0354740407369617, -0.2776402200986114, 0.04868784862466984, 0.14664592739298113, 0.06411700334089497, ... |
709.2741 | Vacuum and semiclassical gravity: a difficulty and its bewildering
significance | We review a long-standing difficulty in some semiclassical models of vacuum
and vacuum decay. Surprisingly enough these models, careless of their
transparent formulation, are affected by, both, technical and conceptual
issues. After proving some general results that are relevant for, both, the
Euclidean and Lorentzia... | gr-qc hep-th | we review a longstanding difficulty in some semiclassical models of vacuum and vacuum decay surprisingly enough these models careless of their transparent formulation are affected by both technical and conceptual issues after proving some general results that are relevant for both the euclidean and lorentzian sectors o... | [['we', 'review', 'a', 'longstanding', 'difficulty', 'in', 'some', 'semiclassical', 'models', 'of', 'vacuum', 'and', 'vacuum', 'decay', 'surprisingly', 'enough', 'these', 'models', 'careless', 'of', 'their', 'transparent', 'formulation', 'are', 'affected', 'by', 'both', 'technical', 'and', 'conceptual', 'issues', 'afte... | [-0.0937027319183422, 0.1523602003848331, -0.0873018472228904, 0.1496605183929205, -0.08179090262667553, -0.1740220491711453, 0.03485150157939643, 0.38983795335012916, -0.2242953669833573, -0.2899221357813961, 0.16088299572977513, -0.2491324302941762, -0.2050448736817752, 0.20193965717948772, -0.10880552602277414, 0.06... |
709.2742 | Threshold scans in diffractive W pair production via QED processes at
the LHC | We propose a new set of measurements which can be performed at the LHC using
roman pot detectors. This new method is based on exploiting excitation curves
to measure kinematical properties of produced particles. We illustrate it in
the case of central diffractive W pair production.
| hep-ph | we propose a new set of measurements which can be performed at the lhc using roman pot detectors this new method is based on exploiting excitation curves to measure kinematical properties of produced particles we illustrate it in the case of central diffractive w pair production | [['we', 'propose', 'a', 'new', 'set', 'of', 'measurements', 'which', 'can', 'be', 'performed', 'at', 'the', 'lhc', 'using', 'roman', 'pot', 'detectors', 'this', 'new', 'method', 'is', 'based', 'on', 'exploiting', 'excitation', 'curves', 'to', 'measure', 'kinematical', 'properties', 'of', 'produced', 'particles', 'we', ... | [-0.055460697115884854, 0.14293891027488786, -0.17866247899465912, 0.05395343185038022, -0.05630037549417466, -0.09235645525420652, 0.029037811307479507, 0.3754375867707574, -0.24711759119173107, -0.2916276515663966, 0.01410831188853911, -0.3115859114281509, -0.03773898355986761, 0.22878351339908398, -0.000102923028980... |
709.2743 | Instability of agegraphic dark energy models | We investigate the agegraphic dark energy models which were recently proposed
to explain the dark energy-dominated universe. For this purpose, we calculate
their equation of states and squared speeds of sound. We find that the squared
speed for agegraphic dark energy is always negative. This means that the
perfect fl... | gr-qc | we investigate the agegraphic dark energy models which were recently proposed to explain the dark energydominated universe for this purpose we calculate their equation of states and squared speeds of sound we find that the squared speed for agegraphic dark energy is always negative this means that the perfect fluid for... | [['we', 'investigate', 'the', 'agegraphic', 'dark', 'energy', 'models', 'which', 'were', 'recently', 'proposed', 'to', 'explain', 'the', 'dark', 'energydominated', 'universe', 'for', 'this', 'purpose', 'we', 'calculate', 'their', 'equation', 'of', 'states', 'and', 'squared', 'speeds', 'of', 'sound', 'we', 'find', 'that... | [-0.1179826755974388, 0.18484226955244173, -0.18459474171440188, 0.19931680807897534, -0.10897009402441864, -0.16462169809696767, -0.07143895807317817, 0.31104071523564364, -0.22869833579931695, -0.3781039880731931, -0.012868681164064373, -0.24725632462650537, -0.04989688023208426, 0.13650885630721368, 0.02209182651713... |
709.2744 | Efficient generation of an isolated single-cycle attosecond pulse | A new method for efficiently generating an isolated single-cycle attosecond
pulse is proposed. It is shown that the ultraviolet (UV) attosecond pulse can
be utilized as a robust tool to control the dynamics of electron wave packets
(EWPs). By adding a UV attosecond pulse to an infrared (IR) few-cycle pulse at
a prope... | physics.atom-ph physics.optics | a new method for efficiently generating an isolated singlecycle attosecond pulse is proposed it is shown that the ultraviolet uv attosecond pulse can be utilized as a robust tool to control the dynamics of electron wave packets ewps by adding a uv attosecond pulse to an infrared ir fewcycle pulse at a proper time only ... | [['a', 'new', 'method', 'for', 'efficiently', 'generating', 'an', 'isolated', 'singlecycle', 'attosecond', 'pulse', 'is', 'proposed', 'it', 'is', 'shown', 'that', 'the', 'ultraviolet', 'uv', 'attosecond', 'pulse', 'can', 'be', 'utilized', 'as', 'a', 'robust', 'tool', 'to', 'control', 'the', 'dynamics', 'of', 'electron'... | [-0.060386204093447304, 0.17094988889621163, -0.11349674851808231, 0.05906503241203609, -0.02987254541949369, -0.12411982278863434, 0.043061710076290186, 0.5224531474057585, -0.25106247833828094, -0.3325582646415569, 0.02193898706100299, -0.2638705911755096, -0.06657776904758066, 0.26471704640352983, -0.050016624422278... |
709.2745 | Thermodynamical properties of dark energy with the equation of state $%
\omega =\omega_{0}+\omega_{1}z$ | The thermodynamical properties of dark energy are usually investigated with
the equation of state $\omega =\omega_{0}+\omega_{1}z$. Recent observations
show that our universe is accelerating, and the apparent horizon and the event
horizon vary with redshift $z$. When definitions of the temperature and entropy
of a bl... | astro-ph | the thermodynamical properties of dark energy are usually investigated with the equation of state omega omega_0omega_1z recent observations show that our universe is accelerating and the apparent horizon and the event horizon vary with redshift z when definitions of the temperature and entropy of a black hole are used ... | [['the', 'thermodynamical', 'properties', 'of', 'dark', 'energy', 'are', 'usually', 'investigated', 'with', 'the', 'equation', 'of', 'state', 'omega', 'omega_0omega_1z', 'recent', 'observations', 'show', 'that', 'our', 'universe', 'is', 'accelerating', 'and', 'the', 'apparent', 'horizon', 'and', 'the', 'event', 'horizo... | [-0.1368995197540657, 0.13084703552621332, -0.13771884213201702, 0.13897506478701183, -0.0902790356723761, -0.07469709750236661, -0.009274978716293293, 0.33934377358915907, -0.20536345834702704, -0.29868757578008104, 0.1677602675768095, -0.3339278813677304, 0.007711608442618992, 0.16586651859688573, -0.0270996339703825... |
709.2746 | Low energy H+CO scattering revisited: CO rotational excitation with new
potential surfaces | A recent modeling study of brightness ratios for CO rotational transitions in
gas typical of the diffuse ISM by Liszt found the role of H collisions to be
more important than previously assumed. This conclusion was based on quantum
scattering calculations using the so-called WKS potential energy surface (PES)
which r... | astro-ph | a recent modeling study of brightness ratios for co rotational transitions in gas typical of the diffuse ism by liszt found the role of h collisions to be more important than previously assumed this conclusion was based on quantum scattering calculations using the socalled wks potential energy surface pes which reporte... | [['a', 'recent', 'modeling', 'study', 'of', 'brightness', 'ratios', 'for', 'co', 'rotational', 'transitions', 'in', 'gas', 'typical', 'of', 'the', 'diffuse', 'ism', 'by', 'liszt', 'found', 'the', 'role', 'of', 'h', 'collisions', 'to', 'be', 'more', 'important', 'than', 'previously', 'assumed', 'this', 'conclusion', 'wa... | [-0.06251375145568032, 0.12524709588427457, -0.02545539957160751, 0.09320560969870477, 0.042189924522072715, -0.11885967186742252, 0.0501170516813985, 0.3739271234740974, -0.1796838144736705, -0.3209628776374263, -0.018456784723531856, -0.2936490110311938, -0.047833917767650655, 0.16274000592629917, 0.07236240052127389... |
709.2747 | Spin squeezing and maximal-squeezing time | Spin squeezing of a nonlinear interaction model with Josephson-like coupling
is studied to obtain time scale of maximal squeezing. Based upon two exactly
solvable cases for two and three particles, we find that the maximal-squeezing
time depends on the level spacing between the ground state and its next
neighbor eige... | quant-ph cond-mat.other | spin squeezing of a nonlinear interaction model with josephsonlike coupling is studied to obtain time scale of maximal squeezing based upon two exactly solvable cases for two and three particles we find that the maximalsqueezing time depends on the level spacing between the ground state and its next neighbor eigenstate | [['spin', 'squeezing', 'of', 'a', 'nonlinear', 'interaction', 'model', 'with', 'josephsonlike', 'coupling', 'is', 'studied', 'to', 'obtain', 'time', 'scale', 'of', 'maximal', 'squeezing', 'based', 'upon', 'two', 'exactly', 'solvable', 'cases', 'for', 'two', 'and', 'three', 'particles', 'we', 'find', 'that', 'the', 'max... | [-0.17647987870499493, 0.2328731348924339, -0.01919200935866684, 0.0603190573095344, -0.008328005596995354, -0.20261572184506804, 0.05488610494881868, 0.37915848463773727, -0.23984607140533626, -0.27284545174334196, 0.07249855457805097, -0.2755829377472401, -0.07494699679315091, 0.19206076208036393, 0.1293411345221102,... |
709.2748 | Super-resolution and non-diffraction longitudinal polarized beam | A method is presented for generation of a subwavelength (0.43 lambda)
longitudinally polarized beam, which propagates without divergence over lengths
of about 4 lambda in free space. This is achieved by controlling the amplitude,
phase and polarization property of the Bessel-Gaussian field on the aperture of
a high n... | physics.pop-ph physics.optics | a method is presented for generation of a subwavelength 043 lambda longitudinally polarized beam which propagates without divergence over lengths of about 4 lambda in free space this is achieved by controlling the amplitude phase and polarization property of the besselgaussian field on the aperture of a high numerical ... | [['a', 'method', 'is', 'presented', 'for', 'generation', 'of', 'a', 'subwavelength', '043', 'lambda', 'longitudinally', 'polarized', 'beam', 'which', 'propagates', 'without', 'divergence', 'over', 'lengths', 'of', 'about', '4', 'lambda', 'in', 'free', 'space', 'this', 'is', 'achieved', 'by', 'controlling', 'the', 'ampl... | [-0.16997673176229, 0.19592108448537496, -0.06430616687374333, 0.002715331719418128, -0.03729928585772331, -0.1117441636026622, 0.0018455351058107156, 0.4583468552535543, -0.2358601349943246, -0.2759074906890209, 0.07512852272618777, -0.24554111525559655, -0.04159578355924728, 0.25253934861393645, 0.027222635636392694,... |
709.2749 | Single Atoms on an Optical Nanofiber | We show that single-atoms can be trapped on the surface of a
subwavelength-diameter silica-fiber, an optical nanofiber, without any external
field, and that single photons spontaneously emitted from the atoms can be
readily detected through the single guided-mode of the nanofiber. A key point
of the work is our findi... | quant-ph | we show that singleatoms can be trapped on the surface of a subwavelengthdiameter silicafiber an optical nanofiber without any external field and that single photons spontaneously emitted from the atoms can be readily detected through the single guidedmode of the nanofiber a key point of the work is our finding that at... | [['we', 'show', 'that', 'singleatoms', 'can', 'be', 'trapped', 'on', 'the', 'surface', 'of', 'a', 'subwavelengthdiameter', 'silicafiber', 'an', 'optical', 'nanofiber', 'without', 'any', 'external', 'field', 'and', 'that', 'single', 'photons', 'spontaneously', 'emitted', 'from', 'the', 'atoms', 'can', 'be', 'readily', '... | [-0.0922976517262803, 0.2595525687303424, -0.06690383377209516, -0.08416481014434576, 0.01053963352362035, -0.15983540006637784, 0.05633796313384049, 0.4908883726932633, -0.2237796850738601, -0.2793693953836468, 0.0006003969768718095, -0.3103095467897578, -0.051207483916635245, 0.24270316625250057, 0.008989137694121562... |
709.275 | A solution to the hierarchy problem from an almost decoupled hidden
sector within a classically scale invariant theory | If scale invariance is a classical symmetry then both the Planck scale and
the weak scale should emerge as quantum effects. We show that this can be
realized in simple scale invariant theories with a hidden sector. The
weak/Planck scale hierarchy emerges in the (technically natural) limit where
the hidden sector deco... | hep-ph hep-th | if scale invariance is a classical symmetry then both the planck scale and the weak scale should emerge as quantum effects we show that this can be realized in simple scale invariant theories with a hidden sector the weakplanck scale hierarchy emerges in the technically natural limit where the hidden sector decouples f... | [['if', 'scale', 'invariance', 'is', 'a', 'classical', 'symmetry', 'then', 'both', 'the', 'planck', 'scale', 'and', 'the', 'weak', 'scale', 'should', 'emerge', 'as', 'quantum', 'effects', 'we', 'show', 'that', 'this', 'can', 'be', 'realized', 'in', 'simple', 'scale', 'invariant', 'theories', 'with', 'a', 'hidden', 'sec... | [-0.15584162121017775, 0.2726645488291979, -0.10272253673523664, 0.1881367214055111, -0.12663163817798098, -0.15030546226538719, -0.022836846336722373, 0.2515947928031286, -0.38849637309710183, -0.30994582895189526, 0.14679704608395697, -0.2436153906583786, -0.1387178848683834, 0.09806380214790503, 0.007960371940086286... |
709.2751 | Instabilities of relativistic mean field models and the role of
nonlinear terms | The instability of nuclear matter due to particle-hole excitation modes has
been studied in the frame-work of several relativistic mean field (RMF) models.
It is found that both the longitudinal and the transversal modes depend
sensitively on the parameter sets used. The important impact of the vector and
vector-scal... | nucl-th astro-ph hep-ph | the instability of nuclear matter due to particlehole excitation modes has been studied in the framework of several relativistic mean field rmf models it is found that both the longitudinal and the transversal modes depend sensitively on the parameter sets used the important impact of the vector and vectorscalar nonlin... | [['the', 'instability', 'of', 'nuclear', 'matter', 'due', 'to', 'particlehole', 'excitation', 'modes', 'has', 'been', 'studied', 'in', 'the', 'framework', 'of', 'several', 'relativistic', 'mean', 'field', 'rmf', 'models', 'it', 'is', 'found', 'that', 'both', 'the', 'longitudinal', 'and', 'the', 'transversal', 'modes', ... | [-0.11236180658313898, 0.15795426847099667, -0.09221030512621792, 0.0880904095166704, -0.04996213440479028, -0.08127383176827489, -0.040293105481432216, 0.33680957410078827, -0.2076161299730734, -0.2897274274987602, 0.056824924481922, -0.22668318716016148, -0.1446290292251523, 0.20741677859632096, -0.01289627468386333,... |
709.2752 | Random Walk Access Times on Partially-Disordered Complex Networks: an
Effective Medium Theory | An analytic effective medium theory is constructed to study the mean access
times for random walks on hybrid disordered structures formed by embedding
complex networks into regular lattices, considering transition rates $F$ that
are different for steps across lattice bonds from the rates $f$ across network
shortcuts.... | cond-mat.dis-nn cond-mat.stat-mech | an analytic effective medium theory is constructed to study the mean access times for random walks on hybrid disordered structures formed by embedding complex networks into regular lattices considering transition rates f that are different for steps across lattice bonds from the rates f across network shortcuts the the... | [['an', 'analytic', 'effective', 'medium', 'theory', 'is', 'constructed', 'to', 'study', 'the', 'mean', 'access', 'times', 'for', 'random', 'walks', 'on', 'hybrid', 'disordered', 'structures', 'formed', 'by', 'embedding', 'complex', 'networks', 'into', 'regular', 'lattices', 'considering', 'transition', 'rates', 'f', '... | [-0.13535283286618172, 0.1726246578594454, -0.03931542119881424, 0.045841704868162594, 0.020814740297853622, -0.1576291505675627, 0.05698361158129644, 0.4623365970940268, -0.2502236032737827, -0.2579951800174848, 0.0639322741215464, -0.2767779327874636, -0.14528030137290132, 0.17911024160520003, 0.004305191504612674, 0... |
709.2753 | Considerations for an Ac Dipole for the LHC | Following successful experience at the BNL AGS, FNAL Tevatron, and CERN SPS,
an AC Dipole will be adopted at the LHC for rapid measurements of ring optics.
This paper describes some of the parameters of the AC dipole for the LHC,
scaling from performance of the FNAL and BNL devices.
| physics.acc-ph | following successful experience at the bnl ags fnal tevatron and cern sps an ac dipole will be adopted at the lhc for rapid measurements of ring optics this paper describes some of the parameters of the ac dipole for the lhc scaling from performance of the fnal and bnl devices | [['following', 'successful', 'experience', 'at', 'the', 'bnl', 'ags', 'fnal', 'tevatron', 'and', 'cern', 'sps', 'an', 'ac', 'dipole', 'will', 'be', 'adopted', 'at', 'the', 'lhc', 'for', 'rapid', 'measurements', 'of', 'ring', 'optics', 'this', 'paper', 'describes', 'some', 'of', 'the', 'parameters', 'of', 'the', 'ac', '... | [-0.06481930767651647, 0.2052975021491875, -0.13970758616924286, 0.0349656472238712, -0.05688559748232365, -0.19436331138014792, -0.019446671397890896, 0.3488938558101654, -0.1891563891246915, -0.2610309511050582, 0.006713462024927139, -0.3544097027182579, 0.06725246084854007, 0.2939001839607954, 0.03563584322109818, 0... |
709.2754 | Slowly Rotating Dilaton Black hole In Anti-de Sitter Spacetime | Rotating dilaton black hole solution for asymptotically anti-de Sitter
spacetime are obtained in the small angular momentum limit with an appropriate
combination of three Liouville-type dilaton potentials. The angular momentum,
magnetic dipole moment and the gyromagnetic ratio of such a black hole are
determined for ... | hep-th gr-qc | rotating dilaton black hole solution for asymptotically antide sitter spacetime are obtained in the small angular momentum limit with an appropriate combination of three liouvilletype dilaton potentials the angular momentum magnetic dipole moment and the gyromagnetic ratio of such a black hole are determined for arbitr... | [['rotating', 'dilaton', 'black', 'hole', 'solution', 'for', 'asymptotically', 'antide', 'sitter', 'spacetime', 'are', 'obtained', 'in', 'the', 'small', 'angular', 'momentum', 'limit', 'with', 'an', 'appropriate', 'combination', 'of', 'three', 'liouvilletype', 'dilaton', 'potentials', 'the', 'angular', 'momentum', 'mag... | [-0.23071278475086168, 0.18486497471754915, 0.007598939602478192, 0.11863436811388685, -0.09688681217197043, -0.17684345089722997, -0.05421924505432029, 0.31491324670899373, -0.1188240097119258, -0.2991219339534067, 0.028116043798106078, -0.30207987086704147, 0.007606321945786476, 0.16939621780497524, 0.023309876103527... |
709.2755 | Different representations of Euclidean geometry and their application to
the space-time geometry | Three different representation of the proper Euclidean geometry are
considered. They differ in the number of basic elements, from which the
geometrical objects are constructed. In E-representation there are three basic
elements (point, segment, angle) and no additional structures. V-representation
contains two basic ... | math.GM | three different representation of the proper euclidean geometry are considered they differ in the number of basic elements from which the geometrical objects are constructed in erepresentation there are three basic elements point segment angle and no additional structures vrepresentation contains two basic elements poi... | [['three', 'different', 'representation', 'of', 'the', 'proper', 'euclidean', 'geometry', 'are', 'considered', 'they', 'differ', 'in', 'the', 'number', 'of', 'basic', 'elements', 'from', 'which', 'the', 'geometrical', 'objects', 'are', 'constructed', 'in', 'erepresentation', 'there', 'are', 'three', 'basic', 'elements'... | [-0.15842222775232248, 0.1351314519269219, -0.0817413542776586, 0.10273205911919117, -0.10695881049377387, -0.1426901325955011, -0.04333097377964881, 0.3847623314530014, -0.29871771497230887, -0.25189353978473267, 0.09926517183186966, -0.2673351757931049, -0.16851736387254637, 0.16400680151171312, -0.06970517732716071,... |
709.2756 | Evolution of the spin Hall effect in Pt nanowires: Size and temperature
effects | We have studied the evolution of the Spin Hall Effect in the regime where the
material size responsible for the spin accumulation is either smaller or larger
than the spin diffusion length. Lateral spin valve structures with Pt
insertions were successfully used to measure the spin absorption efficiency as
well as the... | cond-mat.mtrl-sci cond-mat.mes-hall | we have studied the evolution of the spin hall effect in the regime where the material size responsible for the spin accumulation is either smaller or larger than the spin diffusion length lateral spin valve structures with pt insertions were successfully used to measure the spin absorption efficiency as well as the sp... | [['we', 'have', 'studied', 'the', 'evolution', 'of', 'the', 'spin', 'hall', 'effect', 'in', 'the', 'regime', 'where', 'the', 'material', 'size', 'responsible', 'for', 'the', 'spin', 'accumulation', 'is', 'either', 'smaller', 'or', 'larger', 'than', 'the', 'spin', 'diffusion', 'length', 'lateral', 'spin', 'valve', 'stru... | [-0.14574555214404222, 0.24067601766942662, -0.013453170837646768, 0.023597481504421997, -0.029166243353122196, -0.10197664722222691, -0.026876118748860305, 0.36324047207716825, -0.30489794985037444, -0.2686951956025852, 0.057108418061217484, -0.29746861685096293, -0.09480312478533665, 0.1996838136724117, 0.07253385746... |
709.2757 | Tkachenko modes in a superfluid Fermi gas at unitarity | We calculate the frequencies of the Tkachenko oscillations of a vortex
lattice in a harmonically trapped superfluid Fermi gas. We use the
elasto-hydrodynamic theory by properly accounting for the elastic constants,
the Thomas-Fermi density profile of the atomic cloud, and the boundary
conditions. Thanks to the Fermi ... | cond-mat.other cond-mat.supr-con | we calculate the frequencies of the tkachenko oscillations of a vortex lattice in a harmonically trapped superfluid fermi gas we use the elastohydrodynamic theory by properly accounting for the elastic constants the thomasfermi density profile of the atomic cloud and the boundary conditions thanks to the fermi pressure... | [['we', 'calculate', 'the', 'frequencies', 'of', 'the', 'tkachenko', 'oscillations', 'of', 'a', 'vortex', 'lattice', 'in', 'a', 'harmonically', 'trapped', 'superfluid', 'fermi', 'gas', 'we', 'use', 'the', 'elastohydrodynamic', 'theory', 'by', 'properly', 'accounting', 'for', 'the', 'elastic', 'constants', 'the', 'thoma... | [-0.1959063442097385, 0.2811626131898897, -0.06463560018830507, 0.04857566068836851, -0.012247525599501017, -0.1252163174183313, 0.05919477536433802, 0.31765893021188046, -0.2452659327615747, -0.2318691150300102, 0.03175878375314839, -0.2688394126845366, -0.03084745509964335, 0.19123276242575907, 0.048565112649250015, ... |
709.2758 | Einstein e il Rinnovamento delle Scienze (Einstein and the Renewal of
Science) | As it is well-known, the year 2005 has been the centenary of the "annus
mirabilis" (1905) during which Albert Einstein published four fundamental
papers of his. But already in 1979, for the centenary of Einstein's birth, the
world celebrated his monumantal work. In Italy too, there appeared scientific
books, and many... | physics.hist-ph physics.pop-ph | as it is wellknown the year 2005 has been the centenary of the annus mirabilis 1905 during which albert einstein published four fundamental papers of his but already in 1979 for the centenary of einsteins birth the world celebrated his monumantal work in italy too there appeared scientific books and many semipopulariza... | [['as', 'it', 'is', 'wellknown', 'the', 'year', '2005', 'has', 'been', 'the', 'centenary', 'of', 'the', 'annus', 'mirabilis', '1905', 'during', 'which', 'albert', 'einstein', 'published', 'four', 'fundamental', 'papers', 'of', 'his', 'but', 'already', 'in', '1979', 'for', 'the', 'centenary', 'of', 'einsteins', 'birth',... | [-0.021288857076123244, 0.07621113466675662, -0.13174087521005517, 0.06318402087356101, -0.13237297867524064, -0.1064242508668963, 0.0351663104295116, 0.3024762597030766, -0.16095149185467714, -0.3750364788368269, 0.1255158045403612, -0.31600939703935066, -0.15916569416675963, 0.2097257117470159, -0.1593743826328838, -... |
709.2759 | Stability of the rotating SU(3) Skyrmion | The profile functions of the SU(3) Skyrme soliton are investigated for the
octet, decuplet, and antidecuplet baryons by the mean field approach. In this
approach, the profile functions are affected by the spatial rotation, the
flavor rotation, and the flavor symmetry breaking. The solitons are stable only
in the rest... | hep-ph | the profile functions of the su3 skyrme soliton are investigated for the octet decuplet and antidecuplet baryons by the mean field approach in this approach the profile functions are affected by the spatial rotation the flavor rotation and the flavor symmetry breaking the solitons are stable only in the restricted area... | [['the', 'profile', 'functions', 'of', 'the', 'su3', 'skyrme', 'soliton', 'are', 'investigated', 'for', 'the', 'octet', 'decuplet', 'and', 'antidecuplet', 'baryons', 'by', 'the', 'mean', 'field', 'approach', 'in', 'this', 'approach', 'the', 'profile', 'functions', 'are', 'affected', 'by', 'the', 'spatial', 'rotation', ... | [-0.11646575045467604, 0.23613381633848543, -0.024891057153149408, 0.15602428338485816, -0.06568358753724854, -0.06648235304262673, 0.02408396511218778, 0.36448153665307725, -0.17452309243749864, -0.28437285302299087, 0.057196043268085854, -0.27444572646244625, -0.011944960918056198, 0.07927095559241232, 0.059435597316... |
709.276 | Supervised Machine Learning with a Novel Kernel Density Estimator | In recent years, kernel density estimation has been exploited by computer
scientists to model machine learning problems. The kernel density estimation
based approaches are of interest due to the low time complexity of either O(n)
or O(n*log(n)) for constructing a classifier, where n is the number of sampling
instance... | stat.ML | in recent years kernel density estimation has been exploited by computer scientists to model machine learning problems the kernel density estimation based approaches are of interest due to the low time complexity of either on or onlogn for constructing a classifier where n is the number of sampling instances concerning... | [['in', 'recent', 'years', 'kernel', 'density', 'estimation', 'has', 'been', 'exploited', 'by', 'computer', 'scientists', 'to', 'model', 'machine', 'learning', 'problems', 'the', 'kernel', 'density', 'estimation', 'based', 'approaches', 'are', 'of', 'interest', 'due', 'to', 'the', 'low', 'time', 'complexity', 'of', 'ei... | [-0.07738749001740357, 0.060491199327902936, -0.07287187537512536, 0.07157663412779598, -0.04216202082081773, -0.13413741100821217, 0.04478700505214111, 0.38693607405169317, -0.2630784773402883, -0.29960205290068426, 0.15695429999089822, -0.26259518412602995, -0.14787969336034518, 0.18252442968164603, -0.10341175432043... |
709.2761 | Unbounded-Error Classical and Quantum Communication Complexity | Since the seminal work of Paturi and Simon \cite[FOCS'84 & JCSS'86]{PS86},
the unbounded-error classical communication complexity of a Boolean function
has been studied based on the arrangement of points and hyperplanes. Recently,
\cite[ICALP'07]{INRY07} found that the unbounded-error {\em quantum}
communication comp... | quant-ph | since the seminal work of paturi and simon citefocs84 jcss86ps86 the unboundederror classical communication complexity of a boolean function has been studied based on the arrangement of points and hyperplanes recently citeicalp07inry07 found that the unboundederror em quantum communication complexity in the em oneway c... | [['since', 'the', 'seminal', 'work', 'of', 'paturi', 'and', 'simon', 'citefocs84', 'jcss86ps86', 'the', 'unboundederror', 'classical', 'communication', 'complexity', 'of', 'a', 'boolean', 'function', 'has', 'been', 'studied', 'based', 'on', 'the', 'arrangement', 'of', 'points', 'and', 'hyperplanes', 'recently', 'citeic... | [-0.1847180254633228, 0.09208089094686632, -0.06132903307986756, 0.06026949503924697, -0.04397444154135883, -0.18471222429225842, 0.11590340218429143, 0.34793506167829036, -0.2923469567601569, -0.3050484696558366, 0.06706764204194769, -0.22955873750771086, -0.20378424695382516, 0.20106696260239307, -0.07559044233212868... |
709.2762 | Biomimetic Space-Variant Sampling in a Vision Prosthesis Improves the
User's Skill in a Localization Task | In this experiment, we test the hypothesis of whether a 'retina-like' space
variant sampling pattern can improve the efficiency of a visual prosthesis.
Subjects wearing a visuo-auditory substitution system were tested for their
ability to point at visual targets. The test group (space-variant sampling),
performed sig... | q-bio.NC | in this experiment we test the hypothesis of whether a retinalike space variant sampling pattern can improve the efficiency of a visual prosthesis subjects wearing a visuoauditory substitution system were tested for their ability to point at visual targets the test group spacevariant sampling performed significantly be... | [['in', 'this', 'experiment', 'we', 'test', 'the', 'hypothesis', 'of', 'whether', 'a', 'retinalike', 'space', 'variant', 'sampling', 'pattern', 'can', 'improve', 'the', 'efficiency', 'of', 'a', 'visual', 'prosthesis', 'subjects', 'wearing', 'a', 'visuoauditory', 'substitution', 'system', 'were', 'tested', 'for', 'their... | [-0.07710165682452164, 0.10281526486806829, -0.12134362172720761, 0.06741842095226307, -0.10761932159463565, -0.13767506444998, 0.1408686518412212, 0.426488988058663, -0.25225845245837136, -0.35432599279654864, 0.08078201671650141, -0.21710394579253492, -0.11285486267665508, 0.19253333105609335, -0.13663879440476498, 0... |
709.2763 | Perturbative Theory of Grazing-Incidence Diffuse Nuclear Resonant
Scattering of Synchrotron Radiation | Theoretical description of off-specular grazing-incidence nuclear resonant
scattering of synchrotron radiation (Synchrotron M\"{o}ssbauer Reflectometry,
SMR) is presented. The recently developed SMR, similarly to polarized neutron
reflectometry (PNR), is an analytical tool for the determination of isotopic
and magnet... | cond-mat.other | theoretical description of offspecular grazingincidence nuclear resonant scattering of synchrotron radiation synchrotron mossbauer reflectometry smr is presented the recently developed smr similarly to polarized neutron reflectometry pnr is an analytical tool for the determination of isotopic and magnetic structure of ... | [['theoretical', 'description', 'of', 'offspecular', 'grazingincidence', 'nuclear', 'resonant', 'scattering', 'of', 'synchrotron', 'radiation', 'synchrotron', 'mossbauer', 'reflectometry', 'smr', 'is', 'presented', 'the', 'recently', 'developed', 'smr', 'similarly', 'to', 'polarized', 'neutron', 'reflectometry', 'pnr',... | [-0.09961411071292657, 0.09463484199239666, -0.07459056544390118, 0.05278690192774245, -0.06963295291003944, -0.09680060559377116, 0.03432464830585049, 0.46510011847079785, -0.2546063756831195, -0.2729574888330567, 0.02354958527184163, -0.34783626292259073, -0.1124505846451579, 0.24973512275635704, 0.05405559444001743,... |
709.2764 | Subcritical Lp bounds on spectral clusters for Lipschitz metrics | We establish asymptotic bounds on the L^p norms of spectrally localized
functions in the case of two-dimensional Dirichlet forms with coefficients of
Lipschitz regularity. These bounds are new for the range p>6. A key step in the
proof is bounding the rate at which energy spreads for solutions to hyperbolic
equations... | math.AP | we establish asymptotic bounds on the lp norms of spectrally localized functions in the case of twodimensional dirichlet forms with coefficients of lipschitz regularity these bounds are new for the range p6 a key step in the proof is bounding the rate at which energy spreads for solutions to hyperbolic equations with l... | [['we', 'establish', 'asymptotic', 'bounds', 'on', 'the', 'lp', 'norms', 'of', 'spectrally', 'localized', 'functions', 'in', 'the', 'case', 'of', 'twodimensional', 'dirichlet', 'forms', 'with', 'coefficients', 'of', 'lipschitz', 'regularity', 'these', 'bounds', 'are', 'new', 'for', 'the', 'range', 'p6', 'a', 'key', 'st... | [-0.13662044528043932, 0.07458552495679921, -0.05182677892002242, 0.055546369914534606, -0.08045695825583404, -0.11485210715586112, -0.005835295447872745, 0.31631400201607635, -0.3115039610700613, -0.18899087894156022, 0.1670595181942055, -0.28688793979516186, -0.0794224343219496, 0.24611264363759094, -0.04575362648056... |
709.2765 | Fractional Hamiltonian Monodromy from a Gauss-Manin Monodromy | Fractional Hamiltonian Monodromy is a generalization of the notion of
Hamiltonian Monodromy, recently introduced by N. N. Nekhoroshev, D. A.
Sadovskii and B. I. Zhilinskii for energy-momentum maps whose image has a
particular type of non-isolated singularities. In this paper, we analyze the
notion of Fractional Hamil... | math-ph math.MP | fractional hamiltonian monodromy is a generalization of the notion of hamiltonian monodromy recently introduced by n n nekhoroshev d a sadovskii and b i zhilinskii for energymomentum maps whose image has a particular type of nonisolated singularities in this paper we analyze the notion of fractional hamiltonian monodro... | [['fractional', 'hamiltonian', 'monodromy', 'is', 'a', 'generalization', 'of', 'the', 'notion', 'of', 'hamiltonian', 'monodromy', 'recently', 'introduced', 'by', 'n', 'n', 'nekhoroshev', 'd', 'a', 'sadovskii', 'and', 'b', 'i', 'zhilinskii', 'for', 'energymomentum', 'maps', 'whose', 'image', 'has', 'a', 'particular', 't... | [-0.22865017398220042, 0.07188691316253465, -0.07341798723918265, 0.06199226267230899, -0.07991802817939417, -0.1340232450545401, -0.012020412338998816, 0.25579398576899065, -0.27679476613664755, -0.2216646236812939, 0.06144650681222708, -0.27034759670293523, -0.2167319721268976, 0.13708197356343432, -0.122648635950020... |
709.2766 | The wave equation on Schwarzschild-de Sitter spacetimes | We consider solutions to the linear wave equation $\Box_g\phi=0$ on a
non-extremal maximally extended Schwarzschild-de Sitter spacetime arising from
arbitrary smooth initial data prescribed on an arbitrary Cauchy hypersurface.
(In particular, no symmetry is assumed on initial data, and the support of the
solutions ma... | gr-qc math.AP math.DG | we consider solutions to the linear wave equation box_gphi0 on a nonextremal maximally extended schwarzschildde sitter spacetime arising from arbitrary smooth initial data prescribed on an arbitrary cauchy hypersurface in particular no symmetry is assumed on initial data and the support of the solutions may contain the... | [['we', 'consider', 'solutions', 'to', 'the', 'linear', 'wave', 'equation', 'box_gphi0', 'on', 'a', 'nonextremal', 'maximally', 'extended', 'schwarzschildde', 'sitter', 'spacetime', 'arising', 'from', 'arbitrary', 'smooth', 'initial', 'data', 'prescribed', 'on', 'an', 'arbitrary', 'cauchy', 'hypersurface', 'in', 'parti... | [-0.1537385104442544, 0.0852055812412104, -0.07994855310836876, 0.11106397154601579, -0.0970074178300292, -0.12268867481350439, -0.013894708850133566, 0.30147786577013724, -0.21581670862944496, -0.253775884682258, 0.15176204918006314, -0.31209200210466886, -0.07622162168299389, 0.2027350286177049, -0.05950299330809539,... |
709.2767 | Approximate Model of Neutron Resonant Scattering in a Crystal | In the theory of resonant scattering, the double differential cross section
involves the computation of a multifold integral of a 4-point correlation
function, which generalizes the traditional 2-point correlation function of
Van-Hove for potential scattering. In the case of a neutron-crystal
interaction, the numeric... | cond-mat.other | in the theory of resonant scattering the double differential cross section involves the computation of a multifold integral of a 4point correlation function which generalizes the traditional 2point correlation function of vanhove for potential scattering in the case of a neutroncrystal interaction the numerical computa... | [['in', 'the', 'theory', 'of', 'resonant', 'scattering', 'the', 'double', 'differential', 'cross', 'section', 'involves', 'the', 'computation', 'of', 'a', 'multifold', 'integral', 'of', 'a', '4point', 'correlation', 'function', 'which', 'generalizes', 'the', 'traditional', '2point', 'correlation', 'function', 'of', 'va... | [-0.12954131189463103, 0.09370246206402269, -0.1267266964388645, 0.11463971733927536, -0.0396031317118014, -0.04884818852998507, 0.0312435652097512, 0.30957481035819423, -0.276962040975276, -0.24497329915722466, -0.00022313850892023143, -0.30917000464904004, -0.1615298418726167, 0.19237245184082824, 0.07056141002392237... |
709.2768 | Shape and orientation of stellar velocity ellipsoids in spiral galaxies | We present a numerical study of the properties of the stellar velocity
distribution in stellar discs which have developed a saturated, two-armed
spiral structure. We follow the growth of the spiral structure deeply into the
non-linear regime by solving the Boltzmann moment equations up to second order.
By adopting th... | astro-ph | we present a numerical study of the properties of the stellar velocity distribution in stellar discs which have developed a saturated twoarmed spiral structure we follow the growth of the spiral structure deeply into the nonlinear regime by solving the boltzmann moment equations up to second order by adopting the thind... | [['we', 'present', 'a', 'numerical', 'study', 'of', 'the', 'properties', 'of', 'the', 'stellar', 'velocity', 'distribution', 'in', 'stellar', 'discs', 'which', 'have', 'developed', 'a', 'saturated', 'twoarmed', 'spiral', 'structure', 'we', 'follow', 'the', 'growth', 'of', 'the', 'spiral', 'structure', 'deeply', 'into',... | [-0.13664985642572822, 0.11720597251535278, -0.08894781903874079, 0.07170442503411323, -0.10844844256604269, 0.006543880409335709, -0.027186979123733548, 0.3720466896411048, -0.2490173135889422, -0.3126643403309938, 0.034181342123195395, -0.2539140294456416, -0.08323705334367988, 0.15835607956380468, 0.0035068208190131... |
709.2769 | Time-Dependent {\boldmath $CP$}-Violating Asymmetry in
$B^0\to\rho^0\gamma$ Decays | We report the first measurement of CP-violation parameters in
$B^0\to\rho^0\gamma$ decays based on a data sample of $657\times 10^6
B\bar{B}$ pairs collected with the Belle detector at the KEKB asymmetric-energy
$e^+ e^-$ collider. The flavor of the $B$ meson is identified from the decay
products of the accompanyin... | hep-ex | we report the first measurement of cpviolation parameters in b0torho0gamma decays based on a data sample of 657times 106 bbarb pairs collected with the belle detector at the kekb asymmetricenergy e e collider the flavor of the b meson is identified from the decay products of the accompanying b meson we obtain the timed... | [['we', 'report', 'the', 'first', 'measurement', 'of', 'cpviolation', 'parameters', 'in', 'b0torho0gamma', 'decays', 'based', 'on', 'a', 'data', 'sample', 'of', '657times', '106', 'bbarb', 'pairs', 'collected', 'with', 'the', 'belle', 'detector', 'at', 'the', 'kekb', 'asymmetricenergy', 'e', 'e', 'collider', 'the', 'fl... | [-0.12809533481636354, 0.20379608596164372, -0.05457442829896125, 0.04823215686032669, -0.05268288865279887, -0.11305934811882194, 0.10866000495227654, 0.2634508093638766, -0.1377940683835937, -0.26051027153528505, -0.02737174108586905, -0.42120270497135576, 0.0699351865708107, 0.16254749517482256, 0.10909831230979293,... |
709.277 | Renormalization of chiral two-pion exchange NN interactions. Momentum
vs. coordinate space | The renormalization of the chiral np interaction in the 1S0 channel to N3LO
in Weinberg counting for the long distance potential with one single momentum
and energy independent counterterm is carried out. This renormalization scheme
yields finite and unique results and is free of short distance off-shell
ambiguities.... | nucl-th | the renormalization of the chiral np interaction in the 1s0 channel to n3lo in weinberg counting for the long distance potential with one single momentum and energy independent counterterm is carried out this renormalization scheme yields finite and unique results and is free of short distance offshell ambiguities we o... | [['the', 'renormalization', 'of', 'the', 'chiral', 'np', 'interaction', 'in', 'the', '1s0', 'channel', 'to', 'n3lo', 'in', 'weinberg', 'counting', 'for', 'the', 'long', 'distance', 'potential', 'with', 'one', 'single', 'momentum', 'and', 'energy', 'independent', 'counterterm', 'is', 'carried', 'out', 'this', 'renormali... | [-0.15106649016782356, 0.17115687034809246, -0.10866551688836458, 0.09046503548026802, -0.07369997608475387, -0.11539451502120265, 0.053257926625799604, 0.36312854593762983, -0.2167787614206855, -0.2488189987659168, -0.01292293412082542, -0.32571315096619613, -0.05874887000088795, 0.09096196474901472, 0.031495395395904... |
709.2771 | Interacting Brownian motions and the Gross-Pitaevskii formula | We review probabilistic approaches to the Gross-Pitaevskii theory describing
interacting dilute systems of particles. The main achievement are large
deviations principles for the mean occupation measure of a large system of
interacting Brownian motions in a trapping potential. The corresponding rate
functions are giv... | math.PR math-ph math.MP | we review probabilistic approaches to the grosspitaevskii theory describing interacting dilute systems of particles the main achievement are large deviations principles for the mean occupation measure of a large system of interacting brownian motions in a trapping potential the corresponding rate functions are given as... | [['we', 'review', 'probabilistic', 'approaches', 'to', 'the', 'grosspitaevskii', 'theory', 'describing', 'interacting', 'dilute', 'systems', 'of', 'particles', 'the', 'main', 'achievement', 'are', 'large', 'deviations', 'principles', 'for', 'the', 'mean', 'occupation', 'measure', 'of', 'a', 'large', 'system', 'of', 'in... | [-0.1355938724092474, 0.14363527625807496, -0.08657020130859953, 0.10063467274553009, 0.004264225759210863, -0.11617506225593388, 0.015535235413283641, 0.28239560599571895, -0.2651785016558798, -0.30013803787421367, 0.05086354986789437, -0.3218703423626721, -0.11396216309263504, 0.1661221485950851, -0.00070186764267938... |
709.2772 | Modelling discontinuities and Kelvin-Helmholtz instabilities in SPH | In this paper we discuss the treatment of discontinuities in Smoothed
Particle Hydrodynamics (SPH) simulations. In particular we discuss the
difference between integral and differential representations of the fluid
equations in an SPH context and how this relates to the formulation of dissip
ative terms for the captu... | astro-ph | in this paper we discuss the treatment of discontinuities in smoothed particle hydrodynamics sph simulations in particular we discuss the difference between integral and differential representations of the fluid equations in an sph context and how this relates to the formulation of dissip ative terms for the capture of... | [['in', 'this', 'paper', 'we', 'discuss', 'the', 'treatment', 'of', 'discontinuities', 'in', 'smoothed', 'particle', 'hydrodynamics', 'sph', 'simulations', 'in', 'particular', 'we', 'discuss', 'the', 'difference', 'between', 'integral', 'and', 'differential', 'representations', 'of', 'the', 'fluid', 'equations', 'in', ... | [-0.06103267730132858, 0.07064474831491276, -0.11840029651001613, 0.0624556583231121, -0.04887490295934387, -0.08425956827058043, -0.06104385677463142, 0.3312316269051128, -0.3111208560165121, -0.33132271945942193, 0.06579201570275472, -0.2475181272149914, -0.17209051229615902, 0.2047091326635887, -0.12985761673836452,... |
709.2773 | Applications of dimensional reduction to electroweak and QCD matter | This paper is a slightly modified version of the introductory part of a
doctoral dissertation also containing the articles hep-ph/0311268,
hep-ph/0510375, hep-ph/0512177 and hep-ph/0701250. The thesis discusses
effective field theory methods, in particular dimensional reduction, in the
context of finite temperature f... | hep-ph | this paper is a slightly modified version of the introductory part of a doctoral dissertation also containing the articles hepph0311268 hepph0510375 hepph0512177 and hepph0701250 the thesis discusses effective field theory methods in particular dimensional reduction in the context of finite temperature field theory we ... | [['this', 'paper', 'is', 'a', 'slightly', 'modified', 'version', 'of', 'the', 'introductory', 'part', 'of', 'a', 'doctoral', 'dissertation', 'also', 'containing', 'the', 'articles', 'hepph0311268', 'hepph0510375', 'hepph0512177', 'and', 'hepph0701250', 'the', 'thesis', 'discusses', 'effective', 'field', 'theory', 'meth... | [-0.06872595754499922, 0.14073699029928474, -0.09069490605077454, 0.0770328889870755, -0.06056903266983333, -0.06914382968609283, 0.03943366636239236, 0.2978558935938734, -0.22387947027232044, -0.2603473727869862, 0.0920525678601029, -0.29746184440625606, -0.16572897753103802, 0.1390603354688142, -0.05171567953200402, ... |
709.2774 | Intense terahertz laser fields on a two-dimensional hole gas with Rashba
spin-orbit coupling | We investigate the influence on the density of states and the density of spin
polarization for a two-dimensional hole gas with Rashba spin-orbit coupling
under intense terahertz laser fields. Via Floquet theorem, we solve the
time-dependent Schr\"{o}dinger equation and calculate these densities. It is
shown that a te... | cond-mat.mtrl-sci | we investigate the influence on the density of states and the density of spin polarization for a twodimensional hole gas with rashba spinorbit coupling under intense terahertz laser fields via floquet theorem we solve the timedependent schrodinger equation and calculate these densities it is shown that a terahertz magn... | [['we', 'investigate', 'the', 'influence', 'on', 'the', 'density', 'of', 'states', 'and', 'the', 'density', 'of', 'spin', 'polarization', 'for', 'a', 'twodimensional', 'hole', 'gas', 'with', 'rashba', 'spinorbit', 'coupling', 'under', 'intense', 'terahertz', 'laser', 'fields', 'via', 'floquet', 'theorem', 'we', 'solve'... | [-0.2132439761663527, 0.214568815280705, -0.021828728540287924, 0.06512428193205115, -0.054846083783263035, -0.08618051071413034, 0.003531998129879204, 0.384886925592441, -0.2700936897809422, -0.29077088697127595, 0.009385525554873396, -0.25594844305238057, -0.10007710082730813, 0.20781778043872395, 0.0632501984260572,... |
709.2775 | How often does the ratchet click? Facts, heuristics, asymptotics | The evolutionary force of recombination is lacking in asexually reproducing
populations. As a consequence, the population can suffer an irreversible
accumulation of deleterious mutations, a phenomenon known as Muller's ratchet.
We formulate discrete and continuous time versions of Muller's ratchet.
Inspired by Haigh'... | math.PR q-bio.PE | the evolutionary force of recombination is lacking in asexually reproducing populations as a consequence the population can suffer an irreversible accumulation of deleterious mutations a phenomenon known as mullers ratchet we formulate discrete and continuous time versions of mullers ratchet inspired by haighs 1978 ana... | [['the', 'evolutionary', 'force', 'of', 'recombination', 'is', 'lacking', 'in', 'asexually', 'reproducing', 'populations', 'as', 'a', 'consequence', 'the', 'population', 'can', 'suffer', 'an', 'irreversible', 'accumulation', 'of', 'deleterious', 'mutations', 'a', 'phenomenon', 'known', 'as', 'mullers', 'ratchet', 'we',... | [-0.12619340163443915, 0.17653088787875745, -0.07715123029933735, 0.07324528233712596, -0.03505517741220749, -0.14169342649155156, 0.11778326685907263, 0.32021367097217024, -0.2651699747685625, -0.2768590590380358, 0.06258256640849691, -0.2401440087084969, -0.15300295485578702, 0.20348399943305237, -0.10597691904527672... |
709.2776 | A note on calculating autocovariances of periodic ARMA models | An analytically simple and tractable formula for the start-up autocovariances
of periodic ARMA (PARMA) models is provided.
| stat.ME math.CO stat.CO | an analytically simple and tractable formula for the startup autocovariances of periodic arma parma models is provided | [['an', 'analytically', 'simple', 'and', 'tractable', 'formula', 'for', 'the', 'startup', 'autocovariances', 'of', 'periodic', 'arma', 'parma', 'models', 'is', 'provided']] | [-0.0725640385028194, 0.06090272986758089, -0.10857265365912634, 0.15033530754119376, -0.10012661008273854, -0.2205612017389606, 0.038703192970441544, 0.4103558488628444, -0.2377377498675795, -0.15975893338156097, 0.14974439144134521, -0.20227767096366733, -0.19098459140342824, 0.3078726764549227, -0.08680906946606495,... |
709.2777 | Basic outlines of a new hypothesis on physical reality | The papers mentioned in the bibliography lead to this new hypothesis which
constitutes a wide panorama of the physical reality. Its coherence and its
simplicity are virtues that make interesant to gaze upon it.
| physics.gen-ph | the papers mentioned in the bibliography lead to this new hypothesis which constitutes a wide panorama of the physical reality its coherence and its simplicity are virtues that make interesant to gaze upon it | [['the', 'papers', 'mentioned', 'in', 'the', 'bibliography', 'lead', 'to', 'this', 'new', 'hypothesis', 'which', 'constitutes', 'a', 'wide', 'panorama', 'of', 'the', 'physical', 'reality', 'its', 'coherence', 'and', 'its', 'simplicity', 'are', 'virtues', 'that', 'make', 'interesant', 'to', 'gaze', 'upon', 'it']] | [-0.05755552169725751, 0.07627662649434624, -0.14143604378808627, 0.03370698215087142, -0.14618460884825749, -0.12275624987810399, 0.060995122375474733, 0.3758593733337792, -0.25667449211080867, -0.32241176612054306, 0.08540081191511656, -0.21925849986798834, -0.13937852787079685, 0.1930247921440186, -0.141527431085705... |
709.2778 | A search for Very High Energy gamma-ray emission from Passive
Super-massive Black Holes | Jets of Active Galactic Nuclei (AGN) are established emitters of very high
energy (VHE; >100 GeV) gamma-rays. VHE radiation is also expected to be emitted
from the vicinity of super-massive black holes (SMBH), irrespective of their
activity state. Accreting SMBH rotate and generate a dipolar magnetic field. In
the ma... | astro-ph | jets of active galactic nuclei agn are established emitters of very high energy vhe 100 gev gammarays vhe radiation is also expected to be emitted from the vicinity of supermassive black holes smbh irrespective of their activity state accreting smbh rotate and generate a dipolar magnetic field in the magnetosphere of t... | [['jets', 'of', 'active', 'galactic', 'nuclei', 'agn', 'are', 'established', 'emitters', 'of', 'very', 'high', 'energy', 'vhe', '100', 'gev', 'gammarays', 'vhe', 'radiation', 'is', 'also', 'expected', 'to', 'be', 'emitted', 'from', 'the', 'vicinity', 'of', 'supermassive', 'black', 'holes', 'smbh', 'irrespective', 'of',... | [-0.0666891349359907, 0.18741638039419842, -0.02943775651834181, 0.20811547639843614, -0.14270725258716588, -0.0947883683968232, -0.0012181737757701841, 0.446455553950121, -0.139741269328321, -0.36374046006757355, -0.06431624850180621, -0.3244047692861487, 0.0855883480382747, 0.23333143106073193, 0.031068125938974036, ... |
709.2779 | Full counting statistics of spin transfer through ultrasmall quantum
dots | We analyze the spin-resolved full counting statistics of electron transfer
through an ultrasmall quantum dot coupled to metallic electrodes. Modelling the
setup by the Anderson Hamiltonian, we explicitly take into account the onsite
Coulomb repulsion $U$. We calculate the cumulant generating function for the
probabil... | cond-mat.mes-hall cond-mat.str-el | we analyze the spinresolved full counting statistics of electron transfer through an ultrasmall quantum dot coupled to metallic electrodes modelling the setup by the anderson hamiltonian we explicitly take into account the onsite coulomb repulsion u we calculate the cumulant generating function for the probability to t... | [['we', 'analyze', 'the', 'spinresolved', 'full', 'counting', 'statistics', 'of', 'electron', 'transfer', 'through', 'an', 'ultrasmall', 'quantum', 'dot', 'coupled', 'to', 'metallic', 'electrodes', 'modelling', 'the', 'setup', 'by', 'the', 'anderson', 'hamiltonian', 'we', 'explicitly', 'take', 'into', 'account', 'the',... | [-0.13478234295582617, 0.15870795767809528, -0.06789369285380577, 0.0883865154139451, -0.019250270277124774, -0.13042280452517682, 0.05456678566406481, 0.36126473616048527, -0.253189277547576, -0.291339498698054, 0.0014355134660624625, -0.3097326548355768, -0.08785974965704714, 0.19285449258955745, 0.05771095504956868,... |
709.278 | The stellar content of low redshift BL Lac host galaxies from
multicolour imaging | We present B-band imaging of 18 low redshift (z<0.3) BL Lac objects for which
their host galaxies were previously resolved in the R-band and the
near-infrared H-band. For a subset of the objects, also U- and V-band imaging
is presented. These data are used to investigate the blue-red-near-infrared
colours and the col... | astro-ph | we present bband imaging of 18 low redshift z03 bl lac objects for which their host galaxies were previously resolved in the rband and the nearinfrared hband for a subset of the objects also u and vband imaging is presented these data are used to investigate the bluerednearinfrared colours and the colour gradients of t... | [['we', 'present', 'bband', 'imaging', 'of', '18', 'low', 'redshift', 'z03', 'bl', 'lac', 'objects', 'for', 'which', 'their', 'host', 'galaxies', 'were', 'previously', 'resolved', 'in', 'the', 'rband', 'and', 'the', 'nearinfrared', 'hband', 'for', 'a', 'subset', 'of', 'the', 'objects', 'also', 'u', 'and', 'vband', 'ima... | [-0.0416463472486402, 0.1074503823417427, -0.06864691910584672, 0.12700592013514744, -0.09436898797866888, -0.06846566096154184, 0.03357665904063301, 0.4984409052090576, -0.09624602265270929, -0.39500894177382667, 0.032733535853017554, -0.30083200993876047, -0.041405313345491704, 0.17750171702019332, -0.082395301162838... |
709.2781 | Volume-energy correlations in the slow degrees of freedom of
computer-simulated phospholipid membranes | Constant-pressure molecular-dynamics simulations of phospholipid membranes in
the fluid phase reveal strong correlations between equilibrium fluctuations of
volume and energy on the nanosecond time-scale. The existence of strong
volume-energy correlations was previously deduced indirectly by Heimburg from
experiments... | physics.bio-ph | constantpressure moleculardynamics simulations of phospholipid membranes in the fluid phase reveal strong correlations between equilibrium fluctuations of volume and energy on the nanosecond timescale the existence of strong volumeenergy correlations was previously deduced indirectly by heimburg from experiments focusi... | [['constantpressure', 'moleculardynamics', 'simulations', 'of', 'phospholipid', 'membranes', 'in', 'the', 'fluid', 'phase', 'reveal', 'strong', 'correlations', 'between', 'equilibrium', 'fluctuations', 'of', 'volume', 'and', 'energy', 'on', 'the', 'nanosecond', 'timescale', 'the', 'existence', 'of', 'strong', 'volumeen... | [-0.1438958631339989, 0.22547935695468407, -0.1062818629535563, 0.02134650377126451, 0.07994017104172836, -0.13443966801075832, 0.0293441251244234, 0.38025603142222797, -0.24200135860187205, -0.30941131763646135, 0.06094704738833294, -0.33840204095063003, -0.12846933654509485, 0.13218564315415596, 0.09418182765923279, ... |
709.2782 | Ab initio and Molecular Dynamics Study of the Nanomechanical Properties
of DNA Oligomers | Although a vast amount of experimental information is available on the
elongation, compression, and folding of proteins in biochemical processes, very
little is known about the real structure and molecular dynamics of DNA at an
atomic level. Since this area of work is relatively new, this paper reports the
results of... | cond-mat.mtrl-sci | although a vast amount of experimental information is available on the elongation compression and folding of proteins in biochemical processes very little is known about the real structure and molecular dynamics of dna at an atomic level since this area of work is relatively new this paper reports the results of comput... | [['although', 'a', 'vast', 'amount', 'of', 'experimental', 'information', 'is', 'available', 'on', 'the', 'elongation', 'compression', 'and', 'folding', 'of', 'proteins', 'in', 'biochemical', 'processes', 'very', 'little', 'is', 'known', 'about', 'the', 'real', 'structure', 'and', 'molecular', 'dynamics', 'of', 'dna', ... | [-0.13945505397764277, 0.12199983400893111, -0.05550417474994104, 0.03847256588130832, -0.04037008937193106, -0.06893445518862916, 0.07386164262744101, 0.37492192056259677, -0.3024350973292675, -0.30196333651060925, 0.06650261083069219, -0.23382310616968788, -0.19742639551628127, 0.23473485472471747, -0.030769531742656... |
709.2783 | Three-dimensional aspects of fluid flows in channels. I. Meniscus and
Thin Film regimes | We study the forced displacement of a fluid-fluid interface in a
three-dimensional channel formed by two parallel solid plates. Using a
Lattice-Boltzmann method, we study situations in which a slip velocity arises
from diffusion effects near the contact line. The difference between the slip
and channel velocities det... | physics.flu-dyn | we study the forced displacement of a fluidfluid interface in a threedimensional channel formed by two parallel solid plates using a latticeboltzmann method we study situations in which a slip velocity arises from diffusion effects near the contact line the difference between the slip and channel velocities determines ... | [['we', 'study', 'the', 'forced', 'displacement', 'of', 'a', 'fluidfluid', 'interface', 'in', 'a', 'threedimensional', 'channel', 'formed', 'by', 'two', 'parallel', 'solid', 'plates', 'using', 'a', 'latticeboltzmann', 'method', 'we', 'study', 'situations', 'in', 'which', 'a', 'slip', 'velocity', 'arises', 'from', 'diff... | [-0.15328175730672494, 0.16851959796054516, -0.10352116030436463, -0.0285836563618831, -0.03634591375352678, -0.14146324227813903, 0.027759237971622497, 0.3556964291804811, -0.277382879892773, -0.2803128960587811, 0.055062507072651035, -0.267975072055578, -0.11944731194334297, 0.18638616739403138, -0.02396027405360123,... |
709.2784 | Putting a cap on causality violations in CDT | The formalism of causal dynamical triangulations (CDT) provides us with a
non-perturbatively defined model of quantum gravity, where the sum over
histories includes only causal space-time histories. Path integrals of CDT and
their continuum limits have been studied in two, three and four dimensions.
Here we investiga... | gr-qc hep-th | the formalism of causal dynamical triangulations cdt provides us with a nonperturbatively defined model of quantum gravity where the sum over histories includes only causal spacetime histories path integrals of cdt and their continuum limits have been studied in two three and four dimensions here we investigate a gener... | [['the', 'formalism', 'of', 'causal', 'dynamical', 'triangulations', 'cdt', 'provides', 'us', 'with', 'a', 'nonperturbatively', 'defined', 'model', 'of', 'quantum', 'gravity', 'where', 'the', 'sum', 'over', 'histories', 'includes', 'only', 'causal', 'spacetime', 'histories', 'path', 'integrals', 'of', 'cdt', 'and', 'th... | [-0.15343423937285272, 0.1413728005217412, -0.14394998946521856, 0.09958000210720952, -0.050091293581490275, -0.13564873278830672, 0.055253605414299835, 0.31896553925368226, -0.24181001628690127, -0.2683453274525325, 0.06458370744462914, -0.22995020779692626, -0.19084644612349286, 0.12547021150541834, -0.03633606290633... |
709.2785 | Three-dimensional aspects of fluid flows in channels. II. Effects of
Meniscus and Thin Film regimes on Viscous Fingers | We perform a three-dimensional study of steady state viscous fingers that
develop in linear channels. By means of a three-dimensional Lattice-Boltzmann
scheme that mimics the full macroscopic equations of motion of the fluid
momentum and order parameter, we study the effect of the thickness of the
channel in two case... | physics.flu-dyn | we perform a threedimensional study of steady state viscous fingers that develop in linear channels by means of a threedimensional latticeboltzmann scheme that mimics the full macroscopic equations of motion of the fluid momentum and order parameter we study the effect of the thickness of the channel in two cases first... | [['we', 'perform', 'a', 'threedimensional', 'study', 'of', 'steady', 'state', 'viscous', 'fingers', 'that', 'develop', 'in', 'linear', 'channels', 'by', 'means', 'of', 'a', 'threedimensional', 'latticeboltzmann', 'scheme', 'that', 'mimics', 'the', 'full', 'macroscopic', 'equations', 'of', 'motion', 'of', 'the', 'fluid'... | [-0.13905017359569463, 0.1388930332919596, -0.08267838903042284, -0.0490325636235363, -0.030076481735479114, -0.10761096481405569, 0.021850349335330175, 0.35749705063165926, -0.29066378511290286, -0.2851856637296947, 0.056791609713761466, -0.2497065694778101, -0.11822145301782598, 0.18101483583780573, -0.00973311723176... |
709.2786 | Existence of Unexcited and Excited Biexcitons in Molecular Crystals | The theory of four-body systems is revisited. It is illustrated that the
theory provides a rigorous proof for the formation of ground state (unexcited)
biexcitons in molecular crystals. The generalization of the theory predicts the
possible existence of excited biexcitons in nature. In order to test the
validity of t... | physics.atm-clus physics.chem-ph | the theory of fourbody systems is revisited it is illustrated that the theory provides a rigorous proof for the formation of ground state unexcited biexcitons in molecular crystals the generalization of the theory predicts the possible existence of excited biexcitons in nature in order to test the validity of the exten... | [['the', 'theory', 'of', 'fourbody', 'systems', 'is', 'revisited', 'it', 'is', 'illustrated', 'that', 'the', 'theory', 'provides', 'a', 'rigorous', 'proof', 'for', 'the', 'formation', 'of', 'ground', 'state', 'unexcited', 'biexcitons', 'in', 'molecular', 'crystals', 'the', 'generalization', 'of', 'the', 'theory', 'pred... | [-0.13177952089596115, 0.13939079239029079, -0.06501309001326087, 0.10061843181539555, 0.011566534311624995, -0.15060432361063072, 0.03715357049204932, 0.3093226536232243, -0.1688194313789146, -0.30806158381726656, 0.028852585483579326, -0.22866675503074044, -0.11078893204971232, 0.20773512437090016, 0.0299805173764756... |
709.2787 | Quantum Transport in Metalporphyrins. An ab initio Green's function
approach to nanosensors design | An ab initio Green's function study of the electron transport properties of
the selected metal-porphyrin complexes has been performed. Transmission spectra
and current-voltage dependence have been calculated for the porphyrin molecule
located between gold electrodes in the presence of interaction with metal
atoms, wh... | cond-mat.mtrl-sci | an ab initio greens function study of the electron transport properties of the selected metalporphyrin complexes has been performed transmission spectra and currentvoltage dependence have been calculated for the porphyrin molecule located between gold electrodes in the presence of interaction with metal atoms which are... | [['an', 'ab', 'initio', 'greens', 'function', 'study', 'of', 'the', 'electron', 'transport', 'properties', 'of', 'the', 'selected', 'metalporphyrin', 'complexes', 'has', 'been', 'performed', 'transmission', 'spectra', 'and', 'currentvoltage', 'dependence', 'have', 'been', 'calculated', 'for', 'the', 'porphyrin', 'molec... | [-0.10886370057220726, 0.08287496835606968, -0.026706258630535256, 0.028098825005387577, 0.05205702374999722, -0.15773739342888196, 0.057362704225912844, 0.4436561035302778, -0.2100574519378521, -0.3090676835272461, -0.06292400578677189, -0.3486677383383115, -0.10911050783276248, 0.16400407377708082, 0.0651961482207601... |
709.2788 | Laser control in a bifurcating region | We present a complete analysis of the laser control of a model molecular
system using both optimal control theory and adiabatic techniques. This
molecule has a particular potential energy surface with a bifurcating region
connecting three potential wells which allows a variety of processes such as
isomerization, tunn... | quant-ph | we present a complete analysis of the laser control of a model molecular system using both optimal control theory and adiabatic techniques this molecule has a particular potential energy surface with a bifurcating region connecting three potential wells which allows a variety of processes such as isomerization tunnelli... | [['we', 'present', 'a', 'complete', 'analysis', 'of', 'the', 'laser', 'control', 'of', 'a', 'model', 'molecular', 'system', 'using', 'both', 'optimal', 'control', 'theory', 'and', 'adiabatic', 'techniques', 'this', 'molecule', 'has', 'a', 'particular', 'potential', 'energy', 'surface', 'with', 'a', 'bifurcating', 'regi... | [-0.1318907610501253, 0.06179823658444108, -0.10753034281304046, 0.02954090498538027, 0.005862454367395971, -0.15724022614379082, 0.08344818889200988, 0.390306685240038, -0.2635777233949592, -0.301886806730181, 0.09574635188290549, -0.22955883881501993, -0.1699534900214325, 0.22411628126827698, -0.018024202851407725, 0... |
709.2789 | PT-symmetric Solutions of Schrodinger Equation with position-dependent
mass via Point Canonical Transformation | PT-symmetric solutions of Schrodinger equation are obtained for the Scarf and
generalized harmonic oscillator potentials with the position-dependent mass. A
general point canonical transformation is applied by using a free parameter.
Three different forms of mass distributions are used. A set of the energy
eigenvalue... | quant-ph | ptsymmetric solutions of schrodinger equation are obtained for the scarf and generalized harmonic oscillator potentials with the positiondependent mass a general point canonical transformation is applied by using a free parameter three different forms of mass distributions are used a set of the energy eigenvalues of th... | [['ptsymmetric', 'solutions', 'of', 'schrodinger', 'equation', 'are', 'obtained', 'for', 'the', 'scarf', 'and', 'generalized', 'harmonic', 'oscillator', 'potentials', 'with', 'the', 'positiondependent', 'mass', 'a', 'general', 'point', 'canonical', 'transformation', 'is', 'applied', 'by', 'using', 'a', 'free', 'paramet... | [-0.1095925857527898, 0.14110490223213742, -0.07305541689722583, 0.09271162946959241, -0.026429746378786288, -0.15808245074003935, -0.019804084874116456, 0.33087611387555416, -0.2154712631725348, -0.2600222293000955, 0.04533176901392066, -0.29934153816161246, -0.12511128261685373, 0.21761438224751214, 0.054181603743479... |
709.279 | A Quantum Dot with Impurity in the Lobachevsky Plane | The curvature effect on a quantum dot with impurity is investigated. The
model is considered on the Lobachevsky plane. The confinement and impurity
potentials are chosen so that the model is explicitly solvable. The Green
function as well as the Krein Q-function are computed.
| math-ph math.MP | the curvature effect on a quantum dot with impurity is investigated the model is considered on the lobachevsky plane the confinement and impurity potentials are chosen so that the model is explicitly solvable the green function as well as the krein qfunction are computed | [['the', 'curvature', 'effect', 'on', 'a', 'quantum', 'dot', 'with', 'impurity', 'is', 'investigated', 'the', 'model', 'is', 'considered', 'on', 'the', 'lobachevsky', 'plane', 'the', 'confinement', 'and', 'impurity', 'potentials', 'are', 'chosen', 'so', 'that', 'the', 'model', 'is', 'explicitly', 'solvable', 'the', 'gr... | [-0.09791471924505789, 0.14409747840413314, -0.03964249074289745, 0.1517262483327861, -0.030917305472857235, -0.1810341171645136, -0.040634367821357126, 0.4314141281965104, -0.2348632306199182, -0.24671797932718287, 0.08168256646868857, -0.29844522882591595, -0.1675221466205337, 0.16790922857101329, 0.00816484335386617... |
709.2791 | Kalman Filtering with Equality and Inequality State Constraints | Both constrained and unconstrained optimization problems regularly appear in
recursive tracking problems engineers currently address -- however, constraints
are rarely exploited for these applications. We define the Kalman Filter and
discuss two different approaches to incorporating constraints. Each of these
approac... | math.OC physics.data-an | both constrained and unconstrained optimization problems regularly appear in recursive tracking problems engineers currently address however constraints are rarely exploited for these applications we define the kalman filter and discuss two different approaches to incorporating constraints each of these approaches are ... | [['both', 'constrained', 'and', 'unconstrained', 'optimization', 'problems', 'regularly', 'appear', 'in', 'recursive', 'tracking', 'problems', 'engineers', 'currently', 'address', 'however', 'constraints', 'are', 'rarely', 'exploited', 'for', 'these', 'applications', 'we', 'define', 'the', 'kalman', 'filter', 'and', 'd... | [-0.058360455074132636, 0.014135734709457327, -0.04375548065246011, 0.12442540284544708, -0.1248707253820239, -0.22085328025218004, -0.013041368709542813, 0.4200244740797923, -0.31389519119730747, -0.3576677594310007, 0.21970138773292255, -0.2587414509258591, -0.14716157127315035, 0.24492022667366725, -0.08254238020760... |
709.2792 | Constraining the growth factor with baryon oscillations | The growth factor of linear fluctuations is probably one of the least known
quantity in observational cosmology. Here we discuss the constraints that
baryon oscillations in galaxy power spectra from future surveys can put on a
conveniently parametrized growth factor. We find that spectroscopic surveys of
$5000 deg^2$... | astro-ph | the growth factor of linear fluctuations is probably one of the least known quantity in observational cosmology here we discuss the constraints that baryon oscillations in galaxy power spectra from future surveys can put on a conveniently parametrized growth factor we find that spectroscopic surveys of 5000 deg2 extend... | [['the', 'growth', 'factor', 'of', 'linear', 'fluctuations', 'is', 'probably', 'one', 'of', 'the', 'least', 'known', 'quantity', 'in', 'observational', 'cosmology', 'here', 'we', 'discuss', 'the', 'constraints', 'that', 'baryon', 'oscillations', 'in', 'galaxy', 'power', 'spectra', 'from', 'future', 'surveys', 'can', 'p... | [-0.11271240345193344, 0.10435151013229789, -0.09409833422780615, 0.11496642962532136, -0.1186934844455094, -0.09380116766698442, 0.03733420603031528, 0.3093877065863496, -0.2294451472286171, -0.3536782732586042, 0.10380303560647643, -0.304776173699828, -0.026727976628411924, 0.24028935554455425, -0.03634839689187271, ... |
709.2793 | Cubical convex ear decompositions | We consider the problem of constructing a convex ear decomposition for a
poset. The usual technique, first used by Nyman and Swartz, starts with a
CL-labeling and uses this to shell the `ears' of the decomposition. We
axiomatize the necessary conditions for this technique as a "CL-ced" or
"EL-ced". We find an EL-ced ... | math.CO | we consider the problem of constructing a convex ear decomposition for a poset the usual technique first used by nyman and swartz starts with a cllabeling and uses this to shell the ears of the decomposition we axiomatize the necessary conditions for this technique as a clced or elced we find an elced of the ddivisible... | [['we', 'consider', 'the', 'problem', 'of', 'constructing', 'a', 'convex', 'ear', 'decomposition', 'for', 'a', 'poset', 'the', 'usual', 'technique', 'first', 'used', 'by', 'nyman', 'and', 'swartz', 'starts', 'with', 'a', 'cllabeling', 'and', 'uses', 'this', 'to', 'shell', 'the', 'ears', 'of', 'the', 'decomposition', 'w... | [-0.11552827649898569, 0.1134245575103705, -0.1290615351179238, 0.06167126698144582, -0.08106467494993315, -0.10695149591063252, -0.001345359809218078, 0.43747980639131534, -0.3277707484214463, -0.1597484099523475, 0.15092714883374153, -0.2644142816118094, -0.1652955219049343, 0.1203106592608189, -0.11007794602644733, ... |
709.2794 | Polyhedral tori with minimal coordinates | We give explicit realizations with small integer coordinates for all
triangulated tori with up to 12 vertices. In particular, we provide
coordinate-minimal realizations in general position for all triangulations of
the torus with 7, 8, 9, and 10 vertices. For the unique 7-vertex triangulation
of the torus we show tha... | math.MG math.CO | we give explicit realizations with small integer coordinates for all triangulated tori with up to 12 vertices in particular we provide coordinateminimal realizations in general position for all triangulations of the torus with 7 8 9 and 10 vertices for the unique 7vertex triangulation of the torus we show that all corr... | [['we', 'give', 'explicit', 'realizations', 'with', 'small', 'integer', 'coordinates', 'for', 'all', 'triangulated', 'tori', 'with', 'up', 'to', '12', 'vertices', 'in', 'particular', 'we', 'provide', 'coordinateminimal', 'realizations', 'in', 'general', 'position', 'for', 'all', 'triangulations', 'of', 'the', 'torus', ... | [-0.14351743535435463, 0.11819135261940064, 0.04123148251488641, 0.016917051583692267, -0.029819823064646877, -0.1251115761390263, -0.00749030297079666, 0.40693383917703735, -0.23298053970499025, -0.37325009580824403, 0.12254097554922247, -0.30525058724375054, -0.1213828308077959, 0.13105206705302327, -0.11171220928676... |
709.2795 | Quantum Theory on Lobatchevski Spaces | In this paper we set up a general formalism to deal with quantum theories on
a Lobatchevski space, i.e. a spatial manifold that is homogeneous, isotropic
and has negative curvature. The heart of our approach is the construction of a
suitable basis of plane waves which are eigenfunctions of the Laplace-Beltrami
operat... | hep-th | in this paper we set up a general formalism to deal with quantum theories on a lobatchevski space ie a spatial manifold that is homogeneous isotropic and has negative curvature the heart of our approach is the construction of a suitable basis of plane waves which are eigenfunctions of the laplacebeltrami operator relat... | [['in', 'this', 'paper', 'we', 'set', 'up', 'a', 'general', 'formalism', 'to', 'deal', 'with', 'quantum', 'theories', 'on', 'a', 'lobatchevski', 'space', 'ie', 'a', 'spatial', 'manifold', 'that', 'is', 'homogeneous', 'isotropic', 'and', 'has', 'negative', 'curvature', 'the', 'heart', 'of', 'our', 'approach', 'is', 'the... | [-0.08117907599672296, 0.10018275521687721, -0.10959009399984852, 0.09788380178989906, -0.12306086859523745, -0.1026656291155555, -0.03290257444684157, 0.3552115724453608, -0.2405488014663175, -0.2548784601217988, 0.1168425973047013, -0.23428743841300198, -0.18274416215915107, 0.21604703391223387, -0.11224899539167567,... |
709.2796 | Unoccupied states of individual silver clusters and chains on Ag(111) | Size-selected silver clusters on Ag(111) were fabricated with the tip of a
scanning tunneling microscope. Unoccupied electron resonances give rise to
image contrast and spectral features which shift toward the Fermi level with
increasing cluster size. Linear assemblies exhibit higher resonance energies
than equally s... | cond-mat.mtrl-sci | sizeselected silver clusters on ag111 were fabricated with the tip of a scanning tunneling microscope unoccupied electron resonances give rise to image contrast and spectral features which shift toward the fermi level with increasing cluster size linear assemblies exhibit higher resonance energies than equally sized co... | [['sizeselected', 'silver', 'clusters', 'on', 'ag111', 'were', 'fabricated', 'with', 'the', 'tip', 'of', 'a', 'scanning', 'tunneling', 'microscope', 'unoccupied', 'electron', 'resonances', 'give', 'rise', 'to', 'image', 'contrast', 'and', 'spectral', 'features', 'which', 'shift', 'toward', 'the', 'fermi', 'level', 'wit... | [-0.06046183016278768, 0.1884767748752357, -0.07233904284259228, 0.055147566024073696, 0.031210488298499626, -0.2128776512874214, 0.07003306105496898, 0.44376817577811956, -0.18196913814937618, -0.368687030821018, -0.11880581815765329, -0.3750271584634503, -0.06339969672232768, 0.09568024569267586, 0.06205744742198962,... |
709.2797 | Comments On " Orbits of automorphism groups of fields" | Let $R$ be a commutative $k-$algebra over a field $k$. Assume $R$ is a
noetherian, infinite, integral domain. The group of $k-$automorphisms of
$R$,i.e.$Aut_k(R)$ acts in a natural way on $(R-k)$.In the first part of this
article, we study the structure of $R$ when the orbit space $(R-k)/Aut_k(R)$ is
finite.We note t... | math.AC | let r be a commutative kalgebra over a field k assume r is a noetherian infinite integral domain the group of kautomorphisms of rieaut_kr acts in a natural way on rkin the first part of this article we study the structure of r when the orbit space rkaut_kr is finitewe note that most of the results not particularly rele... | [['let', 'r', 'be', 'a', 'commutative', 'kalgebra', 'over', 'a', 'field', 'k', 'assume', 'r', 'is', 'a', 'noetherian', 'infinite', 'integral', 'domain', 'the', 'group', 'of', 'kautomorphisms', 'of', 'rieaut_kr', 'acts', 'in', 'a', 'natural', 'way', 'on', 'rkin', 'the', 'first', 'part', 'of', 'this', 'article', 'we', 's... | [-0.22044972880658778, 0.10183288239458113, -0.10796302991785166, 0.015271512143292719, -0.07188311121497078, -0.13611374195721565, -0.03698816444640132, 0.3467930054052197, -0.29995664364083274, -0.18693984270265157, 0.10301934276217115, -0.25092120929691714, -0.11160364012793059, 0.20049470282780626, -0.0743665363353... |
709.2798 | The twist subgroup of the mapping class group of a nonorientable surface | Let T(N) be the subgroup of the mapping class group of a nonorientable
surface N (possibly with punctures and/or boundary components) generated by
twists about two-sided circles. We obtain a simple generating set for T(N). As
an application we compute the first homology group (abelianization) of T(N).
| math.GT | let tn be the subgroup of the mapping class group of a nonorientable surface n possibly with punctures andor boundary components generated by twists about twosided circles we obtain a simple generating set for tn as an application we compute the first homology group abelianization of tn | [['let', 'tn', 'be', 'the', 'subgroup', 'of', 'the', 'mapping', 'class', 'group', 'of', 'a', 'nonorientable', 'surface', 'n', 'possibly', 'with', 'punctures', 'andor', 'boundary', 'components', 'generated', 'by', 'twists', 'about', 'twosided', 'circles', 'we', 'obtain', 'a', 'simple', 'generating', 'set', 'for', 'tn', ... | [-0.22751019351144738, 0.10912246765609722, -0.056997931780333216, -0.0014877463988167174, -0.12863432382173995, -0.1310707690550926, 0.036561017538955874, 0.3540496249148186, -0.3131090195730646, -0.25168787299635564, 0.14645006787527273, -0.3000841739171363, -0.11262314043879668, 0.21116553619503975, -0.0922229605568... |
709.2799 | Supersymmetric SU(5) GUT with Stabilized Moduli | We construct a minimal example of a supersymmetric grand unified model in a
toroidal compactification of type I string theory with magnetized D9-branes.
All geometric moduli are stabilized in terms of the background internal
magnetic fluxes which are of "oblique" type (mutually non-commuting). The gauge
symmetry is j... | hep-th hep-ph | we construct a minimal example of a supersymmetric grand unified model in a toroidal compactification of type i string theory with magnetized d9branes all geometric moduli are stabilized in terms of the background internal magnetic fluxes which are of oblique type mutually noncommuting the gauge symmetry is just su5 an... | [['we', 'construct', 'a', 'minimal', 'example', 'of', 'a', 'supersymmetric', 'grand', 'unified', 'model', 'in', 'a', 'toroidal', 'compactification', 'of', 'type', 'i', 'string', 'theory', 'with', 'magnetized', 'd9branes', 'all', 'geometric', 'moduli', 'are', 'stabilized', 'in', 'terms', 'of', 'the', 'background', 'inte... | [-0.16443596361204982, 0.2873528212388181, -0.016355227867978207, 0.12070210320382392, -0.09346144653829759, -0.1392840376407232, -0.05598844113536989, 0.33912875169240264, -0.17288171715926434, -0.2731332253711973, 0.05243363935817573, -0.24311802524101475, -0.05944686561849886, 0.0803084941547148, -0.0397048345024603... |
709.28 | The Broad Line Region of Quasars | The last decade saw long-awaited improvements in our understanding of active
galactic nuclei (AGN) spectral properties. This contribution reviews some
important observational results obtained from optical and UV data as well as
constraints on physical parameters that control the structure and dynamics of
the Broad Li... | astro-ph | the last decade saw longawaited improvements in our understanding of active galactic nuclei agn spectral properties this contribution reviews some important observational results obtained from optical and uv data as well as constraints on physical parameters that control the structure and dynamics of the broad line reg... | [['the', 'last', 'decade', 'saw', 'longawaited', 'improvements', 'in', 'our', 'understanding', 'of', 'active', 'galactic', 'nuclei', 'agn', 'spectral', 'properties', 'this', 'contribution', 'reviews', 'some', 'important', 'observational', 'results', 'obtained', 'from', 'optical', 'and', 'uv', 'data', 'as', 'well', 'as'... | [-0.03442833004420266, 0.04599436494383089, -0.04238185634281724, 0.08397570756472092, -0.10941420305282512, -0.054836248186357475, 0.0654383631066439, 0.4240656057570843, -0.20989713585251904, -0.3458866511887692, 0.1248835771854848, -0.27476888102419833, -0.11777511888996084, 0.2700915980212232, -0.012147289508225476... |
709.2801 | Analogies between analysis on foliated spaces and arithmetic geometry | We point out analogies between (a) the explicit formulas in analytic number
theory and transversal index theory, (b) Lichtenbaum's recent conjectures on
special values of Hasse-Weil zeta functions and a formula for special values of
Ruelle zeta functions, (c) work of Cramer on the zeroes of the Riemann zeta
function ... | math.NT math.DS | we point out analogies between a the explicit formulas in analytic number theory and transversal index theory b lichtenbaums recent conjectures on special values of hasseweil zeta functions and a formula for special values of ruelle zeta functions c work of cramer on the zeroes of the riemann zeta function and a result... | [['we', 'point', 'out', 'analogies', 'between', 'a', 'the', 'explicit', 'formulas', 'in', 'analytic', 'number', 'theory', 'and', 'transversal', 'index', 'theory', 'b', 'lichtenbaums', 'recent', 'conjectures', 'on', 'special', 'values', 'of', 'hasseweil', 'zeta', 'functions', 'and', 'a', 'formula', 'for', 'special', 'va... | [-0.18120458138715054, 0.049717873366634274, -0.12927642588461327, 0.10442817661599045, -0.08005653497424316, -0.10817735411480746, 0.09032316406294492, 0.290033592525023, -0.2129969832127575, -0.22768805437424983, 0.0811307632856452, -0.2642613683975386, -0.22557799717072735, 0.25632353291042487, -0.06042719118489582,... |
709.2802 | The importance of probability interference in social science: rationale
and experiment | Probability interference is a fundamental characteristic of quantum
mechanics. In this paper we attempt to show with the help of some examples,
where this fundamental trait of quantum physics can be found back in a social
science environment. In order to support our thesis that interference can
possibly be found back... | physics.gen-ph | probability interference is a fundamental characteristic of quantum mechanics in this paper we attempt to show with the help of some examples where this fundamental trait of quantum physics can be found back in a social science environment in order to support our thesis that interference can possibly be found back in m... | [['probability', 'interference', 'is', 'a', 'fundamental', 'characteristic', 'of', 'quantum', 'mechanics', 'in', 'this', 'paper', 'we', 'attempt', 'to', 'show', 'with', 'the', 'help', 'of', 'some', 'examples', 'where', 'this', 'fundamental', 'trait', 'of', 'quantum', 'physics', 'can', 'be', 'found', 'back', 'in', 'a', ... | [-0.07881454528614995, 0.13093038382635314, -0.1273398319608532, 0.067682995886571, -0.06915345793095184, -0.1281378008570755, 0.04404306484684639, 0.34533521402045153, -0.3200267244828865, -0.3041762610519072, 0.04449661206854216, -0.24363975995220244, -0.23960845320834778, 0.2023557248758152, -0.1307554526720196, 0.0... |
709.2803 | High-Precision Thermodynamic and Critical Properties from Tensor
Renormalization-Group Flows | The recently developed tensor renormalization-group (TRG) method provides a
highly precise technique for deriving thermodynamic and critical properties of
lattice Hamiltonians. The TRG is a local coarse-graining transformation, with
the elements of the tensor at each lattice site playing the part of the
interactions ... | cond-mat.stat-mech | the recently developed tensor renormalizationgroup trg method provides a highly precise technique for deriving thermodynamic and critical properties of lattice hamiltonians the trg is a local coarsegraining transformation with the elements of the tensor at each lattice site playing the part of the interactions that und... | [['the', 'recently', 'developed', 'tensor', 'renormalizationgroup', 'trg', 'method', 'provides', 'a', 'highly', 'precise', 'technique', 'for', 'deriving', 'thermodynamic', 'and', 'critical', 'properties', 'of', 'lattice', 'hamiltonians', 'the', 'trg', 'is', 'a', 'local', 'coarsegraining', 'transformation', 'with', 'the... | [-0.13551042166798583, 0.16629518879586588, -0.1006377257467943, 0.010531774480893676, -0.04554839299647016, -0.11429695387419264, 0.05050818587641244, 0.3499368620142885, -0.2635881385899016, -0.25791000294825667, 0.08317907671852327, -0.2852664208704872, -0.1178680317500582, 0.18173394489174635, 0.06121715528674291, ... |
709.2804 | The Color Antisymmetric Ghost Propagator and One-Loop Vertex
Renormalization | The color matrix elements of the ghost triangle diagram that appears in the
triple gluon vertex and the ghost-ghost-gluon triangle diagram that appears in
the ghost-gluon-ghost vertex are calculated. The ghost-ghost-gluon triangle
contains a loop consisting of two color diagonal ghosts and one gluon and a
loop consis... | hep-ph hep-lat | the color matrix elements of the ghost triangle diagram that appears in the triple gluon vertex and the ghostghostgluon triangle diagram that appears in the ghostgluonghost vertex are calculated the ghostghostgluon triangle contains a loop consisting of two color diagonal ghosts and one gluon and a loop consisting of t... | [['the', 'color', 'matrix', 'elements', 'of', 'the', 'ghost', 'triangle', 'diagram', 'that', 'appears', 'in', 'the', 'triple', 'gluon', 'vertex', 'and', 'the', 'ghostghostgluon', 'triangle', 'diagram', 'that', 'appears', 'in', 'the', 'ghostgluonghost', 'vertex', 'are', 'calculated', 'the', 'ghostghostgluon', 'triangle'... | [-0.1245153715487483, 0.23441441964864362, -0.14591329567524236, 0.10841308575296818, -0.0857185896291116, -0.13499024015483121, -0.003384620362762795, 0.3718073579677662, -0.17586383750465248, -0.1901696890072767, 0.05400461975490501, -0.2831679146336175, -0.0878657806166556, 0.05271675755394363, -0.01740756841291143,... |
709.2805 | Evidence for Quasar Activity Triggered by Galaxy Mergers in HST
Observations of Dust-reddened Quasars | We present Hubble ACS images of thirteen dust reddened Type-1 quasars
selected from the FIRST/2MASS Red Quasar Survey. These quasars have high
intrinsic luminosities after correction for dust obscuration (-23.5 > M_B >
-26.2 from K-magnitude). The images show strong evidence of recent or ongoing
interaction in eleven... | astro-ph | we present hubble acs images of thirteen dust reddened type1 quasars selected from the first2mass red quasar survey these quasars have high intrinsic luminosities after correction for dust obscuration 235 m_b 262 from kmagnitude the images show strong evidence of recent or ongoing interaction in eleven of the thirteen ... | [['we', 'present', 'hubble', 'acs', 'images', 'of', 'thirteen', 'dust', 'reddened', 'type1', 'quasars', 'selected', 'from', 'the', 'first2mass', 'red', 'quasar', 'survey', 'these', 'quasars', 'have', 'high', 'intrinsic', 'luminosities', 'after', 'correction', 'for', 'dust', 'obscuration', '235', 'm_b', '262', 'from', '... | [-0.03196749780653862, 0.06132237892917035, -0.0696326870503917, 0.12056572525506724, -0.1149177469074187, -0.06764209372672587, 0.05478350368528545, 0.4884310937568284, -0.08595204430738497, -0.3589063968403232, 0.03500357370623469, -0.35321706123323293, -0.0237476265623659, 0.17930627321689635, -0.04820145048168406, ... |
709.2806 | Absolute Momentum Calibration of the HARP TPC | In the HARP experiment the large-angle spectrometer is using a cylindrical
TPC as main tracking and particle identification detector. The momentum scale
of reconstructed tracks in the TPC is the most important systematic error for
the majority of kinematic bins used for the HARP measurements of the
double-differentia... | physics.ins-det | in the harp experiment the largeangle spectrometer is using a cylindrical tpc as main tracking and particle identification detector the momentum scale of reconstructed tracks in the tpc is the most important systematic error for the majority of kinematic bins used for the harp measurements of the doubledifferential pro... | [['in', 'the', 'harp', 'experiment', 'the', 'largeangle', 'spectrometer', 'is', 'using', 'a', 'cylindrical', 'tpc', 'as', 'main', 'tracking', 'and', 'particle', 'identification', 'detector', 'the', 'momentum', 'scale', 'of', 'reconstructed', 'tracks', 'in', 'the', 'tpc', 'is', 'the', 'most', 'important', 'systematic', ... | [-0.05933036129718799, 0.12818182969727276, -0.11668077204955132, 0.053465282932544746, -0.02032186126347348, -0.10879299324652594, -0.0036757041479607948, 0.3524222421236554, -0.19078429693652982, -0.3663345443858215, 0.07422088391259203, -0.3121825548689486, 0.03802706693892765, 0.20337582236885676, -0.03306001245741... |
709.2807 | Observations of VHE gamma-Ray Sources with the MAGIC Telescope | The MAGIC telescope with its 17m diameter mirror is today the largest
operating single-dish Imaging Air Cherenkov Telescope (IACT). It is located on
the Canary Island La Palma, at an altitude of 2200m above sea level, as part of
the Roque de los Muchachos European Northern Observatory. The MAGIC telescope
detects cel... | astro-ph | the magic telescope with its 17m diameter mirror is today the largest operating singledish imaging air cherenkov telescope iact it is located on the canary island la palma at an altitude of 2200m above sea level as part of the roque de los muchachos european northern observatory the magic telescope detects celestial ve... | [['the', 'magic', 'telescope', 'with', 'its', '17m', 'diameter', 'mirror', 'is', 'today', 'the', 'largest', 'operating', 'singledish', 'imaging', 'air', 'cherenkov', 'telescope', 'iact', 'it', 'is', 'located', 'on', 'the', 'canary', 'island', 'la', 'palma', 'at', 'an', 'altitude', 'of', '2200m', 'above', 'sea', 'level'... | [-0.08638896272741405, 0.1984993247299246, -0.03409530979757175, 0.20877182623623564, -0.12695993551999096, -0.09713642479939841, 0.019794126385896223, 0.4177242208228219, -0.1051862524386026, -0.4282092431222829, 0.11940229940136499, -0.35475291608737447, -0.02123522587619194, 0.27726654041059845, -0.03048261655787900... |
709.2808 | Comparison of reduced-order, sequential and variational data
assimilation methods in the tropical Pacific Ocean | This paper presents a comparison of two reduced-order, sequential and
variational data assimilation methods: the SEEK filter and the R-4D-Var. A
hybridization of the two, combining the variational framework and the
sequential evolution of covariance matrices, is also preliminarily investigated
and assessed in the sam... | physics.geo-ph math.AP math.OC | this paper presents a comparison of two reducedorder sequential and variational data assimilation methods the seek filter and the r4dvar a hybridization of the two combining the variational framework and the sequential evolution of covariance matrices is also preliminarily investigated and assessed in the same experime... | [['this', 'paper', 'presents', 'a', 'comparison', 'of', 'two', 'reducedorder', 'sequential', 'and', 'variational', 'data', 'assimilation', 'methods', 'the', 'seek', 'filter', 'and', 'the', 'r4dvar', 'a', 'hybridization', 'of', 'the', 'two', 'combining', 'the', 'variational', 'framework', 'and', 'the', 'sequential', 'ev... | [-0.08445491222517353, 0.047003475589606956, -0.11388673793960692, 0.10805070429139246, -0.03961550794347319, -0.11552153075632604, 0.04147035446787206, 0.35425324445071665, -0.26933843616537656, -0.31266242105077624, 0.12789812554086594, -0.24375345258195472, -0.17555232685872743, 0.2088818449270617, -0.04250859640114... |
709.2809 | Pure Anderson Motives and Abelian \tau-Sheaves | Pure t-motives were introduced by G. Anderson as higher dimensional
generalizations of Drinfeld modules, and as the appropriate analogs of abelian
varieties in the arithmetic of function fields. In order to construct moduli
spaces for pure t-motives the second author has previously introduced the
concept of abelian \... | math.NT math.AG | pure tmotives were introduced by g anderson as higher dimensional generalizations of drinfeld modules and as the appropriate analogs of abelian varieties in the arithmetic of function fields in order to construct moduli spaces for pure tmotives the second author has previously introduced the concept of abelian tausheaf... | [['pure', 'tmotives', 'were', 'introduced', 'by', 'g', 'anderson', 'as', 'higher', 'dimensional', 'generalizations', 'of', 'drinfeld', 'modules', 'and', 'as', 'the', 'appropriate', 'analogs', 'of', 'abelian', 'varieties', 'in', 'the', 'arithmetic', 'of', 'function', 'fields', 'in', 'order', 'to', 'construct', 'moduli',... | [-0.13819853794943218, 0.1144338558877517, -0.1085916344992533, 0.15435959509467584, -0.07014767294142234, -0.0966948848116495, -0.007370997337958492, 0.3239058512566692, -0.31564499539039703, -0.2704314917487943, 0.08515205981498382, -0.1923074781206315, -0.15773111582877944, 0.16230424457108197, -0.17838501030295764,... |
709.281 | Moduli Evolution in the Presence of Matter Fields and Flux
Compactification | We provide a detailed analysis of the dynamics of moduli fields in the KKLT
scenario coupled to a Polonyi field, which plays the role of a hidden matter
sector field. It was previously shown that such matter fields can uplift AdS
vacua to Minkowski or de Sitter vacua. Additionally, we take a background fluid
into acc... | hep-th | we provide a detailed analysis of the dynamics of moduli fields in the kklt scenario coupled to a polonyi field which plays the role of a hidden matter sector field it was previously shown that such matter fields can uplift ads vacua to minkowski or de sitter vacua additionally we take a background fluid into account w... | [['we', 'provide', 'a', 'detailed', 'analysis', 'of', 'the', 'dynamics', 'of', 'moduli', 'fields', 'in', 'the', 'kklt', 'scenario', 'coupled', 'to', 'a', 'polonyi', 'field', 'which', 'plays', 'the', 'role', 'of', 'a', 'hidden', 'matter', 'sector', 'field', 'it', 'was', 'previously', 'shown', 'that', 'such', 'matter', '... | [-0.1714939428134227, 0.1685356370252656, -0.1574976869333694, 0.12008021177941973, -0.11898827437370857, -0.09961434371492013, 0.0074104801652596355, 0.2836631970935838, -0.1919602178473105, -0.3098454725126082, 0.11301843982011556, -0.20179756688315698, -0.17556948603646078, 0.1425943170832668, -0.028886056292128374,... |
709.2811 | How a plantar pressure-based, tongue-placed tactile biofeedback modifies
postural control mechanisms during quiet standing | The purpose of the present study was to determine the effects of a plantar
pressure-based, tongue-placed tactile biofeedback on postural control
mechanisms during quiet standing. To this aim, sixteen young healthy adults
were asked to stand as immobile as possible with their eyes closed in two
conditions of No-biofee... | physics.med-ph q-bio.NC | the purpose of the present study was to determine the effects of a plantar pressurebased tongueplaced tactile biofeedback on postural control mechanisms during quiet standing to this aim sixteen young healthy adults were asked to stand as immobile as possible with their eyes closed in two conditions of nobiofeedback an... | [['the', 'purpose', 'of', 'the', 'present', 'study', 'was', 'to', 'determine', 'the', 'effects', 'of', 'a', 'plantar', 'pressurebased', 'tongueplaced', 'tactile', 'biofeedback', 'on', 'postural', 'control', 'mechanisms', 'during', 'quiet', 'standing', 'to', 'this', 'aim', 'sixteen', 'young', 'healthy', 'adults', 'were'... | [-0.10099510840119276, 0.14044076738333333, -0.07594393782625745, 0.00812148829375891, -0.0678241377384787, -0.1197848852856883, 0.0452499455471236, 0.37219205162578956, -0.24148044015343925, -0.3419345958592524, 0.09344749793294761, -0.24636744717276074, -0.14216866974956952, 0.18275194476477633, -0.13908149720750806,... |
709.2812 | Infraparticle Scattering States in Non-Relativistic QED: II. Mass Shell
Properties | We study the infrared problem in the usual model of QED with non-relativistic
matter. We prove spectral and regularity properties characterizing the mass
shell of an electron and one-electron infraparticle states of this model. Our
results are crucial for the construction of infraparticle scattering states,
which are... | math-ph math.MP | we study the infrared problem in the usual model of qed with nonrelativistic matter we prove spectral and regularity properties characterizing the mass shell of an electron and oneelectron infraparticle states of this model our results are crucial for the construction of infraparticle scattering states which are treate... | [['we', 'study', 'the', 'infrared', 'problem', 'in', 'the', 'usual', 'model', 'of', 'qed', 'with', 'nonrelativistic', 'matter', 'we', 'prove', 'spectral', 'and', 'regularity', 'properties', 'characterizing', 'the', 'mass', 'shell', 'of', 'an', 'electron', 'and', 'oneelectron', 'infraparticle', 'states', 'of', 'this', '... | [-0.07582227251707362, 0.1311444477024242, -0.08074677986307786, 0.08578798218513839, 0.041467476600351244, -0.0792689421841015, -0.020602508714476313, 0.34227399649814916, -0.21048720080692035, -0.27880876355965695, 0.02387281893662965, -0.2769947197789756, -0.10703725109879787, 0.1421696051928358, -0.0213335835768912... |
709.2813 | LDPC codes from Singer cycles | The main goal of coding theory is to devise efficient systems to exploit the
full capacity of a communication channel, thus achieving an arbitrarily small
error probability. Low Density Parity Check (LDPC) codes are a family of block
codes--characterised by admitting a sparse parity check matrix--with good
correction... | cs.IT math.IT | the main goal of coding theory is to devise efficient systems to exploit the full capacity of a communication channel thus achieving an arbitrarily small error probability low density parity check ldpc codes are a family of block codescharacterised by admitting a sparse parity check matrixwith good correction capabilit... | [['the', 'main', 'goal', 'of', 'coding', 'theory', 'is', 'to', 'devise', 'efficient', 'systems', 'to', 'exploit', 'the', 'full', 'capacity', 'of', 'a', 'communication', 'channel', 'thus', 'achieving', 'an', 'arbitrarily', 'small', 'error', 'probability', 'low', 'density', 'parity', 'check', 'ldpc', 'codes', 'are', 'a',... | [-0.25916312950109877, 0.07457239650703622, -0.06389838457782415, 0.07854000747750473, -0.003738734128790489, -0.21653648921410026, 0.0872296627064276, 0.3478914050358361, -0.26348441227784625, -0.25820214877687936, 0.13124490664441787, -0.1970510699354328, -0.12820453978602545, 0.13877417607421894, -0.1530050900098327... |
709.2814 | Reduced-order 4D-Var: a preconditioner for the Incremental 4D-Var data
assimilation method | This study demonstrates how the incremental 4D-Var data assimilation method
can be applied efficiently preconditione d in an application to an
oceanographic problem. The approach consists in performing a few iterations of
the reduced-order 4D-Var prior to the incremental 4D-Var in the full space in
order to achieve f... | physics.geo-ph math.AP math.OC | this study demonstrates how the incremental 4dvar data assimilation method can be applied efficiently preconditione d in an application to an oceanographic problem the approach consists in performing a few iterations of the reducedorder 4dvar prior to the incremental 4dvar in the full space in order to achieve faster c... | [['this', 'study', 'demonstrates', 'how', 'the', 'incremental', '4dvar', 'data', 'assimilation', 'method', 'can', 'be', 'applied', 'efficiently', 'preconditione', 'd', 'in', 'an', 'application', 'to', 'an', 'oceanographic', 'problem', 'the', 'approach', 'consists', 'in', 'performing', 'a', 'few', 'iterations', 'of', 't... | [-0.0552114263274952, 0.0036994018339196614, -0.09905544185863906, 0.03871662309760914, -0.049726538546383384, -0.05665067676944952, 0.05098024746893268, 0.34411762188139716, -0.3183855808683132, -0.33727826698634183, 0.171570155219371, -0.2088640801144433, -0.11106834073894117, 0.21918714344746582, -0.1101512686790604... |
709.2815 | Pure Anderson Motives over Finite Fields | In the arithmetic of function fields Drinfeld modules play the role that
elliptic curves take on in the arithmetic of number fields. As higher
dimensional generalizations of Drinfeld modules, and as the appropriate
analogues of abelian varieties, G. Anderson introduced pure t-motives. In this
article we study the ari... | math.NT math.AG | in the arithmetic of function fields drinfeld modules play the role that elliptic curves take on in the arithmetic of number fields as higher dimensional generalizations of drinfeld modules and as the appropriate analogues of abelian varieties g anderson introduced pure tmotives in this article we study the arithmetic ... | [['in', 'the', 'arithmetic', 'of', 'function', 'fields', 'drinfeld', 'modules', 'play', 'the', 'role', 'that', 'elliptic', 'curves', 'take', 'on', 'in', 'the', 'arithmetic', 'of', 'number', 'fields', 'as', 'higher', 'dimensional', 'generalizations', 'of', 'drinfeld', 'modules', 'and', 'as', 'the', 'appropriate', 'analo... | [-0.16804651843600743, 0.08142776351478946, -0.11547838709004338, 0.12981437216335126, -0.10160342078542209, -0.13389870644554155, -0.030107144899097563, 0.33484753093305436, -0.3026761056585166, -0.21360189741022373, 0.11514903310391313, -0.20082288706596968, -0.1327784271512664, 0.24572411224331336, -0.16711271170327... |
709.2816 | Non-equilibrium emission of complex fragments from p+Au collisions at
2.5 GeV proton beam energy | Energy and angular dependence of double differential cross sections
d$^2\sigma$/d$\Omega$dE was measured for reactions induced by 2.5 GeV protons
on Au target with isotopic identification of light products (H, He, Li, Be, and
B) and with elemental identification of heavier intermediate mass fragments (C,
N, O, F, Ne,... | nucl-ex | energy and angular dependence of double differential cross sections d2sigmadomegade was measured for reactions induced by 25 gev protons on au target with isotopic identification of light products h he li be and b and with elemental identification of heavier intermediate mass fragments c n o f ne na mg and al it was fo... | [['energy', 'and', 'angular', 'dependence', 'of', 'double', 'differential', 'cross', 'sections', 'd2sigmadomegade', 'was', 'measured', 'for', 'reactions', 'induced', 'by', '25', 'gev', 'protons', 'on', 'au', 'target', 'with', 'isotopic', 'identification', 'of', 'light', 'products', 'h', 'he', 'li', 'be', 'and', 'b', 'a... | [-0.057954311011490345, 0.2477923663107532, -0.06956082845273479, 0.09704449379270083, 0.032365543561049065, -0.11382253987702962, -0.014949111089593115, 0.3151043088473811, -0.21243267400463517, -0.35094514475509697, -0.07588399583464812, -0.3654944635064676, 0.062471539139905836, 0.14787004441634166, 0.07976560930192... |
709.2817 | FCNC $B_s$ and $\Lambda_b$ transitions: Standard Model versus a single
Universal Extra Dimension scenario | We study the FCNC $B_s \to \phi \gamma, \phi \nu \bar \nu$ and $\Lambda_b \to
\Lambda \gamma, \Lambda \nu \bar \nu$ transitions in the Standard Model and in
a scenario with a single Universal Extra Dimension. In particular, we focus on
the present knowledge of the hadronic uncertainties and on possible
improvements. ... | hep-ph | we study the fcnc b_s to phi gamma phi nu bar nu and lambda_b to lambda gamma lambda nu bar nu transitions in the standard model and in a scenario with a single universal extra dimension in particular we focus on the present knowledge of the hadronic uncertainties and on possible improvements we discuss how the measure... | [['we', 'study', 'the', 'fcnc', 'b_s', 'to', 'phi', 'gamma', 'phi', 'nu', 'bar', 'nu', 'and', 'lambda_b', 'to', 'lambda', 'gamma', 'lambda', 'nu', 'bar', 'nu', 'transitions', 'in', 'the', 'standard', 'model', 'and', 'in', 'a', 'scenario', 'with', 'a', 'single', 'universal', 'extra', 'dimension', 'in', 'particular', 'we... | [-0.11258298887229823, 0.19649855359369572, -0.031532845156759304, 0.06492115755758758, -0.07556370106297282, -0.15235274502093782, 0.0909295634592813, 0.2938001069398421, -0.264007938358019, -0.24038799956686935, 0.028179042498176952, -0.2894677144457709, -0.039549490243618216, 0.15258548741958122, 0.04213639916105301... |
709.2818 | Lepton Flavour Violation at the ILC | We explore the possibility of detecting lepton flavour violation, now a well
established experimental fact, at the International Linear Collider. Using a
model independent approach we conclude that, given all experimental constraints
available, there is still room to detect lepton flavour violation at the ILC.
| hep-ph | we explore the possibility of detecting lepton flavour violation now a well established experimental fact at the international linear collider using a model independent approach we conclude that given all experimental constraints available there is still room to detect lepton flavour violation at the ilc | [['we', 'explore', 'the', 'possibility', 'of', 'detecting', 'lepton', 'flavour', 'violation', 'now', 'a', 'well', 'established', 'experimental', 'fact', 'at', 'the', 'international', 'linear', 'collider', 'using', 'a', 'model', 'independent', 'approach', 'we', 'conclude', 'that', 'given', 'all', 'experimental', 'constr... | [-0.09512574012042023, 0.1984911199245188, -0.010747581492695543, 0.1380953332849054, -0.11015804963600305, -0.23201046764022773, 0.10176947216192882, 0.3045256712370449, -0.2547804488076104, -0.2916538503434923, 0.06474857034368647, -0.32679903250601555, -0.027902590648995505, 0.1475812018693735, 0.08889026052008073, ... |
709.2819 | A New Supersensitive Flame Detector and its Use for Early Forest Fire
Detection | A new flame detector, three orders of magnitude more powerful than the
existing ones, is presented. This detector needs to be mass-produced for its
use in order to be incorporated in an early forest fire detection system. A
project able to implement its use to overcome the forest fire emergency is
described.
| physics.ins-det | a new flame detector three orders of magnitude more powerful than the existing ones is presented this detector needs to be massproduced for its use in order to be incorporated in an early forest fire detection system a project able to implement its use to overcome the forest fire emergency is described | [['a', 'new', 'flame', 'detector', 'three', 'orders', 'of', 'magnitude', 'more', 'powerful', 'than', 'the', 'existing', 'ones', 'is', 'presented', 'this', 'detector', 'needs', 'to', 'be', 'massproduced', 'for', 'its', 'use', 'in', 'order', 'to', 'be', 'incorporated', 'in', 'an', 'early', 'forest', 'fire', 'detection', ... | [-0.020117481783157788, 0.0510693830373594, -0.06406298427744052, 0.07829081556589629, -0.111828094921433, -0.14402601749707872, -0.00830543001827139, 0.37979338146173036, -0.21179444915077722, -0.2963125576408437, 0.16876669748811624, -0.32103959743220073, -0.09455590190191288, 0.22334322140802845, -0.0892616993873021... |
709.282 | On the behaviour of B and Be stars at low metallicity | We present new results obtained with the VLT GIRAFFE for a large sample of B
and Be stars belonging to the Magellanic Clouds, i.e. at low metallicity.
First, we show the effects of the metallicity of the environment on their
rotation (linear, angular, and at the ZAMS). Second, we present the analysis of
the effects o... | astro-ph | we present new results obtained with the vlt giraffe for a large sample of b and be stars belonging to the magellanic clouds ie at low metallicity first we show the effects of the metallicity of the environment on their rotation linear angular and at the zams second we present the analysis of the effects of metallicity... | [['we', 'present', 'new', 'results', 'obtained', 'with', 'the', 'vlt', 'giraffe', 'for', 'a', 'large', 'sample', 'of', 'b', 'and', 'be', 'stars', 'belonging', 'to', 'the', 'magellanic', 'clouds', 'ie', 'at', 'low', 'metallicity', 'first', 'we', 'show', 'the', 'effects', 'of', 'the', 'metallicity', 'of', 'the', 'environ... | [-0.07940034141453604, 0.11937582511454821, -0.07946383933962124, 0.04262091036168082, -0.09739203171532912, -0.002879035919128607, 0.10400634850957431, 0.3774416121576602, -0.20630503354089644, -0.3571550511134168, 0.07836235177722604, -0.2787876238425573, -0.04340961118383954, 0.21348571962832164, -0.0714762555115157... |
709.2821 | A priori bounds and a Liouville theorem on a half-space for higher order
elliptic Dirichlet problems | We consider the $2m$-th order elliptic boundary value problem $Lu=f(x,u)$ on
a bounded smooth domain $\Omega$ in $R^N$ with Dirichlet boundary conditions.
The operator $L$ is a uniformly elliptic operator of order $2m$. We assume that
for $s\to \pm\infty$ the nonlinearity $f(x,s)$ behaves like $|s|^q$ multiplied
by a... | math.AP | we consider the 2mth order elliptic boundary value problem lufxu on a bounded smooth domain omega in rn with dirichlet boundary conditions the operator l is a uniformly elliptic operator of order 2m we assume that for sto pminfty the nonlinearity fxs behaves like sq multiplied by a continuous and positive function of x... | [['we', 'consider', 'the', '2mth', 'order', 'elliptic', 'boundary', 'value', 'problem', 'lufxu', 'on', 'a', 'bounded', 'smooth', 'domain', 'omega', 'in', 'rn', 'with', 'dirichlet', 'boundary', 'conditions', 'the', 'operator', 'l', 'is', 'a', 'uniformly', 'elliptic', 'operator', 'of', 'order', '2m', 'we', 'assume', 'tha... | [-0.21373828070668074, 0.11904300406080234, -0.05832827901728191, -0.0018120314160661472, -0.12070916026343846, -0.22482566570316057, 0.020518297861147856, 0.2951146839642441, -0.33182063985655047, -0.1175759190276682, 0.17275683944181935, -0.337626480621162, -0.08519604424555245, 0.15948513759726698, -0.06603156092211... |
709.2822 | Soliton Stability in a Generalized Sine-Gordon Potential | We study stability of a generalized sine-Gordon model with two coupled scalar
fields in two dimensions. Topological soliton solutions are found from the
first-order equations that solve the equations of motion. The perturbation
equations can be cast in terms of a Schrodinger-like operators for fluctuations
and their ... | hep-th | we study stability of a generalized sinegordon model with two coupled scalar fields in two dimensions topological soliton solutions are found from the firstorder equations that solve the equations of motion the perturbation equations can be cast in terms of a schrodingerlike operators for fluctuations and their spectra... | [['we', 'study', 'stability', 'of', 'a', 'generalized', 'sinegordon', 'model', 'with', 'two', 'coupled', 'scalar', 'fields', 'in', 'two', 'dimensions', 'topological', 'soliton', 'solutions', 'are', 'found', 'from', 'the', 'firstorder', 'equations', 'that', 'solve', 'the', 'equations', 'of', 'motion', 'the', 'perturbati... | [-0.1848962762951851, 0.14163011648692192, -0.09566568685695528, 0.08371488561853767, -0.050764027093537153, -0.13147273868322373, -0.11258583873510361, 0.26954736264422535, -0.25830521788448096, -0.25681809693574903, 0.10800451782066375, -0.3341123214550316, -0.1665665646828711, 0.1564427358424291, 0.03191746946424246... |
709.2823 | On the nature of early-type emission line objects in NGC6611 | The number and the nature of emission line stars in the young open cluster
NGC6611 is still the object of debates. Due to the presence of a strong and
variable nebulosity in the cluster, the number of emission line stars is highly
depending on the technique and the resolution used for the observations. Thanks
to obse... | astro-ph | the number and the nature of emission line stars in the young open cluster ngc6611 is still the object of debates due to the presence of a strong and variable nebulosity in the cluster the number of emission line stars is highly depending on the technique and the resolution used for the observations thanks to observati... | [['the', 'number', 'and', 'the', 'nature', 'of', 'emission', 'line', 'stars', 'in', 'the', 'young', 'open', 'cluster', 'ngc6611', 'is', 'still', 'the', 'object', 'of', 'debates', 'due', 'to', 'the', 'presence', 'of', 'a', 'strong', 'and', 'variable', 'nebulosity', 'in', 'the', 'cluster', 'the', 'number', 'of', 'emissio... | [-0.057294664760456256, 0.06802674351720926, -0.05377109789471958, 0.05158996945319064, -0.14988630226592428, -0.04756410334969765, 0.07320597885925438, 0.45094789414829817, -0.17804467089752637, -0.35751499790583074, 0.10740364658929523, -0.2696450843293335, -0.018257752161703465, 0.16805003181138298, -0.0628662921545... |
709.2824 | Pseudo-Random Fluctuations, Stochastic Cooperativity and Burstiness in
Dynamically Unstable High-Dimensional Biochemical Networks | The goal of this paper is to outline a scenario of emerging stochasticity in
high-dimensional highly nonlinear systems, such as genetic regulatory networks
(GRN). We focus attention on the fact that in such systems confluence of all
the factors necessary for gene expression is a comparatively rare event, and
only mas... | q-bio.MN q-bio.GN | the goal of this paper is to outline a scenario of emerging stochasticity in highdimensional highly nonlinear systems such as genetic regulatory networks grn we focus attention on the fact that in such systems confluence of all the factors necessary for gene expression is a comparatively rare event and only massive red... | [['the', 'goal', 'of', 'this', 'paper', 'is', 'to', 'outline', 'a', 'scenario', 'of', 'emerging', 'stochasticity', 'in', 'highdimensional', 'highly', 'nonlinear', 'systems', 'such', 'as', 'genetic', 'regulatory', 'networks', 'grn', 'we', 'focus', 'attention', 'on', 'the', 'fact', 'that', 'in', 'such', 'systems', 'confl... | [-0.18263655185106803, 0.11690398080410722, -0.02999114439695735, 0.12039475922757364, -0.057738668599631636, -0.11871492125527848, 0.01809574145061726, 0.3197457670234144, -0.3052464011971923, -0.2577953826001083, 0.07492663931651887, -0.2361307019590723, -0.2502893650459803, 0.19083824110302058, -0.09930428492794321,... |
709.2825 | A reduced-order strategy for 4D-Var data assimilation | This paper presents a reduced-order approach for four-dimensional variational
data assimilation, based on a prior EO F analysis of a model trajectory. This
method implies two main advantages: a natural model-based definition of a mul
tivariate background error covariance matrix $\textbf{B}_r$, and an important
decrea... | physics.geo-ph math.AP math.OC | this paper presents a reducedorder approach for fourdimensional variational data assimilation based on a prior eo f analysis of a model trajectory this method implies two main advantages a natural modelbased definition of a mul tivariate background error covariance matrix textbfb_r and an important decrease of the comp... | [['this', 'paper', 'presents', 'a', 'reducedorder', 'approach', 'for', 'fourdimensional', 'variational', 'data', 'assimilation', 'based', 'on', 'a', 'prior', 'eo', 'f', 'analysis', 'of', 'a', 'model', 'trajectory', 'this', 'method', 'implies', 'two', 'main', 'advantages', 'a', 'natural', 'modelbased', 'definition', 'of... | [-0.07181005504469967, 0.021778434605060848, -0.09230318530756013, 0.022887944059600453, -0.06900752196821758, -0.08422063254406602, 0.05563754281927428, 0.31004632067844623, -0.2629402283007118, -0.3391564688461972, 0.11204328244885679, -0.2300190916944911, -0.1776503745473804, 0.210869282157725, -0.12825726971440898,... |
709.2826 | Sudakov resummation in QCD | In this PhD thesis, we analyze and generalize the renormalization group
approach to the resummation of large logarithms in the perturbative expansion
due to soft and collinear multiparton emissions. In particular, we present a
generalization of this approach to prompt photon production. It is interesting
to see that ... | hep-ph | in this phd thesis we analyze and generalize the renormalization group approach to the resummation of large logarithms in the perturbative expansion due to soft and collinear multiparton emissions in particular we present a generalization of this approach to prompt photon production it is interesting to see that also w... | [['in', 'this', 'phd', 'thesis', 'we', 'analyze', 'and', 'generalize', 'the', 'renormalization', 'group', 'approach', 'to', 'the', 'resummation', 'of', 'large', 'logarithms', 'in', 'the', 'perturbative', 'expansion', 'due', 'to', 'soft', 'and', 'collinear', 'multiparton', 'emissions', 'in', 'particular', 'we', 'present... | [-0.03998118192751967, 0.12296438840543686, -0.15956337300628, 0.15260737532445218, -0.08533461468395781, -0.08102171093013615, 0.02886270926738383, 0.3976955445896022, -0.1923817500408068, -0.2607469387039083, 0.02196377552627813, -0.3131538631838098, -0.08005472301765923, 0.17100937254668955, -0.03125484292456104, 0.... |
709.2827 | An analytically solvable model of the effect of magnetic breakdown on
angle-dependent magnetoresistance in a quasi-two-dimensional metal | We have developed an analytical model of angle-dependent magnetoresistance
oscillations (AMROs) in a quasi-two-dimensional metal in which magnetic
breakdown occurs. The model takes account of all the contributions from
quasiparticles undergoing both magnetic breakdown and Bragg reflection at each
junction and allows ... | cond-mat.str-el | we have developed an analytical model of angledependent magnetoresistance oscillations amros in a quasitwodimensional metal in which magnetic breakdown occurs the model takes account of all the contributions from quasiparticles undergoing both magnetic breakdown and bragg reflection at each junction and allows extremel... | [['we', 'have', 'developed', 'an', 'analytical', 'model', 'of', 'angledependent', 'magnetoresistance', 'oscillations', 'amros', 'in', 'a', 'quasitwodimensional', 'metal', 'in', 'which', 'magnetic', 'breakdown', 'occurs', 'the', 'model', 'takes', 'account', 'of', 'all', 'the', 'contributions', 'from', 'quasiparticles', ... | [-0.13764322493439432, 0.1705168263958941, -0.07013710582329111, 0.021882430655646257, -0.03847606189752362, -0.147974730089264, 0.04875023719244476, 0.3641768321314634, -0.21940998302708412, -0.33243489667944526, 0.03095403951512457, -0.28670803986602844, -0.1406822481310402, 0.22888453591925403, 0.01822712881511998, ... |
709.2828 | Microlensing variability in the gravitationally lensed quasar Q2237+0305
= the Einstein Cross, I. Spectrophotometric monitoring with the VLT | We present the results of the first long-term (2.2 years) spectroscopic
monitoring of a gravitationally lensed quasar, namely the Einstein Cross
Q2237+0305. The goal of this paper is to present the observational facts to be
compared in follow-up papers with theoretical models to constrain the inner
structure of the s... | astro-ph | we present the results of the first longterm 22 years spectroscopic monitoring of a gravitationally lensed quasar namely the einstein cross q22370305 the goal of this paper is to present the observational facts to be compared in followup papers with theoretical models to constrain the inner structure of the source quas... | [['we', 'present', 'the', 'results', 'of', 'the', 'first', 'longterm', '22', 'years', 'spectroscopic', 'monitoring', 'of', 'a', 'gravitationally', 'lensed', 'quasar', 'namely', 'the', 'einstein', 'cross', 'q22370305', 'the', 'goal', 'of', 'this', 'paper', 'is', 'to', 'present', 'the', 'observational', 'facts', 'to', 'b... | [-0.040934563369343153, 0.03724847615235934, -0.05151699003518412, 0.06465336382225678, -0.07601471929892636, -0.0903290268695472, 0.0005673663351652131, 0.4638262286782265, -0.14035172128126744, -0.3348243579105066, 0.05697801894990302, -0.34289581398561336, -0.03798845196867835, 0.19583887097899588, -0.04986300182103... |
709.2829 | Theory of biphoton generation in a single-resonant optical parametric
oscillator far below threshold | We present a quantum-theoretical treatment of biphoton generation in
single-resonant type-II parametric down-conversion. The nonlinear medium is
continuously pumped and is placed inside a cavity which is resonant for the
signal field, but nonresonant for the idler deflected by an intra-cavity
polarizing beam splitter... | quant-ph | we present a quantumtheoretical treatment of biphoton generation in singleresonant typeii parametric downconversion the nonlinear medium is continuously pumped and is placed inside a cavity which is resonant for the signal field but nonresonant for the idler deflected by an intracavity polarizing beam splitter the inte... | [['we', 'present', 'a', 'quantumtheoretical', 'treatment', 'of', 'biphoton', 'generation', 'in', 'singleresonant', 'typeii', 'parametric', 'downconversion', 'the', 'nonlinear', 'medium', 'is', 'continuously', 'pumped', 'and', 'is', 'placed', 'inside', 'a', 'cavity', 'which', 'is', 'resonant', 'for', 'the', 'signal', 'f... | [-0.15136771439651756, 0.20773722838993194, -0.06496751374127158, 0.03709076434861104, -0.04499192007613794, -0.14758932090592602, 0.009452531620742914, 0.44624261893578715, -0.2506001317096467, -0.2563533292491982, 0.029125416967462722, -0.26196677053026507, -0.046747713540958254, 0.23793024868883242, 0.02413645712967... |
709.283 | Behavioral Portfolio Selection in Continuous Time | This paper formulates and studies a general continuous-time behavioral
portfolio selection model under Kahneman and Tversky's (cumulative) prospect
theory, featuring S-shaped utility (value) functions and probability
distortions. Unlike the conventional expected utility maximization model, such
a behavioral model cou... | q-fin.PM math.OC math.PR | this paper formulates and studies a general continuoustime behavioral portfolio selection model under kahneman and tverskys cumulative prospect theory featuring sshaped utility value functions and probability distortions unlike the conventional expected utility maximization model such a behavioral model could be easily... | [['this', 'paper', 'formulates', 'and', 'studies', 'a', 'general', 'continuoustime', 'behavioral', 'portfolio', 'selection', 'model', 'under', 'kahneman', 'and', 'tverskys', 'cumulative', 'prospect', 'theory', 'featuring', 'sshaped', 'utility', 'value', 'functions', 'and', 'probability', 'distortions', 'unlike', 'the',... | [-0.08293024504776386, 0.017586550734396203, -0.09550598453565994, 0.13614133398651201, -0.11418371995198814, -0.20134143331464763, 0.08185326526598895, 0.3932974380057524, -0.2925327700453208, -0.25330521100036363, 0.11716655003153445, -0.24756305846385657, -0.1812960872097927, 0.1911385898464633, -0.1262868524515344,... |
709.2831 | Triangulating the Real Projective Plane | We consider the problem of computing a triangulation of the real projective
plane P2, given a finite point set S={p1, p2,..., pn} as input. We prove that a
triangulation of P2 always exists if at least six points in S are in general
position, i.e., no three of them are collinear. We also design an algorithm for
trian... | cs.CG | we consider the problem of computing a triangulation of the real projective plane p2 given a finite point set sp1 p2 pn as input we prove that a triangulation of p2 always exists if at least six points in s are in general position ie no three of them are collinear we also design an algorithm for triangulating p2 if thi... | [['we', 'consider', 'the', 'problem', 'of', 'computing', 'a', 'triangulation', 'of', 'the', 'real', 'projective', 'plane', 'p2', 'given', 'a', 'finite', 'point', 'set', 'sp1', 'p2', 'pn', 'as', 'input', 'we', 'prove', 'that', 'a', 'triangulation', 'of', 'p2', 'always', 'exists', 'if', 'at', 'least', 'six', 'points', 'i... | [-0.21337772209662945, 0.04752012855187786, -0.05604221704998054, 0.06761693403095706, -0.06038869590265676, -0.16274920849245972, 0.01592709141841624, 0.39008853686973455, -0.2819274232722819, -0.21184187796898185, 0.10737494889472146, -0.27346224563661964, -0.1635675999801606, 0.20400640816660598, -0.0822969470973475... |
709.2832 | The Lyapunov spectrum of some parabolic systems | We study the Hausdorff dimension spectrum for Lyapunov exponents for a class
of interval maps which includes several non-hyperbolic situations. We also
analyze the level sets of points with given lower and upper Lyapunov exponents
and, in particular, with zero lower Lyapunov exponent. We prove that the level
set of p... | math.DS | we study the hausdorff dimension spectrum for lyapunov exponents for a class of interval maps which includes several nonhyperbolic situations we also analyze the level sets of points with given lower and upper lyapunov exponents and in particular with zero lower lyapunov exponent we prove that the level set of points w... | [['we', 'study', 'the', 'hausdorff', 'dimension', 'spectrum', 'for', 'lyapunov', 'exponents', 'for', 'a', 'class', 'of', 'interval', 'maps', 'which', 'includes', 'several', 'nonhyperbolic', 'situations', 'we', 'also', 'analyze', 'the', 'level', 'sets', 'of', 'points', 'with', 'given', 'lower', 'and', 'upper', 'lyapunov... | [-0.2096904297396245, 0.12768332694198878, -0.10815622092091612, 0.10650326917687106, 0.005115431931150693, -0.18663715537903564, 0.1261045690330248, 0.2750606187138825, -0.230051840463328, -0.14819241134035918, 0.11049015617685481, -0.3505602884032423, -0.1629114807952964, 0.27522370715936023, -0.04781216017842766, 0.... |
709.2833 | Distributed Space Time Codes with Low Decoding Complexity for
Asynchronous Relay Networks | Recently Li and Xia have proposed a transmission scheme for wireless relay
networks based on the Alamouti space time code and orthogonal frequency
division multiplexing to combat the effect of timing errors at the relay nodes.
This transmission scheme is amazingly simple and achieves a diversity order of
two for any ... | cs.IT math.IT | recently li and xia have proposed a transmission scheme for wireless relay networks based on the alamouti space time code and orthogonal frequency division multiplexing to combat the effect of timing errors at the relay nodes this transmission scheme is amazingly simple and achieves a diversity order of two for any num... | [['recently', 'li', 'and', 'xia', 'have', 'proposed', 'a', 'transmission', 'scheme', 'for', 'wireless', 'relay', 'networks', 'based', 'on', 'the', 'alamouti', 'space', 'time', 'code', 'and', 'orthogonal', 'frequency', 'division', 'multiplexing', 'to', 'combat', 'the', 'effect', 'of', 'timing', 'errors', 'at', 'the', 'r... | [-0.24310709649148296, 0.02346471038826806, -0.056416763306254204, -0.000879914054328963, -0.07838755008294293, -0.2819152836236033, 0.10429840506340313, 0.43885280009322236, -0.28574004433219236, -0.25100127520445403, 0.09976649434261928, -0.2061773941686174, -0.18327793483115215, 0.17330366488785878, -0.1107154362062... |
709.2834 | Physics of EtaPrime->Pi+Pi-Eta and EtaPrime->Pi+Pi-Pi0 decays | The article describes experimental status of EtaPrime->Pi+Pi-Eta and
EtaPrime->Pi+Pi-Pi0 decays. A theoretical framework used for description of the
decays mechanism is also reviewed. The possibilities for the measurements with
WASA-at-COSY are mentioned.
| nucl-ex hep-ex | the article describes experimental status of etaprimepipieta and etaprimepipipi0 decays a theoretical framework used for description of the decays mechanism is also reviewed the possibilities for the measurements with wasaatcosy are mentioned | [['the', 'article', 'describes', 'experimental', 'status', 'of', 'etaprimepipieta', 'and', 'etaprimepipipi0', 'decays', 'a', 'theoretical', 'framework', 'used', 'for', 'description', 'of', 'the', 'decays', 'mechanism', 'is', 'also', 'reviewed', 'the', 'possibilities', 'for', 'the', 'measurements', 'with', 'wasaatcosy',... | [-0.046880776171262066, 0.18994389375050863, -0.06598878183867782, 0.0799695021356456, -0.06198565978556871, -0.13422763482667505, 0.050484008194568254, 0.2834372182066242, -0.2104415112019827, -0.25918429580827557, 0.03982103765010834, -0.3497711496427655, -0.09103106493130327, 0.25341687941302854, 0.02585467879349986... |
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