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708.1449 | Slow beams of massive molecules | Slow beams of neutral molecules are of great interest for a wide range of
applications, from cold chemistry through precision measurements to tests of
the foundations of quantum mechanics. We report on the quantitative observation
of thermal beams of perfluorinated macromolecules with masses up to 6000 amu,
reaching ... | quant-ph physics.atm-clus physics.bio-ph physics.chem-ph | slow beams of neutral molecules are of great interest for a wide range of applications from cold chemistry through precision measurements to tests of the foundations of quantum mechanics we report on the quantitative observation of thermal beams of perfluorinated macromolecules with masses up to 6000 amu reaching veloc... | [['slow', 'beams', 'of', 'neutral', 'molecules', 'are', 'of', 'great', 'interest', 'for', 'a', 'wide', 'range', 'of', 'applications', 'from', 'cold', 'chemistry', 'through', 'precision', 'measurements', 'to', 'tests', 'of', 'the', 'foundations', 'of', 'quantum', 'mechanics', 'we', 'report', 'on', 'the', 'quantitative',... | [-0.0723661156115378, 0.20935572039049405, -0.021358657881597076, -0.01661571176277453, 0.0027159544854209973, -0.11286976731863323, 0.07574653438967908, 0.41157586743625313, -0.22853925891711815, -0.35948767027930245, 0.05484472322507997, -0.2507550429122952, -0.0034284508265145534, 0.2791075274900912, 0.0003585086797... |
708.145 | Pi-Molecular dielectric layer for organic thin film diode | Very thin (1.2-2.5nm) self-assembled organic dielectric monolayers have been
integrated into organic thin-film diode to achieve electrical characteristics.
These dielectrics are fabricated by self-assembling deposition, resulting in
smooth, strongly adherent, thermally stable, organosiloxane thin films having
interes... | cond-mat.mtrl-sci | very thin 1225nm selfassembled organic dielectric monolayers have been integrated into organic thinfilm diode to achieve electrical characteristics these dielectrics are fabricated by selfassembling deposition resulting in smooth strongly adherent thermally stable organosiloxane thin films having interesting electrical... | [['very', 'thin', '1225nm', 'selfassembled', 'organic', 'dielectric', 'monolayers', 'have', 'been', 'integrated', 'into', 'organic', 'thinfilm', 'diode', 'to', 'achieve', 'electrical', 'characteristics', 'these', 'dielectrics', 'are', 'fabricated', 'by', 'selfassembling', 'deposition', 'resulting', 'in', 'smooth', 'str... | [-0.12216921140524474, 0.2245890046046539, 0.04373342198404399, -0.12805351559072733, 0.049228431828404695, -0.25762627162885937, 0.04408638012510809, 0.5291635209863836, -0.17782117870043623, -0.34858135448938066, 0.021329090928404845, -0.3653654651885683, -0.027719644016840243, 0.22389700731093234, -0.001113207147202... |
708.1451 | Minimal E_6 Supersymmetric Standard Model | We propose a Minimal E_6 Supersymmetric Standard Model (ME$_6$SSM) which
allows Planck scale unification, provides a solution to the $\mu$ problem and
predicts a new Z'. Above the conventional GUT scale $M_{GUT}\sim 10^{16}$ GeV
the gauge group corresponds to a left-right symmetric Supersymmetric Pati-Salam
model, to... | hep-ph | we propose a minimal e_6 supersymmetric standard model me_6ssm which allows planck scale unification provides a solution to the mu problem and predicts a new z above the conventional gut scale m_gutsim 1016 gev the gauge group corresponds to a leftright symmetric supersymmetric patisalam model together with an addition... | [['we', 'propose', 'a', 'minimal', 'e_6', 'supersymmetric', 'standard', 'model', 'me_6ssm', 'which', 'allows', 'planck', 'scale', 'unification', 'provides', 'a', 'solution', 'to', 'the', 'mu', 'problem', 'and', 'predicts', 'a', 'new', 'z', 'above', 'the', 'conventional', 'gut', 'scale', 'm_gutsim', '1016', 'gev', 'the'... | [-0.13581107035608272, 0.262503115218061, -0.0399175935856782, 0.15468037050585196, -0.13716070707111308, -0.20541335605894742, 0.007335326742326868, 0.3249288480863839, -0.23900509374958556, -0.311210839793194, 0.0523113389381383, -0.2262523448774026, -0.03337448497262338, 0.0680639458756111, -0.009812116577370984, -0... |
708.1452 | Holding Dissapearance in RTD-based Quantizers | Multiple-valued Logic (MVL) circuits are one of the most attractive
applications of the Monostable-to-Multistable transition Logic (MML), and they
are on the basis of advanced circuits for communications. The operation of such
quantizer has two steps : sampling and holding. Once the quantizer samples the
signal, it m... | cond-mat.mtrl-sci | multiplevalued logic mvl circuits are one of the most attractive applications of the monostabletomultistable transition logic mml and they are on the basis of advanced circuits for communications the operation of such quantizer has two steps sampling and holding once the quantizer samples the signal it must maintain th... | [['multiplevalued', 'logic', 'mvl', 'circuits', 'are', 'one', 'of', 'the', 'most', 'attractive', 'applications', 'of', 'the', 'monostabletomultistable', 'transition', 'logic', 'mml', 'and', 'they', 'are', 'on', 'the', 'basis', 'of', 'advanced', 'circuits', 'for', 'communications', 'the', 'operation', 'of', 'such', 'qua... | [-0.165732679568151, 0.08596916103836334, -0.058055785464583544, 0.05828025446759076, -0.0674132360408323, -0.19427208773421265, 0.0765890210343685, 0.40079941011724934, -0.27964612911330156, -0.30598719850663214, 0.15614981425585606, -0.2537042210980128, -0.15127549021910394, 0.19749988619017825, -0.11011463824299074,... |
708.1453 | Nano Calculators | The whole circuit is obtained from the sun through a molecule called
"Rhodopsin and bacteriorhodopsin". These molecules have the capability of
trapping and storing energy from the sun light. These molecules are placed on
the outer surface of the calculator to trap the energy and store it themselves
for latter usage. ... | cond-mat.mtrl-sci | the whole circuit is obtained from the sun through a molecule called rhodopsin and bacteriorhodopsin these molecules have the capability of trapping and storing energy from the sun light these molecules are placed on the outer surface of the calculator to trap the energy and store it themselves for latter usage the thi... | [['the', 'whole', 'circuit', 'is', 'obtained', 'from', 'the', 'sun', 'through', 'a', 'molecule', 'called', 'rhodopsin', 'and', 'bacteriorhodopsin', 'these', 'molecules', 'have', 'the', 'capability', 'of', 'trapping', 'and', 'storing', 'energy', 'from', 'the', 'sun', 'light', 'these', 'molecules', 'are', 'placed', 'on',... | [-0.07598357141236275, 0.15212404414672742, -0.024944836497359738, 0.028273139543175188, -0.010911804549819366, -0.16021469549741596, 0.07108595210857774, 0.4015033487653868, -0.26246378011009336, -0.3280370247613808, 0.0981967852937735, -0.2920111348979514, -0.07826499064156617, 0.23567649762315507, -0.021081690524542... |
708.1454 | Cell Architecture for Nanoelectronic Design | Several nanoelectronic devices have been already proved. However, no
architecture which makes use of them provides a feasible opportunity to build
medium/large systems. Nanoarchitecture proposals only solve a small part of the
problems needed to achieve a real design. In this paper, we propose and analyze
a cell arch... | cond-mat.mtrl-sci | several nanoelectronic devices have been already proved however no architecture which makes use of them provides a feasible opportunity to build mediumlarge systems nanoarchitecture proposals only solve a small part of the problems needed to achieve a real design in this paper we propose and analyze a cell architecture... | [['several', 'nanoelectronic', 'devices', 'have', 'been', 'already', 'proved', 'however', 'no', 'architecture', 'which', 'makes', 'use', 'of', 'them', 'provides', 'a', 'feasible', 'opportunity', 'to', 'build', 'mediumlarge', 'systems', 'nanoarchitecture', 'proposals', 'only', 'solve', 'a', 'small', 'part', 'of', 'the',... | [-0.12308640313981953, 0.042077157583277104, -0.03524190347278649, 0.04819989674310279, -0.04932267294596818, -0.16658683062404772, 0.11840571874014685, 0.4076959715398439, -0.23830163473030552, -0.3351003134907302, 0.07708056750056191, -0.23331680655542572, -0.20379896578773604, 0.2397344334650848, -0.0817018485316312... |
708.1455 | Towards a Holistic CAD Platform for Nanotechnologies | Silicon-based CMOS technologies are predicted to reach their ultimate limits
by the middle of the next decade. Research on nanotechnologies is actively
conducted, in a world-wide effort to develop new technologies able to maintain
the Moore's law. They promise revolutionizing the computing systems by
integrating trem... | cond-mat.mtrl-sci | siliconbased cmos technologies are predicted to reach their ultimate limits by the middle of the next decade research on nanotechnologies is actively conducted in a worldwide effort to develop new technologies able to maintain the moores law they promise revolutionizing the computing systems by integrating tremendous n... | [['siliconbased', 'cmos', 'technologies', 'are', 'predicted', 'to', 'reach', 'their', 'ultimate', 'limits', 'by', 'the', 'middle', 'of', 'the', 'next', 'decade', 'research', 'on', 'nanotechnologies', 'is', 'actively', 'conducted', 'in', 'a', 'worldwide', 'effort', 'to', 'develop', 'new', 'technologies', 'able', 'to', '... | [-0.1194916666621187, 0.08049497247389405, -0.043278693968507774, -0.005893234034172363, -0.10049457648387437, -0.12615729680207247, 0.06748600258086096, 0.37535451225832933, -0.2546234769365078, -0.3807453345313358, 0.13945909625747138, -0.24379137557439712, -0.16068650165996384, 0.28676664958281134, -0.12002853542152... |
708.1456 | Nanostructured Immunosensors. Application to the detection of
Progesterone | A novel nanostructured electrochemical immunsensor for the determination of
progesterone is reported. The approach combines the properties of gold
nanoparticles with the use of a graphite-Teflon composite electrode matrix,
into which gold nanoparticles are incorporated by simple physical inclusion.
The antibody anti-... | cond-mat.mtrl-sci | a novel nanostructured electrochemical immunsensor for the determination of progesterone is reported the approach combines the properties of gold nanoparticles with the use of a graphiteteflon composite electrode matrix into which gold nanoparticles are incorporated by simple physical inclusion the antibody antiprogest... | [['a', 'novel', 'nanostructured', 'electrochemical', 'immunsensor', 'for', 'the', 'determination', 'of', 'progesterone', 'is', 'reported', 'the', 'approach', 'combines', 'the', 'properties', 'of', 'gold', 'nanoparticles', 'with', 'the', 'use', 'of', 'a', 'graphiteteflon', 'composite', 'electrode', 'matrix', 'into', 'wh... | [-0.009012138565417334, 0.1384931080179607, -0.016287159225080027, -0.0587762808798111, 0.033677255953434945, -0.17991385869497276, 0.08493399319079954, 0.36532932999203116, -0.16455325177620825, -0.341691561781506, 0.016565928439376876, -0.33753034755553507, -0.10775880367074889, 0.17685981277694426, -0.02234729912805... |
708.1457 | Fusion Phage as a Bioselective Nanomaterial : Evolution of the Concept | Multibillion-clone landscape phage display libraries were prepared by the
fusion of the phage major coat protein pVIII with foreign random peptides.
Phage particles and their proteins specific for cancer and bacterial cells were
selected from the landscape libraries and exploited as molecular recognition
interfaces i... | cond-mat.mtrl-sci | multibillionclone landscape phage display libraries were prepared by the fusion of the phage major coat protein pviii with foreign random peptides phage particles and their proteins specific for cancer and bacterial cells were selected from the landscape libraries and exploited as molecular recognition interfaces in de... | [['multibillionclone', 'landscape', 'phage', 'display', 'libraries', 'were', 'prepared', 'by', 'the', 'fusion', 'of', 'the', 'phage', 'major', 'coat', 'protein', 'pviii', 'with', 'foreign', 'random', 'peptides', 'phage', 'particles', 'and', 'their', 'proteins', 'specific', 'for', 'cancer', 'and', 'bacterial', 'cells', ... | [-0.0511300275957554, 0.1594150109805775, -0.028228371766028406, 0.05227719078816119, -0.02571044517300871, -0.23299019733684606, 0.09136160583746918, 0.40626210367408433, -0.23883443956182585, -0.288678708606634, 0.02226468166819501, -0.2607365531124631, -0.19496459363117105, 0.16815615411163592, -0.05733522377541165,... |
708.1458 | DNA Nanorobotics | This paper presents a molecular mechanics study for new nanorobotic
structures using molecular dynamics (MD) simulations coupled to virtual reality
(VR) techniques. The operator can design and characterize through molecular
dynamics simulation the behavior of bionanorobotic components and structures
through 3-D visua... | cond-mat.mtrl-sci | this paper presents a molecular mechanics study for new nanorobotic structures using molecular dynamics md simulations coupled to virtual reality vr techniques the operator can design and characterize through molecular dynamics simulation the behavior of bionanorobotic components and structures through 3d visualization... | [['this', 'paper', 'presents', 'a', 'molecular', 'mechanics', 'study', 'for', 'new', 'nanorobotic', 'structures', 'using', 'molecular', 'dynamics', 'md', 'simulations', 'coupled', 'to', 'virtual', 'reality', 'vr', 'techniques', 'the', 'operator', 'can', 'design', 'and', 'characterize', 'through', 'molecular', 'dynamics... | [-0.11158832589785259, 0.048048930633813144, -0.0906552371258537, -0.0038232275222738585, -0.03853268462543686, -0.10861014711981018, 0.00792796021172156, 0.3895203584805131, -0.258925788042446, -0.27182360711197057, 0.05814886865516504, -0.21561027163018784, -0.27535967351247864, 0.23806176712115606, -0.01885594885175... |
708.1459 | To study the effects of degradation of phonon distribution on the high
frequency response in nano structures | Under hot electron condition, the hot carriers phonon excited by ultra-short
pulses in polar semiconductors initially loose energy rapidly by emitting
longitudinal optic phonons via dominant Frolic coupling. Thus, energy supplied
to the carriers by high electric fields goes into phonon generation. As the
phonon life ... | cond-mat.mtrl-sci | under hot electron condition the hot carriers phonon excited by ultrashort pulses in polar semiconductors initially loose energy rapidly by emitting longitudinal optic phonons via dominant frolic coupling thus energy supplied to the carriers by high electric fields goes into phonon generation as the phonon life time is... | [['under', 'hot', 'electron', 'condition', 'the', 'hot', 'carriers', 'phonon', 'excited', 'by', 'ultrashort', 'pulses', 'in', 'polar', 'semiconductors', 'initially', 'loose', 'energy', 'rapidly', 'by', 'emitting', 'longitudinal', 'optic', 'phonons', 'via', 'dominant', 'frolic', 'coupling', 'thus', 'energy', 'supplied',... | [-0.11422493839508867, 0.31283048940152697, -0.08556668931133535, 0.07176742033653395, -0.04782323663646024, -0.12005149405481523, 0.08041876073996855, 0.4298493486433609, -0.2447264428052745, -0.2420193015738097, -0.030759512960323938, -0.3374502424753513, -0.035853751212651906, 0.18633676290014528, 0.0126170020658931... |
708.146 | Warm inflation in the DGP brane-world model | Warm inflationary universe models on a warped Dvali-Gabadadze-Porrati brane
are studied. General conditions required for these models to be realizable are
derived and discussed. By using an effective exponential potential we develop
models for constant and variable dissipation coefficient ratio
$r=\frac{\Gamma}{3 H}$... | gr-qc astro-ph hep-th | warm inflationary universe models on a warped dvaligabadadzeporrati brane are studied general conditions required for these models to be realizable are derived and discussed by using an effective exponential potential we develop models for constant and variable dissipation coefficient ratio rfracgamma3 h we use recent ... | [['warm', 'inflationary', 'universe', 'models', 'on', 'a', 'warped', 'dvaligabadadzeporrati', 'brane', 'are', 'studied', 'general', 'conditions', 'required', 'for', 'these', 'models', 'to', 'be', 'realizable', 'are', 'derived', 'and', 'discussed', 'by', 'using', 'an', 'effective', 'exponential', 'potential', 'we', 'dev... | [-0.09580586984305194, 0.12387380068846848, -0.025463312381395587, 0.1324295272567758, -0.10886462491126386, -0.19747060391603521, -0.044279941357672215, 0.384011065190727, -0.17889018101548707, -0.2911049140858705, 0.13353364915302438, -0.18717279994032449, -0.11157255625800679, 0.20489891743960065, -0.038592704468303... |
708.1461 | Production and application of metal-based nanoparticles | A number of metal-based nanopowders such kinds as Fe, Co, Fe/Co alloy, Fe/C,
Fe/organic shell were successfully produced by aerosol synthesis method. The
mechanism of nanoparticles formation and the influence of experimental
parameters on shape, size distribution, structure, chemical and phase
composition of oxide-, ... | cond-mat.mtrl-sci | a number of metalbased nanopowders such kinds as fe co feco alloy fec feorganic shell were successfully produced by aerosol synthesis method the mechanism of nanoparticles formation and the influence of experimental parameters on shape size distribution structure chemical and phase composition of oxide carbon or organi... | [['a', 'number', 'of', 'metalbased', 'nanopowders', 'such', 'kinds', 'as', 'fe', 'co', 'feco', 'alloy', 'fec', 'feorganic', 'shell', 'were', 'successfully', 'produced', 'by', 'aerosol', 'synthesis', 'method', 'the', 'mechanism', 'of', 'nanoparticles', 'formation', 'and', 'the', 'influence', 'of', 'experimental', 'param... | [-0.022978521864609542, 0.1973905035772839, -0.008042243749809426, -0.022238054161740316, 0.02147087442210397, -0.12096884978834439, 0.024584310456506303, 0.5174022613445649, -0.23042208989578727, -0.4054141573708605, 0.046514638576883115, -0.2806485777695638, -0.06074500171077513, 0.1369836872437264, 0.040345646006785... |
708.1462 | Structural Characterization of Magnetic Nano-particles Suspensions,
Using Magnetic Measurements | The paper describes some characteristics of the "P" curves for structural
characterization of magnetic nano-particles suspensions (complex fluids,
complex powders, complex composite materials, or living biological materials
having magnetic properties). In the case of these materials, the magnetic
properties are confe... | cond-mat.mtrl-sci | the paper describes some characteristics of the p curves for structural characterization of magnetic nanoparticles suspensions complex fluids complex powders complex composite materials or living biological materials having magnetic properties in the case of these materials the magnetic properties are conferred to vari... | [['the', 'paper', 'describes', 'some', 'characteristics', 'of', 'the', 'p', 'curves', 'for', 'structural', 'characterization', 'of', 'magnetic', 'nanoparticles', 'suspensions', 'complex', 'fluids', 'complex', 'powders', 'complex', 'composite', 'materials', 'or', 'living', 'biological', 'materials', 'having', 'magnetic'... | [-0.17382599623340508, 0.16487901847865274, -0.09316850169442403, 0.023026949467344418, -0.07369782611664034, -0.09072746202731743, 0.01106484135827766, 0.3997860352516684, -0.2929556214163064, -0.3245844464812778, 0.041335356208838075, -0.2629330840725929, -0.19074130070427608, 0.23880377075730416, -0.0077872672237646... |
708.1463 | Light scalar at LHC: the Higgs or the dilaton? | It is likely that the LHC will observe a color- and charge-neutral scalar
whose decays are consistent with those of the Standard Model (SM) Higgs boson.
The Higgs interpretation of such a discovery is not the only possibility. For
example, electroweak symmetry breaking (EWSB) could be triggered by a
spontaneously bro... | hep-ph | it is likely that the lhc will observe a color and chargeneutral scalar whose decays are consistent with those of the standard model sm higgs boson the higgs interpretation of such a discovery is not the only possibility for example electroweak symmetry breaking ewsb could be triggered by a spontaneously broken nearly ... | [['it', 'is', 'likely', 'that', 'the', 'lhc', 'will', 'observe', 'a', 'color', 'and', 'chargeneutral', 'scalar', 'whose', 'decays', 'are', 'consistent', 'with', 'those', 'of', 'the', 'standard', 'model', 'sm', 'higgs', 'boson', 'the', 'higgs', 'interpretation', 'of', 'such', 'a', 'discovery', 'is', 'not', 'the', 'only'... | [-0.1251709162751066, 0.2995935968576452, -0.06802773253094438, 0.147637155360064, -0.13781799310566606, -0.21751678703029784, -0.016774268709710455, 0.30030604754574597, -0.25047728565295, -0.2595085405161487, 0.05391482235119166, -0.2844351430293508, -0.0542312909367595, 0.11814074614190136, 0.07056525449671254, 0.05... |
708.1464 | Batch fabrication of cluster assembled microarrays for chemical sensing | Deposition of clusters from the gas phase is becoming an enabling technology
for the production of nanostructured devices. Supersonic clusters beam
deposition (SCBD) has been shown as a viable route for the production of
nanostructured thin films. By using SCBD and by exploiting aerodynamical
effects typical of super... | cond-mat.mtrl-sci | deposition of clusters from the gas phase is becoming an enabling technology for the production of nanostructured devices supersonic clusters beam deposition scbd has been shown as a viable route for the production of nanostructured thin films by using scbd and by exploiting aerodynamical effects typical of supersonic ... | [['deposition', 'of', 'clusters', 'from', 'the', 'gas', 'phase', 'is', 'becoming', 'an', 'enabling', 'technology', 'for', 'the', 'production', 'of', 'nanostructured', 'devices', 'supersonic', 'clusters', 'beam', 'deposition', 'scbd', 'has', 'been', 'shown', 'as', 'a', 'viable', 'route', 'for', 'the', 'production', 'of'... | [-0.06112756266688498, 0.19713552306806936, -0.04865609411723339, -0.0764982127924808, -0.008704314318198998, -0.16502225713517804, 0.05351270565655655, 0.4825301831158308, -0.22569093454915742, -0.34469650929363876, 0.07965526504871936, -0.2762801587044333, -0.0101429593623974, 0.28438055434156784, -0.0125477319404196... |
708.1465 | Dispersion Impact on Ballistic CNTFET n+-i-n+ Performances | The designs integrating the promising carbon nanotube transistors (CNTFET)
will have to take into account the constraints implied by the strong dispersion
inherent to nanotube manufacturing. This paper proposes to characterize the
main CNTFET performances : on-current Ion, Ion/Ioff ratio and inverse
sub-threshold slo... | cond-mat.mtrl-sci | the designs integrating the promising carbon nanotube transistors cntfet will have to take into account the constraints implied by the strong dispersion inherent to nanotube manufacturing this paper proposes to characterize the main cntfet performances oncurrent ion ionioff ratio and inverse subthreshold slope s accord... | [['the', 'designs', 'integrating', 'the', 'promising', 'carbon', 'nanotube', 'transistors', 'cntfet', 'will', 'have', 'to', 'take', 'into', 'account', 'the', 'constraints', 'implied', 'by', 'the', 'strong', 'dispersion', 'inherent', 'to', 'nanotube', 'manufacturing', 'this', 'paper', 'proposes', 'to', 'characterize', '... | [-0.12477696149355987, 0.0651441717548578, -0.017474072985351086, 0.002118087020018279, -0.045563200883793106, -0.19873134297262313, 0.05337415807210191, 0.4531046030196277, -0.21698162438009272, -0.31140922608249116, 0.021498067494989795, -0.23231125511158485, -0.10031988885902772, 0.2182755869227659, -0.1077332657648... |
708.1466 | Growth Mechanism and Selective Synthesis of SWNTs | Ever since the landmark discovery of single-walled carbon nanotubes (SWNTs)
in 1993, they have been considered as ideal materials for any kind of
application based on their outstanding properties (e.g. mechanical strength,
thermal conductivity, ultra stability, etc.), and various techniques, including
laser furnace t... | cond-mat.mtrl-sci | ever since the landmark discovery of singlewalled carbon nanotubes swnts in 1993 they have been considered as ideal materials for any kind of application based on their outstanding properties eg mechanical strength thermal conductivity ultra stability etc and various techniques including laser furnace technique arc dis... | [['ever', 'since', 'the', 'landmark', 'discovery', 'of', 'singlewalled', 'carbon', 'nanotubes', 'swnts', 'in', '1993', 'they', 'have', 'been', 'considered', 'as', 'ideal', 'materials', 'for', 'any', 'kind', 'of', 'application', 'based', 'on', 'their', 'outstanding', 'properties', 'eg', 'mechanical', 'strength', 'therma... | [-0.027881928961914108, 0.1419604619217365, -0.07209888798165687, -0.05053767045567028, -0.06565580448629904, -0.13783916829749435, 0.08594047126905092, 0.47537543286955886, -0.25563667369309534, -0.33864373089523897, 0.1040021372740442, -0.24751533515320545, -0.16091446761916184, 0.21965286470981327, -0.07399836686110... |
708.1467 | Numerical Simulation of The Mechanical Properties of Carbon Nanotube
Using the Atomistic-Continuum Mechanics | This paper the utilizes atomistic-continuum mechanics (ACM) to investigate
the mechanical properties of single-walled carbon nanotubes (SWCNTs). By
establishing a linkage between structural mechanics and molecular mechanics,
not only the Young's moduli could be obtained but also the modal analysis could
be achieved. ... | cond-mat.mtrl-sci | this paper the utilizes atomisticcontinuum mechanics acm to investigate the mechanical properties of singlewalled carbon nanotubes swcnts by establishing a linkage between structural mechanics and molecular mechanics not only the youngs moduli could be obtained but also the modal analysis could be achieved in addition ... | [['this', 'paper', 'the', 'utilizes', 'atomisticcontinuum', 'mechanics', 'acm', 'to', 'investigate', 'the', 'mechanical', 'properties', 'of', 'singlewalled', 'carbon', 'nanotubes', 'swcnts', 'by', 'establishing', 'a', 'linkage', 'between', 'structural', 'mechanics', 'and', 'molecular', 'mechanics', 'not', 'only', 'the'... | [-0.06972001995018218, 0.09055559800303441, -0.11166648584714328, -0.01500851379850329, -0.03989850336008451, -0.1612635283170014, 0.054662642438250426, 0.4211443831868978, -0.29320646196984773, -0.3095100868853148, 0.05903987959953321, -0.22642323707061057, -0.1636642475049567, 0.19245962932737629, -0.0817698554389856... |
708.1468 | Optical Characterisation of MOVPE Grown Vertically Correlated InAs/GaAs
Quantum Dots | Structures with self-organised InAs quantum dots in a GaAs matrix were grown
by the low pressure metal-organic vapour phase epitaxy (LP-MOVPE) technique.
Photoluminescence in combination with photomodulated reflectance spectroscopy
were used as the main characterisation methods for the growth optimisation.
Results sh... | cond-mat.mtrl-sci | structures with selforganised inas quantum dots in a gaas matrix were grown by the low pressure metalorganic vapour phase epitaxy lpmovpe technique photoluminescence in combination with photomodulated reflectance spectroscopy were used as the main characterisation methods for the growth optimisation results show that p... | [['structures', 'with', 'selforganised', 'inas', 'quantum', 'dots', 'in', 'a', 'gaas', 'matrix', 'were', 'grown', 'by', 'the', 'low', 'pressure', 'metalorganic', 'vapour', 'phase', 'epitaxy', 'lpmovpe', 'technique', 'photoluminescence', 'in', 'combination', 'with', 'photomodulated', 'reflectance', 'spectroscopy', 'were... | [-0.04503927088893868, 0.1501699912326277, -0.06974617961575003, -0.062375897385851094, 0.0746411735582275, -0.1912732376538984, 0.012288111594149513, 0.5159688971539521, -0.2761950696380261, -0.33763026517322836, 0.03278564999516889, -0.2940576157929814, -0.15926594635547028, 0.24574230411363876, 0.01540794490617426, ... |
708.1469 | The Chiral Model of Sakai-Sugimoto at Finite Baryon Density | In the context of holographic QCD we analyze Sakai-Sugimoto's chiral model at
finite baryon density and zero temperature. The baryon number density is
introduced through compact D4 wrapping S^4 at the tip of D8-\bar{D8}. Each
baryon acts as a chiral point-like source distributed uniformly over R^3, and
leads a non-va... | hep-th hep-ph | in the context of holographic qcd we analyze sakaisugimotos chiral model at finite baryon density and zero temperature the baryon number density is introduced through compact d4 wrapping s4 at the tip of d8bard8 each baryon acts as a chiral pointlike source distributed uniformly over r3 and leads a nonvanishing u1_v po... | [['in', 'the', 'context', 'of', 'holographic', 'qcd', 'we', 'analyze', 'sakaisugimotos', 'chiral', 'model', 'at', 'finite', 'baryon', 'density', 'and', 'zero', 'temperature', 'the', 'baryon', 'number', 'density', 'is', 'introduced', 'through', 'compact', 'd4', 'wrapping', 's4', 'at', 'the', 'tip', 'of', 'd8bard8', 'eac... | [-0.15743065800277456, 0.2775084198061978, -0.06962424006741194, 0.08079628833990184, -0.07054352469501957, -0.08151977767026232, 0.058347599109965224, 0.286981841218808, -0.16943624926911247, -0.24512181500153196, 0.013064720863927036, -0.3319454723623611, -0.04440093455806134, 0.04231958284508437, 0.04579132240746290... |
708.147 | A note on the lambda-structure on the Burnside ring | Let G be a finite group and let S be a G-set. The Burnside ring of G has a
natural structure of a lambda-ring. However, a priori the images of S under the
lambda-operations can only be computed implicitly. In this paper we establish
an explicit formula, expressing these images as linear combinations of classes
of G-s... | math.GR | let g be a finite group and let s be a gset the burnside ring of g has a natural structure of a lambdaring however a priori the images of s under the lambdaoperations can only be computed implicitly in this paper we establish an explicit formula expressing these images as linear combinations of classes of gsets | [['let', 'g', 'be', 'a', 'finite', 'group', 'and', 'let', 's', 'be', 'a', 'gset', 'the', 'burnside', 'ring', 'of', 'g', 'has', 'a', 'natural', 'structure', 'of', 'a', 'lambdaring', 'however', 'a', 'priori', 'the', 'images', 'of', 's', 'under', 'the', 'lambdaoperations', 'can', 'only', 'be', 'computed', 'implicitly', 'i... | [-0.1776773844959966, 0.06511674600213219, -0.14247005303766122, 0.011585930646233783, -0.11719601704297881, -0.13750126922764538, -0.0013093933679588269, 0.34992613787190957, -0.3503288354790002, -0.26187861325186595, 0.09333252186453983, -0.21128591261967494, -0.09927909327834322, 0.18695421969485387, -0.130604183497... |
708.1471 | The Schwinger mechanism and graphene | The Schwinger mechanism, the production of charged particle-antiparticle
pairs in a macroscopic external electric field, is derived for 2+1 dimensional
theories. The rate of pair production per unit area for four species of
massless fermions, with charge $q$, in a constant electric field $E$ is given
by $ \pi^{-2} \h... | cond-mat.mes-hall hep-ph hep-th nucl-th | the schwinger mechanism the production of charged particleantiparticle pairs in a macroscopic external electric field is derived for 21 dimensional theories the rate of pair production per unit area for four species of massless fermions with charge q in a constant electric field e is given by pi2 hbar32 tildec12 q e32 ... | [['the', 'schwinger', 'mechanism', 'the', 'production', 'of', 'charged', 'particleantiparticle', 'pairs', 'in', 'a', 'macroscopic', 'external', 'electric', 'field', 'is', 'derived', 'for', '21', 'dimensional', 'theories', 'the', 'rate', 'of', 'pair', 'production', 'per', 'unit', 'area', 'for', 'four', 'species', 'of', ... | [-0.1664600139690353, 0.25203838154313063, -0.029492110900220372, 0.06927422224262339, -0.013434416529977875, -0.17541162878830707, 0.03950813596959286, 0.32190077398873623, -0.19015925015968782, -0.26194735662636137, -0.01350188405805027, -0.2970508991199876, -0.08930543644518982, 0.1842344300183017, 0.007573921886843... |
708.1472 | Operational definition of (brane induced) space-time and constraints on
the fundamental parameters | First we contemplate the operational definition of space-time in four
dimensions in light of basic principles of quantum mechanics and general
relativity and consider some of its phenomenological consequences. The quantum
gravitational fluctuations of the background metric that comes through the
operational definitio... | hep-th gr-qc hep-ph | first we contemplate the operational definition of spacetime in four dimensions in light of basic principles of quantum mechanics and general relativity and consider some of its phenomenological consequences the quantum gravitational fluctuations of the background metric that comes through the operational definition of... | [['first', 'we', 'contemplate', 'the', 'operational', 'definition', 'of', 'spacetime', 'in', 'four', 'dimensions', 'in', 'light', 'of', 'basic', 'principles', 'of', 'quantum', 'mechanics', 'and', 'general', 'relativity', 'and', 'consider', 'some', 'of', 'its', 'phenomenological', 'consequences', 'the', 'quantum', 'grav... | [-0.1385869661090611, 0.20614810235727216, -0.10800526271567731, 0.12341434992736645, -0.09306650591639078, -0.1497962271403392, -0.02236589413627775, 0.2841698605237373, -0.25772425525630954, -0.30248372603414786, 0.11593592628196348, -0.24917818123422977, -0.14025199602151084, 0.19036709531469065, -0.0815351035044942... |
708.1473 | Waveguide properties of single subwavelength holes demonstrated with
radially and azimuthally polarized light | We investigate the transmission of focused beams through single subwavelength
holes in a silver film. We use radially and azimuthally polarized light,
respectively, to excite higher order waveguide modes as well as to match the
radial symmetry of the aperture geometry. Remarkably, the transmission
properties can be d... | physics.optics | we investigate the transmission of focused beams through single subwavelength holes in a silver film we use radially and azimuthally polarized light respectively to excite higher order waveguide modes as well as to match the radial symmetry of the aperture geometry remarkably the transmission properties can be describe... | [['we', 'investigate', 'the', 'transmission', 'of', 'focused', 'beams', 'through', 'single', 'subwavelength', 'holes', 'in', 'a', 'silver', 'film', 'we', 'use', 'radially', 'and', 'azimuthally', 'polarized', 'light', 'respectively', 'to', 'excite', 'higher', 'order', 'waveguide', 'modes', 'as', 'well', 'as', 'to', 'mat... | [-0.1014927262577283, 0.15135112818440094, -0.03853350759976927, -0.003976275884162854, -0.04112575293573387, -0.1653636954861748, 0.0100606423254837, 0.5020352666649748, -0.23661084356717765, -0.3036760084111901, 0.08339625384713359, -0.2811602125396295, -0.06653864517369691, 0.21829062401358149, 0.009758340003078474,... |
708.1474 | The Status of the Polarized Parton Densities | A survey is given on the present knowledge of the polarized parton
distribution functions. We give an outlook for further developments desired
both on the theoretical as well on the experimental side to complete the
understanding of the spin--structure of nucleons in the future.
| hep-ph astro-ph hep-ex | a survey is given on the present knowledge of the polarized parton distribution functions we give an outlook for further developments desired both on the theoretical as well on the experimental side to complete the understanding of the spinstructure of nucleons in the future | [['a', 'survey', 'is', 'given', 'on', 'the', 'present', 'knowledge', 'of', 'the', 'polarized', 'parton', 'distribution', 'functions', 'we', 'give', 'an', 'outlook', 'for', 'further', 'developments', 'desired', 'both', 'on', 'the', 'theoretical', 'as', 'well', 'on', 'the', 'experimental', 'side', 'to', 'complete', 'the'... | [-0.08659391402563249, 0.08266627768733253, -0.1258346208328889, 0.0770683307967953, -0.10183219603178176, 0.010692726863040165, 0.04018015708160502, 0.3922701721841639, -0.19508346644314853, -0.2551231842424551, 0.08800851460281675, -0.30752747310113837, -0.07034865605898878, 0.2271356237205592, 0.014715820741416379, ... |
708.1475 | Prediction for new magnetoelectric fluorides | We use symmetry considerations in order to predict new magnetoelectric
fluorides. In addition to these magnetoelectric properties, we discuss among
these fluorides the ones susceptible to present multiferroic properties. We
emphasize that several materials present ferromagnetic properties. This
ferromagnetism should ... | cond-mat.mtrl-sci cond-mat.str-el | we use symmetry considerations in order to predict new magnetoelectric fluorides in addition to these magnetoelectric properties we discuss among these fluorides the ones susceptible to present multiferroic properties we emphasize that several materials present ferromagnetic properties this ferromagnetism should enhanc... | [['we', 'use', 'symmetry', 'considerations', 'in', 'order', 'to', 'predict', 'new', 'magnetoelectric', 'fluorides', 'in', 'addition', 'to', 'these', 'magnetoelectric', 'properties', 'we', 'discuss', 'among', 'these', 'fluorides', 'the', 'ones', 'susceptible', 'to', 'present', 'multiferroic', 'properties', 'we', 'emphas... | [-0.1532309528659372, 0.1627426660053578, 0.00529569933446599, 0.06555272108080852, -0.15373088782835825, -0.07349084052896383, 0.06300079591535762, 0.4976830578902188, -0.28789646120048035, -0.28499955132457555, 0.006828866453896112, -0.34998361267806855, -0.2611260835592653, 0.14000923443110844, 0.03021901334617652, ... |
708.1476 | Mott transition in anharmonic confinement | Two effects are identified that affect the visibility of the Mott transition
in an atomic gas in an optical lattice confined in a power-law potential. The
transition can be made more pronounced by increasing the power law, but at the
same time, experimental uncertainty in the number of particles will induce
correspon... | cond-mat.other | two effects are identified that affect the visibility of the mott transition in an atomic gas in an optical lattice confined in a powerlaw potential the transition can be made more pronounced by increasing the power law but at the same time experimental uncertainty in the number of particles will induce corresponding f... | [['two', 'effects', 'are', 'identified', 'that', 'affect', 'the', 'visibility', 'of', 'the', 'mott', 'transition', 'in', 'an', 'atomic', 'gas', 'in', 'an', 'optical', 'lattice', 'confined', 'in', 'a', 'powerlaw', 'potential', 'the', 'transition', 'can', 'be', 'made', 'more', 'pronounced', 'by', 'increasing', 'the', 'po... | [-0.13213573928535266, 0.2516942453793342, -0.07866960919602926, 0.05062304814698088, 0.00960736038152475, -0.13241024719291303, 0.024578412496593108, 0.36433229980946974, -0.2383511757348166, -0.3098213534888833, 0.03195741322422183, -0.31149525350219637, -0.06381345000984363, 0.19998610054202334, 0.009102369701966297... |
708.1477 | Angular momentum transport by internal gravity waves III - Wave
excitation by core convection and the Coriolis effect | This is the third in a series of papers that deal with angular momentum
transport by internal gravity waves. We concentrate on the waves excited by
core convection in a 3Msun, Pop I main sequence star. Here, we want to examine
the role of the Coriolis acceleration in the equations of motion that describe
the behavior... | astro-ph | this is the third in a series of papers that deal with angular momentum transport by internal gravity waves we concentrate on the waves excited by core convection in a 3msun pop i main sequence star here we want to examine the role of the coriolis acceleration in the equations of motion that describe the behavior of wa... | [['this', 'is', 'the', 'third', 'in', 'a', 'series', 'of', 'papers', 'that', 'deal', 'with', 'angular', 'momentum', 'transport', 'by', 'internal', 'gravity', 'waves', 'we', 'concentrate', 'on', 'the', 'waves', 'excited', 'by', 'core', 'convection', 'in', 'a', '3msun', 'pop', 'i', 'main', 'sequence', 'star', 'here', 'we... | [-0.18323143159872607, 0.19934591922026715, -0.09171947584928651, 0.07835604303491939, -0.1335220918721078, -0.03697906421301396, -0.026151911945596927, 0.30814972954164993, -0.2618919494365783, -0.27090720670101676, 0.03715981645080702, -0.25321759064566945, -0.11946216362749079, 0.17473153780018422, -0.02955423055100... |
708.1478 | Exclusive rho^0 production in deep inelastic scattering at HERA | Exclusive rho^0 electroproduction at HERA has been studied with the ZEUS
detector using 120 pb^{-1} of integrated luminosity collected during 1996-2000.
The analysis was carried out in the kinematic range of photon virtuality 2 <
Q^2 < 160 GeV$^2, and gamma^* p centre-of-mass energy 32 < W < 180 GeV. The
results incl... | hep-ex | exclusive rho0 electroproduction at hera has been studied with the zeus detector using 120 pb1 of integrated luminosity collected during 19962000 the analysis was carried out in the kinematic range of photon virtuality 2 q2 160 gev2 and gamma p centreofmass energy 32 w 180 gev the results include the q2 and w dependenc... | [['exclusive', 'rho0', 'electroproduction', 'at', 'hera', 'has', 'been', 'studied', 'with', 'the', 'zeus', 'detector', 'using', '120', 'pb1', 'of', 'integrated', 'luminosity', 'collected', 'during', '19962000', 'the', 'analysis', 'was', 'carried', 'out', 'in', 'the', 'kinematic', 'range', 'of', 'photon', 'virtuality', ... | [-0.04848842174323479, 0.18860614835590364, -0.1273121409423399, 0.10297751115212421, -0.013415516111530176, -0.07046945276132104, 0.025720941012396532, 0.3801519826931112, -0.16264703006194042, -0.3076674042977862, -0.06777299691809482, -0.3710701121369518, 0.09785323925003284, 0.18581577065056426, 0.11917953473954078... |
708.1479 | The rotation of very low-mass stars and brown dwarfs | The evolution of angular momentum is a key to our understanding of star
formation and stellar evolution. The rotational evolution of solar-mass stars
is mostly controlled by magnetic interaction with the circumstellar disc and
angular momentum loss through stellar winds. Major differences in the internal
structure of... | astro-ph | the evolution of angular momentum is a key to our understanding of star formation and stellar evolution the rotational evolution of solarmass stars is mostly controlled by magnetic interaction with the circumstellar disc and angular momentum loss through stellar winds major differences in the internal structure of very... | [['the', 'evolution', 'of', 'angular', 'momentum', 'is', 'a', 'key', 'to', 'our', 'understanding', 'of', 'star', 'formation', 'and', 'stellar', 'evolution', 'the', 'rotational', 'evolution', 'of', 'solarmass', 'stars', 'is', 'mostly', 'controlled', 'by', 'magnetic', 'interaction', 'with', 'the', 'circumstellar', 'disc'... | [-0.09511758039877252, 0.2195659363099817, -0.08965648505475046, 0.14657282134635574, -0.16319278052564964, 0.02809184181133231, 0.041678029948899756, 0.4156731534206751, -0.17552465260101174, -0.39741484679788064, 0.040262228531256605, -0.21860718733893292, -0.04180809279487839, 0.189491663557631, -0.09666692738611142... |
708.148 | Valid formulas, games and network protocols | We describe a remarkable relation between the notion of valid formula of
predicate logic and the specification of network protocols. We give several
examples such as the acknowledgement of one packet or of a sequence of packets.
We show how to specify the composition of protocols.
| cs.LO | we describe a remarkable relation between the notion of valid formula of predicate logic and the specification of network protocols we give several examples such as the acknowledgement of one packet or of a sequence of packets we show how to specify the composition of protocols | [['we', 'describe', 'a', 'remarkable', 'relation', 'between', 'the', 'notion', 'of', 'valid', 'formula', 'of', 'predicate', 'logic', 'and', 'the', 'specification', 'of', 'network', 'protocols', 'we', 'give', 'several', 'examples', 'such', 'as', 'the', 'acknowledgement', 'of', 'one', 'packet', 'or', 'of', 'a', 'sequence... | [-0.2114652853621089, 0.029717901012981714, -0.10018202943889343, 0.08876638399922977, -0.048102674074471, -0.15800653306929313, 0.1381034779630642, 0.3711615737689578, -0.306787794050963, -0.2856902549367236, 0.04761929592401113, -0.22895274663586979, -0.17051168140935022, 0.19330910264777587, -0.10993965163462512, 0.... |
708.1481 | Stanley Decompositions, Pretty Clean Filtrations and Reductions Modulo
Regular Elements | We study the behavior of Stanley decompositions and of pretty clean
filtrations under reduction modulo a regular element.
| math.AC | we study the behavior of stanley decompositions and of pretty clean filtrations under reduction modulo a regular element | [['we', 'study', 'the', 'behavior', 'of', 'stanley', 'decompositions', 'and', 'of', 'pretty', 'clean', 'filtrations', 'under', 'reduction', 'modulo', 'a', 'regular', 'element']] | [-0.13360394770279527, 0.04197485253421797, -0.18464880933364233, 0.07672793418169022, -0.024930315803632967, -0.12875676287027696, 0.027535669609076448, 0.36409157969885403, -0.3687982853088114, -0.16190713023145994, 0.1241339592832244, -0.27270875602132744, -0.130800811560928, 0.15239101379281944, -0.1894725456626879... |
708.1482 | f(R) Gravity: From the Pioneer Anomaly to the Cosmic Acceleration | We use metric formalism in $f(R)$ modified gravity to study the dynamics of
various systems from the solar system to the cosmological scale. we assume an
ansatz for the derivative of action as a function of distance and describe the
Pioneer anomaly and the flat rotation curve of the spiral galaxies. Having the
asympt... | astro-ph gr-qc hep-th | we use metric formalism in fr modified gravity to study the dynamics of various systems from the solar system to the cosmological scale we assume an ansatz for the derivative of action as a function of distance and describe the pioneer anomaly and the flat rotation curve of the spiral galaxies having the asymptotic beh... | [['we', 'use', 'metric', 'formalism', 'in', 'fr', 'modified', 'gravity', 'to', 'study', 'the', 'dynamics', 'of', 'various', 'systems', 'from', 'the', 'solar', 'system', 'to', 'the', 'cosmological', 'scale', 'we', 'assume', 'an', 'ansatz', 'for', 'the', 'derivative', 'of', 'action', 'as', 'a', 'function', 'of', 'distanc... | [-0.13805131777965773, 0.04346504798850219, -0.11165753997435483, 0.07908835756243207, -0.09937958576483652, -0.09620202549073535, -0.0077903515368234364, 0.3313854167121463, -0.22930435207672417, -0.3099443259367642, 0.05783238337705067, -0.2618590707269808, -0.14128009958658366, 0.16610261161307183, -0.03538016806511... |
708.1483 | Memory in the system: trajectory-environment | In the paper the memory effect in the system consisting from a trajectory of
process and an environment is considered. The environment is presented by
scalar potential and noise. The evolution of system is interpreted as process
of the continuous "measurement" of a trajectory by an environment and\or on the
contrary.... | physics.gen-ph | in the paper the memory effect in the system consisting from a trajectory of process and an environment is considered the environment is presented by scalar potential and noise the evolution of system is interpreted as process of the continuous measurement of a trajectory by an environment andor on the contrary in this... | [['in', 'the', 'paper', 'the', 'memory', 'effect', 'in', 'the', 'system', 'consisting', 'from', 'a', 'trajectory', 'of', 'process', 'and', 'an', 'environment', 'is', 'considered', 'the', 'environment', 'is', 'presented', 'by', 'scalar', 'potential', 'and', 'noise', 'the', 'evolution', 'of', 'system', 'is', 'interpreted... | [-0.1629258730692493, 0.1306241533957546, -0.11485649110362038, 0.0594744784910664, -0.03589918408281753, -0.09962384726865235, 0.022666113386387614, 0.34760479022700896, -0.29968162502431983, -0.27772431200909836, 0.1330159961101251, -0.2771006381600469, -0.15870094114792682, 0.15783883234329313, -0.07922847707109595,... |
708.1484 | A quantum dot implementation of the quantum NAND algorithm | We propose a physical implementation of the quantum NAND tree evaluation
algorithm. Our approach, based on continuous time quantum walks, uses the wave
interference of a single electron in a heirarchical set of tunnel coupled
quantum dots. We find that the query complexity of the NAND tree evaluation
does not suffer ... | quant-ph cond-mat.mes-hall | we propose a physical implementation of the quantum nand tree evaluation algorithm our approach based on continuous time quantum walks uses the wave interference of a single electron in a heirarchical set of tunnel coupled quantum dots we find that the query complexity of the nand tree evaluation does not suffer strong... | [['we', 'propose', 'a', 'physical', 'implementation', 'of', 'the', 'quantum', 'nand', 'tree', 'evaluation', 'algorithm', 'our', 'approach', 'based', 'on', 'continuous', 'time', 'quantum', 'walks', 'uses', 'the', 'wave', 'interference', 'of', 'a', 'single', 'electron', 'in', 'a', 'heirarchical', 'set', 'of', 'tunnel', '... | [-0.14161146835734448, 0.11176792415272858, -0.058478095604934624, 0.04661623884716796, -0.05083094484483202, -0.17955072199304897, 0.11287027607775396, 0.40465936918432516, -0.25002643366654714, -0.2662240811934074, 0.05029198443387738, -0.23723798278305266, -0.2030893130771195, 0.21250955410456907, -0.027727410639636... |
708.1485 | Pathwise coordinate optimization | We consider ``one-at-a-time'' coordinate-wise descent algorithms for a class
of convex optimization problems. An algorithm of this kind has been proposed
for the $L_1$-penalized regression (lasso) in the literature, but it seems to
have been largely ignored. Indeed, it seems that coordinate-wise algorithms are
not of... | stat.CO math.OC | we consider oneatatime coordinatewise descent algorithms for a class of convex optimization problems an algorithm of this kind has been proposed for the l_1penalized regression lasso in the literature but it seems to have been largely ignored indeed it seems that coordinatewise algorithms are not often used in convex o... | [['we', 'consider', 'oneatatime', 'coordinatewise', 'descent', 'algorithms', 'for', 'a', 'class', 'of', 'convex', 'optimization', 'problems', 'an', 'algorithm', 'of', 'this', 'kind', 'has', 'been', 'proposed', 'for', 'the', 'l_1penalized', 'regression', 'lasso', 'in', 'the', 'literature', 'but', 'it', 'seems', 'to', 'h... | [-0.005246546287701404, -0.029554212842213948, -0.1468411138090883, 0.10322176168390625, -0.12747868396899234, -0.19630638407339362, 0.0008490733380844123, 0.48882448656933153, -0.3339875205402963, -0.2555491909738222, 0.1552089756859439, -0.22285093162820613, -0.22908561164173333, 0.20789717046720704, -0.1592268475797... |
708.1486 | The low energy spectrum of finite size metallic SWNTs | The electronic spectrum of metallic finite-size single-wall carbon nanotubes
at low energies is derived. It is based on a tight-binding description for the
interacting p_{z} electrons. Not only the forward scattering parts of the
Coulomb interaction, which are diagonalized by bosonization, are considered,
but also al... | cond-mat.mes-hall cond-mat.str-el | the electronic spectrum of metallic finitesize singlewall carbon nanotubes at low energies is derived it is based on a tightbinding description for the interacting p_z electrons not only the forward scattering parts of the coulomb interaction which are diagonalized by bosonization are considered but also all other proc... | [['the', 'electronic', 'spectrum', 'of', 'metallic', 'finitesize', 'singlewall', 'carbon', 'nanotubes', 'at', 'low', 'energies', 'is', 'derived', 'it', 'is', 'based', 'on', 'a', 'tightbinding', 'description', 'for', 'the', 'interacting', 'p_z', 'electrons', 'not', 'only', 'the', 'forward', 'scattering', 'parts', 'of', ... | [-0.14504662455069495, 0.24712436985065964, -0.02800422377309742, 0.12070420895767536, -0.022478066548269164, -0.17407455160579782, 0.007711601389096456, 0.3980268746852241, -0.24053039650142966, -0.2542687561709751, 0.031743447246782956, -0.3282451698596173, -0.05598935352618548, 0.14366616980925678, 0.109091252574023... |
708.1487 | Quasisymmetric and unipotent tensor categories | We classify braided tensor categories over C of exponential growth which are
quasisymmetric, i.e., the squared braiding is the identity on the product of
any two simple objects. This generalizes the classification results of Deligne
on symmetric categories of exponential growth, and of Drinfeld on
quasitriangular qua... | math.QA math.CT | we classify braided tensor categories over c of exponential growth which are quasisymmetric ie the squared braiding is the identity on the product of any two simple objects this generalizes the classification results of deligne on symmetric categories of exponential growth and of drinfeld on quasitriangular quasihopf a... | [['we', 'classify', 'braided', 'tensor', 'categories', 'over', 'c', 'of', 'exponential', 'growth', 'which', 'are', 'quasisymmetric', 'ie', 'the', 'squared', 'braiding', 'is', 'the', 'identity', 'on', 'the', 'product', 'of', 'any', 'two', 'simple', 'objects', 'this', 'generalizes', 'the', 'classification', 'results', 'o... | [-0.17456686231590562, 0.0378332749078764, -0.07176862130481228, 0.05285952046021784, -0.11477223845529501, -0.168473451407017, -0.04659802142844022, 0.39020230174097276, -0.38296449831556356, -0.16180728219240625, 0.11825463665261969, -0.19310918832078106, -0.16228690584164077, 0.20580874690698964, -0.2048036783148108... |
708.1488 | Charmonium and open charm production in nuclear collisions at SPS/FAIR
energies and the possible influence of a hot hadronic medium | We provide predictions for charmonium and open charm production in nuclear
collisions at SPS/FAIR energies within the framework of the statistical
hadronization model. The increasing importance at lower energies of Lambda_c
production is demonstrated and provides a challenge for future experiments. We
also demonstrat... | nucl-th | we provide predictions for charmonium and open charm production in nuclear collisions at spsfair energies within the framework of the statistical hadronization model the increasing importance at lower energies of lambda_c production is demonstrated and provides a challenge for future experiments we also demonstrate tha... | [['we', 'provide', 'predictions', 'for', 'charmonium', 'and', 'open', 'charm', 'production', 'in', 'nuclear', 'collisions', 'at', 'spsfair', 'energies', 'within', 'the', 'framework', 'of', 'the', 'statistical', 'hadronization', 'model', 'the', 'increasing', 'importance', 'at', 'lower', 'energies', 'of', 'lambda_c', 'pr... | [-0.00864670768247119, 0.28194543470808564, -0.11485143101719372, 0.17781016488555632, -0.0006355921925679475, -0.08404583122362108, 0.03909750169870921, 0.3601777935009293, -0.18674253184395304, -0.25524679188295696, -0.05842749765064536, -0.3508392923409824, 0.08751164463215641, 0.1815449754001197, 0.0899062191327924... |
708.1489 | Principle of Minimal Energy in Relativistic Schroedinger Theory | The Hamilton-Lagrange action principle for Relativistic Schr\"odinger Theory
(RST) is converted to a variational principle (with constraints) for the
stationary bound states. The groundstate energy is the minimally possible value
of the corresponding energy functional and the relativistic energy eigenvalue
equations ... | hep-th | the hamiltonlagrange action principle for relativistic schrodinger theory rst is converted to a variational principle with constraints for the stationary bound states the groundstate energy is the minimally possible value of the corresponding energy functional and the relativistic energy eigenvalue equations do appear ... | [['the', 'hamiltonlagrange', 'action', 'principle', 'for', 'relativistic', 'schrodinger', 'theory', 'rst', 'is', 'converted', 'to', 'a', 'variational', 'principle', 'with', 'constraints', 'for', 'the', 'stationary', 'bound', 'states', 'the', 'groundstate', 'energy', 'is', 'the', 'minimally', 'possible', 'value', 'of', ... | [-0.10478074423085193, 0.1434310279043264, -0.10691686359166185, 0.14025594507306466, -0.06251514677872291, -0.1207738837895348, -0.013977970940246021, 0.25394784086181416, -0.26029280294889806, -0.30844918993570675, 0.03263510425462278, -0.2560182809366943, -0.09638846903933271, 0.16848801733978, 0.01702764547308502, ... |
708.149 | Nonequilibrium Opinion Spreading on 2D Small-World Networks | Irreversible opinion spreading phenomena are studied on small-world networks
generated from 2D regular lattices by means of the magnetic Eden model, a
nonequilibrium kinetic model for the growth of binary mixtures in contact with
a thermal bath. In this model, the opinion or decision of an individual is
affected by t... | physics.soc-ph cond-mat.dis-nn cond-mat.stat-mech physics.comp-ph | irreversible opinion spreading phenomena are studied on smallworld networks generated from 2d regular lattices by means of the magnetic eden model a nonequilibrium kinetic model for the growth of binary mixtures in contact with a thermal bath in this model the opinion or decision of an individual is affected by those o... | [['irreversible', 'opinion', 'spreading', 'phenomena', 'are', 'studied', 'on', 'smallworld', 'networks', 'generated', 'from', '2d', 'regular', 'lattices', 'by', 'means', 'of', 'the', 'magnetic', 'eden', 'model', 'a', 'nonequilibrium', 'kinetic', 'model', 'for', 'the', 'growth', 'of', 'binary', 'mixtures', 'in', 'contac... | [-0.12524226582909792, 0.19402113167631874, -0.04982976430397949, 0.07457829331316128, -0.03195169874635025, -0.1379586849299981, 0.07020222874734526, 0.40680069888985115, -0.2658994525350285, -0.2864381947079735, 0.05044633818062528, -0.2998254602645456, -0.15327476094698916, 0.16878221516300068, 0.02264995871124086, ... |
708.1491 | On perfect, amicable, and sociable chains | Let $x = (x_0,...,x_{n-1})$ be an n-chain, i.e., an n-tuple of non-negative
integers $< n$. Consider the operator $s: x \mapsto x' = (x'_0,...,x'_{n-1})$,
where x'_j represents the number of $j$'s appearing among the components of x.
An n-chain x is said to be perfect if $s(x) = x$. For example, (2,1,2,0,0) is a
perf... | math.CO cs.DM math.NT | let x x_0x_n1 be an nchain ie an ntuple of nonnegative integers n consider the operator s x mapsto x x_0x_n1 where x_j represents the number of js appearing among the components of x an nchain x is said to be perfect if sx x for example 21200 is a perfect 5chain analogously to the theory of perfect amicable and sociabl... | [['let', 'x', 'x_0x_n1', 'be', 'an', 'nchain', 'ie', 'an', 'ntuple', 'of', 'nonnegative', 'integers', 'n', 'consider', 'the', 'operator', 's', 'x', 'mapsto', 'x', 'x_0x_n1', 'where', 'x_j', 'represents', 'the', 'number', 'of', 'js', 'appearing', 'among', 'the', 'components', 'of', 'x', 'an', 'nchain', 'x', 'is', 'said'... | [-0.2291804983409399, 0.1368391765832673, -0.03576832983959863, -0.017213218482558003, -0.04264604602444996, -0.18562535020681295, 0.030447317975910104, 0.3292303160229262, -0.3235807991388472, -0.20481896604550012, 0.01455764999449689, -0.360559465165468, -0.0893309673200302, 0.1248927938632984, -0.07472521909685964, ... |
708.1492 | Observed Properties of Dark Matter on Small Spatial Scales | The nature of dark matter is one of the outstanding questions of
astrophysics. The internal motions of member stars reveal that the lowest
luminosity galaxies in the Local Group are the most dark-matter dominated. New
large datasets allow one to go further, and determine systematic properties of
their dark matter hal... | astro-ph | the nature of dark matter is one of the outstanding questions of astrophysics the internal motions of member stars reveal that the lowest luminosity galaxies in the local group are the most darkmatter dominated new large datasets allow one to go further and determine systematic properties of their dark matter haloes we... | [['the', 'nature', 'of', 'dark', 'matter', 'is', 'one', 'of', 'the', 'outstanding', 'questions', 'of', 'astrophysics', 'the', 'internal', 'motions', 'of', 'member', 'stars', 'reveal', 'that', 'the', 'lowest', 'luminosity', 'galaxies', 'in', 'the', 'local', 'group', 'are', 'the', 'most', 'darkmatter', 'dominated', 'new'... | [-0.08990755171122912, 0.11001740993417211, -0.14971070475631246, 0.15579234011697976, -0.16659241541607403, -0.0023089296699158454, -0.038085504098011085, 0.3298574501746579, -0.17583922534035273, -0.3911476772964785, -0.00599381794286034, -0.29536479094531387, -0.046640055450169665, 0.1950053608253304, 0.029264525602... |
708.1493 | From chiral vibration to static chirality in ^{135}Nd | Electromagnetic transition probabilities have been measured for the intra-
and inter-band transitions in the two sequences in the nucleus ^{135}Nd that
were previously identified as a composite chiral pair of rotational bands. The
measurements are in good agreement with results of a new combination of TAC and
RPA cal... | nucl-ex nucl-th | electromagnetic transition probabilities have been measured for the intra and interband transitions in the two sequences in the nucleus 135nd that were previously identified as a composite chiral pair of rotational bands the measurements are in good agreement with results of a new combination of tac and rpa calculation... | [['electromagnetic', 'transition', 'probabilities', 'have', 'been', 'measured', 'for', 'the', 'intra', 'and', 'interband', 'transitions', 'in', 'the', 'two', 'sequences', 'in', 'the', 'nucleus', '135nd', 'that', 'were', 'previously', 'identified', 'as', 'a', 'composite', 'chiral', 'pair', 'of', 'rotational', 'bands', '... | [-0.11827228495799079, 0.1791990241495353, -0.08604286560837768, 0.0433243406847683, -0.0006740492014949652, -0.10400763737331879, 0.05832294710470658, 0.43591861573881224, -0.1868243047011722, -0.2614475738588034, 0.0238500479624092, -0.3405891075289171, -0.14802294128304838, 0.13819582386273205, 0.0671869323000704, 0... |
708.1494 | A new non-perturbative time-dependent string configuration | A time-dependent bosonic string configuration is discussed, in graviton and
dilaton backgrounds, leading to Weyl-symmetry beta-functions which are
homogeneous in X^0, to any order in alpha'. As a consequence, a string
reparametrization can always be implemented, such that beta functions can be
cancelled, to any order... | hep-th gr-qc hep-ph | a timedependent bosonic string configuration is discussed in graviton and dilaton backgrounds leading to weylsymmetry betafunctions which are homogeneous in x0 to any order in alpha as a consequence a string reparametrization can always be implemented such that beta functions can be cancelled to any order in alpha this... | [['a', 'timedependent', 'bosonic', 'string', 'configuration', 'is', 'discussed', 'in', 'graviton', 'and', 'dilaton', 'backgrounds', 'leading', 'to', 'weylsymmetry', 'betafunctions', 'which', 'are', 'homogeneous', 'in', 'x0', 'to', 'any', 'order', 'in', 'alpha', 'as', 'a', 'consequence', 'a', 'string', 'reparametrizatio... | [-0.14257628188745394, 0.20337893355738473, -0.07669323332490283, 0.09807124158980006, -0.09589967657266571, -0.1581434801992801, -0.0015813460697310868, 0.33645237303288605, -0.20203937474336173, -0.20944089541496994, 0.07176703494251915, -0.2442690507836036, -0.12756156854264372, 0.15889913585406165, -0.0504737131760... |
708.1495 | Preliminary Results from MINOS on Muon Neutrino Disappearance Based on
an Exposure of 2.5x10^20 120 GeV Protons on the NuMI Target | Updating our previous measurements with new data and analysis modifications,
we report preliminary results on the energy-dependent deficit of muon neutrinos
from the Fermilab NuMI beam as observed with the MINOS Far Detector located 735
km away in the Soudan Underground Laboratory. From an exposure of 2.50x10^20
prot... | hep-ex hep-ph | updating our previous measurements with new data and analysis modifications we report preliminary results on the energydependent deficit of muon neutrinos from the fermilab numi beam as observed with the minos far detector located 735 km away in the soudan underground laboratory from an exposure of 250x1020 protons on ... | [['updating', 'our', 'previous', 'measurements', 'with', 'new', 'data', 'and', 'analysis', 'modifications', 'we', 'report', 'preliminary', 'results', 'on', 'the', 'energydependent', 'deficit', 'of', 'muon', 'neutrinos', 'from', 'the', 'fermilab', 'numi', 'beam', 'as', 'observed', 'with', 'the', 'minos', 'far', 'detecto... | [-0.07645026207868974, 0.22803120459098178, 0.0054088839870337, 0.1438991027148245, -0.005291645223001292, -0.10394502128637233, 0.15581836641466545, 0.3490552813379693, -0.1457965059655269, -0.379256350698171, 0.03149467985181568, -0.4376531123369688, 0.035779166598706606, 0.19337361905450276, 0.03120955499703182, 0.0... |
708.1496 | A Light-Based Device for Solving the Hamiltonian Path Problem | In this paper we suggest the use of light for performing useful computations.
Namely, we propose a special device which uses light rays for solving the
Hamiltonian path problem on a directed graph. The device has a graph-like
representation and the light is traversing it following the routes given by the
connections ... | cs.AR cs.DC | in this paper we suggest the use of light for performing useful computations namely we propose a special device which uses light rays for solving the hamiltonian path problem on a directed graph the device has a graphlike representation and the light is traversing it following the routes given by the connections betwee... | [['in', 'this', 'paper', 'we', 'suggest', 'the', 'use', 'of', 'light', 'for', 'performing', 'useful', 'computations', 'namely', 'we', 'propose', 'a', 'special', 'device', 'which', 'uses', 'light', 'rays', 'for', 'solving', 'the', 'hamiltonian', 'path', 'problem', 'on', 'a', 'directed', 'graph', 'the', 'device', 'has', ... | [-0.1465316613178419, 0.12489658716257732, -0.0994658436503191, 0.02064794651671963, -0.10685726577626928, -0.17786620357425287, 0.10279380339131919, 0.44111871142116077, -0.3213351735107179, -0.30596839576819035, 0.06413144285610509, -0.29274319841763674, -0.1745071330740345, 0.19088426674935827, -0.05931176635313709,... |
708.1497 | Information Rate Loss due to Radiation Decoherence | The information rates achievable by using electromagnetic radiation affected
by thermal noise and signal decoherence are studied. The standard coherent
Gaussian model is compared with an alternative photon gas model which
represents lack of a shared phase reference between transmitter and receiver.
At any frequency, ... | quant-ph | the information rates achievable by using electromagnetic radiation affected by thermal noise and signal decoherence are studied the standard coherent gaussian model is compared with an alternative photon gas model which represents lack of a shared phase reference between transmitter and receiver at any frequency infor... | [['the', 'information', 'rates', 'achievable', 'by', 'using', 'electromagnetic', 'radiation', 'affected', 'by', 'thermal', 'noise', 'and', 'signal', 'decoherence', 'are', 'studied', 'the', 'standard', 'coherent', 'gaussian', 'model', 'is', 'compared', 'with', 'an', 'alternative', 'photon', 'gas', 'model', 'which', 'rep... | [-0.136336165600155, 0.16799563716074986, -0.007023312653615779, 0.06550502037291653, -0.007174474661987202, -0.1812178769854226, 0.13150803633399455, 0.40727136901342403, -0.24897645706511742, -0.294522163257295, 0.0770471850718262, -0.29666591208318577, -0.04596401582353329, 0.2212302168516223, -0.04434124971557336, ... |
708.1498 | Optimizing Optical Quantum Logic Gates using Genetic Algorithms | We introduce the method of using an annealing genetic algorithm to the
numerically complex problem of looking for quantum logic gates which
simultaneously have highest fidelity and highest success probability. We first
use the linear optical quantum nonlinear sign (NS) gate as an example to
illustrate the efficiency ... | quant-ph | we introduce the method of using an annealing genetic algorithm to the numerically complex problem of looking for quantum logic gates which simultaneously have highest fidelity and highest success probability we first use the linear optical quantum nonlinear sign ns gate as an example to illustrate the efficiency of th... | [['we', 'introduce', 'the', 'method', 'of', 'using', 'an', 'annealing', 'genetic', 'algorithm', 'to', 'the', 'numerically', 'complex', 'problem', 'of', 'looking', 'for', 'quantum', 'logic', 'gates', 'which', 'simultaneously', 'have', 'highest', 'fidelity', 'and', 'highest', 'success', 'probability', 'we', 'first', 'use... | [-0.058909610628486715, 0.10402480702860986, -0.047445377968769104, 0.03401168294335043, -0.027062154552873433, -0.1893573298099606, 0.09793930669062927, 0.4344712955515004, -0.27899386356067324, -0.33712096194115776, 0.09042825949533533, -0.20506859026500024, -0.1691281298861011, 0.2592514501561204, -0.078351501540358... |
708.1499 | Transport processes in stars: diffusion, rotation, magnetic fields and
internal waves | In this paper, I explore various transport processes that have a large impact
of the distribution of elements inside stars and thus, on stellar evolution. A
heuristic description of the physics behind equations is provided, and key
references are given. Finally, for each process, I will briefly review (some)
importan... | astro-ph | in this paper i explore various transport processes that have a large impact of the distribution of elements inside stars and thus on stellar evolution a heuristic description of the physics behind equations is provided and key references are given finally for each process i will briefly review some important results a... | [['in', 'this', 'paper', 'i', 'explore', 'various', 'transport', 'processes', 'that', 'have', 'a', 'large', 'impact', 'of', 'the', 'distribution', 'of', 'elements', 'inside', 'stars', 'and', 'thus', 'on', 'stellar', 'evolution', 'a', 'heuristic', 'description', 'of', 'the', 'physics', 'behind', 'equations', 'is', 'prov... | [-0.05421634204685688, 0.1332323294748568, -0.056065578013658524, 0.07862569737141203, -0.08983016733900975, -0.08532586322813215, 0.019216091468756608, 0.36513573499554297, -0.2403311203786377, -0.2866288352741907, 0.14149397195482594, -0.26763354714612586, -0.17315256753462857, 0.2173041009533582, -0.0453209046598018... |
708.15 | The reverse engineering problem with probabilities and sequential
behavior: Probabilistic Sequential Networks | The reverse engineering problem with probabilities and sequential behavior is
introducing here, using the expression of an algorithm. The solution is
partially founded, because we solve the problem only if we have a Probabilistic
Sequential Network. Therefore the probabilistic structure on sequential
dynamical system... | math.DS math.CT | the reverse engineering problem with probabilities and sequential behavior is introducing here using the expression of an algorithm the solution is partially founded because we solve the problem only if we have a probabilistic sequential network therefore the probabilistic structure on sequential dynamical systems is i... | [['the', 'reverse', 'engineering', 'problem', 'with', 'probabilities', 'and', 'sequential', 'behavior', 'is', 'introducing', 'here', 'using', 'the', 'expression', 'of', 'an', 'algorithm', 'the', 'solution', 'is', 'partially', 'founded', 'because', 'we', 'solve', 'the', 'problem', 'only', 'if', 'we', 'have', 'a', 'proba... | [-0.12975453600001924, 0.05231014701436243, -0.08776413246200684, 0.09339231641599433, -0.06149005284023056, -0.15547402618949158, 0.04499520251721171, 0.4022381956056848, -0.37733227901677363, -0.23703850932201764, 0.12809793647280113, -0.21409081344078057, -0.17033442029097273, 0.16897184235540075, -0.088851053940716... |
708.1501 | Sch'nol's Theorem For Strongly Local Forms | We prove a variant of Sch'nol's theorem in a general setting: for generators
of strongly local Dirichlet forms perturbed by measures. As an application, we
discuss quantum graphs with $\delta$- or Kirchhoff boundary conditions.
| math.SP math.AP | we prove a variant of schnols theorem in a general setting for generators of strongly local dirichlet forms perturbed by measures as an application we discuss quantum graphs with delta or kirchhoff boundary conditions | [['we', 'prove', 'a', 'variant', 'of', 'schnols', 'theorem', 'in', 'a', 'general', 'setting', 'for', 'generators', 'of', 'strongly', 'local', 'dirichlet', 'forms', 'perturbed', 'by', 'measures', 'as', 'an', 'application', 'we', 'discuss', 'quantum', 'graphs', 'with', 'delta', 'or', 'kirchhoff', 'boundary', 'conditions'... | [-0.16743860467139518, 0.09658256533359898, -0.06358670880030276, 0.07433133419941772, -0.0720237262589349, -0.16374863878908483, -0.003666863247582858, 0.3230971023440361, -0.309455931186676, -0.22126118370303602, 0.15497932126957245, -0.26063612856986845, -0.16852555512168416, 0.2066518772097135, -0.13810223084168904... |
708.1502 | The string/gauge theory correspondence in QCD | Ideas about a duality between gauge fields and strings have been around for
many decades. During the last ten years, these ideas have taken a much more
concrete mathematical form. String descriptions of the strongly coupled
dynamics of semi-realistic gauge theories, exhibiting confinement and chiral
symmetry breaking... | hep-ph hep-lat hep-th | ideas about a duality between gauge fields and strings have been around for many decades during the last ten years these ideas have taken a much more concrete mathematical form string descriptions of the strongly coupled dynamics of semirealistic gauge theories exhibiting confinement and chiral symmetry breaking are no... | [['ideas', 'about', 'a', 'duality', 'between', 'gauge', 'fields', 'and', 'strings', 'have', 'been', 'around', 'for', 'many', 'decades', 'during', 'the', 'last', 'ten', 'years', 'these', 'ideas', 'have', 'taken', 'a', 'much', 'more', 'concrete', 'mathematical', 'form', 'string', 'descriptions', 'of', 'the', 'strongly', ... | [-0.09804036182313944, 0.2306701124849162, -0.13512740948976115, 0.08271363278015934, -0.10830673847304678, -0.16883431758795833, -0.03588909283547994, 0.3681996447708586, -0.20621000603911863, -0.2957780217944548, 0.09188207702165277, -0.26313705913636876, -0.1571924956809815, 0.17930547028094873, 0.014176040791488927... |
708.1503 | Defensive forecasting for optimal prediction with expert advice | The method of defensive forecasting is applied to the problem of prediction
with expert advice for binary outcomes. It turns out that defensive forecasting
is not only competitive with the Aggregating Algorithm but also handles the
case of "second-guessing" experts, whose advice depends on the learner's
prediction; t... | cs.LG | the method of defensive forecasting is applied to the problem of prediction with expert advice for binary outcomes it turns out that defensive forecasting is not only competitive with the aggregating algorithm but also handles the case of secondguessing experts whose advice depends on the learners prediction this paper... | [['the', 'method', 'of', 'defensive', 'forecasting', 'is', 'applied', 'to', 'the', 'problem', 'of', 'prediction', 'with', 'expert', 'advice', 'for', 'binary', 'outcomes', 'it', 'turns', 'out', 'that', 'defensive', 'forecasting', 'is', 'not', 'only', 'competitive', 'with', 'the', 'aggregating', 'algorithm', 'but', 'also... | [-0.028073790398875958, 0.06809658953791549, -0.11432914283720712, 0.08848961136416243, -0.15968596145253758, -0.21151139757371154, 0.12210386348807992, 0.3852681107176789, -0.20998640702073945, -0.30828244110633585, 0.1065358994689224, -0.2936545528856845, -0.1521417432512831, 0.2117423038319524, -0.14930589806995, 0.... |
708.1504 | Theoretical study of a localized quantum spin reversal by the sequential
injection of spins in a spin quantum dot | This is a theoretical study of the reversal of a localized quantum spin
induced by sequential injection of spins for a spin quantum dot that has a
quantum spin. The system consists of ``electrode/quantum
well(QW)/dot/QW/electrode" junctions, in which the left QW has an energy level
of conduction electrons with only u... | cond-mat.mes-hall cond-mat.mtrl-sci quant-ph | this is a theoretical study of the reversal of a localized quantum spin induced by sequential injection of spins for a spin quantum dot that has a quantum spin the system consists of electrodequantum wellqwdotqwelectrode junctions in which the left qw has an energy level of conduction electrons with only upspin we cons... | [['this', 'is', 'a', 'theoretical', 'study', 'of', 'the', 'reversal', 'of', 'a', 'localized', 'quantum', 'spin', 'induced', 'by', 'sequential', 'injection', 'of', 'spins', 'for', 'a', 'spin', 'quantum', 'dot', 'that', 'has', 'a', 'quantum', 'spin', 'the', 'system', 'consists', 'of', 'electrodequantum', 'wellqwdotqwelec... | [-0.15085409509125525, 0.19555211024018052, -0.0406333150476959, 0.03760732186123796, -0.001539033361419833, -0.16376124509943152, 0.04635931232130804, 0.3682305669966175, -0.27649845151342367, -0.2732402283647751, 0.032928950252323265, -0.2851242871946609, -0.07987764005009844, 0.20458877385947938, 0.04244218236130422... |
708.1505 | How much is a quantum controller controlled by the controlled system? | We consider unitary transformations on a bipartite system A x B. To what
extent entails the ability to transmit information from A to B the ability to
transfer information in the converse direction? We prove a dimension-dependent
lower bound on the classical channel capacity C(A<--B) in terms of the capacity
C(A-->B)... | quant-ph | we consider unitary transformations on a bipartite system a x b to what extent entails the ability to transmit information from a to b the ability to transfer information in the converse direction we prove a dimensiondependent lower bound on the classical channel capacity cab in terms of the capacity cab for the case t... | [['we', 'consider', 'unitary', 'transformations', 'on', 'a', 'bipartite', 'system', 'a', 'x', 'b', 'to', 'what', 'extent', 'entails', 'the', 'ability', 'to', 'transmit', 'information', 'from', 'a', 'to', 'b', 'the', 'ability', 'to', 'transfer', 'information', 'in', 'the', 'converse', 'direction', 'we', 'prove', 'a', 'd... | [-0.1662930135477643, 0.1394542736915746, -0.07469463462753154, 0.028528645866275452, -0.06115592947142884, -0.1451141275682636, 0.10762790349611308, 0.34101877519812607, -0.2850601780928015, -0.26476985835253114, 0.10982229493237511, -0.2698910517275449, -0.10354888325175898, 0.19094163537932646, -0.07953066561235973,... |
708.1506 | A Soft Interaction Model at Ultra High Energies: Amplitudes, Cross
Sections and Survival Probabilities | In this paper we present a two channel model with the goal of reproducing the
soft scattering data available in the ISR-Tevatron energy range, and extend the
model results to LHC and Cosmic Rays energies. A characteristic feature of the
model is that we represent the sum of all diffractive final states at a vertex,
b... | hep-ph | in this paper we present a two channel model with the goal of reproducing the soft scattering data available in the isrtevatron energy range and extend the model results to lhc and cosmic rays energies a characteristic feature of the model is that we represent the sum of all diffractive final states at a vertex by a si... | [['in', 'this', 'paper', 'we', 'present', 'a', 'two', 'channel', 'model', 'with', 'the', 'goal', 'of', 'reproducing', 'the', 'soft', 'scattering', 'data', 'available', 'in', 'the', 'isrtevatron', 'energy', 'range', 'and', 'extend', 'the', 'model', 'results', 'to', 'lhc', 'and', 'cosmic', 'rays', 'energies', 'a', 'chara... | [-0.05650578664622086, 0.1864615845927362, -0.11014337558299303, 0.11680671308493736, -0.02678839918099293, -0.10464191949628547, 0.00996122501717665, 0.3636794730412717, -0.22860546636578888, -0.28189137933433667, 0.03164125174651442, -0.3182845046414303, -0.04609008080074183, 0.16654457920389312, 0.016916763770780493... |
708.1507 | Quaternionic and Poisson-Lie structures in 3d gravity: the cosmological
constant as deformation parameter | Each of the local isometry groups arising in 3d gravity can be viewed as the
group of unit (split) quaternions over a ring which depends on the cosmological
constant. In this paper we explain and prove this statement, and use it as a
unifying framework for studying Poisson structures associated with the local
isometr... | gr-qc hep-th math-ph math.MP | each of the local isometry groups arising in 3d gravity can be viewed as the group of unit split quaternions over a ring which depends on the cosmological constant in this paper we explain and prove this statement and use it as a unifying framework for studying poisson structures associated with the local isometry grou... | [['each', 'of', 'the', 'local', 'isometry', 'groups', 'arising', 'in', '3d', 'gravity', 'can', 'be', 'viewed', 'as', 'the', 'group', 'of', 'unit', 'split', 'quaternions', 'over', 'a', 'ring', 'which', 'depends', 'on', 'the', 'cosmological', 'constant', 'in', 'this', 'paper', 'we', 'explain', 'and', 'prove', 'this', 'st... | [-0.15625315800999964, 0.07590358317613799, -0.0779502076522404, 0.07350107514151427, -0.1062700428925948, -0.11731598438966452, 0.0017861864993669438, 0.3707207122089847, -0.30639591017145884, -0.2529842293087319, 0.10143778726862533, -0.2147033970050563, -0.17368279733627245, 0.16758839562704897, -0.07981961478312678... |
708.1508 | Elliptic Flow arising from Ridges due to Semi-hard Scattering | Azimuthal anisotropy in heavy-ion collisions is studied by taking into
account the ridges generated by semi-hard scattering of intermediate-momentum
partons, which can be sensitive to the initial spatial configuration of the
medium in non-central collisions. In a simple treatment of the problem where
the recombinatio... | nucl-th | azimuthal anisotropy in heavyion collisions is studied by taking into account the ridges generated by semihard scattering of intermediatemomentum partons which can be sensitive to the initial spatial configuration of the medium in noncentral collisions in a simple treatment of the problem where the recombination of onl... | [['azimuthal', 'anisotropy', 'in', 'heavyion', 'collisions', 'is', 'studied', 'by', 'taking', 'into', 'account', 'the', 'ridges', 'generated', 'by', 'semihard', 'scattering', 'of', 'intermediatemomentum', 'partons', 'which', 'can', 'be', 'sensitive', 'to', 'the', 'initial', 'spatial', 'configuration', 'of', 'the', 'med... | [-0.04548569414115602, 0.28572623455995877, -0.19185171460947104, 0.14564683359215216, -0.009565744670602469, -0.08906522505881627, -0.1294509815629077, 0.42012311488521836, -0.20952287793934213, -0.26476987204473235, -0.03498632921136718, -0.3122293295058529, 0.08695303829823646, 0.1562274119083201, 0.0332168779400047... |
708.1509 | X-ray flares, plateaus, and chromatic breaks of GRB afterglows from
up-scattered forward-shock emission | Scattering of the forward-shock synchrotron emission by a relativistic
outflow located behind the leading blast-wave may produce an X-ray emission
brighter than that coming directly from the forward-shock and may explain four
features displayed by Swift X-ray afterglows: flares, plateaus (slow decays),
chromatic ligh... | astro-ph | scattering of the forwardshock synchrotron emission by a relativistic outflow located behind the leading blastwave may produce an xray emission brighter than that coming directly from the forwardshock and may explain four features displayed by swift xray afterglows flares plateaus slow decays chromatic lightcurve break... | [['scattering', 'of', 'the', 'forwardshock', 'synchrotron', 'emission', 'by', 'a', 'relativistic', 'outflow', 'located', 'behind', 'the', 'leading', 'blastwave', 'may', 'produce', 'an', 'xray', 'emission', 'brighter', 'than', 'that', 'coming', 'directly', 'from', 'the', 'forwardshock', 'and', 'may', 'explain', 'four', ... | [-0.03150491188166708, 0.22948548482307204, -0.09114916575693988, 0.1820047515670663, -0.13013659180160914, -0.1382903074807813, 0.00654028696803058, 0.4500284835230559, -0.2651911846085686, -0.2976447589188148, 0.03193382064649093, -0.32027810908914583, 0.011238348009670532, 0.2218105386548895, 0.009808083263612011, -... |
708.151 | Connecting GRBs and galaxies: the probability of chance coincidence | Studies of GRB host galaxies are crucial to understanding GRBs. However,
since they are identified by the superposition in the plane of the sky of a GRB
afterglow and a galaxy there is always a possibility that an association
represents a chance alignment, rather than a physical connection. We examine a
uniform sampl... | astro-ph | studies of grb host galaxies are crucial to understanding grbs however since they are identified by the superposition in the plane of the sky of a grb afterglow and a galaxy there is always a possibility that an association represents a chance alignment rather than a physical connection we examine a uniform sample of 7... | [['studies', 'of', 'grb', 'host', 'galaxies', 'are', 'crucial', 'to', 'understanding', 'grbs', 'however', 'since', 'they', 'are', 'identified', 'by', 'the', 'superposition', 'in', 'the', 'plane', 'of', 'the', 'sky', 'of', 'a', 'grb', 'afterglow', 'and', 'a', 'galaxy', 'there', 'is', 'always', 'a', 'possibility', 'that'... | [-0.09004543157994377, 0.12537466421175245, -0.06483222912543286, 0.16687084218555798, -0.12498899585065934, -0.09666252774425232, 0.09098959486716642, 0.4704614812269425, -0.16415748860125837, -0.31281629510116404, 0.04679558748000254, -0.31199717911509556, -0.05693958008076805, 0.21045549559997967, -0.034391712827178... |
708.1511 | Simultaneous Multi-Wavelength Observations of Magnetic Activity in
Ultracool Dwarfs. I. The Complex Behavior of the M8.5 Dwarf TVLM513-46546 | [Abridged] We present the first simultaneous radio, X-ray, ultraviolet, and
optical spectroscopic observations of the M8.5 dwarf TVLM513-46546, with a
duration of 9 hours. These observations are part of a program to study the
origin of magnetic activity in ultracool dwarfs, and its impact on
chromospheric and coronal... | astro-ph | abridged we present the first simultaneous radio xray ultraviolet and optical spectroscopic observations of the m85 dwarf tvlm51346546 with a duration of 9 hours these observations are part of a program to study the origin of magnetic activity in ultracool dwarfs and its impact on chromospheric and coronal emission her... | [['abridged', 'we', 'present', 'the', 'first', 'simultaneous', 'radio', 'xray', 'ultraviolet', 'and', 'optical', 'spectroscopic', 'observations', 'of', 'the', 'm85', 'dwarf', 'tvlm51346546', 'with', 'a', 'duration', 'of', '9', 'hours', 'these', 'observations', 'are', 'part', 'of', 'a', 'program', 'to', 'study', 'the', ... | [-0.09559250487512469, 0.15206153947849624, -0.04631433360460963, 0.11121008539502346, -0.1179194585469037, -0.09095953331797846, 0.07762793132178876, 0.46044833474251984, -0.14923166205546448, -0.36352058698446, 0.09649542644758338, -0.29117236539096264, -0.07468795429482092, 0.2376724646835412, -0.023454381081347283,... |
708.1512 | Solving the Hamiltonian path problem with a light-based computer | In this paper we propose a special computational device which uses light rays
for solving the Hamiltonian path problem on a directed graph. The device has a
graph-like representation and the light is traversing it by following the
routes given by the connections between nodes. In each node the rays are
uniquely marke... | cs.AR cs.DC | in this paper we propose a special computational device which uses light rays for solving the hamiltonian path problem on a directed graph the device has a graphlike representation and the light is traversing it by following the routes given by the connections between nodes in each node the rays are uniquely marked so ... | [['in', 'this', 'paper', 'we', 'propose', 'a', 'special', 'computational', 'device', 'which', 'uses', 'light', 'rays', 'for', 'solving', 'the', 'hamiltonian', 'path', 'problem', 'on', 'a', 'directed', 'graph', 'the', 'device', 'has', 'a', 'graphlike', 'representation', 'and', 'the', 'light', 'is', 'traversing', 'it', '... | [-0.14965306271405257, 0.13445553369820118, -0.09240022957440197, 0.009827625774538395, -0.10968847049534627, -0.1771578008798671, 0.10420779895983137, 0.44025470131105676, -0.3361751086164996, -0.31573232113546934, 0.055791634450589794, -0.2984219395685173, -0.1712367181502974, 0.16967065609060228, -0.0718155887131531... |
708.1513 | Low Resolution Spectral Templates For Galaxies From 0.2 -- 10 microns | We built an optimal basis of low resolution templates for galaxies over the
wavelength range from 0.2 to 10 $\mu$m using a variant of the algorithm
presented by Budavari et al. (2000). We derived them using eleven bands of
photometry from the NDWFS, FLAMEX, zBo\"otes and IRAC Shallow surveys for 16033
galaxies in the... | astro-ph | we built an optimal basis of low resolution templates for galaxies over the wavelength range from 02 to 10 mum using a variant of the algorithm presented by budavari et al 2000 we derived them using eleven bands of photometry from the ndwfs flamex zbootes and irac shallow surveys for 16033 galaxies in the ndwfs bootes ... | [['we', 'built', 'an', 'optimal', 'basis', 'of', 'low', 'resolution', 'templates', 'for', 'galaxies', 'over', 'the', 'wavelength', 'range', 'from', '02', 'to', '10', 'mum', 'using', 'a', 'variant', 'of', 'the', 'algorithm', 'presented', 'by', 'budavari', 'et', 'al', '2000', 'we', 'derived', 'them', 'using', 'eleven', '... | [0.02775268949658817, 0.01697397585606571, -0.09372626104353306, 0.10255298392035507, -0.08924523568485812, -0.048070563601666234, 0.06354420439391914, 0.4942254150131096, -0.12487735367418888, -0.37770295281532323, 0.045676729581221785, -0.300792642228771, -0.04608463696179873, 0.21371743657962522, -0.0636654072602848... |
708.1514 | UCD Candidates in the Hydra Cluster | NGC 3311, the giant cD galaxy in the Hydra cluster (A1060), has one of the
largest globular cluster systems known. We describe new Gemini GMOS (g',i')
photometry of the NGC 3311 field which reveals that the red, metal-rich side of
its globular cluster population extends smoothly upward into the mass range
associated ... | astro-ph | ngc 3311 the giant cd galaxy in the hydra cluster a1060 has one of the largest globular cluster systems known we describe new gemini gmos gi photometry of the ngc 3311 field which reveals that the red metalrich side of its globular cluster population extends smoothly upward into the mass range associated with the new c... | [['ngc', '3311', 'the', 'giant', 'cd', 'galaxy', 'in', 'the', 'hydra', 'cluster', 'a1060', 'has', 'one', 'of', 'the', 'largest', 'globular', 'cluster', 'systems', 'known', 'we', 'describe', 'new', 'gemini', 'gmos', 'gi', 'photometry', 'of', 'the', 'ngc', '3311', 'field', 'which', 'reveals', 'that', 'the', 'red', 'metal... | [-0.07455444449085023, 0.08647977886721492, -0.11215009397761733, 0.08559601831968808, -0.15337352565767473, -0.05103270313702524, 0.03726906721120733, 0.4105944506693305, -0.1779174159287083, -0.3318886598418957, 0.014846987683293327, -0.256100243417007, -0.06411029306534481, 0.20941265112834803, -0.07785362871608843,... |
708.1515 | Supernova Remnants in the Large Magellanic Clouds IX: Multiwavelength
Analysis of the Physical Structure of N49 | We present a multiwavelength analysis of the supernova remnant N49 in the
Large Magellanic Cloud. Using high-resolution Hubble Space Telescope WFPC2
images of H-alpha, [S II] and [O III] emission, we study the morphology of the
remnant and calculate the rms electron densities in different regions. We
detect an offset... | astro-ph | we present a multiwavelength analysis of the supernova remnant n49 in the large magellanic cloud using highresolution hubble space telescope wfpc2 images of halpha s ii and o iii emission we study the morphology of the remnant and calculate the rms electron densities in different regions we detect an offset of o iii an... | [['we', 'present', 'a', 'multiwavelength', 'analysis', 'of', 'the', 'supernova', 'remnant', 'n49', 'in', 'the', 'large', 'magellanic', 'cloud', 'using', 'highresolution', 'hubble', 'space', 'telescope', 'wfpc2', 'images', 'of', 'halpha', 's', 'ii', 'and', 'o', 'iii', 'emission', 'we', 'study', 'the', 'morphology', 'of'... | [-0.05976404306711629, 0.07503738402406587, -0.05465100964011495, 0.06866589228969154, -0.08342113414735988, -0.06270285957319618, 0.042945854037155416, 0.4818998328994873, -0.19997138385173627, -0.33868733471216156, 0.0640559605068289, -0.31210781149566175, 0.01875216395182665, 0.16037972034280037, 0.01930366487047353... |
708.1516 | Spectral evolution of non-thermal electron distributions in intense
radiation fields | (abridged) Models of many astrophysical gamma-ray sources assume they contain
a homogeneous distribution of electrons that are injected as a power-law in
energy and evolve by interacting with radiation fields, magnetic fields and
particles in the source and by escaping. This problem is particularly
complicated if the... | astro-ph | abridged models of many astrophysical gammaray sources assume they contain a homogeneous distribution of electrons that are injected as a powerlaw in energy and evolve by interacting with radiation fields magnetic fields and particles in the source and by escaping this problem is particularly complicated if the radiati... | [['abridged', 'models', 'of', 'many', 'astrophysical', 'gammaray', 'sources', 'assume', 'they', 'contain', 'a', 'homogeneous', 'distribution', 'of', 'electrons', 'that', 'are', 'injected', 'as', 'a', 'powerlaw', 'in', 'energy', 'and', 'evolve', 'by', 'interacting', 'with', 'radiation', 'fields', 'magnetic', 'fields', '... | [-0.056836055694147944, 0.17415620689064962, -0.0805884331691941, 0.14945410664798692, -0.06833954635821284, -0.11282586287334562, 0.005816232464276254, 0.41533559273183346, -0.25621608329750595, -0.3140096566155553, 0.041375776837579904, -0.2926064686998725, -0.02233686095383018, 0.2182227612058632, 0.0568910639625974... |
708.1517 | The galaxy power spectrum: precision cosmology from large scale
structure? | Published galaxy power spectra from the 2dFGRS and SDSS are not in good
agreement. We revisit this issue by analyzing both the 2dFGRS and SDSS DR5
catalogues using essentially identical techniques. We confirm that the 2dFGRS
exhibits relatively more large scale power than the SDSS, or, equivalently,
SDSS has more sma... | astro-ph | published galaxy power spectra from the 2dfgrs and sdss are not in good agreement we revisit this issue by analyzing both the 2dfgrs and sdss dr5 catalogues using essentially identical techniques we confirm that the 2dfgrs exhibits relatively more large scale power than the sdss or equivalently sdss has more small scal... | [['published', 'galaxy', 'power', 'spectra', 'from', 'the', '2dfgrs', 'and', 'sdss', 'are', 'not', 'in', 'good', 'agreement', 'we', 'revisit', 'this', 'issue', 'by', 'analyzing', 'both', 'the', '2dfgrs', 'and', 'sdss', 'dr5', 'catalogues', 'using', 'essentially', 'identical', 'techniques', 'we', 'confirm', 'that', 'the... | [-0.03216457815845958, 0.0634933350259786, -0.11669815576617391, 0.13218340885547422, -0.13539377608142056, -0.09089482757825773, 0.0095174467040144, 0.37236727875121783, -0.2090756979944942, -0.35842993479024193, 0.05432571860195748, -0.3501555594417775, -0.07414686629777235, 0.2334426638590097, -0.03555362521467778, ... |
708.1518 | Cluster Structure in Cosmological Simulations I: Correlation to
Observables, Mass Estimates, and Evolution | We use Enzo, a hybrid Eulerian AMR/N-body code including non-gravitational
heating and cooling, to explore the morphology of the X-ray gas in clusters of
galaxies and its evolution in current generation cosmological simulations. We
employ and compare two observationally motivated structure measures: power
ratios and ... | astro-ph | we use enzo a hybrid eulerian amrnbody code including nongravitational heating and cooling to explore the morphology of the xray gas in clusters of galaxies and its evolution in current generation cosmological simulations we employ and compare two observationally motivated structure measures power ratios and centroid s... | [['we', 'use', 'enzo', 'a', 'hybrid', 'eulerian', 'amrnbody', 'code', 'including', 'nongravitational', 'heating', 'and', 'cooling', 'to', 'explore', 'the', 'morphology', 'of', 'the', 'xray', 'gas', 'in', 'clusters', 'of', 'galaxies', 'and', 'its', 'evolution', 'in', 'current', 'generation', 'cosmological', 'simulations... | [-0.07865262042095482, 0.10672512943191188, -0.09684462766554099, 0.13420241224882012, -0.08782798821343879, -0.05331538336056655, 0.05995823799868017, 0.4363172718802014, -0.2347180056498066, -0.3500775359067562, 0.0693005004912996, -0.25792511860735745, -0.061693017056362855, 0.19656401694640804, -0.00691067527361127... |
708.1519 | Classical Theory of Optical Nonlinearity in Conducting Nanoparticles | We develop a classical theory of electron confinement in conducting
nanoparticles. The theory is used to compute the nonlinear optical response of
the nanoparticle to a harmonic external field.
| physics.optics physics.class-ph | we develop a classical theory of electron confinement in conducting nanoparticles the theory is used to compute the nonlinear optical response of the nanoparticle to a harmonic external field | [['we', 'develop', 'a', 'classical', 'theory', 'of', 'electron', 'confinement', 'in', 'conducting', 'nanoparticles', 'the', 'theory', 'is', 'used', 'to', 'compute', 'the', 'nonlinear', 'optical', 'response', 'of', 'the', 'nanoparticle', 'to', 'a', 'harmonic', 'external', 'field']] | [-0.10420753215921336, 0.1577941108944601, -0.1062427186246576, 0.05140072087644888, -0.04277162003363001, -0.12034575265414756, 0.00887574026650139, 0.3917614934516364, -0.2569411703353298, -0.2591430639912342, -0.0012088723255899445, -0.26366594164022084, -0.1898048359515338, 0.16298619233842554, -0.01326368126119005... |
708.152 | Coulomb blockade in a Si channel gated by an Al single-electron
transistor | We incorporate an Al-AlO_x-Al single-electron transistor as the gate of a
narrow (~100 nm) metal-oxide-semiconductor field-effect transistor (MOSFET).
Near the MOSFET channel conductance threshold, we observe oscillations in the
conductance associated with Coulomb blockade in the channel, revealing the
formation of a... | cond-mat.mes-hall | we incorporate an alalo_xal singleelectron transistor as the gate of a narrow 100 nm metaloxidesemiconductor fieldeffect transistor mosfet near the mosfet channel conductance threshold we observe oscillations in the conductance associated with coulomb blockade in the channel revealing the formation of a si singleelectr... | [['we', 'incorporate', 'an', 'alalo_xal', 'singleelectron', 'transistor', 'as', 'the', 'gate', 'of', 'a', 'narrow', '100', 'nm', 'metaloxidesemiconductor', 'fieldeffect', 'transistor', 'mosfet', 'near', 'the', 'mosfet', 'channel', 'conductance', 'threshold', 'we', 'observe', 'oscillations', 'in', 'the', 'conductance', ... | [-0.2162382727505506, 0.11517509364375274, 0.02278316870418342, -0.03070503527576401, 0.06833037083279811, -0.31683464237770553, 0.11146336543264196, 0.4086661990653692, -0.20901193029145484, -0.3251721754106654, -0.12423211780274991, -0.3232368650384435, -0.1528844152872662, 0.21950570652222245, -0.05659830262258399, ... |
708.1521 | Spectroscopy of horizontal branch stars in NGC6752 - Anomalous results
on atmospheric parameters and masses | We used the ESO VLT-FORS2 facility to collect low-resolution spectra of 51
targets distributed along the Horizontal Branch. We determined atmospheric
parameters by comparison with theoretical models through standard fitting
routines, and masses by basic equations. Results are in general in good
agreement with previou... | astro-ph | we used the eso vltfors2 facility to collect lowresolution spectra of 51 targets distributed along the horizontal branch we determined atmospheric parameters by comparison with theoretical models through standard fitting routines and masses by basic equations results are in general in good agreement with previous works... | [['we', 'used', 'the', 'eso', 'vltfors2', 'facility', 'to', 'collect', 'lowresolution', 'spectra', 'of', '51', 'targets', 'distributed', 'along', 'the', 'horizontal', 'branch', 'we', 'determined', 'atmospheric', 'parameters', 'by', 'comparison', 'with', 'theoretical', 'models', 'through', 'standard', 'fitting', 'routin... | [-0.04316591256513046, 0.1487344048554615, -0.07441094251884985, 0.08559803251904786, -0.08136837922417473, -0.1269878611960241, 0.10244947214618416, 0.4397150701447296, -0.14597388849403287, -0.36964056286668623, 0.052050844134634684, -0.3160133782759128, -0.029235455141542292, 0.20849388351792145, -0.0720240645115570... |
708.1522 | Electron Thermal Microscopy | The progress of semiconductor electronics toward ever-smaller length scales
and associated higher power densities brings a need for new high-resolution
thermal microscopy techniques. Traditional thermal microscopy is performed by
detecting infrared radiation with far-field optics, where the resolution is
limited by t... | cond-mat.mtrl-sci | the progress of semiconductor electronics toward eversmaller length scales and associated higher power densities brings a need for new highresolution thermal microscopy techniques traditional thermal microscopy is performed by detecting infrared radiation with farfield optics where the resolution is limited by the wave... | [['the', 'progress', 'of', 'semiconductor', 'electronics', 'toward', 'eversmaller', 'length', 'scales', 'and', 'associated', 'higher', 'power', 'densities', 'brings', 'a', 'need', 'for', 'new', 'highresolution', 'thermal', 'microscopy', 'techniques', 'traditional', 'thermal', 'microscopy', 'is', 'performed', 'by', 'det... | [-0.08163480626535602, 0.15400952847429786, -0.09867325107150368, -0.011440364970200645, -0.05277896412850456, -0.14847397305359328, 0.047679440103820525, 0.4142464650978677, -0.27624637647960826, -0.3337039360286374, 0.06886256896694631, -0.29986633046064526, -0.10300502018684424, 0.2808783628911203, -0.06126162660994... |
708.1523 | Chemical Complexity in Galaxies | ALMA will be able to detect a broad spectrum of molecular lines in galaxies.
Current aperture synthesis observations indicate that the molecular line
emission from galaxies is remarkably variable, even on kpc scales. Imaging
spectroscopy at resolutions of an arcsecond or better will reduce the chemical
complexity by ... | astro-ph | alma will be able to detect a broad spectrum of molecular lines in galaxies current aperture synthesis observations indicate that the molecular line emission from galaxies is remarkably variable even on kpc scales imaging spectroscopy at resolutions of an arcsecond or better will reduce the chemical complexity by allow... | [['alma', 'will', 'be', 'able', 'to', 'detect', 'a', 'broad', 'spectrum', 'of', 'molecular', 'lines', 'in', 'galaxies', 'current', 'aperture', 'synthesis', 'observations', 'indicate', 'that', 'the', 'molecular', 'line', 'emission', 'from', 'galaxies', 'is', 'remarkably', 'variable', 'even', 'on', 'kpc', 'scales', 'imag... | [-0.04679817397695372, 0.05514731842864923, -0.06716325215128219, 0.053472770243513816, -0.08181528014468094, -0.13074747065146422, 0.027363345267829197, 0.4782032906238375, -0.19968553027138114, -0.3373633476359577, 0.10761378251682517, -0.22782465376377362, -0.01848020869034246, 0.20275772593770947, -0.02027294304671... |
708.1524 | Discovery of Two Dust Pillars near the Galactic Plane | We report the discovery of two dust pillars using GLIMPSE archival images
obtained with the Infrared Array Camera on board the Spitzer Space Telescope.
They are located close to the Galactic molecular cloud GRSMC45.453+0.060 and
they appear to be aligned with the ionizing region associated with
GRSMC45.478+0.131. Our... | astro-ph | we report the discovery of two dust pillars using glimpse archival images obtained with the infrared array camera on board the spitzer space telescope they are located close to the galactic molecular cloud grsmc454530060 and they appear to be aligned with the ionizing region associated with grsmc454780131 our three col... | [['we', 'report', 'the', 'discovery', 'of', 'two', 'dust', 'pillars', 'using', 'glimpse', 'archival', 'images', 'obtained', 'with', 'the', 'infrared', 'array', 'camera', 'on', 'board', 'the', 'spitzer', 'space', 'telescope', 'they', 'are', 'located', 'close', 'to', 'the', 'galactic', 'molecular', 'cloud', 'grsmc4545300... | [-0.08337342770508013, 0.1167633436315012, -0.06527016461365112, 0.05230443625409594, -0.09717339668970774, -0.052801831586270775, 0.010569322870911233, 0.468032184033459, -0.17759096212420972, -0.36799052187844233, 0.08382444705974561, -0.27262558081351657, -0.10145445266628966, 0.1608484354742779, -0.0653752244467467... |
708.1525 | Using gamma-rays to probe the clumped structure of stellar winds | Gamma-rays can be produced by the interaction of a relativistic jet and the
matter of the stellar wind in the subclass of massive X-ray binaries known as
"microquasars". The relativistic jet is ejected from the surroundings of the
compact object and interacts with cold protons from the stellar wind, producing
pions t... | astro-ph | gammarays can be produced by the interaction of a relativistic jet and the matter of the stellar wind in the subclass of massive xray binaries known as microquasars the relativistic jet is ejected from the surroundings of the compact object and interacts with cold protons from the stellar wind producing pions that then... | [['gammarays', 'can', 'be', 'produced', 'by', 'the', 'interaction', 'of', 'a', 'relativistic', 'jet', 'and', 'the', 'matter', 'of', 'the', 'stellar', 'wind', 'in', 'the', 'subclass', 'of', 'massive', 'xray', 'binaries', 'known', 'as', 'microquasars', 'the', 'relativistic', 'jet', 'is', 'ejected', 'from', 'the', 'surrou... | [-0.05746633221613283, 0.24044406383318154, -0.0544582715931725, 0.14781221267370942, -0.0849539924954586, -0.06712713779993884, -0.016518242049513132, 0.4014439414261926, -0.25235408066659637, -0.3407826236521838, 0.010235503209417964, -0.2925419372684778, 0.011777581977294692, 0.24925912196701722, 0.00520183011255365... |
708.1526 | Limitations on the extent of off-center displacements in TbMnO3 from
EXAFS measurements | We present EXAFS data at the Mn K and Tb L3 edges that provide upper limits
on the possible displacements of any atoms in TbMnO3. The displacements must be
less than 0.005-0.01A for all atoms which eliminates the possibility of
moderate distortions (0.02A) with a small c-axis component, but for which the
displacement... | cond-mat.str-el cond-mat.mtrl-sci | we present exafs data at the mn k and tb l3 edges that provide upper limits on the possible displacements of any atoms in tbmno3 the displacements must be less than 0005001a for all atoms which eliminates the possibility of moderate distortions 002a with a small caxis component but for which the displacements in the ab... | [['we', 'present', 'exafs', 'data', 'at', 'the', 'mn', 'k', 'and', 'tb', 'l3', 'edges', 'that', 'provide', 'upper', 'limits', 'on', 'the', 'possible', 'displacements', 'of', 'any', 'atoms', 'in', 'tbmno3', 'the', 'displacements', 'must', 'be', 'less', 'than', '0005001a', 'for', 'all', 'atoms', 'which', 'eliminates', 't... | [-0.11548530138108097, 0.18715990179576433, -0.007169604559229421, -0.016828987819150956, -0.004812284651312179, -0.07635021334863268, 0.09421460075100185, 0.4141254417149217, -0.30208072162765476, -0.2741934002925908, 0.04176409515639534, -0.33947139560145195, -0.042159691334485876, 0.1530866970507694, 0.0651906861832... |
708.1527 | A Data-Parallel Version of Aleph | This is to present work on modifying the Aleph ILP system so that it
evaluates the hypothesised clauses in parallel by distributing the data-set
among the nodes of a parallel or distributed machine. The paper briefly
discusses MPI, the interface used to access message- passing libraries for
parallel computers and clu... | cs.AI cs.DC | this is to present work on modifying the aleph ilp system so that it evaluates the hypothesised clauses in parallel by distributing the dataset among the nodes of a parallel or distributed machine the paper briefly discusses mpi the interface used to access message passing libraries for parallel computers and clusters ... | [['this', 'is', 'to', 'present', 'work', 'on', 'modifying', 'the', 'aleph', 'ilp', 'system', 'so', 'that', 'it', 'evaluates', 'the', 'hypothesised', 'clauses', 'in', 'parallel', 'by', 'distributing', 'the', 'dataset', 'among', 'the', 'nodes', 'of', 'a', 'parallel', 'or', 'distributed', 'machine', 'the', 'paper', 'brief... | [-0.13118359714411618, 0.04671146873344819, -0.06898045307548528, 0.013190448790359615, -0.10805326177257249, -0.17358884576896436, 0.06831261860285205, 0.3909709295362569, -0.3179175955703838, -0.33114288562092553, 0.06755603630529988, -0.2632602576082677, -0.05459117417726038, 0.190894200108171, -0.0270480254659785, ... |
708.1528 | Rankin-Cohen Deformations and Representation Theory | In this paper, we use the unitary representation theory of $SL_2(\mathbb R)$
to understand the Rankin-Cohen brackets for modular forms. Then we use this
interpretation to study the corresponding deformation problems that Paula
Cohen, Yuri Manin and Don Zagier initiated. Two uniqueness results are
established.
| math.QA math.CO | in this paper we use the unitary representation theory of sl_2mathbb r to understand the rankincohen brackets for modular forms then we use this interpretation to study the corresponding deformation problems that paula cohen yuri manin and don zagier initiated two uniqueness results are established | [['in', 'this', 'paper', 'we', 'use', 'the', 'unitary', 'representation', 'theory', 'of', 'sl_2mathbb', 'r', 'to', 'understand', 'the', 'rankincohen', 'brackets', 'for', 'modular', 'forms', 'then', 'we', 'use', 'this', 'interpretation', 'to', 'study', 'the', 'corresponding', 'deformation', 'problems', 'that', 'paula', ... | [-0.14579869946464896, 0.027971085706829196, -0.1254561578647958, 0.11134684132929477, -0.13379318005301885, -0.0801327396184206, -0.012855367507371637, 0.3060423507458634, -0.32663010189102754, -0.22265742369410063, 0.056526836905524964, -0.23349485324902666, -0.2992004343205028, 0.16138857754154337, -0.15932533620960... |
708.1529 | Resolution over Linear Equations and Multilinear Proofs | We develop and study the complexity of propositional proof systems of varying
strength extending resolution by allowing it to operate with disjunctions of
linear equations instead of clauses. We demonstrate polynomial-size refutations
for hard tautologies like the pigeonhole principle, Tseitin graph tautologies
and t... | cs.CC cs.LO | we develop and study the complexity of propositional proof systems of varying strength extending resolution by allowing it to operate with disjunctions of linear equations instead of clauses we demonstrate polynomialsize refutations for hard tautologies like the pigeonhole principle tseitin graph tautologies and the cl... | [['we', 'develop', 'and', 'study', 'the', 'complexity', 'of', 'propositional', 'proof', 'systems', 'of', 'varying', 'strength', 'extending', 'resolution', 'by', 'allowing', 'it', 'to', 'operate', 'with', 'disjunctions', 'of', 'linear', 'equations', 'instead', 'of', 'clauses', 'we', 'demonstrate', 'polynomialsize', 'ref... | [-0.11009500317643266, 0.048319892304534394, -0.08205239196899826, 0.09796779976328661, -0.12150730658540171, -0.19187156236638037, 0.06344481036458686, 0.303853199858584, -0.30372121995401996, -0.3048124501686195, 0.11052724982124414, -0.21611616347925128, -0.08747193449564174, 0.246930344034613, -0.1031696438221163, ... |
708.153 | Nontrivial quantized Berry phases for itinerant spin liquids | Quantized Berry phases as local order parameters in t-J models are studied. A
texture pattern of the local order parameters is topologically stable due to
the quantization of non-Abelian Berry phases defined by low-energy states below
a spin gap, which exists in the large J/t case with a few electrons. We have
confir... | cond-mat.str-el | quantized berry phases as local order parameters in tj models are studied a texture pattern of the local order parameters is topologically stable due to the quantization of nonabelian berry phases defined by lowenergy states below a spin gap which exists in the large jt case with a few electrons we have confirmed that ... | [['quantized', 'berry', 'phases', 'as', 'local', 'order', 'parameters', 'in', 'tj', 'models', 'are', 'studied', 'a', 'texture', 'pattern', 'of', 'the', 'local', 'order', 'parameters', 'is', 'topologically', 'stable', 'due', 'to', 'the', 'quantization', 'of', 'nonabelian', 'berry', 'phases', 'defined', 'by', 'lowenergy'... | [-0.24541312489817116, 0.32117768044291223, -0.011395268023331115, 0.06531936044438168, -0.014326421761924916, -0.1836248875070522, 0.06613694041214407, 0.31852645706385374, -0.25367372645501124, -0.2853763608182681, -0.002345631572794407, -0.3101814196227079, -0.16139382336714722, 0.0819814927514365, 0.019435858562033... |
708.1531 | "Unusual" critical states in type-II superconductors | We give a theoretical description of the general critical states in which the
critical currents in type-II superconductors are not perpendicular to the local
magnetic induction. Such states frequently occur in real situations, e.g., when
the sample shape is not sufficiently symmetric or the direction of the external
... | cond-mat.supr-con | we give a theoretical description of the general critical states in which the critical currents in typeii superconductors are not perpendicular to the local magnetic induction such states frequently occur in real situations eg when the sample shape is not sufficiently symmetric or the direction of the external magnetic... | [['we', 'give', 'a', 'theoretical', 'description', 'of', 'the', 'general', 'critical', 'states', 'in', 'which', 'the', 'critical', 'currents', 'in', 'typeii', 'superconductors', 'are', 'not', 'perpendicular', 'to', 'the', 'local', 'magnetic', 'induction', 'such', 'states', 'frequently', 'occur', 'in', 'real', 'situatio... | [-0.16681196961792247, 0.17946517146643132, -0.03777534569944105, 0.053295032264694814, -0.06221363914589728, -0.10097570966538642, 0.03532004696767657, 0.38065037049593464, -0.28084811170795754, -0.26333651564444505, 0.08519776439023835, -0.23923773198959328, -0.11344459285629133, 0.20357868756588188, -0.0072099628163... |
708.1532 | Surface plasmon polaritons assisted diffraction in periodic
subwavelength holes of metal films with reduced interplane coupling | Metal films grown on Si wafer perforated with a periodic array of
subwavelength holes have been fabricated and anomalous enhanced transmission in
the mid-infrared regime has been observed. High order transmission peaks up to
Si(2,2) are clearly revealed due to the large dielectric constant contrast of
the dielectrics... | cond-mat.mes-hall cond-mat.mtrl-sci | metal films grown on si wafer perforated with a periodic array of subwavelength holes have been fabricated and anomalous enhanced transmission in the midinfrared regime has been observed high order transmission peaks up to si22 are clearly revealed due to the large dielectric constant contrast of the dielectrics at the... | [['metal', 'films', 'grown', 'on', 'si', 'wafer', 'perforated', 'with', 'a', 'periodic', 'array', 'of', 'subwavelength', 'holes', 'have', 'been', 'fabricated', 'and', 'anomalous', 'enhanced', 'transmission', 'in', 'the', 'midinfrared', 'regime', 'has', 'been', 'observed', 'high', 'order', 'transmission', 'peaks', 'up',... | [-0.1563460999071443, 0.1817922659896188, -0.04600455206430828, -0.02367102175170051, -0.0400562953006253, -0.19850218148591617, 0.0443008115713989, 0.49323046995171654, -0.20429111756190346, -0.2943670120390986, 0.022743203247955535, -0.3804089382271438, -0.13964509992122962, 0.22586393288414305, 0.03516577622697999, ... |
708.1533 | Magnetic fields and gas in the cluster influenced spiral galaxy NGC4254
- I. Radio and X-rays observations | Radio observations can show how cluster galaxies are affected by various
environmental factors. We made three frequency radio-polarimetric VLA
observations and performed sensitive XMM-Newton observations in X-rays and UV
light of NGC4254. The distribution of total radio intensity at 8.46 4.86 GHz
reveals a global asy... | astro-ph | radio observations can show how cluster galaxies are affected by various environmental factors we made three frequency radiopolarimetric vla observations and performed sensitive xmmnewton observations in xrays and uv light of ngc4254 the distribution of total radio intensity at 846 486 ghz reveals a global asymmetry wi... | [['radio', 'observations', 'can', 'show', 'how', 'cluster', 'galaxies', 'are', 'affected', 'by', 'various', 'environmental', 'factors', 'we', 'made', 'three', 'frequency', 'radiopolarimetric', 'vla', 'observations', 'and', 'performed', 'sensitive', 'xmmnewton', 'observations', 'in', 'xrays', 'and', 'uv', 'light', 'of',... | [-0.10549290257083055, 0.13603969425689633, -0.0741778864697856, 0.10334756987121625, -0.11772506015423016, -0.0597502689044445, 0.013931380140496207, 0.46179664493862527, -0.19602039531930845, -0.30909598663776783, 0.05162880890201027, -0.2696829423813265, -0.03595107545114153, 0.19233995047791028, 0.01046016144194391... |
708.1534 | Measurement of branching fraction and CP asymmetries in B->D0(cp)K
decays | We present a preliminary study of $B^- \to D^0_{CP} \pi^-$ and $B^- \to
D^0_{CP} K^-$ decays, with the $D^0_{CP}$ reconstructed in the CP-odd
eigenstates $K_s \pi^0$, $K_s \omega$, in the CP-even eigenstates $K^+ K^-$,
$\pi^+ \pi^-$, and in the (non-CP) flavor eigenstate $K^\mp \pi^\pm$. Using a
sample of about 382 m... | hep-ex | we present a preliminary study of b to d0_cp pi and b to d0_cp k decays with the d0_cp reconstructed in the cpodd eigenstates k_s pi0 k_s omega in the cpeven eigenstates k k pi pi and in the noncp flavor eigenstate kmp pipm using a sample of about 382 million y4s decays into bbbar pairs collected with the babar detecto... | [['we', 'present', 'a', 'preliminary', 'study', 'of', 'b', 'to', 'd0_cp', 'pi', 'and', 'b', 'to', 'd0_cp', 'k', 'decays', 'with', 'the', 'd0_cp', 'reconstructed', 'in', 'the', 'cpodd', 'eigenstates', 'k_s', 'pi0', 'k_s', 'omega', 'in', 'the', 'cpeven', 'eigenstates', 'k', 'k', 'pi', 'pi', 'and', 'in', 'the', 'noncp', '... | [-0.15038863877465095, 0.24629611188623432, -0.0846937089615191, 0.012549288508792718, 0.04450842350100478, -0.1992990625789389, 0.15548548736454298, 0.25234271268127484, -0.14526526659804706, -0.3409226321304838, -0.11061662711726968, -0.553383908176329, 0.21504888041721035, 0.10610221796766078, -0.004423352717033898,... |
708.1535 | Three-Nucleon Scattering at Intermediate Energies | By means of a technique, which does not employ partial wave (PW)
decompositions, the nucleon-deuteron break-up process is evaluated in the
Faddeev scheme, where only the leading order term of the amplitude is
considered. This technique is then applied to calculate the semi-exclusive
proton-deuteron break-up reaction ... | nucl-th | by means of a technique which does not employ partial wave pw decompositions the nucleondeuteron breakup process is evaluated in the faddeev scheme where only the leading order term of the amplitude is considered this technique is then applied to calculate the semiexclusive protondeuteron breakup reaction dpnpp for pro... | [['by', 'means', 'of', 'a', 'technique', 'which', 'does', 'not', 'employ', 'partial', 'wave', 'pw', 'decompositions', 'the', 'nucleondeuteron', 'breakup', 'process', 'is', 'evaluated', 'in', 'the', 'faddeev', 'scheme', 'where', 'only', 'the', 'leading', 'order', 'term', 'of', 'the', 'amplitude', 'is', 'considered', 'th... | [-0.0447653645480792, 0.17917000959257146, -0.09093657663119656, 0.15747368867848943, -0.014106257984258918, -0.08648459493180924, 0.011530965580035456, 0.3741281558659008, -0.22321804902657008, -0.29709687623322656, -0.022788160008197424, -0.3031583102352971, 0.01019433792680502, 0.19223032618551214, 0.095251187239941... |
708.1536 | Physics and Commonsense - Reassessing the connection in the light of
quantum theory | Scientific realism in classical (i.e. pre-quantum) physics has remained
compatible with the naive realism of everyday thinking on the whole; whereas it
has proven impossible to find any consistent way to visualize the world
underlying quantum theory in terms of our pictures in the everyday world. The
general conclusi... | quant-ph | scientific realism in classical ie prequantum physics has remained compatible with the naive realism of everyday thinking on the whole whereas it has proven impossible to find any consistent way to visualize the world underlying quantum theory in terms of our pictures in the everyday world the general conclusion is tha... | [['scientific', 'realism', 'in', 'classical', 'ie', 'prequantum', 'physics', 'has', 'remained', 'compatible', 'with', 'the', 'naive', 'realism', 'of', 'everyday', 'thinking', 'on', 'the', 'whole', 'whereas', 'it', 'has', 'proven', 'impossible', 'to', 'find', 'any', 'consistent', 'way', 'to', 'visualize', 'the', 'world'... | [-0.02955169926824785, 0.09566092235292052, -0.1327039515266993, 0.10634335839819, -0.06935840574922142, -0.1391464544020102, 0.05786992243368302, 0.2899679590098478, -0.21699410320802048, -0.30138114804995586, 0.00417459422369375, -0.27612382099851146, -0.1823335826847252, 0.15580143853203282, -0.1379965403831083, 0.0... |
708.1537 | Conformally symmetric traversable wormholes | Exact solutions of traversable wormholes are found under the assumption of
spherical symmetry and the existence of a {\it non-static} conformal symmetry,
which presents a more systematic approach in searching for exact wormhole
solutions. In this work, a wide variety of solutions are deduced by considering
choices fo... | gr-qc astro-ph hep-th | exact solutions of traversable wormholes are found under the assumption of spherical symmetry and the existence of a it nonstatic conformal symmetry which presents a more systematic approach in searching for exact wormhole solutions in this work a wide variety of solutions are deduced by considering choices for the for... | [['exact', 'solutions', 'of', 'traversable', 'wormholes', 'are', 'found', 'under', 'the', 'assumption', 'of', 'spherical', 'symmetry', 'and', 'the', 'existence', 'of', 'a', 'it', 'nonstatic', 'conformal', 'symmetry', 'which', 'presents', 'a', 'more', 'systematic', 'approach', 'in', 'searching', 'for', 'exact', 'wormhol... | [-0.19551084978469058, 0.09063836287922884, -0.11131538486778282, 0.11634253052406854, -0.11474110707271526, -0.17502307368544634, -0.050329786913097474, 0.31568991684741, -0.1845990077211953, -0.30147522977743546, 0.08628617068568085, -0.23368814225285883, -0.08213073222489073, 0.143235541539403, -0.005371981178674415... |
708.1538 | Entropy of complex relevant components of Boolean networks | Boolean network models of strongly connected modules are capable of capturing
the high regulatory complexity of many biological gene regulatory circuits. We
study numerically the previously introduced basin entropy, a parameter for the
dynamical uncertainty or information storage capacity of a network as well as
the ... | cond-mat.dis-nn | boolean network models of strongly connected modules are capable of capturing the high regulatory complexity of many biological gene regulatory circuits we study numerically the previously introduced basin entropy a parameter for the dynamical uncertainty or information storage capacity of a network as well as the aver... | [['boolean', 'network', 'models', 'of', 'strongly', 'connected', 'modules', 'are', 'capable', 'of', 'capturing', 'the', 'high', 'regulatory', 'complexity', 'of', 'many', 'biological', 'gene', 'regulatory', 'circuits', 'we', 'study', 'numerically', 'the', 'previously', 'introduced', 'basin', 'entropy', 'a', 'parameter',... | [-0.12866197467083113, 0.10631013904931023, -0.015064246626570821, 0.12263659419986653, -0.024756591743789615, -0.14817956570914248, 0.07545299881603569, 0.3617397817783058, -0.31425886754877863, -0.26019878359802534, 0.1231112888941425, -0.25714083421044054, -0.22255389369674958, 0.22997945584065746, -0.07617342572484... |
708.1539 | The Structure of Classical Extensions of Quantum Probability Theory | On the basis of a suggestive definition of a classical extension of quantum
mechanics in terms of statistical models, we prove that every such classical
extension is essentially given by the so-called Misra-Bugajski reduction map.
We consider how this map enables one to understand quantum mechanics as a
reduced class... | quant-ph | on the basis of a suggestive definition of a classical extension of quantum mechanics in terms of statistical models we prove that every such classical extension is essentially given by the socalled misrabugajski reduction map we consider how this map enables one to understand quantum mechanics as a reduced classical s... | [['on', 'the', 'basis', 'of', 'a', 'suggestive', 'definition', 'of', 'a', 'classical', 'extension', 'of', 'quantum', 'mechanics', 'in', 'terms', 'of', 'statistical', 'models', 'we', 'prove', 'that', 'every', 'such', 'classical', 'extension', 'is', 'essentially', 'given', 'by', 'the', 'socalled', 'misrabugajski', 'reduc... | [-0.09791543237755404, 0.09855358144268393, -0.11131170055664638, 0.11389746212345712, -0.050992157967651594, -0.0990403793149573, 0.02675051388796419, 0.28995952628114646, -0.3214126741184908, -0.2214960068683414, 0.10344567895209526, -0.2366636277998195, -0.20947879153468152, 0.21588791047551614, -0.11477441645282156... |
708.154 | Optimal bounded-error strategies for projective measurements in
non-orthogonal state discrimination | Research in non-orthogonal state discrimination has given rise to two
conventional optimal strategies: unambiguous discrimination (UD) and minimum
error (ME) discrimination. This paper explores the experimentally relevant
range of measurement strategies between the two, where the rate of inconclusive
results is minim... | quant-ph | research in nonorthogonal state discrimination has given rise to two conventional optimal strategies unambiguous discrimination ud and minimum error me discrimination this paper explores the experimentally relevant range of measurement strategies between the two where the rate of inconclusive results is minimized for a... | [['research', 'in', 'nonorthogonal', 'state', 'discrimination', 'has', 'given', 'rise', 'to', 'two', 'conventional', 'optimal', 'strategies', 'unambiguous', 'discrimination', 'ud', 'and', 'minimum', 'error', 'me', 'discrimination', 'this', 'paper', 'explores', 'the', 'experimentally', 'relevant', 'range', 'of', 'measur... | [-0.11025949638589459, 0.07271544239878402, -0.07277746129212743, 0.07099984264024928, -0.05159687990780478, -0.19369690697166628, 0.13942342456943213, 0.39731670009027537, -0.27484550450186607, -0.28958849826338307, 0.09954270580586172, -0.24604020914125999, -0.14402167670334043, 0.2241998216279356, -0.099463710111518... |
708.1541 | Energy Spectra for Fractional Quantum Hall States | Fractional quantum Hall states (FQHS) with the filling factor nu = p/q of q <
21 are examined and their energies are calculated. The classical Coulomb energy
is evaluated among many electrons; that energy is linearly dependent on 1/nu.
The residual binding energies are also evaluated. The electron pair in nearest
Lan... | cond-mat.mes-hall cond-mat.str-el | fractional quantum hall states fqhs with the filling factor nu pq of q 21 are examined and their energies are calculated the classical coulomb energy is evaluated among many electrons that energy is linearly dependent on 1nu the residual binding energies are also evaluated the electron pair in nearest landauorbitals is... | [['fractional', 'quantum', 'hall', 'states', 'fqhs', 'with', 'the', 'filling', 'factor', 'nu', 'pq', 'of', 'q', '21', 'are', 'examined', 'and', 'their', 'energies', 'are', 'calculated', 'the', 'classical', 'coulomb', 'energy', 'is', 'evaluated', 'among', 'many', 'electrons', 'that', 'energy', 'is', 'linearly', 'depende... | [-0.1788642830744555, 0.2472478449646867, 0.009232387008549241, 0.13616405419152153, 0.0016656434358833553, -0.1722095710212378, 0.07571614752979493, 0.3576938590047868, -0.24722577143017646, -0.32850360236345577, -0.046335952545327325, -0.33053981243157304, -0.024056589764940156, 0.15917233458453126, 0.080403887796202... |
708.1542 | Predictability of extreme events in a branching diffusion model | We propose a framework for studying predictability of extreme events in
complex systems. Major conceptual elements -- direct cascading or
fragmentation, spatial dynamics, and external driving -- are combined in a
classical age-dependent multi-type branching diffusion process with
immigration. A complete analytic desc... | nlin.AO | we propose a framework for studying predictability of extreme events in complex systems major conceptual elements direct cascading or fragmentation spatial dynamics and external driving are combined in a classical agedependent multitype branching diffusion process with immigration a complete analytic description of the... | [['we', 'propose', 'a', 'framework', 'for', 'studying', 'predictability', 'of', 'extreme', 'events', 'in', 'complex', 'systems', 'major', 'conceptual', 'elements', 'direct', 'cascading', 'or', 'fragmentation', 'spatial', 'dynamics', 'and', 'external', 'driving', 'are', 'combined', 'in', 'a', 'classical', 'agedependent'... | [-0.09387463749321345, 0.09953909284494994, -0.11081045598571969, 0.14528178468696692, -0.051408157667128355, -0.10310271263189681, 0.03079163121596516, 0.3742834983041158, -0.24991617817851203, -0.289314037172107, 0.08493194005951318, -0.23471685217039004, -0.2004363626673784, 0.18362068184148017, -0.05931532797026070... |
708.1543 | Dipole excitation and geometry of borromean nuclei | We analyze the Coulomb breakup cross sections of $^{11}$Li and $^6$He nuclei
using a three-body model with a density-dependent contact interaction. We show
that the concentration of the B(E1) strength near the threshold can be well
reproduced with this model. With the help of the calculated B(E1) value, we
extract th... | nucl-th | we analyze the coulomb breakup cross sections of 11li and 6he nuclei using a threebody model with a densitydependent contact interaction we show that the concentration of the be1 strength near the threshold can be well reproduced with this model with the help of the calculated be1 value we extract the rootmeansquare rm... | [['we', 'analyze', 'the', 'coulomb', 'breakup', 'cross', 'sections', 'of', '11li', 'and', '6he', 'nuclei', 'using', 'a', 'threebody', 'model', 'with', 'a', 'densitydependent', 'contact', 'interaction', 'we', 'show', 'that', 'the', 'concentration', 'of', 'the', 'be1', 'strength', 'near', 'the', 'threshold', 'can', 'be',... | [-0.034777155994287844, 0.18011331982207257, -0.0986652480476207, 0.12651021151650385, 0.04333695875793383, -0.0946212842331066, 0.09692420674344668, 0.3661845432972158, -0.26015749749551703, -0.3395026248091689, -0.08041765934370874, -0.33608379510029424, -0.03478686011989008, 0.12337534186443301, 0.07469946668333524,... |
708.1544 | Measurement of cos2beta in B0->D(*)h0 Decays with a Time-Dependent
Dalitz Plot Analysis of D->KSpi+pi- | We study the time-dependent Dalitz plot of D->KSpi+pi- in B0->D(*)h0 decays,
where h0 is a pi0, eta, eta', or omega meson and D*->Dpi0 using a data sample
of 383 X 10^6 Upsilon(4S)->BBbar decays collected with the BABAR detector. We
determine cos2beta = 0.42+-0.49+-0.09+-0.13, sin2beta = 0.29+-0.34+-0.03+-0.05,
and |... | hep-ex | we study the timedependent dalitz plot of dkspipi in b0dh0 decays where h0 is a pi0 eta eta or omega meson and ddpi0 using a data sample of 383 x 106 upsilon4sbbbar decays collected with the babar detector we determine cos2beta 042049009013 sin2beta 029034003005 and lambda 101008002 where the first error is statistical... | [['we', 'study', 'the', 'timedependent', 'dalitz', 'plot', 'of', 'dkspipi', 'in', 'b0dh0', 'decays', 'where', 'h0', 'is', 'a', 'pi0', 'eta', 'eta', 'or', 'omega', 'meson', 'and', 'ddpi0', 'using', 'a', 'data', 'sample', 'of', '383', 'x', '106', 'upsilon4sbbbar', 'decays', 'collected', 'with', 'the', 'babar', 'detector'... | [-0.08728358626831323, 0.14231972422012837, -0.06888219601629923, 0.07379142014404005, -0.04560275949188508, -0.13363996124826372, 0.13827690782879168, 0.26496187330312315, -0.16931570404475288, -0.2696190820563407, 0.002235405561458763, -0.41222972897369237, 0.04458051592588336, 0.15368992402467743, 0.0433611906288812... |
708.1545 | The Faint End Slopes Of Galaxy Luminosity Functions In The COSMOS
2-Square Degree Field | We examine the faint-end slope of the rest-frame V-band luminosity function
(LF), with respect to galaxy spectral type, of field galaxies with redshift
z<0.5, using a sample of 80,820 galaxies with photometric redshifts in the
Cosmic Evolution Survey (COSMOS) field. For all galaxy spectral types combined,
the LF slop... | astro-ph | we examine the faintend slope of the restframe vband luminosity function lf with respect to galaxy spectral type of field galaxies with redshift z05 using a sample of 80820 galaxies with photometric redshifts in the cosmic evolution survey cosmos field for all galaxy spectral types combined the lf slope alpha ranges fr... | [['we', 'examine', 'the', 'faintend', 'slope', 'of', 'the', 'restframe', 'vband', 'luminosity', 'function', 'lf', 'with', 'respect', 'to', 'galaxy', 'spectral', 'type', 'of', 'field', 'galaxies', 'with', 'redshift', 'z05', 'using', 'a', 'sample', 'of', '80820', 'galaxies', 'with', 'photometric', 'redshifts', 'in', 'the... | [0.023578600050096616, 0.09288035608453196, -0.08229730971766717, 0.136656755653251, -0.10158473347993158, -0.05919130918212563, 0.010699234336157734, 0.5107859542605074, -0.055005351676014044, -0.39489573143523643, -0.049380124452869475, -0.3210162176990753, 0.09063435608463262, 0.19377947382997932, -0.029165152672666... |
708.1546 | Relationship between macroscopic physical properties and local
distortions of low doping La{1-x}Ca{x}MnO3: an EXAFS study | A temperature-dependent EXAFS investigation of La{1-x}Ca{x}MnO3 is presented
for the concentration range that spans the ferromagnetic-insulator (FMI) to
ferromagnetic-metal (FMM) transition region, x = 0.16-0.22. The samples are
insulating for x = 0.16-0.2 and show a metal/insulator transition for x = 0.22.
All sampl... | cond-mat.str-el | a temperaturedependent exafs investigation of la1xcaxmno3 is presented for the concentration range that spans the ferromagneticinsulator fmi to ferromagneticmetal fmm transition region x 016022 the samples are insulating for x 01602 and show a metalinsulator transition for x 022 all samples are ferromagnetic although t... | [['a', 'temperaturedependent', 'exafs', 'investigation', 'of', 'la1xcaxmno3', 'is', 'presented', 'for', 'the', 'concentration', 'range', 'that', 'spans', 'the', 'ferromagneticinsulator', 'fmi', 'to', 'ferromagneticmetal', 'fmm', 'transition', 'region', 'x', '016022', 'the', 'samples', 'are', 'insulating', 'for', 'x', '... | [-0.13694244194605212, 0.21293675171709137, 0.010007484500890533, 0.057007314417017466, -0.0028359146170510814, -0.12478393664410949, 0.08809511852751743, 0.4266656550964148, -0.25769874954531935, -0.32852951955082343, 0.06773627274980817, -0.3843185258587694, -0.037335149348454534, 0.14671770459420352, 0.0533354558834... |
708.1547 | Strichartz Estimates for the Schroedinger Equation with Time-Periodic
L^{n/2} Potentials | We prove Strichartz estimates for the Schroedinger operator $H = -\Delta +
V(t,x)$ with time-periodic complex potentials $V$ belonging to the
scaling-critical space $L^{n/2}_x L^\infty_t$ in dimensions $n \ge 3$. This is
done directly from estimates on the resolvent rather than using dispersive
bounds, as the latter ... | math.AP math-ph math.MP | we prove strichartz estimates for the schroedinger operator h delta vtx with timeperiodic complex potentials v belonging to the scalingcritical space ln2_x linfty_t in dimensions n ge 3 this is done directly from estimates on the resolvent rather than using dispersive bounds as the latter generally require a stronger r... | [['we', 'prove', 'strichartz', 'estimates', 'for', 'the', 'schroedinger', 'operator', 'h', 'delta', 'vtx', 'with', 'timeperiodic', 'complex', 'potentials', 'v', 'belonging', 'to', 'the', 'scalingcritical', 'space', 'ln2_x', 'linfty_t', 'in', 'dimensions', 'n', 'ge', '3', 'this', 'is', 'done', 'directly', 'from', 'estim... | [-0.10866639083741526, 0.13899161387862957, -0.017055809140009315, 0.09435813364842416, -0.054827065020799634, -0.15737352311905278, 0.0013345798734869612, 0.3619213834404945, -0.2260106804682628, -0.2397817031333321, 0.10574319300021191, -0.32422488469532446, -0.06133931906906104, 0.19210617131504573, -0.0092924142942... |
708.1548 | Comment on ``Precision measurement of the Casimir-Lifshitz force in a
fluid'' | Recently J.N. Munday and F. Capasso [Phys. Rev. A {\bf 75}, 060102(R) (2007);
arXiv:0705.3793] claimed that they have performed a precision measurement of
the Casimir force between a sphere and a plate coated with Au, both immersed in
ethanol. The measurement results were claimed to be consistent with the
Lifshitz th... | physics.atom-ph cond-mat.stat-mech physics.gen-ph quant-ph | recently jn munday and f capasso phys rev a bf 75 060102r 2007 arxiv07053793 claimed that they have performed a precision measurement of the casimir force between a sphere and a plate coated with au both immersed in ethanol the measurement results were claimed to be consistent with the lifshitz theory we demonstrate th... | [['recently', 'jn', 'munday', 'and', 'f', 'capasso', 'phys', 'rev', 'a', 'bf', '75', '060102r', '2007', 'arxiv07053793', 'claimed', 'that', 'they', 'have', 'performed', 'a', 'precision', 'measurement', 'of', 'the', 'casimir', 'force', 'between', 'a', 'sphere', 'and', 'a', 'plate', 'coated', 'with', 'au', 'both', 'immer... | [-0.09693708155257627, 0.10324639080092311, -0.10556691683083773, -0.02283299851603806, -0.027047508593648673, -0.11191807880625129, 0.05298181182146072, 0.367683338008821, -0.17182878591120243, -0.34792101064184683, 0.008193970208987593, -0.3096450662314892, -0.13534248301386834, 0.18438648529350757, -0.07901179940812... |
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