id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
708.2249 | The spin structure of the pion | We present the first calculation of the transverse spin structure of the pion
in lattice QCD. Our simulations are based on two flavors of non-perturbatively
improved Wilson fermions, with pion masses as low as 400 MeV in volumes up to
(2.1 fm)^3 and lattice spacings below 0.1 fm. We find a characteristic
asymmetry in... | hep-lat hep-ph | we present the first calculation of the transverse spin structure of the pion in lattice qcd our simulations are based on two flavors of nonperturbatively improved wilson fermions with pion masses as low as 400 mev in volumes up to 21 fm3 and lattice spacings below 01 fm we find a characteristic asymmetry in the spatia... | [['we', 'present', 'the', 'first', 'calculation', 'of', 'the', 'transverse', 'spin', 'structure', 'of', 'the', 'pion', 'in', 'lattice', 'qcd', 'our', 'simulations', 'are', 'based', 'on', 'two', 'flavors', 'of', 'nonperturbatively', 'improved', 'wilson', 'fermions', 'with', 'pion', 'masses', 'as', 'low', 'as', '400', 'm... | [-0.09152039963301721, 0.3035254430148628, -0.106897283642256, 0.12847332711137094, 0.0026099206454371316, -0.03640957098392831, 0.062016819744462985, 0.43591482927101655, -0.1330009239551785, -0.24987092054101054, -0.0027430849571988642, -0.32138536870479584, 0.00456262504231635, 0.12103499080167039, 0.090189564737726... |
708.225 | Lorentz Invariance Violation from String Theory | In this brief, and by no means complete, review I discuss situations in
string theory, in which Lorentz Invariance Violation may occur in a way
consistent with world-sheet conformal invariance, thereby leading to
acceptable, in principle, string backgrounds. In particular, I first discuss
spontaneous Lorentz violatio... | hep-th gr-qc hep-ph | in this brief and by no means complete review i discuss situations in string theory in which lorentz invariance violation may occur in a way consistent with worldsheet conformal invariance thereby leading to acceptable in principle string backgrounds in particular i first discuss spontaneous lorentz violation in non su... | [['in', 'this', 'brief', 'and', 'by', 'no', 'means', 'complete', 'review', 'i', 'discuss', 'situations', 'in', 'string', 'theory', 'in', 'which', 'lorentz', 'invariance', 'violation', 'may', 'occur', 'in', 'a', 'way', 'consistent', 'with', 'worldsheet', 'conformal', 'invariance', 'thereby', 'leading', 'to', 'acceptable... | [-0.09688757181960568, 0.16168846063755016, -0.06830361167977377, 0.14383643187024187, -0.11470195594736185, -0.18305962186072666, 0.0033697074666833846, 0.3289526544160244, -0.2229502503053134, -0.27960694755618926, 0.06848904138482151, -0.24828140794163014, -0.15457492401452824, 0.14474249260587843, -0.09515693136100... |
708.2251 | First real time detection of Be7 solar neutrinos by Borexino | This paper reports a direct measurement of the Be7 solar neutrino signal rate
performed with the Borexino low background liquid scintillator detector. This
is the first real-time spectral measurement of sub-MeV solar neutrinos. The
result for 0.862 MeV Be7 is 47 +- 7 (stat} +- 12 (sys} counts/(day x 100 ton),
consist... | astro-ph hep-ph nucl-ex | this paper reports a direct measurement of the be7 solar neutrino signal rate performed with the borexino low background liquid scintillator detector this is the first realtime spectral measurement of submev solar neutrinos the result for 0862 mev be7 is 47 7 stat 12 sys countsday x 100 ton consistent with predictions ... | [['this', 'paper', 'reports', 'a', 'direct', 'measurement', 'of', 'the', 'be7', 'solar', 'neutrino', 'signal', 'rate', 'performed', 'with', 'the', 'borexino', 'low', 'background', 'liquid', 'scintillator', 'detector', 'this', 'is', 'the', 'first', 'realtime', 'spectral', 'measurement', 'of', 'submev', 'solar', 'neutrin... | [-0.06039618748406208, 0.27371791927296607, 0.03169885407522565, 0.09349134833109184, 0.01546528413805912, -0.12933421134185352, 0.07447385043096652, 0.27479232310271656, -0.14126469623908156, -0.45174670530880084, 0.04221694740909533, -0.39260059390522417, 0.05154822169054971, 0.213573894116142, -0.02726163480003349, ... |
708.2252 | Focusing and Polarization in Intuitionistic Logic | A focused proof system provides a normal form to cut-free proofs that
structures the application of invertible and non-invertible inference rules.
The focused proof system of Andreoli for linear logic has been applied to both
the proof search and the proof normalization approaches to computation. Various
proof system... | cs.LO | a focused proof system provides a normal form to cutfree proofs that structures the application of invertible and noninvertible inference rules the focused proof system of andreoli for linear logic has been applied to both the proof search and the proof normalization approaches to computation various proof systems in l... | [['a', 'focused', 'proof', 'system', 'provides', 'a', 'normal', 'form', 'to', 'cutfree', 'proofs', 'that', 'structures', 'the', 'application', 'of', 'invertible', 'and', 'noninvertible', 'inference', 'rules', 'the', 'focused', 'proof', 'system', 'of', 'andreoli', 'for', 'linear', 'logic', 'has', 'been', 'applied', 'to'... | [-0.13089133972400907, -0.007312197821120993, -0.13021267946682227, 0.06595008276995915, -0.1419940673136454, -0.20653242108633194, 0.08136533178462774, 0.32724885706850093, -0.2595159342820696, -0.273123815394402, 0.1339897539633286, -0.23093116344388226, -0.14842152190327698, 0.24457631822635265, -0.0922953090795882,... |
708.2253 | The Concept of Entropy and its Concavity for a Finite Protein in its
Environment: An exact study on a Square Lattice | We consider a general lattice model of a finite protein in its environment
and calculate its Boltzmann entropy SB(E) as a function of its energy E in a
microcanonical ensemble, and Gibbs entropy SG(E) as a function of its average
energy E in a canonical ensemble by exact enumeration on a square lattice. We
find that ... | cond-mat.soft cond-mat.other | we consider a general lattice model of a finite protein in its environment and calculate its boltzmann entropy sbe as a function of its energy e in a microcanonical ensemble and gibbs entropy sge as a function of its average energy e in a canonical ensemble by exact enumeration on a square lattice we find that because ... | [['we', 'consider', 'a', 'general', 'lattice', 'model', 'of', 'a', 'finite', 'protein', 'in', 'its', 'environment', 'and', 'calculate', 'its', 'boltzmann', 'entropy', 'sbe', 'as', 'a', 'function', 'of', 'its', 'energy', 'e', 'in', 'a', 'microcanonical', 'ensemble', 'and', 'gibbs', 'entropy', 'sge', 'as', 'a', 'function... | [-0.07958534434376481, 0.1401670227570688, -0.09690988131619074, 0.13151399117053011, -0.027668688188944208, -0.1611744830703461, 0.049889005884005314, 0.39567708322092104, -0.27039485178957284, -0.23498501676020392, 0.09735931637145481, -0.2775249296979031, -0.11687252482219615, 0.1933383779383771, -0.0196475998923313... |
708.2254 | Effective Field Theory for the Anisotropic Wilson Lattice Action | We construct the effective field theory appropriate for describing the low
energy behavior of anisotropic Wilson lattice actions and the O(a) improved
variant thereof. We then apply this effective field theory to the hadron
spectrum and dispersion relations, focussing on the corrections due to the
anisotropy. We poin... | hep-lat | we construct the effective field theory appropriate for describing the low energy behavior of anisotropic wilson lattice actions and the oa improved variant thereof we then apply this effective field theory to the hadron spectrum and dispersion relations focussing on the corrections due to the anisotropy we point out a... | [['we', 'construct', 'the', 'effective', 'field', 'theory', 'appropriate', 'for', 'describing', 'the', 'low', 'energy', 'behavior', 'of', 'anisotropic', 'wilson', 'lattice', 'actions', 'and', 'the', 'oa', 'improved', 'variant', 'thereof', 'we', 'then', 'apply', 'this', 'effective', 'field', 'theory', 'to', 'the', 'hadr... | [-0.11399860466398033, 0.22115493800941163, -0.08650349347486294, 0.10052769504233895, -0.07237505431528136, -0.10985915588597502, 0.048732099079643376, 0.4157878872605839, -0.20113244946281025, -0.2589488049727931, 0.09083961886478521, -0.2700819321658595, -0.12511663254658092, 0.13297392236875435, -0.0124355522400167... |
708.2255 | A Language for Generic Programming in the Large | Generic programming is an effective methodology for developing reusable
software libraries. Many programming languages provide generics and have
features for describing interfaces, but none completely support the idioms used
in generic programming. To address this need we developed the language G. The
central feature... | cs.PL cs.SE | generic programming is an effective methodology for developing reusable software libraries many programming languages provide generics and have features for describing interfaces but none completely support the idioms used in generic programming to address this need we developed the language g the central feature of g ... | [['generic', 'programming', 'is', 'an', 'effective', 'methodology', 'for', 'developing', 'reusable', 'software', 'libraries', 'many', 'programming', 'languages', 'provide', 'generics', 'and', 'have', 'features', 'for', 'describing', 'interfaces', 'but', 'none', 'completely', 'support', 'the', 'idioms', 'used', 'in', 'g... | [-0.11952190080664878, -0.0009248486158867309, -0.07372126290865708, 0.04512929065385833, -0.15500261498527834, -0.17674509349744766, 0.0035698360894457436, 0.3839250462362543, -0.2808243340579793, -0.3206275157048367, 0.10095066213616519, -0.22053501306218096, -0.14648739218973789, 0.22429592668777332, -0.091665229680... |
708.2256 | Automorphisms and isomorphisms of Chevalley groups and algebras | An adjoint Chevalley group of rank at least 2 over a rational algebra (or a
similar ring), its elementary subgroup, and the corresponding Lie ring have the
same automorphism group. These automorphisms are explicitly described.
| math.GR math.RA math.RT | an adjoint chevalley group of rank at least 2 over a rational algebra or a similar ring its elementary subgroup and the corresponding lie ring have the same automorphism group these automorphisms are explicitly described | [['an', 'adjoint', 'chevalley', 'group', 'of', 'rank', 'at', 'least', '2', 'over', 'a', 'rational', 'algebra', 'or', 'a', 'similar', 'ring', 'its', 'elementary', 'subgroup', 'and', 'the', 'corresponding', 'lie', 'ring', 'have', 'the', 'same', 'automorphism', 'group', 'these', 'automorphisms', 'are', 'explicitly', 'desc... | [-0.22189416444993446, 0.044350196687654324, -0.12662481560504862, 0.028716370569808143, -0.1441077932715416, -0.15191215921991638, -0.07367827471877847, 0.39486540641103474, -0.41887500669275013, -0.21059629741523947, 0.18495523408055306, -0.23917102260249, -0.04784155493169757, 0.1361113101709634, -0.1133631374154772... |
708.2257 | Dynamics of Atom-Field Entanglement from Exact Solutions: Towards Strong
Coupling and Non-Markovian Regimes | We examine the dynamics of bipartite entanglement between a two-level atom
and the electromagnetic field. We treat the Jaynes-Cummings model with a single
field mode and examine in detail the exact time evolution of entanglement,
including cases where the atomic state is initially mixed and the atomic
transition is d... | quant-ph | we examine the dynamics of bipartite entanglement between a twolevel atom and the electromagnetic field we treat the jaynescummings model with a single field mode and examine in detail the exact time evolution of entanglement including cases where the atomic state is initially mixed and the atomic transition is detuned... | [['we', 'examine', 'the', 'dynamics', 'of', 'bipartite', 'entanglement', 'between', 'a', 'twolevel', 'atom', 'and', 'the', 'electromagnetic', 'field', 'we', 'treat', 'the', 'jaynescummings', 'model', 'with', 'a', 'single', 'field', 'mode', 'and', 'examine', 'in', 'detail', 'the', 'exact', 'time', 'evolution', 'of', 'en... | [-0.1546424505094298, 0.16613563030011397, -0.04980791504212029, 0.05491080640691548, 0.005742224454248356, -0.15744011152777715, 0.03629825140367983, 0.36391760964514847, -0.22153214404443647, -0.2470243878157462, 0.052426845634403495, -0.2746107453364605, -0.10597276205649483, 0.1506119155250016, 0.048458217257781135... |
708.2258 | The evolution of cosmological gravitational waves in f(R) gravity | We give a rigorous and mathematically clear presentation of the Covariant and
Gauge Invariant theory of gravitational waves in a perturbed
Friedmann-Lemaitre-Robertson-Walker universe for Fourth Order Gravity, where
the matter is described by a perfect fluid with a barotropic equation of state.
As an example of a con... | gr-qc astro-ph | we give a rigorous and mathematically clear presentation of the covariant and gauge invariant theory of gravitational waves in a perturbed friedmannlemaitrerobertsonwalker universe for fourth order gravity where the matter is described by a perfect fluid with a barotropic equation of state as an example of a consistent... | [['we', 'give', 'a', 'rigorous', 'and', 'mathematically', 'clear', 'presentation', 'of', 'the', 'covariant', 'and', 'gauge', 'invariant', 'theory', 'of', 'gravitational', 'waves', 'in', 'a', 'perturbed', 'friedmannlemaitrerobertsonwalker', 'universe', 'for', 'fourth', 'order', 'gravity', 'where', 'the', 'matter', 'is',... | [-0.17180185889866312, 0.14470030377389562, -0.11316626910120249, 0.08859221255338258, -0.10155910235446165, -0.11674897057442542, -0.06882844022201265, 0.2575772695830571, -0.2241171846890425, -0.2750447836430634, 0.08321670818019329, -0.2763629046186586, -0.12112298616317703, 0.16544932874111348, 0.008147125466562368... |
708.2259 | Photometric Calibration of the Swift Ultraviolet/Optical Telescope | We present the photometric calibration of the Swift UltraViolet/Optical
Telescope (UVOT) which includes: optimum photometric and background apertures,
effective area curves, colour transformations, conversion factors for count
rates to flux, and the photometric zero points (which are accurate to better
than 4 per cen... | astro-ph | we present the photometric calibration of the swift ultravioletoptical telescope uvot which includes optimum photometric and background apertures effective area curves colour transformations conversion factors for count rates to flux and the photometric zero points which are accurate to better than 4 per cent for each ... | [['we', 'present', 'the', 'photometric', 'calibration', 'of', 'the', 'swift', 'ultravioletoptical', 'telescope', 'uvot', 'which', 'includes', 'optimum', 'photometric', 'and', 'background', 'apertures', 'effective', 'area', 'curves', 'colour', 'transformations', 'conversion', 'factors', 'for', 'count', 'rates', 'to', 'f... | [-0.030841231000268574, 0.06589211381307637, -0.08597764478231124, 0.08756749622628468, -0.12419082335911172, -0.09352744569236687, 0.08679014789987384, 0.48239469222089115, -0.1276316930460491, -0.41098751254784044, 0.11039719533431525, -0.3124385845609183, -0.0377892591203599, 0.29220249000106496, -0.1131566857608656... |
708.226 | A search for B+ --> tau+ nu with Hadronic B tags | We present a search for the decay B^+ --> tau^+ nu using $383 \times 10^{6}}$
BBbar pairs collected at the Upsilon(4S) resonance with the BABAR detector at
the SLAC PEP-II B Factory. We select a sample of events with one completely
reconstructed tag B in a hadronic decay mode ($B^- \to D^{(*)0} X^-$), and
examine the... | hep-ex | we present a search for the decay b tau nu using 383 times 106 bbbar pairs collected at the upsilon4s resonance with the babar detector at the slac pepii b factory we select a sample of events with one completely reconstructed tag b in a hadronic decay mode b to d0 x and examine the rest of the event to search for a b ... | [['we', 'present', 'a', 'search', 'for', 'the', 'decay', 'b', 'tau', 'nu', 'using', '383', 'times', '106', 'bbbar', 'pairs', 'collected', 'at', 'the', 'upsilon4s', 'resonance', 'with', 'the', 'babar', 'detector', 'at', 'the', 'slac', 'pepii', 'b', 'factory', 'we', 'select', 'a', 'sample', 'of', 'events', 'with', 'one',... | [-0.12889933235180537, 0.24346914628187, -0.05623820504006832, 0.07201482144309514, -0.012462224943368738, -0.19579645921128677, 0.16016229199864138, 0.2699758745451917, -0.2202245390265068, -0.2423508762479273, -0.05557132600163763, -0.4269018471797011, 0.12402296801612003, 0.10475978540055064, 0.13114681535264922, 0.... |
708.2261 | Association of mid-infrared solar plages with Calcium K line emissions
and magnetic structures | Solar mid-IR observations in the 8-15 micrometer band continuum with moderate
angular resolution (18 arcseconds) reveal the presence of bright structures
surrounding sunspots. These plage-like features present good association with
calcium CaII K1v plages and active region magnetograms. We describe a new
optical setu... | astro-ph | solar midir observations in the 815 micrometer band continuum with moderate angular resolution 18 arcseconds reveal the presence of bright structures surrounding sunspots these plagelike features present good association with calcium caii k1v plages and active region magnetograms we describe a new optical setup with re... | [['solar', 'midir', 'observations', 'in', 'the', '815', 'micrometer', 'band', 'continuum', 'with', 'moderate', 'angular', 'resolution', '18', 'arcseconds', 'reveal', 'the', 'presence', 'of', 'bright', 'structures', 'surrounding', 'sunspots', 'these', 'plagelike', 'features', 'present', 'good', 'association', 'with', 'c... | [-0.05761481910350642, 0.17798274469697067, 0.04102747380320873, 0.05610818064850455, -0.07195473472107082, -0.11674706878951721, 0.012242845050247026, 0.5255936594499696, -0.12998226734963547, -0.3933767150306413, 0.06313862660974864, -0.2947435097791435, -0.08537955347058032, 0.14863854241857846, -0.08403606507072842... |
708.2262 | Gauge invariance in fractional field theories | The principle of local gauge invariance is applied to fractional wave
equations and the interaction term is determined up to order $o(\bar{g})$ in
the coupling constant $\bar{g}$. As a first application, based on the
Riemann-Liouville fractional derivative definition, the fractional Zeeman
effect is used to reproduce... | math-ph math.MP | the principle of local gauge invariance is applied to fractional wave equations and the interaction term is determined up to order obarg in the coupling constant barg as a first application based on the riemannliouville fractional derivative definition the fractional zeeman effect is used to reproduce the baryon spectr... | [['the', 'principle', 'of', 'local', 'gauge', 'invariance', 'is', 'applied', 'to', 'fractional', 'wave', 'equations', 'and', 'the', 'interaction', 'term', 'is', 'determined', 'up', 'to', 'order', 'obarg', 'in', 'the', 'coupling', 'constant', 'barg', 'as', 'a', 'first', 'application', 'based', 'on', 'the', 'riemannliouv... | [-0.16013437379151582, 0.12686701387221028, -0.06917583926946723, 0.10069427131342569, -0.14794836440788847, -0.08578835119094168, -0.03962013888438898, 0.3160445350621428, -0.31178664187235494, -0.3129659039899707, 0.08409454345403772, -0.23793214596807957, -0.09796201669845946, 0.1517383260918515, -0.0064055394647376... |
708.2263 | The SN 1987A Link to Others and Gamma-Ray Bursts | Early measurements of SN 1987A can be interpreted in light of a beam/jet
(BJ), with a collimation factor >10,000, which impacted polar ejecta (PE) to
produce the "Mystery Spot" (MS), ~24 lt-d away. Other details of SN 1987A
suggest that it came from a merger of 2 stellar cores of a common envelope (CE)
binary, i.e. a... | astro-ph | early measurements of sn 1987a can be interpreted in light of a beamjet bj with a collimation factor 10000 which impacted polar ejecta pe to produce the mystery spot ms 24 ltd away other details of sn 1987a suggest that it came from a merger of 2 stellar cores of a common envelope ce binary ie a double degenerate dd sn... | [['early', 'measurements', 'of', 'sn', '1987a', 'can', 'be', 'interpreted', 'in', 'light', 'of', 'a', 'beamjet', 'bj', 'with', 'a', 'collimation', 'factor', '10000', 'which', 'impacted', 'polar', 'ejecta', 'pe', 'to', 'produce', 'the', 'mystery', 'spot', 'ms', '24', 'ltd', 'away', 'other', 'details', 'of', 'sn', '1987a... | [-0.05982073213724783, 0.13417259802782727, -0.06981207442179294, 0.21709364701738174, -0.13448461469965706, -0.13472348935788328, 0.08458801168997429, 0.42037318955977354, -0.18035507538965098, -0.30233697434782253, 0.05196109453169257, -0.29741090945409315, -0.01650615650162633, 0.2552031987964673, -0.047861430858116... |
708.2264 | Influence of random roughness on the adhesion between metal surfaces due
to capillary condensation | The capillary force was measured by atomic force microscopy between a gold
coated sphere mounted on a cantilever and gold surfaces with different
roughness. For smooth surfaces the capillary adhesive force surpasses in
magnitude any dispersion, e.g. van der Waals/Casimir, and/or electrostatic
forces. A substantial de... | cond-mat.mtrl-sci | the capillary force was measured by atomic force microscopy between a gold coated sphere mounted on a cantilever and gold surfaces with different roughness for smooth surfaces the capillary adhesive force surpasses in magnitude any dispersion eg van der waalscasimir andor electrostatic forces a substantial decrease in ... | [['the', 'capillary', 'force', 'was', 'measured', 'by', 'atomic', 'force', 'microscopy', 'between', 'a', 'gold', 'coated', 'sphere', 'mounted', 'on', 'a', 'cantilever', 'and', 'gold', 'surfaces', 'with', 'different', 'roughness', 'for', 'smooth', 'surfaces', 'the', 'capillary', 'adhesive', 'force', 'surpasses', 'in', '... | [-0.14002767058887652, 0.2453803625195382, -0.08588937790788193, -0.0111905863765171, -0.046889320386535656, -0.19438458035452938, 0.024283944771088167, 0.34703828823961774, -0.2566022812103739, -0.34116357525012325, -0.04482483608429605, -0.34075515256358346, -0.13357896832939314, 0.24852001420887454, -0.0482614110746... |
708.2265 | Solutions of fractional reaction-diffusion equations in terms of
Mittag-Leffler functions | This paper deals with the solution of unified fractional reaction-diffusion
systems. The results are obtained in compact and elegant forms in terms of
Mittag-Leffler functions and generalized Mittag-Leffler functions, which are
suitable for numerical computation. On account of the most general character of
the derive... | math.CA math-ph math.MP | this paper deals with the solution of unified fractional reactiondiffusion systems the results are obtained in compact and elegant forms in terms of mittagleffler functions and generalized mittagleffler functions which are suitable for numerical computation on account of the most general character of the derived result... | [['this', 'paper', 'deals', 'with', 'the', 'solution', 'of', 'unified', 'fractional', 'reactiondiffusion', 'systems', 'the', 'results', 'are', 'obtained', 'in', 'compact', 'and', 'elegant', 'forms', 'in', 'terms', 'of', 'mittagleffler', 'functions', 'and', 'generalized', 'mittagleffler', 'functions', 'which', 'are', 's... | [-0.07594782260467152, 0.0061624089108878064, -0.021829713703099468, 0.07470709888883376, -0.0690525465791947, -0.1181092883925885, -0.04113863803611725, 0.30317297690597017, -0.25058018938350296, -0.25333803058847, 0.12232917962798015, -0.26166103664160656, -0.20752186801186517, 0.2898637204136896, -0.0750777603821724... |
708.2266 | The study of a new gerrymandering methodology | This paper is to obtain a simple dividing-diagram of the congressional
districts, where the only limit is that each district should contain the same
population if possibly. In order to solve this problem, we introduce three
different standards of the "simple" shape. The first standard is that the final
shape of the c... | cs.CY | this paper is to obtain a simple dividingdiagram of the congressional districts where the only limit is that each district should contain the same population if possibly in order to solve this problem we introduce three different standards of the simple shape the first standard is that the final shape of the congressio... | [['this', 'paper', 'is', 'to', 'obtain', 'a', 'simple', 'dividingdiagram', 'of', 'the', 'congressional', 'districts', 'where', 'the', 'only', 'limit', 'is', 'that', 'each', 'district', 'should', 'contain', 'the', 'same', 'population', 'if', 'possibly', 'in', 'order', 'to', 'solve', 'this', 'problem', 'we', 'introduce',... | [-0.10397499508718346, 0.07520850213344585, -0.09104309525471904, 0.08468941093232592, -0.07425851128470984, -0.1125127660625985, 0.07189145748496725, 0.33227057786188224, -0.2539383524992657, -0.29231533150694977, 0.11258670785272204, -0.26772540096799363, -0.10214548310359886, 0.14912358002547282, -0.1173679800511979... |
708.2267 | Background Field Equations for the Duality Symmetric String | This paper describes the background field equations for strings in T-duality
symmetric formalisms in which the dimension of target space is doubled and the
sigma model supplemented with constraints. These are calculated by demanding
the vanishing of the beta-functional of the sigma model couplings in the
doubled targ... | hep-th | this paper describes the background field equations for strings in tduality symmetric formalisms in which the dimension of target space is doubled and the sigma model supplemented with constraints these are calculated by demanding the vanishing of the betafunctional of the sigma model couplings in the doubled target sp... | [['this', 'paper', 'describes', 'the', 'background', 'field', 'equations', 'for', 'strings', 'in', 'tduality', 'symmetric', 'formalisms', 'in', 'which', 'the', 'dimension', 'of', 'target', 'space', 'is', 'doubled', 'and', 'the', 'sigma', 'model', 'supplemented', 'with', 'constraints', 'these', 'are', 'calculated', 'by'... | [-0.14909595520132118, 0.14747760506967703, -0.022300580546023355, 0.09939177009084868, -0.04015751927351904, -0.11519175325889909, -0.00666671087928412, 0.30105096237763523, -0.22055331922121466, -0.31885375709287705, 0.044062081704078805, -0.26015659797167967, -0.1136990345955368, 0.11308996934103706, -0.025271698359... |
708.2268 | Tropical fans and the moduli spaces of tropical curves | We give a rigorous definition of tropical fans (the "local building blocks
for tropical varieties") and their morphisms. For such a morphism of tropical
fans of the same dimension we show that the number of inverse images (counted
with suitable tropical multiplicities) of a point in the target does not depend
on the ... | math.AG | we give a rigorous definition of tropical fans the local building blocks for tropical varieties and their morphisms for such a morphism of tropical fans of the same dimension we show that the number of inverse images counted with suitable tropical multiplicities of a point in the target does not depend on the chosen po... | [['we', 'give', 'a', 'rigorous', 'definition', 'of', 'tropical', 'fans', 'the', 'local', 'building', 'blocks', 'for', 'tropical', 'varieties', 'and', 'their', 'morphisms', 'for', 'such', 'a', 'morphism', 'of', 'tropical', 'fans', 'of', 'the', 'same', 'dimension', 'we', 'show', 'that', 'the', 'number', 'of', 'inverse', ... | [-0.15225575914924594, 0.07385060047823669, -0.13535064869766472, 0.12067538833526453, -0.07602368830880932, -0.08430758312714236, 0.06751530423524028, 0.29421488723170214, -0.344215645348184, -0.22598739599681084, 0.1279428346759732, -0.23398708205186683, -0.19515687821589353, 0.2365833379813463, -0.18825985421248861,... |
708.2269 | Quasi-periodic stability of normally resonant tori | We study quasi-periodic tori under a normal-internal resonance, possibly with
multiple eigenvalues. Two non-degeneracy conditions play a role. The first of
these generalizes invertibility of the Floquet matrix and prevents drift of the
lower dimensional torus. The second condition involves a Kolmogorov-like
variation... | math.DS | we study quasiperiodic tori under a normalinternal resonance possibly with multiple eigenvalues two nondegeneracy conditions play a role the first of these generalizes invertibility of the floquet matrix and prevents drift of the lower dimensional torus the second condition involves a kolmogorovlike variation of the in... | [['we', 'study', 'quasiperiodic', 'tori', 'under', 'a', 'normalinternal', 'resonance', 'possibly', 'with', 'multiple', 'eigenvalues', 'two', 'nondegeneracy', 'conditions', 'play', 'a', 'role', 'the', 'first', 'of', 'these', 'generalizes', 'invertibility', 'of', 'the', 'floquet', 'matrix', 'and', 'prevents', 'drift', 'o... | [-0.20846320609693272, 0.14624237744662333, -0.06754276012136064, 0.03965672310835249, -0.06722334863841009, -0.10451504288398673, 0.02985610924398815, 0.3398714040235524, -0.2530961873363966, -0.22833565358912022, 0.10883895632430492, -0.19791338752141932, -0.17587295830459662, 0.2124392875588276, -0.03802361565602707... |
708.227 | Capacity of the Degraded Half-Duplex Relay Channel | A discrete memoryless half-duplex relay channel is constructed from a
broadcast channel from the source to the relay and destination and a multiple
access channel from the source and relay to the destination. When the relay
listens, the channel operates in the broadcast mode. The channel switches to
the multiple acce... | cs.IT math.IT | a discrete memoryless halfduplex relay channel is constructed from a broadcast channel from the source to the relay and destination and a multiple access channel from the source and relay to the destination when the relay listens the channel operates in the broadcast mode the channel switches to the multiple access mod... | [['a', 'discrete', 'memoryless', 'halfduplex', 'relay', 'channel', 'is', 'constructed', 'from', 'a', 'broadcast', 'channel', 'from', 'the', 'source', 'to', 'the', 'relay', 'and', 'destination', 'and', 'a', 'multiple', 'access', 'channel', 'from', 'the', 'source', 'and', 'relay', 'to', 'the', 'destination', 'when', 'the... | [-0.2808224145735481, 0.04973804107201951, -0.06292026984372309, -0.02173328924524997, -0.1299238264547395, -0.3987452140769788, 0.16461882558850838, 0.3850167841916638, -0.3701987661314862, -0.18677064363445556, 0.12452901249817971, -0.24401583148166536, -0.09430757622500616, 0.10463667042021241, -0.14466650272054332,... |
708.2271 | Solution of the equation d/dx(pdu/dx)+qu=cu by a solution of the
equation d/dx(pdu/dx)+qu=0 | We give a simple solution of the equation d/dx(pdu/dx)+qu=cu whenever a
nontrivial solution of d/dx(pdu/dx)+qu=0 is known. The method developed for
obtaining this result is based on the theory of pseudoanalytic functions and
their relationship with solutions of the stationary two-dimensional Schrodinger
equation. The... | math-ph math.MP | we give a simple solution of the equation ddxpdudxqucu whenever a nontrivial solution of ddxpdudxqu0 is known the method developed for obtaining this result is based on the theory of pseudoanalytic functions and their relationship with solutions of the stationary twodimensional schrodinger equation the final result tha... | [['we', 'give', 'a', 'simple', 'solution', 'of', 'the', 'equation', 'ddxpdudxqucu', 'whenever', 'a', 'nontrivial', 'solution', 'of', 'ddxpdudxqu0', 'is', 'known', 'the', 'method', 'developed', 'for', 'obtaining', 'this', 'result', 'is', 'based', 'on', 'the', 'theory', 'of', 'pseudoanalytic', 'functions', 'and', 'their'... | [-0.11258595778546747, 0.0036594294304508838, -0.17036290160350262, 0.05576103777369304, -0.09487861635223512, -0.14681522434787644, 0.014252165623474866, 0.2781315775467984, -0.2488534387441412, -0.242862232209694, 0.13013917964041954, -0.272058718266987, -0.19796012585321743, 0.22943493483528013, 0.000987604485764618... |
708.2272 | Reflecting magnons | We study the worldsheet reflection matrix of a string attached to a D-brane
in $AdS_5 \times S^5$. The D-brane corresponds to a maximal giant graviton and
it wraps an $S^3$ inside $S^5$. In the gauge theory, the open string is
described by a spin chain with boundaries. We study an open string with a large
SO(6) charg... | hep-th | we study the worldsheet reflection matrix of a string attached to a dbrane in ads_5 times s5 the dbrane corresponds to a maximal giant graviton and it wraps an s3 inside s5 in the gauge theory the open string is described by a spin chain with boundaries we study an open string with a large so6 charge which allows us to... | [['we', 'study', 'the', 'worldsheet', 'reflection', 'matrix', 'of', 'a', 'string', 'attached', 'to', 'a', 'dbrane', 'in', 'ads_5', 'times', 's5', 'the', 'dbrane', 'corresponds', 'to', 'a', 'maximal', 'giant', 'graviton', 'and', 'it', 'wraps', 'an', 's3', 'inside', 's5', 'in', 'the', 'gauge', 'theory', 'the', 'open', 's... | [-0.17514954520530016, 0.14492171897240635, -0.06667807662519831, 0.07479767059268863, -0.0932201276849604, -0.12900749794588243, 0.03729176499262897, 0.3449848500906296, -0.21575241489335895, -0.2571336152061305, 0.12485158726581777, -0.2723595041024049, -0.10797393966009314, 0.1272483031271295, -0.03957695818986486, ... |
708.2273 | Opportunism in Multiuser Relay Channels: Scheduling, Routing and
Spectrum Reuse | In order to understand the key merits of multiuser diversity techniques in
relay-assisted cellular multihop networks, this paper analyzes the spectral
efficiency of opportunistic (i.e., channel-aware) scheduling algorithms over a
fading multiuser relay channel with $K$ users in the asymptotic regime of large
(but fin... | cs.IT math.IT | in order to understand the key merits of multiuser diversity techniques in relayassisted cellular multihop networks this paper analyzes the spectral efficiency of opportunistic ie channelaware scheduling algorithms over a fading multiuser relay channel with k users in the asymptotic regime of large but finite number of... | [['in', 'order', 'to', 'understand', 'the', 'key', 'merits', 'of', 'multiuser', 'diversity', 'techniques', 'in', 'relayassisted', 'cellular', 'multihop', 'networks', 'this', 'paper', 'analyzes', 'the', 'spectral', 'efficiency', 'of', 'opportunistic', 'ie', 'channelaware', 'scheduling', 'algorithms', 'over', 'a', 'fadin... | [-0.26280336055807235, -0.024011531272550034, -0.06214186349834979, 0.025302936264398977, -0.06451044642682997, -0.22189965806414488, 0.15079248635999226, 0.38359362518816603, -0.24861857177688912, -0.2733774556248796, 0.03785689423329446, -0.2245774344096776, -0.18912767429586524, 0.13911107057869873, -0.1135302465853... |
708.2274 | The first rotation periods in Praesepe | The cluster Praesepe (age 650 Myr) is an ideal laboratory to study stellar
evolution. Specifically, it allows us to trace the long-term decline of
rotation and activity on the main-sequence. Here we present rotation periods
measured for five stars in Praesepe with masses of 0.1-0.5Ms -- the first
rotation periods for... | astro-ph | the cluster praesepe age 650 myr is an ideal laboratory to study stellar evolution specifically it allows us to trace the longterm decline of rotation and activity on the mainsequence here we present rotation periods measured for five stars in praesepe with masses of 0105ms the first rotation periods for members of thi... | [['the', 'cluster', 'praesepe', 'age', '650', 'myr', 'is', 'an', 'ideal', 'laboratory', 'to', 'study', 'stellar', 'evolution', 'specifically', 'it', 'allows', 'us', 'to', 'trace', 'the', 'longterm', 'decline', 'of', 'rotation', 'and', 'activity', 'on', 'the', 'mainsequence', 'here', 'we', 'present', 'rotation', 'period... | [-0.1114752302716801, 0.18660851417533575, -0.09053572545685679, 0.11312787803836341, -0.09721456541890855, -0.056832329120500374, 0.08514785708812661, 0.4218233191364666, -0.19197540041576425, -0.3874887421638403, 0.05923936375468741, -0.23100267154091958, -0.03739814676525299, 0.23777838718487795, -0.0732417645438728... |
708.2275 | Completeness of the classical 2D Ising model and universal quantum
computation | We prove that the 2D Ising model is complete in the sense that the partition
function of any classical q-state spin model (on an arbitrary graph) can be
expressed as a special instance of the partition function of a 2D Ising model
with complex inhomogeneous couplings and external fields. In the case where the
origina... | quant-ph cond-mat.stat-mech | we prove that the 2d ising model is complete in the sense that the partition function of any classical qstate spin model on an arbitrary graph can be expressed as a special instance of the partition function of a 2d ising model with complex inhomogeneous couplings and external fields in the case where the original mode... | [['we', 'prove', 'that', 'the', '2d', 'ising', 'model', 'is', 'complete', 'in', 'the', 'sense', 'that', 'the', 'partition', 'function', 'of', 'any', 'classical', 'qstate', 'spin', 'model', 'on', 'an', 'arbitrary', 'graph', 'can', 'be', 'expressed', 'as', 'a', 'special', 'instance', 'of', 'the', 'partition', 'function',... | [-0.09690344770569936, 0.11966589707049025, -0.029953382924759353, 0.06937905262202548, -0.03894441619195277, -0.20053167527294136, -0.008182659848898766, 0.348231433541514, -0.25862070462608244, -0.2797915728879161, 0.07274958190009784, -0.246312488006879, -0.16514616897438827, 0.1786518635435641, 0.0158333048896111, ... |
708.2276 | Heterotic twistor-string theory | We reformulate twistor-string theory as a heterotic string based on a twisted
(0,2) model. The path integral localizes on holomorphic maps, while the (0,2)
moduli naturally correspond to the states of N=4 super Yang-Mills and conformal
supergravity under the Penrose transform. We show how the standard
twistor-string ... | hep-th | we reformulate twistorstring theory as a heterotic string based on a twisted 02 model the path integral localizes on holomorphic maps while the 02 moduli naturally correspond to the states of n4 super yangmills and conformal supergravity under the penrose transform we show how the standard twistorstring formulae of sca... | [['we', 'reformulate', 'twistorstring', 'theory', 'as', 'a', 'heterotic', 'string', 'based', 'on', 'a', 'twisted', '02', 'model', 'the', 'path', 'integral', 'localizes', 'on', 'holomorphic', 'maps', 'while', 'the', '02', 'moduli', 'naturally', 'correspond', 'to', 'the', 'states', 'of', 'n4', 'super', 'yangmills', 'and'... | [-0.09310829818436722, 0.15859568673176658, -0.11222570265617667, 0.14714408520643318, -0.09854674032983293, -0.10878761846213303, -0.027317441378318524, 0.29164337378140504, -0.19958342027363427, -0.24748061539246402, 0.0803135412332918, -0.272987759766092, -0.2554765384849332, 0.15186642424135102, -0.1219091259729151... |
708.2277 | A Chandra Observation of Abell 13: Investigating the Origin of the Radio
Relic | We present results from the Chandra X-ray observation of Abell 13, a galaxy
cluster that contains an unusual noncentral radio source, also known as a radio
relic. This is the first pointed X-ray observation of Abell 13, providing a
more sensitive study of the properties of the X-ray gas. The X-ray emission
from Abell... | astro-ph | we present results from the chandra xray observation of abell 13 a galaxy cluster that contains an unusual noncentral radio source also known as a radio relic this is the first pointed xray observation of abell 13 providing a more sensitive study of the properties of the xray gas the xray emission from abell 13 is exte... | [['we', 'present', 'results', 'from', 'the', 'chandra', 'xray', 'observation', 'of', 'abell', '13', 'a', 'galaxy', 'cluster', 'that', 'contains', 'an', 'unusual', 'noncentral', 'radio', 'source', 'also', 'known', 'as', 'a', 'radio', 'relic', 'this', 'is', 'the', 'first', 'pointed', 'xray', 'observation', 'of', 'abell',... | [-0.05447926770222879, 0.08866200171381687, -0.11732876795576885, 0.08353691567593823, -0.13314362381727007, -0.0260051365831267, 0.020998728009714286, 0.4534367521261891, -0.1615517849055261, -0.330237032127393, 0.08041962378676112, -0.33224839397106254, -0.01537031854771204, 0.20472507842942694, 0.029126074796510956,... |
708.2278 | Weighted hyperprojective spaces and homotopy invariance in orbifold
cohomology | We show that Chen-Ruan cohomology is a homotopy invariant in certain cases.
We introduce the notion of a T-representation homotopy, which is a stringent
form of homotopy under which Chen-Ruan cohomology is invariant. We show that
while hyperkahler quotients of the cotangent bundle to a complex vector space
by a circl... | math.SG math.DG | we show that chenruan cohomology is a homotopy invariant in certain cases we introduce the notion of a trepresentation homotopy which is a stringent form of homotopy under which chenruan cohomology is invariant we show that while hyperkahler quotients of the cotangent bundle to a complex vector space by a circle s1 her... | [['we', 'show', 'that', 'chenruan', 'cohomology', 'is', 'a', 'homotopy', 'invariant', 'in', 'certain', 'cases', 'we', 'introduce', 'the', 'notion', 'of', 'a', 'trepresentation', 'homotopy', 'which', 'is', 'a', 'stringent', 'form', 'of', 'homotopy', 'under', 'which', 'chenruan', 'cohomology', 'is', 'invariant', 'we', 's... | [-0.2527770855464041, 0.07747874016640707, -0.10491351988166571, 0.153554604841338, -0.12257985664182343, -0.1273421082238201, -0.04716496039181948, 0.4179436854319647, -0.36893098429427484, -0.14959225502680057, 0.0974726097585517, -0.19390952736139297, -0.20225113342748954, 0.17350324631406694, -0.24231694885529578, ... |
708.2279 | Relating gravitational wave constraints from primordial nucleosynthesis,
pulsar timing, laser interferometers, and the CMB: implications for the early
universe | We derive a general master equation relating the gravitational-wave
observables r and Omega_gw(f). Here r is the tensor-to-scalar ratio,
constrained by cosmic-microwave-background (CMB) experiments; and Omega_gw(f)
is the energy spectrum of primordial gravitational-waves, constrained e.g. by
pulsar-timing measurement... | astro-ph gr-qc hep-ph hep-th | we derive a general master equation relating the gravitationalwave observables r and omega_gwf here r is the tensortoscalar ratio constrained by cosmicmicrowavebackground cmb experiments and omega_gwf is the energy spectrum of primordial gravitationalwaves constrained eg by pulsartiming measurements laserinterferometer... | [['we', 'derive', 'a', 'general', 'master', 'equation', 'relating', 'the', 'gravitationalwave', 'observables', 'r', 'and', 'omega_gwf', 'here', 'r', 'is', 'the', 'tensortoscalar', 'ratio', 'constrained', 'by', 'cosmicmicrowavebackground', 'cmb', 'experiments', 'and', 'omega_gwf', 'is', 'the', 'energy', 'spectrum', 'of'... | [-0.1256627522402469, 0.15753833774247195, -0.11827069360658941, 0.0792823770265299, -0.0959470123664821, -0.13279197412168242, 0.024204446713391885, 0.2771488338471409, -0.2339812483303657, -0.32569015818273284, 0.09098920332169554, -0.27161317669129764, -0.07407002265015951, 0.18479060984227763, 0.004677035548052643,... |
708.228 | Minimal Number of Generators and Minimum Order of a Non-Abelian Group
whose Elements Commute with Their Endomorphic Images | A group in which every element commutes with its endomorphic images is called
an $E$-group. If $p$ is a prime number, a $p$-group $G$ which is an $E$-group
is called a $pE$-group. Every abelian group is obviously an $E$-group. We prove
that every 2-generator $E$-group is abelian and that all 3-generator $E$-groups
ar... | math.GR | a group in which every element commutes with its endomorphic images is called an egroup if p is a prime number a pgroup g which is an egroup is called a pegroup every abelian group is obviously an egroup we prove that every 2generator egroup is abelian and that all 3generator egroups are nilpotent of class at most 2 it... | [['a', 'group', 'in', 'which', 'every', 'element', 'commutes', 'with', 'its', 'endomorphic', 'images', 'is', 'called', 'an', 'egroup', 'if', 'p', 'is', 'a', 'prime', 'number', 'a', 'pgroup', 'g', 'which', 'is', 'an', 'egroup', 'is', 'called', 'a', 'pegroup', 'every', 'abelian', 'group', 'is', 'obviously', 'an', 'egroup... | [-0.20988106566770864, 0.1975940809062508, -0.10748311169367253, 0.05857915284616888, -0.11574255500943596, -0.17659932426216096, -0.06409001893935208, 0.37234775766440736, -0.25761852168943733, -0.20254148430183155, 0.11791769202657733, -0.2770828984720836, -0.13325501302210221, 0.2232190384333875, -0.1288399578095609... |
708.2281 | A lower bound for the number of conjugacy classes of finite groups | In 2000, L. H\'{e}thelyi and B. K\"{u}lshammer proved that if $p$ is a prime
number dividing the order of a finite solvable group $G$, then $G$ has at least
$2\sqrt{p-1}$ conjugacy classes. In this paper we show that if $p$ is large,
the result remains true for arbitrary finite groups.
| math.GR | in 2000 l hethelyi and b kulshammer proved that if p is a prime number dividing the order of a finite solvable group g then g has at least 2sqrtp1 conjugacy classes in this paper we show that if p is large the result remains true for arbitrary finite groups | [['in', '2000', 'l', 'hethelyi', 'and', 'b', 'kulshammer', 'proved', 'that', 'if', 'p', 'is', 'a', 'prime', 'number', 'dividing', 'the', 'order', 'of', 'a', 'finite', 'solvable', 'group', 'g', 'then', 'g', 'has', 'at', 'least', '2sqrtp1', 'conjugacy', 'classes', 'in', 'this', 'paper', 'we', 'show', 'that', 'if', 'p', '... | [-0.20098468532063524, 0.1812712082981455, -0.1026242143208427, 0.023269399271194577, -0.07898960906860171, -0.17505606549925037, 0.014324174474031493, 0.3281752551164554, -0.30008650593915764, -0.28935341390648056, 0.06551767318813624, -0.2485444253044469, -0.09575657574079778, 0.1613804246203936, -0.0921005417345738,... |
708.2282 | Minimal blocking sets in PG(n,2) and covering groups by subgroups | In this paper we prove that a set of points $B$ of PG(n,2) is a minimal
blocking set if and only if $<B>=PG(d,2)$ with $d$ odd and $B$ is a set of
$d+2$ points of $PG(d,2)$ no $d+1$ of them in the same hyperplane. As a
corollary to the latter result we show that if $G$ is a finite 2-group and $n$
is a positive intege... | math.GR math.CO | in this paper we prove that a set of points b of pgn2 is a minimal blocking set if and only if bpgd2 with d odd and b is a set of d2 points of pgd2 no d1 of them in the same hyperplane as a corollary to the latter result we show that if g is a finite 2group and n is a positive integer then g admits a mathfrakc_n1cover ... | [['in', 'this', 'paper', 'we', 'prove', 'that', 'a', 'set', 'of', 'points', 'b', 'of', 'pgn2', 'is', 'a', 'minimal', 'blocking', 'set', 'if', 'and', 'only', 'if', 'bpgd2', 'with', 'd', 'odd', 'and', 'b', 'is', 'a', 'set', 'of', 'd2', 'points', 'of', 'pgd2', 'no', 'd1', 'of', 'them', 'in', 'the', 'same', 'hyperplane', '... | [-0.19877269527604502, 0.14901595582308683, -0.04435510306258596, -0.0071049353648577965, -0.04646780976064263, -0.16081826308321567, 0.0837388625345944, 0.33480531126561186, -0.27761198046707336, -0.23932344368508746, 0.09228241123304132, -0.29750355789738314, -0.09737056486999555, 0.14231466472359194, -0.068310067361... |
708.2283 | On quasi-Baer rings of Ore extensions | Let $R$ be a ring and $S=R[x;\sigma,\delta]$ its Ore extension. We prove
under some conditions that $R$ is a quasi-Baer ring if and only if the Ore
extension $R[x;\sigma,\delta]$ is a quasi-Baer ring. Examples are provided to
illustrate and delimit our results.
| math.RA | let r be a ring and srxsigmadelta its ore extension we prove under some conditions that r is a quasibaer ring if and only if the ore extension rxsigmadelta is a quasibaer ring examples are provided to illustrate and delimit our results | [['let', 'r', 'be', 'a', 'ring', 'and', 'srxsigmadelta', 'its', 'ore', 'extension', 'we', 'prove', 'under', 'some', 'conditions', 'that', 'r', 'is', 'a', 'quasibaer', 'ring', 'if', 'and', 'only', 'if', 'the', 'ore', 'extension', 'rxsigmadelta', 'is', 'a', 'quasibaer', 'ring', 'examples', 'are', 'provided', 'to', 'illus... | [-0.18823058930475536, 0.017730370470572535, -0.11742047724745623, 0.025077904898264423, -0.07914154165106393, -0.22267116765241798, -0.08725556392767807, 0.36942732588547034, -0.3549203749110059, -0.12325709245008666, 0.23008519487182905, -0.25781749125297476, -0.12046954653611998, 0.2289764083376745, -0.1301093900053... |
708.2284 | The Role of MHD in the ICM and its Interactions with AGN Outflows | Magnetic fields probably play a central role in the dynamics and
thermodynamics of ICMs and their interactions with AGNs, despite the fact that
the fields usually contribute relatively little pressure; i.e., the ICM is a
``high-$\beta$'' plasma. More typically, the roles of magnetic fields come
through ``microscopic'... | astro-ph | magnetic fields probably play a central role in the dynamics and thermodynamics of icms and their interactions with agns despite the fact that the fields usually contribute relatively little pressure ie the icm is a highbeta plasma more typically the roles of magnetic fields come through microscopic influences on charg... | [['magnetic', 'fields', 'probably', 'play', 'a', 'central', 'role', 'in', 'the', 'dynamics', 'and', 'thermodynamics', 'of', 'icms', 'and', 'their', 'interactions', 'with', 'agns', 'despite', 'the', 'fact', 'that', 'the', 'fields', 'usually', 'contribute', 'relatively', 'little', 'pressure', 'ie', 'the', 'icm', 'is', 'a... | [-0.11702447053853815, 0.25368452773576505, -0.04290828382118458, 0.11341904453859714, -0.061605730529041274, -0.07386825162623274, -0.004886727221310139, 0.35816180741316395, -0.27975506492596314, -0.34086522881529835, 0.061031202475638376, -0.26396647715254834, -0.07794017154772423, 0.20559215169571537, 0.01154414126... |
708.2285 | Mapping an Island in the Landscape | We provide a complete classification and statistical analysis of all type IIA
orientifold compactifications with intersecting D6-branes on the orbifold
T^6/Z'_6. The total number of four dimensional N=1 supersymmetric models is
found to be O(10^23). After a statistical analysis of the gauge sector
properties of all p... | hep-th hep-ph | we provide a complete classification and statistical analysis of all type iia orientifold compactifications with intersecting d6branes on the orbifold t6z_6 the total number of four dimensional n1 supersymmetric models is found to be o1023 after a statistical analysis of the gauge sector properties of all possible solu... | [['we', 'provide', 'a', 'complete', 'classification', 'and', 'statistical', 'analysis', 'of', 'all', 'type', 'iia', 'orientifold', 'compactifications', 'with', 'intersecting', 'd6branes', 'on', 'the', 'orbifold', 't6z_6', 'the', 'total', 'number', 'of', 'four', 'dimensional', 'n1', 'supersymmetric', 'models', 'is', 'fo... | [-0.13651060434886647, 0.12876043369564846, -0.03640342131928684, 0.1402055679948087, -0.07519506265928683, -0.15885140789816013, 0.008700620212878745, 0.3220080771984962, -0.1257036242146009, -0.3062096067990821, 0.12120250550931534, -0.28203957558322984, -0.09480430570413144, 0.09384016848008077, -0.04828114603850945... |
708.2286 | Effective Spin-1/2 Description of Transverse-Field-Induced Random Fields
in Dipolar Spin Glasses with Strong Single-Ion Anisotropy | We present analytical and numerical evidence for the validity of an effective
S=1/2 approach to the description of random field generation in S>=1, and
especially in an S=1, dipolar spin glass models with strong uniaxial Ising
anisotropy and subject to weak external magnetic field Bx transverse to the
Ising direction... | cond-mat.dis-nn cond-mat.stat-mech | we present analytical and numerical evidence for the validity of an effective s12 approach to the description of random field generation in s1 and especially in an s1 dipolar spin glass models with strong uniaxial ising anisotropy and subject to weak external magnetic field bx transverse to the ising direction explicit... | [['we', 'present', 'analytical', 'and', 'numerical', 'evidence', 'for', 'the', 'validity', 'of', 'an', 'effective', 's12', 'approach', 'to', 'the', 'description', 'of', 'random', 'field', 'generation', 'in', 's1', 'and', 'especially', 'in', 'an', 's1', 'dipolar', 'spin', 'glass', 'models', 'with', 'strong', 'uniaxial',... | [-0.12675650758254858, 0.14985197976563575, -0.03996008861189087, 0.07138070383160892, -0.06753065347912963, -0.10626909340973253, -0.03168520017751251, 0.40751394202622276, -0.21448863410839328, -0.29428285718378094, 0.02255731583659158, -0.2766530828550458, -0.11631830355014514, 0.19096336587056242, 0.032781778548464... |
708.2287 | Q7-branes and their coupling to IIB supergravity | We show how, by making use of a new basis of the IIB supergravity
axion-dilaton coset, SL(2,R)/SO(2), 7-branes that belong to different conjugacy
classes of the duality group SL(2,R) naturally couple to IIB supergravity with
appropriate source terms characterized by an SL(2,R) charge matrix Q. The
conjugacy classes a... | hep-th | we show how by making use of a new basis of the iib supergravity axiondilaton coset sl2rso2 7branes that belong to different conjugacy classes of the duality group sl2r naturally couple to iib supergravity with appropriate source terms characterized by an sl2r charge matrix q the conjugacy classes are determined by the... | [['we', 'show', 'how', 'by', 'making', 'use', 'of', 'a', 'new', 'basis', 'of', 'the', 'iib', 'supergravity', 'axiondilaton', 'coset', 'sl2rso2', '7branes', 'that', 'belong', 'to', 'different', 'conjugacy', 'classes', 'of', 'the', 'duality', 'group', 'sl2r', 'naturally', 'couple', 'to', 'iib', 'supergravity', 'with', 'a... | [-0.1795868274399682, 0.18544125657118618, 0.020556460844304906, 0.09114459831257324, -0.12357680696774931, -0.16918531564913472, -0.032999405812006444, 0.3051553894919754, -0.2151056062156225, -0.2515965530345805, 0.09243868939794243, -0.2356024941922549, -0.14590184480852364, 0.10096419500597917, -0.09153266758521032... |
708.2288 | Scalar Trefoils | The knot model is extended by assuming that the trefoils are realized as
either chiral fermions or as scalar bosons. There are then four scalar trefoils
with electric charges (0, -1,2/3,-1/3) that may be classified in the same way
as the chiral fermions: as two isotopic doublets where the two doublets have
different ... | hep-th | the knot model is extended by assuming that the trefoils are realized as either chiral fermions or as scalar bosons there are then four scalar trefoils with electric charges 0 12313 that may be classified in the same way as the chiral fermions as two isotopic doublets where the two doublets have different hypercharge a... | [['the', 'knot', 'model', 'is', 'extended', 'by', 'assuming', 'that', 'the', 'trefoils', 'are', 'realized', 'as', 'either', 'chiral', 'fermions', 'or', 'as', 'scalar', 'bosons', 'there', 'are', 'then', 'four', 'scalar', 'trefoils', 'with', 'electric', 'charges', '0', '12313', 'that', 'may', 'be', 'classified', 'in', 't... | [-0.1567513826865189, 0.30066135834003316, -0.011857028792166664, 0.10201451500801466, -0.039818904278318176, -0.23448427490376192, -0.03366709944334459, 0.33104311286246985, -0.1553504381224449, -0.3083545760460326, 0.01916933502973828, -0.295516277904269, -0.044300002750442845, 0.04800666669977765, 0.0893381493133974... |
708.2289 | Definitive Evidence of Interlayer Coupling Between (Ga,Mn)As Layers
Separated by a Nonmagnetic Spacer | We have used polarized neutron reflectometry to study the structural and
magnetic properties of the individual layers in a series of
(Al,Be,Ga)As/(Ga,Mn)As/GaAs/(Ga,Mn)As multilayer samples. Structurally, we
observe that the samples are virtually identical except for the GaAs spacer
thickness (which varies from 3-12 ... | cond-mat.mtrl-sci | we have used polarized neutron reflectometry to study the structural and magnetic properties of the individual layers in a series of albegaasgamnasgaasgamnas multilayer samples structurally we observe that the samples are virtually identical except for the gaas spacer thickness which varies from 312 nm and confirm that... | [['we', 'have', 'used', 'polarized', 'neutron', 'reflectometry', 'to', 'study', 'the', 'structural', 'and', 'magnetic', 'properties', 'of', 'the', 'individual', 'layers', 'in', 'a', 'series', 'of', 'albegaasgamnasgaasgamnas', 'multilayer', 'samples', 'structurally', 'we', 'observe', 'that', 'the', 'samples', 'are', 'vi... | [-0.12553317013847898, 0.22257119619072013, 0.026361568058179557, -0.028839258219797055, -0.04127533859370843, -0.15501899663966312, 0.07897971338673454, 0.4947636195498964, -0.3112116366678822, -0.32041865620978066, 0.0078947866399624, -0.33132193858424824, -0.07022757158594449, 0.19704662722137256, 0.0411008725826885... |
708.229 | MASA's and certain type I closed faces of C*-algebras | A result of Akemann, Anderson, and Pedersen states that if a sequence of pure
states of a C*-algebra A approaches infinity in a certain sense, then there is
a MASA B such that each of the states has the unique extension property with
respect to B. We generalize this in two ways: We prove that B can be required
to con... | math.OA | a result of akemann anderson and pedersen states that if a sequence of pure states of a calgebra a approaches infinity in a certain sense then there is a masa b such that each of the states has the unique extension property with respect to b we generalize this in two ways we prove that b can be required to contain an a... | [['a', 'result', 'of', 'akemann', 'anderson', 'and', 'pedersen', 'states', 'that', 'if', 'a', 'sequence', 'of', 'pure', 'states', 'of', 'a', 'calgebra', 'a', 'approaches', 'infinity', 'in', 'a', 'certain', 'sense', 'then', 'there', 'is', 'a', 'masa', 'b', 'such', 'that', 'each', 'of', 'the', 'states', 'has', 'the', 'un... | [-0.11217307814065582, 0.1096499188342932, -0.06924023047591057, 0.045005859588295255, -0.06652011279052553, -0.19440730313474958, 0.024398632480789766, 0.3632366804589625, -0.3116967726695853, -0.16767970474729038, 0.11063504933582198, -0.28753441878563113, -0.14877587995187452, 0.16436527611222118, -0.160472838818140... |
708.2291 | The WEBT Campaign on the Blazar 3C279 in 2006 | The quasar 3C279 was the target of an extensive multiwavelength monitoring
campaign from January through April 2006, including an optical-IR-radio
monitoring campaign by the Whole Earth Blazar Telescope (WEBT) collaboration.
In this paper we focus on the results of the WEBT campaign. The source
exhibited substantial ... | astro-ph | the quasar 3c279 was the target of an extensive multiwavelength monitoring campaign from january through april 2006 including an opticalirradio monitoring campaign by the whole earth blazar telescope webt collaboration in this paper we focus on the results of the webt campaign the source exhibited substantial variabili... | [['the', 'quasar', '3c279', 'was', 'the', 'target', 'of', 'an', 'extensive', 'multiwavelength', 'monitoring', 'campaign', 'from', 'january', 'through', 'april', '2006', 'including', 'an', 'opticalirradio', 'monitoring', 'campaign', 'by', 'the', 'whole', 'earth', 'blazar', 'telescope', 'webt', 'collaboration', 'in', 'th... | [-0.09237040849384545, 0.15288011387349695, -0.06745878501593305, 0.06573582192061987, -0.11946185305834622, -0.11732913008843039, 0.058119218753886016, 0.48006097907104445, -0.18414332080673254, -0.3976991031857174, 0.10551939509237741, -0.2757436866204725, -0.05113516481516441, 0.23672410175768352, -0.065224965451016... |
708.2292 | Multiscale Analysis and Localization of Random Operators | A discussion of the method of multiscale analysis in the study of
localization of random operators based on lectures given at \emph{Random
Schr\"odinger operators: methods, results, and perspectives}, \'Etats de la
recherche, Universit\'e Paris 13, June 2002
| math-ph math.MP | a discussion of the method of multiscale analysis in the study of localization of random operators based on lectures given at emphrandom schrodinger operators methods results and perspectives etats de la recherche universite paris 13 june 2002 | [['a', 'discussion', 'of', 'the', 'method', 'of', 'multiscale', 'analysis', 'in', 'the', 'study', 'of', 'localization', 'of', 'random', 'operators', 'based', 'on', 'lectures', 'given', 'at', 'emphrandom', 'schrodinger', 'operators', 'methods', 'results', 'and', 'perspectives', 'etats', 'de', 'la', 'recherche', 'univers... | [-0.08196438758357151, 0.06470198621595832, -0.16150369466206915, 0.03818926889751408, -0.03159781944359074, -0.13954243742281924, -0.03380833306928744, 0.23613202264784156, -0.08723820238122465, -0.31427974034906236, 0.1593115734836288, -0.3594013810963244, -0.21186225216936422, 0.21719504688941949, -0.099366118955249... |
708.2293 | Localization for a continuum Cantor-Anderson Hamiltonian | We prove localization at the bottom of the spectrum for a random
Schr\"odinger operator in the continuum with a single-site potential
probability distribution supported by a Cantor set of zero Lebesgue measure.
This distribution is too singular to be treated by the usual methods. In
particular, an "a priori" Wegner e... | math-ph math.MP | we prove localization at the bottom of the spectrum for a random schrodinger operator in the continuum with a singlesite potential probability distribution supported by a cantor set of zero lebesgue measure this distribution is too singular to be treated by the usual methods in particular an a priori wegner estimate is... | [['we', 'prove', 'localization', 'at', 'the', 'bottom', 'of', 'the', 'spectrum', 'for', 'a', 'random', 'schrodinger', 'operator', 'in', 'the', 'continuum', 'with', 'a', 'singlesite', 'potential', 'probability', 'distribution', 'supported', 'by', 'a', 'cantor', 'set', 'of', 'zero', 'lebesgue', 'measure', 'this', 'distri... | [-0.058157452051234466, 0.09032633842446193, -0.11874871352856142, 0.11129373819915593, -0.057798349005206834, -0.13205513611296557, 0.06089217159677091, 0.3142432334180188, -0.2620958428734576, -0.2620180299263594, 0.11093768228934418, -0.26294525587146617, -0.10846812633603195, 0.17033197043012593, -0.093381195314463... |
708.2294 | A probabilistic regulatory network for the human immune system | In this paper we made a review of some papers about probabilistic regulatory
networks (PRN), in particular we introduce our concept of homomorphisms of PRN
with an example of projection of a regulatory network to a smaller one. We
apply the model PRN (or Probabilistic Boolean Network) to the immune system,
the PRN wo... | q-bio.CB q-bio.BM | in this paper we made a review of some papers about probabilistic regulatory networks prn in particular we introduce our concept of homomorphisms of prn with an example of projection of a regulatory network to a smaller one we apply the model prn or probabilistic boolean network to the immune system the prn works with ... | [['in', 'this', 'paper', 'we', 'made', 'a', 'review', 'of', 'some', 'papers', 'about', 'probabilistic', 'regulatory', 'networks', 'prn', 'in', 'particular', 'we', 'introduce', 'our', 'concept', 'of', 'homomorphisms', 'of', 'prn', 'with', 'an', 'example', 'of', 'projection', 'of', 'a', 'regulatory', 'network', 'to', 'a'... | [-0.11620623392491848, 0.05611588358066189, -0.031084039484032953, 0.06042625059255923, -0.05750031445988978, -0.1504705410836072, 0.06359229928508786, 0.38465824868829773, -0.295888005659498, -0.21649322325320935, 0.08178735378027048, -0.2685307095485643, -0.2506094204459939, 0.11185946500988612, -0.07468147554445541,... |
708.2295 | Product-free subsets of groups, then and now | A subset of a group is product-free if it does not contain elements a, b, c
such that ab = c. We review progress on the problem of determining the size of
the largest product-free subset of an arbitrary finite group, including a lower
bound due to the author, and a recent upper bound due to Gowers. The bound of
Gower... | math.GR math.CO | a subset of a group is productfree if it does not contain elements a b c such that ab c we review progress on the problem of determining the size of the largest productfree subset of an arbitrary finite group including a lower bound due to the author and a recent upper bound due to gowers the bound of gowers is more ge... | [['a', 'subset', 'of', 'a', 'group', 'is', 'productfree', 'if', 'it', 'does', 'not', 'contain', 'elements', 'a', 'b', 'c', 'such', 'that', 'ab', 'c', 'we', 'review', 'progress', 'on', 'the', 'problem', 'of', 'determining', 'the', 'size', 'of', 'the', 'largest', 'productfree', 'subset', 'of', 'an', 'arbitrary', 'finite'... | [-0.15246377997911104, 0.11534429555792615, -0.08389585300132499, 0.02341713870451453, -0.06148548755196056, -0.15538269048140915, 0.10542305000126362, 0.3045880876099026, -0.26285848734966877, -0.29896210147749763, 0.10297863087388189, -0.2489044113838515, -0.10116737866025817, 0.203274188330397, -0.08089075237512589,... |
708.2296 | Linking Jet Emission, X-ray States and Hard X-ray Tails in the Neutron
Star X-ray Binary GX 17+2 | We present the results from simultaneous radio (Very Large Array) and X-ray
(Rossi-X-ray Timing Explorer) observations of the Z-type neutron star X-ray
binary GX~17+2. The aim is to assess the coupling between X-ray and radio
properties throughout its three rapidly variable X-ray states and during the
time-resolved t... | astro-ph | we present the results from simultaneous radio very large array and xray rossixray timing explorer observations of the ztype neutron star xray binary gx172 the aim is to assess the coupling between xray and radio properties throughout its three rapidly variable xray states and during the timeresolved transitions these ... | [['we', 'present', 'the', 'results', 'from', 'simultaneous', 'radio', 'very', 'large', 'array', 'and', 'xray', 'rossixray', 'timing', 'explorer', 'observations', 'of', 'the', 'ztype', 'neutron', 'star', 'xray', 'binary', 'gx172', 'the', 'aim', 'is', 'to', 'assess', 'the', 'coupling', 'between', 'xray', 'and', 'radio', ... | [-0.09393197088606756, 0.12985588901008285, -0.06873426135136608, 0.12558352678122559, -0.08092307110605218, -0.05303850414172951, 0.09010125943793677, 0.4609583475096611, -0.2356923557032263, -0.32430404861929574, 0.08788282713683682, -0.315781421069841, -0.06712521429094298, 0.1993336389311109, 0.0544743606901097, -0... |
708.2297 | Densities, Parton Distributions, and Measuring the Non-Spherical Shape
of the Nucleon | Spin-dependent quark densities, matrix elements of specific density operators
in proton states of definite spin-polarization, indicate that the nucleon may
harbor an infinite variety of non-spherical shapes. We show that these matrix
elements are closely related to specific transverse momentum dependent parton
distri... | nucl-th hep-ex hep-ph nucl-ex | spindependent quark densities matrix elements of specific density operators in proton states of definite spinpolarization indicate that the nucleon may harbor an infinite variety of nonspherical shapes we show that these matrix elements are closely related to specific transverse momentum dependent parton distributions ... | [['spindependent', 'quark', 'densities', 'matrix', 'elements', 'of', 'specific', 'density', 'operators', 'in', 'proton', 'states', 'of', 'definite', 'spinpolarization', 'indicate', 'that', 'the', 'nucleon', 'may', 'harbor', 'an', 'infinite', 'variety', 'of', 'nonspherical', 'shapes', 'we', 'show', 'that', 'these', 'mat... | [-0.05777363863683516, 0.29091764742809584, -0.12117981484991633, 0.1709591408951148, -0.08675799234920452, -0.10321967748822444, 0.01698669817258594, 0.30844680812730585, -0.1991368351424093, -0.25735064593934887, -0.09099106212467035, -0.3650997581100592, 0.03890794409208641, 0.08172302998311978, 0.0766987154180164, ... |
708.2298 | The Number of Different Binary Functions Generated by NK-Kauffman
Networks and the Emergence of Genetic Robustness | We determine the average number $ \vartheta (N, K) $, of \textit{NK}-Kauffman
networks that give rise to the same binary function. We show that, for $ N \gg
1 $, there exists a connectivity critical value $ K_c $ such that $
\vartheta(N,K) \approx e^{\phi N} $ ($ \phi > 0 $) for $ K < K_c $ and
$\vartheta(N,K) \appro... | nlin.AO nlin.CD | we determine the average number vartheta n k of textitnkkauffman networks that give rise to the same binary function we show that for n gg 1 there exists a connectivity critical value k_c such that varthetank approx ephi n phi 0 for k k_c and varthetank approx 1 for k k_c we find that k_c is not a constant but scales v... | [['we', 'determine', 'the', 'average', 'number', 'vartheta', 'n', 'k', 'of', 'textitnkkauffman', 'networks', 'that', 'give', 'rise', 'to', 'the', 'same', 'binary', 'function', 'we', 'show', 'that', 'for', 'n', 'gg', '1', 'there', 'exists', 'a', 'connectivity', 'critical', 'value', 'k_c', 'such', 'that', 'varthetank', '... | [-0.23751476825250742, 0.2038925311778887, -0.0358553860149606, 0.0551690301340736, -0.002679242295786165, -0.23333464784082025, 0.09233094939890389, 0.31425564245392495, -0.25734017295046496, -0.3150842911922015, 0.008852563461494775, -0.3199662047778614, -0.15535925161272574, 0.14353370449792308, 0.0588604810853632, ... |
708.2299 | Global well-posedness for the radial defocusing cubic wave equation on
$\mathbb{R}^{3}$ and for rough data | We prove global well-posedness for the $3D$ radial defocusing cubic wave
equation with data in $H^{s} \times H^{s-1}$, $1>s>{7/10}$.
| math.AP math-ph math.MP | we prove global wellposedness for the 3d radial defocusing cubic wave equation with data in hs times hs1 1s710 | [['we', 'prove', 'global', 'wellposedness', 'for', 'the', '3d', 'radial', 'defocusing', 'cubic', 'wave', 'equation', 'with', 'data', 'in', 'hs', 'times', 'hs1', '1s710']] | [-0.15173536632210016, -0.01047877020513018, 0.00917114814122518, 0.10764865660005146, -0.04753057800957726, -0.09138193798975812, -0.1717918610924648, 0.31202688813209534, -0.24330365285277367, -0.16138476831838489, 0.1997625191320872, -0.34638900371889275, -0.06404479370555943, 0.12422319025629097, 0.0670384091014663... |
708.23 | Observation of Ferromagnetic Clusters in Bi0.125Ca0.875MnO3 | The electron doped manganite system, Bi0.125Ca0.875MnO3, exhibits large bulk
magnetization of unknown origin. To select amongst possible magnetic ordering
models, we have conducted temperature and magnetic field dependent small-angle
neutron scattering measurements. Nontrivial spin structure has been revealed.
Ferrom... | cond-mat.mtrl-sci | the electron doped manganite system bi0125ca0875mno3 exhibits large bulk magnetization of unknown origin to select amongst possible magnetic ordering models we have conducted temperature and magnetic field dependent smallangle neutron scattering measurements nontrivial spin structure has been revealed ferromagnetic spi... | [['the', 'electron', 'doped', 'manganite', 'system', 'bi0125ca0875mno3', 'exhibits', 'large', 'bulk', 'magnetization', 'of', 'unknown', 'origin', 'to', 'select', 'amongst', 'possible', 'magnetic', 'ordering', 'models', 'we', 'have', 'conducted', 'temperature', 'and', 'magnetic', 'field', 'dependent', 'smallangle', 'neu... | [-0.19048388653609435, 0.24564314200124499, -0.023419284727424383, 0.013930753765453118, -0.1096672625571955, -0.1050703528977465, 0.07457945450441912, 0.40656631495803597, -0.2401365156285465, -0.3559659451886546, -0.009870686613430735, -0.32742404397577046, -0.05464014202007093, 0.18984567062871066, 0.085272228880785... |
708.2301 | Ti-rich and Cu-poor grain-boundary layers of CaCu$_3$Ti$_4$O$_{12}$
detected by x-ray photoelectron spectroscopy | Cleaved and polished surfaces of CaCu$_3$Ti$_4$O$_{12}$ ceramics have been
investigated by x-ray photoelectron spectroscopy (XPS) and energy dispersive
x-ray spectroscopy (EDX), respectively. While EDX technique shows the identical
CaCu$_3$Ti$_4$O$_{12}$ stoichiometry for the two surfaces, XPS indicates that
the clea... | cond-mat.mtrl-sci cond-mat.other | cleaved and polished surfaces of cacu_3ti_4o_12 ceramics have been investigated by xray photoelectron spectroscopy xps and energy dispersive xray spectroscopy edx respectively while edx technique shows the identical cacu_3ti_4o_12 stoichiometry for the two surfaces xps indicates that the cleaved surface with grainbound... | [['cleaved', 'and', 'polished', 'surfaces', 'of', 'cacu_3ti_4o_12', 'ceramics', 'have', 'been', 'investigated', 'by', 'xray', 'photoelectron', 'spectroscopy', 'xps', 'and', 'energy', 'dispersive', 'xray', 'spectroscopy', 'edx', 'respectively', 'while', 'edx', 'technique', 'shows', 'the', 'identical', 'cacu_3ti_4o_12', ... | [-0.04514564563558526, 0.1485144408126298, -0.10012291006310141, 0.01728498450422991, 0.027556126605566233, -0.19029059139884089, 0.11703694034256168, 0.5323974419997571, -0.2401871088356392, -0.3078966999605094, -0.030970295304304934, -0.4471112109197635, -0.10368405126851715, 0.19011488546655603, 0.04395524459597591,... |
708.2302 | Nondestructive interaction-free atom-photon controlled-NOT gate | We present a probabilistic (ideally 50%) nondestructive interaction-free
atom-photon controlled-NOT gate, where nondestructive means that all four
outgoing target photon modes of the gate are available and feed-forwardable.
Individual atoms are controlled by a stimulated Raman adiabatic passage
transition and photons... | quant-ph | we present a probabilistic ideally 50 nondestructive interactionfree atomphoton controllednot gate where nondestructive means that all four outgoing target photon modes of the gate are available and feedforwardable individual atoms are controlled by a stimulated raman adiabatic passage transition and photons by a ring ... | [['we', 'present', 'a', 'probabilistic', 'ideally', '50', 'nondestructive', 'interactionfree', 'atomphoton', 'controllednot', 'gate', 'where', 'nondestructive', 'means', 'that', 'all', 'four', 'outgoing', 'target', 'photon', 'modes', 'of', 'the', 'gate', 'are', 'available', 'and', 'feedforwardable', 'individual', 'atom... | [-0.14546213179807335, 0.2699265698384907, -0.024189451047115857, -0.025772498938668932, 0.0012093591555539104, -0.28876815093163816, 0.07927113201779624, 0.4625474608192841, -0.2110940451733768, -0.2777789541830619, 0.006706815848075268, -0.26942538505213126, -0.04178275949218207, 0.25932665076106787, 0.02529011319727... |
708.2303 | Compositional Semantics Grounded in Commonsense Metaphysics | We argue for a compositional semantics grounded in a strongly typed ontology
that reflects our commonsense view of the world and the way we talk about it in
ordinary language. Assuming the existence of such a structure, we show that the
semantics of various natural language phenomena may become nearly trivial.
| cs.AI cs.CL | we argue for a compositional semantics grounded in a strongly typed ontology that reflects our commonsense view of the world and the way we talk about it in ordinary language assuming the existence of such a structure we show that the semantics of various natural language phenomena may become nearly trivial | [['we', 'argue', 'for', 'a', 'compositional', 'semantics', 'grounded', 'in', 'a', 'strongly', 'typed', 'ontology', 'that', 'reflects', 'our', 'commonsense', 'view', 'of', 'the', 'world', 'and', 'the', 'way', 'we', 'talk', 'about', 'it', 'in', 'ordinary', 'language', 'assuming', 'the', 'existence', 'of', 'such', 'a', 's... | [-0.1492084377244407, 0.05580287759977521, -0.134164769622479, 0.14784760725702725, -0.1658845542400491, -0.06441490970296311, 0.04845112682703663, 0.3753973567748771, -0.3215816684395951, -0.3230959031657845, 0.009051251987579698, -0.23798200013298615, -0.21189787722758802, 0.16934865030149618, -0.10990675393601551, -... |
708.2304 | Inverse problems for linear forms over finite sets of integers | Let f(x_1,x_2,...,x_m) = u_1x_1+u_2 x_2+... + u_mx_m be a linear form with
positive integer coefficients, and let N_f(k) = min{|f(A)| : A \subseteq Z and
|A|=k}. A minimizing k-set for f is a set A such that |A|=k and |f(A)| =
N_f(k). A finite sequence (u_1, u_2,...,u_m) of positive integers is called
complete if {\s... | math.NT math.CO | let fx_1x_2x_m u_1x_1u_2 x_2 u_mx_m be a linear form with positive integer coefficients and let n_fk minfa a subseteq z and ak a minimizing kset for f is a set a such that ak and fa n_fk a finite sequence u_1 u_2u_m of positive integers is called complete if sum_jin j u_j j subseteq 12m 012 u where u sum_j1m u_j it is ... | [['let', 'fx_1x_2x_m', 'u_1x_1u_2', 'x_2', 'u_mx_m', 'be', 'a', 'linear', 'form', 'with', 'positive', 'integer', 'coefficients', 'and', 'let', 'n_fk', 'minfa', 'a', 'subseteq', 'z', 'and', 'ak', 'a', 'minimizing', 'kset', 'for', 'f', 'is', 'a', 'set', 'a', 'such', 'that', 'ak', 'and', 'fa', 'n_fk', 'a', 'finite', 'sequ... | [-0.24962461889354567, 0.14421555765030195, -0.01897017785696068, -0.03861777064733847, -0.07083460069120381, -0.2142268739207977, 0.007348238639862776, 0.3236229225165314, -0.34317239945886113, -0.1248462440662387, 0.05496810737414041, -0.3917547274343293, -0.07688484128301191, 0.17374840991176438, -0.0457641888801431... |
708.2305 | Abnormal Electronic Transport in Disordered Graphene Nanoribbon | We investigate the conductivity $\sigma$ of graphene nanoribbons with zigzag
edges as a function of Fermi energy $E_F$ in the presence of the impurities
with different potential range. The dependence of $\sigma(E_F)$ displays four
different types of behavior, classified to different regimes of length scales
decided b... | cond-mat.mes-hall cond-mat.dis-nn | we investigate the conductivity sigma of graphene nanoribbons with zigzag edges as a function of fermi energy e_f in the presence of the impurities with different potential range the dependence of sigmae_f displays four different types of behavior classified to different regimes of length scales decided by the impurity... | [['we', 'investigate', 'the', 'conductivity', 'sigma', 'of', 'graphene', 'nanoribbons', 'with', 'zigzag', 'edges', 'as', 'a', 'function', 'of', 'fermi', 'energy', 'e_f', 'in', 'the', 'presence', 'of', 'the', 'impurities', 'with', 'different', 'potential', 'range', 'the', 'dependence', 'of', 'sigmae_f', 'displays', 'fou... | [-0.1420748817464827, 0.14662002188088719, -0.04476290658982307, 0.01739779605709931, -0.008373104000623388, -0.13559153703732718, 0.057255045641540436, 0.3583316242224292, -0.2714944105807757, -0.36464000043965744, 0.019907862970221527, -0.3253507477276256, -0.12219779891076318, 0.17765932026923748, 0.0018805297757417... |
708.2306 | Effects of impurities on Tamm-like lanthanide-metal surface states | The effects of isolated residual-gas adsorbates on the local electronic
structure of the Dy(0001) surface were spatially mapped by scanning tunneling
microscopy and spectroscopy at 12 K. Less than 15 A away from an adsorbate, a
strong reduction of the intensity and a significant increase of the width of
the majority ... | cond-mat.mtrl-sci | the effects of isolated residualgas adsorbates on the local electronic structure of the dy0001 surface were spatially mapped by scanning tunneling microscopy and spectroscopy at 12 k less than 15 a away from an adsorbate a strong reduction of the intensity and a significant increase of the width of the majority compone... | [['the', 'effects', 'of', 'isolated', 'residualgas', 'adsorbates', 'on', 'the', 'local', 'electronic', 'structure', 'of', 'the', 'dy0001', 'surface', 'were', 'spatially', 'mapped', 'by', 'scanning', 'tunneling', 'microscopy', 'and', 'spectroscopy', 'at', '12', 'k', 'less', 'than', '15', 'a', 'away', 'from', 'an', 'adso... | [-0.129359672541908, 0.17240582060970083, -0.08534041553568304, 0.03370174642500541, 0.029361236045199832, -0.11173003205631891, 0.08647287869237343, 0.35663813411184914, -0.2665784198979146, -0.33917582181564876, 0.025825333085664537, -0.3425537973977207, -0.08390625444858262, 0.14987245135616217, 0.01716693972624587,... |
708.2307 | Small value estimates for the additive group | We generalize Gel'fond's criterion of algebraic independence to the context
of a sequence of polynomials whose first derivatives take small values on large
subsets of a fixed subgroup of the additive group of complex numbers, instead
of just one point. We also provide one extension dealing with a subgroup of the
mult... | math.NT | we generalize gelfonds criterion of algebraic independence to the context of a sequence of polynomials whose first derivatives take small values on large subsets of a fixed subgroup of the additive group of complex numbers instead of just one point we also provide one extension dealing with a subgroup of the multiplica... | [['we', 'generalize', 'gelfonds', 'criterion', 'of', 'algebraic', 'independence', 'to', 'the', 'context', 'of', 'a', 'sequence', 'of', 'polynomials', 'whose', 'first', 'derivatives', 'take', 'small', 'values', 'on', 'large', 'subsets', 'of', 'a', 'fixed', 'subgroup', 'of', 'the', 'additive', 'group', 'of', 'complex', '... | [-0.2252564119795958, 0.09036933660115067, -0.08958273645686476, 0.06987226083711312, -0.1313018953435842, -0.10378689371997066, 0.09572505003368285, 0.28070680060211506, -0.31409729963266536, -0.24732506605224652, 0.12208230987910115, -0.2316151768287742, -0.11738901709516843, 0.18386230666778589, -0.1004346087411569,... |
708.2308 | Intermittent dynamics and 1/f^beta noise in single cardiac muscle cells | Fluctuations in the spontaneous beating activity of isolated cardiac cells
were studied over a timescale of six decades. The beat dynamics of single
cardiac cells were heterogeneous and intermittent. The interbeat intervals
(IBIs) were power-law distributed in a long-time regime. Furthermore, for long
timescales up t... | q-bio.CB | fluctuations in the spontaneous beating activity of isolated cardiac cells were studied over a timescale of six decades the beat dynamics of single cardiac cells were heterogeneous and intermittent the interbeat intervals ibis were powerlaw distributed in a longtime regime furthermore for long timescales up to the expe... | [['fluctuations', 'in', 'the', 'spontaneous', 'beating', 'activity', 'of', 'isolated', 'cardiac', 'cells', 'were', 'studied', 'over', 'a', 'timescale', 'of', 'six', 'decades', 'the', 'beat', 'dynamics', 'of', 'single', 'cardiac', 'cells', 'were', 'heterogeneous', 'and', 'intermittent', 'the', 'interbeat', 'intervals', ... | [-0.1724786232531953, 0.18938968496839056, -0.0569791854481752, 0.07660679155378602, 0.00851256041603751, -0.11980393979281775, 0.030566960416954794, 0.40446358703468976, -0.24205934282049144, -0.26271196493976995, 0.09765482520819396, -0.2778259588307456, -0.1566914080299045, 0.25455215999758557, -0.053176994239421266... |
708.2309 | On Compact Routing for the Internet | While there exist compact routing schemes designed for grids, trees, and
Internet-like topologies that offer routing tables of sizes that scale
logarithmically with the network size, we demonstrate in this paper that in
view of recent results in compact routing research, such logarithmic scaling on
Internet-like topo... | cs.NI | while there exist compact routing schemes designed for grids trees and internetlike topologies that offer routing tables of sizes that scale logarithmically with the network size we demonstrate in this paper that in view of recent results in compact routing research such logarithmic scaling on internetlike topologies i... | [['while', 'there', 'exist', 'compact', 'routing', 'schemes', 'designed', 'for', 'grids', 'trees', 'and', 'internetlike', 'topologies', 'that', 'offer', 'routing', 'tables', 'of', 'sizes', 'that', 'scale', 'logarithmically', 'with', 'the', 'network', 'size', 'we', 'demonstrate', 'in', 'this', 'paper', 'that', 'in', 'vi... | [-0.1849312411051662, 0.09467646804795883, -0.08660649779971831, 0.06630343808925157, -0.09195041326110405, -0.19393430430960806, 0.10175667705472641, 0.4239690474151999, -0.24155887485705788, -0.3263141271250051, 0.0852955467807412, -0.23383827629216203, -0.1634628697876123, 0.1721722271876952, -0.09941354432567671, 0... |
708.231 | Benefiting from Disorder: Source Coding for Unordered Data | The order of letters is not always relevant in a communication task. This
paper discusses the implications of order irrelevance on source coding,
presenting results in several major branches of source coding theory: lossless
coding, universal lossless coding, rate-distortion, high-rate quantization, and
universal los... | cs.IT math.IT | the order of letters is not always relevant in a communication task this paper discusses the implications of order irrelevance on source coding presenting results in several major branches of source coding theory lossless coding universal lossless coding ratedistortion highrate quantization and universal lossy coding t... | [['the', 'order', 'of', 'letters', 'is', 'not', 'always', 'relevant', 'in', 'a', 'communication', 'task', 'this', 'paper', 'discusses', 'the', 'implications', 'of', 'order', 'irrelevance', 'on', 'source', 'coding', 'presenting', 'results', 'in', 'several', 'major', 'branches', 'of', 'source', 'coding', 'theory', 'lossl... | [-0.20601259543440797, 0.1179588232965519, -0.045523479448295094, 0.0643901201943259, -0.01789644437829136, -0.2585653853942252, 0.12871458968018284, 0.3578169805437533, -0.26723286791497636, -0.20744073098628885, 0.11358015637880373, -0.26006304984427214, -0.16187255915428977, 0.2283167189230476, -0.1796371900062594, ... |
708.2311 | Phase Transition Dynamics and Its Alpha' Corrections | We study the dynamics of the first order phase transition in the holographic
hard wall model, namely, Polchinski-Strassler's model and come to the
conclusion that the phase transition is incomplete in large N limit with the
natural boundary condition. We also consider the string length corrections to
both hard wall m... | hep-th hep-ph | we study the dynamics of the first order phase transition in the holographic hard wall model namely polchinskistrasslers model and come to the conclusion that the phase transition is incomplete in large n limit with the natural boundary condition we also consider the string length corrections to both hard wall model an... | [['we', 'study', 'the', 'dynamics', 'of', 'the', 'first', 'order', 'phase', 'transition', 'in', 'the', 'holographic', 'hard', 'wall', 'model', 'namely', 'polchinskistrasslers', 'model', 'and', 'come', 'to', 'the', 'conclusion', 'that', 'the', 'phase', 'transition', 'is', 'incomplete', 'in', 'large', 'n', 'limit', 'with... | [-0.1262393937768965, 0.178974456972245, -0.09230650034309788, 0.09784200802713519, -0.03660190827918775, -0.142262913674737, 0.048745363911924265, 0.34963923218575393, -0.2575977523176169, -0.2787861402682734, 0.10105677127880468, -0.2887203700163148, -0.15525242170163742, 0.06705766717310656, 0.007127265340055932, 0.... |
708.2312 | Markov bases for two-way subtable sum problems | It has been well-known that for two-way contingency tables with fixed row
sums and column sums the set of square-free moves of degree two forms a Markov
basis. However when we impose an additional constraint that the sum of a
subtable is also fixed, then these moves do not necessarily form a Markov
basis. Thus, in th... | math.CO math.AC | it has been wellknown that for twoway contingency tables with fixed row sums and column sums the set of squarefree moves of degree two forms a markov basis however when we impose an additional constraint that the sum of a subtable is also fixed then these moves do not necessarily form a markov basis thus in this paper ... | [['it', 'has', 'been', 'wellknown', 'that', 'for', 'twoway', 'contingency', 'tables', 'with', 'fixed', 'row', 'sums', 'and', 'column', 'sums', 'the', 'set', 'of', 'squarefree', 'moves', 'of', 'degree', 'two', 'forms', 'a', 'markov', 'basis', 'however', 'when', 'we', 'impose', 'an', 'additional', 'constraint', 'that', '... | [-0.16123655095423867, 0.13851514360572853, -0.07895021447230403, 0.03556766167351204, -0.08976592451174993, -0.14548678787016286, 0.10748920787733457, 0.38337157839318603, -0.313151490443, -0.21585219631698438, 0.13537920045342705, -0.23086426477515842, -0.13592112773075338, 0.12739857482133296, -0.03276787387070859, ... |
708.2313 | Comparative study of electron and hole doped High-Tc compounds in
pseudogap regime: LDA+DMFT+Sk approach | Pseudogap regime for the prototype high-Tc compounds hole doped
Bi2Sr2CaCu2O8-x (Bi2212) and electron doped Nd2-xCexCuO4 (NCCO) is described by
means of novel generalized LDA+DMFT+Sk approach. Here conventional dynamical
mean-field theory (DMFT) equations are supplied with additional (momentum
dependent) self-energy ... | cond-mat.str-el cond-mat.supr-con | pseudogap regime for the prototype hightc compounds hole doped bi2sr2cacu2o8x bi2212 and electron doped nd2xcexcuo4 ncco is described by means of novel generalized ldadmftsk approach here conventional dynamical meanfield theory dmft equations are supplied with additional momentum dependent selfenergy sk in the present ... | [['pseudogap', 'regime', 'for', 'the', 'prototype', 'hightc', 'compounds', 'hole', 'doped', 'bi2sr2cacu2o8x', 'bi2212', 'and', 'electron', 'doped', 'nd2xcexcuo4', 'ncco', 'is', 'described', 'by', 'means', 'of', 'novel', 'generalized', 'ldadmftsk', 'approach', 'here', 'conventional', 'dynamical', 'meanfield', 'theory', ... | [-0.16863064115635112, 0.2085260540683059, -0.0209862407618424, 0.08511246554091544, -0.019822637203134715, -0.20713545730344893, 0.07701923923718462, 0.39575998819181846, -0.22885525543166468, -0.26771563979693586, -0.08933948379911719, -0.4239318075087217, -0.11834974929187743, 0.15611452615028987, 0.0629862020647297... |
708.2314 | Spectacular Trailing Streamers near LMC X-1: The First Evidence of a
Jet? | We report VIMOS integral field spectroscopy of the N159F nebula surrounding
LMC X-1. Our observations reveal a rich, extended system of emission line
filaments lining the boundary of a large conical cavity identified in Spitzer
mid-IR imaging. We find that X-ray photoionization cannot be solely responsible
for the ob... | astro-ph | we report vimos integral field spectroscopy of the n159f nebula surrounding lmc x1 our observations reveal a rich extended system of emission line filaments lining the boundary of a large conical cavity identified in spitzer midir imaging we find that xray photoionization cannot be solely responsible for the observed i... | [['we', 'report', 'vimos', 'integral', 'field', 'spectroscopy', 'of', 'the', 'n159f', 'nebula', 'surrounding', 'lmc', 'x1', 'our', 'observations', 'reveal', 'a', 'rich', 'extended', 'system', 'of', 'emission', 'line', 'filaments', 'lining', 'the', 'boundary', 'of', 'a', 'large', 'conical', 'cavity', 'identified', 'in',... | [-0.09664268565900398, 0.10948928638721224, -0.10677021680484441, 0.11177493041913929, -0.12781333553103844, -0.10327849145908134, 0.0325859673537321, 0.4751288212948676, -0.2196777920436227, -0.28027426935450145, 0.07365998133547802, -0.2535100609759066, -0.04587558561682024, 0.1989179084793608, 0.017532579943001496, ... |
708.2315 | Conformal representations of Leibniz algebras | In this note we present a more detailed and explicit exposition of the
definition of a conformal representation of a Leibniz algebra. Recall
(arXiv:math/0611501v3) that Leibniz algebras are exactly Lie dialgebras. The
idea is based on the general fact that every dialgebra that belongs to a
variety $\Var $ can be embe... | math.RA math.QA | in this note we present a more detailed and explicit exposition of the definition of a conformal representation of a leibniz algebra recall arxivmath0611501v3 that leibniz algebras are exactly lie dialgebras the idea is based on the general fact that every dialgebra that belongs to a variety var can be embedded into a ... | [['in', 'this', 'note', 'we', 'present', 'a', 'more', 'detailed', 'and', 'explicit', 'exposition', 'of', 'the', 'definition', 'of', 'a', 'conformal', 'representation', 'of', 'a', 'leibniz', 'algebra', 'recall', 'arxivmath0611501v3', 'that', 'leibniz', 'algebras', 'are', 'exactly', 'lie', 'dialgebras', 'the', 'idea', 'i... | [-0.12460508228105027, 0.032717938175251635, -0.14561907714563527, 0.06542395525188609, -0.1924471677365628, -0.12535823460943488, -0.05752578093299896, 0.36102075781673193, -0.31740150262009015, -0.14764044794719666, 0.1529967783955561, -0.1923456982847049, -0.1952423636155965, 0.17842293067687107, -0.1544514442264864... |
708.2316 | Generalized rational blow-down, torus knots, and Euclidean algorithm | We construct a Kirby diagram of the rational homology ball used in
"generalized rational blow-down" developed by Jongil Park. The diagram consists
of a dotted circle and a torus knot. The link is simpler, but the parameters
are a little complicate. Euclidean Algorithm is used three times in the
construction and the p... | math.GT | we construct a kirby diagram of the rational homology ball used in generalized rational blowdown developed by jongil park the diagram consists of a dotted circle and a torus knot the link is simpler but the parameters are a little complicate euclidean algorithm is used three times in the construction and the proof | [['we', 'construct', 'a', 'kirby', 'diagram', 'of', 'the', 'rational', 'homology', 'ball', 'used', 'in', 'generalized', 'rational', 'blowdown', 'developed', 'by', 'jongil', 'park', 'the', 'diagram', 'consists', 'of', 'a', 'dotted', 'circle', 'and', 'a', 'torus', 'knot', 'the', 'link', 'is', 'simpler', 'but', 'the', 'pa... | [-0.1805235391948372, 0.052093706639985055, -0.14801448522708738, 0.14215789293386757, -0.12380196992307901, -0.16983510034445387, 0.06658747767169888, 0.32185096798751217, -0.20985146110447553, -0.2527236950655396, 0.13633584754559427, -0.20964657344246426, -0.21698047779500484, 0.19655350096917784, -0.174392142315180... |
708.2317 | Effects of nuclear molecular configurations on the astrophysical
S-factor for $^{16}$O + $^{16}$O | The impact of nuclear molecular configurations on the astrophysical S-factor
for $^{16}$O + $^{16}$O is investigated within the realistic two-center shell
model based on Woods-Saxon potentials. These molecular effects refer to the
formation of a neck between the interacting nuclei and the radial dependent
collective ... | nucl-th | the impact of nuclear molecular configurations on the astrophysical sfactor for 16o 16o is investigated within the realistic twocenter shell model based on woodssaxon potentials these molecular effects refer to the formation of a neck between the interacting nuclei and the radial dependent collective mass parameter it ... | [['the', 'impact', 'of', 'nuclear', 'molecular', 'configurations', 'on', 'the', 'astrophysical', 'sfactor', 'for', '16o', '16o', 'is', 'investigated', 'within', 'the', 'realistic', 'twocenter', 'shell', 'model', 'based', 'on', 'woodssaxon', 'potentials', 'these', 'molecular', 'effects', 'refer', 'to', 'the', 'formation... | [-0.05316724644645172, 0.12696431556661777, -0.04317745431919819, 0.1185484851251685, -0.03269356137881165, -0.08918260173032097, 0.046622878328586616, 0.34670869723035425, -0.15358640923046088, -0.34278055383797706, -0.010840242280049579, -0.24781041123959072, -0.07457606241052203, 0.18701035993895038, -0.015066285107... |
708.2318 | Electronic structures of hexagonal RMnO3 (R = Gd, Tb, Dy, and Ho) thin
films | We investigated the electronic structure of multiferroic hexagonal RMnO3 (R =
Gd, Tb, Dy, and Ho) thin films using both optical spectroscopy and
first-principles calculations. Using artificially stabilized hexagonal RMnO3,
we extended the optical spectroscopic studies on the hexagonal multiferroic
manganite system. W... | cond-mat.str-el | we investigated the electronic structure of multiferroic hexagonal rmno3 r gd tb dy and ho thin films using both optical spectroscopy and firstprinciples calculations using artificially stabilized hexagonal rmno3 we extended the optical spectroscopic studies on the hexagonal multiferroic manganite system we observed tw... | [['we', 'investigated', 'the', 'electronic', 'structure', 'of', 'multiferroic', 'hexagonal', 'rmno3', 'r', 'gd', 'tb', 'dy', 'and', 'ho', 'thin', 'films', 'using', 'both', 'optical', 'spectroscopy', 'and', 'firstprinciples', 'calculations', 'using', 'artificially', 'stabilized', 'hexagonal', 'rmno3', 'we', 'extended', ... | [-0.1401132118816559, 0.1647334576647084, 0.04701871767353553, 0.012212786845898686, 0.003883697789681789, -0.11494058043910907, 0.1647887422165905, 0.46386607656112083, -0.2682084971197093, -0.29141408260911705, -0.01223274948917186, -0.3937809398541084, -0.08961634365214895, 0.0843988567420568, 0.07618043642634383, -... |
708.2319 | On Semimeasures Predicting Martin-Loef Random Sequences | Solomonoff's central result on induction is that the posterior of a universal
semimeasure M converges rapidly and with probability 1 to the true sequence
generating posterior mu, if the latter is computable. Hence, M is eligible as a
universal sequence predictor in case of unknown mu. Despite some nearby results
and ... | cs.IT cs.LG math.IT math.PR | solomonoffs central result on induction is that the posterior of a universal semimeasure m converges rapidly and with probability 1 to the true sequence generating posterior mu if the latter is computable hence m is eligible as a universal sequence predictor in case of unknown mu despite some nearby results and proofs ... | [['solomonoffs', 'central', 'result', 'on', 'induction', 'is', 'that', 'the', 'posterior', 'of', 'a', 'universal', 'semimeasure', 'm', 'converges', 'rapidly', 'and', 'with', 'probability', '1', 'to', 'the', 'true', 'sequence', 'generating', 'posterior', 'mu', 'if', 'the', 'latter', 'is', 'computable', 'hence', 'm', 'is... | [-0.12437415330371421, 0.14142874513087528, -0.07723177670368127, 0.12638711537034916, -0.04859209002394761, -0.17074240666947194, 0.08188400255383126, 0.36465383293373244, -0.29333474614790506, -0.2462536196676748, 0.08057591224687972, -0.254170134014317, -0.12670758569347007, 0.20389622787346265, -0.10096083517785051... |
708.232 | The non-viscous Burgers equation associated with random positions in
coordinate space: a threshold for blow up behaviour | It is well known that the solutions to the non-viscous Burgers equation
develop a gradient catastrophe at a critical time provided the initial data
have a negative derivative in certain points. We consider this equation
assuming that the particle paths in the medium are governed by a random process
with a variance wh... | math.AP math.PR | it is well known that the solutions to the nonviscous burgers equation develop a gradient catastrophe at a critical time provided the initial data have a negative derivative in certain points we consider this equation assuming that the particle paths in the medium are governed by a random process with a variance which ... | [['it', 'is', 'well', 'known', 'that', 'the', 'solutions', 'to', 'the', 'nonviscous', 'burgers', 'equation', 'develop', 'a', 'gradient', 'catastrophe', 'at', 'a', 'critical', 'time', 'provided', 'the', 'initial', 'data', 'have', 'a', 'negative', 'derivative', 'in', 'certain', 'points', 'we', 'consider', 'this', 'equati... | [-0.11395079606091199, 0.16346125873696907, -0.10870476403658319, 0.045018148120124016, -0.05490932993226401, -0.11133248046595857, 0.04413477120478493, 0.3239277008550693, -0.2918911271595529, -0.2491237636589046, 0.12126907463885428, -0.29654653998227753, -0.10977421785843622, 0.15443172594112986, -0.0337662325061348... |
708.2321 | Fast learning rates for plug-in classifiers | It has been recently shown that, under the margin (or low noise) assumption,
there exist classifiers attaining fast rates of convergence of the excess Bayes
risk, that is, rates faster than $n^{-1/2}$. The work on this subject has
suggested the following two conjectures: (i) the best achievable fast rate is
of the or... | math.ST stat.TH | it has been recently shown that under the margin or low noise assumption there exist classifiers attaining fast rates of convergence of the excess bayes risk that is rates faster than n12 the work on this subject has suggested the following two conjectures i the best achievable fast rate is of the order n1 and ii the p... | [['it', 'has', 'been', 'recently', 'shown', 'that', 'under', 'the', 'margin', 'or', 'low', 'noise', 'assumption', 'there', 'exist', 'classifiers', 'attaining', 'fast', 'rates', 'of', 'convergence', 'of', 'the', 'excess', 'bayes', 'risk', 'that', 'is', 'rates', 'faster', 'than', 'n12', 'the', 'work', 'on', 'this', 'subj... | [-0.071681232523659, 0.08228141081154994, -0.07653989134275395, 0.13462492774402643, -0.03293088396565746, -0.2221122922780721, 0.08578805006716562, 0.43773818320554236, -0.18193409800448496, -0.24994073837347652, 0.15956374488507763, -0.25130915997306935, -0.14070305431909536, 0.2652933707238054, -0.13372003143329336,... |
708.2322 | Zero | You shall not find any new physics, because all physical events are
interpreted well-known particles (leptons, quarks, photons, gluons, W-bosons,
Z-boson) and forces which have long known (electroweak, gravity, strong
interactions).
Contents: 1. Pointlike events and probability. 2. Leptons' moving equations
and mas... | physics.gen-ph | you shall not find any new physics because all physical events are interpreted wellknown particles leptons quarks photons gluons wbosons zboson and forces which have long known electroweak gravity strong interactions contents 1 pointlike events and probability 2 leptons moving equations and masses 3 fermionantifermion ... | [['you', 'shall', 'not', 'find', 'any', 'new', 'physics', 'because', 'all', 'physical', 'events', 'are', 'interpreted', 'wellknown', 'particles', 'leptons', 'quarks', 'photons', 'gluons', 'wbosons', 'zboson', 'and', 'forces', 'which', 'have', 'long', 'known', 'electroweak', 'gravity', 'strong', 'interactions', 'content... | [-0.13435190517871812, 0.41255572271651364, -0.06673358813416816, 0.28937201609205404, -0.08735773917681104, -0.2191895699443322, -0.04064642148572807, 0.2721804387237824, -0.14089077284795717, -0.41920426368555974, -0.0759507518648629, -0.37324707666543167, 0.048505193403016934, -0.018023053764588605, 0.05635524432266... |
708.2323 | Optimal Unambiguous Discrimination of Quantum States | Unambiguously distinguishing between nonorthogonal but linearly independent
quantum states is a challenging problem in quantum information processing. In
this work, an exact analytic solution to an optimum measurement problem
involving an arbitrary number of pure linearly independent quantum states is
presented. To t... | quant-ph | unambiguously distinguishing between nonorthogonal but linearly independent quantum states is a challenging problem in quantum information processing in this work an exact analytic solution to an optimum measurement problem involving an arbitrary number of pure linearly independent quantum states is presented to this e... | [['unambiguously', 'distinguishing', 'between', 'nonorthogonal', 'but', 'linearly', 'independent', 'quantum', 'states', 'is', 'a', 'challenging', 'problem', 'in', 'quantum', 'information', 'processing', 'in', 'this', 'work', 'an', 'exact', 'analytic', 'solution', 'to', 'an', 'optimum', 'measurement', 'problem', 'involv... | [-0.1124030453844055, 0.05989697707818344, -0.08086355996599036, 0.06066810954195846, -0.11739213837842856, -0.21554967850106693, 0.06032280157697165, 0.32347896582787, -0.3326553889616792, -0.2777355905430066, 0.12199234824058497, -0.2451673634830744, -0.17913844582388208, 0.20056896183698897, -0.05010311265077834, 0.... |
708.2324 | A twist in the geometry of rotating black holes: seeking the cause of
acausality | We investigate Kerr-Newman black holes in which a rotating charged
ring-shaped singularity induces a region which contains closed timelike curves
(CTCs). Contrary to popular belief, it turns out that the time orientation of
the CTC is opposite to the direction in which the singularity or the ergosphere
rotates. In th... | gr-qc physics.hist-ph | we investigate kerrnewman black holes in which a rotating charged ringshaped singularity induces a region which contains closed timelike curves ctcs contrary to popular belief it turns out that the time orientation of the ctc is opposite to the direction in which the singularity or the ergosphere rotates in this sense ... | [['we', 'investigate', 'kerrnewman', 'black', 'holes', 'in', 'which', 'a', 'rotating', 'charged', 'ringshaped', 'singularity', 'induces', 'a', 'region', 'which', 'contains', 'closed', 'timelike', 'curves', 'ctcs', 'contrary', 'to', 'popular', 'belief', 'it', 'turns', 'out', 'that', 'the', 'time', 'orientation', 'of', '... | [-0.182425760910309, 0.10093290168333624, -0.13599882376953387, 0.13817125189682253, -0.15196001742823192, -0.2130951066590989, -0.0033124847686849535, 0.33504949836060405, -0.17292611098561722, -0.20314614576189063, 0.020841594073527422, -0.29053754402243964, -0.1173069109455145, 0.18764067201006512, -0.15667272997877... |
708.2325 | A two-parameter generalization of the complete elliptic integral of
second kind | A two-parameter generalization of the complete elliptic integral of second
kind is expressed in terms of the Appell function $F_{4}$. This function is
further reduced to a quite simple bilinear form in the complete elliptic
integrals $K$ and $E$. The physical applications are briefly mentioned.
| math-ph math.MP | a twoparameter generalization of the complete elliptic integral of second kind is expressed in terms of the appell function f_4 this function is further reduced to a quite simple bilinear form in the complete elliptic integrals k and e the physical applications are briefly mentioned | [['a', 'twoparameter', 'generalization', 'of', 'the', 'complete', 'elliptic', 'integral', 'of', 'second', 'kind', 'is', 'expressed', 'in', 'terms', 'of', 'the', 'appell', 'function', 'f_4', 'this', 'function', 'is', 'further', 'reduced', 'to', 'a', 'quite', 'simple', 'bilinear', 'form', 'in', 'the', 'complete', 'ellipt... | [-0.19093422835899723, 0.04917503541542424, -0.07780542742047045, 0.10837489591342293, -0.1477221395406458, -0.06667381055239174, -0.01718416687928968, 0.2792811793378658, -0.2959483572178417, -0.2193467316735122, 0.05861317867723604, -0.25822268761694434, -0.20056602154961892, 0.25334668291939627, -0.09721785620268848... |
708.2326 | Quantum spin correlations through the superconducting-normal phase
transition in electron-doped superconducting Pr0.88LaCe0.12CuO4-d | The quantum spin fluctuations of the S = 1/2 Cu ions are important in
determining the physical properties of the high-transition temperature
(high-Tc) copper oxide superconductors, but their possible role in the electron
pairing for superconductivity remains an open question. The principal feature
of the spin fluctua... | cond-mat.supr-con cond-mat.str-el | the quantum spin fluctuations of the s 12 cu ions are important in determining the physical properties of the hightransition temperature hightc copper oxide superconductors but their possible role in the electron pairing for superconductivity remains an open question the principal feature of the spin fluctuations in op... | [['the', 'quantum', 'spin', 'fluctuations', 'of', 'the', 's', '12', 'cu', 'ions', 'are', 'important', 'in', 'determining', 'the', 'physical', 'properties', 'of', 'the', 'hightransition', 'temperature', 'hightc', 'copper', 'oxide', 'superconductors', 'but', 'their', 'possible', 'role', 'in', 'the', 'electron', 'pairing'... | [-0.20477278794837028, 0.2614000926230606, 0.00480036667060582, 0.07313467434688703, -0.02532496550526695, -0.12682355136841836, 0.08022273870672555, 0.33798034470403354, -0.2357328382051931, -0.27068821503311996, -0.009533663553767056, -0.3511222158152385, -0.10027643657233191, 0.16221468329067099, 0.05309155386061589... |
708.2327 | Non-cyclic graph of a group | We associate a graph $\Gamma_G$ to a non locally cyclic group $G$ (called the
non-cyclic graph of $G$) as follows: take $G\backslash Cyc(G)$ as vertex set,
where $Cyc(G)=\{x\in G | \left<x,y\right> \text{is cyclic for all} y\in G\}$,
and join two vertices if they do not generate a cyclic subgroup. We study the
proper... | math.GR math.CO | we associate a graph gamma_g to a non locally cyclic group g called the noncyclic graph of g as follows take gbackslash cycg as vertex set where cycgxin g leftxyright textis cyclic for all yin g and join two vertices if they do not generate a cyclic subgroup we study the properties of this graph and we establish some g... | [['we', 'associate', 'a', 'graph', 'gamma_g', 'to', 'a', 'non', 'locally', 'cyclic', 'group', 'g', 'called', 'the', 'noncyclic', 'graph', 'of', 'g', 'as', 'follows', 'take', 'gbackslash', 'cycg', 'as', 'vertex', 'set', 'where', 'cycgxin', 'g', 'leftxyright', 'textis', 'cyclic', 'for', 'all', 'yin', 'g', 'and', 'join', ... | [-0.1953188277608187, 0.18613006545053123, -0.10866349695500024, 0.01824481190139063, -0.16153544875236286, -0.16752957576914623, 0.044182322883964086, 0.44522024602773264, -0.31967656523680565, -0.214950624438718, 0.1110415399793449, -0.2852334412242065, -0.14034488718209912, 0.14667695095179334, -0.11833760858280584,... |
708.2328 | Neutrino oscillations in matter and in twisting magnetic fields | We find the solution to the Dirac equation for a massive neutrino with a
magnetic moment propagating in background matter and interacting with the
twisting magnetic field. In frames of the relativistic quantum mechanics
approach to the description of neutrino evolution we use the obtained solution
to derive neutrino ... | hep-ph hep-th | we find the solution to the dirac equation for a massive neutrino with a magnetic moment propagating in background matter and interacting with the twisting magnetic field in frames of the relativistic quantum mechanics approach to the description of neutrino evolution we use the obtained solution to derive neutrino wav... | [['we', 'find', 'the', 'solution', 'to', 'the', 'dirac', 'equation', 'for', 'a', 'massive', 'neutrino', 'with', 'a', 'magnetic', 'moment', 'propagating', 'in', 'background', 'matter', 'and', 'interacting', 'with', 'the', 'twisting', 'magnetic', 'field', 'in', 'frames', 'of', 'the', 'relativistic', 'quantum', 'mechanics... | [-0.16321996987382, 0.20604239755649925, -0.05152301248666402, 0.12938374137219572, -0.06949334017731049, -0.06837138891647998, 0.010506102763748778, 0.325698146684649, -0.21285742710696887, -0.2979393668246229, 0.026001861826296442, -0.26252882093241486, -0.10690118281195897, 0.17234573333612266, 0.07272601648809221, ... |
708.2329 | Feshbach Molecules in a One-dimensional Optical Lattice | We present the theory of a pair of atoms in a one-dimensional optical lattice
interacting via a narrow Feshbach resonance. Using a two-channel description of
the resonance, we derive analytic results for the scattering states inside the
continuum band and the discrete bound states outside the band. We identify a
Fano... | cond-mat.other quant-ph | we present the theory of a pair of atoms in a onedimensional optical lattice interacting via a narrow feshbach resonance using a twochannel description of the resonance we derive analytic results for the scattering states inside the continuum band and the discrete bound states outside the band we identify a fano resona... | [['we', 'present', 'the', 'theory', 'of', 'a', 'pair', 'of', 'atoms', 'in', 'a', 'onedimensional', 'optical', 'lattice', 'interacting', 'via', 'a', 'narrow', 'feshbach', 'resonance', 'using', 'a', 'twochannel', 'description', 'of', 'the', 'resonance', 'we', 'derive', 'analytic', 'results', 'for', 'the', 'scattering', '... | [-0.1306888297209904, 0.13460415447131405, -0.08116956302546896, 0.07651436954620294, -0.015226867023253968, -0.09696106113066587, 0.11383983129174642, 0.3904575567576103, -0.24410594154081386, -0.2384264254809144, 0.039710354484365475, -0.24528097212896682, -0.13965872830885928, 0.15770725172721237, 0.0589155597263015... |
708.233 | Light dressed-excitons in an incoherent-electron sea: Evidence for
Mollow-triplet and Autler-Townes doublet | We demonstrate that the interaction between excitons and a sea of incoherent
electrons does not preclude excitons dressing by light. We investigate the role
of exciton-electron scattering in the light dressing by measuring the dynamical
absorption spectrum of a modulation-doped CdTe quantum well, which shows a
clear ... | cond-mat.mtrl-sci | we demonstrate that the interaction between excitons and a sea of incoherent electrons does not preclude excitons dressing by light we investigate the role of excitonelectron scattering in the light dressing by measuring the dynamical absorption spectrum of a modulationdoped cdte quantum well which shows a clear eviden... | [['we', 'demonstrate', 'that', 'the', 'interaction', 'between', 'excitons', 'and', 'a', 'sea', 'of', 'incoherent', 'electrons', 'does', 'not', 'preclude', 'excitons', 'dressing', 'by', 'light', 'we', 'investigate', 'the', 'role', 'of', 'excitonelectron', 'scattering', 'in', 'the', 'light', 'dressing', 'by', 'measuring'... | [-0.15530809281127794, 0.2511098282031563, -0.037344727997801135, 0.11533229424599178, 0.011491089157507118, -0.15826466574205314, 0.091067888529268, 0.41822321161779824, -0.218628387491644, -0.2701477568806862, -0.0887586465069777, -0.2991935307521145, -0.1549286856411063, 0.14443162750756863, 0.07521882351506881, -0.... |
708.2331 | The Boron Buckyball has an Unexpected Th Symmetry | The boron buckyball avoids the high symmetry icosahedral cage structure. The
previously reported Ih symmetric structure is not an energy minimum in the
potential energy surface and exhibits a spontaneous symmetry breaking to yield
a puckered cage with a rare Th symmetry. The HOMO-LUMO gap is twice as large as
the rep... | cond-mat.other | the boron buckyball avoids the high symmetry icosahedral cage structure the previously reported ih symmetric structure is not an energy minimum in the potential energy surface and exhibits a spontaneous symmetry breaking to yield a puckered cage with a rare th symmetry the homolumo gap is twice as large as the reported... | [['the', 'boron', 'buckyball', 'avoids', 'the', 'high', 'symmetry', 'icosahedral', 'cage', 'structure', 'the', 'previously', 'reported', 'ih', 'symmetric', 'structure', 'is', 'not', 'an', 'energy', 'minimum', 'in', 'the', 'potential', 'energy', 'surface', 'and', 'exhibits', 'a', 'spontaneous', 'symmetry', 'breaking', '... | [-0.13099440088036, 0.160925223102208, -0.00889461253189131, 0.04866003532827433, -0.04648462770047126, -0.1094889209315471, 0.09438486200116285, 0.39476470287296583, -0.28546086449611496, -0.34625981000627015, 0.027967889064487505, -0.3383348896228648, -0.0786644644497035, 0.0356777075545064, 0.036807674672696494, -0.... |
708.2332 | Metastable state involved resonant tunneling through single InAs/GaAs
quantum dot | A scheme of resonant tunneling through the metastable state of semiconductor
quantum dot is presented and implemented in the transport study of freestanding
InAs quantum dots grown on GaAs(001) under illumination using conductive atomic
force microscopy. The metastable state is achieved by capturing one
photoexcited ... | quant-ph | a scheme of resonant tunneling through the metastable state of semiconductor quantum dot is presented and implemented in the transport study of freestanding inas quantum dots grown on gaas001 under illumination using conductive atomic force microscopy the metastable state is achieved by capturing one photoexcited fermi... | [['a', 'scheme', 'of', 'resonant', 'tunneling', 'through', 'the', 'metastable', 'state', 'of', 'semiconductor', 'quantum', 'dot', 'is', 'presented', 'and', 'implemented', 'in', 'the', 'transport', 'study', 'of', 'freestanding', 'inas', 'quantum', 'dots', 'grown', 'on', 'gaas001', 'under', 'illumination', 'using', 'cond... | [-0.14957111119934968, 0.2072628146519178, -0.03070736476862482, -0.010558219787921628, 0.09784873605802141, -0.24286721023120758, 0.09629815124770112, 0.38508389232487517, -0.25927413030816565, -0.3206289024766663, -0.030921511509423627, -0.3209691022876008, -0.048915370104127914, 0.24978866443391248, 0.01606963693870... |
708.2333 | The coherent {\it d}-wave superconducting gap in underdoped
La$_{2-x}$Sr$_{x}$CuO$_4$ as studied by angle-resolved photoemission | We present angle-resolved photoemission spectroscopy (ARPES) data on
moderately underdoped La$_{1.855}$Sr$_{0.145}$CuO$_4$ at temperatures below and
above the superconducting transition temperature. Unlike previous studies of
this material, we observe sharp spectral peaks along the entire underlying
Fermi surface in ... | cond-mat.supr-con cond-mat.str-el | we present angleresolved photoemission spectroscopy arpes data on moderately underdoped la_1855sr_0145cuo_4 at temperatures below and above the superconducting transition temperature unlike previous studies of this material we observe sharp spectral peaks along the entire underlying fermi surface in the superconducting... | [['we', 'present', 'angleresolved', 'photoemission', 'spectroscopy', 'arpes', 'data', 'on', 'moderately', 'underdoped', 'la_1855sr_0145cuo_4', 'at', 'temperatures', 'below', 'and', 'above', 'the', 'superconducting', 'transition', 'temperature', 'unlike', 'previous', 'studies', 'of', 'this', 'material', 'we', 'observe',... | [-0.1306242843240034, 0.18796963301152572, -0.07308608840452507, 0.059161335941171275, -0.047988047579419796, -0.14403134764637798, 0.1763538016937673, 0.43226287527941165, -0.21058029625564814, -0.3312078483588994, -0.01993967815884389, -0.39970050636678933, -0.04490666676312685, 0.21815600144676864, 0.033839050922542... |
708.2334 | Collective transport in the insulating state of Josephson junction
arrays | We investigate collective Cooper-pair transport of one- and two-dimensional
Josephson junction arrays in the insulating state. We derive an analytical
expression for the current-voltage characteristic revealing thermally activated
conductivity at small voltages and threshold voltage depinning. The activation
energy a... | cond-mat.supr-con cond-mat.mes-hall | we investigate collective cooperpair transport of one and twodimensional josephson junction arrays in the insulating state we derive an analytical expression for the currentvoltage characteristic revealing thermally activated conductivity at small voltages and threshold voltage depinning the activation energy and the r... | [['we', 'investigate', 'collective', 'cooperpair', 'transport', 'of', 'one', 'and', 'twodimensional', 'josephson', 'junction', 'arrays', 'in', 'the', 'insulating', 'state', 'we', 'derive', 'an', 'analytical', 'expression', 'for', 'the', 'currentvoltage', 'characteristic', 'revealing', 'thermally', 'activated', 'conduct... | [-0.20010894493677092, 0.16533853797242526, -0.034841486096982496, 0.03964410318169466, -0.009078276305159262, -0.15371038742201817, 0.09227861660678895, 0.37780932281628127, -0.27217593394827927, -0.2804499190216037, 0.0015125723290141703, -0.2791033509333641, -0.15796974927287025, 0.20615459663393207, 0.0403079313941... |
708.2335 | 2D shift of the centre of gravity of the light beam carrying orbital
angular momentum, which accompanies reflection from a lossy medium | It is shown that after reflection from a lossy medium the $s$- or
$p$-polarized paraxial light beam carrying the orbital angular momentum suffers
the 2D shift of the beam's centre of gravity relative the geometric optic axis.
The mutually orthogonal components of this shift are expressed through the real
and imaginar... | physics.optics | it is shown that after reflection from a lossy medium the s or ppolarized paraxial light beam carrying the orbital angular momentum suffers the 2d shift of the beams centre of gravity relative the geometric optic axis the mutually orthogonal components of this shift are expressed through the real and imaginary parts of... | [['it', 'is', 'shown', 'that', 'after', 'reflection', 'from', 'a', 'lossy', 'medium', 'the', 's', 'or', 'ppolarized', 'paraxial', 'light', 'beam', 'carrying', 'the', 'orbital', 'angular', 'momentum', 'suffers', 'the', '2d', 'shift', 'of', 'the', 'beams', 'centre', 'of', 'gravity', 'relative', 'the', 'geometric', 'optic... | [-0.21303202711767855, 0.17543575002987316, -0.08120155102316884, -0.022239003733704812, -0.0873178380905934, -0.1053792805566142, -0.030939633242677952, 0.4006754946557508, -0.31168833075334196, -0.20076165467068768, 0.04395077308720868, -0.28771117550955305, -0.10521719389784055, 0.17242442067726044, -0.0179130909154... |
708.2336 | Unsatisfiable Linear k-CNFs Exist, for every k | We call a CNF formula linear if any two clauses have at most one variable in
common. Let Linear k-SAT be the problem of deciding whether a given linear
k-CNF formula is satisfiable. Here, a k-CNF formula is a CNF formula in which
every clause has size exactly k. It was known that for k >= 3, Linear k-SAT is
NP-comple... | cs.DM cs.CC cs.LO | we call a cnf formula linear if any two clauses have at most one variable in common let linear ksat be the problem of deciding whether a given linear kcnf formula is satisfiable here a kcnf formula is a cnf formula in which every clause has size exactly k it was known that for k 3 linear ksat is npcomplete if and only ... | [['we', 'call', 'a', 'cnf', 'formula', 'linear', 'if', 'any', 'two', 'clauses', 'have', 'at', 'most', 'one', 'variable', 'in', 'common', 'let', 'linear', 'ksat', 'be', 'the', 'problem', 'of', 'deciding', 'whether', 'a', 'given', 'linear', 'kcnf', 'formula', 'is', 'satisfiable', 'here', 'a', 'kcnf', 'formula', 'is', 'a'... | [-0.13443961034485158, 0.1614336571611242, -0.055016274743669685, 0.11329793421576587, -0.19521293549129626, -0.28512472843426284, 0.12226225720130957, 0.3287623104773737, -0.2616270207932794, -0.2906996448268026, 0.0860026994659159, -0.2965882194678505, -0.12844900628114306, 0.2317358297420878, -0.09451696402758544, 0... |
708.2337 | Evolution of the bursting-layer wave during a Type 1 X-ray burst | In a popular scenario due to Heyl, quasi periodic oscillations (QPOs) which
are seen during type 1 X-ray bursts are produced by giant travelling waves in
neutron-star oceans. Piro and Bildsten have proposed that during the burst
cooling the wave in the bursting layer may convert into a deep crustal
interface wave, wh... | astro-ph | in a popular scenario due to heyl quasi periodic oscillations qpos which are seen during type 1 xray bursts are produced by giant travelling waves in neutronstar oceans piro and bildsten have proposed that during the burst cooling the wave in the bursting layer may convert into a deep crustal interface wave which would... | [['in', 'a', 'popular', 'scenario', 'due', 'to', 'heyl', 'quasi', 'periodic', 'oscillations', 'qpos', 'which', 'are', 'seen', 'during', 'type', '1', 'xray', 'bursts', 'are', 'produced', 'by', 'giant', 'travelling', 'waves', 'in', 'neutronstar', 'oceans', 'piro', 'and', 'bildsten', 'have', 'proposed', 'that', 'during', ... | [-0.158440822389509, 0.2188065041455307, -0.06695339400820167, 0.12723146586462722, -0.11759219362367211, -0.091244003862708, 0.07304575898867499, 0.35508137812971, -0.2383786573141281, -0.2918999671337328, 0.10721223160674397, -0.2594665353984705, -0.10210569827218673, 0.2173515705491549, -0.0029404890025034546, -0.01... |
708.2338 | Magnetic Phase Diagram of Spin-1/2 Two-Leg Ladder with Four-Spin Ring
Exchange | We study the spin-1/2 two-leg Heisenberg ladder with four-spin ring exchanges
under a magnetic field. We introduce an exact duality transformation which is
an extension of the spin-chirality duality developed previously and yields a
new self-dual surface in the parameter space. We then determine the magnetic
phase di... | cond-mat.str-el | we study the spin12 twoleg heisenberg ladder with fourspin ring exchanges under a magnetic field we introduce an exact duality transformation which is an extension of the spinchirality duality developed previously and yields a new selfdual surface in the parameter space we then determine the magnetic phase diagram usin... | [['we', 'study', 'the', 'spin12', 'twoleg', 'heisenberg', 'ladder', 'with', 'fourspin', 'ring', 'exchanges', 'under', 'a', 'magnetic', 'field', 'we', 'introduce', 'an', 'exact', 'duality', 'transformation', 'which', 'is', 'an', 'extension', 'of', 'the', 'spinchirality', 'duality', 'developed', 'previously', 'and', 'yie... | [-0.22584863833956492, 0.18627421543690448, -0.08623581372733241, 0.0717651719313332, -0.06665594342562542, -0.13469277292905937, 0.02988356579709979, 0.35027747518084584, -0.25935207381482844, -0.2227615835122511, 0.036021714808545935, -0.277590863451868, -0.1560877962580439, 0.1406009683692918, 0.09366450675885256, -... |
708.2339 | A pentaquark picture of Lambda(1405) | We test a pentaquark model of the negative parity hyperon Lambda(1405). We
use a model where valence four quarks and one antiquark move in a potential
relativistically and interact with each other and themselves through gluon and
NG boson. Fall-apart decay rate of the system is studied and strong model
dependence is ... | hep-ph | we test a pentaquark model of the negative parity hyperon lambda1405 we use a model where valence four quarks and one antiquark move in a potential relativistically and interact with each other and themselves through gluon and ng boson fallapart decay rate of the system is studied and strong model dependence is pointed... | [['we', 'test', 'a', 'pentaquark', 'model', 'of', 'the', 'negative', 'parity', 'hyperon', 'lambda1405', 'we', 'use', 'a', 'model', 'where', 'valence', 'four', 'quarks', 'and', 'one', 'antiquark', 'move', 'in', 'a', 'potential', 'relativistically', 'and', 'interact', 'with', 'each', 'other', 'and', 'themselves', 'throug... | [-0.08062366820457909, 0.2635316586604825, -0.11567178271124484, 0.14817245479207486, -0.08616868228030701, -0.2314337553128738, 0.11677029616785822, 0.3808502492805322, -0.18590411385176359, -0.2113885342798851, -0.066672075839489, -0.34618036411012765, -0.03298916981590015, 0.04096481524390617, 0.14178468283541776, 0... |
708.234 | Bayesian Galaxy Shape Measurement for Weak Lensing Surveys -I.
Methodology and a Fast Fitting Algorithm | The principles of measuring the shapes of galaxies by a model-fitting
approach are discussed in the context of shape-measurement for surveys of weak
gravitational lensing. It is argued that such an approach should be optimal,
allowing measurement with maximal signal-to-noise, coupled with estimation of
measurement er... | astro-ph | the principles of measuring the shapes of galaxies by a modelfitting approach are discussed in the context of shapemeasurement for surveys of weak gravitational lensing it is argued that such an approach should be optimal allowing measurement with maximal signaltonoise coupled with estimation of measurement errors the ... | [['the', 'principles', 'of', 'measuring', 'the', 'shapes', 'of', 'galaxies', 'by', 'a', 'modelfitting', 'approach', 'are', 'discussed', 'in', 'the', 'context', 'of', 'shapemeasurement', 'for', 'surveys', 'of', 'weak', 'gravitational', 'lensing', 'it', 'is', 'argued', 'that', 'such', 'an', 'approach', 'should', 'be', 'o... | [-0.06739072613809116, 0.031238523432216253, -0.1212149650100192, 0.07260843671870586, -0.0734609644149096, -0.11893851661215757, 0.023117282449175384, 0.4187596416214609, -0.2321070922922542, -0.3553144396389373, 0.12083653155500994, -0.22402891699395333, -0.1089760214285854, 0.25239723408061526, -0.05817622195850197,... |
708.2341 | Unimodality of ordinary multinomials and maximal probabilities of
convolution powers of discrete uniform distribution | We establish the unimodality and the asymptotic strong unimodality of the
ordinary multinomials and give their smallest mode leading to the expression of
the maximal probability of convolution powers of the discrete uniform
distribution. We conclude giving the generating functions of the sequence of
generalized ordin... | math.PR math.CO | we establish the unimodality and the asymptotic strong unimodality of the ordinary multinomials and give their smallest mode leading to the expression of the maximal probability of convolution powers of the discrete uniform distribution we conclude giving the generating functions of the sequence of generalized ordinary... | [['we', 'establish', 'the', 'unimodality', 'and', 'the', 'asymptotic', 'strong', 'unimodality', 'of', 'the', 'ordinary', 'multinomials', 'and', 'give', 'their', 'smallest', 'mode', 'leading', 'to', 'the', 'expression', 'of', 'the', 'maximal', 'probability', 'of', 'convolution', 'powers', 'of', 'the', 'discrete', 'unifo... | [-0.13885436247801408, 0.07368511543086242, -0.11200541545986198, 0.10796448541805148, -0.06226671137847006, -0.043609925371129066, 0.053833438349101925, 0.2977421309624333, -0.31752806760778185, -0.2377741608870565, 0.08374624798307195, -0.2337512024823809, -0.11793006939115003, 0.1624785638123285, -0.0486441890207061... |
708.2342 | Complex dynamics in a nerve fiber model with periodic coefficients | We deal with the periodic boundary value problem for a second-order nonlinear
ODE which includes the case of the Nagumo type equation $v_{xx} - g v + n(x)
F(v) = 0,$ previously considered by Grindrod and Sleeman and by Chen and Bell
in the study of nerve fiber models. In some recent works we discussed the case
of non... | math.DS | we deal with the periodic boundary value problem for a secondorder nonlinear ode which includes the case of the nagumo type equation v_xx g v nx fv 0 previously considered by grindrod and sleeman and by chen and bell in the study of nerve fiber models in some recent works we discussed the case of nonexistence of nontri... | [['we', 'deal', 'with', 'the', 'periodic', 'boundary', 'value', 'problem', 'for', 'a', 'secondorder', 'nonlinear', 'ode', 'which', 'includes', 'the', 'case', 'of', 'the', 'nagumo', 'type', 'equation', 'v_xx', 'g', 'v', 'nx', 'fv', '0', 'previously', 'considered', 'by', 'grindrod', 'and', 'sleeman', 'and', 'by', 'chen',... | [-0.14897273811776707, 0.08494319714514947, -0.026319213431116525, 0.05058510652913644, -0.06004434739943684, -0.16513957247153166, 0.005879620311600043, 0.3054087988547678, -0.28151388652782416, -0.24549775093612147, 0.139339142589739, -0.28441727614953993, -0.20819175438349688, 0.19821163278822673, -0.080638703598633... |
708.2343 | The quantum Chernoff bound as a measure of distinguishability between
density matrices: application to qubit and Gaussian states | Hypothesis testing is a fundamental issue in statistical inference and has
been a crucial element in the development of information sciences. The Chernoff
bound gives the minimal Bayesian error probability when discriminating two
hypotheses given a large number of observations. Recently the combined work of
Audenaert... | quant-ph | hypothesis testing is a fundamental issue in statistical inference and has been a crucial element in the development of information sciences the chernoff bound gives the minimal bayesian error probability when discriminating two hypotheses given a large number of observations recently the combined work of audenaert et ... | [['hypothesis', 'testing', 'is', 'a', 'fundamental', 'issue', 'in', 'statistical', 'inference', 'and', 'has', 'been', 'a', 'crucial', 'element', 'in', 'the', 'development', 'of', 'information', 'sciences', 'the', 'chernoff', 'bound', 'gives', 'the', 'minimal', 'bayesian', 'error', 'probability', 'when', 'discriminating... | [-0.10081523526592978, 0.11017296116599547, -0.09965114419082446, 0.06564970332197845, -0.02119948521522539, -0.14209638003259897, 0.08260563079932971, 0.3065619835889499, -0.20415620772966317, -0.30013324573369965, 0.06284364125026123, -0.2601255331135222, -0.15561720779963903, 0.19274675774787153, -0.127677135001868,... |
708.2344 | Developments and the preliminary tests of Resistive GEMs manufactured by
a screen printing technology | We report promising initial results obtained with new resistive-electrode GEM
(RETGEM) detectors manufactured, for the first time, using screen printing
technology. These new detectors allow one to reach gas gains nearly as high as
with ordinary GEM-like detectors with metallic electrodes; however, due to the
high re... | physics.ins-det | we report promising initial results obtained with new resistiveelectrode gem retgem detectors manufactured for the first time using screen printing technology these new detectors allow one to reach gas gains nearly as high as with ordinary gemlike detectors with metallic electrodes however due to the high resistivity o... | [['we', 'report', 'promising', 'initial', 'results', 'obtained', 'with', 'new', 'resistiveelectrode', 'gem', 'retgem', 'detectors', 'manufactured', 'for', 'the', 'first', 'time', 'using', 'screen', 'printing', 'technology', 'these', 'new', 'detectors', 'allow', 'one', 'to', 'reach', 'gas', 'gains', 'nearly', 'as', 'hig... | [-0.04632200328557416, 0.1525068846710313, -0.030694087859816276, -0.022603787777300637, -0.03872707316558257, -0.22044731011426838, 0.0048174128410290685, 0.40386163077410864, -0.2232900587621437, -0.3448632843131144, 0.11433735391753312, -0.3270838297931092, -0.08090865407717696, 0.26674403054997897, -0.0706027352344... |
708.2345 | Onsager-Machlup theory and work fluctuation theorem for a harmonically
driven Brownian particle | We extend Tooru-Cohen analysis for nonequilirium steady state(NSS) of a
Brownian particle to nonequilibrium oscillatory state (NOS) of Brownian
particle by considering time dependent external drive protocol. We consider an
unbounded charged Brownian particle in the presence of an oscillating electric
field and prove ... | cond-mat.stat-mech | we extend toorucohen analysis for nonequilirium steady statenss of a brownian particle to nonequilibrium oscillatory state nos of brownian particle by considering time dependent external drive protocol we consider an unbounded charged brownian particle in the presence of an oscillating electric field and prove work flu... | [['we', 'extend', 'toorucohen', 'analysis', 'for', 'nonequilirium', 'steady', 'statenss', 'of', 'a', 'brownian', 'particle', 'to', 'nonequilibrium', 'oscillatory', 'state', 'nos', 'of', 'brownian', 'particle', 'by', 'considering', 'time', 'dependent', 'external', 'drive', 'protocol', 'we', 'consider', 'an', 'unbounded'... | [-0.12295152652654302, 0.211697127857808, -0.11171290441004114, 0.06127147474820701, -0.017561142872689308, -0.14683537360742294, 0.03556285521831462, 0.31889513847047246, -0.25070818804155015, -0.2779969108183827, 0.051423206449428625, -0.2357426614591242, -0.07037494440389945, 0.19624213124749013, -0.0358670415661701... |
708.2346 | Apparent density fluctuations in N-constant ensemble simulations | In computer simulations performed in constant number of particles ensembles,
although the total number of particles N contained in the simulation box does
not fluctuate, hence giving a zero apparent compressibility, there are still
local fluctuations in the number of particles. It is shown herein that these
apparent ... | physics.chem-ph physics.comp-ph | in computer simulations performed in constant number of particles ensembles although the total number of particles n contained in the simulation box does not fluctuate hence giving a zero apparent compressibility there are still local fluctuations in the number of particles it is shown herein that these apparent fluctu... | [['in', 'computer', 'simulations', 'performed', 'in', 'constant', 'number', 'of', 'particles', 'ensembles', 'although', 'the', 'total', 'number', 'of', 'particles', 'n', 'contained', 'in', 'the', 'simulation', 'box', 'does', 'not', 'fluctuate', 'hence', 'giving', 'a', 'zero', 'apparent', 'compressibility', 'there', 'ar... | [-0.12212764951933758, 0.171131805947321, -0.08969233912811224, 0.055243199962378586, 0.025904112155991477, -0.06739531319806945, 0.01663267350880502, 0.32852643568006307, -0.24673384023237163, -0.3251933962335633, 0.06381282438563089, -0.2647602194555978, -0.07842950263534094, 0.19081366520281362, 0.001446567613673110... |
708.2347 | Sums of products of generalized Fibonacci and Lucas numbers | In this paper, we establish several formulae for sums and alternating sums of
products of generalized Fibonacci and Lucas numbers. In particular, we recover
and extend all results of Z. Cerin and Z. Cerin & G. M. Gianella, more easily.
| math.NT math.CO | in this paper we establish several formulae for sums and alternating sums of products of generalized fibonacci and lucas numbers in particular we recover and extend all results of z cerin and z cerin g m gianella more easily | [['in', 'this', 'paper', 'we', 'establish', 'several', 'formulae', 'for', 'sums', 'and', 'alternating', 'sums', 'of', 'products', 'of', 'generalized', 'fibonacci', 'and', 'lucas', 'numbers', 'in', 'particular', 'we', 'recover', 'and', 'extend', 'all', 'results', 'of', 'z', 'cerin', 'and', 'z', 'cerin', 'g', 'm', 'giane... | [-0.17342963060299452, 0.12890531375342107, -0.0443354286512153, 0.09117149536743657, -0.051786668145925634, -0.11040880386200216, 0.09144185336319627, 0.35824652875049245, -0.28717408587949145, -0.26658534651829136, 0.1095730675668973, -0.2563483306568944, -0.18567836693384582, 0.24658451652956298, -0.0564346746541559... |
708.2348 | Properties of voids in the Local Volume | Current explanation of the overabundance of dark matter subhalos in the Local
Group (LG) indicates that there maybe a limit on mass of a halo, which can host
a galaxy. This idea can be tested using voids in the distribution of galaxies:
at some level small voids should not contain any (even dwarf) galaxies. We use
ob... | astro-ph | current explanation of the overabundance of dark matter subhalos in the local group lg indicates that there maybe a limit on mass of a halo which can host a galaxy this idea can be tested using voids in the distribution of galaxies at some level small voids should not contain any even dwarf galaxies we use observationa... | [['current', 'explanation', 'of', 'the', 'overabundance', 'of', 'dark', 'matter', 'subhalos', 'in', 'the', 'local', 'group', 'lg', 'indicates', 'that', 'there', 'maybe', 'a', 'limit', 'on', 'mass', 'of', 'a', 'halo', 'which', 'can', 'host', 'a', 'galaxy', 'this', 'idea', 'can', 'be', 'tested', 'using', 'voids', 'in', '... | [-0.08372819261968284, 0.10922045671191086, -0.1026805460381215, 0.12171825478015588, -0.10956998640064392, -0.04690195025357218, 0.01869950506173593, 0.392427568288001, -0.14556937668917339, -0.4011574722293635, 0.04088008331554242, -0.3120736611279571, -0.013495160169454653, 0.14556924797900356, 0.002830533581827559,... |
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