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710.1253 | The forgetful map in rational K-theory | Let G be a connected reductive algebraic group acting on a scheme X. Let R(G)
denote the representation ring of G, and let I be the ideal in R(G) of virtual
representations of rank 0. Let G(X) (resp. G(G,X)) denote the Grothendieck
group of coherent sheaves (resp. G-equivariant coherent sheaves) on X.
Merkurjev prove... | math.AG math.KT | let g be a connected reductive algebraic group acting on a scheme x let rg denote the representation ring of g and let i be the ideal in rg of virtual representations of rank 0 let gx resp ggx denote the grothendieck group of coherent sheaves resp gequivariant coherent sheaves on x merkurjev proved that if the fundamen... | [['let', 'g', 'be', 'a', 'connected', 'reductive', 'algebraic', 'group', 'acting', 'on', 'a', 'scheme', 'x', 'let', 'rg', 'denote', 'the', 'representation', 'ring', 'of', 'g', 'and', 'let', 'i', 'be', 'the', 'ideal', 'in', 'rg', 'of', 'virtual', 'representations', 'of', 'rank', '0', 'let', 'gx', 'resp', 'ggx', 'denote'... | [-0.24998286123983227, 0.09770190719919393, -0.1578674763650843, -0.05334979165156649, -0.13586060421306406, -0.16437955493493392, -0.01334624547880512, 0.3686035662755236, -0.42406392686471744, -0.17547356987556628, 0.07078536158020667, -0.23991981371062565, -0.09853231475629785, 0.19363720284623875, -0.15732055129315... |
710.1254 | A Group Theoretic Model for Information | In this paper we formalize the notions of information elements and
information lattices, first proposed by Shannon. Exploiting this formalization,
we identify a comprehensive parallelism between information lattices and
subgroup lattices. Qualitatively, we demonstrate isomorphisms between
information lattices and sub... | cs.IT math.IT | in this paper we formalize the notions of information elements and information lattices first proposed by shannon exploiting this formalization we identify a comprehensive parallelism between information lattices and subgroup lattices qualitatively we demonstrate isomorphisms between information lattices and subgroup l... | [['in', 'this', 'paper', 'we', 'formalize', 'the', 'notions', 'of', 'information', 'elements', 'and', 'information', 'lattices', 'first', 'proposed', 'by', 'shannon', 'exploiting', 'this', 'formalization', 'we', 'identify', 'a', 'comprehensive', 'parallelism', 'between', 'information', 'lattices', 'and', 'subgroup', 'l... | [-0.118542175076374, 0.04712635901072411, -0.14974968582341935, 0.11381058001524724, -0.09606566373507845, -0.13199431262412334, 0.11464117644454308, 0.37168016396263703, -0.3250312379755598, -0.2666874543121234, 0.07083959387519452, -0.2795012582611432, -0.20056066735782088, 0.1553557296809591, -0.09815872751455255, -... |
710.1255 | Spatial distribution of stars and brown dwarfs in sigma Orionis | I have re-visited the spatial distribution of stars and high-mass brown
dwarfs in the sigma Orionis cluster (~3 Ma, ~360 pc). The input was a catalogue
of 340 cluster members and candidates at separations less than 30 arcmin to
sigma Ori AB. Of them, 70 % have features of extreme youth. I fitted the
normalised cumula... | astro-ph | i have revisited the spatial distribution of stars and highmass brown dwarfs in the sigma orionis cluster 3 ma 360 pc the input was a catalogue of 340 cluster members and candidates at separations less than 30 arcmin to sigma ori ab of them 70 have features of extreme youth i fitted the normalised cumulative number of ... | [['i', 'have', 'revisited', 'the', 'spatial', 'distribution', 'of', 'stars', 'and', 'highmass', 'brown', 'dwarfs', 'in', 'the', 'sigma', 'orionis', 'cluster', '3', 'ma', '360', 'pc', 'the', 'input', 'was', 'a', 'catalogue', 'of', '340', 'cluster', 'members', 'and', 'candidates', 'at', 'separations', 'less', 'than', '30... | [-0.060472274915144966, 0.10835406168314543, -0.11506898742249255, 0.07879615191655655, -0.08284461296348762, -0.07767725222423592, 0.05555789996819791, 0.38145334745246556, -0.1594780064513406, -0.36631466958781966, 0.029472796119979872, -0.30602705585945555, 0.00804778552233612, 0.12968024092548658, -0.01973500871597... |
710.1256 | Complexified Path Integrals and the Phases of Quantum Field Theory | The path integral by which quantum field theories are defined is a particular
solution of a set of functional differential equations arising from the
Schwinger action principle. In fact these equations have a multitude of
additional solutions which are described by integrals over a complexified path.
We discuss prope... | hep-th | the path integral by which quantum field theories are defined is a particular solution of a set of functional differential equations arising from the schwinger action principle in fact these equations have a multitude of additional solutions which are described by integrals over a complexified path we discuss propertie... | [['the', 'path', 'integral', 'by', 'which', 'quantum', 'field', 'theories', 'are', 'defined', 'is', 'a', 'particular', 'solution', 'of', 'a', 'set', 'of', 'functional', 'differential', 'equations', 'arising', 'from', 'the', 'schwinger', 'action', 'principle', 'in', 'fact', 'these', 'equations', 'have', 'a', 'multitude'... | [-0.17777169703643908, 0.10990515882987037, -0.10102168945644899, 0.06373559787903947, -0.07988244347229954, -0.07787285883363987, 0.039194147982117206, 0.2828165082674887, -0.24754997695397055, -0.24061808733653928, 0.10110093356496974, -0.2699774553463117, -0.1656663022176535, 0.1841591254120604, -0.04160329736843114... |
710.1257 | Gauge-Dependence of Green's Functions in QCD and QED | When all Green's functions are known in a given gauge we may raise a question
of whether it is possible or not to derive the corresponding ones in a
different gauge. The answer is negative in QCD but affirmative in QED provided
that we confine ourselves to the covariant gauge characterized by a gauge
parameter $\alph... | hep-th | when all greens functions are known in a given gauge we may raise a question of whether it is possible or not to derive the corresponding ones in a different gauge the answer is negative in qcd but affirmative in qed provided that we confine ourselves to the covariant gauge characterized by a gauge parameter alpha we s... | [['when', 'all', 'greens', 'functions', 'are', 'known', 'in', 'a', 'given', 'gauge', 'we', 'may', 'raise', 'a', 'question', 'of', 'whether', 'it', 'is', 'possible', 'or', 'not', 'to', 'derive', 'the', 'corresponding', 'ones', 'in', 'a', 'different', 'gauge', 'the', 'answer', 'is', 'negative', 'in', 'qcd', 'but', 'affir... | [-0.13423231625839924, 0.19573996712346203, -0.06488010198451005, 0.14600732411222103, -0.11686746490975986, -0.15607121124003942, 0.057905712920742536, 0.3911579340696335, -0.18895473525716136, -0.25694964150181754, 0.04811481117772368, -0.2399193036871461, -0.15458418731577694, 0.12283638154084865, -0.067417798291605... |
710.1258 | Minimization of convex functionals over frame operators | We present results about minimization of convex functionals defined over a
finite set of vectors in a finite dimensional Hilbert space, that extend
several known results for the Benedetto-Fickus frame potential. Our approach
depends on majorization techniques. We also consider some perturbation
problems, where a posi... | math.FA | we present results about minimization of convex functionals defined over a finite set of vectors in a finite dimensional hilbert space that extend several known results for the benedettofickus frame potential our approach depends on majorization techniques we also consider some perturbation problems where a positive pe... | [['we', 'present', 'results', 'about', 'minimization', 'of', 'convex', 'functionals', 'defined', 'over', 'a', 'finite', 'set', 'of', 'vectors', 'in', 'a', 'finite', 'dimensional', 'hilbert', 'space', 'that', 'extend', 'several', 'known', 'results', 'for', 'the', 'benedettofickus', 'frame', 'potential', 'our', 'approach... | [-0.13050418967582486, 0.05775267997051816, -0.07489653651026783, 0.05171385421291799, -0.04783350423708357, -0.08370973960405241, 0.047535486871729024, 0.33331546408904567, -0.30626840766116575, -0.17387795221765298, 0.1207438518302641, -0.2795882853175941, -0.14397824067320372, 0.20188482415333792, -0.088651051329499... |
710.1259 | Calculation of surface tension via area sampling | We examine the performance of several molecular simulation techniques aimed
at evaluation of the surface tension through its thermodynamic definition. For
all methods explored, the surface tension is calculated by approximating the
change in Helmholtz free energy associated with a change in interfacial area
through s... | cond-mat.stat-mech cond-mat.soft | we examine the performance of several molecular simulation techniques aimed at evaluation of the surface tension through its thermodynamic definition for all methods explored the surface tension is calculated by approximating the change in helmholtz free energy associated with a change in interfacial area through simul... | [['we', 'examine', 'the', 'performance', 'of', 'several', 'molecular', 'simulation', 'techniques', 'aimed', 'at', 'evaluation', 'of', 'the', 'surface', 'tension', 'through', 'its', 'thermodynamic', 'definition', 'for', 'all', 'methods', 'explored', 'the', 'surface', 'tension', 'is', 'calculated', 'by', 'approximating',... | [-0.055004395400243024, 0.0942255365608632, -0.08132592872246633, 0.04069630784955333, 0.012830690295293422, -0.1365249608273389, 0.055986899395189166, 0.356381484003485, -0.20763427567849788, -0.3403944129270296, 0.06001279870505934, -0.25594116224891555, -0.1256862114019834, 0.22282750122160336, -0.04396263986798319,... |
710.126 | Three loop MSbar renormalization of QED in the 't~Hooft-Veltman gauge | Quantum electrodynamics (QED) fixed in the 't~Hooft-Veltman gauge is
renormalized to three loops in the MSbar scheme. The beta-functions and
anomalous dimensions are computed as functions of the usual QED coupling and
the additional coupling, xi, which is introduced as part of the nonlinear gauge
fixing condition. Si... | hep-th | quantum electrodynamics qed fixed in the thooftveltman gauge is renormalized to three loops in the msbar scheme the betafunctions and anomalous dimensions are computed as functions of the usual qed coupling and the additional coupling xi which is introduced as part of the nonlinear gauge fixing condition similar to the... | [['quantum', 'electrodynamics', 'qed', 'fixed', 'in', 'the', 'thooftveltman', 'gauge', 'is', 'renormalized', 'to', 'three', 'loops', 'in', 'the', 'msbar', 'scheme', 'the', 'betafunctions', 'and', 'anomalous', 'dimensions', 'are', 'computed', 'as', 'functions', 'of', 'the', 'usual', 'qed', 'coupling', 'and', 'the', 'add... | [-0.1977766523414175, 0.28138549349387176, -0.04800660598266404, 0.09631571920363058, -0.0786815949868469, -0.1805890412069857, -0.020596728158125188, 0.30177645542426035, -0.16839043113577645, -0.23837941760575632, 0.017179053978907177, -0.2614138773060404, -0.11064815926511073, 0.10599894779443275, 0.0178640270023606... |
710.1261 | Coulomb distortion effects in quasi-elastic (e,e') scattering on heavy
nuclei | The influence of the Coulomb distortion for quasi-elastic (e,e') scattering
on highly charged nuclei is investigated in distorted wave Born approximation
for electrons. The Dirac equation is solved numerically in order to obtain
exact electron continuum states in the electrostatic field generated by the
charge distri... | nucl-th | the influence of the coulomb distortion for quasielastic ee scattering on highly charged nuclei is investigated in distorted wave born approximation for electrons the dirac equation is solved numerically in order to obtain exact electron continuum states in the electrostatic field generated by the charge distribution o... | [['the', 'influence', 'of', 'the', 'coulomb', 'distortion', 'for', 'quasielastic', 'ee', 'scattering', 'on', 'highly', 'charged', 'nuclei', 'is', 'investigated', 'in', 'distorted', 'wave', 'born', 'approximation', 'for', 'electrons', 'the', 'dirac', 'equation', 'is', 'solved', 'numerically', 'in', 'order', 'to', 'obtai... | [-0.07885851299157366, 0.1580877862185298, -0.04528170836158097, 0.16626305991085247, 0.025471614887937904, -0.060137002525734715, -0.007522119055502117, 0.3604357734322548, -0.23969681993126868, -0.2726043210551143, -0.05576845753006637, -0.3222114256769419, -0.02809225053526461, 0.13278891699388623, 0.095530155785381... |
710.1262 | Algorithmically detecting the bridge number of hyperbolic knots | We exhibit an algorithm to determine the bridge number of a hyperbolic knot
in the 3-sphere. The proof uses adaptations of almost normal surface theory for
compact surfaces with boundary in ideally triangulated knot exteriors.
| math.GT | we exhibit an algorithm to determine the bridge number of a hyperbolic knot in the 3sphere the proof uses adaptations of almost normal surface theory for compact surfaces with boundary in ideally triangulated knot exteriors | [['we', 'exhibit', 'an', 'algorithm', 'to', 'determine', 'the', 'bridge', 'number', 'of', 'a', 'hyperbolic', 'knot', 'in', 'the', '3sphere', 'the', 'proof', 'uses', 'adaptations', 'of', 'almost', 'normal', 'surface', 'theory', 'for', 'compact', 'surfaces', 'with', 'boundary', 'in', 'ideally', 'triangulated', 'knot', 'e... | [-0.21663882789601172, 0.06953342018490989, -0.16815117626850093, 0.07840610503086022, -0.13163629759635245, -0.19947900158752288, 0.005397034313396684, 0.37224652442548956, -0.27102306341486315, -0.3359807321003505, 0.06584613659153027, -0.20113038303596634, -0.1953237707061427, 0.21611578954117638, -0.206088517260338... |
710.1263 | Preparing for N_f=2 simulations at small lattice spacings | We discuss some large effects of dynamical fermions. One is a cutoff effect,
others concern the contribution of multi-pion states to correlation functions
and are expected to survive the continuum limit. We then turn to the
preparation for simulations at small lattice spacings which we are planning
down to around a=0... | hep-lat | we discuss some large effects of dynamical fermions one is a cutoff effect others concern the contribution of multipion states to correlation functions and are expected to survive the continuum limit we then turn to the preparation for simulations at small lattice spacings which we are planning down to around a004fm in... | [['we', 'discuss', 'some', 'large', 'effects', 'of', 'dynamical', 'fermions', 'one', 'is', 'a', 'cutoff', 'effect', 'others', 'concern', 'the', 'contribution', 'of', 'multipion', 'states', 'to', 'correlation', 'functions', 'and', 'are', 'expected', 'to', 'survive', 'the', 'continuum', 'limit', 'we', 'then', 'turn', 'to... | [-0.12704908007581253, 0.21657442197902127, -0.09112039983156137, 0.10660577907983679, -0.03473961125127971, -0.06208705745084444, 0.07356628975685453, 0.36281525387894364, -0.2571223031496629, -0.27903644581092524, 0.08408849718252895, -0.3374739274411695, -0.06667827732744627, 0.11309109798166901, 0.02973185843438841... |
710.1264 | Photo-gating Carbon Nanotube Transistors | Optoelectronic measurements of carbon nanotube transistors have shown a wide
variety of sensitivites to the incident light. Direct photocurrent processes
compete with a number of extrinsic mechanisms. Here we show that visible light
absorption in the silicon substrate generates a photovoltage that can
electrically ga... | cond-mat.mtrl-sci | optoelectronic measurements of carbon nanotube transistors have shown a wide variety of sensitivites to the incident light direct photocurrent processes compete with a number of extrinsic mechanisms here we show that visible light absorption in the silicon substrate generates a photovoltage that can electrically gate t... | [['optoelectronic', 'measurements', 'of', 'carbon', 'nanotube', 'transistors', 'have', 'shown', 'a', 'wide', 'variety', 'of', 'sensitivites', 'to', 'the', 'incident', 'light', 'direct', 'photocurrent', 'processes', 'compete', 'with', 'a', 'number', 'of', 'extrinsic', 'mechanisms', 'here', 'we', 'show', 'that', 'visible... | [-0.14308311384628666, 0.2031789697723183, -0.022032938110003397, -0.0649717808701098, -0.01788378594673972, -0.1803946446882874, 0.06713477823784393, 0.4798824798019059, -0.28880986485597304, -0.3236642028575977, -0.015258717030262063, -0.2913658907307328, -0.141281917085459, 0.2942986681200234, -0.01808963536565085, ... |
710.1265 | Quantum Monte Carlo calculations of electroweak transition matrix
elements in A = 6,7 nuclei | Green's function Monte Carlo calculations of magnetic dipole, electric
quadrupole, Fermi, and Gamow-Teller transition matrix elements are reported for
A=6,7 nuclei. The matrix elements are extrapolated from mixed estimates that
bracket the relevant electroweak operator between variational Monte Carlo and
GFMC propaga... | nucl-th | greens function monte carlo calculations of magnetic dipole electric quadrupole fermi and gamowteller transition matrix elements are reported for a67 nuclei the matrix elements are extrapolated from mixed estimates that bracket the relevant electroweak operator between variational monte carlo and gfmc propagated wave f... | [['greens', 'function', 'monte', 'carlo', 'calculations', 'of', 'magnetic', 'dipole', 'electric', 'quadrupole', 'fermi', 'and', 'gamowteller', 'transition', 'matrix', 'elements', 'are', 'reported', 'for', 'a67', 'nuclei', 'the', 'matrix', 'elements', 'are', 'extrapolated', 'from', 'mixed', 'estimates', 'that', 'bracket... | [-0.06172481908119823, 0.22673316969487228, -0.06299850818468258, 0.16817684564739466, 0.0016160427543677781, -0.10360785958994376, -0.01997026937376512, 0.4214378023618146, -0.17398493739065568, -0.29158326425883724, -0.01628643685804778, -0.3604835622208683, -0.04651873132802154, 0.13926975293281046, 0.14379526209086... |
710.1266 | Collisional Energy Loss of a Fast Muon in a Hot QED Plasma | We calculate the collisional energy loss of a muon of high energy $E$ in a
hot QED plasma beyond logarithmic accuracy, i.e., we determine the constant
terms of order O(1) in $-dE/dx \propto \ln{E}+ O(1)$. Considering first the
$t$-channel contribution to $-dE/dx$, we show that the terms $\sim O(1)$ are
sensitive to t... | hep-ph | we calculate the collisional energy loss of a muon of high energy e in a hot qed plasma beyond logarithmic accuracy ie we determine the constant terms of order o1 in dedx propto lne o1 considering first the tchannel contribution to dedx we show that the terms sim o1 are sensitive to the full kinematic region for the mo... | [['we', 'calculate', 'the', 'collisional', 'energy', 'loss', 'of', 'a', 'muon', 'of', 'high', 'energy', 'e', 'in', 'a', 'hot', 'qed', 'plasma', 'beyond', 'logarithmic', 'accuracy', 'ie', 'we', 'determine', 'the', 'constant', 'terms', 'of', 'order', 'o1', 'in', 'dedx', 'propto', 'lne', 'o1', 'considering', 'first', 'the... | [-0.1023380881595996, 0.2020231519924334, -0.06048532299877655, 0.11629060655531864, -0.051598447633366434, -0.07124216084729039, 0.05069879670120445, 0.31742695345873795, -0.21965140660158208, -0.31056182314341346, -0.030816085924274258, -0.3097482041485848, -0.0032420613412414826, 0.1560768253410295, 0.01223137496065... |
710.1267 | Production of a pion in association with a high-Q2 dilepton pair in
antiproton-proton annihilation at GSI-FAIR | We evaluate the cross section for anti-p p -> l+ l- pi0 in the forward
direction and for large lepton pair invariant mass. In this kinematical region,
the leading-twist amplitude factorises into a short-distance matrix element,
long-distance dominated antiproton Distribution Amplitudes and proton to pion
Transition D... | hep-ph hep-ex nucl-th | we evaluate the cross section for antip p l l pi0 in the forward direction and for large lepton pair invariant mass in this kinematical region the leadingtwist amplitude factorises into a shortdistance matrix element longdistance dominated antiproton distribution amplitudes and proton to pion transition distribution am... | [['we', 'evaluate', 'the', 'cross', 'section', 'for', 'antip', 'p', 'l', 'l', 'pi0', 'in', 'the', 'forward', 'direction', 'and', 'for', 'large', 'lepton', 'pair', 'invariant', 'mass', 'in', 'this', 'kinematical', 'region', 'the', 'leadingtwist', 'amplitude', 'factorises', 'into', 'a', 'shortdistance', 'matrix', 'elemen... | [-0.0897802908021288, 0.2036398520740943, -0.14404316837541187, 0.1360793735300318, -0.01029019134465414, -0.07001621813068572, 0.05937957210848347, 0.33544668333175093, -0.22556267521129206, -0.19907592862653425, -0.0828806245729375, -0.30401943669391746, -0.009537445462625235, 0.12915847530343738, 0.0882113178597184,... |
710.1268 | Top Hypercharge | We propose a top hypercharge model with gauge symmetry SU(3)_C x SU(2)_L x
U(1)_1 x U(1)_2 where the first two families of the Standard Model (SM)
fermions are charged under U(1)_1 while the third family is charged under
U(1)_2. The U(1)_1 x U(1)_2 gauge symmetry is broken down to the U(1)_Y gauge
symmetry, when a SM... | hep-ph | we propose a top hypercharge model with gauge symmetry su3_c x su2_l x u1_1 x u1_2 where the first two families of the standard model sm fermions are charged under u1_1 while the third family is charged under u1_2 the u1_1 x u1_2 gauge symmetry is broken down to the u1_y gauge symmetry when a sm singlet higgs field acq... | [['we', 'propose', 'a', 'top', 'hypercharge', 'model', 'with', 'gauge', 'symmetry', 'su3_c', 'x', 'su2_l', 'x', 'u1_1', 'x', 'u1_2', 'where', 'the', 'first', 'two', 'families', 'of', 'the', 'standard', 'model', 'sm', 'fermions', 'are', 'charged', 'under', 'u1_1', 'while', 'the', 'third', 'family', 'is', 'charged', 'und... | [-0.13885463432603473, 0.3347887243005211, -0.01735107074213673, 0.13598623434116425, -0.07459531176432188, -0.2221368672187204, 0.02709968273142186, 0.3144514669261094, -0.19775120354928216, -0.25781579760473167, 0.007934970182623825, -0.307243983664397, 0.027077600794302215, -0.0031160894162786095, 0.0695271736441819... |
710.1269 | Generic mixed columnar-plaquette phases in Rokhsar-Kivelson models | We revisit the phase diagram of Rokhsar-Kivelson models, which are used in
fields such as superconductivity, frustrated magnetism, cold bosons, and the
physics of Josephson junction arrays. From an extended height effective theory,
we show that one of two simple generic phase diagrams contains a mixed phase
that inte... | cond-mat.str-el | we revisit the phase diagram of rokhsarkivelson models which are used in fields such as superconductivity frustrated magnetism cold bosons and the physics of josephson junction arrays from an extended height effective theory we show that one of two simple generic phase diagrams contains a mixed phase that interpolates ... | [['we', 'revisit', 'the', 'phase', 'diagram', 'of', 'rokhsarkivelson', 'models', 'which', 'are', 'used', 'in', 'fields', 'such', 'as', 'superconductivity', 'frustrated', 'magnetism', 'cold', 'bosons', 'and', 'the', 'physics', 'of', 'josephson', 'junction', 'arrays', 'from', 'an', 'extended', 'height', 'effective', 'the... | [-0.17015775191862512, 0.18630080984306197, -0.08242266315437101, 0.09074520028661937, -0.01910670381466593, -0.13690259823695236, 0.0706955771199043, 0.39394483249634504, -0.23258473701057358, -0.27077390462023404, 0.04170452198761285, -0.29499790566298395, -0.15888295703729904, 0.14633023923203145, 0.0592498244982588... |
710.127 | Note on graviton MHV amplitudes | Two new formulas which express n-graviton MHV tree amplitudes in terms of
sums of squares of n-gluon amplitudes are discussed. The first formula is
derived from recursion relations. The second formula, simpler because it
involves fewer permutations, is obtained from the variant of the Berends,
Giele, Kuijf formula gi... | hep-th | two new formulas which express ngraviton mhv tree amplitudes in terms of sums of squares of ngluon amplitudes are discussed the first formula is derived from recursion relations the second formula simpler because it involves fewer permutations is obtained from the variant of the berends giele kuijf formula given in arx... | [['two', 'new', 'formulas', 'which', 'express', 'ngraviton', 'mhv', 'tree', 'amplitudes', 'in', 'terms', 'of', 'sums', 'of', 'squares', 'of', 'ngluon', 'amplitudes', 'are', 'discussed', 'the', 'first', 'formula', 'is', 'derived', 'from', 'recursion', 'relations', 'the', 'second', 'formula', 'simpler', 'because', 'it', ... | [-0.15622834158034957, 0.13399816011743887, -0.09418886366813463, 0.16907833416338022, -0.10824492205010385, -0.1302281426531928, 0.06309913794453047, 0.23905583138444594, -0.21655410575224276, -0.2764414038071979, 0.039927056795746395, -0.24925950562999566, -0.2275486347474614, 0.24180245783408078, -0.0672914203032447... |
710.1271 | Flavor Evolution of the Neutronization Neutrino Burst from an O-Ne-Mg
Core-Collapse Supernova | We present results of 3-neutrino flavor evolution simulations for the
neutronization burst from an O-Ne-Mg core-collapse supernova. We find that
nonlinear neutrino self-coupling engineers a single spectral feature of
stepwise conversion in the inverted neutrino mass hierarchy case and in the
normal mass hierarchy cas... | astro-ph hep-ph | we present results of 3neutrino flavor evolution simulations for the neutronization burst from an onemg corecollapse supernova we find that nonlinear neutrino selfcoupling engineers a single spectral feature of stepwise conversion in the inverted neutrino mass hierarchy case and in the normal mass hierarchy case a supe... | [['we', 'present', 'results', 'of', '3neutrino', 'flavor', 'evolution', 'simulations', 'for', 'the', 'neutronization', 'burst', 'from', 'an', 'onemg', 'corecollapse', 'supernova', 'we', 'find', 'that', 'nonlinear', 'neutrino', 'selfcoupling', 'engineers', 'a', 'single', 'spectral', 'feature', 'of', 'stepwise', 'convers... | [-0.04972887343116185, 0.19431529690837612, -0.002925537606721283, 0.210619506547578, -0.10485230144163374, -0.12656297843142222, 0.06755154610671583, 0.3585974029365486, -0.22903046903691143, -0.32100283052091316, 0.020355441808445198, -0.284236187856364, -0.05191329191689209, 0.2029673756721119, 0.05552658573115653, ... |
710.1272 | Coupling Lattice Boltzmann with Atomistic Dynamics for the multiscale
simulation of nano-biological flows | We describe a recent multiscale approach based on the concurrent coupling of
constrained molecular dynamics for long biomolecules with a mesoscopic lattice
Boltzmann treatment of solvent hydrodynamics. The multiscale approach is based
on a simple scheme of exchange of space-time information between the atomistic
and ... | physics.bio-ph physics.flu-dyn | we describe a recent multiscale approach based on the concurrent coupling of constrained molecular dynamics for long biomolecules with a mesoscopic lattice boltzmann treatment of solvent hydrodynamics the multiscale approach is based on a simple scheme of exchange of spacetime information between the atomistic and meso... | [['we', 'describe', 'a', 'recent', 'multiscale', 'approach', 'based', 'on', 'the', 'concurrent', 'coupling', 'of', 'constrained', 'molecular', 'dynamics', 'for', 'long', 'biomolecules', 'with', 'a', 'mesoscopic', 'lattice', 'boltzmann', 'treatment', 'of', 'solvent', 'hydrodynamics', 'the', 'multiscale', 'approach', 'is... | [-0.09948122780770063, 0.09452674547707526, -0.13228660348104312, 0.0186102355137488, -0.02165944268538927, -0.12392456395706783, 0.003608874770967911, 0.3699509994747738, -0.28445561591846247, -0.28021973280313733, -0.007559793275625755, -0.22206883458420634, -0.16833815096373048, 0.17827655555835614, 0.02918499434987... |
710.1273 | Generic canonical form of pairs of matrices with zeros | We consider a family of pairs of m-by-p and m-by-q matrices, in which some
entries are required to be zero and the others are arbitrary, with respect to
transformations (A,B)--> (SAR,SBL) with nonsingular S, R, L. We prove that
almost all of these pairs reduce to the same pair (C, D) from this family,
except for pair... | math.RT | we consider a family of pairs of mbyp and mbyq matrices in which some entries are required to be zero and the others are arbitrary with respect to transformations ab sarsbl with nonsingular s r l we prove that almost all of these pairs reduce to the same pair c d from this family except for pairs whose arbitrary entrie... | [['we', 'consider', 'a', 'family', 'of', 'pairs', 'of', 'mbyp', 'and', 'mbyq', 'matrices', 'in', 'which', 'some', 'entries', 'are', 'required', 'to', 'be', 'zero', 'and', 'the', 'others', 'are', 'arbitrary', 'with', 'respect', 'to', 'transformations', 'ab', 'sarsbl', 'with', 'nonsingular', 's', 'r', 'l', 'we', 'prove',... | [-0.19084499030183238, 0.11849678366119604, -0.02233581577079842, 0.011215600032213491, -0.04542220042771604, -0.17197752875242248, 0.017647116351031125, 0.3635092762197895, -0.298404163894165, -0.2669403384171752, 0.08821527868879578, -0.29684312789734585, -0.12442433370658791, 0.17008721441905722, -0.0078996766627912... |
710.1274 | Gravity model in the Korean highway | We investigate the traffic flows of the Korean highway system, which contains
both public and private transportation information. We find that the traffic
flow T(ij) between city i and j forms a gravity model, the metaphor of physical
gravity as described in Newton's law of gravity, P(i)P(j)/r(ij)^2, where P(i)
repre... | physics.soc-ph physics.geo-ph | we investigate the traffic flows of the korean highway system which contains both public and private transportation information we find that the traffic flow tij between city i and j forms a gravity model the metaphor of physical gravity as described in newtons law of gravity pipjrij2 where pi represents the population... | [['we', 'investigate', 'the', 'traffic', 'flows', 'of', 'the', 'korean', 'highway', 'system', 'which', 'contains', 'both', 'public', 'and', 'private', 'transportation', 'information', 'we', 'find', 'that', 'the', 'traffic', 'flow', 'tij', 'between', 'city', 'i', 'and', 'j', 'forms', 'a', 'gravity', 'model', 'the', 'met... | [-0.17329089441941156, 0.10149745589128892, -0.11089027788525876, 0.07626945149520627, -0.026292293579479938, -0.20833891167645702, 0.05102265157844298, 0.33583733858540654, -0.23767538117961243, -0.294681488180336, 0.09468417624213124, -0.32500019212826514, -0.16018000637324384, 0.15509000604820009, -0.087385178445121... |
710.1275 | On Convergence Properties of Shannon Entropy | Convergence properties of Shannon Entropy are studied. In the differential
setting, it is shown that weak convergence of probability measures, or
convergence in distribution, is not enough for convergence of the associated
differential entropies. A general result for the desired differential entropy
convergence is pr... | cs.IT math.IT | convergence properties of shannon entropy are studied in the differential setting it is shown that weak convergence of probability measures or convergence in distribution is not enough for convergence of the associated differential entropies a general result for the desired differential entropy convergence is provided ... | [['convergence', 'properties', 'of', 'shannon', 'entropy', 'are', 'studied', 'in', 'the', 'differential', 'setting', 'it', 'is', 'shown', 'that', 'weak', 'convergence', 'of', 'probability', 'measures', 'or', 'convergence', 'in', 'distribution', 'is', 'not', 'enough', 'for', 'convergence', 'of', 'the', 'associated', 'di... | [-0.10577125902287662, 0.046837470860336905, -0.1326991481948644, 0.14574609855189918, 0.026748696446418762, -0.09240929977223276, 0.019439440382644533, 0.355211898624897, -0.2624267269074917, -0.21840784338116645, 0.11850936130620539, -0.25686595813930035, -0.09034883014392107, 0.21939139201305807, -0.1184778467901051... |
710.1276 | Riemannian groupoids and solitons for three-dimensional homogeneous
Ricci and cross curvature flows | In this paper we investigate the behavior of three-dimensional homogeneous
solutions of the cross curvature flow using Riemannian groupoids. The
Riemannian groupoid technique, introduced by John Lott, allows us to
investigate the long term behavior of collapsing solutions of the flow,
producing soliton solutions in t... | math.DG | in this paper we investigate the behavior of threedimensional homogeneous solutions of the cross curvature flow using riemannian groupoids the riemannian groupoid technique introduced by john lott allows us to investigate the long term behavior of collapsing solutions of the flow producing soliton solutions in the limi... | [['in', 'this', 'paper', 'we', 'investigate', 'the', 'behavior', 'of', 'threedimensional', 'homogeneous', 'solutions', 'of', 'the', 'cross', 'curvature', 'flow', 'using', 'riemannian', 'groupoids', 'the', 'riemannian', 'groupoid', 'technique', 'introduced', 'by', 'john', 'lott', 'allows', 'us', 'to', 'investigate', 'th... | [-0.1740741631098596, 0.041529924749435544, -0.10475163338317846, 0.05951539263454227, -0.10020408137158181, -0.09586784371640533, -0.05021571872809242, 0.34678374660628225, -0.2672747516432234, -0.2167976467559735, 0.11627159204848188, -0.30361915515838217, -0.15646044360861802, 0.1706988023215672, -0.0851888671992734... |
710.1277 | New results on particle acceleration in the Centaurus A jet and
counterjet from a deep Chandra observation | We present new deep Chandra observations of the Centaurus A jet, with a
combined on-source exposure time of 719 ks. These data allow detailed X-ray
spectral measurements to be made along the jet out to its disappearance at 4.5
kpc from the nucleus. We distinguish several regimes of high-energy particle
acceleration: ... | astro-ph | we present new deep chandra observations of the centaurus a jet with a combined onsource exposure time of 719 ks these data allow detailed xray spectral measurements to be made along the jet out to its disappearance at 45 kpc from the nucleus we distinguish several regimes of highenergy particle acceleration while the ... | [['we', 'present', 'new', 'deep', 'chandra', 'observations', 'of', 'the', 'centaurus', 'a', 'jet', 'with', 'a', 'combined', 'onsource', 'exposure', 'time', 'of', '719', 'ks', 'these', 'data', 'allow', 'detailed', 'xray', 'spectral', 'measurements', 'to', 'be', 'made', 'along', 'the', 'jet', 'out', 'to', 'its', 'disappe... | [-0.07155215310018807, 0.09097413037642244, -0.11864789191852598, 0.10860805319334402, -0.10509744309668058, -0.09104566867432855, 0.025312393366547874, 0.4562109911242147, -0.24546505053058948, -0.3293607953351502, 0.04793284935009319, -0.27928686258839625, 0.022850144484074287, 0.19485800513112003, -0.006314840478201... |
710.1278 | Miniversal deformations of chains of linear mappings | V.I. Arnold [Russian Math. Surveys, 26 (no. 2), 1971, pp. 29-43] gave a
miniversal deformation of matrices of linear operators; that is, a simple
canonical form, to which not only a given square matrix A, but also the family
of all matrices close to A, can be reduced by similarity transformations
smoothly depending o... | math.RT | vi arnold russian math surveys 26 no 2 1971 pp 2943 gave a miniversal deformation of matrices of linear operators that is a simple canonical form to which not only a given square matrix a but also the family of all matrices close to a can be reduced by similarity transformations smoothly depending on the entries of mat... | [['vi', 'arnold', 'russian', 'math', 'surveys', '26', 'no', '2', '1971', 'pp', '2943', 'gave', 'a', 'miniversal', 'deformation', 'of', 'matrices', 'of', 'linear', 'operators', 'that', 'is', 'a', 'simple', 'canonical', 'form', 'to', 'which', 'not', 'only', 'a', 'given', 'square', 'matrix', 'a', 'but', 'also', 'the', 'fa... | [-0.12176181698617126, 0.10519682637766584, -0.05493650602346117, 0.046108780932225674, -0.09271699757097507, -0.14018776503621372, 0.017475873497979983, 0.32361334645455436, -0.3050728976339489, -0.232811760650222, 0.1255303967196809, -0.26173580084721765, -0.2217836419374428, 0.14739593253289532, -0.09807620602720357... |
710.1279 | The 3He + 4He --> 7Be Astrophysical S-factor | We present precision measurements of the 3He + 4He --> 7Be reaction in the
range ECM = 0.33 to 1.23 MeV using a small gas cell and detection of both
prompt gamma rays and 7Be activity. Our prompt and activity measurements are in
good agreement within an experimental uncertainty of several percent. We find
S(0) = 0.59... | nucl-ex astro-ph | we present precision measurements of the 3he 4he 7be reaction in the range ecm 033 to 123 mev using a small gas cell and detection of both prompt gamma rays and 7be activity our prompt and activity measurements are in good agreement within an experimental uncertainty of several percent we find s0 0595 0018 kev b from f... | [['we', 'present', 'precision', 'measurements', 'of', 'the', '3he', '4he', '7be', 'reaction', 'in', 'the', 'range', 'ecm', '033', 'to', '123', 'mev', 'using', 'a', 'small', 'gas', 'cell', 'and', 'detection', 'of', 'both', 'prompt', 'gamma', 'rays', 'and', '7be', 'activity', 'our', 'prompt', 'and', 'activity', 'measurem... | [-0.010870195314055309, 0.15557703386797964, -0.006370046991262, 0.09626633691233258, 0.03664602951767995, -0.04462555572282263, 0.10759679869299235, 0.37073321299908985, -0.16801139500620232, -0.36292737910827233, 0.011205788433746717, -0.39674355440534825, 0.03479553711448991, 0.23166539978918207, -0.0082166390899612... |
710.128 | On the Relationship between Mutual Information and Minimum Mean-Square
Errors in Stochastic Dynamical Systems | We consider a general stochastic input-output dynamical system with output
evolving in time as the solution to a functional coefficients, It\^{o}'s
stochastic differential equation, excited by an input process. This general
class of stochastic systems encompasses not only the classical communication
channel models, b... | cs.IT math.IT | we consider a general stochastic inputoutput dynamical system with output evolving in time as the solution to a functional coefficients itos stochastic differential equation excited by an input process this general class of stochastic systems encompasses not only the classical communication channel models but also a wi... | [['we', 'consider', 'a', 'general', 'stochastic', 'inputoutput', 'dynamical', 'system', 'with', 'output', 'evolving', 'in', 'time', 'as', 'the', 'solution', 'to', 'a', 'functional', 'coefficients', 'itos', 'stochastic', 'differential', 'equation', 'excited', 'by', 'an', 'input', 'process', 'this', 'general', 'class', '... | [-0.1590994924326685, 0.06005771749527838, -0.049792648975057065, 0.12766901111766765, -0.07843136487046508, -0.16044461735563867, 0.06109432011499261, 0.3372715210050001, -0.31164752713781085, -0.29584312952513286, 0.10214818071438568, -0.2051373756034894, -0.1916307611935871, 0.19517147909612098, -0.09580371591612591... |
710.1281 | Normal holomorphic curves from parabolic regions to projective spaces | A holomorphic map from the complex line to a complex projective space is
called normal (a. k. a. Brody curve) if it is uniformly continuous from the
Euclidean metric to the Fubini--Study metric. The paper contains a survey of
known results about such maps, as well as some new theorems.
| math.CV | a holomorphic map from the complex line to a complex projective space is called normal a k a brody curve if it is uniformly continuous from the euclidean metric to the fubinistudy metric the paper contains a survey of known results about such maps as well as some new theorems | [['a', 'holomorphic', 'map', 'from', 'the', 'complex', 'line', 'to', 'a', 'complex', 'projective', 'space', 'is', 'called', 'normal', 'a', 'k', 'a', 'brody', 'curve', 'if', 'it', 'is', 'uniformly', 'continuous', 'from', 'the', 'euclidean', 'metric', 'to', 'the', 'fubinistudy', 'metric', 'the', 'paper', 'contains', 'a',... | [-0.11851717351004482, 0.054327083959942686, -0.11230875282548368, 0.09197833126876503, -0.14429087315686048, -0.10746584276668728, 0.03164878240088001, 0.3580688825249672, -0.3085444250889122, -0.17677367623895407, 0.13976516705006362, -0.3151940722763538, -0.2351933154463768, 0.24719124868512155, -0.1338346225116402,... |
710.1282 | The Relativistic framework of Positioning systems | Emission relativistic coordinates are a class of spacetime coordinates
defined and generated by four emitters (satellites, pulsars) broadcasting their
proper time by radio signals. They are the main ingredient of the simplest
conceivable relativistic positioning system. The emission coordinates are
independent of any... | gr-qc astro-ph | emission relativistic coordinates are a class of spacetime coordinates defined and generated by four emitters satellites pulsars broadcasting their proper time by radio signals they are the main ingredient of the simplest conceivable relativistic positioning system the emission coordinates are independent of any observ... | [['emission', 'relativistic', 'coordinates', 'are', 'a', 'class', 'of', 'spacetime', 'coordinates', 'defined', 'and', 'generated', 'by', 'four', 'emitters', 'satellites', 'pulsars', 'broadcasting', 'their', 'proper', 'time', 'by', 'radio', 'signals', 'they', 'are', 'the', 'main', 'ingredient', 'of', 'the', 'simplest', ... | [-0.15261718397325075, 0.09176609425564741, -0.10246665047121827, 0.06581586036746474, -0.06947073606266217, -0.14469356787475673, 0.003538288465510546, 0.37959880329118195, -0.21367108881558208, -0.309710881983946, 0.09004607583417303, -0.27140553175387055, -0.10779128928922795, 0.2109485016013919, -0.0747139912204478... |
710.1283 | Renewal-type Limit Theorem for the Gauss Map and Continued Fractions | In this paper we prove the following renewal-type limit theorem. Given an
irrational $\alpha$ in (0,1) and R>0, let $q_{n_R}$ be the first denominator of
the convergents of $\alpha$ which exceeds R. The main result in the paper is
that the ratio $q_{n_R}/R$ has a limiting distribution as R tends to infinity.
The exis... | math.DS | in this paper we prove the following renewaltype limit theorem given an irrational alpha in 01 and r0 let q_n_r be the first denominator of the convergents of alpha which exceeds r the main result in the paper is that the ratio q_n_rr has a limiting distribution as r tends to infinity the existence of the limiting dist... | [['in', 'this', 'paper', 'we', 'prove', 'the', 'following', 'renewaltype', 'limit', 'theorem', 'given', 'an', 'irrational', 'alpha', 'in', '01', 'and', 'r0', 'let', 'q_n_r', 'be', 'the', 'first', 'denominator', 'of', 'the', 'convergents', 'of', 'alpha', 'which', 'exceeds', 'r', 'the', 'main', 'result', 'in', 'the', 'pa... | [-0.15368555378434914, 0.07441242421232995, -0.09964556294892515, 0.010858898370393685, -0.006651135494134256, -0.08859490263941032, 0.039385415177925355, 0.2547985870923315, -0.2907219298183918, -0.21741957286306257, 0.10367363570091714, -0.2747538192230942, -0.11107617413092936, 0.17551926991769246, -0.10251449326918... |
710.1284 | Comment on "Similarity analysis in magnetohydrodynamics: effects of Hall
and ion-slip currents on free convection flow and mass transfer of a gas past
a semi-infinite vertical plate," A.A. Megahed, S.R. Komy, A.A. Afify | Comment on Similarity analysis in magnetohydrodynamics:effects of Hall and
ion-slip currents on free convection flow and mass transfer of a gas past a
semi-infinite vertical plate, A.A. Megahed, S.R. Komy, A.A. Afify [Acta
Mechanica 151, 185-194 (2001)]
In the above paper is investigated the boundary layer flow of ... | physics.flu-dyn | comment on similarity analysis in magnetohydrodynamicseffects of hall and ionslip currents on free convection flow and mass transfer of a gas past a semiinfinite vertical plate aa megahed sr komy aa afify acta mechanica 151 185194 2001 in the above paper is investigated the boundary layer flow of an electrically conduc... | [['comment', 'on', 'similarity', 'analysis', 'in', 'magnetohydrodynamicseffects', 'of', 'hall', 'and', 'ionslip', 'currents', 'on', 'free', 'convection', 'flow', 'and', 'mass', 'transfer', 'of', 'a', 'gas', 'past', 'a', 'semiinfinite', 'vertical', 'plate', 'aa', 'megahed', 'sr', 'komy', 'aa', 'afify', 'acta', 'mechanic... | [-0.1542865332850488, 0.17239108755849883, -0.046915300861001014, 0.007994175419444218, -0.00871464402647689, -0.1401510907476768, 0.007819503650534899, 0.37801608972251416, -0.26886570639908314, -0.27158177172765136, 0.12004411492496729, -0.2807731965277344, -0.06387737475335598, 0.19254552435129882, -0.03050722270272... |
710.1285 | Small scale behavior of the physical conditions and the abundance
discrepancy in the Orion nebula | We present results of long-slit spectroscopy in several positions of the
Orion nebula. Our goal is to study the spatial distribution of a large number
of nebular quantities, including line fluxes, physical conditions and ionic
abundances at a spatial resolution of about 1". We find that protoplanetary
disks (proplyds... | astro-ph | we present results of longslit spectroscopy in several positions of the orion nebula our goal is to study the spatial distribution of a large number of nebular quantities including line fluxes physical conditions and ionic abundances at a spatial resolution of about 1 we find that protoplanetary disks proplyds show pro... | [['we', 'present', 'results', 'of', 'longslit', 'spectroscopy', 'in', 'several', 'positions', 'of', 'the', 'orion', 'nebula', 'our', 'goal', 'is', 'to', 'study', 'the', 'spatial', 'distribution', 'of', 'a', 'large', 'number', 'of', 'nebular', 'quantities', 'including', 'line', 'fluxes', 'physical', 'conditions', 'and',... | [-0.06442121778228233, 0.10544050518683606, -0.030453024737818062, 0.056491355612909175, -0.03167977316155678, -0.11697408176282034, 0.04054199183482747, 0.412481086405943, -0.2203676529777816, -0.3295694816850987, 0.028627278172534028, -0.2687743816384167, -0.04522850091046355, 0.14661626999248872, -0.0508644944390738... |
710.1286 | Propagation-based x-ray phase-contrast imaging with broad focus
conventional x-ray sources | A propagation-based x-ray phase-contrast imaging (PBI) setup using a
conventional x-ray source (LFF Cu target) is presented. A virtual x-ray source
of 40 x 50 $\mu$$m^2$ was created by using, horizontally, a $6^o$ take-off
angle (with the x-ray tube working in the line focus geometry) and, vertically,
a 50 $\mu$m sli... | cond-mat.other | a propagationbased xray phasecontrast imaging pbi setup using a conventional xray source lff cu target is presented a virtual xray source of 40 x 50 mum2 was created by using horizontally a 6o takeoff angle with the xray tube working in the line focus geometry and vertically a 50 mum slit the sample was set 12 m from t... | [['a', 'propagationbased', 'xray', 'phasecontrast', 'imaging', 'pbi', 'setup', 'using', 'a', 'conventional', 'xray', 'source', 'lff', 'cu', 'target', 'is', 'presented', 'a', 'virtual', 'xray', 'source', 'of', '40', 'x', '50', 'mum2', 'was', 'created', 'by', 'using', 'horizontally', 'a', '6o', 'takeoff', 'angle', 'with'... | [-0.04842547901595632, 0.10324770302943279, -0.046048251613054744, 0.03685183094794298, -0.040324468803764495, -0.15182846831229665, 0.044920623183169944, 0.45953236649065843, -0.23602262363240215, -0.37300441736631373, 0.10470802723616937, -0.33146770407566456, -0.04108587845320595, 0.2109568461022673, -0.063257383761... |
710.1287 | A Limit Theorem for Birkoff sums of non-integrable functions over
rotations | We consider Birkhoff sums of functions with a singularity of type 1/x over
rotations and prove the following limit theorem. Let $S_N= S_N(\alpha,x)$ be
the N^th non-renormalized Birkhoff sum, where $x in [0,1)$ is the initial
point, $\alpha\in [0,1)$ is the rotation number and $(\alpha, x)$ are uniformly
distributed.... | math.DS | we consider birkhoff sums of functions with a singularity of type 1x over rotations and prove the following limit theorem let s_n s_nalphax be the nth nonrenormalized birkhoff sum where x in 01 is the initial point alphain 01 is the rotation number and alpha x are uniformly distributed we prove that s_nn has a joint li... | [['we', 'consider', 'birkhoff', 'sums', 'of', 'functions', 'with', 'a', 'singularity', 'of', 'type', '1x', 'over', 'rotations', 'and', 'prove', 'the', 'following', 'limit', 'theorem', 'let', 's_n', 's_nalphax', 'be', 'the', 'nth', 'nonrenormalized', 'birkhoff', 'sum', 'where', 'x', 'in', '01', 'is', 'the', 'initial', '... | [-0.19674079713140485, 0.0913685426953001, -0.12841840882938874, 0.04184737839276278, 0.024446871220075255, -0.1228663323246697, 0.061742634689317476, 0.33563034123257746, -0.32433190875792806, -0.1684779774020367, 0.10690264379063362, -0.3319079301119605, -0.044277722573002117, 0.1542571339803406, -0.09563966366002642... |
710.1288 | On Groups with a Supercomplemented Subgroup | Groups, in which every subgroup containing some fixed primary cyclic subgroup
has a complement, are investigated.
| math.GR | groups in which every subgroup containing some fixed primary cyclic subgroup has a complement are investigated | [['groups', 'in', 'which', 'every', 'subgroup', 'containing', 'some', 'fixed', 'primary', 'cyclic', 'subgroup', 'has', 'a', 'complement', 'are', 'investigated']] | [-0.2813874225830659, 0.11495353380450979, -0.09404839435592294, -0.04065955936675891, -0.09180792540428229, -0.19480782534810714, 0.015681596560170874, 0.4364579792600125, -0.31226426374632865, -0.175094892969355, 0.21058144550625002, -0.3181698187254369, -0.048369448457378894, 0.18856636621057987, -0.1655381924356334... |
710.1289 | Medium dependence of asphaltene agglomeration inhibitor efficiency | Applying chemical additives (molecule inhibitors or dispersants) is one of
the common ways to control asphaltene agglomeration and precipitation. However,
it is not clear why at some conditions the synthetic flocculation inhibitors as
well as resins not only do not inhibit the asphaltene agglomeration,, they may
also... | cond-mat.soft cond-mat.mtrl-sci | applying chemical additives molecule inhibitors or dispersants is one of the common ways to control asphaltene agglomeration and precipitation however it is not clear why at some conditions the synthetic flocculation inhibitors as well as resins not only do not inhibit the asphaltene agglomeration they may also promote... | [['applying', 'chemical', 'additives', 'molecule', 'inhibitors', 'or', 'dispersants', 'is', 'one', 'of', 'the', 'common', 'ways', 'to', 'control', 'asphaltene', 'agglomeration', 'and', 'precipitation', 'however', 'it', 'is', 'not', 'clear', 'why', 'at', 'some', 'conditions', 'the', 'synthetic', 'flocculation', 'inhibit... | [-0.05892105495979998, 0.15025552642743098, -0.05819644662872974, 0.06533479885958089, -0.015954902387035588, -0.14200824461420256, 0.08267209355353715, 0.409968733970373, -0.24975372502773835, -0.3002655262276073, 0.07508402643582435, -0.2769230064833137, -0.1791800582378623, 0.14171565971922906, -0.07067031901118351,... |
710.129 | Limiting jump conditions for Josephson junctions in Ginzburg-Landau
theory | We consider a superconducting/normal/superconducting Josephson junction
modeled through the Ginzburg-Landau theory. When the normal material is
sufficiently thin and the applied magnetic field is below the critical field of
vortex nucleation, we prove to leading order that jump boundary conditions of
the type predict... | math.AP math-ph math.MP | we consider a superconductingnormalsuperconducting josephson junction modeled through the ginzburglandau theory when the normal material is sufficiently thin and the applied magnetic field is below the critical field of vortex nucleation we prove to leading order that jump boundary conditions of the type predicted by d... | [['we', 'consider', 'a', 'superconductingnormalsuperconducting', 'josephson', 'junction', 'modeled', 'through', 'the', 'ginzburglandau', 'theory', 'when', 'the', 'normal', 'material', 'is', 'sufficiently', 'thin', 'and', 'the', 'applied', 'magnetic', 'field', 'is', 'below', 'the', 'critical', 'field', 'of', 'vortex', '... | [-0.25040636928931165, 0.17110738090167826, -0.05854576528788759, 0.05553939038117488, -0.07718615530757234, -0.1502717631922748, 0.025093375819359116, 0.31916130774726087, -0.25224400139771974, -0.267615496682433, 0.06106592421061718, -0.21586840105457947, -0.11438671671427213, 0.18861279738708758, 0.01994799851224972... |
710.1291 | A viability criterion for modified gravity with an extra force | A recently proposed theory of modified gravity with an explicit ``anomalous''
coupling of the Ricci curvature to matter is discussed, and an inequality is
derived which expresses a necessary and sufficient condition to avoid the
notorius Dolgov-Kawasaki instability.
| gr-qc | a recently proposed theory of modified gravity with an explicit anomalous coupling of the ricci curvature to matter is discussed and an inequality is derived which expresses a necessary and sufficient condition to avoid the notorius dolgovkawasaki instability | [['a', 'recently', 'proposed', 'theory', 'of', 'modified', 'gravity', 'with', 'an', 'explicit', 'anomalous', 'coupling', 'of', 'the', 'ricci', 'curvature', 'to', 'matter', 'is', 'discussed', 'and', 'an', 'inequality', 'is', 'derived', 'which', 'expresses', 'a', 'necessary', 'and', 'sufficient', 'condition', 'to', 'avoi... | [-0.19610091478790384, 0.10430351280484575, -0.13611810682089748, 0.1382640914651691, -0.15820377677477696, -0.1952942516025458, -0.07553133072419646, 0.22786920487477974, -0.23155714621817744, -0.28939735063829936, 0.09648111477695606, -0.19397813089292598, -0.18004221459095543, 0.13502433375027534, -0.100124639584808... |
710.1292 | Relationship between EIT Post Eruption Arcades, Coronal Mass Ejections,
Coronal Neutral Line and Magnetic Clouds | There is observational evidence that the elongation of an Earth directed
coronal mass ejection (CME) may indicate the orientation of the underlying
erupting flux rope. In this study, we compare orientations of CMEs, MCs,
eruption arcades and coronal neutral line (CNL). We report on good correlations
between i) the di... | astro-ph | there is observational evidence that the elongation of an earth directed coronal mass ejection cme may indicate the orientation of the underlying erupting flux rope in this study we compare orientations of cmes mcs eruption arcades and coronal neutral line cnl we report on good correlations between i the directions of ... | [['there', 'is', 'observational', 'evidence', 'that', 'the', 'elongation', 'of', 'an', 'earth', 'directed', 'coronal', 'mass', 'ejection', 'cme', 'may', 'indicate', 'the', 'orientation', 'of', 'the', 'underlying', 'erupting', 'flux', 'rope', 'in', 'this', 'study', 'we', 'compare', 'orientations', 'of', 'cmes', 'mcs', '... | [-0.1747254609130323, 0.21262768514852118, 0.02910978177251915, 0.12525864025965955, -0.10124715480953456, -0.02456455406577637, -0.0020970441369960705, 0.5591942390799522, -0.15030816327780486, -0.34595301194737355, 0.016589889794122428, -0.20963803888725427, -0.13329113950952887, 0.16795933741804522, -0.0349442373805... |
710.1293 | Old stellar counter-rotating components in early-type galaxies from
elliptical-spiral mergers | We investigate, by means of numerical simulations, the possibility of forming
counter-rotating old stellar components by major mergers between an elliptical
and a spiral galaxy. We show that counter-rotation can appear both in
dissipative and dissipationless retrograde mergers, and it is mostly associated
to the pres... | astro-ph | we investigate by means of numerical simulations the possibility of forming counterrotating old stellar components by major mergers between an elliptical and a spiral galaxy we show that counterrotation can appear both in dissipative and dissipationless retrograde mergers and it is mostly associated to the presence of ... | [['we', 'investigate', 'by', 'means', 'of', 'numerical', 'simulations', 'the', 'possibility', 'of', 'forming', 'counterrotating', 'old', 'stellar', 'components', 'by', 'major', 'mergers', 'between', 'an', 'elliptical', 'and', 'a', 'spiral', 'galaxy', 'we', 'show', 'that', 'counterrotation', 'can', 'appear', 'both', 'in... | [-0.2094457026624613, 0.12535057877688482, -0.09027394107331267, 0.04337902588965583, -0.09908256281844595, 0.010721008478536864, -0.04744343071202324, 0.38454173170876776, -0.21494739967271348, -0.31233032371594827, 0.031061189532258802, -0.25456235867221205, -0.09382790111703798, 0.1825560669266534, -0.00827475955752... |
710.1294 | Transition Distribution Amplitudes for gamma* gamma collisions | We study the exclusive production of pi-pi and rho-pi in hard gamma* gamma
scattering in the forward kinematical region where the virtuality of one photon
provides us with a hard scale in the process. The newly introduced concept of
Transition Distribution Amplitudes (TDA) is used to perform a QCD calculation
of thes... | hep-ph hep-ex nucl-th | we study the exclusive production of pipi and rhopi in hard gamma gamma scattering in the forward kinematical region where the virtuality of one photon provides us with a hard scale in the process the newly introduced concept of transition distribution amplitudes tda is used to perform a qcd calculation of these reacti... | [['we', 'study', 'the', 'exclusive', 'production', 'of', 'pipi', 'and', 'rhopi', 'in', 'hard', 'gamma', 'gamma', 'scattering', 'in', 'the', 'forward', 'kinematical', 'region', 'where', 'the', 'virtuality', 'of', 'one', 'photon', 'provides', 'us', 'with', 'a', 'hard', 'scale', 'in', 'the', 'process', 'the', 'newly', 'in... | [-0.048614738402230774, 0.21489269285298446, -0.14199111880734563, 0.14804419541454564, -0.06473990109584787, -0.11716743912821745, 0.08299460599527639, 0.34437618185492125, -0.19680910443558414, -0.18836391171823968, -0.05844560219933662, -0.3553980728556566, 0.023381319329799973, 0.16226056072285727, 0.12433838475296... |
710.1295 | On freely indecomposable measures | We show that a probability measure is not a nontrivial free additive
convolution if it puts no mass in an interval whose endpoints are atoms. The
analogous results for free multiplicative convolutions are proved as well. The
proofs use analytic subordination.
| math.OA math.PR | we show that a probability measure is not a nontrivial free additive convolution if it puts no mass in an interval whose endpoints are atoms the analogous results for free multiplicative convolutions are proved as well the proofs use analytic subordination | [['we', 'show', 'that', 'a', 'probability', 'measure', 'is', 'not', 'a', 'nontrivial', 'free', 'additive', 'convolution', 'if', 'it', 'puts', 'no', 'mass', 'in', 'an', 'interval', 'whose', 'endpoints', 'are', 'atoms', 'the', 'analogous', 'results', 'for', 'free', 'multiplicative', 'convolutions', 'are', 'proved', 'as',... | [-0.10186100912865297, 0.15602539834408827, -0.10457585845142603, 0.17530037936606876, -0.07941637269970847, -0.12426493164697071, 0.02747582250399651, 0.43976036872623897, -0.2846867869176516, -0.173531304249858, 0.11210520445971137, -0.2781703707466765, -0.14497657865285873, 0.2518702993601015, -0.12742520414474534, ... |
710.1296 | Type IIA/M-theory Moduli fixing in a Class of Orientifold Models | We present the study of type II A flux vacua and their M-theory duals for
compactification on a class of Calabi-Yau orientifolds. The Kaehler potential
is derived from toroidal compactifications and the superpotential contains a
contribution from non-Abelian gauge degrees of freedoms. We obtain complete
stabilisation... | hep-th | we present the study of type ii a flux vacua and their mtheory duals for compactification on a class of calabiyau orientifolds the kaehler potential is derived from toroidal compactifications and the superpotential contains a contribution from nonabelian gauge degrees of freedoms we obtain complete stabilisation of the... | [['we', 'present', 'the', 'study', 'of', 'type', 'ii', 'a', 'flux', 'vacua', 'and', 'their', 'mtheory', 'duals', 'for', 'compactification', 'on', 'a', 'class', 'of', 'calabiyau', 'orientifolds', 'the', 'kaehler', 'potential', 'is', 'derived', 'from', 'toroidal', 'compactifications', 'and', 'the', 'superpotential', 'con... | [-0.14686666727842143, 0.1375913603459291, -0.04738271256598334, 0.14018557348948282, -0.09615235168603249, -0.11213127408991568, 0.02406880956647607, 0.2993579125245257, -0.1622845489376535, -0.297668557393384, 0.10236614588551068, -0.2617250454379246, -0.12257317725452595, 0.13292359958092373, -0.12140590563479539, 0... |
710.1297 | The Fossil Phase in the Life of a Galaxy Group | We investigate the origin and evolution of fossil groups in a concordance
LCDM cosmological simulation. We consider haloes with masses between
$(1-5)\times10^{13} \hMsun$ and study the physical mechanisms that lead to the
formation of the large gap in magnitude between the brightest and the second
most bright group m... | astro-ph | we investigate the origin and evolution of fossil groups in a concordance lcdm cosmological simulation we consider haloes with masses between 15times1013 hmsun and study the physical mechanisms that lead to the formation of the large gap in magnitude between the brightest and the second most bright group member which i... | [['we', 'investigate', 'the', 'origin', 'and', 'evolution', 'of', 'fossil', 'groups', 'in', 'a', 'concordance', 'lcdm', 'cosmological', 'simulation', 'we', 'consider', 'haloes', 'with', 'masses', 'between', '15times1013', 'hmsun', 'and', 'study', 'the', 'physical', 'mechanisms', 'that', 'lead', 'to', 'the', 'formation'... | [-0.13170597951133498, 0.15824668312586468, -0.09994318579234421, 0.09888936217473027, -0.07316281735906972, -0.024780537187557745, 0.03803259243617736, 0.39405218956674987, -0.1961623208437541, -0.3591419383982553, 0.09812235176077787, -0.2503332339643322, -0.07572378933508979, 0.18978953293210113, -0.0190511151647908... |
710.1298 | On isogenous principally polarized abelian surfaces | We study a relationship between two genus 2 curves whose jacobians are
isogenous with kernel equal to a maximal isotropic subspace of p-torsion points
with respect to the Weil pairing. For p = 3 we find an explicit relationship
between the set of Weierstrass points of the two curves extending the classical
results of... | math.AG | we study a relationship between two genus 2 curves whose jacobians are isogenous with kernel equal to a maximal isotropic subspace of ptorsion points with respect to the weil pairing for p 3 we find an explicit relationship between the set of weierstrass points of the two curves extending the classical results of f ric... | [['we', 'study', 'a', 'relationship', 'between', 'two', 'genus', '2', 'curves', 'whose', 'jacobians', 'are', 'isogenous', 'with', 'kernel', 'equal', 'to', 'a', 'maximal', 'isotropic', 'subspace', 'of', 'ptorsion', 'points', 'with', 'respect', 'to', 'the', 'weil', 'pairing', 'for', 'p', '3', 'we', 'find', 'an', 'explici... | [-0.19402222296652885, 0.07131697212619026, -0.12288027484543049, 0.08337575294650518, -0.06645991779290712, -0.15749110345943615, 0.03850242698099464, 0.33479902354570534, -0.2878247159891404, -0.26193962695811374, 0.03236055515276698, -0.3304964978606082, -0.1316604232093176, 0.23699703944417147, -0.09641133479487438... |
710.1299 | Kaluza-Klein relics from warped reheating | It has been suggested that after brane-antibrane inflation in a
Klebanov-Strassler (KS) warped throat, metastable Kaluza-Klein (KK) excitations
can be formed due to nearly-conserved angular momenta along isometric
directions in the throat. If sufficiently long-lived, these relics could
conflict with big bang nucleosy... | hep-th | it has been suggested that after braneantibrane inflation in a klebanovstrassler ks warped throat metastable kaluzaklein kk excitations can be formed due to nearlyconserved angular momenta along isometric directions in the throat if sufficiently longlived these relics could conflict with big bang nucleosynthesis or bar... | [['it', 'has', 'been', 'suggested', 'that', 'after', 'braneantibrane', 'inflation', 'in', 'a', 'klebanovstrassler', 'ks', 'warped', 'throat', 'metastable', 'kaluzaklein', 'kk', 'excitations', 'can', 'be', 'formed', 'due', 'to', 'nearlyconserved', 'angular', 'momenta', 'along', 'isometric', 'directions', 'in', 'the', 't... | [-0.1339375776406251, 0.17901634870206873, -0.08632730259201847, 0.16053778900210725, -0.12273525137336276, -0.12091335682177334, 0.003305581339837233, 0.30430554164830614, -0.19504724246000965, -0.2947055257622962, 0.1156506132523053, -0.24395834268660735, -0.023072378086484546, 0.14055652187913825, -0.022327837910886... |
710.13 | Massive Quark-Gluon Scattering Amplitudes at Tree Level | Results for four-, five-, and six-parton tree amplitudes for massive
quark-antiquark scattering with gluons are calculated using the recursion
relations of Britto, Cachazo, Feng, and Witten. The required diagrams are
generated using shifts of the momenta of a pair of massless legs to complex
values. Checks verifying ... | hep-ph | results for four five and sixparton tree amplitudes for massive quarkantiquark scattering with gluons are calculated using the recursion relations of britto cachazo feng and witten the required diagrams are generated using shifts of the momenta of a pair of massless legs to complex values checks verifying the calculati... | [['results', 'for', 'four', 'five', 'and', 'sixparton', 'tree', 'amplitudes', 'for', 'massive', 'quarkantiquark', 'scattering', 'with', 'gluons', 'are', 'calculated', 'using', 'the', 'recursion', 'relations', 'of', 'britto', 'cachazo', 'feng', 'and', 'witten', 'the', 'required', 'diagrams', 'are', 'generated', 'using',... | [-0.1633585793315433, 0.2555785627939713, -0.08555834836442955, 0.15361358261179703, -0.08225392888198257, -0.09999118575069588, 0.033155800512759015, 0.3500220085843466, -0.12386222038185224, -0.2831807656621095, -0.005050589834354469, -0.3168448818178149, -0.11402117148099933, 0.2039002616184007, 0.04858547283220105,... |
710.1301 | Fault-tolerant quantum computation against biased noise | We formulate a scheme for fault-tolerant quantum computation that works
effectively against highly biased noise, where dephasing is far stronger than
all other types of noise. In our scheme, the fundamental operations performed
by the quantum computer are single-qubit preparations, single-qubit
measurements, and cond... | quant-ph cond-mat.mes-hall cond-mat.supr-con | we formulate a scheme for faulttolerant quantum computation that works effectively against highly biased noise where dephasing is far stronger than all other types of noise in our scheme the fundamental operations performed by the quantum computer are singlequbit preparations singlequbit measurements and conditionalpha... | [['we', 'formulate', 'a', 'scheme', 'for', 'faulttolerant', 'quantum', 'computation', 'that', 'works', 'effectively', 'against', 'highly', 'biased', 'noise', 'where', 'dephasing', 'is', 'far', 'stronger', 'than', 'all', 'other', 'types', 'of', 'noise', 'in', 'our', 'scheme', 'the', 'fundamental', 'operations', 'perform... | [-0.1531683419361315, 0.18058077968343828, -0.006885443179480797, 0.043432385591682936, 0.05968499102885217, -0.22373699310721945, 0.12617007991818266, 0.3830567150648716, -0.19714641277637102, -0.3277178551111601, 0.07807194081905702, -0.24112003783291552, -0.12137844448134436, 0.3002803698676614, -0.08015471006964078... |
710.1302 | Enhanced Non-Gaussianity from Excited Initial States | We use the techniques of effective field theory in an expanding universe to
examine the effect of choosing an excited inflationary initial state built over
the Bunch-Davies state on the CMB bi-spectrum. We find that even for Hadamard
states, there are unexpected enhancements in the bi-spectrum for certain
configurati... | hep-th astro-ph gr-qc | we use the techniques of effective field theory in an expanding universe to examine the effect of choosing an excited inflationary initial state built over the bunchdavies state on the cmb bispectrum we find that even for hadamard states there are unexpected enhancements in the bispectrum for certain configurations in ... | [['we', 'use', 'the', 'techniques', 'of', 'effective', 'field', 'theory', 'in', 'an', 'expanding', 'universe', 'to', 'examine', 'the', 'effect', 'of', 'choosing', 'an', 'excited', 'inflationary', 'initial', 'state', 'built', 'over', 'the', 'bunchdavies', 'state', 'on', 'the', 'cmb', 'bispectrum', 'we', 'find', 'that', ... | [-0.15079369785216373, 0.20774909249495946, -0.11421869296240263, 0.1290033745746582, -0.03638800378872925, -0.08898383799669707, -0.05921398902920863, 0.36028812343700445, -0.2322882470350442, -0.2935993459561251, 0.07496875681532308, -0.2930145177146436, -0.07586587300826596, 0.19714830433512026, 0.018026915999750297... |
710.1303 | Testing Reionization with Gamma Ray Burst Absorption Spectra | We propose to study cosmic reionization using absorption line spectra of
high-redshift Gamma Ray Burst (GRB) afterglows. We show that the statistics of
the dark portions (gaps) in GRB absorption spectra represent exquisite tools to
discriminate among different reionization models. We then compute the
probability to f... | astro-ph | we propose to study cosmic reionization using absorption line spectra of highredshift gamma ray burst grb afterglows we show that the statistics of the dark portions gaps in grb absorption spectra represent exquisite tools to discriminate among different reionization models we then compute the probability to find the l... | [['we', 'propose', 'to', 'study', 'cosmic', 'reionization', 'using', 'absorption', 'line', 'spectra', 'of', 'highredshift', 'gamma', 'ray', 'burst', 'grb', 'afterglows', 'we', 'show', 'that', 'the', 'statistics', 'of', 'the', 'dark', 'portions', 'gaps', 'in', 'grb', 'absorption', 'spectra', 'represent', 'exquisite', 't... | [-0.04725637389851891, 0.12217957614607203, -0.03456966363802463, 0.14058333880153023, -0.08717278120702648, -0.1207540414256818, 0.08398886421325066, 0.5037080321730261, -0.15273717368100154, -0.32959964954720655, -0.03699806958075097, -0.3087251615901309, 0.002455883081553571, 0.19963555889770793, 0.05816623504755165... |
710.1304 | Balanced metrics and noncommutative Kaehler geometry | In this paper we show how Einstein metrics are naturally described using the
quantization of the algebra of functions on a Kahler manifold M. In this setup
one interprets M as the phase space itself, equipped with the Poisson brackets
inherited from the Kahler 2-form. We compare the geometric quantization
framework w... | hep-th math-ph math.DG math.MP | in this paper we show how einstein metrics are naturally described using the quantization of the algebra of functions on a kahler manifold m in this setup one interprets m as the phase space itself equipped with the poisson brackets inherited from the kahler 2form we compare the geometric quantization framework with se... | [['in', 'this', 'paper', 'we', 'show', 'how', 'einstein', 'metrics', 'are', 'naturally', 'described', 'using', 'the', 'quantization', 'of', 'the', 'algebra', 'of', 'functions', 'on', 'a', 'kahler', 'manifold', 'm', 'in', 'this', 'setup', 'one', 'interprets', 'm', 'as', 'the', 'phase', 'space', 'itself', 'equipped', 'wi... | [-0.1740259014738676, 0.06626065396484879, -0.08511570478494987, 0.12056692314043672, -0.09612881496317811, -0.12763090725415027, -0.025805516085889924, 0.3504101587738046, -0.25278741832918084, -0.2526094025701412, 0.08612266424983644, -0.23222390187179875, -0.2444133168627691, 0.179221216798163, -0.17464137229168963,... |
710.1305 | Unique continuation results for Ricci curvature and applications | Unique continuation results are proved for metrics with prescribed Ricci
curvature in the setting of bounded metrics on compact manifolds with boundary,
and in the setting of complete, conformally compact metrics. Related to this
issue, an isometry extension property is proved: continuous groups of
isometries at conf... | math.DG | unique continuation results are proved for metrics with prescribed ricci curvature in the setting of bounded metrics on compact manifolds with boundary and in the setting of complete conformally compact metrics related to this issue an isometry extension property is proved continuous groups of isometries at conformal i... | [['unique', 'continuation', 'results', 'are', 'proved', 'for', 'metrics', 'with', 'prescribed', 'ricci', 'curvature', 'in', 'the', 'setting', 'of', 'bounded', 'metrics', 'on', 'compact', 'manifolds', 'with', 'boundary', 'and', 'in', 'the', 'setting', 'of', 'complete', 'conformally', 'compact', 'metrics', 'related', 'to... | [-0.17970865286004387, 0.06926012341730377, -0.08175752115877051, 0.06939361784086366, -0.14805923385153474, -0.14856024338912807, -0.10639280747426183, 0.36684976206896336, -0.21965647986354797, -0.1806290091848687, 0.14331045889795, -0.2919861565858714, -0.1313284956727569, 0.1664094965243222, -0.1483727303964674, 0.... |
710.1306 | Strain-induced insulator state in La_0.7Sr_0.3CoO_3 | We report on the observation of a strain-induced insulator state in
ferromagnetic La_0.7Sr_0.3CoO_3 films. Tensile strain above 1% is found to
enhance the resistivity by several orders of magnitude. Reversible strain of
0.15% applied using a piezoelectric substrate triggers huge resistance
modulations, including a ch... | cond-mat.str-el cond-mat.mtrl-sci | we report on the observation of a straininduced insulator state in ferromagnetic la_07sr_03coo_3 films tensile strain above 1 is found to enhance the resistivity by several orders of magnitude reversible strain of 015 applied using a piezoelectric substrate triggers huge resistance modulations including a change by a f... | [['we', 'report', 'on', 'the', 'observation', 'of', 'a', 'straininduced', 'insulator', 'state', 'in', 'ferromagnetic', 'la_07sr_03coo_3', 'films', 'tensile', 'strain', 'above', '1', 'is', 'found', 'to', 'enhance', 'the', 'resistivity', 'by', 'several', 'orders', 'of', 'magnitude', 'reversible', 'strain', 'of', '015', '... | [-0.18278557621766772, 0.20942932145324417, 0.018089238945724426, -0.012761653638939349, -0.0016106775492034128, -0.07917770414934618, 0.12695485914941976, 0.39754045260163534, -0.30695303004910857, -0.3086194842476892, 0.007082668766667819, -0.31004692755837354, -0.0721552564630664, 0.18443017171085935, 0.075657716853... |
710.1307 | Common Markets, Strong Currencies & the Collective Welfare | The so called "globalization" process (i.e. the inexorable integration of
markets, currencies, nation-states, technologies and the intensification of
consciousness of the world as a whole) has a behavior exactly equivalent to a
system that is tending to a maximum entropy state. This globalization process
obeys a coll... | q-fin.GN physics.soc-ph | the so called globalization process ie the inexorable integration of markets currencies nationstates technologies and the intensification of consciousness of the world as a whole has a behavior exactly equivalent to a system that is tending to a maximum entropy state this globalization process obeys a collective welfar... | [['the', 'so', 'called', 'globalization', 'process', 'ie', 'the', 'inexorable', 'integration', 'of', 'markets', 'currencies', 'nationstates', 'technologies', 'and', 'the', 'intensification', 'of', 'consciousness', 'of', 'the', 'world', 'as', 'a', 'whole', 'has', 'a', 'behavior', 'exactly', 'equivalent', 'to', 'a', 'sys... | [-0.12751248859179518, 0.10091443068813533, -0.10034192467768056, 0.07068951505270889, -0.03442443124561881, -0.12997581653762608, 0.12531393033568747, 0.3178323547821492, -0.32061270806007086, -0.24489073686224097, 0.13387771699247727, -0.3060345948673785, -0.11987264027896648, 0.10617599204803506, -0.0859996155282715... |
710.1308 | Scaling Laws for NanoFET Sensors | The sensitive conductance change of semiconductor nanowires and carbon
nanotubes in response to binding of charged molecules provide a novel sensing
modality which is generally denoted as nanoFET sensors. In this paper, we study
the scaling laws of nanoplate FET sensors by simplifying nanoplates as random
resistor ne... | cond-mat.mtrl-sci cond-mat.stat-mech | the sensitive conductance change of semiconductor nanowires and carbon nanotubes in response to binding of charged molecules provide a novel sensing modality which is generally denoted as nanofet sensors in this paper we study the scaling laws of nanoplate fet sensors by simplifying nanoplates as random resistor networ... | [['the', 'sensitive', 'conductance', 'change', 'of', 'semiconductor', 'nanowires', 'and', 'carbon', 'nanotubes', 'in', 'response', 'to', 'binding', 'of', 'charged', 'molecules', 'provide', 'a', 'novel', 'sensing', 'modality', 'which', 'is', 'generally', 'denoted', 'as', 'nanofet', 'sensors', 'in', 'this', 'paper', 'we'... | [-0.1634896989035908, 0.1911215185295337, 0.01489727267818082, -0.011385259076459556, 0.0015553412972838573, -0.21173681025227, 0.08680992476417616, 0.4108335743935424, -0.2090280955723886, -0.32465760383222786, 0.025867303944930125, -0.30064083774673883, -0.15149336290085644, 0.1959188714196595, -0.04340881204310184, ... |
710.1309 | Correspondence between Andreev reflection and Klein tunneling in bipolar
graphene | Andreev reflection at a superconductor and Klein tunneling through an n-p
junction in graphene are two processes that couple electrons to holes -- the
former through the superconducting pair potential Delta and the latter through
the electrostatic potential U. We derive that the energy spectra in the two
systems are ... | cond-mat.mes-hall | andreev reflection at a superconductor and klein tunneling through an np junction in graphene are two processes that couple electrons to holes the former through the superconducting pair potential delta and the latter through the electrostatic potential u we derive that the energy spectra in the two systems are identic... | [['andreev', 'reflection', 'at', 'a', 'superconductor', 'and', 'klein', 'tunneling', 'through', 'an', 'np', 'junction', 'in', 'graphene', 'are', 'two', 'processes', 'that', 'couple', 'electrons', 'to', 'holes', 'the', 'former', 'through', 'the', 'superconducting', 'pair', 'potential', 'delta', 'and', 'the', 'latter', '... | [-0.21138626133853738, 0.1690647162478523, -0.056583292469043624, 0.05411767448531464, 0.007827800313349474, -0.19829806467856873, 0.06830728227611292, 0.39434453072873027, -0.23943311201450837, -0.28439544838937847, -0.052132785007018935, -0.3502095290375027, -0.10924070238305086, 0.19338334300766952, 0.06766254059039... |
710.131 | EVLA Observations of OH Masers in ON 1 | This Letter reports on initial Expanded Very Large Array (EVLA) observations
of the 6035 MHz masers in ON 1. The EVLA data are of good quality, lending
confidence in the new receiver system. Nineteen maser features, including six
Zeeman pairs, are detected. The overall distribution of 6035 MHz OH masers is
similar to... | astro-ph | this letter reports on initial expanded very large array evla observations of the 6035 mhz masers in on 1 the evla data are of good quality lending confidence in the new receiver system nineteen maser features including six zeeman pairs are detected the overall distribution of 6035 mhz oh masers is similar to that of t... | [['this', 'letter', 'reports', 'on', 'initial', 'expanded', 'very', 'large', 'array', 'evla', 'observations', 'of', 'the', '6035', 'mhz', 'masers', 'in', 'on', '1', 'the', 'evla', 'data', 'are', 'of', 'good', 'quality', 'lending', 'confidence', 'in', 'the', 'new', 'receiver', 'system', 'nineteen', 'maser', 'features', ... | [-0.14149122755081006, 0.08158260178087014, 0.024811742512823698, 0.007729047536698787, -0.07305454181857987, -0.09790219827600477, 0.016184008441405832, 0.4694115710626175, -0.1797529988220663, -0.29685503140986935, 0.04775668201399604, -0.2324275836384819, 0.0045193553805448015, 0.15869091596006862, 0.019605794425618... |
710.1311 | The star formation histories of early-type galaxies: insights from the
rest-frame ultra-violet | Our current understanding of the star formation histories of early-type
galaxies is reviewed, in the context of recent observational studies of their
ultra-violet (UV) properties. Combination of UV and optical spectro-photometric
data indicates that the bulk of the stellar mass in the early-type population
forms at h... | astro-ph | our current understanding of the star formation histories of earlytype galaxies is reviewed in the context of recent observational studies of their ultraviolet uv properties combination of uv and optical spectrophotometric data indicates that the bulk of the stellar mass in the earlytype population forms at high redshi... | [['our', 'current', 'understanding', 'of', 'the', 'star', 'formation', 'histories', 'of', 'earlytype', 'galaxies', 'is', 'reviewed', 'in', 'the', 'context', 'of', 'recent', 'observational', 'studies', 'of', 'their', 'ultraviolet', 'uv', 'properties', 'combination', 'of', 'uv', 'and', 'optical', 'spectrophotometric', 'd... | [-0.03860878532895402, 0.15011687240473806, -0.028578183006230495, 0.10012284440264994, -0.04565868029302355, 0.0007971978751082105, 0.03459827972547657, 0.45930109560716575, -0.10212804576521503, -0.3924323426852674, 0.025960070432664892, -0.3044972118672201, 0.03721397471505449, 0.1858821166018333, -0.051345504732887... |
710.1312 | On Braid Excitations in Quantum Gravity | We propose a new notation for the states in some models of quantum gravity,
namely 4-valent spin networks embedded in a topological three manifold. With
the help of this notation, equivalence moves, namely translations and
rotations, can be defined, which relate the projections of diffeomorphic
embeddings of a spin n... | hep-th gr-qc math-ph math.MP | we propose a new notation for the states in some models of quantum gravity namely 4valent spin networks embedded in a topological three manifold with the help of this notation equivalence moves namely translations and rotations can be defined which relate the projections of diffeomorphic embeddings of a spin network ce... | [['we', 'propose', 'a', 'new', 'notation', 'for', 'the', 'states', 'in', 'some', 'models', 'of', 'quantum', 'gravity', 'namely', '4valent', 'spin', 'networks', 'embedded', 'in', 'a', 'topological', 'three', 'manifold', 'with', 'the', 'help', 'of', 'this', 'notation', 'equivalence', 'moves', 'namely', 'translations', 'a... | [-0.19791191929834895, 0.17038343614479015, -0.06405482216031996, 0.0752433286570422, -0.05752684949682309, -0.173411844313595, 0.00503055930552124, 0.3386665591970086, -0.28965955890796996, -0.2871921198790545, 0.05194620882892715, -0.25161866094036905, -0.19283909608538335, 0.1346056462460003, -0.08799518501529327, 0... |
710.1313 | Semi--vector spaces and units of measurement | This paper is aimed at introducing an algebraic model for physical scales and
units of measurement. This goal is achieved by means of the concept of
``positive space'' and its rational powers. Positive spaces are 1-dimensional
``semi-vector spaces'' without the zero vector. A direct approach to this
subject might be ... | math.AC math-ph math.MP | this paper is aimed at introducing an algebraic model for physical scales and units of measurement this goal is achieved by means of the concept of positive space and its rational powers positive spaces are 1dimensional semivector spaces without the zero vector a direct approach to this subject might be sufficient on t... | [['this', 'paper', 'is', 'aimed', 'at', 'introducing', 'an', 'algebraic', 'model', 'for', 'physical', 'scales', 'and', 'units', 'of', 'measurement', 'this', 'goal', 'is', 'achieved', 'by', 'means', 'of', 'the', 'concept', 'of', 'positive', 'space', 'and', 'its', 'rational', 'powers', 'positive', 'spaces', 'are', '1dime... | [-0.12346200007390008, 0.10837038656911994, -0.07938266119021362, 0.0851153520809536, -0.11471455908520559, -0.0943878467392539, 0.02552310182956105, 0.31573411772044097, -0.33078077090162356, -0.24521898317657642, 0.12134864859064563, -0.24536423740364546, -0.14936415978863968, 0.19902835265049232, -0.0980624974730004... |
710.1314 | An exact solution to the temperature equation in a column of ice and
bedrock | We construct a solution of a pure conduction problem in ice and bedrock. This
solution is suitable for, and is used in this paper for, verifying a numerical
scheme for conservation of energy. This exact solution forms one of a suite of
verification tests for PISM (Parallel Ice Sheet Model;
https://gna.org/projects/pi... | physics.geo-ph | we construct a solution of a pure conduction problem in ice and bedrock this solution is suitable for and is used in this paper for verifying a numerical scheme for conservation of energy this exact solution forms one of a suite of verification tests for pism parallel ice sheet model httpsgnaorgprojectspism | [['we', 'construct', 'a', 'solution', 'of', 'a', 'pure', 'conduction', 'problem', 'in', 'ice', 'and', 'bedrock', 'this', 'solution', 'is', 'suitable', 'for', 'and', 'is', 'used', 'in', 'this', 'paper', 'for', 'verifying', 'a', 'numerical', 'scheme', 'for', 'conservation', 'of', 'energy', 'this', 'exact', 'solution', 'f... | [-0.12502236265689134, -0.0011070916242897511, -0.0915586810465902, 0.04354960885597393, -0.01898979187011719, -0.1356730154529214, 0.05373190726386383, 0.30010378286242484, -0.24971476763486863, -0.2925891001150012, 0.15863277446944266, -0.23539516983553768, -0.12350731074810029, 0.20170172743033618, 0.002279041968286... |
710.1315 | Renormalization group flow of quartic perturbations in graphene: Strong
coupling and large-N limits | We explore the renormalization group flow of quartic perturbations in the
low-energy theory of graphene, in the strong Coulomb coupling and large-N
limits, where N is the number of fermion flavors. We compute the anomalous
dimensions of the quartic couplings u up to next-to-leading order in 1/N and
find both relevant... | cond-mat.str-el hep-th | we explore the renormalization group flow of quartic perturbations in the lowenergy theory of graphene in the strong coulomb coupling and largen limits where n is the number of fermion flavors we compute the anomalous dimensions of the quartic couplings u up to nexttoleading order in 1n and find both relevant and irrel... | [['we', 'explore', 'the', 'renormalization', 'group', 'flow', 'of', 'quartic', 'perturbations', 'in', 'the', 'lowenergy', 'theory', 'of', 'graphene', 'in', 'the', 'strong', 'coulomb', 'coupling', 'and', 'largen', 'limits', 'where', 'n', 'is', 'the', 'number', 'of', 'fermion', 'flavors', 'we', 'compute', 'the', 'anomalo... | [-0.20583319722855878, 0.21890835233757067, -0.007857533740914531, 0.07262174051235586, -0.028176747954502288, -0.11908541004069978, 0.065833536136779, 0.30232576301528347, -0.22178053012531665, -0.2663748438418325, -0.009444167333034178, -0.3482209199056443, -0.16359451271839337, 0.10507696075364947, 0.080635473675404... |
710.1316 | Elliptic nets and elliptic curves | An elliptic divisibility sequence is an integer recurrence sequence
associated to an elliptic curve over the rationals together with a rational
point on that curve. In this paper we present a higher-dimensional analogue
over arbitrary base fields. Suppose E is an elliptic curve over a field K, and
P_1, ..., P_n are p... | math.NT | an elliptic divisibility sequence is an integer recurrence sequence associated to an elliptic curve over the rationals together with a rational point on that curve in this paper we present a higherdimensional analogue over arbitrary base fields suppose e is an elliptic curve over a field k and p_1 p_n are points on e d... | [['an', 'elliptic', 'divisibility', 'sequence', 'is', 'an', 'integer', 'recurrence', 'sequence', 'associated', 'to', 'an', 'elliptic', 'curve', 'over', 'the', 'rationals', 'together', 'with', 'a', 'rational', 'point', 'on', 'that', 'curve', 'in', 'this', 'paper', 'we', 'present', 'a', 'higherdimensional', 'analogue', '... | [-0.251263373315659, 0.06113901388603946, -0.12430334411595666, 0.019990905005390833, -0.09205874006067394, -0.12327805064071756, -0.003837738407203295, 0.374457090238639, -0.34494846377419225, -0.22372871220064855, 0.05471204456001725, -0.346179326111878, -0.1269712819068462, 0.28034951872781877, -0.14544487156725805,... |
710.1317 | Monitoring noise-resonant effects in cancer growth influenced by
external fluctuations and periodic treatment | In the paper we investigate a mathematical model describing the growth of
tumor in the presence of immune response of a host organism. The dynamics of
tumor and immune cells is based on the generic Michaelis-Menten kinetics
depicting interaction and competition between the tumor and the immune system.
The appropriate... | physics.bio-ph physics.med-ph | in the paper we investigate a mathematical model describing the growth of tumor in the presence of immune response of a host organism the dynamics of tumor and immune cells is based on the generic michaelismenten kinetics depicting interaction and competition between the tumor and the immune system the appropriate phen... | [['in', 'the', 'paper', 'we', 'investigate', 'a', 'mathematical', 'model', 'describing', 'the', 'growth', 'of', 'tumor', 'in', 'the', 'presence', 'of', 'immune', 'response', 'of', 'a', 'host', 'organism', 'the', 'dynamics', 'of', 'tumor', 'and', 'immune', 'cells', 'is', 'based', 'on', 'the', 'generic', 'michaelismenten... | [-0.12927005580608167, 0.11262951179586725, -0.06371930861370821, 0.06908516701100868, -0.014035404882594651, -0.13563610883794872, 0.05459451495770219, 0.3015860997879987, -0.25649975121532587, -0.26478888513885585, 0.07474709975752322, -0.25875665284145405, -0.2035482067213047, 0.17423590811416872, -0.075486486317480... |
710.1318 | New Model Atmospheres: Testing the Solar Spectrum in the UV | We present preliminary results on the calculation of synthetic spectra
obtained with the stellar model atmospheres developed by Cardona, Crivellari,
and Simonneau. These new models have been used as input within the SYNTHE
series of codes developed by Kurucz. As a first step we have tested if SYNTHE
is able to handle... | astro-ph | we present preliminary results on the calculation of synthetic spectra obtained with the stellar model atmospheres developed by cardona crivellari and simonneau these new models have been used as input within the synthe series of codes developed by kurucz as a first step we have tested if synthe is able to handle these... | [['we', 'present', 'preliminary', 'results', 'on', 'the', 'calculation', 'of', 'synthetic', 'spectra', 'obtained', 'with', 'the', 'stellar', 'model', 'atmospheres', 'developed', 'by', 'cardona', 'crivellari', 'and', 'simonneau', 'these', 'new', 'models', 'have', 'been', 'used', 'as', 'input', 'within', 'the', 'synthe',... | [0.02664252700499044, 0.08748223576694727, -0.09128935181607421, 0.08036911372596828, 0.0016370878053399232, -0.12353098866744683, 0.03540980204975663, 0.4128096163559418, -0.2143990317073006, -0.38451177218499094, 0.09845848987864043, -0.24957789006786277, -0.10740467149298638, 0.2342998087621079, -0.02457765304828241... |
710.1319 | The non-existence of certain mod 2 Galois representations of some small
quadratic fields | For a few quadratic fields, the non-existence is proved of continuous
irreducible mod 2 Galois representations of degree 2 unramified outside 2.
| math.NT | for a few quadratic fields the nonexistence is proved of continuous irreducible mod 2 galois representations of degree 2 unramified outside 2 | [['for', 'a', 'few', 'quadratic', 'fields', 'the', 'nonexistence', 'is', 'proved', 'of', 'continuous', 'irreducible', 'mod', '2', 'galois', 'representations', 'of', 'degree', '2', 'unramified', 'outside', '2']] | [-0.2870166904546998, 0.09796970811757175, -0.07936371395110407, 0.04289149855454029, -0.08597919522699984, -0.16954269613647324, -0.10033534551885995, 0.25384727808308194, -0.36218911028382456, -0.23094968684017658, 0.09684148521839896, -0.24082703329622746, -0.10341817372351546, 0.1991558976217427, -0.106372751591896... |
710.132 | Measurements in the L\'{e}vy quantum walk | We study the quantum walk subjected to measurements with a L\'evy
waiting-time distribution. We find that the system has a sub-ballistic behavior
instead of a diffusive one. We obtain an analytical expression for the exponent
of the power law of the variance as a function of the characteristic parameter
of the L\'evy... | quant-ph | we study the quantum walk subjected to measurements with a levy waitingtime distribution we find that the system has a subballistic behavior instead of a diffusive one we obtain an analytical expression for the exponent of the power law of the variance as a function of the characteristic parameter of the levy distribut... | [['we', 'study', 'the', 'quantum', 'walk', 'subjected', 'to', 'measurements', 'with', 'a', 'levy', 'waitingtime', 'distribution', 'we', 'find', 'that', 'the', 'system', 'has', 'a', 'subballistic', 'behavior', 'instead', 'of', 'a', 'diffusive', 'one', 'we', 'obtain', 'an', 'analytical', 'expression', 'for', 'the', 'expo... | [-0.14502946368225342, 0.1363481210376123, -0.19632620325768893, 0.04425691581278477, -0.013051364453342516, -0.1443397009147788, 0.0582370010033285, 0.3199756978395975, -0.26038663215794655, -0.21801934180394658, 0.06016256687459799, -0.2946339617922621, -0.16748531377118714, 0.21659063983638333, -0.013091646626872837... |
710.1321 | Unification with and without Supersymmetry: Adjoint SU(5) | I present two new renormalizable grand unified theories where the neutrino
masses are generated through the type I and type III seesaw mechanisms. These
theories can be considered as the simplest (SUSY) renormalizable grand unified
theories based on the SU(5) gauge symmetry. Several phenomenological and
cosmological ... | hep-ph | i present two new renormalizable grand unified theories where the neutrino masses are generated through the type i and type iii seesaw mechanisms these theories can be considered as the simplest susy renormalizable grand unified theories based on the su5 gauge symmetry several phenomenological and cosmological aspects ... | [['i', 'present', 'two', 'new', 'renormalizable', 'grand', 'unified', 'theories', 'where', 'the', 'neutrino', 'masses', 'are', 'generated', 'through', 'the', 'type', 'i', 'and', 'type', 'iii', 'seesaw', 'mechanisms', 'these', 'theories', 'can', 'be', 'considered', 'as', 'the', 'simplest', 'susy', 'renormalizable', 'gra... | [-0.07644023864458387, 0.23533705493005422, 0.006760651693464472, 0.24819220409083825, -0.1024125811840909, -0.26411406964493483, -0.04203598010085093, 0.3302203341602133, -0.1608337007033137, -0.25090310360806495, 0.06220024234901827, -0.18279302827655697, -0.14329838395441094, 0.10063043415832978, -0.0068015672194843... |
710.1322 | Effects of the disconnected flavor singlet corrections on the hyperfine
splitting in charmonium | Experimentally the charmonium hyperfine splitting is
$M_{J/\psi}-M_{\eta_c}=117$ MeV and current lattice results are generally below
this value. The difference could be due to the effects of the disconnected
flavor singlet diagrams which have not been included in these calculations.
Previous attempts to determine the... | hep-lat | experimentally the charmonium hyperfine splitting is m_jpsim_eta_c117 mev and current lattice results are generally below this value the difference could be due to the effects of the disconnected flavor singlet diagrams which have not been included in these calculations previous attempts to determine the disconnected f... | [['experimentally', 'the', 'charmonium', 'hyperfine', 'splitting', 'is', 'm_jpsim_eta_c117', 'mev', 'and', 'current', 'lattice', 'results', 'are', 'generally', 'below', 'this', 'value', 'the', 'difference', 'could', 'be', 'due', 'to', 'the', 'effects', 'of', 'the', 'disconnected', 'flavor', 'singlet', 'diagrams', 'whic... | [-0.055976765605098594, 0.29964232105171174, -0.04066879708865067, 0.11620718600773593, -0.03724386921030379, -0.09007057272715539, 0.11481759370952027, 0.4476359485444136, -0.12949021984028017, -0.3234917550694152, 0.04701384429808524, -0.3188657810025644, 0.023888737781018746, 0.12716490087928478, 0.02769395622720078... |
710.1323 | Dedekind-Carlitz Polynomials as Lattice-Point Enumerators in Rational
Polyhedra | We study higher-dimensional analogs of the Dedekind-Carlitz polynomials
c(u,v;a,b) := sum_{k=1..b-1} u^[ka/b] v^(k-1), where u and v are indeterminates
and a and b are positive integers. Carlitz proved that these polynomials
satisfy the reciprocity law (v-1) c(u,v;a,b) + (u-1) c(v,u;b,a) = u^(a-1)
v^(b-1) - 1, from w... | math.NT math.CO | we study higherdimensional analogs of the dedekindcarlitz polynomials cuvab sum_k1b1 ukab vk1 where u and v are indeterminates and a and b are positive integers carlitz proved that these polynomials satisfy the reciprocity law v1 cuvab u1 cvuba ua1 vb1 1 from which one easily deduces many classical reciprocity theorems... | [['we', 'study', 'higherdimensional', 'analogs', 'of', 'the', 'dedekindcarlitz', 'polynomials', 'cuvab', 'sum_k1b1', 'ukab', 'vk1', 'where', 'u', 'and', 'v', 'are', 'indeterminates', 'and', 'a', 'and', 'b', 'are', 'positive', 'integers', 'carlitz', 'proved', 'that', 'these', 'polynomials', 'satisfy', 'the', 'reciprocit... | [-0.16865264874124983, 0.05441136693553929, -0.11144365156943402, 0.09183614975440182, -0.10864888865122557, -0.1580285904929042, 0.028464763372772393, 0.2537956436049137, -0.3304436841237366, -0.19438710055905709, 0.07682638451600574, -0.2672153186977358, -0.20090429504451, 0.20645848894141672, -0.12501635680437312, 0... |
710.1324 | Traces of heat operators on Riemannian foliations | We consider the basic heat operator on functions on a Riemannian foliation of
a compact, Riemannian manifold, and we show that the trace of this operator has
a particular short time asymptotic expansion. The coefficients in this
expansion are obtainable from local transverse geometric invariants - functions
computabl... | math.DG | we consider the basic heat operator on functions on a riemannian foliation of a compact riemannian manifold and we show that the trace of this operator has a particular short time asymptotic expansion the coefficients in this expansion are obtainable from local transverse geometric invariants functions computable by an... | [['we', 'consider', 'the', 'basic', 'heat', 'operator', 'on', 'functions', 'on', 'a', 'riemannian', 'foliation', 'of', 'a', 'compact', 'riemannian', 'manifold', 'and', 'we', 'show', 'that', 'the', 'trace', 'of', 'this', 'operator', 'has', 'a', 'particular', 'short', 'time', 'asymptotic', 'expansion', 'the', 'coefficien... | [-0.18476481580776033, 0.065136247611671, -0.11071402105180739, 0.10732583094183704, -0.09001345514694106, -0.07898304861683016, -0.03332428874395718, 0.3175141015829884, -0.29158056862043025, -0.18009783032950816, 0.14042683007743942, -0.27921404929997, -0.18035486201259576, 0.19647249856215215, -0.07925896946760765, ... |
710.1325 | The MIMOME Channel | The MIMOME channel is a Gaussian wiretap channel in which the sender,
receiver, and eavesdropper all have multiple antennas. We characterize the
secrecy capacity as the saddle-value of a minimax problem. Among other
implications, our result establishes that a Gaussian distribution maximizes the
secrecy capacity chara... | cs.IT math.IT | the mimome channel is a gaussian wiretap channel in which the sender receiver and eavesdropper all have multiple antennas we characterize the secrecy capacity as the saddlevalue of a minimax problem among other implications our result establishes that a gaussian distribution maximizes the secrecy capacity characterizat... | [['the', 'mimome', 'channel', 'is', 'a', 'gaussian', 'wiretap', 'channel', 'in', 'which', 'the', 'sender', 'receiver', 'and', 'eavesdropper', 'all', 'have', 'multiple', 'antennas', 'we', 'characterize', 'the', 'secrecy', 'capacity', 'as', 'the', 'saddlevalue', 'of', 'a', 'minimax', 'problem', 'among', 'other', 'implica... | [-0.26472268785453507, 0.021858502541565232, -0.07733059566881921, 0.06488438289638401, -0.06656201267873661, -0.327864791577061, 0.15575148929169194, 0.3355399173167017, -0.2695946524747544, -0.21327173869229024, 0.14454322326281627, -0.2145317346892423, -0.16294211690158894, 0.1548211841740542, -0.1273411170889934, 0... |
710.1326 | Magnetar Driven Bubbles and the Origin of Collimated Outflows from GRBs | We model the interaction between the wind from a newly formed rapidly
rotating magnetar and the surrounding progenitor. In the first few seconds
after core collapse the magnetar inflates a bubble of plasma and magnetic
fields behind the supernova shock, which expands asymmetrically because of the
pinching effect of t... | astro-ph | we model the interaction between the wind from a newly formed rapidly rotating magnetar and the surrounding progenitor in the first few seconds after core collapse the magnetar inflates a bubble of plasma and magnetic fields behind the supernova shock which expands asymmetrically because of the pinching effect of the t... | [['we', 'model', 'the', 'interaction', 'between', 'the', 'wind', 'from', 'a', 'newly', 'formed', 'rapidly', 'rotating', 'magnetar', 'and', 'the', 'surrounding', 'progenitor', 'in', 'the', 'first', 'few', 'seconds', 'after', 'core', 'collapse', 'the', 'magnetar', 'inflates', 'a', 'bubble', 'of', 'plasma', 'and', 'magnet... | [-0.10561541368612694, 0.21895119040001668, -0.02675219792705614, 0.1269828014612415, -0.12155413133981784, -0.06556462807342778, 0.030214041385866468, 0.3943844735622406, -0.20055370771006636, -0.3161818101133466, 0.04788270708687203, -0.2646313320193857, 0.026678400993297054, 0.24724139747493837, 0.008651200488736726... |
710.1327 | Unveiling GRB hard X-ray afterglow emission with Simbol-X | Despite the enormous progress occurred in the last 10 years, the Gamma-Ray
Bursts (GRB) phenomenon is still far to be fully understood. One of the most
important open issues that have still to be settled is the afterglow emission
above 10 keV, which is almost completely unexplored. This is due to the lack of
sensitiv... | astro-ph | despite the enormous progress occurred in the last 10 years the gammaray bursts grb phenomenon is still far to be fully understood one of the most important open issues that have still to be settled is the afterglow emission above 10 kev which is almost completely unexplored this is due to the lack of sensitive enough ... | [['despite', 'the', 'enormous', 'progress', 'occurred', 'in', 'the', 'last', '10', 'years', 'the', 'gammaray', 'bursts', 'grb', 'phenomenon', 'is', 'still', 'far', 'to', 'be', 'fully', 'understood', 'one', 'of', 'the', 'most', 'important', 'open', 'issues', 'that', 'have', 'still', 'to', 'be', 'settled', 'is', 'the', '... | [-0.06118597127836741, 0.15118756377870296, -0.05664582377669701, 0.12948453734445917, -0.10333223398109632, -0.10522466458704523, 0.04044523931917779, 0.4658979972425316, -0.19962993164760215, -0.3362019863523615, 0.09260037308836001, -0.28577528046887546, 0.002473297426366203, 0.2210257018691014, -0.03973291120547358... |
710.1328 | The Galois action on character tables | A geometric interpretation and generalisation for the Galois action on finite
group character tables is sketched. The generalisation is a Galois action on
the space Map_G(G^n,\bar{Q})/S_n for each finite G, where G acts by
simultaneous conjugation on the n-tuples G^n and the symmetric group S_n
permutes the component... | math.GR math.RT | a geometric interpretation and generalisation for the galois action on finite group character tables is sketched the generalisation is a galois action on the space map_ggnbarqs_n for each finite g where g acts by simultaneous conjugation on the ntuples gn and the symmetric group s_n permutes the components | [['a', 'geometric', 'interpretation', 'and', 'generalisation', 'for', 'the', 'galois', 'action', 'on', 'finite', 'group', 'character', 'tables', 'is', 'sketched', 'the', 'generalisation', 'is', 'a', 'galois', 'action', 'on', 'the', 'space', 'map_ggnbarqs_n', 'for', 'each', 'finite', 'g', 'where', 'g', 'acts', 'by', 'si... | [-0.2024405560594924, 0.14091525757883458, -0.11772331989746779, -0.004870559718023906, -0.17196849134176018, -0.08018041560624509, 0.03868858623219297, 0.3330022089500376, -0.31180411085803456, -0.2097245584777061, 0.08281554393668442, -0.26854730411333605, -0.11216851893535003, 0.1789323939604962, -0.1521988890351767... |
710.1329 | Conformal field theory and mapping class groups | Rational conformal field theories produce a tower of finite-dimensional
representations of surface mapping class groups, acting on the conformal blocks
of the theory. We review this formalism. We show that many recent mathematical
developments can be fit into the first 2 floors of this tower. We also review
what is k... | math.QA math.NT | rational conformal field theories produce a tower of finitedimensional representations of surface mapping class groups acting on the conformal blocks of the theory we review this formalism we show that many recent mathematical developments can be fit into the first 2 floors of this tower we also review what is known in... | [['rational', 'conformal', 'field', 'theories', 'produce', 'a', 'tower', 'of', 'finitedimensional', 'representations', 'of', 'surface', 'mapping', 'class', 'groups', 'acting', 'on', 'the', 'conformal', 'blocks', 'of', 'the', 'theory', 'we', 'review', 'this', 'formalism', 'we', 'show', 'that', 'many', 'recent', 'mathema... | [-0.11212129589963567, 0.152113090907396, -0.10833914080393259, 0.07165764967902322, -0.10769102246397072, -0.09684306033886969, -0.05068694106173805, 0.3512306829948944, -0.2573535954924645, -0.26851678384398975, 0.1016505504376255, -0.21360542217304032, -0.26145902489036044, 0.20640655767379534, -0.10877008003148216,... |
710.133 | QCD thermodynamics with 2+1 flavors at nonzero chemical potential | We present results for the QCD equation of state, quark densities and
susceptibilities at nonzero chemical potential, using 2+1 flavor asqtad
ensembles with $N_t=4$. The ensembles lie on a trajectory of constant physics
for which $m_{ud}\approx0.1m_s$. The calculation is performed using the Taylor
expansion method wi... | hep-lat | we present results for the qcd equation of state quark densities and susceptibilities at nonzero chemical potential using 21 flavor asqtad ensembles with n_t4 the ensembles lie on a trajectory of constant physics for which m_udapprox01m_s the calculation is performed using the taylor expansion method with terms up to s... | [['we', 'present', 'results', 'for', 'the', 'qcd', 'equation', 'of', 'state', 'quark', 'densities', 'and', 'susceptibilities', 'at', 'nonzero', 'chemical', 'potential', 'using', '21', 'flavor', 'asqtad', 'ensembles', 'with', 'n_t4', 'the', 'ensembles', 'lie', 'on', 'a', 'trajectory', 'of', 'constant', 'physics', 'for',... | [-0.06671994951410362, 0.19614737121782339, -0.10310116436225004, -0.028706547551197358, 0.001777882150445993, -0.04720197348461415, 0.10576048992627946, 0.35135152939563763, -0.14972196111025718, -0.28200938251729196, 0.08082849233044097, -0.30001754156098914, -0.03695077133866457, 0.11025418298175702, 0.1306508212851... |
710.1331 | Resonance Related Spiral Substructure in a Galactic Gaseous Disk | We use high resolution 2D hydrodynamic simulations to study the formation of
spiral substructure in the gaseous disk of a galaxy. The obtained gaseous
response is driven by a self-consistent non-axisymmetric potential obtained
from an imposed spiral mass distribution. We highlight the importance of
ultraharmonic reso... | astro-ph | we use high resolution 2d hydrodynamic simulations to study the formation of spiral substructure in the gaseous disk of a galaxy the obtained gaseous response is driven by a selfconsistent nonaxisymmetric potential obtained from an imposed spiral mass distribution we highlight the importance of ultraharmonic resonances... | [['we', 'use', 'high', 'resolution', '2d', 'hydrodynamic', 'simulations', 'to', 'study', 'the', 'formation', 'of', 'spiral', 'substructure', 'in', 'the', 'gaseous', 'disk', 'of', 'a', 'galaxy', 'the', 'obtained', 'gaseous', 'response', 'is', 'driven', 'by', 'a', 'selfconsistent', 'nonaxisymmetric', 'potential', 'obtain... | [-0.12420852348605686, 0.09361750761321272, -0.09632855735187772, 0.07309773568811137, -0.07306443817524166, -0.03196873236710658, -0.04498746679927417, 0.3885019080987, -0.2823270971934169, -0.2877359089394242, 0.06331915293207213, -0.26099604589826464, -0.12425023177507107, 0.1632909177313164, 0.01699146640218668, 0.... |
710.1332 | Polyexponentials | We discuss a special function (polyexponential) that extends the natural
exponential function and also the exponential integral. The basic properties of
the polyexponential are listed and some applications are given. In particular,
it is shown that certain Mellin integrals can be evaluated in terms of
polyexponential... | math.NA math.CA | we discuss a special function polyexponential that extends the natural exponential function and also the exponential integral the basic properties of the polyexponential are listed and some applications are given in particular it is shown that certain mellin integrals can be evaluated in terms of polyexponentials the p... | [['we', 'discuss', 'a', 'special', 'function', 'polyexponential', 'that', 'extends', 'the', 'natural', 'exponential', 'function', 'and', 'also', 'the', 'exponential', 'integral', 'the', 'basic', 'properties', 'of', 'the', 'polyexponential', 'are', 'listed', 'and', 'some', 'applications', 'are', 'given', 'in', 'particul... | [-0.1599796203018811, 0.0681916152485288, -0.114932589376202, 0.16095292567848585, -0.11049070444244605, -0.07303910850762174, -0.03820141258721168, 0.3099946981546684, -0.31597449550261864, -0.19100848304537626, 0.11382090137340128, -0.26014894761789875, -0.224666905689698, 0.2275162004507505, -0.05096285894799691, 0.... |
710.1333 | Dynamics and robustness of familiarity memory | When one is presented with an item or a face, one can sometimes have a sense
of recognition without being able to recall where or when one has encountered
it before. This sense of recognition is known as familiarity. Following
previous computational models of familiarity memory we investigate the
dynamical properties... | q-bio.NC | when one is presented with an item or a face one can sometimes have a sense of recognition without being able to recall where or when one has encountered it before this sense of recognition is known as familiarity following previous computational models of familiarity memory we investigate the dynamical properties of f... | [['when', 'one', 'is', 'presented', 'with', 'an', 'item', 'or', 'a', 'face', 'one', 'can', 'sometimes', 'have', 'a', 'sense', 'of', 'recognition', 'without', 'being', 'able', 'to', 'recall', 'where', 'or', 'when', 'one', 'has', 'encountered', 'it', 'before', 'this', 'sense', 'of', 'recognition', 'is', 'known', 'as', 'f... | [-0.07249698623258999, 0.0806449161872202, -0.07091777673433197, 0.06024163049153066, -0.0755916103295496, -0.17611131235785055, 0.021698660471145926, 0.3905273371146641, -0.24146982474063616, -0.3285512742114024, 0.10036655582848324, -0.28055991336662806, -0.1706916218340073, 0.15158131553460777, -0.12709405648427596,... |
710.1334 | Spin Anisotropy in ZnCu_3(OH)_6Cl_2 | The spin anisotropic exchange interaction is suggested to contribute
significantly to the abnormal upturn of the magnetic susceptibility in the
ZnCu$_3$(OH)$_6$Cl$_2$. The saturation of the magnetic susceptibility below 300
mK observed in the muon spin resonance ($\mu$SR) experiment is the quantum
effect of the spin ... | cond-mat.str-el cond-mat.stat-mech | the spin anisotropic exchange interaction is suggested to contribute significantly to the abnormal upturn of the magnetic susceptibility in the zncu_3oh_6cl_2 the saturation of the magnetic susceptibility below 300 mk observed in the muon spin resonance musr experiment is the quantum effect of the spin flipping process | [['the', 'spin', 'anisotropic', 'exchange', 'interaction', 'is', 'suggested', 'to', 'contribute', 'significantly', 'to', 'the', 'abnormal', 'upturn', 'of', 'the', 'magnetic', 'susceptibility', 'in', 'the', 'zncu_3oh_6cl_2', 'the', 'saturation', 'of', 'the', 'magnetic', 'susceptibility', 'below', '300', 'mk', 'observed'... | [-0.17316232538445198, 0.3202768565809473, -0.010585782494633756, 0.10508094108905773, -0.0926027759746153, -0.08694450018253733, 0.04825548040482434, 0.3211016356152423, -0.2519050705385335, -0.3463997413265578, 0.00010078223521246555, -0.3815364274889865, -0.051860557750184486, 0.1854432443394623, 0.12961570105138928... |
710.1335 | Effects of kinked linear defects on planar flux line arrays | In the hard core limit, interacting vortices in planar type II
superconductors can be modeled as non-interacting one dimensional fermions
propagating in imaginary time. We use this analogy to derive analytical
expressions for the probability density and imaginary current of vortex lines
interacting with an isolated b... | cond-mat.supr-con cond-mat.stat-mech | in the hard core limit interacting vortices in planar type ii superconductors can be modeled as noninteracting one dimensional fermions propagating in imaginary time we use this analogy to derive analytical expressions for the probability density and imaginary current of vortex lines interacting with an isolated bent l... | [['in', 'the', 'hard', 'core', 'limit', 'interacting', 'vortices', 'in', 'planar', 'type', 'ii', 'superconductors', 'can', 'be', 'modeled', 'as', 'noninteracting', 'one', 'dimensional', 'fermions', 'propagating', 'in', 'imaginary', 'time', 'we', 'use', 'this', 'analogy', 'to', 'derive', 'analytical', 'expressions', 'fo... | [-0.19134470027233108, 0.15902140934649447, -0.03334827318766646, 0.03257870230447041, -0.052823226773337034, -0.1463548000849616, 0.03576859406959475, 0.41410951873057344, -0.23639769280549097, -0.2450263099430987, 0.031964104282512756, -0.2693383510988415, -0.10815613952810678, 0.13445643640353522, 0.0432648233744954... |
710.1336 | Multi-User Diversity vs. Accurate Channel Feedback for MIMO Broadcast
Channels | A multiple transmit antenna, single receive antenna (per receiver) downlink
channel with limited channel feedback is considered. Given a constraint on the
total system-wide channel feedback, the following question is considered: is it
preferable to get low-rate feedback from a large number of receivers or to
receive ... | cs.IT math.IT | a multiple transmit antenna single receive antenna per receiver downlink channel with limited channel feedback is considered given a constraint on the total systemwide channel feedback the following question is considered is it preferable to get lowrate feedback from a large number of receivers or to receive highratehi... | [['a', 'multiple', 'transmit', 'antenna', 'single', 'receive', 'antenna', 'per', 'receiver', 'downlink', 'channel', 'with', 'limited', 'channel', 'feedback', 'is', 'considered', 'given', 'a', 'constraint', 'on', 'the', 'total', 'systemwide', 'channel', 'feedback', 'the', 'following', 'question', 'is', 'considered', 'is... | [-0.23997642182712298, 0.07400974399934057, 0.0018146388756576926, 0.00027313634745951276, -0.1475515608981368, -0.33404162435545004, 0.1592955422383966, 0.36749971893732436, -0.27251729952331516, -0.31313304920331575, 0.0808209899269059, -0.28053077313620634, -0.1026363448745542, 0.15787573924717435, -0.12160444656910... |
710.1337 | Search for Rare b-hadron Decays at CDF | We report on searches for B^0_s to \mu^+ \mu^-, B^0_d to \mu^+ \mu^- decays
and b to s \mu^+\mu^- transitions in exclusive decays of B mesons.
Using 2 fb^{-1} of data collected by the CDF II detector we find upper limits
on the branching fractions B(B^0_s to \mu^+ \mu^-) < 5.8 x 10^{-8} and B(B^0_d
to \mu^+ \mu^-) ... | hep-ex | we report on searches for b0_s to mu mu b0_d to mu mu decays and b to s mumu transitions in exclusive decays of b mesons using 2 fb1 of data collected by the cdf ii detector we find upper limits on the branching fractions bb0_s to mu mu 58 x 108 and bb0_d to mu mu 18 x 108 at 95 confidence level using 924 pb1 of data w... | [['we', 'report', 'on', 'searches', 'for', 'b0_s', 'to', 'mu', 'mu', 'b0_d', 'to', 'mu', 'mu', 'decays', 'and', 'b', 'to', 's', 'mumu', 'transitions', 'in', 'exclusive', 'decays', 'of', 'b', 'mesons', 'using', '2', 'fb1', 'of', 'data', 'collected', 'by', 'the', 'cdf', 'ii', 'detector', 'we', 'find', 'upper', 'limits', ... | [-0.11428549640438612, 0.2149523667034668, 0.004997332261556441, 0.042361018810052053, 0.026360991980402253, -0.14439560288378783, 0.2912949268047505, 0.277955999081904, -0.1346653383351057, -0.323201019182667, -0.031122525353697843, -0.4550952262639462, 0.1927049124428818, 0.09461809223861778, 0.04385657312751219, 0.1... |
710.1338 | Binary Black Hole Coalescence | The two-body problem in general relativity is reviewed, focusing on the final
stages of the coalescence of the black holes as uncovered by recent successes
in numerical solution of the field equations.
| gr-qc astro-ph hep-th | the twobody problem in general relativity is reviewed focusing on the final stages of the coalescence of the black holes as uncovered by recent successes in numerical solution of the field equations | [['the', 'twobody', 'problem', 'in', 'general', 'relativity', 'is', 'reviewed', 'focusing', 'on', 'the', 'final', 'stages', 'of', 'the', 'coalescence', 'of', 'the', 'black', 'holes', 'as', 'uncovered', 'by', 'recent', 'successes', 'in', 'numerical', 'solution', 'of', 'the', 'field', 'equations']] | [-0.14148413040675223, 0.06406265206169337, -0.054453883320093155, 0.06882316641349462, -0.006735975854098797, -0.06702373991720378, -0.0364219413313549, 0.222351061514928, -0.18535677739419043, -0.304450839292258, 0.11078182790515712, -0.2935597674222663, -0.1393626430653967, 0.18949391483329237, -0.011242099513765424... |
710.1339 | Resonant ratcheting of a Bose-Einstein condensate | We study the rectification process of interacting quantum particles in a
periodic potential exposed to the action of an external ac driving. The
breaking of spatio-temporal symmetries leads to directed motion already in the
absence of interactions. A hallmark of quantum ratcheting is the appearance of
resonant enhanc... | quant-ph | we study the rectification process of interacting quantum particles in a periodic potential exposed to the action of an external ac driving the breaking of spatiotemporal symmetries leads to directed motion already in the absence of interactions a hallmark of quantum ratcheting is the appearance of resonant enhancement... | [['we', 'study', 'the', 'rectification', 'process', 'of', 'interacting', 'quantum', 'particles', 'in', 'a', 'periodic', 'potential', 'exposed', 'to', 'the', 'action', 'of', 'an', 'external', 'ac', 'driving', 'the', 'breaking', 'of', 'spatiotemporal', 'symmetries', 'leads', 'to', 'directed', 'motion', 'already', 'in', '... | [-0.1712431174331672, 0.18373217627683786, -0.05260166746445459, -0.01619729374779372, -0.05828507646062487, -0.09865600403989791, 0.03223858314969048, 0.30827995271711434, -0.25205971189220816, -0.2990775664299223, -0.009193691064767237, -0.2953099946340395, -0.17732622919956575, 0.1434569993415042, -0.016309216476951... |
710.134 | A possible disk mechanism for the 23d QPO in Mkn~501 | Optically thin two-temperature accretion flows may be thermally and viscously
stable, but acoustically unstable. Here we propose that the O-mode instability
of a cooling-dominated optically thin two-temperature inner disk may explain
the 23-day quasi-periodic oscillation (QPO) period observed in the TeV and
X-ray lig... | astro-ph | optically thin twotemperature accretion flows may be thermally and viscously stable but acoustically unstable here we propose that the omode instability of a coolingdominated optically thin twotemperature inner disk may explain the 23day quasiperiodic oscillation qpo period observed in the tev and xray light curves of ... | [['optically', 'thin', 'twotemperature', 'accretion', 'flows', 'may', 'be', 'thermally', 'and', 'viscously', 'stable', 'but', 'acoustically', 'unstable', 'here', 'we', 'propose', 'that', 'the', 'omode', 'instability', 'of', 'a', 'coolingdominated', 'optically', 'thin', 'twotemperature', 'inner', 'disk', 'may', 'explain... | [-0.12955154663457163, 0.20159565233009463, -0.051191383558262825, 0.13024669137706085, -0.06077154007669321, -0.09493088406080488, 0.03591464590093313, 0.3845595392459093, -0.25011995599099807, -0.3140627184857702, 0.09893965011101316, -0.26823572263814877, 0.005038577163771563, 0.23770715452150146, -0.029986061111030... |
710.1341 | Modulated phases in magnetic models frustrated by long-range
interactions | We study an Ising model in one dimension with short range ferromagnetic and
long range (power law) antiferromagnetic interactions. We show that the zero
temperature phase diagram in a (longitudinal) field H involves a sequence of up
and down domains whose size varies continuously with H, between -H_c and H_c
which re... | cond-mat.stat-mech | we study an ising model in one dimension with short range ferromagnetic and long range power law antiferromagnetic interactions we show that the zero temperature phase diagram in a longitudinal field h involves a sequence of up and down domains whose size varies continuously with h between h_c and h_c which represent t... | [['we', 'study', 'an', 'ising', 'model', 'in', 'one', 'dimension', 'with', 'short', 'range', 'ferromagnetic', 'and', 'long', 'range', 'power', 'law', 'antiferromagnetic', 'interactions', 'we', 'show', 'that', 'the', 'zero', 'temperature', 'phase', 'diagram', 'in', 'a', 'longitudinal', 'field', 'h', 'involves', 'a', 'se... | [-0.16688494921393998, 0.24536694419966557, -0.00453133248063825, -0.004124690102387781, -0.021227889828230827, -0.12723567542198994, 0.04349459119281438, 0.4029433421586474, -0.2979778920950955, -0.31562879801510946, 0.0744198329558545, -0.2777417500133384, -0.0683656099877537, 0.19822990624808184, 0.0897455954739237,... |
710.1342 | Marginal Deformations as Lower Dimensional D-brane Solutions in Open
String Field theory | By direct calculation we showed that a finite analytic solution for marginal
deformation of open string field theory, by a matter primary operator with
singular OPE, can be obtained to all orders in the deformation parameter. In
particular, we obtained solutions that describe lower dimensional D-branes and
our result... | hep-th | by direct calculation we showed that a finite analytic solution for marginal deformation of open string field theory by a matter primary operator with singular ope can be obtained to all orders in the deformation parameter in particular we obtained solutions that describe lower dimensional dbranes and our results agree... | [['by', 'direct', 'calculation', 'we', 'showed', 'that', 'a', 'finite', 'analytic', 'solution', 'for', 'marginal', 'deformation', 'of', 'open', 'string', 'field', 'theory', 'by', 'a', 'matter', 'primary', 'operator', 'with', 'singular', 'ope', 'can', 'be', 'obtained', 'to', 'all', 'orders', 'in', 'the', 'deformation', ... | [-0.10440625112031156, 0.12426711447926155, -0.0783939143058969, 0.07217290580668834, -0.05176353017424247, -0.12075375266539962, -0.014605663622965786, 0.33216754358206224, -0.21773714766795957, -0.22912833884136, 0.09754543186950762, -0.25140481583996493, -0.1628922827458426, 0.1951331909217719, -0.052558569181988486... |
710.1343 | Dimension Reduction for the Hyperbolic Space | A dimension reduction for the hyperbolic space is established. When points
are far apart an embedding with bounded distortion into the hyperbolic plane is
achieved.
| math.MG | a dimension reduction for the hyperbolic space is established when points are far apart an embedding with bounded distortion into the hyperbolic plane is achieved | [['a', 'dimension', 'reduction', 'for', 'the', 'hyperbolic', 'space', 'is', 'established', 'when', 'points', 'are', 'far', 'apart', 'an', 'embedding', 'with', 'bounded', 'distortion', 'into', 'the', 'hyperbolic', 'plane', 'is', 'achieved']] | [-0.16107175409793853, 0.13356260998698416, -0.0017388474009931087, 0.057898882525041696, -0.11211791737005114, -0.10929293109104038, -0.0005038079619407654, 0.3486510707437992, -0.3364689952135086, -0.17994619704782963, 0.16160979345440865, -0.36300888877362014, -0.09547394618391991, 0.2736142261326313, -0.10000147458... |
710.1344 | Decoherence rates for Galilean covariant dynamics | We introduce a measure of decoherence for a class of density operators. For
Gaussian density operators in dimension one it coincides with an index used by
Morikawa (1990). Spatial decoherence rates are derived for three large classes
of the Galilean covariant quantum semigroups introduced by Holevo. We also
character... | math-ph math.MP | we introduce a measure of decoherence for a class of density operators for gaussian density operators in dimension one it coincides with an index used by morikawa 1990 spatial decoherence rates are derived for three large classes of the galilean covariant quantum semigroups introduced by holevo we also characterize the... | [['we', 'introduce', 'a', 'measure', 'of', 'decoherence', 'for', 'a', 'class', 'of', 'density', 'operators', 'for', 'gaussian', 'density', 'operators', 'in', 'dimension', 'one', 'it', 'coincides', 'with', 'an', 'index', 'used', 'by', 'morikawa', '1990', 'spatial', 'decoherence', 'rates', 'are', 'derived', 'for', 'three... | [-0.09154187724925578, 0.14938321485697087, -0.10223923737648874, 0.12142637495792315, 0.02637470609770389, -0.09539395651081577, 0.027671233573346398, 0.3153064802259905, -0.2677246812963858, -0.21418974060798063, 0.08666551978967618, -0.236015584517736, -0.12486023791134357, 0.1972190545522608, -0.07208061211276799, ... |
710.1345 | GHASP : an H alpha kinematic survey of spiral and irregular galaxies. V.
Dark matter distribution in 36 nearby spiral galaxies | The results obtained from a study of the mass distribution of 36 spiral
galaxies are presented. The galaxies were observed using Fabry-Perot
interferometry as part of the GHASP survey. The main aim of obtaining high
resolution H alpha 2D velocity fields is to define more accurately the rising
part of the rotation cur... | astro-ph | the results obtained from a study of the mass distribution of 36 spiral galaxies are presented the galaxies were observed using fabryperot interferometry as part of the ghasp survey the main aim of obtaining high resolution h alpha 2d velocity fields is to define more accurately the rising part of the rotation curves w... | [['the', 'results', 'obtained', 'from', 'a', 'study', 'of', 'the', 'mass', 'distribution', 'of', '36', 'spiral', 'galaxies', 'are', 'presented', 'the', 'galaxies', 'were', 'observed', 'using', 'fabryperot', 'interferometry', 'as', 'part', 'of', 'the', 'ghasp', 'survey', 'the', 'main', 'aim', 'of', 'obtaining', 'high', ... | [-0.06434901668834164, 0.07764565866991407, -0.11462309399197243, 0.09693564693251452, -0.08022381152311192, -0.0503307841734199, -0.0029291116642122415, 0.36930623744643226, -0.1634280675657324, -0.37162388171168537, 0.06342970771047757, -0.28173070239972103, -0.0021546830581597137, 0.1952498390209698, -0.007587381384... |
710.1346 | On the Limiting Empirical Measure of the sum of rank one matrices with
log-concave distribution | We consider $n\times n$ real symmetric and hermitian random matrices
$H_{n,m}$ equals the sum of a non-random matrix $H_{n}^{(0)}$ matrix and the
sum of $m$ rank-one matrices determined by $m$ i.i.d. isotropic random vectors
with log-concave probability law and i.i.d. random amplitudes $\{\tau_{\alpha
}\}_{\alpha =1}... | math.PR math.SP | we consider ntimes n real symmetric and hermitian random matrices h_nm equals the sum of a nonrandom matrix h_n0 matrix and the sum of m rankone matrices determined by m iid isotropic random vectors with logconcave probability law and iid random amplitudes tau_alpha _alpha 1m this is a generalization of the case of vec... | [['we', 'consider', 'ntimes', 'n', 'real', 'symmetric', 'and', 'hermitian', 'random', 'matrices', 'h_nm', 'equals', 'the', 'sum', 'of', 'a', 'nonrandom', 'matrix', 'h_n0', 'matrix', 'and', 'the', 'sum', 'of', 'm', 'rankone', 'matrices', 'determined', 'by', 'm', 'iid', 'isotropic', 'random', 'vectors', 'with', 'logconca... | [-0.144910518411332, 0.17963373355227163, -0.022003171371090084, 0.03480112759056143, 0.06313664331817283, -0.16609776038519788, 0.06137548711222525, 0.3638803555379407, -0.2922461455902801, -0.07401243240859073, 0.07345280618923986, -0.37582715106411624, -0.18470754426492092, 0.04151934595546873, -0.08933211756923881,... |
710.1347 | The asymptotic Tian-Yau-Zelditch expansion on Riemann surfaces with
Constant Curvature | Let $M$ be a regular Riemann surface with a metric which has constant scalar
curvature $\rho$. We give the asymptotic expansion of the sum of the square
norm of the sections of the pluricanonical bundles $K_{M}^{m}$. That is,
\[\sum_{i=0}^{d_{m}-1}\|S_{i}(x_{0})\|_{h_{m}}^{2} \sim m(1+\frac{\rho}{2
m})+O(e^{-\frac{(\... | math.DG | let m be a regular riemann surface with a metric which has constant scalar curvature rho we give the asymptotic expansion of the sum of the square norm of the sections of the pluricanonical bundles k_mm that is sum_i0d_m1s_ix_0_h_m2 sim m1fracrho2 moefraclog m28 where s_0s_d_m1 is an orthonormal basis for h0m k_mm for ... | [['let', 'm', 'be', 'a', 'regular', 'riemann', 'surface', 'with', 'a', 'metric', 'which', 'has', 'constant', 'scalar', 'curvature', 'rho', 'we', 'give', 'the', 'asymptotic', 'expansion', 'of', 'the', 'sum', 'of', 'the', 'square', 'norm', 'of', 'the', 'sections', 'of', 'the', 'pluricanonical', 'bundles', 'k_mm', 'that',... | [-0.20764821810343376, 0.14229886350361853, -0.09433629392935053, 0.0008513840998952779, -0.07082519875481151, -0.12542664365341458, -0.06223826740796749, 0.29695371233929807, -0.21543593976933223, -0.19187366496771574, 0.11400279840633559, -0.27660845628438085, -0.10386955367777354, 0.1473539125514575, -0.028656697402... |
710.1348 | Two-step Quantum Key Distribution Schemes Using Polarization and
Frequency Doubly Entangled Photons | A two-step quantum key distribution protocol using frequency and polarization
doubly entangled photons is proposed. In this protocol, information is encoded
by a unitary operation on each of the two doubly entangled photons and sent
from Alice to Bob in two steps. State measurement device is designed. The
security of... | quant-ph | a twostep quantum key distribution protocol using frequency and polarization doubly entangled photons is proposed in this protocol information is encoded by a unitary operation on each of the two doubly entangled photons and sent from alice to bob in two steps state measurement device is designed the security of the co... | [['a', 'twostep', 'quantum', 'key', 'distribution', 'protocol', 'using', 'frequency', 'and', 'polarization', 'doubly', 'entangled', 'photons', 'is', 'proposed', 'in', 'this', 'protocol', 'information', 'is', 'encoded', 'by', 'a', 'unitary', 'operation', 'on', 'each', 'of', 'the', 'two', 'doubly', 'entangled', 'photons'... | [-0.20144635190997548, 0.20080943793679276, -0.11617274641024845, -0.010735293542017677, 0.0550376930170589, -0.31803939810574605, 0.07531132045874579, 0.3958675083186891, -0.26646737312829055, -0.2514448937511555, 0.04325782588286394, -0.3009914371564432, -0.020030911906225676, 0.1591965489572397, -0.06379134740887417... |
710.1349 | Derivation of asymptotic two-dimensional time-dependent equations for
ocean wave propagation | A general method for the derivation of asymptotic nonlinear shallow water and
deep water models is presented. Starting from a general dimensionless version
of the water-wave equations, we reduce the problem to a system of two equations
on the surface elevation and the velocity potential at the free surface. These
equ... | physics.ao-ph | a general method for the derivation of asymptotic nonlinear shallow water and deep water models is presented starting from a general dimensionless version of the waterwave equations we reduce the problem to a system of two equations on the surface elevation and the velocity potential at the free surface these equations... | [['a', 'general', 'method', 'for', 'the', 'derivation', 'of', 'asymptotic', 'nonlinear', 'shallow', 'water', 'and', 'deep', 'water', 'models', 'is', 'presented', 'starting', 'from', 'a', 'general', 'dimensionless', 'version', 'of', 'the', 'waterwave', 'equations', 'we', 'reduce', 'the', 'problem', 'to', 'a', 'system', ... | [-0.0735081561841721, 0.08820504488100886, -0.06784017219379877, 0.06882642101959519, -0.07753884320683237, -0.14765327134788786, 0.008959920127361014, 0.29109216516566927, -0.2898829358905637, -0.26956809172146645, 0.11903444630114685, -0.2557754648859774, -0.17244032071383056, 0.1986523470269027, -0.01161177762050452... |
710.135 | On the Kirchheim-Magnani counterexample to metric differentiability | In this short note we give an interpretation of the Kirchheim-Magnani
counterexample to metric differentiability in terms of dilatation structures.
| math.MG | in this short note we give an interpretation of the kirchheimmagnani counterexample to metric differentiability in terms of dilatation structures | [['in', 'this', 'short', 'note', 'we', 'give', 'an', 'interpretation', 'of', 'the', 'kirchheimmagnani', 'counterexample', 'to', 'metric', 'differentiability', 'in', 'terms', 'of', 'dilatation', 'structures']] | [-0.19252031727841026, 0.01626990467852202, -0.0976422487905151, 0.11651859066669683, -0.09003141747885629, 0.017431819615395444, -0.041410880065278, 0.3814900062586132, -0.29896201428614166, -0.2341220660233184, 0.06037894015102402, -0.25699328729196597, -0.24675986092341573, 0.13384409993886948, -0.2268959258339907, ... |
710.1351 | Strong cosmic censorship for T^2-symmetric spacetimes with cosmological
constant and matter | We address the issue of strong cosmic censorship for T^2-symmetric spacetimes
with positive cosmological constant. In the case of collisionless matter, we
complete the proof of the C^2 formulation of the conjecture for this class of
spacetimes. In the vacuum case, we prove that the conjecture holds for the
special ca... | gr-qc math.AP math.DG | we address the issue of strong cosmic censorship for t2symmetric spacetimes with positive cosmological constant in the case of collisionless matter we complete the proof of the c2 formulation of the conjecture for this class of spacetimes in the vacuum case we prove that the conjecture holds for the special cases where... | [['we', 'address', 'the', 'issue', 'of', 'strong', 'cosmic', 'censorship', 'for', 't2symmetric', 'spacetimes', 'with', 'positive', 'cosmological', 'constant', 'in', 'the', 'case', 'of', 'collisionless', 'matter', 'we', 'complete', 'the', 'proof', 'of', 'the', 'c2', 'formulation', 'of', 'the', 'conjecture', 'for', 'this... | [-0.20811871634665088, 0.07039819436121575, -0.043510970436561276, 0.0724936931141534, -0.07079270221686489, -0.10577402961715845, -0.03611189087616726, 0.26942936472699675, -0.2005149366294729, -0.2160899898850582, 0.11120432092886891, -0.23953810973998002, -0.07768095327331356, 0.19659143413456392, -0.087353778438983... |
710.1352 | NGC 346 in The Small Magellanic Cloud. IV. Triggered Star Formation in
the HII Region N66 | Stellar feedback, expanding HII regions, wind-blown bubbles, and supernovae
are thought to be important triggering mechanisms of star formation. Stellar
associations, being hosts of significant numbers of early-type stars, are the
loci where these mechanisms act. In this part of our photometric study of the
star-form... | astro-ph | stellar feedback expanding hii regions windblown bubbles and supernovae are thought to be important triggering mechanisms of star formation stellar associations being hosts of significant numbers of earlytype stars are the loci where these mechanisms act in this part of our photometric study of the starforming region n... | [['stellar', 'feedback', 'expanding', 'hii', 'regions', 'windblown', 'bubbles', 'and', 'supernovae', 'are', 'thought', 'to', 'be', 'important', 'triggering', 'mechanisms', 'of', 'star', 'formation', 'stellar', 'associations', 'being', 'hosts', 'of', 'significant', 'numbers', 'of', 'earlytype', 'stars', 'are', 'the', 'l... | [-0.10070632156803859, 0.11034790210957268, -0.05725026440254792, 0.09922532692068704, -0.1045366694156891, -0.014851522416359297, 0.08591298471955168, 0.40391494045378984, -0.15107802151469513, -0.31201320200192706, 0.0608209754120455, -0.2598470191436785, -0.06865785479528347, 0.15262909690004395, -0.0482438537546840... |
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