id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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707.373 | Affine linear and D4 symmetric lattice equations : symmetry analysis and
reductions | We consider lattice equations on ${\mathds{Z}}^2$ which are autonomous,
affine linear and possess the symmetries of the square. Some basic properties
of equations of this type are derived, as well as a sufficient linearization
condition and a conservation law. A systematic analysis of the Lie point and
the generalize... | nlin.SI | we consider lattice equations on mathdsz2 which are autonomous affine linear and possess the symmetries of the square some basic properties of equations of this type are derived as well as a sufficient linearization condition and a conservation law a systematic analysis of the lie point and the generalized three and fi... | [['we', 'consider', 'lattice', 'equations', 'on', 'mathdsz2', 'which', 'are', 'autonomous', 'affine', 'linear', 'and', 'possess', 'the', 'symmetries', 'of', 'the', 'square', 'some', 'basic', 'properties', 'of', 'equations', 'of', 'this', 'type', 'are', 'derived', 'as', 'well', 'as', 'a', 'sufficient', 'linearization', ... | [-0.193584194801177, 0.08718114310214596, -0.06496110658652039, 0.06322371897973642, -0.13018342908171396, -0.1363834481966752, -0.02187159375953538, 0.2710045682747037, -0.2929936344585111, -0.2464276428023974, 0.17318187105864968, -0.24736392302739044, -0.16973453335544114, 0.15362901035295698, -0.03134620555436179, ... |
707.3731 | Coupled-mode equations and gap solitons in a two-dimensional nonlinear
elliptic problem with a separable periodic potential | We address a two-dimensional nonlinear elliptic problem with a
finite-amplitude periodic potential. For a class of separable symmetric
potentials, we study the bifurcation of the first band gap in the spectrum of
the linear Schr\"{o}dinger operator and the relevant coupled-mode equations to
describe this bifurcation.... | math.AP nlin.PS physics.optics | we address a twodimensional nonlinear elliptic problem with a finiteamplitude periodic potential for a class of separable symmetric potentials we study the bifurcation of the first band gap in the spectrum of the linear schrodinger operator and the relevant coupledmode equations to describe this bifurcation the coupled... | [['we', 'address', 'a', 'twodimensional', 'nonlinear', 'elliptic', 'problem', 'with', 'a', 'finiteamplitude', 'periodic', 'potential', 'for', 'a', 'class', 'of', 'separable', 'symmetric', 'potentials', 'we', 'study', 'the', 'bifurcation', 'of', 'the', 'first', 'band', 'gap', 'in', 'the', 'spectrum', 'of', 'the', 'linea... | [-0.17503933567501656, 0.0399184207598047, -0.1095671060892356, 0.10520899390160282, -0.057215025713602145, -0.1230918659529017, 0.017755210595010045, 0.29902104505865307, -0.286557251717765, -0.18521942686732415, 0.12760884496074013, -0.2645623802266025, -0.17066453091826264, 0.19080128586668704, 0.0011853196078559735... |
707.3732 | Further Comments on "Residue-to-Binary Converters Based on New Chinese
Remainder Theorems" | Ananda Mohan suggested that the first New Chinese Remainder Theorem
introduced by Wang can be derived from the constructive proof of the well-known
Chinese Remainder Theorem (CRT) and claimed that Wang's approach is the same as
the one proposed earlier by Huang. Ananda Mohan's proof is however erroneous
and we show h... | cs.OH | ananda mohan suggested that the first new chinese remainder theorem introduced by wang can be derived from the constructive proof of the wellknown chinese remainder theorem crt and claimed that wangs approach is the same as the one proposed earlier by huang ananda mohans proof is however erroneous and we show here that... | [['ananda', 'mohan', 'suggested', 'that', 'the', 'first', 'new', 'chinese', 'remainder', 'theorem', 'introduced', 'by', 'wang', 'can', 'be', 'derived', 'from', 'the', 'constructive', 'proof', 'of', 'the', 'wellknown', 'chinese', 'remainder', 'theorem', 'crt', 'and', 'claimed', 'that', 'wangs', 'approach', 'is', 'the', ... | [-0.031733287011201566, 0.042961271345624344, -0.17242498996739203, 0.1175491021713242, -0.10945805669403993, -0.13518039405775759, 0.0772110878274991, 0.25664352531043383, -0.26534882043846525, -0.272857646844708, 0.13102285821134083, -0.18589885177520604, -0.22789439324003, 0.25596031627546134, -0.17400488601997494, ... |
707.3733 | Absence of a structural glass phase in a monoatomic model liquid
predicted to undergo an ideal glass transition | We study numerically a monodisperse model of interacting classical particles
predicted to exhibit a static liquid-glass transition. Using a dynamical Monte
Carlo method we show that the model does not freeze into a glassy phase at low
temperatures. Instead, depending on the choice of the hard-core radius for the
part... | cond-mat.dis-nn | we study numerically a monodisperse model of interacting classical particles predicted to exhibit a static liquidglass transition using a dynamical monte carlo method we show that the model does not freeze into a glassy phase at low temperatures instead depending on the choice of the hardcore radius for the particles t... | [['we', 'study', 'numerically', 'a', 'monodisperse', 'model', 'of', 'interacting', 'classical', 'particles', 'predicted', 'to', 'exhibit', 'a', 'static', 'liquidglass', 'transition', 'using', 'a', 'dynamical', 'monte', 'carlo', 'method', 'we', 'show', 'that', 'the', 'model', 'does', 'not', 'freeze', 'into', 'a', 'glass... | [-0.10589616837315872, 0.25307171691025865, -0.15491430663702185, 0.050627933937262316, -0.015484508390339916, -0.17979841259666948, 0.08248949832603579, 0.36800800679159945, -0.24567063956628324, -0.266582918490787, 0.055141144869162044, -0.29849220305436946, -0.11335123241421019, 0.10572068473003561, 0.08303412882092... |
707.3734 | Malliavin calculus and Clark-Ocone formula for functionals of a
square-integrable L\'evy process | In this paper, we construct a Malliavin derivative for functionals of
square-integrable L\'evy processes and derive a Clark-Ocone formula. The
Malliavin derivative is defined via chaos expansions involving stochastic
integrals with respect to Brownian motion and Poisson random measure. As an
illustration, we compute ... | math.PR | in this paper we construct a malliavin derivative for functionals of squareintegrable levy processes and derive a clarkocone formula the malliavin derivative is defined via chaos expansions involving stochastic integrals with respect to brownian motion and poisson random measure as an illustration we compute the explic... | [['in', 'this', 'paper', 'we', 'construct', 'a', 'malliavin', 'derivative', 'for', 'functionals', 'of', 'squareintegrable', 'levy', 'processes', 'and', 'derive', 'a', 'clarkocone', 'formula', 'the', 'malliavin', 'derivative', 'is', 'defined', 'via', 'chaos', 'expansions', 'involving', 'stochastic', 'integrals', 'with',... | [-0.07964259641753002, 0.07399692668563644, -0.15461867051622408, 0.14292463470288072, -0.13280342200940307, -0.057919337050142614, 0.05412984427953647, 0.3707258019935001, -0.3372901290443472, -0.16248777545671064, 0.13769533711019905, -0.25503765281120483, -0.21152824596925215, 0.163474576162513, -0.14454189408570528... |
707.3735 | Contact line stability of ridges and drops | Within the framework of a semi-microscopic interface displacement model we
analyze the linear stability of sessile ridges and drops of a non-volatile
liquid on a homogeneous, partially wet substrate, for both signs and arbitrary
amplitudes of the three-phase contact line tension. Focusing on perturbations
which corre... | cond-mat.soft | within the framework of a semimicroscopic interface displacement model we analyze the linear stability of sessile ridges and drops of a nonvolatile liquid on a homogeneous partially wet substrate for both signs and arbitrary amplitudes of the threephase contact line tension focusing on perturbations which correspond to... | [['within', 'the', 'framework', 'of', 'a', 'semimicroscopic', 'interface', 'displacement', 'model', 'we', 'analyze', 'the', 'linear', 'stability', 'of', 'sessile', 'ridges', 'and', 'drops', 'of', 'a', 'nonvolatile', 'liquid', 'on', 'a', 'homogeneous', 'partially', 'wet', 'substrate', 'for', 'both', 'signs', 'and', 'arb... | [-0.1533105615978049, 0.16599959749246723, -0.1192427618782325, 0.03686956041251663, -0.021479297252693052, -0.13895070044211402, 0.042811074088415904, 0.3380483680822212, -0.22310168051626533, -0.2543454237346505, 0.07313176379278141, -0.2497943271943047, -0.14729495864393638, 0.14486751955701038, 0.007182566637719242... |
707.3736 | Strong decay $\Delta^{++} \to p\pi$ with light-cone QCD sum rules | In this article, we calculate the strong coupling constant $g_{\Delta N\pi}$
and study the strong decay $\Delta^{++} \to p\pi$ with the light-cone QCD sum
rules. The numerical value of the strong coupling constant $g_{\Delta N\pi}$ is
consistent with the experimental data. The small discrepancy maybe due to
failure t... | hep-ph | in this article we calculate the strong coupling constant g_delta npi and study the strong decay delta to ppi with the lightcone qcd sum rules the numerical value of the strong coupling constant g_delta npi is consistent with the experimental data the small discrepancy maybe due to failure to take into account the pert... | [['in', 'this', 'article', 'we', 'calculate', 'the', 'strong', 'coupling', 'constant', 'g_delta', 'npi', 'and', 'study', 'the', 'strong', 'decay', 'delta', 'to', 'ppi', 'with', 'the', 'lightcone', 'qcd', 'sum', 'rules', 'the', 'numerical', 'value', 'of', 'the', 'strong', 'coupling', 'constant', 'g_delta', 'npi', 'is', ... | [-0.16840228541313032, 0.13336750771850348, -0.03378549881949367, 0.09724445376349122, -0.09798224976188258, -0.09116692677663084, 0.0810115188932079, 0.3061264946795346, -0.2649315869631736, -0.18498314866436677, -0.008896888493102762, -0.3432114013642269, -0.030694417394044108, 0.04702000571578218, 0.0453313507727886... |
707.3737 | A high-velocity transient outflow in Eta Carinae | We analyze velocity profiles of the X-ray spectral lines emitted by the Eta
Carinae stellar binary at four epochs, just before the X-ray minimum
(associated with periastron) and more than two years before the minimum
(~apastron). The profiles are nicely resolved by the HETGS spectrometer on
board Chandra. Far from pe... | astro-ph | we analyze velocity profiles of the xray spectral lines emitted by the eta carinae stellar binary at four epochs just before the xray minimum associated with periastron and more than two years before the minimum apastron the profiles are nicely resolved by the hetgs spectrometer on board chandra far from periastron we ... | [['we', 'analyze', 'velocity', 'profiles', 'of', 'the', 'xray', 'spectral', 'lines', 'emitted', 'by', 'the', 'eta', 'carinae', 'stellar', 'binary', 'at', 'four', 'epochs', 'just', 'before', 'the', 'xray', 'minimum', 'associated', 'with', 'periastron', 'and', 'more', 'than', 'two', 'years', 'before', 'the', 'minimum', '... | [-0.06203371867866673, 0.17420946986510835, -0.07520714191848347, 0.08303841977472545, -0.13024853231578037, -0.14983942254350102, 0.043006344901494166, 0.4942512940069468, -0.20194292266307207, -0.31769505595981046, 0.040027514753606296, -0.32946804877499053, 0.006018357683808125, 0.20508648710172817, -0.0287608398088... |
707.3738 | Non-Hermitian von Roos Hamiltonian's $\eta$-weak-pseudo-Hermiticity,
isospectrality and exact solvability | A complexified von Roos Hamiltonian is considered and a Hermitian first-order
intertwining differential operator is used to obtain the related position
dependent mass $\eta$-weak-pseudo-Hermitian Hamiltonians. Using a
Liouvillean-type change of variables, the $\eta$-weak-pseudo-Hermitian von Roos
Hamiltonians H(x) ar... | quant-ph | a complexified von roos hamiltonian is considered and a hermitian firstorder intertwining differential operator is used to obtain the related position dependent mass etaweakpseudohermitian hamiltonians using a liouvilleantype change of variables the etaweakpseudohermitian von roos hamiltonians hx are mapped into the tr... | [['a', 'complexified', 'von', 'roos', 'hamiltonian', 'is', 'considered', 'and', 'a', 'hermitian', 'firstorder', 'intertwining', 'differential', 'operator', 'is', 'used', 'to', 'obtain', 'the', 'related', 'position', 'dependent', 'mass', 'etaweakpseudohermitian', 'hamiltonians', 'using', 'a', 'liouvilleantype', 'change'... | [-0.1145197030622512, 0.13317187882377765, -0.071816376876086, 0.11678849861607887, -0.0880815606584656, -0.29074413891416045, -0.0709536960721016, 0.3847668403759599, -0.23906557274982332, -0.18804483806714414, 0.032103594322688875, -0.30851508788764476, -0.13167918080464006, 0.17411222404334695, -0.04854948758147657,... |
707.3739 | Non-local Andreev reflection in superconducting quantum dots | With the aid of the Keldysh technique we develop a microscopic theory of
non-local electron transport in three-terminal NSN structures consisting of a
chaotic superconducting quantum dot attached to one superconducting and two
normal electrodes. Our theory fully accounts for non-equilibrium effects and
disorder in a ... | cond-mat.supr-con | with the aid of the keldysh technique we develop a microscopic theory of nonlocal electron transport in threeterminal nsn structures consisting of a chaotic superconducting quantum dot attached to one superconducting and two normal electrodes our theory fully accounts for nonequilibrium effects and disorder in a superc... | [['with', 'the', 'aid', 'of', 'the', 'keldysh', 'technique', 'we', 'develop', 'a', 'microscopic', 'theory', 'of', 'nonlocal', 'electron', 'transport', 'in', 'threeterminal', 'nsn', 'structures', 'consisting', 'of', 'a', 'chaotic', 'superconducting', 'quantum', 'dot', 'attached', 'to', 'one', 'superconducting', 'and', '... | [-0.19602633709875567, 0.14565873201210683, -0.07694576430295444, 0.06747034331568068, -0.02794927474755196, -0.21030170942748677, 0.09586602015015497, 0.33948137385793675, -0.2446567713452595, -0.26224484384910746, -0.04002038000027913, -0.3372363839413465, -0.1597978238326808, 0.199343538453607, 0.0005751690614600608... |
707.374 | Partially quenched chiral perturbation theory in the epsilon-regime | We calculate meson correlators in the epsilon-regime within partially
quenched chiral perturbation theory. The valence quark masses and sea quark
masses can be chosen arbitrary and all non-degenerate. Taking some of the sea
quark masses to infinity, one obtains a smooth connection among the theories
with different nu... | hep-lat hep-ph | we calculate meson correlators in the epsilonregime within partially quenched chiral perturbation theory the valence quark masses and sea quark masses can be chosen arbitrary and all nondegenerate taking some of the sea quark masses to infinity one obtains a smooth connection among the theories with different number of... | [['we', 'calculate', 'meson', 'correlators', 'in', 'the', 'epsilonregime', 'within', 'partially', 'quenched', 'chiral', 'perturbation', 'theory', 'the', 'valence', 'quark', 'masses', 'and', 'sea', 'quark', 'masses', 'can', 'be', 'chosen', 'arbitrary', 'and', 'all', 'nondegenerate', 'taking', 'some', 'of', 'the', 'sea',... | [-0.070083614763324, 0.35433748030724627, -0.09875060804541025, 0.13084553694352508, 0.0020238247234374285, -0.09245054811154577, 0.08218133662276986, 0.3385046756628788, -0.1508596328397592, -0.25287811621797807, 0.04321210024081114, -0.31321670823363645, -0.03984241816215217, 0.0633615663726673, 0.04184213070071895, ... |
707.3741 | Difference Discrete Connection and Curvature on Cubic Lattice | In a way similar to the continuous case formally, we define in different but
equivalent manners the difference discrete connection and curvature on discrete
vector bundle over the regular lattice as base space. We deal with the
difference operators as the discrete counterparts of the derivatives based upon
the differ... | math-ph math.DG math.MP | in a way similar to the continuous case formally we define in different but equivalent manners the difference discrete connection and curvature on discrete vector bundle over the regular lattice as base space we deal with the difference operators as the discrete counterparts of the derivatives based upon the differenti... | [['in', 'a', 'way', 'similar', 'to', 'the', 'continuous', 'case', 'formally', 'we', 'define', 'in', 'different', 'but', 'equivalent', 'manners', 'the', 'difference', 'discrete', 'connection', 'and', 'curvature', 'on', 'discrete', 'vector', 'bundle', 'over', 'the', 'regular', 'lattice', 'as', 'base', 'space', 'we', 'dea... | [-0.09355252334816297, 0.0972790400582281, -0.10056738741166721, 0.09529205191012641, -0.10448424167010341, -0.08422165807992728, 0.05361036029617852, 0.41138946512629365, -0.31264807063747535, -0.21816240676509385, 0.11942623971845023, -0.2556517753559588, -0.17479106576435946, 0.15675407236399638, -0.0638075084134470... |
707.3742 | Spatial simulations of the Kelvin-Helmholtz instability in astrophysical
jets | The long term magnetohydrodynamic stability of magnetized
transonic/supersonic jets is numerically investigated using a spatial approach.
We focus on two-dimensional linearly-unstable slab configurations where the jet
is embedded in a flow-aligned uniform magnetic field of weak amplitude. We
compare our results with ... | astro-ph | the long term magnetohydrodynamic stability of magnetized transonicsupersonic jets is numerically investigated using a spatial approach we focus on twodimensional linearlyunstable slab configurations where the jet is embedded in a flowaligned uniform magnetic field of weak amplitude we compare our results with previous... | [['the', 'long', 'term', 'magnetohydrodynamic', 'stability', 'of', 'magnetized', 'transonicsupersonic', 'jets', 'is', 'numerically', 'investigated', 'using', 'a', 'spatial', 'approach', 'we', 'focus', 'on', 'twodimensional', 'linearlyunstable', 'slab', 'configurations', 'where', 'the', 'jet', 'is', 'embedded', 'in', 'a... | [-0.180391009019958, 0.13918977334294372, -0.07310694179116445, 0.06833733700896213, -0.049506114122645994, -0.07594743622177391, -0.039029431490739085, 0.3623435538807411, -0.2434655323195141, -0.25658772868065677, 0.10780925679001281, -0.2005917800966182, -0.06335303227904547, 0.19859979157649715, 0.00916985752060406... |
707.3743 | A cosmic ray current driven instability in partially ionised media | We investigate the growth of hydromagnetic waves driven by streaming cosmic
rays in the precursor environment of a supernova remnant shock. It is known
that transverse waves propagating parallel to the mean magnetic field are
unstable to anisotropies in the cosmic ray distribution, and may provide a
mechanism to subs... | astro-ph | we investigate the growth of hydromagnetic waves driven by streaming cosmic rays in the precursor environment of a supernova remnant shock it is known that transverse waves propagating parallel to the mean magnetic field are unstable to anisotropies in the cosmic ray distribution and may provide a mechanism to substant... | [['we', 'investigate', 'the', 'growth', 'of', 'hydromagnetic', 'waves', 'driven', 'by', 'streaming', 'cosmic', 'rays', 'in', 'the', 'precursor', 'environment', 'of', 'a', 'supernova', 'remnant', 'shock', 'it', 'is', 'known', 'that', 'transverse', 'waves', 'propagating', 'parallel', 'to', 'the', 'mean', 'magnetic', 'fie... | [-0.14244638941913826, 0.23859643464487407, -0.05857018779985787, 0.11168037989865645, -0.07641158694259753, -0.02976443213174626, -0.02558102347342993, 0.3503491777029695, -0.2894839846587006, -0.2781301667518948, 0.018724916144735544, -0.2531591466336172, -0.0152799492006615, 0.21584172379643943, 0.05485668883783408,... |
707.3744 | 16-20 Jupiter mass RV companion orbiting the brown dwarf candidate
ChaHa8 | We report the discovery of a 16-20 Jupiter mass radial velocity companion
around the very young (~3 Myr) brown dwarf candidate ChaHa8 (M5.75-M6.5). Based
on high-resolution echelle spectra of ChaHa8 taken between 2000 and 2007 with
UVES at the VLT, a companion was detected through RV variability with a
semi-amplitude... | astro-ph | we report the discovery of a 1620 jupiter mass radial velocity companion around the very young 3 myr brown dwarf candidate chaha8 m575m65 based on highresolution echelle spectra of chaha8 taken between 2000 and 2007 with uves at the vlt a companion was detected through rv variability with a semiamplitude of 16 kms a ke... | [['we', 'report', 'the', 'discovery', 'of', 'a', '1620', 'jupiter', 'mass', 'radial', 'velocity', 'companion', 'around', 'the', 'very', 'young', '3', 'myr', 'brown', 'dwarf', 'candidate', 'chaha8', 'm575m65', 'based', 'on', 'highresolution', 'echelle', 'spectra', 'of', 'chaha8', 'taken', 'between', '2000', 'and', '2007... | [-0.11199479819525306, 0.12519584948270832, -0.09320720654526135, 0.05444142653453504, -0.12451502581740298, -0.12052279449317876, 0.09981602907362508, 0.33938452813933356, -0.1247719013410416, -0.392083582849946, 0.0955513714562829, -0.2959761413768297, -0.04012898028737343, 0.2169869513069166, -0.1264694824221096, -0... |
707.3745 | On Categorical Theory-Building: Beyond the Formal | I propose a notion of theory motivated by Category theory.
| math.HO math.CT | i propose a notion of theory motivated by category theory | [['i', 'propose', 'a', 'notion', 'of', 'theory', 'motivated', 'by', 'category', 'theory']] | [-0.11759533649310469, 0.09953156113624573, -0.10305854119360447, 0.037825181521475314, -0.04982007276266813, -0.1838962289970368, 0.055816194112412634, 0.25783393494784834, -0.40910040885210036, -0.2633942705579102, -0.027771893702447415, -0.14842849392443896, -0.32869877889752386, 0.010189646482467651, -0.29534452939... |
707.3746 | Ergodic properties of Poissonian ID processes | We show that a stationary IDp process (i.e., an infinitely divisible
stationary process without Gaussian part) can be written as the independent sum
of four stationary IDp processes, each of them belonging to a different class
characterized by its L\'{e}vy measure. The ergodic properties of each class
are, respective... | math.PR | we show that a stationary idp process ie an infinitely divisible stationary process without gaussian part can be written as the independent sum of four stationary idp processes each of them belonging to a different class characterized by its levy measure the ergodic properties of each class are respectively nonergodici... | [['we', 'show', 'that', 'a', 'stationary', 'idp', 'process', 'ie', 'an', 'infinitely', 'divisible', 'stationary', 'process', 'without', 'gaussian', 'part', 'can', 'be', 'written', 'as', 'the', 'independent', 'sum', 'of', 'four', 'stationary', 'idp', 'processes', 'each', 'of', 'them', 'belonging', 'to', 'a', 'different'... | [-0.081750013778219, 0.1356823315947385, -0.09390768997938088, 0.05416759387961302, -0.04809409912938819, -0.11207510901453055, 0.033036235990711364, 0.38648863966860203, -0.3307125461692719, -0.22077451512007468, 0.11070141985344337, -0.2483692598508914, -0.13158020427774475, 0.1807241973710125, -0.05087750150857534, ... |
707.3747 | p-adic elliptic polylogarithm, p-adic Eisenstein series and Katz measure | The specializations of the motivic elliptic polylog are called motivic
Eisenstein classes. For applications to special values of L-Functions, it is
important to compute the realizations of these classes. In this paper, we prove
that the syntomic realization of the motivic Eisenstein classes, restricted to
the ordinar... | math.NT math.AG | the specializations of the motivic elliptic polylog are called motivic eisenstein classes for applications to special values of lfunctions it is important to compute the realizations of these classes in this paper we prove that the syntomic realization of the motivic eisenstein classes restricted to the ordinary locus ... | [['the', 'specializations', 'of', 'the', 'motivic', 'elliptic', 'polylog', 'are', 'called', 'motivic', 'eisenstein', 'classes', 'for', 'applications', 'to', 'special', 'values', 'of', 'lfunctions', 'it', 'is', 'important', 'to', 'compute', 'the', 'realizations', 'of', 'these', 'classes', 'in', 'this', 'paper', 'we', 'p... | [-0.25252463362073596, 0.014829819886414687, -0.20247907936573029, 0.12077247483443611, -0.12118797777574274, -0.10533851432272151, -0.051415918293244, 0.25458361901625803, -0.36934212357088736, -0.2244841683585244, 0.04058101044413693, -0.19157953974437206, -0.18833303097871285, 0.32266056036600205, -0.173184118292565... |
707.3748 | Parshin Residues via Coboundary Operators | The article consist of two main parts: an analog of the Leray Theory for
Singular Varieties and its application to the Theory of Parshin's Residues. The
first part is independent from the second. It uses the theory of Whitney
stratifications. The second part is an application of the first. In particular,
a geometric ... | math.AG math.GT | the article consist of two main parts an analog of the leray theory for singular varieties and its application to the theory of parshins residues the first part is independent from the second it uses the theory of whitney stratifications the second part is an application of the first in particular a geometric and very ... | [['the', 'article', 'consist', 'of', 'two', 'main', 'parts', 'an', 'analog', 'of', 'the', 'leray', 'theory', 'for', 'singular', 'varieties', 'and', 'its', 'application', 'to', 'the', 'theory', 'of', 'parshins', 'residues', 'the', 'first', 'part', 'is', 'independent', 'from', 'the', 'second', 'it', 'uses', 'the', 'theor... | [-0.1372317426739204, 0.024528346381196046, -0.14028437872008054, 0.05251718693321119, -0.06813386951883633, -0.03399734931405295, -0.019163868938586816, 0.22098178591113538, -0.30976259852336213, -0.21572227317047885, 0.11504781216375926, -0.25850966011145804, -0.21293987541911052, 0.19400239144593026, -0.103424407612... |
707.3749 | Three- and four-jet final states in photoproduction at HERA | Three- and four-jet final states have been measured in photoproduction at
HERA using the ZEUS detector with an integrated luminosity of 121 pb^-1. The
results are presented for jets with transverse energy E_T^jet>6 GeV and
pseudorapidity |eta^jet|<2.4, in the kinematic region given by the virtuality
of the photon Q^2... | hep-ex | three and fourjet final states have been measured in photoproduction at hera using the zeus detector with an integrated luminosity of 121 pb1 the results are presented for jets with transverse energy e_tjet6 gev and pseudorapidity etajet24 in the kinematic region given by the virtuality of the photon q21 gev2 and the i... | [['three', 'and', 'fourjet', 'final', 'states', 'have', 'been', 'measured', 'in', 'photoproduction', 'at', 'hera', 'using', 'the', 'zeus', 'detector', 'with', 'an', 'integrated', 'luminosity', 'of', '121', 'pb1', 'the', 'results', 'are', 'presented', 'for', 'jets', 'with', 'transverse', 'energy', 'e_tjet6', 'gev', 'and... | [-0.012499674063175916, 0.1809616913406644, -0.107294182701502, 0.14182283597213974, 0.05035545935109258, -0.04269995272345841, -0.09738213749974967, 0.41981894636154177, -0.10931719353795051, -0.31735590979643163, -0.05127844167407602, -0.38919740596041086, 0.1375576579719782, 0.1651515107601881, 0.13011403451650402, ... |
707.375 | Recent Advances in Solving the Protein Threading Problem | The fold recognition methods are promissing tools for capturing the structure
of a protein by its amino acid residues sequence but their use is still
restricted by the needs of huge computational resources and suitable efficient
algorithms as well. In the recent version of FROST (Fold Recognition Oriented
Search Tool... | q-bio.QM cs.DC | the fold recognition methods are promissing tools for capturing the structure of a protein by its amino acid residues sequence but their use is still restricted by the needs of huge computational resources and suitable efficient algorithms as well in the recent version of frost fold recognition oriented search tool pac... | [['the', 'fold', 'recognition', 'methods', 'are', 'promissing', 'tools', 'for', 'capturing', 'the', 'structure', 'of', 'a', 'protein', 'by', 'its', 'amino', 'acid', 'residues', 'sequence', 'but', 'their', 'use', 'is', 'still', 'restricted', 'by', 'the', 'needs', 'of', 'huge', 'computational', 'resources', 'and', 'suita... | [-0.10437462288034587, 0.024234162882352486, -0.053758068814173214, 0.033654495378215916, -0.04881869127544073, -0.10909500870750183, 0.047337663013679095, 0.39245891543184847, -0.28007811676953626, -0.3503273133284006, 0.11625990479125872, -0.21772855514278397, -0.17994510210477388, 0.22974945773354644, -0.06269772694... |
707.3751 | Stress Tensor from the Trace Anomaly in Reissner-Nordstrom Spacetimes | The effective action associated with the trace anomaly provides a general
algorithm for approximating the expectation value of the stress tensor of
conformal matter fields in arbitrary curved spacetimes. In static, spherically
symmetric spacetimes, the algorithm involves solving a fourth order linear
differential equ... | gr-qc | the effective action associated with the trace anomaly provides a general algorithm for approximating the expectation value of the stress tensor of conformal matter fields in arbitrary curved spacetimes in static spherically symmetric spacetimes the algorithm involves solving a fourth order linear differential equation... | [['the', 'effective', 'action', 'associated', 'with', 'the', 'trace', 'anomaly', 'provides', 'a', 'general', 'algorithm', 'for', 'approximating', 'the', 'expectation', 'value', 'of', 'the', 'stress', 'tensor', 'of', 'conformal', 'matter', 'fields', 'in', 'arbitrary', 'curved', 'spacetimes', 'in', 'static', 'spherically... | [-0.16664796009453395, 0.11724408165380075, -0.0767049783191231, 0.06264475279352734, -0.08414356035063975, -0.11708786622991531, -0.06791508826162582, 0.31857933140550315, -0.1847520716156313, -0.26697213357229804, 0.08943350123775996, -0.27326891202987597, -0.14157185254787857, 0.16740280456195417, 0.0042568759685805... |
707.3752 | Types of quantum information | Quantum, in contrast to classical, information theory, allows for different
incompatible types (or species) of information which cannot be combined with
each other. Distinguishing these incompatible types is useful in understanding
the role of the two classical bits in teleportation (or one bit in one-bit
teleportati... | quant-ph | quantum in contrast to classical information theory allows for different incompatible types or species of information which cannot be combined with each other distinguishing these incompatible types is useful in understanding the role of the two classical bits in teleportation or one bit in onebit teleportation for dis... | [['quantum', 'in', 'contrast', 'to', 'classical', 'information', 'theory', 'allows', 'for', 'different', 'incompatible', 'types', 'or', 'species', 'of', 'information', 'which', 'can', 'not', 'be', 'combined', 'with', 'each', 'other', 'distinguishing', 'these', 'incompatible', 'types', 'is', 'useful', 'in', 'understandi... | [-0.09825440520768637, 0.14460503094021107, -0.08561316117194, 0.10295597383954593, -0.052490450810272614, -0.23042773981936848, 0.03681792264834947, 0.3221368451428774, -0.26556605950591494, -0.31163183607897915, 0.09748114399985502, -0.26549692853922563, -0.12649041859453525, 0.22258925347353567, -0.13879372894886757... |
707.3753 | Detection of incompatible properties | In a typical two-slits experiments we face the question whether it is
possible or not to attain knowledge about properties incompatible with
Which-Slit property together with the measurement of the final impact point. A
wide family of solutions is concretely found and an ideal experiment realizing
such a detection is... | quant-ph | in a typical twoslits experiments we face the question whether it is possible or not to attain knowledge about properties incompatible with whichslit property together with the measurement of the final impact point a wide family of solutions is concretely found and an ideal experiment realizing such a detection is desi... | [['in', 'a', 'typical', 'twoslits', 'experiments', 'we', 'face', 'the', 'question', 'whether', 'it', 'is', 'possible', 'or', 'not', 'to', 'attain', 'knowledge', 'about', 'properties', 'incompatible', 'with', 'whichslit', 'property', 'together', 'with', 'the', 'measurement', 'of', 'the', 'final', 'impact', 'point', 'a',... | [-0.13145703239466197, 0.0715092027775037, -0.06682066629374665, 0.04433674346988222, -0.08162527763938886, -0.13831200011606729, 0.005567093612626195, 0.3500355595855841, -0.2561942410344879, -0.29479169266830596, 0.16490270082362085, -0.3060526865135346, -0.12499320291126856, 0.21389376229905924, -0.03528647554949635... |
707.3754 | A hermitian analogue of the Broecker-Prestel theorem | The Broecker-Prestel local-global principle characterizes weak isotropy of
quadratic forms over a formally real field in terms of weak isotropy over the
henselizations and isotropy over the real closures of that field. A hermitian
analogue of this principle is presented for algebras of index at most two. An
improved ... | math.RA | the broeckerprestel localglobal principle characterizes weak isotropy of quadratic forms over a formally real field in terms of weak isotropy over the henselizations and isotropy over the real closures of that field a hermitian analogue of this principle is presented for algebras of index at most two an improved result... | [['the', 'broeckerprestel', 'localglobal', 'principle', 'characterizes', 'weak', 'isotropy', 'of', 'quadratic', 'forms', 'over', 'a', 'formally', 'real', 'field', 'in', 'terms', 'of', 'weak', 'isotropy', 'over', 'the', 'henselizations', 'and', 'isotropy', 'over', 'the', 'real', 'closures', 'of', 'that', 'field', 'a', '... | [-0.17397903226001163, 0.07163637484490222, -0.09366631810225441, 0.05786179759847918, -0.07824210219190154, -0.09904370617619912, -0.06827343045405938, 0.33254405246181806, -0.3375819700501177, -0.2320031357902876, 0.09406009320871458, -0.22639883713613093, -0.13765124362749112, 0.26049756775872496, -0.077580490857887... |
707.3755 | Computation of determinants using contour integrals | It is shown how the pre-exponential factor of the Feynman propagator for a
large class of potentials can be computed using contour integrals. This is of
direct relevance in the context of tunnelling processes in quantum theories.
The prerequisites for this analysis are accessible to advanced undergraduate
students an... | hep-th | it is shown how the preexponential factor of the feynman propagator for a large class of potentials can be computed using contour integrals this is of direct relevance in the context of tunnelling processes in quantum theories the prerequisites for this analysis are accessible to advanced undergraduate students and inv... | [['it', 'is', 'shown', 'how', 'the', 'preexponential', 'factor', 'of', 'the', 'feynman', 'propagator', 'for', 'a', 'large', 'class', 'of', 'potentials', 'can', 'be', 'computed', 'using', 'contour', 'integrals', 'this', 'is', 'of', 'direct', 'relevance', 'in', 'the', 'context', 'of', 'tunnelling', 'processes', 'in', 'qu... | [-0.08262982001955001, 0.14480060894663135, -0.10442759955767542, 0.13918213054227332, -0.10957008696471651, -0.1217658513225615, -0.005152115462503086, 0.3445394327243169, -0.247089738988628, -0.32805126092086234, 0.05089660566106128, -0.27002213934126, -0.19785234549393257, 0.24141992044945557, -0.024870291103919348,... |
707.3756 | Finite depth and Jacobson-Bourbaki correspondence | We introduce a notion of depth three tower of three rings C < B < A with
depth two ring extension A | B recovered when B = C. If A = \End B_C and B | C
is a Frobenius extension, this captures the notion of depth three for a
Frobenius extension in arXiv:math/0107064 and arXiv:math/0108067, such that if
B | C is depth ... | math.QA math.OA | we introduce a notion of depth three tower of three rings c b a with depth two ring extension a b recovered when b c if a end b_c and b c is a frobenius extension this captures the notion of depth three for a frobenius extension in arxivmath0107064 and arxivmath0108067 such that if b c is depth three then a c is depth ... | [['we', 'introduce', 'a', 'notion', 'of', 'depth', 'three', 'tower', 'of', 'three', 'rings', 'c', 'b', 'a', 'with', 'depth', 'two', 'ring', 'extension', 'a', 'b', 'recovered', 'when', 'b', 'c', 'if', 'a', 'end', 'b_c', 'and', 'b', 'c', 'is', 'a', 'frobenius', 'extension', 'this', 'captures', 'the', 'notion', 'of', 'dep... | [-0.19024790500013813, 0.10253832144536884, -0.08821203361542242, 0.02268209146285379, -0.04050233750352384, -0.190671634266304, -0.007139635854400694, 0.35355937382256664, -0.3568596037526338, -0.2040587258651047, 0.09962195687411303, -0.2296154679176775, -0.08744416263810284, 0.15943970529211535, -0.0819989954272436,... |
707.3757 | Permafrost - An Alternative Target Material for Ultra High Energy
Neutrino Detection? | The detection of cosmic neutrinos with energies above 1017 eV got growing
interest during recent years. Possible target materials for in-matter arrays of
~100 km3 size under discussion are water, ice and rock salt. Here we propose to
investigate permafrost as an additional alternative, covering ~20% of Earth
land sur... | astro-ph | the detection of cosmic neutrinos with energies above 1017 ev got growing interest during recent years possible target materials for inmatter arrays of 100 km3 size under discussion are water ice and rock salt here we propose to investigate permafrost as an additional alternative covering 20 of earth land surface and r... | [['the', 'detection', 'of', 'cosmic', 'neutrinos', 'with', 'energies', 'above', '1017', 'ev', 'got', 'growing', 'interest', 'during', 'recent', 'years', 'possible', 'target', 'materials', 'for', 'inmatter', 'arrays', 'of', '100', 'km3', 'size', 'under', 'discussion', 'are', 'water', 'ice', 'and', 'rock', 'salt', 'here'... | [-0.07942270975110073, 0.2418408205909546, 0.027743243292700184, 0.0579308067525883, -0.07018057356777964, -0.09390527427480636, 0.04446284377245011, 0.4012352471983246, -0.22404177018078203, -0.38436587094881774, 0.15792010398581624, -0.3106149483582605, -0.07427923524183995, 0.24042123402429397, -0.033719268763611504... |
707.3758 | On Landau--Ginzburg models for Fano varieties | We observe a method for finding weak Landau-Ginzburg models for Fano
varieties and find them for smooth Fano threefolds of genera 9, 10, and 12.
| math.AG | we observe a method for finding weak landauginzburg models for fano varieties and find them for smooth fano threefolds of genera 9 10 and 12 | [['we', 'observe', 'a', 'method', 'for', 'finding', 'weak', 'landauginzburg', 'models', 'for', 'fano', 'varieties', 'and', 'find', 'them', 'for', 'smooth', 'fano', 'threefolds', 'of', 'genera', '9', '10', 'and', '12']] | [-0.1583842453919351, -0.050517139993608, -0.02212929166853428, 0.1928091721981764, -0.000643041804432869, -0.2878507804684341, 0.031405979678966106, 0.36504778772592544, -0.1766295279469341, -0.3468656409904361, 0.008548130095005036, -0.24696255400776862, -0.21933856204152108, 0.2558443806320429, -0.12283297169953585,... |
707.3759 | The space of density states in geometrical quantum mechanics | We present a geometrical description of the space of density states of a
quantum system of finite dimension. After presenting a brief summary of the
geometrical formulation of Quantum Mechanics, we proceed to describe the space
of density states $\D(\Hil)$ from a geometrical perspective identifying the
stratification... | quant-ph | we present a geometrical description of the space of density states of a quantum system of finite dimension after presenting a brief summary of the geometrical formulation of quantum mechanics we proceed to describe the space of density states dhil from a geometrical perspective identifying the stratification associate... | [['we', 'present', 'a', 'geometrical', 'description', 'of', 'the', 'space', 'of', 'density', 'states', 'of', 'a', 'quantum', 'system', 'of', 'finite', 'dimension', 'after', 'presenting', 'a', 'brief', 'summary', 'of', 'the', 'geometrical', 'formulation', 'of', 'quantum', 'mechanics', 'we', 'proceed', 'to', 'describe', ... | [-0.13741634002375142, 0.12376590774879909, -0.13425685294811995, 0.04898631667659264, -0.02443246073155126, -0.06868846918469373, 0.058986879032577426, 0.28812131262056423, -0.2635774236093734, -0.26825100960682186, 0.07087677478147539, -0.23357913033171018, -0.17360270603127043, 0.17958126493900176, -0.07162783308033... |
707.376 | Striped phases in two dimensional dipole systems | We prove that a system of discrete 2D in-plane dipoles with four possible
orientations, interacting via a 3D dipole-dipole interaction plus a nearest
neighbor ferromagnetic term, has periodic striped ground states. As the
strength of the ferromagnetic term is increased, the size of the stripes in the
ground state inc... | cond-mat.stat-mech math-ph math.MP | we prove that a system of discrete 2d inplane dipoles with four possible orientations interacting via a 3d dipoledipole interaction plus a nearest neighbor ferromagnetic term has periodic striped ground states as the strength of the ferromagnetic term is increased the size of the stripes in the ground state increases b... | [['we', 'prove', 'that', 'a', 'system', 'of', 'discrete', '2d', 'inplane', 'dipoles', 'with', 'four', 'possible', 'orientations', 'interacting', 'via', 'a', '3d', 'dipoledipole', 'interaction', 'plus', 'a', 'nearest', 'neighbor', 'ferromagnetic', 'term', 'has', 'periodic', 'striped', 'ground', 'states', 'as', 'the', 's... | [-0.2360743271411522, 0.21428404849260824, 0.013842375242276817, 0.039437210292172294, -0.05274652298011467, -0.17060627331560912, 0.0620019217137353, 0.36723858435103235, -0.26270492688310165, -0.2686517176000362, 0.04737518736200922, -0.3341145043307585, -0.08605062168963412, 0.0955829989901539, 0.12966229829438533, ... |
707.3761 | Energy and composition sensitivity of geosynchrotron radio emission from
EAS | We analyse the sensitivity of geosynchrotron radio emission from inclined
extensive air showers to the energy and mass of primary cosmic rays. We
demonstrate that radio emission measurements at suitable lateral distances can
infer both the number of electrons and positrons in the shower maximum and the
atmospheric de... | astro-ph | we analyse the sensitivity of geosynchrotron radio emission from inclined extensive air showers to the energy and mass of primary cosmic rays we demonstrate that radio emission measurements at suitable lateral distances can infer both the number of electrons and positrons in the shower maximum and the atmospheric depth... | [['we', 'analyse', 'the', 'sensitivity', 'of', 'geosynchrotron', 'radio', 'emission', 'from', 'inclined', 'extensive', 'air', 'showers', 'to', 'the', 'energy', 'and', 'mass', 'of', 'primary', 'cosmic', 'rays', 'we', 'demonstrate', 'that', 'radio', 'emission', 'measurements', 'at', 'suitable', 'lateral', 'distances', 'c... | [-0.10725158265728153, 0.21362382650554965, -0.059943472994411856, 0.0877864500388312, -0.022342265131843522, -0.002102077066993866, 0.028437873471974053, 0.42453296196002227, -0.24507993275029027, -0.3989699835069159, 0.027853983015361298, -0.31305613808142835, 0.03544471815077222, 0.21855034188837066, 0.0299345143935... |
707.3762 | Hanle Effect near Boundaries | The Hanle effect describes suppression of spin polarization due to precession
in a magnetic field. This is a standard spintronics tool and it gives access to
the spin lifetime of samples in which spins are generated homogeneously. We
examine the Hanle effect when spins are generated at a boundary of a diffusive
sampl... | cond-mat.mes-hall | the hanle effect describes suppression of spin polarization due to precession in a magnetic field this is a standard spintronics tool and it gives access to the spin lifetime of samples in which spins are generated homogeneously we examine the hanle effect when spins are generated at a boundary of a diffusive sample by... | [['the', 'hanle', 'effect', 'describes', 'suppression', 'of', 'spin', 'polarization', 'due', 'to', 'precession', 'in', 'a', 'magnetic', 'field', 'this', 'is', 'a', 'standard', 'spintronics', 'tool', 'and', 'it', 'gives', 'access', 'to', 'the', 'spin', 'lifetime', 'of', 'samples', 'in', 'which', 'spins', 'are', 'generat... | [-0.1726343619191776, 0.23096476112107706, -0.05564403303635671, 0.05861312783773705, -0.07658805766993243, -0.12040559263677215, -0.020827366697156558, 0.4095571608910256, -0.3089476964719918, -0.2585937440111909, 0.06585375538207186, -0.25898949401554366, -0.06923212231460797, 0.24144837292640106, 0.00983204309950056... |
707.3763 | REAS2: CORSIKA-based Monte Carlo simulations of geosynchrotron radio
emission | Simulations of geosynchrotron radio emission from extensive air showers
performed with the Monte Carlo code REAS1 used analytical parameterisations to
describe the spatial, temporal, energy and angular particle distributions in
air showers. The successor REAS2 replaces these parameterisations with precise,
multi-dime... | astro-ph | simulations of geosynchrotron radio emission from extensive air showers performed with the monte carlo code reas1 used analytical parameterisations to describe the spatial temporal energy and angular particle distributions in air showers the successor reas2 replaces these parameterisations with precise multidimensional... | [['simulations', 'of', 'geosynchrotron', 'radio', 'emission', 'from', 'extensive', 'air', 'showers', 'performed', 'with', 'the', 'monte', 'carlo', 'code', 'reas1', 'used', 'analytical', 'parameterisations', 'to', 'describe', 'the', 'spatial', 'temporal', 'energy', 'and', 'angular', 'particle', 'distributions', 'in', 'a... | [0.01068748960786156, 0.15314565807424707, -0.1373820814009952, 0.15464090425521135, -0.020796662667079975, -0.04201136800509534, -0.03400164806087942, 0.4538238665971317, -0.21846061779774334, -0.3857100172066375, 0.012949590666807795, -0.29158237376755813, -0.05031648258629598, 0.20082414668592574, 0.0495484351229510... |
707.3764 | A timestepper approach for the systematic bifurcation and stability
analysis of polymer extrusion dynamics | We discuss how matrix-free/timestepper algorithms can efficiently be used
with dynamic non-Newtonian fluid mechanics simulators in performing systematic
stability/bifurcation analysis. The timestepper approach to bifurcation
analysis of large scale systems is applied to the plane Poiseuille flow of an
Oldroyd-B fluid... | math.DS | we discuss how matrixfreetimestepper algorithms can efficiently be used with dynamic nonnewtonian fluid mechanics simulators in performing systematic stabilitybifurcation analysis the timestepper approach to bifurcation analysis of large scale systems is applied to the plane poiseuille flow of an oldroydb fluid with no... | [['we', 'discuss', 'how', 'matrixfreetimestepper', 'algorithms', 'can', 'efficiently', 'be', 'used', 'with', 'dynamic', 'nonnewtonian', 'fluid', 'mechanics', 'simulators', 'in', 'performing', 'systematic', 'stabilitybifurcation', 'analysis', 'the', 'timestepper', 'approach', 'to', 'bifurcation', 'analysis', 'of', 'larg... | [-0.1947151663677771, 0.13731793211412766, -0.1365353363496354, 0.030870545046231688, -0.03514284436234031, -0.14346766377602282, 0.03855468412668399, 0.28899790446088336, -0.3037649615663145, -0.2502520255014169, 0.1411487234741991, -0.24236839600235618, -0.15023010162152514, 0.18582946850532575, -0.029617288489395235... |
707.3765 | Exchange shift of stripe domains in antiferromagnetically coupled
multilayers | Antiferromagnetically coupled multilayers with perpendicular anisotropy, as
[CoPt]/Ru, Co/Ir, Fe/Au, display ferromagnetic stripe phases as the ground
states. It is theoretically shown that the antiferromagnetic interlayer
exchange causes a relative shift of domains in adjacent layers. This ``exchange
shift'' is resp... | cond-mat.mes-hall | antiferromagnetically coupled multilayers with perpendicular anisotropy as coptru coir feau display ferromagnetic stripe phases as the ground states it is theoretically shown that the antiferromagnetic interlayer exchange causes a relative shift of domains in adjacent layers this exchange shift is responsible for sever... | [['antiferromagnetically', 'coupled', 'multilayers', 'with', 'perpendicular', 'anisotropy', 'as', 'coptru', 'coir', 'feau', 'display', 'ferromagnetic', 'stripe', 'phases', 'as', 'the', 'ground', 'states', 'it', 'is', 'theoretically', 'shown', 'that', 'the', 'antiferromagnetic', 'interlayer', 'exchange', 'causes', 'a', ... | [-0.22589993987075643, 0.21814043568334382, -0.012442093450048635, 0.06281642214934417, -0.06373607775918683, -0.10878670755868816, 0.056300984724063655, 0.4043941589699564, -0.295291206686002, -0.2874112762130645, -0.01831765565308457, -0.31848602722950126, -0.11092223174755975, 0.13738122876087316, 0.1313752309187275... |
707.3766 | Wind on the boundary for the Abelian sandpile model | We continue our investigation of the two-dimensional Abelian sandpile model
in terms of a logarithmic conformal field theory with central charge c=-2, by
introducing two new boundary conditions. These have two unusual features: they
carry an intrinsic orientation, and, more strangely, they cannot be imposed
uniformly... | cond-mat.stat-mech hep-th math-ph math.MP | we continue our investigation of the twodimensional abelian sandpile model in terms of a logarithmic conformal field theory with central charge c2 by introducing two new boundary conditions these have two unusual features they carry an intrinsic orientation and more strangely they cannot be imposed uniformly on a whole... | [['we', 'continue', 'our', 'investigation', 'of', 'the', 'twodimensional', 'abelian', 'sandpile', 'model', 'in', 'terms', 'of', 'a', 'logarithmic', 'conformal', 'field', 'theory', 'with', 'central', 'charge', 'c2', 'by', 'introducing', 'two', 'new', 'boundary', 'conditions', 'these', 'have', 'two', 'unusual', 'features... | [-0.12546469624652898, 0.17833159452387176, -0.06695367939218022, 0.03161005189526925, -0.10001335139139102, -0.18704110709538238, 0.01931742438660168, 0.3926373215297451, -0.2732078786444875, -0.26686988817115803, 0.12121682067760225, -0.2541084969333843, -0.1229860121039138, 0.12119380711676735, -0.08164493581156486,... |
707.3767 | Observation of condensed phases of quasi-planar core-softened colloids | We experimentally study the condensed phases of repelling core-softened
spheres in two dimensions. The dipolar pair repulsion between superparamagnetic
spheres trapped in a thin cell is induced by a transverse magnetic field and
softened by suitably adjusting the cell thickness. We scan a broad density
range and we m... | cond-mat.soft cond-mat.stat-mech | we experimentally study the condensed phases of repelling coresoftened spheres in two dimensions the dipolar pair repulsion between superparamagnetic spheres trapped in a thin cell is induced by a transverse magnetic field and softened by suitably adjusting the cell thickness we scan a broad density range and we materi... | [['we', 'experimentally', 'study', 'the', 'condensed', 'phases', 'of', 'repelling', 'coresoftened', 'spheres', 'in', 'two', 'dimensions', 'the', 'dipolar', 'pair', 'repulsion', 'between', 'superparamagnetic', 'spheres', 'trapped', 'in', 'a', 'thin', 'cell', 'is', 'induced', 'by', 'a', 'transverse', 'magnetic', 'field',... | [-0.17167981356068188, 0.2796511891892696, -0.03055040744211839, 0.021188125308849906, 0.021835599933380644, -0.12827578738348624, 0.039926173726478255, 0.44187732709639044, -0.2567868543093104, -0.28072983565100706, -0.0074131537764613705, -0.28932053661983775, -0.14702558863055276, 0.10666532670877066, 0.094989210657... |
707.3768 | Optical Properties of Pentacene and Perfluoropentacene Thin Films | The optical properties of pentacene (PEN) and perfluoropentacene(PFP) thin
films on various SiO2 substrates were studied using variable angle
spectroscopic ellipsometry. Structural characterization was performed using
X-ray reflectivity and atomic force microscopy. A uniaxial model with the optic
axis normal to the s... | cond-mat.soft cond-mat.mtrl-sci | the optical properties of pentacene pen and perfluoropentacenepfp thin films on various sio2 substrates were studied using variable angle spectroscopic ellipsometry structural characterization was performed using xray reflectivity and atomic force microscopy a uniaxial model with the optic axis normal to the sample sur... | [['the', 'optical', 'properties', 'of', 'pentacene', 'pen', 'and', 'perfluoropentacenepfp', 'thin', 'films', 'on', 'various', 'sio2', 'substrates', 'were', 'studied', 'using', 'variable', 'angle', 'spectroscopic', 'ellipsometry', 'structural', 'characterization', 'was', 'performed', 'using', 'xray', 'reflectivity', 'an... | [-0.08497950785721724, 0.10928467086304385, -0.05036117161850994, -0.04287055615061082, -0.027453758187990528, -0.12171152853392041, 0.08241038480646705, 0.5180059292843231, -0.26695026128958815, -0.3305302776085834, 0.008895319155924834, -0.33362700141823065, -0.05300983844044355, 0.16738743676344314, 0.03278039190440... |
707.3769 | Superintegrability on sl(2)-coalgebra spaces | We review a recently introduced set of N-dimensional quasi-maximally
superintegrable Hamiltonian systems describing geodesic motions, that can be
used to generate "dynamically" a large family of curved spaces. From an
algebraic viewpoint, such spaces are obtained through kinetic energy
Hamiltonians defined on either ... | math-ph math.MP nlin.SI | we review a recently introduced set of ndimensional quasimaximally superintegrable hamiltonian systems describing geodesic motions that can be used to generate dynamically a large family of curved spaces from an algebraic viewpoint such spaces are obtained through kinetic energy hamiltonians defined on either the sl2 p... | [['we', 'review', 'a', 'recently', 'introduced', 'set', 'of', 'ndimensional', 'quasimaximally', 'superintegrable', 'hamiltonian', 'systems', 'describing', 'geodesic', 'motions', 'that', 'can', 'be', 'used', 'to', 'generate', 'dynamically', 'a', 'large', 'family', 'of', 'curved', 'spaces', 'from', 'an', 'algebraic', 'vi... | [-0.14635021967724676, 0.1534609530710094, -0.058993338549598345, 0.09082306496067238, -0.1118493752997546, -0.13358590703989778, -0.08618829668765622, 0.373869087777677, -0.31859268649880373, -0.24914981185325555, 0.10743704524578615, -0.24881210298765274, -0.18700109478307977, 0.20048138687741898, -0.1005847780920919... |
707.377 | Genetic progression and the waiting time to cancer | Cancer results from genetic alterations that disturb the normal cooperative
behavior of cells. Recent high-throughput genomic studies of cancer cells have
shown that the mutational landscape of cancer is complex and that individual
cancers may evolve through mutations in as many as 20 different
cancer-associated gene... | q-bio.PE q-bio.QM | cancer results from genetic alterations that disturb the normal cooperative behavior of cells recent highthroughput genomic studies of cancer cells have shown that the mutational landscape of cancer is complex and that individual cancers may evolve through mutations in as many as 20 different cancerassociated genes we ... | [['cancer', 'results', 'from', 'genetic', 'alterations', 'that', 'disturb', 'the', 'normal', 'cooperative', 'behavior', 'of', 'cells', 'recent', 'highthroughput', 'genomic', 'studies', 'of', 'cancer', 'cells', 'have', 'shown', 'that', 'the', 'mutational', 'landscape', 'of', 'cancer', 'is', 'complex', 'and', 'that', 'in... | [-0.05226322361172091, 0.11590883404458453, -0.028575817466300633, 0.11172807449364291, -0.02899177845317832, -0.1375224444338303, 0.1303482898878541, 0.33468806368692483, -0.2597264626379048, -0.23085191403515637, 0.05723040478352635, -0.21608621454269616, -0.2414646344643432, 0.18847405082472965, -0.14540100763983949... |
707.3771 | Evolution of dwarf galaxies in the Centaurus A group | We consider star formation properties of dwarf galaxies in Cen A group
observed within our HST/ACS projects number 9771 and 10235. We model
color-magnitude diagrams of the galaxies under consideration and measure star
formation rate and metallicity dependence on time. We study environmental
dependence of the galaxy e... | astro-ph | we consider star formation properties of dwarf galaxies in cen a group observed within our hstacs projects number 9771 and 10235 we model colormagnitude diagrams of the galaxies under consideration and measure star formation rate and metallicity dependence on time we study environmental dependence of the galaxy evoluti... | [['we', 'consider', 'star', 'formation', 'properties', 'of', 'dwarf', 'galaxies', 'in', 'cen', 'a', 'group', 'observed', 'within', 'our', 'hstacs', 'projects', 'number', '9771', 'and', '10235', 'we', 'model', 'colormagnitude', 'diagrams', 'of', 'the', 'galaxies', 'under', 'consideration', 'and', 'measure', 'star', 'for... | [-0.08771841401426957, 0.054882723239957, -0.12967823929924133, 0.12313356065865734, -0.1356463223246151, 0.04047082352516209, 0.09720529155034957, 0.47107639696834414, -0.08910670084075938, -0.34176229910346967, -0.003684489646573262, -0.27701390792710046, -0.06971990779556077, 0.1538244319300906, -0.03847543519905543... |
707.3772 | Superintegrability on N-dimensional spaces of constant curvature from
so(N+1) and its contractions | The Lie-Poisson algebra so(N+1) and some of its contractions are used to
construct a family of superintegrable Hamiltonians on the ND spherical,
Euclidean, hyperbolic, Minkowskian and (anti-)de Sitter spaces. We firstly
present a Hamiltonian which is a superposition of an arbitrary central
potential with N arbitrary ... | math-ph math.MP nlin.SI | the liepoisson algebra son1 and some of its contractions are used to construct a family of superintegrable hamiltonians on the nd spherical euclidean hyperbolic minkowskian and antide sitter spaces we firstly present a hamiltonian which is a superposition of an arbitrary central potential with n arbitrary centrifugal t... | [['the', 'liepoisson', 'algebra', 'son1', 'and', 'some', 'of', 'its', 'contractions', 'are', 'used', 'to', 'construct', 'a', 'family', 'of', 'superintegrable', 'hamiltonians', 'on', 'the', 'nd', 'spherical', 'euclidean', 'hyperbolic', 'minkowskian', 'and', 'antide', 'sitter', 'spaces', 'we', 'firstly', 'present', 'a', ... | [-0.18207805472537406, 0.1438520748964284, -0.03214102503462876, 0.04763215775425845, -0.06486668857985979, -0.1414076702891843, -0.0522810427849796, 0.3117801956129524, -0.2599696913359206, -0.246268018031692, 0.11657869139738944, -0.2775457160629379, -0.1590054009985413, 0.1613713711142868, -0.06594851973886476, 0.03... |
707.3773 | Conformal paracontact curvature and the local flatness theorem | A curvature-type tensor invariant called para contact (pc) conformal
curvature is defined on a paracontact manifold. It is shown that a paracontact
manifold is locally paracontact conformal to the hyperbolic Heisenberg group or
to a hyperquadric of neutral signature if and only if the pc conformal
curvature vanishes.... | math.DG math.AP | a curvaturetype tensor invariant called para contact pc conformal curvature is defined on a paracontact manifold it is shown that a paracontact manifold is locally paracontact conformal to the hyperbolic heisenberg group or to a hyperquadric of neutral signature if and only if the pc conformal curvature vanishes in the... | [['a', 'curvaturetype', 'tensor', 'invariant', 'called', 'para', 'contact', 'pc', 'conformal', 'curvature', 'is', 'defined', 'on', 'a', 'paracontact', 'manifold', 'it', 'is', 'shown', 'that', 'a', 'paracontact', 'manifold', 'is', 'locally', 'paracontact', 'conformal', 'to', 'the', 'hyperbolic', 'heisenberg', 'group', '... | [-0.20672770227608073, 0.09257892499148992, -0.06164350456749208, 0.08356809675988033, -0.14691188714554548, -0.17840820190329582, -0.09829112343514004, 0.37652942888502383, -0.2439567928469111, -0.17422914952756122, 0.11341311971052016, -0.2663728137198103, -0.18714089410053167, 0.14678178728820804, -0.058752817850018... |
707.3774 | Spin geometry of entangled qubits under bilocal decoherence modes | The Lindblad generators of the master equation define which kind of
decoherence happens in an open quantum system. We are working with a two qubit
system and choose the generators to be projection operators on the eigenstates
of the system and unitary bilocal rotations of them. The resulting decoherence
modes are stu... | quant-ph | the lindblad generators of the master equation define which kind of decoherence happens in an open quantum system we are working with a two qubit system and choose the generators to be projection operators on the eigenstates of the system and unitary bilocal rotations of them the resulting decoherence modes are studied... | [['the', 'lindblad', 'generators', 'of', 'the', 'master', 'equation', 'define', 'which', 'kind', 'of', 'decoherence', 'happens', 'in', 'an', 'open', 'quantum', 'system', 'we', 'are', 'working', 'with', 'a', 'two', 'qubit', 'system', 'and', 'choose', 'the', 'generators', 'to', 'be', 'projection', 'operators', 'on', 'the... | [-0.18583293678623833, 0.17702644798735806, -0.060473782526067464, 0.08592754149951871, 0.0008906439131449077, -0.1386848251404595, 0.01298081332409739, 0.3307029880460136, -0.26463617469646633, -0.24523871030258246, 0.058000783727519704, -0.2725386243980534, -0.10524087570115062, 0.1671324483588461, -0.040483978242143... |
707.3775 | Predicting Knot or Catenane Type of Site-Specific Recombination Products | Site-specific recombination on supercoiled circular DNA yields a variety of
knotted or catenated products. We develop a model of this process, and give
extensive experimental evidence that the assumptions of our model are
reasonable. We then characterize all possible knot or catenane products that
arise from the most... | q-bio.BM q-bio.QM | sitespecific recombination on supercoiled circular dna yields a variety of knotted or catenated products we develop a model of this process and give extensive experimental evidence that the assumptions of our model are reasonable we then characterize all possible knot or catenane products that arise from the most commo... | [['sitespecific', 'recombination', 'on', 'supercoiled', 'circular', 'dna', 'yields', 'a', 'variety', 'of', 'knotted', 'or', 'catenated', 'products', 'we', 'develop', 'a', 'model', 'of', 'this', 'process', 'and', 'give', 'extensive', 'experimental', 'evidence', 'that', 'the', 'assumptions', 'of', 'our', 'model', 'are', ... | [-0.10167143891493861, 0.07798203454854397, -0.0806748585918775, 0.06557784464779476, -0.09193173186280407, -0.17363404610122626, 0.08894792368205694, 0.4222732594380012, -0.26793899292018836, -0.2851526696163301, 0.09954308489910685, -0.24171166627739485, -0.1702959909999313, 0.20919134253636001, -0.0404327720690232, ... |
707.3776 | Polar phonons and spin-phonon coupling in HgCr2S4 and CdCr2S4 | Polar phonons of HgCr2S4 and CdCr2S4 are studied by far-infrared spectroscopy
as a function of temperature and external magnetic field. Eigenfrequencies,
damping constants, effective plasma frequencies and Lyddane-Sachs-Teller
relations, and effective charges are determined. Ferromagnetic CdCr2S4 and
antiferromagneti... | cond-mat.str-el | polar phonons of hgcr2s4 and cdcr2s4 are studied by farinfrared spectroscopy as a function of temperature and external magnetic field eigenfrequencies damping constants effective plasma frequencies and lyddanesachsteller relations and effective charges are determined ferromagnetic cdcr2s4 and antiferromagnetic hgcr2s4 ... | [['polar', 'phonons', 'of', 'hgcr2s4', 'and', 'cdcr2s4', 'are', 'studied', 'by', 'farinfrared', 'spectroscopy', 'as', 'a', 'function', 'of', 'temperature', 'and', 'external', 'magnetic', 'field', 'eigenfrequencies', 'damping', 'constants', 'effective', 'plasma', 'frequencies', 'and', 'lyddanesachsteller', 'relations', ... | [-0.201664278791556, 0.27616565719517233, -0.030151765010711075, 0.06328069219328598, -0.07726610909499552, -0.11424893576422356, 0.05067853496639409, 0.44490456888857094, -0.21647881400987398, -0.2984028003934393, -0.000857900865662816, -0.3257158548179744, -0.1186203359545249, 0.17915201758581173, 0.10633811725689894... |
707.3777 | Nonfibered knots and representation shifts | The authors conjectured previously that a knot is nonfibered if and only if
its infinite cyclic cover has uncountably many finite covers. We prove the
conjecture for a class of knots that includes all knots of genus 1, using
techniques from symbolic dynamics.
| math.GT math.DS | the authors conjectured previously that a knot is nonfibered if and only if its infinite cyclic cover has uncountably many finite covers we prove the conjecture for a class of knots that includes all knots of genus 1 using techniques from symbolic dynamics | [['the', 'authors', 'conjectured', 'previously', 'that', 'a', 'knot', 'is', 'nonfibered', 'if', 'and', 'only', 'if', 'its', 'infinite', 'cyclic', 'cover', 'has', 'uncountably', 'many', 'finite', 'covers', 'we', 'prove', 'the', 'conjecture', 'for', 'a', 'class', 'of', 'knots', 'that', 'includes', 'all', 'knots', 'of', '... | [-0.1916286698434242, 0.128561177745808, -0.15381239254980586, 0.06537970934377246, -0.06802131106730464, -0.1976971039440223, -0.01119586760394795, 0.3568900792404663, -0.2793702222406864, -0.23939996095764082, 0.1056512107742344, -0.25036433910366235, -0.1702209248878928, 0.2746079861034834, -0.11854912758653247, 0.0... |
707.3778 | Renormalization group running cosmologies - from a scale setting to
holographic dark energy | A scale-dependent cosmological constant $\Lambda$ and the Newton constant G
emerge naturally in quantum field theory in a curved space-time background
leading to renormalization group running cosmologies. A scale-setting procedure
is discussed in these cosmological models and the interpretation of the scale
is emphas... | gr-qc astro-ph hep-ph hep-th | a scaledependent cosmological constant lambda and the newton constant g emerge naturally in quantum field theory in a curved spacetime background leading to renormalization group running cosmologies a scalesetting procedure is discussed in these cosmological models and the interpretation of the scale is emphasized this... | [['a', 'scaledependent', 'cosmological', 'constant', 'lambda', 'and', 'the', 'newton', 'constant', 'g', 'emerge', 'naturally', 'in', 'quantum', 'field', 'theory', 'in', 'a', 'curved', 'spacetime', 'background', 'leading', 'to', 'renormalization', 'group', 'running', 'cosmologies', 'a', 'scalesetting', 'procedure', 'is'... | [-0.1564016551053261, 0.1559558892786941, -0.16784238178310368, 0.1421932604670634, -0.15044258602840058, -0.16590009771342226, -0.0708642200607916, 0.3145642158575356, -0.27291718783843166, -0.3473251897184288, 0.02571541023961104, -0.1740406886948382, -0.087185629720197, 0.173069747381241, -0.023971977808019695, 0.00... |
707.3779 | Modeling DACs in UV Lines of Massive Hot Stars | We apply the 3-dimensional radiative transport code Wind3D to 3D hydrodynamic
models of Corotating Interaction Regions to fit the detailed variability of
Discrete Absorption Components observed in Si IV UV resonance lines of HD 64760
(B0.5 Ib). We discuss important effects of the hydrodynamic input parameters on
thes... | astro-ph | we apply the 3dimensional radiative transport code wind3d to 3d hydrodynamic models of corotating interaction regions to fit the detailed variability of discrete absorption components observed in si iv uv resonance lines of hd 64760 b05 ib we discuss important effects of the hydrodynamic input parameters on these large... | [['we', 'apply', 'the', '3dimensional', 'radiative', 'transport', 'code', 'wind3d', 'to', '3d', 'hydrodynamic', 'models', 'of', 'corotating', 'interaction', 'regions', 'to', 'fit', 'the', 'detailed', 'variability', 'of', 'discrete', 'absorption', 'components', 'observed', 'in', 'si', 'iv', 'uv', 'resonance', 'lines', '... | [-0.11287867933140784, 0.05523395418079463, -0.013524183328658089, 0.10063710164918044, -0.0726880428728537, -0.11810706551107815, -0.006209358036265535, 0.4140151094929394, -0.2332784846125139, -0.2892369063515848, 0.03229439174618288, -0.23835826372496893, -0.0653397172760471, 0.1771085279603031, -0.01537652262012963... |
707.378 | Polarization effects on the dielectric properties of molten AgI | The results are reported of molecular dynamics simulations of the static
longitudinal dielectric and response functions for molten AgI at 923 K using
two ionic models. The first one is a rigid ion model, while in the second the
induced dipole moments of the anions are added to the effective pair potentials
of the fir... | cond-mat.soft cond-mat.stat-mech | the results are reported of molecular dynamics simulations of the static longitudinal dielectric and response functions for molten agi at 923 k using two ionic models the first one is a rigid ion model while in the second the induced dipole moments of the anions are added to the effective pair potentials of the first i... | [['the', 'results', 'are', 'reported', 'of', 'molecular', 'dynamics', 'simulations', 'of', 'the', 'static', 'longitudinal', 'dielectric', 'and', 'response', 'functions', 'for', 'molten', 'agi', 'at', '923', 'k', 'using', 'two', 'ionic', 'models', 'the', 'first', 'one', 'is', 'a', 'rigid', 'ion', 'model', 'while', 'in',... | [-0.11238996771404917, 0.18326492635323927, -0.015247311526804828, 0.051207500058644856, 0.0470369544816779, -0.10932781511729353, -0.021848079284752478, 0.4174121492176076, -0.23555848481698652, -0.274218817000811, -0.0013526620230836313, -0.3191640530242009, -0.08677328848332334, 0.11976505407351959, 0.11936422187332... |
707.3781 | Bijective Faithful Translations among Default Logics | In this article, we study translations between variants of defaults logics
such that the extensions of the theories that are the input and the output of
the translation are in a bijective correspondence. We assume that a translation
can introduce new variables and that the result of translating a theory can
either be... | cs.AI cs.LO | in this article we study translations between variants of defaults logics such that the extensions of the theories that are the input and the output of the translation are in a bijective correspondence we assume that a translation can introduce new variables and that the result of translating a theory can either be pro... | [['in', 'this', 'article', 'we', 'study', 'translations', 'between', 'variants', 'of', 'defaults', 'logics', 'such', 'that', 'the', 'extensions', 'of', 'the', 'theories', 'that', 'are', 'the', 'input', 'and', 'the', 'output', 'of', 'the', 'translation', 'are', 'in', 'a', 'bijective', 'correspondence', 'we', 'assume', '... | [-0.11736345472948059, 0.1034348911413437, -0.09815441745171405, 0.09411613150277054, -0.08480563654523829, -0.10706503575910693, 0.03720803192067568, 0.3774412455928067, -0.3269116875229646, -0.2482660797222153, 0.08516375903323617, -0.27341217369489046, -0.12792652166124596, 0.16085601975614933, -0.11046151518416794,... |
707.3782 | Interactive Small-Step Algorithms I: Axiomatization | In earlier work, the Abstract State Machine Thesis -- that arbitrary
algorithms are behaviorally equivalent to abstract state machines -- was
established for several classes of algorithms, including ordinary, interactive,
small-step algorithms. This was accomplished on the basis of axiomatizations of
these classes of... | cs.LO | in earlier work the abstract state machine thesis that arbitrary algorithms are behaviorally equivalent to abstract state machines was established for several classes of algorithms including ordinary interactive smallstep algorithms this was accomplished on the basis of axiomatizations of these classes of algorithms he... | [['in', 'earlier', 'work', 'the', 'abstract', 'state', 'machine', 'thesis', 'that', 'arbitrary', 'algorithms', 'are', 'behaviorally', 'equivalent', 'to', 'abstract', 'state', 'machines', 'was', 'established', 'for', 'several', 'classes', 'of', 'algorithms', 'including', 'ordinary', 'interactive', 'smallstep', 'algorith... | [-0.0694934355160166, 0.08414444910983244, -0.1198761830638562, 0.09858046468302963, -0.13006858243385241, -0.1643407541548922, 0.066975612185585, 0.43271114382715453, -0.2403426973814411, -0.3351174537314191, 0.11908091150246383, -0.23311443012207747, -0.1371647818989697, 0.1963184976950288, -0.12886456028070478, 0.07... |
707.3783 | Network Rewiring Models | Recently we showed that a simple model of network rewiring could be solved
exactly for any time and any parameter value. We also showed that this model
can be recast in terms of several well known models of statistical physics such
as Urn model and the Voter model. We also noted that it has been applied to a
wide ran... | cond-mat.stat-mech | recently we showed that a simple model of network rewiring could be solved exactly for any time and any parameter value we also showed that this model can be recast in terms of several well known models of statistical physics such as urn model and the voter model we also noted that it has been applied to a wide range o... | [['recently', 'we', 'showed', 'that', 'a', 'simple', 'model', 'of', 'network', 'rewiring', 'could', 'be', 'solved', 'exactly', 'for', 'any', 'time', 'and', 'any', 'parameter', 'value', 'we', 'also', 'showed', 'that', 'this', 'model', 'can', 'be', 'recast', 'in', 'terms', 'of', 'several', 'well', 'known', 'models', 'of'... | [-0.025028893092990313, 0.07421290034452747, -0.09213234688841591, 0.09278651991993875, -0.06087382778672403, -0.17971634662612096, 0.03346605471482402, 0.38905620620291875, -0.28133380405702874, -0.3388041110807343, 0.12240312386175471, -0.20490196904804753, -0.23286711846135164, 0.21456201233300626, -0.07357209975720... |
707.3784 | Interaction induced dimerization in zigzag single wall carbon nanotubes | We derive a low-energy effective model of metallic zigzag carbon nanotubes at
half filling. We show that there are three important features characterizing
the low-energy properties of these systems: the long-range Coulomb interaction,
umklapp scattering and an explicit dimerization generated by interactions. The
rati... | cond-mat.str-el | we derive a lowenergy effective model of metallic zigzag carbon nanotubes at half filling we show that there are three important features characterizing the lowenergy properties of these systems the longrange coulomb interaction umklapp scattering and an explicit dimerization generated by interactions the ratio of the ... | [['we', 'derive', 'a', 'lowenergy', 'effective', 'model', 'of', 'metallic', 'zigzag', 'carbon', 'nanotubes', 'at', 'half', 'filling', 'we', 'show', 'that', 'there', 'are', 'three', 'important', 'features', 'characterizing', 'the', 'lowenergy', 'properties', 'of', 'these', 'systems', 'the', 'longrange', 'coulomb', 'inte... | [-0.20683892196652912, 0.24458945460406034, -0.02968679277553675, 0.04932100534217783, 0.015135906471312969, -0.15610061191243702, 0.06177561214691637, 0.41285508919027775, -0.2796020589810381, -0.2553327208071357, 0.03480911722388303, -0.33055752551293754, -0.17221410387647476, 0.10359181368741954, 0.09678645241235632... |
707.3785 | Color superconducting matter in a magnetic field | We investigate the effect of a magnetic field on cold dense three-flavor
quark matter using an effective model with four-Fermi interactions with
electric and color neutrality taken into account. The gap parameters Delta_1,
Delta_2, and Delta_3 representing respectively the predominant pairing between
down and strange... | hep-ph | we investigate the effect of a magnetic field on cold dense threeflavor quark matter using an effective model with fourfermi interactions with electric and color neutrality taken into account the gap parameters delta_1 delta_2 and delta_3 representing respectively the predominant pairing between down and strange ds qua... | [['we', 'investigate', 'the', 'effect', 'of', 'a', 'magnetic', 'field', 'on', 'cold', 'dense', 'threeflavor', 'quark', 'matter', 'using', 'an', 'effective', 'model', 'with', 'fourfermi', 'interactions', 'with', 'electric', 'and', 'color', 'neutrality', 'taken', 'into', 'account', 'the', 'gap', 'parameters', 'delta_1', ... | [-0.1733393279601479, 0.25973072166109645, -0.06108750006383733, 0.10255892270580545, -0.04731198812229304, -0.1350261626327461, 0.10748915626830294, 0.33672073560313937, -0.25069009466860137, -0.3195470775289288, -0.059126647332393124, -0.30401731334891313, -0.04140964192160166, 0.09612752432499813, 0.0574383335805096... |
707.3786 | A new mechanism for non-locality from string theory: UV-IR quantum
entanglement and its imprints on the CMB | Puff field theories (PFT) arise as the decoupling limits of D3 branes in a
Melvin universe and exhibit spatially non-local dynamics. Unlike other
realizations of non-locality in string theory, PFTs have full SO(3) rotational
symmetry. In this work, we analyze the strongly coupled regime of a PFT through
gravitational... | hep-th astro-ph | puff field theories pft arise as the decoupling limits of d3 branes in a melvin universe and exhibit spatially nonlocal dynamics unlike other realizations of nonlocality in string theory pfts have full so3 rotational symmetry in this work we analyze the strongly coupled regime of a pft through gravitational holography ... | [['puff', 'field', 'theories', 'pft', 'arise', 'as', 'the', 'decoupling', 'limits', 'of', 'd3', 'branes', 'in', 'a', 'melvin', 'universe', 'and', 'exhibit', 'spatially', 'nonlocal', 'dynamics', 'unlike', 'other', 'realizations', 'of', 'nonlocality', 'in', 'string', 'theory', 'pfts', 'have', 'full', 'so3', 'rotational',... | [-0.1620507358979338, 0.15272328683381486, -0.1421733669972477, 0.09916855961767933, -0.05552468585739963, -0.13146492907365498, -0.012137532445381228, 0.31273601955781954, -0.2260905469331938, -0.23837463513542062, 0.06621627363030058, -0.24052676855362967, -0.14530516873883942, 0.1308922385856605, -0.0187700991817296... |
707.3787 | Effective su_q(2) models and polynomial algebras for fermion-boson
Hamiltonians | Schematic su(2)+h3 interaction Hamiltonians, where su(2) plays the role of
the pseudo-spin algebra of fermion operators and h3 is the Heisenberg algebra
for bosons, are shown to be closely related to certain nonlinear models defined
on a single quantum algebra q-su(2) of quasifermions. In particular, q-su(2)
analogue... | math-ph math.MP quant-ph | schematic su2h3 interaction hamiltonians where su2 plays the role of the pseudospin algebra of fermion operators and h3 is the heisenberg algebra for bosons are shown to be closely related to certain nonlinear models defined on a single quantum algebra qsu2 of quasifermions in particular qsu2 analogues of the da provid... | [['schematic', 'su2h3', 'interaction', 'hamiltonians', 'where', 'su2', 'plays', 'the', 'role', 'of', 'the', 'pseudospin', 'algebra', 'of', 'fermion', 'operators', 'and', 'h3', 'is', 'the', 'heisenberg', 'algebra', 'for', 'bosons', 'are', 'shown', 'to', 'be', 'closely', 'related', 'to', 'certain', 'nonlinear', 'models',... | [-0.15320151428301118, 0.16538267598751885, -0.03373511401878204, 0.10703180251459096, -0.05964315821485663, -0.15437958350428094, -0.07230089018753741, 0.3352958138710187, -0.2736019471913208, -0.24544741980800475, 0.08193817645179131, -0.2560944239275507, -0.15358527020815713, 0.17267658959292334, -0.0019659138411099... |
707.3788 | Excited-state OH Mainline Masers in AU Geminorum and NML Cygni | Excited-state OH maser emission has previously been reported in the
circumstellar envelopes of only two evolved stars: the Mira star AU Geminorum
and the hypergiant NML Cygni. We present Very Large Array (VLA) observations of
the 1665, 1667, and excited-state 4750 MHz mainline OH transitions in AU Gem
and Expanded Ve... | astro-ph | excitedstate oh maser emission has previously been reported in the circumstellar envelopes of only two evolved stars the mira star au geminorum and the hypergiant nml cygni we present very large array vla observations of the 1665 1667 and excitedstate 4750 mhz mainline oh transitions in au gem and expanded very large a... | [['excitedstate', 'oh', 'maser', 'emission', 'has', 'previously', 'been', 'reported', 'in', 'the', 'circumstellar', 'envelopes', 'of', 'only', 'two', 'evolved', 'stars', 'the', 'mira', 'star', 'au', 'geminorum', 'and', 'the', 'hypergiant', 'nml', 'cygni', 'we', 'present', 'very', 'large', 'array', 'vla', 'observations'... | [-0.07348142847747843, 0.09470452198641297, 0.001124991357025039, 0.039479658447039136, -0.06549582440093848, -0.1435513027770057, 0.07296506116150561, 0.5095951984168132, -0.13755145232392357, -0.2845428501716088, 0.06426018696396768, -0.2723274472670231, -0.027162543176323432, 0.1262933410074282, -0.00909757097938092... |
707.3789 | Interactive Small-Step Algorithms II: Abstract State Machines and
the<br> Characterization Theorem | In earlier work, the Abstract State Machine Thesis -- that arbitrary
algorithms are behaviorally equivalent to abstract state machines -- was
established for several classes of algorithms, including ordinary, interactive,
small-step algorithms. This was accomplished on the basis of axiomatizations of
these classes of... | cs.LO | in earlier work the abstract state machine thesis that arbitrary algorithms are behaviorally equivalent to abstract state machines was established for several classes of algorithms including ordinary interactive smallstep algorithms this was accomplished on the basis of axiomatizations of these classes of algorithms in... | [['in', 'earlier', 'work', 'the', 'abstract', 'state', 'machine', 'thesis', 'that', 'arbitrary', 'algorithms', 'are', 'behaviorally', 'equivalent', 'to', 'abstract', 'state', 'machines', 'was', 'established', 'for', 'several', 'classes', 'of', 'algorithms', 'including', 'ordinary', 'interactive', 'smallstep', 'algorith... | [-0.06457968357866731, 0.06298697758523494, -0.10553589672494082, 0.11549480369869321, -0.13761847063519614, -0.16522404303440802, 0.06682433699614104, 0.42424842570390964, -0.25771443195997473, -0.3247203756555668, 0.104058467253416, -0.22867457208476594, -0.113936174304489, 0.16876205546712433, -0.13978727779029237, ... |
707.379 | Conditions for exact equivalence of Kaluza-Klein and Yang-Mills theories | Although it is well known that Kaluza-Klein and Yang-Mills theories define
equivalent structures on principal bundles, the general conditions for
equivalence of their Lagrangians have not been explicitly stated. In this paper
we address the conditions for equivalence. The formulation of these conditions
is based on p... | gr-qc math-ph math.MP quant-ph | although it is well known that kaluzaklein and yangmills theories define equivalent structures on principal bundles the general conditions for equivalence of their lagrangians have not been explicitly stated in this paper we address the conditions for equivalence the formulation of these conditions is based on previous... | [['although', 'it', 'is', 'well', 'known', 'that', 'kaluzaklein', 'and', 'yangmills', 'theories', 'define', 'equivalent', 'structures', 'on', 'principal', 'bundles', 'the', 'general', 'conditions', 'for', 'equivalence', 'of', 'their', 'lagrangians', 'have', 'not', 'been', 'explicitly', 'stated', 'in', 'this', 'paper', ... | [-0.16916211151970867, 0.14989105491465418, -0.07901826623033305, 0.09928032321552618, -0.12345983492861924, -0.13985579074080526, -0.04252175443940618, 0.3379573512954709, -0.1900363120971161, -0.2556107697952437, 0.07217656493395608, -0.20646234958997514, -0.17643837274505142, 0.12761181727677706, -0.0503935107650856... |
707.3791 | BPS Z(N) String Tensions, Sine Law and Casimir Scaling and Integrable
Field Theories | We consider a Yang-Mills-Higgs theory with spontaneous symmetry breaking of
the gauge group G -> U(1)^r -> C(G), with C(G) being the center of G. We study
two vacua solutions of the theory which produce this symmetry breaking. We show
that for one of these vacua, the theory in the Coulomb phase has the mass
spectrum ... | hep-th hep-lat hep-ph | we consider a yangmillshiggs theory with spontaneous symmetry breaking of the gauge group g u1r cg with cg being the center of g we study two vacua solutions of the theory which produce this symmetry breaking we show that for one of these vacua the theory in the coulomb phase has the mass spectrum of particles and mono... | [['we', 'consider', 'a', 'yangmillshiggs', 'theory', 'with', 'spontaneous', 'symmetry', 'breaking', 'of', 'the', 'gauge', 'group', 'g', 'u1r', 'cg', 'with', 'cg', 'being', 'the', 'center', 'of', 'g', 'we', 'study', 'two', 'vacua', 'solutions', 'of', 'the', 'theory', 'which', 'produce', 'this', 'symmetry', 'breaking', '... | [-0.1666603167792066, 0.19613415288189665, -0.06915888556112082, 0.08430084887032326, -0.03709611949654153, -0.15066697180318908, -0.02282316856420575, 0.31848422919328395, -0.2213869302533567, -0.2467876433311269, 0.08936439170621527, -0.3023072494050631, -0.11407256583348872, 0.121258289901874, -0.006934831047860476,... |
707.3792 | The Bipolar Engines of post-AGB stars: Transient Dynamos and Common
Envelopes | The physical mechanism(s) responsible for transitioning from a spherical
Asymptotic Giant Branch (AGB) star to an asymmetric post-AGB (pAGB) object is
poorly understood. In particular, excess momenta in the outflows of pAGB
objects suggest that a binary may be required to supply an additional source of
energy and ang... | astro-ph | the physical mechanisms responsible for transitioning from a spherical asymptotic giant branch agb star to an asymmetric postagb pagb object is poorly understood in particular excess momenta in the outflows of pagb objects suggest that a binary may be required to supply an additional source of energy and angular moment... | [['the', 'physical', 'mechanisms', 'responsible', 'for', 'transitioning', 'from', 'a', 'spherical', 'asymptotic', 'giant', 'branch', 'agb', 'star', 'to', 'an', 'asymmetric', 'postagb', 'pagb', 'object', 'is', 'poorly', 'understood', 'in', 'particular', 'excess', 'momenta', 'in', 'the', 'outflows', 'of', 'pagb', 'object... | [-0.1416517168343548, 0.14483249988254002, -0.08072385987954124, 0.10425648676373134, -0.11596486191715925, -0.033091971395357, 0.018491750752579094, 0.36790831171916066, -0.23053296871804138, -0.31236260463397797, 0.0856055575798476, -0.2006634270334037, -0.05069292416100815, 0.20237129296617118, -0.08015195937845469,... |
707.3793 | Evidence for a Preferred Handedness of Spiral Galaxies | In this article I study the distribution of spiral galaxies in the Sloan
Digital Sky Survey (SDSS) to investigate whether the universe has an overall
handedness. A preference for spiral galaxies in one sector of the sky to be
left-handed or right-handed spirals would indicate a preferred handedness. The
SDSS data sho... | astro-ph | in this article i study the distribution of spiral galaxies in the sloan digital sky survey sdss to investigate whether the universe has an overall handedness a preference for spiral galaxies in one sector of the sky to be lefthanded or righthanded spirals would indicate a preferred handedness the sdss data show a stro... | [['in', 'this', 'article', 'i', 'study', 'the', 'distribution', 'of', 'spiral', 'galaxies', 'in', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'to', 'investigate', 'whether', 'the', 'universe', 'has', 'an', 'overall', 'handedness', 'a', 'preference', 'for', 'spiral', 'galaxies', 'in', 'one', 'sector', 'of', 'the... | [-0.139627255897969, 0.08517357355775311, -0.04102412582747638, 0.044564106506295505, -0.163498828060925, -0.003679092478007078, -0.030928012127056717, 0.42251942755281924, -0.2119939866513014, -0.29759946521371605, 0.059780317660421134, -0.33208786211535335, -0.01889791932143271, 0.1508837279509753, 0.0011716970987617... |
707.3794 | Binary Models for Marginal Independence | Log-linear models are a classical tool for the analysis of contingency
tables. In particular, the subclass of graphical log-linear models provides a
general framework for modelling conditional independences. However, with the
exception of special structures, marginal independence hypotheses cannot be
accommodated by ... | math.ST stat.TH | loglinear models are a classical tool for the analysis of contingency tables in particular the subclass of graphical loglinear models provides a general framework for modelling conditional independences however with the exception of special structures marginal independence hypotheses cannot be accommodated by these tra... | [['loglinear', 'models', 'are', 'a', 'classical', 'tool', 'for', 'the', 'analysis', 'of', 'contingency', 'tables', 'in', 'particular', 'the', 'subclass', 'of', 'graphical', 'loglinear', 'models', 'provides', 'a', 'general', 'framework', 'for', 'modelling', 'conditional', 'independences', 'however', 'with', 'the', 'exce... | [-0.04099230936993539, 0.039827440552631, -0.12312062938500495, 0.15481913840928435, -0.12483079104691092, -0.18975149488491244, 0.0639399895402025, 0.4376854810075168, -0.2649263394792585, -0.3225183040991317, 0.09790814878082542, -0.2173007143046163, -0.17762862667475357, 0.17556565401083143, -0.0892443510849899, 0.0... |
707.3795 | The halo by halo missing baryon problem | The global missing baryon problem - that the sum of observed baryons falls
short of the number expected form BBN - is well known. In addition to this,
there is also a local missing baryon problem that applies to individual dark
matter halos. This halo by halo missing baryon problem is such that the
observed mass frac... | astro-ph | the global missing baryon problem that the sum of observed baryons falls short of the number expected form bbn is well known in addition to this there is also a local missing baryon problem that applies to individual dark matter halos this halo by halo missing baryon problem is such that the observed mass fraction of b... | [['the', 'global', 'missing', 'baryon', 'problem', 'that', 'the', 'sum', 'of', 'observed', 'baryons', 'falls', 'short', 'of', 'the', 'number', 'expected', 'form', 'bbn', 'is', 'well', 'known', 'in', 'addition', 'to', 'this', 'there', 'is', 'also', 'a', 'local', 'missing', 'baryon', 'problem', 'that', 'applies', 'to', '... | [-0.11542909351028217, 0.16464058492958764, -0.0634187163059948, 0.16531584516011236, -0.09242701000278063, -0.03932922230215871, 0.06897400837846612, 0.3172608725064548, -0.22125190183634066, -0.3379585865088774, -0.009815528041519623, -0.3312199513804708, -0.01758876932608959, 0.10672018876679612, 0.00688169001893119... |
707.3796 | Methods of Modern Differential Geometry in Quantum Chemistry: TD
Theories on Grassmann and Hartree-Fock Manifolds | Hamiltonian and Schrodinger evolution equations on finite-dimensional
projective space are analyzed in detail. Hartree-Fock (HF) manifold is
introduced as a submanifold of many electron projective space of states.
Evolution equations, exact and linearized, on this manifold are studied.
Comparison of matrices of linea... | physics.chem-ph math-ph math.MP | hamiltonian and schrodinger evolution equations on finitedimensional projective space are analyzed in detail hartreefock hf manifold is introduced as a submanifold of many electron projective space of states evolution equations exact and linearized on this manifold are studied comparison of matrices of linearized schro... | [['hamiltonian', 'and', 'schrodinger', 'evolution', 'equations', 'on', 'finitedimensional', 'projective', 'space', 'are', 'analyzed', 'in', 'detail', 'hartreefock', 'hf', 'manifold', 'is', 'introduced', 'as', 'a', 'submanifold', 'of', 'many', 'electron', 'projective', 'space', 'of', 'states', 'evolution', 'equations', ... | [-0.12105285027169073, 0.10653158534475662, -0.014205904200781274, 0.09812870795131667, 2.5208768093114275e-05, -0.10233440782821221, -0.007629755523437701, 0.3316282263869862, -0.22235532762924973, -0.24737710766695278, 0.05670280705068743, -0.3165160332330697, -0.13756956496416664, 0.13697973149661108, 0.046327765937... |
707.3797 | Origin and propagation of cosmic rays (some highlights) | The detection of high-energy particles, cosmic rays (CRs), deep inside the
heliosphere implies that there are, at least, three distinctly different stages
in the lifetime of a CR particle: acceleration, propagation in the interstellar
medium (ISM), and propagation in the heliosphere. Gamma rays produced by
interactio... | astro-ph | the detection of highenergy particles cosmic rays crs deep inside the heliosphere implies that there are at least three distinctly different stages in the lifetime of a cr particle acceleration propagation in the interstellar medium ism and propagation in the heliosphere gamma rays produced by interactions of crs with ... | [['the', 'detection', 'of', 'highenergy', 'particles', 'cosmic', 'rays', 'crs', 'deep', 'inside', 'the', 'heliosphere', 'implies', 'that', 'there', 'are', 'at', 'least', 'three', 'distinctly', 'different', 'stages', 'in', 'the', 'lifetime', 'of', 'a', 'cr', 'particle', 'acceleration', 'propagation', 'in', 'the', 'inter... | [-0.09925464778216864, 0.21873286414291607, -0.036817549864957805, 0.09748426804796231, -0.037328508249599456, -0.022003363079029666, -0.03886748254895672, 0.4454378949262756, -0.2580246184182869, -0.34273879905808563, 0.005347340689079205, -0.2910025782175054, -0.03976146459641043, 0.2272859815525445, 0.03101573067415... |
707.3798 | Pressure-induced metal-insulator transition in MgV_2O_4 | On the basis of experimental thermoelectric power results and ab initio
calculations, we propose that a metal-insulator transition takes place at high
pressure (approximately 6 GPa) in MgV_2O_4.
| cond-mat.str-el | on the basis of experimental thermoelectric power results and ab initio calculations we propose that a metalinsulator transition takes place at high pressure approximately 6 gpa in mgv_2o_4 | [['on', 'the', 'basis', 'of', 'experimental', 'thermoelectric', 'power', 'results', 'and', 'ab', 'initio', 'calculations', 'we', 'propose', 'that', 'a', 'metalinsulator', 'transition', 'takes', 'place', 'at', 'high', 'pressure', 'approximately', '6', 'gpa', 'in', 'mgv_2o_4']] | [-0.14838508657287872, 0.14567135992027552, -0.08115310629364103, -0.07835250440984964, 0.009778187177809221, -0.10461679737948414, 0.2059045751645629, 0.46085843523698194, -0.19327228513014102, -0.28785585093178917, -0.026615100750599856, -0.36905995942652225, -0.15335650984863086, 0.16273944800819404, 0.1158282265532... |
707.3799 | Equivariant Satake category and Kostant-Whittaker reduction | We explain (following V. Drinfeld) how the equivariant derived category of
the affine Grassmannian can be described in terms of coherent sheaves on the
Langlands dual Lie algebra equivariant with respect to the adjoint action, due
to some old results of V. Ginzburg. The global cohomology functor corresponds
under thi... | math.RT | we explain following v drinfeld how the equivariant derived category of the affine grassmannian can be described in terms of coherent sheaves on the langlands dual lie algebra equivariant with respect to the adjoint action due to some old results of v ginzburg the global cohomology functor corresponds under this identi... | [['we', 'explain', 'following', 'v', 'drinfeld', 'how', 'the', 'equivariant', 'derived', 'category', 'of', 'the', 'affine', 'grassmannian', 'can', 'be', 'described', 'in', 'terms', 'of', 'coherent', 'sheaves', 'on', 'the', 'langlands', 'dual', 'lie', 'algebra', 'equivariant', 'with', 'respect', 'to', 'the', 'adjoint', ... | [-0.17075191395752856, -0.011399204399749901, -0.12561219774054744, 0.0784299041214605, -0.15955668283148414, -0.15158869982985532, -0.04408563887164722, 0.3011143184802701, -0.4412510866171524, -0.1608848646679786, 0.07272612417953303, -0.12244495996727353, -0.15720860916807983, 0.14665849245796228, -0.278382606635414... |
707.38 | Higgs production at the LHC in warped extra-dimensional models | The extra-dimensional model in which the bulk geometry is a slice of anti-de
Sitter space is a particularly attractive extension of the Standard Model as it
allows to address the gauge hierarchy problem, as well as the mass hierarchy
prevailing among fermions. However, to allow for the masses of the Kaluza-Klein
exci... | hep-ph | the extradimensional model in which the bulk geometry is a slice of antide sitter space is a particularly attractive extension of the standard model as it allows to address the gauge hierarchy problem as well as the mass hierarchy prevailing among fermions however to allow for the masses of the kaluzaklein excitations ... | [['the', 'extradimensional', 'model', 'in', 'which', 'the', 'bulk', 'geometry', 'is', 'a', 'slice', 'of', 'antide', 'sitter', 'space', 'is', 'a', 'particularly', 'attractive', 'extension', 'of', 'the', 'standard', 'model', 'as', 'it', 'allows', 'to', 'address', 'the', 'gauge', 'hierarchy', 'problem', 'as', 'well', 'as'... | [-0.07744654683366177, 0.29337793533935624, -0.05244785341213868, 0.16673796553443748, -0.10472243078934249, -0.17791066173544173, 0.04202344933003988, 0.3098162097195464, -0.2220199713639925, -0.24715868506820932, 0.0362960277819976, -0.2557322217680555, 0.009486866294987179, 0.08616074842340764, 0.028847988279316054,... |
707.3801 | $N_{\p}$-type quotient modules on the torus | Structure of the quotient modules in $\hh$ is very complicated. A good
understanding of some special examples will shed light on the general picture.
This paper studies the so-call $N_{\p}$-type quotient modules, namely, quotient
modules of the form $\hh\ominus [z-\p]$, where $\p (w)$ is a function in the
classical H... | math.FA | structure of the quotient modules in hh is very complicated a good understanding of some special examples will shed light on the general picture this paper studies the socall n_ptype quotient modules namely quotient modules of the form hhominus zp where p w is a function in the classical hardy space h2g and zp is the s... | [['structure', 'of', 'the', 'quotient', 'modules', 'in', 'hh', 'is', 'very', 'complicated', 'a', 'good', 'understanding', 'of', 'some', 'special', 'examples', 'will', 'shed', 'light', 'on', 'the', 'general', 'picture', 'this', 'paper', 'studies', 'the', 'socall', 'n_ptype', 'quotient', 'modules', 'namely', 'quotient', ... | [-0.1707889411357765, 0.04947936755678292, -0.09001488986770424, 0.0930641564891119, -0.11511266110674216, -0.1689161489393269, -0.01023666969673143, 0.34353990040803223, -0.3751304532202442, -0.17288940027356148, 0.09648549868437473, -0.23240758452219157, -0.18923554411471893, 0.2444024086835679, -0.13003731854887826,... |
707.3802 | Inconsistency of the non-standard definition of work | We show that the recently postulated non-standard definition of work
proportional to force variation rather than to displacement [A. Imparato and L.
Peliti, cond-mat arXiv:0706.1134v1] is thermodynamically inconsistent at both
microscopic and macroscopic scales and leads to non-physical results, including
free energy... | cond-mat.stat-mech cond-mat.soft | we show that the recently postulated nonstandard definition of work proportional to force variation rather than to displacement a imparato and l peliti condmat arxiv07061134v1 is thermodynamically inconsistent at both microscopic and macroscopic scales and leads to nonphysical results including free energy changes that... | [['we', 'show', 'that', 'the', 'recently', 'postulated', 'nonstandard', 'definition', 'of', 'work', 'proportional', 'to', 'force', 'variation', 'rather', 'than', 'to', 'displacement', 'a', 'imparato', 'and', 'l', 'peliti', 'condmat', 'arxiv07061134v1', 'is', 'thermodynamically', 'inconsistent', 'at', 'both', 'microscop... | [-0.08949041346331006, 0.2166580349591601, -0.10649782491078519, 0.07900080361413649, -0.13421690391133662, -0.14759353143365486, 0.023387580419100985, 0.28895524853293825, -0.22360689598945496, -0.3376079417117264, 0.013609054032713175, -0.26125302927001665, -0.1254818825678819, 0.19294398356957929, -0.067480169302459... |
707.3803 | Energy Measurements and Preparation of Canonical Phase States of a
Nano-Mechanical Resonator | We show that a continuous quantum non-demolition measurement of the energy of
a nanomechanical resonator can be achieved by monitoring the resonator with a
quantum point contact via a Cooper-pair box. This technique can further be used
to prepare highly non-classical states of two resonators, such as canonical
phase-... | quant-ph cond-mat.mes-hall | we show that a continuous quantum nondemolition measurement of the energy of a nanomechanical resonator can be achieved by monitoring the resonator with a quantum point contact via a cooperpair box this technique can further be used to prepare highly nonclassical states of two resonators such as canonical phasereferenc... | [['we', 'show', 'that', 'a', 'continuous', 'quantum', 'nondemolition', 'measurement', 'of', 'the', 'energy', 'of', 'a', 'nanomechanical', 'resonator', 'can', 'be', 'achieved', 'by', 'monitoring', 'the', 'resonator', 'with', 'a', 'quantum', 'point', 'contact', 'via', 'a', 'cooperpair', 'box', 'this', 'technique', 'can',... | [-0.14608207990035968, 0.24169878145955778, -0.11121505169473865, -0.025575575257082366, 0.009032998561721158, -0.24199271384902574, 0.0979806141220723, 0.3793825472670573, -0.2411870766017172, -0.25396539070815954, 0.03175214216699479, -0.2615944049148648, -0.09250189389826523, 0.2800788333363555, -0.02812583002486024... |
707.3804 | Approximate reduction of dynamical systems | The reduction of dynamical systems has a rich history, with many important
applications related to stability, control and verification. Reduction of
nonlinear systems is typically performed in an exact manner - as is the case
with mechanical systems with symmetry--which, unfortunately, limits the type of
systems to w... | math.OC math.DS | the reduction of dynamical systems has a rich history with many important applications related to stability control and verification reduction of nonlinear systems is typically performed in an exact manner as is the case with mechanical systems with symmetrywhich unfortunately limits the type of systems to which it can... | [['the', 'reduction', 'of', 'dynamical', 'systems', 'has', 'a', 'rich', 'history', 'with', 'many', 'important', 'applications', 'related', 'to', 'stability', 'control', 'and', 'verification', 'reduction', 'of', 'nonlinear', 'systems', 'is', 'typically', 'performed', 'in', 'an', 'exact', 'manner', 'as', 'is', 'the', 'ca... | [-0.11898372183990213, 0.06766058343974261, -0.08884364655031297, 0.05530757541834776, -0.060028999565953485, -0.11093339964281768, 0.020717024776027222, 0.3292413086007188, -0.27136442313825054, -0.30457542471139504, 0.1892736608764731, -0.23514321599421756, -0.17232814559684997, 0.2685697212871304, -0.102381164224685... |
707.3805 | Subsonic Mechanical Alignment of Irregular Grains | We show that grains can be efficiently aligned by interacting with a subsonic
gaseous flow. The alignment arises from grains having irregularities that
scatter atoms with different efficiency in the right and left directions. The
grains tend to align with long axes perpendicular to magnetic field, which
corresponds t... | astro-ph | we show that grains can be efficiently aligned by interacting with a subsonic gaseous flow the alignment arises from grains having irregularities that scatter atoms with different efficiency in the right and left directions the grains tend to align with long axes perpendicular to magnetic field which corresponds to dav... | [['we', 'show', 'that', 'grains', 'can', 'be', 'efficiently', 'aligned', 'by', 'interacting', 'with', 'a', 'subsonic', 'gaseous', 'flow', 'the', 'alignment', 'arises', 'from', 'grains', 'having', 'irregularities', 'that', 'scatter', 'atoms', 'with', 'different', 'efficiency', 'in', 'the', 'right', 'and', 'left', 'direc... | [-0.13460649196028274, 0.2293955527560471, -0.029810332632684088, 0.03328351112681308, -0.07155367204701746, -0.11390706927624422, -0.047533938830549065, 0.4519894434163323, -0.2859702005667926, -0.30397274664470125, -0.014582187253316599, -0.28554969014261256, 0.013549927201775181, 0.1208693512062264, 0.00651307730608... |
707.3806 | Search for Frame-Dragging-Like Signals Close to Spinning Superconductors | High-resolution accelerometer and laser gyroscope measurements were performed
in the vicinity of spinning rings at cryogenic temperatures. After passing a
critical temperature, which does not coincide with the material's
superconducting temperature, the angular acceleration and angular velocity
applied to the rotatin... | gr-qc | highresolution accelerometer and laser gyroscope measurements were performed in the vicinity of spinning rings at cryogenic temperatures after passing a critical temperature which does not coincide with the materials superconducting temperature the angular acceleration and angular velocity applied to the rotating ring ... | [['highresolution', 'accelerometer', 'and', 'laser', 'gyroscope', 'measurements', 'were', 'performed', 'in', 'the', 'vicinity', 'of', 'spinning', 'rings', 'at', 'cryogenic', 'temperatures', 'after', 'passing', 'a', 'critical', 'temperature', 'which', 'does', 'not', 'coincide', 'with', 'the', 'materials', 'superconducti... | [-0.1584358983298126, 0.20574724268568242, -0.05299134512006887, 0.02856069275071757, -0.051864155168151294, -0.14353785875265881, 0.012848661418679177, 0.35865950419711284, -0.22824299936151546, -0.3477256903862393, 0.08451296983602388, -0.30276293382548647, -0.03121966334222347, 0.26094059450645624, -0.01479957751998... |
707.3807 | How to be correct, lazy and efficient ? | This paper is an introduction to Lambdix, a lazy Lisp interpreter implemented
at the Research Laboratory of Paris XI University (Laboratoire de Recherche en
Informatique, Orsay). Lambdix was devised in the course of an investigation
into the relationship between the semantics of programming languages and their
implem... | cs.PL | this paper is an introduction to lambdix a lazy lisp interpreter implemented at the research laboratory of paris xi university laboratoire de recherche en informatique orsay lambdix was devised in the course of an investigation into the relationship between the semantics of programming languages and their implementatio... | [['this', 'paper', 'is', 'an', 'introduction', 'to', 'lambdix', 'a', 'lazy', 'lisp', 'interpreter', 'implemented', 'at', 'the', 'research', 'laboratory', 'of', 'paris', 'xi', 'university', 'laboratoire', 'de', 'recherche', 'en', 'informatique', 'orsay', 'lambdix', 'was', 'devised', 'in', 'the', 'course', 'of', 'an', 'i... | [-0.08035403397187348, 0.012386414936517594, -0.11961348120973486, 0.09224403180575093, -0.15837737292631704, -0.11746041294848682, -0.016033815820633932, 0.3671841360156195, -0.2280753702127739, -0.3354028391557327, 0.08890781576907181, -0.26606244666407397, -0.1408690966773724, 0.195475876956429, -0.14818448363465891... |
707.3808 | Coherently driven non-classical light emission from a quantum dot | Narrow line-widths and the possibility of enhanced spontaneous emission via
coupling to microcavities make semiconductor quantum dots ideal for harnessing
coherent quantum phenomena at the single photon level. So far, however, all
approaches have relied on incoherent pumping, which limits the desirable
properties of ... | cond-mat.mes-hall | narrow linewidths and the possibility of enhanced spontaneous emission via coupling to microcavities make semiconductor quantum dots ideal for harnessing coherent quantum phenomena at the single photon level so far however all approaches have relied on incoherent pumping which limits the desirable properties of the emi... | [['narrow', 'linewidths', 'and', 'the', 'possibility', 'of', 'enhanced', 'spontaneous', 'emission', 'via', 'coupling', 'to', 'microcavities', 'make', 'semiconductor', 'quantum', 'dots', 'ideal', 'for', 'harnessing', 'coherent', 'quantum', 'phenomena', 'at', 'the', 'single', 'photon', 'level', 'so', 'far', 'however', 'a... | [-0.12518683379810108, 0.20328203670302392, -0.048049276729667544, 0.054964967380116754, -0.011264891248140344, -0.20061213687006244, 0.06469765871490135, 0.4219837264767043, -0.25173068171213, -0.2788797690834206, -0.004027912496935744, -0.27520873206072394, -0.03833542531006094, 0.25738439152255316, 0.039647329784229... |
707.3809 | Characterization of the hot Neptune GJ 436b with Spitzer and
ground-based observations | We present Spitzer Space Telescope infrared photometry of a secondary eclipse
of the hot Neptune GJ436b. The observations were obtained using the 8-micron
band of the InfraRed Array Camera (IRAC). The data spanning the predicted time
of secondary eclipse show a clear flux decrement with the expected shape and
duratio... | astro-ph | we present spitzer space telescope infrared photometry of a secondary eclipse of the hot neptune gj436b the observations were obtained using the 8micron band of the infrared array camera irac the data spanning the predicted time of secondary eclipse show a clear flux decrement with the expected shape and duration the o... | [['we', 'present', 'spitzer', 'space', 'telescope', 'infrared', 'photometry', 'of', 'a', 'secondary', 'eclipse', 'of', 'the', 'hot', 'neptune', 'gj436b', 'the', 'observations', 'were', 'obtained', 'using', 'the', '8micron', 'band', 'of', 'the', 'infrared', 'array', 'camera', 'irac', 'the', 'data', 'spanning', 'the', 'p... | [-0.08887300315345156, 0.11544675064626439, -0.11008728841994087, 0.05081351845332518, -0.08624378170432716, -0.0882068364929151, 0.10496165054721822, 0.4045597105447588, -0.17694627672959728, -0.40698264308659166, 0.06678543865423778, -0.31798040956943213, -0.046983599397032685, 0.1769227900943751, -0.0910517439503094... |
707.381 | Levi-Civita regularization and geodesic flows for the `curved' Kepler
problem | We introduce the regularization Levi-Civita parameter for the `curved
Kepler', i.e., motion under the `Kepler-Coulomb' potential in a configuration
space with any constant curvature and metric of any signature type. Consistent
use of this parameter allows to solve the problem of motion (orbit shape and
time evolution... | math-ph math.MP | we introduce the regularization levicivita parameter for the curved kepler ie motion under the keplercoulomb potential in a configuration space with any constant curvature and metric of any signature type consistent use of this parameter allows to solve the problem of motion orbit shape and time evolution along the orb... | [['we', 'introduce', 'the', 'regularization', 'levicivita', 'parameter', 'for', 'the', 'curved', 'kepler', 'ie', 'motion', 'under', 'the', 'keplercoulomb', 'potential', 'in', 'a', 'configuration', 'space', 'with', 'any', 'constant', 'curvature', 'and', 'metric', 'of', 'any', 'signature', 'type', 'consistent', 'use', 'o... | [-0.1472884574899006, 0.13151734746833346, -0.06549386360195171, 0.04718559990465699, -0.14530644793705194, -0.13109437467462812, 0.004819991068258264, 0.36758160834330966, -0.26183675733090916, -0.2740022570113145, 0.08487398742994902, -0.23644619523506874, -0.1358989963773638, 0.18706658641190071, -0.0847434407296720... |
707.3811 | Global regulation of genome duplication in eukaryotes: an overview from
the epifluorescence microscope | In eukaryotes, DNA replication is initiated along each chromosome at multiple
sites called replication origins. Locally, each replication origin is
"licensed", or specified, at the end of the M and the beginning of G1 phases of
the cell cycle. During S phase when DNA synthesis takes place, origins are
activated in st... | q-bio.GN | in eukaryotes dna replication is initiated along each chromosome at multiple sites called replication origins locally each replication origin is licensed or specified at the end of the m and the beginning of g1 phases of the cell cycle during s phase when dna synthesis takes place origins are activated in stages corres... | [['in', 'eukaryotes', 'dna', 'replication', 'is', 'initiated', 'along', 'each', 'chromosome', 'at', 'multiple', 'sites', 'called', 'replication', 'origins', 'locally', 'each', 'replication', 'origin', 'is', 'licensed', 'or', 'specified', 'at', 'the', 'end', 'of', 'the', 'm', 'and', 'the', 'beginning', 'of', 'g1', 'phas... | [-0.18443338175097274, 0.16025461684661826, -0.025554641985541415, 0.029961654393830233, -0.02712310539209284, -0.11843583693779591, 0.1222301397365906, 0.37556762092022433, -0.2813024285611593, -0.2490016489703622, 0.09644575278248844, -0.19885804986309571, -0.15902653760406085, 0.12617979304826196, -0.075879020274927... |
707.3812 | Foliations on quaternion CR-submanifolds | The purpose of this paper is to study the canonical foliations of a
quaternion CR-submanifold of a quaternion K\"{a}hler manifold.
| math.DG | the purpose of this paper is to study the canonical foliations of a quaternion crsubmanifold of a quaternion kahler manifold | [['the', 'purpose', 'of', 'this', 'paper', 'is', 'to', 'study', 'the', 'canonical', 'foliations', 'of', 'a', 'quaternion', 'crsubmanifold', 'of', 'a', 'quaternion', 'kahler', 'manifold']] | [-0.25283102905377747, -0.0016905895434319973, -0.1491742294281721, 0.08223269768059253, -0.18098567575216293, -0.06983118667267263, -0.13530278498656118, 0.3175205536186695, -0.24378718324005605, -0.17782064010389148, 0.07131162723526359, -0.18568544816225768, -0.26814436353743076, 0.11743759624660015, -0.199837920069... |
707.3813 | Testing cold dark matter with the low mass Tully-Fisher relation | The galaxy circular velocity function at small masses is related to the
matter power spectrum on small scales. Although this function is well-studied
for Local Group dwarfs, theoretical predictions and observational measurements
are difficult for satellite galaxies, because of ram pressure and tidal
stripping. By con... | astro-ph | the galaxy circular velocity function at small masses is related to the matter power spectrum on small scales although this function is wellstudied for local group dwarfs theoretical predictions and observational measurements are difficult for satellite galaxies because of ram pressure and tidal stripping by contrast i... | [['the', 'galaxy', 'circular', 'velocity', 'function', 'at', 'small', 'masses', 'is', 'related', 'to', 'the', 'matter', 'power', 'spectrum', 'on', 'small', 'scales', 'although', 'this', 'function', 'is', 'wellstudied', 'for', 'local', 'group', 'dwarfs', 'theoretical', 'predictions', 'and', 'observational', 'measurement... | [-0.06426816030624181, 0.13029315082146686, -0.07886610094062758, 0.13002949315516352, -0.12459014027754402, -0.0520447513826385, 0.02900930881919541, 0.396332554873966, -0.15859884656240025, -0.3709460897451807, 0.024380063595758242, -0.3179498095210497, -0.01991407683893264, 0.2314377874297239, 0.010833744203583115, ... |
707.3814 | Strangulation in Galaxy Groups | We use a cosmological chemodynamical simulation to study how the group
environment impacts the star formation properties of disk galaxies. The
simulated group has a total mass of M~8x10^12 Msun and a total X-ray luminosity
of L_X~10^41 erg s^-1. Our simulation suggests that ram pressure is not
sufficient in this grou... | astro-ph | we use a cosmological chemodynamical simulation to study how the group environment impacts the star formation properties of disk galaxies the simulated group has a total mass of m8x1012 msun and a total xray luminosity of l_x1041 erg s1 our simulation suggests that ram pressure is not sufficient in this group to remove... | [['we', 'use', 'a', 'cosmological', 'chemodynamical', 'simulation', 'to', 'study', 'how', 'the', 'group', 'environment', 'impacts', 'the', 'star', 'formation', 'properties', 'of', 'disk', 'galaxies', 'the', 'simulated', 'group', 'has', 'a', 'total', 'mass', 'of', 'm8x1012', 'msun', 'and', 'a', 'total', 'xray', 'luminos... | [-0.10063691617654323, 0.09047931343940395, -0.12524469510711686, 0.07418713393569708, -0.08143445245277267, 0.011632024884483842, 0.03820302170974765, 0.40289230330652276, -0.18175239920031366, -0.31242253656260843, 0.045828807022866555, -0.25305473663827927, 0.04527212203978453, 0.19919071340565245, -0.03762065328462... |
707.3815 | Bent-Double Radio Sources as Probes of the Intragroup Medium | Galaxy groups likely contain a significant fraction of the total baryonic
mass in the local universe within their intragroup medium (IGM). However, aside
from a handful of UV absorption line and X-ray observations, almost nothing is
known about the IGM. We present early results from a research program that
combines l... | astro-ph | galaxy groups likely contain a significant fraction of the total baryonic mass in the local universe within their intragroup medium igm however aside from a handful of uv absorption line and xray observations almost nothing is known about the igm we present early results from a research program that combines lowfrequen... | [['galaxy', 'groups', 'likely', 'contain', 'a', 'significant', 'fraction', 'of', 'the', 'total', 'baryonic', 'mass', 'in', 'the', 'local', 'universe', 'within', 'their', 'intragroup', 'medium', 'igm', 'however', 'aside', 'from', 'a', 'handful', 'of', 'uv', 'absorption', 'line', 'and', 'xray', 'observations', 'almost', ... | [-0.0654892191411026, 0.09451712072236709, -0.07620424064256812, 0.0730253041994768, -0.15293400155841022, -0.027140196516386342, 0.10968131649868704, 0.47228317835959055, -0.14463416540053903, -0.33584771375422195, 0.05567820752990903, -0.33184809413968874, -0.038669121331505234, 0.16925841355596177, 0.034592382897753... |
707.3816 | Charging of Fractal Dust Agglomerates in a Plasma Environment | The charge on micron-sized dust grains plays a crucial role in the structure
and evolution of forming aggregates within the dust population during the
coagulation process. The manner in which the charge is arranged on developing
irregular structures can affect the fractal dimension of aggregates formed
during collisi... | astro-ph | the charge on micronsized dust grains plays a crucial role in the structure and evolution of forming aggregates within the dust population during the coagulation process the manner in which the charge is arranged on developing irregular structures can affect the fractal dimension of aggregates formed during collisions ... | [['the', 'charge', 'on', 'micronsized', 'dust', 'grains', 'plays', 'a', 'crucial', 'role', 'in', 'the', 'structure', 'and', 'evolution', 'of', 'forming', 'aggregates', 'within', 'the', 'dust', 'population', 'during', 'the', 'coagulation', 'process', 'the', 'manner', 'in', 'which', 'the', 'charge', 'is', 'arranged', 'on... | [-0.08969776458214603, 0.1596422856350596, -0.09166150729069648, 0.06648072623148316, 0.028223061728199696, -0.05707571913375158, 0.0028178652568795646, 0.37489284035572085, -0.24737540965514915, -0.2866573797678844, 0.03929790646050427, -0.2684279437044991, -0.07072224270288612, 0.10505116738734303, -0.005729481790516... |
707.3817 | Electro-Optic Search for Critical Divergence of the Charge-Density-Wave
Diffusion Constant at the Onset of Depinning | We have used electro-reflectance measurements to study charge-density-wave
(CDW) polarization dynamics at voltages near the CDW depinning onset (Von) in
the quasi-one-dimensional conductor K0.3MoO3 ("blue bronze"). For low voltages,
where the phase-slip rate is low, it is expected that the polarization
relaxation tim... | cond-mat.str-el | we have used electroreflectance measurements to study chargedensitywave cdw polarization dynamics at voltages near the cdw depinning onset von in the quasionedimensional conductor k03moo3 blue bronze for low voltages where the phaseslip rate is low it is expected that the polarization relaxation time should be inversel... | [['we', 'have', 'used', 'electroreflectance', 'measurements', 'to', 'study', 'chargedensitywave', 'cdw', 'polarization', 'dynamics', 'at', 'voltages', 'near', 'the', 'cdw', 'depinning', 'onset', 'von', 'in', 'the', 'quasionedimensional', 'conductor', 'k03moo3', 'blue', 'bronze', 'for', 'low', 'voltages', 'where', 'the'... | [-0.16459392259518305, 0.2431419660056565, -0.04116617222788973, 0.026568296226247658, -0.01641719679321176, -0.15012035578273344, 0.08939521471240922, 0.3625520231890614, -0.2621802650122107, -0.2521874458981219, 0.054254628445419985, -0.33821720341085526, -0.05010231461357393, 0.18817681522341445, 0.01682726724517862... |
707.3818 | Fundamental Superstrings as Holograms | The worldsheet of a macroscopic fundamental superstring in the Green-Schwarz
light-cone gauge is viewed as a possible boundary hologram of the near horizon
region of a small black string. For toroidally compactified strings, the
hologram has global symmetries of AdS_3 \times S^{d-1} \times T^{8-d}, (d
=3,..,8), only ... | hep-th | the worldsheet of a macroscopic fundamental superstring in the greenschwarz lightcone gauge is viewed as a possible boundary hologram of the near horizon region of a small black string for toroidally compactified strings the hologram has global symmetries of ads_3 times sd1 times t8d d 38 only some of which extend to l... | [['the', 'worldsheet', 'of', 'a', 'macroscopic', 'fundamental', 'superstring', 'in', 'the', 'greenschwarz', 'lightcone', 'gauge', 'is', 'viewed', 'as', 'a', 'possible', 'boundary', 'hologram', 'of', 'the', 'near', 'horizon', 'region', 'of', 'a', 'small', 'black', 'string', 'for', 'toroidally', 'compactified', 'strings'... | [-0.16666653176538482, 0.14146449254839732, -0.047725358604025235, 0.11943073186897639, -0.049014897106120184, -0.14088725017546846, 0.002407412923342229, 0.2504059124761771, -0.18509559797626124, -0.21673163501069928, 0.10496533339516852, -0.28536086449957027, -0.10829507672214324, 0.13044613144312897, -0.103690103631... |
707.3819 | Localized states at zigzag edges of bilayer graphene | We report the existence of zero energy surface states localized at zigzag
edges of bilayer graphene. Working within the tight-binding approximation we
derive the analytic solution for the wavefunctions of these peculiar surface
states. It is shown that zero energy edge states in bilayer graphene can be
divided into t... | cond-mat.mes-hall | we report the existence of zero energy surface states localized at zigzag edges of bilayer graphene working within the tightbinding approximation we derive the analytic solution for the wavefunctions of these peculiar surface states it is shown that zero energy edge states in bilayer graphene can be divided into two fa... | [['we', 'report', 'the', 'existence', 'of', 'zero', 'energy', 'surface', 'states', 'localized', 'at', 'zigzag', 'edges', 'of', 'bilayer', 'graphene', 'working', 'within', 'the', 'tightbinding', 'approximation', 'we', 'derive', 'the', 'analytic', 'solution', 'for', 'the', 'wavefunctions', 'of', 'these', 'peculiar', 'sur... | [-0.20784152130046013, 0.18226150154593845, -0.04689967672509903, -0.003532019213095985, 0.025935441287848252, -0.15303726848214866, 0.08071370939512483, 0.3963155993260443, -0.2671752659582787, -0.27183732138523325, -0.012243672227486967, -0.30775993381499905, -0.13617062078026884, 0.13669368462975728, 0.0287375600098... |
707.382 | Structure and Vertical Modes in Finite 2D Plasma Crystals | In this research, formation of finite two-dimensional (2D) plasma crystals
was numerically simulated. The structure was investigated for systems with
various Debye length and it was found there is a transition from a complete
hexagonal structure to a structure with concentric rings on the outer edge and
hexagonal lat... | physics.plasm-ph | in this research formation of finite twodimensional 2d plasma crystals was numerically simulated the structure was investigated for systems with various debye length and it was found there is a transition from a complete hexagonal structure to a structure with concentric rings on the outer edge and hexagonal lattice in... | [['in', 'this', 'research', 'formation', 'of', 'finite', 'twodimensional', '2d', 'plasma', 'crystals', 'was', 'numerically', 'simulated', 'the', 'structure', 'was', 'investigated', 'for', 'systems', 'with', 'various', 'debye', 'length', 'and', 'it', 'was', 'found', 'there', 'is', 'a', 'transition', 'from', 'a', 'comple... | [-0.13915664868100602, 0.1717003314749009, -0.044126720125239126, 0.012495042497346944, -0.03750792091219302, -0.0781882091644494, -0.020111591292216496, 0.3890310558764374, -0.2412575476912453, -0.2591969348709373, 0.09228448077680214, -0.2970207195290748, -0.07104136804118752, 0.20338845492737806, 0.01917071996996288... |
707.3821 | One-way quantum computing in optical lattices with many atom addressing | One of the fundamental conditions for one-way quantum computation (1WQC) is
the ability to make sequential measurements on isolated qubits that comprise
the highly entangled resource for 1WQC, the cluster state. This has been a
significant impediment in the implementation of 1WQC with ultracold atoms
confined in opti... | quant-ph | one of the fundamental conditions for oneway quantum computation 1wqc is the ability to make sequential measurements on isolated qubits that comprise the highly entangled resource for 1wqc the cluster state this has been a significant impediment in the implementation of 1wqc with ultracold atoms confined in optical lat... | [['one', 'of', 'the', 'fundamental', 'conditions', 'for', 'oneway', 'quantum', 'computation', '1wqc', 'is', 'the', 'ability', 'to', 'make', 'sequential', 'measurements', 'on', 'isolated', 'qubits', 'that', 'comprise', 'the', 'highly', 'entangled', 'resource', 'for', '1wqc', 'the', 'cluster', 'state', 'this', 'has', 'be... | [-0.13592634218580582, 0.1848404929639836, -0.02492024448207196, 0.005654265993556493, 0.0049888200905299235, -0.2026939973814272, 0.07443672472301933, 0.40651792391132907, -0.2246335675986875, -0.321056713635775, 0.06696315690925923, -0.24785222145220062, -0.045112492119455165, 0.2337219828051053, -0.04113452827157805... |
707.3822 | Study of the spin-$\frac32$ Hubbard-Kondo lattice model by means of the
Composite Operator Method | We study the spin-$\frac32$ Hubbard-Kondo lattice model by means of the
Composite Operator Method, after applying a Holstein-Primakov transformation.
The spin and particle dynamics in the ferromagnetic state are calculated by
taking into account strong on-site correlations between electrons and
antiferromagnetic exch... | cond-mat.str-el | we study the spinfrac32 hubbardkondo lattice model by means of the composite operator method after applying a holsteinprimakov transformation the spin and particle dynamics in the ferromagnetic state are calculated by taking into account strong onsite correlations between electrons and antiferromagnetic exchange among ... | [['we', 'study', 'the', 'spinfrac32', 'hubbardkondo', 'lattice', 'model', 'by', 'means', 'of', 'the', 'composite', 'operator', 'method', 'after', 'applying', 'a', 'holsteinprimakov', 'transformation', 'the', 'spin', 'and', 'particle', 'dynamics', 'in', 'the', 'ferromagnetic', 'state', 'are', 'calculated', 'by', 'taking... | [-0.13456670076966304, 0.285940674449897, 0.010844539956382985, 0.09391580319980967, 0.009470301223391632, -0.19427900929179676, 0.07191830982436549, 0.3945482869474393, -0.2509008303003491, -0.30452106330754625, -0.05698497526848443, -0.3700103423435171, -0.037362801649098124, 0.10562201850072322, 0.19485032858924484,... |
707.3823 | Room temperature spin filtering in epitaxial cobalt-ferrite tunnel
barriers | We report direct experimental evidence of room temperature spin filtering in
magnetic tunnel junctions (MTJs) containing CoFe2O4 tunnel barriers via
tunneling magnetoresistance (TMR) measurements.
Pt(111)/CoFe2O4(111)/gamma-Al2O3(111)/Co(0001) fully epitaxial MTJs were grown
in order to obtain a high quality system, ... | cond-mat.mtrl-sci | we report direct experimental evidence of room temperature spin filtering in magnetic tunnel junctions mtjs containing cofe2o4 tunnel barriers via tunneling magnetoresistance tmr measurements pt111cofe2o4111gammaal2o3111co0001 fully epitaxial mtjs were grown in order to obtain a high quality system capable of functioni... | [['we', 'report', 'direct', 'experimental', 'evidence', 'of', 'room', 'temperature', 'spin', 'filtering', 'in', 'magnetic', 'tunnel', 'junctions', 'mtjs', 'containing', 'cofe2o4', 'tunnel', 'barriers', 'via', 'tunneling', 'magnetoresistance', 'tmr', 'measurements', 'pt111cofe2o4111gammaal2o3111co0001', 'fully', 'epitax... | [-0.24076734975450367, 0.13205175599622948, -0.027730780283737683, -0.02867982444292474, -0.02142932605886153, -0.20160930139822103, 0.09702023039093223, 0.45263955957978685, -0.24305247332548252, -0.4265547874514188, -0.028007054333161634, -0.30291461973303113, -0.053449784679703904, 0.2517329825580155, 0.079207185464... |
707.3824 | Competing Ordered Phases in URu2Si2: Hydrostatic Pressure and
Re-substitution | A persistent kink in the pressure dependence of the \hidden order" (HO)
transition temperature of URu2-xRexSi2 is observed at a critical pressure Pc=15
kbar for 0 < x < 0.08. In URu2Si2, the kink at Pc is accompanied by the
destruction of superconductivity; a change in the magnitude of a spin
excitation gap, determin... | cond-mat.str-el | a persistent kink in the pressure dependence of the hidden order ho transition temperature of uru2xrexsi2 is observed at a critical pressure pc15 kbar for 0 x 008 in uru2si2 the kink at pc is accompanied by the destruction of superconductivity a change in the magnitude of a spin excitation gap determined from electrica... | [['a', 'persistent', 'kink', 'in', 'the', 'pressure', 'dependence', 'of', 'the', 'hidden', 'order', 'ho', 'transition', 'temperature', 'of', 'uru2xrexsi2', 'is', 'observed', 'at', 'a', 'critical', 'pressure', 'pc15', 'kbar', 'for', '0', 'x', '008', 'in', 'uru2si2', 'the', 'kink', 'at', 'pc', 'is', 'accompanied', 'by', ... | [-0.19671861154629905, 0.2248471182620372, -0.05391814444652375, 0.011041089791037581, -0.02144551681464209, -0.07947030859068036, 0.19580984590027262, 0.30173439798767077, -0.2789603619452785, -0.3032245378283893, -0.0005929195952108678, -0.37026887461543084, -0.03657272522173384, 0.1494689506245777, 0.088377090707859... |
707.3825 | Emergence of noncollinear magnetic ordering in small magnetic clusters:
Mn$_n$ and As@Mn$_n$ | Using first-principles density functional calculations, we have studied the
magnetic ordering in pure Mn$_n$ ($n=2-$10, 13, 15, 19) and As@Mn$_n$
($n=1-$10) clusters. Although, for both pure and doped manganese clusters,
there exists many collinear and noncollinear isomers close in energy, the
smaller clusters with $... | physics.atm-clus | using firstprinciples density functional calculations we have studied the magnetic ordering in pure mn_n n210 13 15 19 and asmn_n n110 clusters although for both pure and doped manganese clusters there exists many collinear and noncollinear isomers close in energy the smaller clusters with nleqslant5 have collinear mag... | [['using', 'firstprinciples', 'density', 'functional', 'calculations', 'we', 'have', 'studied', 'the', 'magnetic', 'ordering', 'in', 'pure', 'mn_n', 'n210', '13', '15', '19', 'and', 'asmn_n', 'n110', 'clusters', 'although', 'for', 'both', 'pure', 'and', 'doped', 'manganese', 'clusters', 'there', 'exists', 'many', 'coll... | [-0.11573204890660503, 0.21057562070268698, 0.004552162967293578, 0.11390848410014501, 0.04525185553904842, -0.04916398184483542, 0.07980602047584184, 0.4019840841784197, -0.1960438602439621, -0.3621355530531967, -0.022791345739353666, -0.34982852964826366, -0.024313296855646458, 0.10165849644416834, 0.1062716762590057... |
707.3826 | More hilltop inflation models | Using analytic expressions, we explore the parameter space for hilltop
inflation models with a potential of the form $V_0\pm m^2\phi^2 -a\phi^p$. With
the positive sign and p>2 this converts the original hybrid inflation model
into a hilltop model, allowing the spectral index to agree with the observed
value n=0.95. ... | hep-ph astro-ph hep-th | using analytic expressions we explore the parameter space for hilltop inflation models with a potential of the form v_0pm m2phi2 aphip with the positive sign and p2 this converts the original hybrid inflation model into a hilltop model allowing the spectral index to agree with the observed value n095 in some cases the ... | [['using', 'analytic', 'expressions', 'we', 'explore', 'the', 'parameter', 'space', 'for', 'hilltop', 'inflation', 'models', 'with', 'a', 'potential', 'of', 'the', 'form', 'v_0pm', 'm2phi2', 'aphip', 'with', 'the', 'positive', 'sign', 'and', 'p2', 'this', 'converts', 'the', 'original', 'hybrid', 'inflation', 'model', '... | [-0.11232827048605451, 0.11239388128026173, -0.07125000176019966, 0.10990262422755433, -0.07826071026233526, -0.22108707529707597, 0.022149398951576305, 0.3391830707828586, -0.2178508853754745, -0.29338605673267293, 0.08110548878590075, -0.23719303643760772, -0.1405739277601242, 0.16501161928216998, -0.0094570910844665... |
707.3827 | Engineering Silicon Nanocrystals: Theoretical study of the effect of
Codoping with Boron and Phosphorus | We show that the optical and electronic properties of nanocrystalline silicon
can be efficiently tuned using impurity doping. In particular, we give
evidence, by means of ab-initio calculations, that by properly controlling the
doping with either one or two atomic species, a significant modification of
both the absor... | cond-mat.other cond-mat.mtrl-sci | we show that the optical and electronic properties of nanocrystalline silicon can be efficiently tuned using impurity doping in particular we give evidence by means of abinitio calculations that by properly controlling the doping with either one or two atomic species a significant modification of both the absorption an... | [['we', 'show', 'that', 'the', 'optical', 'and', 'electronic', 'properties', 'of', 'nanocrystalline', 'silicon', 'can', 'be', 'efficiently', 'tuned', 'using', 'impurity', 'doping', 'in', 'particular', 'we', 'give', 'evidence', 'by', 'means', 'of', 'abinitio', 'calculations', 'that', 'by', 'properly', 'controlling', 'th... | [-0.054977632040143054, 0.13975792762859318, -0.03447312405010923, 0.026667415379407877, 0.03246564846386776, -0.14983536255882776, 0.08395331650675136, 0.45815788831046605, -0.2237181539429312, -0.31553240992213066, -0.005408047817825796, -0.36391453487858016, -0.10580618665157322, 0.15089751306049368, 0.0388493637098... |
707.3828 | Structure, bonding and magnetism in cobalt clusters | The structural, electronic and magnetic properties of Co$_n$ clusters
($n=2-$20) have been investigated using density functional theory within the
pseudopotential plane wave method. An unusual hexagonal growth pattern has been
observed in the intermediate size range, $n=15-$20. The cobalt atoms are
ferromagnetically ... | physics.atm-clus | the structural electronic and magnetic properties of co_n clusters n220 have been investigated using density functional theory within the pseudopotential plane wave method an unusual hexagonal growth pattern has been observed in the intermediate size range n1520 the cobalt atoms are ferromagnetically ordered and the ca... | [['the', 'structural', 'electronic', 'and', 'magnetic', 'properties', 'of', 'co_n', 'clusters', 'n220', 'have', 'been', 'investigated', 'using', 'density', 'functional', 'theory', 'within', 'the', 'pseudopotential', 'plane', 'wave', 'method', 'an', 'unusual', 'hexagonal', 'growth', 'pattern', 'has', 'been', 'observed',... | [-0.13404056482373716, 0.18825909873842822, -0.020753597761405274, 0.05734436549964619, -0.013096856044981866, -0.04179119054188437, 0.011560394777297141, 0.433224235180805, -0.23262920801867137, -0.3470338757863229, 0.0005202032650444419, -0.3267624808544729, -0.08529632966321438, 0.13947742786060305, 0.10932154674826... |
707.3829 | Occupation Statistics of Critical Branching Random Walks in Two or
Higher Dimensions | Consider a critical nearest neighbor branching random walk on the
$d$-dimensional integer lattice initiated by a single particle at the origin.
Let $G_{n}$ be the event that the branching random walk survives to generation
$n$. We obtain limit theorems conditional on the event $G_{n}$ for a variety of
occupation stat... | math.PR | consider a critical nearest neighbor branching random walk on the ddimensional integer lattice initiated by a single particle at the origin let g_n be the event that the branching random walk survives to generation n we obtain limit theorems conditional on the event g_n for a variety of occupation statistics 1 let v_n ... | [['consider', 'a', 'critical', 'nearest', 'neighbor', 'branching', 'random', 'walk', 'on', 'the', 'ddimensional', 'integer', 'lattice', 'initiated', 'by', 'a', 'single', 'particle', 'at', 'the', 'origin', 'let', 'g_n', 'be', 'the', 'event', 'that', 'the', 'branching', 'random', 'walk', 'survives', 'to', 'generation', '... | [-0.12649614299188763, 0.27253100387236256, -0.005723303407522859, 0.032969364500489304, 0.0293359597038367, -0.18605603779306507, 0.05098510726434548, 0.3106577914222005, -0.24879118425328986, -0.25999418976209543, 0.07746479854720764, -0.35341813147879475, -0.04511746283883395, 0.09030936382212999, 0.0154416321679986... |
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