id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
|---|---|---|---|---|---|---|
708.1549 | Improved Measurement of Time-Dependent CP Asymmetries and the CP-Odd
Fraction in the Decay B0->D*+D*- | We present an updated measurement of the CP-odd fraction and the
time-dependent CP asymmetries in the decay B0->D*+D*-using (383 +/- 4) \times
10^{6} BB pairs collected with the Babar detector. We determine the CP-odd
fraction to be $0.143\pm0.034\stat\pm0.008\syst$. The time-dependent CP
asymmetry parameters are det... | hep-ex | we present an updated measurement of the cpodd fraction and the timedependent cp asymmetries in the decay b0ddusing 383 4 times 106 bb pairs collected with the babar detector we determine the cpodd fraction to be 0143pm0034statpm0008syst the timedependent cp asymmetry parameters are determined to be c_ 005pm 014stat pm... | [['we', 'present', 'an', 'updated', 'measurement', 'of', 'the', 'cpodd', 'fraction', 'and', 'the', 'timedependent', 'cp', 'asymmetries', 'in', 'the', 'decay', 'b0ddusing', '383', '4', 'times', '106', 'bb', 'pairs', 'collected', 'with', 'the', 'babar', 'detector', 'we', 'determine', 'the', 'cpodd', 'fraction', 'to', 'be... | [-0.1609280311213051, 0.2081672114375554, -0.014038807183906838, 0.05523256121857746, -0.010294145325551162, -0.13918942781291097, 0.13564522363988027, 0.26832133181695195, -0.19292528744208048, -0.33762552012764924, 0.03200094259148967, -0.410168177316066, 0.10146556417080196, 0.1261261693969671, 0.07273013982921839, ... |
708.155 | Liouville-type theorems for foliations with complex leaves | We discuss various problems regarding the structure of the foliation of some
foliated submanifolds S of C^n, in particular Levi flat ones. As a general
scheme, we suppose that S is bounded along a coordinate (or a subset of
coordinates), and prove that the leaves of its foliation are complex planes.
| math.CV | we discuss various problems regarding the structure of the foliation of some foliated submanifolds s of cn in particular levi flat ones as a general scheme we suppose that s is bounded along a coordinate or a subset of coordinates and prove that the leaves of its foliation are complex planes | [['we', 'discuss', 'various', 'problems', 'regarding', 'the', 'structure', 'of', 'the', 'foliation', 'of', 'some', 'foliated', 'submanifolds', 's', 'of', 'cn', 'in', 'particular', 'levi', 'flat', 'ones', 'as', 'a', 'general', 'scheme', 'we', 'suppose', 'that', 's', 'is', 'bounded', 'along', 'a', 'coordinate', 'or', 'a'... | [-0.2730593001424317, 0.06049257385380128, -0.05191877944504514, 0.0345052265694511, -0.0972184542493493, -0.15113788514452822, -0.02052716136563058, 0.38670479403991326, -0.29628121838265775, -0.15265830997697205, 0.11351207974960334, -0.2737121210050057, -0.13969056022024767, 0.16458782019988433, -0.1283914276453502,... |
708.1551 | Left-symmetric Bialgebras and An Analogue of the Classical Yang-Baxter
Equation | We introduce a notion of left-symmetric bialgebra which is an analogue of the
notion of Lie bialgebra. We prove that a left-symmetric bialgebra is equivalent
to a symplectic Lie algebra with a decomposition into a direct sum of the
underlying vector spaces of two Lagrangian subalgebras. The latter is called a
parak\"... | math.QA math-ph math.MP | we introduce a notion of leftsymmetric bialgebra which is an analogue of the notion of lie bialgebra we prove that a leftsymmetric bialgebra is equivalent to a symplectic lie algebra with a decomposition into a direct sum of the underlying vector spaces of two lagrangian subalgebras the latter is called a parakahler li... | [['we', 'introduce', 'a', 'notion', 'of', 'leftsymmetric', 'bialgebra', 'which', 'is', 'an', 'analogue', 'of', 'the', 'notion', 'of', 'lie', 'bialgebra', 'we', 'prove', 'that', 'a', 'leftsymmetric', 'bialgebra', 'is', 'equivalent', 'to', 'a', 'symplectic', 'lie', 'algebra', 'with', 'a', 'decomposition', 'into', 'a', 'd... | [-0.21340082137612626, 0.020781055687970926, -0.09409657216523416, 0.08799548113165656, -0.22206395294051617, -0.12252925797320831, -0.03581376510499887, 0.35708574426378337, -0.36443155846889286, -0.15844304037343065, 0.10987468637624541, -0.21336291566750823, -0.23702760266538603, 0.12997458831635483, -0.154079168423... |
708.1552 | Demonstration of a mid infrared silicon Raman amplifier | We demonstrate for the first time a mid infrared silicon Raman amplifier.
Amplification of 12 dB is reported for a signal at 3.39 micron wavelength. The
active medium was a 2.5 cm long silicon sample that was pumped with 5ns pulses
at 2.88 micron. The absence of the nonlinear losses which severely limit the
performan... | physics.optics | we demonstrate for the first time a mid infrared silicon raman amplifier amplification of 12 db is reported for a signal at 339 micron wavelength the active medium was a 25 cm long silicon sample that was pumped with 5ns pulses at 288 micron the absence of the nonlinear losses which severely limit the performance of si... | [['we', 'demonstrate', 'for', 'the', 'first', 'time', 'a', 'mid', 'infrared', 'silicon', 'raman', 'amplifier', 'amplification', 'of', '12', 'db', 'is', 'reported', 'for', 'a', 'signal', 'at', '339', 'micron', 'wavelength', 'the', 'active', 'medium', 'was', 'a', '25', 'cm', 'long', 'silicon', 'sample', 'that', 'was', 'p... | [-0.07590069324511138, 0.14282599389251252, -0.025805849599203578, -0.06013449161697214, 0.014043740505628564, -0.14670584671182074, 0.08202114446019684, 0.48191928814372254, -0.21586667312981767, -0.29159063261424845, 0.10812989091479082, -0.3372548176665549, -0.07448480143729183, 0.23329019787100455, -0.0494411398432... |
708.1553 | Single top production associated with a neutral scalar at LHC in
topcolor-assisted technicolor | The topcolor-assisted technicolor (TC2) model predicts a number of neutral
scalars like the top-pion ($\pi^0_t$) and the top-Higgs ($h^0_t$). These
scalars have flavor-changing neutral-current (FCNC) top quark couplings, among
which the top-charm transition couplings may be sizable. Such FCNC couplings
induce single ... | hep-ph | the topcolorassisted technicolor tc2 model predicts a number of neutral scalars like the toppion pi0_t and the tophiggs h0_t these scalars have flavorchanging neutralcurrent fcnc top quark couplings among which the topcharm transition couplings may be sizable such fcnc couplings induce single top productions associated... | [['the', 'topcolorassisted', 'technicolor', 'tc2', 'model', 'predicts', 'a', 'number', 'of', 'neutral', 'scalars', 'like', 'the', 'toppion', 'pi0_t', 'and', 'the', 'tophiggs', 'h0_t', 'these', 'scalars', 'have', 'flavorchanging', 'neutralcurrent', 'fcnc', 'top', 'quark', 'couplings', 'among', 'which', 'the', 'topcharm'... | [-0.06702092150590033, 0.3143568827872514, -0.000677931942846044, 0.1731736612809982, -0.05309723105892772, -0.2099571052731335, 0.07070574612953351, 0.27252274214879435, -0.2285764935586485, -0.2610745117344777, 0.005202234819989826, -0.3380620250318316, 0.013707404486922314, 0.10058527228466119, 0.10973904016282177, ... |
708.1554 | Floer Homology for Symplectomorphism | Let (M,\omega) be a compact symplectic manifold, and \phi be a symplectic
diffeomorphism on M, we define a Floer-type homology FH_*(\phi) which is a gen-
eralization of Floer homology for symplectic fixed points defined by Dostoglou
and Salamon for monotone symplectic manifolds. These homology groups are
modules over... | math.SG | let momega be a compact symplectic manifold and phi be a symplectic diffeomorphism on m we define a floertype homology fh_phi which is a gen eralization of floer homology for symplectic fixed points defined by dostoglou and salamon for monotone symplectic manifolds these homology groups are modules over a suitable novi... | [['let', 'momega', 'be', 'a', 'compact', 'symplectic', 'manifold', 'and', 'phi', 'be', 'a', 'symplectic', 'diffeomorphism', 'on', 'm', 'we', 'define', 'a', 'floertype', 'homology', 'fh_phi', 'which', 'is', 'a', 'gen', 'eralization', 'of', 'floer', 'homology', 'for', 'symplectic', 'fixed', 'points', 'defined', 'by', 'do... | [-0.30365685250920554, 0.07805581806848447, -0.12982526109553874, 0.0866602380546586, -0.10527335855100925, -0.23860717645535867, -0.04676921323407442, 0.3443820688252648, -0.3203563250601292, -0.2223789117919902, 0.07372403375338762, -0.19149714144878088, -0.15988267270537715, 0.18653385654324667, -0.22530489571702977... |
708.1555 | Functions of representations of the class 1 on the homogeneous spaces of
the de Sitter group | Matrix elements and spherical functions of irreducible representations of the
de Sitter group are studied on the various homogeneous spaces of this group.
| math-ph math.MP | matrix elements and spherical functions of irreducible representations of the de sitter group are studied on the various homogeneous spaces of this group | [['matrix', 'elements', 'and', 'spherical', 'functions', 'of', 'irreducible', 'representations', 'of', 'the', 'de', 'sitter', 'group', 'are', 'studied', 'on', 'the', 'various', 'homogeneous', 'spaces', 'of', 'this', 'group']] | [-0.16694894886535147, 0.16677822836715242, -0.13813031728015, 0.0658728627477894, -0.06099356484153996, 0.018795346436293228, -0.11024065210443476, 0.3864736103493234, -0.24170337823907967, -0.16571432744841214, 0.13932597701964172, -0.23984018543168253, -0.1530943103944478, 0.14891495960562126, -0.03721164557930973, ... |
708.1556 | Seip's differentiability concepts as a particular case of the
Bertram--Gloeckner--Neeb construction | From the point of view of unification of differentiation theory, it is of
interest to note that the general construction principle of Bertram, Gloeckner
and Neeb leading to a C^k differentiability concept from a given C^0 one,
besides subsuming the Keller--Bastiani C_c^k differentiabilities on real
Hausdorff locally ... | math.FA | from the point of view of unification of differentiation theory it is of interest to note that the general construction principle of bertram gloeckner and neeb leading to a ck differentiability concept from a given c0 one besides subsuming the kellerbastiani c_ck differentiabilities on real hausdorff locally convex spa... | [['from', 'the', 'point', 'of', 'view', 'of', 'unification', 'of', 'differentiation', 'theory', 'it', 'is', 'of', 'interest', 'to', 'note', 'that', 'the', 'general', 'construction', 'principle', 'of', 'bertram', 'gloeckner', 'and', 'neeb', 'leading', 'to', 'a', 'ck', 'differentiability', 'concept', 'from', 'a', 'given'... | [-0.06252780971312505, 0.051726167740716464, -0.11161280010163249, 0.10464329237165766, -0.08460124947889122, -0.08026120242415956, 0.0426498734494002, 0.3205662484707389, -0.2825899390381075, -0.24341137345997382, 0.14006209957642024, -0.22555864605115739, -0.17064902611762775, 0.2181911863565088, -0.12589061174898625... |
708.1557 | Nilpotent Fuzz | We present a construction of the formalism where fundamental variables are
nilpotent, but in contrast to the supermathematics, commutative. This gives
another possibility to realize classically the Pauli exclusion principle. We
sketch the relevant formalism and discuss simple model of the nilpotent
oscillator to illu... | hep-th | we present a construction of the formalism where fundamental variables are nilpotent but in contrast to the supermathematics commutative this gives another possibility to realize classically the pauli exclusion principle we sketch the relevant formalism and discuss simple model of the nilpotent oscillator to illustrate... | [['we', 'present', 'a', 'construction', 'of', 'the', 'formalism', 'where', 'fundamental', 'variables', 'are', 'nilpotent', 'but', 'in', 'contrast', 'to', 'the', 'supermathematics', 'commutative', 'this', 'gives', 'another', 'possibility', 'to', 'realize', 'classically', 'the', 'pauli', 'exclusion', 'principle', 'we', '... | [-0.103673601613323, 0.1385891440357747, -0.0732981869380693, 0.08323816455929178, -0.1357959349905806, -0.20618022768283073, 0.03547671267629734, 0.2945275806764863, -0.30075525916276535, -0.2209095030414815, 0.04242149266956032, -0.19272139786305476, -0.17825698540831098, 0.16342802383290717, -0.1483214554015775, -0.... |
708.1558 | Construction of a 3-Dimensional MDS code | In this paper, we describe a procedure for constructing $q$--ary
$[N,3,N-2]$--MDS codes, of length $N\leq q+1$ (for $q$ odd) or $N\leq q+2$ (for
$q$ even), using a set of non--degenerate Hermitian forms in $PG(2,q^2)$.
| cs.IT math.IT | in this paper we describe a procedure for constructing qary n3n2mds codes of length nleq q1 for q odd or nleq q2 for q even using a set of nondegenerate hermitian forms in pg2q2 | [['in', 'this', 'paper', 'we', 'describe', 'a', 'procedure', 'for', 'constructing', 'qary', 'n3n2mds', 'codes', 'of', 'length', 'nleq', 'q1', 'for', 'q', 'odd', 'or', 'nleq', 'q2', 'for', 'q', 'even', 'using', 'a', 'set', 'of', 'nondegenerate', 'hermitian', 'forms', 'in', 'pg2q2']] | [-0.25027387781125127, 0.14530437713432492, -0.0007637139466224295, 0.09388380258866219, 0.04164020931630424, -0.282193228687075, 0.017394233865409413, 0.3649773860745358, -0.21087427155086488, -0.17619379248582956, 0.04827244089436576, -0.2382125873683077, -0.14702222607042076, 0.22771867251051872, -0.0378775282791166... |
708.1559 | Investigation on the superluminality of evanescent modes via quantum
Lorentz transformation | Applying the fact that guided photons inside a waveguide can be treated as
massive particles, one can study the superluminality of evanescent modes via
showing that a massive particle can propagate over a spacelike interval, which
corresponds to quantum tunneling effects. For this purpose, we treat the
particle as a ... | quant-ph | applying the fact that guided photons inside a waveguide can be treated as massive particles one can study the superluminality of evanescent modes via showing that a massive particle can propagate over a spacelike interval which corresponds to quantum tunneling effects for this purpose we treat the particle as a quantu... | [['applying', 'the', 'fact', 'that', 'guided', 'photons', 'inside', 'a', 'waveguide', 'can', 'be', 'treated', 'as', 'massive', 'particles', 'one', 'can', 'study', 'the', 'superluminality', 'of', 'evanescent', 'modes', 'via', 'showing', 'that', 'a', 'massive', 'particle', 'can', 'propagate', 'over', 'a', 'spacelike', 'i... | [-0.09265786635398399, 0.2014480000623007, -0.13048216106952168, 0.07947746273945086, -0.08680444520898163, -0.1365759121719748, 0.025136266278568655, 0.361644233558327, -0.2734980424493551, -0.2662513068784028, 0.010626218325924128, -0.2637254699971527, -0.08496877182740718, 0.19110373983508908, -0.061171617535874245,... |
708.156 | Defining amalgams of compact Lie groups | For $n \geq 2$ let $\Delta$ be a Dynkin diagram of rank $n$ and let $I = {1,
>..., n}$ be the set of labels of $\Delta$. A group $G$ admits a weak Phan
system of type $\Delta$ over $\mathbb{C}$ if $G$ is generated by subgroups
$U_i$, $i \in I$, which are central quotients of simply connected compact
semisimple Lie gr... | math.GR | for n geq 2 let delta be a dynkin diagram of rank n and let i 1 n be the set of labels of delta a group g admits a weak phan system of type delta over mathbbc if g is generated by subgroups u_i i in i which are central quotients of simply connected compact semisimple lie groups of rank one and contains subgroups u_ij g... | [['for', 'n', 'geq', '2', 'let', 'delta', 'be', 'a', 'dynkin', 'diagram', 'of', 'rank', 'n', 'and', 'let', 'i', '1', 'n', 'be', 'the', 'set', 'of', 'labels', 'of', 'delta', 'a', 'group', 'g', 'admits', 'a', 'weak', 'phan', 'system', 'of', 'type', 'delta', 'over', 'mathbbc', 'if', 'g', 'is', 'generated', 'by', 'subgroup... | [-0.2480737548250211, 0.11689897417605595, -0.04082940574133528, -0.025814224668892518, -0.1521696845041018, -0.2130946573598602, 0.00400309567894077, 0.3678870538921178, -0.3110724864084096, -0.17614373349312212, 0.11426560951121227, -0.27469917271146865, -0.092468612768757, 0.17639385502417984, -0.1207585187001648, -... |
708.1561 | Towards Quantum Noncommutative $\kappa$-deformed Field Theory | We introduce new $\kappa$-star product describing the multiplication of
quantized $\kappa$-deformed free fields. The $\kappa$-deformation of local free
quantum fields originates from two sources: noncommutativity of space-time and
the $\kappa$-deformation of field oscillators algebra - we relate these two
deformation... | hep-th | we introduce new kappastar product describing the multiplication of quantized kappadeformed free fields the kappadeformation of local free quantum fields originates from two sources noncommutativity of spacetime and the kappadeformation of field oscillators algebra we relate these two deformations we demonstrate that f... | [['we', 'introduce', 'new', 'kappastar', 'product', 'describing', 'the', 'multiplication', 'of', 'quantized', 'kappadeformed', 'free', 'fields', 'the', 'kappadeformation', 'of', 'local', 'free', 'quantum', 'fields', 'originates', 'from', 'two', 'sources', 'noncommutativity', 'of', 'spacetime', 'and', 'the', 'kappadefor... | [-0.1873733538833731, 0.2207768882330877, -0.0835975863217832, 0.0886439768628858, -0.08245008700388542, -0.12157878609281694, -0.0527554941512248, 0.3068220659641298, -0.25735637218301705, -0.24166983977647116, -0.005721069677528126, -0.22324142132954694, -0.16140290178153796, 0.14532924649563242, -0.07734184293406653... |
708.1562 | Products in Residue Classes | We consider a problem of P. Erdos, A. M. Odlyzko and A. Sarkozy about the
representation of residue classes modulo m by products of two not too large
primes. While it seems that even the Extended Riemann Hypothesis is not
powerful enough to achieve the expected results, here we obtain some
unconditional results ``on ... | math.NT | we consider a problem of p erdos a m odlyzko and a sarkozy about the representation of residue classes modulo m by products of two not too large primes while it seems that even the extended riemann hypothesis is not powerful enough to achieve the expected results here we obtain some unconditional results on average ove... | [['we', 'consider', 'a', 'problem', 'of', 'p', 'erdos', 'a', 'm', 'odlyzko', 'and', 'a', 'sarkozy', 'about', 'the', 'representation', 'of', 'residue', 'classes', 'modulo', 'm', 'by', 'products', 'of', 'two', 'not', 'too', 'large', 'primes', 'while', 'it', 'seems', 'that', 'even', 'the', 'extended', 'riemann', 'hypothes... | [-0.17536104887234744, 0.12947067680458227, -0.12588435299506393, 0.16945701255463064, -0.05966843921465404, -0.1724118445576592, 0.05516775213229009, 0.3122000626283651, -0.26642051266713274, -0.31102040270813786, 0.07076128756843808, -0.22978570256758518, -0.13462568584105206, 0.22835458311572143, -0.1175887937318872... |
708.1563 | On the ground state of quantum layers | We provide some new results of the ground state of quantum layers.
| math.DG math-ph math.MP | we provide some new results of the ground state of quantum layers | [['we', 'provide', 'some', 'new', 'results', 'of', 'the', 'ground', 'state', 'of', 'quantum', 'layers']] | [-0.15703681639085212, 0.1667050962569192, -0.0683386605232954, 0.00170579149077336, -0.03216714241231481, -0.10328665655106306, 0.11358674241152282, 0.34273653229077655, -0.2521322158475717, -0.2615706077776849, 0.07128263881895691, -0.27641956601291895, -0.131790057135125, 0.22244959076245627, 0.0028637762491901717, ... |
708.1564 | Learning Phonotactics Using ILP | This paper describes experiments on learning Dutch phonotactic rules using
Inductive Logic Programming, a machine learning discipline based on inductive
logical operators. Two different ways of approaching the problem are
experimented with, and compared against each other as well as with related work
on the task. The... | cs.CL | this paper describes experiments on learning dutch phonotactic rules using inductive logic programming a machine learning discipline based on inductive logical operators two different ways of approaching the problem are experimented with and compared against each other as well as with related work on the task the resul... | [['this', 'paper', 'describes', 'experiments', 'on', 'learning', 'dutch', 'phonotactic', 'rules', 'using', 'inductive', 'logic', 'programming', 'a', 'machine', 'learning', 'discipline', 'based', 'on', 'inductive', 'logical', 'operators', 'two', 'different', 'ways', 'of', 'approaching', 'the', 'problem', 'are', 'experim... | [-0.039006676364113535, -0.007840718636067496, -0.05744517917212631, 0.05053674533874506, -0.1621588573464015, -0.13867433274918722, 0.06852845229427441, 0.38721167599959744, -0.24558736755889618, -0.3503203222395054, 0.09335517272466816, -0.25480067602170275, -0.1484380855690688, 0.24201332257750133, -0.09844201319806... |
708.1565 | Study of Resonances in Exclusive B Decays to Dbar(*)D(*)K | We present a study of resonances in exclusive decays of $B$ mesons to
$\bar{D}^{(*)} D^{(*)} K$. We report the observation of the decays $B \to
\Dbar^{(*)} D^+_{s1}(2536)$ where the $D^+_{s1}(2536)$ is reconstructed in the
$D^{*0}K^+$ and $D^{*+} K^0_S$ decay channels. We report also the observation
of the decays $B ... | hep-ex | we present a study of resonances in exclusive decays of b mesons to bard d k we report the observation of the decays b to dbar d_s12536 where the d_s12536 is reconstructed in the d0k and d k0_s decay channels we report also the observation of the decays b to psi3770 k where the psi3770 decays to dbar0 d0 and d d in add... | [['we', 'present', 'a', 'study', 'of', 'resonances', 'in', 'exclusive', 'decays', 'of', 'b', 'mesons', 'to', 'bard', 'd', 'k', 'we', 'report', 'the', 'observation', 'of', 'the', 'decays', 'b', 'to', 'dbar', 'd_s12536', 'where', 'the', 'd_s12536', 'is', 'reconstructed', 'in', 'the', 'd0k', 'and', 'd', 'k0_s', 'decay', '... | [-0.12577571493122688, 0.2245332943218808, -0.06766697059629868, 0.03452326276534442, -0.01190032162360933, -0.1454744413990448, 0.10013032533271331, 0.29535361883356004, -0.18460123011089385, -0.2588030667777391, -0.034084247539136955, -0.4326638366419373, 0.04781114763798232, 0.09973378232944466, 0.09560103129252051,... |
708.1566 | Markov Chain Modelling for Reliability Estimation of Engineering Systems
at Different Scales - Some Considerations | The concepts of probability, statistics and stochastic theory are being
successfully used in structural engineering. Markov Chain modelling is a simple
stochastic process model that has found its application in both describing
stochastic evolution of system and in system reliability estimation. The recent
development... | stat.AP stat.ME | the concepts of probability statistics and stochastic theory are being successfully used in structural engineering markov chain modelling is a simple stochastic process model that has found its application in both describing stochastic evolution of system and in system reliability estimation the recent developments in ... | [['the', 'concepts', 'of', 'probability', 'statistics', 'and', 'stochastic', 'theory', 'are', 'being', 'successfully', 'used', 'in', 'structural', 'engineering', 'markov', 'chain', 'modelling', 'is', 'a', 'simple', 'stochastic', 'process', 'model', 'that', 'has', 'found', 'its', 'application', 'in', 'both', 'describing... | [-0.05249557737333817, 0.11646413012722405, -0.09212433633219916, 0.0705299063757252, -0.06854753684601747, -0.11443721107498277, 0.03150436745854677, 0.39062509196810424, -0.3027613316779025, -0.31502124055405145, 0.1332954320088902, -0.24213328986079433, -0.16197632532566786, 0.19573539003904444, -0.0467163179491763,... |
708.1567 | Strings, Projected Entangled Pair States, and variational Monte Carlo
methods | We introduce string-bond states, a class of states obtained by placing
strings of operators on a lattice, which encompasses the relevant states in
Quantum Information. For string-bond states, expectation values of local
observables can be computed efficiently using Monte Carlo sampling, making them
suitable for a var... | quant-ph cond-mat.str-el | we introduce stringbond states a class of states obtained by placing strings of operators on a lattice which encompasses the relevant states in quantum information for stringbond states expectation values of local observables can be computed efficiently using monte carlo sampling making them suitable for a variational ... | [['we', 'introduce', 'stringbond', 'states', 'a', 'class', 'of', 'states', 'obtained', 'by', 'placing', 'strings', 'of', 'operators', 'on', 'a', 'lattice', 'which', 'encompasses', 'the', 'relevant', 'states', 'in', 'quantum', 'information', 'for', 'stringbond', 'states', 'expectation', 'values', 'of', 'local', 'observa... | [-0.1030186727776059, 0.16011327479832937, -0.09324714123005313, 0.09931785437677587, 0.0156770561389359, -0.12539688254972653, 0.08101693650241941, 0.33866241004850184, -0.25252371318804634, -0.27085660375388604, 0.09527801169647969, -0.25238410525822214, -0.09844744753624712, 0.22551873445263482, 0.014748076562370573... |
708.1568 | Nonlinear option pricing models for illiquid markets: scaling properties
and explicit solutions | Several models for the pricing of derivative securities in illiquid markets
are discussed. A typical type of nonlinear partial differential equations
arising from these investigation is studied. The scaling properties of these
equations are discussed. Explicit solutions for one of the models are obtained
and studied.... | q-fin.PR math.AP math.GR | several models for the pricing of derivative securities in illiquid markets are discussed a typical type of nonlinear partial differential equations arising from these investigation is studied the scaling properties of these equations are discussed explicit solutions for one of the models are obtained and studied | [['several', 'models', 'for', 'the', 'pricing', 'of', 'derivative', 'securities', 'in', 'illiquid', 'markets', 'are', 'discussed', 'a', 'typical', 'type', 'of', 'nonlinear', 'partial', 'differential', 'equations', 'arising', 'from', 'these', 'investigation', 'is', 'studied', 'the', 'scaling', 'properties', 'of', 'these... | [-0.16075313761425408, 0.03876069313644067, -0.021420255432452035, 0.16291992112984072, -0.07947619546852681, -0.13466233220558776, -0.04343084999076698, 0.34914560996643873, -0.2806253426748773, -0.24342445474441932, 0.22511529113398865, -0.334779008180308, -0.14221175719538462, 0.2560762876401777, -0.0263844644853278... |
708.1569 | Electric Transport Theory of Dirac Fermions in Graphene | Using the self-consistent Born approximation to the Dirac fermions under
finite-range impurity scatterings, we show that the current-current correlation
function is determined by four-coupled integral equations. This is very
different from the case for impurities with short-range potentials. As a test
of the present ... | cond-mat.str-el | using the selfconsistent born approximation to the dirac fermions under finiterange impurity scatterings we show that the currentcurrent correlation function is determined by fourcoupled integral equations this is very different from the case for impurities with shortrange potentials as a test of the present approach w... | [['using', 'the', 'selfconsistent', 'born', 'approximation', 'to', 'the', 'dirac', 'fermions', 'under', 'finiterange', 'impurity', 'scatterings', 'we', 'show', 'that', 'the', 'currentcurrent', 'correlation', 'function', 'is', 'determined', 'by', 'fourcoupled', 'integral', 'equations', 'this', 'is', 'very', 'different',... | [-0.10743440665143027, 0.20980442399236043, -0.0637149216283944, 0.03361862447220555, 0.02328425616964944, -0.18037851830205517, 0.05603373990478841, 0.34982733429632773, -0.21402043490555167, -0.26466860733387515, -0.013861388850318315, -0.37853662423358475, -0.07670220878929639, 0.1586350283108282, 0.0582679627570977... |
708.157 | Theoretical analysis of magnetic force microscopy contrast in
multidomain states of magnetic superlattices with perpendicular anisotropy | Recently synthesized magnetic multilayers with strong perpendicular
anisotropy exhibit unique magnetic properties including the formation of
specific multidomain states. In particular, antiferromagnetically coupled
multilayers own rich phase diagrams that include various multidomain ground
states. Analytical equation... | cond-mat.mes-hall | recently synthesized magnetic multilayers with strong perpendicular anisotropy exhibit unique magnetic properties including the formation of specific multidomain states in particular antiferromagnetically coupled multilayers own rich phase diagrams that include various multidomain ground states analytical equations hav... | [['recently', 'synthesized', 'magnetic', 'multilayers', 'with', 'strong', 'perpendicular', 'anisotropy', 'exhibit', 'unique', 'magnetic', 'properties', 'including', 'the', 'formation', 'of', 'specific', 'multidomain', 'states', 'in', 'particular', 'antiferromagnetically', 'coupled', 'multilayers', 'own', 'rich', 'phase... | [-0.14606702758220735, 0.12129346564838701, -0.06715699662356735, 0.021418677459770514, -0.05978772331882346, -0.10923520876485464, -0.042240197686038886, 0.4214165415549716, -0.22587950364198092, -0.3096446913595383, 0.02497381473349251, -0.2749141103855067, -0.13781236032336638, 0.2525247542734642, 0.0736504528000690... |
708.1571 | Symmetries of quadratic forms classes and of quadratic surds continued
fractions. Part I: A Poincar\'e model for the de Sitter world | The problem of the classification of the indefinite binary quadratic forms
with integer coefficients is solved introducing a special partition of the de
Sitter world, where the coefficients of the forms lie, into separate domains.
Every class of indefinite forms, under the action of the special linear group
acting on... | math.NT math.GM | the problem of the classification of the indefinite binary quadratic forms with integer coefficients is solved introducing a special partition of the de sitter world where the coefficients of the forms lie into separate domains every class of indefinite forms under the action of the special linear group acting on the i... | [['the', 'problem', 'of', 'the', 'classification', 'of', 'the', 'indefinite', 'binary', 'quadratic', 'forms', 'with', 'integer', 'coefficients', 'is', 'solved', 'introducing', 'a', 'special', 'partition', 'of', 'the', 'de', 'sitter', 'world', 'where', 'the', 'coefficients', 'of', 'the', 'forms', 'lie', 'into', 'separat... | [-0.17888524282756632, 0.07809830932729606, -0.04816344720764761, -0.0013649484670135827, -0.12606798462668614, -0.08797124302245479, 0.006748435029809454, 0.2911476857581102, -0.3124803439260716, -0.23525869663376198, 0.1388261782178507, -0.2616146322941424, -0.1689051846454365, 0.20628109457284477, -0.039810117593743... |
708.1572 | Groups of motions and mechanics I: point mechanics | It is shown that physical mechanics for pointlike bodies can be effectively
modeled in terms of the action of transformation groups that act as symmetries
of the solutions of systems of differential equations that describe the
integrability of dynamical states. The equations of motion are then obtained
from these int... | gr-qc math-ph math.MP | it is shown that physical mechanics for pointlike bodies can be effectively modeled in terms of the action of transformation groups that act as symmetries of the solutions of systems of differential equations that describe the integrability of dynamical states the equations of motion are then obtained from these integr... | [['it', 'is', 'shown', 'that', 'physical', 'mechanics', 'for', 'pointlike', 'bodies', 'can', 'be', 'effectively', 'modeled', 'in', 'terms', 'of', 'the', 'action', 'of', 'transformation', 'groups', 'that', 'act', 'as', 'symmetries', 'of', 'the', 'solutions', 'of', 'systems', 'of', 'differential', 'equations', 'that', 'd... | [-0.12316923405064249, 0.1278718271814696, -0.1702139372272151, 0.05707353195764001, -0.04565701105601185, -0.09008409199944524, -0.03502586610860877, 0.2755114278131789, -0.3359948189540224, -0.2739919816542949, 0.09602188621263869, -0.2617141185021335, -0.21538166900339362, 0.17796876268195255, -0.03462941515013821, ... |
708.1573 | The Distinct Effects of Homogeneous Weak Disorder and Dilute Strong
Scatterers on Phase Competetion in the Manganites | We study the two orbital double-exchange model in two dimensions in the
presence of antiferromagnetic (AF) superexchange, strong Jahn-Teller coupling,
and substitutional disorder. At hole doping x=0.5 we explore the `bicritical'
regime where the energy of a ferromagnetic metal and a charge and orbital
ordered (CO-OO)... | cond-mat.str-el | we study the two orbital doubleexchange model in two dimensions in the presence of antiferromagnetic af superexchange strong jahnteller coupling and substitutional disorder at hole doping x05 we explore the bicritical regime where the energy of a ferromagnetic metal and a charge and orbital ordered cooo ce state are cl... | [['we', 'study', 'the', 'two', 'orbital', 'doubleexchange', 'model', 'in', 'two', 'dimensions', 'in', 'the', 'presence', 'of', 'antiferromagnetic', 'af', 'superexchange', 'strong', 'jahnteller', 'coupling', 'and', 'substitutional', 'disorder', 'at', 'hole', 'doping', 'x05', 'we', 'explore', 'the', 'bicritical', 'regime... | [-0.20366507719414748, 0.22673302184320926, 0.008198830449685826, 0.07326054213780576, -0.0007272409313032782, -0.15077762836136105, 0.08974366631771521, 0.3921760403043856, -0.2299663719145687, -0.2506650948425664, -0.013767272448810802, -0.34812416542109437, -0.11689338538553415, 0.09246411354553591, 0.07856242753171... |
708.1574 | Cartier isomorphism and Hodge Theory in the non-commutative case | These are lecture notes from Clay Summer School in Goettingen, in 2006; the
lectures were an attempt at an elementary introduction to math.KT/0611623.
| math.AG math.KT | these are lecture notes from clay summer school in goettingen in 2006 the lectures were an attempt at an elementary introduction to mathkt0611623 | [['these', 'are', 'lecture', 'notes', 'from', 'clay', 'summer', 'school', 'in', 'goettingen', 'in', '2006', 'the', 'lectures', 'were', 'an', 'attempt', 'at', 'an', 'elementary', 'introduction', 'to', 'mathkt0611623']] | [0.0350479314273054, 0.2667478857765673, -0.22005078935233707, 0.04902798070741648, -0.11671460487625816, -0.11106417304836214, -0.1276728460057215, 0.30790253254500305, -0.1184593358087692, -0.4873043926940723, 0.244286815085533, -0.3409573142628439, -0.1857682757783385, 0.1375423943708566, -0.2801222052763809, -0.136... |
708.1575 | Symmetric Homology of Algebras | In this note, we outline the general development of a theory of symmetric
homology of algebras, an analog of cyclic homology where the cyclic groups are
replaced by symmetric groups. This theory is developed using the framework of
crossed simplicial groups and the homological algebra of module-valued
functors. The sy... | math.AT | in this note we outline the general development of a theory of symmetric homology of algebras an analog of cyclic homology where the cyclic groups are replaced by symmetric groups this theory is developed using the framework of crossed simplicial groups and the homological algebra of modulevalued functors the symmetric... | [['in', 'this', 'note', 'we', 'outline', 'the', 'general', 'development', 'of', 'a', 'theory', 'of', 'symmetric', 'homology', 'of', 'algebras', 'an', 'analog', 'of', 'cyclic', 'homology', 'where', 'the', 'cyclic', 'groups', 'are', 'replaced', 'by', 'symmetric', 'groups', 'this', 'theory', 'is', 'developed', 'using', 't... | [-0.2078697778777603, 0.10584865637168096, -0.11631515560781254, 0.09907273004406734, -0.07009243760805796, -0.15756093399489626, -0.07190824024077944, 0.3696032267036464, -0.3846101975013666, -0.1964212803498787, 0.1572472040034721, -0.18674861604676526, -0.21657535169711883, 0.14527824916602933, -0.2015948941156667, ... |
708.1576 | Study of K^0 \to pi^- e^+ nu_e e^+ e^- in chiral perturbation theory | K^0 \to pi^- e^+ nu_e e^+ e^- decay is studied up to the next-to-leading
order O^4 in chiral perturbation theory. It is found that the O^4 terms
appreciably modifiy the shape of the invariant mass distribution of the leptons
and the energy spectrum of the neutrino.
| hep-ph | k0 to pi e nu_e e e decay is studied up to the nexttoleading order o4 in chiral perturbation theory it is found that the o4 terms appreciably modifiy the shape of the invariant mass distribution of the leptons and the energy spectrum of the neutrino | [['k0', 'to', 'pi', 'e', 'nu_e', 'e', 'e', 'decay', 'is', 'studied', 'up', 'to', 'the', 'nexttoleading', 'order', 'o4', 'in', 'chiral', 'perturbation', 'theory', 'it', 'is', 'found', 'that', 'the', 'o4', 'terms', 'appreciably', 'modifiy', 'the', 'shape', 'of', 'the', 'invariant', 'mass', 'distribution', 'of', 'the', 'l... | [-0.12213180937493841, 0.2130140167971452, -0.10235503886101974, 0.12248373116987447, 0.005750842640797297, -0.07783398272262679, -0.03823756088450965, 0.27805670101402535, -0.20496558126889997, -0.2700948187874423, -0.05972128774091187, -0.34257695426543555, -0.018915468123224047, 0.044637380374802485, 0.0775228624542... |
708.1577 | Equivariant homotopy and deformations of diffeomorphisms | We present a way of constructing and deforming diffeomorphisms of manifolds
endowed with a Lie group action. This is applied to the study of exotic
diffeomorphisms and involutions of spheres and to the equivariant homotopy of
Lie groups.
| math.DG math.AT | we present a way of constructing and deforming diffeomorphisms of manifolds endowed with a lie group action this is applied to the study of exotic diffeomorphisms and involutions of spheres and to the equivariant homotopy of lie groups | [['we', 'present', 'a', 'way', 'of', 'constructing', 'and', 'deforming', 'diffeomorphisms', 'of', 'manifolds', 'endowed', 'with', 'a', 'lie', 'group', 'action', 'this', 'is', 'applied', 'to', 'the', 'study', 'of', 'exotic', 'diffeomorphisms', 'and', 'involutions', 'of', 'spheres', 'and', 'to', 'the', 'equivariant', 'ho... | [-0.24994340833080442, 0.08538821567536185, -0.11995943106318775, 0.03464449211759003, -0.1526838882189048, -0.09499806089718875, 0.014284802374037864, 0.3947982450849132, -0.2674132865902625, -0.2630481952066092, 0.11296617710276653, -0.2474292851984501, -0.15610151024731367, 0.1481457128875742, -0.18062053821784885, ... |
708.1578 | Recent photometry of symbiotic stars - XII | We present new photometric observations of 15 symbiotic stars (EG And, Z And,
AE Ara, BF Cyg, CH Cyg, CI Cyg, V1329 Cyg, TX CVn, AG Dra, Draco C-1, RW Hya,
SY Mus, AR Pav, AG Peg, AX Per) covering their last orbital cycle(s) from
2003.9 to 2007.2. We obtained our data by both classical photoelectric and CCD
photometr... | astro-ph | we present new photometric observations of 15 symbiotic stars eg and z and ae ara bf cyg ch cyg ci cyg v1329 cyg tx cvn ag dra draco c1 rw hya sy mus ar pav ag peg ax per covering their last orbital cycles from 20039 to 20072 we obtained our data by both classical photoelectric and ccd photometry main results are eg an... | [['we', 'present', 'new', 'photometric', 'observations', 'of', '15', 'symbiotic', 'stars', 'eg', 'and', 'z', 'and', 'ae', 'ara', 'bf', 'cyg', 'ch', 'cyg', 'ci', 'cyg', 'v1329', 'cyg', 'tx', 'cvn', 'ag', 'dra', 'draco', 'c1', 'rw', 'hya', 'sy', 'mus', 'ar', 'pav', 'ag', 'peg', 'ax', 'per', 'covering', 'their', 'last', '... | [-0.05353133015645047, 0.13393227741859542, -0.05645133319345337, -0.013632753599193637, -0.0640589229564217, -0.19301675688216668, 0.15363282557249208, 0.40232430035852035, -0.18640639476771295, -0.377974541630182, 0.09592086920531949, -0.3399992713118317, -0.08441248922263858, 0.1410372886582519, -0.1752161717697702,... |
708.1579 | Homogeneous temporal activity patterns in a large online communication
space | The many-to-many social communication activity on the popular technology-news
website Slashdot has been studied. We have concentrated on the dynamics of
message production without considering semantic relations and have found
regular temporal patterns in the reaction time of the community to a news-post
as well as in... | cs.NI | the manytomany social communication activity on the popular technologynews website slashdot has been studied we have concentrated on the dynamics of message production without considering semantic relations and have found regular temporal patterns in the reaction time of the community to a newspost as well as in single... | [['the', 'manytomany', 'social', 'communication', 'activity', 'on', 'the', 'popular', 'technologynews', 'website', 'slashdot', 'has', 'been', 'studied', 'we', 'have', 'concentrated', 'on', 'the', 'dynamics', 'of', 'message', 'production', 'without', 'considering', 'semantic', 'relations', 'and', 'have', 'found', 'regul... | [-0.14505212900626974, 0.08960888724760625, -0.09496403981925602, 0.1295599109059591, -0.09758756162288289, -0.13073231770481536, 0.0687334094621727, 0.4036420539993307, -0.25906400571820204, -0.34874520934038405, 0.06242187577215415, -0.30106818368928373, -0.1671824177433534, 0.16576747163840017, -0.07428694368623522,... |
708.158 | Optimal Causal Inference: Estimating Stored Information and
Approximating Causal Architecture | We introduce an approach to inferring the causal architecture of stochastic
dynamical systems that extends rate distortion theory to use causal
shielding---a natural principle of learning. We study two distinct cases of
causal inference: optimal causal filtering and optimal causal estimation.
Filtering corresponds ... | cs.IT cond-mat.stat-mech cs.LG math.IT math.ST stat.TH | we introduce an approach to inferring the causal architecture of stochastic dynamical systems that extends rate distortion theory to use causal shieldinga natural principle of learning we study two distinct cases of causal inference optimal causal filtering and optimal causal estimation filtering corresponds to the ide... | [['we', 'introduce', 'an', 'approach', 'to', 'inferring', 'the', 'causal', 'architecture', 'of', 'stochastic', 'dynamical', 'systems', 'that', 'extends', 'rate', 'distortion', 'theory', 'to', 'use', 'causal', 'shieldinga', 'natural', 'principle', 'of', 'learning', 'we', 'study', 'two', 'distinct', 'cases', 'of', 'causa... | [-0.11999644398686844, 0.035293289794405304, -0.11175428617328483, 0.1471254433912558, -0.11548402330178457, -0.1316143046290866, 0.08718658545997944, 0.33293406873902615, -0.318903063351172, -0.3238633441190662, 0.06903298707948125, -0.23774054585866602, -0.19131618385199545, 0.14014422147738514, -0.08729415348595164,... |
708.1581 | The equivariant cohomology of weighted projective space | We describe the integral equivariant cohomology ring of a weighted projective
space in terms of piecewise polynomials, and thence by generators and
relations. We deduce that the ring is a perfect invariant, and prove a Chern
class formula for weighted projective bundles.
| math.AT math.AG | we describe the integral equivariant cohomology ring of a weighted projective space in terms of piecewise polynomials and thence by generators and relations we deduce that the ring is a perfect invariant and prove a chern class formula for weighted projective bundles | [['we', 'describe', 'the', 'integral', 'equivariant', 'cohomology', 'ring', 'of', 'a', 'weighted', 'projective', 'space', 'in', 'terms', 'of', 'piecewise', 'polynomials', 'and', 'thence', 'by', 'generators', 'and', 'relations', 'we', 'deduce', 'that', 'the', 'ring', 'is', 'a', 'perfect', 'invariant', 'and', 'prove', 'a... | [-0.2569064014990415, 0.03950093861065051, -0.08280955676344179, 0.10105131717587244, -0.09009264152319658, -0.13208361303744218, -0.04755856482578175, 0.33626496266307576, -0.361723108527561, -0.16210916500893377, 0.08846722876131978, -0.20249520989489697, -0.1818061418931133, 0.19523730880713888, -0.1617849053415869,... |
708.1582 | A Littlewood-Richardson rule for Grassmannian Permutations | We give a combinatorial rule for computing intersection numbers on a flag
manifold which come from products of Schubert classes pulled back from
Grassmannian projections. This rule generalizes the known rule for
Grassmannians.
| math.CO | we give a combinatorial rule for computing intersection numbers on a flag manifold which come from products of schubert classes pulled back from grassmannian projections this rule generalizes the known rule for grassmannians | [['we', 'give', 'a', 'combinatorial', 'rule', 'for', 'computing', 'intersection', 'numbers', 'on', 'a', 'flag', 'manifold', 'which', 'come', 'from', 'products', 'of', 'schubert', 'classes', 'pulled', 'back', 'from', 'grassmannian', 'projections', 'this', 'rule', 'generalizes', 'the', 'known', 'rule', 'for', 'grassmanni... | [-0.15034100582653825, -0.00852911752846205, -0.10086484151807698, 0.06283786496020514, -0.15619621341201392, -0.19829867777386398, 0.1609761452189449, 0.2587579529393803, -0.4113188417995292, -0.15905919005021904, 0.10427198759950415, -0.17051286645459407, -0.17657552687733463, 0.21709575854016072, -0.1628375707024877... |
708.1583 | Intransitive geometries | A lemma of Tits establishes a connection between the simple connectivity of
an incidence geometry and the universal completion of an amalgam induced by a
sufficiently transitive group of automorphisms of that geometry. In the present
paper, we generalize this lemma to intransitive geometries, thus opening the
door fo... | math.GT math.GR | a lemma of tits establishes a connection between the simple connectivity of an incidence geometry and the universal completion of an amalgam induced by a sufficiently transitive group of automorphisms of that geometry in the present paper we generalize this lemma to intransitive geometries thus opening the door for num... | [['a', 'lemma', 'of', 'tits', 'establishes', 'a', 'connection', 'between', 'the', 'simple', 'connectivity', 'of', 'an', 'incidence', 'geometry', 'and', 'the', 'universal', 'completion', 'of', 'an', 'amalgam', 'induced', 'by', 'a', 'sufficiently', 'transitive', 'group', 'of', 'automorphisms', 'of', 'that', 'geometry', '... | [-0.16819802441501192, 0.10585375198404239, -0.07725184855184385, 0.06196454286941194, -0.1552517343645117, -0.12115456197144729, 0.08349173911015637, 0.37382772168244366, -0.3331608128334795, -0.22558838443032334, 0.13059966226407727, -0.21201455404017386, -0.21044554811004282, 0.22818081547905292, -0.1811018972258482... |
708.1584 | Physics of Non-Inertial Reference Frames | Physics of non-inertial reference frames is a generalizing of Newton's laws
to any reference frames. The first, Law of Kinematic in non-inertial reference
frames reads: the kinematic state of a body free of forces conserves and
determinates a constant n-th order derivative with respect to time being equal
in absolute... | physics.class-ph physics.gen-ph | physics of noninertial reference frames is a generalizing of newtons laws to any reference frames the first law of kinematic in noninertial reference frames reads the kinematic state of a body free of forces conserves and determinates a constant nth order derivative with respect to time being equal in absolute value to... | [['physics', 'of', 'noninertial', 'reference', 'frames', 'is', 'a', 'generalizing', 'of', 'newtons', 'laws', 'to', 'any', 'reference', 'frames', 'the', 'first', 'law', 'of', 'kinematic', 'in', 'noninertial', 'reference', 'frames', 'reads', 'the', 'kinematic', 'state', 'of', 'a', 'body', 'free', 'of', 'forces', 'conserv... | [-0.17272400127204005, 0.1317788681796607, -0.12188328206227811, 0.011286434920864764, -0.07227605663315761, -0.11381736252630173, -0.005811124319903726, 0.32077196817628517, -0.2984395313271603, -0.2736783237230347, 0.0098981985728917, -0.3067055765842629, -0.040470145066095475, 0.11589935346138339, -0.118568728511427... |
708.1585 | Applications of Poisson Geometry to Physical Problems | We consider Lagrangians in Hamilton's principle defined on the tangent space
$TG$ of a Lie group $G$. Invariance of such a Lagrangian under the action of
$G$ leads to the symmetry-reduced Euler-Lagrange equations called the
Euler-Poincar\'e equations. In this case, the invariant Lagrangian is defined
on the Lie algeb... | math.DS math.CA nlin.SI | we consider lagrangians in hamiltons principle defined on the tangent space tg of a lie group g invariance of such a lagrangian under the action of g leads to the symmetryreduced eulerlagrange equations called the eulerpoincare equations in this case the invariant lagrangian is defined on the lie algebra of the group a... | [['we', 'consider', 'lagrangians', 'in', 'hamiltons', 'principle', 'defined', 'on', 'the', 'tangent', 'space', 'tg', 'of', 'a', 'lie', 'group', 'g', 'invariance', 'of', 'such', 'a', 'lagrangian', 'under', 'the', 'action', 'of', 'g', 'leads', 'to', 'the', 'symmetryreduced', 'eulerlagrange', 'equations', 'called', 'the',... | [-0.21200759455561638, 0.11082197598181664, -0.10489540971524548, 0.06358702337718569, -0.15381435132818297, -0.10513772851089015, -0.09083753824816085, 0.2822905897628516, -0.34683564795181154, -0.2483794647688046, 0.09379369645030237, -0.2486073975195177, -0.14289462614338844, 0.15507184502959717, -0.0969753371342085... |
708.1586 | Multisymplectic and polysymplectic structures on fiber bundles | We introduce the concepts of a multisymplectic structure and a polysymplectic
structure on a general fiber bundle over a general base manifold, define the
concept of the symbol of a multisymplectic form, which is a polysymplectic form
representing its leading order contribution, and prove Darboux theorems for the
exi... | math.DG math-ph math.MP math.SG | we introduce the concepts of a multisymplectic structure and a polysymplectic structure on a general fiber bundle over a general base manifold define the concept of the symbol of a multisymplectic form which is a polysymplectic form representing its leading order contribution and prove darboux theorems for the existenc... | [['we', 'introduce', 'the', 'concepts', 'of', 'a', 'multisymplectic', 'structure', 'and', 'a', 'polysymplectic', 'structure', 'on', 'a', 'general', 'fiber', 'bundle', 'over', 'a', 'general', 'base', 'manifold', 'define', 'the', 'concept', 'of', 'the', 'symbol', 'of', 'a', 'multisymplectic', 'form', 'which', 'is', 'a', ... | [-0.2295067547732648, 0.00176591181002979, -0.12812767265680827, 0.08099082464853055, -0.1582519081333336, -0.06693985371604422, -0.00045918021351099014, 0.28456305206384297, -0.3082010015001837, -0.17460088115536943, 0.06446396198369703, -0.1898910216284248, -0.24366705639744704, 0.11969381282633205, -0.07773639806458... |
708.1587 | Quantum theory and the observation problem | Quantum theory is applicable, in principle, to both the microscopic and
macroscopic realms. It is therefore worthwhile to investigate whether it is
possible to evolve a quantum-compatible view of the properties and states of
macroscopic objects in everyday thinking. It will allow a realistic
interpretation of quantum... | quant-ph | quantum theory is applicable in principle to both the microscopic and macroscopic realms it is therefore worthwhile to investigate whether it is possible to evolve a quantumcompatible view of the properties and states of macroscopic objects in everyday thinking it will allow a realistic interpretation of quantum theory... | [['quantum', 'theory', 'is', 'applicable', 'in', 'principle', 'to', 'both', 'the', 'microscopic', 'and', 'macroscopic', 'realms', 'it', 'is', 'therefore', 'worthwhile', 'to', 'investigate', 'whether', 'it', 'is', 'possible', 'to', 'evolve', 'a', 'quantumcompatible', 'view', 'of', 'the', 'properties', 'and', 'states', '... | [-0.08091340729151852, 0.1194769881497202, -0.1423214904630599, 0.0872127018724727, -0.14486520330485125, -0.15147849940959449, 0.04610413930706934, 0.3499233939219266, -0.31893881292886694, -0.30682649133946555, 0.08583098778895377, -0.2609866029795905, -0.1953994341416877, 0.1768566051879051, -0.11728096161228181, 0.... |
708.1588 | Vorticity and Magnetic Field Generation from Initial Anisotropy in
Ultrarelativistic Gamma-Ray Burst Blastwaves | Because conical segments of quasispherical ultrarelativistic blastwaves are
causally disconnected on angular scales larger than the blastwave inverse
Lorentz factor, astrophysical blastwaves can sustain initial anisotropy,
imprinted by the process that drives the explosion, while they remain
relativistic. We show tha... | astro-ph | because conical segments of quasispherical ultrarelativistic blastwaves are causally disconnected on angular scales larger than the blastwave inverse lorentz factor astrophysical blastwaves can sustain initial anisotropy imprinted by the process that drives the explosion while they remain relativistic we show that init... | [['because', 'conical', 'segments', 'of', 'quasispherical', 'ultrarelativistic', 'blastwaves', 'are', 'causally', 'disconnected', 'on', 'angular', 'scales', 'larger', 'than', 'the', 'blastwave', 'inverse', 'lorentz', 'factor', 'astrophysical', 'blastwaves', 'can', 'sustain', 'initial', 'anisotropy', 'imprinted', 'by', ... | [-0.13031774987730216, 0.2715874006137041, -0.08214663627188441, 0.1949128703921266, -0.10301919922865224, -0.07678753749977024, -0.0982914068165042, 0.38115216968229637, -0.24908811338948753, -0.2884986584408666, -0.014097058780948227, -0.26190559700447713, 0.10309859508108173, 0.20190210482102866, 0.06862711986166618... |
708.1589 | On the gap probability generating function at the spectrum edge in the
case of orthogonal symmetry | The gap probability generating function has as its coefficients the
probability of an interval containing exactly $k$ eigenvalues. For scaled
random matrices with orthogonal symmetry, and the interval at the hard or soft
spectrum edge, the gap probability generating functions have the special
property that they can b... | math-ph math.MP | the gap probability generating function has as its coefficients the probability of an interval containing exactly k eigenvalues for scaled random matrices with orthogonal symmetry and the interval at the hard or soft spectrum edge the gap probability generating functions have the special property that they can be evalu... | [['the', 'gap', 'probability', 'generating', 'function', 'has', 'as', 'its', 'coefficients', 'the', 'probability', 'of', 'an', 'interval', 'containing', 'exactly', 'k', 'eigenvalues', 'for', 'scaled', 'random', 'matrices', 'with', 'orthogonal', 'symmetry', 'and', 'the', 'interval', 'at', 'the', 'hard', 'or', 'soft', 's... | [-0.13414225303418423, 0.11591970930295172, -0.09708686294076845, 0.08567484405528275, -0.02392187830992043, -0.12364520182098271, 0.044554288504397445, 0.38297849083575636, -0.2676195856845946, -0.25432133402487417, 0.08809685143278997, -0.2610103052703305, -0.13977420592569498, 0.1650786108589398, -0.0098546750193628... |
708.159 | On the construction of Nadel multiplier ideal sheaves and the limiting
behavior of the Ricci flow | In this note we construct Nadel multiplier ideal sheaves using the Ricci flow
on Fano manifolds. This extends a result of Phong, Sesum and Sturm. These
sheaves, like their counterparts constructed by Nadel for the continuity
method, can be used to obtain an existence criterion for Kahler-Einstein
metrics.
| math.DG | in this note we construct nadel multiplier ideal sheaves using the ricci flow on fano manifolds this extends a result of phong sesum and sturm these sheaves like their counterparts constructed by nadel for the continuity method can be used to obtain an existence criterion for kahlereinstein metrics | [['in', 'this', 'note', 'we', 'construct', 'nadel', 'multiplier', 'ideal', 'sheaves', 'using', 'the', 'ricci', 'flow', 'on', 'fano', 'manifolds', 'this', 'extends', 'a', 'result', 'of', 'phong', 'sesum', 'and', 'sturm', 'these', 'sheaves', 'like', 'their', 'counterparts', 'constructed', 'by', 'nadel', 'for', 'the', 'co... | [-0.14746444179521254, -0.058517053584788904, -0.15513649821514264, 0.14117781314901853, -0.10514517830840002, -0.15986308619418801, -0.04917610401753336, 0.3355430711429411, -0.28462903122029576, -0.19352163745012754, 0.16002005291860164, -0.228026156546548, -0.1746647662560766, 0.2482287921011448, -0.2299759844512058... |
708.1591 | Every sum system is divisible | We show that every sum system is divisible. Combined with B. V. R. Bhat and
R. Srinivasan's result, this shows that every product system arising from a sum
system (and every generalized CCR flow) is either of type I or type III. A
necessarily and sufficient condition for such a product system to be of type I
is obtai... | math.OA math.FA | we show that every sum system is divisible combined with b v r bhat and r srinivasans result this shows that every product system arising from a sum system and every generalized ccr flow is either of type i or type iii a necessarily and sufficient condition for such a product system to be of type i is obtained | [['we', 'show', 'that', 'every', 'sum', 'system', 'is', 'divisible', 'combined', 'with', 'b', 'v', 'r', 'bhat', 'and', 'r', 'srinivasans', 'result', 'this', 'shows', 'that', 'every', 'product', 'system', 'arising', 'from', 'a', 'sum', 'system', 'and', 'every', 'generalized', 'ccr', 'flow', 'is', 'either', 'of', 'type',... | [-0.16572729963809252, 0.0622631101186612, -0.06296097426193542, -0.03979168168734759, -0.017633727462641125, -0.23177804538562638, 0.021142487566725446, 0.3296309144332491, -0.33405656961659935, -0.1922439350907145, 0.15218705933637403, -0.26719981671214615, -0.15054468024955614, 0.17409211196053517, -0.08700930387391... |
708.1592 | Other Exotic Scenarios at the LHC | The considerable center-of-mass energy and luminosity provided by the Large
Hadron Collider (LHC) will ensure a discovery reach for new particles which
extends well into the multi-TeV region. ATLAS and CMS have carried out many
studies of the implications of this capability for Beyond the Standard Model
physics. In t... | hep-ex | the considerable centerofmass energy and luminosity provided by the large hadron collider lhc will ensure a discovery reach for new particles which extends well into the multitev region atlas and cms have carried out many studies of the implications of this capability for beyond the standard model physics in this paper... | [['the', 'considerable', 'centerofmass', 'energy', 'and', 'luminosity', 'provided', 'by', 'the', 'large', 'hadron', 'collider', 'lhc', 'will', 'ensure', 'a', 'discovery', 'reach', 'for', 'new', 'particles', 'which', 'extends', 'well', 'into', 'the', 'multitev', 'region', 'atlas', 'and', 'cms', 'have', 'carried', 'out',... | [-0.020940325580353678, 0.15375728158831176, -0.043379929985746114, 0.1406634091957092, -0.09443043182853242, -0.15472811541165893, -0.018636885779568742, 0.291408016884201, -0.19114326303300094, -0.32144905974380145, 0.09809193508142054, -0.26371373348987437, -0.03081104786358249, 0.19124370747455724, 0.01714513629542... |
708.1593 | Updating Probabilities with Data and Moments | We use the method of Maximum (relative) Entropy to process information in the
form of observed data and moment constraints. The generic "canonical" form of
the posterior distribution for the problem of simultaneous updating with data
and moments is obtained. We discuss the general problem of non-commuting
constraints... | physics.data-an cs.IT math.IT math.ST physics.comp-ph physics.pop-ph stat.AP stat.CO stat.ME stat.TH | we use the method of maximum relative entropy to process information in the form of observed data and moment constraints the generic canonical form of the posterior distribution for the problem of simultaneous updating with data and moments is obtained we discuss the general problem of noncommuting constraints when the... | [['we', 'use', 'the', 'method', 'of', 'maximum', 'relative', 'entropy', 'to', 'process', 'information', 'in', 'the', 'form', 'of', 'observed', 'data', 'and', 'moment', 'constraints', 'the', 'generic', 'canonical', 'form', 'of', 'the', 'posterior', 'distribution', 'for', 'the', 'problem', 'of', 'simultaneous', 'updating... | [-0.060434672943186725, 0.08667273593855038, -0.08705687169810827, 0.10887039942189161, -0.08560145737108173, -0.14603014063986042, 0.04664241235269988, 0.3724093453345608, -0.3173124040889589, -0.32097935983085935, 0.13455520006474345, -0.277756356659251, -0.09145750327012207, 0.18329765044058424, -0.07524142303515839... |
708.1594 | Resonance phenomena in discrete systems with bichromatic input signal | We undertake a detailed numerical study of the twin phenomena of stochastic
and vibrational resonance in a discrete model system in the presence of
bichromatic input signal. A two parameter cubic map is used as the model that
combines the features of both bistable and threshold settings. Our analysis
brings out sever... | nlin.CD | we undertake a detailed numerical study of the twin phenomena of stochastic and vibrational resonance in a discrete model system in the presence of bichromatic input signal a two parameter cubic map is used as the model that combines the features of both bistable and threshold settings our analysis brings out several i... | [['we', 'undertake', 'a', 'detailed', 'numerical', 'study', 'of', 'the', 'twin', 'phenomena', 'of', 'stochastic', 'and', 'vibrational', 'resonance', 'in', 'a', 'discrete', 'model', 'system', 'in', 'the', 'presence', 'of', 'bichromatic', 'input', 'signal', 'a', 'two', 'parameter', 'cubic', 'map', 'is', 'used', 'as', 'th... | [-0.1302936991701859, 0.060678639128250444, -0.09817863358100792, 0.04294397063272259, -0.050875611569698866, -0.11052410442147169, 0.07914870331349137, 0.3411755193662536, -0.2827222218300711, -0.29509831781903917, 0.07844495384635085, -0.27124618352097163, -0.20024673368043458, 0.2189475154327984, 0.03333829601320463... |
708.1595 | A New Spin Foam Model for 4d Gravity | Starting from Plebanski formulation of gravity as a constrained BF theory we
propose a new spin foam model for 4d Riemannian quantum gravity that
generalises the well-known Barrett-Crane model and resolves the inherent to it
ultra-locality problem. The BF formulation of 4d gravity possesses two sectors:
gravitational... | gr-qc | starting from plebanski formulation of gravity as a constrained bf theory we propose a new spin foam model for 4d riemannian quantum gravity that generalises the wellknown barrettcrane model and resolves the inherent to it ultralocality problem the bf formulation of 4d gravity possesses two sectors gravitational and to... | [['starting', 'from', 'plebanski', 'formulation', 'of', 'gravity', 'as', 'a', 'constrained', 'bf', 'theory', 'we', 'propose', 'a', 'new', 'spin', 'foam', 'model', 'for', '4d', 'riemannian', 'quantum', 'gravity', 'that', 'generalises', 'the', 'wellknown', 'barrettcrane', 'model', 'and', 'resolves', 'the', 'inherent', 't... | [-0.09244185057750362, 0.1166540757572699, -0.10996911258647038, 0.07436473917914554, -0.1382709318441489, -0.1647426426681059, -0.020532693344941965, 0.26431660354301717, -0.22567884469284646, -0.29755217895510744, 0.04341292668100176, -0.2258048602530072, -0.2378530287213864, 0.13048737174868885, -0.12661796058302804... |
708.1596 | On similarity classes of well-rounded sublattices of $\mathbb Z^2$ | A lattice is called well-rounded if its minimal vectors span the
corresponding Euclidean space. In this paper we study the similarity classes of
well-rounded sublattices of ${\mathbb Z}^2$. We relate the set of all such
similarity classes to a subset of primitive Pythagorean triples, and prove that
it has structure o... | math.NT | a lattice is called wellrounded if its minimal vectors span the corresponding euclidean space in this paper we study the similarity classes of wellrounded sublattices of mathbb z2 we relate the set of all such similarity classes to a subset of primitive pythagorean triples and prove that it has structure of a noncommut... | [['a', 'lattice', 'is', 'called', 'wellrounded', 'if', 'its', 'minimal', 'vectors', 'span', 'the', 'corresponding', 'euclidean', 'space', 'in', 'this', 'paper', 'we', 'study', 'the', 'similarity', 'classes', 'of', 'wellrounded', 'sublattices', 'of', 'mathbb', 'z2', 'we', 'relate', 'the', 'set', 'of', 'all', 'such', 'si... | [-0.16792336353536347, 0.07866120455357775, -0.06464161018995072, 0.07401899374827153, -0.09979607914607945, -0.0792383153243627, 0.04335379425818168, 0.40186137996828386, -0.3481506260326333, -0.19735821010754276, 0.06008716173748077, -0.3021276962150662, -0.16444806177705099, 0.13732454944535982, -0.06522184673515852... |
708.1597 | New lower bounds on the non-zero capacity of Pauli Channels | We study encodings that give the best known thresholds for the non-zero
capacity of quantum channels, i.e., the upper bound for correctable noise,
using an entropic approach to calculation of the threshold values. Our results
show that Pauli noise is correctable up to the hashing bound. For a
depolarizing channel, th... | quant-ph | we study encodings that give the best known thresholds for the nonzero capacity of quantum channels ie the upper bound for correctable noise using an entropic approach to calculation of the threshold values our results show that pauli noise is correctable up to the hashing bound for a depolarizing channel this approach... | [['we', 'study', 'encodings', 'that', 'give', 'the', 'best', 'known', 'thresholds', 'for', 'the', 'nonzero', 'capacity', 'of', 'quantum', 'channels', 'ie', 'the', 'upper', 'bound', 'for', 'correctable', 'noise', 'using', 'an', 'entropic', 'approach', 'to', 'calculation', 'of', 'the', 'threshold', 'values', 'our', 'resu... | [-0.16503530885301418, 0.12279130818184167, -0.07021621359623413, 0.09476918291383937, 0.011958017660332705, -0.21120540264632498, 0.19211347250670974, 0.3217309840273724, -0.22034846916238762, -0.26933721104052977, 0.0619279629995685, -0.2472413605004775, -0.13189144666070368, 0.24974347603743646, -0.08587314145215579... |
708.1598 | Genomes: at the edge of chaos with maximum information capacity | We propose an order index, phi, which quantifies the notion of ``life at the
edge of chaos'' when applied to genome sequences. It maps genomes to a number
from 0 (random and of infinite length) to 1 (fully ordered) and applies
regardless of sequence length. The 786 complete genomic sequences in GenBank
were found to ... | q-bio.GN | we propose an order index phi which quantifies the notion of life at the edge of chaos when applied to genome sequences it maps genomes to a number from 0 random and of infinite length to 1 fully ordered and applies regardless of sequence length the 786 complete genomic sequences in genbank were found to have phi value... | [['we', 'propose', 'an', 'order', 'index', 'phi', 'which', 'quantifies', 'the', 'notion', 'of', 'life', 'at', 'the', 'edge', 'of', 'chaos', 'when', 'applied', 'to', 'genome', 'sequences', 'it', 'maps', 'genomes', 'to', 'a', 'number', 'from', '0', 'random', 'and', 'of', 'infinite', 'length', 'to', '1', 'fully', 'ordered... | [-0.1455346814622542, 0.1972337086012523, -0.05964571227673936, 0.05854209159782985, 0.022131704094827967, -0.08414397388284581, 0.05816298185958964, 0.3940505316167806, -0.32171217902703625, -0.2535942792562784, 0.07678957715057727, -0.26336647246230754, -0.13652085877987927, 0.149692396246993, -0.07163070108833534, 0... |
708.1599 | Constructing Merger Trees that Mimic N-Body Simulations | We present a simple and efficient empirical algorithm for constructing
dark-matter halo merger trees that reproduce the distribution of trees in the
Millennium cosmological $N$-body simulation. The generated trees are
significantly better than EPS trees. The algorithm is Markovian, and it
therefore fails to reproduce... | astro-ph | we present a simple and efficient empirical algorithm for constructing darkmatter halo merger trees that reproduce the distribution of trees in the millennium cosmological nbody simulation the generated trees are significantly better than eps trees the algorithm is markovian and it therefore fails to reproduce the nonm... | [['we', 'present', 'a', 'simple', 'and', 'efficient', 'empirical', 'algorithm', 'for', 'constructing', 'darkmatter', 'halo', 'merger', 'trees', 'that', 'reproduce', 'the', 'distribution', 'of', 'trees', 'in', 'the', 'millennium', 'cosmological', 'nbody', 'simulation', 'the', 'generated', 'trees', 'are', 'significantly'... | [-0.07165075274818439, 0.09442687808219256, -0.12878933734696438, 0.15521460556997324, -0.08965218105933015, -0.08427339246338035, 0.02860787184970909, 0.3743400234466498, -0.22136869580742527, -0.30881270886141254, 0.05913335600176806, -0.25698731223894083, -0.06777526534503348, 0.19854818081651676, -0.022505634033339... |
708.16 | Backward-angle photoproduction of $\pi^0$ mesons on the proton at
$E_\gamma$ = 1.5--2.4 GeV | Differential cross sections and photon beam asymmetries for $\pi^0$
photoproduction have been measured at $E_\gamma$ = 1.5--2.4 GeV and at the
$\pi^0$ scattering angles, --1 $<$ cos$\Theta_{c.m.} <$ --0.6. The
energy-dependent slope of differential cross sections for $u$-channel $\pi^0$
production has been determined... | nucl-ex | differential cross sections and photon beam asymmetries for pi0 photoproduction have been measured at e_gamma 1524 gev and at the pi0 scattering angles 1 costheta_cm 06 the energydependent slope of differential cross sections for uchannel pi0 production has been determined an enhancement at backward angles is found abo... | [['differential', 'cross', 'sections', 'and', 'photon', 'beam', 'asymmetries', 'for', 'pi0', 'photoproduction', 'have', 'been', 'measured', 'at', 'e_gamma', '1524', 'gev', 'and', 'at', 'the', 'pi0', 'scattering', 'angles', '1', 'costheta_cm', '06', 'the', 'energydependent', 'slope', 'of', 'differential', 'cross', 'sect... | [-0.07988811836479918, 0.2279963020592205, -0.08902175143655193, 0.16579271802605178, -0.05099314659049636, -0.105951952125485, -0.00508382081201202, 0.41243457962807856, -0.19463972848545957, -0.33871997265439285, -0.10422859635988349, -0.3982085393055489, 0.11019762062320584, 0.19953482484346943, 0.10145880529460938,... |
708.1601 | On the mean square of the divisor function in short intervals | We provide upper bounds for the mean square integral $$
\int_X^{2X}(\Delta_k(x+h) - \Delta_k(x))^2 dx \qquad(h = h(X)\gg1, h = o(x)
{\roman{as}} X\to\infty) $$ where $h$ lies in a suitable range. For $k\ge2$ a
fixed integer, $\Delta_k(x)$ is the error term in the asymptotic formula for
the summatory function of the d... | math.NT | we provide upper bounds for the mean square integral int_x2xdelta_kxh delta_kx2 dx qquadh hxgg1 h ox romanas xtoinfty where h lies in a suitable range for kge2 a fixed integer delta_kx is the error term in the asymptotic formula for the summatory function of the divisor function d_kn generated by zetaks | [['we', 'provide', 'upper', 'bounds', 'for', 'the', 'mean', 'square', 'integral', 'int_x2xdelta_kxh', 'delta_kx2', 'dx', 'qquadh', 'hxgg1', 'h', 'ox', 'romanas', 'xtoinfty', 'where', 'h', 'lies', 'in', 'a', 'suitable', 'range', 'for', 'kge2', 'a', 'fixed', 'integer', 'delta_kx', 'is', 'the', 'error', 'term', 'in', 'the... | [-0.21222226065066124, 0.0772327901226365, -0.048921541321194834, 0.11683760739914659, -0.03433150174613628, -0.14024807690746255, 0.05704400155356982, 0.31431518099788164, -0.2817589481671651, -0.2093971995688561, 0.11992920200961331, -0.28722874851276475, -0.10635406492898862, 0.2283401555692156, -0.05329659167263242... |
708.1602 | Three-Body Forces Produced by a Similarity Renormalization Group
Transformation in a Simple Model | A simple class of unitary renormalization group transformations that force
hamiltonians towards a band-diagonal form produce few-body interactions in
which low- and high-energy states are decoupled, which can greatly simplify
many-body calculations. One such transformation has been applied to
phenomenological and eff... | nucl-th cond-mat.str-el hep-ph | a simple class of unitary renormalization group transformations that force hamiltonians towards a banddiagonal form produce fewbody interactions in which low and highenergy states are decoupled which can greatly simplify manybody calculations one such transformation has been applied to phenomenological and effective fi... | [['a', 'simple', 'class', 'of', 'unitary', 'renormalization', 'group', 'transformations', 'that', 'force', 'hamiltonians', 'towards', 'a', 'banddiagonal', 'form', 'produce', 'fewbody', 'interactions', 'in', 'which', 'low', 'and', 'highenergy', 'states', 'are', 'decoupled', 'which', 'can', 'greatly', 'simplify', 'manybo... | [-0.10405592837923905, 0.18560751401082598, -0.155989886964259, 0.06515091013837566, -0.07058739033770205, -0.16425351117019696, -0.0013378358853515238, 0.38225094021860667, -0.2535628705081763, -0.2863793212673045, -0.019312274245748995, -0.2711575043310101, -0.17544743049074896, 0.12531099561116812, 0.032621445674029... |
708.1603 | How the First Stars Regulated Local Star Formation I: Radiative Feedback | We present numerical simulations of how a 120 M$_\odot$ primordial star
regulates star formation in nearby cosmological halos at $z \sim$ 20 by
photoevaporation. Our models include nine-species primordial chemistry and
self-consistent multifrequency conservative transfer of UV photons with all
relevant radiative proc... | astro-ph | we present numerical simulations of how a 120 m_odot primordial star regulates star formation in nearby cosmological halos at z sim 20 by photoevaporation our models include ninespecies primordial chemistry and selfconsistent multifrequency conservative transfer of uv photons with all relevant radiative processes wheth... | [['we', 'present', 'numerical', 'simulations', 'of', 'how', 'a', '120', 'm_odot', 'primordial', 'star', 'regulates', 'star', 'formation', 'in', 'nearby', 'cosmological', 'halos', 'at', 'z', 'sim', '20', 'by', 'photoevaporation', 'our', 'models', 'include', 'ninespecies', 'primordial', 'chemistry', 'and', 'selfconsisten... | [-0.04105988398614765, 0.1937516751875468, -0.011994503506287498, 0.10906231426407845, -0.08164980821141937, -0.056353569900627176, 0.049753756873825, 0.40247612294641516, -0.15075585518814444, -0.3723524116269014, 0.05372549911895405, -0.28235275258572357, 0.0002859046646547549, 0.14213964226655662, 0.0071036128759004... |
708.1604 | On determination of periods of geometric continued fractions for
two-dimensional algebraic hyperbolic operators | For a given sequence of positive integers we make an explicit construction of
a reduced hyperbolic operator in SL(2,z) with the sequence as a period of a
geometric continued fraction in the sense of Klein. Further we experimentally
study an algorithm to construct a period for an arbitrary operator of SL(2,z)
(the Gau... | math.NT | for a given sequence of positive integers we make an explicit construction of a reduced hyperbolic operator in sl2z with the sequence as a period of a geometric continued fraction in the sense of klein further we experimentally study an algorithm to construct a period for an arbitrary operator of sl2z the gauss reducti... | [['for', 'a', 'given', 'sequence', 'of', 'positive', 'integers', 'we', 'make', 'an', 'explicit', 'construction', 'of', 'a', 'reduced', 'hyperbolic', 'operator', 'in', 'sl2z', 'with', 'the', 'sequence', 'as', 'a', 'period', 'of', 'a', 'geometric', 'continued', 'fraction', 'in', 'the', 'sense', 'of', 'klein', 'further', ... | [-0.18318111729723485, 0.10939118863713124, -0.10907414614815604, 0.05137999030676755, -0.09161251190711152, -0.07402114762331952, 0.06471327645915814, 0.33097500425170767, -0.2929989413104274, -0.2387310491028157, 0.09016537124037065, -0.23074379879134624, -0.20616227545860139, 0.23126915188675576, -0.1197166092185811... |
708.1605 | On families of $BS_{can}$ lagrangian tori in projective spaces | This small note contains two simple remarks about Bohr - Sommerfeld with
respect to the anticanonical class lagrangian tori in the projective spaces,
which are the most popular examples of monotone symplectic manifolds.
| math.SG | this small note contains two simple remarks about bohr sommerfeld with respect to the anticanonical class lagrangian tori in the projective spaces which are the most popular examples of monotone symplectic manifolds | [['this', 'small', 'note', 'contains', 'two', 'simple', 'remarks', 'about', 'bohr', 'sommerfeld', 'with', 'respect', 'to', 'the', 'anticanonical', 'class', 'lagrangian', 'tori', 'in', 'the', 'projective', 'spaces', 'which', 'are', 'the', 'most', 'popular', 'examples', 'of', 'monotone', 'symplectic', 'manifolds']] | [-0.18521091502043419, 0.06674463808849396, 0.023569037555716932, 0.14542190920838038, -0.16037475322082173, -0.1869908546213992, -0.09701467653212603, 0.3459484815830365, -0.2334312241182488, -0.21973795024132414, 0.09072821648805984, -0.34008218711824156, -0.15606512234080583, 0.23313913313904777, -0.2436717995733488... |
708.1606 | A Corona Australis cloud filament seen in NIR scattered light I.
Comparison with extinction of background stars | With current near-infrared (NIR) instruments the near-infrared light
scattered from interstellar clouds can be mapped over large areas. The surface
brightness carries information on the line-of-sight dust column density.
Therefore, scattered light could provide an important tool to study mass
distribution in quiescen... | astro-ph | with current nearinfrared nir instruments the nearinfrared light scattered from interstellar clouds can be mapped over large areas the surface brightness carries information on the lineofsight dust column density therefore scattered light could provide an important tool to study mass distribution in quiescent interstel... | [['with', 'current', 'nearinfrared', 'nir', 'instruments', 'the', 'nearinfrared', 'light', 'scattered', 'from', 'interstellar', 'clouds', 'can', 'be', 'mapped', 'over', 'large', 'areas', 'the', 'surface', 'brightness', 'carries', 'information', 'on', 'the', 'lineofsight', 'dust', 'column', 'density', 'therefore', 'scat... | [-0.04412365471775495, 0.11102503528994587, -0.11256938965727939, 0.09367644041818837, -0.045418459851213774, -0.04833602705174058, 0.049697660292714725, 0.4712966185576026, -0.21764802190296326, -0.33281330882733606, 0.06110762943685784, -0.2925181059534594, -0.04398605122865326, 0.1821266619726489, -0.090219013757355... |
708.1607 | The solar photospheric abundance of phosphorus: results from co5bold 3D
model atmospheres | aims: We determine the solar abundance of phosphorus using co5bold 3D
hydrodynamic model atmospheres. method: High resolution, high signal-to-noise
solar spectra of the PI lines of Multiplet 1 at 1051-1068 nm are compared to
line formation computations performed on a co5bold solar model atmosphere.
results: We find A... | astro-ph | aims we determine the solar abundance of phosphorus using co5bold 3d hydrodynamic model atmospheres method high resolution high signaltonoise solar spectra of the pi lines of multiplet 1 at 10511068 nm are compared to line formation computations performed on a co5bold solar model atmosphere results we find ap546 004 in... | [['aims', 'we', 'determine', 'the', 'solar', 'abundance', 'of', 'phosphorus', 'using', 'co5bold', '3d', 'hydrodynamic', 'model', 'atmospheres', 'method', 'high', 'resolution', 'high', 'signaltonoise', 'solar', 'spectra', 'of', 'the', 'pi', 'lines', 'of', 'multiplet', '1', 'at', '10511068', 'nm', 'are', 'compared', 'to'... | [-0.03546229266435092, 0.1256682526236321, 0.008661555563495639, 0.09392280310584968, -0.023221014481451776, -0.11154589330904002, 0.05674674336361572, 0.42156435633768086, -0.13808788978322237, -0.38941285276302584, -0.004882800714026585, -0.3189076683311551, -0.049640727114438274, 0.18591675299714194, -0.085588888753... |
708.1608 | Similarity classes of 3x3 matrices over a local principal ideal ring | In this paper similarity classes of three by three matrices over a local
principal ideal commutative ring are analyzed. When the residue field is
finite, a generating function for the number of similarity classes for all
finite quotients of the ring is computed explicitly.
| math.GR math.RA | in this paper similarity classes of three by three matrices over a local principal ideal commutative ring are analyzed when the residue field is finite a generating function for the number of similarity classes for all finite quotients of the ring is computed explicitly | [['in', 'this', 'paper', 'similarity', 'classes', 'of', 'three', 'by', 'three', 'matrices', 'over', 'a', 'local', 'principal', 'ideal', 'commutative', 'ring', 'are', 'analyzed', 'when', 'the', 'residue', 'field', 'is', 'finite', 'a', 'generating', 'function', 'for', 'the', 'number', 'of', 'similarity', 'classes', 'for'... | [-0.19751349474642088, 0.09229581538503143, -0.05222958631136201, 0.061457304826366126, -0.010713456695984032, -0.0920252504716204, -0.08028386325564828, 0.34640102655711497, -0.35579728792336857, -0.21111023964741352, 0.0815009283065923, -0.252040707082911, -0.09907759673131461, 0.2114140993746167, -0.0252843515058471... |
708.1609 | Cosmic rays from thermal sources | Energy spectrum of cosmic rays (CR) exhibits power-like behavior with very
characteristic "knee" structure. We consider a generalized statistical model
for the production process of cosmic rays which accounts for such behavior in a
natural way either by assuming existence of temperature fluctuations in the
source of ... | astro-ph hep-ph | energy spectrum of cosmic rays cr exhibits powerlike behavior with very characteristic knee structure we consider a generalized statistical model for the production process of cosmic rays which accounts for such behavior in a natural way either by assuming existence of temperature fluctuations in the source of cr or by... | [['energy', 'spectrum', 'of', 'cosmic', 'rays', 'cr', 'exhibits', 'powerlike', 'behavior', 'with', 'very', 'characteristic', 'knee', 'structure', 'we', 'consider', 'a', 'generalized', 'statistical', 'model', 'for', 'the', 'production', 'process', 'of', 'cosmic', 'rays', 'which', 'accounts', 'for', 'such', 'behavior', '... | [-0.12855029511410976, 0.1676847128692316, -0.10071722043600555, 0.1409475176570633, -0.029818510995634522, -0.08952370468856923, -0.00013591656170319766, 0.3523061128604847, -0.30199260792384547, -0.31468305668871227, -0.01515957908971662, -0.3055461555486545, -0.08429436289831453, 0.17067003814251316, 0.0166435943538... |
708.161 | Relaxation of transport properties in electron doped SrTiO3 | We electron-dope single crystal samples of SrTiO_3 by exposing them to Ar^+
irradiation and observe carrier mobility similar in its magnitude and
temperature dependence to the carrier mobility in other electron-doped SrTiO3
systems. We find that some transport properties are time-dependent. In
particular, the sheet r... | cond-mat.other | we electrondope single crystal samples of srtio_3 by exposing them to ar irradiation and observe carrier mobility similar in its magnitude and temperature dependence to the carrier mobility in other electrondoped srtio3 systems we find that some transport properties are timedependent in particular the sheet resistance ... | [['we', 'electrondope', 'single', 'crystal', 'samples', 'of', 'srtio_3', 'by', 'exposing', 'them', 'to', 'ar', 'irradiation', 'and', 'observe', 'carrier', 'mobility', 'similar', 'in', 'its', 'magnitude', 'and', 'temperature', 'dependence', 'to', 'the', 'carrier', 'mobility', 'in', 'other', 'electrondoped', 'srtio3', 's... | [-0.1064525313383664, 0.17438358544944982, -0.00962054282660892, -0.00028665785888383157, 0.016636020414172167, -0.1326766926851348, 0.14421063769294554, 0.47108923805406294, -0.3089303917599371, -0.33443917176989185, -0.025753594854992467, -0.3601357117295265, -0.08599867852382272, 0.16155412000483352, -0.000203561688... |
708.1611 | DGP Cosmology with a Non-Minimally Coupled Scalar Field on the Brane | We construct a DGP inspired braneworld scenario where a scalar field
non-minimally coupled to the induced Ricci curvature is present on the brane.
First we investigate the status of gravitational potential with non-minimal
coupling and observational constraints on this non-minimal model. Then we
further deepen the id... | hep-th | we construct a dgp inspired braneworld scenario where a scalar field nonminimally coupled to the induced ricci curvature is present on the brane first we investigate the status of gravitational potential with nonminimal coupling and observational constraints on this nonminimal model then we further deepen the idea of e... | [['we', 'construct', 'a', 'dgp', 'inspired', 'braneworld', 'scenario', 'where', 'a', 'scalar', 'field', 'nonminimally', 'coupled', 'to', 'the', 'induced', 'ricci', 'curvature', 'is', 'present', 'on', 'the', 'brane', 'first', 'we', 'investigate', 'the', 'status', 'of', 'gravitational', 'potential', 'with', 'nonminimal',... | [-0.1793976168823885, 0.10683195738067083, -0.0731530534240472, 0.10780236914333906, -0.18402805429079808, -0.1837983032284469, -0.06496734898217826, 0.3179895626472346, -0.18005690522784112, -0.31254222556291256, 0.0322955643539043, -0.22116511678505762, -0.14759263458351293, 0.11069122224808763, -0.018912149047679908... |
708.1612 | Flavor SU(3) analysis of charmless B->PP decays | We perform a global fits to charmless $B \to PP$ decays which independently
constrain the $(\bar\rho,\bar\eta)$ vertex of the unitarity triangle. The
fitted amplitudes and phase are used to predict the branching ratios and CP
asymmetries of all decay modes, including those of the $B_s$ system. Different
schemes of SU... | hep-ph | we perform a global fits to charmless b to pp decays which independently constrain the barrhobareta vertex of the unitarity triangle the fitted amplitudes and phase are used to predict the branching ratios and cp asymmetries of all decay modes including those of the b_s system different schemes of su3 breaking in decay... | [['we', 'perform', 'a', 'global', 'fits', 'to', 'charmless', 'b', 'to', 'pp', 'decays', 'which', 'independently', 'constrain', 'the', 'barrhobareta', 'vertex', 'of', 'the', 'unitarity', 'triangle', 'the', 'fitted', 'amplitudes', 'and', 'phase', 'are', 'used', 'to', 'predict', 'the', 'branching', 'ratios', 'and', 'cp', ... | [-0.10649835530219004, 0.23076201893854886, -0.09530010427503537, 0.11350532530114935, -0.07244327976756419, -0.15976622269954532, 0.08346880483764431, 0.28267605337249635, -0.25095849085806143, -0.22808976880171233, 0.0164185067971832, -0.3205307619064115, -0.004568998171533976, 0.10506763831815785, 0.0973704422358423... |
708.1613 | Simplified Version of the Nucleon and Delta-Isobar Description | Considering synchronous spin-isospin rotation as a collective motion a
simplified scheme of the nucleon and delta isobar description is formulated.
| nucl-th | considering synchronous spinisospin rotation as a collective motion a simplified scheme of the nucleon and delta isobar description is formulated | [['considering', 'synchronous', 'spinisospin', 'rotation', 'as', 'a', 'collective', 'motion', 'a', 'simplified', 'scheme', 'of', 'the', 'nucleon', 'and', 'delta', 'isobar', 'description', 'is', 'formulated']] | [-0.20119131542742252, 0.19327360143652186, -0.11241795783862471, 0.10373573697288521, -0.08068899698555469, -0.13559377952478827, 0.06260723043233156, 0.28005918497219684, -0.20384346551727503, -0.23859600722789764, -0.11443697707727551, -0.15810000374913216, -0.08375904578715562, 0.08224919978529215, -0.0006148927845... |
708.1614 | Measurement of The Time-Dependent CP Asymmetry in B0 --> K*0 gamma
Decays | We present a preliminary measurement of the time-dependent CP asymmetry in B0
--> K*0 (K_S0 pi0) gamma decays based on 431 x 10^6 Upsilon(4S) --> BBbar
decays collected with the BaBar detector at the PEP-II asymmetric-energy e+e-
collider at SLAC. In a sample containing 316 +/- 22 signal events we measure
S_{K* gamma... | hep-ex | we present a preliminary measurement of the timedependent cp asymmetry in b0 k0 k_s0 pi0 gamma decays based on 431 x 106 upsilon4s bbbar decays collected with the babar detector at the pepii asymmetricenergy ee collider at slac in a sample containing 316 22 signal events we measure s_k gamma 008 031 005 and c_k gamma 0... | [['we', 'present', 'a', 'preliminary', 'measurement', 'of', 'the', 'timedependent', 'cp', 'asymmetry', 'in', 'b0', 'k0', 'k_s0', 'pi0', 'gamma', 'decays', 'based', 'on', '431', 'x', '106', 'upsilon4s', 'bbbar', 'decays', 'collected', 'with', 'the', 'babar', 'detector', 'at', 'the', 'pepii', 'asymmetricenergy', 'ee', 'c... | [-0.13309631378135897, 0.21030057407915592, -0.09898002139490211, 0.05546427928757938, -0.042968902190103, -0.14165050766402573, 0.15782209267049577, 0.28262143620910746, -0.15375691059638152, -0.2899628725805969, -0.07381794850384309, -0.6076924351932989, 0.19330733760514043, 0.1485098401035154, 0.08425690906799653, 0... |
708.1615 | Classical limit of the Casimir entropy for scalar massless field | We study the Casimir effect at finite temperature for a massless scalar field
in the parallel plates geometry in N spatial dimensions, under various
combinations of Dirichlet and Neumann boundary conditions on the plates. We
show that in all these cases the entropy, in the limit where energy
equipartitioning applies,... | quant-ph | we study the casimir effect at finite temperature for a massless scalar field in the parallel plates geometry in n spatial dimensions under various combinations of dirichlet and neumann boundary conditions on the plates we show that in all these cases the entropy in the limit where energy equipartitioning applies is a ... | [['we', 'study', 'the', 'casimir', 'effect', 'at', 'finite', 'temperature', 'for', 'a', 'massless', 'scalar', 'field', 'in', 'the', 'parallel', 'plates', 'geometry', 'in', 'n', 'spatial', 'dimensions', 'under', 'various', 'combinations', 'of', 'dirichlet', 'and', 'neumann', 'boundary', 'conditions', 'on', 'the', 'plate... | [-0.19296816693589328, 0.1810994100653463, -0.07353234916393246, 0.021743199797273273, -0.03437556226974323, -0.10978082630280701, -0.03086062397120432, 0.33239038477444816, -0.22504699828162317, -0.24491453575827773, 0.06388524681004504, -0.2599578606230872, -0.09982843206648434, 0.17964729496706572, -0.02542940066713... |
708.1616 | Robustness of the second law of thermodynamics under generalizations of
the maximum entropy method | It is shown that the laws of thermodynamics are extremely robust under
generalizations of the form of entropy. Using the Bregman-type relative
entropy, the Clausius inequality is proved to be always valid. This implies
that thermodynamics is highly universal and does not rule out consistent
generalization of the maxi... | cond-mat.stat-mech | it is shown that the laws of thermodynamics are extremely robust under generalizations of the form of entropy using the bregmantype relative entropy the clausius inequality is proved to be always valid this implies that thermodynamics is highly universal and does not rule out consistent generalization of the maximum en... | [['it', 'is', 'shown', 'that', 'the', 'laws', 'of', 'thermodynamics', 'are', 'extremely', 'robust', 'under', 'generalizations', 'of', 'the', 'form', 'of', 'entropy', 'using', 'the', 'bregmantype', 'relative', 'entropy', 'the', 'clausius', 'inequality', 'is', 'proved', 'to', 'be', 'always', 'valid', 'this', 'implies', '... | [-0.08741817898815497, 0.12114739973098039, -0.17272068277001382, 0.10927714844699948, -0.04187465842813253, -0.19518694994971156, 0.06032089658081532, 0.2646878905966878, -0.26907821398228404, -0.20694457542151212, 0.08783541577868163, -0.2773922475427389, -0.13225291475653647, 0.25374450616538524, -0.1469516083598137... |
708.1617 | Evidence that a cluster of UHECRs was produced by a burst or flare | The angular clustering of 5 Ultrahigh Energy Cosmic Rays (UHECRs) in the
combined published AGASA-HiRes data has a probability of ~ 2 10^-3 of occurring
by chance. A first analysis of the implications of the event energies and
angular spreading is presented, which is applicable if the source is close
enough that GZK ... | astro-ph | the angular clustering of 5 ultrahigh energy cosmic rays uhecrs in the combined published agasahires data has a probability of 2 103 of occurring by chance a first analysis of the implications of the event energies and angular spreading is presented which is applicable if the source is close enough that gzk losses can ... | [['the', 'angular', 'clustering', 'of', '5', 'ultrahigh', 'energy', 'cosmic', 'rays', 'uhecrs', 'in', 'the', 'combined', 'published', 'agasahires', 'data', 'has', 'a', 'probability', 'of', '2', '103', 'of', 'occurring', 'by', 'chance', 'a', 'first', 'analysis', 'of', 'the', 'implications', 'of', 'the', 'event', 'energi... | [-0.13691435630017942, 0.21003306081921264, -0.060582221731090465, 0.14430585612166938, -0.03781790923440476, -0.06866251887608874, 0.009933585006070349, 0.3965725621107865, -0.22859997808857746, -0.3440432397623521, 0.02438981146819109, -0.3329735643001678, 0.0368949554678103, 0.19555142321749716, 0.02333942361528406,... |
708.1618 | Gluon Vortices and Induced Magnetic Field in Compact Stars | The natural candidates for the realization of color superconductivity are the
extremely dense cores of compact stars, many of which have very large magnetic
fields, especially the so-called magnetars. In this paper we discuss how a
color superconducting core can serve to generate and enhance the stellar
magnetic fiel... | astro-ph hep-ph nucl-th | the natural candidates for the realization of color superconductivity are the extremely dense cores of compact stars many of which have very large magnetic fields especially the socalled magnetars in this paper we discuss how a color superconducting core can serve to generate and enhance the stellar magnetic field with... | [['the', 'natural', 'candidates', 'for', 'the', 'realization', 'of', 'color', 'superconductivity', 'are', 'the', 'extremely', 'dense', 'cores', 'of', 'compact', 'stars', 'many', 'of', 'which', 'have', 'very', 'large', 'magnetic', 'fields', 'especially', 'the', 'socalled', 'magnetars', 'in', 'this', 'paper', 'we', 'disc... | [-0.13533939213292406, 0.21046140542187328, -0.0453157235668706, 0.14506420561935687, -0.16338841763873851, -0.05485557972653104, 0.028155647469767637, 0.3978125590697995, -0.19711734454280563, -0.3466182321176997, 0.06456082373915706, -0.1724450285879097, -0.09189117590098508, 0.21773095003196172, -0.04759029395479176... |
708.1619 | Magnetic Phases in Dense Quark Matter | In this paper I discuss the magnetic phases of the three-flavor color
superconductor. These phases can take place at different field strengths in a
highly dense quark system. Given that the best natural candidates for the
realization of color superconductivity are the extremely dense cores of neutron
stars, which typ... | nucl-th astro-ph hep-ph | in this paper i discuss the magnetic phases of the threeflavor color superconductor these phases can take place at different field strengths in a highly dense quark system given that the best natural candidates for the realization of color superconductivity are the extremely dense cores of neutron stars which typically... | [['in', 'this', 'paper', 'i', 'discuss', 'the', 'magnetic', 'phases', 'of', 'the', 'threeflavor', 'color', 'superconductor', 'these', 'phases', 'can', 'take', 'place', 'at', 'different', 'field', 'strengths', 'in', 'a', 'highly', 'dense', 'quark', 'system', 'given', 'that', 'the', 'best', 'natural', 'candidates', 'for'... | [-0.14790873681860311, 0.2539502893973674, -0.048353057960048317, 0.06612581623152697, -0.06742610254191926, -0.07283816376834043, 0.052722395705391785, 0.3941003362515143, -0.187216295275305, -0.31566616826291594, 0.0615020559934367, -0.20564442123619042, -0.07473434624927384, 0.1605346569126206, 0.003586489407877837,... |
708.162 | The group of automorphisms of the first Weyl algebra in prime
characteristic and the restriction map | Let $K$ be a {\em perfect} field of characteristic $p>0$, $A_1:=K< x, \der |
\der x- x\der =1>$ be the first Weyl algebra and $Z:=K[X:=x^p, Y:=\der^p]$ be
its centre. It is proved that $(i)$ the restriction map $\res :\Aut_K(A_1)\ra
\Aut_K(Z), \s \mapsto \s|_Z$, is a monomorphism with $\im (\res) = \G :=\{\tau
\in \A... | math.RA math.AG | let k be a em perfect field of characteristic p0 a_1k x der der x xder 1 be the first weyl algebra and zkxxp yderp be its centre it is proved that i the restriction map res aut_ka_1ra aut_kz s mapsto s_z is a monomorphism with im res g tau in aut_kz cj tau 1 where cj tau is the jacobian of tau note that aut_kzkltimes g... | [['let', 'k', 'be', 'a', 'em', 'perfect', 'field', 'of', 'characteristic', 'p0', 'a_1k', 'x', 'der', 'der', 'x', 'xder', '1', 'be', 'the', 'first', 'weyl', 'algebra', 'and', 'zkxxp', 'yderp', 'be', 'its', 'centre', 'it', 'is', 'proved', 'that', 'i', 'the', 'restriction', 'map', 'res', 'aut_ka_1ra', 'aut_kz', 's', 'maps... | [-0.23613165066457603, 0.11408766675518944, -0.06833954634311706, -0.0013663016551577333, -0.10051380631638997, -0.24473846933123336, 0.0165069645241167, 0.3264309502026038, -0.3489878422844766, -0.1786425868257769, 0.029392828217902178, -0.2740086488001771, -0.10489079928539916, 0.16709412312927419, -0.059462156952984... |
708.1621 | Memorino on the `1/2 vs. 3/2 Puzzle' in $\bar B \to l \bar \nu X_c$ -- a
Year Later and a Bit Wiser | The OPE treatment that has been so successful in describing inclusive $\bar B
\to l \bar \nu X_c$ decays yields sum rules (in particular the Uraltsev sum
rule and its higher moments) implying the dominance of the $P$ wave $j_q = 3/2$
charm states in $X_c$ over their $j_q=1/2$ counterparts. This prediction is
supporte... | hep-ph | the ope treatment that has been so successful in describing inclusive bar b to l bar nu x_c decays yields sum rules in particular the uraltsev sum rule and its higher moments implying the dominance of the p wave j_q 32 charm states in x_c over their j_q12 counterparts this prediction is supported by other general argum... | [['the', 'ope', 'treatment', 'that', 'has', 'been', 'so', 'successful', 'in', 'describing', 'inclusive', 'bar', 'b', 'to', 'l', 'bar', 'nu', 'x_c', 'decays', 'yields', 'sum', 'rules', 'in', 'particular', 'the', 'uraltsev', 'sum', 'rule', 'and', 'its', 'higher', 'moments', 'implying', 'the', 'dominance', 'of', 'the', 'p... | [-0.09022357481263382, 0.1505924111906252, -0.08821246003138317, 0.10107760793401344, -0.0759841279984822, -0.16245944349819136, 0.12824602766871437, 0.3582747109218065, -0.21233998742727278, -0.30406667962344974, 0.06617975042417125, -0.30272110561356275, -0.07410315650324113, 0.14166805689633868, -0.01609637247862123... |
708.1622 | Classifying finite localizations of quasi-coherent sheaves | Given a quasi-compact, quasi-separated scheme X, a bijection between the
tensor localizing subcategories of finite type in Qcoh(X) and the set of all
subsets $Y\subseteq X$ of the form $Y=\bigcup_{i\in\Omega}Y_i$, with
$X\setminus Y_i$ quasi-compact and open for all $i\in\Omega$, is established.
As an application, th... | math.AG math.KT | given a quasicompact quasiseparated scheme x a bijection between the tensor localizing subcategories of finite type in qcohx and the set of all subsets ysubseteq x of the form ybigcup_iinomegay_i with xsetminus y_i quasicompact and open for all iinomega is established as an application there is constructed an isomorphi... | [['given', 'a', 'quasicompact', 'quasiseparated', 'scheme', 'x', 'a', 'bijection', 'between', 'the', 'tensor', 'localizing', 'subcategories', 'of', 'finite', 'type', 'in', 'qcohx', 'and', 'the', 'set', 'of', 'all', 'subsets', 'ysubseteq', 'x', 'of', 'the', 'form', 'ybigcup_iinomegay_i', 'with', 'xsetminus', 'y_i', 'qua... | [-0.1973480274798451, 0.07187402243553251, -0.021107026836374304, 0.054670481609978845, -0.06659066373901953, -0.12501953396905255, -0.0026962700617182388, 0.4072254140871567, -0.40173577943018507, -0.1027326367099534, 0.07066869535381076, -0.22240929789636488, -0.05599507188250485, 0.1514554081310692, -0.1452463334221... |
708.1623 | Unbalanced Renormalization of Tunneling in MOSFET-type Structures in
Strong High-Frequency Electric Fields | Two-dimensional electron gas coupled to adjacent impurity sites in
high-frequency out-of-plane ac control electric field is investigated.
Modification of tunneling rates as a function of the field amplitude is
calculated. Nonlinear dependence on the ac field strength is reported for the
conductivity of two-dimensiona... | cond-mat.mes-hall quant-ph | twodimensional electron gas coupled to adjacent impurity sites in highfrequency outofplane ac control electric field is investigated modification of tunneling rates as a function of the field amplitude is calculated nonlinear dependence on the ac field strength is reported for the conductivity of twodimensional electro... | [['twodimensional', 'electron', 'gas', 'coupled', 'to', 'adjacent', 'impurity', 'sites', 'in', 'highfrequency', 'outofplane', 'ac', 'control', 'electric', 'field', 'is', 'investigated', 'modification', 'of', 'tunneling', 'rates', 'as', 'a', 'function', 'of', 'the', 'field', 'amplitude', 'is', 'calculated', 'nonlinear',... | [-0.23643963959721775, 0.18073190028595632, 0.020504457016403858, 0.04419687068170438, -0.03455773246689485, -0.15469989214593974, 0.02398122312913004, 0.4088086870033294, -0.2516815754083487, -0.23667319351807237, -0.01305577951671484, -0.2958101890533446, -0.08515704174239475, 0.21521989503302252, 0.08597450298391497... |
708.1624 | Designing a Collaborative Research Environment for Students and their
Supervisors (CRESS) | In a previous paper the CSCR domain was defined. Here this is taken to the
next stage where the design of a particular Collaborative Research Environment
to support Students and Supervisors (CRESS) is considered. Following the CSCR
structure this paper deals with an analysis of 13 collaborative working
environments t... | cs.HC | in a previous paper the cscr domain was defined here this is taken to the next stage where the design of a particular collaborative research environment to support students and supervisors cress is considered following the cscr structure this paper deals with an analysis of 13 collaborative working environments to dete... | [['in', 'a', 'previous', 'paper', 'the', 'cscr', 'domain', 'was', 'defined', 'here', 'this', 'is', 'taken', 'to', 'the', 'next', 'stage', 'where', 'the', 'design', 'of', 'a', 'particular', 'collaborative', 'research', 'environment', 'to', 'support', 'students', 'and', 'supervisors', 'cress', 'is', 'considered', 'follow... | [-0.10049634706228971, 0.027908955574368018, -0.06720047313180091, -0.005682745923126197, -0.13877165277717987, -0.08360521350919768, 0.03409880941288303, 0.38762599472766335, -0.22867325487701842, -0.29922702430706954, 0.14215437169321746, -0.23325497797096445, -0.16317462356950063, 0.1485666783283586, -0.107988047838... |
708.1625 | On n-point Amplitudes in N=4 SYM | The computation of n-point planar amplitudes in N=4 SYM at strong coupling is
known to be reduced to the search for solutions of the integrable 2d SO(4,2)
sigma-model with growing asymptotics on the world-sheet and to the study of
their Whitham deformations induced by an epsilon-regularization, which breaks
both inte... | hep-th | the computation of npoint planar amplitudes in n4 sym at strong coupling is known to be reduced to the search for solutions of the integrable 2d so42 sigmamodel with growing asymptotics on the worldsheet and to the study of their whitham deformations induced by an epsilonregularization which breaks both integrability a... | [['the', 'computation', 'of', 'npoint', 'planar', 'amplitudes', 'in', 'n4', 'sym', 'at', 'strong', 'coupling', 'is', 'known', 'to', 'be', 'reduced', 'to', 'the', 'search', 'for', 'solutions', 'of', 'the', 'integrable', '2d', 'so42', 'sigmamodel', 'with', 'growing', 'asymptotics', 'on', 'the', 'worldsheet', 'and', 'to',... | [-0.1570955556390793, 0.14697809910629644, -0.05176332933323472, 0.10064177227540667, -0.08250006840329703, -0.11990394035553317, -0.02440311056508448, 0.33256908879017294, -0.24578109992141942, -0.2412313903603731, 0.15876737273056488, -0.29084810294843644, -0.1817503463075219, 0.17028620893994117, -0.0632907259240231... |
708.1626 | Thermodynamic Entropy And The Accessible States of Some Simple Systems | Comparison of the thermodynamic entropy with Boltzmann's principle shows that
under conditions of constant volume the total number of arrangements in simple
thermodynamic systems with temperature-independent heat capacities is TC/k. A
physical interpretation of this function is given for three such systems; an
ideal ... | physics.gen-ph | comparison of the thermodynamic entropy with boltzmanns principle shows that under conditions of constant volume the total number of arrangements in simple thermodynamic systems with temperatureindependent heat capacities is tck a physical interpretation of this function is given for three such systems an ideal monatom... | [['comparison', 'of', 'the', 'thermodynamic', 'entropy', 'with', 'boltzmanns', 'principle', 'shows', 'that', 'under', 'conditions', 'of', 'constant', 'volume', 'the', 'total', 'number', 'of', 'arrangements', 'in', 'simple', 'thermodynamic', 'systems', 'with', 'temperatureindependent', 'heat', 'capacities', 'is', 'tck',... | [-0.14200149062949421, 0.18043819234993314, -0.059547437805365894, 0.03135792830551128, 0.027227077482487348, -0.12812119000134806, 0.0560011730317842, 0.2756192544170844, -0.23883582396947114, -0.30715152533615336, 0.039178982617491795, -0.2939650328355093, -0.038339694510700996, 0.1875359754046133, -0.034564343583922... |
708.1627 | Rearranging Edgeworth-Cornish-Fisher Expansions | This paper applies a regularization procedure called increasing rearrangement
to monotonize Edgeworth and Cornish-Fisher expansions and any other related
approximations of distribution and quantile functions of sample statistics.
Besides satisfying the logical monotonicity, required of distribution and
quantile funct... | stat.ME econ.EM | this paper applies a regularization procedure called increasing rearrangement to monotonize edgeworth and cornishfisher expansions and any other related approximations of distribution and quantile functions of sample statistics besides satisfying the logical monotonicity required of distribution and quantile functions ... | [['this', 'paper', 'applies', 'a', 'regularization', 'procedure', 'called', 'increasing', 'rearrangement', 'to', 'monotonize', 'edgeworth', 'and', 'cornishfisher', 'expansions', 'and', 'any', 'other', 'related', 'approximations', 'of', 'distribution', 'and', 'quantile', 'functions', 'of', 'sample', 'statistics', 'besid... | [-0.02575093423947692, 0.030836054915562273, -0.17679091452931364, 0.18158359585601527, -0.06734948468705018, -0.1028865898726508, 0.10883499123350096, 0.3559593815356493, -0.23617715258151292, -0.2928710929428538, 0.06591303366197583, -0.30198644840468963, -0.1116793192923069, 0.16194252548739313, -0.09959045510428648... |
708.1628 | Blocks adjustment -- reduction of bias and variance of detrended
fluctuation analysis using Monte Carlo simulation | The length of minimal and maximal blocks equally distant on log-log scale
versus fluctuation function considerably influences bias and variance of DFA.
Through a number of extensive Monte Carlo simulations and different fractional
Brownian motion/fractional Gaussian noise generators, we found the pair of
minimal and ... | cond-mat.stat-mech | the length of minimal and maximal blocks equally distant on loglog scale versus fluctuation function considerably influences bias and variance of dfa through a number of extensive monte carlo simulations and different fractional brownian motionfractional gaussian noise generators we found the pair of minimal and maxima... | [['the', 'length', 'of', 'minimal', 'and', 'maximal', 'blocks', 'equally', 'distant', 'on', 'loglog', 'scale', 'versus', 'fluctuation', 'function', 'considerably', 'influences', 'bias', 'and', 'variance', 'of', 'dfa', 'through', 'a', 'number', 'of', 'extensive', 'monte', 'carlo', 'simulations', 'and', 'different', 'fra... | [-0.12195913790054219, 0.17071287200776158, -0.058242965870166336, 0.12660078978746808, 0.0012953714761752835, -0.12522389257817418, 0.09126334158097825, 0.35811057665400325, -0.3018352172227316, -0.3059718113552819, 0.07911806362330594, -0.341413739658091, -0.09464073495974423, 0.23697179350601408, -0.0247058546976737... |
708.1629 | Fast spectroscopy and imaging with the FORS2 HIT mode | The HIgh-Time resolution (HIT) mode of FORS2 has 3 sub-modes that allow for
imaging and spectroscopy over a range of timescales from milliseconds up to
seconds. It is the only high time resolution spectroscopy mode available on an
8m class telescope. In imaging mode, it can be used to measure the pulse of
pulsars and... | astro-ph | the hightime resolution hit mode of fors2 has 3 submodes that allow for imaging and spectroscopy over a range of timescales from milliseconds up to seconds it is the only high time resolution spectroscopy mode available on an 8m class telescope in imaging mode it can be used to measure the pulse of pulsars and spinning... | [['the', 'hightime', 'resolution', 'hit', 'mode', 'of', 'fors2', 'has', '3', 'submodes', 'that', 'allow', 'for', 'imaging', 'and', 'spectroscopy', 'over', 'a', 'range', 'of', 'timescales', 'from', 'milliseconds', 'up', 'to', 'seconds', 'it', 'is', 'the', 'only', 'high', 'time', 'resolution', 'spectroscopy', 'mode', 'av... | [-0.09836497041947409, 0.1107235077110385, -0.09861396740794785, -0.00527010448009556, -0.09820717691469032, -0.16181208370442227, 0.0741637326144563, 0.44538072424129005, -0.2196756701513722, -0.36352384368561813, 0.13677460943723121, -0.2715057123616036, -0.008835581570196696, 0.26538338429590286, -0.0427518952449129... |
708.163 | Time-Dependent Analysis of the Decay B0 --> rho0 rho0 | We study the decay B0 --> rho0 rho0 in a sample of about 427 million
Upsilon(4S) --> BBbar decays collected with the BABAR detector at the PEP-II
asymmetric-energy e+e- collider at SLAC. We find the branching fraction
B = (0.84 +/- 0.29 +/- 0.17)*1e-6 and longitudinal polarization fraction of
f_L = 0.70 +/- 0.14 +/... | hep-ex | we study the decay b0 rho0 rho0 in a sample of about 427 million upsilon4s bbbar decays collected with the babar detector at the pepii asymmetricenergy ee collider at slac we find the branching fraction b 084 029 0171e6 and longitudinal polarization fraction of f_l 070 014 005 where the first uncertainty is statistical... | [['we', 'study', 'the', 'decay', 'b0', 'rho0', 'rho0', 'in', 'a', 'sample', 'of', 'about', '427', 'million', 'upsilon4s', 'bbbar', 'decays', 'collected', 'with', 'the', 'babar', 'detector', 'at', 'the', 'pepii', 'asymmetricenergy', 'ee', 'collider', 'at', 'slac', 'we', 'find', 'the', 'branching', 'fraction', 'b', '084'... | [-0.10194841448746463, 0.20555129324992064, -0.07087864796811527, 0.0735580516318509, -0.028687855308196803, -0.10035768807179822, 0.09926035721757442, 0.29657723540223613, -0.20407721250094185, -0.26038668942890425, -0.020109950059432852, -0.47295220061963383, 0.05393330234124563, 0.11960699770404676, 0.09799912562882... |
708.1631 | Leading Order Calculation of Shear Viscosity in Hot Quantum
Electrodynamics from Diagrammatic Methods | We compute the shear viscosity at leading order in hot Quantum
Electrodynamics. Starting from the Kubo relation for shear viscosity, we use
diagrammatic methods to write down the appropriate integral equations for
bosonic and fermionic effective vertices. We also show how Ward identities can
be used to put constraint... | hep-ph nucl-th | we compute the shear viscosity at leading order in hot quantum electrodynamics starting from the kubo relation for shear viscosity we use diagrammatic methods to write down the appropriate integral equations for bosonic and fermionic effective vertices we also show how ward identities can be used to put constraints on ... | [['we', 'compute', 'the', 'shear', 'viscosity', 'at', 'leading', 'order', 'in', 'hot', 'quantum', 'electrodynamics', 'starting', 'from', 'the', 'kubo', 'relation', 'for', 'shear', 'viscosity', 'we', 'use', 'diagrammatic', 'methods', 'to', 'write', 'down', 'the', 'appropriate', 'integral', 'equations', 'for', 'bosonic',... | [-0.10759457432295523, 0.12441770838485451, -0.1446938348190037, 0.11385216773032372, -0.11992511614459936, -0.10065558897890671, 0.01487498969982987, 0.29723239294318327, -0.2727687481853216, -0.2708565836093342, 0.05452713802880894, -0.32541437464761, -0.1500952119116968, 0.15973105571914317, 0.015957237485348764, 0.... |
708.1632 | Mechanical properties of the two-filament insulin amyloid fibril: a
theoretical study | We study the two-filament insulin fibril's structure by incorporating recent
simulation results and mechanical measurements. Our investigation suggests that
the persistence length measurement correlates well with the previously proposed
structural model, while the elasticity measurement suggests that stretching the
f... | cond-mat.soft cond-mat.mtrl-sci | we study the twofilament insulin fibrils structure by incorporating recent simulation results and mechanical measurements our investigation suggests that the persistence length measurement correlates well with the previously proposed structural model while the elasticity measurement suggests that stretching the fibril ... | [['we', 'study', 'the', 'twofilament', 'insulin', 'fibrils', 'structure', 'by', 'incorporating', 'recent', 'simulation', 'results', 'and', 'mechanical', 'measurements', 'our', 'investigation', 'suggests', 'that', 'the', 'persistence', 'length', 'measurement', 'correlates', 'well', 'with', 'the', 'previously', 'proposed... | [-0.10128683518738515, 0.12667823390074773, -0.048590557255421676, 0.0010442742627234229, -0.06436621576112005, -0.12419676716108957, 0.03652262397771401, 0.4094576222761985, -0.2763225064207349, -0.29644991614622995, 0.03898674034468469, -0.3041971947757467, -0.24601320862289397, 0.13235595833975822, 0.001505547413422... |
708.1633 | Charmed spectroscopy from a nonperturbatively determined relativistic
heavy quark action in full QCD | We present a preliminary calculation of the charmed meson spectrum using the
2+1 flavor domain wall fermion lattice configurations currently being generated
by the RBC and UKQCD collaborations. The calculation is performed using the
3-parameter, relativistic heavy quark action with nonperturbatively determined
coeffi... | hep-lat | we present a preliminary calculation of the charmed meson spectrum using the 21 flavor domain wall fermion lattice configurations currently being generated by the rbc and ukqcd collaborations the calculation is performed using the 3parameter relativistic heavy quark action with nonperturbatively determined coefficients... | [['we', 'present', 'a', 'preliminary', 'calculation', 'of', 'the', 'charmed', 'meson', 'spectrum', 'using', 'the', '21', 'flavor', 'domain', 'wall', 'fermion', 'lattice', 'configurations', 'currently', 'being', 'generated', 'by', 'the', 'rbc', 'and', 'ukqcd', 'collaborations', 'the', 'calculation', 'is', 'performed', '... | [-0.12075368117919003, 0.3145405439578969, -0.10024936272816705, 0.06385003558893189, -0.023579357704822567, -0.07778182630494669, 0.07907123878206787, 0.4200396322091852, -0.1424063636880854, -0.21966970829374116, 0.05732398799897266, -0.26720138860569487, -0.040570048952772136, 0.11488628920599603, 0.1126557674285942... |
708.1634 | Kontsevich formality and PBW algebras | This paper is based on the author's paper "Koszul duality in deformation
quantization, I", with some improvements. In particular, an Introduction is
added, and the convergence of the spectral sequence in Lemma 2.1 is rigorously
proven. Some informal discussion in Section 1.5 is added.
| math.KT math.RA | this paper is based on the authors paper koszul duality in deformation quantization i with some improvements in particular an introduction is added and the convergence of the spectral sequence in lemma 21 is rigorously proven some informal discussion in section 15 is added | [['this', 'paper', 'is', 'based', 'on', 'the', 'authors', 'paper', 'koszul', 'duality', 'in', 'deformation', 'quantization', 'i', 'with', 'some', 'improvements', 'in', 'particular', 'an', 'introduction', 'is', 'added', 'and', 'the', 'convergence', 'of', 'the', 'spectral', 'sequence', 'in', 'lemma', '21', 'is', 'rigorou... | [-0.10832005162956193, 0.029822957567375852, -0.11066632964436642, 0.07109287389374169, -0.0889480093663389, -0.11579042535529217, -0.014306376891909167, 0.3668598690154878, -0.25019831248474395, -0.24946299195289612, 0.16009839460655878, -0.2607314920698462, -0.21044446527957916, 0.12118954440070824, -0.23386110403490... |
708.1635 | Gravitational brainwaves, quantum fluctuations and stochastic
quantization | It is known that the biological activity of the brain involves radiation of
electric waves. These waves result from ionic currents and charges traveling
among the brain's neurons. But it is obvious that these ions and charges are
carried by their relevant masses which should give rise, according to the
gravitational ... | gr-qc | it is known that the biological activity of the brain involves radiation of electric waves these waves result from ionic currents and charges traveling among the brains neurons but it is obvious that these ions and charges are carried by their relevant masses which should give rise according to the gravitational theory... | [['it', 'is', 'known', 'that', 'the', 'biological', 'activity', 'of', 'the', 'brain', 'involves', 'radiation', 'of', 'electric', 'waves', 'these', 'waves', 'result', 'from', 'ionic', 'currents', 'and', 'charges', 'traveling', 'among', 'the', 'brains', 'neurons', 'but', 'it', 'is', 'obvious', 'that', 'these', 'ions', 'a... | [-0.11734076766438331, 0.1891087724008795, -0.05403257221585572, 0.12974272575229406, -0.09215071914962145, -0.07931863476588118, 0.036575643575016525, 0.3332215810401572, -0.25194960321544324, -0.28246103810391043, 0.01795616451853115, -0.2824444299695468, -0.20487868712481225, 0.1620991949645821, -0.00913570015079746... |
708.1636 | HI and OH absorption in the lensing galaxy of MG J0414+0534 | We report the detection of \HI 21-cm absorption in the $z=0.96$ early-type
lensing galaxy towards MG J0414+0534 with the Green Bank Telescope. The
absorption, with total $N_{\rm HI}=1.6 \times 10^{18} (T_{\rm s}/f) {\rm
cm}^{-2}$, is resolved into two strong components, probably due to the two
strongest lens componen... | astro-ph | we report the detection of hi 21cm absorption in the z096 earlytype lensing galaxy towards mg j04140534 with the green bank telescope the absorption with total n_rm hi16 times 1018 t_rm sf rm cm2 is resolved into two strong components probably due to the two strongest lens components which are separated by 04arcsec unl... | [['we', 'report', 'the', 'detection', 'of', 'hi', '21cm', 'absorption', 'in', 'the', 'z096', 'earlytype', 'lensing', 'galaxy', 'towards', 'mg', 'j04140534', 'with', 'the', 'green', 'bank', 'telescope', 'the', 'absorption', 'with', 'total', 'n_rm', 'hi16', 'times', '1018', 't_rm', 'sf', 'rm', 'cm2', 'is', 'resolved', 'i... | [-0.10253647684863687, 0.09331374106577774, 0.015919341425667855, 0.022299023362828175, -0.05216490411692285, -0.10423158247199288, 0.023041868138218135, 0.47462203257136804, -0.10059161918183816, -0.32437483908311615, 0.03280991192761998, -0.3140580404981755, -0.004539160742896838, 0.14744188366466257, 0.0343299146423... |
708.1637 | Self-organization of heterogeneous topology and symmetry breaking in
networks with adaptive thresholds and rewiring | We study an evolutionary algorithm that locally adapts thresholds and wiring
in Random Threshold Networks, based on measurements of a dynamical order
parameter. A control parameter $p$ determines the probability of threshold
adaptations vs. link rewiring. For any $p < 1$, we find spontaneous symmetry
breaking into a ... | cond-mat.dis-nn cond-mat.stat-mech nlin.AO q-bio.MN | we study an evolutionary algorithm that locally adapts thresholds and wiring in random threshold networks based on measurements of a dynamical order parameter a control parameter p determines the probability of threshold adaptations vs link rewiring for any p 1 we find spontaneous symmetry breaking into a new class of ... | [['we', 'study', 'an', 'evolutionary', 'algorithm', 'that', 'locally', 'adapts', 'thresholds', 'and', 'wiring', 'in', 'random', 'threshold', 'networks', 'based', 'on', 'measurements', 'of', 'a', 'dynamical', 'order', 'parameter', 'a', 'control', 'parameter', 'p', 'determines', 'the', 'probability', 'of', 'threshold', '... | [-0.15718521670911645, 0.1756866718385966, -0.08027377678844773, 0.09987065455586207, -0.014606679566433562, -0.23192216298203214, 0.1205676059278213, 0.38257527421610277, -0.23825430150189605, -0.3127065096890218, 0.017906515719750743, -0.2519687707726767, -0.1858092223343699, 0.09546248169356315, -0.00884751672665665... |
708.1638 | Electrically controlled Bragg resonances of an ambichiral electro-optic
structure: oblique incidence | The Pockels effect can increase the effective birefringence of ambichiral,
electro--optic rejection filters made of materials with a $\bar{4}2m$ point
group symmetry, when a dc electric field is applied parallel to the axis of
nonhomogeneity. The reflectances and the transmittances of such an ambichiral
structure for... | physics.optics | the pockels effect can increase the effective birefringence of ambichiral electrooptic rejection filters made of materials with a bar42m point group symmetry when a dc electric field is applied parallel to the axis of nonhomogeneity the reflectances and the transmittances of such an ambichiral structure for obliquely i... | [['the', 'pockels', 'effect', 'can', 'increase', 'the', 'effective', 'birefringence', 'of', 'ambichiral', 'electrooptic', 'rejection', 'filters', 'made', 'of', 'materials', 'with', 'a', 'bar42m', 'point', 'group', 'symmetry', 'when', 'a', 'dc', 'electric', 'field', 'is', 'applied', 'parallel', 'to', 'the', 'axis', 'of'... | [-0.19255336315089136, 0.1543299080303351, -0.04949569925153201, -0.01604373072201403, -0.1499284056651859, -0.12142133278507364, -0.03712231080088371, 0.39285145809344196, -0.2871370504037776, -0.29572065360844135, 0.08288979690111832, -0.28562025681411457, -0.15489905133604184, 0.20084126182584042, 0.0116384980683172... |
708.1639 | Many-body generalization of the Z2 topological invariant for the quantum
spin Hall effect | We propose a many-body generalization of the Z2 topological invariant for the
quantum spin Hall insulator, which does not rely on single-particle band
structures. The invariant is derived as a topological obstruction that
distinguishes topologically distinct many-body ground states on a torus. It is
also expressed as... | cond-mat.mes-hall | we propose a manybody generalization of the z2 topological invariant for the quantum spin hall insulator which does not rely on singleparticle band structures the invariant is derived as a topological obstruction that distinguishes topologically distinct manybody ground states on a torus it is also expressed as a wilso... | [['we', 'propose', 'a', 'manybody', 'generalization', 'of', 'the', 'z2', 'topological', 'invariant', 'for', 'the', 'quantum', 'spin', 'hall', 'insulator', 'which', 'does', 'not', 'rely', 'on', 'singleparticle', 'band', 'structures', 'the', 'invariant', 'is', 'derived', 'as', 'a', 'topological', 'obstruction', 'that', '... | [-0.2440054596416534, 0.2522062183402124, -0.13297282806819394, 0.1121588822080946, -0.1043747966251676, -0.17612646478745672, 0.010181002536906845, 0.31331282995256876, -0.21414934627209153, -0.22630577802007634, 0.028111074762862353, -0.24826012747657913, -0.2285729885870029, 0.12174852272229535, -0.03888281163138648... |
708.164 | Suppression of electronic susceptibility in metal-Mott insulator
alternating material, (Me-3,5-DIP)[Ni(dmit)2]2 | Frequency shifts and nuclear relaxations of 13C NMR of the metal-insulator
alternating material, (Me-3,5-DIP)[Ni(dmit)2]2, are presented. The NMR
absorption lines originating from metallic and insulating layers are well
resolved, which evidences the coexistence of localized spins (\pi_loc) and
conduction \pi-electron... | cond-mat.str-el | frequency shifts and nuclear relaxations of 13c nmr of the metalinsulator alternating material me35dipnidmit22 are presented the nmr absorption lines originating from metallic and insulating layers are well resolved which evidences the coexistence of localized spins pi_loc and conduction pielectrons the insulating laye... | [['frequency', 'shifts', 'and', 'nuclear', 'relaxations', 'of', '13c', 'nmr', 'of', 'the', 'metalinsulator', 'alternating', 'material', 'me35dipnidmit22', 'are', 'presented', 'the', 'nmr', 'absorption', 'lines', 'originating', 'from', 'metallic', 'and', 'insulating', 'layers', 'are', 'well', 'resolved', 'which', 'evide... | [-0.17710925752388512, 0.25401458169666774, 0.01749971679860859, 0.008298040680529084, 0.0019731727017122985, -0.170621505071592, 0.11538029952706504, 0.4052569431452347, -0.2858365946989839, -0.3018972610318867, 0.00547523632537507, -0.3827175585070758, -0.09631023003437024, 0.07444442760658733, 0.12822793424129486, -... |
708.1641 | Approximating the monomer-dimer constants through matrix permanent | The monomer-dimer model is fundamental in statistical mechanics. However, it
is $#P$-complete in computation, even for two dimensional problems. A
formulation in matrix permanent for the partition function of the monomer-dimer
model is proposed in this paper, by transforming the number of all matchings of
a bipartite... | cond-mat.stat-mech | the monomerdimer model is fundamental in statistical mechanics however it is pcomplete in computation even for two dimensional problems a formulation in matrix permanent for the partition function of the monomerdimer model is proposed in this paper by transforming the number of all matchings of a bipartite graph into t... | [['the', 'monomerdimer', 'model', 'is', 'fundamental', 'in', 'statistical', 'mechanics', 'however', 'it', 'is', 'pcomplete', 'in', 'computation', 'even', 'for', 'two', 'dimensional', 'problems', 'a', 'formulation', 'in', 'matrix', 'permanent', 'for', 'the', 'partition', 'function', 'of', 'the', 'monomerdimer', 'model',... | [-0.12115281442688271, 0.12350934640496482, -0.027300689979033038, 0.031960718961305576, -0.050115073142065245, -0.15041295811957256, 0.01771685856669633, 0.3530157243494283, -0.25643968898802993, -0.31344326320739296, 0.10843435190618038, -0.23511155257848176, -0.17690122511280193, 0.15949033042839306, -0.043018286128... |
708.1642 | Total Reflection and Negative Refraction of Dipole-Exchange Spin Waves
at Magnetic Interfaces: Micromagnetic Modeling Study | We demonstrated that dipole-exchange spin waves traveling in geometrically
restricted magnetic thin films satisfy the same laws of reflection and
refraction as light waves. Moreover, we found for the first time novel wave
behaviors of dipole-exchange spin waves such as total reflection and negative
refraction. The to... | cond-mat.other | we demonstrated that dipoleexchange spin waves traveling in geometrically restricted magnetic thin films satisfy the same laws of reflection and refraction as light waves moreover we found for the first time novel wave behaviors of dipoleexchange spin waves such as total reflection and negative refraction the total ref... | [['we', 'demonstrated', 'that', 'dipoleexchange', 'spin', 'waves', 'traveling', 'in', 'geometrically', 'restricted', 'magnetic', 'thin', 'films', 'satisfy', 'the', 'same', 'laws', 'of', 'reflection', 'and', 'refraction', 'as', 'light', 'waves', 'moreover', 'we', 'found', 'for', 'the', 'first', 'time', 'novel', 'wave', ... | [-0.24119387936312706, 0.3132339636981487, -0.0011175421113148332, 0.007784532059449702, -0.13956172421574592, -0.09992626843042672, -0.03033978872001171, 0.4202942081168294, -0.27425396274775266, -0.2766365598794073, 0.021381503661395983, -0.2979664720594883, -0.1398895194195211, 0.1985506362770684, 0.1041517779650166... |
708.1643 | Local Lorentz Transformation and "Lorentz Violation" | Some solutions to the anomalies of ultra high energy cosmic-ray(UHECR) and
TeV $\gamma$-rays require disturbed non-quadratic dispersion relations, which
suggest the Lorentz violation. Also, some new theories such as quantum gravity,
string theory and the standard model extension imply the Lorentz violation. In
this p... | physics.gen-ph | some solutions to the anomalies of ultra high energy cosmicrayuhecr and tev gammarays require disturbed nonquadratic dispersion relations which suggest the lorentz violation also some new theories such as quantum gravity string theory and the standard model extension imply the lorentz violation in this paper we derive ... | [['some', 'solutions', 'to', 'the', 'anomalies', 'of', 'ultra', 'high', 'energy', 'cosmicrayuhecr', 'and', 'tev', 'gammarays', 'require', 'disturbed', 'nonquadratic', 'dispersion', 'relations', 'which', 'suggest', 'the', 'lorentz', 'violation', 'also', 'some', 'new', 'theories', 'such', 'as', 'quantum', 'gravity', 'str... | [-0.12156686144480382, 0.1681905892947989, -0.11572719146547619, 0.16605180615098566, -0.14518131491958455, -0.16059254936032719, 0.025216138666315425, 0.28043616927599396, -0.2768983976710187, -0.33961459764990437, 0.055241134553466756, -0.2437817660180391, -0.18227725602205722, 0.18916472536261364, -0.011769264418211... |
708.1644 | Ricci curvature and geodesic flows stability in Riemannian twisted flux
tubes | Ricci and sectional curvatures of twisted flux tubes in Riemannian manifold
are computed to investigate the stability of the tubes. The geodesic equations
are used to show that in the case of thick tubes, the curvature of planar
(Frenet torsion-free) tubes have the effect ct of damping the flow speed along
the tube. ... | physics.flu-dyn | ricci and sectional curvatures of twisted flux tubes in riemannian manifold are computed to investigate the stability of the tubes the geodesic equations are used to show that in the case of thick tubes the curvature of planar frenet torsionfree tubes have the effect ct of damping the flow speed along the tube stabilit... | [['ricci', 'and', 'sectional', 'curvatures', 'of', 'twisted', 'flux', 'tubes', 'in', 'riemannian', 'manifold', 'are', 'computed', 'to', 'investigate', 'the', 'stability', 'of', 'the', 'tubes', 'the', 'geodesic', 'equations', 'are', 'used', 'to', 'show', 'that', 'in', 'the', 'case', 'of', 'thick', 'tubes', 'the', 'curva... | [-0.24415441677256516, 0.15810852741053555, -0.04272427455042348, 0.07374343270908645, -0.078906028192829, -0.11720424489061715, -0.13156731628149634, 0.40317574476428103, -0.23760294664966888, -0.20616327093519043, 0.1421647261696776, -0.2764152041265995, -0.08382561160815936, 0.19723296679810368, -0.07612208746881648... |
708.1645 | Cell dynamics simulation of droplet and bridge formation within striped
nano-capillaries | The kinetics of droplet and bridge formation within striped nano-capillaries
is studied when the wetting film grows via interface-limited growth. The
phenomenological time-dependent Ginzburg-Landau (TDGL)-type model with thermal
noise is used and numerically solved using the cell dynamics method. The model
is two-dim... | cond-mat.soft | the kinetics of droplet and bridge formation within striped nanocapillaries is studied when the wetting film grows via interfacelimited growth the phenomenological timedependent ginzburglandau tdgltype model with thermal noise is used and numerically solved using the cell dynamics method the model is twodimensional and... | [['the', 'kinetics', 'of', 'droplet', 'and', 'bridge', 'formation', 'within', 'striped', 'nanocapillaries', 'is', 'studied', 'when', 'the', 'wetting', 'film', 'grows', 'via', 'interfacelimited', 'growth', 'the', 'phenomenological', 'timedependent', 'ginzburglandau', 'tdgltype', 'model', 'with', 'thermal', 'noise', 'is'... | [-0.10881011840713778, 0.19643701537589395, -0.10513214857907162, 0.01185803670303885, -0.003896129555923082, -0.13617965768052806, 0.010575964453095603, 0.3578610556370981, -0.2672097080513923, -0.27687181132506666, 0.03781808304707878, -0.24739450747532957, -0.15658943443118248, 0.15696670705061297, 0.017630939677732... |
708.1646 | Self Excitation of Nano-Mechanical Pillars | Self excitation is a mechanism which is ubiquitous for electromechanical
power devices such as electrical generators. This is conventionally achieved by
making use of the magnetic field component in electrical generators [1], where
a good example are the overall visible wind farm turbines [2]. In other words,
a stati... | cond-mat.mes-hall | self excitation is a mechanism which is ubiquitous for electromechanical power devices such as electrical generators this is conventionally achieved by making use of the magnetic field component in electrical generators 1 where a good example are the overall visible wind farm turbines 2 in other words a static force li... | [['self', 'excitation', 'is', 'a', 'mechanism', 'which', 'is', 'ubiquitous', 'for', 'electromechanical', 'power', 'devices', 'such', 'as', 'electrical', 'generators', 'this', 'is', 'conventionally', 'achieved', 'by', 'making', 'use', 'of', 'the', 'magnetic', 'field', 'component', 'in', 'electrical', 'generators', '1', ... | [-0.1597595687073786, 0.18637260794864544, -0.020043397290803098, 0.004313359886254881, -0.06860617771609753, -0.18346744293913894, 0.042469181993229375, 0.40040519138897096, -0.2667854067819994, -0.33501692618139917, 0.05491672821707376, -0.26872961280264573, -0.1445213204164256, 0.2808486341056189, -0.036445675318799... |
708.1647 | Molecular Hydrogen Formation on Low Temperature Surfaces in Temperature
Programmed Desorption Experiments | The study of the formation of molecular hydrogen on low temperature surfaces
is of interest both because it allows to explore elementary steps in the
heterogeneous catalysis of a simple molecule and because of the applications in
astrochemistry. Here we report results of experiments of molecular hydrogen
formation on... | physics.chem-ph astro-ph | the study of the formation of molecular hydrogen on low temperature surfaces is of interest both because it allows to explore elementary steps in the heterogeneous catalysis of a simple molecule and because of the applications in astrochemistry here we report results of experiments of molecular hydrogen formation on am... | [['the', 'study', 'of', 'the', 'formation', 'of', 'molecular', 'hydrogen', 'on', 'low', 'temperature', 'surfaces', 'is', 'of', 'interest', 'both', 'because', 'it', 'allows', 'to', 'explore', 'elementary', 'steps', 'in', 'the', 'heterogeneous', 'catalysis', 'of', 'a', 'simple', 'molecule', 'and', 'because', 'of', 'the',... | [-0.043175360297290494, 0.14674086282276955, -0.05789475370737084, -0.0035254657072160975, 0.046789946002291, -0.0765776748527739, 0.07508902623127382, 0.43246059273425713, -0.21591133012223135, -0.27992994152009487, 0.05031059609153813, -0.2584291817186469, -0.0705118953157076, 0.1983496728409306, 0.026312031401657915... |
708.1648 | The direct oxygen abundances of metal-rich galaxies derived from
electron temperature | We aim to derive the electron temperature Te in the gas of metal-rich
star-forming galaxies, which can be obtained from their ratios of auroral lines
[O II]7320,7330 to nebular lines [O II]3727, in order to establish a more
robust mass-metallicity relationship, and compare the Te-based (O/H) abundances
with those fro... | astro-ph | we aim to derive the electron temperature te in the gas of metalrich starforming galaxies which can be obtained from their ratios of auroral lines o ii73207330 to nebular lines o ii3727 in order to establish a more robust massmetallicity relationship and compare the tebased oh abundances with those from empirical stron... | [['we', 'aim', 'to', 'derive', 'the', 'electron', 'temperature', 'te', 'in', 'the', 'gas', 'of', 'metalrich', 'starforming', 'galaxies', 'which', 'can', 'be', 'obtained', 'from', 'their', 'ratios', 'of', 'auroral', 'lines', 'o', 'ii73207330', 'to', 'nebular', 'lines', 'o', 'ii3727', 'in', 'order', 'to', 'establish', 'a... | [0.010939549170208243, 0.06410228642107173, -0.024448933247627636, 0.08813550164885367, 0.008648892301360997, -0.09476720096792286, 0.12324287734081146, 0.41246838330739904, -0.1478708857295258, -0.37227165438838095, 0.00087939389191402, -0.31883862074690794, -0.018772849733451086, 0.20054596322230422, -0.0382293367964... |
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