id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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710.3653 | Slow-light enhanced optical detection in liquid-infiltrated photonic
crystals | Slow-light enhanced optical detection in liquid-infiltrated photonic crystals
is theoretically studied. Using a scattering-matrix approach and the
Wigner-Smith delay time concept, we show that optical absorbance benefits both
from slow-light phenomena as well as a high filling factor of the energy
residing in the liq... | physics.optics | slowlight enhanced optical detection in liquidinfiltrated photonic crystals is theoretically studied using a scatteringmatrix approach and the wignersmith delay time concept we show that optical absorbance benefits both from slowlight phenomena as well as a high filling factor of the energy residing in the liquid utili... | [['slowlight', 'enhanced', 'optical', 'detection', 'in', 'liquidinfiltrated', 'photonic', 'crystals', 'is', 'theoretically', 'studied', 'using', 'a', 'scatteringmatrix', 'approach', 'and', 'the', 'wignersmith', 'delay', 'time', 'concept', 'we', 'show', 'that', 'optical', 'absorbance', 'benefits', 'both', 'from', 'slowl... | [-0.1453721186844632, 0.16071315384512921, -0.016774273992764807, -0.03493524077004457, -0.033016400538723574, -0.1581103052594699, 0.06416273334947288, 0.483201178542169, -0.26917171862442046, -0.29222510304217314, 0.018970614099420014, -0.2786320158788426, -0.22175239487974482, 0.2684450270184739, 0.01174885365815663... |
710.3654 | Aggregation for Gaussian regression | This paper studies statistical aggregation procedures in the regression
setting. A motivating factor is the existence of many different methods of
estimation, leading to possibly competing estimators. We consider here three
different types of aggregation: model selection (MS) aggregation, convex (C)
aggregation and l... | math.ST stat.TH | this paper studies statistical aggregation procedures in the regression setting a motivating factor is the existence of many different methods of estimation leading to possibly competing estimators we consider here three different types of aggregation model selection ms aggregation convex c aggregation and linear l agg... | [['this', 'paper', 'studies', 'statistical', 'aggregation', 'procedures', 'in', 'the', 'regression', 'setting', 'a', 'motivating', 'factor', 'is', 'the', 'existence', 'of', 'many', 'different', 'methods', 'of', 'estimation', 'leading', 'to', 'possibly', 'competing', 'estimators', 'we', 'consider', 'here', 'three', 'dif... | [-0.06716845011110256, 0.038003333334140854, -0.07705703858847093, 0.07915926113604248, -0.05509554408490658, -0.20025345041779766, 0.07829364989911167, 0.3797518459173876, -0.26472879742887084, -0.2912149523136756, 0.14702883153312396, -0.26886823316712405, -0.13146723336522184, 0.1734971503657918, -0.1233788566343831... |
710.3655 | Coxeter Groups and Wavelet Sets | A traditional wavelet is a special case of a vector in a separable Hilbert
space that generates a basis under the action of a system of unitary operators
defined in terms of translation and dilation operations. A
Coxeter/fractal-surface wavelet is obtained by defining fractal surfaces on
foldable figures, which tesse... | math.FA | a traditional wavelet is a special case of a vector in a separable hilbert space that generates a basis under the action of a system of unitary operators defined in terms of translation and dilation operations a coxeterfractalsurface wavelet is obtained by defining fractal surfaces on foldable figures which tesselate t... | [['a', 'traditional', 'wavelet', 'is', 'a', 'special', 'case', 'of', 'a', 'vector', 'in', 'a', 'separable', 'hilbert', 'space', 'that', 'generates', 'a', 'basis', 'under', 'the', 'action', 'of', 'a', 'system', 'of', 'unitary', 'operators', 'defined', 'in', 'terms', 'of', 'translation', 'and', 'dilation', 'operations', ... | [-0.14820979561191053, 0.1688471347525982, -0.11754685795333769, 0.08132597751682624, -0.024059303785075568, -0.10451712074822612, 0.009942271088116935, 0.39450494671639585, -0.30298515867242326, -0.17035133823353266, 0.12478151426683845, -0.2668110288230569, -0.20270416748909545, 0.21408606921322643, -0.08789374477429... |
710.3656 | Hyperelliptic Jacobians as Billiard Algebra of Pencils of Quadrics:
Beyond Poncelet Porisms | The thirty years old programme of Griffiths and Harris of understanding
higher-dimensional analogues of Poncelet-type problems and synthetic approach
to higher genera addition theorems has been settled and completed in this
paper. Starting with the observation of the billiard nature of some classical
constructions an... | math.AG math-ph math.MP | the thirty years old programme of griffiths and harris of understanding higherdimensional analogues of poncelettype problems and synthetic approach to higher genera addition theorems has been settled and completed in this paper starting with the observation of the billiard nature of some classical constructions and con... | [['the', 'thirty', 'years', 'old', 'programme', 'of', 'griffiths', 'and', 'harris', 'of', 'understanding', 'higherdimensional', 'analogues', 'of', 'poncelettype', 'problems', 'and', 'synthetic', 'approach', 'to', 'higher', 'genera', 'addition', 'theorems', 'has', 'been', 'settled', 'and', 'completed', 'in', 'this', 'pa... | [-0.12343402371383429, 0.060310693558441535, -0.10180903044450777, 0.04992670418885589, -0.04971558383006728, -0.155588076426386, 0.012786976112774835, 0.30869566570716295, -0.28681418947480475, -0.2538322620460073, 0.10455043039813093, -0.28870302113884894, -0.1698130434849875, 0.23863273336463137, -0.1181267553657879... |
710.3657 | A double supermirror monochromator for neutron instrumentation at LLB | The design and characteristics of a double supermirror monochromator for
neutron instrumentation at the Laboratoire Leon Brillouin is described. The aim
of this monochromator is to reduce the intense gamma-radiation produced by
conventional velocity selectors and to avoid a direct view of the guide while
keeping a co... | physics.ins-det | the design and characteristics of a double supermirror monochromator for neutron instrumentation at the laboratoire leon brillouin is described the aim of this monochromator is to reduce the intense gammaradiation produced by conventional velocity selectors and to avoid a direct view of the guide while keeping a compar... | [['the', 'design', 'and', 'characteristics', 'of', 'a', 'double', 'supermirror', 'monochromator', 'for', 'neutron', 'instrumentation', 'at', 'the', 'laboratoire', 'leon', 'brillouin', 'is', 'described', 'the', 'aim', 'of', 'this', 'monochromator', 'is', 'to', 'reduce', 'the', 'intense', 'gammaradiation', 'produced', 'b... | [-0.07938332707229731, 0.13769045774487482, -0.06390545984217222, 0.016988215841474415, -0.11067556535852129, -0.14263001257769656, 0.0803096055633564, 0.38809813629241957, -0.20379336043328478, -0.3272954848041569, 0.06353644633065045, -0.29331256242711906, 0.02333316556515469, 0.2324348861027671, -0.0654634521815224,... |
710.3658 | Sensitivity of Nonrenormalizable Trajectories to the Bare Scale | Working in scalar field theory, we consider RG trajectories which correspond
to nonrenormalizable theories, in the Wilsonian sense. An interesting question
to ask of such trajectories is, given some fixed starting point in parameter
space, how the effective action at the effective scale, Lambda, changes as the
bare s... | hep-th hep-ph | working in scalar field theory we consider rg trajectories which correspond to nonrenormalizable theories in the wilsonian sense an interesting question to ask of such trajectories is given some fixed starting point in parameter space how the effective action at the effective scale lambda changes as the bare scale and ... | [['working', 'in', 'scalar', 'field', 'theory', 'we', 'consider', 'rg', 'trajectories', 'which', 'correspond', 'to', 'nonrenormalizable', 'theories', 'in', 'the', 'wilsonian', 'sense', 'an', 'interesting', 'question', 'to', 'ask', 'of', 'such', 'trajectories', 'is', 'given', 'some', 'fixed', 'starting', 'point', 'in', ... | [-0.13183371142764572, 0.1610049421835166, -0.13544051307230373, 0.08551338324045289, -0.10601505561412047, -0.13222331777724683, -0.001609475530836898, 0.31476866754828325, -0.28143061413916187, -0.2777218568643824, 0.0770113546637568, -0.2728353633037977, -0.14534265953648964, 0.13838294018245306, -0.0310392070733084... |
710.3659 | Luminosity Dependence of the Quasar Clustering from SDSS DR5 | 43024 objects, which were primarily identified as quasars in SDSS DR5 and
have spectroscopic redshifts were used to study the luminosity dependence of
the quasar clustering with the help of two different techniques. The obtained
results reveal that brighter quasars are more clustered, but this dependence is
weak, whi... | astro-ph | 43024 objects which were primarily identified as quasars in sdss dr5 and have spectroscopic redshifts were used to study the luminosity dependence of the quasar clustering with the help of two different techniques the obtained results reveal that brighter quasars are more clustered but this dependence is weak which is ... | [['43024', 'objects', 'which', 'were', 'primarily', 'identified', 'as', 'quasars', 'in', 'sdss', 'dr5', 'and', 'have', 'spectroscopic', 'redshifts', 'were', 'used', 'to', 'study', 'the', 'luminosity', 'dependence', 'of', 'the', 'quasar', 'clustering', 'with', 'the', 'help', 'of', 'two', 'different', 'techniques', 'the'... | [0.01584192699920095, 0.07435211735719349, -0.09052969519689213, 0.08233746794030594, -0.13599029924080241, -0.08418893697671592, 0.007248664845064923, 0.4431679456611164, -0.08310469554635347, -0.4079331225948408, 0.05592177508879104, -0.3495247809769353, -0.08162103049835423, 0.23475938674528152, -0.03709649009397253... |
710.366 | Electric quadrupole moment of the $5d^2 D_{3/2}$ state in $^{171}Yb^+$ :
A relativistic coupled-cluster analysis | The electric quadrupole moment for the $5d^{2}D_{3/2}$ state of
$\mathrm{^{171}Yb^{+}}$, has been calculated using the relativistic
coupled-cluster method. Earlier a similar calculation was performed for the 4d
$^2D_{5/2}$ state of $\mathrm{^{88}Sr^{+}}$ which is the most accurate
determination to date {[}PRL, \textb... | physics.atom-ph | the electric quadrupole moment for the 5d2d_32 state of mathrm171yb has been calculated using the relativistic coupledcluster method earlier a similar calculation was performed for the 4d 2d_52 state of mathrm88sr which is the most accurate determination to date prl textbf96 193001 2006 the present calculation of the e... | [['the', 'electric', 'quadrupole', 'moment', 'for', 'the', '5d2d_32', 'state', 'of', 'mathrm171yb', 'has', 'been', 'calculated', 'using', 'the', 'relativistic', 'coupledcluster', 'method', 'earlier', 'a', 'similar', 'calculation', 'was', 'performed', 'for', 'the', '4d', '2d_52', 'state', 'of', 'mathrm88sr', 'which', 'i... | [-0.09368017155333962, 0.11190997850019158, -0.06337514664700027, 0.04035691709335273, -0.0378829905591709, -0.04688107519279839, 0.023151462001566727, 0.3399033985966653, -0.1650059445569161, -0.29367029766568487, 0.027015276110257235, -0.31529114482385157, -0.0627407049561091, 0.15103785113611243, 0.02398900026156824... |
710.3661 | Unified description of resonance and decay phenomena | In the Feshbach projection operator formalism, resonance as well as decay
phenomena are described by means of the complex eigenvalues and eigenfunctions
of the non-Hermitian Hamilton operator $H_{\rm eff}$ that appears in an
intermediate stage of the formalism. The formalism can be applied for the
description of isol... | quant-ph | in the feshbach projection operator formalism resonance as well as decay phenomena are described by means of the complex eigenvalues and eigenfunctions of the nonhermitian hamilton operator h_rm eff that appears in an intermediate stage of the formalism the formalism can be applied for the description of isolated reson... | [['in', 'the', 'feshbach', 'projection', 'operator', 'formalism', 'resonance', 'as', 'well', 'as', 'decay', 'phenomena', 'are', 'described', 'by', 'means', 'of', 'the', 'complex', 'eigenvalues', 'and', 'eigenfunctions', 'of', 'the', 'nonhermitian', 'hamilton', 'operator', 'h_rm', 'eff', 'that', 'appears', 'in', 'an', '... | [-0.15761326083451718, 0.1732571640107356, -0.06796579207985888, 0.10122290564656912, -0.004042975340239905, -0.12165845851602687, 0.02484691810034722, 0.3086477618639332, -0.248715284324528, -0.28439439141594275, 0.027667143887122842, -0.28146514624382396, -0.08580367941239446, 0.19905604030055976, 0.04762238639759252... |
710.3662 | Evolution of coherence between the Jaynes - Cummings Eigenstates in the
presence of repeated occupancy measurements: The case of resonant coupling | A two level system resonantly coupled to a single mode cavity field and
subject to ground state occupancy measurement like interaction is considered.
For this situation, the solution to the Lindblad master equation for the
density matrix is obtained with respect to the Jaynes Cummings eigenstate
representation. It is... | quant-ph | a two level system resonantly coupled to a single mode cavity field and subject to ground state occupancy measurement like interaction is considered for this situation the solution to the lindblad master equation for the density matrix is obtained with respect to the jaynes cummings eigenstate representation it is seen... | [['a', 'two', 'level', 'system', 'resonantly', 'coupled', 'to', 'a', 'single', 'mode', 'cavity', 'field', 'and', 'subject', 'to', 'ground', 'state', 'occupancy', 'measurement', 'like', 'interaction', 'is', 'considered', 'for', 'this', 'situation', 'the', 'solution', 'to', 'the', 'lindblad', 'master', 'equation', 'for',... | [-0.14864886124940732, 0.15924283990170807, -0.02203674025188845, -0.0013414398619296173, 0.009642433796006326, -0.17617034938078946, 0.07372016899507099, 0.26810882785894835, -0.2811208924260707, -0.30887796106365456, 0.05890350298544105, -0.3347498504444957, -0.03827039821324153, 0.1461485713505401, -0.01809949339188... |
710.3663 | Constraints on Unparticle Interactions from Particle and Antiparticle
Oscillations | We study unparticle effects on particle and antiparticle osillations in
meson-antimeson, and muonium-antimuonium systems. Unlike usual tree level
contributions to meson oscillations from heavy particle exchange with small
$\Gamma_{12}$, the unparticle may have sizeable contributions to both $M_{12}$
and $\Gamma_{12}$... | hep-ph | we study unparticle effects on particle and antiparticle osillations in mesonantimeson and muoniumantimuonium systems unlike usual tree level contributions to meson oscillations from heavy particle exchange with small gamma_12 the unparticle may have sizeable contributions to both m_12 and gamma_12 due to fractional di... | [['we', 'study', 'unparticle', 'effects', 'on', 'particle', 'and', 'antiparticle', 'osillations', 'in', 'mesonantimeson', 'and', 'muoniumantimuonium', 'systems', 'unlike', 'usual', 'tree', 'level', 'contributions', 'to', 'meson', 'oscillations', 'from', 'heavy', 'particle', 'exchange', 'with', 'small', 'gamma_12', 'the... | [-0.12443350110931889, 0.3234709220654938, -0.08046609172293835, 0.21070105294170588, -0.14126162913263493, -0.18078315800622755, 0.07870453184308565, 0.24890099997105805, -0.2207371294984351, -0.28195978873611793, -0.02624836829389729, -0.3641544962990219, -0.11107833782393162, 0.13054459140757504, 0.07409775007678115... |
710.3664 | Unimodular lattices in dimensions 14 and 15 over the Eisenstein integers | All indecomposable unimodular hermitian lattices in dimensions 14 and 15 over
the ring of integers in $\mathbb{Q}(\sqrt{-3})$ are determined. Precisely one
lattice in dimension 14 and two lattices in dimension 15 have minimal norm 3.
| math.NT math.GR | all indecomposable unimodular hermitian lattices in dimensions 14 and 15 over the ring of integers in mathbbqsqrt3 are determined precisely one lattice in dimension 14 and two lattices in dimension 15 have minimal norm 3 | [['all', 'indecomposable', 'unimodular', 'hermitian', 'lattices', 'in', 'dimensions', '14', 'and', '15', 'over', 'the', 'ring', 'of', 'integers', 'in', 'mathbbqsqrt3', 'are', 'determined', 'precisely', 'one', 'lattice', 'in', 'dimension', '14', 'and', 'two', 'lattices', 'in', 'dimension', '15', 'have', 'minimal', 'norm... | [-0.16551968114716667, 0.2349792701059154, 0.07879091143924077, 0.025702125765383242, 0.031950746064207385, -0.2175363200051444, -0.07104780344026429, 0.40496494052931664, -0.25916473429117887, -0.2224093328629221, 0.15780484105593393, -0.31275402648108347, -0.10391436043095642, 0.14827913335923637, -0.0152136178421122... |
710.3665 | Asymptotics of eigenfunctions on plane domains | We consider a family of domains $(\Omega_N)_{N>0}$ obtained by attaching an
$N\times 1$ rectangle to a fixed set $\Omega_0 = \{(x,y): 0<y<1,
-\phi(y)<x<0\}$, for a Lipschitz function $\phi\geq 0$. We derive full
asymptotic expansions, as $N\to\infty$, for the $m$th Dirichlet eigenvalue (for
any fixed $m$) and for the... | math.SP math.AP | we consider a family of domains omega_n_n0 obtained by attaching an ntimes 1 rectangle to a fixed set omega_0 xy 0y1 phiyx0 for a lipschitz function phigeq 0 we derive full asymptotic expansions as ntoinfty for the mth dirichlet eigenvalue for any fixed m and for the associated eigenfunction on omega_n the second term ... | [['we', 'consider', 'a', 'family', 'of', 'domains', 'omega_n_n0', 'obtained', 'by', 'attaching', 'an', 'ntimes', '1', 'rectangle', 'to', 'a', 'fixed', 'set', 'omega_0', 'xy', '0y1', 'phiyx0', 'for', 'a', 'lipschitz', 'function', 'phigeq', '0', 'we', 'derive', 'full', 'asymptotic', 'expansions', 'as', 'ntoinfty', 'for',... | [-0.16532287197187542, 0.06108136210201668, -0.034106753355908126, 0.03954167080175301, -0.07035381380383941, -0.0949510633691468, 0.04586169658419253, 0.3318734190479683, -0.2863112955078991, -0.19739405397928997, 0.1277168010181578, -0.33093021197075195, -0.09468270459170029, 0.1543242019093172, -0.03030933982438662,... |
710.3666 | Regression for partially observed variables and nonparametric quantiles
of conditional probabilities | Efficient estimation under bias sampling, censoring or truncation is a
difficult question which has been partially answered and the usual estimators
are not always consistent. Several biased designs are considered for models
with variables $(X,Y)$ where $Y$ is an indicator and $X$ an explanatory
variable, or for cont... | math.ST stat.TH | efficient estimation under bias sampling censoring or truncation is a difficult question which has been partially answered and the usual estimators are not always consistent several biased designs are considered for models with variables xy where y is an indicator and x an explanatory variable or for continuous variabl... | [['efficient', 'estimation', 'under', 'bias', 'sampling', 'censoring', 'or', 'truncation', 'is', 'a', 'difficult', 'question', 'which', 'has', 'been', 'partially', 'answered', 'and', 'the', 'usual', 'estimators', 'are', 'not', 'always', 'consistent', 'several', 'biased', 'designs', 'are', 'considered', 'for', 'models',... | [-0.06790771518928418, 0.09106290057357198, -0.07095657551553154, 0.16485564715222226, -0.07295825176507882, -0.247272585687376, 0.031198654431795727, 0.47359361002842587, -0.24281200771962386, -0.21076137946405704, 0.17784589128163847, -0.2576860511621487, -0.09119733632879629, 0.16514245442627673, -0.1702525279741140... |
710.3667 | Conformal changes of generalized complex structures | A conformal change of $TM\oplus T^*M$ is a morphism of the form
$(X,\alpha)\mapsto(X,e^\tau\alpha)$ $(X\in TM,\alpha\in T^*M,\tau\in
C^\infty(M))$. We characterize the generalized almost complex and almost
Hermitian structures that are locally conformal to integrable and to
generalized K\"ahler structures, respective... | math.DG | a conformal change of tmoplus tm is a morphism of the form xalphamapstoxetaualpha xin tmalphain tmtauin cinftym we characterize the generalized almost complex and almost hermitian structures that are locally conformal to integrable and to generalized kahler structures respectively and give examples of such structures | [['a', 'conformal', 'change', 'of', 'tmoplus', 'tm', 'is', 'a', 'morphism', 'of', 'the', 'form', 'xalphamapstoxetaualpha', 'xin', 'tmalphain', 'tmtauin', 'cinftym', 'we', 'characterize', 'the', 'generalized', 'almost', 'complex', 'and', 'almost', 'hermitian', 'structures', 'that', 'are', 'locally', 'conformal', 'to', '... | [-0.20388049295260793, 0.1046642809884534, -0.02918069450450795, 0.08906779472904634, -0.13484046519512222, -0.14302863936782592, -0.0839053836562449, 0.43286047663007465, -0.32674155730221954, -0.1377741163596511, 0.0874754673069609, -0.286863950169867, -0.25047056203974144, 0.15139683619851158, -0.0371072812870677, 0... |
710.3668 | Harmonic sections of tangent bundles equipped with Riemannian
$g$-natural metrics | Let $(M,g)$ be a Riemannian manifold. When $M$ is compact and the tangent
bundle $TM$ is equipped with the Sasaki metric $g^s$, the only vector fields
which define harmonic maps from $(M,g)$ to $(TM,g^s)$, are the parallel ones.
The Sasaki metric, and other well known Riemannian metrics on $TM$, are
particular exampl... | math.DG | let mg be a riemannian manifold when m is compact and the tangent bundle tm is equipped with the sasaki metric gs the only vector fields which define harmonic maps from mg to tmgs are the parallel ones the sasaki metric and other well known riemannian metrics on tm are particular examples of gnatural metrics we equip t... | [['let', 'mg', 'be', 'a', 'riemannian', 'manifold', 'when', 'm', 'is', 'compact', 'and', 'the', 'tangent', 'bundle', 'tm', 'is', 'equipped', 'with', 'the', 'sasaki', 'metric', 'gs', 'the', 'only', 'vector', 'fields', 'which', 'define', 'harmonic', 'maps', 'from', 'mg', 'to', 'tmgs', 'are', 'the', 'parallel', 'ones', 't... | [-0.1918577162494648, 0.09354728311924738, -0.0026803786495646228, 0.07028855288568522, -0.16459739568939397, -0.18762832158019097, -0.06955630190272644, 0.43909283711131913, -0.23172956375965795, -0.22761322012243485, 0.0655177861748227, -0.3101158251588061, -0.200077403440746, 0.15307706887426886, -0.1057221858843582... |
710.3669 | Alpha-determinant cyclic modules and Jacobi polynomials | We study the cyclic $U(\mathfrak{gl}_n)$-module generated by the $l$-th power
of the $\alpha$-determinant. When $l$ is a non-negative integer, for all but
finite exceptional values of $alpha$, one shows that this cyclic module is
isomorphic to the $n$-th tensor space $(S^l(\mathbb{C}^n))^{\otimes n}$ of the
symmetric... | math.RT | we study the cyclic umathfrakgl_nmodule generated by the lth power of the alphadeterminant when l is a nonnegative integer for all but finite exceptional values of alpha one shows that this cyclic module is isomorphic to the nth tensor space slmathbbcnotimes n of the symmetric lth tensor space of mathbbcn if alpha is e... | [['we', 'study', 'the', 'cyclic', 'umathfrakgl_nmodule', 'generated', 'by', 'the', 'lth', 'power', 'of', 'the', 'alphadeterminant', 'when', 'l', 'is', 'a', 'nonnegative', 'integer', 'for', 'all', 'but', 'finite', 'exceptional', 'values', 'of', 'alpha', 'one', 'shows', 'that', 'this', 'cyclic', 'module', 'is', 'isomorph... | [-0.19560095860562737, 0.15786498786671269, -0.036839031548269334, -0.007769953381765875, -0.058719302791981925, -0.13879569807059822, -0.056480087698136845, 0.3104615398953038, -0.3461289811639055, -0.17288069305941461, 0.13710265601384303, -0.25130695202087444, -0.18973580509003612, 0.13263995548890484, -0.0352899878... |
710.367 | Generalized Israel Junction Conditions for a Fourth-Order Brane World | We discuss a general fourth-order theory of gravity on the brane. In general,
the formulation of the junction conditions (except for Euler characteristics
such as Gauss-Bonnet term) leads to the higher powers of the delta function and
requires regularization. We suggest the way to avoid such a problem by imposing
the... | hep-th astro-ph gr-qc | we discuss a general fourthorder theory of gravity on the brane in general the formulation of the junction conditions except for euler characteristics such as gaussbonnet term leads to the higher powers of the delta function and requires regularization we suggest the way to avoid such a problem by imposing the metric a... | [['we', 'discuss', 'a', 'general', 'fourthorder', 'theory', 'of', 'gravity', 'on', 'the', 'brane', 'in', 'general', 'the', 'formulation', 'of', 'the', 'junction', 'conditions', 'except', 'for', 'euler', 'characteristics', 'such', 'as', 'gaussbonnet', 'term', 'leads', 'to', 'the', 'higher', 'powers', 'of', 'the', 'delta... | [-0.17129143392667173, 0.052810308241987514, -0.09281465482781641, 0.07911412040120921, -0.11663091864465969, -0.10965211626316887, 0.001328842076327419, 0.29411998978903287, -0.26823324761353434, -0.28365805875509975, 0.09735210596263641, -0.2608504803138203, -0.14229929629218532, 0.1247036274522543, -0.06070726199541... |
710.3671 | Modelling highway-traffic headway distributions using superstatistics | We study traffic clearance distributions (i.e., the instantaneous gap between
successive vehicles) and time headway distributions by applying Beck and
Cohen's superstatistics. We model the transition from free phase to congested
phase with the increase of vehicle density as a transition from the Poisson
statistics to... | physics.soc-ph | we study traffic clearance distributions ie the instantaneous gap between successive vehicles and time headway distributions by applying beck and cohens superstatistics we model the transition from free phase to congested phase with the increase of vehicle density as a transition from the poisson statistics to that of ... | [['we', 'study', 'traffic', 'clearance', 'distributions', 'ie', 'the', 'instantaneous', 'gap', 'between', 'successive', 'vehicles', 'and', 'time', 'headway', 'distributions', 'by', 'applying', 'beck', 'and', 'cohens', 'superstatistics', 'we', 'model', 'the', 'transition', 'from', 'free', 'phase', 'to', 'congested', 'ph... | [-0.08942606514402196, 0.1357408387987489, -0.14230723348569818, 0.08446290468450933, 0.0068556936622589035, -0.09930495023974671, 0.12271531151537578, 0.3590377343867996, -0.26768417364456154, -0.31879782375047166, 0.056907403372965785, -0.3101068813996637, -0.11040037773772085, 0.14033684460343215, -0.072629819103862... |
710.3672 | Lepton masses and mixings in orbifold models with three Higgs families | We analyse the phenomenological viability of heterotic Z(3) orbifolds with
two Wilson lines, which naturally predict three supersymmetric families of
matter and Higgs fields. Given that these models can accommodate realistic
scenarios for the quark sector avoiding potentially dangerous flavour-changing
neutral curren... | hep-ph | we analyse the phenomenological viability of heterotic z3 orbifolds with two wilson lines which naturally predict three supersymmetric families of matter and higgs fields given that these models can accommodate realistic scenarios for the quark sector avoiding potentially dangerous flavourchanging neutral currents we n... | [['we', 'analyse', 'the', 'phenomenological', 'viability', 'of', 'heterotic', 'z3', 'orbifolds', 'with', 'two', 'wilson', 'lines', 'which', 'naturally', 'predict', 'three', 'supersymmetric', 'families', 'of', 'matter', 'and', 'higgs', 'fields', 'given', 'that', 'these', 'models', 'can', 'accommodate', 'realistic', 'sce... | [-0.1148891960826492, 0.26416946517964524, 0.028656424846880697, 0.21740761563126798, -0.10213377160490841, -0.22161843384345692, 0.054100370982171145, 0.32516625625962614, -0.14405855072301724, -0.31234441792732603, 0.05327198110140299, -0.2583989242732685, -0.021706556667879184, 0.13273221061074286, -0.00603720106144... |
710.3673 | On the Fluctuation Relation for Nose-Hoover Boundary Thermostated
Systems | We discuss the transient and steady state fluctuation relation for a
mechanical system in contact with two deterministic thermostats at different
temperatures. The system is a modified Lorentz gas in which the fixed
scatterers exchange energy with the gas of particles, and the thermostats are
modelled by two Nos\'e-H... | cond-mat.stat-mech | we discuss the transient and steady state fluctuation relation for a mechanical system in contact with two deterministic thermostats at different temperatures the system is a modified lorentz gas in which the fixed scatterers exchange energy with the gas of particles and the thermostats are modelled by two nosehoover t... | [['we', 'discuss', 'the', 'transient', 'and', 'steady', 'state', 'fluctuation', 'relation', 'for', 'a', 'mechanical', 'system', 'in', 'contact', 'with', 'two', 'deterministic', 'thermostats', 'at', 'different', 'temperatures', 'the', 'system', 'is', 'a', 'modified', 'lorentz', 'gas', 'in', 'which', 'the', 'fixed', 'sca... | [-0.1371600315975461, 0.16917248790132555, -0.11870115075924216, 0.09352516547796574, 0.037916178590162324, -0.13327537726293853, 0.03930184922250424, 0.32428941214159923, -0.23754537278548518, -0.28447948619227936, 0.08409110322703627, -0.26041940579864575, -0.057458137147168215, 0.19426161869171452, -0.01850785304930... |
710.3674 | Semigroup algebras of submonoids of polycyclic-by-finite groups and
maximal orders | Necessary and sufficient conditions are given for a prime Noetherian algebra
K[S] of a submonoid S of a polycyclic-by-finite group G to be a maximal order.
These conditions are entirely in terms of the monoid S. This extends earlier
results of Brown concerned with the group ring case and of the authors for the
case w... | math.RA | necessary and sufficient conditions are given for a prime noetherian algebra ks of a submonoid s of a polycyclicbyfinite group g to be a maximal order these conditions are entirely in terms of the monoid s this extends earlier results of brown concerned with the group ring case and of the authors for the case where ks ... | [['necessary', 'and', 'sufficient', 'conditions', 'are', 'given', 'for', 'a', 'prime', 'noetherian', 'algebra', 'ks', 'of', 'a', 'submonoid', 's', 'of', 'a', 'polycyclicbyfinite', 'group', 'g', 'to', 'be', 'a', 'maximal', 'order', 'these', 'conditions', 'are', 'entirely', 'in', 'terms', 'of', 'the', 'monoid', 's', 'thi... | [-0.21308164576404406, 0.043645927048914256, -0.09126289759869458, 0.033727550808508255, -0.10933669296200157, -0.13971276760681486, 0.012365111733832564, 0.3155918541616287, -0.29514063381757893, -0.2275274816488267, 0.13292064787018434, -0.228097672833771, -0.06525322312458617, 0.18837686683066557, -0.121993408965893... |
710.3675 | The combinatorics of Bogoliubov's recursion in renormalization | We describe various combinatorial aspects of the Birkhoff-Connes-Kreimer
factorization in perturbative renormalisation. The analog of Bogoliubov's
preparation map on the Lie algebra of Feynman graphs is identified with the
pre-Lie Magnus expansion. Our results apply to any connected filtered Hopf
algebra, based on th... | math-ph hep-th math.CO math.MP | we describe various combinatorial aspects of the birkhoffconneskreimer factorization in perturbative renormalisation the analog of bogoliubovs preparation map on the lie algebra of feynman graphs is identified with the prelie magnus expansion our results apply to any connected filtered hopf algebra based on the pronilp... | [['we', 'describe', 'various', 'combinatorial', 'aspects', 'of', 'the', 'birkhoffconneskreimer', 'factorization', 'in', 'perturbative', 'renormalisation', 'the', 'analog', 'of', 'bogoliubovs', 'preparation', 'map', 'on', 'the', 'lie', 'algebra', 'of', 'feynman', 'graphs', 'is', 'identified', 'with', 'the', 'prelie', 'm... | [-0.1858736033877358, 0.040449587233306376, -0.1529293959029019, 0.05592621174873784, -0.2018387844786048, -0.04463855266571045, -0.022810555566102265, 0.33296852342318745, -0.3552060141041875, -0.1794107532221824, 0.1413139451551251, -0.1832275335304439, -0.176733790487051, 0.1977803382370621, -0.10740456067025661, -0... |
710.3676 | Outliers in dynamic factor models | Dynamic factor models have a wide range of applications in econometrics and
applied economics. The basic motivation resides in their capability of reducing
a large set of time series to only few indicators (factors). If the number of
time series is large compared to the available number of observations then most
info... | math.ST stat.TH | dynamic factor models have a wide range of applications in econometrics and applied economics the basic motivation resides in their capability of reducing a large set of time series to only few indicators factors if the number of time series is large compared to the available number of observations then most informatio... | [['dynamic', 'factor', 'models', 'have', 'a', 'wide', 'range', 'of', 'applications', 'in', 'econometrics', 'and', 'applied', 'economics', 'the', 'basic', 'motivation', 'resides', 'in', 'their', 'capability', 'of', 'reducing', 'a', 'large', 'set', 'of', 'time', 'series', 'to', 'only', 'few', 'indicators', 'factors', 'if... | [-0.06924453034583826, 0.042927177471117864, -0.052980613972370826, 0.10553956848190293, -0.09471452906248434, -0.14706013669195933, 0.038825374393376945, 0.3920032152650403, -0.27448347491536323, -0.34151608171398, 0.16375054281339615, -0.2709138237565354, -0.12655432377804948, 0.23443310031742678, -0.0948563824195469... |
710.3677 | Five-dimensional PPN formalism and experimental test of Kaluza-Klein
theory | The parametrized post Newtonian formalism for 5-dimensional metric theories
with a compact extra dimension is developed. The relation of the 5-dimensional
and 4-dimensional formulations is then analyzed, in order to compare the higher
dimensional theories of gravity with experiments. It turns out that the value
of po... | gr-qc astro-ph hep-th | the parametrized post newtonian formalism for 5dimensional metric theories with a compact extra dimension is developed the relation of the 5dimensional and 4dimensional formulations is then analyzed in order to compare the higher dimensional theories of gravity with experiments it turns out that the value of post newto... | [['the', 'parametrized', 'post', 'newtonian', 'formalism', 'for', '5dimensional', 'metric', 'theories', 'with', 'a', 'compact', 'extra', 'dimension', 'is', 'developed', 'the', 'relation', 'of', 'the', '5dimensional', 'and', '4dimensional', 'formulations', 'is', 'then', 'analyzed', 'in', 'order', 'to', 'compare', 'the',... | [-0.11430180859386775, 0.14084914772141857, -0.07854479780493706, 0.10302271806251477, -0.08675204399133138, -0.15869788772554375, -0.029487499427369925, 0.23175459871452084, -0.18152509361286373, -0.2873527861346363, 0.049333728157102553, -0.2707069401684053, -0.16624141400497333, 0.17769747229028202, -0.0778630505973... |
710.3678 | An Extension of Alzer's Inequality | In this article, we obtain two interesting general inequalities concerning
Riemman sums of convex functions, which in particular, sharpen Alzer's
inequality and give a suitable converse for it.
| math.CA | in this article we obtain two interesting general inequalities concerning riemman sums of convex functions which in particular sharpen alzers inequality and give a suitable converse for it | [['in', 'this', 'article', 'we', 'obtain', 'two', 'interesting', 'general', 'inequalities', 'concerning', 'riemman', 'sums', 'of', 'convex', 'functions', 'which', 'in', 'particular', 'sharpen', 'alzers', 'inequality', 'and', 'give', 'a', 'suitable', 'converse', 'for', 'it']] | [-0.0991392778897924, 0.011144784645044379, -0.11100567921364148, 0.1735247098965504, -0.08616928962458457, -0.2274253606363865, 0.05558752529655716, 0.26387844647147823, -0.2861828726849386, -0.1904818899264293, 0.15164039308105462, -0.2181867745571903, -0.22136397919218456, 0.26758386720237987, -0.1560152561204242, 0... |
710.3679 | Bayesian inference with rescaled Gaussian process priors | We use rescaled Gaussian processes as prior models for functional parameters
in nonparametric statistical models. We show how the rate of contraction of the
posterior distributions depends on the scaling factor. In particular, we
exhibit rescaled Gaussian process priors yielding posteriors that contract
around the tr... | math.ST stat.TH | we use rescaled gaussian processes as prior models for functional parameters in nonparametric statistical models we show how the rate of contraction of the posterior distributions depends on the scaling factor in particular we exhibit rescaled gaussian process priors yielding posteriors that contract around the true pa... | [['we', 'use', 'rescaled', 'gaussian', 'processes', 'as', 'prior', 'models', 'for', 'functional', 'parameters', 'in', 'nonparametric', 'statistical', 'models', 'we', 'show', 'how', 'the', 'rate', 'of', 'contraction', 'of', 'the', 'posterior', 'distributions', 'depends', 'on', 'the', 'scaling', 'factor', 'in', 'particul... | [-0.024226762423875618, 0.07218047903517066, -0.13225650416909537, 0.13996898070592526, -0.02403512481711249, -0.10449026714760198, 0.134670690445702, 0.4264971135434375, -0.28225286417195933, -0.2331290939377982, 0.07216057543809623, -0.21473049729673274, -0.11666550216223322, 0.20376779250592106, -0.07759984631313761... |
710.368 | Mass and angular-momentum inequalities for axi-symmetric initial data
sets I. Positivity of mass | We extend the validity of Brill's axisymmetric positive energy theorem to all
asymptotically flat initial data sets with positive scalar curvature on simply
connected manifolds.
| gr-qc | we extend the validity of brills axisymmetric positive energy theorem to all asymptotically flat initial data sets with positive scalar curvature on simply connected manifolds | [['we', 'extend', 'the', 'validity', 'of', 'brills', 'axisymmetric', 'positive', 'energy', 'theorem', 'to', 'all', 'asymptotically', 'flat', 'initial', 'data', 'sets', 'with', 'positive', 'scalar', 'curvature', 'on', 'simply', 'connected', 'manifolds']] | [-0.1996726011345163, 0.09432908296585082, -0.044427000526338814, 0.14443876918405293, -0.1357198387943208, -0.19693919442594052, -0.025603871084749697, 0.3388288452103734, -0.12866483643651008, -0.2161634428007528, 0.10978011744096876, -0.2799451917409897, -0.04654247458325699, 0.18446182310581208, -0.0830699122697115... |
710.3681 | Some New Inequalities Between Important Means | In this paper, mainly using the convexity of the function
$\frac{a^x-b^x}{c^x-d^x}$ and convexity or concavity of the function
$\ln\frac{a^x-b^x}{c^x-d^x}$ on the real line, where $a>b\geq c>d>0$ are fixed
real numbers, we obtain some important relations between various important
means of these numbers. Also, we appl... | math.CA | in this paper mainly using the convexity of the function fracaxbxcxdx and convexity or concavity of the function lnfracaxbxcxdx on the real line where abgeq cd0 are fixed real numbers we obtain some important relations between various important means of these numbers also we apply the obtained results to ky fan type in... | [['in', 'this', 'paper', 'mainly', 'using', 'the', 'convexity', 'of', 'the', 'function', 'fracaxbxcxdx', 'and', 'convexity', 'or', 'concavity', 'of', 'the', 'function', 'lnfracaxbxcxdx', 'on', 'the', 'real', 'line', 'where', 'abgeq', 'cd0', 'are', 'fixed', 'real', 'numbers', 'we', 'obtain', 'some', 'important', 'relati... | [-0.11143629267722385, 0.04842532390362716, -0.059494294841507714, 0.13724557133017307, -0.08986085593018547, -0.1100448611624805, 0.07030677459260914, 0.3280879304345165, -0.29832834916721496, -0.28458263421530966, 0.15424576292571146, -0.27815522760751527, -0.208809819193058, 0.234147813591075, -0.0721132578660867, 0... |
710.3682 | Probing Elemental Abundances in SNR 1987A Using XMM-Newton | We report on the latest (2007 Jan) observations of supernova remnant (SNR)
1987A from the XMM-Newton mission. Since the 2003 May observations of Haberl et
al. (2006), 11 emission lines have experienced increases in flux by factors ~ 3
to 10, with the 775 eV line of O VIII showing the greatest increase; we have
observ... | astro-ph | we report on the latest 2007 jan observations of supernova remnant snr 1987a from the xmmnewton mission since the 2003 may observations of haberl et al 2006 11 emission lines have experienced increases in flux by factors 3 to 10 with the 775 ev line of o viii showing the greatest increase we have observed 6 lines of fe... | [['we', 'report', 'on', 'the', 'latest', '2007', 'jan', 'observations', 'of', 'supernova', 'remnant', 'snr', '1987a', 'from', 'the', 'xmmnewton', 'mission', 'since', 'the', '2003', 'may', 'observations', 'of', 'haberl', 'et', 'al', '2006', '11', 'emission', 'lines', 'have', 'experienced', 'increases', 'in', 'flux', 'by... | [-0.039055189312587814, 0.08778091169155362, 0.02653968317686502, 0.04086550131145182, -0.01682204420101343, -0.12314588765788126, 0.09099973727404223, 0.42211776828593706, -0.13724431935122675, -0.3961209333019398, 0.0185414047386097, -0.3190059939926245, 0.0022543995776603304, 0.15166754606346863, -0.0590893024417749... |
710.3683 | Spiral Galaxies Rotation Curves with a Logarithmic Corrected Newtonian
Gravitational Potential | We analyze the rotation curves of 10 spiral galaxies with a newtonian
potential corrected with an extra logarithmic term, using a disc modelization
for the spiral galaxies. There is a new constant associated with the extra term
in the potential. The rotation curve of the chosen sample of spiral galaxies is
well repro... | astro-ph gr-qc hep-th | we analyze the rotation curves of 10 spiral galaxies with a newtonian potential corrected with an extra logarithmic term using a disc modelization for the spiral galaxies there is a new constant associated with the extra term in the potential the rotation curve of the chosen sample of spiral galaxies is well reproduced... | [['we', 'analyze', 'the', 'rotation', 'curves', 'of', '10', 'spiral', 'galaxies', 'with', 'a', 'newtonian', 'potential', 'corrected', 'with', 'an', 'extra', 'logarithmic', 'term', 'using', 'a', 'disc', 'modelization', 'for', 'the', 'spiral', 'galaxies', 'there', 'is', 'a', 'new', 'constant', 'associated', 'with', 'the'... | [-0.13874783089184867, 0.06627221843051043, -0.10576145703228013, 0.11029974139750093, -0.0736093629550721, -0.11296439274502475, 0.003988711253831363, 0.35146350338168086, -0.23622755593221104, -0.31636548479132, 0.06689755166076966, -0.2579595570097722, -0.10594240788902555, 0.18565577747566359, -0.05457880097397026,... |
710.3684 | Weak convergence of Metropolis algorithms for non-i.i.d. target
distributions | In this paper, we shall optimize the efficiency of Metropolis algorithms for
multidimensional target distributions with scaling terms possibly depending on
the dimension. We propose a method for determining the appropriate form for the
scaling of the proposal distribution as a function of the dimension, which
leads t... | math.PR | in this paper we shall optimize the efficiency of metropolis algorithms for multidimensional target distributions with scaling terms possibly depending on the dimension we propose a method for determining the appropriate form for the scaling of the proposal distribution as a function of the dimension which leads to the... | [['in', 'this', 'paper', 'we', 'shall', 'optimize', 'the', 'efficiency', 'of', 'metropolis', 'algorithms', 'for', 'multidimensional', 'target', 'distributions', 'with', 'scaling', 'terms', 'possibly', 'depending', 'on', 'the', 'dimension', 'we', 'propose', 'a', 'method', 'for', 'determining', 'the', 'appropriate', 'for... | [-0.0969436971908323, 0.08921762716732723, -0.12006441903222038, 0.07033666716720235, -0.04851046859858984, -0.1274640374502773, 0.07031525778920805, 0.3301914537168411, -0.22410564810172262, -0.28163054614630806, 0.09320322586734027, -0.2321435709775661, -0.13689078168988408, 0.1985552728355649, -0.07751998245850744, ... |
710.3685 | Indirect search for Dark Matter with the ANTARES neutrino telescope | Relic neutralinos produced after the Big Bang are favoured candidates for
Dark Matter. They can accumulate at the centre of massive celestial objects
like our Sun. Their annihilation can result in a high-energy neutrino flux that
could be detectable as a localised emission with earth-based neutrino
telescopes like AN... | astro-ph | relic neutralinos produced after the big bang are favoured candidates for dark matter they can accumulate at the centre of massive celestial objects like our sun their annihilation can result in a highenergy neutrino flux that could be detectable as a localised emission with earthbased neutrino telescopes like antares ... | [['relic', 'neutralinos', 'produced', 'after', 'the', 'big', 'bang', 'are', 'favoured', 'candidates', 'for', 'dark', 'matter', 'they', 'can', 'accumulate', 'at', 'the', 'centre', 'of', 'massive', 'celestial', 'objects', 'like', 'our', 'sun', 'their', 'annihilation', 'can', 'result', 'in', 'a', 'highenergy', 'neutrino',... | [-0.08570263334654607, 0.2505934904591086, -0.08652324941525304, 0.1875607500786715, -0.10210796122261312, -0.08205649521452991, -0.029510147941528998, 0.33855169200537244, -0.18834285476517057, -0.3939553028746937, 0.10058032636258625, -0.321896720635757, -0.025829472819740854, 0.22248852897560997, 0.01412311477293626... |
710.3686 | Some Results on Inverse Scattering | A review of some of the author's results in the area of inverse scattering is
given. The following topics are discussed: 1) Property $C$ and applications, 2)
Stable inversion of fixed-energy 3D scattering data and its error estimate, 3)
Inverse scattering with ''incomplete`` data, 4) Inverse scattering for
inhomogene... | math-ph math.MP | a review of some of the authors results in the area of inverse scattering is given the following topics are discussed 1 property c and applications 2 stable inversion of fixedenergy 3d scattering data and its error estimate 3 inverse scattering with incomplete data 4 inverse scattering for inhomogeneous schrodinger equ... | [['a', 'review', 'of', 'some', 'of', 'the', 'authors', 'results', 'in', 'the', 'area', 'of', 'inverse', 'scattering', 'is', 'given', 'the', 'following', 'topics', 'are', 'discussed', '1', 'property', 'c', 'and', 'applications', '2', 'stable', 'inversion', 'of', 'fixedenergy', '3d', 'scattering', 'data', 'and', 'its', '... | [-0.07632486051192781, 0.10971883165024576, -0.032788240381318036, 0.11225400818225577, -0.0811269650022026, -0.15064374349828138, -0.0011084389111378275, 0.385024296783949, -0.3032536466957116, -0.3244157963447639, 0.18520934219838533, -0.3474376345068583, -0.12650104206900845, 0.14439505088471305, 0.02473796399875132... |
710.3687 | On invariant measures of stochastic recursions in a critical case | We consider an autoregressive model on $\mathbb{R}$ defined by the recurrence
equation $X_n=A_nX_{n-1}+B_n$, where $\{(B_n,A_n)\}$ are i.i.d. random
variables valued in $\mathbb{R}\times\mathbb{R}^+$ and $\mathbb {E}[\log
A_1]=0$ (critical case). It was proved by Babillot, Bougerol and Elie that
there exists a unique... | math.PR | we consider an autoregressive model on mathbbr defined by the recurrence equation x_na_nx_n1b_n where b_na_n are iid random variables valued in mathbbrtimesmathbbr and mathbb elog a_10 critical case it was proved by babillot bougerol and elie that there exists a unique invariant radon measure of the process x_n the aim... | [['we', 'consider', 'an', 'autoregressive', 'model', 'on', 'mathbbr', 'defined', 'by', 'the', 'recurrence', 'equation', 'x_na_nx_n1b_n', 'where', 'b_na_n', 'are', 'iid', 'random', 'variables', 'valued', 'in', 'mathbbrtimesmathbbr', 'and', 'mathbb', 'elog', 'a_10', 'critical', 'case', 'it', 'was', 'proved', 'by', 'babil... | [-0.14797140761731645, 0.12416448770897193, -0.08061232370626484, 0.07498256590251667, -0.009463678082652591, -0.18902617782304013, -0.0017981769680674817, 0.34764618950115667, -0.3072656851664588, -0.13986602352579702, 0.1225305849432983, -0.3318805105329768, -0.1830388645065722, 0.1480790708383948, -0.105313676233227... |
710.3688 | Partition Function for Two-Dimensional Nearest Neighbour Ising Model in
a Non-Zero Magnetic Field for a Square Lattice of 16 Sites | An explicit expression for the partition function of two-dimensional nearest
neighbour Ising models in the presence of a magnetic field is derived by a
systematic enumeration of all the spin configurations pertaining to a square
lattice of sixteen sites. The critical temperature is shown to be in excellent
agreement ... | cond-mat.stat-mech | an explicit expression for the partition function of twodimensional nearest neighbour ising models in the presence of a magnetic field is derived by a systematic enumeration of all the spin configurations pertaining to a square lattice of sixteen sites the critical temperature is shown to be in excellent agreement with... | [['an', 'explicit', 'expression', 'for', 'the', 'partition', 'function', 'of', 'twodimensional', 'nearest', 'neighbour', 'ising', 'models', 'in', 'the', 'presence', 'of', 'a', 'magnetic', 'field', 'is', 'derived', 'by', 'a', 'systematic', 'enumeration', 'of', 'all', 'the', 'spin', 'configurations', 'pertaining', 'to', ... | [-0.16935311464614988, 0.12379394031507665, 0.026658972507224432, 0.053065599413544294, -0.004688110897347095, -0.0993394694172792, 0.038846407937521615, 0.3495654242615851, -0.18648134788409584, -0.3293143350276209, 0.08539694188059205, -0.2902818536016321, -0.1027603146161825, 0.20686111687904313, 0.06794107674310605... |
710.3689 | Quasi-stationary regime of a branching random walk in presence of an
absorbing wall | A branching random walk in presence of an absorbing wall moving at a constant
velocity $v$ undergoes a phase transition as the velocity $v$ of the wall
varies. Below the critical velocity $v_c$, the population has a non-zero
survival probability and when the population survives its size grows
exponentially. We invest... | cond-mat.stat-mech q-bio.PE | a branching random walk in presence of an absorbing wall moving at a constant velocity v undergoes a phase transition as the velocity v of the wall varies below the critical velocity v_c the population has a nonzero survival probability and when the population survives its size grows exponentially we investigate the hi... | [['a', 'branching', 'random', 'walk', 'in', 'presence', 'of', 'an', 'absorbing', 'wall', 'moving', 'at', 'a', 'constant', 'velocity', 'v', 'undergoes', 'a', 'phase', 'transition', 'as', 'the', 'velocity', 'v', 'of', 'the', 'wall', 'varies', 'below', 'the', 'critical', 'velocity', 'v_c', 'the', 'population', 'has', 'a',... | [-0.10969388929609125, 0.19301911076101347, -0.09646803046015497, 0.03103234584735522, -0.024869216628408488, -0.14949199927445406, 0.09744409133754044, 0.3465712424964668, -0.30330305431897825, -0.2186934093091016, 0.09417155773740095, -0.26616116812548196, -0.07224909153181869, 0.13960059928836133, -0.016749920866762... |
710.369 | Wesson's IMT with a Weylian bulk | The foundations of Wesson's induced matter theory are analyzed. It is shown
that the 5D empty bulk must be regarded rather as a Weylian space than as a
Riemannian one.The framework of a Weyl-Dirac version of Wesson's theory is
elaborated and discussed. The bulk possesses in addition to the metric tensor a
Weylian con... | gr-qc | the foundations of wessons induced matter theory are analyzed it is shown that the 5d empty bulk must be regarded rather as a weylian space than as a riemannian onethe framework of a weyldirac version of wessons theory is elaborated and discussed the bulk possesses in addition to the metric tensor a weylian connection ... | [['the', 'foundations', 'of', 'wessons', 'induced', 'matter', 'theory', 'are', 'analyzed', 'it', 'is', 'shown', 'that', 'the', '5d', 'empty', 'bulk', 'must', 'be', 'regarded', 'rather', 'as', 'a', 'weylian', 'space', 'than', 'as', 'a', 'riemannian', 'onethe', 'framework', 'of', 'a', 'weyldirac', 'version', 'of', 'wesso... | [-0.12369725080776682, 0.17798961536275185, -0.08119149906362624, 0.11279437302839646, -0.09966226623417127, -0.12387410750949478, -0.04711596564355088, 0.3007773171733827, -0.19974991820871513, -0.27591009502437835, 0.04656743766378334, -0.27503879520883584, -0.1794099220906959, 0.12840197949690071, -0.046483629561485... |
710.3691 | A MST algorithm for source detection in gamma-ray images | We developed a source detection algorithm based on the Minimal Spanning Tree
(MST), that is a graph-theoretical method useful for finding clusters in a
given set of points. This algorithm is applied to gamma-ray bidimensional
images where the points correspond to the arrival direction of photons, and the
possible sou... | astro-ph | we developed a source detection algorithm based on the minimal spanning tree mst that is a graphtheoretical method useful for finding clusters in a given set of points this algorithm is applied to gammaray bidimensional images where the points correspond to the arrival direction of photons and the possible sources are ... | [['we', 'developed', 'a', 'source', 'detection', 'algorithm', 'based', 'on', 'the', 'minimal', 'spanning', 'tree', 'mst', 'that', 'is', 'a', 'graphtheoretical', 'method', 'useful', 'for', 'finding', 'clusters', 'in', 'a', 'given', 'set', 'of', 'points', 'this', 'algorithm', 'is', 'applied', 'to', 'gammaray', 'bidimensi... | [-0.08756728144054184, 0.06774868309721027, -0.07660704227596127, 0.08783518092935004, -0.10842582033422855, -0.06636194641461336, 0.08704761134318711, 0.42579553433268374, -0.22059012085217858, -0.35594041238612933, 0.09275753166686916, -0.2863657059123283, -0.12051324151180351, 0.2129966499891428, -0.0494632231756205... |
710.3692 | Universality class of the pair contact process with diffusion | The pair contact process with diffusion (PCPD) is studied with a standard
Monte Carlo approach and with simulations at fixed densities. A standard
analysis of the simulation results, based on the particle densities or on the
pair densities, yields inconsistent estimates for the critical exponents.
However, if a well-... | cond-mat.stat-mech | the pair contact process with diffusion pcpd is studied with a standard monte carlo approach and with simulations at fixed densities a standard analysis of the simulation results based on the particle densities or on the pair densities yields inconsistent estimates for the critical exponents however if a wellchosen lin... | [['the', 'pair', 'contact', 'process', 'with', 'diffusion', 'pcpd', 'is', 'studied', 'with', 'a', 'standard', 'monte', 'carlo', 'approach', 'and', 'with', 'simulations', 'at', 'fixed', 'densities', 'a', 'standard', 'analysis', 'of', 'the', 'simulation', 'results', 'based', 'on', 'the', 'particle', 'densities', 'or', 'o... | [-0.05051926807050897, 0.171299849493927, -0.07750904349504167, 0.0895263101003978, 0.008888980899338084, -0.1657817805748396, 0.05117275013523822, 0.35607406557168775, -0.21830036963271623, -0.27085114183771136, 0.0805765445261161, -0.32897587798277633, -0.07002356929801368, 0.21464430608113508, 0.04253773427208756, 0... |
710.3693 | Exponential mixing for finite-dimensional approximations of the
Schr\"odinger equation with multiplicative noise | We study the ergodicity of finite-dimensional approximations of the
Schr\"odinger equation. The system is driven by a multiplicative scalar noise.
Under general assumptions over the distribution of the noise, we show that the
system has a unique stationary measure $\mu$ on the unit sphere $S$ in $\C^n$,
and $\mu$ is ... | math-ph math.MP | we study the ergodicity of finitedimensional approximations of the schrodinger equation the system is driven by a multiplicative scalar noise under general assumptions over the distribution of the noise we show that the system has a unique stationary measure mu on the unit sphere s in cn and mu is absolutely continuous... | [['we', 'study', 'the', 'ergodicity', 'of', 'finitedimensional', 'approximations', 'of', 'the', 'schrodinger', 'equation', 'the', 'system', 'is', 'driven', 'by', 'a', 'multiplicative', 'scalar', 'noise', 'under', 'general', 'assumptions', 'over', 'the', 'distribution', 'of', 'the', 'noise', 'we', 'show', 'that', 'the',... | [-0.1456056536990218, 0.09472295221639797, -0.09634356884962472, 0.04120880222471897, 0.006686706058098934, -0.1308407409931533, 0.04070146989542991, 0.3622379053151235, -0.29536095780786126, -0.1689396102425235, 0.11925751157177729, -0.2885737754404545, -0.09840997031424195, 0.15500803326722234, -0.08630441185669042, ... |
710.3694 | Measurement of the parity-violating triton emission asymmetry in the
reaction 6Li(n,alfa)3H with polarised cold neutrons | We describe measurements of the parity-violating (P-odd) triton emission
asymmetry coefficient in the 6Li(n,alfa)3H reaction with polarised cold
neutrons. Experiments were carried out at the Petersburg Nuclear Physics
Institute (Gatchina, Russia) and at the Institut Laue-Langevin (Grenoble,
France). We employed an io... | nucl-ex | we describe measurements of the parityviolating podd triton emission asymmetry coefficient in the 6linalfa3h reaction with polarised cold neutrons experiments were carried out at the petersburg nuclear physics institute gatchina russia and at the institut lauelangevin grenoble france we employed an ionisation chamber i... | [['we', 'describe', 'measurements', 'of', 'the', 'parityviolating', 'podd', 'triton', 'emission', 'asymmetry', 'coefficient', 'in', 'the', '6linalfa3h', 'reaction', 'with', 'polarised', 'cold', 'neutrons', 'experiments', 'were', 'carried', 'out', 'at', 'the', 'petersburg', 'nuclear', 'physics', 'institute', 'gatchina',... | [-0.03470435377823401, 0.17936905669332098, -0.11068707640036717, 0.09393036294775674, -0.017402460568737756, -0.10523383482654072, 0.018442020636594184, 0.2626257376285576, -0.17425124927812927, -0.33415663632552456, 0.021099961134369332, -0.33867771456701845, 0.03416250396189811, 0.1721326465942437, 0.023721466336069... |
710.3695 | Magnetic Field Distribution Due to Domain Walls in Unconventional
Superconductors | Steady-state properties of Bloch domain wall (DW) in superconducting
ferromagnet (SCFM) are studied. The distribution of magnetic field above and
below the surface of the SCFM due to the permanent magnetization supercurrent
flowing in the DW plane is calculated by solving Maxwell equations supplemented
by London equa... | cond-mat.supr-con | steadystate properties of bloch domain wall dw in superconducting ferromagnet scfm are studied the distribution of magnetic field above and below the surface of the scfm due to the permanent magnetization supercurrent flowing in the dw plane is calculated by solving maxwell equations supplemented by london equation it ... | [['steadystate', 'properties', 'of', 'bloch', 'domain', 'wall', 'dw', 'in', 'superconducting', 'ferromagnet', 'scfm', 'are', 'studied', 'the', 'distribution', 'of', 'magnetic', 'field', 'above', 'and', 'below', 'the', 'surface', 'of', 'the', 'scfm', 'due', 'to', 'the', 'permanent', 'magnetization', 'supercurrent', 'flo... | [-0.19699769983693075, 0.14682426069814122, -0.02427112704486047, 0.0004951661146294913, -0.07128946955413802, -0.05260953417194909, 0.02978350560327894, 0.3307391801456872, -0.26877084664363216, -0.3479642932450301, 0.05123072800128475, -0.27329125862666653, -0.03395370483815082, 0.2228164373897016, 0.0606543993136208... |
710.3696 | Optical Spectroscopy of Active Galactic Nuclei in SA57 | The cosmological evolution of X-ray-selected and optically selected Active
Galactic Nuclei (AGNs) show different behaviours interpreted in terms of two
different populations. The difference is evident mainly for low luminosity AGNs
(LLAGNs), many of which are lost by optical photometric surveys. We are
conducting a s... | astro-ph | the cosmological evolution of xrayselected and optically selected active galactic nuclei agns show different behaviours interpreted in terms of two different populations the difference is evident mainly for low luminosity agns llagns many of which are lost by optical photometric surveys we are conducting a spectroscopi... | [['the', 'cosmological', 'evolution', 'of', 'xrayselected', 'and', 'optically', 'selected', 'active', 'galactic', 'nuclei', 'agns', 'show', 'different', 'behaviours', 'interpreted', 'in', 'terms', 'of', 'two', 'different', 'populations', 'the', 'difference', 'is', 'evident', 'mainly', 'for', 'low', 'luminosity', 'agns'... | [-0.05200831558624351, 0.1047554486758869, -0.02445722854937668, 0.1828588650443298, -0.07678875533725929, -0.11850410589120454, 0.05402987224601761, 0.49029132395430847, -0.1327282811730617, -0.4017192815326982, 0.058326314318131796, -0.32726611387570975, 0.027347364035193566, 0.2115004951617232, -0.020530142217736552... |
710.3697 | Coupling a branching process to an infinite dimensional epidemic process | Branching process approximation to the initial stages of an epidemic process
has been used since the 1950's as a technique for providing stochastic
counterparts to deterministic epidemic threshold theorems. One way of
describing the approximation is to construct both branching and epidemic
processes on the same proba... | math.PR q-bio.PE | branching process approximation to the initial stages of an epidemic process has been used since the 1950s as a technique for providing stochastic counterparts to deterministic epidemic threshold theorems one way of describing the approximation is to construct both branching and epidemic processes on the same probabili... | [['branching', 'process', 'approximation', 'to', 'the', 'initial', 'stages', 'of', 'an', 'epidemic', 'process', 'has', 'been', 'used', 'since', 'the', '1950s', 'as', 'a', 'technique', 'for', 'providing', 'stochastic', 'counterparts', 'to', 'deterministic', 'epidemic', 'threshold', 'theorems', 'one', 'way', 'of', 'descr... | [-0.09205880288429784, 0.12713583331273498, -0.07816170777824491, 0.09073371780029235, -0.01783753199634528, -0.1390068178309711, 0.11060055886334128, 0.37083361111581326, -0.22386386110964748, -0.27577613952635516, 0.11984324602250274, -0.2627504161944745, -0.16240276334891943, 0.16656848693482879, -0.0564377943742926... |
710.3698 | Nature versus Nurture: The curved spine of the galaxy cluster X-ray
luminosity -- temperature relation | The physical processes that define the spine of the galaxy cluster X-ray
luminosity -- temperature (L-T) relation are investigated using a large
hydrodynamical simulation of the Universe. This simulation models the same
volume and phases as the Millennium Simulation and has a linear extent of 500
h^{-1} Mpc. We demon... | astro-ph | the physical processes that define the spine of the galaxy cluster xray luminosity temperature lt relation are investigated using a large hydrodynamical simulation of the universe this simulation models the same volume and phases as the millennium simulation and has a linear extent of 500 h1 mpc we demonstrate that mer... | [['the', 'physical', 'processes', 'that', 'define', 'the', 'spine', 'of', 'the', 'galaxy', 'cluster', 'xray', 'luminosity', 'temperature', 'lt', 'relation', 'are', 'investigated', 'using', 'a', 'large', 'hydrodynamical', 'simulation', 'of', 'the', 'universe', 'this', 'simulation', 'models', 'the', 'same', 'volume', 'an... | [-0.07235826075720113, 0.1280003745671979, -0.12200474694726013, 0.10643205664394098, -0.07815572992891133, -0.025338523141625855, 0.03894166991720715, 0.3930947713494774, -0.20905480714928773, -0.33588030922507484, 0.1002444410585754, -0.29618634023363627, -0.05429869640751609, 0.22303725520171047, 0.00524658932986240... |
710.3699 | Charge asymmetry for electron (positron)-proton elastic scattering at
large angle | Charge asymmetry in electron (positron) scattering arises from the
interference of the Born amplitude and the box-type amplitude corresponding to
two virtual photons exchange. It can be extracted from electron proton and
positron proton scattering experiments, in the same kinematical conditions.
Considering the virtu... | hep-ph | charge asymmetry in electron positron scattering arises from the interference of the born amplitude and the boxtype amplitude corresponding to two virtual photons exchange it can be extracted from electron proton and positron proton scattering experiments in the same kinematical conditions considering the virtual photo... | [['charge', 'asymmetry', 'in', 'electron', 'positron', 'scattering', 'arises', 'from', 'the', 'interference', 'of', 'the', 'born', 'amplitude', 'and', 'the', 'boxtype', 'amplitude', 'corresponding', 'to', 'two', 'virtual', 'photons', 'exchange', 'it', 'can', 'be', 'extracted', 'from', 'electron', 'proton', 'and', 'posi... | [-0.10628014192558252, 0.23353287640941114, -0.0714725474804604, 0.1654569733628215, -0.01754529946259796, -0.08536782473495874, 0.04134820044900362, 0.3308059301800453, -0.22592170408640344, -0.259992089195965, -0.04738729251011346, -0.33520843130178174, -0.0353724697461495, 0.14283473410536177, 0.09835744508040639, 0... |
710.37 | Nuclear matter in the chiral limit and the in-medium chiral condensate | We investigate nuclear matter, i.e. the nuclear equation-of-state (EOS) as
well as the relativistic mean fields in the chiral limit. The investigations
are based on a chiral nucleon-nucleon EFT interaction where the explicit and
implicit pion mass dependence is known up to next-to-leading order. The nuclear
bulk prop... | nucl-th | we investigate nuclear matter ie the nuclear equationofstate eos as well as the relativistic mean fields in the chiral limit the investigations are based on a chiral nucleonnucleon eft interaction where the explicit and implicit pion mass dependence is known up to nexttoleading order the nuclear bulk properties are fou... | [['we', 'investigate', 'nuclear', 'matter', 'ie', 'the', 'nuclear', 'equationofstate', 'eos', 'as', 'well', 'as', 'the', 'relativistic', 'mean', 'fields', 'in', 'the', 'chiral', 'limit', 'the', 'investigations', 'are', 'based', 'on', 'a', 'chiral', 'nucleonnucleon', 'eft', 'interaction', 'where', 'the', 'explicit', 'an... | [-0.09432303090988282, 0.18192793153585834, -0.13950350248303853, 0.14046473654799915, -0.07021784232194095, -0.04570831943368703, -0.012967298211725918, 0.3265227010604321, -0.17829400519922114, -0.2932883508895573, 0.007082802861348905, -0.27246606033377085, -0.04663782862725815, 0.10940434975680291, 0.08674010365747... |
710.3701 | Population trapping due to cavity losses | In population trapping the occupation of a decaying quantum level keeps a
constant non-zero value. We show that an atom-cavity system interacting with an
environment characterized by a non-flat spectrum, in the non-Markovian limit,
exhibits such a behavior, effectively realizing the preservation of
nonclassical state... | quant-ph | in population trapping the occupation of a decaying quantum level keeps a constant nonzero value we show that an atomcavity system interacting with an environment characterized by a nonflat spectrum in the nonmarkovian limit exhibits such a behavior effectively realizing the preservation of nonclassical states against ... | [['in', 'population', 'trapping', 'the', 'occupation', 'of', 'a', 'decaying', 'quantum', 'level', 'keeps', 'a', 'constant', 'nonzero', 'value', 'we', 'show', 'that', 'an', 'atomcavity', 'system', 'interacting', 'with', 'an', 'environment', 'characterized', 'by', 'a', 'nonflat', 'spectrum', 'in', 'the', 'nonmarkovian', ... | [-0.1845438190503046, 0.17256118227705883, -0.09607127647614107, 0.013790341190542676, 0.012778406427241863, -0.15509842664469034, 0.040118674567202105, 0.32651199266547337, -0.23838390854070896, -0.2771839309483767, -0.00475359297124669, -0.2721325329504907, -0.09942190286819823, 0.2283866064855829, -0.024377127864863... |
710.3702 | Monomial integrals on the classical groups | This paper presents a powerfull method to integrate general monomials on the
classical groups with respect to their invariant (Haar) measure. The method has
first been applied to the orthogonal group in [J. Math. Phys. 43, 3342 (2002)],
and is here used to obtain similar integration formulas for the unitary and the
u... | math-ph cond-mat.mes-hall math.MP math.RT | this paper presents a powerfull method to integrate general monomials on the classical groups with respect to their invariant haar measure the method has first been applied to the orthogonal group in j math phys 43 3342 2002 and is here used to obtain similar integration formulas for the unitary and the unitary symplec... | [['this', 'paper', 'presents', 'a', 'powerfull', 'method', 'to', 'integrate', 'general', 'monomials', 'on', 'the', 'classical', 'groups', 'with', 'respect', 'to', 'their', 'invariant', 'haar', 'measure', 'the', 'method', 'has', 'first', 'been', 'applied', 'to', 'the', 'orthogonal', 'group', 'in', 'j', 'math', 'phys', '... | [-0.09334386542520126, 0.06712835858950454, -0.10207282480835093, 0.0342269538348086, -0.10935034271050978, -0.11448191839690122, 0.012516282103757747, 0.3766993087107741, -0.2685041725360532, -0.28074810003328293, 0.11006826772189546, -0.24051638210467777, -0.13949471141585684, 0.20719527455934095, -0.0768810148135709... |
710.3703 | Spectral Properties and Linear Stability of Self-Similar Wave Maps | We study co--rotational wave maps from $(3+1)$--Minkowski space to the
three--sphere $S^3$. It is known that there exists a countable family $\{f_n\}$
of self--similar solutions. We investigate their stability under linear
perturbations by operator theoretic methods. To this end we study the spectra
of the perturbati... | math-ph gr-qc math.AP math.MP | we study corotational wave maps from 31minkowski space to the threesphere s3 it is known that there exists a countable family f_n of selfsimilar solutions we investigate their stability under linear perturbations by operator theoretic methods to this end we study the spectra of the perturbation operators prove wellpose... | [['we', 'study', 'corotational', 'wave', 'maps', 'from', '31minkowski', 'space', 'to', 'the', 'threesphere', 's3', 'it', 'is', 'known', 'that', 'there', 'exists', 'a', 'countable', 'family', 'f_n', 'of', 'selfsimilar', 'solutions', 'we', 'investigate', 'their', 'stability', 'under', 'linear', 'perturbations', 'by', 'op... | [-0.16180439675344696, 0.0805355192418505, -0.09581907502599532, 0.09088496489102563, -0.049107770880542786, -0.07824348861092253, 0.0028989631918412222, 0.3003154443164321, -0.319968996710981, -0.17667409822439092, 0.17982237263806636, -0.33595330165581233, -0.18138239169095444, 0.14146452279329666, -0.047633847920224... |
710.3704 | The red and blue galaxy populations in the GOODS field: evidence for an
excess of red dwarfs | We study the evolution of the galaxy population up to z\sim3 as a function of
its colour properties. In particular, luminosity functions and luminosity
densities have been derived as a function of redshift for the blue/late and
red/early populations. We use data from the GOODS-MUSIC catalogue which have
typical magni... | astro-ph | we study the evolution of the galaxy population up to zsim3 as a function of its colour properties in particular luminosity functions and luminosity densities have been derived as a function of redshift for the bluelate and redearly populations we use data from the goodsmusic catalogue which have typical magnitude limi... | [['we', 'study', 'the', 'evolution', 'of', 'the', 'galaxy', 'population', 'up', 'to', 'zsim3', 'as', 'a', 'function', 'of', 'its', 'colour', 'properties', 'in', 'particular', 'luminosity', 'functions', 'and', 'luminosity', 'densities', 'have', 'been', 'derived', 'as', 'a', 'function', 'of', 'redshift', 'for', 'the', 'b... | [0.0010733633642259718, 0.06781395206013544, -0.09635743067946298, 0.1198244321036054, -0.05990742440192417, -0.025893858150792, 0.05982584766836983, 0.49358291917960495, -0.1233589540258743, -0.3750270431479455, 0.02914761254641803, -0.3142131405180072, -0.015070131748641361, 0.17219133420891855, -0.02910651063146038,... |
710.3705 | Flavour symmetries and SUSY soft breaking in the LHC era | The so-called supersymmetric flavour problem does not exist in isolation to
the Standard Model flavour problem. We show that a realistic flavour symmetry
can simultaneously solve both problems without ad hoc modifications of the SUSY
model. Furthermore, departures from the SM expectations in these models can be
used ... | hep-ph | the socalled supersymmetric flavour problem does not exist in isolation to the standard model flavour problem we show that a realistic flavour symmetry can simultaneously solve both problems without ad hoc modifications of the susy model furthermore departures from the sm expectations in these models can be used to dis... | [['the', 'socalled', 'supersymmetric', 'flavour', 'problem', 'does', 'not', 'exist', 'in', 'isolation', 'to', 'the', 'standard', 'model', 'flavour', 'problem', 'we', 'show', 'that', 'a', 'realistic', 'flavour', 'symmetry', 'can', 'simultaneously', 'solve', 'both', 'problems', 'without', 'ad', 'hoc', 'modifications', 'o... | [-0.054951617022355397, 0.15859545194854338, -0.02077336434274912, 0.18478994955619177, -0.10117709467808406, -0.2165053876551489, 0.05375897515254716, 0.3456189256285628, -0.27097533614064256, -0.33754484201471013, 0.048846517987549305, -0.2460644784010947, -0.07665398125847181, 0.1179387815700223, -0.0385481549551089... |
710.3706 | The Magellanic Clouds as a template for the study of stellar populations
and galaxy interactions | The Magellanic System represents one of the best places to study the
formation and evolution of galaxies. Photometric surveys of various depths,
areas and wavelengths have had a significant impact on our understanding of the
system; however, a complete picture is still lacking. VMC (the VISTA
near-infrared YJKs surve... | astro-ph | the magellanic system represents one of the best places to study the formation and evolution of galaxies photometric surveys of various depths areas and wavelengths have had a significant impact on our understanding of the system however a complete picture is still lacking vmc the vista nearinfrared yjks survey of the ... | [['the', 'magellanic', 'system', 'represents', 'one', 'of', 'the', 'best', 'places', 'to', 'study', 'the', 'formation', 'and', 'evolution', 'of', 'galaxies', 'photometric', 'surveys', 'of', 'various', 'depths', 'areas', 'and', 'wavelengths', 'have', 'had', 'a', 'significant', 'impact', 'on', 'our', 'understanding', 'of... | [-0.11919063721213816, 0.009362752012624768, -0.13508422641101683, 0.04138696038738363, -0.1199073174118417, -0.04932214519985526, 0.06293934400112015, 0.3544173617169116, -0.24642525134761864, -0.34126670265714953, 0.10842046776766102, -0.2908550896501006, -0.0676877431987414, 0.24296956500366276, -0.05012182420282399... |
710.3707 | Intrinsic avalanches and collective phenomena in a Mn(II)-free radical
ferrimagnetic chain | Magnetic hysteresis loops below 300 mK on single crystals of the Mn(II) -
nitronyl nitroxide free radical chain (Mn(hfac)_2({\it R})-3MLNN) present
abrupt reversals of the magnetization, or avalanches. We show that, below 200
mK, the avalanches occur at a constant field, independent of the sample and so
propose that ... | cond-mat.mtrl-sci cond-mat.other | magnetic hysteresis loops below 300 mk on single crystals of the mnii nitronyl nitroxide free radical chain mnhfac_2it r3mlnn present abrupt reversals of the magnetization or avalanches we show that below 200 mk the avalanches occur at a constant field independent of the sample and so propose that this avalanche field ... | [['magnetic', 'hysteresis', 'loops', 'below', '300', 'mk', 'on', 'single', 'crystals', 'of', 'the', 'mnii', 'nitronyl', 'nitroxide', 'free', 'radical', 'chain', 'mnhfac_2it', 'r3mlnn', 'present', 'abrupt', 'reversals', 'of', 'the', 'magnetization', 'or', 'avalanches', 'we', 'show', 'that', 'below', '200', 'mk', 'the', ... | [-0.1667627775448967, 0.27492965997358126, -0.020252247844738037, 0.051556127286643126, -0.01781534194438295, -0.11373928021216258, 0.06131724031769078, 0.4184092579240149, -0.2710055935111913, -0.291607979668135, 0.04032562415814027, -0.29154743892564017, -0.07281497412318871, 0.17394684476735578, 0.027050253249366173... |
710.3708 | What we have learned so far from 3-fluid hydrodynamics | Available data on heavy-ion collisions at AGS and SPS energies are analyzed
using a 3-fluid dynamical model within a purely hadronic scenario. We
investigate the problems met in reproducing these data within this scheme. In
particular, we try to indicate those data which could point towards the
occurrence of a phase ... | nucl-th hep-ph | available data on heavyion collisions at ags and sps energies are analyzed using a 3fluid dynamical model within a purely hadronic scenario we investigate the problems met in reproducing these data within this scheme in particular we try to indicate those data which could point towards the occurrence of a phase transit... | [['available', 'data', 'on', 'heavyion', 'collisions', 'at', 'ags', 'and', 'sps', 'energies', 'are', 'analyzed', 'using', 'a', '3fluid', 'dynamical', 'model', 'within', 'a', 'purely', 'hadronic', 'scenario', 'we', 'investigate', 'the', 'problems', 'met', 'in', 'reproducing', 'these', 'data', 'within', 'this', 'scheme',... | [-0.09935225629602122, 0.18205745784829544, -0.15356466676050848, 0.10696981396769231, 0.0072357386043624934, -0.08143917532674803, 0.02470110803512873, 0.36974827683967565, -0.21857252911112346, -0.2656769488600239, 0.057427073154079245, -0.28522278108856586, -0.048682280280421264, 0.13520474160353826, 0.0337521623520... |
710.3709 | On measuring standards in Weyl's geometry | In Weyl's geometry the nonintegrability problem and difficulties in defining
measuring standards are reconsidered. Approaches removing the nonintegrability
of lengthin in the interior of atoms are given, so that atoms may serve as
measuring standards. The Weyl space become a well founded framework for
classical theor... | gr-qc | in weyls geometry the nonintegrability problem and difficulties in defining measuring standards are reconsidered approaches removing the nonintegrability of lengthin in the interior of atoms are given so that atoms may serve as measuring standards the weyl space become a well founded framework for classical theories of... | [['in', 'weyls', 'geometry', 'the', 'nonintegrability', 'problem', 'and', 'difficulties', 'in', 'defining', 'measuring', 'standards', 'are', 'reconsidered', 'approaches', 'removing', 'the', 'nonintegrability', 'of', 'lengthin', 'in', 'the', 'interior', 'of', 'atoms', 'are', 'given', 'so', 'that', 'atoms', 'may', 'serve... | [-0.13475240334868432, 0.1369071177393198, -0.08319394174963236, 0.1080646426603198, -0.10447260648477823, -0.18811593822203576, 0.013558619115501642, 0.2704011841863394, -0.2632088804244995, -0.2839786861091852, 0.06612133144866675, -0.28067066034302113, -0.1369938956014812, 0.1914904522895813, -0.11978382160887122, 0... |
710.371 | Some forgotten features of the Bose Einstein Correlations | Notwithstanding the visible maturity of the subject of Bose-Einstein
Correlations (BEC), as witnessed nowadays, we would like to bring to ones
attention two points, which apparently did not received attention they deserve:
the problem of the choice of the form of $C_2(Q)$ correlation function when
effects of partial ... | hep-ph nucl-th | notwithstanding the visible maturity of the subject of boseeinstein correlations bec as witnessed nowadays we would like to bring to ones attention two points which apparently did not received attention they deserve the problem of the choice of the form of c_2q correlation function when effects of partial coherence of ... | [['notwithstanding', 'the', 'visible', 'maturity', 'of', 'the', 'subject', 'of', 'boseeinstein', 'correlations', 'bec', 'as', 'witnessed', 'nowadays', 'we', 'would', 'like', 'to', 'bring', 'to', 'ones', 'attention', 'two', 'points', 'which', 'apparently', 'did', 'not', 'received', 'attention', 'they', 'deserve', 'the',... | [-0.12175546479537278, 0.1167487983176535, -0.09385600476525724, 0.08930596593465354, -0.08510999585426338, -0.11953399448680717, 0.04795206021014098, 0.3704740681962387, -0.24062845669686794, -0.26530878077814907, 0.07942953540761075, -0.3155128699853211, -0.09904345025534968, 0.1935187259852584, -0.011930919050968982... |
710.3711 | Rational subsets of polycyclic monoids and valence automata | We study the classes of languages defined by valence automata with rational
target sets (or equivalently, regular valence grammars with rational target
sets), where the valence monoid is drawn from the important class of polycyclic
monoids. We show that for polycyclic monoids of rank 2 or more, such automata
accept e... | math.RA | we study the classes of languages defined by valence automata with rational target sets or equivalently regular valence grammars with rational target sets where the valence monoid is drawn from the important class of polycyclic monoids we show that for polycyclic monoids of rank 2 or more such automata accept exactly t... | [['we', 'study', 'the', 'classes', 'of', 'languages', 'defined', 'by', 'valence', 'automata', 'with', 'rational', 'target', 'sets', 'or', 'equivalently', 'regular', 'valence', 'grammars', 'with', 'rational', 'target', 'sets', 'where', 'the', 'valence', 'monoid', 'is', 'drawn', 'from', 'the', 'important', 'class', 'of',... | [-0.08453475264362961, 0.10391009432233629, 0.017510246314604076, 0.12058409818564542, -0.09813501036560704, -0.1504323158428193, 0.09417728436810355, 0.3862554473021338, -0.42239919586122154, -0.18893805146968412, 0.05792315055864052, -0.32457370259949275, -0.06086481586774631, 0.17367859060815985, -0.1013757853520914... |
710.3712 | The Milky Way's Kiloparsec Scale Wind: A Hybrid Cosmic-Ray and Thermally
Driven Outflow | We apply a wind model, driven by combined cosmic-ray and thermal-gas
pressure, to the Milky Way, and show that the observed Galactic diffuse soft
X-ray emission can be better explained by a wind than by previous static gas
models. We find that cosmic-ray pressure is essential to driving the observed
wind. Having thus... | astro-ph | we apply a wind model driven by combined cosmicray and thermalgas pressure to the milky way and show that the observed galactic diffuse soft xray emission can be better explained by a wind than by previous static gas models we find that cosmicray pressure is essential to driving the observed wind having thus defined a ... | [['we', 'apply', 'a', 'wind', 'model', 'driven', 'by', 'combined', 'cosmicray', 'and', 'thermalgas', 'pressure', 'to', 'the', 'milky', 'way', 'and', 'show', 'that', 'the', 'observed', 'galactic', 'diffuse', 'soft', 'xray', 'emission', 'can', 'be', 'better', 'explained', 'by', 'a', 'wind', 'than', 'by', 'previous', 'sta... | [-0.07914109641826465, 0.16307202594436923, -0.07513569059836514, 0.14364981957752368, -0.08244678766470101, -0.0352823823761676, 0.029630219325875205, 0.42534805768552947, -0.2605444681145908, -0.3502150824026424, -0.012244958756662741, -0.26798116475316314, -0.06248101867009502, 0.23025888433125252, -0.01997916949296... |
710.3713 | Quasi-gaussian velocity distribution of a vibrated granular bilayer
system | We show by using a Discrete Element Method that a bilayer of vibrated
granular bidisperse spheres exhibits the striking feature that the horizontal
velocity distribution of the top layer particles has a quasi-Gaussian shape,
whereas that of the bottom layer is far from Gaussian. We examine in detail the
relevance of ... | cond-mat.soft | we show by using a discrete element method that a bilayer of vibrated granular bidisperse spheres exhibits the striking feature that the horizontal velocity distribution of the top layer particles has a quasigaussian shape whereas that of the bottom layer is far from gaussian we examine in detail the relevance of all p... | [['we', 'show', 'by', 'using', 'a', 'discrete', 'element', 'method', 'that', 'a', 'bilayer', 'of', 'vibrated', 'granular', 'bidisperse', 'spheres', 'exhibits', 'the', 'striking', 'feature', 'that', 'the', 'horizontal', 'velocity', 'distribution', 'of', 'the', 'top', 'layer', 'particles', 'has', 'a', 'quasigaussian', 's... | [-0.10622817567782476, 0.16078883081208914, -0.1385304321302101, 0.013549546893045772, -0.013405214168597013, -0.10434917914681137, 0.05884818077320233, 0.3720477258320898, -0.2725258949911222, -0.2739690599264577, 0.03635315186547814, -0.2768288310035132, -0.13453632983728311, 0.13429661424597725, 0.01412423028377816,... |
710.3714 | Updated Constraints from B Physics on the MSSM and the NMSSM | We update constraints from B physics observables on the parameters of the
MSSM and the NMSSM, combining them with LEP constraints. Presently available SM
and Susy radiative corrections are included in the calculations, which will be
made public in the form of a Fortran code. Results for the tan(beta) and
M_{H^+} depe... | hep-ph | we update constraints from b physics observables on the parameters of the mssm and the nmssm combining them with lep constraints presently available sm and susy radiative corrections are included in the calculations which will be made public in the form of a fortran code results for the tanbeta and m_h dependence of b ... | [['we', 'update', 'constraints', 'from', 'b', 'physics', 'observables', 'on', 'the', 'parameters', 'of', 'the', 'mssm', 'and', 'the', 'nmssm', 'combining', 'them', 'with', 'lep', 'constraints', 'presently', 'available', 'sm', 'and', 'susy', 'radiative', 'corrections', 'are', 'included', 'in', 'the', 'calculations', 'wh... | [-0.09746575545048922, 0.1886800200758522, -0.025171808347666778, 0.15259400710478546, -0.12951659520346953, -0.2132230279166051, 0.08355959673081675, 0.3391048557936184, -0.2130750703164727, -0.31524293733540404, 0.06246263815981326, -0.2657493461043604, -0.0033234990332075345, 0.18768010234775684, 0.03258035118661581... |
710.3715 | A fretting crack initiation prediction taking into account the surface
roughness and the crack nucleation process volume | This paper presents an experimental study of the fretting crack nucleation
threshold, expressed in terms of loading conditions, with a cylinder/plane
contact. The studied material is a damage tolerant aluminium alloy widely used
in the aerospace application. Since in industrial problems, the surface quality
is often ... | cond-mat.mtrl-sci | this paper presents an experimental study of the fretting crack nucleation threshold expressed in terms of loading conditions with a cylinderplane contact the studied material is a damage tolerant aluminium alloy widely used in the aerospace application since in industrial problems the surface quality is often variable... | [['this', 'paper', 'presents', 'an', 'experimental', 'study', 'of', 'the', 'fretting', 'crack', 'nucleation', 'threshold', 'expressed', 'in', 'terms', 'of', 'loading', 'conditions', 'with', 'a', 'cylinderplane', 'contact', 'the', 'studied', 'material', 'is', 'a', 'damage', 'tolerant', 'aluminium', 'alloy', 'widely', 'u... | [-0.11433095963050922, 0.15165107097564032, -0.09172783500980586, 0.003487225085652123, -0.024921023035421968, -0.09466518555457393, 0.012190192268074801, 0.35179353897770244, -0.24975989426175754, -0.2950495949884256, 0.10466453197412193, -0.22387822774549326, -0.18680372337500253, 0.19471934778615832, -0.073047151286... |
710.3716 | The interplay between hydrodynamic and Brownian fluctuations in
sedimenting colloidal suspensions | We apply a hybrid Molecular Dynamics and mesoscopic simulation technique to
study the steady-state sedimentation of hard sphere particles for Peclet
numbers (Pe) ranging from 0.08 to 12. Hydrodynamic back-flow causes a reduction
of the average sedimentation velocity relative to the Stokes velocity. We find
that this ... | cond-mat.soft | we apply a hybrid molecular dynamics and mesoscopic simulation technique to study the steadystate sedimentation of hard sphere particles for peclet numbers pe ranging from 008 to 12 hydrodynamic backflow causes a reduction of the average sedimentation velocity relative to the stokes velocity we find that this effect is... | [['we', 'apply', 'a', 'hybrid', 'molecular', 'dynamics', 'and', 'mesoscopic', 'simulation', 'technique', 'to', 'study', 'the', 'steadystate', 'sedimentation', 'of', 'hard', 'sphere', 'particles', 'for', 'peclet', 'numbers', 'pe', 'ranging', 'from', '008', 'to', '12', 'hydrodynamic', 'backflow', 'causes', 'a', 'reductio... | [-0.16137976149519814, 0.25426915721928184, -0.1229702728925973, 0.0596307781072918, 0.021117830114003193, -0.07864540900559501, -0.014815377170576694, 0.31383688591671643, -0.2754764790574076, -0.30483466138112103, 0.03665949712368719, -0.2959330251493247, -0.0823623323350722, 0.20349096162707037, -0.00292664498143585... |
710.3717 | A calculation of the bulk viscosity in SU(3) gluodynamics | We perform a lattice Monte-Carlo calculation of the trace-anomaly two-point
function at finite temperature in the SU(3) gauge theory. We obtain the
long-distance properties of the correlator in the continuum limit and extract
the bulk viscosity zeta via a Kubo formula. Unlike the tensor correlator
relevant to the she... | hep-lat hep-ph nucl-th | we perform a lattice montecarlo calculation of the traceanomaly twopoint function at finite temperature in the su3 gauge theory we obtain the longdistance properties of the correlator in the continuum limit and extract the bulk viscosity zeta via a kubo formula unlike the tensor correlator relevant to the shear viscosi... | [['we', 'perform', 'a', 'lattice', 'montecarlo', 'calculation', 'of', 'the', 'traceanomaly', 'twopoint', 'function', 'at', 'finite', 'temperature', 'in', 'the', 'su3', 'gauge', 'theory', 'we', 'obtain', 'the', 'longdistance', 'properties', 'of', 'the', 'correlator', 'in', 'the', 'continuum', 'limit', 'and', 'extract', ... | [-0.1478634639095296, 0.21603960496209124, -0.13080499657046268, 0.04180689701837871, -0.015358760153107784, -0.1134831196792862, 0.06337541386567275, 0.3055846246945507, -0.23168854712344267, -0.19818986622507082, 0.061507876581676744, -0.3408293380552684, -0.06528698403990882, 0.14300685552880169, 0.10158862200401285... |
710.3718 | Weighted Sequences in Finite Cyclic Groups | Let $p>7$ be a prime, let $G=\Z/p\Z$, and let $S_1=\prod_{i=1}^p g_i$ and
$S_2=\prod_{i=1}^p h_i$ be two sequences with terms from $G$. Suppose that the
maximum multiplicity of a term from either $S_1$ or $S_2$ is at most
$\frac{2p+1}{5}$. Then we show that, for each $g\in G$, there exists a
permutation $\sigma$ of $... | math.CO math.NT | let p7 be a prime let gzpz and let s_1prod_i1p g_i and s_2prod_i1p h_i be two sequences with terms from g suppose that the maximum multiplicity of a term from either s_1 or s_2 is at most frac2p15 then we show that for each gin g there exists a permutation sigma of 12 p such that gsum_i1pg_icdot h_sigmai the question i... | [['let', 'p7', 'be', 'a', 'prime', 'let', 'gzpz', 'and', 'let', 's_1prod_i1p', 'g_i', 'and', 's_2prod_i1p', 'h_i', 'be', 'two', 'sequences', 'with', 'terms', 'from', 'g', 'suppose', 'that', 'the', 'maximum', 'multiplicity', 'of', 'a', 'term', 'from', 'either', 's_1', 'or', 's_2', 'is', 'at', 'most', 'frac2p15', 'then',... | [-0.16644716326346887, 0.17988927091604898, -0.09326423157139548, -0.009474620944820345, -0.018258603595729384, -0.187358447031251, -0.002520775449063097, 0.33444254635167975, -0.3327545873637843, -0.22909038831878986, 0.08987103288860193, -0.3540818455462743, -0.08508295048626938, 0.1849188761752365, -0.09051564432946... |
710.3719 | A Neutrino Mass Matrix with Vanishing $\mu$--$\mu$ and $\tau$--$\tau$
Entries | We revisit our earlier proposal for the form of the neutrino mass matrix: a
two-zero ansatz wherein the CP-violating PMNS phase $\delta$ plays a
surprisingly important role. We review its observable consequences and show how
our ansatz follows from a softly-broken symmetry (muon number minus tau lepton
number) in a s... | hep-ph | we revisit our earlier proposal for the form of the neutrino mass matrix a twozero ansatz wherein the cpviolating pmns phase delta plays a surprisingly important role we review its observable consequences and show how our ansatz follows from a softlybroken symmetry muon number minus tau lepton number in a seesaw model ... | [['we', 'revisit', 'our', 'earlier', 'proposal', 'for', 'the', 'form', 'of', 'the', 'neutrino', 'mass', 'matrix', 'a', 'twozero', 'ansatz', 'wherein', 'the', 'cpviolating', 'pmns', 'phase', 'delta', 'plays', 'a', 'surprisingly', 'important', 'role', 'we', 'review', 'its', 'observable', 'consequences', 'and', 'show', 'h... | [-0.12940389852571701, 0.24745756960224494, -0.04102044646528417, 0.15935838651577278, -0.09593698289245367, -0.20330566250985221, 0.06865049679098385, 0.2818287655578128, -0.16539175889088906, -0.3043232968276633, 0.02105228956913509, -0.2575776635868741, -0.14042723521457187, 0.08997416327890408, 0.06015353267347174,... |
710.372 | Operational determination of multi-qubit entanglement classes via tuning
of local operations | We present a physical setup with which it is possible to produce arbitrary
symmetric long-lived multiqubit entangled states in the internal ground levels
of photon emitters, including the paradigmatic GHZ and W states. In the case of
three emitters, where each tripartite entangled state belongs to one of two
well-def... | quant-ph | we present a physical setup with which it is possible to produce arbitrary symmetric longlived multiqubit entangled states in the internal ground levels of photon emitters including the paradigmatic ghz and w states in the case of three emitters where each tripartite entangled state belongs to one of two welldefined en... | [['we', 'present', 'a', 'physical', 'setup', 'with', 'which', 'it', 'is', 'possible', 'to', 'produce', 'arbitrary', 'symmetric', 'longlived', 'multiqubit', 'entangled', 'states', 'in', 'the', 'internal', 'ground', 'levels', 'of', 'photon', 'emitters', 'including', 'the', 'paradigmatic', 'ghz', 'and', 'w', 'states', 'in... | [-0.16193538012693784, 0.25139007573383615, -0.012869993022544995, 0.0338129763028854, 0.027640214857743366, -0.2637253118262283, 0.04242539262141738, 0.428014182534657, -0.2180376364604423, -0.2632475277396703, -0.01024578341074582, -0.2530814607529656, -0.04443411652219335, 0.16547583180822825, 0.028059002675275366, ... |
710.3721 | Electronic correlations in graphite and carbon nanotubes from Auger
spectroscopy | We have determined the screened on-site Coulomb repulsion in graphite and
single wall carbon nanotubes by measuring their Auger spectra and performing a
new theoretical analysis based on an extended Cini-Sawatzky approach where only
one fit parameter is employed. The experimental lineshape is very well
reproduced by ... | cond-mat.str-el cond-mat.mes-hall | we have determined the screened onsite coulomb repulsion in graphite and single wall carbon nanotubes by measuring their auger spectra and performing a new theoretical analysis based on an extended cinisawatzky approach where only one fit parameter is employed the experimental lineshape is very well reproduced by the t... | [['we', 'have', 'determined', 'the', 'screened', 'onsite', 'coulomb', 'repulsion', 'in', 'graphite', 'and', 'single', 'wall', 'carbon', 'nanotubes', 'by', 'measuring', 'their', 'auger', 'spectra', 'and', 'performing', 'a', 'new', 'theoretical', 'analysis', 'based', 'on', 'an', 'extended', 'cinisawatzky', 'approach', 'w... | [-0.04586634332580226, 0.15473389567357645, -0.03649987021440661, 0.056439692250473406, 0.028548324314345206, -0.202056358849814, 0.08317179059236218, 0.43917081582840983, -0.23029910897897496, -0.3563750536682514, -0.003890457781860707, -0.30949910486818694, -0.07132640558775964, 0.13716096110682893, 0.032503082734215... |
710.3722 | Ganea and Whitehead definitions for the tangential
Lusternik-Schnirelmann category of foliations | This work solves the problem of elaborating Ganea and Whitehead definitions
for the tangential category of a foliated manifold. We develop these two
notions in the category $\Tops$ of stratified spaces, that are topological
spaces $X$ endowed with a partition $\cF$ and compare them to a third invariant
defined by usi... | math.AT | this work solves the problem of elaborating ganea and whitehead definitions for the tangential category of a foliated manifold we develop these two notions in the category tops of stratified spaces that are topological spaces x endowed with a partition cf and compare them to a third invariant defined by using open sets... | [['this', 'work', 'solves', 'the', 'problem', 'of', 'elaborating', 'ganea', 'and', 'whitehead', 'definitions', 'for', 'the', 'tangential', 'category', 'of', 'a', 'foliated', 'manifold', 'we', 'develop', 'these', 'two', 'notions', 'in', 'the', 'category', 'tops', 'of', 'stratified', 'spaces', 'that', 'are', 'topological... | [-0.1542267325250255, 0.12705411339892278, -0.05580430722182404, 0.07341407554200556, -0.07864115199757905, -0.1380543208244858, 0.01767163925002553, 0.37271843704430363, -0.30575088379813264, -0.21223234932846094, 0.080817663409199, -0.2725832185861242, -0.09254426625557244, 0.17036044120949198, -0.1326026594932368, -... |
710.3723 | Continuous first order orbital order-disorder transition in Nd1-xCaxMnO3 | The nature of the cooperative Jahn-Teller (JT) transition accompanied by
orbital order-disorder in Nd1-xCaxMnO3 has been studied by high temperature
(300 - 1200K) synchrotron and laboratory X-ray powder diffraction in the low
doping region (0<x<0.1). For very low doping a large temperature range of phase
coexistence ... | cond-mat.mtrl-sci | the nature of the cooperative jahnteller jt transition accompanied by orbital orderdisorder in nd1xcaxmno3 has been studied by high temperature 300 1200k synchrotron and laboratory xray powder diffraction in the low doping region 0x01 for very low doping a large temperature range of phase coexistence associated with a ... | [['the', 'nature', 'of', 'the', 'cooperative', 'jahnteller', 'jt', 'transition', 'accompanied', 'by', 'orbital', 'orderdisorder', 'in', 'nd1xcaxmno3', 'has', 'been', 'studied', 'by', 'high', 'temperature', '300', '1200k', 'synchrotron', 'and', 'laboratory', 'xray', 'powder', 'diffraction', 'in', 'the', 'low', 'doping',... | [-0.16699781696442315, 0.2814204088181898, -0.04263564543197713, 0.002754598081121922, -0.025398325470466446, -0.1115511837815966, 0.14880248420541325, 0.38537764324936813, -0.2446115612583135, -0.2854615682235328, 0.05999333822789291, -0.30394414553959526, -0.06455831277754999, 0.10918399371126647, 0.04918841917226742... |
710.3724 | Comment on "A Lagrangian for DSR Particle and the Role of
Noncommutativity" | In this work, we comment on two special points in the paper by S. Ghosh
[Phys. Rev. D 74, 084019 (2006)]. First of all, the Lagrangian presented by the
author does not describe the Magueijo- Smolin model of Doubly Special
Relativity since it is equivalent to the Lagrangian of the standard free
relativistic particle. ... | hep-th gr-qc | in this work we comment on two special points in the paper by s ghosh phys rev d 74 084019 2006 first of all the lagrangian presented by the author does not describe the magueijo smolin model of doubly special relativity since it is equivalent to the lagrangian of the standard free relativistic particle we also show th... | [['in', 'this', 'work', 'we', 'comment', 'on', 'two', 'special', 'points', 'in', 'the', 'paper', 'by', 's', 'ghosh', 'phys', 'rev', 'd', '74', '084019', '2006', 'first', 'of', 'all', 'the', 'lagrangian', 'presented', 'by', 'the', 'author', 'does', 'not', 'describe', 'the', 'magueijo', 'smolin', 'model', 'of', 'doubly',... | [-0.09182010796959386, 0.10391970671008567, -0.04831388288152379, 0.03135476615814794, -0.09186871826170466, -0.13198403412526524, 0.00839122140786384, 0.28979406008068975, -0.17992166126606282, -0.296009916440911, 0.0007937270943452982, -0.22490510334436958, -0.2061230742901161, 0.16109946446738685, -0.147729983226068... |
710.3725 | Single-electron quantum dot in Si/SiGe with integrated charge-sensing | Single-electron occupation is an essential component to measurement and
manipulation of spin in quantum dots, capabilities that are important for
quantum information processing. Si/SiGe is of interest for semiconductor spin
qubits, but single-electron quantum dots have not yet been achieved in this
system. We report ... | cond-mat.mes-hall | singleelectron occupation is an essential component to measurement and manipulation of spin in quantum dots capabilities that are important for quantum information processing sisige is of interest for semiconductor spin qubits but singleelectron quantum dots have not yet been achieved in this system we report the fabri... | [['singleelectron', 'occupation', 'is', 'an', 'essential', 'component', 'to', 'measurement', 'and', 'manipulation', 'of', 'spin', 'in', 'quantum', 'dots', 'capabilities', 'that', 'are', 'important', 'for', 'quantum', 'information', 'processing', 'sisige', 'is', 'of', 'interest', 'for', 'semiconductor', 'spin', 'qubits'... | [-0.15086507685128195, 0.18466843585717826, -0.017147157736041623, -0.02320003123579385, 0.07326439835900522, -0.2651008067136306, 0.04478502018458169, 0.428627404667761, -0.2337245208454197, -0.2842054060741287, -0.006054390879833828, -0.3307023079579939, -0.10223140808470223, 0.287864462978652, -0.035327079250355775,... |
710.3726 | Linkages in Polytope Graphs | A graph is k-linked if any k disjoint vertex-pairs can be joined by k
disjoint paths. We improve a lower bound on the linkedness of polytopes
slightly, which results in exact values for the minimal linkedness of 7-, 10-
and 13-dimensional polytopes.
We analyze in detail linkedness of polytopes on at most (6d+7)/5 v... | math.CO | a graph is klinked if any k disjoint vertexpairs can be joined by k disjoint paths we improve a lower bound on the linkedness of polytopes slightly which results in exact values for the minimal linkedness of 7 10 and 13dimensional polytopes we analyze in detail linkedness of polytopes on at most 6d75 vertices in that c... | [['a', 'graph', 'is', 'klinked', 'if', 'any', 'k', 'disjoint', 'vertexpairs', 'can', 'be', 'joined', 'by', 'k', 'disjoint', 'paths', 'we', 'improve', 'a', 'lower', 'bound', 'on', 'the', 'linkedness', 'of', 'polytopes', 'slightly', 'which', 'results', 'in', 'exact', 'values', 'for', 'the', 'minimal', 'linkedness', 'of',... | [-0.13668293465871545, 0.14357713325426164, -0.013253416746809351, 0.0674270917789261, -0.06050624175951248, -0.15368873731619337, 0.0863649785609507, 0.32338079229769545, -0.19801271420182298, -0.32455018556267934, 0.13461290284985586, -0.3560469324541528, -0.12928877393828658, 0.2153134396208859, -0.13195361508192813... |
710.3727 | A universal GRB photon energy-peak luminosity relation | The energetics and emission mechanism of GRBs are not well understood. Here
we demonstrate that the instantaneous peak flux or equivalent isotropic peak
luminosity, L_iso ergs s^-1, rather than the integrated fluence or equivalent
isotropic energy, E_iso ergs, underpins the known high-energy correlations.
Using new s... | astro-ph | the energetics and emission mechanism of grbs are not well understood here we demonstrate that the instantaneous peak flux or equivalent isotropic peak luminosity l_iso ergs s1 rather than the integrated fluence or equivalent isotropic energy e_iso ergs underpins the known highenergy correlations using new spectraltemp... | [['the', 'energetics', 'and', 'emission', 'mechanism', 'of', 'grbs', 'are', 'not', 'well', 'understood', 'here', 'we', 'demonstrate', 'that', 'the', 'instantaneous', 'peak', 'flux', 'or', 'equivalent', 'isotropic', 'peak', 'luminosity', 'l_iso', 'ergs', 's1', 'rather', 'than', 'the', 'integrated', 'fluence', 'or', 'equ... | [-0.06045655587293495, 0.1471783819163034, -0.06606018281816559, 0.2290658292964339, -0.11291903187791535, -0.11304589438111369, 0.040278528431287645, 0.4846748089374498, -0.20792390933790958, -0.32296165621969414, 0.0014881343217999783, -0.3112218543808626, -0.006590843931663521, 0.25042753370287885, 0.027676149077854... |
710.3728 | L1Packv2: A Mathematica package for minimizing an $\ell_1$-penalized
functional | L1Packv2 is a Mathematica package that contains a number of algorithms that
can be used for the minimization of an $\ell_1$-penalized least squares
functional. The algorithms can handle a mix of penalized and unpenalized
variables. Several instructive examples are given. Also, an implementation that
yields an exact o... | math.NA | l1packv2 is a mathematica package that contains a number of algorithms that can be used for the minimization of an ell_1penalized least squares functional the algorithms can handle a mix of penalized and unpenalized variables several instructive examples are given also an implementation that yields an exact output when... | [['l1packv2', 'is', 'a', 'mathematica', 'package', 'that', 'contains', 'a', 'number', 'of', 'algorithms', 'that', 'can', 'be', 'used', 'for', 'the', 'minimization', 'of', 'an', 'ell_1penalized', 'least', 'squares', 'functional', 'the', 'algorithms', 'can', 'handle', 'a', 'mix', 'of', 'penalized', 'and', 'unpenalized', ... | [-0.09391186934792334, 0.01679268458839808, -0.11623241252231377, 0.12240523712588819, -0.11472465613580964, -0.19674501986311818, -0.045558633041326645, 0.41034948736153265, -0.26125664903816803, -0.3008529732555703, 0.15423100762483147, -0.2961921636791279, -0.17364094039011332, 0.26562067417910806, -0.11337767581075... |
710.3729 | Direct Numerical Simulation of a separated channel flow with a smooth
profile | A direct numerical simulation (DNS) of a channel flow with one curved surface
was performed at moderate Reynolds number (Re_tau = 395 at the inlet). The
adverse pressure gradient was obtained by a wall curvature through a
mathematical mapping from physical coordinates to Cartesian ones. The code,
using spectral spanw... | physics.flu-dyn physics.comp-ph | a direct numerical simulation dns of a channel flow with one curved surface was performed at moderate reynolds number re_tau 395 at the inlet the adverse pressure gradient was obtained by a wall curvature through a mathematical mapping from physical coordinates to cartesian ones the code using spectral spanwise and nor... | [['a', 'direct', 'numerical', 'simulation', 'dns', 'of', 'a', 'channel', 'flow', 'with', 'one', 'curved', 'surface', 'was', 'performed', 'at', 'moderate', 'reynolds', 'number', 're_tau', '395', 'at', 'the', 'inlet', 'the', 'adverse', 'pressure', 'gradient', 'was', 'obtained', 'by', 'a', 'wall', 'curvature', 'through', ... | [-0.1578069557553913, 0.14893239009720477, -0.09134537793452972, 0.01797569788945164, -0.06079223886321204, -0.11065460491480063, 0.020375025205557114, 0.3801829779142703, -0.2556710949882973, -0.3065359643955742, 0.11098656418692807, -0.2429310209893932, -0.0038120474200695753, 0.21839875682000665, -0.0062657677588741... |
710.373 | Can Terrestrial Planets Form in Hot-Jupiter Systems? | Models of terrestrial planet formation in the presence of a migrating giant
planet have challenged the notion that hot-Jupiter systems lack terrestrial
planets. We briefly review this issue and suggest that hot-Jupiter systems
should be prime targets for future observational missions designed to detect
Earth-sized an... | astro-ph | models of terrestrial planet formation in the presence of a migrating giant planet have challenged the notion that hotjupiter systems lack terrestrial planets we briefly review this issue and suggest that hotjupiter systems should be prime targets for future observational missions designed to detect earthsized and pote... | [['models', 'of', 'terrestrial', 'planet', 'formation', 'in', 'the', 'presence', 'of', 'a', 'migrating', 'giant', 'planet', 'have', 'challenged', 'the', 'notion', 'that', 'hotjupiter', 'systems', 'lack', 'terrestrial', 'planets', 'we', 'briefly', 'review', 'this', 'issue', 'and', 'suggest', 'that', 'hotjupiter', 'syste... | [-0.20836941818100857, 0.1616379119151709, -0.05048736131617001, 0.11988711272299822, -0.18596477939614228, -0.08040327467594524, 0.09422833548516643, 0.2975756329655343, -0.13217874551762124, -0.3670143940942172, 0.11525485543676708, -0.2765050674123423, -0.20383170592047425, 0.20035072909287957, -0.14363619371564412,... |
710.3731 | Regularization of Hele-Shaw flows, multiscaling expansions and the
Painleve I equation | Critical processes of ideal integrable models of Hele-Shaw flows are
considered. A regularization method based on multiscaling expansions of
solutions of the KdV and Toda hierarchies characterized by string equations is
proposed. Examples are exhibited in which the tritronq'ee solution of the
Painleve-I equation turn... | math-ph math.MP nlin.SI | critical processes of ideal integrable models of heleshaw flows are considered a regularization method based on multiscaling expansions of solutions of the kdv and toda hierarchies characterized by string equations is proposed examples are exhibited in which the tritronqee solution of the painlevei equation turns out t... | [['critical', 'processes', 'of', 'ideal', 'integrable', 'models', 'of', 'heleshaw', 'flows', 'are', 'considered', 'a', 'regularization', 'method', 'based', 'on', 'multiscaling', 'expansions', 'of', 'solutions', 'of', 'the', 'kdv', 'and', 'toda', 'hierarchies', 'characterized', 'by', 'string', 'equations', 'is', 'propos... | [-0.1626367463531491, 0.04457890382915173, -0.1081580889745141, 0.10419630694405158, -0.06817782276643897, -0.179213284172188, -0.03992400025369002, 0.2466853111630903, -0.27931233059685184, -0.19842898657650881, 0.1637121800680311, -0.3048986322334353, -0.19794670081222956, 0.1882639156197602, -0.0160036125167642, 0.1... |
710.3732 | Spitzer's View of Edge-on Spirals | Edge-on spiral galaxies offer a unique perspective on disks. One can
accurately determine the height distribution of stars and ISM and the
line-of-sight integration allows for the study of faint structures. The Spitzer
IRAC camera is an ideal instrument to study both the ISM and stellar structure
in nearby galaxies; ... | astro-ph | edgeon spiral galaxies offer a unique perspective on disks one can accurately determine the height distribution of stars and ism and the lineofsight integration allows for the study of faint structures the spitzer irac camera is an ideal instrument to study both the ism and stellar structure in nearby galaxies two of i... | [['edgeon', 'spiral', 'galaxies', 'offer', 'a', 'unique', 'perspective', 'on', 'disks', 'one', 'can', 'accurately', 'determine', 'the', 'height', 'distribution', 'of', 'stars', 'and', 'ism', 'and', 'the', 'lineofsight', 'integration', 'allows', 'for', 'the', 'study', 'of', 'faint', 'structures', 'the', 'spitzer', 'irac... | [-0.08268429435471572, 0.0623050552144932, -0.08047569441386558, 0.08013275044717508, -0.077637029099051, -0.025196445256857793, -0.0005392455261643613, 0.4638471586357166, -0.18530847219091545, -0.3061246512054534, 0.038015770435222515, -0.2609826800174388, -0.057351308573809705, 0.1400428711942102, -0.054508176964435... |
710.3733 | Composite Strings in (2+1)-Dimensional Anisotropic Weakly-Coupled
Yang-Mills Theory | The small-scale structure of a string connecting a pair of static sources is
explored for the weakly-coupled anisotropic SU(2) Yang-Mills theory in (2+1)
dimensions. A crucial ingredient in the formulation of the string Hamiltonian
is the phenomenon of color smearing of the string constituents. The
quark-anti-quark p... | hep-th cond-mat.str-el hep-lat math-ph math.MP | the smallscale structure of a string connecting a pair of static sources is explored for the weaklycoupled anisotropic su2 yangmills theory in 21 dimensions a crucial ingredient in the formulation of the string hamiltonian is the phenomenon of color smearing of the string constituents the quarkantiquark potential is de... | [['the', 'smallscale', 'structure', 'of', 'a', 'string', 'connecting', 'a', 'pair', 'of', 'static', 'sources', 'is', 'explored', 'for', 'the', 'weaklycoupled', 'anisotropic', 'su2', 'yangmills', 'theory', 'in', '21', 'dimensions', 'a', 'crucial', 'ingredient', 'in', 'the', 'formulation', 'of', 'the', 'string', 'hamilto... | [-0.15469012236924934, 0.2155488347787349, -0.09520340361250718, 0.1323976254407469, -0.0469354004560985, -0.11175784829347471, -0.009589439582415536, 0.3067402553546136, -0.17814996902693492, -0.2448546180471045, 0.010809506774406697, -0.2765817113342832, -0.15860292778854243, 0.062049478109254215, 0.00530039074784908... |
710.3734 | Superfluid Fermi-Fermi mixture: phase diagram, stability, and soliton
formation | We study the phase diagram for a dilute Bardeen-Cooper-Schrieffer superfluid
Fermi-Fermi mixture (of distinct mass) at zero temperature using energy
densities for the superfluid fermions in one (1D), two (2D), and three (3D)
dimensions. We also derive the dynamical time-dependent nonlinear
Euler-Lagrange equation sat... | cond-mat.soft nlin.PS | we study the phase diagram for a dilute bardeencooperschrieffer superfluid fermifermi mixture of distinct mass at zero temperature using energy densities for the superfluid fermions in one 1d two 2d and three 3d dimensions we also derive the dynamical timedependent nonlinear eulerlagrange equation satisfied by the mixt... | [['we', 'study', 'the', 'phase', 'diagram', 'for', 'a', 'dilute', 'bardeencooperschrieffer', 'superfluid', 'fermifermi', 'mixture', 'of', 'distinct', 'mass', 'at', 'zero', 'temperature', 'using', 'energy', 'densities', 'for', 'the', 'superfluid', 'fermions', 'in', 'one', '1d', 'two', '2d', 'and', 'three', '3d', 'dimens... | [-0.1338615418171068, 0.17475872672952453, -0.08935989447182707, 0.06608012989331116, 0.015908554075009552, -0.14883640662409856, 0.004623798084232199, 0.3582131139484187, -0.2274189362908177, -0.2585100590925214, 0.07456056190944688, -0.255943800005899, -0.09437245511848448, 0.14957233595610517, 0.05364309154920501, 0... |
710.3735 | The Brownian gyrator: a minimal heat engine on the nano-scale | A Brownian particle moving in the vicinity of a generic potential minimum
under the influence of dissipation and thermal noise from two different heat
baths is shown to act as a minimal heat engine, generating a systematic torque
onto the physical object at the origin of the potential and an opposite torque
onto the ... | cond-mat.stat-mech | a brownian particle moving in the vicinity of a generic potential minimum under the influence of dissipation and thermal noise from two different heat baths is shown to act as a minimal heat engine generating a systematic torque onto the physical object at the origin of the potential and an opposite torque onto the med... | [['a', 'brownian', 'particle', 'moving', 'in', 'the', 'vicinity', 'of', 'a', 'generic', 'potential', 'minimum', 'under', 'the', 'influence', 'of', 'dissipation', 'and', 'thermal', 'noise', 'from', 'two', 'different', 'heat', 'baths', 'is', 'shown', 'to', 'act', 'as', 'a', 'minimal', 'heat', 'engine', 'generating', 'a',... | [-0.15537902560879893, 0.15246015977629276, -0.07213142354458828, 0.010840013731624288, -0.0745658928303626, -0.09248114351568551, 0.0435638561667192, 0.3263016598788893, -0.31945183365766344, -0.2797542667851366, 0.05913578931860433, -0.3148763041686395, -0.07099274244031002, 0.26554231603573686, -0.01897840447531178,... |
710.3736 | Analysis of Proton Radiography Images of Shock Melted/Damaged Tin | Tin coupons were shock damaged/melted under identical conditions with a
diverging high explosive shock wave. Proton Radiography images and velocimetry
data from experiments with seven different tin coupons of varying thickness are
analyzed. Comparing experiments with identical samples allowed us to
distinguish betwee... | physics.data-an physics.ins-det | tin coupons were shock damagedmelted under identical conditions with a diverging high explosive shock wave proton radiography images and velocimetry data from experiments with seven different tin coupons of varying thickness are analyzed comparing experiments with identical samples allowed us to distinguish between rep... | [['tin', 'coupons', 'were', 'shock', 'damagedmelted', 'under', 'identical', 'conditions', 'with', 'a', 'diverging', 'high', 'explosive', 'shock', 'wave', 'proton', 'radiography', 'images', 'and', 'velocimetry', 'data', 'from', 'experiments', 'with', 'seven', 'different', 'tin', 'coupons', 'of', 'varying', 'thickness', ... | [-0.062131724310848783, 0.21282277509037936, -0.05337472095116213, 0.017949228370989844, -0.024193729651730736, -0.1703944299791759, 0.02371722765086333, 0.41528610600044535, -0.260889611606087, -0.32412711167898106, 0.04846203444069441, -0.3466519868495513, -0.006845648457505265, 0.16415710121450222, 0.000175797551566... |
710.3737 | Disorder, Metal-Insulator crossover and Phase diagram in high-Tc
cuprates | We have studied the influence of disorder induced by electron irradiation on
the normal state resistivities $\rho(T)$ of optimally and underdoped YBa2CuOx
single crystals, using pulsed magnetic fields up to 60T to completely restore
the normal state. We evidence that point defect disorder induces low T upturns
of rho... | cond-mat.supr-con cond-mat.str-el | we have studied the influence of disorder induced by electron irradiation on the normal state resistivities rhot of optimally and underdoped yba2cuox single crystals using pulsed magnetic fields up to 60t to completely restore the normal state we evidence that point defect disorder induces low t upturns of rhot which s... | [['we', 'have', 'studied', 'the', 'influence', 'of', 'disorder', 'induced', 'by', 'electron', 'irradiation', 'on', 'the', 'normal', 'state', 'resistivities', 'rhot', 'of', 'optimally', 'and', 'underdoped', 'yba2cuox', 'single', 'crystals', 'using', 'pulsed', 'magnetic', 'fields', 'up', 'to', '60t', 'to', 'completely', ... | [-0.14716772083848925, 0.27460967525708635, -0.0440731521230191, 0.044873758857007284, -0.013906911566433772, -0.13318349276079047, 0.11842250491453099, 0.3827523416642782, -0.2361981063576179, -0.2905181943452064, 0.02985949618709077, -0.3221521139223601, -0.09193045475428373, 0.16796166761975054, 0.002434256578415212... |
710.3738 | Fast optical preparation, control and read-out of single quantum dot
spin | We propose and demonstrate the sequential initialization, optical control,
and read-out of a single spin trapped in a semiconductor quantum dot. Hole spin
preparation is achieved through ionization of a resonantly excited
electron-hole pair. Optical control is observed as a coherent Rabi rotation
between the hole and... | cond-mat.mes-hall | we propose and demonstrate the sequential initialization optical control and readout of a single spin trapped in a semiconductor quantum dot hole spin preparation is achieved through ionization of a resonantly excited electronhole pair optical control is observed as a coherent rabi rotation between the hole and charged... | [['we', 'propose', 'and', 'demonstrate', 'the', 'sequential', 'initialization', 'optical', 'control', 'and', 'readout', 'of', 'a', 'single', 'spin', 'trapped', 'in', 'a', 'semiconductor', 'quantum', 'dot', 'hole', 'spin', 'preparation', 'is', 'achieved', 'through', 'ionization', 'of', 'a', 'resonantly', 'excited', 'ele... | [-0.1775004593686511, 0.24952128257602454, -0.0038942486971306305, 0.03595890305781116, 0.05350098540075123, -0.23226141434783737, 0.057115214600538214, 0.42138326331973075, -0.2160769454141458, -0.27682856080432733, -0.0379409326131766, -0.26713665325194597, 0.018016931967188916, 0.2255358991989245, 0.0476694005774334... |
710.3739 | (Non)Commutative Hopf algebras of trees and (quasi)symmetric functions | The Connes-Kreimer Hopf algebra of rooted trees, its dual, and the Foissy
Hopf algebra of of planar rooted trees are related to each other and to the
well-known Hopf algebras of symmetric and quasi-symmetric functions via a pair
of commutative diagrams. We show how this point of view can simplify
computations in the ... | math.QA math.CO | the conneskreimer hopf algebra of rooted trees its dual and the foissy hopf algebra of of planar rooted trees are related to each other and to the wellknown hopf algebras of symmetric and quasisymmetric functions via a pair of commutative diagrams we show how this point of view can simplify computations in the conneskr... | [['the', 'conneskreimer', 'hopf', 'algebra', 'of', 'rooted', 'trees', 'its', 'dual', 'and', 'the', 'foissy', 'hopf', 'algebra', 'of', 'of', 'planar', 'rooted', 'trees', 'are', 'related', 'to', 'each', 'other', 'and', 'to', 'the', 'wellknown', 'hopf', 'algebras', 'of', 'symmetric', 'and', 'quasisymmetric', 'functions', ... | [-0.17471682766336016, 0.08223177403124282, -0.08428314410230087, 0.09648967229259142, -0.24110435205875547, -0.1136931261207792, 0.013546464935643598, 0.32422611210495234, -0.4491438631666824, -0.1587527400770341, 0.1442688306906348, -0.2216544667389826, -0.24157320745871402, 0.17246640265511815, -0.11948776720964815,... |
710.374 | Masses for the Local Group and the Milky Way | We use the very large Millennium Simulation of the concordance $\Lambda$CDM
cosmogony to calibrate the bias and error distribution of Timing Argument
estimators of the masses of the Local Group and of the Milky Way. From a large
number of isolated spiral-spiral pairs similar to the Milky Way/Andromeda
system, we find... | astro-ph | we use the very large millennium simulation of the concordance lambdacdm cosmogony to calibrate the bias and error distribution of timing argument estimators of the masses of the local group and of the milky way from a large number of isolated spiralspiral pairs similar to the milky wayandromeda system we find the inte... | [['we', 'use', 'the', 'very', 'large', 'millennium', 'simulation', 'of', 'the', 'concordance', 'lambdacdm', 'cosmogony', 'to', 'calibrate', 'the', 'bias', 'and', 'error', 'distribution', 'of', 'timing', 'argument', 'estimators', 'of', 'the', 'masses', 'of', 'the', 'local', 'group', 'and', 'of', 'the', 'milky', 'way', '... | [-0.10228749441595429, 0.07630429205157992, -0.061209043264514894, 0.09797255512534615, -0.035754554795923536, -0.029171435143546882, 0.11502512019423365, 0.31906932395639587, -0.15718190202086763, -0.4223410749791173, 0.055833293454352395, -0.26684366902000867, 0.02120634839085543, 0.22538289397866842, -0.025686212917... |
710.3741 | Additional Gradings in Khovanov Homology | The main goal of the present paper is to construct new invariants of knots
with additional structure by adding new gradings to the Khovanov complex. The
ideas given below work in the case of virtual knots, closed braids and some
other cases of knots with additional structure. The source of our additional
grading may ... | math.GT math.AG | the main goal of the present paper is to construct new invariants of knots with additional structure by adding new gradings to the khovanov complex the ideas given below work in the case of virtual knots closed braids and some other cases of knots with additional structure the source of our additional grading may be to... | [['the', 'main', 'goal', 'of', 'the', 'present', 'paper', 'is', 'to', 'construct', 'new', 'invariants', 'of', 'knots', 'with', 'additional', 'structure', 'by', 'adding', 'new', 'gradings', 'to', 'the', 'khovanov', 'complex', 'the', 'ideas', 'given', 'below', 'work', 'in', 'the', 'case', 'of', 'virtual', 'knots', 'close... | [-0.1692158248979689, 0.0905246527115928, -0.08948274378710222, 0.09923928237034621, -0.13870310032649374, -0.19074306718255507, -0.01738999663815243, 0.35513668650159297, -0.34856639905526055, -0.3104434110293102, 0.0915590806774761, -0.23690504849911098, -0.19501001573957094, 0.18553495944744522, -0.1704222434910196,... |
710.3742 | Bayesian Online Changepoint Detection | Changepoints are abrupt variations in the generative parameters of a data
sequence. Online detection of changepoints is useful in modelling and
prediction of time series in application areas such as finance, biometrics, and
robotics. While frequentist methods have yielded online filtering and
prediction techniques, m... | stat.ML | changepoints are abrupt variations in the generative parameters of a data sequence online detection of changepoints is useful in modelling and prediction of time series in application areas such as finance biometrics and robotics while frequentist methods have yielded online filtering and prediction techniques most bay... | [['changepoints', 'are', 'abrupt', 'variations', 'in', 'the', 'generative', 'parameters', 'of', 'a', 'data', 'sequence', 'online', 'detection', 'of', 'changepoints', 'is', 'useful', 'in', 'modelling', 'and', 'prediction', 'of', 'time', 'series', 'in', 'application', 'areas', 'such', 'as', 'finance', 'biometrics', 'and'... | [-0.06258493338578514, -0.019778564561420353, -0.09518850399513862, 0.07186824502839174, -0.07952402408700436, -0.1414773739109348, 0.05134541146274257, 0.4352305792538183, -0.25098522341743645, -0.3488933228519662, 0.1670618407636149, -0.23948572452978364, -0.18836834573220196, 0.22844089688566913, -0.1020767683014647... |
710.3743 | Current Algebra on the Torus | We derive the N-point one-loop correlation functions for the currents of an
arbitrary affine Kac-Moody algebra. The one-loop amplitudes, which are elliptic
functions defined on the torus Riemann surface, are specified by group
invariant tensors and certain constant tau-dependent functions. We compute the
elliptic fun... | hep-th math.QA | we derive the npoint oneloop correlation functions for the currents of an arbitrary affine kacmoody algebra the oneloop amplitudes which are elliptic functions defined on the torus riemann surface are specified by group invariant tensors and certain constant taudependent functions we compute the elliptic functions via ... | [['we', 'derive', 'the', 'npoint', 'oneloop', 'correlation', 'functions', 'for', 'the', 'currents', 'of', 'an', 'arbitrary', 'affine', 'kacmoody', 'algebra', 'the', 'oneloop', 'amplitudes', 'which', 'are', 'elliptic', 'functions', 'defined', 'on', 'the', 'torus', 'riemann', 'surface', 'are', 'specified', 'by', 'group',... | [-0.18666819946277732, 0.1539845134989264, -0.06460994720691815, 0.15100199524022173, -0.11751578656306567, -0.09415436107277249, -0.05350599653684185, 0.3224080165964551, -0.3006437932466118, -0.20782915054587647, 0.10153747386236016, -0.2322701843562148, -0.19969964614817096, 0.17047959352930775, -0.01799163810210302... |
710.3744 | Combinatorial Hopf algebras and Towers of Algebras | Bergeron and Li have introduced a set of axioms which guarantee that the
Grothendieck groups of a tower of algebras $\bigoplus_{n\ge0}A_n$ can be
endowed with the structure of graded dual Hopf algebras. Hivert and Nzeutzhap,
and independently Lam and Shimozono constructed dual graded graphs from
primitive elements in... | math.CO math.RT | bergeron and li have introduced a set of axioms which guarantee that the grothendieck groups of a tower of algebras bigoplus_nge0a_n can be endowed with the structure of graded dual hopf algebras hivert and nzeutzhap and independently lam and shimozono constructed dual graded graphs from primitive elements in hopf alge... | [['bergeron', 'and', 'li', 'have', 'introduced', 'a', 'set', 'of', 'axioms', 'which', 'guarantee', 'that', 'the', 'grothendieck', 'groups', 'of', 'a', 'tower', 'of', 'algebras', 'bigoplus_nge0a_n', 'can', 'be', 'endowed', 'with', 'the', 'structure', 'of', 'graded', 'dual', 'hopf', 'algebras', 'hivert', 'and', 'nzeutzha... | [-0.14188558362559023, 0.1148751476240984, -0.09503170235800636, 0.05410812075210578, -0.1472788908833032, -0.15742094886029162, -0.03515608279533819, 0.3421219091144312, -0.4008274606642235, -0.21013774960133505, 0.1118382545361991, -0.18650938650166773, -0.19583517976711134, 0.14313964528895645, -0.21150722674441985,... |
710.3745 | Parametric downconversion with optimized spectral properties in
nonlinear photonic crystals | We study the joint spectral properties of photon pairs generated by
spontaneous parametric down-conversion in a one-dimensional nonlinear photonic
crystal in a collinear, degenerate, type-II geometry. We show that the photonic
crystal properties may be exploited to compensate for material dispersion and
obtain photon... | quant-ph | we study the joint spectral properties of photon pairs generated by spontaneous parametric downconversion in a onedimensional nonlinear photonic crystal in a collinear degenerate typeii geometry we show that the photonic crystal properties may be exploited to compensate for material dispersion and obtain photon pairs t... | [['we', 'study', 'the', 'joint', 'spectral', 'properties', 'of', 'photon', 'pairs', 'generated', 'by', 'spontaneous', 'parametric', 'downconversion', 'in', 'a', 'onedimensional', 'nonlinear', 'photonic', 'crystal', 'in', 'a', 'collinear', 'degenerate', 'typeii', 'geometry', 'we', 'show', 'that', 'the', 'photonic', 'cry... | [-0.10361036376015824, 0.1970220176204119, -0.03311767350928283, 0.03196896512038362, -0.10111633520343422, -0.13444109558829187, 0.027319619446463973, 0.47837516467696356, -0.2748453642851041, -0.27770264883652146, 0.03687029512294419, -0.27575716794824895, -0.1206320966248987, 0.22093239922096586, -0.0123776596292485... |
710.3746 | On Algebraic Shift Equivalence of Matrices over Polynomial Rings | The paper studies algebraic strong shift equivalence of matrices over
$n$-variable polynomial rings over a principal ideal domain $D$($n\leq 2$). It
is proved that in the case $n=1$, every non-zero matrix over $D[x]$ has a full
rank factorization and every non-nilpotent matrix over $D[x]$ is algebraically
strong shif... | math.RA math.DS | the paper studies algebraic strong shift equivalence of matrices over nvariable polynomial rings over a principal ideal domain dnleq 2 it is proved that in the case n1 every nonzero matrix over dx has a full rank factorization and every nonnilpotent matrix over dx is algebraically strong shift equivalent to a nonsingul... | [['the', 'paper', 'studies', 'algebraic', 'strong', 'shift', 'equivalence', 'of', 'matrices', 'over', 'nvariable', 'polynomial', 'rings', 'over', 'a', 'principal', 'ideal', 'domain', 'dnleq', '2', 'it', 'is', 'proved', 'that', 'in', 'the', 'case', 'n1', 'every', 'nonzero', 'matrix', 'over', 'dx', 'has', 'a', 'full', 'r... | [-0.17981536382188398, 0.08855089824200453, -0.056844480546812216, 0.015336224921047687, -0.04830157463128368, -0.18673373476912578, -0.07814463224106778, 0.3904728551208973, -0.3505143161614736, -0.09260647645841043, 0.12091429141970972, -0.2707932741070787, -0.17111958968142668, 0.16708508405834435, -0.05735470574349... |
710.3747 | Quantum parallelism as a tool for ensemble spin dynamics calculations | Efficient simulations of quantum evolutions of spin-1/2 systems are relevant
for ensemble quantum computation as well as in typical NMR experiments. We
propose an efficient method to calculate the dynamics of an observable provided
that the initial excitation is "local". It resorts a single entangled pure
initial sta... | quant-ph cond-mat.mes-hall physics.chem-ph | efficient simulations of quantum evolutions of spin12 systems are relevant for ensemble quantum computation as well as in typical nmr experiments we propose an efficient method to calculate the dynamics of an observable provided that the initial excitation is local it resorts a single entangled pure initial state built... | [['efficient', 'simulations', 'of', 'quantum', 'evolutions', 'of', 'spin12', 'systems', 'are', 'relevant', 'for', 'ensemble', 'quantum', 'computation', 'as', 'well', 'as', 'in', 'typical', 'nmr', 'experiments', 'we', 'propose', 'an', 'efficient', 'method', 'to', 'calculate', 'the', 'dynamics', 'of', 'an', 'observable',... | [-0.13137937652339277, 0.22180656492005493, -0.0828193371067755, 0.04882840308434281, 0.014450240429294737, -0.149428921702661, 0.008041532195516322, 0.3719663360205136, -0.2548074284274327, -0.28835183507272677, 0.07958187887714685, -0.23138976780403603, -0.07790550560151276, 0.18678207573922057, 0.07874471323203149, ... |
710.3748 | Searching for Star Formation Outside Galaxies: Multiwavelength Analysis
of the Intragroup Medium of HCG100 | We used multiwavelength data (HI, FUV, NUV, R) to search for evidence of star
formation in the intragroup medium of the Hickson Compact Group 100. We find
that young star-forming regions are located in the intergalactic HI clouds of
the compact group which extend to over 130 kpc away from the main galaxies. A
tidal d... | astro-ph | we used multiwavelength data hi fuv nuv r to search for evidence of star formation in the intragroup medium of the hickson compact group 100 we find that young starforming regions are located in the intergalactic hi clouds of the compact group which extend to over 130 kpc away from the main galaxies a tidal dwarf galax... | [['we', 'used', 'multiwavelength', 'data', 'hi', 'fuv', 'nuv', 'r', 'to', 'search', 'for', 'evidence', 'of', 'star', 'formation', 'in', 'the', 'intragroup', 'medium', 'of', 'the', 'hickson', 'compact', 'group', '100', 'we', 'find', 'that', 'young', 'starforming', 'regions', 'are', 'located', 'in', 'the', 'intergalactic... | [-0.03132692575958129, 0.09089219730624275, -0.011128835738762407, 0.10862889300522117, -0.10669491017186963, 0.001166670147810962, 0.06035333800419058, 0.5183151811109604, -0.0851610244245495, -0.35550607851630933, 0.030068338285452006, -0.32308408122106985, 0.05075443408772903, 0.16563546536899348, -0.005909162227613... |
710.3749 | Completions of quantum coordinate rings | Given an iterated skew polynomial ring C[y_1;t_1,d_1]ldots [y_n;t_n,d_n] over
a complete local ring C with maximal ideal m, we prove, under suitable
assumptions, that the completion at the ideal m + < y_1,y_2,ldots,y_n> is an
iterated skew power series ring. Under further conditions, this completion is a
local, noeth... | math.RA math.QA | given an iterated skew polynomial ring cy_1t_1d_1ldots y_nt_nd_n over a complete local ring c with maximal ideal m we prove under suitable assumptions that the completion at the ideal m y_1y_2ldotsy_n is an iterated skew power series ring under further conditions this completion is a local noetherian auslander regular ... | [['given', 'an', 'iterated', 'skew', 'polynomial', 'ring', 'cy_1t_1d_1ldots', 'y_nt_nd_n', 'over', 'a', 'complete', 'local', 'ring', 'c', 'with', 'maximal', 'ideal', 'm', 'we', 'prove', 'under', 'suitable', 'assumptions', 'that', 'the', 'completion', 'at', 'the', 'ideal', 'm', 'y_1y_2ldotsy_n', 'is', 'an', 'iterated', ... | [-0.20719264365606388, 0.04666348064162421, -0.07303845329147021, 0.05371964660717837, -0.08218394145290604, -0.1872698756613595, -0.09284258861552482, 0.3649858072147531, -0.40211657882999563, -0.07277960923768706, 0.135074500870591, -0.16540095846216052, -0.13319331349142022, 0.2146311020557532, -0.16093245417005936,... |
710.375 | An Imaging Fabry-Perot System for the Robert Stobie Spectrograph on the
Southern African Large Telescope | We present the design of the Fabry-Perot system of the Robert Stobie
Spectrograph on the 10-meter class Southern African Large Telescope and its
characterization as measured in the laboratory. This system provides
spectroscopic imaging at any desired wavelength spanning a bandpass 430 - 860
nm, at four different spec... | astro-ph | we present the design of the fabryperot system of the robert stobie spectrograph on the 10meter class southern african large telescope and its characterization as measured in the laboratory this system provides spectroscopic imaging at any desired wavelength spanning a bandpass 430 860 nm at four different spectral res... | [['we', 'present', 'the', 'design', 'of', 'the', 'fabryperot', 'system', 'of', 'the', 'robert', 'stobie', 'spectrograph', 'on', 'the', '10meter', 'class', 'southern', 'african', 'large', 'telescope', 'and', 'its', 'characterization', 'as', 'measured', 'in', 'the', 'laboratory', 'this', 'system', 'provides', 'spectrosco... | [-0.14246951142779074, 0.12189524508391293, -0.09103952595410315, -0.023300792218336988, -0.07868753628352204, -0.11278661358346408, 0.038467117422889614, 0.4144435577925194, -0.24560730217679128, -0.3757114814191654, 0.09337502639375728, -0.2730752188636846, -0.10563408458177503, 0.23046386324850893, -0.03618026759374... |
710.3751 | Crime and punishment: the economic burden of impunity | Crime is an economically important activity, sometimes called the industry of
crime. It may represent a mechanism of wealth distribution but also a social
and economic charge because of the cost of the law enforcement system.
Sometimes it may be less costly for the society to allow for some level of
criminality. A dr... | nlin.AO | crime is an economically important activity sometimes called the industry of crime it may represent a mechanism of wealth distribution but also a social and economic charge because of the cost of the law enforcement system sometimes it may be less costly for the society to allow for some level of criminality a drawback... | [['crime', 'is', 'an', 'economically', 'important', 'activity', 'sometimes', 'called', 'the', 'industry', 'of', 'crime', 'it', 'may', 'represent', 'a', 'mechanism', 'of', 'wealth', 'distribution', 'but', 'also', 'a', 'social', 'and', 'economic', 'charge', 'because', 'of', 'the', 'cost', 'of', 'the', 'law', 'enforcement... | [-0.09622401896335964, 0.09876117376020306, -0.12259248086796906, 0.1453171330938505, -0.08760956906949852, -0.13045058698296103, 0.11699405571301606, 0.33715502055598173, -0.2722851520160095, -0.3157547248402305, 0.1316424675560348, -0.2795169370443518, -0.1629987030321343, 0.1829821851848166, -0.1386558880052988, 0.0... |
710.3752 | First joint Gravitational Waves search by the
Auriga-Explorer-Nautilus-Virgo collaboration | We present results of the search for coincident burst excitations over a 24
hours long data set collected by AURIGA, EXPLORER, NAUTILUS and Virgo detectors
during September 2005. The search of candidate triggers was performed
independently on each of the data sets from single detectors. We looked for
two-fold time co... | gr-qc | we present results of the search for coincident burst excitations over a 24 hours long data set collected by auriga explorer nautilus and virgo detectors during september 2005 the search of candidate triggers was performed independently on each of the data sets from single detectors we looked for twofold time coinciden... | [['we', 'present', 'results', 'of', 'the', 'search', 'for', 'coincident', 'burst', 'excitations', 'over', 'a', '24', 'hours', 'long', 'data', 'set', 'collected', 'by', 'auriga', 'explorer', 'nautilus', 'and', 'virgo', 'detectors', 'during', 'september', '2005', 'the', 'search', 'of', 'candidate', 'triggers', 'was', 'pe... | [-0.1051507013498981, 0.06304484099487984, -0.03734192077704854, 0.04991176299771051, -0.01838765421754046, -0.0884215186579504, 0.12536356980453475, 0.38037732535082364, -0.20072718107384507, -0.3793817428784256, 0.09978538784839591, -0.32598032108575536, -0.06632799792197952, 0.24728021576015305, -0.00023397007084829... |
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