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 |
|---|---|---|---|---|---|---|
707.153 | Pseudospin Magnetism in Graphene | We predict that neutral graphene bilayers are pseudospin magnets in which the
charge density-contribution from each valley and spin spontaneously shifts to
one of the two layers. The band structure of this system is characterized by a
momentum-space vortex which is responsible for unusual competition between band
and... | cond-mat.str-el | we predict that neutral graphene bilayers are pseudospin magnets in which the charge densitycontribution from each valley and spin spontaneously shifts to one of the two layers the band structure of this system is characterized by a momentumspace vortex which is responsible for unusual competition between band and kine... | [['we', 'predict', 'that', 'neutral', 'graphene', 'bilayers', 'are', 'pseudospin', 'magnets', 'in', 'which', 'the', 'charge', 'densitycontribution', 'from', 'each', 'valley', 'and', 'spin', 'spontaneously', 'shifts', 'to', 'one', 'of', 'the', 'two', 'layers', 'the', 'band', 'structure', 'of', 'this', 'system', 'is', 'c... | [-0.20348339693988732, 0.22588535308561944, -0.005460700860971378, 0.03071800226426143, -0.045621381152743175, -0.16649446051199862, 0.04158028061961594, 0.3993127695572229, -0.26326670635054694, -0.2840139444595502, -0.002882339955698469, -0.2602064827411079, -0.14197980527432613, 0.11525272435428184, 0.07581375980818... |
707.1531 | Spin and orbital magnetic response in metals: susceptibility and NMR
shifts | A DFT-based method is presented which allows the computation of all-electron
NMR shifts of metallic compounds with periodic boundary conditions. NMR shifts
in metals measure two competing physical phenomena. Electrons interact with the
applied magnetic field (i) as magnetic dipoles (or spins), resulting in the
Knight... | cond-mat.mtrl-sci | a dftbased method is presented which allows the computation of allelectron nmr shifts of metallic compounds with periodic boundary conditions nmr shifts in metals measure two competing physical phenomena electrons interact with the applied magnetic field i as magnetic dipoles or spins resulting in the knight shift ii a... | [['a', 'dftbased', 'method', 'is', 'presented', 'which', 'allows', 'the', 'computation', 'of', 'allelectron', 'nmr', 'shifts', 'of', 'metallic', 'compounds', 'with', 'periodic', 'boundary', 'conditions', 'nmr', 'shifts', 'in', 'metals', 'measure', 'two', 'competing', 'physical', 'phenomena', 'electrons', 'interact', 'w... | [-0.11405820481052836, 0.21285106873580623, -0.019083843702950666, 0.03627060358003537, -0.02285222092806991, -0.15255438519729855, 0.0287718668309075, 0.40939445027175386, -0.23846682786589135, -0.304031766370974, -0.00866941994487157, -0.3172158884826294, -0.06581461210137333, 0.18125049212972658, 0.08289366299022977... |
707.1532 | Sorting and Selection in Posets | Classical problems of sorting and searching assume an underlying linear
ordering of the objects being compared. In this paper, we study a more general
setting, in which some pairs of objects are incomparable. This generalization
is relevant in applications related to rankings in sports, college admissions,
or confere... | cs.DS cs.DM | classical problems of sorting and searching assume an underlying linear ordering of the objects being compared in this paper we study a more general setting in which some pairs of objects are incomparable this generalization is relevant in applications related to rankings in sports college admissions or conference subm... | [['classical', 'problems', 'of', 'sorting', 'and', 'searching', 'assume', 'an', 'underlying', 'linear', 'ordering', 'of', 'the', 'objects', 'being', 'compared', 'in', 'this', 'paper', 'we', 'study', 'a', 'more', 'general', 'setting', 'in', 'which', 'some', 'pairs', 'of', 'objects', 'are', 'incomparable', 'this', 'gener... | [-0.09934936190906005, 0.09009924334775549, -0.04437080433689141, 0.07821636881244795, -0.08955842836804993, -0.1266545077126307, 0.1190178098704936, 0.34650777953894996, -0.28326145927707375, -0.33912824298043953, 0.07470455907283483, -0.2945503024955637, -0.1535768937795565, 0.18843582423220365, -0.10593450090070654,... |
707.1533 | The Fate of Dwarf Galaxies in Clusters and the Origin of Intracluster
Stars. I. Isolated Clusters | The main goal of this paper is to compare the relative importance of
destruction by tides, vs. destruction by mergers, in order to assess if tidal
destruction of dwarf galaxies in clusters is a viable scenario for explaining
the origin of intracluster stars. We have designed a simple algorithm for
simulating the evol... | astro-ph | the main goal of this paper is to compare the relative importance of destruction by tides vs destruction by mergers in order to assess if tidal destruction of dwarf galaxies in clusters is a viable scenario for explaining the origin of intracluster stars we have designed a simple algorithm for simulating the evolution ... | [['the', 'main', 'goal', 'of', 'this', 'paper', 'is', 'to', 'compare', 'the', 'relative', 'importance', 'of', 'destruction', 'by', 'tides', 'vs', 'destruction', 'by', 'mergers', 'in', 'order', 'to', 'assess', 'if', 'tidal', 'destruction', 'of', 'dwarf', 'galaxies', 'in', 'clusters', 'is', 'a', 'viable', 'scenario', 'fo... | [-0.11378169585810624, 0.09617393829726748, -0.11413536124855728, 0.14174468750729316, -0.07661992866945054, 0.03402860544944056, 0.04005145502567319, 0.3631470666119927, -0.15132426487323933, -0.3534277036814089, 0.015597386392449638, -0.2606547912652779, -0.09997958514867421, 0.19772663959687142, -0.02744472366792703... |
707.1534 | An Architecture Framework for Complex Data Warehouses | Nowadays, many decision support applications need to exploit data that are
not only numerical or symbolic, but also multimedia, multistructure,
multisource, multimodal, and/or multiversion. We term such data complex data.
Managing and analyzing complex data involves a lot of different issues
regarding their structure... | cs.DB | nowadays many decision support applications need to exploit data that are not only numerical or symbolic but also multimedia multistructure multisource multimodal andor multiversion we term such data complex data managing and analyzing complex data involves a lot of different issues regarding their structure storage an... | [['nowadays', 'many', 'decision', 'support', 'applications', 'need', 'to', 'exploit', 'data', 'that', 'are', 'not', 'only', 'numerical', 'or', 'symbolic', 'but', 'also', 'multimedia', 'multistructure', 'multisource', 'multimodal', 'andor', 'multiversion', 'we', 'term', 'such', 'data', 'complex', 'data', 'managing', 'an... | [-0.09746129077309809, 0.01622478454541281, -0.03910147478442184, 0.09281925964102203, -0.20221408828757972, -0.16054749009768954, 0.06423318500901914, 0.41077871883301426, -0.31041877562340964, -0.34569643131664973, 0.16668400234331732, -0.2657377714787027, -0.1464172749522162, 0.22299218822853545, -0.1269060963079695... |
707.1535 | Unparticle physics effects in B_s mixing | We investigate unparticle effects in B_s mixing. In particular we discuss the
possibility of reproducing the experimental result of \Delta M_s, while having
large effects on the mixing phase \phi_s, which might be visible in current
experiments.
| hep-ph hep-ex | we investigate unparticle effects in b_s mixing in particular we discuss the possibility of reproducing the experimental result of delta m_s while having large effects on the mixing phase phi_s which might be visible in current experiments | [['we', 'investigate', 'unparticle', 'effects', 'in', 'b_s', 'mixing', 'in', 'particular', 'we', 'discuss', 'the', 'possibility', 'of', 'reproducing', 'the', 'experimental', 'result', 'of', 'delta', 'm_s', 'while', 'having', 'large', 'effects', 'on', 'the', 'mixing', 'phase', 'phi_s', 'which', 'might', 'be', 'visible',... | [-0.14884036123702252, 0.3167647485294052, -0.025510587200925156, 0.10529397518650906, -0.05246461031807435, -0.07248137078273136, 0.085788980529115, 0.3248911059801341, -0.24643617057921113, -0.2843520742010426, 0.06189924365576558, -0.2760688399996709, -0.12463413813226931, 0.15122484649858764, -0.0001931162299336613... |
707.1536 | Dark Matter and Particle Physics | [A brief review intended for a general physics colloquium audience.]
Astrophysicists now know that 80% of the matter in the universe is `dark
matter', composed of neutral and weakly interacting elementary particles that
are not part of the Standard Model of particle physics. I will summarize the
evidence for dark mat... | hep-ph astro-ph | a brief review intended for a general physics colloquium audience astrophysicists now know that 80 of the matter in the universe is dark matter composed of neutral and weakly interacting elementary particles that are not part of the standard model of particle physics i will summarize the evidence for dark matter i will... | [['a', 'brief', 'review', 'intended', 'for', 'a', 'general', 'physics', 'colloquium', 'audience', 'astrophysicists', 'now', 'know', 'that', '80', 'of', 'the', 'matter', 'in', 'the', 'universe', 'is', 'dark', 'matter', 'composed', 'of', 'neutral', 'and', 'weakly', 'interacting', 'elementary', 'particles', 'that', 'are',... | [-0.055508181932382286, 0.27629400382749736, -0.14635714782867582, 0.16265205862931909, -0.12236042329110206, -0.15595081442501396, -0.07324340704362839, 0.3266808870434761, -0.21296296619810165, -0.3331695055682212, 0.03602357514435425, -0.30305901911109684, -0.0729988999950001, 0.13215050894184968, -0.003763040117919... |
707.1537 | Numerical Modeling of AGN Jets: Formation of Magnetically Dominated
Lobes and Stability Properties of Current-carrying Jets | We argue the behavior of Poynting flux-dominated outflows from AGN in the
galactic cluster systems by performing three-dimensional MHD simulations within
the framework of the "magnetic tower" model. Of particular interests are the
structure of MHD waves, the cylindrical radial force balance, the
(de)collimation, and ... | astro-ph | we argue the behavior of poynting fluxdominated outflows from agn in the galactic cluster systems by performing threedimensional mhd simulations within the framework of the magnetic tower model of particular interests are the structure of mhd waves the cylindrical radial force balance the decollimation and the stabilit... | [['we', 'argue', 'the', 'behavior', 'of', 'poynting', 'fluxdominated', 'outflows', 'from', 'agn', 'in', 'the', 'galactic', 'cluster', 'systems', 'by', 'performing', 'threedimensional', 'mhd', 'simulations', 'within', 'the', 'framework', 'of', 'the', 'magnetic', 'tower', 'model', 'of', 'particular', 'interests', 'are', ... | [-0.1871496638872058, 0.1759285382594338, -0.0397025801734451, 0.10008276181350298, -0.08473012856591274, 0.0028235511443413354, -0.052063868079772764, 0.3690840974343112, -0.2402587651329882, -0.31040316880406704, 0.028598496264106977, -0.21715462305035224, -0.05910708817571182, 0.1919900575936909, 0.08712311870391097... |
707.1538 | Transition temperature of the homogeneous and dilute Bose gas in
D-dimensions | The phase transition temperature of the homogeneous and dilute Bose gas in
D-dimensions ($2 \le D \le 3$) is calculated by a mean field-based statistical
method. The shift of the phase transition temperature is written up to the
leading order as $\Delta T_c/T_c^0 = c \gam^{\al}$, where $\gam=n^{1/3}a$.
We derived H... | cond-mat.stat-mech | the phase transition temperature of the homogeneous and dilute bose gas in ddimensions 2 le d le 3 is calculated by a mean fieldbased statistical method the shift of the phase transition temperature is written up to the leading order as delta t_ct_c0 c gamal where gamn13a we derived huangs result of the phase transitio... | [['the', 'phase', 'transition', 'temperature', 'of', 'the', 'homogeneous', 'and', 'dilute', 'bose', 'gas', 'in', 'ddimensions', '2', 'le', 'd', 'le', '3', 'is', 'calculated', 'by', 'a', 'mean', 'fieldbased', 'statistical', 'method', 'the', 'shift', 'of', 'the', 'phase', 'transition', 'temperature', 'is', 'written', 'up... | [-0.11017984084330737, 0.19049237839256725, -0.039844682088633086, 0.006820753869582333, 0.060551876900717616, -0.13246894937793852, 0.050390884316727225, 0.3411908399236078, -0.21787594797491444, -0.2696771312484463, 0.05283738402238883, -0.3180012229793504, -0.0862859286112236, 0.13305073846862012, 0.0193661853954122... |
707.1539 | Conjugacy classes and invariant subrings of R-automorphisms of R[x] | We consider the group G of R-automorphisms of the polynomial ring R[x]
especially in the case where R is the ring of integers modulo n. We describe
conjugacy classes in G, and in the case where n = 4, we describe more
explicitly the structure of G and determine all rings of invariants of R[x]
with respect to subgroup... | math.AC | we consider the group g of rautomorphisms of the polynomial ring rx especially in the case where r is the ring of integers modulo n we describe conjugacy classes in g and in the case where n 4 we describe more explicitly the structure of g and determine all rings of invariants of rx with respect to subgroups of g | [['we', 'consider', 'the', 'group', 'g', 'of', 'rautomorphisms', 'of', 'the', 'polynomial', 'ring', 'rx', 'especially', 'in', 'the', 'case', 'where', 'r', 'is', 'the', 'ring', 'of', 'integers', 'modulo', 'n', 'we', 'describe', 'conjugacy', 'classes', 'in', 'g', 'and', 'in', 'the', 'case', 'where', 'n', '4', 'we', 'desc... | [-0.2638378619449213, 0.038020723530927954, -0.03578283884010072, -0.025404139980279163, -0.030062103640067124, -0.14704470153329735, -0.04367646496048418, 0.35284048981838306, -0.312229418795619, -0.261896640556604, 0.07652752463887366, -0.2580973958059893, -0.10167335378306018, 0.16575269698228498, -0.053810920124336... |
707.154 | Two-Frequency Radiative Transfer. II: Maxwell Equations in Random
Dielectrics | The paper addresses the space-frequency correlations of electromagnetic waves
in general random, bi-anisotropic media whose constitutive tensors are complex
Hermitian matrices. The two-frequency Wigner distribution (2f-WD) for polarized
waves is introduced to describe the space-frequency correlations and the closed
f... | physics.optics | the paper addresses the spacefrequency correlations of electromagnetic waves in general random bianisotropic media whose constitutive tensors are complex hermitian matrices the twofrequency wigner distribution 2fwd for polarized waves is introduced to describe the spacefrequency correlations and the closed form wignerm... | [['the', 'paper', 'addresses', 'the', 'spacefrequency', 'correlations', 'of', 'electromagnetic', 'waves', 'in', 'general', 'random', 'bianisotropic', 'media', 'whose', 'constitutive', 'tensors', 'are', 'complex', 'hermitian', 'matrices', 'the', 'twofrequency', 'wigner', 'distribution', '2fwd', 'for', 'polarized', 'wave... | [-0.15629944010990962, 0.15699448300332858, -0.05180513140713346, 0.05966106562971555, -0.13383851325187576, -0.1054760737400823, -0.1051764590553297, 0.309987485254633, -0.2793245396737395, -0.19674446711252475, 0.020731027800075966, -0.31537746696989855, -0.15276621299763693, 0.15781776881937323, 0.09336795378636954,... |
707.1541 | Why we should teach the Bohr model and how to teach it effectively | Some education researchers have claimed that we should not teach the Bohr
model of the atom because it inhibits students' ability to learn the true
quantum nature of electrons in atoms. Although the evidence for this claim is
weak, many have accepted it. This claim has implications for how to present
atoms in classes... | physics.ed-ph | some education researchers have claimed that we should not teach the bohr model of the atom because it inhibits students ability to learn the true quantum nature of electrons in atoms although the evidence for this claim is weak many have accepted it this claim has implications for how to present atoms in classes rangi... | [['some', 'education', 'researchers', 'have', 'claimed', 'that', 'we', 'should', 'not', 'teach', 'the', 'bohr', 'model', 'of', 'the', 'atom', 'because', 'it', 'inhibits', 'students', 'ability', 'to', 'learn', 'the', 'true', 'quantum', 'nature', 'of', 'electrons', 'in', 'atoms', 'although', 'the', 'evidence', 'for', 'th... | [0.031294392062657765, 0.10087989312384847, -0.116090103317567, 0.11676469566376228, -0.1138839802772897, -0.20086023941015205, 0.04750043860205063, 0.39733488126506467, -0.1971491316879524, -0.3709657156378091, 0.010212835974090286, -0.2792967469620753, -0.16246498036089474, 0.2116546618273743, -0.07771364678590884, -... |
707.1542 | Noncommutative geometry through monoidal categories I | After introducing a noncommutative counterpart of commutative algebraic
geometry based on monoidal categories of quasi-coherent sheaves we show that
various constructions in noncommutative geometry (e.g. Morita equivalences,
Hopf-Galois extensions) can be given geometric meaning extending their
geometric interpretati... | math.AG math.KT | after introducing a noncommutative counterpart of commutative algebraic geometry based on monoidal categories of quasicoherent sheaves we show that various constructions in noncommutative geometry eg morita equivalences hopfgalois extensions can be given geometric meaning extending their geometric interpretations in th... | [['after', 'introducing', 'a', 'noncommutative', 'counterpart', 'of', 'commutative', 'algebraic', 'geometry', 'based', 'on', 'monoidal', 'categories', 'of', 'quasicoherent', 'sheaves', 'we', 'show', 'that', 'various', 'constructions', 'in', 'noncommutative', 'geometry', 'eg', 'morita', 'equivalences', 'hopfgalois', 'ex... | [-0.15733068005534487, 0.03327270851750831, -0.12971111725636045, 0.16426886978007635, -0.15182437747716904, -0.21037179179652368, -0.09631972649311014, 0.37278996449578733, -0.455492714282071, -0.20513697648850424, 0.1179164132347457, -0.14662744507229733, -0.2053629533044126, 0.19936510916229663, -0.2982007947081284,... |
707.1543 | A New Experiment to Study Hyperon CP Violation and the Charmonium System | Fermilab operates the world's most intense antiproton source, now exclusively
dedicated to serving the needs of the Tevatron Collider. The anticipated 2009
shutdown of the Tevatron presents the opportunity for a world-leading low- and
medium-energy antiproton program. We summarize the status of the Fermilab
antiproto... | hep-ex | fermilab operates the worlds most intense antiproton source now exclusively dedicated to serving the needs of the tevatron collider the anticipated 2009 shutdown of the tevatron presents the opportunity for a worldleading low and mediumenergy antiproton program we summarize the status of the fermilab antiproton facilit... | [['fermilab', 'operates', 'the', 'worlds', 'most', 'intense', 'antiproton', 'source', 'now', 'exclusively', 'dedicated', 'to', 'serving', 'the', 'needs', 'of', 'the', 'tevatron', 'collider', 'the', 'anticipated', '2009', 'shutdown', 'of', 'the', 'tevatron', 'presents', 'the', 'opportunity', 'for', 'a', 'worldleading', ... | [-0.05755507961281987, 0.18343328883046986, -0.13272936932254034, 0.1269239641184018, -0.1775582115028481, -0.13795704909096487, 0.05917476511514578, 0.2870005956912016, -0.16170000139295626, -0.3532402557320893, 0.0695242886736867, -0.39279929090474475, 0.10443061399349912, 0.2256959820715863, 0.0464850837578539, 0.13... |
707.1544 | Quintessential Kination and Leptogenesis | Thermal leptogenesis induced by the CP-violating decay of a right-handed
neutrino (RHN) is discussed in the background of quintessential kination, i.e.,
in a cosmological model where the energy density of the early Universe is
assumed to be dominated by the kinetic term of a quintessence field during some
epoch of it... | astro-ph hep-ph | thermal leptogenesis induced by the cpviolating decay of a righthanded neutrino rhn is discussed in the background of quintessential kination ie in a cosmological model where the energy density of the early universe is assumed to be dominated by the kinetic term of a quintessence field during some epoch of its evolutio... | [['thermal', 'leptogenesis', 'induced', 'by', 'the', 'cpviolating', 'decay', 'of', 'a', 'righthanded', 'neutrino', 'rhn', 'is', 'discussed', 'in', 'the', 'background', 'of', 'quintessential', 'kination', 'ie', 'in', 'a', 'cosmological', 'model', 'where', 'the', 'energy', 'density', 'of', 'the', 'early', 'universe', 'is... | [-0.11081883133297335, 0.3040661429351365, -0.039052945432944616, 0.13912175530699092, -0.058421879772746856, -0.14732626525537026, 0.03387163758320226, 0.29097360170227615, -0.24170768771066584, -0.322050058562044, 0.0557998835998164, -0.2524524202665568, 0.03436467806750443, 0.16971705582303306, 0.0486521670748268, -... |
707.1545 | Dynamics in Nonlocal Cosmological Models Derived from String Field
Theory | A general class of nonlocal cosmological models is considered. A new method
for solving nonlocal Friedmann equations is proposed, and solutions of the
Friedmann equations with nonlocal operator are presented. The cosmological
properties of these solutions are discussed. Especially indicated is $p$-adic
cosmological m... | hep-th astro-ph gr-qc | a general class of nonlocal cosmological models is considered a new method for solving nonlocal friedmann equations is proposed and solutions of the friedmann equations with nonlocal operator are presented the cosmological properties of these solutions are discussed especially indicated is padic cosmological model in w... | [['a', 'general', 'class', 'of', 'nonlocal', 'cosmological', 'models', 'is', 'considered', 'a', 'new', 'method', 'for', 'solving', 'nonlocal', 'friedmann', 'equations', 'is', 'proposed', 'and', 'solutions', 'of', 'the', 'friedmann', 'equations', 'with', 'nonlocal', 'operator', 'are', 'presented', 'the', 'cosmological',... | [-0.13096805640703274, 0.028991888515237305, -0.1016592357462893, 0.08687045181480547, -0.11519338358452337, -0.2131323030606533, -0.11494800274182732, 0.28888970213010906, -0.23224325614670913, -0.2778575442213979, 0.07413453318489095, -0.27254942268547083, -0.10805453755375412, 0.192001496333008, 0.003860200320680936... |
707.1546 | Producing an Intense, Cool Muon Beam via e+e- Annihilation | We consider a highly unconventional approach to generating muon and antimuon
bunches for a neutrino factory or muon collider: electron-positron annihilation
just above muon-antimuon threshold. This approach can produce low-emittance
bunches at high energy, easing the muon-cooling and acceleration challenges in
such f... | physics.acc-ph | we consider a highly unconventional approach to generating muon and antimuon bunches for a neutrino factory or muon collider electronpositron annihilation just above muonantimuon threshold this approach can produce lowemittance bunches at high energy easing the muoncooling and acceleration challenges in such facilities... | [['we', 'consider', 'a', 'highly', 'unconventional', 'approach', 'to', 'generating', 'muon', 'and', 'antimuon', 'bunches', 'for', 'a', 'neutrino', 'factory', 'or', 'muon', 'collider', 'electronpositron', 'annihilation', 'just', 'above', 'muonantimuon', 'threshold', 'this', 'approach', 'can', 'produce', 'lowemittance', ... | [-0.09305012443440665, 0.2402635964919144, -0.031375450613370666, 0.18975783060272028, -0.08014116385085902, -0.17479249653340856, 0.03356918879509182, 0.37952626716922705, -0.21503665101465205, -0.3232903057761805, 0.03115885740664171, -0.32602621919252506, 0.055256033273623655, 0.25005077823511207, 0.0079748349487256... |
707.1547 | The Next Geminga: Search for Radio and X-ray Pulsations from the Neutron
Star Identified with 3EG J1835+5918 | We report unsuccessful searches for pulsations from the neutron star RX
J1836.2+5925 identified with the EGRET source 3EG J1835+5918. A 24 hr
observation with the NRAO Green Bank Telescope at 820 MHz placed an upper limit
on flux density of 17 uJy for P > 10 ms, and gradually increasing limits for 1
< P < 10 ms. The ... | astro-ph | we report unsuccessful searches for pulsations from the neutron star rx j183625925 identified with the egret source 3eg j18355918 a 24 hr observation with the nrao green bank telescope at 820 mhz placed an upper limit on flux density of 17 ujy for p 10 ms and gradually increasing limits for 1 p 10 ms the equivalent lum... | [['we', 'report', 'unsuccessful', 'searches', 'for', 'pulsations', 'from', 'the', 'neutron', 'star', 'rx', 'j183625925', 'identified', 'with', 'the', 'egret', 'source', '3eg', 'j18355918', 'a', '24', 'hr', 'observation', 'with', 'the', 'nrao', 'green', 'bank', 'telescope', 'at', '820', 'mhz', 'placed', 'an', 'upper', '... | [-0.10842088158579682, 0.13245832559635762, -0.027607413372198974, 0.08435979963086598, -0.133009014108789, -0.13184996319621384, 0.13627707174866, 0.4294396886976314, -0.16133202661794968, -0.380027418531843, 0.12291653930137769, -0.3572239297252827, 0.04374203475945081, 0.26662119785726296, -0.009622884376538117, -0.... |
707.1548 | Data Mining-based Materialized View and Index Selection in Data
Warehouses | Materialized views and indexes are physical structures for accelerating data
access that are casually used in data warehouses. However, these data
structures generate some maintenance overhead. They also share the same storage
space. Most existing studies about materialized view and index selection
consider these str... | cs.DB | materialized views and indexes are physical structures for accelerating data access that are casually used in data warehouses however these data structures generate some maintenance overhead they also share the same storage space most existing studies about materialized view and index selection consider these structure... | [['materialized', 'views', 'and', 'indexes', 'are', 'physical', 'structures', 'for', 'accelerating', 'data', 'access', 'that', 'are', 'casually', 'used', 'in', 'data', 'warehouses', 'however', 'these', 'data', 'structures', 'generate', 'some', 'maintenance', 'overhead', 'they', 'also', 'share', 'the', 'same', 'storage'... | [-0.08970855498471512, 0.061426879545391645, -0.08761832767676633, 0.11057248089173999, -0.1462882168734303, -0.18113814520721253, 0.11317036813572766, 0.46862124388034526, -0.2832286374222559, -0.3702375047481977, 0.11377483542757826, -0.2925344039954675, -0.10580503566620442, 0.15370622646206847, -0.0882853985334245,... |
707.1549 | Fermi arcs in cuprate superconductors: tracking the pseudogap below Tc
and above T* | Using an energy-momentum dispersion for Bi2Sr2CaCu2O8 obtained from
angle-resolved photoelectron spectroscopy we show that the shrinking Fermi arc
model of the pseudogap is inconsistent with Raman scattering below Tc and
specific heat near T*. By simulating the quasiparticle energy dispersion curves
we show that Ferm... | cond-mat.supr-con | using an energymomentum dispersion for bi2sr2cacu2o8 obtained from angleresolved photoelectron spectroscopy we show that the shrinking fermi arc model of the pseudogap is inconsistent with raman scattering below tc and specific heat near t by simulating the quasiparticle energy dispersion curves we show that fermi arcs... | [['using', 'an', 'energymomentum', 'dispersion', 'for', 'bi2sr2cacu2o8', 'obtained', 'from', 'angleresolved', 'photoelectron', 'spectroscopy', 'we', 'show', 'that', 'the', 'shrinking', 'fermi', 'arc', 'model', 'of', 'the', 'pseudogap', 'is', 'inconsistent', 'with', 'raman', 'scattering', 'below', 'tc', 'and', 'specific... | [-0.15387933866845238, 0.21150156135155596, -0.10880245374412173, 0.05943033852209165, -0.05021954538231647, -0.12622193453178085, 0.13375305522371222, 0.4386077880583428, -0.28548307727194494, -0.2422835187020677, -0.06331593151790676, -0.4320218828679235, -0.08780066061902929, 0.26319256699988963, 0.02403859513018418... |
707.155 | Search for Single Top Quark Production Using Likelihood Discriminants at
D0 in Run II | We present an improved search for single top quarks in two production modes,
s-channel (tb) and t-channel (tqb). The search is performed in the
electron+jets and muon+jets decay channels, with one or more b-tagged jets, on
nearly 370 pb^{-1} of D0 Run II data collected between August 2002 and October
2004. Impact-par... | hep-ex | we present an improved search for single top quarks in two production modes schannel tb and tchannel tqb the search is performed in the electronjets and muonjets decay channels with one or more btagged jets on nearly 370 pb1 of d0 run ii data collected between august 2002 and october 2004 impactparameter based bquark t... | [['we', 'present', 'an', 'improved', 'search', 'for', 'single', 'top', 'quarks', 'in', 'two', 'production', 'modes', 'schannel', 'tb', 'and', 'tchannel', 'tqb', 'the', 'search', 'is', 'performed', 'in', 'the', 'electronjets', 'and', 'muonjets', 'decay', 'channels', 'with', 'one', 'or', 'more', 'btagged', 'jets', 'on', ... | [-0.04337709394902769, 0.1600670533545461, -0.09192134672008291, 0.15466583961528818, -0.08844720375734372, -0.15261459564994817, 0.12630419936645162, 0.32976224004280763, -0.14172866635771653, -0.3421571366898306, -0.019938724576035044, -0.4082793961023236, 0.06916408097258882, 0.15003065055410203, 0.09755117386825136... |
707.1551 | Regulatory Dynamics on Random Networks: Asymptotic Periodicity and
Modularity | We study the dynamics of discrete-time regulatory networks on random
digraphs. For this we define ensembles of deterministic orbits of random
regulatory networks, and introduce some statistical indicators related to the
long-term dynamics of the system. We prove that, in a random regulatory
network, initial condition... | math.DS | we study the dynamics of discretetime regulatory networks on random digraphs for this we define ensembles of deterministic orbits of random regulatory networks and introduce some statistical indicators related to the longterm dynamics of the system we prove that in a random regulatory network initial conditions converg... | [['we', 'study', 'the', 'dynamics', 'of', 'discretetime', 'regulatory', 'networks', 'on', 'random', 'digraphs', 'for', 'this', 'we', 'define', 'ensembles', 'of', 'deterministic', 'orbits', 'of', 'random', 'regulatory', 'networks', 'and', 'introduce', 'some', 'statistical', 'indicators', 'related', 'to', 'the', 'longter... | [-0.22308581226971, 0.12554071471095085, -0.04427932603284716, 0.10356637899999441, 0.0010940671840216965, -0.15763453195104377, 0.0512244337995071, 0.4057505615055561, -0.2943534475984052, -0.14278110024170018, 0.1289200444953167, -0.24301552693359554, -0.27634137884306254, 0.13801707773236557, -0.10933923571865307, 0... |
707.1552 | Polynomials with a common composite | Let f and g be nonconstant polynomials over an arbitrary field K. In this
paper we study the intersection of the polynomial rings K[f] and K[g], and in
particular we ask whether this intersection is larger than K. We completely
resolve this question when K has characteristic zero, and in positive
characteristic we pr... | math.AG math.NT | let f and g be nonconstant polynomials over an arbitrary field k in this paper we study the intersection of the polynomial rings kf and kg and in particular we ask whether this intersection is larger than k we completely resolve this question when k has characteristic zero and in positive characteristic we present vari... | [['let', 'f', 'and', 'g', 'be', 'nonconstant', 'polynomials', 'over', 'an', 'arbitrary', 'field', 'k', 'in', 'this', 'paper', 'we', 'study', 'the', 'intersection', 'of', 'the', 'polynomial', 'rings', 'kf', 'and', 'kg', 'and', 'in', 'particular', 'we', 'ask', 'whether', 'this', 'intersection', 'is', 'larger', 'than', 'k... | [-0.19781538994067302, 0.11412243878343577, -0.07572659444442745, 0.0015261237059672505, -0.05422263586167562, -0.16228814183150309, -0.025386006731176906, 0.36614328744363484, -0.31011062879431045, -0.25693358287562507, 0.07756478057866442, -0.22975855355419345, -0.16649988731685078, 0.17932984343398425, -0.0754869823... |
707.1553 | Nonlinear Dirac Equations | We construct nonlinear extensions of Dirac's relativistic electron equation
that preserve its other desirable properties such as locality, separability,
conservation of probability and Poincar\'e invariance. We determine the
constraints that the nonlinear term must obey and classify the resultant
non-polynomial nonli... | hep-th quant-ph | we construct nonlinear extensions of diracs relativistic electron equation that preserve its other desirable properties such as locality separability conservation of probability and poincare invariance we determine the constraints that the nonlinear term must obey and classify the resultant nonpolynomial nonlinearities... | [['we', 'construct', 'nonlinear', 'extensions', 'of', 'diracs', 'relativistic', 'electron', 'equation', 'that', 'preserve', 'its', 'other', 'desirable', 'properties', 'such', 'as', 'locality', 'separability', 'conservation', 'of', 'probability', 'and', 'poincare', 'invariance', 'we', 'determine', 'the', 'constraints', ... | [-0.10020200963916741, 0.08104988062886272, -0.054826580721327636, 0.10610791970059041, -0.14954415273918645, -0.15184761080010903, -0.03375013096727372, 0.3292191707360463, -0.2806380561692274, -0.2809573619142468, 0.09944045449163413, -0.27007584689610353, -0.22710047305862266, 0.17831077152408484, -0.037002465485111... |
707.1554 | Exact Integration of the High Energy Scale in Doped Mott Insulators | We expand on our earlier work (cond-mat/0612130, Phys. Rev. Lett. {\bf 99},
46404 (2007)) in which we constructed the exact low-energy theory of a doped
Mott insulator by explicitly integrating (rather than projecting) out the
degrees of freedom far away from the chemical potential. The exact low-energy
theory contai... | cond-mat.str-el cond-mat.supr-con | we expand on our earlier work condmat0612130 phys rev lett bf 99 46404 2007 in which we constructed the exact lowenergy theory of a doped mott insulator by explicitly integrating rather than projecting out the degrees of freedom far away from the chemical potential the exact lowenergy theory contains degrees of freedom... | [['we', 'expand', 'on', 'our', 'earlier', 'work', 'condmat0612130', 'phys', 'rev', 'lett', 'bf', '99', '46404', '2007', 'in', 'which', 'we', 'constructed', 'the', 'exact', 'lowenergy', 'theory', 'of', 'a', 'doped', 'mott', 'insulator', 'by', 'explicitly', 'integrating', 'rather', 'than', 'projecting', 'out', 'the', 'de... | [-0.12882310966184984, 0.19116052622779361, -0.07290158830499942, 0.030777701672299634, -0.013418254228530541, -0.1302810021814713, 0.06615879711074134, 0.3187946785429847, -0.2306545949585381, -0.27869308622154804, -0.00701021779095754, -0.3030493367108561, -0.1526404624477783, 0.13954482101946183, 0.00841360760830520... |
707.1555 | Changeover from Glassy ferromagnetism of the orbital domain state to
long range ferromagnetic ordering in La{_{0.9}}Sr_{0.1}MnO{_3} | An attempt is made to resolve the controversy related to the low temperature
phase (ground state) of the low-doped ferromagnetic (FM)- insulator(I)
manganite through bulk magnetic measurements on La${_{0.9}}$Sr$_{0.1}$MnO${_3}$
sample. It is shown that the FM phase, formed out of well defined transition in
the low-do... | cond-mat.str-el cond-mat.mtrl-sci | an attempt is made to resolve the controversy related to the low temperature phase ground state of the lowdoped ferromagnetic fm insulatori manganite through bulk magnetic measurements on la_09sr_01mno_3 sample it is shown that the fm phase formed out of well defined transition in the lowdoped system becomes inhomogene... | [['an', 'attempt', 'is', 'made', 'to', 'resolve', 'the', 'controversy', 'related', 'to', 'the', 'low', 'temperature', 'phase', 'ground', 'state', 'of', 'the', 'lowdoped', 'ferromagnetic', 'fm', 'insulatori', 'manganite', 'through', 'bulk', 'magnetic', 'measurements', 'on', 'la_09sr_01mno_3', 'sample', 'it', 'is', 'show... | [-0.14318046897451803, 0.2266179246408696, -0.09164037964428248, 0.03508409884688557, -0.046754364600261125, -0.13335262345833984, 0.06687733120226486, 0.391286203916666, -0.2744288864289073, -0.2912711661099794, 0.06299186364414647, -0.2725234090121112, -0.1005196568166954, 0.09681166188930868, -0.002866506836363587, ... |
707.1556 | How Magnetic is the Neutrino? | The existence of a neutrino magnetic moment implies contributions to the
neutrino mass via radiative corrections. We derive model-independent
"naturalness" upper bounds on the magnetic moments of Dirac and Majorana
neutrinos, generated by physics above the electroweak scale. For Dirac
neutrinos, the bound is several ... | hep-ph | the existence of a neutrino magnetic moment implies contributions to the neutrino mass via radiative corrections we derive modelindependent naturalness upper bounds on the magnetic moments of dirac and majorana neutrinos generated by physics above the electroweak scale for dirac neutrinos the bound is several orders of... | [['the', 'existence', 'of', 'a', 'neutrino', 'magnetic', 'moment', 'implies', 'contributions', 'to', 'the', 'neutrino', 'mass', 'via', 'radiative', 'corrections', 'we', 'derive', 'modelindependent', 'naturalness', 'upper', 'bounds', 'on', 'the', 'magnetic', 'moments', 'of', 'dirac', 'and', 'majorana', 'neutrinos', 'gen... | [-0.1173559394440776, 0.3446044649612671, 0.03575572623538041, 0.2270488231635114, -0.11616142461537768, -0.11372772048637612, 0.07182679504077079, 0.26673587352686795, -0.16615815304963072, -0.39744741006523643, 0.04203176630208046, -0.31358747782373647, 0.04375954698600353, 0.2549449839317368, 0.12450642803461727, 0.... |
707.1557 | Abiotic formation of O2 and O3 in high-CO2 terrestrial atmospheres | Previous research has indicated that high amounts of ozone (O3) and oxygen
(O2) may be produced abiotically in atmospheres with high concentrations of
CO2. The abiotic production of these two gases, which are also characteristic
of photosynthetic life processes, could pose a potential "false-positive" for
remote-sens... | astro-ph | previous research has indicated that high amounts of ozone o3 and oxygen o2 may be produced abiotically in atmospheres with high concentrations of co2 the abiotic production of these two gases which are also characteristic of photosynthetic life processes could pose a potential falsepositive for remotesensing detection... | [['previous', 'research', 'has', 'indicated', 'that', 'high', 'amounts', 'of', 'ozone', 'o3', 'and', 'oxygen', 'o2', 'may', 'be', 'produced', 'abiotically', 'in', 'atmospheres', 'with', 'high', 'concentrations', 'of', 'co2', 'the', 'abiotic', 'production', 'of', 'these', 'two', 'gases', 'which', 'are', 'also', 'charact... | [-0.055626725125695484, 0.20932223896296914, 0.04640323783610522, 0.08281813572969013, 0.029866554912955208, -0.09497480491150881, 0.09211489368512762, 0.38216203048912234, -0.1688184355972661, -0.34116273939406594, 0.11795595271969468, -0.2858597468113679, -0.09582740970677062, 0.16281664246106195, -0.0670565575296023... |
707.1558 | Autonomy with regard to an Attribute | This paper presents a model of autonomy called autonomy with regard to an
attribute applicable to cognitive and not cognitive artificial agents. Three
criteria (global / partial, social / nonsocial, absolute / relative) are
defined and used to describe the main characteristics of this type of autonomy.
A software age... | cs.MA | this paper presents a model of autonomy called autonomy with regard to an attribute applicable to cognitive and not cognitive artificial agents three criteria global partial social nonsocial absolute relative are defined and used to describe the main characteristics of this type of autonomy a software agent autonomous ... | [['this', 'paper', 'presents', 'a', 'model', 'of', 'autonomy', 'called', 'autonomy', 'with', 'regard', 'to', 'an', 'attribute', 'applicable', 'to', 'cognitive', 'and', 'not', 'cognitive', 'artificial', 'agents', 'three', 'criteria', 'global', 'partial', 'social', 'nonsocial', 'absolute', 'relative', 'are', 'defined', '... | [-0.14900858181839188, 0.0019568777393336252, -0.04079803343241414, 0.03944142845963749, -0.13108455231801297, -0.19117643611971288, 0.027883183368248864, 0.41397391830881436, -0.2711442389835914, -0.33442151077712573, 0.027503068818865963, -0.20344287269593528, -0.23718228011081616, 0.1319941831054166, -0.205153043894... |
707.1559 | An accurate finite element method for elliptic interface problems | A finite element method for elliptic problems with discontinuous coefficients
is presented. The discontinuity is assumed to take place along a closed smooth
curve. The proposed method allows to deal with meshes that are not adapted to
the discontinuity line. The (nonconforming) finite element space is enriched
with l... | math.NA | a finite element method for elliptic problems with discontinuous coefficients is presented the discontinuity is assumed to take place along a closed smooth curve the proposed method allows to deal with meshes that are not adapted to the discontinuity line the nonconforming finite element space is enriched with local ba... | [['a', 'finite', 'element', 'method', 'for', 'elliptic', 'problems', 'with', 'discontinuous', 'coefficients', 'is', 'presented', 'the', 'discontinuity', 'is', 'assumed', 'to', 'take', 'place', 'along', 'a', 'closed', 'smooth', 'curve', 'the', 'proposed', 'method', 'allows', 'to', 'deal', 'with', 'meshes', 'that', 'are'... | [-0.11495168147269975, 0.012166905162413252, -0.14302589258912837, 0.03142801612777861, -0.11763778673202703, -0.13231578930704432, 0.011539831602325043, 0.4167722278472149, -0.29138908958570525, -0.15655434542250904, 0.11118340074388085, -0.2524867509352837, -0.06918956874869764, 0.22637109771709552, -0.11363175607314... |
707.156 | The Analysis of Penumbral Fine Structure Using an Advanced Inversion
Technique | We present a method to study the penumbral fine structure using data obtained
by the spectropolarimeter onboard HINODE. For the first time, the penumbral
filaments can be considered as resolved in spectropolarimetric measurements.
This enables us to use inversion codes with only one-component model
atmospheres, and t... | astro-ph | we present a method to study the penumbral fine structure using data obtained by the spectropolarimeter onboard hinode for the first time the penumbral filaments can be considered as resolved in spectropolarimetric measurements this enables us to use inversion codes with only onecomponent model atmospheres and thus ass... | [['we', 'present', 'a', 'method', 'to', 'study', 'the', 'penumbral', 'fine', 'structure', 'using', 'data', 'obtained', 'by', 'the', 'spectropolarimeter', 'onboard', 'hinode', 'for', 'the', 'first', 'time', 'the', 'penumbral', 'filaments', 'can', 'be', 'considered', 'as', 'resolved', 'in', 'spectropolarimetric', 'measur... | [-0.11269207202775819, 0.14045726495506844, -0.04820975582215854, 0.08211358638543957, -0.10783773098683667, -0.07378416862874794, -0.004182424928939385, 0.4652099668336429, -0.23593699950335392, -0.3532025141795601, 0.08158504024479646, -0.21427010730069748, -0.09843952708254508, 0.18017649549108147, -0.01311421802492... |
707.1561 | The Reionization and Galaxy Evolution Probed by z=7 Lyman Alpha Emitters | We made a narrowband NB973 (bandwidth of 200A at 9755A) imaging of the Subaru
Deep Field (SDF) and found two z=7 Lyman alpha emitter (LAE) candidates down to
NB973=24.9. Carrying out deep follow-up spectroscopy, we identified one of them
as a real z=6.96 LAE. This has shown that galaxy formation was in progress just
... | astro-ph | we made a narrowband nb973 bandwidth of 200a at 9755a imaging of the subaru deep field sdf and found two z7 lyman alpha emitter lae candidates down to nb973249 carrying out deep followup spectroscopy we identified one of them as a real z696 lae this has shown that galaxy formation was in progress just 750 myr after the... | [['we', 'made', 'a', 'narrowband', 'nb973', 'bandwidth', 'of', '200a', 'at', '9755a', 'imaging', 'of', 'the', 'subaru', 'deep', 'field', 'sdf', 'and', 'found', 'two', 'z7', 'lyman', 'alpha', 'emitter', 'lae', 'candidates', 'down', 'to', 'nb973249', 'carrying', 'out', 'deep', 'followup', 'spectroscopy', 'we', 'identifie... | [-0.022535393156899636, 0.09901056917946749, -0.06518383761913986, 0.08813425186459012, -0.07596395232733155, -0.08493730828331986, 0.05363077974398759, 0.4609857884899593, -0.10229279927097924, -0.35327468498029035, -0.0034575480176049452, -0.32229571486131686, -0.03772441838582111, 0.15417077223249334, 0.051689304393... |
707.1562 | Percolation cluster formation at ultrarelativistic heavy ion collisions | We expect that the experimental study of percolation cluster formation and
appearance of the critical transparency of the strongly interacting matter can
give the information about the onset state of deconfinement.
| nucl-ex | we expect that the experimental study of percolation cluster formation and appearance of the critical transparency of the strongly interacting matter can give the information about the onset state of deconfinement | [['we', 'expect', 'that', 'the', 'experimental', 'study', 'of', 'percolation', 'cluster', 'formation', 'and', 'appearance', 'of', 'the', 'critical', 'transparency', 'of', 'the', 'strongly', 'interacting', 'matter', 'can', 'give', 'the', 'information', 'about', 'the', 'onset', 'state', 'of', 'deconfinement']] | [-0.1525915215512918, 0.222666296567167, -0.13851846389076355, 0.07998556998227874, -0.04928834724330133, -0.0553434825231952, 0.07000520897488441, 0.3212222447318415, -0.20116352304936416, -0.308532833211845, 0.09320226622625224, -0.28857978637660703, -0.1355229763824853, 0.0729640866479566, 0.05912988428627291, -0.00... |
707.1563 | Rare Decay Modes of Quarter BPS Dyons | The degeneracy of quarter BPS dyons in N=4 supersymmetric string theories is
known to jump across walls of marginal stability on which a quarter BPS dyon
can decay into a pair of half BPS dyons. We show that as long as the electric
and magnetic charges of the original dyon are primitive elements of the charge
lattice... | hep-th | the degeneracy of quarter bps dyons in n4 supersymmetric string theories is known to jump across walls of marginal stability on which a quarter bps dyon can decay into a pair of half bps dyons we show that as long as the electric and magnetic charges of the original dyon are primitive elements of the charge lattice the... | [['the', 'degeneracy', 'of', 'quarter', 'bps', 'dyons', 'in', 'n4', 'supersymmetric', 'string', 'theories', 'is', 'known', 'to', 'jump', 'across', 'walls', 'of', 'marginal', 'stability', 'on', 'which', 'a', 'quarter', 'bps', 'dyon', 'can', 'decay', 'into', 'a', 'pair', 'of', 'half', 'bps', 'dyons', 'we', 'show', 'that'... | [-0.1688218164911422, 0.21389236772576203, -0.023727039978481256, 0.12796438021334605, -0.04263674018438905, -0.13828019233993613, 0.03563655288890004, 0.29709873291878747, -0.1560943866506792, -0.26303157532014526, 0.09774792271827419, -0.3103460085649903, -0.0748688076586964, 0.15796187041112436, -0.03978919829600132... |
707.1564 | Orbital-Driven Electronic Structure Changes and the Resulting Optical
Anisotropy of the Quasi-Two-Dimensional Spin Gap Compound La4Ru2O10 | We investigated the electronic response of the quasi-two-dimensional spin gap
compound La4Ru2O10 using optical spectroscopy. We observed drastic changes in
the optical spectra as the temperature decreased, resulting in anisotropy in
the electronic structure of the spin-singlet ground state. Using the
orbital-dependen... | cond-mat.str-el | we investigated the electronic response of the quasitwodimensional spin gap compound la4ru2o10 using optical spectroscopy we observed drastic changes in the optical spectra as the temperature decreased resulting in anisotropy in the electronic structure of the spinsinglet ground state using the orbitaldependent hopping... | [['we', 'investigated', 'the', 'electronic', 'response', 'of', 'the', 'quasitwodimensional', 'spin', 'gap', 'compound', 'la4ru2o10', 'using', 'optical', 'spectroscopy', 'we', 'observed', 'drastic', 'changes', 'in', 'the', 'optical', 'spectra', 'as', 'the', 'temperature', 'decreased', 'resulting', 'in', 'anisotropy', 'i... | [-0.21132945053146354, 0.1785706915220039, -0.060325628656539176, 0.041155902521004754, 0.0016792005608006128, -0.0487563270957224, 0.09242850256388978, 0.4241669434640143, -0.2833620850292463, -0.29455020450173863, -0.016601170762442052, -0.3080964595789001, -0.1437385393868363, 0.12246148678518477, 0.1128657650025118... |
707.1565 | Quantum state of an injected TROPO above threshold : purity, Glauber
function and photon number distribution | In this paper we investigate several properties of the full signal-idler-pump
mode quantum state generated by a triply resonant non-degenerate Optical
Parametric Oscillator operating above threshold, with an injected wave on the
signal and idler modes in order to lock the phase diffusion process. We
determine and dis... | quant-ph | in this paper we investigate several properties of the full signalidlerpump mode quantum state generated by a triply resonant nondegenerate optical parametric oscillator operating above threshold with an injected wave on the signal and idler modes in order to lock the phase diffusion process we determine and discuss th... | [['in', 'this', 'paper', 'we', 'investigate', 'several', 'properties', 'of', 'the', 'full', 'signalidlerpump', 'mode', 'quantum', 'state', 'generated', 'by', 'a', 'triply', 'resonant', 'nondegenerate', 'optical', 'parametric', 'oscillator', 'operating', 'above', 'threshold', 'with', 'an', 'injected', 'wave', 'on', 'the... | [-0.13383299645845048, 0.18110646793006038, -0.0890020694865217, 0.050372433050537534, 0.005288913521135963, -0.10581888139334529, 0.060819957339450316, 0.3814477178650771, -0.2506635854464717, -0.25797472610463235, 0.07242309247403471, -0.27344772553923286, -0.062200531294901475, 0.17614305278019216, 0.027320583841886... |
707.1566 | K theory of smooth complete toric varieties and related spaces | The K-rings of non-singular complex pro jective varieties as well as quasi-
toric manifolds were described in terms of generators and relations in an
earlier work of the author with V. Uma. In this paper we obtain a similar
description for complete non-singular toric varieties. Indeed, our approach
enables us to obta... | math.AT math.AG | the krings of nonsingular complex pro jective varieties as well as quasi toric manifolds were described in terms of generators and relations in an earlier work of the author with v uma in this paper we obtain a similar description for complete nonsingular toric varieties indeed our approach enables us to obtain such a ... | [['the', 'krings', 'of', 'nonsingular', 'complex', 'pro', 'jective', 'varieties', 'as', 'well', 'as', 'quasi', 'toric', 'manifolds', 'were', 'described', 'in', 'terms', 'of', 'generators', 'and', 'relations', 'in', 'an', 'earlier', 'work', 'of', 'the', 'author', 'with', 'v', 'uma', 'in', 'this', 'paper', 'we', 'obtain'... | [-0.12992391085143723, 0.002762031443425046, -0.09004293053015454, 0.07494485193117177, -0.10267795436722163, -0.14215167290977623, -0.058340776824928206, 0.326561714484267, -0.24040189243164167, -0.2487788075096395, 0.08424463576464977, -0.22701036815263637, -0.1894291382321246, 0.22889701423732794, -0.183215495549805... |
707.1567 | Theory for ultrafast nonequilibrium dynamics in d-wave superconductors | We use density-matrix theory to calculate the ultrafast dynamics of
unconventional superconductors from a microscopic viewpoint. We calculate the
time evolution of the optical conductivity as well as pump-probe spectra for a
d-wave order parameter. Three regimes can be distinguished in the spectra. The
Drude response... | cond-mat.supr-con cond-mat.str-el | we use densitymatrix theory to calculate the ultrafast dynamics of unconventional superconductors from a microscopic viewpoint we calculate the time evolution of the optical conductivity as well as pumpprobe spectra for a dwave order parameter three regimes can be distinguished in the spectra the drude response at low ... | [['we', 'use', 'densitymatrix', 'theory', 'to', 'calculate', 'the', 'ultrafast', 'dynamics', 'of', 'unconventional', 'superconductors', 'from', 'a', 'microscopic', 'viewpoint', 'we', 'calculate', 'the', 'time', 'evolution', 'of', 'the', 'optical', 'conductivity', 'as', 'well', 'as', 'pumpprobe', 'spectra', 'for', 'a', ... | [-0.09046453895727889, 0.2099882217639516, -0.09973782570395842, 0.10063533914975949, -0.042093980472343855, -0.14883058960350531, 0.04353228749002879, 0.3816171874984717, -0.2683428526143583, -0.28763168986536497, 0.034280613417991906, -0.3240280957100515, -0.09271476071916966, 0.19229672294563782, 0.07240180252915901... |
707.1568 | Rapidly Rotating Bose-Einstein Condensates in Homogeneous Traps | We extend the results of a previous paper on the Gross-Pitaevskii description
of rotating Bose-Einstein condensates in two-dimensional traps to confining
potentials of the form V(r) = r^s, $2<s <\infty$. Writing the coupling constant
as $1/\epsilon^2$ we study the limit $\epsilon \to 0$. We derive rigorously the
lead... | math-ph cond-mat.other cond-mat.stat-mech math.MP | we extend the results of a previous paper on the grosspitaevskii description of rotating boseeinstein condensates in twodimensional traps to confining potentials of the form vr rs 2s infty writing the coupling constant as 1epsilon2 we study the limit epsilon to 0 we derive rigorously the leading asymptotics of the grou... | [['we', 'extend', 'the', 'results', 'of', 'a', 'previous', 'paper', 'on', 'the', 'grosspitaevskii', 'description', 'of', 'rotating', 'boseeinstein', 'condensates', 'in', 'twodimensional', 'traps', 'to', 'confining', 'potentials', 'of', 'the', 'form', 'vr', 'rs', '2s', 'infty', 'writing', 'the', 'coupling', 'constant', ... | [-0.1699163088857939, 0.11898758813231901, -0.061553298478026555, 0.04974192347454166, -0.0021847950978369653, -0.14512934374233968, 0.043734681687930814, 0.3196358035872631, -0.1998840953854113, -0.21694171558358247, 0.045937006808286884, -0.29053171808371625, -0.07309268045981851, 0.09171553057046677, 0.0083089787100... |
707.1569 | Cell-to-Cell stochastic fluctuations in apoptotic signaling can decide
between life and death | Apoptosis, or genetically programmed cell death, is a crucial cellular
process that maintains the balance between life and death in cells. The precise
molecular mechanism of apoptosis signaling and how these two pathways are
differentially activated under distinct apoptotic stimuli is poorly understood.
We developed ... | q-bio.MN physics.bio-ph physics.med-ph | apoptosis or genetically programmed cell death is a crucial cellular process that maintains the balance between life and death in cells the precise molecular mechanism of apoptosis signaling and how these two pathways are differentially activated under distinct apoptotic stimuli is poorly understood we developed a mont... | [['apoptosis', 'or', 'genetically', 'programmed', 'cell', 'death', 'is', 'a', 'crucial', 'cellular', 'process', 'that', 'maintains', 'the', 'balance', 'between', 'life', 'and', 'death', 'in', 'cells', 'the', 'precise', 'molecular', 'mechanism', 'of', 'apoptosis', 'signaling', 'and', 'how', 'these', 'two', 'pathways', '... | [-0.13161423420977025, 0.18349655934189169, -0.008144162413845588, 0.10379970630154008, 0.004318602427485443, -0.18145615960273778, 0.12340008466629497, 0.35423746720375693, -0.29203537125664547, -0.22627939248255463, 0.04922646406011906, -0.22822055519756043, -0.2758331098800396, 0.16411210280702979, -0.09607575933985... |
707.157 | About the isotropy constant of random convex sets | Let K be the symmetric convex hull of m independent random vectors uniformly
distributed on the unit sphere of R^n. We prove that, for every $\delta>0$, the
isotropy constant of K is bounded by a constant $c(\delta)$ with high
probability, provided that $m\geq (1+\delta)n$.
| math.MG math.FA | let k be the symmetric convex hull of m independent random vectors uniformly distributed on the unit sphere of rn we prove that for every delta0 the isotropy constant of k is bounded by a constant cdelta with high probability provided that mgeq 1deltan | [['let', 'k', 'be', 'the', 'symmetric', 'convex', 'hull', 'of', 'm', 'independent', 'random', 'vectors', 'uniformly', 'distributed', 'on', 'the', 'unit', 'sphere', 'of', 'rn', 'we', 'prove', 'that', 'for', 'every', 'delta0', 'the', 'isotropy', 'constant', 'of', 'k', 'is', 'bounded', 'by', 'a', 'constant', 'cdelta', 'wi... | [-0.22762737135318192, 0.19695577628656544, 0.0036004127680578017, -0.10027084462820891, -0.028844678583978253, -0.22076686863411768, 0.04329742575910958, 0.3498481120914221, -0.31208528588864615, -0.13161750000224196, 0.09805951636834917, -0.3176164760000326, -0.055356237487020815, 0.13937640976986254, -0.066723116186... |
707.1571 | Observations on the motion of a Tachyon | Some aspects of the motion of a tachyon is discussed. It is shown that the
inertial frame Sigma-Prime around which the tachyon switches the direction of
its motion, does not observe any movement of the tachyon at all. Inertial
frames on either side of Sigma-Prime observe the tachyon to be moving at very
large speeds ... | physics.gen-ph | some aspects of the motion of a tachyon is discussed it is shown that the inertial frame sigmaprime around which the tachyon switches the direction of its motion does not observe any movement of the tachyon at all inertial frames on either side of sigmaprime observe the tachyon to be moving at very large speeds but in ... | [['some', 'aspects', 'of', 'the', 'motion', 'of', 'a', 'tachyon', 'is', 'discussed', 'it', 'is', 'shown', 'that', 'the', 'inertial', 'frame', 'sigmaprime', 'around', 'which', 'the', 'tachyon', 'switches', 'the', 'direction', 'of', 'its', 'motion', 'does', 'not', 'observe', 'any', 'movement', 'of', 'the', 'tachyon', 'at... | [-0.15738470942163812, 0.17630838090493248, -0.1109999828763242, 0.055558110317741966, -0.11643064408175026, -0.1657956794342248, 0.013831651185249766, 0.35369249907255706, -0.28138221173902, -0.2639187484829953, 0.09262298713188752, -0.2513909354706162, -0.0884830174452093, 0.19444173269896833, -0.10089663850764434, -... |
707.1572 | Switched Control of Electron Nuclear Spin Systems | In this article, we study control of electron-nuclear spin dynamics at
magnetic field strengths where the Larmor frequency of the nucleus is
comparable to the hyperfine coupling strength. The quantization axis for the
nuclear spin differs from the static B_0 field direction and depends on the
state of the electron sp... | quant-ph | in this article we study control of electronnuclear spin dynamics at magnetic field strengths where the larmor frequency of the nucleus is comparable to the hyperfine coupling strength the quantization axis for the nuclear spin differs from the static b_0 field direction and depends on the state of the electron spin th... | [['in', 'this', 'article', 'we', 'study', 'control', 'of', 'electronnuclear', 'spin', 'dynamics', 'at', 'magnetic', 'field', 'strengths', 'where', 'the', 'larmor', 'frequency', 'of', 'the', 'nucleus', 'is', 'comparable', 'to', 'the', 'hyperfine', 'coupling', 'strength', 'the', 'quantization', 'axis', 'for', 'the', 'nuc... | [-0.129935875773929, 0.22768787893290127, -0.04593263155464205, 0.01656683993197101, -0.031817934548123164, -0.12695684107446592, 0.01475452667093087, 0.40725059727559876, -0.2772951750023887, -0.265959202391065, 0.06584464329115292, -0.218388007631148, -0.04069233804125509, 0.2258155289428686, 0.034626253606641996, 0.... |
707.1573 | X-ray measured metallicities of the intra-cluster medium: a good measure
for the metal mass? | Aims. We investigate whether X-ray observations map heavy elements in the
Intra-Cluster Medium (ICM) well and whether the X-ray observations yield good
estimates for the metal mass, with respect to predictions on transport mech-
anisms of heavy elements from galaxies into the ICM. We further test the
accuracy of simu... | astro-ph | aims we investigate whether xray observations map heavy elements in the intracluster medium icm well and whether the xray observations yield good estimates for the metal mass with respect to predictions on transport mech anisms of heavy elements from galaxies into the icm we further test the accuracy of simulated metal... | [['aims', 'we', 'investigate', 'whether', 'xray', 'observations', 'map', 'heavy', 'elements', 'in', 'the', 'intracluster', 'medium', 'icm', 'well', 'and', 'whether', 'the', 'xray', 'observations', 'yield', 'good', 'estimates', 'for', 'the', 'metal', 'mass', 'with', 'respect', 'to', 'predictions', 'on', 'transport', 'me... | [0.00144591986923022, 0.11580392398195816, -0.05397228609003565, 0.10926053586972914, -0.004769396268780909, -0.060750750969072766, 0.0792009245654495, 0.4558026343437971, -0.2093737605228728, -0.348069858422512, 0.035194137122244666, -0.377709262474787, -0.05019577494731137, 0.21667470493920002, 0.013411128519595984, ... |
707.1574 | Three loop anomalous dimensions of twist-3 gauge operators in N=4 SYM | We propose a closed expression for the three loop anomalous dimension of a
class of twist-3 operators built with gauge fields and covariant derivatives.
To this aim, we solve the long-range Bethe Ansatz equations at finite spin and
provide a consistent analytical formula obtained assuming maximal
transcendentality vi... | hep-th | we propose a closed expression for the three loop anomalous dimension of a class of twist3 operators built with gauge fields and covariant derivatives to this aim we solve the longrange bethe ansatz equations at finite spin and provide a consistent analytical formula obtained assuming maximal transcendentality violatio... | [['we', 'propose', 'a', 'closed', 'expression', 'for', 'the', 'three', 'loop', 'anomalous', 'dimension', 'of', 'a', 'class', 'of', 'twist3', 'operators', 'built', 'with', 'gauge', 'fields', 'and', 'covariant', 'derivatives', 'to', 'this', 'aim', 'we', 'solve', 'the', 'longrange', 'bethe', 'ansatz', 'equations', 'at', '... | [-0.18803713963318028, 0.15272312434880356, -0.08979308799423866, 0.16668114624151617, -0.13017064295892947, -0.15659528182157756, 0.036488329378986044, 0.23285971660363047, -0.20605478798480412, -0.24039479309201278, 0.020161347093036103, -0.24632988705937015, -0.18513493552975552, 0.1481675536396276, 0.02796283877442... |
707.1575 | Entanglement of a class of mixed two - qutrit states | We compute the measure of entanglement for some classes of states belonging
to the simplex of Bell - diagonal states of two qutrits.
| quant-ph | we compute the measure of entanglement for some classes of states belonging to the simplex of bell diagonal states of two qutrits | [['we', 'compute', 'the', 'measure', 'of', 'entanglement', 'for', 'some', 'classes', 'of', 'states', 'belonging', 'to', 'the', 'simplex', 'of', 'bell', 'diagonal', 'states', 'of', 'two', 'qutrits']] | [-0.15554616329344836, 0.19499761192128062, -0.02156852985816923, 0.06925489194691181, 0.09294155087660659, -0.22192308196628635, 0.06759342652830211, 0.28885419565168297, -0.2237023834059073, -0.20647862943058665, 0.04615440683185377, -0.3349933996796608, -0.028094462542371315, 0.15875264363024721, -0.0098984545858746... |
707.1576 | Symbol calculus and zeta--function regularized determinants | In this work, we use semigroup integral to evaluate zeta-function regularized
determinants. This is especially powerful for non--positive operators such as
the Dirac operator. In order to understand fully the quantum effective action
one should know not only the potential term but also the leading kinetic term.
In th... | math-ph math.MP | in this work we use semigroup integral to evaluate zetafunction regularized determinants this is especially powerful for nonpositive operators such as the dirac operator in order to understand fully the quantum effective action one should know not only the potential term but also the leading kinetic term in this purpos... | [['in', 'this', 'work', 'we', 'use', 'semigroup', 'integral', 'to', 'evaluate', 'zetafunction', 'regularized', 'determinants', 'this', 'is', 'especially', 'powerful', 'for', 'nonpositive', 'operators', 'such', 'as', 'the', 'dirac', 'operator', 'in', 'order', 'to', 'understand', 'fully', 'the', 'quantum', 'effective', '... | [-0.12883705878359547, 0.0806458598479282, -0.07236691413116966, 0.15650980903761635, -0.1717286334145641, -0.1490408787124812, -0.005593076600086724, 0.3138846053828507, -0.2823436666918962, -0.2204145562380206, 0.10253487537793685, -0.29884030288735103, -0.20864512771368027, 0.11867262390550486, -0.036053422984645464... |
707.1577 | k-Ordered Hamilton cycles in digraphs | Given a digraph D, the minimum semi-degree of D is the minimum of its minimum
indegree and its minimum outdegree. D is k-ordered Hamiltonian if for every
ordered sequence of k distinct vertices there is a directed Hamilton cycle
which encounters these vertices in this order. Our main result is that every
digraph D of... | math.CO | given a digraph d the minimum semidegree of d is the minimum of its minimum indegree and its minimum outdegree d is kordered hamiltonian if for every ordered sequence of k distinct vertices there is a directed hamilton cycle which encounters these vertices in this order our main result is that every digraph d of suffic... | [['given', 'a', 'digraph', 'd', 'the', 'minimum', 'semidegree', 'of', 'd', 'is', 'the', 'minimum', 'of', 'its', 'minimum', 'indegree', 'and', 'its', 'minimum', 'outdegree', 'd', 'is', 'kordered', 'hamiltonian', 'if', 'for', 'every', 'ordered', 'sequence', 'of', 'k', 'distinct', 'vertices', 'there', 'is', 'a', 'directed... | [-0.2542953460639262, 0.18072302242296207, -0.04085376915906597, 0.006656827511387351, -0.05215919344766956, -0.20406257625385796, 0.058288359845629086, 0.324755218573441, -0.23462098676954274, -0.33767082489541045, 0.06641029551721421, -0.35998410846957046, -0.16401643630208285, 0.01543979935914926, -0.085371603602138... |
707.1578 | Entangled multi-qubit states without higher-tangle | We analyze mixed multi-qubit states composed of a W class state and a product
state with all qubit in |0>. We find the optimal pure state decomposition and
convex roofs for higher-tangle with bipartite partition between one qubit and
the rest qubits for those mixed states. The optimality of the decomposition is
ensur... | quant-ph | we analyze mixed multiqubit states composed of a w class state and a product state with all qubit in 0 we find the optimal pure state decomposition and convex roofs for highertangle with bipartite partition between one qubit and the rest qubits for those mixed states the optimality of the decomposition is ensured by th... | [['we', 'analyze', 'mixed', 'multiqubit', 'states', 'composed', 'of', 'a', 'w', 'class', 'state', 'and', 'a', 'product', 'state', 'with', 'all', 'qubit', 'in', '0', 'we', 'find', 'the', 'optimal', 'pure', 'state', 'decomposition', 'and', 'convex', 'roofs', 'for', 'highertangle', 'with', 'bipartite', 'partition', 'betwe... | [-0.13249268759699429, 0.21242623838924748, -0.03969350228195681, 0.04620753577362527, 0.0358923732467434, -0.275333089688245, 0.06023294597809367, 0.3118211338186965, -0.25157518261934025, -0.2640182458959958, 0.05280902494046399, -0.27015232966445824, -0.0474883757695994, 0.13441347660606398, -0.030758290190030547, 0... |
707.1579 | Stable stochastic dynamics in yeast cell cycle | Chemical reactions in cell are subject to intense stochastic fluctuations. An
important question is how the fundamental physiological behavior of cell is
kept stable against those noisy perturbations. In this paper a stochastic model
of cell cycle of budding yeast is constructed to analyze the effects of noise
on the... | q-bio.MN | chemical reactions in cell are subject to intense stochastic fluctuations an important question is how the fundamental physiological behavior of cell is kept stable against those noisy perturbations in this paper a stochastic model of cell cycle of budding yeast is constructed to analyze the effects of noise on the cel... | [['chemical', 'reactions', 'in', 'cell', 'are', 'subject', 'to', 'intense', 'stochastic', 'fluctuations', 'an', 'important', 'question', 'is', 'how', 'the', 'fundamental', 'physiological', 'behavior', 'of', 'cell', 'is', 'kept', 'stable', 'against', 'those', 'noisy', 'perturbations', 'in', 'this', 'paper', 'a', 'stocha... | [-0.16733359219506383, 0.18858390871093889, 0.0014479223245871253, 0.08431661607210117, 0.06501019519237161, -0.12432665299638757, 0.12145568892537995, 0.3475070174463326, -0.2810965830576606, -0.25211203983053565, 0.052672223921035766, -0.2453147833875846, -0.2238821209903108, 0.13303950931185682, -0.15679575589456363... |
707.158 | Theoretical Analysis of Astronomical Phased Arrays | Low-noise phased arrays are essential for the next generation of microwave
and submillimetre wave astronomy. We analyze their behaviour from a functional
perspective, and show that their operation is intimately related to the
mathematical theory of frames. No assumptions are made about the orthogonality
or linear ind... | astro-ph | lownoise phased arrays are essential for the next generation of microwave and submillimetre wave astronomy we analyze their behaviour from a functional perspective and show that their operation is intimately related to the mathematical theory of frames no assumptions are made about the orthogonality or linear independe... | [['lownoise', 'phased', 'arrays', 'are', 'essential', 'for', 'the', 'next', 'generation', 'of', 'microwave', 'and', 'submillimetre', 'wave', 'astronomy', 'we', 'analyze', 'their', 'behaviour', 'from', 'a', 'functional', 'perspective', 'and', 'show', 'that', 'their', 'operation', 'is', 'intimately', 'related', 'to', 'th... | [-0.13483358220677943, 0.10037615513832744, -0.10807498032039392, 0.082931990319893, -0.044255366092247346, -0.12706374657310304, 0.019415330029873838, 0.4075679072990052, -0.26303759496734147, -0.2851277075858126, 0.12397789201669154, -0.27208784825878307, -0.12566005599294458, 0.21352955093457093, -0.0324436545086603... |
707.1581 | Statistical Mechanics of the Fluctuating Lattice Boltzmann Equation | We propose a new formulation of the fluctuating lattice Boltzmann equation
that is consistent with both equilibrium statististical mechanics and
fluctuating hydrodynamics. The formalism is based on a generalized lattice-gas
model, with each velocity direction occupied by many particles. We show that
the most probable... | cond-mat.soft | we propose a new formulation of the fluctuating lattice boltzmann equation that is consistent with both equilibrium statististical mechanics and fluctuating hydrodynamics the formalism is based on a generalized latticegas model with each velocity direction occupied by many particles we show that the most probable state... | [['we', 'propose', 'a', 'new', 'formulation', 'of', 'the', 'fluctuating', 'lattice', 'boltzmann', 'equation', 'that', 'is', 'consistent', 'with', 'both', 'equilibrium', 'statististical', 'mechanics', 'and', 'fluctuating', 'hydrodynamics', 'the', 'formalism', 'is', 'based', 'on', 'a', 'generalized', 'latticegas', 'model... | [-0.10644571749530175, 0.18426649670602827, -0.1528854499869656, 0.05520267455568975, -0.0659726056568932, -0.13532070634107146, 0.009943306913634802, 0.30366005544024316, -0.26941476511938556, -0.2672014294354164, 0.033483847043775626, -0.27299286803851, -0.07570308319839608, 0.14959677176565214, 0.004927347682456932,... |
707.1582 | Stripe width and non-local domain walls in the two-dimensional Dipolar
Frustrated Ising Ferromagnet | We describe a novel type of magnetic domain wall which, in contrast to Bloch
or Neel walls, is non-localized and, in a certain temperature range,
non-monotonic. The wall appears as the mean-field solution of the
two-dimensional ferromagnetic Ising model frustrated by the long-ranged dipolar
interaction. We provide ex... | cond-mat.stat-mech cond-mat.mtrl-sci | we describe a novel type of magnetic domain wall which in contrast to bloch or neel walls is nonlocalized and in a certain temperature range nonmonotonic the wall appears as the meanfield solution of the twodimensional ferromagnetic ising model frustrated by the longranged dipolar interaction we provide experimental ev... | [['we', 'describe', 'a', 'novel', 'type', 'of', 'magnetic', 'domain', 'wall', 'which', 'in', 'contrast', 'to', 'bloch', 'or', 'neel', 'walls', 'is', 'nonlocalized', 'and', 'in', 'a', 'certain', 'temperature', 'range', 'nonmonotonic', 'the', 'wall', 'appears', 'as', 'the', 'meanfield', 'solution', 'of', 'the', 'twodimen... | [-0.17390978481652664, 0.21094134028053618, -0.04005963565251822, 0.029214470588064208, -0.07881327220319032, -0.11569956181458486, 0.05011921188922535, 0.3911249661047397, -0.23873161915529134, -0.2574602275251828, 0.028396570528174975, -0.2995799964952186, -0.06999222919192358, 0.13816867019290682, 0.0712739827898170... |
707.1583 | A multi-blob representation of semi-dilute polymer solutions | A coarse-grained multi-blob description of polymer solutions is presented,
based on soft, transferable effective interactions between bonded and
non-bonded blobs. The number of blobs is chosen such that the blob density does
not exceed their overlap threshold, allowing polymer concentrations to be
explored deep into ... | cond-mat.soft cond-mat.stat-mech | a coarsegrained multiblob description of polymer solutions is presented based on soft transferable effective interactions between bonded and nonbonded blobs the number of blobs is chosen such that the blob density does not exceed their overlap threshold allowing polymer concentrations to be explored deep into the semid... | [['a', 'coarsegrained', 'multiblob', 'description', 'of', 'polymer', 'solutions', 'is', 'presented', 'based', 'on', 'soft', 'transferable', 'effective', 'interactions', 'between', 'bonded', 'and', 'nonbonded', 'blobs', 'the', 'number', 'of', 'blobs', 'is', 'chosen', 'such', 'that', 'the', 'blob', 'density', 'does', 'no... | [-0.08868785817898682, 0.12184371321793945, -0.09796208369441266, 0.04646950962032652, -0.052733982689732194, -0.12671428068337598, 0.03333526192468473, 0.39456193926262445, -0.2016723103949736, -0.3101347360449533, 0.008561266430964073, -0.27490442888490085, -0.10743589669428552, 0.15559311850992, 0.014325895630379861... |
707.1584 | On the K^+D Interaction at Low Energies | The Kd reactions are considered in the impulse approximation with NN
final-state interactions (NN FSI) taken into account. The realistic parameters
for the KN phase shifts are used. The "quasi-elastic" energy region, in which
the elementary KN interaction is predominantly elastic, is considered. The
theoretical predi... | nucl-th | the kd reactions are considered in the impulse approximation with nn finalstate interactions nn fsi taken into account the realistic parameters for the kn phase shifts are used the quasielastic energy region in which the elementary kn interaction is predominantly elastic is considered the theoretical predictions are co... | [['the', 'kd', 'reactions', 'are', 'considered', 'in', 'the', 'impulse', 'approximation', 'with', 'nn', 'finalstate', 'interactions', 'nn', 'fsi', 'taken', 'into', 'account', 'the', 'realistic', 'parameters', 'for', 'the', 'kn', 'phase', 'shifts', 'are', 'used', 'the', 'quasielastic', 'energy', 'region', 'in', 'which',... | [-0.07897145873201745, 0.1947600358481785, -0.08532228878876984, 0.14133643818162714, -0.007865267766257083, -0.10560798890739014, -0.04554165618174011, 0.34227031284743653, -0.24524935793929867, -0.23249801639550632, -0.03366658084788859, -0.38404788742108004, -0.019529836943027994, 0.15781070591349686, 0.115801488678... |
707.1585 | Experimental application of sum rules for electron energy loss magnetic
chiral dichroism | We present a derivation of the orbital and spin sum rules for magnetic
circular dichroic spectra measured by electron energy loss spectroscopy in a
transmission electron microscope. These sum rules are obtained from the
differential cross section calculated for symmetric positions in the
diffraction pattern. Orbital ... | cond-mat.other | we present a derivation of the orbital and spin sum rules for magnetic circular dichroic spectra measured by electron energy loss spectroscopy in a transmission electron microscope these sum rules are obtained from the differential cross section calculated for symmetric positions in the diffraction pattern orbital and ... | [['we', 'present', 'a', 'derivation', 'of', 'the', 'orbital', 'and', 'spin', 'sum', 'rules', 'for', 'magnetic', 'circular', 'dichroic', 'spectra', 'measured', 'by', 'electron', 'energy', 'loss', 'spectroscopy', 'in', 'a', 'transmission', 'electron', 'microscope', 'these', 'sum', 'rules', 'are', 'obtained', 'from', 'the... | [-0.15800841737584007, 0.15418762047547938, -0.027835851075218583, 0.06416237655254763, -0.033119858833166156, -0.0595111260375167, 0.047667260430810016, 0.43975231199093706, -0.25869938490412586, -0.32078249970587286, -0.0007181149189042427, -0.3513344880079896, -0.0544411135963789, 0.18156903241647454, 0.084189315743... |
707.1586 | Charged-Particle Multiplicities in Charged-Current Neutrino-- and
Anti-Neutrino--Nucleus Interactions | The CHORUS experiment, designed to search for $\nu_{\mu}\to\nu_{\tau}$
oscillations, consists of a nuclear emulsion target and electronic detectors.
In this paper, results on the production of charged particles in a small sample
of charged-current neutrino-- and anti-neutrino--nucleus interactions at high
energy are ... | hep-ex | the chorus experiment designed to search for nu_mutonu_tau oscillations consists of a nuclear emulsion target and electronic detectors in this paper results on the production of charged particles in a small sample of chargedcurrent neutrino and antineutrinonucleus interactions at high energy are presented for each even... | [['the', 'chorus', 'experiment', 'designed', 'to', 'search', 'for', 'nu_mutonu_tau', 'oscillations', 'consists', 'of', 'a', 'nuclear', 'emulsion', 'target', 'and', 'electronic', 'detectors', 'in', 'this', 'paper', 'results', 'on', 'the', 'production', 'of', 'charged', 'particles', 'in', 'a', 'small', 'sample', 'of', 'c... | [-0.08574067761129053, 0.21073846383033878, -0.07253029620033573, 0.131532893869618, 0.04627350762989508, -0.06452050243069275, -0.03555126793352873, 0.36191580689301456, -0.17843099888822023, -0.3421829672136011, -0.01573611213315795, -0.377622517410421, 0.014704196204016678, 0.1708152594926842, 0.072800475036739, 0.0... |
707.1587 | Constraints on Neutralino masses and mixings from Cosmology and Collider
Physics | Bounds on cross section measurements of chargino pair production at LEP yield
a bound on the chargino mass. If the GUT relation is assumed, the lightest
neutralino must be heavier than $\approx 45 -50\GeV$. If no GUT relation is
assumed, no lower bound on the neutralino mass exists. I derive mass bounds on
the lighte... | hep-ph | bounds on cross section measurements of chargino pair production at lep yield a bound on the chargino mass if the gut relation is assumed the lightest neutralino must be heavier than approx 45 50gev if no gut relation is assumed no lower bound on the neutralino mass exists i derive mass bounds on the lightest neutralin... | [['bounds', 'on', 'cross', 'section', 'measurements', 'of', 'chargino', 'pair', 'production', 'at', 'lep', 'yield', 'a', 'bound', 'on', 'the', 'chargino', 'mass', 'if', 'the', 'gut', 'relation', 'is', 'assumed', 'the', 'lightest', 'neutralino', 'must', 'be', 'heavier', 'than', 'approx', '45', '50gev', 'if', 'no', 'gut'... | [-0.04003498764036016, 0.30165394958910635, -0.017368246238523472, 0.21786226629821057, -0.06591432674031239, -0.19267367046753256, 0.07169500080474084, 0.3133784536540689, -0.17925641738434528, -0.2895415995379962, -0.016859858148058668, -0.3729466923913505, 0.15829502871363527, 0.1675569112137762, 0.11240464106635449... |
707.1588 | A Tight Lower Bound to the Outage Probability of Discrete-Input
Block-Fading Channels | In this correspondence, we propose a tight lower bound to the outage
probability of discrete-input Nakagami-m block-fading channels. The approach
permits an efficient method for numerical evaluation of the bound, providing an
additional tool for system design. The optimal rate-diversity trade-off for the
Nakagami-m b... | cs.IT math.IT | in this correspondence we propose a tight lower bound to the outage probability of discreteinput nakagamim blockfading channels the approach permits an efficient method for numerical evaluation of the bound providing an additional tool for system design the optimal ratediversity tradeoff for the nakagamim blockfading c... | [['in', 'this', 'correspondence', 'we', 'propose', 'a', 'tight', 'lower', 'bound', 'to', 'the', 'outage', 'probability', 'of', 'discreteinput', 'nakagamim', 'blockfading', 'channels', 'the', 'approach', 'permits', 'an', 'efficient', 'method', 'for', 'numerical', 'evaluation', 'of', 'the', 'bound', 'providing', 'an', 'a... | [-0.2543545636017957, 0.02172239875888467, -0.09159021594020869, 0.09915429651324127, -0.015434706470959129, -0.26720559216975687, 0.2141983901120482, 0.37829273303730354, -0.2039760019960663, -0.2900854972146091, 0.05694809883284653, -0.17753344133586413, -0.18478437400453032, 0.2483889521550267, -0.10747229551235514,... |
707.1589 | Analytic theory of narrow lattice solitons | The profiles of narrow lattice solitons are calculated analytically using
perturbation analysis. A stability analysis shows that solitons centered at a
lattice (potential) maximum are unstable, as they drift toward the nearest
lattice minimum. This instability can, however, be so weak that the soliton is
``mathematic... | nlin.PS | the profiles of narrow lattice solitons are calculated analytically using perturbation analysis a stability analysis shows that solitons centered at a lattice potential maximum are unstable as they drift toward the nearest lattice minimum this instability can however be so weak that the soliton is mathematically unstab... | [['the', 'profiles', 'of', 'narrow', 'lattice', 'solitons', 'are', 'calculated', 'analytically', 'using', 'perturbation', 'analysis', 'a', 'stability', 'analysis', 'shows', 'that', 'solitons', 'centered', 'at', 'a', 'lattice', 'potential', 'maximum', 'are', 'unstable', 'as', 'they', 'drift', 'toward', 'the', 'nearest',... | [-0.1962193176294713, 0.16582053352522758, -0.09054409508239622, 0.07464268941129017, -0.046346179083307355, -0.16817573254364868, 0.025971005955898716, 0.37303921784989014, -0.2399241840647346, -0.16062147361623455, 0.18099244893618766, -0.2622763004051088, -0.12779048636786697, 0.14311703826055336, 0.0209387280335722... |
707.159 | Tidal and rotational effects in the perturbations of hierarchical triple
stellar systems. II. Eccentric systems - the case of AS Camelopardalis | We study the perturbations of a relatively close third star on a tidally
distorted eccentric eclipsing binary. We consider both the observational
consequences of the variations of the orbital elements and the interactions of
the stellar rotation with the orbital revolution in the presence of
dissipation. We concentra... | astro-ph | we study the perturbations of a relatively close third star on a tidally distorted eccentric eclipsing binary we consider both the observational consequences of the variations of the orbital elements and the interactions of the stellar rotation with the orbital revolution in the presence of dissipation we concentrate m... | [['we', 'study', 'the', 'perturbations', 'of', 'a', 'relatively', 'close', 'third', 'star', 'on', 'a', 'tidally', 'distorted', 'eccentric', 'eclipsing', 'binary', 'we', 'consider', 'both', 'the', 'observational', 'consequences', 'of', 'the', 'variations', 'of', 'the', 'orbital', 'elements', 'and', 'the', 'interactions'... | [-0.2104625896880042, 0.1212788910889744, -0.07354142869682806, 0.08728349935944099, -0.08615477985663503, -0.03968400994630906, 0.06039948983911045, 0.34395193624462467, -0.2550296829044004, -0.3046709519506436, 0.09058345074830895, -0.25906099651377124, -0.14756473857633232, 0.2108169587828332, -0.041394677418620525,... |
707.1591 | Invisibly decaying Higgs boson in the Littlest Higgs model with T-parity | We show that there are regions in the parameter space of the Littlest Higgs
model with T-parity, allowed by electroweak precision data, where the Higgs
boson can decay invisibly into a pair of heavy photons A_H with a substantial
branching ratio. For a symmetry breaking scale f in the range 450-600 GeV, the
BR(H -> A... | hep-ph | we show that there are regions in the parameter space of the littlest higgs model with tparity allowed by electroweak precision data where the higgs boson can decay invisibly into a pair of heavy photons a_h with a substantial branching ratio for a symmetry breaking scale f in the range 450600 gev the brh a_h a_h can b... | [['we', 'show', 'that', 'there', 'are', 'regions', 'in', 'the', 'parameter', 'space', 'of', 'the', 'littlest', 'higgs', 'model', 'with', 'tparity', 'allowed', 'by', 'electroweak', 'precision', 'data', 'where', 'the', 'higgs', 'boson', 'can', 'decay', 'invisibly', 'into', 'a', 'pair', 'of', 'heavy', 'photons', 'a_h', 'w... | [-0.059787371686979895, 0.3241844822085633, 0.011879443565183985, 0.15798010847148752, -0.07147900693442873, -0.17565798193806717, 0.06859697858869497, 0.3410916318784335, -0.23462909426806228, -0.3456626186380163, 0.012238158168786737, -0.2653731173236987, 0.12344783786725852, 0.17891868534206878, 0.05851722634231139,... |
707.1592 | Light Cone QCD Sum Rules Analysis of the Axial N -> Delta Transition
Form Factors | The axial N-> Delta(1232) transition form factors are calculated within the
light cone QCD sum rules method. A comparison of our results with predictions
of lattice theory and quark model calculations is pre- sented.
| hep-ph | the axial n delta1232 transition form factors are calculated within the light cone qcd sum rules method a comparison of our results with predictions of lattice theory and quark model calculations is pre sented | [['the', 'axial', 'n', 'delta1232', 'transition', 'form', 'factors', 'are', 'calculated', 'within', 'the', 'light', 'cone', 'qcd', 'sum', 'rules', 'method', 'a', 'comparison', 'of', 'our', 'results', 'with', 'predictions', 'of', 'lattice', 'theory', 'and', 'quark', 'model', 'calculations', 'is', 'pre', 'sented']] | [-0.07161677521927391, 0.20388748941888266, -0.11462495649945648, 0.04254341110765167, -0.028488233288311782, -0.09523110775112667, 0.1500629866598448, 0.40843513862722935, -0.14139219822690768, -0.23765411458032973, -0.029282878344768986, -0.33274305036620183, -0.11695441696108044, 0.06754969521973501, 0.1256838271545... |
707.1593 | Impact of and constraints on PDFs at LHC | Uncertainties on parton distribution functions (PDFs) compromise discovery at
the LHC for any new physics which can be described as a contact-interaction.
PDF uncertainties also limit our ability to use W and Z cross-sections as an
accurate luminosity monitor. The impact of the current level of PDF uncertainty
on LHC... | hep-ph hep-ex | uncertainties on parton distribution functions pdfs compromise discovery at the lhc for any new physics which can be described as a contactinteraction pdf uncertainties also limit our ability to use w and z crosssections as an accurate luminosity monitor the impact of the current level of pdf uncertainty on lhc physics... | [['uncertainties', 'on', 'parton', 'distribution', 'functions', 'pdfs', 'compromise', 'discovery', 'at', 'the', 'lhc', 'for', 'any', 'new', 'physics', 'which', 'can', 'be', 'described', 'as', 'a', 'contactinteraction', 'pdf', 'uncertainties', 'also', 'limit', 'our', 'ability', 'to', 'use', 'w', 'and', 'z', 'crosssectio... | [-0.00329139857338025, 0.13726300691241006, -0.12767403051973536, 0.1633724449435249, -0.07062439719358315, -0.06003032804538424, 0.0570783032462574, 0.3303574338555336, -0.22348446550850684, -0.31885851196801435, 0.07577345875593332, -0.31632010638713837, 0.04966968521475792, 0.20519049257899707, 0.017584441093584667,... |
707.1594 | Scale Transformations, Tree-level Perturbation Theory, and the
Cosmological Matter Bispectrum | Scale transformations have played an extremely successful role in studies of
cosmological large-scale structure by relating the non-linear spectrum of
cosmological density fluctuations to the linear primordial power at longer
wavelengths. Here we generalize this approach to investigate the usefulness of
scale transfo... | astro-ph | scale transformations have played an extremely successful role in studies of cosmological largescale structure by relating the nonlinear spectrum of cosmological density fluctuations to the linear primordial power at longer wavelengths here we generalize this approach to investigate the usefulness of scale transformati... | [['scale', 'transformations', 'have', 'played', 'an', 'extremely', 'successful', 'role', 'in', 'studies', 'of', 'cosmological', 'largescale', 'structure', 'by', 'relating', 'the', 'nonlinear', 'spectrum', 'of', 'cosmological', 'density', 'fluctuations', 'to', 'the', 'linear', 'primordial', 'power', 'at', 'longer', 'wav... | [-0.09010113499061845, 0.11219581834598102, -0.14448961733069154, 0.1145995396627768, -0.0881612914690777, -0.09676551979100623, -0.027252292918547028, 0.3466507825651206, -0.2620812127061072, -0.3171813032022328, 0.06859156839527714, -0.23933882562550934, -0.1655651276378194, 0.20658328615536448, 0.019411666380619863,... |
707.1595 | Low Energy Supersymmetry from Non-Geometry | We study a class of flux compactifications that have all the moduli
stabilised, a high (GUT) string scale and a low (TeV) gravitino mass that is
generated dynamically. These non-geometric compactifications correspond to type
II string theories on SU(3)xSU(3) structure orientifolds. The resulting
superpotentials admit... | hep-th | we study a class of flux compactifications that have all the moduli stabilised a high gut string scale and a low tev gravitino mass that is generated dynamically these nongeometric compactifications correspond to type ii string theories on su3xsu3 structure orientifolds the resulting superpotentials admit excluding non... | [['we', 'study', 'a', 'class', 'of', 'flux', 'compactifications', 'that', 'have', 'all', 'the', 'moduli', 'stabilised', 'a', 'high', 'gut', 'string', 'scale', 'and', 'a', 'low', 'tev', 'gravitino', 'mass', 'that', 'is', 'generated', 'dynamically', 'these', 'nongeometric', 'compactifications', 'correspond', 'to', 'type'... | [-0.16512570406371, 0.32002577983847635, -0.04273341929378069, 0.20748146495113717, -0.10699545897381461, -0.16520243881918165, -0.019509117220244978, 0.3084831057359343, -0.16378012932027164, -0.29175739697302167, 0.1113793949626953, -0.21306593130626109, -0.10070134232063656, 0.09144170682715333, -0.0980589186610735,... |
707.1596 | From Useful Algorithms for Slowly Convergent Series to Physical
Predictions Based on Divergent Perturbative Expansions | This review is focused on the borderline region of theoretical physics and
mathematics. First, we describe numerical methods for the acceleration of the
convergence of series. These provide a useful toolbox for theoretical physics
which has hitherto not received the attention it actually deserves. The
unifying concep... | physics.comp-ph physics.atom-ph | this review is focused on the borderline region of theoretical physics and mathematics first we describe numerical methods for the acceleration of the convergence of series these provide a useful toolbox for theoretical physics which has hitherto not received the attention it actually deserves the unifying concept for ... | [['this', 'review', 'is', 'focused', 'on', 'the', 'borderline', 'region', 'of', 'theoretical', 'physics', 'and', 'mathematics', 'first', 'we', 'describe', 'numerical', 'methods', 'for', 'the', 'acceleration', 'of', 'the', 'convergence', 'of', 'series', 'these', 'provide', 'a', 'useful', 'toolbox', 'for', 'theoretical',... | [-0.07125090148740558, 0.04897631454535203, -0.11051584960305295, 0.09553537076492677, -0.10122381943014307, -0.11797755075899023, 0.021752046356495056, 0.3378392791969695, -0.24502259659527478, -0.2383821646993359, 0.1391370373813095, -0.2537348407669507, -0.15260378962656396, 0.2465709082032871, -0.04430773462292798,... |
707.1597 | Toric Resolutions of Heterotic Orbifolds | We investigate resolutions of heterotic orbifolds using toric geometry. Our
starting point is provided by the recently constructed heterotic models on
explicit blowup of C^n/Z_n singularities. We show that the values of the
relevant integrals, computed there, can be obtained as integrals of divisors
(complex codimens... | hep-th | we investigate resolutions of heterotic orbifolds using toric geometry our starting point is provided by the recently constructed heterotic models on explicit blowup of cnz_n singularities we show that the values of the relevant integrals computed there can be obtained as integrals of divisors complex codimension one h... | [['we', 'investigate', 'resolutions', 'of', 'heterotic', 'orbifolds', 'using', 'toric', 'geometry', 'our', 'starting', 'point', 'is', 'provided', 'by', 'the', 'recently', 'constructed', 'heterotic', 'models', 'on', 'explicit', 'blowup', 'of', 'cnz_n', 'singularities', 'we', 'show', 'that', 'the', 'values', 'of', 'the',... | [-0.13392807003239998, 0.011193505554628145, -0.04845404678619363, 0.15587146458629933, -0.05308705706718481, -0.17344407864665198, -0.03129576361970976, 0.34215617747718674, -0.20295679540787306, -0.239684178493917, 0.13482553735068198, -0.24006930215141942, -0.1389645461297025, 0.22130688148253183, -0.148149913377387... |
707.1598 | Theory of radiation trapping by the accelerating solitons in optical
fibers | We present a theory describing trapping of the normally dispersive radiation
by the Raman solitons in optical fibers. Frequency of the radiation component
is continuously blue shifting, while the soliton is red shifting. Underlying
physics of the trapping effect is in the existence of the inertial gravity-like
force ... | physics.optics nlin.PS | we present a theory describing trapping of the normally dispersive radiation by the raman solitons in optical fibers frequency of the radiation component is continuously blue shifting while the soliton is red shifting underlying physics of the trapping effect is in the existence of the inertial gravitylike force acting... | [['we', 'present', 'a', 'theory', 'describing', 'trapping', 'of', 'the', 'normally', 'dispersive', 'radiation', 'by', 'the', 'raman', 'solitons', 'in', 'optical', 'fibers', 'frequency', 'of', 'the', 'radiation', 'component', 'is', 'continuously', 'blue', 'shifting', 'while', 'the', 'soliton', 'is', 'red', 'shifting', '... | [-0.15035131122373666, 0.21971242873890637, -0.08216859199795484, -0.016926257066855518, -0.0561472061323002, -0.08183955046891546, 0.038946334329860596, 0.4496273732278496, -0.21775846157688647, -0.21627463396483412, 0.038413017433291924, -0.2786622836991834, -0.10041752889713583, 0.23337970717887704, -0.0025519237178... |
707.1599 | Involutions on 3-Manifolds and Self-dual, Binary Codes | We study a correspondence between orientation reversing involutions on
compact 3-manifolds with only isolated fixed points and binary, self-dual
codes. We show in particular that every such code can be obtained from such an
involution. We further relate doubly even codes to Pin^- -structures and
Spin-manifolds.
| math.AT | we study a correspondence between orientation reversing involutions on compact 3manifolds with only isolated fixed points and binary selfdual codes we show in particular that every such code can be obtained from such an involution we further relate doubly even codes to pin structures and spinmanifolds | [['we', 'study', 'a', 'correspondence', 'between', 'orientation', 'reversing', 'involutions', 'on', 'compact', '3manifolds', 'with', 'only', 'isolated', 'fixed', 'points', 'and', 'binary', 'selfdual', 'codes', 'we', 'show', 'in', 'particular', 'that', 'every', 'such', 'code', 'can', 'be', 'obtained', 'from', 'such', 'a... | [-0.20360019183515207, 0.10316282698318979, -0.06763925751590211, 0.09230874495013901, -0.048854925917744964, -0.20516295174298727, 0.031045739660444466, 0.4629657068087355, -0.32912027759416757, -0.24103419146622004, 0.09886670003027614, -0.3103537520636683, -0.1863826230426481, 0.2179890330273496, -0.1187352804952989... |
707.16 | Parameter Estimation in Manneville-Pomeau Processes | In this work we study a class of stochastic processes $\{X_t\}_{t\in\N}$,
where $X_t = (\phi \circ T_s^t)(X_0)$ is obtained from the iterations of the
transformation T_s, invariant for an ergodic probability \mu_s on [0,1] and a
continuous by part function $\phi:[0,1] \to \R$. We consider here $T_s:[0,1]\to
[0,1]$ th... | math.ST math.DS stat.TH | in this work we study a class of stochastic processes x_t_tinn where x_t phi circ t_stx_0 is obtained from the iterations of the transformation t_s invariant for an ergodic probability mu_s on 01 and a continuous by part function phi01 to r we consider here t_s01to 01 the mannevillepomeau transformation the autocorrela... | [['in', 'this', 'work', 'we', 'study', 'a', 'class', 'of', 'stochastic', 'processes', 'x_t_tinn', 'where', 'x_t', 'phi', 'circ', 't_stx_0', 'is', 'obtained', 'from', 'the', 'iterations', 'of', 'the', 'transformation', 't_s', 'invariant', 'for', 'an', 'ergodic', 'probability', 'mu_s', 'on', '01', 'and', 'a', 'continuous... | [-0.08380805585995062, 0.0953182893633319, -0.12542771120181578, 0.07599454311588115, -0.003299881142970079, -0.05418054282697093, 0.07654544771907644, 0.3584302939060662, -0.33261393149916685, -0.20078251401806235, 0.13066303370914495, -0.29460251789826614, -0.1447731902749222, 0.1991849776604173, -0.00987838466182096... |
707.1601 | Measurement of Prominent eta Decay Branching Fractions | The decay psi(2S) --> eta J/psi is used to measure, for the first time, all
prominent eta-meson branching fractions with the same experiment in the same
dataset, thereby providing a consistent treatment of systematics across
branching fractions. We present results for eta decays to gamma gamma,
pi+pi-pi0, 3 pi0, pi+ ... | hep-ex | the decay psi2s eta jpsi is used to measure for the first time all prominent etameson branching fractions with the same experiment in the same dataset thereby providing a consistent treatment of systematics across branching fractions we present results for eta decays to gamma gamma pipipi0 3 pi0 pi pi gamma and e e gam... | [['the', 'decay', 'psi2s', 'eta', 'jpsi', 'is', 'used', 'to', 'measure', 'for', 'the', 'first', 'time', 'all', 'prominent', 'etameson', 'branching', 'fractions', 'with', 'the', 'same', 'experiment', 'in', 'the', 'same', 'dataset', 'thereby', 'providing', 'a', 'consistent', 'treatment', 'of', 'systematics', 'across', 'b... | [-0.08510646875418554, 0.23678566784024088, -0.09668797877795919, 0.08478910675521639, 0.002287243332977247, -0.12660584496710486, 0.1288724375343082, 0.3206806906094455, -0.2107326595695934, -0.23171950413873701, -0.07494664614469829, -0.3538756726140326, 0.046979553296672874, 0.24656908744193537, 0.09709248128300062,... |
707.1602 | A 1.4-GHz Arecibo Survey for Pulsars in Globular Clusters | We have surveyed all 22 known Galactic globular clusters observable with the
Arecibo radio telescope and within 70kpc of the Sun for radio pulsations at
~1.4GHz. Data were taken with the Wideband Arecibo Pulsar Processor, which
provided the large bandwidth and high time and frequency resolution needed to
detect fast-... | astro-ph | we have surveyed all 22 known galactic globular clusters observable with the arecibo radio telescope and within 70kpc of the sun for radio pulsations at 14ghz data were taken with the wideband arecibo pulsar processor which provided the large bandwidth and high time and frequency resolution needed to detect fastspinnin... | [['we', 'have', 'surveyed', 'all', '22', 'known', 'galactic', 'globular', 'clusters', 'observable', 'with', 'the', 'arecibo', 'radio', 'telescope', 'and', 'within', '70kpc', 'of', 'the', 'sun', 'for', 'radio', 'pulsations', 'at', '14ghz', 'data', 'were', 'taken', 'with', 'the', 'wideband', 'arecibo', 'pulsar', 'process... | [-0.1416454372261392, 0.14583551561691208, -0.03512175169781389, 0.15468674922838282, -0.17000626492180124, -0.08422685866518055, 0.09413517562343794, 0.427210997132694, -0.15496995589647175, -0.3923009731228542, 0.12024563551557804, -0.3064423181280932, -0.04266565728603917, 0.2968295612631159, -0.02076268363044007, 0... |
707.1603 | A simple formula for the conserved charges of soliton theories | We present a simple formula for all the conserved charges of soliton
theories, evaluated on the solutions belonging to the orbit of the vacuum under
the group of dressing transformations. For pedagogical reasons we perform the
explicit calculations for the case of the sine-Gordon model, taken as a
prototype of solito... | hep-th math-ph math.MP nlin.SI | we present a simple formula for all the conserved charges of soliton theories evaluated on the solutions belonging to the orbit of the vacuum under the group of dressing transformations for pedagogical reasons we perform the explicit calculations for the case of the sinegordon model taken as a prototype of soliton theo... | [['we', 'present', 'a', 'simple', 'formula', 'for', 'all', 'the', 'conserved', 'charges', 'of', 'soliton', 'theories', 'evaluated', 'on', 'the', 'solutions', 'belonging', 'to', 'the', 'orbit', 'of', 'the', 'vacuum', 'under', 'the', 'group', 'of', 'dressing', 'transformations', 'for', 'pedagogical', 'reasons', 'we', 'pe... | [-0.19258877640480504, 0.0802760506322717, -0.07654311684617664, 0.09472824293120272, -0.051013055472068636, -0.10965150073353275, -0.0037671111492147925, 0.3420905265226668, -0.17008976685796298, -0.21474218848800541, 0.12079639122912697, -0.2766399440748215, -0.13789002295108696, 0.20882593324994578, 0.01829998818792... |
707.1604 | Light Quasiparticles Dominate Electronic Transport in Molecular Crystal
Field-Effect Transistors | We report on an infrared spectroscopy study of mobile holes in the
accumulation layer of organic field-effect transistors based on rubrene single
crystals. Our data indicate that both transport and infrared properties of
these transistors at room temperature are governed by light quasiparticles in
molecular orbital b... | cond-mat.mtrl-sci cond-mat.soft | we report on an infrared spectroscopy study of mobile holes in the accumulation layer of organic fieldeffect transistors based on rubrene single crystals our data indicate that both transport and infrared properties of these transistors at room temperature are governed by light quasiparticles in molecular orbital bands... | [['we', 'report', 'on', 'an', 'infrared', 'spectroscopy', 'study', 'of', 'mobile', 'holes', 'in', 'the', 'accumulation', 'layer', 'of', 'organic', 'fieldeffect', 'transistors', 'based', 'on', 'rubrene', 'single', 'crystals', 'our', 'data', 'indicate', 'that', 'both', 'transport', 'and', 'infrared', 'properties', 'of', ... | [-0.12266245383142056, 0.1522584635960663, -0.046240381473599344, 0.009401311266369053, 0.02039736719345864, -0.11127346123055536, 0.09792047284177638, 0.44909077620475873, -0.19256711203833016, -0.3286114221400752, 0.00782048044612213, -0.3487549748803888, -0.124427509760218, 0.23456645654086783, 0.021849976586444036,... |
707.1605 | Secant dimensions of low-dimensional homogeneous varieties | We completely describe the higher secant dimensions of all connected
homogeneous projective varieties of dimension at most 3, in all possible
equivariant embeddings. In particular, we calculate these dimensions for all
Segre-Veronese embeddings of P^1 * P^1, P^1 * P^1 * P^1, and P^2 * P^1, as well
as for the variety ... | math.AG math.RT | we completely describe the higher secant dimensions of all connected homogeneous projective varieties of dimension at most 3 in all possible equivariant embeddings in particular we calculate these dimensions for all segreveronese embeddings of p1 p1 p1 p1 p1 and p2 p1 as well as for the variety f of incident pointline ... | [['we', 'completely', 'describe', 'the', 'higher', 'secant', 'dimensions', 'of', 'all', 'connected', 'homogeneous', 'projective', 'varieties', 'of', 'dimension', 'at', 'most', '3', 'in', 'all', 'possible', 'equivariant', 'embeddings', 'in', 'particular', 'we', 'calculate', 'these', 'dimensions', 'for', 'all', 'segrever... | [-0.13831666810179336, 0.01850157301976449, 0.0012405561774762141, 0.10759652638937243, -0.041196944937109944, -0.20864820170940623, -0.0729696076673766, 0.3512278125828339, -0.2816372614935972, -0.20385681386623117, 0.11272552475048643, -0.29763842700566684, -0.11324917690621482, 0.2590929670880238, -0.093558571466969... |
707.1606 | Exchangeable partitions derived from Markovian coalescents with
simultaneous multiple collisions | Kingman derived the Ewens sampling formula for random partitions from the
genealogy model defined by a Poisson process of mutations along lines of
descent governed by a simple coalescent process. M\"ohle described the
recursion which determines the generalization of the Ewens sampling formula
when the lines of descen... | math.PR | kingman derived the ewens sampling formula for random partitions from the genealogy model defined by a poisson process of mutations along lines of descent governed by a simple coalescent process mohle described the recursion which determines the generalization of the ewens sampling formula when the lines of descent are... | [['kingman', 'derived', 'the', 'ewens', 'sampling', 'formula', 'for', 'random', 'partitions', 'from', 'the', 'genealogy', 'model', 'defined', 'by', 'a', 'poisson', 'process', 'of', 'mutations', 'along', 'lines', 'of', 'descent', 'governed', 'by', 'a', 'simple', 'coalescent', 'process', 'mohle', 'described', 'the', 'rec... | [-0.06522682904257276, 0.13929510718425672, -0.09522058186762103, 0.07150067464644629, -0.029730595011742564, -0.1368767961116354, 0.08629512798399963, 0.3365775264560356, -0.31316807766556054, -0.24349200019800882, 0.018069091589412216, -0.2266922777416099, -0.15775141832974116, 0.1538872329663451, -0.1073461500030660... |
707.1607 | Cactus Framework: Black Holes to Gamma Ray Bursts | Gamma Ray Bursts (GRBs) are intense narrowly-beamed flashes of gamma-rays of
cosmological origin. They are among the most scientifically interesting
astrophysical systems, and the riddle concerning their central engines and
emission mechanisms is one of the most complex and challenging problems of
astrophysics today.... | cs.DC | gamma ray bursts grbs are intense narrowlybeamed flashes of gammarays of cosmological origin they are among the most scientifically interesting astrophysical systems and the riddle concerning their central engines and emission mechanisms is one of the most complex and challenging problems of astrophysics today in this ... | [['gamma', 'ray', 'bursts', 'grbs', 'are', 'intense', 'narrowlybeamed', 'flashes', 'of', 'gammarays', 'of', 'cosmological', 'origin', 'they', 'are', 'among', 'the', 'most', 'scientifically', 'interesting', 'astrophysical', 'systems', 'and', 'the', 'riddle', 'concerning', 'their', 'central', 'engines', 'and', 'emission'... | [-0.1007495314012939, 0.10147320712327629, -0.026604846854324397, 0.12292909570701607, -0.12202216108904823, -0.11350293962716344, -0.003121774181422284, 0.41783081696313973, -0.2924300859808949, -0.3450679917484248, 0.1535855049150996, -0.3071752506554784, -0.11976410345831777, 0.31920506013557315, -0.0546542112510103... |
707.1608 | Dimensional dependence of naked singularity formation in spherical
gravitational collapse | The complete spectrum of the endstates - naked singularities, or blackholes -
of gravitational collapse is analyzed for a wide class of $N$-dimensional
spacetimes in spherical symmetry, which includes and generalizes the dust
solutions and the case of vanishing radial stresses. The final fate of the
collapse is shown... | gr-qc | the complete spectrum of the endstates naked singularities or blackholes of gravitational collapse is analyzed for a wide class of ndimensional spacetimes in spherical symmetry which includes and generalizes the dust solutions and the case of vanishing radial stresses the final fate of the collapse is shown to be fully... | [['the', 'complete', 'spectrum', 'of', 'the', 'endstates', 'naked', 'singularities', 'or', 'blackholes', 'of', 'gravitational', 'collapse', 'is', 'analyzed', 'for', 'a', 'wide', 'class', 'of', 'ndimensional', 'spacetimes', 'in', 'spherical', 'symmetry', 'which', 'includes', 'and', 'generalizes', 'the', 'dust', 'solutio... | [-0.14658256773708578, 0.12325661634205012, -0.10033663571262219, 0.07576969178580481, -0.05477762404154605, -0.1303710462818817, -0.01980716693508402, 0.2614255374018836, -0.19722725390493284, -0.25395175896760985, 0.10918887054884997, -0.26490472189121417, -0.11221507202841224, 0.1491224095353666, -0.0285156318797788... |
707.1609 | Equivariant monads and equivariant lifts versus a 2-category of
distributive laws | Fix a monoidal category C. The 2-category of monads in the 2-category of
C-actegories, colax C-equivarant functors, and C-equivariant natural
transformations of colax functors, may be recast in terms of pairs consisting
of a usual monad and a distributive law between the monad and the action of C,
morphisms of monads... | math.CT | fix a monoidal category c the 2category of monads in the 2category of cactegories colax cequivarant functors and cequivariant natural transformations of colax functors may be recast in terms of pairs consisting of a usual monad and a distributive law between the monad and the action of c morphisms of monads respecting ... | [['fix', 'a', 'monoidal', 'category', 'c', 'the', '2category', 'of', 'monads', 'in', 'the', '2category', 'of', 'cactegories', 'colax', 'cequivarant', 'functors', 'and', 'cequivariant', 'natural', 'transformations', 'of', 'colax', 'functors', 'may', 'be', 'recast', 'in', 'terms', 'of', 'pairs', 'consisting', 'of', 'a', ... | [-0.13715307000980137, 0.10030980753349251, -0.03568574481954177, 0.12162820528361148, -0.13162330721638033, -0.18997829127613278, 0.0552065472661828, 0.37665062178635883, -0.44376087576550033, -0.20678433382445724, 0.04751556078360106, -0.2247731505017284, -0.08276813139895066, 0.14019774953901235, -0.2148098278192005... |
707.161 | How a Vicinal Layer of Solvent Modulates the Dynamics of Proteins | The dynamics of a folded protein is studied in water and glycerol at a series
of temperatures below and above their respective dynamical transition. The
system is modeled in two distinct states whereby the protein is decoupled from
the bulk solvent at low temperatures, and communicates with it through a
vicinal layer... | cond-mat.soft | the dynamics of a folded protein is studied in water and glycerol at a series of temperatures below and above their respective dynamical transition the system is modeled in two distinct states whereby the protein is decoupled from the bulk solvent at low temperatures and communicates with it through a vicinal layer at ... | [['the', 'dynamics', 'of', 'a', 'folded', 'protein', 'is', 'studied', 'in', 'water', 'and', 'glycerol', 'at', 'a', 'series', 'of', 'temperatures', 'below', 'and', 'above', 'their', 'respective', 'dynamical', 'transition', 'the', 'system', 'is', 'modeled', 'in', 'two', 'distinct', 'states', 'whereby', 'the', 'protein', ... | [-0.1209392328155301, 0.19839798859148114, -0.05793202122693103, 0.019706827673997, 0.0289451495717186, -0.13134258144495703, 0.07060762867870464, 0.36368420335745055, -0.2947419164850125, -0.2849550019634306, 0.022549110884832406, -0.25354239337698176, -0.1286480287022189, 0.10556234654209148, -0.004443794692171708, 0... |
707.1611 | Probabilistic Cross-Identification of Astronomical Sources | We present a general probabilistic formalism for cross-identifying
astronomical point sources in multiple observations. Our Bayesian approach,
symmetric in all observations, is the foundation of a unified framework for
object matching, where not only spatial information, but physical properties,
such as colors, redsh... | astro-ph | we present a general probabilistic formalism for crossidentifying astronomical point sources in multiple observations our bayesian approach symmetric in all observations is the foundation of a unified framework for object matching where not only spatial information but physical properties such as colors redshift and lu... | [['we', 'present', 'a', 'general', 'probabilistic', 'formalism', 'for', 'crossidentifying', 'astronomical', 'point', 'sources', 'in', 'multiple', 'observations', 'our', 'bayesian', 'approach', 'symmetric', 'in', 'all', 'observations', 'is', 'the', 'foundation', 'of', 'a', 'unified', 'framework', 'for', 'object', 'match... | [-0.06005713229422413, 0.025601110276017736, -0.10336287591074195, 0.0963994614059283, -0.1622531899650182, -0.10070050660121654, 0.0666756044696307, 0.44051597632822537, -0.22263148978707337, -0.34389732653896016, 0.10005034834944776, -0.22816178442112037, -0.14091783910102787, 0.2364806742496079, -0.0646067092505594,... |
707.1612 | Accretion disc coronae in black hole binaries | Most of the luminosity of accreting black hole is emitted in the X-ray band.
This radiation is believed to emerge, through inverse Compton process, from a
hot (Te ~ 10^8 -10^9 K) optically thin (Thomson optical depth ~ 1) plasma
probably located in the immediate vicinity of the black hole. The mechanisms at
work in t... | astro-ph | most of the luminosity of accreting black hole is emitted in the xray band this radiation is believed to emerge through inverse compton process from a hot te 108 109 k optically thin thomson optical depth 1 plasma probably located in the immediate vicinity of the black hole the mechanisms at work in this so called comp... | [['most', 'of', 'the', 'luminosity', 'of', 'accreting', 'black', 'hole', 'is', 'emitted', 'in', 'the', 'xray', 'band', 'this', 'radiation', 'is', 'believed', 'to', 'emerge', 'through', 'inverse', 'compton', 'process', 'from', 'a', 'hot', 'te', '108', '109', 'k', 'optically', 'thin', 'thomson', 'optical', 'depth', '1', ... | [-0.09039143679151036, 0.1609748673954904, -0.06644808160163154, 0.1315527196897294, -0.08845290435841803, -0.06839864497409152, 0.02636708095449315, 0.4174738003260638, -0.24190546554091702, -0.32089506189294775, 0.08326363172478556, -0.2972058697972865, -0.05695356939748459, 0.2368475506137285, -0.006495511861925823,... |
707.1613 | Morphologies of AGN host galaxies using HST/ACS in the CDFS-GOODS field | Using HST/ACS images in four bands F435W, F606W, F775W and F850LP, we
identify optical counterparts to the X-ray sources in the Chandra Deep Field
South in the GOODS South field. A detailed study has been made of these sources
to study their morphological types. We use methods like decomposition of galaxy
luminosity ... | astro-ph | using hstacs images in four bands f435w f606w f775w and f850lp we identify optical counterparts to the xray sources in the chandra deep field south in the goods south field a detailed study has been made of these sources to study their morphological types we use methods like decomposition of galaxy luminosity profiles ... | [['using', 'hstacs', 'images', 'in', 'four', 'bands', 'f435w', 'f606w', 'f775w', 'and', 'f850lp', 'we', 'identify', 'optical', 'counterparts', 'to', 'the', 'xray', 'sources', 'in', 'the', 'chandra', 'deep', 'field', 'south', 'in', 'the', 'goods', 'south', 'field', 'a', 'detailed', 'study', 'has', 'been', 'made', 'of', ... | [-0.0431489286588897, 0.04258247817102656, -0.07370254487665207, 0.13673502298402845, -0.13750757470628933, -0.06405320739487938, 0.03789235790782984, 0.5586799564199489, -0.11011547039430425, -0.3339055234304907, 0.08049899251547463, -0.345757115918228, -0.03645791115827466, 0.22148364301966994, -0.01427008205894054, ... |
707.1614 | Analysis of the accuracy and convergence of equation-free projection to
a slow manifold | In [C.W. Gear, T.J. Kaper, I.G. Kevrekidis, and A. Zagaris, Projecting to a
Slow Manifold: Singularly Perturbed Systems and Legacy Codes, SIAM J. Appl.
Dyn. Syst. 4 (2005) 711-732], we developed a class of iterative algorithms
within the context of equation-free methods to approximate low-dimensional,
attracting, slo... | math.DS math.NA | in cw gear tj kaper ig kevrekidis and a zagaris projecting to a slow manifold singularly perturbed systems and legacy codes siam j appl dyn syst 4 2005 711732 we developed a class of iterative algorithms within the context of equationfree methods to approximate lowdimensional attracting slow manifolds in systems of dif... | [['in', 'cw', 'gear', 'tj', 'kaper', 'ig', 'kevrekidis', 'and', 'a', 'zagaris', 'projecting', 'to', 'a', 'slow', 'manifold', 'singularly', 'perturbed', 'systems', 'and', 'legacy', 'codes', 'siam', 'j', 'appl', 'dyn', 'syst', '4', '2005', '711732', 'we', 'developed', 'a', 'class', 'of', 'iterative', 'algorithms', 'withi... | [-0.1299257690073512, 0.06838847835570706, -0.08725999828910502, 0.03906504116239638, -0.04256799214583442, -0.14498631103932588, 0.04950539350075923, 0.35153523022443434, -0.30027261618289436, -0.2867562850426197, 0.12257477920880669, -0.22960759837614098, -0.14632095285650976, 0.18197140875121154, -0.0629631296449109... |
707.1615 | Random-phase-approximation-based correlation energy functionals:
Benchmark results for atoms | The random phase approximation (RPA) for the correlation energy functional of
density functional theory has recently attracted renewed interest. Formulated
in terms of the Kohn-Sham (KS) orbitals and eigenvalues, it promises to resolve
some of the fundamental limitations of the local density and generalized
gradient ... | cond-mat.other | the random phase approximation rpa for the correlation energy functional of density functional theory has recently attracted renewed interest formulated in terms of the kohnsham ks orbitals and eigenvalues it promises to resolve some of the fundamental limitations of the local density and generalized gradient approxima... | [['the', 'random', 'phase', 'approximation', 'rpa', 'for', 'the', 'correlation', 'energy', 'functional', 'of', 'density', 'functional', 'theory', 'has', 'recently', 'attracted', 'renewed', 'interest', 'formulated', 'in', 'terms', 'of', 'the', 'kohnsham', 'ks', 'orbitals', 'and', 'eigenvalues', 'it', 'promises', 'to', '... | [-0.0805197664752278, 0.05895188417978032, -0.0856427879813939, 0.11168282974186704, -0.02703519491692407, -0.08528511568160574, 0.04193136961479167, 0.360079237631599, -0.25678451509009875, -0.2917765217754187, 0.058231985085396044, -0.3065502030599794, -0.12845486296242564, 0.15994818436853384, 0.0302751055499966, 0.... |
707.1616 | Modularity and community detection in bipartite networks | The modularity of a network quantifies the extent, relative to a null model
network, to which vertices cluster into community groups. We define a null
model appropriate for bipartite networks, and use it to define a bipartite
modularity. The bipartite modularity is presented in terms of a modularity
matrix B; some ke... | physics.data-an cond-mat.stat-mech physics.soc-ph | the modularity of a network quantifies the extent relative to a null model network to which vertices cluster into community groups we define a null model appropriate for bipartite networks and use it to define a bipartite modularity the bipartite modularity is presented in terms of a modularity matrix b some key proper... | [['the', 'modularity', 'of', 'a', 'network', 'quantifies', 'the', 'extent', 'relative', 'to', 'a', 'null', 'model', 'network', 'to', 'which', 'vertices', 'cluster', 'into', 'community', 'groups', 'we', 'define', 'a', 'null', 'model', 'appropriate', 'for', 'bipartite', 'networks', 'and', 'use', 'it', 'to', 'define', 'a'... | [-0.13789676608212176, 0.019992753995325074, -0.08747885210323147, 0.060449516315202345, -0.0452706176583888, -0.14654353214791627, 0.005610593070741743, 0.38841365920961834, -0.30234896796173416, -0.2830025287148601, 0.06630778986163932, -0.2399179861531593, -0.2228386271854106, 0.13329584829352825, -0.047603773477021... |
707.1617 | Computation of the cover of Shimura curves $X_0(2) \to X(1)$ for the
cyclic cubic field of discriminant 13^2 | We compute the canonical model of the cover of Shimura curves $X_0(2) \to
X(1)$ for the cubic field of discriminant 13^2 described at the end of Elkies'
paper "Shimura curves for level 3 subgroups of the (2,3,7) triangle group".
Last, we list the coordinates of some rational CM points on X(1).
| math.NT math.AG | we compute the canonical model of the cover of shimura curves x_02 to x1 for the cubic field of discriminant 132 described at the end of elkies paper shimura curves for level 3 subgroups of the 237 triangle group last we list the coordinates of some rational cm points on x1 | [['we', 'compute', 'the', 'canonical', 'model', 'of', 'the', 'cover', 'of', 'shimura', 'curves', 'x_02', 'to', 'x1', 'for', 'the', 'cubic', 'field', 'of', 'discriminant', '132', 'described', 'at', 'the', 'end', 'of', 'elkies', 'paper', 'shimura', 'curves', 'for', 'level', '3', 'subgroups', 'of', 'the', '237', 'triangle... | [-0.20033647211305067, -0.024876808199812386, -0.11479132827919196, 0.06741002160033174, -0.06768067232241817, -0.1260275538353359, 0.10442988726301301, 0.3110159147603839, -0.27867514504959773, -0.28511328096775446, 0.11288267090989679, -0.30295774636461453, -0.08302697842465896, 0.25305438951552645, -0.12743695812555... |
707.1618 | The Trade-offs with Space Time Cube Representation of Spatiotemporal
Patterns | Space time cube representation is an information visualization technique
where spatiotemporal data points are mapped into a cube. Fast and correct
analysis of such information is important in for instance geospatial and social
visualization applications. Information visualization researchers have
previously argued th... | cs.HC cs.GR | space time cube representation is an information visualization technique where spatiotemporal data points are mapped into a cube fast and correct analysis of such information is important in for instance geospatial and social visualization applications information visualization researchers have previously argued that s... | [['space', 'time', 'cube', 'representation', 'is', 'an', 'information', 'visualization', 'technique', 'where', 'spatiotemporal', 'data', 'points', 'are', 'mapped', 'into', 'a', 'cube', 'fast', 'and', 'correct', 'analysis', 'of', 'such', 'information', 'is', 'important', 'in', 'for', 'instance', 'geospatial', 'and', 'so... | [-0.06895778249252861, 0.03896399125763335, -0.09300941794121706, 0.10851949093160604, -0.12121664001948175, -0.10673741154359875, 0.05742982989540238, 0.4348408644249953, -0.27061727934371715, -0.3199573445108232, 0.12123915577924665, -0.2789000525510947, -0.16174390939504352, 0.21898892810226445, -0.07916911393019516... |
707.1619 | An Extremely Bright Echo Associated With SN 2002hh | We present new, very late-time optical photometry and spectroscopy of the
interesting Type II-P supernova, SN 2002hh, in NGC 6946. Gemini/GMOS-N has been
used to acquire visible spectra at six epochs between 2004 August and 2006
July, following the evolution of the SN from age 661 to 1358 days. Few optical
spectra of... | astro-ph | we present new very latetime optical photometry and spectroscopy of the interesting type iip supernova sn 2002hh in ngc 6946 geminigmosn has been used to acquire visible spectra at six epochs between 2004 august and 2006 july following the evolution of the sn from age 661 to 1358 days few optical spectra of type ii sup... | [['we', 'present', 'new', 'very', 'latetime', 'optical', 'photometry', 'and', 'spectroscopy', 'of', 'the', 'interesting', 'type', 'iip', 'supernova', 'sn', '2002hh', 'in', 'ngc', '6946', 'geminigmosn', 'has', 'been', 'used', 'to', 'acquire', 'visible', 'spectra', 'at', 'six', 'epochs', 'between', '2004', 'august', 'and... | [-0.02314330277357638, 0.06579224599046765, -0.08907429929569835, 0.07711905594261961, -0.06818859530949957, -0.15290251999486493, 0.037248322760214295, 0.4837749131377871, -0.15946589896088778, -0.3355193001121215, 0.09557205313454252, -0.3620692005452628, -0.04121474115961817, 0.21450789049752395, -0.0835884719361776... |
707.162 | Level Spacings in Random Matrix Theory and Coulomb Blockade Peaks in
Quantum Dots | We obtain analytic formulae for the spacing between conductance peaks in the
Coulomb blockade regime, based on the universal Hamiltonian model of quantum
dots. New random matrix theory results are developed in order to treat
correlations between two and three consecutive spacings in the energy level
spectrum. These a... | cond-mat.mes-hall | we obtain analytic formulae for the spacing between conductance peaks in the coulomb blockade regime based on the universal hamiltonian model of quantum dots new random matrix theory results are developed in order to treat correlations between two and three consecutive spacings in the energy level spectrum these are ge... | [['we', 'obtain', 'analytic', 'formulae', 'for', 'the', 'spacing', 'between', 'conductance', 'peaks', 'in', 'the', 'coulomb', 'blockade', 'regime', 'based', 'on', 'the', 'universal', 'hamiltonian', 'model', 'of', 'quantum', 'dots', 'new', 'random', 'matrix', 'theory', 'results', 'are', 'developed', 'in', 'order', 'to',... | [-0.11901054908055812, 0.14678517554983653, -0.08986138329530756, 0.11391057079657912, 0.05209577274353554, -0.1459651982411742, 0.036697406186722216, 0.4022853082915147, -0.2045713705321153, -0.293381423416237, -0.010351032316684723, -0.30674416999022164, -0.1420931047697862, 0.21119078005043168, -0.000911650098860263... |
707.1621 | Decoupling limits of N=4 super Yang-Mills on R x S^3 | We find new decoupling limits of N=4 super Yang-Mills (SYM) on R x S^3 with
gauge group SU(N). These decoupling limits lead to decoupled theories that are
much simpler than the full N=4 SYM but still contain many of its interesting
features. The decoupling limits correspond to being in a near-critical region,
near a ... | hep-th | we find new decoupling limits of n4 super yangmills sym on r x s3 with gauge group sun these decoupling limits lead to decoupled theories that are much simpler than the full n4 sym but still contain many of its interesting features the decoupling limits correspond to being in a nearcritical region near a point with zer... | [['we', 'find', 'new', 'decoupling', 'limits', 'of', 'n4', 'super', 'yangmills', 'sym', 'on', 'r', 'x', 's3', 'with', 'gauge', 'group', 'sun', 'these', 'decoupling', 'limits', 'lead', 'to', 'decoupled', 'theories', 'that', 'are', 'much', 'simpler', 'than', 'the', 'full', 'n4', 'sym', 'but', 'still', 'contain', 'many', ... | [-0.13432309246531482, 0.20847109262838245, -0.06734329600436063, 0.07274332529858737, -0.019610631273179833, -0.16727508160423626, 0.015340758677296064, 0.32180004369001836, -0.18866871997198797, -0.24011868478178425, 0.09541910805219905, -0.28300796926379446, -0.12650785135445874, 0.10588227772084927, 0.0021195270559... |
707.1622 | Dynamic Failure in Amorphous Solids via a Cavitation Instability | The understanding of dynamic failure in amorphous materials via the
propagation of free boundaries like cracks and voids must go beyond elasticity
theory, since plasticity intervenes in a crucial and poorly understood manner
near the moving free boundary. In this Letter we focus on failure via a
cavitation instabilit... | cond-mat.mtrl-sci cond-mat.dis-nn | the understanding of dynamic failure in amorphous materials via the propagation of free boundaries like cracks and voids must go beyond elasticity theory since plasticity intervenes in a crucial and poorly understood manner near the moving free boundary in this letter we focus on failure via a cavitation instability in... | [['the', 'understanding', 'of', 'dynamic', 'failure', 'in', 'amorphous', 'materials', 'via', 'the', 'propagation', 'of', 'free', 'boundaries', 'like', 'cracks', 'and', 'voids', 'must', 'go', 'beyond', 'elasticity', 'theory', 'since', 'plasticity', 'intervenes', 'in', 'a', 'crucial', 'and', 'poorly', 'understood', 'mann... | [-0.12533393988059355, 0.1933733810209813, -0.08795863894515277, 0.010470562118835286, -0.030214817522420098, -0.07909857408268396, 0.04229576279590454, 0.35358914738693803, -0.31222931541425664, -0.2246154822774001, 0.11797392913788442, -0.23044599076617778, -0.2306946814924325, 0.11793350473888814, -0.027006628607476... |
707.1623 | Derivation of the Quantum Probability Rule without the Frequency
Operator | We present an alternative frequencists' proof of the quantum probability rule
which does not make use of the frequency operator, with expectation that this
can circumvent the recent criticism against the previous proofs which use it.
We also argue that avoiding the frequency operator is not only for technical
merits ... | quant-ph | we present an alternative frequencists proof of the quantum probability rule which does not make use of the frequency operator with expectation that this can circumvent the recent criticism against the previous proofs which use it we also argue that avoiding the frequency operator is not only for technical merits for d... | [['we', 'present', 'an', 'alternative', 'frequencists', 'proof', 'of', 'the', 'quantum', 'probability', 'rule', 'which', 'does', 'not', 'make', 'use', 'of', 'the', 'frequency', 'operator', 'with', 'expectation', 'that', 'this', 'can', 'circumvent', 'the', 'recent', 'criticism', 'against', 'the', 'previous', 'proofs', '... | [-0.04756142078827986, 0.08824203538128843, -0.13205954055381985, 0.07123176311142743, -0.1693893904203846, -0.13678554197827328, 0.07793828713086744, 0.359424809101915, -0.2483344023956148, -0.24365164285552673, 0.11776104443234162, -0.23834201904094737, -0.1956724583481749, 0.19708921703040952, -0.15465658495499604, ... |
707.1624 | Sound beyond the speed of light: destructive interference, anomalous
dispersion and nonlocality of near field | Experimentally fixed sound pulse beyond of light speed in the region of
anomalous dispersion [W. M. Robertson, e. a. Appl. Phys. Lett, 90, 014102
(2007)] can be explained, as well as the similar superluminal phenomena, by
"the nonlocality in the small" of near electromagnetic field at transferring of
relevanted excit... | physics.class-ph physics.optics | experimentally fixed sound pulse beyond of light speed in the region of anomalous dispersion w m robertson e a appl phys lett 90 014102 2007 can be explained as well as the similar superluminal phenomena by the nonlocality in the small of near electromagnetic field at transferring of relevanted excitations | [['experimentally', 'fixed', 'sound', 'pulse', 'beyond', 'of', 'light', 'speed', 'in', 'the', 'region', 'of', 'anomalous', 'dispersion', 'w', 'm', 'robertson', 'e', 'a', 'appl', 'phys', 'lett', '90', '014102', '2007', 'can', 'be', 'explained', 'as', 'well', 'as', 'the', 'similar', 'superluminal', 'phenomena', 'by', 'th... | [-0.1296397201260742, 0.2188077083389674, -0.044165907228099446, -0.007790484769763995, -0.0726322278770029, -0.11234525926601217, 0.08749572037227989, 0.32489897202396273, -0.18554955918569954, -0.38572092057794943, -0.033286015811965476, -0.25761008369546307, -0.10222714588198127, 0.23497306258531706, -0.082866544555... |
707.1625 | Double affine Hecke algebra in logarithmic conformal field theory | We construct the representation of Double Affine Hecke Algebra whose
symmetrization gives the center of the quantum group U_q(sl(2)) and by
Kazhdan--Lusztig duality the Verlinde algebra of (1,p) models of logarithmic
conformal field theory.
| math.QA hep-th | we construct the representation of double affine hecke algebra whose symmetrization gives the center of the quantum group u_qsl2 and by kazhdanlusztig duality the verlinde algebra of 1p models of logarithmic conformal field theory | [['we', 'construct', 'the', 'representation', 'of', 'double', 'affine', 'hecke', 'algebra', 'whose', 'symmetrization', 'gives', 'the', 'center', 'of', 'the', 'quantum', 'group', 'u_qsl2', 'and', 'by', 'kazhdanlusztig', 'duality', 'the', 'verlinde', 'algebra', 'of', '1p', 'models', 'of', 'logarithmic', 'conformal', 'fie... | [-0.15747262212886093, 0.08672272249617997, -0.12739435342304847, 0.04409007668180172, -0.1081786075990428, -0.2222658895942218, -0.010676495569093865, 0.24609514199854696, -0.4147370635148357, -0.15728910930235596, 0.04267363472814288, -0.21348516796441638, -0.21577948156525106, 0.11506447530187228, -0.139649618506048... |
707.1626 | Asymptotically nonexpansive mappings in uniformly convex hyperbolic
spaces | This paper provides a fixed point theorem for asymptotically nonexpansive
mappings in uniformly convex hyperbolic spaces as well as new effective results
on the Krasnoselski-Mann iterations of such mappings. The latter were found
using methods from logic and the paper continues a case study in the general
program of ... | math.FA math.LO | this paper provides a fixed point theorem for asymptotically nonexpansive mappings in uniformly convex hyperbolic spaces as well as new effective results on the krasnoselskimann iterations of such mappings the latter were found using methods from logic and the paper continues a case study in the general program of extr... | [['this', 'paper', 'provides', 'a', 'fixed', 'point', 'theorem', 'for', 'asymptotically', 'nonexpansive', 'mappings', 'in', 'uniformly', 'convex', 'hyperbolic', 'spaces', 'as', 'well', 'as', 'new', 'effective', 'results', 'on', 'the', 'krasnoselskimann', 'iterations', 'of', 'such', 'mappings', 'the', 'latter', 'were', ... | [-0.08159407538949467, 0.04342230708737459, -0.08857534728234723, 0.10574743354744795, -0.020095214462055574, -0.13397066686893738, 0.10040660859787807, 0.3107149098068476, -0.2854088841094857, -0.2299438923715599, 0.1630669624400547, -0.307243327122359, -0.18195181813031908, 0.23001716376489234, -0.128010778303539, 0.... |
707.1627 | Soft X-ray Circular Reflectivity from Ferromagnetic Transition-Metal
Films Near the Brewster's Angle: Theoretical and Numerical X-ray Resonant
Magnetic Scattering Study | We first report a novel phenomenon that manifests itself in a colossal
difference in soft x-ray reflectivity from ferromagnetic transition-metal films
between the left- and right-handed circular polarization (LCP and RCP) modes at
a resonance near normal Brewster's angle. Theoretical and numerical studies of
sft x-ra... | cond-mat.other | we first report a novel phenomenon that manifests itself in a colossal difference in soft xray reflectivity from ferromagnetic transitionmetal films between the left and righthanded circular polarization lcp and rcp modes at a resonance near normal brewsters angle theoretical and numerical studies of sft xray resonant ... | [['we', 'first', 'report', 'a', 'novel', 'phenomenon', 'that', 'manifests', 'itself', 'in', 'a', 'colossal', 'difference', 'in', 'soft', 'xray', 'reflectivity', 'from', 'ferromagnetic', 'transitionmetal', 'films', 'between', 'the', 'left', 'and', 'righthanded', 'circular', 'polarization', 'lcp', 'and', 'rcp', 'modes', ... | [-0.16338444697476334, 0.2624558797776163, -0.05967202137907793, 0.015752146766762242, -0.08989314775136735, -0.1348354690004703, 0.10085540827826041, 0.42775366514277974, -0.3331279829680491, -0.24552679471939587, 0.022364532420907517, -0.3249639080261155, -0.08656045285442161, 0.18417255261665036, 0.04415527501280868... |
707.1628 | On the solutions of a boundary value problem arising in free convection
with prescribed heat flux | For given $a\in\R$, c<0, we are concerned with the solution $f^{}_b$ of the
differential equation
$f^{\prime\prime\prime}+ff^{\prime\prime}+\g(f^{\prime})=0$, satisfying the
initial conditions $f(0)=a$, $f'(0)=b$, $f''(0)=c< 0$, where g is some
nonnegative subquadratic locally Lipschitz function. It is proven that th... | math.DS | for given ainr c0 we are concerned with the solution f_b of the differential equation fprimeprimeprimeffprimeprimegfprime0 satisfying the initial conditions f0a f0b f0c 0 where g is some nonnegative subquadratic locally lipschitz function it is proven that there exists b_0 such that f_b exists on 0infty and is such tha... | [['for', 'given', 'ainr', 'c0', 'we', 'are', 'concerned', 'with', 'the', 'solution', 'f_b', 'of', 'the', 'differential', 'equation', 'fprimeprimeprimeffprimeprimegfprime0', 'satisfying', 'the', 'initial', 'conditions', 'f0a', 'f0b', 'f0c', '0', 'where', 'g', 'is', 'some', 'nonnegative', 'subquadratic', 'locally', 'lips... | [-0.17754440733640478, 0.11766201944272148, -0.04983947322726613, 0.049084205853343915, -0.10678243041379241, -0.21862449339681828, -0.00748902571915717, 0.3618817885247309, -0.3360031387745971, -0.19452806829656588, 0.15408354641290428, -0.3245859596363294, -0.12033986003228986, 0.15726559871535112, -0.066525859925604... |
707.1629 | Storing quantum states in bosonic dissipative networks | Considering a network of dissipative quantum harmonic oscillators we deduce
and analyze the optimum topologies which are able to store, for the largest
period of time, a quantum superposition previously prepared in one of the
network oscillators. The storage of the superposition is made dynamically, in
that the state... | quant-ph | considering a network of dissipative quantum harmonic oscillators we deduce and analyze the optimum topologies which are able to store for the largest period of time a quantum superposition previously prepared in one of the network oscillators the storage of the superposition is made dynamically in that the state to be... | [['considering', 'a', 'network', 'of', 'dissipative', 'quantum', 'harmonic', 'oscillators', 'we', 'deduce', 'and', 'analyze', 'the', 'optimum', 'topologies', 'which', 'are', 'able', 'to', 'store', 'for', 'the', 'largest', 'period', 'of', 'time', 'a', 'quantum', 'superposition', 'previously', 'prepared', 'in', 'one', 'o... | [-0.15763117273429683, 0.19195387042032516, -0.06892393963240391, 0.0003603362135937478, 0.01626317768965905, -0.15923191278897303, 0.060422903511255066, 0.3532219867469097, -0.3104794615385484, -0.2608035840854353, 0.10279201051429371, -0.25276721896109533, -0.12974708741150645, 0.1983732876500913, -0.0261473709109182... |
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