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 |
|---|---|---|---|---|---|---|
706.2214 | Nanorheology of viscoelastic shells: Applications to viral capsids | We study the microrheology of nanoparticle shells [Dinsmore et al. Science
298, 1006 (2002)] and viral capsids [Ivanovska et al. PNAS 101, 7600 (2004)] by
computing the mechanical response function and thermal fluctuation spectrum of
a viscoelastic spherical shell that is permeable to the surrounding solvent. We
dete... | cond-mat.soft q-bio.SC | we study the microrheology of nanoparticle shells dinsmore et al science 298 1006 2002 and viral capsids ivanovska et al pnas 101 7600 2004 by computing the mechanical response function and thermal fluctuation spectrum of a viscoelastic spherical shell that is permeable to the surrounding solvent we determine analytica... | [['we', 'study', 'the', 'microrheology', 'of', 'nanoparticle', 'shells', 'dinsmore', 'et', 'al', 'science', '298', '1006', '2002', 'and', 'viral', 'capsids', 'ivanovska', 'et', 'al', 'pnas', '101', '7600', '2004', 'by', 'computing', 'the', 'mechanical', 'response', 'function', 'and', 'thermal', 'fluctuation', 'spectrum... | [-0.11264920556115815, 0.15786122577911657, -0.08555366921872418, 0.011233133639002012, -0.04515486097403078, -0.07119895694712694, 0.02546788681259689, 0.3501561512045252, -0.26730383845117306, -0.30040838664475206, 0.04179367493149281, -0.30583327367316493, -0.18506843154156943, 0.14495508237612537, -0.02217517612775... |
706.2215 | Constraints on the spectral index for the inflation models in string
landscape | We conjecture that the inflation models with trans-Planckian excursions in
the field space should be in the swampland. We check this conjecture in a few
examples and investigate the constraints on the spectral index for the
slow-roll inflation model in string landscape where the variation of inflaton
during the perio... | hep-th astro-ph | we conjecture that the inflation models with transplanckian excursions in the field space should be in the swampland we check this conjecture in a few examples and investigate the constraints on the spectral index for the slowroll inflation model in string landscape where the variation of inflaton during the period of ... | [['we', 'conjecture', 'that', 'the', 'inflation', 'models', 'with', 'transplanckian', 'excursions', 'in', 'the', 'field', 'space', 'should', 'be', 'in', 'the', 'swampland', 'we', 'check', 'this', 'conjecture', 'in', 'a', 'few', 'examples', 'and', 'investigate', 'the', 'constraints', 'on', 'the', 'spectral', 'index', 'f... | [-0.1568211807115447, 0.21641313517466187, -0.13745878755469762, 0.14950909741206228, -0.07482766315141427, -0.14272045060005484, -0.01310186323133253, 0.31077464834033025, -0.19716385146602988, -0.3460362262225577, 0.12592571322429216, -0.20818049384147994, -0.10625856654119811, 0.17904335651491282, -0.091864369465925... |
706.2216 | Schwinger Pair Production at Finite Temperature in Scalar QED | In scalar QED we study the Schwinger pair production from an initial ensemble
of charged bosons when an electric field is turned on for a finite period
together with or without a constant magnetic field. The scalar QED Hamiltonian
depends on time through the electric field, which causes the initial ensemble
of bosons... | hep-th | in scalar qed we study the schwinger pair production from an initial ensemble of charged bosons when an electric field is turned on for a finite period together with or without a constant magnetic field the scalar qed hamiltonian depends on time through the electric field which causes the initial ensemble of bosons to ... | [['in', 'scalar', 'qed', 'we', 'study', 'the', 'schwinger', 'pair', 'production', 'from', 'an', 'initial', 'ensemble', 'of', 'charged', 'bosons', 'when', 'an', 'electric', 'field', 'is', 'turned', 'on', 'for', 'a', 'finite', 'period', 'together', 'with', 'or', 'without', 'a', 'constant', 'magnetic', 'field', 'the', 'sc... | [-0.1339610702725071, 0.2701869862970797, -0.0852309567148261, 0.04839530990769466, 0.00447509580555212, -0.11734175974634861, 0.030666838228382697, 0.3270137312074164, -0.19847825003054106, -0.22711889641923885, 0.02824825956603757, -0.2770991823918214, 0.006947860166411659, 0.17221304855422315, 0.07492056879393681, 0... |
706.2217 | Unusual superexchange pathways in a Ni triangular lattice of
NiGa$_2$S$_4$ with negative charge-transfer energy | We have studied the electronic structure of the Ni triangular lattice in
NiGa$_2$S$_4$ using photoemission spectroscopy and subsequent model
calculations. The cluster-model analysis of the Ni 2$p$ core-level spectrum
shows that the S 3$p$ to Ni 3$d$ charge-transfer energy is $\sim$ -1 eV and the
ground state is domin... | cond-mat.str-el | we have studied the electronic structure of the ni triangular lattice in niga_2s_4 using photoemission spectroscopy and subsequent model calculations the clustermodel analysis of the ni 2p corelevel spectrum shows that the s 3p to ni 3d chargetransfer energy is sim 1 ev and the ground state is dominated by the d9l conf... | [['we', 'have', 'studied', 'the', 'electronic', 'structure', 'of', 'the', 'ni', 'triangular', 'lattice', 'in', 'niga_2s_4', 'using', 'photoemission', 'spectroscopy', 'and', 'subsequent', 'model', 'calculations', 'the', 'clustermodel', 'analysis', 'of', 'the', 'ni', '2p', 'corelevel', 'spectrum', 'shows', 'that', 'the',... | [-0.14043661835865023, 0.12810193913664375, 0.04128300666997439, 0.08106726072493187, 0.06088717127731593, -0.16430063873236433, 0.10500175226741376, 0.38987676353518214, -0.25168503762950095, -0.27548437251636154, -0.05055775489328492, -0.4229656933398729, -0.04922649779179123, 0.0723596597979829, 0.16293647704290204,... |
706.2218 | The analog of the Schauder inequality for closed surfaces in Euclidean
spaces | The analog of the Schauder inequality for closed surfaces in Euclidean spaces
is obtained in this article.
| math.DG math.AP | the analog of the schauder inequality for closed surfaces in euclidean spaces is obtained in this article | [['the', 'analog', 'of', 'the', 'schauder', 'inequality', 'for', 'closed', 'surfaces', 'in', 'euclidean', 'spaces', 'is', 'obtained', 'in', 'this', 'article']] | [-0.14596395588972988, 0.048598429078564924, -0.08997020077453378, 0.16263861011932879, -0.006986478781875442, -0.07371790071620661, 0.016097916399731356, 0.3321247137946022, -0.2912665373262237, -0.12301845760906444, 0.12677099910455153, -0.2826787216917557, -0.1619651592336595, 0.2813304828151184, -0.2374162813100744... |
706.2219 | On the derivative of the Minkowski question mark function $?(x)$ | Let $ x = [0;a_1,a_2,...]$ be the decomposition of the irrational number $x
\in [0,1]$ into regular continued fraction. Then for the derivative of the
Minkowski function $?(x)$ we prove that $?'(x) = +\infty$ provided $
\limsup_{t\to \infty}\frac{a_1+...+a_t}{t} <\kappa_1 =\frac{2\log
\lambda_1}{\log 2} = 1.388^+$, a... | math.NT | let x 0a_1a_2 be the decomposition of the irrational number x in 01 into regular continued fraction then for the derivative of the minkowski function x we prove that x infty provided limsup_tto inftyfraca_1a_tt kappa_1 frac2log lambda_1log 2 1388 and x 0 provided liminf_tto inftyfraca_1a_tt kappa_2 frac4l_55l_4l_5l_4 4... | [['let', 'x', '0a_1a_2', 'be', 'the', 'decomposition', 'of', 'the', 'irrational', 'number', 'x', 'in', '01', 'into', 'regular', 'continued', 'fraction', 'then', 'for', 'the', 'derivative', 'of', 'the', 'minkowski', 'function', 'x', 'we', 'prove', 'that', 'x', 'infty', 'provided', 'limsup_tto', 'inftyfraca_1a_tt', 'kapp... | [-0.1829398043885611, 0.15859441561759383, -0.007689841845801667, 0.04286257768778697, -0.015762414128614077, -0.16528585728635822, 0.08723499813535507, 0.3534598136185736, -0.30721045139691106, -0.1503922191374274, 0.08936123420869041, -0.33883349570459215, -0.06882870763175837, 0.16099464102729183, -0.039342727046459... |
706.222 | Observation of photoinduced phase transition in phase-separated
Pr$_{0.55}$(Ca$_{1-y}$Sr$_{y}$)$_{0.45}$MnO$_3$ thin films via x-ray
photoemission spectroscopy | Perovskite manganite thin films, $Pr_{0.55}(Ca_{1-y}Sr_y)_{0.45}MnO_3$, have
been studied using x-ray photoemission spectroscopy in order to clarify the
consequence of the competition between ferromagnetic metal (FM) and
charge-orbital ordered insulator (COOI). Films with $y$ = 0.40 undergo uniform
paramagnetic insul... | cond-mat.str-el | perovskite manganite thin films pr_055ca_1ysr_y_045mno_3 have been studied using xray photoemission spectroscopy in order to clarify the consequence of the competition between ferromagnetic metal fm and chargeorbital ordered insulator cooi films with y 040 undergo uniform paramagnetic insulator to fm transition on the ... | [['perovskite', 'manganite', 'thin', 'films', 'pr_055ca_1ysr_y_045mno_3', 'have', 'been', 'studied', 'using', 'xray', 'photoemission', 'spectroscopy', 'in', 'order', 'to', 'clarify', 'the', 'consequence', 'of', 'the', 'competition', 'between', 'ferromagnetic', 'metal', 'fm', 'and', 'chargeorbital', 'ordered', 'insulato... | [-0.1272933367258451, 0.2568932239508887, -0.04264119903073008, -0.00831076800973887, 0.018438231485976477, -0.12022556831847554, 0.14998735870989993, 0.43151658330494025, -0.276610045583816, -0.30975312519979875, 0.02978295680707482, -0.37841945974610924, -0.05037160065230422, 0.13591753945165264, 0.02999770332413806,... |
706.2221 | Generalized pseudo-Newtonian potential for studying accretion disk
dynamics in off-equatorial planes around rotating black holes: Description of
a vector potential | We prescribe a pseudo-Newtonian vector potential for studying accretion disks
around Kerr black holes. The potential is useful to study the inner properties
of disk not confined to the equatorial plane where general relativistic effect
is indispensable. Therefore, we incorporate the essential properties of the
metric... | astro-ph gr-qc | we prescribe a pseudonewtonian vector potential for studying accretion disks around kerr black holes the potential is useful to study the inner properties of disk not confined to the equatorial plane where general relativistic effect is indispensable therefore we incorporate the essential properties of the metric at th... | [['we', 'prescribe', 'a', 'pseudonewtonian', 'vector', 'potential', 'for', 'studying', 'accretion', 'disks', 'around', 'kerr', 'black', 'holes', 'the', 'potential', 'is', 'useful', 'to', 'study', 'the', 'inner', 'properties', 'of', 'disk', 'not', 'confined', 'to', 'the', 'equatorial', 'plane', 'where', 'general', 'rela... | [-0.13241221621865407, 0.07103541268649376, -0.06311046435536506, 0.09167127084995931, -0.07841879783857925, -0.11375907332791636, -0.02968778737510244, 0.345012646385779, -0.2163092592236353, -0.2678142462080965, 0.0813921974884579, -0.2606263521205013, -0.10129577413511773, 0.23930633863589415, -0.03374812960779915, ... |
706.2222 | LHC Signatures of MSSM Higgs-sector CP Violation | We discuss a few new characteristic features of the loop-induced MSSM
Higgs-sector CP violation at the LHC based on two scenarios: (i) CPX and (ii)
Trimixing.
| hep-ph | we discuss a few new characteristic features of the loopinduced mssm higgssector cp violation at the lhc based on two scenarios i cpx and ii trimixing | [['we', 'discuss', 'a', 'few', 'new', 'characteristic', 'features', 'of', 'the', 'loopinduced', 'mssm', 'higgssector', 'cp', 'violation', 'at', 'the', 'lhc', 'based', 'on', 'two', 'scenarios', 'i', 'cpx', 'and', 'ii', 'trimixing']] | [-0.12461614465484253, 0.18289643329066727, 0.0017970809533905524, 0.16405320583054653, -0.11529783460383232, -0.27226564429628736, 0.07020892661351424, 0.2805723502085759, -0.2243628057722862, -0.20976153051910493, 0.061202447127121, -0.2762926461246724, -0.04672877440372339, 0.1348502898338036, 0.04617545814611591, 0... |
706.2223 | Towards the Distribution of the Size of a Largest Planar Matching and
Largest Planar Subgraph in Random Bipartite Graphs | We address the following question: When a randomly chosen regular bipartite
multi--graph is drawn in the plane in the ``standard way'', what is the
distribution of its maximum size planar matching (set of non--crossing disjoint
edges) and maximum size planar subgraph (set of non--crossing edges which may
share endpoi... | math.CO math.PR | we address the following question when a randomly chosen regular bipartite multigraph is drawn in the plane in the standard way what is the distribution of its maximum size planar matching set of noncrossing disjoint edges and maximum size planar subgraph set of noncrossing edges which may share endpoints the problem i... | [['we', 'address', 'the', 'following', 'question', 'when', 'a', 'randomly', 'chosen', 'regular', 'bipartite', 'multigraph', 'is', 'drawn', 'in', 'the', 'plane', 'in', 'the', 'standard', 'way', 'what', 'is', 'the', 'distribution', 'of', 'its', 'maximum', 'size', 'planar', 'matching', 'set', 'of', 'noncrossing', 'disjoin... | [-0.15238812828469406, 0.10573068656173903, -0.04670881612850499, 0.05267763418433164, -0.12352371549584869, -0.11759244828821398, 0.07243878349505795, 0.35647818787969376, -0.31117058271988346, -0.30158198416155046, 0.07918935289870976, -0.3058614953511263, -0.14546883912727782, 0.11032895755671276, -0.121983495609181... |
706.2224 | Existence of Kirillov-Reshetikhin crystals for nonexceptional types | Using the methods of Kang et al. and recent results on the characters of
Kirillov-Reshetikhin modules by Nakajima and Hernandez, the existence of
Kirillov-Reshetikhin crystals B^{r,s} is established for all nonexceptional
affine types. We also prove that the crystals B^{r,s} of type B_n^{(1)},
D_n^{(1)}, and A_{2n-1}... | math.QA math.RT | using the methods of kang et al and recent results on the characters of kirillovreshetikhin modules by nakajima and hernandez the existence of kirillovreshetikhin crystals brs is established for all nonexceptional affine types we also prove that the crystals brs of type b_n1 d_n1 and a_2n12 are isomorphic to recently c... | [['using', 'the', 'methods', 'of', 'kang', 'et', 'al', 'and', 'recent', 'results', 'on', 'the', 'characters', 'of', 'kirillovreshetikhin', 'modules', 'by', 'nakajima', 'and', 'hernandez', 'the', 'existence', 'of', 'kirillovreshetikhin', 'crystals', 'brs', 'is', 'established', 'for', 'all', 'nonexceptional', 'affine', '... | [-0.11833798743279303, 0.07728153185093167, -0.011116472021597674, -0.04163048022635818, -0.13059213838808365, -0.16715963701796482, 0.01399483842680515, 0.34562689031205945, -0.2824227396177791, -0.20889000963987941, 0.08094231781186693, -0.254041386294668, -0.1630507350536221, 0.20365679109374346, -0.1263250345048510... |
706.2225 | Significance Tests for Periodogram Peaks | We discuss methods currently in use for determining the significance of peaks
in the periodograms of time series. We discuss some general methods for
constructing significance tests, false alarm probability functions, and the
role played in these by independent random variables and by empirical and
theoretical cumula... | astro-ph | we discuss methods currently in use for determining the significance of peaks in the periodograms of time series we discuss some general methods for constructing significance tests false alarm probability functions and the role played in these by independent random variables and by empirical and theoretical cumulative ... | [['we', 'discuss', 'methods', 'currently', 'in', 'use', 'for', 'determining', 'the', 'significance', 'of', 'peaks', 'in', 'the', 'periodograms', 'of', 'time', 'series', 'we', 'discuss', 'some', 'general', 'methods', 'for', 'constructing', 'significance', 'tests', 'false', 'alarm', 'probability', 'functions', 'and', 'th... | [-0.09772913516001794, 0.046855381156489684, -0.11056913867665147, 0.12196350967832524, -0.016925825843659852, -0.08119286674083871, 0.1188012692733731, 0.4080067479494706, -0.19521543216321943, -0.28902787580471306, 0.1204572141360383, -0.2545688888419745, -0.1561958159690777, 0.2688935901427153, -0.03244734802328556,... |
706.2226 | The Photonic Module: an on-demand resource for photonic entanglement | Photonic entanglement has a wide range of applications in quantum computation
and communication. Here we introduce a new device: the "photonic module", which
allows for the rapid, deterministic preparation of a large class of entangled
photon states. The module is an application independent, "plug and play"
device, w... | quant-ph | photonic entanglement has a wide range of applications in quantum computation and communication here we introduce a new device the photonic module which allows for the rapid deterministic preparation of a large class of entangled photon states the module is an application independent plug and play device with sufficien... | [['photonic', 'entanglement', 'has', 'a', 'wide', 'range', 'of', 'applications', 'in', 'quantum', 'computation', 'and', 'communication', 'here', 'we', 'introduce', 'a', 'new', 'device', 'the', 'photonic', 'module', 'which', 'allows', 'for', 'the', 'rapid', 'deterministic', 'preparation', 'of', 'a', 'large', 'class', 'o... | [-0.1514998473937559, 0.14452199645341446, -0.056019679851958465, -0.021644894919831882, -0.029173710877236365, -0.21400078794324834, 0.036763091987111314, 0.41652083579964677, -0.26926800296722175, -0.28089780129235364, 0.07512124822824262, -0.2031891925185407, -0.13737408021175912, 0.26137640943814966, -0.06236938654... |
706.2227 | The Norma Cluster (ACO 3627): I. A Dynamical Analysis of the Most
Massive Cluster in the Great Attractor | A detailed dynamical analysis of the nearby rich Norma cluster (ACO 3627) is
presented. From radial velocities of 296 cluster members, we find a mean
velocity of 4871 +/- 54 km/s and a velocity dispersion of 925 km/s. The mean
velocity of the E/S0 population (4979 +/- 85 km/s) is offset with respect to
that of the S/... | astro-ph | a detailed dynamical analysis of the nearby rich norma cluster aco 3627 is presented from radial velocities of 296 cluster members we find a mean velocity of 4871 54 kms and a velocity dispersion of 925 kms the mean velocity of the es0 population 4979 85 kms is offset with respect to that of the sirr population 4812 70... | [['a', 'detailed', 'dynamical', 'analysis', 'of', 'the', 'nearby', 'rich', 'norma', 'cluster', 'aco', '3627', 'is', 'presented', 'from', 'radial', 'velocities', 'of', '296', 'cluster', 'members', 'we', 'find', 'a', 'mean', 'velocity', 'of', '4871', '54', 'kms', 'and', 'a', 'velocity', 'dispersion', 'of', '925', 'kms', ... | [-0.13375248887883795, 0.10092323133465149, -0.11044681229711852, 0.03720665112339546, -0.10010410394157153, -0.041951204598480965, 0.035971604106416796, 0.4273872892140533, -0.21450175278834846, -0.32528153324749415, 0.030171330412428372, -0.2842351431527483, 0.010434227700585424, 0.14286691677330982, 0.00574637405332... |
706.2228 | Periodic harmonic functions on lattices and points count in positive
characteristic | This survey addresses pluri-periodic harmonic functions on lattices with
values in a positive characteristic field. We mention, as a motivation, the
game "Lights Out" following the work of Sutner, Goldwasser-Klostermeyer-Ware,
Barua-Ramakrishnan-Sarkar, Hunzikel-Machiavello-Park e.a.; see also 2 previous
author's pre... | math.AG math.SP | this survey addresses pluriperiodic harmonic functions on lattices with values in a positive characteristic field we mention as a motivation the game lights out following the work of sutner goldwasserklostermeyerware baruaramakrishnansarkar hunzikelmachiavellopark ea see also 2 previous authors preprints for a more det... | [['this', 'survey', 'addresses', 'pluriperiodic', 'harmonic', 'functions', 'on', 'lattices', 'with', 'values', 'in', 'a', 'positive', 'characteristic', 'field', 'we', 'mention', 'as', 'a', 'motivation', 'the', 'game', 'lights', 'out', 'following', 'the', 'work', 'of', 'sutner', 'goldwasserklostermeyerware', 'baruaramak... | [-0.12911528585371687, 0.019035438961362013, -0.1338499977781966, 0.08397026891612473, -0.1236897208035697, -0.11325764279762232, 0.04498401115572936, 0.36600043423272466, -0.24501932361414908, -0.2210118622091171, 0.050829255045706255, -0.2531791965233719, -0.18221013852067897, 0.25763555534335003, -0.0717964964742596... |
706.2229 | AF-embedding of the crossed products of AH-algebras by finitely
generated abelian groups | Let $X$ be a compact metric space and let $\Lambda$ be a $\Z^k$ ($k\ge 1$)
action on $X.$ We give a solution to a version of Voiculescu's problem of
AF-embedding: The crossed product $C(X)\rtimes_{\Lambda}\Z^k$ can be embedded
into a unital simple AF-algebra if and only if $X$ admits a strictly positive
$\Lambda$-inv... | math.OA math.FA | let x be a compact metric space and let lambda be a zk kge 1 action on x we give a solution to a version of voiculescus problem of afembedding the crossed product cxrtimes_lambdazk can be embedded into a unital simple afalgebra if and only if x admits a strictly positive lambdainvariant borel probability measure let c ... | [['let', 'x', 'be', 'a', 'compact', 'metric', 'space', 'and', 'let', 'lambda', 'be', 'a', 'zk', 'kge', '1', 'action', 'on', 'x', 'we', 'give', 'a', 'solution', 'to', 'a', 'version', 'of', 'voiculescus', 'problem', 'of', 'afembedding', 'the', 'crossed', 'product', 'cxrtimes_lambdazk', 'can', 'be', 'embedded', 'into', 'a... | [-0.17613376460668415, 0.16580769317836097, -0.16256024004571668, -0.022986441196560993, -0.11420126210879346, -0.2850090279620178, -0.005726907910271125, 0.4050485598619538, -0.36501032460217525, -0.0905965216589546, 0.09050027797506614, -0.26442956652567545, -0.04442666300732379, 0.1906475992308873, -0.13607281268658... |
706.223 | Limited resolution and multiresolution methods in complex network
community detection | Detecting community structure in real-world networks is a challenging
problem. Recently, it has been shown that the resolution of methods based on
optimizing a modularity measure or a corresponding energy is limited;
communities with sizes below some threshold remain unresolved. One possibility
to go around this prob... | physics.soc-ph | detecting community structure in realworld networks is a challenging problem recently it has been shown that the resolution of methods based on optimizing a modularity measure or a corresponding energy is limited communities with sizes below some threshold remain unresolved one possibility to go around this problem is ... | [['detecting', 'community', 'structure', 'in', 'realworld', 'networks', 'is', 'a', 'challenging', 'problem', 'recently', 'it', 'has', 'been', 'shown', 'that', 'the', 'resolution', 'of', 'methods', 'based', 'on', 'optimizing', 'a', 'modularity', 'measure', 'or', 'a', 'corresponding', 'energy', 'is', 'limited', 'communit... | [-0.06417799540266225, 0.05460500036768446, -0.08163430143825033, 0.09658546808641404, -0.05308499196967618, -0.1493395528770634, 0.03957020972262729, 0.4297969733110883, -0.2589164629070596, -0.34366324820809746, 0.13992569218707188, -0.23521683836165308, -0.17523736562791534, 0.19024652990893545, -0.02748972302810712... |
706.2231 | Study of tau- -> K_S pi- nu_tau decay at Belle | We present a study of the decay tau- -> K_S pi- nu_tau using a 351 fb^-1 data
sample collected with the Belle detector. The analysis is based on 53110
lepton-tagged signal events. The measured branching fraction B(tau- -> K_S pi-
nu_tau)=(0.404 +- 0.002(stat.) +- 0.013(syst.))% is consistent with the world
average va... | hep-ex | we present a study of the decay tau k_s pi nu_tau using a 351 fb1 data sample collected with the belle detector the analysis is based on 53110 leptontagged signal events the measured branching fraction btau k_s pi nu_tau0404 0002stat 0013syst is consistent with the world average value and has better accuracy an analysi... | [['we', 'present', 'a', 'study', 'of', 'the', 'decay', 'tau', 'k_s', 'pi', 'nu_tau', 'using', 'a', '351', 'fb1', 'data', 'sample', 'collected', 'with', 'the', 'belle', 'detector', 'the', 'analysis', 'is', 'based', 'on', '53110', 'leptontagged', 'signal', 'events', 'the', 'measured', 'branching', 'fraction', 'btau', 'k_... | [-0.08330076020412926, 0.16317307215070528, -0.09234296281498913, 0.08875137938029722, -0.04432257393533031, -0.08532526084621038, 0.08100598355593654, 0.3196238952270728, -0.1502938595201288, -0.33260435498870755, 0.0075003199162893, -0.39479229378761077, 0.026755386474067156, 0.16846175800904403, 0.07603968397657178,... |
706.2232 | Characterization of intrinsically harmonic forms | Let $M$ be a closed oriented manifold of dimension $n$ and $\omega$ a closed
1-form on it. We discuss the question whether there exists a Riemannian metric
for which $\omega$ is co-closed. For closed 1-forms with nondegenerate zeros
the question was answered completely by Calabi in 1969. The goal of this paper
is to ... | math.DG | let m be a closed oriented manifold of dimension n and omega a closed 1form on it we discuss the question whether there exists a riemannian metric for which omega is coclosed for closed 1forms with nondegenerate zeros the question was answered completely by calabi in 1969 the goal of this paper is to give an answer in ... | [['let', 'm', 'be', 'a', 'closed', 'oriented', 'manifold', 'of', 'dimension', 'n', 'and', 'omega', 'a', 'closed', '1form', 'on', 'it', 'we', 'discuss', 'the', 'question', 'whether', 'there', 'exists', 'a', 'riemannian', 'metric', 'for', 'which', 'omega', 'is', 'coclosed', 'for', 'closed', '1forms', 'with', 'nondegenera... | [-0.21460376912727952, 0.09755029968336101, -0.05510629260809057, 0.05823428191069979, -0.13550540823618779, -0.19221348335526678, 0.027407445196230482, 0.3363864117483091, -0.2530658525259544, -0.22152072029550457, 0.07492009445235857, -0.26879358023870736, -0.14177139919290008, 0.17809288059975692, -0.134509401872896... |
706.2233 | Two-dimensional defect modes in optically induced photonic lattices | In this article, localized linear defect modes due to bandgap guidance in
two-dimensional photonic lattices with localized or non-localized defects are
investigated theoretically. First, when the defect is localized and weak,
eigenvalues of defect modes bifurcated from edges of Bloch bands are derived
analytically. I... | physics.optics | in this article localized linear defect modes due to bandgap guidance in twodimensional photonic lattices with localized or nonlocalized defects are investigated theoretically first when the defect is localized and weak eigenvalues of defect modes bifurcated from edges of bloch bands are derived analytically it is show... | [['in', 'this', 'article', 'localized', 'linear', 'defect', 'modes', 'due', 'to', 'bandgap', 'guidance', 'in', 'twodimensional', 'photonic', 'lattices', 'with', 'localized', 'or', 'nonlocalized', 'defects', 'are', 'investigated', 'theoretically', 'first', 'when', 'the', 'defect', 'is', 'localized', 'and', 'weak', 'eige... | [-0.1351082551402999, 0.23080095236297207, -0.03340142932339644, 0.054322701899185914, -0.04299452171667884, -0.2022251181726839, 0.022826337120513046, 0.41463421618991764, -0.2743579954424783, -0.21483049039005347, 0.0646861645849214, -0.3305623146448264, -0.15892045067356672, 0.14215054227728188, 0.03165726729479989,... |
706.2234 | A wide deep infrared look at the Pleiades with UKIDSS: new constraints
on the substellar binary fraction and the low mass IMF | We present the results of a deep wide-field near-infrared survey of 12 square
degrees of the Pleiades conducted as part of the UKIDSS Deep Infrared Sky
Survey (UKIDSS) Galactic Cluster Survey (GCS). We have extracted over 340 high
probability proper motion members down to 0.03 solar masses using a combination
of UKID... | astro-ph | we present the results of a deep widefield nearinfrared survey of 12 square degrees of the pleiades conducted as part of the ukidss deep infrared sky survey ukidss galactic cluster survey gcs we have extracted over 340 high probability proper motion members down to 003 solar masses using a combination of ukidss photome... | [['we', 'present', 'the', 'results', 'of', 'a', 'deep', 'widefield', 'nearinfrared', 'survey', 'of', '12', 'square', 'degrees', 'of', 'the', 'pleiades', 'conducted', 'as', 'part', 'of', 'the', 'ukidss', 'deep', 'infrared', 'sky', 'survey', 'ukidss', 'galactic', 'cluster', 'survey', 'gcs', 'we', 'have', 'extracted', 'ov... | [-0.04866617515951435, 0.07985247038709728, -0.08843862329528708, 0.05698920262714281, -0.15311845610647098, -0.02840247126903547, 0.14579904440122293, 0.38704515322739175, -0.10837003012825533, -0.39556052320150903, 0.05169213266496587, -0.3460044652081864, -0.048635385992795065, 0.23055336861162568, -0.07874095667477... |
706.2235 | Sn1987a Revisited after 20 Years: May the Supernova Bang More Than Once? | The observations of supernova 1987A in underground detectors are revisited.
It is shown that, while the LSD detector in the Mont Blanc Laboratory observed
only one burst at 2h 52min 36.8sec U.T., the Kamiokande data show a possible
second burst, in addition to the well known one at 7h 35min 33.7sec U.T. This
second b... | gr-qc astro-ph | the observations of supernova 1987a in underground detectors are revisited it is shown that while the lsd detector in the mont blanc laboratory observed only one burst at 2h 52min 368sec ut the kamiokande data show a possible second burst in addition to the well known one at 7h 35min 337sec ut this second burst consist... | [['the', 'observations', 'of', 'supernova', '1987a', 'in', 'underground', 'detectors', 'are', 'revisited', 'it', 'is', 'shown', 'that', 'while', 'the', 'lsd', 'detector', 'in', 'the', 'mont', 'blanc', 'laboratory', 'observed', 'only', 'one', 'burst', 'at', '2h', '52min', '368sec', 'ut', 'the', 'kamiokande', 'data', 'sh... | [-0.079232731454677, 0.12992046366938773, -0.03591178726843175, 0.11267039475633818, -0.014417545716552174, -0.13293745775214014, 0.025818562792504534, 0.3735685565673253, -0.1911940799697357, -0.3389373143439811, 0.128932259748142, -0.3374159170424237, -0.03693734339493163, 0.21818472589777016, 0.02132468548439005, 0.... |
706.2236 | Solution of the Dirac Equation using the Lanczos Algorithm | Covergent eigensolutions of the Dirac Equation for a relativistic electron in
an external Coulomb potential are obtained using the Lanczos Algorithm. A
tri-diagonal matrix representation of the Dirac Hamiltonian operator is
constructed iteratively and diagonalized after each iteration step to form a
sequence of conve... | math-ph math.GM math.MP | covergent eigensolutions of the dirac equation for a relativistic electron in an external coulomb potential are obtained using the lanczos algorithm a tridiagonal matrix representation of the dirac hamiltonian operator is constructed iteratively and diagonalized after each iteration step to form a sequence of convergen... | [['covergent', 'eigensolutions', 'of', 'the', 'dirac', 'equation', 'for', 'a', 'relativistic', 'electron', 'in', 'an', 'external', 'coulomb', 'potential', 'are', 'obtained', 'using', 'the', 'lanczos', 'algorithm', 'a', 'tridiagonal', 'matrix', 'representation', 'of', 'the', 'dirac', 'hamiltonian', 'operator', 'is', 'co... | [-0.13428926379343525, 0.10923014387519854, -0.10157054013832183, 0.06138623577015871, -0.06033740485789346, -0.1838006635929351, 0.012146686466666489, 0.3336822341089366, -0.31826244404570003, -0.24490994351656467, 0.06594616960024187, -0.30553577412835886, -0.1486844286345495, 0.1230555951717447, 0.052521415772374534... |
706.2237 | A brief note on how to unify dark matter, dark energy, and inflation | A scenario in which inflation, dark energy and dark matter can be unified
into a single scalar field, the inflaton field $\phi$, is studied. The inflaton
is identified with the sneutrino, the scalar partner of the heavy neutrino. We
determine the conditions needed for avoiding the gravitino problem and not
having neg... | hep-ph | a scenario in which inflation dark energy and dark matter can be unified into a single scalar field the inflaton field phi is studied the inflaton is identified with the sneutrino the scalar partner of the heavy neutrino we determine the conditions needed for avoiding the gravitino problem and not having negligible pla... | [['a', 'scenario', 'in', 'which', 'inflation', 'dark', 'energy', 'and', 'dark', 'matter', 'can', 'be', 'unified', 'into', 'a', 'single', 'scalar', 'field', 'the', 'inflaton', 'field', 'phi', 'is', 'studied', 'the', 'inflaton', 'is', 'identified', 'with', 'the', 'sneutrino', 'the', 'scalar', 'partner', 'of', 'the', 'hea... | [-0.16965904276366928, 0.26773694778967183, -0.08257921107724542, 0.18672993870495702, -0.10737831117512542, -0.1884426500328118, -0.02469505493354518, 0.29734271625056863, -0.21490547372377478, -0.35222595278173685, 0.019279150028523873, -0.19103513720619958, 0.005582669458817691, 0.13379054921097122, 0.03910421510227... |
706.2238 | Renormalization Reductions for Systems with Delay | The renormalization method which is a type of perturbation method is extended
to a tool to study weakly nonlinear time-delay systems. For systems with
order-one delay, we show that the renormalization method leads to reduced
systems without delay. For systems with order-one and large-delay, we propose
an extended ren... | nlin.PS nlin.CD | the renormalization method which is a type of perturbation method is extended to a tool to study weakly nonlinear timedelay systems for systems with orderone delay we show that the renormalization method leads to reduced systems without delay for systems with orderone and largedelay we propose an extended renormalizati... | [['the', 'renormalization', 'method', 'which', 'is', 'a', 'type', 'of', 'perturbation', 'method', 'is', 'extended', 'to', 'a', 'tool', 'to', 'study', 'weakly', 'nonlinear', 'timedelay', 'systems', 'for', 'systems', 'with', 'orderone', 'delay', 'we', 'show', 'that', 'the', 'renormalization', 'method', 'leads', 'to', 're... | [-0.12643365282565355, 0.0527421151236922, -0.10997717324755199, 0.04115142683786828, -0.018485824821428173, -0.16804936283179336, 0.0415457053625557, 0.36775900711793275, -0.25327710982500795, -0.28200442504714285, 0.0957537621960953, -0.26127812676436624, -0.22170827242856225, 0.2661364196489255, -0.03052570030004495... |
706.2239 | Infinitesimal Castelnuovo Theory in Abelian Varieties | The purpose of this article is to show that the Castelnuovo theory for
abelian varieties, developed by G. Pareschi and M. Popa, can be
infinitesimalized. More precisely, we prove that an irreducible principally
polarized abelian variety has a finite scheme in extremal position, in the
sense of Castelnuovo theory for ... | math.AG | the purpose of this article is to show that the castelnuovo theory for abelian varieties developed by g pareschi and m popa can be infinitesimalized more precisely we prove that an irreducible principally polarized abelian variety has a finite scheme in extremal position in the sense of castelnuovo theory for abelian v... | [['the', 'purpose', 'of', 'this', 'article', 'is', 'to', 'show', 'that', 'the', 'castelnuovo', 'theory', 'for', 'abelian', 'varieties', 'developed', 'by', 'g', 'pareschi', 'and', 'm', 'popa', 'can', 'be', 'infinitesimalized', 'more', 'precisely', 'we', 'prove', 'that', 'an', 'irreducible', 'principally', 'polarized', '... | [-0.1437172143622234, 0.10609083559783344, -0.1692374501330103, 0.06675665433167656, -0.08706362436161093, -0.1638851564553013, -0.02511524085454859, 0.35551372507884016, -0.3163763361888519, -0.1772280417220748, 0.09511250247453353, -0.22559757760820398, -0.1758711428206036, 0.24119397736343462, -0.19520571024791486, ... |
706.224 | Vibration-mediated resonant tunneling and shot noise through a molecular
quantum dot | Motivated by a recent experiment on nonlinear tunneling in a suspended Carbon
nanotube connected to two normal electrodes [S. Sapmaz, {\it et al}., Phys.
Rev. Lett. {\bf 96}, 26801 (2006)], we investigate nonequilibrium
vibration-mediated sequential tunneling through a molecular quantum dot with
two electronic orbita... | cond-mat.mes-hall | motivated by a recent experiment on nonlinear tunneling in a suspended carbon nanotube connected to two normal electrodes s sapmaz it et al phys rev lett bf 96 26801 2006 we investigate nonequilibrium vibrationmediated sequential tunneling through a molecular quantum dot with two electronic orbitals asymmetrically coup... | [['motivated', 'by', 'a', 'recent', 'experiment', 'on', 'nonlinear', 'tunneling', 'in', 'a', 'suspended', 'carbon', 'nanotube', 'connected', 'to', 'two', 'normal', 'electrodes', 's', 'sapmaz', 'it', 'et', 'al', 'phys', 'rev', 'lett', 'bf', '96', '26801', '2006', 'we', 'investigate', 'nonequilibrium', 'vibrationmediated... | [-0.15810017435879056, 0.1531417487057033, -0.0177549947484918, -0.0369041868346563, -0.05207617972947417, -0.20469386118178767, 0.08424169144352837, 0.3596771656866035, -0.2290514479363112, -0.26191435581553846, -0.07605568354483694, -0.3139521975047706, -0.20636811779413913, 0.18487995106824523, -0.04288369051421121,... |
706.2241 | Dynamics-Controlled Truncation Scheme for Nonlinear Dynamics in
Semiconductor Microcavities | We present a systematic theory of Coulomb-induced correlation effects in the
nonlinear optical processes within the strong-coupling regime. In this paper we
shall set a dynamics controlled truncation scheme \cite{Axt Stahl} microscopic
treatment of nonlinear parametric processes in SMCs including the
electromagnetic ... | cond-mat.mes-hall | we present a systematic theory of coulombinduced correlation effects in the nonlinear optical processes within the strongcoupling regime in this paper we shall set a dynamics controlled truncation scheme citeaxt stahl microscopic treatment of nonlinear parametric processes in smcs including the electromagnetic field qu... | [['we', 'present', 'a', 'systematic', 'theory', 'of', 'coulombinduced', 'correlation', 'effects', 'in', 'the', 'nonlinear', 'optical', 'processes', 'within', 'the', 'strongcoupling', 'regime', 'in', 'this', 'paper', 'we', 'shall', 'set', 'a', 'dynamics', 'controlled', 'truncation', 'scheme', 'citeaxt', 'stahl', 'micros... | [-0.12414575247701419, 0.15469008824531583, -0.10822916286660061, 0.09604814958816016, -0.03401342777035914, -0.11659735593475752, 0.07202595726931063, 0.3307455896359423, -0.25916358675686235, -0.247730182159854, -0.01983173133086656, -0.2673171680366647, -0.16480099287666922, 0.17603194835744257, 0.01765195793721933,... |
706.2242 | HERMES measurements of Collins and Sivers asymmetries from a
transversely polarised hydrogen target | Azimuthal single-spin asymmetries (SSA) in semi-inclusive electroproduction
of pi-mesons and charged K-mesons in deep-inelastic scattering of positrons and
electrons on a transversely polarised hydrogen target were observed.
Significant SSA amplitudes for both the Collins and the Sivers mechanism are
presented for th... | hep-ex | azimuthal singlespin asymmetries ssa in semiinclusive electroproduction of pimesons and charged kmesons in deepinelastic scattering of positrons and electrons on a transversely polarised hydrogen target were observed significant ssa amplitudes for both the collins and the sivers mechanism are presented for the full dat... | [['azimuthal', 'singlespin', 'asymmetries', 'ssa', 'in', 'semiinclusive', 'electroproduction', 'of', 'pimesons', 'and', 'charged', 'kmesons', 'in', 'deepinelastic', 'scattering', 'of', 'positrons', 'and', 'electrons', 'on', 'a', 'transversely', 'polarised', 'hydrogen', 'target', 'were', 'observed', 'significant', 'ssa'... | [-0.03915109798846835, 0.25277476599095045, -0.10404551588861202, 0.1979295267826981, -0.010038572363555431, -0.04826047598315334, -0.04187572361142547, 0.4472472779452801, -0.14129324312563296, -0.16220963580740821, -0.1568570851339717, -0.41437618706927254, 0.11696779817618706, 0.17759950405538635, 0.1842569329568909... |
706.2243 | GAVO Tools for the Analysis of Stars and Nebulae | Within the framework of the German Astrophysical Virtual Observatory (GAVO),
we provide synthetic spectra, simulation software for the calculation of NLTE
model atmospheres, as well as necessary atomic data. This will enable a VO user
to directly compare observation and model-atmosphere spectra on three levels:
The e... | astro-ph | within the framework of the german astrophysical virtual observatory gavo we provide synthetic spectra simulation software for the calculation of nlte model atmospheres as well as necessary atomic data this will enable a vo user to directly compare observation and modelatmosphere spectra on three levels the easiest and... | [['within', 'the', 'framework', 'of', 'the', 'german', 'astrophysical', 'virtual', 'observatory', 'gavo', 'we', 'provide', 'synthetic', 'spectra', 'simulation', 'software', 'for', 'the', 'calculation', 'of', 'nlte', 'model', 'atmospheres', 'as', 'well', 'as', 'necessary', 'atomic', 'data', 'this', 'will', 'enable', 'a'... | [-0.024373949126068814, 0.04783484591280285, -0.06215542290204515, 0.1056845634089162, -0.09177826327892641, -0.1371100948463815, 0.09492431460821535, 0.4051733052978913, -0.20188271742857372, -0.4008657525138309, 0.06327551715367008, -0.27897582386697956, -0.06831928480338927, 0.22931544118376526, -0.00523588903427783... |
706.2244 | The Yule distribution and frailty--a note on spurious preferential
attachment | Preferential attachment is a popular generative mechanism to explain the
widespread observation of power law distributed networks. We introduce an
alternative explanation for the phenomenon by allowing the link growth rates to
vary across the nodes according to a randomized Poisson process. The
distribution of rates,... | physics.soc-ph | preferential attachment is a popular generative mechanism to explain the widespread observation of power law distributed networks we introduce an alternative explanation for the phenomenon by allowing the link growth rates to vary across the nodes according to a randomized poisson process the distribution of rates whic... | [['preferential', 'attachment', 'is', 'a', 'popular', 'generative', 'mechanism', 'to', 'explain', 'the', 'widespread', 'observation', 'of', 'power', 'law', 'distributed', 'networks', 'we', 'introduce', 'an', 'alternative', 'explanation', 'for', 'the', 'phenomenon', 'by', 'allowing', 'the', 'link', 'growth', 'rates', 't... | [-0.1012652852234668, 0.10137175865983249, -0.07861334145726527, 0.09151864121084895, -0.052636713163890674, -0.12163495720254586, 0.10375107328097026, 0.42950895639574704, -0.3210305530468331, -0.28490642586942105, 0.011267410448578862, -0.23565153935901345, -0.16330957982470007, 0.1187535342714731, -0.039168439878552... |
706.2245 | HST Spectroscopy of the Hottest White Dwarfs | Spectral analysis needs the observation of lines of successive ionization
stages in order to evaluate the ionization equilibrium (of a particular
species) which is a sensitive indicator for the effective temperature. Since
stars with effective temperatures as high as 100000 K have their flux maximum
in the extreme ul... | astro-ph | spectral analysis needs the observation of lines of successive ionization stages in order to evaluate the ionization equilibrium of a particular species which is a sensitive indicator for the effective temperature since stars with effective temperatures as high as 100000 k have their flux maximum in the extreme ultravi... | [['spectral', 'analysis', 'needs', 'the', 'observation', 'of', 'lines', 'of', 'successive', 'ionization', 'stages', 'in', 'order', 'to', 'evaluate', 'the', 'ionization', 'equilibrium', 'of', 'a', 'particular', 'species', 'which', 'is', 'a', 'sensitive', 'indicator', 'for', 'the', 'effective', 'temperature', 'since', 's... | [-0.01730010408389044, 0.13189865322624117, -0.0531058540465693, 0.052018798275353155, -0.07446014696942668, -0.10276673590024449, 0.048990025944140266, 0.4402910248210577, -0.12661645868362553, -0.3896521373702953, 0.07840131759190651, -0.2929794550075974, -0.0311848291527633, 0.20659473374938872, -0.04320394603076250... |
706.2246 | Effect of Zn substitution on the suppression of Tc of
Y1-xCaxBa2(Cu1-yZny)3O7-delta superconductors: pseudogap and the systematic
shift of the optimum hole content | The effect of Zn substitution on the superconducting transition temperature,
Tc, was investigated for the sintered Y1-xCaxBa2(Cu1-yZny)3O7-delta compounds
over a wide range of hole concentration per CuO2 plane, p. Ca substitution
enabled us to study the deeply overdoped region. p was changed by changing the
oxygen de... | cond-mat.supr-con | the effect of zn substitution on the superconducting transition temperature tc was investigated for the sintered y1xcaxba2cu1yzny3o7delta compounds over a wide range of hole concentration per cuo2 plane p ca substitution enabled us to study the deeply overdoped region p was changed by changing the oxygen deficiency del... | [['the', 'effect', 'of', 'zn', 'substitution', 'on', 'the', 'superconducting', 'transition', 'temperature', 'tc', 'was', 'investigated', 'for', 'the', 'sintered', 'y1xcaxba2cu1yzny3o7delta', 'compounds', 'over', 'a', 'wide', 'range', 'of', 'hole', 'concentration', 'per', 'cuo2', 'plane', 'p', 'ca', 'substitution', 'ena... | [-0.12245737010962329, 0.17955020618780207, 0.007847343280445784, 0.02365187222021632, -0.017529343041436125, -0.15482634853494043, 0.1654335232723194, 0.35333524252443266, -0.2374378620336453, -0.2903792900654177, 0.0138379057093213, -0.38333665300160646, -0.06191500592200706, 0.16438849919165174, 0.008564628037614359... |
706.2247 | A refinement of Khovanov-Rozansky link homology | This paper has been withdrawn by the author due to an error in the proof of
Theorem 1.
| math.GT math.QA | this paper has been withdrawn by the author due to an error in the proof of theorem 1 | [['this', 'paper', 'has', 'been', 'withdrawn', 'by', 'the', 'author', 'due', 'to', 'an', 'error', 'in', 'the', 'proof', 'of', 'theorem', '1']] | [-0.09137122633142604, -0.0333753545540579, -0.14379465166065428, -0.028218396557753697, -0.045740389058159456, -0.06819083934856786, 0.0025127139524556696, 0.26305313035845757, -0.27529351268377567, -0.3565234085544944, 0.13489262885802114, -0.2752506886091497, -0.12623161439680392, 0.13973752864533, -0.32194805962757... |
706.2248 | Anticorrelation between temperature and fluctuations in moderately
damped Josephson junctions | We study the influence of dissipation on the switching current statistics of
moderately damped Josephson junctions. Different types of both low- and high-
$T_c$ junctions with controlled damping are studied. The damping parameter of
the junctions is tuned in a wide range by changing temperature, magnetic field,
gate ... | cond-mat.supr-con | we study the influence of dissipation on the switching current statistics of moderately damped josephson junctions different types of both low and high t_c junctions with controlled damping are studied the damping parameter of the junctions is tuned in a wide range by changing temperature magnetic field gate voltage in... | [['we', 'study', 'the', 'influence', 'of', 'dissipation', 'on', 'the', 'switching', 'current', 'statistics', 'of', 'moderately', 'damped', 'josephson', 'junctions', 'different', 'types', 'of', 'both', 'low', 'and', 'high', 't_c', 'junctions', 'with', 'controlled', 'damping', 'are', 'studied', 'the', 'damping', 'paramet... | [-0.2445364660833139, 0.23717258014189807, -0.009693320928330439, 0.0214512428569108, -0.0452879164620991, -0.17689590592382717, 0.08882902557894155, 0.33354864917371585, -0.25776608594004874, -0.2984371825485774, 0.04255733525623446, -0.2646902509614069, -0.08669194462540411, 0.24634753516369054, -0.002476568806214609... |
706.2249 | Distributed implementation of standard oracle operators | The standard oracle operator corresponding to a function f is a unitary
operator that computes this function coherently, i.e. it maintains
superpositions. This operator acts on a bipartite system, where the subsystems
are the input and output registers. In distributed quantum computation, these
subsystems may be spat... | quant-ph | the standard oracle operator corresponding to a function f is a unitary operator that computes this function coherently ie it maintains superpositions this operator acts on a bipartite system where the subsystems are the input and output registers in distributed quantum computation these subsystems may be spatially sep... | [['the', 'standard', 'oracle', 'operator', 'corresponding', 'to', 'a', 'function', 'f', 'is', 'a', 'unitary', 'operator', 'that', 'computes', 'this', 'function', 'coherently', 'ie', 'it', 'maintains', 'superpositions', 'this', 'operator', 'acts', 'on', 'a', 'bipartite', 'system', 'where', 'the', 'subsystems', 'are', 't... | [-0.16967195825257886, 0.15341239329397374, -0.053287873346487, 0.03950638721480259, -0.029080977586322818, -0.19955300955615682, 0.052642656536772844, 0.37697101968244234, -0.32815945783051953, -0.24683301743633787, 0.08851536376931672, -0.2688597085837532, -0.1213615480312628, 0.2015706032225541, -0.11108389337414651... |
706.225 | Sign lemma for dimension shifting | There is a surprising occurrence of some minus signs in the isomorphisms
produced in the well-known technique of dimension shifting in calculating
derived functors in homological algebra. We explicitly determine these signs.
Getting these signs right is important in order to avoid basic contradictions.
We illustrate ... | math.AG math.AT | there is a surprising occurrence of some minus signs in the isomorphisms produced in the wellknown technique of dimension shifting in calculating derived functors in homological algebra we explicitly determine these signs getting these signs right is important in order to avoid basic contradictions we illustrate the le... | [['there', 'is', 'a', 'surprising', 'occurrence', 'of', 'some', 'minus', 'signs', 'in', 'the', 'isomorphisms', 'produced', 'in', 'the', 'wellknown', 'technique', 'of', 'dimension', 'shifting', 'in', 'calculating', 'derived', 'functors', 'in', 'homological', 'algebra', 'we', 'explicitly', 'determine', 'these', 'signs', ... | [-0.1878729336513359, 0.06789004434755103, -0.09159895122723012, 0.15050818482948253, -0.12255131821987815, -0.14466838731018247, 0.004954655345559853, 0.32920607391622714, -0.3138299545609072, -0.26126538394171683, 0.11523796003655393, -0.2474195088572861, -0.19310653673820807, 0.17434439096660886, -0.1838627724343391... |
706.2251 | A polaritonic two-component Bose-Hubbard model | We show that polaritons in an array of interacting micro-cavities with strong
atom-photon coupling can form a two-component Bose-Hubbard model. Both
polariton species are thereby protected against spontaneous emission as their
atomic part is stored in two ground states of the atoms. The parameters of the
effective mo... | quant-ph cond-mat.str-el | we show that polaritons in an array of interacting microcavities with strong atomphoton coupling can form a twocomponent bosehubbard model both polariton species are thereby protected against spontaneous emission as their atomic part is stored in two ground states of the atoms the parameters of the effective model can ... | [['we', 'show', 'that', 'polaritons', 'in', 'an', 'array', 'of', 'interacting', 'microcavities', 'with', 'strong', 'atomphoton', 'coupling', 'can', 'form', 'a', 'twocomponent', 'bosehubbard', 'model', 'both', 'polariton', 'species', 'are', 'thereby', 'protected', 'against', 'spontaneous', 'emission', 'as', 'their', 'at... | [-0.1526707839956017, 0.2590446783136653, -0.02093608553619369, 0.033817280361147006, 0.015199675200212943, -0.18844791086341597, 0.04025968242020003, 0.4344276043243314, -0.23992084971580066, -0.29484954928538126, -0.01276630936895105, -0.27250545065065745, -0.08428636006398224, 0.19692830918479318, 0.0610453162930513... |
706.2252 | Time and M-theory | We review our recent proposal for a background independent formulation of a
holographic theory of quantum gravity. The present review incorporates the
necessary background material on geometry of canonical quantum theory,
holography and spacetime thermodynamics, Matrix theory, as well as our specific
proposal for a d... | hep-th | we review our recent proposal for a background independent formulation of a holographic theory of quantum gravity the present review incorporates the necessary background material on geometry of canonical quantum theory holography and spacetime thermodynamics matrix theory as well as our specific proposal for a dynamic... | [['we', 'review', 'our', 'recent', 'proposal', 'for', 'a', 'background', 'independent', 'formulation', 'of', 'a', 'holographic', 'theory', 'of', 'quantum', 'gravity', 'the', 'present', 'review', 'incorporates', 'the', 'necessary', 'background', 'material', 'on', 'geometry', 'of', 'canonical', 'quantum', 'theory', 'holo... | [-0.07683410726132847, 0.11461498590762771, -0.12634726354417147, 0.07713028262923693, -0.06756190269121103, -0.12351230321828985, 0.01603328188371268, 0.25411882666604857, -0.23456863901090055, -0.2866308223633539, 0.08981586424966476, -0.2284776419223774, -0.21873399444988795, 0.1951015144586563, -0.10112022613840443... |
706.2253 | A note on fermions in holographic QCD | We study the fermionic sector of a probe D8-brane in the supergravity
background made of D4-branes compactified on a circle with supersymmetry broken
explicitly by the boundary conditions. At low energies the dual field theory is
effectively four-dimensional and has proved surprisingly successful in
recovering qualit... | hep-th | we study the fermionic sector of a probe d8brane in the supergravity background made of d4branes compactified on a circle with supersymmetry broken explicitly by the boundary conditions at low energies the dual field theory is effectively fourdimensional and has proved surprisingly successful in recovering qualitative ... | [['we', 'study', 'the', 'fermionic', 'sector', 'of', 'a', 'probe', 'd8brane', 'in', 'the', 'supergravity', 'background', 'made', 'of', 'd4branes', 'compactified', 'on', 'a', 'circle', 'with', 'supersymmetry', 'broken', 'explicitly', 'by', 'the', 'boundary', 'conditions', 'at', 'low', 'energies', 'the', 'dual', 'field',... | [-0.12836486712950182, 0.2498045664694299, -0.0816777263442302, 0.13642804500612213, -0.04079828355857666, -0.13289135801506805, -0.0071585861076799, 0.3416724468289102, -0.16076034570528946, -0.2639888627652792, 0.06335609612065031, -0.3021406555013295, -0.08459021629607107, 0.10029664071910876, -0.008775949943810701,... |
706.2254 | Dynamics of cluster deposition on Ar surface | Using a combined quantum mechanical/classical method, we study the dynamics
of deposition of small Na clusters on Ar(001) surface. We work out basic
mechanisms by systematic variation of substrate activity, impact energy,
cluster orientations, cluster sizes, and charges. The soft Ar material is found
to serve as an e... | cond-mat.other | using a combined quantum mechanicalclassical method we study the dynamics of deposition of small na clusters on ar001 surface we work out basic mechanisms by systematic variation of substrate activity impact energy cluster orientations cluster sizes and charges the soft ar material is found to serve as an extremely eff... | [['using', 'a', 'combined', 'quantum', 'mechanicalclassical', 'method', 'we', 'study', 'the', 'dynamics', 'of', 'deposition', 'of', 'small', 'na', 'clusters', 'on', 'ar001', 'surface', 'we', 'work', 'out', 'basic', 'mechanisms', 'by', 'systematic', 'variation', 'of', 'substrate', 'activity', 'impact', 'energy', 'cluste... | [-0.08842442418378121, 0.171952977360978, -0.08871607488008137, 0.04588598960889241, -0.01794408645782567, -0.1140990554302616, 0.05146113645390306, 0.4154481704438656, -0.24618694302298025, -0.35034998224287384, 0.0046562654315494, -0.2599678652682407, -0.03180847299927977, 0.18440631257278295, 0.04163112455624825, -0... |
706.2255 | The magnetic field topology in the reconnecting pulsar magnetosphere | We show that toroidal magnetic field annihilation in the equatorial current
sheet of the pulsar magnetosphere is related to how fast poloidal magnetic
field lines close as we move away from the light cylinder. This determines the
reconnection radial electric field which directly accelerates particles in the
neutral l... | astro-ph | we show that toroidal magnetic field annihilation in the equatorial current sheet of the pulsar magnetosphere is related to how fast poloidal magnetic field lines close as we move away from the light cylinder this determines the reconnection radial electric field which directly accelerates particles in the neutral laye... | [['we', 'show', 'that', 'toroidal', 'magnetic', 'field', 'annihilation', 'in', 'the', 'equatorial', 'current', 'sheet', 'of', 'the', 'pulsar', 'magnetosphere', 'is', 'related', 'to', 'how', 'fast', 'poloidal', 'magnetic', 'field', 'lines', 'close', 'as', 'we', 'move', 'away', 'from', 'the', 'light', 'cylinder', 'this',... | [-0.142976057632283, 0.2505840830815335, 0.01660700181746506, 0.08457855134038254, -0.10919981630092176, -0.045998068836828075, 0.024518197875780363, 0.38617825613667567, -0.27450096582372985, -0.31181594137257584, 0.015104328472322475, -0.22304488273027043, -0.011289790164058407, 0.21992913528423136, -0.01942754712654... |
706.2256 | High-resolution FUSE and HST ultraviolet spectroscopy of the white dwarf
central star of Sh 2-216 | LS V +4621 is the DAO-type central star of the planetary nebula Sh 2-216. We
perform a comprehensive spectral analysis of high-resolution, high-S/N
ultraviolet observations obtained with FUSE and STIS aboard the HST as well as
the optical spectrum of LS V +4621 by means of state-of-the-art NLTE
model-atmosphere techn... | astro-ph | ls v 4621 is the daotype central star of the planetary nebula sh 2216 we perform a comprehensive spectral analysis of highresolution highsn ultraviolet observations obtained with fuse and stis aboard the hst as well as the optical spectrum of ls v 4621 by means of stateoftheart nlte modelatmosphere techniques in order ... | [['ls', 'v', '4621', 'is', 'the', 'daotype', 'central', 'star', 'of', 'the', 'planetary', 'nebula', 'sh', '2216', 'we', 'perform', 'a', 'comprehensive', 'spectral', 'analysis', 'of', 'highresolution', 'highsn', 'ultraviolet', 'observations', 'obtained', 'with', 'fuse', 'and', 'stis', 'aboard', 'the', 'hst', 'as', 'well... | [-0.012070741513114979, 0.057391108156509524, 0.02011558250899637, 0.0493601426283168, -0.022751465787164745, -0.15677751538506499, 0.08503692515190661, 0.43418617269414805, -0.19593097639059828, -0.3719932526995939, 0.016641277980412386, -0.3298558102180851, -0.0071001385879372395, 0.13981932465873298, -0.019111042641... |
706.2257 | Algebraic K-theory and cubical descent | In this note we apply Guillen-Navarro descent theorem, \cite{GN02}, to define
a descent variant of the algebraic $K$-theory of varieties over a field of
characteristic zero, $\mathcal{KD}(X)$, which coincides with $\mathcal{K}(X)$
for smooth varieties. After a result of Haesemeyer, this new theory is
equivalent to th... | math.AG | in this note we apply guillennavarro descent theorem citegn02 to define a descent variant of the algebraic ktheory of varieties over a field of characteristic zero mathcalkdx which coincides with mathcalkx for smooth varieties after a result of haesemeyer this new theory is equivalent to the homotopy algebraic ktheory ... | [['in', 'this', 'note', 'we', 'apply', 'guillennavarro', 'descent', 'theorem', 'citegn02', 'to', 'define', 'a', 'descent', 'variant', 'of', 'the', 'algebraic', 'ktheory', 'of', 'varieties', 'over', 'a', 'field', 'of', 'characteristic', 'zero', 'mathcalkdx', 'which', 'coincides', 'with', 'mathcalkx', 'for', 'smooth', 'v... | [-0.16768513118938333, 0.05304438467588155, -0.1796437112638922, 0.10373636217968117, -0.07497940768277453, -0.14109822320601634, -0.007623490210877912, 0.3145212589672977, -0.3858379130702346, -0.15227648638369096, 0.06613827620505265, -0.15896900351377083, -0.18408996796595953, 0.22920648315020145, -0.249174966627070... |
706.2258 | Growth mechanisms and structure of fullerene-like carbon-based thin
films: superelastic materials for tribological applications | In this chapter we review our findings on the bonding structure and growth
mechanisms of carbon-based thin solid films with fullerene-like (FL)
microstructure. The so-called FL arrangements arise from the curvature and
cross-linking of basal planes in graphitic-like structures, partially
resembling that of molecular ... | cond-mat.mtrl-sci | in this chapter we review our findings on the bonding structure and growth mechanisms of carbonbased thin solid films with fullerenelike fl microstructure the socalled fl arrangements arise from the curvature and crosslinking of basal planes in graphiticlike structures partially resembling that of molecular fullerenes ... | [['in', 'this', 'chapter', 'we', 'review', 'our', 'findings', 'on', 'the', 'bonding', 'structure', 'and', 'growth', 'mechanisms', 'of', 'carbonbased', 'thin', 'solid', 'films', 'with', 'fullerenelike', 'fl', 'microstructure', 'the', 'socalled', 'fl', 'arrangements', 'arise', 'from', 'the', 'curvature', 'and', 'crosslin... | [-0.12386469691360401, 0.1692084869345858, -0.020003378299185953, -0.030564487038645893, -0.03448547704255808, -0.12598310483851086, 0.04650530730779309, 0.44353030358130735, -0.2934927184892408, -0.28191343625470744, 0.07198588683409353, -0.2705341495236771, -0.18687773160478574, 0.14224015944111187, -0.01739241990213... |
706.2259 | Non-equilibrium coherence dynamics in one-dimensional Bose gases | Low-dimensional systems are beautiful examples of many-body quantum physics.
For one-dimensional systems the Luttinger liquid approach provides insight into
universal properties. Much is known of the equilibrium state, both in the
weakly and strongly interacting regime. However, it remains a challenge to
probe the dy... | cond-mat.other cond-mat.supr-con | lowdimensional systems are beautiful examples of manybody quantum physics for onedimensional systems the luttinger liquid approach provides insight into universal properties much is known of the equilibrium state both in the weakly and strongly interacting regime however it remains a challenge to probe the dynamics by ... | [['lowdimensional', 'systems', 'are', 'beautiful', 'examples', 'of', 'manybody', 'quantum', 'physics', 'for', 'onedimensional', 'systems', 'the', 'luttinger', 'liquid', 'approach', 'provides', 'insight', 'into', 'universal', 'properties', 'much', 'is', 'known', 'of', 'the', 'equilibrium', 'state', 'both', 'in', 'the', ... | [-0.16083990643647583, 0.22408816438778145, -0.09410077618985352, 0.05389924765596251, 0.023999953638254242, -0.18018993045923046, 0.01962417391583916, 0.33343826548027045, -0.22707767840898171, -0.26751454848880796, 0.02247891723474657, -0.2741917876145718, -0.13254646453688937, 0.20040483742275023, 0.0331112283070317... |
706.226 | Quantum charge diffusion in underdamped Josephson junctions and
superconducting nanowires | The effect of quantum fluctuations on the current-voltage characteristics of
Josephson junctions and superconducting nanowires is studied in the underdamped
limit. Quantum fluctuations induce transitions between a Coulomb--blockade and
a supercurrent branch, and can significantly modify the shape of
current-voltage c... | cond-mat.mes-hall cond-mat.supr-con | the effect of quantum fluctuations on the currentvoltage characteristics of josephson junctions and superconducting nanowires is studied in the underdamped limit quantum fluctuations induce transitions between a coulombblockade and a supercurrent branch and can significantly modify the shape of currentvoltage character... | [['the', 'effect', 'of', 'quantum', 'fluctuations', 'on', 'the', 'currentvoltage', 'characteristics', 'of', 'josephson', 'junctions', 'and', 'superconducting', 'nanowires', 'is', 'studied', 'in', 'the', 'underdamped', 'limit', 'quantum', 'fluctuations', 'induce', 'transitions', 'between', 'a', 'coulombblockade', 'and',... | [-0.20478414344386411, 0.17545923986830392, -0.11735906772888624, 0.04512464336047952, -0.02902918099783934, -0.1532273543640398, 0.06694374269304368, 0.3313859686255455, -0.22475400638963597, -0.2622096140940602, -0.019246486230538443, -0.28674196992069484, -0.14814447640226439, 0.23137070725743586, -0.028776524101312... |
706.2261 | Uniqueness of $\bf C^*$- and $\bf C_+$-actions on Gizatullin surfaces | A Gizatullin surface is a normal affine surface $V$ over $\bf C$, which can
be completed by a zigzag; that is, by a linear chain of smooth rational curves.
In this paper we deal with the question of uniqueness of $\bf C^*$-actions and
$\bf A^1$-fibrations on such a surface $V$ up to automorphisms. The latter
fibratio... | math.AG | a gizatullin surface is a normal affine surface v over bf c which can be completed by a zigzag that is by a linear chain of smooth rational curves in this paper we deal with the question of uniqueness of bf cactions and bf a1fibrations on such a surface v up to automorphisms the latter fibrations are in one to one corr... | [['a', 'gizatullin', 'surface', 'is', 'a', 'normal', 'affine', 'surface', 'v', 'over', 'bf', 'c', 'which', 'can', 'be', 'completed', 'by', 'a', 'zigzag', 'that', 'is', 'by', 'a', 'linear', 'chain', 'of', 'smooth', 'rational', 'curves', 'in', 'this', 'paper', 'we', 'deal', 'with', 'the', 'question', 'of', 'uniqueness', ... | [-0.18741327560715507, 0.0810744209565169, -0.020291692094768474, -0.01201712791175694, -0.07934654741984559, -0.1763157224451224, 0.017400136011740962, 0.3852000302426389, -0.30300765822928577, -0.2342652789485673, 0.077138032712512, -0.26352372332797225, -0.1387388715364946, 0.21447159959493076, -0.12194881697610856,... |
706.2262 | Adjoints and Formal Adjoints of Matrices of Unbounded Operators | In this paper we {\em discuss} diverse aspects of mutual relationship between
adjoints and formal adjoints of unbounded operators bearing a matrix structure.
We emphasize on the behaviour of row and column operators as they turn out to
be the germs of an arbitrary matrix operator, providing most of the information
ab... | math.FA math-ph math.MP | in this paper we em discuss diverse aspects of mutual relationship between adjoints and formal adjoints of unbounded operators bearing a matrix structure we emphasize on the behaviour of row and column operators as they turn out to be the germs of an arbitrary matrix operator providing most of the information about the... | [['in', 'this', 'paper', 'we', 'em', 'discuss', 'diverse', 'aspects', 'of', 'mutual', 'relationship', 'between', 'adjoints', 'and', 'formal', 'adjoints', 'of', 'unbounded', 'operators', 'bearing', 'a', 'matrix', 'structure', 'we', 'emphasize', 'on', 'the', 'behaviour', 'of', 'row', 'and', 'column', 'operators', 'as', '... | [-0.14053239250334643, 0.08051842279654288, -0.06504745086284071, 0.0825666888474913, -0.09208137449666352, -0.08392245637379207, 0.036760000024638056, 0.3836924888319888, -0.32053709053237117, -0.22524206734941168, 0.1546113967354867, -0.30155495961859696, -0.18560183388417809, 0.09676183188744521, -0.0702800295647170... |
706.2263 | Phase rigidity breaking in open Aharonov-Bohm ring coupled to a
cantilever | The conductance and the transmittance phase shifts of a two-terminal
Aharonov-Bohm (AB) ring are analyzed in the presence of mechanical
displacements due to coupling to an external can- tilever. We show that phase
rigidity is broken, even in the linear response regime, by means of inelastic
scattering due to phonons.... | cond-mat.mes-hall | the conductance and the transmittance phase shifts of a twoterminal aharonovbohm ab ring are analyzed in the presence of mechanical displacements due to coupling to an external can tilever we show that phase rigidity is broken even in the linear response regime by means of inelastic scattering due to phonons our device... | [['the', 'conductance', 'and', 'the', 'transmittance', 'phase', 'shifts', 'of', 'a', 'twoterminal', 'aharonovbohm', 'ab', 'ring', 'are', 'analyzed', 'in', 'the', 'presence', 'of', 'mechanical', 'displacements', 'due', 'to', 'coupling', 'to', 'an', 'external', 'can', 'tilever', 'we', 'show', 'that', 'phase', 'rigidity',... | [-0.2540714616602186, 0.1832425544233212, -0.0677411835746501, -0.051287627745874816, -0.039505918520841406, -0.13697265581735832, 0.08630292770579796, 0.39948811822316865, -0.31210344725034456, -0.25512051027776167, 0.001553169918638146, -0.2809007441709665, -0.20450315909957598, 0.19266543480758133, -0.02336104339073... |
706.2264 | Hard QCD probes to quark-gluon plasma | Completely unexplored regimes of QCD, dominated by high-density/temperature
effects, are available in heavy ion experiments at collider energies. The
successful RHIC program shows how relevant the high transverse momentum part of
the spectrum is for the characterization of the properties of the created
medium. It poi... | hep-ph | completely unexplored regimes of qcd dominated by highdensitytemperature effects are available in heavy ion experiments at collider energies the successful rhic program shows how relevant the high transverse momentum part of the spectrum is for the characterization of the properties of the created medium it points as w... | [['completely', 'unexplored', 'regimes', 'of', 'qcd', 'dominated', 'by', 'highdensitytemperature', 'effects', 'are', 'available', 'in', 'heavy', 'ion', 'experiments', 'at', 'collider', 'energies', 'the', 'successful', 'rhic', 'program', 'shows', 'how', 'relevant', 'the', 'high', 'transverse', 'momentum', 'part', 'of', ... | [-0.08678397521310087, 0.2331099157319321, -0.0910121647383286, 0.10196959299355512, -0.015037949997349642, -0.0785559842562569, -0.01578176897809109, 0.35129301100304083, -0.252057377764556, -0.2937925466586811, 0.07443314702270852, -0.3096455752965994, 0.028714909234882464, 0.18753892881795764, 0.050126112556816746, ... |
706.2265 | Vicinal silicon surfaces: from step density wave to faceting | This paper investigates faceting mechanisms induced by electromigration in
the regime where atomic steps are transparent. For this purpose we study
several vicinal orientations by means of in-situ (optical diffraction,
electronic microscopy) as well as ex-situ (AFM, microprofilometry)
visualization techniques. The da... | cond-mat.mtrl-sci | this paper investigates faceting mechanisms induced by electromigration in the regime where atomic steps are transparent for this purpose we study several vicinal orientations by means of insitu optical diffraction electronic microscopy as well as exsitu afm microprofilometry visualization techniques the data show that... | [['this', 'paper', 'investigates', 'faceting', 'mechanisms', 'induced', 'by', 'electromigration', 'in', 'the', 'regime', 'where', 'atomic', 'steps', 'are', 'transparent', 'for', 'this', 'purpose', 'we', 'study', 'several', 'vicinal', 'orientations', 'by', 'means', 'of', 'insitu', 'optical', 'diffraction', 'electronic',... | [-0.12817603090201074, 0.1639980169520065, -0.11574165794696697, 0.008492514000368552, -0.0647330710552397, -0.0754906823633893, 0.0358649288688026, 0.40191125152396817, -0.28317714251483544, -0.30106673784380117, 0.057712262624556414, -0.22109283551668066, -0.1526189275090347, 0.17145011457909323, 0.005202896674929918... |
706.2266 | The role of the slope of `realistic' potential barriers in preventing
relativistic tunnelling in the Klein zone | The transmission of fermions of mass m and energy E through an electrostatic
potential barrier of rectangular shape (i.e. supporting an infinite electric
field), of height U> E + m - due to the many-body nature of the Dirac equation
evidentiated by the Klein paradox - has been widely studied. We exploit here
the anal... | quant-ph | the transmission of fermions of mass m and energy e through an electrostatic potential barrier of rectangular shape ie supporting an infinite electric field of height u e m due to the manybody nature of the dirac equation evidentiated by the klein paradox has been widely studied we exploit here the analytical solution ... | [['the', 'transmission', 'of', 'fermions', 'of', 'mass', 'm', 'and', 'energy', 'e', 'through', 'an', 'electrostatic', 'potential', 'barrier', 'of', 'rectangular', 'shape', 'ie', 'supporting', 'an', 'infinite', 'electric', 'field', 'of', 'height', 'u', 'e', 'm', 'due', 'to', 'the', 'manybody', 'nature', 'of', 'the', 'di... | [-0.15021699957246454, 0.16442771489047753, -0.03849890586296272, 0.0654222501039874, -0.041317683165752385, -0.1444184250233449, 0.04454100812029726, 0.34637539717808086, -0.25350986065162906, -0.2962235213600029, 0.03647384128230185, -0.2760010422031694, -0.09489440589589682, 0.2139923166723061, 0.008840608859724665,... |
706.2267 | A Review of Recent Results from the Tevatron | The D0 and CDF experiments have been taking data at the Run 2 of the Tevatron
Collider since 2001. We present a selection of recent results, most of them
obtained with an integrated luminosity of $\simeq$ 1 fb$^{-1}$. I will describe
the most important facets of the physics programme and detail some results.
Recent d... | hep-ex | the d0 and cdf experiments have been taking data at the run 2 of the tevatron collider since 2001 we present a selection of recent results most of them obtained with an integrated luminosity of simeq 1 fb1 i will describe the most important facets of the physics programme and detail some results recent direct limits on... | [['the', 'd0', 'and', 'cdf', 'experiments', 'have', 'been', 'taking', 'data', 'at', 'the', 'run', '2', 'of', 'the', 'tevatron', 'collider', 'since', '2001', 'we', 'present', 'a', 'selection', 'of', 'recent', 'results', 'most', 'of', 'them', 'obtained', 'with', 'an', 'integrated', 'luminosity', 'of', 'simeq', '1', 'fb1'... | [-0.011594767307138277, 0.09603127195785216, -0.08227900423419972, 0.06860176034064756, -0.07814085258481403, -0.12004690682644853, -0.006088768646198635, 0.36959167880316574, -0.18712895956964026, -0.3113695371947769, 0.12620999506907538, -0.3516956658180182, -0.014089413646919033, 0.2403086907611901, 0.04527537130181... |
706.2268 | Gelfand-Shilov spaces, Structural and Kernel theorems | It was shown recently that the space isomorphic with an Gelfand Shilov space
is well adapted for the use in quantum field theory with a fundamental length.
It is our believe that all Gelfand Shilov spaces, especially those with
quasianalytic test function spaces, are good domains for the quantum field
theory. The the... | quant-ph math.FA | it was shown recently that the space isomorphic with an gelfand shilov space is well adapted for the use in quantum field theory with a fundamental length it is our believe that all gelfand shilov spaces especially those with quasianalytic test function spaces are good domains for the quantum field theory the theory re... | [['it', 'was', 'shown', 'recently', 'that', 'the', 'space', 'isomorphic', 'with', 'an', 'gelfand', 'shilov', 'space', 'is', 'well', 'adapted', 'for', 'the', 'use', 'in', 'quantum', 'field', 'theory', 'with', 'a', 'fundamental', 'length', 'it', 'is', 'our', 'believe', 'that', 'all', 'gelfand', 'shilov', 'spaces', 'espec... | [-0.0380662546347882, 0.06822738716379384, -0.13492344929329533, 0.17585495289583405, -0.11237076743469011, -0.09783811430622003, -0.02357113293929966, 0.3623338146965102, -0.3146407513851576, -0.1978903121434816, 0.12246679955641601, -0.22966909453752313, -0.21375107208248412, 0.24834507534114442, -0.13629285175131983... |
706.2269 | Topological objects in QCD | Topological excitations are prominent candidates for explaining
nonperturbative effects in QCD like confinement. In these lectures, I cover
both formal treatments and applications of topological objects. The typical
phenomena like BPS bounds, topology, the semiclassical approximation and chiral
fermions are introduce... | hep-th hep-lat hep-ph | topological excitations are prominent candidates for explaining nonperturbative effects in qcd like confinement in these lectures i cover both formal treatments and applications of topological objects the typical phenomena like bps bounds topology the semiclassical approximation and chiral fermions are introduced by vi... | [['topological', 'excitations', 'are', 'prominent', 'candidates', 'for', 'explaining', 'nonperturbative', 'effects', 'in', 'qcd', 'like', 'confinement', 'in', 'these', 'lectures', 'i', 'cover', 'both', 'formal', 'treatments', 'and', 'applications', 'of', 'topological', 'objects', 'the', 'typical', 'phenomena', 'like', ... | [-0.10953921593300263, 0.21113909993850322, -0.049891885887417525, 0.14783143996186324, -0.0932292406918642, -0.1414545769429547, 0.00045683848338178647, 0.36358963249734155, -0.1312591027882364, -0.28819317610957373, 0.11040097177977225, -0.3064575173150472, -0.1867237725916008, 0.17697284445396544, -0.056653624653448... |
706.227 | Kaon production from 1 to 40 A GeV | Kaon production is studied within the Giessen Boltzmann-Uehling-Uhlenbeck
(GiBUU) model. Results are compared with experiment and with other models. The
influence of the kaon potential on the kaon azimuthal distributions at SIS
energies is considered. We also discuss the role of the many-body collisions at
high-densi... | nucl-th | kaon production is studied within the giessen boltzmannuehlinguhlenbeck gibuu model results are compared with experiment and with other models the influence of the kaon potential on the kaon azimuthal distributions at sis energies is considered we also discuss the role of the manybody collisions at highdensity phase of... | [['kaon', 'production', 'is', 'studied', 'within', 'the', 'giessen', 'boltzmannuehlinguhlenbeck', 'gibuu', 'model', 'results', 'are', 'compared', 'with', 'experiment', 'and', 'with', 'other', 'models', 'the', 'influence', 'of', 'the', 'kaon', 'potential', 'on', 'the', 'kaon', 'azimuthal', 'distributions', 'at', 'sis', ... | [-0.01577207859966676, 0.21691741258837283, -0.1103234793474109, 0.1196766933853909, 0.06325423791624453, -0.11469004812593363, -0.04124894329555789, 0.3384475790876515, -0.13870226195538227, -0.2355165665170976, -0.062028424443715084, -0.3903229234512059, 0.005456850616907587, 0.141213790983988, 0.13513750591961554, 0... |
706.2271 | Double quantum dot with integrated charge sensor based on Ge/Si
heterostructure nanowires | Coupled electron spins in semiconductor double quantum dots hold promise as
the basis for solid-state qubits. To date, most experiments have used III-V
materials, in which coherence is limited by hyperfine interactions. Ge/Si
heterostructure nanowires seem ideally suited to overcome this limitation: the
predominance ... | cond-mat.mes-hall cond-mat.mtrl-sci | coupled electron spins in semiconductor double quantum dots hold promise as the basis for solidstate qubits to date most experiments have used iiiv materials in which coherence is limited by hyperfine interactions gesi heterostructure nanowires seem ideally suited to overcome this limitation the predominance of spinzer... | [['coupled', 'electron', 'spins', 'in', 'semiconductor', 'double', 'quantum', 'dots', 'hold', 'promise', 'as', 'the', 'basis', 'for', 'solidstate', 'qubits', 'to', 'date', 'most', 'experiments', 'have', 'used', 'iiiv', 'materials', 'in', 'which', 'coherence', 'is', 'limited', 'by', 'hyperfine', 'interactions', 'gesi', ... | [-0.13479513104952184, 0.1901316683302247, 0.04495971664540298, -0.021147546797647333, 0.018399967909427294, -0.2864917923650103, 0.04091711185545601, 0.4498371059233521, -0.23975115007611902, -0.29720907705565186, -0.04670764463260136, -0.28549635763683007, -0.09669391470399837, 0.2438958209034399, 0.01975572087095244... |
706.2272 | Expanders and the Affine Building of ${\rm Sp}_n$ | For $n \geq 2$ and a local field $K$, let $\Delta_n$ denote the affine
building naturally associated to the symplectic group ${\rm Sp}_n(K)$. We
compute the spectral radius of the subgraph $Y_n$ of $\Delta_n$ induced by the
special vertices in $\Delta_n$, from which it follows that $Y_n$ is an analogue
of a family of... | math.CO | for n geq 2 and a local field k let delta_n denote the affine building naturally associated to the symplectic group rm sp_nk we compute the spectral radius of the subgraph y_n of delta_n induced by the special vertices in delta_n from which it follows that y_n is an analogue of a family of expanders and is nonamenable | [['for', 'n', 'geq', '2', 'and', 'a', 'local', 'field', 'k', 'let', 'delta_n', 'denote', 'the', 'affine', 'building', 'naturally', 'associated', 'to', 'the', 'symplectic', 'group', 'rm', 'sp_nk', 'we', 'compute', 'the', 'spectral', 'radius', 'of', 'the', 'subgraph', 'y_n', 'of', 'delta_n', 'induced', 'by', 'the', 'spec... | [-0.20070057894969195, 0.17723402551915537, -0.05089261925272774, -0.011924424057564977, -0.06305760174597565, -0.10964147826624021, -0.014057275577726071, 0.3360578371252734, -0.3492443509269179, -0.22189415138410895, 0.07866252583590451, -0.33193789099408477, -0.11710312546296209, 0.13879293182113192, -0.098404728497... |
706.2273 | Evolution of Anisotropy of Parton System from Relativistic Heavy-Ion
Collisions | Evolution of anisotropy in momentum and coordinate space of the parton system
produced in relativistic heavy-ion collisions is discussed within the
free-streaming approximation. The momentum distribution evolves from the
prolate shape - elongated along the beam - to the oblate one - squeezed along
the beam. At the sa... | nucl-th hep-ph | evolution of anisotropy in momentum and coordinate space of the parton system produced in relativistic heavyion collisions is discussed within the freestreaming approximation the momentum distribution evolves from the prolate shape elongated along the beam to the oblate one squeezed along the beam at the same time the ... | [['evolution', 'of', 'anisotropy', 'in', 'momentum', 'and', 'coordinate', 'space', 'of', 'the', 'parton', 'system', 'produced', 'in', 'relativistic', 'heavyion', 'collisions', 'is', 'discussed', 'within', 'the', 'freestreaming', 'approximation', 'the', 'momentum', 'distribution', 'evolves', 'from', 'the', 'prolate', 's... | [-0.14913876522096653, 0.2505259906189351, -0.18594638984414597, 0.09200587068519354, -0.0036194014917068844, -0.042044591329567414, -0.08084999327842571, 0.37806010019930103, -0.2695026915473274, -0.23599994062339957, -0.035207312929891994, -0.2762614960628974, 0.07294166964019023, 0.10358641606673033, 0.0628914609168... |
706.2274 | Consistent reasoning about a continuum of hypotheses on the basis of
finite evidence | In the modern Bayesian view classical probability theory is simply an
extension of conventional logic, i.e., a quantitative tool that allows for
consistent reasoning in the presence of uncertainty. Classical theory
presupposes, however, that--at least in principle--the amount of evidence that
an experimenter can accu... | quant-ph math.ST stat.TH | in the modern bayesian view classical probability theory is simply an extension of conventional logic ie a quantitative tool that allows for consistent reasoning in the presence of uncertainty classical theory presupposes however thatat least in principlethe amount of evidence that an experimenter can accumulate always... | [['in', 'the', 'modern', 'bayesian', 'view', 'classical', 'probability', 'theory', 'is', 'simply', 'an', 'extension', 'of', 'conventional', 'logic', 'ie', 'a', 'quantitative', 'tool', 'that', 'allows', 'for', 'consistent', 'reasoning', 'in', 'the', 'presence', 'of', 'uncertainty', 'classical', 'theory', 'presupposes', ... | [-0.08186848175772016, 0.11770485825639504, -0.12874866970401677, 0.12296265479470153, -0.10170451345883551, -0.13368731321947228, 0.06512281768354437, 0.3400759479751991, -0.2538372390032295, -0.30005631644519104, 0.09370753012011729, -0.21631005149674526, -0.11875869351168794, 0.1842138516626531, -0.09346379243333133... |
706.2275 | A dust component 2 kpc above the plane in NGC 891 | The halo of NGC 891 has been the subject of studies for more than a decade.
One of its most striking features is the large asymmetry in H$\alpha$ emission.
In this letter, we will take a quantitative look at this asymmetry at different
wavelengths for the first time. We suggest that NGC 891 is intrinsically almost
sy... | astro-ph | the halo of ngc 891 has been the subject of studies for more than a decade one of its most striking features is the large asymmetry in halpha emission in this letter we will take a quantitative look at this asymmetry at different wavelengths for the first time we suggest that ngc 891 is intrinsically almost symmetric a... | [['the', 'halo', 'of', 'ngc', '891', 'has', 'been', 'the', 'subject', 'of', 'studies', 'for', 'more', 'than', 'a', 'decade', 'one', 'of', 'its', 'most', 'striking', 'features', 'is', 'the', 'large', 'asymmetry', 'in', 'halpha', 'emission', 'in', 'this', 'letter', 'we', 'will', 'take', 'a', 'quantitative', 'look', 'at',... | [-0.08025665164342431, 0.08025847860305003, -0.06659602114733038, 0.0876370910802263, -0.056993607667082266, -0.0619005579176208, -0.022405001957895618, 0.42856774502043615, -0.20558675095327095, -0.32287758624528445, 0.06682037576635019, -0.3007975271915986, -0.02762392027480476, 0.15626333113733742, -0.03604892060432... |
706.2276 | Heavy Flavor Production in DGLAP improved Saturation Model | The saturation model with DGLAP evolution is shown to give good description
of the production of the charm and beauty quarks in deep inelastic scattering.
The modifications of saturation properties caused by the presence of heavy
quarks are also discussed.
| hep-ph | the saturation model with dglap evolution is shown to give good description of the production of the charm and beauty quarks in deep inelastic scattering the modifications of saturation properties caused by the presence of heavy quarks are also discussed | [['the', 'saturation', 'model', 'with', 'dglap', 'evolution', 'is', 'shown', 'to', 'give', 'good', 'description', 'of', 'the', 'production', 'of', 'the', 'charm', 'and', 'beauty', 'quarks', 'in', 'deep', 'inelastic', 'scattering', 'the', 'modifications', 'of', 'saturation', 'properties', 'caused', 'by', 'the', 'presenc... | [-0.024523406327352858, 0.23677388806827365, -0.13498183561023325, 0.17111443527101072, -0.023366130096837877, -0.06574088698253036, -0.013441246328875422, 0.3148747205734253, -0.2495897708577104, -0.25926676727831366, -0.03041057949012611, -0.34479133908171206, -0.0195773143786937, 0.0773510798404459, 0.03400851681362... |
706.2277 | Narrow bandwidth interference filter-stabilized diode laser systems for
the manipulation of neutral atoms | We present and investigate different external cavity diode laser (ECDL)
configurations for the manipulation of neutrals atoms, wavelength-stabilized by
a narrow-band high transmission interference filter. A novel diode laser,
providing high output power of more than 1 W, with a linewidth of less than 200
kHz, based o... | physics.atom-ph physics.optics | we present and investigate different external cavity diode laser ecdl configurations for the manipulation of neutrals atoms wavelengthstabilized by a narrowband high transmission interference filter a novel diode laser providing high output power of more than 1 w with a linewidth of less than 200 khz based on a selfsee... | [['we', 'present', 'and', 'investigate', 'different', 'external', 'cavity', 'diode', 'laser', 'ecdl', 'configurations', 'for', 'the', 'manipulation', 'of', 'neutrals', 'atoms', 'wavelengthstabilized', 'by', 'a', 'narrowband', 'high', 'transmission', 'interference', 'filter', 'a', 'novel', 'diode', 'laser', 'providing',... | [-0.12783626021888678, 0.12467816020392591, -0.059253326773027616, -0.054470744712988, -0.018067356165228112, -0.2736668430321339, 0.052433587670806914, 0.5304527104261422, -0.16372686914250917, -0.30058074266567164, 0.057449441059537594, -0.25227982395388665, -0.03380518640962339, 0.31749932775874773, -0.0634923736009... |
706.2278 | MOST photometry and DDO spectroscopy of the eclipsing (white dwarf + red
dwarf) binary V471 Tau | The Hyades K2V+WD system 471 Tau is a prototype post-common envelope system
and a likely cataclysmic binary progenitor. We present 10 days of nearly
continuous optical photometry by the MOST (Microvariability & Oscillations of
STars) satellite and partly simultaneous optical spectroscopy from DDO (David
Dunlap Observ... | astro-ph | the hyades k2vwd system 471 tau is a prototype postcommon envelope system and a likely cataclysmic binary progenitor we present 10 days of nearly continuous optical photometry by the most microvariability oscillations of stars satellite and partly simultaneous optical spectroscopy from ddo david dunlap observatory of t... | [['the', 'hyades', 'k2vwd', 'system', '471', 'tau', 'is', 'a', 'prototype', 'postcommon', 'envelope', 'system', 'and', 'a', 'likely', 'cataclysmic', 'binary', 'progenitor', 'we', 'present', '10', 'days', 'of', 'nearly', 'continuous', 'optical', 'photometry', 'by', 'the', 'most', 'microvariability', 'oscillations', 'of'... | [-0.1424902632444476, 0.14193215676696128, -0.06884819283053124, 0.05192952793101237, -0.06893672842124943, -0.08878480766240197, 0.07477288736166278, 0.4167080740163025, -0.18132146202309135, -0.3515675664956992, 0.09096278271026677, -0.30771671937157713, -0.05900058872939553, 0.2306476948710042, -0.06514661927164221,... |
706.2279 | Efficient analysis and design of low-loss whispering-gallery-mode
coupled resonator optical waveguide bends | Waveguides composed of electromagnetically-coupled optical microcavities
(coupled resonator optical waveguides or CROWs) can be used for light guiding,
slowing and storage. In this paper, we present a two-dimensional analysis of
finite-size straight and curved CROW sections based on a rigorous Muller
boundary integra... | physics.optics | waveguides composed of electromagneticallycoupled optical microcavities coupled resonator optical waveguides or crows can be used for light guiding slowing and storage in this paper we present a twodimensional analysis of finitesize straight and curved crow sections based on a rigorous muller boundary integral equation... | [['waveguides', 'composed', 'of', 'electromagneticallycoupled', 'optical', 'microcavities', 'coupled', 'resonator', 'optical', 'waveguides', 'or', 'crows', 'can', 'be', 'used', 'for', 'light', 'guiding', 'slowing', 'and', 'storage', 'in', 'this', 'paper', 'we', 'present', 'a', 'twodimensional', 'analysis', 'of', 'finit... | [-0.1849928346272834, 0.14877744720627864, -0.0334064906704481, -0.08543584384972712, -0.09866529191947646, -0.20598132810382933, 0.026445159970575737, 0.46897404978258744, -0.19535222254969456, -0.2760721133418243, 0.028271208940660236, -0.3085658111712999, -0.13025238396496408, 0.20464131066886088, -0.018085749594805... |
706.228 | Longitudinal impedance and wake from XFEL undulators. Impact on
current-enhanced SASE schemes | In this article we derive longitudinal impedance and wake function for an
undulator setup with arbitrary undulator parameter, taking into account a
finite transverse size of the electron bunch. Earlier studies considered a line
density-distribution of electrons instead. We focus our attention on the
long-wavelength a... | physics.acc-ph physics.optics | in this article we derive longitudinal impedance and wake function for an undulator setup with arbitrary undulator parameter taking into account a finite transverse size of the electron bunch earlier studies considered a line densitydistribution of electrons instead we focus our attention on the longwavelength asymptot... | [['in', 'this', 'article', 'we', 'derive', 'longitudinal', 'impedance', 'and', 'wake', 'function', 'for', 'an', 'undulator', 'setup', 'with', 'arbitrary', 'undulator', 'parameter', 'taking', 'into', 'account', 'a', 'finite', 'transverse', 'size', 'of', 'the', 'electron', 'bunch', 'earlier', 'studies', 'considered', 'a'... | [-0.09320022125918369, 0.11113605410807251, -0.07664126746086894, 0.057105804457770366, -0.044277850915616576, -0.1331481692258661, -0.010661155947998754, 0.41552659206484494, -0.1797562492496677, -0.26086337584803054, 0.06099736025131087, -0.23773770813323178, -0.04980823204509522, 0.271781388364769, -0.04386073290140... |
706.2281 | Some questions of Monte-Carlo modeling on nontrivial bundles | In this work are considered some questions of Monte-Carlo modeling on
nontrivial bundles. As a basic example is used problem of generation of
straight lines in 3D space, related with modeling of interaction of a solid
body with a flux of particles and with some other tasks. Space of lines used in
given model is examp... | math-ph math.MP stat.CO | in this work are considered some questions of montecarlo modeling on nontrivial bundles as a basic example is used problem of generation of straight lines in 3d space related with modeling of interaction of a solid body with a flux of particles and with some other tasks space of lines used in given model is example of ... | [['in', 'this', 'work', 'are', 'considered', 'some', 'questions', 'of', 'montecarlo', 'modeling', 'on', 'nontrivial', 'bundles', 'as', 'a', 'basic', 'example', 'is', 'used', 'problem', 'of', 'generation', 'of', 'straight', 'lines', 'in', '3d', 'space', 'related', 'with', 'modeling', 'of', 'interaction', 'of', 'a', 'sol... | [-0.1409939273085067, 0.06413178462653245, -0.027834008677282196, 0.0199040119111052, -0.0791310299984247, -0.15534540225306284, -0.01963960751891136, 0.41690909776134766, -0.23455039463748317, -0.26958724014811974, 0.10567444436204876, -0.25885070620131667, -0.1543757690022281, 0.22804932676566145, -0.0787853986510764... |
706.2282 | Partition Identities and the Coin Exchange Problem | The number of partitions of n into parts divisible by a or b equals the
number of partitions of n in which each part and each difference of two parts
is expressible as a non-negative integer combination of a or b. This
generalizes identities of MacMahon and Andrews. The analogous identities for
three or more integers... | math.CO math.NT | the number of partitions of n into parts divisible by a or b equals the number of partitions of n in which each part and each difference of two parts is expressible as a nonnegative integer combination of a or b this generalizes identities of macmahon and andrews the analogous identities for three or more integers in p... | [['the', 'number', 'of', 'partitions', 'of', 'n', 'into', 'parts', 'divisible', 'by', 'a', 'or', 'b', 'equals', 'the', 'number', 'of', 'partitions', 'of', 'n', 'in', 'which', 'each', 'part', 'and', 'each', 'difference', 'of', 'two', 'parts', 'is', 'expressible', 'as', 'a', 'nonnegative', 'integer', 'combination', 'of',... | [-0.22011744194514904, 0.12659695246838965, -0.04937959156814031, 0.013373198788031004, -0.03262207275838591, -0.16027707738248864, 0.032470695761730894, 0.23277453493210487, -0.2580268132442143, -0.2993234507885063, 0.06816387636536092, -0.3080727648775792, -0.12756273596096435, 0.15715646061653388, -0.019012111399206... |
706.2283 | Search for Supernova Neutrino Bursts at Super-Kamiokande | The result of a search for neutrino bursts from supernova explosions using
the Super-Kamiokande detector is reported. Super-Kamiokande is sensitive to
core-collapse supernova explosions via observation of their neutrino emissions.
The expected number of events comprising such a burst is ~10^4 and the average
energy o... | astro-ph hep-ex | the result of a search for neutrino bursts from supernova explosions using the superkamiokande detector is reported superkamiokande is sensitive to corecollapse supernova explosions via observation of their neutrino emissions the expected number of events comprising such a burst is 104 and the average energy of the neu... | [['the', 'result', 'of', 'a', 'search', 'for', 'neutrino', 'bursts', 'from', 'supernova', 'explosions', 'using', 'the', 'superkamiokande', 'detector', 'is', 'reported', 'superkamiokande', 'is', 'sensitive', 'to', 'corecollapse', 'supernova', 'explosions', 'via', 'observation', 'of', 'their', 'neutrino', 'emissions', 't... | [-0.06520290277363859, 0.12524282110646343, -0.02238523416741231, 0.14459597741937047, -0.08537157273540642, -0.01614879868628288, 0.1135527036960128, 0.3563986428190845, -0.18153141559760824, -0.39670266952462396, 0.09465039044984483, -0.3606768028036534, 0.005785216465471433, 0.2500531289109646, -0.003834618724937030... |
706.2284 | On advanced fluid modelling of drift wave turbulence | The Dupree-Weinstock renormalization is used to prove that a reactive closure
exists for drift wave turbulence in magnetized plasmas. The result is used to
explain recent results in gyrokinetic simulations and is also related to the
Mattor-Parker closure. The level of closure is found in terms of applied
external sou... | physics.plasm-ph | the dupreeweinstock renormalization is used to prove that a reactive closure exists for drift wave turbulence in magnetized plasmas the result is used to explain recent results in gyrokinetic simulations and is also related to the mattorparker closure the level of closure is found in terms of applied external sources | [['the', 'dupreeweinstock', 'renormalization', 'is', 'used', 'to', 'prove', 'that', 'a', 'reactive', 'closure', 'exists', 'for', 'drift', 'wave', 'turbulence', 'in', 'magnetized', 'plasmas', 'the', 'result', 'is', 'used', 'to', 'explain', 'recent', 'results', 'in', 'gyrokinetic', 'simulations', 'and', 'is', 'also', 're... | [-0.13689068080081293, 0.1290031566847271, -0.0743686326701815, 0.10640377404827935, -0.037800792953930795, -0.03013106649935556, -0.056745280511677265, 0.3241291617353757, -0.2651204270853971, -0.2306168679303179, 0.04655711149340883, -0.23486193981564915, -0.10147711541503668, 0.2532756883301772, -0.03918686728381241... |
706.2285 | Universal power law behaviors in genomic sequences and evolutionary
models | We study the length distribution of a particular class of DNA sequences known
as 5'UTR exons. These exons belong to the messanger RNA of protein coding
genes, but they are not coding (they are located upstream of the coding portion
of the mRNA) and are thus less constrained from an evolutionary point of view.
We show... | q-bio.GN cond-mat.other physics.bio-ph q-bio.QM | we study the length distribution of a particular class of dna sequences known as 5utr exons these exons belong to the messanger rna of protein coding genes but they are not coding they are located upstream of the coding portion of the mrna and are thus less constrained from an evolutionary point of view we show that bo... | [['we', 'study', 'the', 'length', 'distribution', 'of', 'a', 'particular', 'class', 'of', 'dna', 'sequences', 'known', 'as', '5utr', 'exons', 'these', 'exons', 'belong', 'to', 'the', 'messanger', 'rna', 'of', 'protein', 'coding', 'genes', 'but', 'they', 'are', 'not', 'coding', 'they', 'are', 'located', 'upstream', 'of'... | [-0.12406465439894462, 0.1373364259953694, -0.0949786820457977, 0.11384533089133504, -0.03738719900364725, -0.17526176319123038, 0.057887831734475294, 0.4113071427400251, -0.2973885548671762, -0.2671249440319619, 0.05397475301853191, -0.24029267578638946, -0.21752538767109797, 0.1839415262457779, -0.12938676619884168, ... |
706.2286 | Spectral Methods for Numerical Relativity | Equations arising in General Relativity are usually too complicated to be
solved analytically and one has to rely on numerical methods to solve sets of
coupled partial differential equations. Among the possible choices, this paper
focuses on a class called spectral methods where, typically, the various
functions are ... | gr-qc math.SP | equations arising in general relativity are usually too complicated to be solved analytically and one has to rely on numerical methods to solve sets of coupled partial differential equations among the possible choices this paper focuses on a class called spectral methods where typically the various functions are expand... | [['equations', 'arising', 'in', 'general', 'relativity', 'are', 'usually', 'too', 'complicated', 'to', 'be', 'solved', 'analytically', 'and', 'one', 'has', 'to', 'rely', 'on', 'numerical', 'methods', 'to', 'solve', 'sets', 'of', 'coupled', 'partial', 'differential', 'equations', 'among', 'the', 'possible', 'choices', '... | [-0.10158996436343602, 0.07040995967476384, -0.060416760854423046, 0.11031812138451068, -0.10335357480584399, -0.1251235966245938, -0.0018985622299001797, 0.34724800247993126, -0.23452223595231772, -0.2583254908162512, 0.14936920270801668, -0.26930473194837473, -0.11666610493128629, 0.24092428876442443, -0.050213687690... |
706.2287 | Simulation of two spin-$s$ singlet correlations for all $s$ involving
spin measurements | In a recent paper [A. Ahanj et al., quant-ph/0603053], we gave a classical
protocol to simulate quantum correlations corresponding to the spin $s$ singlet
state for the infinite sequence of spins satisfying $2s+1 = 2^{n}$. In the
present paper, we have generalized this result by giving a classical protocol
to exactly... | quant-ph | in a recent paper a ahanj et al quantph0603053 we gave a classical protocol to simulate quantum correlations corresponding to the spin s singlet state for the infinite sequence of spins satisfying 2s1 2n in the present paper we have generalized this result by giving a classical protocol to exactly simulate quantum corr... | [['in', 'a', 'recent', 'paper', 'a', 'ahanj', 'et', 'al', 'quantph0603053', 'we', 'gave', 'a', 'classical', 'protocol', 'to', 'simulate', 'quantum', 'correlations', 'corresponding', 'to', 'the', 'spin', 's', 'singlet', 'state', 'for', 'the', 'infinite', 'sequence', 'of', 'spins', 'satisfying', '2s1', '2n', 'in', 'the',... | [-0.16832500618071325, 0.184147796264076, -0.0052152623707849175, 0.051566020207246765, -0.005635644711043325, -0.22834432139361818, 0.026348334814106384, 0.32406627062347626, -0.2260810134616951, -0.33546956186933863, 0.06368655633583155, -0.32951040758991673, -0.06794481463692782, 0.13483123609330505, -0.037751545930... |
706.2288 | The fraction of binary systems in the core of thirteen low-density
Galactic globular clusters | We used deep observations collected with ACS@HST to derive the fraction of
binary systems in a sample of thirteen low-density Galactic globular clusters.
By analysing the color distribution of Main Sequence stars we derived the
minimum fraction of binary systems required to reproduce the observed
color-magnitude diag... | astro-ph | we used deep observations collected with acshst to derive the fraction of binary systems in a sample of thirteen lowdensity galactic globular clusters by analysing the color distribution of main sequence stars we derived the minimum fraction of binary systems required to reproduce the observed colormagnitude diagram mo... | [['we', 'used', 'deep', 'observations', 'collected', 'with', 'acshst', 'to', 'derive', 'the', 'fraction', 'of', 'binary', 'systems', 'in', 'a', 'sample', 'of', 'thirteen', 'lowdensity', 'galactic', 'globular', 'clusters', 'by', 'analysing', 'the', 'color', 'distribution', 'of', 'main', 'sequence', 'stars', 'we', 'deriv... | [-0.11009954370188811, 0.11482519384719862, -0.07294935928580683, 0.07871727118120264, -0.04262923145251087, -0.0003055397859843802, 0.12814575697060612, 0.37485419818361804, -0.1989159681199288, -0.39577672966132477, 0.0581469145874793, -0.29362315297403857, -0.042371449876427054, 0.18485080908160378, -0.0133585500807... |
706.2289 | Laser cooling of unbound atoms in nondissipative optical lattices | The semiclassical theory of laser cooling is applied for the analysis of
cooling of unbound atoms with the values of the ground and exited state angular
moments 1/2 in a one-dimensional nondissipative optical lattice. We show that
in the low-saturation limit with respect to the pumping field a qualitative
interpretat... | physics.optics | the semiclassical theory of laser cooling is applied for the analysis of cooling of unbound atoms with the values of the ground and exited state angular moments 12 in a onedimensional nondissipative optical lattice we show that in the lowsaturation limit with respect to the pumping field a qualitative interpretation of... | [['the', 'semiclassical', 'theory', 'of', 'laser', 'cooling', 'is', 'applied', 'for', 'the', 'analysis', 'of', 'cooling', 'of', 'unbound', 'atoms', 'with', 'the', 'values', 'of', 'the', 'ground', 'and', 'exited', 'state', 'angular', 'moments', '12', 'in', 'a', 'onedimensional', 'nondissipative', 'optical', 'lattice', '... | [-0.12929570646889077, 0.2177775063133542, -0.05586571325851685, 0.04764962032693776, -0.0013893527802133906, -0.10604211260510636, 0.07991268430951227, 0.3726817063879276, -0.2674220390820309, -0.257129419398025, 0.026785404693024855, -0.26526711512491125, -0.06538362643155067, 0.18677158409432656, 0.03570054092552459... |
706.229 | Study of the Born-Oppenheimer Approximation for Mass-Scaling of Cold
Collision Properties | Asymptotic levels of the A $^1\Sigma_u^+$ state of the two isotopomers
$^{39}{\rm K}_2$ and $^{39}{\rm K}^{41}{\rm K}$ up to the dissociation limit
are investigated with a Doppler-free high resolution laser-spectroscopic
experiment in a molecular beam. The observed level structure can be reproduced
correctly only if ... | cond-mat.other | asymptotic levels of the a 1sigma_u state of the two isotopomers 39rm k_2 and 39rm k41rm k up to the dissociation limit are investigated with a dopplerfree high resolution laserspectroscopic experiment in a molecular beam the observed level structure can be reproduced correctly only if a mass dependent correction term ... | [['asymptotic', 'levels', 'of', 'the', 'a', '1sigma_u', 'state', 'of', 'the', 'two', 'isotopomers', '39rm', 'k_2', 'and', '39rm', 'k41rm', 'k', 'up', 'to', 'the', 'dissociation', 'limit', 'are', 'investigated', 'with', 'a', 'dopplerfree', 'high', 'resolution', 'laserspectroscopic', 'experiment', 'in', 'a', 'molecular',... | [-0.13032188234277642, 0.15035430122560894, -0.09250628516579476, 0.09460758726681189, 0.02881881647492544, -0.10880501417425247, 0.04153411095075381, 0.34119997820100534, -0.236177348216118, -0.3188530166919988, 0.018867369938211944, -0.30907770855209005, -0.027978151817268763, 0.12447000065675148, 0.02589304175209970... |
706.2291 | Existence theorem and blow-up criterion of the strong solutions to the
Magneto-micropolar fluid equations | In this paper we study the magneto-micropolar fluid equations in $\R^3$,
prove the existence of the strong solution with initial data in $H^s(\R^3)$ for
$s> {3/2}$, and set up its blow-up criterion. The tool we mainly use is
Littlewood-Paley decomposition, by which we obtain a Beale-Kato-Majda type
blow-up criterion ... | math.AP | in this paper we study the magnetomicropolar fluid equations in r3 prove the existence of the strong solution with initial data in hsr3 for s 32 and set up its blowup criterion the tool we mainly use is littlewoodpaley decomposition by which we obtain a bealekatomajda type blowup criterion for smooth solution uomegab w... | [['in', 'this', 'paper', 'we', 'study', 'the', 'magnetomicropolar', 'fluid', 'equations', 'in', 'r3', 'prove', 'the', 'existence', 'of', 'the', 'strong', 'solution', 'with', 'initial', 'data', 'in', 'hsr3', 'for', 's', '32', 'and', 'set', 'up', 'its', 'blowup', 'criterion', 'the', 'tool', 'we', 'mainly', 'use', 'is', '... | [-0.16180582966686027, -0.018354524957535208, -0.10568551917667271, 0.04410355942720761, -0.0764905146521623, -0.1318297925267796, 0.024601116724938275, 0.26149802940485417, -0.28979387232026116, -0.2113099537148583, 0.17043300788490803, -0.24226258074498322, -0.09534807848270799, 0.17516675260925635, -0.05593809491542... |
706.2292 | First observations of beam losses due to bound-free pair production in a
heavy-ion collider | We report the first observations of beam losses due to bound-free pair
production at the interaction point of a heavy-ion collider. This process is
expected to be a major luminosity limit for the Large Hadron Collider (LHC)
when it operates with 208Pb82+ ions because the localized energy deposition by
the lost ions m... | physics.acc-ph nucl-ex | we report the first observations of beam losses due to boundfree pair production at the interaction point of a heavyion collider this process is expected to be a major luminosity limit for the large hadron collider lhc when it operates with 208pb82 ions because the localized energy deposition by the lost ions may quenc... | [['we', 'report', 'the', 'first', 'observations', 'of', 'beam', 'losses', 'due', 'to', 'boundfree', 'pair', 'production', 'at', 'the', 'interaction', 'point', 'of', 'a', 'heavyion', 'collider', 'this', 'process', 'is', 'expected', 'to', 'be', 'a', 'major', 'luminosity', 'limit', 'for', 'the', 'large', 'hadron', 'collid... | [-0.07475498454153949, 0.2741903796460659, -0.06209949156504095, 0.07120746686487969, 0.021915511198811174, -0.13328120692845757, -0.027554012395030872, 0.38020581105269313, -0.20448159608315294, -0.31456825910796093, -0.009052706086700122, -0.3733075867135694, 0.11979359327485477, 0.18985575858474246, 0.08741833561092... |
706.2293 | Resource control of object-oriented programs | A sup-interpretation is a tool which provides an upper bound on the size of a
value computed by some symbol of a program. Sup-interpretations have shown
their interest to deal with the complexity of first order functional programs.
For instance, they allow to characterize all the functions bitwise computable
in Alogt... | cs.PL cs.LO | a supinterpretation is a tool which provides an upper bound on the size of a value computed by some symbol of a program supinterpretations have shown their interest to deal with the complexity of first order functional programs for instance they allow to characterize all the functions bitwise computable in alogtime thi... | [['a', 'supinterpretation', 'is', 'a', 'tool', 'which', 'provides', 'an', 'upper', 'bound', 'on', 'the', 'size', 'of', 'a', 'value', 'computed', 'by', 'some', 'symbol', 'of', 'a', 'program', 'supinterpretations', 'have', 'shown', 'their', 'interest', 'to', 'deal', 'with', 'the', 'complexity', 'of', 'first', 'order', 'f... | [-0.12737984963655635, 0.06957084711963533, -0.12319076078144454, 0.07931496118261289, -0.09785098333191951, -0.15323598532055596, 0.07163645434028477, 0.3166244004366804, -0.28392177825150766, -0.30192292301165585, 0.12131831315613921, -0.22180629383146236, -0.13666940451212292, 0.20101048198602764, -0.087242422295750... |
706.2294 | On the origin of thermal string gas | We investigate decaying D-branes as the origin of the thermal string gas of
string gas cosmology. We consider initial configurations of low-dimensional
branes and argue that they can time evolve to thermal string gas. We find that
there is a range in the weak string coupling and fast brane decay time regimes,
where t... | hep-th astro-ph gr-qc | we investigate decaying dbranes as the origin of the thermal string gas of string gas cosmology we consider initial configurations of lowdimensional branes and argue that they can time evolve to thermal string gas we find that there is a range in the weak string coupling and fast brane decay time regimes where the init... | [['we', 'investigate', 'decaying', 'dbranes', 'as', 'the', 'origin', 'of', 'the', 'thermal', 'string', 'gas', 'of', 'string', 'gas', 'cosmology', 'we', 'consider', 'initial', 'configurations', 'of', 'lowdimensional', 'branes', 'and', 'argue', 'that', 'they', 'can', 'time', 'evolve', 'to', 'thermal', 'string', 'gas', 'w... | [-0.192351591782224, 0.25327660381380057, -0.07157706998016995, 0.13456663215927417, -0.04619472643308756, -0.1634749346994795, -0.0019325612326307844, 0.3347789773769263, -0.26862490982360515, -0.24186013545194227, 0.07540018870430584, -0.23911065992433578, -0.02392760175280273, 0.12342732664223553, 0.0339671243046824... |
706.2295 | Exact treatment of linear difference equations with noncommutative
coefficients | The exact solution of a Cauchy problem related to a linear second-order
difference equation with constant noncommutative coefficients is reported.
| math-ph math.MP | the exact solution of a cauchy problem related to a linear secondorder difference equation with constant noncommutative coefficients is reported | [['the', 'exact', 'solution', 'of', 'a', 'cauchy', 'problem', 'related', 'to', 'a', 'linear', 'secondorder', 'difference', 'equation', 'with', 'constant', 'noncommutative', 'coefficients', 'is', 'reported']] | [-0.17781269513070583, 0.016856093984097244, -0.06111042210832238, 0.06209241336327977, -0.1862642290070653, -0.1765599087346345, -0.04859669413417578, 0.23433771785348653, -0.37603586753830315, -0.19595022285357117, 0.1294204456731677, -0.35541105885058644, -0.16407376937568188, 0.1590078515931964, -0.0130918521434068... |
706.2296 | Signatures of fractal clustering of aerosols advected under gravity | Aerosols under chaotic advection often approach a strange attractor. They
move chaotically on this fractal set but, in the presence of gravity, they have
a net vertical motion downwards. In practical situations, observational data
may be available only at a given level, for example at the ground level. We
uncover two... | nlin.CD physics.ao-ph physics.flu-dyn | aerosols under chaotic advection often approach a strange attractor they move chaotically on this fractal set but in the presence of gravity they have a net vertical motion downwards in practical situations observational data may be available only at a given level for example at the ground level we uncover two fractal ... | [['aerosols', 'under', 'chaotic', 'advection', 'often', 'approach', 'a', 'strange', 'attractor', 'they', 'move', 'chaotically', 'on', 'this', 'fractal', 'set', 'but', 'in', 'the', 'presence', 'of', 'gravity', 'they', 'have', 'a', 'net', 'vertical', 'motion', 'downwards', 'in', 'practical', 'situations', 'observational'... | [-0.1397309703020645, 0.16126552581609715, -0.12071953308546828, 0.0965242332013856, -0.047825416918134404, -0.12900310554763392, 0.05765222772246315, 0.3000608402526095, -0.28696293339488055, -0.2670427253514174, 0.11419821803103246, -0.2947854084007087, -0.14349695324365583, 0.21046858444100336, -0.04948500602788824,... |
706.2297 | The Minimal Number of Periodic Orbits of Periods Guaranteed in
Sharkovskii's Theorem | Let f(x) be a continuous function from a compact real interval into itself
with a periodic orbit of minimal period m, where m is not an integral power of
2. Then, by Sharkovsky's theorem, for every positive integer n with m \prec n
in the Sharkovsky's ordering defined below, a lower bound on the number of
periodic or... | math.DS math.NT | let fx be a continuous function from a compact real interval into itself with a periodic orbit of minimal period m where m is not an integral power of 2 then by sharkovskys theorem for every positive integer n with m prec n in the sharkovskys ordering defined below a lower bound on the number of periodic orbits of fx w... | [['let', 'fx', 'be', 'a', 'continuous', 'function', 'from', 'a', 'compact', 'real', 'interval', 'into', 'itself', 'with', 'a', 'periodic', 'orbit', 'of', 'minimal', 'period', 'm', 'where', 'm', 'is', 'not', 'an', 'integral', 'power', 'of', '2', 'then', 'by', 'sharkovskys', 'theorem', 'for', 'every', 'positive', 'intege... | [-0.20070908623590564, 0.17364198498554093, -0.05208890382305122, 0.01962771071408865, -0.07241695902174276, -0.16177324638335724, 0.07190386592698272, 0.30294830520543153, -0.2679444869791859, -0.3094534422427918, 0.10013121811756759, -0.27127467242352077, -0.11277999829113734, 0.22630820205968835, -0.0948159941943006... |
706.2298 | Local coherence and deflation of the low quark modes in lattice QCD | The spontaneous breaking of chiral symmetry in QCD is known to be linked to a
non-zero density of eigenvalues of the massless Dirac operator near the origin.
Numerical studies of two-flavour QCD now suggest that the low quark modes are
locally coherent to a certain extent. As a consequence, the modes can be
simultane... | hep-lat | the spontaneous breaking of chiral symmetry in qcd is known to be linked to a nonzero density of eigenvalues of the massless dirac operator near the origin numerical studies of twoflavour qcd now suggest that the low quark modes are locally coherent to a certain extent as a consequence the modes can be simultaneously d... | [['the', 'spontaneous', 'breaking', 'of', 'chiral', 'symmetry', 'in', 'qcd', 'is', 'known', 'to', 'be', 'linked', 'to', 'a', 'nonzero', 'density', 'of', 'eigenvalues', 'of', 'the', 'massless', 'dirac', 'operator', 'near', 'the', 'origin', 'numerical', 'studies', 'of', 'twoflavour', 'qcd', 'now', 'suggest', 'that', 'the... | [-0.11322168008085678, 0.21746223141354593, -0.11445289564911615, 0.0451030494497073, -0.09578898740636016, -0.08853416957638481, 0.06417864370583133, 0.3554879439740696, -0.22224955767901106, -0.22767211912697266, 0.10408195035151122, -0.2951908045871691, -0.08745827127078717, 0.12139234493528916, 0.013392765963958069... |
706.2299 | Diffuse HI Disks in Isolated Galaxies | In order to investigate the contribution of diffuse components to their total
HI emission, we have obtained high precision HI line flux densities with the
100m Green Bank Telescope for a sample of 100 isolated spiral and irregular
galaxies which we have previously observed with the 43m telescope. A comparison
of the ... | astro-ph | in order to investigate the contribution of diffuse components to their total hi emission we have obtained high precision hi line flux densities with the 100m green bank telescope for a sample of 100 isolated spiral and irregular galaxies which we have previously observed with the 43m telescope a comparison of the obse... | [['in', 'order', 'to', 'investigate', 'the', 'contribution', 'of', 'diffuse', 'components', 'to', 'their', 'total', 'hi', 'emission', 'we', 'have', 'obtained', 'high', 'precision', 'hi', 'line', 'flux', 'densities', 'with', 'the', '100m', 'green', 'bank', 'telescope', 'for', 'a', 'sample', 'of', '100', 'isolated', 'spi... | [-0.07301940334389687, 0.05518857177752906, -0.03600022251494866, 0.10051365493961936, -0.04934174093640704, -0.06216815197900033, 0.01634497847308556, 0.4694706191643117, -0.10078966468333816, -0.3562209570748556, 0.06788222211598156, -0.29318695266842526, -0.040058197980472006, 0.18415547980435398, 0.0134131351016207... |
706.23 | The few-body problem in terms of correlated gaussians | In their textbook, Suzuki and Varga [Y. Suzuki and K. Varga, {\em Stochastic
Variational Approach to Quantum-Mechanical Few-Body Problems} (Springer,
Berlin, 1998)] present the stochastic variational method in a very exhaustive
way. In this framework, the so-called correlated gaussian bases are often
employed. Genera... | hep-ph physics.comp-ph | in their textbook suzuki and varga y suzuki and k varga em stochastic variational approach to quantummechanical fewbody problems springer berlin 1998 present the stochastic variational method in a very exhaustive way in this framework the socalled correlated gaussian bases are often employed general formulae for the ma... | [['in', 'their', 'textbook', 'suzuki', 'and', 'varga', 'y', 'suzuki', 'and', 'k', 'varga', 'em', 'stochastic', 'variational', 'approach', 'to', 'quantummechanical', 'fewbody', 'problems', 'springer', 'berlin', '1998', 'present', 'the', 'stochastic', 'variational', 'method', 'in', 'a', 'very', 'exhaustive', 'way', 'in',... | [-0.06370619056304182, 0.07333710985232542, -0.11808197057469427, 0.14134416601057126, -0.08935017313636026, -0.13029133130506682, 0.016787164253691415, 0.36325001201647167, -0.2531223617134099, -0.2929007173163675, 0.07684640216684173, -0.26138427950629667, -0.18555902774218752, 0.2160209172460086, -0.0904475058342854... |
706.2301 | X-ray detection of the substellar twin 2MASS J11011926-7732383 AB | 2MASS J11011926-7732383 AB (hereafter 2M1101AB), located in the Cha I star
forming region, is a rare wide-separation brown dwarf binary. XMM-Newton and
Chandra observations of 2M1101AB have allowed us to examine the influence of
physical parameters (mass, bolometric luminosity and effective temperature) on
X-ray emis... | astro-ph | 2mass j110119267732383 ab hereafter 2m1101ab located in the cha i star forming region is a rare wideseparation brown dwarf binary xmmnewton and chandra observations of 2m1101ab have allowed us to examine the influence of physical parameters mass bolometric luminosity and effective temperature on xray emission from a co... | [['2mass', 'j110119267732383', 'ab', 'hereafter', '2m1101ab', 'located', 'in', 'the', 'cha', 'i', 'star', 'forming', 'region', 'is', 'a', 'rare', 'wideseparation', 'brown', 'dwarf', 'binary', 'xmmnewton', 'and', 'chandra', 'observations', 'of', '2m1101ab', 'have', 'allowed', 'us', 'to', 'examine', 'the', 'influence', '... | [-0.024475103401623313, 0.14259442616631055, -0.07800422892018798, 0.09801674476503172, -0.1602014123617361, -0.10861639603750692, 0.10426951579505667, 0.4379841883256588, -0.12867239725033175, -0.34221793305394904, 0.058602550810402526, -0.3524045137156333, -0.008303863161598288, 0.17895938709800593, -0.06521775839708... |
706.2302 | Measuring the surface stress polar dependence | While measurements of the polar dependence of the surface free energy are
easily available, measurements of the whole polar dependence of the surface
stress of a crystal do not exist. In this paper is presented a new procedure
that allows, for the first time, the experimental determination of the surface
stress polar... | cond-mat.mtrl-sci | while measurements of the polar dependence of the surface free energy are easily available measurements of the whole polar dependence of the surface stress of a crystal do not exist in this paper is presented a new procedure that allows for the first time the experimental determination of the surface stress polar depen... | [['while', 'measurements', 'of', 'the', 'polar', 'dependence', 'of', 'the', 'surface', 'free', 'energy', 'are', 'easily', 'available', 'measurements', 'of', 'the', 'whole', 'polar', 'dependence', 'of', 'the', 'surface', 'stress', 'of', 'a', 'crystal', 'do', 'not', 'exist', 'in', 'this', 'paper', 'is', 'presented', 'a',... | [-0.12774695891191737, 0.14840997428252872, -0.11840810638878652, -0.011369328044066337, -0.09119385731419627, -0.08876847732536705, 0.03076189310244009, 0.356629104832266, -0.2842390319778466, -0.3177410187986745, 0.07653177528835597, -0.21717499154400569, -0.11041764895969504, 0.20867789149838564, -0.0082638711786605... |
706.2303 | Riccati equation-based generalization of Dawson's integral function | A new generalization of Dawson's integral function based on the link between
a Riccati nonlinear differential equation and a second-order ordinary
differential equation is reported. The MacLaurin expansion of this generalized
function is built up and to this end an explicit formula for a generic cofactor
of a triangu... | math-ph math.MP | a new generalization of dawsons integral function based on the link between a riccati nonlinear differential equation and a secondorder ordinary differential equation is reported the maclaurin expansion of this generalized function is built up and to this end an explicit formula for a generic cofactor of a triangular m... | [['a', 'new', 'generalization', 'of', 'dawsons', 'integral', 'function', 'based', 'on', 'the', 'link', 'between', 'a', 'riccati', 'nonlinear', 'differential', 'equation', 'and', 'a', 'secondorder', 'ordinary', 'differential', 'equation', 'is', 'reported', 'the', 'maclaurin', 'expansion', 'of', 'this', 'generalized', 'f... | [-0.14551025149054253, -0.00503407298478683, -0.14308238074255103, 0.0703902060251074, -0.15970359538466886, -0.12310561552966157, -0.008191574436540786, 0.23663000986338234, -0.3175551091822294, -0.22509124423735416, 0.08746930409688503, -0.27101614533099705, -0.22250169988435048, 0.2174335515144496, -0.01337108936590... |
706.2304 | Charged Condensation | We consider Bose-Einstein condensation of massive electrically charged
scalars in a uniform background of charged fermions. We focus on the case when
the scalar condensate screens the background charge, while the net charge of
the system resides on its boundary surface. A distinctive signature of this
substance is th... | hep-th | we consider boseeinstein condensation of massive electrically charged scalars in a uniform background of charged fermions we focus on the case when the scalar condensate screens the background charge while the net charge of the system resides on its boundary surface a distinctive signature of this substance is that the... | [['we', 'consider', 'boseeinstein', 'condensation', 'of', 'massive', 'electrically', 'charged', 'scalars', 'in', 'a', 'uniform', 'background', 'of', 'charged', 'fermions', 'we', 'focus', 'on', 'the', 'case', 'when', 'the', 'scalar', 'condensate', 'screens', 'the', 'background', 'charge', 'while', 'the', 'net', 'charge'... | [-0.1714541800431907, 0.2862547792047262, -0.05357533809915185, 0.06954827975761145, -0.02520995271578431, -0.14118496180325746, 0.017785267814993858, 0.31620496843755247, -0.14010421157255767, -0.279363615045324, 0.006240164713002741, -0.3171523227915168, -0.03846949455887079, 0.11724620732851326, -0.00890216851234436... |
706.2305 | Absolute surface energy determination | Experimental determination of absolute surface energies remains a challenge.
We propose a simple method based on two independent measurements on 3D and 2D
equilibrium shapes completed by the analysis of the thermal fluctuation of an
isolated step. Using then basic equations (Wulff' theorem, Gibbs-Thomson
equation, th... | cond-mat.mtrl-sci | experimental determination of absolute surface energies remains a challenge we propose a simple method based on two independent measurements on 3d and 2d equilibrium shapes completed by the analysis of the thermal fluctuation of an isolated step using then basic equations wulff theorem gibbsthomson equation thermodynam... | [['experimental', 'determination', 'of', 'absolute', 'surface', 'energies', 'remains', 'a', 'challenge', 'we', 'propose', 'a', 'simple', 'method', 'based', 'on', 'two', 'independent', 'measurements', 'on', '3d', 'and', '2d', 'equilibrium', 'shapes', 'completed', 'by', 'the', 'analysis', 'of', 'the', 'thermal', 'fluctua... | [-0.07906594057785016, 0.09159668001686833, -0.14768808329408276, 0.020240680824869496, -0.019817944141714092, -0.14173186979491578, 0.03178881371620102, 0.3606558881317065, -0.25161001091022217, -0.3182084943629175, 0.05897657844351135, -0.2794500404609004, -0.0848376886205417, 0.19766854397325873, -0.0261702554770440... |
706.2306 | Thermoelectric effects in superconducting proximity structures | Attaching a superconductor in good contact with a normal metal makes rise to
a proximity effect where the superconducting correlations leak into the normal
metal. An additional contact close to the first one makes it possible to carry
a supercurrent through the metal. Forcing this supercurrent flow along with an
addi... | cond-mat.supr-con | attaching a superconductor in good contact with a normal metal makes rise to a proximity effect where the superconducting correlations leak into the normal metal an additional contact close to the first one makes it possible to carry a supercurrent through the metal forcing this supercurrent flow along with an addition... | [['attaching', 'a', 'superconductor', 'in', 'good', 'contact', 'with', 'a', 'normal', 'metal', 'makes', 'rise', 'to', 'a', 'proximity', 'effect', 'where', 'the', 'superconducting', 'correlations', 'leak', 'into', 'the', 'normal', 'metal', 'an', 'additional', 'contact', 'close', 'to', 'the', 'first', 'one', 'makes', 'it... | [-0.14780329056456684, 0.15537853881926275, -0.09708223284734413, 0.06314269569702446, -0.11458984535373748, -0.1633377741649747, 0.08996143332123756, 0.3540326237082481, -0.29802588833868504, -0.2953782839626074, -0.011578671450726687, -0.32705392561107877, -0.12510331335477531, 0.18212232424132527, -0.011298091758042... |
706.2307 | The periodic table of $n$-categories for low dimensions II: degenerate
tricategories | We continue the project begun in ``The periodic table of $n$-categories for
low dimensions I'' by examining degenerate tricategories and comparing them
with the structures predicted by the Periodic table. For triply degenerate
tricategories we exhibit a triequivalence with the partially discrete
tricategory of commut... | math.CT | we continue the project begun in the periodic table of ncategories for low dimensions i by examining degenerate tricategories and comparing them with the structures predicted by the periodic table for triply degenerate tricategories we exhibit a triequivalence with the partially discrete tricategory of commutative mono... | [['we', 'continue', 'the', 'project', 'begun', 'in', 'the', 'periodic', 'table', 'of', 'ncategories', 'for', 'low', 'dimensions', 'i', 'by', 'examining', 'degenerate', 'tricategories', 'and', 'comparing', 'them', 'with', 'the', 'structures', 'predicted', 'by', 'the', 'periodic', 'table', 'for', 'triply', 'degenerate', ... | [-0.11472733813479863, 0.0835878740518865, -0.04668623869656585, 0.13402102231611934, -0.09688704081963806, -0.14163590256612224, 0.046042979245612514, 0.3908396710176021, -0.3553208249504678, -0.22729831730248407, 0.06167111009290238, -0.21249682291818317, -0.15180732277121933, 0.14184399615623988, -0.1215540557841450... |
706.2308 | Spirals on Si(111) at sublimation and growth: REM and LODREM
observations | Using recently proposed improvements of Reflection Electron Microsopy (REM)
we study in perfectly controlled thermodynamics conditions spiral shapes and
spirals on Si(111) surface. It is shown that the new method named low
distortion reflection electron microscopy (LODREM) is a powerful instrument,
resolving in much ... | cond-mat.mtrl-sci | using recently proposed improvements of reflection electron microsopy rem we study in perfectly controlled thermodynamics conditions spiral shapes and spirals on si111 surface it is shown that the new method named low distortion reflection electron microscopy lodrem is a powerful instrument resolving in much more detai... | [['using', 'recently', 'proposed', 'improvements', 'of', 'reflection', 'electron', 'microsopy', 'rem', 'we', 'study', 'in', 'perfectly', 'controlled', 'thermodynamics', 'conditions', 'spiral', 'shapes', 'and', 'spirals', 'on', 'si111', 'surface', 'it', 'is', 'shown', 'that', 'the', 'new', 'method', 'named', 'low', 'dis... | [-0.08130498126966058, 0.13614893108973836, -0.132445817781707, 0.06845264318122891, -0.017069201058633153, -0.14959140587351444, 0.02160439803906306, 0.377344992745794, -0.26333320031921237, -0.30172777944491086, 0.03896145885849719, -0.29901862771139814, -0.13730261419007903, 0.1975168710815231, -0.020704247570454568... |
706.2309 | Formation and Persistence of Spatiotemporal Turing Patterns | This article is concerned with the stability and long-time dynamics of
structures arising from a structureless state. The paradigm is suggested by
developmental biology, where morphogenesis is thought to result from a
competition between chemical reactions and spatial diffusion. A system of two
reaction-diffusion equ... | nlin.PS | this article is concerned with the stability and longtime dynamics of structures arising from a structureless state the paradigm is suggested by developmental biology where morphogenesis is thought to result from a competition between chemical reactions and spatial diffusion a system of two reactiondiffusion equations ... | [['this', 'article', 'is', 'concerned', 'with', 'the', 'stability', 'and', 'longtime', 'dynamics', 'of', 'structures', 'arising', 'from', 'a', 'structureless', 'state', 'the', 'paradigm', 'is', 'suggested', 'by', 'developmental', 'biology', 'where', 'morphogenesis', 'is', 'thought', 'to', 'result', 'from', 'a', 'compet... | [-0.1652618567560516, 0.1064720788322713, -0.08512683984894387, 0.061571988391021834, 0.004654277354585129, -0.11294948745458185, -0.0286893706323336, 0.239740383458332, -0.3063831737912867, -0.24235077144618591, 0.1258736847059639, -0.2873078886794088, -0.2061262134330995, 0.16294882107404587, -0.02976676742748722, 0.... |
706.231 | Space-time coding techniques with bit-interleaved coded modulations for
MIMO block-fading channels | The space-time bit-interleaved coded modulation (ST-BICM) is an efficient
technique to obtain high diversity and coding gain on a block-fading MIMO
channel. Its maximum-likelihood (ML) performance is computed under ideal
interleaving conditions, which enables a global optimization taking into
account channel coding. ... | cs.IT math.IT | the spacetime bitinterleaved coded modulation stbicm is an efficient technique to obtain high diversity and coding gain on a blockfading mimo channel its maximumlikelihood ml performance is computed under ideal interleaving conditions which enables a global optimization taking into account channel coding thanks to a di... | [['the', 'spacetime', 'bitinterleaved', 'coded', 'modulation', 'stbicm', 'is', 'an', 'efficient', 'technique', 'to', 'obtain', 'high', 'diversity', 'and', 'coding', 'gain', 'on', 'a', 'blockfading', 'mimo', 'channel', 'its', 'maximumlikelihood', 'ml', 'performance', 'is', 'computed', 'under', 'ideal', 'interleaving', '... | [-0.230647896233043, 0.007189961694772744, -0.07793897044559178, 0.03795769050008279, -0.0698131105887252, -0.25025073613153037, 0.08044083040405178, 0.38897461466717, -0.2697661392475394, -0.2572848371668387, 0.11707204522099346, -0.20037678653501312, -0.1567921699024737, 0.16390720668785047, -0.13958138254979116, 0.0... |
706.2311 | Stable crystalline lattices in two-dimensional binary mixtures of
dipolar particles | The phase diagram of binary mixtures of particles interacting via a pair
potential of parallel dipoles is computed at zero temperature as a function of
composition and the ratio of their magnetic susceptibilities. Using lattice
sums, a rich variety of different stable crystalline structures is identified
including $A... | cond-mat.soft cond-mat.stat-mech | the phase diagram of binary mixtures of particles interacting via a pair potential of parallel dipoles is computed at zero temperature as a function of composition and the ratio of their magnetic susceptibilities using lattice sums a rich variety of different stable crystalline structures is identified including a_mb_n... | [['the', 'phase', 'diagram', 'of', 'binary', 'mixtures', 'of', 'particles', 'interacting', 'via', 'a', 'pair', 'potential', 'of', 'parallel', 'dipoles', 'is', 'computed', 'at', 'zero', 'temperature', 'as', 'a', 'function', 'of', 'composition', 'and', 'the', 'ratio', 'of', 'their', 'magnetic', 'susceptibilities', 'using... | [-0.18899611670490915, 0.28371971164854753, -0.04017596399675297, 0.02016438566667514, -0.010689133994561513, -0.11447768889169778, 0.030565084271396682, 0.3858836183769513, -0.2502857794742042, -0.2828305168819111, 0.043454619811691214, -0.3010793573560968, -0.08563888152758385, 0.12801771243185267, 0.1092262863741973... |
706.2312 | Carrier-carrier entanglement and transport resonances in semiconductor
quantum dots | We study theoretically the entanglement created in a scattering between an
electron, incoming from a source lead, and another electron bound in the ground
state of a quantum dot, connected to two leads. We analyze the role played by
the different kinds of resonances in the transmission spectra and by the number
of sc... | cond-mat.mes-hall quant-ph | we study theoretically the entanglement created in a scattering between an electron incoming from a source lead and another electron bound in the ground state of a quantum dot connected to two leads we analyze the role played by the different kinds of resonances in the transmission spectra and by the number of scatteri... | [['we', 'study', 'theoretically', 'the', 'entanglement', 'created', 'in', 'a', 'scattering', 'between', 'an', 'electron', 'incoming', 'from', 'a', 'source', 'lead', 'and', 'another', 'electron', 'bound', 'in', 'the', 'ground', 'state', 'of', 'a', 'quantum', 'dot', 'connected', 'to', 'two', 'leads', 'we', 'analyze', 'th... | [-0.18394533263955026, 0.1886671537091212, -0.10307082878425718, 0.07636994782519797, 0.025348834302877227, -0.15571924022609188, 0.046194973156126515, 0.3402329480981514, -0.2562029676421756, -0.30291456475613576, 0.0004575537389985496, -0.32529855252754303, -0.13849228658983784, 0.19613340721135178, 0.017692603483315... |
706.2313 | Cohomology of diffeological spaces and foliations | Let (M,F) be a foliated manifold. We study the relationship between the basic
cohomology Hb(M,F) of the foliation and the De Rham cohomology H(DF) of the
space of leaves M/F as a quotient diffeological space. We prove that for an
arbitrary foliation there is a morphism from H(DF) to Hb(M,F). It is an
isomorphism when... | math.DG | let mf be a foliated manifold we study the relationship between the basic cohomology hbmf of the foliation and the de rham cohomology hdf of the space of leaves mf as a quotient diffeological space we prove that for an arbitrary foliation there is a morphism from hdf to hbmf it is an isomorphism when f is a qfoliation | [['let', 'mf', 'be', 'a', 'foliated', 'manifold', 'we', 'study', 'the', 'relationship', 'between', 'the', 'basic', 'cohomology', 'hbmf', 'of', 'the', 'foliation', 'and', 'the', 'de', 'rham', 'cohomology', 'hdf', 'of', 'the', 'space', 'of', 'leaves', 'mf', 'as', 'a', 'quotient', 'diffeological', 'space', 'we', 'prove', ... | [-0.24191565547204977, 0.06290603312715705, -0.18468916003725358, 0.1001236096469386, -0.1277486656659416, -0.10074899728143853, -0.06410921508047197, 0.35108875163963865, -0.3711094191031797, -0.1970512322482786, 0.07409898648204814, -0.21227566690816144, -0.1684707590029575, 0.1457263368065469, -0.17993875935540668, ... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.