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 |
|---|---|---|---|---|---|---|
709.0935 | The Algebraic Complexity of Maximum Likelihood Estimation for Bivariate
Missing Data | We study the problem of maximum likelihood estimation for general patterns of
bivariate missing data for normal and multinomial random variables, under the
assumption that the data is missing at random (MAR). For normal data, the score
equations have nine complex solutions, at least one of which is real and
statistic... | math.ST math.AG stat.CO stat.TH | we study the problem of maximum likelihood estimation for general patterns of bivariate missing data for normal and multinomial random variables under the assumption that the data is missing at random mar for normal data the score equations have nine complex solutions at least one of which is real and statistically sig... | [['we', 'study', 'the', 'problem', 'of', 'maximum', 'likelihood', 'estimation', 'for', 'general', 'patterns', 'of', 'bivariate', 'missing', 'data', 'for', 'normal', 'and', 'multinomial', 'random', 'variables', 'under', 'the', 'assumption', 'that', 'the', 'data', 'is', 'missing', 'at', 'random', 'mar', 'for', 'normal', ... | [-0.12373230329831131, 0.08934840906710763, -0.07992212343794693, 0.09200759246180366, -0.0706705970681339, -0.13960709899713816, 0.04237669008476327, 0.33052341836238547, -0.25904188168767306, -0.3041931520149644, 0.13784763916503703, -0.3275601858061106, -0.15466478273447137, 0.173155322302981, -0.054450709239712784,... |
709.0936 | New Curved Spacetime Dirac Equations - On the Anomalous Gyromagnetic
Ratio | I propose three new curved spacetime versions of the Dirac Equation. These
equations have been developed mainly to try and account in a natural way for
the observed anomalous gyromagnetic ratio of Fermions. The derived equations
suggest that particles including the Electron which is thought to be a point
particle do ... | physics.gen-ph | i propose three new curved spacetime versions of the dirac equation these equations have been developed mainly to try and account in a natural way for the observed anomalous gyromagnetic ratio of fermions the derived equations suggest that particles including the electron which is thought to be a point particle do have... | [['i', 'propose', 'three', 'new', 'curved', 'spacetime', 'versions', 'of', 'the', 'dirac', 'equation', 'these', 'equations', 'have', 'been', 'developed', 'mainly', 'to', 'try', 'and', 'account', 'in', 'a', 'natural', 'way', 'for', 'the', 'observed', 'anomalous', 'gyromagnetic', 'ratio', 'of', 'fermions', 'the', 'derive... | [-0.12180875017743051, 0.15535519116994864, -0.10532266907559255, 0.11923873232203651, -0.07627248560621254, -0.127191473473657, -0.011815663460868042, 0.32180135517474817, -0.23629370400218497, -0.3286698929656892, 0.05896478070463839, -0.30323839069691283, -0.12881292803102784, 0.16270873601790847, -0.012298575194673... |
709.0937 | On the reliability of linear band structure methods | We discuss an efficiency of various band structure algorithms in determining
the Fermi surface (FS) of the paramagnetic ErGa3. The linear muffin-tin orbital
(LMTO) in the atomic sphere approximation (ASA) method and three full potential
(FP) codes: FP-LMTO, FP linear augmented plane wave (FLAPW), and FP local
orbital... | cond-mat.mtrl-sci cond-mat.str-el | we discuss an efficiency of various band structure algorithms in determining the fermi surface fs of the paramagnetic erga3 the linear muffintin orbital lmto in the atomic sphere approximation asa method and three full potential fp codes fplmto fp linear augmented plane wave flapw and fp local orbitals fplo methods are... | [['we', 'discuss', 'an', 'efficiency', 'of', 'various', 'band', 'structure', 'algorithms', 'in', 'determining', 'the', 'fermi', 'surface', 'fs', 'of', 'the', 'paramagnetic', 'erga3', 'the', 'linear', 'muffintin', 'orbital', 'lmto', 'in', 'the', 'atomic', 'sphere', 'approximation', 'asa', 'method', 'and', 'three', 'full... | [-0.12877263267815045, 0.05905677639324444, -0.09719772360484125, 0.1142860788802847, -0.03901018633575546, -0.10967552803302986, -0.014244661480615583, 0.4102403490778503, -0.24777795608932957, -0.2811783854465146, -0.006903656500972671, -0.29654155322136955, -0.09186396870223823, 0.227813396637046, 0.0411844661869450... |
709.0938 | Half-metallic graphene nanodots | A comprehensive first-principles theoretical study of the electronic
properties and half-metallic nature of finite rectangular graphene nanoribbons
is presented. We identify the bisanthrene isomer of the C28H14 molecule to be
the smallest polycyclic aromatic hydrocarbon to present a spin polarized ground
state. Even ... | cond-mat.mtrl-sci cond-mat.other | a comprehensive firstprinciples theoretical study of the electronic properties and halfmetallic nature of finite rectangular graphene nanoribbons is presented we identify the bisanthrene isomer of the c28h14 molecule to be the smallest polycyclic aromatic hydrocarbon to present a spin polarized ground state even at thi... | [['a', 'comprehensive', 'firstprinciples', 'theoretical', 'study', 'of', 'the', 'electronic', 'properties', 'and', 'halfmetallic', 'nature', 'of', 'finite', 'rectangular', 'graphene', 'nanoribbons', 'is', 'presented', 'we', 'identify', 'the', 'bisanthrene', 'isomer', 'of', 'the', 'c28h14', 'molecule', 'to', 'be', 'the'... | [-0.2117793807035519, 0.222812615880927, -0.010120114430578218, 0.060381565468075375, -0.015932456376807142, -0.16157753585786042, 0.026457499331122056, 0.4763715477453338, -0.26989015210549244, -0.28804971603676677, 0.03965922768628742, -0.30473262866338097, -0.06049014694031535, 0.1384947959631164, 0.0824394851910053... |
709.0939 | Dimension Six Corrections to the Vector Sector of AdS/QCD Model | We study the effects of dimension six terms on the predictions of the
holographic model for the vector meson form factors and determine the
corrections to the electric radius, the magnetic and the quadrupole moments of
the rho-meson. We show that the only dimension six terms which contribute
nontrivially to the vecto... | hep-ph | we study the effects of dimension six terms on the predictions of the holographic model for the vector meson form factors and determine the corrections to the electric radius the magnetic and the quadrupole moments of the rhomeson we show that the only dimension six terms which contribute nontrivially to the vector mes... | [['we', 'study', 'the', 'effects', 'of', 'dimension', 'six', 'terms', 'on', 'the', 'predictions', 'of', 'the', 'holographic', 'model', 'for', 'the', 'vector', 'meson', 'form', 'factors', 'and', 'determine', 'the', 'corrections', 'to', 'the', 'electric', 'radius', 'the', 'magnetic', 'and', 'the', 'quadrupole', 'moments'... | [-0.11935565874877352, 0.2010857679312014, -0.028365212527138216, 0.0910014664452454, -0.06261726624021928, -0.046238590438884716, 0.01318786365876871, 0.29302783048263303, -0.21580837524185578, -0.25663518508620287, 0.009729327618454893, -0.3123313519965719, -0.11337009263742301, 0.11389145744895493, 0.063181999118791... |
709.094 | Coherent network analysis for triggered gravitational wave burst
searches | Searches for gravitational wave bursts that are triggered by the observation
of astronomical events require a different mode of analysis than all-sky, blind
searches. For one, much more prior information is usually available in a
triggered search which can and should be used in the analysis. Second, since
the data vo... | gr-qc | searches for gravitational wave bursts that are triggered by the observation of astronomical events require a different mode of analysis than allsky blind searches for one much more prior information is usually available in a triggered search which can and should be used in the analysis second since the data volume is ... | [['searches', 'for', 'gravitational', 'wave', 'bursts', 'that', 'are', 'triggered', 'by', 'the', 'observation', 'of', 'astronomical', 'events', 'require', 'a', 'different', 'mode', 'of', 'analysis', 'than', 'allsky', 'blind', 'searches', 'for', 'one', 'much', 'more', 'prior', 'information', 'is', 'usually', 'available'... | [-0.09012925557525063, 0.10098778186178704, -0.09848733873705762, 0.131768302550691, -0.13813146099072787, -0.11259906016680044, 0.07499755204514448, 0.37567102325026147, -0.2141689561422943, -0.3645602831862463, 0.17392258191131085, -0.2898324698772888, -0.11443409010183153, 0.2693926022305016, 6.225036616011183e-05, ... |
709.0941 | Ettore Majorana's Inaugural Lecture on Theoretical Physics (Naples,
Italy; Jan.13, 1938) | Ettore Majorana was a member of Enrico Fermi's research group in Rome, Italy.
Fermi did regard Majorana as much brihter than himself as far as theoretical
physics was concerned (more information can be found particularly in the
arXives' e-print physics/9810023, in Italian, and refs therein, and also in the
recent mul... | physics.hist-ph physics.ed-ph | ettore majorana was a member of enrico fermis research group in rome italy fermi did regard majorana as much brihter than himself as far as theoretical physics was concerned more information can be found particularly in the arxives eprint physics9810023 in italian and refs therein and also in the recent multilanguage a... | [['ettore', 'majorana', 'was', 'a', 'member', 'of', 'enrico', 'fermis', 'research', 'group', 'in', 'rome', 'italy', 'fermi', 'did', 'regard', 'majorana', 'as', 'much', 'brihter', 'than', 'himself', 'as', 'far', 'as', 'theoretical', 'physics', 'was', 'concerned', 'more', 'information', 'can', 'be', 'found', 'particularl... | [-0.037146500058118335, 0.12136259850513141, -0.1045449302840864, 0.08977546001577091, -0.13396679309469253, -0.17598741356584377, 0.06877654293190086, 0.2726648505600464, -0.14871081489536864, -0.3572795852555133, 0.103469986259616, -0.3314237400541676, -0.11045286851918822, 0.20521526697282902, -0.14538179517532476, ... |
709.0942 | Matters of Gravity, The Newsletter of the Topical Group in Gravitation
of the American Physical Society, Volume 30, Fall 2007 | GGR News:
-we hear that..., by David Garfinkle
-News from the GRG Society, by Abhay Ashtekar
-LIGO/GEO/Virgo work together, by Peter Saulson
-GWIC Ten Years on, by Stan Whitcomb
Research Briefs:
-Quasi-local energy, by Bjoern S. Schmekel
-The current status of cosmic strings, by Patrick Peter
-Gravita... | gr-qc | ggr news we hear that by david garfinkle news from the grg society by abhay ashtekar ligogeovirgo work together by peter saulson gwic ten years on by stan whitcomb research briefs quasilocal energy by bjoern s schmekel the current status of cosmic strings by patrick peter gravitational waves from mountains on neutron s... | [['ggr', 'news', 'we', 'hear', 'that', 'by', 'david', 'garfinkle', 'news', 'from', 'the', 'grg', 'society', 'by', 'abhay', 'ashtekar', 'ligogeovirgo', 'work', 'together', 'by', 'peter', 'saulson', 'gwic', 'ten', 'years', 'on', 'by', 'stan', 'whitcomb', 'research', 'briefs', 'quasilocal', 'energy', 'by', 'bjoern', 's', ... | [-0.09714121031728419, 0.1479496008788164, -0.08130230343962026, 0.024997664697386405, -0.16855044827213164, -0.06722993174936254, 0.050293917481142744, 0.19341981662744348, -0.08249581192241429, -0.4021705081993407, 0.06148880593329003, -0.35440309484908866, -0.18609195771616893, 0.196234469542505, -0.2077277323005946... |
709.0943 | On the Frobenius functor and colon ideals | In this paper we study the commutativity of the Frobenius functor and the
colon operation of two ideals for Noetherian rings of positive characteristic
$p$. New characterizations of regular rings and local UFDs are given.
| math.AC | in this paper we study the commutativity of the frobenius functor and the colon operation of two ideals for noetherian rings of positive characteristic p new characterizations of regular rings and local ufds are given | [['in', 'this', 'paper', 'we', 'study', 'the', 'commutativity', 'of', 'the', 'frobenius', 'functor', 'and', 'the', 'colon', 'operation', 'of', 'two', 'ideals', 'for', 'noetherian', 'rings', 'of', 'positive', 'characteristic', 'p', 'new', 'characterizations', 'of', 'regular', 'rings', 'and', 'local', 'ufds', 'are', 'giv... | [-0.25201787826206, -0.008074988717479366, -0.04683939553797245, 0.054262981121428314, -0.033999617876751084, -0.1612796218267509, -0.10569887235428073, 0.3228089036952172, -0.4279149613210133, -0.1325705503512706, 0.0729278395185247, -0.2296796901567307, -0.09964055280600276, 0.17294755900012596, -0.16913836640971047,... |
709.0944 | An m sin i = 24 Earth Mass Planetary Companion To The Nearby M Dwarf GJ
176 | We report the detection of a planetary companion with a minimum mass of m sin
i = 0.0771 M_Jup = 24.5 M_Earth to the nearby (d = 9.4 pc) M2.5V star GJ 176.
The star was observed as part of our M dwarf planet search at the Hobby-Eberly
Telescope (HET). The detection is based on 5 years of high-precision
differential r... | astro-ph | we report the detection of a planetary companion with a minimum mass of m sin i 00771 m_jup 245 m_earth to the nearby d 94 pc m25v star gj 176 the star was observed as part of our m dwarf planet search at the hobbyeberly telescope het the detection is based on 5 years of highprecision differential radial velocity rv me... | [['we', 'report', 'the', 'detection', 'of', 'a', 'planetary', 'companion', 'with', 'a', 'minimum', 'mass', 'of', 'm', 'sin', 'i', '00771', 'm_jup', '245', 'm_earth', 'to', 'the', 'nearby', 'd', '94', 'pc', 'm25v', 'star', 'gj', '176', 'the', 'star', 'was', 'observed', 'as', 'part', 'of', 'our', 'm', 'dwarf', 'planet', ... | [-0.18261071429311662, 0.17282583184098288, -0.02894082912875308, -0.014564473332661615, -0.15345237243297052, -0.09224741728739592, 0.13184210318298537, 0.298606690157489, -0.06944776728544068, -0.44888719862674253, 0.08351387607498031, -0.31631597657924737, -0.020008030671121207, 0.18021357368176677, -0.1094072672057... |
709.0945 | The Survival Rate of Ejected Terrestrial Planets with Moons | During planet formation, a gas giant will interact with smaller protoplanets
that stray within its sphere of gravitational influence. We investigate the
outcome of interactions between gas giants and terrestrial-sized protoplanets
with lunar-sized companions. An interaction between a giant planet and a
protoplanet bi... | astro-ph | during planet formation a gas giant will interact with smaller protoplanets that stray within its sphere of gravitational influence we investigate the outcome of interactions between gas giants and terrestrialsized protoplanets with lunarsized companions an interaction between a giant planet and a protoplanet binary ma... | [['during', 'planet', 'formation', 'a', 'gas', 'giant', 'will', 'interact', 'with', 'smaller', 'protoplanets', 'that', 'stray', 'within', 'its', 'sphere', 'of', 'gravitational', 'influence', 'we', 'investigate', 'the', 'outcome', 'of', 'interactions', 'between', 'gas', 'giants', 'and', 'terrestrialsized', 'protoplanets... | [-0.13424822882245577, 0.17290581672067948, -0.05497618450290458, 0.06115614720457775, -0.11303874595458945, -0.012088079020640878, 0.044044884573668244, 0.3405388899667319, -0.21298961144936987, -0.35418606655628876, 0.0888998000395246, -0.2903579021132616, -0.08195428647490781, 0.21693279874770968, -0.042152575913513... |
709.0946 | The Warm Spitzer Mission: Prospects for Studies of the Distant Universe | IRAC excels at detecting distant objects. Due to a combination of the shapes
of the spectral energy distributions of galaxies and the low background
achieved from space, IRAC reaches greater depth in comparable exposure time at
3.6 and 4.5 micron than any ground- or space-based facility currently can at
2.2 micron. F... | astro-ph | irac excels at detecting distant objects due to a combination of the shapes of the spectral energy distributions of galaxies and the low background achieved from space irac reaches greater depth in comparable exposure time at 36 and 45 micron than any ground or spacebased facility currently can at 22 micron furthermore... | [['irac', 'excels', 'at', 'detecting', 'distant', 'objects', 'due', 'to', 'a', 'combination', 'of', 'the', 'shapes', 'of', 'the', 'spectral', 'energy', 'distributions', 'of', 'galaxies', 'and', 'the', 'low', 'background', 'achieved', 'from', 'space', 'irac', 'reaches', 'greater', 'depth', 'in', 'comparable', 'exposure'... | [-0.046850348156814894, 0.13301684887393223, -0.06462498236679518, 0.0785387736429131, -0.08421112236411031, -0.07030306197171712, 0.05705684911505719, 0.41502335416896713, -0.1924138673131457, -0.3943172684505922, 0.08794866119442372, -0.2905006529940398, -0.027607343479204825, 0.1890550978133492, -0.01971313752191488... |
709.0947 | A search for CO+ in planetary nebulae | We have carried out a systematic search for the molecular ion CO+ in a sample
of 8 protoplanetary and planetary nebulae in order to determine the origin of
the unexpectedly strong HCO+ emission previously detected in these sources. An
understanding of the HCO+ chemistry may provide direct clues to the physical
and ch... | astro-ph | we have carried out a systematic search for the molecular ion co in a sample of 8 protoplanetary and planetary nebulae in order to determine the origin of the unexpectedly strong hco emission previously detected in these sources an understanding of the hco chemistry may provide direct clues to the physical and chemical... | [['we', 'have', 'carried', 'out', 'a', 'systematic', 'search', 'for', 'the', 'molecular', 'ion', 'co', 'in', 'a', 'sample', 'of', '8', 'protoplanetary', 'and', 'planetary', 'nebulae', 'in', 'order', 'to', 'determine', 'the', 'origin', 'of', 'the', 'unexpectedly', 'strong', 'hco', 'emission', 'previously', 'detected', '... | [-0.047474099078068606, 0.0554426831956095, -0.017995577592611018, 0.042596672122415746, -0.03897384856092302, -0.03438845223894245, 0.04632714700296913, 0.4439722728572394, -0.20421473599088036, -0.33484593102414356, 0.001148899232870654, -0.22025549509317466, -0.062123825077555685, 0.16542861151607022, 0.075561649068... |
709.0948 | QUBIT4MATLAB V3.0: A program package for quantum information science and
quantum optics for MATLAB | A program package for MATLAB is introduced that helps calculations in quantum
information science and quantum optics. It has commands for the following
operations: (i) Reordering the qudits of a quantum register, computing the
reduced state of a quantum register. (ii) Defining important quantum states
easily. (iii) F... | quant-ph | a program package for matlab is introduced that helps calculations in quantum information science and quantum optics it has commands for the following operations i reordering the qudits of a quantum register computing the reduced state of a quantum register ii defining important quantum states easily iii formatted inpu... | [['a', 'program', 'package', 'for', 'matlab', 'is', 'introduced', 'that', 'helps', 'calculations', 'in', 'quantum', 'information', 'science', 'and', 'quantum', 'optics', 'it', 'has', 'commands', 'for', 'the', 'following', 'operations', 'i', 'reordering', 'the', 'qudits', 'of', 'a', 'quantum', 'register', 'computing', '... | [-0.1339717800443878, 0.2348149220877308, -0.02167428997155203, 0.032118983674860956, -0.012841181002785357, -0.29567634297727263, 0.047723509566098145, 0.32333890610963717, -0.29017990324361137, -0.23677743891995323, 0.08737197603284362, -0.2807300793843306, -0.12917089881375432, 0.171898420503344, -0.0317018122497793... |
709.0949 | The nearby young visual binary HIP 115147 and its common proper motion
companion LSPM J2322+7847 | We report a late M-type, common proper motion companion to a nearby young
visual binary HIP 115147 (V368 Cep), separated by 963 arcseconds from the
primary K0 dwarf. This optically dim star has been identified as a candidate
high proper motion, nearby dwarf LSPM J2322+7847 by L{\'e}pine in 2005. The
wide companion is... | astro-ph | we report a late mtype common proper motion companion to a nearby young visual binary hip 115147 v368 cep separated by 963 arcseconds from the primary k0 dwarf this optically dim star has been identified as a candidate high proper motion nearby dwarf lspm j23227847 by lepine in 2005 the wide companion is one of the lat... | [['we', 'report', 'a', 'late', 'mtype', 'common', 'proper', 'motion', 'companion', 'to', 'a', 'nearby', 'young', 'visual', 'binary', 'hip', '115147', 'v368', 'cep', 'separated', 'by', '963', 'arcseconds', 'from', 'the', 'primary', 'k0', 'dwarf', 'this', 'optically', 'dim', 'star', 'has', 'been', 'identified', 'as', 'a'... | [-0.06649525958902328, 0.10714699833351336, -0.09955408351768734, 0.053481262495331944, -0.17000763180108064, -0.10957445317114092, 0.10766723633456121, 0.4216921089326809, -0.15642864907614198, -0.35866259201281486, 0.052763302096426726, -0.312368553001315, 0.01119934412603308, 0.17840632556116054, -0.1924029655979240... |
709.095 | Cosmic Strings from Supersymmetric Flat Directions | Flat directions are a generic feature of the scalar potential in
supersymmetric gauge field theories. They can arise, for example, from D-terms
associated with an extra abelian gauge symmetry. Even when supersymmetry is
broken softly, there often remain directions in the scalar field space along
which the potential i... | hep-ph astro-ph hep-th | flat directions are a generic feature of the scalar potential in supersymmetric gauge field theories they can arise for example from dterms associated with an extra abelian gauge symmetry even when supersymmetry is broken softly there often remain directions in the scalar field space along which the potential is almost... | [['flat', 'directions', 'are', 'a', 'generic', 'feature', 'of', 'the', 'scalar', 'potential', 'in', 'supersymmetric', 'gauge', 'field', 'theories', 'they', 'can', 'arise', 'for', 'example', 'from', 'dterms', 'associated', 'with', 'an', 'extra', 'abelian', 'gauge', 'symmetry', 'even', 'when', 'supersymmetry', 'is', 'bro... | [-0.1787622854855851, 0.25443992681228444, -0.06440518805000962, 0.17609597039986083, -0.10489256026493943, -0.1321270243691591, -0.01719648324343193, 0.3477977426905726, -0.22613883523756048, -0.3027813286211095, 0.07554573787607126, -0.2764233406314738, -0.07509264488740322, 0.1545801764039689, 0.014390072096775994, ... |
709.0951 | Three-Dimensional Simulations of Inflows Irradiated by a Precessing
Accretion Disk in Active Galactic Nuclei: Formation of Outflows | We present three-dimensional (3-D) hydrodynamical simulations of gas flows in
the vicinity of an active galactic nucleus (AGN) powered by a precessing
accretion disk. We consider the effects of the radiation force from such a disk
on its environment on a relatively large scale (up to ~10 pc. We implicitly
include the... | astro-ph | we present threedimensional 3d hydrodynamical simulations of gas flows in the vicinity of an active galactic nucleus agn powered by a precessing accretion disk we consider the effects of the radiation force from such a disk on its environment on a relatively large scale up to 10 pc we implicitly include the precessing ... | [['we', 'present', 'threedimensional', '3d', 'hydrodynamical', 'simulations', 'of', 'gas', 'flows', 'in', 'the', 'vicinity', 'of', 'an', 'active', 'galactic', 'nucleus', 'agn', 'powered', 'by', 'a', 'precessing', 'accretion', 'disk', 'we', 'consider', 'the', 'effects', 'of', 'the', 'radiation', 'force', 'from', 'such',... | [-0.17353222652230985, 0.1353747163387314, -0.04586716969855703, 0.010638717807327898, -0.07481789335083121, -0.06509966329456522, 0.0020318186447884027, 0.38972179379600747, -0.27204833094938063, -0.29643174244616277, 0.0900124001846192, -0.24256482265698603, -0.015444329244872698, 0.17592181713523294, -0.015072818379... |
709.0952 | Measuring AGN Feedback with the Sunyaev-Zel'dovich Effect | One of the most important and poorly-understood issues in structure formation
is the role of outflows driven by active galactic nuclei (AGN). Using
large-scale cosmological simulations, we compute the impact of such outflows on
the small-scale distribution of the cosmic microwave background (CMB). Like
gravitationall... | astro-ph | one of the most important and poorlyunderstood issues in structure formation is the role of outflows driven by active galactic nuclei agn using largescale cosmological simulations we compute the impact of such outflows on the smallscale distribution of the cosmic microwave background cmb like gravitationallyheated stru... | [['one', 'of', 'the', 'most', 'important', 'and', 'poorlyunderstood', 'issues', 'in', 'structure', 'formation', 'is', 'the', 'role', 'of', 'outflows', 'driven', 'by', 'active', 'galactic', 'nuclei', 'agn', 'using', 'largescale', 'cosmological', 'simulations', 'we', 'compute', 'the', 'impact', 'of', 'such', 'outflows', ... | [-0.09223465276154456, 0.1563128903246252, -0.029997003846801817, 0.15117660074974992, -0.1473255972348852, -0.03881069034396205, -0.018754860557965002, 0.42770619427319617, -0.20126157635386335, -0.30032966209400913, 0.0385916451268713, -0.338315002138188, -0.026416948649421103, 0.23112958650453946, 0.0513124075805535... |
709.0953 | Intrinsic Structure and Kinematics of the Sub-Parsec Scale Jet of M87 | We report new results from a sub-parsec scale study of the inner jet in M87
performed at 15 GHz with the Very Long Baseline Array. We have detected a limb
brightened structure of the jet along with a faint 3 mas long counter-feature
which we also find to be limb brightened. Typical speeds of separate jet
features are... | astro-ph | we report new results from a subparsec scale study of the inner jet in m87 performed at 15 ghz with the very long baseline array we have detected a limb brightened structure of the jet along with a faint 3 mas long counterfeature which we also find to be limb brightened typical speeds of separate jet features are measu... | [['we', 'report', 'new', 'results', 'from', 'a', 'subparsec', 'scale', 'study', 'of', 'the', 'inner', 'jet', 'in', 'm87', 'performed', 'at', '15', 'ghz', 'with', 'the', 'very', 'long', 'baseline', 'array', 'we', 'have', 'detected', 'a', 'limb', 'brightened', 'structure', 'of', 'the', 'jet', 'along', 'with', 'a', 'faint... | [-0.07339598110486423, 0.11363886102222867, -0.11106321046489381, 0.09938141450195784, -0.14260801683750846, -0.12294743434646196, -0.03376708665502168, 0.48126901068514394, -0.22410239492272657, -0.3637714477075684, 0.05004377198826161, -0.2267752311282581, 0.007393596303318778, 0.21417131690804156, 0.0075649658097855... |
709.0954 | Polaron tunneling dynamics in the DNA molecule | The formation of polaron and its migration in a DNA chain are studied within
a semiclassical Peyrard-Biship-Holstein polaron model. Comparing the energetics
of the polaron system found from the quantum chemical and semiclassical
calculations, we extract the charge-phonon coupling constant for poly DNA
sequences. The ... | cond-mat.soft | the formation of polaron and its migration in a dna chain are studied within a semiclassical peyrardbishipholstein polaron model comparing the energetics of the polaron system found from the quantum chemical and semiclassical calculations we extract the chargephonon coupling constant for poly dna sequences the coupling... | [['the', 'formation', 'of', 'polaron', 'and', 'its', 'migration', 'in', 'a', 'dna', 'chain', 'are', 'studied', 'within', 'a', 'semiclassical', 'peyrardbishipholstein', 'polaron', 'model', 'comparing', 'the', 'energetics', 'of', 'the', 'polaron', 'system', 'found', 'from', 'the', 'quantum', 'chemical', 'and', 'semiclass... | [-0.13885990098296178, 0.14685426530029091, -0.012388462222935189, 0.07200765771170457, 0.032656619662330265, -0.1274103305790396, 0.09512104224081018, 0.36972709409892557, -0.28199135289926613, -0.289392322390562, -0.002975051157132146, -0.26940294652290286, -0.07272086320444941, 0.171080609078386, 0.05958268215569357... |
709.0955 | Fastest mixing Markov chain on graphs with symmetries | We show how to exploit symmetries of a graph to efficiently compute the
fastest mixing Markov chain on the graph (i.e., find the transition
probabilities on the edges to minimize the second-largest eigenvalue modulus of
the transition probability matrix). Exploiting symmetry can lead to significant
reduction in both ... | math.PR math.CO math.OC | we show how to exploit symmetries of a graph to efficiently compute the fastest mixing markov chain on the graph ie find the transition probabilities on the edges to minimize the secondlargest eigenvalue modulus of the transition probability matrix exploiting symmetry can lead to significant reduction in both the numbe... | [['we', 'show', 'how', 'to', 'exploit', 'symmetries', 'of', 'a', 'graph', 'to', 'efficiently', 'compute', 'the', 'fastest', 'mixing', 'markov', 'chain', 'on', 'the', 'graph', 'ie', 'find', 'the', 'transition', 'probabilities', 'on', 'the', 'edges', 'to', 'minimize', 'the', 'secondlargest', 'eigenvalue', 'modulus', 'of'... | [-0.12081113008620298, 0.06678368658050085, -0.041083439237073714, 0.08496621823262261, -0.10778856694941287, -0.10776386804797727, 0.07620622544731621, 0.40681281928782875, -0.2871430423191708, -0.3117104751462846, 0.1287955128689013, -0.2749343750284701, -0.17643167584446137, 0.1491305171046406, -0.030141984123696126... |
709.0956 | The gas density around SN 1006 | The density of the ambient medium where the supernova remnant evolves is a
relevant parameter for its hydrodynamical evolution, for the mechanism of
particle acceleration, and for the emission at TeV energies. Using XMM-Newton
X-ray observations, we present a study of the ambient medium density of the
historical supe... | astro-ph | the density of the ambient medium where the supernova remnant evolves is a relevant parameter for its hydrodynamical evolution for the mechanism of particle acceleration and for the emission at tev energies using xmmnewton xray observations we present a study of the ambient medium density of the historical supernova re... | [['the', 'density', 'of', 'the', 'ambient', 'medium', 'where', 'the', 'supernova', 'remnant', 'evolves', 'is', 'a', 'relevant', 'parameter', 'for', 'its', 'hydrodynamical', 'evolution', 'for', 'the', 'mechanism', 'of', 'particle', 'acceleration', 'and', 'for', 'the', 'emission', 'at', 'tev', 'energies', 'using', 'xmmne... | [-0.0792553448740956, 0.13228059087360147, -0.07701588040145561, 0.0828927546200819, -0.07261295040145285, -0.032465570631559734, 0.020578604085955684, 0.3930130091950644, -0.19795002567747882, -0.2980770383087933, 0.06869205209072823, -0.2883806394597212, 0.02421861988051917, 0.15029576927010158, 0.015385478362373379,... |
709.0957 | Counting and Locating the Solutions of Polynomial Systems of Maximum
Likelihood Equations, II: The Behrens-Fisher Problem | Let $\mu$ be a $p$-dimensional vector, and let $\Sigma_1$ and $\Sigma_2$ be
$p \times p$ positive definite covariance matrices. On being given random
samples of sizes $N_1$ and $N_2$ from independent multivariate normal
populations $N_p(\mu,\Sigma_1)$ and $N_p(\mu,\Sigma_2)$, respectively, the
Behrens-Fisher problem ... | math.ST math.AG stat.CO stat.TH | let mu be a pdimensional vector and let sigma_1 and sigma_2 be p times p positive definite covariance matrices on being given random samples of sizes n_1 and n_2 from independent multivariate normal populations n_pmusigma_1 and n_pmusigma_2 respectively the behrensfisher problem is to solve the likelihood equations for... | [['let', 'mu', 'be', 'a', 'pdimensional', 'vector', 'and', 'let', 'sigma_1', 'and', 'sigma_2', 'be', 'p', 'times', 'p', 'positive', 'definite', 'covariance', 'matrices', 'on', 'being', 'given', 'random', 'samples', 'of', 'sizes', 'n_1', 'and', 'n_2', 'from', 'independent', 'multivariate', 'normal', 'populations', 'n_pm... | [-0.13346981620330603, 0.14661928155211681, -0.029417187539399217, 0.07530449710705173, -0.01245545647149786, -0.20771645476033382, 0.0027986881985337638, 0.36451548307177123, -0.2889082493311768, -0.25804011073014743, 0.10849432687065777, -0.32356385324457915, -0.09397225843052542, 0.15056217619892928, -0.010337304776... |
709.0958 | Spectroscopy and Strong Decays of Charmed Baryons | Spectroscopy and strong decays of the charmed baryons are reviewed. Possible
spin-parity quantum numbers of several newly observed charmed baryon resonances
are discussed. Strong decays of charmed baryons are analyzed in the framework
of heavy hadron chiral perturbation theory in which heavy quark symmetry and
chiral... | hep-ph hep-ex | spectroscopy and strong decays of the charmed baryons are reviewed possible spinparity quantum numbers of several newly observed charmed baryon resonances are discussed strong decays of charmed baryons are analyzed in the framework of heavy hadron chiral perturbation theory in which heavy quark symmetry and chiral symm... | [['spectroscopy', 'and', 'strong', 'decays', 'of', 'the', 'charmed', 'baryons', 'are', 'reviewed', 'possible', 'spinparity', 'quantum', 'numbers', 'of', 'several', 'newly', 'observed', 'charmed', 'baryon', 'resonances', 'are', 'discussed', 'strong', 'decays', 'of', 'charmed', 'baryons', 'are', 'analyzed', 'in', 'the', ... | [-0.1262643106794935, 0.40424803100830436, -0.04581146886838334, 0.2262086496897498, -0.07017324663394568, -0.16736176442735048, 0.024397025652210778, 0.299094753643992, -0.1516136141607956, -0.19638576407973862, -0.10491710021730741, -0.41679067786174767, 0.05527931223718487, -0.006700985741858579, 0.17390205908794792... |
709.0959 | The Morse-Bott inequalities via dynamical systems | Let $f:M \to \mathbb{R}$ be a Morse-Bott function on a compact smooth finite
dimensional manifold $M$. The polynomial Morse inequalities and an explicit
perturbation of $f$ defined using Morse functions $f_j$ on the critical
submanifolds $C_j$ of $f$ show immediately that $MB_t(f) = P_t(M) + (1+t)R(t)$,
where $MB_t(f... | math.AT math.DG math.DS | let fm to mathbbr be a morsebott function on a compact smooth finite dimensional manifold m the polynomial morse inequalities and an explicit perturbation of f defined using morse functions f_j on the critical submanifolds c_j of f show immediately that mb_tf p_tm 1trt where mb_tf is the morsebott polynomial of f and p... | [['let', 'fm', 'to', 'mathbbr', 'be', 'a', 'morsebott', 'function', 'on', 'a', 'compact', 'smooth', 'finite', 'dimensional', 'manifold', 'm', 'the', 'polynomial', 'morse', 'inequalities', 'and', 'an', 'explicit', 'perturbation', 'of', 'f', 'defined', 'using', 'morse', 'functions', 'f_j', 'on', 'the', 'critical', 'subma... | [-0.22723571674873097, 0.10849726119802752, -0.06863655243068933, 0.022919283960348095, -0.03875936272182829, -0.16878453552773273, -0.00913315371065904, 0.3332312153023038, -0.2941917059565517, -0.19733500327896075, 0.06610190610926775, -0.278630082901391, -0.15389217210404976, 0.1814733132959117, -0.04452015740822095... |
709.096 | Exact edge singularities and dynamical correlations in spin-1/2 chains | Exact formulas for the singularities of the dynamical structure factor,
S^{zz}(q,omega), of the S=1/2 xxz spin chain at all q and any anisotropy and
magnetic field in the critical regime are derived, expressing the exponents in
terms of the phase shifts which are known exactly from the Bethe ansatz
solution. We also ... | cond-mat.str-el | exact formulas for the singularities of the dynamical structure factor szzqomega of the s12 xxz spin chain at all q and any anisotropy and magnetic field in the critical regime are derived expressing the exponents in terms of the phase shifts which are known exactly from the bethe ansatz solution we also study the long... | [['exact', 'formulas', 'for', 'the', 'singularities', 'of', 'the', 'dynamical', 'structure', 'factor', 'szzqomega', 'of', 'the', 's12', 'xxz', 'spin', 'chain', 'at', 'all', 'q', 'and', 'any', 'anisotropy', 'and', 'magnetic', 'field', 'in', 'the', 'critical', 'regime', 'are', 'derived', 'expressing', 'the', 'exponents',... | [-0.1764965756947911, 0.14058580685428582, -0.06186833385876272, 0.10510573962291833, -0.02819205246064379, -0.1179568970611124, 0.026475943535631305, 0.3614378614353861, -0.2419315984494291, -0.2683151762196144, 0.10016766307214925, -0.28142811284335545, -0.10359260387891947, 0.18321035724841558, 0.09537850989135074, ... |
709.0961 | A New Distributed Topology Control Algorithm for Wireless Environments
with Non-Uniform Path Loss and Multipath Propagation | Each node in a wireless multi-hop network can adjust the power level at which
it transmits and thus change the topology of the network to save energy by
choosing the neighbors with which it directly communicates. Many previous
algorithms for distributed topology control have assumed an ability at each
node to deduce ... | cs.NI | each node in a wireless multihop network can adjust the power level at which it transmits and thus change the topology of the network to save energy by choosing the neighbors with which it directly communicates many previous algorithms for distributed topology control have assumed an ability at each node to deduce some... | [['each', 'node', 'in', 'a', 'wireless', 'multihop', 'network', 'can', 'adjust', 'the', 'power', 'level', 'at', 'which', 'it', 'transmits', 'and', 'thus', 'change', 'the', 'topology', 'of', 'the', 'network', 'to', 'save', 'energy', 'by', 'choosing', 'the', 'neighbors', 'with', 'which', 'it', 'directly', 'communicates',... | [-0.15805746072152327, 0.04744609438759236, -0.05111241899246696, 0.036734310677505135, -0.11527940553333242, -0.17899497834737357, 0.10906251952035552, 0.42342368189453444, -0.3079620855068972, -0.3463169086815167, 0.07590136071160922, -0.262421135174059, -0.17068242529069402, 0.1715149969035546, -0.12003073762373431,... |
709.0962 | An Estimation of the Gamma-Ray Burst Afterglow Apparent Optical
Brightness Distribution Function | By using recent publicly available observational data obtained in conjunction
with the NASA Swift gamma-ray burst mission and a novel data analysis
technique, we have been able to make some rough estimates of the GRB afterglow
apparent optical brightness distribution function. The results suggest that 71%
of all burs... | astro-ph | by using recent publicly available observational data obtained in conjunction with the nasa swift gammaray burst mission and a novel data analysis technique we have been able to make some rough estimates of the grb afterglow apparent optical brightness distribution function the results suggest that 71 of all burst afte... | [['by', 'using', 'recent', 'publicly', 'available', 'observational', 'data', 'obtained', 'in', 'conjunction', 'with', 'the', 'nasa', 'swift', 'gammaray', 'burst', 'mission', 'and', 'a', 'novel', 'data', 'analysis', 'technique', 'we', 'have', 'been', 'able', 'to', 'make', 'some', 'rough', 'estimates', 'of', 'the', 'grb'... | [-0.04133794172269891, 0.06763917587105503, -0.12067110972955476, 0.13133695152274139, -0.13648915993475694, -0.11117418756159816, 0.05888682213438631, 0.46832671675239074, -0.20828445175980298, -0.3904418215307212, 0.1153255973079841, -0.3398285644461018, -0.055626183582195475, 0.2775703719275635, -0.03937262842114004... |
709.0963 | Enhanced sensitivity to variation of $m_{e}/m_{p}$ in molecular spectra | We propose new experiments with high sensitivity to a possible spatial or
temporal variation of the electron-to-proton mass ratio $\mu \equiv m_e/m_p$.
We consider a nearly-degenerate pair of molecular vibrational levels, where
each state is associated with a different electronic potential. The change in
the splittin... | physics.atom-ph | we propose new experiments with high sensitivity to a possible spatial or temporal variation of the electrontoproton mass ratio mu equiv m_em_p we consider a nearlydegenerate pair of molecular vibrational levels where each state is associated with a different electronic potential the change in the splitting between suc... | [['we', 'propose', 'new', 'experiments', 'with', 'high', 'sensitivity', 'to', 'a', 'possible', 'spatial', 'or', 'temporal', 'variation', 'of', 'the', 'electrontoproton', 'mass', 'ratio', 'mu', 'equiv', 'm_em_p', 'we', 'consider', 'a', 'nearlydegenerate', 'pair', 'of', 'molecular', 'vibrational', 'levels', 'where', 'eac... | [-0.14336970791471407, 0.1760759961248718, 0.01371694636495354, 0.05029056105782869, 0.01833227191057701, -0.11064181853166352, 0.06532522783919166, 0.40124691859818995, -0.2678765922677345, -0.33618147340166615, 0.020043704984485745, -0.257248068604475, -0.04486030831601685, 0.13394036734825931, -0.004464220676499491,... |
709.0964 | Computing quantum phase transitions | This article first gives a concise introduction to quantum phase transitions,
emphasizing similarities with and differences to classical thermal transitions.
After pointing out the computational challenges posed by quantum phase
transitions, a number of successful computational approaches is discussed. The
focus is o... | cond-mat.stat-mech cond-mat.str-el | this article first gives a concise introduction to quantum phase transitions emphasizing similarities with and differences to classical thermal transitions after pointing out the computational challenges posed by quantum phase transitions a number of successful computational approaches is discussed the focus is on clas... | [['this', 'article', 'first', 'gives', 'a', 'concise', 'introduction', 'to', 'quantum', 'phase', 'transitions', 'emphasizing', 'similarities', 'with', 'and', 'differences', 'to', 'classical', 'thermal', 'transitions', 'after', 'pointing', 'out', 'the', 'computational', 'challenges', 'posed', 'by', 'quantum', 'phase', '... | [-0.08967587125215043, 0.15618234902773642, -0.05601128714624792, 0.06992948245081096, -0.03428778136376201, -0.18501966730577918, 0.08601084004849105, 0.33709119042245356, -0.25677198058039674, -0.29281128807811113, 0.11366048838273145, -0.3056772543094689, -0.18424990496075735, 0.2125086206488493, -0.0508287181657534... |
709.0965 | The Induced Bounded-Degree Subgraph Problem and Stream Control in MIMO
Networks | In this report, we consider maximal solutions to the induced bounded-degree
subgraph problem and relate it to issues concerning stream control in
multiple-input multiple-output (MIMO) networks. We present a new distributed
algorithm that completes in logarithmic time with high probability and is
guaranteed to complet... | cs.NI | in this report we consider maximal solutions to the induced boundeddegree subgraph problem and relate it to issues concerning stream control in multipleinput multipleoutput mimo networks we present a new distributed algorithm that completes in logarithmic time with high probability and is guaranteed to complete in line... | [['in', 'this', 'report', 'we', 'consider', 'maximal', 'solutions', 'to', 'the', 'induced', 'boundeddegree', 'subgraph', 'problem', 'and', 'relate', 'it', 'to', 'issues', 'concerning', 'stream', 'control', 'in', 'multipleinput', 'multipleoutput', 'mimo', 'networks', 'we', 'present', 'a', 'new', 'distributed', 'algorith... | [-0.24462271013539538, 0.021912896182796317, -0.012305834777142904, -0.00545113506943804, -0.08300859700531175, -0.1452329722871009, 0.08538580401234444, 0.3800018892865883, -0.2790303237940351, -0.28180378842588566, 0.09916122059962929, -0.25460985564460903, -0.20194695155098014, 0.1499903581985464, -0.143176827311822... |
709.0966 | Can giant planets form by gravitational fragmentation of discs? | Gravitational fragmentation has been proposed as a mechanism for the
formation of giant planets in close orbits around solar-type stars. However, it
is debatable whether this mechanism can function in the inner regions (R<40 AU)
of real discs. We use a newly developed method for treating the energy equation
and the e... | astro-ph | gravitational fragmentation has been proposed as a mechanism for the formation of giant planets in close orbits around solartype stars however it is debatable whether this mechanism can function in the inner regions r40 au of real discs we use a newly developed method for treating the energy equation and the equation o... | [['gravitational', 'fragmentation', 'has', 'been', 'proposed', 'as', 'a', 'mechanism', 'for', 'the', 'formation', 'of', 'giant', 'planets', 'in', 'close', 'orbits', 'around', 'solartype', 'stars', 'however', 'it', 'is', 'debatable', 'whether', 'this', 'mechanism', 'can', 'function', 'in', 'the', 'inner', 'regions', 'r4... | [-0.04537932718819786, 0.1384655561884581, -0.08249648910960261, 0.09259379755141554, -0.059820517144458886, -0.05064075190558627, 0.013698890512019939, 0.3808039876767937, -0.1740177795487705, -0.31060936143228285, 0.05081911289959516, -0.252623157225934, -0.0435694299677623, 0.16785628682203557, -0.020475408528000116... |
709.0967 | Fault Tolerance in Cellular Automata at High Fault Rates | A commonly used model for fault-tolerant computation is that of cellular
automata. The essential difficulty of fault-tolerant computation is present in
the special case of simply remembering a bit in the presence of faults, and
that is the case we treat in this paper. We are concerned with the degree (the
number of n... | math.PR | a commonly used model for faulttolerant computation is that of cellular automata the essential difficulty of faulttolerant computation is present in the special case of simply remembering a bit in the presence of faults and that is the case we treat in this paper we are concerned with the degree the number of neighbori... | [['a', 'commonly', 'used', 'model', 'for', 'faulttolerant', 'computation', 'is', 'that', 'of', 'cellular', 'automata', 'the', 'essential', 'difficulty', 'of', 'faulttolerant', 'computation', 'is', 'present', 'in', 'the', 'special', 'case', 'of', 'simply', 'remembering', 'a', 'bit', 'in', 'the', 'presence', 'of', 'fault... | [-0.1664068458564076, 0.12214290508321331, 0.006796789905140261, 0.06173148886080378, -0.019200725703256892, -0.1866635873028589, 0.0902034233042106, 0.3540626651531941, -0.24993014896103927, -0.28191186828740145, 0.1267210018117325, -0.24028167915467574, -0.18378272185286693, 0.18047264083141779, -0.11966571784845705,... |
709.0968 | Characteristics of EGRET Blazars in the VLBA Imaging and Polarimetry
Survey (VIPS) | We examine the radio properties of EGRET-detected blazars observed as part of
the VLBA Imaging and Polarimetry Survey (VIPS). VIPS has a flux limit roughly
an order of magnitude below the MOJAVE survey and most other samples that have
been used to study the properties of EGRET blazars. At lower flux levels, radio
flu... | astro-ph | we examine the radio properties of egretdetected blazars observed as part of the vlba imaging and polarimetry survey vips vips has a flux limit roughly an order of magnitude below the mojave survey and most other samples that have been used to study the properties of egret blazars at lower flux levels radio flux densit... | [['we', 'examine', 'the', 'radio', 'properties', 'of', 'egretdetected', 'blazars', 'observed', 'as', 'part', 'of', 'the', 'vlba', 'imaging', 'and', 'polarimetry', 'survey', 'vips', 'vips', 'has', 'a', 'flux', 'limit', 'roughly', 'an', 'order', 'of', 'magnitude', 'below', 'the', 'mojave', 'survey', 'and', 'most', 'other... | [-0.0720188002659511, 0.1702273824995929, -0.029325643846642796, 0.14396247513554855, -0.10257494616845664, -0.07536259214699703, 0.03881679220043503, 0.48561951496305256, -0.13807907443320255, -0.38534013502109443, 0.05730005769045466, -0.3092211626102998, 0.02342565799553464, 0.24635709366118738, 0.01997397492986417,... |
709.0969 | Chiral vibrations in the A=135 region | Chiral vibrations are studied with the RPA plus self-consistent tilted axis
cranking formalism in the A=135 region. In this method chiral vibrations appear
as a precursor to the static chiral regime. The properties of the RPA phonons
are discussed and compared to experimental data. We discuss the limits the
chiral re... | nucl-th | chiral vibrations are studied with the rpa plus selfconsistent tilted axis cranking formalism in the a135 region in this method chiral vibrations appear as a precursor to the static chiral regime the properties of the rpa phonons are discussed and compared to experimental data we discuss the limits the chiral region an... | [['chiral', 'vibrations', 'are', 'studied', 'with', 'the', 'rpa', 'plus', 'selfconsistent', 'tilted', 'axis', 'cranking', 'formalism', 'in', 'the', 'a135', 'region', 'in', 'this', 'method', 'chiral', 'vibrations', 'appear', 'as', 'a', 'precursor', 'to', 'the', 'static', 'chiral', 'regime', 'the', 'properties', 'of', 't... | [-0.14659502016027168, 0.17988006590367778, -0.056821711778897666, 0.048652873460829645, -0.039627359441385186, -0.06761798085564555, 0.038246938701847505, 0.40902692541993896, -0.20563057151719413, -0.18942638030596848, 0.012161919305197381, -0.3266645634932251, -0.10103614781662051, 0.09599520381668518, 0.05338260524... |
709.097 | A Bayesian periodogram finds evidence for three planets in HD 11964 | A Bayesian multi-planet Kepler periodogram has been developed for the
analysis of precision radial velocity data (Gregory 2005b and 2007). The
periodogram employs a parallel tempering Markov chain Monte Carlo algorithm.
The HD 11964 data (Butler et al. 2006) has been re-analyzed using 1, 2, 3 and 4
planet models. Ass... | astro-ph | a bayesian multiplanet kepler periodogram has been developed for the analysis of precision radial velocity data gregory 2005b and 2007 the periodogram employs a parallel tempering markov chain monte carlo algorithm the hd 11964 data butler et al 2006 has been reanalyzed using 1 2 3 and 4 planet models assuming that all... | [['a', 'bayesian', 'multiplanet', 'kepler', 'periodogram', 'has', 'been', 'developed', 'for', 'the', 'analysis', 'of', 'precision', 'radial', 'velocity', 'data', 'gregory', '2005b', 'and', '2007', 'the', 'periodogram', 'employs', 'a', 'parallel', 'tempering', 'markov', 'chain', 'monte', 'carlo', 'algorithm', 'the', 'hd... | [-0.12947001316416096, 0.11784126242534172, -0.07458995462058146, 0.05848308952319567, -0.07440554144923672, -0.16850823283258345, 0.034697163437258885, 0.36895591386256776, -0.17667020441024375, -0.3614813685531448, 0.11987348546079743, -0.3020737775091862, -0.07410980634994097, 0.21706343893578814, -0.050781394175019... |
709.0971 | $k$-Ribbon Fibonacci Tableaux | We extend the notion of $k$-ribbon tableaux to the Fibonacci lattice, a
differential poset defined by R. Stanley in 1975. Using this notion, we
describe an insertion algorithm that takes $k$-colored permutations to pairs of
$k$-ribbon Fibonacci tableaux of the same shape, and we demonstrate a
color-to-spin property, ... | math.CO | we extend the notion of kribbon tableaux to the fibonacci lattice a differential poset defined by r stanley in 1975 using this notion we describe an insertion algorithm that takes kcolored permutations to pairs of kribbon fibonacci tableaux of the same shape and we demonstrate a colortospin property similar to that des... | [['we', 'extend', 'the', 'notion', 'of', 'kribbon', 'tableaux', 'to', 'the', 'fibonacci', 'lattice', 'a', 'differential', 'poset', 'defined', 'by', 'r', 'stanley', 'in', '1975', 'using', 'this', 'notion', 'we', 'describe', 'an', 'insertion', 'algorithm', 'that', 'takes', 'kcolored', 'permutations', 'to', 'pairs', 'of',... | [-0.1289933907548682, 0.14306028053775102, -0.10005341819487512, 0.13121743902649122, -0.09196592797749102, -0.10360155554595761, 0.10591367826250811, 0.37659807946944895, -0.34166894493123084, -0.3136889274733571, -0.016597028156796183, -0.23992635951771474, -0.18859232199163392, 0.1390810007489143, -0.199404025145878... |
709.0972 | Electron Energy Distributions at Relativistic Shock Sites: Observational
Constraints from the Cygnus A Hotspots | We report new detections of the hotspots in Cygnus A at 4.5 and 8.0 microns
with the Spitzer Space Telescope. Together with detailed published radio
observations and synchrotron self-Compton modeling of previous X-ray
detections, we reconstruct the underlying electron energy spectra of the two
brightest hotspots (A a... | astro-ph | we report new detections of the hotspots in cygnus a at 45 and 80 microns with the spitzer space telescope together with detailed published radio observations and synchrotron selfcompton modeling of previous xray detections we reconstruct the underlying electron energy spectra of the two brightest hotspots a and d the ... | [['we', 'report', 'new', 'detections', 'of', 'the', 'hotspots', 'in', 'cygnus', 'a', 'at', '45', 'and', '80', 'microns', 'with', 'the', 'spitzer', 'space', 'telescope', 'together', 'with', 'detailed', 'published', 'radio', 'observations', 'and', 'synchrotron', 'selfcompton', 'modeling', 'of', 'previous', 'xray', 'detec... | [-0.059092480495004665, 0.1609279981364083, -0.0710329204791577, 0.14941325985182027, -0.07226493562238649, -0.10678120884452237, 0.045581105097338856, 0.4202564254353773, -0.18426448805026388, -0.3723751719916141, -0.0021069422156075076, -0.34131207378636674, -0.0002331777417181146, 0.18057800789783085, 0.034729788383... |
709.0973 | Green-Schwarz, Nambu-Goto Actions, and Cayley's Hyperdeterminant | It has been recently shown that Nambu-Goto action can be re-expressed in
terms of Cayley's hyperdeterminant with the manifest SL(2,R) X SL(2,R) X
SL(2,R) symmetry. In the present paper, we show that the same feature is shared
by Green-Schwarz sigma-model for N=2 superstring whose target space-time is
D=2+2. When its ... | hep-th | it has been recently shown that nambugoto action can be reexpressed in terms of cayleys hyperdeterminant with the manifest sl2r x sl2r x sl2r symmetry in the present paper we show that the same feature is shared by greenschwarz sigmamodel for n2 superstring whose target spacetime is d22 when its zweibein field is elimi... | [['it', 'has', 'been', 'recently', 'shown', 'that', 'nambugoto', 'action', 'can', 'be', 'reexpressed', 'in', 'terms', 'of', 'cayleys', 'hyperdeterminant', 'with', 'the', 'manifest', 'sl2r', 'x', 'sl2r', 'x', 'sl2r', 'symmetry', 'in', 'the', 'present', 'paper', 'we', 'show', 'that', 'the', 'same', 'feature', 'is', 'shar... | [-0.1670403432503359, 0.16808309254242645, -0.08627653282887318, 0.08215761717752014, -0.1155899131932018, -0.17773118449309677, -0.05898336344909152, 0.3324761145764537, -0.2022119054832218, -0.1908497412999471, 0.10023882978068861, -0.25946253241579, -0.22350537007380472, 0.07974405211739634, -0.14170406819647996, 0.... |
709.0974 | Finding Paths and Cycles in Graphs | A polynomial time algorithm which detects all paths and cycles of all lengths
in form of vertex pairs (start, finish).
| cs.DM cs.CC cs.DS math.CO | a polynomial time algorithm which detects all paths and cycles of all lengths in form of vertex pairs start finish | [['a', 'polynomial', 'time', 'algorithm', 'which', 'detects', 'all', 'paths', 'and', 'cycles', 'of', 'all', 'lengths', 'in', 'form', 'of', 'vertex', 'pairs', 'start', 'finish']] | [-0.26884347666054964, 0.2015189841389656, -0.039967842400074005, 0.026252802461385727, -0.03341757864691317, -0.1515512418700382, 0.08238490112125874, 0.36626910604536533, -0.3085414424538612, -0.2759390208637342, 0.034229639469413084, -0.26762638743966816, -0.1335250373929739, 0.19584086425602437, 0.01837175567634403... |
709.0975 | Multiloop realization of extended affine Lie algebras and Lie tori | An important theorem in the theory of infinite dimensional Lie algebras
states that any affine Kac-Moody algebra can be realized (that is to say
constructed explicitly) using loop algebras. In this paper, we consider the
corresponding problem for a class of Lie algebras called extended affine Lie
algebras (EALAs) tha... | math.RA math.RT | an important theorem in the theory of infinite dimensional lie algebras states that any affine kacmoody algebra can be realized that is to say constructed explicitly using loop algebras in this paper we consider the corresponding problem for a class of lie algebras called extended affine lie algebras ealas that general... | [['an', 'important', 'theorem', 'in', 'the', 'theory', 'of', 'infinite', 'dimensional', 'lie', 'algebras', 'states', 'that', 'any', 'affine', 'kacmoody', 'algebra', 'can', 'be', 'realized', 'that', 'is', 'to', 'say', 'constructed', 'explicitly', 'using', 'loop', 'algebras', 'in', 'this', 'paper', 'we', 'consider', 'the... | [-0.17043045430643242, 0.0904870097133738, -0.047036827037125147, 0.10003579194916995, -0.13961016004620733, -0.16047181939094804, -0.04543029954514772, 0.39848466076753064, -0.33809749332775596, -0.20595793081300853, 0.15726520355083476, -0.15669844316617224, -0.1789962238425972, 0.2424001357169779, -0.170196912358052... |
709.0976 | Multifractal regime transition in a modified minority game model | The search for more realistic modeling of financial time series reveals
several stylized facts of real markets. In this work we focus on the
multifractal properties found in price and index signals. Although the usual
Minority Game (MG) models do not exhibit multifractality, we study here one of
its variants that doe... | q-fin.TR physics.soc-ph | the search for more realistic modeling of financial time series reveals several stylized facts of real markets in this work we focus on the multifractal properties found in price and index signals although the usual minority game mg models do not exhibit multifractality we study here one of its variants that does we sh... | [['the', 'search', 'for', 'more', 'realistic', 'modeling', 'of', 'financial', 'time', 'series', 'reveals', 'several', 'stylized', 'facts', 'of', 'real', 'markets', 'in', 'this', 'work', 'we', 'focus', 'on', 'the', 'multifractal', 'properties', 'found', 'in', 'price', 'and', 'index', 'signals', 'although', 'the', 'usual... | [-0.07982841791732319, 0.07215698788914938, -0.15258213819470257, 0.13262820926662672, -0.03524166052503621, -0.11081172304436811, 0.03904769675436375, 0.41279051803490696, -0.2863719764864072, -0.24511829942382654, 0.08092251884655151, -0.2946599826648119, -0.22560957721297575, 0.21218914716412066, -0.0220879292858572... |
709.0977 | Frustration-driven successive metamagnetic transitions in TbB4 | Resonant magnetic x-ray diffraction experiments on the Shastry-Sutherland
lattice TbB$_4$ were carried out under strong pulsed magnetic fields up to 30
T. TbB$_4$ exhibits a multi-step magnetization process above 16 T when magnetic
fields are applied along the c-axis. We examined the intensity of the 010
magnetic ref... | cond-mat.other cond-mat.mtrl-sci | resonant magnetic xray diffraction experiments on the shastrysutherland lattice tbb_4 were carried out under strong pulsed magnetic fields up to 30 t tbb_4 exhibits a multistep magnetization process above 16 t when magnetic fields are applied along the caxis we examined the intensity of the 010 magnetic reflection as a... | [['resonant', 'magnetic', 'xray', 'diffraction', 'experiments', 'on', 'the', 'shastrysutherland', 'lattice', 'tbb_4', 'were', 'carried', 'out', 'under', 'strong', 'pulsed', 'magnetic', 'fields', 'up', 'to', '30', 't', 'tbb_4', 'exhibits', 'a', 'multistep', 'magnetization', 'process', 'above', '16', 't', 'when', 'magnet... | [-0.18316080865784073, 0.246014016473947, -0.019583813582529436, 0.05232363152886394, -0.06050257486475737, -0.10697472436828012, 0.0686099360222524, 0.4424483957788292, -0.27788425200917527, -0.3239237116474026, 0.027216140772787115, -0.25529905186772767, -0.06759433374072443, 0.23264426043705205, 0.07642743651939661,... |
709.0978 | Cyclotron modeling phase-resolved infrared spectroscopy of polars I: EF
Eridani | We present phase-resolved low resolution infrared spectra of the polar EF
Eridani obtained over a period of 2 years with SPEX on the IRTF. The spectra,
covering the wavelength range 0.8 to 2.4 microns, are dominated by cyclotron
emission at all phases. We use a ``Constant Lambda'' prescription to attempt to
model the... | astro-ph | we present phaseresolved low resolution infrared spectra of the polar ef eridani obtained over a period of 2 years with spex on the irtf the spectra covering the wavelength range 08 to 24 microns are dominated by cyclotron emission at all phases we use a constant lambda prescription to attempt to model the changing cyc... | [['we', 'present', 'phaseresolved', 'low', 'resolution', 'infrared', 'spectra', 'of', 'the', 'polar', 'ef', 'eridani', 'obtained', 'over', 'a', 'period', 'of', '2', 'years', 'with', 'spex', 'on', 'the', 'irtf', 'the', 'spectra', 'covering', 'the', 'wavelength', 'range', '08', 'to', '24', 'microns', 'are', 'dominated', ... | [-0.060189671871355835, 0.08876953531814959, -0.08565756362966365, 0.04718613483580864, -0.04963926322525367, -0.1564301514519482, 0.02910735537103998, 0.44585322592821386, -0.20851721904344028, -0.36617503907117577, 0.046536471891320416, -0.3033389197145071, -0.04211843207000735, 0.19156256070386413, -0.02272022789079... |
709.0979 | Rare Semileptonic Decays of Heavy Mesons with Flavor SU(3) Symmetry | In this paper, we calculate the decay rates of $D^+ \to D^0 e^+ \nu$, $D^+_S
\to D^0 e^+ \nu$, $B^0_S \to B^+ e^- \bar{\nu}$, $D^+_S \to D^+ e^- e^+$ and
$B^0_S \to B^0 e^-e^+$ semileptonic decay processes, in which only the light
quarks decay, while the heavy flavors remain unchanged. The branching ratios of
these d... | hep-ph | in this paper we calculate the decay rates of d to d0 e nu d_s to d0 e nu b0_s to b e barnu d_s to d e e and b0_s to b0 ee semileptonic decay processes in which only the light quarks decay while the heavy flavors remain unchanged the branching ratios of these decay processes are calculated with the flavor su3 symmetry ... | [['in', 'this', 'paper', 'we', 'calculate', 'the', 'decay', 'rates', 'of', 'd', 'to', 'd0', 'e', 'nu', 'd_s', 'to', 'd0', 'e', 'nu', 'b0_s', 'to', 'b', 'e', 'barnu', 'd_s', 'to', 'd', 'e', 'e', 'and', 'b0_s', 'to', 'b0', 'ee', 'semileptonic', 'decay', 'processes', 'in', 'which', 'only', 'the', 'light', 'quarks', 'decay... | [-0.0812259323372148, 0.2915083197793657, -0.03602145346979212, 0.10583565352031396, -0.005271991881142769, -0.1577618666591921, 0.10564106082685092, 0.2799861221906862, -0.23727715615781822, -0.21016927311679215, -0.013461950485569625, -0.3766283100703731, 0.03515795599326209, 0.11929986543379657, 0.11020759050318572,... |
709.098 | The Minimally Tuned Minimal Supersymmetric Standard Model | The regions in the Minimal Supersymmetric Standard Model with the minimal
amount of fine-tuning of electroweak symmetry breaking are presented for
general messenger scale. No a priori relations among the soft supersymmetry
breaking parameters are assumed and fine-tuning is minimized with respect to
all the important ... | hep-ph | the regions in the minimal supersymmetric standard model with the minimal amount of finetuning of electroweak symmetry breaking are presented for general messenger scale no a priori relations among the soft supersymmetry breaking parameters are assumed and finetuning is minimized with respect to all the important param... | [['the', 'regions', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'with', 'the', 'minimal', 'amount', 'of', 'finetuning', 'of', 'electroweak', 'symmetry', 'breaking', 'are', 'presented', 'for', 'general', 'messenger', 'scale', 'no', 'a', 'priori', 'relations', 'among', 'the', 'soft', 'supersymmetry', '... | [-0.1083920610859534, 0.3195949065052353, 0.043034816065765154, 0.16711908559509725, -0.10528168123814144, -0.17281174519793036, 0.020800724530554548, 0.3336212508408923, -0.24790364758548689, -0.4105226397876656, 0.09135937355268671, -0.2533691811793465, -0.0025776594364065298, 0.11192432011487152, 0.00414194840176401... |
709.0981 | A characterization of the rational normal curve | We give a characterization of the rational normal curve in terms of the rank
function associated to a curve.
| math.AG | we give a characterization of the rational normal curve in terms of the rank function associated to a curve | [['we', 'give', 'a', 'characterization', 'of', 'the', 'rational', 'normal', 'curve', 'in', 'terms', 'of', 'the', 'rank', 'function', 'associated', 'to', 'a', 'curve']] | [-0.19806057092194496, -0.019158328197112207, -0.16971270112614883, 0.05403564056675685, -0.07356681103671067, -0.08923161750365245, 0.0961312063430485, 0.3181154484811582, -0.2917499044223836, -0.19207142273846425, 0.09263648484269843, -0.23548359737584465, -0.21626715411088968, 0.2726221555157712, -0.1449155290856173... |
709.0982 | Detecting Cosmic Strings in the CMB with the Canny Algorithm | Line discontinuities in cosmic microwave background anisotropy maps are a
distinctive prediction of models with cosmic strings. These signatures are
visible in anisotropy maps with good angular resolution and should be
identifiable using edge detection algorithms. One such algorithm is the Canny
algorithm. We study t... | astro-ph gr-qc hep-ph hep-th | line discontinuities in cosmic microwave background anisotropy maps are a distinctive prediction of models with cosmic strings these signatures are visible in anisotropy maps with good angular resolution and should be identifiable using edge detection algorithms one such algorithm is the canny algorithm we study the po... | [['line', 'discontinuities', 'in', 'cosmic', 'microwave', 'background', 'anisotropy', 'maps', 'are', 'a', 'distinctive', 'prediction', 'of', 'models', 'with', 'cosmic', 'strings', 'these', 'signatures', 'are', 'visible', 'in', 'anisotropy', 'maps', 'with', 'good', 'angular', 'resolution', 'and', 'should', 'be', 'identi... | [-0.13349223029023657, 0.13769263252337016, -0.03771087634183156, 0.08400003137552024, -0.06659584785035501, -0.08503263096014659, -0.0033727059916903576, 0.4051260691524173, -0.27145197316228104, -0.3774735659516106, 0.07983978986546086, -0.3170754139544442, -0.056350188632495704, 0.22734279298456386, 0.02532944639873... |
709.0983 | The Luminosity Function of Low-Redshift Abell Galaxy Clusters | We present the results from a survey of 57 low-redshift Abell galaxy clusters
to study the radial dependence of the luminosity function (LF). The dynamical
radius of each cluster, r200, was estimated from the photometric measurement of
cluster richness, Bgc. The shape of the LFs are found to correlate with radius
suc... | astro-ph | we present the results from a survey of 57 lowredshift abell galaxy clusters to study the radial dependence of the luminosity function lf the dynamical radius of each cluster r200 was estimated from the photometric measurement of cluster richness bgc the shape of the lfs are found to correlate with radius such that the... | [['we', 'present', 'the', 'results', 'from', 'a', 'survey', 'of', '57', 'lowredshift', 'abell', 'galaxy', 'clusters', 'to', 'study', 'the', 'radial', 'dependence', 'of', 'the', 'luminosity', 'function', 'lf', 'the', 'dynamical', 'radius', 'of', 'each', 'cluster', 'r200', 'was', 'estimated', 'from', 'the', 'photometric'... | [-0.010856357504432711, 0.11540109286582483, -0.1376687790966534, 0.09852614500069697, -0.09004386112297534, -0.07150407735850316, 0.035315351331651756, 0.4868893909535789, -0.09139228833668209, -0.3511081178600029, 0.009250719498028519, -0.33043308047057407, -0.06714086113912374, 0.1864173730601074, -0.031176675636787... |
709.0984 | Characterization of the near-Earth Asteroid 2002NY40 | In August 2002, the near-Earth asteroid 2002 NY40, made its closest approach
to the Earth. This provided an opportunity to study a near-Earth asteroid with
a variety of instruments. Several of the telescopes at the Maui Space
Surveillance System were trained at the asteroid and collected adaptive optics
images, photo... | astro-ph | in august 2002 the nearearth asteroid 2002 ny40 made its closest approach to the earth this provided an opportunity to study a nearearth asteroid with a variety of instruments several of the telescopes at the maui space surveillance system were trained at the asteroid and collected adaptive optics images photometry and... | [['in', 'august', '2002', 'the', 'nearearth', 'asteroid', '2002', 'ny40', 'made', 'its', 'closest', 'approach', 'to', 'the', 'earth', 'this', 'provided', 'an', 'opportunity', 'to', 'study', 'a', 'nearearth', 'asteroid', 'with', 'a', 'variety', 'of', 'instruments', 'several', 'of', 'the', 'telescopes', 'at', 'the', 'mau... | [-0.07164625457953662, 0.08758076090180111, -0.1994509870710317, 0.018234837079944555, -0.07871858652215451, -0.042544548254227266, 0.0113895931863226, 0.386896510515362, -0.1911258049600292, -0.3823536459240131, 0.11857769636408193, -0.3610339789534919, -0.15284224145580083, 0.25189151221420614, -0.18156041286420077, ... |
709.0985 | Matterwave Transport Without Transit | Classically it is impossible to have transport without transit, i.e., if the
points one, two and three lie sequentially along a path then an object moving
from one to three must, at some point in time, be located at two. However, for
a quantum particle in a three-well system it is possible to transport the
particle b... | cond-mat.other physics.atom-ph quant-ph | classically it is impossible to have transport without transit ie if the points one two and three lie sequentially along a path then an object moving from one to three must at some point in time be located at two however for a quantum particle in a threewell system it is possible to transport the particle between wells... | [['classically', 'it', 'is', 'impossible', 'to', 'have', 'transport', 'without', 'transit', 'ie', 'if', 'the', 'points', 'one', 'two', 'and', 'three', 'lie', 'sequentially', 'along', 'a', 'path', 'then', 'an', 'object', 'moving', 'from', 'one', 'to', 'three', 'must', 'at', 'some', 'point', 'in', 'time', 'be', 'located'... | [-0.1287584098200768, 0.19306063700263976, -0.08801024291442888, 0.05614422557509232, 0.008558552945032716, -0.18177491081197086, 0.041221624998930874, 0.3728238903610717, -0.2727272445790288, -0.3014847213209311, 0.08607157695791456, -0.29745227159795967, -0.07759540831022782, 0.19442300927234676, -0.00122513906499967... |
709.0986 | Self-injective algebras and the second Hochschild cohomology group | In this paper we study the second Hochschild cohomology group
${HH}^2(\Lambda)$ of a finite dimensional algebra $\Lambda$. In particular, we
determine ${HH}^2(\Lambda)$ where $\Lambda$ is a finite dimensional
self-injective algebra of finite representation type over an algebraically
closed field $K$ and show that thi... | math.RT | in this paper we study the second hochschild cohomology group hh2lambda of a finite dimensional algebra lambda in particular we determine hh2lambda where lambda is a finite dimensional selfinjective algebra of finite representation type over an algebraically closed field k and show that this group is zero for most such... | [['in', 'this', 'paper', 'we', 'study', 'the', 'second', 'hochschild', 'cohomology', 'group', 'hh2lambda', 'of', 'a', 'finite', 'dimensional', 'algebra', 'lambda', 'in', 'particular', 'we', 'determine', 'hh2lambda', 'where', 'lambda', 'is', 'a', 'finite', 'dimensional', 'selfinjective', 'algebra', 'of', 'finite', 'repr... | [-0.1906584546562623, 0.10856025785434406, -0.07910172251462372, 0.023516450904549634, -0.11291710723360832, -0.15369985244857767, -0.03378035531513336, 0.3553509043783627, -0.33981004072473187, -0.133277748485632, 0.10541086406341162, -0.2031276552641595, -0.12746662209798215, 0.16836996177550068, -0.071834610669281, ... |
709.0987 | The combinatorics of associated Hermite polynomials | We develop a combinatorial model of the associated Hermite polynomials and
their moments, and prove their orthogonality with a sign-reversing involution.
We find combinatorial interpretations of the moments as complete matchings,
connected complete matchings, oscillating tableaux, and rooted maps and show
weight-pres... | math.CO | we develop a combinatorial model of the associated hermite polynomials and their moments and prove their orthogonality with a signreversing involution we find combinatorial interpretations of the moments as complete matchings connected complete matchings oscillating tableaux and rooted maps and show weightpreserving bi... | [['we', 'develop', 'a', 'combinatorial', 'model', 'of', 'the', 'associated', 'hermite', 'polynomials', 'and', 'their', 'moments', 'and', 'prove', 'their', 'orthogonality', 'with', 'a', 'signreversing', 'involution', 'we', 'find', 'combinatorial', 'interpretations', 'of', 'the', 'moments', 'as', 'complete', 'matchings',... | [-0.1776567987887369, 0.08175946938835325, -0.08811352867633104, 0.16963390131000308, -0.16575596935205883, -0.10638163077284492, 0.07824794132912141, 0.3653848972622185, -0.35726305157426863, -0.2949598567567826, 0.06611752944938358, -0.28316909345167296, -0.21311377544677065, 0.12035003982694639, -0.09972793927989833... |
709.0988 | On the Embeddability of Skeleta of Spheres | We consider a generalization of the van Kampen-Flores Theorem and relate it
to the long-standing $g$-conjecture for simplicial spheres.
| math.CO math.AT | we consider a generalization of the van kampenflores theorem and relate it to the longstanding gconjecture for simplicial spheres | [['we', 'consider', 'a', 'generalization', 'of', 'the', 'van', 'kampenflores', 'theorem', 'and', 'relate', 'it', 'to', 'the', 'longstanding', 'gconjecture', 'for', 'simplicial', 'spheres']] | [-0.09257893553493839, -0.0034601306542754173, -0.09956282671344907, 0.15079343701271633, -0.05800385537900423, -0.15645192472852373, 0.03310519760768665, 0.23292403109371662, -0.32095570141743673, -0.2430322482005546, 0.04343887756725675, -0.2915980308071563, -0.22612184678253375, 0.1929722214607816, -0.20250233493157... |
709.0989 | Trans-phonon effects in ultrafast nano-devices | We report a novel phenomenon in carbon nanotube (CNT) based devices, the
transphonon effects, which resemble the transonic effects in aerodynamics. It
is caused by dissipative resonance of nanotube phonons similar to the radial
breathing mode, and subsequent drastic surge of the dragging force on the
sliding tube, an... | cond-mat.mtrl-sci cond-mat.stat-mech | we report a novel phenomenon in carbon nanotube cnt based devices the transphonon effects which resemble the transonic effects in aerodynamics it is caused by dissipative resonance of nanotube phonons similar to the radial breathing mode and subsequent drastic surge of the dragging force on the sliding tube and multipl... | [['we', 'report', 'a', 'novel', 'phenomenon', 'in', 'carbon', 'nanotube', 'cnt', 'based', 'devices', 'the', 'transphonon', 'effects', 'which', 'resemble', 'the', 'transonic', 'effects', 'in', 'aerodynamics', 'it', 'is', 'caused', 'by', 'dissipative', 'resonance', 'of', 'nanotube', 'phonons', 'similar', 'to', 'the', 'ra... | [-0.17878607389183693, 0.23223096030522827, -0.07422521204492193, -0.029545569522191346, -0.08651936289647387, -0.15863552732669092, 0.049358941384671645, 0.3998109848686942, -0.2873865443247336, -0.2738862564488326, 0.042184912815207136, -0.2642741835587026, -0.1619927449364583, 0.2078638023806069, -0.0453820724304719... |
709.099 | Some discretizations of geometric evolution equations and the Ricci
iteration on the space of Kahler metrics, I | In this article and in its sequel we propose the study of certain
discretizations of geometric evolution equations as an approach to the study of
the existence problem of some elliptic partial differential equations of a
geometric nature as well as a means to obtain interesting dynamics on certain
infinite-dimensiona... | math.DG math.AP | in this article and in its sequel we propose the study of certain discretizations of geometric evolution equations as an approach to the study of the existence problem of some elliptic partial differential equations of a geometric nature as well as a means to obtain interesting dynamics on certain infinitedimensional s... | [['in', 'this', 'article', 'and', 'in', 'its', 'sequel', 'we', 'propose', 'the', 'study', 'of', 'certain', 'discretizations', 'of', 'geometric', 'evolution', 'equations', 'as', 'an', 'approach', 'to', 'the', 'study', 'of', 'the', 'existence', 'problem', 'of', 'some', 'elliptic', 'partial', 'differential', 'equations', ... | [-0.16782539077873324, 0.014317687618686029, -0.09575760176564317, 0.11207922093609984, -0.10041276815279228, -0.1174191991825554, -0.04140826743436841, 0.3237958520696294, -0.3056988980303087, -0.25717684882125114, 0.15491284300834396, -0.2567569466262329, -0.21155386067154566, 0.19661673580483738, -0.1442161198597537... |
709.0991 | Comments on a faint old stellar system at 150 kpc | Context.Recent study of SDSS J1257+3419 has revealed that this stellar system
is either a faint and small dwarf galaxy or a faint and widely extended
globular cluster (see also arXiv:0709.0327 [astro-ph]). Aims.In this short
note, the author suggests that this system is one of the smallest dwarf
spheroidals (dSphs) i... | astro-ph | contextrecent study of sdss j12573419 has revealed that this stellar system is either a faint and small dwarf galaxy or a faint and widely extended globular cluster see also arxiv07090327 astroph aimsin this short note the author suggests that this system is one of the smallest dwarf spheroidals dsphs in the milky way ... | [['contextrecent', 'study', 'of', 'sdss', 'j12573419', 'has', 'revealed', 'that', 'this', 'stellar', 'system', 'is', 'either', 'a', 'faint', 'and', 'small', 'dwarf', 'galaxy', 'or', 'a', 'faint', 'and', 'widely', 'extended', 'globular', 'cluster', 'see', 'also', 'arxiv07090327', 'astroph', 'aimsin', 'this', 'short', 'n... | [-0.09406858207582827, 0.0644405402239382, -0.15941910690537864, 0.14945621362177566, -0.15651803686764212, -0.05266230081343242, 0.012674356900876569, 0.36518856119965354, -0.14609245572149032, -0.36353617882536304, 0.03069370367466622, -0.28948161116380605, -0.09273947653878901, 0.22080823467225738, -0.10370946346571... |
709.0992 | Graphene nano-ribbon under tension | The mechanical response of graphene nano-ribbon under tensile loading has
been investigated using atomistic simulation. Lattice symmetry dependence of
elastic properties are found, which fits prediction from Cauchy-Born rule well.
Concurrent brittle and ductile behaviors are observed in the failure process at
elastic... | cond-mat.mtrl-sci | the mechanical response of graphene nanoribbon under tensile loading has been investigated using atomistic simulation lattice symmetry dependence of elastic properties are found which fits prediction from cauchyborn rule well concurrent brittle and ductile behaviors are observed in the failure process at elastic limit ... | [['the', 'mechanical', 'response', 'of', 'graphene', 'nanoribbon', 'under', 'tensile', 'loading', 'has', 'been', 'investigated', 'using', 'atomistic', 'simulation', 'lattice', 'symmetry', 'dependence', 'of', 'elastic', 'properties', 'are', 'found', 'which', 'fits', 'prediction', 'from', 'cauchyborn', 'rule', 'well', 'c... | [-0.09615002815490184, 0.20086276867305455, -0.07747366323567711, 0.017834058656671255, -0.05669846839568429, -0.16472459765340108, 0.0574863444932777, 0.45191782982884976, -0.30050669378344563, -0.27316823747494945, 0.03996319505656003, -0.31313712905714475, -0.13307559310688058, 0.10529098719817356, 0.044022879758984... |
709.0993 | The Description of Information in 4-Dimensional Pseudo-Euclidean
Information Space | This article is presented new method of description information systems in
abstract 4-dimensional pseudo-Euclidean information space (4-DPIES) with using
special relativity (SR) methods. This purpose core postulates of existence
4-DPIES are formulated. The theorem setting existence criteria of the invariant
velocity ... | cs.IT math.IT nlin.AO physics.soc-ph | this article is presented new method of description information systems in abstract 4dimensional pseudoeuclidean information space 4dpies with using special relativity sr methods this purpose core postulates of existence 4dpies are formulated the theorem setting existence criteria of the invariant velocity of the infor... | [['this', 'article', 'is', 'presented', 'new', 'method', 'of', 'description', 'information', 'systems', 'in', 'abstract', '4dimensional', 'pseudoeuclidean', 'information', 'space', '4dpies', 'with', 'using', 'special', 'relativity', 'sr', 'methods', 'this', 'purpose', 'core', 'postulates', 'of', 'existence', '4dpies', ... | [-0.10937167300863762, 0.08323552470008408, -0.10299930798829342, 0.09356382066516059, -0.08758674241747501, -0.1356775743744088, 0.038245546027500854, 0.32439572997531624, -0.2621951215858361, -0.31308352338365425, 0.10234761346147943, -0.2522196043200847, -0.14742322157525536, 0.18881298610519373, -0.0847838902658778... |
709.0994 | Molecular dynamics simulations of reflection and adhesion behavior in
Lennard-Jones cluster deposition | We conduct molecular dynamics simulations of the collision of atomic clusters
with a weakly-attractive surface. We focus on an intermediate regime, between
soft-landing and fragmentation, where the cluster undergoes deformation on
impact but remains largely intact, and will either adhere to the surface (and
possibly ... | cond-mat.other | we conduct molecular dynamics simulations of the collision of atomic clusters with a weaklyattractive surface we focus on an intermediate regime between softlanding and fragmentation where the cluster undergoes deformation on impact but remains largely intact and will either adhere to the surface and possibly slide or ... | [['we', 'conduct', 'molecular', 'dynamics', 'simulations', 'of', 'the', 'collision', 'of', 'atomic', 'clusters', 'with', 'a', 'weaklyattractive', 'surface', 'we', 'focus', 'on', 'an', 'intermediate', 'regime', 'between', 'softlanding', 'and', 'fragmentation', 'where', 'the', 'cluster', 'undergoes', 'deformation', 'on',... | [-0.1241015558056159, 0.19444034636629354, -0.10423475000352117, 0.021615381084672695, -0.009842307073995471, -0.09452055264545146, 0.05295842102536904, 0.3807774311511885, -0.271490721961006, -0.303306756218212, 0.03854326622141759, -0.27266307093727227, -0.13297761739091246, 0.1623736316585052, 0.004282932229522597, ... |
709.0995 | Inertial Screening in Sedimentation | We use particle image velocimetry to measure the sedimentation dynamics of a
semi-dilute suspension of non-Brownian spheres at Reynolds numbers, $0.001\le
Re\le 2.3$, extending from the Stokes to the moderately inertial regime. We
find that the onset of inertial corrections to Stokes sedimentation occurs when
the ine... | physics.flu-dyn | we use particle image velocimetry to measure the sedimentation dynamics of a semidilute suspension of nonbrownian spheres at reynolds numbers 0001le rele 23 extending from the stokes to the moderately inertial regime we find that the onset of inertial corrections to stokes sedimentation occurs when the inertial screeni... | [['we', 'use', 'particle', 'image', 'velocimetry', 'to', 'measure', 'the', 'sedimentation', 'dynamics', 'of', 'a', 'semidilute', 'suspension', 'of', 'nonbrownian', 'spheres', 'at', 'reynolds', 'numbers', '0001le', 'rele', '23', 'extending', 'from', 'the', 'stokes', 'to', 'the', 'moderately', 'inertial', 'regime', 'we',... | [-0.1316817236980528, 0.2887897448865383, -0.1035886722397101, 0.046845097225577975, 0.008264043567220816, -0.11532422138922167, -0.05269509532980705, 0.27011185997490134, -0.29748424026707, -0.2765786555200669, -0.0153398392525805, -0.289383967731441, -0.037146836585951234, 0.16153094230031365, -0.032298170134760024, ... |
709.0996 | $\Lambda d$ correlations from the $^4$He(stopped-$K^-$,$d$) reaction | We have observed an intense high-energy component in an inclusive
$^4$He(stopped $K^-$, $d$) spectrum. For back-to-back $\Lambda d$ pairs a
prominent event cluster has been found just below the
$m_{^4\textrm{He}}+m_{K^-}-m_{n}$ mass threshold in the $\Lambda d$ invariant
mass spectrum of $\Lambda dn$ events, which is... | nucl-ex | we have observed an intense highenergy component in an inclusive 4hestopped k d spectrum for backtoback lambda d pairs a prominent event cluster has been found just below the m_4textrmhem_km_n mass threshold in the lambda d invariant mass spectrum of lambda dn events which is evidence for a threenucleon absorption proc... | [['we', 'have', 'observed', 'an', 'intense', 'highenergy', 'component', 'in', 'an', 'inclusive', '4hestopped', 'k', 'd', 'spectrum', 'for', 'backtoback', 'lambda', 'd', 'pairs', 'a', 'prominent', 'event', 'cluster', 'has', 'been', 'found', 'just', 'below', 'the', 'm_4textrmhem_km_n', 'mass', 'threshold', 'in', 'the', '... | [-0.1682272703362653, 0.1731038755121529, -0.07574075559613766, 0.12238978089658599, 0.028227949297273312, -0.1408279667390728, -0.0018840670198589176, 0.38812416758049617, -0.20871326187020772, -0.2878059252715585, -0.07332112035387522, -0.3891639117780444, -0.00285740222709326, 0.13169508529585097, 0.0784643975921072... |
709.0997 | Short-time critical dynamics of the three-dimensional systems with
long-range correlated disorder | Monte Carlo simulations of the short-time dynamic behavior are reported for
three-dimensional Ising and XY models with long-range correlated disorder at
criticality, in the case corresponding to linear defects. The static and
dynamic critical exponents are determined for systems starting separately from
ordered and d... | cond-mat.dis-nn | monte carlo simulations of the shorttime dynamic behavior are reported for threedimensional ising and xy models with longrange correlated disorder at criticality in the case corresponding to linear defects the static and dynamic critical exponents are determined for systems starting separately from ordered and disorder... | [['monte', 'carlo', 'simulations', 'of', 'the', 'shorttime', 'dynamic', 'behavior', 'are', 'reported', 'for', 'threedimensional', 'ising', 'and', 'xy', 'models', 'with', 'longrange', 'correlated', 'disorder', 'at', 'criticality', 'in', 'the', 'case', 'corresponding', 'to', 'linear', 'defects', 'the', 'static', 'and', '... | [-0.11697061856587727, 0.19111377926310524, -0.07938053803001013, 0.07717137660624253, 0.06880209896610015, -0.14426476040130687, 0.019283826367205215, 0.36836945473785615, -0.20961919255658157, -0.2800004527386692, 0.05898359096609056, -0.3670793794095516, -0.12611461755198736, 0.18886150773355945, 0.11440454261998335... |
709.0998 | Teichm\"uller Spaces and Bundles with Negatively Curved Fibers | We study the Teichm\"uller space of negatively curved metrics on a high
dimensional manifold, with applications to bundles with negatively curved
fibers.
| math.DG math.GT | we study the teichmuller space of negatively curved metrics on a high dimensional manifold with applications to bundles with negatively curved fibers | [['we', 'study', 'the', 'teichmuller', 'space', 'of', 'negatively', 'curved', 'metrics', 'on', 'a', 'high', 'dimensional', 'manifold', 'with', 'applications', 'to', 'bundles', 'with', 'negatively', 'curved', 'fibers']] | [-0.1548273270441727, 0.15030327082389372, 0.015076537701216612, 0.020018931478261948, -0.06245543443682519, -0.17187110315585, -0.1141739831390706, 0.5528025308793242, -0.15888694995506245, -0.1950726073912599, 0.09925564012320881, -0.31037616987966676, -0.20898910984396935, 0.19965306034480984, -0.26910765473307535, ... |
709.0999 | Classification of Toric log Del Pezzo Surfaces having Picard Number 1
and Index $\le 3$ | Toric log Del Pezzo surfaces with Picard number 1 have been completely
classified whenever their index is $\le 2$: In this paper we extend the
classification for those having index 3: We prove that, up to isomorphism,
there are exactly 18 surfaces of this kind.
| math.AG math.CO | toric log del pezzo surfaces with picard number 1 have been completely classified whenever their index is le 2 in this paper we extend the classification for those having index 3 we prove that up to isomorphism there are exactly 18 surfaces of this kind | [['toric', 'log', 'del', 'pezzo', 'surfaces', 'with', 'picard', 'number', '1', 'have', 'been', 'completely', 'classified', 'whenever', 'their', 'index', 'is', 'le', '2', 'in', 'this', 'paper', 'we', 'extend', 'the', 'classification', 'for', 'those', 'having', 'index', '3', 'we', 'prove', 'that', 'up', 'to', 'isomorphis... | [-0.1408767994493246, 0.0787524399244123, -0.06143206435048746, 0.08130924046401762, -0.00783904381096363, -0.23294710744586256, -0.019952986407507624, 0.38479235933886635, -0.2619204714273413, -0.39877182944781253, 0.10281030432993753, -0.3309240443011125, -0.14023594027385117, 0.16177808654805023, -0.1891508693392906... |
709.1 | Measurement of the $K^+\to\pi^+\nu\bar{\nu}$ Branching Ratio | Experiment E949 at Brookhaven National Laboratory studied the rare decay
\$K^+\to\pi^+\nu\bar{\nu}$ and other processes with an exposure of $1.77\times
10^{12}$ $K^+$'s. The data were analyzed using a blind analysis technique
yielding one candidate event with an estimated background of $0.30\pm0.03$
events. Combining... | hep-ex | experiment e949 at brookhaven national laboratory studied the rare decay ktopinubarnu and other processes with an exposure of 177times 1012 ks the data were analyzed using a blind analysis technique yielding one candidate event with an estimated background of 030pm003 events combining this result with the observation o... | [['experiment', 'e949', 'at', 'brookhaven', 'national', 'laboratory', 'studied', 'the', 'rare', 'decay', 'ktopinubarnu', 'and', 'other', 'processes', 'with', 'an', 'exposure', 'of', '177times', '1012', 'ks', 'the', 'data', 'were', 'analyzed', 'using', 'a', 'blind', 'analysis', 'technique', 'yielding', 'one', 'candidate... | [-0.07459166239350452, 0.11367090844760241, -0.07317491292196791, 0.0629383723178762, -0.02833364725811407, -0.11525875448714942, 0.0847704593790695, 0.3067433983553201, -0.12884751236997544, -0.4095269273966551, 0.08689626875711838, -0.34885651846416293, -0.02622531907982193, 0.21774210356816184, 0.020281124929897486,... |
709.1001 | Tunable high-energy ion source via oblique laser pulse incidence on a
double-layer target | The laser-driven acceleration of high quality proton beams from a
double-layer target, comprised of a high-Z ion layer and a thin disk of
hydrogen, is investigated with three-dimensional particle-in-cell simulations
in the case of oblique incidence of a laser pulse. It is shown that the proton
beam energy reaches its... | physics.plasm-ph physics.acc-ph | the laserdriven acceleration of high quality proton beams from a doublelayer target comprised of a highz ion layer and a thin disk of hydrogen is investigated with threedimensional particleincell simulations in the case of oblique incidence of a laser pulse it is shown that the proton beam energy reaches its maximum at... | [['the', 'laserdriven', 'acceleration', 'of', 'high', 'quality', 'proton', 'beams', 'from', 'a', 'doublelayer', 'target', 'comprised', 'of', 'a', 'highz', 'ion', 'layer', 'and', 'a', 'thin', 'disk', 'of', 'hydrogen', 'is', 'investigated', 'with', 'threedimensional', 'particleincell', 'simulations', 'in', 'the', 'case',... | [-0.07389582554727288, 0.2405653765211658, -0.03193304090139767, 0.05322163480013842, -0.0026484824484214187, -0.12225742077134782, 0.013630440526564295, 0.4665549623314291, -0.258470559764343, -0.29515894630276307, 0.01547456245922755, -0.27193196790661506, 0.031560822625275854, 0.2344193131236049, 0.03768526406687064... |
709.1002 | Identification of shallow two-body bound states in finite volume | We discuss signatures of bound-state formation in finite volume via the
Luscher finite size method. Assuming that the phase-shift formula in this
method inherits all aspects of the quantum scattering theory, we may expect
that the bound-state formation induces the sign of the scattering length to be
changed. If it we... | hep-lat hep-ph | we discuss signatures of boundstate formation in finite volume via the luscher finite size method assuming that the phaseshift formula in this method inherits all aspects of the quantum scattering theory we may expect that the boundstate formation induces the sign of the scattering length to be changed if it were true ... | [['we', 'discuss', 'signatures', 'of', 'boundstate', 'formation', 'in', 'finite', 'volume', 'via', 'the', 'luscher', 'finite', 'size', 'method', 'assuming', 'that', 'the', 'phaseshift', 'formula', 'in', 'this', 'method', 'inherits', 'all', 'aspects', 'of', 'the', 'quantum', 'scattering', 'theory', 'we', 'may', 'expect'... | [-0.12927129469599208, 0.20448691632828955, -0.11424974020696993, 0.10969180095564275, -0.04739114488647492, -0.12352576869666393, 0.056178478210054936, 0.32465597427806553, -0.24262114354685224, -0.2433137318800652, 0.05126129887081154, -0.2602972771661977, -0.09132631191477915, 0.15954662055455515, 0.0231888536967475... |
709.1003 | Weak lensing goes bananas: What flexion really measures | In weak gravitational lensing, the image distortion caused by shear measures
the projected tidal gravitational field of the deflecting mass distribution. To
lowest order, the shear is proportional to the mean image ellipticity. If the
image sizes are not small compared to the scale over which the shear varies,
higher... | astro-ph | in weak gravitational lensing the image distortion caused by shear measures the projected tidal gravitational field of the deflecting mass distribution to lowest order the shear is proportional to the mean image ellipticity if the image sizes are not small compared to the scale over which the shear varies higherorder d... | [['in', 'weak', 'gravitational', 'lensing', 'the', 'image', 'distortion', 'caused', 'by', 'shear', 'measures', 'the', 'projected', 'tidal', 'gravitational', 'field', 'of', 'the', 'deflecting', 'mass', 'distribution', 'to', 'lowest', 'order', 'the', 'shear', 'is', 'proportional', 'to', 'the', 'mean', 'image', 'elliptici... | [-0.1295022582729443, 0.12074606745473455, -0.07689642222248949, 0.07475091776594876, -0.06165115416789537, -0.046945382420637866, -0.04636447626912473, 0.3388016381273594, -0.32815360309306174, -0.2974783917923239, 0.0802439318773823, -0.2565190951093374, -0.0991833601044217, 0.2005970629855737, -0.014297289706626222,... |
709.1004 | Measurement of focusing properties for high numerical aperture optics
using an automated submicron beamprofiler | The focusing properties of three aspheric lenses with numerical aperture (NA)
between 0.53 and 0.68 were directly measured using an interferometrically
referenced scanning knife-edge beam profiler with sub-micron resolution. The
results obtained for two of the three lenses tested were in agreement with
paraxial gauss... | physics.optics physics.ins-det | the focusing properties of three aspheric lenses with numerical aperture na between 053 and 068 were directly measured using an interferometrically referenced scanning knifeedge beam profiler with submicron resolution the results obtained for two of the three lenses tested were in agreement with paraxial gaussian beam ... | [['the', 'focusing', 'properties', 'of', 'three', 'aspheric', 'lenses', 'with', 'numerical', 'aperture', 'na', 'between', '053', 'and', '068', 'were', 'directly', 'measured', 'using', 'an', 'interferometrically', 'referenced', 'scanning', 'knifeedge', 'beam', 'profiler', 'with', 'submicron', 'resolution', 'the', 'resul... | [-0.04906539084751987, 0.08988180269322281, -0.07377881041934921, -0.006837005761169874, -0.04992250325158239, -0.1871296579639117, -0.037735659004344294, 0.49599198299563596, -0.16517089394231638, -0.37842741809371444, 0.09031860420234605, -0.28667618797885047, -0.08050349601027039, 0.27049228580047685, -0.02651041047... |
709.1005 | A dynamical system approach to inhomogeneous dust solutions | We examine numerically and qualitatively the Lema\^\i tre--Tolman--Bondi
(LTB) inhomogeneous dust solutions as a 3--dimensional dynamical system
characterized by six critical points. One of the coordinates of the phase space
is an average density parameter, $<\Omega>$, which behaves as the ordinary
$\Omega$ in Friedm... | gr-qc astro-ph math.DS nlin.SI | we examine numerically and qualitatively the lemai tretolmanbondi ltb inhomogeneous dust solutions as a 3dimensional dynamical system characterized by six critical points one of the coordinates of the phase space is an average density parameter omega which behaves as the ordinary omega in friedmanlemai trerobertsonwalk... | [['we', 'examine', 'numerically', 'and', 'qualitatively', 'the', 'lemai', 'tretolmanbondi', 'ltb', 'inhomogeneous', 'dust', 'solutions', 'as', 'a', '3dimensional', 'dynamical', 'system', 'characterized', 'by', 'six', 'critical', 'points', 'one', 'of', 'the', 'coordinates', 'of', 'the', 'phase', 'space', 'is', 'an', 'av... | [-0.18381393321628686, 0.13702594213042052, -0.10425165865397402, 0.08379826374069045, -0.04941884578767582, -0.13071425415070548, -0.014014635782272316, 0.33828705886697186, -0.23359406656754608, -0.23882364725619398, 0.13025766403418237, -0.28715477905035774, -0.0879093749843585, 0.1375375802855632, -0.00828864609523... |
709.1006 | A New Efficient Method of Hartree-Fock-Bogoliubov Calculation for Weakly
Bound Nuclei | We propose a new method to solve the Hartree-Fock-Bogoliubov equations for
weakly bound nuclei, which works for both spherical and axially deformed cases.
In this approach, the quasiparticle wave functions are expanded in a complete
set of analytical Poschl-Teller-Ginocchio and Bessel/Coulomb wave functions.
Correct ... | nucl-th | we propose a new method to solve the hartreefockbogoliubov equations for weakly bound nuclei which works for both spherical and axially deformed cases in this approach the quasiparticle wave functions are expanded in a complete set of analytical poschltellerginocchio and besselcoulomb wave functions correct asymptotic ... | [['we', 'propose', 'a', 'new', 'method', 'to', 'solve', 'the', 'hartreefockbogoliubov', 'equations', 'for', 'weakly', 'bound', 'nuclei', 'which', 'works', 'for', 'both', 'spherical', 'and', 'axially', 'deformed', 'cases', 'in', 'this', 'approach', 'the', 'quasiparticle', 'wave', 'functions', 'are', 'expanded', 'in', 'a... | [-0.08558903770754114, 0.07981675925548189, -0.10850579364050646, 0.12105731283081696, -0.03556869421154261, -0.09612874173180899, 0.02746407948434353, 0.34273171215318143, -0.14904012799379415, -0.24642912191920913, 0.01280227269307943, -0.2772040056530386, -0.1233346296590753, 0.1968397749005817, 0.019541478155588266... |
709.1007 | Reanalysis of the $e^+e^-\to\eta\gamma$ reaction cross section | In the experiment with the SND detector at the VEPP-2M $e^+e^-$ collider
measuring the $e^+e^-\to \eta\gamma$ cross section in the energy range
$0.6<\sqrt{s}<1.38 \mathrm{GeV}$ the reanalysis of data is performed. The goal
is to improve the accuracy of the previous results by analysing ambiguities in
the approximatio... | hep-ex | in the experiment with the snd detector at the vepp2m ee collider measuring the eeto etagamma cross section in the energy range 06sqrts138 mathrmgev the reanalysis of data is performed the goal is to improve the accuracy of the previous results by analysing ambiguities in the approximation of energy dependence of the e... | [['in', 'the', 'experiment', 'with', 'the', 'snd', 'detector', 'at', 'the', 'vepp2m', 'ee', 'collider', 'measuring', 'the', 'eeto', 'etagamma', 'cross', 'section', 'in', 'the', 'energy', 'range', '06sqrts138', 'mathrmgev', 'the', 'reanalysis', 'of', 'data', 'is', 'performed', 'the', 'goal', 'is', 'to', 'improve', 'the'... | [-0.05123821474527093, 0.07489902452057735, -0.10379591608017852, 0.070223338132068, -0.022252071797001092, -0.041414424650032415, 0.03481020769951018, 0.325834815940735, -0.15318896266928111, -0.3022209425372156, -0.03598433889617974, -0.3560051331931556, 0.025189034979451786, 0.20850241686672566, 0.0687449162677777, ... |
709.1008 | Generalized solutions of the Cauchy problem for the Navier-Stokes system
and diffusion processes | We reduce the construction of a weak solution of the Cauchy problem for the
Navier-Stokes system to the construction of a solution to a stochastic problem.
Namely, we construct diffusion processes which allow us to obtain a
probabilistic representation of a weak (in distributional sense) solution to
the Cauchy proble... | math.PR math.AP | we reduce the construction of a weak solution of the cauchy problem for the navierstokes system to the construction of a solution to a stochastic problem namely we construct diffusion processes which allow us to obtain a probabilistic representation of a weak in distributional sense solution to the cauchy problem for t... | [['we', 'reduce', 'the', 'construction', 'of', 'a', 'weak', 'solution', 'of', 'the', 'cauchy', 'problem', 'for', 'the', 'navierstokes', 'system', 'to', 'the', 'construction', 'of', 'a', 'solution', 'to', 'a', 'stochastic', 'problem', 'namely', 'we', 'construct', 'diffusion', 'processes', 'which', 'allow', 'us', 'to', '... | [-0.1302837496877394, -0.052762627364559604, -0.10393992386419665, 0.070769303931262, -0.12563213895667683, -0.11969803364270112, 0.025089398534460502, 0.22925756106322462, -0.38677873526784506, -0.22367064438506284, 0.16107604082631455, -0.2571745711294087, -0.1270195986906236, 0.17624825438992545, -0.0693766712973063... |
709.1009 | The H$\alpha$ Luminosity Function and Star Formation Rate at $z \approx
0.24$ in the Cosmos 2 Square-Degree Field | To derive a new H$\alpha$ luminosity function and to understand the
clustering properties of star-forming galaxies at $z \approx 0.24$, we have
made a narrow-band imaging survey for H$\alpha$ emitting galaxies in the HST
COSMOS 2 square degree field. We used the narrow-band filter NB816 ($\lambda_c
= 8150$ \AA, $\Del... | astro-ph | to derive a new halpha luminosity function and to understand the clustering properties of starforming galaxies at z approx 024 we have made a narrowband imaging survey for halpha emitting galaxies in the hst cosmos 2 square degree field we used the narrowband filter nb816 lambda_c 8150 aa delta lambda 120 aa and sample... | [['to', 'derive', 'a', 'new', 'halpha', 'luminosity', 'function', 'and', 'to', 'understand', 'the', 'clustering', 'properties', 'of', 'starforming', 'galaxies', 'at', 'z', 'approx', '024', 'we', 'have', 'made', 'a', 'narrowband', 'imaging', 'survey', 'for', 'halpha', 'emitting', 'galaxies', 'in', 'the', 'hst', 'cosmos'... | [-0.02843402504855405, 0.06941246543219765, -0.0010404697872553636, 0.15041419734457254, -0.058911257574913424, -0.07087653230884773, 0.009240083276487444, 0.5229423531914329, -0.048134154538416025, -0.3477715017834624, 0.007310389896551852, -0.35485179085302554, 0.06599264753331403, 0.18984420918317024, 0.041049752934... |
709.101 | On the Correspondence between Poincar\'e Symmetry of Commutative QFT and
Twisted Poincar\'e Symmetry of Noncommutative QFT | The space-time symmetry of noncommutative quantum field theories with a
deformed quantization is described by the twisted Poincar\'e algebra, while
that of standard commutative quantum field theories is described by the
Poincar\'e algebra. Based on the equivalence of the deformed theory with a
commutative field theor... | hep-th | the spacetime symmetry of noncommutative quantum field theories with a deformed quantization is described by the twisted poincare algebra while that of standard commutative quantum field theories is described by the poincare algebra based on the equivalence of the deformed theory with a commutative field theory the cor... | [['the', 'spacetime', 'symmetry', 'of', 'noncommutative', 'quantum', 'field', 'theories', 'with', 'a', 'deformed', 'quantization', 'is', 'described', 'by', 'the', 'twisted', 'poincare', 'algebra', 'while', 'that', 'of', 'standard', 'commutative', 'quantum', 'field', 'theories', 'is', 'described', 'by', 'the', 'poincare... | [-0.14579296892043203, 0.16044705774309853, -0.12762930961177935, 0.1145439614709984, -0.04848580617487194, -0.1561721913656959, -0.05219044852613782, 0.29407238045204726, -0.307715863225952, -0.23129049863570209, 0.0509780200811783, -0.209712922513958, -0.1714642739721707, 0.12887581137733328, -0.07917850922759888, -0... |
709.1011 | Generic features of Einstein-Aether black holes | We reconsider spherically symmetric black hole solutions in Einstein-Aether
theory with the condition that this theory has identical PPN parameters as
those for general relativity, which is the main difference from the previous
research. In contrast with previous study, we allow superluminal propagation of
a spin-0 A... | gr-qc hep-ph hep-th | we reconsider spherically symmetric black hole solutions in einsteinaether theory with the condition that this theory has identical ppn parameters as those for general relativity which is the main difference from the previous research in contrast with previous study we allow superluminal propagation of a spin0 aethergr... | [['we', 'reconsider', 'spherically', 'symmetric', 'black', 'hole', 'solutions', 'in', 'einsteinaether', 'theory', 'with', 'the', 'condition', 'that', 'this', 'theory', 'has', 'identical', 'ppn', 'parameters', 'as', 'those', 'for', 'general', 'relativity', 'which', 'is', 'the', 'main', 'difference', 'from', 'the', 'prev... | [-0.13014386063424763, 0.1435393199057401, -0.11001849949251914, 0.13290475554970108, -0.13453375397627984, -0.16611520626811663, -0.03549955283607773, 0.3260238290506253, -0.17072480441530005, -0.2860774137134549, 0.10186181036650838, -0.28881489856175374, -0.08887460097110411, 0.1778643036149847, -0.06072445827590275... |
709.1012 | Insertion of a magnesium(II)-octacarboranyl(hexylsulfanyl) porphyrazine
into liposomes: a physico-chemical study | The synthesis, characterization and liposome insertion of a novel
magnesium(II) carboranyl-porphyrazine, i.e. [2,3,7,8,12,13,17,18-octakis-
(1,2-dicarba-closo-dodecaboranyl)-hexylthio-5,10,15,20-
porphyrazine]magnesium(II) complex, MgHECSPz, is described. MgHECSPz was
designed to improve the potentiality in multiple ... | cond-mat.soft physics.bio-ph | the synthesis characterization and liposome insertion of a novel magnesiumii carboranylporphyrazine ie 237812131718octakis 12dicarbaclosododecaboranylhexylthio5101520 porphyrazinemagnesiumii complex mghecspz is described mghecspz was designed to improve the potentiality in multiple approach anticancer therapy liposomal... | [['the', 'synthesis', 'characterization', 'and', 'liposome', 'insertion', 'of', 'a', 'novel', 'magnesiumii', 'carboranylporphyrazine', 'ie', '237812131718octakis', '12dicarbaclosododecaboranylhexylthio5101520', 'porphyrazinemagnesiumii', 'complex', 'mghecspz', 'is', 'described', 'mghecspz', 'was', 'designed', 'to', 'im... | [-0.0829057808281974, 0.14977209022148483, -0.05270117257661637, -0.019532588207268067, -0.04964587473941426, -0.17175295511861483, 0.01880495144700211, 0.4113306703586732, -0.22575214517212683, -0.3311322691790279, 0.05924439550031938, -0.2890869575222173, -0.14569778656286578, 0.15824665390555898, -0.0567774387628531... |
709.1013 | Empirical processes indexed by estimated functions | We consider the convergence of empirical processes indexed by functions that
depend on an estimated parameter $\eta$ and give several alternative conditions
under which the ``estimated parameter'' $\eta_n$ can be replaced by its natural
limit $\eta_0$ uniformly in some other indexing set $\Theta$. In particular we
re... | math.ST stat.TH | we consider the convergence of empirical processes indexed by functions that depend on an estimated parameter eta and give several alternative conditions under which the estimated parameter eta_n can be replaced by its natural limit eta_0 uniformly in some other indexing set theta in particular we reconsider some examp... | [['we', 'consider', 'the', 'convergence', 'of', 'empirical', 'processes', 'indexed', 'by', 'functions', 'that', 'depend', 'on', 'an', 'estimated', 'parameter', 'eta', 'and', 'give', 'several', 'alternative', 'conditions', 'under', 'which', 'the', 'estimated', 'parameter', 'eta_n', 'can', 'be', 'replaced', 'by', 'its', ... | [-0.059071278857902206, 0.11039899224609447, -0.08576551404107234, 0.0888638875385368, -0.04798694497413248, -0.09459994900864603, 0.07206598016963309, 0.3484169289512538, -0.2483534954445458, -0.2880425247759826, 0.1297476291281824, -0.21442423478282732, -0.1526348535801102, 0.23909966636920113, -0.10353070776374347, ... |
709.1014 | Critical phenomena and renormalization-group flow of multi-parameter
\Phi^4 field theories | In the framework of the renormalization-group (RG) approach, critical
phenomena can be investigated by studying the RG flow of multi-parameter
$\Phi^4$ field theories with an $N$-component fundamental field, containing up
to 4th-order polynomials of the field. Some physically interesting systems
require $\Phi^4$ fiel... | hep-lat cond-mat.stat-mech hep-th | in the framework of the renormalizationgroup rg approach critical phenomena can be investigated by studying the rg flow of multiparameter phi4 field theories with an ncomponent fundamental field containing up to 4thorder polynomials of the field some physically interesting systems require phi4 field theories with sever... | [['in', 'the', 'framework', 'of', 'the', 'renormalizationgroup', 'rg', 'approach', 'critical', 'phenomena', 'can', 'be', 'investigated', 'by', 'studying', 'the', 'rg', 'flow', 'of', 'multiparameter', 'phi4', 'field', 'theories', 'with', 'an', 'ncomponent', 'fundamental', 'field', 'containing', 'up', 'to', '4thorder', '... | [-0.17960628243029225, 0.1762177585408497, -0.10020479512662231, 0.05485670194247563, -0.0807584771809416, -0.17959324253736425, -0.020230557049269512, 0.3490550349392801, -0.21502985798237886, -0.2670452977905867, 0.07684347748491752, -0.2838497323205145, -0.179427537926399, 0.19425275833379452, 0.03660935269527995, 0... |
709.1015 | Two-dimensional semiconducting nanostructures based on single graphene
sheets with lines of adsorbed hydrogen atoms | It is shown that lines of adsorbed hydrogen pair atoms divide the graphene
sheet into strips and form hydrogen-based superlattice structures (2HG-SL). We
show that the forming of 2HG-SL drastically changes the electronic properties
of graphene from semimetal to semiconductor. The electronic spectra of "zigzag"
(n,0) ... | cond-mat.mtrl-sci | it is shown that lines of adsorbed hydrogen pair atoms divide the graphene sheet into strips and form hydrogenbased superlattice structures 2hgsl we show that the forming of 2hgsl drastically changes the electronic properties of graphene from semimetal to semiconductor the electronic spectra of zigzag n0 2hgsl is simil... | [['it', 'is', 'shown', 'that', 'lines', 'of', 'adsorbed', 'hydrogen', 'pair', 'atoms', 'divide', 'the', 'graphene', 'sheet', 'into', 'strips', 'and', 'form', 'hydrogenbased', 'superlattice', 'structures', '2hgsl', 'we', 'show', 'that', 'the', 'forming', 'of', '2hgsl', 'drastically', 'changes', 'the', 'electronic', 'pro... | [-0.162475756264287, 0.17170066559805436, -0.019786436439990396, -0.027152541613281525, 0.014643251866506732, -0.18598788552870504, 0.06975575733807578, 0.46982828584603137, -0.2464527671197147, -0.2857793065333607, -0.030272743034392896, -0.32984228223336465, -0.15043703553436155, 0.15482041007848552, 0.04006673324138... |
709.1016 | Charge Form Factor and Cluster Structure of $^6$Li Nucleus | The charge form factor of ${}^6$Li nucleus is considered on the basis of its
cluster structure. The charge density of ${}^6$Li is presented as a
superposition of two terms. One of them is a folded density and the second one
is a sum of ${}^4$He and the deuteron densities. Using the available
experimental data for ${}... | nucl-th | the charge form factor of 6li nucleus is considered on the basis of its cluster structure the charge density of 6li is presented as a superposition of two terms one of them is a folded density and the second one is a sum of 4he and the deuteron densities using the available experimental data for 4he and deuteron charge... | [['the', 'charge', 'form', 'factor', 'of', '6li', 'nucleus', 'is', 'considered', 'on', 'the', 'basis', 'of', 'its', 'cluster', 'structure', 'the', 'charge', 'density', 'of', '6li', 'is', 'presented', 'as', 'a', 'superposition', 'of', 'two', 'terms', 'one', 'of', 'them', 'is', 'a', 'folded', 'density', 'and', 'the', 'se... | [-0.09958474648996227, 0.14158118235808548, -0.06340604365593003, 0.04769563375626721, 0.04821344892123854, -0.04810197237298213, 0.06542018599688046, 0.30037855446058254, -0.1904131459693114, -0.27317680919202425, 0.002016011228714819, -0.31541436171579745, -0.01761240327870974, 0.17801814250678064, 0.0743451051771395... |
709.1017 | A multibeam atom laser: coherent atom beam splitting from a single far
detuned laser | We report the experimental realisation of a multibeam atom laser. A single
continuous atom laser is outcoupled from a Bose-Einstein condensate (BEC) via
an optical Raman transition. The atom laser is subsequently split into up to
five atomic beams with slightly different momenta, resulting in multiple,
nearly co-prop... | cond-mat.other | we report the experimental realisation of a multibeam atom laser a single continuous atom laser is outcoupled from a boseeinstein condensate bec via an optical raman transition the atom laser is subsequently split into up to five atomic beams with slightly different momenta resulting in multiple nearly copropagating co... | [['we', 'report', 'the', 'experimental', 'realisation', 'of', 'a', 'multibeam', 'atom', 'laser', 'a', 'single', 'continuous', 'atom', 'laser', 'is', 'outcoupled', 'from', 'a', 'boseeinstein', 'condensate', 'bec', 'via', 'an', 'optical', 'raman', 'transition', 'the', 'atom', 'laser', 'is', 'subsequently', 'split', 'into... | [-0.13936440760006358, 0.2676539101071698, -0.09811127398896849, -0.07285815894516932, -0.00926681575036109, -0.18505054566952767, 0.05948556008080792, 0.4800486888623599, -0.2685975787239243, -0.21673774110586053, -0.03379144640686461, -0.2637881116019656, -0.027081776833669705, 0.24323515771333165, 0.0206934203948787... |
709.1018 | Corner Multifractality for Reflex Angles and Conformal Invariance at 2D
Anderson Metal-Insulator Transition with Spin-Orbit Scattering | We investigate boundary multifractality of critical wave functions at the
Anderson metal-insulator transition in two-dimensional disordered
non-interacting electron systems with spin-orbit scattering. We show
numerically that multifractal exponents at a corner with an opening angle
\theta=3\pi/2 are directly related ... | cond-mat.dis-nn cond-mat.mes-hall | we investigate boundary multifractality of critical wave functions at the anderson metalinsulator transition in twodimensional disordered noninteracting electron systems with spinorbit scattering we show numerically that multifractal exponents at a corner with an opening angle theta3pi2 are directly related to those ne... | [['we', 'investigate', 'boundary', 'multifractality', 'of', 'critical', 'wave', 'functions', 'at', 'the', 'anderson', 'metalinsulator', 'transition', 'in', 'twodimensional', 'disordered', 'noninteracting', 'electron', 'systems', 'with', 'spinorbit', 'scattering', 'we', 'show', 'numerically', 'that', 'multifractal', 'ex... | [-0.16213877062210275, 0.13355729825777346, -0.07049653319588217, -0.01382371752025882, -0.05642929347231984, -0.14606078722191831, 0.0750258476831592, 0.33766025891908125, -0.2012478603879012, -0.23364418908917847, -0.01447323902707117, -0.322228016918346, -0.21506351116113365, 0.17081394001769906, -0.0225993067814180... |
709.1019 | Realistic Neutrinogenesis with Radiative Vertex Correction | We propose a new model for naturally light Dirac neutrinos and explain the
baryon asymmetry of the universe through neutrinogenesis. We extend the
standard model with a real singlet scalar, a heavy singlet Dirac fermion and a
heavy doublet scalar besides three right-handed neutrinos, respecting lepton
number conserva... | hep-ph | we propose a new model for naturally light dirac neutrinos and explain the baryon asymmetry of the universe through neutrinogenesis we extend the standard model with a real singlet scalar a heavy singlet dirac fermion and a heavy doublet scalar besides three righthanded neutrinos respecting lepton number conservation a... | [['we', 'propose', 'a', 'new', 'model', 'for', 'naturally', 'light', 'dirac', 'neutrinos', 'and', 'explain', 'the', 'baryon', 'asymmetry', 'of', 'the', 'universe', 'through', 'neutrinogenesis', 'we', 'extend', 'the', 'standard', 'model', 'with', 'a', 'real', 'singlet', 'scalar', 'a', 'heavy', 'singlet', 'dirac', 'fermi... | [-0.13726349184641018, 0.3408027592873085, -0.01303222248295568, 0.18602571004866944, -0.10336248229884501, -0.19059873861114277, 0.05410729769292235, 0.24614196186504508, -0.2239116598682115, -0.30295835130806986, -0.04469668153386399, -0.33031595885495907, 0.004574307709135725, 0.03736188578999267, 0.0911441887230993... |
709.102 | Evolution Strategies in Optimization Problems | Evolution Strategies are inspired in biology and part of a larger research
field known as Evolutionary Algorithms. Those strategies perform a random
search in the space of admissible functions, aiming to optimize some given
objective function. We show that simple evolution strategies are a useful tool
in optimal cont... | math.OC | evolution strategies are inspired in biology and part of a larger research field known as evolutionary algorithms those strategies perform a random search in the space of admissible functions aiming to optimize some given objective function we show that simple evolution strategies are a useful tool in optimal control p... | [['evolution', 'strategies', 'are', 'inspired', 'in', 'biology', 'and', 'part', 'of', 'a', 'larger', 'research', 'field', 'known', 'as', 'evolutionary', 'algorithms', 'those', 'strategies', 'perform', 'a', 'random', 'search', 'in', 'the', 'space', 'of', 'admissible', 'functions', 'aiming', 'to', 'optimize', 'some', 'gi... | [-0.08611643704437259, 0.02715994462314352, -0.11398018448465112, 0.1304920703658591, -0.12376729204602864, -0.14200345670426454, 0.05768673329789569, 0.427824005484581, -0.2822480471129867, -0.32578445711861487, 0.1280457113424073, -0.18429283380670392, -0.21815106683019278, 0.23560469653929814, -0.087950154842026, 0.... |
709.1021 | Spacetime structure of 5D hypercylindrical vacuum solutions with tension | We investigate geometrical properties of 5D cylindrical vacuum solutions with
a transverse spherical symmetry. The metric is uniform along the fifth
direction and characterized by tension and mass densities. The solutions are
classified by the tension-to-mass ratio. One particular example is the
well-known Schwarzsch... | gr-qc hep-th | we investigate geometrical properties of 5d cylindrical vacuum solutions with a transverse spherical symmetry the metric is uniform along the fifth direction and characterized by tension and mass densities the solutions are classified by the tensiontomass ratio one particular example is the wellknown schwarzschild blac... | [['we', 'investigate', 'geometrical', 'properties', 'of', '5d', 'cylindrical', 'vacuum', 'solutions', 'with', 'a', 'transverse', 'spherical', 'symmetry', 'the', 'metric', 'is', 'uniform', 'along', 'the', 'fifth', 'direction', 'and', 'characterized', 'by', 'tension', 'and', 'mass', 'densities', 'the', 'solutions', 'are'... | [-0.1971423328795936, 0.11673449125257983, -0.09517933510836553, 0.07067452029117373, -0.0939745207795733, -0.17768118677089328, -0.06840915396671997, 0.3448376565409655, -0.1973840577252717, -0.25894202407587064, 0.1381300609421239, -0.326897618889978, -0.05081949050178413, 0.1404722633411769, -0.04696226632288678, 0.... |
709.1022 | b\to s\nu\bar{\nu} decay in the MSSM: Implication of b\to s\gamma at
large tan beta | The decay $b\to s\nu\bar{\nu}$ is discussed in the minimal supersymmetric
standard model with general flavor mixing for squarks, at large $\tan\beta$. In
this case, in addition to the chargino loop contributions which were analyzed
in previously studies, $\tan\beta$-enhanced contributions from the gluino and
charged ... | hep-ph | the decay bto snubarnu is discussed in the minimal supersymmetric standard model with general flavor mixing for squarks at large tanbeta in this case in addition to the chargino loop contributions which were analyzed in previously studies tanbetaenhanced contributions from the gluino and charged higgs boson loops might... | [['the', 'decay', 'bto', 'snubarnu', 'is', 'discussed', 'in', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'with', 'general', 'flavor', 'mixing', 'for', 'squarks', 'at', 'large', 'tanbeta', 'in', 'this', 'case', 'in', 'addition', 'to', 'the', 'chargino', 'loop', 'contributions', 'which', 'were', 'analyzed',... | [-0.0281833734367795, 0.2687395076500252, 0.01391218101623683, 0.202573911507408, -0.09136063358164392, -0.16604643246570888, 0.07622972001823095, 0.28097914899430737, -0.21225123857416642, -0.23426641111906904, 0.03616394778118075, -0.33754998869083536, -0.03758563754560713, 0.18276126427540126, 0.033914825458151214, ... |
709.1023 | Constraint optimization and landscapes | We describe an effective landscape introduced in [1] for the analysis of
Constraint Satisfaction problems, such as Sphere Packing, K-SAT and Graph
Coloring. This geometric construction reexpresses these problems in the more
familiar terms of optimization in rugged energy landscapes. In particular, it
allows one to un... | quant-ph cond-mat.stat-mech cs.CC nlin.AO | we describe an effective landscape introduced in 1 for the analysis of constraint satisfaction problems such as sphere packing ksat and graph coloring this geometric construction reexpresses these problems in the more familiar terms of optimization in rugged energy landscapes in particular it allows one to understand t... | [['we', 'describe', 'an', 'effective', 'landscape', 'introduced', 'in', '1', 'for', 'the', 'analysis', 'of', 'constraint', 'satisfaction', 'problems', 'such', 'as', 'sphere', 'packing', 'ksat', 'and', 'graph', 'coloring', 'this', 'geometric', 'construction', 'reexpresses', 'these', 'problems', 'in', 'the', 'more', 'fam... | [-0.06758876651991158, 0.08145606353762559, -0.09489052912220358, 0.18168510739225893, -0.12157011066873868, -0.1547317597704629, 0.02942971666653951, 0.35779514074325564, -0.300771975244085, -0.3889078024029732, 0.0866518078930676, -0.2248780713015003, -0.2057518237332503, 0.15995913943896692, -0.11723843859508634, 0.... |
709.1024 | Computational performance of a parallelized high-order spectral and
mortar element toolbox | In this paper, a comprehensive performance review of a MPI-based high-order
spectral and mortar element method C++ toolbox is presented. The focus is put
on the performance evaluation of several aspects with a particular emphasis on
the parallel efficiency. The performance evaluation is analyzed and compared to
predi... | cs.DC cs.PF | in this paper a comprehensive performance review of a mpibased highorder spectral and mortar element method c toolbox is presented the focus is put on the performance evaluation of several aspects with a particular emphasis on the parallel efficiency the performance evaluation is analyzed and compared to predictions gi... | [['in', 'this', 'paper', 'a', 'comprehensive', 'performance', 'review', 'of', 'a', 'mpibased', 'highorder', 'spectral', 'and', 'mortar', 'element', 'method', 'c', 'toolbox', 'is', 'presented', 'the', 'focus', 'is', 'put', 'on', 'the', 'performance', 'evaluation', 'of', 'several', 'aspects', 'with', 'a', 'particular', '... | [-0.07546216549148949, -0.03219444585945642, -0.07772571881910288, 0.013363182402935138, -0.09593430570658702, -0.12790418216626687, 0.052852998972907295, 0.4088048748487588, -0.1878673170813092, -0.3045104696037303, 0.12944306327504945, -0.25658857586821265, -0.13622445343431122, 0.2616719605198296, -0.046844262477312... |
709.1025 | Coexistence of CDW with staggered superconductivity in a ferromagnetic
material | In usual superconductivity (SC), the pairs have zero total momentum
irrespective of their symmetry. Staggered SC would involve, instead, pairs with
a finite commensurate total momentum, but such exotic states have never been
proven to be realized in nature. Here we study for the first time the influence
of particle-h... | cond-mat.supr-con cond-mat.str-el | in usual superconductivity sc the pairs have zero total momentum irrespective of their symmetry staggered sc would involve instead pairs with a finite commensurate total momentum but such exotic states have never been proven to be realized in nature here we study for the first time the influence of particlehole asymmet... | [['in', 'usual', 'superconductivity', 'sc', 'the', 'pairs', 'have', 'zero', 'total', 'momentum', 'irrespective', 'of', 'their', 'symmetry', 'staggered', 'sc', 'would', 'involve', 'instead', 'pairs', 'with', 'a', 'finite', 'commensurate', 'total', 'momentum', 'but', 'such', 'exotic', 'states', 'have', 'never', 'been', '... | [-0.21746032617799937, 0.25207421188801526, -0.07717885670810938, 0.0682315580630675, -0.03525221435725689, -0.11540940629690885, 0.10359871982969343, 0.38606896296143534, -0.22376372179761528, -0.28838180828094484, 0.014674017077311873, -0.3089678023904562, -0.09873519369959831, 0.06887921626120806, 0.0733893366232514... |
709.1026 | Parton showers from the dipole formalism | We present an implementation of a parton shower algorithm for hadron
colliders and electron-positron colliders based on the dipole factorisation
formulae. The algorithm treats initial-state partons on equal footing with
final-state partons. We implemented the algorithm for massless and massive
partons.
| hep-ph | we present an implementation of a parton shower algorithm for hadron colliders and electronpositron colliders based on the dipole factorisation formulae the algorithm treats initialstate partons on equal footing with finalstate partons we implemented the algorithm for massless and massive partons | [['we', 'present', 'an', 'implementation', 'of', 'a', 'parton', 'shower', 'algorithm', 'for', 'hadron', 'colliders', 'and', 'electronpositron', 'colliders', 'based', 'on', 'the', 'dipole', 'factorisation', 'formulae', 'the', 'algorithm', 'treats', 'initialstate', 'partons', 'on', 'equal', 'footing', 'with', 'finalstate... | [-0.06884170120309402, 0.2778687402334493, -0.2271481303997883, 0.22371272561026784, -0.0698944098066266, -0.06936742911660453, -0.1127519193957219, 0.46775373057803005, -0.038318178730040064, -0.19721432688941315, -0.1377668472733803, -0.31479589050499407, 0.04684290480686397, 0.09160965199514133, 0.13173705321259616,... |
709.1027 | A parton shower algorithm based on Catani-Seymour dipole factorisation | In this publication the implementation of a new parton shower model based on
the Catani-Seymour dipole factorisation, as first suggested by Z. Nagy and D.
E. Soper, is discussed. First results obtained with the new algorithm are
compared with experimental data.
| hep-ph | in this publication the implementation of a new parton shower model based on the cataniseymour dipole factorisation as first suggested by z nagy and d e soper is discussed first results obtained with the new algorithm are compared with experimental data | [['in', 'this', 'publication', 'the', 'implementation', 'of', 'a', 'new', 'parton', 'shower', 'model', 'based', 'on', 'the', 'cataniseymour', 'dipole', 'factorisation', 'as', 'first', 'suggested', 'by', 'z', 'nagy', 'and', 'd', 'e', 'soper', 'is', 'discussed', 'first', 'results', 'obtained', 'with', 'the', 'new', 'algo... | [-0.04922576692727644, 0.08246256557588534, -0.11519294931757741, 0.045527139178863384, -0.05165219597700166, -0.08693437662157344, -0.005179912624199216, 0.38177898398986676, -0.14114547266465863, -0.30118818172230954, 0.03890858032661149, -0.2629771652154443, -0.09856003341151447, 0.1906000774342385, 0.00426899534990... |
709.1028 | Analytic evidence for the Gubser-Mitra conjecture | A simple master equation for the static perturbation of charged black strings
is derived while employing the gauge proposed by Kol. As the charge is varied
it is found that the potential in the master equation for the perturbations
becomes positive exactly when the specific heat turns positive thus forbidding
a bound... | hep-th gr-qc | a simple master equation for the static perturbation of charged black strings is derived while employing the gauge proposed by kol as the charge is varied it is found that the potential in the master equation for the perturbations becomes positive exactly when the specific heat turns positive thus forbidding a bound st... | [['a', 'simple', 'master', 'equation', 'for', 'the', 'static', 'perturbation', 'of', 'charged', 'black', 'strings', 'is', 'derived', 'while', 'employing', 'the', 'gauge', 'proposed', 'by', 'kol', 'as', 'the', 'charge', 'is', 'varied', 'it', 'is', 'found', 'that', 'the', 'potential', 'in', 'the', 'master', 'equation', '... | [-0.14791745554998909, 0.15060737813381772, -0.08456785498971217, 0.13000994233880192, -0.07458660343759939, -0.1663614640796655, 0.03855682609504775, 0.23295729779883434, -0.22570117177490734, -0.2465547193429972, 0.12335245985733835, -0.30126935611478983, -0.15448773377329894, 0.17948791708209014, 0.00393493489215248... |
709.1029 | Four-lepton LHC events from MSSM Higgs boson decays into neutralino and
chargino pairs | Heavy neutral Higgs boson production and decay into neutralino and chargino
pairs is studied at the Large Hadron Collider in the context of the Minimal
Supersymmetric Standard Model. Higgs boson decays into the heavier neutralino
and chargino states, i.e., H^0 or A^0 to tilde{chi}_i^0 tilde{chi}_j^0 (i,j =
2,3,4) as ... | hep-ph | heavy neutral higgs boson production and decay into neutralino and chargino pairs is studied at the large hadron collider in the context of the minimal supersymmetric standard model higgs boson decays into the heavier neutralino and chargino states ie h0 or a0 to tildechi_i0 tildechi_j0 ij 234 as well as h0 or a0 to ti... | [['heavy', 'neutral', 'higgs', 'boson', 'production', 'and', 'decay', 'into', 'neutralino', 'and', 'chargino', 'pairs', 'is', 'studied', 'at', 'the', 'large', 'hadron', 'collider', 'in', 'the', 'context', 'of', 'the', 'minimal', 'supersymmetric', 'standard', 'model', 'higgs', 'boson', 'decays', 'into', 'the', 'heavier'... | [-0.058396241650916635, 0.2726975175047604, -0.006162472221573504, 0.2031203292198673, -0.07315722430163683, -0.23145994366301845, 0.05237203160844122, 0.3091351303970441, -0.1986210800056142, -0.2879051016255592, 0.031976471919915636, -0.30282944890010793, 0.059609614992708275, 0.14099717579132023, 0.07768177368113054... |
709.103 | Detection of long-lived staus and gravitinos at the ILC | A study is presented illustrating the excellent potential of future
International Linear Collider (ILC) experiments to detect metastable staus
$\stau$, measure precisely their mass and lifetime, and to determine the mass
of the gravitino $\sG$ from the decay $\stau\to\tau\sG$, thus providing direct
access to the gr... | hep-ph | a study is presented illustrating the excellent potential of future international linear collider ilc experiments to detect metastable staus stau measure precisely their mass and lifetime and to determine the mass of the gravitino sg from the decay stautotausg thus providing direct access to the gravitational coupling ... | [['a', 'study', 'is', 'presented', 'illustrating', 'the', 'excellent', 'potential', 'of', 'future', 'international', 'linear', 'collider', 'ilc', 'experiments', 'to', 'detect', 'metastable', 'staus', 'stau', 'measure', 'precisely', 'their', 'mass', 'and', 'lifetime', 'and', 'to', 'determine', 'the', 'mass', 'of', 'the'... | [-0.11615325280106437, 0.18732759632094173, -0.039779060653277805, 0.16111613633538768, -0.10559262098193321, -0.1586909979648356, 0.03589566010145508, 0.31502873868662484, -0.27306556920235864, -0.304246846557956, 0.1149278848612567, -0.29832956058030224, 0.04179623234560903, 0.1897510530579151, 0.09552190224735105, 0... |
709.1031 | How to Detect `Decoupled' Heavy Supersymmetric Higgs Bosons | Heretofore neglected decay modes of heavy MSSM Higgs bosons into a variety of
neutralino pairs may push the LHC discovery reach for these crucial elements of
an extended Higgs sector to nearly the TeV-scale -- if sparticle-sector MSSM
input parameters are favorable. This is well into the so-called decoupling
region, ... | hep-ph | heretofore neglected decay modes of heavy mssm higgs bosons into a variety of neutralino pairs may push the lhc discovery reach for these crucial elements of an extended higgs sector to nearly the tevscale if sparticlesector mssm input parameters are favorable this is well into the socalled decoupling region including ... | [['heretofore', 'neglected', 'decay', 'modes', 'of', 'heavy', 'mssm', 'higgs', 'bosons', 'into', 'a', 'variety', 'of', 'neutralino', 'pairs', 'may', 'push', 'the', 'lhc', 'discovery', 'reach', 'for', 'these', 'crucial', 'elements', 'of', 'an', 'extended', 'higgs', 'sector', 'to', 'nearly', 'the', 'tevscale', 'if', 'spa... | [-0.10788723221645714, 0.30874853430531146, 0.015479052310976654, 0.18519037115635376, -0.12069475742277856, -0.24214308985317937, 0.055569280796006724, 0.29059677231961334, -0.22120029270613137, -0.2916893851286612, 0.036955354997189716, -0.2600038380161352, 0.027293703214337047, 0.1427747913451943, -0.013824982685410... |
709.1032 | Weyl asymptotics for magnetic Schr\"odinger operators and de Gennes'
boundary condition | This paper is concerned with the discrete spectrum of the self-adjoint
realization of the semi-classical Schr\"odinger operator with constant magnetic
field and associated with the de Gennes (Fourier/Robin) boundary condition. We
derive an asymptotic expansion of the number of eigenvalues below the essential
spectrum... | math.SP | this paper is concerned with the discrete spectrum of the selfadjoint realization of the semiclassical schrodinger operator with constant magnetic field and associated with the de gennes fourierrobin boundary condition we derive an asymptotic expansion of the number of eigenvalues below the essential spectrum weyltype ... | [['this', 'paper', 'is', 'concerned', 'with', 'the', 'discrete', 'spectrum', 'of', 'the', 'selfadjoint', 'realization', 'of', 'the', 'semiclassical', 'schrodinger', 'operator', 'with', 'constant', 'magnetic', 'field', 'and', 'associated', 'with', 'the', 'de', 'gennes', 'fourierrobin', 'boundary', 'condition', 'we', 'de... | [-0.15525537285290353, 0.05199194003126986, -0.0934394610254732, -0.03584563006225922, -0.09696255657464674, -0.06346831252568796, -0.000173763587292641, 0.2540758942215614, -0.1596859020407452, -0.30991990662702956, 0.09170819960585604, -0.2859460665997475, -0.15010760295880984, 0.1602113164789107, -0.0763464688438258... |
709.1033 | The investigation of particle acceleration in colliding-wind massive
binaries with SIMBOL-X | An increasing number of early-type (O and Wolf-Rayet) colliding wind binaries
(CWBs) is known to accelerate particles up to relativistic energies. In this
context, non-thermal emission processes such as inverse Compton (IC) scattering
are expected to produce a high energy spectrum, in addition to the strong
thermal e... | astro-ph | an increasing number of earlytype o and wolfrayet colliding wind binaries cwbs is known to accelerate particles up to relativistic energies in this context nonthermal emission processes such as inverse compton ic scattering are expected to produce a high energy spectrum in addition to the strong thermal emission from t... | [['an', 'increasing', 'number', 'of', 'earlytype', 'o', 'and', 'wolfrayet', 'colliding', 'wind', 'binaries', 'cwbs', 'is', 'known', 'to', 'accelerate', 'particles', 'up', 'to', 'relativistic', 'energies', 'in', 'this', 'context', 'nonthermal', 'emission', 'processes', 'such', 'as', 'inverse', 'compton', 'ic', 'scatteri... | [-0.05736894279057231, 0.21329623842285325, -0.02847020215361969, 0.1684983360895688, -0.08072721556838573, -0.09827681117556022, -0.022340335826325507, 0.39559419362144616, -0.24945391402117736, -0.37138109430955113, 0.03884688369976001, -0.30858908146122144, 0.04019354464386711, 0.24105044215284857, 0.046803214163155... |
709.1034 | Heat kernel estimates and spectral properties of a pseudorelativistic
operator with magnetic field | Based on the Mehler heat kernel of the Schroedinger operator for a free
electron in a constant magnetic field an estimate for the kernel of E_A is
derived, where E_A represents the kinetic energy of a Dirac electron within the
pseudorelativistic no-pair Brown-Ravenhall model. This estimate is used to
provide the bott... | math-ph math.MP math.SP | based on the mehler heat kernel of the schroedinger operator for a free electron in a constant magnetic field an estimate for the kernel of e_a is derived where e_a represents the kinetic energy of a dirac electron within the pseudorelativistic nopair brownravenhall model this estimate is used to provide the bottom of ... | [['based', 'on', 'the', 'mehler', 'heat', 'kernel', 'of', 'the', 'schroedinger', 'operator', 'for', 'a', 'free', 'electron', 'in', 'a', 'constant', 'magnetic', 'field', 'an', 'estimate', 'for', 'the', 'kernel', 'of', 'e_a', 'is', 'derived', 'where', 'e_a', 'represents', 'the', 'kinetic', 'energy', 'of', 'a', 'dirac', '... | [-0.11374521618604325, 0.15952659793622567, -0.03214044995564089, 0.09897316042386163, -0.023996547131349195, -0.11730513597702545, 0.013097989325819726, 0.3014800923803214, -0.23784505166741235, -0.24612376974958383, 0.018984054045207546, -0.2860820045841209, -0.018598216657757006, 0.18705584602221176, 0.0482573841117... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.