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 |
|---|---|---|---|---|---|---|
709.0735 | Magnetogenesis from Rotating Cosmic String Loops | We present a mechanism to create vortices in a plasma via gravitational
dragging behind rotating cosmic string loops. The vortical motions create
magnetic fields by means of the Harrison-Rees mechanism; the fields are further
enhanced through galactic collapse and dynamo amplification. Employing the
Velocity dependen... | astro-ph hep-th | we present a mechanism to create vortices in a plasma via gravitational dragging behind rotating cosmic string loops the vortical motions create magnetic fields by means of the harrisonrees mechanism the fields are further enhanced through galactic collapse and dynamo amplification employing the velocity dependent one ... | [['we', 'present', 'a', 'mechanism', 'to', 'create', 'vortices', 'in', 'a', 'plasma', 'via', 'gravitational', 'dragging', 'behind', 'rotating', 'cosmic', 'string', 'loops', 'the', 'vortical', 'motions', 'create', 'magnetic', 'fields', 'by', 'means', 'of', 'the', 'harrisonrees', 'mechanism', 'the', 'fields', 'are', 'fur... | [-0.18352222721169592, 0.25986482106837566, -0.049127577004306346, 0.14620955854542958, -0.1015501580727489, -0.05115020962219442, 0.00913745255978859, 0.3948797542682808, -0.24804292177862447, -0.32990146184380614, 0.044940737758145624, -0.18038431613746544, -0.08133239919097042, 0.21237067369815044, 0.064938248130087... |
709.0736 | On the Emergence of Unstable Modes in an Expanding Domain for
Energy-Conserving Wave Equations | Motivated by recent work on instabilities in expanding domains in
reaction-diffusion settings, we propose an analog of such mechanisms in
energy-conserving wave equations. In particular, we consider a nonlinear
Schr{\"o}dinger equation in a finite domain and show how the expansion or
contraction of the domain, under ... | nlin.PS | motivated by recent work on instabilities in expanding domains in reactiondiffusion settings we propose an analog of such mechanisms in energyconserving wave equations in particular we consider a nonlinear schrodinger equation in a finite domain and show how the expansion or contraction of the domain under appropriate ... | [['motivated', 'by', 'recent', 'work', 'on', 'instabilities', 'in', 'expanding', 'domains', 'in', 'reactiondiffusion', 'settings', 'we', 'propose', 'an', 'analog', 'of', 'such', 'mechanisms', 'in', 'energyconserving', 'wave', 'equations', 'in', 'particular', 'we', 'consider', 'a', 'nonlinear', 'schrodinger', 'equation'... | [-0.1678275480800498, 0.13965512720885506, -0.08108929397983361, 0.050526124819808234, -0.07003762843128525, -0.09242491859250364, -0.00042443430727034546, 0.33086565529012774, -0.3026517121558102, -0.20024725128855325, 0.1364466899447555, -0.215729389277872, -0.19652345047365313, 0.17258008289155014, -0.03051951356681... |
709.0737 | On the existence of tight contact structures on Seifert fibered
3-manifolds | We determine the closed, oriented Seifert fibered 3-manifolds which carry
positive tight contact structures. Our main tool is a new non-vanishing
criterion for the contact Ozsvath-Szabo invariant.
| math.SG math.GT | we determine the closed oriented seifert fibered 3manifolds which carry positive tight contact structures our main tool is a new nonvanishing criterion for the contact ozsvathszabo invariant | [['we', 'determine', 'the', 'closed', 'oriented', 'seifert', 'fibered', '3manifolds', 'which', 'carry', 'positive', 'tight', 'contact', 'structures', 'our', 'main', 'tool', 'is', 'a', 'new', 'nonvanishing', 'criterion', 'for', 'the', 'contact', 'ozsvathszabo', 'invariant']] | [-0.35728978158699143, 0.0923636191421085, -0.15702785565345376, 0.20580525932988772, -0.15193995629885682, -0.29344215490682807, 0.013318386480764107, 0.3192372422803331, -0.2490874862091409, -0.29219543247449176, -0.001573386196805923, -0.20012648301888947, -0.2352559144427586, 0.20333849155792483, -0.127781765880408... |
709.0738 | A quantum characterization of NP | In this article we introduce a new complexity class called PQMA_log(2).
Informally, this is the class of languages for which membership has a
logarithmic-size quantum proof with perfect completeness and soundness which is
polynomially close to 1 in a context where the verifier is provided a proof
with two unentangled... | quant-ph | in this article we introduce a new complexity class called pqma_log2 informally this is the class of languages for which membership has a logarithmicsize quantum proof with perfect completeness and soundness which is polynomially close to 1 in a context where the verifier is provided a proof with two unentangled parts ... | [['in', 'this', 'article', 'we', 'introduce', 'a', 'new', 'complexity', 'class', 'called', 'pqma_log2', 'informally', 'this', 'is', 'the', 'class', 'of', 'languages', 'for', 'which', 'membership', 'has', 'a', 'logarithmicsize', 'quantum', 'proof', 'with', 'perfect', 'completeness', 'and', 'soundness', 'which', 'is', 'p... | [-0.06937409095466136, 0.06452671138104052, -0.10480095695937053, 0.07433828360401094, -0.1189421654259786, -0.19190301785245537, 0.06531618540640921, 0.30417573522776364, -0.3027839259058237, -0.2934022776875645, 0.09408955534454436, -0.2308321549370885, -0.12228765032254159, 0.2088194295950234, -0.12817898948676884, ... |
709.0739 | Reply to Comment on the paper ``Energy Loss of Charm Quarks in the
Quark-Gluon Plasma: Collisional vs Radiative'' by Mishra et al | The comments raised in Ref. [1] by Mishra et al aim at two papers contained
in Ref. [2]. We show that those comments on Ref. [2] pointed out by Mishra et
al in Ref.[1] are not relevant and the concept used in Ref.[2] is consistent
and in compliance with the classical approximation of the transport
coefficients [3]. W... | hep-ph | the comments raised in ref 1 by mishra et al aim at two papers contained in ref 2 we show that those comments on ref 2 pointed out by mishra et al in ref1 are not relevant and the concept used in ref2 is consistent and in compliance with the classical approximation of the transport coefficients 3 we would also like to ... | [['the', 'comments', 'raised', 'in', 'ref', '1', 'by', 'mishra', 'et', 'al', 'aim', 'at', 'two', 'papers', 'contained', 'in', 'ref', '2', 'we', 'show', 'that', 'those', 'comments', 'on', 'ref', '2', 'pointed', 'out', 'by', 'mishra', 'et', 'al', 'in', 'ref1', 'are', 'not', 'relevant', 'and', 'the', 'concept', 'used', 'i... | [-0.037899648607154154, 0.1622284464732123, -0.030573499906971675, 0.05696902577793004, -0.0660802487150899, -0.13041433955853185, 0.027439721483027653, 0.36055414374208167, -0.1282732103954047, -0.33135792289284016, 0.05020230634753326, -0.35069555181655143, -0.15527684172238446, 0.16925905494662447, -0.13274124484520... |
709.074 | High-temperature behaviour of the helium-like K ALPHA G ratio: the
effect of improved recombination rate coefficients for calcium, iron, and
nickel | It is shown that above the temperature of maximum abundance, recombination
rates into the excited states of He-like ions that are calculated using
earlier, more approximate methods differ markedly from rates obtained from
recent distorted-wave and R-Matrix calculations (unified recombination rate
coefficients) for Ca... | astro-ph physics.atom-ph | it is shown that above the temperature of maximum abundance recombination rates into the excited states of helike ions that are calculated using earlier more approximate methods differ markedly from rates obtained from recent distortedwave and rmatrix calculations unified recombination rate coefficients for ca fe and n... | [['it', 'is', 'shown', 'that', 'above', 'the', 'temperature', 'of', 'maximum', 'abundance', 'recombination', 'rates', 'into', 'the', 'excited', 'states', 'of', 'helike', 'ions', 'that', 'are', 'calculated', 'using', 'earlier', 'more', 'approximate', 'methods', 'differ', 'markedly', 'from', 'rates', 'obtained', 'from', ... | [0.0011062182926835904, 0.0851258174800634, -0.02082814298612812, 0.07590589040396238, 0.03562893659740203, -0.12202248402039399, 0.08850234513924607, 0.4197671971966349, -0.18618186460879013, -0.3373529632355421, 0.022686151245552053, -0.3020959850329593, -0.011340151271224733, 0.2861520674076102, 0.047613844175943894... |
709.0741 | Galois extensions and subspaces of bilinear forms with special rank
properties | Let K be a field admitting a cyclic Galois extension of degree n. The main
result of this paper is a decomposition theorem for the space of alternating
bilinear forms defined on a vector space of odd dimension n over K. We show
that this space of forms is the direct sum of (n-1)/2 subspaces, each of
dimension n, and ... | math.AC | let k be a field admitting a cyclic galois extension of degree n the main result of this paper is a decomposition theorem for the space of alternating bilinear forms defined on a vector space of odd dimension n over k we show that this space of forms is the direct sum of n12 subspaces each of dimension n and the nonzer... | [['let', 'k', 'be', 'a', 'field', 'admitting', 'a', 'cyclic', 'galois', 'extension', 'of', 'degree', 'n', 'the', 'main', 'result', 'of', 'this', 'paper', 'is', 'a', 'decomposition', 'theorem', 'for', 'the', 'space', 'of', 'alternating', 'bilinear', 'forms', 'defined', 'on', 'a', 'vector', 'space', 'of', 'odd', 'dimensi... | [-0.22007804100027645, 0.17291361338184139, -0.027543137288942445, -0.014608447000071346, -0.03448270132276611, -0.13746992932235608, 0.005975056064628126, 0.2968926804720378, -0.30495013770376345, -0.2172550170483892, 0.07422357622522587, -0.25958940244783635, -0.12549324351130053, 0.1513881950684991, -0.0267012333936... |
709.0742 | Suppression of elliptic flow in a minimally viscous quark-gluon plasma | We compute the time evolution of elliptic flow in non-central relativistic
heavy-ion collisions, using a (2+1)-dimensional code with longitudinal
boost-invariance to simulate viscous fluid dynamics in the causal
Israel-Stewart formulation. We show that even ``minimal'' shear viscosity
eta/s=hbar/(4pi) leads to a larg... | nucl-th | we compute the time evolution of elliptic flow in noncentral relativistic heavyion collisions using a 21dimensional code with longitudinal boostinvariance to simulate viscous fluid dynamics in the causal israelstewart formulation we show that even minimal shear viscosity etashbar4pi leads to a large reduction of ellipt... | [['we', 'compute', 'the', 'time', 'evolution', 'of', 'elliptic', 'flow', 'in', 'noncentral', 'relativistic', 'heavyion', 'collisions', 'using', 'a', '21dimensional', 'code', 'with', 'longitudinal', 'boostinvariance', 'to', 'simulate', 'viscous', 'fluid', 'dynamics', 'in', 'the', 'causal', 'israelstewart', 'formulation'... | [-0.13252534953062423, 0.15871418084046154, -0.18793185845468985, 0.08266882467168299, -0.06142980469898744, -0.13730371270723868, -0.14056846214931062, 0.252804828024554, -0.31682997343666625, -0.2705585519627978, 0.01956051805719846, -0.323389030654322, 0.022152148204799178, 0.16956713795661926, -0.01721257558374694,... |
709.0743 | Semitransitive and transitive subsemigroups of the inverse symmetric
semigroups | We classify minimal transitive subsemigroups of the finitary inverse
symmetric semigroup modulo the classification of minimal transitive subgroups
of finite symmetric groups; and semitransitive subsemigroups of the finite
inverse symmetric semigroup of the minimal cardinality modulo the
classification of transitive s... | math.GR | we classify minimal transitive subsemigroups of the finitary inverse symmetric semigroup modulo the classification of minimal transitive subgroups of finite symmetric groups and semitransitive subsemigroups of the finite inverse symmetric semigroup of the minimal cardinality modulo the classification of transitive subg... | [['we', 'classify', 'minimal', 'transitive', 'subsemigroups', 'of', 'the', 'finitary', 'inverse', 'symmetric', 'semigroup', 'modulo', 'the', 'classification', 'of', 'minimal', 'transitive', 'subgroups', 'of', 'finite', 'symmetric', 'groups', 'and', 'semitransitive', 'subsemigroups', 'of', 'the', 'finite', 'inverse', 's... | [-0.17702531601701463, 0.14691498847108106, 0.014417060061681027, 0.11898132938207412, -0.1658779669705094, -0.1181321640555956, 0.04304931368393709, 0.3400885646934716, -0.4043277042860888, -0.11368841130514534, 0.14924811791362508, -0.353621523751288, 0.0037213807678496353, 0.12234034723773295, -0.161995781091403, 0.... |
709.0744 | The High Voltage Feedthroughs for the ATLAS Liquid Argon Calorimeters | The purpose, design specifications, construction techniques, and testing
methods are described for the high voltage feedthrough ports and filters of the
ATLAS Liquid Argon calorimeters. These feedthroughs carry about 5000 high
voltage wires from a room-temperature environment (300 K) through the cryostat
walls to the... | physics.ins-det | the purpose design specifications construction techniques and testing methods are described for the high voltage feedthrough ports and filters of the atlas liquid argon calorimeters these feedthroughs carry about 5000 high voltage wires from a roomtemperature environment 300 k through the cryostat walls to the calorime... | [['the', 'purpose', 'design', 'specifications', 'construction', 'techniques', 'and', 'testing', 'methods', 'are', 'described', 'for', 'the', 'high', 'voltage', 'feedthrough', 'ports', 'and', 'filters', 'of', 'the', 'atlas', 'liquid', 'argon', 'calorimeters', 'these', 'feedthroughs', 'carry', 'about', '5000', 'high', 'v... | [-0.12748020262746462, 0.1841306559227664, 0.007560352302402601, -0.043587881992785155, -0.006945852200960976, -0.22335592794349823, 0.0827045736449032, 0.3975544785759572, -0.20534749562456006, -0.39782350816517725, 0.11401456339691562, -0.31950777271312886, 0.03883958844221786, 0.2051505943647875, -0.0290550372386672... |
709.0745 | Comment on 'Discreteness Effects in Simulations of Hot/Warm Dark Matter'
by J. Wang & S.D.M. White | Wang and White (2007) have discussed some problems with N-body simulation
methods. These problems are a special case of a more general problem which has
been largely unacknowledged for approximately 25 years, and affects results of
all dark matter simulations on small scales (the definition of 'small' varying
with ti... | astro-ph | wang and white 2007 have discussed some problems with nbody simulation methods these problems are a special case of a more general problem which has been largely unacknowledged for approximately 25 years and affects results of all dark matter simulations on small scales the definition of small varying with time extensi... | [['wang', 'and', 'white', '2007', 'have', 'discussed', 'some', 'problems', 'with', 'nbody', 'simulation', 'methods', 'these', 'problems', 'are', 'a', 'special', 'case', 'of', 'a', 'more', 'general', 'problem', 'which', 'has', 'been', 'largely', 'unacknowledged', 'for', 'approximately', '25', 'years', 'and', 'affects', ... | [-0.0909671672998229, 0.1768545945551956, -0.06890704862529501, 0.05993875207648324, -0.03865390861894758, -0.104206360208558, -0.03560904457256021, 0.3376476479295109, -0.22862863352721824, -0.3953540597022289, 0.08813473954381022, -0.2789565231166004, -0.09669674388715066, 0.22869186852906187, -0.03733595916058957, 0... |
709.0746 | Geometric Complexity Theory: Introduction | These are lectures notes for the introductory graduate courses on geometric
complexity theory (GCT) in the computer science department, the university of
Chicago. Part I consists of the lecture notes for the course given by the first
author in the spring quarter, 2007. It gives introduction to the basic
structure of ... | cs.CC | these are lectures notes for the introductory graduate courses on geometric complexity theory gct in the computer science department the university of chicago part i consists of the lecture notes for the course given by the first author in the spring quarter 2007 it gives introduction to the basic structure of gct part... | [['these', 'are', 'lectures', 'notes', 'for', 'the', 'introductory', 'graduate', 'courses', 'on', 'geometric', 'complexity', 'theory', 'gct', 'in', 'the', 'computer', 'science', 'department', 'the', 'university', 'of', 'chicago', 'part', 'i', 'consists', 'of', 'the', 'lecture', 'notes', 'for', 'the', 'course', 'given',... | [-0.07209169449244472, 0.10702401649528484, -0.11973050977237415, 0.06193673978274916, -0.1260163574714026, -0.1231424544046787, -0.03963150832343096, 0.2602582709032962, -0.20233703562453817, -0.3822908176363801, 0.14465253926284288, -0.2717835656065735, -0.188664954257861, 0.16086906749292834, -0.16595376238328494, -... |
709.0747 | On Lyubeznik numbers of projective schemes | Let $X$ be an arbitrary projective scheme over a field $k$. Let $A$ be the
local ring at the vertex of the affine cone for some embedding $\iota:
X\hookrightarrow \mathbb{P}^n_k$. G. Lyubeznik asked (in \cite{l2}) whether the
integers $\lambda_{i,j}(A)$ (defined in \cite{l1}), called the Lyubeznik
numbers of $A$, dep... | math.AC math.AG | let x be an arbitrary projective scheme over a field k let a be the local ring at the vertex of the affine cone for some embedding iota xhookrightarrow mathbbpn_k g lyubeznik asked in citel2 whether the integers lambda_ija defined in citel1 called the lyubeznik numbers of a depend only on x but not on the embedding in ... | [['let', 'x', 'be', 'an', 'arbitrary', 'projective', 'scheme', 'over', 'a', 'field', 'k', 'let', 'a', 'be', 'the', 'local', 'ring', 'at', 'the', 'vertex', 'of', 'the', 'affine', 'cone', 'for', 'some', 'embedding', 'iota', 'xhookrightarrow', 'mathbbpn_k', 'g', 'lyubeznik', 'asked', 'in', 'citel2', 'whether', 'the', 'int... | [-0.19579470707057958, 0.08629894711881278, -0.0848830842513445, 0.015005599230290483, -0.06468655972275883, -0.18607182789356538, 0.02942854278451562, 0.3448399697686089, -0.33978697255838153, -0.21605977578563432, 0.07293558388254513, -0.23679223993573995, -0.09597478765656478, 0.20403298595007144, -0.120694290673104... |
709.0748 | On P vs. NP, Geometric Complexity Theory, and the Flip I: a high level
view | Geometric complexity theory (GCT) is an approach to the $P$ vs. $NP$ and
related problems through algebraic geometry and representation theory. This
article gives a high-level exposition of the basic plan of GCT based on the
principle, called the flip, without assuming any background in algebraic
geometry or represen... | cs.CC | geometric complexity theory gct is an approach to the p vs np and related problems through algebraic geometry and representation theory this article gives a highlevel exposition of the basic plan of gct based on the principle called the flip without assuming any background in algebraic geometry or representation theory | [['geometric', 'complexity', 'theory', 'gct', 'is', 'an', 'approach', 'to', 'the', 'p', 'vs', 'np', 'and', 'related', 'problems', 'through', 'algebraic', 'geometry', 'and', 'representation', 'theory', 'this', 'article', 'gives', 'a', 'highlevel', 'exposition', 'of', 'the', 'basic', 'plan', 'of', 'gct', 'based', 'on', '... | [-0.08206821492873133, 0.045959777254902294, -0.190917062968947, 0.10536697878502309, -0.15127890851348638, -0.13320956441573797, 0.024218453431967647, 0.26717382777482274, -0.3195021311193705, -0.342856072075665, 0.0635245217452757, -0.21390263732522727, -0.23703663226682692, 0.16765594385098667, -0.1598954270593822, ... |
709.0749 | Geometric Complexity Theory VII: Nonstandard quantum group for the
plethysm problem | This article describes a {\em nonstandard} quantum group that may be used to
derive a positive formula for the plethysm problem, just as the standard
(Drinfeld-Jimbo) quantum group can be used to derive the positive
Littlewood-Richardson rule for arbitrary complex semisimple Lie groups. The
sequel \cite{GCT8} gives c... | cs.CC | this article describes a em nonstandard quantum group that may be used to derive a positive formula for the plethysm problem just as the standard drinfeldjimbo quantum group can be used to derive the positive littlewoodrichardson rule for arbitrary complex semisimple lie groups the sequel citegct8 gives conjecturally c... | [['this', 'article', 'describes', 'a', 'em', 'nonstandard', 'quantum', 'group', 'that', 'may', 'be', 'used', 'to', 'derive', 'a', 'positive', 'formula', 'for', 'the', 'plethysm', 'problem', 'just', 'as', 'the', 'standard', 'drinfeldjimbo', 'quantum', 'group', 'can', 'be', 'used', 'to', 'derive', 'the', 'positive', 'lit... | [-0.15099683461353333, 0.07686368243373705, -0.12719615723119315, 0.12212083259517459, -0.15886729375242886, -0.1827016626202473, 0.018646988493268086, 0.297104586263874, -0.349111045489671, -0.20852091604334566, 0.06673220862314631, -0.1811190451862234, -0.1748383466220188, 0.18592035904470267, -0.10157810165687944, -... |
709.075 | Reddening law and interstellar dust properties along Magellanic
sight-lines | This study establishes that SMC, LMC and Milky Way extinction curves obey the
same extinction law which depends on the 2200A bump size and one parameter, and
generalizes the Cardelli, Clayton and Mathis (1989) relationship. This suggests
that extinction in all three galaxies is of the same nature. The role of linear
... | astro-ph | this study establishes that smc lmc and milky way extinction curves obey the same extinction law which depends on the 2200a bump size and one parameter and generalizes the cardelli clayton and mathis 1989 relationship this suggests that extinction in all three galaxies is of the same nature the role of linear reddening... | [['this', 'study', 'establishes', 'that', 'smc', 'lmc', 'and', 'milky', 'way', 'extinction', 'curves', 'obey', 'the', 'same', 'extinction', 'law', 'which', 'depends', 'on', 'the', '2200a', 'bump', 'size', 'and', 'one', 'parameter', 'and', 'generalizes', 'the', 'cardelli', 'clayton', 'and', 'mathis', '1989', 'relationsh... | [-0.0632529223075835, 0.0460830248426646, -0.14668090376071632, 0.09487600501161068, -0.08285201149410568, -0.07359964947681874, 0.06626042941061314, 0.37408895692788063, -0.21377188634942285, -0.3040691690519452, 0.013663645129418001, -0.2361157810606528, -0.12296455013565719, 0.22792899563210084, -0.11581089659593999... |
709.0751 | Geometric Complexity Theory VIII: On canonical bases for the nonstandard
quantum groups | This article gives conjecturally correct algorithms to construct canonical
bases of the irreducible polynomial representations and the matrix coordinate
rings of the nonstandard quantum groups in GCT4 and GCT7, and canonical bases
of the dually paired nonstandard deformations of the symmetric group algebra
therein. T... | cs.CC | this article gives conjecturally correct algorithms to construct canonical bases of the irreducible polynomial representations and the matrix coordinate rings of the nonstandard quantum groups in gct4 and gct7 and canonical bases of the dually paired nonstandard deformations of the symmetric group algebra therein these... | [['this', 'article', 'gives', 'conjecturally', 'correct', 'algorithms', 'to', 'construct', 'canonical', 'bases', 'of', 'the', 'irreducible', 'polynomial', 'representations', 'and', 'the', 'matrix', 'coordinate', 'rings', 'of', 'the', 'nonstandard', 'quantum', 'groups', 'in', 'gct4', 'and', 'gct7', 'and', 'canonical', '... | [-0.14716034806380518, 0.06901919182314716, -0.11352656086709237, 0.06759367879912859, -0.11050108658394428, -0.13573851611822693, -0.019757499339792765, 0.2891536003467862, -0.386235799226496, -0.18343433737490242, 0.061651295032164065, -0.2096594985988405, -0.179272420459775, 0.15548082545512554, -0.09573207563259686... |
709.0752 | Sky in Google Earth: The Next Frontier in Astronomical Data Discovery
and Visualization | Astronomy began as a visual science, first through careful observations of
the sky using either an eyepiece or the naked eye, then on to the preservation
of those images with photographic media and finally the digital encoding of
that information via CCDs. This last step has enabled astronomy to move into a
fully aut... | astro-ph | astronomy began as a visual science first through careful observations of the sky using either an eyepiece or the naked eye then on to the preservation of those images with photographic media and finally the digital encoding of that information via ccds this last step has enabled astronomy to move into a fully automate... | [['astronomy', 'began', 'as', 'a', 'visual', 'science', 'first', 'through', 'careful', 'observations', 'of', 'the', 'sky', 'using', 'either', 'an', 'eyepiece', 'or', 'the', 'naked', 'eye', 'then', 'on', 'to', 'the', 'preservation', 'of', 'those', 'images', 'with', 'photographic', 'media', 'and', 'finally', 'the', 'digi... | [-0.05303137772279341, 0.056885837608641736, -0.10588149730763245, 0.05432968225171512, -0.19397337780609517, -0.11545488847410874, 0.06034606497433089, 0.4383131996881514, -0.24672340004849183, -0.345054961347454, 0.17398567879168064, -0.314491841867741, -0.11445689767581617, 0.2529010757795172, -0.08087093202821351, ... |
709.0753 | On the structure of the Si(103) surface | Although (103) is a stable nominal orientation for both silicon and
germanium, experimental observations revealed that in the case of silicon this
surface remains disordered on an atomic scale even after careful annealing. We
report here a set of low-energy reconstruction models corresponding to $1\times
2$, $2\times... | cond-mat.mtrl-sci | although 103 is a stable nominal orientation for both silicon and germanium experimental observations revealed that in the case of silicon this surface remains disordered on an atomic scale even after careful annealing we report here a set of lowenergy reconstruction models corresponding to 1times 2 2times 2 and 1times... | [['although', '103', 'is', 'a', 'stable', 'nominal', 'orientation', 'for', 'both', 'silicon', 'and', 'germanium', 'experimental', 'observations', 'revealed', 'that', 'in', 'the', 'case', 'of', 'silicon', 'this', 'surface', 'remains', 'disordered', 'on', 'an', 'atomic', 'scale', 'even', 'after', 'careful', 'annealing', ... | [-0.08513862003411095, 0.19850197806968375, -0.010451225483288558, 0.045730060033607654, 0.04571677212907861, -0.12845686636193512, 0.028245638993282158, 0.4391530531888398, -0.20566864302740073, -0.38025931489224046, 0.1046756704924449, -0.2850896088549724, -0.12918106484665678, 0.1982346776371392, 0.01104125083656981... |
709.0754 | Coherent Control of Trapped Bosons | We investigate the quantum behavior of a mesoscopic two-boson system produced
by number-squeezing ultracold gases of alkali metal atoms. The quantum Poincare
maps of the wavefunctions are affected by chaos in those regions of the phase
space where the classical dynamics produces features that are comparable to
hbar. ... | physics.atom-ph | we investigate the quantum behavior of a mesoscopic twoboson system produced by numbersqueezing ultracold gases of alkali metal atoms the quantum poincare maps of the wavefunctions are affected by chaos in those regions of the phase space where the classical dynamics produces features that are comparable to hbar we als... | [['we', 'investigate', 'the', 'quantum', 'behavior', 'of', 'a', 'mesoscopic', 'twoboson', 'system', 'produced', 'by', 'numbersqueezing', 'ultracold', 'gases', 'of', 'alkali', 'metal', 'atoms', 'the', 'quantum', 'poincare', 'maps', 'of', 'the', 'wavefunctions', 'are', 'affected', 'by', 'chaos', 'in', 'those', 'regions',... | [-0.16857272940687834, 0.2856736978593593, -0.0801934746055243, 0.043925378165052584, 0.056091849342919886, -0.10797104477339113, 0.08959181306806083, 0.346020931036522, -0.29284615302458405, -0.23182088340787838, 0.02361370538613604, -0.2781988921769274, -0.13872753416653721, 0.21224179941539964, 0.01110764421755448, ... |
709.0755 | Perfect state transfer over distance-regular spin networks | By considering distance-regular graphs as spin networks, first we introduce
some particular spin Hamiltonians which are extended version of those of
Refs.\cite{8,9''}. Then, by using spectral analysis techniques and algebraic
combinatoric structure of distance-regular graphs such as stratification
introduced in \cite... | quant-ph | by considering distanceregular graphs as spin networks first we introduce some particular spin hamiltonians which are extended version of those of refscite89 then by using spectral analysis techniques and algebraic combinatoric structure of distanceregular graphs such as stratification introduced in citeobata js and bo... | [['by', 'considering', 'distanceregular', 'graphs', 'as', 'spin', 'networks', 'first', 'we', 'introduce', 'some', 'particular', 'spin', 'hamiltonians', 'which', 'are', 'extended', 'version', 'of', 'those', 'of', 'refscite89', 'then', 'by', 'using', 'spectral', 'analysis', 'techniques', 'and', 'algebraic', 'combinatoric... | [-0.1432343949299221, 0.11997746780627605, -0.034657604597283134, 0.06920791033277937, -0.06286742113474192, -0.17668951576386904, 0.026449305986082465, 0.405442159174885, -0.2780562481105638, -0.28960286878811364, 0.12232364972023237, -0.24524970227767798, -0.20111729034794157, 0.17457444344428508, -0.0527518750477060... |
709.0756 | Calculating effective resistances on underlying networks of association
schemes | Recently, in Refs. \cite{jsj} and \cite{res2}, calculation of effective
resistances on distance-regular networks was investigated, where in the first
paper, the calculation was based on stratification and Stieltjes function
associated with the network, whereas in the latter one a recursive formula for
effective resis... | math-ph math.MP | recently in refs citejsj and citeres2 calculation of effective resistances on distanceregular networks was investigated where in the first paper the calculation was based on stratification and stieltjes function associated with the network whereas in the latter one a recursive formula for effective resistances was give... | [['recently', 'in', 'refs', 'citejsj', 'and', 'citeres2', 'calculation', 'of', 'effective', 'resistances', 'on', 'distanceregular', 'networks', 'was', 'investigated', 'where', 'in', 'the', 'first', 'paper', 'the', 'calculation', 'was', 'based', 'on', 'stratification', 'and', 'stieltjes', 'function', 'associated', 'with... | [-0.14347562833158467, 0.07029375483850615, -0.047219178407570464, 0.04363306583721308, -0.062381308309750645, -0.1743322729367998, 0.03800212588425524, 0.3893264656475334, -0.25148608141603906, -0.24278980301447142, 0.09150023630197235, -0.2560916933470179, -0.2054149367687133, 0.1606059688193774, -0.04989575383175785... |
709.0757 | Morita equivalence of dual operator algebras | We consider a variant of the notion of Morita equivalence appropriate to
weak* closed algebras of Hilbert space operators, which we call {\em weak
Morita equivalence}. We obtain new variants, appropriate to the dual algebra
setting, of the basic theory of strong Morita equivalence, and new
nonselfadjoint variants of ... | math.OA math.FA | we consider a variant of the notion of morita equivalence appropriate to weak closed algebras of hilbert space operators which we call em weak morita equivalence we obtain new variants appropriate to the dual algebra setting of the basic theory of strong morita equivalence and new nonselfadjoint variants of aspects of ... | [['we', 'consider', 'a', 'variant', 'of', 'the', 'notion', 'of', 'morita', 'equivalence', 'appropriate', 'to', 'weak', 'closed', 'algebras', 'of', 'hilbert', 'space', 'operators', 'which', 'we', 'call', 'em', 'weak', 'morita', 'equivalence', 'we', 'obtain', 'new', 'variants', 'appropriate', 'to', 'the', 'dual', 'algebr... | [-0.18998696757480502, 0.07787329836494543, -0.04921763640066439, 0.20736306489191272, -0.14139472652988677, -0.2148979669521478, -0.003474371433681385, 0.3314298805526712, -0.45839526612650267, -0.16022805764593862, 0.05727499751374125, -0.16706828671422871, -0.13772579738870264, 0.09772956205362623, -0.21411936352537... |
709.0758 | Simulation of an All-Silicon Tracker | We present recent improvements in the performance of the reconstruction of
non-prompt track in the SiD Detector Concept Design, including initial results
on the effect of longitudinal segmentation in the SiD tracker. We also describe
a generic tracking validation package developed at SCIPP.
| physics.ins-det | we present recent improvements in the performance of the reconstruction of nonprompt track in the sid detector concept design including initial results on the effect of longitudinal segmentation in the sid tracker we also describe a generic tracking validation package developed at scipp | [['we', 'present', 'recent', 'improvements', 'in', 'the', 'performance', 'of', 'the', 'reconstruction', 'of', 'nonprompt', 'track', 'in', 'the', 'sid', 'detector', 'concept', 'design', 'including', 'initial', 'results', 'on', 'the', 'effect', 'of', 'longitudinal', 'segmentation', 'in', 'the', 'sid', 'tracker', 'we', 'a... | [-0.04617675145286634, 0.007068834018482025, -0.10978972816536593, 0.013891022565752961, -0.01144058281165916, -0.1074089361463002, -0.10044343079180391, 0.3764647401566076, -0.16512280871528526, -0.3265799232866875, 0.07221128196228123, -0.2972242645919323, -0.12165271746384543, 0.20119304095698132, -0.091621220133505... |
709.0759 | Optical Cluster-Finding with An Adaptive Matched-Filter Technique:
Algorithm and Comparison with Simulations | We present a modified adaptive matched filter algorithm designed to identify
clusters of galaxies in wide-field imaging surveys such as the Sloan Digital
Sky Survey. The cluster-finding technique is fully adaptive to imaging surveys
with spectroscopic coverage, multicolor photometric redshifts, no redshift
informatio... | astro-ph | we present a modified adaptive matched filter algorithm designed to identify clusters of galaxies in widefield imaging surveys such as the sloan digital sky survey the clusterfinding technique is fully adaptive to imaging surveys with spectroscopic coverage multicolor photometric redshifts no redshift information at al... | [['we', 'present', 'a', 'modified', 'adaptive', 'matched', 'filter', 'algorithm', 'designed', 'to', 'identify', 'clusters', 'of', 'galaxies', 'in', 'widefield', 'imaging', 'surveys', 'such', 'as', 'the', 'sloan', 'digital', 'sky', 'survey', 'the', 'clusterfinding', 'technique', 'is', 'fully', 'adaptive', 'to', 'imaging... | [-0.026130584411199063, 0.047857524389932536, -0.06639060455136528, 0.09437980527060141, -0.10982677986232928, -0.03939015823308854, 0.06095745217728266, 0.4492443167179337, -0.1663106397862303, -0.39346518398910435, 0.08725593705299695, -0.3112897373072844, -0.011314889618560024, 0.2456327194755115, -0.020522804848872... |
709.076 | Quantum electron transport in toroidal carbon nanotubes with metallic
leads | A recursive Green's function method is employed to calculate the
density-of-states, transmission function, and current through a 150 layer (3,3)
armchair nanotorus (1800 atoms) with laterally attached metallic leads as
functions of relative lead angle and magnetic flux. Plateaus in the
transmissivity through the toru... | quant-ph | a recursive greens function method is employed to calculate the densityofstates transmission function and current through a 150 layer 33 armchair nanotorus 1800 atoms with laterally attached metallic leads as functions of relative lead angle and magnetic flux plateaus in the transmissivity through the torus occur over ... | [['a', 'recursive', 'greens', 'function', 'method', 'is', 'employed', 'to', 'calculate', 'the', 'densityofstates', 'transmission', 'function', 'and', 'current', 'through', 'a', '150', 'layer', '33', 'armchair', 'nanotorus', '1800', 'atoms', 'with', 'laterally', 'attached', 'metallic', 'leads', 'as', 'functions', 'of', ... | [-0.1632243077414976, 0.15694299499458358, -0.007434070608775381, -0.00291356632918854, -0.02630918405451615, -0.12230408989207846, 0.09199681148280613, 0.4328695988990891, -0.26504068564571126, -0.3351607801733722, 0.010001309304563721, -0.251675199940276, -0.08869946769661677, 0.2468701044595997, 0.017573691878310392... |
709.0761 | The coupling between pulsation and mass loss in massive stars | To what extent can pulsational instabilities resolve the mass-loss problem of
massive stars? How important is pulsation in structuring and modulating the
winds of these stars? What role does pulsation play in redistributing angular
momentum in massive stars? Although I cannot offer answers to these questions,
I hope ... | astro-ph | to what extent can pulsational instabilities resolve the massloss problem of massive stars how important is pulsation in structuring and modulating the winds of these stars what role does pulsation play in redistributing angular momentum in massive stars although i cannot offer answers to these questions i hope at the ... | [['to', 'what', 'extent', 'can', 'pulsational', 'instabilities', 'resolve', 'the', 'massloss', 'problem', 'of', 'massive', 'stars', 'how', 'important', 'is', 'pulsation', 'in', 'structuring', 'and', 'modulating', 'the', 'winds', 'of', 'these', 'stars', 'what', 'role', 'does', 'pulsation', 'play', 'in', 'redistributing'... | [-0.07496858646207658, 0.21660061052343885, -0.10824495032582371, 0.1808159863061012, -0.21866020198422867, -0.1245791572833159, 0.061851067743340475, 0.42192349375271404, -0.2633650272657148, -0.3561683054097363, 0.03782442885596061, -0.24709693776046643, -0.07926743211163605, 0.17001109358808789, -0.14045819814973434... |
709.0762 | Regularizations of the Euler product representation for zeta functions
and the Birch--Swinnerton-Dyer conjecture | We consider a variant expression to regularize the Euler product
representation of the zeta functions, where we mainly apply to that of the
Riemann zeta function in this paper. The regularization itself is identical to
that of the zeta function of the summation expression, but the non-use of the
M\"oebius function en... | math-ph math.MP | we consider a variant expression to regularize the euler product representation of the zeta functions where we mainly apply to that of the riemann zeta function in this paper the regularization itself is identical to that of the zeta function of the summation expression but the nonuse of the moebius function enable us ... | [['we', 'consider', 'a', 'variant', 'expression', 'to', 'regularize', 'the', 'euler', 'product', 'representation', 'of', 'the', 'zeta', 'functions', 'where', 'we', 'mainly', 'apply', 'to', 'that', 'of', 'the', 'riemann', 'zeta', 'function', 'in', 'this', 'paper', 'the', 'regularization', 'itself', 'is', 'identical', 't... | [-0.16044548671463044, 0.027256682555536114, -0.16432899231456707, 0.08403166913248981, -0.1086283240980843, -0.08776367945753247, 0.03458688492238278, 0.2892308033497952, -0.2928790941521108, -0.2333506584737589, 0.09584650849253287, -0.25049068307434424, -0.17987448904907036, 0.1831776938166156, -0.05380439338770425,... |
709.0763 | U(1)' solution to the mu-problem and the proton decay problem in
supersymmetry without R-parity | The Minimal Supersymmetric Standard Model (MSSM) is plagued by two major
fine-tuning problems: the mu-problem and the proton decay problem. We present a
simultaneous solution to both problems within the framework of a U(1)'-extended
MSSM (UMSSM), without requiring R-parity conservation. We identify several
classes of... | hep-ph | the minimal supersymmetric standard model mssm is plagued by two major finetuning problems the muproblem and the proton decay problem we present a simultaneous solution to both problems within the framework of a u1extended mssm umssm without requiring rparity conservation we identify several classes of phenomenological... | [['the', 'minimal', 'supersymmetric', 'standard', 'model', 'mssm', 'is', 'plagued', 'by', 'two', 'major', 'finetuning', 'problems', 'the', 'muproblem', 'and', 'the', 'proton', 'decay', 'problem', 'we', 'present', 'a', 'simultaneous', 'solution', 'to', 'both', 'problems', 'within', 'the', 'framework', 'of', 'a', 'u1exte... | [-0.12531369087837968, 0.22446917255177715, 0.018941741592434655, 0.19737677973736623, -0.12646321137435734, -0.2234024194778821, 0.053214534972696105, 0.26795359563740906, -0.20357280546075598, -0.33905512576175345, 0.09140289254237417, -0.2532288392881157, -0.05992372543551028, 0.09328291313960009, -0.012551741111003... |
709.0764 | On the ruin time distribution for a Sparre Andersen process with
exponential claim sizes | We derive a closed-form (infinite series) representation for the distribution
of the ruin time for the Sparre Andersen model with exponentially distributed
claims. This extends a recent result of Dickson et al. (2005) for such
processes with Erlang inter-claim times. We illustrate our result in the cases
of gamma and... | math.PR | we derive a closedform infinite series representation for the distribution of the ruin time for the sparre andersen model with exponentially distributed claims this extends a recent result of dickson et al 2005 for such processes with erlang interclaim times we illustrate our result in the cases of gamma and mixed expo... | [['we', 'derive', 'a', 'closedform', 'infinite', 'series', 'representation', 'for', 'the', 'distribution', 'of', 'the', 'ruin', 'time', 'for', 'the', 'sparre', 'andersen', 'model', 'with', 'exponentially', 'distributed', 'claims', 'this', 'extends', 'a', 'recent', 'result', 'of', 'dickson', 'et', 'al', '2005', 'for', '... | [-0.08387835254384712, 0.07273330624977296, -0.11149841563945467, 0.03895363525529815, -0.010286625051362948, -0.09032153954560107, 0.10409889576787298, 0.32853094503622166, -0.2369028399486772, -0.28697531177577645, 0.09437925089785659, -0.24159355017949236, -0.13314380191943861, 0.1820602893490683, -0.112205536722798... |
709.0765 | Leptonic color models from Z_8 orbifolded AdS/CFT | We study orbifold compactifications of the type IIB superstring on AdS_5 x
S^5/Gamma, where Gamma is the abelian group Z_8, which can lead to non-SUSY
three and four family models based on quartification. In particular, we focus
on two models, one fully quartified model and one a model with two
trinification families... | hep-ph | we study orbifold compactifications of the type iib superstring on ads_5 x s5gamma where gamma is the abelian group z_8 which can lead to nonsusy three and four family models based on quartification in particular we focus on two models one fully quartified model and one a model with two trinification families and one q... | [['we', 'study', 'orbifold', 'compactifications', 'of', 'the', 'type', 'iib', 'superstring', 'on', 'ads_5', 'x', 's5gamma', 'where', 'gamma', 'is', 'the', 'abelian', 'group', 'z_8', 'which', 'can', 'lead', 'to', 'nonsusy', 'three', 'and', 'four', 'family', 'models', 'based', 'on', 'quartification', 'in', 'particular', ... | [-0.0792014769730017, 0.1318444942095966, -0.027350977500618406, 0.11350386675313172, -0.09384304696383576, -0.23884465820579368, 0.001863597080845273, 0.3449373379928257, -0.17979692498391325, -0.2559317325411195, 0.1354500834431471, -0.2943515630128483, -0.10833782984903365, 0.15660152457668586, -0.06522650745076437,... |
709.0766 | Search for Gravitational Waves Associated with 39 Gamma-Ray Bursts Using
Data from the Second, Third, and Fourth LIGO Runs | We present the results of a search for short-duration gravitational-wave
bursts associated with 39 gamma-ray bursts (GRBs) detected by gamma-ray
satellite experiments during LIGO's S2, S3, and S4 science runs. The search
involves calculating the crosscorrelation between two interferometer data
streams surrounding the... | gr-qc astro-ph | we present the results of a search for shortduration gravitationalwave bursts associated with 39 gammaray bursts grbs detected by gammaray satellite experiments during ligos s2 s3 and s4 science runs the search involves calculating the crosscorrelation between two interferometer data streams surrounding the grb trigger... | [['we', 'present', 'the', 'results', 'of', 'a', 'search', 'for', 'shortduration', 'gravitationalwave', 'bursts', 'associated', 'with', '39', 'gammaray', 'bursts', 'grbs', 'detected', 'by', 'gammaray', 'satellite', 'experiments', 'during', 'ligos', 's2', 's3', 'and', 's4', 'science', 'runs', 'the', 'search', 'involves',... | [-0.11090911860071917, 0.1132080054080804, -0.020764763657296747, 0.1436379332010289, -0.08856137638183566, -0.03949518718752008, 0.08329624337082739, 0.3907462421418782, -0.15894666176790437, -0.33967436017317293, 0.10878609962522662, -0.3344036208720982, -0.06322898757691273, 0.3085177415901521, 0.06016815044009481, ... |
709.0767 | Exact Foldy-Wouthuysen transformation for gravitational waves and
magnetic field background | We consider an exact Foldy-Wouthuysen transformation for the Dirac spinor
field on the combined background of a gravitational wave and constant uniform
magnetic field. By taking the classical limit of the spinor field Hamiltonian
we arrive at the equations of motion for the non-relativistic spinning
particle. Two dif... | gr-qc | we consider an exact foldywouthuysen transformation for the dirac spinor field on the combined background of a gravitational wave and constant uniform magnetic field by taking the classical limit of the spinor field hamiltonian we arrive at the equations of motion for the nonrelativistic spinning particle two different... | [['we', 'consider', 'an', 'exact', 'foldywouthuysen', 'transformation', 'for', 'the', 'dirac', 'spinor', 'field', 'on', 'the', 'combined', 'background', 'of', 'a', 'gravitational', 'wave', 'and', 'constant', 'uniform', 'magnetic', 'field', 'by', 'taking', 'the', 'classical', 'limit', 'of', 'the', 'spinor', 'field', 'ha... | [-0.1701688409825279, 0.19103434730588395, -0.04902545152316717, 0.09326419422551142, -0.0797737280711193, -0.06733021177774803, -0.04415170392021537, 0.31188420731235633, -0.20781551047482275, -0.29693794936492024, 0.0566321781529537, -0.20722951372577386, -0.0895912922241471, 0.24239283824889837, 0.06904857915995473,... |
709.0768 | Muon Identification without Iron | Muons can be identified with high efficiency and purity and reconstructed
with high precision is a detector with a dual readout calorimeter and a dual
solenoid to return the flux without iron. We shown CERN test beam data for the
calorimeter and calculations for the magnetic fields and the track
reconstruction. For i... | physics.ins-det | muons can be identified with high efficiency and purity and reconstructed with high precision is a detector with a dual readout calorimeter and a dual solenoid to return the flux without iron we shown cern test beam data for the calorimeter and calculations for the magnetic fields and the track reconstruction for isola... | [['muons', 'can', 'be', 'identified', 'with', 'high', 'efficiency', 'and', 'purity', 'and', 'reconstructed', 'with', 'high', 'precision', 'is', 'a', 'detector', 'with', 'a', 'dual', 'readout', 'calorimeter', 'and', 'a', 'dual', 'solenoid', 'to', 'return', 'the', 'flux', 'without', 'iron', 'we', 'shown', 'cern', 'test',... | [0.0005477929740330912, 0.26194198829659693, -0.03966520848670896, 0.07397690898915885, 0.05265285825671654, -0.1246964184134464, -0.000728166576894656, 0.3905895655633698, -0.1575336944784077, -0.4561495414187371, 0.018731684312486733, -0.40557001312066554, 0.17080182317172138, 0.19454919831486236, -0.0010903019484289... |
709.0769 | Strain Hardening of Polymer Glasses: Entanglements, Energetics, and
Plasticity | Simulations are used to examine the microscopic origins of strain hardening
in polymer glasses. While stress-strain curves for a wide range of temperature
can be fit to the functional form predicted by entropic network models, many
other results are fundamentally inconsistent with the physical picture
underlying thes... | cond-mat.soft cond-mat.mtrl-sci | simulations are used to examine the microscopic origins of strain hardening in polymer glasses while stressstrain curves for a wide range of temperature can be fit to the functional form predicted by entropic network models many other results are fundamentally inconsistent with the physical picture underlying these mod... | [['simulations', 'are', 'used', 'to', 'examine', 'the', 'microscopic', 'origins', 'of', 'strain', 'hardening', 'in', 'polymer', 'glasses', 'while', 'stressstrain', 'curves', 'for', 'a', 'wide', 'range', 'of', 'temperature', 'can', 'be', 'fit', 'to', 'the', 'functional', 'form', 'predicted', 'by', 'entropic', 'network',... | [-0.10989759687552268, 0.23327394458287248, -0.08888224869882291, 0.06706920047810777, -0.05511739355898363, -0.17521135768100143, 0.0015967931329678902, 0.40537502677080794, -0.3046599585455198, -0.28353625800871746, 0.06349288286304379, -0.27781715983663624, -0.11279825534810253, 0.15907106883489489, -0.0186436348545... |
709.077 | General K=-1 Friedman-Lema\^itre models and the averaging problem in
cosmology | We introduce the notion of general K=-1 Friedman-Lema\^itre (compact)
cosmologies and the notion of averaged evolution by means of an averaging map.
We then analyze the Friedman-Lema\^itre equations and the role of gravitational
energy on the universe evolution. We distinguish two asymptotic behaviors:
radiative and ... | gr-qc | we introduce the notion of general k1 friedmanlemaitre compact cosmologies and the notion of averaged evolution by means of an averaging map we then analyze the friedmanlemaitre equations and the role of gravitational energy on the universe evolution we distinguish two asymptotic behaviors radiative and mass gap we dis... | [['we', 'introduce', 'the', 'notion', 'of', 'general', 'k1', 'friedmanlemaitre', 'compact', 'cosmologies', 'and', 'the', 'notion', 'of', 'averaged', 'evolution', 'by', 'means', 'of', 'an', 'averaging', 'map', 'we', 'then', 'analyze', 'the', 'friedmanlemaitre', 'equations', 'and', 'the', 'role', 'of', 'gravitational', '... | [-0.13577943141162313, 0.10084150817402647, -0.10407317251782622, 0.12771148154423875, -0.03982681909282609, -0.06221937750240226, 0.015738894340455445, 0.36828347489502306, -0.26068631356262423, -0.2703399873695463, 0.09713924367507071, -0.24025972604960996, -0.08043506295701279, 0.15884158920948588, -0.02417068880605... |
709.0771 | Theory of light-induced current in molecular-tunneling junctions excited
with intense shaped pulses | A theory for light-induced current by strong optical pulses in
molecular-tunneling junctions is described. We consider a molecular bridge
represented by its highest occupied and lowest unoccupied levels, HOMO and
LUMO, respectively. We take into account two types of couplings between the
molecule and the metal leads:... | cond-mat.mes-hall cond-mat.other | a theory for lightinduced current by strong optical pulses in moleculartunneling junctions is described we consider a molecular bridge represented by its highest occupied and lowest unoccupied levels homo and lumo respectively we take into account two types of couplings between the molecule and the metal leads electron... | [['a', 'theory', 'for', 'lightinduced', 'current', 'by', 'strong', 'optical', 'pulses', 'in', 'moleculartunneling', 'junctions', 'is', 'described', 'we', 'consider', 'a', 'molecular', 'bridge', 'represented', 'by', 'its', 'highest', 'occupied', 'and', 'lowest', 'unoccupied', 'levels', 'homo', 'and', 'lumo', 'respective... | [-0.14469770108377722, 0.14961258126615953, -0.03245676435973768, 0.04833669632679285, 0.013848679237557447, -0.1660827787573939, 0.08289791050453366, 0.41101539358978384, -0.26215889186805097, -0.2764453922796308, -0.02998016581716064, -0.2792218272325358, -0.10549691075796326, 0.1900257010550784, 0.03443183314761725,... |
709.0772 | Astrophysics Motivation behind the Pierre Auger Southern Observatory
Enhancements | The Pierre Auger Collaboration intends to extend the energy range of its
southern observatory in Argentina for high quality data from 0.1 to 3 EeV. The
extensions, described in accompanying papers, include three additional
fluorescence telescopes with a more elevated field of view (HEAT) and a nested
surface array wi... | astro-ph | the pierre auger collaboration intends to extend the energy range of its southern observatory in argentina for high quality data from 01 to 3 eev the extensions described in accompanying papers include three additional fluorescence telescopes with a more elevated field of view heat and a nested surface array with 750 a... | [['the', 'pierre', 'auger', 'collaboration', 'intends', 'to', 'extend', 'the', 'energy', 'range', 'of', 'its', 'southern', 'observatory', 'in', 'argentina', 'for', 'high', 'quality', 'data', 'from', '01', 'to', '3', 'eev', 'the', 'extensions', 'described', 'in', 'accompanying', 'papers', 'include', 'three', 'additional... | [-0.06310973994862709, 0.14905642315227075, -0.03699555964929994, 0.1046210949757731, -0.057542311577494704, -0.019394694709108543, 0.018823849243811717, 0.366198440992647, -0.2333451017979427, -0.41089479173244225, 0.07718689333171305, -0.33722002595126377, -0.047299825433789, 0.2138584945140417, 0.0051621717537653315... |
709.0773 | Self-similar stable processes arising from high-density limits of
occupation times of particle systems | We extend results on time-rescaled occupation time fluctuation limits of the
$(d,\alpha, \beta)$-branching particle system $(0<\alpha \leq 2, 0<\beta \leq
1)$ with Poisson initial condition. The earlier results in the homogeneous case
(i.e., with Lebesgue initial intensity measure) were obtained for dimensions
$d>\al... | math.PR | we extend results on timerescaled occupation time fluctuation limits of the dalpha betabranching particle system 0alpha leq 2 0beta leq 1 with poisson initial condition the earlier results in the homogeneous case ie with lebesgue initial intensity measure were obtained for dimensions dalpha beta only since the particle... | [['we', 'extend', 'results', 'on', 'timerescaled', 'occupation', 'time', 'fluctuation', 'limits', 'of', 'the', 'dalpha', 'betabranching', 'particle', 'system', '0alpha', 'leq', '2', '0beta', 'leq', '1', 'with', 'poisson', 'initial', 'condition', 'the', 'earlier', 'results', 'in', 'the', 'homogeneous', 'case', 'ie', 'wi... | [-0.08906057729138973, 0.20262854080996975, -0.02479085533643869, 0.07981656414512625, 0.030225563566540187, -0.12976682352006053, 0.02809773678061964, 0.36981212272600555, -0.22154704724786237, -0.23470883757723376, 0.11189170941848371, -0.28884911260571605, -0.059579821789133576, 0.20955916327452326, -0.0470425902711... |
709.0774 | Entropy of (2+1)-dimensional de Sitter black hole to all orders in the
Planck length | We calculate the statistical entropy of a scalar field on the background of
(2+1)-dimensional de Sitter space without an artificial cutoff considering
corrections to all orders in the Planck length from a generalized uncertainty
principle (GUP) on the quantum state density. The desired entropy proportional
to the hor... | gr-qc | we calculate the statistical entropy of a scalar field on the background of 21dimensional de sitter space without an artificial cutoff considering corrections to all orders in the planck length from a generalized uncertainty principle gup on the quantum state density the desired entropy proportional to the horizon peri... | [['we', 'calculate', 'the', 'statistical', 'entropy', 'of', 'a', 'scalar', 'field', 'on', 'the', 'background', 'of', '21dimensional', 'de', 'sitter', 'space', 'without', 'an', 'artificial', 'cutoff', 'considering', 'corrections', 'to', 'all', 'orders', 'in', 'the', 'planck', 'length', 'from', 'a', 'generalized', 'uncer... | [-0.1507822159202952, 0.17864559007627095, -0.12377689957764804, 0.13717499900581864, -0.05865326161295468, -0.0615599883501144, -0.00630376625386085, 0.23108303455599383, -0.24104836265392163, -0.2632339602591945, 0.054815305737029835, -0.3394943290371813, -0.022239689514333128, 0.17298507193724313, -0.069832869750611... |
709.0775 | More Visible Effects of the Hidden Sector | There is a growing appreciation that hidden sector dynamics may affect the
supersymmetry breaking parameters in the visible sector (supersymmetric
standard model), especially when the dynamics is strong and superconformal. We
point out that there are effects that have not been previously discussed in the
literature. ... | hep-ph hep-th | there is a growing appreciation that hidden sector dynamics may affect the supersymmetry breaking parameters in the visible sector supersymmetric standard model especially when the dynamics is strong and superconformal we point out that there are effects that have not been previously discussed in the literature for exa... | [['there', 'is', 'a', 'growing', 'appreciation', 'that', 'hidden', 'sector', 'dynamics', 'may', 'affect', 'the', 'supersymmetry', 'breaking', 'parameters', 'in', 'the', 'visible', 'sector', 'supersymmetric', 'standard', 'model', 'especially', 'when', 'the', 'dynamics', 'is', 'strong', 'and', 'superconformal', 'we', 'po... | [-0.12048766849562526, 0.23511837863828988, -0.012693550530239009, 0.18618260741466655, -0.10242583142826334, -0.17094395096879453, -0.006665136087685823, 0.38231636784243167, -0.19337243407033383, -0.2981225047633052, 0.11380495658377185, -0.26988066850230097, -0.12982343642041086, 0.11209910582518205, -0.032376290149... |
709.0776 | Born reciprocity and the 1/r potential | Many structures in nature are invariant under the transformation
(p,r)->(br,-p/b), where b is some scale factor. Born's reciprocity hypothesis
affirms that this invariance extends to the entire Hamiltonian and equations of
motion. We investigate this idea for atomic physics and galactic motion, where
one is basically... | hep-th astro-ph physics.class-ph | many structures in nature are invariant under the transformation prbrpb where b is some scale factor borns reciprocity hypothesis affirms that this invariance extends to the entire hamiltonian and equations of motion we investigate this idea for atomic physics and galactic motion where one is basically dealing with a 1... | [['many', 'structures', 'in', 'nature', 'are', 'invariant', 'under', 'the', 'transformation', 'prbrpb', 'where', 'b', 'is', 'some', 'scale', 'factor', 'borns', 'reciprocity', 'hypothesis', 'affirms', 'that', 'this', 'invariance', 'extends', 'to', 'the', 'entire', 'hamiltonian', 'and', 'equations', 'of', 'motion', 'we',... | [-0.14588265226883512, 0.16130874069909545, -0.08527897751729896, 0.09028111068752184, -0.12526638368244775, -0.124141502439455, 0.0049533847599260265, 0.3422307634065228, -0.27766388192051844, -0.3424891385932638, 0.06116746457028253, -0.23981421848418571, -0.08110574895373023, 0.18773195349676433, -0.0208092093222364... |
709.0777 | Precise Numerical Evaluation of the Scalar One-Loop Integrals with the
Infrared Divergence | We present a new approach for obtaining very precise integration results for
infrared vertex and box diagrams, where the integration is carried out directly
without performing any analytic integration of Feynman parameters. Using an
appropriate numerical integration routine with an extrapolation method,
together with... | hep-ph | we present a new approach for obtaining very precise integration results for infrared vertex and box diagrams where the integration is carried out directly without performing any analytic integration of feynman parameters using an appropriate numerical integration routine with an extrapolation method together with a mu... | [['we', 'present', 'a', 'new', 'approach', 'for', 'obtaining', 'very', 'precise', 'integration', 'results', 'for', 'infrared', 'vertex', 'and', 'box', 'diagrams', 'where', 'the', 'integration', 'is', 'carried', 'out', 'directly', 'without', 'performing', 'any', 'analytic', 'integration', 'of', 'feynman', 'parameters', ... | [-0.0704369153222674, 0.04732993916742951, -0.0985058785065428, 0.056403454225328935, -0.10323979348161971, -0.1054546732951391, 0.09597522104703277, 0.4335695002953728, -0.1472932663383325, -0.34108953320651086, 0.1250834094357447, -0.2510699022972545, -0.08546058234891721, 0.30119298637372915, 0.008086792429207594, 0... |
709.0778 | Modular co-evolution of metabolic networks | The architecture of biological networks has been reported to exhibit high
level of modularity, and to some extent, topological modules of networks
overlap with known functional modules. However, how the modular topology of the
molecular network affects the evolution of its member proteins remains unclear.
In this wor... | q-bio.MN | the architecture of biological networks has been reported to exhibit high level of modularity and to some extent topological modules of networks overlap with known functional modules however how the modular topology of the molecular network affects the evolution of its member proteins remains unclear in this work the f... | [['the', 'architecture', 'of', 'biological', 'networks', 'has', 'been', 'reported', 'to', 'exhibit', 'high', 'level', 'of', 'modularity', 'and', 'to', 'some', 'extent', 'topological', 'modules', 'of', 'networks', 'overlap', 'with', 'known', 'functional', 'modules', 'however', 'how', 'the', 'modular', 'topology', 'of', ... | [-0.14017917232599875, 0.0772019498444234, -0.08259518868648089, 0.09294420405267141, -0.05502635883644987, -0.1421404823159369, 0.02629917355445333, 0.4100353235235581, -0.29897713953485855, -0.3044820953005304, 0.048321657160368674, -0.20733947323109858, -0.2601775325010889, 0.13799096760757937, -0.0486959861113857, ... |
709.0779 | Low-frequency spectroscopy of superconducting photonic crystals | Transmission, reflection and absorption of electromagnetic radiation and
photon dispersion law for 2D photonic crystals with superconducting elements
are studied. The calculation of optical properties of photonic crystals is
studied by layer-by-layer Korringa-Kohn-Rostoker techniques. The results of
numerical calcula... | cond-mat.mes-hall | transmission reflection and absorption of electromagnetic radiation and photon dispersion law for 2d photonic crystals with superconducting elements are studied the calculation of optical properties of photonic crystals is studied by layerbylayer korringakohnrostoker techniques the results of numerical calculations per... | [['transmission', 'reflection', 'and', 'absorption', 'of', 'electromagnetic', 'radiation', 'and', 'photon', 'dispersion', 'law', 'for', '2d', 'photonic', 'crystals', 'with', 'superconducting', 'elements', 'are', 'studied', 'the', 'calculation', 'of', 'optical', 'properties', 'of', 'photonic', 'crystals', 'is', 'studied... | [-0.16867665716475158, 0.16327977715653363, -0.052068023753677015, -0.04105375270886027, -0.028607814092979286, -0.1531192221387167, 0.047693827976190456, 0.46153244605720645, -0.1944307027234122, -0.2998017246054128, 0.011663787982972207, -0.3171722416276808, -0.11056599299884354, 0.24068118806756714, 0.06130045315608... |
709.078 | Eigenvalues Estimates For The Dirac Operator In Terms Of Codazzi Tensors | We prove a lower bound for the first eigenvalue of the Dirac operator on a
compact Riemannian spin manifold depending on the scalar curvature as well as a
chosen Codazzi tensor. The inequality generalizes the classical estimate from
[2].
| math.DG | we prove a lower bound for the first eigenvalue of the dirac operator on a compact riemannian spin manifold depending on the scalar curvature as well as a chosen codazzi tensor the inequality generalizes the classical estimate from 2 | [['we', 'prove', 'a', 'lower', 'bound', 'for', 'the', 'first', 'eigenvalue', 'of', 'the', 'dirac', 'operator', 'on', 'a', 'compact', 'riemannian', 'spin', 'manifold', 'depending', 'on', 'the', 'scalar', 'curvature', 'as', 'well', 'as', 'a', 'chosen', 'codazzi', 'tensor', 'the', 'inequality', 'generalizes', 'the', 'clas... | [-0.1298635100515989, 0.10600885865875544, -0.08060043706343724, 0.11578640630707526, -0.14340174594559732, -0.16407873678522614, -0.03128372887388254, 0.25150595180308205, -0.22283801124789393, -0.27068345511379915, 0.14363852260598484, -0.2847073861421683, -0.15978565571668485, 0.19366870207998615, -0.033346363725379... |
709.0781 | Structure of logarithmically divergent one-loop lattice Feynman
integrals | For logarithmically divergent one-loop lattice Feynman integrals I(p,a),
subject to mild general conditions, we prove the following expected and crucial
structural result: I(p,a) = f(p)log(aM)+g(p)+h(p,M) up to terms which vanish
for lattice spacing a -> 0. Here p denotes collectively the external momenta
and M is a ... | hep-lat math-ph math.MP | for logarithmically divergent oneloop lattice feynman integrals ipa subject to mild general conditions we prove the following expected and crucial structural result ipa fplogamgphpm up to terms which vanish for lattice spacing a 0 here p denotes collectively the external momenta and m is a mass scale which may be chose... | [['for', 'logarithmically', 'divergent', 'oneloop', 'lattice', 'feynman', 'integrals', 'ipa', 'subject', 'to', 'mild', 'general', 'conditions', 'we', 'prove', 'the', 'following', 'expected', 'and', 'crucial', 'structural', 'result', 'ipa', 'fplogamgphpm', 'up', 'to', 'terms', 'which', 'vanish', 'for', 'lattice', 'spaci... | [-0.1302396337545114, 0.1887227915951556, -0.10006697631788329, 0.0965237612431569, -0.06772966906073172, -0.14653137954291334, 0.010496136179919971, 0.3605250948882204, -0.2840487926061881, -0.22845653601985236, 0.08803915126067666, -0.24806069871568578, -0.11164163202599828, 0.13507196760610124, -0.030197962400823106... |
709.0782 | Cluster-Spin Gaussian Model for Lattice-Ising Models | In this paper we lay special stress on analyzing the topological properties
of the lattice systems and try to ovoid the conventional ways to calculate the
critical points. Only those clusters with finite sizes can execute the self
similar transformations of infinite hierarchies. Each ordered cluster has
fractal dimen... | physics.gen-ph | in this paper we lay special stress on analyzing the topological properties of the lattice systems and try to ovoid the conventional ways to calculate the critical points only those clusters with finite sizes can execute the self similar transformations of infinite hierarchies each ordered cluster has fractal dimension... | [['in', 'this', 'paper', 'we', 'lay', 'special', 'stress', 'on', 'analyzing', 'the', 'topological', 'properties', 'of', 'the', 'lattice', 'systems', 'and', 'try', 'to', 'ovoid', 'the', 'conventional', 'ways', 'to', 'calculate', 'the', 'critical', 'points', 'only', 'those', 'clusters', 'with', 'finite', 'sizes', 'can', ... | [-0.14907133943684722, 0.13801069020854762, -0.08492252292250346, 0.05907992726865786, -0.015871558990618734, -0.15127516399941737, 0.09668612224519867, 0.3362054343245669, -0.26999069752622834, -0.27102880482995734, 0.08129169232131023, -0.30043642251370534, -0.14255627891430572, 0.1694305786727031, -0.003845618911932... |
709.0783 | Godel's theorem as a corollary of impossibility of complete
axiomatization of geometry | Not any geometry can be axiomatized. The paradoxical Godel's theorem starts
from the supposition that any geometry can be axiomatized and goes to the
result, that not any geometry can be axiomatized. One considers example of two
close geometries (Riemannian geometry and $\sigma $-Riemannian one), which are
constructe... | math.GM | not any geometry can be axiomatized the paradoxical godels theorem starts from the supposition that any geometry can be axiomatized and goes to the result that not any geometry can be axiomatized one considers example of two close geometries riemannian geometry and sigma riemannian one which are constructed by differen... | [['not', 'any', 'geometry', 'can', 'be', 'axiomatized', 'the', 'paradoxical', 'godels', 'theorem', 'starts', 'from', 'the', 'supposition', 'that', 'any', 'geometry', 'can', 'be', 'axiomatized', 'and', 'goes', 'to', 'the', 'result', 'that', 'not', 'any', 'geometry', 'can', 'be', 'axiomatized', 'one', 'considers', 'examp... | [-0.09141107369214296, 0.09838576178514848, -0.15109862467664995, 0.1468407456147956, -0.15547725629567363, -0.17643181994244064, -0.03607957264017544, 0.30580258599401994, -0.31062046210798955, -0.281441663219421, 0.1465388761508497, -0.24093168681878366, -0.15840064414581398, 0.2025405039412924, -0.17463172343272118,... |
709.0784 | Connections between high energy QCD and statistical physics | It has been proposed that the energy evolution of QCD amplitudes in the
high-energy regime falls in the universality class of reaction-diffusion
processes. We review the arguments for this correspondence, and we explain how
it enables one to compute analytically asymptotic features of QCD amplitudes.
| hep-ph | it has been proposed that the energy evolution of qcd amplitudes in the highenergy regime falls in the universality class of reactiondiffusion processes we review the arguments for this correspondence and we explain how it enables one to compute analytically asymptotic features of qcd amplitudes | [['it', 'has', 'been', 'proposed', 'that', 'the', 'energy', 'evolution', 'of', 'qcd', 'amplitudes', 'in', 'the', 'highenergy', 'regime', 'falls', 'in', 'the', 'universality', 'class', 'of', 'reactiondiffusion', 'processes', 'we', 'review', 'the', 'arguments', 'for', 'this', 'correspondence', 'and', 'we', 'explain', 'ho... | [-0.09023254124654664, 0.1448493481717176, -0.1812929718988016, 0.13952885476820584, -0.057919046613905165, -0.06860341498007377, 0.0530325908627775, 0.3504551487664382, -0.21590819391939375, -0.2166522059796585, 0.04747089783971508, -0.26638106303030834, -0.17470714702374404, 0.13691131948596902, 0.015844665384954878,... |
709.0785 | A description based on Schubert classes of cohomology of flag manifolds | We describe the integral cohomology rings of the flag manifolds of types B_n,
D_n, G_2 and F_4 in terms of their Schubert classes. The main tool is the
divided difference operators of Bernstein-Gelfand-Gelfand and Demazure. As an
application, we compute the Chow rings of the corresponding complex algebraic
groups, re... | math.AT math.AG | we describe the integral cohomology rings of the flag manifolds of types b_n d_n g_2 and f_4 in terms of their schubert classes the main tool is the divided difference operators of bernsteingelfandgelfand and demazure as an application we compute the chow rings of the corresponding complex algebraic groups recovering t... | [['we', 'describe', 'the', 'integral', 'cohomology', 'rings', 'of', 'the', 'flag', 'manifolds', 'of', 'types', 'b_n', 'd_n', 'g_2', 'and', 'f_4', 'in', 'terms', 'of', 'their', 'schubert', 'classes', 'the', 'main', 'tool', 'is', 'the', 'divided', 'difference', 'operators', 'of', 'bernsteingelfandgelfand', 'and', 'demazu... | [-0.21725520923999803, -0.021344839303960077, -0.06614009024841445, 0.08040072745019902, -0.0634803592984099, -0.09287735801522753, -0.07191908989833402, 0.3015242843123685, -0.34419589177040116, -0.21673331251700542, 0.11642800373894195, -0.22124779185313465, -0.15031578845810145, 0.19158982078079134, -0.1589684135979... |
709.0786 | Low accretion rates at the AGN cosmic downsizing epoch | Context: X-ray surveys of Active Galactic Nuclei (AGN) indicate `cosmic
downsizing', with the comoving number density of high-luminosity objects
peaking at higher redshifts (z about 2) than low-luminosity AGN (z<1). Aims: We
test whether downsizing is caused by activity shifting towards low-mass black
holes accreting... | astro-ph | context xray surveys of active galactic nuclei agn indicate cosmic downsizing with the comoving number density of highluminosity objects peaking at higher redshifts z about 2 than lowluminosity agn z1 aims we test whether downsizing is caused by activity shifting towards lowmass black holes accreting at neareddington r... | [['context', 'xray', 'surveys', 'of', 'active', 'galactic', 'nuclei', 'agn', 'indicate', 'cosmic', 'downsizing', 'with', 'the', 'comoving', 'number', 'density', 'of', 'highluminosity', 'objects', 'peaking', 'at', 'higher', 'redshifts', 'z', 'about', '2', 'than', 'lowluminosity', 'agn', 'z1', 'aims', 'we', 'test', 'whet... | [-0.02549604514284144, 0.1348146817713632, -0.008983078188504334, 0.1916769585043284, -0.08626473485779615, -0.09163668138308474, 0.07251037238932256, 0.45233779056419315, -0.04498086066019756, -0.37494379675606027, 0.052434524847482, -0.3627897893583331, 0.060655269131530076, 0.246701389222517, -0.02345975383959665, -... |
709.0787 | Sound Generation by a Turbulent Flow in Musical Instruments -
Multiphysics Simulation Approach - | Total computational costs of scientific simulations are analyzed between
direct numerical simulations (DNS) and multiphysics simulations (MPS) for sound
generation in musical instruments. In order to produce acoustic sound by a
turbulent flow in a simple recorder-like instrument, compressible fluid dynamic
calculatio... | physics.comp-ph cs.CE physics.flu-dyn | total computational costs of scientific simulations are analyzed between direct numerical simulations dns and multiphysics simulations mps for sound generation in musical instruments in order to produce acoustic sound by a turbulent flow in a simple recorderlike instrument compressible fluid dynamic calculations with a... | [['total', 'computational', 'costs', 'of', 'scientific', 'simulations', 'are', 'analyzed', 'between', 'direct', 'numerical', 'simulations', 'dns', 'and', 'multiphysics', 'simulations', 'mps', 'for', 'sound', 'generation', 'in', 'musical', 'instruments', 'in', 'order', 'to', 'produce', 'acoustic', 'sound', 'by', 'a', 't... | [-0.13621950615844172, 0.14056741922265953, -0.07845136761251423, 0.025334067780662467, -0.08924131318969929, -0.08434887715460111, 0.005583482104595061, 0.35846917925368027, -0.24560235006113848, -0.3639878484558452, 0.09281064682269331, -0.28337982960942165, -0.11394603267156829, 0.2643790447209203, 0.001984674814459... |
709.0788 | Laplacian comparison for Alexandrov spaces | We consider an infinitesimal version of the Bishop-Gromov relative volume
comparison condition as generalized notion of Ricci curvature bounded below for
Alexandrov spaces. We prove a Laplacian comparison theorem for Alexandrov
spaces under the condition. As an application we prove a topological splitting
theorem.
| math.DG math.MG | we consider an infinitesimal version of the bishopgromov relative volume comparison condition as generalized notion of ricci curvature bounded below for alexandrov spaces we prove a laplacian comparison theorem for alexandrov spaces under the condition as an application we prove a topological splitting theorem | [['we', 'consider', 'an', 'infinitesimal', 'version', 'of', 'the', 'bishopgromov', 'relative', 'volume', 'comparison', 'condition', 'as', 'generalized', 'notion', 'of', 'ricci', 'curvature', 'bounded', 'below', 'for', 'alexandrov', 'spaces', 'we', 'prove', 'a', 'laplacian', 'comparison', 'theorem', 'for', 'alexandrov',... | [-0.18268399401991206, 0.0829375468846675, -0.09503969742747193, 0.20835142174143007, -0.09407417340712114, -0.1096227274763144, -0.024468485392968763, 0.3212644471575252, -0.2905146289955486, -0.18723665770481934, 0.16291743649212134, -0.25804024699821393, -0.1250948102890768, 0.18911542315882715, -0.22565976447764446... |
709.0789 | Structural peculiarities of plastically-deformed cementite and their
influence on magnetic characteristics and Mossbauer parameters | Cementite Fe3C is studied with first-principles calculations. Two possible
positions of carbon atoms in the iron sublattice are considered: with prismatic
or octahedral environment. Mossbauer spectra (MS) with parameters calculated
for both modifications are simulated above and below the Curie temperature. A
possibil... | cond-mat.mtrl-sci | cementite fe3c is studied with firstprinciples calculations two possible positions of carbon atoms in the iron sublattice are considered with prismatic or octahedral environment mossbauer spectra ms with parameters calculated for both modifications are simulated above and below the curie temperature a possibility to de... | [['cementite', 'fe3c', 'is', 'studied', 'with', 'firstprinciples', 'calculations', 'two', 'possible', 'positions', 'of', 'carbon', 'atoms', 'in', 'the', 'iron', 'sublattice', 'are', 'considered', 'with', 'prismatic', 'or', 'octahedral', 'environment', 'mossbauer', 'spectra', 'ms', 'with', 'parameters', 'calculated', 'f... | [-0.05647233819066363, 0.2001780419620142, -0.017586432407066848, 0.021975735297019128, -0.011747206929915896, -0.13801112847856226, 0.09322177723515779, 0.5044669668811063, -0.24918170876723403, -0.341827630220602, 0.03817727076360219, -0.3009285797112777, -0.049784552492686394, 0.1863324977797068, 0.01280216571467463... |
709.079 | MarlinTPC: A Marlin based common TPC software framework for the LC-TPC
collaboration | We describe the goals and present functionality of MarlinTPC, a common
software framework for the LC-TPC collaboration based on LCIO, Marlin and other
ilcsoft tools.
| physics.ins-det | we describe the goals and present functionality of marlintpc a common software framework for the lctpc collaboration based on lcio marlin and other ilcsoft tools | [['we', 'describe', 'the', 'goals', 'and', 'present', 'functionality', 'of', 'marlintpc', 'a', 'common', 'software', 'framework', 'for', 'the', 'lctpc', 'collaboration', 'based', 'on', 'lcio', 'marlin', 'and', 'other', 'ilcsoft', 'tools']] | [-0.06107472933151505, -0.01749963090035387, -0.10740444876930931, 0.03975577157160098, -0.10317870356481183, -0.12322883627546782, 0.01656008078597634, 0.3734862519936128, -0.16674694469706577, -0.32381053624505346, 0.11865501120601865, -0.24585976047356697, -0.17211995294994928, 0.24567422645420514, -0.03391726683317... |
709.0791 | Magneto-optical behaviour of EuIn_2P_2 | We report results of a magneto-optical investigation of the Zintl-phase
compound EuIn$_2$P$_2$. The compound orders magnetically at $T_C$=24 K and
exhibits concomitant large magnetoresistance effects. For $T\le$50 K and
increasing magnetic fields we observe a transfer of spectral weight in
$\sigma_1(\omega)$ from ene... | cond-mat.str-el cond-mat.mtrl-sci | we report results of a magnetooptical investigation of the zintlphase compound euin_2p_2 the compound orders magnetically at t_c24 k and exhibits concomitant large magnetoresistance effects for tle50 k and increasing magnetic fields we observe a transfer of spectral weight in sigma_1omega from energies above 1 ev into ... | [['we', 'report', 'results', 'of', 'a', 'magnetooptical', 'investigation', 'of', 'the', 'zintlphase', 'compound', 'euin_2p_2', 'the', 'compound', 'orders', 'magnetically', 'at', 't_c24', 'k', 'and', 'exhibits', 'concomitant', 'large', 'magnetoresistance', 'effects', 'for', 'tle50', 'k', 'and', 'increasing', 'magnetic',... | [-0.14280568500866228, 0.2141884809502326, -0.03514380687389706, 0.02272296706061871, -0.04996161545115355, -0.12434030932252157, 0.08442128709036491, 0.39007289168142456, -0.26618504974242974, -0.3216367915089502, -0.015523208853918448, -0.33414225329141145, -0.11096211593430184, 0.17979615542381147, 0.036156856248796... |
709.0792 | Brownian dynamics of a microswimmer | We report on dynamic properties of a simple model microswimmer composed of
three spheres and propelling itself in a viscous fluid by spinning motion of
the spheres under zero net torque constraint. At a fixed temperature and
increasing the spinning frequency, the swimmer demonstrates a transition from
dissipation-dom... | physics.flu-dyn physics.bio-ph | we report on dynamic properties of a simple model microswimmer composed of three spheres and propelling itself in a viscous fluid by spinning motion of the spheres under zero net torque constraint at a fixed temperature and increasing the spinning frequency the swimmer demonstrates a transition from dissipationdominate... | [['we', 'report', 'on', 'dynamic', 'properties', 'of', 'a', 'simple', 'model', 'microswimmer', 'composed', 'of', 'three', 'spheres', 'and', 'propelling', 'itself', 'in', 'a', 'viscous', 'fluid', 'by', 'spinning', 'motion', 'of', 'the', 'spheres', 'under', 'zero', 'net', 'torque', 'constraint', 'at', 'a', 'fixed', 'temp... | [-0.17859432135890352, 0.2286748460271444, -0.08713699430624795, -0.06084383219741739, -0.0445168135239084, -0.14224543457669092, 0.029486567358395492, 0.32782172323091, -0.26627916066975493, -0.30520270187862036, 0.035022097682330486, -0.24558351220699345, -0.12288647233622103, 0.1753631410453037, -0.02838310490862080... |
709.0793 | The formation and ordering of local magnetic moments in Fe-Al alloys | With density functional theory, studied are the local magnetic moments in
Fe-Al alloys depending on concentration and Fe nearest environment. At zero
temperature, the system can be in different states: ferromagnetic,
antiferromagnetic and spin-spiral waves (SSW) which has a minimum energy. Both
SSW and negative momen... | cond-mat.mtrl-sci | with density functional theory studied are the local magnetic moments in feal alloys depending on concentration and fe nearest environment at zero temperature the system can be in different states ferromagnetic antiferromagnetic and spinspiral waves ssw which has a minimum energy both ssw and negative moment of fe atom... | [['with', 'density', 'functional', 'theory', 'studied', 'are', 'the', 'local', 'magnetic', 'moments', 'in', 'feal', 'alloys', 'depending', 'on', 'concentration', 'and', 'fe', 'nearest', 'environment', 'at', 'zero', 'temperature', 'the', 'system', 'can', 'be', 'in', 'different', 'states', 'ferromagnetic', 'antiferromagn... | [-0.13013519755276365, 0.21554613091228975, 0.0014383465362091858, 0.046303693819070416, -0.016295584226359745, -0.12051921690969418, 0.05886979093650423, 0.43247407163393553, -0.23011043657814817, -0.35342031473382596, 0.009928836828164225, -0.3734531847183548, -0.03192756396518754, 0.14207362560998826, 0.090168567978... |
709.0794 | The thermal width of heavy quarkonia moving in quark gluon plasma | The velocity dependence of the thermal width of heavy quarkonia traveling
with respect to the quark gluon plasma is calculated up to the NLO in
perturbative QCD. At the LO, the width decreases with increasing speed, whereas
at the NLO it increases with a magnitude approximately proportional to the
expectation value o... | hep-ph | the velocity dependence of the thermal width of heavy quarkonia traveling with respect to the quark gluon plasma is calculated up to the nlo in perturbative qcd at the lo the width decreases with increasing speed whereas at the nlo it increases with a magnitude approximately proportional to the expectation value of the... | [['the', 'velocity', 'dependence', 'of', 'the', 'thermal', 'width', 'of', 'heavy', 'quarkonia', 'traveling', 'with', 'respect', 'to', 'the', 'quark', 'gluon', 'plasma', 'is', 'calculated', 'up', 'to', 'the', 'nlo', 'in', 'perturbative', 'qcd', 'at', 'the', 'lo', 'the', 'width', 'decreases', 'with', 'increasing', 'speed... | [-0.061643353414987105, 0.24263885899512558, -0.12165867084593968, 0.05341431281670148, 0.00028033451675329096, -0.02212678048174915, 0.026717593828432782, 0.3544622630660617, -0.23083323928078117, -0.24116393790355622, -0.01814040699621749, -0.3556567668524939, 0.1017882626958538, 0.09102087420259797, 0.05132515775581... |
709.0795 | Quasisymmetric structures on surfaces | We show that a locally Ahlfors 2-regular and locally linearly locally
contractible metric surface is locally quasisymmetrically equivalent to the
disk. We also discuss an application of this result to the problem of
characterizing surfaces in some Euclidean space that are locally bi-Lipschitz
equivalent to an open su... | math.MG math.CV | we show that a locally ahlfors 2regular and locally linearly locally contractible metric surface is locally quasisymmetrically equivalent to the disk we also discuss an application of this result to the problem of characterizing surfaces in some euclidean space that are locally bilipschitz equivalent to an open subset ... | [['we', 'show', 'that', 'a', 'locally', 'ahlfors', '2regular', 'and', 'locally', 'linearly', 'locally', 'contractible', 'metric', 'surface', 'is', 'locally', 'quasisymmetrically', 'equivalent', 'to', 'the', 'disk', 'we', 'also', 'discuss', 'an', 'application', 'of', 'this', 'result', 'to', 'the', 'problem', 'of', 'char... | [-0.16225356743762306, 0.11766922722317223, -0.051686816027059275, 0.09152813379963239, -0.09904288777204998, -0.08705656722589743, -0.012810108142302316, 0.48308852227295146, -0.3680962286159104, -0.14042842022015475, 0.13425112514546617, -0.2628072308120774, -0.17416730439107792, 0.2366544749660819, -0.18814700104150... |
709.0796 | On frames in Hilbert modules over pro-C*-algebras | We introduce the concept of frame of multipliers in Hilbert modules over
pro-C*-algebras and show that many properties of frames in Hilbert C*-modules
are valid for frames of multipliers in Hilbert modules over pro-C*-algebras.
| math.OA math.FA | we introduce the concept of frame of multipliers in hilbert modules over procalgebras and show that many properties of frames in hilbert cmodules are valid for frames of multipliers in hilbert modules over procalgebras | [['we', 'introduce', 'the', 'concept', 'of', 'frame', 'of', 'multipliers', 'in', 'hilbert', 'modules', 'over', 'procalgebras', 'and', 'show', 'that', 'many', 'properties', 'of', 'frames', 'in', 'hilbert', 'cmodules', 'are', 'valid', 'for', 'frames', 'of', 'multipliers', 'in', 'hilbert', 'modules', 'over', 'procalgebras... | [-0.17024211256819613, 0.07125343768583502, -0.07467252201476025, 0.02914449093205964, 0.021253647484734434, -0.07006025626598035, -0.1006732658647439, 0.48428894973853054, -0.3713323627324665, -0.0950459686710554, 0.0757882978171384, -0.15876491263727932, -0.09797141550327926, 0.28715030465494185, -0.21389075686388156... |
709.0797 | Copies of a one-ended group in a Mapping Class Group | We establish that, given $\Sigma$ a compact orientable surface, and $G$ a
finitely presented one-ended group, the set of copies of $G$ in the mapping
class group $\mathcal{MCG}(\Sigma)$ consisting of only pseudo-anosov elements
except identity, is finite up to conjugacy. This relies on a result of Bowditch
on the sam... | math.GR | we establish that given sigma a compact orientable surface and g a finitely presented oneended group the set of copies of g in the mapping class group mathcalmcgsigma consisting of only pseudoanosov elements except identity is finite up to conjugacy this relies on a result of bowditch on the same problem for images of ... | [['we', 'establish', 'that', 'given', 'sigma', 'a', 'compact', 'orientable', 'surface', 'and', 'g', 'a', 'finitely', 'presented', 'oneended', 'group', 'the', 'set', 'of', 'copies', 'of', 'g', 'in', 'the', 'mapping', 'class', 'group', 'mathcalmcgsigma', 'consisting', 'of', 'only', 'pseudoanosov', 'elements', 'except', '... | [-0.19586766848371095, 0.08004113821156114, -0.11864432203365821, 0.03782004050183693, -0.10936853383171642, -0.11675166879197425, 0.08721752932173348, 0.35133162241812066, -0.27591434082399324, -0.2925755010186651, 0.08369956850879347, -0.2795254216294422, -0.1284736904063236, 0.24324856044846438, -0.17840145395146073... |
709.0798 | Optimizing the electronic control loop of a solid-state ring laser
gyroscope | We study in this Letter the dynamical effects of the limited bandwidth of the
control electronics in a solid-state (Nd-YAG) ring laser gyroscope. We derive a
stability condition for the rotation-sensing regime in the case of a
first-order control loop, showing that the smallest measurable rotation speed
depends direc... | physics.optics | we study in this letter the dynamical effects of the limited bandwidth of the control electronics in a solidstate ndyag ring laser gyroscope we derive a stability condition for the rotationsensing regime in the case of a firstorder control loop showing that the smallest measurable rotation speed depends directly on the... | [['we', 'study', 'in', 'this', 'letter', 'the', 'dynamical', 'effects', 'of', 'the', 'limited', 'bandwidth', 'of', 'the', 'control', 'electronics', 'in', 'a', 'solidstate', 'ndyag', 'ring', 'laser', 'gyroscope', 'we', 'derive', 'a', 'stability', 'condition', 'for', 'the', 'rotationsensing', 'regime', 'in', 'the', 'case... | [-0.19302776975498076, 0.1375964508938884, -0.05912352844496213, -0.014915701486022464, -0.04913685770912303, -0.11432315440412374, 0.07644006357129131, 0.39201014814159224, -0.24952501838745933, -0.272682190118801, 0.10128545883806452, -0.24152194302056043, -0.09669358513894535, 0.2699766883900064, -0.0899108921635955... |
709.0799 | Appropriate SCF basis sets for orbital studies of galaxies and a
`quantum-mechanical' method to compute them | We address the question of an appropriate choice of basis functions for the
self-consistent field (SCF) method of simulation of the N-body problem. Our
criterion is based on a comparison of the orbits found in N-body realizations
of analytical potential-density models of triaxial galaxies, in which the
potential is f... | astro-ph | we address the question of an appropriate choice of basis functions for the selfconsistent field scf method of simulation of the nbody problem our criterion is based on a comparison of the orbits found in nbody realizations of analytical potentialdensity models of triaxial galaxies in which the potential is fitted by t... | [['we', 'address', 'the', 'question', 'of', 'an', 'appropriate', 'choice', 'of', 'basis', 'functions', 'for', 'the', 'selfconsistent', 'field', 'scf', 'method', 'of', 'simulation', 'of', 'the', 'nbody', 'problem', 'our', 'criterion', 'is', 'based', 'on', 'a', 'comparison', 'of', 'the', 'orbits', 'found', 'in', 'nbody',... | [-0.11833502757887711, 0.03758857362589251, -0.10210112364090403, 0.046191920331207066, -0.015058205880283733, -0.06998683815546544, 0.05528951923257973, 0.31328200046374777, -0.2538685488586747, -0.28879814787479247, 0.06549858340327824, -0.2528937070689518, -0.1273505439822772, 0.22372111988366208, -0.006089827167132... |
709.08 | Elation generalised quadrangles of order (s,p), where p is prime | We show that an elation generalised quadrangle which has p+1 lines on each
point, for some prime p, is classical or arises from a flock of a quadratic
cone (i.e., is a flock quadrangle).
| math.CO math.GR | we show that an elation generalised quadrangle which has p1 lines on each point for some prime p is classical or arises from a flock of a quadratic cone ie is a flock quadrangle | [['we', 'show', 'that', 'an', 'elation', 'generalised', 'quadrangle', 'which', 'has', 'p1', 'lines', 'on', 'each', 'point', 'for', 'some', 'prime', 'p', 'is', 'classical', 'or', 'arises', 'from', 'a', 'flock', 'of', 'a', 'quadratic', 'cone', 'ie', 'is', 'a', 'flock', 'quadrangle']] | [-0.2167777310618583, 0.04595600785251008, -0.1314148534746731, 0.019127743024214664, -0.12145426606430727, -0.2208020437426646, 0.023584846461958745, 0.3395876845564036, -0.3565295952207902, -0.15873267451602527, 0.06662864120581242, -0.32035427058444305, -0.15017574125051716, 0.16125130315776914, -0.11799316012012936... |
709.0801 | Lie admissible algebras are Volichenko | Withdrawn on account of a crucial error in the main theorem
| math.RT | withdrawn on account of a crucial error in the main theorem | [['withdrawn', 'on', 'account', 'of', 'a', 'crucial', 'error', 'in', 'the', 'main', 'theorem']] | [-0.15422422997653484, -0.098627263256772, -0.13387677987868135, 0.14313536069609903, 0.038328029892661354, -0.09185178810730577, 0.0816514478488402, 0.23239376937801187, -0.22051021016456865, -0.29385083947669377, 0.07926423427521843, -0.1721055218103257, -0.08225782351060347, 0.21508272263136777, -0.31481023818593135... |
709.0802 | Robust Preparation of GHZ and W States of Three Distant Atoms | Schemes to generate Greenberger-Horne-Zeilinger(GHZ) and W states of three
distant atoms are proposed in this paper. The schemes use the effects of
quantum statistics of indistinguishable photons emitted by the atoms inside
optical cavities. The advantages of the schemes are their robustness against
detection ineffic... | quant-ph | schemes to generate greenbergerhornezeilingerghz and w states of three distant atoms are proposed in this paper the schemes use the effects of quantum statistics of indistinguishable photons emitted by the atoms inside optical cavities the advantages of the schemes are their robustness against detection inefficiency an... | [['schemes', 'to', 'generate', 'greenbergerhornezeilingerghz', 'and', 'w', 'states', 'of', 'three', 'distant', 'atoms', 'are', 'proposed', 'in', 'this', 'paper', 'the', 'schemes', 'use', 'the', 'effects', 'of', 'quantum', 'statistics', 'of', 'indistinguishable', 'photons', 'emitted', 'by', 'the', 'atoms', 'inside', 'op... | [-0.1221618637464915, 0.14693724325449806, -0.03370564943817381, 0.036552219053216865, 0.023981689207562027, -0.1796207968145609, 0.09163113665441688, 0.43265697594783076, -0.20369061638205632, -0.2670604978777366, 0.016565847441821983, -0.3030939907958246, -0.04178731417768214, 0.23993595675660986, -0.0683895714121730... |
709.0803 | On non-monotonic orbital velocity profiles around rapidly rotating
Kerr-(anti)de Sitter black holes: acomment to the recently published results | Critical discussion of the recently published results [Muller, A. and
Aschenbach, B. 2007 Class. Quantum Grav. 24, p. 2637; arXiv:0704.3963] on the
non-monotonic orbital velocity profiles of the Keplerian motion of test
particles and l = const motion of test perfect fluid around K(a)dS black holes
is given, and the d... | gr-qc | critical discussion of the recently published results muller a and aschenbach b 2007 class quantum grav 24 p 2637 arxiv07043963 on the nonmonotonic orbital velocity profiles of the keplerian motion of test particles and l const motion of test perfect fluid around kads black holes is given and the discrepancies concerne... | [['critical', 'discussion', 'of', 'the', 'recently', 'published', 'results', 'muller', 'a', 'and', 'aschenbach', 'b', '2007', 'class', 'quantum', 'grav', '24', 'p', '2637', 'arxiv07043963', 'on', 'the', 'nonmonotonic', 'orbital', 'velocity', 'profiles', 'of', 'the', 'keplerian', 'motion', 'of', 'test', 'particles', 'an... | [-0.20408354625105857, 0.12903711579274385, -0.0954142331960611, 0.06808262954873498, -0.08612620871281251, -0.1501533662318252, -0.007110355122131295, 0.25744099798321257, -0.14979949964908884, -0.3165387743385509, 0.02511528806062415, -0.29508538339578083, -0.06706265122047625, 0.18436162414145657, -0.092482322660362... |
709.0804 | Measurable entanglement for tripartite quantum pure states of qubits | We show that for tripartite quantum pure states of qubits, all the kinds of
entanglement in terms of SLOCC classification are experimentally measurable by
simple projective measurements, provided that four copies of the composite
quantum system are available. In particular, the entanglement of reduced
density matrice... | quant-ph | we show that for tripartite quantum pure states of qubits all the kinds of entanglement in terms of slocc classification are experimentally measurable by simple projective measurements provided that four copies of the composite quantum system are available in particular the entanglement of reduced density matrices even... | [['we', 'show', 'that', 'for', 'tripartite', 'quantum', 'pure', 'states', 'of', 'qubits', 'all', 'the', 'kinds', 'of', 'entanglement', 'in', 'terms', 'of', 'slocc', 'classification', 'are', 'experimentally', 'measurable', 'by', 'simple', 'projective', 'measurements', 'provided', 'that', 'four', 'copies', 'of', 'the', '... | [-0.1453576899780034, 0.2510213473105978, -0.04777429741807282, 0.04438883482362144, 0.0445112823815036, -0.21862904479923218, -0.0278987708611806, 0.3628957325984773, -0.23955226791287332, -0.2751922446094747, 0.07572319367318414, -0.27991782559547573, -0.134249133492918, 0.2203332714393343, -0.05708360007817024, 0.10... |
709.0805 | Weak approximation of a fractional SDE | In this note, a diffusion approximation result is shown for stochastic
differential equations driven by a (Liouville) fractional Brownian motion B
with Hurst parameter H in (1/3,1/2). More precisely, we resort to the
Kac-Stroock type approximation using a Poisson process studied in Bardina,
Jolis and Tudor (2003) and... | math.PR | in this note a diffusion approximation result is shown for stochastic differential equations driven by a liouville fractional brownian motion b with hurst parameter h in 1312 more precisely we resort to the kacstroock type approximation using a poisson process studied in bardina jolis and tudor 2003 and delgado and jol... | [['in', 'this', 'note', 'a', 'diffusion', 'approximation', 'result', 'is', 'shown', 'for', 'stochastic', 'differential', 'equations', 'driven', 'by', 'a', 'liouville', 'fractional', 'brownian', 'motion', 'b', 'with', 'hurst', 'parameter', 'h', 'in', '1312', 'more', 'precisely', 'we', 'resort', 'to', 'the', 'kacstroock'... | [-0.059718005009926856, 0.04609342458460367, -0.10171463024435622, 0.05697703681226179, -0.08777253335398255, -0.12686147879470477, 0.042302081373760084, 0.287784474901855, -0.26006137958558445, -0.2925243739772475, 0.08951183024151815, -0.22700714494920138, -0.20907627619100932, 0.20186910835433414, -0.140921873252161... |
709.0806 | The UV colours of high-redshift early-type galaxies: evidence for recent
star formation and stellar mass assembly over the last 8 billion years | We combine deep UBVRIzJK photometry from the Multiwavelength Survey by
Yale-Chile (MUSYC) with redshifts from the COMBO-17 survey to perform a
large-scale study of the rest-frame ultraviolet (UV) properties of 674
high-redshift (0.5<z<1) early-type galaxies, drawn from the Extended Chandra
Deep Field South (E-CDFS). ... | astro-ph | we combine deep ubvrizjk photometry from the multiwavelength survey by yalechile musyc with redshifts from the combo17 survey to perform a largescale study of the restframe ultraviolet uv properties of 674 highredshift 05z1 earlytype galaxies drawn from the extended chandra deep field south ecdfs galaxy morphologies ar... | [['we', 'combine', 'deep', 'ubvrizjk', 'photometry', 'from', 'the', 'multiwavelength', 'survey', 'by', 'yalechile', 'musyc', 'with', 'redshifts', 'from', 'the', 'combo17', 'survey', 'to', 'perform', 'a', 'largescale', 'study', 'of', 'the', 'restframe', 'ultraviolet', 'uv', 'properties', 'of', '674', 'highredshift', '05... | [-0.01632800376182606, 0.1145254985536099, -0.06519285891768284, 0.10615347995765125, -0.10706099207382355, -0.007074586205964856, 0.07022461430270872, 0.4812087497854303, -0.0674424382026046, -0.3841741388486956, 0.03220379112652787, -0.2971760646783813, -0.005319669446999966, 0.20104602416086342, -0.05005373504461919... |
709.0807 | A SIMBOL-X View of Microquasars | Based on spectral simulations, I show how focusing of the X-ray radiations
above 10 keV will open a new window for the study of microquasars. With
simulations of soft and hard state spectra of Galactic sources, I discuss how
SIMBOL-X can help to precisely measure the spin of black holes. Spectral study
on short ~1 s ... | astro-ph | based on spectral simulations i show how focusing of the xray radiations above 10 kev will open a new window for the study of microquasars with simulations of soft and hard state spectra of galactic sources i discuss how simbolx can help to precisely measure the spin of black holes spectral study on short 1 s time scal... | [['based', 'on', 'spectral', 'simulations', 'i', 'show', 'how', 'focusing', 'of', 'the', 'xray', 'radiations', 'above', '10', 'kev', 'will', 'open', 'a', 'new', 'window', 'for', 'the', 'study', 'of', 'microquasars', 'with', 'simulations', 'of', 'soft', 'and', 'hard', 'state', 'spectra', 'of', 'galactic', 'sources', 'i'... | [-0.06379281907610482, 0.1421830792061166, -0.08116571000551409, 0.15085966433539535, -0.10101949686720742, -0.12699777216325994, 0.03892474558740629, 0.44064635924543394, -0.23142401375596158, -0.32523504102066386, 0.1225910913754805, -0.31752219197347364, -0.06185787934880478, 0.23331075434389553, -0.0150387852759608... |
709.0808 | Circular invasion of fluid into a quenched disordered media | The Hele-Shaw experiment is performed with a circular invasion to study the
scaling and dynamic behavior of the interface. We did not find any universal
power law. The time exponent varies with the range of scale, as has been
reported in the literature but not captured by existing models. We ascribe this
distinct dif... | cond-mat.dis-nn | the heleshaw experiment is performed with a circular invasion to study the scaling and dynamic behavior of the interface we did not find any universal power law the time exponent varies with the range of scale as has been reported in the literature but not captured by existing models we ascribe this distinct difference... | [['the', 'heleshaw', 'experiment', 'is', 'performed', 'with', 'a', 'circular', 'invasion', 'to', 'study', 'the', 'scaling', 'and', 'dynamic', 'behavior', 'of', 'the', 'interface', 'we', 'did', 'not', 'find', 'any', 'universal', 'power', 'law', 'the', 'time', 'exponent', 'varies', 'with', 'the', 'range', 'of', 'scale', ... | [-0.09620865009492263, 0.15786055131162435, -0.08606920964287026, 0.047843901582224214, -0.0933465734140001, -0.15151793348385303, 0.011658662590849892, 0.35658997190994735, -0.26834371648020233, -0.3227191599511096, 0.0902182770666474, -0.28401881326863077, -0.0924289493161031, 0.18137605044909794, -0.0362351028926913... |
709.0809 | Group velocity control in the ultraviolet domain via interacting
dark-state resonances | The propagation of a weak probe field in a laser-driven four-level atomic
system is investigated. We choose mercury as our model system, where the probe
transition is in the ultraviolet region. A high-resolution peak appears in the
optical spectra due to the presence of interacting dark resonances. We show
that this ... | quant-ph | the propagation of a weak probe field in a laserdriven fourlevel atomic system is investigated we choose mercury as our model system where the probe transition is in the ultraviolet region a highresolution peak appears in the optical spectra due to the presence of interacting dark resonances we show that this narrow pe... | [['the', 'propagation', 'of', 'a', 'weak', 'probe', 'field', 'in', 'a', 'laserdriven', 'fourlevel', 'atomic', 'system', 'is', 'investigated', 'we', 'choose', 'mercury', 'as', 'our', 'model', 'system', 'where', 'the', 'probe', 'transition', 'is', 'in', 'the', 'ultraviolet', 'region', 'a', 'highresolution', 'peak', 'appe... | [-0.1360946333352958, 0.20408340398440988, -0.0684130640844975, 0.04548796214231547, -0.07203927096220311, -0.17849425295094862, 0.04337651397220505, 0.4254632619819764, -0.29121460745127165, -0.2899675169108628, 0.04168681962945466, -0.2415864708078704, -0.08548697047055988, 0.18411759441268855, 0.011788682307363569, ... |
709.081 | A Comparative Study of Stochastic Volatility Models | The correlated stochastic volatility models constitute a natural extension of
the Black and Scholes-Merton framework: here the volatility is not a constant,
but a stochastic process correlated with the price log-return one. At present,
several stochastic volatility models are discussed in the literature, differing
in... | q-fin.ST physics.soc-ph | the correlated stochastic volatility models constitute a natural extension of the black and scholesmerton framework here the volatility is not a constant but a stochastic process correlated with the price logreturn one at present several stochastic volatility models are discussed in the literature differing in the dyna... | [['the', 'correlated', 'stochastic', 'volatility', 'models', 'constitute', 'a', 'natural', 'extension', 'of', 'the', 'black', 'and', 'scholesmerton', 'framework', 'here', 'the', 'volatility', 'is', 'not', 'a', 'constant', 'but', 'a', 'stochastic', 'process', 'correlated', 'with', 'the', 'price', 'logreturn', 'one', 'at... | [-0.01604260788844066, 0.005127625208687993, -0.09698809276860049, 0.17558912597502407, -0.0846814037278354, -0.11269748759545148, 0.04135039457531171, 0.4254217944652873, -0.27447531606687453, -0.2632864087948853, 0.1554608610623542, -0.335531164728541, -0.15276050506559222, 0.22030429568691576, -0.10644250370666107, ... |
709.0811 | Survival of icy grains in debris discs. The role of photosputtering | We put theoretical constraints on the presence and survival of icy grains in
debris discs. Particular attention is paid to UV sputtering of water ice, which
has so far not been studied in detail in this context. We present a
photosputtering model based on available experimental and theoretical studies.
We quantitativ... | astro-ph | we put theoretical constraints on the presence and survival of icy grains in debris discs particular attention is paid to uv sputtering of water ice which has so far not been studied in detail in this context we present a photosputtering model based on available experimental and theoretical studies we quantitatively es... | [['we', 'put', 'theoretical', 'constraints', 'on', 'the', 'presence', 'and', 'survival', 'of', 'icy', 'grains', 'in', 'debris', 'discs', 'particular', 'attention', 'is', 'paid', 'to', 'uv', 'sputtering', 'of', 'water', 'ice', 'which', 'has', 'so', 'far', 'not', 'been', 'studied', 'in', 'detail', 'in', 'this', 'context'... | [-0.04547687574262399, 0.15920162030097068, -0.06286883091194216, 0.04794121351248274, -0.020590425270546057, -0.04600974513970979, 0.061383987057717714, 0.3879064208806746, -0.22179302593312142, -0.30002999211975484, 0.09006084269838704, -0.278783647126781, -0.048223696472026255, 0.15427271779944104, -0.06099292748375... |
709.0812 | Combinatorial aspects of boundary loop models | We discuss in this paper combinatorial aspects of boundary loop models, that
is models of self-avoiding loops on a strip where loops get different weights
depending on whether they touch the left, the right, both or no boundary. These
models are described algebraically by a generalization of the Temperley-Lieb
algebr... | math-ph cond-mat.stat-mech math.MP math.RT | we discuss in this paper combinatorial aspects of boundary loop models that is models of selfavoiding loops on a strip where loops get different weights depending on whether they touch the left the right both or no boundary these models are described algebraically by a generalization of the temperleylieb algebra dubbed... | [['we', 'discuss', 'in', 'this', 'paper', 'combinatorial', 'aspects', 'of', 'boundary', 'loop', 'models', 'that', 'is', 'models', 'of', 'selfavoiding', 'loops', 'on', 'a', 'strip', 'where', 'loops', 'get', 'different', 'weights', 'depending', 'on', 'whether', 'they', 'touch', 'the', 'left', 'the', 'right', 'both', 'or'... | [-0.10958149936050177, 0.1256049543004693, -0.04894894845363565, 0.06336809787199013, -0.05158792114361448, -0.1451525649027829, -0.011007893870801743, 0.3540171477313441, -0.25045043367654424, -0.2404548652589153, 0.14439379152687812, -0.2535589716600296, -0.19308431912738747, 0.17806966096701982, -0.06511571763356433... |
709.0813 | The night-sky at the Calar Alto Observatory | We present a characterization of the main properties of the night-sky at the
Calar Alto observatory for the time period between 2004 and 2007. We use
optical spectrophotometric data, photometric calibrated images taken in
moonless observing periods, together with the observing conditions regularly
monitored at the ... | astro-ph | we present a characterization of the main properties of the nightsky at the calar alto observatory for the time period between 2004 and 2007 we use optical spectrophotometric data photometric calibrated images taken in moonless observing periods together with the observing conditions regularly monitored at the observat... | [['we', 'present', 'a', 'characterization', 'of', 'the', 'main', 'properties', 'of', 'the', 'nightsky', 'at', 'the', 'calar', 'alto', 'observatory', 'for', 'the', 'time', 'period', 'between', '2004', 'and', '2007', 'we', 'use', 'optical', 'spectrophotometric', 'data', 'photometric', 'calibrated', 'images', 'taken', 'in... | [-0.08254208623930026, 0.13552209253657566, -0.08737289052260166, 0.05527465771945117, -0.026349296853368287, -0.1006766919963411, 0.05874129120405769, 0.4286720299242006, -0.15378916227291484, -0.37721893275192997, 0.14554470969505928, -0.33340654048026863, -0.05011883427869179, 0.2346102789424549, -0.0945581505166046... |
709.0814 | A Morphological and Statistical Analysis of Ansae in Barred Galaxies | Many barred galaxies show a set of symmetric enhancements at the ends of the
stellar bar, called {\it ansae}, or the ``handles'' of the bar. The ansa bars
have been in the literature for some decades, but their origin has still not
been specifically addressed, although, they could be related to the growth
process of ... | astro-ph | many barred galaxies show a set of symmetric enhancements at the ends of the stellar bar called it ansae or the handles of the bar the ansa bars have been in the literature for some decades but their origin has still not been specifically addressed although they could be related to the growth process of bars but even t... | [['many', 'barred', 'galaxies', 'show', 'a', 'set', 'of', 'symmetric', 'enhancements', 'at', 'the', 'ends', 'of', 'the', 'stellar', 'bar', 'called', 'it', 'ansae', 'or', 'the', 'handles', 'of', 'the', 'bar', 'the', 'ansa', 'bars', 'have', 'been', 'in', 'the', 'literature', 'for', 'some', 'decades', 'but', 'their', 'ori... | [-0.10149433122777347, 0.06373575638281181, -0.08810753049744692, 0.11353240766172641, -0.06193391720963908, -0.08192768439611038, -0.025896377737288794, 0.44727511422700317, -0.17231366020028613, -0.3054629241482222, 0.11019646173372166, -0.26600102084246047, -0.12484377032108439, 0.19216717717478918, -0.0722611005143... |
709.0815 | Nonequilibrium Electron Interactions in Metal Films | Ultrafast relaxation dynamics of an athermal electron distribution is
investigated in silver films using a femtosecond pump-probe technique with 18
fs pulses in off-resonant conditions. The results yield evidence for an
increase with time of the electron-gas energy loss rate to the lattice and of
the free electron da... | cond-mat.str-el | ultrafast relaxation dynamics of an athermal electron distribution is investigated in silver films using a femtosecond pumpprobe technique with 18 fs pulses in offresonant conditions the results yield evidence for an increase with time of the electrongas energy loss rate to the lattice and of the free electron damping ... | [['ultrafast', 'relaxation', 'dynamics', 'of', 'an', 'athermal', 'electron', 'distribution', 'is', 'investigated', 'in', 'silver', 'films', 'using', 'a', 'femtosecond', 'pumpprobe', 'technique', 'with', '18', 'fs', 'pulses', 'in', 'offresonant', 'conditions', 'the', 'results', 'yield', 'evidence', 'for', 'an', 'increas... | [-0.10885063335479658, 0.22452745315864117, -0.09861278471847375, 0.04413582261102939, 0.07020481660618402, -0.08599694512806655, 0.026425020381187398, 0.43002001863039496, -0.25005039060488343, -0.2880083058234526, 0.036721628579904235, -0.2953436712379612, -0.08014619823855658, 0.23061820502126856, 0.0383353600156537... |
709.0816 | Noncommutative Quantum Mechanics Viewed from Feynman Formalism | Dyson published in 1990 a proof due to Feynman of the Maxwell equations. This
proof is based on the assumption of simple commutation relations between
position and velocity. We first study a nonrelativistic particle using Feynman
formalism. We show that Poincar\'{e}'s magnetic angular momentum and Dirac
magnetic mono... | hep-th | dyson published in 1990 a proof due to feynman of the maxwell equations this proof is based on the assumption of simple commutation relations between position and velocity we first study a nonrelativistic particle using feynman formalism we show that poincares magnetic angular momentum and dirac magnetic monopole are t... | [['dyson', 'published', 'in', '1990', 'a', 'proof', 'due', 'to', 'feynman', 'of', 'the', 'maxwell', 'equations', 'this', 'proof', 'is', 'based', 'on', 'the', 'assumption', 'of', 'simple', 'commutation', 'relations', 'between', 'position', 'and', 'velocity', 'we', 'first', 'study', 'a', 'nonrelativistic', 'particle', 'u... | [-0.09541122479291231, 0.16305169224848642, -0.14915381026837757, 0.06915792940965142, -0.17236537740145827, -0.05325214135204898, -0.0025738191211084815, 0.30057821490381864, -0.24738408188682562, -0.33353952867179815, -0.01980739145987101, -0.2209132291084411, -0.17427946560486568, 0.17947459059502638, -0.04113240122... |
709.0817 | Competition between final-state and pairing-gap effects in the
radio-frequency spectra of ultracold Fermi atoms | The radio-frequency spectra of ultracold Fermi atoms are calculated by
including final-state interactions affecting the excited level of the
transition, and compared with the experimental data. A competition is revealed
between pairing-gap effects which tend to push the oscillator strength toward
high frequencies awa... | cond-mat.supr-con cond-mat.other | the radiofrequency spectra of ultracold fermi atoms are calculated by including finalstate interactions affecting the excited level of the transition and compared with the experimental data a competition is revealed between pairinggap effects which tend to push the oscillator strength toward high frequencies away from ... | [['the', 'radiofrequency', 'spectra', 'of', 'ultracold', 'fermi', 'atoms', 'are', 'calculated', 'by', 'including', 'finalstate', 'interactions', 'affecting', 'the', 'excited', 'level', 'of', 'the', 'transition', 'and', 'compared', 'with', 'the', 'experimental', 'data', 'a', 'competition', 'is', 'revealed', 'between', '... | [-0.08805880063183365, 0.20131503920864455, -0.058821131828896984, 0.03563939610255822, -0.04265150231539562, -0.12724019327671618, 0.11316122856336616, 0.3481313844201385, -0.2541907411769673, -0.3230904721684994, 0.004659349188929604, -0.33132693013276465, -0.054339987245859, 0.1714668004718479, 0.05447914477397678, ... |
709.0818 | SPH simulations of the chemical evolution of bulges | We have implemented a chemical evolution model on the parallel AP3M+SPH DEVA
code which we use to perform high resolution simulations of spiral galaxy
formation. It includes feedback by SNII and SNIa using the Qij matrix
formalism. We also include a diffusion mechanism that spreads newly introduced
metals. The gas co... | astro-ph | we have implemented a chemical evolution model on the parallel ap3msph deva code which we use to perform high resolution simulations of spiral galaxy formation it includes feedback by snii and snia using the qij matrix formalism we also include a diffusion mechanism that spreads newly introduced metals the gas cooling ... | [['we', 'have', 'implemented', 'a', 'chemical', 'evolution', 'model', 'on', 'the', 'parallel', 'ap3msph', 'deva', 'code', 'which', 'we', 'use', 'to', 'perform', 'high', 'resolution', 'simulations', 'of', 'spiral', 'galaxy', 'formation', 'it', 'includes', 'feedback', 'by', 'snii', 'and', 'snia', 'using', 'the', 'qij', '... | [-0.08784518330711373, 0.11202712837374358, -0.08751627128679372, 0.09633930347419144, -0.04451790014198715, -0.0910191015323757, 0.06346780176058278, 0.3855497784180833, -0.23534314045017318, -0.31892626652344397, 0.0663862472980067, -0.24898033410447948, -0.07574809805165776, 0.18835144686662325, -0.01577056404702099... |
709.0819 | Spin-gravity coupling and gravity-induced quantum phases | External gravitational fields induce phase factors in the wave functions of
particles. The phases are exact to first order in the background gravitational
field, are manifestly covariant and gauge invariant and provide a useful tool
for the study of spin-gravity coupling and of the optics of particles in
gravitationa... | gr-qc | external gravitational fields induce phase factors in the wave functions of particles the phases are exact to first order in the background gravitational field are manifestly covariant and gauge invariant and provide a useful tool for the study of spingravity coupling and of the optics of particles in gravitational or ... | [['external', 'gravitational', 'fields', 'induce', 'phase', 'factors', 'in', 'the', 'wave', 'functions', 'of', 'particles', 'the', 'phases', 'are', 'exact', 'to', 'first', 'order', 'in', 'the', 'background', 'gravitational', 'field', 'are', 'manifestly', 'covariant', 'and', 'gauge', 'invariant', 'and', 'provide', 'a', ... | [-0.22450895295552317, 0.23464973018105542, -0.08187839052536422, 0.10069358354759594, -0.06587023934763339, -0.05313444554450966, -0.06613724310660646, 0.34460168994135326, -0.19541162488952515, -0.2895200583078558, 0.028556551414704513, -0.21932845174645385, -0.19290503509534848, 0.17315552619818067, 0.05838092305653... |
709.082 | Astrometry of Galactic Star Forming Region Sharpless 269 with VERA :
Parallax Measurements and Constraint on Outer Rotation Curve | We have performed high-precision astrometry of H2O maser sources in Galactic
star forming region Sharpless 269 (S269) with VERA. We have successfully
detected a trigonometric parallax of 189+/-8 micro-arcsec, corresponding to the
source distance of 5.28 +0.24/-0.22 kpc. This is the smallest parallax ever
measured, an... | astro-ph | we have performed highprecision astrometry of h2o maser sources in galactic star forming region sharpless 269 s269 with vera we have successfully detected a trigonometric parallax of 1898 microarcsec corresponding to the source distance of 528 024022 kpc this is the smallest parallax ever measured and the first one det... | [['we', 'have', 'performed', 'highprecision', 'astrometry', 'of', 'h2o', 'maser', 'sources', 'in', 'galactic', 'star', 'forming', 'region', 'sharpless', '269', 's269', 'with', 'vera', 'we', 'have', 'successfully', 'detected', 'a', 'trigonometric', 'parallax', 'of', '1898', 'microarcsec', 'corresponding', 'to', 'the', '... | [-0.10145602951389412, 0.04775945312260513, -0.09463521598104131, 0.03006280331724403, -0.12941029188836844, -0.047200794586218724, 0.04120912632089137, 0.3804548468960579, -0.2094682531743563, -0.37310366466814693, 0.09139469221718031, -0.29382146772199363, 0.04980938843552514, 0.2241320706571835, -0.03311461176521996... |
709.0821 | Random colourings of aperiodic graphs: Ergodic and spectral properties | We study randomly coloured graphs embedded into Euclidean space, whose vertex
sets are infinite, uniformly discrete subsets of finite local complexity. We
construct the appropriate ergodic dynamical systems, explicitly characterise
ergodic measures, and prove an ergodic theorem. For covariant operators of
finite rang... | math.SP math-ph math.MP math.PR | we study randomly coloured graphs embedded into euclidean space whose vertex sets are infinite uniformly discrete subsets of finite local complexity we construct the appropriate ergodic dynamical systems explicitly characterise ergodic measures and prove an ergodic theorem for covariant operators of finite range define... | [['we', 'study', 'randomly', 'coloured', 'graphs', 'embedded', 'into', 'euclidean', 'space', 'whose', 'vertex', 'sets', 'are', 'infinite', 'uniformly', 'discrete', 'subsets', 'of', 'finite', 'local', 'complexity', 'we', 'construct', 'the', 'appropriate', 'ergodic', 'dynamical', 'systems', 'explicitly', 'characterise', ... | [-0.14188255536956368, 0.17239514998867958, -0.08735774480306578, 0.14311564309281055, -0.019827806897444167, -0.10416459665672544, 0.07005679892932272, 0.36774507718574667, -0.25899038605254004, -0.2251108712301141, 0.10087968856398086, -0.29579711660604785, -0.10343425869251843, 0.12554712550007496, -0.06806491878685... |
709.0822 | Supersymmetric lattice models in one and two dimensions | We study and simulate N=2 supersymmetric Wess-Zumino models in one and two
dimensions. For any choice of the lattice derivative, the theories can be made
manifestly supersymmetric by adding appropriate improvement terms corresponding
to discretizations of surface integrals. In particular, we check that fermionic
and ... | hep-lat | we study and simulate n2 supersymmetric wesszumino models in one and two dimensions for any choice of the lattice derivative the theories can be made manifestly supersymmetric by adding appropriate improvement terms corresponding to discretizations of surface integrals in particular we check that fermionic and bosonic ... | [['we', 'study', 'and', 'simulate', 'n2', 'supersymmetric', 'wesszumino', 'models', 'in', 'one', 'and', 'two', 'dimensions', 'for', 'any', 'choice', 'of', 'the', 'lattice', 'derivative', 'the', 'theories', 'can', 'be', 'made', 'manifestly', 'supersymmetric', 'by', 'adding', 'appropriate', 'improvement', 'terms', 'corre... | [-0.0906264910702466, 0.1408764994591602, -0.061047618093179566, 0.11851248056755388, -0.043818370734137316, -0.1508680684906622, 0.012290311078636665, 0.3554980339775857, -0.17036431257243026, -0.31324301751518674, 0.10192941968673713, -0.29509353074436523, -0.112763465821507, 0.15246248661942322, -0.04431595014127558... |
709.0823 | Reply to ''Comment on 'Regularizing Capacity of Metabolic Networks' '' | In a recent paper [C. Marr, M. Mueller-Linow, and M.-T. Huett, Phys. Rev. E
75, 041917 (2007)] we discuss the pronounced potential of real metabolic
network topologies, compared to randomized counterparts, to regularize complex
binary dynamics. In their comment [P. Holme and M. Huss, arXiv:0705.4084v1],
Holme and Hus... | q-bio.MN nlin.CG | in a recent paper c marr m muellerlinow and mt huett phys rev e 75 041917 2007 we discuss the pronounced potential of real metabolic network topologies compared to randomized counterparts to regularize complex binary dynamics in their comment p holme and m huss arxiv07054084v1 holme and huss criticize our approach and ... | [['in', 'a', 'recent', 'paper', 'c', 'marr', 'm', 'muellerlinow', 'and', 'mt', 'huett', 'phys', 'rev', 'e', '75', '041917', '2007', 'we', 'discuss', 'the', 'pronounced', 'potential', 'of', 'real', 'metabolic', 'network', 'topologies', 'compared', 'to', 'randomized', 'counterparts', 'to', 'regularize', 'complex', 'binar... | [-0.11885591617409283, 0.06895420004506238, -0.06582565987527442, 0.06694106397648844, -0.04051890396513045, -0.11657748759204808, 0.11933505322891645, 0.37268864841272054, -0.21100773239651552, -0.30723257354962136, -0.00098812363217943, -0.2826395290187345, -0.22809097280601587, 0.16595064488311226, -0.06523974473194... |
709.0824 | On Random Unitary Channels | In this article we provide necessary and sufficient conditions for a
completely positive trace-preserving (CPT) map to be decomposable into a convex
combination of unitary maps. Additionally, we set out to define a proper
distance measure between a given CPT map and the set of random unitary maps,
and methods for cal... | quant-ph | in this article we provide necessary and sufficient conditions for a completely positive tracepreserving cpt map to be decomposable into a convex combination of unitary maps additionally we set out to define a proper distance measure between a given cpt map and the set of random unitary maps and methods for calculating... | [['in', 'this', 'article', 'we', 'provide', 'necessary', 'and', 'sufficient', 'conditions', 'for', 'a', 'completely', 'positive', 'tracepreserving', 'cpt', 'map', 'to', 'be', 'decomposable', 'into', 'a', 'convex', 'combination', 'of', 'unitary', 'maps', 'additionally', 'we', 'set', 'out', 'to', 'define', 'a', 'proper',... | [-0.08252570735251842, 0.11069992256040374, -0.09356373994766425, 0.07515657919510785, -0.04414645436271611, -0.15030944160082274, 0.1128691847423195, 0.39962944123480054, -0.31671901697085963, -0.22388636610574192, 0.09259620188838906, -0.2245064386477073, -0.1390422475317286, 0.19782300532226346, -0.07210691596517588... |
709.0825 | Shaping Planetary Nebulae by Jets | We conduct 2D axisymmetrical hydrodynamical simulations to investigate the
interaction of a collimated fast wind (CFW; wide jets) with a spherical AGB
wind. The code includes radiative cooling. We find that the shape of the
planetary nebula (PN) is sensitive to the exact mass loss history of the AGB
wind, and the ope... | astro-ph | we conduct 2d axisymmetrical hydrodynamical simulations to investigate the interaction of a collimated fast wind cfw wide jets with a spherical agb wind the code includes radiative cooling we find that the shape of the planetary nebula pn is sensitive to the exact mass loss history of the agb wind and the opening angle... | [['we', 'conduct', '2d', 'axisymmetrical', 'hydrodynamical', 'simulations', 'to', 'investigate', 'the', 'interaction', 'of', 'a', 'collimated', 'fast', 'wind', 'cfw', 'wide', 'jets', 'with', 'a', 'spherical', 'agb', 'wind', 'the', 'code', 'includes', 'radiative', 'cooling', 'we', 'find', 'that', 'the', 'shape', 'of', '... | [-0.11059210271209935, 0.09272417037449623, -0.06426771382036847, 0.10697627117866124, -0.09324062005880307, -0.06874144120352729, -0.029465991313973407, 0.45099295703869946, -0.19450538893195116, -0.3265547875033797, 0.03745613298884083, -0.23298634303171398, -0.018762463448955765, 0.23536533823693698, -0.013513061416... |
709.0826 | Diffuse Galactic light at high Galactic latitude: nature and
interpretation | The hypothesis of an extended red emission (ERE) in diffuse Galactic light
(DGL) has been put forward in 1998 by Gordon, Witt and Friedmann who found that
scattered starlight was not enough to explain the amount of DGL in the R band,
in some high Galactic latitude directions. This paper re-investigates, for high
Gala... | astro-ph | the hypothesis of an extended red emission ere in diffuse galactic light dgl has been put forward in 1998 by gordon witt and friedmann who found that scattered starlight was not enough to explain the amount of dgl in the r band in some high galactic latitude directions this paper reinvestigates for high galactic latitu... | [['the', 'hypothesis', 'of', 'an', 'extended', 'red', 'emission', 'ere', 'in', 'diffuse', 'galactic', 'light', 'dgl', 'has', 'been', 'put', 'forward', 'in', '1998', 'by', 'gordon', 'witt', 'and', 'friedmann', 'who', 'found', 'that', 'scattered', 'starlight', 'was', 'not', 'enough', 'to', 'explain', 'the', 'amount', 'of... | [-0.018760183645600035, 0.0844022547990867, -0.12982432892574935, 0.08694972647372055, -0.15290349562717384, -0.09241082205242196, 0.02327970014758726, 0.42927544737819495, -0.18569655680321445, -0.3387036283984203, 0.0019316097510285503, -0.2956188202207518, -0.038936122963132785, 0.19062930436501668, -0.1111784144485... |
709.0827 | Sympathetic cooling in a mixture of diamagnetic and paramagnetic atoms | We have experimentally realized a hybrid trap for ultracold paramagnetic
rubidium and diamagnetic ytterbium atoms by combining a bichromatic optical
dipole trap for ytterbium with a Ioffe-Pritchard-type magnetic trap for
rubidium. In this hybrid trap, sympathetic cooling of five different ytterbium
isotopes through e... | physics.atom-ph | we have experimentally realized a hybrid trap for ultracold paramagnetic rubidium and diamagnetic ytterbium atoms by combining a bichromatic optical dipole trap for ytterbium with a ioffepritchardtype magnetic trap for rubidium in this hybrid trap sympathetic cooling of five different ytterbium isotopes through elastic... | [['we', 'have', 'experimentally', 'realized', 'a', 'hybrid', 'trap', 'for', 'ultracold', 'paramagnetic', 'rubidium', 'and', 'diamagnetic', 'ytterbium', 'atoms', 'by', 'combining', 'a', 'bichromatic', 'optical', 'dipole', 'trap', 'for', 'ytterbium', 'with', 'a', 'ioffepritchardtype', 'magnetic', 'trap', 'for', 'rubidium... | [-0.07364987332204526, 0.36001729599736404, 0.06438755357257006, -0.05643030995182044, 0.15349026010230635, -0.23270944229355364, 0.10180889576969837, 0.48775572736154904, -0.12331022864038294, -0.21640283258801157, -0.12386605885959315, -0.3111672816854535, 0.0787001708522439, 0.20008817546521174, 0.1047324189690478, ... |
709.0828 | Study of the core-excited Fano Resonances in the neutron-rich C-isotopes | Fano Resonances are a new continuum excitation mode in light exotic nuclei.
By the QPC model we explain these sharp and asymmetric structures as due to the
coupling of a single particle elastic channel to the closed core-excited
channels. Theoretical model calculations are compared for 15C, 17C and 19C. The
theoretic... | nucl-th nucl-ex | fano resonances are a new continuum excitation mode in light exotic nuclei by the qpc model we explain these sharp and asymmetric structures as due to the coupling of a single particle elastic channel to the closed coreexcited channels theoretical model calculations are compared for 15c 17c and 19c the theoretical resu... | [['fano', 'resonances', 'are', 'a', 'new', 'continuum', 'excitation', 'mode', 'in', 'light', 'exotic', 'nuclei', 'by', 'the', 'qpc', 'model', 'we', 'explain', 'these', 'sharp', 'and', 'asymmetric', 'structures', 'as', 'due', 'to', 'the', 'coupling', 'of', 'a', 'single', 'particle', 'elastic', 'channel', 'to', 'the', 'c... | [-0.09628995879357981, 0.1354781941871249, -0.09202508171719889, 0.1353611119669832, 0.01264615761747043, -0.20554874573023088, 0.06168397745838569, 0.423612198522014, -0.18357594102440822, -0.30175031195845337, -0.032495282857017894, -0.34759673851752476, -0.08731038652871165, 0.1859135265263068, 0.028435786975727927,... |
709.0829 | Long GRBs from binary stars: runaway, Wolf-Rayet progenitors | The collapsar model for long gamma-ray bursts requires a rapidly rotating
Wolf-Rayet star as progenitor. We test the idea of producing rapidly rotating
Wolf-Rayet stars in massive close binaries through mass accretion and
consecutive quasi-chemically homogeneous evolution; the latter had previously
been shown to prov... | astro-ph | the collapsar model for long gammaray bursts requires a rapidly rotating wolfrayet star as progenitor we test the idea of producing rapidly rotating wolfrayet stars in massive close binaries through mass accretion and consecutive quasichemically homogeneous evolution the latter had previously been shown to provide coll... | [['the', 'collapsar', 'model', 'for', 'long', 'gammaray', 'bursts', 'requires', 'a', 'rapidly', 'rotating', 'wolfrayet', 'star', 'as', 'progenitor', 'we', 'test', 'the', 'idea', 'of', 'producing', 'rapidly', 'rotating', 'wolfrayet', 'stars', 'in', 'massive', 'close', 'binaries', 'through', 'mass', 'accretion', 'and', '... | [-0.10549626785255636, 0.2164072469138179, -0.029501896541641683, 0.18555504475169035, -0.14653750926693332, -0.11361561188170193, 0.09858663194356676, 0.39046637658790057, -0.142111030540296, -0.3141831078243499, 0.01216813160358377, -0.22866294526361994, 0.016721825495514334, 0.24350497133944335, -0.05317947556910922... |
709.083 | Small Angle Scattering and Zeta Potential of Liposomes Loaded with
Octa(carboranyl)porphyrazine | In this work the physicochemical characterization of liposomes loaded with a
newly synthesised carboranyl porphyrazine (H2HECASPz) is described. This
molecule represents a potential drug for different anticancer therapies, such
as Boron Neutron Capture Therapy, Photodynamic Therapy and Photothermal
Therapy. Different... | cond-mat.soft physics.bio-ph | in this work the physicochemical characterization of liposomes loaded with a newly synthesised carboranyl porphyrazine h2hecaspz is described this molecule represents a potential drug for different anticancer therapies such as boron neutron capture therapy photodynamic therapy and photothermal therapy different loading... | [['in', 'this', 'work', 'the', 'physicochemical', 'characterization', 'of', 'liposomes', 'loaded', 'with', 'a', 'newly', 'synthesised', 'carboranyl', 'porphyrazine', 'h2hecaspz', 'is', 'described', 'this', 'molecule', 'represents', 'a', 'potential', 'drug', 'for', 'different', 'anticancer', 'therapies', 'such', 'as', '... | [-0.08229723453111605, 0.18800380688754484, -0.04208076348391558, 0.05079892276115545, -0.014382314300079137, -0.16306032809063603, 0.03575997608243872, 0.3938409055865139, -0.23868188076148475, -0.2823156759467557, 0.05877417783250759, -0.2969448109746936, -0.13448166696850314, 0.18412011440569928, 0.00486154335234826... |
709.0831 | Eigenvalue pinching and application to the stability and the almost
umbilicity of hypersurfaces | In this paper we give pinching theorems for the first nonzero eigenvalue of
the Laplacian on the compact hypersurfaces of ambient spaces with bounded
sectional curvature. As application we deduce rigidity results for stable
constant mean curvature hypersurfaces $M$ of these spaces $N$. Indeed, we prove
that if $M$ is... | math.DG | in this paper we give pinching theorems for the first nonzero eigenvalue of the laplacian on the compact hypersurfaces of ambient spaces with bounded sectional curvature as application we deduce rigidity results for stable constant mean curvature hypersurfaces m of these spaces n indeed we prove that if m is included i... | [['in', 'this', 'paper', 'we', 'give', 'pinching', 'theorems', 'for', 'the', 'first', 'nonzero', 'eigenvalue', 'of', 'the', 'laplacian', 'on', 'the', 'compact', 'hypersurfaces', 'of', 'ambient', 'spaces', 'with', 'bounded', 'sectional', 'curvature', 'as', 'application', 'we', 'deduce', 'rigidity', 'results', 'for', 'st... | [-0.21872865172246328, 0.12866767390457157, -0.07122355553188495, 0.06628492961965174, -0.07116372224741749, -0.15062873902638535, -0.037792570662561926, 0.36742202745197894, -0.22514733700350356, -0.22188883093646267, 0.1329547611684385, -0.2922735427925875, -0.15136115149605078, 0.17859303826404796, -0.14469014634224... |
709.0832 | SPLASH: An interactive visualisation tool for Smoothed Particle
Hydrodynamics simulations | This paper presents SPLASH, a publicly available interactive visualisation
tool for Smoothed Particle Hydrodynamics (SPH) simulations. Visualisation of
SPH data is more complicated than for grid-based codes because the data is
defined on a set of irregular points and therefore requires a mapping procedure
to a two di... | astro-ph | this paper presents splash a publicly available interactive visualisation tool for smoothed particle hydrodynamics sph simulations visualisation of sph data is more complicated than for gridbased codes because the data is defined on a set of irregular points and therefore requires a mapping procedure to a two dimension... | [['this', 'paper', 'presents', 'splash', 'a', 'publicly', 'available', 'interactive', 'visualisation', 'tool', 'for', 'smoothed', 'particle', 'hydrodynamics', 'sph', 'simulations', 'visualisation', 'of', 'sph', 'data', 'is', 'more', 'complicated', 'than', 'for', 'gridbased', 'codes', 'because', 'the', 'data', 'is', 'de... | [-0.05367296089025331, 0.03152425843738736, -0.16748645453033253, 0.09790649303557494, -0.08924838125060958, -0.14981717690646362, -0.029527258717840035, 0.3895213245055996, -0.22653822957251507, -0.3490329850106858, 0.10635915519154739, -0.2487704884305668, -0.1250353508333389, 0.26411484876119246, -0.0524971553554328... |
709.0833 | An Introduction to Galactic Chemical Evolution | The formalism of the simple model of galactic chemical evolution (GCE) and
its main ingredients (stellar properties, initial mass function, star formation
rate and gas flows) are presented in this tutorial. It is stressed that GCE is
not (yet) an astrophysical theory, but it merely provides a framework in which
the l... | astro-ph | the formalism of the simple model of galactic chemical evolution gce and its main ingredients stellar properties initial mass function star formation rate and gas flows are presented in this tutorial it is stressed that gce is not yet an astrophysical theory but it merely provides a framework in which the large body of... | [['the', 'formalism', 'of', 'the', 'simple', 'model', 'of', 'galactic', 'chemical', 'evolution', 'gce', 'and', 'its', 'main', 'ingredients', 'stellar', 'properties', 'initial', 'mass', 'function', 'star', 'formation', 'rate', 'and', 'gas', 'flows', 'are', 'presented', 'in', 'this', 'tutorial', 'it', 'is', 'stressed', '... | [-0.05888891101428519, 0.09988660061489182, -0.09755179105030204, 0.10694756171142217, -0.07361366101593542, -0.02149381657363847, 0.026236879484548063, 0.3667810938786715, -0.22735813750081102, -0.3484381588641554, 0.027937039056930436, -0.26180004118941724, -0.10555704348635944, 0.2324212808982173, -0.042983740060166... |
709.0834 | AC/DC Susceptibility of the Heavy-Fermion Superconductor CePt3Si under
Pressure | We have investigated the pressure dependence of ac and dc susceptibilities of
the heavy-fermion superconductor CePt3Si (Tc= 0.75 K) that coexists with
antiferromagnetism (TN = 2.2 K). As hydrostatic pressure is increased, Tc first
decreases rapidly, then rather slowly near the critical pressure Pc = 0.6 GPa
and shows... | cond-mat.supr-con | we have investigated the pressure dependence of ac and dc susceptibilities of the heavyfermion superconductor cept3si tc 075 k that coexists with antiferromagnetism tn 22 k as hydrostatic pressure is increased tc first decreases rapidly then rather slowly near the critical pressure pc 06 gpa and shows a stronger decrea... | [['we', 'have', 'investigated', 'the', 'pressure', 'dependence', 'of', 'ac', 'and', 'dc', 'susceptibilities', 'of', 'the', 'heavyfermion', 'superconductor', 'cept3si', 'tc', '075', 'k', 'that', 'coexists', 'with', 'antiferromagnetism', 'tn', '22', 'k', 'as', 'hydrostatic', 'pressure', 'is', 'increased', 'tc', 'first', ... | [-0.20006859488785267, 0.26018496701942273, -0.046508179308363685, -0.0016631439060869593, -0.03350576453117861, -0.12493372499528858, 0.16089033380719936, 0.3594825037099697, -0.25473324904839195, -0.2697167061545231, 0.02052751033635879, -0.36540341071991456, -0.063111113494745, 0.12533440418472444, 0.062729601389556... |
Subsets and Splits
No community queries yet
The top public SQL queries from the community will appear here once available.