id float64 706 1.8k | title stringlengths 1 343 | abstract stringlengths 6 6.09k | categories stringlengths 5 125 | processed_abstract stringlengths 2 5.96k | tokenized_abstract stringlengths 8 8.74k | centroid stringlengths 2.1k 2.17k |
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709.3435 | Lepton flavor violating $\mu\to e\gamma$ and $\mu-e$ conversion in
unparticle physics | We have studied lepton flavor violation processes $\mu\to e\gamma$ and
$\mu-e$ conversion in nuclei induced by unparticle. Both ${\rm Br}(\mu\to
e\gamma)$ and $\mu-e$ conversion rate ${\rm CR}(\mu-e,{\rm Nuclei})$ strongly
depend on the scale dimension $d_{\cal U}$ and the unparticle coupling
$\lambda^{ff'}_{\rm K}$(... | hep-ph | we have studied lepton flavor violation processes muto egamma and mue conversion in nuclei induced by unparticle both rm brmuto egamma and mue conversion rate rm crmuerm nuclei strongly depend on the scale dimension d_cal u and the unparticle coupling lambdaff_rm kkv a s p present experimental upper bounds on rm brmuto... | [['we', 'have', 'studied', 'lepton', 'flavor', 'violation', 'processes', 'muto', 'egamma', 'and', 'mue', 'conversion', 'in', 'nuclei', 'induced', 'by', 'unparticle', 'both', 'rm', 'brmuto', 'egamma', 'and', 'mue', 'conversion', 'rate', 'rm', 'crmuerm', 'nuclei', 'strongly', 'depend', 'on', 'the', 'scale', 'dimension', ... | [-0.11664568546361156, 0.30142239201813936, 0.05917432718348527, 0.1993134981316943, -0.08437323479706214, -0.20672457406689074, 0.05113341665590212, 0.2722859859636556, -0.2194725793475906, -0.2859420927448405, -0.025140377464667258, -0.3402440351034914, 0.03501822867630316, 0.1472635313218075, 0.1243791850283742, 0.0... |
709.3436 | Higher Homotopy Hopf Algebras Found: A Ten Year Retrospective | The search for higher homotopy Hopf algebras (known today as
A_\infty-bialgebras) began in 1996 during a conference at Vassar College
honoring Jim Stasheff in the year of his 60th birthday. In a talk entitled "In
Search of Higher Homotopy Hopf Algebras", I indicated that a DG Hopf algebra
could be thought of as some ... | math.AT | the search for higher homotopy hopf algebras known today as a_inftybialgebras began in 1996 during a conference at vassar college honoring jim stasheff in the year of his 60th birthday in a talk entitled in search of higher homotopy hopf algebras i indicated that a dg hopf algebra could be thought of as some unknown hi... | [['the', 'search', 'for', 'higher', 'homotopy', 'hopf', 'algebras', 'known', 'today', 'as', 'a_inftybialgebras', 'began', 'in', '1996', 'during', 'a', 'conference', 'at', 'vassar', 'college', 'honoring', 'jim', 'stasheff', 'in', 'the', 'year', 'of', 'his', '60th', 'birthday', 'in', 'a', 'talk', 'entitled', 'in', 'searc... | [-0.15012698719302925, 0.06166733045912614, -0.08929806924840834, 0.09122817468180854, -0.1724201244604566, -0.1408157186711573, -0.012370171325788501, 0.27818966828220126, -0.33123496597233626, -0.29473028114755706, 0.13624396044074924, -0.20898660134324537, -0.21539914902366167, 0.13360770215513185, -0.19792803029330... |
709.3437 | Azimuthal distinguishability of entangled photons generated in
spontaneous parametric down-conversion | We experimentally demonstrate that paired photons generated in different
sections of a down-conversion cone, when some of the interacting waves show
Poynting vector walk-off, carry different spatial correlations, and therefore a
different degree of spatial entanglement. This is shown to be in agreement with
theoretic... | quant-ph | we experimentally demonstrate that paired photons generated in different sections of a downconversion cone when some of the interacting waves show poynting vector walkoff carry different spatial correlations and therefore a different degree of spatial entanglement this is shown to be in agreement with theoretical resul... | [['we', 'experimentally', 'demonstrate', 'that', 'paired', 'photons', 'generated', 'in', 'different', 'sections', 'of', 'a', 'downconversion', 'cone', 'when', 'some', 'of', 'the', 'interacting', 'waves', 'show', 'poynting', 'vector', 'walkoff', 'carry', 'different', 'spatial', 'correlations', 'and', 'therefore', 'a', '... | [-0.15644942726503358, 0.21172378480550832, -0.07355301490169949, 0.07838324012700468, -0.03718062329571694, -0.11778881907230243, -0.02299790157703683, 0.42389712454751133, -0.26266075726598503, -0.2564225438516587, 0.023353182851860766, -0.29470174744492394, -0.1026965943921823, 0.20039261842612177, 0.022004479978932... |
709.3438 | High Energy Neutrinos with a Mediterranean Neutrino Telescope | The high energy neutrino detection by a km^3 Neutrino Telescope placed in the
Mediterranean sea provides a unique tool to both determine the diffuse
astrophysical neutrino flux and the neutrino-nucleon cross section in the
extreme kinematical region, which could unveil the presence of new physics.
Here is performed a... | astro-ph hep-ph | the high energy neutrino detection by a km3 neutrino telescope placed in the mediterranean sea provides a unique tool to both determine the diffuse astrophysical neutrino flux and the neutrinonucleon cross section in the extreme kinematical region which could unveil the presence of new physics here is performed a brief... | [['the', 'high', 'energy', 'neutrino', 'detection', 'by', 'a', 'km3', 'neutrino', 'telescope', 'placed', 'in', 'the', 'mediterranean', 'sea', 'provides', 'a', 'unique', 'tool', 'to', 'both', 'determine', 'the', 'diffuse', 'astrophysical', 'neutrino', 'flux', 'and', 'the', 'neutrinonucleon', 'cross', 'section', 'in', 't... | [-0.07739459055509153, 0.1796972268493846, -0.028575687561117644, 0.2000889987123498, -0.06313461015400078, -0.06902178367766153, 0.048242236637244265, 0.29716408166236113, -0.15299102599965408, -0.3504071897560997, 0.05545460011489922, -0.29035900138218756, -0.05959560575761965, 0.2271749474041696, 0.05451001244728104... |
709.3439 | Multiple minor mergers: formation of elliptical galaxies and constraints
for the growth of spiral disks | Multiple, sequential mergers are unavoidable in the hierarchical build-up
picture of galaxies, in particular for the minor mergers that are frequent and
highly likely to have occured several times for most present-day galaxies.
However, the effect of repeated minor mergers on galactic structure and
evolution has not ... | astro-ph | multiple sequential mergers are unavoidable in the hierarchical buildup picture of galaxies in particular for the minor mergers that are frequent and highly likely to have occured several times for most presentday galaxies however the effect of repeated minor mergers on galactic structure and evolution has not been stu... | [['multiple', 'sequential', 'mergers', 'are', 'unavoidable', 'in', 'the', 'hierarchical', 'buildup', 'picture', 'of', 'galaxies', 'in', 'particular', 'for', 'the', 'minor', 'mergers', 'that', 'are', 'frequent', 'and', 'highly', 'likely', 'to', 'have', 'occured', 'several', 'times', 'for', 'most', 'presentday', 'galaxie... | [-0.11435705058026761, 0.10516109150344634, -0.07446051626225356, 0.12789642409067145, -0.07290667814005905, -0.0044197455542322635, -0.043291949276643774, 0.46383359270563734, -0.13749414449407124, -0.34033649688153045, 0.06040011087265909, -0.2546299154135591, -0.0997956592493273, 0.2165621135841477, -0.0267037873774... |
709.344 | New target transverse spin dependent azimuthal asymmetries from COMPASS
experiment | In general, eight target transverse spin-dependent azimuthal modulations are
allowed in semi inclusive deep inelastic scattering of polarized leptons on a
transversely polarized target. In the QCD parton model four of these
asymmetries can be interpreted within the leading order approach. Two of them,
namely Collins ... | hep-ex hep-ph | in general eight target transverse spindependent azimuthal modulations are allowed in semi inclusive deep inelastic scattering of polarized leptons on a transversely polarized target in the qcd parton model four of these asymmetries can be interpreted within the leading order approach two of them namely collins and siv... | [['in', 'general', 'eight', 'target', 'transverse', 'spindependent', 'azimuthal', 'modulations', 'are', 'allowed', 'in', 'semi', 'inclusive', 'deep', 'inelastic', 'scattering', 'of', 'polarized', 'leptons', 'on', 'a', 'transversely', 'polarized', 'target', 'in', 'the', 'qcd', 'parton', 'model', 'four', 'of', 'these', '... | [-0.05064282688381864, 0.2723541830004863, -0.15537835196287275, 0.14722442908090688, -0.025763179715200563, -0.08819950514290238, -0.045903646676566136, 0.468593962595006, -0.19631243200002185, -0.25226644896597505, -0.030443461755482116, -0.34485937994426097, 0.03384760713256965, 0.1823485404292174, 0.125724771112953... |
709.3441 | Arp 220 - IC 4553/4: understanding the system and diagnosing the ISM | Arp220 is a nearby system in final stages of galaxy merger with powerful
ongoing star-formation at and surrounding the two nuclei. Arp 220 was detected
in HI absorption and OH Megamaser emission and later recognized as the nearest
ultra-luminous infrared galaxy also showing powerful molecular and X-ray
emissions. In ... | astro-ph | arp220 is a nearby system in final stages of galaxy merger with powerful ongoing starformation at and surrounding the two nuclei arp 220 was detected in hi absorption and oh megamaser emission and later recognized as the nearest ultraluminous infrared galaxy also showing powerful molecular and xray emissions in this pa... | [['arp220', 'is', 'a', 'nearby', 'system', 'in', 'final', 'stages', 'of', 'galaxy', 'merger', 'with', 'powerful', 'ongoing', 'starformation', 'at', 'and', 'surrounding', 'the', 'two', 'nuclei', 'arp', '220', 'was', 'detected', 'in', 'hi', 'absorption', 'and', 'oh', 'megamaser', 'emission', 'and', 'later', 'recognized',... | [-0.04067125426198559, 0.015074201213395299, -0.03634936393549045, 0.10594133676254544, -0.052223243782746384, -0.0404305231607594, 0.005564607724001439, 0.4993236305984272, -0.13252673160563083, -0.2903147018354001, 0.06497400163555112, -0.3034806988448247, -0.014334768795504653, 0.1483022498646644, 0.0783310033081249... |
709.3442 | Sensitivity and Insensitivity of Galaxy Cluster Surveys to New Physics | We study the implications and limitations of galaxy cluster surveys for
constraining models of particle physics and gravity beyond the Standard Model.
Flux limited cluster counts probe the history of large scale structure
formation in the universe, and as such provide useful constraints on
cosmological parameters. As... | hep-ph astro-ph | we study the implications and limitations of galaxy cluster surveys for constraining models of particle physics and gravity beyond the standard model flux limited cluster counts probe the history of large scale structure formation in the universe and as such provide useful constraints on cosmological parameters as a re... | [['we', 'study', 'the', 'implications', 'and', 'limitations', 'of', 'galaxy', 'cluster', 'surveys', 'for', 'constraining', 'models', 'of', 'particle', 'physics', 'and', 'gravity', 'beyond', 'the', 'standard', 'model', 'flux', 'limited', 'cluster', 'counts', 'probe', 'the', 'history', 'of', 'large', 'scale', 'structure'... | [-0.05488010881751891, 0.10586162880870163, -0.09254738260586837, 0.19115126371076427, -0.1268057290383029, -0.07520385698856998, 0.0016478728310963542, 0.30783441436198566, -0.24682923053036032, -0.3759352785832796, 0.10348972480158447, -0.22921647192891112, -0.08856570993348495, 0.24142632709657677, 0.018073386071038... |
709.3443 | On the steady compressible Navier-Stokes-Fourier system | We study the motion of the steady compressible heat conducting viscous fluid
in a bounded three dimensional domain governed by the compressible
Navier-Stokes-Fourier system. Our main result is the existence of a weak
solution to these equations for arbitrarily large data. A key element of the
proof is a special appro... | math.AP math-ph math.MP | we study the motion of the steady compressible heat conducting viscous fluid in a bounded three dimensional domain governed by the compressible navierstokesfourier system our main result is the existence of a weak solution to these equations for arbitrarily large data a key element of the proof is a special approximati... | [['we', 'study', 'the', 'motion', 'of', 'the', 'steady', 'compressible', 'heat', 'conducting', 'viscous', 'fluid', 'in', 'a', 'bounded', 'three', 'dimensional', 'domain', 'governed', 'by', 'the', 'compressible', 'navierstokesfourier', 'system', 'our', 'main', 'result', 'is', 'the', 'existence', 'of', 'a', 'weak', 'solu... | [-0.1711919198940067, 0.07228771129034851, -0.07364460072038989, 0.0517954931373855, -0.06908730109418301, -0.12350520525421751, 0.03307103172410279, 0.2537495852497063, -0.2923813570290804, -0.2574601178817255, 0.16754400842136852, -0.21493367227529617, -0.06867601638169665, 0.19042245173630745, -0.08027457586109736, ... |
709.3444 | On period spaces for p-divisible groups | In their book Rapoport and Zink constructed rigid analytic period spaces for
Fontaine's filtered isocrystals, and period morphisms from moduli spaces of
p-divisible groups to some of these period spaces. We determine the image of
these period morphisms, thereby contributing to a question of Grothendieck. We
give exam... | math.NT math.AG | in their book rapoport and zink constructed rigid analytic period spaces for fontaines filtered isocrystals and period morphisms from moduli spaces of pdivisible groups to some of these period spaces we determine the image of these period morphisms thereby contributing to a question of grothendieck we give examples sho... | [['in', 'their', 'book', 'rapoport', 'and', 'zink', 'constructed', 'rigid', 'analytic', 'period', 'spaces', 'for', 'fontaines', 'filtered', 'isocrystals', 'and', 'period', 'morphisms', 'from', 'moduli', 'spaces', 'of', 'pdivisible', 'groups', 'to', 'some', 'of', 'these', 'period', 'spaces', 'we', 'determine', 'the', 'i... | [-0.1873154645963084, 0.09214079575169654, -0.1115292601863898, 0.1600738216195226, -0.10328947394228881, -0.07533949705225135, 0.028872039982132496, 0.4081814233065834, -0.3683331777962546, -0.21847068944147655, 0.12990733460404924, -0.18590549197757528, -0.1526158516339603, 0.269126085727106, -0.24521571314997143, -0... |
709.3445 | Opportunities for maser studies with the Square Kilometre Array | The Square Kilometre Array (SKA) is the radio telescope of the next
generation, providing an increase in sensitivity and angular resolution of two
orders of magnitude over existing telescopes. Currently, the SKA is expected to
span the frequency range 0.1-25 GHz with capabilities including a wide
field-of-view and me... | astro-ph | the square kilometre array ska is the radio telescope of the next generation providing an increase in sensitivity and angular resolution of two orders of magnitude over existing telescopes currently the ska is expected to span the frequency range 0125 ghz with capabilities including a wide fieldofview and measurement o... | [['the', 'square', 'kilometre', 'array', 'ska', 'is', 'the', 'radio', 'telescope', 'of', 'the', 'next', 'generation', 'providing', 'an', 'increase', 'in', 'sensitivity', 'and', 'angular', 'resolution', 'of', 'two', 'orders', 'of', 'magnitude', 'over', 'existing', 'telescopes', 'currently', 'the', 'ska', 'is', 'expected... | [-0.07649759496825936, 0.09848629782311491, 0.023224986871355213, 0.07366112400814018, -0.11774899845113396, -0.06576725854574761, 0.014459798716416117, 0.4372645501716761, -0.1761773676444136, -0.37684569838893367, 0.12497093251787561, -0.28793804905922116, -0.019293828579975525, 0.24081676603282176, 0.001603465523658... |
709.3446 | The integrals in Gradshteyn and Ryzhik. Part 10: the digamma function | Many integrals in the classical table by Gradshteyn and Ryzhik can be
evaluated in terms of the digamma function (= the logarithmic derivative of the
gamma function). Some of them are presented here.
| math.CA | many integrals in the classical table by gradshteyn and ryzhik can be evaluated in terms of the digamma function the logarithmic derivative of the gamma function some of them are presented here | [['many', 'integrals', 'in', 'the', 'classical', 'table', 'by', 'gradshteyn', 'and', 'ryzhik', 'can', 'be', 'evaluated', 'in', 'terms', 'of', 'the', 'digamma', 'function', 'the', 'logarithmic', 'derivative', 'of', 'the', 'gamma', 'function', 'some', 'of', 'them', 'are', 'presented', 'here']] | [-0.12481604161439463, 0.09441308200621279, -0.07034925535481307, 0.11896551499376073, -0.05460492451675236, -0.05812018451979384, 0.03510906955216342, 0.3363325676182285, -0.31821768556255847, -0.2682660500286147, 0.11311169447071734, -0.3092106159310788, -0.1910613727523014, 0.25760829728096724, -0.04601513517263811,... |
709.3447 | Hodge cohomology of invertible sheaves | v2: We improved a little bit according to the referee's wishes.
v1: On $X$ projective smooth over a field $k$, Pink and Roessler conjecture
that the dimension of the Hodge cohomology of an invertible $n$-torsion sheaf
$L$ is the same as the one of its $a$-th power $L^a$ if $a$ is prime to $n$,
under the assumptions... | math.AG | v2 we improved a little bit according to the referees wishes v1 on x projective smooth over a field k pink and roessler conjecture that the dimension of the hodge cohomology of an invertible ntorsion sheaf l is the same as the one of its ath power la if a is prime to n under the assumptions that x lifts to w_2k and dim... | [['v2', 'we', 'improved', 'a', 'little', 'bit', 'according', 'to', 'the', 'referees', 'wishes', 'v1', 'on', 'x', 'projective', 'smooth', 'over', 'a', 'field', 'k', 'pink', 'and', 'roessler', 'conjecture', 'that', 'the', 'dimension', 'of', 'the', 'hodge', 'cohomology', 'of', 'an', 'invertible', 'ntorsion', 'sheaf', 'l',... | [-0.22784675921271133, 0.10391257056577491, -0.13859216403216124, 0.03507598331092264, -0.03484164740128273, -0.22559065983038057, -0.022858678562227976, 0.3342643096069382, -0.35486935912208123, -0.20089665764773434, 0.01871268909255212, -0.2658609831240028, -0.09093904112338681, 0.17211260235529732, -0.14118033749982... |
709.3448 | On the auxiliary particle filter | In this article we study asymptotic properties of weighted samples produced
by the auxiliary particle filter (APF) proposed by pitt and shephard (1999).
Besides establishing a central limit theorem (CLT) for smoothed particle
estimates, we also derive bounds on the Lp error and bias of the same for a
finite particle ... | math.ST stat.TH | in this article we study asymptotic properties of weighted samples produced by the auxiliary particle filter apf proposed by pitt and shephard 1999 besides establishing a central limit theorem clt for smoothed particle estimates we also derive bounds on the lp error and bias of the same for a finite particle sample siz... | [['in', 'this', 'article', 'we', 'study', 'asymptotic', 'properties', 'of', 'weighted', 'samples', 'produced', 'by', 'the', 'auxiliary', 'particle', 'filter', 'apf', 'proposed', 'by', 'pitt', 'and', 'shephard', '1999', 'besides', 'establishing', 'a', 'central', 'limit', 'theorem', 'clt', 'for', 'smoothed', 'particle', ... | [-0.05280113514108618, 0.06852027449651428, -0.12900004406538704, 0.11704252344854879, -0.02022701730283926, -0.10138504102580109, 0.10185836824667552, 0.33467145789994523, -0.23938236033921745, -0.32947886622739286, 0.14097555967285033, -0.2463254934826971, -0.12673327799904038, 0.23092507901447737, -0.102840608789778... |
709.3449 | Blind Signal Separation Methods for the Identification of Interstellar
Carbonaceous Nanoparticles | The use of Blind Signal Separation methods (ICA and other approaches) for the
analysis of astrophysical data remains quite unexplored. In this paper, we
present a new approach for analyzing the infrared emission spectra of
interstellar dust, obtained with NASA's Spitzer Space Telescope, using FastICA
and Non-negative... | astro-ph | the use of blind signal separation methods ica and other approaches for the analysis of astrophysical data remains quite unexplored in this paper we present a new approach for analyzing the infrared emission spectra of interstellar dust obtained with nasas spitzer space telescope using fastica and nonnegative matrix fa... | [['the', 'use', 'of', 'blind', 'signal', 'separation', 'methods', 'ica', 'and', 'other', 'approaches', 'for', 'the', 'analysis', 'of', 'astrophysical', 'data', 'remains', 'quite', 'unexplored', 'in', 'this', 'paper', 'we', 'present', 'a', 'new', 'approach', 'for', 'analyzing', 'the', 'infrared', 'emission', 'spectra', ... | [-0.01422634260405017, 0.049822169198128194, -0.14954553874938384, 0.07383271593337312, -0.07984352557231551, -0.06813616507241259, -0.015636456554310153, 0.46464381354010625, -0.23435754517457733, -0.3137414312395065, 0.05557689455884468, -0.28319148518469023, -0.10727233641335497, 0.18818381554244654, -0.000241525762... |
709.345 | Fermion Masses and Mixings from Dihedral Flavor Symmetries with
Preserved Subgroups | We perform a systematic study of dihedral groups used as flavor symmetry. The
key feature here is the fact that we do not allow the dihedral groups to be
broken in an arbitrary way, but in all cases some
(non-trivial) subgroup has to be preserved. In this way we arrive at only
five possible (Dirac) mass matrix stru... | hep-ph | we perform a systematic study of dihedral groups used as flavor symmetry the key feature here is the fact that we do not allow the dihedral groups to be broken in an arbitrary way but in all cases some nontrivial subgroup has to be preserved in this way we arrive at only five possible dirac mass matrix structures which... | [['we', 'perform', 'a', 'systematic', 'study', 'of', 'dihedral', 'groups', 'used', 'as', 'flavor', 'symmetry', 'the', 'key', 'feature', 'here', 'is', 'the', 'fact', 'that', 'we', 'do', 'not', 'allow', 'the', 'dihedral', 'groups', 'to', 'be', 'broken', 'in', 'an', 'arbitrary', 'way', 'but', 'in', 'all', 'cases', 'some',... | [-0.14213398800073368, 0.22998785376955122, -0.05088206989304075, 0.07846562234632108, -0.06490525987596725, -0.13279198319387606, 0.05661001690610681, 0.37720385641562487, -0.2567512534541201, -0.28880836420850653, 0.08471666327106574, -0.26972955442824453, -0.1098633619078066, 0.1220901854516376, -0.00873157543806745... |
709.3451 | Search for photospheric footpoints of quiet Sun transition region loops | CONTEXT:The footpoints of quiet Sun Transition Region (TR) loops do not seem
to coincide with the photospheric magnetic structures appearing in traditional
low-sensitivity magnetograms.
AIMS: To look for the so-far unidentified photospheric footpoints of TR loops
using G-band bright points (BPs) as proxies for phot... | astro-ph | contextthe footpoints of quiet sun transition region tr loops do not seem to coincide with the photospheric magnetic structures appearing in traditional lowsensitivity magnetograms aims to look for the sofar unidentified photospheric footpoints of tr loops using gband bright points bps as proxies for photospheric magne... | [['contextthe', 'footpoints', 'of', 'quiet', 'sun', 'transition', 'region', 'tr', 'loops', 'do', 'not', 'seem', 'to', 'coincide', 'with', 'the', 'photospheric', 'magnetic', 'structures', 'appearing', 'in', 'traditional', 'lowsensitivity', 'magnetograms', 'aims', 'to', 'look', 'for', 'the', 'sofar', 'unidentified', 'pho... | [-0.1118598419946947, 0.21255036274156094, 0.024883660251897012, 0.15519486268407062, -0.12650403626920545, -0.13549336770494633, 0.022884680315174218, 0.5087487227420378, -0.12213113053482683, -0.36347199689172316, 0.11104862632483299, -0.2754201486514991, -0.07425702217391089, 0.15080461189962294, -0.0739890971610079... |
709.3452 | An Auslander-type result for Gorenstein-projective modules | An artin algebra $A$ is said to be CM-finite if there are only finitely many,
up to isomorphisms, indecomposable finitely generated Gorenstein-projective
$A$-modules. We prove that for a Gorenstein artin algebra, it is CM-finite if
and only if every its Gorenstein-projective module is a direct sum of finitely
generat... | math.RT math.RA | an artin algebra a is said to be cmfinite if there are only finitely many up to isomorphisms indecomposable finitely generated gorensteinprojective amodules we prove that for a gorenstein artin algebra it is cmfinite if and only if every its gorensteinprojective module is a direct sum of finitely generated gorensteinpr... | [['an', 'artin', 'algebra', 'a', 'is', 'said', 'to', 'be', 'cmfinite', 'if', 'there', 'are', 'only', 'finitely', 'many', 'up', 'to', 'isomorphisms', 'indecomposable', 'finitely', 'generated', 'gorensteinprojective', 'amodules', 'we', 'prove', 'that', 'for', 'a', 'gorenstein', 'artin', 'algebra', 'it', 'is', 'cmfinite',... | [-0.16759675490902737, 0.08844810756681909, -0.11684908551978879, 0.06043101983777888, -0.11013827932765707, -0.22953018598491326, -0.1426239818392787, 0.4250573239987716, -0.5303628754336387, -0.057934672106057405, 0.14579461859102594, -0.2612326451926492, -0.11006738520245563, 0.23919241763360333, -0.2156975076213712... |
709.3453 | L-algebras, triplicial-algebras, within an equivalence of categories
motivated by graphs | In a previous work, we gave a coalgebraic framework of directed graphs
equipped with weights (or probability vectors) in terms of (Markov)
L-coalgebras. They are K-vector spaces equipped with two co-operations,
\Delta_M, \tilde{\Delta}_M verifying,
(\tilde{\Delta}_M \otimes id)\Delta_M =(id \otimes \Delta_M)\tilde{... | math-ph math.MP | in a previous work we gave a coalgebraic framework of directed graphs equipped with weights or probability vectors in terms of markov lcoalgebras they are kvector spaces equipped with two cooperations delta_m tildedelta_m verifying tildedelta_m otimes iddelta_m id otimes delta_mtildedelta_m in this paper we study the c... | [['in', 'a', 'previous', 'work', 'we', 'gave', 'a', 'coalgebraic', 'framework', 'of', 'directed', 'graphs', 'equipped', 'with', 'weights', 'or', 'probability', 'vectors', 'in', 'terms', 'of', 'markov', 'lcoalgebras', 'they', 'are', 'kvector', 'spaces', 'equipped', 'with', 'two', 'cooperations', 'delta_m', 'tildedelta_m... | [-0.17305145906478478, 0.12546816339584974, -0.03649414381167541, 0.09521042779968598, -0.13317338350969246, -0.17788031979692348, -0.011372189994196957, 0.41056891339711654, -0.3307514786451625, -0.19241786910853803, 0.1022588126130032, -0.2532642087227522, -0.16449856879906014, 0.15730230942314777, -0.149001813344418... |
709.3454 | First Stars VIII -- Enrichment of the neutron-capture elements in the
early Galaxy | Our aim is to measure accurate, homogeneous neutron-capture element
abundances for the sample of 32 EMP giant stars studied earlier in this series,
including 22 stars with [Fe/H] $< -$3.0. Based on high-resolution, high S/N
spectra from the ESO VLT/UVES, 1D, LTE model atmospheres, and synthetic
spectrum fits, we dete... | astro-ph | our aim is to measure accurate homogeneous neutroncapture element abundances for the sample of 32 emp giant stars studied earlier in this series including 22 stars with feh 30 based on highresolution high sn spectra from the eso vltuves 1d lte model atmospheres and synthetic spectrum fits we determine abundances or upp... | [['our', 'aim', 'is', 'to', 'measure', 'accurate', 'homogeneous', 'neutroncapture', 'element', 'abundances', 'for', 'the', 'sample', 'of', '32', 'emp', 'giant', 'stars', 'studied', 'earlier', 'in', 'this', 'series', 'including', '22', 'stars', 'with', 'feh', '30', 'based', 'on', 'highresolution', 'high', 'sn', 'spectra... | [-0.021422874491068174, 0.149871102104232, 0.014113654831407575, 0.10804366749692457, 0.009890984931566359, -0.09149654623045511, 0.09552725483828564, 0.38150403662878385, -0.16132782107672175, -0.35114462288418524, -0.04473931940801039, -0.37271146693577367, 0.002763907414617705, 0.16857898785252343, -0.04596834806966... |
709.3455 | The Evolution of AGN Host Galaxies: From Blue to Red and the Influence
of Large-Scale Structures | We present an analysis of 109 moderate-luminosity (41.9 < Log L{0.5-8.0 keV}
< 43.7) AGN in the Extended Chandra Deep Field-South survey, which is drawn
from 5,549 galaxies from the COMBO-17 and GEMS surveys having 0.4 < z < 1.1.
These obscured or optically-weak AGN facilitate the study of their host
galaxies since t... | astro-ph | we present an analysis of 109 moderateluminosity 419 log l0580 kev 437 agn in the extended chandra deep fieldsouth survey which is drawn from 5549 galaxies from the combo17 and gems surveys having 04 z 11 these obscured or opticallyweak agn facilitate the study of their host galaxies since the agn provide an insubstant... | [['we', 'present', 'an', 'analysis', 'of', '109', 'moderateluminosity', '419', 'log', 'l0580', 'kev', '437', 'agn', 'in', 'the', 'extended', 'chandra', 'deep', 'fieldsouth', 'survey', 'which', 'is', 'drawn', 'from', '5549', 'galaxies', 'from', 'the', 'combo17', 'and', 'gems', 'surveys', 'having', '04', 'z', '11', 'thes... | [-0.0456331272258958, 0.11621103531161116, -0.05131610900299985, 0.104088604079069, -0.06788882525981238, -0.06233042452268359, 0.09359178093758663, 0.4904267335303496, -0.0674557793166616, -0.36859806133398765, 0.045416375960775794, -0.35172057362205167, 0.008276331740406699, 0.16662290672176663, -0.024981628069406226... |
709.3456 | Dynamics of Bloch Electrons in Time Dependent External Electric Fields:
Bounds for Interband Transitions | Using adiabatic expansions formalism, upper bounds for interband transitions
for Bloch electrons in slowly varying in time electric fields are obtained.
These bounds imply the validity of one-band approximation on long time scales.
| math-ph cond-mat.other math.MP | using adiabatic expansions formalism upper bounds for interband transitions for bloch electrons in slowly varying in time electric fields are obtained these bounds imply the validity of oneband approximation on long time scales | [['using', 'adiabatic', 'expansions', 'formalism', 'upper', 'bounds', 'for', 'interband', 'transitions', 'for', 'bloch', 'electrons', 'in', 'slowly', 'varying', 'in', 'time', 'electric', 'fields', 'are', 'obtained', 'these', 'bounds', 'imply', 'the', 'validity', 'of', 'oneband', 'approximation', 'on', 'long', 'time', '... | [-0.18019264229841417, 0.2620067676585732, -0.06606088323292858, 0.15724638759186774, -0.0050128634003075686, -0.13391506122989635, 0.12689242511987686, 0.3743568823644609, -0.18272659893740306, -0.3262220851399682, 0.03659956259511863, -0.20300767576378403, -0.023997336513165272, 0.2857214949573531, 0.1112758169007120... |
709.3457 | Concerning Hidden Momentum | The fact that the author of an excellent textbook on electromagnetism could
be duped by "hidden momentum" vividly illustrates the problematic nature of its
use.
| physics.class-ph | the fact that the author of an excellent textbook on electromagnetism could be duped by hidden momentum vividly illustrates the problematic nature of its use | [['the', 'fact', 'that', 'the', 'author', 'of', 'an', 'excellent', 'textbook', 'on', 'electromagnetism', 'could', 'be', 'duped', 'by', 'hidden', 'momentum', 'vividly', 'illustrates', 'the', 'problematic', 'nature', 'of', 'its', 'use']] | [-0.10720302723348141, 0.07059672783907445, -0.14655572672684988, 0.12520423221091428, -0.15893974815844558, -0.06844109054266785, 0.016350932496910293, 0.31571604947869975, -0.27216105613236624, -0.35153597756288946, 0.07000553499286373, -0.27190346852876246, -0.1827515933352212, 0.20741606007019678, -0.10317997207554... |
709.3458 | Large-angle production of charged pions by 3 GeV/c - 12.9 GeV/c protons
on beryllium, aluminium and lead targets | Measurements of the double-differential $\pi^{\pm}$ production cross-section
in the range of momentum $100 \MeVc \leq p < 800 \MeVc$ and angle $0.35 \rad
\leq \theta < 2.15 \rad$ in proton--beryllium, proton--aluminium and
proton--lead collisions are presented. The data were taken with the HARP
detector in the T9 bea... | hep-ex | measurements of the doubledifferential pipm production crosssection in the range of momentum 100 mevc leq p 800 mevc and angle 035 rad leq theta 215 rad in protonberyllium protonaluminium and protonlead collisions are presented the data were taken with the harp detector in the t9 beam line of the cern ps the pions were... | [['measurements', 'of', 'the', 'doubledifferential', 'pipm', 'production', 'crosssection', 'in', 'the', 'range', 'of', 'momentum', '100', 'mevc', 'leq', 'p', '800', 'mevc', 'and', 'angle', '035', 'rad', 'leq', 'theta', '215', 'rad', 'in', 'protonberyllium', 'protonaluminium', 'and', 'protonlead', 'collisions', 'are', '... | [-0.044800601455693444, 0.30194602362898876, -0.07707414895606537, 0.01507139044503371, 0.04375366582069546, -0.13307702670106664, -0.06111049017558495, 0.41474158671995004, -0.14451967297975596, -0.40118521094322207, -0.059229430186872684, -0.4069992517059048, 0.21816901839648684, 0.1925613716073955, 0.062856318770597... |
709.3459 | Did one observe couplings of right-handed quarks to W ? | I consider non standard EW couplings of light right-handed quarks to W and Z
suggested in a systematic non decoupling bottom-up low-energy effective theory
approach to possible extensions of the Standard Model. New experimental tests
in K^L_{mu3} decays based on recent measurements and scalar form factor
analysis are... | hep-ph hep-ex | i consider non standard ew couplings of light righthanded quarks to w and z suggested in a systematic non decoupling bottomup lowenergy effective theory approach to possible extensions of the standard model new experimental tests in kl_mu3 decays based on recent measurements and scalar form factor analysis are discusse... | [['i', 'consider', 'non', 'standard', 'ew', 'couplings', 'of', 'light', 'righthanded', 'quarks', 'to', 'w', 'and', 'z', 'suggested', 'in', 'a', 'systematic', 'non', 'decoupling', 'bottomup', 'lowenergy', 'effective', 'theory', 'approach', 'to', 'possible', 'extensions', 'of', 'the', 'standard', 'model', 'new', 'experim... | [-0.03867605516941033, 0.15157330435326774, -0.04224972299892794, 0.12538428940619764, -0.0781274946321818, -0.2182083461701757, 0.06480039245533672, 0.3357800829478286, -0.21507070857015523, -0.2847161777705575, 0.02369600974347894, -0.3206145296465944, -0.03752842117242063, 0.15277802122573397, 0.024511405633706036, ... |
709.346 | Superconducting charge qubits from a microscopic many-body perspective | The quantised Josephson junction equation that underpins the behaviour of
charge qubits and other tunnel devices is usually derived through cannonical
quantisation of the classical macroscopic Josephson relations. However, this
approach may neglect effects due to the fact that the charge qubit consists of
a supercond... | cond-mat.mes-hall cond-mat.supr-con quant-ph | the quantised josephson junction equation that underpins the behaviour of charge qubits and other tunnel devices is usually derived through cannonical quantisation of the classical macroscopic josephson relations however this approach may neglect effects due to the fact that the charge qubit consists of a superconducti... | [['the', 'quantised', 'josephson', 'junction', 'equation', 'that', 'underpins', 'the', 'behaviour', 'of', 'charge', 'qubits', 'and', 'other', 'tunnel', 'devices', 'is', 'usually', 'derived', 'through', 'cannonical', 'quantisation', 'of', 'the', 'classical', 'macroscopic', 'josephson', 'relations', 'however', 'this', 'a... | [-0.1711447966539047, 0.1688498518747193, -0.06787713864310221, 0.07686343512667174, -0.10342535744421184, -0.16938002084127882, 0.07387295797975225, 0.2763043064642592, -0.2583298671990633, -0.2882375335151499, -0.00553633259524676, -0.2713333230996134, -0.1300380016846413, 0.20524252936328677, -0.03137148709290407, 0... |
709.3461 | Fast Algorithm and Implementation of Dissimilarity Self-Organizing Maps | In many real world applications, data cannot be accurately represented by
vectors. In those situations, one possible solution is to rely on dissimilarity
measures that enable sensible comparison between observations. Kohonen's
Self-Organizing Map (SOM) has been adapted to data described only through their
dissimilari... | cs.NE cs.LG | in many real world applications data cannot be accurately represented by vectors in those situations one possible solution is to rely on dissimilarity measures that enable sensible comparison between observations kohonens selforganizing map som has been adapted to data described only through their dissimilarity matrix ... | [['in', 'many', 'real', 'world', 'applications', 'data', 'can', 'not', 'be', 'accurately', 'represented', 'by', 'vectors', 'in', 'those', 'situations', 'one', 'possible', 'solution', 'is', 'to', 'rely', 'on', 'dissimilarity', 'measures', 'that', 'enable', 'sensible', 'comparison', 'between', 'observations', 'kohonens',... | [-0.06654099454438048, 0.004201817873815474, -0.09877506879125056, 0.07319342240225524, -0.08840438518140997, -0.15013589038946, 0.06306028616814209, 0.42443039717418807, -0.2746732364169189, -0.3409659282836531, 0.11127075505575963, -0.2648294590067651, -0.18289676023913282, 0.2428999968019447, -0.09112216542341879, 0... |
709.3462 | Can High Frequency Acoustic Waves Heat the Quiet Sun Chromosphere? | We use Hinode/SOT Ca II H-line and blue continuum broadband observations to
study the presence and power of high frequency acoustic waves at high spatial
resolution. We find that there is no dominant power at small spatial scales;
the integrated power using the full resolution of Hinode (0.05'' pixels, 0.16''
resolut... | astro-ph | we use hinodesot ca ii hline and blue continuum broadband observations to study the presence and power of high frequency acoustic waves at high spatial resolution we find that there is no dominant power at small spatial scales the integrated power using the full resolution of hinode 005 pixels 016 resolution is larger ... | [['we', 'use', 'hinodesot', 'ca', 'ii', 'hline', 'and', 'blue', 'continuum', 'broadband', 'observations', 'to', 'study', 'the', 'presence', 'and', 'power', 'of', 'high', 'frequency', 'acoustic', 'waves', 'at', 'high', 'spatial', 'resolution', 'we', 'find', 'that', 'there', 'is', 'no', 'dominant', 'power', 'at', 'small'... | [-0.0977085561624595, 0.14975825347272412, 0.03978877333024034, 0.06290707045949863, -0.059959327555926784, -0.07084616179844098, 0.04987215994125498, 0.40543262202824865, -0.19093776980963803, -0.37079275566419323, 0.09549771543326123, -0.31047911329660566, -0.01706836688432044, 0.18707174668753787, -0.039513301636491... |
709.3463 | Quantum Ratchets for Quantum Communication with Optical Superlattices | We propose to use a quantum ratchet to transport quantum information in a
chain of atoms trapped in an optical superlattice. The quantum ratchet is
created by a continuous modulation of the optical superlattice which is
periodic in time and in space. Though there is zero average force acting on the
atoms, we show tha... | quant-ph cond-mat.other | we propose to use a quantum ratchet to transport quantum information in a chain of atoms trapped in an optical superlattice the quantum ratchet is created by a continuous modulation of the optical superlattice which is periodic in time and in space though there is zero average force acting on the atoms we show that ind... | [['we', 'propose', 'to', 'use', 'a', 'quantum', 'ratchet', 'to', 'transport', 'quantum', 'information', 'in', 'a', 'chain', 'of', 'atoms', 'trapped', 'in', 'an', 'optical', 'superlattice', 'the', 'quantum', 'ratchet', 'is', 'created', 'by', 'a', 'continuous', 'modulation', 'of', 'the', 'optical', 'superlattice', 'which... | [-0.17605862830385355, 0.21051381575026554, -0.04909812018593561, -0.0037477353559748, -0.002182661759065865, -0.19882298271242482, 0.10919685188616049, 0.4458297086950344, -0.27613280303894155, -0.23417669340166486, 0.03066152157674579, -0.26970817858082113, -0.11949532785116919, 0.19219531021906133, -0.03863224679293... |
709.3464 | Large-angle production of charged pions by 3 GeV/c - 12 GeV/c protons on
carbon, copper and tin targets | A measurement of the double-differential $\pi^{\pm}$ production cross-section
in proton--carbon, proton--copper and proton--tin collisions in the range of
pion momentum $100 \MeVc \leq p < 800 \MeVc$ and angle $0.35 \rad \le \theta
<2.15 \rad$ is presented. The data were taken with the HARP detector in the T9
beam li... | hep-ex | a measurement of the doubledifferential pipm production crosssection in protoncarbon protoncopper and protontin collisions in the range of pion momentum 100 mevc leq p 800 mevc and angle 035 rad le theta 215 rad is presented the data were taken with the harp detector in the t9 beam line of the cern ps the pions were pr... | [['a', 'measurement', 'of', 'the', 'doubledifferential', 'pipm', 'production', 'crosssection', 'in', 'protoncarbon', 'protoncopper', 'and', 'protontin', 'collisions', 'in', 'the', 'range', 'of', 'pion', 'momentum', '100', 'mevc', 'leq', 'p', '800', 'mevc', 'and', 'angle', '035', 'rad', 'le', 'theta', '215', 'rad', 'is'... | [-0.07196806519682532, 0.2970827550859507, -0.08341948054304582, 0.023115935122994313, 0.06138157549242056, -0.11881023199989421, -0.06645323197081895, 0.39981285333108735, -0.15380770898289636, -0.363214592567422, -0.0637815734092802, -0.38930668352617764, 0.20313863300810187, 0.1833000467437595, 0.06786863273009658, ... |
709.3465 | Dynamical Quantum Geometry (DQG Programme) | In this brief note (written as a lengthy letter), we describe the
construction of a representation for the Weyl-algebra underlying Loop Quantum
Geometry constructed from a diffeomorphism variant state, which corresponds to
a ''condensate'' of Loop Quantum Geometry, resembling a static spatial
geometry. We present the... | gr-qc | in this brief note written as a lengthy letter we describe the construction of a representation for the weylalgebra underlying loop quantum geometry constructed from a diffeomorphism variant state which corresponds to a condensate of loop quantum geometry resembling a static spatial geometry we present the kinematical ... | [['in', 'this', 'brief', 'note', 'written', 'as', 'a', 'lengthy', 'letter', 'we', 'describe', 'the', 'construction', 'of', 'a', 'representation', 'for', 'the', 'weylalgebra', 'underlying', 'loop', 'quantum', 'geometry', 'constructed', 'from', 'a', 'diffeomorphism', 'variant', 'state', 'which', 'corresponds', 'to', 'a',... | [-0.14034458103294417, 0.19447222005159923, -0.15413395808612154, 0.0865598512393218, -0.09304431532850353, -0.13146294050469495, -0.0019165610599263412, 0.2940685707655531, -0.2658028055966275, -0.25913262718766017, 0.07888526448315554, -0.19927152585828814, -0.1708493589894937, 0.10979346974423473, -0.067689097952097... |
709.3466 | Iwasawa decompositions of split Kac-Moody groups | We characterize all fields F for which a group with an F-locally split root
group datum admits an Iwasawa decomposition. This class of groups in particular
includes the split semisimple algebraic groups and the split Kac-Moody groups.
| math.GR | we characterize all fields f for which a group with an flocally split root group datum admits an iwasawa decomposition this class of groups in particular includes the split semisimple algebraic groups and the split kacmoody groups | [['we', 'characterize', 'all', 'fields', 'f', 'for', 'which', 'a', 'group', 'with', 'an', 'flocally', 'split', 'root', 'group', 'datum', 'admits', 'an', 'iwasawa', 'decomposition', 'this', 'class', 'of', 'groups', 'in', 'particular', 'includes', 'the', 'split', 'semisimple', 'algebraic', 'groups', 'and', 'the', 'split'... | [-0.2788287656019545, 0.05461614755606408, -0.1480775230253736, 0.023451364091468148, -0.19481042693627793, -0.10181344609655854, -0.06746624953423937, 0.3513294484259354, -0.3557853371732765, -0.2021739537206789, 0.11579533683511221, -0.16091082027802864, -0.10309031510001256, 0.1991544653299368, -0.1335718506274538, ... |
709.3467 | Eigenvalue bounds for polynomial central potentials in d dimensions | If a single particle obeys non-relativistic QM in R^d and has the Hamiltonian
H = - Delta + f(r), where f(r)=sum_{i = 1}^{k}a_ir^{q_i}, 2\leq q_i < q_{i+1},
a_i \geq 0$, then the eigenvalues E = E_{n\ell}^{(d)}(\lambda) are given
approximately by the semi-classical expression E = \min_{r > 0}[\frac{1}{r^2} +
\sum_{i ... | math-ph math.MP | if a single particle obeys nonrelativistic qm in rd and has the hamiltonian h delta fr where frsum_i 1ka_irq_i 2leq q_i q_i1 a_i geq 0 then the eigenvalues e e_nelldlambda are given approximately by the semiclassical expression e min_r 0frac1r2 sum_i 1ka_ip_irq_i it is proved that this formula yields a lower bound if p... | [['if', 'a', 'single', 'particle', 'obeys', 'nonrelativistic', 'qm', 'in', 'rd', 'and', 'has', 'the', 'hamiltonian', 'h', 'delta', 'fr', 'where', 'frsum_i', '1ka_irq_i', '2leq', 'q_i', 'q_i1', 'a_i', 'geq', '0', 'then', 'the', 'eigenvalues', 'e', 'e_nelldlambda', 'are', 'given', 'approximately', 'by', 'the', 'semiclass... | [-0.10256715419997747, 0.1483010864908395, -0.01640433123550163, -0.03374898198078601, -0.023209658813161345, -0.21466768903818984, 0.05487956425998933, 0.2787236036804433, -0.15729633834069737, -0.3082138764671981, -0.02959791597050543, -0.3259161234403459, -0.14207407219621998, 0.1779570760232253, -0.0784914595791353... |
709.3468 | Ergodic behaviour of "signed voter models" | We consider some questions raised by the recent paper of Gantert, L\"owe and
Steif (2005) concerning ``signed'' voter models on locally finite graphs. These
are voter model like processes with the difference that the edges are
considered to be either positive or negative. If an edge between a site $x$ and
a site $y$ ... | math.PR | we consider some questions raised by the recent paper of gantert lowe and steif 2005 concerning signed voter models on locally finite graphs these are voter model like processes with the difference that the edges are considered to be either positive or negative if an edge between a site x and a site y is negative respe... | [['we', 'consider', 'some', 'questions', 'raised', 'by', 'the', 'recent', 'paper', 'of', 'gantert', 'lowe', 'and', 'steif', '2005', 'concerning', 'signed', 'voter', 'models', 'on', 'locally', 'finite', 'graphs', 'these', 'are', 'voter', 'model', 'like', 'processes', 'with', 'the', 'difference', 'that', 'the', 'edges', ... | [-0.12620135950969485, 0.18433047285485904, 0.019793569746359093, 0.049636935686022496, -0.037920591307849416, -0.22470602573736048, 0.08664796595524134, 0.40883135772878076, -0.27193476024038366, -0.24421285351783764, 0.13264001948509094, -0.36544689922252804, -0.11184586178250157, 0.12879391688649067, -0.060493468059... |
709.3469 | On geodesic homotopies of controlled width and conjugacies in isometry
groups | We give an analytical proof of the Poincare-type inequalities for widths of
geodesic homotopies between equivariant maps valued in Hadamard metric spaces.
As an application we obtain a linear bound for the length of an element
conjugating two finite lists in a group acting on an Hadamard space.
| math.GT math.AP math.MG | we give an analytical proof of the poincaretype inequalities for widths of geodesic homotopies between equivariant maps valued in hadamard metric spaces as an application we obtain a linear bound for the length of an element conjugating two finite lists in a group acting on an hadamard space | [['we', 'give', 'an', 'analytical', 'proof', 'of', 'the', 'poincaretype', 'inequalities', 'for', 'widths', 'of', 'geodesic', 'homotopies', 'between', 'equivariant', 'maps', 'valued', 'in', 'hadamard', 'metric', 'spaces', 'as', 'an', 'application', 'we', 'obtain', 'a', 'linear', 'bound', 'for', 'the', 'length', 'of', 'a... | [-0.18380392919061705, 0.09149297647551673, -0.08946917550444293, 0.10084016023514171, -0.07930186782808353, -0.09203062685749804, 0.00174201640766114, 0.40638849635918933, -0.30914209177717566, -0.18084430818756422, 0.11066166939660131, -0.2840963678706127, -0.1298177557376524, 0.2830212007199104, -0.09767514273213844... |
709.347 | Constraints on sigma_8 from galaxy clustering in N-body simulations and
semi-analytic models | We generate mock galaxy catalogues for a grid of different cosmologies, using
rescaled N-body simulations in tandem with a semi-analytic model run using
consistent parameters. Because we predict the galaxy bias, rather than fitting
it as a nuisance parameter, we obtain an almost pure constraint on sigma_8 by
comparin... | astro-ph | we generate mock galaxy catalogues for a grid of different cosmologies using rescaled nbody simulations in tandem with a semianalytic model run using consistent parameters because we predict the galaxy bias rather than fitting it as a nuisance parameter we obtain an almost pure constraint on sigma_8 by comparing the pr... | [['we', 'generate', 'mock', 'galaxy', 'catalogues', 'for', 'a', 'grid', 'of', 'different', 'cosmologies', 'using', 'rescaled', 'nbody', 'simulations', 'in', 'tandem', 'with', 'a', 'semianalytic', 'model', 'run', 'using', 'consistent', 'parameters', 'because', 'we', 'predict', 'the', 'galaxy', 'bias', 'rather', 'than', ... | [-0.005465300138277268, -0.009193429978593655, -0.13371530761234243, 0.15940946488360716, -0.1243209488123481, -0.08196336336499244, 0.04613667621811013, 0.42067774829634447, -0.16368432408362105, -0.3769038594899732, 0.0628889551895469, -0.31390698613566265, -0.031246001724622142, 0.24042874344723975, -0.0142254021579... |
709.3471 | Possible solution of the J/psi production puzzle | We argue that the s-channel cut contribution to J/psi hadroproduction can be
significantly larger than the usual cut contribution of the color-singlet
mechanism, which is known to underestimate the experimental measurements. A
scenario accounting for intermediate $c\bar(c)$ interactions is proposed that
reproduces th... | hep-ph hep-ex nucl-th | we argue that the schannel cut contribution to jpsi hadroproduction can be significantly larger than the usual cut contribution of the colorsinglet mechanism which is known to underestimate the experimental measurements a scenario accounting for intermediate cbarc interactions is proposed that reproduces the data at lo... | [['we', 'argue', 'that', 'the', 'schannel', 'cut', 'contribution', 'to', 'jpsi', 'hadroproduction', 'can', 'be', 'significantly', 'larger', 'than', 'the', 'usual', 'cut', 'contribution', 'of', 'the', 'colorsinglet', 'mechanism', 'which', 'is', 'known', 'to', 'underestimate', 'the', 'experimental', 'measurements', 'a', ... | [-0.048814526805654165, 0.27628380923664997, -0.15461715836094558, 0.16473914267927675, -0.08390270865056663, -0.14482806359550782, -0.011732308127518212, 0.3500693336661373, -0.1890813547718738, -0.23836191381726946, -0.10305315292207524, -0.3940174331356372, 0.09848164612028215, 0.14364359469951263, 0.092700734534966... |
709.3472 | ACTIVIA: Calculation of Isotope Production Cross-sections and Yields | We present a C++ computer package, ACTIVIA, that can calculate target-product
cross-sections and the production and decay yields of isotopes from cosmic ray
activation using data tables and semi-empirical formulae. We describe the
structure and user interface of the computer code as well as provide
comparisons betwee... | nucl-ex | we present a c computer package activia that can calculate targetproduct crosssections and the production and decay yields of isotopes from cosmic ray activation using data tables and semiempirical formulae we describe the structure and user interface of the computer code as well as provide comparisons between the calc... | [['we', 'present', 'a', 'c', 'computer', 'package', 'activia', 'that', 'can', 'calculate', 'targetproduct', 'crosssections', 'and', 'the', 'production', 'and', 'decay', 'yields', 'of', 'isotopes', 'from', 'cosmic', 'ray', 'activation', 'using', 'data', 'tables', 'and', 'semiempirical', 'formulae', 'we', 'describe', 'th... | [-0.005270957435939962, 0.06555296653247901, -0.08594851528030278, 0.13345316194220266, -0.04488965276795537, -0.14352089488434036, 0.04441018805338709, 0.4210003711172004, -0.23523461738073115, -0.35414477040184966, 0.0760224780950473, -0.30439724461801015, -0.1251914059159471, 0.2906131566373576, 0.04181893185170284,... |
709.3473 | Exact solutions for the populations of the n-level ion | We present a matrix solution to the full equations of statistical equilibrium
that give the energy level populations of collisionally-excited ions in
photoionised gaseous nebulae. The rationale for such a calculation is to
maintain a parity between improvements in the quantum-mechanically evaluated
values for collisi... | astro-ph | we present a matrix solution to the full equations of statistical equilibrium that give the energy level populations of collisionallyexcited ions in photoionised gaseous nebulae the rationale for such a calculation is to maintain a parity between improvements in the quantummechanically evaluated values for collision st... | [['we', 'present', 'a', 'matrix', 'solution', 'to', 'the', 'full', 'equations', 'of', 'statistical', 'equilibrium', 'that', 'give', 'the', 'energy', 'level', 'populations', 'of', 'collisionallyexcited', 'ions', 'in', 'photoionised', 'gaseous', 'nebulae', 'the', 'rationale', 'for', 'such', 'a', 'calculation', 'is', 'to'... | [-0.034047832499449475, 0.05680935129935928, -0.02947823046249271, 0.09226569466035081, -0.02806503992427939, -0.1517519033264502, 0.039448402505201687, 0.3799578095069072, -0.2098816514763582, -0.3268270154882755, 0.07577669670032004, -0.27516015454228704, -0.05042857437427821, 0.20748352695289732, 0.03445869257367511... |
709.3474 | Quasar Clustering at $25\kpch$ from a Complete Sample of Binaries | We present spectroscopy of binary quasar candidates selected from Data
Release 4 of the Sloan Digital Sky Survey (SDSS DR4) using Kernel Density
Estimation (KDE). We present 27 new sets of observations, 10 of which are
binary quasars, roughly doubling the number of known $g < 21$ binaries with
component separations o... | astro-ph | we present spectroscopy of binary quasar candidates selected from data release 4 of the sloan digital sky survey sdss dr4 using kernel density estimation kde we present 27 new sets of observations 10 of which are binary quasars roughly doubling the number of known g 21 binaries with component separations of 3 to 6 only... | [['we', 'present', 'spectroscopy', 'of', 'binary', 'quasar', 'candidates', 'selected', 'from', 'data', 'release', '4', 'of', 'the', 'sloan', 'digital', 'sky', 'survey', 'sdss', 'dr4', 'using', 'kernel', 'density', 'estimation', 'kde', 'we', 'present', '27', 'new', 'sets', 'of', 'observations', '10', 'of', 'which', 'are... | [-0.06779134768237104, 0.07379536071635884, -0.07118826694421324, 0.11012879463515299, -0.14257375064634664, -0.095217237356758, 0.04652346937515426, 0.4271969935400229, -0.14163566971672517, -0.37707069652228087, 0.07664667303381743, -0.3525962747779547, -0.01788937356323004, 0.21023262013936891, -0.025235695559896673... |
709.3475 | On the mathematical origin of quantum space-time | An Euclidean topological space E is homeomorphic to the subset of
delta-functions of the space D'(E) of Schwartz distributions on E. Herewith,
any smooth function of compact support on E is extended onto D'(E). One can
think of these extensions as sue generis quantum deformations. In quantum
models, one therefore sho... | math-ph math.MP | an euclidean topological space e is homeomorphic to the subset of deltafunctions of the space de of schwartz distributions on e herewith any smooth function of compact support on e is extended onto de one can think of these extensions as sue generis quantum deformations in quantum models one therefore should replace in... | [['an', 'euclidean', 'topological', 'space', 'e', 'is', 'homeomorphic', 'to', 'the', 'subset', 'of', 'deltafunctions', 'of', 'the', 'space', 'de', 'of', 'schwartz', 'distributions', 'on', 'e', 'herewith', 'any', 'smooth', 'function', 'of', 'compact', 'support', 'on', 'e', 'is', 'extended', 'onto', 'de', 'one', 'can', '... | [-0.12840882166609413, 0.11084123813288599, -0.1365136033473689, 0.05797117382486458, -0.08333400055216472, -0.09041169391120554, -0.04561157981086461, 0.3198272786179527, -0.23359855087321313, -0.18839358236091058, 0.04260741757442717, -0.27736360130862137, -0.11522316169299063, 0.2513112131750486, -0.1290299118053717... |
709.3476 | On Brill-Noether loci over Quot schemes and a Torelli theorem | We prove a non abelian Torelli type result for smooth projective curves by
working in the derived category of some associated polarized Quot schemes and
defining Brill-Noether loci and Abel-Jacobi maps on them.
| math.AG math.KT | we prove a non abelian torelli type result for smooth projective curves by working in the derived category of some associated polarized quot schemes and defining brillnoether loci and abeljacobi maps on them | [['we', 'prove', 'a', 'non', 'abelian', 'torelli', 'type', 'result', 'for', 'smooth', 'projective', 'curves', 'by', 'working', 'in', 'the', 'derived', 'category', 'of', 'some', 'associated', 'polarized', 'quot', 'schemes', 'and', 'defining', 'brillnoether', 'loci', 'and', 'abeljacobi', 'maps', 'on', 'them']] | [-0.22784017410242197, -0.011913812105459247, -0.1104078847124721, 0.16398287722558685, -0.08745984716171568, -0.2194857047447427, 0.05019518614492633, 0.34172566929324105, -0.36742960198810604, -0.12322507993402806, 0.10253675552578925, -0.17850911354109872, -0.13495543805148566, 0.3098924821524909, -0.254348593368900... |
709.3477 | Realization and application of a 111 million pixel backside-illuminated
detector and camera | A full-wafer, 10,580 $\times$ 10,560 pixel (95 $\times$ 95 mm) CCD was
designed and tested at Semiconductor Technology Associates (STA) with 9 um
square pixels and 16 outputs. The chip was successfully fabricated in 2006 at
DALSA and some performance results are presented here. This program was funded
by the Office o... | astro-ph | a fullwafer 10580 times 10560 pixel 95 times 95 mm ccd was designed and tested at semiconductor technology associates sta with 9 um square pixels and 16 outputs the chip was successfully fabricated in 2006 at dalsa and some performance results are presented here this program was funded by the office of naval research t... | [['a', 'fullwafer', '10580', 'times', '10560', 'pixel', '95', 'times', '95', 'mm', 'ccd', 'was', 'designed', 'and', 'tested', 'at', 'semiconductor', 'technology', 'associates', 'sta', 'with', '9', 'um', 'square', 'pixels', 'and', '16', 'outputs', 'the', 'chip', 'was', 'successfully', 'fabricated', 'in', '2006', 'at', '... | [-0.06811777680926025, 0.09771318897046148, 0.015862665991298854, -0.028087084596045316, -0.0595539970099926, -0.195493906237185, 0.05996025058627129, 0.39626432085037233, -0.1504244883963838, -0.42293204690515995, 0.14883802405744792, -0.31119951486215, -0.04658217808231711, 0.2536601948812604, -0.07680663778446614, 0... |
709.3478 | On perturbative field theory and twistor string theory | It is well-known that perturbative calculations in field theory can lead to
far simpler answers than the Feynman diagram approach might suggest. In some
cases scattering amplitudes can be constructed for processes with any desired
number of external legs yielding compact expressions which are inaccessible
from the po... | hep-th hep-ph | it is wellknown that perturbative calculations in field theory can lead to far simpler answers than the feynman diagram approach might suggest in some cases scattering amplitudes can be constructed for processes with any desired number of external legs yielding compact expressions which are inaccessible from the point ... | [['it', 'is', 'wellknown', 'that', 'perturbative', 'calculations', 'in', 'field', 'theory', 'can', 'lead', 'to', 'far', 'simpler', 'answers', 'than', 'the', 'feynman', 'diagram', 'approach', 'might', 'suggest', 'in', 'some', 'cases', 'scattering', 'amplitudes', 'can', 'be', 'constructed', 'for', 'processes', 'with', 'a... | [-0.12061761692508727, 0.1721514783165723, -0.12045149473442125, 0.15012198360196605, -0.10502839826063073, -0.10815568666067757, 0.0372235639056997, 0.3253235056968954, -0.17360536607976282, -0.25858099023936737, 0.057758044008314295, -0.2488444958277391, -0.20675242760124765, 0.16656399211169323, -0.04610552201673638... |
709.3479 | Rotating De Sitter Space | An exact solution of the vacuum Einstein equations with a cosmological
constant is exhibited which can perhaps be used to describe the interior of
compact rotating objects. The physical part of this solution has the topology
of a torus, which may shed light on the origin of highly collimated jets from
compact objects... | gr-qc astro-ph | an exact solution of the vacuum einstein equations with a cosmological constant is exhibited which can perhaps be used to describe the interior of compact rotating objects the physical part of this solution has the topology of a torus which may shed light on the origin of highly collimated jets from compact objects | [['an', 'exact', 'solution', 'of', 'the', 'vacuum', 'einstein', 'equations', 'with', 'a', 'cosmological', 'constant', 'is', 'exhibited', 'which', 'can', 'perhaps', 'be', 'used', 'to', 'describe', 'the', 'interior', 'of', 'compact', 'rotating', 'objects', 'the', 'physical', 'part', 'of', 'this', 'solution', 'has', 'the'... | [-0.1499156268436532, 0.08568231606189346, -0.1577790891575926, 0.06280667185431944, -0.15747608177645026, -0.11367921329120982, -0.032237252853107905, 0.32673128293651454, -0.2298203236862736, -0.26998183503746986, 0.14788269802471096, -0.2264914209602998, -0.0740182413807455, 0.21666829941688842, -0.07612890351282538... |
709.348 | Quasi-fractal sets in space | The focus here is on connected fractal sets with topological dimension 1 and
a lot of topological activity, and their connections with analysis.
| math.CA | the focus here is on connected fractal sets with topological dimension 1 and a lot of topological activity and their connections with analysis | [['the', 'focus', 'here', 'is', 'on', 'connected', 'fractal', 'sets', 'with', 'topological', 'dimension', '1', 'and', 'a', 'lot', 'of', 'topological', 'activity', 'and', 'their', 'connections', 'with', 'analysis']] | [-0.1419466431050197, 0.17169268858497558, -0.054881056203790336, 0.02058517992111814, -0.07337457668441145, -0.1356256804024072, 0.06185031253034654, 0.3621303401887417, -0.23547963911424513, -0.2658698931538864, 0.1666830203131489, -0.35501444744675054, -0.24678152840098608, 0.18992757374096825, -0.059827716211261955... |
709.3481 | Energy resolution improvement in room-temperature CZT detectors | We present methods to improve the energy resolution of single-channel,
room-temperature Cadmium-Zinc-Telluride (CZT) detectors. A new preamplifier
design enables the acquisition of the actual transient current from the
crystals and straightforward data analysis methods yield unprecedented energy
resolution for our te... | physics.ins-det | we present methods to improve the energy resolution of singlechannel roomtemperature cadmiumzinctelluride czt detectors a new preamplifier design enables the acquisition of the actual transient current from the crystals and straightforward data analysis methods yield unprecedented energy resolution for our testdetector... | [['we', 'present', 'methods', 'to', 'improve', 'the', 'energy', 'resolution', 'of', 'singlechannel', 'roomtemperature', 'cadmiumzinctelluride', 'czt', 'detectors', 'a', 'new', 'preamplifier', 'design', 'enables', 'the', 'acquisition', 'of', 'the', 'actual', 'transient', 'current', 'from', 'the', 'crystals', 'and', 'str... | [-0.021884898164946782, 0.04660747281266499, -0.03263906319870761, -0.0003805142474256603, -0.010085240170653714, -0.13422233715751453, 0.01682412773125658, 0.4168179916708093, -0.187745838710352, -0.4201434422112805, 0.09463829537853599, -0.3638438676434912, 0.023837615678233927, 0.24479458340946095, -0.05054331818889... |
709.3482 | Effective gluon mass and infrared fixed point in QCD | We report on a special type of solutions for the gluon propagator of pure
QCD, obtained from the corresponding non-linear Schwinger-Dyson equation
formulated in the Feynman gauge of the background field method. These solutions
reach a finite value in the deep infrared and may be fitted using a massive
propagator, wit... | hep-ph | we report on a special type of solutions for the gluon propagator of pure qcd obtained from the corresponding nonlinear schwingerdyson equation formulated in the feynman gauge of the background field method these solutions reach a finite value in the deep infrared and may be fitted using a massive propagator with the c... | [['we', 'report', 'on', 'a', 'special', 'type', 'of', 'solutions', 'for', 'the', 'gluon', 'propagator', 'of', 'pure', 'qcd', 'obtained', 'from', 'the', 'corresponding', 'nonlinear', 'schwingerdyson', 'equation', 'formulated', 'in', 'the', 'feynman', 'gauge', 'of', 'the', 'background', 'field', 'method', 'these', 'solut... | [-0.0874778982407103, 0.17207177772576904, -0.14001543445650627, 0.08920778572231669, -0.05697034908182643, -0.07852501876790215, 0.05515242423775985, 0.2904739974273576, -0.20540996894792274, -0.24182785261180942, 0.05843966535844461, -0.2623315315020995, -0.09376370124863806, 0.14678988349106575, 0.008175097930210607... |
709.3483 | Near-field imaging and frequency tuning of a high-Q photonic crystal
membrane microcavity | We discuss experimental studies of the interaction between a nanoscopic
object and a photonic crystal membrane resonator of quality factor Q=55000. By
controlled actuation of a glass fiber tip in the near-field of a photonic
crystal, we constructed a complete spatio-spectral map of the resonator mode
and its coupling... | cond-mat.other | we discuss experimental studies of the interaction between a nanoscopic object and a photonic crystal membrane resonator of quality factor q55000 by controlled actuation of a glass fiber tip in the nearfield of a photonic crystal we constructed a complete spatiospectral map of the resonator mode and its coupling with t... | [['we', 'discuss', 'experimental', 'studies', 'of', 'the', 'interaction', 'between', 'a', 'nanoscopic', 'object', 'and', 'a', 'photonic', 'crystal', 'membrane', 'resonator', 'of', 'quality', 'factor', 'q55000', 'by', 'controlled', 'actuation', 'of', 'a', 'glass', 'fiber', 'tip', 'in', 'the', 'nearfield', 'of', 'a', 'ph... | [-0.15948158209702293, 0.11583140804922502, -0.10793835272718418, -0.06463883816991654, -0.0749024597829894, -0.17570260038043847, 0.07105112902865042, 0.46544748147655474, -0.20581341752161583, -0.2702762006308165, 0.040271435122887944, -0.2869699020837352, -0.17063283511404798, 0.2846049370342179, -0.0079300820372034... |
709.3484 | Deep MMT Transit Survey of the Open Cluster M37 II: Variable Stars | We have conducted a deep ($15 \la r \la 23$), 20 night survey for transiting
planets in the intermediate age ($\sim 550 {\rm Myr}$) open cluster M37 (NGC
2099) using the Megacam wide-field mosaic CCD camera on the 6.5m Multiple
Mirror Telescope (MMT). In this paper we present a catalog and light curves for
1445 varia... | astro-ph | we have conducted a deep 15 la r la 23 20 night survey for transiting planets in the intermediate age sim 550 rm myr open cluster m37 ngc 2099 using the megacam widefield mosaic ccd camera on the 65m multiple mirror telescope mmt in this paper we present a catalog and light curves for 1445 variable stars 1430 99 of the... | [['we', 'have', 'conducted', 'a', 'deep', '15', 'la', 'r', 'la', '23', '20', 'night', 'survey', 'for', 'transiting', 'planets', 'in', 'the', 'intermediate', 'age', 'sim', '550', 'rm', 'myr', 'open', 'cluster', 'm37', 'ngc', '2099', 'using', 'the', 'megacam', 'widefield', 'mosaic', 'ccd', 'camera', 'on', 'the', '65m', '... | [-0.15329379040880928, 0.19845402766680179, -0.05682484754028597, 0.06648869874368843, -0.13465251474796483, -0.15013360967194395, 0.13441137875862685, 0.3564421375570375, -0.12127475543779188, -0.4163078144281393, 0.06159666747442402, -0.366200722995702, -0.02593351113499098, 0.2371681200451262, -0.0891856940064047, -... |
709.3485 | The Australia Telescope 20 GHz (AT20G) Survey: The Bright Source Sample | The Australia Telescope 20 GHz (AT20G) Survey is a blind survey of the whole
Southern sky at 20 GHz (with follow-up observations at 4.8 and 8.6 GHz) carried
out with the Australia Telescope Compact Array (ATCA) from 2004 to 2007. The
Bright Source Sample (BSS) is a complete flux-limited subsample of the AT20G
Survey ... | astro-ph | the australia telescope 20 ghz at20g survey is a blind survey of the whole southern sky at 20 ghz with followup observations at 48 and 86 ghz carried out with the australia telescope compact array atca from 2004 to 2007 the bright source sample bss is a complete fluxlimited subsample of the at20g survey catalogue compr... | [['the', 'australia', 'telescope', '20', 'ghz', 'at20g', 'survey', 'is', 'a', 'blind', 'survey', 'of', 'the', 'whole', 'southern', 'sky', 'at', '20', 'ghz', 'with', 'followup', 'observations', 'at', '48', 'and', '86', 'ghz', 'carried', 'out', 'with', 'the', 'australia', 'telescope', 'compact', 'array', 'atca', 'from', ... | [-0.0711486677771055, 0.07862836149775122, -0.006982994779936178, 0.0027935241267396205, -0.06402353581712804, -0.07764767114751955, 0.122260073580536, 0.4750967483670838, -0.09832996731279912, -0.4162501175779709, 0.10826466695520928, -0.3606692043718247, 0.03000242653121529, 0.2005987195712741, 0.016946064155812547, ... |
709.3486 | Probing the ground state in gauge theories | We consider two very different models of the flux tube linking two heavy
quarks: a string linking the matter fields and a Coulombic description of two
separately gauge invariant charges. We compare how close they are to the
unknown true ground state in compact U(1) and the SU(2) Higgs model.
Simulations in compact U(... | hep-lat hep-ph hep-th | we consider two very different models of the flux tube linking two heavy quarks a string linking the matter fields and a coulombic description of two separately gauge invariant charges we compare how close they are to the unknown true ground state in compact u1 and the su2 higgs model simulations in compact u1 show tha... | [['we', 'consider', 'two', 'very', 'different', 'models', 'of', 'the', 'flux', 'tube', 'linking', 'two', 'heavy', 'quarks', 'a', 'string', 'linking', 'the', 'matter', 'fields', 'and', 'a', 'coulombic', 'description', 'of', 'two', 'separately', 'gauge', 'invariant', 'charges', 'we', 'compare', 'how', 'close', 'they', 'a... | [-0.14430853320873674, 0.22549519781023264, -0.09150417988046498, 0.15042878306861493, -0.011120458117733567, -0.14819232241834623, -0.0006398811701574694, 0.38020957231332186, -0.15920407256364064, -0.27937504305046496, 0.0165664012962163, -0.2756434105715509, -0.0905756334758411, 0.10999745196441851, -0.0221164318480... |
709.3487 | Complete 1-loop test of AdS/CFT | We analyze nested Bethe ansatz (NBA) and the corresponding finite size
corrections. We find an integral equation which describes these corrections in
a closed form. As an application we considered the conjectured
Beisert-Staudacher (BS) equations with the Hernandez-Lopez dressing factor
where the finite size correcti... | hep-th | we analyze nested bethe ansatz nba and the corresponding finite size corrections we find an integral equation which describes these corrections in a closed form as an application we considered the conjectured beisertstaudacher bs equations with the hernandezlopez dressing factor where the finite size corrections should... | [['we', 'analyze', 'nested', 'bethe', 'ansatz', 'nba', 'and', 'the', 'corresponding', 'finite', 'size', 'corrections', 'we', 'find', 'an', 'integral', 'equation', 'which', 'describes', 'these', 'corrections', 'in', 'a', 'closed', 'form', 'as', 'an', 'application', 'we', 'considered', 'the', 'conjectured', 'beisertstaud... | [-0.14152446151796752, 0.15173049599444352, -0.0786052361184994, 0.11031480415358545, -0.05894776972787786, -0.10887732949576404, 0.030511941572228456, 0.28315841290025623, -0.23545585100773286, -0.23978137500024188, 0.05855070611681972, -0.3067247244169467, -0.08896582155972127, 0.13587119649742885, -0.026481134668449... |
709.3488 | Non-BPS Attractors in 5d and 6d Extended Supergravity | We connect the attractor equations of a certain class of N=2, d=5
supergravities with their (1,0), d=6 counterparts, by relating the moduli space
of non-BPS d=5 black hole/black string attractors to the moduli space of
extremal dyonic black string d=6 non-BPS attractors. For d = 5 real special
symmetric spaces and fo... | hep-th | we connect the attractor equations of a certain class of n2 d5 supergravities with their 10 d6 counterparts by relating the moduli space of nonbps d5 black holeblack string attractors to the moduli space of extremal dyonic black string d6 nonbps attractors for d 5 real special symmetric spaces and for n 468 theories we... | [['we', 'connect', 'the', 'attractor', 'equations', 'of', 'a', 'certain', 'class', 'of', 'n2', 'd5', 'supergravities', 'with', 'their', '10', 'd6', 'counterparts', 'by', 'relating', 'the', 'moduli', 'space', 'of', 'nonbps', 'd5', 'black', 'holeblack', 'string', 'attractors', 'to', 'the', 'moduli', 'space', 'of', 'extre... | [-0.17269616995638767, 0.13413118786203476, 0.037166535550828224, 0.16095863469048968, -0.0315526726938385, -0.17891035647231288, 0.01801345429745587, 0.26769985498062204, -0.13365143752889708, -0.2672903756143309, 0.1308073890873597, -0.3587820564051591, -0.18204461275100975, 0.08540796057994678, -0.0578320799208346, ... |
709.3489 | Homotopy type and v1-periodic homotopy groups of p-compact groups | We determine the v1-periodic homotopy groups of all irreducible p-compact
groups (BX,X). In the most difficult, modular, cases, we follow a direct path
from their associated invariant polynomials to these homotopy groups. We show
that, if p is odd, every irreducible p-compact group has X of the homotopy type
of a pro... | math.AT | we determine the v1periodic homotopy groups of all irreducible pcompact groups bxx in the most difficult modular cases we follow a direct path from their associated invariant polynomials to these homotopy groups we show that if p is odd every irreducible pcompact group has x of the homotopy type of a product of explici... | [['we', 'determine', 'the', 'v1periodic', 'homotopy', 'groups', 'of', 'all', 'irreducible', 'pcompact', 'groups', 'bxx', 'in', 'the', 'most', 'difficult', 'modular', 'cases', 'we', 'follow', 'a', 'direct', 'path', 'from', 'their', 'associated', 'invariant', 'polynomials', 'to', 'these', 'homotopy', 'groups', 'we', 'sho... | [-0.24084757205805388, 0.10319946007000218, -0.13733370149315433, 0.11601324573937996, -0.13366834192279856, -0.11695793861972875, 0.010106281594148484, 0.42763090706912094, -0.34942719266661604, -0.16919867871008043, 0.0833069850542133, -0.22667145439230935, -0.15735440593662448, 0.19411673226618562, -0.14221481542135... |
709.349 | Structure formation and the origin of dark energy | Cosmological constant a.k.a. dark energy problem is considered to be one
major challenge in modern cosmology. Here we present a model where large scale
structure formation causes spatially-flat FRW universe to fragment into
numerous `FRW islands' surrounded by vacuum. We show that this mechanism can
explain the origi... | astro-ph gr-qc hep-th | cosmological constant aka dark energy problem is considered to be one major challenge in modern cosmology here we present a model where large scale structure formation causes spatiallyflat frw universe to fragment into numerous frw islands surrounded by vacuum we show that this mechanism can explain the origin of dark ... | [['cosmological', 'constant', 'aka', 'dark', 'energy', 'problem', 'is', 'considered', 'to', 'be', 'one', 'major', 'challenge', 'in', 'modern', 'cosmology', 'here', 'we', 'present', 'a', 'model', 'where', 'large', 'scale', 'structure', 'formation', 'causes', 'spatiallyflat', 'frw', 'universe', 'to', 'fragment', 'into', ... | [-0.1247852864291738, 0.11755443103374644, -0.12249537307641231, 0.1432505913236288, -0.15194589492645771, -0.12781715623614395, -0.07667945415995941, 0.3456999378269721, -0.23284758900420047, -0.3633092704466453, 0.06544551939027858, -0.17388197217209667, -0.06932256219214668, 0.14874037296520362, -0.04022779437832023... |
709.3491 | Family Unification with SO(10) | Unification based on the group SO(10)^3 \times S_3 is studied. Each family
has its own SO(10) group, and the S_3 permutes the three families and SO(10)
factors. This is the maximal local symmetry for the known fermions. Family
unification is achieved in the sense that all known fermions are in a single
irreducible mu... | hep-ph | unification based on the group so103 times s_3 is studied each family has its own so10 group and the s_3 permutes the three families and so10 factors this is the maximal local symmetry for the known fermions family unification is achieved in the sense that all known fermions are in a single irreducible multiplet of the... | [['unification', 'based', 'on', 'the', 'group', 'so103', 'times', 's_3', 'is', 'studied', 'each', 'family', 'has', 'its', 'own', 'so10', 'group', 'and', 'the', 's_3', 'permutes', 'the', 'three', 'families', 'and', 'so10', 'factors', 'this', 'is', 'the', 'maximal', 'local', 'symmetry', 'for', 'the', 'known', 'fermions',... | [-0.19445752202324113, 0.2796031398679681, 0.0008965140702773114, 0.1306639952722899, -0.12429688904643516, -0.1583124148013184, 0.02508035712229202, 0.3448512286175879, -0.22749665535378213, -0.26865954794065683, 0.07975537383724574, -0.24356197778667724, -0.04984284748266242, 0.05590924952293233, 0.00983535151985683,... |
709.3492 | The Spitzer c2d Survey of Large, Nearby, Interstellar Clouds: VII.
Ophiuchus Observed with MIPS | We present maps of 14.4 deg^2 of the Ophiuchus dark clouds observed by the
Spitzer Space Telescope Multiband Imaging Photometer for Spitzer (MIPS). These
high quality maps depict both numerous point sources as well as extended dust
emission within the star-forming and non-star-forming portions of these clouds.
Using ... | astro-ph | we present maps of 144 deg2 of the ophiuchus dark clouds observed by the spitzer space telescope multiband imaging photometer for spitzer mips these high quality maps depict both numerous point sources as well as extended dust emission within the starforming and nonstarforming portions of these clouds using psffitting ... | [['we', 'present', 'maps', 'of', '144', 'deg2', 'of', 'the', 'ophiuchus', 'dark', 'clouds', 'observed', 'by', 'the', 'spitzer', 'space', 'telescope', 'multiband', 'imaging', 'photometer', 'for', 'spitzer', 'mips', 'these', 'high', 'quality', 'maps', 'depict', 'both', 'numerous', 'point', 'sources', 'as', 'well', 'as', ... | [-0.01799296314063461, 0.08458179859515054, -0.027823170509443364, 0.11632778822218603, -0.05763978319538927, -0.04021954237285889, 0.09393416041557705, 0.4772225068599889, -0.13022520981912472, -0.4257431775895935, 0.060393771873681217, -0.3501322576987811, -0.023644408087641226, 0.15904012992695876, -0.01140498397007... |
709.3493 | Kliem and Toeroek Reply | Reply to Comment on "Torus Instability" by J. Chen, Phys. Rev. Lett. 99,
099501 (2007). Refers to "Torus Instability" by Kliem and Toeroek, Phys. Rev.
Lett. 96, 255002 (2006).
| physics.plasm-ph | reply to comment on torus instability by j chen phys rev lett 99 099501 2007 refers to torus instability by kliem and toeroek phys rev lett 96 255002 2006 | [['reply', 'to', 'comment', 'on', 'torus', 'instability', 'by', 'j', 'chen', 'phys', 'rev', 'lett', '99', '099501', '2007', 'refers', 'to', 'torus', 'instability', 'by', 'kliem', 'and', 'toeroek', 'phys', 'rev', 'lett', '96', '255002', '2006']] | [-0.08828565392091318, 0.03672757510233809, 0.12773559651234084, -0.3690989765735274, -0.188280007319042, -0.09277616427452476, 0.23645593239753335, 0.1970671776820112, 0.1697705454080952, -0.4319456884706462, -0.17819092221799548, -0.26304019803043316, -0.2733556321925587, 0.17772896077345918, -0.4252731041913783, -0.... |
709.3494 | Role of Resonances in Heavy Meson Processes within Standard Model and
Beyond | The effective theory based on combined chiral and heavy quark symmetry, the
heavy meson chiral perturbation theory, is applied to studying the role of
resonances in various processes of heavy mesons within and beyond the Standard
Model. Chiral corrections including both positive and negative parity heavy
meson double... | hep-ph | the effective theory based on combined chiral and heavy quark symmetry the heavy meson chiral perturbation theory is applied to studying the role of resonances in various processes of heavy mesons within and beyond the standard model chiral corrections including both positive and negative parity heavy meson doublets ar... | [['the', 'effective', 'theory', 'based', 'on', 'combined', 'chiral', 'and', 'heavy', 'quark', 'symmetry', 'the', 'heavy', 'meson', 'chiral', 'perturbation', 'theory', 'is', 'applied', 'to', 'studying', 'the', 'role', 'of', 'resonances', 'in', 'various', 'processes', 'of', 'heavy', 'mesons', 'within', 'and', 'beyond', '... | [-0.07106690633887418, 0.26138633033386094, -0.04837325119998733, 0.1539825603500259, -0.0601764518681089, -0.15220430349607184, 0.07002769265999823, 0.28051380446482554, -0.19689110000001214, -0.219167963513302, -0.042148653504792084, -0.36542343999822385, -0.0405173318188181, 0.09662040376211167, 0.11636289833893487,... |
709.3495 | Anomalous Relativistic Tunneling and Exotic Point Interactions | We examine one-dimensional quantum scattering of a Dirac particle off
relativistic potential barriers. With proper considerations of Dirac sea,
existence of anomalous tunneling at zero incident-energy is revealed for a
particular type of relativistic potential having same magnitudes and opposite
signs for scalar and ... | quant-ph hep-ph nucl-th | we examine onedimensional quantum scattering of a dirac particle off relativistic potential barriers with proper considerations of dirac sea existence of anomalous tunneling at zero incidentenergy is revealed for a particular type of relativistic potential having same magnitudes and opposite signs for scalar and vector... | [['we', 'examine', 'onedimensional', 'quantum', 'scattering', 'of', 'a', 'dirac', 'particle', 'off', 'relativistic', 'potential', 'barriers', 'with', 'proper', 'considerations', 'of', 'dirac', 'sea', 'existence', 'of', 'anomalous', 'tunneling', 'at', 'zero', 'incidentenergy', 'is', 'revealed', 'for', 'a', 'particular',... | [-0.1595691256056119, 0.21643131833374238, -0.11083373417627186, 0.09469578337983318, -0.06632304189336155, -0.1798734569080895, 0.032208194586283136, 0.3585592587628672, -0.21647467366569945, -0.2500930477174059, -0.01660482472957923, -0.3131614505733934, -0.11274557556175897, 0.1826801763100159, 0.03639141555064388, ... |
709.3496 | On the spectrum of infinite dimensional random products of compact
operators | We consider an infinite dimensional separable Hilbert space and its family of
compact integrable cocycles over a dynamical system f. Assuming that f acts in
a compact Hausdorff space X and preserves a Borel regular ergodic measure which
is positive on non-empty open sets, we conclude that there is a residual subset
o... | math.DS math.SP | we consider an infinite dimensional separable hilbert space and its family of compact integrable cocycles over a dynamical system f assuming that f acts in a compact hausdorff space x and preserves a borel regular ergodic measure which is positive on nonempty open sets we conclude that there is a residual subset of coc... | [['we', 'consider', 'an', 'infinite', 'dimensional', 'separable', 'hilbert', 'space', 'and', 'its', 'family', 'of', 'compact', 'integrable', 'cocycles', 'over', 'a', 'dynamical', 'system', 'f', 'assuming', 'that', 'f', 'acts', 'in', 'a', 'compact', 'hausdorff', 'space', 'x', 'and', 'preserves', 'a', 'borel', 'regular',... | [-0.24438435945659875, 0.1410693886707304, -0.10334010037283102, 0.043534231010514, -0.03526320959130923, -0.13512110102456062, 0.0511686560511589, 0.39775221904118857, -0.3166145432988803, -0.06519875888402263, 0.1343731854033346, -0.29143484388788543, -0.0925733302688847, 0.22789186102648576, -0.10538399135383467, -0... |
709.3497 | Gauge-gravity duality -- Super Yang Mills Quantum Mechanics | We describe the conjectured holographic duality between Yang-Mills quantum
mechanics and type IIa string theory. This duality allows us to use lattice
Monte Carlo simulations to probe the physics of the gravitational theory - for
example, at low energies it provides a computation of black hole entropy in
terms of a s... | hep-lat hep-th | we describe the conjectured holographic duality between yangmills quantum mechanics and type iia string theory this duality allows us to use lattice monte carlo simulations to probe the physics of the gravitational theory for example at low energies it provides a computation of black hole entropy in terms of a sum over... | [['we', 'describe', 'the', 'conjectured', 'holographic', 'duality', 'between', 'yangmills', 'quantum', 'mechanics', 'and', 'type', 'iia', 'string', 'theory', 'this', 'duality', 'allows', 'us', 'to', 'use', 'lattice', 'monte', 'carlo', 'simulations', 'to', 'probe', 'the', 'physics', 'of', 'the', 'gravitational', 'theory... | [-0.08458132294139692, 0.15867209636074092, -0.14073052377040898, 0.13399104323470964, -0.04156367325423552, -0.14519489967663374, 0.04607628242312265, 0.2736462882054704, -0.20455638913304677, -0.2878353019910199, 0.0254533299960063, -0.30149752394250495, -0.14005223207974007, 0.16486147429594503, -0.01655893757498623... |
709.3498 | The conductivity measure for the Anderson model | We study the ac-conductivity in linear response theory for the Anderson
tight-binding model. We define the electrical ac-conductivity and calculate the
linear-response current at zero temperature for arbitrary Fermi energy. In
particular, the Fermi energy may lie in a spectral region where extended states
are believe... | math-ph math.MP | we study the acconductivity in linear response theory for the anderson tightbinding model we define the electrical acconductivity and calculate the linearresponse current at zero temperature for arbitrary fermi energy in particular the fermi energy may lie in a spectral region where extended states are believed to exis... | [['we', 'study', 'the', 'acconductivity', 'in', 'linear', 'response', 'theory', 'for', 'the', 'anderson', 'tightbinding', 'model', 'we', 'define', 'the', 'electrical', 'acconductivity', 'and', 'calculate', 'the', 'linearresponse', 'current', 'at', 'zero', 'temperature', 'for', 'arbitrary', 'fermi', 'energy', 'in', 'par... | [-0.15075965104430603, 0.17630476205764958, -0.05640538643153074, 0.13639286210915694, -0.013427875111422813, -0.15282637236911492, 0.06397409093672952, 0.3426358499176179, -0.24476517678704113, -0.2470436665074279, 0.012403766394224173, -0.30049381804807734, -0.11529135264572687, 0.16077551656538466, 0.022641505536133... |
709.3499 | Noncommutative Field Theory from Quantum Mechanical Space-Space
Noncommutativity | We investigate the incorporation of space noncommutativity into field theory
by extending to the spectral continuum the minisuperspace action of the quantum
mechanical harmonic oscillator propagator with an enlarged Heisenberg algebra.
In addition to the usual $\star$-product deformation of the algebra of field
funct... | hep-th | we investigate the incorporation of space noncommutativity into field theory by extending to the spectral continuum the minisuperspace action of the quantum mechanical harmonic oscillator propagator with an enlarged heisenberg algebra in addition to the usual starproduct deformation of the algebra of field functions we... | [['we', 'investigate', 'the', 'incorporation', 'of', 'space', 'noncommutativity', 'into', 'field', 'theory', 'by', 'extending', 'to', 'the', 'spectral', 'continuum', 'the', 'minisuperspace', 'action', 'of', 'the', 'quantum', 'mechanical', 'harmonic', 'oscillator', 'propagator', 'with', 'an', 'enlarged', 'heisenberg', '... | [-0.1621455738126342, 0.17978962791111466, -0.08395197026348158, 0.05902690640581188, -0.08832604296283046, -0.07980215454946703, -0.05656334569455305, 0.3550528942315436, -0.2774332882419451, -0.23086282150792098, 0.015724313506203246, -0.18087339775685443, -0.15144614669591633, 0.14199034696611673, -0.071076974328329... |
709.35 | Bowen blend echo-tomography of low mass X-ray binaries | We present simultaneous high time resolution (1-10 Hz) X-ray and optical
observations of the persistent LMXBs Sco X-1 and V801 Ara(=4U 1636-536). In the
case of Sco X-1 we find that the Bowen/HeII emission lags the X-ray
light-curves with a light travel time of ~11-16s which is consistent with
reprocessing in the don... | astro-ph | we present simultaneous high time resolution 110 hz xray and optical observations of the persistent lmxbs sco x1 and v801 ara4u 1636536 in the case of sco x1 we find that the bowenheii emission lags the xray lightcurves with a light travel time of 1116s which is consistent with reprocessing in the donor star we also pr... | [['we', 'present', 'simultaneous', 'high', 'time', 'resolution', '110', 'hz', 'xray', 'and', 'optical', 'observations', 'of', 'the', 'persistent', 'lmxbs', 'sco', 'x1', 'and', 'v801', 'ara4u', '1636536', 'in', 'the', 'case', 'of', 'sco', 'x1', 'we', 'find', 'that', 'the', 'bowenheii', 'emission', 'lags', 'the', 'xray',... | [-0.07744215975368493, 0.10440450782740587, -0.07638840994944698, 0.08437726051963278, -0.09179462770882406, -0.09224036527356427, 0.10376824135861458, 0.4868426784480873, -0.17736859435803795, -0.30690017052386936, 0.13428282431375824, -0.3362229216059572, -0.073057430179324, 0.23479101212303105, -0.05564477958863503,... |
709.3501 | Perturbative finiteness of the three-dimensional Susy QED to all orders | Within the superfield formalism, we study the ultraviolet properties of the
three-dimensional supersymmetric quantum electrodynamics. The theory is shown
to be finite at all loops orders in a particular gauge.
| hep-th | within the superfield formalism we study the ultraviolet properties of the threedimensional supersymmetric quantum electrodynamics the theory is shown to be finite at all loops orders in a particular gauge | [['within', 'the', 'superfield', 'formalism', 'we', 'study', 'the', 'ultraviolet', 'properties', 'of', 'the', 'threedimensional', 'supersymmetric', 'quantum', 'electrodynamics', 'the', 'theory', 'is', 'shown', 'to', 'be', 'finite', 'at', 'all', 'loops', 'orders', 'in', 'a', 'particular', 'gauge']] | [-0.09732123049519335, 0.22874398898954193, -0.06533803469501435, 0.0897765762056224, -0.02500408625540634, -0.0646267904434353, -0.05234623212600127, 0.3623067882532875, -0.17599234767258168, -0.23087643936742097, 0.025607706082519145, -0.2850048577412963, -0.18682540679971377, 0.1292347953033944, -0.00504358455073088... |
709.3502 | Electronic Structure of Single-Walled Carbon Nanotubes Governed by
Odd-Electrons Interaction | For the first time, an approach is suggested for the quantitative description
of the electronic structure of single-walled carbon nanotubes and the
prediction of active sites for the tube controlled functionalization in view of
the tube length and ends structure. The approach is based on the tube
characteristic featu... | cond-mat.mtrl-sci cond-mat.supr-con | for the first time an approach is suggested for the quantitative description of the electronic structure of singlewalled carbon nanotubes and the prediction of active sites for the tube controlled functionalization in view of the tube length and ends structure the approach is based on the tube characteristic feature co... | [['for', 'the', 'first', 'time', 'an', 'approach', 'is', 'suggested', 'for', 'the', 'quantitative', 'description', 'of', 'the', 'electronic', 'structure', 'of', 'singlewalled', 'carbon', 'nanotubes', 'and', 'the', 'prediction', 'of', 'active', 'sites', 'for', 'the', 'tube', 'controlled', 'functionalization', 'in', 'vie... | [-0.12580143202974545, 0.135129703861984, -0.004738317327422461, 0.04366351654838271, 0.029295556534960018, -0.1389408005378777, 0.04136420677915761, 0.45687147993140104, -0.225436504952973, -0.2795047684746787, 0.06260974418345415, -0.26514642659907905, -0.09295913120315266, 0.17475326958763587, 0.027504283253376078, ... |
709.3503 | Black Hole Production from High Energy Scattering in AdS/CFT | In this article we show how to set up initial states in ${\cal N} =4$ SYM
theory that correspond to high energy graviton collisions, leading to black
hole formation in $AdS_5\times S^5$. For this purpose, we study states in the
gauge theory that are dual to graviton wavepackets localized at the center of
$AdS_5$, and... | hep-th | in this article we show how to set up initial states in cal n 4 sym theory that correspond to high energy graviton collisions leading to black hole formation in ads_5times s5 for this purpose we study states in the gauge theory that are dual to graviton wavepackets localized at the center of ads_5 and carrying large an... | [['in', 'this', 'article', 'we', 'show', 'how', 'to', 'set', 'up', 'initial', 'states', 'in', 'cal', 'n', '4', 'sym', 'theory', 'that', 'correspond', 'to', 'high', 'energy', 'graviton', 'collisions', 'leading', 'to', 'black', 'hole', 'formation', 'in', 'ads_5times', 's5', 'for', 'this', 'purpose', 'we', 'study', 'state... | [-0.13507561095053655, 0.198596785896021, -0.09040950493239877, 0.10725490204295364, -0.06961027299722204, -0.1211385165293843, -0.024278293540674963, 0.3314157875496789, -0.22180546030907308, -0.24393604004934513, 0.06065189086642685, -0.303717461435682, -0.11108228134380727, 0.11218808377378668, 0.0038433313155336315... |
709.3504 | Forty-Four Pass Fibre Optic Loop for Improving the Sensitivity of
Surface Plasmon Resonance Sensors | A forty-four pass fibre optic surface plasmon resonance sensor that enhances
detection sensitivity according to the number of passes is demonstrated for the
first time. The technique employs a fibre optic recirculation loop that passes
the detection spot forty- four times, thus enhancing sensitivity by a factor of
fo... | physics.gen-ph | a fortyfour pass fibre optic surface plasmon resonance sensor that enhances detection sensitivity according to the number of passes is demonstrated for the first time the technique employs a fibre optic recirculation loop that passes the detection spot forty four times thus enhancing sensitivity by a factor of fortyfou... | [['a', 'fortyfour', 'pass', 'fibre', 'optic', 'surface', 'plasmon', 'resonance', 'sensor', 'that', 'enhances', 'detection', 'sensitivity', 'according', 'to', 'the', 'number', 'of', 'passes', 'is', 'demonstrated', 'for', 'the', 'first', 'time', 'the', 'technique', 'employs', 'a', 'fibre', 'optic', 'recirculation', 'loop... | [-0.1501257105316553, 0.16176292434748676, -0.05818348678035869, -0.057812381068813715, -0.06030755301213099, -0.13235066005856627, 0.08003760782950041, 0.3561049642248286, -0.21768793642727866, -0.320590159493602, 0.08230974280870416, -0.27795775977687703, -0.1288703475173356, 0.2612323048731519, -0.06043292449580299,... |
709.3505 | The Outer Disks of Early-Type Galaxies. I. Surface-Brightness Profiles
of Barred Galaxies | We present a study of 66 barred, early-type (S0-Sb) disk galaxies, focused on
the disk surface brightness profile outside the bar region and the nature of
Freeman Type I and II profiles, their origins, and their possible relation to
disk truncations. This paper discusses the data and their reduction, outlines
our cla... | astro-ph | we present a study of 66 barred earlytype s0sb disk galaxies focused on the disk surface brightness profile outside the bar region and the nature of freeman type i and ii profiles their origins and their possible relation to disk truncations this paper discusses the data and their reduction outlines our classification ... | [['we', 'present', 'a', 'study', 'of', '66', 'barred', 'earlytype', 's0sb', 'disk', 'galaxies', 'focused', 'on', 'the', 'disk', 'surface', 'brightness', 'profile', 'outside', 'the', 'bar', 'region', 'and', 'the', 'nature', 'of', 'freeman', 'type', 'i', 'and', 'ii', 'profiles', 'their', 'origins', 'and', 'their', 'possi... | [-0.05247053026582664, 0.024509290023874357, -0.03762892144229665, 0.08419897184429168, -0.07248386346212447, -0.08943040919717964, 0.0628310052368944, 0.3911285249687222, -0.18918429631212216, -0.3640274655470866, 0.11060053463289288, -0.3119742751311324, -0.056491389040661, 0.18508347410544512, -0.04434989200871046, ... |
709.3506 | Distinguished tame supercuspidal representations | This paper studies the behavior of Jiu-Kang Yu's tame supercuspidal
representations relative to involutions of reductive p-adic groups. Symmetric
space methods are used to illuminate various aspects of Yu's construction.
Necessary conditions for a tame supercuspidal representation of G to be
distinguished by (the fix... | math.RT math.GR | this paper studies the behavior of jiukang yus tame supercuspidal representations relative to involutions of reductive padic groups symmetric space methods are used to illuminate various aspects of yus construction necessary conditions for a tame supercuspidal representation of g to be distinguished by the fixed points... | [['this', 'paper', 'studies', 'the', 'behavior', 'of', 'jiukang', 'yus', 'tame', 'supercuspidal', 'representations', 'relative', 'to', 'involutions', 'of', 'reductive', 'padic', 'groups', 'symmetric', 'space', 'methods', 'are', 'used', 'to', 'illuminate', 'various', 'aspects', 'of', 'yus', 'construction', 'necessary', ... | [-0.20785922039630672, 0.08489292167606406, -0.1521785154322823, 0.0710369050277457, -0.1558102037599911, -0.12478848684188579, -0.02128911926317209, 0.32608336117118597, -0.35052734757623366, -0.22366127074365655, 0.06897538186017153, -0.1832416510254505, -0.1600109621536948, 0.22159836347395134, -0.16831189788307152,... |
709.3507 | OZI violating eight-quark interactions as a thermometer for chiral
transitions | This work is a follow-up of our recent observation that in the SU(3) flavor
limit with vanishing current quark masses the temperature for the chiral
transition is substantially reduced by adding eight-quark interactions to the
Nambu - Jona-Lasinio Lagrangian with U_A(1) breaking. Here we generalize the
case to realis... | hep-ph | this work is a followup of our recent observation that in the su3 flavor limit with vanishing current quark masses the temperature for the chiral transition is substantially reduced by adding eightquark interactions to the nambu jonalasinio lagrangian with u_a1 breaking here we generalize the case to realistic light an... | [['this', 'work', 'is', 'a', 'followup', 'of', 'our', 'recent', 'observation', 'that', 'in', 'the', 'su3', 'flavor', 'limit', 'with', 'vanishing', 'current', 'quark', 'masses', 'the', 'temperature', 'for', 'the', 'chiral', 'transition', 'is', 'substantially', 'reduced', 'by', 'adding', 'eightquark', 'interactions', 'to... | [-0.1352141205213904, 0.28120685458528777, -0.053788431522984716, 0.08362395258248603, -0.08328200946749759, -0.13619351337077998, 0.10481021168168574, 0.3195045752781293, -0.15998243625020428, -0.2558748766539558, 0.04309469479654405, -0.30287062468743253, -0.07120611229648573, 0.06064962616918849, 0.05290810288786287... |
709.3508 | Fictitious Cavity Approach to the Casimir Effect | We obtain expressions for the Casimir energy and force following an approach
which may be applied to cavities made up of arbitrary materials. In the case of
planar cavities we obtain the well known Lifshitz formula. The approach is
easily generalizable to other geometries.
| quant-ph | we obtain expressions for the casimir energy and force following an approach which may be applied to cavities made up of arbitrary materials in the case of planar cavities we obtain the well known lifshitz formula the approach is easily generalizable to other geometries | [['we', 'obtain', 'expressions', 'for', 'the', 'casimir', 'energy', 'and', 'force', 'following', 'an', 'approach', 'which', 'may', 'be', 'applied', 'to', 'cavities', 'made', 'up', 'of', 'arbitrary', 'materials', 'in', 'the', 'case', 'of', 'planar', 'cavities', 'we', 'obtain', 'the', 'well', 'known', 'lifshitz', 'formul... | [-0.0952743120406839, 0.08824990274131944, -0.08813574102664874, 0.05167879226924428, -0.0689737937963483, -0.19893643624064597, -0.009841225109994411, 0.4161952755159952, -0.21263416678729383, -0.32771095392209565, 0.04540048352051103, -0.2420561650598591, -0.1572553340493786, 0.3001187663440677, -0.02425748977640813,... |
709.3509 | Spherical characters: the supercuspidal case | We exhibit a basis for the space of spherical characters of a distinguished
supercuspidal representation $\pi$ of a connected reductive $p$-adic group,
subject to the assumption that $\pi$ is obtained via induction from a
representation of an open compact mod centre subgroup. We derive an integral
formula for each sp... | math.RT math.GR | we exhibit a basis for the space of spherical characters of a distinguished supercuspidal representation pi of a connected reductive padic group subject to the assumption that pi is obtained via induction from a representation of an open compact mod centre subgroup we derive an integral formula for each spherical chara... | [['we', 'exhibit', 'a', 'basis', 'for', 'the', 'space', 'of', 'spherical', 'characters', 'of', 'a', 'distinguished', 'supercuspidal', 'representation', 'pi', 'of', 'a', 'connected', 'reductive', 'padic', 'group', 'subject', 'to', 'the', 'assumption', 'that', 'pi', 'is', 'obtained', 'via', 'induction', 'from', 'a', 'rep... | [-0.19523591032624243, 0.07374761210766155, -0.1672870883643627, 0.04230948980897665, -0.13689492821320892, -0.12217558534443379, 0.029101781811565162, 0.32866541228815915, -0.31159005417488517, -0.17732891650497914, 0.06441538143809884, -0.19266646526008843, -0.155636875865981, 0.23649758175574243, -0.0737358409631997... |
709.351 | Non-linear Preheating with Scalar Metric Perturbations | We have studied preheating of field perturbations in a 3-dimensional lattice
including the effect of scalar metric perturbations, in two generic models of
inflation: chaotic inflation with a quartic potential, and standard hybrid
inflation. We have prepared the initial state for the classical evolution of
the system ... | astro-ph hep-ph | we have studied preheating of field perturbations in a 3dimensional lattice including the effect of scalar metric perturbations in two generic models of inflation chaotic inflation with a quartic potential and standard hybrid inflation we have prepared the initial state for the classical evolution of the system with va... | [['we', 'have', 'studied', 'preheating', 'of', 'field', 'perturbations', 'in', 'a', '3dimensional', 'lattice', 'including', 'the', 'effect', 'of', 'scalar', 'metric', 'perturbations', 'in', 'two', 'generic', 'models', 'of', 'inflation', 'chaotic', 'inflation', 'with', 'a', 'quartic', 'potential', 'and', 'standard', 'hy... | [-0.1920136665062946, 0.2247890555451365, -0.07637153595090794, 0.07335889270390003, -0.08816407285300056, -0.10607779356127484, -0.09036391894140187, 0.2995124641783844, -0.2535240440656977, -0.2779271748997051, 0.10470905662004522, -0.2595487262012806, -0.14438611512573865, 0.13769209232269483, 0.032461490034340665, ... |
709.3511 | The effect of galaxy mass ratio on merger--driven starbursts | We employ numerical simulations of galaxy mergers to explore the effect of
galaxy mass ratio on merger--driven starbursts. Our numerical simulations
include radiative cooling of gas, star formation, and stellar feedback to
follow the interaction and merger of four disk galaxies. The galaxy models span
a factor of 23 ... | astro-ph | we employ numerical simulations of galaxy mergers to explore the effect of galaxy mass ratio on mergerdriven starbursts our numerical simulations include radiative cooling of gas star formation and stellar feedback to follow the interaction and merger of four disk galaxies the galaxy models span a factor of 23 in total... | [['we', 'employ', 'numerical', 'simulations', 'of', 'galaxy', 'mergers', 'to', 'explore', 'the', 'effect', 'of', 'galaxy', 'mass', 'ratio', 'on', 'mergerdriven', 'starbursts', 'our', 'numerical', 'simulations', 'include', 'radiative', 'cooling', 'of', 'gas', 'star', 'formation', 'and', 'stellar', 'feedback', 'to', 'fol... | [-0.09340637954661779, 0.10918891064847656, -0.038470301401092616, 0.13279263204554986, -0.10517438073061505, -0.016630697686357044, 0.00977528244421809, 0.40627657528142486, -0.12576829703098197, -0.34072369129388735, 0.02370695158039772, -0.2557083349282167, -0.0411896874769632, 0.2102248482138281, -0.008501088741210... |
709.3512 | A Bayesian Approach to Network Modularity | We present an efficient, principled, and interpretable technique for
inferring module assignments and for identifying the optimal number of modules
in a given network. We show how several existing methods for finding modules
can be described as variant, special, or limiting cases of our work, and how
the method overc... | physics.data-an cond-mat.stat-mech stat.ML | we present an efficient principled and interpretable technique for inferring module assignments and for identifying the optimal number of modules in a given network we show how several existing methods for finding modules can be described as variant special or limiting cases of our work and how the method overcomes the... | [['we', 'present', 'an', 'efficient', 'principled', 'and', 'interpretable', 'technique', 'for', 'inferring', 'module', 'assignments', 'and', 'for', 'identifying', 'the', 'optimal', 'number', 'of', 'modules', 'in', 'a', 'given', 'network', 'we', 'show', 'how', 'several', 'existing', 'methods', 'for', 'finding', 'modules... | [-0.021029898173375323, -0.025414806637724854, -0.07624107168105963, 0.08705356282319242, -0.08902790774092344, -0.16498745150082478, 0.047832180203321126, 0.42602642924300327, -0.2718328802480495, -0.34683996698835734, 0.11552127686237716, -0.1842111112596935, -0.21902175774240668, 0.258809891949308, -0.07694787301339... |
709.3513 | Loop induced interference effects in Higgs Boson plus two jet production
at the LHC | We calculate the order O(alpha^2 alpha_s^3) interference effect between the
gluon fusion and weak boson fusion processes allowed at the one-loop level in
Higgs boson plus 2 jet production at the LHC. The corresponding one-loop
amplitudes, which have not been considered in the literature so far, are
evaluated analytic... | hep-ph | we calculate the order oalpha2 alpha_s3 interference effect between the gluon fusion and weak boson fusion processes allowed at the oneloop level in higgs boson plus 2 jet production at the lhc the corresponding oneloop amplitudes which have not been considered in the literature so far are evaluated analytically using ... | [['we', 'calculate', 'the', 'order', 'oalpha2', 'alpha_s3', 'interference', 'effect', 'between', 'the', 'gluon', 'fusion', 'and', 'weak', 'boson', 'fusion', 'processes', 'allowed', 'at', 'the', 'oneloop', 'level', 'in', 'higgs', 'boson', 'plus', '2', 'jet', 'production', 'at', 'the', 'lhc', 'the', 'corresponding', 'one... | [-0.07772443836543665, 0.2016597916245887, -0.0712347072885787, 0.1946175124563546, -0.044654874327446685, -0.1252432249553771, 0.022760335600048483, 0.3845551821391985, -0.1944764689093523, -0.2353785408728094, 0.023151302885499794, -0.2884454002017604, -0.08299284587692783, 0.12790547273155436, 0.07822279322398715, 0... |
709.3514 | Self-assembly of polymers or copolymers and ferrofluids leading to
either 1-d, 2-d or 3-d aggregates decorated with magnetic nanoparticles | A novel type of hybrid colloids is presented, based on the association of
several polymeric systems and ferrofluids. On the one hand, we use inorganic
nanoparticles made of magnetic iron oxide prepared at the LI2C, which response
to a magnetic field of low intensity. On the other hand the organic part is
made either ... | cond-mat.soft | a novel type of hybrid colloids is presented based on the association of several polymeric systems and ferrofluids on the one hand we use inorganic nanoparticles made of magnetic iron oxide prepared at the li2c which response to a magnetic field of low intensity on the other hand the organic part is made either of long... | [['a', 'novel', 'type', 'of', 'hybrid', 'colloids', 'is', 'presented', 'based', 'on', 'the', 'association', 'of', 'several', 'polymeric', 'systems', 'and', 'ferrofluids', 'on', 'the', 'one', 'hand', 'we', 'use', 'inorganic', 'nanoparticles', 'made', 'of', 'magnetic', 'iron', 'oxide', 'prepared', 'at', 'the', 'li2c', 'w... | [-0.13897958007951577, 0.18006083340694506, -0.04768024358277519, -0.041974518866821506, -0.01978044394714137, -0.19080440914879243, -0.018441442344337703, 0.424349835117658, -0.2369748273740212, -0.23802320079257092, 0.08373086052636305, -0.2837280650436878, -0.13949363331310452, 0.14894940667785705, 0.049762790724635... |
709.3515 | Uma forma bidimensional que maximiza a resist\^encia aerodin\^amica
newtoniana | (English)
In a previous work [Nonlinearity, 20:2271-2287, 2007; arXiv:math/0703895] it
is investigated, by means of computational simulations, shapes of nonconvex
bodies that maximize resistance to its motion on a rarefied medium, considering
that bodies are moving forward and at the same time slowly rotating. Here... | math-ph math.MP math.OC | english in a previous work nonlinearity 2022712287 2007 arxivmath0703895 it is investigated by means of computational simulations shapes of nonconvex bodies that maximize resistance to its motion on a rarefied medium considering that bodies are moving forward and at the same time slowly rotating here the previous resul... | [['english', 'in', 'a', 'previous', 'work', 'nonlinearity', '2022712287', '2007', 'arxivmath0703895', 'it', 'is', 'investigated', 'by', 'means', 'of', 'computational', 'simulations', 'shapes', 'of', 'nonconvex', 'bodies', 'that', 'maximize', 'resistance', 'to', 'its', 'motion', 'on', 'a', 'rarefied', 'medium', 'conside... | [-0.15774850422840517, -0.01616392190978209, -0.1375268164660726, 0.0294110195810295, -0.10501744640025018, -0.18904150255483143, -0.08327137561686121, 0.2881613200002197, -0.13210129186358135, -0.26668354132170996, 0.031047708091652717, -0.3508095551184865, -0.168709252365003, 0.13411669226870662, -0.26172539578931436... |
709.3516 | Optical Integral in the Cuprates and the Question of Sum Rule Violation | Much attention has been given to a possible violation of the optical sum rule
in the cuprates, and the connection this might have to kinetic energy lowering.
The optical integral is composed of a cut-off independent term (whose
temperature dependence is a measure of the sum rule violation), plus a cut-off
dependent t... | cond-mat.supr-con cond-mat.str-el | much attention has been given to a possible violation of the optical sum rule in the cuprates and the connection this might have to kinetic energy lowering the optical integral is composed of a cutoff independent term whose temperature dependence is a measure of the sum rule violation plus a cutoff dependent term that ... | [['much', 'attention', 'has', 'been', 'given', 'to', 'a', 'possible', 'violation', 'of', 'the', 'optical', 'sum', 'rule', 'in', 'the', 'cuprates', 'and', 'the', 'connection', 'this', 'might', 'have', 'to', 'kinetic', 'energy', 'lowering', 'the', 'optical', 'integral', 'is', 'composed', 'of', 'a', 'cutoff', 'independent... | [-0.14003456281498075, 0.17481492763273074, -0.10743931707822614, 0.09405733926601156, -0.1073169748954199, -0.11886032223011608, 0.09366283309818418, 0.3092376773297373, -0.259394018807345, -0.2910083830356598, 0.06309659213810745, -0.2967810095322353, -0.07683980599632141, 0.13168057299874447, 0.02225942278660282, -0... |
709.3517 | Generation of Fourier transform limited heralded single photons | In this paper we study the spectral (temporal) properties of heralded single
photon wavepackets, triggered by the detection of an idler photon in the
process of parametric downconversion. The generated single photons are studied
within the framework of the chronocyclic Wigner function, from which the single
photon sp... | quant-ph | in this paper we study the spectral temporal properties of heralded single photon wavepackets triggered by the detection of an idler photon in the process of parametric downconversion the generated single photons are studied within the framework of the chronocyclic wigner function from which the single photon spectral ... | [['in', 'this', 'paper', 'we', 'study', 'the', 'spectral', 'temporal', 'properties', 'of', 'heralded', 'single', 'photon', 'wavepackets', 'triggered', 'by', 'the', 'detection', 'of', 'an', 'idler', 'photon', 'in', 'the', 'process', 'of', 'parametric', 'downconversion', 'the', 'generated', 'single', 'photons', 'are', 's... | [-0.08856500246648602, 0.1733299673101463, -0.07545140523265685, 0.03138707441531044, -0.016872205449045694, -0.14098939670052016, 0.07032980435255883, 0.4798671294959773, -0.2640101900839337, -0.28262047415220104, 0.007892756464281243, -0.22499675880623074, -0.031863803497260125, 0.2156656994958268, -0.032386240856392... |
709.3518 | Magnetism of NiMn2O4-Fe3O4 Spinel Interfaces | We investigate the magnetic properties of the isostructural spinel-spinel
interface of NiMn2O4(NMO)-Fe3O4. Although the magnetic transition temperature
of the NMO film is preserved, both bulk and interface sensitive measurements
demonstrate that the interface exhibits strong interfacial magnetic coupling up
to room t... | cond-mat.str-el cond-mat.mtrl-sci | we investigate the magnetic properties of the isostructural spinelspinel interface of nimn2o4nmofe3o4 although the magnetic transition temperature of the nmo film is preserved both bulk and interface sensitive measurements demonstrate that the interface exhibits strong interfacial magnetic coupling up to room temperatu... | [['we', 'investigate', 'the', 'magnetic', 'properties', 'of', 'the', 'isostructural', 'spinelspinel', 'interface', 'of', 'nimn2o4nmofe3o4', 'although', 'the', 'magnetic', 'transition', 'temperature', 'of', 'the', 'nmo', 'film', 'is', 'preserved', 'both', 'bulk', 'and', 'interface', 'sensitive', 'measurements', 'demonst... | [-0.15499950005059046, 0.22639878539220346, -0.021635443903505802, -0.0440986010243333, -0.03250008626756343, -0.13011000693818045, 0.0535762842125471, 0.44799162153239275, -0.2679825066588819, -0.3452718034386635, 0.028497855184303426, -0.34533190416087484, -0.060040925124088644, 0.18253706777679987, 0.112346619692702... |
709.3519 | Designing Gapped Soft Functions for Jet Production | Distributions in jet production often depend on a soft function, S, which
describes hadronic radiation between the jets. Near kinematic thresholds S
encodes nonperturbative information, while far from thresholds S can be
computed with an operator product expansion (OPE). We design soft functions for
jets that serve t... | hep-ph hep-th nucl-th | distributions in jet production often depend on a soft function s which describes hadronic radiation between the jets near kinematic thresholds s encodes nonperturbative information while far from thresholds s can be computed with an operator product expansion ope we design soft functions for jets that serve this dual ... | [['distributions', 'in', 'jet', 'production', 'often', 'depend', 'on', 'a', 'soft', 'function', 's', 'which', 'describes', 'hadronic', 'radiation', 'between', 'the', 'jets', 'near', 'kinematic', 'thresholds', 's', 'encodes', 'nonperturbative', 'information', 'while', 'far', 'from', 'thresholds', 's', 'can', 'be', 'comp... | [-0.10009788545299202, 0.13706359283166802, -0.153795723686175, 0.12424390030454004, -0.07841871432479351, -0.08851484644617284, 0.04993316931650042, 0.3853847845592686, -0.25511992418717955, -0.2749150063722364, 0.048887987887006136, -0.2595922250901499, -0.07609273904273586, 0.11831131073826504, -0.027833668596576898... |
709.352 | Pseudoclassical description of scalar particle in non-Abelian background
and path-integral representations | Path-integral representations for a scalar particle propagator in non-Abelian
external backgrounds are derived. To this aim, we generalize the procedure
proposed by Gitman and Schvartsman 1993 of path-integral construction to any
representation of SU(N) given in terms of antisymmetric generators. And for
arbitrary re... | hep-th | pathintegral representations for a scalar particle propagator in nonabelian external backgrounds are derived to this aim we generalize the procedure proposed by gitman and schvartsman 1993 of pathintegral construction to any representation of sun given in terms of antisymmetric generators and for arbitrary representati... | [['pathintegral', 'representations', 'for', 'a', 'scalar', 'particle', 'propagator', 'in', 'nonabelian', 'external', 'backgrounds', 'are', 'derived', 'to', 'this', 'aim', 'we', 'generalize', 'the', 'procedure', 'proposed', 'by', 'gitman', 'and', 'schvartsman', '1993', 'of', 'pathintegral', 'construction', 'to', 'any', ... | [-0.10086002407513747, 0.203998967879237, -0.11066064382577592, 0.10923608117930901, -0.08856855973690039, -0.10457013163804299, 0.0135709526033939, 0.37261551889103084, -0.17586493369890377, -0.2867339287019734, 0.04594577592936167, -0.20819333880873664, -0.18683196849278397, 0.13797432420930514, -0.08364712877664715,... |
709.3521 | Spin-orbit mediated anisotropic spin interaction in interacting electron
systems | We investigate interactions between spins of strongly correlated electrons
subject to the spin-orbit interaction. Our main finding is that of a novel,
spin-orbit mediated anisotropic spin-spin coupling of the van der Waals type.
Unlike the standard exchange, this interaction does not require the wave
functions to ove... | cond-mat.mes-hall cond-mat.str-el | we investigate interactions between spins of strongly correlated electrons subject to the spinorbit interaction our main finding is that of a novel spinorbit mediated anisotropic spinspin coupling of the van der waals type unlike the standard exchange this interaction does not require the wave functions to overlap we a... | [['we', 'investigate', 'interactions', 'between', 'spins', 'of', 'strongly', 'correlated', 'electrons', 'subject', 'to', 'the', 'spinorbit', 'interaction', 'our', 'main', 'finding', 'is', 'that', 'of', 'a', 'novel', 'spinorbit', 'mediated', 'anisotropic', 'spinspin', 'coupling', 'of', 'the', 'van', 'der', 'waals', 'typ... | [-0.24225592525137296, 0.24126772932618498, 0.026448814234140902, 0.07753271239259875, -0.0764313037773729, -0.14030815535842114, 0.020181792774181587, 0.36799382428492766, -0.28353154266544855, -0.26185349146106157, -0.10023434324532253, -0.3410163365124938, -0.15360304580002754, 0.12958951025124055, 0.114449538413928... |
709.3522 | Topological confinement in bilayer graphene | We study a new type of one-dimensional chiral states that can be created in
bilayer graphene (BLG) by electrostatic lateral confinement. These states
appear on the domain walls separating insulating regions experiencing the
opposite gating polarity. While the states are similar to conventional
solitonic zero-modes, t... | cond-mat.mes-hall | we study a new type of onedimensional chiral states that can be created in bilayer graphene blg by electrostatic lateral confinement these states appear on the domain walls separating insulating regions experiencing the opposite gating polarity while the states are similar to conventional solitonic zeromodes their prop... | [['we', 'study', 'a', 'new', 'type', 'of', 'onedimensional', 'chiral', 'states', 'that', 'can', 'be', 'created', 'in', 'bilayer', 'graphene', 'blg', 'by', 'electrostatic', 'lateral', 'confinement', 'these', 'states', 'appear', 'on', 'the', 'domain', 'walls', 'separating', 'insulating', 'regions', 'experiencing', 'the',... | [-0.19681156225052182, 0.28309049086829463, -0.04947584687353491, 0.048627933022914106, -0.0350136102642864, -0.15974635728583722, 0.05481527047743509, 0.40276991751986546, -0.23480412109939197, -0.2659945680585864, 0.0011886224332316728, -0.2655828791967296, -0.18040493407010377, 0.08591890063106113, -0.02440153793329... |
709.3523 | Adaptive Optics Imaging of Lyman Break Galaxies as Progenitors of
Spheroids in the Local Universe | In order to reveal the stellar mass distribution of z~3 galaxies, we are
conducting deep imaging observations of U-dropout Lyman Break Galaxies (LBGs)
with Adaptive Optics (AO) systems in K-band, which corresponds to rest-frame
V-band of z~3 galaxies. The results of the Subaru intensive-program
observations with AO36... | astro-ph | in order to reveal the stellar mass distribution of z3 galaxies we are conducting deep imaging observations of udropout lyman break galaxies lbgs with adaptive optics ao systems in kband which corresponds to restframe vband of z3 galaxies the results of the subaru intensiveprogram observations with ao36ngsircs indicate... | [['in', 'order', 'to', 'reveal', 'the', 'stellar', 'mass', 'distribution', 'of', 'z3', 'galaxies', 'we', 'are', 'conducting', 'deep', 'imaging', 'observations', 'of', 'udropout', 'lyman', 'break', 'galaxies', 'lbgs', 'with', 'adaptive', 'optics', 'ao', 'systems', 'in', 'kband', 'which', 'corresponds', 'to', 'restframe'... | [-0.009004932702313992, 0.07349425105014874, -0.06266839496803077, 0.13346631955003962, -0.07834391994108944, -0.07231433410783233, -0.011489288172678752, 0.5164868978537479, -0.02090822569088741, -0.36979659939837883, 0.009385549419401389, -0.3412401651459857, -0.03372453325761207, 0.13708928663119488, -0.032232070036... |
709.3524 | Estimates on Monge-Amp\`ere operators derived from a local algebra
inequality | The goal of this short note is to relate the integrability property of the
exponential $e^{-2\phi}$ of a plurisubharmonic function $\phi$ with isolated or
compactly supported singularities, to a priori bounds for the Monge-Amp\`ere
mass of $(dd^c\phi)^n$. The inequality is valid locally or globally on an
arbitrary op... | math.CV math.AG | the goal of this short note is to relate the integrability property of the exponential e2phi of a plurisubharmonic function phi with isolated or compactly supported singularities to a priori bounds for the mongeampere mass of ddcphin the inequality is valid locally or globally on an arbitrary open subset omega in bcn w... | [['the', 'goal', 'of', 'this', 'short', 'note', 'is', 'to', 'relate', 'the', 'integrability', 'property', 'of', 'the', 'exponential', 'e2phi', 'of', 'a', 'plurisubharmonic', 'function', 'phi', 'with', 'isolated', 'or', 'compactly', 'supported', 'singularities', 'to', 'a', 'priori', 'bounds', 'for', 'the', 'mongeampere'... | [-0.13551654401191762, 0.058503384382309495, -0.09654190341907197, 0.0760300475603544, -0.05721862658980154, -0.15608783137209922, 0.031862367962913536, 0.3242982512635884, -0.2624250286624323, -0.2189698208201781, 0.1122271429919246, -0.24516201588525394, -0.10911764412961691, 0.2090716906627379, -0.08097744998130425,... |
709.3525 | Parameterization of the Woods-Saxon Potential for Shell-Model
Calculations | The drastically expanded use of the Woods-Saxon potential in modern day
nuclear physics and the availability of new nuclear data motivated us to review
and optimize the parameters of this potential to the experimental
single-nucleon spectra around the doubly-magic nuclei between $^{16}$O and
$^{208}$Pb. We obtain a p... | nucl-th | the drastically expanded use of the woodssaxon potential in modern day nuclear physics and the availability of new nuclear data motivated us to review and optimize the parameters of this potential to the experimental singlenucleon spectra around the doublymagic nuclei between 16o and 208pb we obtain a parameterization ... | [['the', 'drastically', 'expanded', 'use', 'of', 'the', 'woodssaxon', 'potential', 'in', 'modern', 'day', 'nuclear', 'physics', 'and', 'the', 'availability', 'of', 'new', 'nuclear', 'data', 'motivated', 'us', 'to', 'review', 'and', 'optimize', 'the', 'parameters', 'of', 'this', 'potential', 'to', 'the', 'experimental',... | [0.005556366098505899, 0.08675555593126323, -0.12363807641139085, 0.12518591453871605, -0.021213769522103028, -0.09389376458192383, 0.05045517938873492, 0.3597200837925323, -0.203774534924002, -0.2831530087313402, -0.04945537846724018, -0.2840937324799597, -0.01530407257532039, 0.17018686056768229, 0.049751992291224394... |
709.3526 | The log-linear group-lasso estimator and its asymptotic properties | We define the group-lasso estimator for the natural parameters of the
exponential families of distributions representing hierarchical log-linear
models under multinomial sampling scheme. Such estimator arises as the solution
of a convex penalized likelihood optimization problem based on the group-lasso
penalty. We il... | math.ST stat.TH | we define the grouplasso estimator for the natural parameters of the exponential families of distributions representing hierarchical loglinear models under multinomial sampling scheme such estimator arises as the solution of a convex penalized likelihood optimization problem based on the grouplasso penalty we illustrat... | [['we', 'define', 'the', 'grouplasso', 'estimator', 'for', 'the', 'natural', 'parameters', 'of', 'the', 'exponential', 'families', 'of', 'distributions', 'representing', 'hierarchical', 'loglinear', 'models', 'under', 'multinomial', 'sampling', 'scheme', 'such', 'estimator', 'arises', 'as', 'the', 'solution', 'of', 'a'... | [-0.06156571182628097, 0.019003577967026123, -0.0996468211757696, 0.1222588661814455, -0.060730091021342074, -0.16158835779940492, 0.07619806829038574, 0.3675959023083885, -0.30648334789885817, -0.2933467793695325, 0.11959620692488347, -0.25069795336728634, -0.17727387573050205, 0.14451192314384592, -0.0990697087592791... |
709.3527 | Type II critical phenomena of neutron star collapse | We investigate spherically-symmetric, general relativistic systems of
collapsing perfect fluid distributions. We consider neutron star models that
are driven to collapse by the addition of an initially "in-going" velocity
profile to the nominally static star solution. The neutron star models we use
are Tolman-Oppenhe... | gr-qc astro-ph | we investigate sphericallysymmetric general relativistic systems of collapsing perfect fluid distributions we consider neutron star models that are driven to collapse by the addition of an initially ingoing velocity profile to the nominally static star solution the neutron star models we use are tolmanoppenheimervolkof... | [['we', 'investigate', 'sphericallysymmetric', 'general', 'relativistic', 'systems', 'of', 'collapsing', 'perfect', 'fluid', 'distributions', 'we', 'consider', 'neutron', 'star', 'models', 'that', 'are', 'driven', 'to', 'collapse', 'by', 'the', 'addition', 'of', 'an', 'initially', 'ingoing', 'velocity', 'profile', 'to'... | [-0.13388671964784413, 0.13769563504374335, -0.09914462244635598, 0.057016865087106176, -0.043164277170504216, -0.12814018204634697, 0.015051161474114434, 0.31753577064051763, -0.2131957718017887, -0.293265272076502, 0.06886959427270622, -0.2805728085687231, -0.04112812036052577, 0.159994415217495, 0.007902307792527671... |
709.3528 | Autour de la cohomologie de Bott-Chern | The goal of the memoir is to develop a new cohomology theory which
encompasses De Rham and Dolbeault cohomology as well as Deligne Beilinson
cohomology, in the context of general complex analytic manifolds. The special
case of the Iwasawa manifold is investigated as a typical example of what
occurs in the non K\"ahle... | math.AG math.DG | the goal of the memoir is to develop a new cohomology theory which encompasses de rham and dolbeault cohomology as well as deligne beilinson cohomology in the context of general complex analytic manifolds the special case of the iwasawa manifold is investigated as a typical example of what occurs in the non kahler case... | [['the', 'goal', 'of', 'the', 'memoir', 'is', 'to', 'develop', 'a', 'new', 'cohomology', 'theory', 'which', 'encompasses', 'de', 'rham', 'and', 'dolbeault', 'cohomology', 'as', 'well', 'as', 'deligne', 'beilinson', 'cohomology', 'in', 'the', 'context', 'of', 'general', 'complex', 'analytic', 'manifolds', 'the', 'specia... | [-0.1920822207416807, 0.017355993054141955, -0.09453448584037168, 0.15196250324204033, -0.1484337660883154, -0.11727904994040728, -0.076734770179194, 0.25180762620958763, -0.2906926568464509, -0.2667580901911216, 0.09098514762507486, -0.1875463532350425, -0.23934322710099099, 0.18131276401046698, -0.20584837812930346, ... |
709.3529 | Transport of Molecular Motor Dimers in Burnt-Bridge Models | Dynamics of molecular motor dimers, consisting of rigidly bound particles
that move along two parallel lattices and interact with underlying molecular
tracks, is investigated theoretically by analyzing discrete-state stochastic
continuous-time burnt-bridge models. In these models the motion of molecular
motors is vie... | cond-mat.stat-mech cond-mat.soft | dynamics of molecular motor dimers consisting of rigidly bound particles that move along two parallel lattices and interact with underlying molecular tracks is investigated theoretically by analyzing discretestate stochastic continuoustime burntbridge models in these models the motion of molecular motors is viewed as a... | [['dynamics', 'of', 'molecular', 'motor', 'dimers', 'consisting', 'of', 'rigidly', 'bound', 'particles', 'that', 'move', 'along', 'two', 'parallel', 'lattices', 'and', 'interact', 'with', 'underlying', 'molecular', 'tracks', 'is', 'investigated', 'theoretically', 'by', 'analyzing', 'discretestate', 'stochastic', 'conti... | [-0.1371247322630074, 0.21901511003942056, -0.033973736562213655, 0.029342015434186748, 0.01651463806589718, -0.15869016064946556, 0.02925424111643964, 0.4087423712046722, -0.27173991926987184, -0.2816658228915974, 0.022051166329667034, -0.2692171891221887, -0.13449870724175758, 0.17586276284665642, 0.00986347043535561... |
709.353 | Star Formation at Very Low Metallicity. IV. Fragmentation Does Not
Depend on Metallicity for Cold Initial Conditions | Primordial star formation appears to result in stars at least an order of
magnitude more massive than modern star formation. It has been proposed that
the transition from primordial to modern initial mass functions occurs due to
the onset of effective metal line cooling at a metallicity Z/Z_sun = 10^{-3.5}.
However, ... | astro-ph | primordial star formation appears to result in stars at least an order of magnitude more massive than modern star formation it has been proposed that the transition from primordial to modern initial mass functions occurs due to the onset of effective metal line cooling at a metallicity zz_sun 1035 however these simulat... | [['primordial', 'star', 'formation', 'appears', 'to', 'result', 'in', 'stars', 'at', 'least', 'an', 'order', 'of', 'magnitude', 'more', 'massive', 'than', 'modern', 'star', 'formation', 'it', 'has', 'been', 'proposed', 'that', 'the', 'transition', 'from', 'primordial', 'to', 'modern', 'initial', 'mass', 'functions', 'o... | [-0.06073898506076766, 0.1822375686930155, -0.04649246022390407, 0.11863625868230292, -0.02134938433022198, -0.10206872826602542, 0.031064892945249684, 0.40017273039980367, -0.19753662974275113, -0.32338505366852766, 0.06951465829538457, -0.23435296946319106, -0.042663909601822994, 0.18369933783687187, 0.04227698229823... |
709.3531 | On the Hopf Lemma | The Hopf Lemma for second order elliptic operators is proved to hold in
domains with $C^{1,\alpha}$, and even less regular, boundaries. It need not
hold for $C^1$ boundaries. Corresponding results are proved for second order
parabolic operators.
| math.AP math.DG | the hopf lemma for second order elliptic operators is proved to hold in domains with c1alpha and even less regular boundaries it need not hold for c1 boundaries corresponding results are proved for second order parabolic operators | [['the', 'hopf', 'lemma', 'for', 'second', 'order', 'elliptic', 'operators', 'is', 'proved', 'to', 'hold', 'in', 'domains', 'with', 'c1alpha', 'and', 'even', 'less', 'regular', 'boundaries', 'it', 'need', 'not', 'hold', 'for', 'c1', 'boundaries', 'corresponding', 'results', 'are', 'proved', 'for', 'second', 'order', 'p... | [-0.13906984912181222, 0.08355592915826049, -0.02238759947185581, 0.12213584429873908, -0.13264683508188338, -0.22512894896538677, -0.06446395431821411, 0.3684596299521021, -0.2520552140635413, -0.19651848666772648, 0.2290776121096585, -0.2911584936271145, -0.08226181642227881, 0.2728510781417827, -0.14967025625141891,... |
709.3532 | Brane tunneling and virtual brane-antibrane pairs | We survey barrier penetration by quantum tunneling for four cases:
nonrelativistic point particles, scalar fields, relativistic point particles,
and DBI branes. We examine two novel features that arise for DBI brane
tunneling: the rate can sometimes increase as the barrier gets higher; and the
instanton "wrinkles". W... | hep-th | we survey barrier penetration by quantum tunneling for four cases nonrelativistic point particles scalar fields relativistic point particles and dbi branes we examine two novel features that arise for dbi brane tunneling the rate can sometimes increase as the barrier gets higher and the instanton wrinkles we show that ... | [['we', 'survey', 'barrier', 'penetration', 'by', 'quantum', 'tunneling', 'for', 'four', 'cases', 'nonrelativistic', 'point', 'particles', 'scalar', 'fields', 'relativistic', 'point', 'particles', 'and', 'dbi', 'branes', 'we', 'examine', 'two', 'novel', 'features', 'that', 'arise', 'for', 'dbi', 'brane', 'tunneling', '... | [-0.15728322792749264, 0.2425687712935829, -0.08069388410321583, 0.17932720359041063, -0.047970310417249015, -0.17743843640690962, 0.0271615736419335, 0.29644194545567426, -0.2396846304120692, -0.2676943637259108, 0.00018450405638615943, -0.3183652941921824, -0.14846636555892856, 0.15474142954534678, -0.027281984729741... |
709.3533 | Robustness of operator quantum error correction with respect to
initialization errors | In the theory of operator quantum error correction (OQEC), the notion of
correctability is defined under the assumption that states are perfectly
initialized inside a particular subspace, a factor of which (a subsystem)
contains the protected information. If the initial state of the system does not
belong entirely to... | quant-ph | in the theory of operator quantum error correction oqec the notion of correctability is defined under the assumption that states are perfectly initialized inside a particular subspace a factor of which a subsystem contains the protected information if the initial state of the system does not belong entirely to the subs... | [['in', 'the', 'theory', 'of', 'operator', 'quantum', 'error', 'correction', 'oqec', 'the', 'notion', 'of', 'correctability', 'is', 'defined', 'under', 'the', 'assumption', 'that', 'states', 'are', 'perfectly', 'initialized', 'inside', 'a', 'particular', 'subspace', 'a', 'factor', 'of', 'which', 'a', 'subsystem', 'cont... | [-0.14454277107205657, 0.1309160964379025, -0.07910618255259938, 0.09518373179777863, -0.014491834271558486, -0.17683347788967674, 0.0366470509032022, 0.34832557997994607, -0.28310734382328046, -0.2759411774321104, 0.15374015115214873, -0.2240306807945423, -0.11847405856359657, 0.1705602568828856, -0.13064957954485318,... |
709.3534 | Meridional Almost Normal Surfaces in Knot Complements | Suppose $K$ is a knot in a closed 3-manifold $M$ such that $\bar{M-N(K)}$ is
irreducible. We show that for any positive integer $b$ there exists a
triangulation of $\bar{M-N(K)}$ such that any weakly incompressible bridge
surface for $K$ of $b$ bridges or fewer is isotopic to an almost normal bridge
surface.
| math.GT | suppose k is a knot in a closed 3manifold m such that barmnk is irreducible we show that for any positive integer b there exists a triangulation of barmnk such that any weakly incompressible bridge surface for k of b bridges or fewer is isotopic to an almost normal bridge surface | [['suppose', 'k', 'is', 'a', 'knot', 'in', 'a', 'closed', '3manifold', 'm', 'such', 'that', 'barmnk', 'is', 'irreducible', 'we', 'show', 'that', 'for', 'any', 'positive', 'integer', 'b', 'there', 'exists', 'a', 'triangulation', 'of', 'barmnk', 'such', 'that', 'any', 'weakly', 'incompressible', 'bridge', 'surface', 'for... | [-0.25580357354875577, 0.1915471204203121, -0.1042298425217064, 0.004742291145387809, -0.06608319809014092, -0.23647588709065195, 0.02940660730308416, 0.39443289716633, -0.2859171774162322, -0.24394422142329264, 0.016573738304384966, -0.29708035430889956, -0.17356362430929986, 0.16943150316840228, -0.08616013070378377,... |
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