15,449 research outputs found
Corrections to the Gell-Mann-Oakes-Renner relation and chiral couplings and
Next to leading order corrections to the
Gell-Mann-Oakes-Renner relation (GMOR) are obtained using weighted QCD Finite
Energy Sum Rules (FESR) involving the pseudoscalar current correlator. Two
types of integration kernels in the FESR are used to suppress the contribution
of the kaon radial excitations to the hadronic spectral function, one with
local and the other with global constraints. The result for the pseudoscalar
current correlator at zero momentum is , leading to the chiral corrections to GMOR: . The resulting uncertainties are mostly due to variations in the upper
limit of integration in the FESR, within the stability regions, and to a much
lesser extent due to the uncertainties in the strong coupling and the strange
quark mass. Higher order quark mass corrections, vacuum condensates, and the
hadronic resonance sector play a negligible role in this determination. These
results confirm an independent determination from chiral perturbation theory
giving also very large corrections, i.e. roughly an order of magnitude larger
than the corresponding corrections in chiral . Combining
these results with our previous determination of the corrections to GMOR in
chiral , , we are able to determine two low
energy constants of chiral perturbation theory, i.e. , and , both at the
scale of the -meson mass.Comment: Revised version with minor correction
Gas expulsion in highly substructured embedded star clusters
We investigate the response of initially substructured, young, embedded star
clusters to instantaneous gas expulsion of their natal gas. We introduce
primordial substructure to the stars and the gas by simplistically modelling
the star formation process so as to obtain a variety of substructure
distributed within our modelled star forming regions. We show that, by
measuring the virial ratio of the stars alone (disregarding the gas
completely), we can estimate how much mass a star cluster will retain after gas
expulsion to within 10% accuracy, no matter how complex the background
structure of the gas is, and we present a simple analytical recipe describing
this behaviour. We show that the evolution of the star cluster while still
embedded in the natal gas, and the behavior of the gas before being expelled,
are crucial processes that affect the timescale on which the cluster can evolve
into a virialized spherical system. Embedded star clusters that have high
levels of substructure are subvirial for longer times, enabling them to survive
gas expulsion better than a virialized and spherical system. By using a more
realistic treatment for the background gas than our previous studies, we find
it very difficult to destroy the young clusters with instantaneous gas
expulsion. We conclude that gas removal may not be the main culprit for the
dissolution of young star clusters.Comment: 19 pages, 8 figures, 2 tables. Accepted for publication in MNRA
A Correlation Between Hard Gamma-ray Sources and Cosmic Voids Along the Line of Sight
We estimate the galaxy density along lines of sight to hard extragalactic
gamma-ray sources by correlating source positions on the sky with a void
catalog based on the Sloan Digital Sky Survey (SDSS). Extragalactic gamma-ray
sources that are detected at very high energy (VHE; E>100 GeV) or have been
highlighted as VHE-emitting candidates in the Fermi Large Area Telescope hard
source catalog (together referred to as "VHE-like" sources) are distributed
along underdense lines of sight at the 2.4 sigma level. There is also a less
suggestive correlation for the Fermi hard source population (1.7 sigma). A
correlation between 10-500 GeV flux and underdense fraction along the line of
sight for VHE-like and Fermi hard sources is found at 2.4 sigma and 2.6 sigma,
respectively. The preference for underdense sight lines is not displayed by
gamma-ray emitting galaxies within the second Fermi catalog, containing sources
detected above 100 MeV, or the SDSS DR7 quasar catalog. We investigate whether
this marginal correlation might be a result of lower extragalactic background
light (EBL) photon density within the underdense regions and find that, even in
the most extreme case of a entirely underdense sight line, the EBL photon
density is only 2% less than the nominal EBL density. Translating this into
gamma-ray attenuation along the line of sight for a highly attenuated source
with opacity tau(E,z) ~5, we estimate that the attentuation of gamma-rays
decreases no more than 10%. This decrease, although non-neglible, is unable to
account for the apparent hard source correlation with underdense lines of
sight.Comment: Accepted by MNRA
Mesoscopic Theory of Critical Fluctuations in Isolated Granular Gases
Fluctuating hydrodynamics is used to describe the total energy fluctuations
of a freely evolving gas of inelastic hard spheres near the threshold of the
clustering instability. They are shown to be governed by vorticity fluctuations
only, that also lead to a renormalization of the average total energy. The
theory predicts a power-law divergent behavior of the scaled second moment of
the fluctuations, and a scaling property of their probability distribution,
both in agreement with simulations results. A more quantitative comparison
between theory and simulation for the critical amplitudes and the form of the
scaling function is also carried out
Chiral corrections to the Gell-Mann-Oakes-Renner relation
The next to leading order chiral corrections to the
Gell-Mann-Oakes-Renner (GMOR) relation are obtained using the pseudoscalar
correlator to five-loop order in perturbative QCD, together with new finite
energy sum rules (FESR) incorporating polynomial, Legendre type, integration
kernels. The purpose of these kernels is to suppress hadronic contributions in
the region where they are least known. This reduces considerably the systematic
uncertainties arising from the lack of direct experimental information on the
hadronic resonance spectral function. Three different methods are used to
compute the FESR contour integral in the complex energy (squared) s-plane, i.e.
Fixed Order Perturbation Theory, Contour Improved Perturbation Theory, and a
fixed renormalization scale scheme. We obtain for the corrections to the GMOR
relation, , the value . This result
is substantially more accurate than previous determinations based on QCD sum
rules; it is also more reliable as it is basically free of systematic
uncertainties. It implies a light quark condensate . As a byproduct, the chiral perturbation theory (unphysical) low energy
constant is predicted to be , or .Comment: A comment about the value of the strong coupling has been added at
the end of Section 4. No change in results or conslusion
(Pseudo)Scalar Charmonium in Finite Temperature QCD
The hadronic parameters of pseudoscalar () and scalar ()
charmonium are determined at finite temperature from Hilbert moment QCD sum
rules. These parameters are the hadron mass, leptonic decay constant, total
width, and continuum threshold (). Results for in both channels
indicate that starts approximately constant, and then it decreases
monotonically with increasing until it reaches the QCD threshold, , at a critical temperature T = T_c \simeq 180 \; \mbox{MeV}
interpreted as the deconfinement temperature. The other hadronic parameters
behave qualitatively similarly to those of the , as determined in this
same framework. The hadron mass is essentially constant, the total width is
initially independent of T, and after it begins to increase
with increasing up to for
(), and subsequently it decreases sharply up to , for (), beyond which the sum rules are no
longer valid. The decay constant of at first remains basically flat up
to , then it starts to decrease up to , and finally it increases sharply with increasing . In the case of
the decay constant does not change up to where
it begins a gentle increase up to beyond which it
increases dramatically with increasing . This behaviour contrasts with that
of light-light and heavy-light quark systems, and it suggests the survival of
the and the states beyond the critical temperature, as
already found for the from similar QCD sum rules. These conclusions
are very stable against changes in the critical temperature in the wide range
T_c = 180 - 260 \; \mbox{MeV}.Comment: 12 pages, 5 figures. A wide range of critical temperatures has been
considered. No qualitative changes to the conclusion
Fanatismo religioso y decadencia nacional. Los escritos afrancesados de Manuel Alonso de Viado
Los escritos que Manuel Alonso de Viado publicó durante la Guerra de la Independencia son una buena muestra del papel que los partidarios de José Bonaparte desempeñaron en los orígenes ideológicos del progresismo español. En ellos se repite, con una contundencia hasta entonces impensable en España, una idea común de los ilustrados europeos: que la decadencia española era fruto del fanatismo religioso. Pero no por eso carecen de patriotismo. Con la misma claridad, se enfrentan al tópico que atribuía la decadencia nacional al carácter del pueblo español e insisten en culpar únicamente a clérigos y gobernantes. De este modo, defienden el honor patrio al mismo tiempo que justifican la intervención napoleónica en España: sólo un cambio drástico en el gobierno y en las leyes del país podía permitir que los talentos españoles contribuyesen libremente al progreso de su patria.The writings of Manuel Alonso de Viado during the Peninsular War offer evidence of the significant but largely ignored role played by the supporters of Joseph Bonaparte in the ideological development of modern Spanish liberalism. With an openness previously unthinkable in Spain, those writings repeated an idea many times expressed in other European countries since the Early Enlightenment: that the decline of Spain was caused by religious fanaticism. But however much they copied some arguments from the so-called Black Legend, these were not anti-patriotic writings. They firmly rejected the widespread attribution of Spanish decline to the national character of its people, and insisted that clerics and rulers were the only ones to blame. In this way they defended the honour of the nation while at the same time justifying the Napoleonic intervention in Spain: only a drastic change in the country’s government and legislation could free Spanish minds from the chains that until then had prevented them from contributing to national progress.Les écrits que Manuel Alonso de Viado publia pendant la Guerre d’Indépendance constituent un bel exemple du rôle joué par les partisans de Joseph Bonaparte dans les origines idéologiques du progressisme espagnol. On retrouve répété dans ces derniers, avec une force jusque là impensable en Espagne, une idée récurrente chez les penseurs des Lumières en Europe : à savoir que la décadence espagnole était le fruit du fanatisme religieux. Pour autant ces écrits ne manquent pas de patriotisme. Avec la même franchise, ils s’attaquent au lieu commun qui attribuait la décadence nationale au caractère du peuple espagnol et insistent pour faire porter la culpabilité aux clercs et aux dirigeants. Ainsi, ils défendent l’honneur national en même temps qu’ils justifient l’intervention napoléonienne en Espagne : seul un changement drastique dans le gouvernement et dans les lois du pays pourra permettre aux talents espagnols de contribuer librement au progrès de leur patrie
Hadronic contribution to the muon g-2: a theoretical determination
The leading order hadronic contribution to the muon g-2, , is
determined entirely from theory using an approach based on Cauchy's theorem in
the complex squared energy s-plane. This is possible after fitting the
integration kernel in with a simpler function of . The
integral determining in the light-quark region is then split
into a low energy and a high energy part, the latter given by perturbative QCD
(PQCD). The low energy integral involving the fit function to the integration
kernel is determined by derivatives of the vector correlator at the origin,
plus a contour integral around a circle calculable in PQCD. These derivatives
are calculated using hadronic models in the light-quark sector. A similar
procedure is used in the heavy-quark sector, except that now everything is
calculable in PQCD, thus becoming the first entirely theoretical calculation of
this contribution. Using the dual resonance model realization of Large
QCD to compute the derivatives of the correlator leads to agreement with the
experimental value of . Accuracy, though, is currently limited by the
model dependent calculation of derivatives of the vector correlator at the
origin. Future improvements should come from more accurate chiral perturbation
theory and/or lattice QCD information on these derivatives, allowing for this
method to be used to determine accurately entirely from theory,
independently of any hadronic model.Comment: Several additional clarifying paragraphs have been added. 1/N_c
corrections have been estimated. No change in result
Charm-quark mass from weighted finite energy QCD sum rules
The running charm-quark mass in the scheme is determined from
weighted finite energy QCD sum rules (FESR) involving the vector current
correlator. Only the short distance expansion of this correlator is used,
together with integration kernels (weights) involving positive powers of ,
the squared energy. The optimal kernels are found to be a simple {\it pinched}
kernel, and polynomials of the Legendre type. The former kernel reduces
potential duality violations near the real axis in the complex s-plane, and the
latter allows to extend the analysis to energy regions beyond the end point of
the data. These kernels, together with the high energy expansion of the
correlator, weigh the experimental and theoretical information differently from
e.g. inverse moments FESR. Current, state of the art results for the vector
correlator up to four-loop order in perturbative QCD are used in the FESR,
together with the latest experimental data. The integration in the complex
s-plane is performed using three different methods, fixed order perturbation
theory (FOPT), contour improved perturbation theory (CIPT), and a fixed
renormalization scale (FMUPT). The final result is , in a wide region of stability against changes in the
integration radius in the complex s-plane.Comment: A short discussion on convergence issues has been added at the end of
the pape
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