Two photons plus jet al LHC: the NNLO contribution from the gg initiated process

The production of the Standard Model Higgs boson of mass ~ 100-140 GeV at the LHC likely gives clear signals in the $\gamma \gamma$ (1) and in the $\gamma \gamma jet$ (2) channels. The quantitative evaluation of the background to channel (1) is very hard since the next-to-leading order (NLO) and next-to-next-to-leading order (NNLO) QCD corrections are large. In particular, the contributions of the NNLO QCD subprocess $gg -> \gamma \gamma$ to inclusive $\gamma\gamma$ production is comparable to the contribution of the leading order subprocess $q\bar{q} -> \gamma \gamma$. The quantitative description of the background to channel (1), therefore, requires to calculate all corrections up to the NNNLO level. In this letter we present results on the contribution of the NNLO QCD subprocess $gg -> g \gamma \gamma$ to the production rate of channel (2). We have found that in this case this NNLO contribution is less than 20% of the Born contribution. Since the NNLO contributions will likely be dominated by this subprocess one can argue that in the case of channel (2) - contrary to the case of channel (1)- a quantitative description of the background can be achieved already at next-to-leading order accuracy.Comment: 7 pages, two figures include

Resonance-continuum interference in the di-photon Higgs signal at the LHC

A low mass Standard Model Higgs boson should be visible at the Large Hadron Collider through its production via gluon-gluon fusion and its decay to two photons. We compute the interference of this resonant process, gg -> H -> gamma gamma, with the continuum QCD background, gg -> gamma gamma induced by quark loops. Helicity selection rules suppress the effect, which is dominantly due to the imaginary part of the two-loop gg -> gamma gamma scattering amplitude. The interference is destructive, but only of order 5% in the Standard Model, which is still below the 10-20% present accuracy of the total cross section prediction. We comment on the potential size of such effects in other Higgs models.Comment: 10 pages, 2 figure

Local order and magnetic behavior of amorphous and nanocrystalline yttrium iron garnet produced by swift heavy ion irradiations

International audienceThin epitaxial films of gallium or scandium-doped and undoped yttrium iron garnet (Y3Fe5O12 or YIG) on nonmagnetic Gd3Ga5O12 substrates were irradiated with swift heavy ions (50 MeV 32S, 50 MeV 63Cu, and 235 MeV 84Kr) in the electronic slowing down regime. The mean electronic stopping power in the films was always larger than the threshold for amorphous track formation in YIG which is around 4.5 MeV/μm in this low ion-velocity range. The local order and magnetic properties of the damaged films were then studied at room temperature by 57Fe conversion electron Mössbauer spectroscopy (CEMS) and x-ray absorption spectroscopy (XAS) at the iron K edge in the fluorescence mode. In the case of paramagnetic gallium or scandium-substituted films (YIG:Ga, YIG:Sc) irradiated with 32S or 63Cu ions, the CEMS data show that the tetrahedral Fe3+ sites are preferentially damaged, while the octahedral sites are conserved. This is confirmed by the decrease of the pre-edge peak in the XAS data of the ferrimagnetic undoped YIG films showing that the number of tetrahedral iron sites is decreased in the amorphous phase obtained with 84Kr ion irradiation, due to the formation of fivefold-coordinated pyramidal sites, as already found in a previous study on undoped YIG sinters amorphized by 3.5 GeV 132Xe ion irradiation. In the case of the nanophase induced by ion-beam recrystallization of the tracks with 32S or 63Cu irradiations, a further decrease of the pre-edge peak is found. This is interpreted by (i) an increase of the fivefold-coordinated pyramidal sites and/or (ii) a probable decomposition of the garnet into orthoferrite (YFeO3) and haematite (α-Fe2O3) under the high-pressure and high-temperature conditions in the thermal spike generated by the ions. The CEMS data of irradiated undoped YIG also show that both the amorphous and nanocrystalline phases have a paramagnetic behavior at room temperature. The nanophase magnetic behavior is analyzed on the basis of a superparamagnetic relaxation above the blocking temperature, whereas the amorphous phase behavior is ascribed to a speromagnetic state

Numerical Schemes for Multivalued Backward Stochastic Differential Systems

We define some approximation schemes for different kinds of generalized backward stochastic differential systems, considered in the Markovian framework. We propose a mixed approximation scheme for a decoupled system of forward reflected SDE and backward stochastic variational inequality. We use an Euler scheme type, combined with Yosida approximation techniques.Comment: 13 page

Diffusion Process in a Flow

We establish circumstances under which the dispersion of passive contaminants in a forced, deterministic or random, flow can be consistently interpreted as a Markovian diffusion process. In case of conservative forcing the repulsive case only, $\vec{F}=\vec{\nabla }V$ with $V(\vec{x},t)$ bounded from below, is unquestionably admitted by the compatibility conditions. A class of diffusion processes is exemplified, such that the attractive forcing is allowed as well, due to an appropriate compensation coming from the "pressure" term. The compressible Euler flows form their subclass, when regarded as stochastic processes. We establish circumstances under which the dispersion of passive contaminants in a forced, deterministic or random, flow can be consistently interpreted as a Markovian diffusion process. In case of conservative forcing the repulsive case only, $\vec{F}=\vec{\nabla }V$ with $V(\vec{x},t)$ bounded from below, is unquestionably admitted by the compatibility conditions. A class of diffusion processes is exemplified, such that the attractive forcing is allowed as well, due to an appropriate compensation coming from the "pressure" term. The compressible Euler flows form their subclass, when regarded as stochastic processes.Comment: 10 pages, Late

Diffusion and Current of Brownian Particles in Tilted Piecewise Linear Potentials: Amplification and Coherence

Overdamped motion of Brownian particles in tilted piecewise linear periodic potentials is considered. Explicit algebraic expressions for the diffusion coefficient, current, and coherence level of Brownian transport are derived. Their dependencies on temperature, tilting force, and the shape of the potential are analyzed. The necessary and sufficient conditions for the non-monotonic behavior of the diffusion coefficient as a function of temperature are determined. The diffusion coefficient and coherence level are found to be extremely sensitive to the asymmetry of the potential. It is established that at the values of the external force, for which the enhancement of diffusion is most rapid, the level of coherence has a wide plateau at low temperatures with the value of the Peclet factor 2. An interpretation of the amplification of diffusion in comparison with free thermal diffusion in terms of probability distribution is proposed.Comment: To appear in PR

Non-equilibrium phase transition in a sheared granular mixture

The dynamics of an impurity (or tracer particle) immersed in a dilute granular gas under uniform shear flow is investigated. A non-equilibrium phase transition is identified from an exact solution of the inelastic Boltzmann equation for a granular binary mixture in the tracer limit, where the impurity carries either a vanishing (disordered phase) or a finite (ordered phase) fraction of the total kinetic energy of the system. In the disordered phase, the granular temperature ratio (impurity "temperature" over that of the host fluid) is finite, while it diverges in the ordered phase. To correctly capture this extreme violation of energy equipartition, we show that the picture of an impurity enslaved to the host fluid is insufficient

Relationship between Strain Rate and Myocardial Structure in Severe Aortic Stenosis

Introducción: En la estenosis aórtica sintomática grave (EASG), la alteración del strain global longitudinal sistólico (SGLS) tendría correlación con las modificaciones de la histoarquitectura y podría identificar compromiso contráctil temprano en pacientes con fracción de eyección conservada (FEyC). Objetivo: Analizar el SGLS, el volumen de colágeno (VC), el área miocitaria (ArMi) y el compromiso contráctil en pacientes con EASG y FEyC. Material y métodos: Se incorporaron 26 pacientes con EASG y FEyC (edad 67 ± 11 años, 53% hombres). Se realizaron un estudio hemodinámico preoperatorio y una biopsia endomiocárdica intraoperatoria para determinar el VC y el ArMi. Se identificaron tres grupos de pacientes: G1, hipertrofia ventricular izquierda (HVI) compensada sin enfermedad coronaria (n = 8); G2, HVI descompensada sin enfermedad coronaria (n = 7) y G3, HVI descompensada con enfermedad coronaria (n = 11). El SGLS se normalizó por volumen sistólico, estrés meridional de fin de sístole (δ) y diámetro de fin de diástole (DFD). Resultados: G1, G2 y G3, sin diferencias en volumen sistólico, δ y DFD y con diferencias en VC (%) (G1: 4,7 ± 1,2; G2: 8,4 ± 1,2; G3: 11,0 ± 3,0; p < 0,01), ArMi (mm2) (G1: 328,7 ± 66,2; G2: 376,7 ± 21,9; G3: 385,0 ± 13,0; p = 0,01), PFDVI (mm Hg) (G1: 13,1 ± 1,5; G2: 19,0 ± 3,8; G3: 23,6 ± 5,8; p < 0,01), +dP/dtmáx (mm Hg/seg / PFDVI, mm Hg) (G1: 176,4 ± 45,5; G2: 89,6 ± 20,1; G3: 113,1 ± 43,7; p < 0,01), SGLS (%) (G1: -17,9 ± 4,2; G2: -13,5 ± 2,5; G3: -13,6 ± 3; p = 0,021). El SGLS se correlacionó con VC y PFDVI y hubo tendencia con un índice de contractilidad (+dP/dtmáx mm Hg/seg / PFDVI, mm Hg). Conclusiones: Las alteraciones del SGLS en pacientes con EASG y FEyC son expresión de alteraciones estructurales delBackground: In severe symptomatic aortic stenosis (SSAS) altered global longitudinal systolic strain (GLSS) would correlate with changes in myocardial histological architecture and could identify early contractile involvement in patients with preserved ejection fraction (PEF). Objective: The aim of this study was to analyze GLSS, collagen volume (CV), myocyte area (MyAr) and contractile involvement in patients with SSAS and PEF. Methods: Twenty six patients with SSAS and PEF (67±11 years old, 53% male) were included in the study. A preoperative hemodynamic study and an intraoperative endomyocardial biopsy were performed to determine CV and MyAr. Three groups of patients were identified: G1: compensated left ventricular hypertrophy (LVH) without coronary disease (n=8); G2: decompensated LVH without coronary disease (n=7) and G3: decompensated LVH with coronary disease (n=11). GLSS was normalized by stroke volume, meridional end-systolic wall stress (δ) and end-diastolic diameter (EDD). Results: No significant differences in stroke volume, δ and EDD were observed between groups G1, G2 and G3. Differences between groups were observed in: CV (%) (G1: 4.7 ± 1.2, G2: 8.4 ± 1.2, G3: 11.0 ± 3.0; p < 0.01), MyAr (mm2) (G1: 328.7 ± 66.2, G2: 376.7 ± 21.9, G3: 385.0 ± 13.0; p = 0.01), LVEDP (mm Hg) (G1: 13.1 ± 1.5, G2: 19.0 ± 3.8, G3: 23.6 ± 5.8; p < 0.01), +dP/dtmax (mm Hg/sec / LVEDP, mm Hg) (G1: 176.4 ± 45.5, G2: 89.6 ± 20.1, G3: 113.1 ± 43.7; p < 0.01), and GLSS (%) (G1: -17.9 ± 4.2, G2: -13.5 ± 2.5, G3: -13.6 ± 3; p = 0.021). GLSS correlated with CV and LVEDP and it evidenced a trend to correlate with a contractility index (+dP/dtmax mm Hg/s / LVEDP, mm Hg). Conclusions: Altered GLSS in patients with SSAS and PEF expresses myocardial structural changes related to increase in C V, which is associated with enhanced LVEDP and probable myocardial contractile failure.Fil: Hita, Alejandro. Hospital Universitario Austral; Argentina. Sociedad Argentina de Cardiología; ArgentinaFil: Baratta, Sergio. Hospital Universitario Austral; Argentina. Sociedad Argentina de Cardiología; ArgentinaFil: Chejtman, Demian. Hospital Universitario Austral; ArgentinaFil: Benticuaga, Alejandro. Hospital Universitario Austral; ArgentinaFil: Constantini, Ricardo. Hospital Universitario Austral; ArgentinaFil: Vaccarino, Guillermo. Sociedad Argentina de Cardiología; Argentina. Hospital Universitario Austral; ArgentinaFil: Donato, Pablo Martín. Hospital Universitario Austral; Argentina. Sociedad Argentina de Cardiología; Argentina. Universidad de Buenos Aires. Facultad de Medicina. Departamento de Patología; Argentina. Consejo Nacional de Investigaciones Científicas y Técnicas; ArgentinaFil: Gelpi, Ricardo Jorge. Sociedad Argentina de Cardiología; Argentina. Universidad de Buenos Aires. Facultad de Medicina. Instituto de Fisiopatología Cardiovascular; Argentina. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Houssay. Instituto de Bioquímica y Medicina Molecular. Universidad de Buenos Aires. Facultad Medicina. Instituto de Bioquímica y Medicina Molecular; ArgentinaFil: Matoso, Miriam. Universidad de Buenos Aires. Facultad de Medicina. Instituto de Fisiopatología Cardiovascular; ArgentinaFil: Morales, Celina. Universidad de Buenos Aires. Facultad de Medicina. Instituto de Fisiopatología Cardiovascular; Argentin