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ResearchHub is incentivizing healthy research behavior. At this time, first authors of open access papers are eligible for rewards. Visit the publications tab to view your eligible publications.
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Mohamad Mikati
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Compton Scattering by the Proton
Jorun Rugkåsa
et al.
Feb 6, 2001
Compton scattering by the proton has been measured over a wide range coveringphoton energies 250 MeV < E_\gamma < 800 MeV and photon scattering angles 30^0< \theta^{lab}_\gamma < 150^0, using the tagged-photon facility at MAMI (Mainz)and the large-acceptance arrangement LARA. The data are in good agreement withthe dispersion theory based on the SAID-SM99K parameterization of photo-mesonamplitudes. From the subset of data between 280 and 360 MeV the resonancepion-photoproduction amplitudes were evaluated leading to the multipole E2/M1ratio EMR(340 MeV) =(-1.6 \pm 0.4(stat+syst) \pm 0.2(model)%. From all databelow 455 MeV the proton's backward spin polarizability was determined to be\gamma_\pi=(-37.9 \pm 0.6(stat+syst) \pm 3.5(model))x10^{-4}fm^4.
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Supergravity Inspired Warped Compactifications and Effective Cosmological Constants
Jesus Perez
et al.
Oct 8, 1999
We propose a supergravity inspired derivation of a Randall-Sundrum's typeaction as an effective description of the dynamics of a brane coupled to thebulk through gravity only. The cosmological constants in the bulk and on thebrane appear at the classical level when solving the equations of motiondescribing the bosonic sector of supergravities in ten and eleven dimensionscoupled to the brane. They are related to physical quantities like the braneelectric charge and thus inherit some of their physical properties. The mostappealing property is their quantization: in d_\perp extra dimensions,Lambda_brane goes like N and Lambda_bulk like N^{2/(2-d_perp)}. This dynamicalorigin also explains the apparent fine-tuning required in the Randall-Sundrumscenario. In our approach, the cosmological constants are derived parametersand cannot be chosen arbitrarily; instead they are determined by the underlyingLagrangian. Some of the branes we construct that support cosmological constantin the bulk have supersymmetric properties: D3-branes of type IIB superstringtheory provide an explicit example.
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Type I Vacua from Diagonal $Z_3$-Orbifolds
David Erritzoe
et al.
Dec 22, 1999
We discuss the open descendants of diagonal irrational $Z_3$ orbifolds,starting from the $c=2$ case and analyzing six-dimensional and four-dimensionalmodels. As recently argued, their consistency is linked to the presence ofgeometric discrete moduli. The different classes of open descendants, relatedto different resolutions of the fixed-point ambiguities, are distinguished bythe number of geometric fixed points surviving the unoriented projection.
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On quasi-linear PDAEs with convection: applications, indices, numerical solution
Philip Lightfoot
et al.
Mar 17, 2013
For a class of partial differential algebraic equations (PDAEs) ofquasi-linear type which include nonlinear terms of convection type apossibility to determine a time and spatial index is considered. As a typicalexample we investigate an application from plasma physics. Especially wediscuss the numerical solution of initial boundary value problems by means of acorresponding finite difference splitting procedure which is a modification ofa well known fractional step method coupled with a matrix factorization. Theconvergence of the numerical solution towards the exact solution of thecorresponding initial boundary value problem is investigated. Some results of anumerical solution of the plasma PDAE are given.
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Nuclear matter hole spectral function in the Bethe-Brueckner-Goldstone approach
Raymond W. Lam
et al.
Dec 19, 2001
The hole spectral function is calculated in nuclear matter to assess therelevance of nucleon-nucleon short range correlations. The calculation iscarried out within the Brueckner scheme of many-body theory by using severalnucleon-nucleon realistic interactions. Results are compared with otherapproaches based on variational methods and transport theory. Discrepanciesappear in the high energy region, which is sensitive to short rangecorrelations, and are due to the different many-body treatment more than to thespecific N-N interaction used. Another conclusion is that the momentumdependence of the G-matrix should be taken into account in any self consistentapproach.
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