<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi>Q</mml:mi></mml:mrow><mml:mrow><mml:mn>2</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>dependence of diffractive vector meson electroproduction

Martin, A. D.; Ryskin, M.G.; Teubner, T.

doi:10.1103/physrevd.62.014022

Cited by 142 publications

(201 citation statements)

References 30 publications

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“…with the same subprocess amplitude as in (25). The generalization of (25) and (28) to other pseudoscalar mesons and even to vector mesons [46] (where μ V = m V ) is straightforward.…”

Section: Generalizations and Applicationsmentioning

confidence: 99%

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Status of DVMP, DVCS and GPDs

Kroll

2015

EPJ Web of Conferences

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Abstract. The analysis of exclusive meson leptoproduction (DVMP) within the handbag approach is reviewed and the parametrization of the generalized parton distributions (GPDs) is discussed in some detail with the main interest focused of the GPDs H and E. Applications of the GPDs extracted from DVMP to other hard exclusive processes as for instance deeply virtual Compton scattering (DVCS) and an evaluation of Ji's sum rule are also presented.

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“…with the same subprocess amplitude as in (25). The generalization of (25) and (28) to other pseudoscalar mesons and even to vector mesons [46] (where μ V = m V ) is straightforward.…”

Section: Generalizations and Applicationsmentioning

confidence: 99%

“…The modified perturbative approach utilized in [8], is designed in such a way that asymptotically the leading-twist result [2] emerges. In passing I would like to remark that the treatment of the gluonic part of the amplitudes bears resemblance to the color-dipole model, see for instance [25][26][27].…”

Section: Extraction Of the Gpd H From Dvmpmentioning

confidence: 99%

Status of DVMP, DVCS and GPDs

Kroll

2015

EPJ Web of Conferences

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“…The allowed mass window is claimed to be [25][26][27][28][29][30][31][32][33][34][35] GeV. Within such a scenario there should exist a spectrum ofgg bound states (gluinoballs or gluinonia), which may reveal themselves in gluon-gluon collisions.…”

Section: Gluinoball Productionmentioning

confidence: 99%

Prospects for new physics observations in diffractive processes at the LHC and Tevatron

2002

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We study the double-diffractive production of various heavy systems (e.g. Higgs, dijet, tt and SUSY particles) at LHC and Tevatron collider energies. In each case we compute the probability that the rapidity gaps, which occur on either side of the produced system, survive the effects of soft rescattering and QCD bremsstrahlung effects. We calculate both the luminosity for different production mechanisms, and a wide variety of subprocess cross sections. The results allow numerical predictions to be readily made for the cross sections of all these processes at the LHC and the Tevatron collider. For example, we predict that the cross section for the exclusive double-diffractive production of a 120 GeV Higgs boson at the LHC is about 3 fb, and that the QCD background in the bb decay mode is about 4 times smaller than the Higgs signal if the experimental missing-mass resolution is 1 GeV. For completeness we also discuss production via γγ or W W fusion.

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“…The impact of these NMSSM specific features on sparticle production and on cascade decays has already been addressed: sparticle decays into singlino-like neutralinos have been studied in [16][17][18][19][20][21], sparticle decays into neutralinos in [22], decays of stops, sbottoms and staus in [23], the associated production of a light CP-odd Higgs boson with a chargino pair in [24], neutralino decays into light Higgs bosons in [25], neutralino decays into soft leptons in [26], and neutralino and chargino decays into many leptons in [27].…”

Section: Introductionmentioning

confidence: 99%

NMSDECAY: A Fortran code for supersymmetric particle decays in the Next-to-Minimal Supersymmetric Standard Model

Das

Ellwanger

Teixeira

2012

Computer Physics Communications

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The code NMSDECAY allows to compute widths and branching ratios of sparticle decays in the Next-to-Minimal Supersymmetric Standard Model. It is based on a generalization of SDECAY, to include the extended Higgs and neutralino sectors of the NMSSM. Slepton 3-body decays, possibly relevant in the case of a singlino-like lightest supersymmetric particle, have been added. NMSDECAY will be part of the NMSSMTools package, which computes Higgs, sparticle masses and Higgs decays in the NMSSM.

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Q2dependence of diffractive vector meson electroproduction

Cited by 142 publications

References 30 publications

Status of DVMP, DVCS and GPDs

Status of DVMP, DVCS and GPDs

Prospects for new physics observations in diffractive processes at the LHC and Tevatron

NMSDECAY: A Fortran code for supersymmetric particle decays in the Next-to-Minimal Supersymmetric Standard Model

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