0000000000052114

AUTHOR

Gustav Kramer

showing 14 related works from this author

Inclusive B-meson production at small p_T in the general-mass variable-flavor-number scheme

2015

We calculate the cross section for the inclusive production of B mesons in pp and ppbar collisions at next-to-leading order in the general-mass variable-flavor-number scheme and show that a suitable choice of factorization scales leads to a smooth transition to the fixed-flavor-number scheme. Our numerical results are in good agreement with data from the Tevatron and LHC experiments at small and at large transverse momenta.

Particle physicsPhysics and Astronomy (miscellaneous)TevatronFOS: Physical scienceslow [transverse momentum]01 natural sciencesCross section (physics)High Energy Physics - Phenomenology (hep-ph)Factorization0103 physical sciencesscattering [p p]Order (group theory)B mesonddc:530Batavia TEVATRON Collinclusive production [B]factorization [scale]010306 general physicsnumerical calculationsNuclear ExperimentEngineering (miscellaneous)Variable (mathematics)PhysicsLarge Hadron Colliderscattering [anti-p p]higher-order [correction]010308 nuclear & particles physicsHigh Energy Physics::Phenomenologycalculated [total cross section]Transverse planeHigh Energy Physics - PhenomenologyCERN LHC Coll[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment1 [higher-order]correction [total cross section]
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Photon plus jet cross sections in deep inelastic ep collisions at order O(α2αs)

2000

The production of a hard and isolated photon accompanied by one or two jets in large- Q2 deep inelastic ep scattering is calculated at next-to-leading order. We include consistently contributions from quark-to-photon fragmentation and study various differential cross sections and their dependence on isolation cut parameters. Numerical results relevant for HERA experiments are presented.

PhysicsNuclear physicsNuclear and High Energy PhysicsPhotonFragmentation (mass spectrometry)ScatteringHigh Energy Physics::ExperimentHERADeep inelastic scatteringNuclear Physics B
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Photon Plus Jet Production in Large-Q2 ep Collisions at Next-to-Leading Order QCD

1999

The production of photons accompanied by jets in large-Q2 deep inelastic ep scattering is calculated in next-to-leading order. We describe how to consistently include contributions from quark-to-photon fragmentation and give numerical results relevant for HERA experiments.

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - PhenomenologyPhotonHigh Energy Physics - Phenomenology (hep-ph)ScatteringFOS: Physical sciencesHigh Energy Physics::ExperimentHERA
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Inclusive D∗-meson production in ep scattering at low Q2 in the GM-VFN scheme at NLO

2009

Abstract We have calculated the next-to-leading order cross sections for the inclusive production of D ∗ -mesons in ep collisions at HERA for finite, although very small Q 2 . In this Q 2 -range, the same approximations as for photoproduction can be used. Our calculation is performed in the general-mass variable-flavour-number scheme. In this approach, large logarithms of the charm transverse momentum are resummed and finite terms depending on m 2 / p T 2 are kept in the hard scattering cross sections. The theoretical results are compared with recent data from the ZEUS Collaboration at HERA. On average, we find good agreement.

PhysicsNuclear and High Energy PhysicsParticle physicsZEUS (particle detector)LogarithmMesonScatteringHigh Energy Physics::PhenomenologyHERANuclear physicsD mesonOrder (group theory)High Energy Physics::ExperimentCharm (quantum number)Physics Letters B
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Inclusive photoproduction of bottom quarks for low and medium p T in the general-mass variable-flavour-number scheme

2016

We present predictions for b-quark production in photoprodcution and compare with experimental data from HERA. Our theoretical predictions are obtained at next-to-leading-order in the general-mass variable-flavor-number scheme, an approach which takes into account the finite mass of the b quarks. We use realistic evolved nonperturbative fragmentation functions obtained from fits to e+e- data. We find in general good agreement of data with both the GM-VFNS and the FFNS calculations, while the more precise ZEUS data seem to prefer the GM-VFNS predictions.

electronQuarkParticle physicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeFlavourphotoproduction [bottom]FOS: Physical sciencesmass [bottom]01 natural sciencesquarkNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530010306 general physicsfinite [mass]Finite massPhysics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyExperimental dataZEUSHERAnonperturbative [fragmentation function]lcsh:QC1-999High Energy Physics - PhenomenologyDESY HERA StorTransverse momentumproduction [bottom]High Energy Physics::Experimentlcsh:PhysicsPhysics Letters B
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Finite-Mass Effects on Inclusive B-Meson Hadroproduction

2007

We calculate the transverse-momentum (p_T) distribution for the inclusive hadroproduction of B mesons at intermediate values of p_T at next-to-leading order (NLO) in a dedicated finite-mass scheme using realistic non-perturbative fragmentation functions that are obtained through a global fit to e^+e^- data from CERN LEP1 and SLAC SLC exploiting their universality and scaling violations. We find that finite-mass effects moderately enhance the cross section, by about 20% at p_T = 2 m_b, and rapidly fade out with increasing value of p_T, so that the zero-mass prediction is reached. We also perform comparisons with recent ppbar data taken by the CDF Collaboration in run II at the Fermilab Tevat…

Quantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMeson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciences01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]0103 physical sciencesPhysics::Accelerator PhysicsB mesonddc:530High Energy Physics::ExperimentFermilab010306 general physicsNuclear ExperimentScalingFinite mass
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Study of heavy meson production in p–Pb collisions atS=5.02TeV in the general-mass variable-flavour-number scheme

2017

Abstract We study inclusive charm and bottom production, for both D and B mesons, in p–Pb collisions at the LHC. Numerical results for p T -differential production cross sections are obtained at next-to-leading-order in the general-mass variable-flavour-number scheme. We compare our results with recent data from ALICE, LHCb and CMS at a centre-of-mass energy of 5 TeV and find good agreement. A comparison with p–p cross sections does not reveal the presence of nuclear initial-state interaction effects that could be expected to become visible as deviations of the ratio of p–Pb and p–p cross sections from one.

PhysicsNuclear and High Energy PhysicsParticle physicsMeson productionLarge Hadron Collider010308 nuclear & particles physicsMonte Carlo methodFlavour01 natural sciences0103 physical sciencesHigh Energy Physics::ExperimentB mesonCharm (quantum number)010306 general physicsVariable (mathematics)Nuclear Physics B
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Calculation of theO(? s 2 ) parity-violating structure functions in $$e^ + e^ - \to q\bar qg$$

1986

We calculate the two nonvanishingO(αs2) parity-violating structure functions that contribute to\(e^ + e^ - \xrightarrow{{\gamma ,Z}}q\bar qg\). We discuss how these can be measured. We work with massless quarks and gluons and use dimensional regularization to regularize ultra-violet and infrared singularities. We carefully discuss how to deal withγ5 in the dimensional regularization scheme when infrared singularities are present.

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::LatticeElectron–positron annihilationHigh Energy Physics::PhenomenologyElementary particleParity (physics)Massless particleDimensional regularizationQuark–gluon plasmaHigh Energy Physics::ExperimentGravitational singularityQuantum field theoryEngineering (miscellaneous)Zeitschrift f�r Physik C Particles and Fields
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Inclusive D* production in gamma-gamma collisions: including the single-resolved contribution with massive quarks

2003

We have calculated the next-to-leading order cross section for the inclusive production of charm quarks as a function of the transverse momentum p_T and the rapidity in two approaches using massive or massless charm quarks. For the single-resolved cross section we have derived the massless limit from the massive theory. We find that this limit differs from the genuine massless version with MS-bar factorization by finite corrections. By adjusting subtraction terms we establish a massive theory with MS-bar subtraction which approaches the massless theory very fast with increasing transverse momentum. With these results and including the equivalent results for the direct cross section obtained…

QuarkPhysicsAlephParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyFOS: Physical sciencesGamma gammaCharm quarkMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationTransverse momentumRapidityHigh Energy Physics::ExperimentEngineering (miscellaneous)
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Reconciling open charm production at the Fermilab Tevatron with QCD

2005

We study the inclusive hadrodroduction of D^0, D^+, D^{*+}, and D_s^+ mesons at next-to-leading order in the parton model of quantum chromodynamics endowed with universal non-perturbative fragmentation functions (FFs) fitted to e^+e^- annihilation data from CERN LEP1. Working in the general-mass variable-flavor-number scheme, we resum the large logarithms through the evolution of the FFs and, at the same time, retain the full dependence on the charm-quark mass without additional theoretical assumptions. In this way, the cross section distributions in transverse momentum recently measured by the CDF Collaboration in run II at the Fermilab Tevatron are described within errors.

Quarkperturbation theory [quantum chromodynamics]Particle physicsMesoninclusive reaction [anti-p p]High Energy Physics::LatticeTevatronhadroproduction [charmed meson]General Physics and AstronomyFOS: Physical sciencesPartontransverse momentum [differential cross section]High Energy Physics - ExperimentNuclear physicsDGLAP equationHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Factorizationddc:550Fermilabnumerical calculationsNuclear ExperimentCDF [interpretation of experiments]PhysicsQuantum chromodynamicsAnnihilation1960 GeV-cmsHigh Energy Physics::PhenomenologyD*(2010)nonperturbative [fragmentation function]parton [model]D0High Energy Physics - PhenomenologyD+charm [mass]High Energy Physics::Experiment
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b-Hadron production in the general-mass variable-flavour-number scheme and LHC data

2018

We study inclusive b-hadron production in pp collisions at the LHC at different center-of-mass energies and compare with experimental data from the LHCb and CMS collaborations. Our predictions for cross sections differential in the transverse momentum and (pseudo-)rapidity agree with data within uncertainties due to renormalization scale variations. A small tension is found if data and theory predictions are compared for cross section ratios at different center-of-mass energies.

PhysicsParticle physicsLarge Hadron ColliderScale (ratio)010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsHadronFOS: Physical sciencesExperimental data01 natural sciencesRenormalizationVariable (computer science)Cross section (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Rapidity010306 general physics
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Inclusive D* Production in Photon-Photon Collisions at Next-to-Leading Order QCD

2001

The next-to-leading order cross section for the inclusive production of charm quarks in gamma-gamma collisions is calculated as a function of the transverse momentum pT and the rapidity y in approaches using massive or massless charm quarks. For the direct cross section we derive the massless limit from the massive theory with the result that this limit differs from the massless version with MSbar factorization by finite corrections. Subtracting or adding these corrections allows us to compare the two approaches on equal footing. We establish massless and massive versions with 3 and 4 initial flavours which are shown to approach the massless approximations very fast with increasing pT. With…

Quantum chromodynamicsPhysicsParticle physicsPhotonPhysics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyFOS: Physical sciencesCharm quarkMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationTransverse momentumRapidityHigh Energy Physics::ExperimentEngineering (miscellaneous)
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Open charm hadroproduction and the charm content of the proton

2009

We advocate charmed-hadron inclusive hadroproduction as a laboratory to probe intrinsic charm (IC) inside the colliding hadrons. Working at next-to-leading order in the general-mass variable-flavor-number scheme endowed with non-perturbative fragmentation functions recently extracted from a global fit to e^+e^- annihilation data from KEKB, CESR, and LEP1, we first assess the sensitivity of Tevatron data of D^0, D^+, and D^{*+} inclusive production to the IC parameterizations provided by Pumplin et al. We then argue that similar data from pp collisions at RHIC would have the potential to discriminate between different IC models provided they reach out to sufficiently large values of transver…

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilation010308 nuclear & particles physicsHadronHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciences01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyKEKBHigh Energy Physics - Phenomenology (hep-ph)[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]0103 physical sciencesTransverse momentumHigh Energy Physics::ExperimentOpen charm010306 general physicsNuclear Experiment12.38.Bx 13.85.Ni 13.87.Fh 14.40.Nd
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Λc± production in pp collisions with a new fragmentation function

2020

We study inclusive ${\mathrm{\ensuremath{\Lambda}}}_{c}^{\ifmmode\pm\else\textpm\fi{}}$-baryon production in $pp$ collisions in the general-mass variable-flavor-number scheme and compare with data from the LHCb, ALICE, and CMS collaborations. We perform a new fit of the $c\ensuremath{\rightarrow}{\mathrm{\ensuremath{\Lambda}}}_{c}^{+}$ fragmentation function combining ${e}^{+}{e}^{\ensuremath{-}}$ data from OPAL and Belle. The agreement with LHC data is slightly worse compared with a calculation using an older fragmentation function, and the tension between different determinations of ${\mathrm{\ensuremath{\Lambda}}}_{c}^{\ifmmode\pm\else\textpm\fi{}}$ production cross sections from the LHC…

PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::Phenomenology0103 physical sciencesFragmentation functionHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsLambda01 natural sciencesSlightly worsePhysical Review D
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