0000000001210106

AUTHOR

H. Spiesberger

showing 18 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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$\Lambda_b^0$-baryon production in pp collisions in the general-mass variable-flavour-number scheme and comparison with CMS and LHCb data

2018

We calculate the next-to-leading-order cross section for the inclusive production of $\Lambda_b$ baryons in pp collisions in the general-mass variable-flavor-number scheme. We use realistic evolved non-perturbative fragmentation functions obtained from fits to B-meson production in $e^+ e^-$ annihilation and compare our results for transverse-momentum and rapidity distributions with recent experimental data from the CMS and the LHCb collaborations at the CERN LHC. We find satisfactory agreement in general, with some indication for the need to modify the available fragmentation functions at larger values of the scale variable.

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationLarge Hadron Collider010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsFlavourHigh Energy Physics::PhenomenologyAstronomy and AstrophysicsLambda01 natural sciencesBaryonHigh Energy Physics - Phenomenology0103 physical sciencesTransverse momentumRapidityHigh Energy Physics::Experiment010306 general physicsNuclear ExperimentInstrumentation
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Running of the Charm-Quark Mass from HERA Deep-Inelastic Scattering Data

2017

Physics letters / B 775, 233 - 238 (2017). doi:10.1016/j.physletb.2017.11.002

Nuclear and High Energy PhysicsParticle physicsPhotonHigh Energy Physics::LatticeFOS: Physical sciencesContext (language use)53001 natural sciencesCharm quarkrenormalizationNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)deep inelastic scattering0103 physical sciencesddc:530Charm (quantum number)quantum chromodynamics: perturbation theory010306 general physicsPhysicsQuantum chromodynamics010308 nuclear & particles physicsScatteringPhysicsHigh Energy Physics::Phenomenologyhigher-order: 1charm: productionHERADeep inelastic scatteringlcsh:QC1-999quark: massHigh Energy Physics - PhenomenologyDESY HERA Storscale dependence[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]charmlcsh:Physics
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How strange is pion electroproduction?

2015

We consider pion production in parity-violating electron scattering (PVES) in the presence of nucleon strangeness in the framework of partial wave analysis with unitarity. Using the experimental bounds on the strange form factors obtained in elastic PVES, we study the sensitivity of the parity-violating asymmetry to strange nucleon form factors. For forward kinematics and electron energies above 1 GeV, we observe that this sensitivity may reach about 20\% in the threshold region. With parity-violating asymmetries being as large as tens p.p.m., this study suggests that threshold pion production in PVES can be used as a promising way to better constrain strangeness contributions. Using this m…

Nuclear and High Energy PhysicsParticle physicsProtonNuclear Theorymedia_common.quotation_subjectPartial wave analysisNuclear TheoryFOS: Physical sciencesStrangeness01 natural sciencesAsymmetryNuclear physicsNuclear Theory (nucl-th)PionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear Experimentmedia_commonPhysicsNeutral currentUnitarity010308 nuclear & particles physicslcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics::ExperimentNucleonlcsh:Physics
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Reduced uncertainty of the axial γZ-box diagram correction to the proton’s weak charge

2019

We present the fully up-to-date calculation of the γZ-box correction which needs to be taken into account to determine the weak mixing angle at low energies from parity-violating electron proton scattering. We make use of neutrino and antineutrino inclusive scattering data to predict the parity-violating structure function F3γZ by isospin symmetry. Our new analysis confirms previous results for the axial contribution to the γZ-box graph and reduces the uncertainty by a factor of 2. In addition, we note that the presence of parity-violating photon-hadron interactions induces an additional contribution via F3γγ. Using experimental and theoretical constraints on the nucleon anapole moment we a…

PhysicsParticle physics010308 nuclear & particles physicsScatteringStructure functionElectron01 natural sciencesGraphProton scatteringIsospin0103 physical sciencesNeutrino010306 general physicsNucleonPhysical Review
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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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D* Mesons in photoproduction at HERA

2009

Ringberg Workshop on New Trends in HERA Physics 2008, Ringberg Castle, Germany, 5 Oct 2008 - 10 Oct 2008; Nuclear physics <Amsterdam> / B / Proceedings supplements 191, 183 - 192 (2009). doi:10.1016/j.nuclphysbps.2009.03.125

PhysicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyHigh Energy Physics::Experimentddc:530HERANuclear Experiment530Atomic and Molecular Physics and Optics
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Tests of quark-hadron duality in tau-decays

2016

An exhaustive number of QCD finite energy sum rules for $\tau$-decay together with the latest updated ALEPH data is used to test the assumption of global duality. Typical checks are the absence of the dimension $d=2$ condensate, the equality of the gluon condensate extracted from vector or axial vector spectral functions, the Weinberg sum rules, the chiral condensates of dimensions $d=6$ and $d=8$, as well as the extraction of some low-energy parameters of chiral perturbation theory. Suitable pinched linear integration kernels are introduced in the sum rules in order to suppress potential quark-hadron duality violations and experimental errors. We find no compelling indications of duality v…

QuarkNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryHadronLinearity of integrationGeneral Physics and AstronomyDuality (optimization)FOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciences010306 general physicsPseudovectorPhysicsQuantum chromodynamics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyAstronomy and AstrophysicsGluon condensateHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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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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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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Quark–hadron duality: Pinched kernel approach

2016

Hadronic spectral functions measured by the ALEPH collaboration in the vector and axial-vector channels are used to study potential quark-hadron duality violations (DV). This is done entirely in the framework of pinched kernel finite energy sum rules (FESR), i.e. in a model independent fashion. The kinematical range of the ALEPH data is effectively extended up to $s = 10\; {\mbox{GeV}^2}$ by using an appropriate kernel, and assuming that in this region the spectral functions are given by perturbative QCD. Support for this assumption is obtained by using $e^+ e^-$ annihilation data in the vector channel. Results in both channels show a good saturation of the pinched FESR, without further nee…

High Energy Physics - TheoryQuarkNuclear and High Energy PhysicsParticle physicsAlephHadronFOS: Physical sciencesGeneral Physics and AstronomyDuality (optimization)01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)High Energy Physics - Lattice0103 physical sciences010306 general physicsPhysicsQCD sum rulesAnnihilation010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyPerturbative QCDAstronomy and AstrophysicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Kernel (statistics)High Energy Physics::ExperimentModern Physics Letters A
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Anomalous magnetic moment of the muon: A hybrid approach

2017

A new QCD sum rule determination of the leading order hadronic vacuum polarization contribution to the anomalous magnetic moment of the muon, $a_{\mu}^{\rm hvp}$, is proposed. This approach combines data on $e^{+}e^{-}$ annihilation into hadrons, perturbative QCD and lattice QCD results for the first derivative of the electromagnetic current correlator at zero momentum transfer, $\Pi_{\rm EM}^\prime(0)$. The idea is based on the observation that, in the relevant kinematic domain, the integration kernel $K(s)$, entering the formula relating $a_{\mu}^{\rm hvp}$ to $e^{+}e^{-}$ annihilation data, behaves like $1/s$ times a very smooth function of $s$, the squared energy. We find an expression …

PhysicsQuantum chromodynamicsParticle physicsMuonAnnihilationAnomalous magnetic dipole moment010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)Hadronhep-latFOS: Physical sciencesPerturbative QCDhep-phLattice QCD01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentSum rule in quantum mechanics010306 general physicsPhysical Review D
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Inclusive D-Meson Production at the LHC

2012

I present predictions for the inclusive production of $D$ mesons at the CERN LHC in the general-mass variable-flavor-number scheme at next-to-leading order. Numerical results are compared to data where available, and uncertainties to scale variations, parton distribution functions and charm mass are discussed. I point out that measurements at large rapidity have the potential to pin down models of intrinsic charm.

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CERN LHC Collmass [charm]PhysicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics::ExperimentNuclear Experimentdistribution function [parton]numerical calculationsinclusive production [D]1 [higher-order]
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The Large Hadron–Electron Collider at the HL-LHC

2021

The Large Hadron-Electron Collider (LHeC) is designed to move the field of deep inelastic scattering (DIS) to the energy and intensity frontier of particle physics. Exploiting energy-recovery technology, it collides a novel, intense electron beam with a proton or ion beam from the High-Luminosity Large Hadron Collider (HL-LHC). The accelerator and interaction region are designed for concurrent electron-proton and proton-proton operations. This report represents an update to the LHeC's conceptual design report (CDR), published in 2012. It comprises new results on the parton structure of the proton and heavier nuclei, QCD dynamics, and electroweak and top-quark physics. It is shown how the LH…

energy recoverylepton nucleus: scatteringparton: distribution functionhiukkasfysiikka7. Clean energy01 natural sciencesaccelerator physicsHigh Energy Physics - Phenomenology (hep-ph)HEAVY FLAVOR CONTRIBUTIONSenergy-recovery- linacNuclear Experimentcolliding beams [electron p]deep-inelastic scatteringtop and electroweak physicsnew physicsPhysicsSTRUCTURE-FUNCTION RATIOSMonte Carlo [numerical calculations]buildingsprimary [vertex]High Energy Physics - Phenomenologyelectron p: colliding beamskinematicsNuclear Physics - Theoryfinal state: hadronicp: distribution functionbeyond Standard Modelvertex: primarynumerical calculations: Monte Carlodistribution function [parton]High-lumiLHCSTRUCTURE-FUNCTION F-2(X[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]ion: beam[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciencesNuclear Theory (nucl-th)deep inelastic scatteringquantum chromodynamicsddc:530010306 general physicsdeep-inelastic scattering; high-lumi LHC; QCD; Higgs; top and electroweak physics; nuclear physics; beyond standard Model; energy-recovery- linac; accelerator physics010308 nuclear & particles physicshigh-lumi LHCresolutionscattering [electron p]structure function [nucleus]sensitivitybeam [electron]energy-recovery-linacHiggsacceptanceNuclear TheoryHIGH-ENERGY FACTORIZATIONdistribution function [p]density [parton]Higgs; High-lumi LHCHigh Energy Physics - Experimentdesign [detector]High Energy Physics - Experiment (hep-ex)electron: linear acceleratorelectron hadron: scatteringCERN LHC Coll: upgrade[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]scattering [electron hadron]FCCelectron: beamNuclear Experiment (nucl-ex)linear accelerator [electron]Nuclear ExperimentlatticesuperconductivityEnergy-recoverylinacBeyond Standard ModeNuclear physics; QCDelectron nucleus: colliding beamsparton: densitycolliding beams [electron nucleus]Particle Physics - ExperimentNUCLEON STRUCTURE FUNCTIONSNuclear and High Energy Physicsscattering [lepton nucleus]beam [ion]FOS: Physical sciencesnucleus: structure functionhadronic [final state]electron p: scatteringTRANSVERSE-MOMENTUM DEPENDENCEnuclear physics0103 physical sciencesNuclear Physics - Experimentstructureupgrade [CERN LHC Coll]detector: designParticle Physics - PhenomenologyDEEP-INELASTIC-SCATTERINGelectroweak interaction3-LOOP SPLITTING FUNCTIONSCLASSICAL RADIATION ZEROScalibrationAccelerators and Storage RingsQCDmagnethigh [current]13. Climate action[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]LHeCPhysics::Accelerator PhysicsJET CROSS-SECTIONSHigh Energy Physics::Experimentcurrent: highJournal of Physics G: Nuclear and Particle Physics
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Heavy flavour production at the LHC: Theoretical Aspects

2008

CERN-DESY workshop on "HERA and the LHC" DESY-PROC-2009-02; ISBN 978-3-935702-32-4; ISSN 1435-8077; International audience; A proper inclusion of heavy quark mass effects in Parton Distribution Function fits has proved crucial. We present a review these effects in DIS and their impact on global analyses and lay out all elements of a properly defined general mass variable flavor number scheme (GM VFNS) that are shared by all modern formulations of the problem. We also report about progress in a number of theoretical problems related to exclusive measurements of heavy flavors. These topics include fragmentation functions for charmed mesons including finite mass effects, fragmentation function…

High Energy Physics::Lattice[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::PhenomenologyHigh Energy Physics::ExperimentNuclear Experiment
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$\Lambda_c^{\pm}$ production in pp collisions with a new fragmentation function

2020

Physical review / D D 101(11), 114021 (2020). doi:10.1103/PhysRevD.101.114021

p p: scatteringLambda/c+: productiondata analysis methodPhysics::Instrumentation and Detectors14.40.NdBELLEannihilation [electron positron]electron positron: annihilationfragmentation [charm]530fragmentation functionquarkALICEfragmentationscattering [p p]ddc:530charm: fragmentationStrong InteractionsNuclear Experimentproduction [Lambda/c+]OPALCMSviolation [universality]High Energy Physics::PhenomenologytensionLHC-B12.39.StHigh Energy Physics - Phenomenology12.38.BxCERN LHC Coll[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experimentuniversality: violation13.85.Ni
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New Physics Constraints from Atomic Parity Violation in $^{133}$Cs

2021

Our improved calculation of the nuclear spin-independent parity violating electric dipole transition amplitude ($E1_{PV}$) for $6s ~ ^2S_{1/2} - 7s ~ ^2S_{1/2}$ in $^{133}$Cs in combination with the most accurate (0.3\%) measurement of this quantity yields a new value for the nuclear weak charge $Q_W=-73.71(26)_{ex} (23)_{th}$ against the Standard Model (SM) prediction $Q_W^{\text{SM}}=-73.23(1)$. The advances in our calculation of $E1_{PV}$ have been achieved by using a variant of the perturbed relativistic coupled-cluster theory which treats the contributions of the core, valence and excited states to $E1_{PV}$ on the same footing unlike the previous high precision calculations. Furthermo…

High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Atomic Physics (physics.atom-ph)FOS: Physical sciencesPhysics - Atomic Physics
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Study of heavy meson production in p-Pb collisions at $\sqrt{S}$=5.02 TeV in the general-mass variable-flavour-number scheme

2017

Nuclear physics / B 925, 415 - 430 (2017). doi:10.1016/j.nuclphysb.2017.10.016

CMSnucleusFOS: Physical sciencesinitial-state interaction530High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CERN LHC CollALICEproduction [bottom]heavy [meson]ddc:530High Energy Physics::Experimentcross section [p p]Nuclear Experimentnumerical calculationscharmproduction [meson]1 [higher-order]
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