Jean-Philippe Lansberg

ORCID: 0000-0003-2746-5986
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About
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Research Areas
  • Particle physics theoretical and experimental studies
  • High-Energy Particle Collisions Research
  • Quantum Chromodynamics and Particle Interactions
  • Particle Detector Development and Performance
  • Superconducting Materials and Applications
  • Particle Accelerators and Free-Electron Lasers
  • Atomic and Subatomic Physics Research
  • Cosmology and Gravitation Theories
  • Dark Matter and Cosmic Phenomena
  • Black Holes and Theoretical Physics
  • Pulsars and Gravitational Waves Research
  • Physics of Superconductivity and Magnetism
  • Advanced Data Storage Technologies
  • Crystallography and Radiation Phenomena
  • Advanced X-ray Imaging Techniques
  • Nuclear physics research studies
  • Scientific Research and Discoveries
  • Distributed and Parallel Computing Systems
  • Advanced Materials Characterization Techniques
  • Cold Atom Physics and Bose-Einstein Condensates
  • High-pressure geophysics and materials
  • Advanced Graph Neural Networks
  • Galaxies: Formation, Evolution, Phenomena
  • Quantum and Classical Electrodynamics
  • Twentieth Century Scientific Developments

Laboratoire de Physique des 2 Infinis Irène Joliot-Curie
2020-2025

Université Paris-Saclay
2015-2025

Centre National de la Recherche Scientifique
2015-2025

Warsaw University of Technology
2024

Institut National de Physique Nucléaire et de Physique des Particules
2012-2021

Institut de Physique
2012-2021

Université Paris-Sud
2005-2019

Centre de Gestion Scientifique
2019

European Organization for Nuclear Research
2016-2017

Council of Science Editors
2016

We provide a concise overview on transverse momentum dependent (TMD) parton distribution functions, their application to topical issues in high-energy physics phenomenology, and theoretical connections with QCD resummation, evolution factorization theorems. illustrate the use of TMDs via examples multi-scale problems hadronic collisions. These include q_T spectra Higgs vector bosons for low q_T, azimuthal correlations production multiple jets associated heavy at large jet masses. discuss...

10.5506/aphyspolb.46.2501 article EN Acta Physica Polonica B 2015-01-01

10.1016/j.physrep.2020.08.007 article EN publisher-specific-oa Physics Reports 2020-10-09

We update the theoretical predictions for direct Upsilon(nS) hadroproduction in framework of nonrelativistic QCD. show that next-to-leading order corrections alpha(S) to color-singlet transition significantly raise differential cross section at high p(T) and substantially affect polarization Upsilon. Motivated by remaining gap between yield cross-section measurements Fermilab Tevatron, we evaluate leading part alpha(S)(5) contributions, namely, those coming from associated with three light...

10.1103/physrevlett.101.152001 article EN Physical Review Letters 2008-10-08

10.1140/epjc/s10052-008-0826-9 article EN The European Physical Journal C 2008-12-18

We study the relevance of experimental data on heavy-flavor [${D}^{0}$, $J/\ensuremath{\psi}$, $B\ensuremath{\rightarrow}J/\ensuremath{\psi}$ and $\mathrm{\ensuremath{\Upsilon}}(1S)$ mesons] production in proton-lead collisions at LHC to improve our knowledge gluon-momentum distribution inside heavy nuclei. observe that nuclear effects encoded both most recent global fits parton densities next-to-leading order (nCTEQ15 EPPS16) provide a good overall description data. interpret this as hint...

10.1103/physrevlett.121.052004 article EN cc-by Physical Review Letters 2018-08-03

The future opportunities for high-density QCD studies with ion and proton beams at the LHC are presented. Four major scientific goals identified: characterisation of macroscopic long wavelength Quark-Gluon Plasma (QGP) properties unprecedented precision, investigation microscopic parton dynamics underlying QGP properties, development a unified picture particle production from small (pp) to large (nucleus--nucleus) systems, exploration densities in nuclei broad ($x$, $Q^2$) kinematic range...

10.2172/1501772 preprint EN 2019-03-15

We demonstrate that the recent studies of J/ψ-pair production by CMS at LHC and D0 Tevatron reveal presence different mechanisms in kinematical regions. find out next-to-leading-order single parton scattering contributions αs5 dominate yield large transverse momenta pair. Our analysis further emphasises importance double scatterings – which are expected to J/ψ-rapidity differences invariant masses pair acceptance, thereby solve a discrepancy between theory data. In addition, we provide first...

10.1016/j.physletb.2015.10.083 article EN cc-by Physics Letters B 2015-11-04

We argue that the study of heavy quarkonia, in particular $\mathrm{\ensuremath{\Upsilon}}$, produced back to with an isolated photon $pp$ collisions at LHC is best---and currently unique---way access distribution both transverse momentum and polarization gluon unpolarized proton. These encode fundamental information on dynamics QCD. derive analytical expressions for various transverse-momentum distributions can be measured which allow a direct extraction aforementioned quantities. To assess...

10.1103/physrevlett.112.212001 article EN Physical Review Letters 2014-05-27

We calculate the cross sections for direct hadroproduction of J/psi and Upsilon associated with a heavy-quark pair same flavour at leading order in alpha_S v NRQCD. These processes provide an interesting signature that could be studied Tevatron LHC also constitute gauge-invariant subset NLO corrections to inclusive Upsilon. find fragmentation approximation commonly used evaluate contribution these quarkonium production sizeably underestimates exact calculation kinematical region accessible...

10.1016/j.physletb.2007.04.031 article EN cc-by Physics Letters B 2007-04-25

We proceed for the first time to evaluation of Born cross section J / ψ + η(c) production, namely, via g → J/ψ+ g, and show that it has a harder P(T) spectrum than J/ψ-pair yield at level. If one stuck comparison level, would conclude production surpass large P(T). This is nonetheless not case since ψ-pair as single ψ, receives leading-P(T) contributions higher orders in α(s). also present these next-to-leading order contributions. These are indeed significant increasing essential relevance...

10.1103/physrevlett.111.122001 article EN Physical Review Letters 2013-09-20

We propose a simple and model-independent procedure to account for the impact of nuclear modification gluon density as encoded in collinear PDF sets on two-to-two partonic hard processes proton-nucleus collisions. This applies good approximation quarkonium, D B meson production, generically referred H. Our consists parametrising square parton scattering amplitude, A_{gg -> H X} constraining it from proton-proton data. Doing so, we have been able compute corresponding factors J/psi, Upsilon...

10.1140/epjc/s10052-016-4575-x article EN cc-by The European Physical Journal C 2016-12-27

We update our previous studies of nuclear-matter effects on J/Psi production in proton-nucleus for the recent LHC pPb runs at sqrt(s_NN)=5 TeV. have analysed modification gluon PDFs nucleus, using an exact kinematics a 2->2 process, namely g+g->J/Psi+g as expected from LO pQCD. This allows to constrain transverse-momentum while computing nuclear factor different rapidities, unlike with usual simplified kinematics. Owing absence measurement pp collisions same sqrt(s_NN) and owing significant...

10.1103/physrevc.88.047901 article EN Physical Review C 2013-10-09

The goal of this white paper is to give a comprehensive overview the rich field forward physics.We discuss occurrences BFKL re-summation effects in special final states, such as Mueller-Navelet jets, jet-gap-jets, and heavy quarkonium production.It further addresses TMD factorization at low x manifestation semi-hard saturation scale (generalized) PDFs.More theoretical aspects low-x physics, probes quark-gluon plasma, well possibility use photonhadron collisions LHC constrain hadronic...

10.5506/aphyspolb.54.3-a2 article EN Acta Physica Polonica B 2023-01-01

We update the study of total $\ensuremath{\psi}$ and $\ensuremath{\Upsilon}$ production cross section in proton-proton collisions at RHIC energies using QCD-based color-singlet model, including next-to-leading order partonic matrix elements. also include charm-quark initiated processes which appear leading ${\ensuremath{\alpha}}_{s}$, so far overlooked such studies. Contrary to earlier claims, we show that yield is consistent with measurements over a broad range $J/\ensuremath{\psi}$...

10.1103/physrevd.81.051502 article EN Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D, Particles, fields, gravitation, and cosmology 2010-03-11

Cold nuclear matter effects on J/psi production in proton-nucleus and nucleus-nucleus collisions are evaluated taking into account the specific kinematics at partonic level, shadowing of initial parton distributions absorption matter. We consider two different processes for c-cbar pair production: one with collinear gluons a recoiling gluon final state other carrying intrinsic transverse momentum. Our results compared to RHIC observables. The smaller values modification factor R_AA forward...

10.1016/j.physletb.2009.07.076 article EN cc-by Physics Letters B 2009-08-19

We show that the production of J/psi or Upsilon pairs in unpolarised pp collisions is currently best process to measure momentum-distribution linearly-polarised gluons inside protons through study azimuthal asymmetries. Not only short-distance coefficients for such reactions induce largest possible cos 4 phi modulations, but analysed data are already available. Among various final states previously studied within TMD factorisation approach, di-J/psi exhibits by far asymmetries, up 50% region...

10.1016/j.physletb.2018.08.004 article EN cc-by Physics Letters B 2018-08-06

We present predictions for double-quarkonium production in the kinematical region relevant proposed fixed-target experiment using LHC beams (dubbed as AFTER@LHC). These include all spin-triplet S -wave charmonium and bottomonium pairs, i.e. Psi(n_1S) + Psi(n_2S), Upsilon(m_1S) Upsilon(m_2S ) with n_1,n_2 = 1,2 m_1,m_2 1,2,3. calculate contributions from double-parton scatterings single-parton scatterings. With an integrated luminosity of 20 fb-1 to be collected at AFTER@LHC, we find that...

10.1016/j.nuclphysb.2015.09.005 article EN cc-by Nuclear Physics B 2015-09-24
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