Production and hadronization of heavy quarks
E Norrbin, T Sjöstrand - The European Physical Journal C-Particles and …, 2000 - Springer
Heavy long-lived quarks, ie charm and bottom, are frequently studied both as tests of QCD
and as probes for other physics aspects within and beyond the standard model. The long …
and as probes for other physics aspects within and beyond the standard model. The long …
Toward the global fit of the TMD gluon density in the proton from the LHC data
AV Lipatov, GI Lykasov, MA Malyshev - Physical Review D, 2023 - APS
We propose a new analytical expression for the transverse-momentum-dependent (TMD, or
unintegrated) gluon density in the proton. Essential phenomenological parameters are …
unintegrated) gluon density in the proton. Essential phenomenological parameters are …
[HTML][HTML] Self-consistent description of HERA data at low Q2 and soft hadron production at LHC
AV Lipatov, GI Lykasov, MA Malyshev - Physics Letters B, 2024 - Elsevier
Using the analytical expression for transverse momentum dependent (TMD) gluon density in
a proton, a self-consistent simultaneous description of low Q 2 data on proton structure …
a proton, a self-consistent simultaneous description of low Q 2 data on proton structure …
Production mechanisms of charm hadrons in the string model
E Norrbin, T Sjöstrand - Physics Letters B, 1998 - Elsevier
In the hadroproduction of charm in the context of string fragmentation, the pull of a beam
remnant at the other end of a string may give a charm hadron more energy than the …
remnant at the other end of a string may give a charm hadron more energy than the …
An interpolating mass formula and Regge trajectories for light and heavy quarkonia
MN Sergeenko - Zeitschrift für Physik C Particles and Fields, 1994 - Springer
Simple interpolating formula for the square of the quarkonium mass and an analytic
expression for the Regge trajectories α (t) in a whole region of both light and heavy …
expression for the Regge trajectories α (t) in a whole region of both light and heavy …
Exclusive charm production in collisions at GeV
AI Titov, B Kämpfer - Physical Review C—Nuclear Physics, 2008 - APS
We discuss the open charm production in the peripheral reactions p¯ p→ Y¯ c Y c and p¯
p→ M c M¯ c, where Y c and M c stand for Λ c+, Σ c+ and D, D*, respectively, at s≲ 15 GeV …
p→ M c M¯ c, where Y c and M c stand for Λ c+, Σ c+ and D, D*, respectively, at s≲ 15 GeV …
Role of gluons in soft and semi-hard multiple hadron production in pp collisions at LHC
VA Bednyakov, AA Grinyuk, GI Lykasov… - International Journal of …, 2012 - World Scientific
Hadron inclusive spectra in pp collisions are analyzed within the modified quark–gluon
string model including both the longitudinal and transverse motion of quarks in the proton in …
string model including both the longitudinal and transverse motion of quarks in the proton in …
Transition between soft physics at the LHC and low- physics at HERA
AA Grinyuk, AV Lipatov, GI Lykasov, NP Zotov - Physical Review D—Particles …, 2013 - APS
We find out the connection between the unintegrated gluon distribution at low intrinsic
transverse momenta and the inclusive spectrum of the hadrons produced in pp collision at …
transverse momenta and the inclusive spectrum of the hadrons produced in pp collision at …
Employing RHIC and LHC data to determine the transverse momentum dependent gluon density in a proton
NA Abdulov, H Jung, AV Lipatov, GI Lykasov… - Physical Review D, 2018 - APS
Transverse momentum dependent (TMD) parton distributions in a proton are important in
high-energy physics from both theoretical and phenomenological points of view. Using the …
high-energy physics from both theoretical and phenomenological points of view. Using the …
Prompt fluxes in present and future neutrino experiments
MC Gonzalez-Garcia, JJ Gomez-Cadenas - Physical Review D, 1997 - APS
We use a nonperturbative QCD approach, the quark-gluon string model, to compute the τ-
neutrino fluxes produced by fixed target pA collisions (where A is a target material) for …
neutrino fluxes produced by fixed target pA collisions (where A is a target material) for …