Tomasz Stebel (with Leszek Motyka and Mariusz Sadzikowski) M. Smoluchowski Institute of Physics, Jagiellonian University.

Slides:



Advertisements
Similar presentations
Triumvirate of Running Couplings in Small-x Evolution Yuri Kovchegov The Ohio State University Based on work done in collaboration with Heribert Weigert,
Advertisements

Small-x Physics in DIS Small-x Physics in DIS Yuri Kovchegov The Ohio State University.
Running Coupling in Small-x Evolution Yuri Kovchegov The Ohio State University Based on work done in collaboration with Heribert Weigert, hep-ph/
Neutrino Nucleon Cross Sections: GeV to ZeV Hallsie Reno University of Iowa January 2009.
Introduction to the Physics of Saturation Introduction to the Physics of Saturation Yuri Kovchegov The Ohio State University.
SSAs at small x and the the anomalous magnetic moment Jian Zhou Regensburg University Based on: Phys.Rev. D89 (2014) ZJ arXiV: A. Schafer.
What is the twist of TMDs? Como, June 12, 2013 Oleg Teryaev JINR, Dubna.
Overview of saturation Yoshitaka Hatta (Saclay) Low-x meeting, 2007, Helsinki.
1 QCD evolution equations at small x (A simple physical picture) Wei Zhu East China Normal University KITPC A simple physical picture.
1 TMDs, offering opportunities at small k T and small x! Piet Mulders Annual Meeting of the GDR PH-QCD (December 15-17, 2014) Ecole Polytechnique,
1 Color Entanglement and Universality of TMDs Piet Mulders POETIC V – International Workshop on Physics Opportunities at an ElecTron-Ion.
Mary Hall Reno High Energy Neutrino Cross Sections Neutrino 2004, 18 June 2004.
Mini review on saturation and recent developements Cyrille Marquet Service de Physique Théorique - CEA/Saclay ICHEP 2006, Moscow, Russia.
Drell-Yan Di-Lepton Production Why Drell-Yan? Asymmetries depend on PD only (SIDIS→convolution with QFF) Why ? Each valence quark can contribuite to the.
Understanding forward particle production Opportunities for Drell-Yan Physics at RHIC May 13 th, 2011 Roman Pasechnik Uppsala University, THEP group 1.
1 Antishadowing effect in the unitarized BFKL equation Jianhong Ruan, Zhenqi Shen, Jifeng Yang and Wei Zhu East China Normal University.
1 Why GLR-MQ-ZRS equation is necessary for understanding STAR BES program? Wei Zhu East China Normal University KITPC
Mary Hall Reno Neutrino Cross Sections at HERA and Beyond ISVHECRI September 10, 2004.
DIS’03 St.Petersburg April 23-27, 2003 V. Fadin Institute of Nuclear Physics, Novosibirsk WGA Theory Low x BFKL and DGLAP BK Structure functions Diffraction.
1 Diffractive heavy quark production in AA collisions at the LHC at NLO* Mairon Melo Machado GFPAE – IF – UFRGS
TMDs of a Large Nucleus: Quasi-Classical Approximation and Quantum Evolution Yuri Kovchegov The Ohio State University based on work with Matt Sievert.
Distribution of linearly polarized gluons inside a large nucleus Jian Zhou Regensburg University Based on: Phys.Rev. D84 (2011) A. Metz and ZJ.
Azimuthal Asymmetry In The Unpolarized Drell-Yan Process Zhou Jian ShanDong University, China & LBNL, US Collaborators: Feng Yuan (LBNL, US) Zuo-tang Liang.
UINTEGRATED GLUON DISTRIBUTION AND UINTEGRATED GLUON DISTRIBUTION AND SATURATION EFFECT IN P-P AT LHC SATURATION EFFECT IN P-P AT LHC AT AT MPI-2012, CERN,
1 Azimuthal quadrupole correlation from gluon interference in 200 GeV and 7 TeV p+p collisions Lanny Ray – University of Texas at Austin The 2 nd International.
1 Antishadowing effect in the unitarized BFKL equation Jianhong Ruan, Zhenqi Shen, Jifeng Yang and Wei Zhu East China Normal University Nuclear Physics.
Solution of the NLO BFKL Equation (and a strategy for solving the all-order BFKL equation) Yuri Kovchegov The Ohio State University based on arXiv:
Testing BFKL evolution with Mueller-Navelet jets
A T : novel variable to study low transverse momentum vector boson production at hadron colliders. Rosa María Durán Delgado The University of Manchester.
Single-Transverse Spin Asymmetries in Hadronic Scattering
Diffractive production of cc(0,1,2) mesons at LHC, Tevatron and RHIC
ShanDong University Jian Zhou
Dr. Terrance Figy Assistant Professor
Small-x and Diffraction in DIS at HERA I Henri Kowalski DESY 12th CTEQ Summer School Madison - Wisconsin June 2004.
Computing gluon TMDs at small-x in the Color Glass Condensate
Prompt Photons at ATLAS
Lecture 2 Evolution and resummation
Cyrille Marquet Centre de Physique Théorique Ecole Polytechnique
Cyrille Marquet Centre de Physique Théorique
New processes? New ideas
Low-x gluon TMDs, the dipole picture and diffraction
Villa Olmo (Como), 7−10th. September 2005
Physics with polarized antiprotons at GSI-PAX
The Tevatron Connection
Running coupling corrections to inclusive gluon production
Semi-inclusive DIS at Small-x
JSA/HUGS Fellowship Seminar-2016
Can We Learn Quark Orbital Motion from SSAs?
Unique Description for SSAs in DIS and Hadronic Collisions
Computing gluon TMDs at small-x in the Color Glass Condensate
past and future experiments
past and future experiments
Feng Yuan Lawrence Berkeley National Laboratory
Daniel A. Pitonyak Department of Physics, Temple University
Quark and Gluon Sivers Functions
Electron ion collisions and the Color Glass Condensate
Unique Description for Single Transverse Spin Asymmetries
PROTON STRUCTURE AND HARD P-P PROCESSES
Bs → PV decays and effects of next-to-leading order contributions in the perturbative QCD factorization approach Da-cheng Yan Ping Yang, Xin Liu, Zhen-Jun.
Spin effects and partonic intrinsic k┴
Singluarity and Gauge Link in Light Cone Gauge
Unifying the Mechanisms for SSAs in Hard Process
A QCD evolution equation and
Spin Studies via Drell-Yan Process at PANDA
Introduction to Monte Carlo Event Generators
Sangem Rajesh in collaboration with Asmita Mukherjee IIT Bombay, India
Y.Kitadono (Hiroshima ),
Azimuthal dependence in unpolarized proton-induced Drell-Yan processes
Angular Distribution in Unpolarized Proton-induced Drell-Yan Process
BFKL and High Energy Phenomenology
Presentation transcript:

Tomasz Stebel (with Leszek Motyka and Mariusz Sadzikowski) M. Smoluchowski Institute of Physics, Jagiellonian University

2

3 ATLAS, arXiv:

4 Phys. Rev. D 21 (1980) 2712 It is valid up to NLO, at the leading twist. Checked for the DY dipole model approach Motyka, Sadzikowski, TS, JHEP 1505 (2015) 087 NNLO corrections L-T rel. breaking Mirkes and Ohnemus, Phys. Rev. D 51, 4891 (1995). Boer, Phys. Rev. D 60, (1999) Boer and Mulders, Phys. Rev. D 57, 5780 (1998) Peng, Chang, McClellan, Teryaev, Phys.Lett. B758 (2016)

Recent ATLAS analysis for 8 TeV 5 JHEP 1608 (2016) 159, arXiv:

Parton shower: 6

7 Gribov Balitsky, Fadin, Kuraev, Lipatov, Levin, Ryskin Catani, Ciafaloni, Collins, Ellis kT approach in DY: Brodsky, Habecker, Quack Kopeliovich Nefedov, Nikolaev, Saleev Baranov, Lipatov, Zotov

Following: Nefedov, Nikolaev, Saleev; Phys.Rev. D87 (2013) no.1, ; arXiv: Quark Parton Reggeization Approach Gluon Transverse- momentum-dependent distribution (TDM) Hautmann, Hentschinski, Jung, arXiv:

9 Gluon TDM: Jung, Hautmann, arXiv:

Two channels: 2 diagrams Approximate NNLO = no gluon emission included Brodsky, Arthur Hebecker, E. Quack; Phys.Rev. D55 (1997) Schäfer, Szczurek, Phys.Rev. D93 (2016) no.7, diagrams NEW 10

 Jung, Hautmann (JH)  LO BFKL solution for TMD (with GBW initial condition): 11 arXiv: Mellin tr.  Weisacker–Williams-type gluon:

12

13 WWJH BFKL

14

15

 ATLAS data for 7 TeV, small dilepton mass (photon mediated). 16 arXiv: Martin, Ryskin, Watt, Phys. Rev. D 70, (2004); Lipatov, Malyshev, Zotov, JHEP 1112, 117 (2011).

15