Accessing the gluon Wigner distribution in ep and pA collisions

Slides:



Advertisements
Similar presentations
December 17, 2004 JLab Hall A Upgrade 1 Semi-Inclusive DIS --opportunities at JLab upgrade Feng Yuan RBRC, Brookhaven National Laboratory.
Advertisements

Cédric Lorcé IPN Orsay - LPT Orsay Observability of the different proton spin decompositions June , University of Glasgow, UK CLAS12 3rd European.
Eccentricity and v2 in proton-proton collisions at the LHC
Constraining the polarized gluon PDF in polarized pp collisions at RHIC Frank Ellinghaus University of Colorado (for the PHENIX and STAR Collaborations)
Xiangdong Ji University of Maryland/SJTU Physics of gluon polarization Jlab, May 9, 2013.
Working Group on e-p Physics A. Bruell, E. Sichtermann, W. Vogelsang, C. Weiss Antje Bruell, JLab EIC meeting, Stony Brook, Dec Physics Topics Working.
Xiangdong Ji University of Maryland/SJTU
9/19/20151 Nucleon Spin: Final Solution at the EIC Feng Yuan Lawrence Berkeley National Laboratory.
9/19/20151 Semi-inclusive DIS: factorization Feng Yuan Lawrence Berkeley National Laboratory RBRC, Brookhaven National Laboratory.
THE DEEP INELASTIC SCATTERING ON THE POLARIZED NUCLEONS AT EIC E.S.Timoshin, S.I.Timoshin.
Future Opportunities at an Electron-Ion Collider Oleg Eyser Brookhaven National Laboratory.
Quark Helicity Distribution at large-x Collaborators: H. Avakian, S. Brodsky, A. Deur, arXiv: [hep-ph] Feng Yuan Lawrence Berkeley National Laboratory.
Columbia University Christine Aidala September 4, 2004 Solving the Proton Spin Crisis at ISSP, Erice.
6/1/20161 TMD Evolution Feng Yuan Lawrence Berkeley National Laboratory.
Cédric Lorcé IFPA Liège Multidimensional pictures of the nucleon (3/3) June 30-July 4, 2014, LPT, Paris-Sud University, Orsay, France Second International.
12/13/20151 Transverse Spin Overview: Theory Perspective Feng Yuan Lawrence Berkeley National Laboratory RBRC, Brookhaven National Laboratory.
Generalized TMDs of the Proton Barbara Pasquini Pavia U. & INFN, Pavia in collaboration with Cédric Lorcé Mainz U. & INFN, Pavia.
The Quark Structure of the Nucleon Inti Lehmann & Ralf Kaiser University of Glasgow Cosener’s House Meeting 23/05/2007 Nucleon Structure Generalised Parton.
Measurements with Polarized Hadrons T.-A. Shibata Tokyo Institute of Technology Aug 15, 2003 Lepton-Photon 2003.
Measurement of Flavor Separated Quark Polarizations at HERMES Polina Kravchenko (DESY) for the collaboration  Motivation of this work  HERMES experiment.
Cédric Lorcé IPN Orsay - LPT Orsay Introduction to the GTMDs and the Wigner distributions June , Palace Hotel, Como, Italy.
Wigner distributions and quark orbital angular momentum Cédric Lorcé and May , JLab, Newport News, VA, USA.
Single spin asymmetries in pp scattering Piet Mulders Trento July 2-6, 2006 _.
Distribution of linearly polarized gluons inside a large nucleus Jian Zhou Regensburg University Based on: Phys.Rev. D84 (2011) A. Metz and ZJ.
3/8/20161 Nucleon Tomography --Parton Imaging in 3D Feng Yuan Lawrence Berkeley National Laboratory.
Nucleon spin decomposition at twist-three Yoshitaka Hatta (Yukawa inst., Kyoto U.) TexPoint fonts used in EMF. Read the TexPoint manual before you delete.
Transverse Spin Physics with an Electron Ion Collider Oleg Eyser 4 th International Workshop on Transverse Polarisation Phenomena in Hard Processes Chia,
Inclusive diffraction in DIS and the dipole picture Cyrille Marquet RIKEN BNL Research Center arXiv:
6/28/20161 Future Challenges of Spin Physics Feng Yuan Lawrence Berkeley National Laboratory.
Proton spin structure in phase-space May 17, FSU Alumni Center, Tallahassee, Florida, USA Cédric Lorcé CPhT Baryons May 2016 Florida State University.
Xiangdong Ji U. Maryland/ 上海交通大学 Recent progress in understanding the spin structure of the nucleon RIKEN, July 29, 2013 PHENIX Workshop on Physics Prospects.
A sideways look into the proton Transverse momentum and transverse spin in QCD Alessandro Bacchetta.
Renormalization Group Evolution of Multi-gluon Correlators in High Energy QCD Jamal Jalilian-Marian Baruch College QCD Evolution Workshop 2012, JLAB.
Transversely Polarized Neutron DVCS with SoLID-SIDIS Setup Zhihong Ye Duke University 05/15/2015, SoLID Collaobration Meeting.
Timelike Compton Scattering at JLab
Gluon orbital angular momentum in the nucleon
Nucleon spin decomposition
Quantum imaging of the proton via Wigner distributions
Sep 21st 2015, INFN Frascati National Laboratories, Frascati, Italy
June 28, Temple University, Philadelphia, USA
June , Dipartimento di Fisica, Universita’ di Pavia, Italy
ShanDong University Jian Zhou
Centre de Physique Théorique
May , JLab, Newport News, VA, USA
Probing the gluon Wigner distribution in diffractive dijet production
Wigner, Husimi and GTMD at small-x
Computing gluon TMDs at small-x in the Color Glass Condensate
Physics of the EIC Cyrille Marquet Theory Division - CERN.
Measurements of quark transversity and orbital motion in hard scattering Yoshiyuki Miyachi Tokyo Institute of Technology.
Groupement de Recherche (GDR) QCD
Physics with Nuclei at an Electron-Ion Collider
Low-x gluon TMDs, the dipole picture and diffraction
3/19/20181 Nucleon Spin: Final Solution at the EIC Feng Yuan Lawrence Berkeley National Laboratory.
Semi-inclusive DIS at Small-x
Quark’s angular momentum densities in position space
August 29, Riken Tokyo Office, Tokyo, Japan
Beam Spin Asymmetry Measurements from Deeply Virtual Meson Production
September 29th, IPNO, Orsay
Transverse Momentum Dependent Parton Distributions
Unique Description for SSAs in DIS and Hadronic Collisions
Selected Physics Topics at the Electron-Ion-Collider
Computing gluon TMDs at small-x in the Color Glass Condensate
PHENIX Transverse-Spin Physics
Forward spin + cold nuclear measurements and forward Calorimetry
Feng Yuan Lawrence Berkeley National Laboratory
TMDs in nuclei Jian Zhou Temple University
高能物理学会第八届全国会员代表大会暨学术年会
Unique Description for Single Transverse Spin Asymmetries
Single Spin Asymmetry with a Transversely Polarized
Single spin asymmetries in semi-inclusive DIS
Presentation transcript:

Accessing the gluon Wigner distribution in ep and pA collisions Yoshitaka Hatta (Yukawa inst. Kyoto U.) YH, B. Xiao, F. Yuan, PRL116 (2016) 202301 Y. Hagiwara, YH, R. Pasechnik, M. Tasevsky, O. Teryaev, PRD96 (2017) 034009

Contents Introduction: Phase space distributions in QCD Wigner distribution at small-x Diffractive dijet production in ep and pA.

Nucleon tomography

1D tomography: Parton distribution function (PDF) Probability distribution of quarks and gluons with longitudinal momentum fraction The nucleon is much more complicated! Partons also have transverse momentum and are spread in impact parameter space

3D tomography: Transverse momentum dependent distributions (TMD) Relevant in semi-inclusive DIS (SIDIS), etc.

3D tomography: Generalized parton distributions (GPD) distribution of partons in impact parameter space Fourier transform Deeply Virtual Compton Scattering (DVCS)

5D tomography: Wigner distribution— the “mother distribution” Belitsky, Ji, Yuan (2003); Lorce, Pasquini (2011) TMD GPD PDF Form factor charge

5D tomography: Generalized TMD and Husimi GTMD Husimi Meissner, Metz, Schlegel (2009) Hagiwara, YH (2015) Gaussian smearing in k, b Probabilistic interpretation! PDF Form factor charge TMD GPD

Wigner distribution and orbital angular momentum Nucleon spin decomposition Quarks’ helicity Gluons’ helicity Canonical Orbital angular momentum Lorce, Pasquini, (2011); YH (2011)

Electron-Ion Collider (EIC)  Abhay’s talk A future (2025~), high-luminosity  experiment dedicated to the study of nucleon structure. arXiv:1212.1701

Wigner distribution: Is it measurable? In quantum optics, yes! What about in QCD? Go to small-x!

Gluon Wigner distribution There are two ways to make it gauge invariant Dominguez, Marquet, Xiao, Yuan (2011) Dipole distribution Weizsacker-Williams distribution

Dipole gluon Wigner distribution at small-x YH, Xiao, Yuan (2016) Approximate ``Dipole S-matrix” correlation expected ``Elliptic Wigner” ``OAM Wigner”

Gluon Wigner from Balitsky-Kovchegov equation Hagiwara, YH, Ueda (2016) Peak at the saturation momentum Small in magnitude (a few percent effect) Distinct functional dependence on

Elliptic Wigner in DVCS YH, Xiao, Yuan (2017) Gluon transversity GPD Elliptic Wigner (GTMD)

Elliptic Wigner in high-multiplicity pp and pA Hagiwara, YH, Xiao, Yuan (2017) see also, Kopeliovich et al. (2008), Levin Rezaeian (2011),.. Elliptic flow observed in high-multiplicity pp and pA. Initial state or final state effect? 1509.04776 Double parton scattering + Elliptic Wigner = Elliptic flow

Direct measurement of the Wigner distribution Find a process sensitive to both and …. Nontrivial! cf. Vector meson production One can study the dependence on Munier, Stasto, Mueller, 2001 but not on

Probing Wigner (GTMD) in exclusive diffractive dijet in ep YH, Xiao, Yuan (2016), see also Altinoluk, Armesto, Beuf, Rezaeian (2015) NLO calculation by Boussarie et al. (2016) Jet 1 Jet 2 𝑒 − Proportional to GTMD

Ultra-peripheral pA collisions! Hagiwara, YH, Pasechnik, Tasevsky, Teryaev, (2017) preferably small Use the Weiszacker-Williams photons in UPC! YH, Xiao, Yuan (2016) photon flux

Analytically invert these relations to get GTMD BK model MV model Can be done also for UPC in AA collisions

Nucleon spin puzzle and small-x Nonzero contribution from `large’-x region de Florian, Sassot, Stratmann,Vogelsang (2014) Huge uncertainty in from the small-x region. Maybe after including the small-x contribution. OAM not needed? Δ𝐺

- Longitudinal single spin asymmetry in diffractive dijet 2 2 YH, Nakagawa, Xiao, Yuan, Zhao (2016) 2 2 - ‘Odderon’ at small-x !?

Conclusions Physics of nucleon structure has literally expanded its dimensions, from 1D (PDF) to 3D (GPD/TMD) and 5D (Wigher/Husimi/GTMD). Exciting times ahead at the future EIC. First ideas to measure 5D gluon distributions: Diffractive dijet events in ep (photoproduction) and pA (UPC). Look for      and angular dependences. Extension to spin-dependent part (OAM), moderate-x, quark Wigner. YH, Nakagawa, Xiao, Yuan, Zhao (2017) Ji, Yuan, Zhao (2017) Bhattacharya, Metz, Zhou (2017)

Homodyne Detection Two electromagnetic fields are incident on a beam splitter Photon count difference at detectors C and D : Probability distribution of (coherent state with phase ) c.f. Reconstruct via the inverse Radon transformation