Recent study on γγ*  ηc transition form factor and χcJ  γγ

Slides:



Advertisements
Similar presentations
Rumin Wang G. R.. Lu& Y. D. Yang Work done in collaboration with G. R.. Lu & Y. D. Yang Huazhong Normal University Henan Normal University November 15,
Advertisements

1.  Motivation  Theoretical framework  Perturbative QCD Approach  Numerical Results  Summary 2.
C.D. LuICFP31 Some progress in PQCD approach Cai-Dian Lü (IHEP, Beijing) Formalism of Perturbative QCD (PQCD) Direct CP asymmetry Polarization in B 
1 V cb : experimental and theoretical highlights Marina Artuso Syracuse University.
Iain Stewart MIT Iain Stewart MIT Nonleptonic Decays and the Soft Collinear Effective Theory Super B Factory Workshop, Hawaii, 2004.
From Factorization to Resummation for Single Top Production at the LHC with Effective Theory Chong Sheng Li ITP, Peking Unversity Based on the work with.
Method of Regions and Its Applications The Interdisciplinary Center for Theoretical Study, USTC 1 Graduate University of the CAS Deshan Yang.
Xiangdong Ji University of Maryland/SJTU Physics of gluon polarization Jlab, May 9, 2013.
Run-Hui Li Yonsei University Mainly based on R.H. Li, C.D. Lu, and W. Wang, PRD83:
International Conference on QCD and Hadronic Physics, Peking University Pion Electromagnetic Form Factor in the K T Factorization Formulae Xing-Gang.
J/ψ Production in pPb Collisions at the LHC Zhang, Hong-Fei Third Military Medical University.
Non-Relativistic Quantum Chromo Dynamics (NRQCD) Heavy quark systems as a test of non-perturbative effects in the Standard Model Victor Haverkort en Tom.
Breakdown of NRQCD Factorization ?? J. P. Ma Institute of Theoretical Physics, Beijing 北京 May Taipei Summer Institute on Strings, Particles.
1 Noncommutative QCDCorrections to the Gluonic Decays of Heavy Quarkonia Stefano Di Chiara A. Devoto, S. Di Chiara, W. W. Repko, Phys. Lett. B 588, 85.
P. Gubler, K. Morita, and M. Oka, Phys. Rev. Lett. 107, (2011) K. Suzuki, P. Gubler, K. Morita, and M. Oka, arxiv: [hep-th]
Some Issues in Charmonium Physics Some Issues in Charmonium Physics K-T Chao Peking University.
Dian-Yong Chen Institute of Modern Physics, CAS FHNP’15 Beijing Hadronic Loop Contributions to Heavy Quarkonium Decay
Hot quarkonium spectral functions from QCD sum rules and MEM Heavy quarks and quarkonia in thermal ECT*, Villazzano, Italy Philipp Gubler.
Precise α s from  Decays(*) M. Davier, S. Descotes-Genon, A. Hoecker, B. Malaescu, and Z. Zhang Tau08 Workshop Novosibirsk, Sept (*) arxiv: ;
June 25, 2004 Jianwei Qiu, ISU 1 Introduction to Heavy Quark Production Jianwei Qiu Iowa State University CTEQ Summer School on QCD Analysis and Phenomenology.
Inclusive four charm hadron production at Belle June 16-20, 2005 International Conference on QCD and Hadronic Physics, Beijing JUNGIL LEE.
Threshold Resummation for Top- Quark Pair Production at ILC J.P. Ma ITP, CAS, Beijing 2005 年直线对撞机国际研讨会, Tsinghua Univ.
Resummation of Large Endpoint Corrections to Color-Octet J/  Photoproduction Adam Leibovich University of Pittsburgh 10/17/07 With Sean Fleming and Thomas.
Double charm production in e + e - -annihilation Anatoly Likhoded, IHEP, Protvino The conflict between Theory and Experiment in double charmonium production.
Heavy hadron phenomenology on light front Zheng-Tao Wei Nankai University 年两岸粒子物理与宇宙学 研讨会,重庆, 5.7—5.12 。
Contents Introduction NLO Calculations Numerical Results Summary.
Learning  ( 0 ) from B decays Chuan-Hung Chen Department of Physics, National Cheng-Kung University, Tainan, Taiwan  Introduction & Our question  
Exclusive charmonium production in hard exclusive processes. V.V. Braguta Institute for High Energy Physics Protvino, Russia.
Inclusive Charm Production in Bottomonium Decays Yu, Chaehyun (Korea University) In collaboration with Hee Sok Chung, Daekyoung Kang, Taewon Kim, and Jungile.

Yan-Qing Ma ( 马滟青 ) Peking University The Second Sino-Americas Workshop and School on the Bound-State Problem in Continuum QCD, Central China Normal University,
Applications of the light-cone distribution amplitudes for quakonia 南昌大学 第八届全国高能物理大会 1 Based on Yu Jia & DSY, NPB814, 217 (2009); in preparation.
Convergence of chiral effective theory for nucleon magnetic moments P. Wang, D. B. Leinweber, A. W. Thomas, A. G. Williams and R. Young.
Paolo Gambino CKM 2006 Nagoya 1 The B  X s γ BF at NNLO Paolo Gambino Università di Torino.
QQ systems are ideal for strong interactions studies Scales and Effective Field Theories:systematic approach pNRQCD: the QQbar and QQQ potentials Applications.
Measurements of Heavy Quarkonium Production and Polarization at CMS Linlin ZHANG (张琳琳) and Sijin QIAN (钱思进) Peking University 中国物理学会 高能物理分会 2014 学术年会 武汉,湖北,
Refactorizing NRQCD short-distance coefficients in exclusive quarkonium production KITPC-EFT in Nuclear Physics & Particle Physics 1 Based on.
A T : novel variable to study low transverse momentum vector boson production at hadron colliders. Rosa María Durán Delgado The University of Manchester.
Low energy scattering and charmonium radiative decay from lattice QCD
seminar at Academia Sinica
Effects of charmed meson loops on charmonium transitions
Lattice College of William and Mary
Polarization in charmless B VV decays
Problems in Charmonium Production in e+e Annihilation and B Decay
Exotic States in QCD Sum Rules
A crisis of NRQCD in describing charmonium?
Unique Description for SSAs in DIS and Hadronic Collisions
Polarized Structure Function of Nucleon and Orbital Angular Momentum
R.R. Silva, M.E. Bracco, S.H. Lee, M. Nielsen
B physics at hadron collider
The Color Octet Effect from at B Factorry
Double charmonium production in e+e– annihilation
Revisiting some long-standing puzzles in charmonium decays
Nonleptonic Two Body Decays of Charmed Mesons
Heavy-to-light transitions on the light cone
Towards Understanding the In-medium φ Meson with Finite Momentum
Improved alpha_s from Tau Decays(*)
Pseudoscalar Quarkonium Exclusive Decays to Vector Meson Pair Cong-Feng Qiao Graduate.
Inclusive decays at order v7
in the Rein-Sehgal Model
Productions and Decays of Charmonium Application of perturbative QCD
Spin-singlet Quarkonia at the LHC
Charmonium Decays at BESIII
Associated production of Higgs boson with μ+μ - at CEPC
Pion transition form factor in the light front quark model
Factorization in some exclusive B meson decays
Calculation of Pure Annihilation Type B Decay in PQCD Approach
Y.Kitadono (Hiroshima ),
Run-Hui Li Yonsei University
Lifetime of doubly charmed baryons
Presentation transcript:

Recent study on γγ*  ηc transition form factor and χcJ  γγ 桑 文 龙 SouthWest University, ChongQing In collaboration with Feng Feng, Yu Jia, Shuang-Ran Liang QCD Study Group 2016 workshop 2016.4.2-2016.4.4 上海交大 (SJTU)

Contents Brief introduction to NRQCD factorization NNLO QCD correction to γγ*  ηc form factor and confront the BaBar data NNLO QCD correction to χcJ  γγ and confront the BESIII data Summaries

Nonrelativistic QCD (NRQCD): the modern effective field theory to tackle heavy quarkonium Caswell, Lepage (1986); Bodwin, Braaten, Lepage (1995) This scale separation is usually referred to as NRQCD factorization. The NRQCD short-dist. coefficients can be computed in perturbation theory, order by order

production at hadron colliders …… NRQCD gains popularity in quarkonium physics (see Brambilla et al. EPJC 2011 for a recent review) Nowadays, NRQCD becomes an important approach to tackle various quarkonium production and decay processes charmonium: bottomonium: Exemplified by at B factories production at hadron colliders ……

The underlying problems Most of the NRQCD successes based on the NLO QCD predictions. However, the NLO QCD corrections are often large: Zhang et.al. Gong et.al. Campbell et.al. Mackenzie et.al. … …

Question: How about the convergence of the QCD correction? So calculating the higher order QCD correction is very necessary to test NRQCD predictions!

Investigation on γγ*  ηc form factor Experiment BaBar Collaboration: Phys.Rev. D81 (2010) 052010 Babar measures the transition form factor in the momentum transfer range from 2 to 50 GeV2.

Investigation on γγ*  ηc form factor Experiment BaBar Collaboration: Phys.Rev. D81 (2010) 052010

Investigation on γγ*  ηc form factor Experiment BaBar Collaboration: Phys.Rev. D81 (2010) 052010 The solid curve is from a simple monopole fit: The dotted curve is from pQCD prediction Feldmann and Kroll, Phys. Lett. B 413, 410 (1997)

Investigation on γγ*  ηc form factor Previous investigation factorization: Feldmann et.al., Cao and Huang Lattice QCD: Dudek et.al., J/ψ -pole-dominance: Lees et.al., QCD sum rules: Lucha et.al., light-front quark model: Geng et.al., All yield predictions compatible with the data, at least in the small Q2 range. So far, so good. Unlike γγ*  π0 , there is no open puzzle here

Investigation on γγ*  ηc form factor Our motivations Model-independent method is always welcome. In the normalized form factor, nonperturbative NRQCD matrix element cancels. Therefore, our predictions are free from any freely adjustable parameters! Is LO NRQCD prediction enough? The momentum transferred is not large enough, we are not bothered by the large logarithmic resummation. Jia and Yang

Investigation on γγ*  ηc form factor Theoretical descriptions Definition for form factor: NRQCD factorization defines: Factorization scale Short-distance coefficient We are going to compute it!

Investigation on γγ*  ηc form factor Theoretical descriptions Upon general consideration, the SDC can be written as IR pole matches anomalous dimension of NRQCD pseudo-scalar density RGE invariance

Investigation on γγ*  ηc form factor Theoretical calculation Tree-level SDC NLO QCD correction

Investigation on γγ*  ηc form factor Feynman diagrams Numer of diagrams 2 8 108 12

Investigation on γγ*  ηc form factor NNLO corrections At , the value of is compatible with asymptotic behavior in Jia, Yang, NPB 2009 Light-by-light UV/IR finite regular Reproduce known NNLO corr. to ηc->γγ Czarnecki et al. 2001

Investigation on γγ*  ηc form factor NNLO corrections Contribution from lbl is not always negligible!

γγ*  ηc : NNLO prediction seriously fails to describe data! Investigation on γγ*  ηc form factor Theory vs Experiment Our Prediction is free of any nonperturbative parameters! γγ*  ηc : NNLO prediction seriously fails to describe data!

Investigation on γγ*  ηc form factor Prediction to γγ*  ηb Convergence of perturbation series is rather good. Wait for CEPC/ILC to test our prediction?

Investigation on c0,2 2γ Experiment  BESIII gives updated measurements: (BESIII, PRD, 2012) Decay width of c0  2 γ Ratio of decay width of c2  2 γ to that of c0  2 γ Ratio of the two-photon widths for helicity λ= 0 and helicity λ= 2 components in c2  2 γ

Investigation on c0,2 2γ Various theoretical predictions  Review of previous theoretical works Numerous work based on phenomenological models R. Barbieri, R. Gatto, R. Kogerler (PLB, 1976) L. Bergstrom, G. Hulth, H. Snellman (Z. Phys. C, 1983) Z. P. Li, F. E. Close, T. Barnes (PRD, 1991) H. W. Huang, C. F. Qiao, K. T. Chao (PRD, 1996) S. N. Gupta, J. M. Johnson, W. W. Repko (PRD, 1996) G. L. Wang (PLB, 2007) C. W. Hwang, R. S. Guo (PRD, 2010) … … … Lattice QCD prediction for c0 2 γ by J. Dudek and R. Edwards (PRL 2006), obtains partial width of , based on the algorithm proposed by X. D. Ji and C. W. Jung (PRL 2001; PRD, 2001)

Investigation on c0,2 2γ NRQCD formula According to the NRQCD factorization The short-distance coefficients can be systematically expanded

Investigation on c0,2 2γ NRQCD formula

Investigation on c0,2 2γ NRQCD calculation

Investigation on c0,2 2γ NRQCD calculation

Investigation on c0,2 2γ Theory vs Experiment (BESIII, PRD, 2012) By assuming HQSS, we predict

Investigation on c0,2 2γ Theory vs Experiment

Investigation on c0,2 2γ Theory vs Experiment Giving up HQSS

Summaries The NNLO NRQCD predictions to γγ*  ηc form factor and c0,2 2γ fail to explain the experiment! The convergence of QCD expansions for the short-distance coefficients is poor! NRQCD predictions should be tested at high order!

Thanks for your attention!