Kao, Chung-Wen 高崇文 Chung Yuan Christian University 臺灣中原大學

Slides:



Advertisements
Similar presentations
1 The and -Z Exchange Corrections to Parity Violating Elastic Scattering 周海清 / 东南大学物理系 based on PRL99,262001(2007) in collaboration with C.W.Kao, S.N.Yang.
Advertisements

1 First Measurement of the Structure Function b 1 on Tensor Polarized Deuteron Target at HERMES A.Nagaitsev Joint Institute for Nuclear Research, Dubna.
Pawan Kumar NetrakantiPANIC-2005, Santa Fe1 Pion, proton and anti-proton transverse momentum spectra in p+p and d+Au collisions at  s NN = 200 GeV Outline:
Measurement of polarized distribution functions at HERMES Alessandra Fantoni (on behalf of the HERMES Collaboration) The spin puzzle & the HERMES experiment.
Mauro Anselmino, Prague, August 1, 2005 Hadron Structure and Hadron Spectroscopy Transversity (transverse spin and transverse motion) Transversity distributions.
Review of  G in DIS and pp … a lot has happened since Kyoto Frank Ellinghaus University of Mainz / University of Colorado October 2008 SPIN’08, Charlottesville,
Constraining the polarized gluon PDF in polarized pp collisions at RHIC Frank Ellinghaus University of Colorado (for the PHENIX and STAR Collaborations)
QCD Analysis and Fragmentation Functions in the BELLE Experiment
THE DEEP INELASTIC SCATTERING ON THE POLARIZED NUCLEONS AT EIC E.S.Timoshin, S.I.Timoshin.
1 Flavor Symmetry of Parton Distributions and Fragmentation Functions Jen-Chieh Peng Workshop on “Future Prospects in QCD at High Energy” BNL, July 17-22,
Spin-Flavor Decomposition J. P. Chen, Jefferson Lab PVSA Workshop, April 26-27, 2007, Brookhaven National Lab  Polarized Inclusive DIS,  u/u and  d/d.
Spin and azimuthal asymmetries in SIDIS at JLAB  Physics Motivation  Jlab kinematics and factorization  Double spin asymmetries  Single Spin Asymmetries.
New results on SIDIS SSA from JLab  Physics Motivation  Double spin asymmetries  Single Spin Asymmetries  Future measurements  Summary H. Avakian.
Future Physics at JLab Andrew Puckett LANL medium energy physics internal review 12/14/
Error Estimation of Fragmentation Functions Based on Global QCD Analysis Tokyo Inst. of Tech. 1. Motivation 2. Analysis Method 3. Results 4. Summary Contents.
The Role of Higher Twists in Determining Polarized Parton Densities E. Leader (London), A. Sidorov (Dubna), D. Stamenov (Sofia) 10th International Workshop.
1 E.C. Aschenauer Recent results from lepton proton scattering on the spin structure of the nucleon.
1 On extraction of the total photoabsorption cross section on the neutron from data on the deuteron  Motivation: GRAAL experiment (proton, deuteron) 
03/03/31 日本物理学会 1 HERMES による横偏極水素標的を 用いた quark transversity の測定 大須賀弘, 田中秀和, 宮地義之, 柴田利明, 他 HERMES Collaboration 東京工業大学 柴田研究室.
Quark Structure of the Proton – The Horizons Broaden! On behalf of the HERMES collaboration H. E. Jackson highlights.
Strangeness and Spin in Fundamental Physics Mauro Anselmino: The transverse spin structure of the nucleon Delia Hasch: The transverse spin structure of.
R. Joosten, Oct. 7, 2008 Measurement of TMDs in Semi-Inclusive DIS in Semi-Inclusive DIS Rainer Joosten University of Bonn Charlottesville, VA, October.
JPARC DY Workshop, April 7 Ralf Seidl (RBRC) R.Seidl: Transverse Spin 1RIKEN, April 7 In JPARC Drell Yan accessible with: UU(unpolarized beam, unpolarized.
The nucleon helicity as seen by HERMES From g 1 to  G Patricia Liebing RIKEN-BNL Research Center for the collaboration Annual RHIC and AGS Users Meeting,
Twist-3 predictions for single spin asymmetry for light-hadron productions at RHIC Koichi Kanazawa (Niigata Univ) ・ KK and Y. Koike, PRD 83, (2011)
Measurement of Flavor Separated Quark Polarizations at HERMES Polina Kravchenko (DESY) for the collaboration  Motivation of this work  HERMES experiment.
Exploring New Kinematic Dependences of Semi- Inclusive Double-Spin Asymmetries at HERMES Joshua G. Rubin Argonne National Laboratory DIS2010 April 12,
TMD flavor decomposition at CLAS12 Patrizia Rossi - Laboratori Nazionali di Frascati, INFN  Introduction  Spin-orbit correlations in kaon production.
Delia Hasch Transversity & friends from HERMES International workshop on hadron and spectroscopy, Torino, Italy, 31. March – 02. April 2008 outline outline.
Tensor and Flavor-singlet Axial Charges and Their Scale Dependencies Hanxin He China Institute of Atomic Energy.
Global QCD Analysis of Polarized SIDIS Data and Fragmentation Functions Tokyo Tech 1. Motivation 2. pQCD Analysis of Fragment Functions (FFs) 3. Results.
The transverse structure of the nucleon (resolving the quark motion inside a nucleon) Mauro Anselmino, Torino University and INFN, JLab, December 15, 2006.
R. Joosten, Oct. 7, 2008 Measurement of TMDs in Semi-Inclusive DIS in Semi-Inclusive DIS Rainer Joosten University of Bonn Charlottesville, VA, October.
1 CLAS-eg1 pol.-proton analysis H.Avakian (JLab) semi-SANE Collaboration Meeting April 21, 2005.
Spin physics with COMPASS
Flavor decomposition at LO
Mark T. Heinz Yale University
Probing strangeness in hard processes Laboratori Nazionali di Frascati
Unpolarized Azimuthal Asymmetries from the COMPASS Experiment
COMPASS Present issues and near future
COMPASS results on inclusive and semi–inclusive polarised DIS
Kao, Chung-Wen Chung Yuan Christian University
Hadron-structure studies at a neutrino factory
Measurements of quark transversity and orbital motion in hard scattering Yoshiyuki Miyachi Tokyo Institute of Technology.
Luciano Pappalardo for the collaboration
The Spin of the Nucleon --- The View from HERMES ---
Experimental Study of Transversity
Prague 2007 Collins and Sivers asymmetries
Inclusive and dijet b productions at CDF
M. Contalbrigo (on behalf of HERMES collaboration)
--- New Results from HERMES ---
Status and Implications of PID measurements at high pT
Selected Physics Topics at the Electron-Ion-Collider
SINGLE HADRON TRANSVERSE SPIN ASYMMETRIES FROM COMPASS
Studies of Strange Sea Distribution Functions using Kaons with CLAS12
Study of Strange Quark in the Nucleon with Neutrino Scattering
Masanori HIRAI 2006, Nov 9, Tokyo-u
Searching for intrinsic motion effects in SIDIS
University of Erlangen-Nürnberg & DESY
Kao, Chung-Wen Chung Yuan Christian University
NLO QCD fits to polarized semi-inclusive DIS data
Single Spin Asymmetry with a Transversely Polarized
Chung-Wen Kao Chung-Yuan Christian University
高崇文 Chung-Wen Kao Chung-Yuan Christian University, Taiwan
Spin effects and partonic intrinsic k┴
- 縦偏極パートン分布関数解析に対する、破砕関数の影響 -
Spin Studies via Drell-Yan Process at PANDA
Probing Fragmentation Func. With SIDIS
New results on SIDIS SSA from JLab
The Helicity Structure of the Nucleon from Lepton Nucleon Scattering
Presentation transcript:

Kao, Chung-Wen 高崇文 Chung Yuan Christian University 臺灣中原大學 Kaon and Pion Fragmentation functions and SIDIS off deuteron Kao, Chung-Wen 高崇文 Chung Yuan Christian University 臺灣中原大學 2016/7/26 Menu 2016

How to extract Fragmentation functions?

SIDIS off deuteron target p: proton, n: neutron

SIDIS using deuteron target Charge Conjugation

SIDIS using deuteron target Assume PDFs are charge symmetric:

SIDIS using deuteron target DQ>>DS

Constrains on A and B Since S(x)>0, Q(x)>0, then S(x)/Q(x) is positive! At fixed x and Q2 : Note that the values of and are independent of x!

HERMES Data of Pion multiplicity

Let’s shopping!

Choices of FFs

Elementary Fragmentation Functions One step fragmentation process q(k) →h(p)+Q(k-p) With a vertex of quark-quark-PS meson, one can calculate the elementary FFs.

Elementary Fragmentation functions One step fragmentation process q(k) →h(p)+Q(k-p)

Nonlocal Chiral quark model Non-local vertex of quark-quark-PS meson

Inclusion of quark-jet contribution

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08 8.SMKA 9.DSEHS

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08 8.SMKA 9.DSEHS

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08 8.SMKA 9.DSEHS

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08 8.SMKA 9.DSEHS

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08 8.SMKA 9.DSEHS

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08 8.SMKA 9.DSEHS

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08 8.SMKA 9.DSEHS

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08 8.SMKA 9.DSEHS

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08 8.SMKA 9.DSEHS

HERMES Kaon Data A. Airapetian et al. (HERMES Collaboration), Phys. Rev. D 448 89, 097101 (2014).

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08

HKNS (LO) HKNS (NLO) DSS (LO) DSS (NLO) 5.NJL-Jet Model 6.Nonlocal Chiral Quark Model 7.AKK08

Inclusion of error bar

Inclusion of error bar

Including the error bar

Inclusion of error bar

Is there inconsistency? To make sense of our result, we try to figure out the best values of DQ and DS to fit the HERMES data. If we assume the values of DQ and DS are not sensitive to Q2 then we only need to plug in PDFs S(x) and Q(x) then we should decide the values of DQ and DS .

Best fit values of DQ and DS DQ<<DS!

Best fit values of DQ and DS

M.Stolarski (COMPASS Collaboration), in SPIN2014, 21st International Symposium on Spin Physics, Beijing, October 19–24, 2014

Best fit values of DQ and DS DKQ DKS DSK<0!

Can CSB explain inconsistency? Assume

Can CSB explain inconsistency?

Can CSB explain inconsistency?

Conclusion To be consistent with HERMES data, the u quark is more likely to fragment to pion rather than kaon. S(x)/Q(x) derived from pion and kaon multiplicity of SIDIS are not consistent with the one from PDFs. None of fragmentation functions can be used to extract PDFs from HERMES data consistently in the LO analysis. CSB is unlikely to explain this problem!

Outlook: NLO analysis

Outlook: NLO analysis HERMES data is challenge for FF modeling !

Thank you for your attention And hope that I have convince you that it is fun to study SIDIS!