Chung-Wen Kao Chung-Yuan Christian University Taiwan TBE effects for both parity-conserving and...
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Transcript of Chung-Wen Kao Chung-Yuan Christian University Taiwan TBE effects for both parity-conserving and...
Chung-Wen KaoChung-Yuan
Christian University Taiwan
TBE effects for both parity-conserving and parity-violating ep elastic scattering
12th International Conference on the Structure of the Baryon , Dec 7-11, RCNP, Osaka University, Japan
Collaboration and Reference
In Collaboration with Hai-Qing Zhou(SouthEast U, China), Keitaro Nagata(CYCU, Taiwan), Yu-Chun Chen(AS, Taiwan), M. Vanderhaeghen(Mainz, Germany), Shin-Nan Yang (NTU,Taiwan)
This talk is based on the following works:(1) H-Q Zhou, CWK, S-N. Yang: Phys.Rev.Lett.99:262001,2007(2) K.Nagata, H-Q Zhou, CWK, S-NYang: Phys.Rev.C79:062501,2009.(3) H-Q Zhou, CWK,S-N Yang, K. Nagata: Phys.Rev.C81:035208,2010(4) Y.C. Chen, CWK, M. Vanderhaeghen: arXiv: 0903.1098
Part 1: TPE in parity-conserving ep elastic scattering
3
Form factor in quantum mechanics
2)(e)( rrdqF rqi
Atomic form factor:
( ) ~ ( ) q F q2
is the Fourier transform of the charge density.
The cross section:
E.g., the hydrogen atom in the ground state:
2
2
2201)(
qaqF
30
2/
8e)(
0
ar
ar
2)()( rr
charge density
m105.04 1020
ecm
a with Bohr radius
ei k r
rki 'e
Nucleon E.M form factors
Hofstadter determined the precise size of the proton and neutron by measuring their form factor.
"for his pioneering studies of electron scattering in atomic nuclei and for his thereby achieved discoveries concerning the structure of the nucleons
Rosenbluth Separation MethodWithin one-photon-exchange framework:
Polarization Transfer Method
Polarization transfer cannot determine the values of GE and GM but can determine their ratio R.
Inconsistency between two methods
SLAC, JLab Rosenbluth data
JLab/HallA Polarization data
Jones et al. (2000)Gayou et al (2002)
Go beyond One-Photon exchange
New Structure
P. A. M. Guichon and M. Vanderhaeghen, Phys. Rev. Lett. 91, 142303 (2003).
Two-Photon-Exchange Effects on two techniques
large
small
P. A. M. Guichon and M. Vanderhaeghen, Phys. Rev. Lett. 91, 142303 (2003).
One way or another……. There are two ways to estimate the TPE effect:
Use models to calculate Two-Photon-Exchange diagrams:Like parton model, hadronic model and so on…..
Direct analyze the cross section and polarization data by including the TPE effects:
One-Photon-exchange Two-photon-exchange
Results of hadronic model
Insert the on-shell form factors
P.G.Blunden, W.Melnitchouk and J.A.Tjon, Phys.Rev.Lett. 91 (2003) 142304
Inclusion of resonance
Insert the on-shell form factors
S.Kondratyuk, P.G.Blunden, W.Melnitchouk and J.A.Tjon, Phys.Rev.Lett. 95 (2005) 172503
Partonic Model Calculation
GPDs
A. V. Afanasev, S. J. Brodsky, C. E. Carlson, Y.-C. Chen, and M. Vanderhaeghen, Phys. Rev. D 72, 013008 (2005).
5/6
GPDsx x
t
DVCSDeeply Virtual Compton
Scattering Longitudinal response only
GPDs can be accessed via exclusive reactions in the Bjorken kinematic regime.
The DVCS process is identified via double (eg) or triple (egN) coincidences, allowing for small scale detectors and large luminosities.
Factorisation applies only to longitudinally polarized virtual photons whose contribution to the electroproduction cross section must be isolated..
GPDsx
x
DA
L
DVMPDeeply Virtual
Meson Production),(
),(
t
Hard gluon
QCD factorization approach
1γ
1γ+2 γ(BLW)
1γ+2 γ(COZ)
N.Kivel and M.Vanderhaeghen, Phys. Rev. Lett.103 (2009) 092004
The leading perturbative QCD (pQCD) contribution to the 2 γ exchange correction to the elastic ep amplitude is given by a convolution integral of the proton distribution amplitudes (DAs) with the hard coefficient function
Comparison with data
arXiv:1012.0339 JLab Hall C
Empirical extraction of TPE
Upcoming TPE experiments
J.Guttmann, N. Kivel, M. Meziane,and M. Vanderhaeghen, arXiv1012.0564
Olympus@DESY experimentare underway. Over the measured range of this experiment, the 2TPE corrections to the e+p/e−p elastic cross section ratio are predicted to vary in the 1 - 6 % range.
Part 2: TPE effect in parity-violating ep elastic scattering
20
Strangeness in the nucleon
Goal: Determine the contributions of the strange quark sea ( ) to the charge and current/spin distributions in the nucleon :
“strange form factors” GsE and Gs
M
ss
Puuduu dd ss g +.....•
« sea »
• s quark: cleanest candidate to study the sea quarks
Parity Violating ep Elastic Scattering
EMEM JQ
M lQ2
4 NC
VNC
AFNC
PV JgJgGM 55
22
Interference with EM amplitude makes Neutral Current (NC) amplitude accessible
22
~~Z
EM
NCPV
LR
LRPV M
QM
MA
Tiny (~10-6) cross section asymmetry isolates weak interaction
Interference: ~ |MEM |2 + |MNC |2 + 2Re(MEM*)MNC
OPE vs OZE
Isolating the neutral weak form factors: vary the kinematics or the targets
p
AMEF AAAQGA
24
2
~ few parts per millionFor a proton:
Forward angle Backward angle
eA
pMWA
ZM
pMM
ZE
pEE GGAGGAGGA '2sin41 , ,
sME
dME
uMEME GGGG //// 3
131
32
sMEW
dMEW
uMEW
ZME GGGG /
2/
2/
2/ sin
341sin
341sin
381
NC probes same hadronic flavour structure, with different couplings:
GZE/M provide an important new benchmark for testing
non-perturbative QCD structure of the nucleon
NF
Mqi
FNNuuNJN
qqq
qEM
21 2
Q
Flavour decomposition
Apply Charge Symmetry
snME
spME
unME
dpME
dnME
upME GGGGGG ,
/,/
,/
,/
,/
,/ ,,
GpE,M
GsE,M
GuE,M
GdE,MGn
E,MCharge
symmetryGp
E,M<N| sγμ s |N>
GnE,M
GpE,M
GsE,M
ShuffleWell
Measured
As
MEn
MEp
MEFZ
LR
LRPV GGGGQG
M
MMA ,,,F
2 ///
2
2
sME
dME
uME
pME GGGG ///
,/ 3
131
32
s
MEu
MEd
MEnME GGGG ///
,/ 3
131
32
Tree Level is not enough! The strange form factors are found to
be very small, just few percents. To make sure the extracted values
are accurate, it is necessary to take the radiative correction into consideration!
So one has to draw many diagrams as follows…..
Electroweak radiative corrections
Squeeze eq→eq amplitudes into 4-Fermion contact interactions
Extraction of strange form factors with radiative corrections
ρ and κ are from electroweak radiative corrections
Strange form factors
Be aware of the Box! Box diagram is intricate because it is
related with nucleon intermediate states. Box diagram is special because of its complicated Q2 and ε
dependence
So how one can squeeze the box diagrams?
Zero Transfer Momentum Approximations for Box diagrams
p
q
Q2=t=(p-q)2 =0
Approximation made in previous analysis:
p=q=k
Marciano, Sirlin (1983)
Pe=Pe’=0Pe
Pe’
High and Low Momentum Integration
N
Low Loop momentum Integration:Only include N intermediate state.Insert the on-shell form factors
High Loop momentum Integration:Lepton and a single quark exchange bosons.Convoluation with PDF
N
=l l
MS approximation Initially it is for atomic parity violation. Two exchanged boson carry the same 4-
momentum and lepton momenta are set to be zero. In other words MS approximation is three-fold approximation:
Q2=0. Elab=0 Coulomb force is taken away
Indeed MS is not good enough !
HQ. Zhou, CWK and SN Yang, PRL, 99, 262001 (2007)
Adding resonances….
Δ(1232) plays an important role in the low energy regime due to its light mass and its strong coupling to πN systeam.
arXiv:0811.3539 PRC79:062501 2009
Keitaro Nagata, Hai Qing Zhou, CWK and SN Yang
Nagata et al, arXiv:0811.3539 PRC79:062501 2009
Partonic calculation of Box diagrams
=
Yu-Chun Chen, C-W K, M. Vanderhaeghen, arXiv 0903.1098
Result of Partonic calculation
Comparison with Marciano and Sirlin’s approximation
Qweak experiment
δQw / Qw = 4% δsin2θW / sin2θW = 0.3%
Dispersion relation approach
M.Gorchtein and C.J.Horowitz, Phys.Rev.Lett. 102} (2009) 091806
Dispersion calculation
The result of hadronic model is quite different
δN=0.6%δΔ=-0.1%
H.Q. Zhou, CWK and S. N.Yang, in progress.
Conclusion and Outlook
TBE are crucial for the extraction of the EM form factors and strangeness inside the nucleon!
More delicate estimate of the TBE effect is needed badly! (including more resonances, consider quark-level contributions…….)
Upcoming positron-proton scattering will provide us the precious information of TPE effects.
Uncertainty of TBE may jeopardize the interpretation of QWEAK data and requests an answer.
Personal comment….
Two bosons are too many,But two cups of ice cream are just perfect!