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Transcript of Chung-Wen Kao Chung-Yuan Christian University, Taiwan 23.5.2008 National Taiwan University, Lattice...
![Page 1: Chung-Wen Kao Chung-Yuan Christian University, Taiwan 23.5.2008 National Taiwan University, Lattice QCD Journal Club Two is too many: A personal review.](https://reader035.fdocuments.in/reader035/viewer/2022062523/5a4d1aec7f8b9ab05997b378/html5/thumbnails/1.jpg)
Chung-Wen KaoChung-Yuan Christian University,
Taiwan
23.5.2008 National Taiwan University,Lattice QCD Journal Club
Two is too many: A personal review of Two-Photon Physics
In Collaboration with Hai-Qing Zhou, Yu-Chun Chen, Shin-Nan Yang
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Q
e
p p p hadr
oniz
atio
n
( )Q
e
xp
p
)(Q
e
xp
2
X
Qx 2, mp p
xp
q q
PD
One-Photon Physics: From Low to High
Low Q2, elastic, exclusive High Q2, deeply inelastic, inclusive
Form factors Parton distribution
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Hofstadter determined the precise size of the proton and neutron by measuring their form factor.
Nucleon Form Factors
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Why bother to go beyond One-photon-exchange framework?
Since αEM=1/137, the two-photon-exchange effect is just few percent. However, few percent may be crucial for high precision electroweak experiments. Surprisingly, two-photon-exchange effect is more important than we thought !
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Rosenbluth Separation MethodWithin one-photon-exchange framework:
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Polarization Transfer Method
Polarization transfer cannot determine the values of GE and GM but can determine their ratio R.
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Two methods, Two Results!
SLAC, JLab Rosenbluth data
JLab/HallA Polarization data
Jones et al. (2000)Gayou et al (2002)
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Go beyond One-Photon Exchange….
How to explain it?
New Structure
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Two-Photon-Exchange Effects Two-Photon-Exchange Effects on two techniqueson two techniques
large
small
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Possible explanation 2-photon-exchange effect can be large
on Rosenbluth method when Q2 is large. 2-Photon-exchange effect is much
smaller on polarization transfer method. Therefore 2-photon-exchange may
explain the difference between two results.
Guichon, Vanderhaeghen, PRL 91 (2003)
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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 data by including the TPE effects:
One-Photon-exchange Two-photon-exchange
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Hadronic Model Result
Blunden, Tjon, Melnitchouk (2003, 2005)
Insert on-shell form factors
+ Cross diagram
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Results of hadronic model
Blunden, Tjon, Melnitchouk (2003, 2005)
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PPartonicartonic Model Model CCalculationalculation
GPDs
Y.C.Chen, Afanasev,Brodsky, Carlson, Vanderhaeghen(2004)
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Model-independent analysis
Determined from polarization transfer data
TPE effects
From crossing symmetry and charge conjugation:Inputs
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Our Choice of F(Q2, ε)
Fit (A)
Fit (B)
ε→ 1, y→0, F→0 ε→0, y→1, F≠0
YC Chen, CWK ,SN Yang, PLB B652 (2007)
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Result of fitsDashed Line: Rosenbluth
Solid line: Fit (A)
Dotted line: Fit (B)
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Result of fitsDashed Line: Rosenbluth
Solid line: Fit (A)
Dotted line: Fit (B)
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Puzzle about nonlinearityV.Tvaskis et al, PRC 73, 2005
Purely due to TPE
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Fit (A) :
Fit (B):
TPE vs OPE
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Dashed Line : Fit (B) Solid line: Fit (A)
TPE contribution to slope
SLOPE(TPE)/SLOPE(OPE)=C1/(GE/τ)
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Fit (A)
Fit (B)
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Common features of Two fits
GM increase few percents compared with Rosenbluth results
GE are much smaller than Rosenbluth Result at high Q2
OPE-TPE interference effects are always destructive
TPE play important role in the slope TPE give very small curvature
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Any other places for TPE?
Normal spin asymmetries in elastic eN scatteringdirectly proportional to the imaginary part of 2-photon exchange amplitudes
spin of beam OR target NORMAL to scattering plane
Comparison of e-p/e+p :Amp(e-p)=Amp(1γ)+Amp(2γ)
Amp(e+p)=Amp(1γ)-Amp(2γ)Due to Charge conjugation
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Fit (A) Fit (B)
Q^2=1.75 GeV^2 Q^2=1.75 GeV^2
Q^2=3.25 GeV^2
Q^2=5 GeV^2
Q^2=5 GeV^2
Q^2=3.25 GeV^2
R=σ(e+p) / σ(e-p)
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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
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Parity Violating Electron Scattering
EMEM JQ
M
lQ24
NCV
NCA
FNCPV JgJgGM 5
5
22
Interference with EM amplitude makes Neutral Current (NC) amplitude accessible
2
2
~~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
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sME
dME
uMEME GGGG //// 3
131
32
sMEW
dMEW
uMEW
ZME GGGG /
2/
2/
2/ sin
341sin
341sin
381
NC probes same hadronic flavor 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
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Charge SymmetrysnME
spME
unME
dpME
dnME
upME GGGGGG ,
/,/
,/
,/
,/
,/ ,,
GpE,M
GsE,M
GuE,M
GdE,MGn
E,MCharge symmetry
GpE,M
<N| ss |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
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Isolating the form factors: vary the kinematics or target
p
AMEF AAAQGA
24
2
~ few parts per millionFor a proton:
eAA
eA
sME
nME
nV
pME
pVW
ZME
RFsGG
GGRGRG
,,,2
, )1()1)(sin41(
Forward angle Backward angle
eA
pMWA
ZM
pMM
ZE
pEE GGAGGAGGA '2sin41 , ,
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Extraction of strange form factors
ρand κare from electroweak radiative corrections
Strange form factors
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Electroweak radiative corrections
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Zero Transfer Momentum Approximations
p
q
Q2=(p-q)^2
Approximation made in previous analysis:
p=q=k
Marciano, Sirlin (1984)
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One-loop-diagrams
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HQ. Zhou, CWK and SN Yang, PRL, 99, 262001 (2007)
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Old
New
Impact of our results
Avoid double counting
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Change of the results of Strange form factors
-14.6 -45.05
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Preliminary
GMs = 0.28 +/- 0.20GEs = -0.006 +/- 0.016~3% +/- 2.3% of proton magnetic moment~20% +/- 15% of isoscalar magnetic moment~0.2 +/- 0.5% of Electric distribution
This above plot should be modified !!!
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Summary and Outlook Two-Photon physics is important to obtain the information of
nucleon structure even it is small! Two-photon-exchange effect is crucial to extract electric and
magnetic form factors. Two-boson exchange effect is also crucial to extract the
strange form factors! More TPE-related research is going: N→ Δ transition form
factor, normal beam asymmetry and so on… In particular, low energy precision measurement of
electroweak experiments which is sensitive to NEW PHYSICS rely on the good theoretical understand of Two-photon physics!
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Thank you for listening
Two photons may be too many, but two cups of Italian ice cream are not………