Title: Gerald A' Miller
1Model Independent Nucleon results
Gerald A. Miller University of Washington
Everything that rises, Martin Puryear
2Outline
- Phenomenological considerations
- proton is not round.
- Model independent
- neutron charge density,
- proton magnetization
- shape of proton
- Experimental progress-Jefferson lab INT program
Jlab-12 Fall 09
3Naive Model of Nucleon
- Proton 2 u, 1 d, Neutron 2 d, 1 u
- Confined quarks move with zero orbital angular
momentum
Spin Crisis Quarks carry only 30 of proton
spin three ideas- u,d quarks surrounded by s
s gluons carry angular momentum quarks
carry orbital angular momentum
4Definitions
2
5Expectations- Pre Jlab
Jlab
QF2 /F1
GE/GM
GE/GM
QF2/F1
Q2
Q2
Proton
6Old Interpretation of GE(Q2) is Fourier
transform of charge density
This is correct in non-relativistic physics
- invariant same in initial and final frame
Relativity ? is frame dependent, initial and
final wave functions have different momentum OLD
interpretation of Sachs wrong
-
7Why relativity if Q2 ltltM2
- QCD- photon hits ¼ massless quarks
- No matter how small Q2 is, there
- is a boost correction / Q2
- GE n Q2 (s d3r r2?2C/(mq)2)
8Need relativistic 3-quark model Implement
Relativity-Light Cone Cooordinates
Time xc t z x0x3 Evolve
p-(p0-p3) Space x-ct-zx0-x3 Momentum
pp0p3 Bjorken variable Transverse position
b, momentum p Separate internal and cm
coordinates
9Relativistic formalism-kinematic subgroup of
Poincare
- Lorentz transformation transverse velocity v
k- such that k2 not changed
Transverse boosts act like non-relativistic
10Impulse Approximation 1995
Frank, Jennings, Miller 95
g
Correct wave function includes PQCD, Feynman
mechanisms
11Ratio of Pauli to Dirac Form Factors 1995 theory,
data 2000
12Relativistic Model Explanation
13Model exists
- lower components of Dirac spinor
- orbital angular momentum
- shape of proton?? Wigner Eckart
- no quadrupole moment
- spin dependent densities SDD
- non-relativistic example
14?
s r
15Shapes of the proton
three vectors n, K, S
MODEL , HOW TO MEASURE?
16Model Independent Densities and Shapes
Phys.Rev.Lett.99112001,2007 charge
density arxiv0711.0972 magnetization
density arXiv0708.2297 nucl-th in PRC- shape
Model independent charge densities using form
factors- magnetization density of proton Model
independent shape of proton from (e, p ? e, ?
X)
17What is charge density at the center of the
neutron?
- Neutron has no charge, but charge density need
not vanish - Is central density positive or negative?
-
18n p ?-
4? r2?n(r)
TTM
One gluon exchange also givespositive central
charge density
Today- model independent information
19Generalized Parton Distribution
A0, t(p-p)2 -Q2 -
20Hq(x,0)q(x) (PDF)
transverse center of mass R
21Burkardt
Integrate on x, Left sets x-0 qy(0,b)
q(0,b) DENSITY right 2 Dim. Fourier T. of F1
22 RESULT
Soper 77
(2?)2
Density
Two dimensional Fourier Transform
?Q2/4M2
? GM ¼ GE at low Q2
For neutron
23neutron
proton
24hep-ex/0602017
25Results
BBBA
Kelly
Negative
26GeV2
G
GeV2
Negative F1 means central density negative
27Neutron Interpretation
-
b
Why ?
28(No Transcript)
29(No Transcript)
30Shapes of the proton
- Relate spin dependent density SDD to experiment
31Field theoretic SDD
- Probability to have momentum K, and spin
direction n
Matrix elements depend on three vectors n, K, S
32Transverse Momentum Distributions TMDs
- xK/P
- Mulders Tangerman 96
?i?5 ??i ?0 ?i
33Relate SDD to TMD
- SDD depend on Kx, Ky , Kz equal time
correlation function - TMD depend on x, Kx , Ky ?0 tz correlation
function - Integrate SDD over Kz --gt t0,z0
- Integrate TMD over x ! ?0, t0,z0
- Result non-spherical nature of proton related to
h1T?
34Transverse spin-dependent densities
n
n
S
35Measure e, p ? e, ? X
ST
e
?
e
Cross section has term proportional to cos 3?
Boer Mulders 98
36Summary of SDD
- SDD are closely related to TMDs
- If h1T? is not 0, proton is not round.
Experiment can show - proton aint round.
The Proton
37Spares follow
38Spin density operator d(r-rp) s . n
PRB65, 144429
- Canted ferromagnetic structure of UNiGe high
magnetic fields - Neutron magnetic scattering
- Neutron, B, crystal
39Summary of density
- Model independent information on charge density
- Central charge density of neutron is negative
- Pion cloud at large b
40Charge symmetry u in proton is d in neutron, d
in proton is u in neutron ?u?p?n/2 ?d?p2?n
?p4/3?u-1/3 ?d