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Gerald A' Miller

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Naive Model of Nucleon. Proton 2 u, 1 d, Neutron 2 d, 1 u ... kinematic subgroup of Poincare. Lorentz transformation transverse velocity v ... – PowerPoint PPT presentation

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Title: Gerald A' Miller


1
Model Independent Nucleon results
Gerald A. Miller University of Washington
Everything that rises, Martin Puryear
2
Outline
  • 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

3
Naive 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
4
Definitions
2
5
Expectations- Pre Jlab
Jlab
QF2 /F1
GE/GM
GE/GM
QF2/F1
Q2
Q2
Proton
6
Old 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
-
7
Why 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)

8
Need 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
9
Relativistic formalism-kinematic subgroup of
Poincare
  • Lorentz transformation transverse velocity v

k- such that k2 not changed
Transverse boosts act like non-relativistic
10
Impulse Approximation 1995
Frank, Jennings, Miller 95
g
Correct wave function includes PQCD, Feynman
mechanisms
11
Ratio of Pauli to Dirac Form Factors 1995 theory,
data 2000
12
Relativistic Model Explanation
13
Model 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
15
Shapes of the proton
three vectors n, K, S
MODEL , HOW TO MEASURE?
16
Model 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)
17
What 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?

18
n p ?-
4? r2?n(r)
TTM
One gluon exchange also givespositive central
charge density
Today- model independent information
19
Generalized Parton Distribution
A0, t(p-p)2 -Q2 -
20
Hq(x,0)q(x) (PDF)
transverse center of mass R
21
Burkardt
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
23
neutron
proton
24
hep-ex/0602017
25
Results
BBBA
Kelly
Negative
26
GeV2
G
GeV2
Negative F1 means central density negative
27
Neutron Interpretation

-
b
Why ?
28
(No Transcript)
29
(No Transcript)
30
Shapes of the proton
  • Relate spin dependent density SDD to experiment

31
Field theoretic SDD
  • Probability to have momentum K, and spin
    direction n

Matrix elements depend on three vectors n, K, S
32
Transverse Momentum Distributions TMDs
  • xK/P
  • Mulders Tangerman 96

?i?5 ??i ?0 ?i
33
Relate 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?

34
Transverse spin-dependent densities
n
n
S
35
Measure e, p ? e, ? X
ST
e
?
e
Cross section has term proportional to cos 3?
Boer Mulders 98
36
Summary 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
37
Spares follow
38
Spin density operator d(r-rp) s . n
PRB65, 144429
  • Canted ferromagnetic structure of UNiGe high
    magnetic fields
  • Neutron magnetic scattering
  • Neutron, B, crystal

39
Summary of density
  • Model independent information on charge density
  • Central charge density of neutron is negative
  • Pion cloud at large b

40
Charge 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
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