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Coulomb distortions in the Lead Radius Experiment PREX

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Interested in neutron densities of heavy nuclei. ... Relation of neutron density to: Pressure of neutron matter (Alex Brown) Density dependence of symmetry ... – PowerPoint PPT presentation

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Title: Coulomb distortions in the Lead Radius Experiment PREX


1
Coulomb distortions in the Lead Radius Experiment
(PREX)
Tim Cooper (Univ. College Fraser Valley) C. J.
Horowitz (Indiana)
2
Coulomb distortions
  • Interested in neutron densities of heavy nuclei.
    These have large Z and important coulomb
    distortions.
  • Solve Dirac equ for electron in both coulomb V(r)
    and weak axial A(r) potentials.
  • In helicity basis, right handed e feels pot VA
    and left handed feels V-A
  • Subtract cross sec for V-A from cross sec VA

3
Numerics
  • Crucial help from E. D. Cooper! His code RUNT
    for relativistic proton-nucleus scattering in S,
    V optical pots Helped B. C. Clark with Dirac
    phenom. numerics.
  • Worry about subtraction of two large cross
    sections???
  • Each cross sec is very hard numerical problem
    because convergence of partial waves is poor.
    Standard tricks to speed convergence.
  • Backward cross section is much much harder
    numerical problem (need phase shifts to many
    places) than forward angle asymmetry.
  • Now several independent codes agree.

4
Coulomb distortion results
208Pb at 850 MeV
  • Distortions reduce asym. by 30 and somewhat
    reduce sensitivity to neutron density.
  • Largest correction to asymmetry.
  • Can be accurately calculated and charge density
    is known.

5
Vector Analyzing power An
  • Test distortion physics with vector analyzing
    power An left right asymmetry for transversely
    polarized beam.
  • An0 in Born approx. from time reversal. Nonzero
    value only from 2 or more photons.
  • An is large for high Z of nucleus, since
    distortions large .
  • An is potential systematic error for parity
    experiments.
  • We exactly solve Dirac equation to sum photon
    exchanges to all orders. Only keep elastic
    intermediate states. These are coherent / Z2
    for heavy nucleus.
  • Hard numerical problem two independent codes
    RUNT (E.D. Cooper) and ELASTIC (CJH). Agree with
    published results at lower energies (15 MeV).

6
850 MeV
An
At forward angles, An grows with increasing Z of
target
7
208Pb at 850 MeV
An
Elastic intermediate states only!
An ¼ -.4 ppm comparable to parity violating A¼ .6
ppm because of large Z. Measure An during PREX.
8
PREX History
  • 1989 Donnelly, Dubach, Sick ? PV for n densities.
  • 1998 CJH calculates PV asy with Coulomb
    distortions.
  • 1999 Michaels CJH optimize PREX kinematics.
  • 2000 PREX discussed at ECT PV conference.
  • 2001 Relation of neutron density to
  • Pressure of neutron matter (Alex Brown)
  • Density dependence of symmetry energy
  • Many neutron star properties
  • 2000- HAPPEX, HAPPEX II, HAPPEX He experiments

9
PREX History
  • Electron scattering workshop, INT 1997

10
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