Electron- and Positron-proton elastic scattering in clas larry Weinstein



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tarix18.04.2018
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Electron- and Positron-proton elastic scattering in CLAS

  • Larry Weinstein

  • Old Dominion University


The Proton Charge Form Factor



How to measure Two Photon Exchange



Recap:



Positrons to the rescue?





JLab CLAS



CLAS in Maintenance Position



Experiment Features/Bugs

  • Identical mixed e+/e− beam (250 pA each)

  • Continuous beam energy distribution

    • Wide Q2 and angle (ε) coverage
  • Simultaneous cross section measurements

    • Minimize systematic uncertainty
    • Allows 1-2% measurement of e+/e− cross section ratio
  • Reverse magnetic fields (chicane/Torus) to reduce acceptance effects

  • Overdetermined ep kinematics allows background rejection

  • Unprecedented photon luminosity (1000 times!)









Oct 2006 test run

  • 3-Dipole chicane with photon blocker

  • Remove material from tagger exit line

  • Shield tagger exit line (bunker)

  • Tagger dump cooling

  • Lepton-beam fiber monitor (FIU)

  • LOTS of new shielding and collimation

    • Collimate after chicane
    • Collimate before CLAS
  • LOTS of modifications during the test run







2006 Test Run Results: Luminosity

  • Maximum luminosity achieved:

  • 80 nA 3.2 GeV electrons

  • 0.5% radiator, 5% convertor

  • Figure of Merit: 20 pA (80nA*0.5%*5%)

  • Limited by drift chamber occupancies (3% limit)

    • Region 1 DC occupancy 2.3%
    • Region 3 DC occupancy 0.7%
  • Test run achieved 4% of proposal luminosity

  • Luminosity and backgrounds agreed with simulations.

  • Factor of 10-20 improvement on previous test runs!



How to do better

  • Limitations:

  • Target and heat exchanger apertures

  • Moller electrons trapped by the CLAS magnetic field

  • Background from the tagger vacuum box

  • Background from other (diffuse) sources

  • Limited beam monitoring

  • Improvements:

  • Reduce pre-CLAS collimator aperture from 6 to 4 cm

  • Add minitorus and Moller catcher

  • Shield tagger vacuum box (6 mm Pb)

  • Large concrete pipe and disk shield

  • Double target length

  • Build a position sensitive removable beam-line calorimeter for beam characterization



New beamline shielding



Target shielding and Moller electrons



Luminosity vs time



2006 Test Run Data Analysis



Kinematic cuts:



Kinematic cuts II:



Kinematic Cuts III:



Data Analysis: Acceptance



Data Analysis: Kinematics



Data Analysis: Binning



Results: e+p/e-p double ratios



Test Run vs the World!



What next?



Summary:

  • GEp measured by Rosenbluth and Polarization transfer expts differ by a factor of 3 at Q2 = 6

  • Two Photon Exchange might explain the discrepancy

  • The e+p/e-p ratio is the only way to measure the real part of the TPE amplitude



Summary:

  • The TPE Engineering Test Run

    • Produced a mixed identical electron/positron beam
    • Validated beam line simulations
    • Measured the e+p to e-p elastic scattering ratio at low Q2
      • small systematic uncertainties
  • The TPE experiment

    • Will be able to achieve the proposed luminosity
    • Will cover a wide kinematic range
    • Will determine precisely the TPE contribution and resolve the GE problem
    • Will be ready to run in 2010
  • Anti-matter beams are cool!



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