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Recent results from BLAST detector. Bates Linear Accelerator center. Siberian Snake. 850 MeV cw polarized electron beam Beam polarization longitudinal at target Storage ring filled to 225 mA; helicity flipped each fill Lifetime 25 to 30 minutes
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Recent results from BLAST detector Evgeni Tsentalovich MIT
Bates Linear Accelerator center Siberian Snake • 850 MeV cw polarized electron beam • Beam polarization longitudinal at target • Storage ring filled to 225 mA; helicity flipped each fill • Lifetime 25 to 30 minutes • Automated synchronization of ring fill, detector HV ramp, data taking, ring dump using the EPICS control system Evgeni Tsentalovich MIT
Electron beam polarization Compton polarimeter • Compton polarimeter provides online control of stored beam polarization • Laser beam helicity flipped with a Pockels cell (~10Hz) • Backscattered photons are detected with CsI crystal • Electron beam polarization flipped every new fill • Average beam polarization 67% Evgeni Tsentalovich MIT
Polarized Internal Target • ABS (Atomic Beam Source) produces flux of Hydrogen or Deuterium atoms • ABS intensity ~ • Dri-film coated T-shaped storage cell. • Target thickness ~ • Hydrogen polarization Pz78% • Deuterium polarization Pz72%, Pzz 68% • Target polarization flipped every 5 min Evgeni Tsentalovich MIT
TARGET BEAM BEAM BLAST • Toroidal field 3.8 kG • 2 instrumented sectors in the horizontal plane - Drift chambers - Cerenkov detectors - Time of Flight scintillators - Neutron detectors BLAST DATA: 2004, Hydrogen - Pz78%, 81 pb-1 2004, Deuterium - Pz84%, 130 pb-1 Pzz68% 2005, Deuterium - Pz72%, 180 pb-1 Pzz56% Evgeni Tsentalovich MIT
Electron Left Electron Right Kinematics for spin-dependent electron scattering Electron scattering into left sector : q vector ~ perpendicular to target spin (perpendicular kinematics) Electron scattering into right sector : q vector ~ parallel to target spin (parallel kinematics) B p e’ q e Evgeni Tsentalovich MIT
BLAST physics program Pol Vect.-Pol -production Tens.-Pol Evgeni Tsentalovich MIT
Measurements of neutron form factor Product of beam and target polarizations (hPz) is determined from 2H(e,e’p)n reaction and verified with 2H(e,e’n)p in parallel kinematics The Form Factors ratio is measured in perpendicular kinematics Evgeni Tsentalovich MIT
Preliminary results • Small systematic errors: • The largest contribution (5%)– from the uncertainty in the target polarization angle (~12 % per degree) • Uncertainty in hPz 2.5% • Uncertainty in magnetic Form Factor 1.5 % • Model dependency < 3% • Radiative effects <1% Evgeni Tsentalovich MIT
Measurements of deuteron form factors Evgeni Tsentalovich MIT
Preliminary results The largest systematic error(~5%) – from the normalization on low-q points Evgeni Tsentalovich MIT
, In the Born approximation vanishes in the L=0 model for deuteron (no L=2 admixture) => is a good measure of L=2 component is a good measure of L=2 component and reaction mechanisms : MEC, IC, RC Evgeni Tsentalovich MIT
Vector Asymmetry Evgeni Tsentalovich MIT
Tensor Asymmetry Evgeni Tsentalovich MIT
Separation of charge and magnetic proton form factors Existing data: 1.Rosenbluth separation 2.Polarization transfer measurements (scattering of polarized electrons on Hydrogen target and measuring a polarization of recoil protons) Evgeni Tsentalovich MIT
World Data Evgeni Tsentalovich MIT
Scattering of polarized electrons on polarized protons Super ratio Evgeni Tsentalovich MIT
Preliminary Results from BLAST BLAST Left Sector BLAST Right Sector Evgeni Tsentalovich MIT
Preliminary Results from BLAST Evgeni Tsentalovich MIT
Preliminary Results from BLAST with World Data Evgeni Tsentalovich MIT
Conclusion • Preliminary results from BLAST • quasi-elastic d(en) ( ) • elastic d(ed)(T20) • quasi-elastic d(ep) • elastic p(ep)( ) • Factor of two more data to analyze • Also analyzing data on production, resonance, T10/T11, • inclusive…. • More results to come ! Evgeni Tsentalovich MIT