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Neutron (e,e’π±) Target Single-Spin Asymmetry in Semi-inclusive DIS on a Transversely Polarized 3He Target - Kalyan Allada, Chiranjib Dutta, Mitra Shabestari,

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Presentation on theme: "Neutron (e,e’π±) Target Single-Spin Asymmetry in Semi-inclusive DIS on a Transversely Polarized 3He Target - Kalyan Allada, Chiranjib Dutta, Mitra Shabestari,"— Presentation transcript:

1 Neutron (e,e’π±) Target Single-Spin Asymmetry in Semi-inclusive DIS on a Transversely Polarized 3He Target - Kalyan Allada, Chiranjib Dutta, Mitra Shabestari, Xin Qian On the behalf of Transversity Collaboration Two experiments with the highest scientific rate: A Nucleon Structure Characteristics of Transversity Detector system & 3He Target Nucleon anomalous magnetic moment (Stern, Nobel Prize 1943) Electromagnetic form factor from electron scattering (Hofstadter, Nobel Prize 1961) Deep-in-elastic scattering, quark underlying structure of the nucleon (Freedman, Kendell, Taylor, Nobel Prize 1990) Well Known, since first measurement at 70s. Beam - 6Gev, 15 microA electron beam Target Reasonable Known with 20 years effort. Transversity, business just started. HALL-A 3He Target 40-cm long Rb-K spin-exchange hybrid cell at 10 atm . ~42% target polarization with spin-flip frequency of 20 minutes. A third set of Helmholtz coil will be added together with the laser optics to allow vertical polarization of the 3He target. Some characteristics of transversity : h1T = g1L for non-relativistic quarks In non-relativistic case, boosts and rotations commute. Important inequalities: |h1Tq| ≤ f1q ; |h1Tq| ≤ (f1q + g1Lq )/2. h1T and gluons do not mix Q2-evolution for h1T and g1L are different Chiral-odd → not accessible in inclusive DIS HRS HRS Understanding the underlying nucleon structure (Spin, flavor, charge, current distribution) from quantum chromodynamics (confinement region) is essential. q q state Helicity Electronuclear Scattering A powerful tool to study nuclear structure Target Polarimetry NMR and EPR will be used to measure the target polarization. N N - + Spectrum: Inclusive: (the main tool) detecting electron only Semi-inclusive: (providing additional information) detecting electron and one of the hadrons coincidently Hall-A Setup It takes two Chiral-odd objects to measure transversity Drell-Yan (Doubly transversely polarized p-p collision) Semi-inclusive DIS Chiral-odd distributions function (transversity) Chiral-odd fragmentation function (Collins function) Asymmetry in Semi-Inclusive DIS with polarized target Collins and Sivers Asymmetry Electron detection - BigBite spectrometer, solid angle = 64msr, at 300 What is Semi-Inclusive Deep Inelastic Scattering (SIDIS) Collins effect ( Sin(φh+ φS) ) Access to transversity Artru model Based on LUND fragmentation picture. Scattering plane Parton distribution Function (PDF) Charged pion detection - Hall-A High Resolution Spectrometer, at -160 Projections First direct data on neutron AUT At high-x Clear separation of Collins and Sivers effect. Statistical uncertainty dominates. Kinematics comparable to the HERMES experiment. Fragmentation function (FF) DXs~PDF*FF The kinematics and coordinate Sivers effect ( Sin(φh- φS) ) A new type of PDF, T-odd, depends on intrinsically quark transverse momentum quark orbital momentum E’ is the energy of scattered electron θe is the scattering angle ν =E-E’ is the energy transfer. kT: quark transverse momentum HERMES: 3 years COMPASS: 1 year Beam direction DIS: Q2 (1/λ) and ν is large, but x is finite. Into the page HALL A: 29 days


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