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Showing 1 to 8 of 8 for “"Qweak"”.

  1. Compton polarimeter for Qweak Experiment at Jefferson Laboratory

    The Qweak experiment at Jefferson Lab aims to make the first precision measurement of the proton's weak charge, QP = 1 - 4 sin 2 9w at Q2 = 0.026GeV 2 . Given the precision goals in the Qweak experiment, the electron beam polarization must be known to an absolute uncertainty of 1%. A new Compton …

    mit Repository record for Compton polarimeter for Qweak Experiment at Jefferson Laboratory (opens in a new tab)

  2. Precision Measurement of the Proton's Weak Charge using Parity-Violating Electron Scattering

    The Qweak experiment has precisely determined the weak charge of the proton Qp w by measuring the parity-violating asymmetry in elastic electron-proton scattering at a low momentum transfer of Q2 = 0.0249 (GeV/c)2 . Qpw has a definite prediction in the Standard Model, and a value of sin2 θW can be …

    vt Repository record for Precision Measurement of the Proton's Weak Charge using Parity-Violating Electron Scattering (opens in a new tab)

  3. First determination of the weak charge of the proton

    The Qweak experiment measures the parity violating asymmetry in elastic e[upper script right arrow]p scattering at Q² = 0.02455 (GeV/c)² with a 180 [mu]A and 88.7% longitudinally polarized electron beam of 1.165 GeV and a 34.4 cm liquid hydrogen target in experimental Hall C at Jefferson Lab. As …

    mit Repository record for First determination of the weak charge of the proton (opens in a new tab)

  4. Measuring the Weak Charge of the Proton and the Hadronic Parity Violation of the N →Δ Transition

    Qweak will determine the weak charge of the proton, QpW, via an asymmetry measurement of parity-violating elastic electron-proton scattering at low four momentum transfer to a precision of 4%. QpW has firm Standard Model prediction and is related to the weak mixing angle, sin20W, a well-defined …

    vt Repository record for Measuring the Weak Charge of the Proton and the Hadronic Parity Violation of the N →Δ Transition (opens in a new tab)

  5. Precision measurement of the weak charge of the proton and parity violation in the N → ∆ transition

    … analog to the electric charge of the proton. Qweak measured the parity-violating asymmetry in elastic electron-proton scattering at an extreme forward angle (Q² = 0.0249 (GeV/c)² ). From the data gathered via the 1.16 GeV 180 μA longitudinally polarized electron beam scattering off the …

    vt Repository record for Precision measurement of the weak charge of the proton and parity violation in the N → ∆ transition (opens in a new tab)

  6. DIRECT DETERMINATION OF THE WEAK CHARGE OF THE PROTON VIA PARITY-VIOLATING ELECTRON SCATTERING

    … weak charge of the proton is determined via Qweak experiment at Thomas Jefferson Laboratory in Newport News, VA. A longitudinally polarized electron beam was scattered by a liquid hydrogen target. The spin direction of the electron beam was switched between left and right helicity states. The …

    syracuse-diss Repository record for DIRECT DETERMINATION OF THE WEAK CHARGE OF THE PROTON VIA PARITY-VIOLATING ELECTRON SCATTERING (opens in a new tab)

  7. Parity-Violating Elastic Electron Nucleon Scattering: Measurement of the Strange Quark Content of the Nucleon and Towards a Measurement of the Weak Charge of the Proton

    The experiments discussed in this thesis exploit parity violation in elastic electron proton scattering in order to measure properties of the nucleon. Both experiments make use of the high quality, highly polarized electron beam available at Thomas Jefferson National Accelerator Facility. …

    vt Repository record for Parity-Violating Elastic Electron Nucleon Scattering: Measurement of the Strange Quark Content of the Nucleon and Towards a Measurement of the Weak Charge of the Proton (opens in a new tab)

  8. Instrument Design Optimization with Computational Methods

    <p>Using Finite Element Analysis to approximate the solution of differential equations, two different instruments in experimental Hall C at the Thomas Jefferson National Accelerator Facility are analyzed. The time dependence of density fluctuations from the liquid hydrogen (LH2) target used in the …

    odu Repository record for Instrument Design Optimization with Computational Methods (opens in a new tab)