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The Weak Charge of the Proton and New Physics
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The Weak Charge of the Proton and New Physics
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We address the physics implications of a precision determination of the weak charge of the proton, QWP, from a parity violating elastic electron proton scattering experiment to be performed at the Jefferson Laboratory. We present the Standard Model (SM) expression for QWP including one-loop radiative corrections, and discuss in detail the theoretical uncertainties and missing higher order QCD corrections. Owing to a fortuitous cancellation, the value of QWP is suppressed in the SM, making it a unique place to look for physics beyond the SM. Examples include extra neutral gauge bosons, supersymmetry, and leptoquarks. We argue that a QWP measurement will provide an important complement to both high energy collider experiments and other low energy electroweak measurements. The anticipated experimental precision requires the knowledge of the order alpha_s corrections to the pure electroweak box contributions. We compute these contributions for QWP, as well as for the weak charges of heavy elements as determined from atomic parity violation.
Forward citations
Cited by 2 Pith papers
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Relative enhancement of low-mass vector-boson exchange in higher waves matrix elements: parity non-conservation in hydrogen
A light Z' boson can mix hydrogen's 3p and 3d states with no Standard Model Z background, offering a potentially clean atomic probe of new physics.
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Parity Nonconservation in Hydrogen Induced by Low-Mass Vector-Boson Exchange
The ratio of low-mass Z' to SM Z contributions to PNC in hydrogen and deuterium is computed for arbitrary Z' mass, showing faster-than-1/Z² growth at low Z for both nuclear-spin-independent and dependent cases.
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