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Probing low-mass vector bosons with parity nonconservation and nuclear anapole moment measurements in atoms and molecules

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arxiv 1709.10009 v2 pith:HRHWFSIL submitted 2017-09-28 physics.atom-ph hep-phnucl-th

classification physics.atom-phhep-phnucl-th
keywords vectoranapolenuclearbosonseffectsexchangeatomsboson
verification ladder T0 review T1 audit T2 compute T3 formal

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abstract

In the presence of P-violating interactions, the exchange of vector bosons between electrons and nucleons induces parity-nonconserving (PNC) effects in atoms and molecules, while the exchange of vector bosons between nucleons induces anapole moments of nuclei. We perform calculations of such vector-mediated PNC effects in Cs, Ba$^+$, Yb, Tl, Fr and Ra$^+$ using the same relativistic many-body approaches as in earlier calculations of standard-model PNC effects, but with the long-range operator of the weak interaction. We calculate nuclear anapole moments due to vector boson exchange using a simple nuclear model. From measured and predicted (within the standard model) values for the PNC amplitudes in Cs, Yb and Tl, as well as the nuclear anapole moment of $^{133}$Cs, we constrain the P-violating vector-pseudovector nucleon-electron and nucleon-proton interactions mediated by a generic vector boson of arbitrary mass. Our limits improve on existing bounds from other experiments by many orders of magnitude over a very large range of vector-boson masses.

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Forward citations

Cited by 2 Pith papers

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  1. The X17 Existence Hinted at by Nuclear Reactor Neutrinos

    hep-ph 2026-05 unverdicted novelty 6.0 of 10

    Reactor neutrino data from CONUS+ and Dresden-II combined with COHERENT and IceCube data singles out a region of neutrino and nuclear couplings consistent with the X17 particle.

  2. The X17 with Chiral Couplings

    hep-ph 2026-02 conditional novelty 6.0 of 10

    A spin-1 X17 with chiral couplings fits the ATOMKI nuclear anomalies at 99% CL only in a parameter region that atomic parity violation and KLOE-2/NA64 exclude, driven mainly by the 12C(17.23) transition.

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