2019
DOI: 10.1016/j.ppnp.2018.08.002
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New physics searches in nuclear and neutron β decay

Abstract: The status of tests of the standard electroweak model and of searches for new physics in allowed nuclear β decay and neutron decay is reviewed including both theoretical and experimental developments. The sensitivity and complementarity of recent and ongoing experiments are discussed with emphasis on their potential to look for new physics. Measurements are interpreted using a model-independent effective field theory approach enabling to recast the outcome of the analysis in many specific new physics models. S… Show more

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Cited by 240 publications
(304 citation statements)
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References 546 publications
(1,271 reference statements)
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“…The hadronic uncertainty of the forward γZ-box correction has recently raised a significant interest [28][29][30][31][32][33][34][35][36][37][38][39][40] in the context of a precision determination of the weak mixing angle with parity-violating electron scattering [41,42]. Similarly, recent works on reducing hadronic and nuclear uncertainties of the γWbox correction [43][44][45][46][47] prove central in extracting the V ud element of the Cabibbo-Kobayashi-Maskawa (CKM) matrix and testing the CKM unitarity, a sensitive probe of the SM extensions [48]. Experimental observables explicitly sensitive to the TPE mechanism are instrumental in developing a dispersion-theoretical framework for TPE.The lepton-proton scattering amplitude in presence of TPE can be parameterized in terms of six generalized form factorsG E (Q 2 , ε),G M (Q 2 , ε) andF i (Q 2 , ε), i = 3, ..., 6 [49], where Q 2 is the negative four-momentum transfer squared, and ε = (1 + 2(1 + Q 2 4M 2 ) tan 2 θ 2 ) −1 , with M and θ being the nucleon mass and the lepton scattering angle, respectively.…”
mentioning
confidence: 99%
“…The hadronic uncertainty of the forward γZ-box correction has recently raised a significant interest [28][29][30][31][32][33][34][35][36][37][38][39][40] in the context of a precision determination of the weak mixing angle with parity-violating electron scattering [41,42]. Similarly, recent works on reducing hadronic and nuclear uncertainties of the γWbox correction [43][44][45][46][47] prove central in extracting the V ud element of the Cabibbo-Kobayashi-Maskawa (CKM) matrix and testing the CKM unitarity, a sensitive probe of the SM extensions [48]. Experimental observables explicitly sensitive to the TPE mechanism are instrumental in developing a dispersion-theoretical framework for TPE.The lepton-proton scattering amplitude in presence of TPE can be parameterized in terms of six generalized form factorsG E (Q 2 , ε),G M (Q 2 , ε) andF i (Q 2 , ε), i = 3, ..., 6 [49], where Q 2 is the negative four-momentum transfer squared, and ε = (1 + 2(1 + Q 2 4M 2 ) tan 2 θ 2 ) −1 , with M and θ being the nucleon mass and the lepton scattering angle, respectively.…”
mentioning
confidence: 99%
“…This calculation was performed without the inclusion of electromagnetism, at a single lattice spacing and volume, and at the SU(3) flavor-symmetric point with degenerate up, down and strange quark masses corresponding to a larger-than-physical pion mass of m π ∼ 806 MeV. While all of these caveats are possibly important, the key qualitative result of that work was to reveal the potential significance of an operator that contributes to the ββ-decay of nuclei, but not to single-β decays, namely the isotensor axial polarizability, β (2) A , of the 1 S 0 two-nucleon system. This polarizability is defined from M 2ν GT by subtracting the term corresponding to an intermediate deuteron state, i.e., the 'Born' term as in forward Compton scattering:…”
Section: Neutrinoful Double-β Decaymentioning
confidence: 99%
“…The coefficient of the term linear in t in Eq. (46), which determines the isotensor axial polarizability β (2) A defined in Eq. (41), can be extracted from the large-time limit of…”
Section: Lattice Qcd Calculationsmentioning
confidence: 99%
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“…There are many past and current experiments to measure these decay parameters such as lifetimes, angular/spin correlations, and energy spectra, to name a few [1][2][3][4][5][6][7]. The Fierz interference term is one such decay parameter in the neutron β-decay rate (explained below) which vanishes in the Standard Model but would serve as a probe for beyond Standard Model physics in scalar and tensor couplings [1,4,8,9].In this publication, the UCNA collaboration presents a measurement of the Fierz interference term, b n , using the energy-dependence of the neutron β-decay asymmetry for the 2010 [10], and 2011-2013 data-taking runs [11]. For completeness, the electron energy spectra from the 2011-2013 data-taking runs are also used to extract b n arXiv:1911.05829v1 [nucl-ex]…”
mentioning
confidence: 99%