Revisiting parity nonconservation in cesium.

@article{Dzuba2012RevisitingPN,
  title={Revisiting parity nonconservation in cesium.},
  author={V. A. Dzuba and Julian C. Berengut and Victor V. Flambaum and Benjamin M. Roberts},
  journal={Physical review letters},
  year={2012},
  volume={109 20},
  pages={
          203003
        }
}
We apply the sum-over-states approach to calculate partial contributions to parity nonconservation (PNC) in cesium [Porsev, Beloy, and Drevianko, Phys. Rev. Lett. 102, 181601 (2009)]. We find significant corrections to two nondominating terms coming from the contribution of the core and highly excited states (n>9, the so called tail). When these differences are taken into account the result of Porsev et al., E(PNC)=0.8906(24)×10(-11)i(-Q(W)/N) changes to 0.8977 (40), coming into good agreement… 
Isotopic variation of parity violation in atomic ytterbium
The weak force is the only fundamental interaction known to violate the symmetry with respect to spatial inversion (parity). This parity violation can be used to isolate the effects of the weak
Enhanced nuclear-spin-dependent parity-violation effects using the HgH199 molecule
Electron interactions with the nuclear-spin-dependent (NSD) parity-nonconserving (PNC) anapole moment are strongly enhanced within heteronuclear diatomic molecules. A low-energy optical rotation
Confronting B anomalies with low-energy parity violation
Indirect searches have the potential to probe scales beyond the realm of direct searches. In this letter we consider the implications of two parity violating experiments: weak charge of proton
Measurement of parity violation in electron–quark scattering
TLDR
A measurement of the parity-violating asymmetry in electron–quark scattering yields a determination of 2C2u − C2d with a precision increased by a factor of five relative to the earlier result, providing evidence with greater than 95 per cent confidence that the C2q couplings are non-zero, as predicted by the electroweak theory.
The Qweak experiment: An overview and preliminary analysis
The Qweak experiment completed data taking at Jefferson Laboratory in 2012, with the aim of making the first experimental determination of the proton’s weak charge, QWp, which is the neutral-weak
Early Results from the Qweak Experiment
A subset of results from the recently completed Jefferson Lab Qweak experiment are reported. This experiment, sensitive to physics beyond the Standard Model, exploits the small parity-violating
First result from Qweak
Initial results are presented from the recently-completed Qweak experiment at Jefferson Lab. The goal is a precise measurement of the proton's weak charge Q p ,t o yield a test of the standard model
Probing the standard model with rare charm decays
This thesis comprises a study of rare charm decays in the standard model (SM) and beyond. Within an effective theory framework, we calculate the SM Wilson coefficients to (partly) next-to-next-to
Compilation of low-energy constraints on 4-fermion operators in the SMEFT
A bstractWe compile information from low-energy observables sensitive to flavor-conserving 4-fermion operators with two or four leptons. Our analysis includes data from e+e− colliders, neutrino
Optical-lattice-based method for precise measurements of atomic parity violation
We propose a method for measuring parity violation in neutral atoms. It is an adaptation of a seminal work by Fortson [Phys. Rev. Lett. 70, 2383 (1993)], proposing a scheme for a single trapped ion.
...
1
2
3
4
5
...