Measurement of parity violation in the elastic scattering of polarized electrons fromC12

1990 ◽  
Vol 65 (6) ◽  
pp. 694-697 ◽  
Author(s):  
P. A. Souder ◽  
R. Holmes ◽  
D.-H. Kim ◽  
K. S. Kumar ◽  
M. E. Schulze ◽  
...  
1985 ◽  
Vol 446 (1-2) ◽  
pp. 377-379 ◽  
Author(s):  
J. Ahrens ◽  
H.G. Andresen ◽  
H.-W. Blasius ◽  
A. Bornheimer ◽  
D. Conrath ◽  
...  

1988 ◽  
Vol 66 (6) ◽  
pp. 513-519
Author(s):  
Reiner Neuhausen

The standard theory of electroweak interactions predicts a parity nonconserving asymmetry in the order of 1 × 10−5 for the quasi-elastic scattering of 300 MeV longitudinally polarized electrons from nuclei at backward angles. The experimental setup for the detection of such small effects is described, and the procedure of data taking and analysis is discussed with regard to systematic uncertainties. The experimental asymmetry is found to be Aexp = (−3.51 ± 0.68 ± 0.20) × 10−6, where the first quoted error specifies the statistical uncertainty, the second one, the systematical. Aexp is interpreted in terms of model-independent coupling constants between the weak neutral current and the nucleon.


1988 ◽  
Vol 66 (6) ◽  
pp. 520-523 ◽  
Author(s):  
S. Kowalski

An experiment designed to measure precisely the parity-violating interference in the elastic scattering of longitudinally polarized electrons from 12C is under way at the Bates Accelerator Center. The experiment has required the construction of a high-intensity polarized injector whose successful operation has recently been demonstrated. Present efforts are aimed towards the understanding and control of sources of systematic errors.


2021 ◽  
Vol 2021 (6) ◽  
Author(s):  
P. S. Bhupal Dev ◽  
Werner Rodejohann ◽  
Xun-Jie Xu ◽  
Yongchao Zhang

Abstract The P2 experiment aims at high-precision measurements of the parity-violating asymmetry in elastic electron-proton and electron-12C scatterings with longitudinally polarized electrons. We discuss here the sensitivity of P2 to new physics mediated by an additional neutral gauge boson Z′ of a new U(1)′ gauge symmetry. If the charge assignment of the U(1)′ is chiral, i.e., left- and right-handed fermions have different charges under U(1)′, additional parity-violation is induced directly. On the other hand, if the U(1)′ has a non-chiral charge assignment, additional parity-violation can be induced via mass or kinetic Z-Z′ mixing. By comparing the P2 sensitivity to existing constraints, we show that in both cases P2 has discovery potential over a wide range of Z′ mass. In particular, for chiral models, the P2 experiment can probe gauge couplings at the order of 10−5 when the Z′ boson is light, and heavy Z′ bosons up to 79 (90) TeV in the proton (12C) mode. For non-chiral models with mass mixing, the P2 experiment is sensitive to mass mixing angles smaller than roughly 10−4, depending on model details and gauge coupling magnitude.


1976 ◽  
Vol 37 (19) ◽  
pp. 1258-1261 ◽  
Author(s):  
M. J. Alguard ◽  
W. W. Ash ◽  
G. Baum ◽  
J. E. Clendenin ◽  
P. S. Cooper ◽  
...  

1984 ◽  
Vol 29 (2) ◽  
pp. 538-552 ◽  
Author(s):  
B. Blankleider ◽  
R. M. Woloshyn

2007 ◽  
Vol 40 (20) ◽  
pp. 4119-4129 ◽  
Author(s):  
Md F Ahmed ◽  
W Ji ◽  
R P McEachran ◽  
A D Stauffer

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