On the electroweak mixing angle in E(∞)

2000 ◽  
Vol 11 (11) ◽  
pp. 1803-1807 ◽  
Author(s):  
M.S. El Naschie
2005 ◽  
Vol 731 (1-2) ◽  
pp. 213-224 ◽  
Author(s):  
W. Hollik ◽  
U. Meier ◽  
S. Uccirati

1986 ◽  
Vol 177 (3-4) ◽  
pp. 446-452 ◽  
Author(s):  
J.V. Allaby ◽  
U. Amaldi ◽  
G. Barbiellini ◽  
M. Baubillier ◽  
F. Bergsma ◽  
...  

1993 ◽  
Vol 309 (3-4) ◽  
pp. 451-462 ◽  
Author(s):  
O. Adriani ◽  
M. Aguilar-Benitez ◽  
S. Ahlen ◽  
J. Alcaraz ◽  
A. Aloisio ◽  
...  

1998 ◽  
Vol 13 (38) ◽  
pp. 3099-3107 ◽  
Author(s):  
M. MALTONI ◽  
M. I. VYSOTSKY

It happens that s2 and ŝ2 are equal with 0.1% accuracy, though they are split by radiative corrections and a natural estimate for their difference is 1%. This degeneracy occurs only for mt value close to 170 GeV, so no deep physical reason can be attributed to it. However, another puzzle of the standard model, the degeneracy of [Formula: see text] and s2, is not independent of the previous one since a good physical reason exists for [Formula: see text] and ŝ2 degeneracy. We present explicit formulas which relate these three angles.


2019 ◽  
Vol 214 ◽  
pp. 06022
Author(s):  
Dimitri Bourilkov

The use of machine learning techniques for classification is well established. They are applied widely to improve the signal-to-noise ratio and the sensitivity of searches for new physics at colliders. In this study I explore the use of machine learning for optimizing the output of high precision experiments by selecting the most sensitive variables to the quantity being measured. The precise determination of the electroweak mixing angle at the Large Hadron Collider using linear or deep neural network regressors is developed as a test case.


1989 ◽  
Vol 232 (4) ◽  
pp. 539-548 ◽  
Author(s):  
D. Geiregat ◽  
P. Vilain ◽  
G. Wilquet ◽  
F. Bergsma ◽  
U. Binder ◽  
...  

2011 ◽  
Vol 89 (1) ◽  
pp. 69-72 ◽  
Author(s):  
G. S. Giri ◽  
O. O. Versolato ◽  
L. W. Wansbeek ◽  
J. E. van den Berg ◽  
D. J. van der Hoek ◽  
...  

Atomic parity violation (APV) can be measured in a single Ra+ ion, enabling a precise measurement of the electroweak mixing angle in the Standard Model of particle physics at low momentum transfer. This provides sensitivity to new particles such as extra Z0 bosons or leptoquarks. The Weinberg angle can be measured via a determination of the light shift in the forbidden 72S1/2–62D3/2 transition in a single trapped Ra+. Ultra-narrow transitions in such an ideal system can also be exploited to realize a high stability frequency standard. At the TRIμP facility of KVI, we have succeeded in the production of a series of radioactive short-lived radium isotopes. The radium isotopes produced were stopped and thermalized to Ra+ in a thermal ionizer, mass separated in a Wien filter, cooled in a gas filled radio frequency quadrupole and subsequently trapped as a cloud in a linear Paul trap. Laser spectroscopy in the trapped radium ions has been performed. The results of hyperfine structure, isotope shift, and lifetime measurements are important experimental inputs to test the accuracy of atomic theory, the precision of which is indispensable for extracting the Weinberg angle. These results are also of relevance for a possible atomic clock, based on trapped Ra+.


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