Radiative Correction to Eikonal Functions in Electrodynamics

1970 ◽  
Vol 1 (8) ◽  
pp. 2316-2327 ◽  
Author(s):  
York-Peng Yao
Keyword(s):  
Radiative Correction ◽  
Eikonal Functions

Quantum Radiative Correction on the Mass of Electron in a Cavity

1997 ◽  
Vol 14 (1) ◽  
pp. 9-12
Author(s):  
Ni Guang-jiong ◽  
Chen Su-qing
Keyword(s):  
Radiative Correction

Radiative Correction to e+ e- ->   in Electroweak Theory

1987 ◽  
Vol 77 (1) ◽  
pp. 118-131 ◽  
Author(s):  
J. Fujimoto ◽  
M. Igarashi ◽  
Y. Shimizu
Keyword(s):  
Radiative Correction ◽  
Electroweak Theory

Radiative Correction toKl3Decay

1970 ◽  
Vol 1 (5) ◽  
pp. 1452-1468 ◽  
Author(s):  
T. Becherrawy
Keyword(s):  
Radiative Correction

scholarly journals THE THERMAL FORM OF THE PHOTOEFFECT WITH THE DEBYE AND THE WIGNER CRYSTAL

2021 ◽  
Vol 10 (1) ◽  
Author(s):  
Miroslav Pardy ◽  
Keyword(s):  
Specific Heat ◽  
Work Function ◽  
Radiative Correction ◽  
Photoelectric Effect ◽  
Wigner Crystal ◽  
Photon Propagator ◽  
Crystal Medium

We define the photoelectric effect with the specific heat term replacing the work function. The photon propagator involving the radiative correction is also considered. We consider the Debye specific head for the 3D crystal medium, the specific heat for the 2D medium and specific heat for the Wigner crystal.

scholarly journals Radiative corrections in 2 + 1 dimensional supergravity

2018 ◽  
Vol 96 (12) ◽  
pp. 1409-1412 ◽  
Author(s):  
D.G.C. McKeon
Keyword(s):  
Gauge Theory ◽  
Radiative Correction ◽  
Effective Action ◽  
Spin Connection ◽  
Dynamical Generation ◽  
Effective Lagrangian ◽  
Majorana Spinor ◽  
The One ◽  
Brst Invariance ◽  
Topological Mass

Supergravity in 2 + 1 dimensions has a set of first-class constraints that result in two bosonic and one fermionic gauge invariances. When one uses Faddeev–Popov quantization, these gauge invariances result in four fermionic scalar ghosts and two bosonic Majorana spinor ghosts. The BRST invariance of the effective Lagrangian is found. As an example of a radiative correction, we compute the phase of the one-loop effective action in the presence of a background spin connection, and show that it vanishes. This indicates that unlike a spinor coupled to a gauge field in 2 + 1 dimensions, there is no dynamical generation of a topological mass in this model. An additional example of how a BRST invariant effective action can arise in a gauge theory is provided in Appendix B where the BRST effective action for the classical Palatini action in 1 + 1 dimensions is examined.

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