Erratum: Electric‐Quadrupole and Magnetic‐Dipole Radiation in Linear Molecules. Applications to 1Π–3Π Transitions

1969 ◽  
Vol 51 (12) ◽  
pp. 5734-5734
Author(s):  
Ying‐Nan Chiu
2014 ◽  
Vol 22 (9) ◽  
pp. 10693 ◽  
Author(s):  
D. L. Markovich ◽  
P. Ginzburg ◽  
A. K. Samusev ◽  
P. A. Belov ◽  
A. V. Zayats

2004 ◽  
Vol 69 (2) ◽  
Author(s):  
J. A. Alcántara-Núñez ◽  
J. R. B. Oliveira ◽  
E. W. Cybulska ◽  
N. H. Medina ◽  
M. N. Rao ◽  
...  

1988 ◽  
Vol 03 (01) ◽  
pp. 225-242 ◽  
Author(s):  
J.A. GRIFOLS ◽  
S. PERIS ◽  
J. SOLÅ

The experimental constraint on [Formula: see text] and the experimental rate of the process KL→μμ are used to bound hypothetical nonstandard self-interactions of the electroweak bosons. In particular, we give bounds on anomalous magnetic dipole and electric quadrupole moments of the charged weak boson.


Author(s):  
Xiao-Bo Zhang ◽  
Xin Qiao ◽  
Li-Hong Cheng ◽  
Ai-Xia Zhang ◽  
Ju-Kui Xue

1987 ◽  
Vol 34 (1-4) ◽  
pp. 87-89
Author(s):  
M. P. Avotina ◽  
T. I. Kracíková

Author(s):  
J. Pierrus

This chapter begins by expressing the multipole expansion of the dynamic vector potential A ( r, t) in terms of electric and magnetic multipole moments. Differentiation of A ( r, t) leads directly to the fields E ( r, t) and B ( r, t), which have a component transporting energy away from the sources to infinity. This component is called electromagnetic radiation and it arises only when electric charges experience an acceleration. A range of questions deal with the various types of radiation, including electric dipole and magnetic dipole–electric quadrupole. Larmor’s formula is applied in both its non-relativistic and relativistic forms. Also considered are some applications involving antennas, antenna arrays and the scattering of radiation by a free electron.


Sign in / Sign up

Export Citation Format

Share Document