Equilibrium of random classical electromagnetic radiation in the presence of a nonrelativistic nonlinear electric dipole oscillator

1976 ◽  
Vol 13 (10) ◽  
pp. 2832-2845 ◽  
Author(s):  
Timothy H. Boyer
Keyword(s):  
Electromagnetic Radiation ◽  
Electric Dipole ◽  
Dipole Oscillator

Electromagnetic radiation

2018 ◽  
Author(s):  
J. Pierrus
Keyword(s):  
Electromagnetic Radiation ◽  
Magnetic Dipole ◽  
Antenna Arrays ◽  
Electric Dipole ◽  
Free Electron ◽  
Vector Potential ◽  
Electric Quadrupole ◽  
Multipole Expansion ◽  
Multipole Moments

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.

scholarly journals Electromagnetic radiation and the self-field of a spherical dipole oscillator

2020 ◽  
Vol 88 (9) ◽  
pp. 693-703
Author(s):  
Masud Mansuripur ◽  
Per K. Jakobsen
Keyword(s):  
Electromagnetic Radiation ◽  
The Self ◽  
Dipole Oscillator

Multichannel calculation of the electric-dipole oscillator strengths for the discrete 1Se1Po transitions in helium within the hyperspherical adiabatic approach

1991 ◽  
Vol 152 (9) ◽  
pp. 467-471 ◽  
Author(s):  
A.G. Abrashkevich ◽  
D.G. Abrashkevich ◽  
M.I. Gaysak ◽  
V.I. Lendyel ◽  
I.V. Puzynin ◽  
...  
Keyword(s):  
Electric Dipole ◽  
Oscillator Strengths ◽  
Adiabatic Approach ◽  
Dipole Oscillator ◽  
Hyperspherical Adiabatic

Electric Dipole Oscillator Strengths and Radiative Lifetimes in the Boron Isoelectronic Sequence

1987 ◽  
Vol 499 (6) ◽  
pp. 412-418 ◽  
Author(s):  
Th. M. El-Sherbini ◽  
A. A. Farrag ◽  
H. M. Mansour ◽  
A. A. Rahman
Keyword(s):  
Electric Dipole ◽  
Oscillator Strengths ◽  
Isoelectronic Sequence ◽  
Radiative Lifetimes ◽  
Dipole Oscillator

Systematic Trends in Atomic Oscillator Strengths: The Helium Isoelectronic Sequence

1972 ◽  
Vol 50 (12) ◽  
pp. 1363-1369 ◽  
Author(s):  
M. Cohen ◽  
R. P. McEachran
Keyword(s):  
Electric Dipole ◽  
Nuclear Charge ◽  
Principal Quantum Number ◽  
Wave Functions ◽  
Oscillator Strengths ◽  
Isoelectronic Sequence ◽  
Dipole Oscillator ◽  
Good Agreement ◽  
Comparison Data ◽  
Dipole Length

Electric dipole oscillator strengths (f values) have been calculated for a large number of singlet and triplet S–P, P–D, and D–F transitions in the helium isoelectronic sequence through O+6. The analytical orbital wave functions employed were of frozen-core type, and generally produce very good agreement between length and velocity values of the calculated oscillator strengths. A conspicuous exception occurs in many cases where the principal quantum number remains unchanged in the transition, and the more reliable dipole length values have been adopted for such transitions. The smooth variation of the calculated f values as functions of the inverse of the nuclear charge Z provided a sensitive check on the accuracy of the computations and indicated a considerable number of P–D transitions where the velocity values seemed the more reliable. Wherever comparison data are available, our calculated oscillator strengths are in excellent agreement with the most accurate values; in other cases, the absolute uncertainty in the f values should in no case exceed 5%.

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