Computing the normalized dirac wave function for oblique electric and magnetic fields

1991 ◽  
Vol 106 (3) ◽  
pp. 253-261
Author(s):  
F. Melia ◽  
M. Fatuzzo
Keyword(s):  
Wave Function ◽  
Magnetic Fields ◽  
Electric And Magnetic Fields ◽  
Dirac Wave Function

scholarly journals The Quaternionic Commutator Bracket and Its Implications

Symmetry ◽  
2018 ◽  
Vol 10 (10) ◽  
pp. 513 ◽  
Author(s):  
Arbab Arbab ◽  
Mudhahir Al Ajmi
Keyword(s):  
Wave Function ◽  
Electromagnetic Field ◽  
Angular Momentum ◽  
Charged Particle ◽  
Magnetic Fields ◽  
Interaction Energy ◽  
Internal Structure ◽  
Magnetic Moments ◽  
Electric And Magnetic Fields ◽  
Aharonov Bohm

A quaternionic commutator bracket for position and momentum shows that the quaternionic wave function, viz. ψ ˜ = ( i c ψ 0 , ψ → ) , represents a state of a particle with orbital angular momentum, L = 3 ℏ , resulting from the internal structure of the particle. This angular momentum can be attributed to spin of the particle. The vector ψ → , points in an opposite direction of L → . When a charged particle is placed in an electromagnetic field, the interaction energy reveals that the magnetic moments interact with the electric and magnetic fields giving rise to terms similar to Aharonov–Bohm and Aharonov–Casher effects.

scholarly journals Field of a moving locked charge in classical electrodynamics

2020 ◽  
Vol 35 (32) ◽  
pp. 2050267
Author(s):  
Alexander J. Silenko
Keyword(s):  
Wave Function ◽  
Spatial Distribution ◽  
Magnetic Fields ◽  
Electric Field ◽  
Charge Density ◽  
Maxwell Equations ◽  
Classical Electrodynamics ◽  
Closed Space ◽  
Electric And Magnetic Fields ◽  
Average Electric Field

The paradox of a field of a moving locked charge (confined in a closed space) is considered and solved with the use of the integral Maxwell equations. While known formulas obtained for instantaneous fields of charges moving along straight and curved lines are fully correct, measurable quantities are average electric and magnetic fields of locked charges. It is shown that the average electric field of locked charges does not depend on their motion. The average electric field of protons moving in nuclei coincides with that of protons being at rest and having the same spatial distribution of the charge density. The electric field of a twisted electron is equivalent to the field of a centroid with immobile charges whose spatial distribution is defined by the wave function of the twisted electron.

INTRODUCTORY TALK ON EFFECTS OF ELECTRIC AND MAGNETIC FIELDS ON HIGH RYDBERG ATOMS

1982 ◽  
Vol 43 (C2) ◽  
pp. C2-13-C2-18
Author(s):  
S. Feneuille
Keyword(s):  
Magnetic Fields ◽  
Rydberg Atoms ◽  
Electric And Magnetic Fields

49. Evaluation of Electric and Magnetic Fields Around an Induction Cap Sealer

1999 ◽  
Author(s):  
F. Rosenthal ◽  
M. Carter ◽  
S. Hampton ◽  
T. Mays
Keyword(s):  
Magnetic Fields ◽  
Electric And Magnetic Fields

Electric and magnetic fields at power frequencies

2010 ◽  
Vol 29 (Supplement 1) ◽  
pp. 69-83
Author(s):  
Anthony B. Miller ◽  
Lois M. Green
Keyword(s):  
Magnetic Fields ◽  
Electric And Magnetic Fields

A System for Exposing Biological Objects to Variable Combinations of Electric and Magnetic Fields

1986 ◽  
Vol 5 (2) ◽  
pp. 171-185
Author(s):  
K. Saali ◽  
J. Juutilainen ◽  
T. Lahtinen
Keyword(s):  
Magnetic Fields ◽  
Biological Objects ◽  
Electric And Magnetic Fields

Exploiting Electric and Magnetic Fields for Underwater Characterization

2011 ◽  
Author(s):  
Gregory Schultz
Keyword(s):  
Magnetic Fields ◽  
Electric And Magnetic Fields

Development of a method of probing electric and magnetic fields in a plasma with beams of charged particles

1972 ◽  
Author(s):  
A. I. Morozov ◽  
B. V. Dauter ◽  
S. M. Temchin
Keyword(s):  
Magnetic Fields ◽  
Charged Particles ◽  
Electric And Magnetic Fields
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