Difference between revisions of "Electron and Proton Spin Resonance Induced by Circularly Polarized Radiation: A Classical Derivation"
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==Abstract== | ==Abstract== | ||
− | Classical electrodynamics is used to demonstrate electron and proton spin resonance induced by classical, monochromatic, circularly polarized radiation. The effect is present in SU(2) symmetry as indicated by the minimal prescription, whose covering group is O(3). The interaction Hamiltonian is shown to be, H = -aS3sZ ? k, where a is the electron or proton polarizability; S3 is the third Stokes parameter; sZ is the Pauli matrix; and k is a unit vector in Z. | + | Classical electrodynamics is used to demonstrate electron and proton spin resonance induced by classical, monochromatic, circularly polarized radiation. The effect is present in SU(2) symmetry as indicated by the minimal prescription, whose covering group is O(3). The interaction Hamiltonian is shown to be, H = -aS3sZ ? k, where a is the electron or proton polarizability; S3 is the third Stokes parameter; sZ is the Pauli matrix; and k is a unit vector in Z. |
− | [[Category:Electrodynamics]] | + | [[Category:Scientific Paper|electron proton spin resonance induced circularly polarized radiation classical derivation]] |
+ | |||
+ | [[Category:Electrodynamics|electron proton spin resonance induced circularly polarized radiation classical derivation]] |
Latest revision as of 19:30, 1 January 2017
Scientific Paper | |
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Title | Electron and Proton Spin Resonance Induced by Circularly Polarized Radiation: A Classical Derivation |
Read in full | Link to paper |
Author(s) | Lawrence B Crowell, Myron W Evans |
Keywords | Electron and proton spin resonance induced by radiation, B(3) field. |
Published | 1998 |
Journal | Apeiron |
Volume | 5 |
Number | 3-4 |
No. of pages | 4 |
Pages | 165-168 |
Read the full paper here
Abstract
Classical electrodynamics is used to demonstrate electron and proton spin resonance induced by classical, monochromatic, circularly polarized radiation. The effect is present in SU(2) symmetry as indicated by the minimal prescription, whose covering group is O(3). The interaction Hamiltonian is shown to be, H = -aS3sZ ? k, where a is the electron or proton polarizability; S3 is the third Stokes parameter; sZ is the Pauli matrix; and k is a unit vector in Z.