1964
DOI: 10.1103/physrevlett.12.533
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Electron Cyclotron Maser

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Cited by 198 publications
(48 citation statements)
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“…Hirshfield and Bekefi (1963) pointed out that coherent mechanisms could be at work in planetary magnetospheres such as that of Jupiter when they endeavored to explain the observation of Jovian decametric radiation. Hirshfield and Wachtel (1964) actually demonstrated the emission in a laboratory experiment with relativistic electrons. Non-relativistic versions of electron-cyclotron maser emission had been developed in other papers by Gaponov (1959b), Harris (1959) (who suggested that certain non-thermal electron-velocity distributions favor the emission) and Sagdeev and Shafranov (1960).…”
Section: Historymentioning
confidence: 94%
“…Hirshfield and Bekefi (1963) pointed out that coherent mechanisms could be at work in planetary magnetospheres such as that of Jupiter when they endeavored to explain the observation of Jovian decametric radiation. Hirshfield and Wachtel (1964) actually demonstrated the emission in a laboratory experiment with relativistic electrons. Non-relativistic versions of electron-cyclotron maser emission had been developed in other papers by Gaponov (1959b), Harris (1959) (who suggested that certain non-thermal electron-velocity distributions favor the emission) and Sagdeev and Shafranov (1960).…”
Section: Historymentioning
confidence: 94%
“…Any escaping radiation is based on the dynamics of electrons. In the electron equation of motion it is bound to the third time derivative ··· v of the electron velocity v. Gyro and synchrotron radiation is thus weak (providing very weak energy losses only), though it is comparably easy to treat (see, e.g., Jackson, 1975) while, when detected, it maps temperature, magnetic field strength and mean plasma density (see, e.g., Rybicki and Lightman, 1979). Guided by the whistler instability, nonthermal radiation in the free space modes X and O from hot plasmas has early on provoked attempts to base it on thermal anisotropies in the electron distribution (Twiss and Roberts, 1958;Hirshfield and Bekefi, 1963;Melrose, 1976;Melrose and White, 1978).…”
Section: Review and Justificationmentioning
confidence: 99%
“…The feedback of the radiation, in case of a true laser system is usually secured by a Fabry-Perot type linear resonator arrangement. Besides, already in the sixties of the last century, in the context of cyclotron masers [32] and cavity electrodynamics, more general cavity effects have also been studied [33][34]. In the cyclotron maser the fundamental or low harmonics are generated, on the other hand, in the synchrotron radiation very high harmonics are dominant.…”
Section: Introductionmentioning
confidence: 99%