1986
DOI: 10.1070/sm1986v055n02abeh003013
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The Linear Theory of Landau Damping

Abstract: Measurements of the variation of formation time of a Q-switched ruby laser as a function of loop gain are presented. The loop gains were calculated from integrated pump intensities and the measured resonator loss at threshold. The relationship between formation time and loop gain predicted by fast Q-switching theory was confirmed. Although large optical distortions are to be expected in rubies pumped to Q-switching levels, no indication of increasing resonator loss was found under these conditions.

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Cited by 30 publications
(19 citation statements)
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“…1. A number of other works regarding the linearized Vlasov equations followed, providing mathematically rigorous treatments, clarifications, and generalizations [1,10,16,17,29,32,38]. The phenomenon is now known as Landau damping and is a cornerstone of plasma physics in approximately collisionless regimes; see, e.g., [7,34,37].…”
Section: Landau Damping and Existing Resultsmentioning
confidence: 99%
“…1. A number of other works regarding the linearized Vlasov equations followed, providing mathematically rigorous treatments, clarifications, and generalizations [1,10,16,17,29,32,38]. The phenomenon is now known as Landau damping and is a cornerstone of plasma physics in approximately collisionless regimes; see, e.g., [7,34,37].…”
Section: Landau Damping and Existing Resultsmentioning
confidence: 99%
“…The mathematically rigorous theory of the linear damping was pioneered by Backus [4] and Penrose [73] as discussed above, and further clarified by many mathematicians, see e.g. [23,59]. Penrose seemed optimistic that Landau damping should occur in the nonlinear equations, and highlighted the fact that near equilibrium, the linear evolution would cause the nonlinear electric field to decay and that the nonlinear equations would be asymptotically linear.…”
Section: V N )mentioning
confidence: 99%
“…[23][24][25][26][27][28][29][30] The present study is concerned with the behavior of solutions at intermediate times that are neither asymptotically large ͑t → ϱ͒ nor asymptotically small ͑t → 0 + ͒ and, in particular, on the range of timescales from roughly one plasma period ͑the inverse of the electron plasma frequency͒ to hundreds or even thousands of plasma periods. [23][24][25][26][27][28][29][30] The present study is concerned with the behavior of solutions at intermediate times that are neither asymptotically large ͑t → ϱ͒ nor asymptotically small ͑t → 0 + ͒ and, in particular, on the range of timescales from roughly one plasma period ͑the inverse of the electron plasma frequency͒ to hundreds or even thousands of plasma periods.…”
Section: Introductionmentioning
confidence: 99%