2012
DOI: 10.1007/s11141-012-9310-3
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Applied research using a 30 GHz free-electron maser: Experimental study of interacton of high-power pulsed radiation with metals

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Cited by 7 publications
(3 citation statements)
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“…For the sake of calculation simplicity, the input (upstream) Bragg reflector was replaced by a lumped mirror with the reflection coefficient R in ¼ 1. The efficiency of LF generation in these regimes was about 3%-5%, which is much lower compared with the results of the previous experiments [1][2][3][4] and can be explained by the fact that the optimal beam parameters for the high-harmonic radiation are substantially different from those of the conventional single-frequency FEM regime. It should also be noted that for the chosen cavity geometry the radiation at harmonics higher than s > 3 and n > 2 was rather small.…”
Section: Figcontrasting
confidence: 67%
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“…For the sake of calculation simplicity, the input (upstream) Bragg reflector was replaced by a lumped mirror with the reflection coefficient R in ¼ 1. The efficiency of LF generation in these regimes was about 3%-5%, which is much lower compared with the results of the previous experiments [1][2][3][4] and can be explained by the fact that the optimal beam parameters for the high-harmonic radiation are substantially different from those of the conventional single-frequency FEM regime. It should also be noted that for the chosen cavity geometry the radiation at harmonics higher than s > 3 and n > 2 was rather small.…”
Section: Figcontrasting
confidence: 67%
“…Evidently, for the efficient LF and HF coexcitation by the same electron beam all the conditions (2), (4), and (6) should be fulfilled simultaneously. Figure 2 presents a dispersion diagram illustrating interaction of the beam electrons with LF and HF waves in the FEM multiplier.…”
Section: Operating Principles and Simulations Of The Fem Multipliersmentioning
confidence: 99%
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