2015
DOI: 10.1103/physrevlett.115.114802
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Generation of Electromagnetic Fields of Extremely High Intensity by Coherent Summation of Cherenkov Superradiance Pulses

Abstract: We demonstrate both theoretically and experimentally the possibility of correlating the phase of a Cherenkov superradiance (SR) pulse to the sharp edge of a current pulse, when spontaneous emission of the electron bunch edge serves as the seed for SR processes. By division of the driving voltage pulse across several parallel channels equipped with independent cathodes we can synchronize several SR sources to arrange a two-dimensional array. In experiments carried out, coherent summation of radiation from four … Show more

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Cited by 72 publications
(19 citation statements)
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“…Ginzburg et al [12] have successfully demonstrated the coherent summation of Cherenkov sources, which provides a pathway to achieving very high intensity fields by combining several sources.…”
Section: Cherenkov Sourcesmentioning
confidence: 99%
“…Ginzburg et al [12] have successfully demonstrated the coherent summation of Cherenkov sources, which provides a pathway to achieving very high intensity fields by combining several sources.…”
Section: Cherenkov Sourcesmentioning
confidence: 99%
“…There are high-power, high-efficiency rf sources with controllable phase at frequencies above X-band [1][2][3][4]. These sources can have output powers from tens of megawatts to gigawatts, pulse length varying from nanoseconds to microseconds, and repetition rates the might reach the kilohertz level.…”
Section: High-power Rf Sources and Traveling-wave Accelerator Resonatorsmentioning
confidence: 99%
“…There are nanosecond, GW power level, rf Cherenkov sources driven by relativistic beams with repetition rate up to 1 kHz [3,4]. Rf phase is controllable by either a low power master-source (in amplifiers) or by precise synchronization with the voltage front (in oscillators).…”
Section: Traveling-wave Gun Fed By a Nanosecond Rf Pulsementioning
confidence: 99%
“…The reason is that TE 11 mode is the lowest mode which is propagating in an oversize waveguide. The TE 11 − ⊥, ∥ directions according to waveguide wall with angle θ each plane makes with parallel axis. k sin θ = k ⊥ and k cos θ = β z = k ∥ (propagation constant inside waveguide).…”
Section: Power Combiner With the Output Te 11 -Modementioning
confidence: 99%
“…Also, in Ref. 11 it was demonstrated that by dividing the driving voltage pulse across several parallel channels equipped with independent cathodes, four synchronized superradiant sources in the form of a 2D array can be achieved which can generate fields of extremely high intensity.…”
Section: Introductionmentioning
confidence: 99%