2016
DOI: 10.1063/1.4942791
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Giant amplification in degenerate band edge slow-wave structures interacting with an electron beam

Abstract: We propose a new amplification regime based on synchronous operation of four degenerate electromagnetic (EM) modes in a slow-wave structure and the electron beam, referred to as super synchronization. These four EM modes arise in a Fabry-Pérot cavity (FPC) when degenerate band edge (DBE) condition is satisfied. The modes interact constructively with the electron beam resulting in superior amplification. In particular, much larger gains are achieved for smaller beam currents compared to conventional structures … Show more

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Cited by 43 publications
(72 citation statements)
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“…[10][11][12][13][14][15][16][17][18] However, a very few experiments have been carried out to actually generate high power microwaves with an electron beam passing through an MTM structure. [19][20][21][22][23] At MIT, in our previous experiment, 19 we built a structure with two MTM plates loaded in a waveguide with dimensions below the cut-off of the TM 11 mode.…”
Section: Introductionmentioning
confidence: 99%
“…[10][11][12][13][14][15][16][17][18] However, a very few experiments have been carried out to actually generate high power microwaves with an electron beam passing through an MTM structure. [19][20][21][22][23] At MIT, in our previous experiment, 19 we built a structure with two MTM plates loaded in a waveguide with dimensions below the cut-off of the TM 11 mode.…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, applications featuring slow-light properties associated with the DBE has been proposed such as small/directive antennas [12], [20]- [23], lowthreshold switching [10], [13], pulse compression [24], and filters [11]. The theory of four mode degeneracy was furthermore utilized for the first time to show giant gain enhancement [10] in slow-wave structures with DBE, for high power amplifiers [17] and oscillators [18], [25], when interacting with an electron beam. Since DBE involves four degenerate modes, it requires sophisticated theoretical framework to reveal its unique properties; such as coupled transmission line theory developed in [3], [6], with a nondiagonalizable system matrix.…”
Section: Introductionmentioning
confidence: 99%
“…At a fourth-order EPD, the transfer matrix becomes similar to a four-dimensional Jordan matrix, nde nd e nd e [22,70]. Similar to the second-order EPD, the wavenumber near a fourth-order EPD asymptotically follows the fractional power expansion…”
Section: I)mentioning
confidence: 83%
“…Note that the homogenous solutions of (3) are constructed from the four eigenvectors in (7) in the case where the matrix T can be diagonalized. When T is not diagonalizable, i.e., at an EPD, generalized eigenvectors are used instead of the regular eigenvectors in (7) [22]. The four eigenvalues of (7) are determined from…”
Section: A State Vector Evolution and Transfer Matrixmentioning
confidence: 99%
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