2020
DOI: 10.1088/1748-0221/15/01/p01016
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Microwave source with enhanced radiation power based on orbitron MASERs

Abstract: We have proposed the design of high power microwave source in a vacuum tube based on the theory of negative mass instability. The proposed source does not operate based on a slow-wave structure but instead makes use of accelerated charged particles. In our structure, an electron emitter injects the charged particles into to the cavity. Emitted particles move around the anode, which leads to electron acceleration and emission of electromagnetic waves with a specific frequency. In this paper, we have enhanced th… Show more

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Cited by 4 publications
(4 citation statements)
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“…As a result, the Q factor can be considered a relation between the real and imaginary parts of the ϖ. In addition, by considering perturbation theory, if changes in RI are homogenous, the difference in RI of samples shifts the resonance frequencies, which can be seen in the following equation where the permeability is constant; Equation (2) is simplified as [20]: ω(k)ωres=1WtruetruetrueV()δεε.WedV=1WtruetruetrueVδεrε0|Eres|2dV $\frac{\partial \omega (k)}{{\omega }_{res}}=-\frac{1}{W}\int \int \underset{V}{\int }\left(\frac{\delta \varepsilon }{\varepsilon }.We\right)dV=-\frac{1}{W}\int \int \underset{V}{\int }\left(\delta {\varepsilon }_{r}{\varepsilon }_{0}{\vert {E}_{res}\vert }^{2}\right)dV$ W e is the electric energy densit, W is the total energy stored in a cavity, E res is the original electric field, ɛ 0 represents the free space permittivity, ɛ r is the relative permittivity, and ω(k) $\partial \omega (k)$ represents the resonance shift. As we know n=εrμr $n=\sqrt{{\varepsilon }_{r}{\mu }_{r}}$ , which n is RI and ω(k)ωres $\frac{\partial \omega (k)}{{\omega }_{res}}$ can be considered as [8]: ω(k)ωres=σ()δnn $\frac{\partial \omega (k)}{{\omega }_{res}}=-\sigma \left(\frac{\delta n}{n}\right)$ …”
Section: Theory and Designmentioning
confidence: 99%
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“…As a result, the Q factor can be considered a relation between the real and imaginary parts of the ϖ. In addition, by considering perturbation theory, if changes in RI are homogenous, the difference in RI of samples shifts the resonance frequencies, which can be seen in the following equation where the permeability is constant; Equation (2) is simplified as [20]: ω(k)ωres=1WtruetruetrueV()δεε.WedV=1WtruetruetrueVδεrε0|Eres|2dV $\frac{\partial \omega (k)}{{\omega }_{res}}=-\frac{1}{W}\int \int \underset{V}{\int }\left(\frac{\delta \varepsilon }{\varepsilon }.We\right)dV=-\frac{1}{W}\int \int \underset{V}{\int }\left(\delta {\varepsilon }_{r}{\varepsilon }_{0}{\vert {E}_{res}\vert }^{2}\right)dV$ W e is the electric energy densit, W is the total energy stored in a cavity, E res is the original electric field, ɛ 0 represents the free space permittivity, ɛ r is the relative permittivity, and ω(k) $\partial \omega (k)$ represents the resonance shift. As we know n=εrμr $n=\sqrt{{\varepsilon }_{r}{\mu }_{r}}$ , which n is RI and ω(k)ωres $\frac{\partial \omega (k)}{{\omega }_{res}}$ can be considered as [8]: ω(k)ωres=σ()δnn $\frac{\partial \omega (k)}{{\omega }_{res}}=-\sigma \left(\frac{\delta n}{n}\right)$ …”
Section: Theory and Designmentioning
confidence: 99%
“…As a result, the Q factor can be considered a relation between the real and imaginary parts of the ϖ. In addition, by considering perturbation theory, if changes in RI are homogenous, the difference in RI of samples shifts the resonance frequencies, which can be seen in the following equation where the permeability is constant; Equation ( 2) is simplified as [20]:…”
Section: Theory and Designmentioning
confidence: 99%
See 1 more Smart Citation
“…Due to the periodic nature of PCs, they exhibit PBGs in all directions, acting as ideal mirrors for incident light waves. This property holds potential applications in different fileds suchas lasers [2], filters [3,4], optical waveguides [5][6][7][8][9], optical fibers [10][11][12], all-optical logic gates [12][13][14][15][16], biosensors [17][18][19], splitters [20,21], imaging [22] and all-optical analog to digital converters [23,24]. Also, PCs photonic crystals have found a highly practical application in the field of all-optical logic gates, garnering substantial attention because of their versatility in various all-optical signal processing applications.…”
Section: Introductionmentioning
confidence: 99%