2006
DOI: 10.2528/pier06020701
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Time-Domain Analysis of Open Resonators. Analytical Grounds.

Abstract: Abstract-The paper is concerned with the development and mathematical justification of the methodology for applying the timedomain methods in the study of spectral characteristics of open electrodynamic resonant structures.

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Cited by 27 publications
(23 citation statements)
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“…The processing errors of the designed QOBR are also considered. Similar to the practical applications of a quasi-optical open resonator sustaining Gaussian modes [31][32][33][34][35][36][37][38], we believe that the designed QOBR, besides the production of Bessel-type modes, have many promising applications in millimeter range, such as frequency measurement, spectrum analysis, transmission characteristic research, power combination, and dielectric parameter measurement. Therefore, the study of the QOBR in these spectrum ranges has important practical significance.…”
Section: Discussionmentioning
confidence: 91%
“…The processing errors of the designed QOBR are also considered. Similar to the practical applications of a quasi-optical open resonator sustaining Gaussian modes [31][32][33][34][35][36][37][38], we believe that the designed QOBR, besides the production of Bessel-type modes, have many promising applications in millimeter range, such as frequency measurement, spectrum analysis, transmission characteristic research, power combination, and dielectric parameter measurement. Therefore, the study of the QOBR in these spectrum ranges has important practical significance.…”
Section: Discussionmentioning
confidence: 91%
“…8(a)). The amplitude of free-oscillating field U (g 1 , t) decreases with time t as exp(−t|Imk|), so the value of |Imk| and, thus the Q-factor, can be found (see [30][31][32] for methodology). For the combined compressor/radiator element considered here, Imk = −0.095 and the Q-factor (see (13) in Part I) is Q ≈ 1225.8.…”
Section: Combined Compressor/radiator Array Elementsmentioning
confidence: 99%
“…Indeed, proceeding from (24) to the generalized Cauchy problem [27] and using the fundamental solution G(λ, t) = χ(t)λ −1 sin λt of the operator D(λ) ≡ ∂ 2 t + λ 2 (see [14]), it becomes clear that both (20) and (24) define the same function w n1 (t, ϕ). From the equation in (4), it follows that w n1 (t, ϕ), µ n1 (ρ), and , ϕ)) .…”
Section: Exact Absorbing Conditions For Waveguide Units and Their Locmentioning
confidence: 99%
“…It should be noted here that the proposed method allows the transient analysis to be carried for long time intervals and can provide highly accurate and reliable numerical data pertinent to physical processes under resonant conditions [14,[23][24][25]. The proposed method is especially useful for accurate analysis of long-duration processes in resonant radiators and energy compressors with different types of storage units (e.g., waveguide and open resonators with metal, semitransparent, and frequency-selective mirrors) and switches (e.g., distributed grating-type switches, interference and resonant switches).…”
Section: Introductionmentioning
confidence: 99%