1983
DOI: 10.1103/physreva.27.1427
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Quantum fluctuations and transverse effects in superfluorescence

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Cited by 52 publications
(5 citation statements)
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“…In those earlier studies, the pump pulse is typically along the long axis direction of the gas sample that is typically about several centimeters long [17,19]. Theoretical analysis included both propagation retardation and transverse diffractive effects [25,26]. In the recent MIT experiment, the sample size is much smaller and the pump pulse is along the transverse direction of the long axis [4].…”
Section: Sequential Superradiancementioning
confidence: 99%
“…In those earlier studies, the pump pulse is typically along the long axis direction of the gas sample that is typically about several centimeters long [17,19]. Theoretical analysis included both propagation retardation and transverse diffractive effects [25,26]. In the recent MIT experiment, the sample size is much smaller and the pump pulse is along the transverse direction of the long axis [4].…”
Section: Sequential Superradiancementioning
confidence: 99%
“…The delay time statistics and timing jitter of SR pulses in atomic (molecular) ensembles have been thoroughly studied previously by both classical and quantum mechanical approaches. In some conditions, the standard deviation of the SR delay time was found to be 10-12 % [30,31]. However, the results of previous studies can hardly be applied to our case of semiconductor laser structures.…”
Section: Resultsmentioning
confidence: 73%
“…ε -средняя (по резонатору и по частотам генерации) диэлектрическая проницаемость матрицы активной среды, усредненный фактор заполненияŴ ≤ 1 учитывает возможное отличие профиля моды от профиля концентрации активных центров [15][16][17]. Несмотря на то что обсуждавшееся ранее время жизни фотона T E в " холодном" (т. е. при n ≡ 0) резонаторе играет важнейшую роль в динамике лазера, соответствующая безразмерная скорость релаксации поля в различных модах Ŵ E = 1/(ν c T E ) явно в уравнениях не фигурирует, а задается неявно брэгговской модуляцией диэлектрической проницаемости и граничными условиями на зеркалах лазерного резонатора с коэффициентом отражения R (для простоты мы не учитываем возможные омические и дифракционные потери):…”
Section: единая модель лазеров класса B C и Dunclassified