Spatial–temporal gain distribution of a CuBr vapor brightness amplifier / F. A. Gubarev [et al.]

Уровень набора: Applied Physics B, Lasers and OpticsАльтернативный автор-лицо: Gubarev, F. A., specialist in the field of electronics, Associate Professor of Tomsk Polytechnic University, Candidate of physical and mathematical sciences, 1979-, Fedor Aleksandrovich;Li Lin, specialist in the field of electronics, research engineer at Tomsk Polytechnic University, 1990-;Klenovsky, M. S., Miron Stanislavovich;Shiyanov, D. V., specialist in the field of electronics, Engineer of Tomsk Polytechnic University, 1973-, Dmitry ValeryevichКоллективный автор (вторичный): Национальный исследовательский Томский политехнический университет (ТПУ), Институт неразрушающего контроля (ИНК), Кафедра промышленной и медицинской электроники (ПМЭ)Язык: английский.Резюме или реферат: The paper presents the results of study of the radial distribution of radiation inside the copper bromide vapor amplifiers depending on the time of return of their own reflected radiation. This technique allows us to estimate the changes of the gain profile during the lasing pulse. The profile distribution which is close to the Gaussian’s one is as follows for the first 7–12 ns without the addition of HBr and up to 18 ns with HBr. By the end of the lasing pulse, the profile becomes ring-shaped. The results from this study indicate that the inversion in the center of the beam disappears earlier than at the periphery. This is equally true for both the green lasing line (510.6 nm) and the yellow one (578.2 nm). The radiation profile can be flattened partially by introducing the active HBr doping, but it does not provide a uniform profile throughout the lasing pulse..Примечания о наличии в документе библиографии/указателя: [References: 48 tit.].Аудитория: .Тематика: электронный ресурс | труды учёных ТПУ | пространственно-временное распределение | усиление Ресурсы он-лайн:Щелкните здесь для доступа в онлайн
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[References: 48 tit.]

The paper presents the results of study of the radial distribution of radiation inside the copper bromide vapor amplifiers depending on the time of return of their own reflected radiation. This technique allows us to estimate the changes of the gain profile during the lasing pulse. The profile distribution which is close to the Gaussian’s one is as follows for the first 7–12 ns without the addition of HBr and up to 18 ns with HBr. By the end of the lasing pulse, the profile becomes ring-shaped. The results from this study indicate that the inversion in the center of the beam disappears earlier than at the periphery. This is equally true for both the green lasing line (510.6 nm) and the yellow one (578.2 nm). The radiation profile can be flattened partially by introducing the active HBr doping, but it does not provide a uniform profile throughout the lasing pulse.

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