2016
DOI: 10.1007/s00340-016-6559-9
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Spatial–temporal gain distribution of a CuBr vapor brightness amplifier

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Cited by 15 publications
(5 citation statements)
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“…The wavelengths of radiation are 510.6 nm (~70%) and 578.2 nm (~30%). The operation mode of the brightness amplifier was optimised to provide the beam shape close to Gaussian without the dip of intensity in the center [12]. Brightness amplifier operates at 20 kHz pulse repetition frequency with 50 ns amplified spontaneous emission pulse duration.…”
Section: Experimental Techniquementioning
confidence: 99%
See 1 more Smart Citation
“…The wavelengths of radiation are 510.6 nm (~70%) and 578.2 nm (~30%). The operation mode of the brightness amplifier was optimised to provide the beam shape close to Gaussian without the dip of intensity in the center [12]. Brightness amplifier operates at 20 kHz pulse repetition frequency with 50 ns amplified spontaneous emission pulse duration.…”
Section: Experimental Techniquementioning
confidence: 99%
“…Gaseous metal vapor active media have unique characteristics such as high single pass gain, high pulse repetition frequency, operation in a visible spectral region, high average power and ability to control laser radiation parameters [10][11][12][13][14][15]. This makes these media appropriate for use as brightness amplifiers in laser projection microscopes and laser monitors [16][17][18][19][20].…”
Section: Introductionmentioning
confidence: 99%
“…На основе данного усилителя яркости был реали-зован лазерный монитор, в котором удалось визуализировать объекты, расположенные на расстоянии 10 m. При этом временная зависимость усиления и передачи контраста в таких усилителях яркости до сих пор не изучена. О временной зависимости усиления и оптимальной временной задержке сообщается в работе [9] для усилителя яркости с типичной длительностью.…”
Section: поступило в редакцию 6 апреля 2017 гunclassified
“…Gaseous metal vapor active media have unique characteristics such as narrow natural bandwidth of amplification, high single pass gain, high pulse repetition frequency, operation in the visible spectral region, high average power and ability to control laser radiation parameters [18][19][20][21][22][23][24][25][26], which make them appropriate for use as brightness amplifiers in laser monitors. These imaging systems allow observation through the flame or plasma and visualization of the processes shielded by intensive background lighting.…”
Section: Introductionmentioning
confidence: 99%