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Picosecond pulse generation in InGaN blue lasers with saturable absorber

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dc.contributor.author DOBROVOLSCHI, V.
dc.contributor.author RUSU, S.
dc.contributor.author TRONCIU, V.
dc.date.accessioned 2024-11-26T13:37:44Z
dc.date.available 2024-11-26T13:37:44Z
dc.date.issued 2024
dc.identifier.citation DOBROVOLSCHI, V.; S.RUSU and V.TRONCIU. Picosecond pulse generation in InGaN blue lasers with saturable absorber. In: Materials Science and Condensed-Matter Physics: MSCMP: 10th International Conference dedicated to the 60th anniversary from the foundation of the Institute of Applied Physics, October 1-4, 2024. Book of abstracts. Chişinău: CEP USM, 2024, p. 57. ISBN 978-9975-62-763-4. en_US
dc.identifier.isbn 978-9975-62-763-4
dc.identifier.uri http://repository.utm.md/handle/5014/28627
dc.description Only Abstract. en_US
dc.description.abstract In this paper we report the results of theoretical investigations of generation of ps-pulses by blue InGaN with saturable absorber. We study numerically, using the single mode rate equations, the influence of wavelength of laser, and the length of saturable absorber on the features of output pulses. We investigate also, the impact of different material and laser parameters on properties of pulses. The mechanism belong to pulse generation is also presented. Finally, we discuss the applications of ps-pulses in distant measurements, free-space communications, material processing and spectroscopy. Figure 1 shows an analytical model of investigated setup. It consists of an InGaN active layer and a saturable absorber (SA). The active layer is composed by six QWs, and the emitting wavelength is 405 nm. Lasers with different cavity length and wavelengths have been investigated theoretically. To simulate the generation of pulses in an InGaN lasers we use the single mode model [1], which is given by the following rate equations for photon number S and injected carrier number n1 in active region and n2 in the saturable absorber. We integrate numerically this set of equations by studying the features of pulses in dependence of laser wavelength and length of SA. Figure 3 shows the dependence of pulse energy and maximum of output pulse on the laser wavelength. One can see that a large wavelength implies a low maximum of pulses, as well as a decrease of their energy. Figures 3 c) and d) shows the dependence of the same pulse features on length of SA. Large SA length lead to low energy and peak of pulse due to the increase of losses in SA. We believe that our work provides a good basis for future experimental study of pico-seconds pulses generated by blue InGaN laser with saturable absorber. en_US
dc.language.iso en en_US
dc.publisher Institute of Applied Physics, Moldova State University en_US
dc.rights Attribution-NonCommercial-NoDerivs 3.0 United States *
dc.rights.uri http://creativecommons.org/licenses/by-nc-nd/3.0/us/ *
dc.subject blue InGaN en_US
dc.subject laser en_US
dc.subject wavelength en_US
dc.title Picosecond pulse generation in InGaN blue lasers with saturable absorber en_US
dc.type Article en_US


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