Laser-induced damage threshold of the nonlinear crystals BaGa4Se7 and BaGa2GeSe6 at 2091 nm in the nanosecond regime

Nadezhda Yu. Kostyukova; Nadezhda Yu. Kostyukova; Nadezhda Yu. Kostyukova; Nadezhda Yu. Kostyukova; Andrey A. Boyko; Andrey A. Boyko; Andrey A. Boyko; Andrey A. Boyko; Ilya D. Eranov; Ilya D. Eranov; Oleg L. Antipov; Oleg L. Antipov; Dmitry B. Kolker; Dmitry B. Kolker; Anton I. Kostyukov; Evgenii Yu. Erushin; Evgenii Yu. Erushin; Evgenii Yu. Erushin; Ilya B. Miroshnichenko; Ilya B. Miroshnichenko; Dmitrii V. Badikov; Valeriy V. Badikov

doi:10.1364/JOSAB.396746

Journal of the Optical Society of America B
Vol. 37,
Issue 9,
pp. 2655-2659
(2020)
•https://doi.org/10.1364/JOSAB.396746

Laser-induced damage threshold of the nonlinear crystals BaGa₄Se₇ and BaGa₂GeSe₆ at 2091 nm in the nanosecond regime

Nadezhda Yu. Kostyukova, Andrey A. Boyko, Ilya D. Eranov, Oleg L. Antipov, Dmitry B. Kolker, Anton I. Kostyukov, Evgenii Yu. Erushin, Ilya B. Miroshnichenko, Dmitrii V. Badikov, and Valeriy V. Badikov

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Nadezhda Yu. Kostyukova, Andrey A. Boyko, Ilya D. Eranov, Oleg L. Antipov, Dmitry B. Kolker, Anton I. Kostyukov, Evgenii Yu. Erushin, Ilya B. Miroshnichenko, Dmitrii V. Badikov, and Valeriy V. Badikov, "Laser-induced damage threshold of the nonlinear crystals BaGa₄Se₇ and BaGa₂GeSe₆ at 2091 nm in the nanosecond regime," J. Opt. Soc. Am. B 37, 2655-2659 (2020)

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- Nonlinear or High Field Optics
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About this Article
History
- Original Manuscript: May 4, 2020
- Revised Manuscript: July 16, 2020
- Manuscript Accepted: July 21, 2020
- Published: August 18, 2020

Abstract

The surface laser-induced damage threshold (LIDT) of ${{\rm BaGa}_4}{{\rm Se}_7}$ and ${{\rm BaGa}_2}{{\rm GeSe}_6}$ nonlinear crystals was studied at 2091 nm. Both yellow and dark yellow phases of ${{\rm BaGa}_4}{{\rm Se}_7}$ were investigated. The Ho:YAG laser generating nanosecond pulses at 2 kHz, 5 kHz, and 10 kHz was used as a radiation source. The R-on-1 procedure was applied to determine the 0% probability damage threshold. The LIDT of the dark yellow phase of ${{\rm BaGa}_4}{{\rm Se}_7}$ without cleavage planes is very close to the ${{\rm BaGa}_2}{{\rm GeSe}_6}$ LIDT and exceeds by ca. 30% the LIDT of the yellow phase of ${{\rm BaGa}_4}{{\rm Se}_7}$ at 2 and 5 kHz.

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Tested Plates	Cut Angle	Dimensions
BGSe #1	$θ = {46.46}^{\circ}$	$12.7 \times 11.7 \times 1.5 m m$
yellow phase	$ϕ = 0^{\circ}$
BGSe #2	$θ = {46.46}^{\circ}$	$8.5 \times 15.4 \times 3.2 m m$
dark yellow phase	$ϕ = 0^{\circ}$
BGGSe #1	$θ = 30^{\circ}$	$10.0 \times 13.0 \times 1.9 m m$
	$ϕ = 30^{\circ}$
BGGSe #2	$θ = 30^{\circ}$	$7.0 \times 7.0 \times 2.5 m m$
	$ϕ = 0^{\circ}$

	$f_{p}$	2 kHz	5 kHz	10 kHz
BGSe#1	Surface	r(5)	r(4), b(1)	r(3), b(2)
	$2 ω$ (µm)	200	260	360
	$F_{0 %}$ ( $J / {c m}^{2}$ )	4.49	3.30	2.24
	$τ_{p}$ (ns)	13	15	17
	$I_{0 %}$ ( $M W / {c m}^{2}$ )	345	220	132
	$F_{c 0 %}$ ( $J / {c m}^{2}$ )	4.82	3.30	2.11
BGSe#2	Surface	r(4), b(1)	r(4), b(1)	r(4), b(1)
	$2 ω$ (µm)	200	260	360
	$F_{0 %}$ ( $J / {c m}^{2}$ )	6.15	5.06	2.66
	$τ_{p}$ (ns)	13	15	17
	$I_{0 %}$ ( $M W / {c m}^{2}$ )	473	337	157
	$F_{c 0 %}$ ( $J / {c m}^{2}$ )	6.61	5.06	2.50
BGGSe#1	Surface	r(4), b(1)	r(5)	r(3), b(2)
	$2 ω$ (µm)	200	260	360
	$F_{0 %}$ ( $J / {c m}^{2}$ )	6.05	4.33	2.84
	$τ_{p}$ (ns)	13	15	17
	$I_{0 %}$ ( $M W / {c m}^{2}$ )	466	289	167
	$F_{c 0 %}$ ( $J / {c m}^{2}$ )	6.50	4.33	2.67
BGGSe#2	Surface	r(5)	r(5)	r(4), b(1)
	$2 ω$ (µm)	200	260	360
	$F_{0 %}$ ( $J / {c m}^{2}$ )	6.07	4.25	2.97
	$τ_{p}$ (ns)	13	15	17
	$I_{0 %}$ ( $M W / {c m}^{2}$ )	467	283	175
	$F_{c 0 %}$ ( $J / {c m}^{2}$ )	6.50	4.25	2.67

Tested Plates	Cut Angle	Dimensions
BGSe #1	$θ = {46.46}^{\circ}$	$12.7 \times 11.7 \times 1.5 m m$
yellow phase	$ϕ = 0^{\circ}$
BGSe #2	$θ = {46.46}^{\circ}$	$8.5 \times 15.4 \times 3.2 m m$
dark yellow phase	$ϕ = 0^{\circ}$
BGGSe #1	$θ = 30^{\circ}$	$10.0 \times 13.0 \times 1.9 m m$
	$ϕ = 30^{\circ}$
BGGSe #2	$θ = 30^{\circ}$	$7.0 \times 7.0 \times 2.5 m m$
	$ϕ = 0^{\circ}$

	$f_{p}$	2 kHz	5 kHz	10 kHz
BGSe#1	Surface	r(5)	r(4), b(1)	r(3), b(2)
	$2 ω$ (µm)	200	260	360
	$F_{0 %}$ ( $J / {c m}^{2}$ )	4.49	3.30	2.24
	$τ_{p}$ (ns)	13	15	17
	$I_{0 %}$ ( $M W / {c m}^{2}$ )	345	220	132
	$F_{c 0 %}$ ( $J / {c m}^{2}$ )	4.82	3.30	2.11
BGSe#2	Surface	r(4), b(1)	r(4), b(1)	r(4), b(1)
	$2 ω$ (µm)	200	260	360
	$F_{0 %}$ ( $J / {c m}^{2}$ )	6.15	5.06	2.66
	$τ_{p}$ (ns)	13	15	17
	$I_{0 %}$ ( $M W / {c m}^{2}$ )	473	337	157
	$F_{c 0 %}$ ( $J / {c m}^{2}$ )	6.61	5.06	2.50
BGGSe#1	Surface	r(4), b(1)	r(5)	r(3), b(2)
	$2 ω$ (µm)	200	260	360
	$F_{0 %}$ ( $J / {c m}^{2}$ )	6.05	4.33	2.84
	$τ_{p}$ (ns)	13	15	17
	$I_{0 %}$ ( $M W / {c m}^{2}$ )	466	289	167
	$F_{c 0 %}$ ( $J / {c m}^{2}$ )	6.50	4.33	2.67
BGGSe#2	Surface	r(5)	r(5)	r(4), b(1)
	$2 ω$ (µm)	200	260	360
	$F_{0 %}$ ( $J / {c m}^{2}$ )	6.07	4.25	2.97
	$τ_{p}$ (ns)	13	15	17
	$I_{0 %}$ ( $M W / {c m}^{2}$ )	467	283	175
	$F_{c 0 %}$ ( $J / {c m}^{2}$ )	6.50	4.25	2.67

Nadezhda Yu. Kostyukova	https://orcid.org/0000-0002-4990-3759
Oleg L. Antipov	https://orcid.org/0000-0001-6095-6387

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Journal of the Optical Society of America B