Indium iodide single crystal: breakthrough material for infrared acousto-optics

Dmitriy L. Porokhovnichenko; Evgeniy A. Dyakonov; Sergey V. Kuznetsov; Valerii V. Voronov; Pavel P. Fedorov; Kseniya S. Zaramenskikh; Ahmed A. Gasanov; Liya V. Zhukova; Alexandr S. Korsakov; Dmitrii D. Salimgareev

doi:10.1364/OL.393737

Optics Letters
Vol. 45,
Issue 13,
pp. 3435-3438
(2020)
•https://doi.org/10.1364/OL.393737

Indium iodide single crystal: breakthrough material for infrared acousto-optics

Dmitriy L. Porokhovnichenko, Evgeniy A. Dyakonov, Sergey V. Kuznetsov, Valerii V. Voronov, Pavel P. Fedorov, Kseniya S. Zaramenskikh, Ahmed A. Gasanov, Liya V. Zhukova, Alexandr S. Korsakov, and Dmitrii D. Salimgareev

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Dmitriy L. Porokhovnichenko, Evgeniy A. Dyakonov, Sergey V. Kuznetsov, Valerii V. Voronov, Pavel P. Fedorov, Kseniya S. Zaramenskikh, Ahmed A. Gasanov, Liya V. Zhukova, Alexandr S. Korsakov, and Dmitrii D. Salimgareev, "Indium iodide single crystal: breakthrough material for infrared acousto-optics," Opt. Lett. 45, 3435-3438 (2020)

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Abstract

Measurements of the refractive indices and the full set of longitudinal acousto-optical figures of merit in an orthorhombic single-crystal indium iodide (InI) were carried out. The high acousto-optic characteristics (${{\boldsymbol M}_2}$ up to $1100 \times {10^{ - 15}}\,\,{{\rm s}^3}\,{\rm kg}^{ - 1}$) and strong optical anisotropy ($\Delta {n} = 0.47$) make it possible to design various types of high-performance acousto-optic devices of the middle and far-infrared spectral range. In combination with a wide transparency range ($0.62 - 51\,\,{\unicode{x00B5}\rm m}$), the obtained characteristics make the crystal extremely promising in comparison with most existing analogs.

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			$M_{2} \times 10^{- 15}, s^{3} {k g}^{- 1}$	$M_{2} \times 10^{- 15}, s^{3} {k g}^{- 1}$
Material	Crystal System	Transparency Range, $µ m$	Longitudinal	Shear
InI [15]	orthorhombic	$0.62 \dots 51$	1100	n/a
KRS-5	cubic	$0.53 \dots 45$	1150	1200
KRS-6	cubic	$0.4 \dots 30$	715	880
Si	cubic	$1.5 \dots 10$	6	24
Ge	cubic	$1.5 \dots 22$	190	290
${H g}_{2} {C l}_{2}$	tetragonal	$0.38 \dots 20$	560	580
${H g}_{2} {B r}_{2}$	tetragonal	$0.42 \dots 30$	1150 (est.)	1700 (est.)
${H g}_{2} I_{2}$	tetragonal	$0.53 \dots 40$	3200 (est.)	5100 (est.)
${P b B r}_{2}$	orthorhombic	$0.36 \dots 30$	430	n/a

Ultrasound Wave		Electromagnetic Radiation		$M_{2} \times 10^{- 15} s^{3} {k g}^{- 1}$		$p_{e f f}$	$n$
Direction	Polarization	Direction	Polarization	$1.15 µ m$ [15]	$0.65 µ m$ [this Letter]	$p_{e f f}$	$n$
$x$	$x$	$z$	$x$	$1100 \pm 200$	$1100 \pm 100$	$p_{11}$	$n_{x}$
$x$	$x$	$y$	$x$	$1100 \pm 200$	$1100 \pm 100$	$p_{11}$
$y$	$y$	$z$	$x$	$120 \pm 25$	$300 \pm 50$	$p_{12}$
$z$	$z$	$y$	$x$	$120 \pm 25$	$300 \pm 50$	$p_{13}$
$x$	$x$	$z$	$y$	$90 \pm 20$		$p_{21}$	$n_{y}$
$y$	$y$	$z$	$y$	$260 \pm 50$		$p_{22}$
$y$	$y$	$x$	$y$		$230 \pm 20$	$p_{22}$
$z$	$z$	$x$	$y$		$80 \pm 10$	$p_{23}$
$x$	$x$	$y$	$z$		$110 \pm 25$	$p_{31}$	$n_{z}$
$y$	$y$	$x$	$z$		$110 \pm 10$	$p_{32}$
$z$	$z$	$x$	$z$		$860 \pm 80$	$p_{33}$

			$M_{2} \times 10^{- 15}, s^{3} {k g}^{- 1}$	$M_{2} \times 10^{- 15}, s^{3} {k g}^{- 1}$
Material	Crystal System	Transparency Range, $µ m$	Longitudinal	Shear
InI [15]	orthorhombic	$0.62 \dots 51$	1100	n/a
KRS-5	cubic	$0.53 \dots 45$	1150	1200
KRS-6	cubic	$0.4 \dots 30$	715	880
Si	cubic	$1.5 \dots 10$	6	24
Ge	cubic	$1.5 \dots 22$	190	290
${H g}_{2} {C l}_{2}$	tetragonal	$0.38 \dots 20$	560	580
${H g}_{2} {B r}_{2}$	tetragonal	$0.42 \dots 30$	1150 (est.)	1700 (est.)
${H g}_{2} I_{2}$	tetragonal	$0.53 \dots 40$	3200 (est.)	5100 (est.)
${P b B r}_{2}$	orthorhombic	$0.36 \dots 30$	430	n/a

Ultrasound Wave		Electromagnetic Radiation		$M_{2} \times 10^{- 15} s^{3} {k g}^{- 1}$		$p_{e f f}$	$n$
Direction	Polarization	Direction	Polarization	$1.15 µ m$ [15]	$0.65 µ m$ [this Letter]	$p_{e f f}$	$n$
$x$	$x$	$z$	$x$	$1100 \pm 200$	$1100 \pm 100$	$p_{11}$	$n_{x}$
$x$	$x$	$y$	$x$	$1100 \pm 200$	$1100 \pm 100$	$p_{11}$
$y$	$y$	$z$	$x$	$120 \pm 25$	$300 \pm 50$	$p_{12}$
$z$	$z$	$y$	$x$	$120 \pm 25$	$300 \pm 50$	$p_{13}$
$x$	$x$	$z$	$y$	$90 \pm 20$		$p_{21}$	$n_{y}$
$y$	$y$	$z$	$y$	$260 \pm 50$		$p_{22}$
$y$	$y$	$x$	$y$		$230 \pm 20$	$p_{22}$
$z$	$z$	$x$	$y$		$80 \pm 10$	$p_{23}$
$x$	$x$	$y$	$z$		$110 \pm 25$	$p_{31}$	$n_{z}$
$y$	$y$	$x$	$z$		$110 \pm 10$	$p_{32}$
$z$	$z$	$x$	$z$		$860 \pm 80$	$p_{33}$

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