Three-dimensional dirac semi-metal material-based infrared saturable absorption device
A three-dimensional Dirac semi-saturable absorption technology, applied in the field of lasers, can solve problems such as reducing the repeatability of devices, limiting the generation and optimization of infrared pulsed lasers, and having no reliable control scheme for nonlinear optical parameters.
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Embodiment 1
[0029] Embodiment 1: This embodiment provides a design scheme of a reflective three-dimensional Dirac semi-metal material infrared saturable absorption device. to combine image 3 As shown, the specific scheme is as follows; the functional layer (1) is deposited on one side of the gallium arsenide substrate (2) polished on both sides by laser pulse deposition, including optical anti-reflection coating and Al 2 o 3 passivation layer. Then a 200nm three-dimensional Dirac semimetal Cd was grown on the other side of the GaAs substrate using molecular beam epitaxy. 3 As 2 Thin films (3) were finally evaporated on Cd using electron beam 3 As 2 A 1 μm gold film (4) was evaporated on the surface. Among them, Cd 3 As 2 The specific conditions for thin film molecular beam epitaxy growth are as follows: the use of purity ~ 99.999% (5N) cadmium source and arsenic source, the initial pressure in the equipment chamber is about 10 -8 mbar; grow Cd under the condition of substrate te...
Embodiment 2
[0030] Embodiment 2: This embodiment provides a specific design scheme of a transmission-type three-dimensional Dirac semi-metal material infrared saturable absorption device. Such as Figure 4 As shown, Cd with a thickness of 200 nm was grown on the surface of GaAs(2) by molecular beam epitaxy 3 As 2 Thin film (3), then functional layers (1) (optical anti-reflection coating and passivation layer) were coated on both sides of the device using electron beam evaporation.
Embodiment 3
[0031] Embodiment 3: This embodiment provides a design scheme of a semiconductor pulsed laser based on a three-dimensional Dirac semi-metal material infrared saturable absorption device. Such as Figure 5 As shown, the pump source (5) pumps the semiconductor gain structure (6), thereby generating infrared continuous laser light, which passes through the output coupling mirror mirror (7) and reflective three-dimensional Dirac semi-metal material infrared saturable absorption device After the formed microcavity can realize mode-locking or Q-switching, so as to output infrared pulsed laser.
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