InAS is a III-V compound semiconductor with narrow band gap (0.35 EV) and high electron mobility (33,000 CMยฒ/VยทS). Its manufacturing requires precise control of stoichiometric ratio and crystal defects
High purity indium (IN) and arsenic (AS) are purified to 99.9999% (6N) or more by vacuum distillation or regional smelting.
Synthesis of INAS polycrystal: IN and AS are sealed in a quartz tube at a molar ratio of 1:1. At high temperature (800-900โ), they are sublimated into arsenic vapor. The arsenic vapor reacts with indium melt in the crystal growth crucible at high temperature to form indium arsenide melt, and then INAS ingot is generated by cooling.
Molecular beam epitaxy (MBE): In ultra-high vacuum (10โปยนโฐ TORR), IN and AS atoms are evaporated by electron beam to grow high quality single crystal thin films on GAAS, INP or SI substrates, suitable for quantum well and quantum dot structures.
Metal organic chemical vapor deposition (MOCVD): using trimethylindium (TMIN) and arsine (ASHโ) as precursors, INAS layer is deposited at 500-700โ, suitable for large area uniform film preparation.
Bridgeman Method (BRIDGMAN): Used to grow large INAS single crystal ingots, the integrity of the crystal is controlled by a vertical temperature gradient to obtain substrate material up to 3 inches in diameter.
Doping regulation: silicon (SI) as N-type dopant (concentration 10ยนโถ-10ยนโน CMโปยณ), zinc (ZN) or carbon (C) as P-type dopant.
Heterojunction preparation: quantum well (such as INAS/GASB superlattice) is formed by combining with materials such as GASB and INGAAS for infrared detector.
Surface treatment: chemical corrosion (such as HโSOโ:HโOโ:HโO mixture) to remove the surface oxide layer to ensure stable device performance.
Mid-wave infrared response: covers the 3-5 ฮM band, suitable for night vision devices, thermal imaging devices and remote sensing.
High quantum efficiency: more than 80% at room temperature, more stable than cadmium telluride mercury (HGCDTE).
Fast response time: about 10 NS, suitable for high-speed dynamic target detection.
High electron mobility: 33,000 CMยฒ/VยทS at 300K (8,500 CMยฒ/VยทS for GAAS), supports high frequency electronic devices, suitable for millimeter wave (30-300 GHZ) communication devices. Low defect density improves device performance
Low noise characteristics: the noise factor is less than 0.5 DB in HEMT (high electron mobility transistor), which is used for radar and satellite communication.
Advantages of zero-dimensional structure: INAS quantum dots have adjustable band gap (0.3-1.5 EV) for single photon emitters and qubits.
Spin-orbit coupling: Strong spin-orbit interaction is conducive to the construction of spin qubits and reduces decoherence effects.
Low thermal conductivity: 0.025 W/CMยทK (300K), combined with high electrical conductivity, ZT value (thermoelectric value) can reach 1.5, suitable for thermoelectric power generation.
High temperature stability: the structure is stable below 400โ, which is better than traditional BIโTEโ-based materials.
Stacked solar cells: as intermediate sub-cells (band gap 0.35 EV), they are composed of three junction cells with GAAS (1.42 EV) and GE (0.67 EV), with an efficiency of over 40%.
Laser diode: INAS quantum dot laser operates at wavelengths of 1.3-1.55 ฮM for optical fiber communication.
| metric ย ย ย ย ย ย ย ย ย ย ย ย ย ย | INAS ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย | GAAS ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย | INSB
| band gap (EV) ย ย ย ย ย ย ย ย | 0.35 (direct) ย ย ย ย ย ย ย ย ย ย ย ย ย 1.42 (direct) ย ย ย ย ย ย ย ย ย ย ย ย ย | 0.17 (direct)
| Electron mobility (CMยฒ/V ยท S) | 33,000 (300K) ย ย ย ย ย ย ย ย ย | 8,500๏ผ300K๏ผ ย ย ย ย ย ย ย ย ย ย ย ย | 77,000๏ผ300K๏ผ
| Thermal conductivity (W/CMยทK) | 0.025 (300K) ย ย ย ย ย ย ย ย ย ย ย ย | 0.46 ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย | 0.23
| Response wavelength (ฮM) | 3-5 (mid-wave infrared) ย ย ย ย ย ย ย ย ย ย | 0.8-1.8 (near infrared) ย ย ย ย ย ย ย ย | 3-5.5 (mid-wave infrared)
| ZT value (thermoelectric) | 1.5 (400K) ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย | 0.4 ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย ย | 0.7
As a representative of narrow band gap semiconductors, INAS has unique advantages in the fields of infrared detection, high frequency electronics and quantum technology. The application needs in military, communication and energy fields are driving technological innovation. With the development of heterojunction integration and nanotechnology, INAS is expected to become the core material of next-generation semiconductor devices.
Mid-wave infrared response: covers the 3-5 ฮM band, suitable for night vision devices, thermal imaging devices and remote sensing.
High quantum efficiency: more than 80% at room temperature, more stable than cadmium telluride mercury (HGCDTE).
Fast response time: about 10 NS, suitable for high-speed dynamic target detection.
High electron mobility: 33,000 CMยฒ/VยทS at 300K (8,500 CMยฒ/VยทS for GAAS), supports high frequency electronic devices, suitable for millimeter wave (30-300 GHZ) communication devices. Low defect density improves device performance
Low noise characteristics: the noise factor is less than 0.5 DB in HEMT (high electron mobility transistor), which is used for radar and satellite communication.
Advantages of zero-dimensional structure: INAS quantum dots have adjustable band gap (0.3-1.5 EV) for single photon emitters and qubits.
Spin-orbit coupling: Strong spin-orbit interaction is conducive to the construction of spin qubits and reduces decoherence effects.
Low thermal conductivity: 0.025 W/CMยทK (300K), combined with high electrical conductivity, ZT value (thermoelectric value) can reach 1.5, suitable for thermoelectric power generation.
High temperature stability: the structure is stable below 400โ, which is better than traditional BIโTEโ-based materials.
Stacked solar cells: as intermediate sub-cells (band gap 0.35 EV), they are composed of three junction cells with GAAS (1.42 EV) and GE (0.67 EV), with an efficiency of over 40%.
Laser diode: INAS quantum dot laser operates at wavelengths of 1.3-1.55 ฮM for optical fiber communication.
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