Silicon-based annular multi-waveband detector and manufacturing method thereof
A manufacturing method and multi-band technology, applied in the field of sensors, can solve the problems of light loss, large size, poor reliability, etc., and achieve the effects of avoiding light loss, small size, and high device integration.
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Embodiment 1
[0036] Embodiment 1 This embodiment provides an AlGaN circular multi-band detector structure and its preparation process
[0037] The detector structure from bottom to top is the lower electrode 8, the P-silicon substrate 1, the N+ silicon layer 2 with a band gap of Eg1, the N+ nitride layer 3, and the i-nitride layer 4 with a band gap of Eg2. P+ nitride layer 5, upper electrode 6, wherein Eg2>Eg1; wherein the upper electrode 6 is located at the end of the P+ nitride layer 5, and the middle electrode 7 is located near the end of the N+ silicon layer 2 and covers part The end of the N+ nitride layer 3; the middle electrode 7 and the upper electrode 6 are ring structures. The upper electrode 6 has a width of 100 nm and a thickness of 50 nm; the middle electrode 7 has a width of 100 nm and a thickness of 50 nm. The exposed N+ nitride layer 3 is a circular or square ring structure, and the nitride is AlGaN or GaN, a group III-V nitride.
[0038] The exposed N+ nitride layer 3 ha...
Embodiment 2
[0046] Embodiment 2 This embodiment provides a preparation process for an AlGaN square ring multi-band detector
[0047] like image 3 (a) shows the structure of a square AlGaN multi-band detector on silicon. The initial weakly p-type doped p-silicon substrate 1 is selected, and the doping concentration is 10 17 cm -2 ;
[0048] Ion diffusion (downward implantation) is used to form a heavily N-type doped N+ silicon layer 2 with a thickness of about 200nm, doped with arsenic as an impurity, and a doping concentration of 10 20 cm -3 ;
[0049] Molecular beam epitaxy (MBE) is used to sequentially form an N-type doped N+AlGaN layer 3, an intrinsically undoped i-AlGaN layer 4 and a P+AlGaN layer 5 from bottom to top, wherein N+Al The gallium nitride layer 3 has a thickness of 200nm and a doping concentration of 10 20 cm -3 , the doping impurity is silicon; the thickness of the i-aluminum gallium nitride layer 4 is 600nm, the thickness of the uppermost P+aluminum gallium nitr...
Embodiment 3
[0054] Embodiment 3 This embodiment provides a preparation process of a gallium nitride circular multi-band detector
[0055] like image 3 (b) shows the selected initial weakly p-type doped p-silicon substrate 1 with a doping concentration of 10 18 cm -2 ;
[0056] A heavily N-type doped N+ silicon layer 2 is formed by ion diffusion (downward implantation), with a thickness of about 400nm, doped with antimony as impurity, and a doping concentration of 10 21 cm -3 ;
[0057] N-type doped N+ gallium nitride layer 3, intrinsically undoped i-gallium nitride layer 4 and P+ gallium nitride layer 5 are sequentially formed from bottom to top using molecular beam epitaxy (MBE), wherein N+ nitrogen The gallium chloride layer 3 has a thickness of 200nm and a doping concentration of 10 20 cm -3 , the doping impurity is silicon; the thickness of the i-gallium nitride layer 4 is 600nm, the thickness of the uppermost P+gallium nitride layer 5 is 60nm, and the doping concentration is ...
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Abstract
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