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STANFORD High-Power High-Speed Photodiode for LIGO II David Jackrel Ph.D. Candidate- Dept. of Materials Science & Engineering Advisor- Dr. James S. Harris n LIGO-G000241-00-D
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STANFORD Outline l Motivation l Diode structure & Materials choices l Graded buffer layer l Processing procedure l Simulations l Absorption QE l Frequency response l Electronic noise l Experimental results & Future work
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STANFORD P-I-N Device Characteristics l Large E-field in I- region Depletion Width Width of I- region Frequency response max ( sat /W I ) l RC time constant Tuned to a specific
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STANFORD Photodiode Advantages l High Power l Linear Response l Optimum E g l High Speed Proposed PD (Rear-Illuminated)Conventional PD
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STANFORD InGaAs/GaAs PD Structure InGaAs for i-layer InAlAs for the n- and p- layers P-I-N structure MBE Grading layer AR coating & Au/Pt contacts
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STANFORD Band Gap Diagram w/ Heterojunctions InAlAs Optically transparent to 1.06 m radiation l Absorption occurs in i-region N-layer: In.22 Al.78 As E g2 =2.0eV P-layer: In.22 Al.78 As E g2 =2.0eV I-layer: In.22 Ga.78 As E g1 =1.1eV n- i- p-
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STANFORD III-V Lattice Constants and Band Gaps l InAlAs and InGaAs well lattice matched l InAlAs much wider band gap
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STANFORD Lattice Mismatched Growth l Lattice Constant for In x Ga (1-x) As: a=5.6536+0.4054x In.4 Ga.6 As: h c 100 Å
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STANFORD Solution: Graded Buffer Layer l Dislocations propagate downwards l Active region free from dislocations Susan Marie Lord, Ph.D Thesis, Stanford Univ., 1993
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STANFORD Graded Buffer Dislocations Biaxial stress in film causes dislocations to glide Misfit growth often results in surface striations Hsu, et al. (1992)
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STANFORD Rear Contact (#637)
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STANFORD Processing: Slide #1
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STANFORD Processing: Slide #2
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STANFORD Processing: Slide #3
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STANFORD Processing: Slide #4
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STANFORD Absorption Simulation (1)
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STANFORD Absorption Simulation (2)
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STANFORD Frequency Response Simulation (1)
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STANFORD Frequency Response Simulation (2)
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STANFORD Electronic Noise
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STANFORD Electronic Noise Simulation (1)
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STANFORD Electronic Noise Simulation (2)
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STANFORD Electronic Noise Simulation (3)
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STANFORD I-V Curves: Mounted Diodes
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STANFORD Possible Solution- Insulating Layer
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STANFORD Diagnostics by Processing Step I.) MBE Growth Transmission XRD TEM II.) AR Coating Transmission III.) N- and P- Contacts TLM I-V Measurements C-V Measurements IV.) Etch Mesa I-V Measurements C-V Measurements Low Power LASER testing V.) Insulating Layer I-V Measurements VI.) Mounting to Heat sink & Wire Bonding I-V Measurements High Power LASER Testing (10W) i. QE ii. Response Linearity iii. Bandwidth iv. Power Dissipation
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STANFORD Transmission Spectra
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STANFORD XRD Measurements
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STANFORD Compositions- XRD & Transmission
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STANFORD TEM Images of Confined Dislocations Device Layers: -few dislocations Graded Buffer: -many dislocations
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STANFORD Absorption Data: #649 (w/ ARC)
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STANFORD GaAs Substrate Absorption
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