InP/InGaAsP/InGaAs SWIR APDs

Slides:



Advertisements
Similar presentations
MICROWAVE FET Microwave FET : operates in the microwave frequencies
Advertisements

Chapter 9. PN-junction diodes: Applications
LECTURE- 5 CONTENTS  PHOTOCONDUCTING MATERIALS  CONSTRUCTION OF PHOTOCONDUCTING MATERIALS  APPLICATIONS OF PHOTOCONDUCTING MATERIALS.
Solomon Assefa, Nature, March 2010 Reinventing germanium avalanche photodetector for nanophotonic on- chip optical interconnects Jeong-Min Lee
Semiconductor Optical Sources
Status on long-wavelength InP waveguide heterojunction phototransistors Samuel Dupont, Vincent Magnin, Manuel Fendler, Filippe Jorge, Sophie Maricot, Jean-Pierre.
© S.N. Sabki Revision CHAPTER 9 CHAPTER 9 Part II.
What Does SPAD Afterpulsing Actually Tell Us About Defects in InP? Mark Itzler, Mark Entwistle, and Xudong Jiang SPW2011 – June 2011.
Cell and module construction. Photovoltaic effect and basic solar cell parameters To obtain a potential difference that may be used as a source of electrical.
XYZ 6/10/2015 Fabricated Arrays Si>2e18 n
EE 230: Optical Fiber Communication Lecture 11 From the movie Warriors of the Net Detectors.
Solar Cell Operation Key aim is to generate power by:
Photodetector.
EE580 – Solar Cells Todd J. Kaiser
Fiber-Optic Communications
9. Semiconductors Optics Absorption and gain in semiconductors Principle of semiconductor lasers (diode lasers) Low dimensional materials: Quantum wells,
Near-infrared (NIR) Single Photon Counting Detectors (SPADs)
Photo Detectors Parameters: Parameters: Responsivity (Efficiency): Output current/input optical powerResponsivity (Efficiency): Output current/input optical.
Fiber Optic Light Sources
Fiber Optic Receiver A fiber optic receiver is an electro-optic device that accepts optical signals from an optical fiber and converts them into electrical.
OPTICAL DETECTORS IN FIBER OPTIC RECEIVERS.
Optical Receiver Lecture 6.
Chapter 6 Photodetectors.
V. Semiconductor Photodetectors (PD)
Min-Hyeong Kim High-Speed Circuits and Systems Laboratory E.E. Engineering at YONSEI UNIVERITY
Photon detection Visible or near-visible wavelengths
Solar Cells, Sluggish Capacitance, and a Puzzling Observation Tim Gfroerer Davidson College, Davidson, NC with Mark Wanlass National Renewable Energy Lab,
Chapter 5 Optical Detector.
References Hans Kuzmany : Solid State Spectroscopy (Springer) Chap 5 S.M. Sze: Physics of semiconductor devices (Wiley) Chap 13 PHOTODETECTORS Detection.
Incident light with an energy of hv>Eg excites an electron and causes it to jump from the valence band to the conduction band, thereby creating an electron-hole.
Previous work on CVD-grown SiNWs Single SiNW NATURE| Vol 449| 18 October Removed from the growth substrate and laid on a foreign substrate Contacts.
Light Emitting Diode Sumitesh Majumder.
Chapter 6 Photodetectors.
2 光源(Optical Sources)與檢光器(Photodetectors)重要參數量測
OSC’s Industrial Affiliates Workshop, Tucson, Arizona March, 2005 GaAsSb QUANTUM WELLS FOR OPTOELECTRONICS AND INTEGRATED OPTICS Alan R. Kost, Xiaolan.
Chapter 6 Photodetectors
University of California Santa Barbara Yingda Dong Characterization of Contact Resistivity on InAs/GaSb Interface Y. Dong, D. Scott, A.C. Gossard and M.J.
References Hans Kuzmany : Solid State Spectroscopy (Springer) Chap 5 S.M. Sze Physics of semiconductor devices (Wiley) Chap 13 PHOTODETECTORS.
InAs Inserted HEMT 연성진.
Module 2/7: Solar PV Module Technologies. Module 1 : Solar Technology Basics Module 2: Solar Photo Voltaic Module Technologies Module 3: Designing Solar.
Photo Detectors for Fiber Optic Communication
Optical Detectors Abdul Rehman. Optical Detector Optical detector is an essential component of an optical receiver which converts received optical signal.
1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors.
Photodetectors What is photodetector (PD)? Photodetector properties
Photodetectors. Principle of the p-n junction Photodiode  Schematic diagram of a reverse biased p-n junction photodiode SiO 2 Electrode  net –eN.
Optical Receivers Theory and Operation
Photovoltaic effect and cell principles. 1. Light absorption in materials and excess carrier generation Photon energy h = hc/ (h is the Planck constant)
C. Kadow, J.-U. Bae, M. Dahlstrom, M. Rodwell, A. C. Gossard *University of California, Santa Barbara G. Nagy, J. Bergman, B. Brar, G. Sullivan Rockwell.
Waveguide Ge-PD Simulation
Avalanche Photodiodes from the Start.
Topic Report Photodetector and CCD
Bandgap (eV) Lattice Constant (Å) Wavelength ( ㎛ ) GaN AlN InN 6H-SiC ZnO AlP GaP AlAs.
Date of download: 6/25/2016 Copyright © 2016 SPIE. All rights reserved. (a) Cartoon of flip-chip InGaAs FPA with InP substrate. SWIR light passes through.
Date of download: 6/26/2016 Copyright © 2016 SPIE. All rights reserved. (a) AFM image of a single contacted nanowire comprised of p- and n-doped sections.
Date of download: 7/9/2016 Copyright © 2016 SPIE. All rights reserved. Band profile and local density of states of a 40-nm GaAs pin junction solar cell.
Application of photodiodes
Contents GaAs HEMTs overview RF (Radio Frequency) characteristics
GaAs Process & Devices Anurag Nigam.
WP 2 Materials for Security : Overview - ESR 5, 6, 7 & 8
Electronics & Communication Engineering
PN-junction diodes: Applications
Date of download: 10/22/2017 Copyright © ASME. All rights reserved.
Photo Detectors.
Photodetectors.
V. Semiconductor Photodetectors (PD)
High Power, Uncooled InGaAs Photodiodes with High Quantum Efficiency for 1.2 to 2.2 Micron Wavelength Coherent Lidars Shubhashish Datta and Abhay Joshi.
Fabricated Arrays CCS-0888-A CCS-0889-A CCS-0890-A CCS-1061-A
500 nm WRITE VOLTAGE 0 V.
Optical Receivers 1. Photo Detectors
PbWO4 Cherenkov light contribution to Hamamatsu S8148 and Zinc Sulfide–Silicon avalanche photodiodes signals F. KOCAK, I. TAPAN Department of Physics,
Presentation transcript:

InP/InGaAsP/InGaAs SWIR APDs Separate absorption, grading, charge, and multiplication (SAGCM) structure Carrier collection in absorber: low but finite field in absorber (avoid tunneling) Multiplication gain: high field for impact ionization i - n + InP buffer InGaAsP grading InP charge InP cap SiNx passivation p-contact metallization InP substrate n-contact metallization optical input E InGaAs absorption multiplication region p+-InP diffused region anti-reflection coating Al0.6InAsSb multiplication Long-wavelength absorber

External Quantum Efficiency 60% 30% 50% 40% 70%

External Quantum Efficiency 60% 30% 50% 40% 70%

AlInAsSb SACM APD p-type contact blocking layer graded bandgap p+:GaSb 11019, 30 nm p+: AlxIn1-xAlyAs1-y x = 0.7 to 0.4, 100 nm p+: Al0.7In0.3As0.3Sb0.7 21018, 100 nm n+: GaSb, 11018, buffer n+:GaSb Substrate n-: Al0.4In0.6As0.3Sb0.7, 1,000 nm p+: AlxIn1-xAlyAs1-y x = 0.4 to 0.7, 100 nm p: Al0.7In0.3As0.3Sb0.7 1.251017, 150 nm n-: Al0.7In0.3As0.3Sb0.7, 1,000 nm absorption layer multiplication layer n-type contact charge layer p-type contact graded bandgap blocking layer Electric field

AlInAsSb SACM Current-Voltage Characteristics 10-9 10-8 10-7 10-6 10-5 10-4 10-3 Gain Photocurrent Dark current

Noise Measurement of AlInAsSb k= 0.07 ↑ Measured with a 100 µm device. k= 0.05 from fitting, <M>=1.33 @ punch-through.

APD Comparison 100 Gb/s Ethernet 400 Gb/s Ethernet 2q(iph+idark)M2F(M)