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Advanced LIGO Photodiode Development ______

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Advanced LIGO Photodiode Development ______. David Jackrel, PhD Candidate Stanford University Dept. of Materials Science and Engineering James S. Harris Hannover, Germany August 20 th , 2003 LIGO-G030495-00-Z. Outline. Motivation & Introduction AdLIGO PD Specifications - PowerPoint PPT Presentation
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STANFORD Advanced LIGO Photodiode Development ______ David Jackrel, PhD Candidate Stanford University Dept. of Materials Science and Engineering James S. Harris Hannover, Germany August 20 th , 2003 LIGO-G030495-00-Z
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STANFORD

Advanced LIGO Photodiode Development

______

David Jackrel, PhD Candidate

Stanford University

Dept. of Materials Science and Engineering

James S. Harris

Hannover, Germany

August 20th, 2003

LIGO-G030495-00-Z

STANFORD

Outline

Motivation & Introduction AdLIGO PD Specifications Device Materials and Design

InGaAs vs. GaInNAs

Device Results Thinned Device QE InGaAs & GaInNAs I-V 2m Thick GaInNAs Absorption

Predictions

STANFORD

Advanced LIGO Schematic

Power Stabilization

Auxiliary Length Sensing

STANFORD

Photodiode Specifications

LIGO I Advanced LIGO

Detector

Bank of 6PDs

Power Stabilizati

on

RF Detection GW Channel

Steady-State Power

0.6 W 1W/ 10 – 100mW 30mW

Operating

Frequency

~29 MHz 100 kHz 200MHz 100 kHz

Quantum

Efficiency

80% > 80% 95%

e.g. 1W/0.70=1.43W

Resonating Tank Circuit Thinned Substrate

STANFORD

GaInNAs vs. InGaAs

GaInNAs

25% InGaAs

53% InGaAs

1064nm light 1.13eV

STANFORD

InGaAs vs. GaInNAs PD Designs

2 m

GaInNAs lattice-matched to

GaAs!

STANFORD

Rear-Illuminated PD Advantages

Conventional PD Adv. LIGO Rear-Illuminated PD

High Power Linear

Response High Speed

STANFORD

Development Flow-Chart

AdLIGO Photodiodes

InGaAs GaInNAs

500um

Substrate

150um

Substrate1um I-Layer 2um I-Layer

100um

Substrate

100um

Substrate

90% QE

@

1 Watt

90% QE

@

1 Watt

~70% QE

@

Low-Power

60% QE

@

300mW

500um

Substrate

Stanford

& Vendor???

Hamamatsu

Product

30% QE

@

300mW

STANFORD

Thinned Device QE (10mW)

STANFORD

Thinned Device QE (w/ 100m, 3e17cm-3 Substrate)

STANFORD

DC Device Efficiency (w/ ARC)E

xt.

Eff

icie

ncy

Optical Power (mW)

Bias (Volts)

STANFORD

InGaAs vs. GaInNAs Dark Current

STANFORD

InGaAs vs. GaInNAs Dark Current

STANFORD

GaInNAs Device Transmission

STANFORD

Predictions (I think we can do it…)

DetectorPower

Stabilization

RF Detection

GW Channel

Diameter 4.5mm 1.5mm 1mm

Bias -25V -25V -25V

Steady-State Power

1130mW 110mW 50mW

3-dB 1/RC Bandwidth

3MHz30MHz

( 180MHz)60MHz

Quantum Efficiency

~ 90% ~ 90% ~ 90%

STANFORD

Laser Interferometer Gravitational Wave Observatory (LIGO)

Arm Length 4km

Beam Tube Diameter 4 ft.

Vacuum Pressure ~10-10 atm

Differential Strain ~10-18 m

180W

1064nm

STANFORD

MBE Crystal Growth

Effusion cells for In, Ga, Al

Cracking cell for As Abrupt interfaces Chamber is under

UHV conditions to avoid incorporating contaminants

RHEED can be used to analyze crystal growth in situ due to UHV environment

T=450-600C

N Plasma Source

Atomic source of nitrogen needed Plasma Source!

STANFORD

Heterojunction Band Gap Diagram

N-layer:

In.25Al.75As or GaAs

Eg2=2.0-1.4eV

P-layer:

In.25Al.75As or GaAs

Eg2=2.0-1.4eV

I-layer:

In.25Ga.75As, or Ga.88In.12N.01As.99

Eg1=1.1eV

n-

i-

p-

InAlAs and GaAs transparent at 1.064m

Absorption occurs in I-region (in E-field )

STANFORD

Full Structure Simulated by ATLAS

STANFORD

High Efficiency Detector Process (1)

1. Deposit and Pattern P-Contact

2. Etch Mesa – H2SO4:H2O2:H20 and Passivate in (NH4)2S+

3. Encapsulate Exposed Junction

4. Flip-Chip Bond

- N+ GaAs Substrate

- Epitaxial Layers

- Au Contacts

- Polyimide Insulator

- SiNx AR Coating

- AlN Ceramic

STANFORD

High Efficiency Detector Process (2)

6. Deposit AR Coating & N-Contact

7. Saw, Package and Wire-Bond

- N+ GaAs Substrate

- Epitaxial Layers

- Au Contacts

- Polyimide Insulator

- SiNx AR Coating

- AlN Ceramic

5. Thin N+ GaAs Substrate

STANFORD

Free-Carrier Absorption

(1-T-R) and (1-T-R)/(1-R)

-0.2

0

0.2

0.4

0.6

0.8

1

1.2

850 950 1050 1150 1250 1350 1450 1550 1650 1750

Wavelength (nm)

Ab

sorp

tio

n (

no

rm.)

GaAs N+

GaAs S-I

GaAs N+ (W)

GaAs S-I (W)

32.9% N+

S-I

STANFORD

Free-Carrier Absorption

STANFORD

Free-Carrier Absorption

STANFORD

Free-Carrier Absorption 5e17cm^-3

STANFORD

Thinned Device QE (w/ ARC)

STANFORD

Photodiode Specifications

LIGO I Advanced LIGO

Detector

Bank of 6PDs

Power Stabilizati

on

RF Detection GW Channel

Steady-State Power

0.6 W 1W/ 10 – 100mW 30mW

Operating

Frequency

~29 MHz 100 kHz 200MHz 100 kHz

Quantum

Efficiency

80% > 80% 90%-95%

STANFORD

Thinned Device Photocurrent

STANFORD

DC Device Response

STANFORD

DC Device Efficiency

STANFORD

Free-Carrier Absorption

A = 1 – exp(-tsub•fc) , fc = Nd * 3e-18

STANFORD

Surface Passivation Results (2)

STANFORD

(NH4)2S+ Surface States

(Green and Spicer, 1993)

GaAs(111)A GaAs(111)B

STANFORD

Surface Passivation Results

STANFORD

Large InGaAs Devices, –20V Bias

STANFORD

InGaAs vs. GaInNAs Dark Current

STANFORD

GaInNAs Dark Current

STANFORD

InGaAs Dark Current

STANFORD

GaInNAs H2SO4 vs. (NH4)2S+

STANFORD

GaInNAs H2SO4 vs. (NH4)2S+

STANFORD

Theoretical Saturation Powers

STANFORD

Theoretical Saturation Powers

STANFORD

RC-Circuit Bode Plot

3-dB

30MHz

STANFORD

RC- and LCR- Transmittance

RC-Circuit

LCR-Circuit

STANFORD

LCR- Circuit Impedance

s

iV

RCZ

Zin

out

20

1||

||||

0

s

iV

RCZ

Zin

out

20

1||

||||

0

STANFORD

RC- vs. LCR-Circuits

RC- PD acting as a Low-Pass Filter LCR #1- PD // Inductor as a Tuned Band-Pass Filter (with large R=50)

LCR #2,3- PD // Inductor as a Tuned Band-Pass Filter (Rs=1)

STANFORD

Transfer Function LCR #3


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