1 stephen schultzfiber optics fall 2005 semiconductor optical detectors

11
1 Semiconductor Optical Detectors

Upload: natalie-reeves

Post on 20-Jan-2016

224 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: 1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors

1

Semiconductor Optical Detectors

Page 2: 1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors

2

Semiconductor Optical Detectors

• Inverse device with semiconductor lasers

– Source: convert electric current to optical power

– Detector: convert optical power to electrical current

• Use pin structures similar to lasers

• Electrical power is proportional to i2

– Electrical power is proportional to optical power squared

– Called square law device

• Important characteristics

– Modulation bandwidth (response speed)

– Optical conversion efficiency

– Noise

– Area

Page 3: 1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors

3

p-n Diode

• p-n junction has a space charge region at the interface of the two material types

• This region is depleted of most carriers

• A photon generates an electron-hole pair in this region that moves rapidly at the drift velocity by the electric field

• An electron-hole pair generated outside the depletion region they move by diffusion at a much slower rate

• Junction is typically reversed biased to increase the width of the depletion region

Page 4: 1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors

4

p-n Diode

Page 5: 1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors

5

Semiconductor pin Detector

• Intrinsic layer is introduced

– Increase the space charge region

– Minimize the diffusion current

Page 6: 1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors

6

I-V Characteristic of Reversed Biased pin

• Photocurrent increases with incident optical power

• Dark current, Id: current with no incident optical power

Page 7: 1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors

7

Light Absorption

• Dominant interaction

– Photon absorbed

– Electron is excited to CB

– Hole left in the VB

• Depends on the energy band gap (similar to lasers)

• Absorption ( requires the photon energy to be smaller than the material band gap

gEhc

meVEE

hc

gg

24.1

Page 8: 1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors

8

Quantum Efficiency

• Probability that photon generates an electron-hole pair

• Absorption requires

– Photon gets into the depletion region

– Be absorbed

• Reflection off of the surface

• Photon absorbed before it gets to the depletion region

• Photon gets absorbed in the depletion region

• Fraction of incident photons that are absorbed

le

R 1

de 1

dl eeR 11

Page 9: 1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors

9

Detector Responsivity

• Each absorbed photon generates an electron hole pair

Iph = (Number of absorbed photons) * (charge of electron)

• Rate of incident photons depends on

– Incident optical power Pinc

– Energy of the photon Ephoton= hf

• Generated current

• Detector responsivity

– Current generated per unit optical power

in units of m

fh

qPI incph

WAfh

q

24.1

Page 10: 1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors

10

Responsivity

• Depends on quantum efficiency , and photon energy

WAhf

q

24.1

Page 11: 1 Stephen SchultzFiber Optics Fall 2005 Semiconductor Optical Detectors

11

Minimum Detectable Power

• Important detector Specifications

– Responsivity

– Noise Equivalent noise power in or noise equivalent power NEP

– Often grouped into minimum detectable power Pmin at a specific data rate

• Pmin scales with data rate

• Common InGaAs pin photodetector

– Pmin=-22 dBm @B=2.5 Gbps, BER=10-10

• Common InGaAs APD

– Pmin=-32 dBm @B=2.5 Gbps, BER=10-10

– Limited to around B=2.5 Gbps