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1 ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik ECE 5900/6900: Fundamentals of Sensor Design Lecture 8 Optical Sensing
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Page 1: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

1

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

ECE 5900/6900: Fundamentals of Sensor Design

Lecture 8Optical Sensing

Page 2: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

2

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Optical Sensing

Q: What are we measuring?

A: Electromagnetic radiation labeled as Ultraviolet (UV),

visible, or near,mid-, far-infrared (IR)

SI Units: Lumen (lm), Lux (lx=lm/m2), Candela (cd)

Page 3: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

3

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Optical Sensors

Photoresistor Photodiode PhototransistorFairchild QSD2030F Honeywell SDP8406-003Sparkfun SEN-09088

Thermopile Infrared CMOS Image Sensors

Amphenol ZTP-101T Lumex SNR-40135 Samsung

S5K9A1On Semiconductor

KAC-06040

Page 4: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

4

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Applications of Optical Sensors

Proximity (Distance)

Sensing

Smoke Detector

Page 5: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

5

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Applications of Optical Sensors

Controlling Gas valve with Thermopiles

Gas valve in

Fireplace

Gas valve in

Waterheater

Page 6: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

6

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Applications of Optical Sensors

Smartphone/tablet Camera

Military Night Vision Camera

Page 7: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

7

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Types of Optical Sensors

Quantum Detectors

Photoresistor (Photocell)

Photodiode

Phototransistor

Thermal Detectors

Thermopile

Image Sensors

CMOS Image Sensor

Page 8: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

8

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Photoelectic Effect

Einstein discovered that when high energy photons interact with electrons, it is

possible for the electrons to be ejected from the material

Photon absorption and emission of electrons

Ref: http://sargosis.com/articles/science/how-pv-modules-work/the-photoelectric-and-photovoltaic-effects/

Page 9: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

9

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Photoconductive Effect

Given small bandgap, incident photons can make the electrons jump into the

conduction band.

The resulting free electrons (and holes) increase conductance and hence lower

resistivity of a material

Photon absorption and increase in conductivity

Page 10: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

10

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Photoresistor (or Photocell or Photoconductor)Light Dependent Resistor (LDR) CdS (Cadmium sulfide)

Track

Light-controlled variable resistor

The resistance of a photoresistor decreases with increasing

light intensity

An active semiconductor layer (e.g. CdS) that is deposited

on an insulating substrate

The semiconductor is normally lightly doped

Less light-sensitive than photodiodes and phototransistors

Page 11: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

11

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

LDR Circuit Example

When LDR is exposed to light, LDR resistance is low which makes

the base voltage of Q1 high enough for the collector current to sink

As a result LED turns on

When LDR is blocked,

the resistance goes up

(MΩ), and base voltage

drops down and shuts

off the transistor

As a result LED

turns off

Page 12: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

12

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Types of Optical Sensors

Quantum Detectors

Photoresistor (Photocell)

Photodiode

Phototransistor

Thermal Detectors

Thermopile

Image Sensors

CMOS Image Sensor

Page 13: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

13

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

PhotodiodePhotodiode

p-type material is doped with boron

(donor), n-type material is doped with

acceptor atoms.

When the light energy is greater than the

band gap energy, the electrons move into the

conduction band creating electron-hole pairs.

In the depletion layer the electric field

accelerates these electrons toward the n-layer

and holes toward the p-layer.

This results in a positive charge in the

p-layer and a negative charge in the n-layer.

If an external circuit is connected between

the PN junction, electrons will flow away

from n-layer, and holes will flow away from

the p-layer

Page 14: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

14

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

PhotodiodePhotodiode Operation

Light-controlled current through a diode

When exposed to light, electron-hole pairs are created

Newly generated electron-hole pairs are swept away by the existing

PN junction and current (also known as photo current) is created

Must be reverse-biased so that the depletion region is larger

Photodiode

Mode

Solar Cell

ModeAvalanche

Phtodiode

Responsivity (λ)

=Photocurrent/Incide

nt Light Power

Page 15: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

15

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Photodiode Model

Ref: thorlabs.us

IPD= Photo Current, ID= Dark Current=Saturation Current=Leakage Current

at zero bias, Cj=Junction Capacitance, RS=Shunt Resistance of zero-biased PN

junction

Photoconductive mode: under reverse bias, the measured output current is

linearly proportional to the input optical power

Photovoltaic mode: under zero bias, the current is held constant vice is

restricted and a voltage builds up, dark current is kept at a minimum

Cj

RS

Page 16: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

16

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Photodiode Circuit Example

Light Detector Circuits based on GaP Photodiode

Ref: thorlabs.us

Reverse Bias (improve bandwidth and lower

junction capacitance) or Zero Bias (minimum

dark current)

Page 17: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

17

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Types of Optical Sensors

Quantum Detectors

Photoresistor (Photocell)

Photodiode

Phototransistor

Thermal Detectors

Thermopile

Image Sensors

CMOS Image Sensor

Page 18: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

18

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Photovoltaic Effect

If a high energy photon strikes an electron, the electron can escape into conduction

band and creates holes and electrons (free charge carriers)

Photon absorption and emission of electrons

Page 19: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

19

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Phototransistor

Phototransistor operation

Large Base and Collector areas

Active region operation

Base is left open and is

exposed to light

Light causes hole electron

pairs to be generated

This occurs in the reverse

biased base-collector junction

(BCJ)

The hole-electron pairs move

under the electric field in the

depletion region and provide the

base current, causing electrons to

be injected into the collector

E

Page 20: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

20

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Phototransistor Example

Detect light in near-infrared (λ=700 nm-

1100nm

-CE: Current is amplified and Vout is

generated

-CC: Vout switches from Low to High state

Both can be operated in Active or Switch mode

Active mode: phototransistor generates a

response proportional to the light received

Switch mode: phototransistor will either be

”off” (cut-off) or ”on” (saturated) in response to

the light.

Common-Emitter

(CE) Amplifier

Common-Collector

(CC) Amplifier

Page 21: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

21

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Phototransistor Modes: CC Amplifier

Common-Collector (CC) Amplifier (object detection, encoder)1) Low state to a high state when light is detected

2) No light: Vout=0V

3) Light: base current IB is generated,

which is amplified by the collector, IC is generated

-with Ron ~0 Ω, Vout=(RE/(RE+Ron))Vcc

Vout=Vcc

4) Mode is set by adusting RE

Active Mode (Vout propotional to light level):

Vcc > RE x IC

Switch Mode: Vcc < RE x IC

where IC=max collector current for specific light

levelRef: http://datasheet.eeworld.com.cn/pdf/371989,FAIRCHILD,AN-3005.pdf

Page 22: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

22

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Phototransistor Modes: CE Amplifier

Common-Emitter (CE) Amplifier (compare two levels of light)1) High state to a low state when light is detected

2) No light: Vout=VCC

3) Light: base current IB is generated,

which is amplified by the collector, IC is generated

-with Ron ~0 Ω, Vout=(Ron/(Ron+Ron))Vcc

Vout=0V

4) Mode is set by adusting RC

Active Mode (Vout propotional to light level):

Vcc > RC x IC

Switch Mode: Vcc < RC x IC

where IC=max collector current for specific light

levelRef: http://datasheet.eeworld.com.cn/pdf/371989,FAIRCHILD,AN-3005.pdf

Page 23: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

23

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Phototransistor Example Circuit

Source signal current passes through the input LED which emits an infra-red

light whose intensity is proportional to the electrical signal

IR light generates current in the base and it is amplified at the collector.

When the current flowing through the LED is interrupted (e.g. digital data), the

IR light is cut off and the photo transistor cuts off

Optocouplers are used to switch transistors or other components as they provide

electrical isolation between a lower voltage control signal and the higher voltage or

current output signal.

Examples: Microprocessor input/output switching (turn on/off motor, heater,

lights), DC and AC power control

Optocoupler

Page 24: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

24

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Types of Optical Sensors

Quantum Detectors

Photoresistor (Photocell)

Photodiode

Phototransistor

Thermal Detectors

Thermopile

Image Sensors

CMOS Image Sensor

Page 25: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

25

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Thermopile SensorsThermopile Basics

a: thermopile with a reference temperature sensor attached, x and y are different

materials

b: micromachined thermopile sensor (note the semiconductor reference

temperature sensor on the silicon frame where the cold junctions are deposited)

c: sensor in a TO-5 package

Thermopiles detect thermal radiation (heat)

Thermopile is a chain of serially connected thermocouples*, typically 50–100

junctions.

*Thermocouples: https://www.picotech.com/library/application-note/thermocouple-application-note

Page 26: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

26

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Thermopile SensorsThermopile Operation

IR light is absorbed by or emanated from the membrane and

temperature of the membrane changes

Since the membrane carries “hot” junctions, the temperature differential

with respect to the “cold” junctions located on the frame generate

thermoelectric voltage

Membrane may be thermally coupled with a reference temperature

sensor or attached to a thermostat having a precisely known temperature

Example circuit: measured temp. is amplified and processed via DSP

Thermopile Example Circuit (Melexis MLX90615)

Measure

surface

temp. of package

Page 27: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

27

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Types of Optical Sensors

Quantum Detectors

Photoresistor (Photocell)

Photodiode

Phototransistor

Thermal Detectors

Thermopile

Image Sensors

CMOS Image Sensor

Page 28: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

28

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Image Sensor BasicsCharge Coupled Device (CCD) (Tutorial: https://www.youtube.com/watch?v=Xkput-1xNYE)

CCD chip is divided into pixels*

Each pixel has a potential well that collects the electrons produced by the

photoelectric effect.

After the exposure (incoming photons), each pixel has collected a finite amount of

electrons (and hence charge) proportional to the amount of light

CCD is then read out by cycling the voltages applied to the chip in a process called

“clocking.” Clocking causes the charge in one pixel to be transferred to an adjacent pixel

* More at https://www.microscopyu.com/articles/digitalimaging/ccdintro.html

Page 29: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

29

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

Image Sensor BasicsCMOS Image Sensor*

Like CCDs, CMOS imagers have an array of photo diodes, one diode

within each pixel

Unlike CCDs, each pixel in a CMOS imager has its own individual

amplifier

Each pixel in a CMOS imager can be read directly on an x–y coordinate

system

While a CCD pixel always transfers a charge, a CMOS pixel always

detects a photon directly and converts it to a voltage

* More in http://www.onsemi.com/pub_link/Collateral/KAC-06040-D.PDF

Page 30: Lecture 8 - Weber State Universityfaculty.weber.edu/snaik/ECE5900_ECE6900/08Lec08_Optical.pdf · at zero bias, C j =Junction Capacitance, R S =Shunt Resistance of zero-biased PN junction

30

ECE 5900/6900 Fundamentals of Sensor Design Dr. Suketu Naik

CMOS Image Sensor: An Example

On Semiconductor KAC-06040

Resolution: 2832 (H) x 2128

(V), 6 megapixel

Fabrication Technology:

4.7 μm 5T CMOS

200 MHz DDR at 400

Mbps data rate

* More in http://www.onsemi.com/pub_link/Collateral/KAC-06040-D.PDF


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