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EE 330 Lecture 13 Devices in Semiconductor Processes Resistors Diodes Capacitors MOSFETs

EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

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Page 1: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

EE 330Lecture 13

Devices in Semiconductor Processes

• Resistors

• Diodes

• Capacitors

• MOSFETs

Page 2: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Exam 1 ScheduleExam 1 will be given on Friday September 18

Format: Open-Book, Open Notes

Exam will be posted at 9:00 a.m. on the class WEB site and will be due at 1:00 p.m. as a .pdf upload on CANVAS

It will be structured to be a 50-minute closed-book closed-notes exam but administered as an open-book, open-notes exam with a 4 hour open interval so reserving the normal lecture period for taking the exam should provide adequate time

For anyone with approved special accommodations, the 4-hour open interval should cover extra time allocations but if for any reason this does not meet special accommodation expectations, please contact the instructor by Monday Sept. 14 if alternative accommodations are requested.

Honor System Expected

It is expected that this exam be an individual effort and that students should not have input in any form from anyone else during the 4-hour open interval of the exam except from the course instructor who will be responding to email messages from 11:00 a.m. to 1:00 p.m. on the date of the exam.

Special Accommodations

Page 3: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Resistivity of Materials used in Semiconductor Processing

• Cu: 1.7E-6 cm

• Al: 2.7E-4 cm

• Gold: 2.4E-6 cm

• Platinum: 3.0E-6 cm

• Polysilicon: 1E-2 to 1E4 cm*

• n-Si: typically .25 to 5 cm* (but larger range possible)

• intrinsic Si: 2.5E5cm

• SiO2: E14 cm

* But fixed in a given process

Page 4: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

http://www.cleanroom.byu.edu/ResistivityCal.phtml

Page 5: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

http://www.cleanroom.byu.edu/ResistivityCal.phtml

Page 6: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

http://www.cleanroom.byu.edu/ResistivityCal.phtml

Page 7: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Temperature CoefficientsUsed for indicating temperature sensitivity of resistors & capacitors

6

op. temp

1 dRTCR 10 ppm C

R dT

This diff eqn can easily be solved if TCR is a constant

TCR

10

TT

12

6

12

TRTR

e

6121210

TCRTT1 TRTR

For a resistor:

Identical Expressions for Capacitors

It follows that If TCR*(T2-T1) is small,

xe 1 x If x is small,

Page 8: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Voltage CoefficientsUsed for indicating voltage sensitivity of resistors & capacitors

6

ref voltage

1 dRVCR 10 ppm V

R dV

This diff eqn can easily be solved if VCR is a constant

VCR

VV

12

12

VRVR610

e

6121210

VCRVV VRVR 1

For a resistor:

Identical Expressions for Capacitors

It follows that If VCR*(V2-V1) is small,

Page 9: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Temperature and Voltage Coefficients

• Temperature and voltage coefficients often quite large for diffused resistors

• Temperature and voltage coefficients often quite small for poly and metal film (e.g. SiCr) resistors

Page 10: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

From:F. Maloberti : Design of CMOS Analog Integrated Circuits - “Resistors, Capacitors, Switches”

(absolute)

(relative accuracy much better and can be controlled by designer)

Page 11: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William
Page 12: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

From Allen Holberg Third Edition

Page 13: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

From ECE 6440 Lecture by P. Allen

Page 14: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William
Page 15: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Example: Determine the percent change in resistance of a 5K Polysilicon

resistor as the temperature increases from 30oC to 60oC if the TCR is

constant and equal to 1500 ppm/oC

Thus the resistor increases by 4.5%

2 1 2 1 61

10

TCRR T R T T T

2 1 6

2 1

2 1

15001 30

10

1 .045

1.045

oR T R T C

R T R T

R T R T

What is R(T1) as stated in this example ? 5K?It is around 5K but if we want to be specific, would need to specify T

Did not need R(T1) to answer this question !

Page 16: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Basic Devices and Device Models

• Resistor

• Diode

• Capacitor

• MOSFET

• BJT

Page 17: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

http://www.dayah.com/periodic/Images/periodic%20table.png

Page 18: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William
Page 19: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

4 valence-band

Electrons

group (or family)

All elements in group IV have 4 valence-band electrons

Page 20: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Only 3 Valence-

band Electrons

Serves as an “acceptor” of electrons

Acts as a p-type impurity when used as a silicon dopant

All elements in group III have 3 valence-band electrons

Page 21: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

http://www.oftc.usyd.edu.au/edweb/devices/semicdev/doping4.html

Page 22: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Five Valence-

band Electrons

Serves as an “donor ” of electrons

Acts as an n-type impurity when used as a silicon dopant All elements in group V have 5 valence-band electrons

Page 23: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William
Page 24: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William
Page 25: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

B (Boron) widely used a dopant for creating p-type regions

P (Phosphorus) widely used a dopant for creating n-type regions

(bulk doping, diffuses fast)

As (Arsenic) widely used a dopant for creating n-type regions

(Active region doping, diffuses slower)

Silicon Dopants in Semiconductor Processes

Page 26: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Diodes (pn junctions)

Depletion region created that is ionized but void of carriers

Page 27: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

pn Junctions

Physical Boundary

Separating n-type and

p-type regions

If doping levels identical, depletion region extends

equally into n-type and p-type regions

Page 28: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

pn Junctions

Physical Boundary

Separating n-type and

p-type regions

Extends farther into p-type region if p-doping lower

than n-doping

Page 29: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

pn Junctions

Physical Boundary

Separating n-type and

p-type regions

Extends farther into n-type region if n-doping lower

than p-doping

Page 30: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

pn Junctions

VD

ID

• Positive voltages across the p to n junction are referred to forward bias

• As forward bias increases, depletion region thins and current starts to flow

• Current grows very rapidly as forward bias increases

• Current is very small under revere bias

• Negative voltages across the p to n junction are referred to reverse bias

Page 31: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

pn Junctions

ID

VD

Anode

Cathode

Anode

CathodeCircuit Symbol

Page 32: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

pn Junctions

• As forward bias increases, depletion region thins and current starts to flow

• Current grows very rapidly as forward bias increases

ID

VD

Anode

Cathode

Simple Diode Model:

D D

D D

V =0 I >0

I =0 V <0

VD

ID

Simple model often referred to as the “Ideal” diode model

Page 33: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

pn JunctionsID

VD

Simple Diode Model:

VD

ID

pn junction serves as a “rectifier” passing current in one direction and blocking it

in the other direction

Page 34: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Rectifier Application: Simple Diode Model:

VD

ID

1K

VOUT

D1

VIN=VMsinωt

VIN

VM

t

VM

t

VIN

VOUT

Page 35: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

I-V characteristics of pn junction(signal or rectifier diode)

Vd

Id

d

t

V

nV

D SI I e 1

Diode Equation

Improved Diode Model:IS in the 10fA to 100fA range

What is Vt at room temp?

t

kTV =

q

k= 1.380 64852 × 10−23JK-1

q = −1.60217662×10−19 Ck/q=8.62× 10−5 VK-1

Vt is about 26mV at room temp

Diode equation due to William

Shockley, inventor of BJT

In 1919, William Henry Eccles

coined the term diode

In 1940, Russell Ohl “stumbled

upon” the p-n junction diode

IS proportional to junction area

n typically about 1

Page 36: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

I-V characteristics of pn junction(signal or rectifier diode)

Vd

Id

SD II

Diode Characteristics

0

0.002

0.004

0.006

0.008

0.01

0 0.1 0.2 0.3 0.4 0.5 0.6 0.7

Vd (volts)

Id (

am

ps)

d

t

V

nV

D SI I e 1

Diode Equation

Under reverse bias (Vd<0),

Under forward bias (Vd>0),

d

t

V

nV

D SI I e

Diode Equation or forward bias simplification is unwieldy to work with analytically

Improved Diode Model:

Simplification of Diode Equation:

Simplification essentially identical model except for Vd very close to 0

IS in 10fA -100fA range (for signal diodes)

Vt is about 26mV at room temp

t

kTV =

q

k/q=8.62× 10−5 VK-1

n typically about 1

Page 37: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Diode Equation (even simplification) unwieldly to work with analytically. Why?

World’s simplest diode circuit 1K

VOUTD1

VIN=5V

VIN

ID + -VD

Determine VOUT

5

1

D

t

D OUT

OUT D

V

nV

D S

V V

V I K

I I e

Assume forward bias , simplified diode equation model

5

1OUT

t

V

nV

OUT SV I e K

VOUT=?

Explicit expression does not exist for VOUT !

3 independent equations and 3 unknowns

Page 38: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

I-V characteristics of pn junction(signal or rectifier diode)

SD II

d

t

V

nV

D SI I e 1

Diode Equation

Under reverse bias,

Under forward bias,

d

t

V

nV

D SI I e

Improved Diode Model:

Simplification of Diode Equation:

IS often in the 10fA to 100fA range

Vt is about 26mV at room temp

How much error is introduced using the simplification for Vd > 0.5V ? (assume n=1)

9

0 5

026

14 4 10

.

.

.

e

How much error is introduced using the simplification for Vd < - 0.5V? 0 5

9026 4 4 10.

. .e

Simplification almost never introduces any significant error

1eI

eI1eI

t

d

t

d

t

d

V

V

S

V

V

S

V

V

S

IS proportional to junction area

Page 39: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Will you impress your colleagues or your boss if you use the more exact diode equation when Vd < -0.5V or Vd > +0.5V ?

Will your colleagues or your boss be unimpressed if you use the more exact diode equation when Vd < -0.5V or Vd > +0.5V ?

Page 40: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

pn Junctions

VI

0V0

0VAeJITnV

V

S

I

V

Diode Equation:(good enough for most applications)

JS= Sat Current Density (in the 1aA/u2 to 1fA/u2 range)

A= Junction Cross Section Area

VT=kT/q (k/q=1.381x10-23V•C/°K/1.6x10-19C=8.62x10-5V/°K)

n is approximately 1

Anode

Cathode

Note: IS=JsA

Page 41: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

pn Junctions

0V0

0VAeJITnV

V

S I

V

Diode Equation:Anode

Cathode

JS is strongly temperature dependent

G0

t

-V

nVm

S SXJ J T e

With n=1, for V>0,

Typical values for key parameters: JSX=0.5A/μ2, VG0=1.17V, m=2.3, n=1

G0 D

t t

-V V

nV nVm

SXI(T) J T e Ae

Page 42: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

Stay Safe and Stay Healthy !

Page 43: EE 330 Lecture 13 Devices in Semiconductor Processesclass.ece.iastate.edu/ee330/lectures/EE 330 Lect 13 Fall...Diode equation due to William Shockley, inventor of BJT In 1919, William

End of Lecture 13