Basic Semiconductor Processes Devices in Semiconductor

37
EE 434 Lecture 13 Basic Semiconductor Processes Devices in Semiconductor Processes

Transcript of Basic Semiconductor Processes Devices in Semiconductor

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EE 434Lecture 13

Basic Semiconductor Processes Devices in Semiconductor Processes

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Quiz 9 The top view of a device fabricated in a bulk CMOS process is shown in the figure below

a) Identify the deviceb) Sketch a cross-section along the AA’ section line

Metal 1

Poly 1

A A’

Active

p-select

n-well

Contact

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And the number is ….

631

24578

9

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Quiz 9 Solution

A A’

a) p-channel MOS Transistor

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• Process Flow is a “recipe” for the process– Shows what can and can not be made – Gives insight into performance capabilities and

limitations– Designer has control only of top view– Some masks may be automatically generated– Geometric Description File (GDF) contains all

information about a layout and serves as interface with foundry

Review from Last Time

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A A’

B’B

C

C’

D

D’

Guard Rings and Bulk Attachment

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Basic Devices and Device Models

• Resistor• Diode• Capacitor• MOSFET• BJT

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Basic Devices and Device Models

• Resistor• Diode • Capacitor• MOSFET• BJT

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Device ModelingGoal: Obtain a mathematical relationship between the port variables of a device.

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Device ModelingGoal: Obtain a mathematical relationship between the port variables of a device.

I1

I2

I3 V1V2

V3

4-TerminalDevice

Without loss of generality, one terminal can be selected as a reference(this can be done in one of 4 ways!)

Thus modeling problem is that of determining mathematical relationshipBetween the six variables I1, I2, I3, V1, V2, and V3

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Device Modeling

I1

I2

I3 V1V2

V3

4-TerminalDevice

Goal: Obtain a mathematical relationship between the port variables of a device.

Any 3 of the 6 variables I1, I2, I3, V1, V2, V3 can be selected as independent variables and the remaining 3 variables can be selected as dependent variables

There are 20!3!3

!636

==⎟⎟⎠

⎞⎜⎜⎝

⎛ ways this can be done

Thus there are 4x20=80 different mathematical representations of a 4-terminaldevice and all predict identical performance !

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Device Modeling

I1

I2

I3 V1V2

V3

4-TerminalDevice

Goal: Obtain a mathematical relationship between the port variables of a device.

By convention, will pick V1, V2, V3 as the independent variables and I1, I2, I3as the dependent variables

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Device Modeling

I1

I2

I3 V1V2

V3

4-TerminalDevice

Goal: Obtain a mathematical relationship between the port variables of a device.

Modeling Goal: Obtain f1, f2, and f3 that sufficiently accurately characterize the device

( )( )( ) ⎪

⎪⎬

===

32111

32111

32111

V,,VVfIV,,VVfIV,,VVfI

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Device Modeling

( )( )( ) ⎪

⎪⎬

===

32133

32122

32111

V,,VVfIV,,VVfIV,,VVfI

Goal: Obtain a mathematical relationship between the port variables of a device.

( )( ) ⎭

⎬⎫

==

2122

2111

,VVfI,VVfI

( ) 111 VfI =

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Resistors• Generally thin-film devices• Almost any thin-film layer can be used as a resistor

– Diffused resistors– Poly Resistors– Metal Resistors– “Thin-film” adders (SiCr or NiCr)

• Subject to process variations, gradient effects and local randomvariations

• Often temperature and voltage dependent– Ambient temperature– Local Heating

• Nonlinearities often a cause of distortion when used in circuits• Trimming possible resistors

– Laser,links,switches

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Resistor Model

V

W d

L

I

IVR =

Model:

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Resistivity

• Volumetric measure of conduction capability of a material

LR

Areais A

LAR

for homogeneousmaterial,ρ ⊥ A, R, Lunits : ohm cm

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Sheet Resistance

R

W d

L

LRW R = ( for d << w, d << L ) units : ohms /

for homogeneous materials, R is independent of W, L, R

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Relationship between ρ and R

d WA ×=LAR

RWA

=ρLRW R =

RxdRW

dW RWA

===ρ

Number of squares, NS, often used instead of L / W in determining resistance of film resistors

R=RNS

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Example 1

W

R = ?

L

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Example 1

W

L

SNWL

=

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Example 1

.4 8 7 6 5 4 3 2 1

R = ?

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Example 1

.4 8 7 6 5 4 3 2 1

R = R (8.4)

R = ?

NS=8.4

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Corners in Film Resistors

Rule of Thumb: .55 squares for each corner

Corner

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Example 2Determine R if R = 100 Ω /

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Example 2

1 2 3 4 5 6 .55

1 2 3 4 5 6 7 .55

1

2

3

NS=17.1R = (17.1) RR = 1710 Ω

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Resistivity of Materials used in Semiconductor Processing

• Cu: 1.7E-6 Ωcm• Al: 2.7E-4 Ωcm• Gold: 2.4E-6 Ωcm• Platinum: 3.0E-6 Ωcm• n-Si: .25 to 5 Ωcm• intrinsic Si: 2.5E5 Ωcm• SiO2: E14 Ωcm

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Temperature CoefficientsUsed for indicating temperature sensitivity of resistors & capacitors

Cppm dTdR

R1TCR

610

tempop.

°⎟⎠⎞

⎜⎝⎛=

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

( ) ( )TCR

10TT

126

12

TRTR−

= e

( ) ( ) ( ) ⎥⎦⎤

⎢⎣⎡ −+≈ 61212 10

TCRTT1 TRTR

For a resistor:

Identical Expressions for Capacitors

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Voltage CoefficientsUsed for indicating voltage sensitivity of resistors & capacitors

Vppm dVdR

R1VCR

610

voltage ref

⎟⎠⎞

⎜⎝⎛=

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

( ) ( )VCRVV

12

12

VRVR 610−

= e

( ) ( ) ( ) ⎥⎦⎤

⎢⎣⎡ −+≈ 61212 10

VCRVV VRVR 1

For a resistor:

Identical Expressions for Capacitors

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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 resistors

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End of Lecture 13

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Basic Devices and Device Models

• Resistor• Diode• Capacitor• MOSFET• BJT

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Diodes (pn junctions)

Depletion region created that is ionized but void of carriers

N P

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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

N P

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pn Junctions

Physical Boundary Separating n-type and p-type regions

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

N+ P-

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pn Junctions

Physical Boundary Separating n-type and p-type regions

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

N- P+

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pn Junctions

VI

N P