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EE 434 Lecture 11 Process Flow Device Modeling in Semiconductor Processes

EE 434 Lecture 11

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Page 1: EE 434 Lecture 11

EE 434Lecture 11

Process Flow

Device Modeling in Semiconductor Processes

Page 2: EE 434 Lecture 11

Quiz 5Three methods of attaching the die to a package or circuit were discussed. Give two of them.

Page 3: EE 434 Lecture 11

And the number is ….

6

31

2

45

7

8

9

Page 4: EE 434 Lecture 11

And the number is ….

6

31

2

4

5

7

8

9

Page 5: EE 434 Lecture 11

Quiz 5Three methods of attaching the die to a package or circuit were discussed. Give two of them.

Solution:

EutecticSolder PreformConductive Epoxy

Page 6: EE 434 Lecture 11

Review from Last TimeInterconnects Introduce Parasitic Capacitances

Vertical Layer to LayerC=AOLCD

Lateral Layer to LayerMore difficult to Model

DiffusionBottom (area dependent)

C=ADCDSidewall (fringe)

C=PDCDL

Back-End Processing StepsNot closely coupled with specific front-end processDicingDie AttachBondingPackaging

Page 7: EE 434 Lecture 11

Review from Last TimeInterconnects Introduce Parasitic Capacitances

Vertical Layer to LayerC=AOLCD

Lateral Layer to LayerMore difficult to Model

DiffusionBottom (area dependent)

C=ADCDSidewall (fringe)

C=PDCDL

Back-End Processing StepsNot closely coupled with specific front-end processDicingDie AttachBondingPackaging

Page 8: EE 434 Lecture 11

Basic Semiconductor ProcessesMOS (Metal Oxide Semiconductor)

1. NMOS n-ch2. PMOS p-ch3. CMOS n-ch & p-ch– Basic Device: MOSFET– Niche Device: MESFET– Other Devices: Diode

BJTResistorsCapacitorsSchottky Diode

Review from Last Time

Page 9: EE 434 Lecture 11

Basic Semiconductor Processes

1. T2L2. ECL3. I2L4. Linear ICs

– Basic Device: BJT (Bipolar Junction Transistor)– Niche Devices: HBJT (Heterojunction Bipolar Transistor)

HBT– Other Devices: Diode

ResistorCapacitorSchottky DiodeJFET (Junction Field Effect Transistor)

Bipolar

Review from Last Time

Page 10: EE 434 Lecture 11

Basic Semiconductor Processes

• Thin and Thick Film Processes– Basic Device: Resistor

• BiMOS or BiCMOS– Combines both MOS & Bipolar Processes– Basic Devices: MOSFET & BJT

• SiGe– BJT with HBT implementation

• SiGe / MOS– Combines HBT & MOSFET technology

• SOI / SOS (Silicon on Insulator / Silicon on Sapphire)• Twin-Well & Twin Tub CMOS

– Very similar to basic CMOS but more optimal transistor char.

Other Processes

Review from Last Time

Page 11: EE 434 Lecture 11

Summary of Devices by Processes• Standard CMOS Process

– MOS Transistors• n-channel• p-channel

– Capacitors– Resistors– Diodes– BJT (in some processes)

• npn• pnp

– JFET (in some processes)• n-channel• p-channel

• Standard Bipolar Process– BJT

• npn• pnp

– JFET • n-channel• p-channel

– Diodes– Resistors– Capacitors

• Niche Devices– Photodetectors (photodiodes, phototransistors, photoresistors)– MESFET– HBT– Schottky Diode (not Shockley)

– MEM Devices– ….

Review from Last Time

Page 12: EE 434 Lecture 11

Process Flow

Processing Steps Have Been Discussed

Wafer Prep, Photolithography, Deposition, Etching, Diffusion, …

Combining these Processing Steps to Make Useful Integrated Circuits constitutes a Process Flow

Each Process has a unique process flowProcess flow constitutes very valuable IP

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Basic Devices• Devices in Standard Processes

– MOS Transistors• n-channel• p-channel

– Capacitors– Resistors– Diodes– BJT (in some processes)

• npn• pnp

• Niche Devices– Photodetectors– MESFET– Schottky Diode (not Shockley)

– MEM Devices– ….

Primary Consideration in This Course

Limited Consideration in This Course

Page 27: EE 434 Lecture 11

Basic Devices and Device Models

• Resistor• Capacitor• MOSFET• Diode• BJT

Page 28: EE 434 Lecture 11

Basic Devices and Device Models

• Resistor• Capacitor• MOSFET• Diode• BJT

- Resistors and Capacitors were discussed previously in the context ofinterconnects

- Were generally considered parasitics in earlier discussions- Will now be considered as desired components- Models obviously will be very similar or identical

Page 29: EE 434 Lecture 11

Basic Devices and Device Models

• Resistor• Capacitor • MOSFET• Diode• BJT

Page 30: EE 434 Lecture 11

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

Page 31: EE 434 Lecture 11

Resistor Model

V

W d

L

I

IVR =

Model:

Page 32: EE 434 Lecture 11

Resistivity

• Volumetric measure of conduction capability of a material

LR

Areais A

LAR

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

Page 33: EE 434 Lecture 11

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

Page 34: EE 434 Lecture 11

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

Page 35: EE 434 Lecture 11

Example 1

W

R = ?

L

Page 36: EE 434 Lecture 11

Example 1

W

L

SNWL

=

Page 37: EE 434 Lecture 11

Example 1

.4 8 7 6 5 4 3 2 1

R = ?

Page 38: EE 434 Lecture 11

Example 1

.4 8 7 6 5 4 3 2 1

R = R (8.4)

R = ?

NS=8.4

Page 39: EE 434 Lecture 11

Corners in Film Resistors

Rule of Thumb: .55 squares for each corner

Corner

Page 40: EE 434 Lecture 11

Example 2Determine R if R = 100 Ω /

Page 41: EE 434 Lecture 11

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

Page 42: EE 434 Lecture 11

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

Page 43: EE 434 Lecture 11

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

Page 44: EE 434 Lecture 11

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

Page 45: EE 434 Lecture 11

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

Page 46: EE 434 Lecture 11

Capacitance and Resistance in Interconnects

• See MOSIS WEB site for process parameters that characterize parasitic resistances and capacitances

www.mosis.org

Page 47: EE 434 Lecture 11

Basic Devices and Device Models

• Resistor• Capacitor • MOSFET• Diode• BJT

Page 48: EE 434 Lecture 11

CapacitanceC

A1

cond1 insulator

A2cond2

Parallel Plate

dAC ∈

= A = area of intersection of A1 & A2

d

Page 49: EE 434 Lecture 11

Capacitance

dC hereA wCC

areaunit CapC If ddd

∈===

Parallel Plate

Page 50: EE 434 Lecture 11

Capacitance

d pn

depletionregion

C

Junction Capacitor

dAC ∈

=

Note: d is voltage dependent-capacitance is voltage dependent-usually parasitic caps-varicaps or varactor diodes exploit

voltage dep. of C