Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John...

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Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University

Transcript of Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John...

Page 1: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon

Chun Hyung Cho & John Sunwoo

Electrical & Computer Engineering

Auburn University

Page 2: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

OUTLINE Introduction

Piezoresistive Theory

Results of Measurements

Discussion

Conclusion

Page 3: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

INTRODUCTION Stress due to mechanical loadings

Degradation of performance

Stress analyses of electronic packages and their components have been performed

Page 4: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

INTRODUCTION(continued)

The basic application concepts

Semiconductor chips are incorporated into electronic packages

The sensors have most often been resistors

Page 5: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

Schematic of normal 4PB fixture

Page 6: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

Basic BMW2 Test Chip (200 x 200 mils)

The doped active region

is typically designed

using a serpentine

pattern

Electrical isolation

between the doped

surface resistor and the

bulk of the chip

Page 7: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

(111) silicon wafer & stress-induced resistance changes

Page 8: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

Result: p-type resistance changeTypical vaule: B1

p =507/TPa, B2p = -145/TPa

R0/R0 vs. Stress: P-type (111 Silicon)

y = 4.588E-04x + 1.514E-04

R2 = 9.998E-01

0.000E+00

5.000E-03

1.000E-02

1.500E-02

2.000E-02

2.500E-02

3.000E-02

0 10 20 30 40 50 60 70

Uniaxial Stress (:Mpa)

R/R

R90/R90 vs. Stress: P-type (111 Silicon)

y = -1.249E-04x + 1.453E-04

R2 = 9.986E-01

-1.2000E-02

-1.0000E-02

-8.0000E-03

-6.0000E-03

-4.0000E-03

-2.0000E-03

0.0000E+00

2.0000E-03

0 20 40 60 80 100

Uniaxial Stress (:Mpa)

R/

R

Page 9: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

Result: n-type resistance changeTypical vaule: B1

n =-230/TPa, B2n =

207/TPa

R0/R0 vs. Stress: n-type (111 Silicon)

y = -2.031E-04x

R2 = 9.880E-01

-1.400E-02

-1.200E-02

-1.000E-02

-8.000E-03

-6.000E-03

-4.000E-03

-2.000E-03

0.000E+00

0 10 20 30 40 50 60 70

Uniaxial Stress (:Mpa)

R/R

R90/R90 vs. Stress: n-type (111 Silicon)

y = 1.967E-04x

R2 = 9.967E-01

-2.0000E-03

0.0000E+00

2.0000E-03

4.0000E-03

6.0000E-03

8.0000E-03

1.0000E-02

1.2000E-02

1.4000E-02

0 10 20 30 40 50 60 70

Uniaxial Stress ( :Mpa)

R/

R

Page 10: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

Discussion: Typical piezo-resistive coefficient values for BMW2

Typical Piezoresistive Coefficient Values For BMW-2

Test Chips (TPa)-1

Piezoresistive p-type n-type

Coefficient Silicon Silicon

507 -230

-145 207

[From J . C. Suhling, R. W. J ohnson, and R. C. J aeger]

B1

B2

Page 11: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

DISCUSSION IntelliSuite software is used Under-estimated result Measured resistance changes was

assumed to be independent of T Beam rotation error Loading symmetry error Weight and length measurement

error

Page 12: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

CONCLUSION Measurements of piezoresistive

coefficients in lightly doped (111) silicon Applications of piezoresistive sensors in

electronic packaging. The sensors are not mounted on the chips. Integral part of the structure to be

analyzed by the way of the fabrication process.

Page 13: Measurements of Piezoresistive Coefficients in Lightly Doped (111) Silicon Chun Hyung Cho & John Sunwoo Electrical & Computer Engineering Auburn University.

CONCLUSION (Continued)

The sensor are capable of providing non-intrusive measurements of surface on chip even within encapsulated packages.

Piezoresistive stress sensors have much higher sensitivity than metallic stress sensors.