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Barcelona, 31 May- 2 June 2010 Barcelona, 31 May- 2 June 2010 1 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

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Page 1: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 11

Contacts to High-Resistivity Semiconductors

Arie Ruzin

School of EE, Faculty of Engineering, Tel Aviv University, Israel

Page 2: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 22

Outline

• Motivation

• Schottky and Ohmic contacts to Low- semiconductors

• Simulated results for Low- and High- semiconductors

• Injecting contacts to High- semiconductors

• Space Charge Limited Current

• Summary

Page 3: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 33

“Classic” Presentation for High- Energy Bands (??)

Page 4: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 44

Taking Into Account Majority Carriers Only (??)

Majority Carriers only?

Page 5: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 55

Thermionic Emission (??)

Thermionic emission ?

Page 6: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 66

Thermionic emission ?

Thermionic Emission (??), 1.5eV barriers (?)

Page 7: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 77

Textbook Contacts (Low-Textbook Contacts (Low- Semiconductor) Semiconductor)

Ei

Schottky Ohmic Ohmic injecting?

EF

qB EC

EV

Metal Semiconductor

qF

qs

EF

Ei

EC

EV

qF

Metal Semiconductor

EF

Ei

EC

EV

qF

qB

Metal Semiconductor

Page 8: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 88

Low- CdTe Diode (ND=1015,B=1eV)(The diode is 1 mm long)

Zoom on the front 10 m

Zero Bias

Low Bias

-2

-1.5

-1

-0.5

0

0.5

1

1.5

0 2 4 6 8 10

Depth [m]

En

erg

y [

eV

]

ConductionBandEnergy

ValenceBandEnergy

eQuasiFermiPotential

-2.5

-2

-1.5

-1

-0.5

0

0.5

1

1.5

0 2 4 6 8 10

Depth [m]

En

erg

y [

eV

]

C-Band V-Band

C_Band-0.5V V_Band-0.5V

C-Band+0.5V V-Band+0.5V

Energy band structure

Page 9: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 99

Forward Bias

-2.E+03

0.E+00

2.E+03

4.E+03

6.E+03

8.E+03

1.E+04

1.E+04

1.E+04

2.E+04

2.E+04

0 2 4 6 8 10Depth [um]

E-F

ield

[V

/cm

]

VB=0V

VB=0.5V

VB=2V

VB=5V

VB=8V

VB=10V

Reverse Bias

-1.E+04

0.E+00

1.E+04

2.E+04

3.E+04

4.E+04

5.E+04

6.E+04

7.E+04

0 2 4 6 8 10Depth [um]

E-F

ield

[V

/cm

]

VB=0V

VB=-0.5V

VB=-2V

VB=-5V

VB=-8V

VB=-10V

Low- CdTe Diode (ND=1015,B=1eV)(The diode is 1 mm long)

Zoom on the front 10 mE-field profiles under bias

Page 10: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 1010

Reverse Bias

1.E-01

1.E+01

1.E+03

1.E+05

1.E+07

1.E+09

1.E+11

1.E+13

1.E+15

0 2 4 6 8 10Depth [m]

e-

De

ns

ity

[c

m-3

]

VB=0V

VB=-0.5V

VB=-2V

VB=-5V

VB=-8V

VB=-10V

Reverse Bias

1.E-111.E-09

1.E-071.E-051.E-031.E-01

1.E+011.E+031.E+05

1.E+071.E+09

0 10 20 30 40 50Depth [m]

h-

De

ns

ity

[c

m-3

]

VB=0V

VB=-0.5V

VB=-2V

VB=-5V

VB=-8V

VB=-10V

Forward Bias

0.E+001.E+142.E+143.E+144.E+145.E+146.E+147.E+148.E+149.E+141.E+15

0 2 4 6 8 10

Depth [um]

e-D

ensi

ty [

cm-3

]

VB=0V

VB=0.5V

VB=2V

VB=5V

VB=8V

VB=10V

Forward Bias

1.E-06

1.E-04

1.E-02

1.E+00

1.E+02

1.E+04

1.E+06

1.E+08

1.E+10

0 200 400 600 800 1000

Depth [um]

h-D

en

sit

y [

cm

-3]

VB=0V VB=0.5V

VB=2V VB=5V

VB=8V VB=10V

Low- CdTe Diode (ND=1015,B=1eV)Free carrier densities

Page 11: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 1111

Low- CdTe Diode (ND=1015,B=1eV)(The diode is 1 mm long)

Current density

1.E-07

1.E-05

1.E-03

1.E-01

1.E+01

1.E+03

1.E+05

1.E+07

1.E+09

-1 0 1 2Bias [V]

J [

nA

/cm

2 ]

JT0.8eV [nA/cm2]

JT1.0eV [nA/cm2]

JT1.5eV [nA/cm2]

JT1.3eV [nA/cm2]

Thermionic emission limited

Bulk limited

2

0.16

1.50.16 2.4

0.1

nq n

V AJ

cm cm

E

Page 12: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 1212

EF

Ei

qB EC

EV

Metal Semiconductor

qF

qs

EF

Ei

EC

EV

qF

qB

Metal Semiconductor

EF

Ei

EC

EV

qF

Metal Semiconductor

High- Schottky Diode (?)

Schottky Ohmic Ohmic injecting?

Page 13: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 1313

-1

-0.5

0

0.5

1

1.5

0 200 400 600 800 1000

Depth [m]

En

erg

y [

eV

]

-3.5

-3

-2.5

-2

-1.5

-1

-0.5

0

0.5

1

1.5

0 200 400 600 800 1000

Depth [m]

En

erg

y [

eV

]

C-Band V-BandC-Band-0.5V V-Band-0.5VC-Band-2V V-Band-2V

-1.5

-1

-0.5

0

0.5

1

1.5

2

2.5

3

0 200 400 600 800 1000

Depth [m]

En

erg

y [

eV

]

C-Band V-Band

C-Band+0.5V V-Band+0.5V

C-Band+2V V-Band+2V

High- CdTe Diode (ND=106,B=1eV)

Zero Bias

Low Bias

Energy band structure

Page 14: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 1414

Reverse Bias

1.E+03

1.E+04

1.E+05

1.E+06

1.E+07

1.E+08

1.E+09

0 200 400 600 800 1000

Depth [m]

h-

De

ns

ity

[cm

-3]

VB=0V

VB=-0.5V

VB=-2V

VB=-5V

VB=-8V

VB=-10V

Reverse Bias

1.E+01

1.E+02

1.E+03

1.E+04

1.E+05

1.E+06

0 200 400 600 800 1000Depth [m]

e-

De

ns

ity

[c

m-3

]

VB=0V

VB=-0.5V

VB=-2V

VB=-5V

VB=-8V

VB=-10V

Forward Bias

1.E+03

1.E+04

1.E+05

1.E+06

1.E+07

1.E+08

1.E+09

1.E+10

0 200 400 600 800 1000

Depth [m]

h-D

en

sit

y [

cm

-3]

VB=0V

VB=0.5V

VB=2V

VB=5V

VB=8V

VB=10V

Forward Bias

1.0E+00

1.0E+01

1.0E+02

1.0E+03

1.0E+04

1.0E+05

1.0E+06

1.0E+07

0 200 400 600 800 1000Depth [m]

e-D

en

sit

y [

cm

-3]

VB=0V

VB=0.5V

VB=2V

VB=5V

VB=8V

VB=10V

High- CdTe Diode (ND=106,B=1eV)

Free carrier densities

Page 15: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 1515

-5.0E-13

0.0E+00

5.0E-13

1.0E-12

1.5E-12

2.0E-12

2.5E-12

-10 -5 0 5 10

Bias [V]

Cu

rren

t [A

]

-4.0E-17

-3.5E-17

-3.0E-17

-2.5E-17

-2.0E-17

-1.5E-17

-1.0E-17

-5.0E-18

0.0E+00

-10 -8 -6 -4 -2 0

Bias [V]

Cu

rren

t [A

]

High- CdTe Diode (ND=106,B=1eV)

Forward and Reverse Currents

Page 16: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 1616

-1.5

-1

-0.5

0

0.5

1

1.5

0 200 400 600 800 1000

Depth [ m ]

En

erg

y [e

V]

-1.5

-1

-0.5

0

0.5

1

1.5

2

2.5

3

0 200 400 600 800 1000

Depth [m]

En

erg

y [e

V]

C-Band V-Band

C-Band+0.5V V-Band+0.5V

C-Band+2V V-Band+2V

-3.5-3

-2.5-2

-1.5-1

-0.50

0.51

1.52

0 200 400 600 800 1000Depth [m]

En

erg

y [e

V]

C-Band V-Band

C-Band-0.5V V-Band-0.5V

C-Band-2V V-Band-2V

High- CdTe Diode (ND=106,B=1.3eV)

Zero Bias

Low Bias

Energy band structure

Page 17: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 1717

High- CdTe Diode (ND=106,B=1.3eV)Free Carrier Concentration

Reverse Bias

1.E-04

1.E-02

1.E+00

1.E+02

1.E+04

1.E+06

1.E+08

0 200 400 600 800 1000

Depth [m]

e- D

ensi

ty [

cm-3

]

VB=0V VB=-0.5V

VB=-2V VB=-5V

VB=-8V VB=-10V

Reverse Bias

1.E+03

1.E+05

1.E+07

1.E+09

1.E+11

1.E+13

1.E+15

0 200 400 600 800 1000

Depth [m]

h-

Den

sity

[cm

-3]

VB=0V

VB=-0.5V

VB=-2V

VB=-5V

VB=-8V

VB=-10V

Forward Bias

1.E-04

1.E-02

1.E+00

1.E+02

1.E+04

1.E+06

1.E+08

1.E+10

0 200 400 600 800 1000

Depth [m]

e-D

ensi

ty [

cm-3

]

VB=0V VB=0.5V

VB=2V VB=5V

VB=8V VB=10V

Forward Bias

1.E+03

1.E+05

1.E+07

1.E+09

1.E+11

1.E+13

1.E+15

0 200 400 600 800 1000Depth [m]

h-D

ensi

ty [

cm-3

]

VB=0V VB=0.5V

VB=2V VB=5V

VB=8V VB=10V

Page 18: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 1818

High- CdTe Diode (ND=106,B=1.3eV)

E-Field and Potential profilesReverse Bias

-12

-10

-8

-6

-4

-2

0

2

0 200 400 600 800 1000Depth [m]

Po

ten

tial

[eV

]

VB=0V

VB=-0.5V

VB=-2V

VB=-5V

VB=-8V

VB=-10V

Reverse Bias

1

10

100

1000

0 200 400 600 800 1000

Depth [um]

E-F

ield

[V

/cm

]

VB=0V VB=-0.5V VB=-2V

VB=-5V VB=-8V VB=-10V

Forward Bias

-2

0

2

4

6

8

10

12

0 200 400 600 800 1000

Depth [m]

Po

ten

tia

l [e

V]

VB=0V

VB=0.5VVB=2V

VB=5V

VB=8VVB=10V

Forward Bias

0.01

0.1

1

10

100

1000

0 200 400 600 800 1000Depth [m]

E-F

ield

[V

/cm

]

VB=0V VB=0.5VVB=2V VB=5V

VB=8V VB=10V

Page 19: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 1919

Forward Bias =10V

-1

-0.5

0

0.5

1

1.5

2

0 50 100 150 200 250 300

Depth [m]E

ne

rgy

Ba

nd

s [

eV

]

High- CdTe Diode (ND=106,B=1.3eV)

Band Structure under forward bias

EC

EV

Forward Bias

-1

-0.5

0

0.5

1

1.5

2

0 200 400 600 800 1000Depth [m]

Va

len

ce

Ba

nd

En

erg

y [

eV

]

VB=0V

VB=0.5V

VB=2V

VB=5V

VB=8V

VB=10V

Page 20: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 2020

High- CdTe Diode (ND=106,B=1.3eV)

Forward and Reverse Currents

-4.E-17

-4.E-17

-3.E-17

-3.E-17

-2.E-17

-2.E-17

-1.E-17

-5.E-18

0.E+00

-10 -8 -6 -4 -2 0Bias [V]

Cur

rent

[A

]

-5.E-12

0.E+00

5.E-12

1.E-11

2.E-11

2.E-11

3.E-11

3.E-11

-10 -5 0 5 10Bias [V]

Cu

rren

t [A

]0.E+00

5.E-12

1.E-11

2.E-11

2.E-11

3.E-11

3.E-11

0 2 4 6 8 10Bias [V]

I [A

]

Itotal,1.3eV

J*A (Mott's)

2

0 3

9

8Mott CdTe

VJ

L

Mott’s Law fit:

Page 21: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 2121

Reverse Bias

1.E-041.E-031.E-021.E-011.E+001.E+011.E+021.E+031.E+041.E+051.E+061.E+07

0 200 400 600 800 1000

Depth [m]

e-

De

ns

ity

[cm

-3]

VB=0V VB=-0.5V

VB=-2V VB=-5V

VB=-8V VB=-10V

Reverse Bias

1.E+031.E+041.E+051.E+061.E+071.E+081.E+091.E+101.E+111.E+121.E+131.E+14

0 200 400 600 800 1000

Depth [m]

h-

De

ns

ity

[c

m-3

]

VB=0V

VB=-0.5V

VB=-2V

VB=-5V

VB=-8V

VB=-10V

High- CdTe Diode (ND=106,B=1.3eV,SRH)

With SRH RecombinationReverse Bias

1.E-04

1.E-02

1.E+00

1.E+02

1.E+04

1.E+06

1.E+08

0 200 400 600 800 1000

Depth [m]

e- D

ensi

ty [

cm-3

]

VB=0V VB=-0.5V

VB=-2V VB=-5V

VB=-8V VB=-10V

Reverse Bias

1.E+03

1.E+05

1.E+07

1.E+09

1.E+11

1.E+13

1.E+15

0 200 400 600 800 1000

Depth [m]

h-

Den

sity

[cm

-3]

VB=0V

VB=-0.5V

VB=-2V

VB=-5V

VB=-8V

VB=-10V

Without SRH Recombination

Free Carrier Concentration with and without SRH

Page 22: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 2222

Forward Bias

1.E+03

1.E+05

1.E+07

1.E+09

1.E+11

1.E+13

1.E+15

0 200 400 600 800 1000

Depth [m]

h-D

en

sit

y [

cm

-3]

VB=0V VB=0.5VVB=2V VB=5V

VB=8V VB=10V

Forward Bias

1.E-04

1.E-02

1.E+00

1.E+02

1.E+04

1.E+06

1.E+08

0 200 400 600 800 1000Depth [m]

e-D

en

sit

y [

cm

-3]

VB=0V VB=0.5V

VB=2V VB=5V

VB=8V VB=10V

High- CdTe Diode (ND=106,B=1.3eV,SRH)Free Carrier Concentration with and without SRH

With SRH Recombination Without SRH RecombinationForward Bias

1.E-04

1.E-02

1.E+00

1.E+02

1.E+04

1.E+06

1.E+08

1.E+10

0 200 400 600 800 1000

Depth [m]

e-D

ensi

ty [

cm-3

]

VB=0V VB=0.5V

VB=2V VB=5V

VB=8V VB=10V

Forward Bias

1.E+03

1.E+05

1.E+07

1.E+09

1.E+11

1.E+13

1.E+15

0 200 400 600 800 1000Depth [m]

h-D

ensi

ty [

cm-3

]

VB=0V VB=0.5V

VB=2V VB=5V

VB=8V VB=10V

Page 23: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 2323

High- CdTe Diode (ND=106,B=1.3eV,SRH)Currents with and without SRH

-5.E-12

0.E+00

5.E-12

1.E-11

2.E-11

2.E-11

3.E-11

3.E-11

-10 -5 0 5 10

Bias [V]

Cu

rre

nt

[A]

Itotal, 1.3eV, +SRH

Itotal,1.3eV, -SRH

1.E-19

1.E-18

1.E-17

1.E-16

1.E-15

1.E-14

-10 -8 -6 -4 -2 0

Bias [V]

AB

S(C

urr

en

t) [

A]

Itotal, 1.3eV, +SRH

Itotal,1.3eV, -SRH

Page 24: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 2424

High- CdTe Diode (ND=106,B=0.2eV)Energy band structure

-2

-1.5

-1

-0.5

0

0.5

1

0 200 400 600 800 1000

Depth [m]

En

erg

y [e

V]

EC

EV

-3.5

-3

-2.5

-2

-1.5

-1

-0.5

0

0.5

1

0 200 400 600 800 1000

Depth [m]

En

erg

y [

eV

]

C-Band V-BandC-Band-0.5V V-Band-0.5VC-Band-2V V-Band-2V

-2

-1.5

-1

-0.5

0

0.5

1

1.5

2

2.5

3

0 200 400 600 800 1000Depth [m]

En

erg

y [

eV

]

C-Band V-BandC-Band+0.5V V-Band+0.5VC-Band+2V V-Band+2V

Page 25: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 2525

High- CdTe Diode (ND=106,B=0.2eV)Free Carrier Concentration

Reverse Bias

1.E-05

1.E-03

1.E-01

1.E+01

1.E+03

1.E+05

1.E+07

0 200 400 600 800 1000

Depth [m]

h-

De

ns

ity

[c

m-3

]

VB=0V VB=-0.5V VB=-2V

VB=-5V VB=-8V VB=-10V

Reverse Bias

1.E+00

1.E+02

1.E+04

1.E+06

1.E+08

1.E+10

1.E+12

1.E+14

1.E+16

0 200 400 600 800 1000

Depth [m]

e- D

ensi

ty [

cm-3

]

VB=0V VB=-0.5V

VB=-2V VB=-5V

VB=-8V VB=-10V

Forward Bias

1.E-05

1.E-03

1.E-01

1.E+01

1.E+03

1.E+05

0 200 400 600 800 1000

Depth [m]

h-D

ensi

ty [

cm-3

]

VB=0V VB=0.5VVB=2V VB=5VVB=8V VB=10V

Forward Bias

1.E+04

1.E+06

1.E+08

1.E+10

1.E+12

1.E+14

1.E+16

0 200 400 600 800 1000Depth [m]

e-D

ensi

ty [

cm-3

]

VB=0V VB=0.5V

VB=2V VB=5V

VB=8V VB=10V

Page 26: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 2626

High- CdTe Diode (ND=106,B=0.2eV)

Reverse Bias

1.E-02

1.E-01

1.E+00

1.E+01

1.E+02

1.E+03

1.E+04

0 200 400 600 800 1000

Depth [m]

E-F

ield

[V

/cm

]

VB=0V VB=-0.5VVB=-2V VB=-5VVB=-8V VB=-10V

Forward Bias

1.E+01

1.E+02

1.E+03

1.E+04

0 200 400 600 800 1000

Depth [m]

E-F

ield

[V

/cm

]

VB=0V VB=0.5VVB=2V VB=5V

VB=8V VB=10V

Forward Bias

0

2

4

6

8

10

12

0 200 400 600 800 1000

Depth [m]

Po

ten

tia

l [e

V]

VB=0V

VB=0.5V

VB=2V

VB=5V

VB=8V

VB=10V

Reverse Bias

-12

-10

-8

-6

-4

-2

0

2

0 200 400 600 800 1000

Depth [m]

Po

ten

tia

l [e

V]

VB=0V VB=-0.5V

VB=-2V VB=-5V

VB=-8V VB=-10V

E-Field and Potential profiles

Page 27: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 2727

High- CdTe Diode (ND=106,B=0.2eV)

Reverse Bias

-3

-2.5

-2

-1.5

-1

-0.5

0

0.5

1

0 200 400 600 800 1000Depth [m]

Co

nd

uct

ion

Ban

d E

ner

gy

[eV

]

VB=0V VB=-0.5V

VB=-2V VB=-5VVB=-8V VB=-10V

Reverse Bias=-10V

-2

-1.5

-1

-0.5

0

0.5

1

0 100 200 300 400

Depth [um]

Co

nd

uc

tio

n B

an

d E

ne

rgy

[e

V]

Band Structure

Page 28: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 2828

High- CdTe Diode (ND=106,B=0.2eV)Currents

Itotal,1.3eV

-4.0E-10

-3.5E-10

-3.0E-10

-2.5E-10

-2.0E-10

-1.5E-10

-1.0E-10

-5.0E-11

0.0E+00

5.0E-11

-10 -8 -6 -4 -2 0

Bias [V]

Cu

rre

nt

[A]

Itotal,0.2eV

J*A (Mott's)

-4.E-10

-4.E-10

-3.E-10

-3.E-10

-2.E-10

-2.E-10

-1.E-10

-5.E-11

0.E+00

5.E-11

-10 -5 0 5 10

Bias [V]

Cu

rre

nt

[A]

0.E+00

1.E-14

2.E-14

3.E-14

4.E-14

5.E-14

6.E-14

0 2 4 6 8 10Bias [V]

Cu

rren

t [A

]

2

0 3

9

8Mott CdTe

VJ

L

Mott’s Law fit:

Page 29: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 2929

Conclusions

• Band bending in high- semiconductors is mainly attributed to free carrier charge – NOT dopant ions

• In high- semiconductors Schottky devices thermionic emission is not the dominant forward current mechanism

• In case on any band bending (positive or “negative” barrier) the “bulk” resistivity is strongly affected by free carrier injection

• In case of significant Schottky barrier the current transport is dominated by minority carriers

• Space Charge Limited Current may occur both, in Schottky and “Ohmic” contacts (except flat-band conditions)

Page 30: Barcelona, 31 May- 2 June 20101 Contacts to High-Resistivity Semiconductors Arie Ruzin School of EE, Faculty of Engineering, Tel Aviv University, Israel

Barcelona, 31 May- 2 June 2010Barcelona, 31 May- 2 June 2010 3030

Thank you