electric properties of holes in narrow channels of si/sige heterostructures l. c. li a ( 李良箴...

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Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李李李 ) , W. H. Hsieh b ( 李李李 ), H.H. Cheng c ( 李李 李 ), C. H. Kuan b ( 李李李 ), and Y. W. Suen a ( 李李李 ) a.Department of Physics, National Chung Hsing University, Taichung, Taiwan, R.O.C. b.Department of Electrical Engineering, National Taiwan University, Taipei, Taiwan, R.O.C. c.Condensed Matter Science Center, National Taiwan University, Taipei, Taiwan, R.O.C.

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Introduction  Recently, quantum-ballistic transport in N-type Si/SiGe Heterostructure Has been investigated. The mobility is around several 10 5 cm 2 /Vs at 1.2K. [1],[2]  Generating nanostructure in the p-type Si/SiGe heterostructure  The mobility of samples we use is around several 10 3 cm 2 /Vs at 10K

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Page 1: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Electric properties of holes in narrow channels of Si/SiGe heterostructures

L. C. Lia(李良箴 ), W. H. Hsiehb(謝文興 ), H.H. Chengc(鄭鴻祥 ),C. H. Kuanb(管傑雄 ), and Y. W. Suena(孫允武 )

a.Department of Physics, National Chung Hsing University, Taichung, Taiwan, R.O.C.b.Department of Electrical Engineering, National Taiwan University, Taipei, Taiwan, R.O.C.c.Condensed Matter Science Center, National Taiwan University, Taipei, Taiwan, R.O.C.

Page 2: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Outline

Introduction Samples Process Results & Discussion Conclusion & Future work References

Page 3: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Introduction

Recently, quantum-ballistic transport in N-type Si/SiGe Heterostructure Has been investigated. The mobility is around several 105 cm2/Vs at 1.2K.[1],[2]

Generating nanostructure in the p-type Si/SiGe heterostructure

The mobility of samples we use is around several 103 cm2/Vs at 10K

Page 4: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Samples

N383

Page 5: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Samples

N384

Page 6: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Samples

N492

Page 7: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Samples

N384

δ-doping(B): 1.6×1012cm-2

5kΩ-Si substrate

500 Å Si

200 Å_strained Sispacer_layer

300Å Si0.8Ge0.2

3000Å Si buffer

Page 8: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Process

Lithography1.Ohmic Contact

Coating Al 1000 AAnnealing 470 C/15min

2.MesaEtching Solution: HF:HNO3:CH3COOH=1:6:2[4]

3.Metal GateCoating Ti/Al: 100A/500A

Page 9: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Process

E-beam LithographyPMMA

E-beam Writing by NPGS

Development Etching:

KOH:H2O=1:4[4]

Coating: Ti/AuLift Off

Page 10: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Results & Discussion

Quantum Point Contact Device

Page 11: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Results & Discussion

Unfortunately, we did not get what we expect.

Below 77K, the device does not work. Problems: 1.Stress?

2.Damage of structure?3.Etching process?

Page 12: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Results & Discussion

Damage of device

Page 13: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

Conclusion & Future work

More Investigations of process:1.Etching SolutionICPRIE?

2.Where does the stress come from?strained-Si? -doping Boron?3.Traditional hall pattern does not work?

Device measurement Saw as a detector

Page 14: Electric properties of holes in narrow channels of Si/SiGe heterostructures L. C. Li a ( 李良箴 ), W. H. Hsieh b ( 謝文興 ), H.H. Cheng c ( 鄭鴻祥 ), C. H. Kuan

References

Ballistic transport in an etch-defined Si/SiGe quantum point contact, U. Wiesera, U. Kunze, K. Ismail, and J. O. Chu, Applied Physics Letter Vol.81, No.9 26 Aug. 2002

Fabrication of Si/SiGe quantum point contacts by electron-beam lithography and shallow wet-chemical etching, U. Wiesera, U. Kunze, K. Ismail, and J. O. Chu, Physica E 13 (2002) 1047 – 1050

Low-dimensional inverted Si/SiGe modulation-doped electron gases using selective ex-suti ion implantation, D.J. Paul, A. Ahmed, A.C. Churchill, D.J. Robbins, and W.Y. Leong, reference paper of Cavendish Laboratory, University of Cambridge, Cambridge, UK

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