the sixth international workshop on junction technology (iwjt), may 15-16, 2006, shanghai, china

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The Sixth International Workshop on Junction Technology (IWJT), May 15-16, 2006, Shanghai, China. RBS characterization on the PtSi-based ohmic cont acts with n-InP Wen-Chang Huang Conclusion Inter-diffusion of elements was occurred in the contac t schemes, Si/Pt/InP and Au/Si/Pt/InP after thermal an nealing which were observed in the RBS analysis. The Au/Si/Pt/InP contact showed better ohmicity than that of Si/Pt/InP contact. This is due to the alloyed reac tion and forming In-compounds in the Au/Si/Pt/InP cont act. The wetting effect of Au on the contact was also shown. 半半 半半半半半 Abstract PtSi based ohmic contact on InP substrate was dis cussed in the research. The inter-diffusion between the elements of the contacts after various annealing temperature were analyzed by Rutherford backscattering analysis (RBS). A bett er specific contact resistance was obtained at th e Au/Si/Pt/InP contact scheme. The ohmicity was due to the silicon doping effect to InP substrate. The existence of Au on the contact could improv e the doping effect. Introduction Au-Ge[1,2] based electrode to n-InP shows excellent ohmic behavi or, however, which is not always stable for the heat excursion o f the contacts because the reaction products at the contact inte rface change due to diffusion upon annealing. The diffusion of the dopant element deep into the substrate is also disadvantage of the electrode for the device applications. Solid phase reacti on was a good process to avoid the disadvantage of Au-Ge based c ontact schemes. The contact schemes such as Ge/Pd[3], Ge/Pt[4], Ni/Si [5], AlxMo1-x[6] and Pd/In/Pd [7] were all based on solid phase reaction. They gave a shallow and uniform contact interface after ohmicity was reached. Based on the ideal, the n ew contact scheme Si/Pt/n-InP was designed at the research. The element of Si was chosen to be a dopant element to InP substrate. The element of Pt was used to improve the doping effect. Anot her contact scheme, Au/Si/Pt/n-InP was designed to compare the r esults of Si/Pt/n-InP. Experimental procedures Contacts were made on n-type InP wafers which had an epitaxial layer grown on the semi-insulating substrate by metal organic chemical vapor deposition (MOCVD). The thickness of the epitaxial layer was approximately 0.2 m. The doping concentrat ion of electron is 210 18 cm -3 which doped by silicon. Contact metals of layered structures of Si(1300Å) /Pt(750Å) /n-InP and Au(2000Å)/Si(1300Å) /Pt(750Å) /n-InP were deposited layer by layer directly on the InP epi-wafers in an electron-beam evaporation system. RTA was applied to anneal the samples. Results and Discussion [1] J. S. Huang, C. B. Vartuli, T. Nguyen, N. Bar-Chaim, J. Shearer, C. Fisher and S. Anderson, Journal of Material Research, 17 (2002) 2929. [2] T. Arai, K. Sawada, N. Hara, Journal of Vacuum Science and Technology - Section B, 21 (2003) 795. [3] P. Jian, D. G. Ivey, R. Bruce and G. Knight, Journal of Electronic Mater. 23 (1994) 953. [4] W. C. Huang, T. F. Lei, and C. L. Lee, J. Appl. Phys. 78, (1995) 6108. [5] C. C. Han, X. Z. Wang, L. C. Wang, E. D. Marshall, S. S. Lau, S. A. Schwarz, C. J. Palmstrom, J. P. Harbison, L. T. Florez, R. M. Potemski, M. A. Tischler, and T. F. Kuech, J. Appl. Phys. 68 (1990) 5714. [6] R. Atsuchi, M. B. Takeyama, A. Noya, T. Hashizume, H. Hasegawa, 13th IPRM, May (2001) 14. [7] L. C. Wang, X. Z. Wang, S. S. Lau, T. Sands, W. K. Chan, and T. F. Kuech, Appl. Phys. Lett. 56 (1990) 2129. Acknowledgments The authors would like to thank the National Science Council of the Republic of China, for financially supporting the research under Contract No. NSC-94-2216-E-168-004. References 10 -5 0.0001 0.001 300 350 400 450 500 550 600 650 Si/Pt/InP Au/Si/Pt/InP Annealing Tem perature (C ) Specific contact resistance-- A low specific contact resistance of 3.3210 -5 - cm 2 was obtained after RTA at 550C for 30 sec. XRD– The XRD results of the Si/Pt/n-InP contact after RTA at 550C for 30 sec and The XRD results of the Au/Si/Pt/n-InP contact after RTA at 550C for 30 sec 0 20 40 60 80 100 0 0.5 1 1.5 2 U nannealed Au/Si/Pt/InP Energy (M eV) Si In Pt Au 0 20 40 60 80 100 0 0.5 1 1.5 2 Au/Si/Pt/InP R TA 550C 30sec Energy (M eV) Au Pt In 0 20 40 60 80 100 0 0.5 1 1.5 2 Si/Pt/InP R TA 550C 30sec Energy (M eV) Si In Pt RBS– As deposited Au/Si/Ni/InP contact RBS-- 550C annealed Au/Si/Ni/InP contact Au in-diffusion, platinum-silicide, In out-diffusion RBS-- 550C annealed Si/Ni/InP contact Si/SiPt/SiPt1.5InP/Pt1.5InP /n-InP AFM--The AFM pictures of the Au/Si/Pt/n-InP contact, (a) without annealing, (b) with 450C annealing and (c) with 550C annealing AFM--The AFM pictures of the Si/Pt/n-InP contact, (a) without annealing, (b) with 450C annealing and (c) with 550C annealing

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半導體元件研究室. The Sixth International Workshop on Junction Technology (IWJT), May 15-16, 2006, Shanghai, China. RBS characterization on the PtSi-based ohmic contacts with n-InP. W en- C hang Huang. Abstract. - PowerPoint PPT Presentation

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Page 1: The Sixth International Workshop on Junction Technology (IWJT), May 15-16, 2006, Shanghai, China

The Sixth International Workshop on Junction Technology (IWJT), May 15-16, 2006, Shanghai, China.

RBS characterization on the PtSi-based ohmic contacts with n-InP

Wen-Chang Huang

Conclusion

Inter-diffusion of elements was occurred in the contact schemes, Si/Pt/InP and Au/Si/Pt/InP after thermal annealing which were observed in the RBS analysis. The Au/Si/Pt/InP contact showed better ohmicity than that of Si/Pt/InP contact. This is due to the alloyed reaction and forming In-compounds in the Au/Si/Pt/InP contact. The wetting effect of Au on the contact was also shown.

半導體元件研究室

Abstract

PtSi based ohmic contact on InP substrate was discussed in the research. The inter-diffusion between the elements of the contacts after various annealing temperature were analyzed by Rutherford backscattering analysis (RBS). A better specific contact resistance was obtained at the Au/Si/Pt/InP contact scheme. The ohmicity was due to the silicon doping effect to InP substrate. The existence of Au on the contact could improve the doping effect.

IntroductionAu-Ge[1,2] based electrode to n-InP shows excellent ohmic behavior, however, which is not always stable for the heat excursion of the contacts because the reaction products at the contact interface change due to diffusion upon annealing. The diffusion of the dopant element deep into the substrate is also disadvantage of the electrode for the device applications. Solid phase reaction was a good process to avoid the disadvantage of Au-Ge based contact schemes. The contact schemes such as Ge/Pd[3], Ge/Pt[4], Ni/Si [5], AlxMo1-x[6] and Pd/In/Pd [7] were all based on solid phase reaction. They gave a shallow and uniform contact interface after ohmicity was reached. Based on the ideal, the new contact scheme Si/Pt/n-InP was designed at the research. The element of Si was chosen to be a dopant element to InP substrate. The element of Pt was used to improve the doping effect. Another contact scheme, Au/Si/Pt/n-InP was designed to compare the results of Si/Pt/n-InP.

Experimental proceduresContacts were made on n-type InP wafers which had an epitaxial layer grown on the semi-insulating substrate by metal organic chemical vapor deposition (MOCVD). The thickness of the epitaxial layer was approximately 0.2 m. The doping concentration of electron is 21018 cm-3 which doped by silicon. Contact metals of layered structures of Si(1300Å) /Pt(750Å) /n-InP and Au(2000Å)/Si(1300Å) /Pt(750Å) /n-InP were deposited layer by layer directly on the InP epi-wafers in an electron-beam evaporation system. RTA was applied to anneal the samples.

Results and Discussion

[1] J. S. Huang, C. B. Vartuli, T. Nguyen, N. Bar-Chaim, J. Shearer, C. Fisher and S. Anderson, Journal of Material Research, 17 (2002) 2929.[2] T. Arai, K. Sawada, N. Hara, Journal of Vacuum Science and Technology - Section B, 21 (2003) 795.[3] P. Jian, D. G. Ivey, R. Bruce and G. Knight, Journal of Electronic Mater. 23 (1994) 953.[4] W. C. Huang, T. F. Lei, and C. L. Lee, J. Appl. Phys. 78, (1995) 6108.[5] C. C. Han, X. Z. Wang, L. C. Wang, E. D. Marshall, S. S. Lau, S. A. Schwarz, C. J. Palmstrom, J. P. Harbison, L. T. Florez, R. M. Potemski, M. A. Tischler, and T. F. Kuech, J. Appl. Phys. 68 (1990) 5714.[6] R. Atsuchi, M. B. Takeyama, A. Noya, T. Hashizume, H. Hasegawa, 13th IPRM, May (2001) 14.[7] L. C. Wang, X. Z. Wang, S. S. Lau, T. Sands, W. K. Chan, and T. F. Kuech, Appl. Phys. Lett. 56 (1990) 2129.

AcknowledgmentsThe authors would like to thank the National Science Council of the Republic of China, for financially supporting the research under Contract No. NSC-94-2216-E-168-004.

References

10-5

0.0001

0.001

300 350 400 450 500 550 600 650

Si/Pt/InPAu/Si/Pt/InP

Annealing Temperature (C)

Specific contact resistance-- A low specific contact resistance of 3.3210-5 -cm2 was obtained after RTA at 550C for 30 sec.

XRD– The XRD results of the Si/Pt/n-InP contact after RTA at 550C for 30 sec and The XRD results of the Au/Si/Pt/n-InP contact after RTA at 550C for 30 sec

0

20

40

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80

100

0 0.5 1 1.5 2

Unannealed Au/Si/Pt/InP

Energy (MeV)

Si In

Pt Au

0

20

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0 0.5 1 1.5 2

Au/Si/Pt/InP RTA 550C 30sec

Energy (MeV)

AuPtIn

0

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100

0 0.5 1 1.5 2

Si/Pt/InP RTA 550C 30sec

Energy (MeV)

SiIn Pt

RBS– As deposited Au/Si/Ni/InP contactRBS-- 550C annealed Au/Si/Ni/InP contact

Au in-diffusion, platinum-silicide, In out-diffusionRBS-- 550C annealed Si/Ni/InP contact

Si/SiPt/SiPt1.5InP/Pt1.5InP /n-InP

AFM--The AFM pictures of the Au/Si/Pt/n-InP contact, (a) without annealing, (b) with 450C annealing and (c) with 550C annealingAFM--The AFM pictures of the Si/Pt/n-InP contact, (a) without annealing, (b) with 450C annealing and (c) with 550C annealing