Modeling of boron and phosphorus implantation into (100) Germanium

Boron and phosphorus implants into germanium and silicon with energies from 20 to 320 keV and ion doses from 5/spl times/10/sup 13/ to 5/spl times/10/sup 16/ cm/sup -2/ were characterized using secondary ion mass spectrometry. The first four moments of all implants were calculated from the experimental data. Both the phosphorus and boron implants were found to be shallower in the germanium than in the silicon for the same implant parameters and high hole concentrations, as high as 2/spl times/10/sup 20/ cm/sup -3/, were detected by spreading resistance profiling immediately after boron implants without subsequent annealing. Channeling experiments using nuclear reaction analysis also indicated high substitutional fractions (/spl sim/19%) even in the highest dose case immediately after implant. A greater straggle (second moment) is, however, observed in the boron implants in the germanium than in the silicon despite having a shorter projected range in the germanium. Implant profiles predicted by Monte Carlo simulations and Lindhard-Scharff-Schiott theory were calculated to help clarify the implant behavior. Finally, the experimentally obtained moments were used to calculate Pearson distribution fits to the boron and phosphorus implants for rapid simulation of nonamorphizing doses over the entire energy range examined.

[1]  J. Lindhard,et al.  ENERGY DISSIPATION BY IONS IN THE kev REGION , 1961 .

[2]  Alan G. R. Evans,et al.  Diffusion of ion-implanted boron in germanium , 2001 .

[3]  R. Tauber,et al.  Formation of amorphous layers by ion implantation , 1985 .

[4]  C. O. Chui,et al.  Activation and diffusion studies of ion-implanted p and n dopants in germanium , 2003 .

[5]  Aaas News,et al.  Book Reviews , 1893, Buffalo Medical and Surgical Journal.

[6]  Phosphorus and Boron Implantation into (100) Germanium , 2004 .

[7]  J. Ziegler THE STOPPING AND RANGE OF IONS IN SOLIDS , 1988 .

[8]  Jacqueline Grennon , 2nd Ed. , 2002, The Journal of nervous and mental disease.

[9]  S. Csutak,et al.  High-speed interdigitated Ge PIN photodetectors , 2002, IEEE Photonics Technology Letters.

[10]  Robert Oven,et al.  Representation of ion implantation profiles by Pearson frequency distribution curves , 1990 .

[11]  Gianlorenzo Masini,et al.  Si based optoelectronics for communications , 2002 .

[12]  K. B. Winterbon Pearson distributions for ion ranges , 1983 .

[13]  W. Haensch,et al.  High mobility p-channel germanium MOSFETs with a thin Ge oxynitride gate dielectric , 2002, Digest. International Electron Devices Meeting,.

[14]  Eugene E. Haller,et al.  ION IMPLANTATION OF BORON IN GERMANIUM , 1987 .

[15]  C. Kenway-Jackson,et al.  Secondary ion mass spectrometry , 1984 .

[16]  M. V. Rao,et al.  Phosphorus and boron implantation in 6H–SiC , 1997 .

[17]  Zhiping Zhou,et al.  Simulation of Georgia Tech's CMOS baseline using TSUPREM-4 and MEDICI , 2001, Proceedings of the Fourteenth Biennial University/Government/Industry Microelectronics Symposium (Cat. No.01CH37197).

[18]  A. Benninghoven,et al.  Secondary ion mass spectrometry : SIMS V : proceedings of the fifth international conference, Washington, DC, September 30-October 4, 1985 , 1986 .