journal article·2009-02

Transition from amorphous semiconductor to amorphous insulator in hydrogenated carbon–germanium films investigated by IR spectroscopy

P. Kazimierski, Ł. Jóźwiak

Journal of Non-Crystalline Solids· Volume 355· Issue 4-5
Publisher page

Abstract

Abstract Thin a-GeXC1−X:H plasma polymerized films, depending on deposition conditions, can be produced in two very different structures, namely amorphous semiconductor and amorphous insulator. The transition from amorphous insulator to amorphous semiconductor is related to the formation of germanium nanoclusters due to ions bombarding the surface of the growing material. This paper concentrates on investigations of the transition by means of IR spectroscopy. To this end a quantitative analysis of IR spectra obtained for thin films deposited on silicon substrate has been described and used for estimation of hydrogen atom concentration and bonding in the investigated material. It was found that the probability that a given H atom is bonded to a germanium or to a carbon atom is almost the same. This conclusion is true both for a-S and a-I films. The average concentration of hydrogen in the investigated material was found to be about 2.4–3.4 × 1022 cm−2 which means that there are two times more atoms of the carbon family than hydrogen atoms in the film structure.
Source: openaire · Quality: candidate unverified · Source record ↗

Research context

OpenAlex topics: Diamond and Carbon-based Materials Research · Thin-Film Transistor Technologies · Semiconductor materials and devices

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (26)

Show source-provided references
1. Tyczkowski · J. Phys. D – Appl. Phys. · 1994 · 27 · 17910.1088/0022-3727/27/1/029 ↗
2. J. Tyczkowski, P. Kazimierski, Amorphous covalent dielectrics-new category of materials, in: J. Lewiner, D. Morisseau and C. Alquie (Eds.), Proceedings of 8th International Symposium on Electrets (ISE 8), Paris, France. IEEE Dielectr. & Electr. Insulation Soc. 7–9 September 1994, New York, NY, USA, 1994.
3. Kazimierski · J. Non-Cryst. Solids · 2003 · 325 · 20610.1016/S0022-3093(03)00336-3 ↗
4. Tyczkowski · J. Vac. Sci. Technol. · 1999 · A17 · 47010.1116/1.581608 ↗
5. Kazimierski · J. Non-Cryst. Solids · 1998 · 227-230 · 42210.1016/S0022-3093(98)00177-X ↗
6. Tyczkowski · Thin Solid Films · 1993 · 241 · 29110.1016/0040-6090(94)90444-8 ↗
7. Kazimierski · Chem. Mater. · 2002 · 14 · 469410.1021/cm020428s ↗
8. Vilcarromero · J. Appl. Phys. · 1998 · 84 · 17410.1063/1.368093 ↗
9. Bermejo · J. Non-Cryst. Solids · 1979 · 32 · 42110.1016/0022-3093(79)90086-3 ↗
10. Cardona · Phys. Stat. Sol. (B) · 1983 · 118 · 46310.1002/pssb.2221180202 ↗
11. Sunil · J. Appl. Phys. · 1990 · 69 · 371910.1063/1.348464 ↗
12. Stamate · Appl. Surf. Sci. · 2001 · 172 · 4710.1016/S0169-4332(00)00827-8 ↗
13. Mui · Phys. Rev. B · 1987 · 35 · 808910.1103/PhysRevB.35.8089 ↗
14. Chou · J. Appl. Phys. · 1998 · 83 · 411110.1063/1.367229 ↗
15. J. Tyczkowski, P. Kazimierski, W. Fallman and F. Olcaytug, Three-Electrode Reactor for Plasma Deposition of Thin Multilayer (Dielectric – Semiconductor) Systems, Poland, 1992.
16. Tolstoy · 2003
17. Bounouh · Diam. Relat. Mater. · 1996 · 5 · 45310.1016/0925-9635(95)00502-1 ↗
18. Akkerman · J. Appl. Phys. · 1996 · 80 · 306810.1063/1.363167 ↗
19. Gazicki · Thin Solid Films · 1995 · 256 · 3110.1016/0040-6090(94)06295-1 ↗
20. Bounouh · Diam. Relat. Mater. · 1995 · 4 · 49210.1016/0925-9635(94)05210-7 ↗
21. Jacox · J. Phys. Chem. Ref. Data · 2003 · 32 · 110.1063/1.1497629 ↗
22. McKenzie · J. Phys. D · 1985 · 18 · 193510.1088/0022-3727/18/9/023 ↗
23. Shinar · J. Appl. Phys. · 1987 · 62 · 80810.1063/1.339710 ↗
24. Mulato · J. Appl. Phys. · 1996 · 79 · 445310.1063/1.361756 ↗
25. Fang · J. Non-Cryst. Solids · 1980 · 35&36 · 25510.1016/0022-3093(80)90603-1 ↗
26. Vilcarromero · Thin Solid Films · 1999 · 343&344 · 44510.1016/S0040-6090(98)01663-0 ↗