Electrical conduction in undoped ultrananocrystalline diamond thin films and its dependence on chemical composition and crystalline structure

The electrical conduction behavior of undoped ultrananocrystalline diamond (UNCD) and its dependence on deposition temperature and chemical structure are presented. UNCD films were grown using a microwave plasma-enhanced chemical vapor deposition technique at deposition temperatures of 400 °C and 800 °C. The chemical structure of the UNCD films is characterized with several tools including: Elastic recoil detection analysis, Fourier transform infrared spectroscopy, electron energy loss spectroscopy, Raman spectroscopy, and environmental scanning electron microscope. The results show a higher content of sp2-bonded carbon for the 800 °C deposition samples (∼65%) in comparison with the 400 °C samples (∼38%). In both kinds of films, the hydrocarbon bonds have the saturated sp3 structures, while there is lower hydrogen content in the 800 °C samples (∼8%) than in the 400 °C samples (∼10%). For conduction properties, experiments are conducted using a probe station and conductive-atomic force microscopy. Experime...

[1]  Wei-Kan Chu,et al.  Chapter 3 – Concepts of Backscattering Spectrometry , 1978 .

[2]  R. Egerton,et al.  Preparation and characterization of carbon nitride thin films , 1996 .

[3]  S. Prawer,et al.  Electrical conduction in polycrystalline diamond and the effects of UV irradiation , 1997 .

[4]  D. K. Reinhard,et al.  Electric field-dependent conductivity of polycrystalline diamond thin films , 1991 .

[5]  L. Colombo,et al.  On the electrical activity of sp2-bonded grain boundaries in nanocrystalline diamond , 1999 .

[6]  J. Robertson Diamond-like amorphous carbon , 2002 .

[7]  J. Blank,et al.  Astrobiology: Future Perspectives , 2005 .

[8]  Olof Engström,et al.  Steady-state and transient current transport in undoped polycrystalline diamond films , 1997 .

[9]  Jacqueline A. Johnson,et al.  Interpretation of the Raman spectra of ultrananocrystalline diamond , 2005 .

[10]  Michael Nastasi,et al.  Handbook of modern ion beam materials analysis , 1995 .

[11]  Synthetic theory of Poole and Poole-Frenkel (PF) effects , 1991 .

[12]  John A. Carlisle,et al.  Low temperature growth of ultrananocrystalline diamond , 2004 .

[13]  D. Gruen,et al.  Microstructure of ultrananocrystalline diamond films grown by microwave Ar–CH4 plasma chemical vapor deposition with or without added H2 , 2001 .

[14]  Stefan Höhn,et al.  Field emission conduction mechanisms in chemical vapor deposited diamond and diamondlike carbon films , 1998 .

[15]  David N. Jamieson,et al.  Poole–Frenkel conduction in polycrystalline diamond , 1996 .

[16]  A. Ishitani,et al.  RAMAN SCATTERING FROM NANOMETER-SIZED DIAMOND , 1995 .

[17]  Takashi Sugino,et al.  Electrical conduction in undoped diamond films prepared by chemical vapor deposition , 1991 .

[18]  Derrick C. Mancini,et al.  Ultrananocrystalline diamond thin films for MEMS and moving mechanical assembly devices , 2001 .

[19]  Glass,et al.  Analysis of the composite structures in diamond thin films by Raman spectroscopy. , 1990, Physical review. B, Condensed matter.

[20]  Robert M. Hill,et al.  Poole-Frenkel conduction in amorphous solids , 1971 .

[21]  F. Cataldo From Elemental Carbon to Complex Macromolecular Networks in Space , 2004 .