Field emission properties of nanocrystalline chemically vapor deposited-diamond films

Citation
O. Groning et al., Field emission properties of nanocrystalline chemically vapor deposited-diamond films, J VAC SCI B, 17(5), 1999, pp. 1970-1986
Citations number
51
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Material Science & Engineering
Journal title
JOURNAL OF VACUUM SCIENCE & TECHNOLOGY B
ISSN journal
10711023 → ACNP
Volume
17
Issue
5
Year of publication
1999
Pages
1970 - 1986
Database
ISI
SICI code
1071-1023(199909/10)17:5<1970:FEPONC>2.0.ZU;2-Y
Abstract
We have deposited nanocrystalline diamond films on p-type Si(100) substrate s using plasma enhanced chemical vapor deposition (CVD). The diamond films were deposited at substrate temperatures between 950 and 980 degrees C usin g a high methane concentration of 5% in H-2. The films obtained showed good field emission properties with threshold fields of around 5 V mu m(-1) (fo r 1 nA emission current). X-ray photoelectron spectroscopy and ultraviolet photoelectron spectroscopy showed that the nanocrystalline films still exhi bit the basic electronic features of diamond with a band gap of 5.5 eV and a negative electron affinity when the Surface is hydrogen plasma treated. T he Fermi level position in these films is found to be 1+/-0.2 eV above the valence band maximum. The energy resolved field emission measurements show the typical asymmetric peak shape of Fowler-Nordheim (FN) tunneling through a surface potential barrier. The electrons emitted originate from a contin uum of electronic states at the Fermi energy of the emitter. From a combine d measurement of the field emitted electron energy distribution and the fie ld emission I-V characteristic of an emitter we could independently determi ne the work function and the local electric field present at the emission s ite. In the case of nanocrystalline CVD diamond emitters we determined work function values around 5.7 eV and local fields in the range of 2000-3000 V mu m(-1) (for emission currents of 10-1000 pA). The corresponding field en hancement factors can range from 250 to 1700. Simultaneous field and photoe lectron emission spectroscopy showed no indication of field penetration. De viations from the FN law in the high current regime of the I-V plots may be related to an internal resistance of the emitter. (C) 1999 American Vacuum Society. [S0734-211X(99)03205-9].