Investigations of polycrystalline chemical vapor deposited diamond films by electron‐spin‐resonance (ESR), light‐induced (L)ESR, and the constant photoconductivity method have identified dispersed substitutional nitrogen (P1 center) as the main paramagnetic form of N incorporated in the CVD diamond. The density of N‐related paramagnetic states is strongly affected by illumination and heat treatment. It is found that the P1 center in CVD diamond gives rise to a deep donor state about 1.5 eV below the conduction band.
REFERENCES
1.
Properties and Growth of Diamond, edited by INSPEC 1994 (Short Run, Exeter, 1994).
2.
W. V. Smith, P. P. Sorokin, I. L. Gelles, and G. J. Lasher, Phys. Rev. 115, 1546 (1959). For a review on electron spin resonance in natural and high pressure synthetic diamond see, J. H. N. Loubser and J. A. van Wyk, Rep. Prog. Phys. 41, 1201 (1978).
3.
S. A.
Kajihara
,A.
Antonelli
,B.
Bernholconkin
, andK.
Okumura
, Appl. Phys. Lett.
59
, 3148
(1991
). 4.
5.
M. Roesler, R. Zachai, H.-J. Füsser, X. Jiang, and C.-P. Klages, in Proceedings of the 2nd International Conference on the Application of Diamond Films and Related Materials, edited by M. Yoshikawa, M. Murakawa, Y. Tzeng, and W. A. Yarbrough (MYU, Tokyo, 1993), p. 691.
6.
E. Rohrer, C. F. O. Graeff, R. Jansen, C. E Nebel, M. Stutzmann, H. Güttler, and R. Zachai, Phys. Rev. B 54 (in press).
7.
8.
9.
M.
Hoinkis
,E. R.
Weber
,M. I.
Landstrass
,M. A.
Plano
,S.
Han
, andD. R.
Kania
, Appl. Phys. Lett.
59
, 1870
(1991
). 10.
11.
C. F. O. Graeff, C. E. Nebel, M. Stutzmann, A. Flöter, and R. Zachai, J. Appl. Phys. (in press).
12.
13.
This content is only available via PDF.
© 1996 American Institute of Physics.
1996
American Institute of Physics
You do not currently have access to this content.