Towards improving the quality of semiconducting diamond layers doped with large atoms

被引:18
作者
Prins, JF [1 ]
机构
[1] Univ Witwatersrand, Schonland Res Ctr Nucl Sci, Johannesburg, South Africa
关键词
diamond; n-type doping; ion implantation;
D O I
10.1016/S0925-9635(99)00035-7
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Previous studies on phosphorus- and aluminium-dopant activation in ion-implanted diamonds indicated that vacancies can either act to compensate the dopants or, when annealed at a temperature where they diffuse (600 degrees C), they can interact to passivate these same dopant atoms. In order to improve the quality of diamond layers doped with large atoms, ways must be found to counteract such passivation. In this study, multiple cold implantation-rapid annealing (CIRA) steps were used to study the activation of phosphorus atoms which had been implanted into diamonds. To prevent large-scale passivation by the vacancies, the annealing temperature was chosen to be only 500 degrees C. The results prove that enough phosphorus-dopant atoms can be activated to exceed the compensating vacancy density, and that the density of the activated donor atoms can be steadily increased by merely increasing the number of CIRA steps. In the case where the phosphorus-donor density N(PD) just exceeded the density of the compensating vacancy accepters N(V), conduction occurred with an activation energy of approximate to 0.62 eV. With increasing R=N(PD)/N(V), the measured activation energies decreased. A model is proposed that relates this decrease to the negative electron affinity (NEA) of diamond. For the number of CIRA steps done to date, the resulting resistances of the layers are, unfortunately, still too high to allow any Hall-effect measurements. These high resistances can also be a result of the large density of unannealed vacancies, as well as the fact that the implanted layers only have an average depth of 80 nm, which is less than the surface roughness of the diamonds. Thermal EMF (Electro-Motive Force) measurements, whilst maintaining a stationary temperature gradient over the length of the diamond, confirmed n-type conduction. (C) 1999 Elsevier Science S.A. All rights reserved.
引用
收藏
页码:1635 / 1641
页数:7
相关论文
共 49 条
[1]  
AKASHI M, 1993, SCIENCE, V259, P1592
[2]   SEMICONDUCTING DIAMONDS MADE IN THE USSR [J].
ALEXENKO, AE ;
SPITSYN, BV .
DIAMOND AND RELATED MATERIALS, 1992, 1 (5-6) :705-709
[3]  
ALLEN MG, 1993, APPL PHYS LETT, V63, P2026
[4]  
BEKKU K, 1994, ADV NEW DIAMOND SCI, P701
[5]   CHANNELING ANALYSIS OF HIGH-TEMPERATURE ION-IMPLANTED DIAMOND [J].
BRAUNSTEIN, G ;
KALISH, R .
NUCLEAR INSTRUMENTS & METHODS, 1981, 182 (APR) :691-697
[6]   DAMAGE AND LATTICE LOCATION STUDIES IN HIGH-TEMPERATURE ION-IMPLANTED DIAMOND [J].
BRAUNSTEIN, G ;
KALISH, R .
APPLIED PHYSICS LETTERS, 1981, 38 (06) :416-418
[7]   GROWTH OF PHOSPHORUS AND NITROGEN CO-DOPED DIAMOND FILMS [J].
CAO, GZ ;
GILING, LJ ;
ALKEMADE, PFA .
DIAMOND AND RELATED MATERIALS, 1995, 4 (5-6) :775-779
[8]  
CARLSON RO, 1969, T METALL SOC AIME, V245, P483
[9]   NATURE OF ACCEPTOR CENTRE IN SEMICONDUCTING DIAMOND [J].
COLLINS, AT ;
WILLIAMS, AW .
JOURNAL OF PHYSICS PART C SOLID STATE PHYSICS, 1971, 4 (13) :1789-&
[10]  
Davidson L. A., 1971, Radiation Effects, V7, P35, DOI 10.1080/00337577108232562