Cathodoluminescence Studies of Bound Excitons and Near Band Gap Emission Lines in Boron- and Phosphorus-Doped CVD-Diamon
- PDF / 438,018 Bytes
- 6 Pages / 414.72 x 648 pts Page_size
- 107 Downloads / 219 Views
		    Mat. Res. Soc. Symp. Proc. Vol. 423 * 1996 Materials Research Society
 
 RESULTS AND DISCUSSION a) Boron-doped CVD-diamond films Fig. 1 shows a selection of CL spectra demonstrating the general trends upon increasing boron concentrations. The topmost spectrum exhibits dominantly free exciton radiation as TO-, TA-, and TO- plus Or-phonon assisted recombination lines (FEW: 5.27 eV, FETA: 5.32 eV, and FET°+r : 5.105 eV). Weakly, observed is radiation from excitons localized at isolated boron atoms ("bound exciton", BE: 5.215 eV). These line positions are in accord with the basic luminescence data in Ref. [2]. This sample was not intentionally boron doped but contaminated in the growth apparatus. All other samples in Fig. 1 were intentionally boron-doped during hot filament CVD-growth. The boron concentrations were determined by SIMS and increase from top to bottom. They are listed in Table I for all samples investigated. In Fig. 1, for sample TD 219A with [B] = 40 ppm, the FE lines have almost disappeared; the BET° line has largely increased and broadened yet maintaining its energy position. As a new feature, the BET°+°r transition is visible, and towards lower energies, there is a rise in intensity up to the boron-related emission band peaking at 4.5 eV [3]. For the next concentration, [B] = 825 ppm
 
 (sample B 113), the bound exciton lines have shifted and broadened even more. Finally, for [B] = 3500
 
 Wavelength (nm)
 
 Z60
 
 Z•o
 
 z30
 
 240
 
 ppm (sample B1110), this trend is continued: The BET° and BET°+°r lines merge due to their largely enhanced widths, however, the two components remain distinguishable with energy spacing of around 165 meV = hfl (Or). At the same time, the lines are shifted down in energy significantly. A lineshape analysis demonstrates that the BE spectra
 
 V
 
 4 T
 
 8KFIM
 
 a)
 
 BE,
 
 3
 
 \
 
 B,
 
 o.,ý 'Ir //
 
 ,further ,
 
 b)
 
 of all samples can be generated progressively from
 
 T•219A
 
 ""the low-doping c)
 
 71
 
 case by simple Gaussian-broadening
 
 Table 1: of the boron-doped diamond films indicating the List total boron and phosphorus concentrations as determined by SIMS measurements. The substrates were in all cases Si:B. Sensitivity limit of SIMS < 0.01 ppm. Sample
 
 B-concentration (ppm) 20 Nr 3 S.2 40 TD219A 81 Nr 5 S.2 140 WD 13 225 Nr 7 S.2 340 W)D 12 500 Nr 8 S.2 630 Nr 9 S.2 715 Nr 10 S.2 825 B113 3500 Bll0
 
 Photon Energy (eV)
 
 Fig. 1:
 
 Near-band edge boron-doped diamond CLspectra at 80 K. (a) Spectrum from a nominally undoped MW-CVD film grown on Si:B exhibiting TO-phonon and (TO+Or)phonon assisted free exciton radiation (FE', FETO+Or) along with boron bound exciton radiation (BET°). (b - d) Spectra from hot filament grown films with intentional boron doping of 40 ppm, 825 ppm, and 3500 ppm, respectively (see Table 1).
 
 694
 
 P-concentration (ppm) -
 
 < 0.01 -		
Data Loading...
 
	 
	 
	 
	 
	 
	 
	 
	 
	 
	 
	