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Journal of Crystal Growth
Volume 192, Issues 3-4 , 1 September 1998, Pages 386-394

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doi:10.1016/S0022-0248(98)00365-0    How to cite or link using doi (opens new window) Cite or link using doi  
Copyright © 1998 Elsevier Science B.V. All rights reserved

Heat treatments of ZnSe starting materials for physical vapor transport

Ching-Hua Sua, *, W. Palosz1, a, S. Feth2, a and S. L. Lehoczkya

a Space Sciences Laboratory, NASA Marshall Space Flight Center, Huntsville, AL 35812, USA

Received 10 November 1997; accepted 9 February 1998. Available online 21 December 1998.


Abstract

The effect of different heat treatments on stoichiometry and residual gas pressure in ZnSe physical vapor transport system was investigated. The dependence of the amount and composition of the residual gas on various heat treatment procedures is reported. Heat treatment of ZnSe starting materials by baking under the condition of dynamic vacuum to adjust its stoichiometry was performed and the effectiveness of the treatment was confirmed by the measurements of the partial pressure of Se2, PSe2, in equilibrium with the heat treated samples. Optimum heat treatment procedures on the ZnSe starting material for the physical vapor transport process are discussed and verified experimentally.


Article Outline

1. Introduction
2. Experimental procedure
2.1. Residual gas
2.1.1. Sample preparation and treatments
2.1.2. Residual gas measurements
2.2. Partial pressure
2.2.1. Sample preparation and heat treatment
2.2.2. Partial pressure measurements
2.3. Crystal growth experiments
3. Results and discussion
3.1. Residual gas pressure and compositions
3.2. Partial pressure measurements
3.3. Crystal growth
4. Conclusions
Acknowledgements
References



Enlarge Image
(5K)
Fig. 1. Theoretically calculated mass flux of ZnSe as a function of the residual gas pressure for different partial pressure ratios at the source, small alpha, Greek(L), with the source temperature at 1080°C, capital Delta, GreekT =20°C and transport length L=10 cm. The composition of the inert gas used in the calculation was 35% CO2, 50% CO and 15% H2. The solid dots on the left axis are the respective mass flux values assuming zero inert gas pressure.

Enlarge Image
(6K)
Fig. 2. The measured partial pressures of Se2, PSe2, for the optical cells ZnSe(O)-1, -2, -3 and -4, in equilibrium with ZnSe solid at different temperatures. The pressure ratio, small alpha, Greek, at the highest experimental temperature of each cell was labelled. The calculated Pse2 for the congruent sublimation condition is also given.

Enlarge Image
(112K)
Fig. 3. The ampoules after the crystal growth process. (a) Chunk source material, baked at 280°C under dynamic vacuum for 13 min. (b) Powdered source, annealed under H2 atmosphere at 1015°C for 30 min then baked at 1045°C for 20 min.



Table 1. Source preprocess and sample treatment procedures for residual gas pressure measurements. Vendor I – Cleveland crystals, 59 purity; vendor II – Eagle–Picher high purity grade View Table (<1K)

Table 2. Residual gas pressures and compositions in the processed ZnSe ampoules View Table (<1K)

Table 3. Sample heat treatment procedures for the partial pressure measurements. Source sample: ground Eagle–Picher high-purity grade ZnSe View Table (11K)

References

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*Corresponding author. Fax: +1 205 544 8762.

1Universities Space Research Association.

2Raytheon STX Corp.



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Journal of Crystal Growth
Volume 192, Issues 3-4 , 1 September 1998, Pages 386-394


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