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The Improved Procedure of Ga-doped PbTe Films One Stage Synthesis by Modified HWE Technique |
Alexander M. Samoylov , Sergey V. Belenko , Alexey I. Dontsov , Sergey V. Kannykin , Valentin M. Ievlev |
Voronezh State University (VGU), Universitetskaya Sq., 1, Voronezh 394006, Russian Federation |
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Table 1. The comparison of the estimated data z*Ga and the real experimental results zGa concerning the concentration of Ga atoms in Pb1–zGazTe films fabricated by the improved one stage synthesis. The thin films and single crystals of PbTe doped with Ga are the perspective materials for fabrication of the optoelectronic devices employed in infrared (IR) radiation middle wave range [1]. The IR sensitivity of these materials is similar to that of Cd1–xHgxTe but processing procedures are much less demanding. Under influence of the presence of III A group metals the energy spectrum of PbTe and its solid solutions can change significantly and depends not only the concentrations of the impurity atoms but from the method of investigated samples synthesis also [2]. The main purpose of this work is to emphasize the improvements of Ga-doped PbTe films one stage synthesis with predicted concentration of the impurity atoms by modified HWE technique. Earlier, Ga-doped PbTe thin films on Si-substrates had been prepared by the two stage procedure [3]. This doping procedure was based on the two-zone annealing in atmosphere of the saturated vapor, which corresponds th the three-phase equilibrium L1 + GaTe(S) + V in Ga - Te binary system, of the undoped PbTe/Si heterostructures previously formed by modified HWE technique. The EPMA and XPS experimental results clear demonstrated that after this treatment Ga impurity atoms have distributed on the surface layers quiet irregular. Later, another method of PbTe<Ga> heterostructures preparation was created. This procedure offers direct one stage synthesis, in which the doping and the layer condensation processes proceed simultaneously [4]. Despite the greater difference in fugitives between pure Pb and Ga the results of high-temperature mass-spectroscopy study have shown that saturated vapor phase over Ga1–xPb x is enriched with IIIA group metal at temperature interval T = 980 - 1300 K [5]. Fig. 1. The dependence of Ga atoms concentration in saturated vapor over Ga1–xPbx melts xVGa upon the values of Ga partial pressure pGa and the integral pressure Pint of all components in Ga - Pb binary system. At the first step of this work the mass-spectroscopic experimental data [5] allow us to determine the concentration of Ga atoms in the saturated vapor over Ga1–xPb x melts xVGa dependence upon the values of Ga partial pressure pGa and the integral pressure Pint of all components in Ga - Pb binary system (Fig. 1). For xVGa - pGa - and xVGa - Pint - projections of the convolute shown in Fig. 1 it has been established that concentration of Ga atoms in equilibrium vapor phase may be expressed by the equations: xVGa(pGa) = A1 + B1×exp(C1×pGa) (1a) xVGa(Pint) = A2 + B2×exp(–C2×Pint) (1b) At the second step by the general solution of the equations (1a) and (1b) the regimes (the values of pGa, pPb, Pint, temperature T, and compositions of initial Ga1–xPbx melts) of Ga1–yPby binary layers have been defined. The synthesis of Ga1–yPby samples is necessary to evaluate the degree of the discrepancy from the thermodynamic equilibrium in the HWE reaction chamber. The results of EPMA have shown that in prepared Ga1–yPby binary layers Ga atoms concentration is higher than xVGa. In order to take into account the major part of physicochemical processes resulting in the discrepancy from the thermodynamic equilibrium the analitical equation of factor K1 = yGa/xVGa as the function of pGa, Pint, and the concentration of Ga atoms in initial Ga1–xPbx melts has been defined. At the third step we have realized the results of the detail analysis of the quantitative composition of Ga1–yPby binary layers in the improving of the one stage synthesis of ternary Pb1– zGazTe films. It has been found that the presence of tellurium vapor has increased in the degree of the deviation from thermodynamic equilibrium in HWE reaction chamber. The values of factor K2 = zGa/xVGa are higher than the values of K1 in the most cases. On the basis of the general solution of the equations (2a) and (2b): z*Ga(pGa) = A1 + B1×pGa + C1×p2Ga (2a) z*Ga(Pint) = A2 + B2×Pint + C2×P2int (2b) the improved conditions of ternary Pb1–zGazTe films one stage synthesis have been designed. The comparison of the estimated z*Ga and the real experimental results zGa concerning the concentration of Ga atoms in fabricated Pb1–zGazTe films is presented in Table 1. It has been established that compositions of Pb1–zGazTe samples synthesized by improved one stage method are characterized by the complete concurrence to expected z*Ga values practically. References:
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Presentation: Poster at 17th International Conference on Crystal Growth and Epitaxy - ICCGE-17, General Session 10, by Alexander M. SamoylovSee On-line Journal of 17th International Conference on Crystal Growth and Epitaxy - ICCGE-17 Submitted: 2013-04-06 06:49 Revised: 2013-07-19 23:52 |