Luminescence spectra and kinetics of disordered solid solutions

被引:45
作者
Klochikhin, A [1 ]
Reznitsky, A
Permogorov, S
Breitkopf, T
Grün, M
Hetterich, M
Klingshirn, C
Lyssenko, V
Langbein, W
Hvam, JM
机构
[1] Petersburg Nucl Phys Inst, St Petersburg, Russia
[2] AF Ioffe Phys Tech Inst, St Petersburg 194021, Russia
[3] Univ Karlsruhe, Inst Angew Phys, D-76128 Karlsruhe, Germany
[4] Inst Microelect Technol, Chernogolovka 142432, Moscow District, Russia
[5] Tech Univ Denmark, Mikroelect Ctr, DK-2800 Lyngby, Denmark
关键词
D O I
10.1103/PhysRevB.59.12947
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We have studied both theoretically and experimentally the luminescence spectra and kinetics of crystalline, disordered solid solutions after pulsed excitation. First, we present the model calculations of the steady-state luminescence band shape caused by recombination of excitons localized in the wells of random potential induced by disorder. Classification of optically active tail states of the main exciton band into two groups is proposed. The majority of the states responsible for the optical absorption corresponds to the group of extended states belonging to the percolation cluster, whereas only a relatively small group of ''radiative" states forms the steady-state luminescence band. The continuum percolation theory is applied to distinguish the ''radiative'' localized states, which are isolated in space and have no ways for nonradiative transitions along the tail states. It is found that the analysis of the exciton-phonon interaction gives the information about the character of the localization of excitons. We have shown that the model used describes quite well the experimental cw spectra of CdS(1-c) Se-c and ZnSe(1-c)Tec solid solutions. Further, the experimental results are presented for the temporal evolution of the luminescence band. It is shown that the changes of band shape with time come from the interplay of population dynamics of extended states and spatially isolated ''radiative" states. Finally, the measurements of the decay of the spectrally integrated luminescence intensity at long delay times are presented. It is shown that the observed temporal behavior can be described in terms of relaxation of separated pairs followed by subsequent exciton formation and radiative recombination. Electron tunneling processes are supposed to be responsible for the luminescence in the long-time limit at excitation below the exciton mobility edge. At excitation by photons with higher energies the diffusion of electrons can account for the observed behavior of the luminescence. [S0163-1829(99)11419-X].
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页码:12947 / 12972
页数:26
相关论文
共 90 条
[1]  
AAVIKSOO Y, 1987, JETP LETT+, V45, P498
[2]  
ABDUKADYROV AG, 1990, ZH EKSP TEOR FIZ+, V98, P2056
[3]   LUMINESCENCE OF EXCITONS BOUND BY DISORDER-POTENTIAL FLUCTUATIONS IN CDS1-XSEX - SPATIAL DIFFUSION, EXCITATION-LEVEL DEPENDENCE, AND KINETICS [J].
AGEKYAN, V ;
BINDEMANN, R ;
SCHWABE, R ;
STEPANOV, Y ;
STREIT, I .
PHYSICA STATUS SOLIDI B-BASIC RESEARCH, 1983, 116 (01) :K43-K46
[4]   EFFECT OF LATTICE DISORDER ON THE EXCITONIC STATES IN SUPERIONIC CRYSTALS [J].
AKOPYAN, IC ;
GROMOV, DN ;
KLOCHIKHIN, AA ;
NOVIKOV, BV ;
OGLOBLIN, SG .
PHYSICA STATUS SOLIDI B-BASIC SOLID STATE PHYSICS, 1988, 148 (01) :185-195
[5]   ABSENCE OF DIFFUSION IN CERTAIN RANDOM LATTICES [J].
ANDERSON, PW .
PHYSICAL REVIEW, 1958, 109 (05) :1492-1505
[6]  
ANDO T, 1988, ANDERSON LOCALIZATIO
[7]  
[Anonymous], NUOVO CIMENTO SUPPL, DOI DOI 10.1007/BF02746071
[8]  
[Anonymous], 1972, PHASE TRANSITIONS CR
[9]  
ANSELM AI, 1955, ZH EKSP TEOR FIZ, V28, P151
[10]  
AVEN M, 1967, PHYSICS CHEM 2 6 COM