HIGH-PRESSURE PHASE-TRANSITIONS IN ZN1-XMNXSE - A RAMAN-SCATTERING AND PHOTOLUMINESCENCE STUDY

Citation
Ak. Arora et T. Sakuntala, HIGH-PRESSURE PHASE-TRANSITIONS IN ZN1-XMNXSE - A RAMAN-SCATTERING AND PHOTOLUMINESCENCE STUDY, Physical review. B, Condensed matter, 52(15), 1995, pp. 11052-11058
Citations number
28
Categorie Soggetti
Physics, Condensed Matter
ISSN journal
01631829
Volume
52
Issue
15
Year of publication
1995
Pages
11052 - 11058
Database
ISI
SICI code
0163-1829(1995)52:15<11052:HPIZ-A>2.0.ZU;2-V
Abstract
High-pressure phase transitions in semiconductor mixed crystals Zn1-xM nxSe (x less than or equal to 0.29) are investigated using Raman scatt ering and photoluminescence (PL) up to a pressure of 150 kbar. The sam ples are characterized for composition and crystal structure. A new Ra man mode is observed between TO and LO frequencies for samples with x less than or equal to 0.097 and is assigned to a disorder activated zo ne boundary phonon. Apart from the PL band at 2.1 eV due to the T-4(1) --> (6)A(1) transition between the crystal field split levels of Mn2, a PL band is observed at 1.94 eV in the samples with x = 0.063 which is assigned to a native defect forming a complex with Mn2+. The inten sity of the PL band reduces drastically with pressure and completely d isappears at about 15 kbar. A possible model for this behavior is pres ented. The pressure dependence of the phonon frequencies and the behav ior of PL suggest three transitions P-1, P-2, and P-3 for the mixed cr ystals with re = 0.29, whereas those with x = 0.063 and 0.097 show onl y P-2 and P-3 transitions. In the sample with x = 0.29. TO mode splits into two components across P-1 and the low-frequency component exhibi ts softening. The crystals turn opaque across P-2 and the PL signal di sappears suggesting that the band gap changes from direct to indirect. Intensities of Raman lines decrease and completely disappear across P -3. The difference in the behavior of the phase transitions for the lo w and the high values of a is understood on the basis of their differe nt crystal structures.