Garcia, J. A.Fernández Sánchez, PalomaRemon, A.Piqueras de Noriega, JavierMunoz, V.Triboulet, R.2023-06-202023-06-202001-05[1] Marfaing Y 1996 J. Cryst. Growth 161 205 [2] Pautrat J L, Magnea N and Faurie J P 1982 J. Appl. Phys. 53 8668 [3] Nakamura S 1997 MRS Bull. 22 29 [4] Kuhn W S et al 1995 Prog. Cryst. Growth Charac. Mater. 31 119 [5] Naumov A, Wolf K, Reisinger T, Stanzl H, Wagner H P and Gebhardt W 1993 Physica B 185 250 [6] Wolf K, Naumov A, Reisinger T, Kastner M, Stanzl H, Kuhn W and Gebhardt K W 1994 J. Cryst. Growth 135 113 [7] García J A, Rem´on A, Mu˜noz V and Triboulet R 1999 J. Cryst. Growth 197 794 [8] Fernández P, García A, Rem´on A, Piqueras J, Muñoz V and Triboulet R 1998 Semicond. Sci. Technol. 13 410 [9] García J A, Remon A, Mu˜noz V and Triboulet R 1998 J. Cryst. Growth 191 685 [10] Domínguez-Adame F, Piqueras J and Fernández P 1991 Appl. Phys. Lett. 58 2570268-124210.1088/0268-1242/16/5/302https://hdl.handle.net/20.500.14352/59125© 2001 IOP Publishing Ltd. This paper was partially supported by the Spanish Comisión Interministerial para Ciencia y Tecnolog´ıa under grants MAT98-0975-C02-01 and 1FD97-0086.Samples of zinc telluride bulk single crystals, which were deformed in uniaxial compression, have been studied by photoluminescence (PL) and cathodoluminescence (CL). As a particular feature the deformed samples present a PL emission band peaked at 603 nm, whose intensity increases as the plastic deformation does. This band is related to the density of dislocations produced during the interaction of slip systems. This hypothesis is supported by CL images. which reveal the activation of the successive slip systems corresponding to different levels of deformation.engjournal articlehttp://dx.doi.org/10.1088/0268-1242/16/5/302http://iopscience.iop.orgopen access538.9II-Vi CompoundsGrown ZnteDefectsLuminescenceFísica de materiales