Optoelectronic properties of thin film CdS formed by ultraviolet and infrared pulsed-laser deposition

Citation
B. Ullrich et al., Optoelectronic properties of thin film CdS formed by ultraviolet and infrared pulsed-laser deposition, THIN SOL FI, 385(1-2), 2001, pp. 220-224
Citations number
25
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science","Material Science & Engineering
Journal title
THIN SOLID FILMS
ISSN journal
00406090 → ACNP
Volume
385
Issue
1-2
Year of publication
2001
Pages
220 - 224
Database
ISI
SICI code
0040-6090(20010402)385:1-2<220:OPOTFC>2.0.ZU;2-M
Abstract
Thin CdS films on glass are formed by ultraviolet (UV) and infrared (IR) pu lsed-laser deposition (PLD) at 355 and 1064 nm with a repetition rate of 10 Hz and a pulse width of 10 ns and 150-180 mus, respectively. The applied l aser fluence is kept in the range of 2-3 J cm(-2). By UV-PLD, the orientati on of the c-axis with respect to the glass surface is adjustable via laser fluence, resulting in perpendicular and parallel oriented films at 2 and 4 J cm(-2), respectively. The orientation of IR-PLD samples is maintained per pendicularly, independent of the fluence. The optoelectronic properties of the films are studied by photocurrent (PC) and photoluminescence (PL) spect roscopy at 300 K. The PC of the UV-PLD samples reflects the turn of the c-a xis, i.e. the absorption anisotropy, of CdS. The IR-PLD films, however, do not show PC because of high dark conductivity. The UV-PLD samples show PL i n the range (2.27-2.45 eV). The emission below 2.45 eV is caused by formati on of recombination centers. Notably, the film formed at 3 J cm emits the s pectral sum of the films formed at 2 and 4 J cm(-2). The IR-PLD samples sho w green emission (2.493 eV) clearly above the CdS bandgap due to band filli ng. The results pave the way for the creation of smart photonic gratings, w hich exhibit locally tunable optoelectronic properties. (C) 2001 Elsevier S cience B.V. All rights reserved.