Growth and characterization of ZnO1−xSx highly mismatched alloys over the entire composition
Creators
- 1. Department of Mechanical Engineering, University of California, Berkeley, California 94720 (United States)
- 2. Materials Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720 (United States)
- 3. Department of Physics and Materials Science, City University of Hong Kong, Kowloon (Hong Kong)
- 4. Joint Center for Artificial Photosynthesis, Lawrence Berkeley National Laboratory, Berkeley, California 94720 (United States)
- 5. Department of Electrical Engineering and Computer Sciences, University of California, Berkeley, California 94720 (United States)
- 6. ICMUV, Instituto de Ciencia de Materiales, Universitat de València, P.O. Box 22085, 46071 Valencia (Spain)
- 7. Department of Experimental Physics, Wrocław University of Technology, Wybrzeze Wyspianskiego 27, 50-370 Wrocław (Poland)
- 8. Department of Materials Science and Engineering, University of California, Berkeley, California 94720 (United States)
Description
Alloys from ZnO and ZnS have been synthesized by radio-frequency magnetron sputtering over the entire alloying range. The ZnO1−xSx films are crystalline for all compositions. The optical absorption edge of these alloys decreases rapidly with small amount of added sulfur (x ∼ 0.02) and continues to red shift to a minimum of 2.6 eV at x = 0.45. At higher sulfur concentrations (x > 0.45), the absorption edge shows a continuous blue shift. The strong reduction in the band gap for O-rich alloys is the result of the upward shift of the valence-band edge with x as observed by x-ray photoelectron spectroscopy. As a result, the room temperature bandgap of ZnO1−xSx alloys can be tuned from 3.7 eV to 2.6 eV. The observed large bowing in the composition dependence of the energy bandgap arises from the anticrossing interactions between (1) the valence-band of ZnO and the localized sulfur level at 0.30 eV above the ZnO valence-band maximum for O-rich alloys and (2) the conduction-band of ZnS and the localized oxygen level at 0.20 eV below the ZnS conduction band minimum for the S-rich alloys. The ability to tune the bandgap and knowledge of the location of the valence and conduction-band can be advantageous in applications, such as heterojunction solar cells, where band alignment is crucial
Additional details
Identifiers
- DOI
- 10.1063/1.4936551;
Publishing Information
- Journal Title
- Journal of Applied Physics
- Journal Volume
- 118
- Journal Issue
- 21
- Journal Page Range
- p. 215702-215702.7
- ISSN
- 0021-8979
- CODEN
- JAPIAU
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 47063147
- Subject category
- S36: MATERIALS SCIENCE;
- Descriptors DEI
- ABUNDANCE; ALLOYS; EV RANGE; HETEROJUNCTIONS; MAGNETRONS; OXYGEN; RADIOWAVE RADIATION; RED SHIFT; SOLAR CELLS; SPUTTERING; SULFUR; TEMPERATURE RANGE 0273-0400 K; THIN FILMS; VALENCE; X-RAY PHOTOELECTRON SPECTROSCOPY; ZINC OXIDES; ZINC SULFIDES
- Descriptors DEC
- CHALCOGENIDES; DIRECT ENERGY CONVERTERS; ELECTROMAGNETIC RADIATION; ELECTRON SPECTROSCOPY; ELECTRON TUBES; ELECTRONIC EQUIPMENT; ELEMENTS; ENERGY RANGE; EQUIPMENT; FILMS; INORGANIC PHOSPHORS; MICROWAVE EQUIPMENT; MICROWAVE TUBES; NONMETALS; OXIDES; OXYGEN COMPOUNDS; PHOSPHORS; PHOTOELECTRIC CELLS; PHOTOELECTRON SPECTROSCOPY; PHOTOVOLTAIC CELLS; RADIATIONS; SEMICONDUCTOR JUNCTIONS; SOLAR EQUIPMENT; SPECTROSCOPY; SULFIDES; SULFUR COMPOUNDS; TEMPERATURE RANGE; ZINC COMPOUNDS
Optional Information
- Notes
- (c) 2015 AIP Publishing LLC