Published March 2016 | Version v1
Journal article

Bandgap engineering of the LuxY1−xPO4 mixed crystals

  • 1. Physics Faculty, Moscow State University, Leninskiye Gory 1-2, 11991 Moscow (Russian Federation)
  • 2. Institute of Physics, University of Tartu, Ravila 14c, 50411 Tartu (Estonia)
  • 3. Skobeltsyn Institute of Nuclear Physics, Moscow State University, Leninskiye Gory 1-2, 11991 Moscow (Russian Federation)
  • 4. A. Alikhanyan National Science Laboratory, Yerevan Physics Institute, Alikhanyan Yeghbayrneri St. 2, 0036 Yerevan (Armenia)
  • 5. Institute of Physics, Polish Academy of Sciences, Al. Lotników 32/46, 02-668 Warsaw (Poland)
  • 6. Institute of Physics, Jan Dlugosz University, Armii Krajowej 13/15, PL-42200 Czestochowa (Poland)
  • 7. College of Sciences, Chongqing University of Posts and Telecommunications, 400065 Chongqing (China)
  • 8. Central Research and Development Institute of Chemistry and Mechanics, Nagatinskaya St. 16a, 115487 Moscow (Russian Federation)
  • 9. Institute of Light and Matter, CNRS, University Lyon1, 69622 Villeurbanne (France)

Description

Bandgap modification of the LuxY1−xPO4 mixed crystals has been studied by thermostimulated luminescence (TSL) and ab-initio calculation methods. Doping of LuxY1−xPO4 with Ce3+ allowed to follow up the changes of electron traps depth, caused by the modification of the bottom of conduction band. The observed gradual shift of the most intensive TSL peaks to higher temperatures with increase of x value was connected with the high-energy shift of the conduction band bottom. According to the band structure calculations the bottom of the conduction band is formed by the 5d and 4d states of Lu and Y, respectively. Therefore, substitution of one cation by another is responsible for the observed variation of the electronic and optical properties. Doping with Eu3+ was used to study the modification of the hole traps and the top of the valence band in LuxY1−xPO4. The independence of the TSL peaks position on x value in LuxY1−xPO4:Eu3+ allows to conclude that the top of the valence band is negligibly affected by the cation substitution. According to the band structure calculations the top of the valence band is formed by the O 2p electronic states, which are not affected by the cation substitution. The resulting increase of the bandgap with x value is confirmed by the data of ab-initio calculations. - Highlights: • Band structure modification with x in LuxY1−xPO4:RE3+ (RE=Ce, Eu) is studied. • Depth of electron traps is affected by the bandgap modification. • Increase of bandgap with x is due to the shift of conduction band bottom.

Availability note (English)

Available from http://dx.doi.org/10.1016/j.jlumin.2015.10.074

Additional details

Identifiers

DOI
10.1016/j.jlumin.2015.10.074;
PII
S0022-2313(15)00651-1;

Publishing Information

Journal Title
Journal of Luminescence
Journal Volume
171
Journal Page Range
p. 33-39
ISSN
0022-2313
CODEN
JLUMA8

INIS

Country of Publication
Netherlands
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
49022611
Subject category
S36: MATERIALS SCIENCE;
Descriptors DEI
CALCULATION METHODS; CATIONS; CERIUM IONS; CRYSTALS; EUROPIUM IONS; LUTETIUM COMPOUNDS; MODIFICATIONS; OPTICAL PROPERTIES; TEMPERATURE RANGE 0400-1000 K; THERMOLUMINESCENCE
Descriptors DEC
CHARGED PARTICLES; EMISSION; IONS; LUMINESCENCE; PHOTON EMISSION; PHYSICAL PROPERTIES; RARE EARTH COMPOUNDS; TEMPERATURE RANGE

Optional Information

Copyright
Copyright (c) 2015 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.