25-29 June 2018
Africa/Johannesburg timezone
General information and Registration for SAIP2018 is handled by Eastern Sun Events at: http://www.saipconference.co.za/ <p> Deadline for papers for the conference proceedings is 28 July 2018

The thermal quenching process of the La<sub>2</sub>O<sub>2</sub>S:Eu(III) phosphor material

26 Jun 2018, 12:20
20m
Oral Presentation Track A - Physics of Condensed Matter and Materials Physics of Condensed Matter and Materials

Speaker

Mr Lucas Erasmus (University of the Free State)

Description

This study is concentrating on the measurement of the emission of commercially available lanthanum oxysulphide doped with europium(III) (La2O2S:Eu(III)) phosphor material at various temperatures. For the thermal quenching process, the average activation energies for the emission from the 5D2, 5D1 and 5D0 excited states were determined as 0.49 eV, 0.55 eV and 0.77 eV, respectively and the average pre-exponential constant was determined as 9.5×107 s-1. The optical band gap of La2O2S:Eu(III) was determined as 2.75 eV. It was also established that the sulphur(II) to europium(III) (Eu(III)) charge transfer band absorbs ultraviolet light and transfers the excited electrons to the excited states of the Eu(III) ions from where emission can take place. The lifetime of the luminescence results indicated that the higher excited states have a double exponential lifetime that results from the emission from both the conventional Eu(III) ions and Eu(III) ions that are in the vicinity of a defect or impurity group. It was determined that in the case of the La2O2S:Eu(III) phosphor material, the presence of defect or impurity groups is due to the hydroxide groups that forms when the material was exposed to water vapour in the atmosphere at room temperature. The average emission decay constants of the 5D2, 5D1 and 5D0 excited states were determined as 10 ns, 80 ns and 340 ns respectively. It was also revealed that La2O2S:Eu(III) can be utilised as a temperature sensor by using the fluorescence intensity ratio of the emission from the 5D1 and 5D0 excited states. This worked well for the temperature range from 80 °C to 180 °C.

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Hendrik C. Swart, Department of Physics, University of the Free State, Bloemfontein, South Africa, SwartHC@ufs.ac.za

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Primary authors

Prof. Hendrik Swart (University of the Free State) Prof. JJ (Koos) Terblans (UFS) Mr Lucas Erasmus (University of the Free State) Dr Valentin Craciun (National Institute for Laser, Plasma and Radiation Physics)

Presentation Materials

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