Abstract

The infrared to visible upconversion processes have been investigated for ${\mathrm{Nd}}^{3+}$-doped chalcohalide glasses with different halide modifiers by using steady-state and time-resolved laser spectroscopy. Two different upconversion mechanisms have been identified depending on the infrared excitation wavelength. When the excitation wavelength is resonant with the ${}^{4}{F}_{3/2}$ state, three main bands at 538, 600, and 675 nm are observed and attributed to emissions from the ${}^{4}{G}_{7/2}$ level. These upconverted emissions occur via energy-transfer upconversion involving two neodymium ions in the ${}^{4}{F}_{3/2}$ state. However, nonresonant excitation at higher energies than that of ${}^{4}{F}_{3/2}$ state (between states ${}^{4}{F}_{3/2}$ and ${}^{4}{F}_{5/2})$ or in resonance with the ${}^{4}{F}_{5/2}$ state, causes an additional blue emission to originate from the ${}^{2}{P}_{1/2}$ state. This latter upconverted emission can be attributed to excited-state absorption of the pump radiation. The proposed upconversion mechanisms responsible for the different emissions from levels ${}^{2}{P}_{1/2}$ and ${}^{4}{G}_{7/2}$ are supported by both the time evolution of the upconversion luminescence after infrared pulsed excitation and the upconversion luminescence excitation spectra.

Highlights

  • Neodymium has been recognized as one of the most efficient rare-earthREions for solid-state lasers in different hosts[1,2] due to its intense emission at 1.06 ␮m

  • Infrared-to-visible upconversion in Nd3ϩ-doped chalcohalide glasses has been investigated under continuous-wave and pulsed-laser excitation for different halide modifiers

  • Similar upconverted emission spectra are found with different halideCl, Br, Imodifiers; glass modified with CsCl shows the highest intensity for the blue emission

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Summary

Introduction

Neodymium has been recognized as one of the most efficient rare-earthREions for solid-state lasers in different hosts[1,2] due to its intense emission at 1.06 ␮m. The germanium-gallium-sulfideGGSglass system has been studied for its potential as a low phonon energy glass for lasers and fiber-optic amplifier applications.[21,22,23,24] Sulfide glasses, usually show a low-energy band gap that causes strong absorption of visible light, as in Ga-and Gebased glasses,[25,26] which can limit applications such as upconversion. This drawback is partly circumvented in Ge-

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