Absorption spectra of Cs2ZrCl6 doped with Re(IV) and Tm(III) at levels
up to 5 mol% were used to confirm and establish the energy levels of
these two ions in this host. Steady-state luminescence spectroscopy es
tablished that Re to Tm energy transfer occurs with an efficiency that
increases with Tm concentration as well as with lower temperature. Co
nsistent with this, the 86 us lifetime of the ReCl62- Gamma(7)(T-2(2g)
) state at 90 K was reduced to 48 mu s by the presence of 1% Tm and so
me early, non-exponential decay became evident. At the same time, the
long-lived, 450 mu s, luminescence from the Tm(H-3(4)) state appeared
with a 48 mu s risetime. At 5% incorporated Tm, the non-exponentiality
of the Re luminescence decay and the rise of the Tm luminescence beca
me much more marked, with double exponential curves giving decay lifet
imes of 5 and 24 mu s for Re, and a rise time of 6 us and decay time o
f 430 mu s for Tm. Over the temperature range 80-298 K, excitation of
a 5% Re/5% Tm doped sample with 150 mW 647.1 nm radiated led to Re Gam
ma(7)(T-2(2g)) and Tm(H-3(4)) luminescence, plus up-conversion lumines
cence from the Tm(D-1(2)) state with only a small Tm((1)G(4)) componen
t. The first two signals were linear in excitation power while the Tm(
D-1(2)) luminescence increased quadratically. The 5% Mo(III)/5% Tm(III
) doped Cs2NaYCl6 sample also showed up-conversion when excited at 514
nm into the Mo(III) (T-2(2g)) state. The up-converted luminescence wa
s now mainly from Tm((1)G(4)), with minor contributions from higher st
ates. On irradiation into the Tm(H-3(4)) state with 150 mW of radiatio
n of 12 500 cm(-1), up-converted luminescence from Tm((1)G(4)) was aga
in seen, but accompanied by luminescence from Mo(T-2(2g)). Energy tran
sfer therefore occurs in both directions.