Temperature dependences of the CW-EPR spectrum as well as the
electron spin−lattice relaxation time
T
1
and phase memory time T
M determined by electron
spin echo were measured for Cu2+ ions in
(NH4)2Mg(SO4)2·6H2O single crystal.
The dependences are dominated by vibronic behavior of the
Cu(H2O)6
2+
complex
and connected to the dynamic Jahn−Teller effect producing
reorientations between two lowest energy wells
of the adiabatic potential surface. Below 70 K the static
Jahn−Teller effect is observed, and the system is
strongly localized, by the local strains, in the deepest potential well
leaving higher wells not populated. Above
this temperature the second well becomes progressively populated, and a
rapid averaging of the g
z
and
g
y
factors as well as corresponding hyperfine splittings appears. The
Boltzmann population of these two wells
is achieved at 160 K. Simultaneously with g factors
averaging a continuous broadening of the hyperfine
lines is observed with line shape transformed from Gaussian at 70 K to
Lorentzian at 160 K. The averaging
and broadening processes are thermally activated with energy barrier
δ12 = 108 ± 3 cm-1 = 156
K = 1.26
kJ/mol being the energy difference between the two deepest potential
wells. Electron spin relaxation was
measured below 50 K where electron spin-echo signal was detectable.
Spin−lattice relaxation is driven by
the direct and Raman processes with relaxation rate
1/T
1 = aT +
bT
5 as expected for dynamic
Jahn−Teller
systems. Spin−spin phase relaxation described by the phase
memory time T
M depends on temperature
as
1/T
M = a + bT +
c exp(−Δ/kT) with Δ = 102 ± 2
cm-1. At low temperatures the higher
energy well is not
populated; thus, Δ can be assigned as the energy of the first excited
vibronic level in the deepest well. The
Δ and δ12 are temperature-independent, indicating that
adiabatic potential surface is not affected by
temperature.
We suggest that the deviations of experimental data from
theoretically predicted vibronic g-factors
averaging
observed for Cu2+ in many Tutton salt type crystals are
not due to temperature variations of the local strains
or barrier height but are due to the fact that Boltzmann population of
the potential wells cannot exist at low
temperatures. This effect is especially pronounced for
Cu2+ ions in
(NH4)2Mg(SO4)2·6H2O
since the energy
Δ of the first vibronic level is lower than the energy difference
δ12 between adjacent wells. In such case
the
phonon-assisted tunneling jumps between the energy wells induced by
two-phonon Raman processes via
virtual state of energy δ12 become to be effective when
kT ≥ δ12/2, and the Boltzmann population of
the
second well is achieved via direct phonon process when thermal phonons
of energy kT ≥ δ12 are
available.