화학공학소재연구정보센터
Journal of Physical Chemistry A, Vol.113, No.45, 12591-12598, 2009
Energy Gaps in the 4f(13)5d(1) Manifold and Multiple Spontaneous Emissions in Yb2+-Doped CsCaBr3
Multiple spontaneous; 4f(13)5d(1) -> 4f(14) emissions are predicted in Yb2+-doped CsCaBr3 crystal% by ab initio quantum chemical calculations. Four emission bands are found at 23 900, 26 600, 34 600, and 43 900 cm(-1) that should be experimentally observable at low temperatures The first. third, and fourth hands are slow, electric dipole forbidden emissions that can be described as spin-forbidden The second band is a fast, electric dipole-allowed emission that cannot be described as spin-allowed, but as spin-enabled, its radiative emission lifetime is 400 ns. Large energy gaps (23 900, 4600, 4000 cm(-1), respectively). relative to the maximum local phonon energies calculated (around 185 cm(-1)), art found below the emitting levels of the slow bands. which indicates that these states should be significantly Stable and multiphonon relaxation to the lower states should be negligible A smaller gap (2600 cm(-1)) separates the states of the fast band, which should result in a temperature dependent competition between radiative and nonradiative decay. Differential correlation between 4f-4f and 4f-5d pairs. splitting of the 5d shell by interactions with the host. and spin-orbit effects within the 4f(13) subshell, am found to be responsible for the existence of the gaps, which, in turn, split the absorption spectrum into four groups of separate bands, three of which could he below the host absorption threshold The quantum chemical methods employed make use of explicit wave functions expanded in terms of flexible basis sets, multiconfigurational self-consistent-field and multireference second-order perturbation methods to account for nondynamic and dynamic electron correlation, scalar and relativistic terms in the (YbBr6)(4-) defect cluster Hamiltonian, and quantum mechanical embedding potentials to represent the host crystal.