The spin-selective photokinetics of a single matrix-isolated impurity molecule with a triplet-triplet optical transition, T0–T1, is considered and the manifestations of the photokinetics in the fluorescence excitation spectra and intensity autocorrelation functions g(2)(τ) of the molecule undergoing narrow-band optical excitation is studied to resolve the fine structure of the transition. The rates of intersystem crossings (ISCs) T1→S→T0 to and from a nonradiating singlet state S of the molecule and the rate of population relaxation among the ground (T0) state sublevels can be obtained from the spectra and g(2)(τ) using the analytical expressions obtained. New experiments on an individual NV defect center in nanocrystals of diamond, where, for the first time, the fine structure of its triplet-triplet 3A-3E zero-phonon optical transition (~637 nm) at 1.4 K was resolved, are interpreted. It is concluded that the rate of the ISC transition from the mS=0 sublevel of the excited 3E state to the singlet 1A state (~1 kHz) is much slower than the rates from the mS=±1 substates, while the rates of ISC transitions to different mS substates of the ground 3A state are close to each other (~1 Hz). As a result, only the optical transition between mS=0 sublevels in the 3A-3E manifold contributes strongly to the fluorescence. The experimentally observed double-exponential decay of the g(2)(τ) function is explained by the two pathways available to the center for it to leave the S state: (i) the S→ T0(mS)=0) transition and (ii) the S→T0(mS=±1) transitions followed by the slow spin-lattice relaxation T0(mS=±1)→T0(mS=0) (rate ~0.1 Hz). The work is important for studies where the NV center is used as a single photon source or for quantum information processing.
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