Abstract
We report transient spectral hole-burning studies of the R 2(±1/2) line in 130, 20 ppm and 0.6 ppm ruby between 2.4 and 70 K. The homogeneous line width Γ h is found to be 142 ± 6 MHz at 2.4 K for both 20 and 130 ppm crystals; this value is in agreement with the T 1 value of 1.1 ns ( Γ h = 1/2 πT 1 = 140 MHz) for the 2 A ¯ state obtained by Rives and Meltzer who used pulsed, non-selective laser excitation. The line width is dominated by a direct one-phonon relaxation process 2 A ¯ → E ¯ up to 50 K whereas at higher temperatures two-phonon Raman scattering becomes dominant. Cross-relaxation and spin-lattice relaxation times significantly affect pseudo-CW experiments.
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