Magnetic tensors for the and states of

Y Sun, T Böttger, CW Thiel, RL Cone - Physical Review B—Condensed Matter …, 2008 - APS
Y Sun, T Böttger, CW Thiel, RL Cone
Physical Review B—Condensed Matter and Materials Physics, 2008APS
We present the complete Zeeman g tensors for the lowest-energy I 15∕ 2 4 and I 13∕ 2 4
states of Er 3+ doped into Y 2 Si O 5 for both crystallographic sites deduced from orientation-
dependent optical Zeeman spectroscopy over three orthogonal crystal planes. From these
data, principal axes of the g tensors were determined for each crystallographic site. Along
axes with maximum values, the effective g factors are 14.65 (site 1) and 15.46 (site 2) for the
ground state, and 12.97 (site 1) and 13.77 (site 2) for the excited state. To minimize optical …
We present the complete Zeeman tensors for the lowest-energy and states of doped into for both crystallographic sites deduced from orientation-dependent optical Zeeman spectroscopy over three orthogonal crystal planes. From these data, principal axes of the tensors were determined for each crystallographic site. Along axes with maximum values, the effective factors are 14.65 (site 1) and 15.46 (site 2) for the ground state, and 12.97 (site 1) and 13.77 (site 2) for the excited state. To minimize optical decoherence and spectral diffusion in device applications and high resolution spectroscopy, special directions for applying an external magnetic field have been found for each site, for which the ground- and excited-state factors are equal. Among those directions, choices are presented that also maximize the ground-state splittings for all four magnetically inequivalent sites, thus optimizing the prospects for freezing out electron spin fluctuations and reducing decoherence and spectral diffusion significantly.
American Physical Society
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