corner
corner

Phys. Rev. B 52, 3963–3969 (1995)

Homogeneous broadening and hyperfine structure of optical transitions in Pr3+:Y2SiO5

Download: PDF (317 kB) Buy this article Export: BibTeX or EndNote (RIS)

R. W. Equall and R. L. Cone
Physics Department, Montana State University, Bozeman, Montana 59717

R. M. Macfarlane
IBM Almaden Research Center, 650 Harry Road, San Jose, California 95120

Received 20 March 1995; published in the issue dated 1 August 1995

Contributions to the homogeneous linewidth of the 3H4(1)1D2(1) transition for the two crystallographic sites of Pr3+ in Y2SiO5 have been investigated using photon echoes. The effects of excitation-intensity-dependent dephasing or instantaneous diffusion were systematically studied to allow accurate determination of the optical resonance widths. Homogeneous linewidths of 2.8 kHz (site 1) and 1 kHz (site 2) were measured with no applied magnetic field and with sufficiently low laser intensity to minimize the effects of instantaneous diffusion. Using the same excitation intensity, widths of 2.1 kHz (site 1) and 0.85 kHz (site 2) were obtained with an applied magnetic field of 77 G, demonstrating a significant contribution of 89Y nuclear-spin fluctuations to the zero-field homogeneous linewidth. Extrapolation to zero excitation intensity yielded optical resonance widths that were only slightly narrower than the measured values. Optically detected nuclear magnetic resonance measurements determined the hyperfine structure of the 3H4 ground state for each site; the hyperfine levels of the lowest component of the 1D2 manifold for each site were determined using photon echo nuclear double resonance. The relatively large oscillator strength of 3×10-7 for a rare-earth ion, in conjunction with long dephasing times makes this material a useful candidate for demonstration of time-domain signal processing and optical data storage.

© 1995 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevB.52.3963
DOI:
10.1103/PhysRevB.52.3963
PACS:
42.50.Md, 78.50.Ec