Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Optics Communications

Observation of laser-jitter-enhanced hyperfine spectroscopy and two-photon spectral hole-burning

Byoung Seung HAM, Philip Hemmer, M. S. Shahriar

Published Jun 1, 1999• 3 citations
Publisher
DOI
10.1016/s0030-4018(99)00155-8

Related papers

Observation of laser-jitter-enhanced hyperfine spectroscopy and two-photon spectral hole-burning

Hanscom Afb

•Jan 1, 1999•0 citations

Toward a powerful application of laser spectroscopy: photon-gated persistent spectral hole burning

W. E. Moerner, R. M. Macfarlane

Conference on Lasers and Electro-Optics•Apr 26, 1987•0 citations

Hyperfine spectroscopy by optical hole burning and optical-radio-frequency double resonance (A)

Robert M. Shelby, R. M. Macfarlane

Journal of the Optical Society of America A•Jan 1, 1983•0 citations

Photon-gated spectral hole burning in LiGa 5 O 8 :Co 2+

R. M. Macfarlane, J. C. Vial

Photon-gated hole burning, or selective bleaching enabled by a second light source, has been observed in ${\mathrm{Co}}^{2+}$ in tetrahedral sites of ${\mathrm{LiGa}}_{5}$${\mathrm{O}}_{8}$. This leads to long-lived spectral holes with a width of \ensuremath{\sim}1 GHz at 1.6 K. It is proposed that two-step photoionization of ${\mathrm{Co}}^{2+}$ is responsible for the hole burning. Much narrower (\ensuremath{\sim}40 MHz) transient holes and antiholes were burned using population storage in nuclear hyperfine levels. These two mechanisms of hole burning are reported here for transition-metal ions for what is believed to be the first time.

•Jun 9, 1986•0 citations

Photon-gated spectral hole burning in LiGa5 O8 : Co2+

R. M. Macfarlane, J. C. Vial

Photon-gated hole burning, or selective bleaching enabled by a second light source, has been observed in ${\mathrm{Co}}^{2+}$ in tetrahedral sites of ${\mathrm{LiGa}}_{5}$${\mathrm{O}}_{8}$. This leads to long-lived spectral holes with a width of \ensuremath{\sim}1 GHz at 1.6 K. It is proposed that two-step photoionization of ${\mathrm{Co}}^{2+}$ is responsible for the hole burning. Much narrower (\ensuremath{\sim}40 MHz) transient holes and antiholes were burned using population storage in nuclear hyperfine levels. These two mechanisms of hole burning are reported here for transition-metal ions for what is believed to be the first time.

Physical review. B, Condensed matter•Jul 1, 1986•47 citations

Photon-gated spectral hole burning in Pr^3+:YAG

R. M. Macfarlane, G. Wittmann

We observed photon-gated spectral hole burning in Pr:YAG and assigned the hole-burning mechanism to selective photoionization of trivalent praseodymium. Gated holes were observed in absorption lines to the two lowest components of the (1)D(2) manifold. At 1.4 K the gating ratio is in excess of 1.5 x 10(4). Strong competition from the transient mechanism of optical pumping of hyperfine levels occurs below 6 K.

Optics Letters•Aug 15, 1996•15 citations
Photon-gated hole burning, or selective bleaching enabled by a second light source, has been observed in Co2+{\mathrm{Co}}^{2+}Co2+ in tetrahedral sites of LiGa5{\mathrm{LiGa}}_{5}LiGa5​O8{\mathrm{O}}_{8}O8​. This leads to long-lived spectral holes with a width of \ensuremath{\sim}1 GHz at 1.6 K. It is proposed that two-step photoionization of Co2+{\mathrm{Co}}^{2+}Co2+ is responsible for the hole burning. Much narrower (\ensuremath{\sim}40 MHz) transient holes and antiholes were burned using population storage in nuclear hyperfine levels. These two mechanisms of hole burning are reported here for transition-metal ions for what is believed to be the first time.
Photon-gated hole burning, or selective bleaching enabled by a second light source, has been observed in Co2+{\mathrm{Co}}^{2+}Co2+ in tetrahedral sites of LiGa5{\mathrm{LiGa}}_{5}LiGa5​O8{\mathrm{O}}_{8}O8​. This leads to long-lived spectral holes with a width of \ensuremath{\sim}1 GHz at 1.6 K. It is proposed that two-step photoionization of Co2+{\mathrm{Co}}^{2+}Co2+ is responsible for the hole burning. Much narrower (\ensuremath{\sim}40 MHz) transient holes and antiholes were burned using population storage in nuclear hyperfine levels. These two mechanisms of hole burning are reported here for transition-metal ions for what is believed to be the first time.