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

Coherent Pulse Technique in the Optical Detection of the 0 ↔ 0 Ground State Hyperfine Resonance in Rubidium 87

C. O. Alley

Published Jan 1, 1960• 2 citations
OpenAlex

Related papers

Two-Photon Coherent Manipulation of Hyperfine Ground States in Rubidium Vapor

王晓晨 Wang Xiaochen, 蒋小军 Jiang Xiaojun, 赵子豪 Zhao Zihao +4 more

Acta Optica Sinica•Jan 1, 2018•0 citations

Measurement of the hyperfine structure of Pr^3::YAG by quantum-beat free-induction decay, hole burning, and optically detected nuclear quadrupole resonance

Robert M. Shelby, A.C. Tropper, Richard T. Harley +1 more

The hyperfine splitting of the ground state and the lowest electronic component of the (1)D(2) excited state have been measured for Pr(3+) in YAG. We show that a particularly simple and powerful technique is the production of sublevel coherence by short-pulse (impact) excitation, which is detected by coherent forward scattering of a weak probe beam and Fourier transformation of the resulting quantum-beat signal. This yielded excited-state splittings of 6.49 and 8.29 MHz. The ground state shows large pseudoquadrupole splittings of 33.4 and 41.6 MHz, which were obtained by optically detected nuclear quadrupole resonance.

Optics Letters•Jun 1, 1983•48 citations

Coherent dark states of rubidium 87 in a buffer gas using pulsed laser light

S. Brattke, U. Kallmann, W.-D. Hartmann

The coherent dark resonance between the hyperfine levels F=1, m F =0 and F=2, m F =0 of the rubidium ground state has been observed experimentally with the light of a pulsed mode-locked diode laser operating at the D1 transition frequency. The resonance occurs whenever the pulse repetition frequency matches an integer fraction of the rubidium 87 ground state hyperfine splitting of 6.8 GHz. Spectra have been taken by varying the pulse repetition frequency. Using cells with argon as a buffer gas a linewidth as narrow as 149 Hz was obtained. The rubidium ground state decoherence cross section for collisions with xenon atoms has been measured for the first time with this method using a pure isotope rubidium vapor cell and xenon as a buffer gas.

arXiv:quant-ph/9803081•The European Physical Journal D•Jan 1, 1998•13 citations

A detailed study of the quantum coherent and saturating resonances using the hyperfine lines of rubidium

Sekhar Dey, Chandan Das, Saswati Dey +2 more

Hyperfine Interactions•May 13, 2019•0 citations

Optical Signal Processing Method of the Rubidium-87 Quantum Frequency Standard

Anton Valov, Valentin I. Dudkin, Nikita A. Lukashev +1 more

Springer proceedings in physics•Nov 27, 2020•0 citations

Electromagnetically induced transparency in rubidium vapor prepared by a comb of short optical pulses

Vladimir A. Sautenkov, Yuri V. Rostovtsev, C. Y. Ye +3 more

It was shown by Kocharovskaya and Khanin [Sov. Phys. JETP 63, 945 (1986)] that a comb of optical pulses can induce a ground-state atomic coherence and change the optical response of an atomic medium. In our experiment, we studied the propagation of a comb of optical pulses produced by a mode-locked diode laser in rubidium atomic vapor. Electromagnetically induced transparency (EIT) was observed when the pulse repetition rate is a subharmonic of the hyperfine splitting of the ground state. The width of the EIT resonance is determined by the relaxation rate of the ground-state coherence. Possible applications to magnetometery, atomic clocks, and frequency chains are discussed.

Physical Review A•Jun 14, 2005•62 citations
The hyperfine splitting of the ground state and the lowest electronic component of the (1)D(2) excited state have been measured for Pr(3+) in YAG. We show that a particularly simple and powerful technique is the production of sublevel coherence by short-pulse (impact) excitation, which is detected by coherent forward scattering of a weak probe beam and Fourier transformation of the resulting quantum-beat signal. This yielded excited-state splittings of 6.49 and 8.29 MHz. The ground state shows large pseudoquadrupole splittings of 33.4 and 41.6 MHz, which were obtained by optically detected nuclear quadrupole resonance.
The coherent dark resonance between the hyperfine levels F=1, m F =0 and F=2, m F =0 of the rubidium ground state has been observed experimentally with the light of a pulsed mode-locked diode laser operating at the D1 transition frequency. The resonance occurs whenever the pulse repetition frequency matches an integer fraction of the rubidium 87 ground state hyperfine splitting of 6.8 GHz. Spectra have been taken by varying the pulse repetition frequency. Using cells with argon as a buffer gas a linewidth as narrow as 149 Hz was obtained. The rubidium ground state decoherence cross section for collisions with xenon atoms has been measured for the first time with this method using a pure isotope rubidium vapor cell and xenon as a buffer gas.
It was shown by Kocharovskaya and Khanin [Sov. Phys. JETP 63, 945 (1986)] that a comb of optical pulses can induce a ground-state atomic coherence and change the optical response of an atomic medium. In our experiment, we studied the propagation of a comb of optical pulses produced by a mode-locked diode laser in rubidium atomic vapor. Electromagnetically induced transparency (EIT) was observed when the pulse repetition rate is a subharmonic of the hyperfine splitting of the ground state. The width of the EIT resonance is determined by the relaxation rate of the ground-state coherence. Possible applications to magnetometery, atomic clocks, and frequency chains are discussed.