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

Журнал технической физики

Resonant upconversion of light at wavelength lambda = 1.06 micron in rubidium vapor

V. A. Kiyashko, A. K. Popov, V. P. Timofeev, G. V. Yurov

Published Nov 1, 1982• 0 citations
OpenAlex

Related papers

Resonant upconversion of ?=1.06 ?m radiation in rubidium vapors

V. A. Kiyashko, A. K. Popov, V. P. Timofeev +1 more

Applied Physics B•Mar 1, 1983•3 citations

The conversion of 1.06 micron radiation into the 420-nm range in rubidium vapor

Vasily G. Arkhipkin, A. K. Popov, V. P. Timofeev

Pisma v Zhurnal Tekhnischeskoi Fiziki•Feb 1, 1978•0 citations

Upconversion of λ=3.39 μm He-Ne laser radiation in two-photon resonantly pumped Na vapor

Vasily G. Arkhipkin, A. K. Popov, V. P. Timofeev

Applied Physics A•Jun 1, 1978•0 citations

Intensity correlation in frequency upconversion via four-wave mixing in rubidium vapor

Yong Sup Ihn, Kwang-Kyoon Park, Yosep Kim +2 more

We report a study on the transfer of intensity correlation properties in frequency upconversion via four-wave mixing (FWM) in rubidium (Rb) vapor. The 5S1/2−5P3/2−5D5/2 two-photon transition in Rb85 leads to collimated blue light (CBL) generation at 420 nm by absorbing two input photons of wavelengths 780 nm and 776 nm. The g(2)(τ) intensity correlation measurement of the CBL field reveals that the intensity correlations of the input fields are transferred to the CBL field due to strong atomic coherence in the FWM loop. We also demonstrate that the measured values of g(2)(τ) of the CBL field are reduced by the effect of Doppler broadening of Rb vapor.

Journal of the Optical Society of America B•Oct 13, 2017•9 citations

Unusual resonance effect of flourescence emitting from sinters of rare-earth-oxide Er2O3 and some inorganic oxides

Zhengwei Liu, Jian Liu, Zhezhao Zeng

We report for the first time that energy upconversion occurs when the same material was excited by monochrome light of different wavelength. The TTQLL (Three Times Quantum Liquid Law) Fermi Resonance Fluorescence Law advanced by the author in reference 1 is further proved, that is, the peak value of the excited fluorescence posses the following relationships with the wavelength of the excitation light: (lambda) 0/4, (lambda) 0/3, (lambda) 0/2, 2(lambda) 0/3, 3(lambda) 0/4, (lambda) 0, 5(lambda) 0/4, 4(lambda) 0/3, 3(lambda) 0/2, 2(lambda) 0, 3(lambda) 0. We also further discussed the radiation mechanism of this fluorescence and provided a theory model.

Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE•Oct 3, 1996•0 citations

Up-conversion of 780 nm or 795 nm laser radiation to 420 nm in rubidium atomic vapor

Armen D. Sargsyan, Anahit L. Gogyan, David G. Sarkisyan

Spectrochimica Acta Part B Atomic Spectroscopy•Jul 29, 2025•13 citations
We report a study on the transfer of intensity correlation properties in frequency upconversion via four-wave mixing (FWM) in rubidium (Rb) vapor. The 5S1/2−5P3/2−5D5/2 two-photon transition in Rb85 leads to collimated blue light (CBL) generation at 420 nm by absorbing two input photons of wavelengths 780 nm and 776 nm. The g(2)(τ) intensity correlation measurement of the CBL field reveals that the intensity correlations of the input fields are transferred to the CBL field due to strong atomic coherence in the FWM loop. We also demonstrate that the measured values of g(2)(τ) of the CBL field are reduced by the effect of Doppler broadening of Rb vapor.
We report for the first time that energy upconversion occurs when the same material was excited by monochrome light of different wavelength. The TTQLL (Three Times Quantum Liquid Law) Fermi Resonance Fluorescence Law advanced by the author in reference 1 is further proved, that is, the peak value of the excited fluorescence posses the following relationships with the wavelength of the excitation light: (lambda) 0/4, (lambda) 0/3, (lambda) 0/2, 2(lambda) 0/3, 3(lambda) 0/4, (lambda) 0, 5(lambda) 0/4, 4(lambda) 0/3, 3(lambda) 0/2, 2(lambda) 0, 3(lambda) 0. We also further discussed the radiation mechanism of this fluorescence and provided a theory model.