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

ZhETF Pisma Redaktsiiu

Two-quantum Anti-Stokes Processes in the Excitation of Dyes

Alina Veduță, M. D. Galanin, B. P. Kirsanov, Zoya A Chizhikova

Published Feb 1, 1970• 1 citation
OpenAlex

Related papers

Cooling of a dye solution by anti-stokes fluorescence

Christoph Zander, Karl Heinz Drexhage

European Quantum Electronics Conference (EQEC)•Jan 1, 1994•1 citation

Observation of anti-Stokes fluorescence in organic dye solutions

M. S. Chang, S. Elliott, T. Kenneth Gustafson +2 more

IEEE Journal of Quantum Electronics•Jun 1, 1972•21 citations

Nonlinear resonance effects in atomic gases—spontaneous and stimulated electronic Raman scattering of Na atoms excited resonantly atDlines by a tunable dye laser

Masanori Jyumonji, T. Kobayasi, Humio Inaba

A report is given of the first quantitative study of the spontaneous and stimulated electronic Raman scattering by a resonance doublet of the sodium atom excited resonantly at the D 1 and D 2 lines by a tunable dye laser. Theoretical and experimental analyses of the differential scattering cross section and polarization properties at the Stokes and anti-Stokes frequencies show that the observed scattering is due to a nearly resonant process involving the ground state 3 S 1/2 as the dominant intermediate state. The stimulated Stokes and anti-Stokes scattering lines, which are shifted from the D 1 and D 2 lines by an amount corresponding to the frequency separation between lowest-lying excited doublets 3 P 1/2 and 3 P 3/2 , are observed by exciting a sodium vapor cell with a passively mode-locked dye laser.

Soviet Journal of Quantum Electronics•Apr 30, 1976•2 citations

Electronic Raman Processes in Rydberg Matter of Cs: Circular Rydberg States in Cs and Cs+

Robert Svensson, Leif Holmlid

We report the first Raman study of the Rydberg matter form of Cs, using a ns pulsed dye laser. Electronic Raman anti-Stokes and mixed Stokes processes are detected in the range 290--920 nm after nonresonant excitation at 564 nm. No fluorescence is observed. The anti-Stokes transitions are from a high circular Rydberg state to a low circular state $8J$ in ${\mathrm{Cs}}^{+}$, close to $4F$ in Cs. The Stokes transitions are mixed in one more step with the laser radiation, and go from low circular states to Rydberg matter states. The transitions observed agree well with transitions in ${\mathrm{Cs}}^{+}$.

Physical Review Letters•Aug 30, 1999•41 citations

Anti-Stokes femtosecond photon echo in a polymer film

S. V. Petrushkin, В. В. Самарцев

An anti-Stokes model is proposed which explains the room-temperature blue shift of the echo-signal spectrum compared to the spectrum of exciting femtosecond pulses in a polymer film doped with dye molecules. The possibility of realising the anti-Stokes regime of coherent laser cooling of such films is analysed.

Quantum Electronics•Dec 31, 2007•3 citations

Quantum statistics of anti-stokes luminescence

P. F. González‐Díaz

Optics Communications•Sep 1, 1978•1 citation
A report is given of the first quantitative study of the spontaneous and stimulated electronic Raman scattering by a resonance doublet of the sodium atom excited resonantly at the D 1 and D 2 lines by a tunable dye laser. Theoretical and experimental analyses of the differential scattering cross section and polarization properties at the Stokes and anti-Stokes frequencies show that the observed scattering is due to a nearly resonant process involving the ground state 3 S 1/2 as the dominant intermediate state. The stimulated Stokes and anti-Stokes scattering lines, which are shifted from the D 1 and D 2 lines by an amount corresponding to the frequency separation between lowest-lying excited doublets 3 P 1/2 and 3 P 3/2 , are observed by exciting a sodium vapor cell with a passively mode-locked dye laser.
We report the first Raman study of the Rydberg matter form of Cs, using a ns pulsed dye laser. Electronic Raman anti-Stokes and mixed Stokes processes are detected in the range 290--920 nm after nonresonant excitation at 564 nm. No fluorescence is observed. The anti-Stokes transitions are from a high circular Rydberg state to a low circular state 8J8J8J in Cs+{\mathrm{Cs}}^{+}Cs+, close to 4F4F4F in Cs. The Stokes transitions are mixed in one more step with the laser radiation, and go from low circular states to Rydberg matter states. The transitions observed agree well with transitions in Cs+{\mathrm{Cs}}^{+}Cs+.