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

Proceedings of SPIE, the International Society for Optical Engineering/Proceedings of SPIE

Influence of rapid relaxation on light storage

Gor Nikoghosyan, Gayane G. Grigoryan

Published May 2, 2006• 0 citations
Publisher

Abstract

By solving the self-consistent system of Maxwell and derithty matrix equations in the case when the relaxation time is much shorter than the pulse duration, we obtain an analytical solution for the probe pulse propagation. This solution allows one to analyze the process of the information storage not only qualitatively, but also quantitatively In particular, it explains the fact that in well-known experiments only fractions of pulses were stored The conditions for effective storage are obtained.

DOI
10.1117/12.682378

Related papers

Influence of relaxation on propagation, storage, and retrieving of light pulses in a medium with electromagnetically induced transparency

Gor Nikoghosyan, Gayane Grigoryan

By solving the self-consistent system of Maxwell and density-matrix equations in the case where the time of relaxations to the ground state is much shorter than the pulse duration we derive an analytical solution for the probe pulse propagation. We obtain an excellent consistency of our analytical solution with direct numerical integration. We investigate the asymptotic behavior of analytical solution and show that under certain conditions it passes to the well-known dark-state polariton propagation regime. We analyzed the dynamics of propagation and, in particular, explain the fact that in the well-known experiments only fractions of pulses were stored.

arXiv:quant-ph/0503209•Physical Review A•Oct 19, 2005•11 citations

Storage of intense optical pulses in solids

G. G. Grigoryan

Possibility to store optical information in media with fast relaxations is studied in case of arbitrary intensities of probe and control pulses. Analytical solution of the self-consistent system of equations for propagation and density matrix is obtained with allowance for the first non-stationary corrections. A new scheme of storage is proposed which allows an essential reduction of the optical length needed for storage.

Journal of Contemporary Physics (Armenian Academy of Sciences)•Apr 1, 2008•0 citations

Electromagnetically induced transparency: record, storage and recover of short pulses

A.V. Grigorievich, T.I. Vladimirovich

Summary form only given. In this report the propagation of a weak probe pulse in an optically dense medium in presence of strong coupling pulse, resonant to conjugated transition, is investigated. We consider the case when at the medium entrance both pulses have the identical shape, but duration of coupling pulse is greater than duration of probe pulse. The intensity of the probe pulse is considered much less than the intensity of the coupling one. The features of spatial and temporal evolution of the probe pulse and the atomic coherence are analyzed at different relations between pulse duration and relaxation time of the medium.

Quantum Electronics and Laser Science Conference•Jun 25, 2003•0 citations

Analysis of Quantum Light Memory in Atomic Systems (Final)

Hassan Kaatuzian, Ali Rostami, Ahmad Ajdarzadeh Oskouei

We extend the theory of quantum light memory in atomic ensemble of Lambda type atoms with considering lower levels coherence decay rate and one and two-photon detunings from resonances in low intensity and adiabatic passage limit. We obtain that with considering these parameters, that there will be a considerable decay of probe pulse and stored information; also, we obtain that the group velocity of probe (light) pulse and its amplitude does not tend to zero by turning off the control field. We propose a method to keep the probe pulse in small values in turn off time of control field and to reduce the loss of the stored probe pulse. In addition, we obtain that in the Off-resonance case there will be a considerable distortion of the output light pulse that causes in loss of the stored information, then we present limitations for detunings and therefore for bandwidths of practical lasers also limitations for maximum storage time to have negligible distortion of stored information. We finally present the numerical calculations and compare them with analytical results.

arXiv:quant-ph/0402057•Feb 9, 2004•0 citations

Short-length storage of intense optical pulses in solids by adiabatic passage

G. G. Grigoryan, Y. Pashayan-Leroy, Claude Leroy +1 more

We propose a scheme of storage of intense pulses that allows a significant reduction of the storage length with respect to standard schemes. This scheme is particularly adapted to store optical information in media with fast relaxations.

arXiv:0806.3723•Physical Review A•Jan 14, 2009•2 citations

Propagation and superposition of light pulses in a dye medium

S. L. Chin, Andrzej Zardecki

We have developed a self-consistent description, based on the semiclassical radiation theory of the propagation of a light pulse in a dye medium. The multilevel nature of the energy bands of a dye molecule and the solvent cage effect in a solution are taken into account. In the case of light pulses whose duration is much shorter than the solvent-solute relaxation time but much longer than the time of atomic phase memory, the latter being of the order of ${10}^{\ensuremath{-}12}$ sec for dyes, we solve the coupled system of equations for the field and the medium by the perturbation procedure. The hole-burning effect is incorporated into the solution in a natural manner. This is especially clear in the direct transition approximation where all the intermediate transitions are neglected. A recent idea of pulse superposition, consisting in storing the energy of a pulse in the form of population inversion followed by stimulated emission triggered by another pulse, is further discussed. Contrary to the orginal model developed by one of us (S.L.C.), we show that no cw pumping is required. The feasibility of the pulse superposition is supported by some experimental results obtained by sending a train of 10-psec pulses through a glycerine solution of oxazine 1 perchlorate.

Physical Review A•Apr 1, 1976•3 citations
By solving the self-consistent system of Maxwell and derithty matrix equations in the case when the relaxation time is much shorter than the pulse duration, we obtain an analytical solution for the probe pulse propagation. This solution allows one to analyze the process of the information storage not only qualitatively, but also quantitatively In particular, it explains the fact that in well-known experiments only fractions of pulses were stored The conditions for effective storage are obtained.
By solving the self-consistent system of Maxwell and density-matrix equations in the case where the time of relaxations to the ground state is much shorter than the pulse duration we derive an analytical solution for the probe pulse propagation. We obtain an excellent consistency of our analytical solution with direct numerical integration. We investigate the asymptotic behavior of analytical solution and show that under certain conditions it passes to the well-known dark-state polariton propagation regime. We analyzed the dynamics of propagation and, in particular, explain the fact that in the well-known experiments only fractions of pulses were stored.
Summary form only given. In this report the propagation of a weak probe pulse in an optically dense medium in presence of strong coupling pulse, resonant to conjugated transition, is investigated. We consider the case when at the medium entrance both pulses have the identical shape, but duration of coupling pulse is greater than duration of probe pulse. The intensity of the probe pulse is considered much less than the intensity of the coupling one. The features of spatial and temporal evolution of the probe pulse and the atomic coherence are analyzed at different relations between pulse duration and relaxation time of the medium.
We extend the theory of quantum light memory in atomic ensemble of Lambda type atoms with considering lower levels coherence decay rate and one and two-photon detunings from resonances in low intensity and adiabatic passage limit. We obtain that with considering these parameters, that there will be a considerable decay of probe pulse and stored information; also, we obtain that the group velocity of probe (light) pulse and its amplitude does not tend to zero by turning off the control field. We propose a method to keep the probe pulse in small values in turn off time of control field and to reduce the loss of the stored probe pulse. In addition, we obtain that in the Off-resonance case there will be a considerable distortion of the output light pulse that causes in loss of the stored information, then we present limitations for detunings and therefore for bandwidths of practical lasers also limitations for maximum storage time to have negligible distortion of stored information. We finally present the numerical calculations and compare them with analytical results.
We have developed a self-consistent description, based on the semiclassical radiation theory of the propagation of a light pulse in a dye medium. The multilevel nature of the energy bands of a dye molecule and the solvent cage effect in a solution are taken into account. In the case of light pulses whose duration is much shorter than the solvent-solute relaxation time but much longer than the time of atomic phase memory, the latter being of the order of ${10}^{\ensuremath{-}12}$ sec for dyes, we solve the coupled system of equations for the field and the medium by the perturbation procedure. The hole-burning effect is incorporated into the solution in a natural manner. This is especially clear in the direct transition approximation where all the intermediate transitions are neglected. A recent idea of pulse superposition, consisting in storing the energy of a pulse in the form of population inversion followed by stimulated emission triggered by another pulse, is further discussed. Contrary to the orginal model developed by one of us (S.L.C.), we show that no cw pumping is required. The feasibility of the pulse superposition is supported by some experimental results obtained by sending a train of 10-psec pulses through a glycerine solution of oxazine 1 perchlorate.