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

Journal of Physics B Atomic Molecular and Optical Physics

Controlled release of stored pulses in a double-quantum-well structure

F. Carreño, M. A. Antón

Published Oct 26, 2009• 2 citations
Publisher

Abstract

We show that an asymmetric double-quantum-well structure can operate as an optical memory. The double quantum wells are modelled like an atomic ensemble of four-level atoms in the Λ–V-type configuration with vacuum-induced coherence arising from resonant tunnelling through the ultra-thin potential energy barrier between the wells. A weak quantum field connects the ground level with the two upper levels and an auxiliary classical control field connects the intermediate level with the upper levels. The quantum field can be mapped into two channels. One channel results from the adiabatic change of the control field which maps the incoming quantum field into the coherence of the two lower levels like in a Λ-type atomic ensemble. The other channel results from the mapping of the quantum field into a combination of coherences between the two upper levels and the ground level, and it is allowed by the adiabatic change of the upper level splitting via an external voltage. The possibility of releasing multiple pulses from the medium resulting from the existence of a non-evolving component of the two-channel memory is shown. A physical picture has been developed providing an explanation of the performance of the device.

DOI
10.1088/0953-4075/42/21/215508

Related papers

Controlled release of stored optical pulses in an atomic ensemble into two separate photonic channels

Bo Wang, Shujing Li, Haibin Wu +3 more

We report an experiment in which optical pulses stored in an atomic system can be controllably released into two different photonic channels. By controllably turning on the retrieve control pulses at either 795 or $780\phantom{\rule{0.3em}{0ex}}\mathrm{nm}$ to read the stored optical pulses in a four-level double $\ensuremath{\Lambda}$-type atomic medium, we can obtain the released probe pulse at 795 or $780\phantom{\rule{0.3em}{0ex}}\mathrm{nm}$, respectively. These readout pulses can be further separated spatially and directed into different optical propagation channels through a grating. Such controlled release of stored optical pulses may extend the capabilities of the quantum information storage technique, and can have applications in multichannel all-optical switching, all-optical routing, quantum information processing, and image storage systems.

Physical Review A•Oct 4, 2005•32 citations

An efficient quantum memory based on two-level atoms

Ivan Iakoupov, Anders Søndberg Sørensen

We propose a method to implement a quantum memory for light based on ensembles of two-level atoms. Our protocol is based on controlled reversible inhomogeneous broadening (CRIB), where an external field first dephases the atomic polarization and thereby stores an incoming light pulse into collective states of the atomic ensemble, and later a reversal of the applied field leads to a rephasing of the atomic polarization and a reemission of the light. As opposed to previous proposals for CRIB-based quantum memories, we propose only applying the broadening for a short period after most of the pulse has already been absorbed by the ensemble. We show that with this procedure there exist certain modes of the incoming light field that can be stored with an efficiency approaching 100% in the limit of high optical depth and long coherence time of the atoms. These results demonstrate that it is possible to operate an efficient quantum memory without any optical control fields.

arXiv:1301.0705•New Journal of Physics•Aug 13, 2013•17 citations

Quantum light memory in atomic ensemble, further development of the theory and its results

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 coherency decay rate and one and two-photon detunings from resonances in low intensity and adiabatic passage limit. We obtain that with considering these parameters, group velocity of probe (information) pulse and its amplitude does not tend to zero by turning off the control field, therefore there is no complete storage of light. Also, we obtain that there will be a considerable decay of probe pulse and stored information. We calculate the minimum velocity and decay rate for probe (information) 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.

•Feb 9, 2004•0 citations

Controlled light storage in a double lambda system

Andrzej Raczyński, Jarosław Zaremba, Instytut Fizyki Uniwersytet Miko̷laja Kopernika

The possibility is predicted that after light storing in a medium of four-level atoms it is possible to release a new pulse of a different frequency, the process being steered by another driving beam. It is also possible to store one pulse and to release two different ones, with their time separation and heights being controlled.

•Jan 24, 2002•23 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

Quantum memory and all-optical switching in positive charged quantum dots via Zeeman coherent oscillations

M. A. Antón, F. Carreño

Linear and nonlinear properties in an ensemble of single-hole spin InGaAs/GaAs quantum dots are theoretically studied. The application of a DC magnetic field in the semiconductor growth plane induces a Zeeman splitting of the hole levels which can be modeled like a four-level atom in the X -type configuration. All-optical and magneto-optical switching of a weak probe field are shown to be feasible in this system either by changing the Rabi frequency of an auxiliary control field or by changing the magnitude of the external magnetic field. We analyze the feasibility to store and release a weak pulse from the medium resulting from Zeeman coherent oscillations, thus the system is expected to be useful to develop a variable semiconductor optical buffer.

Journal of Optics•Sep 24, 2010•5 citations
We show that an asymmetric double-quantum-well structure can operate as an optical memory. The double quantum wells are modelled like an atomic ensemble of four-level atoms in the Λ–V-type configuration with vacuum-induced coherence arising from resonant tunnelling through the ultra-thin potential energy barrier between the wells. A weak quantum field connects the ground level with the two upper levels and an auxiliary classical control field connects the intermediate level with the upper levels. The quantum field can be mapped into two channels. One channel results from the adiabatic change of the control field which maps the incoming quantum field into the coherence of the two lower levels like in a Λ-type atomic ensemble. The other channel results from the mapping of the quantum field into a combination of coherences between the two upper levels and the ground level, and it is allowed by the adiabatic change of the upper level splitting via an external voltage. The possibility of releasing multiple pulses from the medium resulting from the existence of a non-evolving component of the two-channel memory is shown. A physical picture has been developed providing an explanation of the performance of the device.
We report an experiment in which optical pulses stored in an atomic system can be controllably released into two different photonic channels. By controllably turning on the retrieve control pulses at either 795 or 780nm780\phantom{\rule{0.3em}{0ex}}\mathrm{nm}780nm to read the stored optical pulses in a four-level double $\ensuremath{\Lambda}$-type atomic medium, we can obtain the released probe pulse at 795 or 780nm780\phantom{\rule{0.3em}{0ex}}\mathrm{nm}780nm, respectively. These readout pulses can be further separated spatially and directed into different optical propagation channels through a grating. Such controlled release of stored optical pulses may extend the capabilities of the quantum information storage technique, and can have applications in multichannel all-optical switching, all-optical routing, quantum information processing, and image storage systems.
We propose a method to implement a quantum memory for light based on ensembles of two-level atoms. Our protocol is based on controlled reversible inhomogeneous broadening (CRIB), where an external field first dephases the atomic polarization and thereby stores an incoming light pulse into collective states of the atomic ensemble, and later a reversal of the applied field leads to a rephasing of the atomic polarization and a reemission of the light. As opposed to previous proposals for CRIB-based quantum memories, we propose only applying the broadening for a short period after most of the pulse has already been absorbed by the ensemble. We show that with this procedure there exist certain modes of the incoming light field that can be stored with an efficiency approaching 100% in the limit of high optical depth and long coherence time of the atoms. These results demonstrate that it is possible to operate an efficient quantum memory without any optical control fields.
We extend the theory of quantum light memory in atomic ensemble of Lambda type atoms with considering lower levels coherency decay rate and one and two-photon detunings from resonances in low intensity and adiabatic passage limit. We obtain that with considering these parameters, group velocity of probe (information) pulse and its amplitude does not tend to zero by turning off the control field, therefore there is no complete storage of light. Also, we obtain that there will be a considerable decay of probe pulse and stored information. We calculate the minimum velocity and decay rate for probe (information) 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 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.
Linear and nonlinear properties in an ensemble of single-hole spin InGaAs/GaAs quantum dots are theoretically studied. The application of a DC magnetic field in the semiconductor growth plane induces a Zeeman splitting of the hole levels which can be modeled like a four-level atom in the X -type configuration. All-optical and magneto-optical switching of a weak probe field are shown to be feasible in this system either by changing the Rabi frequency of an auxiliary control field or by changing the magnitude of the external magnetic field. We analyze the feasibility to store and release a weak pulse from the medium resulting from Zeeman coherent oscillations, thus the system is expected to be useful to develop a variable semiconductor optical buffer.