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Laser Physics

Storage and reconstruction of quantum information using exciton resonance in a solid

A. D. Gazazyan, E. A. Gazazyan

Published Dec 1, 2006• 5 citations
Publisher

Abstract

The methods for storage and reconstruction of quantum information in a crystal with impurity ∧ atoms are studied in the case when the upper state is located in the exciton band. The upper level of the impurity atom forms a Fano resonant state similar to the autoionization atomic state due to the configuration interaction with the continuum of the exciton band. The slowing of light pulses is realized in the presence of a control field, so that the group velocity appears much lower than the velocity of light in vacuum. The processes are considered in the adiabatic limit of the field activation. The possibility for the storage and reconstruction of a quantum pulse is studied in the case of the instantaneous on-off switching of the control field. It is demonstrated that the shape and quantum state of the light pulse are preserved in the case of its propagation and reconstruction. The polariton states are obtained and their properties are studied for the case of transitions through the exciton resonance.

DOI
10.1134/s1054660x06120164

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The methods for storage and reconstruction of quantum information in a crystal with impurity ∧ atoms are studied in the case when the upper state is located in the exciton band. The upper level of the impurity atom forms a Fano resonant state similar to the autoionization atomic state due to the configuration interaction with the continuum of the exciton band. The slowing of light pulses is realized in the presence of a control field, so that the group velocity appears much lower than the velocity of light in vacuum. The processes are considered in the adiabatic limit of the field activation. The possibility for the storage and reconstruction of a quantum pulse is studied in the case of the instantaneous on-off switching of the control field. It is demonstrated that the shape and quantum state of the light pulse are preserved in the case of its propagation and reconstruction. The polariton states are obtained and their properties are studied for the case of transitions through the exciton resonance.
We study the possibility to store and retrieve quantum information with use of “dark” and ”bright” polaritons in solids with excitonic resonances. In a crystal with Λ-type impurity atoms the upper level lying in the excitonic band of the crystal forms a Fano-type resonant state via configuration interaction with the continuum of crystal’s excitonic band. Polariton states are introduced in case of transitions through excitonic resonance and the properties of these states are studied. We also investigate propagation of dark polariton and show that its shape and quantum state are preserved during propagation. Limiting cases of adiabatic and non-adiabatic turning-on the fields are analyzed in detail.
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.
Atomic coherence is the interaction process between light and atoms, that is one or more coherent fields couple the different atomic states and cause the quantum interference between the different transition channels. Atomic coherence has led to many interesting and unexpected consequences, such as the Hanle effects, electromagnetically induced transparency (EIT), coherence population trapping (CPT), stimulated Raman adiabatic passage (STIRAP), spontaneous emission control, resonant enhancement of optical nonlinearity, slow and superluminal light propagation, quantum light storage, etc. In which, light storage based on atomic coherence plays an important role in the coherent control of light pulse information. In this chapter, we present some previous works on atomic coherence and optical storage. Firstly, we present the storage and recovery of light pulse based on F-STIRAP, which is fundamentally different from the conventional EIT-based process. Secondly, we present the applications of light storage based on EIT in a Pr3+:Y2SiO5 crystal, which includes the erasure of stored optical information, all-optical routing by light storage, and the coherent control of double light pulses. At last, we propose theoretically and demonstrate experimentally a method to control the atomic coherence by a STIRAP or F-STIRAP process.
We extend the theory to describe the quantum light memory in type atoms with considering (lower levels coherency decay rate) and detuning for the probe and the control fields. We obtain that with considering these parameters, group velocity of the probe pulse does not tend to zero by turning off the control field. We show that there are considerable decay for the probe pulse and the stored information. Also, it is inferred that the light field does not tend to zero when the control field is turned off. In addition, we obtain that in the off-resonance case there is considerable distortion of the output light pulse (with fast oscillations) that destroys the stored information. Then we present the limitations on detuning (bandwidths) of the probe and the control fields to achieve negligible distortion. We finally present the numerical calculations and compare them with obtained analytical results.
Coherent interactions of laser light with atomic ensembles allow one to modify dispersive properties of a medium and lead to new optical phenomena. Studies of the controlled light propagation and storing in such media have recently become a dynamically developing field of research motivated both by the fundamental character of the processes and by potential applications. This article briefly reviews basic theoretical approach to the dynamics of the propagation of laser pulses in optically modified media. The method and the physical processes are discussed that allow one to slow down the group velocity of laser pulse to zero (stopping of light), to transfer the state of a light pulse to atomic coherences and to restore the pulse. The interpretation of these phenomena in the formalism of dark-state polaritons is presented. Examples of possible coherent manipulations on a stored light are also discussed.