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Chinese Optics Letters

Preparing of coherent superposition state in serial multi-∧-type system by stimulated Raman adiabatic passage

李奇芳, 旷冶

Published Jan 1, 2008• 0 citations
OpenAlex

Abstract

A scheme for creating an arbitrary coherent superposition of two atomic states in serial multi-(?)-type system is proposed.This technique with the application of a control field is based on the existence of two degenerate dark states and their interaction.The mixing of the dark states can be controlled by changing the relative delay time of the control pulse.One can get any desired superposition by changing the delay time of the control pulse.

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•Jan 1, 2005•0 citations
A scheme for creating an arbitrary coherent superposition of two atomic states in serial multi-(?)-type system is proposed.This technique with the application of a control field is based on the existence of two degenerate dark states and their interaction.The mixing of the dark states can be controlled by changing the relative delay time of the control pulse.One can get any desired superposition by changing the delay time of the control pulse.
We propose a scheme for creating coherent atomic superposition states via the technique of stimulated Raman adiabatic passage (STIRAP) in a Λ-type system where final states are composed of manifold of levels and the intermediate levels could be more than one level. If the pump pulses and Stokes pulses are kept in the same order of ordinary STIRAP, through the control the delay time between the Stokes pulses and pump pulse, we could create arbitrary superposition states in the manifold of levels.
We propose a scheme for creating atomic coherent superposition states via the technique of stimulated Raman adiabatic passage in a $\ensuremath{\Lambda}$-type system where the final state has twofold levels. With the application of a control field, it is found that the presence of double dark states leads to two arbitrary coherent superposition states with equal amplitude but inverse relative phases, even though the condition of multiphoton resonance is not met. In particular, two orthogonal maximal coherent superposition states are created when the control field is resonant with the transition of the twofold levels. This scheme can also be extended to manifold $\ensuremath{\Lambda}$-type systems.
We propose a scheme for creating atomic coherent superpositions via stimulated Raman adiabatic passage in a Lambda-type system where the final state has twofold levels. In the employ of a control field, the presence of double dark states leads to two arbitrary coherent superposition states with equal amplitude but inverse relative phase without the condition of multi-photon resonance. In particular, two orthogonal maximal coherent superposition states are created when the control field is resonant with the transition of the twofold levels. This scheme can also be extended to manifold Lambda-type systems.
A technique for creation of coherent superposition state of initial populated state and final state in serial multi-Λ system is proposed.It is based on an extension of the technique of fractional stimulated Raman adiabatic passage(f-STIRAP).But unlike the f-STIRAP,a new pulse sequence has been proposed,in which each Stoke laser precedes the corresponding pump laser by τ,and the first of Stokes pulses and the last of pump pulses should vanish simultaneously after all the intermediate pulses,which vanish simultaneously too.Furthermore,we provide numerical simulation of the robustness against variations in the pulse delay,and the detuning.In order to create desired superposition state,we must not only keep two-photon resonance,but also keep single-photon resonance.
Using the technique of stimulated Raman adiabatic passage, we propose schemes for creating arbi- trary coherent superposition states of atoms in four-level systems: a A-type system with twofold final states and a four-level ladder system. With the use of a control field, arbitrary coherent superposition states are created without the condition of multiphoton resonance. Suitable manipulation of detunings and the control field can create either a single state or any superposition states desired. (c) 2005 Pleiades Publishing, Inc.