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arXiv:1712.07613

Controlling a d-level atom in a cavity

Hofmann, Thomas, Michael Keyl

Published Dec 20, 2017• 6 citations
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Abstract

In this paper we study controllability of a $d$-level atom interacting with the electromagnetic field in a cavity. The system is modelled by an ordered graph $Γ$. The vertices of $Γ$ describe the energy levels and the edges allowed transitions. To each edge of $Γ$ we associate a harmonic oscillator representing one mode of the electromagnetic field. The dynamics of the system (drift) is given by a natural generalization of the Jaynes-Cummings Hamiltonian. If we add in addition sufficient control over the atom, the overall system (atom and em-field) becomes strongly controllable, i.e. each unitary on the system Hilbert space can be approximated with arbitrary precision in the strong topology by control unitaries. A key role in the proof is played by a topological *-algebra which is (roughly speaking) a representation of the path algebra of $Γ$. It contains crucial structural information about the control problem, and is therefore an important tool for the implementation of control tasks like preparing a particular state from the ground state. This is demonstrated by a detailed discussion of different versions of three-level systems.

DOI
10.48550/arxiv.1712.07613

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In this paper we study controllability of a ddd-level atom interacting with the electromagnetic field in a cavity. The system is modelled by an ordered graph ΓΓΓ. The vertices of ΓΓΓ describe the energy levels and the edges allowed transitions. To each edge of ΓΓΓ we associate a harmonic oscillator representing one mode of the electromagnetic field. The dynamics of the system (drift) is given by a natural generalization of the Jaynes-Cummings Hamiltonian. If we add in addition sufficient control over the atom, the overall system (atom and em-field) becomes strongly controllable, i.e. each unitary on the system Hilbert space can be approximated with arbitrary precision in the strong topology by control unitaries. A key role in the proof is played by a topological *-algebra which is (roughly speaking) a representation of the path algebra of ΓΓΓ. It contains crucial structural information about the control problem, and is therefore an important tool for the implementation of control tasks like preparing a particular state from the ground state. This is demonstrated by a detailed discussion of different versions of three-level systems.
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