Abstract

In this letter we present a protocol to engineer interactions confined to subspaces of the Fock space in trapped ions: we show how to engineer upper-, lower-bounded and sliced Jaynes-Cummings (JC) and anti-Jaynes-Cummings (AJC) Hamiltonians. The upper-bounded (lower-bounded) interaction acting upon Fock subspaces ranging from ∣0⟩\left\vert 0\right\rangle to ∣M⟩\left\vert M\right\rangle (∣N⟩\left\vert N\right\rangle to ∞\ \infty), and the sliced one confined to Fock subspace ranging from ∣M⟩\left\vert M\right\rangle to ∣N⟩\left\vert N\right\rangle , whatever M<NM<N. Whereas the upper-bounded JC or AJC interactions is shown to drive any initial state to a steady Fock state ∣N⟩\left\vert N\right\rangle , the sliced one is shown to produce steady superpositions of Fock states confined to the sliced subspace {∣N⟩,∣N+1⟩}\left\{ \left\vert N\right\rangle \text{,}\left\vert N+1\right\rangle \right\} .

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