Abstract

We have investigated theoretically and experimentally a method for preparing Dicke states in trapped atomic ions. We consider a linear chain of NN ion qubits that is prepared in a particular Fock state of motion, ∣m>|m>. The mm phonons are removed by applying a laser pulse globally to the NN qubits, and converting the motional excitation to mm flipped spins. The global nature of this pulse ensures that the mm flipped spins are shared by all the target ions in a state that is a close approximation to the Dicke state $\D{N}{m}$. We calculate numerically the fidelity limits of the protocol and find small deviations from the ideal state for m=1m = 1 and m=2m = 2. We have demonstrated the basic features of this protocol by preparing the state $\D{2}{1}$ in two 25^{25}Mg+^+ target ions trapped simultaneously with an 27^{27}Al+^+ ancillary ion.

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