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Zhou, X. et al. Field locked to a fock state by quantum feedback with single photon corrections.
Here | { N s, i }, t 〉 is a Fock state in which N s, i particles of species s occupy mode i.
Therefore, we prepare an ensemble of N two-level atoms initially in ground state, and a single mode of the radiation field is excited in a 'Fock' state (so called one-photon state).
Therefore, the results suggest that a Fock state photon will evolve into a different Fock state of (|n_{0} is {mathcal{P}}_{n}^{{left( {n_{0} } right)}} left( t right)).
Owing toits controllability [11 14], a CPB has been proposed to couple to the NR to drive an NR into asuperposition of spatially separated states and probe the decay of the NR [15], to prepare the NR in a Fock state and perform a quantum non-demolitionmeasurement of the Fock state [16], and to cool the NR to its ground state [17].
In modern physics notation, the quantum state of the electromagnetic field is written as a Fock state, a tensor product of the states for each electromagnetic mode :|n_{k_0}\rangle\otimes|n_{k_1}\rangle\otimes\dots\otimes|n_{k_n}\rangle\dots where |n_{k_i}\rangle represents the state in which \, n_{k_i} photons are in the mode k_i.
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Researchers can precisely tune the quantum state of that light by, for instance, putting it in a so-called Fock state that consists of a definite number of photons but lacks the usual properties of a classical light wave.
In this work, a chain of N identical two-level atoms coupled with a quantized electromagnetic field, initially prepared via a single-photon Fock state, is investigated.
Thus, in this work, we investigated a chain of N identical two-level long distanced atoms prepared 'via a single-photon Fock state'.
In the present paper, a system (chain) of N identical two-level non-interacting atoms, prepared 'via a single-photon Fock state' in the one- or two-mode resonator, is investigated.
Discussion of a lossy MZI for Fock state inputs is also discussed in previous works [15, 16].
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