Dicke state

Dicke states are defined in a system of N spin-s particles as the simultaneous eigenstates of the angular momentum operators {\vec J}^2 and J_z by the equations : {\vec J}^2|j,j_z,\alpha\rangle = j(j+1)|j,j_z,\alpha\rangle and : J_z |j,j_z,\alpha\rangle = j_z|j,j_z,\alpha\rangle. Here, \alpha is a label used to distinguish several states orthogonal to each other, for which the two eigenvalues are the same. It is instructive to consider the s=1/2 case, namely an N-qubit system. For j=N/2, Dicke states are symmetric. In this case, we do not need the additional parameter \alpha, since for a given j_z, there is only a single simultaneous eigenstate of {\vec J}^2 and J_z. It is also common to use for the characterization of these states the quantity n=N/2-j_z. They can be written as : |D_n^{(N)}\rangle = \binom{N}{n}^{-1/2}\sum_{k} {\mathcal{P}}_{k}(|0\rangle^{\otimes(N-n)} \otimes |1\rangle^{\otimes n}), where n=0,1,...,N is the number of 1's, and the summation is over all distinct permutations. A W-state is given as : |W\rangle = \frac1{\sqrt{N}}(|1000...000\rangle+|0100...000\rangle+|0010...000\rangle+... +|0000...001\rangle) and it equals the Dicke state |D_1^{(N)}\rangle. The entanglement properties of symmetric Dicke states have been studied extensively. Symmetric Dicke states of N spin-s particles can easily be mapped to symmetric Dicke states of 2sN spin-1/2 particles. The case of j i.e., the case of non-symmetric Dicke states in multi-qubit systems is more complicated. In this case, the simultaneous eigenstates are denoted by |j,j_z,\alpha\rangle, and we need now the \alpha label to dinstinguish several eigenstates with the same eigenvalues orthogonal to each other. These states can also be obtained explicitly. == Fidelity ==

In an experiment, determining the fidelity with respect to pure quantum states is not an easy task in general. However, for states in the symmetric (bosonic) subspace, the necessary measurement effort increases only polynomially with the number of particles. For instance, for N qubits it is bounded from above by N^2/2+3N/2+1 local measurement settings, which is known from the theory of permutationally invariant quantum state tomography. It is also a valid bound for measuring the fidelity with respect to symmetric Dicke states. For the 4-qubit case, 7 local measurement settings is sufficient, while for the 6-qubit case 21 local measuement settings is sufficient. == Entanglement properties ==

When a Dicke states has been prepared in an experiment, it is important to verify that the state has been prepared with a good quality. Apart from obtaining the fidelity, a usual goal is to show that the quantum state was highly entangled. If for a quantum state \varrho the fidelity with respect to W-states : {\rm Tr}(\varrho|W\rangle\langle W|)> 1-1/N holds then the quantum state is genuine multipartite entangled. This means that all the particles are entangled with each other, and the quantum state cannot be put together with entangled quantum states of smaller units by trivial operations such as making a tensor product and mixing. Note that the bound is approaching 1 for a large N, which can make experiments with large systems difficult. For the symmetric Dicke state |D_{N/2}^{(N)}\rangle , if for the fidelity of a quantum state : {\rm Tr}(\varrho|D_{N/2}^{(N)}\rangle\langle D_{N/2}^{(N)}|)> \frac{1}{2} \frac{N}{N-1} holds then the quantum state is genuine multipartite entangled. Now the bound approaches 1/2 for large N, which makes experiments for detecting genuine multipartite entanglement feasible even for a large N. Unlike in the case of GHZ states, the entanglement of Dicke states can be detected by measuring collective observables. It is also possible to detect multipartite entanglement or entanglement depth of such states based on collective measurements. Finally, there are efficient methods to detect multipartite entanglement of noisey Dicke states based on their density matrix. == Metrological properties ==

For an N-qubit quantum state, : F_Q[\varrho,J_l]\le N^2 holds for l=x,y,z, where J_l are the components of the collective angular momentum : J_l=\frac 1 2 \sum_{n=1}^N \sigma_l^{(n)}, and \sigma_l are the Pauli spin matrices. Here, F_Q[\varrho,H] denotes the quantum Fisher information characterizing how well the state \varrho can be used to estimate the parameter \theta in the unitary dynamics : U=\exp(-iH\theta). For separable states the bound discovered by Pezzé and Smerzi : F_Q[\varrho,J_l]\le N holds, which is relevant for linear interferometers, a very large class of interferometers used in experiments. For the Dicke state |D_{N/2}^{(N)}\rangle : F_Q[\varrho,J_x]=F_Q[\varrho,J_y]=N(N+2)/2 holds, which corresponds to a quadratic scaling in the particle number, that is, a Heisenberg scaling. Such Dicke states also saturate the relation : F_Q[\varrho,J_x]+F_Q[\varrho,J_y]+F_Q[\varrho,J_z]\le N(N+2), which is valid for any quantum state. Greenberger–Horne–Zeilinger (GHZ) states also saturate this relation. == Experiments ==

W-states of three qubits have been created in photons. Symmetric Dicke states |D_{N/2}^{(N)}\rangle have been created in a four and a six-qubit photonic experiment in which genuine four- and six-particle entanglement, respectively, has been demonstrated. They have also been prepared in a Bose-Einstein condensate with thousands of atoms. Dicke states have also been used for quantum metrology in cold gases and photonic systems. In these experiments it has been demonstrated that the experimentally created Dicke states outperform separable states in metrology. Multipartite entanglement and the depth of entanglement has been detected in Dicke states in an ensemble of cold atoms. Bipartite entanglement and Einstein–Podolsky–Rosen (EPR) steering has been detected in Dicke states of an ensemble of thousands of cold atoms. == See also ==