We present a physical setup with which it is possible to produce arbitrary symmetric long-lived multiqubit entangled states in the internal ground levels of photon emitters, including the paradigmatic GHZ and W states. In the case of three emitters, where each tripartite entangled state belongs to one of two well-defined entanglement classes, we prove a one-to-one correspondence between welldefined sets of experimental parameters, i.e., locally tunable polarizer orientations, and multiqubit entanglement classes inside the symmetric subspace.PACS numbers: 42.50. Ex, 03.65.Ud, 03.67.Bg, 42.50.Dv Entanglement is a distinctive property of quantum physics associated with the nonseparable character of multipartite quantum systems. For the case of two-qubit systems, entanglement is well understood and can be precisely quantified [1]. Apart from the trivial disentangled case, three qubits possess two genuine tripartite inequivalent entanglement classes [2,3]. Efforts have been done recently towards higher number of qubits [4,5,6], including an inductive method [7], though so far no comprehensive and scalable classification has been developed. In this letter, we introduce a physical setup consisting of N emitters, incoherently radiating single photons that may be absorbed remotely by detectors equipped with polarizers and producing long-lived multiqubit entangled states among the emitters. We show that it is possible to associate well-defined sets of locally tuned polarizer orientations with multiqubit entanglement classes, allowing their monitoring in an operational manner. Hereby, multipath quantum interferences, associated with qubit permutation symmetry, play a key role in explaining the underlying physics.We consider a chain of N equally separated single photon emitters, say trapped neutral atoms, trapped ions, quantum dots, or any other equivalent physical system with access to similar behaviour. Each emitter defines a three-level Λ system, where |e denotes the excited state and the two long-lived sublevels, |+ and |− , define a qubit. We assume that the transitions between the excited state and the two lower sublevels have an equal wavenumber and dipole moment, and that they are circularly polarized, σ + and σ − , respectively. Figure 1 exemplifies the N -emitter case discussed throughout this paper. All emitters are initially excited and we will study the cases in which all spontaneously emitted photons are detected by N detectors located in the far-field re- gion, each of them being equipped with a polarization filter in front. The far-field detection ensures the erasure of which-way information of the arriving photons, and the polarizers allow the generation of quantum superpositions of the lower atomic states when considering arbitrary polarizations. As a consequence each photodetection event projects the emitters onto linear combinations of the long-lived states |+ and |− [8]. This results at the end in a coherent superposition between the qubit states |±, . . . , ± . The indeterminacy of which detector