and a stationary state in atoms [2], ions [3], semiconductor quantum dots [4], color defect centers [5] and even superconducting qubits [6]. A Bell measurement on two photons of each of two such states would then immediately establish entanglement between two stationary, possibly dissimilar states [7,8]. However, two dissimilar systems may emit light at vastly different wavelengths. It is not possible to entangle such systems with different transition energies via a Bell state measurement. One possible solution of this problem is to use a two-color pair of entangled photons, which are color-matched to these two different transitions as shown in Fig. 1a. The two-color photon pair source mediates entanglement between two dissimilar wavelengths. In the same manner, it can convert the wavelength of flying qubits as shown in Fig. 1b. This is especially helpful if entanglement should be established over long distances, e.g., via optical fibers in the telecom band. The key building block in these two applications is a source of non-degenerate entangled photons. Especially when working with systems whose wavelengths are hundreds of nanometers apart, such a source has to generate highly non-degenerate photons. In contrast to previous highly non-degenerate sources [9], our source introduces wavelength-insensitive components and is thus in principle widely tunable. This is another important requirement when working with a variety of different systems in hybrid systems, in particular with systems that may vary in time or from experiment to experiment.Up to now, the brightest and most practical sources of entangled photon pairs rely on spontaneous parametric down-conversion in nonlinear crystals [10]. With appropriate phase matching, two-color sources with photons at different wavelengths can be realized [9,11,12]. For subsequent fiber coupling, collinear down-conversion schemes are most convenient. Furthermore, the collinear alignment enables further integration and can be used in a monolithic design [12].
AbstractWe demonstrate a two-color entangled photon pair source which can be adapted easily to a wide range of wavelength combinations. A Fresnel rhomb as a geometrical quarter-wave plate and a versatile combination of compensation crystals are key components of the source. Entanglement of two photons at the Cs D1 line (894.3 nm) and at the telecom O-band (1313.1 nm) with a fidelity of F = 0.753 ± 0.021 is demonstrated, and improvements of the setup are discussed.