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Furthermore, when r1 and r2 coincide, spectral degree of coherence has the value |µ(r, r, ω)| = 1. The spectral degree of coherence in the context of scalar fields, describes under suitable conditions, the visibility of intensity fringes in the classical Young’s two-pinhole experiment [24]. The generalization of the spectral degree of coherence to electromagnetic fields has been proposed, akin to the scalar case, by considering the visibility of interference fringes in Young’s experiment [76, 77].

After internal relaxation, characterized by a (non-radiative) vibrational relaxation rate K, the donor resides in the excited state |e1 . The excited donor then couples by dipole-dipole interaction to the excited level |v2 of the acceptor molecule. The dipole-dipole coupling factor J12 for two molecules has the form [166] ↔ J12 = −µ2 · G (r2 , r1 , ω) · µ1 , (112) where µ1 and µ2 are the dipole transition moments associated with the transitions between the levels |e1 and |g1 , and |v2 and |g2 , of the two molecules located at r1 and r2 , respectively.

J. Greffet, “Near-field effects in spatial coherence of thermal sources”, Phys. Rev. Lett. 82, 1660–1663 (1999). [20] C. Henkel, K. Joulain, R. -J. Greffet, “Spatial coherence of thermal near fields”, Opt. Commun. 186, 57–67 (2000). [21] A. V. Shchegrov, K. Joulain, R. -J. Greffet, “Near-field spectral effects due to electromagnetic surface excitations”, Phys. Rev. Lett. 85, 1548–1551 (2000). [22] T. Set¨al¨a, M. Kaivola, and A. T. Friberg, “Degree of polarization in near fields of thermal sources: effects of surface waves”, Phys.

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