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1
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84926834018
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Field correlations within a completely incoherent primary spherical source
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J. T. Foley, W. H. Carter, and E. Wolf, "Field correlations within a completely incoherent primary spherical source," J. Opt. Soc. Am. A 3, 1090-1096 (1986).
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Foley, J.T.1
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2
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33847301232
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Field correlations within a Bessel-correlated spherical source
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J. T. Foley, K. Kim, and H. M. Nussenzveig, "Field correlations within a Bessel-correlated spherical source," J. Opt. Soc. Am. A 5, 1694-1708 (1988).
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Foley, J.T.1
Kim, K.2
Nussenzveig, H.M.3
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3
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33847319183
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Arbitrarily short coherence length within finite lossless source regions
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K. Blomstedt, T. Setälä, and A. T. Friberg, "Arbitrarily short coherence length within finite lossless source regions," Phys. Rev. E 75, 026610 (2007).
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Phys. Rev. e
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Blomstedt, K.1
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4
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18244424161
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Near-Field Effects in Spatial Coherence of Thermal Sources
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R. Carminati and J.-J. Greffet, "Near-field effects in spatial coherence of thermal sources," Phys. Rev. Lett. 82, 1660-1663 (1999). (Pubitemid 129577766)
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Carminati, R.1
Greffet, J.-J.2
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5
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0034250508
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Near-field spectral effects due to electromagnetic surface excitations
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A. V. Shchegrov, K. Joulain, R. Carminati, and J.-J. Greffet, "Near-field spectral effects due to electromagnetic surface excitations," Phys. Rev. Lett. 85, 1548-1551 (2000).
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Shchegrov, A.V.1
Joulain, K.2
Carminati, R.3
Greffet, J.-J.4
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6
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0037171215
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Degree of polarization in near fields of thermal sources: Effects of surface waves
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T. Setälä, M. Kaivola, and A. T. Friberg, "Degree of polarization in near fields of thermal sources: effects of surface waves," Phys. Rev. Lett. 88, 123902 (2002).
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Setälä, T.1
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8
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33748681925
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Degree of polarization for optical near fields
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T. Setälä, A. Shevchenko, M. Kaivola, and A. T. Friberg, "Degree of polarization for optical near fields," Phys. Rev. E 66, 016615 (2002).
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Setälä, T.1
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9
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33846249009
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Symmetry properties and polarization description for an arbitrary electromagnetic wavefield
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E. Wolf, ed. Elsevier
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C. Brosseau and A. Dogariu, "Symmetry properties and polarization description for an arbitrary electromagnetic wavefield," in Vol. 49 of Progress in Optics, E. Wolf, ed. (Elsevier, 2006), p. 315.
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Brosseau, C.1
Dogariu, A.2
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10
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38949091669
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Polarimetric characterization of light and media: Physical quantities involved in polarimetric phenomena
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J. J. Gil, "Polarimetric characterization of light and media: physical quantities involved in polarimetric phenomena," Eur. Phys. J. Appl. Phys. 40, 1-47 (2007).
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Gil, J.J.1
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11
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70350648349
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Degree of polarization in 3D optical fields generated from a partially polarized plane wave
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T. Setälä, K. Lindfors, and A. T. Friberg, "Degree of polarization in 3D optical fields generated from a partially polarized plane wave," Opt. Lett. 34, 3394-3396 (2009).
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Setälä, T.1
Lindfors, K.2
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14
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8744301961
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Theory of partially coherent electromagnetic fields in the space-frequency domain
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J. Tervo, T. Setälä, and A. T. Friberg, "Theory of partially coherent electromagnetic fields in the space-frequency domain," J. Opt. Soc. Am. A 21, 2205-2215 (2004).
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J. Opt. Soc. Am. A
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Tervo, J.1
Setälä, T.2
Friberg, A.T.3
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15
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1242331549
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Degree of coherence for electromagnetic fields
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J. Tervo, T. Setälä, and A. T. Friberg, "Degree of coherence for electromagnetic fields," Opt. Express 11, 1137-1143 (2003).
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Tervo, J.1
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16
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17544392525
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Complete electromagnetic coherence in the space-frequency domain
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T. Setälä, J. Tervo, and A. T. Friberg, "Complete electromagnetic coherence in the space-frequency domain," Opt. Lett. 29, 328-330 (2004).
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Setälä, T.1
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Friberg, A.T.3
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17
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33749610511
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Contrasts of Stokes parameters in Young's interference experiment and electromagnetic degree of coherence
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DOI 10.1364/OL.31.002669
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T. Setälä, J. Tervo, and A. T. Friberg, "Contrasts of Stokes parameters in Young's interference experiment and electromagnetic degree of coherence," Opt. Lett. 31, 2669-2671 (2006). (Pubitemid 44547092)
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Setala, T.1
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21
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84942362946
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The form of the Fresnel coefficient for p polarization given in Eq. (13) is valid only for an evanescent wave. For propagating waves, the factor √2ñ2γ2 + 1 is absent in the numerator. However, the factor follows directly from the boundary conditions, if the (complex) vector p̂2 related to the evanescent wave is normalized to unity. For example, in [19,20], the square-root factor is missing since in those treatments p̂2 is not normalized; more precisely, p̂*2 · p̂2 ≠ 1 but instead p̂2 · p̂2 = 1. The form of t p given in Eq. (13) preserves the physical meaning of the Fresnel coefficients as the ratio of the complex amplitudes on the opposite sides of the surface. See also [23].
-
The form of the Fresnel coefficient for p polarization given in Eq. (13) is valid only for an evanescent wave. For propagating waves, the factor √2ñ2γ2 + 1 is absent in the numerator. However, the factor follows directly from the boundary conditions, if the (complex) vector p̂2 related to the evanescent wave is normalized to unity. For example, in [19,20], the square-root factor is missing since in those treatments p̂2 is not normalized; more precisely, p̂*2 · p̂2 ≠ 1 but instead p̂2 · p̂2 = 1. The form of t p given in Eq. (13) preserves the physical meaning of the Fresnel coefficients as the ratio of the complex amplitudes on the opposite sides of the surface. See also [23].
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-
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22
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84975542054
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New Green-function formalism for surface optics
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J. E. Sipe, "New Green-function formalism for surface optics," J. Opt. Soc. Am. B 4, 481-489 (1987).
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Sipe, J.E.1
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23
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84942362947
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The p-polarized amplitude of the evanescent wave looks different from that given in [19,20], but it is the same. The variances in the appearance originate from the differences in the Fresnel coefficients for the p-polarized light. However, for the Fresnel coefficient in Eq. (13), the energy density of the p-polarized evanescent wave is of the intuitive form given in Eq. (22). For the evanescent wave of [19,20], the energy density contains an additional factor, wp = |tp|2|Ep| 2(2ñ2γ2 + 1. See also [21] above
-
The p-polarized amplitude of the evanescent wave looks different from that given in [19,20], but it is the same. The variances in the appearance originate from the differences in the Fresnel coefficients for the p-polarized light. However, for the Fresnel coefficient in Eq. (13), the energy density of the p-polarized evanescent wave is of the intuitive form given in Eq. (22). For the evanescent wave of [19,20], the energy density contains an additional factor, wp = |tp|2|Ep| 2(2ñ2γ2 + 1. See also [21] above.
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26
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34047127411
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Direct measurement of the evanescent-wave polarization state
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DOI 10.1364/JOSAB.24.000624
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L. Józefowski, J. Fiutowski, T. Kawalec, and H.-G. Rubahn, "Direct measurement of the evanescent-wave polarization state," J. Opt. Soc. Am. B 24, 624-628 (2007). (Pubitemid 46522928)
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, Issue.3
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Jozefowski, L.1
Fiutowski, J.2
Kawalec, T.3
Rubahn, H.-G.4
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