Abstract

The authors of the Comment [Opt. Lett. 34, 1001 (2009) ] do not mention that no claim was made in the orginal letter that the cross-spectral density matrix of polarized light must be of a factorized form.

© 2009 Optical Society of America

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References

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  1. J. Tervo and J. Turunen, Opt. Lett. 34, 1001 (2009).
    [CrossRef] [PubMed]
  2. E. Wolf, Opt. Lett. 33, 642 (2008).
    [CrossRef] [PubMed]
  3. L. Mandel and E. Wolf, Optical Coherence and Quantum Optics (Cambridge U. Press, 1995).
  4. E. Wolf, Introduction to the Theory of Coherence and Polarization of Light (Cambridge U. Press, 2007).
  5. M. Lahiri and E. Wolf, Opt. Lett. 34, 551 (2009).
    [CrossRef]

2009 (2)

2008 (1)

Lahiri, M.

Mandel, L.

L. Mandel and E. Wolf, Optical Coherence and Quantum Optics (Cambridge U. Press, 1995).

Tervo, J.

Turunen, J.

Wolf, E.

M. Lahiri and E. Wolf, Opt. Lett. 34, 551 (2009).
[CrossRef]

E. Wolf, Opt. Lett. 33, 642 (2008).
[CrossRef] [PubMed]

L. Mandel and E. Wolf, Optical Coherence and Quantum Optics (Cambridge U. Press, 1995).

E. Wolf, Introduction to the Theory of Coherence and Polarization of Light (Cambridge U. Press, 2007).

Opt. Lett. (3)

Other (2)

L. Mandel and E. Wolf, Optical Coherence and Quantum Optics (Cambridge U. Press, 1995).

E. Wolf, Introduction to the Theory of Coherence and Polarization of Light (Cambridge U. Press, 2007).

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Equations (1)

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W ( p ) ( ρ 1 , ρ 2 , z ; ω ) = ( E x * ( ρ 1 , z ; ω ) E x ( ρ 2 , z ; ω ) E x * ( ρ 1 , z ; ω ) E y ( ρ 2 , z ; ω ) E y * ( ρ 1 , z ; ω ) E x ( ρ 2 , z ; ω ) E y * ( ρ 1 , z ; ω ) E y ( ρ 2 , z ; ω ) ) ,

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