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In Eq. (10) of Ref. 8 the photon propagator in the Feynman gauge is used; on the other hand in Eq. (19) of Ref. 8 the three-dimensional transverse gauge is applied. In QED one has to use a unique gauge fixing condition throughout calculations. Because of the inconsistent choices of gauge fixing conditions, Eq. (10), Eq. (20), and the following equations in Ref. 8 should be modified by using a correct photon propagator in the three-dimensional transverse gauge.
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In Eq. (10) of Ref. 8 the photon propagator in the Feynman gauge is used; on the other hand in Eq. (19) of Ref. 8 the three-dimensional transverse gauge is applied. In QED one has to use a unique gauge fixing condition throughout calculations. Because of the inconsistent choices of gauge fixing conditions, Eq. (10), Eq. (20), and the following equations in Ref. 8 should be modified by using a correct photon propagator in the three-dimensional transverse gauge.
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18
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85037908962
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International Tables for Crystallography, edited by A. J. C. Wilson (Kluwer Academic, Dordrecht, 1992), Vol. C.
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International Tables for Crystallography, edited by A. J. C. Wilson (Kluwer Academic, Dordrecht, 1992), Vol. C.
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20
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0000730726
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21
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85037891997
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In equations for MEXH (reciprocal holography), Eqs. (15) and (16) in Ref. 20, the phase factor should read (Formula presented) because of the different wave direction in XFH and MEXH.
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In equations for MEXH (reciprocal holography), Eqs. (15) and (16) in Ref. 20, the phase factor should read (Formula presented) because of the different wave direction in XFH and MEXH.
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22
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0000866088
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P.M. Len, T. Gog, D. Novikov, R.A. Eisenhower, G. Materlik, and C.S. Fadley, Phys. Rev. B 56, 1529 (1997).
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