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Volumn 60, Issue 22, 1999, Pages 15074-15083

Holographies and exafs in quantum electrodynamics

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EID: 0000687488     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.60.15074     Document Type: Article
Times cited : (25)

References (24)
  • 2
    • 0000952945 scopus 로고
    • AIP T. Attwood and J. Boker
    • A. Szöke, in Short Wavelength Coherent Radiation: Generation and Applications, edited by T. Attwood and J. Boker, AIP Conf. Proc. No 147 (AIP, New York, 1986), p. 361.
    • (1986) AIP Conf. Proc. , pp. 361
    • Szöke, A.1
  • 15
    • 85037879406 scopus 로고    scopus 로고
    • V. B. Berestetskii, E. M. Lifshitz, and L. P. Pitaevskii, in Quantum Electrodynamics, edited by L. D. Landau and E. M. Lifshitz, Vol. 4 of Course of Theoretical Physics, 2nd ed. (Pergaman, Oxford, 1982).
    • V. B. Berestetskii, E. M. Lifshitz, and L. P. Pitaevskii, in Quantum Electrodynamics, edited by L. D. Landau and E. M. Lifshitz, Vol. 4 of Course of Theoretical Physics, 2nd ed. (Pergaman, Oxford, 1982).
  • 16
    • 0003570366 scopus 로고
    • Benjamin/Cummings, Menlo Park S. F. Tuan
    • J. J. Sakurai, in Modern Quantum Mechanics, edited by S. F. Tuan (Benjamin/Cummings, Menlo Park, 1985).
    • (1985) Modern Quantum Mechanics
    • Sakurai, J.J.1
  • 17
    • 85037892051 scopus 로고    scopus 로고
    • 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.
    • 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.
  • 18
    • 85037908962 scopus 로고    scopus 로고
    • International Tables for Crystallography, edited by A. J. C. Wilson (Kluwer Academic, Dordrecht, 1992), Vol. C.
    • International Tables for Crystallography, edited by A. J. C. Wilson (Kluwer Academic, Dordrecht, 1992), Vol. C.
  • 21
    • 85037891997 scopus 로고    scopus 로고
    • 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.
    • 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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