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note
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-1 for the neon form factor) when we interpolate on these data in order to obtain the predictions given in Table II. Even with this procedure, elastic cross sections based on the tabulation of Hubbell et al. [14] still have limited precision (at the ≈ 1 % level) for large momentum transfers, reflecting the precision of the published data in Ref. [14]. Thus the deviations of these predictions (Table II, column 5) from the "best" predictions (Table II. column 3) for 59.54 keV at finite angle (corresponding to large momentum transfers) do not correspond exactly to the appropriate Rayleigh corrections given in Sec. III.
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28
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0000569003
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In photoeffect angular distributions and cross sections, even when quadrupole effects matter, quadrupole correlations have not been found to be important, except perhaps at threshold [M.Ya. Amusia, A.S. Baltenkov, Z. Felfli, and A.Z. Msezane, Phys. Rev. A 59, R2544 (1999); W.R. Johnson, A. Derevianko, K.T. Cheng, V.K. Dolmatov, and S.T. Manson, ibid. 59, 3609 (1999)], which suggests, in consideration of the optical theorem, a similar situation for Rayleigh scattering.
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Msezane, A.Z.4
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29
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0001572096
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In photoeffect angular distributions and cross sections, even when quadrupole effects matter, quadrupole correlations have not been found to be important, except perhaps at threshold [M.Ya. Amusia, A.S. Baltenkov, Z. Felfli, and A.Z. Msezane, Phys. Rev. A 59, R2544 (1999); W.R. Johnson, A. Derevianko, K.T. Cheng, V.K. Dolmatov, and S.T. Manson, ibid. 59, 3609 (1999)], which suggests, in consideration of the optical theorem, a similar situation for Rayleigh scattering.
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Johnson, W.R.1
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