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T. Moriya, J. Phys. Soc. Jpn. 19, 681 (1964); Moriya's estimates were later corrected: R. E. Walstedt, V. Jaccarino, and N. Kaplan, J. Phys. Soc. Jpn. 21, 1843 (1966); M. B. Salamon, ibid. 21, 2746 (1966). These results are summarised in Table 1 of: B. G. Turrell, Hyperfine Interact. 7, 429 (1980).
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T. Moriya, J. Phys. Soc. Jpn. 19, 681 (1964); Moriya's estimates were later corrected: R. E. Walstedt, V. Jaccarino, and N. Kaplan, J. Phys. Soc. Jpn. 21, 1843 (1966); M. B. Salamon, ibid. 21, 2746 (1966). These results are summarised in Table 1 of: B. G. Turrell, Hyperfine Interact. 7, 429 (1980).
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We know of another instance where a link was reported between relaxation in zero field and a layered structure: N. A. Lesnik and V. O. Golub, Int. J. Mod. Phys. B 7, 511 (1993). However, we did not observe any systematic dependance of SLR on the layer thickness. A dependence of SLR on nuclear spin waves was demonstrated: G. Seewald, E. Hagh, and H. Zech, Phys. Rev. Lett. 78, 5002 (1997).
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We know of another instance where a link was reported between relaxation in zero field and a layered structure: N. A. Lesnik and V. O. Golub, Int. J. Mod. Phys. B 7, 511 (1993). However, we did not observe any systematic dependance of SLR on the layer thickness. A dependence of SLR on nuclear spin waves was demonstrated: G. Seewald, E. Hagh, and H. Zech, Phys. Rev. Lett. 78, 5002 (1997).
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Therefore the arguments developed in pp. 257-260 of Ref. 20 apply. The mean value for α delined in Eq. (55) of Abragam's book is (1+1/2), obtained with m = 1/2
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2, as expected, see equations (5.372) in Slichter's book
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2, as expected, see equations (5.372) in Slichter's book.
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