By Lavekar, G.S. and Menon, T.V. and Central Council for Research in Ayurveda and Siddha (India)
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16. Ni, polycrystalline, annealed for 2 h at 800 “C in Ar, furnace-cooled. 001 wt% S. Reversible part of the magnetic flux density change LIB, during sinusoidal stress cycling at room temperature as a 0 [Ref. p. 72 2 1 3 Id/m 4 H- function of applied magnetic field strength H. Parameteris the stressamplitude a, applied parallel to the magnetic field [9lRl]. a compression cycle, b tension cycle. 7 Magnetic moments, Compton profiles SeeLB III/I9A, p. 52-57 For a comparison of theoretical and experimental values of the spin and orbital magnetic moments of bee Fe, fee Co and fee Ni see Tables 1 and 3.
J. Phys. : Phys. Rev. : Solid StateCommun. : J. Phys. : Phys. Rev. : J. Phys. : Zh. Tekh. Fiz. 55 (1985) 1624; Sov. Phys. Tech. Phys. (Engl. : Phys. Rev. : Phys. Rev. : J. Phys. : Europhys. Lett. , in: Landolt-Bornstein, New Series, Vol. ), Berlin, Heidelberg, New York: Springer (1986) p. : Hyperfine Interact. : J. Phys. : J. Phys. Sot. Jpn. : J. Phys. Chem. , in: Landolt-Bbrnstein, New Series, Vol. ), Berlin, Heidelberg, New York: Springer (1986) p. : Hypertine Interact. : J. Phys. : Hyperfine Interact.
Sc Ti V Cr Mn Fe. Co Ni Cu Zn Fig. 26. Ni with 3d substitutional impurities. Local magnetic moment of the 3d impurity. Curve calculated from the LDOS curves of Fig. 61 over the impurity Wigner-Seitz sphere [85Dl, 87B2, 87221. Experimental values are indicated by open circles: A [56Sl], B [63C2], C [63Ll], D [63Cl], E [63Ll, 65Cl], F [68Cl], G, I, J [69Cl, 73A1, 73111, H [7lCl], K [74Cl], L [7411-J,M [76Ll], N [76Cl], P [79Kl], Q [80Kl], R [81Cl]. Fig. 27. Ni with 4d substitutional impurities. Local magnetic moment of the 4d impurity.
A Practical Handbook of Panchakarma Procedures by Lavekar, G.S. and Menon, T.V. and Central Council for Research in Ayurveda and Siddha (India)