By P. Novák (auth.), H.P.J. Wijn (eds.)
Volume III/27 covers the magnetic homes of inorganic compounds in response to transition parts. it could actually for that reason be regarded as a complement to volumes III/4 and III/12 "Magnetic and different houses of magnetic oxides and comparable compounds" which seemed in 1970 and within the interval 1978 - 1982 respectively. In a manner this quantity additionally types a counterpart to quantity III/19, during which the magnetic homes of met- als, alloys and steel compounds are compiled. the 1st subvolume, III/27a, which seemed in past due 1988, bargains with the magnetic houses of pnictides and chalcogenides which comprise 3d components. Subvolume III/27d treats oxy-spinels. within the current subvolume III/27e oxidic compounds with the garnet constitution are thought of; they contain either iron and non-iron ingredients. actual and chemical houses that are of curiosity in reference to the magnetism of the garnets, were given the mandatory realization. Lists of iron and non-iron garnets support the consumer of this subvolume to discover the substance he's attracted to, and that are to be present in a number of components of volumes III/4, III/12 and III/27.
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P. 6’ 0” 120” 150” 180” I 30” I 60” I 90” I 120” I 150” I 180” 8- Fig. 87. Y,-,Sm,Fe,O,,. 2 K [79V4]. Fig. 88. ,O,,, [Ill]-oriented film. 15 GHz and at T=295 K [8OGl]. 2 FMR linewidth The motion of the magnetization may be described by the Gilbert equation dM - d( =yerr(MxH)-; (2) where a is the Gilbert damping parameter. An alternative fomr of the damping term given by Landau and Lifschitz is (3) Landau-Lifschitz damping parameter I. is related to a by the equation The linewidth AH is proportional to the damping parameter AH=2aH,,, .
113 I I I I 150 200 250 I 0 50 100 l I -'Oo I 50 I 100 I 150 I 200 I 250 0 . 55kOe 0 Fig. 60. Y3-,Er,FeSO1,. vs. temperaturefor different magnetic fields. Data for H=O were obtained by extrapolation [79 K 23. K, 25 *lo' J/m3 20 1751 125 0I I 50 I 100 1;0 200 250 I , Y,, I I I K 300 I25 -10’ J/m3 20 25 0 ! -25 2 1 -VI “V 0 50 100 150 200 250 K 300 I, 0 50 I 100 I I- 150 200 250 K 300 Fig. 62. Eu,Fe,O,,. Contributions AK, and AK2 of Eu3+ ion to Kl and K2 vs. temperature. Solid curves were calculated from the single ion theory [8OY 11.
50 orb. units 40 3: orb. units I 20 . Fig. 109. Y,Fe,O,,. 5 mm. Field of the magnetostatic modesvs. 144 GHz and RT. values are restricted to the roots of J&R)=0 where Jo is the zero order Bessel function. The spin wave modesare given by full circles, n denotesthe mode number. The applied magnetic field is perpendicular to the disk plane. The full curve shows the theoretical dispersion for the magnetostaticbranch, dashed curves give the theoretical spin wave branches [86 B 11. 4 Fig. 110. 6 pm. Brillouin light scattering intensity I of magnetostatic surface wave (S) and spin wave (p) vs.
Garnets by P. Novák (auth.), H.P.J. Wijn (eds.)