Abstract

Results of detailed ferromagnetic resonance measurements taken on amorphous (a-) Fe90+XZr10−X alloys with X=0 and 1 in the horizontal-parallel and vertical-parallel sample configurations at a fixed microwave frequency of ≂9.23 GHz in the temperature range 77 to 300 K before and after these alloys have undergone isothermal annealing treatment at 400 K for durations of time, tA, ranging from 10 to 240 min are presented and discussed. While only a single (primary) resonance is observed for T≲TC (the Curie temperature), an additional (secondary) resonance first appears at T≂TC and then gets fully resolved for T≳(TC+10 K). For the primary resonance (i) the ‘‘in-plane’’ uniaxial anisotropy field, Hk, and the Gilbert damping parameter, λ, both scale with the saturation magnetization, MS, in the temperature ranges 77 K≤T≲TC and 0.5TC≲T≲0.8TC, respectively, at all tA including tA=0; (ii) isothermal annealing has essentially no effect on MS(T), the ‘‘peak-to-peak’’ linewidth, ΔHpp(T), ΔH0 (the frequency- and temperature-independent contribution to ΔHpp) and λ(T); (iii) with increasing Fe concentration, the value corresponding to the peak in λ(T) decreases, λ(0.5TC) increases while λ(300 K) stays constant at 1×108 s−1, and (iv) isothermal annealing up to a time duration of 30 min results in an enhancement of about 1.5% in TC and a reduction of nearly 40% in the characteristic temperature T0 (which is a measure of the re-entrant transition temperature) whereas no further change occurs in both TC and T0 at higher annealing times. By contrast, for the secondary resonance, (a) Hk≂0 at all temperatures T≳TC and values of tA covered in the present experiments, (b) isothermal annealing leaves the resonance field unaltered, and (c) a steep decline in the value of ΔHpp′ occurs for tA≤10 min but at higher values of tA, ΔHpp′ remains constant for a-Fe90Zr10 whereas it increases at first and then saturates in the case of a-Fe91Zr9. The effect of isothermal annealing on the quantities of interest, i.e., TC, T0, ΔHpp, etc., can be qualitatively understood in terms of a finite spin clusters plus an infinite ferromagnetic matrix model.

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