1996
DOI: 10.1103/physrevb.53.32
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Enhanced magnetic anisotropy energy density for superparamagnetic particles of cobalt

Abstract: We use our measurements of the magnetization and the magnetoresistance for very small superparamagnetic particles of Co to obtain the low-temperature value of the magnetic anisotropy energy density, CϷ3ϫ10 8 erg/cm 3 . This is nearly two orders of magnitude larger than the corresponding value for C for bulk Co. The enormous enhancement of C for very small particles of Co is consistent with results previously reported for very small particles of Fe and of FeNi.

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Cited by 37 publications
(21 citation statements)
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“…For typical laboratory experiments, ln(τm/τ0) is on the order of 25 [41]. For the observed blocking temperature, Tb = 14 K, we obtain an activation barrier KV of 0.30 eV, which coincides with the reported spin pairing interaction [9] and is on the same order as the average splitting of energy levels with 6-8 states per eV near the Fermi energy given above.…”
Section: Epr Observation Of a Blocking Temperaturesupporting
confidence: 79%
See 1 more Smart Citation
“…For typical laboratory experiments, ln(τm/τ0) is on the order of 25 [41]. For the observed blocking temperature, Tb = 14 K, we obtain an activation barrier KV of 0.30 eV, which coincides with the reported spin pairing interaction [9] and is on the same order as the average splitting of energy levels with 6-8 states per eV near the Fermi energy given above.…”
Section: Epr Observation Of a Blocking Temperaturesupporting
confidence: 79%
“…For a cluster radius of ca. 0.5 nm we obtain K ≈ 0.6 eV nm −3 (1 × 10 9 erg•cm −3 ) which is even larger than the value of 1 × 10 8 erg•cm −3 reported for nanometer size granular Co20Ag80 and Co25Ag75 (indices are percent composition) and two orders of magnitude larger than for bulk fcc cobalt (4 × 10 6 erg•cm −3 ) [40], but it was pointed out that, for such small particles, the anisotropy energy is more a surface than a volume property [41]. It appears that it is straightforward to explain the temperature-dependence of the magnetization in Figure 5 based on what is known about classical superparamagnetic nanoparticles with a single macroscopic superspin.…”
Section: Epr Observation Of a Blocking Temperaturementioning
confidence: 72%
“…The blocking Previous studies have demonstrated that the magnetic anisotropy energy density depends on properties such as particle shape and surface texture as well as the stresses in the particle, rather than being an intrinsic property of a superparamagnetic nanoparticle [50]. The same phenomenon was observed for the necklace-like FePt-Au HNCs, as shown in Fig.…”
Section: Magnetic Propertiessupporting
confidence: 62%
“…In addition, surface effects, including both structural changes and electronic hybridization effects, can significantly modify the magnetic moments of the magnetic component and the anisotropy [183]. For instance, comparing FePt-Au heterodimers with FePt particles reveals that blocking temperature of heterodimers (25 K) is reduced from 40 K to 25 K as a result of anisotropy decrease and surface texture changing [90,184]. However, it has been shown that, while depending on the surface termination, an increasing anisotropy of this system is possible [183].…”
Section: Tailored Properties Of Selected Heterodimersmentioning
confidence: 99%