1995
DOI: 10.1016/0304-8853(94)00961-9
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Influence of the crystal field on the magnetic behaviour of Er2Ni17

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Cited by 5 publications
(7 citation statements)
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“…On the other hand, the large difference in magnitude between the two moments reflects their different anisotropy. As shown in Table II, [18]. Taking into account the different radial extension of the 5f and 4f wave functions [19,20] and the different Stevens coefficients [21], we obtain for site 2b B …”
Section: Experimental Details and Resultsmentioning
confidence: 99%
“…On the other hand, the large difference in magnitude between the two moments reflects their different anisotropy. As shown in Table II, [18]. Taking into account the different radial extension of the 5f and 4f wave functions [19,20] and the different Stevens coefficients [21], we obtain for site 2b B …”
Section: Experimental Details and Resultsmentioning
confidence: 99%
“…Using this relationship V zz latt ϭ Ϫ4cB 2 0 /␣ J ͗r 2 ͘ with cϭ185, 12 ␣ J the second-order Stevens parameter and ͗r 2 ͘ the radial integral of the 4 f electron cloud, we calculated B 2 0 ϭϪ2.8͑5͒ K. The sign of B 2 0 corresponds to a c-axis anisotropy as also observed by susceptibility and ϩ SR measurements. 1,4-6 Its strength, however, is twice as large as the value derived from the susceptibility measurements.…”
Section: ͓S0163-1829͑96͒02746-4͔mentioning
confidence: 90%
“…Moreover, at T ¼ 4.2 K, the 166 Er spectrum of Er 2 Ni 17 shows two subspectra measured by Gubbens et al (1995b) as shown in Fig. 4.37.…”
Section: à2mentioning
confidence: 96%
“…Therefore, an explanation as given for Dy 2 Ni 17 does not hold. Presumably, influences of higher order crystal field terms have to be considered in order to explain the difference in hyperfine field at the Er sites in Er 2 Ni 17 (Gubbens et al, 1995b). The determined values of the spectrum at T ¼ 0.6 K are H eff ¼ 783(3) T and QS ¼ 0.32(10) cm/s for Er site I, and H eff ¼ 665(3) T and QS ¼ 0.50(10) cm/s for Er site II.…”
Section: à2mentioning
confidence: 99%
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