1998
DOI: 10.1016/s0038-1098(98)00161-6
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Measurements of magnetic susceptibilities and anisotropy of erbium pyrogermanate (Er2Ge2O7) crystal

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Cited by 9 publications
(11 citation statements)
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“…To temperature of θ w = −14.4(2)K. We find a negative Weiss temperature indicating antiferromagnetic (AFM) order in agreement with Ghosh et al 31 . However, the absolute value of our Weiss temperature is larger than previously reported, we attribute this to the finer temperature steps and higher temperature cutoff (120 K) used in our analysis the former of which allows for the range of linear behavior to be more carefully determined 31 .…”
Section: B Zero-field Magnetic Structuresupporting
confidence: 91%
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“…To temperature of θ w = −14.4(2)K. We find a negative Weiss temperature indicating antiferromagnetic (AFM) order in agreement with Ghosh et al 31 . However, the absolute value of our Weiss temperature is larger than previously reported, we attribute this to the finer temperature steps and higher temperature cutoff (120 K) used in our analysis the former of which allows for the range of linear behavior to be more carefully determined 31 .…”
Section: B Zero-field Magnetic Structuresupporting
confidence: 91%
“…We observe no evidence of magnetic ordering down to 2 K. Above ∼ 100 K typical Curie-Weiss behavior is seen as reported for both Ho 2 Ge 2 O 7 and Dy 2 Ge 2 O 7 . Fitting the inverse susceptibility by the Curie-Wiess law (χ −1 = C(T −θ w )) we obtain an effective magnetic moment of µ ef f = 9.8(3)µ B /Er and a Weiss temperature of θ w = −14.4(2)K. We find a negative Weiss temperature indicating antiferromagnetic (AFM) order in agreement with Ghosh et al 31 . However, the absolute value of our Weiss temperature is larger than previously reported, we attribute this to the finer temperature steps and higher temperature cutoff (120 K) used in our analysis the former of which allows for the range of linear behavior to be more carefully determined 31 .…”
Section: B Zero-field Magnetic Structuresupporting
confidence: 89%
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“…The coordination polyhedron of the rare earth is a distorted pentagonal bipyramid [1][2] with its axis almost parallel to the crystallographic c direction. The optical properties [3][4] and magnetic susceptibility of the R 2 Ge 2 O 7 compounds [3,[5][6][7][8] have often been interpreted in light of the four equivalent magnetic sites per unit cell and their local 5-fold symmetry, though the findings of a Mossbauer study on Er 2 Ge 2 O 7 [9] indicate that the pentagonal crystal field model around the R atoms is invalid at least in that case.…”
Section: Introductionmentioning
confidence: 99%