2011
DOI: 10.1103/physrevb.83.144429
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Variable temperature study of the crystal and magnetic structures of the giant magnetoresistant materialsLMnAsO(L=La, Nd)

Abstract: A variable temperature neutron and synchrotron diffraction study has been performed on the giant magnetoresistant oxypnictides LMnAsO (L = La, Nd). The low-temperature magnetic structures have been studied, and results show a spin reorientation of the Mn 2+ spins below T N (Nd) for NdMnAsO. The Mn 2+ spins rotate from alignment along c to alignment into the basal plane, and the Mn 2+ and Nd 3+ moments refine to 3.54(4) μ B and 1.93(4) μ B , respectively, at 2 K. In contrast, there is no change in magnetic stru… Show more

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Cited by 78 publications
(96 citation statements)
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References 38 publications
(79 reference statements)
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“…In contrast to these results, via neutron diffraction measurements performed at 290 K, the refined magnetic moment of Mn was 2.43μ B , which is more than one μ B lower compared to our theoretical result. In a later experiment, 21 however, it was shown that the moments at 2 K are 3.34 μ B , which is in good agreement with our calculations. In the case of LiMnAs, our neutron-diffraction data also show a similar trend as a function of temperature, where at 300 K the Mn moments are reduced from 3.72 to 2.62 μ B (see Table I).…”
Section: E Dft Calculationssupporting
confidence: 92%
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“…In contrast to these results, via neutron diffraction measurements performed at 290 K, the refined magnetic moment of Mn was 2.43μ B , which is more than one μ B lower compared to our theoretical result. In a later experiment, 21 however, it was shown that the moments at 2 K are 3.34 μ B , which is in good agreement with our calculations. In the case of LiMnAs, our neutron-diffraction data also show a similar trend as a function of temperature, where at 300 K the Mn moments are reduced from 3.72 to 2.62 μ B (see Table I).…”
Section: E Dft Calculationssupporting
confidence: 92%
“…Instead of canting, in agreement with Ref. 21 we explain the small remanent total moment of these compounds with the formation of MnAs as an impurity phase. This is because during synthesis, independent of the method used, tiny amounts of MnAs ( 1%) can easily be formed, which cannot be detected by techniques such as XRD or energy-dispersive x-ray spectroscopy (EDX).…”
Section: B Crystal and Magnetic Structuresupporting
confidence: 91%
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“…Various studies of the parent LnMnP nO have shown that the MnP n planes are universally antiferromagnetic [3][4][5][6][7][8][9][10] with in-plane checkerboard magnetic structure similar to the in-plane magnetic ordering in the various Mn-122 compounds. For compounds with moment-bearing rare-earth ions (Ln), a second low temperature magnetic ordering of the rare-earth element (i.e., Ce, Nd, and Pr) accompanied by a Mn-spin reorientation transition have been observed [4][5][6][7][8][9]. Other Mn-1111 compounds with variations on the Ln or P n sites have also been shown to order with the same in-plane * yliu@ameslab.gov AFM structure, albeit with uniform or alternate stacking of the AFM planes [11,12].…”
Section: Introductionmentioning
confidence: 99%
“…Depending on the actual choice of the pnictide element X in combination with a transition metal M , different electronic properties can be achieved 1 ranging from high-T c bulk superconductivity (with T c values up to 55 K for M = Fe and X = As) [2][3][4][5][6] to ferromagnetism with rare Kondo features (typically for M = Ru and X = P) 7,8 or with large -even colossal -magnetoresistance (M = Co, Mn and X = As, P). [9][10][11][12][13][14][15] However, the complex multi-orbital nature of the fermiology, 16,17 together with the open issue about the importance of electronic correlations, 18,19 makes the overall understanding of these materials still not complete and currently highly debated.…”
Section: Introductionmentioning
confidence: 99%