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Determination of the magnetic q vectors in the heavy fermion superconductor Ce3PtIn11

Naoki Shioda, Kazuki Kumeda, Hideto Fukazawa, Tetsuo Ohama, Yoh Kohori, Debarchan Das, Joanna Bławat, Dariusz Kaczorowski, Koudai Sugimoto

DOI 10.1103/PhysRevB.104.245119 · Physical Review B

T1

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Abstract

An analysis with a transferred hyperfine field has been performed on the spectra of the In115 nuclear quadrupole resonance experiments of heavy fermion superconductor Ce3PtIn11 exhibiting co-occurrence of two successive antiferromagnetic orderings (TN1 = 2.2 K and TN2 = 2.0 K) followed by a superconducting transition (Tc = 0.32 K). The spectral changes at magnetic transition temperatures TN1 and TN2 indicate that the Ce(2) site has the dominant magnetic contribution, with a small magnetic moment, but not negligible, at the Ce(1) site. Our analysis using a transferred hyperfine field which overcomes the previous simple dipolar model evinces the magnetic structures of Ce3PtIn11. ForTN2<T<TN1, the propagation vectors at the Ce(1) and Ce(2) sublattices are q1=q2=(12,12,0or12). On the other hand, for T<TN2, the propagation vectors are q1=(12,12,16or13) and q2=(12,12,12or0), respectively.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Ce3PtIn11

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0.32Pressure unresolvedunknown
Ce3PdIn11

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown
CeIn3

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown
CeRhIn5

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—1.6 GPaunknown
Ce2RhIn8

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—1.3 GPaunknown

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