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            "citation": "Anomalous Nernst and Righi-Leduc Effects in Mn3Sn: Berry curvature and Entropy flow (arXiv1612.06128v4)",
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      "statement": "# Large anomalous Nernst response and transverse heat transport in Mn3Sn\n\nIndependent teams measured a sizable, hysteretic transverse thermoelectric response in the noncollinear antiferromagnet Mn3Sn near room temperature despite its small net magnetization. Ikhlas and colleagues reported a remanent Nernst signal of about 0.35 microvolt per kelvin at 300 K in one crystal. Li and colleagues additionally measured anomalous thermal Hall transport and found its ratio to electrical Hall transport approximately consistent with the Wiedemann–Franz value over their measured high-temperature magnetic phase. Berry-curvature calculations and transport comparisons supplied an interpretation of the response.\n\n## Scientific scope\n\nThis family combines two independent experimental originals, with separate bylines, sample compositions, magnetic phases and uncertainties. Zero-field values are remanent signals after magnetic preparation. Full hysteretic jumps differ from a single-branch signal. The thermal Hall comparison has appreciable contact and geometrical uncertainties; it does not uniquely establish a microscopic mechanism. Calculated Weyl-point and Fermi-energy explanations are model interpretations, and useful thermoelectric generators were proposed rather than demonstrated.\n\n## Reading status\n\nThis is a source-linked WRS catalogue note. A full explanatory guide and independent scientific reconstruction have not been completed for this entry. Read the identified original work for its complete narrative and arguments.\n\n## People and systems\n\nXiaokang Li; Liangcai Xu; Linchao Ding; Jinhua Wang; Mingsong Shen; Xiufang Lu; Zengwei Zhu; Kamran Behnia; Muhammad Ikhlas; Takahiro Tomita; Takashi Koretsune; Michi-To Suzuki; Daisuke Nishio-Hamane; Ryotaro Arita; Yoshichika Otani; Satoru Nakatsuji\n\nThese are the listed authors of the cited contribution sources. Paper authorship does not quantify individual effort. An incomplete list is explicitly marked; same names are not automatically merged.\n\n\n\n## Original sources\n\n- [Anomalous Nernst and Righi-Leduc Effects in Mn3Sn: Berry curvature and Entropy flow (arXiv1612.06128v4)](https://arxiv.org/pdf/1612.06128v4)\n- [Large anomalous Nernst effect at room temperature in a chiral antiferromagnet (arXiv1710.00062v1)](https://arxiv.org/pdf/1710.00062v1)\n",
      "summary": "Independent teams measured a sizable, hysteretic transverse thermoelectric response in the noncollinear antiferromagnet Mn3Sn near room temperature despite its small net magnetization. Ikhlas and colleagues reported a remanent Nernst signal of about 0.35 microvolt per kelvin at 300 K in one crystal. Li and colleagues additionally measured anomalous thermal Hall transport and found its ratio to electrical Hall transport approximately consistent with the Wiedemann–Franz value over their measured high-temperature magnetic phase. Berry-curvature calculations and transport comparisons supplied an interpretation of the response.",
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    "scope": "Independent teams measured a sizable, hysteretic transverse thermoelectric response in the noncollinear antiferromagnet Mn3Sn near room temperature despite its small net magnetization. Ikhlas and colleagues reported a remanent Nernst signal of about 0.35 microvolt per kelvin at 300 K in one crystal. Li and colleagues additionally measured anomalous thermal Hall transport and found its ratio to electrical Hall transport approximately consistent with the Wiedemann–Franz value over their measured high-temperature magnetic phase. Berry-curvature calculations and transport comparisons supplied an interpretation of the response. This family combines two independent experimental originals, with separate bylines, sample compositions, magnetic phases and uncertainties. Zero-field values are remanent signals after magnetic preparation. Full hysteretic jumps differ from a single-branch signal. The thermal Hall comparison has appreciable contact and geometrical uncertainties; it does not uniquely establish a microscopic mechanism. Calculated Weyl-point and Fermi-energy explanations are model interpretations, and useful thermoelectric generators were proposed rather than demonstrated.",
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