000022670 001__ 22670 000022670 005__ 20230426083037.0 000022670 0247_ $$2DOI$$a10.1103/PhysRevB.86.081415 000022670 0247_ $$2WOS$$aWOS:000308210000003 000022670 0247_ $$2Handle$$a2128/10844 000022670 037__ $$aPreJuSER-22670 000022670 041__ $$aeng 000022670 082__ $$a530 000022670 084__ $$2WoS$$aPhysics, Condensed Matter 000022670 1001_ $$0P:(DE-HGF)0$$aChoi, Y.-K.$$b0 000022670 245__ $$aWeak antiferromagnetic superexchange interaction in fcc C60Hn 000022670 260__ $$aCollege Park, Md.$$bAPS$$c2012 000022670 300__ $$a081415(R) 000022670 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article 000022670 3367_ $$2DataCite$$aOutput Types/Journal article 000022670 3367_ $$00$$2EndNote$$aJournal Article 000022670 3367_ $$2BibTeX$$aARTICLE 000022670 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000022670 3367_ $$2DRIVER$$aarticle 000022670 440_0 $$04919$$aPhysical Review B$$v86$$x1098-0121$$y081415 000022670 500__ $$3POF3_Assignment on 2016-02-29 000022670 500__ $$aThis work was supported by National Research Foundation of Korea (NRF) grant funded by the Korean Government (NRF-2011-0015754). The calculations were performed by KISTI supercomputing center through the strategic support program (KSC-2011-C3-08) for the supercomputing application research. 000022670 520__ $$aA recent density-functional calculation for fcc C60Hn (n = odd) [ K.W. Lee and C. E. Lee, Phys. Rev. Lett. 106, 166402 (2011)] proposed the existence of Stoner ferromagnetism based on an itinerant band model. However, our density-functional calculation shows that the antiferromagnetic (AFM) configuration is slightly more stable than the ferromagnetic (FM) one. This preference for antiferromagnetism over ferromagnetism is analogous to the case of a dimer (C60H)(2), where each C60H is spin polarized by an intramolecular exchange and the two magnetic moments are antiferromagnetically coupled with each other. 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