000877404 001__ 877404 000877404 005__ 20210401192801.0 000877404 0247_ $$2doi$$a10.1038/s42005-020-0365-8 000877404 0247_ $$2Handle$$a2128/25049 000877404 0247_ $$2altmetric$$aaltmetric:83225709 000877404 0247_ $$2WOS$$aWOS:000553489000002 000877404 037__ $$aFZJ-2020-02173 000877404 082__ $$a530 000877404 1001_ $$0P:(DE-HGF)0$$aSong, Yu$$b0 000877404 245__ $$aNature of the spin resonance mode in CeCoIn5 000877404 260__ $$aLondon$$bSpringer Nature$$c2020 000877404 3367_ $$2DRIVER$$aarticle 000877404 3367_ $$2DataCite$$aOutput Types/Journal article 000877404 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1617219170_12335 000877404 3367_ $$2BibTeX$$aARTICLE 000877404 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000877404 3367_ $$00$$2EndNote$$aJournal Article 000877404 520__ $$aSpin-fluctuation-mediated unconventional superconductivity can emerge at the border of magnetism, featuring a superconducting order parameter that changes sign in momentum space. Detection of such a sign-change is experimentally challenging, since most probes are not phase-sensitive. The observation of a spin resonance mode (SRM) from inelastic neutron scattering is often seen as strong phase-sensitive evidence for a sign-changing superconducting order parameter, by assuming the SRM is a spin-excitonic bound state. Here we show that for the heavy fermion superconductor CeCoIn5, its SRM defies expectations for a spin-excitonic bound state, and is not a manifestation of sign-changing superconductivity. Instead, the SRM in CeCoIn5 likely arises from a reduction of damping to a magnon-like mode in the superconducting state, due to its proximity to magnetic quantum criticality. Our findings emphasize the need for more stringent tests of whether SRMs are spin-excitonic, when using their presence to evidence sign-changing superconductivity. 000877404 536__ $$0G:(DE-HGF)POF3-6G15$$a6G15 - FRM II / MLZ (POF3-6G15)$$cPOF3-6G15$$fPOF III$$x0 000877404 536__ $$0G:(DE-HGF)POF3-6G4$$a6G4 - Jülich Centre for Neutron Research (JCNS) (POF3-623)$$cPOF3-623$$fPOF III$$x1 000877404 588__ $$aDataset connected to CrossRef 000877404 65027 $$0V:(DE-MLZ)SciArea-120$$2V:(DE-HGF)$$aCondensed Matter Physics$$x0 000877404 65027 $$0V:(DE-MLZ)SciArea-170$$2V:(DE-HGF)$$aMagnetism$$x1 000877404 65017 $$0V:(DE-MLZ)GC-1604-2016$$2V:(DE-HGF)$$aMagnetic Materials$$x0 000877404 693__ $$0EXP:(DE-MLZ)PANDA-20140101$$1EXP:(DE-MLZ)FRMII-20140101$$5EXP:(DE-MLZ)PANDA-20140101$$6EXP:(DE-MLZ)SR2-20140101$$aForschungs-Neutronenquelle Heinz Maier-Leibnitz $$ePANDA: Cold three axes spectrometer$$fSR2$$x0 000877404 7001_ $$0P:(DE-HGF)0$$aWang, Weiyi$$b1 000877404 7001_ $$0P:(DE-HGF)0$$aS. Van Dyke, John$$b2 000877404 7001_ $$0P:(DE-HGF)0$$aPouse, Naveen$$b3 000877404 7001_ $$0P:(DE-HGF)0$$aRan, Sheng$$b4 000877404 7001_ $$0P:(DE-HGF)0$$aYazici, Duygu$$b5 000877404 7001_ $$0P:(DE-Juel1)156579$$aSchneidewind, A.$$b6 000877404 7001_ $$0P:(DE-Juel1)159141$$aCermak, Petr$$b7 000877404 7001_ $$0P:(DE-HGF)0$$aQiu, Y.$$b8 000877404 7001_ $$0P:(DE-HGF)0$$aMaple, M. 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