Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/3537
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dc.contributor.authorUtz, Yannicen_US
dc.contributor.authorSINGH, SURJEETen_US
dc.date.accessioned2019-07-01T05:55:27Z
dc.date.available2019-07-01T05:55:27Z
dc.date.issued2017-09en_US
dc.identifier.citationPhysical Review B, 96(11), 115135.en_US
dc.identifier.issn2469-9969en_US
dc.identifier.issn2469-9950en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/3537-
dc.identifier.urihttps://doi.org/10.1103/PhysRevB.96.115135en_US
dc.description.abstractThe S = 1 / 2 Heisenberg spin chain compound SrCuO 2 doped with different amounts of nickel (Ni), palladium (Pd), zinc (Zn), and cobalt (Co) has been studied by means of Cu nuclear magnetic resonance (NMR). Replacing only a few of the S = 1 / 2 Cu ions with Ni, Pd, Zn, or Co has a major impact on the magnetic properties of the spin chain system. In the case of Ni, Pd, and Zn an unusual line broadening in the low temperature NMR spectra reveals the existence of an impurity-induced local alternating magnetization (LAM), while strongly decaying spin-lattice relaxation rates T − 1 1 towards low temperatures indicate the opening of spin gaps. A distribution of gap magnitudes is implied by a stretched spin-lattice relaxation and a variation of T − 1 1 within the broad resonance lines. These observations depend strongly on the impurity concentration and therefore can be understood using the model of finite segments of the spin 1 / 2 antiferromagnetic Heisenberg chain, i.e., pure chain segmentation due to S = 0 impurities. This is surprising for Ni as it was previously assumed to be a magnetic impurity with S = 1 which is screened by the neighboring copper spins. In order to confirm the S = 0 state of the Ni, we performed x-ray absorption spectroscopy (XAS) and compared the measurements to simulated XAS spectra based on multiplet ligand-field theory. Furthermore, Zn doping leads to much smaller effects on both the NMR spectra and the spin-lattice relaxation rates, indicating that Zn avoids occupying Cu sites. For magnetic Co impurities, T − 1 1 does not obey the gaplike decrease, and the low-temperature spectra get very broad. This could be related to an increase of the Néel temperature and is most likely an effect of the impurity spin S ≠ 0 .en_US
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.subjectEffect of differenten_US
dc.subjectChain impuritiesen_US
dc.subjectSrCuO2 probed by NMRen_US
dc.subjectSpin chain compounden_US
dc.subject2017en_US
dc.titleEffect of different in-chain impurities on the magnetic properties of the spin chain compound SrCuO2 probed by NMRen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitlePhysical Review Ben_US
dc.publication.originofpublisherForeignen_US
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