<div class="csl-bib-body">
<div class="csl-entry">Mazumdar, C., Rotter, M., Frontzek, M., Michor, H., Doerr, M., Kreyssig, A., Koza, M., Hiess, A., Voigt, J., Behr, G., Gupta, L. C., Prager, M., & Loewenhaupt, M. (2008). Crystalline electric field effects in PrNi₂B₂C: Inelastic neutron scattering. <i>Physical Review B</i>, <i>78</i>(144422). https://doi.org/10.1103/physrevb.78.144422</div>
</div>
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dc.identifier.issn
2469-9950
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dc.identifier.uri
http://hdl.handle.net/20.500.12708/170506
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dc.description.abstract
PrNi2B2C as a member of the borocarbide series is characterized by antiferromagnetic order below TN=4 K and the absence of superconductivity (at least down to 100 mK). There are two effects responsible for the absence of superconductivity in PrNi2B2C. These are the strong conduction electron-Pr moment interaction and a comparatively lower density of states. We studied the crystalline electric field (CEF) excitations and excitons in this compound by inelastic neutron scattering. The CEF level scheme obtained from these data comprises a singlet ground state, a doublet at 1 meV, and further higher levels at 5.2, 24.3 (doublet), 25.1, 29.4, and 31.5 meV. Large dispersion was found for the 1 meV excitation and explained theoretically taking into account magnetic exchange interactions. The calculated crystal-field parameters explain satisfactorily the neutron spectra as well as the heat-capacity and magnetic-susceptibility data. This leads to the conclusion that PrNi2B2C can be described by the standard model of rare-earth magnetism. Thus the heavy-fermion concept, suggested by some groups earlier in literature, is not the cause of the suppression of superconductivity. Excitation spectra of the diluted series Pr1−xYxNi2B2C were also investigated. No drastic changes in the CEF level scheme have been observed in these compounds. Hence the CEF level scheme of the full compound, i.e., PrNi2B2C, is reasonably valid for these samples too. The superconducting-transition temperature TC~15.5 K for YNi2B2C decreases linearly with decreasing Y concentration x. Samples with x<=0.65 do not exhibit superconductivity down to 2 K.
en
dc.language.iso
en
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dc.publisher
AMER PHYSICAL SOC
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dc.relation.ispartof
Physical Review B
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dc.subject
Condensed Matter Physics
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dc.subject
Electronic, Optical and Magnetic Materials
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dc.title
Crystalline electric field effects in PrNi₂B₂C: Inelastic neutron scattering
en
dc.type
Artikel
de
dc.type
Article
en
dc.type.category
Original Research Article
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tuw.container.volume
78
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tuw.container.issue
144422
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tuw.journal.peerreviewed
true
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tuw.peerreviewed
true
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tuw.researchTopic.id
M3
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tuw.researchTopic.id
C1
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tuw.researchTopic.id
Q6
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tuw.researchTopic.name
Metallic Materials
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tuw.researchTopic.name
Computational Materials Science
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tuw.researchTopic.name
Quantum Many-Body Systems
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tuw.researchTopic.value
20
-
tuw.researchTopic.value
20
-
tuw.researchTopic.value
60
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dcterms.isPartOf.title
Physical Review B
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tuw.publication.orgunit
E138-03 - Forschungsbereich Functional and Magnetic Materials
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tuw.publisher.doi
10.1103/physrevb.78.144422
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dc.identifier.eissn
2469-9969
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dc.description.numberOfPages
9
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wb.sci
true
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wb.sciencebranch
Physik, Mechanik, Astronomie
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wb.sciencebranch.oefos
12
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en
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Publications
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Publications
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http://purl.org/coar/resource_type/c_18cf
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http://purl.org/coar/resource_type/c_18cf
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no Fulltext
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none
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Artikel
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item.openairetype
Article
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crisitem.author.dept
E138-03 - Forschungsbereich Functional and Magnetic Materials