TY - JOUR
T1 - Crystalline electric field effects in PrNi2B2C
T2 - Inelastic neutron scattering
AU - Mazumdar, Chandan
AU - Rotter, M.
AU - Frontzek, M.
AU - Michor, H.
AU - Doerr, M.
AU - Kreyssig, A.
AU - Koza, M.
AU - Hiess, A.
AU - Voigt, J.
AU - Behr, G.
AU - Gupta, L. C.
AU - Prager, M.
AU - Loewenhaupt, M.
PY - 2008/10/28
Y1 - 2008/10/28
N2 - 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 PrNi2B 2C. 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 YNi 2B2C decreases linearly with decreasing Y concentration x. Samples with x≤0.65 do not exhibit superconductivity down to 2 K.
AB - 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 PrNi2B 2C. 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 YNi 2B2C decreases linearly with decreasing Y concentration x. Samples with x≤0.65 do not exhibit superconductivity down to 2 K.
UR - http://www.scopus.com/inward/record.url?scp=55549088932&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.78.144422
DO - 10.1103/PhysRevB.78.144422
M3 - Article
AN - SCOPUS:55549088932
SN - 1098-0121
VL - 78
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 14
M1 - 144422
ER -