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Raman Scattering from Spin Fluctuations and Phonons in UPt3
Abstract Since the discovery of its strongly enhanced magnetic susceptibility1, the compound UPt3 has become of increasingly greater interest. The finding of bulk superconductivity2,3 in UPt3 together with a T3. In T term in the low temperature specif lcheat, attributed to spin fluctuations, led to speculations3,4 about non-BCS or triplet pairing in this5heavy fermion superconductor. Neutron measurements of UPt 3 5 have confirmed the xistence of spin fluctuations for momentum transfers q ≥ 1Å−1 by detecting a broad line in the magnetic scattering cross section. The spin fluctuation temperature TSF or the spin relaxation rate of UPt3, given by the half widtn at half maximum (HWHM), Γ/2, of this quasielastic line, is found to be≈ 100 K. Below a characteristic temperature T*≃ 18 K, given by the maximum of the magnetic susceptibility, the coherence of UPt3 is described in terms of Fermi liquid theory, yielding for the spin fluctuations Γ/2∼vF·q, where vF is the Fermi velocity. The important question was whether q≈0 Raman measurements could prove this linear q dependence.
Raman Scattering from Spin Fluctuations and Phonons in UPt3
Abstract Since the discovery of its strongly enhanced magnetic susceptibility1, the compound UPt3 has become of increasingly greater interest. The finding of bulk superconductivity2,3 in UPt3 together with a T3. In T term in the low temperature specif lcheat, attributed to spin fluctuations, led to speculations3,4 about non-BCS or triplet pairing in this5heavy fermion superconductor. Neutron measurements of UPt 3 5 have confirmed the xistence of spin fluctuations for momentum transfers q ≥ 1Å−1 by detecting a broad line in the magnetic scattering cross section. The spin fluctuation temperature TSF or the spin relaxation rate of UPt3, given by the half widtn at half maximum (HWHM), Γ/2, of this quasielastic line, is found to be≈ 100 K. Below a characteristic temperature T*≃ 18 K, given by the maximum of the magnetic susceptibility, the coherence of UPt3 is described in terms of Fermi liquid theory, yielding for the spin fluctuations Γ/2∼vF·q, where vF is the Fermi velocity. The important question was whether q≈0 Raman measurements could prove this linear q dependence.
Raman Scattering from Spin Fluctuations and Phonons in UPt3
Brenten, E. (Autor:in) / Zirngiebl, E. (Autor:in) / Wire, M. S. (Autor:in) / Blumenröder, S. (Autor:in) / Pofahl, G. (Autor:in) / Güntherodt, G. (Autor:in) / Fisk, Z. (Autor:in)
01.01.1987
4 pages
Aufsatz/Kapitel (Buch)
Elektronische Ressource
Englisch
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