Input.Output Inc - X-Vib

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Zhu, and Q. Si, Phys. Rev. Lett. 91, 066405 (2003). 120 J. Custers, P. Gegenwart, H. Wilhelm, K. Neumaier, Y. Tokiwa, O. Trovarelli, C. Geibel, F. Steglich, C. Pepin, and P. Coleman, Nature 424, 524 (2003). 40 P. FULDE ET AL. 6). The wedge above the QCP is the region where NFL behavior of thermodynamic coefficients and transport properties is observed. This qualitative picture is hard to quantify. In fact the Kondo lattice model is an unsolved problem and only various approximative and numerical methods have been applied to it.

Zwicknagl, N. Stuesser, H. Jeevan, T. Cichorek, R. Loewenhaupt, C. Geibel, and F. Steglich, Phys. Rev. Lett. 92, 136401 (2004). STRONGLY CORRELATED ELECTRONS 23 To calculate the quasiparticle bands in CeCu2 Si2 by means of the renormalized band method, we adopt the doublet-quartet CEF scheme suggested in Ref. [77]. The ground state is separated from the excited quartet by δ 330 K. The results for the Fermi surface78,80 can be summarized as follows: We find two separate sheets of the Fermi surface for heavy and light quasiparticles.

P. Regnault, W. A. C. Erkelens, J. Rossat-Mignot, P. Lejay, and J. Flouquet, Phys. Rev. B 38, 4481 (1988). 71 G. Zwicknagl, E. Runge, and N. E. Christensen, Physica B 163, 97 (1990). 72 A. K. Albessard, T. Ebihara, I. Umehara, K. Satoh, Y. Onuki, H. Aoki, S. Uji, and T. Shimizu, Physica B 186–188, 147 (1993). 73 H. Aoki, S. Uji, A. K. Albessard, and Y. Onuki, Phys. Rev. Lett. 71, 2110 (1993). 74 F. S. Tautz, S. R. Julian, G. J. McMullen, and G. G. Lonzarich, Physica B 206–207, 29 (1995). 75 C. A.

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