Abstract
In solid state physics one is in the situation that it is possible to write down the Hamiltonian governing the physics of the systems under investigation. The quantum mechanical Schrödinger equation describing the electrons and nuclei that form the solid contains their kinetic energy terms and the Coulomb interactions between the particles. This situation means effectively that one has a ‘theory of everything’ available, describing in principle all material properties below the energy scales of solidification. From a reductionist point of view this is a fait accompli.
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Notes
- 1.
One has to point out though that developments in numerical calculations have made great advances in recent years and are now a useful tool in the understanding of band structures of crystalline materials. Especially the availability of tool sets such as Wien2K [1] and CASTEP [2] make the use of the techniques available to non-experts and become more and more used in the lab environment. However, they are based on certain approximations of the full Hamiltonian and therefore currently unable to treat problems going beyond these approximations.
References
Blaha P, Schwarz K, Sorantin P, Trickey SB (1990) Full-potential, linearized augmented plane-wave programs for crystalline systems. Comp Phys Commun 59(2):399–415
Segall MD, Lindan PJD, Probert MJ, Pickard CJ, Hasnip PJ, Clark SJ, Payne MC (2002) First-principles simulation: ideas, illustrations and the CASTEP code. J Phys Condens Matter 14(11):2717–2744
Mackenzie AP, Maeno Y (2003) The superconductivity of Sr2RuO4 and the physics of spin-triplet pairing. Rev Mod Phys 75(2):657–712
Stewart GR (2001) Non-Fermi-liquid behavior in d- and f-electron metals. Rev Mod Phys 73(4):797–855
Kondo J (1964) Resistance minimum in dilute magnetic alloys. Prog Theor Phys 32:37
Tsui DC, Störmer HL, Gossard AC (1982) Two-dimensional magnetotransport in the extreme quantum limit. Phys Rev Lett 48(22):1559–1562
Laughlin RB (1983) Anomalous quantum Hall-effect—an incompressible quantum fluid with fractionally charged excitations. Phys Rev Lett 50(18):1395–1398
Diep HP (2005) Frustrated spin systems. World Scientific Publishing, Singapore, London
Mathur ND, Grosche FM, Julian SR, Walker IR, Freye DM, Haselwimmer RKW, Lonzarich GG (1998) Magnetically mediated superconductivity in heavy Fermion compounds. Nature 394(6688):39–43
Löhneysen Hv, Rosch A, Vojta M, Wölfle P (2007) Fermi-liquid instabilities at magnetic quantum phase transitions. Rev Mod Phys 79(3):1015–1075
Custers J, Gegenwart P, Wilhelm H, Neumaier K, Tokiwa Y, Trovarelli O, Geibel C, Steglich F, Pepin C, Coleman P (2003) The break-up of heavy electrons at a quantum critical point. Nature 424(6948):524–527
Schröder A, Aeppli G, Coldea R, Adams M, Stockert O, von Löhneysen H, Bucher E, Ramazashvili R, Coleman P (2000) Onset of antiferromagnetism in heavy-Fermion metals. Nature 407(6802):351–355
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Rost, A.W. (2010). Introduction. In: Magnetothermal Properties near Quantum Criticality in the Itinerant Metamagnet Sr3Ru2O7 . Springer Theses. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-14524-7_1
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DOI: https://doi.org/10.1007/978-3-642-14524-7_1
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