Quantum phase transition in a common metal

A. Yeh, Yeong-Ah Soh, J. Brooke, G. Aeppli (), T. F. Rosenbaum and S. M. Hayden
Additional contact information
A. Yeh: NEC Research Institute
Yeong-Ah Soh: NEC Research Institute
J. Brooke: NEC Research Institute
G. Aeppli: NEC Research Institute
T. F. Rosenbaum: The University of Chicago
S. M. Hayden: University of Bristol

Nature, 2002, vol. 419, issue 6906, 459-462

Abstract: Abstract The classical theory of solids, based on the quantum mechanics of single electrons moving in periodic potentials, provides an excellent description of substances ranging from semiconducting silicon to superconducting aluminium. Over the last fifteen years, it has become increasingly clear that there are substances for which the conventional approach fails. Among these are certain rare earth compounds1,2 and transition metal oxides3,4, including high-temperature superconductors5,6. A common feature of these materials is complexity, in the sense that they have relatively large unit cells containing heterogeneous mixtures of atoms. Although many explanations have been put forward for their anomalous properties7, it is still possible that the classical theory might suffice. Here we show that a very common chromium alloy has some of the same peculiarities as the more exotic materials, including a quantum critical point8, a strongly temperature-dependent Hall resistance4,5 and evidence for a ‘pseudogap’9. This implies that complexity is not a prerequisite for unconventional behaviour. Moreover, it should simplify the general task of explaining anomalous properties because chromium is a relatively simple system in which to work out in quantitative detail the consequences of the conventional theory of solids.

Date: 2002
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DOI: 10.1038/nature01044

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