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Letter
Nature 441, 617-620 (1 June 2006) | doi:10.1038/nature04732; Received 25 August 2005; Accepted 13 March 2006
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Dimensional reduction at a quantum critical point
S. E. Sebastian1, N. Harrison2, C. D. Batista3, L. Balicas4, M. Jaime2, P. A. Sharma2, N. Kawashima5 & I. R. Fisher1
- Geballe Laboratory for Advanced Materials and Department of Applied Physics, Stanford University, Stanford, California 94305, USA
- NHMFL, MS-E536, Los Alamos National Laboratory,
- Theoretical Division, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
- National High Magnetic Field Laboratory, Tallahassee, Florida 32310, USA
- Institute for Solid State Physics, University of Tokyo, Kashiwa, Chiba 277-8581, Japan
Correspondence to: S. E. Sebastian1 Correspondence and requests for materials should be addressed to S.E.S. (Email: suchitra@stanfordalumni.org).
Abstract
Competition between electronic ground states near a quantum critical point1, 2 (QCP)—the location of a zero-temperature phase transition driven solely by quantum-mechanical fluctuations—is expected to lead to unconventional behaviour in low-dimensional systems3. New electronic phases of matter have been predicted to occur in the vicinity of a QCP by two-dimensional theories3, 4, 5, 6, 7, 8, and explanations based on these ideas have been proposed for significant unsolved problems in condensed-matter physics, such as non-Fermi-liquid behaviour and high-temperature superconductivity. But the real materials to which these ideas have been applied are usually rendered three-dimensional by a finite electronic coupling between their component layers; a two-dimensional QCP has not been experimentally observed in any bulk three-dimensional system, and mechanisms for dimensional reduction have remained the subject of theoretical conjecture9, 10, 11. Here we show evidence that the Bose–Einstein condensate of spin triplets in the three-dimensional Mott insulator BaCuSi2O6 (refs 12–16) provides an experimentally verifiable example of dimensional reduction at a QCP. The interplay of correlations on a geometrically frustrated lattice causes the individual two-dimensional layers of spin-½ Cu2+ pairs (spin dimers) to become decoupled at the QCP, giving rise to a two-dimensional QCP characterized by linear power law scaling distinctly different from that of its three-dimensional counterpart. Thus the very notion of dimensionality can be said to acquire an 'emergent' nature: although the individual particles move on a three-dimensional lattice, their collective behaviour occurs in lower-dimensional space.
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