Continuous and discontinuous quantum phase transitions in a model two-dimensional magnet

Author:

Haravifard S.12,Banerjee A.2,Lang J. C.1,Srajer G.1,Silevitch D. M.2,Gaulin B. D.345,Dabkowska H. A.4,Rosenbaum T. F.2

Affiliation:

1. Advanced Photon Source, Argonne National Laboratory, 9700 S. Cass Avenue, Argonne, IL 60439;

2. James Franck Institute and Department of Physics, University of Chicago, 929 E 57th Street, Chicago, IL 60637;

3. Department of Physics and Astronomy, McMaster University, 1280 Main Street W, Hamilton, Ontario, L8S 4M1, Canada;

4. Canadian Institute for Advanced Research, 180 Dundas Street W, Toronto, Ontario, M5G 1Z8, Canada; and

5. Brockhouse Institute for Material Research, McMaster University, 1280 Main Street W, Hamilton, Ontario, L8S 4M1, Canada

Abstract

The Shasty–Sutherland model, which consists of a set of spin 1/2 dimers on a 2D square lattice, is simple and soluble but captures a central theme of condensed matter physics by sitting precariously on the quantum edge between isolated, gapped excitations and collective, ordered ground states. We compress the model Shastry–Sutherland material, SrCu 2 (BO 3 ) 2 , in a diamond anvil cell at cryogenic temperatures to continuously tune the coupling energies and induce changes in state. High-resolution X-ray measurements exploit what emerges as a remarkably strong spin-lattice coupling to both monitor the magnetic behavior and the absence or presence of structural discontinuities. In the low-pressure spin-singlet regime, the onset of magnetism results in an expansion of the lattice with decreasing temperature, which permits a determination of the pressure-dependent energy gap and the almost isotropic spin-lattice coupling energies. The singlet-triplet gap energy is suppressed continuously with increasing pressure, vanishing completely by 2 GPa. This continuous quantum phase transition is followed by a structural distortion at higher pressure.

Publisher

Proceedings of the National Academy of Sciences

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