Abstract
The recent discovery of two heavy-fermion materials PuCoGa5 and NpPd5Al2, which transform directly from Curie paramagnets into superconductors, reveals a new class of superconductors where local moments quench directly into the superconducting condensate. Unlike other heavy-electron superconductors, where Cooper pairing is thought to be driven by spin fluctuations, these higher-transition-temperature materials do not seem to be close to a magnetic instability. Large-N expansions have been invaluable in describing heavy-fermion metals, but so far cannot treat superconductivity. Here, we introduce a new class of large-N expansion that uses symplectic symmetry to protect the odd time-reversal parity of spin and sustain Cooper pairs as well-defined singlets. We show that when a lattice of magnetic ions exchange spin with their metallic environment in two distinct symmetry channels, they can simultaneously satisfy both channels by forming a condensate of composite pairs between local moments and electrons. In the tetragonal crystalline environment relevant to PuCoGa5 and NpPd5Al2, the lattice structure selects a natural pair of spin exchange channels, predicting a unique anisotropic paired state with either d- or g-wave symmetry. This pairing mechanism also predicts a large upturn in the NMR relaxation rate above Tc and strong enhancement of Andreev reflection in tunnelling measurements.
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Acknowledgements
This research was supported by the National Science Foundation grant DMR-0605935 and US Department of Energy grant DE-FE02 00ER45790 (M.D.). The authors would like to thank N. Andrei, K. Basu, E. Miranda, R. Moessner, P. Pagliuso, S. Sachdev, N. Read, G. Zarand and particularly S. Thomas, for discussions related to this work.
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Flint, R., Dzero, M. & Coleman, P. Heavy electrons and the symplectic symmetry of spin. Nature Phys 4, 643–648 (2008). https://doi.org/10.1038/nphys1024
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DOI: https://doi.org/10.1038/nphys1024
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