How many spin liquids are there in Ca10Cr7O28?
ORAL
Abstract
Ca10Cr7O28 is a novel magnetic insulator with S=1/2 Cr5+ ions on a bilayer breathing–Kagome lattice. Exchange interactions in Ca10Cr7O28 are predominantly ferromagnetic, giving rise to a positive Curie-Weiss temperature of 2.35 K. None the less, no magnetic order is observed down to 19 mK, making Ca10Cr7O28 an unusual example of a two-dimensional quantum spin liquid.
In this talk we explore the nature and origin of the spin liquid observed in Ca10Cr7O28, using semi-classical molecular-dynamics simulations. We analyze the evolution of spin dynamics in Ca10Cr7O28 in applied magnetic field, and explicitly compare to published inelastic neutron scattering data.
To our surprise, we find that excitations encode not one, but two distinct types of spin liquids at different time scales. Fast fluctuations reveal a “coulombic spin liquid”, seen by broad “bow-tie” features in the magnetic scattering function which evolve in applied field into distinct “pinch-points”, as known from the classical Kagome antiferromagnet. On the other hand, slow fluctuations reveal a “spiral spin liquid”, which can be seen in form of “rings” in the magnetic scattering function, and understood by a mapping onto an effective spin-3/2 honeycomb model.
In this talk we explore the nature and origin of the spin liquid observed in Ca10Cr7O28, using semi-classical molecular-dynamics simulations. We analyze the evolution of spin dynamics in Ca10Cr7O28 in applied magnetic field, and explicitly compare to published inelastic neutron scattering data.
To our surprise, we find that excitations encode not one, but two distinct types of spin liquids at different time scales. Fast fluctuations reveal a “coulombic spin liquid”, seen by broad “bow-tie” features in the magnetic scattering function which evolve in applied field into distinct “pinch-points”, as known from the classical Kagome antiferromagnet. On the other hand, slow fluctuations reveal a “spiral spin liquid”, which can be seen in form of “rings” in the magnetic scattering function, and understood by a mapping onto an effective spin-3/2 honeycomb model.
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Presenters
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Rico Pohle
Okinawa Inst of Sci & Tech
Authors
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Rico Pohle
Okinawa Inst of Sci & Tech
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Han Yan
Okinawa Inst of Sci & Tech
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Nicholas Shannon
Okinawa Inst of Sci & Tech