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Home > Physics > Events > Condensed Matter Seminar 14/03/18: The long road to the kagome lattice antiferromagnet: a few materials met along the way...
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Condensed Matter Seminar 14/03/18: The long road to the kagome lattice antiferromagnet: a few materials met along the way...

Physics Department, Seminar room T125
14/03/2018 (14:00-15:00)

The condensed matter seminars are held most Wednesdays at 2pm during Term time in Room T125. They are arranged by Dr. Andrew Ho.


Kagome lattice

Dr. Gøran Nilsen, Polarised neutron scientist at ISIS, Rutherford Appleton Laboratory writes:

When geometric frustration - the inability of a spin system to satisfy all of its internal interactions - is combined with strong quantum fluctuations, exotic states called spin liquids can result. One of the enduring mysteries in quantum frustrated magnetism is the nature of the spin liquid state in the kagome lattice antiferromagnet model, which consists of a two-dimensional tiling of corner-sharing triangles populated by antiferromagnetically coupled spins. Despite significant recent theoretical progress towards this goal, unequivocal evidence of the predicted states has not been found in experiments. This is partly due to the imperfections of the materials - typically Cu2+ minerals - used to study the model. These include chemical disorder, lattice distortions, anisotropic exchange, and further neighbour exchange, all of which conspire to relieve the frustration and generate more conventional magnetic states. 
In this talk, I will aim to give an overview of the materials studied as realizations of the kagome lattice antiferromagnet, focusing on three in particular: herbertsmithite (Cu3Zn(OH)6Cl2), volborthite (Cu3V2O7(OH)2.2H2O), and KCu3As2O7(OH)3. I will aim to show how the crystallography and chemistry of these materials lead to the above imperfections, and discuss their implications in each case. Throughout, the main probe used will be neutron scattering. Although the study of kagome lattice materials shows that realizing the intrinsic properties of the model is extremely difficult, it also demonstrates the rich variety of physics which emerges in the presence of quantum fluctuations and magnetic frustration.


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