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Special temperatures in frustrated ferromagnets

Laura BovoDepartment of Innovation and Enterprise, University College London, 90 Tottenham Court Rd, Fitzrovia, London, W1T 4TJ, UKMikael TwengströmDepartment of Physics, Royal Institute of Technology, SE-106 91, Stockholm, Sweden. [email protected]O. A. PetrenkoDepartment of Physics, University of Warwick, Coventry, CV4 7AL, UKT. FennellLaboratory for Neutron Scattering and Imaging, Paul Scherrer Institut, 5232, Villigen PSI, SwitzerlandMichel J. P. GingrasCanadian Institute for Advanced Research, 180 Dundas St. W., Toronto, ON, M5G 1Z8, CanadaS. T. BramwellLondon Centre for Nanotechnology and Department of Physics and Astronomy, University College London, 17-19 Gordon Street, London, WC1H OAH, UKP. HeneliusDepartment of Physics, Royal Institute of Technology, SE-106 91, Stockholm, Sweden
2018en
ABI

Аннотация

Abstract The description and detection of unconventional magnetic states, such as spin liquids, is a recurring topic in condensed matter physics. While much of the efforts have traditionally been directed at geometrically frustrated antiferromagnets, recent studies reveal that systems featuring competing antiferromagnetic and ferromagnetic interactions are also promising candidate materials. We find that this competition leads to the notion of special temperatures, analogous to those of gases, at which the competing interactions balance, and the system is quasi-ideal. Although induced by weak perturbing interactions, these special temperatures are surprisingly high and constitute an accessible experimental diagnostic of eventual order or spin-liquid properties. The well characterised Hamiltonian and extended low-temperature susceptibility measurement of the canonical frustrated ferromagnet Dy 2 Ti 2 O 7 enables us to formulate both a phenomenological and microscopic theory of special temperatures for magnets. Other members of this class of magnets include kapellasite Cu 3 Zn(OH) 6 Cl 2 and the spinel GeCo 2 O 4 .

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