Inelastic neutron scattering studies on the odd-membered antiferromagnetic wheel Cr8 Ni
Author(s) -
Michael L. Baker,
O. Waldmann,
Stergios Piligkos,
R. Bircher,
Olivier Cador,
Stefano Carretta,
David Collison,
Félix Fernández-Alonso,
Eric J. L. McInnes,
H. Mutka,
A. Podlesnyak,
Floriana Tuna,
Stefan T. Ochsenbein,
Roberta Sessoli,
A. Sieber,
Grigore A. Timco,
Høgni Weihe,
Hans U. Güdel,
Richard E. P. Winpenny
Publication year - 2012
Publication title -
physical review b
Language(s) - English
Resource type - Journals
eISSN - 1538-4489
pISSN - 1098-0121
DOI - 10.1103/physrevb.86.064405
Subject(s) - inelastic neutron scattering , excited state , antiferromagnetism , physics , magnetic susceptibility , ground state , atomic physics , condensed matter physics , neutron , crystallography , neutron scattering , quantum mechanics , chemistry
International audience[(iC3H7)2NH2][Cr8NiF9(O2CCMe)18], or Cr8Ni, is a prominent example of an odd-membered antiferromagnetic "wheel." A detailed characterization of the magnetic properties of Cr8Ni has been conducted. Inelastic neutron scattering (INS) is used to investigate the energy and momentum transfer dependence of the low-lying spin excitations, including excited states inaccessible by other experimental techniques. The richness of the INS data, in conjunction with microscopic spin Hamiltonian simulations, enables an accurate characterization of the magnetic properties of Cr8Ni. Nearest-neighbor exchange constants of JCrCr = 1.31 meV and JCrNi = 3.22 meV are determined, and clear evidence of axial single-ion anisotropy is found. The parameters determined by INS are shown to fit magnetic susceptibility. The spectroscopic identification of several successive S=1 excited total spin states and lowest spin band excitations show that the rotational band picture, valid for bipartite AFM wheels, breaks down for this odd-numbered wheel. The exchange constants determined here differ from previous efforts based on bulk measurements, and possible reasons are discussed. The large JCrNi/JCrCr ratio in Cr8Ni puts this wheel into a regime with strong quantum fluctuations in which the ground state can be described with a valence bond solid state picture
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