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STRUCTURE OF LOCAL SPIN EXCITATIONS IN A GEOMETRICALLY FRUSTRATED ANTIFERROMAGNET
For many crystalline magnetic materials, only a long range ordered spin configuration can satisfy all near neighbor spin interactions. Such systems generally display a finite temperature transition to a broken symmetry phase with longrange magnetic order. However, on certain lattices with weak connectivity and a triangular motif, shortrange interactions can be satisfied without longrange order [1].
To explore this possibility we examined magnetic order and fluctuation in ZnCr_{2}O_{4}. The Bsite of this spinel lattice is solely occupied by spin3/2 Cr^{3+}, and this leads to a magnet with dominant nearest neighbor interactions on the lattice of cornersharing tetrahedra shown in Fig. 1.
Exchange interactions in this structure are satisfied at the mean field classical level when every tetrahedron carries zero net magnetization. Not only are there many ways that a tetrahedron can have no moment, but there are also many ways to organize such nonmagnetic tetrahedra on the cornersharing lattice. The result is a "geometrically frustrated" spin system with many ways to satisfy interactions without longrange order.
Analysis of specific spin models on the Bsite spinel (or pyrochlore) lattice indicates that spin1/2 and spin models have shortrange order down to T = 0 [2], while longrange order is induced by quantum fluctuations for an unknown intermediate range of spin values. Experiments indicate that spin3/2 ZnCr2O4 is "close" to the quantum critical point that separates the low spin quantumdisordered phase from the intermediate spin longrange ordered phase. Specifically, the relaxation rate for magnetic excitations, G, follows a powerlaw that extrapolates to zero as T approaches 0, indicating quantum criticality [3]. This state of affairs, however, does not persist to the lowest temperatures. Instead, at T_{N} = 12.5 K a first order structural transition from the cubic cooperative paramagnet to tetragonal Néel order intervenes.
Figure 2 shows that a gapless continuum of magnetic scattering above T_{N} is pushed into a local spin resonance at hw 4.5 meV J with remarkably little dispersion throughout the Brillouin zone. The result is analogous to the spinPeierls transition of the uniform spin1/2 chain, where quantum critical fluctuations are pushed into a finite energy singlettriplet transition through structural dimerization. Our recent synchrotron Xray and neutron powder experiments indicate that deformation of tetrahedra does indeed occur for ZnCr_{2}O_{4}. However, the structural changes push the system to long range order rather than to quantum disorder, as indicated by the magnetic Bragg peaks and spin wave excitations.
Our single crystal experiment [4] also enabled unique insight into the local structure of spinfluctuations in geometrically frustrated systems. Figure 3 shows the Qdependence of low energy magnetic scattering in two high symmetry planes above and below TN. While the spectrum for spin fluctuations changes dramatically at the first order phase transition, the structure factor clearly does not. Also shown in the figure is the structure factor for six spins of <111> type kagomé hexagons precessing with phase shift between neighbors. The proposal by O. Tchernyshyov et al. [5] that these are the dominant low energy spin fluctuation for spins on the Bsite spinel lattice is clearly borne out by the data.
The present data for ZnCr_{2}O_{4} show that geometrically frustrated lattices have composite low energy degrees of freedom analogous to rigid unit modes in certain open framework lattice structures. To better understand the unusual type of phase transition that occurs in this system, it must be determined what defines the 4.5 meV energy scale for hexagon excitation in the ordered phase. Do quantum fluctuations play a significant role or does the broken symmetry between exchange interactions within tetrahedra induce the resonance? The answer to this question is now being pursued through an accurate determination of the complex low temperature lattice and magnetic structure.
References:
[1] P.W. Anderson et al., Philos. Mag. 25, 1 (1972); J. Villain, Z. Phys. B 33, 31 (1979).
[2] R. Moessner et al., Phys. Rev. Lett. 80, 2929 (1998); B. Canals et al., Phys. Rev. Lett. 80, 2933 (1998).
[3] S.H. Lee, C. Broholm, T.H. Kim, W. Ratcliff II, and SW. Cheong, Phys. Rev. Lett. 84, 3718 (2000).
[4] S.H. Lee et al., unpublished (2001).
[5] O. Tchernyshyov et al., unpublished (2001).
Last modified 19March2003 by website owner: NCNR (attn: Jeff Krzywon)