Geometrical frustration in the pyrochlore lattice: spin liquids and spin ices

Figure 1. Susceptibility components versus T in Ho2Ti2O7 (top) and Yb2Ti2O7 (bottom). Dashed lines: CEF-only calculation; solid lines: calculation including an effective exchange. In Yb2Ti2O7, the anisotropy of the molecular field due to the exchange is reversed with respect to the crystal field anisotropy (XY type). From Ref. [2]

*In chemically ordered compounds with short-range magnetic interactions, geometrical frustration appears when all interactions cannot be satisfied simultaneously due to the lattice geometry. A well-known example is a triangle of antiferromagnetically coupled spins. This frustration results in a strong degeneracy of the ground state, since many configurations have the same energy. It now appears as a powerful ingredient for designing materials or tuning physical properties, since frustrated magnetic states may be easily switched by small changes in the energy balance. Pyrochlores R _{2}Ti_{2}O_{7} (where R^{3+} is a rare earth ion) are model systems showing exotic short-range magnetic orders called “spin liquids” and “spin ices”, with unconventional excitations akin to magnetic monopoles, and a huge sensitivity to perturbations. Various aspects have been studied in collaborations with P. Bonville and A. Forget (IRAMIS/SPEC, Saclay), G. Dhalenne and C. Decorse (ICMMO, Orsay), and H. Mutka (ILL, Grenoble).*

**Local susceptibility in R_{2}Ti_{2}O_{7} pyrochlores (R = Tb, Ho, Yb, Er)**

Rare earth titanate pyrochlores of *Fd*-3*m* space group, where the *R*^{3+} ions occupy the summits of corner-sharing tetrahedra and the Ti^{4+} ions are nonmagnetic, show very different ground states, such as spin-liquid (Tb) and spin-ice (Ho) states, short range orders, planar antiferromagnetism (Er), and 2D ferromagnetism (Yb). Their physics is governed by the exchange and dipolar interactions between the *R*^{3+} ions, together with the crystal-field anisotropy along the <111> axes. The study of the paramagnetic state under applied fields points to precursor effects of these ground states. Single-crystal polarized neutron diffraction gives access to the local susceptibility tensor in the Gukasov-Brown model [1], which reduces to 2 components χ_{//} and χ_{⊥} with respect to the <111> local axis, owing to the high symmetry the *R*^{3+} site. This allows one to describe the complex field-induced structures using only two parameters. This tensor cannot be derived from the bulk magnetization due to the equivalent <111> axes. Measurements performed in four typical cases where the *R-R* interactions may be F or AF, and the crystal-field anisotropy either Ising- or *XY*-type, showed that the local susceptibility is highly anisotropic (Figure 1). This is the first determination of the local susceptibility in the Ho_{2}Ti_{2}O_{7} spin ice with (F, Ising) behavior. Comparison with a calculation of the non-interacting susceptibility deduced from the crystal-field scheme (measured independently by inelastic neutron scattering) yields the tensor of exchange interactions, which is also found to be anisotropic [2]. As a surprising consequence, in Yb_{2}Ti_{2}O_{7} with (F, *XY*) behavior, crystal-field and exchange anisotropies nearly compensate, yielding a Curie susceptibility and ground state fluctuations in an original “exchange spin-ice” ground state [3].

[1] Determination of atomic site susceptibility tensors from polarized neutron diffraction data, A. Gukasov and J. Brown, J. Phys. Condens. Matter **14**, 8831, (2002).

[2] *Ising versus XY Anisotropy in Frustrated R _{2}Ti_{2}O_{7} Compounds as “Seen” by Polarized Neutrons*, H. Cao, A. Gukasov, I. Mirebeau, P. Bonville, C. Decorse, G. Dhalenne, Physical Review Letters

[3]* Anisotropic exchange in frustrated pyrochlore Yb _{2}Ti_{2}O_{7}*

H. Cao, A. Gukasov, I. Mirebeau, P. Bonville, J. Phys. Cond. Mat. Fast Track,

**Evolution of the spin liquid Tb _{2}Ti_{2}O_{7} ground state under applied field**

Tb_{2}Ti_{2}O_{7} realizes the (AF, uniaxial) case with a highly tunable spin-liquid ground state, which is easily destabilized by an applied field, pressure, or magnetic substitution. This tunability results from the peculiar Tb^{3+ }crystal field scheme, with two low-energy doublets easily populated by temperature, or mixed by the magnetic field, and from *R-R* effective (dipolar + exchange) interactions at the border between the F and AF characters. Starting from the spin-liquid ground state, a magnetic field close to a <110> axis splits the system into two sublattices (*α* and *b* chains) and induces spin-ice–like local structures with ** k** = 0 propagation vector, but with different moment values on the two sublattices [1]. Above 2 teslas, magnetic structures with

[1] *Field-Induced Spin-Ice-Like Orders in Spin Liquid Tb _{2}Ti_{2}O_{7}*

H. Cao, A. Gukasov, I. Mirebeau, P. Bonville, Phys. Rev. Lett.

[2] T. Fennell et al. Nature Physics **3**, 566 (2007); D. J. P. Morris et al., Science **326**, 411, (2009).

Figure 2. Magnetic diffraction pattern in Tb2Sn2O7 ordered spin ice, at 0.06 K under a pressure of 4.6 GPa. Together with the Bragg peaks of the ordered spin ice [k0 = 0 propagation vector, fcc lattice], new antiferromagnetic Bragg peaks [k1=(0,0,1) propagation vector, simple cubic lattice] appear under pressure. Top: the spin structures corresponding to the refinement (solid lines). From Ref.[2]

**An ordered spin ice Tb _{2}Sn_{2}O_{7} under high pressure**

Starting from the Tb_{2}Ti_{2}O_{7} spin liquid, substitution of Ti by Sn yields a lattice expansion and the onset of an ordered spin-ice state. The change in the energy balance is understood as follows: the lattice expansion favors the dipolar (F) Tb–Tb interactions at the expense of the (AF) superexchange interactions, since superexchange depends more strongly on interatomic distances. The ordered or “soft” spin ice, whose anisotropy is reduced in comparison with the true spin ice, has the local spin ice spin structure (mathematically identical to proton order in water ice) but not its degeneracy, since all tetrahedra of the pyrochlore structure have the same orientations. This leads to long-range order, ferromagnetic magnetization, and intricate spin dynamics [1]. What happens when one pressurizes a soft spin ice? We observed three effects: a reorientation of the spin-ice structure, the onset of antiferromagnetic order, and the enhancement of spin-liquid fluctuations [2]. It is worth noting that only the soft spin ice Tb_{2}Sn_{2}O_{7 }is sensitive to pressure (Figure 2). In the true spin ice Ho_{2}Ti_{2}O_{2}, although theory predicts a pressure tuning of the magnetic monopoles, it was not observed up to now. Very high pressures are likely necessary to disturb the crystal- field scheme and exchange interactions.

[1] *Investigation of magnetic fluctuations in Tb*_{2}Sn_{2}O_{7} ordered spin ice by high-resolution energy-resolved neutron scattering

I. Mirebeau, H. Mutka, P. Bonville, A. Apetrei A. Forget, Phys. Rev. B 78, 174416, (2008)

[2] *Magnetic order in Tb _{2}Sn_{2}O_{7} under high pressure: From ordered spin ice to spin liquid and antiferromagnetic order*

I. Mirebeau, I. Goncharenko, H. Cao, A. Forget, Physical Review B, Rapid Commun.

Maj : 13/09/2013 (1991)