We investigate the magnetic properties of the Cu-O planes in stoichiometric Sr_n-1{Cu}ₙ₊₁O₂ₙ (n=3,5,7, . . .) which consist of CuO double chains periodically intergrown within the CuO₂ planes. The double chains break up the two-dimensional antiferromagnetic planes into Heisenberg spin ladders with nᵣ=1/2(n-1) rungs and nₗ=1/2(n+1) legs and described by the usual antiferromagnetic coupling J inside each ladder and a weak and frustrated interladder coupling J'. The resulting lattice is a new two-dimensional trellis lattice. We first examine the spin excitation spectra of isolated quasi-one-dimensional Heisenberg ladders which exhibit a gapless spectrum when nᵣ is even and nₗ is odd (corresponding to n=5,9, . . .) and a gapped spectrum when nᵣ is odd and nₗ is even (corresponding to n=3,7, . . .). We use the bond operator representation of quantum S=1/2 spins in a mean-field treatment with self-energy corrections and obtain a spin gap of {}1/2J for the simplest single-rung ladder (n=3), in agreement with numerical estimates. We also present results of the dynamical structure factor S(q,{ω}). The spin gap decreases considerably on increasing the width of the ladders. For a double ladder with four legs and three rungs (n=7) we obtain a spin gap of only 0.1J. However, a frustrated coupling, such as that of a trellis lattice, introduced between the double ladders leads to an enhancement of the gap. Thus stoichiometric Sr_n-1{Cu}ₙ₊₁O₂ₙ compounds with n=3,7,11, . . ., will be frustrated quantum antiferromagnets with a quantum-disordered or spin-liquid ground state.
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Gopalan et al. (1994) studied this question.
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