Abstract
The excitation spectrum of the antiferromagnetic spin-1/2 Heisenberg Hamiltonian H=tsumJSj on L×L lattices is evaluated by a projector quantum Monte Carlo method. These results suggest that the exact spectrum for the finite lattice is ωZ(L)ωkSW, for all k, where ωkSW=4JS 1-γk2 with γk=(coskx+cosky)/2 is from linear-spin-wave theory. We find Z(L)=ZE+B/L3, leading to ZE=1.21±0.03 for L=. A comparison with experiments on La2CuO4 is discussed.
| Original language | English |
|---|---|
| Pages (from-to) | 2933-2938 |
| Number of pages | 6 |
| Journal | Physical Review B |
| Volume | 46 |
| Issue number | 5 |
| DOIs | |
| Publication status | Published - 1 Jan 1992 |
| Externally published | Yes |
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