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We identify a large class of quantum many-body systems that can be solved exactly: natural frustration-free spin-1/2 nearest-neighbor Hamiltonians on arbitrary lattices.
B. S. Shastry, B. Sutherland, Physica B 108
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J. Eisert and H. J. Briegel, Phys. Rev. A 64
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F. Verstraete, J. I. Cirac, and V. Murg, Adv. Phys. 57
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K. M. R. Audenaert, J. Eisert, M. B. Plenio, and R. F. Werner, Phys. Rev. A 66
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G. Vidal, Phys. Rev. Lett. 99
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S. Bravyi, quant-ph/0602108
Cited in the paper.
R. Movassagh, E. Farhi, J. Goldstone, D. Nagaj, T. J. Osborne, and P. W. Shor, arXiv:1001.1006
Cited in the paper.
We similarly accumulate any single-spin contributions in H U ′ H^{\prime}_{U} which arise from single-spin contributions in H U H_{U}
Cited in the paper.
While we effectively ignore single-spin terms in our analysis, such terms do impose constraints on the ground state manifold, and thus on whether the Hamiltonian is frustration free. However, these may be accounted for with little difficulty
Cited in the paper.
S. Bravyi, M. B. Hastings, and S. Michalakis, arXiv:1001.0344
Cited in the paper.
However, for systems whose ground states have very localized correlations, estimating with respect to a subspace spanned by a small number of product states may scale poorly for large systems. For instance, when the variational set 𝒦 \mathcal{K} is the symmetric subspace Symm ( ℂ N ) \Symm(\mathbb{C}^{N}) , the very symmetry of states in 𝒦 \mathcal{K} entails that correlations do not decay spatially but rather are constant
Cited in the paper.
The approach taken here is also expected to work for slightly frustrated Hamiltonians reminiscent of Shastry-Sutherland-type models
Cited in the paper.
One could also perform more sophisticated quantum circuits, such as constant-depth quantum circuits or partial MERA reductions: there will then exist a trade-off between accuracy of the simulation and the efficiency of the procedure
Cited in the paper.
P. Silvi, V. Giovannetti, S. Montangero, M. Rizzi, J. I. Cirac, and R. Fazio, arXiv:0912.0466
Cited in the paper.
D. Aharonov, D. Gottesman, S. Irani, and J. Kempe, Comm. Math. Phys. 287
2009
Later among the works it cites.
J. Eisert, M. Cramer, and M. B. Plenio, Rev. Mod. Phys. 82
2010
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C. R. Laumann, A. M. Läuchli, R. Moessner, A. Scardicchio, and S. L. Sondhi, arXiv:0910.2058
2058
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