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Isometric tensor network optimization for extensive Hamiltonians is free of barren plateaus

Published 27 Apr 2023 in quant-ph, cond-mat.str-el, and physics.comp-ph | (2304.14320v2)

Abstract: We explain why and numerically confirm that there are no barren plateaus in the energy optimization of isometric tensor network states (TNS) for extensive Hamiltonians with finite-range interactions which are, for example, typical in condensed matter physics. Specifically, we consider matrix product states (MPS) with open boundary conditions, tree tensor network states (TTNS), and the multiscale entanglement renormalization ansatz (MERA). MERA are isometric by construction and, for the MPS and TTNS, the tensor network gauge freedom allows us to choose all tensors as partial isometries. The variance of the energy gradient, evaluated by taking the Haar average over the TNS tensors, has a leading system-size independent term and decreases according to a power law in the bond dimension. For a hierarchical TNS (TTNS and MERA) with branching ratio $b$, the variance of the gradient with respect to a tensor in layer $\tau$ scales as $(b\eta)\tau$, where $\eta$ is the second largest eigenvalue of a Haar-average doubled layer-transition channel and decreases algebraically with increasing bond dimension. The absence of barren plateaus substantiates that isometric TNS are a promising route for an efficient quantum-computation-based investigation of strongly-correlated quantum matter. The observed scaling properties of the gradient amplitudes bear implications for efficient TNS initialization procedures.

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  1. For a system of L𝐿Litalic_L sites, the expectation value ⟨Ψ|h^1⊗h^2⊗⋯⊗h^L|Ψ⟩quantum-operator-productΨtensor-productsubscript^ℎ1subscript^ℎ2⋯subscript^ℎ𝐿Ψ\langle\Psi|\hat{h}_{1}\otimes\hat{h}_{2}\otimes\dotsb\otimes\hat{h}_{L}|\Psi\rangle⟨ roman_Ψ | over^ start_ARG italic_h end_ARG start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ⊗ over^ start_ARG italic_h end_ARG start_POSTSUBSCRIPT 2 end_POSTSUBSCRIPT ⊗ ⋯ ⊗ over^ start_ARG italic_h end_ARG start_POSTSUBSCRIPT italic_L end_POSTSUBSCRIPT | roman_Ψ ⟩ for normalized states ΨΨ\Psiroman_Ψ is simply minimized by the tensor product |Ψ⟩=|ψ1⟩⊗⋯⊗|ψL⟩ketΨtensor-productketsubscript𝜓1⋯ketsubscript𝜓𝐿|\Psi\rangle=|\psi_{1}\rangle\otimes\dotsb\otimes|\psi_{L}\rangle| roman_Ψ ⟩ = | italic_ψ start_POSTSUBSCRIPT 1 end_POSTSUBSCRIPT ⟩ ⊗ ⋯ ⊗ | italic_ψ start_POSTSUBSCRIPT italic_L end_POSTSUBSCRIPT ⟩ of the lowest-eigenvalue eigenstates ψisubscript𝜓𝑖\psi_{i}italic_ψ start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT of the single-site Hamiltonians h^isubscript^ℎ𝑖\hat{h}_{i}over^ start_ARG italic_h end_ARG start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT. The same holds for sums ⟨Ψ|∑i=1Lh^i|Ψ⟩quantum-operator-productΨsuperscriptsubscript𝑖1𝐿subscript^ℎ𝑖Ψ\langle\Psi|\sum_{i=1}^{L}\hat{h}_{i}|\Psi\rangle⟨ roman_Ψ | ∑ start_POSTSUBSCRIPT italic_i = 1 end_POSTSUBSCRIPT start_POSTSUPERSCRIPT italic_L end_POSTSUPERSCRIPT over^ start_ARG italic_h end_ARG start_POSTSUBSCRIPT italic_i end_POSTSUBSCRIPT | roman_Ψ ⟩ of single-site Hamiltonians.
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