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arXiv:2505.06478 · Leibniz international proceedings in informatics

Hamiltonian Locality Testing via Trotterized Postselection

John Kallaugher, Daniel Liang

Published Jan 1, 2025• 1 citation
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Abstract

The (tolerant) Hamiltonian locality testing problem, introduced in [Bluhm, Caro,Oufkir `24], is to determine whether a Hamiltonian $H$ is $\varepsilon_1$-close to being $k$-local (i.e. can be written as the sum of weight-$k$ Pauli operators) or $\varepsilon_2$-far from any $k$-local Hamiltonian, given access to its time evolution operator and using as little total evolution time as possible, with distance typically defined by the normalized Frobenius norm. We give the tightest known bounds for this problem, proving an $\text{O}\left(\sqrt{\frac{\varepsilon_2}{(\varepsilon_2-\varepsilon_1)^5}}\right)$ evolution time upper bound and an $Ω\left(\frac{1}{\varepsilon_2-\varepsilon_1}\right)$ lower bound. Our algorithm does not require reverse time evolution or controlled application of the time evolution operator, although our lower bound applies to algorithms using either tool. Furthermore, we show that if we are allowed reverse time evolution, this lower bound is tight, giving a matching $\text{O}\left(\frac{1}{\varepsilon_2-\varepsilon_1}\right)$ evolution time algorithm.

DOI
10.4230/lipics.tqc.2025.10

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We consider the problems of testing and learning an n -qubit Hamiltonian H=∑xλxσxH=\sum _x \lambda _x \sigma _xH=∑x​λx​σx​ expressed in its Pauli basis, from queries to its evolution operator U=e−iHtU=e^{-iHt}U=e−iHt . To this end, we prove the following results. Testing : We give a tolerant testing protocol to decide if a Hamiltonian is ε1\varepsilon _1ε1​ -close to k -local or ε2\varepsilon _2ε2​ -far from k -local in the ℓ2\ell _2ℓ2​ norm of the coefficients, with O(1/(ε2−ε1)4)O(1/(\varepsilon _2-\varepsilon _1)^{4})O(1/(ε2​−ε1​)4) queries, thereby solving two open questions posed in a recent work by Bluhm, Caro and Oufkir (Bluhm, A., Caro, M.C., Oufkir, A.). We give a protocol for testing whether a Hamiltonian is ε1\varepsilon _1ε1​ -close to being s -sparse or ε2\varepsilon _2ε2​ -far from being s -sparse in the ℓ2\ell _2ℓ2​ norm of the coefficients, with O(s6/(ε22−ε12)6)O(s^{6}/(\varepsilon _2^2-\varepsilon _1^2)^{6})O(s6/(ε22​−ε12​)6) queries. Learning : We give a protocol to ε\varepsilon ε -learn unstructured Hamiltonian in the ℓ∞\ell _\infty ℓ∞​ norm of the coefficients with O(1/ε4)O(1/\varepsilon ^4)O(1/ε4) queries. Combining this with the non-commutative Bohnenblust-Hille inequality, we obtain an algorithm for learning k -local Hamiltonians in ℓ2\ell _2ℓ2​ norm of the coefficients that only uses O(exp⁡(k2+klog⁡(1/ε)))O(\exp (k^2+k\log (1/\varepsilon )))O(exp(k2+klog(1/ε))) queries. For Hamiltonians that are s -sparse in the Pauli basis, we can learn them in the ℓ2\ell _2ℓ2​ norm with O(s2/ε4)O(s^2/\varepsilon ^4)O(s2/ε4) queries. Learning without quantum memory : The learning results stated above have no dependence on the system size n , but require n -qubit quantum memory. We give subroutines that allow us to reproduce all the above learning results without quantum memory; squaring the query complexity and paying a (log⁡n)(\log n)(logn) -factor in the local case and an n -factor in the sparse case. Testing without quantum memory : We give a new subroutine called Pauli hashing , which allows one to tolerantly test s -sparse Hamiltonians in the ℓ2\ell _2ℓ2​ norm using O~(s14/(ε22−ε12)18)\tilde{O}(s^{14}/(\varepsilon _2^2-\varepsilon _1^2)^{18})O~(s14/(ε22​−ε12​)18) query complexity. A key ingredient is showing that s -sparse Pauli channels can be tested in a tolerant fashion as being ε1\varepsilon _1ε1​ -close to being s -sparse or ε2\varepsilon _2ε2​ -far under the diamond norm, using O~(s2/(ε2−ε1)6)\tilde{O}(s^2/(\varepsilon _2-\varepsilon _1)^6)O~(s2/(ε2​−ε1​)6) queries via Pauli hashing. In order to prove these results, we prove new structural theorems for local Hamiltonians, sparse Pauli channels and sparse Hamiltonians. We complement our learning algorithms with lower bounds that are polynomially weaker. Furthermore, our algorithms use short time evolutions and do not assume prior knowledge of the terms on which the Pauli spectrum is supported on, i.e., we do not require prior knowledge of the support of the Hamiltonian.
We establish lower bounds for Hamiltonian property testing with access to the time-evolution operator but not its inverse. Each experiment may query the time-evolution operator multiple times, and distances between Hamiltonians are measured in the normalized Frobenius norm. In this model, we show that testing whether a Hamiltonian is kkk-local or ε\varepsilonε-far from every kkk-local Hamiltonian requires Ω(1/ε2)Ω(1/\varepsilon^2)Ω(1/ε2) total evolution time, matching the upper bound of Kallaugher and Liang (TQC'25). We also prove that testing whether an unknown Hamiltonian equals a target Hamiltonian or is ε\varepsilonε-far from it requires Ω(1/ε2)Ω(1/\varepsilon^2)Ω(1/ε2) total evolution time, matching the upper bound of Sinha and Tong (2025). These are the first lower bounds for natural problems in Hamiltonian learning and testing that rule out Heisenberg-limited scaling of 1/ε1/\varepsilon1/ε. As a third result, we show that amplitude estimation to precision ε\varepsilonε requires Ω(1/ε2)Ω(1/\varepsilon^2)Ω(1/ε2) total time evolution, recovering the result of Tang and Wright (QIP'26) in the continuous-time query model. All three results follow from the hardness of distinguishing the zero Hamiltonian from a suitably chosen ensemble of random Hamiltonians. We establish this hardness by adapting the continuous-time adversary method to forward Hamiltonian evolution.
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We consider the problems of testing and learning an unknown n -qubit quantum Hamiltonian H =∑ x λ x σ x expressed in its Pauli basis, from queries to its evolution operator e − iHt under the normalized Frobenius norm. To this end, we prove the following results (with and without quantum memory) for Hamiltonians whose Pauli spectrum involves only k -local terms or has sparsity at most s : (1) Local Hamiltonians : We give a tolerant testing protocol to decide if a Hamiltonian is ε 1 -close to k -local or ε 2 -far from k -local, with O (1/(ε 2 −ε 1 ) 4 ) queries, thereby solving two open questions posed in a recent work by Bluhm, Caro and Oufkir [BCO’24]. For learning a k -local Hamiltonian up to error ε, we give a protocol with query complexity and total time evolution exp( O ( k 2 + k log(1/ε))). Our algorithm leverages the non-commutative Bohnenblust-Hille inequality in order to get a complexity independent of n . (2) Sparse Hamiltonians : We give a protocol for testing whether a Hamiltonian is ε 1 -close to being s -sparse or ε 2 -far from being s -sparse, with O ( s 6 /(ε 2 2 −ε 1 2 ) 6 ) queries. For learning up to error ε, we show that O ( s 4 /ε 8 ) queries suffices. (3) Learning without quantum memory : The learning results stated above have no dependence on the system size n , but require n -qubit quantum memory. We give subroutines that allow us to reproduce all the above learning results without quantum memory; increasing the query complexity by a (log n )-factor in the local case and an n -factor in the sparse case. (4) Testing without quantum memory : We give a new subroutine called Pauli hashing , which allows one to tolerantly test s -sparse Hamiltonians using Õ( s 14 /(ε 2 2 −ε 1 2 ) 18 ) query complexity. A key ingredient is showing that s -sparse Pauli channels can be tested in a tolerant fashion as being ε 1 -close to being s -sparse or ε 2 -far under the diamond norm, using Õ( s 2 /(ε 2 −ε 1 ) 6 ) queries via Pauli hashing. In order to prove these results, we prove new structural theorems for local Hamiltonians, sparse Pauli channels and sparse Hamiltonians. We complement our learning algorithms with lower bounds that are polynomially weaker. Furthermore, our algorithms use short time evolutions and do not assume prior knowledge of the terms on which the Pauli spectrum is supported on, i.e., we do not require prior knowledge about the support of the Hamiltonian terms.