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Operators · VQE Hamiltonians and observables

Commuting observable group

Measurement partition for shared basis estimation. Representative form: G_k={P_j : [P_i,P_j]_qw=0}.

Attested & literatureUpdated

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  • Primary sourceVerteletskyi, Yen & Izmaylov 2019, §II A
  • RelationQubit-wise commutativity, Eq. (4)
  • Not an equivalence relationTransitivity fails
  • Papers1

This record, used inside a worked example

This page says To use this record in VQE — here is a concrete, runnable instance of it.

VQE on a 2-qubit transverse-field Ising Hamiltonian

2 qubits, H = Z⊗Z + 0.5*(X⊗I + I⊗X), a stated toy Hamiltonian (not a molecule), minimised with a hardware-efficient ansatz.

q0q1RY(π/2)RY(5π/4)CXRY(0)RY(0)

Where it ends up

  • 1043%
  • 0143%
  • 007%
  • 117%

At these angles the ansatz's energy ⟨H⟩ reaches E0 = −√2, the Hamiltonian's exact ground energy; a real VQE run reaches these angles by repeating measure-the-energy then update-the-angles, not by a closed-form solution.

Open that example in Studio

The relation is not the one this record used to state. Its form was Gk={Pj:[Pi,Pj]=0}G_k = \{P_j : [P_i,P_j] = 0\} — ordinary commutativity — and the cited paper shows that is the wrong condition. Two Pauli words that commute need not be simultaneously measurable by single-qubit projective measurements, and the paper's own counterexample is [x^1x^2,y^1y^2]=0[\hat{x}_1\hat{x}_2, \hat{y}_1\hat{y}_2] = 0 while the two are not qubit-wise commuting. Their common eigenstates are entangled superpositions rather than product states, so no set of single-qubit measurements resolves both. The relation that does the work is the qubit-wise commutator of Eq. (4), which vanishes only when every single-qubit factor of PIP_I commutes with its counterpart in PJP_J. Qubit-wise commuting implies commuting; the converse fails.

The property worth knowing about this object is that it is not a partition. Qubit-wise commutativity is reflexive and symmetric but not transitive — the paper's example is [x^1,y^2]qw=0[\hat{x}_1,\hat{y}_2]_{qw} = 0 and [y^2,z^1]qw=0[\hat{y}_2,\hat{z}_1]_{qw} = 0 while [x^1,z^1]qw≠0[\hat{x}_1,\hat{z}_1]_{qw} \neq 0. So it is not an equivalence relation, there are no equivalence classes, and a Hamiltonian has no unique grouping of its terms.

That is why the object is a group in the loose sense and never a partition, and it is the reason the optimization problem is a minimum clique cover over a graph rather than a sort into buckets. Represent each Pauli word as a vertex and join qubit-wise commuting pairs by an edge; a set of mutually measurable terms is then a clique, and the best grouping is a minimum cover by cliques — which the paper notes is NP-hard, hence the heuristics.

Why this record exists beside the method record, which cites the same paper. It was written to test whether it should. The answer is that the two carry different halves and neither is the other's summary: the algebraic facts above — which relation, why it is not transitive, why no unique grouping exists — are properties of the object and hold whatever procedure you use. What belongs to vqe-measurement-grouping instead is the procedure and its measured result: which heuristics were benchmarked, and that grouping reduced the operator count roughly threefold against the total number of Hamiltonian terms. An object record that repeated the threefold figure would be restating the method from the object's side, and this one does not.

References

Attested & literature
  • Peer-reviewed paper
Method
arXiv:1907.03358 was read end to end, specifically to test whether an object record can say anything a method record citing the same paper does not.
Result
Pass, and one correction shipped · the form was [Pᵢ,Pⱼ]=0 and is now the qubit-wise commutator, because the paper shows plain commutativity does not give simultaneous single-qubit measurability.
Caveat
Indices, coefficients, basis conventions, mappings, and units are instance dependent and must be recorded in an executable experiment.
Measurement Optimization in the Variational Quantum Eigensolver Using a Minimum Clique Cover ↗
Kind
curated reference
Reviewed by
Leona Quantum curation pass
License
Citation metadata only; source publication terms apply
VQE operatorHamiltoniancommuting observable groupqubit-wise commutativityminimum clique cover

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