Barren Plateaus in Quantum Linear Combinations: Interference and Lie-Algebraic Control
Organizations: Division of Engineering Science, University of Toronto · Department of Computer and Mathematical Sciences, University of Toronto Scarborough · Department of Electrical and Computer Engineering, University of Toronto
Abstract
A coherent sum of quantum circuits introduces interference that can alter the training signal. We distinguish a single linear combination of unitaries (LCU) from a circuit that repeatedly alternates branch operations and ancilla mixing. For a single-pass LCU, independent branches with zero matrix means cannot erase the differentiated branch's gradient variance: the total variance is at least the branch variance times the fourth power of its coefficient magnitude. This bound holds at any gate position and does not require the circuit unitaries to be Haar-random. Beyond this lower bound, we derive exact loss and gradient formulas that quantify the additional contributions from interference between branches. One of these terms depends on relative coefficient phases and vanishes when the branch ensemble is invariant under multiplication by ; a four-qubit matchgate example shows that it can be nonzero. For repeated interleaving with full special-unitary ancilla control, we determine the generated Lie algebra from the associative algebra of the branches, including the available central phase directions. This control result predicts concentration only with additional assumptions on circuit sampling. Matchgate examples exhibit polynomial single-pass LCU variances and exponential concentration under joint Haar-random sampling. We also derive coefficient-selection rules and bounds for postselection, measurement error, and approximate moments.
Figures & tables
| Symbol | Lives in | Definition | Role |
|---|---|---|---|
| DLA of branch (branch layer) | |||
| ; equal to for fixed coefficients | DLA of the coefficient layer, acting on the ancilla alone | ||
| diagonal ancilla generators: no mixing between branches | |||
| coefficient layer embedded in the joint space | |||
| branch layer embedded in the joint space; block diagonal in the ancilla index | |||
| coefficient directions already supplied by the branch layer |
| Argument | Hypotheses to check | Proof location |
|---|---|---|
| Gradient floor, Proposition 4.1 | Fixed coefficients; independent branch data; zero means of the other branches; finite second moments | Section 4.1 |
| Single-pass LCU loss and pairings | Independence and zero means for the decomposition; required Haar-measure moments for invariant pairings | Appendix B |
| Single-pass LCU and joint gradients | Stated gate placement and ensemble factorization for closed forms; membership for sector formulas | Appendix C |
| Bounds, saturation, graph control | Specified generator families; full special-unitary mixer for saturation; central directions for the exact upper bound | Appendix D |
| Joint-space variance | Joint first and second moments; state or observable membership for the sector formula | Appendix E |
| Matchgate and Pauli examples | Actual branch groups and envelopes; specified input, observable, and ensemble | Appendix F |
Barren Plateaus
Barren plateaus are quantum-circuit optimization landscapes where gradients vanish with system size, hindering the training of variational algorithms.
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