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Stochastic Quantum Sampling for Non-Logconcave Distributions and Estimating Partition Functions
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Gives quantum simulated-annealing samplers for non-logconcave Gibbs distributions based on ULA (full and stochastic gradients) and a quantum partition-function estimator, using MALA as a reversible bridge for the analysis.
Problem
Quantum sampling from possibly non-logconcave Gibbs distributions exp(-beta f(x)) with finite-sum f, where ULA is non-reversible and existing quantum walk spectral-gap analyses do not apply; also estimating partition functions for such distributions.
Approach
Quantum simulated annealing over a sequence of Gaussian-tempered targets, with quantum walk operators built from unadjusted Langevin transitions (optionally with mini-batch stochastic gradients); the error from replacing the reversible MALA walk by the non-reversible ULA walk is bounded via Hellinger distance and a perturbation analysis, using MALA as a hypothetical reversible bridge.
Key results
- Quantum MALA samples with Õ(βd ρ^-1 c_LSI^-1) queries to full gradient and evaluation oracles.
- Quantum ULA needs Õ(β d^{3/2} ε^-1 ρ^-1 c_LSI^-1) full-gradient queries, versus classical ULA Õ(d/ε^2) per the paper's comparison table.
- Stochastic quantum ULA needs Õ(β^2 d^{3/2} ε^-2 ρ^-2 c_LSI^-1) mini-batch oracle queries, each with O(d) gradient calculations (total Õ(d^{5/2}/ε^2) gradient evaluations).
Measured effects reported in the paper
| What was changed | Where | Measured | Effect |
|---|---|---|---|
| Use quantum simulated annealing with MALA walks instead of classical MALA sampling | Non-logconcave Gibbs sampling · Non-logconcave Gibbs sampling | dimension dependence of query complexity: \tilde{O}(d^{2}) -> \tilde{O}(d ) | Helped |
| Use quantum ULA instead of classical ULA | Non-logconcave Gibbs sampling · Non-logconcave Gibbs sampling | dimension dependence of query complexity: \tilde{O}(d/\epsilon^2) -> \tilde{O}(d^{3/2}/\epsilon) | Helped |
| Use stochastic-gradient quantum ULA rather than classical SGLD | Non-logconcave Gibbs sampling · Non-logconcave Gibbs sampling | dimension dependence of query complexity: \tilde{O}(d^4/\epsilon^2) -> \tilde{O}(d^{5/2}/\epsilon^2) | Helped |
| Replace the full-gradient oracle with a stochastic-gradient oracle | Quantum ULA · Non-logconcave Gibbs sampling | oracle access cost | Mixed |
Surprising findings
- The quantum walk for non-reversible ULA can be analyzed despite no detailed balance, by bounding its deviation from a reversible MALA bridge chain.
Limitations
- Results are theoretical query-complexity bounds with no implementation or experiments.
- Stochastic variant's gradient complexity scales as d^{5/2}/ε^2 and carries stronger dependence on ρ and β.
- Assumes smoothness and dissipativeness; relies on Cheeger and log-Sobolev constants that may be exponential in dimension for general f.
Experimental setup
Metrics: query complexity total variation distance
Baselines: classical ULA classical MALA SGLD quantum MALA
Builds on: Childs et al. quantum MALA via simulated annealing Szegedy quantum walk Metropolis-adjusted Langevin algorithm fixed-point amplitude amplification
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