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The published data set of Madsen et al., Nature 606, 75 (2022) (Apache-2.0), all five instances, held to the engine's exact Gaussian-state computations, a signed receipt per run. The module gains what the experiment needs, each tested against exact small cases: - GaussianState::through: squeezed, thermal or squashed inputs through any subunitary transfer matrix (a different loss on every path); an amplifying matrix is refused. - Loops: a time-domain interferometer of fibre loops from its program. It rebuilds every published T and U (16 to 288 modes) to within 2.3e-16 per entry. - photon_moments (exact first- and second-order photon-number cumulants) and photon_number_distribution (the exact total-photon distribution, from the eigenvalues of I - Q^-1 and the generating function on the unit circle; it holds at 576 x 576). In every total, the hafnian probabilities sum to it within 3e-15. - photon_table: what every pattern probability needs, computed once; photon_probability keeps its bits (bit_identity unchanged). examples/gbs_loops.rs reads the pinned data set (wai/tools/quantum-gbs/fetch.sh). tests/gbs_reference.rs holds the receipts to the published values and re-runs the 16-mode comparison up to four photons bit for bit. - 16 modes, 84,096,000 samples: fidelity 99.87-99.66%, total variation distance 3.95-6.51% for three to six photons (paper: >99%, <=6.5%). The sample count alone gives 0.4-3.0%. Thermal, squashed and coherent light are farther off in every total. - The stated means reproduce: 21.120 +- 0.006, 22.416 +- 0.006, 124.35 +- 0.02, max 219. - The ground truth explains the pair cumulants best in all five instances. - Fig. 3b's Bayesian scores for 10-14 photons are above zero against thermal, squashed and coherent light. Co-Authored-By: Claude Opus 5.5 <[email protected]> |
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