Analysis API Reference¶
Advanced references for the analysis stack. The governed
research-lane registry currently classifies 74 ordinary
analysis/ and gauge/ modules by maturity, differentiable relevance, and
claim status.
This is an advanced module reference. Use Stable Facades API and Kuramoto Core Facade for first-path workflows, then drop into this page when a specific analysis probe or low-level diagnostic is needed.
Experimental QSL, Hamiltonian-learning, Koopman, minimum-QMI, magic, and SFF routes are governed by the Theory-Hook Promotion Matrix and its typed API. Importability does not grant control, differentiability, criticality, hardware, consciousness, or publication claims.
RL-adjacent witness discovery and the unimplemented pulse shell are governed by RL Research Governance and its typed API. Research execution is disabled by default and requires preregistration, fixed seeds, and explicit budgets.
The broader module inventory is enforced by
assert_research_lane_inventory(). Consult the
Research-lane Registry API before treating an
importable analysis helper as a supported integration surface.
Synchronization Detection¶
sync_order_parameter — Z-Basis Synchronisation Proxy¶
SyncOrderParameter consumes computational-basis counts and returns the absolute
mean Z-basis spin per shot. The compatibility key sync_order is preserved for
existing result artefacts, but it is an alias of sync_order_z_magnetisation.
The callable also emits is_xy_kuramoto_order_parameter = 0.0 because a counts-only
Z-basis record does not measure the continuous Kuramoto
\(R = \|(1/N)\sum_j(\langle X_j\rangle+i\langle Y_j\rangle)\|\).
from scpn_quantum_control.analysis.sync_order_parameter import SyncOrderParameter
observable = SyncOrderParameter()
result = observable({"000": 75, "111": 25})
assert result["sync_order"] == result["sync_order_z_magnetisation"]
assert result["is_xy_kuramoto_order_parameter"] == 0.0
Use analysis.sync_witness for X/Y-count witnesses and phase statevector
helpers for true Kuramoto-R calculations.
thermodynamic_witness — Calibrated Work Samples¶
ThermodynamicWitness summarizes explicitly supplied work values from a
calibrated protocol. It rejects counts-only calls and does not infer work from
bitstrings; callers must provide either work_samples_joule or work_joule.
All work, free-energy, and inverse-temperature inputs are validated at runtime
with explicit exceptions, so the fail-closed contract is unchanged under
optimized Python bytecode.
from scpn_quantum_control.analysis.thermodynamic_witness import ThermodynamicWitness
witness = ThermodynamicWitness()
result = witness(
counts={"0": 10, "1": 6},
work_samples_joule=[1.0e-21, 1.2e-21, 0.8e-21],
delta_free_energy_joule=0.9e-21,
beta_per_joule=2.5e20,
)
assert result["mean_work_joule"] > 0.0
assert "jarzynski_delta_free_energy_joule" in result
| Input | Requirement |
|---|---|
work_samples_joule |
Non-empty finite iterable of calibrated work samples |
work_joule |
Finite scalar work value when no sample iterable is supplied |
delta_free_energy_joule |
Optional finite free-energy difference |
beta_per_joule |
Optional finite positive inverse temperature |
sync_witness — Synchronization Witness Operators¶
Three Hermitian witness constructions that certify quantum synchronization from hardware measurement counts. No state tomography required.
from scpn_quantum_control.analysis.sync_witness import (
WitnessResult,
correlation_witness_from_counts,
fiedler_witness_from_counts,
fiedler_witness_from_correlator,
topological_witness_from_correlator,
evaluate_all_witnesses,
calibrate_thresholds,
)
| Function | Input | Output | Description |
|---|---|---|---|
correlation_witness_from_counts |
X/Y counts, n_qubits, threshold |
WitnessResult |
Mean pairwise XY correlator vs threshold |
fiedler_witness_from_counts |
X/Y counts, n_qubits, threshold |
WitnessResult |
Algebraic connectivity of correlation Laplacian |
fiedler_witness_from_correlator |
corr_matrix, threshold |
WitnessResult |
From pre-computed correlation matrix |
topological_witness_from_correlator |
corr_matrix, threshold, max_dim |
WitnessResult |
Persistent H₁ via Vietoris-Rips (requires ripser) |
evaluate_all_witnesses |
X/Y counts, n_qubits, thresholds |
dict[str, WitnessResult] |
All three witnesses from one measurement set |
calibrate_thresholds |
K, omega, K_base_range, n_samples |
dict[str, float] |
Classical Kuramoto calibration of thresholds |
WitnessResult fields: witness_name, expectation_value (negative = synchronised),
threshold, is_synchronized, raw_observable, n_qubits.
Full theory and examples: Research Gems — Gem 1.
witness_discovery — Automated Witness Search¶
Bayesian plus bandit search over Kuramoto control candidates, scored by the existing correlation and Fiedler synchronisation witnesses.
from scpn_quantum_control.analysis.witness_discovery import (
WitnessCandidate,
WitnessDiscoverySpec,
discover_kuramoto_witnesses,
score_witness_candidates,
)
| Function | Description |
|---|---|
discover_kuramoto_witnesses(K_nm, omega, theta0, spec) |
Run deterministic initial design, RBF Bayesian UCB, and bandit local exploration. |
score_witness_candidates(K_nm, omega, candidates) |
Score fixed candidates through the same witness objective. |
WitnessDiscoveryResult.ranked(limit) |
Return candidates sorted by descending witness score. |
The Rust path kuramoto_witness_candidate_features evaluates final order
parameter, mean pairwise correlation, and final phases for candidate batches.
The Python scorer then evaluates the existing witness objects, so the discovery
loop stays connected to the hardware-measurable witness definitions.
RLDiscoveryAgent is a compatibility wrapper around the same production search.
It accepts only the wired objective: correlation and Fiedler observables with
reward_function="witness_score", positive n_episodes, and no external
runner. Unsupported compatibility parameters fail at construction instead of
being silently ignored.
sync_entanglement_witness — R as Entanglement Witness¶
The Kuramoto order parameter \(R\) reinterpreted as an entanglement witness. For separable states, \(R \leq R_{\mathrm{sep}}\). Exceeding the separable bound certifies entanglement.
from scpn_quantum_control.analysis.sync_entanglement_witness import (
EntanglementWitnessResult,
R_entanglement_scan,
R_from_statevector,
R_separable_bound,
R_separable_bound_at_energy,
detect_entanglement_from_R,
)
| Function | Description |
|---|---|
R_from_statevector(psi, n_qubits) |
Compute \(R = \|(1/N)\sum_i(\langle X_i\rangle + i\langle Y_i\rangle)\|\) |
R_separable_bound(n_qubits) |
Maximum \(R\) achievable by any separable state (= 1.0) |
R_separable_bound_at_energy(K, omega, target_energy, n_samples=1000, seed=42, *, max_dense_gib=None) |
Dense exact max \(R\) over sampled product states at fixed energy |
detect_entanglement_from_R(K, omega, n_samples=2000, seed=42, *, max_dense_gib=None) |
Ground-state witness evaluation with dense exact small-system guard |
R_entanglement_scan(K, omega, K_base_range=None, n_K_values=15, n_samples=500, seed=42, *, max_dense_gib=None) |
Coupling scan of \(R_\mathrm{ground}\) and the energy-constrained separable bound |
The returned entanglement_depth is a certified lower bound from this witness:
1 when the separable bound is not violated and 2 when entanglement is
certified. The R witness alone does not certify stronger multipartite depth;
that requires separate k-producibility bounds or a dedicated depth witness.
critical_concordance — Multi-Probe \(K_c\) Agreement¶
Runs a finite-size dense exact coupling scan and compares where the order parameter, QFI, spectral gap, and concurrence-graph probes localise the same coupling region.
from scpn_quantum_control.analysis.critical_concordance import (
critical_concordance,
ConcordanceResult,
)
critical_concordance(omega, K_topology, k_range=None, concurrence_threshold=1e-4, *, max_dense_gib=None) returns ConcordanceResult with
fields: k_values, R_values, qfi_values, gap_values, fiedler_values,
n_entangled_pairs, k_c_from_gap, k_c_from_qfi, k_c_from_fiedler,
k_c_from_R_deriv, and concordance_spread.
Phase Transition Probes¶
qfi_criticality — Quantum Fisher Information at \(K_c\)¶
QFI diverges where the spectral gap closes — the synchronization transition is a metrological sweet spot.
from scpn_quantum_control.analysis.qfi_criticality import (
QFICriticalityResult,
qfi_single_coupling,
qfi_vs_coupling,
)
qfi_single_coupling(K, omega, *, max_dense_gib=None) returns the maximum
coupling-parameter QFI diagonal, spectral gap, and QFI trace for one dense exact
Kuramoto-XY Hamiltonian.
qfi_vs_coupling(omega, K_topology, k_range=None, *, max_dense_gib=None) returns
QFICriticalityResult with k_values, max_qfi, spectral_gap, total_qfi,
peak_k, and peak_qfi. The scan is dense exact and small-system only; pass
max_dense_gib to fail closed before Hamiltonian or derivative-operator
allocation.
sensing — S11 QFI-Criticality Readiness¶
Combines the QFI criticality scan with a classical sync-order Fisher proxy and a pair-level Cramer-Rao operating-point recommendation. This is a no-submit readiness surface, not hardware evidence.
from scpn_quantum_control.analysis.sensing import (
CriticalitySensingTail,
QuantumSensingReadinessConfig,
metrological_gain_vs_k,
optimal_sensing_k,
qfi_criticality_sensing_tail,
)
metrological_gain_vs_k(omega, topology, k_grid, *, config=None) returns a
SensingGainScan over the finite coupling grid. optimal_sensing_k(...) returns
the row with the largest QFI/classical-Fisher ratio.
qfi_criticality_sensing_tail(omega, topology, k_grid, *, measurements=10000,
geometric_epsilon=0.005, run_geometric_crosscheck=True, config=None) selects the
QFI peak, recomputes the full QFI matrix at that coupling, identifies the most
informative coupling-pair generator, reports the Cramer-Rao variance and standard
deviation bounds for the measurement budget, and records whether the spectral
route agrees with the geometric QGT cross-check.
entanglement_percolation — Finite-Size Entanglement Percolation¶
Compares the concurrence-graph percolation point with a selected finite-size order-parameter threshold. This is a dense exact diagnostic, not a standalone thermodynamic-limit proof.
from scpn_quantum_control.analysis.entanglement_percolation import (
percolation_scan,
PercolationScanResult,
)
percolation_scan(omega, K_topology, k_range=None, concurrence_threshold=1e-4, R_threshold=0.5, *, max_dense_gib=None) →
PercolationScanResult with: k_values, fiedler_values,
max_concurrence, mean_concurrence, n_entangled_pairs, R_values,
k_percolation, and k_sync.
berry_phase — Berry Connection and Fidelity Susceptibility¶
Finite-size dense exact scan of ground-state overlaps. On the one-dimensional open coupling path, the accumulated Berry connection is gauge-dependent; the fidelity and fidelity susceptibility are the gauge-invariant diagnostics.
berry_phase_scan(omega, K_topology, k_range=None, *, max_dense_gib=None) →
BerryPhaseResult with: k_values, berry_connection, berry_curvature,
accumulated_phase, fidelity, fidelity_susceptibility, spectral_gap,
and curvature_peak_k.
finite_size_scaling — Finite-Size Gap-Minimum Scaling¶
Fits finite-size gap-minimum estimates to a BKT-motivated \(K_c(N) = K_c(\infty) + a/(\ln N)^2\) ansatz and a power-law comparison model.
from scpn_quantum_control.analysis.finite_size_scaling import (
FSSFitDiagnostics,
finite_size_scaling,
FSSResult,
)
finite_size_scaling(system_sizes=None, k_range=None, *, max_dense_gib=None) → FSSResult
with: system_sizes, k_c_values, gap_min_values,
k_c_extrapolated_bkt, k_c_extrapolated_power, bkt_fit, power_fit,
and claim_boundary. The optional FSSFitDiagnostics records expose the
linearized ansatz name, extrapolated intercept, correction coefficient,
pointwise residuals, residual norm, maximum absolute residual, design-matrix
condition number, rank, point count, and the same non-promotional claim
boundary. By default the scan uses system sizes [2, 3, 4, 5].
system_sizes must be unique integer qubit counts from 2 through the available
frequency table; k_range must be one-dimensional, finite, strictly
increasing, and at least two points. The scan is local dense exact finite-size
evidence only, not hardware execution, isolated performance evidence, or a
thermodynamic-limit proof.
adiabatic_preparation — Adiabatic State Preparation¶
Finite-size dense exact adiabatic path from a weak-coupling initial ground state to the target XY Hamiltonian. Computes instantaneous gap and fidelity along the selected schedule.
adiabatic_ramp(omega, K_topology, K_target, T_total=10.0, n_steps=50, *, max_dense_gib=None) →
AdiabaticResult with: times, K_schedule, fidelity, gap,
final_fidelity, min_gap, min_gap_K.
The array fields are explicit float64 contracts; the dense evolution keeps
its internal statevector as complex128.
All numeric inputs must already be real numeric scalars or arrays; string,
boolean, object, and complex values are rejected before dense Hamiltonian
construction or fidelity/gap diagnostics.
Entanglement and Correlations¶
entanglement_entropy — Half-Chain Entropy and Schmidt Gap¶
Entanglement entropy and Schmidt gap across the synchronization transition. At BKT criticality, entropy follows CFT scaling \(S \sim (c/3)\ln L\) with \(c = 1\).
from scpn_quantum_control.analysis.entanglement_entropy import (
entanglement_vs_coupling,
EntanglementScanResult,
)
entanglement_vs_coupling(omega, K_topology, k_range=None) →
EntanglementScanResult with: k_values, entropy, schmidt_gap,
spectral_gap, entropy_peak_K, schmidt_gap_min_K.
Rust acceleration: Hamiltonian construction via build_xy_hamiltonian_dense (Qiskit-free).
entanglement_spectrum — Full Entanglement Spectrum¶
Computes the full entanglement spectrum (all Schmidt coefficients) and estimates the CFT central charge from the entropy scaling.
from scpn_quantum_control.analysis.entanglement_spectrum import (
entanglement_spectrum,
cft_central_charge,
)
pairing_correlator — Richardson Pairing \(\langle S^+_i S^-_j\rangle\)¶
Detects Richardson pairing (the superconducting analogue of synchronization) via spin-raising/lowering correlators. Strong pairing = synchronised phase.
from scpn_quantum_control.analysis.pairing_correlator import (
pairing_map,
pairing_vs_anisotropy,
PairingResult,
)
pairing_map(omega, K_topology, K_base, delta=0.0, *, max_dense_gib=None) →
PairingResult with the full pairing matrix, maximum/mean pairing, topology
correlation, qubit count, anisotropy, and base coupling.
pairing_vs_anisotropy(omega, K_topology, K_base, delta_range=None, *, max_dense_gib=None)
forwards the dense budget to every XXZ ground-state solve in the scan.
Quantum Chaos and Dynamics¶
otoc — Out-of-Time-Order Correlator¶
Core OTOC computation: \(F(t) = \langle W^\dagger(t) V^\dagger W(t) V\rangle\).
compute_otoc(K, omega, times, w_qubit=0, v_qubit=None) → OTOCResult with:
times, otoc_values, lyapunov_estimate, scrambling_time.
Rust acceleration: When scpn_quantum_engine is installed, OTOC uses eigendecomposition
+ rayon-parallel time loop (\(O(d^2)\) per time point vs \(O(d^3)\) scipy.expm). Hamiltonian
construction uses build_xy_hamiltonian_dense (bitwise, Qiskit-free). 10-50× faster for n ≤ 8.
otoc_sync_probe — OTOC Scan Across \(K_c\)¶
Scans OTOC diagnostics vs coupling strength to detect the synchronization transition via chaos measures.
otoc_sync_scan(K, omega, K_base_range=None, n_K_values=15, t_max=2.0) →
OTOCSyncScanResult with: K_base_values, lyapunov_values, scrambling_times,
otoc_final_values, R_classical, peak_scrambling_K.
spectral_form_factor — SFF and Level Statistics¶
Exact finite-system spectral-form-factor and adjacent-gap-ratio diagnostics. Interpretation requires a specified symmetry sector, ensemble, energy window, null distribution, and finite-size protocol; these values do not by themselves certify quantum chaos or a Poisson-to-RMT transition.
from scpn_quantum_control.analysis.spectral_form_factor import (
compute_sff,
sff_vs_coupling,
SFFResult,
SFFScanResult,
)
| Function | Description |
|---|---|
compute_sff(K, omega, t_max=20.0, n_times=200, *, level_spacing_basis="magnetisation", magnetisation=None, parity=None, max_dense_gib=None) |
Full-spectrum normalized SFF plus selected-sector and full-spectrum gap ratios |
sff_vs_coupling(omega, K_topology, k_range=None, ..., max_dense_gib=None) |
Finite coupling-grid diagnostics; chaos_onset_K is a heuristic threshold crossing only |
The default spacing ratio is resolved in a U(1) magnetisation sector. The SFF
itself still uses the full spectrum, and both selected-sector and full-spectrum
ratios remain explicit in SFFResult.
loschmidt_echo — Loschmidt Echo and DQPT¶
Dynamical Quantum Phase Transitions detected via non-analyticities in the Loschmidt return rate \(\lambda(t) = -\ln\mathcal{L}(t)/N\).
loschmidt_echo(K, omega, K_i, K_f, times) → LoschmidtResult with:
times, echo_values, return_rate, dqpt_times (cusp locations).
Rust acceleration: Hamiltonian construction via build_xy_hamiltonian_dense (Qiskit-free).
krylov_complexity — Operator Spreading Complexity¶
Lanczos coefficients \(b_n\) and Krylov complexity \(C_K(t) = \sum_n n |\phi_n(t)|^2\). Maximum at \(K_c\).
from scpn_quantum_control.analysis.krylov_complexity import (
krylov_complexity,
krylov_vs_coupling,
KrylovResult,
)
krylov_complexity(H, O_init, t_max=10.0, n_times=100, max_lanczos=50) →
KrylovResult with Lanczos coefficients, times, complexity values, peak
complexity, and realised Krylov dimension.
krylov_vs_coupling(omega, K_topology, k_range=None, t_max=10.0, n_times=50, *, max_dense_gib=None)
builds the dense Hamiltonian/probe workspace under the caller's budget before
scanning peak complexity against coupling.
Rust acceleration: Lanczos b-coefficients computed via lanczos_b_coefficients (complex
matrix commutator loop in Rust, 5-10× for dim ≤ 256). Hamiltonian via build_xy_hamiltonian_dense.
Quantum Information Measures¶
qfi — Quantum Fisher Information Matrix¶
Full QFI matrix for parameter estimation precision bounds.
from scpn_quantum_control.analysis.qfi import (
quantum_fisher_information,
spectral_gap,
precision_bounds,
)
| Function | Description |
|---|---|
quantum_fisher_information(state, generators) |
QFI matrix \(F_{ij}\) |
spectral_gap(H) |
\(E_1 - E_0\) |
precision_bounds(qfi_matrix) |
Cramér-Rao lower bounds \(\delta\theta_i \geq 1/\sqrt{F_{ii}}\) |
QuantumFisherInformation is the observable-wrapper adapter for production
metrology calls. When coupling_matrix and natural_frequencies are supplied
it routes to the spectral QFI engine and validates that the coupling matrix is
square, symmetric, finite-valued, and dimension-compatible with the frequency
vector. Optional coupling_pairs must be distinct in-range integer index pairs,
and n_measurements must be a positive integer because it rescales the
Cramér-Rao precision bound. Counts-derived sync/DLA estimates are exposed only
through the explicit allow_proxy_estimate=True diagnostic path and are labelled
as proxy values, never as production QFI.
magic_nonstabilizerness — Stabilizer Rényi Entropy¶
Exact small-system stabilizer Rényi-2 resource diagnostic \(M_2 = -\log_2(\sum_P \langle P\rangle^4 / 2^N)\). The implementation enumerates all \(4^N\) Pauli strings. A finite-grid maximum is not a critical-point estimator, a fault-tolerant resource-cost certificate, or evidence of classical hardness or quantum advantage.
from scpn_quantum_control.analysis.magic_nonstabilizerness import (
magic_at_coupling,
magic_vs_coupling,
MagicResult,
)
magic_at_coupling(omega, K_topology, K_base, *, max_dense_gib=None) computes
the dense exact ground state and Stabilizer Renyi entropy at one coupling.
magic_vs_coupling(omega, K_topology, k_range=None, *, max_dense_gib=None)
forwards the dense eigensolver budget to every coupling point and returns a
MagicScanResult with the scanned values and peak location.
quantum_phi — Minimum Bipartite Quantum Mutual Information¶
compute_quantum_phi(K, omega) is a compatibility-named routine that computes
quantum mutual information over all non-trivial bipartitions of the exact
Kuramoto-XY ground state. It reports the minimum and maximum QMI plus the
minimum-information partition. It does not compute Integrated Information
Theory Φ: there is no causal model, intervention repertoire, cause-effect
structure, or IIT composition/exclusion calculation.
IntegratedInformationPhi is the dashboard-facing wrapper. When supplied with
coupling_matrix and natural_frequencies, it fails closed unless
allow_mutual_information_proxy=True is explicit. The diagnostic returns
minimum_bipartite_mutual_information, sets phi_available = 0.0 and
is_integrated_information = 0.0, and never returns a phi key. Counts-only
entropy similarly requires allow_entropy_proxy=True.
This route is tier D research-only and authorises no consciousness, sentience, cognition, or clinical interpretation. See the Theory-Hook Promotion Matrix.
shadow_tomography — Classical Shadow Estimation¶
\(O(\log M)\) shots for \(M\) observables via random Clifford measurements.
from scpn_quantum_control.analysis.shadow_tomography import (
random_clifford_shadow,
estimate_observable,
ShadowResult,
)
quantum_speed_limit — Bounded State-Evolution Speed Limits¶
compute_qsl(...) evaluates a Mandelstam–Tamm target-overlap bound and a legacy
Margolus–Levitin orthogonalization-time reference from
the frequency-encoded product state and records the first simulated crossing
of a visibility-aware local-phase-order threshold. The threshold time is a
finite closed-system diagnostic, not a measured synchronisation time, critical
exponent, or BKT certificate.
When the simulated target is not orthogonal to the initial state, tau_ML is
not an arbitrary-fidelity lower bound for that target. The compatibility field
remains explicitly labelled until an extended Margolus–Levitin contract is
implemented and tested.
qsl_vs_coupling(K, omega, K_base_range=None, n_K_values=15, t_target=5.0,
R_threshold=0.5, *, max_dense_gib=None) returns finite-grid K_base,
tau_MT, tau_ML, tau_actual, delta_E, and R_final lists. The scan does
not fit a critical point or distinguish BKT from power-law scaling.
Topological Analysis¶
quantum_persistent_homology — Full PH Pipeline¶
Hardware counts → correlation matrix → distance → Vietoris-Rips → persistence diagram → \(p_{H_1}\).
from scpn_quantum_control.analysis.quantum_persistent_homology import (
counts_to_persistence,
coupling_scan_persistence,
PersistenceResult,
PersistenceScanResult,
)
| Function | Description |
|---|---|
counts_to_persistence(x_counts, y_counts, n_qubits, max_dim=1) |
Single-point PH from hardware counts |
coupling_scan_persistence(K, omega, K_range, ...) |
\(p_{H_1}\) vs coupling strength |
persistent_homology — Classical PH Utilities¶
Distance matrix construction, Rips filtration, Betti number extraction.
h1_persistence — Vortex Density at BKT¶
\(H_1\) persistence as a function of coupling — the topological order parameter for the BKT transition.
vortex_binding — Kosterlitz RG Flow¶
Vortex-antivortex binding energy and Kosterlitz renormalization group flow equations.
Algebraic Structure¶
dynamical_lie_algebra — DLA Computation¶
Computes the Dynamical Lie Algebra and its dimension for the Kuramoto-XY Hamiltonian. Result: \(\dim(\mathrm{DLA}) = 2^{2N-1} - 2\) for non-degenerate frequencies.
compute_dla(K, omega) → DLAResult with: generators (list of Pauli strings),
dimension, n_qubits, predicted_dim (\(2^{2N-1} - 2\)).
dla_parity_theorem — Z₂ Parity Proof¶
Formal verification that Z₂ parity is the only symmetry of the heterogeneous XY Hamiltonian.
from scpn_quantum_control.analysis.dla_parity_theorem import (
verify_z2_parity,
ParityTheoremResult,
)
BKT Phase Analysis¶
bkt_analysis — Core BKT Diagnostics¶
Fiedler eigenvalue, \(T_{\mathrm{BKT}}\), \(p_{H_1}\) prediction from coupling structure.
bkt_universals — Candidate Expressions for the Open \(p_{H_1}\) Threshold¶
Systematic negative-control search over candidate expressions for the open empirical/theoretical \(p_{H_1}=0.72\) threshold. The square-lattice expression is the closest numerical fit, but the K_nm graph check keeps the threshold open.
p_h1_derivation — \(A_{HP} \times \sqrt{2/\pi}\) Negative Control¶
Audits the square-lattice coincidence and records why it does not derive the K_nm graph threshold. The current status remains open rather than promoted.
p_h1_open_guard — Public Open-Claim Guard¶
Scans outward-facing Markdown for wording that would turn the open
empirical/theoretical \(p_{H_1}=0.72\) parameter into a closed derivation,
universal constant, or measured TCBO reproduction. The guard is runnable through
scripts/check_p_h1_open_claim_guard.py.
phase_diagram — \(K_c\) vs \(T_{\mathrm{eff}}\) Boundary¶
Full synchronization phase diagram in the coupling-temperature plane.
xxz_phase_diagram — \(K_c\) vs Anisotropy \(\Delta\)¶
Finite-size gap-minimum diagnostics in the \((K, \Delta)\) plane from XY-like (\(\Delta=0\)) to Heisenberg-like (\(\Delta=1\)) Hamiltonians.
from scpn_quantum_control.analysis.xxz_phase_diagram import (
anisotropy_phase_diagram,
PhaseDiagramResult,
)
anisotropy_phase_diagram(omega, K_topology, delta_range=None, k_range=None, *, max_dense_gib=None) → PhaseDiagramResult
with: delta_values, k_c_values, gap_min_values, and scans.
Open Quantum Systems¶
quantum_mpemba — Quantum Mpemba Effect¶
Ordered states thermalize faster under amplitude damping — the quantum Mpemba effect in synchronization dynamics.
mpemba_experiment(omega, K, K_base=1.0, gamma=0.1, t_max=5.0, n_steps=50) →
MpembaResult with: times, fidelity_ground, fidelity_plus (|+⟩^N),
mpemba_detected (True if |+⟩ thermalizes faster).
lindblad_ness — Non-Equilibrium Steady State¶
Lindblad NESS under amplitude damping: the long-time limit that retains synchronization signatures.
ness_vs_coupling(K, omega, gamma=0.1, K_base_range=None, n_K=15) → NESSResult
with: K_values, R_ness (order parameter of NESS), purity_ness, entropy_ness.
Reservoir Computing¶
qrc_phase_detector — Exact QRC-Style Feature Map¶
The Kuramoto-XY Hamiltonian supplies exact dense ground-state Pauli features for a ridge-regression classifier. This is a deterministic small-system feature-map reference, not a scalable reservoir simulator.
from scpn_quantum_control.analysis.qrc_phase_detector import (
qrc_phase_detection,
QRCPhaseResult,
)
qrc_phase_detection(omega, K_topology, k_train, k_test, k_threshold, alpha=0.1, max_weight=2, *, max_dense_gib=None) →
QRCPhaseResult with: accuracy, n_train, n_test, n_features,
weights, and k_boundary_predicted.
Classical Simulations¶
monte_carlo_xy — Classical XY Monte Carlo¶
Metropolis Monte Carlo for the classical XY model. Uses the Rust engine
(scpn_quantum_engine) when available; falls back to pure Python.
graph_topology_scan — Coupling Graph Analysis¶
Network topology metrics (clustering, betweenness, modularity) of the \(K_{nm}\) matrix.
koopman — Koopman Linearisation¶
Finite, reference-point-dependent Koopman-style closure over phase identities
and pairwise sine/cosine observables. Higher-order terms are truncated, so the
matrix and its spectrum are classical local-baseline diagnostics, not an exact
finite invariant subspace or full nonlinear dynamics. The Hermitian projection
i(L-L†)/2 discards the symmetric part of L; it does not establish dynamical
equivalence, BQP-completeness, or quantum advantage.
build_koopman_generator_rust() now routes to the optional
scpn_quantum_engine.koopman_generator kernel when that export is present and
falls back to the validated NumPy generator otherwise. Set require_rust=True
when a benchmark or release gate must prove that the native kernel, not the
fallback, served the dense generator.
hamiltonian_learning — Recover \(K_{nm}\) from Measurements¶
learn_hamiltonian(C_measured, omega, K_init=None, maxiter=100) performs a
small dense fit of a symmetric non-negative coupling matrix to supplied exact
ground-state XX+YY correlators. It uses COBYLA, not compressed sensing.
The input name preserves compatibility but does not establish measurement provenance. A low in-sample residual is not an identifiability, uncertainty, held-out, noise-robustness, or experimental-recovery certificate.
hamiltonian_self_consistency — Self-Consistency Loop¶
Round-trip verification: \(K_{nm}\) → Hamiltonian → ground state → correlators → \(K_{nm}^{\mathrm{eff}}\).
from scpn_quantum_control.analysis.hamiltonian_self_consistency import (
self_consistency_check,
correlator_shot_noise,
SelfConsistencyResult,
)
enaqt — Environment-Assisted Quantum Transport¶
enaqt_scan(...) evolves a single excitation over the site Hamiltonian
diag(omega) + K, with local dephasing, an irreversible target sink, and an
optional competing loss channel. It maximises finite-horizon sink population,
not a Kuramoto phase proxy. The result records explicit efficiency fields, the
exact zero-dephasing endpoint, the largest-scanned-gamma endpoint, and a strict
intermediate-optimum classification. Legacy *_r fields remain read-only
aliases only.
The trace-preserving Lindblad generator is applied through
scipy.sparse.linalg.expm_multiply; max_dense_gib gates the site-basis
density workspace before Hamiltonian allocation. See
ENAQT Optimal-Noise Scan for equations, evidence,
primary citations, negative controls, and the no-setpoint boundary.
entanglement_enhanced_sync — Entangled Initial-State Coherence Study¶
simulate_sync_trajectory(K, omega, state_type, t_max=2.0, n_steps=20, *, max_dense_gib=None)
evolves product, Bell-pair, GHZ, or W initial states under the dense exact
Kuramoto-XY Hamiltonian. It records a visibility-aware local phase order and a
separate pairwise transverse-exchange-coherence score. When local transverse
visibility vanishes, phase_defined is false and the compatibility R value
is zero; the historical false atan2(0, 0) -> R=1 mapping is removed.
compare_all_initial_states(K, omega, t_max=2.0, n_steps=20, *, max_dense_gib=None)
uses one budgeted exact propagator for all pure states.
compare_initial_states_with_dephased_controls(...) adds population-matched
computational-basis-dephased controls and retains the separable product row as
an attribution control. entanglement_advantage(...) is a compatibility name
that now returns descriptive differences with a BL-65 no-advantage
certificate; it does not report speedup or an entanglement-specific effect.
See Entangled initial-state coherence study for equations, committed evidence, primary-source scope, and limitations.