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Raman Imaging (spontaneous inelastic photon scattering) L1-137

SpectroscopyVibrational hyperspectral microscopyδ=3 · standardL_DAG = 2.7📋 Stub — not mineable
📋

Unclaimed Principle — open for contribution

This Principle is declared in the catalog but has no reference solver, no pinned dataset, and is not registered on-chain. There is no reward pool. Submitting a cert against this Principle today will record the cert for reproducibility but pay zero PWM.

To claim it as a Bounty #7 contribution: open a PR adding (1) a reference solver, (2) ≥1 dataset pinned to IPFS, (3) updates to the L3 manifest with dataset CIDs. After verifier-agent triple-review, the founders' 3-of-5 multisig signs PWMRegistry.register() and the Principle becomes mineable.

Forward model E

A narrowband laser at omega_L excites a sample; vibrational modes at frequencies omega_v cause inelastic scattering at omega_L +/- omega_v (Stokes/anti-Stokes). The cross-section is ~10^-30 cm^2/molecule/steradian (1e7 weaker than fluorescence). A spectrograph disperses scattered light onto a 2D detector, measured per spatial position via raster scan or line-focus.

L-DAG

S.scatter.inelastic -> L.disperse.spectral -> int.temporal
S.scatter.inelasticL.disperse.spectralint.temporal

Well-posedness W

Existence:
true
Uniqueness:
identifiable under linear-mixing with known sigma_k
Stability:
conditional
κ:
200

Linear inverse problem mapping concentration to spectral signal; conditioning governed by spectral overlap (correlation of pure-component spectra). Mismatch: fluorescence background, wavenumber drift, laser-power fluctuation.

Solvability C

Solver class:
Classical-least-squares (CLS), NNMF, MCR-ALS, VCA, SVM classification, U-Net / spectral-transformer learned unmixing
Convergence rate q:
2
Complexity:
CLS: O(H*W*K*N_lambda); MCR-ALS: O(iter * H*W*K*N_lambda); learned single forward

Specs (0)

No L2 specs registered yet for this principle.