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Neutron Radiography and Tomography L1-130

Scientific InstrumentationNeutron transmission imaging complementary to X-rayδ=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 collimated thermal (2.5 meV) or cold (1 meV) neutron beam traverses the sample; attenuation is governed by mu_n(r, lambda) = Sigma_tot = n * sigma_tot (Sigma ~ 1/E for thermal). Neutrons excel at light elements (H, Li, B, Cd) hidden behind heavy metals (Pb, W) where X-rays fail. Scintillator (LiF/ZnS:Ag) + CCD or MCP+Timepix records transmitted beam.

L-DAG

L.absorb.lambert -> L.project.ray -> int.spatial
L.absorb.lambertL.project.rayint.spatial

Well-posedness W

Existence:
true
Uniqueness:
Radon inversion unique with full-angle coverage; limited angle ill-posed
Stability:
conditional
κ:
200

Beer-Lambert linear; CT reconstruction via FBP/ASTRA. Mismatch: beam hardening (lambda-dependent), scatter, flux inhomogeneity, motion.

Solvability C

Solver class:
FBP, iterative SART, TV-regularized ASTRA, learned (DnCNN denoise, FBP-ConvNet)
Convergence rate q:
2
Complexity:
FBP O(N^2 * log N); SART O(N_iter * N_ray * N_voxel)

Specs (0)

No L2 specs registered yet for this principle.