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SAXS — Small-Angle X-ray Scattering L1-126

Scientific InstrumentationNanoscale structural scattering (1-100 nm)δ=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

X-rays scatter elastically at small momentum transfer q = 4*pi*sin(theta)/lambda < 0.5 Å^-1 from inhomogeneities ~ 2*pi/q nm. Radially integrated intensity I(q) encodes pair-distance distribution function P(r) via Fourier transform (Fourier-Bessel). For biomolecules, provides radius of gyration Rg and maximum dimension Dmax.

L-DAG

L.scatter.elastic -> L.project.q -> int.angular
L.scatter.elasticL.project.qint.angular

Well-posedness W

Existence:
true
Uniqueness:
Rg, Dmax unique up to buffer matching; 3D shape ambiguous (envelope only)
Stability:
conditional
κ:
500

Inverse Fourier transform from I(q) to P(r) is ill-posed (ATSAS-GNOM uses regularization); shape reconstruction requires ab-initio bead models. Mismatch: aggregation, polydispersity, buffer mismatch.

Solvability C

Solver class:
Guinier fit (Rg), GNOM (indirect FT), DAMMIN/DAMMIF (bead ab-initio), EOM (ensemble models), learned (BIFT, SAX-ML)
Convergence rate q:
2
Complexity:
Guinier O(N_q); GNOM O(N_r * N_q); DAMMIF O(iter * N_beads * N_q)

Specs (0)

No L2 specs registered yet for this principle.