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docs: add superconductivity Allen-Dynes source gate
Merge superconductivity Allen-Dynes source gate, source-policy acceptance, verifier artifacts, and CI skip guards for absent platform projects.
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‎.github/workflows/ci.yml‎

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steps:
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- uses: actions/checkout@v4
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- name: Detect Rust workspace
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id: rust-workspace
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run: |
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if [ -f Cargo.toml ]; then
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echo "present=true" >> "$GITHUB_OUTPUT"
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else
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echo "present=false" >> "$GITHUB_OUTPUT"
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echo "No root Cargo.toml found; skipping Rust checks for this corpus-only checkout."
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fi
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- name: Install Rust
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if: steps.rust-workspace.outputs.present == 'true'
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uses: dtolnay/rust-toolchain@stable
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with:
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components: clippy, rustfmt
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- name: Cache cargo
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if: steps.rust-workspace.outputs.present == 'true'
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uses: actions/cache@v4
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with:
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path: |
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${{ runner.os }}-cargo-
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- name: Check formatting
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if: steps.rust-workspace.outputs.present == 'true'
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run: cargo fmt --all -- --check
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- name: Clippy
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if: steps.rust-workspace.outputs.present == 'true'
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run: cargo clippy --workspace --all-targets -- -D warnings
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continue-on-error: true
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- name: Build
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if: steps.rust-workspace.outputs.present == 'true'
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run: cargo build --release --workspace
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# ==================== Next.js Frontend ====================
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steps:
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- uses: actions/checkout@v4
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- name: Detect Next.js app
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id: next-app
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working-directory: .
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run: |
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if [ -f uet_web/package-lock.json ]; then
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echo "present=true" >> "$GITHUB_OUTPUT"
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else
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echo "present=false" >> "$GITHUB_OUTPUT"
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echo "No uet_web/package-lock.json found; skipping Next.js checks for this corpus-only checkout."
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fi
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- name: Setup Node.js
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if: steps.next-app.outputs.present == 'true'
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uses: actions/setup-node@v4
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with:
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node-version: '20'
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cache: 'npm'
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cache-dependency-path: './uet_web/package-lock.json'
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- name: Install dependencies
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if: steps.next-app.outputs.present == 'true'
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run: npm ci --legacy-peer-deps
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- name: Lint
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if: steps.next-app.outputs.present == 'true'
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run: npm run lint
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continue-on-error: true
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- name: Build
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if: steps.next-app.outputs.present == 'true'
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run: npm run build
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env:
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NEXT_TELEMETRY_DISABLED: 1

‎docs/data/external/condensed_matter/superconductivity/row_resolution_targets/a15_adjacent_phonon_context_report.json‎

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{
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"schema_version": "1.0",
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"source_class": "external_adjacent_phonon_context_report",
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"checked_date": "2026-05-12",
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"scope": "Adjacent phonon-context literature that may help the next A15 live capture pass without being promoted to canonical row evidence",
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"materials": [
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{
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"material": "Nb3Sn",
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"adjacent_sources": [
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{
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"title_or_doi": "10.1103/PhysRevB.19.4023",
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"article_title": "Phonon dispersion in Nb3Sn",
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"role": "adjacent phonon-context source",
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"note": "This source appears useful for understanding specific softened phonon modes in Nb3Sn, but it is not the canonical table-layer source currently chosen for the benchmark-row phonon capture."
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}
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]
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},
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{
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"material": "Nb3Ge",
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"adjacent_sources": [
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{
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"title_or_doi": "IBM Research: Large anisotropic vibrational correlations in A15 Nb3Ge",
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"article_title": "Large anisotropic vibrational correlations in A15 Nb3Ge",
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"role": "adjacent phonon-context source",
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"note": "This source appears useful for qualitative vibrational context in Nb3Ge, but it is not the canonical table-layer source currently chosen for the benchmark-row phonon capture."
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}
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]
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}
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],
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"practical_result": "Adjacent phonon-context literature is now pinned for both A15 rows, which may help orient a future full-text pass if the canonical source remains difficult to capture, but these sources still do not replace the chosen canonical row-capture path.",
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"claim_boundary": "This report holds search-guidance context only. It does not certify any numeric value and does not unblock patch review."
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}

‎docs/data/external/condensed_matter/superconductivity/row_resolution_targets/a15_field_extraction_plan.json‎

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{
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"schema_version": "1.0",
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"source_class": "external_field_extraction_plan",
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"source_role": "execution-ready field extraction plan for the A15 residual blocker pair",
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"source_label": "A15 field extraction plan for Nb3Sn and Nb3Ge",
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"checked_date": "2026-05-07",
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"materials": [
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{
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"material": "Nb3Sn",
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"steps": [
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{
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"order": 1,
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"field": "Tc_observed",
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"preferred_reference": "10.1103/PhysRev.95.1435",
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"target_capture": [
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"explicit Tc statement or row",
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"table_or_figure_identifier or equivalent text locator",
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"unit_basis = K"
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],
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"success_condition": "A repo-local archive entry can point to one exact Tc statement or row from the primary publication anchor."
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},
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{
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"order": 2,
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"field": "Theta_D_K_or_omega_log_K",
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"preferred_reference": "10.1103/PhysRevB.27.1568",
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"target_capture": [
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"phonon-spectrum moment or omega_log style row if present",
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"proxy convention note",
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"unit_basis = K"
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],
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"success_condition": "One explicit phonon proxy convention is archived and can be named in topic review."
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},
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{
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"order": 3,
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"field": "lambda_ep",
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"preferred_reference": "10.1016/0378-4363(84)90167-0",
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"target_capture": [
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"explicit lambda or e-ph parameter statement",
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"locator for the lambda source row or text statement",
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"compatibility note against the chosen phonon proxy convention"
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],
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"success_condition": "A lambda value or named coupling statement is archived from a source that is compatible with the chosen A15 proxy convention."
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},
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{
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"order": 4,
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"field": "mu_star",
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"preferred_reference": null,
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"target_capture": [
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"row-specific source if available",
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"otherwise explicit family-convention note"
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],
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"success_condition": "The review packet can say honestly whether mu_star is row-specific or retained as a family convention."
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}
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]
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},
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{
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"material": "Nb3Ge",
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"steps": [
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{
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"order": 1,
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"field": "Tc_observed",
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"preferred_reference": "10.1063/1.1654966",
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"target_capture": [
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"explicit Tc statement or row",
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"table_or_figure_identifier or equivalent text locator",
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"unit_basis = K"
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],
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"success_condition": "A repo-local archive entry can point to one exact Tc statement or row from the primary publication anchor."
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},
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{
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"order": 2,
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"field": "Theta_D_K_or_omega_log_K",
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"preferred_reference": "10.1103/PhysRevB.27.1568",
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"target_capture": [
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"phonon-spectrum moment or omega_log style row if present",
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"proxy convention note",
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"unit_basis = K"
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],
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"success_condition": "One explicit phonon proxy convention is archived and can be named in topic review."
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},
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{
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"order": 3,
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"field": "lambda_ep",
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"preferred_reference": "10.1016/0378-4363(84)90167-0",
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"target_capture": [
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"explicit lambda or e-ph parameter statement",
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"locator for the lambda source row or text statement",
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"compatibility note against the chosen phonon proxy convention"
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],
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"success_condition": "A lambda value or named coupling statement is archived from a source that is compatible with the chosen A15 proxy convention."
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},
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{
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"order": 4,
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"field": "mu_star",
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"preferred_reference": null,
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"target_capture": [
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"row-specific source if available",
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"otherwise explicit family-convention note"
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],
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"success_condition": "The review packet can say honestly whether mu_star is row-specific or retained as a family convention."
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}
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]
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}
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],
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"claim_boundary": "This plan sequences extraction work only. It does not certify any captured value until the archive and topic handoff gates are passed."
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}

‎docs/data/external/condensed_matter/superconductivity/row_resolution_targets/a15_first_live_capture_target_packet.json‎

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{
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"schema_version": "1.0",
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"source_class": "external_pair_first_live_capture_target_packet",
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"pair_label": "A15 residual blocker pair",
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"checked_date": "2026-05-12",
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"purpose": "Identify and track the single first live numeric capture target across the A15 pair without requiring the operator to reconstruct priority from multiple workflow files.",
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"current_status": "first_live_capture_value_obtained_pending_review",
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"selected_first_target": {
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"material": "Nb3Sn",
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"field": "Theta_D_K_or_omega_log_K",
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"reason_for_selection": [
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"Nb3Sn remains the strongest A15 shortcut candidate.",
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"Its phonon field was the narrowest decisive blocker before the abstract-level lambda=1.5 capture could gain more practical weight, and it now has a provisional Table II value pending review.",
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"The PRB source family already says phonon moments are tabulated and prefers omega_log-style interpretation over Debye temperature."
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],
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"execution_packet": "docs/data/external/condensed_matter/superconductivity/row_resolution_targets/nb3sn_phonon_first_numeric_execution_packet.json",
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"critical_blocker_packet": "docs/data/external/condensed_matter/superconductivity/row_resolution_targets/nb3sn_phonon_critical_blocker_packet.json",
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"numeric_capture_record": "docs/data/external/condensed_matter/superconductivity/row_resolution_targets/nb3sn/phonon_numeric_capture_record.json",
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"acceptance_gate": "docs/data/external/condensed_matter/superconductivity/row_resolution_targets/nb3sn_phonon_capture_acceptance_gate.json",
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"live_capture_attempt_template": "docs/data/external/condensed_matter/superconductivity/row_resolution_targets/nb3sn_phonon_live_capture_attempt_template.json",
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"live_capture_bundle": "docs/data/external/condensed_matter/superconductivity/row_resolution_targets/nb3sn_phonon_live_capture_bundle.json"
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},
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"what_success_looks_like": [
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"One row-specific phonon numeric value is captured for Nb3Sn; this is now provisionally satisfied by Nb3Sn I omega_log=127 K from Table II.",
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"The capture records archived_raw_path, locator fields, quoted text, and unit basis.",
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"The capture explicitly states whether the accepted proxy is omega_log or another phonon moment.",
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"The downstream Nb3Sn lambda=1.5 abstract capture can then be reviewed against a resolved same-family phonon convention."
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],
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"what_not_to_do": [
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"Do not treat abstract-only convention text as if it were the phonon numeric capture.",
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"Do not promote the abstract-level lambda value to row-usable status before the Nb3Sn phonon convention is resolved.",
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"Do not skip to Nb3Ge lambda before the first Nb3Sn phonon pass is attempted."
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],
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"claim_boundary": "This packet records that the first live capture target has produced a provisional value. It does not certify that value as benchmark-ready and does not unblock patch review by itself."
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}

‎docs/data/external/condensed_matter/superconductivity/row_resolution_targets/a15_fulltext_table_target_map.json‎

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{
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"schema_version": "1.0",
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"source_class": "external_fulltext_table_target_map",
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"source_role": "maps the most likely full-text table or section targets for the next A15 numeric extraction pass",
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"source_label": "A15 full-text table target map",
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"checked_date": "2026-05-11",
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"materials": [
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{
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"material": "Nb3Sn",
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"targets": [
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{
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"field": "Tc_observed",
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"source_title_or_doi": "10.1103/PhysRev.95.1435",
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"host_layer": "APS abstract and full article",
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"target_section_hint": "Abstract first, then discovery discussion or measurement summary in full text",
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"why_this_section": "The abstract already exposes the Tc statement; the full-text pass should now confirm exact page context and row identity."
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},
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{
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"field": "Theta_D_K_or_omega_log_K",
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"source_title_or_doi": "10.1103/PhysRevB.27.1568",
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"host_layer": "OSTI summary and full PRB article",
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"target_section_hint": "Tables or sections containing experimentally determined moments of the phonon spectra, especially omega_log, because the abstract says these values are tabulated",
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"why_this_section": "The primary-host abstract explicitly says phonon-spectrum moments including omega_log are included and tabulated, and also says Debye temperature is generally a bad estimate of omega_log."
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},
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{
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"field": "lambda_ep",
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"source_title_or_doi": "10.1016/0378-4363(84)90167-0",
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"host_layer": "ScienceDirect abstract and full article",
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"target_section_hint": "Sections, tables, or figures reporting alpha^2F(omega), full phonon dispersion, or explicit lambda values for Nb3Sn",
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"why_this_section": "The abstract confirms that Nb3Sn-specific electron-phonon calculations and lambda are present, so the next pass should target the numeric presentation layer."
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}
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]
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},
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{
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"material": "Nb3Ge",
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"targets": [
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{
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"field": "Tc_observed",
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"source_title_or_doi": "10.1063/1.1654966",
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"host_layer": "Publication record and full article",
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"target_section_hint": "Summary statement first, then the film or sample description in full text",
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"why_this_section": "The record layer already exposes the 22.3 K statement; the full-text pass should now confirm page context and sample identity."
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},
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{
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"field": "Theta_D_K_or_omega_log_K",
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"source_title_or_doi": "10.1103/PhysRevB.27.1568",
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"host_layer": "OSTI summary and full PRB article",
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"target_section_hint": "Tables or sections containing experimentally determined moments of the phonon spectra, especially omega_log, because the abstract says these values are tabulated",
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"why_this_section": "The same A15 phonon-spectrum source should be checked for Nb3Ge row-level moments once the full table is visible, because the primary-host abstract says the moments are tabulated."
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},
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{
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"field": "lambda_ep",
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"source_title_or_doi": "10.1016/0378-4363(84)90167-0",
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"host_layer": "ScienceDirect abstract and full article",
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"target_section_hint": "Sections, tables, or figures reporting alpha^2F(omega), full phonon dispersion, or explicit lambda values for Nb3Ge",
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"why_this_section": "The abstract confirms that Nb3Ge-specific electron-phonon calculations and lambda are present, so the next pass should target the numeric presentation layer."
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}
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]
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}
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],
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"claim_boundary": "This map only narrows where to look in full text. It does not certify any value until a row-specific capture is archived."
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}

‎docs/data/external/condensed_matter/superconductivity/row_resolution_targets/a15_lambda_abstract_numeric_review_packet.json‎

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{
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"schema_version": "1.0",
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"source_class": "external_pair_lambda_abstract_numeric_review_packet",
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"pair_label": "A15 residual blocker pair",
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"checked_date": "2026-05-12",
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"purpose": "Summarize what the newly captured A15 abstract-level lambda numerics do and do not resolve before any row-level patch review is allowed.",
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"source_anchor": {
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"article_title": "The phonons in high Tc A15 compounds",
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"source_title_or_doi": "10.1016/0378-4363(84)90167-0",
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"journal_citation": "Physica B+C 126(1-3), 217-228",
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"host_layer": "ScienceDirect primary-host abstract text"
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},
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"materials": [
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{
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"material": "Nb3Sn",
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"working_lambda_ep": 1.8,
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"abstract_lambda_ep": 1.5,
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"difference_direction": "external_lower_than_working_row",
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"compatibility_state": "same_family_numeric_signal_present_but_not_row_usable",
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"interpretation": "The abstract-level value is close enough to keep the row in the same strong-coupling family, but the new Nb3Sn omega_log sensitivity review shows that lambda=1.5 should not be promoted by itself; stronger archival support and convention review are still required."
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},
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{
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"material": "Nb3Ge",
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"working_lambda_ep": 2.1,
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"abstract_lambda_ep": 1.9,
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"difference_direction": "external_lower_than_working_row",
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"compatibility_state": "same_family_numeric_signal_present_but_not_row_usable",
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"interpretation": "The abstract-level value is again close enough to keep the row in the same strong-coupling family, but it still cannot settle the benchmark row until the phonon convention is fixed and stronger archival support is attached."
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}
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],
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"shared_unresolved_conditions": [
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"Nb3Sn has a provisional Table II omega_log capture, but it is not row-usable until sample-choice, repo archive, and same-family review are complete; Nb3Ge still lacks a row-specific phonon numeric capture.",
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"Neither row has a raw-page or table-level lambda capture with archived_raw_path and row locator.",
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"The pair still needs same-family review to show that the abstract-level lambda values are compatible with the phonon convention chosen for the benchmark rows."
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],
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"practical_result": "The A15 pair now has source-family-consistent lambda numerics at abstract level, which is stronger than support-only text and stronger than weak secondary hints, but still not enough to unblock patch review.",
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"claim_boundary": "This review packet records abstract-level numeric compatibility only. It does not certify row edits and does not change the FAIL status of the raw McMillan baseline."
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}

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