{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:YGRXZMNFWJX6467CO22KH724EF","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"138049d2211ab383688943cde3482fa13313cb0b46a3a0c95b91bc9e1bc5b357","cross_cats_sorted":["physics.atm-clus"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2016-09-30T09:26:00Z","title_canon_sha256":"4c0b58e7c679a3f5a8f75f66740b9f3227d301ca90423edcdf94eba4a37c0a14"},"schema_version":"1.0","source":{"id":"1610.04262","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.04262","created_at":"2026-05-18T01:02:20Z"},{"alias_kind":"arxiv_version","alias_value":"1610.04262v1","created_at":"2026-05-18T01:02:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.04262","created_at":"2026-05-18T01:02:20Z"},{"alias_kind":"pith_short_12","alias_value":"YGRXZMNFWJX6","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"YGRXZMNFWJX6467C","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"YGRXZMNF","created_at":"2026-05-18T12:30:53Z"}],"graph_snapshots":[{"event_id":"sha256:e8f3994da54ebe2cdffec05c4be5bafa28fb871bbb1c4dbf8c2136e0b283d032","target":"graph","created_at":"2026-05-18T01:02:20Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"The existence of the limit of a sample scattering intensity, as the scattering vector approaches zero, requires and is ensured by the property that the mean value of the scattering density fluctuation over volume $V$ asymptotically behaves, at large $V$s, as $\\nu V^{-1/2}$, $\\nu$ being an appropriate constant. Then, the limit of the normalized scattering intensity is equal to $\\nu^2$. The implications of this result are also analyzed in the case of samples made up of two homogeneous phases.16 pages, 3 figures","authors_text":"Salvino Ciccariello","cross_cats":["physics.atm-clus"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2016-09-30T09:26:00Z","title":"Scattering intensity limit value at very small angles"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.04262","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:782fbd321f97296c295c60e5d62c99eaa3eacabecf756dfbd5c6dd2cfd3ffc67","target":"record","created_at":"2026-05-18T01:02:20Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"138049d2211ab383688943cde3482fa13313cb0b46a3a0c95b91bc9e1bc5b357","cross_cats_sorted":["physics.atm-clus"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2016-09-30T09:26:00Z","title_canon_sha256":"4c0b58e7c679a3f5a8f75f66740b9f3227d301ca90423edcdf94eba4a37c0a14"},"schema_version":"1.0","source":{"id":"1610.04262","kind":"arxiv","version":1}},"canonical_sha256":"c1a37cb1a5b26fee7be276b4a3ff5c2172d1fbe9d73b36aa0f49e436f78cbaa4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c1a37cb1a5b26fee7be276b4a3ff5c2172d1fbe9d73b36aa0f49e436f78cbaa4","first_computed_at":"2026-05-18T01:02:20.194689Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:02:20.194689Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"OMfME/811d/Bf1fc63IEzKlS2BzC5VQ9XYCH2KiMQAyU6baPAAqhFlrLyWTIJd/TWXXQAoVuSbesGX8srd0gDA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:02:20.195332Z","signed_message":"canonical_sha256_bytes"},"source_id":"1610.04262","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:782fbd321f97296c295c60e5d62c99eaa3eacabecf756dfbd5c6dd2cfd3ffc67","sha256:e8f3994da54ebe2cdffec05c4be5bafa28fb871bbb1c4dbf8c2136e0b283d032"],"state_sha256":"bd3a4a6f336c9ed6d13a5517f6cd00d0f04b0c903cfe8adda0c426ec2c95578d"}