{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:HHQYFGWJ2IEHKJ2VASCAG2M4Q3","short_pith_number":"pith:HHQYFGWJ","schema_version":"1.0","canonical_sha256":"39e1829ac9d208752755048403699c86de90bcd6f0c40ad9327f860b0748896d","source":{"kind":"arxiv","id":"1507.06801","version":3},"attestation_state":"computed","paper":{"title":"Small-angle scattering behavior of thread-like and film-like systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Alvise Benedetti, Pietro Riello, Salvino Ciccariello","submitted_at":"2015-07-24T10:39:34Z","abstract_excerpt":"A film-like or a thread-like system is a system such that one of its constituting homogeneous phases has a constant thickness $\\delta$ or a constant normal section of largest diameter $\\delta$. The stick probability function of this phase, in the limit $\\delta \\to 0$, naturally leads to the definition of the correlation function (CF) of a surface or a curve. This CF fairly approximates the generating stick probability function in the range of distances larger than $\\delta$. The surface and the curve CFs respectively behave as $1/r$ and $1/r^2$ as $r \\to 0$. In the two cases, this result implie"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1507.06801","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mtrl-sci","submitted_at":"2015-07-24T10:39:34Z","cross_cats_sorted":[],"title_canon_sha256":"a5ccd9f44486ec394676b1284d90ac942b4daf3148fe923275d3c8b7fea171c9","abstract_canon_sha256":"3397b3020b374d9ee1cbf119dade7971de02ff952934f892bf58fa56f40d7354"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:26:02.631926Z","signature_b64":"4uwTQSIa7dLkn5Ti4YdQRlAETFdqhfxxyAn531Mvc4FtLB/KGuEbR8LaFBX/1fqJ4iwqQhy0TGTc+0Q8m7PtBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"39e1829ac9d208752755048403699c86de90bcd6f0c40ad9327f860b0748896d","last_reissued_at":"2026-05-18T01:26:02.631354Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:26:02.631354Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Small-angle scattering behavior of thread-like and film-like systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mtrl-sci","authors_text":"Alvise Benedetti, Pietro Riello, Salvino Ciccariello","submitted_at":"2015-07-24T10:39:34Z","abstract_excerpt":"A film-like or a thread-like system is a system such that one of its constituting homogeneous phases has a constant thickness $\\delta$ or a constant normal section of largest diameter $\\delta$. The stick probability function of this phase, in the limit $\\delta \\to 0$, naturally leads to the definition of the correlation function (CF) of a surface or a curve. This CF fairly approximates the generating stick probability function in the range of distances larger than $\\delta$. The surface and the curve CFs respectively behave as $1/r$ and $1/r^2$ as $r \\to 0$. In the two cases, this result implie"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.06801","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1507.06801","created_at":"2026-05-18T01:26:02.631454+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.06801v3","created_at":"2026-05-18T01:26:02.631454+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.06801","created_at":"2026-05-18T01:26:02.631454+00:00"},{"alias_kind":"pith_short_12","alias_value":"HHQYFGWJ2IEH","created_at":"2026-05-18T12:29:25.134429+00:00"},{"alias_kind":"pith_short_16","alias_value":"HHQYFGWJ2IEHKJ2V","created_at":"2026-05-18T12:29:25.134429+00:00"},{"alias_kind":"pith_short_8","alias_value":"HHQYFGWJ","created_at":"2026-05-18T12:29:25.134429+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HHQYFGWJ2IEHKJ2VASCAG2M4Q3","json":"https://pith.science/pith/HHQYFGWJ2IEHKJ2VASCAG2M4Q3.json","graph_json":"https://pith.science/api/pith-number/HHQYFGWJ2IEHKJ2VASCAG2M4Q3/graph.json","events_json":"https://pith.science/api/pith-number/HHQYFGWJ2IEHKJ2VASCAG2M4Q3/events.json","paper":"https://pith.science/paper/HHQYFGWJ"},"agent_actions":{"view_html":"https://pith.science/pith/HHQYFGWJ2IEHKJ2VASCAG2M4Q3","download_json":"https://pith.science/pith/HHQYFGWJ2IEHKJ2VASCAG2M4Q3.json","view_paper":"https://pith.science/paper/HHQYFGWJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.06801&json=true","fetch_graph":"https://pith.science/api/pith-number/HHQYFGWJ2IEHKJ2VASCAG2M4Q3/graph.json","fetch_events":"https://pith.science/api/pith-number/HHQYFGWJ2IEHKJ2VASCAG2M4Q3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HHQYFGWJ2IEHKJ2VASCAG2M4Q3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HHQYFGWJ2IEHKJ2VASCAG2M4Q3/action/storage_attestation","attest_author":"https://pith.science/pith/HHQYFGWJ2IEHKJ2VASCAG2M4Q3/action/author_attestation","sign_citation":"https://pith.science/pith/HHQYFGWJ2IEHKJ2VASCAG2M4Q3/action/citation_signature","submit_replication":"https://pith.science/pith/HHQYFGWJ2IEHKJ2VASCAG2M4Q3/action/replication_record"}},"created_at":"2026-05-18T01:26:02.631454+00:00","updated_at":"2026-05-18T01:26:02.631454+00:00"}