{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2000:4PT2A3AKKT3CMQ747JXPM6ZW52","short_pith_number":"pith:4PT2A3AK","schema_version":"1.0","canonical_sha256":"e3e7a06c0a54f62643fcfa6ef67b36eeac770a008939f559d11a24d8d70cc35f","source":{"kind":"arxiv","id":"nucl-ex/0002004","version":1},"attestation_state":"computed","paper":{"title":"Nuclear multifragmentation, percolation and the Fisher Droplet Model: common features of reducibility and thermal scaling","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"G. J. Wozniak, J. B. Elliott, L. G. Moretto, L. Phair, the EOS Collaboration","submitted_at":"2000-02-04T23:34:44Z","abstract_excerpt":"It is shown that the Fisher Droplet Model (FDM), percolation and nuclear multifragmentation share the common features of reducibility (stochasticity in multiplicity distributions) and thermal scaling (one-fragment production probabilities are Boltzmann factors). Barriers obtained, for cluster production on percolation lattices, from the Boltzmann factors show a power-law dependence on cluster size with an exponent of 0.42 +- 0.02. The EOS Au multifragmentation data yield barriers with a power-law exponent of 0.68 +- 0.03. Values of the surface energy coefficient of a low density nuclear system"},"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":"nucl-ex/0002004","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-ex","submitted_at":"2000-02-04T23:34:44Z","cross_cats_sorted":[],"title_canon_sha256":"1fdedc03b5fa275f555034a73eeb61ae4a67cd6f40420b269db38d687c1392b6","abstract_canon_sha256":"16c25b9cb349200bab4abce58367a4032535436476da79b7757a4202e6e3f791"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:35:38.274992Z","signature_b64":"xwWBeMG7Fxl72ILWCNjMNdEZOOiODdmD1w/gTBb7PLBK0sa/j7glT+2viihF46Cu7yTprbxnthfb1h2fLd5uAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e3e7a06c0a54f62643fcfa6ef67b36eeac770a008939f559d11a24d8d70cc35f","last_reissued_at":"2026-05-18T02:35:38.274505Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:35:38.274505Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Nuclear multifragmentation, percolation and the Fisher Droplet Model: common features of reducibility and thermal scaling","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"G. J. Wozniak, J. B. Elliott, L. G. Moretto, L. Phair, the EOS Collaboration","submitted_at":"2000-02-04T23:34:44Z","abstract_excerpt":"It is shown that the Fisher Droplet Model (FDM), percolation and nuclear multifragmentation share the common features of reducibility (stochasticity in multiplicity distributions) and thermal scaling (one-fragment production probabilities are Boltzmann factors). Barriers obtained, for cluster production on percolation lattices, from the Boltzmann factors show a power-law dependence on cluster size with an exponent of 0.42 +- 0.02. The EOS Au multifragmentation data yield barriers with a power-law exponent of 0.68 +- 0.03. Values of the surface energy coefficient of a low density nuclear system"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-ex/0002004","kind":"arxiv","version":1},"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":"nucl-ex/0002004","created_at":"2026-05-18T02:35:38.274579+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-ex/0002004v1","created_at":"2026-05-18T02:35:38.274579+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-ex/0002004","created_at":"2026-05-18T02:35:38.274579+00:00"},{"alias_kind":"pith_short_12","alias_value":"4PT2A3AKKT3C","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_16","alias_value":"4PT2A3AKKT3CMQ74","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_8","alias_value":"4PT2A3AK","created_at":"2026-05-18T12:25:49.631198+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/4PT2A3AKKT3CMQ747JXPM6ZW52","json":"https://pith.science/pith/4PT2A3AKKT3CMQ747JXPM6ZW52.json","graph_json":"https://pith.science/api/pith-number/4PT2A3AKKT3CMQ747JXPM6ZW52/graph.json","events_json":"https://pith.science/api/pith-number/4PT2A3AKKT3CMQ747JXPM6ZW52/events.json","paper":"https://pith.science/paper/4PT2A3AK"},"agent_actions":{"view_html":"https://pith.science/pith/4PT2A3AKKT3CMQ747JXPM6ZW52","download_json":"https://pith.science/pith/4PT2A3AKKT3CMQ747JXPM6ZW52.json","view_paper":"https://pith.science/paper/4PT2A3AK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-ex/0002004&json=true","fetch_graph":"https://pith.science/api/pith-number/4PT2A3AKKT3CMQ747JXPM6ZW52/graph.json","fetch_events":"https://pith.science/api/pith-number/4PT2A3AKKT3CMQ747JXPM6ZW52/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4PT2A3AKKT3CMQ747JXPM6ZW52/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4PT2A3AKKT3CMQ747JXPM6ZW52/action/storage_attestation","attest_author":"https://pith.science/pith/4PT2A3AKKT3CMQ747JXPM6ZW52/action/author_attestation","sign_citation":"https://pith.science/pith/4PT2A3AKKT3CMQ747JXPM6ZW52/action/citation_signature","submit_replication":"https://pith.science/pith/4PT2A3AKKT3CMQ747JXPM6ZW52/action/replication_record"}},"created_at":"2026-05-18T02:35:38.274579+00:00","updated_at":"2026-05-18T02:35:38.274579+00:00"}