{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:ZCPNW3NTRPQQJMCOV3LQBGT5HG","short_pith_number":"pith:ZCPNW3NT","schema_version":"1.0","canonical_sha256":"c89edb6db38be104b04eaed7009a7d39a3d6a7c22dfc36cb396cf1342292ccab","source":{"kind":"arxiv","id":"1604.06278","version":1},"attestation_state":"computed","paper":{"title":"Second--order equation of state with the Skyrme interaction. Cutoff and dimensional regularization with the inclusion of rearrangement terms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"C.J. Yang, G. Col\\`o, K. Moghrabi, M. Grasso, X. Roca-Maza","submitted_at":"2016-04-21T12:39:28Z","abstract_excerpt":"We evaluate the second--order (beyond--mean--field) contribution to the equation of state of nuclear matter with the effective Skyrme force and use cutoff and dimensional regularizations to treat the ultraviolet divergence produced by the zero--range character of this interaction. An adjustment of the force parameters is then performed in both cases to remove any double counting generated by the explicit computation of beyond--mean--field corrections with the Skyrme force. In addition, we include at second order the rearrangement terms associated to the density--dependent part of the Skyrme fo"},"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":"1604.06278","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-04-21T12:39:28Z","cross_cats_sorted":[],"title_canon_sha256":"e4fdcec449b0c3e3812c2781c491e44eeb26e43cb2b5cd95a6c9051df3411857","abstract_canon_sha256":"a6bfb9f7ef4fcda216dbf58c3f3e8f3a5f49c554a722f9859f5a90dd267112c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:04:13.233712Z","signature_b64":"geMKTHVxKc7rwxK3F0Xva0ZnCG5vTZX5yr9OL7OJjA+rw/UnrtS9QxlftBXeMh3P+khEAfdP5UPbL+YifJvGAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c89edb6db38be104b04eaed7009a7d39a3d6a7c22dfc36cb396cf1342292ccab","last_reissued_at":"2026-05-18T01:04:13.233289Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:04:13.233289Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Second--order equation of state with the Skyrme interaction. Cutoff and dimensional regularization with the inclusion of rearrangement terms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"C.J. Yang, G. Col\\`o, K. Moghrabi, M. Grasso, X. Roca-Maza","submitted_at":"2016-04-21T12:39:28Z","abstract_excerpt":"We evaluate the second--order (beyond--mean--field) contribution to the equation of state of nuclear matter with the effective Skyrme force and use cutoff and dimensional regularizations to treat the ultraviolet divergence produced by the zero--range character of this interaction. An adjustment of the force parameters is then performed in both cases to remove any double counting generated by the explicit computation of beyond--mean--field corrections with the Skyrme force. In addition, we include at second order the rearrangement terms associated to the density--dependent part of the Skyrme fo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.06278","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":"1604.06278","created_at":"2026-05-18T01:04:13.233355+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.06278v1","created_at":"2026-05-18T01:04:13.233355+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.06278","created_at":"2026-05-18T01:04:13.233355+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZCPNW3NTRPQQ","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZCPNW3NTRPQQJMCO","created_at":"2026-05-18T12:30:53.716459+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZCPNW3NT","created_at":"2026-05-18T12:30:53.716459+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/ZCPNW3NTRPQQJMCOV3LQBGT5HG","json":"https://pith.science/pith/ZCPNW3NTRPQQJMCOV3LQBGT5HG.json","graph_json":"https://pith.science/api/pith-number/ZCPNW3NTRPQQJMCOV3LQBGT5HG/graph.json","events_json":"https://pith.science/api/pith-number/ZCPNW3NTRPQQJMCOV3LQBGT5HG/events.json","paper":"https://pith.science/paper/ZCPNW3NT"},"agent_actions":{"view_html":"https://pith.science/pith/ZCPNW3NTRPQQJMCOV3LQBGT5HG","download_json":"https://pith.science/pith/ZCPNW3NTRPQQJMCOV3LQBGT5HG.json","view_paper":"https://pith.science/paper/ZCPNW3NT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.06278&json=true","fetch_graph":"https://pith.science/api/pith-number/ZCPNW3NTRPQQJMCOV3LQBGT5HG/graph.json","fetch_events":"https://pith.science/api/pith-number/ZCPNW3NTRPQQJMCOV3LQBGT5HG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZCPNW3NTRPQQJMCOV3LQBGT5HG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZCPNW3NTRPQQJMCOV3LQBGT5HG/action/storage_attestation","attest_author":"https://pith.science/pith/ZCPNW3NTRPQQJMCOV3LQBGT5HG/action/author_attestation","sign_citation":"https://pith.science/pith/ZCPNW3NTRPQQJMCOV3LQBGT5HG/action/citation_signature","submit_replication":"https://pith.science/pith/ZCPNW3NTRPQQJMCOV3LQBGT5HG/action/replication_record"}},"created_at":"2026-05-18T01:04:13.233355+00:00","updated_at":"2026-05-18T01:04:13.233355+00:00"}