{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:TJWNI3JMQRY6G4KP7F2AEQMBLS","short_pith_number":"pith:TJWNI3JM","schema_version":"1.0","canonical_sha256":"9a6cd46d2c8471e3714ff9740241815c9e14dca90702fce735db89923bb56df3","source":{"kind":"arxiv","id":"1908.07578","version":1},"attestation_state":"computed","paper":{"title":"Renormalization of pionless effective field theory in the A-body sector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Mehdi Drissi, Thomas Duguet, Vittorio Soma","submitted_at":"2019-08-20T19:28:07Z","abstract_excerpt":"Current models of inter-nucleon interactions are built within the frame of Effective Field Theories (EFTs). Contrary to traditional nuclear potentials, EFT interactions require a renormalization of their parameters in order to derive meaningful estimations of observable. In this paper, a renormalization procedure is designed in connection with many-body approximations applicable to large-A systems and formulated within the frame of many-body perturbation theory. The procedure is shown to generate counterterms that are independent of the targeted A-body sector. As an example, the procedure is a"},"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":"1908.07578","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-08-20T19:28:07Z","cross_cats_sorted":[],"title_canon_sha256":"5c6d7c117ec56ced2b15fa36611629c38d0790f2ccf51c88706f950d6fc63810","abstract_canon_sha256":"3860ee25049663fd5a424423212821354741fe4f4c27b68a60562e490f01a28c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:03:20.197800Z","signature_b64":"ML1ecIi2qdI+YPdEXXV1uZqoHieaYpAgHLLVKM/GiShWJ0YK9DmKu2Fs8hMiUq2XnmVH8rVShxhoop7LdShbDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9a6cd46d2c8471e3714ff9740241815c9e14dca90702fce735db89923bb56df3","last_reissued_at":"2026-07-05T01:03:20.197306Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:03:20.197306Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Renormalization of pionless effective field theory in the A-body sector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Mehdi Drissi, Thomas Duguet, Vittorio Soma","submitted_at":"2019-08-20T19:28:07Z","abstract_excerpt":"Current models of inter-nucleon interactions are built within the frame of Effective Field Theories (EFTs). Contrary to traditional nuclear potentials, EFT interactions require a renormalization of their parameters in order to derive meaningful estimations of observable. In this paper, a renormalization procedure is designed in connection with many-body approximations applicable to large-A systems and formulated within the frame of many-body perturbation theory. The procedure is shown to generate counterterms that are independent of the targeted A-body sector. As an example, the procedure is a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.07578","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1908.07578/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1908.07578","created_at":"2026-07-05T01:03:20.197375+00:00"},{"alias_kind":"arxiv_version","alias_value":"1908.07578v1","created_at":"2026-07-05T01:03:20.197375+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.07578","created_at":"2026-07-05T01:03:20.197375+00:00"},{"alias_kind":"pith_short_12","alias_value":"TJWNI3JMQRY6","created_at":"2026-07-05T01:03:20.197375+00:00"},{"alias_kind":"pith_short_16","alias_value":"TJWNI3JMQRY6G4KP","created_at":"2026-07-05T01:03:20.197375+00:00"},{"alias_kind":"pith_short_8","alias_value":"TJWNI3JM","created_at":"2026-07-05T01:03:20.197375+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/TJWNI3JMQRY6G4KP7F2AEQMBLS","json":"https://pith.science/pith/TJWNI3JMQRY6G4KP7F2AEQMBLS.json","graph_json":"https://pith.science/api/pith-number/TJWNI3JMQRY6G4KP7F2AEQMBLS/graph.json","events_json":"https://pith.science/api/pith-number/TJWNI3JMQRY6G4KP7F2AEQMBLS/events.json","paper":"https://pith.science/paper/TJWNI3JM"},"agent_actions":{"view_html":"https://pith.science/pith/TJWNI3JMQRY6G4KP7F2AEQMBLS","download_json":"https://pith.science/pith/TJWNI3JMQRY6G4KP7F2AEQMBLS.json","view_paper":"https://pith.science/paper/TJWNI3JM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1908.07578&json=true","fetch_graph":"https://pith.science/api/pith-number/TJWNI3JMQRY6G4KP7F2AEQMBLS/graph.json","fetch_events":"https://pith.science/api/pith-number/TJWNI3JMQRY6G4KP7F2AEQMBLS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TJWNI3JMQRY6G4KP7F2AEQMBLS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TJWNI3JMQRY6G4KP7F2AEQMBLS/action/storage_attestation","attest_author":"https://pith.science/pith/TJWNI3JMQRY6G4KP7F2AEQMBLS/action/author_attestation","sign_citation":"https://pith.science/pith/TJWNI3JMQRY6G4KP7F2AEQMBLS/action/citation_signature","submit_replication":"https://pith.science/pith/TJWNI3JMQRY6G4KP7F2AEQMBLS/action/replication_record"}},"created_at":"2026-07-05T01:03:20.197375+00:00","updated_at":"2026-07-05T01:03:20.197375+00:00"}