{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2009:X7WTIPU7YSKVCZ6UOB7JGDBNNA","short_pith_number":"pith:X7WTIPU7","schema_version":"1.0","canonical_sha256":"bfed343e9fc4955167d4707e930c2d680adfb6d5d3f7a65ff4a8e0bb3893931f","source":{"kind":"arxiv","id":"0909.4641","version":1},"attestation_state":"computed","paper":{"title":"More effective theory of nuclear forces","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Michael C. Birse (Manchester)","submitted_at":"2009-09-25T08:57:22Z","abstract_excerpt":"I outline why the renormalisation group is needed to analyse the scale dependence and hence determine the power counting for effective theories of strongly interacting systems. I summarise the results of several such analyses for two- and three-body forces in nuclear physics. These show that a number of terms should be significantly promoted relative to naive dimensional analysis."},"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":"0909.4641","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2009-09-25T08:57:22Z","cross_cats_sorted":[],"title_canon_sha256":"4fd8ac2f7d2cb0cd0572aa90666beb1d7b27a167afb7e0274e519dc40ed53645","abstract_canon_sha256":"a046ea9fd31017093a7995bfb00fd74ed0f610d2fc956f0c9fb945bddb58c1e0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:34:27.652254Z","signature_b64":"B8tJ0Vg9K2hHDltSPIUxA6jKNN15glNsMV9NEzq69hxrsoqRrt25fkEz9HcnifQiNsOcJjrEB/jXWudbmxm+Dw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bfed343e9fc4955167d4707e930c2d680adfb6d5d3f7a65ff4a8e0bb3893931f","last_reissued_at":"2026-05-18T02:34:27.651685Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:34:27.651685Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"More effective theory of nuclear forces","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Michael C. Birse (Manchester)","submitted_at":"2009-09-25T08:57:22Z","abstract_excerpt":"I outline why the renormalisation group is needed to analyse the scale dependence and hence determine the power counting for effective theories of strongly interacting systems. I summarise the results of several such analyses for two- and three-body forces in nuclear physics. These show that a number of terms should be significantly promoted relative to naive dimensional analysis."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0909.4641","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":"0909.4641","created_at":"2026-05-18T02:34:27.651764+00:00"},{"alias_kind":"arxiv_version","alias_value":"0909.4641v1","created_at":"2026-05-18T02:34:27.651764+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0909.4641","created_at":"2026-05-18T02:34:27.651764+00:00"},{"alias_kind":"pith_short_12","alias_value":"X7WTIPU7YSKV","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_16","alias_value":"X7WTIPU7YSKVCZ6U","created_at":"2026-05-18T12:26:02.257875+00:00"},{"alias_kind":"pith_short_8","alias_value":"X7WTIPU7","created_at":"2026-05-18T12:26:02.257875+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/X7WTIPU7YSKVCZ6UOB7JGDBNNA","json":"https://pith.science/pith/X7WTIPU7YSKVCZ6UOB7JGDBNNA.json","graph_json":"https://pith.science/api/pith-number/X7WTIPU7YSKVCZ6UOB7JGDBNNA/graph.json","events_json":"https://pith.science/api/pith-number/X7WTIPU7YSKVCZ6UOB7JGDBNNA/events.json","paper":"https://pith.science/paper/X7WTIPU7"},"agent_actions":{"view_html":"https://pith.science/pith/X7WTIPU7YSKVCZ6UOB7JGDBNNA","download_json":"https://pith.science/pith/X7WTIPU7YSKVCZ6UOB7JGDBNNA.json","view_paper":"https://pith.science/paper/X7WTIPU7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0909.4641&json=true","fetch_graph":"https://pith.science/api/pith-number/X7WTIPU7YSKVCZ6UOB7JGDBNNA/graph.json","fetch_events":"https://pith.science/api/pith-number/X7WTIPU7YSKVCZ6UOB7JGDBNNA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/X7WTIPU7YSKVCZ6UOB7JGDBNNA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/X7WTIPU7YSKVCZ6UOB7JGDBNNA/action/storage_attestation","attest_author":"https://pith.science/pith/X7WTIPU7YSKVCZ6UOB7JGDBNNA/action/author_attestation","sign_citation":"https://pith.science/pith/X7WTIPU7YSKVCZ6UOB7JGDBNNA/action/citation_signature","submit_replication":"https://pith.science/pith/X7WTIPU7YSKVCZ6UOB7JGDBNNA/action/replication_record"}},"created_at":"2026-05-18T02:34:27.651764+00:00","updated_at":"2026-05-18T02:34:27.651764+00:00"}