{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:ENCFGBU7VGA3DC7RRXMOHTVNQQ","short_pith_number":"pith:ENCFGBU7","schema_version":"1.0","canonical_sha256":"234453069fa981b18bf18dd8e3cead842c28ba68cec783ca0a57e130ef26a80f","source":{"kind":"arxiv","id":"nucl-th/0507077","version":4},"attestation_state":"computed","paper":{"title":"Power counting with one-pion exchange","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Michael C. Birse (Manchester)","submitted_at":"2005-07-29T14:17:24Z","abstract_excerpt":"Techniques developed for handing inverse-power-law potentials in atomic physics are applied to the tensor one-pion exchange potential to determine the regions in which it can be treated perturbatively. In S-, P- and D-waves the critical values of the relative momentum are less than or of the order of 400 MeV. The RG is then used to determine the power counting for short-range interaction in the presence of this potential. In the P-and D-waves, where there are no low-energy bound or virtual states, these interactions have half-integer RG eigenvalues and are substantially promoted relative to na"},"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-th/0507077","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2005-07-29T14:17:24Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"72d91369de923e558e1bfa1e4fb753ee64d43cfefcb636b333a7e9342e32e54c","abstract_canon_sha256":"bd3c264b36daf77270c298f632d7fd425a78364cf53944bc68a1d3d0475568a5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:56:58.268519Z","signature_b64":"2GLGdG9WEwfnmp6bltjRLnFsiW+/Kbi68Cm7CTeplLCM8jzvkWk9LCGgdCk0wuIdEeWkdhx6EbUAJOZOiXHHDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"234453069fa981b18bf18dd8e3cead842c28ba68cec783ca0a57e130ef26a80f","last_reissued_at":"2026-07-04T16:56:58.268004Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:56:58.268004Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Power counting with one-pion exchange","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Michael C. Birse (Manchester)","submitted_at":"2005-07-29T14:17:24Z","abstract_excerpt":"Techniques developed for handing inverse-power-law potentials in atomic physics are applied to the tensor one-pion exchange potential to determine the regions in which it can be treated perturbatively. In S-, P- and D-waves the critical values of the relative momentum are less than or of the order of 400 MeV. The RG is then used to determine the power counting for short-range interaction in the presence of this potential. In the P-and D-waves, where there are no low-energy bound or virtual states, these interactions have half-integer RG eigenvalues and are substantially promoted relative to na"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0507077","kind":"arxiv","version":4},"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/nucl-th/0507077/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":"nucl-th/0507077","created_at":"2026-07-04T16:56:58.268103+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0507077v4","created_at":"2026-07-04T16:56:58.268103+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0507077","created_at":"2026-07-04T16:56:58.268103+00:00"},{"alias_kind":"pith_short_12","alias_value":"ENCFGBU7VGA3","created_at":"2026-07-04T16:56:58.268103+00:00"},{"alias_kind":"pith_short_16","alias_value":"ENCFGBU7VGA3DC7R","created_at":"2026-07-04T16:56:58.268103+00:00"},{"alias_kind":"pith_short_8","alias_value":"ENCFGBU7","created_at":"2026-07-04T16:56:58.268103+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2603.28842","citing_title":"Dimer Effective Field Theory","ref_index":15,"is_internal_anchor":true},{"citing_arxiv_id":"2604.14985","citing_title":"Perturbative calculations of light nuclei up to N$^3$LO in chiral effective field theory","ref_index":40,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ENCFGBU7VGA3DC7RRXMOHTVNQQ","json":"https://pith.science/pith/ENCFGBU7VGA3DC7RRXMOHTVNQQ.json","graph_json":"https://pith.science/api/pith-number/ENCFGBU7VGA3DC7RRXMOHTVNQQ/graph.json","events_json":"https://pith.science/api/pith-number/ENCFGBU7VGA3DC7RRXMOHTVNQQ/events.json","paper":"https://pith.science/paper/ENCFGBU7"},"agent_actions":{"view_html":"https://pith.science/pith/ENCFGBU7VGA3DC7RRXMOHTVNQQ","download_json":"https://pith.science/pith/ENCFGBU7VGA3DC7RRXMOHTVNQQ.json","view_paper":"https://pith.science/paper/ENCFGBU7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0507077&json=true","fetch_graph":"https://pith.science/api/pith-number/ENCFGBU7VGA3DC7RRXMOHTVNQQ/graph.json","fetch_events":"https://pith.science/api/pith-number/ENCFGBU7VGA3DC7RRXMOHTVNQQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ENCFGBU7VGA3DC7RRXMOHTVNQQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ENCFGBU7VGA3DC7RRXMOHTVNQQ/action/storage_attestation","attest_author":"https://pith.science/pith/ENCFGBU7VGA3DC7RRXMOHTVNQQ/action/author_attestation","sign_citation":"https://pith.science/pith/ENCFGBU7VGA3DC7RRXMOHTVNQQ/action/citation_signature","submit_replication":"https://pith.science/pith/ENCFGBU7VGA3DC7RRXMOHTVNQQ/action/replication_record"}},"created_at":"2026-07-04T16:56:58.268103+00:00","updated_at":"2026-07-04T16:56:58.268103+00:00"}