{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:XPXVHRVFABBEGQ56VQHAXGJABZ","short_pith_number":"pith:XPXVHRVF","schema_version":"1.0","canonical_sha256":"bbef53c6a500424343beac0e0b99200e5b40bafe9a934d98d86df448e161f244","source":{"kind":"arxiv","id":"1007.0734","version":2},"attestation_state":"computed","paper":{"title":"On Parity-Violating Three-Nucleon Interactions and the Predictive Power of Few-Nucleon EFT at Very Low Energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Harald W. Griesshammer, Matthias R. Schindler (George Washington U.)","submitted_at":"2010-07-05T17:57:29Z","abstract_excerpt":"We address the typical strengths of hadronic parity-violating three-nucleon interactions in \"pion-less\" Effective Field Theory in the nucleon-deuteron (iso-doublet) system. By analysing the superficial degree of divergence of loop diagrams, we conclude that no such interactions are needed at leading order. The only two linearly independent parity-violating three-nucleon structures with one derivative mix two-S and two-P-half waves with iso-spin transitions Delta I = 0 or 1. Due to their structure, they cannot absorb any divergence ostensibly appearing at next-to-leading order. This observation"},"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":"1007.0734","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2010-07-05T17:57:29Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"addc5e54ce259b87b9e59431e980f9007ff90911afb05222d115ce99a60a86d8","abstract_canon_sha256":"182c0e2afe396f9d13b4f268f5a362a3602cba521c80a72e5c39c23325c440ab"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:33:15.332403Z","signature_b64":"fxKWNqpZp0R0OnF34AYwg99o9Krb67jLWqjScVzwAXb/IooaPvTzHynwQcS50Wcf/rJ6AFBrO35rk9RgFJNUDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bbef53c6a500424343beac0e0b99200e5b40bafe9a934d98d86df448e161f244","last_reissued_at":"2026-05-18T02:33:15.331816Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:33:15.331816Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On Parity-Violating Three-Nucleon Interactions and the Predictive Power of Few-Nucleon EFT at Very Low Energies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Harald W. Griesshammer, Matthias R. Schindler (George Washington U.)","submitted_at":"2010-07-05T17:57:29Z","abstract_excerpt":"We address the typical strengths of hadronic parity-violating three-nucleon interactions in \"pion-less\" Effective Field Theory in the nucleon-deuteron (iso-doublet) system. By analysing the superficial degree of divergence of loop diagrams, we conclude that no such interactions are needed at leading order. The only two linearly independent parity-violating three-nucleon structures with one derivative mix two-S and two-P-half waves with iso-spin transitions Delta I = 0 or 1. Due to their structure, they cannot absorb any divergence ostensibly appearing at next-to-leading order. This observation"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1007.0734","kind":"arxiv","version":2},"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":"1007.0734","created_at":"2026-05-18T02:33:15.331920+00:00"},{"alias_kind":"arxiv_version","alias_value":"1007.0734v2","created_at":"2026-05-18T02:33:15.331920+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1007.0734","created_at":"2026-05-18T02:33:15.331920+00:00"},{"alias_kind":"pith_short_12","alias_value":"XPXVHRVFABBE","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_16","alias_value":"XPXVHRVFABBEGQ56","created_at":"2026-05-18T12:26:17.028572+00:00"},{"alias_kind":"pith_short_8","alias_value":"XPXVHRVF","created_at":"2026-05-18T12:26:17.028572+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.19062","citing_title":"Coulomb Corrections to Three-Nucleon Moments","ref_index":58,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XPXVHRVFABBEGQ56VQHAXGJABZ","json":"https://pith.science/pith/XPXVHRVFABBEGQ56VQHAXGJABZ.json","graph_json":"https://pith.science/api/pith-number/XPXVHRVFABBEGQ56VQHAXGJABZ/graph.json","events_json":"https://pith.science/api/pith-number/XPXVHRVFABBEGQ56VQHAXGJABZ/events.json","paper":"https://pith.science/paper/XPXVHRVF"},"agent_actions":{"view_html":"https://pith.science/pith/XPXVHRVFABBEGQ56VQHAXGJABZ","download_json":"https://pith.science/pith/XPXVHRVFABBEGQ56VQHAXGJABZ.json","view_paper":"https://pith.science/paper/XPXVHRVF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1007.0734&json=true","fetch_graph":"https://pith.science/api/pith-number/XPXVHRVFABBEGQ56VQHAXGJABZ/graph.json","fetch_events":"https://pith.science/api/pith-number/XPXVHRVFABBEGQ56VQHAXGJABZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XPXVHRVFABBEGQ56VQHAXGJABZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XPXVHRVFABBEGQ56VQHAXGJABZ/action/storage_attestation","attest_author":"https://pith.science/pith/XPXVHRVFABBEGQ56VQHAXGJABZ/action/author_attestation","sign_citation":"https://pith.science/pith/XPXVHRVFABBEGQ56VQHAXGJABZ/action/citation_signature","submit_replication":"https://pith.science/pith/XPXVHRVFABBEGQ56VQHAXGJABZ/action/replication_record"}},"created_at":"2026-05-18T02:33:15.331920+00:00","updated_at":"2026-05-18T02:33:15.331920+00:00"}