{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:P7B42R4H4SLKB37SIVD2UMFSBH","short_pith_number":"pith:P7B42R4H","schema_version":"1.0","canonical_sha256":"7fc3cd4787e496a0eff24547aa30b209e168c0ec8070204a4c7ba8bd926fe3a5","source":{"kind":"arxiv","id":"1102.4068","version":2},"attestation_state":"computed","paper":{"title":"Parity- and Time-Reversal-Violating Form Factors of the Deuteron","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"E. Mereghetti, J. de Vries, R.G.E. Timmermans, U. van Kolck","submitted_at":"2011-02-20T13:34:49Z","abstract_excerpt":"We calculate the electric-dipole and magnetic-quadrupole form factors of the deuteron that arise as a low-energy manifestation of parity and time-reversal violation in quark-gluon interactions of effective dimension four and six: the QCD vacuum angle, the quark electric and chromo-electric dipole moments, and the gluon chromo-electric dipole moment. Within the framework of two-flavor chiral perturbation theory, we show that the relative sizes of the corresponding moments allow an identification of the symmetry-breaking source."},"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":"1102.4068","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-02-20T13:34:49Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"d2eda32fcd304901358f33501f1d1d576d285ccc5791115f85119efe9d0dc29e","abstract_canon_sha256":"23d6c28ea505dfea370cad9541a91a90c6e150ffabcea238d4f5ce3eb651be52"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:14:05.845783Z","signature_b64":"xxZMfL1pLKbz411rSmbM/J5MGrpIDlnGYHtjd5Up96YIsUDmXlForbSkv2aBoklBFkB/1AM41YkVflXaAWUTAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7fc3cd4787e496a0eff24547aa30b209e168c0ec8070204a4c7ba8bd926fe3a5","last_reissued_at":"2026-05-18T04:14:05.845106Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:14:05.845106Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Parity- and Time-Reversal-Violating Form Factors of the Deuteron","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"E. Mereghetti, J. de Vries, R.G.E. Timmermans, U. van Kolck","submitted_at":"2011-02-20T13:34:49Z","abstract_excerpt":"We calculate the electric-dipole and magnetic-quadrupole form factors of the deuteron that arise as a low-energy manifestation of parity and time-reversal violation in quark-gluon interactions of effective dimension four and six: the QCD vacuum angle, the quark electric and chromo-electric dipole moments, and the gluon chromo-electric dipole moment. Within the framework of two-flavor chiral perturbation theory, we show that the relative sizes of the corresponding moments allow an identification of the symmetry-breaking source."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1102.4068","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":"1102.4068","created_at":"2026-05-18T04:14:05.845198+00:00"},{"alias_kind":"arxiv_version","alias_value":"1102.4068v2","created_at":"2026-05-18T04:14:05.845198+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1102.4068","created_at":"2026-05-18T04:14:05.845198+00:00"},{"alias_kind":"pith_short_12","alias_value":"P7B42R4H4SLK","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_16","alias_value":"P7B42R4H4SLKB37S","created_at":"2026-05-18T12:26:39.201973+00:00"},{"alias_kind":"pith_short_8","alias_value":"P7B42R4H","created_at":"2026-05-18T12:26:39.201973+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2510.14933","citing_title":"Nucleon Electric Dipole Moments in Paramagnetic Molecules through Effective Field Theory","ref_index":56,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/P7B42R4H4SLKB37SIVD2UMFSBH","json":"https://pith.science/pith/P7B42R4H4SLKB37SIVD2UMFSBH.json","graph_json":"https://pith.science/api/pith-number/P7B42R4H4SLKB37SIVD2UMFSBH/graph.json","events_json":"https://pith.science/api/pith-number/P7B42R4H4SLKB37SIVD2UMFSBH/events.json","paper":"https://pith.science/paper/P7B42R4H"},"agent_actions":{"view_html":"https://pith.science/pith/P7B42R4H4SLKB37SIVD2UMFSBH","download_json":"https://pith.science/pith/P7B42R4H4SLKB37SIVD2UMFSBH.json","view_paper":"https://pith.science/paper/P7B42R4H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1102.4068&json=true","fetch_graph":"https://pith.science/api/pith-number/P7B42R4H4SLKB37SIVD2UMFSBH/graph.json","fetch_events":"https://pith.science/api/pith-number/P7B42R4H4SLKB37SIVD2UMFSBH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/P7B42R4H4SLKB37SIVD2UMFSBH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/P7B42R4H4SLKB37SIVD2UMFSBH/action/storage_attestation","attest_author":"https://pith.science/pith/P7B42R4H4SLKB37SIVD2UMFSBH/action/author_attestation","sign_citation":"https://pith.science/pith/P7B42R4H4SLKB37SIVD2UMFSBH/action/citation_signature","submit_replication":"https://pith.science/pith/P7B42R4H4SLKB37SIVD2UMFSBH/action/replication_record"}},"created_at":"2026-05-18T04:14:05.845198+00:00","updated_at":"2026-05-18T04:14:05.845198+00:00"}