{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:ADANCSL2MNEGWC6HABIY6FWYGD","short_pith_number":"pith:ADANCSL2","schema_version":"1.0","canonical_sha256":"00c0d1497a63486b0bc700518f16d830ce119e73d8f1ab7eb172fbc7aa7e90d8","source":{"kind":"arxiv","id":"2501.13429","version":2},"attestation_state":"computed","paper":{"title":"Proton decay matrix elements on PACS configurations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Eigo Shintani, Ryutaro Tsuji, Yasumichi Aoki, Yoshinobu Kuramashi","submitted_at":"2025-01-23T07:24:15Z","abstract_excerpt":"We report the preliminary results of lattice computation for the proton decay matrix elements in $N_f=2+1$ physical point with Wilson-clover fermion. We perform it on the PACS configurations of $64^4$ lattice volume with lattice spacing $a=0.085$ fm, and carefully estimate the systematic uncertainties, especially for the excited state contamination and associated error of the renormalization constant with Regularization Independent (RI, Rome-Southampton) scheme. Our preliminary results of the twelve relevant transition modes in proton decay matrix element and comparison with other lattice resu"},"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":"2501.13429","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2025-01-23T07:24:15Z","cross_cats_sorted":[],"title_canon_sha256":"3e5b861a548c4fc4d76d078fb5acae638e2d21c79157e339e05ae1d48c893bb3","abstract_canon_sha256":"c2309385bdd96b7accdb4f81a0b23e6140e18f4a65aca34e88b2a9b5a387a80f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:05:17.152899Z","signature_b64":"ejzkHKBdmiDZHVzTde4f2PFomEOqAhtNe23aT9d5RpcqE9Geo7warbzj+uJ5iX5Vmc5cUMp/8L3lKP0ydZXqAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"00c0d1497a63486b0bc700518f16d830ce119e73d8f1ab7eb172fbc7aa7e90d8","last_reissued_at":"2026-07-05T10:05:17.152392Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:05:17.152392Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Proton decay matrix elements on PACS configurations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Eigo Shintani, Ryutaro Tsuji, Yasumichi Aoki, Yoshinobu Kuramashi","submitted_at":"2025-01-23T07:24:15Z","abstract_excerpt":"We report the preliminary results of lattice computation for the proton decay matrix elements in $N_f=2+1$ physical point with Wilson-clover fermion. We perform it on the PACS configurations of $64^4$ lattice volume with lattice spacing $a=0.085$ fm, and carefully estimate the systematic uncertainties, especially for the excited state contamination and associated error of the renormalization constant with Regularization Independent (RI, Rome-Southampton) scheme. Our preliminary results of the twelve relevant transition modes in proton decay matrix element and comparison with other lattice resu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2501.13429","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2501.13429/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":"2501.13429","created_at":"2026-07-05T10:05:17.152453+00:00"},{"alias_kind":"arxiv_version","alias_value":"2501.13429v2","created_at":"2026-07-05T10:05:17.152453+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2501.13429","created_at":"2026-07-05T10:05:17.152453+00:00"},{"alias_kind":"pith_short_12","alias_value":"ADANCSL2MNEG","created_at":"2026-07-05T10:05:17.152453+00:00"},{"alias_kind":"pith_short_16","alias_value":"ADANCSL2MNEGWC6H","created_at":"2026-07-05T10:05:17.152453+00:00"},{"alias_kind":"pith_short_8","alias_value":"ADANCSL2","created_at":"2026-07-05T10:05:17.152453+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/ADANCSL2MNEGWC6HABIY6FWYGD","json":"https://pith.science/pith/ADANCSL2MNEGWC6HABIY6FWYGD.json","graph_json":"https://pith.science/api/pith-number/ADANCSL2MNEGWC6HABIY6FWYGD/graph.json","events_json":"https://pith.science/api/pith-number/ADANCSL2MNEGWC6HABIY6FWYGD/events.json","paper":"https://pith.science/paper/ADANCSL2"},"agent_actions":{"view_html":"https://pith.science/pith/ADANCSL2MNEGWC6HABIY6FWYGD","download_json":"https://pith.science/pith/ADANCSL2MNEGWC6HABIY6FWYGD.json","view_paper":"https://pith.science/paper/ADANCSL2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2501.13429&json=true","fetch_graph":"https://pith.science/api/pith-number/ADANCSL2MNEGWC6HABIY6FWYGD/graph.json","fetch_events":"https://pith.science/api/pith-number/ADANCSL2MNEGWC6HABIY6FWYGD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ADANCSL2MNEGWC6HABIY6FWYGD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ADANCSL2MNEGWC6HABIY6FWYGD/action/storage_attestation","attest_author":"https://pith.science/pith/ADANCSL2MNEGWC6HABIY6FWYGD/action/author_attestation","sign_citation":"https://pith.science/pith/ADANCSL2MNEGWC6HABIY6FWYGD/action/citation_signature","submit_replication":"https://pith.science/pith/ADANCSL2MNEGWC6HABIY6FWYGD/action/replication_record"}},"created_at":"2026-07-05T10:05:17.152453+00:00","updated_at":"2026-07-05T10:05:17.152453+00:00"}