{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:C67NMJY5KE22YX3POJYAMDF6HY","short_pith_number":"pith:C67NMJY5","schema_version":"1.0","canonical_sha256":"17bed6271d5135ac5f6f7270060cbe3e173c02de6d23e3d3f89dfdd23c4124f9","source":{"kind":"arxiv","id":"2305.17120","version":2},"attestation_state":"computed","paper":{"title":"Sphaleron rate from a modified Backus-Gilbert inversion method","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"Claudio Bonanno, Francesco D'Angelo, Lorenzo Maio, Manuel Naviglio, Massimo D'Elia","submitted_at":"2023-05-26T17:41:40Z","abstract_excerpt":"We compute the sphaleron rate in quenched QCD for a temperature $T \\simeq 1.24~T_c$ from the inversion of the Euclidean lattice time correlator of the topological charge density. We explore and compare two different strategies: one follows a new approach proposed in this study and consists in extracting the rate from finite lattice spacing correlators, and then in taking the continuum limit at fixed smoothing radius followed by a zero-smoothing extrapolation; the other follows the traditional approach of extracting the rate after performing such double extrapolation directly on the correlator."},"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":"2305.17120","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2023-05-26T17:41:40Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"ba0cbcaf89413e4f6c7250bcaf20d079702d6c3affa8ed79e2d311668ac0e56a","abstract_canon_sha256":"da4bf194cd0645d68c883bf1b97b316366ad72c2fc9d96e486fe6bdd679defc4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:45:50.550286Z","signature_b64":"agJcD5eBMyHA3vCyqdU5S8ponmaeyTMRNEuaVo+2I/XogOtlby0U8vaN8fnNbuJaP9TF9IGcPI2J7cy7mY4fAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"17bed6271d5135ac5f6f7270060cbe3e173c02de6d23e3d3f89dfdd23c4124f9","last_reissued_at":"2026-07-05T06:45:50.549792Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:45:50.549792Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Sphaleron rate from a modified Backus-Gilbert inversion method","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"hep-lat","authors_text":"Claudio Bonanno, Francesco D'Angelo, Lorenzo Maio, Manuel Naviglio, Massimo D'Elia","submitted_at":"2023-05-26T17:41:40Z","abstract_excerpt":"We compute the sphaleron rate in quenched QCD for a temperature $T \\simeq 1.24~T_c$ from the inversion of the Euclidean lattice time correlator of the topological charge density. We explore and compare two different strategies: one follows a new approach proposed in this study and consists in extracting the rate from finite lattice spacing correlators, and then in taking the continuum limit at fixed smoothing radius followed by a zero-smoothing extrapolation; the other follows the traditional approach of extracting the rate after performing such double extrapolation directly on the correlator."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.17120","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/2305.17120/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":"2305.17120","created_at":"2026-07-05T06:45:50.549853+00:00"},{"alias_kind":"arxiv_version","alias_value":"2305.17120v2","created_at":"2026-07-05T06:45:50.549853+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.17120","created_at":"2026-07-05T06:45:50.549853+00:00"},{"alias_kind":"pith_short_12","alias_value":"C67NMJY5KE22","created_at":"2026-07-05T06:45:50.549853+00:00"},{"alias_kind":"pith_short_16","alias_value":"C67NMJY5KE22YX3P","created_at":"2026-07-05T06:45:50.549853+00:00"},{"alias_kind":"pith_short_8","alias_value":"C67NMJY5","created_at":"2026-07-05T06:45:50.549853+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2607.01116","citing_title":"Inclusive $\\bar B_s\\mapsto X_{\\bar sc} \\ell \\bar \\nu$ decays from lattice QCD: computational strategy and a first physical result","ref_index":29,"is_internal_anchor":false},{"citing_arxiv_id":"2605.14652","citing_title":"Extraction of spectral densities from lattice correlators: decoupling signal from noise","ref_index":14,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/C67NMJY5KE22YX3POJYAMDF6HY","json":"https://pith.science/pith/C67NMJY5KE22YX3POJYAMDF6HY.json","graph_json":"https://pith.science/api/pith-number/C67NMJY5KE22YX3POJYAMDF6HY/graph.json","events_json":"https://pith.science/api/pith-number/C67NMJY5KE22YX3POJYAMDF6HY/events.json","paper":"https://pith.science/paper/C67NMJY5"},"agent_actions":{"view_html":"https://pith.science/pith/C67NMJY5KE22YX3POJYAMDF6HY","download_json":"https://pith.science/pith/C67NMJY5KE22YX3POJYAMDF6HY.json","view_paper":"https://pith.science/paper/C67NMJY5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2305.17120&json=true","fetch_graph":"https://pith.science/api/pith-number/C67NMJY5KE22YX3POJYAMDF6HY/graph.json","fetch_events":"https://pith.science/api/pith-number/C67NMJY5KE22YX3POJYAMDF6HY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/C67NMJY5KE22YX3POJYAMDF6HY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/C67NMJY5KE22YX3POJYAMDF6HY/action/storage_attestation","attest_author":"https://pith.science/pith/C67NMJY5KE22YX3POJYAMDF6HY/action/author_attestation","sign_citation":"https://pith.science/pith/C67NMJY5KE22YX3POJYAMDF6HY/action/citation_signature","submit_replication":"https://pith.science/pith/C67NMJY5KE22YX3POJYAMDF6HY/action/replication_record"}},"created_at":"2026-07-05T06:45:50.549853+00:00","updated_at":"2026-07-05T06:45:50.549853+00:00"}