{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:SF22TFERHFTYWQRWJSNGXQQUKL","short_pith_number":"pith:SF22TFER","canonical_record":{"source":{"id":"2209.14864","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-09-29T15:31:35Z","cross_cats_sorted":[],"title_canon_sha256":"6425a3aa1e933be138c0a6df04a8a367cfd556266a1812cf8ea19708bc7896f9","abstract_canon_sha256":"2e192e49beed5b4e93d2f09c93432bfa015f889016133f97e95ea6a62720e1a5"},"schema_version":"1.0"},"canonical_sha256":"9175a9949139678b42364c9a6bc21452d50b6cb57b8435072f993aa4099e97f4","source":{"kind":"arxiv","id":"2209.14864","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2209.14864","created_at":"2026-07-05T06:03:58Z"},{"alias_kind":"arxiv_version","alias_value":"2209.14864v1","created_at":"2026-07-05T06:03:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.14864","created_at":"2026-07-05T06:03:58Z"},{"alias_kind":"pith_short_12","alias_value":"SF22TFERHFTY","created_at":"2026-07-05T06:03:58Z"},{"alias_kind":"pith_short_16","alias_value":"SF22TFERHFTYWQRW","created_at":"2026-07-05T06:03:58Z"},{"alias_kind":"pith_short_8","alias_value":"SF22TFER","created_at":"2026-07-05T06:03:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:SF22TFERHFTYWQRWJSNGXQQUKL","target":"record","payload":{"canonical_record":{"source":{"id":"2209.14864","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-09-29T15:31:35Z","cross_cats_sorted":[],"title_canon_sha256":"6425a3aa1e933be138c0a6df04a8a367cfd556266a1812cf8ea19708bc7896f9","abstract_canon_sha256":"2e192e49beed5b4e93d2f09c93432bfa015f889016133f97e95ea6a62720e1a5"},"schema_version":"1.0"},"canonical_sha256":"9175a9949139678b42364c9a6bc21452d50b6cb57b8435072f993aa4099e97f4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:03:58.887298Z","signature_b64":"iuvLdL9O+h1foEyw5+PV689JmLDaQDvqU+1nAAIPG7vAIGwI5xT7DO2Ah/UQxEQyC+JOmqV8syjwibCdqQOzAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9175a9949139678b42364c9a6bc21452d50b6cb57b8435072f993aa4099e97f4","last_reissued_at":"2026-07-05T06:03:58.886961Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:03:58.886961Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2209.14864","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T06:03:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CtrAiK6LPr+83bWOA6T/sgiN/yi79qnVB2yKe+2b3fdORbV8/z5VkvM4gZYeLR3dxgV8pTjqKCEXI810BwoCDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T12:27:51.349602Z"},"content_sha256":"7dacf70f840e8a94142a2018a4e5ae687ac94ec0e30210c66833996a41cfbf04","schema_version":"1.0","event_id":"sha256:7dacf70f840e8a94142a2018a4e5ae687ac94ec0e30210c66833996a41cfbf04"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:SF22TFERHFTYWQRWJSNGXQQUKL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Overlap quark propagator near the physical pion mass","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Adam Virgili, Derek Leinweber, Waseem Kamleh","submitted_at":"2022-09-29T15:31:35Z","abstract_excerpt":"The Landau-gauge quark propagator is calculated using overlap fermions on 2+1-flavour dynamical fermion gauge fields from the PACS-CS collaboration with pion mass $m_\\pi \\sim 156\\text{ MeV}$ and spatial volume $\\sim (3 \\text{ fm})^3.$ The observed features of the mass and renormalisation functions are discussed, including a comparison with recent results using $\\mathcal{O}(a)$-improved Wilson fermions on 2-flavour dynamical gauge fields."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.14864","kind":"arxiv","version":1},"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/2209.14864/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T06:03:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RaChbHL+ItOMRzlHZbOYN2psLpR/rOcQ2YsGroCqRGiAqXWD9yJzRc+0aFRc9EYqbzjd0o379QbTks+SW1c7Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-09T12:27:51.350091Z"},"content_sha256":"d62386d744e49e003f6d678f3066bd430de4f69faa0f4da859323b78feec566a","schema_version":"1.0","event_id":"sha256:d62386d744e49e003f6d678f3066bd430de4f69faa0f4da859323b78feec566a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SF22TFERHFTYWQRWJSNGXQQUKL/bundle.json","state_url":"https://pith.science/pith/SF22TFERHFTYWQRWJSNGXQQUKL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SF22TFERHFTYWQRWJSNGXQQUKL/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-09T12:27:51Z","links":{"resolver":"https://pith.science/pith/SF22TFERHFTYWQRWJSNGXQQUKL","bundle":"https://pith.science/pith/SF22TFERHFTYWQRWJSNGXQQUKL/bundle.json","state":"https://pith.science/pith/SF22TFERHFTYWQRWJSNGXQQUKL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SF22TFERHFTYWQRWJSNGXQQUKL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:SF22TFERHFTYWQRWJSNGXQQUKL","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"2e192e49beed5b4e93d2f09c93432bfa015f889016133f97e95ea6a62720e1a5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-09-29T15:31:35Z","title_canon_sha256":"6425a3aa1e933be138c0a6df04a8a367cfd556266a1812cf8ea19708bc7896f9"},"schema_version":"1.0","source":{"id":"2209.14864","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2209.14864","created_at":"2026-07-05T06:03:58Z"},{"alias_kind":"arxiv_version","alias_value":"2209.14864v1","created_at":"2026-07-05T06:03:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.14864","created_at":"2026-07-05T06:03:58Z"},{"alias_kind":"pith_short_12","alias_value":"SF22TFERHFTY","created_at":"2026-07-05T06:03:58Z"},{"alias_kind":"pith_short_16","alias_value":"SF22TFERHFTYWQRW","created_at":"2026-07-05T06:03:58Z"},{"alias_kind":"pith_short_8","alias_value":"SF22TFER","created_at":"2026-07-05T06:03:58Z"}],"graph_snapshots":[{"event_id":"sha256:d62386d744e49e003f6d678f3066bd430de4f69faa0f4da859323b78feec566a","target":"graph","created_at":"2026-07-05T06:03:58Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2209.14864/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The Landau-gauge quark propagator is calculated using overlap fermions on 2+1-flavour dynamical fermion gauge fields from the PACS-CS collaboration with pion mass $m_\\pi \\sim 156\\text{ MeV}$ and spatial volume $\\sim (3 \\text{ fm})^3.$ The observed features of the mass and renormalisation functions are discussed, including a comparison with recent results using $\\mathcal{O}(a)$-improved Wilson fermions on 2-flavour dynamical gauge fields.","authors_text":"Adam Virgili, Derek Leinweber, Waseem Kamleh","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-09-29T15:31:35Z","title":"Overlap quark propagator near the physical pion mass"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.14864","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:7dacf70f840e8a94142a2018a4e5ae687ac94ec0e30210c66833996a41cfbf04","target":"record","created_at":"2026-07-05T06:03:58Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"2e192e49beed5b4e93d2f09c93432bfa015f889016133f97e95ea6a62720e1a5","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2022-09-29T15:31:35Z","title_canon_sha256":"6425a3aa1e933be138c0a6df04a8a367cfd556266a1812cf8ea19708bc7896f9"},"schema_version":"1.0","source":{"id":"2209.14864","kind":"arxiv","version":1}},"canonical_sha256":"9175a9949139678b42364c9a6bc21452d50b6cb57b8435072f993aa4099e97f4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9175a9949139678b42364c9a6bc21452d50b6cb57b8435072f993aa4099e97f4","first_computed_at":"2026-07-05T06:03:58.886961Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:03:58.886961Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"iuvLdL9O+h1foEyw5+PV689JmLDaQDvqU+1nAAIPG7vAIGwI5xT7DO2Ah/UQxEQyC+JOmqV8syjwibCdqQOzAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T06:03:58.887298Z","signed_message":"canonical_sha256_bytes"},"source_id":"2209.14864","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7dacf70f840e8a94142a2018a4e5ae687ac94ec0e30210c66833996a41cfbf04","sha256:d62386d744e49e003f6d678f3066bd430de4f69faa0f4da859323b78feec566a"],"state_sha256":"890f6fec7f7cd196eb86ad4fb390d021b15cbd143c72363a77515a50e0420ad0"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GTpYwQPuATbjcacLEOrJ8cvBChtrqW6WRUpwB0VjWKDNDFZQKAhIDFpBq/SOAI+cRwItElJl9VKBRYSWFhOuCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-09T12:27:51.355234Z","bundle_sha256":"2d4743b2c844bd9f2729f1718c404aec84238269257141c3d83af182bd28e87a"}}