{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:YAOCIGN5H2D45GJKDPPL62BZ64","short_pith_number":"pith:YAOCIGN5","canonical_record":{"source":{"id":"1310.3763","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-10-14T18:03:25Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"c61390faf9ed2e1274b0304d9f3834793f02a28a1bdd220fd629d12b213fc72b","abstract_canon_sha256":"28c3c5b902acaeb19bd29f10174bd56596421d793bfa83115fcfaab220b68557"},"schema_version":"1.0"},"canonical_sha256":"c01c2419bd3e87ce992a1bdebf6839f7358a194261d596f318454b47b0b3b7c8","source":{"kind":"arxiv","id":"1310.3763","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.3763","created_at":"2026-05-18T02:58:13Z"},{"alias_kind":"arxiv_version","alias_value":"1310.3763v4","created_at":"2026-05-18T02:58:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.3763","created_at":"2026-05-18T02:58:13Z"},{"alias_kind":"pith_short_12","alias_value":"YAOCIGN5H2D4","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"YAOCIGN5H2D45GJK","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"YAOCIGN5","created_at":"2026-05-18T12:28:06Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:YAOCIGN5H2D45GJKDPPL62BZ64","target":"record","payload":{"canonical_record":{"source":{"id":"1310.3763","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-10-14T18:03:25Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"c61390faf9ed2e1274b0304d9f3834793f02a28a1bdd220fd629d12b213fc72b","abstract_canon_sha256":"28c3c5b902acaeb19bd29f10174bd56596421d793bfa83115fcfaab220b68557"},"schema_version":"1.0"},"canonical_sha256":"c01c2419bd3e87ce992a1bdebf6839f7358a194261d596f318454b47b0b3b7c8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:58:13.099602Z","signature_b64":"vZ6AGnpUGm6243rj+Aaxlbt1g7CpMPN0FVQPS4ZfGpH0yswbAPCKQk+LCR5alkHx3BqiKsjykjXLwyKUL55ADA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c01c2419bd3e87ce992a1bdebf6839f7358a194261d596f318454b47b0b3b7c8","last_reissued_at":"2026-05-18T02:58:13.098859Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:58:13.098859Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1310.3763","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:58:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mcd1sD6fv7c6FgQIQRWY0xGibo0/0m/T2/Eqt6BLYLJ1UonxQ6sbhF5Kh+Gh75WXawY2s0RFfFy/0eK48RmVCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:09:05.009732Z"},"content_sha256":"36f2a2a1c9b97e104f8b9d0d2643b4bc38e91fbe604ee5d5123a2626051e3291","schema_version":"1.0","event_id":"sha256:36f2a2a1c9b97e104f8b9d0d2643b4bc38e91fbe604ee5d5123a2626051e3291"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:YAOCIGN5H2D45GJKDPPL62BZ64","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"High statistics determination of the strong coupling constant in Taylor scheme and its OPE Wilson coefficient from lattice QCD with a dynamical charm","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"B. Blossier, F. de Soto, J. Rodr\\'iguez-Quintero, K. Petrov, M. Brinet, O. P\\`ene, Ph. Boucaud, V. Morenas","submitted_at":"2013-10-14T18:03:25Z","abstract_excerpt":"This paper reports on the determination of $\\alpha_S$ from lattice simulations with 2+1+1 twisted-mass dynamical flavours {\\it via} the computation of the ghost-gluon coupling renormalized in the MOM Taylor scheme. A high-statistics sample of gauge configurations, used to evaluate the coupling from ghost and gluon propagators, allows for the appropriate update of previous results, now performing an improved analysis of data with reduced statistical errors and the systematical uncertainties under a better control."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.3763","kind":"arxiv","version":4},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:58:13Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rnpV+f1h6xjB5nHFcYe4Mki7rvtE/SdCWJylgzgplnhygDxezlBXmE6stkRMHbV8mVkPNBPzQpH0kQlnsjhJCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T21:09:05.010392Z"},"content_sha256":"09a9166ecf1bc6aab710403cb7c39b72f32c8cbf7cc89295a43fc77a34171803","schema_version":"1.0","event_id":"sha256:09a9166ecf1bc6aab710403cb7c39b72f32c8cbf7cc89295a43fc77a34171803"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YAOCIGN5H2D45GJKDPPL62BZ64/bundle.json","state_url":"https://pith.science/pith/YAOCIGN5H2D45GJKDPPL62BZ64/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YAOCIGN5H2D45GJKDPPL62BZ64/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":"2026-05-27T21:09:05Z","links":{"resolver":"https://pith.science/pith/YAOCIGN5H2D45GJKDPPL62BZ64","bundle":"https://pith.science/pith/YAOCIGN5H2D45GJKDPPL62BZ64/bundle.json","state":"https://pith.science/pith/YAOCIGN5H2D45GJKDPPL62BZ64/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YAOCIGN5H2D45GJKDPPL62BZ64/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:YAOCIGN5H2D45GJKDPPL62BZ64","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":"28c3c5b902acaeb19bd29f10174bd56596421d793bfa83115fcfaab220b68557","cross_cats_sorted":["hep-lat"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-10-14T18:03:25Z","title_canon_sha256":"c61390faf9ed2e1274b0304d9f3834793f02a28a1bdd220fd629d12b213fc72b"},"schema_version":"1.0","source":{"id":"1310.3763","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1310.3763","created_at":"2026-05-18T02:58:13Z"},{"alias_kind":"arxiv_version","alias_value":"1310.3763v4","created_at":"2026-05-18T02:58:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.3763","created_at":"2026-05-18T02:58:13Z"},{"alias_kind":"pith_short_12","alias_value":"YAOCIGN5H2D4","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_16","alias_value":"YAOCIGN5H2D45GJK","created_at":"2026-05-18T12:28:06Z"},{"alias_kind":"pith_short_8","alias_value":"YAOCIGN5","created_at":"2026-05-18T12:28:06Z"}],"graph_snapshots":[{"event_id":"sha256:09a9166ecf1bc6aab710403cb7c39b72f32c8cbf7cc89295a43fc77a34171803","target":"graph","created_at":"2026-05-18T02:58:13Z","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"},"paper":{"abstract_excerpt":"This paper reports on the determination of $\\alpha_S$ from lattice simulations with 2+1+1 twisted-mass dynamical flavours {\\it via} the computation of the ghost-gluon coupling renormalized in the MOM Taylor scheme. A high-statistics sample of gauge configurations, used to evaluate the coupling from ghost and gluon propagators, allows for the appropriate update of previous results, now performing an improved analysis of data with reduced statistical errors and the systematical uncertainties under a better control.","authors_text":"B. Blossier, F. de Soto, J. Rodr\\'iguez-Quintero, K. Petrov, M. Brinet, O. P\\`ene, Ph. Boucaud, V. Morenas","cross_cats":["hep-lat"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-10-14T18:03:25Z","title":"High statistics determination of the strong coupling constant in Taylor scheme and its OPE Wilson coefficient from lattice QCD with a dynamical charm"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.3763","kind":"arxiv","version":4},"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":"sha256:36f2a2a1c9b97e104f8b9d0d2643b4bc38e91fbe604ee5d5123a2626051e3291","target":"record","created_at":"2026-05-18T02:58:13Z","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":"28c3c5b902acaeb19bd29f10174bd56596421d793bfa83115fcfaab220b68557","cross_cats_sorted":["hep-lat"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-10-14T18:03:25Z","title_canon_sha256":"c61390faf9ed2e1274b0304d9f3834793f02a28a1bdd220fd629d12b213fc72b"},"schema_version":"1.0","source":{"id":"1310.3763","kind":"arxiv","version":4}},"canonical_sha256":"c01c2419bd3e87ce992a1bdebf6839f7358a194261d596f318454b47b0b3b7c8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c01c2419bd3e87ce992a1bdebf6839f7358a194261d596f318454b47b0b3b7c8","first_computed_at":"2026-05-18T02:58:13.098859Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:58:13.098859Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vZ6AGnpUGm6243rj+Aaxlbt1g7CpMPN0FVQPS4ZfGpH0yswbAPCKQk+LCR5alkHx3BqiKsjykjXLwyKUL55ADA==","signature_status":"signed_v1","signed_at":"2026-05-18T02:58:13.099602Z","signed_message":"canonical_sha256_bytes"},"source_id":"1310.3763","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:36f2a2a1c9b97e104f8b9d0d2643b4bc38e91fbe604ee5d5123a2626051e3291","sha256:09a9166ecf1bc6aab710403cb7c39b72f32c8cbf7cc89295a43fc77a34171803"],"state_sha256":"0d537cec8acf51894e39673bc98f42ce5c933a749d98af7af5d12f4152fb5581"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"16UPSSJm5MxuQprs7xyO2Su6Twf4HoDwXYC1AId4Hso5wlhbLyM15PXCAHqgbwWpjNf/wPBVzge8kN/HnxiKDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T21:09:05.013770Z","bundle_sha256":"1072f90ada2b4b0819451c9fd6cd56438618c9635b53c309a81749fff5b74379"}}