{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2026:7M3FG2Q5K4F4S52B7AGFOIVF4Q","short_pith_number":"pith:7M3FG2Q5","canonical_record":{"source":{"id":"2603.18711","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-03-19T10:11:14Z","cross_cats_sorted":[],"title_canon_sha256":"df90375d6c80ee285ea93b9bcf50130c10d4c456a0f8019d1281a889d5bcecfa","abstract_canon_sha256":"6088f5d9a80ab96b7a691bf855471e4e6a78e25ecf44d6cd3598409e74c3e20a"},"schema_version":"1.0"},"canonical_sha256":"fb36536a1d570bc97741f80c5722a5e409e15457bb4dc7c07dbdf1f5362a9bf2","source":{"kind":"arxiv","id":"2603.18711","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2603.18711","created_at":"2026-06-02T02:04:16Z"},{"alias_kind":"arxiv_version","alias_value":"2603.18711v3","created_at":"2026-06-02T02:04:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.18711","created_at":"2026-06-02T02:04:16Z"},{"alias_kind":"pith_short_12","alias_value":"7M3FG2Q5K4F4","created_at":"2026-06-02T02:04:16Z"},{"alias_kind":"pith_short_16","alias_value":"7M3FG2Q5K4F4S52B","created_at":"2026-06-02T02:04:16Z"},{"alias_kind":"pith_short_8","alias_value":"7M3FG2Q5","created_at":"2026-06-02T02:04:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2026:7M3FG2Q5K4F4S52B7AGFOIVF4Q","target":"record","payload":{"canonical_record":{"source":{"id":"2603.18711","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-03-19T10:11:14Z","cross_cats_sorted":[],"title_canon_sha256":"df90375d6c80ee285ea93b9bcf50130c10d4c456a0f8019d1281a889d5bcecfa","abstract_canon_sha256":"6088f5d9a80ab96b7a691bf855471e4e6a78e25ecf44d6cd3598409e74c3e20a"},"schema_version":"1.0"},"canonical_sha256":"fb36536a1d570bc97741f80c5722a5e409e15457bb4dc7c07dbdf1f5362a9bf2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-02T02:04:16.306630Z","signature_b64":"a6mt99sDa4XHeqyl+gW9AzBdETr4OeXGgg9OBauLxJAPQGuqoqxOITcVjKVfnYjZVEBXqZAFogMEL7/xSJozBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fb36536a1d570bc97741f80c5722a5e409e15457bb4dc7c07dbdf1f5362a9bf2","last_reissued_at":"2026-06-02T02:04:16.306044Z","signature_status":"signed_v1","first_computed_at":"2026-06-02T02:04:16.306044Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2603.18711","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-02T02:04:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vwHsxpDmnUnH4iNK59VVLqWp/Q6BwQU+2J0xhfZzmzx7OdeQAxVzIv5T8QMaMh03lYSg78LOux08MlcSyibpDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T21:14:42.294681Z"},"content_sha256":"1882df4fe9e6984dac984d20e5fab1ed35f9cca22c839b8ebffce30336904b03","schema_version":"1.0","event_id":"sha256:1882df4fe9e6984dac984d20e5fab1ed35f9cca22c839b8ebffce30336904b03"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2026:7M3FG2Q5K4F4S52B7AGFOIVF4Q","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Correlator of heavy-light quark currents in HQET in the large $\\beta_0$ limit","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"The leading 1/β₀ term approximates the perturbative contribution to the heavy-light quark current correlator in HQET up to quadratic light-quark masses.","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andrey G. Grozin","submitted_at":"2026-03-19T10:11:14Z","abstract_excerpt":"The perturbative contribution to the correlator of two heavy-light quark currents in HQET expanded in light-quark masses up to quadratic terms is calculated at the leading order in $1/\\beta_0$. Ultraviolet and infrared renormalon poles of Borel images of the Wilson coefficients are discussed."},"claims":{"count":4,"items":[{"kind":"strongest_claim","text":"The perturbative contribution to the correlator of two heavy-light quark currents in HQET expanded in light-quark masses up to quadratic terms is calculated at the leading order in 1/β₀.","source":"verdict.strongest_claim","status":"machine_extracted","claim_id":"C1","attestation":"unclaimed"},{"kind":"weakest_assumption","text":"That the leading 1/β₀ term faithfully approximates the full perturbative series for the Wilson coefficients of this particular correlator once the light-quark mass expansion is performed.","source":"verdict.weakest_assumption","status":"machine_extracted","claim_id":"C2","attestation":"unclaimed"},{"kind":"one_line_summary","text":"Perturbative HQET correlator of heavy-light currents computed to O(m_q²) at leading 1/β₀ order with explicit renormalon-pole locations.","source":"verdict.one_line_summary","status":"machine_extracted","claim_id":"C3","attestation":"unclaimed"},{"kind":"headline","text":"The leading 1/β₀ term approximates the perturbative contribution to the heavy-light quark current correlator in HQET up to quadratic light-quark masses.","source":"verdict.pith_extraction.headline","status":"machine_extracted","claim_id":"C4","attestation":"unclaimed"}],"snapshot_sha256":"9aed026681ea5834d0857e7cc05709bc874980dbfb978363a8d37dfedc7aedd3"},"source":{"id":"2603.18711","kind":"arxiv","version":3},"verdict":{"id":"cc6995ac-acff-4535-b01e-1a0c3452b0bc","model_set":{"reader":"grok-4.3"},"created_at":"2026-05-15T09:09:32.283689Z","strongest_claim":"The perturbative contribution to the correlator of two heavy-light quark currents in HQET expanded in light-quark masses up to quadratic terms is calculated at the leading order in 1/β₀.","one_line_summary":"Perturbative HQET correlator of heavy-light currents computed to O(m_q²) at leading 1/β₀ order with explicit renormalon-pole locations.","pipeline_version":"pith-pipeline@v0.9.0","weakest_assumption":"That the leading 1/β₀ term faithfully approximates the full perturbative series for the Wilson coefficients of this particular correlator once the light-quark mass expansion is performed.","pith_extraction_headline":"The leading 1/β₀ term approximates the perturbative contribution to the heavy-light quark current correlator in HQET up to quadratic light-quark masses."},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2603.18711/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":2,"snapshot_sha256":"383b923d936768f3b524f61b9bb21b9d18c6c5050e143eae237dda4d48d51f8f"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":"cc6995ac-acff-4535-b01e-1a0c3452b0bc"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-02T02:04:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HpAjJkIiTeLgwHVMnmPRM0vQDw6l8fYaGRTViIOMnU2Oy1a5mAG3b4A+WIO4FPzJiGp1PkzNzHYhW+3kS7RbAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T21:14:42.295757Z"},"content_sha256":"d31edeaff04ee1782435887e300dc1957151189f40784968c337776202ab9b3d","schema_version":"1.0","event_id":"sha256:d31edeaff04ee1782435887e300dc1957151189f40784968c337776202ab9b3d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7M3FG2Q5K4F4S52B7AGFOIVF4Q/bundle.json","state_url":"https://pith.science/pith/7M3FG2Q5K4F4S52B7AGFOIVF4Q/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7M3FG2Q5K4F4S52B7AGFOIVF4Q/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":"2026-06-11T21:14:42Z","links":{"resolver":"https://pith.science/pith/7M3FG2Q5K4F4S52B7AGFOIVF4Q","bundle":"https://pith.science/pith/7M3FG2Q5K4F4S52B7AGFOIVF4Q/bundle.json","state":"https://pith.science/pith/7M3FG2Q5K4F4S52B7AGFOIVF4Q/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7M3FG2Q5K4F4S52B7AGFOIVF4Q/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:7M3FG2Q5K4F4S52B7AGFOIVF4Q","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":"6088f5d9a80ab96b7a691bf855471e4e6a78e25ecf44d6cd3598409e74c3e20a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-03-19T10:11:14Z","title_canon_sha256":"df90375d6c80ee285ea93b9bcf50130c10d4c456a0f8019d1281a889d5bcecfa"},"schema_version":"1.0","source":{"id":"2603.18711","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2603.18711","created_at":"2026-06-02T02:04:16Z"},{"alias_kind":"arxiv_version","alias_value":"2603.18711v3","created_at":"2026-06-02T02:04:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.18711","created_at":"2026-06-02T02:04:16Z"},{"alias_kind":"pith_short_12","alias_value":"7M3FG2Q5K4F4","created_at":"2026-06-02T02:04:16Z"},{"alias_kind":"pith_short_16","alias_value":"7M3FG2Q5K4F4S52B","created_at":"2026-06-02T02:04:16Z"},{"alias_kind":"pith_short_8","alias_value":"7M3FG2Q5","created_at":"2026-06-02T02:04:16Z"}],"graph_snapshots":[{"event_id":"sha256:d31edeaff04ee1782435887e300dc1957151189f40784968c337776202ab9b3d","target":"graph","created_at":"2026-06-02T02:04:16Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"The perturbative contribution to the correlator of two heavy-light quark currents in HQET expanded in light-quark masses up to quadratic terms is calculated at the leading order in 1/β₀."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"That the leading 1/β₀ term faithfully approximates the full perturbative series for the Wilson coefficients of this particular correlator once the light-quark mass expansion is performed."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Perturbative HQET correlator of heavy-light currents computed to O(m_q²) at leading 1/β₀ order with explicit renormalon-pole locations."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"The leading 1/β₀ term approximates the perturbative contribution to the heavy-light quark current correlator in HQET up to quadratic light-quark masses."}],"snapshot_sha256":"9aed026681ea5834d0857e7cc05709bc874980dbfb978363a8d37dfedc7aedd3"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"383b923d936768f3b524f61b9bb21b9d18c6c5050e143eae237dda4d48d51f8f"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2603.18711/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The perturbative contribution to the correlator of two heavy-light quark currents in HQET expanded in light-quark masses up to quadratic terms is calculated at the leading order in $1/\\beta_0$. Ultraviolet and infrared renormalon poles of Borel images of the Wilson coefficients are discussed.","authors_text":"Andrey G. Grozin","cross_cats":[],"headline":"The leading 1/β₀ term approximates the perturbative contribution to the heavy-light quark current correlator in HQET up to quadratic light-quark masses.","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-03-19T10:11:14Z","title":"Correlator of heavy-light quark currents in HQET in the large $\\beta_0$ limit"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.18711","kind":"arxiv","version":3},"verdict":{"created_at":"2026-05-15T09:09:32.283689Z","id":"cc6995ac-acff-4535-b01e-1a0c3452b0bc","model_set":{"reader":"grok-4.3"},"one_line_summary":"Perturbative HQET correlator of heavy-light currents computed to O(m_q²) at leading 1/β₀ order with explicit renormalon-pole locations.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"The leading 1/β₀ term approximates the perturbative contribution to the heavy-light quark current correlator in HQET up to quadratic light-quark masses.","strongest_claim":"The perturbative contribution to the correlator of two heavy-light quark currents in HQET expanded in light-quark masses up to quadratic terms is calculated at the leading order in 1/β₀.","weakest_assumption":"That the leading 1/β₀ term faithfully approximates the full perturbative series for the Wilson coefficients of this particular correlator once the light-quark mass expansion is performed."}},"verdict_id":"cc6995ac-acff-4535-b01e-1a0c3452b0bc"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:1882df4fe9e6984dac984d20e5fab1ed35f9cca22c839b8ebffce30336904b03","target":"record","created_at":"2026-06-02T02:04:16Z","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":"6088f5d9a80ab96b7a691bf855471e4e6a78e25ecf44d6cd3598409e74c3e20a","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2026-03-19T10:11:14Z","title_canon_sha256":"df90375d6c80ee285ea93b9bcf50130c10d4c456a0f8019d1281a889d5bcecfa"},"schema_version":"1.0","source":{"id":"2603.18711","kind":"arxiv","version":3}},"canonical_sha256":"fb36536a1d570bc97741f80c5722a5e409e15457bb4dc7c07dbdf1f5362a9bf2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fb36536a1d570bc97741f80c5722a5e409e15457bb4dc7c07dbdf1f5362a9bf2","first_computed_at":"2026-06-02T02:04:16.306044Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-02T02:04:16.306044Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"a6mt99sDa4XHeqyl+gW9AzBdETr4OeXGgg9OBauLxJAPQGuqoqxOITcVjKVfnYjZVEBXqZAFogMEL7/xSJozBQ==","signature_status":"signed_v1","signed_at":"2026-06-02T02:04:16.306630Z","signed_message":"canonical_sha256_bytes"},"source_id":"2603.18711","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1882df4fe9e6984dac984d20e5fab1ed35f9cca22c839b8ebffce30336904b03","sha256:d31edeaff04ee1782435887e300dc1957151189f40784968c337776202ab9b3d"],"state_sha256":"1d4fcf8b255802fe593ee4fd3705e650bb1a01921cde051f8bd8cbb49ea2dd64"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JXyJlpSWLADBxta67HYD8cI5Sw0x+p/ZEBZ9iGZCLYPIWqxDIPICZMkOagHZwgSIGyjkVNMrJNO9OGSzqePACQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T21:14:42.301225Z","bundle_sha256":"9fb8c814b4bb6423cbf0c7eb1d374c4667cffbc3a4e5c656ec563f9e50f89b59"}}