{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:S5DKVAJ54WASI5YVZFVT7YLBN5","short_pith_number":"pith:S5DKVAJ5","canonical_record":{"source":{"id":"2205.03410","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-05-06T18:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"762f8d27f041be7dd377c846163877144ad8788f3f5654acc37547d73d491a5e","abstract_canon_sha256":"94fd8c342360803ccfb8182e4d5803c90d831f5a23b9e7afa7b80dadfcb79529"},"schema_version":"1.0"},"canonical_sha256":"9746aa813de581247715c96b3fe1616f58d2f3506b052b2d1fb4e1593b90f476","source":{"kind":"arxiv","id":"2205.03410","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2205.03410","created_at":"2026-07-05T04:50:56Z"},{"alias_kind":"arxiv_version","alias_value":"2205.03410v1","created_at":"2026-07-05T04:50:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.03410","created_at":"2026-07-05T04:50:56Z"},{"alias_kind":"pith_short_12","alias_value":"S5DKVAJ54WAS","created_at":"2026-07-05T04:50:56Z"},{"alias_kind":"pith_short_16","alias_value":"S5DKVAJ54WASI5YV","created_at":"2026-07-05T04:50:56Z"},{"alias_kind":"pith_short_8","alias_value":"S5DKVAJ5","created_at":"2026-07-05T04:50:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:S5DKVAJ54WASI5YVZFVT7YLBN5","target":"record","payload":{"canonical_record":{"source":{"id":"2205.03410","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-05-06T18:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"762f8d27f041be7dd377c846163877144ad8788f3f5654acc37547d73d491a5e","abstract_canon_sha256":"94fd8c342360803ccfb8182e4d5803c90d831f5a23b9e7afa7b80dadfcb79529"},"schema_version":"1.0"},"canonical_sha256":"9746aa813de581247715c96b3fe1616f58d2f3506b052b2d1fb4e1593b90f476","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:50:56.740667Z","signature_b64":"ocwR+jk0aRlOtqk/NsX70BC78XwfnM7R2E37vDlvDnddbPJ5NxtpsT5zflKOBb28bGOZ6XABETLxHIH1uIKNBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9746aa813de581247715c96b3fe1616f58d2f3506b052b2d1fb4e1593b90f476","last_reissued_at":"2026-07-05T04:50:56.740106Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:50:56.740106Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2205.03410","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":"2026-07-05T04:50:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qOtidnhDuGNgsdzMTXi6Eu5O9Zvm+M6UXDFBBhPQMlTQXJuCAzdh5izYy0wG7FhxPAWvLDHOg5kFkQzgQkikDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T00:59:03.263650Z"},"content_sha256":"219a4ce87f800d29da39e063528eed8f36e404c8d0874837ae2ddaa849089b75","schema_version":"1.0","event_id":"sha256:219a4ce87f800d29da39e063528eed8f36e404c8d0874837ae2ddaa849089b75"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:S5DKVAJ54WASI5YVZFVT7YLBN5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A first glance to the kinematic moments of $B \\to X_c \\ell \\nu$ at third order","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Kay Sch\\\"onwald, Matteo Fael, Matthias Steinhauser","submitted_at":"2022-05-06T18:00:00Z","abstract_excerpt":"We study the impact of third-order QCD corrections for several kinematic moments of the inclusive semileptonic $B$ decays, to first order in the $1/m_b$ expansion. We consider the first four moments of the charged-lepton energy $E_\\ell$ spectrum, the total leptonic invariant mass $q^2$ and the hadronic invariant mass $M_X^2$. No experimental cuts are applied. Our analytic results are obtained via an asymptotic expansion around the limit $m_b \\simeq m_c$. After converting the scheme for the bottom mass to the kinetic scheme we compare the size of higher QCD corrections to the contributions from"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.03410","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/2205.03410/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":"2026-07-05T04:50:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PMS+lTqxW8lyNd6miCGq90Rf67l6TBldyyfQLuODkgxpUUvRixs3gRMiWJSTGWdTelf9G7H+Dfj6WApwH9L7Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T00:59:03.264065Z"},"content_sha256":"3074ecb3975755fdff73723981a7af30058811e51a0be2a376ee65b13856e890","schema_version":"1.0","event_id":"sha256:3074ecb3975755fdff73723981a7af30058811e51a0be2a376ee65b13856e890"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/S5DKVAJ54WASI5YVZFVT7YLBN5/bundle.json","state_url":"https://pith.science/pith/S5DKVAJ54WASI5YVZFVT7YLBN5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/S5DKVAJ54WASI5YVZFVT7YLBN5/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":"2026-08-04T00:59:03Z","links":{"resolver":"https://pith.science/pith/S5DKVAJ54WASI5YVZFVT7YLBN5","bundle":"https://pith.science/pith/S5DKVAJ54WASI5YVZFVT7YLBN5/bundle.json","state":"https://pith.science/pith/S5DKVAJ54WASI5YVZFVT7YLBN5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/S5DKVAJ54WASI5YVZFVT7YLBN5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:S5DKVAJ54WASI5YVZFVT7YLBN5","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":"94fd8c342360803ccfb8182e4d5803c90d831f5a23b9e7afa7b80dadfcb79529","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-05-06T18:00:00Z","title_canon_sha256":"762f8d27f041be7dd377c846163877144ad8788f3f5654acc37547d73d491a5e"},"schema_version":"1.0","source":{"id":"2205.03410","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2205.03410","created_at":"2026-07-05T04:50:56Z"},{"alias_kind":"arxiv_version","alias_value":"2205.03410v1","created_at":"2026-07-05T04:50:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.03410","created_at":"2026-07-05T04:50:56Z"},{"alias_kind":"pith_short_12","alias_value":"S5DKVAJ54WAS","created_at":"2026-07-05T04:50:56Z"},{"alias_kind":"pith_short_16","alias_value":"S5DKVAJ54WASI5YV","created_at":"2026-07-05T04:50:56Z"},{"alias_kind":"pith_short_8","alias_value":"S5DKVAJ5","created_at":"2026-07-05T04:50:56Z"}],"graph_snapshots":[{"event_id":"sha256:3074ecb3975755fdff73723981a7af30058811e51a0be2a376ee65b13856e890","target":"graph","created_at":"2026-07-05T04:50:56Z","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/2205.03410/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study the impact of third-order QCD corrections for several kinematic moments of the inclusive semileptonic $B$ decays, to first order in the $1/m_b$ expansion. We consider the first four moments of the charged-lepton energy $E_\\ell$ spectrum, the total leptonic invariant mass $q^2$ and the hadronic invariant mass $M_X^2$. No experimental cuts are applied. Our analytic results are obtained via an asymptotic expansion around the limit $m_b \\simeq m_c$. After converting the scheme for the bottom mass to the kinetic scheme we compare the size of higher QCD corrections to the contributions from","authors_text":"Kay Sch\\\"onwald, Matteo Fael, Matthias Steinhauser","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-05-06T18:00:00Z","title":"A first glance to the kinematic moments of $B \\to X_c \\ell \\nu$ at third order"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.03410","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":"sha256:219a4ce87f800d29da39e063528eed8f36e404c8d0874837ae2ddaa849089b75","target":"record","created_at":"2026-07-05T04:50:56Z","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":"94fd8c342360803ccfb8182e4d5803c90d831f5a23b9e7afa7b80dadfcb79529","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-05-06T18:00:00Z","title_canon_sha256":"762f8d27f041be7dd377c846163877144ad8788f3f5654acc37547d73d491a5e"},"schema_version":"1.0","source":{"id":"2205.03410","kind":"arxiv","version":1}},"canonical_sha256":"9746aa813de581247715c96b3fe1616f58d2f3506b052b2d1fb4e1593b90f476","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9746aa813de581247715c96b3fe1616f58d2f3506b052b2d1fb4e1593b90f476","first_computed_at":"2026-07-05T04:50:56.740106Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:50:56.740106Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ocwR+jk0aRlOtqk/NsX70BC78XwfnM7R2E37vDlvDnddbPJ5NxtpsT5zflKOBb28bGOZ6XABETLxHIH1uIKNBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T04:50:56.740667Z","signed_message":"canonical_sha256_bytes"},"source_id":"2205.03410","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:219a4ce87f800d29da39e063528eed8f36e404c8d0874837ae2ddaa849089b75","sha256:3074ecb3975755fdff73723981a7af30058811e51a0be2a376ee65b13856e890"],"state_sha256":"4b5ba1d1207fcef373f6db66f7677c575dc65687a525365fcb1b8e2c925dfffa"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aqX6rhD1p+hZsD/+1ezc+gCzOX3DIkUXtYWkrQ9AWcNgECwlQ6Dt6+NuycBlYwRVmCQZ6KSCYKFXFBfLYBYCCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T00:59:03.266736Z","bundle_sha256":"d354b9042caa770e71b6b359f9061cd7c489fa26e1ed27e7eba55cb2dc8f0996"}}