{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:NBOLCZ6ML7JXFC6BNR3CGEIXIJ","short_pith_number":"pith:NBOLCZ6M","canonical_record":{"source":{"id":"1605.05645","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-05-18T16:22:49Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"d9105422c3c8b656a331746aa6236415bae3f6e35196483c36db91f014c6d892","abstract_canon_sha256":"ff3a66b8d09f774f6f1248394584ecd5c7708cb49f0be544e27fdc37baa8b2a6"},"schema_version":"1.0"},"canonical_sha256":"685cb167cc5fd3728bc16c76231117424e7917e191df44cd25fc84d6575dfc6e","source":{"kind":"arxiv","id":"1605.05645","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.05645","created_at":"2026-05-18T01:14:20Z"},{"alias_kind":"arxiv_version","alias_value":"1605.05645v2","created_at":"2026-05-18T01:14:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.05645","created_at":"2026-05-18T01:14:20Z"},{"alias_kind":"pith_short_12","alias_value":"NBOLCZ6ML7JX","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"NBOLCZ6ML7JXFC6B","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"NBOLCZ6M","created_at":"2026-05-18T12:30:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:NBOLCZ6ML7JXFC6BNR3CGEIXIJ","target":"record","payload":{"canonical_record":{"source":{"id":"1605.05645","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-05-18T16:22:49Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"d9105422c3c8b656a331746aa6236415bae3f6e35196483c36db91f014c6d892","abstract_canon_sha256":"ff3a66b8d09f774f6f1248394584ecd5c7708cb49f0be544e27fdc37baa8b2a6"},"schema_version":"1.0"},"canonical_sha256":"685cb167cc5fd3728bc16c76231117424e7917e191df44cd25fc84d6575dfc6e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:14:20.134090Z","signature_b64":"g9RHi5oKsOEE5XP6sDRBvNm1V6Oy9+NikqtM6Vh8UV2SJ4fdKGlvQLqh/GGye7AjweZ04/LsT3iLFgdtJap0Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"685cb167cc5fd3728bc16c76231117424e7917e191df44cd25fc84d6575dfc6e","last_reissued_at":"2026-05-18T01:14:20.133275Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:14:20.133275Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1605.05645","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:14:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"13Jr+qUxYmDZA39059zk/iFGUPFpsMSZdXs+/VpLAAgDbN331C9wmS5smO2advgvC+KuvS+/wo+MGzUQY30gBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T16:04:26.740345Z"},"content_sha256":"323a634c0366952a29f803ebc39128d4e4adb83ac789ba272e1e76294f97e6b9","schema_version":"1.0","event_id":"sha256:323a634c0366952a29f803ebc39128d4e4adb83ac789ba272e1e76294f97e6b9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:NBOLCZ6ML7JXFC6BNR3CGEIXIJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Semileptonic $B_c$ decays from full lattice QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-lat","authors_text":"Andrew Lytle, Brian Colquhoun, Christine Davies, Craig McNeile, Jonna Koponen","submitted_at":"2016-05-18T16:22:49Z","abstract_excerpt":"We present first lattice QCD results for semileptonic form factors for the decays $B_c \\to \\eta_c l \\nu$ and $B_c \\to J/\\psi l \\nu$ over the full $q^2$ range, using both improved non-relativistic QCD (NRQCD) and fully relativistic (HISQ) formalisms. These can be viewed as prototype calculations for pseudoscalar to pseudoscalar and pseudoscalar to vector decays involving a $b \\to c$ transition. In particular we can use information from the relativistic computations to fix the NRQCD current normalisations, which can then be used in improved computations of decays such as $B \\to D l \\nu$ and $B \\"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.05645","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":""},"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":"2026-05-18T01:14:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"J7rGxs3EB5kFRZq74CYb1xp/Z72Ro+e8SDJ6EZ8fWl+ZxdVAoYiLXxt+kttU50caXHO0mv1jEy2i2WHV+uwrDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T16:04:26.740829Z"},"content_sha256":"03b00bc928b17ff9dbfa347ac205dff56f2af273da0b01d6f34ed4fc29643a7c","schema_version":"1.0","event_id":"sha256:03b00bc928b17ff9dbfa347ac205dff56f2af273da0b01d6f34ed4fc29643a7c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NBOLCZ6ML7JXFC6BNR3CGEIXIJ/bundle.json","state_url":"https://pith.science/pith/NBOLCZ6ML7JXFC6BNR3CGEIXIJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NBOLCZ6ML7JXFC6BNR3CGEIXIJ/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":"2026-05-26T16:04:26Z","links":{"resolver":"https://pith.science/pith/NBOLCZ6ML7JXFC6BNR3CGEIXIJ","bundle":"https://pith.science/pith/NBOLCZ6ML7JXFC6BNR3CGEIXIJ/bundle.json","state":"https://pith.science/pith/NBOLCZ6ML7JXFC6BNR3CGEIXIJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NBOLCZ6ML7JXFC6BNR3CGEIXIJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:NBOLCZ6ML7JXFC6BNR3CGEIXIJ","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":"ff3a66b8d09f774f6f1248394584ecd5c7708cb49f0be544e27fdc37baa8b2a6","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-05-18T16:22:49Z","title_canon_sha256":"d9105422c3c8b656a331746aa6236415bae3f6e35196483c36db91f014c6d892"},"schema_version":"1.0","source":{"id":"1605.05645","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1605.05645","created_at":"2026-05-18T01:14:20Z"},{"alias_kind":"arxiv_version","alias_value":"1605.05645v2","created_at":"2026-05-18T01:14:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.05645","created_at":"2026-05-18T01:14:20Z"},{"alias_kind":"pith_short_12","alias_value":"NBOLCZ6ML7JX","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"NBOLCZ6ML7JXFC6B","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"NBOLCZ6M","created_at":"2026-05-18T12:30:32Z"}],"graph_snapshots":[{"event_id":"sha256:03b00bc928b17ff9dbfa347ac205dff56f2af273da0b01d6f34ed4fc29643a7c","target":"graph","created_at":"2026-05-18T01:14:20Z","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":"We present first lattice QCD results for semileptonic form factors for the decays $B_c \\to \\eta_c l \\nu$ and $B_c \\to J/\\psi l \\nu$ over the full $q^2$ range, using both improved non-relativistic QCD (NRQCD) and fully relativistic (HISQ) formalisms. These can be viewed as prototype calculations for pseudoscalar to pseudoscalar and pseudoscalar to vector decays involving a $b \\to c$ transition. In particular we can use information from the relativistic computations to fix the NRQCD current normalisations, which can then be used in improved computations of decays such as $B \\to D l \\nu$ and $B \\","authors_text":"Andrew Lytle, Brian Colquhoun, Christine Davies, Craig McNeile, Jonna Koponen","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-05-18T16:22:49Z","title":"Semileptonic $B_c$ decays from full lattice QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.05645","kind":"arxiv","version":2},"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":"sha256:323a634c0366952a29f803ebc39128d4e4adb83ac789ba272e1e76294f97e6b9","target":"record","created_at":"2026-05-18T01:14:20Z","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":"ff3a66b8d09f774f6f1248394584ecd5c7708cb49f0be544e27fdc37baa8b2a6","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2016-05-18T16:22:49Z","title_canon_sha256":"d9105422c3c8b656a331746aa6236415bae3f6e35196483c36db91f014c6d892"},"schema_version":"1.0","source":{"id":"1605.05645","kind":"arxiv","version":2}},"canonical_sha256":"685cb167cc5fd3728bc16c76231117424e7917e191df44cd25fc84d6575dfc6e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"685cb167cc5fd3728bc16c76231117424e7917e191df44cd25fc84d6575dfc6e","first_computed_at":"2026-05-18T01:14:20.133275Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:14:20.133275Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"g9RHi5oKsOEE5XP6sDRBvNm1V6Oy9+NikqtM6Vh8UV2SJ4fdKGlvQLqh/GGye7AjweZ04/LsT3iLFgdtJap0Aw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:14:20.134090Z","signed_message":"canonical_sha256_bytes"},"source_id":"1605.05645","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:323a634c0366952a29f803ebc39128d4e4adb83ac789ba272e1e76294f97e6b9","sha256:03b00bc928b17ff9dbfa347ac205dff56f2af273da0b01d6f34ed4fc29643a7c"],"state_sha256":"6d7ca672f4d96b9e9ae2cd04b759f25477f23e167e0c131df75c1282ce662e75"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cRrSYLLKQZX6jkGI8JeVMShl7SGM+M1gRy3csukxlnDnuNFppjZp2P9IV+54hZ6Tcb30KbPnY0h+L5h38nBRBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T16:04:26.743271Z","bundle_sha256":"749412366d7afd08d50cbd9304302fc12e78073b0ec75ea947e45ee1d6aa77b6"}}