{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:NMSVFHM23ZKT62BFCNSAQWOKHL","short_pith_number":"pith:NMSVFHM2","canonical_record":{"source":{"id":"1610.01469","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-04T10:52:56Z","cross_cats_sorted":[],"title_canon_sha256":"d1990b2aee1ab46f6c4878d1c39c3aa2109593b58b5d45616004a3d2f8ad8c4d","abstract_canon_sha256":"bafdd1cfe1ceb2608a8af34b8d0bf2f9d8d7e64cfe4114cdc95e469af86a6209"},"schema_version":"1.0"},"canonical_sha256":"6b25529d9ade553f682513640859ca3acac2f6c2c5eda89e3fd30a2db3bcfcca","source":{"kind":"arxiv","id":"1610.01469","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.01469","created_at":"2026-05-18T00:48:26Z"},{"alias_kind":"arxiv_version","alias_value":"1610.01469v3","created_at":"2026-05-18T00:48:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.01469","created_at":"2026-05-18T00:48:26Z"},{"alias_kind":"pith_short_12","alias_value":"NMSVFHM23ZKT","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"NMSVFHM23ZKT62BF","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"NMSVFHM2","created_at":"2026-05-18T12:30:32Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:NMSVFHM23ZKT62BFCNSAQWOKHL","target":"record","payload":{"canonical_record":{"source":{"id":"1610.01469","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-04T10:52:56Z","cross_cats_sorted":[],"title_canon_sha256":"d1990b2aee1ab46f6c4878d1c39c3aa2109593b58b5d45616004a3d2f8ad8c4d","abstract_canon_sha256":"bafdd1cfe1ceb2608a8af34b8d0bf2f9d8d7e64cfe4114cdc95e469af86a6209"},"schema_version":"1.0"},"canonical_sha256":"6b25529d9ade553f682513640859ca3acac2f6c2c5eda89e3fd30a2db3bcfcca","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:48:26.344981Z","signature_b64":"p2L0qlA3WFmquukQMJKA1tViNTHU8pcZuW8CW+wqmK9twNW60EZs1yQuH618+w1yQ41lm61bfl4oJV71l3/JAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6b25529d9ade553f682513640859ca3acac2f6c2c5eda89e3fd30a2db3bcfcca","last_reissued_at":"2026-05-18T00:48:26.344333Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:48:26.344333Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1610.01469","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":"2026-05-18T00:48:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ln8vCqzCEWIUezkn99oKJDYq7/HsqB4zjDEY2uHTX3qHTrqGHEP/h/7dyO3EfDVFQITf7hb5l2F91HZoQvbHDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T05:01:42.272536Z"},"content_sha256":"95cffe7671e322a5666945d4c786ccd65b3e59e0c82fb47a4f3f10457cf7ab23","schema_version":"1.0","event_id":"sha256:95cffe7671e322a5666945d4c786ccd65b3e59e0c82fb47a4f3f10457cf7ab23"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:NMSVFHM23ZKT62BFCNSAQWOKHL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Searching for New Physics in Semi-Leptonic Baryon Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Elvio Di Salvo, Ziad J. Ajaltouni","submitted_at":"2016-10-04T10:52:56Z","abstract_excerpt":"We propose two different and complementary observables for singling out possible signals of physics beyond the standard model in the semi-leptonic decays $\\Lambda_b \\to \\Lambda_c \\ell{\\bar \\nu}_{\\ell}$, both with the $\\tau$ lepton and with a light lepton. The two observables are the partial decay width and a T-odd asymmetry, whose respective sensitivities to scalar and/or pseudo-scalar coupling are calculated as functions of the parameters characterizing new physics. Two different form factors are used. Three particular cases are discussed and analyzed in detail."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.01469","kind":"arxiv","version":3},"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":"2026-05-18T00:48:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jOXOpvscuT9mI9DG9S9PtDbM2Ha5+Y0erHy5Ty5HSQTZZ1do2d/8CfXP8xY2V1hMM02znV0jHOLSgpRi6e5zCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-29T05:01:42.272872Z"},"content_sha256":"49f5e62cebe5df5b336f140956a3b215306ca69c4b34cfa9212cea5258e6036b","schema_version":"1.0","event_id":"sha256:49f5e62cebe5df5b336f140956a3b215306ca69c4b34cfa9212cea5258e6036b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NMSVFHM23ZKT62BFCNSAQWOKHL/bundle.json","state_url":"https://pith.science/pith/NMSVFHM23ZKT62BFCNSAQWOKHL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NMSVFHM23ZKT62BFCNSAQWOKHL/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":"2026-06-29T05:01:42Z","links":{"resolver":"https://pith.science/pith/NMSVFHM23ZKT62BFCNSAQWOKHL","bundle":"https://pith.science/pith/NMSVFHM23ZKT62BFCNSAQWOKHL/bundle.json","state":"https://pith.science/pith/NMSVFHM23ZKT62BFCNSAQWOKHL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NMSVFHM23ZKT62BFCNSAQWOKHL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:NMSVFHM23ZKT62BFCNSAQWOKHL","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":"bafdd1cfe1ceb2608a8af34b8d0bf2f9d8d7e64cfe4114cdc95e469af86a6209","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-04T10:52:56Z","title_canon_sha256":"d1990b2aee1ab46f6c4878d1c39c3aa2109593b58b5d45616004a3d2f8ad8c4d"},"schema_version":"1.0","source":{"id":"1610.01469","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.01469","created_at":"2026-05-18T00:48:26Z"},{"alias_kind":"arxiv_version","alias_value":"1610.01469v3","created_at":"2026-05-18T00:48:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.01469","created_at":"2026-05-18T00:48:26Z"},{"alias_kind":"pith_short_12","alias_value":"NMSVFHM23ZKT","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"NMSVFHM23ZKT62BF","created_at":"2026-05-18T12:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"NMSVFHM2","created_at":"2026-05-18T12:30:32Z"}],"graph_snapshots":[{"event_id":"sha256:49f5e62cebe5df5b336f140956a3b215306ca69c4b34cfa9212cea5258e6036b","target":"graph","created_at":"2026-05-18T00:48:26Z","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 propose two different and complementary observables for singling out possible signals of physics beyond the standard model in the semi-leptonic decays $\\Lambda_b \\to \\Lambda_c \\ell{\\bar \\nu}_{\\ell}$, both with the $\\tau$ lepton and with a light lepton. The two observables are the partial decay width and a T-odd asymmetry, whose respective sensitivities to scalar and/or pseudo-scalar coupling are calculated as functions of the parameters characterizing new physics. Two different form factors are used. Three particular cases are discussed and analyzed in detail.","authors_text":"Elvio Di Salvo, Ziad J. Ajaltouni","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-04T10:52:56Z","title":"Searching for New Physics in Semi-Leptonic Baryon Decays"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.01469","kind":"arxiv","version":3},"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":"sha256:95cffe7671e322a5666945d4c786ccd65b3e59e0c82fb47a4f3f10457cf7ab23","target":"record","created_at":"2026-05-18T00:48:26Z","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":"bafdd1cfe1ceb2608a8af34b8d0bf2f9d8d7e64cfe4114cdc95e469af86a6209","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-10-04T10:52:56Z","title_canon_sha256":"d1990b2aee1ab46f6c4878d1c39c3aa2109593b58b5d45616004a3d2f8ad8c4d"},"schema_version":"1.0","source":{"id":"1610.01469","kind":"arxiv","version":3}},"canonical_sha256":"6b25529d9ade553f682513640859ca3acac2f6c2c5eda89e3fd30a2db3bcfcca","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6b25529d9ade553f682513640859ca3acac2f6c2c5eda89e3fd30a2db3bcfcca","first_computed_at":"2026-05-18T00:48:26.344333Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:48:26.344333Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"p2L0qlA3WFmquukQMJKA1tViNTHU8pcZuW8CW+wqmK9twNW60EZs1yQuH618+w1yQ41lm61bfl4oJV71l3/JAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:48:26.344981Z","signed_message":"canonical_sha256_bytes"},"source_id":"1610.01469","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:95cffe7671e322a5666945d4c786ccd65b3e59e0c82fb47a4f3f10457cf7ab23","sha256:49f5e62cebe5df5b336f140956a3b215306ca69c4b34cfa9212cea5258e6036b"],"state_sha256":"fd0fc5061ca77bea419c8871e4d3c6c8b3cc2388bcd909b2e4dc8d8076d2f220"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zPdgfsNu/Nxv3RVE89peEb1IHSheRS/T/jtV34FyRAh0qxWA2cC/pM8nmWMQsWMzVplWN7SqqNVP8Rsa5v9rBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-29T05:01:42.274907Z","bundle_sha256":"882a79796e3c827b11dd64279dc0de2c067be8f27ae3528a04b52c60e111bd25"}}