{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:5PPD4PPZ7ZJWBK36SAHUO25QR2","short_pith_number":"pith:5PPD4PPZ","canonical_record":{"source":{"id":"1602.05322","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-02-17T07:08:11Z","cross_cats_sorted":[],"title_canon_sha256":"075c01274fcd02ed4d70d6d95f3d1f97d9de2ce46d7040e470c5ae0f5890d3b6","abstract_canon_sha256":"eac0f5872dd5d5bcfb5ca4643de8a7006097012250c9a8a65b9686c16b7406a2"},"schema_version":"1.0"},"canonical_sha256":"ebde3e3df9fe5360ab7e900f476bb08eb92a740bbd1edd08e9c100a2a24fcdda","source":{"kind":"arxiv","id":"1602.05322","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.05322","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"arxiv_version","alias_value":"1602.05322v1","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.05322","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"pith_short_12","alias_value":"5PPD4PPZ7ZJW","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"5PPD4PPZ7ZJWBK36","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"5PPD4PPZ","created_at":"2026-05-18T12:30:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:5PPD4PPZ7ZJWBK36SAHUO25QR2","target":"record","payload":{"canonical_record":{"source":{"id":"1602.05322","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-02-17T07:08:11Z","cross_cats_sorted":[],"title_canon_sha256":"075c01274fcd02ed4d70d6d95f3d1f97d9de2ce46d7040e470c5ae0f5890d3b6","abstract_canon_sha256":"eac0f5872dd5d5bcfb5ca4643de8a7006097012250c9a8a65b9686c16b7406a2"},"schema_version":"1.0"},"canonical_sha256":"ebde3e3df9fe5360ab7e900f476bb08eb92a740bbd1edd08e9c100a2a24fcdda","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:02:04.505187Z","signature_b64":"thdLTg9wMw93hE/2iAnaZI8SDPb94Bt87gFPBQFaRmS7n7rZP6j1V6E88geuFmR/dA4JyT0nGPm2rk95gRsRCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ebde3e3df9fe5360ab7e900f476bb08eb92a740bbd1edd08e9c100a2a24fcdda","last_reissued_at":"2026-05-18T01:02:04.504581Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:02:04.504581Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1602.05322","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":"2026-05-18T01:02:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bQJEVlT8sWg76CPeafvbwBr+JipmV98O5OJw6OdO8NdarNF9cdj6LBiXglHjihdBeVRMuOpvN/IBPjMJ+GaQAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:24:47.678414Z"},"content_sha256":"f2615ace7ccbad2d58209c16b8217c001b759c3e74970f2d8993a15b34ae5b2c","schema_version":"1.0","event_id":"sha256:f2615ace7ccbad2d58209c16b8217c001b759c3e74970f2d8993a15b34ae5b2c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:5PPD4PPZ7ZJWBK36SAHUO25QR2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Hadron energy spectrum in polarized top quark decays considering the effects of hadron and bottom quark masses","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Mahboobe Balali, S. Mohammad Moosavi Nejad","submitted_at":"2016-02-17T07:08:11Z","abstract_excerpt":"We present the analytical expressions for the next-to-leading order corrections to the partial decay width $t(\\uparrow) \\rightarrow bW^+$, followed by $b\\rightarrow H_bX$, for nonzero b-quark mass ($m_b\\neq 0$) in the fixed-flavor-number scheme (FFNs). To make the predictions for the energy distribution of outgoing hadrons $H_b$, as a function of the normalized $H_b$-energy fraction $x_H$, we apply the general-mass variable-flavor-number scheme (GM-VFNs) in a specific helicity coordinate system where the polarization of top quark is evaluated relative to the b-quark momentum. We also study the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.05322","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":""},"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":"2026-05-18T01:02:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rgXnk5JiIMm/ux6cdB8jmDYzvzHGkfcdASNejXx5D8C5jQ1nQm7mNL86H4yW5Zm8XVQ4gVbt6q1/MHY1F9teBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:24:47.679064Z"},"content_sha256":"821e2cfd98ea588e22b7fb6ce20a4cf884125e7095fce58fc5cbad7b9ce0ca1b","schema_version":"1.0","event_id":"sha256:821e2cfd98ea588e22b7fb6ce20a4cf884125e7095fce58fc5cbad7b9ce0ca1b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5PPD4PPZ7ZJWBK36SAHUO25QR2/bundle.json","state_url":"https://pith.science/pith/5PPD4PPZ7ZJWBK36SAHUO25QR2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5PPD4PPZ7ZJWBK36SAHUO25QR2/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":"2026-05-25T21:24:47Z","links":{"resolver":"https://pith.science/pith/5PPD4PPZ7ZJWBK36SAHUO25QR2","bundle":"https://pith.science/pith/5PPD4PPZ7ZJWBK36SAHUO25QR2/bundle.json","state":"https://pith.science/pith/5PPD4PPZ7ZJWBK36SAHUO25QR2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5PPD4PPZ7ZJWBK36SAHUO25QR2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:5PPD4PPZ7ZJWBK36SAHUO25QR2","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":"eac0f5872dd5d5bcfb5ca4643de8a7006097012250c9a8a65b9686c16b7406a2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-02-17T07:08:11Z","title_canon_sha256":"075c01274fcd02ed4d70d6d95f3d1f97d9de2ce46d7040e470c5ae0f5890d3b6"},"schema_version":"1.0","source":{"id":"1602.05322","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.05322","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"arxiv_version","alias_value":"1602.05322v1","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.05322","created_at":"2026-05-18T01:02:04Z"},{"alias_kind":"pith_short_12","alias_value":"5PPD4PPZ7ZJW","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_16","alias_value":"5PPD4PPZ7ZJWBK36","created_at":"2026-05-18T12:30:01Z"},{"alias_kind":"pith_short_8","alias_value":"5PPD4PPZ","created_at":"2026-05-18T12:30:01Z"}],"graph_snapshots":[{"event_id":"sha256:821e2cfd98ea588e22b7fb6ce20a4cf884125e7095fce58fc5cbad7b9ce0ca1b","target":"graph","created_at":"2026-05-18T01:02:04Z","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 the analytical expressions for the next-to-leading order corrections to the partial decay width $t(\\uparrow) \\rightarrow bW^+$, followed by $b\\rightarrow H_bX$, for nonzero b-quark mass ($m_b\\neq 0$) in the fixed-flavor-number scheme (FFNs). To make the predictions for the energy distribution of outgoing hadrons $H_b$, as a function of the normalized $H_b$-energy fraction $x_H$, we apply the general-mass variable-flavor-number scheme (GM-VFNs) in a specific helicity coordinate system where the polarization of top quark is evaluated relative to the b-quark momentum. We also study the","authors_text":"Mahboobe Balali, S. Mohammad Moosavi Nejad","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-02-17T07:08:11Z","title":"Hadron energy spectrum in polarized top quark decays considering the effects of hadron and bottom quark masses"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.05322","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:f2615ace7ccbad2d58209c16b8217c001b759c3e74970f2d8993a15b34ae5b2c","target":"record","created_at":"2026-05-18T01:02:04Z","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":"eac0f5872dd5d5bcfb5ca4643de8a7006097012250c9a8a65b9686c16b7406a2","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-02-17T07:08:11Z","title_canon_sha256":"075c01274fcd02ed4d70d6d95f3d1f97d9de2ce46d7040e470c5ae0f5890d3b6"},"schema_version":"1.0","source":{"id":"1602.05322","kind":"arxiv","version":1}},"canonical_sha256":"ebde3e3df9fe5360ab7e900f476bb08eb92a740bbd1edd08e9c100a2a24fcdda","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ebde3e3df9fe5360ab7e900f476bb08eb92a740bbd1edd08e9c100a2a24fcdda","first_computed_at":"2026-05-18T01:02:04.504581Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:02:04.504581Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"thdLTg9wMw93hE/2iAnaZI8SDPb94Bt87gFPBQFaRmS7n7rZP6j1V6E88geuFmR/dA4JyT0nGPm2rk95gRsRCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:02:04.505187Z","signed_message":"canonical_sha256_bytes"},"source_id":"1602.05322","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f2615ace7ccbad2d58209c16b8217c001b759c3e74970f2d8993a15b34ae5b2c","sha256:821e2cfd98ea588e22b7fb6ce20a4cf884125e7095fce58fc5cbad7b9ce0ca1b"],"state_sha256":"019d0fe0232eb95eeabc6d592fb2c4bf7167c77677855c09db0066513ebc414d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RC06s3YDV3GWgEZSlvPQzjxK3ExtCxK6yMUMbIykVTa9u+EAZlsKSddXJcdovxQBSnl+fiMhoxLRNuJzbsJZDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T21:24:47.682539Z","bundle_sha256":"d8326b4302b7f0d4f6ea5f428ae8ff06f0d5969c9c4409a687074adb7382a6ad"}}