{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:7KFSDBPFDNIT5ON46UHM3ST24H","short_pith_number":"pith:7KFSDBPF","schema_version":"1.0","canonical_sha256":"fa8b2185e51b513eb9bcf50ecdca7ae1e5c9f92f1a935ee8da597931d8409049","source":{"kind":"arxiv","id":"1008.0247","version":2},"attestation_state":"computed","paper":{"title":"B Physics (Experiment)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"Michal Kreps","submitted_at":"2010-08-02T07:56:30Z","abstract_excerpt":"In past few years the flavor physics made important transition from the work on confirmation the standard model of particle physics to the phase of search for effects of a new physics beyond standard model. In this paper we review current state of the physics of b-hadrons with emphasis on results with a sensitivity to new physics."},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1008.0247","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2010-08-02T07:56:30Z","cross_cats_sorted":[],"title_canon_sha256":"eb2d649d465ca9451b9b19c10acbd25fe313a0f5a7e1427924d92a9eb0c7d100","abstract_canon_sha256":"8a5b429a700a7026232e97f883bb6dcc8be300f7095fe526dcf1c65aab99ef47"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:42:14.437836Z","signature_b64":"s3zZiNR1/lvfzZ/O6vBFOUip4mFl0viiLJ0O5RUGVMgPtrqRZgfSaV+GzZvVnq11PGIldUcP43AIILhSt87sCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fa8b2185e51b513eb9bcf50ecdca7ae1e5c9f92f1a935ee8da597931d8409049","last_reissued_at":"2026-05-18T04:42:14.437393Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:42:14.437393Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"B Physics (Experiment)","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"Michal Kreps","submitted_at":"2010-08-02T07:56:30Z","abstract_excerpt":"In past few years the flavor physics made important transition from the work on confirmation the standard model of particle physics to the phase of search for effects of a new physics beyond standard model. In this paper we review current state of the physics of b-hadrons with emphasis on results with a sensitivity to new physics."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1008.0247","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1008.0247","created_at":"2026-05-18T04:42:14.437467+00:00"},{"alias_kind":"arxiv_version","alias_value":"1008.0247v2","created_at":"2026-05-18T04:42:14.437467+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1008.0247","created_at":"2026-05-18T04:42:14.437467+00:00"},{"alias_kind":"pith_short_12","alias_value":"7KFSDBPFDNIT","created_at":"2026-05-18T12:26:04.259169+00:00"},{"alias_kind":"pith_short_16","alias_value":"7KFSDBPFDNIT5ON4","created_at":"2026-05-18T12:26:04.259169+00:00"},{"alias_kind":"pith_short_8","alias_value":"7KFSDBPF","created_at":"2026-05-18T12:26:04.259169+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7KFSDBPFDNIT5ON46UHM3ST24H","json":"https://pith.science/pith/7KFSDBPFDNIT5ON46UHM3ST24H.json","graph_json":"https://pith.science/api/pith-number/7KFSDBPFDNIT5ON46UHM3ST24H/graph.json","events_json":"https://pith.science/api/pith-number/7KFSDBPFDNIT5ON46UHM3ST24H/events.json","paper":"https://pith.science/paper/7KFSDBPF"},"agent_actions":{"view_html":"https://pith.science/pith/7KFSDBPFDNIT5ON46UHM3ST24H","download_json":"https://pith.science/pith/7KFSDBPFDNIT5ON46UHM3ST24H.json","view_paper":"https://pith.science/paper/7KFSDBPF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1008.0247&json=true","fetch_graph":"https://pith.science/api/pith-number/7KFSDBPFDNIT5ON46UHM3ST24H/graph.json","fetch_events":"https://pith.science/api/pith-number/7KFSDBPFDNIT5ON46UHM3ST24H/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7KFSDBPFDNIT5ON46UHM3ST24H/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7KFSDBPFDNIT5ON46UHM3ST24H/action/storage_attestation","attest_author":"https://pith.science/pith/7KFSDBPFDNIT5ON46UHM3ST24H/action/author_attestation","sign_citation":"https://pith.science/pith/7KFSDBPFDNIT5ON46UHM3ST24H/action/citation_signature","submit_replication":"https://pith.science/pith/7KFSDBPFDNIT5ON46UHM3ST24H/action/replication_record"}},"created_at":"2026-05-18T04:42:14.437467+00:00","updated_at":"2026-05-18T04:42:14.437467+00:00"}