{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:FCX6SXIJ2DFUPR4H5TOZ3TN3EI","short_pith_number":"pith:FCX6SXIJ","schema_version":"1.0","canonical_sha256":"28afe95d09d0cb47c787ecdd9dcdbb2222b5145043f3250f15f1fa929807e490","source":{"kind":"arxiv","id":"1601.04137","version":1},"attestation_state":"computed","paper":{"title":"Insight into $f_0(980)$ through the $B_{(s)}$ charmed decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Si-Yang Wang, Xing-Ke Ma, Zhi-Qing Zhang","submitted_at":"2016-01-16T08:52:21Z","abstract_excerpt":"Through analyzing the $B_{(s)}$ charmed decays $B^{0}\\to \\bar D_{0}f_0(980)$ and $B_{s}\\to \\bar D_{0}f_0(980)$ within the framework of the PQCD factorization approach and comparing with the current data, we find that there are two possible regions for the $f_0(980)-f_0(500)$ mixing angle $\\theta$: one is centered at $34^\\circ\\sim38^\\circ$ and the other is falls into $142^\\circ\\sim154^\\circ$. The former can overlap mostly with one of allowed angle regions extracted from the decay $B^{0}\\to \\bar D_{0}f_0(500)$. The branching fractions of $B_s$ decay modes are less sensitive to the mixing angle c"},"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":"1601.04137","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-01-16T08:52:21Z","cross_cats_sorted":[],"title_canon_sha256":"345bbbbfebc68b3324a9c0bf34de2f05f86e54dd622b99b325427a026144d63e","abstract_canon_sha256":"39267bb800ead0ce0a0931ff24d7683cb86b451a4ad564e03579fffafbb24a7e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:08.404598Z","signature_b64":"7r/UOoaqsCSvwhR81cd7DSaA9Cao1Kk8kDMR0Cy1+408wYrffRGVAAV63qCv+eb5b77vw/T+c0DzircmJGWFAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"28afe95d09d0cb47c787ecdd9dcdbb2222b5145043f3250f15f1fa929807e490","last_reissued_at":"2026-05-18T01:18:08.403829Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:08.403829Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Insight into $f_0(980)$ through the $B_{(s)}$ charmed decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Si-Yang Wang, Xing-Ke Ma, Zhi-Qing Zhang","submitted_at":"2016-01-16T08:52:21Z","abstract_excerpt":"Through analyzing the $B_{(s)}$ charmed decays $B^{0}\\to \\bar D_{0}f_0(980)$ and $B_{s}\\to \\bar D_{0}f_0(980)$ within the framework of the PQCD factorization approach and comparing with the current data, we find that there are two possible regions for the $f_0(980)-f_0(500)$ mixing angle $\\theta$: one is centered at $34^\\circ\\sim38^\\circ$ and the other is falls into $142^\\circ\\sim154^\\circ$. The former can overlap mostly with one of allowed angle regions extracted from the decay $B^{0}\\to \\bar D_{0}f_0(500)$. The branching fractions of $B_s$ decay modes are less sensitive to the mixing angle c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1601.04137","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1601.04137","created_at":"2026-05-18T01:18:08.403946+00:00"},{"alias_kind":"arxiv_version","alias_value":"1601.04137v1","created_at":"2026-05-18T01:18:08.403946+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1601.04137","created_at":"2026-05-18T01:18:08.403946+00:00"},{"alias_kind":"pith_short_12","alias_value":"FCX6SXIJ2DFU","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_16","alias_value":"FCX6SXIJ2DFUPR4H","created_at":"2026-05-18T12:30:15.759754+00:00"},{"alias_kind":"pith_short_8","alias_value":"FCX6SXIJ","created_at":"2026-05-18T12:30:15.759754+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2502.04191","citing_title":"Systematic Analysis of $B_s \\to SP$ Decays in Perturbative QCD Approach","ref_index":31,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FCX6SXIJ2DFUPR4H5TOZ3TN3EI","json":"https://pith.science/pith/FCX6SXIJ2DFUPR4H5TOZ3TN3EI.json","graph_json":"https://pith.science/api/pith-number/FCX6SXIJ2DFUPR4H5TOZ3TN3EI/graph.json","events_json":"https://pith.science/api/pith-number/FCX6SXIJ2DFUPR4H5TOZ3TN3EI/events.json","paper":"https://pith.science/paper/FCX6SXIJ"},"agent_actions":{"view_html":"https://pith.science/pith/FCX6SXIJ2DFUPR4H5TOZ3TN3EI","download_json":"https://pith.science/pith/FCX6SXIJ2DFUPR4H5TOZ3TN3EI.json","view_paper":"https://pith.science/paper/FCX6SXIJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1601.04137&json=true","fetch_graph":"https://pith.science/api/pith-number/FCX6SXIJ2DFUPR4H5TOZ3TN3EI/graph.json","fetch_events":"https://pith.science/api/pith-number/FCX6SXIJ2DFUPR4H5TOZ3TN3EI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FCX6SXIJ2DFUPR4H5TOZ3TN3EI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FCX6SXIJ2DFUPR4H5TOZ3TN3EI/action/storage_attestation","attest_author":"https://pith.science/pith/FCX6SXIJ2DFUPR4H5TOZ3TN3EI/action/author_attestation","sign_citation":"https://pith.science/pith/FCX6SXIJ2DFUPR4H5TOZ3TN3EI/action/citation_signature","submit_replication":"https://pith.science/pith/FCX6SXIJ2DFUPR4H5TOZ3TN3EI/action/replication_record"}},"created_at":"2026-05-18T01:18:08.403946+00:00","updated_at":"2026-05-18T01:18:08.403946+00:00"}