{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:GJ2JTUTDAW5ULJXZPQ4V75WQ2O","short_pith_number":"pith:GJ2JTUTD","schema_version":"1.0","canonical_sha256":"327499d26305bb45a6f97c395ff6d0d39b2912e7de09b80d2799e47c57369095","source":{"kind":"arxiv","id":"1402.4125","version":1},"attestation_state":"computed","paper":{"title":"High statistics study of the reaction $\\gamma p\\to p\\pi^0\\eta$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"E. Gutz, The CBELSA/TAPS Collaboration","submitted_at":"2014-02-17T09:43:32Z","abstract_excerpt":"Photoproduction off protons of the $p\\pi^0\\eta$ three-body final state was studied with the Crystal Barrel/TAPS detector at the electron stretcher accelerator ELSA at Bonn for incident energies from the $\\pi^0\\eta$ production threshold up to 2.5\\,GeV. Differential cross sections and the total cross section are presented. The use of linearly polarized photons gives access to the polarization observables $\\Sigma$, $I^{s}$ and $I^{c}$, the latter two characterize beam asymmetries in case of three-body final states. $\\Delta(1232)\\eta$, $N(1535){1/2^-}\\pi$, and $p a_0(980)$ are the dominant isobars"},"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":"1402.4125","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2014-02-17T09:43:32Z","cross_cats_sorted":[],"title_canon_sha256":"9d24bb756373d90c67dd3bf47fc8d7a2df812c10416f9efc83f3cf022860ed38","abstract_canon_sha256":"25aed6f8d121906624426df15c878e08ed5a70ec43c67afccc19664b13338e6f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:10:00.253412Z","signature_b64":"i8xzp8Y3hnbJSzZ1tW4UaXHYSve59FdK5HNPnFr6suBn6CN2OKz5i5uMDgCkM4mxVJyP+TqiHDSNrFrvr+sIAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"327499d26305bb45a6f97c395ff6d0d39b2912e7de09b80d2799e47c57369095","last_reissued_at":"2026-05-18T01:10:00.252887Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:10:00.252887Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"High statistics study of the reaction $\\gamma p\\to p\\pi^0\\eta$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"E. Gutz, The CBELSA/TAPS Collaboration","submitted_at":"2014-02-17T09:43:32Z","abstract_excerpt":"Photoproduction off protons of the $p\\pi^0\\eta$ three-body final state was studied with the Crystal Barrel/TAPS detector at the electron stretcher accelerator ELSA at Bonn for incident energies from the $\\pi^0\\eta$ production threshold up to 2.5\\,GeV. Differential cross sections and the total cross section are presented. The use of linearly polarized photons gives access to the polarization observables $\\Sigma$, $I^{s}$ and $I^{c}$, the latter two characterize beam asymmetries in case of three-body final states. $\\Delta(1232)\\eta$, $N(1535){1/2^-}\\pi$, and $p a_0(980)$ are the dominant isobars"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.4125","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":"1402.4125","created_at":"2026-05-18T01:10:00.252971+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.4125v1","created_at":"2026-05-18T01:10:00.252971+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.4125","created_at":"2026-05-18T01:10:00.252971+00:00"},{"alias_kind":"pith_short_12","alias_value":"GJ2JTUTDAW5U","created_at":"2026-05-18T12:28:30.664211+00:00"},{"alias_kind":"pith_short_16","alias_value":"GJ2JTUTDAW5ULJXZ","created_at":"2026-05-18T12:28:30.664211+00:00"},{"alias_kind":"pith_short_8","alias_value":"GJ2JTUTD","created_at":"2026-05-18T12:28:30.664211+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.31503","citing_title":"The Large-Scale Structure of the Universe through the SKA lenses","ref_index":49,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GJ2JTUTDAW5ULJXZPQ4V75WQ2O","json":"https://pith.science/pith/GJ2JTUTDAW5ULJXZPQ4V75WQ2O.json","graph_json":"https://pith.science/api/pith-number/GJ2JTUTDAW5ULJXZPQ4V75WQ2O/graph.json","events_json":"https://pith.science/api/pith-number/GJ2JTUTDAW5ULJXZPQ4V75WQ2O/events.json","paper":"https://pith.science/paper/GJ2JTUTD"},"agent_actions":{"view_html":"https://pith.science/pith/GJ2JTUTDAW5ULJXZPQ4V75WQ2O","download_json":"https://pith.science/pith/GJ2JTUTDAW5ULJXZPQ4V75WQ2O.json","view_paper":"https://pith.science/paper/GJ2JTUTD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.4125&json=true","fetch_graph":"https://pith.science/api/pith-number/GJ2JTUTDAW5ULJXZPQ4V75WQ2O/graph.json","fetch_events":"https://pith.science/api/pith-number/GJ2JTUTDAW5ULJXZPQ4V75WQ2O/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GJ2JTUTDAW5ULJXZPQ4V75WQ2O/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GJ2JTUTDAW5ULJXZPQ4V75WQ2O/action/storage_attestation","attest_author":"https://pith.science/pith/GJ2JTUTDAW5ULJXZPQ4V75WQ2O/action/author_attestation","sign_citation":"https://pith.science/pith/GJ2JTUTDAW5ULJXZPQ4V75WQ2O/action/citation_signature","submit_replication":"https://pith.science/pith/GJ2JTUTDAW5ULJXZPQ4V75WQ2O/action/replication_record"}},"created_at":"2026-05-18T01:10:00.252971+00:00","updated_at":"2026-05-18T01:10:00.252971+00:00"}