{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:WORALFOHC66L5OPLJLHLPFLZM6","short_pith_number":"pith:WORALFOH","schema_version":"1.0","canonical_sha256":"b3a20595c717bcbeb9eb4aceb79579678a734f5f491e76e10e408efc3c82b18e","source":{"kind":"arxiv","id":"1604.05704","version":1},"attestation_state":"computed","paper":{"title":"The Impact of New Polarization Data from Bonn, Mainz and Jefferson Laboratory on $\\gamma p \\to \\pi N$ Multipoles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Sarantsev, A. Thiel, A.V. Anisovich R. Beck, D. R\\\"onchen, E. Klempt, I. Strakovsky, J. Hartmann, L. Tiator, M. D\\\"oring, M. Gottschall, M. Ostrick, R. Workman, Ulf-G. Mei{\\ss}ner, U. Thoma, V. Kashevarov, V. Nikonov, Y. Wunderlich","submitted_at":"2016-04-19T19:41:04Z","abstract_excerpt":"New data on pion-photoproduction off the proton have been included in the partial wave analyses Bonn-Gatchina and SAID and in the dynamical coupled-channel approach J\\\"ulich-Bonn. All reproduce the recent new data well: the double polarization data for E, G, H, P and T in $\\gamma p \\to \\pi^0 p$ from ELSA, the beam asymmetry $\\Sigma$ for $\\gamma p \\to \\pi^0 p$ and $\\pi^+ n$ from Jefferson Laboratory, and the precise new differential cross section and beam asymmetry data $\\Sigma$ for $\\gamma p \\to \\pi^0 p$ from MAMI. The new fit results for the multipoles are compared with predictions not taking"},"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":"1604.05704","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-04-19T19:41:04Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"f424c460dab0270ad8e68d051969a65fd836e0d223dcad0ab68283966e00bf97","abstract_canon_sha256":"15b12c04f200d91202e7bba715b7464cbb81cce386e6224ae60244907edd22e0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:16:37.933612Z","signature_b64":"iWqltya5lO0g2zoZwY4rEmcnWudEy/iPUTrIyVEVsAnXZgOSDBJp23JoVaWYgp+zXf7CYR5S+te+HlSlLgcUBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b3a20595c717bcbeb9eb4aceb79579678a734f5f491e76e10e408efc3c82b18e","last_reissued_at":"2026-05-18T01:16:37.932941Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:16:37.932941Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Impact of New Polarization Data from Bonn, Mainz and Jefferson Laboratory on $\\gamma p \\to \\pi N$ Multipoles","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"A. Sarantsev, A. Thiel, A.V. Anisovich R. Beck, D. R\\\"onchen, E. Klempt, I. Strakovsky, J. Hartmann, L. Tiator, M. D\\\"oring, M. Gottschall, M. Ostrick, R. Workman, Ulf-G. Mei{\\ss}ner, U. Thoma, V. Kashevarov, V. Nikonov, Y. Wunderlich","submitted_at":"2016-04-19T19:41:04Z","abstract_excerpt":"New data on pion-photoproduction off the proton have been included in the partial wave analyses Bonn-Gatchina and SAID and in the dynamical coupled-channel approach J\\\"ulich-Bonn. All reproduce the recent new data well: the double polarization data for E, G, H, P and T in $\\gamma p \\to \\pi^0 p$ from ELSA, the beam asymmetry $\\Sigma$ for $\\gamma p \\to \\pi^0 p$ and $\\pi^+ n$ from Jefferson Laboratory, and the precise new differential cross section and beam asymmetry data $\\Sigma$ for $\\gamma p \\to \\pi^0 p$ from MAMI. The new fit results for the multipoles are compared with predictions not taking"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.05704","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":"1604.05704","created_at":"2026-05-18T01:16:37.933048+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.05704v1","created_at":"2026-05-18T01:16:37.933048+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.05704","created_at":"2026-05-18T01:16:37.933048+00:00"},{"alias_kind":"pith_short_12","alias_value":"WORALFOHC66L","created_at":"2026-05-18T12:30:51.357362+00:00"},{"alias_kind":"pith_short_16","alias_value":"WORALFOHC66L5OPL","created_at":"2026-05-18T12:30:51.357362+00:00"},{"alias_kind":"pith_short_8","alias_value":"WORALFOH","created_at":"2026-05-18T12:30:51.357362+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/WORALFOHC66L5OPLJLHLPFLZM6","json":"https://pith.science/pith/WORALFOHC66L5OPLJLHLPFLZM6.json","graph_json":"https://pith.science/api/pith-number/WORALFOHC66L5OPLJLHLPFLZM6/graph.json","events_json":"https://pith.science/api/pith-number/WORALFOHC66L5OPLJLHLPFLZM6/events.json","paper":"https://pith.science/paper/WORALFOH"},"agent_actions":{"view_html":"https://pith.science/pith/WORALFOHC66L5OPLJLHLPFLZM6","download_json":"https://pith.science/pith/WORALFOHC66L5OPLJLHLPFLZM6.json","view_paper":"https://pith.science/paper/WORALFOH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.05704&json=true","fetch_graph":"https://pith.science/api/pith-number/WORALFOHC66L5OPLJLHLPFLZM6/graph.json","fetch_events":"https://pith.science/api/pith-number/WORALFOHC66L5OPLJLHLPFLZM6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WORALFOHC66L5OPLJLHLPFLZM6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WORALFOHC66L5OPLJLHLPFLZM6/action/storage_attestation","attest_author":"https://pith.science/pith/WORALFOHC66L5OPLJLHLPFLZM6/action/author_attestation","sign_citation":"https://pith.science/pith/WORALFOHC66L5OPLJLHLPFLZM6/action/citation_signature","submit_replication":"https://pith.science/pith/WORALFOHC66L5OPLJLHLPFLZM6/action/replication_record"}},"created_at":"2026-05-18T01:16:37.933048+00:00","updated_at":"2026-05-18T01:16:37.933048+00:00"}