{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:E762PLI5OKEWOK62JEFOJQWEUJ","short_pith_number":"pith:E762PLI5","schema_version":"1.0","canonical_sha256":"27fda7ad1d7289672bda490ae4c2c4a26d96f53217afad47caeed32e80778b62","source":{"kind":"arxiv","id":"1710.02730","version":3},"attestation_state":"computed","paper":{"title":"Average CsI neutron density distribution from COHERENT data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"C. Giunti, M. Cadeddu, Y.F. Li, Y.Y. Zhang","submitted_at":"2017-10-07T19:35:05Z","abstract_excerpt":"Using the coherent elastic neutrino-nucleus scattering data of the COHERENT experiment, we determine for the first time the average neutron rms radius of $^{133}\\text{Cs}$ and $^{127}\\text{I}$. We obtain the practically model-independent value $ R_{n} = 5.5 {}^{+0.9}_{-1.1} \\, \\text{fm} $ using the symmetrized Fermi and Helm form factors. We also point out that the COHERENT data show a $2.3\\sigma$ evidence of the nuclear structure suppression of the full coherence."},"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":"1710.02730","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-10-07T19:35:05Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"2adcf3724c4871b09ad5a19d1e089116c9fe1da5c7c4913985cdb85858bcaf35","abstract_canon_sha256":"0b1c49895d1c23c004e849ac8030664f0d490895e0e7931506cd557bc939a5ce"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:22:58.425780Z","signature_b64":"oRUwSS/wOd4++Vp9BCxDI1FkeI9ZGSwP6QrEc9SUV1r9PfWO33g9UqvZvoIjdTY22CQqPambiZvUYs2Q/l21Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"27fda7ad1d7289672bda490ae4c2c4a26d96f53217afad47caeed32e80778b62","last_reissued_at":"2026-05-18T00:22:58.425278Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:22:58.425278Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Average CsI neutron density distribution from COHERENT data","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"C. Giunti, M. Cadeddu, Y.F. Li, Y.Y. Zhang","submitted_at":"2017-10-07T19:35:05Z","abstract_excerpt":"Using the coherent elastic neutrino-nucleus scattering data of the COHERENT experiment, we determine for the first time the average neutron rms radius of $^{133}\\text{Cs}$ and $^{127}\\text{I}$. We obtain the practically model-independent value $ R_{n} = 5.5 {}^{+0.9}_{-1.1} \\, \\text{fm} $ using the symmetrized Fermi and Helm form factors. We also point out that the COHERENT data show a $2.3\\sigma$ evidence of the nuclear structure suppression of the full coherence."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.02730","kind":"arxiv","version":3},"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":"1710.02730","created_at":"2026-05-18T00:22:58.425381+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.02730v3","created_at":"2026-05-18T00:22:58.425381+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.02730","created_at":"2026-05-18T00:22:58.425381+00:00"},{"alias_kind":"pith_short_12","alias_value":"E762PLI5OKEW","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_16","alias_value":"E762PLI5OKEWOK62","created_at":"2026-05-18T12:31:12.930513+00:00"},{"alias_kind":"pith_short_8","alias_value":"E762PLI5","created_at":"2026-05-18T12:31:12.930513+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.07975","citing_title":"Phenomenological implications of the high-precision COHERENT germanium CE$\\nu$NS data","ref_index":37,"is_internal_anchor":true},{"citing_arxiv_id":"2512.19788","citing_title":"Coherent Elastic Neutrino-Nucleus Scattering at the Japan Proton Accelerator Research Complex","ref_index":56,"is_internal_anchor":true},{"citing_arxiv_id":"2605.07975","citing_title":"Phenomenological implications of the high-precision COHERENT germanium CE$\\nu$NS data","ref_index":36,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/E762PLI5OKEWOK62JEFOJQWEUJ","json":"https://pith.science/pith/E762PLI5OKEWOK62JEFOJQWEUJ.json","graph_json":"https://pith.science/api/pith-number/E762PLI5OKEWOK62JEFOJQWEUJ/graph.json","events_json":"https://pith.science/api/pith-number/E762PLI5OKEWOK62JEFOJQWEUJ/events.json","paper":"https://pith.science/paper/E762PLI5"},"agent_actions":{"view_html":"https://pith.science/pith/E762PLI5OKEWOK62JEFOJQWEUJ","download_json":"https://pith.science/pith/E762PLI5OKEWOK62JEFOJQWEUJ.json","view_paper":"https://pith.science/paper/E762PLI5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.02730&json=true","fetch_graph":"https://pith.science/api/pith-number/E762PLI5OKEWOK62JEFOJQWEUJ/graph.json","fetch_events":"https://pith.science/api/pith-number/E762PLI5OKEWOK62JEFOJQWEUJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/E762PLI5OKEWOK62JEFOJQWEUJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/E762PLI5OKEWOK62JEFOJQWEUJ/action/storage_attestation","attest_author":"https://pith.science/pith/E762PLI5OKEWOK62JEFOJQWEUJ/action/author_attestation","sign_citation":"https://pith.science/pith/E762PLI5OKEWOK62JEFOJQWEUJ/action/citation_signature","submit_replication":"https://pith.science/pith/E762PLI5OKEWOK62JEFOJQWEUJ/action/replication_record"}},"created_at":"2026-05-18T00:22:58.425381+00:00","updated_at":"2026-05-18T00:22:58.425381+00:00"}