{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:23C3W4IU2YRJ5KAHYJV4EMPH2J","short_pith_number":"pith:23C3W4IU","schema_version":"1.0","canonical_sha256":"d6c5bb7114d6229ea807c26bc231e7d27b4aec1673390c9e55309d92d477daed","source":{"kind":"arxiv","id":"1509.08702","version":2},"attestation_state":"computed","paper":{"title":"The COHERENT Experiment at the Spallation Neutron Source","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"physics.ins-det","authors_text":"A. Bolozdynya, A. Burenkov, A. Etenko, A. Galindo-Uribarri, A.G. Dolgolenko, A. Khromov, A. Konovalov, A. Kovalenko, A. Kumpan, A. Shakirov, A. Sosnovtsev, A. Tolstukhin, B. Becker, B. Cabrera-Palmer, B. Scholz, B. Suh, C. Awe, C. Cuesta, C.H. Yu, C. Leadbetter, COHERENT Collaboration: D. Akimov, D. Dean, D. Hornback, D. Markoff, D. Parno, D. Radford, D. Reyna, D. Rimal, D. Rudik, E.B. Iverson, G.C. Rich, G. Perumpilly, H. Ray, J. Detwiler, J.I. Collar, J. Newby, J. Raybern, K. Miller, K. Scholberg, K. Vetter, L. Kaufman, L. Li, M. Green, M. Heath, M. Middlebrook, N. Fields, P. An, P. Barton, P. Mueller, P. Naumov, P.S. Barbeau, R.J. Cooper, R.L. Cooper, R. Tayloe, R.T. Thornton, S. Hedges, S. Penttila, S.R. Elliott, S.R. Klein, S. Suchyta, V. Belov, W. Fox, W. Lu, W.M. Snow, Y. Efremenko, Y. Melikyan","submitted_at":"2015-09-29T12:01:50Z","abstract_excerpt":"The COHERENT collaboration's primary objective is to measure coherent elastic neutrino-nucleus scattering (CEvNS) using the unique, high-quality source of tens-of-MeV neutrinos provided by the Spallation Neutron Source (SNS) at Oak Ridge National Laboratory (ORNL). In spite of its large cross section, the CEvNS process has never been observed, due to tiny energies of the resulting nuclear recoils which are out of reach for standard neutrino detectors. The measurement of CEvNS has now become feasible, thanks to the development of ultra-sensitive technology for rare decay and weakly-interacting "},"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":"1509.08702","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2015-09-29T12:01:50Z","cross_cats_sorted":["hep-ex","nucl-ex"],"title_canon_sha256":"1dfe069804061afc7cc749632bbc957e265af0345b60bfe62467583916ab7655","abstract_canon_sha256":"57b25909c8d89ee932102bc4d943032afda5aefbc461774925b6f1bd4bb9047c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:17:52.469879Z","signature_b64":"PvGA7AAQjNKAeGodZqB2sY6P7CxR9B95ZFAfsEcurBt9hZFE7V7/tuHb442m28R+D5XK+xmwioDlWmAB95vjCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d6c5bb7114d6229ea807c26bc231e7d27b4aec1673390c9e55309d92d477daed","last_reissued_at":"2026-05-18T01:17:52.469206Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:17:52.469206Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The COHERENT Experiment at the Spallation Neutron Source","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex"],"primary_cat":"physics.ins-det","authors_text":"A. Bolozdynya, A. Burenkov, A. Etenko, A. Galindo-Uribarri, A.G. Dolgolenko, A. Khromov, A. Konovalov, A. Kovalenko, A. Kumpan, A. Shakirov, A. Sosnovtsev, A. Tolstukhin, B. Becker, B. Cabrera-Palmer, B. Scholz, B. Suh, C. Awe, C. Cuesta, C.H. Yu, C. Leadbetter, COHERENT Collaboration: D. Akimov, D. Dean, D. Hornback, D. Markoff, D. Parno, D. Radford, D. Reyna, D. Rimal, D. Rudik, E.B. Iverson, G.C. Rich, G. Perumpilly, H. Ray, J. Detwiler, J.I. Collar, J. Newby, J. Raybern, K. Miller, K. Scholberg, K. Vetter, L. Kaufman, L. Li, M. Green, M. Heath, M. Middlebrook, N. Fields, P. An, P. Barton, P. Mueller, P. Naumov, P.S. Barbeau, R.J. Cooper, R.L. Cooper, R. Tayloe, R.T. Thornton, S. Hedges, S. Penttila, S.R. Elliott, S.R. Klein, S. Suchyta, V. Belov, W. Fox, W. Lu, W.M. Snow, Y. Efremenko, Y. Melikyan","submitted_at":"2015-09-29T12:01:50Z","abstract_excerpt":"The COHERENT collaboration's primary objective is to measure coherent elastic neutrino-nucleus scattering (CEvNS) using the unique, high-quality source of tens-of-MeV neutrinos provided by the Spallation Neutron Source (SNS) at Oak Ridge National Laboratory (ORNL). In spite of its large cross section, the CEvNS process has never been observed, due to tiny energies of the resulting nuclear recoils which are out of reach for standard neutrino detectors. The measurement of CEvNS has now become feasible, thanks to the development of ultra-sensitive technology for rare decay and weakly-interacting "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.08702","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":"1509.08702","created_at":"2026-05-18T01:17:52.469306+00:00"},{"alias_kind":"arxiv_version","alias_value":"1509.08702v2","created_at":"2026-05-18T01:17:52.469306+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.08702","created_at":"2026-05-18T01:17:52.469306+00:00"},{"alias_kind":"pith_short_12","alias_value":"23C3W4IU2YRJ","created_at":"2026-05-18T12:28:59.999130+00:00"},{"alias_kind":"pith_short_16","alias_value":"23C3W4IU2YRJ5KAH","created_at":"2026-05-18T12:28:59.999130+00:00"},{"alias_kind":"pith_short_8","alias_value":"23C3W4IU","created_at":"2026-05-18T12:28:59.999130+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.15214","citing_title":"Neutral-current neutrino-nucleus scattering off I (127) and Cs (133): Coherent and incoherent contributions with electroweak refinements for odd-A nuclei","ref_index":2,"is_internal_anchor":true},{"citing_arxiv_id":"2605.04393","citing_title":"Medium Characterization with Hard Probes: From Cherenkov Light in QED to Jet Drift in QCD","ref_index":18,"is_internal_anchor":true},{"citing_arxiv_id":"2605.04393","citing_title":"Medium Characterization with Hard Probes: From Cherenkov Light in QED to Jet Drift in QCD","ref_index":18,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/23C3W4IU2YRJ5KAHYJV4EMPH2J","json":"https://pith.science/pith/23C3W4IU2YRJ5KAHYJV4EMPH2J.json","graph_json":"https://pith.science/api/pith-number/23C3W4IU2YRJ5KAHYJV4EMPH2J/graph.json","events_json":"https://pith.science/api/pith-number/23C3W4IU2YRJ5KAHYJV4EMPH2J/events.json","paper":"https://pith.science/paper/23C3W4IU"},"agent_actions":{"view_html":"https://pith.science/pith/23C3W4IU2YRJ5KAHYJV4EMPH2J","download_json":"https://pith.science/pith/23C3W4IU2YRJ5KAHYJV4EMPH2J.json","view_paper":"https://pith.science/paper/23C3W4IU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1509.08702&json=true","fetch_graph":"https://pith.science/api/pith-number/23C3W4IU2YRJ5KAHYJV4EMPH2J/graph.json","fetch_events":"https://pith.science/api/pith-number/23C3W4IU2YRJ5KAHYJV4EMPH2J/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/23C3W4IU2YRJ5KAHYJV4EMPH2J/action/timestamp_anchor","attest_storage":"https://pith.science/pith/23C3W4IU2YRJ5KAHYJV4EMPH2J/action/storage_attestation","attest_author":"https://pith.science/pith/23C3W4IU2YRJ5KAHYJV4EMPH2J/action/author_attestation","sign_citation":"https://pith.science/pith/23C3W4IU2YRJ5KAHYJV4EMPH2J/action/citation_signature","submit_replication":"https://pith.science/pith/23C3W4IU2YRJ5KAHYJV4EMPH2J/action/replication_record"}},"created_at":"2026-05-18T01:17:52.469306+00:00","updated_at":"2026-05-18T01:17:52.469306+00:00"}