{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:CN524Q3WNUW6756GLHGWDJZ7CC","short_pith_number":"pith:CN524Q3W","schema_version":"1.0","canonical_sha256":"137bae43766d2deff7c659cd61a73f10a7bccb6596a4051798dcbfb8a9c3f902","source":{"kind":"arxiv","id":"2504.06692","version":1},"attestation_state":"computed","paper":{"title":"SHiP experiment at the SPS Beam Dump Facility","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-ex","authors_text":"HI-ECN3 Project Team, SHiP Collaboration","submitted_at":"2025-04-09T08:53:20Z","abstract_excerpt":"In 2024, the SHiP experiment, together with the associated Beam Dump Facility (BDF) under the auspices of the High Intensity ECN3 (HI-ECN3) project, was selected for the future physics exploitation of the ECN3 experimental facility at the SPS. The SHiP experiment is a general-purpose intensity-frontier setup designed to search for physics beyond the Standard Model in the domain of Feebly Interacting Particles at the GeV-scale. It comprises a multi-system apparatus that provides discovery sensitivity to both decay and scattering signatures of models with feebly interacting particles, such as da"},"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":"2504.06692","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2025-04-09T08:53:20Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"3a4dfaa7f24c89416c8ceeca34d2414be51c0b1050735b8a92dbf922cd4f4ab8","abstract_canon_sha256":"12691b4091a18e8f894e7d3a848ea58d983afc6087e321719cd474d7c2f151b7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T10:46:44.212460Z","signature_b64":"cMH8Q8ZEqSEj+azSbXM0dA2vr2nSDx/osjfyTrz0AE8HqJ7BpOy8ZKTVyUztfgags4yTEyGqAzennBs6FBo6Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"137bae43766d2deff7c659cd61a73f10a7bccb6596a4051798dcbfb8a9c3f902","last_reissued_at":"2026-07-05T10:46:44.211968Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T10:46:44.211968Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"SHiP experiment at the SPS Beam Dump Facility","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-ex","authors_text":"HI-ECN3 Project Team, SHiP Collaboration","submitted_at":"2025-04-09T08:53:20Z","abstract_excerpt":"In 2024, the SHiP experiment, together with the associated Beam Dump Facility (BDF) under the auspices of the High Intensity ECN3 (HI-ECN3) project, was selected for the future physics exploitation of the ECN3 experimental facility at the SPS. The SHiP experiment is a general-purpose intensity-frontier setup designed to search for physics beyond the Standard Model in the domain of Feebly Interacting Particles at the GeV-scale. It comprises a multi-system apparatus that provides discovery sensitivity to both decay and scattering signatures of models with feebly interacting particles, such as da"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2504.06692","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2504.06692/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2504.06692","created_at":"2026-07-05T10:46:44.212032+00:00"},{"alias_kind":"arxiv_version","alias_value":"2504.06692v1","created_at":"2026-07-05T10:46:44.212032+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2504.06692","created_at":"2026-07-05T10:46:44.212032+00:00"},{"alias_kind":"pith_short_12","alias_value":"CN524Q3WNUW6","created_at":"2026-07-05T10:46:44.212032+00:00"},{"alias_kind":"pith_short_16","alias_value":"CN524Q3WNUW6756G","created_at":"2026-07-05T10:46:44.212032+00:00"},{"alias_kind":"pith_short_8","alias_value":"CN524Q3W","created_at":"2026-07-05T10:46:44.212032+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.11039","citing_title":"The SHiP/NA67 experiment at the ECN3 high-intensity beam facility at the CERN SPS","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"2506.22616","citing_title":"A novel phenomenological approach to total charm cross-section measurements at the LHC","ref_index":72,"is_internal_anchor":false},{"citing_arxiv_id":"2512.05380","citing_title":"Illuminating sequential freeze-in dark matter with dark photon signal at the CERN SHiP experiment","ref_index":26,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19348","citing_title":"Probing the neutrino trident process using the Scattering and Neutrino Detector at HL-LHC and SHiP","ref_index":12,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CN524Q3WNUW6756GLHGWDJZ7CC","json":"https://pith.science/pith/CN524Q3WNUW6756GLHGWDJZ7CC.json","graph_json":"https://pith.science/api/pith-number/CN524Q3WNUW6756GLHGWDJZ7CC/graph.json","events_json":"https://pith.science/api/pith-number/CN524Q3WNUW6756GLHGWDJZ7CC/events.json","paper":"https://pith.science/paper/CN524Q3W"},"agent_actions":{"view_html":"https://pith.science/pith/CN524Q3WNUW6756GLHGWDJZ7CC","download_json":"https://pith.science/pith/CN524Q3WNUW6756GLHGWDJZ7CC.json","view_paper":"https://pith.science/paper/CN524Q3W","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2504.06692&json=true","fetch_graph":"https://pith.science/api/pith-number/CN524Q3WNUW6756GLHGWDJZ7CC/graph.json","fetch_events":"https://pith.science/api/pith-number/CN524Q3WNUW6756GLHGWDJZ7CC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CN524Q3WNUW6756GLHGWDJZ7CC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CN524Q3WNUW6756GLHGWDJZ7CC/action/storage_attestation","attest_author":"https://pith.science/pith/CN524Q3WNUW6756GLHGWDJZ7CC/action/author_attestation","sign_citation":"https://pith.science/pith/CN524Q3WNUW6756GLHGWDJZ7CC/action/citation_signature","submit_replication":"https://pith.science/pith/CN524Q3WNUW6756GLHGWDJZ7CC/action/replication_record"}},"created_at":"2026-07-05T10:46:44.212032+00:00","updated_at":"2026-07-05T10:46:44.212032+00:00"}