{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:VHWXF5K7BRDTDVC455W4HCQSH4","short_pith_number":"pith:VHWXF5K7","schema_version":"1.0","canonical_sha256":"a9ed72f55f0c4731d45cef6dc38a123f2ff6e8b9d214b4647a8e346b554131a2","source":{"kind":"arxiv","id":"2210.02784","version":3},"attestation_state":"computed","paper":{"title":"SND@LHC: The Scattering and Neutrino Detector at the LHC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.ins-det"],"primary_cat":"hep-ex","authors_text":"The SND@LHC Collaboration","submitted_at":"2022-10-06T09:46:56Z","abstract_excerpt":"SND@LHC is a compact and stand-alone experiment designed to perform measurements with neutrinos produced at the LHC in the pseudo-rapidity region of ${7.2 < \\eta < 8.4}$. The experiment is located 480 m downstream of the ATLAS interaction point, in the TI18 tunnel. The detector is composed of a hybrid system based on an 830 kg target made of tungsten plates, interleaved with emulsion and electronic trackers, also acting as an electromagnetic calorimeter, and followed by a hadronic calorimeter and a muon identification system. The detector is able to distinguish interactions of all three neutri"},"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":"2210.02784","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2022-10-06T09:46:56Z","cross_cats_sorted":["physics.ins-det"],"title_canon_sha256":"c190a42900ab13eb17a12cbecb29bc96cfeec368c3ddc8b93268a0683003746b","abstract_canon_sha256":"5af7855cc1dc9e4acac770709a48e810c81ac08805d309dea408fe0a8b75749a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:40:04.710445Z","signature_b64":"HvMzeSmEqYNFl8in2S6Utkxhaum0641Ry5nusD11dBZpzUL/K0Kl3rCXWSKtrQhBoztRnMfFs724nYRr7HiIBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a9ed72f55f0c4731d45cef6dc38a123f2ff6e8b9d214b4647a8e346b554131a2","last_reissued_at":"2026-07-05T08:40:04.709962Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:40:04.709962Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"SND@LHC: The Scattering and Neutrino Detector at the LHC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.ins-det"],"primary_cat":"hep-ex","authors_text":"The SND@LHC Collaboration","submitted_at":"2022-10-06T09:46:56Z","abstract_excerpt":"SND@LHC is a compact and stand-alone experiment designed to perform measurements with neutrinos produced at the LHC in the pseudo-rapidity region of ${7.2 < \\eta < 8.4}$. The experiment is located 480 m downstream of the ATLAS interaction point, in the TI18 tunnel. The detector is composed of a hybrid system based on an 830 kg target made of tungsten plates, interleaved with emulsion and electronic trackers, also acting as an electromagnetic calorimeter, and followed by a hadronic calorimeter and a muon identification system. The detector is able to distinguish interactions of all three neutri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.02784","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2210.02784/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":"2210.02784","created_at":"2026-07-05T08:40:04.710024+00:00"},{"alias_kind":"arxiv_version","alias_value":"2210.02784v3","created_at":"2026-07-05T08:40:04.710024+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.02784","created_at":"2026-07-05T08:40:04.710024+00:00"},{"alias_kind":"pith_short_12","alias_value":"VHWXF5K7BRDT","created_at":"2026-07-05T08:40:04.710024+00:00"},{"alias_kind":"pith_short_16","alias_value":"VHWXF5K7BRDTDVC4","created_at":"2026-07-05T08:40:04.710024+00:00"},{"alias_kind":"pith_short_8","alias_value":"VHWXF5K7","created_at":"2026-07-05T08:40:04.710024+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.06773","citing_title":"Lepton interactions from GeV to EeV","ref_index":25,"is_internal_anchor":false},{"citing_arxiv_id":"2606.05406","citing_title":"Muon-induced di-tau production as a probe of new physics","ref_index":65,"is_internal_anchor":false},{"citing_arxiv_id":"2508.00761","citing_title":"Non-Standard Neutrino Interactions at a Muon Collider Neutrino Detector","ref_index":28,"is_internal_anchor":false},{"citing_arxiv_id":"2505.00272","citing_title":"Future Circular Collider Feasibility Study Report: Volume 1, Physics, Experiments, Detectors","ref_index":290,"is_internal_anchor":false},{"citing_arxiv_id":"2602.21881","citing_title":"SND@LHC Upgrade for the High-Luminosity LHC: Physics Reach and Installation Scenarios","ref_index":2,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VHWXF5K7BRDTDVC455W4HCQSH4","json":"https://pith.science/pith/VHWXF5K7BRDTDVC455W4HCQSH4.json","graph_json":"https://pith.science/api/pith-number/VHWXF5K7BRDTDVC455W4HCQSH4/graph.json","events_json":"https://pith.science/api/pith-number/VHWXF5K7BRDTDVC455W4HCQSH4/events.json","paper":"https://pith.science/paper/VHWXF5K7"},"agent_actions":{"view_html":"https://pith.science/pith/VHWXF5K7BRDTDVC455W4HCQSH4","download_json":"https://pith.science/pith/VHWXF5K7BRDTDVC455W4HCQSH4.json","view_paper":"https://pith.science/paper/VHWXF5K7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2210.02784&json=true","fetch_graph":"https://pith.science/api/pith-number/VHWXF5K7BRDTDVC455W4HCQSH4/graph.json","fetch_events":"https://pith.science/api/pith-number/VHWXF5K7BRDTDVC455W4HCQSH4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VHWXF5K7BRDTDVC455W4HCQSH4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VHWXF5K7BRDTDVC455W4HCQSH4/action/storage_attestation","attest_author":"https://pith.science/pith/VHWXF5K7BRDTDVC455W4HCQSH4/action/author_attestation","sign_citation":"https://pith.science/pith/VHWXF5K7BRDTDVC455W4HCQSH4/action/citation_signature","submit_replication":"https://pith.science/pith/VHWXF5K7BRDTDVC455W4HCQSH4/action/replication_record"}},"created_at":"2026-07-05T08:40:04.710024+00:00","updated_at":"2026-07-05T08:40:04.710024+00:00"}