{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:LC53EXJ6VN63GO2QFFC7LULZF5","short_pith_number":"pith:LC53EXJ6","schema_version":"1.0","canonical_sha256":"58bbb25d3eab7db33b502945f5d1792f7aed175db0b29211a00be94134721d35","source":{"kind":"arxiv","id":"1509.02853","version":1},"attestation_state":"computed","paper":{"title":"Model-Independent Measurement of the e+e- -> HZ Cross Section at a Future e+e- Linear Collider using Hadronic Z Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-ex","authors_text":"Mark Thomson","submitted_at":"2015-09-09T17:09:10Z","abstract_excerpt":"A future e+e- collider, such as the ILC or CLIC, would allow the Higgs sector to be probed with a precision significantly beyond that achievable at the High-Luminosity LHC. A central part of the Higgs programme at an e+e- collider is the model-independent determination of the absolute Higgs couplings to fermions and to gauge bosons. Here the measurement of the e+e-->HZ Higgsstrahlung cross section, using the recoil mass technique, sets the absolute scale for all Higgs coupling measurements. Previous studies have considered e+e- ->ZH with Z->l+l-, where l = electron or muon. In this paper it is"},"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":"1509.02853","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2015-09-09T17:09:10Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"72a449b3ec9b52b054a168a28b1b9794b724c0a00c1005e0000e114293d19308","abstract_canon_sha256":"05e82341796dd3946f7c93e92611901af65589a9335e569eaaeef060ea5918c1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:33.197956Z","signature_b64":"q0mPCzDooysabalAjKdgfDaEy92oe+hgu4ezFQvwUOCmsPab6tp3h2BF58imiiAHc7HnDauk5glRaUyH9NN4Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"58bbb25d3eab7db33b502945f5d1792f7aed175db0b29211a00be94134721d35","last_reissued_at":"2026-05-18T01:18:33.197519Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:33.197519Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Model-Independent Measurement of the e+e- -> HZ Cross Section at a Future e+e- Linear Collider using Hadronic Z Decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-ex","authors_text":"Mark Thomson","submitted_at":"2015-09-09T17:09:10Z","abstract_excerpt":"A future e+e- collider, such as the ILC or CLIC, would allow the Higgs sector to be probed with a precision significantly beyond that achievable at the High-Luminosity LHC. A central part of the Higgs programme at an e+e- collider is the model-independent determination of the absolute Higgs couplings to fermions and to gauge bosons. Here the measurement of the e+e-->HZ Higgsstrahlung cross section, using the recoil mass technique, sets the absolute scale for all Higgs coupling measurements. Previous studies have considered e+e- ->ZH with Z->l+l-, where l = electron or muon. In this paper it is"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1509.02853","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":"1509.02853","created_at":"2026-05-18T01:18:33.197588+00:00"},{"alias_kind":"arxiv_version","alias_value":"1509.02853v1","created_at":"2026-05-18T01:18:33.197588+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1509.02853","created_at":"2026-05-18T01:18:33.197588+00:00"},{"alias_kind":"pith_short_12","alias_value":"LC53EXJ6VN63","created_at":"2026-05-18T12:29:29.992203+00:00"},{"alias_kind":"pith_short_16","alias_value":"LC53EXJ6VN63GO2Q","created_at":"2026-05-18T12:29:29.992203+00:00"},{"alias_kind":"pith_short_8","alias_value":"LC53EXJ6","created_at":"2026-05-18T12:29:29.992203+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/LC53EXJ6VN63GO2QFFC7LULZF5","json":"https://pith.science/pith/LC53EXJ6VN63GO2QFFC7LULZF5.json","graph_json":"https://pith.science/api/pith-number/LC53EXJ6VN63GO2QFFC7LULZF5/graph.json","events_json":"https://pith.science/api/pith-number/LC53EXJ6VN63GO2QFFC7LULZF5/events.json","paper":"https://pith.science/paper/LC53EXJ6"},"agent_actions":{"view_html":"https://pith.science/pith/LC53EXJ6VN63GO2QFFC7LULZF5","download_json":"https://pith.science/pith/LC53EXJ6VN63GO2QFFC7LULZF5.json","view_paper":"https://pith.science/paper/LC53EXJ6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1509.02853&json=true","fetch_graph":"https://pith.science/api/pith-number/LC53EXJ6VN63GO2QFFC7LULZF5/graph.json","fetch_events":"https://pith.science/api/pith-number/LC53EXJ6VN63GO2QFFC7LULZF5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LC53EXJ6VN63GO2QFFC7LULZF5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LC53EXJ6VN63GO2QFFC7LULZF5/action/storage_attestation","attest_author":"https://pith.science/pith/LC53EXJ6VN63GO2QFFC7LULZF5/action/author_attestation","sign_citation":"https://pith.science/pith/LC53EXJ6VN63GO2QFFC7LULZF5/action/citation_signature","submit_replication":"https://pith.science/pith/LC53EXJ6VN63GO2QFFC7LULZF5/action/replication_record"}},"created_at":"2026-05-18T01:18:33.197588+00:00","updated_at":"2026-05-18T01:18:33.197588+00:00"}