{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:UPZ5OW6IVBHNLLDOPQAHZUQ7P6","short_pith_number":"pith:UPZ5OW6I","schema_version":"1.0","canonical_sha256":"a3f3d75bc8a84ed5ac6e7c007cd21f7fbed8fb9ee1d8ac12c5674bd943cfab64","source":{"kind":"arxiv","id":"1708.04053","version":2},"attestation_state":"computed","paper":{"title":"Measurement of the exclusive $\\gamma \\gamma \\rightarrow \\mu^+ \\mu^-$ process in proton--proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2017-08-14T09:49:55Z","abstract_excerpt":"The production of exclusive $\\gamma \\gamma \\rightarrow \\mu^+ \\mu^-$ events in proton--proton collisions at a centre-of-mass energy of 13 TeV is measured with the ATLAS detector at the LHC, using data corresponding to an integrated luminosity of 3.2 fb$^{-1}$. The measurement is performed for a dimuon invariant mass of 12 GeV $<m_{\\mu^+\\mu^-}<$ 70 GeV. The integrated cross-section is determined within a fiducial acceptance region of the ATLAS detector and differential cross-sections are measured as a function of the dimuon invariant mass. The results are compared to theoretical predictions that"},"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":"1708.04053","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2017-08-14T09:49:55Z","cross_cats_sorted":[],"title_canon_sha256":"c35fd8f1b5294a49c3bb3117b3bbf4cae11669906e3e70fd45e574a9a1376018","abstract_canon_sha256":"eef3e0970a137d74a2ac260eacbac3332ef5fe6e915e5e55ff942cba155a2f26"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:26:45.832298Z","signature_b64":"1SSRqc86PyPRHodYmV7QvUJ4WXZhqvxCdgEjS9rte3NJRwkdRtbTyuTRgf6TQswdau9PG5hL1VBvY0e+h2NtCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a3f3d75bc8a84ed5ac6e7c007cd21f7fbed8fb9ee1d8ac12c5674bd943cfab64","last_reissued_at":"2026-05-18T00:26:45.831710Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:26:45.831710Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the exclusive $\\gamma \\gamma \\rightarrow \\mu^+ \\mu^-$ process in proton--proton collisions at $\\sqrt{s}=13$ TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2017-08-14T09:49:55Z","abstract_excerpt":"The production of exclusive $\\gamma \\gamma \\rightarrow \\mu^+ \\mu^-$ events in proton--proton collisions at a centre-of-mass energy of 13 TeV is measured with the ATLAS detector at the LHC, using data corresponding to an integrated luminosity of 3.2 fb$^{-1}$. The measurement is performed for a dimuon invariant mass of 12 GeV $<m_{\\mu^+\\mu^-}<$ 70 GeV. The integrated cross-section is determined within a fiducial acceptance region of the ATLAS detector and differential cross-sections are measured as a function of the dimuon invariant mass. The results are compared to theoretical predictions that"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.04053","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":"1708.04053","created_at":"2026-05-18T00:26:45.831792+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.04053v2","created_at":"2026-05-18T00:26:45.831792+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.04053","created_at":"2026-05-18T00:26:45.831792+00:00"},{"alias_kind":"pith_short_12","alias_value":"UPZ5OW6IVBHN","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_16","alias_value":"UPZ5OW6IVBHNLLDO","created_at":"2026-05-18T12:31:46.661854+00:00"},{"alias_kind":"pith_short_8","alias_value":"UPZ5OW6I","created_at":"2026-05-18T12:31:46.661854+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2606.19604","citing_title":"Sensitivity of the photon-induced processes to the proton radius","ref_index":15,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UPZ5OW6IVBHNLLDOPQAHZUQ7P6","json":"https://pith.science/pith/UPZ5OW6IVBHNLLDOPQAHZUQ7P6.json","graph_json":"https://pith.science/api/pith-number/UPZ5OW6IVBHNLLDOPQAHZUQ7P6/graph.json","events_json":"https://pith.science/api/pith-number/UPZ5OW6IVBHNLLDOPQAHZUQ7P6/events.json","paper":"https://pith.science/paper/UPZ5OW6I"},"agent_actions":{"view_html":"https://pith.science/pith/UPZ5OW6IVBHNLLDOPQAHZUQ7P6","download_json":"https://pith.science/pith/UPZ5OW6IVBHNLLDOPQAHZUQ7P6.json","view_paper":"https://pith.science/paper/UPZ5OW6I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.04053&json=true","fetch_graph":"https://pith.science/api/pith-number/UPZ5OW6IVBHNLLDOPQAHZUQ7P6/graph.json","fetch_events":"https://pith.science/api/pith-number/UPZ5OW6IVBHNLLDOPQAHZUQ7P6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UPZ5OW6IVBHNLLDOPQAHZUQ7P6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UPZ5OW6IVBHNLLDOPQAHZUQ7P6/action/storage_attestation","attest_author":"https://pith.science/pith/UPZ5OW6IVBHNLLDOPQAHZUQ7P6/action/author_attestation","sign_citation":"https://pith.science/pith/UPZ5OW6IVBHNLLDOPQAHZUQ7P6/action/citation_signature","submit_replication":"https://pith.science/pith/UPZ5OW6IVBHNLLDOPQAHZUQ7P6/action/replication_record"}},"created_at":"2026-05-18T00:26:45.831792+00:00","updated_at":"2026-05-18T00:26:45.831792+00:00"}