{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:XMSIM7JE3I7KW5AKHZFSIC7Y2D","short_pith_number":"pith:XMSIM7JE","schema_version":"1.0","canonical_sha256":"bb24867d24da3eab740a3e4b240bf8d0c9f3547c7b2a585551f1d5f42621711f","source":{"kind":"arxiv","id":"1103.6218","version":1},"attestation_state":"computed","paper":{"title":"Search for high mass dilepton resonances in pp collisions at sqrt{s}=7 TeV with the ATLAS experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The ATLAS Collaboration","submitted_at":"2011-03-31T15:49:09Z","abstract_excerpt":"This article presents a search for high mass e e or mu mu resonances in pp collisions at sqrt{s} = 7 TeV at the LHC. The data were recorded by the ATLAS experiment during 2010 and correspond to a total integrated luminosity of ~40/pb. No statistically significant excess above the Standard Model expectation is observed in the search region of dilepton invariant mass above 110 GeV. Upper limits at the 95% confidence level are set on the cross section times branching ratio of Z' resonances decaying to dielectrons and dimuons as a function of the resonance mass. A lower mass limit of 1.048 TeV on "},"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":"1103.6218","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2011-03-31T15:49:09Z","cross_cats_sorted":[],"title_canon_sha256":"0f734a82e3a032c04f4cb599767a4d88ea1a0f39c18ab5aa7c846e8fcb54b9b0","abstract_canon_sha256":"bad75f2107266c574c6e3065986a5d7dc44929617a1d05f9b9b64a5147fe2f06"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:48:00.700043Z","signature_b64":"GWCKDpUNkhKwfqlvTIZOEuPgUCMAkSoJPr4RINcC5zGG2PK8UpmY25+5/j/L2cBecFrrICS5t8D27DcJiWqQDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bb24867d24da3eab740a3e4b240bf8d0c9f3547c7b2a585551f1d5f42621711f","last_reissued_at":"2026-05-18T03:48:00.699682Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:48:00.699682Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for high mass dilepton resonances in pp collisions at sqrt{s}=7 TeV with the ATLAS experiment","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"The ATLAS Collaboration","submitted_at":"2011-03-31T15:49:09Z","abstract_excerpt":"This article presents a search for high mass e e or mu mu resonances in pp collisions at sqrt{s} = 7 TeV at the LHC. The data were recorded by the ATLAS experiment during 2010 and correspond to a total integrated luminosity of ~40/pb. No statistically significant excess above the Standard Model expectation is observed in the search region of dilepton invariant mass above 110 GeV. Upper limits at the 95% confidence level are set on the cross section times branching ratio of Z' resonances decaying to dielectrons and dimuons as a function of the resonance mass. A lower mass limit of 1.048 TeV on "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1103.6218","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":"1103.6218","created_at":"2026-05-18T03:48:00.699741+00:00"},{"alias_kind":"arxiv_version","alias_value":"1103.6218v1","created_at":"2026-05-18T03:48:00.699741+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1103.6218","created_at":"2026-05-18T03:48:00.699741+00:00"},{"alias_kind":"pith_short_12","alias_value":"XMSIM7JE3I7K","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_16","alias_value":"XMSIM7JE3I7KW5AK","created_at":"2026-05-18T12:26:47.523578+00:00"},{"alias_kind":"pith_short_8","alias_value":"XMSIM7JE","created_at":"2026-05-18T12:26:47.523578+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/XMSIM7JE3I7KW5AKHZFSIC7Y2D","json":"https://pith.science/pith/XMSIM7JE3I7KW5AKHZFSIC7Y2D.json","graph_json":"https://pith.science/api/pith-number/XMSIM7JE3I7KW5AKHZFSIC7Y2D/graph.json","events_json":"https://pith.science/api/pith-number/XMSIM7JE3I7KW5AKHZFSIC7Y2D/events.json","paper":"https://pith.science/paper/XMSIM7JE"},"agent_actions":{"view_html":"https://pith.science/pith/XMSIM7JE3I7KW5AKHZFSIC7Y2D","download_json":"https://pith.science/pith/XMSIM7JE3I7KW5AKHZFSIC7Y2D.json","view_paper":"https://pith.science/paper/XMSIM7JE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1103.6218&json=true","fetch_graph":"https://pith.science/api/pith-number/XMSIM7JE3I7KW5AKHZFSIC7Y2D/graph.json","fetch_events":"https://pith.science/api/pith-number/XMSIM7JE3I7KW5AKHZFSIC7Y2D/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XMSIM7JE3I7KW5AKHZFSIC7Y2D/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XMSIM7JE3I7KW5AKHZFSIC7Y2D/action/storage_attestation","attest_author":"https://pith.science/pith/XMSIM7JE3I7KW5AKHZFSIC7Y2D/action/author_attestation","sign_citation":"https://pith.science/pith/XMSIM7JE3I7KW5AKHZFSIC7Y2D/action/citation_signature","submit_replication":"https://pith.science/pith/XMSIM7JE3I7KW5AKHZFSIC7Y2D/action/replication_record"}},"created_at":"2026-05-18T03:48:00.699741+00:00","updated_at":"2026-05-18T03:48:00.699741+00:00"}