{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:FDEDRS3MZ5MJIWJOILAGNJ7EU3","short_pith_number":"pith:FDEDRS3M","schema_version":"1.0","canonical_sha256":"28c838cb6ccf5894592e42c066a7e4a6ee4cc685b5658061b8506d331adbed73","source":{"kind":"arxiv","id":"1510.03818","version":3},"attestation_state":"computed","paper":{"title":"Measurement of the differential cross-section of highly boosted top quarks as a function of their transverse momentum in $\\sqrt{s}$ = 8 TeV proton-proton collisions using the ATLAS detector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2015-10-13T18:58:07Z","abstract_excerpt":"The differential cross-section for pair production of top quarks with high transverse momentum is measured in 20.3 fb$^{-1}$ of proton-proton collisions at a center-of-mass energy of 8 TeV. The measurement is performed for $t\\bar{t}$ events in the lepton+jets channel. The cross-section is reported as a function of the hadronically decaying top quark transverse momentum for values above 300 GeV. The hadronically decaying top quark is reconstructed as an anti-$k_t$ jet with radius parameter $R=1.0$ and identified with jet substructure techniques. The observed yield is corrected for detector effe"},"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":"1510.03818","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2015-10-13T18:58:07Z","cross_cats_sorted":[],"title_canon_sha256":"823011ea29e5147edbbfaf35a2d3744ed87118e03449bd795d58d1fb5eefb9a3","abstract_canon_sha256":"0d2ec9c90af76a342aa879f51f7cf003370b43a3061e13457462683206ca1700"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:19:29.292250Z","signature_b64":"9y+KpEx9vA8NqBCmKdobyImfw3ir++t1zI3h/kNUlrWqFBfNufMC2pUbyDZFd+Y+V/w3UP0atYFR9dlBj75MDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"28c838cb6ccf5894592e42c066a7e4a6ee4cc685b5658061b8506d331adbed73","last_reissued_at":"2026-05-18T01:19:29.291549Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:19:29.291549Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurement of the differential cross-section of highly boosted top quarks as a function of their transverse momentum in $\\sqrt{s}$ = 8 TeV proton-proton collisions using the ATLAS detector","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2015-10-13T18:58:07Z","abstract_excerpt":"The differential cross-section for pair production of top quarks with high transverse momentum is measured in 20.3 fb$^{-1}$ of proton-proton collisions at a center-of-mass energy of 8 TeV. The measurement is performed for $t\\bar{t}$ events in the lepton+jets channel. The cross-section is reported as a function of the hadronically decaying top quark transverse momentum for values above 300 GeV. The hadronically decaying top quark is reconstructed as an anti-$k_t$ jet with radius parameter $R=1.0$ and identified with jet substructure techniques. The observed yield is corrected for detector effe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.03818","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":""},"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":"1510.03818","created_at":"2026-05-18T01:19:29.291652+00:00"},{"alias_kind":"arxiv_version","alias_value":"1510.03818v3","created_at":"2026-05-18T01:19:29.291652+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.03818","created_at":"2026-05-18T01:19:29.291652+00:00"},{"alias_kind":"pith_short_12","alias_value":"FDEDRS3MZ5MJ","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_16","alias_value":"FDEDRS3MZ5MJIWJO","created_at":"2026-05-18T12:29:19.899920+00:00"},{"alias_kind":"pith_short_8","alias_value":"FDEDRS3M","created_at":"2026-05-18T12:29:19.899920+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2510.00160","citing_title":"Measurement of the dineutrino system kinematic variables in dileptonic top quark pair production in proton-proton collisions at$\\sqrt{s}$ = 13 TeV","ref_index":8,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FDEDRS3MZ5MJIWJOILAGNJ7EU3","json":"https://pith.science/pith/FDEDRS3MZ5MJIWJOILAGNJ7EU3.json","graph_json":"https://pith.science/api/pith-number/FDEDRS3MZ5MJIWJOILAGNJ7EU3/graph.json","events_json":"https://pith.science/api/pith-number/FDEDRS3MZ5MJIWJOILAGNJ7EU3/events.json","paper":"https://pith.science/paper/FDEDRS3M"},"agent_actions":{"view_html":"https://pith.science/pith/FDEDRS3MZ5MJIWJOILAGNJ7EU3","download_json":"https://pith.science/pith/FDEDRS3MZ5MJIWJOILAGNJ7EU3.json","view_paper":"https://pith.science/paper/FDEDRS3M","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1510.03818&json=true","fetch_graph":"https://pith.science/api/pith-number/FDEDRS3MZ5MJIWJOILAGNJ7EU3/graph.json","fetch_events":"https://pith.science/api/pith-number/FDEDRS3MZ5MJIWJOILAGNJ7EU3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FDEDRS3MZ5MJIWJOILAGNJ7EU3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FDEDRS3MZ5MJIWJOILAGNJ7EU3/action/storage_attestation","attest_author":"https://pith.science/pith/FDEDRS3MZ5MJIWJOILAGNJ7EU3/action/author_attestation","sign_citation":"https://pith.science/pith/FDEDRS3MZ5MJIWJOILAGNJ7EU3/action/citation_signature","submit_replication":"https://pith.science/pith/FDEDRS3MZ5MJIWJOILAGNJ7EU3/action/replication_record"}},"created_at":"2026-05-18T01:19:29.291652+00:00","updated_at":"2026-05-18T01:19:29.291652+00:00"}