{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:TIGSSR6VAUIRRWFSCKC36BQJTA","short_pith_number":"pith:TIGSSR6V","schema_version":"1.0","canonical_sha256":"9a0d2947d5051118d8b21285bf0609980871327e78061bc707286238dcbe4f56","source":{"kind":"arxiv","id":"1908.07305","version":2},"attestation_state":"computed","paper":{"title":"Measurements of top-quark pair differential and double-differential cross-sections in the $\\ell$+jets channel with $pp$ collisions at $\\sqrt{s}=13$ TeV using the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2019-08-20T12:45:22Z","abstract_excerpt":"Single- and double-differential cross-section measurements are presented for the production of top-quark pairs, in the lepton + jets channel at particle and parton level. Two topologies, resolved and boosted, are considered and the results are presented as a function of several kinematic variables characterising the top and $t\\bar{t}$ system and jet multiplicities. The study was performed using data from $pp$ collisions at centre-of-mass energy of 13 TeV collected in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider (LHC), corresponding to an integrated luminosity of $36~\\m"},"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":"1908.07305","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2019-08-20T12:45:22Z","cross_cats_sorted":[],"title_canon_sha256":"81e84a5ceb1fba037fea893126b8e341a63a29ea64b44b1d408779d62411e8ef","abstract_canon_sha256":"aa92c925fde7ceaee3670fadcd998700a49d3521e0457a95b1c52e3267fe78f1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:32:39.029245Z","signature_b64":"6cmwXBn1HggZG5y9k03jnINzPtPwEW7F+JKjuqkke8zRkhi95ObXPeyjLNBvJ2fyXHtcT37mVLdYp1RyG1AoCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9a0d2947d5051118d8b21285bf0609980871327e78061bc707286238dcbe4f56","last_reissued_at":"2026-07-05T00:32:39.028859Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:32:39.028859Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Measurements of top-quark pair differential and double-differential cross-sections in the $\\ell$+jets channel with $pp$ collisions at $\\sqrt{s}=13$ TeV using the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2019-08-20T12:45:22Z","abstract_excerpt":"Single- and double-differential cross-section measurements are presented for the production of top-quark pairs, in the lepton + jets channel at particle and parton level. Two topologies, resolved and boosted, are considered and the results are presented as a function of several kinematic variables characterising the top and $t\\bar{t}$ system and jet multiplicities. The study was performed using data from $pp$ collisions at centre-of-mass energy of 13 TeV collected in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider (LHC), corresponding to an integrated luminosity of $36~\\m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.07305","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1908.07305/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":"1908.07305","created_at":"2026-07-05T00:32:39.028907+00:00"},{"alias_kind":"arxiv_version","alias_value":"1908.07305v2","created_at":"2026-07-05T00:32:39.028907+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.07305","created_at":"2026-07-05T00:32:39.028907+00:00"},{"alias_kind":"pith_short_12","alias_value":"TIGSSR6VAUIR","created_at":"2026-07-05T00:32:39.028907+00:00"},{"alias_kind":"pith_short_16","alias_value":"TIGSSR6VAUIRRWFS","created_at":"2026-07-05T00:32:39.028907+00:00"},{"alias_kind":"pith_short_8","alias_value":"TIGSSR6V","created_at":"2026-07-05T00:32:39.028907+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.06199","citing_title":"Simultaneous efficiency measurements of $b$- and $c$-jets in $t\\bar{t}$ events from $\\sqrt{s}=13.6$ TeV $pp$ collision data collected with the ATLAS detector","ref_index":69,"is_internal_anchor":true},{"citing_arxiv_id":"2605.28538","citing_title":"Search for pair-produced vector-like $T$-quarks decaying into $Ht$ final states in the lepton-plus-jets channel in $pp$ collisions at $\\sqrt{s}$=13 TeV with the ATLAS detector","ref_index":86,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TIGSSR6VAUIRRWFSCKC36BQJTA","json":"https://pith.science/pith/TIGSSR6VAUIRRWFSCKC36BQJTA.json","graph_json":"https://pith.science/api/pith-number/TIGSSR6VAUIRRWFSCKC36BQJTA/graph.json","events_json":"https://pith.science/api/pith-number/TIGSSR6VAUIRRWFSCKC36BQJTA/events.json","paper":"https://pith.science/paper/TIGSSR6V"},"agent_actions":{"view_html":"https://pith.science/pith/TIGSSR6VAUIRRWFSCKC36BQJTA","download_json":"https://pith.science/pith/TIGSSR6VAUIRRWFSCKC36BQJTA.json","view_paper":"https://pith.science/paper/TIGSSR6V","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1908.07305&json=true","fetch_graph":"https://pith.science/api/pith-number/TIGSSR6VAUIRRWFSCKC36BQJTA/graph.json","fetch_events":"https://pith.science/api/pith-number/TIGSSR6VAUIRRWFSCKC36BQJTA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TIGSSR6VAUIRRWFSCKC36BQJTA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TIGSSR6VAUIRRWFSCKC36BQJTA/action/storage_attestation","attest_author":"https://pith.science/pith/TIGSSR6VAUIRRWFSCKC36BQJTA/action/author_attestation","sign_citation":"https://pith.science/pith/TIGSSR6VAUIRRWFSCKC36BQJTA/action/citation_signature","submit_replication":"https://pith.science/pith/TIGSSR6VAUIRRWFSCKC36BQJTA/action/replication_record"}},"created_at":"2026-07-05T00:32:39.028907+00:00","updated_at":"2026-07-05T00:32:39.028907+00:00"}