{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:4ZW4LLPT24HZUCTG75YLSRSXVY","short_pith_number":"pith:4ZW4LLPT","schema_version":"1.0","canonical_sha256":"e66dc5adf3d70f9a0a66ff70b94657ae19156da3262887821e1af3658ade5514","source":{"kind":"arxiv","id":"1710.07171","version":2},"attestation_state":"computed","paper":{"title":"A search for pair-produced resonances in four-jet final states 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":"2017-10-19T15:02:23Z","abstract_excerpt":"A search for massive coloured resonances which are pair-produced and decay into two jets is presented. The analysis uses 36.7 fb$^{-1}$ of $\\sqrt{s}=$ 13 TeV pp collision data recorded by the ATLAS experiment at the LHC in 2015 and 2016. No significant deviation from the background prediction is observed. Results are interpreted in a SUSY simplified model where the lightest supersymmetric particle is the top squark, $\\tilde{t}$, which decays promptly into two quarks through $R$-parity-violating couplings. Top squarks with masses in the range 100 GeV < $m_{\\tilde{t}}$ < 410 GeV are excluded at "},"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":"1710.07171","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2017-10-19T15:02:23Z","cross_cats_sorted":[],"title_canon_sha256":"346c179ca71cbc4c66dcb5aab0bb3d6a67a6c9a3e095f4f8199c5cbc84397b06","abstract_canon_sha256":"66fc8b2abac8894c8f0e5430529f26ec70ae544e99be710466fe3e7b06e696e0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:19:03.278129Z","signature_b64":"bfIw57/QqpuZuTFIojW5/fl9/+ujRZhBFRhOKzpcwGJH4e2jpDModMCtJVjVh7d7oczO5JrS01mTsjZQbEfxCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e66dc5adf3d70f9a0a66ff70b94657ae19156da3262887821e1af3658ade5514","last_reissued_at":"2026-05-18T00:19:03.277413Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:19:03.277413Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A search for pair-produced resonances in four-jet final states 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":"2017-10-19T15:02:23Z","abstract_excerpt":"A search for massive coloured resonances which are pair-produced and decay into two jets is presented. The analysis uses 36.7 fb$^{-1}$ of $\\sqrt{s}=$ 13 TeV pp collision data recorded by the ATLAS experiment at the LHC in 2015 and 2016. No significant deviation from the background prediction is observed. Results are interpreted in a SUSY simplified model where the lightest supersymmetric particle is the top squark, $\\tilde{t}$, which decays promptly into two quarks through $R$-parity-violating couplings. Top squarks with masses in the range 100 GeV < $m_{\\tilde{t}}$ < 410 GeV are excluded at "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1710.07171","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":"1710.07171","created_at":"2026-05-18T00:19:03.277533+00:00"},{"alias_kind":"arxiv_version","alias_value":"1710.07171v2","created_at":"2026-05-18T00:19:03.277533+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1710.07171","created_at":"2026-05-18T00:19:03.277533+00:00"},{"alias_kind":"pith_short_12","alias_value":"4ZW4LLPT24HZ","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_16","alias_value":"4ZW4LLPT24HZUCTG","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_8","alias_value":"4ZW4LLPT","created_at":"2026-05-18T12:31:00.734936+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2511.09632","citing_title":"Octet scalars shaping LHC distributions in 4-jet final states","ref_index":54,"is_internal_anchor":true},{"citing_arxiv_id":"2604.24849","citing_title":"Accidental Peccei-Quinn Symmetry from Chiral Gauge Symmetry and Mirror QCD","ref_index":56,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4ZW4LLPT24HZUCTG75YLSRSXVY","json":"https://pith.science/pith/4ZW4LLPT24HZUCTG75YLSRSXVY.json","graph_json":"https://pith.science/api/pith-number/4ZW4LLPT24HZUCTG75YLSRSXVY/graph.json","events_json":"https://pith.science/api/pith-number/4ZW4LLPT24HZUCTG75YLSRSXVY/events.json","paper":"https://pith.science/paper/4ZW4LLPT"},"agent_actions":{"view_html":"https://pith.science/pith/4ZW4LLPT24HZUCTG75YLSRSXVY","download_json":"https://pith.science/pith/4ZW4LLPT24HZUCTG75YLSRSXVY.json","view_paper":"https://pith.science/paper/4ZW4LLPT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1710.07171&json=true","fetch_graph":"https://pith.science/api/pith-number/4ZW4LLPT24HZUCTG75YLSRSXVY/graph.json","fetch_events":"https://pith.science/api/pith-number/4ZW4LLPT24HZUCTG75YLSRSXVY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4ZW4LLPT24HZUCTG75YLSRSXVY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4ZW4LLPT24HZUCTG75YLSRSXVY/action/storage_attestation","attest_author":"https://pith.science/pith/4ZW4LLPT24HZUCTG75YLSRSXVY/action/author_attestation","sign_citation":"https://pith.science/pith/4ZW4LLPT24HZUCTG75YLSRSXVY/action/citation_signature","submit_replication":"https://pith.science/pith/4ZW4LLPT24HZUCTG75YLSRSXVY/action/replication_record"}},"created_at":"2026-05-18T00:19:03.277533+00:00","updated_at":"2026-05-18T00:19:03.277533+00:00"}