{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:VHD3MX5WXSQDJKRA7ERXKW7KT7","short_pith_number":"pith:VHD3MX5W","schema_version":"1.0","canonical_sha256":"a9c7b65fb6bca034aa20f923755bea9ff98c8f91c7fc6264f1ba151219ea189c","source":{"kind":"arxiv","id":"2505.02429","version":2},"attestation_state":"computed","paper":{"title":"Search for emerging jets in $pp$ collisions at $\\sqrt{s} = 13.6$ TeV with the ATLAS experiment","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2025-05-05T07:48:02Z","abstract_excerpt":"A search for emerging jets is presented using 51.8 fb$^{-1}$ of proton-proton collision data at $\\sqrt{s} = 13.6$ TeV, collected by the ATLAS experiment during 2022 and 2023. The search explores a hypothetical dark sector featuring 'dark quarks', which are charged under a confining gauge group and couple to the Standard Model via a new mediator particle. These dark quarks undergo showering and hadronization within the dark sector, forming long-lived dark mesons that decay back into Standard Model particles. This results in jets which contain multiple displaced vertices known as emerging jets. "},"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":"2505.02429","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2025-05-05T07:48:02Z","cross_cats_sorted":[],"title_canon_sha256":"8df17626b473cac978d99cfa7e251e1fa1babb43a57a7c67b6e474a3001424d9","abstract_canon_sha256":"165ecd4f73af473765e780ecb42b9b39e35c3bdc8fa2120997592467f1b83e04"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T12:07:06.850439Z","signature_b64":"Xaqiu9MumafHtHmBDtxUrwaWoUMJC8sv4+NI17Z9Q3UnJRzKGlNd7tNbKQURPicq/YYtSyPk5HHHgFRWsrtTBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a9c7b65fb6bca034aa20f923755bea9ff98c8f91c7fc6264f1ba151219ea189c","last_reissued_at":"2026-07-05T12:07:06.850008Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T12:07:06.850008Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for emerging jets in $pp$ collisions at $\\sqrt{s} = 13.6$ TeV with the ATLAS experiment","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2025-05-05T07:48:02Z","abstract_excerpt":"A search for emerging jets is presented using 51.8 fb$^{-1}$ of proton-proton collision data at $\\sqrt{s} = 13.6$ TeV, collected by the ATLAS experiment during 2022 and 2023. The search explores a hypothetical dark sector featuring 'dark quarks', which are charged under a confining gauge group and couple to the Standard Model via a new mediator particle. These dark quarks undergo showering and hadronization within the dark sector, forming long-lived dark mesons that decay back into Standard Model particles. This results in jets which contain multiple displaced vertices known as emerging jets. "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.02429","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/2505.02429/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":"2505.02429","created_at":"2026-07-05T12:07:06.850064+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.02429v2","created_at":"2026-07-05T12:07:06.850064+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.02429","created_at":"2026-07-05T12:07:06.850064+00:00"},{"alias_kind":"pith_short_12","alias_value":"VHD3MX5WXSQD","created_at":"2026-07-05T12:07:06.850064+00:00"},{"alias_kind":"pith_short_16","alias_value":"VHD3MX5WXSQDJKRA","created_at":"2026-07-05T12:07:06.850064+00:00"},{"alias_kind":"pith_short_8","alias_value":"VHD3MX5W","created_at":"2026-07-05T12:07:06.850064+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.20015","citing_title":"Search for soft unclustered energy patterns containing muons in the final state in $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector","ref_index":13,"is_internal_anchor":false},{"citing_arxiv_id":"2507.13430","citing_title":"Stopping Dark Mesons in Their Tracks with Long-Lived Particle and Resonant Signatures","ref_index":10,"is_internal_anchor":false},{"citing_arxiv_id":"2605.07585","citing_title":"Track and Vertex Reconstruction with the ATLAS Inner Detector","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VHD3MX5WXSQDJKRA7ERXKW7KT7","json":"https://pith.science/pith/VHD3MX5WXSQDJKRA7ERXKW7KT7.json","graph_json":"https://pith.science/api/pith-number/VHD3MX5WXSQDJKRA7ERXKW7KT7/graph.json","events_json":"https://pith.science/api/pith-number/VHD3MX5WXSQDJKRA7ERXKW7KT7/events.json","paper":"https://pith.science/paper/VHD3MX5W"},"agent_actions":{"view_html":"https://pith.science/pith/VHD3MX5WXSQDJKRA7ERXKW7KT7","download_json":"https://pith.science/pith/VHD3MX5WXSQDJKRA7ERXKW7KT7.json","view_paper":"https://pith.science/paper/VHD3MX5W","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.02429&json=true","fetch_graph":"https://pith.science/api/pith-number/VHD3MX5WXSQDJKRA7ERXKW7KT7/graph.json","fetch_events":"https://pith.science/api/pith-number/VHD3MX5WXSQDJKRA7ERXKW7KT7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VHD3MX5WXSQDJKRA7ERXKW7KT7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VHD3MX5WXSQDJKRA7ERXKW7KT7/action/storage_attestation","attest_author":"https://pith.science/pith/VHD3MX5WXSQDJKRA7ERXKW7KT7/action/author_attestation","sign_citation":"https://pith.science/pith/VHD3MX5WXSQDJKRA7ERXKW7KT7/action/citation_signature","submit_replication":"https://pith.science/pith/VHD3MX5WXSQDJKRA7ERXKW7KT7/action/replication_record"}},"created_at":"2026-07-05T12:07:06.850064+00:00","updated_at":"2026-07-05T12:07:06.850064+00:00"}