{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:GZKBCWLEMUYOMNG4AN552I7ST7","short_pith_number":"pith:GZKBCWLE","schema_version":"1.0","canonical_sha256":"36541159646530e634dc037bdd23f29ffef42f7e586386af95dc8ea48d5f203a","source":{"kind":"arxiv","id":"2505.01634","version":2},"attestation_state":"computed","paper":{"title":"Search for new physics in final states with semi-visible jets or anomalous signatures 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":"2025-05-02T23:56:12Z","abstract_excerpt":"A search is presented for hadronic signatures of beyond the Standard Model (BSM) physics, with an emphasis on signatures of a strongly-coupled hidden dark sector accessed via resonant production of a $Z'$ mediator. The ATLAS experiment dataset collected at the Large Hadron Collider from 2015 to 2018 is used, consisting of proton-proton collisions at $\\sqrt{s}$ = 13 TeV and corresponding to an integrated luminosity of 140 fb$^{-1}$. The $Z'$ mediator is considered to decay to two dark quarks, which each hadronize and decay to showers containing both dark and Standard Model particles, producing "},"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":"2505.01634","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2025-05-02T23:56:12Z","cross_cats_sorted":[],"title_canon_sha256":"d455e9d2d17a8d681b021297d7dd78ddd3f3717dde41d6337ddf9212bf1570eb","abstract_canon_sha256":"44c2b579b1a239648012886849d27ee879f64ae55d9fb4c91bd7e1ad8684f1cc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T12:00:27.570674Z","signature_b64":"mENv8TinBy6PzwoHaSCaNYgkHlUCR19BZ+Mm+R9iOUJuzW9/ky2foimhrLpSFxT3I/13JSwKVeV+fclJofaaDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"36541159646530e634dc037bdd23f29ffef42f7e586386af95dc8ea48d5f203a","last_reissued_at":"2026-07-05T12:00:27.570227Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T12:00:27.570227Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for new physics in final states with semi-visible jets or anomalous signatures 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":"2025-05-02T23:56:12Z","abstract_excerpt":"A search is presented for hadronic signatures of beyond the Standard Model (BSM) physics, with an emphasis on signatures of a strongly-coupled hidden dark sector accessed via resonant production of a $Z'$ mediator. The ATLAS experiment dataset collected at the Large Hadron Collider from 2015 to 2018 is used, consisting of proton-proton collisions at $\\sqrt{s}$ = 13 TeV and corresponding to an integrated luminosity of 140 fb$^{-1}$. The $Z'$ mediator is considered to decay to two dark quarks, which each hadronize and decay to showers containing both dark and Standard Model particles, producing "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2505.01634","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/2505.01634/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":"2505.01634","created_at":"2026-07-05T12:00:27.570283+00:00"},{"alias_kind":"arxiv_version","alias_value":"2505.01634v2","created_at":"2026-07-05T12:00:27.570283+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2505.01634","created_at":"2026-07-05T12:00:27.570283+00:00"},{"alias_kind":"pith_short_12","alias_value":"GZKBCWLEMUYO","created_at":"2026-07-05T12:00:27.570283+00:00"},{"alias_kind":"pith_short_16","alias_value":"GZKBCWLEMUYOMNG4","created_at":"2026-07-05T12:00:27.570283+00:00"},{"alias_kind":"pith_short_8","alias_value":"GZKBCWLE","created_at":"2026-07-05T12:00:27.570283+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"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":11,"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":9,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GZKBCWLEMUYOMNG4AN552I7ST7","json":"https://pith.science/pith/GZKBCWLEMUYOMNG4AN552I7ST7.json","graph_json":"https://pith.science/api/pith-number/GZKBCWLEMUYOMNG4AN552I7ST7/graph.json","events_json":"https://pith.science/api/pith-number/GZKBCWLEMUYOMNG4AN552I7ST7/events.json","paper":"https://pith.science/paper/GZKBCWLE"},"agent_actions":{"view_html":"https://pith.science/pith/GZKBCWLEMUYOMNG4AN552I7ST7","download_json":"https://pith.science/pith/GZKBCWLEMUYOMNG4AN552I7ST7.json","view_paper":"https://pith.science/paper/GZKBCWLE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2505.01634&json=true","fetch_graph":"https://pith.science/api/pith-number/GZKBCWLEMUYOMNG4AN552I7ST7/graph.json","fetch_events":"https://pith.science/api/pith-number/GZKBCWLEMUYOMNG4AN552I7ST7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GZKBCWLEMUYOMNG4AN552I7ST7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GZKBCWLEMUYOMNG4AN552I7ST7/action/storage_attestation","attest_author":"https://pith.science/pith/GZKBCWLEMUYOMNG4AN552I7ST7/action/author_attestation","sign_citation":"https://pith.science/pith/GZKBCWLEMUYOMNG4AN552I7ST7/action/citation_signature","submit_replication":"https://pith.science/pith/GZKBCWLEMUYOMNG4AN552I7ST7/action/replication_record"}},"created_at":"2026-07-05T12:00:27.570283+00:00","updated_at":"2026-07-05T12:00:27.570283+00:00"}