{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:7PHMWJIGHFVCMAQ3TWSRQXAOWX","short_pith_number":"pith:7PHMWJIG","schema_version":"1.0","canonical_sha256":"fbcecb2506396a26021b9da5185c0eb5ddea7a8f2d8c609329a5e4367c806c4b","source":{"kind":"arxiv","id":"2508.21660","version":1},"attestation_state":"computed","paper":{"title":"Probing the coupling of axions to tops and gluons with LHC measurements","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Fabian Esser, Jon Butterworth, Joseph Egan, Maria Ubiali, Matthew Cullingworth, Veronica Sanz","submitted_at":"2025-08-29T14:22:35Z","abstract_excerpt":"We study axion-like particles (ALPs) whose dominant interactions are with gluons and third-generation quarks, and whose couplings to light Standard Model (SM) particles arise at one loop. These loop-induced effects lead to ALP decays and production channels that can be probed at the LHC, even when tree-level couplings are absent. Using an effective field theory (EFT) description that includes momentum-dependent corrections from radiative effects, we reinterpret a wide range of LHC measurements via the CONTUR framework to derive model-independent constraints on the ALP parameter space. We show "},"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":"2508.21660","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"hep-ph","submitted_at":"2025-08-29T14:22:35Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"4026869ee04a467f82845d5dc673fe0f178d95863d0182b97628d6fd1b1268b7","abstract_canon_sha256":"0df079d068feb4ed919a63690583cb64a602c8c058d59124f3f6932c434f5736"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T12:01:47.501733Z","signature_b64":"vQ4pLzDb9vEAPqqu1lGTHCLO07qLN/pwAx5QAi09H1iKIz8tOV4HDxqEdjAWvqU+SwlAgB0M+PpSiMLie0+4Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fbcecb2506396a26021b9da5185c0eb5ddea7a8f2d8c609329a5e4367c806c4b","last_reissued_at":"2026-07-05T12:01:47.501208Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T12:01:47.501208Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Probing the coupling of axions to tops and gluons with LHC measurements","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Fabian Esser, Jon Butterworth, Joseph Egan, Maria Ubiali, Matthew Cullingworth, Veronica Sanz","submitted_at":"2025-08-29T14:22:35Z","abstract_excerpt":"We study axion-like particles (ALPs) whose dominant interactions are with gluons and third-generation quarks, and whose couplings to light Standard Model (SM) particles arise at one loop. These loop-induced effects lead to ALP decays and production channels that can be probed at the LHC, even when tree-level couplings are absent. Using an effective field theory (EFT) description that includes momentum-dependent corrections from radiative effects, we reinterpret a wide range of LHC measurements via the CONTUR framework to derive model-independent constraints on the ALP parameter space. We show "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2508.21660","kind":"arxiv","version":1},"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/2508.21660/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":"2508.21660","created_at":"2026-07-05T12:01:47.501272+00:00"},{"alias_kind":"arxiv_version","alias_value":"2508.21660v1","created_at":"2026-07-05T12:01:47.501272+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2508.21660","created_at":"2026-07-05T12:01:47.501272+00:00"},{"alias_kind":"pith_short_12","alias_value":"7PHMWJIGHFVC","created_at":"2026-07-05T12:01:47.501272+00:00"},{"alias_kind":"pith_short_16","alias_value":"7PHMWJIGHFVCMAQ3","created_at":"2026-07-05T12:01:47.501272+00:00"},{"alias_kind":"pith_short_8","alias_value":"7PHMWJIG","created_at":"2026-07-05T12:01:47.501272+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2603.22864","citing_title":"A search for heavy axion-like particles in light-by-light scattering at the FCC-hh","ref_index":71,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7PHMWJIGHFVCMAQ3TWSRQXAOWX","json":"https://pith.science/pith/7PHMWJIGHFVCMAQ3TWSRQXAOWX.json","graph_json":"https://pith.science/api/pith-number/7PHMWJIGHFVCMAQ3TWSRQXAOWX/graph.json","events_json":"https://pith.science/api/pith-number/7PHMWJIGHFVCMAQ3TWSRQXAOWX/events.json","paper":"https://pith.science/paper/7PHMWJIG"},"agent_actions":{"view_html":"https://pith.science/pith/7PHMWJIGHFVCMAQ3TWSRQXAOWX","download_json":"https://pith.science/pith/7PHMWJIGHFVCMAQ3TWSRQXAOWX.json","view_paper":"https://pith.science/paper/7PHMWJIG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2508.21660&json=true","fetch_graph":"https://pith.science/api/pith-number/7PHMWJIGHFVCMAQ3TWSRQXAOWX/graph.json","fetch_events":"https://pith.science/api/pith-number/7PHMWJIGHFVCMAQ3TWSRQXAOWX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7PHMWJIGHFVCMAQ3TWSRQXAOWX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7PHMWJIGHFVCMAQ3TWSRQXAOWX/action/storage_attestation","attest_author":"https://pith.science/pith/7PHMWJIGHFVCMAQ3TWSRQXAOWX/action/author_attestation","sign_citation":"https://pith.science/pith/7PHMWJIGHFVCMAQ3TWSRQXAOWX/action/citation_signature","submit_replication":"https://pith.science/pith/7PHMWJIGHFVCMAQ3TWSRQXAOWX/action/replication_record"}},"created_at":"2026-07-05T12:01:47.501272+00:00","updated_at":"2026-07-05T12:01:47.501272+00:00"}