{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:PGGVXSEIE2TBECKQOA3WHTSMOT","short_pith_number":"pith:PGGVXSEI","schema_version":"1.0","canonical_sha256":"798d5bc88826a6120950703763ce4c74c4efd1f876106fd3dcc7fbdbd7aeb4b6","source":{"kind":"arxiv","id":"2607.09852","version":1},"attestation_state":"computed","paper":{"title":"Darkly Charged ALPs","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Aneesh V. Manohar, Bel\\'en Gavela, Elizabeth E. Jenkins, Enrique Fern\\'andez-Mart\\'inez, Nicol\\'as M. Arenaza, Pablo Qu\\'ilez, Thomas Steingasser","submitted_at":"2026-07-10T18:00:01Z","abstract_excerpt":"The established $d=5$ ALP effective Lagrangian describes the interaction of scalars with approximate shift-symmetry which carry no Standard Model (SM) charges with SM fields. It implicitly assumes that ALPs are not charged under any symmetries of the dark sector. In this paper, we remove this assumption. For ALPs carrying conserved dark charges, no $d=5$ ALP effective interaction to SM particles is possible. We build the effective Lagrangian for these darkly charged ALPs stemming from a general breaking pattern, and we show that the lowest-order shift-symmetric effective Lagrangian contains ju"},"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":"2607.09852","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-07-10T18:00:01Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"f793af0f29b5939a97f83ef32e08bfd9049aef4bfe1c13bc2624618d63f718d3","abstract_canon_sha256":"b7382560e53dd333ad0313a6c713ca60fc15e43baa08f099a783c06b5ad1bfc1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-14T00:18:39.705735Z","signature_b64":"zoxjb+gXFKPBsTvU8aqktbUDE5sAo/SEPEq8HJsFC8AlEbGvkJLm8BQS6y5XE2K4EWAZCOnEDuto6WyAdb8dBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"798d5bc88826a6120950703763ce4c74c4efd1f876106fd3dcc7fbdbd7aeb4b6","last_reissued_at":"2026-07-14T00:18:39.704780Z","signature_status":"signed_v1","first_computed_at":"2026-07-14T00:18:39.704780Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Darkly Charged ALPs","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Aneesh V. Manohar, Bel\\'en Gavela, Elizabeth E. Jenkins, Enrique Fern\\'andez-Mart\\'inez, Nicol\\'as M. Arenaza, Pablo Qu\\'ilez, Thomas Steingasser","submitted_at":"2026-07-10T18:00:01Z","abstract_excerpt":"The established $d=5$ ALP effective Lagrangian describes the interaction of scalars with approximate shift-symmetry which carry no Standard Model (SM) charges with SM fields. It implicitly assumes that ALPs are not charged under any symmetries of the dark sector. In this paper, we remove this assumption. For ALPs carrying conserved dark charges, no $d=5$ ALP effective interaction to SM particles is possible. We build the effective Lagrangian for these darkly charged ALPs stemming from a general breaking pattern, and we show that the lowest-order shift-symmetric effective Lagrangian contains ju"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.09852","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/2607.09852/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":"2607.09852","created_at":"2026-07-14T00:18:39.705212+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.09852v1","created_at":"2026-07-14T00:18:39.705212+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.09852","created_at":"2026-07-14T00:18:39.705212+00:00"},{"alias_kind":"pith_short_12","alias_value":"PGGVXSEIE2TB","created_at":"2026-07-14T00:18:39.705212+00:00"},{"alias_kind":"pith_short_16","alias_value":"PGGVXSEIE2TBECKQ","created_at":"2026-07-14T00:18:39.705212+00:00"},{"alias_kind":"pith_short_8","alias_value":"PGGVXSEI","created_at":"2026-07-14T00:18:39.705212+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/PGGVXSEIE2TBECKQOA3WHTSMOT","json":"https://pith.science/pith/PGGVXSEIE2TBECKQOA3WHTSMOT.json","graph_json":"https://pith.science/api/pith-number/PGGVXSEIE2TBECKQOA3WHTSMOT/graph.json","events_json":"https://pith.science/api/pith-number/PGGVXSEIE2TBECKQOA3WHTSMOT/events.json","paper":"https://pith.science/paper/PGGVXSEI"},"agent_actions":{"view_html":"https://pith.science/pith/PGGVXSEIE2TBECKQOA3WHTSMOT","download_json":"https://pith.science/pith/PGGVXSEIE2TBECKQOA3WHTSMOT.json","view_paper":"https://pith.science/paper/PGGVXSEI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.09852&json=true","fetch_graph":"https://pith.science/api/pith-number/PGGVXSEIE2TBECKQOA3WHTSMOT/graph.json","fetch_events":"https://pith.science/api/pith-number/PGGVXSEIE2TBECKQOA3WHTSMOT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PGGVXSEIE2TBECKQOA3WHTSMOT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PGGVXSEIE2TBECKQOA3WHTSMOT/action/storage_attestation","attest_author":"https://pith.science/pith/PGGVXSEIE2TBECKQOA3WHTSMOT/action/author_attestation","sign_citation":"https://pith.science/pith/PGGVXSEIE2TBECKQOA3WHTSMOT/action/citation_signature","submit_replication":"https://pith.science/pith/PGGVXSEIE2TBECKQOA3WHTSMOT/action/replication_record"}},"created_at":"2026-07-14T00:18:39.705212+00:00","updated_at":"2026-07-14T00:18:39.705212+00:00"}