{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:FTQLFJGM5P2J2MYVRMYWNOHXFL","short_pith_number":"pith:FTQLFJGM","schema_version":"1.0","canonical_sha256":"2ce0b2a4ccebf49d33158b3166b8f72ad5d3c207bf3a9cde14aac2b9b84d96a3","source":{"kind":"arxiv","id":"2305.08662","version":2},"attestation_state":"computed","paper":{"title":"Precision prediction of a democratic up-family philic KSVZ axion model at the LHC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Anupam Ghosh, Partha Konar","submitted_at":"2023-05-15T14:11:57Z","abstract_excerpt":"In this work, we study the $SU(2)_L$ singlet complex scalar extended KSVZ model that, in addition to providing a natural solution to the strong-CP problem, furnishes two components of dark matter that satisfy observer relic density without fine-tuning the model's parameters. A colored vector-like quark (VLQ) is naturally present in the KSVZ axion model, providing a rich dark matter and collider phenomenology. In this extended model, scalar dark matter interacts with the Standard Model up-type quarks (up, charm, top) through VLQ. We explore the possibility of democratic Yukawa interaction of th"},"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":"2305.08662","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2023-05-15T14:11:57Z","cross_cats_sorted":[],"title_canon_sha256":"0b5b5a026eb278ade1ec6cf6f8ec7068bf34ca751cf34fe5b26ba6e7bbfd2762","abstract_canon_sha256":"2221cdf399ce3eed5ca0eb74b594281feaad5017fcedec245e846d3178a2bfa7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:55:51.808158Z","signature_b64":"bF1RZamAEu9t7omzND6GEqCIx4i+0XzFu6qz7llWYyg75LrQfNxrrQiSV61alVb+h//6jJBUlMO+W0It+pVYDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2ce0b2a4ccebf49d33158b3166b8f72ad5d3c207bf3a9cde14aac2b9b84d96a3","last_reissued_at":"2026-07-05T09:55:51.807640Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:55:51.807640Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Precision prediction of a democratic up-family philic KSVZ axion model at the LHC","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Anupam Ghosh, Partha Konar","submitted_at":"2023-05-15T14:11:57Z","abstract_excerpt":"In this work, we study the $SU(2)_L$ singlet complex scalar extended KSVZ model that, in addition to providing a natural solution to the strong-CP problem, furnishes two components of dark matter that satisfy observer relic density without fine-tuning the model's parameters. A colored vector-like quark (VLQ) is naturally present in the KSVZ axion model, providing a rich dark matter and collider phenomenology. In this extended model, scalar dark matter interacts with the Standard Model up-type quarks (up, charm, top) through VLQ. We explore the possibility of democratic Yukawa interaction of th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.08662","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/2305.08662/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":"2305.08662","created_at":"2026-07-05T09:55:51.807701+00:00"},{"alias_kind":"arxiv_version","alias_value":"2305.08662v2","created_at":"2026-07-05T09:55:51.807701+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.08662","created_at":"2026-07-05T09:55:51.807701+00:00"},{"alias_kind":"pith_short_12","alias_value":"FTQLFJGM5P2J","created_at":"2026-07-05T09:55:51.807701+00:00"},{"alias_kind":"pith_short_16","alias_value":"FTQLFJGM5P2J2MYV","created_at":"2026-07-05T09:55:51.807701+00:00"},{"alias_kind":"pith_short_8","alias_value":"FTQLFJGM","created_at":"2026-07-05T09:55:51.807701+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2603.29076","citing_title":"Probing Heavy Neutral Higgs Bosons via Single Vector-Like Bottom Quark Production at the HL-LHC","ref_index":43,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07161","citing_title":"Impact of hidden heavy Higgs channels of VLB-Quarks below 1 TeV in 2HDM","ref_index":42,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FTQLFJGM5P2J2MYVRMYWNOHXFL","json":"https://pith.science/pith/FTQLFJGM5P2J2MYVRMYWNOHXFL.json","graph_json":"https://pith.science/api/pith-number/FTQLFJGM5P2J2MYVRMYWNOHXFL/graph.json","events_json":"https://pith.science/api/pith-number/FTQLFJGM5P2J2MYVRMYWNOHXFL/events.json","paper":"https://pith.science/paper/FTQLFJGM"},"agent_actions":{"view_html":"https://pith.science/pith/FTQLFJGM5P2J2MYVRMYWNOHXFL","download_json":"https://pith.science/pith/FTQLFJGM5P2J2MYVRMYWNOHXFL.json","view_paper":"https://pith.science/paper/FTQLFJGM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2305.08662&json=true","fetch_graph":"https://pith.science/api/pith-number/FTQLFJGM5P2J2MYVRMYWNOHXFL/graph.json","fetch_events":"https://pith.science/api/pith-number/FTQLFJGM5P2J2MYVRMYWNOHXFL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FTQLFJGM5P2J2MYVRMYWNOHXFL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FTQLFJGM5P2J2MYVRMYWNOHXFL/action/storage_attestation","attest_author":"https://pith.science/pith/FTQLFJGM5P2J2MYVRMYWNOHXFL/action/author_attestation","sign_citation":"https://pith.science/pith/FTQLFJGM5P2J2MYVRMYWNOHXFL/action/citation_signature","submit_replication":"https://pith.science/pith/FTQLFJGM5P2J2MYVRMYWNOHXFL/action/replication_record"}},"created_at":"2026-07-05T09:55:51.807701+00:00","updated_at":"2026-07-05T09:55:51.807701+00:00"}