{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:H33VSQITWAYQ2A4NEXFOKUBRNB","short_pith_number":"pith:H33VSQIT","schema_version":"1.0","canonical_sha256":"3ef7594113b0310d038d25cae5503168785487d1b598cac7369375c8b468f56d","source":{"kind":"arxiv","id":"1701.04131","version":3},"attestation_state":"computed","paper":{"title":"Minimal renormalizable simplified dark matter model with a pseudoscalar mediator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Jinmian Li, P. Ko, Seungwon Baek","submitted_at":"2017-01-16T01:00:46Z","abstract_excerpt":"We consider a minimal renormalizable and gauge invariant dark matter (DM) model, in which the singlet fermion DM has only axial couplings to a new pseudoscalar mediator. The mixing between the pseudoscalar mediator and the standard model (SM) Higgs boson induces the interactions between the DM and SM particles. The DM candidate in this model can provide the correct thermal relic density and evades all direct detections, while it can produce observable signals in indirect detection experiments due to its large annihilation cross section. A comparative study for DM phenomenology at the LHC is co"},"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":"1701.04131","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-01-16T01:00:46Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"599731f625f35fce3f5f3bea367ea7b0e801f3ba73250ac0adbae5d69c77faff","abstract_canon_sha256":"7f6f47051383a526722bfa764b1746075a13ca2e069ce37953ed9c075d84c545"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:46:37.959819Z","signature_b64":"+7w8/s3bsoSwWu41ijDj1FS8ZpKZAxlx+XWl/TsDQRCCVpCFm/EiFY7e9AACMH+fHltiULgdaHIu/pN92aGkBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3ef7594113b0310d038d25cae5503168785487d1b598cac7369375c8b468f56d","last_reissued_at":"2026-05-18T00:46:37.959261Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:46:37.959261Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Minimal renormalizable simplified dark matter model with a pseudoscalar mediator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Jinmian Li, P. Ko, Seungwon Baek","submitted_at":"2017-01-16T01:00:46Z","abstract_excerpt":"We consider a minimal renormalizable and gauge invariant dark matter (DM) model, in which the singlet fermion DM has only axial couplings to a new pseudoscalar mediator. The mixing between the pseudoscalar mediator and the standard model (SM) Higgs boson induces the interactions between the DM and SM particles. The DM candidate in this model can provide the correct thermal relic density and evades all direct detections, while it can produce observable signals in indirect detection experiments due to its large annihilation cross section. A comparative study for DM phenomenology at the LHC is co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1701.04131","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1701.04131","created_at":"2026-05-18T00:46:37.959364+00:00"},{"alias_kind":"arxiv_version","alias_value":"1701.04131v3","created_at":"2026-05-18T00:46:37.959364+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1701.04131","created_at":"2026-05-18T00:46:37.959364+00:00"},{"alias_kind":"pith_short_12","alias_value":"H33VSQITWAYQ","created_at":"2026-05-18T12:31:18.294218+00:00"},{"alias_kind":"pith_short_16","alias_value":"H33VSQITWAYQ2A4N","created_at":"2026-05-18T12:31:18.294218+00:00"},{"alias_kind":"pith_short_8","alias_value":"H33VSQIT","created_at":"2026-05-18T12:31:18.294218+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.07618","citing_title":"Multi Component Dark Matter in a Minimal Model","ref_index":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/H33VSQITWAYQ2A4NEXFOKUBRNB","json":"https://pith.science/pith/H33VSQITWAYQ2A4NEXFOKUBRNB.json","graph_json":"https://pith.science/api/pith-number/H33VSQITWAYQ2A4NEXFOKUBRNB/graph.json","events_json":"https://pith.science/api/pith-number/H33VSQITWAYQ2A4NEXFOKUBRNB/events.json","paper":"https://pith.science/paper/H33VSQIT"},"agent_actions":{"view_html":"https://pith.science/pith/H33VSQITWAYQ2A4NEXFOKUBRNB","download_json":"https://pith.science/pith/H33VSQITWAYQ2A4NEXFOKUBRNB.json","view_paper":"https://pith.science/paper/H33VSQIT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1701.04131&json=true","fetch_graph":"https://pith.science/api/pith-number/H33VSQITWAYQ2A4NEXFOKUBRNB/graph.json","fetch_events":"https://pith.science/api/pith-number/H33VSQITWAYQ2A4NEXFOKUBRNB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/H33VSQITWAYQ2A4NEXFOKUBRNB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/H33VSQITWAYQ2A4NEXFOKUBRNB/action/storage_attestation","attest_author":"https://pith.science/pith/H33VSQITWAYQ2A4NEXFOKUBRNB/action/author_attestation","sign_citation":"https://pith.science/pith/H33VSQITWAYQ2A4NEXFOKUBRNB/action/citation_signature","submit_replication":"https://pith.science/pith/H33VSQITWAYQ2A4NEXFOKUBRNB/action/replication_record"}},"created_at":"2026-05-18T00:46:37.959364+00:00","updated_at":"2026-05-18T00:46:37.959364+00:00"}