{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:AYMKQQG7OCXKIYHJQNV4W6WHFW","short_pith_number":"pith:AYMKQQG7","schema_version":"1.0","canonical_sha256":"0618a840df70aea460e9836bcb7ac72d90d0d460488bf9c92c6760c79af1bcb5","source":{"kind":"arxiv","id":"1611.05048","version":2},"attestation_state":"computed","paper":{"title":"$Z$ boson mediated dark matter beyond the effective theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Aaron Pierce, John Kearney, Nicholas Orlofsky","submitted_at":"2016-11-15T21:00:08Z","abstract_excerpt":"Direct detection bounds are beginning to constrain a very simple model of weakly interacting dark matter---a Majorana fermion with a coupling to the $Z$ boson. In a particularly straightforward gauge-invariant realization, this coupling is introduced via a higher-dimensional operator. While attractive in its simplicity, this model generically induces a large $\\rho$ parameter. An ultraviolet completion that avoids an overly large contribution to $\\rho$ is the singlet-doublet model. We revisit this model, focusing on the Higgs blind spot region of parameter space where spin-independent interacti"},"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":"1611.05048","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2016-11-15T21:00:08Z","cross_cats_sorted":[],"title_canon_sha256":"2ee7434359d257875c6137291994b403c878249edcb2f05eb57b90c820dd326d","abstract_canon_sha256":"6b3d204f7c29327a0f26bbbf279af86c68d2852991dbfe97ce0e12eb27aba5e4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:46:44.046652Z","signature_b64":"fFH6nG5weGI7Z7VmDrdjDDEY3outk46KybXoamPmdTdWpnIrNkkKlvoakwAAWj4vD3fMc/L4PUaKE5JMJ1WKDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0618a840df70aea460e9836bcb7ac72d90d0d460488bf9c92c6760c79af1bcb5","last_reissued_at":"2026-05-18T00:46:44.046030Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:46:44.046030Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$Z$ boson mediated dark matter beyond the effective theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Aaron Pierce, John Kearney, Nicholas Orlofsky","submitted_at":"2016-11-15T21:00:08Z","abstract_excerpt":"Direct detection bounds are beginning to constrain a very simple model of weakly interacting dark matter---a Majorana fermion with a coupling to the $Z$ boson. In a particularly straightforward gauge-invariant realization, this coupling is introduced via a higher-dimensional operator. While attractive in its simplicity, this model generically induces a large $\\rho$ parameter. An ultraviolet completion that avoids an overly large contribution to $\\rho$ is the singlet-doublet model. We revisit this model, focusing on the Higgs blind spot region of parameter space where spin-independent interacti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.05048","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":""},"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":"1611.05048","created_at":"2026-05-18T00:46:44.046128+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.05048v2","created_at":"2026-05-18T00:46:44.046128+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.05048","created_at":"2026-05-18T00:46:44.046128+00:00"},{"alias_kind":"pith_short_12","alias_value":"AYMKQQG7OCXK","created_at":"2026-05-18T12:30:07.202191+00:00"},{"alias_kind":"pith_short_16","alias_value":"AYMKQQG7OCXKIYHJ","created_at":"2026-05-18T12:30:07.202191+00:00"},{"alias_kind":"pith_short_8","alias_value":"AYMKQQG7","created_at":"2026-05-18T12:30:07.202191+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/AYMKQQG7OCXKIYHJQNV4W6WHFW","json":"https://pith.science/pith/AYMKQQG7OCXKIYHJQNV4W6WHFW.json","graph_json":"https://pith.science/api/pith-number/AYMKQQG7OCXKIYHJQNV4W6WHFW/graph.json","events_json":"https://pith.science/api/pith-number/AYMKQQG7OCXKIYHJQNV4W6WHFW/events.json","paper":"https://pith.science/paper/AYMKQQG7"},"agent_actions":{"view_html":"https://pith.science/pith/AYMKQQG7OCXKIYHJQNV4W6WHFW","download_json":"https://pith.science/pith/AYMKQQG7OCXKIYHJQNV4W6WHFW.json","view_paper":"https://pith.science/paper/AYMKQQG7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.05048&json=true","fetch_graph":"https://pith.science/api/pith-number/AYMKQQG7OCXKIYHJQNV4W6WHFW/graph.json","fetch_events":"https://pith.science/api/pith-number/AYMKQQG7OCXKIYHJQNV4W6WHFW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AYMKQQG7OCXKIYHJQNV4W6WHFW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AYMKQQG7OCXKIYHJQNV4W6WHFW/action/storage_attestation","attest_author":"https://pith.science/pith/AYMKQQG7OCXKIYHJQNV4W6WHFW/action/author_attestation","sign_citation":"https://pith.science/pith/AYMKQQG7OCXKIYHJQNV4W6WHFW/action/citation_signature","submit_replication":"https://pith.science/pith/AYMKQQG7OCXKIYHJQNV4W6WHFW/action/replication_record"}},"created_at":"2026-05-18T00:46:44.046128+00:00","updated_at":"2026-05-18T00:46:44.046128+00:00"}