{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:OHZPA7K54SDANEUKMRF4JAXHUL","short_pith_number":"pith:OHZPA7K5","schema_version":"1.0","canonical_sha256":"71f2f07d5de48606928a644bc482e7a2c204fe8f18781962646caddeac25f59e","source":{"kind":"arxiv","id":"hep-ph/0506151","version":2},"attestation_state":"computed","paper":{"title":"Invisible Quarkonium Decays as a Sensitive Probe of Dark Matter","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bob McElrath","submitted_at":"2005-06-15T20:04:53Z","abstract_excerpt":"We examine in a model-independent manner the measurements that can be performed at B-factories with sensitivity to dark matter. If a singlet scalar, pseudo-scalar, or vector is present and mediates the Standard Model - dark matter interaction, it can mediate invisible decays of quarkonium states such as the $\\Upsilon$, $J/\\Psi$, and $\\eta$. Such scenarios have arisen in the context of supersymmetry, extended Higgs sectors, solutions the supersymmetric $\\mu$ problem, and extra U(1) gauge groups from grand unified theories and string theory. Existing B-factories running at the $\\Upsilon(4S)$ can"},"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":"hep-ph/0506151","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-06-15T20:04:53Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"990610c675eb0a8f72d4d315b33ac46168dfcd524fb8a2aadf8870380f641d7d","abstract_canon_sha256":"8676065096563d7c3b196c9012b13d59c7025794c3c866bbbb7e628d91d72f9c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:04.983607Z","signature_b64":"/xNaphQTSUaL5UgPPLz7R0yIHpQnm84/YEqAa2H0a7mO+QXgwryzas403+ZPD8FrUPkaJbDXN3/7lr/CebETDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"71f2f07d5de48606928a644bc482e7a2c204fe8f18781962646caddeac25f59e","last_reissued_at":"2026-05-18T01:39:04.983012Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:04.983012Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Invisible Quarkonium Decays as a Sensitive Probe of Dark Matter","license":"","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Bob McElrath","submitted_at":"2005-06-15T20:04:53Z","abstract_excerpt":"We examine in a model-independent manner the measurements that can be performed at B-factories with sensitivity to dark matter. If a singlet scalar, pseudo-scalar, or vector is present and mediates the Standard Model - dark matter interaction, it can mediate invisible decays of quarkonium states such as the $\\Upsilon$, $J/\\Psi$, and $\\eta$. Such scenarios have arisen in the context of supersymmetry, extended Higgs sectors, solutions the supersymmetric $\\mu$ problem, and extra U(1) gauge groups from grand unified theories and string theory. Existing B-factories running at the $\\Upsilon(4S)$ can"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0506151","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":"hep-ph/0506151","created_at":"2026-05-18T01:39:04.983086+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0506151v2","created_at":"2026-05-18T01:39:04.983086+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0506151","created_at":"2026-05-18T01:39:04.983086+00:00"},{"alias_kind":"pith_short_12","alias_value":"OHZPA7K54SDA","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_16","alias_value":"OHZPA7K54SDANEUK","created_at":"2026-05-18T12:25:53.335082+00:00"},{"alias_kind":"pith_short_8","alias_value":"OHZPA7K5","created_at":"2026-05-18T12:25:53.335082+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2601.00068","citing_title":"Braking protons at the EIC: from invisible meson decay to new physics searches","ref_index":37,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OHZPA7K54SDANEUKMRF4JAXHUL","json":"https://pith.science/pith/OHZPA7K54SDANEUKMRF4JAXHUL.json","graph_json":"https://pith.science/api/pith-number/OHZPA7K54SDANEUKMRF4JAXHUL/graph.json","events_json":"https://pith.science/api/pith-number/OHZPA7K54SDANEUKMRF4JAXHUL/events.json","paper":"https://pith.science/paper/OHZPA7K5"},"agent_actions":{"view_html":"https://pith.science/pith/OHZPA7K54SDANEUKMRF4JAXHUL","download_json":"https://pith.science/pith/OHZPA7K54SDANEUKMRF4JAXHUL.json","view_paper":"https://pith.science/paper/OHZPA7K5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0506151&json=true","fetch_graph":"https://pith.science/api/pith-number/OHZPA7K54SDANEUKMRF4JAXHUL/graph.json","fetch_events":"https://pith.science/api/pith-number/OHZPA7K54SDANEUKMRF4JAXHUL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OHZPA7K54SDANEUKMRF4JAXHUL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OHZPA7K54SDANEUKMRF4JAXHUL/action/storage_attestation","attest_author":"https://pith.science/pith/OHZPA7K54SDANEUKMRF4JAXHUL/action/author_attestation","sign_citation":"https://pith.science/pith/OHZPA7K54SDANEUKMRF4JAXHUL/action/citation_signature","submit_replication":"https://pith.science/pith/OHZPA7K54SDANEUKMRF4JAXHUL/action/replication_record"}},"created_at":"2026-05-18T01:39:04.983086+00:00","updated_at":"2026-05-18T01:39:04.983086+00:00"}