{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:5HWXKRRLBO6WQGI4H77H3XUWIA","short_pith_number":"pith:5HWXKRRL","schema_version":"1.0","canonical_sha256":"e9ed75462b0bbd68191c3ffe7dde964000f5d7150f9a182c267df9d4e5e484d3","source":{"kind":"arxiv","id":"2404.06627","version":1},"attestation_state":"computed","paper":{"title":"A Beehive Haloscope for High-mass Axion Dark Matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ins-det"],"primary_cat":"hep-ex","authors_text":"Chao-Lin Kuo, Matthew O. Withers","submitted_at":"2024-04-09T21:33:55Z","abstract_excerpt":"We propose a new haloscope geometry that can arbitrarily increase the resonator volume for a given target axion mass. This geometry consists of closely packed, overlapping coaxial cavities operating as a single resonator. While the resonant frequency is still determined by the dimensions of the individual \"cells,\" the strong interactions between the cells encourage the entire \"beehive\" to oscillate in phase, a phenomenon expected of tightly coupled harmonic oscillators. This synchronization behavior allows the construction of a singly connected large-volume resonator at high frequency by simpl"},"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":"2404.06627","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ex","submitted_at":"2024-04-09T21:33:55Z","cross_cats_sorted":["physics.ins-det"],"title_canon_sha256":"3000a9be194f8fc0791c18b1f748a1ab332b36875911016938f2087f5f226bcc","abstract_canon_sha256":"2dbd96c4dd15d48cc50c51ca5e280f7ad3291a14fca332a628732749b4d46eea"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:06:14.970249Z","signature_b64":"gqZDN9s+881D8YKuyJyMv0T+1ByhwS98/8QxLSRfWHQw9YD/+MzN3M9Neg6xxwzxnKPaiG2+uRJn5bNks9EgCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e9ed75462b0bbd68191c3ffe7dde964000f5d7150f9a182c267df9d4e5e484d3","last_reissued_at":"2026-07-05T08:06:14.969902Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:06:14.969902Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Beehive Haloscope for High-mass Axion Dark Matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ins-det"],"primary_cat":"hep-ex","authors_text":"Chao-Lin Kuo, Matthew O. Withers","submitted_at":"2024-04-09T21:33:55Z","abstract_excerpt":"We propose a new haloscope geometry that can arbitrarily increase the resonator volume for a given target axion mass. This geometry consists of closely packed, overlapping coaxial cavities operating as a single resonator. While the resonant frequency is still determined by the dimensions of the individual \"cells,\" the strong interactions between the cells encourage the entire \"beehive\" to oscillate in phase, a phenomenon expected of tightly coupled harmonic oscillators. This synchronization behavior allows the construction of a singly connected large-volume resonator at high frequency by simpl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.06627","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/2404.06627/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":"2404.06627","created_at":"2026-07-05T08:06:14.969956+00:00"},{"alias_kind":"arxiv_version","alias_value":"2404.06627v1","created_at":"2026-07-05T08:06:14.969956+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.06627","created_at":"2026-07-05T08:06:14.969956+00:00"},{"alias_kind":"pith_short_12","alias_value":"5HWXKRRLBO6W","created_at":"2026-07-05T08:06:14.969956+00:00"},{"alias_kind":"pith_short_16","alias_value":"5HWXKRRLBO6WQGI4","created_at":"2026-07-05T08:06:14.969956+00:00"},{"alias_kind":"pith_short_8","alias_value":"5HWXKRRL","created_at":"2026-07-05T08:06:14.969956+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2411.13776","citing_title":"Maximizing Quantum Enhancement in Axion Dark Matter Experiments","ref_index":51,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5HWXKRRLBO6WQGI4H77H3XUWIA","json":"https://pith.science/pith/5HWXKRRLBO6WQGI4H77H3XUWIA.json","graph_json":"https://pith.science/api/pith-number/5HWXKRRLBO6WQGI4H77H3XUWIA/graph.json","events_json":"https://pith.science/api/pith-number/5HWXKRRLBO6WQGI4H77H3XUWIA/events.json","paper":"https://pith.science/paper/5HWXKRRL"},"agent_actions":{"view_html":"https://pith.science/pith/5HWXKRRLBO6WQGI4H77H3XUWIA","download_json":"https://pith.science/pith/5HWXKRRLBO6WQGI4H77H3XUWIA.json","view_paper":"https://pith.science/paper/5HWXKRRL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2404.06627&json=true","fetch_graph":"https://pith.science/api/pith-number/5HWXKRRLBO6WQGI4H77H3XUWIA/graph.json","fetch_events":"https://pith.science/api/pith-number/5HWXKRRLBO6WQGI4H77H3XUWIA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5HWXKRRLBO6WQGI4H77H3XUWIA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5HWXKRRLBO6WQGI4H77H3XUWIA/action/storage_attestation","attest_author":"https://pith.science/pith/5HWXKRRLBO6WQGI4H77H3XUWIA/action/author_attestation","sign_citation":"https://pith.science/pith/5HWXKRRLBO6WQGI4H77H3XUWIA/action/citation_signature","submit_replication":"https://pith.science/pith/5HWXKRRLBO6WQGI4H77H3XUWIA/action/replication_record"}},"created_at":"2026-07-05T08:06:14.969956+00:00","updated_at":"2026-07-05T08:06:14.969956+00:00"}