{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:YNRRAADMTWSQYT6WBYA4MPYETT","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"4148521a5acd86edb1dacd728b695365a9432b98fe73c8a11473867ffe809539","cross_cats_sorted":["astro-ph.CO","hep-ex","physics.atom-ph","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-10-07T23:20:18Z","title_canon_sha256":"24bc8fc212c64d92f0e08fb679965de9a024aee5128b28ebe9dde12b6d1a2a10"},"schema_version":"1.0","source":{"id":"2410.05549","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2410.05549","created_at":"2026-05-20T00:00:16Z"},{"alias_kind":"arxiv_version","alias_value":"2410.05549v3","created_at":"2026-05-20T00:00:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2410.05549","created_at":"2026-05-20T00:00:16Z"},{"alias_kind":"pith_short_12","alias_value":"YNRRAADMTWSQ","created_at":"2026-05-20T00:00:16Z"},{"alias_kind":"pith_short_16","alias_value":"YNRRAADMTWSQYT6W","created_at":"2026-05-20T00:00:16Z"},{"alias_kind":"pith_short_8","alias_value":"YNRRAADM","created_at":"2026-05-20T00:00:16Z"}],"graph_snapshots":[{"event_id":"sha256:a351156fd438ad992553ac98e98ae6e9ccd9655e4a92fd8675e615e049ac3790","target":"graph","created_at":"2026-05-20T00:00:16Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2410.05549/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We propose using highly excited cyclotron states of a trapped electron to detect meV axion and dark photon dark matter, marking a significant improvement over our previous proposal and demonstration [Phys. Rev. Lett. 129, 261801]. When the axion mass matches the cyclotron frequency $\\omega_c$, the cyclotron state is resonantly excited, with a transition probability proportional to its initial quantum number, $n_c$. The sensitivity is enhanced by taking $n_c \\sim 10^6 \\left( \\frac{0.1~\\text{meV}}{\\omega_c} \\right)^2$. By optimizing key experimental parameters, we minimize the required averaging","authors_text":"Gerald Gabrielse, Harikrishnan Ramani, Peter W. Graham, Samuel S. Y. Wong, Xing Fan, Yawen Xiao","cross_cats":["astro-ph.CO","hep-ex","physics.atom-ph","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-10-07T23:20:18Z","title":"Highly Excited Electron Cyclotron for QCD Axion and Dark-Photon Detection"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.05549","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:99179e5f851bfbc78ec24a4a4d465f18d61732e7725e1ea4c1b6b2495def9c86","target":"record","created_at":"2026-05-20T00:00:16Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"4148521a5acd86edb1dacd728b695365a9432b98fe73c8a11473867ffe809539","cross_cats_sorted":["astro-ph.CO","hep-ex","physics.atom-ph","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-10-07T23:20:18Z","title_canon_sha256":"24bc8fc212c64d92f0e08fb679965de9a024aee5128b28ebe9dde12b6d1a2a10"},"schema_version":"1.0","source":{"id":"2410.05549","kind":"arxiv","version":3}},"canonical_sha256":"c36310006c9da50c4fd60e01c63f049ce0ecae3528034a55448f7c644ef36f59","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c36310006c9da50c4fd60e01c63f049ce0ecae3528034a55448f7c644ef36f59","first_computed_at":"2026-05-20T00:00:16.491043Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-20T00:00:16.491043Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"LSR+VuIBlGxCIhacySyEA88iId5EPti2eGtMl3D4y2V4rnDh52ZUE4MSU2fzgLGiFEdHPLw7PUAKFSC4qZmsCA==","signature_status":"signed_v1","signed_at":"2026-05-20T00:00:16.491885Z","signed_message":"canonical_sha256_bytes"},"source_id":"2410.05549","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:99179e5f851bfbc78ec24a4a4d465f18d61732e7725e1ea4c1b6b2495def9c86","sha256:a351156fd438ad992553ac98e98ae6e9ccd9655e4a92fd8675e615e049ac3790"],"state_sha256":"4f6928a13cbd7d2e59a20e0365f1bd8828693f01f28c2981f0df642dae9bf581"}