{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2024:YNRRAADMTWSQYT6WBYA4MPYETT","short_pith_number":"pith:YNRRAADM","canonical_record":{"source":{"id":"2410.05549","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-10-07T23:20:18Z","cross_cats_sorted":["astro-ph.CO","hep-ex","physics.atom-ph","quant-ph"],"title_canon_sha256":"24bc8fc212c64d92f0e08fb679965de9a024aee5128b28ebe9dde12b6d1a2a10","abstract_canon_sha256":"4148521a5acd86edb1dacd728b695365a9432b98fe73c8a11473867ffe809539"},"schema_version":"1.0"},"canonical_sha256":"c36310006c9da50c4fd60e01c63f049ce0ecae3528034a55448f7c644ef36f59","source":{"kind":"arxiv","id":"2410.05549","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"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2024:YNRRAADMTWSQYT6WBYA4MPYETT","target":"record","payload":{"canonical_record":{"source":{"id":"2410.05549","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-10-07T23:20:18Z","cross_cats_sorted":["astro-ph.CO","hep-ex","physics.atom-ph","quant-ph"],"title_canon_sha256":"24bc8fc212c64d92f0e08fb679965de9a024aee5128b28ebe9dde12b6d1a2a10","abstract_canon_sha256":"4148521a5acd86edb1dacd728b695365a9432b98fe73c8a11473867ffe809539"},"schema_version":"1.0"},"canonical_sha256":"c36310006c9da50c4fd60e01c63f049ce0ecae3528034a55448f7c644ef36f59","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-20T00:00:16.491885Z","signature_b64":"LSR+VuIBlGxCIhacySyEA88iId5EPti2eGtMl3D4y2V4rnDh52ZUE4MSU2fzgLGiFEdHPLw7PUAKFSC4qZmsCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c36310006c9da50c4fd60e01c63f049ce0ecae3528034a55448f7c644ef36f59","last_reissued_at":"2026-05-20T00:00:16.491043Z","signature_status":"signed_v1","first_computed_at":"2026-05-20T00:00:16.491043Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2410.05549","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-20T00:00:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"X27GIr7GNXgAXZp9rkk65wES2P3L231kRlEtX261JYiwUTGDGb4b2n6hvZI1X6ja3dRSGVSYfu3w0sqRjlNJBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T15:36:09.516457Z"},"content_sha256":"99179e5f851bfbc78ec24a4a4d465f18d61732e7725e1ea4c1b6b2495def9c86","schema_version":"1.0","event_id":"sha256:99179e5f851bfbc78ec24a4a4d465f18d61732e7725e1ea4c1b6b2495def9c86"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2024:YNRRAADMTWSQYT6WBYA4MPYETT","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Highly Excited Electron Cyclotron for QCD Axion and Dark-Photon Detection","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["astro-ph.CO","hep-ex","physics.atom-ph","quant-ph"],"primary_cat":"hep-ph","authors_text":"Gerald Gabrielse, Harikrishnan Ramani, Peter W. Graham, Samuel S. Y. Wong, Xing Fan, Yawen Xiao","submitted_at":"2024-10-07T23:20:18Z","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"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2410.05549","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2410.05549/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-20T00:00:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NhAgY0BnFLmJ4+XwMK96++LlteHhyiKVmB0bJFKp2SabEcqpfhLi0V7qOoLOyzWfzRNz7nKlBc+QgO2ghdoiCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T15:36:09.517150Z"},"content_sha256":"a351156fd438ad992553ac98e98ae6e9ccd9655e4a92fd8675e615e049ac3790","schema_version":"1.0","event_id":"sha256:a351156fd438ad992553ac98e98ae6e9ccd9655e4a92fd8675e615e049ac3790"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YNRRAADMTWSQYT6WBYA4MPYETT/bundle.json","state_url":"https://pith.science/pith/YNRRAADMTWSQYT6WBYA4MPYETT/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YNRRAADMTWSQYT6WBYA4MPYETT/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-23T15:36:09Z","links":{"resolver":"https://pith.science/pith/YNRRAADMTWSQYT6WBYA4MPYETT","bundle":"https://pith.science/pith/YNRRAADMTWSQYT6WBYA4MPYETT/bundle.json","state":"https://pith.science/pith/YNRRAADMTWSQYT6WBYA4MPYETT/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YNRRAADMTWSQYT6WBYA4MPYETT/bundle.json"},"state":{"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"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sNSYHpAmREd7wMl08KTbCdQiKcJEiMaT/NhGIbQoXfjAPsFuL/6nwBmd/GWTGdHstX2DV3khC8C7hrDWYWk1Aw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-23T15:36:09.521003Z","bundle_sha256":"97f8121c6ed45d63b81f63455ed399fb15e41767f8da9434a6c1574e181fdb9e"}}