{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:AQIFRJX3V3LORKAGZVYVSIDH4W","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":"02e3c5d3be6563d2658157389588eeaaf7ed4320f2c01f60283b208fa2d0a416","cross_cats_sorted":["cond-mat.mes-hall","hep-ex","physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-05-30T18:00:01Z","title_canon_sha256":"c9ca8449157d02327d95dfc3cffabdca10cd04bcff4d24278666990c40ee3b0d"},"schema_version":"1.0","source":{"id":"2506.00115","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2506.00115","created_at":"2026-07-05T11:27:13Z"},{"alias_kind":"arxiv_version","alias_value":"2506.00115v1","created_at":"2026-07-05T11:27:13Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2506.00115","created_at":"2026-07-05T11:27:13Z"},{"alias_kind":"pith_short_12","alias_value":"AQIFRJX3V3LO","created_at":"2026-07-05T11:27:13Z"},{"alias_kind":"pith_short_16","alias_value":"AQIFRJX3V3LORKAG","created_at":"2026-07-05T11:27:13Z"},{"alias_kind":"pith_short_8","alias_value":"AQIFRJX3","created_at":"2026-07-05T11:27:13Z"}],"graph_snapshots":[{"event_id":"sha256:1be068fe0acf671daef0628626eb9375ce4240981ec9f5b73beed4751a226feb","target":"graph","created_at":"2026-07-05T11:27:13Z","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/2506.00115/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Light dark matter candidates such as axions and dark photons generically couple to electromagnetism, yielding dark-matter-to-photon conversion as a key search strategy. In addition to resonant conversion in cavities and circuits, light dark matter bosons efficiently convert to photons on material interfaces, with a broadband power proportional to the total area of these interfaces. In this work, we make use of interface conversion to develop a new experimental dark matter detector design: the disordered dielectric detector. We show that a volume filled with dielectric powder is an efficient, r","authors_text":"Dip Joti Paul, Junwu Huang, Karl K. Berggren, Masha Baryakhtar, Otavio D. A. R. Bittencourt, Stewart Koppell","cross_cats":["cond-mat.mes-hall","hep-ex","physics.ins-det"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-05-30T18:00:01Z","title":"Dark Matter Haloscope with a Disordered Dielectric Absorber"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2506.00115","kind":"arxiv","version":1},"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:f11568d30af3ca57b1bbdc03e8d55d74487b08665f17c2f0f3d7edd611d14fc6","target":"record","created_at":"2026-07-05T11:27:13Z","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":"02e3c5d3be6563d2658157389588eeaaf7ed4320f2c01f60283b208fa2d0a416","cross_cats_sorted":["cond-mat.mes-hall","hep-ex","physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-05-30T18:00:01Z","title_canon_sha256":"c9ca8449157d02327d95dfc3cffabdca10cd04bcff4d24278666990c40ee3b0d"},"schema_version":"1.0","source":{"id":"2506.00115","kind":"arxiv","version":1}},"canonical_sha256":"041058a6fbaed6e8a806cd71592067e592872844c7f33f889d94f880fb2dc48b","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"041058a6fbaed6e8a806cd71592067e592872844c7f33f889d94f880fb2dc48b","first_computed_at":"2026-07-05T11:27:13.989058Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:27:13.989058Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"9ei8Sh2X5ttJ2rJs0Q+K0BdCeoYoyUDRIVz1l9+WqCjzl+G6PZFtlzxR6I66wzsBwDyEL7djVPAqJCqiO51qAw==","signature_status":"signed_v1","signed_at":"2026-07-05T11:27:13.989548Z","signed_message":"canonical_sha256_bytes"},"source_id":"2506.00115","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f11568d30af3ca57b1bbdc03e8d55d74487b08665f17c2f0f3d7edd611d14fc6","sha256:1be068fe0acf671daef0628626eb9375ce4240981ec9f5b73beed4751a226feb"],"state_sha256":"1bc077669dd9d512f22bb96f39eabd54669d358209b737005353adca0abb22ff"}