{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:5AD3VWUGNFR7NXGXZRX75QWUON","short_pith_number":"pith:5AD3VWUG","schema_version":"1.0","canonical_sha256":"e807bada866963f6dcd7cc6ffec2d47378945aa00f1b1cb5f715c0302eb0cb52","source":{"kind":"arxiv","id":"2408.11158","version":3},"attestation_state":"computed","paper":{"title":"A Transition Edge Sensor Operated in Coincidence with a High Sensitivity Athermal Phonon Sensor for Photon Coupled Rare Event Searches","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"Bernard Sadoulet, Bruno Serfass, Ivar Rydstrom, Maggie Reed, Mark Platt, Matt Pyle, Roger K. Romani, Rupak Mahapatra, Yen-Yung Chang","submitted_at":"2024-08-20T19:28:14Z","abstract_excerpt":"Experimental searches for axions or dark photons that couple to the standard model photon require photosensors with low noise, broadband sensitivity, and near zero backgrounds. Here, we introduce an experimental architecture, in which a small photon sensor, in our case a Transition Edge Sensor (TES) with a photon energy resolution $\\sigma_\\gamma = 368.4 \\pm 0.4$ meV, is colocated on the same substrate as a large high sensitivity athermal phonon sensor (APS) with a phonon energy resolution $\\sigma_\\mathrm{phonon} = 701 \\pm 2$ meV. We show that single 3.061 eV photons absorbed in the photon-sens"},"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":"2408.11158","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2024-08-20T19:28:14Z","cross_cats_sorted":[],"title_canon_sha256":"99693c5ae0dcf24d7ddc6e96b79ae8a5adba06154686134b4ede8fd107e15a8f","abstract_canon_sha256":"6af3f6a9e52fc0f9742f754e4d10880fab9537ffb6b21a86b2af753d8ca5d75d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:11:34.230437Z","signature_b64":"KlaZn5mfUxd7374rSHrlBH64oVTbXkjBqctHminTHxHV4ham7fYrX8MxxjDPdNTj5ysgX1Nu6p8dkMMgUkGHAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e807bada866963f6dcd7cc6ffec2d47378945aa00f1b1cb5f715c0302eb0cb52","last_reissued_at":"2026-07-05T11:11:34.229867Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:11:34.229867Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A Transition Edge Sensor Operated in Coincidence with a High Sensitivity Athermal Phonon Sensor for Photon Coupled Rare Event Searches","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.ins-det","authors_text":"Bernard Sadoulet, Bruno Serfass, Ivar Rydstrom, Maggie Reed, Mark Platt, Matt Pyle, Roger K. Romani, Rupak Mahapatra, Yen-Yung Chang","submitted_at":"2024-08-20T19:28:14Z","abstract_excerpt":"Experimental searches for axions or dark photons that couple to the standard model photon require photosensors with low noise, broadband sensitivity, and near zero backgrounds. Here, we introduce an experimental architecture, in which a small photon sensor, in our case a Transition Edge Sensor (TES) with a photon energy resolution $\\sigma_\\gamma = 368.4 \\pm 0.4$ meV, is colocated on the same substrate as a large high sensitivity athermal phonon sensor (APS) with a phonon energy resolution $\\sigma_\\mathrm{phonon} = 701 \\pm 2$ meV. We show that single 3.061 eV photons absorbed in the photon-sens"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.11158","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/2408.11158/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":"2408.11158","created_at":"2026-07-05T11:11:34.229933+00:00"},{"alias_kind":"arxiv_version","alias_value":"2408.11158v3","created_at":"2026-07-05T11:11:34.229933+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.11158","created_at":"2026-07-05T11:11:34.229933+00:00"},{"alias_kind":"pith_short_12","alias_value":"5AD3VWUGNFR7","created_at":"2026-07-05T11:11:34.229933+00:00"},{"alias_kind":"pith_short_16","alias_value":"5AD3VWUGNFR7NXGX","created_at":"2026-07-05T11:11:34.229933+00:00"},{"alias_kind":"pith_short_8","alias_value":"5AD3VWUG","created_at":"2026-07-05T11:11:34.229933+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.07423","citing_title":"Characterization of a Two-Channel Optical and Near-infrared Transition Edge Sensor System for Rare-Event Searches","ref_index":15,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5AD3VWUGNFR7NXGXZRX75QWUON","json":"https://pith.science/pith/5AD3VWUGNFR7NXGXZRX75QWUON.json","graph_json":"https://pith.science/api/pith-number/5AD3VWUGNFR7NXGXZRX75QWUON/graph.json","events_json":"https://pith.science/api/pith-number/5AD3VWUGNFR7NXGXZRX75QWUON/events.json","paper":"https://pith.science/paper/5AD3VWUG"},"agent_actions":{"view_html":"https://pith.science/pith/5AD3VWUGNFR7NXGXZRX75QWUON","download_json":"https://pith.science/pith/5AD3VWUGNFR7NXGXZRX75QWUON.json","view_paper":"https://pith.science/paper/5AD3VWUG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2408.11158&json=true","fetch_graph":"https://pith.science/api/pith-number/5AD3VWUGNFR7NXGXZRX75QWUON/graph.json","fetch_events":"https://pith.science/api/pith-number/5AD3VWUGNFR7NXGXZRX75QWUON/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5AD3VWUGNFR7NXGXZRX75QWUON/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5AD3VWUGNFR7NXGXZRX75QWUON/action/storage_attestation","attest_author":"https://pith.science/pith/5AD3VWUGNFR7NXGXZRX75QWUON/action/author_attestation","sign_citation":"https://pith.science/pith/5AD3VWUGNFR7NXGXZRX75QWUON/action/citation_signature","submit_replication":"https://pith.science/pith/5AD3VWUGNFR7NXGXZRX75QWUON/action/replication_record"}},"created_at":"2026-07-05T11:11:34.229933+00:00","updated_at":"2026-07-05T11:11:34.229933+00:00"}