{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:O6GKCX4UVYB2AH3S5MDHMGBD74","short_pith_number":"pith:O6GKCX4U","schema_version":"1.0","canonical_sha256":"778ca15f94ae03a01f72eb06761823ff12bd5bc4cae72697f0c1fb61385b1642","source":{"kind":"arxiv","id":"2403.01160","version":1},"attestation_state":"computed","paper":{"title":"Electron Spectroscopy using Transition-Edge Sensors","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.app-ph"],"primary_cat":"physics.ins-det","authors_text":"A. G .Shard, C. N. Thomas, D. J. Goldie, K. M. Patel, S. Withington","submitted_at":"2024-03-02T10:24:09Z","abstract_excerpt":"Transition-edge sensors (TESs) have the potential to perform electron spectroscopic measurements with far greater measurement rates and efficiencies than can be achieved using existing electron spectrometers. Existing spectrometers filter electrons by energy before detecting a narrow energy band at a time, discarding the vast majority of electrons available for measurement. In contrast, transition-edge sensors (TES) have intrinsic energy sensitivity and so do not require prior filtering to perform energy-resolved measurements. Despite this fundamental advantage, TES electron spectroscopy has n"},"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":"2403.01160","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2024-03-02T10:24:09Z","cross_cats_sorted":["physics.app-ph"],"title_canon_sha256":"00a7e981ca4f2777204911f3e09db76ab9906307bcf0e3fff75143c67c40e2de","abstract_canon_sha256":"98423f45b69d1b277192b5ffb543cc297036c7f7a9e01ad2ebaba587cd295344"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:51:43.178755Z","signature_b64":"wImLR0z8ZFVdpTDGBnrk7XFYT9zDnKwqOsvhK7pdupr23BQiCYhiMCbMv/qAkRosPxMSAOaMF4rRC4Z08klvCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"778ca15f94ae03a01f72eb06761823ff12bd5bc4cae72697f0c1fb61385b1642","last_reissued_at":"2026-07-05T07:51:43.178242Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:51:43.178242Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electron Spectroscopy using Transition-Edge Sensors","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["physics.app-ph"],"primary_cat":"physics.ins-det","authors_text":"A. G .Shard, C. N. Thomas, D. J. Goldie, K. M. Patel, S. Withington","submitted_at":"2024-03-02T10:24:09Z","abstract_excerpt":"Transition-edge sensors (TESs) have the potential to perform electron spectroscopic measurements with far greater measurement rates and efficiencies than can be achieved using existing electron spectrometers. Existing spectrometers filter electrons by energy before detecting a narrow energy band at a time, discarding the vast majority of electrons available for measurement. In contrast, transition-edge sensors (TES) have intrinsic energy sensitivity and so do not require prior filtering to perform energy-resolved measurements. Despite this fundamental advantage, TES electron spectroscopy has n"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.01160","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/2403.01160/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":"2403.01160","created_at":"2026-07-05T07:51:43.178303+00:00"},{"alias_kind":"arxiv_version","alias_value":"2403.01160v1","created_at":"2026-07-05T07:51:43.178303+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.01160","created_at":"2026-07-05T07:51:43.178303+00:00"},{"alias_kind":"pith_short_12","alias_value":"O6GKCX4UVYB2","created_at":"2026-07-05T07:51:43.178303+00:00"},{"alias_kind":"pith_short_16","alias_value":"O6GKCX4UVYB2AH3S","created_at":"2026-07-05T07:51:43.178303+00:00"},{"alias_kind":"pith_short_8","alias_value":"O6GKCX4U","created_at":"2026-07-05T07:51:43.178303+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.20324","citing_title":"Demonstration of a cryogenic, switchable electron source for low-temperature detector calibration","ref_index":21,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/O6GKCX4UVYB2AH3S5MDHMGBD74","json":"https://pith.science/pith/O6GKCX4UVYB2AH3S5MDHMGBD74.json","graph_json":"https://pith.science/api/pith-number/O6GKCX4UVYB2AH3S5MDHMGBD74/graph.json","events_json":"https://pith.science/api/pith-number/O6GKCX4UVYB2AH3S5MDHMGBD74/events.json","paper":"https://pith.science/paper/O6GKCX4U"},"agent_actions":{"view_html":"https://pith.science/pith/O6GKCX4UVYB2AH3S5MDHMGBD74","download_json":"https://pith.science/pith/O6GKCX4UVYB2AH3S5MDHMGBD74.json","view_paper":"https://pith.science/paper/O6GKCX4U","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2403.01160&json=true","fetch_graph":"https://pith.science/api/pith-number/O6GKCX4UVYB2AH3S5MDHMGBD74/graph.json","fetch_events":"https://pith.science/api/pith-number/O6GKCX4UVYB2AH3S5MDHMGBD74/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/O6GKCX4UVYB2AH3S5MDHMGBD74/action/timestamp_anchor","attest_storage":"https://pith.science/pith/O6GKCX4UVYB2AH3S5MDHMGBD74/action/storage_attestation","attest_author":"https://pith.science/pith/O6GKCX4UVYB2AH3S5MDHMGBD74/action/author_attestation","sign_citation":"https://pith.science/pith/O6GKCX4UVYB2AH3S5MDHMGBD74/action/citation_signature","submit_replication":"https://pith.science/pith/O6GKCX4UVYB2AH3S5MDHMGBD74/action/replication_record"}},"created_at":"2026-07-05T07:51:43.178303+00:00","updated_at":"2026-07-05T07:51:43.178303+00:00"}