{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:BIQPBQHB5SDTERMIQ5UC3OYKYB","short_pith_number":"pith:BIQPBQHB","schema_version":"1.0","canonical_sha256":"0a20f0c0e1ec8732458887682dbb0ac060b8335c20a504bee083cc838bcbec19","source":{"kind":"arxiv","id":"2010.15874","version":4},"attestation_state":"computed","paper":{"title":"Effect on Dark Matter Exclusion Limits from New Silicon Photoelectric Absorption Measurements","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-ex","authors_text":"Belina von Krosigk, Blas Cabrera, Chih-Pan Wu, Chris Stanford, Daniel Jardin, Francisco Ponce, Matthew J. Wilson, Noah A. Kurinsky, Robert Calkins","submitted_at":"2020-10-29T18:28:00Z","abstract_excerpt":"Recent breakthroughs in cryogenic silicon detector technology allow for the observation of single electron-hole pairs released via particle interactions within the target material. This implies sensitivity to energy depositions as low as the smallest band gap, which is $\\sim1.2$ eV for silicon, and therefore sensitivity to eV/$c^2$-scale bosonic dark matter and to thermal dark matter at masses below 100 MeV/$c^2$. Various interaction channels that can probe the lowest currently accessible masses in direct searches are related to standard photoelectric absorption. In any of these respective dar"},"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":"2010.15874","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2020-10-29T18:28:00Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"5d8ae8cd1d53429d01b9954f2588fbdafa28d9f5fe4886b364cc72268a53b887","abstract_canon_sha256":"1d2c206eb22c09aacf1c7c3896ff7552258b56808c68d1bef3f096846e2f43f4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:14:05.470734Z","signature_b64":"H3X70eGZgXPCqUi8RVYNFx1IILV/qkvpY7add6RhQE5CQUTWnj50nm/wfiMX9Xb2OwbRBPZkUiDQXK+EMyL3AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0a20f0c0e1ec8732458887682dbb0ac060b8335c20a504bee083cc838bcbec19","last_reissued_at":"2026-07-05T03:14:05.470284Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:14:05.470284Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effect on Dark Matter Exclusion Limits from New Silicon Photoelectric Absorption Measurements","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-ex","authors_text":"Belina von Krosigk, Blas Cabrera, Chih-Pan Wu, Chris Stanford, Daniel Jardin, Francisco Ponce, Matthew J. Wilson, Noah A. Kurinsky, Robert Calkins","submitted_at":"2020-10-29T18:28:00Z","abstract_excerpt":"Recent breakthroughs in cryogenic silicon detector technology allow for the observation of single electron-hole pairs released via particle interactions within the target material. This implies sensitivity to energy depositions as low as the smallest band gap, which is $\\sim1.2$ eV for silicon, and therefore sensitivity to eV/$c^2$-scale bosonic dark matter and to thermal dark matter at masses below 100 MeV/$c^2$. Various interaction channels that can probe the lowest currently accessible masses in direct searches are related to standard photoelectric absorption. In any of these respective dar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2010.15874","kind":"arxiv","version":4},"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/2010.15874/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":"2010.15874","created_at":"2026-07-05T03:14:05.470343+00:00"},{"alias_kind":"arxiv_version","alias_value":"2010.15874v4","created_at":"2026-07-05T03:14:05.470343+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2010.15874","created_at":"2026-07-05T03:14:05.470343+00:00"},{"alias_kind":"pith_short_12","alias_value":"BIQPBQHB5SDT","created_at":"2026-07-05T03:14:05.470343+00:00"},{"alias_kind":"pith_short_16","alias_value":"BIQPBQHB5SDTERMI","created_at":"2026-07-05T03:14:05.470343+00:00"},{"alias_kind":"pith_short_8","alias_value":"BIQPBQHB","created_at":"2026-07-05T03:14:05.470343+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BIQPBQHB5SDTERMIQ5UC3OYKYB","json":"https://pith.science/pith/BIQPBQHB5SDTERMIQ5UC3OYKYB.json","graph_json":"https://pith.science/api/pith-number/BIQPBQHB5SDTERMIQ5UC3OYKYB/graph.json","events_json":"https://pith.science/api/pith-number/BIQPBQHB5SDTERMIQ5UC3OYKYB/events.json","paper":"https://pith.science/paper/BIQPBQHB"},"agent_actions":{"view_html":"https://pith.science/pith/BIQPBQHB5SDTERMIQ5UC3OYKYB","download_json":"https://pith.science/pith/BIQPBQHB5SDTERMIQ5UC3OYKYB.json","view_paper":"https://pith.science/paper/BIQPBQHB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2010.15874&json=true","fetch_graph":"https://pith.science/api/pith-number/BIQPBQHB5SDTERMIQ5UC3OYKYB/graph.json","fetch_events":"https://pith.science/api/pith-number/BIQPBQHB5SDTERMIQ5UC3OYKYB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BIQPBQHB5SDTERMIQ5UC3OYKYB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BIQPBQHB5SDTERMIQ5UC3OYKYB/action/storage_attestation","attest_author":"https://pith.science/pith/BIQPBQHB5SDTERMIQ5UC3OYKYB/action/author_attestation","sign_citation":"https://pith.science/pith/BIQPBQHB5SDTERMIQ5UC3OYKYB/action/citation_signature","submit_replication":"https://pith.science/pith/BIQPBQHB5SDTERMIQ5UC3OYKYB/action/replication_record"}},"created_at":"2026-07-05T03:14:05.470343+00:00","updated_at":"2026-07-05T03:14:05.470343+00:00"}