{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:BQWLVVTQLRZK2PNVEG23XGGWUR","short_pith_number":"pith:BQWLVVTQ","schema_version":"1.0","canonical_sha256":"0c2cbad6705c72ad3db521b5bb98d6a4749a95b296f6d408cd02b727d9bba6ff","source":{"kind":"arxiv","id":"2303.16807","version":2},"attestation_state":"computed","paper":{"title":"Development of low-threshold detectors for low-mass dark matter searches with a p-type germanium detector operated at cryogenic temperature","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.ins-det","authors_text":"Dongming Mei, Guojian Wang, Hao Mei, Kyler Kooi, Mathbar Raut, Rajendra Panth, Sanjay Bhattarai","submitted_at":"2023-03-29T15:51:13Z","abstract_excerpt":"This study investigates new technology for enhancing the sensitivity of low-mass dark matter detection by analyzing charge transport in a p-type germanium detector at 5.2 K. To achieve low-threshold detectors, precise calculations of the binding energies of dipole and cluster dipole states, as well as the cross-sections of trapping affected by the electric field, are essential. The detector was operated in two modes: depleted at 77 K before cooling to 5.2 K and cooled directly to 5.2 K with various bias voltages. Our results indicate that the second mode produces lower binding energies and sug"},"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":"2303.16807","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"physics.ins-det","submitted_at":"2023-03-29T15:51:13Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"a8e37bf9a76f84f5ed8d342df7cc11c25214fe4d749daa0d823a3f66cc62d9cd","abstract_canon_sha256":"5c50d6d73b7d7133fec9e6db475ba74c21fa2b4318f278f3d445f4a750906e6a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:27:19.606266Z","signature_b64":"/5DbBJ+llI6USfPnrWZU+GrNa5zFQGo+Mki1L1bfjK4IIlzCyAVT7Nl1Meo2Yn0Jnj28lbH0pkDHcPngeGhkDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0c2cbad6705c72ad3db521b5bb98d6a4749a95b296f6d408cd02b727d9bba6ff","last_reissued_at":"2026-07-05T06:27:19.605757Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:27:19.605757Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Development of low-threshold detectors for low-mass dark matter searches with a p-type germanium detector operated at cryogenic temperature","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.ins-det","authors_text":"Dongming Mei, Guojian Wang, Hao Mei, Kyler Kooi, Mathbar Raut, Rajendra Panth, Sanjay Bhattarai","submitted_at":"2023-03-29T15:51:13Z","abstract_excerpt":"This study investigates new technology for enhancing the sensitivity of low-mass dark matter detection by analyzing charge transport in a p-type germanium detector at 5.2 K. To achieve low-threshold detectors, precise calculations of the binding energies of dipole and cluster dipole states, as well as the cross-sections of trapping affected by the electric field, are essential. The detector was operated in two modes: depleted at 77 K before cooling to 5.2 K and cooled directly to 5.2 K with various bias voltages. Our results indicate that the second mode produces lower binding energies and sug"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2303.16807","kind":"arxiv","version":2},"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/2303.16807/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":"2303.16807","created_at":"2026-07-05T06:27:19.605816+00:00"},{"alias_kind":"arxiv_version","alias_value":"2303.16807v2","created_at":"2026-07-05T06:27:19.605816+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2303.16807","created_at":"2026-07-05T06:27:19.605816+00:00"},{"alias_kind":"pith_short_12","alias_value":"BQWLVVTQLRZK","created_at":"2026-07-05T06:27:19.605816+00:00"},{"alias_kind":"pith_short_16","alias_value":"BQWLVVTQLRZK2PNV","created_at":"2026-07-05T06:27:19.605816+00:00"},{"alias_kind":"pith_short_8","alias_value":"BQWLVVTQ","created_at":"2026-07-05T06:27:19.605816+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.01815","citing_title":"Ge-based Quantum Sensors for Low-Energy Physics","ref_index":25,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/BQWLVVTQLRZK2PNVEG23XGGWUR","json":"https://pith.science/pith/BQWLVVTQLRZK2PNVEG23XGGWUR.json","graph_json":"https://pith.science/api/pith-number/BQWLVVTQLRZK2PNVEG23XGGWUR/graph.json","events_json":"https://pith.science/api/pith-number/BQWLVVTQLRZK2PNVEG23XGGWUR/events.json","paper":"https://pith.science/paper/BQWLVVTQ"},"agent_actions":{"view_html":"https://pith.science/pith/BQWLVVTQLRZK2PNVEG23XGGWUR","download_json":"https://pith.science/pith/BQWLVVTQLRZK2PNVEG23XGGWUR.json","view_paper":"https://pith.science/paper/BQWLVVTQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2303.16807&json=true","fetch_graph":"https://pith.science/api/pith-number/BQWLVVTQLRZK2PNVEG23XGGWUR/graph.json","fetch_events":"https://pith.science/api/pith-number/BQWLVVTQLRZK2PNVEG23XGGWUR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BQWLVVTQLRZK2PNVEG23XGGWUR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BQWLVVTQLRZK2PNVEG23XGGWUR/action/storage_attestation","attest_author":"https://pith.science/pith/BQWLVVTQLRZK2PNVEG23XGGWUR/action/author_attestation","sign_citation":"https://pith.science/pith/BQWLVVTQLRZK2PNVEG23XGGWUR/action/citation_signature","submit_replication":"https://pith.science/pith/BQWLVVTQLRZK2PNVEG23XGGWUR/action/replication_record"}},"created_at":"2026-07-05T06:27:19.605816+00:00","updated_at":"2026-07-05T06:27:19.605816+00:00"}