{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:RSIQOLOJLCDOD6GSGEQS3EE2KL","short_pith_number":"pith:RSIQOLOJ","canonical_record":{"source":{"id":"2210.01550","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-10-04T12:22:42Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"5e916788130a05406c1f283d12b496a5d21a4a9478c12f00f04eef86b9c570c6","abstract_canon_sha256":"b913954fd37f74d9b429e5a71b0b75ce3eaaec2f53e0363d8a235782df8da460"},"schema_version":"1.0"},"canonical_sha256":"8c91072dc95886e1f8d231212d909a52ee8d8928b76064fd0bb5027d68e47581","source":{"kind":"arxiv","id":"2210.01550","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2210.01550","created_at":"2026-07-05T05:03:11Z"},{"alias_kind":"arxiv_version","alias_value":"2210.01550v1","created_at":"2026-07-05T05:03:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.01550","created_at":"2026-07-05T05:03:11Z"},{"alias_kind":"pith_short_12","alias_value":"RSIQOLOJLCDO","created_at":"2026-07-05T05:03:11Z"},{"alias_kind":"pith_short_16","alias_value":"RSIQOLOJLCDOD6GS","created_at":"2026-07-05T05:03:11Z"},{"alias_kind":"pith_short_8","alias_value":"RSIQOLOJ","created_at":"2026-07-05T05:03:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:RSIQOLOJLCDOD6GSGEQS3EE2KL","target":"record","payload":{"canonical_record":{"source":{"id":"2210.01550","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-10-04T12:22:42Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"5e916788130a05406c1f283d12b496a5d21a4a9478c12f00f04eef86b9c570c6","abstract_canon_sha256":"b913954fd37f74d9b429e5a71b0b75ce3eaaec2f53e0363d8a235782df8da460"},"schema_version":"1.0"},"canonical_sha256":"8c91072dc95886e1f8d231212d909a52ee8d8928b76064fd0bb5027d68e47581","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:03:11.937442Z","signature_b64":"5II1zQuJ7DZUZgOJrB/pAPd41fbD/BXcSNXnMmxWatkWCI0ONAMGnsrAFOTk+qGYNYwFmW16KjR7sXdpMsrBBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8c91072dc95886e1f8d231212d909a52ee8d8928b76064fd0bb5027d68e47581","last_reissued_at":"2026-07-05T05:03:11.937036Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:03:11.937036Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2210.01550","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T05:03:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TpwNjrHiFMh+MYrPekc9mC4G8vabOhYvrfy72JSLmMnXnyRf9fUKUYAm+o5rSvXomaylr4+Y88TK+OT2gkIIAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T21:02:24.141534Z"},"content_sha256":"65c1a3f045e45dbef1cc64bf3ba39b4d8727ebcc742affa9a71ba05103823b91","schema_version":"1.0","event_id":"sha256:65c1a3f045e45dbef1cc64bf3ba39b4d8727ebcc742affa9a71ba05103823b91"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:RSIQOLOJLCDOD6GSGEQS3EE2KL","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Energy loss due to defect creation in solid state detectors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"physics.ins-det","authors_text":"Kai Nordlund, Kimmo Tuominen, Matti Heikinheimo, Nader Mirabolfathi, Sebastian Sassi","submitted_at":"2022-10-04T12:22:42Z","abstract_excerpt":"The threshold displacement energy in solid state detector materials varies from several eV to ~100 eV. If a stable or long lived defect is created as a result of a nuclear recoil event, some part of the recoil energy is stored in the deformed lattice and is therefore not observable in a phonon detector. Thus, an accurate model of this effect is necessary for precise calibration of the recoil energy measurement in low threshold phonon detectors. Furthermore, the sharpness of the defect creation threshold varies between materials. For a hard material such as diamond, the sharp threshold will cau"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.01550","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/2210.01550/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T05:03:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"D69dWEXQXQ/LR7HJfLniLh1QHdHHg0VzOuPbcOSN6DLoHUTNuLKkO4aUADBHXZgIakp7l13Ohwr3sSIN9hSqBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T21:02:24.141910Z"},"content_sha256":"2a49262716be38ff46a0d0a4f048400f228d03600d6952e4f0c3eb4c67e48984","schema_version":"1.0","event_id":"sha256:2a49262716be38ff46a0d0a4f048400f228d03600d6952e4f0c3eb4c67e48984"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RSIQOLOJLCDOD6GSGEQS3EE2KL/bundle.json","state_url":"https://pith.science/pith/RSIQOLOJLCDOD6GSGEQS3EE2KL/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RSIQOLOJLCDOD6GSGEQS3EE2KL/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-04T21:02:24Z","links":{"resolver":"https://pith.science/pith/RSIQOLOJLCDOD6GSGEQS3EE2KL","bundle":"https://pith.science/pith/RSIQOLOJLCDOD6GSGEQS3EE2KL/bundle.json","state":"https://pith.science/pith/RSIQOLOJLCDOD6GSGEQS3EE2KL/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RSIQOLOJLCDOD6GSGEQS3EE2KL/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:RSIQOLOJLCDOD6GSGEQS3EE2KL","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":"b913954fd37f74d9b429e5a71b0b75ce3eaaec2f53e0363d8a235782df8da460","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-10-04T12:22:42Z","title_canon_sha256":"5e916788130a05406c1f283d12b496a5d21a4a9478c12f00f04eef86b9c570c6"},"schema_version":"1.0","source":{"id":"2210.01550","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2210.01550","created_at":"2026-07-05T05:03:11Z"},{"alias_kind":"arxiv_version","alias_value":"2210.01550v1","created_at":"2026-07-05T05:03:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.01550","created_at":"2026-07-05T05:03:11Z"},{"alias_kind":"pith_short_12","alias_value":"RSIQOLOJLCDO","created_at":"2026-07-05T05:03:11Z"},{"alias_kind":"pith_short_16","alias_value":"RSIQOLOJLCDOD6GS","created_at":"2026-07-05T05:03:11Z"},{"alias_kind":"pith_short_8","alias_value":"RSIQOLOJ","created_at":"2026-07-05T05:03:11Z"}],"graph_snapshots":[{"event_id":"sha256:2a49262716be38ff46a0d0a4f048400f228d03600d6952e4f0c3eb4c67e48984","target":"graph","created_at":"2026-07-05T05:03:11Z","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/2210.01550/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The threshold displacement energy in solid state detector materials varies from several eV to ~100 eV. If a stable or long lived defect is created as a result of a nuclear recoil event, some part of the recoil energy is stored in the deformed lattice and is therefore not observable in a phonon detector. Thus, an accurate model of this effect is necessary for precise calibration of the recoil energy measurement in low threshold phonon detectors. Furthermore, the sharpness of the defect creation threshold varies between materials. For a hard material such as diamond, the sharp threshold will cau","authors_text":"Kai Nordlund, Kimmo Tuominen, Matti Heikinheimo, Nader Mirabolfathi, Sebastian Sassi","cross_cats":["hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-10-04T12:22:42Z","title":"Energy loss due to defect creation in solid state detectors"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.01550","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":"sha256:65c1a3f045e45dbef1cc64bf3ba39b4d8727ebcc742affa9a71ba05103823b91","target":"record","created_at":"2026-07-05T05:03:11Z","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":"b913954fd37f74d9b429e5a71b0b75ce3eaaec2f53e0363d8a235782df8da460","cross_cats_sorted":["hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2022-10-04T12:22:42Z","title_canon_sha256":"5e916788130a05406c1f283d12b496a5d21a4a9478c12f00f04eef86b9c570c6"},"schema_version":"1.0","source":{"id":"2210.01550","kind":"arxiv","version":1}},"canonical_sha256":"8c91072dc95886e1f8d231212d909a52ee8d8928b76064fd0bb5027d68e47581","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8c91072dc95886e1f8d231212d909a52ee8d8928b76064fd0bb5027d68e47581","first_computed_at":"2026-07-05T05:03:11.937036Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:03:11.937036Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5II1zQuJ7DZUZgOJrB/pAPd41fbD/BXcSNXnMmxWatkWCI0ONAMGnsrAFOTk+qGYNYwFmW16KjR7sXdpMsrBBQ==","signature_status":"signed_v1","signed_at":"2026-07-05T05:03:11.937442Z","signed_message":"canonical_sha256_bytes"},"source_id":"2210.01550","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:65c1a3f045e45dbef1cc64bf3ba39b4d8727ebcc742affa9a71ba05103823b91","sha256:2a49262716be38ff46a0d0a4f048400f228d03600d6952e4f0c3eb4c67e48984"],"state_sha256":"f7d71b9f5b78b9a33008613152d573928f4dd439b42e17d1b5ff3cace81ed6f6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/HOLH9gylmCP2yyF+VQNeQKXWnqCnc2jM5/thku8IU/62irRFJ7LuiFs79a/vtiEEwoiOsb0NXNNiDawkZUKAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T21:02:24.144238Z","bundle_sha256":"e52922a20eab02e036f7c94c6f63a185fe5e22b78a58309bf548566b847213ea"}}