{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:YR4IBKESEZ7MLWENMC2VUJFXLR","short_pith_number":"pith:YR4IBKES","canonical_record":{"source":{"id":"1602.08005","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-02-25T17:27:29Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"f30fd590e8b58f5e33f04b83f7983d912b6788910b3b977169b991fdde5afe93","abstract_canon_sha256":"8bf890fcb53ca90b3f47f70bacb11fff5b9ae3619db8ae96f9a04936f38f6d63"},"schema_version":"1.0"},"canonical_sha256":"c47880a892267ec5d88d60b55a24b75c606a5aa583501f6d59f5a353ef9ab185","source":{"kind":"arxiv","id":"1602.08005","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.08005","created_at":"2026-05-18T00:44:01Z"},{"alias_kind":"arxiv_version","alias_value":"1602.08005v4","created_at":"2026-05-18T00:44:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.08005","created_at":"2026-05-18T00:44:01Z"},{"alias_kind":"pith_short_12","alias_value":"YR4IBKESEZ7M","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"YR4IBKESEZ7MLWEN","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"YR4IBKES","created_at":"2026-05-18T12:30:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:YR4IBKESEZ7MLWENMC2VUJFXLR","target":"record","payload":{"canonical_record":{"source":{"id":"1602.08005","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-02-25T17:27:29Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"f30fd590e8b58f5e33f04b83f7983d912b6788910b3b977169b991fdde5afe93","abstract_canon_sha256":"8bf890fcb53ca90b3f47f70bacb11fff5b9ae3619db8ae96f9a04936f38f6d63"},"schema_version":"1.0"},"canonical_sha256":"c47880a892267ec5d88d60b55a24b75c606a5aa583501f6d59f5a353ef9ab185","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:44:01.554747Z","signature_b64":"vCuYDZX3ytH+/QCmN5z+oBNWABV/4YKZJtK9x4HtqoZyNpT4ZuzYYzGTPw9r/8MjKzI8wZk1/ad0ITSKglZiDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c47880a892267ec5d88d60b55a24b75c606a5aa583501f6d59f5a353ef9ab185","last_reissued_at":"2026-05-18T00:44:01.554115Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:44:01.554115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1602.08005","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:44:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bPzyrB1sNaiSfq4siaBAIbYnFl5+FE2Ap9T6rRHfwiBp9qe7KMq+1fJNdsCT/SktGI7QJfDHGtgCqN/joxYWDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T19:46:53.133778Z"},"content_sha256":"a07df7086c60094ec03729dc289548d7993d80d910a5dbd1b4b8e428228c708b","schema_version":"1.0","event_id":"sha256:a07df7086c60094ec03729dc289548d7993d80d910a5dbd1b4b8e428228c708b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:YR4IBKESEZ7MLWENMC2VUJFXLR","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Average Energy Expended Per e-h Pair and Energy Scale Function for Germanium-Based Dark Matter Experiments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.ins-det","authors_text":"D.-M. Mei, L. Wang, W.-Z. Wei","submitted_at":"2016-02-25T17:27:29Z","abstract_excerpt":"We report a new result of the temperature-dependent average energy expended per electron-hole (e-h) pair, $\\varepsilon$, for germanium detectors. Applying energy partition mechanism in ionization for a given energy deposition, the Fano factor and the value of $\\varepsilon$ can be determined separately. Subsequently, we illustrate the variation of $\\varepsilon$ as a function of temperature. The impact of $\\varepsilon$ on the energy threshold and energy scale for germanium detectors at a given temperature is evaluated. We demonstrate an absolute energy scale function of low-energy recoils for ge"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.08005","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":""},"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":"2026-05-18T00:44:01Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dVPur++bT0Hn0GBDQHcIvDDOUE8knoKpH3Nyd2OMyAC6rLRxQIlzyjc/e1JIgx+HPvFQAnJOvAYWBLXe1IqLCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T19:46:53.134125Z"},"content_sha256":"5761b84349a822785b1b89e5e14743d2b409a8f485701b86b2f8ad4851409c81","schema_version":"1.0","event_id":"sha256:5761b84349a822785b1b89e5e14743d2b409a8f485701b86b2f8ad4851409c81"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YR4IBKESEZ7MLWENMC2VUJFXLR/bundle.json","state_url":"https://pith.science/pith/YR4IBKESEZ7MLWENMC2VUJFXLR/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YR4IBKESEZ7MLWENMC2VUJFXLR/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":"2026-06-02T19:46:53Z","links":{"resolver":"https://pith.science/pith/YR4IBKESEZ7MLWENMC2VUJFXLR","bundle":"https://pith.science/pith/YR4IBKESEZ7MLWENMC2VUJFXLR/bundle.json","state":"https://pith.science/pith/YR4IBKESEZ7MLWENMC2VUJFXLR/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YR4IBKESEZ7MLWENMC2VUJFXLR/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:YR4IBKESEZ7MLWENMC2VUJFXLR","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":"8bf890fcb53ca90b3f47f70bacb11fff5b9ae3619db8ae96f9a04936f38f6d63","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-02-25T17:27:29Z","title_canon_sha256":"f30fd590e8b58f5e33f04b83f7983d912b6788910b3b977169b991fdde5afe93"},"schema_version":"1.0","source":{"id":"1602.08005","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.08005","created_at":"2026-05-18T00:44:01Z"},{"alias_kind":"arxiv_version","alias_value":"1602.08005v4","created_at":"2026-05-18T00:44:01Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.08005","created_at":"2026-05-18T00:44:01Z"},{"alias_kind":"pith_short_12","alias_value":"YR4IBKESEZ7M","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_16","alias_value":"YR4IBKESEZ7MLWEN","created_at":"2026-05-18T12:30:53Z"},{"alias_kind":"pith_short_8","alias_value":"YR4IBKES","created_at":"2026-05-18T12:30:53Z"}],"graph_snapshots":[{"event_id":"sha256:5761b84349a822785b1b89e5e14743d2b409a8f485701b86b2f8ad4851409c81","target":"graph","created_at":"2026-05-18T00:44:01Z","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"},"paper":{"abstract_excerpt":"We report a new result of the temperature-dependent average energy expended per electron-hole (e-h) pair, $\\varepsilon$, for germanium detectors. Applying energy partition mechanism in ionization for a given energy deposition, the Fano factor and the value of $\\varepsilon$ can be determined separately. Subsequently, we illustrate the variation of $\\varepsilon$ as a function of temperature. The impact of $\\varepsilon$ on the energy threshold and energy scale for germanium detectors at a given temperature is evaluated. We demonstrate an absolute energy scale function of low-energy recoils for ge","authors_text":"D.-M. Mei, L. Wang, W.-Z. Wei","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-02-25T17:27:29Z","title":"Average Energy Expended Per e-h Pair and Energy Scale Function for Germanium-Based Dark Matter Experiments"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.08005","kind":"arxiv","version":4},"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:a07df7086c60094ec03729dc289548d7993d80d910a5dbd1b4b8e428228c708b","target":"record","created_at":"2026-05-18T00:44:01Z","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":"8bf890fcb53ca90b3f47f70bacb11fff5b9ae3619db8ae96f9a04936f38f6d63","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2016-02-25T17:27:29Z","title_canon_sha256":"f30fd590e8b58f5e33f04b83f7983d912b6788910b3b977169b991fdde5afe93"},"schema_version":"1.0","source":{"id":"1602.08005","kind":"arxiv","version":4}},"canonical_sha256":"c47880a892267ec5d88d60b55a24b75c606a5aa583501f6d59f5a353ef9ab185","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c47880a892267ec5d88d60b55a24b75c606a5aa583501f6d59f5a353ef9ab185","first_computed_at":"2026-05-18T00:44:01.554115Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:44:01.554115Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vCuYDZX3ytH+/QCmN5z+oBNWABV/4YKZJtK9x4HtqoZyNpT4ZuzYYzGTPw9r/8MjKzI8wZk1/ad0ITSKglZiDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:44:01.554747Z","signed_message":"canonical_sha256_bytes"},"source_id":"1602.08005","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a07df7086c60094ec03729dc289548d7993d80d910a5dbd1b4b8e428228c708b","sha256:5761b84349a822785b1b89e5e14743d2b409a8f485701b86b2f8ad4851409c81"],"state_sha256":"e3a91be21554a3e786a6a66dc948e1b5a66cceef6d74c84238fb417f51fb3709"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yMvCdrvrA4gZDrJbZSgk4ZzeElN5/+kykkurKXsn88g8BNm/GOAtCsfUrnO5GGCKnE8h8ACzbkVxFWx3DG6qCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T19:46:53.136847Z","bundle_sha256":"06e5af5ff933fd91424df3b31f7583c0124f11b06db411da22e32e6828f033a8"}}