{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2021:2FS4WXUD32JUHAY6LN24LYS5R4","short_pith_number":"pith:2FS4WXUD","canonical_record":{"source":{"id":"2109.11487","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2021-09-23T16:39:51Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"19da4d403729233c091c766b1753239c306d4472c96d6f28301e5d9271ac44fe","abstract_canon_sha256":"877cbe799106889475c7661bc8a1ce0a4eaac7e728bdeb97ea666c707e41657a"},"schema_version":"1.0"},"canonical_sha256":"d165cb5e83de9343831e5b75c5e25d8f21210a696199be3476175e7c3225a41a","source":{"kind":"arxiv","id":"2109.11487","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2109.11487","created_at":"2026-07-05T03:40:47Z"},{"alias_kind":"arxiv_version","alias_value":"2109.11487v2","created_at":"2026-07-05T03:40:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2109.11487","created_at":"2026-07-05T03:40:47Z"},{"alias_kind":"pith_short_12","alias_value":"2FS4WXUD32JU","created_at":"2026-07-05T03:40:47Z"},{"alias_kind":"pith_short_16","alias_value":"2FS4WXUD32JUHAY6","created_at":"2026-07-05T03:40:47Z"},{"alias_kind":"pith_short_8","alias_value":"2FS4WXUD","created_at":"2026-07-05T03:40:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2021:2FS4WXUD32JUHAY6LN24LYS5R4","target":"record","payload":{"canonical_record":{"source":{"id":"2109.11487","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2021-09-23T16:39:51Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"19da4d403729233c091c766b1753239c306d4472c96d6f28301e5d9271ac44fe","abstract_canon_sha256":"877cbe799106889475c7661bc8a1ce0a4eaac7e728bdeb97ea666c707e41657a"},"schema_version":"1.0"},"canonical_sha256":"d165cb5e83de9343831e5b75c5e25d8f21210a696199be3476175e7c3225a41a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:40:47.403766Z","signature_b64":"NtqsWyqcqgwMSwlBYaMrnh+yfHR0u2oDUKi3ip6Ry4ciTE0Z/3bvDEhRn2/mCUlih+10Pm43OAYMSy9jDB2ABQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d165cb5e83de9343831e5b75c5e25d8f21210a696199be3476175e7c3225a41a","last_reissued_at":"2026-07-05T03:40:47.403280Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:40:47.403280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2109.11487","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T03:40:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fJB3bpo43uExuUo53msZozCSnqWG+hq9IQtmmD8OidAvMszkPEQGGGaUfhGawi6fvYDUR1eGW7w56CN9qS9BCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T14:24:10.288913Z"},"content_sha256":"f8fe8f164e6ea2031deec3623b16383f485dde192a26606b09c26bda17affc28","schema_version":"1.0","event_id":"sha256:f8fe8f164e6ea2031deec3623b16383f485dde192a26606b09c26bda17affc28"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2021:2FS4WXUD32JUHAY6LN24LYS5R4","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Measurement of Charge and Light Yields for $^{127}$Xe L-Shell Electron Captures in Liquid Xenon","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"physics.ins-det","authors_text":"Alissa Monte, Amy Cottle, C Eric Dahl, Daniel Baxter, Dylan J Temples, Jack Bargemann, Jacob McLaughlin, Jason Phelan, W Hugh Lippincott","submitted_at":"2021-09-23T16:39:51Z","abstract_excerpt":"Dark matter searches using dual-phase xenon time-projection chambers (LXe-TPCs) rely on their ability to reject background electron recoils (ERs) while searching for signal-like nuclear recoils (NRs). ER response is typically calibrated using $\\beta$-decay sources, such as tritium, but these calibrations do not characterize events accompanied by an atomic vacancy, as in solar neutrino scatters off inner shell electrons. Such events lead to emission of X-rays and Auger electrons, resulting in higher electron-ion recombination and thus a more NR-like response than inferred from $\\beta$-decay cal"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2109.11487","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/2109.11487/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":"2026-07-05T03:40:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"msRBsLEtaH6t/bqK/vImJASkDiADyYVAU3b8pUKHG0078Ep6uCTPZGMnf3ULBba5C6FIsFf19o02Qje5TfqXBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T14:24:10.289453Z"},"content_sha256":"3fc886fd1ede63bf87ea27f0a47a8db0c217ac121f4003dc1aaf9781d3332df9","schema_version":"1.0","event_id":"sha256:3fc886fd1ede63bf87ea27f0a47a8db0c217ac121f4003dc1aaf9781d3332df9"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2FS4WXUD32JUHAY6LN24LYS5R4/bundle.json","state_url":"https://pith.science/pith/2FS4WXUD32JUHAY6LN24LYS5R4/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2FS4WXUD32JUHAY6LN24LYS5R4/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":"2026-08-04T14:24:10Z","links":{"resolver":"https://pith.science/pith/2FS4WXUD32JUHAY6LN24LYS5R4","bundle":"https://pith.science/pith/2FS4WXUD32JUHAY6LN24LYS5R4/bundle.json","state":"https://pith.science/pith/2FS4WXUD32JUHAY6LN24LYS5R4/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2FS4WXUD32JUHAY6LN24LYS5R4/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:2FS4WXUD32JUHAY6LN24LYS5R4","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":"877cbe799106889475c7661bc8a1ce0a4eaac7e728bdeb97ea666c707e41657a","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2021-09-23T16:39:51Z","title_canon_sha256":"19da4d403729233c091c766b1753239c306d4472c96d6f28301e5d9271ac44fe"},"schema_version":"1.0","source":{"id":"2109.11487","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2109.11487","created_at":"2026-07-05T03:40:47Z"},{"alias_kind":"arxiv_version","alias_value":"2109.11487v2","created_at":"2026-07-05T03:40:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2109.11487","created_at":"2026-07-05T03:40:47Z"},{"alias_kind":"pith_short_12","alias_value":"2FS4WXUD32JU","created_at":"2026-07-05T03:40:47Z"},{"alias_kind":"pith_short_16","alias_value":"2FS4WXUD32JUHAY6","created_at":"2026-07-05T03:40:47Z"},{"alias_kind":"pith_short_8","alias_value":"2FS4WXUD","created_at":"2026-07-05T03:40:47Z"}],"graph_snapshots":[{"event_id":"sha256:3fc886fd1ede63bf87ea27f0a47a8db0c217ac121f4003dc1aaf9781d3332df9","target":"graph","created_at":"2026-07-05T03:40:47Z","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/2109.11487/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Dark matter searches using dual-phase xenon time-projection chambers (LXe-TPCs) rely on their ability to reject background electron recoils (ERs) while searching for signal-like nuclear recoils (NRs). ER response is typically calibrated using $\\beta$-decay sources, such as tritium, but these calibrations do not characterize events accompanied by an atomic vacancy, as in solar neutrino scatters off inner shell electrons. Such events lead to emission of X-rays and Auger electrons, resulting in higher electron-ion recombination and thus a more NR-like response than inferred from $\\beta$-decay cal","authors_text":"Alissa Monte, Amy Cottle, C Eric Dahl, Daniel Baxter, Dylan J Temples, Jack Bargemann, Jacob McLaughlin, Jason Phelan, W Hugh Lippincott","cross_cats":["hep-ex"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2021-09-23T16:39:51Z","title":"Measurement of Charge and Light Yields for $^{127}$Xe L-Shell Electron Captures in Liquid Xenon"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2109.11487","kind":"arxiv","version":2},"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:f8fe8f164e6ea2031deec3623b16383f485dde192a26606b09c26bda17affc28","target":"record","created_at":"2026-07-05T03:40:47Z","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":"877cbe799106889475c7661bc8a1ce0a4eaac7e728bdeb97ea666c707e41657a","cross_cats_sorted":["hep-ex"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.ins-det","submitted_at":"2021-09-23T16:39:51Z","title_canon_sha256":"19da4d403729233c091c766b1753239c306d4472c96d6f28301e5d9271ac44fe"},"schema_version":"1.0","source":{"id":"2109.11487","kind":"arxiv","version":2}},"canonical_sha256":"d165cb5e83de9343831e5b75c5e25d8f21210a696199be3476175e7c3225a41a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d165cb5e83de9343831e5b75c5e25d8f21210a696199be3476175e7c3225a41a","first_computed_at":"2026-07-05T03:40:47.403280Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:40:47.403280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NtqsWyqcqgwMSwlBYaMrnh+yfHR0u2oDUKi3ip6Ry4ciTE0Z/3bvDEhRn2/mCUlih+10Pm43OAYMSy9jDB2ABQ==","signature_status":"signed_v1","signed_at":"2026-07-05T03:40:47.403766Z","signed_message":"canonical_sha256_bytes"},"source_id":"2109.11487","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f8fe8f164e6ea2031deec3623b16383f485dde192a26606b09c26bda17affc28","sha256:3fc886fd1ede63bf87ea27f0a47a8db0c217ac121f4003dc1aaf9781d3332df9"],"state_sha256":"852db3152699db7d263893f8ecf865a5110ed30f9602ae4370011a871787e889"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hDL3aaBmdUNv114Ee4c7kasw8pdErPm1OmW2dUkiI1H800r4WdigeYdZYomymllKkd66BQBxXJd8XlCZZSGYBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T14:24:10.293924Z","bundle_sha256":"de7db9ca7ea7a152b545826922c6738decfc456eecacdca1301e6b9b9dd2fa94"}}