{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:3K2TQJ7NP3JVTIWR63SA4725FB","short_pith_number":"pith:3K2TQJ7N","canonical_record":{"source":{"id":"1709.09415","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2017-09-27T09:43:34Z","cross_cats_sorted":["physics.ins-det"],"title_canon_sha256":"efadeea903b9daa6ec75e11a3ac7bf70fd7209c61ef6d232ebc507a7f3a2d1a6","abstract_canon_sha256":"6d52047b6ca918cebcd001351bb20780dafdf71d9d2f9acbe8e1592744396d6e"},"schema_version":"1.0"},"canonical_sha256":"dab53827ed7ed359a2d1f6e40e7f5d285565f2c681701ec233c3fdbca6ced953","source":{"kind":"arxiv","id":"1709.09415","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.09415","created_at":"2026-05-18T00:27:43Z"},{"alias_kind":"arxiv_version","alias_value":"1709.09415v1","created_at":"2026-05-18T00:27:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.09415","created_at":"2026-05-18T00:27:43Z"},{"alias_kind":"pith_short_12","alias_value":"3K2TQJ7NP3JV","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"3K2TQJ7NP3JVTIWR","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"3K2TQJ7N","created_at":"2026-05-18T12:30:58Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:3K2TQJ7NP3JVTIWR63SA4725FB","target":"record","payload":{"canonical_record":{"source":{"id":"1709.09415","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2017-09-27T09:43:34Z","cross_cats_sorted":["physics.ins-det"],"title_canon_sha256":"efadeea903b9daa6ec75e11a3ac7bf70fd7209c61ef6d232ebc507a7f3a2d1a6","abstract_canon_sha256":"6d52047b6ca918cebcd001351bb20780dafdf71d9d2f9acbe8e1592744396d6e"},"schema_version":"1.0"},"canonical_sha256":"dab53827ed7ed359a2d1f6e40e7f5d285565f2c681701ec233c3fdbca6ced953","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:27:43.056711Z","signature_b64":"2fncdoBQNawX2w6YeXB2Hi5Vn6GjMTGBHhxxUHoi5OF55S1/utOESkSOLU/4taJKy3vAlqW6G1D+Sn/RNHA8DA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dab53827ed7ed359a2d1f6e40e7f5d285565f2c681701ec233c3fdbca6ced953","last_reissued_at":"2026-05-18T00:27:43.056105Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:27:43.056105Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1709.09415","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":"2026-05-18T00:27:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Kp3GW64l4+XkaoYlbeAGSCgK653rgajUrod0A5dJcTSsLsSITR3/y/vo+q+N4k2362f7AOACqnLdfDZ7ZnEdDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T05:35:18.350410Z"},"content_sha256":"b928a3fad2c1dc9277295a02b1b03be775dbaa014c1ecdd08f661454c8e2a912","schema_version":"1.0","event_id":"sha256:b928a3fad2c1dc9277295a02b1b03be775dbaa014c1ecdd08f661454c8e2a912"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:3K2TQJ7NP3JVTIWR63SA4725FB","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"High Precision Measurement of the $^{19}$Ne Half-life using real-time digital acquisition","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.ins-det"],"primary_cat":"nucl-ex","authors_text":"A. Jevremovi\\'c, A. M. S\\'anchez-Ben\\'itez, B. Bastin, B. Blank, B. Carniol, C. Borcea, C. Fontbonne, C. Spitaels, D. Etasse, D. Ramos, D. Toprek, F. Boulay, F. Delaunay, F. de Oliveira Santos, F. Rotaru, G. de France, G.F. Grinyer, G. Fremont, H. Bouzomita, I. Martel, I. \\v{C}elikovi\\'c, J. B. Briand, J. C. Thomas, J. Harang, J. Hommet, J. M. Fontbonne, J. Mrazek, J. Poincheval, M. Lewitowicz, M. Parlog, M. Stanoiu, N. L. Achouri, P. Delahaye, P. Uji\\'c, R. Borcea, V. Girard Alcindor, X. Fl\\'echard","submitted_at":"2017-09-27T09:43:34Z","abstract_excerpt":"The half-life of $^{19}$Ne has been measured using a real-time digital multiparametric acquisition system providing an accurate time-stamp and relevant information on the detectors signals for each decay event. An exhaustive offline analysis of the data gave unique access to experimental effects potentially biasing the measurement. After establishing the influence factors impacting the measurement such as after-pulses, pile-up, gain and base line fluctuations, their effects were accurately estimated and the event selection optimized. The resulting half-life, $17.2569\\pm0.0019_{(stat)}\\pm0.0009"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.09415","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":""},"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":"2026-05-18T00:27:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"v72A9eOK1dBlNEf9JmPfdZPmawHHUjnobLibwgVwnRlNP11EjUtfoKBuHfV3RVUaIGVPfJCvlLtKhp303ZtRDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T05:35:18.350796Z"},"content_sha256":"46a11fd2a8009036d1e155a58ffafb4f3565d76994260fdc3f0787df9edb2a14","schema_version":"1.0","event_id":"sha256:46a11fd2a8009036d1e155a58ffafb4f3565d76994260fdc3f0787df9edb2a14"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3K2TQJ7NP3JVTIWR63SA4725FB/bundle.json","state_url":"https://pith.science/pith/3K2TQJ7NP3JVTIWR63SA4725FB/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3K2TQJ7NP3JVTIWR63SA4725FB/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":"2026-05-27T05:35:18Z","links":{"resolver":"https://pith.science/pith/3K2TQJ7NP3JVTIWR63SA4725FB","bundle":"https://pith.science/pith/3K2TQJ7NP3JVTIWR63SA4725FB/bundle.json","state":"https://pith.science/pith/3K2TQJ7NP3JVTIWR63SA4725FB/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3K2TQJ7NP3JVTIWR63SA4725FB/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:3K2TQJ7NP3JVTIWR63SA4725FB","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":"6d52047b6ca918cebcd001351bb20780dafdf71d9d2f9acbe8e1592744396d6e","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2017-09-27T09:43:34Z","title_canon_sha256":"efadeea903b9daa6ec75e11a3ac7bf70fd7209c61ef6d232ebc507a7f3a2d1a6"},"schema_version":"1.0","source":{"id":"1709.09415","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1709.09415","created_at":"2026-05-18T00:27:43Z"},{"alias_kind":"arxiv_version","alias_value":"1709.09415v1","created_at":"2026-05-18T00:27:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.09415","created_at":"2026-05-18T00:27:43Z"},{"alias_kind":"pith_short_12","alias_value":"3K2TQJ7NP3JV","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_16","alias_value":"3K2TQJ7NP3JVTIWR","created_at":"2026-05-18T12:30:58Z"},{"alias_kind":"pith_short_8","alias_value":"3K2TQJ7N","created_at":"2026-05-18T12:30:58Z"}],"graph_snapshots":[{"event_id":"sha256:46a11fd2a8009036d1e155a58ffafb4f3565d76994260fdc3f0787df9edb2a14","target":"graph","created_at":"2026-05-18T00:27:43Z","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":"The half-life of $^{19}$Ne has been measured using a real-time digital multiparametric acquisition system providing an accurate time-stamp and relevant information on the detectors signals for each decay event. An exhaustive offline analysis of the data gave unique access to experimental effects potentially biasing the measurement. After establishing the influence factors impacting the measurement such as after-pulses, pile-up, gain and base line fluctuations, their effects were accurately estimated and the event selection optimized. The resulting half-life, $17.2569\\pm0.0019_{(stat)}\\pm0.0009","authors_text":"A. Jevremovi\\'c, A. M. S\\'anchez-Ben\\'itez, B. Bastin, B. Blank, B. Carniol, C. Borcea, C. Fontbonne, C. Spitaels, D. Etasse, D. Ramos, D. Toprek, F. Boulay, F. Delaunay, F. de Oliveira Santos, F. Rotaru, G. de France, G.F. Grinyer, G. Fremont, H. Bouzomita, I. Martel, I. \\v{C}elikovi\\'c, J. B. Briand, J. C. Thomas, J. Harang, J. Hommet, J. M. Fontbonne, J. Mrazek, J. Poincheval, M. Lewitowicz, M. Parlog, M. Stanoiu, N. L. Achouri, P. Delahaye, P. Uji\\'c, R. Borcea, V. Girard Alcindor, X. Fl\\'echard","cross_cats":["physics.ins-det"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2017-09-27T09:43:34Z","title":"High Precision Measurement of the $^{19}$Ne Half-life using real-time digital acquisition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.09415","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:b928a3fad2c1dc9277295a02b1b03be775dbaa014c1ecdd08f661454c8e2a912","target":"record","created_at":"2026-05-18T00:27:43Z","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":"6d52047b6ca918cebcd001351bb20780dafdf71d9d2f9acbe8e1592744396d6e","cross_cats_sorted":["physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2017-09-27T09:43:34Z","title_canon_sha256":"efadeea903b9daa6ec75e11a3ac7bf70fd7209c61ef6d232ebc507a7f3a2d1a6"},"schema_version":"1.0","source":{"id":"1709.09415","kind":"arxiv","version":1}},"canonical_sha256":"dab53827ed7ed359a2d1f6e40e7f5d285565f2c681701ec233c3fdbca6ced953","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dab53827ed7ed359a2d1f6e40e7f5d285565f2c681701ec233c3fdbca6ced953","first_computed_at":"2026-05-18T00:27:43.056105Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:27:43.056105Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2fncdoBQNawX2w6YeXB2Hi5Vn6GjMTGBHhxxUHoi5OF55S1/utOESkSOLU/4taJKy3vAlqW6G1D+Sn/RNHA8DA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:27:43.056711Z","signed_message":"canonical_sha256_bytes"},"source_id":"1709.09415","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b928a3fad2c1dc9277295a02b1b03be775dbaa014c1ecdd08f661454c8e2a912","sha256:46a11fd2a8009036d1e155a58ffafb4f3565d76994260fdc3f0787df9edb2a14"],"state_sha256":"ab320ced79813df23ce84ce8f42485fb287dee3fa4a107bcd352ec3632f5772b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fcNfpOVwX4uWWzfMbQebXJuprtsuIaoEbUiaEkanwLgtpIV853uhcKRPVBzKTFHY+u2Dkwv59mIBiLPsWakoAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T05:35:18.353368Z","bundle_sha256":"fbaf3d84d142c2ccbc0042d4298708c948cae76a1fa66a303b1065fa22718f08"}}