{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:ER35MKGHKHP6ZN6WADZX6RU5X5","short_pith_number":"pith:ER35MKGH","canonical_record":{"source":{"id":"1111.3260","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2011-11-14T16:07:14Z","cross_cats_sorted":["astro-ph.IM","physics.ins-det"],"title_canon_sha256":"654ff9911b11c3c3d1b45b0e5f8d2943123a1f13d1a0f019c020a05cb226bc77","abstract_canon_sha256":"2199a8fee70683049cc9565f27f10035d333e3d44515f41a85a936ce681b499d"},"schema_version":"1.0"},"canonical_sha256":"2477d628c751dfecb7d600f37f469dbf59269761131bb8766c3efae7d7a1f771","source":{"kind":"arxiv","id":"1111.3260","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1111.3260","created_at":"2026-05-18T03:48:59Z"},{"alias_kind":"arxiv_version","alias_value":"1111.3260v2","created_at":"2026-05-18T03:48:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.3260","created_at":"2026-05-18T03:48:59Z"},{"alias_kind":"pith_short_12","alias_value":"ER35MKGHKHP6","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_16","alias_value":"ER35MKGHKHP6ZN6W","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_8","alias_value":"ER35MKGH","created_at":"2026-05-18T12:26:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:ER35MKGHKHP6ZN6WADZX6RU5X5","target":"record","payload":{"canonical_record":{"source":{"id":"1111.3260","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2011-11-14T16:07:14Z","cross_cats_sorted":["astro-ph.IM","physics.ins-det"],"title_canon_sha256":"654ff9911b11c3c3d1b45b0e5f8d2943123a1f13d1a0f019c020a05cb226bc77","abstract_canon_sha256":"2199a8fee70683049cc9565f27f10035d333e3d44515f41a85a936ce681b499d"},"schema_version":"1.0"},"canonical_sha256":"2477d628c751dfecb7d600f37f469dbf59269761131bb8766c3efae7d7a1f771","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:48:59.034784Z","signature_b64":"zEaqx+7sTWrZjKyUQN/dyr7/iQLq7KBF/kutkk+SOjGaJ1CruUM9C5V+RnDFA8VOdeig1Nhjb8WdqIyyhd8xBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2477d628c751dfecb7d600f37f469dbf59269761131bb8766c3efae7d7a1f771","last_reissued_at":"2026-05-18T03:48:59.033472Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:48:59.033472Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1111.3260","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":"2026-05-18T03:48:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZzLNs8OtCWjTQL9tHTGLOBm1E9xrGKq+hJ5uyiNOrq4QeVrGhqXTgbYg0X9pLrSFCZ34gkhQ4maADoLiMTWkBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T21:32:05.383794Z"},"content_sha256":"c7045e28a3a719264e97dc73a029d1d029a5df8a5ce3ea8afb5b0f7b6fa2b597","schema_version":"1.0","event_id":"sha256:c7045e28a3a719264e97dc73a029d1d029a5df8a5ce3ea8afb5b0f7b6fa2b597"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:ER35MKGHKHP6ZN6WADZX6RU5X5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Scintillation yield and time dependence from electronic and nuclear recoils in liquid neon","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["astro-ph.IM","physics.ins-det"],"primary_cat":"nucl-ex","authors_text":"D. Gastler, D. N. McKinsey, E. Kearns, J. A. Nikkel, K. J. Coakley, W. H. Lippincott","submitted_at":"2011-11-14T16:07:14Z","abstract_excerpt":"We have performed measurements of scintillation light in liquid neon, observing a signal yield in our detector as high as (3.5 $\\pm$ 0.4) photoelectrons/keV. We measure pulse shape discrimination efficiency between electronic and nuclear recoils in liquid neon from 50 and 300 keV nuclear recoil energy. We also measure the \\leff\\, parameter in liquid neon between 30 and 370 keV nuclear recoil energy, observing an average \\leff$=0.24$ above 50 keV. We observe a dependence of the scintillation time distribution and signal yield on the pressure and temperature of the liquid neon."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.3260","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":""},"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":"2026-05-18T03:48:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7W/oEBLWp4R3+Xiu1JeBqUD08+0qsm+yxJ9e4LEzDMWM/AM0xSGAi0ctstwSq+SyzY2g7Ib6zb8Fd4Jhe2X/Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T21:32:05.384148Z"},"content_sha256":"81fa8c03bfc6d5edab3f4edaea278001902b9d2c74643ee066861b9dab7cef49","schema_version":"1.0","event_id":"sha256:81fa8c03bfc6d5edab3f4edaea278001902b9d2c74643ee066861b9dab7cef49"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ER35MKGHKHP6ZN6WADZX6RU5X5/bundle.json","state_url":"https://pith.science/pith/ER35MKGHKHP6ZN6WADZX6RU5X5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ER35MKGHKHP6ZN6WADZX6RU5X5/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":"2026-06-01T21:32:05Z","links":{"resolver":"https://pith.science/pith/ER35MKGHKHP6ZN6WADZX6RU5X5","bundle":"https://pith.science/pith/ER35MKGHKHP6ZN6WADZX6RU5X5/bundle.json","state":"https://pith.science/pith/ER35MKGHKHP6ZN6WADZX6RU5X5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ER35MKGHKHP6ZN6WADZX6RU5X5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:ER35MKGHKHP6ZN6WADZX6RU5X5","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":"2199a8fee70683049cc9565f27f10035d333e3d44515f41a85a936ce681b499d","cross_cats_sorted":["astro-ph.IM","physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2011-11-14T16:07:14Z","title_canon_sha256":"654ff9911b11c3c3d1b45b0e5f8d2943123a1f13d1a0f019c020a05cb226bc77"},"schema_version":"1.0","source":{"id":"1111.3260","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1111.3260","created_at":"2026-05-18T03:48:59Z"},{"alias_kind":"arxiv_version","alias_value":"1111.3260v2","created_at":"2026-05-18T03:48:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.3260","created_at":"2026-05-18T03:48:59Z"},{"alias_kind":"pith_short_12","alias_value":"ER35MKGHKHP6","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_16","alias_value":"ER35MKGHKHP6ZN6W","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_8","alias_value":"ER35MKGH","created_at":"2026-05-18T12:26:28Z"}],"graph_snapshots":[{"event_id":"sha256:81fa8c03bfc6d5edab3f4edaea278001902b9d2c74643ee066861b9dab7cef49","target":"graph","created_at":"2026-05-18T03:48:59Z","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 have performed measurements of scintillation light in liquid neon, observing a signal yield in our detector as high as (3.5 $\\pm$ 0.4) photoelectrons/keV. We measure pulse shape discrimination efficiency between electronic and nuclear recoils in liquid neon from 50 and 300 keV nuclear recoil energy. We also measure the \\leff\\, parameter in liquid neon between 30 and 370 keV nuclear recoil energy, observing an average \\leff$=0.24$ above 50 keV. We observe a dependence of the scintillation time distribution and signal yield on the pressure and temperature of the liquid neon.","authors_text":"D. Gastler, D. N. McKinsey, E. Kearns, J. A. Nikkel, K. J. Coakley, W. H. Lippincott","cross_cats":["astro-ph.IM","physics.ins-det"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2011-11-14T16:07:14Z","title":"Scintillation yield and time dependence from electronic and nuclear recoils in liquid neon"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.3260","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:c7045e28a3a719264e97dc73a029d1d029a5df8a5ce3ea8afb5b0f7b6fa2b597","target":"record","created_at":"2026-05-18T03:48:59Z","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":"2199a8fee70683049cc9565f27f10035d333e3d44515f41a85a936ce681b499d","cross_cats_sorted":["astro-ph.IM","physics.ins-det"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2011-11-14T16:07:14Z","title_canon_sha256":"654ff9911b11c3c3d1b45b0e5f8d2943123a1f13d1a0f019c020a05cb226bc77"},"schema_version":"1.0","source":{"id":"1111.3260","kind":"arxiv","version":2}},"canonical_sha256":"2477d628c751dfecb7d600f37f469dbf59269761131bb8766c3efae7d7a1f771","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2477d628c751dfecb7d600f37f469dbf59269761131bb8766c3efae7d7a1f771","first_computed_at":"2026-05-18T03:48:59.033472Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:48:59.033472Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zEaqx+7sTWrZjKyUQN/dyr7/iQLq7KBF/kutkk+SOjGaJ1CruUM9C5V+RnDFA8VOdeig1Nhjb8WdqIyyhd8xBA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:48:59.034784Z","signed_message":"canonical_sha256_bytes"},"source_id":"1111.3260","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c7045e28a3a719264e97dc73a029d1d029a5df8a5ce3ea8afb5b0f7b6fa2b597","sha256:81fa8c03bfc6d5edab3f4edaea278001902b9d2c74643ee066861b9dab7cef49"],"state_sha256":"276dcce181ee79790f37153cc6fe7571734df784563e7aa1dbe3993cda187c84"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Zpzykq79GaXCfAr8ZtHzW+QWQHjCzo9U6y+wcIeEFM8ZsPM6jlJK1Pg/C121YEzPagvGI+SKXGsMBHqdtDSdCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T21:32:05.386447Z","bundle_sha256":"b63b6b43e8de3908de500483671c7e2cf1b4aaf6c4e2ead7b05e2ee894b86329"}}