{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:G5ZDESADX3CNKG7W5RKZ5FPU3R","short_pith_number":"pith:G5ZDESAD","canonical_record":{"source":{"id":"1110.6282","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-10-28T09:37:05Z","cross_cats_sorted":[],"title_canon_sha256":"b068c370ad64988eda417c28487df794d946a9d28cafae5d3f6f7c4a1e6396ee","abstract_canon_sha256":"fd570d8884331980ff30d214136e5678888e651597024f9240c3bde8c3b9aa02"},"schema_version":"1.0"},"canonical_sha256":"3772324803bec4d51bf6ec559e95f4dc41e25cbffe5f43bb57ee74e986ab8461","source":{"kind":"arxiv","id":"1110.6282","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1110.6282","created_at":"2026-05-18T00:58:43Z"},{"alias_kind":"arxiv_version","alias_value":"1110.6282v1","created_at":"2026-05-18T00:58:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.6282","created_at":"2026-05-18T00:58:43Z"},{"alias_kind":"pith_short_12","alias_value":"G5ZDESADX3CN","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_16","alias_value":"G5ZDESADX3CNKG7W","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_8","alias_value":"G5ZDESAD","created_at":"2026-05-18T12:26:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:G5ZDESADX3CNKG7W5RKZ5FPU3R","target":"record","payload":{"canonical_record":{"source":{"id":"1110.6282","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-10-28T09:37:05Z","cross_cats_sorted":[],"title_canon_sha256":"b068c370ad64988eda417c28487df794d946a9d28cafae5d3f6f7c4a1e6396ee","abstract_canon_sha256":"fd570d8884331980ff30d214136e5678888e651597024f9240c3bde8c3b9aa02"},"schema_version":"1.0"},"canonical_sha256":"3772324803bec4d51bf6ec559e95f4dc41e25cbffe5f43bb57ee74e986ab8461","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:58:43.292275Z","signature_b64":"BKPkXUU7yIemvbApFFpi265IqIpjKmidxIDwaOnuMYKIMQwvM9ptC0CBf676AvaZ0VadiHI3v++tZkmz1tU7BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3772324803bec4d51bf6ec559e95f4dc41e25cbffe5f43bb57ee74e986ab8461","last_reissued_at":"2026-05-18T00:58:43.291541Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:58:43.291541Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1110.6282","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":"2026-05-18T00:58:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AzAykdaMJk62TfKAYFA5AlouZKRsIv30CMEcthv7xYPBPS9vcfD7Ccg5BM7KXUnsccLLOUwjd8oxZrFBZCCXCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T05:44:54.358861Z"},"content_sha256":"384f5e6cffc60d3990481ed69a07c1b614e81d7c1b7e802208fce3693f17440e","schema_version":"1.0","event_id":"sha256:384f5e6cffc60d3990481ed69a07c1b614e81d7c1b7e802208fce3693f17440e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:G5ZDESADX3CNKG7W5RKZ5FPU3R","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Temperature Dependence Cancellation of the Cs Clock Frequency in the Presence of Ne Buffer Gas","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.atom-ph","authors_text":"Emeric de Clercq, Olga Kozlova, Rodolphe Boudot, St\\'ephane Gu\\'erandel","submitted_at":"2011-10-28T09:37:05Z","abstract_excerpt":"The temperature dependence of the Cs clock transition frequency in a vapor cell filled with Ne buffer gas has been measured. The experimental setup is based on the coherent population trapping (CPT) technique and a temporal Ramsey interrogation allowing a high resolution. A quadratic dependence of the frequency shift is shown. The temperature of the shift cancellation is evaluated. The actual Ne pressure in the cell is determined from the frequency shift of the 895nm optical transition. We can then determine the Cs-Ne collisional temperature coefficients of the clock frequency. These results c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.6282","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":"2026-05-18T00:58:43Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HjnPbeCkaIAAX4SSGjv/SnGuDLSUHw9z27AUqJrfElTqDt4qUQ6kAdp8Q5Tq/ivv6XYjOKmrT8KshG00YtrEDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T05:44:54.359602Z"},"content_sha256":"5d43698f1b56ac9619b0b92fe30533f70e26f7dd31a277d1ea6b5bf305e9d5b1","schema_version":"1.0","event_id":"sha256:5d43698f1b56ac9619b0b92fe30533f70e26f7dd31a277d1ea6b5bf305e9d5b1"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/G5ZDESADX3CNKG7W5RKZ5FPU3R/bundle.json","state_url":"https://pith.science/pith/G5ZDESADX3CNKG7W5RKZ5FPU3R/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/G5ZDESADX3CNKG7W5RKZ5FPU3R/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":"2026-06-12T05:44:54Z","links":{"resolver":"https://pith.science/pith/G5ZDESADX3CNKG7W5RKZ5FPU3R","bundle":"https://pith.science/pith/G5ZDESADX3CNKG7W5RKZ5FPU3R/bundle.json","state":"https://pith.science/pith/G5ZDESADX3CNKG7W5RKZ5FPU3R/state.json","well_known_bundle":"https://pith.science/.well-known/pith/G5ZDESADX3CNKG7W5RKZ5FPU3R/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:G5ZDESADX3CNKG7W5RKZ5FPU3R","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":"fd570d8884331980ff30d214136e5678888e651597024f9240c3bde8c3b9aa02","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-10-28T09:37:05Z","title_canon_sha256":"b068c370ad64988eda417c28487df794d946a9d28cafae5d3f6f7c4a1e6396ee"},"schema_version":"1.0","source":{"id":"1110.6282","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1110.6282","created_at":"2026-05-18T00:58:43Z"},{"alias_kind":"arxiv_version","alias_value":"1110.6282v1","created_at":"2026-05-18T00:58:43Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.6282","created_at":"2026-05-18T00:58:43Z"},{"alias_kind":"pith_short_12","alias_value":"G5ZDESADX3CN","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_16","alias_value":"G5ZDESADX3CNKG7W","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_8","alias_value":"G5ZDESAD","created_at":"2026-05-18T12:26:28Z"}],"graph_snapshots":[{"event_id":"sha256:5d43698f1b56ac9619b0b92fe30533f70e26f7dd31a277d1ea6b5bf305e9d5b1","target":"graph","created_at":"2026-05-18T00:58:43Z","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 temperature dependence of the Cs clock transition frequency in a vapor cell filled with Ne buffer gas has been measured. The experimental setup is based on the coherent population trapping (CPT) technique and a temporal Ramsey interrogation allowing a high resolution. A quadratic dependence of the frequency shift is shown. The temperature of the shift cancellation is evaluated. The actual Ne pressure in the cell is determined from the frequency shift of the 895nm optical transition. We can then determine the Cs-Ne collisional temperature coefficients of the clock frequency. These results c","authors_text":"Emeric de Clercq, Olga Kozlova, Rodolphe Boudot, St\\'ephane Gu\\'erandel","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-10-28T09:37:05Z","title":"Temperature Dependence Cancellation of the Cs Clock Frequency in the Presence of Ne Buffer Gas"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.6282","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":"sha256:384f5e6cffc60d3990481ed69a07c1b614e81d7c1b7e802208fce3693f17440e","target":"record","created_at":"2026-05-18T00:58:43Z","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":"fd570d8884331980ff30d214136e5678888e651597024f9240c3bde8c3b9aa02","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2011-10-28T09:37:05Z","title_canon_sha256":"b068c370ad64988eda417c28487df794d946a9d28cafae5d3f6f7c4a1e6396ee"},"schema_version":"1.0","source":{"id":"1110.6282","kind":"arxiv","version":1}},"canonical_sha256":"3772324803bec4d51bf6ec559e95f4dc41e25cbffe5f43bb57ee74e986ab8461","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3772324803bec4d51bf6ec559e95f4dc41e25cbffe5f43bb57ee74e986ab8461","first_computed_at":"2026-05-18T00:58:43.291541Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:58:43.291541Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BKPkXUU7yIemvbApFFpi265IqIpjKmidxIDwaOnuMYKIMQwvM9ptC0CBf676AvaZ0VadiHI3v++tZkmz1tU7BA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:58:43.292275Z","signed_message":"canonical_sha256_bytes"},"source_id":"1110.6282","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:384f5e6cffc60d3990481ed69a07c1b614e81d7c1b7e802208fce3693f17440e","sha256:5d43698f1b56ac9619b0b92fe30533f70e26f7dd31a277d1ea6b5bf305e9d5b1"],"state_sha256":"f76db8190c5164f5ada29525a17047dde72e9289be44aa388f081fc400c5c3a8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Q0AnNHg8+7Im1L462ZK6rpzHJgWNKkcmrKyqCl9I26Xoeg3HyWo5NgyKYQphWMNu4RJsc2R87v7ODec7iHakAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-12T05:44:54.363356Z","bundle_sha256":"37f08a62c401461007d499921587e6765a3112c5282d756077df88dd7a8a7b4c"}}