{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:4L74IZVYK7TK7NRVX237EXJGYZ","short_pith_number":"pith:4L74IZVY","canonical_record":{"source":{"id":"1503.02959","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-03-10T15:59:49Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"157c8b20bf25e1a7716021661dd0a79c2e4638409d093695386be87ce0dd04b2","abstract_canon_sha256":"b4031836da2aeb6e42c74f09efbb6ac89e238842ca356a748170d5c7bbeb312a"},"schema_version":"1.0"},"canonical_sha256":"e2ffc466b857e6afb635beb7f25d26c641289ff2fb3694284b082c45177dc160","source":{"kind":"arxiv","id":"1503.02959","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1503.02959","created_at":"2026-05-18T01:35:10Z"},{"alias_kind":"arxiv_version","alias_value":"1503.02959v4","created_at":"2026-05-18T01:35:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.02959","created_at":"2026-05-18T01:35:10Z"},{"alias_kind":"pith_short_12","alias_value":"4L74IZVYK7TK","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_16","alias_value":"4L74IZVYK7TK7NRV","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_8","alias_value":"4L74IZVY","created_at":"2026-05-18T12:29:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:4L74IZVYK7TK7NRVX237EXJGYZ","target":"record","payload":{"canonical_record":{"source":{"id":"1503.02959","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-03-10T15:59:49Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"157c8b20bf25e1a7716021661dd0a79c2e4638409d093695386be87ce0dd04b2","abstract_canon_sha256":"b4031836da2aeb6e42c74f09efbb6ac89e238842ca356a748170d5c7bbeb312a"},"schema_version":"1.0"},"canonical_sha256":"e2ffc466b857e6afb635beb7f25d26c641289ff2fb3694284b082c45177dc160","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:35:10.955081Z","signature_b64":"B4e8JTVr705d0KxO7zWOYKfRAs8tlrnaa3elcaF08ljaP2oCACfGA8dOlsHwB+/GXbTfEaPAVkmQ0tnmuqSNDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e2ffc466b857e6afb635beb7f25d26c641289ff2fb3694284b082c45177dc160","last_reissued_at":"2026-05-18T01:35:10.954501Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:35:10.954501Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1503.02959","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":"2026-05-18T01:35:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ay6FyJ3nWA8LuaNFRMb74fyDrROUAlefNKNdWv8hnv0sIQTeWlZFgqxGug5aq0EG1bscN+vWiRIah5ZBGfU4DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:58:09.722583Z"},"content_sha256":"c78dcaabd1e22559e66743fdc24a027d5a8411a625033f630ace481b80868ccf","schema_version":"1.0","event_id":"sha256:c78dcaabd1e22559e66743fdc24a027d5a8411a625033f630ace481b80868ccf"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:4L74IZVYK7TK7NRVX237EXJGYZ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Generalized Hyper-Ramsey Resonance with separated oscillating fields","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.atom-ph","authors_text":"A.V. Taichenachev, T. Zanon-Willette, V.I. Yudin","submitted_at":"2015-03-10T15:59:49Z","abstract_excerpt":"An exact generalization of the Ramsey transition probability is derived to improve ultra-high precision measurement and quantum state engineering when a particle is subjected to independently-tailored separated oscillating fields. The phase-shift accumulated at the end of the interrogation scheme offering high-level control of quantum states throughout various laser parameters conditions. The Generalized Hyper-Ramsey Resonance based on independent manipulation of interaction time, field amplitude, phase and frequency detuning is presented to increase the performance of next generation of atomi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.02959","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":"2026-05-18T01:35:10Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7e0Xxx1+qxk91NLqZWodJE5u2M+I+jqEK2DzpXWbow8qmxlRDW1APU9XDcolFcxyLcOQMaqOcxoiOQhHbJwkDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T06:58:09.723126Z"},"content_sha256":"0a780711ec4561b1189b813a33a14b556ed223bee4d3743d01a11542ada60b57","schema_version":"1.0","event_id":"sha256:0a780711ec4561b1189b813a33a14b556ed223bee4d3743d01a11542ada60b57"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4L74IZVYK7TK7NRVX237EXJGYZ/bundle.json","state_url":"https://pith.science/pith/4L74IZVYK7TK7NRVX237EXJGYZ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4L74IZVYK7TK7NRVX237EXJGYZ/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":"2026-05-30T06:58:09Z","links":{"resolver":"https://pith.science/pith/4L74IZVYK7TK7NRVX237EXJGYZ","bundle":"https://pith.science/pith/4L74IZVYK7TK7NRVX237EXJGYZ/bundle.json","state":"https://pith.science/pith/4L74IZVYK7TK7NRVX237EXJGYZ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4L74IZVYK7TK7NRVX237EXJGYZ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:4L74IZVYK7TK7NRVX237EXJGYZ","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":"b4031836da2aeb6e42c74f09efbb6ac89e238842ca356a748170d5c7bbeb312a","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-03-10T15:59:49Z","title_canon_sha256":"157c8b20bf25e1a7716021661dd0a79c2e4638409d093695386be87ce0dd04b2"},"schema_version":"1.0","source":{"id":"1503.02959","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1503.02959","created_at":"2026-05-18T01:35:10Z"},{"alias_kind":"arxiv_version","alias_value":"1503.02959v4","created_at":"2026-05-18T01:35:10Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.02959","created_at":"2026-05-18T01:35:10Z"},{"alias_kind":"pith_short_12","alias_value":"4L74IZVYK7TK","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_16","alias_value":"4L74IZVYK7TK7NRV","created_at":"2026-05-18T12:29:05Z"},{"alias_kind":"pith_short_8","alias_value":"4L74IZVY","created_at":"2026-05-18T12:29:05Z"}],"graph_snapshots":[{"event_id":"sha256:0a780711ec4561b1189b813a33a14b556ed223bee4d3743d01a11542ada60b57","target":"graph","created_at":"2026-05-18T01:35:10Z","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":"An exact generalization of the Ramsey transition probability is derived to improve ultra-high precision measurement and quantum state engineering when a particle is subjected to independently-tailored separated oscillating fields. The phase-shift accumulated at the end of the interrogation scheme offering high-level control of quantum states throughout various laser parameters conditions. The Generalized Hyper-Ramsey Resonance based on independent manipulation of interaction time, field amplitude, phase and frequency detuning is presented to increase the performance of next generation of atomi","authors_text":"A.V. Taichenachev, T. Zanon-Willette, V.I. Yudin","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-03-10T15:59:49Z","title":"Generalized Hyper-Ramsey Resonance with separated oscillating fields"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.02959","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:c78dcaabd1e22559e66743fdc24a027d5a8411a625033f630ace481b80868ccf","target":"record","created_at":"2026-05-18T01:35:10Z","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":"b4031836da2aeb6e42c74f09efbb6ac89e238842ca356a748170d5c7bbeb312a","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2015-03-10T15:59:49Z","title_canon_sha256":"157c8b20bf25e1a7716021661dd0a79c2e4638409d093695386be87ce0dd04b2"},"schema_version":"1.0","source":{"id":"1503.02959","kind":"arxiv","version":4}},"canonical_sha256":"e2ffc466b857e6afb635beb7f25d26c641289ff2fb3694284b082c45177dc160","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e2ffc466b857e6afb635beb7f25d26c641289ff2fb3694284b082c45177dc160","first_computed_at":"2026-05-18T01:35:10.954501Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:35:10.954501Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"B4e8JTVr705d0KxO7zWOYKfRAs8tlrnaa3elcaF08ljaP2oCACfGA8dOlsHwB+/GXbTfEaPAVkmQ0tnmuqSNDw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:35:10.955081Z","signed_message":"canonical_sha256_bytes"},"source_id":"1503.02959","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c78dcaabd1e22559e66743fdc24a027d5a8411a625033f630ace481b80868ccf","sha256:0a780711ec4561b1189b813a33a14b556ed223bee4d3743d01a11542ada60b57"],"state_sha256":"cca9dee03659d06af17d62045c69b1d00968ad71f40f4c0f56a83a18c94d0e34"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nZ1nieyWDR7B/dSfd2NQ0m+wX0NThnS7XHIdGYmWHkGCaTK0eNpmojOm1As2oKoO/JEqZuv/8XaNNreyqzrKAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T06:58:09.726287Z","bundle_sha256":"0dd655bca3b7c57af78fc89dbfd2569e45c87c000b6885c8f167875f8ce142ca"}}