{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:IXTSZ4MDPIOZ7HPQ2OS6EJ75XP","short_pith_number":"pith:IXTSZ4MD","schema_version":"1.0","canonical_sha256":"45e72cf1837a1d9f9df0d3a5e227fdbbcf4fa2d1bf16d5d6e6ce15beddc452ee","source":{"kind":"arxiv","id":"0803.1039","version":1},"attestation_state":"computed","paper":{"title":"Frequency Light Shifts Caused by the Effects of Quantization of Atomic Motion in an Optical Lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"physics.atom-ph","authors_text":"A. V. Taichenachev, V. D. Ovsiannikov, V. G. Pal'chikov, V. I. Yudin","submitted_at":"2008-03-07T09:20:05Z","abstract_excerpt":"Frequency light shifts resulting from the localization effects and effects of the quantization of translational atomic motion in an optical lattice is studied for a forbidden optical transition $J$=0$\\to$$J$=0. In the Lamb-Dicke regime this shift is proportional to the square root from the lattice field intensity. With allowance made for magneto-dipole and quadrupole transitions, the shift does not vanish at the magic wavelength, at which the linear in intensity shift is absent. Preliminary estimates show that this shift can have a principal significance for the lattice-based atomic clocks wit"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"0803.1039","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2008-03-07T09:20:05Z","cross_cats_sorted":["physics.optics"],"title_canon_sha256":"ae6229617101a912a39d610f8404e75f1162e85a36292c4065d689da631465a7","abstract_canon_sha256":"6f45ab0b2212560a76298be87ebda3ec44460b8e126a200445fae63c6055258e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:24:43.069648Z","signature_b64":"ws+cdJgyBzFt9xdZT25KDbCv2se67qFKoaYwtr0iRIjslE8F+Wb/BUUsHGbxrNWBQXpAcWCXMf+W4psYYWtOAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"45e72cf1837a1d9f9df0d3a5e227fdbbcf4fa2d1bf16d5d6e6ce15beddc452ee","last_reissued_at":"2026-05-18T03:24:43.069134Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:24:43.069134Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Frequency Light Shifts Caused by the Effects of Quantization of Atomic Motion in an Optical Lattice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.optics"],"primary_cat":"physics.atom-ph","authors_text":"A. V. Taichenachev, V. D. Ovsiannikov, V. G. Pal'chikov, V. I. Yudin","submitted_at":"2008-03-07T09:20:05Z","abstract_excerpt":"Frequency light shifts resulting from the localization effects and effects of the quantization of translational atomic motion in an optical lattice is studied for a forbidden optical transition $J$=0$\\to$$J$=0. In the Lamb-Dicke regime this shift is proportional to the square root from the lattice field intensity. With allowance made for magneto-dipole and quadrupole transitions, the shift does not vanish at the magic wavelength, at which the linear in intensity shift is absent. Preliminary estimates show that this shift can have a principal significance for the lattice-based atomic clocks wit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0803.1039","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"0803.1039","created_at":"2026-05-18T03:24:43.069213+00:00"},{"alias_kind":"arxiv_version","alias_value":"0803.1039v1","created_at":"2026-05-18T03:24:43.069213+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0803.1039","created_at":"2026-05-18T03:24:43.069213+00:00"},{"alias_kind":"pith_short_12","alias_value":"IXTSZ4MDPIOZ","created_at":"2026-05-18T12:25:57.157939+00:00"},{"alias_kind":"pith_short_16","alias_value":"IXTSZ4MDPIOZ7HPQ","created_at":"2026-05-18T12:25:57.157939+00:00"},{"alias_kind":"pith_short_8","alias_value":"IXTSZ4MD","created_at":"2026-05-18T12:25:57.157939+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP","json":"https://pith.science/pith/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP.json","graph_json":"https://pith.science/api/pith-number/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP/graph.json","events_json":"https://pith.science/api/pith-number/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP/events.json","paper":"https://pith.science/paper/IXTSZ4MD"},"agent_actions":{"view_html":"https://pith.science/pith/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP","download_json":"https://pith.science/pith/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP.json","view_paper":"https://pith.science/paper/IXTSZ4MD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0803.1039&json=true","fetch_graph":"https://pith.science/api/pith-number/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP/graph.json","fetch_events":"https://pith.science/api/pith-number/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP/action/storage_attestation","attest_author":"https://pith.science/pith/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP/action/author_attestation","sign_citation":"https://pith.science/pith/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP/action/citation_signature","submit_replication":"https://pith.science/pith/IXTSZ4MDPIOZ7HPQ2OS6EJ75XP/action/replication_record"}},"created_at":"2026-05-18T03:24:43.069213+00:00","updated_at":"2026-05-18T03:24:43.069213+00:00"}