{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:FZT6SAADPR3TOO26FBWAYWO3TJ","short_pith_number":"pith:FZT6SAAD","canonical_record":{"source":{"id":"1704.04134","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-04-13T13:44:55Z","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"title_canon_sha256":"dccdd33f28340304a966ff3d7ec905785d9b2a52028bd0bf7a72562302a9c209","abstract_canon_sha256":"e3650ed384ec857c5b82ab82193484322641403dccb507ffb6da243a764e88a0"},"schema_version":"1.0"},"canonical_sha256":"2e67e900037c77373b5e286c0c59db9a5e79ffd8e5161f30e3de858835cf1e94","source":{"kind":"arxiv","id":"1704.04134","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.04134","created_at":"2026-05-18T00:40:58Z"},{"alias_kind":"arxiv_version","alias_value":"1704.04134v1","created_at":"2026-05-18T00:40:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.04134","created_at":"2026-05-18T00:40:58Z"},{"alias_kind":"pith_short_12","alias_value":"FZT6SAADPR3T","created_at":"2026-05-18T12:31:15Z"},{"alias_kind":"pith_short_16","alias_value":"FZT6SAADPR3TOO26","created_at":"2026-05-18T12:31:15Z"},{"alias_kind":"pith_short_8","alias_value":"FZT6SAAD","created_at":"2026-05-18T12:31:15Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:FZT6SAADPR3TOO26FBWAYWO3TJ","target":"record","payload":{"canonical_record":{"source":{"id":"1704.04134","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-04-13T13:44:55Z","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"title_canon_sha256":"dccdd33f28340304a966ff3d7ec905785d9b2a52028bd0bf7a72562302a9c209","abstract_canon_sha256":"e3650ed384ec857c5b82ab82193484322641403dccb507ffb6da243a764e88a0"},"schema_version":"1.0"},"canonical_sha256":"2e67e900037c77373b5e286c0c59db9a5e79ffd8e5161f30e3de858835cf1e94","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:40:58.012993Z","signature_b64":"juv4OnH787BPsFvdYRBqz7NHXbhn/xp5QxDe+hZbXKhRhnZbWwuGpPIZM+PgVEWN6e4+TUmziPZFYttQnsXvCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2e67e900037c77373b5e286c0c59db9a5e79ffd8e5161f30e3de858835cf1e94","last_reissued_at":"2026-05-18T00:40:58.012575Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:40:58.012575Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1704.04134","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":"2026-05-18T00:40:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"i03AvaCUR0BvQ1gGikXQWWCLK+MMPSyAcYCqDGlfolqyO6XEPBKNBlCb29Si5Olx8syCV+dco1O3Qw9VEgJgDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T07:31:25.777240Z"},"content_sha256":"8c2336f3e1e1a27fdc829c62ff1e387bfbca2511bf51bded8e1276165509b6d9","schema_version":"1.0","event_id":"sha256:8c2336f3e1e1a27fdc829c62ff1e387bfbca2511bf51bded8e1276165509b6d9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:FZT6SAADPR3TOO26FBWAYWO3TJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Anisotropic optical trapping as a manifestation of the complex electronic structure of ultracold lanthanide atoms: the example of holmium","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","quant-ph"],"primary_cat":"physics.atom-ph","authors_text":"Hui Li, Jean-Fran\\c{c}ois Wyart, Maxence Lepers, Olivier Dulieu","submitted_at":"2017-04-13T13:44:55Z","abstract_excerpt":"The efficiency of optical trapping is determined by the atomic dynamic dipole polarizability, whose real and imaginary parts are associated with the potential energy and photon-scattering rate respectively. In this article we develop a formalism to calculate analytically the real and imaginary parts of the scalar, vector and tensor polarizabilities of lanthanide atoms. We assume that the sum-over-state formula only comprises transitions involving electrons in the valence orbitals like $6s$, $5d$, $6p$ or $7s$, while transitions involving $4f$ core electrons are neglected. Applying this formali"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.04134","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":"2026-05-18T00:40:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5MS2kRYfnDNtcS8MpxQ17cviIvwYDMLShC9NuWTExlnduAdoAnMqbbCzyoI2eEiN7AbGaNu3/8I+13iCYfO2Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T07:31:25.777648Z"},"content_sha256":"d56ec7a2292b48ce5bf999e806ff8e87d273712e13762f4aac46e28f28e81e4a","schema_version":"1.0","event_id":"sha256:d56ec7a2292b48ce5bf999e806ff8e87d273712e13762f4aac46e28f28e81e4a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FZT6SAADPR3TOO26FBWAYWO3TJ/bundle.json","state_url":"https://pith.science/pith/FZT6SAADPR3TOO26FBWAYWO3TJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FZT6SAADPR3TOO26FBWAYWO3TJ/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":"2026-05-30T07:31:25Z","links":{"resolver":"https://pith.science/pith/FZT6SAADPR3TOO26FBWAYWO3TJ","bundle":"https://pith.science/pith/FZT6SAADPR3TOO26FBWAYWO3TJ/bundle.json","state":"https://pith.science/pith/FZT6SAADPR3TOO26FBWAYWO3TJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FZT6SAADPR3TOO26FBWAYWO3TJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:FZT6SAADPR3TOO26FBWAYWO3TJ","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":"e3650ed384ec857c5b82ab82193484322641403dccb507ffb6da243a764e88a0","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-04-13T13:44:55Z","title_canon_sha256":"dccdd33f28340304a966ff3d7ec905785d9b2a52028bd0bf7a72562302a9c209"},"schema_version":"1.0","source":{"id":"1704.04134","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.04134","created_at":"2026-05-18T00:40:58Z"},{"alias_kind":"arxiv_version","alias_value":"1704.04134v1","created_at":"2026-05-18T00:40:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.04134","created_at":"2026-05-18T00:40:58Z"},{"alias_kind":"pith_short_12","alias_value":"FZT6SAADPR3T","created_at":"2026-05-18T12:31:15Z"},{"alias_kind":"pith_short_16","alias_value":"FZT6SAADPR3TOO26","created_at":"2026-05-18T12:31:15Z"},{"alias_kind":"pith_short_8","alias_value":"FZT6SAAD","created_at":"2026-05-18T12:31:15Z"}],"graph_snapshots":[{"event_id":"sha256:d56ec7a2292b48ce5bf999e806ff8e87d273712e13762f4aac46e28f28e81e4a","target":"graph","created_at":"2026-05-18T00:40:58Z","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 efficiency of optical trapping is determined by the atomic dynamic dipole polarizability, whose real and imaginary parts are associated with the potential energy and photon-scattering rate respectively. In this article we develop a formalism to calculate analytically the real and imaginary parts of the scalar, vector and tensor polarizabilities of lanthanide atoms. We assume that the sum-over-state formula only comprises transitions involving electrons in the valence orbitals like $6s$, $5d$, $6p$ or $7s$, while transitions involving $4f$ core electrons are neglected. Applying this formali","authors_text":"Hui Li, Jean-Fran\\c{c}ois Wyart, Maxence Lepers, Olivier Dulieu","cross_cats":["cond-mat.quant-gas","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-04-13T13:44:55Z","title":"Anisotropic optical trapping as a manifestation of the complex electronic structure of ultracold lanthanide atoms: the example of holmium"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.04134","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":"sha256:8c2336f3e1e1a27fdc829c62ff1e387bfbca2511bf51bded8e1276165509b6d9","target":"record","created_at":"2026-05-18T00:40:58Z","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":"e3650ed384ec857c5b82ab82193484322641403dccb507ffb6da243a764e88a0","cross_cats_sorted":["cond-mat.quant-gas","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2017-04-13T13:44:55Z","title_canon_sha256":"dccdd33f28340304a966ff3d7ec905785d9b2a52028bd0bf7a72562302a9c209"},"schema_version":"1.0","source":{"id":"1704.04134","kind":"arxiv","version":1}},"canonical_sha256":"2e67e900037c77373b5e286c0c59db9a5e79ffd8e5161f30e3de858835cf1e94","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2e67e900037c77373b5e286c0c59db9a5e79ffd8e5161f30e3de858835cf1e94","first_computed_at":"2026-05-18T00:40:58.012575Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:40:58.012575Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"juv4OnH787BPsFvdYRBqz7NHXbhn/xp5QxDe+hZbXKhRhnZbWwuGpPIZM+PgVEWN6e4+TUmziPZFYttQnsXvCg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:40:58.012993Z","signed_message":"canonical_sha256_bytes"},"source_id":"1704.04134","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8c2336f3e1e1a27fdc829c62ff1e387bfbca2511bf51bded8e1276165509b6d9","sha256:d56ec7a2292b48ce5bf999e806ff8e87d273712e13762f4aac46e28f28e81e4a"],"state_sha256":"9c7e397a9dc2ae9980bb18cbe0f9f95525306786b3fb2df62ce39ad47b8c3e3e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9RwK6F1SPCv8pycLD+G3hraf78a5lh5B6sVl51lAtFaIgg0Y+gfIHeIkV3XixqwWlYOvzZjXS5bpN/fDIyEhCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T07:31:25.779845Z","bundle_sha256":"288563cc25e60f3e1aeb5961522f4ae76f82075fcc986043cab4934ff4fef16f"}}