{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:BXA7VLEN53YK736KM4QW22ZF3M","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":"e0cf4625d5cb806b8210f5690d3360a5b6c799655f6275a891a5c1dc319c603e","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-05-20T15:30:21Z","title_canon_sha256":"fa90fffaba4c029aa6db147fe4b98b9ee1421fa2bbbf524c80957d01a63eeffe"},"schema_version":"1.0","source":{"id":"1305.4556","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1305.4556","created_at":"2026-05-18T01:49:48Z"},{"alias_kind":"arxiv_version","alias_value":"1305.4556v1","created_at":"2026-05-18T01:49:48Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.4556","created_at":"2026-05-18T01:49:48Z"},{"alias_kind":"pith_short_12","alias_value":"BXA7VLEN53YK","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_16","alias_value":"BXA7VLEN53YK736K","created_at":"2026-05-18T12:27:40Z"},{"alias_kind":"pith_short_8","alias_value":"BXA7VLEN","created_at":"2026-05-18T12:27:40Z"}],"graph_snapshots":[{"event_id":"sha256:a1119682a3b0ace9e872332cfbc9b67f2f302b8bcb59df52b4b198295ddfff59","target":"graph","created_at":"2026-05-18T01:49:48Z","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 investigate the influence of intense, elliptically polarized driving fields on high-order harmonic spectra from aligned diatomic molecules. We derive a generalized two-center interference condition for elliptically polarized fields, which accounts for s-p mixing and the orbital symmetry, within the strong-field and the single-active electron approximation. We show that the non-vanishing ellipticity introduces an effective dynamic shift in the angle for which the two-center interference maxima and minima occur, with regard to the existing condition for linearly polarized fields. This shift d","authors_text":"B. B. Augstein, C. Figueira de Morisson Faria, T. Das","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-05-20T15:30:21Z","title":"High-order harmonic generation from diatomic molecules in elliptically polarized driving fields: a generalized interference condition"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.4556","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":"sha256:48aa13c7d5be9e8b939e896c6b71cb6c147be2bc0d6a7600265471a8105cd059","target":"record","created_at":"2026-05-18T01:49:48Z","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":"e0cf4625d5cb806b8210f5690d3360a5b6c799655f6275a891a5c1dc319c603e","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-05-20T15:30:21Z","title_canon_sha256":"fa90fffaba4c029aa6db147fe4b98b9ee1421fa2bbbf524c80957d01a63eeffe"},"schema_version":"1.0","source":{"id":"1305.4556","kind":"arxiv","version":1}},"canonical_sha256":"0dc1faac8deef0afefca67216d6b25db12c9e62fc54090a717c75a87bd882635","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0dc1faac8deef0afefca67216d6b25db12c9e62fc54090a717c75a87bd882635","first_computed_at":"2026-05-18T01:49:48.718635Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:49:48.718635Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5eMm0KC11yxje5kVv4FXYgQ2tD0ErJmfrSclyrFUZh8djHPmhAEWj5AujA4t3S0T9fTcwY4LXghjX5LQ4iDWAA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:49:48.719117Z","signed_message":"canonical_sha256_bytes"},"source_id":"1305.4556","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:48aa13c7d5be9e8b939e896c6b71cb6c147be2bc0d6a7600265471a8105cd059","sha256:a1119682a3b0ace9e872332cfbc9b67f2f302b8bcb59df52b4b198295ddfff59"],"state_sha256":"d2f8368b0e08e98935ae31259fce89eae9ac0f47ac66a52f4f54d7a811817b37"}