{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:SBE2ZVUVJNJHKSOHOVS2AW3O77","short_pith_number":"pith:SBE2ZVUV","schema_version":"1.0","canonical_sha256":"9049acd6954b527549c77565a05b6effc43c485d9846fd195830d0df97c8e797","source":{"kind":"arxiv","id":"1312.5147","version":1},"attestation_state":"computed","paper":{"title":"Collective-field-corrected strong field approximation for laser-irradiated metal clusters","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atm-clus","quant-ph"],"primary_cat":"physics.atom-ph","authors_text":"D. Bauer, Th. Keil","submitted_at":"2013-12-18T14:12:21Z","abstract_excerpt":"The strong field approximation (SFA) formulated in terms of so-called \"quantum orbits\" led to much insight into intense-laser driven ionization dynamics. In plain SFA, the emitted electron is treated as a free electron in the laser field alone. However, with improving experimental techniques and more advanced numerical simulations it becomes more and more obvious that the plain SFA misses interesting effects even on a qualitative level. Examples are holographic side lobes, the low-energy structure, radial patterns in photoelectron spectra at low kinetic energies, and strongly rotated angular d"},"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":"1312.5147","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.atom-ph","submitted_at":"2013-12-18T14:12:21Z","cross_cats_sorted":["physics.atm-clus","quant-ph"],"title_canon_sha256":"167a4c0f097b92f911e3ce55571e3398005a3a15a74fefc2132d5a8a10823876","abstract_canon_sha256":"7c0ead7415078a3f68ad5239d10454000d6cd154a66afd5c0e37355059121c4b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:30:18.126835Z","signature_b64":"da6ncwqSWRSHDtqzqMjIhkJ+QhHoCP/L0o5NwHQ5n2nDQDWom6giaDC0OAxjvhjsvKVHQ48HQf5z+5WWlH1kBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9049acd6954b527549c77565a05b6effc43c485d9846fd195830d0df97c8e797","last_reissued_at":"2026-05-18T00:30:18.126132Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:30:18.126132Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Collective-field-corrected strong field approximation for laser-irradiated metal clusters","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.atm-clus","quant-ph"],"primary_cat":"physics.atom-ph","authors_text":"D. Bauer, Th. Keil","submitted_at":"2013-12-18T14:12:21Z","abstract_excerpt":"The strong field approximation (SFA) formulated in terms of so-called \"quantum orbits\" led to much insight into intense-laser driven ionization dynamics. In plain SFA, the emitted electron is treated as a free electron in the laser field alone. However, with improving experimental techniques and more advanced numerical simulations it becomes more and more obvious that the plain SFA misses interesting effects even on a qualitative level. Examples are holographic side lobes, the low-energy structure, radial patterns in photoelectron spectra at low kinetic energies, and strongly rotated angular d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1312.5147","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":"1312.5147","created_at":"2026-05-18T00:30:18.126240+00:00"},{"alias_kind":"arxiv_version","alias_value":"1312.5147v1","created_at":"2026-05-18T00:30:18.126240+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1312.5147","created_at":"2026-05-18T00:30:18.126240+00:00"},{"alias_kind":"pith_short_12","alias_value":"SBE2ZVUVJNJH","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_16","alias_value":"SBE2ZVUVJNJHKSOH","created_at":"2026-05-18T12:27:59.945178+00:00"},{"alias_kind":"pith_short_8","alias_value":"SBE2ZVUV","created_at":"2026-05-18T12:27:59.945178+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/SBE2ZVUVJNJHKSOHOVS2AW3O77","json":"https://pith.science/pith/SBE2ZVUVJNJHKSOHOVS2AW3O77.json","graph_json":"https://pith.science/api/pith-number/SBE2ZVUVJNJHKSOHOVS2AW3O77/graph.json","events_json":"https://pith.science/api/pith-number/SBE2ZVUVJNJHKSOHOVS2AW3O77/events.json","paper":"https://pith.science/paper/SBE2ZVUV"},"agent_actions":{"view_html":"https://pith.science/pith/SBE2ZVUVJNJHKSOHOVS2AW3O77","download_json":"https://pith.science/pith/SBE2ZVUVJNJHKSOHOVS2AW3O77.json","view_paper":"https://pith.science/paper/SBE2ZVUV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1312.5147&json=true","fetch_graph":"https://pith.science/api/pith-number/SBE2ZVUVJNJHKSOHOVS2AW3O77/graph.json","fetch_events":"https://pith.science/api/pith-number/SBE2ZVUVJNJHKSOHOVS2AW3O77/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SBE2ZVUVJNJHKSOHOVS2AW3O77/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SBE2ZVUVJNJHKSOHOVS2AW3O77/action/storage_attestation","attest_author":"https://pith.science/pith/SBE2ZVUVJNJHKSOHOVS2AW3O77/action/author_attestation","sign_citation":"https://pith.science/pith/SBE2ZVUVJNJHKSOHOVS2AW3O77/action/citation_signature","submit_replication":"https://pith.science/pith/SBE2ZVUVJNJHKSOHOVS2AW3O77/action/replication_record"}},"created_at":"2026-05-18T00:30:18.126240+00:00","updated_at":"2026-05-18T00:30:18.126240+00:00"}