{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:R7VVRIF7P2N5J4KPNLVB22U5HF","short_pith_number":"pith:R7VVRIF7","schema_version":"1.0","canonical_sha256":"8feb58a0bf7e9bd4f14f6aea1d6a9d396563e84481b47df836ac6d482b402793","source":{"kind":"arxiv","id":"1803.04952","version":2},"attestation_state":"computed","paper":{"title":"Strong-field control and enhancement of chiral response in bi-elliptical high-order harmonic generation: an analytical model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"David Ayuso, Olga Smirnova, Piero Decleva, Serguei Patchkovskii","submitted_at":"2018-03-13T17:35:31Z","abstract_excerpt":"The generation of high-order harmonics in a medium of chiral molecules driven by intense bi-elliptical laser fields can lead to strong chiroptical response in a broad range of harmonic numbers and ellipticities [D. Ayuso et al, J. Phys. B 51, 06LT01 (2018)]. Here we present a comprehensive analytical model that can describe the most relevant features arising in the high-order harmonic spectra of chiral molecules driven by strong bi-elliptical fields. Our model recovers the physical picture underlying chiral high-order harmonic generation based on ultrafast chiral hole motion and identifies the"},"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":"1803.04952","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.optics","submitted_at":"2018-03-13T17:35:31Z","cross_cats_sorted":[],"title_canon_sha256":"652b1017044394162b9f472298c18c512fef0ba192fa8ce3321f9b18bbdb85be","abstract_canon_sha256":"871029863c385b59b60eff719d92528845716a014f51a52227cbe440dd569e74"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:11:37.482567Z","signature_b64":"mkUAY7x3UD07wLWeecV9l85ekiLS5Lq7dct+CJU5j8VM+KegfQ5/BD2zoRMljH13YsLREVbNC5Dddiz+prBgDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8feb58a0bf7e9bd4f14f6aea1d6a9d396563e84481b47df836ac6d482b402793","last_reissued_at":"2026-05-18T00:11:37.481843Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:11:37.481843Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Strong-field control and enhancement of chiral response in bi-elliptical high-order harmonic generation: an analytical model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.optics","authors_text":"David Ayuso, Olga Smirnova, Piero Decleva, Serguei Patchkovskii","submitted_at":"2018-03-13T17:35:31Z","abstract_excerpt":"The generation of high-order harmonics in a medium of chiral molecules driven by intense bi-elliptical laser fields can lead to strong chiroptical response in a broad range of harmonic numbers and ellipticities [D. Ayuso et al, J. Phys. B 51, 06LT01 (2018)]. Here we present a comprehensive analytical model that can describe the most relevant features arising in the high-order harmonic spectra of chiral molecules driven by strong bi-elliptical fields. Our model recovers the physical picture underlying chiral high-order harmonic generation based on ultrafast chiral hole motion and identifies the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1803.04952","kind":"arxiv","version":2},"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":"1803.04952","created_at":"2026-05-18T00:11:37.481962+00:00"},{"alias_kind":"arxiv_version","alias_value":"1803.04952v2","created_at":"2026-05-18T00:11:37.481962+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1803.04952","created_at":"2026-05-18T00:11:37.481962+00:00"},{"alias_kind":"pith_short_12","alias_value":"R7VVRIF7P2N5","created_at":"2026-05-18T12:32:50.500415+00:00"},{"alias_kind":"pith_short_16","alias_value":"R7VVRIF7P2N5J4KP","created_at":"2026-05-18T12:32:50.500415+00:00"},{"alias_kind":"pith_short_8","alias_value":"R7VVRIF7","created_at":"2026-05-18T12:32:50.500415+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/R7VVRIF7P2N5J4KPNLVB22U5HF","json":"https://pith.science/pith/R7VVRIF7P2N5J4KPNLVB22U5HF.json","graph_json":"https://pith.science/api/pith-number/R7VVRIF7P2N5J4KPNLVB22U5HF/graph.json","events_json":"https://pith.science/api/pith-number/R7VVRIF7P2N5J4KPNLVB22U5HF/events.json","paper":"https://pith.science/paper/R7VVRIF7"},"agent_actions":{"view_html":"https://pith.science/pith/R7VVRIF7P2N5J4KPNLVB22U5HF","download_json":"https://pith.science/pith/R7VVRIF7P2N5J4KPNLVB22U5HF.json","view_paper":"https://pith.science/paper/R7VVRIF7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1803.04952&json=true","fetch_graph":"https://pith.science/api/pith-number/R7VVRIF7P2N5J4KPNLVB22U5HF/graph.json","fetch_events":"https://pith.science/api/pith-number/R7VVRIF7P2N5J4KPNLVB22U5HF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/R7VVRIF7P2N5J4KPNLVB22U5HF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/R7VVRIF7P2N5J4KPNLVB22U5HF/action/storage_attestation","attest_author":"https://pith.science/pith/R7VVRIF7P2N5J4KPNLVB22U5HF/action/author_attestation","sign_citation":"https://pith.science/pith/R7VVRIF7P2N5J4KPNLVB22U5HF/action/citation_signature","submit_replication":"https://pith.science/pith/R7VVRIF7P2N5J4KPNLVB22U5HF/action/replication_record"}},"created_at":"2026-05-18T00:11:37.481962+00:00","updated_at":"2026-05-18T00:11:37.481962+00:00"}