{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:5ZLLAHZVWNU32XVFVV3IXB7DBC","short_pith_number":"pith:5ZLLAHZV","schema_version":"1.0","canonical_sha256":"ee56b01f35b369bd5ea5ad768b87e308957a0adaac30c45a0596cb4d317b70d9","source":{"kind":"arxiv","id":"2608.11189","version":1},"attestation_state":"computed","paper":{"title":"Floquet Green's functions for lattice electrons driven by Gaussian quantum light","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.optics","quant-ph"],"primary_cat":"cond-mat.str-el","authors_text":"Atsushi Ono","submitted_at":"2026-08-11T17:50:00Z","abstract_excerpt":"We formulate Floquet Green's functions for noninteracting single-band lattice electrons driven by a reservoir-stabilized single-mode Gaussian quantum light source. The source is prescribed externally and is not updated by the many-electron polarization, while an active electronic probe still conditions the source evolution through the Peierls coupling. The two time arguments of a Green's function share one source history: the lesser and greater components are obtained by convolving a shared-history four-endpoint kernel with the continuous bath kernels before the final source trace, while the b"},"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":"2608.11189","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2026-08-11T17:50:00Z","cross_cats_sorted":["cond-mat.mes-hall","physics.optics","quant-ph"],"title_canon_sha256":"41f31f4dc343b974ab2c600ac883f7a349f99cb2e38321f66e94eb7fe7854dc5","abstract_canon_sha256":"c01d17b235373d4a047a3a369ba19af16c6989858c9e3212109d05190245a4a2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-12T01:24:46.724327Z","signature_b64":"tALkLN5MgQUm0ZHC4Z0Bhyc7DmONKPJmCgGgz6nc5qdvzDJcGCug83SdGHoJb5pNiTHKa0rA05ewrxRHpUNLBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ee56b01f35b369bd5ea5ad768b87e308957a0adaac30c45a0596cb4d317b70d9","last_reissued_at":"2026-08-12T01:24:46.722696Z","signature_status":"signed_v1","first_computed_at":"2026-08-12T01:24:46.722696Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Floquet Green's functions for lattice electrons driven by Gaussian quantum light","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.optics","quant-ph"],"primary_cat":"cond-mat.str-el","authors_text":"Atsushi Ono","submitted_at":"2026-08-11T17:50:00Z","abstract_excerpt":"We formulate Floquet Green's functions for noninteracting single-band lattice electrons driven by a reservoir-stabilized single-mode Gaussian quantum light source. The source is prescribed externally and is not updated by the many-electron polarization, while an active electronic probe still conditions the source evolution through the Peierls coupling. The two time arguments of a Green's function share one source history: the lesser and greater components are obtained by convolving a shared-history four-endpoint kernel with the continuous bath kernels before the final source trace, while the b"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.11189","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2608.11189/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2608.11189","created_at":"2026-08-12T01:24:46.726538+00:00"},{"alias_kind":"arxiv_version","alias_value":"2608.11189v1","created_at":"2026-08-12T01:24:46.726538+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.11189","created_at":"2026-08-12T01:24:46.726538+00:00"},{"alias_kind":"pith_short_12","alias_value":"5ZLLAHZVWNU3","created_at":"2026-08-12T01:24:46.726538+00:00"},{"alias_kind":"pith_short_16","alias_value":"5ZLLAHZVWNU32XVF","created_at":"2026-08-12T01:24:46.726538+00:00"},{"alias_kind":"pith_short_8","alias_value":"5ZLLAHZV","created_at":"2026-08-12T01:24:46.726538+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/5ZLLAHZVWNU32XVFVV3IXB7DBC","json":"https://pith.science/pith/5ZLLAHZVWNU32XVFVV3IXB7DBC.json","graph_json":"https://pith.science/api/pith-number/5ZLLAHZVWNU32XVFVV3IXB7DBC/graph.json","events_json":"https://pith.science/api/pith-number/5ZLLAHZVWNU32XVFVV3IXB7DBC/events.json","paper":"https://pith.science/paper/5ZLLAHZV"},"agent_actions":{"view_html":"https://pith.science/pith/5ZLLAHZVWNU32XVFVV3IXB7DBC","download_json":"https://pith.science/pith/5ZLLAHZVWNU32XVFVV3IXB7DBC.json","view_paper":"https://pith.science/paper/5ZLLAHZV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2608.11189&json=true","fetch_graph":"https://pith.science/api/pith-number/5ZLLAHZVWNU32XVFVV3IXB7DBC/graph.json","fetch_events":"https://pith.science/api/pith-number/5ZLLAHZVWNU32XVFVV3IXB7DBC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5ZLLAHZVWNU32XVFVV3IXB7DBC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5ZLLAHZVWNU32XVFVV3IXB7DBC/action/storage_attestation","attest_author":"https://pith.science/pith/5ZLLAHZVWNU32XVFVV3IXB7DBC/action/author_attestation","sign_citation":"https://pith.science/pith/5ZLLAHZVWNU32XVFVV3IXB7DBC/action/citation_signature","submit_replication":"https://pith.science/pith/5ZLLAHZVWNU32XVFVV3IXB7DBC/action/replication_record"}},"created_at":"2026-08-12T01:24:46.726538+00:00","updated_at":"2026-08-12T01:24:46.726538+00:00"}