{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:QTFQTOQ3MDZPDKHMTJEMHPR7KY","short_pith_number":"pith:QTFQTOQ3","schema_version":"1.0","canonical_sha256":"84cb09ba1b60f2f1a8ec9a48c3be3f56391d6560a78ea3a6683fc7aeb20399f7","source":{"kind":"arxiv","id":"1806.02568","version":2},"attestation_state":"computed","paper":{"title":"Adiabatic perturbation theory of nonequilibrium light-controlled superconductivity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Andrea Secchi, Marco Polini","submitted_at":"2018-06-07T09:05:24Z","abstract_excerpt":"Recent experiments, in which Terahertz (THz) light has been used to induce nonequilibrium superconducting states, have raised a number of intriguing fundamental questions. Theoretically, these experiments are most often described within the Floquet formalism, which suffers a number of well-known limitations (e.g. Floquet heating). Alternative approaches rely on heavy numerical methods. In this Article we develop an analytical theory of nonequilibrium superconductivity that combines path integrals on the Kostantinov-Perel' time contour with adiabatic perturbation theory [G. Rigolin, G. Ortiz, a"},"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":"1806.02568","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2018-06-07T09:05:24Z","cross_cats_sorted":[],"title_canon_sha256":"1da7cf3d501e69ddafab24b53316b5e430568f43d27040fe3ad1141c2bfaa915","abstract_canon_sha256":"0fb3af0c436bd723a49ad368dbe446dd6117c502ff2d79d498e49cbc35104c6c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:02:44.767307Z","signature_b64":"7xf67EnD+KowGSR1/EIQaEaiHyaBRdU2rnC8iQsjzafGd/VS9gaOs/FhTn2yRtO7LfB4q0Y9kFCbxWYqzpMFCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"84cb09ba1b60f2f1a8ec9a48c3be3f56391d6560a78ea3a6683fc7aeb20399f7","last_reissued_at":"2026-05-18T00:02:44.766855Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:02:44.766855Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Adiabatic perturbation theory of nonequilibrium light-controlled superconductivity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Andrea Secchi, Marco Polini","submitted_at":"2018-06-07T09:05:24Z","abstract_excerpt":"Recent experiments, in which Terahertz (THz) light has been used to induce nonequilibrium superconducting states, have raised a number of intriguing fundamental questions. Theoretically, these experiments are most often described within the Floquet formalism, which suffers a number of well-known limitations (e.g. Floquet heating). Alternative approaches rely on heavy numerical methods. In this Article we develop an analytical theory of nonequilibrium superconductivity that combines path integrals on the Kostantinov-Perel' time contour with adiabatic perturbation theory [G. Rigolin, G. Ortiz, a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1806.02568","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":"1806.02568","created_at":"2026-05-18T00:02:44.766914+00:00"},{"alias_kind":"arxiv_version","alias_value":"1806.02568v2","created_at":"2026-05-18T00:02:44.766914+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1806.02568","created_at":"2026-05-18T00:02:44.766914+00:00"},{"alias_kind":"pith_short_12","alias_value":"QTFQTOQ3MDZP","created_at":"2026-05-18T12:32:46.962924+00:00"},{"alias_kind":"pith_short_16","alias_value":"QTFQTOQ3MDZPDKHM","created_at":"2026-05-18T12:32:46.962924+00:00"},{"alias_kind":"pith_short_8","alias_value":"QTFQTOQ3","created_at":"2026-05-18T12:32:46.962924+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/QTFQTOQ3MDZPDKHMTJEMHPR7KY","json":"https://pith.science/pith/QTFQTOQ3MDZPDKHMTJEMHPR7KY.json","graph_json":"https://pith.science/api/pith-number/QTFQTOQ3MDZPDKHMTJEMHPR7KY/graph.json","events_json":"https://pith.science/api/pith-number/QTFQTOQ3MDZPDKHMTJEMHPR7KY/events.json","paper":"https://pith.science/paper/QTFQTOQ3"},"agent_actions":{"view_html":"https://pith.science/pith/QTFQTOQ3MDZPDKHMTJEMHPR7KY","download_json":"https://pith.science/pith/QTFQTOQ3MDZPDKHMTJEMHPR7KY.json","view_paper":"https://pith.science/paper/QTFQTOQ3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1806.02568&json=true","fetch_graph":"https://pith.science/api/pith-number/QTFQTOQ3MDZPDKHMTJEMHPR7KY/graph.json","fetch_events":"https://pith.science/api/pith-number/QTFQTOQ3MDZPDKHMTJEMHPR7KY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QTFQTOQ3MDZPDKHMTJEMHPR7KY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QTFQTOQ3MDZPDKHMTJEMHPR7KY/action/storage_attestation","attest_author":"https://pith.science/pith/QTFQTOQ3MDZPDKHMTJEMHPR7KY/action/author_attestation","sign_citation":"https://pith.science/pith/QTFQTOQ3MDZPDKHMTJEMHPR7KY/action/citation_signature","submit_replication":"https://pith.science/pith/QTFQTOQ3MDZPDKHMTJEMHPR7KY/action/replication_record"}},"created_at":"2026-05-18T00:02:44.766914+00:00","updated_at":"2026-05-18T00:02:44.766914+00:00"}