{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:U7ESKXKIVYZFBZNUUGPBXB3GEU","short_pith_number":"pith:U7ESKXKI","schema_version":"1.0","canonical_sha256":"a7c9255d48ae3250e5b4a19e1b87662524c6a1f394d11c501f951a392a9c1844","source":{"kind":"arxiv","id":"1609.05023","version":1},"attestation_state":"computed","paper":{"title":"Finite time St\\\"uckelberg interferometry with nanomechanical modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Eva M. Weig, Hugo Ribeiro, Johannes K\\\"olbl, Maximilian J. Seitner, Thomas Faust","submitted_at":"2016-09-16T12:32:45Z","abstract_excerpt":"St\\\"uckelberg interferometry describes the interference of two strongly coupled modes during a double passage through an avoided energy level crossing. In this work, we experimentally investigate finite time effects in St\\\"uckelberg interference and provide an exact analytical solution of the St\\\"uckelberg problem. Approximating this solution in distinct limits reveals uncharted parameter regimes of St\\\"uckelberg interferometry. Experimentally, we study these regimes using a purely classical, strongly coupled nanomechanical two-mode system of high quality factor. The classical two-mode system "},"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":"1609.05023","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-09-16T12:32:45Z","cross_cats_sorted":[],"title_canon_sha256":"ca0a8384ae36b3ed3081d2e5b710296a6e023a328653edad7a142247c0bff036","abstract_canon_sha256":"77611b23afe08c0044e74abb60fc4766b0f61bad79489d17c45a8ec593f87bdd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:49:32.077366Z","signature_b64":"4mTfWYLerrXmVjTV7L+ZBv/zNYBPNp9/KmLCdZQx2MNiGe5oP4mD8C3h67VOyE1e+BacV257lQ/rFleikjaZCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a7c9255d48ae3250e5b4a19e1b87662524c6a1f394d11c501f951a392a9c1844","last_reissued_at":"2026-05-18T00:49:32.076695Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:49:32.076695Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite time St\\\"uckelberg interferometry with nanomechanical modes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Eva M. Weig, Hugo Ribeiro, Johannes K\\\"olbl, Maximilian J. Seitner, Thomas Faust","submitted_at":"2016-09-16T12:32:45Z","abstract_excerpt":"St\\\"uckelberg interferometry describes the interference of two strongly coupled modes during a double passage through an avoided energy level crossing. In this work, we experimentally investigate finite time effects in St\\\"uckelberg interference and provide an exact analytical solution of the St\\\"uckelberg problem. Approximating this solution in distinct limits reveals uncharted parameter regimes of St\\\"uckelberg interferometry. Experimentally, we study these regimes using a purely classical, strongly coupled nanomechanical two-mode system of high quality factor. The classical two-mode system "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1609.05023","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":"1609.05023","created_at":"2026-05-18T00:49:32.076804+00:00"},{"alias_kind":"arxiv_version","alias_value":"1609.05023v1","created_at":"2026-05-18T00:49:32.076804+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1609.05023","created_at":"2026-05-18T00:49:32.076804+00:00"},{"alias_kind":"pith_short_12","alias_value":"U7ESKXKIVYZF","created_at":"2026-05-18T12:30:46.583412+00:00"},{"alias_kind":"pith_short_16","alias_value":"U7ESKXKIVYZFBZNU","created_at":"2026-05-18T12:30:46.583412+00:00"},{"alias_kind":"pith_short_8","alias_value":"U7ESKXKI","created_at":"2026-05-18T12:30:46.583412+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/U7ESKXKIVYZFBZNUUGPBXB3GEU","json":"https://pith.science/pith/U7ESKXKIVYZFBZNUUGPBXB3GEU.json","graph_json":"https://pith.science/api/pith-number/U7ESKXKIVYZFBZNUUGPBXB3GEU/graph.json","events_json":"https://pith.science/api/pith-number/U7ESKXKIVYZFBZNUUGPBXB3GEU/events.json","paper":"https://pith.science/paper/U7ESKXKI"},"agent_actions":{"view_html":"https://pith.science/pith/U7ESKXKIVYZFBZNUUGPBXB3GEU","download_json":"https://pith.science/pith/U7ESKXKIVYZFBZNUUGPBXB3GEU.json","view_paper":"https://pith.science/paper/U7ESKXKI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1609.05023&json=true","fetch_graph":"https://pith.science/api/pith-number/U7ESKXKIVYZFBZNUUGPBXB3GEU/graph.json","fetch_events":"https://pith.science/api/pith-number/U7ESKXKIVYZFBZNUUGPBXB3GEU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/U7ESKXKIVYZFBZNUUGPBXB3GEU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/U7ESKXKIVYZFBZNUUGPBXB3GEU/action/storage_attestation","attest_author":"https://pith.science/pith/U7ESKXKIVYZFBZNUUGPBXB3GEU/action/author_attestation","sign_citation":"https://pith.science/pith/U7ESKXKIVYZFBZNUUGPBXB3GEU/action/citation_signature","submit_replication":"https://pith.science/pith/U7ESKXKIVYZFBZNUUGPBXB3GEU/action/replication_record"}},"created_at":"2026-05-18T00:49:32.076804+00:00","updated_at":"2026-05-18T00:49:32.076804+00:00"}