{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1993:WB56DP55WXCSYX6ZZFCQGKIBEB","short_pith_number":"pith:WB56DP55","schema_version":"1.0","canonical_sha256":"b07be1bfbdb5c52c5fd9c945032901205e6c97f6c1ab0b45163c9394034531cf","source":{"kind":"arxiv","id":"chao-dyn/9305011","version":1},"attestation_state":"computed","paper":{"title":"Threshold Analysis for the Inverse ac Josephson Effect","license":"","headline":"","cross_cats":["nlin.CD"],"primary_cat":"chao-dyn","authors_text":"B. A. Malomed (Dept. Appl. Math., G. Filatrella (Phys. Inst., R. D. Parmentier (Dept. Phys., Tel Aviv Univ.), Univ. Salerno), Univ. Tuebingen)","submitted_at":"1993-05-28T12:37:00Z","abstract_excerpt":"The inverse ac Josephson effect involves rf-induced (Shapiro) steps that cross over the zero-current axis; the phenomenon is of interest in voltage standard applications. The standard analysis of the step height in current, which yields the well-known Bessel-function dependence on an effective ac drive amplitude, is valid only when the drive frequency is large compared with the junction plasma frequency or when the drive amplitude is large compared with the zero-voltage Josephson current. Using a first-order Krylov-Bogoliubov power-balance approach we derive an expression for the threshold val"},"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":"chao-dyn/9305011","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"chao-dyn","submitted_at":"1993-05-28T12:37:00Z","cross_cats_sorted":["nlin.CD"],"title_canon_sha256":"19db06828e1d9260841c7ef66be9c8cc18d9c8ec1bcb5113acce2cddb8cafd6c","abstract_canon_sha256":"22be8b6fde43ae17b12d7007478df128bf98f52d715f1aeac8c41d9001a5aeee"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:55:10.119204Z","signature_b64":"vpsbJpOosEbWHSlsVwjsEVvNLpMKTI4BdVJT+vtNcNBMjSb4/xBSt2PusO4iM9E1lzh0HjcWN31wfEbtabrUCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b07be1bfbdb5c52c5fd9c945032901205e6c97f6c1ab0b45163c9394034531cf","last_reissued_at":"2026-07-04T15:55:10.118790Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:55:10.118790Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Threshold Analysis for the Inverse ac Josephson Effect","license":"","headline":"","cross_cats":["nlin.CD"],"primary_cat":"chao-dyn","authors_text":"B. A. Malomed (Dept. Appl. Math., G. Filatrella (Phys. Inst., R. D. Parmentier (Dept. Phys., Tel Aviv Univ.), Univ. Salerno), Univ. Tuebingen)","submitted_at":"1993-05-28T12:37:00Z","abstract_excerpt":"The inverse ac Josephson effect involves rf-induced (Shapiro) steps that cross over the zero-current axis; the phenomenon is of interest in voltage standard applications. The standard analysis of the step height in current, which yields the well-known Bessel-function dependence on an effective ac drive amplitude, is valid only when the drive frequency is large compared with the junction plasma frequency or when the drive amplitude is large compared with the zero-voltage Josephson current. Using a first-order Krylov-Bogoliubov power-balance approach we derive an expression for the threshold val"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"chao-dyn/9305011","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/chao-dyn/9305011/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":"chao-dyn/9305011","created_at":"2026-07-04T15:55:10.118847+00:00"},{"alias_kind":"arxiv_version","alias_value":"chao-dyn/9305011v1","created_at":"2026-07-04T15:55:10.118847+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.chao-dyn/9305011","created_at":"2026-07-04T15:55:10.118847+00:00"},{"alias_kind":"pith_short_12","alias_value":"WB56DP55WXCS","created_at":"2026-07-04T15:55:10.118847+00:00"},{"alias_kind":"pith_short_16","alias_value":"WB56DP55WXCSYX6Z","created_at":"2026-07-04T15:55:10.118847+00:00"},{"alias_kind":"pith_short_8","alias_value":"WB56DP55","created_at":"2026-07-04T15:55:10.118847+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/WB56DP55WXCSYX6ZZFCQGKIBEB","json":"https://pith.science/pith/WB56DP55WXCSYX6ZZFCQGKIBEB.json","graph_json":"https://pith.science/api/pith-number/WB56DP55WXCSYX6ZZFCQGKIBEB/graph.json","events_json":"https://pith.science/api/pith-number/WB56DP55WXCSYX6ZZFCQGKIBEB/events.json","paper":"https://pith.science/paper/WB56DP55"},"agent_actions":{"view_html":"https://pith.science/pith/WB56DP55WXCSYX6ZZFCQGKIBEB","download_json":"https://pith.science/pith/WB56DP55WXCSYX6ZZFCQGKIBEB.json","view_paper":"https://pith.science/paper/WB56DP55","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=chao-dyn/9305011&json=true","fetch_graph":"https://pith.science/api/pith-number/WB56DP55WXCSYX6ZZFCQGKIBEB/graph.json","fetch_events":"https://pith.science/api/pith-number/WB56DP55WXCSYX6ZZFCQGKIBEB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WB56DP55WXCSYX6ZZFCQGKIBEB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WB56DP55WXCSYX6ZZFCQGKIBEB/action/storage_attestation","attest_author":"https://pith.science/pith/WB56DP55WXCSYX6ZZFCQGKIBEB/action/author_attestation","sign_citation":"https://pith.science/pith/WB56DP55WXCSYX6ZZFCQGKIBEB/action/citation_signature","submit_replication":"https://pith.science/pith/WB56DP55WXCSYX6ZZFCQGKIBEB/action/replication_record"}},"created_at":"2026-07-04T15:55:10.118847+00:00","updated_at":"2026-07-04T15:55:10.118847+00:00"}