{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:RDFXYCYRXTFLGBDPKTSI3QR2M2","short_pith_number":"pith:RDFXYCYR","schema_version":"1.0","canonical_sha256":"88cb7c0b11bccab3046f54e48dc23a6695714dbd52c6ddc448b0cfb4fcb1bab3","source":{"kind":"arxiv","id":"cond-mat/9509153","version":1},"attestation_state":"computed","paper":{"title":"Adiabatic Dynamics of Superconducting Quantum Point Contacts","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"A.Bardas (SUNY at Stony Brook), D. AVERIN","submitted_at":"1995-09-25T20:50:21Z","abstract_excerpt":"Starting from the quasiclassical equations for non-equilibrium Green's functions we derive a simple kinetic equation that governs ac Josephson effect in a superconducting quantum point contact at small bias voltages. In contrast to existing approaches the kinetic equation is valid for voltages with arbitrary time dependence. We use this equation to calculate frequency-dependent linear conductance, and dc $I\\!-\\!V$ characteristics with and without microwave radiation for resistively shunted quantum point contacts. A novel feature of the $I\\!-\\!V$ characteristics is the excess current $2I_c/\\pi$"},"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":"cond-mat/9509153","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1995-09-25T20:50:21Z","cross_cats_sorted":[],"title_canon_sha256":"30229c457d252de9ac4a5db4b328e4db753ffa82a03a47c1f5362026093d23b1","abstract_canon_sha256":"9be371a47c6e03bf75530cffa09a149ce5f98ba224f2d7bfbfc9e1a4716a19ef"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:58:40.439550Z","signature_b64":"+vG2BYHtcqjNnqu1pD3P3WGY/dlYNGptuhAeDG4s0vUvegY3gxuHvuvnTVgqpWsEvgct9CUqPqAiNuB7enAoCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"88cb7c0b11bccab3046f54e48dc23a6695714dbd52c6ddc448b0cfb4fcb1bab3","last_reissued_at":"2026-07-04T15:58:40.439185Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:58:40.439185Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Adiabatic Dynamics of Superconducting Quantum Point Contacts","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"A.Bardas (SUNY at Stony Brook), D. AVERIN","submitted_at":"1995-09-25T20:50:21Z","abstract_excerpt":"Starting from the quasiclassical equations for non-equilibrium Green's functions we derive a simple kinetic equation that governs ac Josephson effect in a superconducting quantum point contact at small bias voltages. In contrast to existing approaches the kinetic equation is valid for voltages with arbitrary time dependence. We use this equation to calculate frequency-dependent linear conductance, and dc $I\\!-\\!V$ characteristics with and without microwave radiation for resistively shunted quantum point contacts. A novel feature of the $I\\!-\\!V$ characteristics is the excess current $2I_c/\\pi$"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9509153","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/cond-mat/9509153/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":"cond-mat/9509153","created_at":"2026-07-04T15:58:40.439243+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9509153v1","created_at":"2026-07-04T15:58:40.439243+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9509153","created_at":"2026-07-04T15:58:40.439243+00:00"},{"alias_kind":"pith_short_12","alias_value":"RDFXYCYRXTFL","created_at":"2026-07-04T15:58:40.439243+00:00"},{"alias_kind":"pith_short_16","alias_value":"RDFXYCYRXTFLGBDP","created_at":"2026-07-04T15:58:40.439243+00:00"},{"alias_kind":"pith_short_8","alias_value":"RDFXYCYR","created_at":"2026-07-04T15:58:40.439243+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/RDFXYCYRXTFLGBDPKTSI3QR2M2","json":"https://pith.science/pith/RDFXYCYRXTFLGBDPKTSI3QR2M2.json","graph_json":"https://pith.science/api/pith-number/RDFXYCYRXTFLGBDPKTSI3QR2M2/graph.json","events_json":"https://pith.science/api/pith-number/RDFXYCYRXTFLGBDPKTSI3QR2M2/events.json","paper":"https://pith.science/paper/RDFXYCYR"},"agent_actions":{"view_html":"https://pith.science/pith/RDFXYCYRXTFLGBDPKTSI3QR2M2","download_json":"https://pith.science/pith/RDFXYCYRXTFLGBDPKTSI3QR2M2.json","view_paper":"https://pith.science/paper/RDFXYCYR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9509153&json=true","fetch_graph":"https://pith.science/api/pith-number/RDFXYCYRXTFLGBDPKTSI3QR2M2/graph.json","fetch_events":"https://pith.science/api/pith-number/RDFXYCYRXTFLGBDPKTSI3QR2M2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RDFXYCYRXTFLGBDPKTSI3QR2M2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RDFXYCYRXTFLGBDPKTSI3QR2M2/action/storage_attestation","attest_author":"https://pith.science/pith/RDFXYCYRXTFLGBDPKTSI3QR2M2/action/author_attestation","sign_citation":"https://pith.science/pith/RDFXYCYRXTFLGBDPKTSI3QR2M2/action/citation_signature","submit_replication":"https://pith.science/pith/RDFXYCYRXTFLGBDPKTSI3QR2M2/action/replication_record"}},"created_at":"2026-07-04T15:58:40.439243+00:00","updated_at":"2026-07-04T15:58:40.439243+00:00"}