{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:VSN7NR537VEQSJBTMDRP32EYSE","short_pith_number":"pith:VSN7NR53","schema_version":"1.0","canonical_sha256":"ac9bf6c7bbfd4909243360e2fde8989133e8bad6ace2a037775dbe443edda5ef","source":{"kind":"arxiv","id":"1003.5785","version":1},"attestation_state":"computed","paper":{"title":"Transport properties of \\nu=1 quantum Hall bilayers. Phenomenological description","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"D. V. Fil, S. I. Shevchenko","submitted_at":"2010-03-30T10:40:52Z","abstract_excerpt":"We propose a phenomenological model that describes counterflow and drag experiments with quantum Hall bilayers in a \\nu_T=1 state. We consider the system consisting of statistically distributed areas with local total filling factors \\nu_{T1}>1 and \\nu_{T2}<1. The excess or deficit of electrons  in a given area results in an appearance of vortex excitations. The vortices in quantum Hall bilayers are charged. They are responsible for a decay of the exciton supercurrent, and, at the same time, contribute to the conductivity directly. The experimental temperature dependence of the counterflow and "},"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":"1003.5785","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2010-03-30T10:40:52Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"374bcf16ad828942ef66f791b28c7b4104063ebd76b511f1c4ad49249e13a438","abstract_canon_sha256":"f75592ca777feb1a435aa70f622636f6cc80265fd5542146a16868b9e614a949"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:08:15.801572Z","signature_b64":"ZDm7b+MSYWih/6rxZaU8Qxwumbh7+4+eSkI6m9cF9vRQlj1Ieozykx+ZIW+yUshMLi/ykOuVGgexl7qUiGvEBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ac9bf6c7bbfd4909243360e2fde8989133e8bad6ace2a037775dbe443edda5ef","last_reissued_at":"2026-05-18T02:08:15.800952Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:08:15.800952Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Transport properties of \\nu=1 quantum Hall bilayers. Phenomenological description","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.str-el","authors_text":"D. V. Fil, S. I. Shevchenko","submitted_at":"2010-03-30T10:40:52Z","abstract_excerpt":"We propose a phenomenological model that describes counterflow and drag experiments with quantum Hall bilayers in a \\nu_T=1 state. We consider the system consisting of statistically distributed areas with local total filling factors \\nu_{T1}>1 and \\nu_{T2}<1. The excess or deficit of electrons  in a given area results in an appearance of vortex excitations. The vortices in quantum Hall bilayers are charged. They are responsible for a decay of the exciton supercurrent, and, at the same time, contribute to the conductivity directly. The experimental temperature dependence of the counterflow and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1003.5785","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":"1003.5785","created_at":"2026-05-18T02:08:15.801041+00:00"},{"alias_kind":"arxiv_version","alias_value":"1003.5785v1","created_at":"2026-05-18T02:08:15.801041+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1003.5785","created_at":"2026-05-18T02:08:15.801041+00:00"},{"alias_kind":"pith_short_12","alias_value":"VSN7NR537VEQ","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_16","alias_value":"VSN7NR537VEQSJBT","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_8","alias_value":"VSN7NR53","created_at":"2026-05-18T12:26:15.391820+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/VSN7NR537VEQSJBTMDRP32EYSE","json":"https://pith.science/pith/VSN7NR537VEQSJBTMDRP32EYSE.json","graph_json":"https://pith.science/api/pith-number/VSN7NR537VEQSJBTMDRP32EYSE/graph.json","events_json":"https://pith.science/api/pith-number/VSN7NR537VEQSJBTMDRP32EYSE/events.json","paper":"https://pith.science/paper/VSN7NR53"},"agent_actions":{"view_html":"https://pith.science/pith/VSN7NR537VEQSJBTMDRP32EYSE","download_json":"https://pith.science/pith/VSN7NR537VEQSJBTMDRP32EYSE.json","view_paper":"https://pith.science/paper/VSN7NR53","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1003.5785&json=true","fetch_graph":"https://pith.science/api/pith-number/VSN7NR537VEQSJBTMDRP32EYSE/graph.json","fetch_events":"https://pith.science/api/pith-number/VSN7NR537VEQSJBTMDRP32EYSE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VSN7NR537VEQSJBTMDRP32EYSE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VSN7NR537VEQSJBTMDRP32EYSE/action/storage_attestation","attest_author":"https://pith.science/pith/VSN7NR537VEQSJBTMDRP32EYSE/action/author_attestation","sign_citation":"https://pith.science/pith/VSN7NR537VEQSJBTMDRP32EYSE/action/citation_signature","submit_replication":"https://pith.science/pith/VSN7NR537VEQSJBTMDRP32EYSE/action/replication_record"}},"created_at":"2026-05-18T02:08:15.801041+00:00","updated_at":"2026-05-18T02:08:15.801041+00:00"}