{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:2LFNGR5P7QLTJEFIAT6IC7PIY3","short_pith_number":"pith:2LFNGR5P","schema_version":"1.0","canonical_sha256":"d2cad347affc173490a804fc817de8c6d23c9addc0f29d7dc28f13b6d8765167","source":{"kind":"arxiv","id":"2607.16315","version":1},"attestation_state":"computed","paper":{"title":"Thermal and viscous contrast in quantum Hall scanning-probe images","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"P. Shubham Parashar","submitted_at":"2026-07-15T02:42:12Z","abstract_excerpt":"Quantum Hall scanning images are often read as maps of a local potential, temperature, or viscosity, whereas a probe records a finite-resolution functional of a transport operator. We formulate this functional using Landau-level projection, a particle-number Ward identity, magnetization-subtracted thermoelectric transport, a hydrodynamic Stokes-Ohm inversion, and finite-tip Fisher information. Two results follow in complementary transport regimes. In the strong-field, sharp-Landau-level regime, the defect-induced thermoelectric and electrical Hall contrasts of a smooth scalar defect obey $\\del"},"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":"2607.16315","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2026-07-15T02:42:12Z","cross_cats_sorted":[],"title_canon_sha256":"344f30638bf07bffbd3ab4247691e5c695d39b6306969005be174dedd7d13a32","abstract_canon_sha256":"023899060ac6752e9a49835cea2bf2b968870c8153ae615a93d07e52953c4741"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-21T00:20:11.850276Z","signature_b64":"WrGLUAZWQYVlxRvXPE69ewSOjtQWOMCexn3oK2Q0ss9C7Aof0i0nQhoBnJTs085qCluwz+eQ7JTIx1ODDXhIBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d2cad347affc173490a804fc817de8c6d23c9addc0f29d7dc28f13b6d8765167","last_reissued_at":"2026-07-21T00:20:11.849424Z","signature_status":"signed_v1","first_computed_at":"2026-07-21T00:20:11.849424Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermal and viscous contrast in quantum Hall scanning-probe images","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"P. Shubham Parashar","submitted_at":"2026-07-15T02:42:12Z","abstract_excerpt":"Quantum Hall scanning images are often read as maps of a local potential, temperature, or viscosity, whereas a probe records a finite-resolution functional of a transport operator. We formulate this functional using Landau-level projection, a particle-number Ward identity, magnetization-subtracted thermoelectric transport, a hydrodynamic Stokes-Ohm inversion, and finite-tip Fisher information. Two results follow in complementary transport regimes. In the strong-field, sharp-Landau-level regime, the defect-induced thermoelectric and electrical Hall contrasts of a smooth scalar defect obey $\\del"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.16315","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/2607.16315/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":"2607.16315","created_at":"2026-07-21T00:20:11.849862+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.16315v1","created_at":"2026-07-21T00:20:11.849862+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.16315","created_at":"2026-07-21T00:20:11.849862+00:00"},{"alias_kind":"pith_short_12","alias_value":"2LFNGR5P7QLT","created_at":"2026-07-21T00:20:11.849862+00:00"},{"alias_kind":"pith_short_16","alias_value":"2LFNGR5P7QLTJEFI","created_at":"2026-07-21T00:20:11.849862+00:00"},{"alias_kind":"pith_short_8","alias_value":"2LFNGR5P","created_at":"2026-07-21T00:20:11.849862+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/2LFNGR5P7QLTJEFIAT6IC7PIY3","json":"https://pith.science/pith/2LFNGR5P7QLTJEFIAT6IC7PIY3.json","graph_json":"https://pith.science/api/pith-number/2LFNGR5P7QLTJEFIAT6IC7PIY3/graph.json","events_json":"https://pith.science/api/pith-number/2LFNGR5P7QLTJEFIAT6IC7PIY3/events.json","paper":"https://pith.science/paper/2LFNGR5P"},"agent_actions":{"view_html":"https://pith.science/pith/2LFNGR5P7QLTJEFIAT6IC7PIY3","download_json":"https://pith.science/pith/2LFNGR5P7QLTJEFIAT6IC7PIY3.json","view_paper":"https://pith.science/paper/2LFNGR5P","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.16315&json=true","fetch_graph":"https://pith.science/api/pith-number/2LFNGR5P7QLTJEFIAT6IC7PIY3/graph.json","fetch_events":"https://pith.science/api/pith-number/2LFNGR5P7QLTJEFIAT6IC7PIY3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2LFNGR5P7QLTJEFIAT6IC7PIY3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2LFNGR5P7QLTJEFIAT6IC7PIY3/action/storage_attestation","attest_author":"https://pith.science/pith/2LFNGR5P7QLTJEFIAT6IC7PIY3/action/author_attestation","sign_citation":"https://pith.science/pith/2LFNGR5P7QLTJEFIAT6IC7PIY3/action/citation_signature","submit_replication":"https://pith.science/pith/2LFNGR5P7QLTJEFIAT6IC7PIY3/action/replication_record"}},"created_at":"2026-07-21T00:20:11.849862+00:00","updated_at":"2026-07-21T00:20:11.849862+00:00"}