{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:OAUTH43XHQKQQDEGHXFRCE4AGD","short_pith_number":"pith:OAUTH43X","schema_version":"1.0","canonical_sha256":"702933f3773c15080c863dcb11138030dab5c25367dbb9d0c05f714069da927b","source":{"kind":"arxiv","id":"1605.02782","version":2},"attestation_state":"computed","paper":{"title":"Hall viscosity and electromagnetic response of electrons in graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Alessandro Principi, Giovanni Vignale, Mohammad Sherafati","submitted_at":"2016-05-09T21:05:19Z","abstract_excerpt":"We derive an analytic expression for the geometric Hall viscosity of non-interacting electrons in a single graphene layer in the presence of a perpendicular magnetic field. We show that a recently-derived formula in [C. Hoyos and D. T. Son, Phys. Rev. Lett. {\\bf 108}, 066805 (2012)], which connects the coefficient of $q^2$ in the wave vector expansion of the Hall conductivity $\\sigma_{xy}(q)$ of the two-dimensional electron gas (2DEG) to the Hall viscosity and the orbital diamagnetic susceptibility of that system, continues to hold for graphene -- in spite of the lack of Galilean invariance --"},"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":"1605.02782","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2016-05-09T21:05:19Z","cross_cats_sorted":[],"title_canon_sha256":"95d66273eda33b4e22d89598c5a4c6485c22ffcff7167ca29abca4fe453c7dd2","abstract_canon_sha256":"75ce102ed5c6bd9cd738e37bad21d039a2d19bc7342accd3cd2aa568a72add38"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:04:32.802607Z","signature_b64":"js0LeokqMNaJi2A7/EOPmKgXFfQL7IJz6BhDcW72AW2zF360wDZRUk0Bi7QE7L5cTzDbIUhRbqvIk2BP1PTjBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"702933f3773c15080c863dcb11138030dab5c25367dbb9d0c05f714069da927b","last_reissued_at":"2026-05-18T01:04:32.801711Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:04:32.801711Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hall viscosity and electromagnetic response of electrons in graphene","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Alessandro Principi, Giovanni Vignale, Mohammad Sherafati","submitted_at":"2016-05-09T21:05:19Z","abstract_excerpt":"We derive an analytic expression for the geometric Hall viscosity of non-interacting electrons in a single graphene layer in the presence of a perpendicular magnetic field. We show that a recently-derived formula in [C. Hoyos and D. T. Son, Phys. Rev. Lett. {\\bf 108}, 066805 (2012)], which connects the coefficient of $q^2$ in the wave vector expansion of the Hall conductivity $\\sigma_{xy}(q)$ of the two-dimensional electron gas (2DEG) to the Hall viscosity and the orbital diamagnetic susceptibility of that system, continues to hold for graphene -- in spite of the lack of Galilean invariance --"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.02782","kind":"arxiv","version":2},"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":"1605.02782","created_at":"2026-05-18T01:04:32.801857+00:00"},{"alias_kind":"arxiv_version","alias_value":"1605.02782v2","created_at":"2026-05-18T01:04:32.801857+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.02782","created_at":"2026-05-18T01:04:32.801857+00:00"},{"alias_kind":"pith_short_12","alias_value":"OAUTH43XHQKQ","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_16","alias_value":"OAUTH43XHQKQQDEG","created_at":"2026-05-18T12:30:36.002864+00:00"},{"alias_kind":"pith_short_8","alias_value":"OAUTH43X","created_at":"2026-05-18T12:30:36.002864+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/OAUTH43XHQKQQDEGHXFRCE4AGD","json":"https://pith.science/pith/OAUTH43XHQKQQDEGHXFRCE4AGD.json","graph_json":"https://pith.science/api/pith-number/OAUTH43XHQKQQDEGHXFRCE4AGD/graph.json","events_json":"https://pith.science/api/pith-number/OAUTH43XHQKQQDEGHXFRCE4AGD/events.json","paper":"https://pith.science/paper/OAUTH43X"},"agent_actions":{"view_html":"https://pith.science/pith/OAUTH43XHQKQQDEGHXFRCE4AGD","download_json":"https://pith.science/pith/OAUTH43XHQKQQDEGHXFRCE4AGD.json","view_paper":"https://pith.science/paper/OAUTH43X","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1605.02782&json=true","fetch_graph":"https://pith.science/api/pith-number/OAUTH43XHQKQQDEGHXFRCE4AGD/graph.json","fetch_events":"https://pith.science/api/pith-number/OAUTH43XHQKQQDEGHXFRCE4AGD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OAUTH43XHQKQQDEGHXFRCE4AGD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OAUTH43XHQKQQDEGHXFRCE4AGD/action/storage_attestation","attest_author":"https://pith.science/pith/OAUTH43XHQKQQDEGHXFRCE4AGD/action/author_attestation","sign_citation":"https://pith.science/pith/OAUTH43XHQKQQDEGHXFRCE4AGD/action/citation_signature","submit_replication":"https://pith.science/pith/OAUTH43XHQKQQDEGHXFRCE4AGD/action/replication_record"}},"created_at":"2026-05-18T01:04:32.801857+00:00","updated_at":"2026-05-18T01:04:32.801857+00:00"}