{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:PA2F5NO5QFV22IEHSWESX3EBWA","short_pith_number":"pith:PA2F5NO5","schema_version":"1.0","canonical_sha256":"78345eb5dd816bad208795892bec81b02ee7290f0d63737ea12cccc196a8b70c","source":{"kind":"arxiv","id":"1812.08792","version":2},"attestation_state":"computed","paper":{"title":"Thermal Hall effect in square-lattice spin liquids: A Schwinger boson mean-field study","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Mathias S. Scheurer, Rhine Samajdar, Shubhayu Chatterjee, Subir Sachdev","submitted_at":"2018-12-20T19:00:00Z","abstract_excerpt":"Motivated by recent transport measurements in high-$T_c$ cuprate superconductors in a magnetic field, we study the thermal Hall conductivity in materials with topological order, focusing on the contribution from neutral spinons. Specifically, different Schwinger boson mean-field ans\\\"{a}tze for the Heisenberg antiferromagnet on the square lattice are analyzed. We allow for both Dzyaloshinskii-Moriya interactions, and additional terms associated with scalar spin chiralities that break time-reversal and reflection symmetries, but preserve their product. It is shown that these scalar spin chirali"},"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":"1812.08792","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2018-12-20T19:00:00Z","cross_cats_sorted":["cond-mat.mes-hall","cond-mat.supr-con"],"title_canon_sha256":"9afe6cd692d658138e2bfb3c6419b346026db5883b16cca3bf9de3a1333a3bf3","abstract_canon_sha256":"5bddb6150bd8fa0cac0bdf171f3a468c669fc067b780e9aa09d1722a46eccb88"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:47:58.765671Z","signature_b64":"LhSs6Ykm8ZTqN/9CAB4cbUDiqNA2f/vwbnNo6PCZhViHNZjtwsUe+fgN1yp6KoO2Ees7e8fGa4gOSMuXmYziCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"78345eb5dd816bad208795892bec81b02ee7290f0d63737ea12cccc196a8b70c","last_reissued_at":"2026-05-17T23:47:58.765196Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:47:58.765196Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermal Hall effect in square-lattice spin liquids: A Schwinger boson mean-field study","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","cond-mat.supr-con"],"primary_cat":"cond-mat.str-el","authors_text":"Mathias S. Scheurer, Rhine Samajdar, Shubhayu Chatterjee, Subir Sachdev","submitted_at":"2018-12-20T19:00:00Z","abstract_excerpt":"Motivated by recent transport measurements in high-$T_c$ cuprate superconductors in a magnetic field, we study the thermal Hall conductivity in materials with topological order, focusing on the contribution from neutral spinons. Specifically, different Schwinger boson mean-field ans\\\"{a}tze for the Heisenberg antiferromagnet on the square lattice are analyzed. We allow for both Dzyaloshinskii-Moriya interactions, and additional terms associated with scalar spin chiralities that break time-reversal and reflection symmetries, but preserve their product. It is shown that these scalar spin chirali"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.08792","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":"1812.08792","created_at":"2026-05-17T23:47:58.765280+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.08792v2","created_at":"2026-05-17T23:47:58.765280+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.08792","created_at":"2026-05-17T23:47:58.765280+00:00"},{"alias_kind":"pith_short_12","alias_value":"PA2F5NO5QFV2","created_at":"2026-05-18T12:32:43.782077+00:00"},{"alias_kind":"pith_short_16","alias_value":"PA2F5NO5QFV22IEH","created_at":"2026-05-18T12:32:43.782077+00:00"},{"alias_kind":"pith_short_8","alias_value":"PA2F5NO5","created_at":"2026-05-18T12:32:43.782077+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/PA2F5NO5QFV22IEHSWESX3EBWA","json":"https://pith.science/pith/PA2F5NO5QFV22IEHSWESX3EBWA.json","graph_json":"https://pith.science/api/pith-number/PA2F5NO5QFV22IEHSWESX3EBWA/graph.json","events_json":"https://pith.science/api/pith-number/PA2F5NO5QFV22IEHSWESX3EBWA/events.json","paper":"https://pith.science/paper/PA2F5NO5"},"agent_actions":{"view_html":"https://pith.science/pith/PA2F5NO5QFV22IEHSWESX3EBWA","download_json":"https://pith.science/pith/PA2F5NO5QFV22IEHSWESX3EBWA.json","view_paper":"https://pith.science/paper/PA2F5NO5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.08792&json=true","fetch_graph":"https://pith.science/api/pith-number/PA2F5NO5QFV22IEHSWESX3EBWA/graph.json","fetch_events":"https://pith.science/api/pith-number/PA2F5NO5QFV22IEHSWESX3EBWA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PA2F5NO5QFV22IEHSWESX3EBWA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PA2F5NO5QFV22IEHSWESX3EBWA/action/storage_attestation","attest_author":"https://pith.science/pith/PA2F5NO5QFV22IEHSWESX3EBWA/action/author_attestation","sign_citation":"https://pith.science/pith/PA2F5NO5QFV22IEHSWESX3EBWA/action/citation_signature","submit_replication":"https://pith.science/pith/PA2F5NO5QFV22IEHSWESX3EBWA/action/replication_record"}},"created_at":"2026-05-17T23:47:58.765280+00:00","updated_at":"2026-05-17T23:47:58.765280+00:00"}