{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:UAAYKWMSCHCMSEKQWSJQEIKJFV","short_pith_number":"pith:UAAYKWMS","schema_version":"1.0","canonical_sha256":"a00185599211c4c91150b4930221492d6a2aa6e0bb870dbc0ff6cc8b33cf63a3","source":{"kind":"arxiv","id":"1408.1200","version":2},"attestation_state":"computed","paper":{"title":"Orbital magnetic moments in insulating Dirac systems: Impact on magnetotransport in graphene van der Waals heterostructures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Fran\\c{c}ois M. Peeters, Marko M. Gruji\\'c, Milan \\v{Z}. Tadi\\'c","submitted_at":"2014-08-06T07:44:59Z","abstract_excerpt":"In honeycomb Dirac systems with broken inversion symmetry, orbital magnetic moments coupled to the valley degree of freedom arise due to the topology of the band structure, leading to valley-selective optical dichroism. On the other hand, in Dirac systems with prominent spin-orbit coupling, similar orbital magnetic moments emerge as well. These moments are coupled to spin, but otherwise have the same functional form as the moments stemming from spatial inversion breaking. After reviewing the basic properties of these moments, which are relevant for a whole set of newly discovered materials, su"},"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":"1408.1200","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2014-08-06T07:44:59Z","cross_cats_sorted":[],"title_canon_sha256":"790de6eaf51837d70d9ef2cb6387d35c008f574975ff5c4fa231d2663450f44d","abstract_canon_sha256":"47d48214bb6de287dad1908cd91561f6d5e132ca7e38295d684f0761616302c0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:37:38.095629Z","signature_b64":"5RSNvdOesRV0NEcnoekTMwi8FR3KNXR8K72Yab9O01o0sGmKBJys+y4ubR8k/x5ot4zmew7T9l7h47sS+5YrCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a00185599211c4c91150b4930221492d6a2aa6e0bb870dbc0ff6cc8b33cf63a3","last_reissued_at":"2026-05-18T02:37:38.095206Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:37:38.095206Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Orbital magnetic moments in insulating Dirac systems: Impact on magnetotransport in graphene van der Waals heterostructures","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Fran\\c{c}ois M. Peeters, Marko M. Gruji\\'c, Milan \\v{Z}. Tadi\\'c","submitted_at":"2014-08-06T07:44:59Z","abstract_excerpt":"In honeycomb Dirac systems with broken inversion symmetry, orbital magnetic moments coupled to the valley degree of freedom arise due to the topology of the band structure, leading to valley-selective optical dichroism. On the other hand, in Dirac systems with prominent spin-orbit coupling, similar orbital magnetic moments emerge as well. These moments are coupled to spin, but otherwise have the same functional form as the moments stemming from spatial inversion breaking. After reviewing the basic properties of these moments, which are relevant for a whole set of newly discovered materials, su"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.1200","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":"1408.1200","created_at":"2026-05-18T02:37:38.095259+00:00"},{"alias_kind":"arxiv_version","alias_value":"1408.1200v2","created_at":"2026-05-18T02:37:38.095259+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.1200","created_at":"2026-05-18T02:37:38.095259+00:00"},{"alias_kind":"pith_short_12","alias_value":"UAAYKWMSCHCM","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_16","alias_value":"UAAYKWMSCHCMSEKQ","created_at":"2026-05-18T12:28:52.271510+00:00"},{"alias_kind":"pith_short_8","alias_value":"UAAYKWMS","created_at":"2026-05-18T12:28:52.271510+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/UAAYKWMSCHCMSEKQWSJQEIKJFV","json":"https://pith.science/pith/UAAYKWMSCHCMSEKQWSJQEIKJFV.json","graph_json":"https://pith.science/api/pith-number/UAAYKWMSCHCMSEKQWSJQEIKJFV/graph.json","events_json":"https://pith.science/api/pith-number/UAAYKWMSCHCMSEKQWSJQEIKJFV/events.json","paper":"https://pith.science/paper/UAAYKWMS"},"agent_actions":{"view_html":"https://pith.science/pith/UAAYKWMSCHCMSEKQWSJQEIKJFV","download_json":"https://pith.science/pith/UAAYKWMSCHCMSEKQWSJQEIKJFV.json","view_paper":"https://pith.science/paper/UAAYKWMS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1408.1200&json=true","fetch_graph":"https://pith.science/api/pith-number/UAAYKWMSCHCMSEKQWSJQEIKJFV/graph.json","fetch_events":"https://pith.science/api/pith-number/UAAYKWMSCHCMSEKQWSJQEIKJFV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UAAYKWMSCHCMSEKQWSJQEIKJFV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UAAYKWMSCHCMSEKQWSJQEIKJFV/action/storage_attestation","attest_author":"https://pith.science/pith/UAAYKWMSCHCMSEKQWSJQEIKJFV/action/author_attestation","sign_citation":"https://pith.science/pith/UAAYKWMSCHCMSEKQWSJQEIKJFV/action/citation_signature","submit_replication":"https://pith.science/pith/UAAYKWMSCHCMSEKQWSJQEIKJFV/action/replication_record"}},"created_at":"2026-05-18T02:37:38.095259+00:00","updated_at":"2026-05-18T02:37:38.095259+00:00"}