{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:EWRBCS24NXF7FBKP43W6OITSRW","short_pith_number":"pith:EWRBCS24","canonical_record":{"source":{"id":"2208.07661","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-08-16T10:47:03Z","cross_cats_sorted":["hep-th","quant-ph"],"title_canon_sha256":"772eb733c7e38482a533203d8d8107543e34147d6af0429f0eb87184ed69dd09","abstract_canon_sha256":"09326f76698c644860d99666a9e7cb4ed32896a67a3371e79f138c8f8e6c6579"},"schema_version":"1.0"},"canonical_sha256":"25a2114b5c6dcbf2854fe6ede722728da13bd8b646307212e075ae703a3b1bf3","source":{"kind":"arxiv","id":"2208.07661","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2208.07661","created_at":"2026-07-05T05:31:02Z"},{"alias_kind":"arxiv_version","alias_value":"2208.07661v2","created_at":"2026-07-05T05:31:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2208.07661","created_at":"2026-07-05T05:31:02Z"},{"alias_kind":"pith_short_12","alias_value":"EWRBCS24NXF7","created_at":"2026-07-05T05:31:02Z"},{"alias_kind":"pith_short_16","alias_value":"EWRBCS24NXF7FBKP","created_at":"2026-07-05T05:31:02Z"},{"alias_kind":"pith_short_8","alias_value":"EWRBCS24","created_at":"2026-07-05T05:31:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:EWRBCS24NXF7FBKP43W6OITSRW","target":"record","payload":{"canonical_record":{"source":{"id":"2208.07661","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-08-16T10:47:03Z","cross_cats_sorted":["hep-th","quant-ph"],"title_canon_sha256":"772eb733c7e38482a533203d8d8107543e34147d6af0429f0eb87184ed69dd09","abstract_canon_sha256":"09326f76698c644860d99666a9e7cb4ed32896a67a3371e79f138c8f8e6c6579"},"schema_version":"1.0"},"canonical_sha256":"25a2114b5c6dcbf2854fe6ede722728da13bd8b646307212e075ae703a3b1bf3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:31:02.724560Z","signature_b64":"g64eEbU6xRcCgXoo91FWLg26iEbYYYPzUlfzKkVIcvpG714eZClv3tPBoNvRbf1g9iziyMlmvWceiSeSzfKCBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"25a2114b5c6dcbf2854fe6ede722728da13bd8b646307212e075ae703a3b1bf3","last_reissued_at":"2026-07-05T05:31:02.724128Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:31:02.724128Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2208.07661","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T05:31:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lYk+oInn3z/QI/JojeL2uc85OHHOrGnfwPiRmVic3Hc0J8nS1yabjJ0qb/VW0L0+TK1Rvcg3Y4FGSgKcwOCeDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T22:34:41.583451Z"},"content_sha256":"71234eff6864f49cbf7f2e9cac2863a5850505115951b425bf49354421388bc0","schema_version":"1.0","event_id":"sha256:71234eff6864f49cbf7f2e9cac2863a5850505115951b425bf49354421388bc0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:EWRBCS24NXF7FBKP43W6OITSRW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Rashba contribution of 2D Dirac-Weyl fermions: Beyond ordinary quantum regime","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Ahmed Jellal, Dariush Jahani, Omid Akhavan","submitted_at":"2022-08-16T10:47:03Z","abstract_excerpt":"We study the energy levels of Dirac-Weyl fermions in graphene subject to a magnetic field with Rashba contribution in the minimal length situation. The exact solution for the energy dispersion of Dirac-like charge carriers coupled to the magnetic moments in a (2+1)-dimension is obtained by the use of the momentum space representation. Moreover, as it comes to applications for 2D Dirac-like quasiparticles, we also extend our theory and results in some special cases, showing that the emerging energy spectrum at the high magnetic field limit becomes independent of the Rashba coupling, $\\lambda_{R"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2208.07661","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2208.07661/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T05:31:02Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"z0arqafW8KKDj/GiTy2HqJlc4mm4d9j5Fw8qRgryTXS38TGUo/lFBezQ6gmyhtYJHwcZbEQBJgk8fYDXZk8rAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T22:34:41.583957Z"},"content_sha256":"10f5d5d9df3b9478241858b706ec3503b877b4b06665e9237bcb9e868e599620","schema_version":"1.0","event_id":"sha256:10f5d5d9df3b9478241858b706ec3503b877b4b06665e9237bcb9e868e599620"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/EWRBCS24NXF7FBKP43W6OITSRW/bundle.json","state_url":"https://pith.science/pith/EWRBCS24NXF7FBKP43W6OITSRW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/EWRBCS24NXF7FBKP43W6OITSRW/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-08-03T22:34:41Z","links":{"resolver":"https://pith.science/pith/EWRBCS24NXF7FBKP43W6OITSRW","bundle":"https://pith.science/pith/EWRBCS24NXF7FBKP43W6OITSRW/bundle.json","state":"https://pith.science/pith/EWRBCS24NXF7FBKP43W6OITSRW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/EWRBCS24NXF7FBKP43W6OITSRW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:EWRBCS24NXF7FBKP43W6OITSRW","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"09326f76698c644860d99666a9e7cb4ed32896a67a3371e79f138c8f8e6c6579","cross_cats_sorted":["hep-th","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-08-16T10:47:03Z","title_canon_sha256":"772eb733c7e38482a533203d8d8107543e34147d6af0429f0eb87184ed69dd09"},"schema_version":"1.0","source":{"id":"2208.07661","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2208.07661","created_at":"2026-07-05T05:31:02Z"},{"alias_kind":"arxiv_version","alias_value":"2208.07661v2","created_at":"2026-07-05T05:31:02Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2208.07661","created_at":"2026-07-05T05:31:02Z"},{"alias_kind":"pith_short_12","alias_value":"EWRBCS24NXF7","created_at":"2026-07-05T05:31:02Z"},{"alias_kind":"pith_short_16","alias_value":"EWRBCS24NXF7FBKP","created_at":"2026-07-05T05:31:02Z"},{"alias_kind":"pith_short_8","alias_value":"EWRBCS24","created_at":"2026-07-05T05:31:02Z"}],"graph_snapshots":[{"event_id":"sha256:10f5d5d9df3b9478241858b706ec3503b877b4b06665e9237bcb9e868e599620","target":"graph","created_at":"2026-07-05T05:31:02Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2208.07661/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study the energy levels of Dirac-Weyl fermions in graphene subject to a magnetic field with Rashba contribution in the minimal length situation. The exact solution for the energy dispersion of Dirac-like charge carriers coupled to the magnetic moments in a (2+1)-dimension is obtained by the use of the momentum space representation. Moreover, as it comes to applications for 2D Dirac-like quasiparticles, we also extend our theory and results in some special cases, showing that the emerging energy spectrum at the high magnetic field limit becomes independent of the Rashba coupling, $\\lambda_{R","authors_text":"Ahmed Jellal, Dariush Jahani, Omid Akhavan","cross_cats":["hep-th","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-08-16T10:47:03Z","title":"Rashba contribution of 2D Dirac-Weyl fermions: Beyond ordinary quantum regime"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2208.07661","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:71234eff6864f49cbf7f2e9cac2863a5850505115951b425bf49354421388bc0","target":"record","created_at":"2026-07-05T05:31:02Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"09326f76698c644860d99666a9e7cb4ed32896a67a3371e79f138c8f8e6c6579","cross_cats_sorted":["hep-th","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2022-08-16T10:47:03Z","title_canon_sha256":"772eb733c7e38482a533203d8d8107543e34147d6af0429f0eb87184ed69dd09"},"schema_version":"1.0","source":{"id":"2208.07661","kind":"arxiv","version":2}},"canonical_sha256":"25a2114b5c6dcbf2854fe6ede722728da13bd8b646307212e075ae703a3b1bf3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"25a2114b5c6dcbf2854fe6ede722728da13bd8b646307212e075ae703a3b1bf3","first_computed_at":"2026-07-05T05:31:02.724128Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:31:02.724128Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"g64eEbU6xRcCgXoo91FWLg26iEbYYYPzUlfzKkVIcvpG714eZClv3tPBoNvRbf1g9iziyMlmvWceiSeSzfKCBw==","signature_status":"signed_v1","signed_at":"2026-07-05T05:31:02.724560Z","signed_message":"canonical_sha256_bytes"},"source_id":"2208.07661","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:71234eff6864f49cbf7f2e9cac2863a5850505115951b425bf49354421388bc0","sha256:10f5d5d9df3b9478241858b706ec3503b877b4b06665e9237bcb9e868e599620"],"state_sha256":"4cfa41ab1545ec80d7f3efb19e40aa0ead751a229a104dd9194b34b608d5b6d2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aHgyCEr8g+d4dptJv2Erv8CUGgJ+CxhBbFdEM6vrDGFEMjSciW9JMFDWVCoX3dCfpgmRtDW4QkMkc2jDcgEPBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T22:34:41.588627Z","bundle_sha256":"9c8c79d1cc308b42a19ea001850d0275cceed6c9d1d519c55dc5f8ba5f2b278c"}}