{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:IEBPVEKLUDDRGFVZCDPROALFEW","short_pith_number":"pith:IEBPVEKL","canonical_record":{"source":{"id":"1112.2743","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-12-12T23:30:10Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"48f18e14f8f9c47e8781a476cea47709a9fb2db736609fad89098e78993548c3","abstract_canon_sha256":"08b5be01208cbaf38f7cc8026713badbc61d4217734519df217ce1c1cc31740a"},"schema_version":"1.0"},"canonical_sha256":"4102fa914ba0c71316b910df17016525823fe29bc04cfa4609c6b144bfde0a1e","source":{"kind":"arxiv","id":"1112.2743","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.2743","created_at":"2026-05-18T03:59:12Z"},{"alias_kind":"arxiv_version","alias_value":"1112.2743v1","created_at":"2026-05-18T03:59:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.2743","created_at":"2026-05-18T03:59:12Z"},{"alias_kind":"pith_short_12","alias_value":"IEBPVEKLUDDR","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_16","alias_value":"IEBPVEKLUDDRGFVZ","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_8","alias_value":"IEBPVEKL","created_at":"2026-05-18T12:26:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:IEBPVEKLUDDRGFVZCDPROALFEW","target":"record","payload":{"canonical_record":{"source":{"id":"1112.2743","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-12-12T23:30:10Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"48f18e14f8f9c47e8781a476cea47709a9fb2db736609fad89098e78993548c3","abstract_canon_sha256":"08b5be01208cbaf38f7cc8026713badbc61d4217734519df217ce1c1cc31740a"},"schema_version":"1.0"},"canonical_sha256":"4102fa914ba0c71316b910df17016525823fe29bc04cfa4609c6b144bfde0a1e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:59:12.141589Z","signature_b64":"JxWTCStOKgE7UNWYFBKYRjdH8+erte6XC+dzmrYj7DS2sze4d/Ej62hsZjW9er0ncSBFLAxgHGkr3rI2RZMTCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4102fa914ba0c71316b910df17016525823fe29bc04cfa4609c6b144bfde0a1e","last_reissued_at":"2026-05-18T03:59:12.141086Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:59:12.141086Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1112.2743","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:59:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aUS5sFEFf8hkzKt/zu2Gc/JVYAb89yucKFKaneSZg3BP1lfeAT8lXSDahs1xkdps+pashtE31pVoUL0p003kBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:59:02.508699Z"},"content_sha256":"db08e55be85e21eb0d8a2bc93b033077951aa3417e490285ca1d09dce2fa9c18","schema_version":"1.0","event_id":"sha256:db08e55be85e21eb0d8a2bc93b033077951aa3417e490285ca1d09dce2fa9c18"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:IEBPVEKLUDDRGFVZCDPROALFEW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Two dimensional Dirac fermions in the presence of long-range correlated disorder","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.mes-hall","authors_text":"Andrei A. Fedorenko, David Carpentier, Edmond Orignac","submitted_at":"2011-12-12T23:30:10Z","abstract_excerpt":"We consider 2D Dirac fermions in the presence of three types of disorder: random scalar potential, random gauge potential and random mass with long-range correlations decaying as a power law. Using various methods such as the self-consistent Born approximation (SCBA), renormalization group (RG), the matrix Green function formalism and bosonisation we calculate the density of states and study the full counting statistics of fermionic transport at lower energy. The SCBA and RG show that the random correlated scalar potentials generate an algebraically small energy scale below which the density o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.2743","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":""},"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":"2026-05-18T03:59:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pK1fYVbqeGZaovxGHCoTbLNSqctxcJ4MpyAIT902SJNLxeYnlfbA5onKo24dOdMXiQ0QznL7nkXCwaJlkE7WBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:59:02.509417Z"},"content_sha256":"0842a46841a8649e16925e6f825191628b2d508922a7394bb49db01c222f27db","schema_version":"1.0","event_id":"sha256:0842a46841a8649e16925e6f825191628b2d508922a7394bb49db01c222f27db"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/IEBPVEKLUDDRGFVZCDPROALFEW/bundle.json","state_url":"https://pith.science/pith/IEBPVEKLUDDRGFVZCDPROALFEW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/IEBPVEKLUDDRGFVZCDPROALFEW/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":"2026-05-25T18:59:02Z","links":{"resolver":"https://pith.science/pith/IEBPVEKLUDDRGFVZCDPROALFEW","bundle":"https://pith.science/pith/IEBPVEKLUDDRGFVZCDPROALFEW/bundle.json","state":"https://pith.science/pith/IEBPVEKLUDDRGFVZCDPROALFEW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/IEBPVEKLUDDRGFVZCDPROALFEW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:IEBPVEKLUDDRGFVZCDPROALFEW","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":"08b5be01208cbaf38f7cc8026713badbc61d4217734519df217ce1c1cc31740a","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-12-12T23:30:10Z","title_canon_sha256":"48f18e14f8f9c47e8781a476cea47709a9fb2db736609fad89098e78993548c3"},"schema_version":"1.0","source":{"id":"1112.2743","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.2743","created_at":"2026-05-18T03:59:12Z"},{"alias_kind":"arxiv_version","alias_value":"1112.2743v1","created_at":"2026-05-18T03:59:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.2743","created_at":"2026-05-18T03:59:12Z"},{"alias_kind":"pith_short_12","alias_value":"IEBPVEKLUDDR","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_16","alias_value":"IEBPVEKLUDDRGFVZ","created_at":"2026-05-18T12:26:30Z"},{"alias_kind":"pith_short_8","alias_value":"IEBPVEKL","created_at":"2026-05-18T12:26:30Z"}],"graph_snapshots":[{"event_id":"sha256:0842a46841a8649e16925e6f825191628b2d508922a7394bb49db01c222f27db","target":"graph","created_at":"2026-05-18T03:59:12Z","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"},"paper":{"abstract_excerpt":"We consider 2D Dirac fermions in the presence of three types of disorder: random scalar potential, random gauge potential and random mass with long-range correlations decaying as a power law. Using various methods such as the self-consistent Born approximation (SCBA), renormalization group (RG), the matrix Green function formalism and bosonisation we calculate the density of states and study the full counting statistics of fermionic transport at lower energy. The SCBA and RG show that the random correlated scalar potentials generate an algebraically small energy scale below which the density o","authors_text":"Andrei A. Fedorenko, David Carpentier, Edmond Orignac","cross_cats":["cond-mat.dis-nn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-12-12T23:30:10Z","title":"Two dimensional Dirac fermions in the presence of long-range correlated disorder"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.2743","kind":"arxiv","version":1},"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:db08e55be85e21eb0d8a2bc93b033077951aa3417e490285ca1d09dce2fa9c18","target":"record","created_at":"2026-05-18T03:59:12Z","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":"08b5be01208cbaf38f7cc8026713badbc61d4217734519df217ce1c1cc31740a","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-12-12T23:30:10Z","title_canon_sha256":"48f18e14f8f9c47e8781a476cea47709a9fb2db736609fad89098e78993548c3"},"schema_version":"1.0","source":{"id":"1112.2743","kind":"arxiv","version":1}},"canonical_sha256":"4102fa914ba0c71316b910df17016525823fe29bc04cfa4609c6b144bfde0a1e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4102fa914ba0c71316b910df17016525823fe29bc04cfa4609c6b144bfde0a1e","first_computed_at":"2026-05-18T03:59:12.141086Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:59:12.141086Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"JxWTCStOKgE7UNWYFBKYRjdH8+erte6XC+dzmrYj7DS2sze4d/Ej62hsZjW9er0ncSBFLAxgHGkr3rI2RZMTCw==","signature_status":"signed_v1","signed_at":"2026-05-18T03:59:12.141589Z","signed_message":"canonical_sha256_bytes"},"source_id":"1112.2743","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:db08e55be85e21eb0d8a2bc93b033077951aa3417e490285ca1d09dce2fa9c18","sha256:0842a46841a8649e16925e6f825191628b2d508922a7394bb49db01c222f27db"],"state_sha256":"82642e1a67d364ba3ea38bb32265865a4815efb0d96130872b52cb2a49cf7ae2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HDCh4XvfJUsi65iZuh4ieHY1GybNTeNdxDVORBjQ6hL5yrBqd2Qnc9z5cV321hES9tW50/arjeYqC+xqKmvpAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T18:59:02.513396Z","bundle_sha256":"8cb4841004fcca688abdecf3d8dfb9048a0f0d4f9a605091a3b625c7e9239ad4"}}