{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:W26M3H3QH64664UPWZSLGTE3H7","short_pith_number":"pith:W26M3H3Q","canonical_record":{"source":{"id":"1602.01360","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-02-03T16:39:39Z","cross_cats_sorted":[],"title_canon_sha256":"91a7710f96d0c23362ad3b85297788731127e82d3b3a13f12e3235d2c6a29ca4","abstract_canon_sha256":"6970041c3276647274db93018d283738cf8cad980447f5cb1a4201c0fce640de"},"schema_version":"1.0"},"canonical_sha256":"b6bccd9f703fb9ef728fb664b34c9b3fd71f33957294f54f25af369656bdd9ff","source":{"kind":"arxiv","id":"1602.01360","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.01360","created_at":"2026-05-18T00:44:04Z"},{"alias_kind":"arxiv_version","alias_value":"1602.01360v3","created_at":"2026-05-18T00:44:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.01360","created_at":"2026-05-18T00:44:04Z"},{"alias_kind":"pith_short_12","alias_value":"W26M3H3QH646","created_at":"2026-05-18T12:30:48Z"},{"alias_kind":"pith_short_16","alias_value":"W26M3H3QH64664UP","created_at":"2026-05-18T12:30:48Z"},{"alias_kind":"pith_short_8","alias_value":"W26M3H3Q","created_at":"2026-05-18T12:30:48Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:W26M3H3QH64664UPWZSLGTE3H7","target":"record","payload":{"canonical_record":{"source":{"id":"1602.01360","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-02-03T16:39:39Z","cross_cats_sorted":[],"title_canon_sha256":"91a7710f96d0c23362ad3b85297788731127e82d3b3a13f12e3235d2c6a29ca4","abstract_canon_sha256":"6970041c3276647274db93018d283738cf8cad980447f5cb1a4201c0fce640de"},"schema_version":"1.0"},"canonical_sha256":"b6bccd9f703fb9ef728fb664b34c9b3fd71f33957294f54f25af369656bdd9ff","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:44:04.264550Z","signature_b64":"sPXfm0707MWcVqw0q/pdWuL7RKSAc3sVEantzUYcAgy22nebtC5vDXrC36w47AvLh7V3SpJptasDyOti9bYmDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b6bccd9f703fb9ef728fb664b34c9b3fd71f33957294f54f25af369656bdd9ff","last_reissued_at":"2026-05-18T00:44:04.264130Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:44:04.264130Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1602.01360","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:44:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"51RWbc0EfTNJvRdWSpOjEzi+q54TLC5/PZij6kjqI5sIZLu/2n/Zz5CWjIoZtw7+HAwoLVWOpZvQb3dnNpEcDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T11:01:39.392274Z"},"content_sha256":"f261976a75f9d4fa2f15cc78457f9aa12c95d42f0a927c6687a0e6919ff2f308","schema_version":"1.0","event_id":"sha256:f261976a75f9d4fa2f15cc78457f9aa12c95d42f0a927c6687a0e6919ff2f308"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:W26M3H3QH64664UPWZSLGTE3H7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The role of band-index-dependent transport relaxation times in anomalous Hall effect","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Cong Xiao, Dingping Li, Zhongshui Ma","submitted_at":"2016-02-03T16:39:39Z","abstract_excerpt":"We revisit model calculations of the anomalous Hall effect (AHE) and show that, in isotropic Rashba-coupled two-dimensional electron gas (2DEG) with pointlike potential impurities, the full solution of the semiclassical Boltzmann equation (SBE) may differ from the widely-used $1/\\tau^{||}$ & $1/\\tau^{\\perp}$ solution [Phys. Rev. B 68, 165311 (2003)]. Our approach to AHE is analogous to the SBE-based analysis of the anisotropic magnetoresistance leading to an integral equation for the distribution function [Phys. Rev. B 79, 045427 (2009)] but in the present case, we reduce the description to ba"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.01360","kind":"arxiv","version":3},"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":"2026-05-18T00:44:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AGid4EdJRY2nUaF+2eXBoPruy6H5Qg2aVKsfSp7KZD0gc/S6x1Cg34NYxk0VvU8vcElgtwUYL0fuSoVIYfcnDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T11:01:39.392634Z"},"content_sha256":"4716c1a36106f72e83fa5c105652574296b43b8d579cf6abf69197fe34714ee6","schema_version":"1.0","event_id":"sha256:4716c1a36106f72e83fa5c105652574296b43b8d579cf6abf69197fe34714ee6"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/W26M3H3QH64664UPWZSLGTE3H7/bundle.json","state_url":"https://pith.science/pith/W26M3H3QH64664UPWZSLGTE3H7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/W26M3H3QH64664UPWZSLGTE3H7/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":"2026-06-26T11:01:39Z","links":{"resolver":"https://pith.science/pith/W26M3H3QH64664UPWZSLGTE3H7","bundle":"https://pith.science/pith/W26M3H3QH64664UPWZSLGTE3H7/bundle.json","state":"https://pith.science/pith/W26M3H3QH64664UPWZSLGTE3H7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/W26M3H3QH64664UPWZSLGTE3H7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:W26M3H3QH64664UPWZSLGTE3H7","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":"6970041c3276647274db93018d283738cf8cad980447f5cb1a4201c0fce640de","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-02-03T16:39:39Z","title_canon_sha256":"91a7710f96d0c23362ad3b85297788731127e82d3b3a13f12e3235d2c6a29ca4"},"schema_version":"1.0","source":{"id":"1602.01360","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1602.01360","created_at":"2026-05-18T00:44:04Z"},{"alias_kind":"arxiv_version","alias_value":"1602.01360v3","created_at":"2026-05-18T00:44:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1602.01360","created_at":"2026-05-18T00:44:04Z"},{"alias_kind":"pith_short_12","alias_value":"W26M3H3QH646","created_at":"2026-05-18T12:30:48Z"},{"alias_kind":"pith_short_16","alias_value":"W26M3H3QH64664UP","created_at":"2026-05-18T12:30:48Z"},{"alias_kind":"pith_short_8","alias_value":"W26M3H3Q","created_at":"2026-05-18T12:30:48Z"}],"graph_snapshots":[{"event_id":"sha256:4716c1a36106f72e83fa5c105652574296b43b8d579cf6abf69197fe34714ee6","target":"graph","created_at":"2026-05-18T00:44:04Z","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 revisit model calculations of the anomalous Hall effect (AHE) and show that, in isotropic Rashba-coupled two-dimensional electron gas (2DEG) with pointlike potential impurities, the full solution of the semiclassical Boltzmann equation (SBE) may differ from the widely-used $1/\\tau^{||}$ & $1/\\tau^{\\perp}$ solution [Phys. Rev. B 68, 165311 (2003)]. Our approach to AHE is analogous to the SBE-based analysis of the anisotropic magnetoresistance leading to an integral equation for the distribution function [Phys. Rev. B 79, 045427 (2009)] but in the present case, we reduce the description to ba","authors_text":"Cong Xiao, Dingping Li, Zhongshui Ma","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-02-03T16:39:39Z","title":"The role of band-index-dependent transport relaxation times in anomalous Hall effect"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1602.01360","kind":"arxiv","version":3},"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:f261976a75f9d4fa2f15cc78457f9aa12c95d42f0a927c6687a0e6919ff2f308","target":"record","created_at":"2026-05-18T00:44:04Z","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":"6970041c3276647274db93018d283738cf8cad980447f5cb1a4201c0fce640de","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2016-02-03T16:39:39Z","title_canon_sha256":"91a7710f96d0c23362ad3b85297788731127e82d3b3a13f12e3235d2c6a29ca4"},"schema_version":"1.0","source":{"id":"1602.01360","kind":"arxiv","version":3}},"canonical_sha256":"b6bccd9f703fb9ef728fb664b34c9b3fd71f33957294f54f25af369656bdd9ff","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b6bccd9f703fb9ef728fb664b34c9b3fd71f33957294f54f25af369656bdd9ff","first_computed_at":"2026-05-18T00:44:04.264130Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:44:04.264130Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"sPXfm0707MWcVqw0q/pdWuL7RKSAc3sVEantzUYcAgy22nebtC5vDXrC36w47AvLh7V3SpJptasDyOti9bYmDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:44:04.264550Z","signed_message":"canonical_sha256_bytes"},"source_id":"1602.01360","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f261976a75f9d4fa2f15cc78457f9aa12c95d42f0a927c6687a0e6919ff2f308","sha256:4716c1a36106f72e83fa5c105652574296b43b8d579cf6abf69197fe34714ee6"],"state_sha256":"d8358bd70f6670c38d1636645e9f5a9c38936cbea13bda793485f9a6fcec53da"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xiBUNcs74SbLPuQqqtM7K2pnuWGSqu7K79qo8/PYONDTUARRnXfFEvtrZNjBLzyn3Z0hnv6GMkx1h1yJlotpAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-26T11:01:39.394579Z","bundle_sha256":"af3966e7ce2c230811b47277263b0b5ce9ebf0b503d42ffe0ded5b27392ff249"}}