{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1994:3ZZVJLOP53HOS6H5SU6SK4R4MM","short_pith_number":"pith:3ZZVJLOP","canonical_record":{"source":{"id":"cond-mat/9411023","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1994-11-04T22:26:24Z","cross_cats_sorted":[],"title_canon_sha256":"f028c73708117da949907125cf81334d73759c1cb25fff60d51912a79d06d392","abstract_canon_sha256":"960f9d100e95db1e15712231293e3bfc0270cbacc984af3a206dafe270b03b23"},"schema_version":"1.0"},"canonical_sha256":"de7354adcfeecee978fd953d25723c6301f2b03a825233eeb66214e352de3ac1","source":{"kind":"arxiv","id":"cond-mat/9411023","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9411023","created_at":"2026-07-04T15:56:49Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9411023v1","created_at":"2026-07-04T15:56:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9411023","created_at":"2026-07-04T15:56:49Z"},{"alias_kind":"pith_short_12","alias_value":"3ZZVJLOP53HO","created_at":"2026-07-04T15:56:49Z"},{"alias_kind":"pith_short_16","alias_value":"3ZZVJLOP53HOS6H5","created_at":"2026-07-04T15:56:49Z"},{"alias_kind":"pith_short_8","alias_value":"3ZZVJLOP","created_at":"2026-07-04T15:56:49Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1994:3ZZVJLOP53HOS6H5SU6SK4R4MM","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/9411023","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1994-11-04T22:26:24Z","cross_cats_sorted":[],"title_canon_sha256":"f028c73708117da949907125cf81334d73759c1cb25fff60d51912a79d06d392","abstract_canon_sha256":"960f9d100e95db1e15712231293e3bfc0270cbacc984af3a206dafe270b03b23"},"schema_version":"1.0"},"canonical_sha256":"de7354adcfeecee978fd953d25723c6301f2b03a825233eeb66214e352de3ac1","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:56:49.854507Z","signature_b64":"jke1FRLyPDqVN/nW0/Pr0CN0Ob79V7kjkm7Dx3AIdjKzIZZB2+vVYXiMR2uNhEteGfexP/E6qGPt/Ftm92rNBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"de7354adcfeecee978fd953d25723c6301f2b03a825233eeb66214e352de3ac1","last_reissued_at":"2026-07-04T15:56:49.854122Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:56:49.854122Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/9411023","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":"2026-07-04T15:56:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"+iBu4N2ETz9YzxBXurdc3YMED3sfGyAfUQ/T0inhJIM6DBTWpXFio69JbqJ7lcZCbrkTqA4FlW1nlQeUyd6vAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T12:43:48.573027Z"},"content_sha256":"9ca8c7876f47ea6a79e549f4af4ac260bf9b9be8564aef5e9f692e687fd77193","schema_version":"1.0","event_id":"sha256:9ca8c7876f47ea6a79e549f4af4ac260bf9b9be8564aef5e9f692e687fd77193"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1994:3ZZVJLOP53HOS6H5SU6SK4R4MM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Solution of the Boltzmann equation in a random magnetic field","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"Anders Smith, Per Hedegard","submitted_at":"1994-11-04T22:26:24Z","abstract_excerpt":"A general framework for solving the Boltzmann equation for a 2-dimensional electron gas (2DEG) in random magnetic fields is presented, when the random fields are included in the driving force. The formalism is applied to some recent experiments, and a possible extension to composite fermions at $\\nu=1/2$ is discussed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9411023","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/cond-mat/9411023/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":"2026-07-04T15:56:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EeZ19K+PRzfC8O1jaolp9zoJnQRxyl8FScues1zEmT6S3IkaM+duH1rNEk0mtwbJgb6IAMGHqFgKF0DeELtoCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T12:43:48.573946Z"},"content_sha256":"7e7d5028399f4935f5c0244493cf1175d289f184b67ca583063b56242c379bd3","schema_version":"1.0","event_id":"sha256:7e7d5028399f4935f5c0244493cf1175d289f184b67ca583063b56242c379bd3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3ZZVJLOP53HOS6H5SU6SK4R4MM/bundle.json","state_url":"https://pith.science/pith/3ZZVJLOP53HOS6H5SU6SK4R4MM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3ZZVJLOP53HOS6H5SU6SK4R4MM/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":"2026-08-15T12:43:48Z","links":{"resolver":"https://pith.science/pith/3ZZVJLOP53HOS6H5SU6SK4R4MM","bundle":"https://pith.science/pith/3ZZVJLOP53HOS6H5SU6SK4R4MM/bundle.json","state":"https://pith.science/pith/3ZZVJLOP53HOS6H5SU6SK4R4MM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3ZZVJLOP53HOS6H5SU6SK4R4MM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1994:3ZZVJLOP53HOS6H5SU6SK4R4MM","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":"960f9d100e95db1e15712231293e3bfc0270cbacc984af3a206dafe270b03b23","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat","submitted_at":"1994-11-04T22:26:24Z","title_canon_sha256":"f028c73708117da949907125cf81334d73759c1cb25fff60d51912a79d06d392"},"schema_version":"1.0","source":{"id":"cond-mat/9411023","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9411023","created_at":"2026-07-04T15:56:49Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9411023v1","created_at":"2026-07-04T15:56:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9411023","created_at":"2026-07-04T15:56:49Z"},{"alias_kind":"pith_short_12","alias_value":"3ZZVJLOP53HO","created_at":"2026-07-04T15:56:49Z"},{"alias_kind":"pith_short_16","alias_value":"3ZZVJLOP53HOS6H5","created_at":"2026-07-04T15:56:49Z"},{"alias_kind":"pith_short_8","alias_value":"3ZZVJLOP","created_at":"2026-07-04T15:56:49Z"}],"graph_snapshots":[{"event_id":"sha256:7e7d5028399f4935f5c0244493cf1175d289f184b67ca583063b56242c379bd3","target":"graph","created_at":"2026-07-04T15:56:49Z","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/cond-mat/9411023/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A general framework for solving the Boltzmann equation for a 2-dimensional electron gas (2DEG) in random magnetic fields is presented, when the random fields are included in the driving force. The formalism is applied to some recent experiments, and a possible extension to composite fermions at $\\nu=1/2$ is discussed.","authors_text":"Anders Smith, Per Hedegard","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat","submitted_at":"1994-11-04T22:26:24Z","title":"Solution of the Boltzmann equation in a random magnetic field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9411023","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":"sha256:9ca8c7876f47ea6a79e549f4af4ac260bf9b9be8564aef5e9f692e687fd77193","target":"record","created_at":"2026-07-04T15:56:49Z","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":"960f9d100e95db1e15712231293e3bfc0270cbacc984af3a206dafe270b03b23","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat","submitted_at":"1994-11-04T22:26:24Z","title_canon_sha256":"f028c73708117da949907125cf81334d73759c1cb25fff60d51912a79d06d392"},"schema_version":"1.0","source":{"id":"cond-mat/9411023","kind":"arxiv","version":1}},"canonical_sha256":"de7354adcfeecee978fd953d25723c6301f2b03a825233eeb66214e352de3ac1","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"de7354adcfeecee978fd953d25723c6301f2b03a825233eeb66214e352de3ac1","first_computed_at":"2026-07-04T15:56:49.854122Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:56:49.854122Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jke1FRLyPDqVN/nW0/Pr0CN0Ob79V7kjkm7Dx3AIdjKzIZZB2+vVYXiMR2uNhEteGfexP/E6qGPt/Ftm92rNBA==","signature_status":"signed_v1","signed_at":"2026-07-04T15:56:49.854507Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/9411023","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9ca8c7876f47ea6a79e549f4af4ac260bf9b9be8564aef5e9f692e687fd77193","sha256:7e7d5028399f4935f5c0244493cf1175d289f184b67ca583063b56242c379bd3"],"state_sha256":"eb3e99420e542e4dab8d60c33e3729945876c657110f0a7ef5d2c443880bbad8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"iEZFyRywrFzrSxxTNFRkt1pQckhimUXJBlB/EdsyniG6n35QdVIv8bvN5zsM+1IjlB4RzTazT7VdTPKahC5cBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-15T12:43:48.580106Z","bundle_sha256":"c4221c2266a4c9199db2621c2b9420aea31b48e57aa9336a54369165351dc41a"}}