{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:AMJDZIFQTUXWMILQKYG5B5JEUE","short_pith_number":"pith:AMJDZIFQ","canonical_record":{"source":{"id":"1706.10080","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-06-30T09:31:51Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"9010bce76f275445d6ac030353d13cbcacd3f64c2582ca3f761e85e54bbde871","abstract_canon_sha256":"a16d6338f1a381f57609f730c9d0e60d0d4e7b87e622383b73c1642bd44ba081"},"schema_version":"1.0"},"canonical_sha256":"03123ca0b09d2f662170560dd0f524a119a061b3e25dfeb579cfbc1555f32980","source":{"kind":"arxiv","id":"1706.10080","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.10080","created_at":"2026-05-18T00:13:32Z"},{"alias_kind":"arxiv_version","alias_value":"1706.10080v3","created_at":"2026-05-18T00:13:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.10080","created_at":"2026-05-18T00:13:32Z"},{"alias_kind":"pith_short_12","alias_value":"AMJDZIFQTUXW","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_16","alias_value":"AMJDZIFQTUXWMILQ","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_8","alias_value":"AMJDZIFQ","created_at":"2026-05-18T12:31:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:AMJDZIFQTUXWMILQKYG5B5JEUE","target":"record","payload":{"canonical_record":{"source":{"id":"1706.10080","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-06-30T09:31:51Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"9010bce76f275445d6ac030353d13cbcacd3f64c2582ca3f761e85e54bbde871","abstract_canon_sha256":"a16d6338f1a381f57609f730c9d0e60d0d4e7b87e622383b73c1642bd44ba081"},"schema_version":"1.0"},"canonical_sha256":"03123ca0b09d2f662170560dd0f524a119a061b3e25dfeb579cfbc1555f32980","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:13:32.465166Z","signature_b64":"etuh9+ERz4U4i70snfJPuTKVA6hGD4qqv6TNxMNtVLZYDVEXddMFAam45trVImrl9gbml8QnFfqZVV0mTw1pBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"03123ca0b09d2f662170560dd0f524a119a061b3e25dfeb579cfbc1555f32980","last_reissued_at":"2026-05-18T00:13:32.464549Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:13:32.464549Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1706.10080","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":"2026-05-18T00:13:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"x62LF+GbeGtki++zfJYe5HuGMTr7qRpAqi6QHosZuCWYQxeFSVLJQawBDv03HqjUlhtTYkOmZe+Za37bHJwAAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T13:48:19.548780Z"},"content_sha256":"847849db9d255f5b734711221343f05cd7e925ef9a62aadf4f1ff1016381e66a","schema_version":"1.0","event_id":"sha256:847849db9d255f5b734711221343f05cd7e925ef9a62aadf4f1ff1016381e66a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:AMJDZIFQTUXWMILQKYG5B5JEUE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum Brownian motion in a magnetic field: Transition from monotonic to oscillatory behaviour","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"quant-ph","authors_text":"Supurna Sinha, Urbashi Satpathi","submitted_at":"2017-06-30T09:31:51Z","abstract_excerpt":"We investigate the Brownian motion of a charged particle in a magnetic field. We study this in the high temperature classical and low temperature quantum domains. In both domains, we observe a transition of the mean square displacement from a monotonic behaviour to a damped oscillatory behaviour as one increases the strength of the magnetic field. When the strength of the magnetic field is negligible, the mean square displacement grows linearly with time in the classical domain and logarithmically with time in the quantum domain. We notice that these features of the mean square displacement ar"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.10080","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":"2026-05-18T00:13:32Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PvDaNbxVMOxWnWue+kjhVNaLqxJ4LNQWFxjPVJhe8STZixXRwejc3kJEJZNZZAo9iL/qkJRgqsG1kzBHKAnMCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T13:48:19.549512Z"},"content_sha256":"acb1db52a8efa0d6aab0fc696eb0a06eeaea80fd169b4f6c77598b8bee06ac15","schema_version":"1.0","event_id":"sha256:acb1db52a8efa0d6aab0fc696eb0a06eeaea80fd169b4f6c77598b8bee06ac15"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AMJDZIFQTUXWMILQKYG5B5JEUE/bundle.json","state_url":"https://pith.science/pith/AMJDZIFQTUXWMILQKYG5B5JEUE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AMJDZIFQTUXWMILQKYG5B5JEUE/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":"2026-05-28T13:48:19Z","links":{"resolver":"https://pith.science/pith/AMJDZIFQTUXWMILQKYG5B5JEUE","bundle":"https://pith.science/pith/AMJDZIFQTUXWMILQKYG5B5JEUE/bundle.json","state":"https://pith.science/pith/AMJDZIFQTUXWMILQKYG5B5JEUE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AMJDZIFQTUXWMILQKYG5B5JEUE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:AMJDZIFQTUXWMILQKYG5B5JEUE","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":"a16d6338f1a381f57609f730c9d0e60d0d4e7b87e622383b73c1642bd44ba081","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-06-30T09:31:51Z","title_canon_sha256":"9010bce76f275445d6ac030353d13cbcacd3f64c2582ca3f761e85e54bbde871"},"schema_version":"1.0","source":{"id":"1706.10080","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1706.10080","created_at":"2026-05-18T00:13:32Z"},{"alias_kind":"arxiv_version","alias_value":"1706.10080v3","created_at":"2026-05-18T00:13:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.10080","created_at":"2026-05-18T00:13:32Z"},{"alias_kind":"pith_short_12","alias_value":"AMJDZIFQTUXW","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_16","alias_value":"AMJDZIFQTUXWMILQ","created_at":"2026-05-18T12:31:05Z"},{"alias_kind":"pith_short_8","alias_value":"AMJDZIFQ","created_at":"2026-05-18T12:31:05Z"}],"graph_snapshots":[{"event_id":"sha256:acb1db52a8efa0d6aab0fc696eb0a06eeaea80fd169b4f6c77598b8bee06ac15","target":"graph","created_at":"2026-05-18T00:13:32Z","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 investigate the Brownian motion of a charged particle in a magnetic field. We study this in the high temperature classical and low temperature quantum domains. In both domains, we observe a transition of the mean square displacement from a monotonic behaviour to a damped oscillatory behaviour as one increases the strength of the magnetic field. When the strength of the magnetic field is negligible, the mean square displacement grows linearly with time in the classical domain and logarithmically with time in the quantum domain. We notice that these features of the mean square displacement ar","authors_text":"Supurna Sinha, Urbashi Satpathi","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-06-30T09:31:51Z","title":"Quantum Brownian motion in a magnetic field: Transition from monotonic to oscillatory behaviour"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.10080","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":"sha256:847849db9d255f5b734711221343f05cd7e925ef9a62aadf4f1ff1016381e66a","target":"record","created_at":"2026-05-18T00:13:32Z","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":"a16d6338f1a381f57609f730c9d0e60d0d4e7b87e622383b73c1642bd44ba081","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-06-30T09:31:51Z","title_canon_sha256":"9010bce76f275445d6ac030353d13cbcacd3f64c2582ca3f761e85e54bbde871"},"schema_version":"1.0","source":{"id":"1706.10080","kind":"arxiv","version":3}},"canonical_sha256":"03123ca0b09d2f662170560dd0f524a119a061b3e25dfeb579cfbc1555f32980","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"03123ca0b09d2f662170560dd0f524a119a061b3e25dfeb579cfbc1555f32980","first_computed_at":"2026-05-18T00:13:32.464549Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:13:32.464549Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"etuh9+ERz4U4i70snfJPuTKVA6hGD4qqv6TNxMNtVLZYDVEXddMFAam45trVImrl9gbml8QnFfqZVV0mTw1pBg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:13:32.465166Z","signed_message":"canonical_sha256_bytes"},"source_id":"1706.10080","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:847849db9d255f5b734711221343f05cd7e925ef9a62aadf4f1ff1016381e66a","sha256:acb1db52a8efa0d6aab0fc696eb0a06eeaea80fd169b4f6c77598b8bee06ac15"],"state_sha256":"83ae456e03c6dea9f7f87a89960fda617cfb801ced9b0b526b0f1aab9c1df5ad"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8JB9qqxi+ETnxGSOUItQB1kP0Gqo8HQXw+xccIt2h03Whe/gz31WJZF0JIy9Nn8SzgOhw07vbSsrZnMgRweoBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T13:48:19.552247Z","bundle_sha256":"8d4ddf30eaa055bb517e80ce12da4352851972c408405960abfe6a1734999700"}}