{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:WXUM6VIJEYJ4AYH253XTMMZ7PA","short_pith_number":"pith:WXUM6VIJ","canonical_record":{"source":{"id":"1110.6883","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-10-31T18:17:40Z","cross_cats_sorted":[],"title_canon_sha256":"18fa70484463cc8a5a577dfd1bf5dfcc14b835bfc06f8d274bafa716e8f99a4c","abstract_canon_sha256":"94099181170ab28bbf6cbc6ff826d24ac8f1dedec551bbdc05333eb4f721178e"},"schema_version":"1.0"},"canonical_sha256":"b5e8cf55092613c060faeeef36333f783517cf84a75ccc562c11145278c018c0","source":{"kind":"arxiv","id":"1110.6883","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1110.6883","created_at":"2026-05-18T04:09:53Z"},{"alias_kind":"arxiv_version","alias_value":"1110.6883v1","created_at":"2026-05-18T04:09:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.6883","created_at":"2026-05-18T04:09:53Z"},{"alias_kind":"pith_short_12","alias_value":"WXUM6VIJEYJ4","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"WXUM6VIJEYJ4AYH2","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"WXUM6VIJ","created_at":"2026-05-18T12:26:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:WXUM6VIJEYJ4AYH253XTMMZ7PA","target":"record","payload":{"canonical_record":{"source":{"id":"1110.6883","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-10-31T18:17:40Z","cross_cats_sorted":[],"title_canon_sha256":"18fa70484463cc8a5a577dfd1bf5dfcc14b835bfc06f8d274bafa716e8f99a4c","abstract_canon_sha256":"94099181170ab28bbf6cbc6ff826d24ac8f1dedec551bbdc05333eb4f721178e"},"schema_version":"1.0"},"canonical_sha256":"b5e8cf55092613c060faeeef36333f783517cf84a75ccc562c11145278c018c0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:09:53.978562Z","signature_b64":"2hhzGlNYoVtWa3x1lM9TT1IeqWuWTEuxr6FfQBE/tiSxXs9j9VXHRbahF2BxyGNKzRyT4HItal/2J4AgAs0yDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b5e8cf55092613c060faeeef36333f783517cf84a75ccc562c11145278c018c0","last_reissued_at":"2026-05-18T04:09:53.978062Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:09:53.978062Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1110.6883","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":"2026-05-18T04:09:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8cG4faALgiKck0pYT1VPW8CGcAqmMe3DrWdB62YDIl8X76dEaHQ2ZUwo0AfkVuYkfgrUU4SXaKMOgHB0CsjUDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T02:13:30.383545Z"},"content_sha256":"0a851c72976abe0756cb2cd0312399e97f96b7055dca730d0bb6cdff42d9eda4","schema_version":"1.0","event_id":"sha256:0a851c72976abe0756cb2cd0312399e97f96b7055dca730d0bb6cdff42d9eda4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:WXUM6VIJEYJ4AYH253XTMMZ7PA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fundamental switching field distribution of a single domain particle derived from the N\\'eel-Brown model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Bernhard Bergmair, Christoph Vogler, Dieter Suess, Hubert Brueckl, Leoni Breth, Markus Fuger, Rudolf Heer","submitted_at":"2011-10-31T18:17:40Z","abstract_excerpt":"We present an analytical derivation of the switching field distribution for a single domain particle from the N\\'eel-Brown model in the presence of a linearly swept magnetic field and influenced by thermal fluctuations. We show that the switching field distribution corresponds to a probability density function and can be obtained by solving a master equation for the not-switching probability together with the transition rate for the magnetization according to the Arrhenius-N\\'eel Law. By calculating the first and second moments of the probability density function we succeed in modeling rate-de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.6883","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":"2026-05-18T04:09:53Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"oQaDGYWiOPClEXAqympf+p1wQCKWdrb6gP1EuK7x+GuJfrvBY8KzwRJds0gc6St5knhcyrDaeGVWrr0Gk8mKDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-27T02:13:30.384238Z"},"content_sha256":"cf0b0e4da16e71755663a63e3047e90d7e49db50e4e5719790c3368df7402269","schema_version":"1.0","event_id":"sha256:cf0b0e4da16e71755663a63e3047e90d7e49db50e4e5719790c3368df7402269"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WXUM6VIJEYJ4AYH253XTMMZ7PA/bundle.json","state_url":"https://pith.science/pith/WXUM6VIJEYJ4AYH253XTMMZ7PA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WXUM6VIJEYJ4AYH253XTMMZ7PA/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":"2026-05-27T02:13:30Z","links":{"resolver":"https://pith.science/pith/WXUM6VIJEYJ4AYH253XTMMZ7PA","bundle":"https://pith.science/pith/WXUM6VIJEYJ4AYH253XTMMZ7PA/bundle.json","state":"https://pith.science/pith/WXUM6VIJEYJ4AYH253XTMMZ7PA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WXUM6VIJEYJ4AYH253XTMMZ7PA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:WXUM6VIJEYJ4AYH253XTMMZ7PA","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":"94099181170ab28bbf6cbc6ff826d24ac8f1dedec551bbdc05333eb4f721178e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-10-31T18:17:40Z","title_canon_sha256":"18fa70484463cc8a5a577dfd1bf5dfcc14b835bfc06f8d274bafa716e8f99a4c"},"schema_version":"1.0","source":{"id":"1110.6883","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1110.6883","created_at":"2026-05-18T04:09:53Z"},{"alias_kind":"arxiv_version","alias_value":"1110.6883v1","created_at":"2026-05-18T04:09:53Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.6883","created_at":"2026-05-18T04:09:53Z"},{"alias_kind":"pith_short_12","alias_value":"WXUM6VIJEYJ4","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"WXUM6VIJEYJ4AYH2","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"WXUM6VIJ","created_at":"2026-05-18T12:26:44Z"}],"graph_snapshots":[{"event_id":"sha256:cf0b0e4da16e71755663a63e3047e90d7e49db50e4e5719790c3368df7402269","target":"graph","created_at":"2026-05-18T04:09:53Z","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 present an analytical derivation of the switching field distribution for a single domain particle from the N\\'eel-Brown model in the presence of a linearly swept magnetic field and influenced by thermal fluctuations. We show that the switching field distribution corresponds to a probability density function and can be obtained by solving a master equation for the not-switching probability together with the transition rate for the magnetization according to the Arrhenius-N\\'eel Law. By calculating the first and second moments of the probability density function we succeed in modeling rate-de","authors_text":"Bernhard Bergmair, Christoph Vogler, Dieter Suess, Hubert Brueckl, Leoni Breth, Markus Fuger, Rudolf Heer","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-10-31T18:17:40Z","title":"Fundamental switching field distribution of a single domain particle derived from the N\\'eel-Brown model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.6883","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":"sha256:0a851c72976abe0756cb2cd0312399e97f96b7055dca730d0bb6cdff42d9eda4","target":"record","created_at":"2026-05-18T04:09:53Z","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":"94099181170ab28bbf6cbc6ff826d24ac8f1dedec551bbdc05333eb4f721178e","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-10-31T18:17:40Z","title_canon_sha256":"18fa70484463cc8a5a577dfd1bf5dfcc14b835bfc06f8d274bafa716e8f99a4c"},"schema_version":"1.0","source":{"id":"1110.6883","kind":"arxiv","version":1}},"canonical_sha256":"b5e8cf55092613c060faeeef36333f783517cf84a75ccc562c11145278c018c0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b5e8cf55092613c060faeeef36333f783517cf84a75ccc562c11145278c018c0","first_computed_at":"2026-05-18T04:09:53.978062Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:09:53.978062Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2hhzGlNYoVtWa3x1lM9TT1IeqWuWTEuxr6FfQBE/tiSxXs9j9VXHRbahF2BxyGNKzRyT4HItal/2J4AgAs0yDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:09:53.978562Z","signed_message":"canonical_sha256_bytes"},"source_id":"1110.6883","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0a851c72976abe0756cb2cd0312399e97f96b7055dca730d0bb6cdff42d9eda4","sha256:cf0b0e4da16e71755663a63e3047e90d7e49db50e4e5719790c3368df7402269"],"state_sha256":"5883bfce0f735c62c88c7b633739627e081a59c302a927c9c6cc7be98b2c37e1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WG+Z3WuUWcbzgIHOvp6GhyWAjNL4QG1/+0bAz/nOVVdJ8kjBiKvmRsHjxe8NkT2y40TifayVqxzhB9e6nWqIBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-27T02:13:30.387802Z","bundle_sha256":"736d499c125cc3ab3504faf9ba821cd68314bde1290733957ae4790706d00748"}}