{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:NSEYHKUBIKAXPWIE6QHLRJDB55","short_pith_number":"pith:NSEYHKUB","canonical_record":{"source":{"id":"1109.2996","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-09-14T05:50:57Z","cross_cats_sorted":[],"title_canon_sha256":"e956030b58e78dfd1f2d89b8de19fcff35fa3803878e82efb1f40e8dac38a7fe","abstract_canon_sha256":"ab87c2e0b0f55b6b686392711454cc50afc8b77ce9f6dc5d1671c423890f45b7"},"schema_version":"1.0"},"canonical_sha256":"6c8983aa81428177d904f40eb8a461ef54924325e631675dd0999448d97ef995","source":{"kind":"arxiv","id":"1109.2996","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1109.2996","created_at":"2026-05-18T03:53:45Z"},{"alias_kind":"arxiv_version","alias_value":"1109.2996v2","created_at":"2026-05-18T03:53:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.2996","created_at":"2026-05-18T03:53:45Z"},{"alias_kind":"pith_short_12","alias_value":"NSEYHKUBIKAX","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_16","alias_value":"NSEYHKUBIKAXPWIE","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_8","alias_value":"NSEYHKUB","created_at":"2026-05-18T12:26:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:NSEYHKUBIKAXPWIE6QHLRJDB55","target":"record","payload":{"canonical_record":{"source":{"id":"1109.2996","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-09-14T05:50:57Z","cross_cats_sorted":[],"title_canon_sha256":"e956030b58e78dfd1f2d89b8de19fcff35fa3803878e82efb1f40e8dac38a7fe","abstract_canon_sha256":"ab87c2e0b0f55b6b686392711454cc50afc8b77ce9f6dc5d1671c423890f45b7"},"schema_version":"1.0"},"canonical_sha256":"6c8983aa81428177d904f40eb8a461ef54924325e631675dd0999448d97ef995","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:53:45.103760Z","signature_b64":"CH1T/Paq+lSSRtFRa949caTNtvk3cDciWZfQyVarFUGUi3GykS/g3HkNBZGhjkLBYozt7FVTZJOcLnSy45ZBDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6c8983aa81428177d904f40eb8a461ef54924325e631675dd0999448d97ef995","last_reissued_at":"2026-05-18T03:53:45.102950Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:53:45.102950Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1109.2996","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:53:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QSjJemBnZdtVpmOlf05Pnfz85mDO5Expl2wM5qc5Og8c/dme34T5mn1Id/NpKuxJeYvH4KoV8kTUmF7Z16WMAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T21:00:39.807711Z"},"content_sha256":"b1ea33692acbdc135cdecb89de30488d6c0cb5b3a2944d0c08dcfbd6df5bfc47","schema_version":"1.0","event_id":"sha256:b1ea33692acbdc135cdecb89de30488d6c0cb5b3a2944d0c08dcfbd6df5bfc47"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:NSEYHKUBIKAXPWIE6QHLRJDB55","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Domain-wall dynamics in translationally noninvariant nanowires: theory and applications","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.mes-hall","authors_text":"Ar. Abanov, O. A. Tretiakov, Y. Liu","submitted_at":"2011-09-14T05:50:57Z","abstract_excerpt":"We generalize domain-wall dynamics to the case of translationally noninvariant ferromagnetic nanowires. The obtained equations of motion make the description of the domain-wall propagation more realistic by accounting for the variations along the wire, such as disorder or change in the wire shape. We show that the effective equations of motion are very general and do not depend on the model details. As an example of their use, we consider an hourglass-shaped nanostrip in detail. A transverse domain wall is trapped in the middle and has two stable magnetization directions. We study the switchin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.2996","kind":"arxiv","version":2},"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":"2026-05-18T03:53:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7J141DkkWVpQNuvVWlp1k4wEEYiTyA+5Ax8Qkqqoxe7kmXHh/vvOHs8YqYFV/S16EpEskRBlm7W+Fmv8onQaDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T21:00:39.808391Z"},"content_sha256":"6b815e14688876c55857ad75f8ea1b6310bd04bcccc3af9768ff56f6c2bb9d30","schema_version":"1.0","event_id":"sha256:6b815e14688876c55857ad75f8ea1b6310bd04bcccc3af9768ff56f6c2bb9d30"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NSEYHKUBIKAXPWIE6QHLRJDB55/bundle.json","state_url":"https://pith.science/pith/NSEYHKUBIKAXPWIE6QHLRJDB55/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NSEYHKUBIKAXPWIE6QHLRJDB55/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":"2026-05-26T21:00:39Z","links":{"resolver":"https://pith.science/pith/NSEYHKUBIKAXPWIE6QHLRJDB55","bundle":"https://pith.science/pith/NSEYHKUBIKAXPWIE6QHLRJDB55/bundle.json","state":"https://pith.science/pith/NSEYHKUBIKAXPWIE6QHLRJDB55/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NSEYHKUBIKAXPWIE6QHLRJDB55/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:NSEYHKUBIKAXPWIE6QHLRJDB55","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":"ab87c2e0b0f55b6b686392711454cc50afc8b77ce9f6dc5d1671c423890f45b7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-09-14T05:50:57Z","title_canon_sha256":"e956030b58e78dfd1f2d89b8de19fcff35fa3803878e82efb1f40e8dac38a7fe"},"schema_version":"1.0","source":{"id":"1109.2996","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1109.2996","created_at":"2026-05-18T03:53:45Z"},{"alias_kind":"arxiv_version","alias_value":"1109.2996v2","created_at":"2026-05-18T03:53:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.2996","created_at":"2026-05-18T03:53:45Z"},{"alias_kind":"pith_short_12","alias_value":"NSEYHKUBIKAX","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_16","alias_value":"NSEYHKUBIKAXPWIE","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_8","alias_value":"NSEYHKUB","created_at":"2026-05-18T12:26:37Z"}],"graph_snapshots":[{"event_id":"sha256:6b815e14688876c55857ad75f8ea1b6310bd04bcccc3af9768ff56f6c2bb9d30","target":"graph","created_at":"2026-05-18T03:53:45Z","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 generalize domain-wall dynamics to the case of translationally noninvariant ferromagnetic nanowires. The obtained equations of motion make the description of the domain-wall propagation more realistic by accounting for the variations along the wire, such as disorder or change in the wire shape. We show that the effective equations of motion are very general and do not depend on the model details. As an example of their use, we consider an hourglass-shaped nanostrip in detail. A transverse domain wall is trapped in the middle and has two stable magnetization directions. We study the switchin","authors_text":"Ar. Abanov, O. A. Tretiakov, Y. Liu","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-09-14T05:50:57Z","title":"Domain-wall dynamics in translationally noninvariant nanowires: theory and applications"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.2996","kind":"arxiv","version":2},"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:b1ea33692acbdc135cdecb89de30488d6c0cb5b3a2944d0c08dcfbd6df5bfc47","target":"record","created_at":"2026-05-18T03:53:45Z","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":"ab87c2e0b0f55b6b686392711454cc50afc8b77ce9f6dc5d1671c423890f45b7","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2011-09-14T05:50:57Z","title_canon_sha256":"e956030b58e78dfd1f2d89b8de19fcff35fa3803878e82efb1f40e8dac38a7fe"},"schema_version":"1.0","source":{"id":"1109.2996","kind":"arxiv","version":2}},"canonical_sha256":"6c8983aa81428177d904f40eb8a461ef54924325e631675dd0999448d97ef995","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6c8983aa81428177d904f40eb8a461ef54924325e631675dd0999448d97ef995","first_computed_at":"2026-05-18T03:53:45.102950Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:53:45.102950Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"CH1T/Paq+lSSRtFRa949caTNtvk3cDciWZfQyVarFUGUi3GykS/g3HkNBZGhjkLBYozt7FVTZJOcLnSy45ZBDA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:53:45.103760Z","signed_message":"canonical_sha256_bytes"},"source_id":"1109.2996","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b1ea33692acbdc135cdecb89de30488d6c0cb5b3a2944d0c08dcfbd6df5bfc47","sha256:6b815e14688876c55857ad75f8ea1b6310bd04bcccc3af9768ff56f6c2bb9d30"],"state_sha256":"63462631b60e24699b3a0339be5494eb3ae5762c31231bea25fdec16cc760a0b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ma8vYAtdqjdBmFitog9VPAGV3X8XMs92LpmUmu7x8kukMe/AfEvtSgjHDvoKzn5AyizY7pqTi6bMA99dF6iTBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T21:00:39.811889Z","bundle_sha256":"47210c90bb7ef51927b28930c2f9b596aba681eff83deb95f19e62e3c708cbc0"}}