{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:UCRMO2VRVLSKK6OYOVIVIUC5K7","short_pith_number":"pith:UCRMO2VR","canonical_record":{"source":{"id":"cond-mat/0410035","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2004-10-01T16:29:04Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"53ce89f4f20942d5137d91e5d4208e3572b6b25cd94ec80823fa0babfdf72733","abstract_canon_sha256":"123718ecc1c3eaa44f6dd1babcb5499535f9a3e89d0186f5ed860acdd750c924"},"schema_version":"1.0"},"canonical_sha256":"a0a2c76ab1aae4a579d8755154505d57d0f78dd79db77f330338bbb7e961b0a8","source":{"kind":"arxiv","id":"cond-mat/0410035","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0410035","created_at":"2026-07-04T16:47:07Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0410035v1","created_at":"2026-07-04T16:47:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0410035","created_at":"2026-07-04T16:47:07Z"},{"alias_kind":"pith_short_12","alias_value":"UCRMO2VRVLSK","created_at":"2026-07-04T16:47:07Z"},{"alias_kind":"pith_short_16","alias_value":"UCRMO2VRVLSKK6OY","created_at":"2026-07-04T16:47:07Z"},{"alias_kind":"pith_short_8","alias_value":"UCRMO2VR","created_at":"2026-07-04T16:47:07Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:UCRMO2VRVLSKK6OYOVIVIUC5K7","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0410035","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2004-10-01T16:29:04Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"53ce89f4f20942d5137d91e5d4208e3572b6b25cd94ec80823fa0babfdf72733","abstract_canon_sha256":"123718ecc1c3eaa44f6dd1babcb5499535f9a3e89d0186f5ed860acdd750c924"},"schema_version":"1.0"},"canonical_sha256":"a0a2c76ab1aae4a579d8755154505d57d0f78dd79db77f330338bbb7e961b0a8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:47:07.997015Z","signature_b64":"CRsfLQvkZoIXc8LhZAF5CRkvSn3roDtPFM+9m3esHGNP6o7E83WIJxnlPEsY41PpzCnWLwKVcLSobXG3qQQBCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a0a2c76ab1aae4a579d8755154505d57d0f78dd79db77f330338bbb7e961b0a8","last_reissued_at":"2026-07-04T16:47:07.996672Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:47:07.996672Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0410035","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":"2026-07-04T16:47:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"2iXYXSC5mXAXudMIdGCGQTi1U4BGsSoo8HwJ8+Lf1nFxSC2eOIXRTylUJG0O1bfKAyMW8/u4TcsZrFPbTTTZCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T17:13:32.040055Z"},"content_sha256":"16821cfec781feb242c3b7413c37a46ab1dc3a64eea6f1400dbee5420df1dabb","schema_version":"1.0","event_id":"sha256:16821cfec781feb242c3b7413c37a46ab1dc3a64eea6f1400dbee5420df1dabb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:UCRMO2VRVLSKK6OYOVIVIUC5K7","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Current-spin coupling for ferromagnetic domain walls in fine wires","license":"","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"S. E. Barnes, S. Maekawa","submitted_at":"2004-10-01T16:29:04Z","abstract_excerpt":"The coupling between a current and a domain wall is examined. In the presence of a finite current and the absence of a potential which breaks the translational symmetry, there is a perfect transfer of angular momentum from the conduction electrons to the wall. As a result, the ground state is in uniform motion. This remains the case when relaxation is accounted for. This is described by, appropriately modified, Landau-Lifshitz-Gilbert equations."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0410035","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/0410035/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":"2026-07-04T16:47:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fFDU9+Ui++RzdM1npmZMHO6wz58Z8ry7FhK21W0E+krV0RGFk1ceNbYp63Aa5wtGhV/5WCqxYF0QM2KlU4ELCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-07T17:13:32.040979Z"},"content_sha256":"43ae454938a482b13b2e9fc9fa1fedabb40f001cf604cd15dc259d19881613c2","schema_version":"1.0","event_id":"sha256:43ae454938a482b13b2e9fc9fa1fedabb40f001cf604cd15dc259d19881613c2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UCRMO2VRVLSKK6OYOVIVIUC5K7/bundle.json","state_url":"https://pith.science/pith/UCRMO2VRVLSKK6OYOVIVIUC5K7/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UCRMO2VRVLSKK6OYOVIVIUC5K7/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":"2026-08-07T17:13:32Z","links":{"resolver":"https://pith.science/pith/UCRMO2VRVLSKK6OYOVIVIUC5K7","bundle":"https://pith.science/pith/UCRMO2VRVLSKK6OYOVIVIUC5K7/bundle.json","state":"https://pith.science/pith/UCRMO2VRVLSKK6OYOVIVIUC5K7/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UCRMO2VRVLSKK6OYOVIVIUC5K7/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:UCRMO2VRVLSKK6OYOVIVIUC5K7","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":"123718ecc1c3eaa44f6dd1babcb5499535f9a3e89d0186f5ed860acdd750c924","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2004-10-01T16:29:04Z","title_canon_sha256":"53ce89f4f20942d5137d91e5d4208e3572b6b25cd94ec80823fa0babfdf72733"},"schema_version":"1.0","source":{"id":"cond-mat/0410035","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0410035","created_at":"2026-07-04T16:47:07Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0410035v1","created_at":"2026-07-04T16:47:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0410035","created_at":"2026-07-04T16:47:07Z"},{"alias_kind":"pith_short_12","alias_value":"UCRMO2VRVLSK","created_at":"2026-07-04T16:47:07Z"},{"alias_kind":"pith_short_16","alias_value":"UCRMO2VRVLSKK6OY","created_at":"2026-07-04T16:47:07Z"},{"alias_kind":"pith_short_8","alias_value":"UCRMO2VR","created_at":"2026-07-04T16:47:07Z"}],"graph_snapshots":[{"event_id":"sha256:43ae454938a482b13b2e9fc9fa1fedabb40f001cf604cd15dc259d19881613c2","target":"graph","created_at":"2026-07-04T16:47:07Z","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/0410035/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The coupling between a current and a domain wall is examined. In the presence of a finite current and the absence of a potential which breaks the translational symmetry, there is a perfect transfer of angular momentum from the conduction electrons to the wall. As a result, the ground state is in uniform motion. This remains the case when relaxation is accounted for. This is described by, appropriately modified, Landau-Lifshitz-Gilbert equations.","authors_text":"S. E. Barnes, S. Maekawa","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"","primary_cat":"cond-mat.str-el","submitted_at":"2004-10-01T16:29:04Z","title":"Current-spin coupling for ferromagnetic domain walls in fine wires"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0410035","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":"sha256:16821cfec781feb242c3b7413c37a46ab1dc3a64eea6f1400dbee5420df1dabb","target":"record","created_at":"2026-07-04T16:47:07Z","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":"123718ecc1c3eaa44f6dd1babcb5499535f9a3e89d0186f5ed860acdd750c924","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"","primary_cat":"cond-mat.str-el","submitted_at":"2004-10-01T16:29:04Z","title_canon_sha256":"53ce89f4f20942d5137d91e5d4208e3572b6b25cd94ec80823fa0babfdf72733"},"schema_version":"1.0","source":{"id":"cond-mat/0410035","kind":"arxiv","version":1}},"canonical_sha256":"a0a2c76ab1aae4a579d8755154505d57d0f78dd79db77f330338bbb7e961b0a8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a0a2c76ab1aae4a579d8755154505d57d0f78dd79db77f330338bbb7e961b0a8","first_computed_at":"2026-07-04T16:47:07.996672Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:47:07.996672Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"CRsfLQvkZoIXc8LhZAF5CRkvSn3roDtPFM+9m3esHGNP6o7E83WIJxnlPEsY41PpzCnWLwKVcLSobXG3qQQBCw==","signature_status":"signed_v1","signed_at":"2026-07-04T16:47:07.997015Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0410035","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:16821cfec781feb242c3b7413c37a46ab1dc3a64eea6f1400dbee5420df1dabb","sha256:43ae454938a482b13b2e9fc9fa1fedabb40f001cf604cd15dc259d19881613c2"],"state_sha256":"439d0e01505b8d95993cff715edd1c009539d109489e36496a5cd364cb61761e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yZcKhv594rMcYwqb87jDXM9OFl2oqVHkzVL3tuqheVfP3UGqR8eIaIp6eJpgpFJaa2av4tKMMpLlkmDj8f4LCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-07T17:13:32.048594Z","bundle_sha256":"b945d2981dbc5f72fa4e71e7d83c7856c8e5c5e84f2e383fa38bc82ca16d2494"}}