{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:TSCWUGK3OZLAVSRQQN4GWN7HNW","short_pith_number":"pith:TSCWUGK3","canonical_record":{"source":{"id":"1703.01502","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-04T17:55:44Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"118726fb24452f61ac39c6726a15145756f5fe87cd7ded2ccb206826dbbbe5e0","abstract_canon_sha256":"2bdb52aaf14c1ae90e1ae03520d9afb191f4131866a917f075d048ee6a2d08e2"},"schema_version":"1.0"},"canonical_sha256":"9c856a195b76560aca3083786b37e76dabedd654c4ad1739f8332b054d4e9b24","source":{"kind":"arxiv","id":"1703.01502","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.01502","created_at":"2026-05-18T00:49:30Z"},{"alias_kind":"arxiv_version","alias_value":"1703.01502v1","created_at":"2026-05-18T00:49:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.01502","created_at":"2026-05-18T00:49:30Z"},{"alias_kind":"pith_short_12","alias_value":"TSCWUGK3OZLA","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_16","alias_value":"TSCWUGK3OZLAVSRQ","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_8","alias_value":"TSCWUGK3","created_at":"2026-05-18T12:31:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:TSCWUGK3OZLAVSRQQN4GWN7HNW","target":"record","payload":{"canonical_record":{"source":{"id":"1703.01502","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-04T17:55:44Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"118726fb24452f61ac39c6726a15145756f5fe87cd7ded2ccb206826dbbbe5e0","abstract_canon_sha256":"2bdb52aaf14c1ae90e1ae03520d9afb191f4131866a917f075d048ee6a2d08e2"},"schema_version":"1.0"},"canonical_sha256":"9c856a195b76560aca3083786b37e76dabedd654c4ad1739f8332b054d4e9b24","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:49:30.508163Z","signature_b64":"Nm8bVF67ojg2B+Hv857d47ZmPxWCk56sd8YaNVMBmedILUdlPDTZQZz52ipgQ7DV/IBUEgveI0SVYsNtE1+XBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9c856a195b76560aca3083786b37e76dabedd654c4ad1739f8332b054d4e9b24","last_reissued_at":"2026-05-18T00:49:30.507415Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:49:30.507415Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1703.01502","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":"2026-05-18T00:49:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BG070IUO6k20Hs0eKYXNOMj+8gq7t5FUMYvJBVsCbl278vwhX4kbtwi5tQt4CkECNwtMAwYKRXgqttJ0RfiOAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T09:27:28.602743Z"},"content_sha256":"6e1697e338fa95cac2c0db9e08845af0e50b2209eb6a848904e70d5df159b632","schema_version":"1.0","event_id":"sha256:6e1697e338fa95cac2c0db9e08845af0e50b2209eb6a848904e70d5df159b632"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:TSCWUGK3OZLAVSRQQN4GWN7HNW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamics of domain walls in weak ferromagnets","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.stat-mech","authors_text":"A. K. Zvezdin","submitted_at":"2017-03-04T17:55:44Z","abstract_excerpt":"It is shown that the total set of equations, which determines the dynamics of the domain bounds (DB) in a weak ferromagnet, has the same type of specific solution as the well-known Walker's solution for ferromagnets. We calculated the functional dependence of the velocity of the DB on the magnetic field, which is described by the obtained solution. This function has a maximum at a finite field and a section of the negative differential mobility of the DB. According to the calculation, the maximum velocity $ c \\approx 2 \\times 10^6$ cm/sec in YFeO$_3$ is reached at $H_m \\approx 4 \\times 10^3$ O"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.01502","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":"2026-05-18T00:49:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kMVCot8rHPRsjPD2ua7wmaIHGvhl1RHfD40yDQrdHYxPrz4L3/33n5dc5UJtQ9AGWHW0f4iGDq1qr1+JnxiiAA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T09:27:28.603158Z"},"content_sha256":"a230ac509521f27efdc4a54ed02eb3da2e50514ce81554696e216ed2975e878b","schema_version":"1.0","event_id":"sha256:a230ac509521f27efdc4a54ed02eb3da2e50514ce81554696e216ed2975e878b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TSCWUGK3OZLAVSRQQN4GWN7HNW/bundle.json","state_url":"https://pith.science/pith/TSCWUGK3OZLAVSRQQN4GWN7HNW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TSCWUGK3OZLAVSRQQN4GWN7HNW/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":"2026-05-25T09:27:28Z","links":{"resolver":"https://pith.science/pith/TSCWUGK3OZLAVSRQQN4GWN7HNW","bundle":"https://pith.science/pith/TSCWUGK3OZLAVSRQQN4GWN7HNW/bundle.json","state":"https://pith.science/pith/TSCWUGK3OZLAVSRQQN4GWN7HNW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TSCWUGK3OZLAVSRQQN4GWN7HNW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:TSCWUGK3OZLAVSRQQN4GWN7HNW","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":"2bdb52aaf14c1ae90e1ae03520d9afb191f4131866a917f075d048ee6a2d08e2","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-04T17:55:44Z","title_canon_sha256":"118726fb24452f61ac39c6726a15145756f5fe87cd7ded2ccb206826dbbbe5e0"},"schema_version":"1.0","source":{"id":"1703.01502","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1703.01502","created_at":"2026-05-18T00:49:30Z"},{"alias_kind":"arxiv_version","alias_value":"1703.01502v1","created_at":"2026-05-18T00:49:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.01502","created_at":"2026-05-18T00:49:30Z"},{"alias_kind":"pith_short_12","alias_value":"TSCWUGK3OZLA","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_16","alias_value":"TSCWUGK3OZLAVSRQ","created_at":"2026-05-18T12:31:46Z"},{"alias_kind":"pith_short_8","alias_value":"TSCWUGK3","created_at":"2026-05-18T12:31:46Z"}],"graph_snapshots":[{"event_id":"sha256:a230ac509521f27efdc4a54ed02eb3da2e50514ce81554696e216ed2975e878b","target":"graph","created_at":"2026-05-18T00:49:30Z","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":"It is shown that the total set of equations, which determines the dynamics of the domain bounds (DB) in a weak ferromagnet, has the same type of specific solution as the well-known Walker's solution for ferromagnets. We calculated the functional dependence of the velocity of the DB on the magnetic field, which is described by the obtained solution. This function has a maximum at a finite field and a section of the negative differential mobility of the DB. According to the calculation, the maximum velocity $ c \\approx 2 \\times 10^6$ cm/sec in YFeO$_3$ is reached at $H_m \\approx 4 \\times 10^3$ O","authors_text":"A. K. Zvezdin","cross_cats":["cond-mat.mtrl-sci"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-04T17:55:44Z","title":"Dynamics of domain walls in weak ferromagnets"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.01502","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":"sha256:6e1697e338fa95cac2c0db9e08845af0e50b2209eb6a848904e70d5df159b632","target":"record","created_at":"2026-05-18T00:49:30Z","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":"2bdb52aaf14c1ae90e1ae03520d9afb191f4131866a917f075d048ee6a2d08e2","cross_cats_sorted":["cond-mat.mtrl-sci"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-03-04T17:55:44Z","title_canon_sha256":"118726fb24452f61ac39c6726a15145756f5fe87cd7ded2ccb206826dbbbe5e0"},"schema_version":"1.0","source":{"id":"1703.01502","kind":"arxiv","version":1}},"canonical_sha256":"9c856a195b76560aca3083786b37e76dabedd654c4ad1739f8332b054d4e9b24","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9c856a195b76560aca3083786b37e76dabedd654c4ad1739f8332b054d4e9b24","first_computed_at":"2026-05-18T00:49:30.507415Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:49:30.507415Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Nm8bVF67ojg2B+Hv857d47ZmPxWCk56sd8YaNVMBmedILUdlPDTZQZz52ipgQ7DV/IBUEgveI0SVYsNtE1+XBA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:49:30.508163Z","signed_message":"canonical_sha256_bytes"},"source_id":"1703.01502","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6e1697e338fa95cac2c0db9e08845af0e50b2209eb6a848904e70d5df159b632","sha256:a230ac509521f27efdc4a54ed02eb3da2e50514ce81554696e216ed2975e878b"],"state_sha256":"24bb0a8f0286c41a774c073023a8a644268c5ebcc7036f36a38da1bb17ca8e25"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9z08puwJuGNWxXccRFtcj9FfPKGIdhT7DXcUKKfPsUiUwce8CB9Koqr7S4ckPx7ZpTgsU41QgU25FnyHJUg3Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T09:27:28.606351Z","bundle_sha256":"bb4dd03e61e2a7e5c46d31530c4f3dba63de473375884d98eb4bbd5d372dd5c6"}}