{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:PXNEQ2VF4Q5V6BZEAPTTE4AKPD","short_pith_number":"pith:PXNEQ2VF","canonical_record":{"source":{"id":"1604.03726","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-04-13T11:50:57Z","cross_cats_sorted":["cond-mat.stat-mech","physics.comp-ph"],"title_canon_sha256":"3794de0e2c94fa9ad748e998ef6753514eb5c4fac48bb947175e427fe90019b5","abstract_canon_sha256":"e7505a8cc7bd04bf6b159949179272c5cacdd53c7a43aaf18d2e1c4ed2ce33bd"},"schema_version":"1.0"},"canonical_sha256":"7dda486aa5e43b5f072403e732700a78ca130055a799bffd1a0d370fc17ad91d","source":{"kind":"arxiv","id":"1604.03726","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.03726","created_at":"2026-05-18T00:46:42Z"},{"alias_kind":"arxiv_version","alias_value":"1604.03726v3","created_at":"2026-05-18T00:46:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.03726","created_at":"2026-05-18T00:46:42Z"},{"alias_kind":"pith_short_12","alias_value":"PXNEQ2VF4Q5V","created_at":"2026-05-18T12:30:39Z"},{"alias_kind":"pith_short_16","alias_value":"PXNEQ2VF4Q5V6BZE","created_at":"2026-05-18T12:30:39Z"},{"alias_kind":"pith_short_8","alias_value":"PXNEQ2VF","created_at":"2026-05-18T12:30:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:PXNEQ2VF4Q5V6BZEAPTTE4AKPD","target":"record","payload":{"canonical_record":{"source":{"id":"1604.03726","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-04-13T11:50:57Z","cross_cats_sorted":["cond-mat.stat-mech","physics.comp-ph"],"title_canon_sha256":"3794de0e2c94fa9ad748e998ef6753514eb5c4fac48bb947175e427fe90019b5","abstract_canon_sha256":"e7505a8cc7bd04bf6b159949179272c5cacdd53c7a43aaf18d2e1c4ed2ce33bd"},"schema_version":"1.0"},"canonical_sha256":"7dda486aa5e43b5f072403e732700a78ca130055a799bffd1a0d370fc17ad91d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:46:42.694464Z","signature_b64":"+faHHKG/tyYuC8gd3Ii69GZTY9aM+tMx6F1CsahW7YWNtbnQGcq91wJTa9WHVaHIWQ8g3obMb/yM54V/wN1eDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7dda486aa5e43b5f072403e732700a78ca130055a799bffd1a0d370fc17ad91d","last_reissued_at":"2026-05-18T00:46:42.693816Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:46:42.693816Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1604.03726","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":"2026-05-18T00:46:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"H5CRj3KfpoF82wFa53m1Ek8e+JdaJqba6BzrH4DiOvvBAHUuvJRUauemID9NsG5buw28jVSK3f41mxpay+JxDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T22:32:31.285573Z"},"content_sha256":"29fe7c4f3789c8ea944878a7d95b8f28b050516debc7749b1d14bed5b9d37151","schema_version":"1.0","event_id":"sha256:29fe7c4f3789c8ea944878a7d95b8f28b050516debc7749b1d14bed5b9d37151"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:PXNEQ2VF4Q5V6BZEAPTTE4AKPD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spatio-temporal patterns in ultra-slow domain wall creep dynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","physics.comp-ph"],"primary_cat":"cond-mat.dis-nn","authors_text":"Alberto Rosso, Alejandro B. Kolton, Ezequiel E. Ferrero, Laura Foini, Thierry Giamarchi","submitted_at":"2016-04-13T11:50:57Z","abstract_excerpt":"In presence of impurities, ferromagnetic and ferroelectric domain walls slide only above a finite external field. Close to this depinning threshold, they proceed by large and abrupt jumps, called avalanches, while, at much smaller field, these interfaces creep by thermal activation. In this work we develop a novel numerical technique that captures the ultra-slow creep regime over huge time scales. We point out the existence of activated events that involve collective reorganizations similar to avalanches, but, at variance with them, display correlated spatio-temporal patterns that resemble the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.03726","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":"2026-05-18T00:46:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IoC1LibZow2FGX/4vVSWfVgruM//A0v+Uixfztq1x5YQvSUlN0AkBKFuW6FRga98u9Na1jIsEA6AADGmO1riDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T22:32:31.286227Z"},"content_sha256":"9133c8c5c7e43cfbb4f44efcabdaa2eb9fdfd40cf5aaa44e5b05a611a437603b","schema_version":"1.0","event_id":"sha256:9133c8c5c7e43cfbb4f44efcabdaa2eb9fdfd40cf5aaa44e5b05a611a437603b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PXNEQ2VF4Q5V6BZEAPTTE4AKPD/bundle.json","state_url":"https://pith.science/pith/PXNEQ2VF4Q5V6BZEAPTTE4AKPD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PXNEQ2VF4Q5V6BZEAPTTE4AKPD/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":"2026-05-29T22:32:31Z","links":{"resolver":"https://pith.science/pith/PXNEQ2VF4Q5V6BZEAPTTE4AKPD","bundle":"https://pith.science/pith/PXNEQ2VF4Q5V6BZEAPTTE4AKPD/bundle.json","state":"https://pith.science/pith/PXNEQ2VF4Q5V6BZEAPTTE4AKPD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PXNEQ2VF4Q5V6BZEAPTTE4AKPD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:PXNEQ2VF4Q5V6BZEAPTTE4AKPD","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":"e7505a8cc7bd04bf6b159949179272c5cacdd53c7a43aaf18d2e1c4ed2ce33bd","cross_cats_sorted":["cond-mat.stat-mech","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-04-13T11:50:57Z","title_canon_sha256":"3794de0e2c94fa9ad748e998ef6753514eb5c4fac48bb947175e427fe90019b5"},"schema_version":"1.0","source":{"id":"1604.03726","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1604.03726","created_at":"2026-05-18T00:46:42Z"},{"alias_kind":"arxiv_version","alias_value":"1604.03726v3","created_at":"2026-05-18T00:46:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.03726","created_at":"2026-05-18T00:46:42Z"},{"alias_kind":"pith_short_12","alias_value":"PXNEQ2VF4Q5V","created_at":"2026-05-18T12:30:39Z"},{"alias_kind":"pith_short_16","alias_value":"PXNEQ2VF4Q5V6BZE","created_at":"2026-05-18T12:30:39Z"},{"alias_kind":"pith_short_8","alias_value":"PXNEQ2VF","created_at":"2026-05-18T12:30:39Z"}],"graph_snapshots":[{"event_id":"sha256:9133c8c5c7e43cfbb4f44efcabdaa2eb9fdfd40cf5aaa44e5b05a611a437603b","target":"graph","created_at":"2026-05-18T00:46:42Z","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":"In presence of impurities, ferromagnetic and ferroelectric domain walls slide only above a finite external field. Close to this depinning threshold, they proceed by large and abrupt jumps, called avalanches, while, at much smaller field, these interfaces creep by thermal activation. In this work we develop a novel numerical technique that captures the ultra-slow creep regime over huge time scales. We point out the existence of activated events that involve collective reorganizations similar to avalanches, but, at variance with them, display correlated spatio-temporal patterns that resemble the","authors_text":"Alberto Rosso, Alejandro B. Kolton, Ezequiel E. Ferrero, Laura Foini, Thierry Giamarchi","cross_cats":["cond-mat.stat-mech","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-04-13T11:50:57Z","title":"Spatio-temporal patterns in ultra-slow domain wall creep dynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.03726","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":"sha256:29fe7c4f3789c8ea944878a7d95b8f28b050516debc7749b1d14bed5b9d37151","target":"record","created_at":"2026-05-18T00:46:42Z","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":"e7505a8cc7bd04bf6b159949179272c5cacdd53c7a43aaf18d2e1c4ed2ce33bd","cross_cats_sorted":["cond-mat.stat-mech","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-04-13T11:50:57Z","title_canon_sha256":"3794de0e2c94fa9ad748e998ef6753514eb5c4fac48bb947175e427fe90019b5"},"schema_version":"1.0","source":{"id":"1604.03726","kind":"arxiv","version":3}},"canonical_sha256":"7dda486aa5e43b5f072403e732700a78ca130055a799bffd1a0d370fc17ad91d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7dda486aa5e43b5f072403e732700a78ca130055a799bffd1a0d370fc17ad91d","first_computed_at":"2026-05-18T00:46:42.693816Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:46:42.693816Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"+faHHKG/tyYuC8gd3Ii69GZTY9aM+tMx6F1CsahW7YWNtbnQGcq91wJTa9WHVaHIWQ8g3obMb/yM54V/wN1eDg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:46:42.694464Z","signed_message":"canonical_sha256_bytes"},"source_id":"1604.03726","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:29fe7c4f3789c8ea944878a7d95b8f28b050516debc7749b1d14bed5b9d37151","sha256:9133c8c5c7e43cfbb4f44efcabdaa2eb9fdfd40cf5aaa44e5b05a611a437603b"],"state_sha256":"d5a97f3c8a02ac792f2cbcc5c358303a30b83e8a9f9591b46cfd58bc6e110275"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OY3z26Pp8bCEI2S2rpVotZuKyIsYOny7mKoPQO1rUMPb+x0a9oomLUm3+zhfTfVHL2FvyeWpd7Wqu0UHavT9AA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T22:32:31.289917Z","bundle_sha256":"5971eabe11dced9e7c6d8c2424ec65950a4b878fe36a3cb12fa252bc032cbd8e"}}