{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:BXDJR5OYTY5BXLMUKXCPBBZUHA","short_pith_number":"pith:BXDJR5OY","canonical_record":{"source":{"id":"1210.3914","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-10-15T06:27:26Z","cross_cats_sorted":["cond-mat.stat-mech","physics.comp-ph"],"title_canon_sha256":"af67e0889aa215b5c7f9e4ebe42969957590f2eaa943941504fcee2fee0a7f7c","abstract_canon_sha256":"b3674d5767e5d53187226b66e56ee77772ad612b8d4974dfd0e446c2cedec2a6"},"schema_version":"1.0"},"canonical_sha256":"0dc698f5d89e3a1bad9455c4f08734381d028be38d7a78438f1e0489e558b0e2","source":{"kind":"arxiv","id":"1210.3914","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.3914","created_at":"2026-05-18T03:43:16Z"},{"alias_kind":"arxiv_version","alias_value":"1210.3914v1","created_at":"2026-05-18T03:43:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.3914","created_at":"2026-05-18T03:43:16Z"},{"alias_kind":"pith_short_12","alias_value":"BXDJR5OYTY5B","created_at":"2026-05-18T12:27:01Z"},{"alias_kind":"pith_short_16","alias_value":"BXDJR5OYTY5BXLMU","created_at":"2026-05-18T12:27:01Z"},{"alias_kind":"pith_short_8","alias_value":"BXDJR5OY","created_at":"2026-05-18T12:27:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:BXDJR5OYTY5BXLMUKXCPBBZUHA","target":"record","payload":{"canonical_record":{"source":{"id":"1210.3914","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2012-10-15T06:27:26Z","cross_cats_sorted":["cond-mat.stat-mech","physics.comp-ph"],"title_canon_sha256":"af67e0889aa215b5c7f9e4ebe42969957590f2eaa943941504fcee2fee0a7f7c","abstract_canon_sha256":"b3674d5767e5d53187226b66e56ee77772ad612b8d4974dfd0e446c2cedec2a6"},"schema_version":"1.0"},"canonical_sha256":"0dc698f5d89e3a1bad9455c4f08734381d028be38d7a78438f1e0489e558b0e2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:43:16.767666Z","signature_b64":"zOqIE7IVEtaad0vnkT/scfGy28A2CYPw+yCPWD8PlnVp8kT3WJ4M0rnr2Bty5w/Fy0zbkwO8/Rbuo5Kcl9ZNBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0dc698f5d89e3a1bad9455c4f08734381d028be38d7a78438f1e0489e558b0e2","last_reissued_at":"2026-05-18T03:43:16.767056Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:43:16.767056Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1210.3914","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":"2026-05-18T03:43:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cijvGN4OjmxjzzoBWE6lbPB4qtBIndJh00GvPidtwDdpD3uYtaEIzFqaEPJtS6dVw2qvOJ5zGhZIKAUOGwm6AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T03:29:22.897970Z"},"content_sha256":"3cd7765b4b37c847bb0e698f680abe020636429ef90b35359b8142c4f9140dbe","schema_version":"1.0","event_id":"sha256:3cd7765b4b37c847bb0e698f680abe020636429ef90b35359b8142c4f9140dbe"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:BXDJR5OYTY5BXLMUKXCPBBZUHA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Depinning phase transition in two-dimensional clock model with quenched randomness","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":"B. Zheng, N. J. Zhou, X. P. Qin","submitted_at":"2012-10-15T06:27:26Z","abstract_excerpt":"With Monte Carlo simulations, we systematically investigate the depinning phase transition in the two-dimensional driven random-field clock model. Based on the short-time dynamic approach, we determine the transition field and critical exponents. The results show that the critical exponents vary with the form of the random-field distribution and the strength of the random fields, and the roughening dynamics of the domain interface belongs to the new subclass with $\\zeta \\neq \\zeta_{loc} \\neq \\zeta_s$ and $\\zeta_{loc} \\neq 1$. More importantly, we find that the transition field and critical exp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.3914","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":"2026-05-18T03:43:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rL8jJ1FvEfjSFFUqYuYVq9a+gX0en1RTcDMGK6ztXrE5LV2QL47L7+k2AoEtg3clA0ywxi3XO/7Sk3N35aiJCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T03:29:22.898333Z"},"content_sha256":"6cd5a56710fa2b4d00aac6b835ff9a2b745bdd9fb13df883b421a1e25c39a2d7","schema_version":"1.0","event_id":"sha256:6cd5a56710fa2b4d00aac6b835ff9a2b745bdd9fb13df883b421a1e25c39a2d7"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BXDJR5OYTY5BXLMUKXCPBBZUHA/bundle.json","state_url":"https://pith.science/pith/BXDJR5OYTY5BXLMUKXCPBBZUHA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BXDJR5OYTY5BXLMUKXCPBBZUHA/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":"2026-06-04T03:29:22Z","links":{"resolver":"https://pith.science/pith/BXDJR5OYTY5BXLMUKXCPBBZUHA","bundle":"https://pith.science/pith/BXDJR5OYTY5BXLMUKXCPBBZUHA/bundle.json","state":"https://pith.science/pith/BXDJR5OYTY5BXLMUKXCPBBZUHA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BXDJR5OYTY5BXLMUKXCPBBZUHA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:BXDJR5OYTY5BXLMUKXCPBBZUHA","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":"b3674d5767e5d53187226b66e56ee77772ad612b8d4974dfd0e446c2cedec2a6","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":"2012-10-15T06:27:26Z","title_canon_sha256":"af67e0889aa215b5c7f9e4ebe42969957590f2eaa943941504fcee2fee0a7f7c"},"schema_version":"1.0","source":{"id":"1210.3914","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1210.3914","created_at":"2026-05-18T03:43:16Z"},{"alias_kind":"arxiv_version","alias_value":"1210.3914v1","created_at":"2026-05-18T03:43:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1210.3914","created_at":"2026-05-18T03:43:16Z"},{"alias_kind":"pith_short_12","alias_value":"BXDJR5OYTY5B","created_at":"2026-05-18T12:27:01Z"},{"alias_kind":"pith_short_16","alias_value":"BXDJR5OYTY5BXLMU","created_at":"2026-05-18T12:27:01Z"},{"alias_kind":"pith_short_8","alias_value":"BXDJR5OY","created_at":"2026-05-18T12:27:01Z"}],"graph_snapshots":[{"event_id":"sha256:6cd5a56710fa2b4d00aac6b835ff9a2b745bdd9fb13df883b421a1e25c39a2d7","target":"graph","created_at":"2026-05-18T03:43:16Z","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":"With Monte Carlo simulations, we systematically investigate the depinning phase transition in the two-dimensional driven random-field clock model. Based on the short-time dynamic approach, we determine the transition field and critical exponents. The results show that the critical exponents vary with the form of the random-field distribution and the strength of the random fields, and the roughening dynamics of the domain interface belongs to the new subclass with $\\zeta \\neq \\zeta_{loc} \\neq \\zeta_s$ and $\\zeta_{loc} \\neq 1$. More importantly, we find that the transition field and critical exp","authors_text":"B. Zheng, N. J. Zhou, X. P. Qin","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":"2012-10-15T06:27:26Z","title":"Depinning phase transition in two-dimensional clock model with quenched randomness"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1210.3914","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":"sha256:3cd7765b4b37c847bb0e698f680abe020636429ef90b35359b8142c4f9140dbe","target":"record","created_at":"2026-05-18T03:43:16Z","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":"b3674d5767e5d53187226b66e56ee77772ad612b8d4974dfd0e446c2cedec2a6","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":"2012-10-15T06:27:26Z","title_canon_sha256":"af67e0889aa215b5c7f9e4ebe42969957590f2eaa943941504fcee2fee0a7f7c"},"schema_version":"1.0","source":{"id":"1210.3914","kind":"arxiv","version":1}},"canonical_sha256":"0dc698f5d89e3a1bad9455c4f08734381d028be38d7a78438f1e0489e558b0e2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0dc698f5d89e3a1bad9455c4f08734381d028be38d7a78438f1e0489e558b0e2","first_computed_at":"2026-05-18T03:43:16.767056Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:43:16.767056Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zOqIE7IVEtaad0vnkT/scfGy28A2CYPw+yCPWD8PlnVp8kT3WJ4M0rnr2Bty5w/Fy0zbkwO8/Rbuo5Kcl9ZNBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:43:16.767666Z","signed_message":"canonical_sha256_bytes"},"source_id":"1210.3914","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3cd7765b4b37c847bb0e698f680abe020636429ef90b35359b8142c4f9140dbe","sha256:6cd5a56710fa2b4d00aac6b835ff9a2b745bdd9fb13df883b421a1e25c39a2d7"],"state_sha256":"548f602ff8ef5f0c3e5a05937ab8c5b972497be4b7fbafe16e5ffbdb66d39708"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rrklhggyTrX4oKxQQwawqwkXblmeuZURXQTotqmFvYHziPWd8ooZoymcuyVuhP4G9bS9yOefvUNBvpD/CY5xDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T03:29:22.900289Z","bundle_sha256":"235ac861966a56bf827024e9b599f3fcc03124162241c37e3131a4317f0fb763"}}