{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:53MTILRXH7RZNVVUYOXZJVJLIS","short_pith_number":"pith:53MTILRX","canonical_record":{"source":{"id":"1206.6020","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-06-26T15:14:20Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"4dc8e2c79b1d78c1b3642f20ef5f67146b141186e37f79b91ce17e602dbb5269","abstract_canon_sha256":"0d7d548fe4c2938116787d0a833a11816cb1f9b02424c27b102acb0d3d17b1cf"},"schema_version":"1.0"},"canonical_sha256":"eed9342e373fe396d6b4c3af94d52b449cc6a806df91fed6b46fdb75a553a4a6","source":{"kind":"arxiv","id":"1206.6020","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.6020","created_at":"2026-05-18T03:40:14Z"},{"alias_kind":"arxiv_version","alias_value":"1206.6020v2","created_at":"2026-05-18T03:40:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.6020","created_at":"2026-05-18T03:40:14Z"},{"alias_kind":"pith_short_12","alias_value":"53MTILRXH7RZ","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"53MTILRXH7RZNVVU","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"53MTILRX","created_at":"2026-05-18T12:26:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:53MTILRXH7RZNVVUYOXZJVJLIS","target":"record","payload":{"canonical_record":{"source":{"id":"1206.6020","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-06-26T15:14:20Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"4dc8e2c79b1d78c1b3642f20ef5f67146b141186e37f79b91ce17e602dbb5269","abstract_canon_sha256":"0d7d548fe4c2938116787d0a833a11816cb1f9b02424c27b102acb0d3d17b1cf"},"schema_version":"1.0"},"canonical_sha256":"eed9342e373fe396d6b4c3af94d52b449cc6a806df91fed6b46fdb75a553a4a6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:40:14.032858Z","signature_b64":"vgt4bzdKeGRfsbsDpu2rX+0mADGe/xYhLBIThvKVT7TAmN9I1kISps45v2V0Cdp1CyF2AQ/TYhDMUWZTBimABA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eed9342e373fe396d6b4c3af94d52b449cc6a806df91fed6b46fdb75a553a4a6","last_reissued_at":"2026-05-18T03:40:14.032384Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:40:14.032384Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1206.6020","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":"2026-05-18T03:40:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lHi9OU/enT8qBhEZNNo/3ZjFLwnFwoqSbzqOHF9EBoygAVyP71YaM7lu80gGV+nNAHHf+2qZfMLTFQENIbw4DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T13:17:35.643991Z"},"content_sha256":"a2eeb5c52077e4b8034497d45d995319494fd75624701fcefc5d6665181966cb","schema_version":"1.0","event_id":"sha256:a2eeb5c52077e4b8034497d45d995319494fd75624701fcefc5d6665181966cb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:53MTILRXH7RZNVVUYOXZJVJLIS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spatiotemporal sine-Wiener Bounded Noise and its effect on Ginzburg-Landau model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"cond-mat.stat-mech","authors_text":"Alberto d'Onofrio, Sebastiano de Franciscis","submitted_at":"2012-06-26T15:14:20Z","abstract_excerpt":"In this work, we introduce a kind of spatiotemporal bounded noise derived by the sine-Wiener noise and by the spatially colored unbounded noise introduced by Garc\\'ia-Ojalvo, Sancho and Ram\\'irez-Piscina (GSR noise). We characterize the behavior of the distribution of this novel noise by showing its dependence on both the temporal and the spatial autocorrelation strengths. In particular, we show that the distribution experiences a stochastic transition from bimodality to trimodality.\n  Then, we employ the noise here defined to study phase transitions on Ginzburg-Landau model. Various phenomena"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.6020","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":"2026-05-18T03:40:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"h9HWD9lA04MpnpfQfx2NeuQGUIPzLWi9j5WtaeaRuPHqJ9kcmc4cMFtKdbwly8bgvbz7eFDmllXaCLtmmndSCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-25T13:17:35.644479Z"},"content_sha256":"9f5bf55cc20f2ee3da9a1497013f80eda0bbd713f812710967aa8593f7883d27","schema_version":"1.0","event_id":"sha256:9f5bf55cc20f2ee3da9a1497013f80eda0bbd713f812710967aa8593f7883d27"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/53MTILRXH7RZNVVUYOXZJVJLIS/bundle.json","state_url":"https://pith.science/pith/53MTILRXH7RZNVVUYOXZJVJLIS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/53MTILRXH7RZNVVUYOXZJVJLIS/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":"2026-06-25T13:17:35Z","links":{"resolver":"https://pith.science/pith/53MTILRXH7RZNVVUYOXZJVJLIS","bundle":"https://pith.science/pith/53MTILRXH7RZNVVUYOXZJVJLIS/bundle.json","state":"https://pith.science/pith/53MTILRXH7RZNVVUYOXZJVJLIS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/53MTILRXH7RZNVVUYOXZJVJLIS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:53MTILRXH7RZNVVUYOXZJVJLIS","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":"0d7d548fe4c2938116787d0a833a11816cb1f9b02424c27b102acb0d3d17b1cf","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-06-26T15:14:20Z","title_canon_sha256":"4dc8e2c79b1d78c1b3642f20ef5f67146b141186e37f79b91ce17e602dbb5269"},"schema_version":"1.0","source":{"id":"1206.6020","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1206.6020","created_at":"2026-05-18T03:40:14Z"},{"alias_kind":"arxiv_version","alias_value":"1206.6020v2","created_at":"2026-05-18T03:40:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1206.6020","created_at":"2026-05-18T03:40:14Z"},{"alias_kind":"pith_short_12","alias_value":"53MTILRXH7RZ","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"53MTILRXH7RZNVVU","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"53MTILRX","created_at":"2026-05-18T12:26:53Z"}],"graph_snapshots":[{"event_id":"sha256:9f5bf55cc20f2ee3da9a1497013f80eda0bbd713f812710967aa8593f7883d27","target":"graph","created_at":"2026-05-18T03:40:14Z","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 this work, we introduce a kind of spatiotemporal bounded noise derived by the sine-Wiener noise and by the spatially colored unbounded noise introduced by Garc\\'ia-Ojalvo, Sancho and Ram\\'irez-Piscina (GSR noise). We characterize the behavior of the distribution of this novel noise by showing its dependence on both the temporal and the spatial autocorrelation strengths. In particular, we show that the distribution experiences a stochastic transition from bimodality to trimodality.\n  Then, we employ the noise here defined to study phase transitions on Ginzburg-Landau model. Various phenomena","authors_text":"Alberto d'Onofrio, Sebastiano de Franciscis","cross_cats":["math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-06-26T15:14:20Z","title":"Spatiotemporal sine-Wiener Bounded Noise and its effect on Ginzburg-Landau model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1206.6020","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:a2eeb5c52077e4b8034497d45d995319494fd75624701fcefc5d6665181966cb","target":"record","created_at":"2026-05-18T03:40:14Z","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":"0d7d548fe4c2938116787d0a833a11816cb1f9b02424c27b102acb0d3d17b1cf","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-06-26T15:14:20Z","title_canon_sha256":"4dc8e2c79b1d78c1b3642f20ef5f67146b141186e37f79b91ce17e602dbb5269"},"schema_version":"1.0","source":{"id":"1206.6020","kind":"arxiv","version":2}},"canonical_sha256":"eed9342e373fe396d6b4c3af94d52b449cc6a806df91fed6b46fdb75a553a4a6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"eed9342e373fe396d6b4c3af94d52b449cc6a806df91fed6b46fdb75a553a4a6","first_computed_at":"2026-05-18T03:40:14.032384Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:40:14.032384Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vgt4bzdKeGRfsbsDpu2rX+0mADGe/xYhLBIThvKVT7TAmN9I1kISps45v2V0Cdp1CyF2AQ/TYhDMUWZTBimABA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:40:14.032858Z","signed_message":"canonical_sha256_bytes"},"source_id":"1206.6020","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a2eeb5c52077e4b8034497d45d995319494fd75624701fcefc5d6665181966cb","sha256:9f5bf55cc20f2ee3da9a1497013f80eda0bbd713f812710967aa8593f7883d27"],"state_sha256":"1eb0f9495c217a227db15c83de79f266153b95a6e847effe9e0d7eb9c2624090"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"B3LzG6y9rBcfyDh+oeHi/eVdIZQ/BHUbwg1zthIDl6iEOvQzGa4YmcFsANLfr9YLlODL0wqtY0w/kgZ4l2TXAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-25T13:17:35.647069Z","bundle_sha256":"50b6544852705a741cc3ed436f3d33b7994b4676397b4b1b39cc14ed04f53530"}}