{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:PYF7MCOY45UFWLU54MHFWXJSVU","short_pith_number":"pith:PYF7MCOY","canonical_record":{"source":{"id":"1809.11014","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.PR","submitted_at":"2018-09-28T13:27:17Z","cross_cats_sorted":[],"title_canon_sha256":"6fb2ab670e2971ef1aa66c386fd67a33337f4bbaaedbdbd7967786392dd3eb78","abstract_canon_sha256":"55fc1025b33410428c00e060c46b6c17e1f7ba71277c10a7172971a0e6c580d0"},"schema_version":"1.0"},"canonical_sha256":"7e0bf609d8e7685b2e9de30e5b5d32ad1b7ee8e12496e167b3d7456313c8269d","source":{"kind":"arxiv","id":"1809.11014","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1809.11014","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"arxiv_version","alias_value":"1809.11014v1","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.11014","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"pith_short_12","alias_value":"PYF7MCOY45UF","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_16","alias_value":"PYF7MCOY45UFWLU5","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_8","alias_value":"PYF7MCOY","created_at":"2026-05-18T12:32:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:PYF7MCOY45UFWLU54MHFWXJSVU","target":"record","payload":{"canonical_record":{"source":{"id":"1809.11014","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.PR","submitted_at":"2018-09-28T13:27:17Z","cross_cats_sorted":[],"title_canon_sha256":"6fb2ab670e2971ef1aa66c386fd67a33337f4bbaaedbdbd7967786392dd3eb78","abstract_canon_sha256":"55fc1025b33410428c00e060c46b6c17e1f7ba71277c10a7172971a0e6c580d0"},"schema_version":"1.0"},"canonical_sha256":"7e0bf609d8e7685b2e9de30e5b5d32ad1b7ee8e12496e167b3d7456313c8269d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:33.606882Z","signature_b64":"2NsNxXaX4THE4SAYnOo49acJ0git4mpAWva+TrrWcTaTz+z6YEoZlpYvUFe3QQHFM/LDv6qs3VtyCFTlBACLAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7e0bf609d8e7685b2e9de30e5b5d32ad1b7ee8e12496e167b3d7456313c8269d","last_reissued_at":"2026-05-18T00:04:33.606288Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:33.606288Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1809.11014","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":"2026-05-18T00:04:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZteXpogbAiGqxQi5VPqcb9ShHh7cvYMdxfDwb+GsJdbWOYcjSGMyleqAbmaasL1u0DyKFGWBgpsLFtqTF1AhBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T04:20:30.090679Z"},"content_sha256":"3c742d7ebe73fb9e69cccb337b499ec43414d4d3bf529a0e6055055b93a58401","schema_version":"1.0","event_id":"sha256:3c742d7ebe73fb9e69cccb337b499ec43414d4d3bf529a0e6055055b93a58401"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:PYF7MCOY45UFWLU54MHFWXJSVU","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamical Gibbs-non-Gibbs transitions in Curie-Weiss Widom-Rowlinson models","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"math.PR","authors_text":"Christof Kuelske, Sascha Kissel","submitted_at":"2018-09-28T13:27:17Z","abstract_excerpt":"We consider the Curie-Weiss Widom-Rowlinson model for particles with spins and holes, with a repulsion strength beta between particles of opposite spins. We provide a closed solution of the model, and investigate dynamical Gibbs-non-Gibbs transitions for the time-evolved model under independent stochastic symmetric spin-flip dynamics. We show that, for sufficiently large beta after a transition time, continuously many bad empirical measures appear. These lie on (unions of) curves on the simplex whose time-evolution we describe."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.11014","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":"2026-05-18T00:04:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OrmWyZ0IOvkOqEXsX4eqdW1JVTsC+D+KpDJibUTxwNbp3cT5Ev8GJ77Y33iPTV7Q9TM/EFnzselfSL8cVsUBCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T04:20:30.091026Z"},"content_sha256":"e668e61a55aaed49b13c348bbc89b81eeae5973dc6c60656ef48e55107ce7b86","schema_version":"1.0","event_id":"sha256:e668e61a55aaed49b13c348bbc89b81eeae5973dc6c60656ef48e55107ce7b86"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PYF7MCOY45UFWLU54MHFWXJSVU/bundle.json","state_url":"https://pith.science/pith/PYF7MCOY45UFWLU54MHFWXJSVU/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PYF7MCOY45UFWLU54MHFWXJSVU/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":"2026-06-02T04:20:30Z","links":{"resolver":"https://pith.science/pith/PYF7MCOY45UFWLU54MHFWXJSVU","bundle":"https://pith.science/pith/PYF7MCOY45UFWLU54MHFWXJSVU/bundle.json","state":"https://pith.science/pith/PYF7MCOY45UFWLU54MHFWXJSVU/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PYF7MCOY45UFWLU54MHFWXJSVU/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:PYF7MCOY45UFWLU54MHFWXJSVU","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":"55fc1025b33410428c00e060c46b6c17e1f7ba71277c10a7172971a0e6c580d0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.PR","submitted_at":"2018-09-28T13:27:17Z","title_canon_sha256":"6fb2ab670e2971ef1aa66c386fd67a33337f4bbaaedbdbd7967786392dd3eb78"},"schema_version":"1.0","source":{"id":"1809.11014","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1809.11014","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"arxiv_version","alias_value":"1809.11014v1","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.11014","created_at":"2026-05-18T00:04:33Z"},{"alias_kind":"pith_short_12","alias_value":"PYF7MCOY45UF","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_16","alias_value":"PYF7MCOY45UFWLU5","created_at":"2026-05-18T12:32:46Z"},{"alias_kind":"pith_short_8","alias_value":"PYF7MCOY","created_at":"2026-05-18T12:32:46Z"}],"graph_snapshots":[{"event_id":"sha256:e668e61a55aaed49b13c348bbc89b81eeae5973dc6c60656ef48e55107ce7b86","target":"graph","created_at":"2026-05-18T00:04:33Z","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":"We consider the Curie-Weiss Widom-Rowlinson model for particles with spins and holes, with a repulsion strength beta between particles of opposite spins. We provide a closed solution of the model, and investigate dynamical Gibbs-non-Gibbs transitions for the time-evolved model under independent stochastic symmetric spin-flip dynamics. We show that, for sufficiently large beta after a transition time, continuously many bad empirical measures appear. These lie on (unions of) curves on the simplex whose time-evolution we describe.","authors_text":"Christof Kuelske, Sascha Kissel","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.PR","submitted_at":"2018-09-28T13:27:17Z","title":"Dynamical Gibbs-non-Gibbs transitions in Curie-Weiss Widom-Rowlinson models"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.11014","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":"sha256:3c742d7ebe73fb9e69cccb337b499ec43414d4d3bf529a0e6055055b93a58401","target":"record","created_at":"2026-05-18T00:04:33Z","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":"55fc1025b33410428c00e060c46b6c17e1f7ba71277c10a7172971a0e6c580d0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math.PR","submitted_at":"2018-09-28T13:27:17Z","title_canon_sha256":"6fb2ab670e2971ef1aa66c386fd67a33337f4bbaaedbdbd7967786392dd3eb78"},"schema_version":"1.0","source":{"id":"1809.11014","kind":"arxiv","version":1}},"canonical_sha256":"7e0bf609d8e7685b2e9de30e5b5d32ad1b7ee8e12496e167b3d7456313c8269d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7e0bf609d8e7685b2e9de30e5b5d32ad1b7ee8e12496e167b3d7456313c8269d","first_computed_at":"2026-05-18T00:04:33.606288Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:04:33.606288Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"2NsNxXaX4THE4SAYnOo49acJ0git4mpAWva+TrrWcTaTz+z6YEoZlpYvUFe3QQHFM/LDv6qs3VtyCFTlBACLAA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:04:33.606882Z","signed_message":"canonical_sha256_bytes"},"source_id":"1809.11014","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:3c742d7ebe73fb9e69cccb337b499ec43414d4d3bf529a0e6055055b93a58401","sha256:e668e61a55aaed49b13c348bbc89b81eeae5973dc6c60656ef48e55107ce7b86"],"state_sha256":"4461db79bc7a1b71b2808b37b5e17f52bf54eb0ba88cd4da9a4db8174e6dbb0f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"b+9bTG1QGDzU4zmYvP3UVVn35C8zb9Bv96fRYiNKLHquET/RcCbbsXLAuJPFeHyqIBzpzXgn+e6YsfP8KxLBCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T04:20:30.093034Z","bundle_sha256":"b844ff8d7515834cef0851c9f28615c4fa55d6df606d8c5169452e9bbdf56e2b"}}