{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:COJK5OYNWSA6Y3J4DVDAVSOHE5","short_pith_number":"pith:COJK5OYN","canonical_record":{"source":{"id":"1807.10235","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-07-26T16:39:37Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"d7e021a5c88393d13cd35ce6480af9317095df82debdc489de4c29652622ddd9","abstract_canon_sha256":"bab8fbd0192afad5d0874056cfeeae983cc4915b8819a1b00aef1dc04fadfc8d"},"schema_version":"1.0"},"canonical_sha256":"1392aebb0db481ec6d3c1d460ac9c72750a7f2f24113701fb94981b78e9dfbe8","source":{"kind":"arxiv","id":"1807.10235","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.10235","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"arxiv_version","alias_value":"1807.10235v2","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.10235","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"pith_short_12","alias_value":"COJK5OYNWSA6","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_16","alias_value":"COJK5OYNWSA6Y3J4","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_8","alias_value":"COJK5OYN","created_at":"2026-05-18T12:32:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:COJK5OYNWSA6Y3J4DVDAVSOHE5","target":"record","payload":{"canonical_record":{"source":{"id":"1807.10235","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-07-26T16:39:37Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"d7e021a5c88393d13cd35ce6480af9317095df82debdc489de4c29652622ddd9","abstract_canon_sha256":"bab8fbd0192afad5d0874056cfeeae983cc4915b8819a1b00aef1dc04fadfc8d"},"schema_version":"1.0"},"canonical_sha256":"1392aebb0db481ec6d3c1d460ac9c72750a7f2f24113701fb94981b78e9dfbe8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:58:04.339748Z","signature_b64":"hdwDCDIcS+weNXD3anuwvcLATHDnXEnpaUFSCwxMtM3/AubvUnwr8csLvKewTfhL/PW7TU5Bgrra8CveUlqkBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1392aebb0db481ec6d3c1d460ac9c72750a7f2f24113701fb94981b78e9dfbe8","last_reissued_at":"2026-05-17T23:58:04.339223Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:58:04.339223Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1807.10235","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":"2026-05-17T23:58:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"71DNsx18roL+7jenDdP5Kk0zQk+gL9tzz1XhObvqM3yzZP3fBmuS5fbiBSpQW89ksZ1pkiaJVo9ZN3Ri2GXuBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T15:09:24.410633Z"},"content_sha256":"b174c40b322e9914a038bb0416585ccc73f6ffbbe1c85735eac1f5c44cb630b0","schema_version":"1.0","event_id":"sha256:b174c40b322e9914a038bb0416585ccc73f6ffbbe1c85735eac1f5c44cb630b0"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:COJK5OYNWSA6Y3J4DVDAVSOHE5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Dynamical criticality in open systems: non-perturbative physics, microscopic origin and direct observation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"cond-mat.stat-mech","authors_text":"Carlos P\\'erez-Espigares, Federico Carollo, Juan P. Garrahan, Pablo I. Hurtado","submitted_at":"2018-07-26T16:39:37Z","abstract_excerpt":"Driven diffusive systems may undergo phase transitions to sustain atypical values of the current. This leads in some cases to symmetry-broken space-time trajectories which enhance the probability of such fluctuations. Here we shed light on both the macroscopic large deviation properties and the microscopic origin of such spontaneous symmetry breaking in the open weakly asymmetric exclusion process. By studying the joint fluctuations of the current and a collective order parameter, we uncover the full dynamical phase diagram for arbitrary boundary driving, which is reminiscent of a $\\mathbb{Z}_"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.10235","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":"2026-05-17T23:58:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7IpjSxeat1khXQyrZXQH4yNgKtVhG3S+pu9Z4DwQJ5LgH/n1tP3wKrNLWS6PHabugFboZcHtDey3gf0ieDvACQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T15:09:24.410992Z"},"content_sha256":"33f2851abc4b5a8658d025f4d8444af15b5aa3cebd6b4c39bda4da69a3c34975","schema_version":"1.0","event_id":"sha256:33f2851abc4b5a8658d025f4d8444af15b5aa3cebd6b4c39bda4da69a3c34975"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/COJK5OYNWSA6Y3J4DVDAVSOHE5/bundle.json","state_url":"https://pith.science/pith/COJK5OYNWSA6Y3J4DVDAVSOHE5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/COJK5OYNWSA6Y3J4DVDAVSOHE5/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":"2026-05-30T15:09:24Z","links":{"resolver":"https://pith.science/pith/COJK5OYNWSA6Y3J4DVDAVSOHE5","bundle":"https://pith.science/pith/COJK5OYNWSA6Y3J4DVDAVSOHE5/bundle.json","state":"https://pith.science/pith/COJK5OYNWSA6Y3J4DVDAVSOHE5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/COJK5OYNWSA6Y3J4DVDAVSOHE5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:COJK5OYNWSA6Y3J4DVDAVSOHE5","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":"bab8fbd0192afad5d0874056cfeeae983cc4915b8819a1b00aef1dc04fadfc8d","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-07-26T16:39:37Z","title_canon_sha256":"d7e021a5c88393d13cd35ce6480af9317095df82debdc489de4c29652622ddd9"},"schema_version":"1.0","source":{"id":"1807.10235","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1807.10235","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"arxiv_version","alias_value":"1807.10235v2","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.10235","created_at":"2026-05-17T23:58:04Z"},{"alias_kind":"pith_short_12","alias_value":"COJK5OYNWSA6","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_16","alias_value":"COJK5OYNWSA6Y3J4","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_8","alias_value":"COJK5OYN","created_at":"2026-05-18T12:32:16Z"}],"graph_snapshots":[{"event_id":"sha256:33f2851abc4b5a8658d025f4d8444af15b5aa3cebd6b4c39bda4da69a3c34975","target":"graph","created_at":"2026-05-17T23:58:04Z","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":"Driven diffusive systems may undergo phase transitions to sustain atypical values of the current. This leads in some cases to symmetry-broken space-time trajectories which enhance the probability of such fluctuations. Here we shed light on both the macroscopic large deviation properties and the microscopic origin of such spontaneous symmetry breaking in the open weakly asymmetric exclusion process. By studying the joint fluctuations of the current and a collective order parameter, we uncover the full dynamical phase diagram for arbitrary boundary driving, which is reminiscent of a $\\mathbb{Z}_","authors_text":"Carlos P\\'erez-Espigares, Federico Carollo, Juan P. Garrahan, Pablo I. Hurtado","cross_cats":["math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-07-26T16:39:37Z","title":"Dynamical criticality in open systems: non-perturbative physics, microscopic origin and direct observation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.10235","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:b174c40b322e9914a038bb0416585ccc73f6ffbbe1c85735eac1f5c44cb630b0","target":"record","created_at":"2026-05-17T23:58:04Z","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":"bab8fbd0192afad5d0874056cfeeae983cc4915b8819a1b00aef1dc04fadfc8d","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2018-07-26T16:39:37Z","title_canon_sha256":"d7e021a5c88393d13cd35ce6480af9317095df82debdc489de4c29652622ddd9"},"schema_version":"1.0","source":{"id":"1807.10235","kind":"arxiv","version":2}},"canonical_sha256":"1392aebb0db481ec6d3c1d460ac9c72750a7f2f24113701fb94981b78e9dfbe8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1392aebb0db481ec6d3c1d460ac9c72750a7f2f24113701fb94981b78e9dfbe8","first_computed_at":"2026-05-17T23:58:04.339223Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:58:04.339223Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hdwDCDIcS+weNXD3anuwvcLATHDnXEnpaUFSCwxMtM3/AubvUnwr8csLvKewTfhL/PW7TU5Bgrra8CveUlqkBQ==","signature_status":"signed_v1","signed_at":"2026-05-17T23:58:04.339748Z","signed_message":"canonical_sha256_bytes"},"source_id":"1807.10235","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b174c40b322e9914a038bb0416585ccc73f6ffbbe1c85735eac1f5c44cb630b0","sha256:33f2851abc4b5a8658d025f4d8444af15b5aa3cebd6b4c39bda4da69a3c34975"],"state_sha256":"fc5bd4ee4d3cf45fc1032a736b7b8f4c3dc4d4589e36bd75895d9f08166d0d0f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"b94PJHoARnMPedYxiVXcFnXArhggkpgplREdOK5Df/TQUcm7KQDQ+kg2xD+hV7onwUXMG87x+PlsS440pUi6AQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T15:09:24.413324Z","bundle_sha256":"2557e65b28712bfc01fddfd50feceaf91f433f36e082d96f0435aba2bdf150ba"}}