{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:XLPYALCO75LLVHGX3A36JXI3HM","short_pith_number":"pith:XLPYALCO","canonical_record":{"source":{"id":"1510.05254","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-10-18T14:59:03Z","cross_cats_sorted":[],"title_canon_sha256":"3164c4fd22e1460d611f0663c353d96ed2b2b26710b2d471f9bde8b2fb18937d","abstract_canon_sha256":"fa9ea4fc0f75d6c909f26c9f200ee769b07b1d0d8b43ad1e85f73c5572b8fc75"},"schema_version":"1.0"},"canonical_sha256":"badf802c4eff56ba9cd7d837e4dd1b3b28c4619216d3db4edeb85f65f0af0290","source":{"kind":"arxiv","id":"1510.05254","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1510.05254","created_at":"2026-05-18T01:12:07Z"},{"alias_kind":"arxiv_version","alias_value":"1510.05254v1","created_at":"2026-05-18T01:12:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.05254","created_at":"2026-05-18T01:12:07Z"},{"alias_kind":"pith_short_12","alias_value":"XLPYALCO75LL","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_16","alias_value":"XLPYALCO75LLVHGX","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_8","alias_value":"XLPYALCO","created_at":"2026-05-18T12:29:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:XLPYALCO75LLVHGX3A36JXI3HM","target":"record","payload":{"canonical_record":{"source":{"id":"1510.05254","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-10-18T14:59:03Z","cross_cats_sorted":[],"title_canon_sha256":"3164c4fd22e1460d611f0663c353d96ed2b2b26710b2d471f9bde8b2fb18937d","abstract_canon_sha256":"fa9ea4fc0f75d6c909f26c9f200ee769b07b1d0d8b43ad1e85f73c5572b8fc75"},"schema_version":"1.0"},"canonical_sha256":"badf802c4eff56ba9cd7d837e4dd1b3b28c4619216d3db4edeb85f65f0af0290","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:12:07.746063Z","signature_b64":"7pkYQWjfygwz4+h5hGS4DygQSg4oLem8A+2zEvu8ZEm+Z0mVnSL5Uyw1GhOZYKLdk63PJqXndl4Xh86KxaOJCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"badf802c4eff56ba9cd7d837e4dd1b3b28c4619216d3db4edeb85f65f0af0290","last_reissued_at":"2026-05-18T01:12:07.745617Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:12:07.745617Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1510.05254","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":"2026-05-18T01:12:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"T18tvP97Sj2ErMjAKu/mjVs6YgaGEG84Nob8QdVcafJ/e/LKjLbNoEsRXShaUKpseg40TLHyu7TvXUVBWKkpBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-03T01:09:09.167254Z"},"content_sha256":"66cf2ffea60bfc4d914b5a36a87c614b75420b8064692ba9c5f0df7f9d2fc590","schema_version":"1.0","event_id":"sha256:66cf2ffea60bfc4d914b5a36a87c614b75420b8064692ba9c5f0df7f9d2fc590"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:XLPYALCO75LLVHGX3A36JXI3HM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Le Chatelier principle for out of equilibrium and boundary driven systems : application to dynamical phase transitions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Eric Akkermans, Ohad Shpielberg","submitted_at":"2015-10-18T14:59:03Z","abstract_excerpt":"A stability analysis of out of equilibrium and boundary driven systems is presented. It is performed in the framework of the hydrodynamic macroscopic fluctuation theory and assuming the additivity principle whose interpretation is discussed with the help of a Hamiltonian description. An extension of Le Chatelier principle for out of equilibrium situations is presented which allows to formulate the conditions of validity of the additivity principle. Examples of application of these results in the realm of classical and quantum systems are provided."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.05254","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":"2026-05-18T01:12:07Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XxLqk+jVfo8PNXR8HJFG7RfwKfGK+hUeaOPwBxiu70He1722Pg53+aN3OhQvIKdgbcVqQingf68oLRDytTP9Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-03T01:09:09.167634Z"},"content_sha256":"5105f2a88613682ec9c1dceafd26154a3739f2a964a4a1fe8e37cf7bff1e209b","schema_version":"1.0","event_id":"sha256:5105f2a88613682ec9c1dceafd26154a3739f2a964a4a1fe8e37cf7bff1e209b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/XLPYALCO75LLVHGX3A36JXI3HM/bundle.json","state_url":"https://pith.science/pith/XLPYALCO75LLVHGX3A36JXI3HM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/XLPYALCO75LLVHGX3A36JXI3HM/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":"2026-07-03T01:09:09Z","links":{"resolver":"https://pith.science/pith/XLPYALCO75LLVHGX3A36JXI3HM","bundle":"https://pith.science/pith/XLPYALCO75LLVHGX3A36JXI3HM/bundle.json","state":"https://pith.science/pith/XLPYALCO75LLVHGX3A36JXI3HM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/XLPYALCO75LLVHGX3A36JXI3HM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:XLPYALCO75LLVHGX3A36JXI3HM","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":"fa9ea4fc0f75d6c909f26c9f200ee769b07b1d0d8b43ad1e85f73c5572b8fc75","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-10-18T14:59:03Z","title_canon_sha256":"3164c4fd22e1460d611f0663c353d96ed2b2b26710b2d471f9bde8b2fb18937d"},"schema_version":"1.0","source":{"id":"1510.05254","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1510.05254","created_at":"2026-05-18T01:12:07Z"},{"alias_kind":"arxiv_version","alias_value":"1510.05254v1","created_at":"2026-05-18T01:12:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1510.05254","created_at":"2026-05-18T01:12:07Z"},{"alias_kind":"pith_short_12","alias_value":"XLPYALCO75LL","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_16","alias_value":"XLPYALCO75LLVHGX","created_at":"2026-05-18T12:29:50Z"},{"alias_kind":"pith_short_8","alias_value":"XLPYALCO","created_at":"2026-05-18T12:29:50Z"}],"graph_snapshots":[{"event_id":"sha256:5105f2a88613682ec9c1dceafd26154a3739f2a964a4a1fe8e37cf7bff1e209b","target":"graph","created_at":"2026-05-18T01:12:07Z","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":"A stability analysis of out of equilibrium and boundary driven systems is presented. It is performed in the framework of the hydrodynamic macroscopic fluctuation theory and assuming the additivity principle whose interpretation is discussed with the help of a Hamiltonian description. An extension of Le Chatelier principle for out of equilibrium situations is presented which allows to formulate the conditions of validity of the additivity principle. Examples of application of these results in the realm of classical and quantum systems are provided.","authors_text":"Eric Akkermans, Ohad Shpielberg","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-10-18T14:59:03Z","title":"Le Chatelier principle for out of equilibrium and boundary driven systems : application to dynamical phase transitions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1510.05254","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":"sha256:66cf2ffea60bfc4d914b5a36a87c614b75420b8064692ba9c5f0df7f9d2fc590","target":"record","created_at":"2026-05-18T01:12:07Z","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":"fa9ea4fc0f75d6c909f26c9f200ee769b07b1d0d8b43ad1e85f73c5572b8fc75","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-10-18T14:59:03Z","title_canon_sha256":"3164c4fd22e1460d611f0663c353d96ed2b2b26710b2d471f9bde8b2fb18937d"},"schema_version":"1.0","source":{"id":"1510.05254","kind":"arxiv","version":1}},"canonical_sha256":"badf802c4eff56ba9cd7d837e4dd1b3b28c4619216d3db4edeb85f65f0af0290","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"badf802c4eff56ba9cd7d837e4dd1b3b28c4619216d3db4edeb85f65f0af0290","first_computed_at":"2026-05-18T01:12:07.745617Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:12:07.745617Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"7pkYQWjfygwz4+h5hGS4DygQSg4oLem8A+2zEvu8ZEm+Z0mVnSL5Uyw1GhOZYKLdk63PJqXndl4Xh86KxaOJCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:12:07.746063Z","signed_message":"canonical_sha256_bytes"},"source_id":"1510.05254","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:66cf2ffea60bfc4d914b5a36a87c614b75420b8064692ba9c5f0df7f9d2fc590","sha256:5105f2a88613682ec9c1dceafd26154a3739f2a964a4a1fe8e37cf7bff1e209b"],"state_sha256":"70b3941bee5278da1cd18319594dd16fb6750944daf78f33cebe3914304e689d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pAHn+YQuvvneCWjkO2NRqWzuVb9E8qcs9urtUlZUXNFQA4R0Ii+EFWw71GZ0ZgSyaqhct6E8GAxgMgpkk9HYDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-03T01:09:09.169914Z","bundle_sha256":"f05b58df460e31baaae5a15eed56ced7530d284de6e104364338409921b57cfb"}}