{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:MSC77JFNV2MZGXKNUM5FTKFEVW","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":"26d10ec976503c879428ff0aff6e4d9a2754a04ed52a9024ef54ca0fc9e1df9b","cross_cats_sorted":["cond-mat.str-el","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2013-02-13T14:44:28Z","title_canon_sha256":"549e98e1521123ac0abd856691591d796f3e56e043491dd9f7f5d22ad79b0051"},"schema_version":"1.0","source":{"id":"1302.3125","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1302.3125","created_at":"2026-05-18T01:36:21Z"},{"alias_kind":"arxiv_version","alias_value":"1302.3125v2","created_at":"2026-05-18T01:36:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.3125","created_at":"2026-05-18T01:36:21Z"},{"alias_kind":"pith_short_12","alias_value":"MSC77JFNV2MZ","created_at":"2026-05-18T12:27:52Z"},{"alias_kind":"pith_short_16","alias_value":"MSC77JFNV2MZGXKN","created_at":"2026-05-18T12:27:52Z"},{"alias_kind":"pith_short_8","alias_value":"MSC77JFN","created_at":"2026-05-18T12:27:52Z"}],"graph_snapshots":[{"event_id":"sha256:6dd346db7b71bf608a12a4468ed089877d78cccb3e5dbf8624281db37186fb78","target":"graph","created_at":"2026-05-18T01:36:21Z","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 present a construction of non-equilibrium steady states in one-dimensional quantum critical systems carrying energy and charge fluxes. This construction is based on a scattering approach within a real-time hamiltonian reservoir formulation. Using conformal field theory techniques, we prove convergence towards steady states at large time. We discuss in which circumstances these states describe the universal non-equilibrium regime at low temperatures. We compute the exact large deviation functions for both energy and charge transfers, which encode for the quantum and statistical fluctuations ","authors_text":"Benjamin Doyon, Denis Bernard","cross_cats":["cond-mat.str-el","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2013-02-13T14:44:28Z","title":"Non-equilibrium steady-states in conformal field theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.3125","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":"sha256:220bc09fd3270b1c8d4515df457066f9da2a6a57b366d7316954fed81f6e82cb","target":"record","created_at":"2026-05-18T01:36:21Z","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":"26d10ec976503c879428ff0aff6e4d9a2754a04ed52a9024ef54ca0fc9e1df9b","cross_cats_sorted":["cond-mat.str-el","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"math-ph","submitted_at":"2013-02-13T14:44:28Z","title_canon_sha256":"549e98e1521123ac0abd856691591d796f3e56e043491dd9f7f5d22ad79b0051"},"schema_version":"1.0","source":{"id":"1302.3125","kind":"arxiv","version":2}},"canonical_sha256":"6485ffa4adae99935d4da33a59a8a4adb930cce98fc7c175037a7a37486b3ccc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6485ffa4adae99935d4da33a59a8a4adb930cce98fc7c175037a7a37486b3ccc","first_computed_at":"2026-05-18T01:36:21.161923Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:36:21.161923Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Az2hAhTbC+KezDJG3zl2fTbOIjpwChc6zaYB+OAa6HULNeDo5SHzv+fQK3og8XsRQ+DBl8D5oPCFZ5f5RhxABw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:36:21.162494Z","signed_message":"canonical_sha256_bytes"},"source_id":"1302.3125","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:220bc09fd3270b1c8d4515df457066f9da2a6a57b366d7316954fed81f6e82cb","sha256:6dd346db7b71bf608a12a4468ed089877d78cccb3e5dbf8624281db37186fb78"],"state_sha256":"dba18c8b1e7428e17e65a43e9a05c808e1bde9b473aba717247e513173340931"}