{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:U27LOQSMZT4WPACSG6W3RSXWMS","short_pith_number":"pith:U27LOQSM","canonical_record":{"source":{"id":"1201.0097","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.AO","submitted_at":"2011-12-30T10:12:26Z","cross_cats_sorted":[],"title_canon_sha256":"159e20e269ac072545fad584e88bf0dc1630839596e5041859bc32d0ac89d4de","abstract_canon_sha256":"125f6c269e10a0b0d2da812f29331e4dcd231105f111dca63e74bcd51b063e40"},"schema_version":"1.0"},"canonical_sha256":"a6beb7424cccf967805237adb8caf664a74f8f0559d3da391754bee0273c7074","source":{"kind":"arxiv","id":"1201.0097","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.0097","created_at":"2026-05-18T04:05:26Z"},{"alias_kind":"arxiv_version","alias_value":"1201.0097v1","created_at":"2026-05-18T04:05:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.0097","created_at":"2026-05-18T04:05:26Z"},{"alias_kind":"pith_short_12","alias_value":"U27LOQSMZT4W","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"U27LOQSMZT4WPACS","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"U27LOQSM","created_at":"2026-05-18T12:26:42Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:U27LOQSMZT4WPACSG6W3RSXWMS","target":"record","payload":{"canonical_record":{"source":{"id":"1201.0097","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.AO","submitted_at":"2011-12-30T10:12:26Z","cross_cats_sorted":[],"title_canon_sha256":"159e20e269ac072545fad584e88bf0dc1630839596e5041859bc32d0ac89d4de","abstract_canon_sha256":"125f6c269e10a0b0d2da812f29331e4dcd231105f111dca63e74bcd51b063e40"},"schema_version":"1.0"},"canonical_sha256":"a6beb7424cccf967805237adb8caf664a74f8f0559d3da391754bee0273c7074","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:05:26.214421Z","signature_b64":"YIHYY9AaOndVQKV5+yqlZCf5RnWtJVv+LPBU7AQcHHX2/O6QWZqHXDpjGrIgZf/lrmoCfcXozPvUWOOkaQG6CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a6beb7424cccf967805237adb8caf664a74f8f0559d3da391754bee0273c7074","last_reissued_at":"2026-05-18T04:05:26.213751Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:05:26.213751Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1201.0097","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":"2026-05-18T04:05:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Hh8Ws2X0b3EhgYq5PEBrQY21kq+7WFS0gx7yRByQjLflzVE6Qxbkct++Q4XaSNvpWjP8svtVCkunQO6A4m5ABA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T13:33:37.383695Z"},"content_sha256":"680730176a339c2f8091526f03f51b99ff019981cafdf3a3575d067afbc256b2","schema_version":"1.0","event_id":"sha256:680730176a339c2f8091526f03f51b99ff019981cafdf3a3575d067afbc256b2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:U27LOQSMZT4WPACSG6W3RSXWMS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Critical non-equilibrium steady states of the Lorentz channel","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nlin.AO","authors_text":"Alexandros K. Karlis, Christoph Petri, Fotios K. Diakonos, Peter Schmelcher","submitted_at":"2011-12-30T10:12:26Z","abstract_excerpt":"We investigate the transport properties of non-interacting particles propagating in a finite Lorentz channel (LC). We show that interparticle power-law correlations emerge, when the dynamics is described at a spatially coarse-grained level. This behaviour appears in the non-equilibrium steady state of the LC under flux boundary conditions and persists even in the presence of external driving, provided that the billiard's horizon is infinite in a static or temporal sense. We show that Fermi acceleration permits the synchronization of particle motion with the periodic appearance of the ballistic"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.0097","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":"2026-05-18T04:05:26Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Oeg/n9BDe5eBSr+H0RBbCOBa3kQyI54ZPOLsxxoOgJCBNUd9KJWPM5Bfe45YisBLT4j4u3m7gYZ7JpBSGT3UAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T13:33:37.384024Z"},"content_sha256":"d913cbe9e2c097e840569bcf844e21fc9bb85df3b88a4d46339a7b4562eef953","schema_version":"1.0","event_id":"sha256:d913cbe9e2c097e840569bcf844e21fc9bb85df3b88a4d46339a7b4562eef953"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/U27LOQSMZT4WPACSG6W3RSXWMS/bundle.json","state_url":"https://pith.science/pith/U27LOQSMZT4WPACSG6W3RSXWMS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/U27LOQSMZT4WPACSG6W3RSXWMS/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":"2026-06-02T13:33:37Z","links":{"resolver":"https://pith.science/pith/U27LOQSMZT4WPACSG6W3RSXWMS","bundle":"https://pith.science/pith/U27LOQSMZT4WPACSG6W3RSXWMS/bundle.json","state":"https://pith.science/pith/U27LOQSMZT4WPACSG6W3RSXWMS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/U27LOQSMZT4WPACSG6W3RSXWMS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:U27LOQSMZT4WPACSG6W3RSXWMS","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":"125f6c269e10a0b0d2da812f29331e4dcd231105f111dca63e74bcd51b063e40","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.AO","submitted_at":"2011-12-30T10:12:26Z","title_canon_sha256":"159e20e269ac072545fad584e88bf0dc1630839596e5041859bc32d0ac89d4de"},"schema_version":"1.0","source":{"id":"1201.0097","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1201.0097","created_at":"2026-05-18T04:05:26Z"},{"alias_kind":"arxiv_version","alias_value":"1201.0097v1","created_at":"2026-05-18T04:05:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.0097","created_at":"2026-05-18T04:05:26Z"},{"alias_kind":"pith_short_12","alias_value":"U27LOQSMZT4W","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_16","alias_value":"U27LOQSMZT4WPACS","created_at":"2026-05-18T12:26:42Z"},{"alias_kind":"pith_short_8","alias_value":"U27LOQSM","created_at":"2026-05-18T12:26:42Z"}],"graph_snapshots":[{"event_id":"sha256:d913cbe9e2c097e840569bcf844e21fc9bb85df3b88a4d46339a7b4562eef953","target":"graph","created_at":"2026-05-18T04:05:26Z","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 investigate the transport properties of non-interacting particles propagating in a finite Lorentz channel (LC). We show that interparticle power-law correlations emerge, when the dynamics is described at a spatially coarse-grained level. This behaviour appears in the non-equilibrium steady state of the LC under flux boundary conditions and persists even in the presence of external driving, provided that the billiard's horizon is infinite in a static or temporal sense. We show that Fermi acceleration permits the synchronization of particle motion with the periodic appearance of the ballistic","authors_text":"Alexandros K. Karlis, Christoph Petri, Fotios K. Diakonos, Peter Schmelcher","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.AO","submitted_at":"2011-12-30T10:12:26Z","title":"Critical non-equilibrium steady states of the Lorentz channel"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.0097","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":"sha256:680730176a339c2f8091526f03f51b99ff019981cafdf3a3575d067afbc256b2","target":"record","created_at":"2026-05-18T04:05:26Z","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":"125f6c269e10a0b0d2da812f29331e4dcd231105f111dca63e74bcd51b063e40","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nlin.AO","submitted_at":"2011-12-30T10:12:26Z","title_canon_sha256":"159e20e269ac072545fad584e88bf0dc1630839596e5041859bc32d0ac89d4de"},"schema_version":"1.0","source":{"id":"1201.0097","kind":"arxiv","version":1}},"canonical_sha256":"a6beb7424cccf967805237adb8caf664a74f8f0559d3da391754bee0273c7074","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a6beb7424cccf967805237adb8caf664a74f8f0559d3da391754bee0273c7074","first_computed_at":"2026-05-18T04:05:26.213751Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:05:26.213751Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"YIHYY9AaOndVQKV5+yqlZCf5RnWtJVv+LPBU7AQcHHX2/O6QWZqHXDpjGrIgZf/lrmoCfcXozPvUWOOkaQG6CQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:05:26.214421Z","signed_message":"canonical_sha256_bytes"},"source_id":"1201.0097","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:680730176a339c2f8091526f03f51b99ff019981cafdf3a3575d067afbc256b2","sha256:d913cbe9e2c097e840569bcf844e21fc9bb85df3b88a4d46339a7b4562eef953"],"state_sha256":"5caffaa011a5df5f3292be0fbf99c9ecf8637eb088d1c6ce4d84089d493ad9d8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rwjzhiq3cCBQ86yCMSTAsc83fn22bZGH8hZjW3mX1qIiiUPLuh7hIFxKd7vCMpnIyeIp1fHJiwsrGcuLLLBGDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T13:33:37.385859Z","bundle_sha256":"41ae19c313c8e8abfdf7db69b5baee46f7845642c4e96c4930b8a93efa6665c4"}}