{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:R4OFXG7P6D473XLH4PJSBZPBDC","short_pith_number":"pith:R4OFXG7P","canonical_record":{"source":{"id":"1503.04310","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-03-14T14:49:55Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"7db68ea13fb8199f7549a3a8a9fd902840b889c25294de5b9034273c30ff5f23","abstract_canon_sha256":"d81bb34a7fae076266581779d08a9fe6408fd9aa935dc99eb8721c76a4d4e463"},"schema_version":"1.0"},"canonical_sha256":"8f1c5b9beff0f9fddd67e3d320e5e118bcd3254366d9c8e7286abd4c8b645c8e","source":{"kind":"arxiv","id":"1503.04310","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1503.04310","created_at":"2026-05-18T01:36:31Z"},{"alias_kind":"arxiv_version","alias_value":"1503.04310v4","created_at":"2026-05-18T01:36:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.04310","created_at":"2026-05-18T01:36:31Z"},{"alias_kind":"pith_short_12","alias_value":"R4OFXG7P6D47","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_16","alias_value":"R4OFXG7P6D473XLH","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_8","alias_value":"R4OFXG7P","created_at":"2026-05-18T12:29:39Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:R4OFXG7P6D473XLH4PJSBZPBDC","target":"record","payload":{"canonical_record":{"source":{"id":"1503.04310","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-03-14T14:49:55Z","cross_cats_sorted":["cond-mat.mes-hall"],"title_canon_sha256":"7db68ea13fb8199f7549a3a8a9fd902840b889c25294de5b9034273c30ff5f23","abstract_canon_sha256":"d81bb34a7fae076266581779d08a9fe6408fd9aa935dc99eb8721c76a4d4e463"},"schema_version":"1.0"},"canonical_sha256":"8f1c5b9beff0f9fddd67e3d320e5e118bcd3254366d9c8e7286abd4c8b645c8e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:36:31.109539Z","signature_b64":"8lDYZpRMRY1CYf9Xb+f3TDHXauxX3mFf4EVb9cUFpkx/3l4LkG4qq+i5LAhp7ohqgBNMhZfDciGw01SGBPJTAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8f1c5b9beff0f9fddd67e3d320e5e118bcd3254366d9c8e7286abd4c8b645c8e","last_reissued_at":"2026-05-18T01:36:31.109029Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:36:31.109029Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1503.04310","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:36:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"HCUI9fnkrWOs3YvjPDqSWYVAdK2Xek/PtNAKKOqOFcOhURevZhbY9OcPFrnwOIUL8eN6/O4r5GX2NpvJJukDAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:23:30.405387Z"},"content_sha256":"001b10093194162eaf31ff07c0be6e62bb421023d9602a60dc2cad60e3f1fd09","schema_version":"1.0","event_id":"sha256:001b10093194162eaf31ff07c0be6e62bb421023d9602a60dc2cad60e3f1fd09"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:R4OFXG7P6D473XLH4PJSBZPBDC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Efficiency Statistics and Bounds for Systems with Broken Time-Reversal Symmetry","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["cond-mat.mes-hall"],"primary_cat":"cond-mat.stat-mech","authors_text":"Bijay Kumar Agarwalla, Dvira Segal, Jian-Hua Jiang","submitted_at":"2015-03-14T14:49:55Z","abstract_excerpt":"Universal properties of the statistics of stochastic efficiency for mesoscopic time-reversal symmetry broken energy transducers are revealed in the Gaussian approximation. We also discuss how the second law of thermodynamics restricts the statistics of stochastic efficiency. The tight-coupling (reversible) limit becomes unfavorable, characterized by an infinitely broad distribution of efficiency at {\\em all times}, when time-reversal symmetry breaking leads to an asymmetric Onsager response matrix. The underlying physics is demonstrated through the integer quantum Hall effect and further elabo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.04310","kind":"arxiv","version":4},"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":"2026-05-18T01:36:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1sCSAMtC8rVhMDgmH8KmrsvSq+tVT4ReoszJk2AQBm6B0BHmg0I1VvsieUBqQM1cEhj33q+E6Tp5oKc6l2EKAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T18:23:30.406104Z"},"content_sha256":"f2c174c7a2aa68dc592b1c84040915feba28885b6be836800125331be63c4993","schema_version":"1.0","event_id":"sha256:f2c174c7a2aa68dc592b1c84040915feba28885b6be836800125331be63c4993"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/R4OFXG7P6D473XLH4PJSBZPBDC/bundle.json","state_url":"https://pith.science/pith/R4OFXG7P6D473XLH4PJSBZPBDC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/R4OFXG7P6D473XLH4PJSBZPBDC/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":"2026-05-25T18:23:30Z","links":{"resolver":"https://pith.science/pith/R4OFXG7P6D473XLH4PJSBZPBDC","bundle":"https://pith.science/pith/R4OFXG7P6D473XLH4PJSBZPBDC/bundle.json","state":"https://pith.science/pith/R4OFXG7P6D473XLH4PJSBZPBDC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/R4OFXG7P6D473XLH4PJSBZPBDC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:R4OFXG7P6D473XLH4PJSBZPBDC","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":"d81bb34a7fae076266581779d08a9fe6408fd9aa935dc99eb8721c76a4d4e463","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-03-14T14:49:55Z","title_canon_sha256":"7db68ea13fb8199f7549a3a8a9fd902840b889c25294de5b9034273c30ff5f23"},"schema_version":"1.0","source":{"id":"1503.04310","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1503.04310","created_at":"2026-05-18T01:36:31Z"},{"alias_kind":"arxiv_version","alias_value":"1503.04310v4","created_at":"2026-05-18T01:36:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1503.04310","created_at":"2026-05-18T01:36:31Z"},{"alias_kind":"pith_short_12","alias_value":"R4OFXG7P6D47","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_16","alias_value":"R4OFXG7P6D473XLH","created_at":"2026-05-18T12:29:39Z"},{"alias_kind":"pith_short_8","alias_value":"R4OFXG7P","created_at":"2026-05-18T12:29:39Z"}],"graph_snapshots":[{"event_id":"sha256:f2c174c7a2aa68dc592b1c84040915feba28885b6be836800125331be63c4993","target":"graph","created_at":"2026-05-18T01:36:31Z","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":"Universal properties of the statistics of stochastic efficiency for mesoscopic time-reversal symmetry broken energy transducers are revealed in the Gaussian approximation. We also discuss how the second law of thermodynamics restricts the statistics of stochastic efficiency. The tight-coupling (reversible) limit becomes unfavorable, characterized by an infinitely broad distribution of efficiency at {\\em all times}, when time-reversal symmetry breaking leads to an asymmetric Onsager response matrix. The underlying physics is demonstrated through the integer quantum Hall effect and further elabo","authors_text":"Bijay Kumar Agarwalla, Dvira Segal, Jian-Hua Jiang","cross_cats":["cond-mat.mes-hall"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-03-14T14:49:55Z","title":"Efficiency Statistics and Bounds for Systems with Broken Time-Reversal Symmetry"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1503.04310","kind":"arxiv","version":4},"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":"sha256:001b10093194162eaf31ff07c0be6e62bb421023d9602a60dc2cad60e3f1fd09","target":"record","created_at":"2026-05-18T01:36:31Z","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":"d81bb34a7fae076266581779d08a9fe6408fd9aa935dc99eb8721c76a4d4e463","cross_cats_sorted":["cond-mat.mes-hall"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2015-03-14T14:49:55Z","title_canon_sha256":"7db68ea13fb8199f7549a3a8a9fd902840b889c25294de5b9034273c30ff5f23"},"schema_version":"1.0","source":{"id":"1503.04310","kind":"arxiv","version":4}},"canonical_sha256":"8f1c5b9beff0f9fddd67e3d320e5e118bcd3254366d9c8e7286abd4c8b645c8e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8f1c5b9beff0f9fddd67e3d320e5e118bcd3254366d9c8e7286abd4c8b645c8e","first_computed_at":"2026-05-18T01:36:31.109029Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:36:31.109029Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"8lDYZpRMRY1CYf9Xb+f3TDHXauxX3mFf4EVb9cUFpkx/3l4LkG4qq+i5LAhp7ohqgBNMhZfDciGw01SGBPJTAg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:36:31.109539Z","signed_message":"canonical_sha256_bytes"},"source_id":"1503.04310","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:001b10093194162eaf31ff07c0be6e62bb421023d9602a60dc2cad60e3f1fd09","sha256:f2c174c7a2aa68dc592b1c84040915feba28885b6be836800125331be63c4993"],"state_sha256":"e3c8183a447dbdded5da7afa6d3fb826f36439eac4c24df72c22cece68039ffb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wDj9d685aac/dOQSNmSpPxhhSKA9SHUbfOzzpjKQE80K7nzT7Ada2zt4T0EFEZ4VRdp5ZkY3xNpOEW3jC6NEAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T18:23:30.410024Z","bundle_sha256":"7f3acac2959b2a2b6c0ec289a5669a8ead1ad944abe5a6e3fcd5384acfa3ff60"}}