{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:P63SIPH7H72KCIRSFM2GUSJNZS","short_pith_number":"pith:P63SIPH7","canonical_record":{"source":{"id":"1704.01078","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-04-04T15:51:26Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"b0d70a00fc4b4360e99c38257312e8c22fe3dbde4db589a9878f0fdde23ff625","abstract_canon_sha256":"3a8eb3ad0171599f1d068530b24a8b9211f5637115685ecada4a1238ac62633c"},"schema_version":"1.0"},"canonical_sha256":"7fb7243cff3ff4a122322b346a492dccb572bbef48a4ebdcb6128b16c8295999","source":{"kind":"arxiv","id":"1704.01078","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.01078","created_at":"2026-05-18T00:31:36Z"},{"alias_kind":"arxiv_version","alias_value":"1704.01078v2","created_at":"2026-05-18T00:31:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.01078","created_at":"2026-05-18T00:31:36Z"},{"alias_kind":"pith_short_12","alias_value":"P63SIPH7H72K","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_16","alias_value":"P63SIPH7H72KCIRS","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_8","alias_value":"P63SIPH7","created_at":"2026-05-18T12:31:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:P63SIPH7H72KCIRSFM2GUSJNZS","target":"record","payload":{"canonical_record":{"source":{"id":"1704.01078","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-04-04T15:51:26Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"b0d70a00fc4b4360e99c38257312e8c22fe3dbde4db589a9878f0fdde23ff625","abstract_canon_sha256":"3a8eb3ad0171599f1d068530b24a8b9211f5637115685ecada4a1238ac62633c"},"schema_version":"1.0"},"canonical_sha256":"7fb7243cff3ff4a122322b346a492dccb572bbef48a4ebdcb6128b16c8295999","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:31:36.050568Z","signature_b64":"4hJ0gQZ2M6o4FIG4H5oMd6xlubT7+UVGtnFyAShkn5Zda3kqOOob55B7jyUfRgvHyGilMF6Ox43CzvML49ShDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7fb7243cff3ff4a122322b346a492dccb572bbef48a4ebdcb6128b16c8295999","last_reissued_at":"2026-05-18T00:31:36.049733Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:31:36.049733Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1704.01078","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":"2026-05-18T00:31:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hofSRrbp3MV87I+fzDpbaIXHUQegDvNK5ehkKBSHP+tzcTlppAuFt0ZyyBLLCObH/q+GEGTDfkkCaJA0A3BgBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T16:34:05.442030Z"},"content_sha256":"2b142d2a9c2f42e84d88edd4a531b8714c6fc5e32f873875b1092e584e18d4b4","schema_version":"1.0","event_id":"sha256:2b142d2a9c2f42e84d88edd4a531b8714c6fc5e32f873875b1092e584e18d4b4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:P63SIPH7H72KCIRSFM2GUSJNZS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Full counting statistics approach to the quantum non-equilibrium Landauer bound","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"quant-ph","authors_text":"Bassano Vacchini, Giacomo Guarnieri, John Goold, Mauro Paternostro, Simon Pigeon, Steve Campbell","submitted_at":"2017-04-04T15:51:26Z","abstract_excerpt":"We develop the full counting statistics of dissipated heat to explore the relation with Landauer's principle. Combining the two-time measurement protocol for the reconstruction of the statistics of heat with the minimal set of assumptions for Landauer's principle to hold, we derive a general one-parameter family of upper and lower bounds on the mean dissipated heat from a system to its environment. Furthermore, we establish a connection with the degree of non-unitality of the system's dynamics and show that, if a large deviation function exists as stationary limit of the above cumulant generat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.01078","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":"2026-05-18T00:31:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WA6WpuW6nh1pZZEtEpLgzVEWPILI/iSzl955lGgX8tfnEt/oJpVm9zfGp4fPmDpzXO8Rg3FP825azm5D9p71Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T16:34:05.442389Z"},"content_sha256":"32bb0bf453699d7717fb02746d150994dff8144cbf0cfbfa93467ad3e84a8217","schema_version":"1.0","event_id":"sha256:32bb0bf453699d7717fb02746d150994dff8144cbf0cfbfa93467ad3e84a8217"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/P63SIPH7H72KCIRSFM2GUSJNZS/bundle.json","state_url":"https://pith.science/pith/P63SIPH7H72KCIRSFM2GUSJNZS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/P63SIPH7H72KCIRSFM2GUSJNZS/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":"2026-06-03T16:34:05Z","links":{"resolver":"https://pith.science/pith/P63SIPH7H72KCIRSFM2GUSJNZS","bundle":"https://pith.science/pith/P63SIPH7H72KCIRSFM2GUSJNZS/bundle.json","state":"https://pith.science/pith/P63SIPH7H72KCIRSFM2GUSJNZS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/P63SIPH7H72KCIRSFM2GUSJNZS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:P63SIPH7H72KCIRSFM2GUSJNZS","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":"3a8eb3ad0171599f1d068530b24a8b9211f5637115685ecada4a1238ac62633c","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-04-04T15:51:26Z","title_canon_sha256":"b0d70a00fc4b4360e99c38257312e8c22fe3dbde4db589a9878f0fdde23ff625"},"schema_version":"1.0","source":{"id":"1704.01078","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1704.01078","created_at":"2026-05-18T00:31:36Z"},{"alias_kind":"arxiv_version","alias_value":"1704.01078v2","created_at":"2026-05-18T00:31:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.01078","created_at":"2026-05-18T00:31:36Z"},{"alias_kind":"pith_short_12","alias_value":"P63SIPH7H72K","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_16","alias_value":"P63SIPH7H72KCIRS","created_at":"2026-05-18T12:31:37Z"},{"alias_kind":"pith_short_8","alias_value":"P63SIPH7","created_at":"2026-05-18T12:31:37Z"}],"graph_snapshots":[{"event_id":"sha256:32bb0bf453699d7717fb02746d150994dff8144cbf0cfbfa93467ad3e84a8217","target":"graph","created_at":"2026-05-18T00:31:36Z","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 develop the full counting statistics of dissipated heat to explore the relation with Landauer's principle. Combining the two-time measurement protocol for the reconstruction of the statistics of heat with the minimal set of assumptions for Landauer's principle to hold, we derive a general one-parameter family of upper and lower bounds on the mean dissipated heat from a system to its environment. Furthermore, we establish a connection with the degree of non-unitality of the system's dynamics and show that, if a large deviation function exists as stationary limit of the above cumulant generat","authors_text":"Bassano Vacchini, Giacomo Guarnieri, John Goold, Mauro Paternostro, Simon Pigeon, Steve Campbell","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-04-04T15:51:26Z","title":"Full counting statistics approach to the quantum non-equilibrium Landauer bound"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.01078","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":"sha256:2b142d2a9c2f42e84d88edd4a531b8714c6fc5e32f873875b1092e584e18d4b4","target":"record","created_at":"2026-05-18T00:31:36Z","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":"3a8eb3ad0171599f1d068530b24a8b9211f5637115685ecada4a1238ac62633c","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-04-04T15:51:26Z","title_canon_sha256":"b0d70a00fc4b4360e99c38257312e8c22fe3dbde4db589a9878f0fdde23ff625"},"schema_version":"1.0","source":{"id":"1704.01078","kind":"arxiv","version":2}},"canonical_sha256":"7fb7243cff3ff4a122322b346a492dccb572bbef48a4ebdcb6128b16c8295999","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7fb7243cff3ff4a122322b346a492dccb572bbef48a4ebdcb6128b16c8295999","first_computed_at":"2026-05-18T00:31:36.049733Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:31:36.049733Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"4hJ0gQZ2M6o4FIG4H5oMd6xlubT7+UVGtnFyAShkn5Zda3kqOOob55B7jyUfRgvHyGilMF6Ox43CzvML49ShDA==","signature_status":"signed_v1","signed_at":"2026-05-18T00:31:36.050568Z","signed_message":"canonical_sha256_bytes"},"source_id":"1704.01078","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:2b142d2a9c2f42e84d88edd4a531b8714c6fc5e32f873875b1092e584e18d4b4","sha256:32bb0bf453699d7717fb02746d150994dff8144cbf0cfbfa93467ad3e84a8217"],"state_sha256":"e5a265676b10be61d00dda2ae4204f6a1f92896a73ecd5211fba04c1e3f2c05e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DpdwT/O85rmM1Wra2h43kan013d0ZFOY30BaePg5jpEidRGPdF9FtkZ4pZDFs76nfw2sxuNRZsIedf/nxZ8zCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T16:34:05.444414Z","bundle_sha256":"dce72751ee416f40abeaaedf48f908a35a68649951b56af5c6bb87fc98578b2f"}}