{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:RKODM5L6ZYBQZD7YZOXSOT3EWH","short_pith_number":"pith:RKODM5L6","canonical_record":{"source":{"id":"1801.08057","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-01-24T16:14:47Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"9cc25a3ce74cb0f1b0421db06f6c51cbde1b2bfdfe552e517508596b720c7391","abstract_canon_sha256":"a6ac12d88fb426c6c86c8c7bf3346d421a3a0415c97e6e14a652b1ee96c8c4bb"},"schema_version":"1.0"},"canonical_sha256":"8a9c36757ece030c8ff8cbaf274f64b1e0ffd92389fbc8d7c2f13a6ebce8cd13","source":{"kind":"arxiv","id":"1801.08057","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.08057","created_at":"2026-05-18T00:13:21Z"},{"alias_kind":"arxiv_version","alias_value":"1801.08057v3","created_at":"2026-05-18T00:13:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.08057","created_at":"2026-05-18T00:13:21Z"},{"alias_kind":"pith_short_12","alias_value":"RKODM5L6ZYBQ","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"RKODM5L6ZYBQZD7Y","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"RKODM5L6","created_at":"2026-05-18T12:32:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:RKODM5L6ZYBQZD7YZOXSOT3EWH","target":"record","payload":{"canonical_record":{"source":{"id":"1801.08057","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-01-24T16:14:47Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"9cc25a3ce74cb0f1b0421db06f6c51cbde1b2bfdfe552e517508596b720c7391","abstract_canon_sha256":"a6ac12d88fb426c6c86c8c7bf3346d421a3a0415c97e6e14a652b1ee96c8c4bb"},"schema_version":"1.0"},"canonical_sha256":"8a9c36757ece030c8ff8cbaf274f64b1e0ffd92389fbc8d7c2f13a6ebce8cd13","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:13:21.595269Z","signature_b64":"XI51xdeSDcZF0pO8LGAWttVO2Y3rukEaQvazetQ1sOH2fN91RMxBxtbRo7aU7BxHSaRWbGfONdpgQNHmdaRRDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8a9c36757ece030c8ff8cbaf274f64b1e0ffd92389fbc8d7c2f13a6ebce8cd13","last_reissued_at":"2026-05-18T00:13:21.594723Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:13:21.594723Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1801.08057","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:13:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Q6T9h6ROhNfqu1UL/P5L1jr9DsnqULm67ZBaSI/624jpBBSKc1btp0E23AyrNq+cSspMnBEuL+iMdPEDkJXmAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T13:38:31.133820Z"},"content_sha256":"7e4f7e1bd2f6cecf544dddb1489ec001dc38a0595c1d161473aa7e43c6705e06","schema_version":"1.0","event_id":"sha256:7e4f7e1bd2f6cecf544dddb1489ec001dc38a0595c1d161473aa7e43c6705e06"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:RKODM5L6ZYBQZD7YZOXSOT3EWH","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Energy-temperature uncertainty relation in quantum thermodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"quant-ph","authors_text":"Harry J. D. Miller, Janet Anders","submitted_at":"2018-01-24T16:14:47Z","abstract_excerpt":"It is known that temperature estimates of macroscopic systems in equilibrium are most precise when their energy fluctuations are large. However, for nanoscale systems deviations from standard thermodynamics arise due to their interactions with the environment. Here we include such interactions and, using quantum estimation theory, derive a generalised thermodynamic uncertainty relation valid for classical and quantum systems at all coupling strengths. We show that the non-commutativity between the system's state and its effective energy operator gives rise to quantum fluctuations that increase"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.08057","kind":"arxiv","version":3},"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":"2026-05-18T00:13:21Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nG99Eea13MPdeW/sP2vGkbj/KMVkVVbFRvFA8gCFAy3+TvThubU4V19RPK2aWoBpkfclg9nhpkYuTlmxVsjlBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T13:38:31.134610Z"},"content_sha256":"51b828635b0fdd2442fd6c83c39b29e86e511b871d098f95f8d21ef44017d3e2","schema_version":"1.0","event_id":"sha256:51b828635b0fdd2442fd6c83c39b29e86e511b871d098f95f8d21ef44017d3e2"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RKODM5L6ZYBQZD7YZOXSOT3EWH/bundle.json","state_url":"https://pith.science/pith/RKODM5L6ZYBQZD7YZOXSOT3EWH/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RKODM5L6ZYBQZD7YZOXSOT3EWH/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":"2026-05-31T13:38:31Z","links":{"resolver":"https://pith.science/pith/RKODM5L6ZYBQZD7YZOXSOT3EWH","bundle":"https://pith.science/pith/RKODM5L6ZYBQZD7YZOXSOT3EWH/bundle.json","state":"https://pith.science/pith/RKODM5L6ZYBQZD7YZOXSOT3EWH/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RKODM5L6ZYBQZD7YZOXSOT3EWH/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:RKODM5L6ZYBQZD7YZOXSOT3EWH","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":"a6ac12d88fb426c6c86c8c7bf3346d421a3a0415c97e6e14a652b1ee96c8c4bb","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-01-24T16:14:47Z","title_canon_sha256":"9cc25a3ce74cb0f1b0421db06f6c51cbde1b2bfdfe552e517508596b720c7391"},"schema_version":"1.0","source":{"id":"1801.08057","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1801.08057","created_at":"2026-05-18T00:13:21Z"},{"alias_kind":"arxiv_version","alias_value":"1801.08057v3","created_at":"2026-05-18T00:13:21Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1801.08057","created_at":"2026-05-18T00:13:21Z"},{"alias_kind":"pith_short_12","alias_value":"RKODM5L6ZYBQ","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_16","alias_value":"RKODM5L6ZYBQZD7Y","created_at":"2026-05-18T12:32:50Z"},{"alias_kind":"pith_short_8","alias_value":"RKODM5L6","created_at":"2026-05-18T12:32:50Z"}],"graph_snapshots":[{"event_id":"sha256:51b828635b0fdd2442fd6c83c39b29e86e511b871d098f95f8d21ef44017d3e2","target":"graph","created_at":"2026-05-18T00:13:21Z","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":"It is known that temperature estimates of macroscopic systems in equilibrium are most precise when their energy fluctuations are large. However, for nanoscale systems deviations from standard thermodynamics arise due to their interactions with the environment. Here we include such interactions and, using quantum estimation theory, derive a generalised thermodynamic uncertainty relation valid for classical and quantum systems at all coupling strengths. We show that the non-commutativity between the system's state and its effective energy operator gives rise to quantum fluctuations that increase","authors_text":"Harry J. D. Miller, Janet Anders","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-01-24T16:14:47Z","title":"Energy-temperature uncertainty relation in quantum thermodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1801.08057","kind":"arxiv","version":3},"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":"sha256:7e4f7e1bd2f6cecf544dddb1489ec001dc38a0595c1d161473aa7e43c6705e06","target":"record","created_at":"2026-05-18T00:13:21Z","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":"a6ac12d88fb426c6c86c8c7bf3346d421a3a0415c97e6e14a652b1ee96c8c4bb","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2018-01-24T16:14:47Z","title_canon_sha256":"9cc25a3ce74cb0f1b0421db06f6c51cbde1b2bfdfe552e517508596b720c7391"},"schema_version":"1.0","source":{"id":"1801.08057","kind":"arxiv","version":3}},"canonical_sha256":"8a9c36757ece030c8ff8cbaf274f64b1e0ffd92389fbc8d7c2f13a6ebce8cd13","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8a9c36757ece030c8ff8cbaf274f64b1e0ffd92389fbc8d7c2f13a6ebce8cd13","first_computed_at":"2026-05-18T00:13:21.594723Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:13:21.594723Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"XI51xdeSDcZF0pO8LGAWttVO2Y3rukEaQvazetQ1sOH2fN91RMxBxtbRo7aU7BxHSaRWbGfONdpgQNHmdaRRDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:13:21.595269Z","signed_message":"canonical_sha256_bytes"},"source_id":"1801.08057","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7e4f7e1bd2f6cecf544dddb1489ec001dc38a0595c1d161473aa7e43c6705e06","sha256:51b828635b0fdd2442fd6c83c39b29e86e511b871d098f95f8d21ef44017d3e2"],"state_sha256":"53a468029f1b2a624397389b62c197ef8d93cb02e2b54d4acff858fd446c80a2"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BpEDKjffwljxaxPJ8RtgS6R95czYJmtHm+co7hgVL03XCc/Yek+pwvBSTKYfaSMHj4U/MoA9aJQMtxWEWBalDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T13:38:31.139033Z","bundle_sha256":"af3879bd6516c5cb53b4ccf407c267259220aadefd691bdfa2b7b73eb3a70125"}}