{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:A5LA55AKOQI6HBKK72C47JPDUP","short_pith_number":"pith:A5LA55AK","canonical_record":{"source":{"id":"1508.07635","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-08-30T21:02:39Z","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP"],"title_canon_sha256":"a19363cae47701a33fb39d7268ab7b46e2d08151a9c8accdcd05c7a2fa0a0aed","abstract_canon_sha256":"089fc30adcc877dea8e7e367193db61ec1d71b65edb19f351f69970bf6216db6"},"schema_version":"1.0"},"canonical_sha256":"07560ef40a7411e3854afe85cfa5e3a3f7247cb51cd656da38dcc3a5dee37028","source":{"kind":"arxiv","id":"1508.07635","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1508.07635","created_at":"2026-05-18T00:58:35Z"},{"alias_kind":"arxiv_version","alias_value":"1508.07635v2","created_at":"2026-05-18T00:58:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.07635","created_at":"2026-05-18T00:58:35Z"},{"alias_kind":"pith_short_12","alias_value":"A5LA55AKOQI6","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_16","alias_value":"A5LA55AKOQI6HBKK","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_8","alias_value":"A5LA55AK","created_at":"2026-05-18T12:29:10Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:A5LA55AKOQI6HBKK72C47JPDUP","target":"record","payload":{"canonical_record":{"source":{"id":"1508.07635","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-08-30T21:02:39Z","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP"],"title_canon_sha256":"a19363cae47701a33fb39d7268ab7b46e2d08151a9c8accdcd05c7a2fa0a0aed","abstract_canon_sha256":"089fc30adcc877dea8e7e367193db61ec1d71b65edb19f351f69970bf6216db6"},"schema_version":"1.0"},"canonical_sha256":"07560ef40a7411e3854afe85cfa5e3a3f7247cb51cd656da38dcc3a5dee37028","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:58:35.108200Z","signature_b64":"RT+ajU+stEgk8ojKVEDffdGsPLQO/g9x4a1xYpaQaF78ituSdxowSpWKXuH9f2zAkkgVt5SK+LpeUAQIThiyCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"07560ef40a7411e3854afe85cfa5e3a3f7247cb51cd656da38dcc3a5dee37028","last_reissued_at":"2026-05-18T00:58:35.107584Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:58:35.107584Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1508.07635","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":"2026-05-18T00:58:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LFdzWHgcAkB02uZNaVruLSO0BjM322Jl3wZ5X2c1zVtmZ/6fjhj8+LOSPGD5jykqqsD2iiArRstpz0TLD/z3AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T18:19:16.074492Z"},"content_sha256":"52593c6669a64e1bfee24f575fb09b17814e5d158a35a056f67698583c91f87f","schema_version":"1.0","event_id":"sha256:52593c6669a64e1bfee24f575fb09b17814e5d158a35a056f67698583c91f87f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:A5LA55AKOQI6HBKK72C47JPDUP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Statistics of the dissipated energy in driven diffusive systems","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech","math-ph","math.MP"],"primary_cat":"cond-mat.soft","authors_text":"A. Lasanta, A. Prados, Pablo I. Hurtado","submitted_at":"2015-08-30T21:02:39Z","abstract_excerpt":"Understanding the physics of non-equilibrium systems remains as one of the major open questions in statistical physics. This problem can be partially handled by investigating macroscopic fluctuations of key magnitudes that characterise the non-equilibrium behaviour of the system of interest; their statistics, associated structures and microscopic origin. During the last years, some new general and powerful methods have appeared to delve into fluctuating behaviour that have drastically changed the way to address this problem in the realm of diffusive systems: macroscopic fluctuation theory (MFT"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.07635","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":"2026-05-18T00:58:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"0VAgh0jgOU5ryuRntxCcEk45V87TvTIwMz+saRZc1o0n4baXax0tOYKrZUxogYzOZBk4f48WIrGkWEr8lnBnCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-29T18:19:16.074847Z"},"content_sha256":"cbd54604f391721d67aa62504a45e819a5ff300177916ecf92a5215b4982162e","schema_version":"1.0","event_id":"sha256:cbd54604f391721d67aa62504a45e819a5ff300177916ecf92a5215b4982162e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/A5LA55AKOQI6HBKK72C47JPDUP/bundle.json","state_url":"https://pith.science/pith/A5LA55AKOQI6HBKK72C47JPDUP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/A5LA55AKOQI6HBKK72C47JPDUP/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":"2026-05-29T18:19:16Z","links":{"resolver":"https://pith.science/pith/A5LA55AKOQI6HBKK72C47JPDUP","bundle":"https://pith.science/pith/A5LA55AKOQI6HBKK72C47JPDUP/bundle.json","state":"https://pith.science/pith/A5LA55AKOQI6HBKK72C47JPDUP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/A5LA55AKOQI6HBKK72C47JPDUP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:A5LA55AKOQI6HBKK72C47JPDUP","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":"089fc30adcc877dea8e7e367193db61ec1d71b65edb19f351f69970bf6216db6","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-08-30T21:02:39Z","title_canon_sha256":"a19363cae47701a33fb39d7268ab7b46e2d08151a9c8accdcd05c7a2fa0a0aed"},"schema_version":"1.0","source":{"id":"1508.07635","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1508.07635","created_at":"2026-05-18T00:58:35Z"},{"alias_kind":"arxiv_version","alias_value":"1508.07635v2","created_at":"2026-05-18T00:58:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.07635","created_at":"2026-05-18T00:58:35Z"},{"alias_kind":"pith_short_12","alias_value":"A5LA55AKOQI6","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_16","alias_value":"A5LA55AKOQI6HBKK","created_at":"2026-05-18T12:29:10Z"},{"alias_kind":"pith_short_8","alias_value":"A5LA55AK","created_at":"2026-05-18T12:29:10Z"}],"graph_snapshots":[{"event_id":"sha256:cbd54604f391721d67aa62504a45e819a5ff300177916ecf92a5215b4982162e","target":"graph","created_at":"2026-05-18T00:58:35Z","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":"Understanding the physics of non-equilibrium systems remains as one of the major open questions in statistical physics. This problem can be partially handled by investigating macroscopic fluctuations of key magnitudes that characterise the non-equilibrium behaviour of the system of interest; their statistics, associated structures and microscopic origin. During the last years, some new general and powerful methods have appeared to delve into fluctuating behaviour that have drastically changed the way to address this problem in the realm of diffusive systems: macroscopic fluctuation theory (MFT","authors_text":"A. Lasanta, A. Prados, Pablo I. Hurtado","cross_cats":["cond-mat.stat-mech","math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-08-30T21:02:39Z","title":"Statistics of the dissipated energy in driven diffusive systems"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.07635","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":"sha256:52593c6669a64e1bfee24f575fb09b17814e5d158a35a056f67698583c91f87f","target":"record","created_at":"2026-05-18T00:58:35Z","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":"089fc30adcc877dea8e7e367193db61ec1d71b65edb19f351f69970bf6216db6","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.soft","submitted_at":"2015-08-30T21:02:39Z","title_canon_sha256":"a19363cae47701a33fb39d7268ab7b46e2d08151a9c8accdcd05c7a2fa0a0aed"},"schema_version":"1.0","source":{"id":"1508.07635","kind":"arxiv","version":2}},"canonical_sha256":"07560ef40a7411e3854afe85cfa5e3a3f7247cb51cd656da38dcc3a5dee37028","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"07560ef40a7411e3854afe85cfa5e3a3f7247cb51cd656da38dcc3a5dee37028","first_computed_at":"2026-05-18T00:58:35.107584Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:58:35.107584Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"RT+ajU+stEgk8ojKVEDffdGsPLQO/g9x4a1xYpaQaF78ituSdxowSpWKXuH9f2zAkkgVt5SK+LpeUAQIThiyCw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:58:35.108200Z","signed_message":"canonical_sha256_bytes"},"source_id":"1508.07635","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:52593c6669a64e1bfee24f575fb09b17814e5d158a35a056f67698583c91f87f","sha256:cbd54604f391721d67aa62504a45e819a5ff300177916ecf92a5215b4982162e"],"state_sha256":"19e09f4e4a5c02fe931a94686363bb7d007d64e108f83590b1f33fe8f79304f7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GkNu/DZVfcKEkZ6AxEDjk4XUvJzpCKZvOj0I7JQe6TjV23sGEEsxTFtYOPB+IFvuDX9tNwxppI/eYdmMIMRDCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-29T18:19:16.077443Z","bundle_sha256":"8d030ca54874d7bb43455e4267b86919574c7616ac045bb00d86098b734ad6fe"}}