{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:5T5WP4NXUZHIXZ4GULVK3HC6CD","short_pith_number":"pith:5T5WP4NX","canonical_record":{"source":{"id":"1712.00795","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-12-03T16:42:04Z","cross_cats_sorted":["cond-mat.mes-hall","physics.bio-ph"],"title_canon_sha256":"366c0606dba3ada5694b9a03de70a988bfa38626dff223d4fc850949133e2beb","abstract_canon_sha256":"072f3d2fd97e824d7528facf0d33464c3a25bac309d6441d96d1ada9eae7090a"},"schema_version":"1.0"},"canonical_sha256":"ecfb67f1b7a64e8be786a2eaad9c5e10c89a7b9a772421fc7a9decca236a9c9e","source":{"kind":"arxiv","id":"1712.00795","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1712.00795","created_at":"2026-05-18T00:06:05Z"},{"alias_kind":"arxiv_version","alias_value":"1712.00795v2","created_at":"2026-05-18T00:06:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.00795","created_at":"2026-05-18T00:06:05Z"},{"alias_kind":"pith_short_12","alias_value":"5T5WP4NXUZHI","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_16","alias_value":"5T5WP4NXUZHIXZ4G","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_8","alias_value":"5T5WP4NX","created_at":"2026-05-18T12:31:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:5T5WP4NXUZHIXZ4GULVK3HC6CD","target":"record","payload":{"canonical_record":{"source":{"id":"1712.00795","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-12-03T16:42:04Z","cross_cats_sorted":["cond-mat.mes-hall","physics.bio-ph"],"title_canon_sha256":"366c0606dba3ada5694b9a03de70a988bfa38626dff223d4fc850949133e2beb","abstract_canon_sha256":"072f3d2fd97e824d7528facf0d33464c3a25bac309d6441d96d1ada9eae7090a"},"schema_version":"1.0"},"canonical_sha256":"ecfb67f1b7a64e8be786a2eaad9c5e10c89a7b9a772421fc7a9decca236a9c9e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:06:05.558626Z","signature_b64":"arc8FCzGgzoo85ZBKZAuhRH5W+AqrPV+jVFXEB0Ad47zoEMrIQNDPoD+loGp5uhdq/DBkIHhpGiFGWbLiN1KCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ecfb67f1b7a64e8be786a2eaad9c5e10c89a7b9a772421fc7a9decca236a9c9e","last_reissued_at":"2026-05-18T00:06:05.557951Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:06:05.557951Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1712.00795","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":"2026-05-18T00:06:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WoA7pxTLvuPuCb3+tbgiwQLF1eFqqES30tm3kLL1bOgAwfgzD38nbYoZIXDlSTejd3WfjXHdmghWwL5HYxEQAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T09:59:38.212810Z"},"content_sha256":"c3cc0617928746846b7ac5a65810f2e138cdd4491621462cc4e0583f56c29a37","schema_version":"1.0","event_id":"sha256:c3cc0617928746846b7ac5a65810f2e138cdd4491621462cc4e0583f56c29a37"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:5T5WP4NXUZHIXZ4GULVK3HC6CD","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Arcsine Laws in Stochastic Thermodynamics","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.mes-hall","physics.bio-ph"],"primary_cat":"cond-mat.stat-mech","authors_text":"Andre C. Barato, \\'Edgar Rold\\'an, Ignacio A. Mart\\'inez, Simone Pigolotti","submitted_at":"2017-12-03T16:42:04Z","abstract_excerpt":"We show that the fraction of time a thermodynamic current spends above its average value follows the arcsine law, a prominent result obtained by L\\'evy for Brownian motion. Stochastic currents with long streaks above or below their average are much more likely than those that spend similar fractions of time above and below their average. Our result is confirmed with experimental data from a Brownian Carnot engine. We also conjecture that two other random times associated with currents obey the arcsine law: the time a current reaches its maximum value and the last time a current crosses its ave"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.00795","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":"2026-05-18T00:06:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ud9U7/ddBlxIISCPMpLbGHiO5TRyCqg56PMahXT4qx63tA6XAzwQkILge0fwL8ZfT7hNMBGPIbriXfF2AXxEDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T09:59:38.213530Z"},"content_sha256":"d7dcf4a725cd6a194dab16b0fe172d303f564962bd57cd313625d94886ef6389","schema_version":"1.0","event_id":"sha256:d7dcf4a725cd6a194dab16b0fe172d303f564962bd57cd313625d94886ef6389"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5T5WP4NXUZHIXZ4GULVK3HC6CD/bundle.json","state_url":"https://pith.science/pith/5T5WP4NXUZHIXZ4GULVK3HC6CD/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5T5WP4NXUZHIXZ4GULVK3HC6CD/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":"2026-05-31T09:59:38Z","links":{"resolver":"https://pith.science/pith/5T5WP4NXUZHIXZ4GULVK3HC6CD","bundle":"https://pith.science/pith/5T5WP4NXUZHIXZ4GULVK3HC6CD/bundle.json","state":"https://pith.science/pith/5T5WP4NXUZHIXZ4GULVK3HC6CD/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5T5WP4NXUZHIXZ4GULVK3HC6CD/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:5T5WP4NXUZHIXZ4GULVK3HC6CD","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":"072f3d2fd97e824d7528facf0d33464c3a25bac309d6441d96d1ada9eae7090a","cross_cats_sorted":["cond-mat.mes-hall","physics.bio-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-12-03T16:42:04Z","title_canon_sha256":"366c0606dba3ada5694b9a03de70a988bfa38626dff223d4fc850949133e2beb"},"schema_version":"1.0","source":{"id":"1712.00795","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1712.00795","created_at":"2026-05-18T00:06:05Z"},{"alias_kind":"arxiv_version","alias_value":"1712.00795v2","created_at":"2026-05-18T00:06:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1712.00795","created_at":"2026-05-18T00:06:05Z"},{"alias_kind":"pith_short_12","alias_value":"5T5WP4NXUZHI","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_16","alias_value":"5T5WP4NXUZHIXZ4G","created_at":"2026-05-18T12:31:00Z"},{"alias_kind":"pith_short_8","alias_value":"5T5WP4NX","created_at":"2026-05-18T12:31:00Z"}],"graph_snapshots":[{"event_id":"sha256:d7dcf4a725cd6a194dab16b0fe172d303f564962bd57cd313625d94886ef6389","target":"graph","created_at":"2026-05-18T00:06:05Z","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 show that the fraction of time a thermodynamic current spends above its average value follows the arcsine law, a prominent result obtained by L\\'evy for Brownian motion. Stochastic currents with long streaks above or below their average are much more likely than those that spend similar fractions of time above and below their average. Our result is confirmed with experimental data from a Brownian Carnot engine. We also conjecture that two other random times associated with currents obey the arcsine law: the time a current reaches its maximum value and the last time a current crosses its ave","authors_text":"Andre C. Barato, \\'Edgar Rold\\'an, Ignacio A. Mart\\'inez, Simone Pigolotti","cross_cats":["cond-mat.mes-hall","physics.bio-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-12-03T16:42:04Z","title":"Arcsine Laws in Stochastic Thermodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1712.00795","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:c3cc0617928746846b7ac5a65810f2e138cdd4491621462cc4e0583f56c29a37","target":"record","created_at":"2026-05-18T00:06:05Z","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":"072f3d2fd97e824d7528facf0d33464c3a25bac309d6441d96d1ada9eae7090a","cross_cats_sorted":["cond-mat.mes-hall","physics.bio-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2017-12-03T16:42:04Z","title_canon_sha256":"366c0606dba3ada5694b9a03de70a988bfa38626dff223d4fc850949133e2beb"},"schema_version":"1.0","source":{"id":"1712.00795","kind":"arxiv","version":2}},"canonical_sha256":"ecfb67f1b7a64e8be786a2eaad9c5e10c89a7b9a772421fc7a9decca236a9c9e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ecfb67f1b7a64e8be786a2eaad9c5e10c89a7b9a772421fc7a9decca236a9c9e","first_computed_at":"2026-05-18T00:06:05.557951Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:06:05.557951Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"arc8FCzGgzoo85ZBKZAuhRH5W+AqrPV+jVFXEB0Ad47zoEMrIQNDPoD+loGp5uhdq/DBkIHhpGiFGWbLiN1KCg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:06:05.558626Z","signed_message":"canonical_sha256_bytes"},"source_id":"1712.00795","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c3cc0617928746846b7ac5a65810f2e138cdd4491621462cc4e0583f56c29a37","sha256:d7dcf4a725cd6a194dab16b0fe172d303f564962bd57cd313625d94886ef6389"],"state_sha256":"bc1915e861f1a7b989983e501e38ed7fcfbce4bfbdf0d414a233a7a8150bcb88"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"dcT9ky8Vp2X/oqys0HQuwqxsoQqHBSrQZhpeB/Zm2aVcumA+EdYQnY3/8+rF+k1u81Qizo5Ia+dYkvag8z1hBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T09:59:38.218542Z","bundle_sha256":"540e0ad9cc9e9f9d9055bf4dc602321bd1b2c7ff26e11de402f06f184edb6109"}}