{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:GFJKKKX2E7LMFWSKU2F7KI2GW2","short_pith_number":"pith:GFJKKKX2","canonical_record":{"source":{"id":"1102.2049","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-02-10T07:40:37Z","cross_cats_sorted":[],"title_canon_sha256":"1f5fec2e8c3f9bf6ebf08786d109876645ec83bd7bd4ec1a5d8a7318cf1d524e","abstract_canon_sha256":"ab86f15108ece537bf04ff9626ba2e057d9269dcf8919047593a7d1d774992a3"},"schema_version":"1.0"},"canonical_sha256":"3152a52afa27d6c2da4aa68bf52346b688de3775158b9370ccc40a24335913ea","source":{"kind":"arxiv","id":"1102.2049","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1102.2049","created_at":"2026-05-18T02:03:12Z"},{"alias_kind":"arxiv_version","alias_value":"1102.2049v1","created_at":"2026-05-18T02:03:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1102.2049","created_at":"2026-05-18T02:03:12Z"},{"alias_kind":"pith_short_12","alias_value":"GFJKKKX2E7LM","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_16","alias_value":"GFJKKKX2E7LMFWSK","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_8","alias_value":"GFJKKKX2","created_at":"2026-05-18T12:26:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:GFJKKKX2E7LMFWSKU2F7KI2GW2","target":"record","payload":{"canonical_record":{"source":{"id":"1102.2049","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-02-10T07:40:37Z","cross_cats_sorted":[],"title_canon_sha256":"1f5fec2e8c3f9bf6ebf08786d109876645ec83bd7bd4ec1a5d8a7318cf1d524e","abstract_canon_sha256":"ab86f15108ece537bf04ff9626ba2e057d9269dcf8919047593a7d1d774992a3"},"schema_version":"1.0"},"canonical_sha256":"3152a52afa27d6c2da4aa68bf52346b688de3775158b9370ccc40a24335913ea","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:03:12.804468Z","signature_b64":"0QX6R+2aXY6IXyjsBFf+k+1jofj+pL7e5hOUObegMuXMB7kB0xHCags5f9rtfQljbNk9zU18b9lstT5xOfagAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3152a52afa27d6c2da4aa68bf52346b688de3775158b9370ccc40a24335913ea","last_reissued_at":"2026-05-18T02:03:12.803715Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:03:12.803715Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1102.2049","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:03:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xRW15vsH0vaS0lHXQLkgHXQR86gSYyPUYE5e1dtk2pxJX/FzCRYDT3S/DIf1UpuD76eJpfb4eNIIVIal1XZ6DQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T11:07:17.644674Z"},"content_sha256":"bc936f282fbb8f95e41c56320cecf2f5ef13053611852131c0e0cb8407280da1","schema_version":"1.0","event_id":"sha256:bc936f282fbb8f95e41c56320cecf2f5ef13053611852131c0e0cb8407280da1"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:GFJKKKX2E7LMFWSKU2F7KI2GW2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Finite sampling effects on generalized fluctuation-dissipation relations for steady states","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Artem Petrosyan (Phys-ENS), Juan Ruben Gomez-Solano (Phys-ENS), Sergio Ciliberto (Phys-ENS)","submitted_at":"2011-02-10T07:40:37Z","abstract_excerpt":"We study the effects of the finite number of experimental data on the computation of a generalized fluctuation-dissipation relation around a nonequilibrium steady state of a Brownian particle in a toroidal optical trap. We show that the finite sampling has two different effects, which can give rise to a poor estimate of the linear response function. The first concerns the accessibility of the generalized fluctuation-dissipation relation due to the finite number of actual perturbations imposed to the control parameter. The second concerns the propagation of the error made at the initial samplin"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1102.2049","kind":"arxiv","version":1},"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":"2026-05-18T02:03:12Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UHrXFh7XEa21b7nwO8txu2zoADfaasgJ7oQXhNWaOtPxqyt/ACKYXmGOyshMtSfy2uTHdKgCVlwGKzAXBIQBCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T11:07:17.645426Z"},"content_sha256":"a4e634dfc33fd75a3f8cba57dde1d6f34c1bab1005b1dd6dbcb7d4529902a2eb","schema_version":"1.0","event_id":"sha256:a4e634dfc33fd75a3f8cba57dde1d6f34c1bab1005b1dd6dbcb7d4529902a2eb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/GFJKKKX2E7LMFWSKU2F7KI2GW2/bundle.json","state_url":"https://pith.science/pith/GFJKKKX2E7LMFWSKU2F7KI2GW2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/GFJKKKX2E7LMFWSKU2F7KI2GW2/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":"2026-06-06T11:07:17Z","links":{"resolver":"https://pith.science/pith/GFJKKKX2E7LMFWSKU2F7KI2GW2","bundle":"https://pith.science/pith/GFJKKKX2E7LMFWSKU2F7KI2GW2/bundle.json","state":"https://pith.science/pith/GFJKKKX2E7LMFWSKU2F7KI2GW2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/GFJKKKX2E7LMFWSKU2F7KI2GW2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:GFJKKKX2E7LMFWSKU2F7KI2GW2","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":"ab86f15108ece537bf04ff9626ba2e057d9269dcf8919047593a7d1d774992a3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-02-10T07:40:37Z","title_canon_sha256":"1f5fec2e8c3f9bf6ebf08786d109876645ec83bd7bd4ec1a5d8a7318cf1d524e"},"schema_version":"1.0","source":{"id":"1102.2049","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1102.2049","created_at":"2026-05-18T02:03:12Z"},{"alias_kind":"arxiv_version","alias_value":"1102.2049v1","created_at":"2026-05-18T02:03:12Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1102.2049","created_at":"2026-05-18T02:03:12Z"},{"alias_kind":"pith_short_12","alias_value":"GFJKKKX2E7LM","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_16","alias_value":"GFJKKKX2E7LMFWSK","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_8","alias_value":"GFJKKKX2","created_at":"2026-05-18T12:26:28Z"}],"graph_snapshots":[{"event_id":"sha256:a4e634dfc33fd75a3f8cba57dde1d6f34c1bab1005b1dd6dbcb7d4529902a2eb","target":"graph","created_at":"2026-05-18T02:03:12Z","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 study the effects of the finite number of experimental data on the computation of a generalized fluctuation-dissipation relation around a nonequilibrium steady state of a Brownian particle in a toroidal optical trap. We show that the finite sampling has two different effects, which can give rise to a poor estimate of the linear response function. The first concerns the accessibility of the generalized fluctuation-dissipation relation due to the finite number of actual perturbations imposed to the control parameter. The second concerns the propagation of the error made at the initial samplin","authors_text":"Artem Petrosyan (Phys-ENS), Juan Ruben Gomez-Solano (Phys-ENS), Sergio Ciliberto (Phys-ENS)","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-02-10T07:40:37Z","title":"Finite sampling effects on generalized fluctuation-dissipation relations for steady states"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1102.2049","kind":"arxiv","version":1},"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:bc936f282fbb8f95e41c56320cecf2f5ef13053611852131c0e0cb8407280da1","target":"record","created_at":"2026-05-18T02:03:12Z","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":"ab86f15108ece537bf04ff9626ba2e057d9269dcf8919047593a7d1d774992a3","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-02-10T07:40:37Z","title_canon_sha256":"1f5fec2e8c3f9bf6ebf08786d109876645ec83bd7bd4ec1a5d8a7318cf1d524e"},"schema_version":"1.0","source":{"id":"1102.2049","kind":"arxiv","version":1}},"canonical_sha256":"3152a52afa27d6c2da4aa68bf52346b688de3775158b9370ccc40a24335913ea","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3152a52afa27d6c2da4aa68bf52346b688de3775158b9370ccc40a24335913ea","first_computed_at":"2026-05-18T02:03:12.803715Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:03:12.803715Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"0QX6R+2aXY6IXyjsBFf+k+1jofj+pL7e5hOUObegMuXMB7kB0xHCags5f9rtfQljbNk9zU18b9lstT5xOfagAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:03:12.804468Z","signed_message":"canonical_sha256_bytes"},"source_id":"1102.2049","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bc936f282fbb8f95e41c56320cecf2f5ef13053611852131c0e0cb8407280da1","sha256:a4e634dfc33fd75a3f8cba57dde1d6f34c1bab1005b1dd6dbcb7d4529902a2eb"],"state_sha256":"8affd7230d4c24e9c0104aa882f13ed238f78e78a8bfdc90ec1008d2b2c82a2f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cwt7ddEbB3omhJZ9v9BxHX11kdetKzPPjKJAwUQkhXpBPpa+e5zwYFEIQmltRG3+8+Jd1VcZ8LmTi5IzfqdEBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T11:07:17.649595Z","bundle_sha256":"f89b3039a43049b72b6568fd10bd84e34f052c9eda0f20dff6946d38fd6cefca"}}