{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:RVT2FL7SOYXYK4KJL4GSNGYRA2","short_pith_number":"pith:RVT2FL7S","canonical_record":{"source":{"id":"1610.01418","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-10-05T13:50:09Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"10b816fc64c5a029d0b8841122c6dcc28eeed22a0fab750e11cccf178a7e4e4a","abstract_canon_sha256":"cdc04b5ff192a2dcd3af68e3d5317d5d827c7fb56edd2f12f365bf43e07cc794"},"schema_version":"1.0"},"canonical_sha256":"8d67a2aff2762f8571495f0d269b11069a64936f895749adce19ed06afb47f3f","source":{"kind":"arxiv","id":"1610.01418","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.01418","created_at":"2026-05-18T00:45:54Z"},{"alias_kind":"arxiv_version","alias_value":"1610.01418v3","created_at":"2026-05-18T00:45:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.01418","created_at":"2026-05-18T00:45:54Z"},{"alias_kind":"pith_short_12","alias_value":"RVT2FL7SOYXY","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_16","alias_value":"RVT2FL7SOYXYK4KJ","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_8","alias_value":"RVT2FL7S","created_at":"2026-05-18T12:30:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:RVT2FL7SOYXYK4KJL4GSNGYRA2","target":"record","payload":{"canonical_record":{"source":{"id":"1610.01418","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-10-05T13:50:09Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"10b816fc64c5a029d0b8841122c6dcc28eeed22a0fab750e11cccf178a7e4e4a","abstract_canon_sha256":"cdc04b5ff192a2dcd3af68e3d5317d5d827c7fb56edd2f12f365bf43e07cc794"},"schema_version":"1.0"},"canonical_sha256":"8d67a2aff2762f8571495f0d269b11069a64936f895749adce19ed06afb47f3f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:45:54.183104Z","signature_b64":"a7AkbCyIM986Krc7NHZJq4sjTW0hbNuSl5expwRorzrBkbR/JyciqN/gP+hREVIiwjdJhU41rb9YfB9BDCgZBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8d67a2aff2762f8571495f0d269b11069a64936f895749adce19ed06afb47f3f","last_reissued_at":"2026-05-18T00:45:54.182501Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:45:54.182501Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1610.01418","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":"2026-05-18T00:45:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QMNjVRTeXEtsKDH4HK+gKLPVa3qLbI3ATWQzHH0VhgX1l5sK4ZiqaRDxjYFVZcK49beNETYKohRx2MEV2fsTBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T17:51:05.678407Z"},"content_sha256":"dee4918f2ede5357b5a37734e9ca05da3a9191090d3672d8beee2236613d480c","schema_version":"1.0","event_id":"sha256:dee4918f2ede5357b5a37734e9ca05da3a9191090d3672d8beee2236613d480c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:RVT2FL7SOYXYK4KJL4GSNGYRA2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"A statics-dynamics equivalence through the fluctuation-dissipation ratio provides a window into the spin-glass phase from nonequilibrium measurements","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"A. Cruz, A. Gordillo-Guerrero, A. Maiorano, A. Mu\\~noz-Sudupe, A. Tarancon, B. Seoane, D. I\\~niguez, D. Navarro, D. Yllanes, E. Calore, E. Marinari, F. Ricci-Tersenghi, G. Parisi, Janus Collaboration: M. Baity-Jesi, J.J. Ruiz-Lorenzo, J.M. Gil-Narvion, J. Monforte-Garcia, L.A. Fernandez, R. Tripiccione, S.F. Schifano, S. Perez-Gaviro, V. Martin-Mayor","submitted_at":"2016-10-05T13:50:09Z","abstract_excerpt":"The unifying feature of glass formers (such as polymers, supercooled liquids, colloids, granulars, spin glasses, superconductors, ...) is a sluggish dynamics at low temperatures. Indeed, their dynamics is so slow that thermal equilibrium is never reached in macroscopic samples: in analogy with living beings, glasses are said to age. Here, we show how to relate experimentally relevant quantities with the experimentally unreachable low-temperature equilibrium phase. We have performed a very accurate computation of the non-equilibrium fluctuation-dissipation ratio for the three-dimensional Edward"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.01418","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":"2026-05-18T00:45:54Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"DIHN0HMgrI+e3owpGf2Q/BjBMGkE5EPS8qgB0JAdSWgszGti5ezq0cLSukrvoOxwzZwXxDFB1rnWnz5I8ABaBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T17:51:05.678755Z"},"content_sha256":"67328bf923026f8ceb3125739f28d18c0aef627ceb8421f675a0b211b19a725f","schema_version":"1.0","event_id":"sha256:67328bf923026f8ceb3125739f28d18c0aef627ceb8421f675a0b211b19a725f"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RVT2FL7SOYXYK4KJL4GSNGYRA2/bundle.json","state_url":"https://pith.science/pith/RVT2FL7SOYXYK4KJL4GSNGYRA2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RVT2FL7SOYXYK4KJL4GSNGYRA2/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":"2026-06-01T17:51:05Z","links":{"resolver":"https://pith.science/pith/RVT2FL7SOYXYK4KJL4GSNGYRA2","bundle":"https://pith.science/pith/RVT2FL7SOYXYK4KJL4GSNGYRA2/bundle.json","state":"https://pith.science/pith/RVT2FL7SOYXYK4KJL4GSNGYRA2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RVT2FL7SOYXYK4KJL4GSNGYRA2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:RVT2FL7SOYXYK4KJL4GSNGYRA2","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":"cdc04b5ff192a2dcd3af68e3d5317d5d827c7fb56edd2f12f365bf43e07cc794","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-10-05T13:50:09Z","title_canon_sha256":"10b816fc64c5a029d0b8841122c6dcc28eeed22a0fab750e11cccf178a7e4e4a"},"schema_version":"1.0","source":{"id":"1610.01418","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1610.01418","created_at":"2026-05-18T00:45:54Z"},{"alias_kind":"arxiv_version","alias_value":"1610.01418v3","created_at":"2026-05-18T00:45:54Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1610.01418","created_at":"2026-05-18T00:45:54Z"},{"alias_kind":"pith_short_12","alias_value":"RVT2FL7SOYXY","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_16","alias_value":"RVT2FL7SOYXYK4KJ","created_at":"2026-05-18T12:30:41Z"},{"alias_kind":"pith_short_8","alias_value":"RVT2FL7S","created_at":"2026-05-18T12:30:41Z"}],"graph_snapshots":[{"event_id":"sha256:67328bf923026f8ceb3125739f28d18c0aef627ceb8421f675a0b211b19a725f","target":"graph","created_at":"2026-05-18T00:45:54Z","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":"The unifying feature of glass formers (such as polymers, supercooled liquids, colloids, granulars, spin glasses, superconductors, ...) is a sluggish dynamics at low temperatures. Indeed, their dynamics is so slow that thermal equilibrium is never reached in macroscopic samples: in analogy with living beings, glasses are said to age. Here, we show how to relate experimentally relevant quantities with the experimentally unreachable low-temperature equilibrium phase. We have performed a very accurate computation of the non-equilibrium fluctuation-dissipation ratio for the three-dimensional Edward","authors_text":"A. Cruz, A. Gordillo-Guerrero, A. Maiorano, A. Mu\\~noz-Sudupe, A. Tarancon, B. Seoane, D. I\\~niguez, D. Navarro, D. Yllanes, E. Calore, E. Marinari, F. Ricci-Tersenghi, G. Parisi, Janus Collaboration: M. Baity-Jesi, J.J. Ruiz-Lorenzo, J.M. Gil-Narvion, J. Monforte-Garcia, L.A. Fernandez, R. Tripiccione, S.F. Schifano, S. Perez-Gaviro, V. Martin-Mayor","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-10-05T13:50:09Z","title":"A statics-dynamics equivalence through the fluctuation-dissipation ratio provides a window into the spin-glass phase from nonequilibrium measurements"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1610.01418","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:dee4918f2ede5357b5a37734e9ca05da3a9191090d3672d8beee2236613d480c","target":"record","created_at":"2026-05-18T00:45:54Z","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":"cdc04b5ff192a2dcd3af68e3d5317d5d827c7fb56edd2f12f365bf43e07cc794","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2016-10-05T13:50:09Z","title_canon_sha256":"10b816fc64c5a029d0b8841122c6dcc28eeed22a0fab750e11cccf178a7e4e4a"},"schema_version":"1.0","source":{"id":"1610.01418","kind":"arxiv","version":3}},"canonical_sha256":"8d67a2aff2762f8571495f0d269b11069a64936f895749adce19ed06afb47f3f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8d67a2aff2762f8571495f0d269b11069a64936f895749adce19ed06afb47f3f","first_computed_at":"2026-05-18T00:45:54.182501Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:45:54.182501Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"a7AkbCyIM986Krc7NHZJq4sjTW0hbNuSl5expwRorzrBkbR/JyciqN/gP+hREVIiwjdJhU41rb9YfB9BDCgZBg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:45:54.183104Z","signed_message":"canonical_sha256_bytes"},"source_id":"1610.01418","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:dee4918f2ede5357b5a37734e9ca05da3a9191090d3672d8beee2236613d480c","sha256:67328bf923026f8ceb3125739f28d18c0aef627ceb8421f675a0b211b19a725f"],"state_sha256":"6418ddb67a56d898ad9bebc67ecffb6e811eccd32554a7521c3016f9e7b3b236"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VzIztqHhRGjgHIbfTy8MNVxY0q9QIJdX8Wf5WE96V18vEdjGr0yQqugOf1Ua6l16tDQ4I3y1WiSVAhVqLX/nAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T17:51:05.680894Z","bundle_sha256":"aa3e8aa474561f12658aedc8c598c92e4cab4cf371d400dcfa374c8cc0fe86fd"}}