{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:WPMBCDEG2HAHFILW7TSLWFMFCJ","short_pith_number":"pith:WPMBCDEG","schema_version":"1.0","canonical_sha256":"b3d8110c86d1c072a176fce4bb1585125242e698e57ae561b9831d80518b5fcb","source":{"kind":"arxiv","id":"cond-mat/9910232","version":2},"attestation_state":"computed","paper":{"title":"Off-Equilibrium Dynamics at Very Low Temperatures in 3d Spin Glasses","license":"","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"E. Marinari, F. Ricci-Tersenghi, G. Parisi, J. J. Ruiz-Lorenzo","submitted_at":"1999-10-15T11:23:20Z","abstract_excerpt":"We present a high statistic systematic study of the overlap correlation function well below the critical temperature in the three dimensional Gaussian spin glass. The off-equilibrium correlation function has been studied confirming the power law behavior for the dynamical correlation length. In particular we have computed the dynamical critical exponent $z$ in a wide range of temperatures, $0.35 \\le T \\le 0.9$, obtaining a dependence $z(T)=6.2/T$ in a very good agreement with recent experiments. Moreover, we report a study of the violation of the fluctuation-dissipation theorem for very low te"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"cond-mat/9910232","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"cond-mat.dis-nn","submitted_at":"1999-10-15T11:23:20Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"62dc2f9e7fc227439090414d94fb49a6c8f9613a913a30cbfeb4b131c840893b","abstract_canon_sha256":"ec03a377a72e00c59d4a5aa8515d0da3eca60d72af40b8a6700eb345abec7cf2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:13:23.815730Z","signature_b64":"30lq0ipBso7Ea0AXB3Ex29xfXNeIGdBr6Y+7DtdFui8FEH0GlpPfBRMEf2yc9hrAzxAuthM/lBfl/zVqR8QjDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b3d8110c86d1c072a176fce4bb1585125242e698e57ae561b9831d80518b5fcb","last_reissued_at":"2026-07-04T16:13:23.815308Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:13:23.815308Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Off-Equilibrium Dynamics at Very Low Temperatures in 3d Spin Glasses","license":"","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"E. Marinari, F. Ricci-Tersenghi, G. Parisi, J. J. Ruiz-Lorenzo","submitted_at":"1999-10-15T11:23:20Z","abstract_excerpt":"We present a high statistic systematic study of the overlap correlation function well below the critical temperature in the three dimensional Gaussian spin glass. The off-equilibrium correlation function has been studied confirming the power law behavior for the dynamical correlation length. In particular we have computed the dynamical critical exponent $z$ in a wide range of temperatures, $0.35 \\le T \\le 0.9$, obtaining a dependence $z(T)=6.2/T$ in a very good agreement with recent experiments. Moreover, we report a study of the violation of the fluctuation-dissipation theorem for very low te"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9910232","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/cond-mat/9910232/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9910232","created_at":"2026-07-04T16:13:23.815380+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9910232v2","created_at":"2026-07-04T16:13:23.815380+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9910232","created_at":"2026-07-04T16:13:23.815380+00:00"},{"alias_kind":"pith_short_12","alias_value":"WPMBCDEG2HAH","created_at":"2026-07-04T16:13:23.815380+00:00"},{"alias_kind":"pith_short_16","alias_value":"WPMBCDEG2HAHFILW","created_at":"2026-07-04T16:13:23.815380+00:00"},{"alias_kind":"pith_short_8","alias_value":"WPMBCDEG","created_at":"2026-07-04T16:13:23.815380+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WPMBCDEG2HAHFILW7TSLWFMFCJ","json":"https://pith.science/pith/WPMBCDEG2HAHFILW7TSLWFMFCJ.json","graph_json":"https://pith.science/api/pith-number/WPMBCDEG2HAHFILW7TSLWFMFCJ/graph.json","events_json":"https://pith.science/api/pith-number/WPMBCDEG2HAHFILW7TSLWFMFCJ/events.json","paper":"https://pith.science/paper/WPMBCDEG"},"agent_actions":{"view_html":"https://pith.science/pith/WPMBCDEG2HAHFILW7TSLWFMFCJ","download_json":"https://pith.science/pith/WPMBCDEG2HAHFILW7TSLWFMFCJ.json","view_paper":"https://pith.science/paper/WPMBCDEG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9910232&json=true","fetch_graph":"https://pith.science/api/pith-number/WPMBCDEG2HAHFILW7TSLWFMFCJ/graph.json","fetch_events":"https://pith.science/api/pith-number/WPMBCDEG2HAHFILW7TSLWFMFCJ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WPMBCDEG2HAHFILW7TSLWFMFCJ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WPMBCDEG2HAHFILW7TSLWFMFCJ/action/storage_attestation","attest_author":"https://pith.science/pith/WPMBCDEG2HAHFILW7TSLWFMFCJ/action/author_attestation","sign_citation":"https://pith.science/pith/WPMBCDEG2HAHFILW7TSLWFMFCJ/action/citation_signature","submit_replication":"https://pith.science/pith/WPMBCDEG2HAHFILW7TSLWFMFCJ/action/replication_record"}},"created_at":"2026-07-04T16:13:23.815380+00:00","updated_at":"2026-07-04T16:13:23.815380+00:00"}