{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:BCKGPZGMSJSCOUET5VYCE2C6YA","short_pith_number":"pith:BCKGPZGM","canonical_record":{"source":{"id":"1105.2949","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-05-15T14:40:20Z","cross_cats_sorted":[],"title_canon_sha256":"4adf34a8682a0486b7156d0d548b5fbcc64d1e4130e4502844277fdda17e92d1","abstract_canon_sha256":"5f70b0d71b701bce7001474da4c5cb62d4dff55ddc3cb425406938cfa4eab7ba"},"schema_version":"1.0"},"canonical_sha256":"089467e4cc9264275093ed7022685ec039734e696a0d2839c80a58d6847a942c","source":{"kind":"arxiv","id":"1105.2949","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.2949","created_at":"2026-05-18T02:01:58Z"},{"alias_kind":"arxiv_version","alias_value":"1105.2949v1","created_at":"2026-05-18T02:01:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.2949","created_at":"2026-05-18T02:01:58Z"},{"alias_kind":"pith_short_12","alias_value":"BCKGPZGMSJSC","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"BCKGPZGMSJSCOUET","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"BCKGPZGM","created_at":"2026-05-18T12:26:24Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:BCKGPZGMSJSCOUET5VYCE2C6YA","target":"record","payload":{"canonical_record":{"source":{"id":"1105.2949","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-05-15T14:40:20Z","cross_cats_sorted":[],"title_canon_sha256":"4adf34a8682a0486b7156d0d548b5fbcc64d1e4130e4502844277fdda17e92d1","abstract_canon_sha256":"5f70b0d71b701bce7001474da4c5cb62d4dff55ddc3cb425406938cfa4eab7ba"},"schema_version":"1.0"},"canonical_sha256":"089467e4cc9264275093ed7022685ec039734e696a0d2839c80a58d6847a942c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:01:58.178999Z","signature_b64":"AjfJt5rUzpE1zQuERQgsFQx7F8wRWCPLSr2fTwL/eRqYTV5H+lFwSe6avmQXSiVHC3SSA4tS3yh9f5gcJZpLDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"089467e4cc9264275093ed7022685ec039734e696a0d2839c80a58d6847a942c","last_reissued_at":"2026-05-18T02:01:58.178280Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:01:58.178280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1105.2949","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":"2026-05-18T02:01:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4f121Ui4XeYQWNU8PIQJ/f/fAsy44xo4Qr0zSoBm0alfeVvbJgsGvbOba9w5Y5LI5KivAmkUzc0hXy43aH/yBQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T03:59:31.754760Z"},"content_sha256":"bd9315cac2ecc67dded0054bc6c7a27bdf0b3f45761e1a8b038886e8efcac9df","schema_version":"1.0","event_id":"sha256:bd9315cac2ecc67dded0054bc6c7a27bdf0b3f45761e1a8b038886e8efcac9df"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:BCKGPZGMSJSCOUET5VYCE2C6YA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Fluctuations of two-time quantities and time-reparametrization invariance in spin-glasses","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Claudio Chamon, Federico Corberi, Leticia F. Cugliandolo","submitted_at":"2011-05-15T14:40:20Z","abstract_excerpt":"This article is a contribution to the understanding of fluctuations in the out of equilibrium dynamics of glassy systems. By extending theoretical ideas based on the assumption that time-reparametrization invariance develops asymptotically we deduce the scaling properties of diverse high-order correlation functions. We examine these predictions with numerical tests in a standard glassy model, the 3d Edwards-Anderson spin-glass, and in a system where time-reparametrization invariance is not expected to hold, the 2d ferromagnetic Ising model, both at low temperatures. Our results enlighten a qua"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.2949","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":"2026-05-18T02:01:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CX5JgGDD7eu3QPAbTSx7BlGtb/67/Xs3WBubsFXDynP2WXQ6YyF8l6jYgMUCT1+DyLauNba4/YM1Vk3a0imeDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T03:59:31.755149Z"},"content_sha256":"cc0552b151ac9c1d7733cb246e48a3db1e50b1aa0b7e7e1a47cf6dc7a3635049","schema_version":"1.0","event_id":"sha256:cc0552b151ac9c1d7733cb246e48a3db1e50b1aa0b7e7e1a47cf6dc7a3635049"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BCKGPZGMSJSCOUET5VYCE2C6YA/bundle.json","state_url":"https://pith.science/pith/BCKGPZGMSJSCOUET5VYCE2C6YA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BCKGPZGMSJSCOUET5VYCE2C6YA/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":"2026-05-31T03:59:31Z","links":{"resolver":"https://pith.science/pith/BCKGPZGMSJSCOUET5VYCE2C6YA","bundle":"https://pith.science/pith/BCKGPZGMSJSCOUET5VYCE2C6YA/bundle.json","state":"https://pith.science/pith/BCKGPZGMSJSCOUET5VYCE2C6YA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BCKGPZGMSJSCOUET5VYCE2C6YA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:BCKGPZGMSJSCOUET5VYCE2C6YA","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":"5f70b0d71b701bce7001474da4c5cb62d4dff55ddc3cb425406938cfa4eab7ba","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-05-15T14:40:20Z","title_canon_sha256":"4adf34a8682a0486b7156d0d548b5fbcc64d1e4130e4502844277fdda17e92d1"},"schema_version":"1.0","source":{"id":"1105.2949","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1105.2949","created_at":"2026-05-18T02:01:58Z"},{"alias_kind":"arxiv_version","alias_value":"1105.2949v1","created_at":"2026-05-18T02:01:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1105.2949","created_at":"2026-05-18T02:01:58Z"},{"alias_kind":"pith_short_12","alias_value":"BCKGPZGMSJSC","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_16","alias_value":"BCKGPZGMSJSCOUET","created_at":"2026-05-18T12:26:24Z"},{"alias_kind":"pith_short_8","alias_value":"BCKGPZGM","created_at":"2026-05-18T12:26:24Z"}],"graph_snapshots":[{"event_id":"sha256:cc0552b151ac9c1d7733cb246e48a3db1e50b1aa0b7e7e1a47cf6dc7a3635049","target":"graph","created_at":"2026-05-18T02:01:58Z","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":"This article is a contribution to the understanding of fluctuations in the out of equilibrium dynamics of glassy systems. By extending theoretical ideas based on the assumption that time-reparametrization invariance develops asymptotically we deduce the scaling properties of diverse high-order correlation functions. We examine these predictions with numerical tests in a standard glassy model, the 3d Edwards-Anderson spin-glass, and in a system where time-reparametrization invariance is not expected to hold, the 2d ferromagnetic Ising model, both at low temperatures. Our results enlighten a qua","authors_text":"Claudio Chamon, Federico Corberi, Leticia F. Cugliandolo","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-05-15T14:40:20Z","title":"Fluctuations of two-time quantities and time-reparametrization invariance in spin-glasses"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1105.2949","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:bd9315cac2ecc67dded0054bc6c7a27bdf0b3f45761e1a8b038886e8efcac9df","target":"record","created_at":"2026-05-18T02:01:58Z","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":"5f70b0d71b701bce7001474da4c5cb62d4dff55ddc3cb425406938cfa4eab7ba","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2011-05-15T14:40:20Z","title_canon_sha256":"4adf34a8682a0486b7156d0d548b5fbcc64d1e4130e4502844277fdda17e92d1"},"schema_version":"1.0","source":{"id":"1105.2949","kind":"arxiv","version":1}},"canonical_sha256":"089467e4cc9264275093ed7022685ec039734e696a0d2839c80a58d6847a942c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"089467e4cc9264275093ed7022685ec039734e696a0d2839c80a58d6847a942c","first_computed_at":"2026-05-18T02:01:58.178280Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:01:58.178280Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"AjfJt5rUzpE1zQuERQgsFQx7F8wRWCPLSr2fTwL/eRqYTV5H+lFwSe6avmQXSiVHC3SSA4tS3yh9f5gcJZpLDg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:01:58.178999Z","signed_message":"canonical_sha256_bytes"},"source_id":"1105.2949","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:bd9315cac2ecc67dded0054bc6c7a27bdf0b3f45761e1a8b038886e8efcac9df","sha256:cc0552b151ac9c1d7733cb246e48a3db1e50b1aa0b7e7e1a47cf6dc7a3635049"],"state_sha256":"1857b26f721269ffe340cba19b53af15e929acef81e6aba817219c470efd638b"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"mEg3pCKzHeDDT3alRiUEtVroGYqa1+VVT8FDWTV7yByoJReRRfVEmP3ah1nl6pE0GJvX8MF0E1CysoFRqPAuBA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T03:59:31.759394Z","bundle_sha256":"64e380397d753435bd4ad4e4f277bbbb8f61040cc2f0efd4ff2ad30d9aa6ea2e"}}