{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2015:UQWYXPVPOPWJAMHUWGMMAR5K24","short_pith_number":"pith:UQWYXPVP","canonical_record":{"source":{"id":"1508.03368","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2015-08-13T21:44:12Z","cross_cats_sorted":[],"title_canon_sha256":"8c49072bf696bf5ded1d0cdc01c5bf6bd5e30d4bf158e08a143f44db1ba907d9","abstract_canon_sha256":"3220d11c114d3a4140c1b31811585e569798572d40146d8fa774461c4f3a0239"},"schema_version":"1.0"},"canonical_sha256":"a42d8bbeaf73ec9030f4b198c047aad738884e122c105109e9c8fbc37969a9f4","source":{"kind":"arxiv","id":"1508.03368","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1508.03368","created_at":"2026-05-18T01:22:37Z"},{"alias_kind":"arxiv_version","alias_value":"1508.03368v1","created_at":"2026-05-18T01:22:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.03368","created_at":"2026-05-18T01:22:37Z"},{"alias_kind":"pith_short_12","alias_value":"UQWYXPVPOPWJ","created_at":"2026-05-18T12:29:44Z"},{"alias_kind":"pith_short_16","alias_value":"UQWYXPVPOPWJAMHU","created_at":"2026-05-18T12:29:44Z"},{"alias_kind":"pith_short_8","alias_value":"UQWYXPVP","created_at":"2026-05-18T12:29:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2015:UQWYXPVPOPWJAMHUWGMMAR5K24","target":"record","payload":{"canonical_record":{"source":{"id":"1508.03368","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2015-08-13T21:44:12Z","cross_cats_sorted":[],"title_canon_sha256":"8c49072bf696bf5ded1d0cdc01c5bf6bd5e30d4bf158e08a143f44db1ba907d9","abstract_canon_sha256":"3220d11c114d3a4140c1b31811585e569798572d40146d8fa774461c4f3a0239"},"schema_version":"1.0"},"canonical_sha256":"a42d8bbeaf73ec9030f4b198c047aad738884e122c105109e9c8fbc37969a9f4","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:22:37.053255Z","signature_b64":"oeAe87vyIYcs+P8xNXHCd2mJod+kS+6wYgGTTtmOPwU9T8Axd4WPPmuhRUA8WVCtFoGOIHPPngXd0akAWZQpAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a42d8bbeaf73ec9030f4b198c047aad738884e122c105109e9c8fbc37969a9f4","last_reissued_at":"2026-05-18T01:22:37.052810Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:22:37.052810Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1508.03368","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":"2026-05-18T01:22:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sscUx478tPK7lvkThGMYZUjn/EXI0NqLCFYvLUg4O0SI0Hh+MO/FFirHD+05dqzaEac82008v+FprIIO2QapDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T20:28:47.553676Z"},"content_sha256":"a5e974873c80fe6e860c66b521c5660589ab7ed7286951a83ad5c5ea81042583","schema_version":"1.0","event_id":"sha256:a5e974873c80fe6e860c66b521c5660589ab7ed7286951a83ad5c5ea81042583"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2015:UQWYXPVPOPWJAMHUWGMMAR5K24","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Non-self-averaging in Ising spin glasses; hyperuniversality","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.dis-nn","authors_text":"I. A. Campbell, P. H. Lundow","submitted_at":"2015-08-13T21:44:12Z","abstract_excerpt":"Ising spin glasses with bimodal and Gaussian near-neighbor interaction distributions are studied through numerical simulations. The non-self-averaging (normalized inter-sample variance) parameter $U_{22}(T,L)$ for the spin glass susceptibility (and for higher moments $U_{nn}(T,L)$) is reported for dimensions 2, 3, 4, 5 and 7. In each dimension $d$ the non-self-averaging parameters in the paramagnetic regime vary with the sample size L and the correlation length $\\xi(T,L)$ as $U_{nn}(\\beta,L) = [K_{d}\\xi(T,L)/L]^d$, and so follow a renormalization group law due to Aharony and Harris (1991). Emp"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.03368","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":"2026-05-18T01:22:37Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"l0rboKuv94Ja8fWN455PkGJCvG6GclsUkhGFi+1o/B0vZbfIRQWDThuoPzBsEGbsbcSdXGHRisa+Q+Ok7+Y5Cw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T20:28:47.554337Z"},"content_sha256":"02180a44a227958991b350cc4006fb9cac758b0072743976c069fa0f9fbad22c","schema_version":"1.0","event_id":"sha256:02180a44a227958991b350cc4006fb9cac758b0072743976c069fa0f9fbad22c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UQWYXPVPOPWJAMHUWGMMAR5K24/bundle.json","state_url":"https://pith.science/pith/UQWYXPVPOPWJAMHUWGMMAR5K24/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UQWYXPVPOPWJAMHUWGMMAR5K24/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":"2026-05-26T20:28:47Z","links":{"resolver":"https://pith.science/pith/UQWYXPVPOPWJAMHUWGMMAR5K24","bundle":"https://pith.science/pith/UQWYXPVPOPWJAMHUWGMMAR5K24/bundle.json","state":"https://pith.science/pith/UQWYXPVPOPWJAMHUWGMMAR5K24/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UQWYXPVPOPWJAMHUWGMMAR5K24/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2015:UQWYXPVPOPWJAMHUWGMMAR5K24","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":"3220d11c114d3a4140c1b31811585e569798572d40146d8fa774461c4f3a0239","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2015-08-13T21:44:12Z","title_canon_sha256":"8c49072bf696bf5ded1d0cdc01c5bf6bd5e30d4bf158e08a143f44db1ba907d9"},"schema_version":"1.0","source":{"id":"1508.03368","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1508.03368","created_at":"2026-05-18T01:22:37Z"},{"alias_kind":"arxiv_version","alias_value":"1508.03368v1","created_at":"2026-05-18T01:22:37Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1508.03368","created_at":"2026-05-18T01:22:37Z"},{"alias_kind":"pith_short_12","alias_value":"UQWYXPVPOPWJ","created_at":"2026-05-18T12:29:44Z"},{"alias_kind":"pith_short_16","alias_value":"UQWYXPVPOPWJAMHU","created_at":"2026-05-18T12:29:44Z"},{"alias_kind":"pith_short_8","alias_value":"UQWYXPVP","created_at":"2026-05-18T12:29:44Z"}],"graph_snapshots":[{"event_id":"sha256:02180a44a227958991b350cc4006fb9cac758b0072743976c069fa0f9fbad22c","target":"graph","created_at":"2026-05-18T01:22:37Z","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":"Ising spin glasses with bimodal and Gaussian near-neighbor interaction distributions are studied through numerical simulations. The non-self-averaging (normalized inter-sample variance) parameter $U_{22}(T,L)$ for the spin glass susceptibility (and for higher moments $U_{nn}(T,L)$) is reported for dimensions 2, 3, 4, 5 and 7. In each dimension $d$ the non-self-averaging parameters in the paramagnetic regime vary with the sample size L and the correlation length $\\xi(T,L)$ as $U_{nn}(\\beta,L) = [K_{d}\\xi(T,L)/L]^d$, and so follow a renormalization group law due to Aharony and Harris (1991). Emp","authors_text":"I. A. Campbell, P. H. Lundow","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2015-08-13T21:44:12Z","title":"Non-self-averaging in Ising spin glasses; hyperuniversality"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1508.03368","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:a5e974873c80fe6e860c66b521c5660589ab7ed7286951a83ad5c5ea81042583","target":"record","created_at":"2026-05-18T01:22:37Z","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":"3220d11c114d3a4140c1b31811585e569798572d40146d8fa774461c4f3a0239","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2015-08-13T21:44:12Z","title_canon_sha256":"8c49072bf696bf5ded1d0cdc01c5bf6bd5e30d4bf158e08a143f44db1ba907d9"},"schema_version":"1.0","source":{"id":"1508.03368","kind":"arxiv","version":1}},"canonical_sha256":"a42d8bbeaf73ec9030f4b198c047aad738884e122c105109e9c8fbc37969a9f4","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a42d8bbeaf73ec9030f4b198c047aad738884e122c105109e9c8fbc37969a9f4","first_computed_at":"2026-05-18T01:22:37.052810Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:22:37.052810Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"oeAe87vyIYcs+P8xNXHCd2mJod+kS+6wYgGTTtmOPwU9T8Axd4WPPmuhRUA8WVCtFoGOIHPPngXd0akAWZQpAw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:22:37.053255Z","signed_message":"canonical_sha256_bytes"},"source_id":"1508.03368","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a5e974873c80fe6e860c66b521c5660589ab7ed7286951a83ad5c5ea81042583","sha256:02180a44a227958991b350cc4006fb9cac758b0072743976c069fa0f9fbad22c"],"state_sha256":"494ea31dae54bbc5be7b32f7f8c241a54766614b7920abec0a2113f0b8b7334e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"y07UrFrRkBoW6VLX9AfDub2lNVQH3jLFT1Z0mKDU6zs5FRRUahJQZhA/Q54B6YMgwS73t2U+GkdFJhYNRQU5DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T20:28:47.557668Z","bundle_sha256":"09ab0fd78cd413ce2eec05678e4f2024566c3accebfd1de3320dd816de240c69"}}