{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:AO5U7MT6LAZ622OHZBJKOYATPE","short_pith_number":"pith:AO5U7MT6","canonical_record":{"source":{"id":"cond-mat/0212302","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-12-12T19:34:17Z","cross_cats_sorted":[],"title_canon_sha256":"acf41ddeeb00f574ab7ab48d7c4909b008f389faa845af2367241b2c3a5440f8","abstract_canon_sha256":"ff132667152b73faa4a362fc5e36db99e1d63ca25910bc7a2cbf6ece466a8702"},"schema_version":"1.0"},"canonical_sha256":"03bb4fb27e5833ed69c7c852a760137907b05532b7e7038b741c8858ca24c102","source":{"kind":"arxiv","id":"cond-mat/0212302","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0212302","created_at":"2026-05-18T03:47:42Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0212302v1","created_at":"2026-05-18T03:47:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0212302","created_at":"2026-05-18T03:47:42Z"},{"alias_kind":"pith_short_12","alias_value":"AO5U7MT6LAZ6","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"AO5U7MT6LAZ622OH","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"AO5U7MT6","created_at":"2026-05-18T12:25:50Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:AO5U7MT6LAZ622OHZBJKOYATPE","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/0212302","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-12-12T19:34:17Z","cross_cats_sorted":[],"title_canon_sha256":"acf41ddeeb00f574ab7ab48d7c4909b008f389faa845af2367241b2c3a5440f8","abstract_canon_sha256":"ff132667152b73faa4a362fc5e36db99e1d63ca25910bc7a2cbf6ece466a8702"},"schema_version":"1.0"},"canonical_sha256":"03bb4fb27e5833ed69c7c852a760137907b05532b7e7038b741c8858ca24c102","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:42.148567Z","signature_b64":"36liuaEy7PKvTQx3mmYCuX4uJZWu4iC0MKstxcCxYjy9KJ7Ub8iLtvcMNIVLlpkFLPKI+AUQ2zzLGwPUFUK3Bg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"03bb4fb27e5833ed69c7c852a760137907b05532b7e7038b741c8858ca24c102","last_reissued_at":"2026-05-18T03:47:42.147673Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:42.147673Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/0212302","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":"2026-05-18T03:47:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ksxh1DuZo/1Ul9cFeZLhbellqg9E9nObg9Vsl1Qt7kWxx+RDYCWOBaDxycQiTS+xolr6fEJFvAm2c/wP30qVAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T03:44:09.561567Z"},"content_sha256":"376f605a1bd70b1106d9862855bdf56fdc10526a3bf91ac53b3c60a30e631d25","schema_version":"1.0","event_id":"sha256:376f605a1bd70b1106d9862855bdf56fdc10526a3bf91ac53b3c60a30e631d25"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:AO5U7MT6LAZ622OHZBJKOYATPE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Short-Time Dynamics of an Ising Model with Competing Interactions","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Jr., J. R. Drugowich de Felicio, N. Alves","submitted_at":"2002-12-12T19:34:17Z","abstract_excerpt":"In this work the two-dimensional Ising model with nearest- and next-nearest-neighbor interactions is revisited. We obtain the dynamic critical exponents $z$ and $\\theta$ from short-time Monte Carlo simulations. The dynamic critical exponent $z$ was obtained from the time behavior of the ratio $F_2=< M^2>_{m_0=0}/< M>^2_{m_0=1}\\sim t^{d/z}$, whereas the non-universal exponent $\\theta$ was estimated from the time correlation of the order parameter $<M(0)M(t)>\\sim t^{\\theta}$, where $M(t)$ is the order parameter at instant $t$, $d$ is the dimension of the system and $<(...)>$ is the average of th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0212302","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":"2026-05-18T03:47:42Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4ZW/NlirHSPPkxSFn7TrpMMmkNfVH/gXKbUfXbAMggdtyhdlMPF1jNDHQw5cKH3gdbJJQSWmXuHWMVYbbgeqBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-26T03:44:09.562072Z"},"content_sha256":"cc6ccdbedb1521f8b137af52605b2cca9eb4be4a00966a0caecdc0363cfbb94d","schema_version":"1.0","event_id":"sha256:cc6ccdbedb1521f8b137af52605b2cca9eb4be4a00966a0caecdc0363cfbb94d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/AO5U7MT6LAZ622OHZBJKOYATPE/bundle.json","state_url":"https://pith.science/pith/AO5U7MT6LAZ622OHZBJKOYATPE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/AO5U7MT6LAZ622OHZBJKOYATPE/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":"2026-06-26T03:44:09Z","links":{"resolver":"https://pith.science/pith/AO5U7MT6LAZ622OHZBJKOYATPE","bundle":"https://pith.science/pith/AO5U7MT6LAZ622OHZBJKOYATPE/bundle.json","state":"https://pith.science/pith/AO5U7MT6LAZ622OHZBJKOYATPE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/AO5U7MT6LAZ622OHZBJKOYATPE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:AO5U7MT6LAZ622OHZBJKOYATPE","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":"ff132667152b73faa4a362fc5e36db99e1d63ca25910bc7a2cbf6ece466a8702","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-12-12T19:34:17Z","title_canon_sha256":"acf41ddeeb00f574ab7ab48d7c4909b008f389faa845af2367241b2c3a5440f8"},"schema_version":"1.0","source":{"id":"cond-mat/0212302","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/0212302","created_at":"2026-05-18T03:47:42Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/0212302v1","created_at":"2026-05-18T03:47:42Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/0212302","created_at":"2026-05-18T03:47:42Z"},{"alias_kind":"pith_short_12","alias_value":"AO5U7MT6LAZ6","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_16","alias_value":"AO5U7MT6LAZ622OH","created_at":"2026-05-18T12:25:50Z"},{"alias_kind":"pith_short_8","alias_value":"AO5U7MT6","created_at":"2026-05-18T12:25:50Z"}],"graph_snapshots":[{"event_id":"sha256:cc6ccdbedb1521f8b137af52605b2cca9eb4be4a00966a0caecdc0363cfbb94d","target":"graph","created_at":"2026-05-18T03:47:42Z","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":"In this work the two-dimensional Ising model with nearest- and next-nearest-neighbor interactions is revisited. We obtain the dynamic critical exponents $z$ and $\\theta$ from short-time Monte Carlo simulations. The dynamic critical exponent $z$ was obtained from the time behavior of the ratio $F_2=< M^2>_{m_0=0}/< M>^2_{m_0=1}\\sim t^{d/z}$, whereas the non-universal exponent $\\theta$ was estimated from the time correlation of the order parameter $<M(0)M(t)>\\sim t^{\\theta}$, where $M(t)$ is the order parameter at instant $t$, $d$ is the dimension of the system and $<(...)>$ is the average of th","authors_text":"Jr., J. R. Drugowich de Felicio, N. Alves","cross_cats":[],"headline":"","license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-12-12T19:34:17Z","title":"Short-Time Dynamics of an Ising Model with Competing Interactions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/0212302","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":"sha256:376f605a1bd70b1106d9862855bdf56fdc10526a3bf91ac53b3c60a30e631d25","target":"record","created_at":"2026-05-18T03:47:42Z","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":"ff132667152b73faa4a362fc5e36db99e1d63ca25910bc7a2cbf6ece466a8702","cross_cats_sorted":[],"license":"","primary_cat":"cond-mat.stat-mech","submitted_at":"2002-12-12T19:34:17Z","title_canon_sha256":"acf41ddeeb00f574ab7ab48d7c4909b008f389faa845af2367241b2c3a5440f8"},"schema_version":"1.0","source":{"id":"cond-mat/0212302","kind":"arxiv","version":1}},"canonical_sha256":"03bb4fb27e5833ed69c7c852a760137907b05532b7e7038b741c8858ca24c102","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"03bb4fb27e5833ed69c7c852a760137907b05532b7e7038b741c8858ca24c102","first_computed_at":"2026-05-18T03:47:42.147673Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:47:42.147673Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"36liuaEy7PKvTQx3mmYCuX4uJZWu4iC0MKstxcCxYjy9KJ7Ub8iLtvcMNIVLlpkFLPKI+AUQ2zzLGwPUFUK3Bg==","signature_status":"signed_v1","signed_at":"2026-05-18T03:47:42.148567Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/0212302","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:376f605a1bd70b1106d9862855bdf56fdc10526a3bf91ac53b3c60a30e631d25","sha256:cc6ccdbedb1521f8b137af52605b2cca9eb4be4a00966a0caecdc0363cfbb94d"],"state_sha256":"5cfbe7eede010403e073b5f1929ba842d3d3b352901c7718aeb74a505d9a01e9"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/2r2lghQP2lV9icVRWTOXod8ReeJjia+Lqfsh1V7R8nXy6lRxwZ4ldQLBSBfYK/bva3uprF2tFj9/UOuED+OAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-26T03:44:09.564495Z","bundle_sha256":"792a8bf1c5c27838d6f22c7ea348ad798d6e1f58a6ca134c6aa583312a4f5892"}}