{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:UCDZDLQXSS7OQBTN4CDIMTN75Z","short_pith_number":"pith:UCDZDLQX","canonical_record":{"source":{"id":"1203.5419","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-24T14:44:36Z","cross_cats_sorted":[],"title_canon_sha256":"37458f7b0cd651b94da434f39c477bc2934024aa540106beefaffbfd18fafa3b","abstract_canon_sha256":"99d9d72625cd26bb9d53269a041f5c261ed73c7ec5403cfd6d0a6140244dcdc0"},"schema_version":"1.0"},"canonical_sha256":"a08791ae1794bee8066de086864dbfee7c6421862ee66255d90e64e0c07cd2fc","source":{"kind":"arxiv","id":"1203.5419","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1203.5419","created_at":"2026-05-18T03:51:35Z"},{"alias_kind":"arxiv_version","alias_value":"1203.5419v1","created_at":"2026-05-18T03:51:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.5419","created_at":"2026-05-18T03:51:35Z"},{"alias_kind":"pith_short_12","alias_value":"UCDZDLQXSS7O","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"UCDZDLQXSS7OQBTN","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"UCDZDLQX","created_at":"2026-05-18T12:27:23Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:UCDZDLQXSS7OQBTN4CDIMTN75Z","target":"record","payload":{"canonical_record":{"source":{"id":"1203.5419","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-24T14:44:36Z","cross_cats_sorted":[],"title_canon_sha256":"37458f7b0cd651b94da434f39c477bc2934024aa540106beefaffbfd18fafa3b","abstract_canon_sha256":"99d9d72625cd26bb9d53269a041f5c261ed73c7ec5403cfd6d0a6140244dcdc0"},"schema_version":"1.0"},"canonical_sha256":"a08791ae1794bee8066de086864dbfee7c6421862ee66255d90e64e0c07cd2fc","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:51:35.319580Z","signature_b64":"potghSZ7zVT+gMohD11aEFMtZ6OflyQO5jRTxItrUaswW1HzkKGvOCb2qkWofod+PuD10NjQ68+ASSFZyh2yAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a08791ae1794bee8066de086864dbfee7c6421862ee66255d90e64e0c07cd2fc","last_reissued_at":"2026-05-18T03:51:35.318984Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:51:35.318984Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1203.5419","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":"2026-05-18T03:51:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5FMBNa7YMpPI6FXeOfvtMpoOgBFB0MmAFlde3LHIjwdwlB93XwSW6HNdnB9/fO+6mxGfPiD0xlPg3P3KOzB2CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T09:43:06.887135Z"},"content_sha256":"0b8f1d74f3e77fab35d6cb9e35f25e4925e46005dfa7e76fddfacfcb89d6335a","schema_version":"1.0","event_id":"sha256:0b8f1d74f3e77fab35d6cb9e35f25e4925e46005dfa7e76fddfacfcb89d6335a"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:UCDZDLQXSS7OQBTN4CDIMTN75Z","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nonequilibrium phase transitions and stationary state solutions of a three-dimensional random-field Ising model under a time dependent periodic external field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Erol Vatansever, Hamza Polat, \\\"Umit Ak{\\i}nc{\\i}, Yusuf Y\\\"uksel","submitted_at":"2012-03-24T14:44:36Z","abstract_excerpt":"Nonequilibrium behavior and dynamic phase transition properties of a kinetic Ising model under the influence of periodically oscillating random-fields have been analyzed within the framework of effective field theory (EFT) based on a decoupling approximation (DA). Dynamic equation of motion has been solved for a simple cubic lattice ($q=6$) by utilizing a Glauber type stochastic process. Amplitude of the sinusoidally oscillating magnetic field is randomly distributed on the lattice sites according to bimodal and trimodal distribution functions. For a bimodal type of amplitude distribution, it "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.5419","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":"2026-05-18T03:51:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ylDUYa5UTpNw0sEmPftK/0ag32FdpaLQYXoq7xi7A1MLatsR7rFf8d0V+b6cgwrRXyU5RUPUZkwh1CdIORrBAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-03T09:43:06.887498Z"},"content_sha256":"b569ab9f166509a826c257f7fe98d1d351d6f2d6c118961f8960e4fb51e60f41","schema_version":"1.0","event_id":"sha256:b569ab9f166509a826c257f7fe98d1d351d6f2d6c118961f8960e4fb51e60f41"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/UCDZDLQXSS7OQBTN4CDIMTN75Z/bundle.json","state_url":"https://pith.science/pith/UCDZDLQXSS7OQBTN4CDIMTN75Z/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/UCDZDLQXSS7OQBTN4CDIMTN75Z/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":"2026-06-03T09:43:06Z","links":{"resolver":"https://pith.science/pith/UCDZDLQXSS7OQBTN4CDIMTN75Z","bundle":"https://pith.science/pith/UCDZDLQXSS7OQBTN4CDIMTN75Z/bundle.json","state":"https://pith.science/pith/UCDZDLQXSS7OQBTN4CDIMTN75Z/state.json","well_known_bundle":"https://pith.science/.well-known/pith/UCDZDLQXSS7OQBTN4CDIMTN75Z/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:UCDZDLQXSS7OQBTN4CDIMTN75Z","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":"99d9d72625cd26bb9d53269a041f5c261ed73c7ec5403cfd6d0a6140244dcdc0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-24T14:44:36Z","title_canon_sha256":"37458f7b0cd651b94da434f39c477bc2934024aa540106beefaffbfd18fafa3b"},"schema_version":"1.0","source":{"id":"1203.5419","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1203.5419","created_at":"2026-05-18T03:51:35Z"},{"alias_kind":"arxiv_version","alias_value":"1203.5419v1","created_at":"2026-05-18T03:51:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.5419","created_at":"2026-05-18T03:51:35Z"},{"alias_kind":"pith_short_12","alias_value":"UCDZDLQXSS7O","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_16","alias_value":"UCDZDLQXSS7OQBTN","created_at":"2026-05-18T12:27:23Z"},{"alias_kind":"pith_short_8","alias_value":"UCDZDLQX","created_at":"2026-05-18T12:27:23Z"}],"graph_snapshots":[{"event_id":"sha256:b569ab9f166509a826c257f7fe98d1d351d6f2d6c118961f8960e4fb51e60f41","target":"graph","created_at":"2026-05-18T03:51:35Z","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":"Nonequilibrium behavior and dynamic phase transition properties of a kinetic Ising model under the influence of periodically oscillating random-fields have been analyzed within the framework of effective field theory (EFT) based on a decoupling approximation (DA). Dynamic equation of motion has been solved for a simple cubic lattice ($q=6$) by utilizing a Glauber type stochastic process. Amplitude of the sinusoidally oscillating magnetic field is randomly distributed on the lattice sites according to bimodal and trimodal distribution functions. For a bimodal type of amplitude distribution, it ","authors_text":"Erol Vatansever, Hamza Polat, \\\"Umit Ak{\\i}nc{\\i}, Yusuf Y\\\"uksel","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-24T14:44:36Z","title":"Nonequilibrium phase transitions and stationary state solutions of a three-dimensional random-field Ising model under a time dependent periodic external field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.5419","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":"sha256:0b8f1d74f3e77fab35d6cb9e35f25e4925e46005dfa7e76fddfacfcb89d6335a","target":"record","created_at":"2026-05-18T03:51:35Z","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":"99d9d72625cd26bb9d53269a041f5c261ed73c7ec5403cfd6d0a6140244dcdc0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2012-03-24T14:44:36Z","title_canon_sha256":"37458f7b0cd651b94da434f39c477bc2934024aa540106beefaffbfd18fafa3b"},"schema_version":"1.0","source":{"id":"1203.5419","kind":"arxiv","version":1}},"canonical_sha256":"a08791ae1794bee8066de086864dbfee7c6421862ee66255d90e64e0c07cd2fc","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a08791ae1794bee8066de086864dbfee7c6421862ee66255d90e64e0c07cd2fc","first_computed_at":"2026-05-18T03:51:35.318984Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:51:35.318984Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"potghSZ7zVT+gMohD11aEFMtZ6OflyQO5jRTxItrUaswW1HzkKGvOCb2qkWofod+PuD10NjQ68+ASSFZyh2yAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:51:35.319580Z","signed_message":"canonical_sha256_bytes"},"source_id":"1203.5419","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:0b8f1d74f3e77fab35d6cb9e35f25e4925e46005dfa7e76fddfacfcb89d6335a","sha256:b569ab9f166509a826c257f7fe98d1d351d6f2d6c118961f8960e4fb51e60f41"],"state_sha256":"99d766a298a9081dae8ba39480aed32fe415aa1accef87967a7228bd8e418343"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O/Se1GSMvVneLNwi/j24fAuIjGqjO4UVDYJ7j9vfdnHDmStuudpr9GoeDwojaFRjeDt2TYFrREq2vM6Ntx9tDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-03T09:43:06.889705Z","bundle_sha256":"4c4c1aa19e9dd419fa796c2210079865d5f014932b3d8f13571fc2dbecb4f73c"}}