{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2010:YZXELQOKKR73JLQ4QTPXNYUI6K","short_pith_number":"pith:YZXELQOK","canonical_record":{"source":{"id":"1010.5346","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2010-10-26T09:53:45Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"3a8ff5e387a8ca3b1bc7f14eed76ac40d4242d084d3e10fc5693b3c31653c3db","abstract_canon_sha256":"41b8d4d7af0a079f1bcb4805fe69e651556637b3a0bf8a4203fb2d056323d1fd"},"schema_version":"1.0"},"canonical_sha256":"c66e45c1ca547fb4ae1c84df76e288f289bc4333874c68f7b7b554b650895f8e","source":{"kind":"arxiv","id":"1010.5346","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.5346","created_at":"2026-05-18T02:04:58Z"},{"alias_kind":"arxiv_version","alias_value":"1010.5346v2","created_at":"2026-05-18T02:04:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.5346","created_at":"2026-05-18T02:04:58Z"},{"alias_kind":"pith_short_12","alias_value":"YZXELQOKKR73","created_at":"2026-05-18T12:26:17Z"},{"alias_kind":"pith_short_16","alias_value":"YZXELQOKKR73JLQ4","created_at":"2026-05-18T12:26:17Z"},{"alias_kind":"pith_short_8","alias_value":"YZXELQOK","created_at":"2026-05-18T12:26:17Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2010:YZXELQOKKR73JLQ4QTPXNYUI6K","target":"record","payload":{"canonical_record":{"source":{"id":"1010.5346","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2010-10-26T09:53:45Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"3a8ff5e387a8ca3b1bc7f14eed76ac40d4242d084d3e10fc5693b3c31653c3db","abstract_canon_sha256":"41b8d4d7af0a079f1bcb4805fe69e651556637b3a0bf8a4203fb2d056323d1fd"},"schema_version":"1.0"},"canonical_sha256":"c66e45c1ca547fb4ae1c84df76e288f289bc4333874c68f7b7b554b650895f8e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:04:58.368069Z","signature_b64":"Yt6H/HJfNxrE8o45Bnfdslw50EfzFER0U6JkHJeRNn6qIftpevJ09dR6ItFcgIqVdNmzSQQjFiu/FiARVjdECw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c66e45c1ca547fb4ae1c84df76e288f289bc4333874c68f7b7b554b650895f8e","last_reissued_at":"2026-05-18T02:04:58.367413Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:04:58.367413Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1010.5346","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:04:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tbBHN6k1E3BWRfPlEWEmMWuOylHfob4fdKM48OlJcWMi3nT2FsVA8Dlt0g7lGShwPErNCdxnOjBphl0T3qO1Ag==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T22:41:38.854020Z"},"content_sha256":"a89cc10c9974b42ffc0b91bfd0828691983d3ad9db05ae8e608eb00ec8a2c070","schema_version":"1.0","event_id":"sha256:a89cc10c9974b42ffc0b91bfd0828691983d3ad9db05ae8e608eb00ec8a2c070"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2010:YZXELQOKKR73JLQ4QTPXNYUI6K","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Partial annealing of a coupled mean-field spin-glass model with an embedded pattern","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"Ayaka Sakata, Koji Hukushima","submitted_at":"2010-10-26T09:53:45Z","abstract_excerpt":"A partially annealed mean-field spin-glass model with a locally embedded pattern is studied. The model consists of two dynamical variables, spins and interactions, that are in contact with thermal baths at temperatures T_S and T_J, respectively. Unlike the quenched system, characteristic correlations among the interactions are induced by the partial annealing. The model exhibits three phases, which are paramagnetic, ferromagnetic and spin-glass phases. In the ferromagnetic phase, the embedded pattern is stably realized. The phase diagram depends significantly on the ratio of two temperatures n"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.5346","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":""},"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":"2026-05-18T02:04:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ekx82hW7lIfNT4KGDCZM4mffsbnpSPvmxNsWdMpa21b1vLuDG2gxScOSD3OEgBbWZr50Iv6mc+R7G5HhG/q+Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-02T22:41:38.854388Z"},"content_sha256":"3caca169fecc2f98e717b646c7695d446a050c1e8a6c0e121ca0b12f6f31bd9e","schema_version":"1.0","event_id":"sha256:3caca169fecc2f98e717b646c7695d446a050c1e8a6c0e121ca0b12f6f31bd9e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YZXELQOKKR73JLQ4QTPXNYUI6K/bundle.json","state_url":"https://pith.science/pith/YZXELQOKKR73JLQ4QTPXNYUI6K/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YZXELQOKKR73JLQ4QTPXNYUI6K/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":"2026-06-02T22:41:38Z","links":{"resolver":"https://pith.science/pith/YZXELQOKKR73JLQ4QTPXNYUI6K","bundle":"https://pith.science/pith/YZXELQOKKR73JLQ4QTPXNYUI6K/bundle.json","state":"https://pith.science/pith/YZXELQOKKR73JLQ4QTPXNYUI6K/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YZXELQOKKR73JLQ4QTPXNYUI6K/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2010:YZXELQOKKR73JLQ4QTPXNYUI6K","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":"41b8d4d7af0a079f1bcb4805fe69e651556637b3a0bf8a4203fb2d056323d1fd","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2010-10-26T09:53:45Z","title_canon_sha256":"3a8ff5e387a8ca3b1bc7f14eed76ac40d4242d084d3e10fc5693b3c31653c3db"},"schema_version":"1.0","source":{"id":"1010.5346","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1010.5346","created_at":"2026-05-18T02:04:58Z"},{"alias_kind":"arxiv_version","alias_value":"1010.5346v2","created_at":"2026-05-18T02:04:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1010.5346","created_at":"2026-05-18T02:04:58Z"},{"alias_kind":"pith_short_12","alias_value":"YZXELQOKKR73","created_at":"2026-05-18T12:26:17Z"},{"alias_kind":"pith_short_16","alias_value":"YZXELQOKKR73JLQ4","created_at":"2026-05-18T12:26:17Z"},{"alias_kind":"pith_short_8","alias_value":"YZXELQOK","created_at":"2026-05-18T12:26:17Z"}],"graph_snapshots":[{"event_id":"sha256:3caca169fecc2f98e717b646c7695d446a050c1e8a6c0e121ca0b12f6f31bd9e","target":"graph","created_at":"2026-05-18T02:04:58Z","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":"A partially annealed mean-field spin-glass model with a locally embedded pattern is studied. The model consists of two dynamical variables, spins and interactions, that are in contact with thermal baths at temperatures T_S and T_J, respectively. Unlike the quenched system, characteristic correlations among the interactions are induced by the partial annealing. The model exhibits three phases, which are paramagnetic, ferromagnetic and spin-glass phases. In the ferromagnetic phase, the embedded pattern is stably realized. The phase diagram depends significantly on the ratio of two temperatures n","authors_text":"Ayaka Sakata, Koji Hukushima","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2010-10-26T09:53:45Z","title":"Partial annealing of a coupled mean-field spin-glass model with an embedded pattern"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1010.5346","kind":"arxiv","version":2},"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:a89cc10c9974b42ffc0b91bfd0828691983d3ad9db05ae8e608eb00ec8a2c070","target":"record","created_at":"2026-05-18T02:04:58Z","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":"41b8d4d7af0a079f1bcb4805fe69e651556637b3a0bf8a4203fb2d056323d1fd","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2010-10-26T09:53:45Z","title_canon_sha256":"3a8ff5e387a8ca3b1bc7f14eed76ac40d4242d084d3e10fc5693b3c31653c3db"},"schema_version":"1.0","source":{"id":"1010.5346","kind":"arxiv","version":2}},"canonical_sha256":"c66e45c1ca547fb4ae1c84df76e288f289bc4333874c68f7b7b554b650895f8e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c66e45c1ca547fb4ae1c84df76e288f289bc4333874c68f7b7b554b650895f8e","first_computed_at":"2026-05-18T02:04:58.367413Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:04:58.367413Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Yt6H/HJfNxrE8o45Bnfdslw50EfzFER0U6JkHJeRNn6qIftpevJ09dR6ItFcgIqVdNmzSQQjFiu/FiARVjdECw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:04:58.368069Z","signed_message":"canonical_sha256_bytes"},"source_id":"1010.5346","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a89cc10c9974b42ffc0b91bfd0828691983d3ad9db05ae8e608eb00ec8a2c070","sha256:3caca169fecc2f98e717b646c7695d446a050c1e8a6c0e121ca0b12f6f31bd9e"],"state_sha256":"567ad6a23aefccbe9f70d2cae929e08900565d645f33b879bdf431240d024f5a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5lVwGoISTXeq4T7qjVO5yHLfbzURSRHiPmE/c8z/2X4qM3ctpXcpObz/NvnFBBLQtHrBS1rtJqBqs+gguuqDCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-02T22:41:38.856275Z","bundle_sha256":"a47353a9184dd21a091a3b66565e32c6bd4656577331b62a677284ef71ed7d0e"}}