{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:7CT4ITHA5VOHBP4PXQYZCQ6XEA","short_pith_number":"pith:7CT4ITHA","canonical_record":{"source":{"id":"1403.4560","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-03-18T18:13:00Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"d23d6562c99b3942dd85023491218320fb9647b8e9da9b35808cc610160c3224","abstract_canon_sha256":"677231e1417699ca533f680ad5bb1712618a30efdb8fb34f2749772784f8df98"},"schema_version":"1.0"},"canonical_sha256":"f8a7c44ce0ed5c70bf8fbc319143d72014581ada91ffc2c3caa4109d1911e4c0","source":{"kind":"arxiv","id":"1403.4560","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.4560","created_at":"2026-05-18T02:56:05Z"},{"alias_kind":"arxiv_version","alias_value":"1403.4560v1","created_at":"2026-05-18T02:56:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.4560","created_at":"2026-05-18T02:56:05Z"},{"alias_kind":"pith_short_12","alias_value":"7CT4ITHA5VOH","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"7CT4ITHA5VOHBP4P","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"7CT4ITHA","created_at":"2026-05-18T12:28:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:7CT4ITHA5VOHBP4PXQYZCQ6XEA","target":"record","payload":{"canonical_record":{"source":{"id":"1403.4560","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-03-18T18:13:00Z","cross_cats_sorted":["cond-mat.dis-nn"],"title_canon_sha256":"d23d6562c99b3942dd85023491218320fb9647b8e9da9b35808cc610160c3224","abstract_canon_sha256":"677231e1417699ca533f680ad5bb1712618a30efdb8fb34f2749772784f8df98"},"schema_version":"1.0"},"canonical_sha256":"f8a7c44ce0ed5c70bf8fbc319143d72014581ada91ffc2c3caa4109d1911e4c0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:56:05.543743Z","signature_b64":"21B27gcNKIhtDDXnnNHN6CvCy4uozJgTRLSRolbVVIeA3EVpFcYg5kXDtZIQFLwbG0QE6kjUIppSWL8oJNhgBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f8a7c44ce0ed5c70bf8fbc319143d72014581ada91ffc2c3caa4109d1911e4c0","last_reissued_at":"2026-05-18T02:56:05.543279Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:56:05.543279Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1403.4560","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":"2026-05-18T02:56:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"03Da32JQ+9jNdztdpsjBgtwYrSgZXZcYxd4AlewGTBW8OqDvHROHQLupE1dfSPoxfC6CeBQeS2D27IrptoEICw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T05:45:26.916535Z"},"content_sha256":"7a41b6032a4bbd44d9f3becdaadab34d6f47fcee2dac4b79ee84c3fc447e90d6","schema_version":"1.0","event_id":"sha256:7a41b6032a4bbd44d9f3becdaadab34d6f47fcee2dac4b79ee84c3fc447e90d6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:7CT4ITHA5VOHBP4PXQYZCQ6XEA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Three Dimensional Edwards-Anderson Spin Glass Model in an External Field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.dis-nn"],"primary_cat":"cond-mat.stat-mech","authors_text":"J. Ramanujam, Juana Moreno, Ka-Ming Tam, Mark Jarrell, Sheng Feng, Ye Fang, Zhifeng Yun","submitted_at":"2014-03-18T18:13:00Z","abstract_excerpt":"We study the Edwards-Anderson model on a simple cubic lattice with a finite constant external field. We employ an indicator composed of a ratio of susceptibilities at finite wavenumbers, which was recently proposed to avoid the difficulties of a zero momentum quantity, for capturing the spin glass phase transition. Unfortunately, this new indicator is fairly noisy, so a large pool of samples at low temperature and small external field are needed to generate results with sufficiently small statistical error for analysis. We thus implement the Monte Carlo method using graphics processing units t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.4560","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":"2026-05-18T02:56:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nmYEE9V0/CwNB6St928ojWuebJHpoDEgIVOBJ7ZokFDVxDhnqecIco4cp3gHuKNFECIz8EHaSp+nMkmRM/L0DA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T05:45:26.916879Z"},"content_sha256":"d45b7ce2e2c11518d4dd04d228fae4cdb68f24fa05dd5e4d3e49ebaf3291d94e","schema_version":"1.0","event_id":"sha256:d45b7ce2e2c11518d4dd04d228fae4cdb68f24fa05dd5e4d3e49ebaf3291d94e"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7CT4ITHA5VOHBP4PXQYZCQ6XEA/bundle.json","state_url":"https://pith.science/pith/7CT4ITHA5VOHBP4PXQYZCQ6XEA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7CT4ITHA5VOHBP4PXQYZCQ6XEA/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":"2026-06-01T05:45:26Z","links":{"resolver":"https://pith.science/pith/7CT4ITHA5VOHBP4PXQYZCQ6XEA","bundle":"https://pith.science/pith/7CT4ITHA5VOHBP4PXQYZCQ6XEA/bundle.json","state":"https://pith.science/pith/7CT4ITHA5VOHBP4PXQYZCQ6XEA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7CT4ITHA5VOHBP4PXQYZCQ6XEA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:7CT4ITHA5VOHBP4PXQYZCQ6XEA","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":"677231e1417699ca533f680ad5bb1712618a30efdb8fb34f2749772784f8df98","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-03-18T18:13:00Z","title_canon_sha256":"d23d6562c99b3942dd85023491218320fb9647b8e9da9b35808cc610160c3224"},"schema_version":"1.0","source":{"id":"1403.4560","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.4560","created_at":"2026-05-18T02:56:05Z"},{"alias_kind":"arxiv_version","alias_value":"1403.4560v1","created_at":"2026-05-18T02:56:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.4560","created_at":"2026-05-18T02:56:05Z"},{"alias_kind":"pith_short_12","alias_value":"7CT4ITHA5VOH","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_16","alias_value":"7CT4ITHA5VOHBP4P","created_at":"2026-05-18T12:28:16Z"},{"alias_kind":"pith_short_8","alias_value":"7CT4ITHA","created_at":"2026-05-18T12:28:16Z"}],"graph_snapshots":[{"event_id":"sha256:d45b7ce2e2c11518d4dd04d228fae4cdb68f24fa05dd5e4d3e49ebaf3291d94e","target":"graph","created_at":"2026-05-18T02:56:05Z","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":"We study the Edwards-Anderson model on a simple cubic lattice with a finite constant external field. We employ an indicator composed of a ratio of susceptibilities at finite wavenumbers, which was recently proposed to avoid the difficulties of a zero momentum quantity, for capturing the spin glass phase transition. Unfortunately, this new indicator is fairly noisy, so a large pool of samples at low temperature and small external field are needed to generate results with sufficiently small statistical error for analysis. We thus implement the Monte Carlo method using graphics processing units t","authors_text":"J. Ramanujam, Juana Moreno, Ka-Ming Tam, Mark Jarrell, Sheng Feng, Ye Fang, Zhifeng Yun","cross_cats":["cond-mat.dis-nn"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-03-18T18:13:00Z","title":"Three Dimensional Edwards-Anderson Spin Glass Model in an External Field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.4560","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":"sha256:7a41b6032a4bbd44d9f3becdaadab34d6f47fcee2dac4b79ee84c3fc447e90d6","target":"record","created_at":"2026-05-18T02:56:05Z","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":"677231e1417699ca533f680ad5bb1712618a30efdb8fb34f2749772784f8df98","cross_cats_sorted":["cond-mat.dis-nn"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-03-18T18:13:00Z","title_canon_sha256":"d23d6562c99b3942dd85023491218320fb9647b8e9da9b35808cc610160c3224"},"schema_version":"1.0","source":{"id":"1403.4560","kind":"arxiv","version":1}},"canonical_sha256":"f8a7c44ce0ed5c70bf8fbc319143d72014581ada91ffc2c3caa4109d1911e4c0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f8a7c44ce0ed5c70bf8fbc319143d72014581ada91ffc2c3caa4109d1911e4c0","first_computed_at":"2026-05-18T02:56:05.543279Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:56:05.543279Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"21B27gcNKIhtDDXnnNHN6CvCy4uozJgTRLSRolbVVIeA3EVpFcYg5kXDtZIQFLwbG0QE6kjUIppSWL8oJNhgBw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:56:05.543743Z","signed_message":"canonical_sha256_bytes"},"source_id":"1403.4560","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7a41b6032a4bbd44d9f3becdaadab34d6f47fcee2dac4b79ee84c3fc447e90d6","sha256:d45b7ce2e2c11518d4dd04d228fae4cdb68f24fa05dd5e4d3e49ebaf3291d94e"],"state_sha256":"b7be84dc588cb0a83b4b1dbe595188f4198f12fad70f945f2f2a5a877a304f22"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4IBE4GPTCbCuiQ8y6rtTYrTf3uFv+YjUKKwVClE/LkLi586EB18ZkLjRKvuFARiAjy/scrBGZz18EO9szv2aCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T05:45:26.919034Z","bundle_sha256":"559177f9e98ad7706e05198d94b8fc591d69d72ebcad4d2ddbadd903365b3bd2"}}