{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:55VYCQFN7M7YTE42SANTNW2K7M","short_pith_number":"pith:55VYCQFN","canonical_record":{"source":{"id":"1311.7211","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2013-11-28T05:27:50Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"3ad620225f03481e34bc50f0c3ff9f3d072c4626efc13020805fb3a12bdc5ea3","abstract_canon_sha256":"d236028a5cea154226e96b23a074ceaed2ddfabc4883159b28cca0a01ef09aad"},"schema_version":"1.0"},"canonical_sha256":"ef6b8140adfb3f89939a901b36db4afb1afd6d0c37b86def8880aff9c70d068a","source":{"kind":"arxiv","id":"1311.7211","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.7211","created_at":"2026-05-18T01:02:14Z"},{"alias_kind":"arxiv_version","alias_value":"1311.7211v1","created_at":"2026-05-18T01:02:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.7211","created_at":"2026-05-18T01:02:14Z"},{"alias_kind":"pith_short_12","alias_value":"55VYCQFN7M7Y","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"55VYCQFN7M7YTE42","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"55VYCQFN","created_at":"2026-05-18T12:27:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:55VYCQFN7M7YTE42SANTNW2K7M","target":"record","payload":{"canonical_record":{"source":{"id":"1311.7211","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2013-11-28T05:27:50Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"3ad620225f03481e34bc50f0c3ff9f3d072c4626efc13020805fb3a12bdc5ea3","abstract_canon_sha256":"d236028a5cea154226e96b23a074ceaed2ddfabc4883159b28cca0a01ef09aad"},"schema_version":"1.0"},"canonical_sha256":"ef6b8140adfb3f89939a901b36db4afb1afd6d0c37b86def8880aff9c70d068a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:02:14.284770Z","signature_b64":"b5SfzniZ/sXHdReEnBB0vs+J40dvtIvyimqmOkfu9Ml5zzsMkrOyz6clkvna5cpvblSf3k2xNNH6HMC2k6adDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ef6b8140adfb3f89939a901b36db4afb1afd6d0c37b86def8880aff9c70d068a","last_reissued_at":"2026-05-18T01:02:14.284072Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:02:14.284072Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1311.7211","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":"2026-05-18T01:02:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8hIfDLcy3Awa1I/qmIflwkRVF2wB721Fza9yNz9EPlP3dTZFrdasIZu/Y9kjdtvceb1aX9PmLPku+mu4x49CBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T12:20:23.729425Z"},"content_sha256":"c112ca38491c3283c30965d5e18a90b8eb22405baabf3f4ef83446c5fd56cefa","schema_version":"1.0","event_id":"sha256:c112ca38491c3283c30965d5e18a90b8eb22405baabf3f4ef83446c5fd56cefa"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:55VYCQFN7M7YTE42SANTNW2K7M","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Random Field XY Model in Three Dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.dis-nn","authors_text":"D. A. Garanin, E. M. Chudnovsky, T. Proctor","submitted_at":"2013-11-28T05:27:50Z","abstract_excerpt":"We study random-field xy spin model at T=0 numerically on lattices of up to 1000 x 1000 x 1000 spins with the accent on the weak random field. Our numerical method is physically equivalent to slow cooling in which the system is gradually losing the energy and relaxing to an energy minimum. The system shows glass properties, the resulting spin states depending strongly on the initial conditions. Random initial condition for the spins leads to the vortex glass (VG) state with short-range spin-spin correlations defined by the average distance between vortex lines. Collinear and some other vortex-"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.7211","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":"2026-05-18T01:02:14Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yb/3ejyulWgJUiKp5T7c6RdxoFV8v3zeCPaxjx7R3nWLzxS4PnY53bGJzBvNbUqJUuPC+ZPpaCeT52KYBPPfAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-24T12:20:23.729812Z"},"content_sha256":"91296826087aea89d59e13e0ce241b497579d4ad3736f886469598b4c0bc81b4","schema_version":"1.0","event_id":"sha256:91296826087aea89d59e13e0ce241b497579d4ad3736f886469598b4c0bc81b4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/55VYCQFN7M7YTE42SANTNW2K7M/bundle.json","state_url":"https://pith.science/pith/55VYCQFN7M7YTE42SANTNW2K7M/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/55VYCQFN7M7YTE42SANTNW2K7M/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":"2026-05-24T12:20:23Z","links":{"resolver":"https://pith.science/pith/55VYCQFN7M7YTE42SANTNW2K7M","bundle":"https://pith.science/pith/55VYCQFN7M7YTE42SANTNW2K7M/bundle.json","state":"https://pith.science/pith/55VYCQFN7M7YTE42SANTNW2K7M/state.json","well_known_bundle":"https://pith.science/.well-known/pith/55VYCQFN7M7YTE42SANTNW2K7M/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:55VYCQFN7M7YTE42SANTNW2K7M","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":"d236028a5cea154226e96b23a074ceaed2ddfabc4883159b28cca0a01ef09aad","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2013-11-28T05:27:50Z","title_canon_sha256":"3ad620225f03481e34bc50f0c3ff9f3d072c4626efc13020805fb3a12bdc5ea3"},"schema_version":"1.0","source":{"id":"1311.7211","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.7211","created_at":"2026-05-18T01:02:14Z"},{"alias_kind":"arxiv_version","alias_value":"1311.7211v1","created_at":"2026-05-18T01:02:14Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.7211","created_at":"2026-05-18T01:02:14Z"},{"alias_kind":"pith_short_12","alias_value":"55VYCQFN7M7Y","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"55VYCQFN7M7YTE42","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"55VYCQFN","created_at":"2026-05-18T12:27:34Z"}],"graph_snapshots":[{"event_id":"sha256:91296826087aea89d59e13e0ce241b497579d4ad3736f886469598b4c0bc81b4","target":"graph","created_at":"2026-05-18T01:02:14Z","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 random-field xy spin model at T=0 numerically on lattices of up to 1000 x 1000 x 1000 spins with the accent on the weak random field. Our numerical method is physically equivalent to slow cooling in which the system is gradually losing the energy and relaxing to an energy minimum. The system shows glass properties, the resulting spin states depending strongly on the initial conditions. Random initial condition for the spins leads to the vortex glass (VG) state with short-range spin-spin correlations defined by the average distance between vortex lines. Collinear and some other vortex-","authors_text":"D. A. Garanin, E. M. Chudnovsky, T. Proctor","cross_cats":["cond-mat.stat-mech"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2013-11-28T05:27:50Z","title":"Random Field XY Model in Three Dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.7211","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:c112ca38491c3283c30965d5e18a90b8eb22405baabf3f4ef83446c5fd56cefa","target":"record","created_at":"2026-05-18T01:02:14Z","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":"d236028a5cea154226e96b23a074ceaed2ddfabc4883159b28cca0a01ef09aad","cross_cats_sorted":["cond-mat.stat-mech"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.dis-nn","submitted_at":"2013-11-28T05:27:50Z","title_canon_sha256":"3ad620225f03481e34bc50f0c3ff9f3d072c4626efc13020805fb3a12bdc5ea3"},"schema_version":"1.0","source":{"id":"1311.7211","kind":"arxiv","version":1}},"canonical_sha256":"ef6b8140adfb3f89939a901b36db4afb1afd6d0c37b86def8880aff9c70d068a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ef6b8140adfb3f89939a901b36db4afb1afd6d0c37b86def8880aff9c70d068a","first_computed_at":"2026-05-18T01:02:14.284072Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:02:14.284072Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"b5SfzniZ/sXHdReEnBB0vs+J40dvtIvyimqmOkfu9Ml5zzsMkrOyz6clkvna5cpvblSf3k2xNNH6HMC2k6adDg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:02:14.284770Z","signed_message":"canonical_sha256_bytes"},"source_id":"1311.7211","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c112ca38491c3283c30965d5e18a90b8eb22405baabf3f4ef83446c5fd56cefa","sha256:91296826087aea89d59e13e0ce241b497579d4ad3736f886469598b4c0bc81b4"],"state_sha256":"567b18ef548262e373d60ec3143f7d0217fbc6ac4a54beda65f603e67430d906"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OOnML+oUewnfj029QGzjPl1YkhbuRXrsSCiPdgvB/KWznTJrrTn8DXwHsRwaWV/yZDRwvJ3QOpU33iVA+USXAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-24T12:20:23.731933Z","bundle_sha256":"dc22d7f14f0e3f61a2d423ab377df66aaea71064d0ca9c57d5d27174ad04cae2"}}