{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:PMPLA4DOTW3PCTEQ3K76XIQBH5","short_pith_number":"pith:PMPLA4DO","canonical_record":{"source":{"id":"1404.6670","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-04-26T18:48:48Z","cross_cats_sorted":[],"title_canon_sha256":"ebbe4669d56adcc52f170b906079a77904237b6044f1e39b05b2ab7f10ae90f9","abstract_canon_sha256":"a889a41a7f0402c7713e9f4bf8a2dc4fe96210047a41eda9fcf48d6c98691ae6"},"schema_version":"1.0"},"canonical_sha256":"7b1eb0706e9db6f14c90dabfeba2013f4bbf7b85e501370c8e2fef9a470531d8","source":{"kind":"arxiv","id":"1404.6670","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.6670","created_at":"2026-05-18T02:50:51Z"},{"alias_kind":"arxiv_version","alias_value":"1404.6670v1","created_at":"2026-05-18T02:50:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.6670","created_at":"2026-05-18T02:50:51Z"},{"alias_kind":"pith_short_12","alias_value":"PMPLA4DOTW3P","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"PMPLA4DOTW3PCTEQ","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"PMPLA4DO","created_at":"2026-05-18T12:28:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:PMPLA4DOTW3PCTEQ3K76XIQBH5","target":"record","payload":{"canonical_record":{"source":{"id":"1404.6670","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-04-26T18:48:48Z","cross_cats_sorted":[],"title_canon_sha256":"ebbe4669d56adcc52f170b906079a77904237b6044f1e39b05b2ab7f10ae90f9","abstract_canon_sha256":"a889a41a7f0402c7713e9f4bf8a2dc4fe96210047a41eda9fcf48d6c98691ae6"},"schema_version":"1.0"},"canonical_sha256":"7b1eb0706e9db6f14c90dabfeba2013f4bbf7b85e501370c8e2fef9a470531d8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:50:51.440087Z","signature_b64":"BDvVzad8HlPwf9JzkJgB4IZBTm17ns+/XMErZY4AQSTixygVSeZjaEExJ8iwATktemF0O1ynvFlmY/rwtv3ZDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7b1eb0706e9db6f14c90dabfeba2013f4bbf7b85e501370c8e2fef9a470531d8","last_reissued_at":"2026-05-18T02:50:51.439610Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:50:51.439610Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1404.6670","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":"2026-05-18T02:50:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YdGBovx1jxRjgBG6wYY5EFVgnBLePWoRELnNI3hfTnS1CGSZ23zHGU5RaTKZAm59phFSkVZWS/269wuGfMqDCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T04:31:05.404182Z"},"content_sha256":"e21cc58f7079776ef223e33113cc77fd0a9ebca5c7569a5eace9c974a41699d2","schema_version":"1.0","event_id":"sha256:e21cc58f7079776ef223e33113cc77fd0a9ebca5c7569a5eace9c974a41699d2"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:PMPLA4DOTW3PCTEQ3K76XIQBH5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Nonextensive lattice gauge theories: algorithms and methods","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Rafael B. Frigori","submitted_at":"2014-04-26T18:48:48Z","abstract_excerpt":"High-energy phenomena presenting strong dynamical correlations, long-range interactions and microscopic memory effects are well described by nonextensive versions of the canonical Boltzmann-Gibbs statistical mechanics. After a brief theoretical review, we introduce a class of generalized heat-bath algorithms that enable Monte Carlo lattice simulations of gauge fields on the nonextensive statistical ensemble of Tsallis. The algorithmic performance is evaluated as a function of the Tsallis parameter q in equilibrium and nonequilibrium setups. Then, we revisit short-time dynamic techniques, which"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.6670","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":"2026-05-18T02:50:51Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"C7aeHNmAN+iF6QJNQ2CngDs3xmQEssPH6Vq9IEAwQCcOWBgs2mEt9phhX1m4+4BowmN1LAqTkZvAmcbVmy70CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-09T04:31:05.404908Z"},"content_sha256":"3b819188d01e41d136116d35b6ec43e9c7fdeb4dea80178e3f44fc8c649c6590","schema_version":"1.0","event_id":"sha256:3b819188d01e41d136116d35b6ec43e9c7fdeb4dea80178e3f44fc8c649c6590"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PMPLA4DOTW3PCTEQ3K76XIQBH5/bundle.json","state_url":"https://pith.science/pith/PMPLA4DOTW3PCTEQ3K76XIQBH5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PMPLA4DOTW3PCTEQ3K76XIQBH5/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":"2026-06-09T04:31:05Z","links":{"resolver":"https://pith.science/pith/PMPLA4DOTW3PCTEQ3K76XIQBH5","bundle":"https://pith.science/pith/PMPLA4DOTW3PCTEQ3K76XIQBH5/bundle.json","state":"https://pith.science/pith/PMPLA4DOTW3PCTEQ3K76XIQBH5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PMPLA4DOTW3PCTEQ3K76XIQBH5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:PMPLA4DOTW3PCTEQ3K76XIQBH5","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":"a889a41a7f0402c7713e9f4bf8a2dc4fe96210047a41eda9fcf48d6c98691ae6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-04-26T18:48:48Z","title_canon_sha256":"ebbe4669d56adcc52f170b906079a77904237b6044f1e39b05b2ab7f10ae90f9"},"schema_version":"1.0","source":{"id":"1404.6670","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1404.6670","created_at":"2026-05-18T02:50:51Z"},{"alias_kind":"arxiv_version","alias_value":"1404.6670v1","created_at":"2026-05-18T02:50:51Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1404.6670","created_at":"2026-05-18T02:50:51Z"},{"alias_kind":"pith_short_12","alias_value":"PMPLA4DOTW3P","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"PMPLA4DOTW3PCTEQ","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"PMPLA4DO","created_at":"2026-05-18T12:28:43Z"}],"graph_snapshots":[{"event_id":"sha256:3b819188d01e41d136116d35b6ec43e9c7fdeb4dea80178e3f44fc8c649c6590","target":"graph","created_at":"2026-05-18T02:50:51Z","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":"High-energy phenomena presenting strong dynamical correlations, long-range interactions and microscopic memory effects are well described by nonextensive versions of the canonical Boltzmann-Gibbs statistical mechanics. After a brief theoretical review, we introduce a class of generalized heat-bath algorithms that enable Monte Carlo lattice simulations of gauge fields on the nonextensive statistical ensemble of Tsallis. The algorithmic performance is evaluated as a function of the Tsallis parameter q in equilibrium and nonequilibrium setups. Then, we revisit short-time dynamic techniques, which","authors_text":"Rafael B. Frigori","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-04-26T18:48:48Z","title":"Nonextensive lattice gauge theories: algorithms and methods"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1404.6670","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:e21cc58f7079776ef223e33113cc77fd0a9ebca5c7569a5eace9c974a41699d2","target":"record","created_at":"2026-05-18T02:50:51Z","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":"a889a41a7f0402c7713e9f4bf8a2dc4fe96210047a41eda9fcf48d6c98691ae6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2014-04-26T18:48:48Z","title_canon_sha256":"ebbe4669d56adcc52f170b906079a77904237b6044f1e39b05b2ab7f10ae90f9"},"schema_version":"1.0","source":{"id":"1404.6670","kind":"arxiv","version":1}},"canonical_sha256":"7b1eb0706e9db6f14c90dabfeba2013f4bbf7b85e501370c8e2fef9a470531d8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7b1eb0706e9db6f14c90dabfeba2013f4bbf7b85e501370c8e2fef9a470531d8","first_computed_at":"2026-05-18T02:50:51.439610Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:50:51.439610Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BDvVzad8HlPwf9JzkJgB4IZBTm17ns+/XMErZY4AQSTixygVSeZjaEExJ8iwATktemF0O1ynvFlmY/rwtv3ZDw==","signature_status":"signed_v1","signed_at":"2026-05-18T02:50:51.440087Z","signed_message":"canonical_sha256_bytes"},"source_id":"1404.6670","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e21cc58f7079776ef223e33113cc77fd0a9ebca5c7569a5eace9c974a41699d2","sha256:3b819188d01e41d136116d35b6ec43e9c7fdeb4dea80178e3f44fc8c649c6590"],"state_sha256":"13dff57ec7ecae64aa2a4edc19fa825d50c3131c5180997b27b00134813769e6"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"7LjpHdCJ9EGzu3TqUikYV0Ig77vJJzGIOqrCXcl6EnjHfQ6AdXKBF5+CKSBlWBuGc2E9cYM6BbMANBo1On+IDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-09T04:31:05.409171Z","bundle_sha256":"27bbaab3f83bb3aefd188f58da469e3deafc02a45e2c1f397e119793b8cf3471"}}