{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2007:NVZULKUCGZKTA4OG7EBE3GBJGA","short_pith_number":"pith:NVZULKUC","canonical_record":{"source":{"id":"0712.3514","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-12-20T18:15:38Z","cross_cats_sorted":["hep-lat","hep-th","nucl-th"],"title_canon_sha256":"aa4d014ad2fa9f85292c1cbee2b01b034ed9b21ae86ad2bda9a09a72c295660c","abstract_canon_sha256":"415399f4cb53bf29b938a37fb6fd5cc89f0641e5e98042907176f958f982ce91"},"schema_version":"1.0"},"canonical_sha256":"6d7345aa8236553071c6f9024d98293012aed22dc2d8afd8f2e79bff18fe3a06","source":{"kind":"arxiv","id":"0712.3514","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0712.3514","created_at":"2026-07-04T15:28:05Z"},{"alias_kind":"arxiv_version","alias_value":"0712.3514v2","created_at":"2026-07-04T15:28:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0712.3514","created_at":"2026-07-04T15:28:05Z"},{"alias_kind":"pith_short_12","alias_value":"NVZULKUCGZKT","created_at":"2026-07-04T15:28:05Z"},{"alias_kind":"pith_short_16","alias_value":"NVZULKUCGZKTA4OG","created_at":"2026-07-04T15:28:05Z"},{"alias_kind":"pith_short_8","alias_value":"NVZULKUC","created_at":"2026-07-04T15:28:05Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2007:NVZULKUCGZKTA4OG7EBE3GBJGA","target":"record","payload":{"canonical_record":{"source":{"id":"0712.3514","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2007-12-20T18:15:38Z","cross_cats_sorted":["hep-lat","hep-th","nucl-th"],"title_canon_sha256":"aa4d014ad2fa9f85292c1cbee2b01b034ed9b21ae86ad2bda9a09a72c295660c","abstract_canon_sha256":"415399f4cb53bf29b938a37fb6fd5cc89f0641e5e98042907176f958f982ce91"},"schema_version":"1.0"},"canonical_sha256":"6d7345aa8236553071c6f9024d98293012aed22dc2d8afd8f2e79bff18fe3a06","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:28:05.021373Z","signature_b64":"hsVe3Qx1qifDdnxzcFFVpydDH/tWoyGQTbU/7oO99Mvkj8v+ao8+JOf0a68CuspyLL+Fbka4LK2FH9LTAtPRCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6d7345aa8236553071c6f9024d98293012aed22dc2d8afd8f2e79bff18fe3a06","last_reissued_at":"2026-07-04T15:28:05.020961Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:28:05.020961Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0712.3514","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":"2026-07-04T15:28:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"P2Xpo44JCwdatHLBi+DTAhGCUmEdeItBqJHkcXVW0AvWeViEeX+Cto4sFZQV221nD/mdrUa+Jkg40xWJv3tKBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-19T08:43:35.931265Z"},"content_sha256":"03ef1e2c131ac2e1464352154c9a527df88958ec497c3e76ceeda10bff6820a7","schema_version":"1.0","event_id":"sha256:03ef1e2c131ac2e1464352154c9a527df88958ec497c3e76ceeda10bff6820a7"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2007:NVZULKUCGZKTA4OG7EBE3GBJGA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Bottom-up isotropization in classical-statistical lattice gauge theory","license":"","headline":"","cross_cats":["hep-lat","hep-th","nucl-th"],"primary_cat":"hep-ph","authors_text":"D. Sexty, J. Berges, S. Scheffler","submitted_at":"2007-12-20T18:15:38Z","abstract_excerpt":"We compute nonequilibrium dynamics for classical-statistical SU(2) pure gauge theory on a lattice. We consider anisotropic initial conditions with high occupation numbers in the transverse plane on a characteristic scale ~ Q_s. This is used to investigate the very early stages of the thermalization process in the context of heavy-ion collisions. We find Weibel or \"primary\" instabilities with growth rates similar to those obtained from previous treatments employing anisotropic distributions of hard modes (particles) in the weak coupling limit. We observe \"secondary\" growth rates for higher-mome"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0712.3514","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0712.3514/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T15:28:05Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"LqXBSMRgUKuVEySooUrHfy7mVIJKy3yEI5ePBnz/t0Ob9Hhgavlzx3fB3QBFfYaoUdWlNeaimPv4GrwWzW54CA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-19T08:43:35.931610Z"},"content_sha256":"68b3dc2aba2dd87368ba59aea152223bc7328f26264282b791a55523ad3dcb69","schema_version":"1.0","event_id":"sha256:68b3dc2aba2dd87368ba59aea152223bc7328f26264282b791a55523ad3dcb69"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NVZULKUCGZKTA4OG7EBE3GBJGA/bundle.json","state_url":"https://pith.science/pith/NVZULKUCGZKTA4OG7EBE3GBJGA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NVZULKUCGZKTA4OG7EBE3GBJGA/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":"2026-08-19T08:43:35Z","links":{"resolver":"https://pith.science/pith/NVZULKUCGZKTA4OG7EBE3GBJGA","bundle":"https://pith.science/pith/NVZULKUCGZKTA4OG7EBE3GBJGA/bundle.json","state":"https://pith.science/pith/NVZULKUCGZKTA4OG7EBE3GBJGA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NVZULKUCGZKTA4OG7EBE3GBJGA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2007:NVZULKUCGZKTA4OG7EBE3GBJGA","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":"415399f4cb53bf29b938a37fb6fd5cc89f0641e5e98042907176f958f982ce91","cross_cats_sorted":["hep-lat","hep-th","nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2007-12-20T18:15:38Z","title_canon_sha256":"aa4d014ad2fa9f85292c1cbee2b01b034ed9b21ae86ad2bda9a09a72c295660c"},"schema_version":"1.0","source":{"id":"0712.3514","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0712.3514","created_at":"2026-07-04T15:28:05Z"},{"alias_kind":"arxiv_version","alias_value":"0712.3514v2","created_at":"2026-07-04T15:28:05Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0712.3514","created_at":"2026-07-04T15:28:05Z"},{"alias_kind":"pith_short_12","alias_value":"NVZULKUCGZKT","created_at":"2026-07-04T15:28:05Z"},{"alias_kind":"pith_short_16","alias_value":"NVZULKUCGZKTA4OG","created_at":"2026-07-04T15:28:05Z"},{"alias_kind":"pith_short_8","alias_value":"NVZULKUC","created_at":"2026-07-04T15:28:05Z"}],"graph_snapshots":[{"event_id":"sha256:68b3dc2aba2dd87368ba59aea152223bc7328f26264282b791a55523ad3dcb69","target":"graph","created_at":"2026-07-04T15:28:05Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/0712.3514/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We compute nonequilibrium dynamics for classical-statistical SU(2) pure gauge theory on a lattice. We consider anisotropic initial conditions with high occupation numbers in the transverse plane on a characteristic scale ~ Q_s. This is used to investigate the very early stages of the thermalization process in the context of heavy-ion collisions. We find Weibel or \"primary\" instabilities with growth rates similar to those obtained from previous treatments employing anisotropic distributions of hard modes (particles) in the weak coupling limit. We observe \"secondary\" growth rates for higher-mome","authors_text":"D. Sexty, J. Berges, S. Scheffler","cross_cats":["hep-lat","hep-th","nucl-th"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2007-12-20T18:15:38Z","title":"Bottom-up isotropization in classical-statistical lattice gauge theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0712.3514","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":"sha256:03ef1e2c131ac2e1464352154c9a527df88958ec497c3e76ceeda10bff6820a7","target":"record","created_at":"2026-07-04T15:28:05Z","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":"415399f4cb53bf29b938a37fb6fd5cc89f0641e5e98042907176f958f982ce91","cross_cats_sorted":["hep-lat","hep-th","nucl-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2007-12-20T18:15:38Z","title_canon_sha256":"aa4d014ad2fa9f85292c1cbee2b01b034ed9b21ae86ad2bda9a09a72c295660c"},"schema_version":"1.0","source":{"id":"0712.3514","kind":"arxiv","version":2}},"canonical_sha256":"6d7345aa8236553071c6f9024d98293012aed22dc2d8afd8f2e79bff18fe3a06","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6d7345aa8236553071c6f9024d98293012aed22dc2d8afd8f2e79bff18fe3a06","first_computed_at":"2026-07-04T15:28:05.020961Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:28:05.020961Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hsVe3Qx1qifDdnxzcFFVpydDH/tWoyGQTbU/7oO99Mvkj8v+ao8+JOf0a68CuspyLL+Fbka4LK2FH9LTAtPRCg==","signature_status":"signed_v1","signed_at":"2026-07-04T15:28:05.021373Z","signed_message":"canonical_sha256_bytes"},"source_id":"0712.3514","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:03ef1e2c131ac2e1464352154c9a527df88958ec497c3e76ceeda10bff6820a7","sha256:68b3dc2aba2dd87368ba59aea152223bc7328f26264282b791a55523ad3dcb69"],"state_sha256":"08017b4a940ce9cecbb4733d5d5f2bc2021d9ccbf3eb51cc91fc9b9a7246222f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BYr7D5EEY8K/5JBmqoSY6s8RDvu14wTvPy0ahjAmaBmA8ij/WYdnLWreWlPnoHL8Ph4/T+0/v8loi6AyA0sMDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-19T08:43:35.935104Z","bundle_sha256":"6cfdb55705a80b10c4966dfad0256cb7fcb4da85e0d2d53b3412928571825a0f"}}