{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:CMOPACCQSLY6GDVW5JNR6CD47R","short_pith_number":"pith:CMOPACCQ","canonical_record":{"source":{"id":"1811.01887","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-11-05T18:06:50Z","cross_cats_sorted":[],"title_canon_sha256":"12c56ac980421505dd6e5b666021018eec0e26db6a3a02b258c71d8b7d27daae","abstract_canon_sha256":"9549e51ecb74e743cdfcd0df1070957c95fb647cfbf00a48d934b88ed6339650"},"schema_version":"1.0"},"canonical_sha256":"131cf0085092f1e30eb6ea5b1f087cfc448592cd3fa71893184e886cd4b7d1ef","source":{"kind":"arxiv","id":"1811.01887","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1811.01887","created_at":"2026-05-18T00:01:33Z"},{"alias_kind":"arxiv_version","alias_value":"1811.01887v1","created_at":"2026-05-18T00:01:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.01887","created_at":"2026-05-18T00:01:33Z"},{"alias_kind":"pith_short_12","alias_value":"CMOPACCQSLY6","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_16","alias_value":"CMOPACCQSLY6GDVW","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_8","alias_value":"CMOPACCQ","created_at":"2026-05-18T12:32:16Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:CMOPACCQSLY6GDVW5JNR6CD47R","target":"record","payload":{"canonical_record":{"source":{"id":"1811.01887","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-11-05T18:06:50Z","cross_cats_sorted":[],"title_canon_sha256":"12c56ac980421505dd6e5b666021018eec0e26db6a3a02b258c71d8b7d27daae","abstract_canon_sha256":"9549e51ecb74e743cdfcd0df1070957c95fb647cfbf00a48d934b88ed6339650"},"schema_version":"1.0"},"canonical_sha256":"131cf0085092f1e30eb6ea5b1f087cfc448592cd3fa71893184e886cd4b7d1ef","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:01:33.002904Z","signature_b64":"O1R+QE4EDmTqmCSIb+qvgOnQks2Yt/z3tQCe8XFzr1BezDo6fQsmlWzhyOgVfAGrFQNLNV63eO9vS9Fa1vrUDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"131cf0085092f1e30eb6ea5b1f087cfc448592cd3fa71893184e886cd4b7d1ef","last_reissued_at":"2026-05-18T00:01:33.002430Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:01:33.002430Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1811.01887","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":"2026-05-18T00:01:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"wNmowqh+4dVWtFHF3h+4QrD0nlfOtRQf7PiEOJGNHeqYUAm+BwPCDx3FTP+Xhn/KWP82dvImh/llMF3PMS7/Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T19:29:49.433189Z"},"content_sha256":"e802077063b01f19a81eb44d36818efc98174cbd950f66d66f88a326d76949d3","schema_version":"1.0","event_id":"sha256:e802077063b01f19a81eb44d36818efc98174cbd950f66d66f88a326d76949d3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:CMOPACCQSLY6GDVW5JNR6CD47R","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Localization in SU(3) gauge theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"Reka A. Vig, Tamas G. Kovacs","submitted_at":"2018-11-05T18:06:50Z","abstract_excerpt":"In this paper we study the localization transition of Dirac eigenmodes in quenched QCD. We determined the temperature dependence of the mobility edge in the quark-gluon plasma phase near the deconfining critical temperature. We calculated the critical temperature where all of the localized modes disappear from the spectrum and compared it with the critical temperature of the deconfining transition. We found that the localization transition happens at the same temperature as the deconfining transition which indicates a strong relation between the two phenomena."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.01887","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":"2026-05-18T00:01:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Foanb+21CRsxBL8ZweUTk19YjnP5TFCZio88e7+pQX/CBK/Xx+UVjfuQnLtzbr+2cY2RGe9SicBAGp7czwd7Bw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T19:29:49.433873Z"},"content_sha256":"54f5bfb83a299b95b9a0bb1dbec5db90cd5fa5b2b5006bb4e3c5a02b0f0283da","schema_version":"1.0","event_id":"sha256:54f5bfb83a299b95b9a0bb1dbec5db90cd5fa5b2b5006bb4e3c5a02b0f0283da"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CMOPACCQSLY6GDVW5JNR6CD47R/bundle.json","state_url":"https://pith.science/pith/CMOPACCQSLY6GDVW5JNR6CD47R/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CMOPACCQSLY6GDVW5JNR6CD47R/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":"2026-05-25T19:29:49Z","links":{"resolver":"https://pith.science/pith/CMOPACCQSLY6GDVW5JNR6CD47R","bundle":"https://pith.science/pith/CMOPACCQSLY6GDVW5JNR6CD47R/bundle.json","state":"https://pith.science/pith/CMOPACCQSLY6GDVW5JNR6CD47R/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CMOPACCQSLY6GDVW5JNR6CD47R/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:CMOPACCQSLY6GDVW5JNR6CD47R","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":"9549e51ecb74e743cdfcd0df1070957c95fb647cfbf00a48d934b88ed6339650","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-11-05T18:06:50Z","title_canon_sha256":"12c56ac980421505dd6e5b666021018eec0e26db6a3a02b258c71d8b7d27daae"},"schema_version":"1.0","source":{"id":"1811.01887","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1811.01887","created_at":"2026-05-18T00:01:33Z"},{"alias_kind":"arxiv_version","alias_value":"1811.01887v1","created_at":"2026-05-18T00:01:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.01887","created_at":"2026-05-18T00:01:33Z"},{"alias_kind":"pith_short_12","alias_value":"CMOPACCQSLY6","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_16","alias_value":"CMOPACCQSLY6GDVW","created_at":"2026-05-18T12:32:16Z"},{"alias_kind":"pith_short_8","alias_value":"CMOPACCQ","created_at":"2026-05-18T12:32:16Z"}],"graph_snapshots":[{"event_id":"sha256:54f5bfb83a299b95b9a0bb1dbec5db90cd5fa5b2b5006bb4e3c5a02b0f0283da","target":"graph","created_at":"2026-05-18T00:01:33Z","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":"In this paper we study the localization transition of Dirac eigenmodes in quenched QCD. We determined the temperature dependence of the mobility edge in the quark-gluon plasma phase near the deconfining critical temperature. We calculated the critical temperature where all of the localized modes disappear from the spectrum and compared it with the critical temperature of the deconfining transition. We found that the localization transition happens at the same temperature as the deconfining transition which indicates a strong relation between the two phenomena.","authors_text":"Reka A. Vig, Tamas G. Kovacs","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-11-05T18:06:50Z","title":"Localization in SU(3) gauge theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.01887","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:e802077063b01f19a81eb44d36818efc98174cbd950f66d66f88a326d76949d3","target":"record","created_at":"2026-05-18T00:01:33Z","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":"9549e51ecb74e743cdfcd0df1070957c95fb647cfbf00a48d934b88ed6339650","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2018-11-05T18:06:50Z","title_canon_sha256":"12c56ac980421505dd6e5b666021018eec0e26db6a3a02b258c71d8b7d27daae"},"schema_version":"1.0","source":{"id":"1811.01887","kind":"arxiv","version":1}},"canonical_sha256":"131cf0085092f1e30eb6ea5b1f087cfc448592cd3fa71893184e886cd4b7d1ef","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"131cf0085092f1e30eb6ea5b1f087cfc448592cd3fa71893184e886cd4b7d1ef","first_computed_at":"2026-05-18T00:01:33.002430Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:01:33.002430Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"O1R+QE4EDmTqmCSIb+qvgOnQks2Yt/z3tQCe8XFzr1BezDo6fQsmlWzhyOgVfAGrFQNLNV63eO9vS9Fa1vrUDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:01:33.002904Z","signed_message":"canonical_sha256_bytes"},"source_id":"1811.01887","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e802077063b01f19a81eb44d36818efc98174cbd950f66d66f88a326d76949d3","sha256:54f5bfb83a299b95b9a0bb1dbec5db90cd5fa5b2b5006bb4e3c5a02b0f0283da"],"state_sha256":"7735c70ec8a6a8524781810b066cace3741c7ddf8f51f46059712631d21a4964"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"nlg0n1ChGvN7Uus99+E8slDT1m/JwJ6fRHKwH6Q0Xn/Rd81acvYz2xdfePtbh8RHzpzrn2dGfqkIuJNAEt+oAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T19:29:49.437452Z","bundle_sha256":"e0623368de02826ae531d82d3e973e8a36a201737cda609f4d67b60beba03300"}}