{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1993:L3MHFRWBC3SYHXKDPXJPZTDQVE","short_pith_number":"pith:L3MHFRWB","canonical_record":{"source":{"id":"hep-lat/9310023","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1993-10-21T19:01:08Z","cross_cats_sorted":[],"title_canon_sha256":"d61f5b583b46f4452eac1aa9e7e96d6755e56a2249131fdee8b301cc61376d69","abstract_canon_sha256":"1d11895c0e8ac63f74414cbfe7c170d4b223b0337393a5cb09537c8cda8f297d"},"schema_version":"1.0"},"canonical_sha256":"5ed872c6c116e583dd437dd2fccc70a91327436ff4ba88bc1e73002707d47c45","source":{"kind":"arxiv","id":"hep-lat/9310023","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9310023","created_at":"2026-07-04T15:50:28Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9310023v1","created_at":"2026-07-04T15:50:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9310023","created_at":"2026-07-04T15:50:28Z"},{"alias_kind":"pith_short_12","alias_value":"L3MHFRWBC3SY","created_at":"2026-07-04T15:50:28Z"},{"alias_kind":"pith_short_16","alias_value":"L3MHFRWBC3SYHXKD","created_at":"2026-07-04T15:50:28Z"},{"alias_kind":"pith_short_8","alias_value":"L3MHFRWB","created_at":"2026-07-04T15:50:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1993:L3MHFRWBC3SYHXKDPXJPZTDQVE","target":"record","payload":{"canonical_record":{"source":{"id":"hep-lat/9310023","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-lat","submitted_at":"1993-10-21T19:01:08Z","cross_cats_sorted":[],"title_canon_sha256":"d61f5b583b46f4452eac1aa9e7e96d6755e56a2249131fdee8b301cc61376d69","abstract_canon_sha256":"1d11895c0e8ac63f74414cbfe7c170d4b223b0337393a5cb09537c8cda8f297d"},"schema_version":"1.0"},"canonical_sha256":"5ed872c6c116e583dd437dd2fccc70a91327436ff4ba88bc1e73002707d47c45","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:50:28.267517Z","signature_b64":"CrxOZInhv7f0q/6yRmt0HWUrAdE5advfBliC022A+5Au5nb+O8J968RE3C7O8pwUj8gMzIWfZwNZq0hhtz4ICg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5ed872c6c116e583dd437dd2fccc70a91327436ff4ba88bc1e73002707d47c45","last_reissued_at":"2026-07-04T15:50:28.267051Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:50:28.267051Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-lat/9310023","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":"2026-07-04T15:50:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8oHG71fwkwLt43fZqSqtjvR84g8w1Ni70JdCXCWHC1jrcz+dOhtKaqC6YU+WUJSps7ORWfKdUNdQoGts+Tl+Dw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-07T07:10:20.303245Z"},"content_sha256":"d268c7149c2473e6535647de1f599150f30484e586932eeebc2bd685efc1b90b","schema_version":"1.0","event_id":"sha256:d268c7149c2473e6535647de1f599150f30484e586932eeebc2bd685efc1b90b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1993:L3MHFRWBC3SYHXKDPXJPZTDQVE","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The nature of the thermal phase transition with Wilson quarks","license":"","headline":"","cross_cats":[],"primary_cat":"hep-lat","authors_text":"A. Hasenfratz, Carleton DeTar, Claude Bernard, D. Toussaint, Leo Karkkainen, R. L. Sugar, Steven Gottlieb, Thomas A. DeGrand","submitted_at":"1993-10-21T19:01:08Z","abstract_excerpt":"We describe a series of simulations of high temperature QCD with two flavors of Wilson quarks aimed at clarifying the nature of the high temperature phase found in current simulations. Most of our work is with four time slices, although we include some runs with six and eight time slices for comparison. In addition to the usual thermodynamic observables we study the quark mass defined by the divergence of the axial current and the quark propagator in the Landau gauge. We find that the sharpness of the $N_t=4$ thermal transition has a maximum around $\\kappa=0.19$ and $6/g^2=4.8$."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9310023","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-lat/9310023/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":"2026-07-04T15:50:28Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"TB9Bjf96+iXn+ODZXLSnrm1swODL2t5kOSKVAalIIb6QE0STl68/lsFFUdi4O1k434FfB8COzCf6CuezA3fHCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-07T07:10:20.303622Z"},"content_sha256":"8b40013690bf17d5a6b6a66e6ef896c280e2f1285f5b55f02dc8b94b1fbd05ca","schema_version":"1.0","event_id":"sha256:8b40013690bf17d5a6b6a66e6ef896c280e2f1285f5b55f02dc8b94b1fbd05ca"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/L3MHFRWBC3SYHXKDPXJPZTDQVE/bundle.json","state_url":"https://pith.science/pith/L3MHFRWBC3SYHXKDPXJPZTDQVE/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/L3MHFRWBC3SYHXKDPXJPZTDQVE/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":"2026-07-07T07:10:20Z","links":{"resolver":"https://pith.science/pith/L3MHFRWBC3SYHXKDPXJPZTDQVE","bundle":"https://pith.science/pith/L3MHFRWBC3SYHXKDPXJPZTDQVE/bundle.json","state":"https://pith.science/pith/L3MHFRWBC3SYHXKDPXJPZTDQVE/state.json","well_known_bundle":"https://pith.science/.well-known/pith/L3MHFRWBC3SYHXKDPXJPZTDQVE/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1993:L3MHFRWBC3SYHXKDPXJPZTDQVE","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":"1d11895c0e8ac63f74414cbfe7c170d4b223b0337393a5cb09537c8cda8f297d","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"1993-10-21T19:01:08Z","title_canon_sha256":"d61f5b583b46f4452eac1aa9e7e96d6755e56a2249131fdee8b301cc61376d69"},"schema_version":"1.0","source":{"id":"hep-lat/9310023","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-lat/9310023","created_at":"2026-07-04T15:50:28Z"},{"alias_kind":"arxiv_version","alias_value":"hep-lat/9310023v1","created_at":"2026-07-04T15:50:28Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-lat/9310023","created_at":"2026-07-04T15:50:28Z"},{"alias_kind":"pith_short_12","alias_value":"L3MHFRWBC3SY","created_at":"2026-07-04T15:50:28Z"},{"alias_kind":"pith_short_16","alias_value":"L3MHFRWBC3SYHXKD","created_at":"2026-07-04T15:50:28Z"},{"alias_kind":"pith_short_8","alias_value":"L3MHFRWB","created_at":"2026-07-04T15:50:28Z"}],"graph_snapshots":[{"event_id":"sha256:8b40013690bf17d5a6b6a66e6ef896c280e2f1285f5b55f02dc8b94b1fbd05ca","target":"graph","created_at":"2026-07-04T15:50:28Z","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/hep-lat/9310023/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We describe a series of simulations of high temperature QCD with two flavors of Wilson quarks aimed at clarifying the nature of the high temperature phase found in current simulations. Most of our work is with four time slices, although we include some runs with six and eight time slices for comparison. In addition to the usual thermodynamic observables we study the quark mass defined by the divergence of the axial current and the quark propagator in the Landau gauge. We find that the sharpness of the $N_t=4$ thermal transition has a maximum around $\\kappa=0.19$ and $6/g^2=4.8$.","authors_text":"A. Hasenfratz, Carleton DeTar, Claude Bernard, D. Toussaint, Leo Karkkainen, R. L. Sugar, Steven Gottlieb, Thomas A. DeGrand","cross_cats":[],"headline":"","license":"","primary_cat":"hep-lat","submitted_at":"1993-10-21T19:01:08Z","title":"The nature of the thermal phase transition with Wilson quarks"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-lat/9310023","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:d268c7149c2473e6535647de1f599150f30484e586932eeebc2bd685efc1b90b","target":"record","created_at":"2026-07-04T15:50:28Z","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":"1d11895c0e8ac63f74414cbfe7c170d4b223b0337393a5cb09537c8cda8f297d","cross_cats_sorted":[],"license":"","primary_cat":"hep-lat","submitted_at":"1993-10-21T19:01:08Z","title_canon_sha256":"d61f5b583b46f4452eac1aa9e7e96d6755e56a2249131fdee8b301cc61376d69"},"schema_version":"1.0","source":{"id":"hep-lat/9310023","kind":"arxiv","version":1}},"canonical_sha256":"5ed872c6c116e583dd437dd2fccc70a91327436ff4ba88bc1e73002707d47c45","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"5ed872c6c116e583dd437dd2fccc70a91327436ff4ba88bc1e73002707d47c45","first_computed_at":"2026-07-04T15:50:28.267051Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:50:28.267051Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"CrxOZInhv7f0q/6yRmt0HWUrAdE5advfBliC022A+5Au5nb+O8J968RE3C7O8pwUj8gMzIWfZwNZq0hhtz4ICg==","signature_status":"signed_v1","signed_at":"2026-07-04T15:50:28.267517Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-lat/9310023","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d268c7149c2473e6535647de1f599150f30484e586932eeebc2bd685efc1b90b","sha256:8b40013690bf17d5a6b6a66e6ef896c280e2f1285f5b55f02dc8b94b1fbd05ca"],"state_sha256":"f53338af05bba21f32831672ef6002d29f67e8a0e9349a45b2edd12663686e24"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"f81WbhdmMzCwlajrq4Zvsr2jpXma3QbF+2FKs3KruZDwQI/dcZT12OYe7gIzF+bT4pyKIHvss2LNLJAlZeDpCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-07T07:10:20.305504Z","bundle_sha256":"30f0c043fce34413ae4f835bd6afd78ae775777da7736b851ea48760a9ed2a6b"}}