{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:HREXVU2AJ2KNTLBLLXYGE2DDOG","short_pith_number":"pith:HREXVU2A","canonical_record":{"source":{"id":"hep-th/9506191","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1995-06-29T11:35:45Z","cross_cats_sorted":[],"title_canon_sha256":"5079d00794901a75e5c17e92c92e3b518f5a5301bd4cb721ea47db822463f0c0","abstract_canon_sha256":"9acc6a6e2ed9a0235cb6e570cf4cbba0f18677ef9949dde47dbe0c30004be4b8"},"schema_version":"1.0"},"canonical_sha256":"3c497ad3404e94d9ac2b5df062686371a3fcb9a2286149ddf657a421c599e0b3","source":{"kind":"arxiv","id":"hep-th/9506191","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9506191","created_at":"2026-07-05T03:59:11Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9506191v1","created_at":"2026-07-05T03:59:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9506191","created_at":"2026-07-05T03:59:11Z"},{"alias_kind":"pith_short_12","alias_value":"HREXVU2AJ2KN","created_at":"2026-07-05T03:59:11Z"},{"alias_kind":"pith_short_16","alias_value":"HREXVU2AJ2KNTLBL","created_at":"2026-07-05T03:59:11Z"},{"alias_kind":"pith_short_8","alias_value":"HREXVU2A","created_at":"2026-07-05T03:59:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:HREXVU2AJ2KNTLBLLXYGE2DDOG","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/9506191","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1995-06-29T11:35:45Z","cross_cats_sorted":[],"title_canon_sha256":"5079d00794901a75e5c17e92c92e3b518f5a5301bd4cb721ea47db822463f0c0","abstract_canon_sha256":"9acc6a6e2ed9a0235cb6e570cf4cbba0f18677ef9949dde47dbe0c30004be4b8"},"schema_version":"1.0"},"canonical_sha256":"3c497ad3404e94d9ac2b5df062686371a3fcb9a2286149ddf657a421c599e0b3","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:59:11.505695Z","signature_b64":"mYhM2AUDgxR0ToFNx1j4q3K4lO+QVcKYFEenALGyURTTmMalTeNPNxcUs6fct+wUphHnFaV4wV9HXNP8/8XhAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3c497ad3404e94d9ac2b5df062686371a3fcb9a2286149ddf657a421c599e0b3","last_reissued_at":"2026-07-05T03:59:11.505238Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:59:11.505238Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/9506191","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":"2026-07-05T03:59:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"8c0Nt9b3sq/PzJp4hujm4Hgz6rw36UnP8VnWygot2N2vuqzpJeNzRL6xYh0gVpt46ZfXcWCWytMjCeQekA3FBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T10:30:15.339669Z"},"content_sha256":"e2b1add92d0f01b1410177fc23fcb4a7158fb695fba8a100bcf109b3b53fcbc9","schema_version":"1.0","event_id":"sha256:e2b1add92d0f01b1410177fc23fcb4a7158fb695fba8a100bcf109b3b53fcbc9"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:HREXVU2AJ2KNTLBLLXYGE2DDOG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Renormalized finite temperature effective potential of $SU(2)$ Yang-Mills theory","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"K. Sailer, W. Greiner","submitted_at":"1995-06-29T11:35:45Z","abstract_excerpt":"It is shown that the renormalized finite temperature effective potential for continuum $SU(2)$ Yang-Mills theory develops a non-perturbative minimum for sufficiently strong coupling, i.e. below a critical temperature. The corresponding phase can be the candidate for the confining phase of the continuum theory and becomes energetically favoured basicly due to the decay of the $A^0$ condensate into three gluons."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9506191","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-th/9506191/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":"2026-07-05T03:59:11Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"GpzIgqBG3X+fwKhK4e6yjfQbQVSIJ8r4RB1c7YFxpvRgrkvfj+09FM/hUTkops1HHk94dq3vvV9sKPz7SoznAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-05T10:30:15.340168Z"},"content_sha256":"e88e94e580848038869ce52811220d4edc46020b919f131d33ace0796c257a2c","schema_version":"1.0","event_id":"sha256:e88e94e580848038869ce52811220d4edc46020b919f131d33ace0796c257a2c"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/HREXVU2AJ2KNTLBLLXYGE2DDOG/bundle.json","state_url":"https://pith.science/pith/HREXVU2AJ2KNTLBLLXYGE2DDOG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/HREXVU2AJ2KNTLBLLXYGE2DDOG/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":"2026-08-05T10:30:15Z","links":{"resolver":"https://pith.science/pith/HREXVU2AJ2KNTLBLLXYGE2DDOG","bundle":"https://pith.science/pith/HREXVU2AJ2KNTLBLLXYGE2DDOG/bundle.json","state":"https://pith.science/pith/HREXVU2AJ2KNTLBLLXYGE2DDOG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/HREXVU2AJ2KNTLBLLXYGE2DDOG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:HREXVU2AJ2KNTLBLLXYGE2DDOG","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":"9acc6a6e2ed9a0235cb6e570cf4cbba0f18677ef9949dde47dbe0c30004be4b8","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1995-06-29T11:35:45Z","title_canon_sha256":"5079d00794901a75e5c17e92c92e3b518f5a5301bd4cb721ea47db822463f0c0"},"schema_version":"1.0","source":{"id":"hep-th/9506191","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/9506191","created_at":"2026-07-05T03:59:11Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9506191v1","created_at":"2026-07-05T03:59:11Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9506191","created_at":"2026-07-05T03:59:11Z"},{"alias_kind":"pith_short_12","alias_value":"HREXVU2AJ2KN","created_at":"2026-07-05T03:59:11Z"},{"alias_kind":"pith_short_16","alias_value":"HREXVU2AJ2KNTLBL","created_at":"2026-07-05T03:59:11Z"},{"alias_kind":"pith_short_8","alias_value":"HREXVU2A","created_at":"2026-07-05T03:59:11Z"}],"graph_snapshots":[{"event_id":"sha256:e88e94e580848038869ce52811220d4edc46020b919f131d33ace0796c257a2c","target":"graph","created_at":"2026-07-05T03:59:11Z","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-th/9506191/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"It is shown that the renormalized finite temperature effective potential for continuum $SU(2)$ Yang-Mills theory develops a non-perturbative minimum for sufficiently strong coupling, i.e. below a critical temperature. The corresponding phase can be the candidate for the confining phase of the continuum theory and becomes energetically favoured basicly due to the decay of the $A^0$ condensate into three gluons.","authors_text":"K. Sailer, W. Greiner","cross_cats":[],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"1995-06-29T11:35:45Z","title":"Renormalized finite temperature effective potential of $SU(2)$ Yang-Mills theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9506191","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:e2b1add92d0f01b1410177fc23fcb4a7158fb695fba8a100bcf109b3b53fcbc9","target":"record","created_at":"2026-07-05T03:59:11Z","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":"9acc6a6e2ed9a0235cb6e570cf4cbba0f18677ef9949dde47dbe0c30004be4b8","cross_cats_sorted":[],"license":"","primary_cat":"hep-th","submitted_at":"1995-06-29T11:35:45Z","title_canon_sha256":"5079d00794901a75e5c17e92c92e3b518f5a5301bd4cb721ea47db822463f0c0"},"schema_version":"1.0","source":{"id":"hep-th/9506191","kind":"arxiv","version":1}},"canonical_sha256":"3c497ad3404e94d9ac2b5df062686371a3fcb9a2286149ddf657a421c599e0b3","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"3c497ad3404e94d9ac2b5df062686371a3fcb9a2286149ddf657a421c599e0b3","first_computed_at":"2026-07-05T03:59:11.505238Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:59:11.505238Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"mYhM2AUDgxR0ToFNx1j4q3K4lO+QVcKYFEenALGyURTTmMalTeNPNxcUs6fct+wUphHnFaV4wV9HXNP8/8XhAg==","signature_status":"signed_v1","signed_at":"2026-07-05T03:59:11.505695Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/9506191","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e2b1add92d0f01b1410177fc23fcb4a7158fb695fba8a100bcf109b3b53fcbc9","sha256:e88e94e580848038869ce52811220d4edc46020b919f131d33ace0796c257a2c"],"state_sha256":"94bcae45ddf6a2ba9a517141ce746b8ab0c7a36ee19361344ecc9499ab969bee"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ttMdiWcUn8QYB0AOcCUdCtL8s9aiwgqN/kgm7BmGLJiXRbQNEPKmx5vTLH2345OjFlOsgBp9i1DksRa2Evo2BQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-05T10:30:15.343922Z","bundle_sha256":"97edca4cd310cf4b2ad3d0427faebe8f4e28ca469d8e710af83d8b2b412e8330"}}