{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:4WC4CQHIUUY2DBQRTWK43WCHVJ","short_pith_number":"pith:4WC4CQHI","canonical_record":{"source":{"id":"1205.0290","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-05-01T23:52:15Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"24d5df83ded14dfb572067959388a7c5e049ac8ef360f818031cc31fc8ed62c2","abstract_canon_sha256":"38b8c3360030a10fdf0bdd6040342a171a61cf4586a3bddf057fe756f3ce746a"},"schema_version":"1.0"},"canonical_sha256":"e585c140e8a531a186119d95cdd847aa6623b461ae12fff6b8ec995442e1e8d5","source":{"kind":"arxiv","id":"1205.0290","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1205.0290","created_at":"2026-05-18T01:57:39Z"},{"alias_kind":"arxiv_version","alias_value":"1205.0290v2","created_at":"2026-05-18T01:57:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.0290","created_at":"2026-05-18T01:57:39Z"},{"alias_kind":"pith_short_12","alias_value":"4WC4CQHIUUY2","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"4WC4CQHIUUY2DBQR","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"4WC4CQHI","created_at":"2026-05-18T12:26:53Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:4WC4CQHIUUY2DBQRTWK43WCHVJ","target":"record","payload":{"canonical_record":{"source":{"id":"1205.0290","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-05-01T23:52:15Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"24d5df83ded14dfb572067959388a7c5e049ac8ef360f818031cc31fc8ed62c2","abstract_canon_sha256":"38b8c3360030a10fdf0bdd6040342a171a61cf4586a3bddf057fe756f3ce746a"},"schema_version":"1.0"},"canonical_sha256":"e585c140e8a531a186119d95cdd847aa6623b461ae12fff6b8ec995442e1e8d5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:57:39.188904Z","signature_b64":"JfagPVeE6VCQbmmgfVAvmLQ0ZZjZuGKFGLufdjIbElhjRr3+n0ajtRItdWNxGeGRAmQ9HZa565wr8/pcjWReCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e585c140e8a531a186119d95cdd847aa6623b461ae12fff6b8ec995442e1e8d5","last_reissued_at":"2026-05-18T01:57:39.188277Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:57:39.188277Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1205.0290","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":"2026-05-18T01:57:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lC1+Y4/DCHdatWcu1HDd2Yrk6bWvkA1ydm9S8OM+L8Tye29NnER0zTUXYmgB1AbPQ7AuEL33qeCGisEEpDDfCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T19:14:35.217431Z"},"content_sha256":"5e4a32c6098f81fe66f4a79e3bb42a9dc1c5ee450d52caf4ef79f3938dd8cb3b","schema_version":"1.0","event_id":"sha256:5e4a32c6098f81fe66f4a79e3bb42a9dc1c5ee450d52caf4ef79f3938dd8cb3b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:4WC4CQHIUUY2DBQRTWK43WCHVJ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Continuity, Deconfinement, and (Super) Yang-Mills Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Erich Poppitz, Mithat Unsal, Thomas Schaefer","submitted_at":"2012-05-01T23:52:15Z","abstract_excerpt":"We study the phase diagram of SU(2) Yang-Mills theory with one adjoint Weyl fermion on R^3xS^1 as a function of the fermion mass m and the compactification scale L. This theory reduces to thermal pure gauge theory as m->infinity and to circle-compactified (non-thermal) supersymmetric gluodynamics in the limit m->0. In the m-L plane, there is a line of center symmetry changing phase transitions. In the limit m->infinity, this transition takes place at L_c=1/T_c, where T_c is the critical temperature of the deconfinement transition in pure Yang-Mills theory. We show that near m=0, the critical c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.0290","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":""},"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":"2026-05-18T01:57:39Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"KIkCoF98u+x2/J61fcs6bpX+v1X2AuwSbU0lzxijHW0/Gv4ZAhSd8MkqpaHwufN44ZRnkv6nCOiv9qfBZ1AECA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T19:14:35.218140Z"},"content_sha256":"7e31160a8e1d997d7eef432d638a37faf01e5e1feed1f49a858581068f081556","schema_version":"1.0","event_id":"sha256:7e31160a8e1d997d7eef432d638a37faf01e5e1feed1f49a858581068f081556"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4WC4CQHIUUY2DBQRTWK43WCHVJ/bundle.json","state_url":"https://pith.science/pith/4WC4CQHIUUY2DBQRTWK43WCHVJ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4WC4CQHIUUY2DBQRTWK43WCHVJ/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":"2026-05-23T19:14:35Z","links":{"resolver":"https://pith.science/pith/4WC4CQHIUUY2DBQRTWK43WCHVJ","bundle":"https://pith.science/pith/4WC4CQHIUUY2DBQRTWK43WCHVJ/bundle.json","state":"https://pith.science/pith/4WC4CQHIUUY2DBQRTWK43WCHVJ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4WC4CQHIUUY2DBQRTWK43WCHVJ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:4WC4CQHIUUY2DBQRTWK43WCHVJ","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":"38b8c3360030a10fdf0bdd6040342a171a61cf4586a3bddf057fe756f3ce746a","cross_cats_sorted":["hep-lat","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-05-01T23:52:15Z","title_canon_sha256":"24d5df83ded14dfb572067959388a7c5e049ac8ef360f818031cc31fc8ed62c2"},"schema_version":"1.0","source":{"id":"1205.0290","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1205.0290","created_at":"2026-05-18T01:57:39Z"},{"alias_kind":"arxiv_version","alias_value":"1205.0290v2","created_at":"2026-05-18T01:57:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1205.0290","created_at":"2026-05-18T01:57:39Z"},{"alias_kind":"pith_short_12","alias_value":"4WC4CQHIUUY2","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_16","alias_value":"4WC4CQHIUUY2DBQR","created_at":"2026-05-18T12:26:53Z"},{"alias_kind":"pith_short_8","alias_value":"4WC4CQHI","created_at":"2026-05-18T12:26:53Z"}],"graph_snapshots":[{"event_id":"sha256:7e31160a8e1d997d7eef432d638a37faf01e5e1feed1f49a858581068f081556","target":"graph","created_at":"2026-05-18T01:57:39Z","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":"We study the phase diagram of SU(2) Yang-Mills theory with one adjoint Weyl fermion on R^3xS^1 as a function of the fermion mass m and the compactification scale L. This theory reduces to thermal pure gauge theory as m->infinity and to circle-compactified (non-thermal) supersymmetric gluodynamics in the limit m->0. In the m-L plane, there is a line of center symmetry changing phase transitions. In the limit m->infinity, this transition takes place at L_c=1/T_c, where T_c is the critical temperature of the deconfinement transition in pure Yang-Mills theory. We show that near m=0, the critical c","authors_text":"Erich Poppitz, Mithat Unsal, Thomas Schaefer","cross_cats":["hep-lat","hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-05-01T23:52:15Z","title":"Continuity, Deconfinement, and (Super) Yang-Mills Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1205.0290","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":"sha256:5e4a32c6098f81fe66f4a79e3bb42a9dc1c5ee450d52caf4ef79f3938dd8cb3b","target":"record","created_at":"2026-05-18T01:57:39Z","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":"38b8c3360030a10fdf0bdd6040342a171a61cf4586a3bddf057fe756f3ce746a","cross_cats_sorted":["hep-lat","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-05-01T23:52:15Z","title_canon_sha256":"24d5df83ded14dfb572067959388a7c5e049ac8ef360f818031cc31fc8ed62c2"},"schema_version":"1.0","source":{"id":"1205.0290","kind":"arxiv","version":2}},"canonical_sha256":"e585c140e8a531a186119d95cdd847aa6623b461ae12fff6b8ec995442e1e8d5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e585c140e8a531a186119d95cdd847aa6623b461ae12fff6b8ec995442e1e8d5","first_computed_at":"2026-05-18T01:57:39.188277Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:57:39.188277Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"JfagPVeE6VCQbmmgfVAvmLQ0ZZjZuGKFGLufdjIbElhjRr3+n0ajtRItdWNxGeGRAmQ9HZa565wr8/pcjWReCA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:57:39.188904Z","signed_message":"canonical_sha256_bytes"},"source_id":"1205.0290","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5e4a32c6098f81fe66f4a79e3bb42a9dc1c5ee450d52caf4ef79f3938dd8cb3b","sha256:7e31160a8e1d997d7eef432d638a37faf01e5e1feed1f49a858581068f081556"],"state_sha256":"6480dc7e9025b99a375906a28774ca39a161d34a800bcc8dfaf750ed826d64e7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tny9pHHHDmQvrMhwU9hQc0ABX0sKX30xEjDhi1YMVaUGNdHgf6m37y2tSJha2CEGIu3+WHWk9GLJYtO4ZiE6DA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-23T19:14:35.221941Z","bundle_sha256":"b3787782d23c9948d77bb726f05f4b683a1ca82b15cbf3759ecf9c5d849e7c95"}}