{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:N7PEWE2OL4JDUUCVZYCFEFROIM","short_pith_number":"pith:N7PEWE2O","canonical_record":{"source":{"id":"1111.6101","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-11-25T20:52:10Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"7847dbbf67a9ee8e7248b6b540a2b5634d93cd21074346d6f32f90e048e9697c","abstract_canon_sha256":"c9b21a21e2f7f5df2e57fcad73737c80f6cb0dfc768d27bacf00c4cfc362ad76"},"schema_version":"1.0"},"canonical_sha256":"6fde4b134e5f123a5055ce0452162e4330b261bb11ede95692bc7658231b3341","source":{"kind":"arxiv","id":"1111.6101","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1111.6101","created_at":"2026-05-18T03:53:17Z"},{"alias_kind":"arxiv_version","alias_value":"1111.6101v2","created_at":"2026-05-18T03:53:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.6101","created_at":"2026-05-18T03:53:17Z"},{"alias_kind":"pith_short_12","alias_value":"N7PEWE2OL4JD","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_16","alias_value":"N7PEWE2OL4JDUUCV","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_8","alias_value":"N7PEWE2O","created_at":"2026-05-18T12:26:37Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:N7PEWE2OL4JDUUCVZYCFEFROIM","target":"record","payload":{"canonical_record":{"source":{"id":"1111.6101","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-11-25T20:52:10Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"7847dbbf67a9ee8e7248b6b540a2b5634d93cd21074346d6f32f90e048e9697c","abstract_canon_sha256":"c9b21a21e2f7f5df2e57fcad73737c80f6cb0dfc768d27bacf00c4cfc362ad76"},"schema_version":"1.0"},"canonical_sha256":"6fde4b134e5f123a5055ce0452162e4330b261bb11ede95692bc7658231b3341","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:53:17.481937Z","signature_b64":"+3TXb1e79WzTYExdyvhOJVrOKPUV5ldDKX+jfX5nD/DAPn6fTzD6t4w31BTI/jfdY2Bgyvg+HtuNfQUgotxCDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6fde4b134e5f123a5055ce0452162e4330b261bb11ede95692bc7658231b3341","last_reissued_at":"2026-05-18T03:53:17.481189Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:53:17.481189Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1111.6101","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":"2026-05-18T03:53:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"JnEtfSBZbhVleKknoHIkFtMSoWW25zhunTxhg3FvuM0w15BSe7//DV/by6xKHNtovQ0sFwKDthOAMvYS4cz7Dg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T00:15:07.011552Z"},"content_sha256":"4befe80529e90f50b5e5a7cfded8b830a5f26ac19bce5f877ad9d53b05ff7a8e","schema_version":"1.0","event_id":"sha256:4befe80529e90f50b5e5a7cfded8b830a5f26ac19bce5f877ad9d53b05ff7a8e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:N7PEWE2OL4JDUUCVZYCFEFROIM","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Confinement in a Higgs Model on $R^{3}\\times S^{1}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Hiromichi Nishimura, Michael C. Ogilvie","submitted_at":"2011-11-25T20:52:10Z","abstract_excerpt":"We determine the phase structure of an SU(2) gauge theory with an adjoint scalar on $R^{3}\\times S^{1}$ using semiclassical methods. There are two global symmetries: a $Z(2)_{H}$ symmetry associated with the Higgs field and a $Z(2)_{C}$ center symmetry. We analyze the order of the deconfining phase transition when different deformation terms are used. After finding order parameters for the global symmetries, we show that there are four distinct phases: a deconfined phase, a confined phase, a Higgs phase, and a mixed confined phase. The mixed confined phase occurs where one might expect a phase"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.6101","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":"2026-05-18T03:53:17Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"gKHza4cc12v1L7FcsfTPoeOD0ilQwUvXEjyEjkNcUsQJbagfTDiC6FHpaByn9j7QX80aIK4s0w+i8hAzKj5rCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T00:15:07.012209Z"},"content_sha256":"fd7c4354de40346426b6ecc56aa46ff5637acbd10648ea7048a0a1801c0a4ecb","schema_version":"1.0","event_id":"sha256:fd7c4354de40346426b6ecc56aa46ff5637acbd10648ea7048a0a1801c0a4ecb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/N7PEWE2OL4JDUUCVZYCFEFROIM/bundle.json","state_url":"https://pith.science/pith/N7PEWE2OL4JDUUCVZYCFEFROIM/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/N7PEWE2OL4JDUUCVZYCFEFROIM/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":"2026-06-01T00:15:07Z","links":{"resolver":"https://pith.science/pith/N7PEWE2OL4JDUUCVZYCFEFROIM","bundle":"https://pith.science/pith/N7PEWE2OL4JDUUCVZYCFEFROIM/bundle.json","state":"https://pith.science/pith/N7PEWE2OL4JDUUCVZYCFEFROIM/state.json","well_known_bundle":"https://pith.science/.well-known/pith/N7PEWE2OL4JDUUCVZYCFEFROIM/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:N7PEWE2OL4JDUUCVZYCFEFROIM","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":"c9b21a21e2f7f5df2e57fcad73737c80f6cb0dfc768d27bacf00c4cfc362ad76","cross_cats_sorted":["hep-lat","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-11-25T20:52:10Z","title_canon_sha256":"7847dbbf67a9ee8e7248b6b540a2b5634d93cd21074346d6f32f90e048e9697c"},"schema_version":"1.0","source":{"id":"1111.6101","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1111.6101","created_at":"2026-05-18T03:53:17Z"},{"alias_kind":"arxiv_version","alias_value":"1111.6101v2","created_at":"2026-05-18T03:53:17Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1111.6101","created_at":"2026-05-18T03:53:17Z"},{"alias_kind":"pith_short_12","alias_value":"N7PEWE2OL4JD","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_16","alias_value":"N7PEWE2OL4JDUUCV","created_at":"2026-05-18T12:26:37Z"},{"alias_kind":"pith_short_8","alias_value":"N7PEWE2O","created_at":"2026-05-18T12:26:37Z"}],"graph_snapshots":[{"event_id":"sha256:fd7c4354de40346426b6ecc56aa46ff5637acbd10648ea7048a0a1801c0a4ecb","target":"graph","created_at":"2026-05-18T03:53:17Z","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 determine the phase structure of an SU(2) gauge theory with an adjoint scalar on $R^{3}\\times S^{1}$ using semiclassical methods. There are two global symmetries: a $Z(2)_{H}$ symmetry associated with the Higgs field and a $Z(2)_{C}$ center symmetry. We analyze the order of the deconfining phase transition when different deformation terms are used. After finding order parameters for the global symmetries, we show that there are four distinct phases: a deconfined phase, a confined phase, a Higgs phase, and a mixed confined phase. The mixed confined phase occurs where one might expect a phase","authors_text":"Hiromichi Nishimura, Michael C. Ogilvie","cross_cats":["hep-lat","hep-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-11-25T20:52:10Z","title":"Confinement in a Higgs Model on $R^{3}\\times S^{1}$"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1111.6101","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":"sha256:4befe80529e90f50b5e5a7cfded8b830a5f26ac19bce5f877ad9d53b05ff7a8e","target":"record","created_at":"2026-05-18T03:53:17Z","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":"c9b21a21e2f7f5df2e57fcad73737c80f6cb0dfc768d27bacf00c4cfc362ad76","cross_cats_sorted":["hep-lat","hep-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2011-11-25T20:52:10Z","title_canon_sha256":"7847dbbf67a9ee8e7248b6b540a2b5634d93cd21074346d6f32f90e048e9697c"},"schema_version":"1.0","source":{"id":"1111.6101","kind":"arxiv","version":2}},"canonical_sha256":"6fde4b134e5f123a5055ce0452162e4330b261bb11ede95692bc7658231b3341","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6fde4b134e5f123a5055ce0452162e4330b261bb11ede95692bc7658231b3341","first_computed_at":"2026-05-18T03:53:17.481189Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:53:17.481189Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"+3TXb1e79WzTYExdyvhOJVrOKPUV5ldDKX+jfX5nD/DAPn6fTzD6t4w31BTI/jfdY2Bgyvg+HtuNfQUgotxCDA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:53:17.481937Z","signed_message":"canonical_sha256_bytes"},"source_id":"1111.6101","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4befe80529e90f50b5e5a7cfded8b830a5f26ac19bce5f877ad9d53b05ff7a8e","sha256:fd7c4354de40346426b6ecc56aa46ff5637acbd10648ea7048a0a1801c0a4ecb"],"state_sha256":"9e1839d70dfa3f5aab2e3c40b81b8254f06a2d8d4b2d392f92e84553490af7bb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"NBAI9KwhBbc8Zkc+P5nBmksimvTQoOj+vhQs/GvGmEjd0PQXInNuOhhhjbx8CSvdCElJmHckqgGP02abPqp4BQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T00:15:07.015151Z","bundle_sha256":"4bd3f010190d866c0920334751ade1a4d7817934eb0c4750ef75475f94fe9bb3"}}