{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:2JJPQN3WXY7KDPOIUCNQV2V67R","short_pith_number":"pith:2JJPQN3W","canonical_record":{"source":{"id":"1403.2265","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-10T15:23:41Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"2e8f9d73ccfb3547f9ce18168086e82922cb694f3159cc592ae8bc796a913c3d","abstract_canon_sha256":"008176fe4b48273eee4087169c64a2ac5b33f7e1949cb916c4b0b22b01073379"},"schema_version":"1.0"},"canonical_sha256":"d252f83776be3ea1bdc8a09b0aeabefc6c12718791860e24535a6855b87321be","source":{"kind":"arxiv","id":"1403.2265","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.2265","created_at":"2026-05-18T02:48:36Z"},{"alias_kind":"arxiv_version","alias_value":"1403.2265v2","created_at":"2026-05-18T02:48:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.2265","created_at":"2026-05-18T02:48:36Z"},{"alias_kind":"pith_short_12","alias_value":"2JJPQN3WXY7K","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"2JJPQN3WXY7KDPOI","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"2JJPQN3W","created_at":"2026-05-18T12:28:11Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:2JJPQN3WXY7KDPOIUCNQV2V67R","target":"record","payload":{"canonical_record":{"source":{"id":"1403.2265","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-10T15:23:41Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"2e8f9d73ccfb3547f9ce18168086e82922cb694f3159cc592ae8bc796a913c3d","abstract_canon_sha256":"008176fe4b48273eee4087169c64a2ac5b33f7e1949cb916c4b0b22b01073379"},"schema_version":"1.0"},"canonical_sha256":"d252f83776be3ea1bdc8a09b0aeabefc6c12718791860e24535a6855b87321be","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:48:36.695853Z","signature_b64":"rQUJDMeBkwZH8GVsQqkgOuNvsaqqCuDCOoBLeudfEMIDvByBBqeX3qz5ytibc2rDeSqFynB7dsHCFeMFNsJrAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d252f83776be3ea1bdc8a09b0aeabefc6c12718791860e24535a6855b87321be","last_reissued_at":"2026-05-18T02:48:36.695166Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:48:36.695166Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1403.2265","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":"2026-05-18T02:48:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"4kr0hHNXnqGUziRUUUDf4W0TVETG1gRocgMRg0z0XH8PObvJXNbhKm0bOUE3A/D7fPfmERNOafp/UFZzUuOTCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T01:32:08.859185Z"},"content_sha256":"7242fa2ebdeb63e2dcdbb2311aadc9e1be8bcb2c6105527c05e6797fd30e6158","schema_version":"1.0","event_id":"sha256:7242fa2ebdeb63e2dcdbb2311aadc9e1be8bcb2c6105527c05e6797fd30e6158"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:2JJPQN3WXY7KDPOIUCNQV2V67R","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Phase structure of $SU(3)$ gauge-Higgs unification models at finite temperature","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Kouji Kashiwa, Yuya Tanizaki","submitted_at":"2014-03-10T15:23:41Z","abstract_excerpt":"Five-dimensional $SU(3)$ gauge-Higgs unification models are studied at finite temperature in the warped extra dimension $S^1/\\mathbb{Z}_2$. In order to investigate the phase structure, we developed a technique to compute the one-loop effective potential with the nontrivial Polyakov loop phase and with the nontrivial Wilson line phase along the extra dimension. Effective potentials as functions of two gauge-field condensations are shown for several simple matter contents, including fundamental, sextet, and adjoint representational Dirac fermions. Possible extensions and applications of our form"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.2265","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":"2026-05-18T02:48:36Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"zKjyYaSp11q4mT0i7DXsPr7+ezeigcGTW8Vfj/DcIgl6Ug1IfWfJ9jrMXJgw/9PcOM9ZXqX7iLtdGW9Q5LdgAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T01:32:08.859561Z"},"content_sha256":"8df31bdd9f39932154372add5c8d1e0e9db6fc744cc4f72a634a7f2fda27c3d5","schema_version":"1.0","event_id":"sha256:8df31bdd9f39932154372add5c8d1e0e9db6fc744cc4f72a634a7f2fda27c3d5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/2JJPQN3WXY7KDPOIUCNQV2V67R/bundle.json","state_url":"https://pith.science/pith/2JJPQN3WXY7KDPOIUCNQV2V67R/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/2JJPQN3WXY7KDPOIUCNQV2V67R/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":"2026-06-04T01:32:08Z","links":{"resolver":"https://pith.science/pith/2JJPQN3WXY7KDPOIUCNQV2V67R","bundle":"https://pith.science/pith/2JJPQN3WXY7KDPOIUCNQV2V67R/bundle.json","state":"https://pith.science/pith/2JJPQN3WXY7KDPOIUCNQV2V67R/state.json","well_known_bundle":"https://pith.science/.well-known/pith/2JJPQN3WXY7KDPOIUCNQV2V67R/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:2JJPQN3WXY7KDPOIUCNQV2V67R","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":"008176fe4b48273eee4087169c64a2ac5b33f7e1949cb916c4b0b22b01073379","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-10T15:23:41Z","title_canon_sha256":"2e8f9d73ccfb3547f9ce18168086e82922cb694f3159cc592ae8bc796a913c3d"},"schema_version":"1.0","source":{"id":"1403.2265","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1403.2265","created_at":"2026-05-18T02:48:36Z"},{"alias_kind":"arxiv_version","alias_value":"1403.2265v2","created_at":"2026-05-18T02:48:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.2265","created_at":"2026-05-18T02:48:36Z"},{"alias_kind":"pith_short_12","alias_value":"2JJPQN3WXY7K","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_16","alias_value":"2JJPQN3WXY7KDPOI","created_at":"2026-05-18T12:28:11Z"},{"alias_kind":"pith_short_8","alias_value":"2JJPQN3W","created_at":"2026-05-18T12:28:11Z"}],"graph_snapshots":[{"event_id":"sha256:8df31bdd9f39932154372add5c8d1e0e9db6fc744cc4f72a634a7f2fda27c3d5","target":"graph","created_at":"2026-05-18T02:48:36Z","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":"Five-dimensional $SU(3)$ gauge-Higgs unification models are studied at finite temperature in the warped extra dimension $S^1/\\mathbb{Z}_2$. In order to investigate the phase structure, we developed a technique to compute the one-loop effective potential with the nontrivial Polyakov loop phase and with the nontrivial Wilson line phase along the extra dimension. Effective potentials as functions of two gauge-field condensations are shown for several simple matter contents, including fundamental, sextet, and adjoint representational Dirac fermions. Possible extensions and applications of our form","authors_text":"Kouji Kashiwa, Yuya Tanizaki","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-10T15:23:41Z","title":"Phase structure of $SU(3)$ gauge-Higgs unification models at finite temperature"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.2265","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":"sha256:7242fa2ebdeb63e2dcdbb2311aadc9e1be8bcb2c6105527c05e6797fd30e6158","target":"record","created_at":"2026-05-18T02:48:36Z","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":"008176fe4b48273eee4087169c64a2ac5b33f7e1949cb916c4b0b22b01073379","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-03-10T15:23:41Z","title_canon_sha256":"2e8f9d73ccfb3547f9ce18168086e82922cb694f3159cc592ae8bc796a913c3d"},"schema_version":"1.0","source":{"id":"1403.2265","kind":"arxiv","version":2}},"canonical_sha256":"d252f83776be3ea1bdc8a09b0aeabefc6c12718791860e24535a6855b87321be","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d252f83776be3ea1bdc8a09b0aeabefc6c12718791860e24535a6855b87321be","first_computed_at":"2026-05-18T02:48:36.695166Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:48:36.695166Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"rQUJDMeBkwZH8GVsQqkgOuNvsaqqCuDCOoBLeudfEMIDvByBBqeX3qz5ytibc2rDeSqFynB7dsHCFeMFNsJrAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:48:36.695853Z","signed_message":"canonical_sha256_bytes"},"source_id":"1403.2265","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7242fa2ebdeb63e2dcdbb2311aadc9e1be8bcb2c6105527c05e6797fd30e6158","sha256:8df31bdd9f39932154372add5c8d1e0e9db6fc744cc4f72a634a7f2fda27c3d5"],"state_sha256":"8e5975b2039417f4c691e580c293260319ca23080e4378f30add0968475433e1"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"XfBKmtYtwFZoJJ902nv85voq8qVJLNQJqoUXGn4xzfC5bsO9LXGJHT1r9OVDRfLJN9e/eiq+Iopm38JufIg/Bw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T01:32:08.861604Z","bundle_sha256":"d3a9ec56cf9421068b45d154f3044d3ab375b85deb01d39f4adebbd00aa48a67"}}