{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1997:6L5CRFHDCAP6I77XPFAZO5RM26","short_pith_number":"pith:6L5CRFHD","canonical_record":{"source":{"id":"hep-ph/9704416","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-04-28T09:37:13Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"4dc2a35ad111b234bb684031c411c8028747f521d6cc290f58f80d70eac9d378","abstract_canon_sha256":"4fc5cc1f17f07fe5b1bd49baf27de46eb5eb0baa491e294fe2fa99c16c2e832b"},"schema_version":"1.0"},"canonical_sha256":"f2fa2894e3101fe47ff7794197762cd79d6963f14e80fb23dc86eeff51628c09","source":{"kind":"arxiv","id":"hep-ph/9704416","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9704416","created_at":"2026-07-04T16:04:56Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9704416v1","created_at":"2026-07-04T16:04:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9704416","created_at":"2026-07-04T16:04:56Z"},{"alias_kind":"pith_short_12","alias_value":"6L5CRFHDCAP6","created_at":"2026-07-04T16:04:56Z"},{"alias_kind":"pith_short_16","alias_value":"6L5CRFHDCAP6I77X","created_at":"2026-07-04T16:04:56Z"},{"alias_kind":"pith_short_8","alias_value":"6L5CRFHD","created_at":"2026-07-04T16:04:56Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1997:6L5CRFHDCAP6I77XPFAZO5RM26","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/9704416","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-04-28T09:37:13Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"4dc2a35ad111b234bb684031c411c8028747f521d6cc290f58f80d70eac9d378","abstract_canon_sha256":"4fc5cc1f17f07fe5b1bd49baf27de46eb5eb0baa491e294fe2fa99c16c2e832b"},"schema_version":"1.0"},"canonical_sha256":"f2fa2894e3101fe47ff7794197762cd79d6963f14e80fb23dc86eeff51628c09","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:04:56.707942Z","signature_b64":"hnOTqbDW59zb/3yfsbdJXIIYtmfzpmh82kLi5rR3u9WZT4nCJSCaYxvByoE6yJL1r0BadXItHzC+KX+TIAFdBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f2fa2894e3101fe47ff7794197762cd79d6963f14e80fb23dc86eeff51628c09","last_reissued_at":"2026-07-04T16:04:56.707490Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:04:56.707490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/9704416","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":"2026-07-04T16:04:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"aged0kByEjgAEvibNpjggJSAO+HxJkCGC4edOkEXTWpRPDfkzZhyPDjllANGv4E0k4GjdZgTcILUBR8cd6hpAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T09:42:33.834110Z"},"content_sha256":"a1fc3536b107155499feeb7ef1b5495654744bfb2c761f54e0722d6fec4a4443","schema_version":"1.0","event_id":"sha256:a1fc3536b107155499feeb7ef1b5495654744bfb2c761f54e0722d6fec4a4443"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1997:6L5CRFHDCAP6I77XPFAZO5RM26","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"3d SU(N) + adjoint Higgs theory and finite temperature QCD","license":"","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"K. Kajantie, K. Rummukainen, M. Laine, M. Shaposhnikov","submitted_at":"1997-04-28T09:37:13Z","abstract_excerpt":"We study to what extent the three-dimensional SU(N)+adjoint Higgs theory can be used as an effective theory for finite temperature SU(N) gauge theory, with N=2,3. The parameters of the 3d theory are computed in 2-loop perturbation theory in terms of T/Lambda_MSbar,N,N_f. The perturbative effective potential of the 3d theory is computed to two loops for N=2. While the Z(N) symmetry probably driving the 4d confinement-deconfinement phase transition (for N_f=0) is not explicit in the effective Lagrangian, it is partly reinstated by radiative effects in the 3d theory. Lattice simulations in the 3d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9704416","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-ph/9704416/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":"2026-07-04T16:04:56Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QyWH3oWWgV1LK3HTyUDGajURJ96zW39XvjOlAfeCUd+zq/9iAOkUpf5TzBHUEjuhYrWdalT664avYJRmUhSOAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T09:42:33.834501Z"},"content_sha256":"12e18176ac841eeac7ab0cd91294b587d54b6501488c963f483e787ad44d7b62","schema_version":"1.0","event_id":"sha256:12e18176ac841eeac7ab0cd91294b587d54b6501488c963f483e787ad44d7b62"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/6L5CRFHDCAP6I77XPFAZO5RM26/bundle.json","state_url":"https://pith.science/pith/6L5CRFHDCAP6I77XPFAZO5RM26/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/6L5CRFHDCAP6I77XPFAZO5RM26/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":"2026-08-04T09:42:33Z","links":{"resolver":"https://pith.science/pith/6L5CRFHDCAP6I77XPFAZO5RM26","bundle":"https://pith.science/pith/6L5CRFHDCAP6I77XPFAZO5RM26/bundle.json","state":"https://pith.science/pith/6L5CRFHDCAP6I77XPFAZO5RM26/state.json","well_known_bundle":"https://pith.science/.well-known/pith/6L5CRFHDCAP6I77XPFAZO5RM26/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1997:6L5CRFHDCAP6I77XPFAZO5RM26","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":"4fc5cc1f17f07fe5b1bd49baf27de46eb5eb0baa491e294fe2fa99c16c2e832b","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"hep-ph","submitted_at":"1997-04-28T09:37:13Z","title_canon_sha256":"4dc2a35ad111b234bb684031c411c8028747f521d6cc290f58f80d70eac9d378"},"schema_version":"1.0","source":{"id":"hep-ph/9704416","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/9704416","created_at":"2026-07-04T16:04:56Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9704416v1","created_at":"2026-07-04T16:04:56Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9704416","created_at":"2026-07-04T16:04:56Z"},{"alias_kind":"pith_short_12","alias_value":"6L5CRFHDCAP6","created_at":"2026-07-04T16:04:56Z"},{"alias_kind":"pith_short_16","alias_value":"6L5CRFHDCAP6I77X","created_at":"2026-07-04T16:04:56Z"},{"alias_kind":"pith_short_8","alias_value":"6L5CRFHD","created_at":"2026-07-04T16:04:56Z"}],"graph_snapshots":[{"event_id":"sha256:12e18176ac841eeac7ab0cd91294b587d54b6501488c963f483e787ad44d7b62","target":"graph","created_at":"2026-07-04T16:04:56Z","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-ph/9704416/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study to what extent the three-dimensional SU(N)+adjoint Higgs theory can be used as an effective theory for finite temperature SU(N) gauge theory, with N=2,3. The parameters of the 3d theory are computed in 2-loop perturbation theory in terms of T/Lambda_MSbar,N,N_f. The perturbative effective potential of the 3d theory is computed to two loops for N=2. While the Z(N) symmetry probably driving the 4d confinement-deconfinement phase transition (for N_f=0) is not explicit in the effective Lagrangian, it is partly reinstated by radiative effects in the 3d theory. Lattice simulations in the 3d","authors_text":"K. Kajantie, K. Rummukainen, M. Laine, M. Shaposhnikov","cross_cats":["hep-lat"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"1997-04-28T09:37:13Z","title":"3d SU(N) + adjoint Higgs theory and finite temperature QCD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9704416","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:a1fc3536b107155499feeb7ef1b5495654744bfb2c761f54e0722d6fec4a4443","target":"record","created_at":"2026-07-04T16:04:56Z","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":"4fc5cc1f17f07fe5b1bd49baf27de46eb5eb0baa491e294fe2fa99c16c2e832b","cross_cats_sorted":["hep-lat"],"license":"","primary_cat":"hep-ph","submitted_at":"1997-04-28T09:37:13Z","title_canon_sha256":"4dc2a35ad111b234bb684031c411c8028747f521d6cc290f58f80d70eac9d378"},"schema_version":"1.0","source":{"id":"hep-ph/9704416","kind":"arxiv","version":1}},"canonical_sha256":"f2fa2894e3101fe47ff7794197762cd79d6963f14e80fb23dc86eeff51628c09","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f2fa2894e3101fe47ff7794197762cd79d6963f14e80fb23dc86eeff51628c09","first_computed_at":"2026-07-04T16:04:56.707490Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:04:56.707490Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"hnOTqbDW59zb/3yfsbdJXIIYtmfzpmh82kLi5rR3u9WZT4nCJSCaYxvByoE6yJL1r0BadXItHzC+KX+TIAFdBA==","signature_status":"signed_v1","signed_at":"2026-07-04T16:04:56.707942Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/9704416","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a1fc3536b107155499feeb7ef1b5495654744bfb2c761f54e0722d6fec4a4443","sha256:12e18176ac841eeac7ab0cd91294b587d54b6501488c963f483e787ad44d7b62"],"state_sha256":"67dbca4e0b862d49913a08012b9d54ee366c020c5aaded3923dd8d038b0b6054"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"V0Zo004ADH381WnpEtopvWVKg0om7NrFNR63QRADPddYztJaIf04rqR2NA0gQxtwy3VH1tHDTmkJIVSlI01DBQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T09:42:33.837202Z","bundle_sha256":"55d0672216b84cfbb2dcd1bb9bb1becdffa3002a520b13079bb782e343ff85b4"}}