{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:1995:CM7OU6T7TDZSLIUP3KL7XYRHLA","short_pith_number":"pith:CM7OU6T7","canonical_record":{"source":{"id":"cond-mat/9502039","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1995-02-09T14:57:06Z","cross_cats_sorted":["hep-ph","supr-con"],"title_canon_sha256":"df7ebeaffa1ceaf9ee100645fc571e521cd29b2460423e2fec2ee328378f19dc","abstract_canon_sha256":"b2d6b02d86ecb8be97f9d9d6eb49871eb212f4e68fce7bfd4ef9f7ce65b9bb69"},"schema_version":"1.0"},"canonical_sha256":"133eea7a7f98f325a28fda97fbe22758083b5d6610c716ab8317d0239024ad95","source":{"kind":"arxiv","id":"cond-mat/9502039","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9502039","created_at":"2026-05-18T01:39:35Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9502039v1","created_at":"2026-05-18T01:39:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9502039","created_at":"2026-05-18T01:39:35Z"},{"alias_kind":"pith_short_12","alias_value":"CM7OU6T7TDZS","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"CM7OU6T7TDZSLIUP","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"CM7OU6T7","created_at":"2026-05-18T12:25:47Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:1995:CM7OU6T7TDZSLIUP3KL7XYRHLA","target":"record","payload":{"canonical_record":{"source":{"id":"cond-mat/9502039","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1995-02-09T14:57:06Z","cross_cats_sorted":["hep-ph","supr-con"],"title_canon_sha256":"df7ebeaffa1ceaf9ee100645fc571e521cd29b2460423e2fec2ee328378f19dc","abstract_canon_sha256":"b2d6b02d86ecb8be97f9d9d6eb49871eb212f4e68fce7bfd4ef9f7ce65b9bb69"},"schema_version":"1.0"},"canonical_sha256":"133eea7a7f98f325a28fda97fbe22758083b5d6610c716ab8317d0239024ad95","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:39:35.317302Z","signature_b64":"Fc5wIitwMvOwo5EGdZZ65kmcJBtk3a7gh78veythTj0uz2DX/4acmSuPsuxxhlBhoRIWMKs2XrPmN1zsvSmRAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"133eea7a7f98f325a28fda97fbe22758083b5d6610c716ab8317d0239024ad95","last_reissued_at":"2026-05-18T01:39:35.316786Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:39:35.316786Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"cond-mat/9502039","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":"2026-05-18T01:39:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"R3QR9SEVXSe0r9ZtlLusBCibfEZqh37qFflIdpYLC/lXxe+ZVueRNpODEpVzPZB0Zy1nGOSPmPgjwZZh8e+fDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T23:47:47.116205Z"},"content_sha256":"4af92fbe4272e883ccef2f6db7b6458f95ee33e1ef40296d00a1e8a18c1e7985","schema_version":"1.0","event_id":"sha256:4af92fbe4272e883ccef2f6db7b6458f95ee33e1ef40296d00a1e8a18c1e7985"},{"event_type":"graph_snapshot","subject_pith_number":"pith:1995:CM7OU6T7TDZSLIUP3KL7XYRHLA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"PHASE TRANSITION OF N-COMPONENT SUPERCONDUCTORS","license":"","headline":"","cross_cats":["hep-ph","supr-con"],"primary_cat":"cond-mat","authors_text":"B.Bergerhoff, C.Wetterich, D.Litim, S.Lola","submitted_at":"1995-02-09T14:57:06Z","abstract_excerpt":"We investigate the phase transition in the three-dimensional abelian Higgs model for N complex scalar fields, using the gauge-invariant average action \\Gamma_{k}. The dependence of \\Gamma_{k} on the effective infra-red cut-off k is described by a non-perturbative flow equation. The transition turns out to be first- or second-order, depending on the ratio between scalar and gauge coupling. We look at the fixed points of the theory for various N and compute the critical exponents of the model. Comparison with results from the \\epsilon-expansion shows a rather poor convergence for \\epsilon=1 even"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9502039","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":""},"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":"2026-05-18T01:39:35Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xETms0i5vZfpRa1lEkVh+jIao/n9W2XPDvvQtbzYc2zRk6mVO8uturbiugxgz6ELnTLq+hdyCxg23kEEEF2oBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T23:47:47.116589Z"},"content_sha256":"033b6a8976a19193cf12fd7b00cf46519fc9a4dbe99296226cb0341d7a743c93","schema_version":"1.0","event_id":"sha256:033b6a8976a19193cf12fd7b00cf46519fc9a4dbe99296226cb0341d7a743c93"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/CM7OU6T7TDZSLIUP3KL7XYRHLA/bundle.json","state_url":"https://pith.science/pith/CM7OU6T7TDZSLIUP3KL7XYRHLA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/CM7OU6T7TDZSLIUP3KL7XYRHLA/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":"2026-05-26T23:47:47Z","links":{"resolver":"https://pith.science/pith/CM7OU6T7TDZSLIUP3KL7XYRHLA","bundle":"https://pith.science/pith/CM7OU6T7TDZSLIUP3KL7XYRHLA/bundle.json","state":"https://pith.science/pith/CM7OU6T7TDZSLIUP3KL7XYRHLA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/CM7OU6T7TDZSLIUP3KL7XYRHLA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:1995:CM7OU6T7TDZSLIUP3KL7XYRHLA","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":"b2d6b02d86ecb8be97f9d9d6eb49871eb212f4e68fce7bfd4ef9f7ce65b9bb69","cross_cats_sorted":["hep-ph","supr-con"],"license":"","primary_cat":"cond-mat","submitted_at":"1995-02-09T14:57:06Z","title_canon_sha256":"df7ebeaffa1ceaf9ee100645fc571e521cd29b2460423e2fec2ee328378f19dc"},"schema_version":"1.0","source":{"id":"cond-mat/9502039","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"cond-mat/9502039","created_at":"2026-05-18T01:39:35Z"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9502039v1","created_at":"2026-05-18T01:39:35Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9502039","created_at":"2026-05-18T01:39:35Z"},{"alias_kind":"pith_short_12","alias_value":"CM7OU6T7TDZS","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_16","alias_value":"CM7OU6T7TDZSLIUP","created_at":"2026-05-18T12:25:47Z"},{"alias_kind":"pith_short_8","alias_value":"CM7OU6T7","created_at":"2026-05-18T12:25:47Z"}],"graph_snapshots":[{"event_id":"sha256:033b6a8976a19193cf12fd7b00cf46519fc9a4dbe99296226cb0341d7a743c93","target":"graph","created_at":"2026-05-18T01:39:35Z","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 investigate the phase transition in the three-dimensional abelian Higgs model for N complex scalar fields, using the gauge-invariant average action \\Gamma_{k}. The dependence of \\Gamma_{k} on the effective infra-red cut-off k is described by a non-perturbative flow equation. The transition turns out to be first- or second-order, depending on the ratio between scalar and gauge coupling. We look at the fixed points of the theory for various N and compute the critical exponents of the model. Comparison with results from the \\epsilon-expansion shows a rather poor convergence for \\epsilon=1 even","authors_text":"B.Bergerhoff, C.Wetterich, D.Litim, S.Lola","cross_cats":["hep-ph","supr-con"],"headline":"","license":"","primary_cat":"cond-mat","submitted_at":"1995-02-09T14:57:06Z","title":"PHASE TRANSITION OF N-COMPONENT SUPERCONDUCTORS"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9502039","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":"sha256:4af92fbe4272e883ccef2f6db7b6458f95ee33e1ef40296d00a1e8a18c1e7985","target":"record","created_at":"2026-05-18T01:39:35Z","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":"b2d6b02d86ecb8be97f9d9d6eb49871eb212f4e68fce7bfd4ef9f7ce65b9bb69","cross_cats_sorted":["hep-ph","supr-con"],"license":"","primary_cat":"cond-mat","submitted_at":"1995-02-09T14:57:06Z","title_canon_sha256":"df7ebeaffa1ceaf9ee100645fc571e521cd29b2460423e2fec2ee328378f19dc"},"schema_version":"1.0","source":{"id":"cond-mat/9502039","kind":"arxiv","version":1}},"canonical_sha256":"133eea7a7f98f325a28fda97fbe22758083b5d6610c716ab8317d0239024ad95","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"133eea7a7f98f325a28fda97fbe22758083b5d6610c716ab8317d0239024ad95","first_computed_at":"2026-05-18T01:39:35.316786Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:39:35.316786Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Fc5wIitwMvOwo5EGdZZ65kmcJBtk3a7gh78veythTj0uz2DX/4acmSuPsuxxhlBhoRIWMKs2XrPmN1zsvSmRAA==","signature_status":"signed_v1","signed_at":"2026-05-18T01:39:35.317302Z","signed_message":"canonical_sha256_bytes"},"source_id":"cond-mat/9502039","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4af92fbe4272e883ccef2f6db7b6458f95ee33e1ef40296d00a1e8a18c1e7985","sha256:033b6a8976a19193cf12fd7b00cf46519fc9a4dbe99296226cb0341d7a743c93"],"state_sha256":"10a222f17400522d7360d537e4985946ee61c3c33f137fe3a4f16055459104fa"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ODvn6ybotDRSRMF2R4k2kiS2zmnx4i1x/l+1yM9kLZ8eaX/WCyi8mYOrcVs3O2qzkj6doInnrpFDGJ7BnTmDCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T23:47:47.118620Z","bundle_sha256":"3bc0937ed745e408c0fd96673a86f9f3cf0e59315488c1e16f54e1384eb1e700"}}