{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:46A34BDBD5DZ6D4XMCIERVJR46","short_pith_number":"pith:46A34BDB","canonical_record":{"source":{"id":"2205.07241","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-05-15T09:54:03Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"2372d9a7184399a1cc09bedf0e99a58f6cb7cbcbd2bc57845e24156cf13850ea","abstract_canon_sha256":"390a01c33a179eee37889c17d8dfbc2518d2dcc4644c7b5464efaf357609a81e"},"schema_version":"1.0"},"canonical_sha256":"e781be04611f479f0f97609048d531e79a10f27dba90d87138aab8c95f6496f6","source":{"kind":"arxiv","id":"2205.07241","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2205.07241","created_at":"2026-07-05T08:30:00Z"},{"alias_kind":"arxiv_version","alias_value":"2205.07241v3","created_at":"2026-07-05T08:30:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.07241","created_at":"2026-07-05T08:30:00Z"},{"alias_kind":"pith_short_12","alias_value":"46A34BDBD5DZ","created_at":"2026-07-05T08:30:00Z"},{"alias_kind":"pith_short_16","alias_value":"46A34BDBD5DZ6D4X","created_at":"2026-07-05T08:30:00Z"},{"alias_kind":"pith_short_8","alias_value":"46A34BDB","created_at":"2026-07-05T08:30:00Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:46A34BDBD5DZ6D4XMCIERVJR46","target":"record","payload":{"canonical_record":{"source":{"id":"2205.07241","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-05-15T09:54:03Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"2372d9a7184399a1cc09bedf0e99a58f6cb7cbcbd2bc57845e24156cf13850ea","abstract_canon_sha256":"390a01c33a179eee37889c17d8dfbc2518d2dcc4644c7b5464efaf357609a81e"},"schema_version":"1.0"},"canonical_sha256":"e781be04611f479f0f97609048d531e79a10f27dba90d87138aab8c95f6496f6","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:30:00.470096Z","signature_b64":"s7WxekPVAB0W/M+m3nnUtXL2V2apzJZ5HPavyljTxdfJgOj132EVZLRglU7OLtSzhlKU2cu6logsUKiZutSDAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e781be04611f479f0f97609048d531e79a10f27dba90d87138aab8c95f6496f6","last_reissued_at":"2026-07-05T08:30:00.469695Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:30:00.469695Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2205.07241","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-05T08:30:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MKVcpY5fClhnOSyn5en+NGxuHY6FJSzf4cc0Op4z6uUNa8Z2rdF9XwJ00ZULvPqTVq73D2GN/toolsZtvR7uDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T19:41:58.509860Z"},"content_sha256":"56dbcd31ca1fc3cc74b752a91827f2c53a1435fda376e4db445a2520845817ff","schema_version":"1.0","event_id":"sha256:56dbcd31ca1fc3cc74b752a91827f2c53a1435fda376e4db445a2520845817ff"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:46A34BDBD5DZ6D4XMCIERVJR46","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Radiative first-order phase transitions to next-to-next-to-leading order","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Andreas Ekstedt, Johan L\\\"ofgren, Oliver Gould","submitted_at":"2022-05-15T09:54:03Z","abstract_excerpt":"We develop new perturbative tools to accurately study radiatively-induced first-order phase transitions. Previous perturbative methods have suffered internal inconsistencies and been unsuccessful in reproducing lattice data, which is often attributed to infrared divergences of massless modes (the Linde problem). We employ a consistent power counting scheme to perform calculations, and compare our results against lattice data. We conclude that the consistent expansion removes many previous issues, and indicates that the infamous Linde problem is not as big a factor in these calculations as prev"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.07241","kind":"arxiv","version":3},"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/2205.07241/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":"2026-07-05T08:30:00Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"AydQaDEY8Tn3copvbSWEgkQ36ynFywVujNLb3sl3sMkCQToDvlzLjaFcaFtIX6W1GOYj3L8E+64MZFHZ2vsWCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-03T19:41:58.510354Z"},"content_sha256":"3237c07ebf0a0c5ee0befcbc8fe4dc90916e622e6c61a74912d1f73c43d75045","schema_version":"1.0","event_id":"sha256:3237c07ebf0a0c5ee0befcbc8fe4dc90916e622e6c61a74912d1f73c43d75045"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/46A34BDBD5DZ6D4XMCIERVJR46/bundle.json","state_url":"https://pith.science/pith/46A34BDBD5DZ6D4XMCIERVJR46/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/46A34BDBD5DZ6D4XMCIERVJR46/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":"2026-08-03T19:41:58Z","links":{"resolver":"https://pith.science/pith/46A34BDBD5DZ6D4XMCIERVJR46","bundle":"https://pith.science/pith/46A34BDBD5DZ6D4XMCIERVJR46/bundle.json","state":"https://pith.science/pith/46A34BDBD5DZ6D4XMCIERVJR46/state.json","well_known_bundle":"https://pith.science/.well-known/pith/46A34BDBD5DZ6D4XMCIERVJR46/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:46A34BDBD5DZ6D4XMCIERVJR46","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":"390a01c33a179eee37889c17d8dfbc2518d2dcc4644c7b5464efaf357609a81e","cross_cats_sorted":["hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-05-15T09:54:03Z","title_canon_sha256":"2372d9a7184399a1cc09bedf0e99a58f6cb7cbcbd2bc57845e24156cf13850ea"},"schema_version":"1.0","source":{"id":"2205.07241","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2205.07241","created_at":"2026-07-05T08:30:00Z"},{"alias_kind":"arxiv_version","alias_value":"2205.07241v3","created_at":"2026-07-05T08:30:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.07241","created_at":"2026-07-05T08:30:00Z"},{"alias_kind":"pith_short_12","alias_value":"46A34BDBD5DZ","created_at":"2026-07-05T08:30:00Z"},{"alias_kind":"pith_short_16","alias_value":"46A34BDBD5DZ6D4X","created_at":"2026-07-05T08:30:00Z"},{"alias_kind":"pith_short_8","alias_value":"46A34BDB","created_at":"2026-07-05T08:30:00Z"}],"graph_snapshots":[{"event_id":"sha256:3237c07ebf0a0c5ee0befcbc8fe4dc90916e622e6c61a74912d1f73c43d75045","target":"graph","created_at":"2026-07-05T08:30:00Z","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/2205.07241/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We develop new perturbative tools to accurately study radiatively-induced first-order phase transitions. Previous perturbative methods have suffered internal inconsistencies and been unsuccessful in reproducing lattice data, which is often attributed to infrared divergences of massless modes (the Linde problem). We employ a consistent power counting scheme to perform calculations, and compare our results against lattice data. We conclude that the consistent expansion removes many previous issues, and indicates that the infamous Linde problem is not as big a factor in these calculations as prev","authors_text":"Andreas Ekstedt, Johan L\\\"ofgren, Oliver Gould","cross_cats":["hep-th"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-05-15T09:54:03Z","title":"Radiative first-order phase transitions to next-to-next-to-leading order"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.07241","kind":"arxiv","version":3},"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":"sha256:56dbcd31ca1fc3cc74b752a91827f2c53a1435fda376e4db445a2520845817ff","target":"record","created_at":"2026-07-05T08:30:00Z","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":"390a01c33a179eee37889c17d8dfbc2518d2dcc4644c7b5464efaf357609a81e","cross_cats_sorted":["hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-05-15T09:54:03Z","title_canon_sha256":"2372d9a7184399a1cc09bedf0e99a58f6cb7cbcbd2bc57845e24156cf13850ea"},"schema_version":"1.0","source":{"id":"2205.07241","kind":"arxiv","version":3}},"canonical_sha256":"e781be04611f479f0f97609048d531e79a10f27dba90d87138aab8c95f6496f6","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e781be04611f479f0f97609048d531e79a10f27dba90d87138aab8c95f6496f6","first_computed_at":"2026-07-05T08:30:00.469695Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:30:00.469695Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"s7WxekPVAB0W/M+m3nnUtXL2V2apzJZ5HPavyljTxdfJgOj132EVZLRglU7OLtSzhlKU2cu6logsUKiZutSDAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T08:30:00.470096Z","signed_message":"canonical_sha256_bytes"},"source_id":"2205.07241","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:56dbcd31ca1fc3cc74b752a91827f2c53a1435fda376e4db445a2520845817ff","sha256:3237c07ebf0a0c5ee0befcbc8fe4dc90916e622e6c61a74912d1f73c43d75045"],"state_sha256":"509ba580d49a81b2c24617b221631cc37ffa283f81f9249ed2ec3274f244f8ed"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"K4f8+lCFuh1A1pROVgFt6nWqyMB0JbxVCf9mybJKkghTS9WqwPqnB9nl3+9YokBQFmauslbqr2xrOsVL6KbSAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-03T19:41:58.514024Z","bundle_sha256":"c0be50151c78040333eebf3e1b61d68ed6446c3993371fba88232bd7fb17ef08"}}