{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:7P2OQG7DMQFS7EXHMHBTQCJANN","merge_version":"pith-open-graph-merge-v1","event_count":7,"valid_event_count":7,"invalid_event_count":0,"equivocation_count":1,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"7f37564edab7b0084b51113453415d5d9f15b494c497701bd8783cb3249f5863","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-05-14T17:57:40Z","title_canon_sha256":"a8fc8626e5c754144648088e2987086215f2695133b7dbf6c96ca1eb250ee6f5"},"schema_version":"1.0","source":{"id":"2605.15176","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2605.15176","created_at":"2026-05-17T21:18:32Z"},{"alias_kind":"arxiv_version","alias_value":"2605.15176v1","created_at":"2026-05-17T21:18:32Z"},{"alias_kind":"pith_short_12","alias_value":"7P2OQG7DMQFS","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_16","alias_value":"7P2OQG7DMQFS7EXH","created_at":"2026-05-18T12:33:37Z"},{"alias_kind":"pith_short_8","alias_value":"7P2OQG7D","created_at":"2026-05-18T12:33:37Z"}],"graph_snapshots":[{"event_id":"sha256:af43f5bd0b7f1f505bd928fe33eaf2c4d07b6e39195963fdd14d9047339a97ee","target":"graph","created_at":"2026-05-17T21:57:18Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"This work automates the matching of generic three-dimensional dimension-five and -six operators for arbitrary models containing scalars, fermions, and gauge fields, implemented as an extension of the Mathematica package DRalgo."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"The high-temperature expansion remains valid and the chosen operator basis after field redefinitions captures all relevant contributions without missing gauge-dependent artifacts that affect physical observables."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"The authors automate matching of generic 3D dimension-five and -six operators for arbitrary models, implemented in an extension of DRalgo with public code and examples for scalar-Yukawa, hot QCD, and the full Standard Model."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Generic models with scalars, fermions and gauge fields now have automated matching of dimension-five and -six operators in their three-dimensional high-temperature effective theories."}],"snapshot_sha256":"659c32693540e457dfaa6a0514ca027ae12627874b01f1591c3eafa5dd594432"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"High-temperature dimensional reduction provides a systematic effective field theory framework for studying finite-temperature thermodynamics and cosmological phase transitions. While the matching of super-renormalizable operators in the resulting three-dimensional effective theories is well established, the matching of higher-dimensional operators has recently been reinvigorated. These operators become phenomenologically relevant in strong first-order phase transitions where they quantify the convergence of the high-temperature expansion. This work automates the matching of generic three-dimen","authors_text":"Fabio Bernardo, Philipp Schicho, Romain Guillermo Reinle","cross_cats":[],"headline":"Generic models with scalars, fermions and gauge fields now have automated matching of dimension-five and -six operators in their three-dimensional high-temperature effective theories.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-05-14T17:57:40Z","title":"Matching higher-dimensional operators at finite temperature for general models"},"references":{"count":85,"internal_anchors":45,"resolved_work":85,"sample":[{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":1,"title":"Auclairet al.(LISA Cosmology Working Group), Cosmol- ogy with the Laser Interferometer Space Antenna, Living Rev","work_id":"264d2696-4222-4047-a5f7-4d3ff5a2e546","year":2023},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":2,"title":"P. H. Ginsparg, First Order and Second Order Phase Transitions in Gauge Theo ries at Finite Temperature, Nucl. Phys. B 170 (1980) 388. 29","work_id":"51f7b22c-de48-4c71-8883-f0adb0fa018f","year":1980},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":3,"title":"T. Appelquist and R. D. Pisarski, High-Temperature Yang-Mills Theories and Three-Dimensional Quantum Chromodynamics, Phys. Rev. D 23 (1981) 2305","work_id":"cf4af85b-0e85-4896-ba2e-23c001f0e58b","year":1981},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":4,"title":"Nadkarni, Dimensional Reduction in Finite Temperature Quantum Chrom odynamics","work_id":"abb3048a-7e0e-4bcf-aed8-9952595217a6","year":1988},{"cited_arxiv_id":"","doi":"","is_internal_anchor":false,"ref_index":5,"title":"N. P. Landsman, Limitations to Dimensional Reduction at High Temperature, Nucl. Phys. B 322 (1989) 498","work_id":"bd134f31-186b-455b-9b05-d27c27261410","year":1989}],"snapshot_sha256":"8a55819bc0ee8e19d9d32710ff543230682a1713efdda82b930a5da919adc013"},"source":{"id":"2605.15176","kind":"arxiv","version":1},"verdict":{"created_at":"2026-05-15T02:55:01.467995Z","id":"af2bcaa2-3b71-4071-84e9-793a11dba78c","model_set":{"reader":"grok-4.3"},"one_line_summary":"The authors automate matching of generic 3D dimension-five and -six operators for arbitrary models, implemented in an extension of DRalgo with public code and examples for scalar-Yukawa, hot QCD, and the full Standard Model.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Generic models with scalars, fermions and gauge fields now have automated matching of dimension-five and -six operators in their three-dimensional high-temperature effective theories.","strongest_claim":"This work automates the matching of generic three-dimensional dimension-five and -six operators for arbitrary models containing scalars, fermions, and gauge fields, implemented as an extension of the Mathematica package DRalgo.","weakest_assumption":"The high-temperature expansion remains valid and the chosen operator basis after field redefinitions captures all relevant contributions without missing gauge-dependent artifacts that affect physical observables."}},"verdict_id":"af2bcaa2-3b71-4071-84e9-793a11dba78c"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:628fdd67eaf37438af6d8baf3b434799b7f03af1614d20890ffd80d851b4eed0","target":"record","created_at":"2026-05-17T21:18:32Z","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":"7f37564edab7b0084b51113453415d5d9f15b494c497701bd8783cb3249f5863","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-05-14T17:57:40Z","title_canon_sha256":"a8fc8626e5c754144648088e2987086215f2695133b7dbf6c96ca1eb250ee6f5"},"schema_version":"1.0","source":{"id":"2605.15176","kind":"arxiv","version":1}},"canonical_sha256":"fbf4e81be3640b2f92e761c33809206b516d2e87581935f836c925e5d3edd7dd","receipt":{"builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fbf4e81be3640b2f92e761c33809206b516d2e87581935f836c925e5d3edd7dd","first_computed_at":"2026-05-17T21:40:25.228869Z","kind":"pith_receipt","last_reissued_at":"2026-05-17T21:57:18.576396Z","receipt_version":"0.2","signature_status":"unsigned_v0"},"source_id":"2605.15176","source_kind":"arxiv","source_version":1}}},"equivocations":[{"signer_id":"pith.science","event_type":"integrity_finding","target":"integrity","event_ids":["sha256:14ce11d94802328454fc235ae31a8da481a586d0c7766ea38e5ef89140b25bde","sha256:223351cc25f4b056a9125ae254deb0c56a117c848fdbfffda1357290668b9818","sha256:5a73c84832547b3439ae45c2f3a395373a3a203bc4d6a9e1b2b70eaf1be5dae8","sha256:be505fa68db7ad5ba8b252fd3df93c0ce480e3dc14e633cc28582bf0c7699009","sha256:e10334f122127e189a7e629664670b387370fdfb869d1c3c7486b322dc994fb8"]}],"invalid_events":[],"applied_event_ids":["sha256:628fdd67eaf37438af6d8baf3b434799b7f03af1614d20890ffd80d851b4eed0","sha256:af43f5bd0b7f1f505bd928fe33eaf2c4d07b6e39195963fdd14d9047339a97ee"],"state_sha256":"03bea8bc2d5847fc1cfcbff0d52f3713bc8369f3e287dae01e56cc4a8fc8880c"}