{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:UJHCZ7R6Q5XH6RYONBJOTMFUYJ","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":"b6cf01d82ca0d2d489d80d71d546272b7edb679456362afdb80eb8990467f39f","cross_cats_sorted":["gr-qc","hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-07-20T11:04:13Z","title_canon_sha256":"590c5cca06c7c1545f6195ab1392f1820fb137db6aecd3bc49b0145a3010d00c"},"schema_version":"1.0","source":{"id":"2207.09817","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2207.09817","created_at":"2026-07-05T06:52:00Z"},{"alias_kind":"arxiv_version","alias_value":"2207.09817v3","created_at":"2026-07-05T06:52:00Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2207.09817","created_at":"2026-07-05T06:52:00Z"},{"alias_kind":"pith_short_12","alias_value":"UJHCZ7R6Q5XH","created_at":"2026-07-05T06:52:00Z"},{"alias_kind":"pith_short_16","alias_value":"UJHCZ7R6Q5XH6RYO","created_at":"2026-07-05T06:52:00Z"},{"alias_kind":"pith_short_8","alias_value":"UJHCZ7R6","created_at":"2026-07-05T06:52:00Z"}],"graph_snapshots":[{"event_id":"sha256:c5d992a336ac67662f046dabd222597f2cc0779dba625d8c5c8642440dbdf522","target":"graph","created_at":"2026-07-05T06:52:00Z","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/2207.09817/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We present a comprehensive non-perturbative study of the phase structure of the asymptotically safe Standard Model. The physics scales included range from the asymptotically safe trans-Planckian regime in the ultraviolet, the intermediate high-energy regime with electroweak symmetry breaking to strongly correlated QCD in the infrared. All flows are computed with a self-consistent functional renormalisation group approach, using a vertex expansion in the fluctuation fields. In particular, this approach takes care of all physical threshold effects and the respective decoupling of ultraviolet deg","authors_text":"\\'Alvaro Pastor-Guti\\'errez, Jan M. Pawlowski, Manuel Reichert","cross_cats":["gr-qc","hep-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-07-20T11:04:13Z","title":"The Asymptotically Safe Standard Model: From quantum gravity to dynamical chiral symmetry breaking"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2207.09817","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":"sha256:8e8213e35b096190421c18032f2f21b613738e9e3cec7dd04c82d0c8ad78b707","target":"record","created_at":"2026-07-05T06:52:00Z","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":"b6cf01d82ca0d2d489d80d71d546272b7edb679456362afdb80eb8990467f39f","cross_cats_sorted":["gr-qc","hep-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-07-20T11:04:13Z","title_canon_sha256":"590c5cca06c7c1545f6195ab1392f1820fb137db6aecd3bc49b0145a3010d00c"},"schema_version":"1.0","source":{"id":"2207.09817","kind":"arxiv","version":3}},"canonical_sha256":"a24e2cfe3e876e7f470e6852e9b0b4c248f8a25b31a52f1fc3268ea81412913f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a24e2cfe3e876e7f470e6852e9b0b4c248f8a25b31a52f1fc3268ea81412913f","first_computed_at":"2026-07-05T06:52:00.308616Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:52:00.308616Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"WTtWISfjF4A1GG882GR3gvjkxhdxyZCn/LbqbANj6FV46utYc8q2IYE4o+9eVnqa82m5Y5R4w3bAz01oxz7gDQ==","signature_status":"signed_v1","signed_at":"2026-07-05T06:52:00.309066Z","signed_message":"canonical_sha256_bytes"},"source_id":"2207.09817","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8e8213e35b096190421c18032f2f21b613738e9e3cec7dd04c82d0c8ad78b707","sha256:c5d992a336ac67662f046dabd222597f2cc0779dba625d8c5c8642440dbdf522"],"state_sha256":"87e93353aba93f5628e35dc9ea1a967371520b03604f48d24a634eb8afefbd81"}