{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:EESWTPDS4APXRYX3NCYEGEGABP","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":"2dc460aff4737e3c1680860bb819311d686a48f1a76f4194f022b47a709b19f0","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.str-el","hep-ph","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2026-07-28T18:00:01Z","title_canon_sha256":"948e676ac8e44979cb2e5e03a02e15dc7b37b2bf564d4f5f8a7255b1057a0a15"},"schema_version":"1.0","source":{"id":"2607.26132","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2607.26132","created_at":"2026-07-30T00:08:26Z"},{"alias_kind":"arxiv_version","alias_value":"2607.26132v1","created_at":"2026-07-30T00:08:26Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.26132","created_at":"2026-07-30T00:08:26Z"},{"alias_kind":"pith_short_12","alias_value":"EESWTPDS4APX","created_at":"2026-07-30T00:08:26Z"},{"alias_kind":"pith_short_16","alias_value":"EESWTPDS4APXRYX3","created_at":"2026-07-30T00:08:26Z"},{"alias_kind":"pith_short_8","alias_value":"EESWTPDS","created_at":"2026-07-30T00:08:26Z"}],"graph_snapshots":[{"event_id":"sha256:b3e212941beba1ce4455d73af8148d1da993a8c7c812aced9292ef9f3024eb72","target":"graph","created_at":"2026-07-30T00:08:26Z","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/2607.26132/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Non-Abelian gauge theories with dynamical matter govern the strong interaction and a broad class of strongly correlated quantum systems, yet their ground-state properties remain difficult to obtain from first principles. Using a continuous-group variational Monte Carlo approach that retains the full SU$(2)$ gauge field without truncation, we determine the ground-state behavior of the SU$(2)$ lattice gauge theory with staggered fermions on an $L\\times L$ square lattice. Treating the magnetic and electric couplings $\\lambda$ and $g^2$ independently, we find a magnetic-flux transition at $\\lambda","authors_text":"Gabriel Rouxinol, Jad C. Halimeh, Julian Bender, Michele Grossi, Patrick Emonts","cross_cats":["cond-mat.quant-gas","cond-mat.str-el","hep-ph","quant-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2026-07-28T18:00:01Z","title":"Quantum Phase Diagram of the $2+1$D Untruncated SU$(2)$ Lattice Gauge Theory with Dynamical Fermions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.26132","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":"sha256:77f63f4e7c52481fe6e386adaf5106809b5f48252d7216541f8172f017c9dad2","target":"record","created_at":"2026-07-30T00:08:26Z","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":"2dc460aff4737e3c1680860bb819311d686a48f1a76f4194f022b47a709b19f0","cross_cats_sorted":["cond-mat.quant-gas","cond-mat.str-el","hep-ph","quant-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2026-07-28T18:00:01Z","title_canon_sha256":"948e676ac8e44979cb2e5e03a02e15dc7b37b2bf564d4f5f8a7255b1057a0a15"},"schema_version":"1.0","source":{"id":"2607.26132","kind":"arxiv","version":1}},"canonical_sha256":"212569bc72e01f78e2fb68b04310c00bd0de21eb10c7ae71db20060f793eb637","receipt":{"builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"212569bc72e01f78e2fb68b04310c00bd0de21eb10c7ae71db20060f793eb637","first_computed_at":"2026-07-30T00:08:26.264338Z","kind":"pith_receipt","last_reissued_at":"2026-07-30T00:08:26.264338Z","receipt_version":"0.3","signature_status":"unsigned_v0"},"source_id":"2607.26132","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:77f63f4e7c52481fe6e386adaf5106809b5f48252d7216541f8172f017c9dad2","sha256:b3e212941beba1ce4455d73af8148d1da993a8c7c812aced9292ef9f3024eb72"],"state_sha256":"4082795a1bb1fb2c0d5c9f5936a6dc7b769e5c0721879a45cb64f0ff52990d20"}