{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2020:BYSVRHP3VHIU3E4BIQMBMF2YLG","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":"36396619ffe2d0b6ba7f51819ee787eef65565efc39159189650847c4d3ab6e6","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-07-07T15:23:02Z","title_canon_sha256":"079f3490a900e4e8cc552b94b89c92f30c0e1015dee40074064bbc7f2068e01f"},"schema_version":"1.0","source":{"id":"2007.03683","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2007.03683","created_at":"2026-07-05T02:17:27Z"},{"alias_kind":"arxiv_version","alias_value":"2007.03683v1","created_at":"2026-07-05T02:17:27Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2007.03683","created_at":"2026-07-05T02:17:27Z"},{"alias_kind":"pith_short_12","alias_value":"BYSVRHP3VHIU","created_at":"2026-07-05T02:17:27Z"},{"alias_kind":"pith_short_16","alias_value":"BYSVRHP3VHIU3E4B","created_at":"2026-07-05T02:17:27Z"},{"alias_kind":"pith_short_8","alias_value":"BYSVRHP3","created_at":"2026-07-05T02:17:27Z"}],"graph_snapshots":[{"event_id":"sha256:354d7aa4147776a55aaf09b3cb5170c599289057c5e5673a2abce8a0b8f111bb","target":"graph","created_at":"2026-07-05T02:17:27Z","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/2007.03683/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We study the integrable bi-Yang-Baxter deformation of the $SU(2)$ principal chiral model (PCM) and its finite action uniton solutions. Under an adiabatic compactification on an $S^1$, we obtain a quantum mechanics with an elliptic Lam\\'e-like potential.\n  We perform a perturbative calculation of the ground state energy in this quantum mechanics to large orders obtaining an asymptotic series. Using the Borel-Pad\\'e technique, we determine the expected locations of branch cuts in the Borel plane of the perturbative series and show that they match the values of the uniton actions. Therefore, we c","authors_text":"Daniel C. Thompson, Lucas Schepers","cross_cats":["math-ph","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-07-07T15:23:02Z","title":"Resurgence in the Bi-Yang-Baxter Model"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2007.03683","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":"sha256:4586d5dd7766a290caa220a06f165cde8e19128d1606b329375a73214a80ba9a","target":"record","created_at":"2026-07-05T02:17:27Z","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":"36396619ffe2d0b6ba7f51819ee787eef65565efc39159189650847c4d3ab6e6","cross_cats_sorted":["math-ph","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-07-07T15:23:02Z","title_canon_sha256":"079f3490a900e4e8cc552b94b89c92f30c0e1015dee40074064bbc7f2068e01f"},"schema_version":"1.0","source":{"id":"2007.03683","kind":"arxiv","version":1}},"canonical_sha256":"0e25589dfba9d14d9381441816175859aeffd0e9bcd00632709a0b142601c513","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"0e25589dfba9d14d9381441816175859aeffd0e9bcd00632709a0b142601c513","first_computed_at":"2026-07-05T02:17:27.802832Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T02:17:27.802832Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Qf+B8lK9JHDhnYDMP6Q30WqFohoDZu+Cwpb/PbOdr28eLlf6nqHWZAf5RRbwGfncfw7axnjkcFvlPYzuwgWRDg==","signature_status":"signed_v1","signed_at":"2026-07-05T02:17:27.803262Z","signed_message":"canonical_sha256_bytes"},"source_id":"2007.03683","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4586d5dd7766a290caa220a06f165cde8e19128d1606b329375a73214a80ba9a","sha256:354d7aa4147776a55aaf09b3cb5170c599289057c5e5673a2abce8a0b8f111bb"],"state_sha256":"4547c09a5ff98ab5dde53de9446da2c758424dfa52ba4604490a212b35b2f819"}