{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2023:J7KW6BTXLYAFFTT4YL7ITVUPTZ","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":"b81c7c281933cda39553be01ffe24a3168138c9ca7bbcd4fcd5faf7f8cf77a25","cross_cats_sorted":["cond-mat.stat-mech","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-01-04T18:25:08Z","title_canon_sha256":"19a5a72c3873ac6ac31c06cee337f8e8f39269a3ddd1f2fe1e9cbad050f8f71b"},"schema_version":"1.0","source":{"id":"2301.01745","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2301.01745","created_at":"2026-07-05T05:50:57Z"},{"alias_kind":"arxiv_version","alias_value":"2301.01745v1","created_at":"2026-07-05T05:50:57Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2301.01745","created_at":"2026-07-05T05:50:57Z"},{"alias_kind":"pith_short_12","alias_value":"J7KW6BTXLYAF","created_at":"2026-07-05T05:50:57Z"},{"alias_kind":"pith_short_16","alias_value":"J7KW6BTXLYAFFTT4","created_at":"2026-07-05T05:50:57Z"},{"alias_kind":"pith_short_8","alias_value":"J7KW6BTX","created_at":"2026-07-05T05:50:57Z"}],"graph_snapshots":[{"event_id":"sha256:cc58952f43e4562f531d5bac5fa54e4c1597c38a1f42f1824d2dcae3e3e80cbe","target":"graph","created_at":"2026-07-05T05:50:57Z","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/2301.01745/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"All standard measures of bipartite entanglement in one-dimensional quantum field theories can be expressed in terms of correlators of branch point twist fields, here denoted by $\\mathcal{T}$ and $\\mathcal{T}^\\dagger$. These are symmetry fields associated to cyclic permutation symmetry in a replica theory and having the smallest conformal dimension at the critical point. Recently, other twist fields (composite twist fields), typically of higher dimension, have been shown to play a role in the study of a new measure of entanglement known as the symmetry resolved entanglement entropy. In this pap","authors_text":"Michele Mazzoni, Olalla A. Castro-Alvaredo","cross_cats":["cond-mat.stat-mech","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-01-04T18:25:08Z","title":"Two-Point Functions of Composite Twist Fields in the Ising Field Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2301.01745","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:f97e43e5f87a7b9a2ae6c3e269811e949775f3c0b3e0dfd8797029d939a8e596","target":"record","created_at":"2026-07-05T05:50:57Z","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":"b81c7c281933cda39553be01ffe24a3168138c9ca7bbcd4fcd5faf7f8cf77a25","cross_cats_sorted":["cond-mat.stat-mech","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2023-01-04T18:25:08Z","title_canon_sha256":"19a5a72c3873ac6ac31c06cee337f8e8f39269a3ddd1f2fe1e9cbad050f8f71b"},"schema_version":"1.0","source":{"id":"2301.01745","kind":"arxiv","version":1}},"canonical_sha256":"4fd56f06775e0052ce7cc2fe89d68f9e64af9a86d698b79a46bf4526d3784aba","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4fd56f06775e0052ce7cc2fe89d68f9e64af9a86d698b79a46bf4526d3784aba","first_computed_at":"2026-07-05T05:50:57.585254Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:50:57.585254Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"d43Zy/9YXOUvK/sXVWm1etxAaZSfduTaiCmilzaIbbx1+4NUCnF60iiof47GIvZAlbXZothFokwgGBFr2rv4CA==","signature_status":"signed_v1","signed_at":"2026-07-05T05:50:57.585755Z","signed_message":"canonical_sha256_bytes"},"source_id":"2301.01745","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:f97e43e5f87a7b9a2ae6c3e269811e949775f3c0b3e0dfd8797029d939a8e596","sha256:cc58952f43e4562f531d5bac5fa54e4c1597c38a1f42f1824d2dcae3e3e80cbe"],"state_sha256":"ba767006984b8b56b5c245adff5d9eafefee78d5b070fa52a3b9bef99bc176fb"}