{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:KRQKGMM2S7FWWFHGVJX33GEFQR","short_pith_number":"pith:KRQKGMM2","schema_version":"1.0","canonical_sha256":"5460a3319a97cb6b14e6aa6fbd98858474ef5e4b869d85c36c2ffb859cef4ac6","source":{"kind":"arxiv","id":"1703.09148","version":2},"attestation_state":"computed","paper":{"title":"Defects in the Tri-critical Ising model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Gerard M T Watts, Isao Makabe","submitted_at":"2017-03-27T15:36:56Z","abstract_excerpt":"We consider two different conformal field theories with central charge c=7/10. One is the diagonal invariant minimal model in which all fields have integer spins; the other is the local fermionic theory with superconformal symmetry in which fields can have half-integer spin. We construct new conformal (but not topological or factorised) defects in the minimal model. We do this by first constructing defects in the fermionic model as boundary conditions in a fermionic theory of central charge c=7/5, using the folding trick as first proposed by Gang and Yamaguchi. We then acting on these with int"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1703.09148","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-03-27T15:36:56Z","cross_cats_sorted":[],"title_canon_sha256":"2d306f95dd386589034d45eac0d83205ae3419d074ee2610fbf62efac69ff418","abstract_canon_sha256":"bc3c1d945799a356e555afbff1274460831e4287e900f507ef7ab29ecb0f14dc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:34:51.518283Z","signature_b64":"88Bn8VpAvob1uB+WZCeXyr6UslF89IzaBO0sX3/XwOXz2eBe81Wl3HJ6M8w65h6eUfUDy+iPOpnLtlmSd2qCDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5460a3319a97cb6b14e6aa6fbd98858474ef5e4b869d85c36c2ffb859cef4ac6","last_reissued_at":"2026-05-18T00:34:51.517584Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:34:51.517584Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Defects in the Tri-critical Ising model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Gerard M T Watts, Isao Makabe","submitted_at":"2017-03-27T15:36:56Z","abstract_excerpt":"We consider two different conformal field theories with central charge c=7/10. One is the diagonal invariant minimal model in which all fields have integer spins; the other is the local fermionic theory with superconformal symmetry in which fields can have half-integer spin. We construct new conformal (but not topological or factorised) defects in the minimal model. We do this by first constructing defects in the fermionic model as boundary conditions in a fermionic theory of central charge c=7/5, using the folding trick as first proposed by Gang and Yamaguchi. We then acting on these with int"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.09148","kind":"arxiv","version":2},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1703.09148","created_at":"2026-05-18T00:34:51.517703+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.09148v2","created_at":"2026-05-18T00:34:51.517703+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.09148","created_at":"2026-05-18T00:34:51.517703+00:00"},{"alias_kind":"pith_short_12","alias_value":"KRQKGMM2S7FW","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_16","alias_value":"KRQKGMM2S7FWWFHG","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_8","alias_value":"KRQKGMM2","created_at":"2026-05-18T12:31:28.150371+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.01151","citing_title":"Entanglement fingerprint of a non-invertible symmetry: exact Fibonacci cut charges on the lattice","ref_index":21,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KRQKGMM2S7FWWFHGVJX33GEFQR","json":"https://pith.science/pith/KRQKGMM2S7FWWFHGVJX33GEFQR.json","graph_json":"https://pith.science/api/pith-number/KRQKGMM2S7FWWFHGVJX33GEFQR/graph.json","events_json":"https://pith.science/api/pith-number/KRQKGMM2S7FWWFHGVJX33GEFQR/events.json","paper":"https://pith.science/paper/KRQKGMM2"},"agent_actions":{"view_html":"https://pith.science/pith/KRQKGMM2S7FWWFHGVJX33GEFQR","download_json":"https://pith.science/pith/KRQKGMM2S7FWWFHGVJX33GEFQR.json","view_paper":"https://pith.science/paper/KRQKGMM2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.09148&json=true","fetch_graph":"https://pith.science/api/pith-number/KRQKGMM2S7FWWFHGVJX33GEFQR/graph.json","fetch_events":"https://pith.science/api/pith-number/KRQKGMM2S7FWWFHGVJX33GEFQR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KRQKGMM2S7FWWFHGVJX33GEFQR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KRQKGMM2S7FWWFHGVJX33GEFQR/action/storage_attestation","attest_author":"https://pith.science/pith/KRQKGMM2S7FWWFHGVJX33GEFQR/action/author_attestation","sign_citation":"https://pith.science/pith/KRQKGMM2S7FWWFHGVJX33GEFQR/action/citation_signature","submit_replication":"https://pith.science/pith/KRQKGMM2S7FWWFHGVJX33GEFQR/action/replication_record"}},"created_at":"2026-05-18T00:34:51.517703+00:00","updated_at":"2026-05-18T00:34:51.517703+00:00"}