{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:CJGZ7H6H3VAPFDRERDSYKQEEY2","short_pith_number":"pith:CJGZ7H6H","schema_version":"1.0","canonical_sha256":"124d9f9fc7dd40f28e2488e5854084c6aa4631ae4d84e6fad58d80de884716d6","source":{"kind":"arxiv","id":"1903.07624","version":3},"attestation_state":"computed","paper":{"title":"Free Field Realizations from the Higgs Branch","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP","math.QA"],"primary_cat":"hep-th","authors_text":"Carlo Meneghelli, Christopher Beem, Leonardo Rastelli","submitted_at":"2019-03-18T18:00:01Z","abstract_excerpt":"We present free field realizations for the associated vertex operator algebras of a number of four-dimensional $\\mathcal{N}=2$ superconformal field theories. Our constructions utilize an exceptionally small set of chiral bosons whose number matches the complex dimensionality of the Higgs branch of the superconformal field theory. In the case of theories whose Higgs branches support additional degrees of freedom (free vector multiplets or decoupled interacting SCFTs), the corresponding \"free field realizations\" include additional ingredients: symplectic fermions in the case of vector multiplets"},"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":"1903.07624","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-03-18T18:00:01Z","cross_cats_sorted":["math-ph","math.MP","math.QA"],"title_canon_sha256":"7e1d0b7a25138d423e2de13952607c51181501bb4404318bf2c700a8ecdc4efa","abstract_canon_sha256":"ee434e4d5e6ed88a805d8513b066b0bea9b417397f39eadf15c5839b9300ac29"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:49:40.735910Z","signature_b64":"affJfHBXs5EupUhv4P81XA3++hLcJDMTUm13exwBAdGEfzcD9Hj8NKw/5ptB5cNpFvhNHmV6+oZTmz3QLs+ZDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"124d9f9fc7dd40f28e2488e5854084c6aa4631ae4d84e6fad58d80de884716d6","last_reissued_at":"2026-07-05T04:49:40.735432Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:49:40.735432Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Free Field Realizations from the Higgs Branch","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP","math.QA"],"primary_cat":"hep-th","authors_text":"Carlo Meneghelli, Christopher Beem, Leonardo Rastelli","submitted_at":"2019-03-18T18:00:01Z","abstract_excerpt":"We present free field realizations for the associated vertex operator algebras of a number of four-dimensional $\\mathcal{N}=2$ superconformal field theories. Our constructions utilize an exceptionally small set of chiral bosons whose number matches the complex dimensionality of the Higgs branch of the superconformal field theory. In the case of theories whose Higgs branches support additional degrees of freedom (free vector multiplets or decoupled interacting SCFTs), the corresponding \"free field realizations\" include additional ingredients: symplectic fermions in the case of vector multiplets"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1903.07624","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1903.07624/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"1903.07624","created_at":"2026-07-05T04:49:40.735496+00:00"},{"alias_kind":"arxiv_version","alias_value":"1903.07624v3","created_at":"2026-07-05T04:49:40.735496+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1903.07624","created_at":"2026-07-05T04:49:40.735496+00:00"},{"alias_kind":"pith_short_12","alias_value":"CJGZ7H6H3VAP","created_at":"2026-07-05T04:49:40.735496+00:00"},{"alias_kind":"pith_short_16","alias_value":"CJGZ7H6H3VAPFDRE","created_at":"2026-07-05T04:49:40.735496+00:00"},{"alias_kind":"pith_short_8","alias_value":"CJGZ7H6H","created_at":"2026-07-05T04:49:40.735496+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2602.15944","citing_title":"Towards a classification of graded unitary ${\\mathcal W}_3$ algebras","ref_index":5,"is_internal_anchor":false},{"citing_arxiv_id":"2604.19885","citing_title":"On non-relativistic integrable models and 4d SCFTs","ref_index":100,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CJGZ7H6H3VAPFDRERDSYKQEEY2","json":"https://pith.science/pith/CJGZ7H6H3VAPFDRERDSYKQEEY2.json","graph_json":"https://pith.science/api/pith-number/CJGZ7H6H3VAPFDRERDSYKQEEY2/graph.json","events_json":"https://pith.science/api/pith-number/CJGZ7H6H3VAPFDRERDSYKQEEY2/events.json","paper":"https://pith.science/paper/CJGZ7H6H"},"agent_actions":{"view_html":"https://pith.science/pith/CJGZ7H6H3VAPFDRERDSYKQEEY2","download_json":"https://pith.science/pith/CJGZ7H6H3VAPFDRERDSYKQEEY2.json","view_paper":"https://pith.science/paper/CJGZ7H6H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1903.07624&json=true","fetch_graph":"https://pith.science/api/pith-number/CJGZ7H6H3VAPFDRERDSYKQEEY2/graph.json","fetch_events":"https://pith.science/api/pith-number/CJGZ7H6H3VAPFDRERDSYKQEEY2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CJGZ7H6H3VAPFDRERDSYKQEEY2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CJGZ7H6H3VAPFDRERDSYKQEEY2/action/storage_attestation","attest_author":"https://pith.science/pith/CJGZ7H6H3VAPFDRERDSYKQEEY2/action/author_attestation","sign_citation":"https://pith.science/pith/CJGZ7H6H3VAPFDRERDSYKQEEY2/action/citation_signature","submit_replication":"https://pith.science/pith/CJGZ7H6H3VAPFDRERDSYKQEEY2/action/replication_record"}},"created_at":"2026-07-05T04:49:40.735496+00:00","updated_at":"2026-07-05T04:49:40.735496+00:00"}