{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:4DNKGPUTMXHGSRLOUDXOK2EB2A","short_pith_number":"pith:4DNKGPUT","schema_version":"1.0","canonical_sha256":"e0daa33e9365ce69456ea0eee56881d001e07ecc98cc94d7f55c588276908a09","source":{"kind":"arxiv","id":"1804.09694","version":3},"attestation_state":"computed","paper":{"title":"Universal Features of BPS Strings in Six-dimensional SCFTs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Guglielmo Lockhart, Michele Del Zotto","submitted_at":"2018-04-25T17:42:20Z","abstract_excerpt":"In theories with extended supersymmetry the protected observables of UV superconformal fixed points are found in a number of contexts to be encoded in the BPS solitons along an IR Coulomb-like phase. For six-dimensional SCFTs such a role is played by the BPS strings on the tensorial Coulomb branch. In this paper we develop a uniform description of the worldsheet theories of a BPS string for rank-one 6d SCFTs. These strings are the basic constituents of the BPS string spectrum of arbitrary rank six-dimensional models, which they generate by forming bound states. Motivated by geometric engineeri"},"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":"1804.09694","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2018-04-25T17:42:20Z","cross_cats_sorted":[],"title_canon_sha256":"4ae61c2791a20189b6f23ddcb651a63bb8d893ed8141edaa815ad28ea37aea6a","abstract_canon_sha256":"fdbe6a35a7cdff8da3c3cdaba95a7cc0fc6d47c2d3524513dd9b0b69f17c1929"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:04:58.748035Z","signature_b64":"JiIOgKh66AZRUjL6Zb98ALfI+nFlKUOeJq41TcTk+pIlcy8B1FwOYqgPcP+JiITqwAd2aM9N0NR9P7PmWNxMDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e0daa33e9365ce69456ea0eee56881d001e07ecc98cc94d7f55c588276908a09","last_reissued_at":"2026-05-18T00:04:58.747326Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:04:58.747326Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Universal Features of BPS Strings in Six-dimensional SCFTs","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Guglielmo Lockhart, Michele Del Zotto","submitted_at":"2018-04-25T17:42:20Z","abstract_excerpt":"In theories with extended supersymmetry the protected observables of UV superconformal fixed points are found in a number of contexts to be encoded in the BPS solitons along an IR Coulomb-like phase. For six-dimensional SCFTs such a role is played by the BPS strings on the tensorial Coulomb branch. In this paper we develop a uniform description of the worldsheet theories of a BPS string for rank-one 6d SCFTs. These strings are the basic constituents of the BPS string spectrum of arbitrary rank six-dimensional models, which they generate by forming bound states. Motivated by geometric engineeri"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1804.09694","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":""},"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":"1804.09694","created_at":"2026-05-18T00:04:58.747429+00:00"},{"alias_kind":"arxiv_version","alias_value":"1804.09694v3","created_at":"2026-05-18T00:04:58.747429+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1804.09694","created_at":"2026-05-18T00:04:58.747429+00:00"},{"alias_kind":"pith_short_12","alias_value":"4DNKGPUTMXHG","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_16","alias_value":"4DNKGPUTMXHGSRLO","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_8","alias_value":"4DNKGPUT","created_at":"2026-05-18T12:32:05.422762+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2605.16497","citing_title":"5d Trinions and Tetraons","ref_index":62,"is_internal_anchor":true},{"citing_arxiv_id":"2605.12594","citing_title":"String probes, simple currents, and the no global symmetries conjecture","ref_index":39,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4DNKGPUTMXHGSRLOUDXOK2EB2A","json":"https://pith.science/pith/4DNKGPUTMXHGSRLOUDXOK2EB2A.json","graph_json":"https://pith.science/api/pith-number/4DNKGPUTMXHGSRLOUDXOK2EB2A/graph.json","events_json":"https://pith.science/api/pith-number/4DNKGPUTMXHGSRLOUDXOK2EB2A/events.json","paper":"https://pith.science/paper/4DNKGPUT"},"agent_actions":{"view_html":"https://pith.science/pith/4DNKGPUTMXHGSRLOUDXOK2EB2A","download_json":"https://pith.science/pith/4DNKGPUTMXHGSRLOUDXOK2EB2A.json","view_paper":"https://pith.science/paper/4DNKGPUT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1804.09694&json=true","fetch_graph":"https://pith.science/api/pith-number/4DNKGPUTMXHGSRLOUDXOK2EB2A/graph.json","fetch_events":"https://pith.science/api/pith-number/4DNKGPUTMXHGSRLOUDXOK2EB2A/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4DNKGPUTMXHGSRLOUDXOK2EB2A/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4DNKGPUTMXHGSRLOUDXOK2EB2A/action/storage_attestation","attest_author":"https://pith.science/pith/4DNKGPUTMXHGSRLOUDXOK2EB2A/action/author_attestation","sign_citation":"https://pith.science/pith/4DNKGPUTMXHGSRLOUDXOK2EB2A/action/citation_signature","submit_replication":"https://pith.science/pith/4DNKGPUTMXHGSRLOUDXOK2EB2A/action/replication_record"}},"created_at":"2026-05-18T00:04:58.747429+00:00","updated_at":"2026-05-18T00:04:58.747429+00:00"}