{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:OFVAK6MQ7HQ2QKGW3OGXAVJA7W","short_pith_number":"pith:OFVAK6MQ","schema_version":"1.0","canonical_sha256":"716a057990f9e1a828d6db8d705520fd84137ebe59c1c701d5a50a137b494693","source":{"kind":"arxiv","id":"1908.01913","version":2},"attestation_state":"computed","paper":{"title":"Heterotic-$\\mathbf{F}$-theory Duality with Wilson Line Symmetry-breaking","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Herbert Clemens, Stuart Raby","submitted_at":"2019-08-06T00:43:22Z","abstract_excerpt":"We begin with an $E_{8}\\times E_{8}$ Heterotic model broken to an $SU(5)_{gauge}$ and a mirror $SU(5)_{gauge}$, where one $SU(5)$ and its spectrum is identified as the visible sector while the other can be identified as a hidden mirror world. In both cases we obtain the minimal supersymmetric standard model spectrum after Wilson-line symmetry-breaking enhanced by a low energy R-parity enforced by a local (or global) $U(1)_{X}$-symmetry. Using Heterotic/$F$-theory duality, we show how to eliminate the vector-like exotics which were obtained in previous constructions. In these constructions, the"},"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":"1908.01913","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-08-06T00:43:22Z","cross_cats_sorted":["math-ph","math.MP"],"title_canon_sha256":"a470018ae70bcc239dab26f37b2f05d61358fc36d8c929272e5b8455a64a0df9","abstract_canon_sha256":"c03932df07e40a69eed592ac153212a6db38dc32f0673088a585b62f3803a846"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:36:31.033418Z","signature_b64":"c/ahr/Dk+QXFmBesKFB81q81NVDLAdfXPICHRMEUkYwqpQsgqDcUqrrjGm4TLvCym486/y4eCB14iqIZcRlLAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"716a057990f9e1a828d6db8d705520fd84137ebe59c1c701d5a50a137b494693","last_reissued_at":"2026-07-05T00:36:31.032801Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:36:31.032801Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Heterotic-$\\mathbf{F}$-theory Duality with Wilson Line Symmetry-breaking","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Herbert Clemens, Stuart Raby","submitted_at":"2019-08-06T00:43:22Z","abstract_excerpt":"We begin with an $E_{8}\\times E_{8}$ Heterotic model broken to an $SU(5)_{gauge}$ and a mirror $SU(5)_{gauge}$, where one $SU(5)$ and its spectrum is identified as the visible sector while the other can be identified as a hidden mirror world. In both cases we obtain the minimal supersymmetric standard model spectrum after Wilson-line symmetry-breaking enhanced by a low energy R-parity enforced by a local (or global) $U(1)_{X}$-symmetry. Using Heterotic/$F$-theory duality, we show how to eliminate the vector-like exotics which were obtained in previous constructions. In these constructions, the"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1908.01913","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/1908.01913/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":"1908.01913","created_at":"2026-07-05T00:36:31.032862+00:00"},{"alias_kind":"arxiv_version","alias_value":"1908.01913v2","created_at":"2026-07-05T00:36:31.032862+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1908.01913","created_at":"2026-07-05T00:36:31.032862+00:00"},{"alias_kind":"pith_short_12","alias_value":"OFVAK6MQ7HQ2","created_at":"2026-07-05T00:36:31.032862+00:00"},{"alias_kind":"pith_short_16","alias_value":"OFVAK6MQ7HQ2QKGW","created_at":"2026-07-05T00:36:31.032862+00:00"},{"alias_kind":"pith_short_8","alias_value":"OFVAK6MQ","created_at":"2026-07-05T00:36:31.032862+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OFVAK6MQ7HQ2QKGW3OGXAVJA7W","json":"https://pith.science/pith/OFVAK6MQ7HQ2QKGW3OGXAVJA7W.json","graph_json":"https://pith.science/api/pith-number/OFVAK6MQ7HQ2QKGW3OGXAVJA7W/graph.json","events_json":"https://pith.science/api/pith-number/OFVAK6MQ7HQ2QKGW3OGXAVJA7W/events.json","paper":"https://pith.science/paper/OFVAK6MQ"},"agent_actions":{"view_html":"https://pith.science/pith/OFVAK6MQ7HQ2QKGW3OGXAVJA7W","download_json":"https://pith.science/pith/OFVAK6MQ7HQ2QKGW3OGXAVJA7W.json","view_paper":"https://pith.science/paper/OFVAK6MQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1908.01913&json=true","fetch_graph":"https://pith.science/api/pith-number/OFVAK6MQ7HQ2QKGW3OGXAVJA7W/graph.json","fetch_events":"https://pith.science/api/pith-number/OFVAK6MQ7HQ2QKGW3OGXAVJA7W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OFVAK6MQ7HQ2QKGW3OGXAVJA7W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OFVAK6MQ7HQ2QKGW3OGXAVJA7W/action/storage_attestation","attest_author":"https://pith.science/pith/OFVAK6MQ7HQ2QKGW3OGXAVJA7W/action/author_attestation","sign_citation":"https://pith.science/pith/OFVAK6MQ7HQ2QKGW3OGXAVJA7W/action/citation_signature","submit_replication":"https://pith.science/pith/OFVAK6MQ7HQ2QKGW3OGXAVJA7W/action/replication_record"}},"created_at":"2026-07-05T00:36:31.032862+00:00","updated_at":"2026-07-05T00:36:31.032862+00:00"}