{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:LVJJMSRVUIPDNPLWQJ54MLVIPO","short_pith_number":"pith:LVJJMSRV","schema_version":"1.0","canonical_sha256":"5d52964a35a21e36bd76827bc62ea87b8404a48c54ea688eb4c65ec2096604a5","source":{"kind":"arxiv","id":"2011.00024","version":3},"attestation_state":"computed","paper":{"title":"Quantum Corrections in 4d N=1 Infinite Distance Limits and the Weak Gravity Conjecture","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daniel Klaewer, Max Wiesner, Seung-Joo Lee, Timo Weigand","submitted_at":"2020-10-30T18:07:26Z","abstract_excerpt":"We study quantum corrections in four-dimensional theories with $N=1$ supersymmetry in the context of Quantum Gravity Conjectures. According to the Emergent String Conjecture, infinite distance limits in quantum gravity either lead to decompactification of the theory or result in a weakly coupled string theory. We verify this conjecture in the framework of $N=1$ supersymmetric F-theory compactifications to four dimensions including perturbative $\\alpha'$ as well as non-perturbative corrections. After proving uniqueness of the emergent critical string at the classical level, we show that quantum"},"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":"2011.00024","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2020-10-30T18:07:26Z","cross_cats_sorted":[],"title_canon_sha256":"a776b74367cb0be5cb3afcf5a6d3b0bf6e2306a2d2323f88f22096b605409351","abstract_canon_sha256":"b7fd04250de5556c02a06b321eaff0eb24e275a31d3d04ca616ddeefb3c5bec6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:31:44.522255Z","signature_b64":"OMIHCKTD+JqRUy1Sxf7OIpRKkejKVi32w2tQz9Uq07Drj70348M+7NIATHYODN32NFLdL8ncaFGLPSni1rscAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5d52964a35a21e36bd76827bc62ea87b8404a48c54ea688eb4c65ec2096604a5","last_reissued_at":"2026-07-05T02:31:44.521762Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:31:44.521762Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum Corrections in 4d N=1 Infinite Distance Limits and the Weak Gravity Conjecture","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Daniel Klaewer, Max Wiesner, Seung-Joo Lee, Timo Weigand","submitted_at":"2020-10-30T18:07:26Z","abstract_excerpt":"We study quantum corrections in four-dimensional theories with $N=1$ supersymmetry in the context of Quantum Gravity Conjectures. According to the Emergent String Conjecture, infinite distance limits in quantum gravity either lead to decompactification of the theory or result in a weakly coupled string theory. We verify this conjecture in the framework of $N=1$ supersymmetric F-theory compactifications to four dimensions including perturbative $\\alpha'$ as well as non-perturbative corrections. After proving uniqueness of the emergent critical string at the classical level, we show that quantum"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2011.00024","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/2011.00024/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":"2011.00024","created_at":"2026-07-05T02:31:44.521822+00:00"},{"alias_kind":"arxiv_version","alias_value":"2011.00024v3","created_at":"2026-07-05T02:31:44.521822+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2011.00024","created_at":"2026-07-05T02:31:44.521822+00:00"},{"alias_kind":"pith_short_12","alias_value":"LVJJMSRVUIPD","created_at":"2026-07-05T02:31:44.521822+00:00"},{"alias_kind":"pith_short_16","alias_value":"LVJJMSRVUIPDNPLW","created_at":"2026-07-05T02:31:44.521822+00:00"},{"alias_kind":"pith_short_8","alias_value":"LVJJMSRV","created_at":"2026-07-05T02:31:44.521822+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":7,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.19440","citing_title":"Moduli Stabilisation for ADD and the Dark Dimension Scenario","ref_index":55,"is_internal_anchor":false},{"citing_arxiv_id":"2605.26212","citing_title":"EFTs with Symmetric Moduli Spaces: the Landscape and the Swampland","ref_index":43,"is_internal_anchor":false},{"citing_arxiv_id":"2105.09326","citing_title":"F-theory flux vacua at large complex structure","ref_index":65,"is_internal_anchor":false},{"citing_arxiv_id":"2404.07980","citing_title":"ISCOs and the weak gravity conjecture bound in higher derivative theories of gravity","ref_index":36,"is_internal_anchor":false},{"citing_arxiv_id":"2601.08909","citing_title":"The CFT Distance Conjecture and Tensionless String Limits in $\\mathcal N=2$ Quiver Gauge Theories","ref_index":14,"is_internal_anchor":false},{"citing_arxiv_id":"2603.11163","citing_title":"Alice in Warpland: KK modes, Warped Compactifications and the Swampland","ref_index":50,"is_internal_anchor":false},{"citing_arxiv_id":"2603.12315","citing_title":"Quantum obstructions for $N=1$ infinite distance limits -- Part I: $g_s$ obstructions","ref_index":40,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LVJJMSRVUIPDNPLWQJ54MLVIPO","json":"https://pith.science/pith/LVJJMSRVUIPDNPLWQJ54MLVIPO.json","graph_json":"https://pith.science/api/pith-number/LVJJMSRVUIPDNPLWQJ54MLVIPO/graph.json","events_json":"https://pith.science/api/pith-number/LVJJMSRVUIPDNPLWQJ54MLVIPO/events.json","paper":"https://pith.science/paper/LVJJMSRV"},"agent_actions":{"view_html":"https://pith.science/pith/LVJJMSRVUIPDNPLWQJ54MLVIPO","download_json":"https://pith.science/pith/LVJJMSRVUIPDNPLWQJ54MLVIPO.json","view_paper":"https://pith.science/paper/LVJJMSRV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2011.00024&json=true","fetch_graph":"https://pith.science/api/pith-number/LVJJMSRVUIPDNPLWQJ54MLVIPO/graph.json","fetch_events":"https://pith.science/api/pith-number/LVJJMSRVUIPDNPLWQJ54MLVIPO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LVJJMSRVUIPDNPLWQJ54MLVIPO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LVJJMSRVUIPDNPLWQJ54MLVIPO/action/storage_attestation","attest_author":"https://pith.science/pith/LVJJMSRVUIPDNPLWQJ54MLVIPO/action/author_attestation","sign_citation":"https://pith.science/pith/LVJJMSRVUIPDNPLWQJ54MLVIPO/action/citation_signature","submit_replication":"https://pith.science/pith/LVJJMSRVUIPDNPLWQJ54MLVIPO/action/replication_record"}},"created_at":"2026-07-05T02:31:44.521822+00:00","updated_at":"2026-07-05T02:31:44.521822+00:00"}