{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:OGCHJ7Y7RBDVBA66BJVHQPK4SI","short_pith_number":"pith:OGCHJ7Y7","schema_version":"1.0","canonical_sha256":"718474ff1f88475083de0a6a783d5c920b7d813b4548c8d9ae5381cb552b7df0","source":{"kind":"arxiv","id":"2210.10797","version":2},"attestation_state":"computed","paper":{"title":"Quantum Gravity Bounds on N=1 Effective Theories in Four Dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Luca Martucci, Nicolo Risso, Timo Weigand","submitted_at":"2022-10-19T18:00:02Z","abstract_excerpt":"We propose quantum gravitational constraints on effective four-dimensional theories with N=1 supersymmetry. These Swampland constraints arise by demanding consistency of the worldsheet theory of a class of axionic, or EFT, strings whose existence follows from the Completeness Conjecture of quantum gravity. Modulo certain assumptions, we derive positivity bounds and quantization conditions for the axionic couplings to the gauge and gravitational sector at the two- and four-derivative level, respectively. We furthermore obtain general bounds on the rank of the gauge sector in terms of the gravit"},"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":"2210.10797","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2022-10-19T18:00:02Z","cross_cats_sorted":[],"title_canon_sha256":"54af6655db1708dc0b7a14bcf8ccd4b7f036d926e981445c0550465798f9269d","abstract_canon_sha256":"4d6beff1953575daef1c11f2d5fcee69dec5613e989882d28c6510393096d302"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:05:30.327521Z","signature_b64":"xONAfKJgQF37TLznMT2UdTwEC6SF78duhKAGEHHODgUyY+1lbqqJUZUZXk0BYISoKIGJqxppBteK+4CoePZRBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"718474ff1f88475083de0a6a783d5c920b7d813b4548c8d9ae5381cb552b7df0","last_reissued_at":"2026-07-05T06:05:30.327053Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:05:30.327053Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum Gravity Bounds on N=1 Effective Theories in Four Dimensions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Luca Martucci, Nicolo Risso, Timo Weigand","submitted_at":"2022-10-19T18:00:02Z","abstract_excerpt":"We propose quantum gravitational constraints on effective four-dimensional theories with N=1 supersymmetry. These Swampland constraints arise by demanding consistency of the worldsheet theory of a class of axionic, or EFT, strings whose existence follows from the Completeness Conjecture of quantum gravity. Modulo certain assumptions, we derive positivity bounds and quantization conditions for the axionic couplings to the gauge and gravitational sector at the two- and four-derivative level, respectively. We furthermore obtain general bounds on the rank of the gauge sector in terms of the gravit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.10797","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/2210.10797/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":"2210.10797","created_at":"2026-07-05T06:05:30.327104+00:00"},{"alias_kind":"arxiv_version","alias_value":"2210.10797v2","created_at":"2026-07-05T06:05:30.327104+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.10797","created_at":"2026-07-05T06:05:30.327104+00:00"},{"alias_kind":"pith_short_12","alias_value":"OGCHJ7Y7RBDV","created_at":"2026-07-05T06:05:30.327104+00:00"},{"alias_kind":"pith_short_16","alias_value":"OGCHJ7Y7RBDVBA66","created_at":"2026-07-05T06:05:30.327104+00:00"},{"alias_kind":"pith_short_8","alias_value":"OGCHJ7Y7","created_at":"2026-07-05T06:05:30.327104+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.26004","citing_title":"Non-invertible symmetries in the axiverse, and the imaginary wormholes","ref_index":61,"is_internal_anchor":false},{"citing_arxiv_id":"2605.15276","citing_title":"Bordisms between 9d type IIB supergravities and commutator widths of duality groups","ref_index":206,"is_internal_anchor":false},{"citing_arxiv_id":"2605.15276","citing_title":"Bordisms between 9d type IIB supergravities and commutator widths of duality groups","ref_index":206,"is_internal_anchor":false},{"citing_arxiv_id":"2511.09613","citing_title":"Bounds on Discrete Gauge Symmetries in Supergravity","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2604.25988","citing_title":"On Quantum Obstructions in Type IIA Orientifolds","ref_index":9,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/OGCHJ7Y7RBDVBA66BJVHQPK4SI","json":"https://pith.science/pith/OGCHJ7Y7RBDVBA66BJVHQPK4SI.json","graph_json":"https://pith.science/api/pith-number/OGCHJ7Y7RBDVBA66BJVHQPK4SI/graph.json","events_json":"https://pith.science/api/pith-number/OGCHJ7Y7RBDVBA66BJVHQPK4SI/events.json","paper":"https://pith.science/paper/OGCHJ7Y7"},"agent_actions":{"view_html":"https://pith.science/pith/OGCHJ7Y7RBDVBA66BJVHQPK4SI","download_json":"https://pith.science/pith/OGCHJ7Y7RBDVBA66BJVHQPK4SI.json","view_paper":"https://pith.science/paper/OGCHJ7Y7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2210.10797&json=true","fetch_graph":"https://pith.science/api/pith-number/OGCHJ7Y7RBDVBA66BJVHQPK4SI/graph.json","fetch_events":"https://pith.science/api/pith-number/OGCHJ7Y7RBDVBA66BJVHQPK4SI/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/OGCHJ7Y7RBDVBA66BJVHQPK4SI/action/timestamp_anchor","attest_storage":"https://pith.science/pith/OGCHJ7Y7RBDVBA66BJVHQPK4SI/action/storage_attestation","attest_author":"https://pith.science/pith/OGCHJ7Y7RBDVBA66BJVHQPK4SI/action/author_attestation","sign_citation":"https://pith.science/pith/OGCHJ7Y7RBDVBA66BJVHQPK4SI/action/citation_signature","submit_replication":"https://pith.science/pith/OGCHJ7Y7RBDVBA66BJVHQPK4SI/action/replication_record"}},"created_at":"2026-07-05T06:05:30.327104+00:00","updated_at":"2026-07-05T06:05:30.327104+00:00"}