{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:DDK5STVTAKV2HWCY4G6VIPWY23","short_pith_number":"pith:DDK5STVT","schema_version":"1.0","canonical_sha256":"18d5d94eb302aba3d858e1bd543ed8d6dbb6915610c8e5051eeff9b0a33eb314","source":{"kind":"arxiv","id":"2408.06440","version":2},"attestation_state":"computed","paper":{"title":"Gravity and a universal cutoff for field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Simon Caron-Huot, Yue-Zhou Li","submitted_at":"2024-08-12T18:40:17Z","abstract_excerpt":"We analyze the one-loop effects of massive fields on 2-to-2 scattering processes involving gravitons. It has been suggested that in the presence of gravity, any local effective field theory description must break down at the \"species scale\". We first observe that unitarity and analyticity of the amplitude indeed imply a species-type bound $G\\Lambda^{d-2}N\\leq O(1)$, where $N$ counts parametrically light species and $\\Lambda$ is an energy scale above which new unknown ingredients must modify the graviton amplitude. To clarify what happens at this scale, we contrast the partial wave decompositio"},"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":"2408.06440","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-08-12T18:40:17Z","cross_cats_sorted":[],"title_canon_sha256":"cbf36700b062d0452c090fc66c0a4e6314da66a3e63dbe14b9a9636edd659216","abstract_canon_sha256":"8b113652d67fd114834ad0226dd00953409c245663e978314c41315a14031ab3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:58:46.601683Z","signature_b64":"GCpre9avnG/EPSCyxhlGRG9TPeMgtvpQa2wdjiNMgZGKh/MPLWnTR//KoBOs5ACQSQyvmjxH4+yb6fDbh921DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"18d5d94eb302aba3d858e1bd543ed8d6dbb6915610c8e5051eeff9b0a33eb314","last_reissued_at":"2026-07-05T08:58:46.601178Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:58:46.601178Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gravity and a universal cutoff for field theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Simon Caron-Huot, Yue-Zhou Li","submitted_at":"2024-08-12T18:40:17Z","abstract_excerpt":"We analyze the one-loop effects of massive fields on 2-to-2 scattering processes involving gravitons. It has been suggested that in the presence of gravity, any local effective field theory description must break down at the \"species scale\". We first observe that unitarity and analyticity of the amplitude indeed imply a species-type bound $G\\Lambda^{d-2}N\\leq O(1)$, where $N$ counts parametrically light species and $\\Lambda$ is an energy scale above which new unknown ingredients must modify the graviton amplitude. To clarify what happens at this scale, we contrast the partial wave decompositio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2408.06440","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/2408.06440/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":"2408.06440","created_at":"2026-07-05T08:58:46.601244+00:00"},{"alias_kind":"arxiv_version","alias_value":"2408.06440v2","created_at":"2026-07-05T08:58:46.601244+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2408.06440","created_at":"2026-07-05T08:58:46.601244+00:00"},{"alias_kind":"pith_short_12","alias_value":"DDK5STVTAKV2","created_at":"2026-07-05T08:58:46.601244+00:00"},{"alias_kind":"pith_short_16","alias_value":"DDK5STVTAKV2HWCY","created_at":"2026-07-05T08:58:46.601244+00:00"},{"alias_kind":"pith_short_8","alias_value":"DDK5STVT","created_at":"2026-07-05T08:58:46.601244+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":13,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.19283","citing_title":"A Dispersive Bootstrap for the Virasoro-Shapiro Amplitude","ref_index":55,"is_internal_anchor":false},{"citing_arxiv_id":"2606.08244","citing_title":"Stochastic Survival near Swampland Boundaries","ref_index":40,"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":167,"is_internal_anchor":false},{"citing_arxiv_id":"2411.01105","citing_title":"UV Effects and Short-Lived Hawking Radiation: Alternative Resolution of Information Paradox","ref_index":107,"is_internal_anchor":false},{"citing_arxiv_id":"2605.21582","citing_title":"Multipositivity Constrains the Chiral Lagrangian","ref_index":114,"is_internal_anchor":false},{"citing_arxiv_id":"2506.22546","citing_title":"Primal S-matrix bootstrap with dispersion relations","ref_index":60,"is_internal_anchor":false},{"citing_arxiv_id":"2605.20319","citing_title":"The Equivalence Principle at High Energies Completes the Spectrum","ref_index":106,"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":167,"is_internal_anchor":false},{"citing_arxiv_id":"2509.06630","citing_title":"Positivity bounds from thermal field theory entropy","ref_index":51,"is_internal_anchor":false},{"citing_arxiv_id":"2603.11163","citing_title":"Alice in Warpland: KK modes, Warped Compactifications and the Swampland","ref_index":142,"is_internal_anchor":false},{"citing_arxiv_id":"2603.15755","citing_title":"Negative running of gravitational positivity","ref_index":11,"is_internal_anchor":false},{"citing_arxiv_id":"2604.15235","citing_title":"Sampling the Graviton Pole and Deprojecting the Swampland","ref_index":53,"is_internal_anchor":false},{"citing_arxiv_id":"2605.04152","citing_title":"Consistent Scattering Amplitudes, Yang-Mills, the Higgs Mechanism and the EFTs Beyond","ref_index":43,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DDK5STVTAKV2HWCY4G6VIPWY23","json":"https://pith.science/pith/DDK5STVTAKV2HWCY4G6VIPWY23.json","graph_json":"https://pith.science/api/pith-number/DDK5STVTAKV2HWCY4G6VIPWY23/graph.json","events_json":"https://pith.science/api/pith-number/DDK5STVTAKV2HWCY4G6VIPWY23/events.json","paper":"https://pith.science/paper/DDK5STVT"},"agent_actions":{"view_html":"https://pith.science/pith/DDK5STVTAKV2HWCY4G6VIPWY23","download_json":"https://pith.science/pith/DDK5STVTAKV2HWCY4G6VIPWY23.json","view_paper":"https://pith.science/paper/DDK5STVT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2408.06440&json=true","fetch_graph":"https://pith.science/api/pith-number/DDK5STVTAKV2HWCY4G6VIPWY23/graph.json","fetch_events":"https://pith.science/api/pith-number/DDK5STVTAKV2HWCY4G6VIPWY23/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DDK5STVTAKV2HWCY4G6VIPWY23/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DDK5STVTAKV2HWCY4G6VIPWY23/action/storage_attestation","attest_author":"https://pith.science/pith/DDK5STVTAKV2HWCY4G6VIPWY23/action/author_attestation","sign_citation":"https://pith.science/pith/DDK5STVTAKV2HWCY4G6VIPWY23/action/citation_signature","submit_replication":"https://pith.science/pith/DDK5STVTAKV2HWCY4G6VIPWY23/action/replication_record"}},"created_at":"2026-07-05T08:58:46.601244+00:00","updated_at":"2026-07-05T08:58:46.601244+00:00"}