{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:SLAV3FVUQ6VU3BJELBJLBYDV5B","short_pith_number":"pith:SLAV3FVU","schema_version":"1.0","canonical_sha256":"92c15d96b487ab4d85245852b0e075e84ca9013cbaf12d95a74ebe556e79286c","source":{"kind":"arxiv","id":"2401.06114","version":1},"attestation_state":"computed","paper":{"title":"Computing NMHV Gravity Amplitudes at Infinity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dawit Belayneh, Freddy Cachazo, Pablo Leon","submitted_at":"2024-01-11T18:49:06Z","abstract_excerpt":"In this note we show how the solutions to the scattering equations in the NMHV sector fully decompose into subsectors in the $z\\to \\infty$ limit of a Risager deformation. Each subsector is characterized by the punctures that coalesce in the limit. This naturally decomposes the $E(n-3,1)$ solutions into sets characterized by partitions of $n-3$ elements so that exactly one subset has more than one element. We present analytic expressions for the leading order of the solutions in an expansion around infinite $z$ for any $n$. We also give a simple algorithm for numerically computing arbitrarily h"},"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":"2401.06114","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2024-01-11T18:49:06Z","cross_cats_sorted":[],"title_canon_sha256":"5e2af1b1cddc05fa0e61b297c678c8bcbc57d812f49cb42356fb5e10d7bbe0a6","abstract_canon_sha256":"118ad1944ab5e01cd07c1c9715438eb2421a9dbf6c154e376141474db3126c79"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:32:40.608128Z","signature_b64":"o7RblxEeyrP4u0v28fqip8KZIawwOM1SHzVmvY95F9NVT8kVcnfwLejeAU8bgnizxxPhaNZMh47Vp6f6Rg+yBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"92c15d96b487ab4d85245852b0e075e84ca9013cbaf12d95a74ebe556e79286c","last_reissued_at":"2026-07-05T07:32:40.607456Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:32:40.607456Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Computing NMHV Gravity Amplitudes at Infinity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Dawit Belayneh, Freddy Cachazo, Pablo Leon","submitted_at":"2024-01-11T18:49:06Z","abstract_excerpt":"In this note we show how the solutions to the scattering equations in the NMHV sector fully decompose into subsectors in the $z\\to \\infty$ limit of a Risager deformation. Each subsector is characterized by the punctures that coalesce in the limit. This naturally decomposes the $E(n-3,1)$ solutions into sets characterized by partitions of $n-3$ elements so that exactly one subset has more than one element. We present analytic expressions for the leading order of the solutions in an expansion around infinite $z$ for any $n$. We also give a simple algorithm for numerically computing arbitrarily h"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2401.06114","kind":"arxiv","version":1},"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/2401.06114/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":"2401.06114","created_at":"2026-07-05T07:32:40.607666+00:00"},{"alias_kind":"arxiv_version","alias_value":"2401.06114v1","created_at":"2026-07-05T07:32:40.607666+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2401.06114","created_at":"2026-07-05T07:32:40.607666+00:00"},{"alias_kind":"pith_short_12","alias_value":"SLAV3FVUQ6VU","created_at":"2026-07-05T07:32:40.607666+00:00"},{"alias_kind":"pith_short_16","alias_value":"SLAV3FVUQ6VU3BJE","created_at":"2026-07-05T07:32:40.607666+00:00"},{"alias_kind":"pith_short_8","alias_value":"SLAV3FVU","created_at":"2026-07-05T07:32:40.607666+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/SLAV3FVUQ6VU3BJELBJLBYDV5B","json":"https://pith.science/pith/SLAV3FVUQ6VU3BJELBJLBYDV5B.json","graph_json":"https://pith.science/api/pith-number/SLAV3FVUQ6VU3BJELBJLBYDV5B/graph.json","events_json":"https://pith.science/api/pith-number/SLAV3FVUQ6VU3BJELBJLBYDV5B/events.json","paper":"https://pith.science/paper/SLAV3FVU"},"agent_actions":{"view_html":"https://pith.science/pith/SLAV3FVUQ6VU3BJELBJLBYDV5B","download_json":"https://pith.science/pith/SLAV3FVUQ6VU3BJELBJLBYDV5B.json","view_paper":"https://pith.science/paper/SLAV3FVU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2401.06114&json=true","fetch_graph":"https://pith.science/api/pith-number/SLAV3FVUQ6VU3BJELBJLBYDV5B/graph.json","fetch_events":"https://pith.science/api/pith-number/SLAV3FVUQ6VU3BJELBJLBYDV5B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SLAV3FVUQ6VU3BJELBJLBYDV5B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SLAV3FVUQ6VU3BJELBJLBYDV5B/action/storage_attestation","attest_author":"https://pith.science/pith/SLAV3FVUQ6VU3BJELBJLBYDV5B/action/author_attestation","sign_citation":"https://pith.science/pith/SLAV3FVUQ6VU3BJELBJLBYDV5B/action/citation_signature","submit_replication":"https://pith.science/pith/SLAV3FVUQ6VU3BJELBJLBYDV5B/action/replication_record"}},"created_at":"2026-07-05T07:32:40.607666+00:00","updated_at":"2026-07-05T07:32:40.607666+00:00"}