{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:JE7GM5L5DFSTRD52QOFV6NDK4V","short_pith_number":"pith:JE7GM5L5","schema_version":"1.0","canonical_sha256":"493e66757d1965388fba838b5f346ae547b846260c9fd2f74a633c8905c3551a","source":{"kind":"arxiv","id":"1708.09673","version":2},"attestation_state":"computed","paper":{"title":"Condition on Ramond-Ramond fluxes for factorization of worldsheet scattering in anti-de Sitter space","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Linus Wulff","submitted_at":"2017-08-31T11:28:59Z","abstract_excerpt":"Factorization of scattering is the hallmark of integrable 1+1 dimensional quantum field theories. For factorization of scattering to be possible the set of masses and momenta must be conserved in any two-to-two scattering process. We use this fact to constrain the form of the Ramond-Ramond fluxes for integrable supergravity anti-de Sitter backgrounds by analysing tree-level scattering of two AdS bosons into two fermions on the worldsheet of a BMN string. We find a condition which can be efficiently used to rule out integrability of AdS strings and therefore of the corresponding AdS/CFT dualiti"},"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":"1708.09673","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-08-31T11:28:59Z","cross_cats_sorted":[],"title_canon_sha256":"e854e8bc95a7b5de3463d8bf02b561fa722312940b5301acc000569c756dbcd1","abstract_canon_sha256":"6712eafeecffb7800b0bde56a7f5d9f3928fd197a3f9c98d7eded7111faa07f3"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:29:29.058768Z","signature_b64":"OTvqUDkCDxhTXID8OZ53LXKWH/Q+un6vik4bwzj7FN1ZyvhQ8AMxQpwcDUWUeaST9ek9Tloc2mKWonQYJjmfCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"493e66757d1965388fba838b5f346ae547b846260c9fd2f74a633c8905c3551a","last_reissued_at":"2026-05-18T00:29:29.058247Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:29:29.058247Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Condition on Ramond-Ramond fluxes for factorization of worldsheet scattering in anti-de Sitter space","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Linus Wulff","submitted_at":"2017-08-31T11:28:59Z","abstract_excerpt":"Factorization of scattering is the hallmark of integrable 1+1 dimensional quantum field theories. For factorization of scattering to be possible the set of masses and momenta must be conserved in any two-to-two scattering process. We use this fact to constrain the form of the Ramond-Ramond fluxes for integrable supergravity anti-de Sitter backgrounds by analysing tree-level scattering of two AdS bosons into two fermions on the worldsheet of a BMN string. We find a condition which can be efficiently used to rule out integrability of AdS strings and therefore of the corresponding AdS/CFT dualiti"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1708.09673","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":""},"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":"1708.09673","created_at":"2026-05-18T00:29:29.058332+00:00"},{"alias_kind":"arxiv_version","alias_value":"1708.09673v2","created_at":"2026-05-18T00:29:29.058332+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1708.09673","created_at":"2026-05-18T00:29:29.058332+00:00"},{"alias_kind":"pith_short_12","alias_value":"JE7GM5L5DFST","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_16","alias_value":"JE7GM5L5DFSTRD52","created_at":"2026-05-18T12:31:24.725408+00:00"},{"alias_kind":"pith_short_8","alias_value":"JE7GM5L5","created_at":"2026-05-18T12:31:24.725408+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.12257","citing_title":"Evidence for a $4$-dimensional $\\mathcal{N}=1$ integrable quiver in massive type IIA","ref_index":34,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JE7GM5L5DFSTRD52QOFV6NDK4V","json":"https://pith.science/pith/JE7GM5L5DFSTRD52QOFV6NDK4V.json","graph_json":"https://pith.science/api/pith-number/JE7GM5L5DFSTRD52QOFV6NDK4V/graph.json","events_json":"https://pith.science/api/pith-number/JE7GM5L5DFSTRD52QOFV6NDK4V/events.json","paper":"https://pith.science/paper/JE7GM5L5"},"agent_actions":{"view_html":"https://pith.science/pith/JE7GM5L5DFSTRD52QOFV6NDK4V","download_json":"https://pith.science/pith/JE7GM5L5DFSTRD52QOFV6NDK4V.json","view_paper":"https://pith.science/paper/JE7GM5L5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1708.09673&json=true","fetch_graph":"https://pith.science/api/pith-number/JE7GM5L5DFSTRD52QOFV6NDK4V/graph.json","fetch_events":"https://pith.science/api/pith-number/JE7GM5L5DFSTRD52QOFV6NDK4V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JE7GM5L5DFSTRD52QOFV6NDK4V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JE7GM5L5DFSTRD52QOFV6NDK4V/action/storage_attestation","attest_author":"https://pith.science/pith/JE7GM5L5DFSTRD52QOFV6NDK4V/action/author_attestation","sign_citation":"https://pith.science/pith/JE7GM5L5DFSTRD52QOFV6NDK4V/action/citation_signature","submit_replication":"https://pith.science/pith/JE7GM5L5DFSTRD52QOFV6NDK4V/action/replication_record"}},"created_at":"2026-05-18T00:29:29.058332+00:00","updated_at":"2026-05-18T00:29:29.058332+00:00"}