{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:EMHPKDH77E4BOIEWG7CJPVLHRK","short_pith_number":"pith:EMHPKDH7","schema_version":"1.0","canonical_sha256":"230ef50cfff93817209637c497d5678ab0f054ab706cf0b9da0ef2c62d9a7282","source":{"kind":"arxiv","id":"0705.0303","version":4},"attestation_state":"computed","paper":{"title":"Gluon scattering amplitudes at strong coupling","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Juan Maldacena, Luis F. Alday","submitted_at":"2007-05-02T19:44:54Z","abstract_excerpt":"We describe how to compute planar gluon scattering amplitudes at strong coupling in N=4 super Yang Mills by using the gauge/string duality. The computation boils down to finding a certain classical string configuration whose boundary conditions are determined by the gluon momenta. The results are infrared divergent. We introduce the gravity version of dimensional regularization to define finite quantities. The leading and subleading IR divergencies are characterized by two functions of the coupling that we compute at strong coupling. We compute also the full finite form for the four point ampl"},"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":"0705.0303","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2007-05-02T19:44:54Z","cross_cats_sorted":[],"title_canon_sha256":"b75d6d0fa770d796c42eba7dcf276afadab562b226816b21964ae1e877108ba2","abstract_canon_sha256":"b88967866e4b5837632cc1393a677b98683b7ca5a5643e3afbab55fd5681a418"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:03:28.038529Z","signature_b64":"KGSpkG/sQuFDElRcitEkqT8mVSXU6mYraxX6g7Es5wEQgZ/Qna5F4el8EpBTfs5KnDfhmlA7RmT3lCPQiH2IDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"230ef50cfff93817209637c497d5678ab0f054ab706cf0b9da0ef2c62d9a7282","last_reissued_at":"2026-07-04T17:03:28.038172Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:03:28.038172Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gluon scattering amplitudes at strong coupling","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Juan Maldacena, Luis F. Alday","submitted_at":"2007-05-02T19:44:54Z","abstract_excerpt":"We describe how to compute planar gluon scattering amplitudes at strong coupling in N=4 super Yang Mills by using the gauge/string duality. The computation boils down to finding a certain classical string configuration whose boundary conditions are determined by the gluon momenta. The results are infrared divergent. We introduce the gravity version of dimensional regularization to define finite quantities. The leading and subleading IR divergencies are characterized by two functions of the coupling that we compute at strong coupling. We compute also the full finite form for the four point ampl"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0705.0303","kind":"arxiv","version":4},"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/0705.0303/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":"0705.0303","created_at":"2026-07-04T17:03:28.038228+00:00"},{"alias_kind":"arxiv_version","alias_value":"0705.0303v4","created_at":"2026-07-04T17:03:28.038228+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0705.0303","created_at":"2026-07-04T17:03:28.038228+00:00"},{"alias_kind":"pith_short_12","alias_value":"EMHPKDH77E4B","created_at":"2026-07-04T17:03:28.038228+00:00"},{"alias_kind":"pith_short_16","alias_value":"EMHPKDH77E4BOIEW","created_at":"2026-07-04T17:03:28.038228+00:00"},{"alias_kind":"pith_short_8","alias_value":"EMHPKDH7","created_at":"2026-07-04T17:03:28.038228+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":10,"internal_anchor_count":7,"sample":[{"citing_arxiv_id":"2606.24018","citing_title":"Null limit of large-charge correlators in planar $\\mathcal{N}=4$ Super-Yang-Mills theory","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2606.20981","citing_title":"Gluon GTMD at strong coupling: fixed-spin saddle factorization and Reggeization","ref_index":76,"is_internal_anchor":true},{"citing_arxiv_id":"2606.08582","citing_title":"Soft Algebra for ${\\cal N}=4$ SYM","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2605.28926","citing_title":"Multi-Loop Negative Geometries","ref_index":9,"is_internal_anchor":true},{"citing_arxiv_id":"2605.16034","citing_title":"Walking Sudakov: From Cusp to Octagon","ref_index":93,"is_internal_anchor":true},{"citing_arxiv_id":"2605.17056","citing_title":"Five legs @ three loops: N=4 sYM amplitude near mass-shell","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2601.09707","citing_title":"Precision asymptotics of string amplitudes","ref_index":20,"is_internal_anchor":true},{"citing_arxiv_id":"2605.03887","citing_title":"Classical correlation functions at strong coupling from hexagonalization","ref_index":45,"is_internal_anchor":false},{"citing_arxiv_id":"2604.22683","citing_title":"Landau Analysis of One-Cycle Negative Geometries","ref_index":24,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21015","citing_title":"Form factors of $\\mathscr{N}=4$ self-dual Yang-Mills from the chiral algebra bootstrap","ref_index":29,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EMHPKDH77E4BOIEWG7CJPVLHRK","json":"https://pith.science/pith/EMHPKDH77E4BOIEWG7CJPVLHRK.json","graph_json":"https://pith.science/api/pith-number/EMHPKDH77E4BOIEWG7CJPVLHRK/graph.json","events_json":"https://pith.science/api/pith-number/EMHPKDH77E4BOIEWG7CJPVLHRK/events.json","paper":"https://pith.science/paper/EMHPKDH7"},"agent_actions":{"view_html":"https://pith.science/pith/EMHPKDH77E4BOIEWG7CJPVLHRK","download_json":"https://pith.science/pith/EMHPKDH77E4BOIEWG7CJPVLHRK.json","view_paper":"https://pith.science/paper/EMHPKDH7","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0705.0303&json=true","fetch_graph":"https://pith.science/api/pith-number/EMHPKDH77E4BOIEWG7CJPVLHRK/graph.json","fetch_events":"https://pith.science/api/pith-number/EMHPKDH77E4BOIEWG7CJPVLHRK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EMHPKDH77E4BOIEWG7CJPVLHRK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EMHPKDH77E4BOIEWG7CJPVLHRK/action/storage_attestation","attest_author":"https://pith.science/pith/EMHPKDH77E4BOIEWG7CJPVLHRK/action/author_attestation","sign_citation":"https://pith.science/pith/EMHPKDH77E4BOIEWG7CJPVLHRK/action/citation_signature","submit_replication":"https://pith.science/pith/EMHPKDH77E4BOIEWG7CJPVLHRK/action/replication_record"}},"created_at":"2026-07-04T17:03:28.038228+00:00","updated_at":"2026-07-04T17:03:28.038228+00:00"}