{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:7VFWYNGGYR55CYMQCCQBGLLFLW","short_pith_number":"pith:7VFWYNGG","schema_version":"1.0","canonical_sha256":"fd4b6c34c6c47bd1619010a0132d655d846b21a4f471d426e05496d6ff83a483","source":{"kind":"arxiv","id":"hep-th/0404134","version":2},"attestation_state":"computed","paper":{"title":"Scattering of Gauge, Matter, and Moduli Fields from Intersecting Branes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. Lust, P. Mayr, R. Richter, S. Stieberger","submitted_at":"2004-04-19T19:57:33Z","abstract_excerpt":"We calculate various tree-level (disk) scattering amplitudes involving gauge, matter and moduli fields in type IIB toroidal orbifold/orientifold backgrounds with D9,D5 respectively D7,D3-branes or via T-duality D6-branes in type IIA compactifications. In type IIB the D-branes may have non-vanishing fluxes on their world-volume. From these results we extract the moduli and flux dependence of the tree-level gauge couplings, the metrics for the moduli and matter fields. The non-vanishing fluxes correspond in the T-dual type IIA description to intersecting D6-branes. This allows us to determine th"},"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":"hep-th/0404134","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-04-19T19:57:33Z","cross_cats_sorted":[],"title_canon_sha256":"a1ac34c8f0a8da6141e44fda4ba704a132ccc458bb82ce7eb68c07dd324ab6e1","abstract_canon_sha256":"27c2dcc4b7fedc5317e38d8170dae712cf21096995e3f3fa109d3def7dee2f3b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:20:28.731372Z","signature_b64":"/g+uxlsJGpGgDdL3iDXtblPrvMfROJ+7NEn4uU1t/LmQX8zWBnt518iaU7yytnQ1S9ZpNG/NNTwlpuryMk3+CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fd4b6c34c6c47bd1619010a0132d655d846b21a4f471d426e05496d6ff83a483","last_reissued_at":"2026-07-04T15:20:28.730957Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:20:28.730957Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Scattering of Gauge, Matter, and Moduli Fields from Intersecting Branes","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"D. Lust, P. Mayr, R. Richter, S. Stieberger","submitted_at":"2004-04-19T19:57:33Z","abstract_excerpt":"We calculate various tree-level (disk) scattering amplitudes involving gauge, matter and moduli fields in type IIB toroidal orbifold/orientifold backgrounds with D9,D5 respectively D7,D3-branes or via T-duality D6-branes in type IIA compactifications. In type IIB the D-branes may have non-vanishing fluxes on their world-volume. From these results we extract the moduli and flux dependence of the tree-level gauge couplings, the metrics for the moduli and matter fields. The non-vanishing fluxes correspond in the T-dual type IIA description to intersecting D6-branes. This allows us to determine th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0404134","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/hep-th/0404134/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":"hep-th/0404134","created_at":"2026-07-04T15:20:28.731017+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0404134v2","created_at":"2026-07-04T15:20:28.731017+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0404134","created_at":"2026-07-04T15:20:28.731017+00:00"},{"alias_kind":"pith_short_12","alias_value":"7VFWYNGGYR55","created_at":"2026-07-04T15:20:28.731017+00:00"},{"alias_kind":"pith_short_16","alias_value":"7VFWYNGGYR55CYMQ","created_at":"2026-07-04T15:20:28.731017+00:00"},{"alias_kind":"pith_short_8","alias_value":"7VFWYNGG","created_at":"2026-07-04T15:20:28.731017+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2512.21141","citing_title":"Three-Family Supersymmetric Pati-Salam Flux Models from Rigid D-Branes","ref_index":34,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/7VFWYNGGYR55CYMQCCQBGLLFLW","json":"https://pith.science/pith/7VFWYNGGYR55CYMQCCQBGLLFLW.json","graph_json":"https://pith.science/api/pith-number/7VFWYNGGYR55CYMQCCQBGLLFLW/graph.json","events_json":"https://pith.science/api/pith-number/7VFWYNGGYR55CYMQCCQBGLLFLW/events.json","paper":"https://pith.science/paper/7VFWYNGG"},"agent_actions":{"view_html":"https://pith.science/pith/7VFWYNGGYR55CYMQCCQBGLLFLW","download_json":"https://pith.science/pith/7VFWYNGGYR55CYMQCCQBGLLFLW.json","view_paper":"https://pith.science/paper/7VFWYNGG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0404134&json=true","fetch_graph":"https://pith.science/api/pith-number/7VFWYNGGYR55CYMQCCQBGLLFLW/graph.json","fetch_events":"https://pith.science/api/pith-number/7VFWYNGGYR55CYMQCCQBGLLFLW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7VFWYNGGYR55CYMQCCQBGLLFLW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7VFWYNGGYR55CYMQCCQBGLLFLW/action/storage_attestation","attest_author":"https://pith.science/pith/7VFWYNGGYR55CYMQCCQBGLLFLW/action/author_attestation","sign_citation":"https://pith.science/pith/7VFWYNGGYR55CYMQCCQBGLLFLW/action/citation_signature","submit_replication":"https://pith.science/pith/7VFWYNGGYR55CYMQCCQBGLLFLW/action/replication_record"}},"created_at":"2026-07-04T15:20:28.731017+00:00","updated_at":"2026-07-04T15:20:28.731017+00:00"}