{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:PQN3X5XJQFWZ45SECPVHCSCU3X","short_pith_number":"pith:PQN3X5XJ","schema_version":"1.0","canonical_sha256":"7c1bbbf6e9816d9e764413ea714854ddf4b0639a8afe05baed62a2a937c7c4e1","source":{"kind":"arxiv","id":"hep-th/9910159","version":3},"attestation_state":"computed","paper":{"title":"Limits of the D-brane action","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Aleksandr Zheltukhin (Stockholm U., Kharkov IPT), Maxim Zabzine (Stockholm U.), Ulf Lindstrom","submitted_at":"1999-10-20T09:59:22Z","abstract_excerpt":"For background geometries whose metric contain a scale $\\gamma$ we reformulate the Born-Infeld\n D-brane action in terms of $\\epsilon \\equiv \\gamma /(2\\pi \\alpha ')$.\n This may be taken as a starting point for various perturbative treatments of the theory. We study two limits that arise at zeroth order of such perturbations. In the first limit, that corresponds to the $g_s\\to\\infty$ with $\\epsilon$ fix, we find a \"string parton\" picture, also in the presense of some background\n RR-fields. In the second limit, $\\epsilon\\to 0$, we find a topological model."},"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/9910159","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"1999-10-20T09:59:22Z","cross_cats_sorted":[],"title_canon_sha256":"d8dd593cea7d7bea9880025e290b8e9d678675e8f1a2b2eff0eb8b685e0a1ab7","abstract_canon_sha256":"a880b95ae48aa02ea83e69a1ffaa89c07590b7a1b105c8cf2a583315b33b2123"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:54.789272Z","signature_b64":"LS1To6ww8b1dyH4adnbipxqzMW6SMjcu4eXR4VtqJFgFIby6ZKRyq+oes+W0aK0MVsQNkEMzYPeH7kSLPR4tBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7c1bbbf6e9816d9e764413ea714854ddf4b0639a8afe05baed62a2a937c7c4e1","last_reissued_at":"2026-05-18T01:05:54.788732Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:54.788732Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Limits of the D-brane action","license":"","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Aleksandr Zheltukhin (Stockholm U., Kharkov IPT), Maxim Zabzine (Stockholm U.), Ulf Lindstrom","submitted_at":"1999-10-20T09:59:22Z","abstract_excerpt":"For background geometries whose metric contain a scale $\\gamma$ we reformulate the Born-Infeld\n D-brane action in terms of $\\epsilon \\equiv \\gamma /(2\\pi \\alpha ')$.\n This may be taken as a starting point for various perturbative treatments of the theory. We study two limits that arise at zeroth order of such perturbations. In the first limit, that corresponds to the $g_s\\to\\infty$ with $\\epsilon$ fix, we find a \"string parton\" picture, also in the presense of some background\n RR-fields. In the second limit, $\\epsilon\\to 0$, we find a topological model."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9910159","kind":"arxiv","version":3},"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":"hep-th/9910159","created_at":"2026-05-18T01:05:54.788818+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/9910159v3","created_at":"2026-05-18T01:05:54.788818+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/9910159","created_at":"2026-05-18T01:05:54.788818+00:00"},{"alias_kind":"pith_short_12","alias_value":"PQN3X5XJQFWZ","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_16","alias_value":"PQN3X5XJQFWZ45SE","created_at":"2026-05-18T12:25:49.631198+00:00"},{"alias_kind":"pith_short_8","alias_value":"PQN3X5XJ","created_at":"2026-05-18T12:25:49.631198+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/PQN3X5XJQFWZ45SECPVHCSCU3X","json":"https://pith.science/pith/PQN3X5XJQFWZ45SECPVHCSCU3X.json","graph_json":"https://pith.science/api/pith-number/PQN3X5XJQFWZ45SECPVHCSCU3X/graph.json","events_json":"https://pith.science/api/pith-number/PQN3X5XJQFWZ45SECPVHCSCU3X/events.json","paper":"https://pith.science/paper/PQN3X5XJ"},"agent_actions":{"view_html":"https://pith.science/pith/PQN3X5XJQFWZ45SECPVHCSCU3X","download_json":"https://pith.science/pith/PQN3X5XJQFWZ45SECPVHCSCU3X.json","view_paper":"https://pith.science/paper/PQN3X5XJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/9910159&json=true","fetch_graph":"https://pith.science/api/pith-number/PQN3X5XJQFWZ45SECPVHCSCU3X/graph.json","fetch_events":"https://pith.science/api/pith-number/PQN3X5XJQFWZ45SECPVHCSCU3X/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/PQN3X5XJQFWZ45SECPVHCSCU3X/action/timestamp_anchor","attest_storage":"https://pith.science/pith/PQN3X5XJQFWZ45SECPVHCSCU3X/action/storage_attestation","attest_author":"https://pith.science/pith/PQN3X5XJQFWZ45SECPVHCSCU3X/action/author_attestation","sign_citation":"https://pith.science/pith/PQN3X5XJQFWZ45SECPVHCSCU3X/action/citation_signature","submit_replication":"https://pith.science/pith/PQN3X5XJQFWZ45SECPVHCSCU3X/action/replication_record"}},"created_at":"2026-05-18T01:05:54.788818+00:00","updated_at":"2026-05-18T01:05:54.788818+00:00"}