{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:Y2FE6G2MTFYDZ6VSNQNVUBXMAE","short_pith_number":"pith:Y2FE6G2M","schema_version":"1.0","canonical_sha256":"c68a4f1b4c99703cfab26c1b5a06ec013ec47be98d2a65a840b13b451a7e9d33","source":{"kind":"arxiv","id":"1203.1329","version":4},"attestation_state":"computed","paper":{"title":"On higher derivative corrections to Wess-Zumino and Tachyonic actions in type II super string theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ehsan Hatefi","submitted_at":"2012-03-06T21:05:34Z","abstract_excerpt":"We evaluate in detail the string scattering amplitude to compute different interactions of two massless scalars, one tachyon and one closed string Ramond-Ramond field in type II super string theory. In particular we find two scalar field and two tachyon couplings to all orders of $\\alpha'$ up to on-shell ambiguity. We then obtain the momentum expansion of this amplitude and apply this infinite number of couplings to actually check that the infinite number of tachyon poles of S-matrix element of this amplitude for the $p=n$ case (where $p$ is the spatial dimension of a D$_p$-brane and $n$ is 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":"1203.1329","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-03-06T21:05:34Z","cross_cats_sorted":[],"title_canon_sha256":"2c9659f3d37d71b8637a83de6e2ad01b8a6994db806d68e53cd88edb8b1e4a0b","abstract_canon_sha256":"65b20f47ed4f51409d112878b6d2465985169e4f6f6237faf1d9f4e19be8f61d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:27:43.314342Z","signature_b64":"0O2oPdFX6h+PcFCV7MQ6Glf/EdfQGM5kW0YIpLL1zp5HmWZAbxgbEscgOC6B3p/8xS01EcEwbLPDMela4KBUCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c68a4f1b4c99703cfab26c1b5a06ec013ec47be98d2a65a840b13b451a7e9d33","last_reissued_at":"2026-05-18T03:27:43.313684Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:27:43.313684Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On higher derivative corrections to Wess-Zumino and Tachyonic actions in type II super string theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Ehsan Hatefi","submitted_at":"2012-03-06T21:05:34Z","abstract_excerpt":"We evaluate in detail the string scattering amplitude to compute different interactions of two massless scalars, one tachyon and one closed string Ramond-Ramond field in type II super string theory. In particular we find two scalar field and two tachyon couplings to all orders of $\\alpha'$ up to on-shell ambiguity. We then obtain the momentum expansion of this amplitude and apply this infinite number of couplings to actually check that the infinite number of tachyon poles of S-matrix element of this amplitude for the $p=n$ case (where $p$ is the spatial dimension of a D$_p$-brane and $n$ is th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1203.1329","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":""},"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":"1203.1329","created_at":"2026-05-18T03:27:43.313763+00:00"},{"alias_kind":"arxiv_version","alias_value":"1203.1329v4","created_at":"2026-05-18T03:27:43.313763+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1203.1329","created_at":"2026-05-18T03:27:43.313763+00:00"},{"alias_kind":"pith_short_12","alias_value":"Y2FE6G2MTFYD","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_16","alias_value":"Y2FE6G2MTFYDZ6VS","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_8","alias_value":"Y2FE6G2M","created_at":"2026-05-18T12:27:27.928770+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/Y2FE6G2MTFYDZ6VSNQNVUBXMAE","json":"https://pith.science/pith/Y2FE6G2MTFYDZ6VSNQNVUBXMAE.json","graph_json":"https://pith.science/api/pith-number/Y2FE6G2MTFYDZ6VSNQNVUBXMAE/graph.json","events_json":"https://pith.science/api/pith-number/Y2FE6G2MTFYDZ6VSNQNVUBXMAE/events.json","paper":"https://pith.science/paper/Y2FE6G2M"},"agent_actions":{"view_html":"https://pith.science/pith/Y2FE6G2MTFYDZ6VSNQNVUBXMAE","download_json":"https://pith.science/pith/Y2FE6G2MTFYDZ6VSNQNVUBXMAE.json","view_paper":"https://pith.science/paper/Y2FE6G2M","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1203.1329&json=true","fetch_graph":"https://pith.science/api/pith-number/Y2FE6G2MTFYDZ6VSNQNVUBXMAE/graph.json","fetch_events":"https://pith.science/api/pith-number/Y2FE6G2MTFYDZ6VSNQNVUBXMAE/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Y2FE6G2MTFYDZ6VSNQNVUBXMAE/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Y2FE6G2MTFYDZ6VSNQNVUBXMAE/action/storage_attestation","attest_author":"https://pith.science/pith/Y2FE6G2MTFYDZ6VSNQNVUBXMAE/action/author_attestation","sign_citation":"https://pith.science/pith/Y2FE6G2MTFYDZ6VSNQNVUBXMAE/action/citation_signature","submit_replication":"https://pith.science/pith/Y2FE6G2MTFYDZ6VSNQNVUBXMAE/action/replication_record"}},"created_at":"2026-05-18T03:27:43.313763+00:00","updated_at":"2026-05-18T03:27:43.313763+00:00"}