{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:FO37Z4XJDAG6ETENAVE554EEGP","short_pith_number":"pith:FO37Z4XJ","schema_version":"1.0","canonical_sha256":"2bb7fcf2e9180de24c8d0549def08433f41faabdebe71528c2620d2c3a3d6632","source":{"kind":"arxiv","id":"1703.00024","version":3},"attestation_state":"computed","paper":{"title":"Subleading Soft Graviton Theorem for Loop Amplitudes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Ashoke Sen","submitted_at":"2017-02-28T19:00:17Z","abstract_excerpt":"Superstring field theory gives expressions for heterotic and type II string loop amplitudes that are free from ultraviolet and infrared divergences when the number of non-compact space-time dimensions is five or more. We prove the subleading soft graviton theorem in these theories to all orders in perturbation theory for S-matrix elements of arbitrary number of finite energy external states but only one external soft graviton. We also prove the leading soft graviton theorem for arbitrary number of finite energy external states and arbitrary number of soft gravitons. Since our analysis is based"},"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":"1703.00024","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2017-02-28T19:00:17Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"9a907deaf3a8d80be07ed9bd6533df11110c5777e2410826bee08e7ed38bbeef","abstract_canon_sha256":"138a6bd116748dd1cb849f93ce49b5c89ea1afb394a32692314f78c9b39eab9e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:26:01.022032Z","signature_b64":"29+qV0I5IvSPgbZGoYQ5YkgP0W5L4b+knrk1dNexDj2tuAEFq/7qR5CphQqfhjHwkQCM2Gl0kH8eHfu+JKfnDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2bb7fcf2e9180de24c8d0549def08433f41faabdebe71528c2620d2c3a3d6632","last_reissued_at":"2026-05-18T00:26:01.021370Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:26:01.021370Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Subleading Soft Graviton Theorem for Loop Amplitudes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Ashoke Sen","submitted_at":"2017-02-28T19:00:17Z","abstract_excerpt":"Superstring field theory gives expressions for heterotic and type II string loop amplitudes that are free from ultraviolet and infrared divergences when the number of non-compact space-time dimensions is five or more. We prove the subleading soft graviton theorem in these theories to all orders in perturbation theory for S-matrix elements of arbitrary number of finite energy external states but only one external soft graviton. We also prove the leading soft graviton theorem for arbitrary number of finite energy external states and arbitrary number of soft gravitons. Since our analysis is based"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1703.00024","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":"1703.00024","created_at":"2026-05-18T00:26:01.021467+00:00"},{"alias_kind":"arxiv_version","alias_value":"1703.00024v3","created_at":"2026-05-18T00:26:01.021467+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1703.00024","created_at":"2026-05-18T00:26:01.021467+00:00"},{"alias_kind":"pith_short_12","alias_value":"FO37Z4XJDAG6","created_at":"2026-05-18T12:31:15.632608+00:00"},{"alias_kind":"pith_short_16","alias_value":"FO37Z4XJDAG6ETEN","created_at":"2026-05-18T12:31:15.632608+00:00"},{"alias_kind":"pith_short_8","alias_value":"FO37Z4XJ","created_at":"2026-05-18T12:31:15.632608+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":7,"internal_anchor_count":6,"sample":[{"citing_arxiv_id":"2212.12892","citing_title":"Tree level amplitudes from soft theorems","ref_index":37,"is_internal_anchor":true},{"citing_arxiv_id":"2305.04620","citing_title":"Tree and $1$-loop fundamental BCJ relations from soft theorems","ref_index":38,"is_internal_anchor":true},{"citing_arxiv_id":"2401.03879","citing_title":"Multi-trace YMS amplitudes from soft behavior","ref_index":18,"is_internal_anchor":true},{"citing_arxiv_id":"2406.03034","citing_title":"Towards tree Yang-Mills and Yang-Mills-scalar amplitudes with higher-derivative interactions","ref_index":15,"is_internal_anchor":true},{"citing_arxiv_id":"2406.04622","citing_title":"On soft factors and transmutation operators","ref_index":19,"is_internal_anchor":true},{"citing_arxiv_id":"2509.02542","citing_title":"Soft Theorems in Chern-Simons Matter Theories","ref_index":15,"is_internal_anchor":true},{"citing_arxiv_id":"2605.05130","citing_title":"Subleading Chern-Simons soft factors in perturbative de Sitter","ref_index":26,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FO37Z4XJDAG6ETENAVE554EEGP","json":"https://pith.science/pith/FO37Z4XJDAG6ETENAVE554EEGP.json","graph_json":"https://pith.science/api/pith-number/FO37Z4XJDAG6ETENAVE554EEGP/graph.json","events_json":"https://pith.science/api/pith-number/FO37Z4XJDAG6ETENAVE554EEGP/events.json","paper":"https://pith.science/paper/FO37Z4XJ"},"agent_actions":{"view_html":"https://pith.science/pith/FO37Z4XJDAG6ETENAVE554EEGP","download_json":"https://pith.science/pith/FO37Z4XJDAG6ETENAVE554EEGP.json","view_paper":"https://pith.science/paper/FO37Z4XJ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1703.00024&json=true","fetch_graph":"https://pith.science/api/pith-number/FO37Z4XJDAG6ETENAVE554EEGP/graph.json","fetch_events":"https://pith.science/api/pith-number/FO37Z4XJDAG6ETENAVE554EEGP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FO37Z4XJDAG6ETENAVE554EEGP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FO37Z4XJDAG6ETENAVE554EEGP/action/storage_attestation","attest_author":"https://pith.science/pith/FO37Z4XJDAG6ETENAVE554EEGP/action/author_attestation","sign_citation":"https://pith.science/pith/FO37Z4XJDAG6ETENAVE554EEGP/action/citation_signature","submit_replication":"https://pith.science/pith/FO37Z4XJDAG6ETENAVE554EEGP/action/replication_record"}},"created_at":"2026-05-18T00:26:01.021467+00:00","updated_at":"2026-05-18T00:26:01.021467+00:00"}