{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:ZFD2P36LIBRYEZO2JYDLXS6FL3","short_pith_number":"pith:ZFD2P36L","schema_version":"1.0","canonical_sha256":"c947a7efcb40638265da4e06bbcbc55ecc3205988d70945e9c1da0cf6aa50ba3","source":{"kind":"arxiv","id":"2212.09509","version":1},"attestation_state":"computed","paper":{"title":"AdS correction to the Faddeev-Kulish state: Migrating from the Flat Peninsula","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Sarthak Duary","submitted_at":"2022-12-19T14:45:39Z","abstract_excerpt":"The IR finiteness of $\\mathcal{S}$-matrix in flat spacetime is tied to the Faddeev-Kulish dressed state, which suggests dressing the Fock space scattering state with the soft photon modes. We instigate a construction for the Faddeev-Kulish dressed state in the language of AdS/CFT. A salient feature of AdS spacetime is that it acquits itself as a quintessential IR regulator. The IR divergences will take shape after taking the zoomed in limit. We explore the Faddeev-Kulish dressed state to account for the AdS radius corrections. The Wilson line dressing stands as a guiding principle in the study"},"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":"2212.09509","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"hep-th","submitted_at":"2022-12-19T14:45:39Z","cross_cats_sorted":[],"title_canon_sha256":"5bbb4aa97a633864a24f22afe99b94be611110a13392361d1a8d7d8d947b2ac9","abstract_canon_sha256":"cdf4269e5ad59e7d14a4fe496fe13c9febcce0800e9e38031de2dd68679b2f10"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:09:47.279483Z","signature_b64":"JNip6sReIJryTBsBFL897zE8vYm7Ud71pcFR/Mj8dgBaQbHUphV0k1sL2O6xDypIG9NClPWDG8NxEWbvhel6CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c947a7efcb40638265da4e06bbcbc55ecc3205988d70945e9c1da0cf6aa50ba3","last_reissued_at":"2026-07-05T06:09:47.279062Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:09:47.279062Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"AdS correction to the Faddeev-Kulish state: Migrating from the Flat Peninsula","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"Sarthak Duary","submitted_at":"2022-12-19T14:45:39Z","abstract_excerpt":"The IR finiteness of $\\mathcal{S}$-matrix in flat spacetime is tied to the Faddeev-Kulish dressed state, which suggests dressing the Fock space scattering state with the soft photon modes. We instigate a construction for the Faddeev-Kulish dressed state in the language of AdS/CFT. A salient feature of AdS spacetime is that it acquits itself as a quintessential IR regulator. The IR divergences will take shape after taking the zoomed in limit. We explore the Faddeev-Kulish dressed state to account for the AdS radius corrections. The Wilson line dressing stands as a guiding principle in the study"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.09509","kind":"arxiv","version":1},"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/2212.09509/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":"2212.09509","created_at":"2026-07-05T06:09:47.279129+00:00"},{"alias_kind":"arxiv_version","alias_value":"2212.09509v1","created_at":"2026-07-05T06:09:47.279129+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.09509","created_at":"2026-07-05T06:09:47.279129+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZFD2P36LIBRY","created_at":"2026-07-05T06:09:47.279129+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZFD2P36LIBRYEZO2","created_at":"2026-07-05T06:09:47.279129+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZFD2P36L","created_at":"2026-07-05T06:09:47.279129+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.05395","citing_title":"Li\\'enard--Wiechert fields in AdS and flat-space antipodal matching from geodesic-centered Coulombic data","ref_index":40,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZFD2P36LIBRYEZO2JYDLXS6FL3","json":"https://pith.science/pith/ZFD2P36LIBRYEZO2JYDLXS6FL3.json","graph_json":"https://pith.science/api/pith-number/ZFD2P36LIBRYEZO2JYDLXS6FL3/graph.json","events_json":"https://pith.science/api/pith-number/ZFD2P36LIBRYEZO2JYDLXS6FL3/events.json","paper":"https://pith.science/paper/ZFD2P36L"},"agent_actions":{"view_html":"https://pith.science/pith/ZFD2P36LIBRYEZO2JYDLXS6FL3","download_json":"https://pith.science/pith/ZFD2P36LIBRYEZO2JYDLXS6FL3.json","view_paper":"https://pith.science/paper/ZFD2P36L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2212.09509&json=true","fetch_graph":"https://pith.science/api/pith-number/ZFD2P36LIBRYEZO2JYDLXS6FL3/graph.json","fetch_events":"https://pith.science/api/pith-number/ZFD2P36LIBRYEZO2JYDLXS6FL3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZFD2P36LIBRYEZO2JYDLXS6FL3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZFD2P36LIBRYEZO2JYDLXS6FL3/action/storage_attestation","attest_author":"https://pith.science/pith/ZFD2P36LIBRYEZO2JYDLXS6FL3/action/author_attestation","sign_citation":"https://pith.science/pith/ZFD2P36LIBRYEZO2JYDLXS6FL3/action/citation_signature","submit_replication":"https://pith.science/pith/ZFD2P36LIBRYEZO2JYDLXS6FL3/action/replication_record"}},"created_at":"2026-07-05T06:09:47.279129+00:00","updated_at":"2026-07-05T06:09:47.279129+00:00"}