{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:W6DMP7PHX466F4JPMRAJI5VBE4","short_pith_number":"pith:W6DMP7PH","schema_version":"1.0","canonical_sha256":"b786c7fde7bf3de2f12f64409476a12716362ba584cdbe43bc7b7d51ca3cf84a","source":{"kind":"arxiv","id":"hep-th/0603115","version":2},"attestation_state":"computed","paper":{"title":"The Pomeron and Gauge/String Duality","license":"","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Chung-I Tan (Brown. U), Joseph Polchinski (KITP), Matthew J. Strassler (U. Washington), Richard C. Brower (Boston U.)","submitted_at":"2006-03-14T21:09:23Z","abstract_excerpt":"The traditional description of high-energy small-angle scattering in QCD has two components -- a soft Pomeron Regge pole for the tensor glueball, and a hard BFKL Pomeron in leading order at weak coupling. On the basis of gauge/string duality, we present a coherent treatment of the Pomeron. In large-N QCD-like theories, we use curved-space string-theory to describe simultaneously both the BFKL regime and the classic Regge regime. The problem reduces to finding the spectrum of a single j-plane Schrodinger operator. For ultraviolet-conformal theories, the spectrum exhibits a set of Regge trajecto"},"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/0603115","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2006-03-14T21:09:23Z","cross_cats_sorted":["hep-lat","hep-ph"],"title_canon_sha256":"de07a3306ebb1eb7e78831e42bea8ffdd18b47e45ea8973f559e0e17e7f2da4d","abstract_canon_sha256":"5c872dece9d3f1f606b26931f5407f8f62555e0be2a6254b15a303f3832e8a07"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:54:11.738622Z","signature_b64":"LqfPeUKeIHDmXew4tKg/pqXtNSyYX95vpF+3IM03NL/kDKSlb0etlseuyAqUNZhAgCX6xFNRNf17h+JrvnbCCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b786c7fde7bf3de2f12f64409476a12716362ba584cdbe43bc7b7d51ca3cf84a","last_reissued_at":"2026-07-04T15:54:11.738164Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:54:11.738164Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Pomeron and Gauge/String Duality","license":"","headline":"","cross_cats":["hep-lat","hep-ph"],"primary_cat":"hep-th","authors_text":"Chung-I Tan (Brown. U), Joseph Polchinski (KITP), Matthew J. Strassler (U. Washington), Richard C. Brower (Boston U.)","submitted_at":"2006-03-14T21:09:23Z","abstract_excerpt":"The traditional description of high-energy small-angle scattering in QCD has two components -- a soft Pomeron Regge pole for the tensor glueball, and a hard BFKL Pomeron in leading order at weak coupling. On the basis of gauge/string duality, we present a coherent treatment of the Pomeron. In large-N QCD-like theories, we use curved-space string-theory to describe simultaneously both the BFKL regime and the classic Regge regime. The problem reduces to finding the spectrum of a single j-plane Schrodinger operator. For ultraviolet-conformal theories, the spectrum exhibits a set of Regge trajecto"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0603115","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/0603115/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/0603115","created_at":"2026-07-04T15:54:11.738226+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0603115v2","created_at":"2026-07-04T15:54:11.738226+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0603115","created_at":"2026-07-04T15:54:11.738226+00:00"},{"alias_kind":"pith_short_12","alias_value":"W6DMP7PHX466","created_at":"2026-07-04T15:54:11.738226+00:00"},{"alias_kind":"pith_short_16","alias_value":"W6DMP7PHX466F4JP","created_at":"2026-07-04T15:54:11.738226+00:00"},{"alias_kind":"pith_short_8","alias_value":"W6DMP7PH","created_at":"2026-07-04T15:54:11.738226+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2606.20981","citing_title":"Gluon GTMD at strong coupling: fixed-spin saddle factorization and Reggeization","ref_index":62,"is_internal_anchor":true},{"citing_arxiv_id":"1907.01416","citing_title":"Differential and total cross sections of high energy proton-proton scattering in holographic QCD","ref_index":3,"is_internal_anchor":true},{"citing_arxiv_id":"2512.18274","citing_title":"High-Energy Pion Scattering in Holographic QCD: A Comparison with Experimental Data","ref_index":22,"is_internal_anchor":true},{"citing_arxiv_id":"2604.12038","citing_title":"Holographic Open/Closed Exchange in Double Deeply Virtual Compton Scattering: Fixed-$j$ Structural Matching to the $\\pm$-Basis Wilson Kernels","ref_index":53,"is_internal_anchor":false},{"citing_arxiv_id":"2604.12037","citing_title":"From Vacuum to Nucleon: Fixed-$j$ Kernel Matching of Holographic Current Correlators to QCD","ref_index":29,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/W6DMP7PHX466F4JPMRAJI5VBE4","json":"https://pith.science/pith/W6DMP7PHX466F4JPMRAJI5VBE4.json","graph_json":"https://pith.science/api/pith-number/W6DMP7PHX466F4JPMRAJI5VBE4/graph.json","events_json":"https://pith.science/api/pith-number/W6DMP7PHX466F4JPMRAJI5VBE4/events.json","paper":"https://pith.science/paper/W6DMP7PH"},"agent_actions":{"view_html":"https://pith.science/pith/W6DMP7PHX466F4JPMRAJI5VBE4","download_json":"https://pith.science/pith/W6DMP7PHX466F4JPMRAJI5VBE4.json","view_paper":"https://pith.science/paper/W6DMP7PH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0603115&json=true","fetch_graph":"https://pith.science/api/pith-number/W6DMP7PHX466F4JPMRAJI5VBE4/graph.json","fetch_events":"https://pith.science/api/pith-number/W6DMP7PHX466F4JPMRAJI5VBE4/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/W6DMP7PHX466F4JPMRAJI5VBE4/action/timestamp_anchor","attest_storage":"https://pith.science/pith/W6DMP7PHX466F4JPMRAJI5VBE4/action/storage_attestation","attest_author":"https://pith.science/pith/W6DMP7PHX466F4JPMRAJI5VBE4/action/author_attestation","sign_citation":"https://pith.science/pith/W6DMP7PHX466F4JPMRAJI5VBE4/action/citation_signature","submit_replication":"https://pith.science/pith/W6DMP7PHX466F4JPMRAJI5VBE4/action/replication_record"}},"created_at":"2026-07-04T15:54:11.738226+00:00","updated_at":"2026-07-04T15:54:11.738226+00:00"}