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The eigenfunctions and eigenvalues of the odderon solution are the same as for the dipole BFKL equation and are given by the functions $E^{n,\\nu}$ and $\\chi (n,\\nu)$ correspondingly, where the $C$-odd initial condition allows only for odd values of $n$. The leading high-energy odderon intercept is given by $\\alpha_{odd} - 1 = \\frac{2 \\as N_c}{\\pi} \\chi (n=1 ,\\nu=0) = 0$ in agreement with the solution found by B"},"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-ph/0309281","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2003-09-25T19:18:01Z","cross_cats_sorted":[],"title_canon_sha256":"64b91b902476ba7c5b5fbdf74f14686f165dbcb9ec327413f71a2cc4d7d4fbdc","abstract_canon_sha256":"a274559ff2759ba888b4bc02aae0b326f2199aa2d6f705609aff6564016ea078"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:40:53.905827Z","signature_b64":"ZyTtvIRoQqFdlQJqJ22b3zkJ+Mcv+oAxeg+6obn+OI4QqHEYlrQF/kvQfPlLtmcP32R6h6PSrnhLjA7+IuUGDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"30a20b77328b20d6c89f9fe85d9fd95562b0262fb0bdda4a4770daae31146b12","last_reissued_at":"2026-07-04T16:40:53.905411Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:40:53.905411Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Perturbative Odderon in the Dipole Model","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Lech Szymanowski, Samuel Wallon, Yuri V. 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