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The $N(1710)$ resonance, a state with spin 1/2 and positive parity ($J^P = \\frac{1}{2}^+$), can possibly be interpreted as the second radial excitation of the nucleon, after the Roper, $N(1440)$. We calculate the $\\gamma^\\ast N \\to N(1710)$ helicity amplitudes, and predict that they are almost identical to those of the $\\gamma^\\ast N \\to N(1440)$ reacti"},"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":"1402.3234","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-02-13T17:42:04Z","cross_cats_sorted":["hep-ex","nucl-ex","nucl-th"],"title_canon_sha256":"7b32447dd75fa41829bf17f5c51051f5d5cbfab569aa75322eeb73aaced98491","abstract_canon_sha256":"d8bc3c938bd38d837e5708396f9026b227ccf62c66363bbbc38d266381e70d57"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:54:22.267854Z","signature_b64":"bBo/W+oQs+C3H+v32bpO3KFOybhSHwK5AaBUIrmSxBtmEB9tSQbjQ/lnDBRbwiTA7be75NiDJQJGrdnIlp+YBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a76c781eedf2cef2a286f91c087cc256b4afdbb427fac3d768270b7d508e9fdc","last_reissued_at":"2026-05-18T02:54:22.267424Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:54:22.267424Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"$\\gamma^\\ast N \\to N(1710)$ transition at high momentum transfer","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex","nucl-ex","nucl-th"],"primary_cat":"hep-ph","authors_text":"G. 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