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We point out in the case of $e^+e^-\\to TP$ transition due to charge conjugation invariance, only three channels are allowed: $e^+e^-\\to a_2^{\\pm} \\pi^\\mp$, $e^+e^-\\to K_2^{*\\pm} K^\\mp$ and the V-spin suppressed $e^+e^-\\to K_2^{*0} \\bar K^0+\\overline K_2^{*0} K^0 $. Cross sections of $e^+e^-\\to VP$ and $e^+e^-\\to TP$ at $\\sqrt{s}=3.67$ GeV and $\\sqrt{s}=10.58$ GeV are calculated and t"},"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":"1802.09718","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-02-27T04:51:27Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"7a1e62471f0429acea49b7ebee0a5fa72644996ff9d90b08e89dc8705adaaf37","abstract_canon_sha256":"c8d6306b41f71da3adcd14519ee64af6ad8e9428fc861a7296e1e36eddd2c1bd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:12:53.073444Z","signature_b64":"Ja+Rrjauy0ieik9LV53haV/Hmh6tr3Y0I5AhJb0hSpLmHLBppmV6tUVSBWOleaiqRVEDy88P6RUV1m4oEQjUDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"49b8502dd9e038c8e0329f4c73bbfb03bb466d5d114a65783a3e09804b5dbbfc","last_reissued_at":"2026-05-18T00:12:53.072836Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:12:53.072836Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Perturbative QCD Analysis of Exclusive Processes $e^+e^-\\rightarrow VP$ and $e^+e^-\\rightarrow TP$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Cai-Dian L\\\"u, Qi-An Zhang, Wei Wang, Ye Xing","submitted_at":"2018-02-27T04:51:27Z","abstract_excerpt":"We study the $e^+e^-\\to VP$ and $e^+e^-\\to TP$ processes in the perturbative QCD approach based on $k_T$ factorization, where the $P,V$ and $T$ denotes a light pseudo-scalar, vector and tensor meson, respectively. We point out in the case of $e^+e^-\\to TP$ transition due to charge conjugation invariance, only three channels are allowed: $e^+e^-\\to a_2^{\\pm} \\pi^\\mp$, $e^+e^-\\to K_2^{*\\pm} K^\\mp$ and the V-spin suppressed $e^+e^-\\to K_2^{*0} \\bar K^0+\\overline K_2^{*0} K^0 $. 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