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Because of the properties of <jats:inline-formula><jats:alternatives><jats:tex-math>A^0<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\"><mml:msup><mml:mi>A<\/mml:mi><mml:mn>0<\/mml:mn><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\ncoupling to the other fields, the main contribution comes from the\ntop-quark triangle loop diagrams. We obtain the \u201ctimelike\u201d transition\nform factor which describes the production amplitude of\n<jats:inline-formula><jats:alternatives><jats:tex-math>A^0<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\"><mml:msup><mml:mi>A<\/mml:mi><mml:mn>0<\/mml:mn><\/mml:msup><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\nin the <jats:inline-formula><jats:alternatives><jats:tex-math>e^+e^-<\/jats:tex-math><mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\"><mml:mrow><mml:msup><mml:mi>e<\/mml:mi><mml:mo>+<\/mml:mo><\/mml:msup><mml:msup><mml:mi>e<\/mml:mi><mml:mo>\u2212<\/mml:mo><\/mml:msup><\/mml:mrow><\/mml:math><\/jats:alternatives><\/jats:inline-formula>\ncollisions. 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