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The running coupling method with next-to-leading order accuracy and pion, kaon elm form fac

a r X i v :h e p -p h /9805278v 1 11 M a y 1998THE RUNNING COUPLING METHOD WITH NEXT-TO-LEADING ORDER ACCURACY AND PION,KAON ELM FORM F ACTORS Shahin S.Agaev ∗High Energy Physics Lab.,Baku State University,Z.Khalilov st.23,1370148Baku,Azerbaijan Abstract The pion and kaon electromagnetic form factors F M (Q 2)are c
alculated at the leading order of pQCD using the running coupling constant method.In calculations the leading and next-to-leading order terms in αS ((1−x )(1−y )Q 2)expansion in terms of αS (Q 2)are taken into account.The resummed expression for F M (Q 2)is found.Results of numerical calculations for the pion (asymptotic distribution amplitude)are presented.

a r X i v :h e p -p h /9805278v 1 11 M a y 1998THE RUNNING COUPLING METHOD WITH NEXT-TO-LEADING ORDER ACCURACY AND PION,KAON ELM FORM F ACTORS Shahin S.Agaev ∗High Energy Physics Lab.,Baku State University,Z.Khalilov st.23,1370148Baku,Azerbaijan Abstract The pion and kaon electromagnetic form factors F M (Q 2)are calculated at the leading order of pQCD using the running coupling constant method.In calculations the leading and next-to-leading order terms in αS ((1−x )(1−y )Q 2)expansion in terms of αS (Q 2)are taken into account.The resummed expression for F M (Q 2)is found.Results of numerical calculations for the pion (asymptotic distribution amplitude)are presented.

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