The QCD analysis of the $xF_3$ structure function measured in deep-inelastic scattering of neutrinos and antineutrinos on an iron target at the Fermilab Tevatron is done in 1--, 2-- and 3--loop order of QCD. The x dependence of the higher--twist contributi
[19]S.Bethke,Nucl.Phys.(Proc.Suppl.)39B,C(1995)198.
[20]CCFR-NUTEVCollab.,D.Harrisetal.,FERMILAB-Conf-95-114,March,1995.
[21]D.J.Gross,C.H.Llewellyn-Smith,Nucl.Phys.B14(1969)337.
[22]E.V.ShuryakandA.I.Vainshtein,Nucl.Phys.B199(1982)451.
[23]V.M.BraunandA.V.Kolesnichenko,Nucl.Phys.B283(1987)723.
[24]G.G.RossandR.G.Roberts,Phys.Lett.B322,425(1994).
[25]I.I.Balitsky,V.M.BraunandA.V.Kolesnichenko,Phys.Lett.B242(1990)245;
(E)ibid.B318(1993)648;
V.M.Braun,[hep-ph/9505317],toappearintheProceedingsoftheXXXthRencon-tresdeMoriond“QCDandHighEnergyHadronicInteractions”LesArcs,France,March1995.
[26]L.L.Frankfurt,M.I.Strikman,Nucl.Phys.B316(1989)340.
[27]A.V.Sidorov,ChineseJ.Phys.34,916(1996).
[28]W.BernreutherandW.Wetzel,Nucl.Phys.B197(1982)228;
W.Marciano,Phys.Rev.D29(1984)580;
D.V.Shirkov,Nucl.Phys.B371(1992)267;
D.V.ShirkovandS.V.Mikhailov,Z.Phys.C63(1994)463;
D.V.Shirkov,S.V.Mikhailov,A.V.Sidorov,JINRE2-96-285,Dubna,1996[hep-ph/9607472].