Abstract. The NuTeV experiment obtained high statistics samples of neutrino and antineutrino charged current events during the 1996-1997 Fermilab fixed target run. The experiment combines sign-selected neutrino and antineutrino beams and the upgraded CCFR iron-scintillator neutrino detector. A precision continuous calibration beam was used to determine the muon and hadron energy scales to a precision of 0.7% and 0.43% respectively. The structure functions F 2 (x, Q 2 ) and xF 3 (x, Q 2 ) obtained by fitting the y-dependence of the sum and the difference of the ν and ν differential cross sections are presented.Neutrino deep inelastic scattering (DIS) provides a unique information for the structure of the proton and QCD, allowing the measurement of two structure functions (SF): F 2 (x, Q 2 ), and the parity-violating xF 3 (x, Q 2 ),which is accessible only by neutrino DIS [1]. The NuTeV experiment is a high-energy fixed target ν − Fe scattering experiment, which combines two new features: Separate high-purity neutrino and antineutrino beams, used to tag the primary lepton in charged-current interactions, and a continuous precision calibration beam, which improves the experiment's knowledge of the absolute energy scale for hadrons and muon, produced in neutrino interactions, to a precision of 0.43% and 0.7% respectively [2]. NuTeV took data during 1996-97 and collected 8.6 × 10 5 ν and 2.4 × 10 5 ν charged-current (CC) interactions that passed analysis cuts.
ν-FE CHARGE CURRENT DIFFERENTIAL CROSS SECTIONThe differential cross section is determined fromwhere Φ(E) is the ν(ν) flux in energy bins. The cross section event sample is required to pass fiducial volume cuts, µ track reconstruction quality cuts, a minimum muon energy threshold E µ > 15 GeV, a minimum hadronic energy threshold E HAD > 10 GeV, and a minimum neutrino energy threshold E ν > 30 GeV. Selected events are binned in x, y, and E ν bins, and corrected for acceptance and smearing using a fast detector simulation. Q 2 > 1 GeV 2 is required to minimize the non-perturbative contribution to the cross section. NuTeV data ranges from 10 −3 to 0.95 in x, 0.05 to 0.95 in y, and from 30 GeV to 360 GeV in E ν . The flux is determined from data with E HAD < 20 GeV using the "fixed ν 0 " relative flux extraction method [1]. The integrated number of events in this sample is propor-