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After completion of the data taking for the νμ→ντ oscillation search, the CHORUS lead–scintillator calorimeter was used in the 1998 run as an active target. High-statistics samples of charged-current interactions were collected in the CERN SPS west area neutrino beam. This beam contained predominantly muon (anti-)neutrinos from sign-selected pions and kaons. We measure the flux and energy spectrum of the incident neutrinos and compare them with beam simulations. The neutrino–nucleon and anti-neutrino–nucleon differential cross-sections are measured in the range 0.01<x<0.7 , 0.05<y<0.95 , 10<Eν<200 GeV . We extract the neutrino–nucleon structure functions F2(x,Q2) , xF3(x,Q2) , and R(x,Q2) and compare these with results from other experiments.
The measured F2 and xF3 at X = 0.020.
The measured F2 and xF3 at X = 0.045.
The measured F2 and xF3 at X = 0.080.
The measured F2 and xF3 at X = 0.125.
The measured F2 and xF3 at X = 0.175.
The measured F2 and xF3 at X = 0.225.
The measured F2 and xF3 at X = 0.275.
The measured F2 and xF3 at X = 0.350.
The measured F2 and xF3 at X = 0.450.
The measured F2 and xF3 at X = 0.550.
The measured F2 and xF3 at X = 0.650.
The measured R (=sigL/sigT)) at X = 0.020.
The measured R (=sigL/sigT)) at X = 0.045.
The measured R (=sigL/sigT)) at X = 0.080.
The measured R (=sigL/sigT)) at X = 0.125.
The measured R (=sigL/sigT)) at X = 0.175.
The measured R (=sigL/sigT)) at X = 0.225.
The measured R (=sigL/sigT)) at X = 0.275.
The measured R (=sigL/sigT)) at X = 0.350.
The measured R (=sigL/sigT)) at X = 0.450.
The measured R (=sigL/sigT)) at X = 0.550.
The measured R (=sigL/sigT)) at X = 0.650.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.020.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.045.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.080.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.125.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.175.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.225.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.275.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.350.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.450.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.550.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 25.0 GeV and X =0.650.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.020.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.045.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.080.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.125.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.175.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.225.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.275.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.350.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.450.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.550.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 35.0 GeV and X =0.650.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.020.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.045.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.080.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.125.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.175.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.225.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.275.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.350.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.450.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.550.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 45.0 GeV and X =0.650.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.020.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.045.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.080.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.125.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.175.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.225.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.275.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.350.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.450.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.550.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 55.0 GeV and X =0.650.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.020.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.045.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.080.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.125.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.175.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.225.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.275.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.350.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.450.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.550.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 70.0 GeV and X =0.650.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.020.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.045.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.080.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.125.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.175.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.225.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.275.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.350.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.450.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.550.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 90.0 GeV and X =0.650.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.020.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.045.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.080.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.125.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.175.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.225.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.275.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.350.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.450.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.550.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 110.0 GeV and X =0.650.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.020.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.045.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.080.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.125.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.175.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.225.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.275.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.350.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.450.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.550.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 130.0 GeV and X =0.650.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.020.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.045.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.080.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.125.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.175.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.225.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.275.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.350.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.450.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.550.
Measured cross sections for neutrino and anti-neutrino interactions at a mean energy 170.0 GeV and X =0.650.
We present results on a high statistics study of the proton structure functions F 2 ( x , Q 2 ) and R = σ L / σ T measured in deep inelastic scattering of muons on a hydrogen target. The analysis is based on 1.8 × 10 6 events after all cuts, recorded at beam energies of 100, 120, 200 and 280 GeV and covering a kinematic range 0.06 ⩽ x ⩽ 0.80 and 7 GeV 2 ⩽ Q 2 ⩽260 GeV 2 . At small x , we find R to be different from zero in agreement with predictions of perturbative QCD.
THE AVERAGE VALUES OF Q**2 AT EACH OF THE X VALUES LISTED IN THIS TABLE ARE 15,20,20,25,30,35,40,45,50,50.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE ZERO.
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
R=SIG(L)/SIG(T) IS TAKEN TO BE R(QCD).
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