Showing 3 of 3 results
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.
A high-statistics measurement of the differential cross-sections for neutrino-iron scattering in the wide-band neutrino beam at the CERN SPS is presented. Nucleon structure functions are extracted and theirQ2 evolution is compared with the predictions of quantum chromodynamics.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
Structure functions for neutrino and antineutrino combined.
Structure functions for neutrino and antineutrino combined.
Structure functions for neutrino and antineutrino combined.
Structure functions for neutrino and antineutrino combined.
Structure functions for neutrino and antineutrino combined.
Structure functions for neutrino and antineutrino combined.
Structure functions for neutrino and antineutrino combined.
Structure functions for neutrino and antineutrino combined.
Structure functions for neutrino and antineutrino combined.
Structure functions for neutrino and antineutrino combined.
Structure functions for neutrino and antineutrino combined.
Neutrino and Antineutrino data combined.
Neutrino and Antineutrino data combined.
Neutrino and Antineutrino data combined.
Neutrino and Antineutrino data combined.
Neutrino and Antineutrino data combined.
Neutrino and Antineutrino data combined.
Neutrino and Antineutrino data combined.
Neutrino and Antineutrino data combined.
Neutrino and Antineutrino data combined.
Neutrino and Antineutrino data combined.
Neutrino and Antineutrino data combined.
The x and Q 2 dependence of the single photon exchange cross section d 2 σ /d Q 2 d x and the proton structure functions F 2 ( x , Q 2 ) and R ( x , Q 2 ) have been measured in deep inelastic muon proton scattering in the region 0.02 < x < 0.8 and 3 < Q 2 < 190 GeV 2 . By comparing data at different incident muon energies R was found to have little kinematic dependence and an average value of −0.010 ± 0.037 (stat.) ± 0.102 (stat.). The observed deviations from scaling gave the value of Λ MS , the QCD mass scale parameter, to be 105 −45 +55 (stat.) −45 +85 (syst.) MeV. The fraction of the momentum of the nucleon carried by gluons was found to be ∼56% at Q 2 ∼22.5 GeV 2 . It is shown that to obtain a description of the data for F 2 ( x , Q 2 ) together with that measured in deep inelastic electron-proton scattering at lower Q 2 it is necessary to include additional higher twist contributions. The value of Λ MS remains unchanged with the inclusion of these contributions which were found to have an x -dependence of the form x 3 /(1 − x ).
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
No description provided.
VALUES OF Q**2 CORRESPONDING TO THE ENTRIES IN THIS TABLE ARE 15., 20., 27., 36., 48. RESPECTIVELY.
VALUES OF Q**2 CORRESPONDING TO THE ENTRIES IN THIS TABLE ARE 11.5, 15., 20., 27., 36., RESPECTIVELY.
VALUES OF Q**2 CORRESPONDING TO THE ENTRIES IN THIS TABLE ARE 27., 36., 48., 65. RESPECTIVELY.
VALUES OF Q**2 CORRESPONDING TO THE ENTRIES IN THIS TABLE ARE 15., 20., 27., 36., 48.,65., 90. RESPECTIVELY.
VALUES OF Q**2 CORRESPONDING TO THE ENTRIES IN THIS TABLE ARE 11.5, 15., 20., 27., 36., 48.,65.RESPECTIVELY.
When you search on a word, e.g. 'collisions', we will automatically search across everything we store about a record. But sometimes you may wish to be more specific. Here we show you how.
Guidance on the query string syntax can also be found in the OpenSearch documentation.
About HEPData Submitting to HEPData HEPData File Formats HEPData Coordinators HEPData Terms of Use HEPData Cookie Policy
Status Email Forum Twitter GitHub
Copyright ~1975-Present, HEPData | Powered by Invenio, funded by STFC, hosted and originally developed at CERN, supported and further developed at IPPP Durham.