Showing 10 of 15 results
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 ).
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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.
We report on measurements of the ϒ(1S), ϒ(2S), and ϒ(3S) differential, (d2σdPtdy)y=0, and integrated cross sections in pp¯ collisions at s=1.8 TeV using a sample of 16.6 ± 0.6 pb−1 collected by the Collider Detector at Fermilab. The three resonances were reconstructed through the decay ϒ→μ+μ−. Comparison is made to a leading order QCD prediction.
SIG*Br(UPSI --> MU+ MU-).
SIG*Br(UPSI --> MU+ MU-).
SIG*Br(UPSI --> MU+ MU-).
SIG*Br(UPSI --> MU+ MU-).
The first (asymmetric) systematic error represents the uncertainty in the decay angular distribution of the form (1 + a*cos(theta*)**2) where a = +1 and -1 respectively. The second is the quadratic sum of the other systematic errors.
The first (asymmetric) systematic error represents the uncertainty in the decay angular distribution of the form (1 + a*cos(theta*)**2) where a = +1 and -1 respectively. The second is the quadratic sum of the other systematic errors.
The first (asymmetric) systematic error represents the uncertainty in the decay angular distribution of the form (1 + a*cos(theta*)**2) where a = +1 and -1 respectively. The second is the quadratic sum of the other systematic errors.
The semi-inclusive reaction e+ p -> e+ X p was studied with the ZEUS detector at HERA using an integrated luminosity of 12.8 pb-1. The final-state proton, which was detected with the ZEUS leading proton spectrometer, carried a large fraction of the incoming proton energy, xL>0.32, and its transverse momentum squared satisfied pT^2<0.5 GeV^2/ the exchanged photon virtuality, Q^2, was greater than 3 GeV^2 and the range of the masses of the photon-proton system was 45<W<225 GeV. The leading proton production cross section and rates are presented as a function of xL, pT^2, Q^2 and the Bjorken scaling variable, x.
Double differential cross sections as a funtion of PT**2 for the XL range 0.32 TO 0.38. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.38 TO 0.44. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.44 TO 0.50. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.50 TO 0.56. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.56 TO 0.62. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.62 TO 0.65. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.65 TO 0.68. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.68 TO 0.71. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.71 TO 0.74. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.74 TO 0.77. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.77 TO 0.80. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.80 TO 0.83. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.83 TO 0.86. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.86 TO 0.89. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.89 TO 0.92. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.92 TO 0.95. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.95 TO 0.98. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Double differential cross sections as a funtion of PT**2 for the XL range 0.98 TO 1.00. The methods S123 and S456 are the results using different stations of the silicon microstrip detectors.
Leading proton production rate as a funtion of XL in 3 PT**2 ranges.
Leading proton production rate as a funtion of XL for the PT**2 region < 0.5 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 9.6E-5 and mean Q**2 of 4.2 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.7E-4 and mean Q**2 of 4.2 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.5E-4 and mean Q**2 of 4.2 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 6.9E-4 and mean Q**2 of 4.2 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.46E-3 and mean Q**2 of 4.2 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.9E-4 and mean Q**2 of 7.3 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.4E-4 and mean Q**2 of 7.3 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 6.9E-4 and mean Q**2 of 7.3 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.36E-3 and mean Q**2 of 7.3 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 2.67E-3 and mean Q**2 of 7.3 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 2.6E-4 and mean Q**2 of 11 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 4.6E-4 and mean Q**2 of 11 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 9.2E-4 and mean Q**2 of 11 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.83E-3 and mean Q**2 of 11 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.98E-3 and mean Q**2 of 11 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 5.1E-4 and mean Q**2 of 22 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 9.2E-4 and mean Q**2 of 22 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.84E-3 and mean Q**2 of 22 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.66E-3 and mean Q**2 of 22 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 7.83E-3 and mean Q**2 of 22 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.03E-3 and mean Q**2 of 44 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.86E-3 and mean Q**2 of 44 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.68E-3 and mean Q**2 of 44 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 7.33E-3 and mean Q**2 of 44 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.54E-2 and mean Q**2 of 44 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 2.00E-3 and mean Q**2 of 88 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.59E-3 and mean Q**2 of 88 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 7.37E-3 and mean Q**2 of 88 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.42E-2 and mean Q**2 of 88 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.01E-2 and mean Q**2 of 88 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 4.00E-3 and mean Q**2 of 237 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 7.52E-3 and mean Q**2 of 237 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 1.47E-2 and mean Q**2 of 237 GeV**2.
Leading proton production rate as a function of XL for the PT**2 region < 0.5 GeV**2, a mean X of 3.25E-2 and mean Q**2 of 237 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.04 to 0.15 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of XL for protons with PT**2 in the range 0.15 to 0.5 GeV**2.
Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production rate as a function of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production rate, averaged over X, as a function of Q**2 for protons with PT**2 < 0.5 GeV**2 in two XL ranges.
Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
Leading proton production structure function F2(C=Lp) as a fujnction of X in Q**2 bins for protons with XL in the range 0.32 to 0.92 and PT**2 < 0.5 GeV**2.
The production of jets is studied in deep-inelastic ep scattering at large negative four momentum transfer squared 150<Q^2<15000 GeV^2 using HERA data taken in 1999-2007, corresponding to an integrated luminosity of 395 pb^-1. Inclusive jet, 2-jet and 3-jet cross sections, normalised to the neutral current deep-inelastic scattering cross sections, are measured as functions of Q^2, jet transverse momentum and proton momentum fraction. The measurements are well described by perturbative QCD calculations at next-to-leading order corrected for hadronisation effects. The strong coupling as determined from these measurements is alpha_s(M_Z) = 0.1168 +/-0.0007 (exp.) +0.0046/-0.0030 (th.) +/-0.0016(pdf).
Normalised inclusive jet cross section in bins of $Q^{2}$.
Normalised 2-jet cross section in bins of $Q^{2}$.
Normalised 3-jet cross section in bins of $Q^{2}$.
3-jet cross section normalised to 2-jet cross section in bins of $Q^{2}$.
Normalised inclusive jet cross section in bins of $Q^{2}$ and $P_{T}$.
Normalised 2-jet cross section in bins of $Q^{2}$ and $\langle P_{T} \rangle$.
Normalised 2-jet cross sections in bins of $Q^2$ and $\xi$.
Inclusive non-diffractive photoproduction of rho(770)^0, K^*(892)^0 and phi(1020) mesons is investigated with the H1 detector in ep collisions at HERA. The corresponding average \gamma p centre-of-mass energy is 210 GeV. The mesons are measured in the transverse momentum range 0.5<p_T<7 GeV and the rapidity range |y_{lab}|<1. Differential cross sections are presented as a function of transverse momentum and rapidity, and are compared to the predictions of hadroproduction models.
Inclusive non-diffractive photoproduction cross sections in the specified kinematic region.
Ratios of cross sections.
Inclusive non-diffractive photoproduction invariant differential cross sections as a function of PT in the specified kinematic range.
Inclusive non-diffractive photoproduction single differential cross sections as a function of rapidity in the specified kinematic range.
The production of jets is studied in deep-inelastic e+p scattering at low negative four momentum transfer squared 5<Q^2<100 GeV^2 and at inelasticity 0.2<y<0.7 using data recorded by the H1 detector at HERA in the years 1999 and 2000, corresponding to an integrated luminosity of 43.5 pb^-1. Inclusive jet, 2-jet and 3-jet cross sections as well as the ratio of 3-jet to 2-jet cross sections are measured as a function of Q^2 and jet transverse momentum. The 2-jet cross section is also measured as a function of the proton momentum fraction xi. The measurements are well described by perturbative quantum chromodynamics at next-to-leading order corrected for hadronisation effects and are subsequently used to extract the strong coupling alpha_s.
Inclusive Jet Cross Section ${\rm\frac{d\sigma_{jet}}{dQ^2}}$.
2-Jet Cross Section ${\rm\frac{d\sigma_{2-jet}}{dQ^2}}$.
3-Jet Cross Section ${\rm\frac{d\sigma_{3-jet}}{dQ^2}}$.
Inclusive Jet Cross Section ${\rm\frac{d\sigma_{jet}}{dP_T}}$.
2-Jet Cross Section ${\rm\frac{d\sigma_{2-jet}}{d\langle P_T \rangle}}$.
3-Jet Cross Section ${\rm\frac{d\sigma_{3-jet}}{d\langle P_T \rangle}}$.
Inclusive Jet Cross Section ${\rm\frac{d^2\sigma_{jet}}{dQ^2dP_T}}$.
2-Jet Cross Section ${\rm\frac{d^2\sigma_{2-jet}}{dQ^2d\langle P_T \rangle}}$.
2-Jet Cross Section ${\rm\frac{d^2\sigma_{2-jet}}{dQ^2d\xi}}$.
3-Jet Cross Section ${\rm\frac{d^2\sigma_{3-jet}}{dQ^2d\langle P_T \rangle}}$.
3-Jet to 2-Jet Cross Sections Ratio ${\rm\frac{d\sigma_{3-jet}}{dQ^2}/\frac{d\sigma_{2-jet}}{dQ^2}}$.
3-Jet to 2-Jet Cross Sections Ratio ${\rm\frac{d\sigma_{3-jet}}{d\langle P_T \rangle}/\frac{d\sigma_{2-jet}}{d\langle P_T \rangle}}$.
3-Jet to 2-Jet Cross Sections Ratio ${\rm\frac{d^2\sigma_{3-jet}}{dQ^2d\langle P_T \rangle}/\frac{d^2\sigma_{2-jet}}{dQ^2d\langle P_T \rangle}}$.
We report on double-differential inclusive cross-sections of the production of secondary protons, charged pions, and deuterons, in the interactions with a 5% nuclear interaction length thick stationary carbon target, of proton and pion beams with momentum from \pm 3 GeV/c to \pm 15 GeV/c. Results are given for secondary particles with production angles between 20 and 125 degrees. Cross-sections on carbon nuclei are compared with cross-sections on beryllium, copper, tantalum and lead nuclei.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 20 to 30 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 30 to 45 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 45 to 60 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 65 to 90 degrees.
The measured deuteron to proton ratios for each of the 8 GeV Proton, PI+ and PI- beams for the angular range 90 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 3 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a P beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for P production from a PI- beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 30 to 40 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 40 to 50 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 60 to 75 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 75 to 90 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 90 to 105 degrees.
Measured cross section as a function of PT for PI+ production from a PI- beam of momentum 5 GeV/c in the angular range 105 to 125 degrees.
Measured cross section as a function of PT for PI- production from a PI- beam of momentum 5 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 8 GeV/c in the angular range 50 to 60 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 20 to 30 degrees.
Measured cross section as a function of PT for PI- production from a PI+ beam of momentum 12 GeV/c in the angular range 30 to 40 degrees.
Results of inclusive measurements of inelastic electron and positron scattering from unpolarized protons and deuterons at the HERMES experiment are presented. The structure functions $F_2^p$ and $F_2^d$ are determined using a parameterization of existing data for the longitudinal-to-transverse virtual-photon absorption cross-section ratio. The HERMES results provide data in the ranges $0.006\leq x\leq 0.9$ and 0.1 GeV$^2\leq Q^2\leq$ 20 GeV$^2$, covering the transition region between the perturbative and the non-perturbative regimes of QCD in a so-far largely unexplored kinematic region. They are in agreement with existing world data in the region of overlap. The measured cross sections are used, in combination with data from other experiments, to perform fits to the photon-nucleon cross section using the functional form of the ALLM model. The deuteron-to-proton cross-section ratio is also determined.
Results on the differential Born cross section $\frac{d^2\sigma^p}{dx\,dQ^2}$ and $F_2^p$. The statistical uncertainty $\delta_{stat.}$ and the systematic uncertainties $\delta_{PID}$ (particle identification), $\delta_{model}$ (model dependence outside the acceptance), $\delta_{mis.}$ (misalignment), and $\delta_{rad.}$ (Bethe-Heitler efficiencies) are given in percent. Corresponding $x$ bin numbers and $Q^2$ bin numbers and the average values $\langle x \rangle$ and $\langle {Q^2} \rangle$ are listed in the first four columns. The overall normalization uncertainty is 7.6 %. The structure function $F_2^p$ is derived using the parameterization $R=R_{1998}$.
Results on the differential Born cross section $\frac{d^2\sigma^d}{dx\,dQ^2}$ and $F_2^d$. The statistical uncertainty $\delta_{stat.}$ and the systematic uncertainties $\delta_{PID}$ (particle identification), $\delta_{model}$ (model dependence outside the acceptance), $\delta_{mis.}$ (misalignment), and $\delta_{rad.}$ (Bethe-Heitler efficiencies), are given in percent. Corresponding $x$ bin numbers and $Q^2$ bin numbers and the average values $\langle x \rangle$ and $\langle{Q^2}\rangle$ are listed in the first four columns. The overall normalization uncertainty is 7.5 %. The structure function $F_2^d$ is derived using the parameterization $R=R_{1998}$.
Results on the inelastic Born cross-section ratio ${\sigma^d}/{\sigma^p}$. The statistical uncertainty $\delta_{stat.}$, the systematic uncertainty $\delta_{rad.}$ due to radiative corrections and $\delta_{model}$ due to the model dependence outside the acceptance are given in percent. The average values of $x$ and $Q^2$ are listed in the first two columns. The overall normalization uncertainty is 1.4$\%$.
The inclusive J/psi production cross-section and fraction of J/psi mesons produced in B-hadron decays are measured in proton-proton collisions at sqrt(s) = 7 TeV with the ATLAS detector at the LHC, as a function of the transverse momentum and rapidity of the J/psi, using 2.3 pb-1 of integrated luminosity. The cross-section is measured from a minimum pT of 1 GeV to a maximum of 70 GeV and for rapidities within |y| < 2.4 giving the widest reach of any measurement of J/psi production to date. The differential production cross-sections of prompt and non-prompt J/psi are separately determined and are compared to Colour Singlet NNLO*, Colour Evaporation Model, and FONLL predictions.
We report on double-differential inclusive cross-sections of the production of secondary protons, charged pions, and deuterons, in the interactions with a 5% nuclear interaction length thick stationary tin target, of proton and pion beams with momentum from \pm3 GeV/c to \pm15 GeV/c. Results are given for secondary particles with production angles between 20 and 125 degrees. Cross-sections on tin nuclei are compared with cross-sections on beryllium, carbon, copper, tantalum and lead nuclei.
Ratio of deuterons to protons for polar angle 20-30 deg.
Ratio of deuterons to protons for polar angle 30-45 deg.
Ratio of deuterons to protons for polar angle 45-65 deg.
Ratio of deuterons to protons for polar angle 65-90 deg.
Ratio of deuterons to protons for polar angle 90-125 deg.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 3 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 5 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 8 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 12 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive P production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI+ production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in P Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI+ Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 20-30 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 30-40 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 40-50 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 50-60 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 60-75 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 75-90 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 90-105 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
The double-differential cross section as a function of PT in the polar ange range 105-125 deg. for inclusive PI- production in PI- Tin interactions at a beam energy of 15 GeV.
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