[819] | 1 | G4NuMuXQ2Integration.cc & G4NuMuXYIntegration.cc |
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| 2 | ================================================ |
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| 3 | Makes integration of d(sig)/dxdQ2 (DIS) for neutrino/antineutrino over x and then over Q2, |
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| 4 | having as an intermediate result the d(sig)/dQ2 distribution and as a final result sig_tot. |
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| 5 | Separation of QES (W<M_N+m_pi) is planned at this time. |
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| 6 | Output for 20 points equidistant from ln(E_min) to ln(E_max=300 (GeV)) (A=12): |
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| 7 | ------------------------------------------------------------------------------ |
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| 8 | >>>>Emin=0.111651,lEi=-2.19238,lEa=5.70378,dlE=0.394808 (sig_t, 10^-38 cm^2 GeV^-1) |
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| 9 | -----------------+----------+ |
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| 10 | I(Idx)dQ2,exp=.67| I(Idx)dy | ! NOT UP TO DATE ! |
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| 11 | -----------------+----------+ |
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| 12 | E_nu sig_t/E | sig_t/E | |
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| 13 | -----------------+----------+ |
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| 14 | .136017 0.158940 | 0.188611 | |
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| 15 | .201863 0.347557 | 0.354376 | |
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| 16 | .299584 0.482431 | 0.484008 | |
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| 17 | .444613 0.587544 | 0.587829 | |
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| 18 | .659850 0.663442 | 0.663354 | |
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| 19 | .979282 0.710895 | 0.710521 | |
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| 20 | 1.45335 0.734348 | 0.733853 | |
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| 21 | 2.15692 0.741216 | 0.740403 | |
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| 22 | 3.20108 0.737759 | 0.736918 | |
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| 23 | 4.75073 0.729512 | 0.728337 | |
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| 24 | 7.05055 0.718947 | 0.717549 | |
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| 25 | 10.4637 0.707357 | 0.705886 | |
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| 26 | 15.5292 0.695349 | 0.693841 | |
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| 27 | 23.0469 0.683188 | 0.681529 | |
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| 28 | 34.2038 0.671010 | 0.669100 | |
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| 29 | 50.7619 0.658915 | 0.656679 | |
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| 30 | 75.3357 0.646951 | 0.644425 | |
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| 31 | 111.806 0.635081 | 0.632419 | |
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| 32 | 165.931 0.622685 | 0.620626 | |
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| 33 | 246.258 0.610883 | 0.608874 | |
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| 34 | -----------------+----------+ |
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| 35 | I(Idx)dQ2,exp=.34| I(Idx)dy | |
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| 36 | -----------------+----------+ |
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| 37 | E_anu sig_t/E | sig_t/E | |
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| 38 | -----------------+----------+ |
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| 39 | .136017 0.134604 | 0.162247 | |
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| 40 | .201863 0.267721 | 0.274488 | |
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| 41 | .299584 0.335296 | 0.337052 | |
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| 42 | .444613 0.368757 | 0.369132 | |
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| 43 | .659850 0.379554 | 0.379583 | |
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| 44 | .979282 0.377011 | 0.376908 | |
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| 45 | 1.45335 0.368407 | 0.368181 | |
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| 46 | 2.15692 0.358362 | 0.357970 | |
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| 47 | 3.20108 0.349276 | 0.348610 | |
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| 48 | 4.75073 0.341937 | 0.341011 | |
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| 49 | 7.05055 0.336524 | 0.335304 | |
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| 50 | 10.4637 0.332704 | 0.331202 | |
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| 51 | 15.5292 0.330011 | 0.328298 | |
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| 52 | 23.0469 0.328097 | 0.326188 | |
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| 53 | 34.2038 0.326474 | 0.324666 | |
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| 54 | 50.7619 0.325437 | 0.323606 | |
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| 55 | 75.3357 0.324840 | 0.322993 | |
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| 56 | 111.806 0.324660 | 0.322805 | |
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| 57 | 165.931 0.324814 | 0.322974 | |
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| 58 | 246.258 0.325131 | 0.323362 | |
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| 59 | -----------------+----------+ |
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| 60 | Conclusion (05.10.2005): |
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| 61 | a) at high energies sig(nu) and sig(anu) look to be close to the experimental values |
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| 62 | b) fL OFF increase less then by 10% -> the only hope is to modify C(Q2), which is bigger |
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| 63 | c) both waysof calculation give the same result (within the accuracy of calculation)(?) |
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