Charged-Current Neutrino-Nucleus Scattering off the Even Molybdenum Isotopes

<table>Numerical errors in the cross section for the charged-current neutrino-nucleus scattering off <svg height="16.049999" id="M199" style="vertical-align:-0.16379pt" version="1.1" viewbox="0 0 41.25 16.049999" width="41.25" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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</svg> due to the use of barycentric Lagrange interpolation. The errors are shown for various energies <svg height="15.4" id="M200" style="vertical-align:-3.3907pt" version="1.1" viewbox="0 0 17.825001 15.4" width="17.825001" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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<g transform="matrix(.012,-0,0,-.012,10.8,15.187)"><path d="M509 373q0 -52 -42.5 -118.5t-124.5 -159.5l-94 -107h-27q-22 209 -78 342q-21 48 -41 48q-18 0 -63 -62l-22 21q77 111 125 111q30 0 52 -21.5t38 -75.5q37 -130 52 -285q48 62 74.5 99.5t53.5 87t27 76.5q0 43 -17 60q-5 5 -5 15q0 17 12.5 30.5t28.5 13.5
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</svg> of the incoming neutrino. In the figure, <svg height="19.362499" id="M201" style="vertical-align:-3.3907pt" version="1.1" viewbox="0 0 224 19.362499" width="224" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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<g transform="matrix(.012,-0,0,-.012,129.25,19.15)"><path d="M509 373q0 -52 -42.5 -118.5t-124.5 -159.5l-94 -107h-27q-22 209 -78 342q-21 48 -41 48q-18 0 -63 -62l-22 21q77 111 125 111q30 0 52 -21.5t38 -75.5q37 -130 52 -285q48 62 74.5 99.5t53.5 87t27 76.5q0 43 -17 60q-5 5 -5 15q0 17 12.5 30.5t28.5 13.5
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<g transform="matrix(.017,-0,0,-.017,218.062,15.075)"><path d="M275 270q0 -296 -211 -440l-19 23q75 62 116.5 174t41.5 243t-42 243t-116 173l19 24q211 -144 211 -440z" id="x29"></path></g>
</svg>. </table>

Advances in High Energy Physics

fig2

Figure 2

Figure 2: Charged-Current Neutrino-Nucleus Scattering off the Even Molybdenum Isotopes 