various fixes
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@@ -548,8 +548,8 @@ The classical Coulomb barrier $V$ they used are given by:
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\label{eqn:classical_coulomb_barrier}
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\end{equation}
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where $z$ and $Z$ are the charges of the outgoing particle and of the residual
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nucleus respectively, $e^2 = 1.44 \si{\MeV}$, $r_0 = 1.35 \textrm{ fm}$, and
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$\rho = 0 \textrm{ fm}$ for protons were taken.
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nucleus respectively, $e^2 = 1.44 \si{\MeV}\cdot\textrm{fm}$, $r_0 = 1.35
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\textrm{ fm}$, and $\rho = 0 \textrm{ fm}$ for protons were taken.
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\begin{figure}[htb]
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\centering
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\includegraphics[width=0.48\textwidth]{figs/wyttenbach_rate_1p}
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@@ -684,25 +684,25 @@ al.~\cite{VilgelmovaEvseev.etal.1971} observed.
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%nucleus & calculation & experiment & calculation & experiment \\
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%\textbf{Col1}\\
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\midrule
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$^{27}_{13}$Al & 9.7 & {(4.7)} & 40 & {$> 28 \pm 4$} &(70)\\
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$^{27}_{13}$Al & 9.7 & {(4.7)} & 40 & {$> 28 $} &(70)\\
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$^{28}_{14}$Si & 32 & 53 \pm 10 & 144 & 150 \pm 30 & \\
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$^{31}_{15}$P & 6.7 & {(6.3)} & 35 & {$> 61 \pm 6$}&(91) \\
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$^{31}_{15}$P & 6.7 & {(6.3)} & 35 & {$> 61$}&(91) \\
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$^{39}_{19}$K & 19 & 32 \pm 6 & 67 & {} \\
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$^{41}_{19}$K & 5.1 & {(4.7)} & 30 & {$> 28 \pm 4$} &(70)\\
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$^{51 }_{23}$V &3.7 &2.9 \pm 0.4 &25 &{$>20 \pm 1.8$}& (32)\\
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$^{55 }_{25}$Mn &2.4 &2.8 \pm 0.4 &16 &{$>26 \pm 2.5$}& (35)\\
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$^{59 }_{27}$Co &3.3 &1.9 \pm 0.2 &21 &{$>37 \pm 3.4$}& (50)\\
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$^{60 }_{28}$Ni &8.9 &21.4 \pm 2.3 &49 &40 \pm 5&\\
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$^{63 }_{29}$Cu &4.0 &2.9 \pm 0.6 &25 &{$>17 \pm 3 $}& (36)\\
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$^{65 }_{29}$Cu &1.2 &{(2.3)} &11 &{$>35 \pm 4.5$}& (36)\\
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$^{75 }_{33}$As &1.5 &1.4 \pm 0.2 &14 &{$>14 \pm 1.3$}& (19)\\
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$^{79 }_{35}$Br &2.7 &{} &22 & &\\
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$^{107}_{47}$Ag &2.3 &{} &18 & &\\
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$^{115}_{49}$In &0.63 &{(0.77)} &7.2 &{$>11 \pm 1$} &(12)\\
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$^{133}_{55}$Cs &0.75 &0.48 \pm 0.07 &8.7 &{$>4.9 \pm 0.5$} &(6.7)\\
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$^{165}_{67}$Ho &0.26 &0.30 \pm 0.04 &4.1 &{$>3.4 \pm 0.3$} &(4.6)\\
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$^{181}_{73}$Ta &0.15 &0.26 \pm 0.04 &2.8 &{$>0.7 \pm 0.1$} &(3.0)\\
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$^{208}_{82}$Pb &0.14 &0.13 \pm 0.02 &1.1 &{$>3.0 \pm 0.8$} &(4.1)\\
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$^{41}_{19}$K & 5.1 & {(4.7)} & 30 & {$> 28$} &(70)\\
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%$^{51 }_{23}$V &3.7 &2.9 \pm 0.4 &25 &{$>20 \pm 1.8$}& (32)\\
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%$^{55 }_{25}$Mn &2.4 &2.8 \pm 0.4 &16 &{$>26 \pm 2.5$}& (35)\\
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%$^{59 }_{27}$Co &3.3 &1.9 \pm 0.2 &21 &{$>37 \pm 3.4$}& (50)\\
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%$^{60 }_{28}$Ni &8.9 &21.4 \pm 2.3 &49 &40 \pm 5&\\
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%$^{63 }_{29}$Cu &4.0 &2.9 \pm 0.6 &25 &{$>17 \pm 3 $}& (36)\\
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%$^{65 }_{29}$Cu &1.2 &{(2.3)} &11 &{$>35 \pm 4.5$}& (36)\\
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%$^{75 }_{33}$As &1.5 &1.4 \pm 0.2 &14 &{$>14 \pm 1.3$}& (19)\\
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%$^{79 }_{35}$Br &2.7 &{} &22 & &\\
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%$^{107}_{47}$Ag &2.3 &{} &18 & &\\
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%$^{115}_{49}$In &0.63 &{(0.77)} &7.2 &{$>11 \pm 1$} &(12)\\
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%$^{133}_{55}$Cs &0.75 &0.48 \pm 0.07 &8.7 &{$>4.9 \pm 0.5$} &(6.7)\\
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%$^{165}_{67}$Ho &0.26 &0.30 \pm 0.04 &4.1 &{$>3.4 \pm 0.3$} &(4.6)\\
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%$^{181}_{73}$Ta &0.15 &0.26 \pm 0.04 &2.8 &{$>0.7 \pm 0.1$} &(3.0)\\
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%$^{208}_{82}$Pb &0.14 &0.13 \pm 0.02 &1.1 &{$>3.0 \pm 0.8$} &(4.1)\\
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\bottomrule
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\end{tabular}
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\end{center}
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