deletions | additions       diff --git a/Higgs properties at 240 GeV.tex b/Higgs properties at 240 GeV.tex  index 22f5c38..a97262a 100644  --- a/Higgs properties at 240 GeV.tex  +++ b/Higgs properties at 240 GeV.tex 
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\begin{table}  \begin{center}  \caption{Table~\ref{tab:HiggsCross}: Integrated luminosity for the  TLEP ($\sqrt{s} programme at $\sqrt{s}  = 240$ GeV) GeV (summed over the four IPs)  and for the  ILC ($\sqrt{s} programme at $\sqrt{s}  = 250$ GeV), {\it (i)} per year and per IP; and {\it (ii)} over of period of five years, summed over the four IPs in the case of TLEP. GeV.  No beam polarization is assumed for TLEP. For the comparison with linear colliders, the ${\rm e}^-$ (${\rm e}^+$) beam of ILC is supposed to be polarized at a level of 80\% (30\%), leading to a cross section increase of 40\% at $\sqrt{s}$ = 250 GeV. for the Higgsstrahlung process and 134% for the WW fusion with respect to the unpolarized cross sections.  The total numbers of Higgs boson producedin the Higgs-strahlung process and in the boson-fusion processes (plus interference)  are also indicated.\label{tab:HiggsCross}} \begin{tabular}{|r|r|r|}  \hline Collider & TLEP 240 & ILC 250 \\ \hline   \hlineIntegrated Luminosity / Year / IP ($\small \infb$) & {\bf 500} & 75 \\   \hline  Total Integrated Luminosityin 5 years  ($\small \inab$) & {\bf 10} & 0.375 0.250  \\ \hline Number of Higgs bosons from ${\small \epemto {\rm HZ}}$ & {\bf 2,000,000} & 105,000 70,000  \\ \hline Number of Higgs bosons from boson fusion & {\bf 50,000} & 1,500 3,000  \\ \hline \end{tabular}  \end{center}  \end{table}