deletions | additions       diff --git a/Higgs properties at 240 GeV.tex b/Higgs properties at 240 GeV.tex  index 12b258c..f062c60 100644  --- a/Higgs properties at 240 GeV.tex  +++ b/Higgs properties at 240 GeV.tex 
...
\subsection{Measurements at $\sqrt{s}=240$ GeV}  At $\sqrt{s} = 240$ GeV, the TLEP instantaneous luminosity is expected to $5\times 10^{34} \cms$ at each interaction point (IP), in a configuration with four IPs. The total integrated luminosity accumulated in five years, assuming running for $10^7$ seconds per year, is shown in Table~\ref{fig:HiggsCross}, together with the corresponding numbers of Higgs bosons produced.The numbers for the ILC baseline programme at $\sqrt{s} = 250$ GeV are also displayed in the table, for a direct comparison.  \begin{table}  \begin{center}  \caption{Table~\ref{tab:HiggsCross}: Integrated luminosity for and number of Higgs bosons produced with  TLEP at $\sqrt{s} = 240$ GeV (summed over the four IPs) IPs), for the Higgsstrahlung process  and the WW fusion. For illusration, the corresponding numbers are also shown  for the baseline  ILC programme  at $\sqrt{s} = 250$ GeV, in the baseline programmes. No beam polarization is assumed for TLEP. The total numbers of Higgs boson produced are also indicated. The ${\rm e}^-$ (${\rm e}^+$) beam of ILC is supposed to be with beams  polarized at a level of 80\% (30\%), leading for electrons and 30\% for positrons (leading  to a cross section increase of 40\% for the Higgsstrahlung process and 134\% for the WW fusion, with respect to the unpolarized cross sections. \label{tab:HiggsCross}} sections.\label{tab:HiggsCross}}  \begin{tabular}{|r|r|r|}  \hline Collider & TLEP 240 & ILC 250 \\ \hline   \hline Total Integrated Luminosity ($\small \inab$) & {\bf 10} & 0.250 \\