the soft SUSY breaking scalar masses in addition to the Scherk-Schwarz SUSY breaking and obtaining the heavy Higgs mass due to the effect of the scalar mass has also been discussed.

LHC/ILC Connection
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If a low-energy SUSY scenario with squarks/gluinos below $\sim$ 2-3 TeV is realized, the LHC will see SUSY signals. Many channels from squark and/or gluino decays may be observed and measured. If the decay chain is long enough, like the first squark decay chain shown in fig.\[fig:chain\](a), from a knowledge of kinematical endpoints, in particular those of the invariant mass distributions $m_{qll}$, $m_{ql(low)}$, $m_{ql(high)}$ and $m_{ll}$, the masses of the unstable particles can be reconstructed [@Baer:1995va]. Indeed, the endpoints of these distributions can be expressed explicitly in terms of $m_{\tilde{q}}$, $m_{\tilde{\chi}^0_{2,3}}$, $m_{\tilde{\chi}^0_{1}}$ and $m_{\tilde{l}}$. However, ambiguities in the masses extracted from endpoint measurements can occur (even when experimental uncertainties are neglected) since the kinematical endpoints are composite functions of the unknown masses. This is shown in fig.\[fig:chain\](b) where the false minimum around 80 GeV is found [@Gjelsten:2005sv]. Moreover, the same visible final state $l^+l^-q$ can be generated by a different SUSY decay chain (second decay chain in fig.\[fig:chain\](a)), or a Kaluza-Klein decay chain in a non-supersymmetric 