mSUGRA : m_{h} < ∼ 124 GeV, tan β > ∼ 3.3
Channel TeV LHC LC γC μC
V^{∗} → V h → V bb̄ ± 10%  ± 10%
V V → h → bb̄  ± 10%
V^{∗} → V h → V cc̄  M_{1/2} < ∼ 350 : ± 20%

V^{∗} → V h → V W W^{∗} M_{1/2} < ∼ 300 : ±20%, for tan β < ∼ 30 or > ∼ 50

V^{∗} → V h → W W^{∗} M_{1/2} < ∼ 300 : ±20%, for tan β < ∼ 30 or > ∼ 50

V^{∗} → V h → V τ^{+}τ^{−}  \begin{matrix}M_{1/2} < ∼ 300 : ±50%, \\ for tan β > ∼ 50 \end{matrix}
V V → h → τ^{+}τ^{−}  \begin{matrix}M_{1/2} < ∼ 300 : ±50%, \\ for tan β > ∼ 50 \end{matrix}
V^{∗} → V h → V gg  M_{1/2} < ∼ 350 : ± 20%
V V → h → gg  M_{1/2} < ∼ 350 : ± 20%
gg → h → γγ  \begin{matrix}M_{1/2} < ∼ 300 : ±20% \\ tan β < ∼ 30 or > ∼ 50 \end{matrix}
tt̄→ tt̄h → tt̄bb̄  SM like
γγ → h → bb̄  M_{1/2} < ∼ 300 : +50%
γγ → h → W W^{∗}  \begin{matrix}M_{1/2} < ∼ 350 : \\ −20% ÷ +50% \end{matrix}

γγ → h → τ^{+}τ^{−}

tan β ∼ 50 : ±50%
tan β < 50 : +50%
for M_{1/2} < ∼ 300
γγ → h → γγ  \begin{matrix}M_{1/2} < ∼ 350 : \\ −20% ÷ +50% \end{matrix}
μ^{+}μ^{−} → h → bb̄  \begin{matrix}M_{1/2} < ∼ 400, M_{0} < ∼ 600 : +50% \\ M_{1/2} < ∼ 300, tan β > 50 : −50% \end{matrix}
μ^{+}μ^{−} → h → W W^{∗}  ± 10%
μ^{+}μ^{−} → h → τ^{+}τ^{−}  \begin{matrix}M_{1/2} < ∼ 400, M_{0} < ∼ 600 : +50% \\ M_{1/2} < ∼ 300, tan β > 50 : −50% \end{matrix}