Channel  Collider  m_{h}  mSUGRA  mGMSB  mAMSB
V^{∗} → V h → V bb̄  {Tev \atop LC}  \begin{matrix}< ∼ 135 \\ < ∼ 0.7\sqrt{s} \end{matrix}  ± 10%  ± 10%  M_{A} < ∼ 300 : +50%
V V → h → bb̄  LHC  < ∼ 120  ± 10%  ± 10%  M_{A} < ∼ 300 : +50%
V^{∗} → V h → V cc̄  LC  < ∼ 0.7\sqrt{s}  M_{A} < ∼ 500 : ±20%  \begin{matrix}M_{A} < ∼ 200 : < ∼ − 50% \\ 200 < ∼ M_{A} < ∼ 400 : −50% \\ 400 < ∼ M_{A} < ∼ 600 : −20% \end{matrix} \begin{matrix}500 < ∼ M_{A} < ∼ 650 : −20% \\ 300 < ∼ M_{A} < ∼ 500 : −50% \\ M_{A} < ∼ 300 : < ∼ − 50% \end{matrix}

V^{∗} → (V)h → (V)W W^{∗} (LC), LHC ( < ∼ 0.7\sqrt{s}), > ∼ 110

M_{A} < ∼ 150 : ±20%,
for tan β < ∼ 30 or > ∼ 50

like V cc̄ like V cc̄

\begin{matrix}V^{∗} → V h → V τ^{+}τ^{−} \\ V V → h → τ^{+}τ^{−} \end{matrix}  {LC \atop LHC}  \begin{matrix}< ∼ 0.7\sqrt{s} \\ < ∼ 150 \end{matrix}  \begin{matrix}M_{A} < ∼ 150 : ±50%, \\ for tan β > ∼ 50 \end{matrix}  tan β > ∼ 50 : > ∼ 50%  M_{A} < ∼ 500 : +50%

V^{∗} → (V)h → (V)gg (LC), LHC  ?  M_{A} < ∼ 200 : ± 20%  like V cc̄  \begin{matrix}550 < ∼ M_{A} < ∼ 650 : −20% \\ 250 < ∼ M_{A} < ∼ 550 : −50% \\ M_{A} < ∼ 250 : < ∼ − 50% \end{matrix}

gg → h → γγ  LHC  < ∼ 150  \begin{matrix}M_{A} < ∼ 150 : ±20% \\ tan β < ∼ 30 or > ∼ 50 \end{matrix}  like V cc̄  \begin{matrix}550 < ∼ M_{A} < ∼ 750 : −20% \\ 250 < ∼ M_{A} < ∼ 550 : −50% \\ M_{A} < ∼ 250 : < ∼ − 50% \end{matrix}

tt̄→ tt̄h → tt̄bb̄  LHC  < ∼ 130  SM like

SM like +50% for tan β > ∼ 50

M_{A} < ∼ 300 : +50%
γγ → h → bb̄  γC  ?  M_{A} < ∼ 150 : +50%  SM like  M_{A} < ∼ 300 : +50%
γγ → h → W W^{∗}  γC  ?  \begin{matrix}M_{A} < ∼ 200 : \\ −20% ÷ +50% \end{matrix}  \begin{matrix}M_{A} < ∼ 200 : < ∼ − 50% \\ 200 < ∼ M_{A} < ∼ 400 : −50% \\ 400 < ∼ M_{A} < ∼ 600 : −20% \end{matrix} \begin{matrix}500 < ∼ M_{A} < ∼ 650 : −20% \\ 250 < ∼ M_{A} < ∼ 500 : −50% \\ M_{A} < ∼ 250 : < ∼ − 50% \end{matrix}

γγ → h → τ^{+}τ^{−}  γC  ?

tan β ∼ 50 : ±50%
tan β < 50 : +50%
for M_{A} < ∼ 150

tan β > ∼ 50 : > ∼ 50% M_{A} < ∼ 600 : +50%

γγ → h → γγ  γC  ?  \begin{matrix}M_{A} < ∼ 200 : \\ −20% ÷ +50% \end{matrix}  like γγ → h → W W^{∗}  \begin{matrix}500 < ∼ M_{A} < ∼ 650 : −20% \\ 250 < ∼ M_{A} < ∼ 500 : −50% \\ M_{A} < ∼ 250 : < ∼ − 50% \end{matrix}

μ^{+}μ^{−} → h → bb̄  μC  up to \sqrt{s} < 2m_{W}  \begin{matrix}M_{A} < ∼ 250 : +50% \\ M_{A} < ∼ 150, tan β > 50 : −50% \end{matrix} \begin{matrix}200 < ∼ M_{A} < ∼ 600 : +50% \\ M_{A} < ∼ 200 : > ∼ 50% \end{matrix} \begin{matrix}450 < ∼ M_{A} < ∼ 900 : +50% \\ M_{A} < ∼ 450 : > ∼ 50% \end{matrix}
μ^{+}μ^{−} → h → W W^{∗}  μC  up to \sqrt{s} < 2m_{W}  ± 10%  tan β ≃ 50 : +50%  M_{A} < ∼ 600 : +50%
μ^{+}μ^{−} → h → τ^{+}τ^{−}  μC  up to \sqrt{s} < 2m_{W}  \begin{matrix}M_{A} < ∼ 250 : +50% \\ M_{A} < ∼ 150, tan β > 50 : −50% \end{matrix}  like μ^{+}μ^{−} → h → bb̄  like μ^{+}μ^{−} → h → bb̄