We study the Hong-Mandel 2n th-order squeezing of the Hermitian operator, X θ ≡ X1 cos θ + X2 sin θ and amplitude n th-power squeezing of the Hermitian operator, = a n , a is the annihilation operator, α, θ, r and ϕ are arbitrary and the only restriction on these is the normalization condition of the superposed state. We show that the Hong-Mandel 2n th-order squeezing and amplitude odd-power squeezing exhibited by even coherent state enhance in its superposition with vacuum state. Variations of these higher-orders squeezing with different parameters near its maxima have also been discussed.