Let \({\mathcal {H}}_{s+1,N}=(H_s(n),n/N)_{n=0}^{N-1}\) be the s+1-dimensional Hammersley’s point set. Let \(D(\bar{\textbf{x}},(\mathcal {H}_{s+1,N})_{n=0}^{N-1} )\) be the local discrepancy of \((\mathcal {H}_{s+1,N})_{n=0}^{N-1}\) , and let \(D_{s,p} ( (\mathcal {H}_{s+1,N})_{n=0}^{N-1})\) be the \(L_p\) discrepancy of \((\mathcal {H}_{s+1,N})_{n=0}^{N-1}\) . In this Part II of our paper, we prove the Central Limit Theorem for Hammersley’s net: \(\begin{aligned} D(\bar{\textbf{x}},\mathcal {H}_{s+1,N} ) /D_{s+1,2}(\mathcal {H}_{s+1,N}) \overset{w}{\rightarrow }\ \mathcal {N}(0,1), \end{aligned}\) where \(\bar{\textbf{x}}\) is a uniformly distributed random variable in \([0,1]^{s+1}\) and we claim that the lower bound of \(L_p\) discrepancy for p>0 is of the same order as the upper bound: \(\begin{aligned} \frac{ D_{s+1,p}( \mathcal {H}_{s+1,N} )}{ D_{s+1,2}( \mathcal {H}_{s+1,N} )} \overset{N \rightarrow \infty }{\longrightarrow }\ \kappa _p^{1/p}, \quad \kappa _p= \frac{1}{\sqrt{2 \pi }}\int _{-\infty }^{\infty } |u|^p e^{-u^2/2} d u. \end{aligned}\)