We construct a two-parameter continuum of type II blow up solutions for the energy-critical nonlinear Schrödinger equation in dimension \( d = 3\) . The solutions collapse to a single energy bubble in finite time and have the form \(\begin{aligned} u(t,x) = e^{i \alpha (t)}\lambda (t)^{\frac{1}{2}}W(\lambda (t) x) + \eta (t, x ),~ ~ t \in [0, T),~ x \in {{\,\mathrm{\mathbb {R}}\,}}^3, \end{aligned}\) where \( W( x) = \big ( 1 + \frac{|x|^2}{3}\big )^{-\frac{1}{2}}\) is the ground state solution, \(\lambda (t) = (T -t)^{- \frac{1}{2} - \nu } \) for suitable \( \nu > 0 \) , \( \alpha (t) = \alpha _0 \log (T - t)\) and \( T= T(\nu , \alpha _0) > 0 \) . Further there holds \( \Vert \eta (t) - \eta _T\Vert _{\dot{H}^1 \cap \dot{H}^2} = o(1)\) as \( t \rightarrow T^-\) for some \( \eta _T \in \dot{H}^{1} \cap \dot{H}^2\) .
