I am looking at the following exercise:
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Could you give me some hints how we could show that?
Do we use the matrix of the Weingarten map with respect to the basis $\{\sigma_u,\sigma_v\}$ of the tangent plane? But how exactly?
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EDIT1:
The matrix of the Weingarten map with respect to the basis $\{\sigma_u,\sigma_v\}$ of the tangent plane is $$\mathcal{F}_I^{-1}\mathcal{F}_{II}= \begin{pmatrix} \cos^2 v & 0 \\ 0 & 1 \end{pmatrix}^{-1}\begin{pmatrix} -\cos^2 v & 0 \\ 0 & -1 \end{pmatrix}=\frac{1}{\cos^2 v}\begin{pmatrix} -\cos^2 v & 0 \\ 0 & -\cos^2 v \end{pmatrix}=\begin{pmatrix} -1 & 0 \\ 0 & -1 \end{pmatrix}$$
We have that $$\mathcal{F}_I^{-1}\mathcal{F}_{II}= \begin{pmatrix} a & c \\ b & d \end{pmatrix}$$ where $-\textbf{N}_u=a\sigma_u+b\sigma_v$ and $-\textbf{N}_v=c\sigma_u+d\sigma_v$.
Therefore, we get $-\textbf{N}_u=-\sigma_u\Rightarrow \textbf{N}_u=\sigma_u \Rightarrow \textbf{N}=\sigma+A(v)$ and $-\textbf{N}_v=-\sigma_v \Rightarrow \textbf{N}_v=\sigma_v \Rightarrow \textbf{N}=\sigma+B(u)$.
From the relations $\textbf{N}=\sigma+A(v)$ and $\textbf{N}=\sigma+B(u)$, we see that $A(v)=B(u)$ must be a constant. So $\textbf{N}=\sigma+\tilde{C}$.
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EDIT2:
Could you give me some hints how we could find a parametrization of $S^2$ with the above first and second fundamental forms?


With the important difference that it isn't an open subset of 'the' unit-sphere, but of a unit sphere, in your case centered at $-\tilde{C}$.
– Georg Lehner Jan 09 '16 at 19:53