You are rotating the coordinate axes, not the points. Let $(x,y)$ be a point in the plane. Then $(x,y)=x(1,0)+y(0,1)$. A rotation of the coordinates by $45^{\circ}$ takes $(1,0)$ to $(\frac{1}{\sqrt{2}},\frac{1}{\sqrt{2}})$ and $(0,1)$ to $(\frac{-1}{\sqrt{2}},\frac{1}{\sqrt{2}})$.
To find the new coordinates $(x',y')$ we must solve $$x'(\frac{1}{\sqrt{2}},\frac{1}{\sqrt{2}})+y'(\frac{-1}{\sqrt{2}},\frac{1}{\sqrt{2}})=(x,y)$$
Grouping terms on the left of the equation and equating coordinates gives $$x'-y'=\sqrt{2}x$$ $$x'+y'=\sqrt{2}y$$
The $\sqrt{2}$ corresponds to the length of the diagonal of a unit square which is $2$ in taxicab geometry. Replacing $\sqrt{2}$ with $2$ in out system of equations gives us $$x'-y'=2x$$ $$x'+y'=2y$$
We can solve this system for $x'$ and $y'$ to obtain $$x'=x+y$$ $$y'=y-x$$.
Edit:
I see many saying that this transformation is a rotation followed by a dilation but this is not accurate. A rotation must preserve length. In this case the length is the taxicab length. Take $(1,0)$. It has a taxicab length of $1$ from the origin. If we rotate this by $45^{\circ}$ under the standard metric we get $(\frac{1}{\sqrt{2}}, \frac{1}{\sqrt{2}})$. But the same rotation under the taxicab metric must give $(\frac{1}{2},\frac{1}{2})$ to preserve the length of the rotated vector.
My proof above can be confusing because I don't make that adjustment until after the rotation with respect to the standard metric.