in Chiswell/Hodge exercisee 2.6.2d it asks for the proof of $\{\lnot(\phi\leftrightarrow\psi)\}\vdash((\lnot\phi)\leftrightarrow\psi)$. I've managed to produce half the proof, but I'm unable to produce the other half indicated at D.
$$ \frac{(1)\frac{D^{(1)}}{((\lnot\phi)\rightarrow\psi)}(\rightarrow I) \qquad \frac{\cfrac{(6)\frac{\phi^{(6)}\quad\psi^{(2)}}{\phi\rightarrow\psi}(\rightarrow I)\quad (5)\frac{\psi^{(5)}\quad\phi^{(4)}}{\psi\rightarrow\phi}(\rightarrow I)}{\phi\leftrightarrow\psi}(\leftrightarrow I)\qquad \lnot(\phi\leftrightarrow\psi)}{(4)\cfrac{\bot}{(2)\cfrac{\lnot \phi}{(\psi\rightarrow(\lnot\phi))}(\rightarrow I)}(\lnot I)}(\lnot E)} {((\lnot\phi)\leftrightarrow\psi)}(\leftrightarrow I) $$
I had considered...
$$(1)\frac{\cfrac{\phi\quad\lnot\phi^{(1)}}{\cfrac{\bot}{\psi}(RAA)}(\lnot E)} {((\lnot\phi)\rightarrow\psi)}(\rightarrow I)$$
But that leaves me with an undischarged $\phi$. I'm otherwise unsure of how to produce the $\psi$ for the $(\rightarrow I)$ in the left branch, as an absurdity (other than as proposed) discharges $\lnot\psi$, and I can't use this to construct an absurdity against the assumption $\lnot(\phi\leftrightarrow\psi)$ similar to how I did in the right branch.
At this point in the text, the only rules available are elimination/introduction of $\land$, $\rightarrow$,$\leftrightarrow$,$\lnot$ and RAA.
I would be very grateful to understand this particular exercise further as I'm losing sleep over it.
(Also if someone has formatting advice regarding \frac or some suitable alternative via PM, I would be further grateful.)

This answer is only possible due to the answer provided by MauroAllegranza; however, their answer is in Fitch style, and I wanted to provide a Gentzen style to match the question, in case someone searches for this in the future.
The following is only the solution to D, as provided by Mauro, to sub into the overall proof. For formatting reasons I had to further break it down, hence D1.
Part#1 (D1) $$ D1=\dfrac{(4)\cfrac{\cfrac{\cfrac{\psi^{(4)}\quad\lnot\psi^{(3)}}{\bot}(\lnot E)}{\phi}(RAA)}{\psi\rightarrow\phi}(\rightarrow I)\quad (2)\cfrac{\cfrac{\cfrac{\phi^{(2)}\quad\lnot\phi^{(1)}}{\bot}(\lnot E)}{\psi}(RAA)}{\phi\rightarrow\psi}(\rightarrow I)}{(\phi\leftrightarrow\psi)}(\leftrightarrow I) $$
Part#2 (D)
$$ D= (1)\dfrac{(3)\cfrac{\cfrac{\cfrac{D1^{(3)(1)}}{(\phi\leftrightarrow\psi)}\qquad\lnot(\phi\leftrightarrow\psi)}{\bot}(\lnot E)}{\psi}(RAA)}{((\lnot\phi)\rightarrow\psi)}(\rightarrow I) $$