Let \(K = \ker \psi\text{.}\) We first define a function \(\eta \colon R/K \rightarrow \psi(R)\) by \(\eta(r + K) = \psi(r)\text{.}\) We must show that \(\eta\) is well-defined. If \(r' = r + k\) is a different element of the coset \(r+K\text{,}\) where \(k \in K\text{,}\) then
\begin{equation*}
\psi(r') = \psi(r + k) = \psi(r) + \psi(k) = \psi(r) + 0 = \psi(r).
\end{equation*}
Therefore, \(\eta(r)\) does not depend on the choice of representative from the coset \(r + K\text{.}\) Furthermore, \(\eta\) is uniquely defined since \(\psi = \eta\phi\text{.}\)
In order to show that \(\eta\) is a ring homomorphism, we need to show that it preserves addition and multiplication. Suppose that \(r\) and \(s\) are any two elements of \(R\text{.}\) Then,
\begin{align*}
\eta((r + K) + (s+K)) &= \eta((r+s) + K)\\
&= \psi(r + s)\\
&= \psi(r) + \psi(s)\\
&= \eta(r + K) + \eta(s+K).
\end{align*}
The calculation for multiplciation is similar:
\begin{align*}
\eta( (r + K)( s +K )) & = \eta(r s +K )\\
& = \psi(r s)\\
& = \psi(r) \psi(s)\\
& = \eta( r + K ) \eta( s + K ).
\end{align*}
Therefore, \(\eta\) is a homomorphism.
It is clear that
\(\eta\) is onto. To show that
\(\eta\) is one-to-one, suppose that
\(\eta(r + K) = \eta(r'+K)\text{.}\) Then
\(\psi(r) = \psi(r')\) and so
\(\psi(r-r') = \psi(r) - \psi(r') = 0\text{.}\) Therefore,
\(r-r' \in K\text{,}\) so
\(r\) and
\(r'\) are in the same coset, which shows that
\(\eta\) is one-to-one.