Start with the assumption that \(\RE s > 1\text{.}\) Now compute the logarithmic derivative of \(\zeta\text{:}\)
\begin{align*}
\frac{\zeta\dd}{\zeta} \amp= \frac{d}{ds} \log \zeta(s) = \frac{d}{ds} \log \prod_p (1 - p^{-s})\inv\\
\amp= \frac{d}{ds} \sum_p \log (1-p^{-s})\inv\\
\amp= -\sum_p \frac{d}{ds} \log (1-p^{-s})\\
\amp= -\sum_p \frac{\log p} {p^s(1-p^{-s})}\\
\amp= -(\sum_p \frac{\log p}{p^s} + \sum_p \frac{\log p}{p^s(p^s - 1)}).\\
\amp= -(\Phi(s) + \sum_p \frac{\log p}{p^s(p^s - 1)})
\end{align*}
This gives the identity
\begin{equation*}
-\frac{\zeta\dd}{\zeta} = \Phi(s) + \sum_p\frac{\log p}{p^s(p^s - 1)}.
\end{equation*}
Notice that the series on the right hand side converges for \(\RE s > \frac{1}{2}\text{.}\) From Step II above, we know that \(\zeta - \frac{1}{s-1}\) is holomorphic on \(\RE s > 0\text{,}\) and so
\begin{equation*}
\zeta = (\zeta -\frac{1}{s-1}) + \frac{1}{s-1}
\end{equation*}
is meromorphic on \(\RE s \geq 0\) with a simple pole at \(s = 1\text{.}\) Likewise, \(\zeta\dd\) will be meromorphic with a pole at \(s = 1\) of order 2. Then \(\zeta\dd/\zeta\) is also a meromorphic function on \(\RE s > 0\) with poles at \(s = 1\) and at the zeros of \(\zeta\text{,}\) which implies for \(\Phi\text{,}\) which is
\begin{equation}
\Phi = -\frac{\zeta\dd}{\zeta} - \sum_p\frac{\log p}{p^s(p^s - 1)},\tag{3.3.1}
\end{equation}
that we have a meromorphic extension of \(\Phi\) to \(\RE s > \frac{1}{2}\) with poles at \(s = 1\) and the zeros of \(\zeta\text{.}\)
Now let's analyze the zeros. First, because \(\zeta(s) = \cc{\zeta(\cc s)}\text{,}\) we see that if \(s\) is zero of \(\zeta\) then so is \(\cc{s}\text{.}\) Now let \(a\in \R\text{.}\) If \(s_0 = 1 + ia\) is a zero of \(\zeta\) of order \(\mu \geq 0\text{,}\) then \(\zeta = (s - s_0)^\mu h(s)\) for some holomorphic function \(h\) that is non-zero near \(s_0\text{.}\) Computing the logarithmic derivative gets us
\begin{equation*}
-\frac{\zeta\dd}{\zeta} = -\frac{\mu}{s - s_0} + H(s)
\end{equation*}
for some function \(H = \log h\) holomorphic near \(s_0\text{.}\) The function \(\Phi(s_0 + \eps)\) then has a simple pole at \(\eps = 0\text{,}\) and by the residue theorem
\begin{equation*}
\lim_{\eps \to 0} \eps \Phi(1 + \eps + ia) = -\mu.
\end{equation*}
Now, consider
\begin{equation*}
\Phi(1+\eps) = \sum_p \frac{\log p}{p^{1 + \eps}},
\end{equation*}
and note that the terms are positive for \(\eps > 0\text{.}\) Then
\begin{equation*}
\sum_p \frac{\log p}{p^{1 + \eps}}(p^{\frac{ia}{2}} + p^{\frac{-ia}{2}})^2 \geq 0.
\end{equation*}
Multiplying this out gives
\begin{equation*}
\Phi(1 + \eps -ia) + 2\Phi(1 + \eps) + \Phi(1 + \eps + ia) \geq 0.
\end{equation*}
From Part II, as noted above we have that \(s = 1\) is a simple pole of \(-\zeta\dd/\zeta\) with residue 1, and so
\begin{equation*}
\lim_{\eps \to 0} \eps \Phi(1_+ \eps) = 1.
\end{equation*}
Then
\begin{align*}
\amp\lim_{\eps \to 0} \eps(\Phi(1 + \eps -ia) + 2\Phi(1 + \eps) + \Phi(1 + \eps + ia))\\
\amp= -2\mu + 2 \geq 0
\end{align*}
and so \(0 \leq \mu \leq 1\text{.}\) As we intend to show that \(\mu = 0\text{,}\) we need more. So assume as well that \(\zeta\) has a zero at \(s_1 = 1 \pm i2a\) with order \(\nu \geq 0\text{.}\) (That is, we are admitting the possibility that there is no zero at those points.) Again, note that
\begin{equation*}
\lim_{\eps \to 0} \eps \Phi(1 + \eps \pm i2a) = -\nu.
\end{equation*}
Then the same idea applied to
\begin{equation*}
\sum_p \frac{\log p}{p^{1 + \eps}}(p^{\frac{ia}{2}} + p^{\frac{-ia}{2}})^4 \geq 0
\end{equation*}
produces the equation
\begin{equation*}
6 - 8 \mu - 2 \nu \geq 0.
\end{equation*}
This requires that \(\mu = 0\) since \(\mu, \nu \geq 0\text{.}\) We have shown that if \(\zeta\) has a zero of the form \(s_0 = 1 + ia\text{,}\) then it must have order 0, and hence not be a zero. That is, \(\zeta\) has no zeros on the line \(\RE s > 1\text{.}\)
Finally, recall that the poles of
\(\Phi\) are
\(s = 1\) and the zeros of
\(\zeta\text{,}\) none of which can lie on
\(\RE s = 1\text{.}\) If we trace through the form of
\(\Phi\) from
(3.3.1) and the implications of Step II, we conclude that
\(\Phi - \frac{1}{s-1}\) is holomorphic on
\(\RE s \geq 1\text{.}\)