Let \(g_1, g_2 \in H\) be arbitrary and put \(g_3 = g_1g_2\text{.}\) Let \(M_i\) be the fixed field of \(g_i\text{,}\) let \(\pi_i \in A_{M_i}\) be a uniformizer of \(M_i\text{,}\) and put \(\rho_i = r'(g_i) = \Norm_{M_i/K}(\pi_i) \in A_K\text{.}\) Put \(\rho = \rho_1 \rho_2/\rho_3\text{;}\) note that
\begin{equation*}
v_K(\rho_i) = f(M_i/K) v_{M_i}(\pi_i) = f(M_i/K) = d_K(g_i),
\end{equation*}
which implies that
\(v_K(\rho) = 0\) and hence
\(\rho \in U_K\text{.}\) Our goal is to check that
\(\rho \in \Norm_{L/K} A_{L}\text{;}\) our plan is to rephrase this as a relation among units, to which
Lemma 5.2.4 will apply.
We first make an adjustment at the level of group elements. Put \(G = \Gal(L^{\unr}/K^{\unr})\text{.}\) Choose \(\phi \in H\) such that \(d_K(\phi) = 1\text{.}\) Put \(d_i = d_K(g_i)\) and \(\tau_i = g_i^{-1} \phi^{d_i} \in G\text{;}\) then
\begin{equation*}
\tau_3 = g_2^{-1} g_1^{-1} \phi^{d_1 + d_2} = g_2^{-1} \phi^{d_2} (\phi^{-d_2} g_1 \phi^{d_2})^{-1} \phi^{d_1}.
\end{equation*}
It will be convenient to replace \(g_1\) and \(\tau_1\) with
\begin{equation*}
g_1' = \phi^{-d_2} g_1 \phi^{d_2}, \qquad \tau_1' = (g_1')^{-1} \phi^{g_1},
\end{equation*}
so that \(\tau_1' \tau_2 = \tau_3\text{.}\) We correspondingly define \(M_1'\) to be the fixed field of \(g_1'\) and set \(\pi_1' = \pi_1^{\phi^{n_2}} \in A_{M_1'}\text{,}\) noting that \(\Norm_{M_1'/K}(\pi_1') = \Norm_{M_1/K}(\pi_1) = \rho_1\text{.}\)
Let \(N\) be a finite subextension of \(L^{\unr}/L\) containing \(M_1, M_2, M_3, M_1'\text{.}\) Set
\begin{equation*}
\sigma_i = \pi_i \pi_i^\phi \cdots \pi_i^{\phi^{d_i-1}}, \qquad \sigma_1' = (\pi_1') (\pi_1')^\phi \cdots (\pi_1')^{\phi^{d_1-1}}
\end{equation*}
and
\(u = \sigma_1' \sigma_2 / \sigma_3 \in U_N\text{;}\) by
Proposition 5.2.3 we have
\(\rho = \Norm_G(u)\text{.}\) By defining
\begin{equation*}
u_1 = (\pi_1')^{1-\tau_2}, u_2 = \pi_2/\pi_1', u_3 = \pi_3/\pi_1' \in U_N
\end{equation*}
and using the equality \(\tau_1' \tau_2 = \tau_3\text{,}\) we compute that
\begin{equation*}
u^{\phi-1} = (\pi_1')^{\tau_1' - 1} \pi_2^{\tau_2 - 1} / \pi_3^{\tau_3 - 1} = u_1^{\tau_1'-1} u_2^{\tau_2 - 1} / u_3^{\tau_3 - 1}
\end{equation*}
vanishes in
\(H_0(G, U_N)\text{;}\) by
Lemma 5.2.4 we obtain
\(\Norm_G(u) \in \Norm_{N/K} U_N\text{,}\) proving the claim.