\section{The exact projective optimum} \label{app:pvmexact} We now match a lower bound over every complex orthonormal basis with an explicit four-result measurement. Throughout this appendix, \(k=1000001/1000000\), the preparation space is the original \(\C^4\), and the prior and loss are those of Eq.~\eqref{eq:principalprior}. The tensor operators below encode one readout basis; they do not supply additional encoded copies. \subsection{An attaining basis and its exact risk} Use \(\beta_1,\beta_2,\beta_3,D_0,D_2,\delta\) as defined in the main text. The equation \begin{equation} (\beta_1D_0-D_2\beta_3h)^2(1+h^2)-\beta_2^2\delta^2h^2=0, \qquad h>\frac{\beta_1D_0}{D_2\beta_3}, \label{eq:pvmquartic} \end{equation} selects a unique positive root \(h_*\). Indeed, on this interval the equation is equivalent to \((D_2\beta_3-\beta_1D_0/h)\sqrt{1+h^2}=\beta_2\delta\). Its left side increases strictly from zero to infinity, whereas the right side is positive. The ancillary \texttt{candidate.json} also specifies a rational isolating interval for this root. Set \(x_*=h_*/\sqrt{1+h_*^2}\) and \(y_*=1/\sqrt{1+h_*^2}\). The four vectors displayed in the main text are orthonormal: \(x_*^2+y_*^2=1\) and \(1+\omega+\omega^2=0\) give their norms and inner products directly. For \(P_j=v_jv_j^\dagger\), \(j=0,1,2\), \[ \Tr(S_kP_j)=\frac{\tau_*}{3},\qquad \Tr(B_kP_j)=\frac{A_*\omega^j}{3}, \] whereas \(\Tr(B_kP_3)=0\). Completing the square separately at each outcome gives the optimal reports stated above and the attained risk \begin{equation} \mathcal L_*=100-g_*,\qquad g_*=A_*^2/\tau_*. \label{eq:pvmattainedrisk} \end{equation} No stationarity or restricted-family argument is used as a global lower bound in this step. All quantities needed by the bound lie in the real algebraic field \(K=\Q[h_*]\). In particular, \[ y_* =\frac{D_2\beta_3h_*-\beta_1D_0}{\beta_2\delta h_*},\qquad x_*=h_*y_*. \] The selected branch makes \(y_*>0\), and Eq.~\eqref{eq:pvmquartic} gives \(x_*^2+y_*^2=1\). Thus the square roots in the basis introduce no additional field for the risk or the certificate coefficients. The exact enclosure of the final optimum is \begin{equation} \begin{split} 94.555744248543241682944116234978 &<\mathcal L_{\mathrm{PVM},k}\\ &<94.555744248543241682944116234979. \end{split} \label{eq:pvmexactenclosure} \end{equation} The enclosure describes the algebraic value in Eq.~\eqref{eq:mainpvmexact}; equality of upper and lower risks follows from the proof below, not from the width of this interval. \subsection{A denominator bound with exact contact} For any rank-one PVM write \(s_i=\Tr(S_kP_i)\) and \(w_i=|\Tr(B_kP_i)|^2\). Since \(S_k\succeq pI\), \(s_i\ge p>0\). For \(\alpha=\tau_*/3\), define \[ H_\alpha(s)=\frac1\alpha-\frac{s-\alpha}{\alpha^2} +\frac{(s-\alpha)^2}{p\alpha^2}. \] The exact identity \begin{equation} H_\alpha(s)-\frac1s =\frac{(s-\alpha)^2(s-p)}{p\alpha^2s}\ge0 \label{eq:pvmcontactmajorant} \end{equation} holds for every competing outcome. With \[ G_2=\sum_iw_i,\quad D_3=\sum_iw_i(s_i-p),\quad D_4=\sum_iw_i(s_i-p)^2, \] it gives \begin{equation} \sum_i\frac{w_i}{s_i} \le \frac{G_2}{p}-\frac{2\alpha-p}{p\alpha^2}D_3 +\frac{D_4}{p\alpha^2}. \label{eq:pvmcontactgain} \end{equation} At the proposed basis the three signal probabilities equal \(\alpha\), and the remaining \(w_i\) vanishes. Thus this inequality has exact contact there, unlike the reciprocal secant. \subsection{Universal moments of complex projective measurements} Let \(R=\sum_iP_i\otimes P_i\) and \(Q=R^{\top_2}\), with the partial transpose convention of Appendix~\ref{app:pvmmoments}. Both are orthogonal projections. Moreover, \[ \Tr_2R=I,\qquad T_3=R_{12}R_{23}=\sum_iP_i^{\otimes3},\qquad T_4=R_{12}R_{23}R_{34}=\sum_iP_i^{\otimes4}. \] These facts hold for arbitrary complex basis vectors. The latter tensors are positive, and their row and column indices are separately symmetric. They express \(D_3\) and \(D_4\) as polynomials of degree two and three in the entries of \(\mathsf R\), the matrix of \(R\) in the normalized symmetric basis of Appendix~\ref{app:pvmmoments}. Average these polynomial moments over \(D(e^{i\phi})\otimes D(e^{i\phi})\) and complex conjugation. The real ladder and diagonal \(S_k\) make all three objective components invariant. This is an average of moment vectors of genuine complex bases, not an assumption that a competitor is real or covariant. For lexicographically ordered pairs \(A=(a,b)\), \(a\le b\), put \[ m_A=\begin{cases}1,&a=b,\\2,&a