\subsection{Category \texorpdfstring{$\mathcal O$}{O} and the spectral filtration}\label{fin:kzsection} Let \(V_\Gamma\) be the original cell lattice of a finite left cell \(\Gamma\), with its canonical basis. For a root of unity \(\zeta\), choose a positive real \(\lambda\) with \(\exp(2\pi\mathrm i\lambda)=\zeta\), and use the complete local ring \(R=\mathbb C[[u]]\) with \(v=\exp(2\pi\mathrm i(\lambda+u))\). This identifies \(R\) with the completion at \(v=\zeta\), since the linear term of \(v-\zeta\) is nonzero. Use the corresponding Cherednik category \(\mathcal O_R\), with standard module \(\Delta_R(U)\) for an ordinary group label \(U\). This category has the finite split highest-weight realization of \cite[Theorem~5.2]{RouquierSchur}. Its KZ functor is exact, represented by the projective \(P_{\mathrm{KZ}}\), and sends that projective to the regular Hecke module. These statements follow from \cite[Theorems~5.13, 5.15 and 5.16]{GGOR} and \cite[Proposition~4.36 and \S5.2]{RouquierSchur}, with the KZ normalization in \cite[\S15]{RouquierErrata}. Set \[ F_R(M)=\bigl(\mathrm{KZ}_R(M)\bigr)^\dagger, \] where the superscript denotes twisting the Hecke action by \(\dagger\). For type \(B\) the Dunkl--Griffeth parameters on this line are \[ c_0=-2a(\lambda+u),\qquad d_0-d_1=-4b(\lambda+u),\qquad d_0+d_1=0. \] In the monodromy normalization of \cite[(1.18)]{DunklGriffeth}, the generators \(T_i\) attached to \(s_i\) have roots \(v^b,-v^{-b}\) for \(i=0\) and \(v^{2a},-1\) for \(i>0\). Thus \(N_{s_0}=T_0\) and \(N_{s_i}=v^{-a}T_i\) for \(i>0\). For a finite multiset \(Z\) with decreasing list \(z_1,\ldots,z_m\), write \(n(Z)=\sum_{i=1}^{m}(i-1)z_i\). For a partition \(U\), \(n(U)\) applies this definition to its list of row lengths. \begin{lemma}\label{fin:strict} In the residue category at each positive logarithmic lift, write \(\Delta(U)\) for the residue standard and \(L(U)\) for its simple head. If \(L(U')\) occurs in \(\Delta(U)\) and \(U'\ne U\), then \(a_{\mathrm{Sch}}(U')0}\). Form the two-variable Hecke algebra over \(\mathbb Z[v^{\pm1},t^{\pm1}]\) with lexicographic exponent order, primary variable \(v\), and weights \((a,0)\), \((ra,1)\). Specializing \(v=z^N\) and \(t=z\) for sufficiently large integral \(N\) preserves all required strict signs in the finite canonical basis and the orders of the Schur degrees. For a fixed primary spectral threshold the selected simple labels thus form a spectral threshold at \((Na,Nra+1)\), which is off the wall. The corresponding coordinate span lifts to a two-variable coordinate ideal. Indeed one chooses \(N\) so that the specialization is injective on each finite exponent support of the relevant structure coefficients and the matrix coefficients in integral generic Specht models. Vanishing into excluded coordinates and vanishing in excluded irreducibles lift. Its dimension is the sum of the squares of dimensions of the selected labels, as at the one-variable specialization, so the lifted ideal has precisely their generic support. At \(t=1\) the specialized basis changes to the wall canonical basis by a constant integral unitriangular matrix. Every lexicographically negative term has nonpositive primary exponent, so the transition and its inverse have coefficients in \(\mathbb Z[v^{-1}]\). The transition is bar invariant and hence constant. The primary Schur degrees are the wall degrees. In the cancellation-free Schur product \cite[Theorem~3.2]{ChlouverakiJacon}, use the Ariki--Koike parameters \(q=v^{2a}\), \(Q_0=v^{2ra}t^2\), \(Q_1=-1\). Each cross factor with zero primary exponent is \(1+t^2\) or \(1+t^{-2}\), which becomes \(2\), and the highest primary coefficient of every other factor survives. Over \(\mathbb Q(v)\) the wall Hecke algebra is split semisimple. Its generic primitive idempotents are regular at \(t=1\), since the finite Schur elements are units in that local ring and the trace-dual basis is integral. The lifted coordinate ideal is saturated, so it is the image of the sum of the selected idempotents over that local ring: this equality holds generically and both submodules are saturated. It follows that its specialized constant rational coordinate subspace is exactly the required spectral ideal. It remains to show that this subspace is coordinate in the wall basis. The Schur maximum degree is constant on Rouquier blocks of the two-colour integral-charge cyclotomic algebra by \cite[Proposition~3.18]{BroueKim}. Apply this to the Ariki--Koike generators \(v^bN_{s_0}\) and \(v^aN_{s_i}\) for \(i>0\), with parameters \(x,x^r,-1\), where \(x=v^{2a}\). The change from normalized generators uses only Laurent units. Substituting \(x=v^{2a}\) sends each allowed denominator \(x^m-1\) to \(v^{2am}-1\), so the aggregate block idempotent specializes in the same integral localization. Thus the spectral projector belongs to the Hecke algebra over \(\mathbb Z[v^{\pm1},(v^m-1)^{-1}:m\geq1]\). This ring expands in integer Laurent series in \(v^{-1}\), since every inverted denominator is monic at infinity. The projector is orthogonal for the positive original trace form, whose wall canonical Gram matrix tends to the identity. Its range is the constant subspace just obtained. Therefore its limit is the Euclidean orthogonal projector onto that subspace. Each diagonal entry of the limit is the limit of the trace of \(C_wC_w^*\) multiplied by the central idempotent. This trace is in the displayed integral ring and lies between zero and \(\tau(C_wC_w^*)\to1\). Its limit is an integer, hence zero or one. An orthogonal projector with such diagonal entries is coordinate, since the squared norm of its image of a unit coordinate vector equals the corresponding diagonal entry. The wall spectral ideal is therefore a \(C\)-coordinate span. \end{proof}