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| \section{The exact rank--error frontier under unitary holonomy} | |
| The exact completion rank can be discontinuous under perturbation. A | |
| different and quantitatively meaningful problem fixes an error tolerance | |
| while retaining the parallel structure required by the binary module action. | |
| This section gives the complete answer for unitary flat coefficient bundles. | |
| All dimensions in this section are complex dimensions. | |
| Let $M$ be a connected compact Riemannian manifold, and let | |
| $(V,\nabla)$ be a rank-$n$ flat Hermitian vector bundle with unitary | |
| holonomy. Let $B\in\Omega^k(M;V)$, with $k\ge3$, and put | |
| $F=d_\nabla B$. An admissible subspace of coefficient directions is a | |
| parallel subbundle $W\subseteq V$, with its parallel orthogonal projector | |
| $P_W$. Its projected model is $B_W=P_WB$. Flatness and parallelism give | |
| \[ | |
| d_\nabla B_W=P_WF,\qquad d_\nabla(P_WF)=0. | |
| \] | |
| Thus the projected data admit the usual central completion with auxiliary | |
| bundle $W$. Equivalently, if one keeps $B$ fixed and uses $P_WF$ as the | |
| cancelled defect, the uncancelled square of the graded differential is | |
| $(I-P_W)F$. These are two precise interpretations of the same error | |
| criterion, not a claim that an incompletely cancelled model is homological. | |
| Define | |
| \[ | |
| \mathcal E_r(F)= | |
| \min_{\substack{W\text{ parallel}\\\operatorname{rank}W\le r}} | |
| \|(I-P_W)F\|_{L^2}^2, | |
| \qquad 0\le r\le n. \tag{U1} | |
| \] | |
| For a fixed $W$, the same minimum is obtained if one optimizes over all | |
| closed $W$-valued forms $G$ in place of $P_WF$: the pointwise orthogonal | |
| projection is already the best approximation, and it is closed. | |
| Fix $o\in M$ and identify $V_o$ with $\mathbb C^n$. Let $H\subseteq U(n)$ | |
| be the closure of the holonomy group. For almost every $x$, choose a | |
| measurable family of parallel transports $T_x:V_x\to V_o$. If | |
| $F_x=\sum_\alpha f_\alpha(x)\,e_\alpha(x)$ in an orthonormal frame of | |
| exterior forms, define the seed Gramian and its compact-group average by | |
| \[ | |
| C=\int_M\sum_\alpha | |
| T_x f_\alpha(x)\,\bigl(T_xf_\alpha(x)\bigr)^*\,dx, | |
| \qquad | |
| \widehat C=\int_H h C h^*\,dh. \tag{U2} | |
| \] | |
| The Haar measure is normalized to have mass one. One can construct the | |
| measurable choices using a countable coordinate cover, one chosen path to | |
| each chart, local flat frames, and a measurable partition of that cover. | |
| The integral is finite because $\operatorname{tr}C=\|F\|_{L^2}^2$. | |
| Changing the chosen paths conjugates each pointwise summand by an element | |
| of the holonomy group, so its Haar average is unchanged. Consequently | |
| $\widehat C$ is independent of these path choices. | |
| Choose the unitary isotypic decomposition | |
| \[ | |
| V_o=\bigoplus_{\lambda} | |
| \bigl(\mathbb C^{m_\lambda}\otimes E_\lambda\bigr), | |
| \qquad d_\lambda=\dim E_\lambda, | |
| \] | |
| where the $E_\lambda$ are pairwise inequivalent irreducible $H$-modules. | |
| Let $C_\lambda$ be the \emph{unnormalized} partial trace over $E_\lambda$ | |
| of the corresponding diagonal block of $C$. Write its eigenvalues as | |
| \[ | |
| \alpha_{\lambda,1}\ge\cdots\ge | |
| \alpha_{\lambda,m_\lambda}\ge0. | |
| \] | |
| \begin{theorem}[Unitary completion rank--error law] | |
| The quantities above satisfy | |
| \[ | |
| \widehat C | |
| =\bigoplus_\lambda | |
| \left(\frac{C_\lambda}{d_\lambda}\otimes I_{E_\lambda}\right), | |
| \tag{U3} | |
| \] | |
| and the exact error frontier is | |
| \[ | |
| \boxed{\displaystyle | |
| \mathcal E_r(F)=\operatorname{tr}C- | |
| \max_{\substack{0\le k_\lambda\le m_\lambda\\ | |
| \sum_\lambda d_\lambda k_\lambda\le r}} | |
| \sum_\lambda\sum_{j=1}^{k_\lambda} | |
| \alpha_{\lambda,j}.} \tag{U4} | |
| \] | |
| In particular, the exact minimum rank is | |
| \[ | |
| r_{\mathrm{exact}} | |
| =\sum_\lambda d_\lambda\operatorname{rank}C_\lambda | |
| =\operatorname{rank}\widehat C. \tag{U5} | |
| \] | |
| This is the dimension of the smallest parallel subbundle containing the | |
| values of $F$. Formula (U4) allows ranks with unused budget; not every | |
| integer is necessarily a possible rank of a parallel subbundle. | |
| \end{theorem} | |
| \begin{proof} | |
| An orthogonal projector determines a parallel subbundle precisely when | |
| its value $P$ at $o$ commutes with the holonomy group, equivalently with | |
| $H$. The associated global projector is | |
| $P_x=T_x^{-1}PT_x$, independent of the path choices. Therefore | |
| \[ | |
| \|(I-P_W)F\|_{L^2}^2 | |
| =\operatorname{tr}((I-P)C) | |
| =\operatorname{tr}((I-P)\widehat C). \tag{U6} | |
| \] | |
| The last equality uses $h^*Ph=P$ and cyclicity of trace. | |
| Compact-group averaging annihilates off-diagonal blocks between | |
| inequivalent irreducibles. On an isotypic block it is scalar on the | |
| irreducible factor by Schur's lemma. Taking the partial trace identifies | |
| that scalar factor and gives (U3). Every orthogonal projector in the | |
| commutant has the form | |
| \[ | |
| P=\bigoplus_\lambda(P_\lambda\otimes I_{E_\lambda}), | |
| \] | |
| where $P_\lambda$ is an arbitrary orthogonal projector on the multiplicity | |
| space. If its rank is $k_\lambda$, then the full rank contribution is | |
| $d_\lambda k_\lambda$, while the captured energy is | |
| $\operatorname{tr}(P_\lambda C_\lambda)$. | |
| For a positive matrix with eigenvalues $\alpha_1\ge\cdots\ge\alpha_m$, | |
| the maximum of $\operatorname{tr}(PC)$ over rank-$k$ orthogonal | |
| projectors is $\sum_{j\le k}\alpha_j$. Indeed in an eigenbasis the | |
| diagonal entries $p_j$ of $P$ lie in $[0,1]$ and sum to $k$, so that | |
| $\sum\alpha_jp_j\le\sum_{j\le k}\alpha_j$; the spectral projector | |
| attains equality. This is the classical Ky Fan variational principle. | |
| Optimizing the integer ranks gives (U4). | |
| Zero error means retaining every positive eigenvalue in every reduced | |
| block. Thus (U5) follows. Alternatively, the range of $\widehat C$ is | |
| invariant, and every vector orthogonal to it has zero integrated squared | |
| pairing with the transported curvature and all its holonomy transforms. | |
| Continuity of $F$ promotes almost-everywhere vanishing to pointwise | |
| vanishing. Its range is therefore exactly the required holonomy-saturated | |
| coefficient subspace. | |
| \end{proof} | |
| \paragraph{Finite optimization and why a greedy rule is insufficient.} | |
| Given the isotypic decomposition and the reduced spectra, put | |
| $A_\lambda(k)=\sum_{j\le k}\alpha_{\lambda,j}$. A budget dynamic | |
| program, one isotypic block at a time, uses the recurrence | |
| \[ | |
| D_\lambda(r)= | |
| \max_{0\le k\le\min(m_\lambda,\lfloor r/d_\lambda\rfloor)} | |
| \{D_{\lambda-1}(r-d_\lambda k)+A_\lambda(k)\}. | |
| \tag{U7} | |
| \] | |
| With $D_0(r)=0$, the maximum in (U4) is the final $D_\lambda(r)$. | |
| At fixed spectra this requires at most $O(n^2)$ arithmetic comparisons | |
| over all budgets $0,\ldots,n$. Computing an isotypic decomposition or | |
| exact spectra from arbitrary input is a separate problem. | |
| An elementary example has two inequivalent irreducibles, each of | |
| multiplicity one, with $(d_1,\alpha_{1,1})=(2,3)$ and | |
| $(d_2,\alpha_{2,1})=(3,4)$. For budget three the optimum captures four | |
| units of energy by choosing the second block. A rule that first chooses | |
| the greater energy per dimension instead takes the first block and | |
| captures only three. Such irreducibles occur, for example, in the direct | |
| sum of the defining two-dimensional representation of $SU(2)$ and the | |
| defining three-dimensional representation of $SO(3)$, as a representation | |
| of their product. A flat holonomy group can have this product as its | |
| compact closure. | |
| \begin{corollary}[An arbitrarily large all-or-nothing barrier in dimension five] | |
| For every $d\ge2$, there is a closed connected oriented five-manifold, | |
| a rank-$d$ flat unitary coefficient bundle, and a smooth exact curvature | |
| $F=d_\nabla B\ne0$ whose values lie in one local parallel line wherever | |
| they are nonzero, such that | |
| \[ | |
| \mathcal E_r(F)=\|F\|_{L^2}^2\quad(0\le r<d), | |
| \qquad \mathcal E_d(F)=0. \tag{U8} | |
| \] | |
| For suitable measurable path choices, the untwirled Gramian $C$ has rank | |
| one. Its ordinary unconstrained rank-one approximation has zero error, | |
| while every compatible parallel model of rank less than $d$ retains the | |
| entire curvature error. | |
| \end{corollary} | |
| \begin{proof} | |
| Take $M=(S^1\times S^4)\mathbin{\#}(S^1\times S^4)$, so | |
| $\pi_1(M)$ is the free group on two generators. On $\mathbb C^d$, let $X$ be the cyclic permutation of the standard | |
| basis, and let $Y$ act on the first two coordinates by | |
| \[ | |
| \begin{pmatrix}0&-1\\1&0\end{pmatrix} | |
| \] | |
| and as the identity on all other coordinates. These integer orthogonal | |
| matrices define a flat Hermitian bundle. Their common representation is | |
| irreducible over $\mathbb C$. For $d\ge3$, the conjugates | |
| $X^jY^2X^{-j}$ negate the two coordinates of every cyclic adjacent pair. | |
| Those sign patterns distinguish every pair of coordinates, so a matrix | |
| commuting with all of them is diagonal. Commuting also with $X$ forces | |
| that diagonal matrix to be scalar. For $d=2$, the direct equations for | |
| commuting with $X$ and $Y$ have the same scalar solution. Every invariant | |
| subspace is reducing because the generators are unitary; its orthogonal | |
| projector therefore belongs to this scalar commutant and is zero or the | |
| identity. | |
| Choose a coordinate ball with a flat frame, a nonzero constant coefficient | |
| vector $v$, and a smooth compactly supported scalar function $\phi$ with | |
| $\partial_5\phi\not\equiv0$. In that ball set | |
| \[ | |
| B=\phi(x)v\,dx^1\wedge dx^2\wedge dx^3\wedge dx^4, | |
| \] | |
| and extend by zero. This is a global smooth four-form. Its curvature is | |
| $F=(\partial_5\phi)v\,dx^1\wedge\cdots\wedge dx^5$, since | |
| moving $dx^5$ past four factors has positive sign. It is nonzero and | |
| locally line-valued. Choose the paths on this ball through the fixed | |
| flat frame. All nonzero transported coefficients are multiples of the | |
| same vector, and hence $C$ has rank one. | |
| Irreducibility implies that the only parallel subbundles are $0$ and the | |
| whole coefficient bundle. This proves (U8) directly. Equivalently, | |
| $\widehat C=(\operatorname{tr}C/d)I_d$ has full rank, but there is no | |
| nontrivial projector in the commutant. | |
| \end{proof} | |
| \paragraph{Quantitative stability at fixed rank.} | |
| For two seed Gramians $C,C'$, their optimal retained energies at budget | |
| $r$ differ by at most $\|\widehat C-\widehat C'\|_*$, since every | |
| admissible projector has operator norm at most one. Combining this with | |
| the trace difference gives | |
| \[ | |
| |\mathcal E_r(C)-\mathcal E_r(C')| | |
| \le 2\|\widehat C-\widehat C'\|_*. | |
| \] | |
| One may instead obtain the sharper direct bound | |
| $|\mathcal E_r(C)-\mathcal E_r(C')| | |
| \le\|\widehat C-\widehat C'\|_*$ by expressing the error as the | |
| minimum of $\operatorname{tr}((I-P)\widehat C)$ and using | |
| $\|I-P\|_{\mathrm{op}}\le1$. Thus the full error curve is Lipschitz | |
| in trace norm even when the exact zero-error rank is discontinuous. | |
| The group average is trace-norm contractive on Hermitian matrices, so | |
| the same bound holds with $\|C-C'\|_*$ for fixed holonomy representation. | |
| \begin{proposition}[Stability under perturbing the holonomy generators] | |
| Let $U_1,\ldots,U_m\in U(n)$ act irreducibly, and let | |
| \[ | |
| \mathcal L(S)=([S,U_1],\ldots,[S,U_m]) | |
| \] | |
| on the traceless matrix space, with Hilbert--Schmidt norms. Set | |
| $s=\sigma_{\min}(\mathcal L)>0$. If unitary matrices $U_i'$ satisfy | |
| $\max_i\|U_i'-U_i\|_{\mathrm{op}}\le\epsilon$, then | |
| \[ | |
| \sigma_{\min}(\mathcal L')\ge s-2\sqrt m\,\epsilon. | |
| \] | |
| In particular irreducibility, and hence the all-or-nothing barrier, | |
| persists for $\epsilon<s/(2\sqrt m)$. | |
| If the $U_i$ are integer orthogonal matrices, the entirely explicit | |
| sufficient condition | |
| \[ | |
| \epsilon<(4m)^{-(n^2-1)/2} | |
| \] | |
| also guarantees persistence. This bound is deliberately conservative. | |
| \end{proposition} | |
| \begin{proof} | |
| Schur's lemma makes the kernel of the commutator map consist precisely of | |
| scalar matrices, so its restriction to the traceless subspace is | |
| injective. Moreover | |
| $\|[S,U_i'-U_i]\|_{\mathrm{HS}} | |
| \le2\epsilon\|S\|_{\mathrm{HS}}$. | |
| Combining the $m$ inequalities and applying the reverse triangle | |
| inequality gives the stated singular-value bound. A nontrivial invariant | |
| subspace of the perturbed unitary family would give a nonzero traceless | |
| commuting projector, so injectivity implies irreducibility. | |
| For the explicit estimate, the full positive operator | |
| $T=\mathcal L^*\mathcal L$ has an integer matrix in the matrix-unit basis, | |
| one zero eigenvalue, and $n^2-1$ positive eigenvalues. Each eigenvalue is | |
| at most $4m$. The product of the nonzero eigenvalues is the absolute | |
| value of the linear coefficient of its integer characteristic polynomial, | |
| and hence is at least one. Its least positive eigenvalue is therefore | |
| at least $(4m)^{-(n^2-2)}$. Taking a square root and dividing by | |
| $2\sqrt m=\sqrt{4m}$ gives the displayed sufficient radius. | |
| \end{proof} | |
| \begin{corollary}[Arbitrarily weak unitary holonomy still forces full rank] | |
| For every $d\ge2$ and every $\eta>0$, the all-or-nothing example in | |
| (U8) can be chosen with both specified holonomy generators at operator-norm | |
| distance less than $\eta$ from the identity. More precisely, let | |
| \[ | |
| A=\operatorname{diag}(1,\ldots,d),\qquad J=(1)_{i,j=1}^d, | |
| \] | |
| and for $0<|\tau|<2\pi/d$ set | |
| \[ | |
| U_1(\tau)=e^{i\tau A},\qquad | |
| U_2(\tau)=e^{i\tau J} | |
| =I+\frac{e^{i d\tau}-1}{d}J. \tag{U9} | |
| \] | |
| The resulting representation of the free group on two generators is | |
| irreducible, while | |
| \[ | |
| \|U_j(\tau)-I\|_{\mathrm{op}}\le d|\tau|\quad(j=1,2). | |
| \] | |
| On the fixed closed five-manifold | |
| $(S^1\times S^4)\mathbin{\#}(S^1\times S^4)$, choose the same nonzero, | |
| locally supported exact curvature in a common flat coordinate frame for | |
| each parameter. Every nonzero $\tau$ in (U9) then requires auxiliary | |
| rank $d$ even to reduce its curvature error. At $\tau=0$, the trivial | |
| holonomy representation admits zero error with auxiliary rank one. | |
| Thus the exact rank--error frontier is discontinuous at trivial holonomy, | |
| even though the generators converge to the identity and the local | |
| curvature data are fixed. | |
| \end{corollary} | |
| \begin{proof} | |
| The diagonal entries of $U_1(\tau)$ are distinct under the displayed | |
| parameter restriction. A commuting orthogonal projector is therefore | |
| diagonal. Every off-diagonal entry of $U_2(\tau)$ is the same nonzero | |
| number, so commuting with $U_2(\tau)$ forces all diagonal entries of | |
| that projector to agree. Hence it is zero or the identity, proving | |
| irreducibility. The exponential bounds follow from | |
| $|e^{it}-1|\le|t|$ and $\|A\|_{\mathrm{op}}=\|J\|_{\mathrm{op}}=d$. | |
| Taking $0<|\tau|<\min(2\pi/d,\eta/d)$ gives the first claim. | |
| Use the compactly supported four-form from the previous corollary in a | |
| fixed flat chart. Its curvature values occupy the same coefficient line | |
| for every parameter and have the same $L^2$ norm. The irreducibility | |
| argument gives (U8) at each nonzero parameter. At zero, every fixed | |
| coefficient subspace is parallel, and the one coefficient line suffices. | |
| This is a statement about this explicit family of representations and | |
| locally fixed data; no unmentioned global identification of different | |
| flat connections is required. | |
| \end{proof} | |
| \paragraph{A perturbation radius proportional to holonomy strength.} | |
| Define on traceless matrices | |
| \[ | |
| \mathcal L_0(S)=([S,A],[S,J]),\qquad | |
| s_0=\sigma_{\min}(\mathcal L_0)>0. | |
| \] | |
| The positivity follows by the same diagonal-then-all-entries commutant | |
| argument. The exponential remainder estimate gives | |
| \[ | |
| \|\mathcal L_\tau-i\tau\mathcal L_0\| | |
| \le\sqrt2\,d^2\tau^2. | |
| \] | |
| Consequently, when | |
| $0<|\tau|\le s_0/(2\sqrt2\,d^2)$, | |
| \[ | |
| \sigma_{\min}(\mathcal L_\tau)\ge\tfrac12s_0|\tau|. | |
| \] | |
| By the preceding perturbation proposition, arbitrary unitary changes of | |
| the two generators by less than | |
| $s_0|\tau|/(4\sqrt2)$ preserve irreducibility and the all-or-nothing | |
| barrier. The robust radius therefore has a positive linear lower bound | |
| in the nonzero holonomy parameter, although that radius necessarily | |
| shrinks toward the singular trivial-holonomy limit. | |
| \paragraph{Established ingredients and scope.} | |
| Compact-group averaging, Schur's lemma, and the spectral variational | |
| principle are established tools. A primary reference for the latter is | |
| K.~Fan, \emph{On a Theorem of Weyl Concerning Eigenvalues of Linear | |
| Transformations I}, Proc.~Natl.~Acad.~Sci.~USA \textbf{35}(11) (1949), | |
| 652--655, \url{https://doi.org/10.1073/pnas.35.11.652}. | |
| The result here is their explicit application to globally compatible | |
| central defect cancellation, including its exact budget frontier and | |
| the fixed-dimension all-or-nothing obstruction. It does not solve a | |
| general noncentral completion problem, and it does not treat a | |
| nonunitary local system as though it had a parallel Hermitian metric. | |