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Graph views, holonomy, and reconstruction

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Part IV The geometry of exact realization

A categorical space of realizations does not come with a numerical distance by default. In a declared linear model, the compatibility equations become a bounded operator. Closed range, holonomy, and conditioning then determine what small residuals actually guarantee.

17 Graph views, holonomy, and reconstruction

17.1 Actual transports on a finite graph

Let a finite connected simple graph have vertex set \(V\), root \(o\), and a chosen route \(p_i:o\to i\) for every vertex, with the route at \(o\) empty. Use a common real normed fiber \(H\). An inverse consistent connection assigns continuous linear equivalences \(\tau_{ij}\), with \(\tau_{ji}=\tau_{ij}^{-1}\). Our convention is that \(\tau_{ij}\) carries the value at \(j\) into the coordinates at \(i\).

The candidate and residual spaces are finite products with maximum norms:

\[ E=\prod_{i\in V}H,\qquad R=\prod_{(i,j)\in\vec E}H,\qquad (dx)_{ij}=\tau_{ij}x_j-x_i. \]

Both orientations of an edge are retained. If \(M\) bounds the norms of all measured edge maps, then \({\left\lVert d\right\rVert}\le M+1\). The empty edge case has the usual zero residual.

Distinct walks are retained as arrows of the view category. The product along a walk \(q=(i_0,\ldots,i_m)\) is

\[ T_q=\tau_{i_0i_1}\cdots\tau_{i_{m-1}i_m}. \]

Concatenation gives the restriction composition law. An exact vertex family defines a coherent walk-view section, and a coherent walk-view section satisfies every edge equation. Thus this graph construction returns to the original ambient realization type rather than creating a disconnected numerical model.

17.2 Transported residuals and path gains

Proposition 17.1: The path telescope

For a walk \(q=(i_0,\ldots,i_m)\),

\[ T_qx_{i_m}-x_{i_0} =\sum_{k=0}^{m-1} (\tau_{i_0i_1}\cdots\tau_{i_{k-1}i_k})(dx)_{i_ki_{k+1}}. \]

The empty prefix is the identity. If \(\gamma(q)\) is the sum of the products of preceding edge norms, then

\[ {\left\lVert T_qx_{i_m}-x_{i_0}\right\rVert}\le\gamma(q){\left\lVert dx\right\rVert}_\infty. \]

Proof

Write \(U_0=I\) and \(U_k=\tau_{i_0i_1}\cdots\tau_{i_{k-1}i_k}\) for \(1\le k\le m\). The transport convention makes every \(U_k\) a map from the fiber at \(i_k\) to that at \(i_0\). Since \(U_{k+1}=U_k\tau_{i_ki_{k+1}}\), the \(k\)-th transported defect is

\[ U_k(dx)_{i_ki_{k+1}} =U_{k+1}x_{i_{k+1}}-U_kx_{i_k}. \]

Summing over \(k=0,\ldots,m-1\) cancels each interior value once with each sign. The remaining terms are \(U_mx_{i_m}-U_0x_{i_0}=T_qx_{i_m}-x_{i_0}\), proving the identity with its actual ordered products. For an empty walk both sides are zero.

The triangle inequality and the operator norm bound now give

\[ {\left\lVert T_qx_{i_m}-x_{i_0}\right\rVert} \le\sum_{k=0}^{m-1}{\left\lVert U_k\right\rVert}{\left\lVert(dx)_{i_ki_{k+1}}\right\rVert} \le\left(\sum_{k=0}^{m-1}\prod_{j=0}^{k-1}{\left\lVert\tau_{i_ji_{j+1}}\right\rVert}\right){\left\lVert dx\right\rVert}_\infty. \]

The bracket is \(\gamma(q)\), with the empty product equal to one. Repeated vertices or edges do not affect the cancellation. Reordering the edge maps would, in general, invalidate it.

For isometric maps, \(\gamma(q)\le|q|\). For arbitrary bounded equivalences, route length cannot replace the amplification gain. Reversing a route can have a different gain, even though its transport is the inverse map.

17.3 Holonomy is the remaining exactness condition

Write \(T_i=T_{p_i}\). Reconstruction from a proposed root value is

\[ (R_pz)_i=T_i^{-1}z. \]

For each directed edge define the root loop operator

\[ K_{ij}=T_i\tau_{ij}T_j^{-1},\qquad K=\bigcap_{(i,j)\in\vec E}\ker(K_{ij}-I). \]

Each \(K_{ij}\) is the transport around an actual rooted loop. No flatness assumption has been made.

Theorem 17.2: Holonomy classification

Evaluation at the root and reconstruction give an equivalence

\[ K\simeq_L\ker d. \]

A root value extends to an exact vertex family precisely when it lies in \(K\), and that extension is unique. The space \(K\) is independent of the chosen routes. Reconstruction is route independent on \(K\).

Proof

Every \(T_i\) is a continuous linear equivalence, being a finite ordered composition of such maps. Reconstruction is therefore well defined. For an edge \((i,j)\), apply \(T_i\) to its defect:

\[ T_i\bigl(\tau_{ij}T_j^{-1}z-T_i^{-1}z\bigr) =T_i\tau_{ij}T_j^{-1}z-z=K_{ij}z-z. \]

Because \(T_i\) is injective, that edge defect is zero if and only if the corresponding root loop fixes \(z\). Thus \(dR_pz=0\) holds exactly for \(z\in K\). The root route is empty, so \((R_pz)_o=z\).

Conversely, let \(x\in\ker d\). The path telescope along \(p_i\) has all zero summands, hence \(T_ix_i=x_o\) for every vertex. Applying \(T_i^{-1}\) gives \(x_i=T_i^{-1}x_o\), so \(x=R_p(x_o)\). The first part then places \(x_o\) in \(K\). We have proved both inverse equations and uniqueness of an exact extension of a root value.

The maps are linear. On the finite vertex product,

\[ {\left\lVert R_pz\right\rVert}_\infty\le\left(\max_i{\left\lVert T_i^{-1}\right\rVert}\right){\left\lVert z\right\rVert}, \qquad {\left\lVert x_o\right\rVert}\le{\left\lVert x\right\rVert}_\infty. \]

These bounds also hold on the subspaces \(K\) and \(\ker d\), proving continuity of both directions. No completeness is needed for these finite bounds.

For route independence, the proved equivalence identifies \(K\) with the image of root evaluation from the intrinsically defined space \(\ker d\). That image does not refer to any chosen routes, so every route system yields the same \(K\). For \(z\in K\), reconstruction using either system is an exact family with root \(z\), and uniqueness makes the families equal. For \(z\notin K\), this uniqueness argument does not assert equality of the two generally inconsistent reconstructed families.

With isometric transports the equivalence is an isometry for the vertex maximum norm, because every reconstructed coordinate has the root norm. With general bounded equivalences, it need not be an isometry.

Tree routes reconstruct from an anchor. The remaining edges close loops and impose fixed-vector equations at that anchor. A nontrivial loop can obstruct an arbitrary seed without preventing every nonzero seed from extending. The fixed space, rather than the identity of the whole loop operator, is the relevant realization condition.
Figure 14. Tree routes reconstruct from an anchor. The remaining edges close loops and impose fixed-vector equations at that anchor. A nontrivial loop can obstruct an arbitrary seed without preventing every nonzero seed from extending. The fixed space, rather than the identity of the whole loop operator, is the relevant realization condition.

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17.4 Prescribed observations remain visible

If a prescribed vertex set \(U\) contains \(o\), a candidate \(x\) has an exact repair preserving \(x|_U\) precisely when

\[ x_o\in K\quad\text{and}\quad (R_px_o)|_U=x|_U. \]

Necessity follows from the classification. Sufficiency is the reconstructed family itself. The source identifies this criterion with the earlier obstruction class in \(R/d(\ker p_U)\). A graph seed test is therefore an instance of the same protected correction problem, not a replacement for it.

18 Closed range is the stability boundary

18.1 Projection exists before a residual estimate

Let \(E\) be a real Hilbert space and \(R\) a real Banach space. Let \(D:E\to R\) be continuous linear. The kernel \(K=\ker D\) is closed, so its orthogonal projection \(q=P_K\) exists [4].

Proposition 18.1: Exact orthogonal repair

For every \(x\in E\),

\[ D(qx)=0,\quad q^2=q,\quad{\left\lVert qx\right\rVert}\le{\left\lVert x\right\rVert}, \]

and \(qx\) is the unique closest point to \(x\) in \(K\).

Proof

Boundedness of \(D\) makes \(K=\ker D\) closed. Lemma E.1 constructs \(q=P_K\) and gives the orthogonal decomposition \(x=qx+(x-qx)\). The first term belongs to \(K\), so \(Dqx=0\). Projection fixes every point of \(K\), giving \(q(qx)=qx\).

Pythagoras applied to that decomposition gives \({\left\lVert x\right\rVert}^2={\left\lVert qx\right\rVert}^2+{\left\lVert x-qx\right\rVert}^2\), hence \({\left\lVert qx\right\rVert}\le{\left\lVert x\right\rVert}\). For any \(y\in K\), the vector \(qx-y\) lies in \(K\), whereas \(x-qx\) lies in its orthogonal complement. Consequently

\[ {\left\lVert x-y\right\rVert}^2={\left\lVert x-qx\right\rVert}^2+{\left\lVert qx-y\right\rVert}^2\ge{\left\lVert x-qx\right\rVert}^2. \]

Equality holds only when \({\left\lVert qx-y\right\rVert}=0\), or \(y=qx\). This proves nearest-point uniqueness without any closedness assumption on \({\operatorname{ran}} D\). Closedness of the kernel and of the range serve different purposes.

No closed range assumption on \(D\) is needed for this projection. Such an assumption enters when the size of the residual is asked to control the distance to the exact space.

Theorem 18.2: Closed range and quantitative exactness

The following are equivalent:

  1. \({\operatorname{ran}} D\) is closed.

  2. There is \(C\ge0\) with \({\left\lVert x-qx\right\rVert}\le C{\left\lVert Dx\right\rVert}\) for all \(x\).

  3. There is \(C\ge0\) such that every \(x\) has some exact \(y\) with \({\left\lVert x-y\right\rVert}\le C{\left\lVert Dx\right\rVert}\).

When the range is closed, the least admissible constant is the operator norm of the inverse of \(D:K^\perp\to{\operatorname{ran}} D\). In the zero operator case that inverse has zero dimensional domain and its norm is zero.

Proof

Let \(K=\ker D\) and \(K^\perp\) carry the induced Hilbert norm. Define \(D_\perp u=Du\), but regard its target as \({\operatorname{ran}} D\) with the norm inherited from \(R\). It is injective: \(Du=0\) puts \(u\) in both \(K\) and \(K^\perp\), so \(u=0\). It is surjective onto that target: if \(r=Dx\), then \(u=x-qx\in K^\perp\) and \(Du=Dx=r\). Thus it is a bounded linear bijection before any continuity of its inverse is claimed.

Suppose first that the range is closed. Because \(R\) is Banach, \({\operatorname{ran}} D\) is then Banach. The domain \(K^\perp\) is also complete. The bounded inverse theorem, proved in Appendix E, gives a bounded inverse \(A=D_\perp^{-1}\). Applying it to \(Dx=D(x-qx)\) yields

\[ x-qx=A(Dx),\qquad {\left\lVert x-qx\right\rVert}\le{\left\lVert A\right\rVert}{\left\lVert Dx\right\rVert}. \]

Hence condition 2 holds. If any \(C\ge0\) satisfies condition 2, then for every \(r\in{\operatorname{ran}} D\) apply it to \(u=Ar\in K^\perp\). Since \(qu=0\), it gives \({\left\lVert Ar\right\rVert}\le C{\left\lVert r\right\rVert}\). Taking the operator norm proves \({\left\lVert A\right\rVert}\le C\). This establishes the least constant, not just a sufficient one. If \(D=0\), both \(K^\perp\) and the range are zero spaces and \({\left\lVert A\right\rVert}=0\).

Now assume condition 2. To prove closedness, take an arbitrary sequence \(r_n\in{\operatorname{ran}} D\) with \(r_n\to r\) in \(R\). Choose \(x_n\) with \(Dx_n=r_n\) and put \(u_n=x_n-qx_n\). Then \(u_n\in K^\perp\) and \(Du_n=r_n\). Applying the estimate to \(u_n-u_m\) gives

\[ {\left\lVert u_n-u_m\right\rVert}\le C{\left\lVert r_n-r_m\right\rVert}. \]

Thus \((u_n)\) is Cauchy in the complete space \(K^\perp\). Let its limit be \(u\). Continuity gives \(Du=\lim_n r_n=r\), so \(r\in{\operatorname{ran}} D\). In a normed space, a set containing the limits of all its convergent sequences is closed. This proves condition 1 without presupposing that the initially unbounded inverse is continuous.

Condition 2 implies condition 3 by choosing \(y=qx\). Conversely, if condition 3 supplies an exact \(y\) for a given \(x\), the nearest-point property of \(qx\) gives

\[ {\left\lVert x-qx\right\rVert}\le{\left\lVert x-y\right\rVert}\le C{\left\lVert Dx\right\rVert}. \]

The same \(C\) works for all \(x\), proving condition 2. This last implication does not require the selected answers \(y\) to depend linearly or continuously on \(x\).

The last equivalence is important. A nonlinear choice of exact answers cannot bypass the failure of a uniform residual bound. Failure of closed range is not merely a defect of one selected projection algorithm.

18.2 A small residual far from exactness

On \(\ell^2({\mathbb N})\), index the standard basis from one and define \(De_n=n^{-1}e_n\). The map is bounded and injective, so its exact space is zero. Yet

\[ {\left\lVert e_n\right\rVert}=1,\qquad{\left\lVert De_n\right\rVert}=1/n\longrightarrow0. \]

No finite \(C\) can bound \({\operatorname{dist}}(e_n,\ker D)\) by \(C{\left\lVert De_n\right\rVert}\). The range is not closed. For example finite truncations of \((1/n)_{n\ge1}\) belong to the range and converge in \(\ell^2\), but a preimage of the limit would be the constant sequence, which does not belong to \(\ell^2\).

This diagonal model is formalized on the infinite Hilbert space used in Section 30. In the namespace KomorebiSpace.DiagonalRegularization, T_not_closed_range applies the general obstruction theorem to actual unit coordinate vectors. The declaration w_mem_closure_not_range proves that the displayed limiting datum belongs to the closure of the range but not to the range itself. Formal coordinate \(j\) represents the printed coordinate \(n=j+1\).

Residual size controls distance to the exact space only when transverse directions have a positive lower bound. The diagonal example sends unit vectors to residuals tending to zero, so no uniform inverse gain exists. Exact projection still exists.
Figure 15. Residual size controls distance to the exact space only when transverse directions have a positive lower bound. The diagonal example sends unit vectors to residuals tending to zero, so no uniform inverse gain exists. Exact projection still exists.

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18.3 Norm zero versus algebraic zero

If an additive correction image is not closed, distance to that image can vanish without actual membership. Thus an infimum of residual error can be zero while the exact protected correction is unattained. The algebraic obstruction quotient and its possible seminorm answer different questions. One must identify a closed image, compactness condition, or other attainment principle before replacing one question by the other.

18.4 Stable repair with protected data

The preceding orthogonal projection does not generally preserve a separately declared observable. To join the analytic theory to Section 4, let \(p:E\to S\) be continuous linear into a normed space. Define

\[ M=\ker p,\qquad B=D|_M:M\to R,\qquad H=M\cap\ker D. \]

The closed subspace \(M\) inherits its Hilbert structure from \(E\). A candidate \(x\) is feasible for protected repair when an exact \(y\) with \(p(y)=p(x)\) exists. The algebraic criterion is still \(Dx\in{\operatorname{ran}} B\).

Theorem 18.3: Nearest feasible protected repair

Every feasible \(x\) has a unique closest exact answer \(y_*\) preserving \(p(x)\). Its correction \(h_*=x-y_*\) is the unique vector in the orthogonal complement of \(\ker B\) inside \(M\) satisfying \(Bh_*=Dx\). For every other feasible answer \(y\),

\[ {\left\lVert x-y\right\rVert}^2={\left\lVert x-y_*\right\rVert}^2+{\left\lVert y_*-y\right\rVert}^2. \]

Moreover, the following conditions are equivalent:

\[ {\operatorname{ran}} B\text{ is closed} \quad\Longleftrightarrow\quad \exists C\ge0\ \forall\text{ feasible }x: {\left\lVert x-y_*\right\rVert}\le C{\left\lVert Dx\right\rVert}. \]

When these conditions hold, the least nonnegative constant is the transverse inverse norm of \(B\), including the zero-range case.

Proof

Feasibility gives some \(h_0=x-y_0\in M\) with \(Bh_0=Dx\). Conversely, every \(h\in M\) satisfying \(Bh=Dx\) produces an exact protected answer \(y=x-h\). Thus the answer problem and the correction problem are equivalent, with correction set

\[ \{h\in M:Bh=Dx\}=h_0+\ker B. \]

This is a nonempty closed affine subset of the Hilbert space \(M\). Closedness of \(\ker B\) follows from continuity of \(B\), independently of whether its image is closed.

Let \(k_0=P^M_{\ker B}h_0\) and \(h_*=h_0-k_0\). Then \(Bh_*=Bh_0=Dx\) and \(h_*\perp\ker B\) in \(M\). If a different initial correction is chosen, it differs from \(h_0\) by an element of \(\ker B\). Its orthogonal-complement component is therefore again \(h_*\). This proves that the construction is independent of the feasibility witness.

Every other correction can be written uniquely as \(h_*+k\) with \(k\in\ker B\). Orthogonality gives

\[ {\left\lVert h_*+k\right\rVert}^2={\left\lVert h_*\right\rVert}^2+{\left\lVert k\right\rVert}^2. \]

Writing \(y_*=x-h_*\) and \(y=x-h_*-k\), we have \(x-y=h_*+k\) and \(y_*-y=k\). Substitution proves the stated Pythagorean identity. Its last term vanishes only when \(y=y_*\), establishing the unique closest answer.

If \({\operatorname{ran}} B\) is closed, Theorem 18.2 applied on \(M\) gives a bounded inverse of \(B\) on \((\ker B)^{\perp_M}\). The vector \(h_*\) is exactly that inverse applied to \(Dx\), so its norm obeys the required bound.

For the converse, suppose the bound holds for every feasible raw candidate. Every \(x\in M\) is feasible, because \(y=0\) has \(Dy=0\) and \(py=px=0\). Its closest protected exact answer is \(P^M_{\ker B}x\). Thus the assumed estimate reduces on \(M\) to

\[ {\left\lVert x-P^M_{\ker B}x\right\rVert}\le C{\left\lVert Bx\right\rVert}\qquad(x\in M). \]

Theorem 18.2 forces \({\operatorname{ran}} B\) to be closed. The same restriction also proves that no smaller nonnegative constant than the transverse inverse norm can work. If the range is zero, feasible candidates are already exact under permitted correction and the least correction is zero, so the optimal gain is zero.

The relevant stability boundary is therefore \(D(\ker p)\), not automatically \(D(E)\). Restricting permitted changes can turn a well-conditioned unconstrained problem into an obstructed or poorly conditioned protected one. The nearest protected answer is generally not \(P_{\ker D}x\).

For \(D(x_1,x_2,x_3)=x_1-x_2\), \(p(x)=(x_1,x_3)\), and \(x=(2,0,5)\), the ordinary orthogonal answer is \((1,1,5)\). The protected answer is \((2,2,5)\). The respective squared errors are two and four. Both have zero residual, but only the latter preserves the declared data. The theorem is formalized in ProtectedHilbertRepair.lean, using the actual operator on \(\ker p\). The displayed three-coordinate values are an illustrative calculation, not a separate universal algorithm.

The same compatibility equation permits different repair problems. Orthogonal repair chooses the nearest point on the diagonal. Preserving the first coordinate forces a vertical correction to a different point. The third coordinate is fixed at five throughout.
Figure 16. The same compatibility equation permits different repair problems. Orthogonal repair chooses the nearest point on the diagonal. Preserving the first coordinate forces a vertical correction to a different point. The third coordinate is fixed at five throughout.

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19 Holonomy repair and transport amplification

19.1 An orthogonal anchor, not a global least squares answer

Return to the graph model with a real Hilbert fiber. The root residual is

\[ \mathcal H z=(K_{ij}z-z)_{ij},\qquad K=\ker\mathcal H. \]

Let \(q=P_K\), and define

\[ Px=R_p(qx_o). \]

This is always exact, fixes exact families, and is idempotent. It is the unique exact family preserving the feasible component \(qx_o\) of the anchor. Its orthogonality is on the anchor fiber. The vertex and edge norms are still maximum norms.

For example on a two-vertex identity connection, \((0,2)\) with root value zero is repaired to \((0,0)\). The constant family \((1,1)\) is closer in the maximum norm, but it does not preserve the anchor. The operator \(P\) is not being claimed to be a global nearest-point projection in that norm.

19.2 Every factor in the bound has a meaning

Define the route gain

\[ A_p=\max_i\gamma(\overline{p_i}), \]

using reverse routes so that the error is measured in each destination view. The path telescope gives

\[ {\left\lVert x-R_p(x_o)\right\rVert}_\infty\le A_p{\left\lVert dx\right\rVert}_\infty. \]

Let \(N_p\) be the residual normalization \((N_pr)_{ij}=T_ir_{ij}\). The exact identity \(\mathcal H=N_pdR_p\) implies

\[ {\left\lVert\mathcal H(x_o)\right\rVert}_\infty \le{\left\lVert N_p\right\rVert}({\left\lVert d\right\rVert} A_p+1){\left\lVert dx\right\rVert}_\infty. \]

Theorem 19.1: Amplified holonomy repair

If \({\operatorname{ran}}\mathcal H\) is closed and \(\kappa\) is its transverse inverse gain, then

\[ {\left\lVert x-Px\right\rVert}_\infty\le \left[A_p+{\left\lVert R_p\right\rVert}\kappa{\left\lVert N_p\right\rVert}({\left\lVert d\right\rVert} A_p+1)\right] {\left\lVert dx\right\rVert}_\infty. \]
(19.1)

The range condition is necessary for the existence of any uniform bound of distance to an exact family by \({\left\lVert dx\right\rVert}_\infty\). It is automatic for a fixed finite dimensional fiber, but not uniformly quantitative across all connections.

Proof

First quantify the residual seen at the root. The identity \(\mathcal H=N_pdR_p\), applied to \(x_o\), gives

\[ \begin{aligned} {\left\lVert\mathcal H(x_o)\right\rVert}_\infty &={\left\lVert N_p\bigl(d(R_px_o-x)+dx\bigr)\right\rVert}_\infty\\ &\le{\left\lVert N_p\right\rVert}\bigl({\left\lVert d\right\rVert}{\left\lVert R_px_o-x\right\rVert}_\infty+{\left\lVert dx\right\rVert}_\infty\bigr)\\ &\le{\left\lVert N_p\right\rVert}({\left\lVert d\right\rVert} A_p+1){\left\lVert dx\right\rVert}_\infty. \end{aligned} \]

Closed range of \(\mathcal H\) lets Theorem 18.2 control the anchor correction by \({\left\lVert x_o-qx_o\right\rVert}\le\kappa{\left\lVert\mathcal H(x_o)\right\rVert}_\infty\). Insert the uncorrected reconstruction between \(x\) and \(Px=R_pqx_o\):

\[ {\left\lVert x-Px\right\rVert}_\infty \le{\left\lVert x-R_px_o\right\rVert}_\infty+{\left\lVert R_p\right\rVert}{\left\lVert x_o-qx_o\right\rVert}. \]

Substituting the two preceding bounds yields (19.1). The finite maximum-norm residual product is a Banach space because its fiber is Hilbert, so the target completeness needed in Theorem 18.2 is available.

For necessity, suppose a constant \(C\) satisfies \({\operatorname{dist}}(w,\ker d)\le C{\left\lVert dw\right\rVert}_\infty\) for every vertex family \(w\). Fix \(z\in K^\perp\) and take \(w=R_pz\). Every exact family \(e\) has \(e_o\in K\), and root evaluation has norm at most one. Therefore

\[ {\left\lVert z\right\rVert}={\operatorname{dist}}(z,K)\le{\left\lVert z-e_o\right\rVert}\le{\left\lVert R_pz-e\right\rVert}_\infty. \]

Taking the infimum over \(e\in\ker d\) is legitimate without assuming that this global nearest point is attained. It gives

\[ {\left\lVert z\right\rVert}\le C{\left\lVert dR_pz\right\rVert}_\infty \le C{\left\lVert N_p^{-1}\right\rVert}{\left\lVert\mathcal Hz\right\rVert}_\infty. \]

Here \(N_p\) is a continuous linear equivalence on the finite edge product because every component \(T_i\) is one. For a general root vector, remove its projection onto \(K\); this leaves the same \(\mathcal H\)-image and puts it in \(K^\perp\). Thus the displayed estimate is a uniform residual bound of the kind in Theorem 18.2, which forces \({\operatorname{ran}}\mathcal H\) to be closed. A finite-dimensional fiber makes that image finite dimensional and hence closed. It does not give a uniform numerical value of the inverse gain across different connections.

For isometric transports, one can use \({\left\lVert R_p\right\rVert}\le1\), \({\left\lVert N_p\right\rVert}\le1\), \({\left\lVert d\right\rVert}\le2\), and \(A_p\le r\), where \(r\) is the route radius. The bound reduces to

\[ {\left\lVert x-Px\right\rVert}_\infty\le[r+\kappa(2r+1)]{\left\lVert dx\right\rVert}_\infty. \]

The exact repair is route independent for a fixed root and inner product. A chosen upper bound involving route gains need not have the same numerical value for different routes.

19.3 Flatness does not remove amplification

Consider a scalar chain with \(n+1\) vertices, where \(n\ge1\), and coordinates \(e_i(z)=2^iz\). Set \(\tau_{ij}=e_ie_j^{-1}\). This connection is flat, but reverse transport along one edge multiplies norms by two. Let

\[ x_i=8\cdot2^i-1,\qquad y_i=7\cdot2^i. \]

The family \(y\) is exact and preserves \(x_o=7\). On a forward edge the residual of \(x\) is \(1/2\), and on its reverse it is \(-1\). Thus

\[ {\left\lVert dx\right\rVert}_\infty=1,\qquad {\left\lVert x-Px\right\rVert}_\infty=2^n-1. \]

For \(n\ge2\), a route length bound of \(n\) fails. This is amplification with trivial holonomy, distinct from poor conditioning of the fixed space of a nearly trivial loop.

A flat connection can still amplify a fixed residual. Both orientations of every edge are measured, giving residual norm one. Root-preserving repair has error (2 n-1 ), which exceeds the route-length estimate once (n ge 2 ). The vertical scale is logarithmic.
Figure 17. A flat connection can still amplify a fixed residual. Both orientations of every edge are measured, giving residual norm one. Root-preserving repair has error \(2^n-1\), which exceeds the route-length estimate once \(n\ge2\). The vertical scale is logarithmic.

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19.4 Small holonomy can still be poorly conditioned

In \({\mathbb R}^2\), the rational rotation

\[ U_t=\frac1{1+t^2} \begin{pmatrix}1-t^2&-2t\\2t&1-t^2\end{pmatrix} \]

satisfies

\[ {\left\lVert(U_t-I)z\right\rVert}^2=\frac{4t^2}{1+t^2}{\left\lVert z\right\rVert}^2. \]

For \(t\ne0\) its fixed space is zero and its residual gain is \(\sqrt{1+t^2}/(2|t|)\), which diverges as \(t\to0\). At \(t=0\), the entire fiber is fixed. Therefore small loop discrepancy does not supply a uniform stable realization estimate. The fixed directions and their conditioning must be analyzed together.

20 Quantitative descent in a common Hilbert model

20.1 Local exactness and matching are separate operators

Let \(E\) be a real Hilbert space of raw local candidates. Let \(D:E\to R\) and \(C:E\to Y\) be continuous linear maps into Banach spaces, measuring local equation defects and overlap mismatch, respectively. Put

\[ L=\ker D,\qquad B=C|_L, \qquad M=\ker D\cap\ker C. \]

The exact matched families form \(M\). First project to \(L\), then project inside \(L\) to \(\ker B\). Denote the resulting map by \(P\).

Theorem 20.1: The two-stage repair is the joint projection

The operator \(P\) is the orthogonal projection onto \(M\), equivalently onto the kernel of \(\Delta=(D,C)\). If \(u=x-P_Lx\) and \(v=P_Lx-Px\), then

\[ u\perp v,\qquad{\left\lVert x-Px\right\rVert}^2={\left\lVert u\right\rVert}^2+{\left\lVert v\right\rVert}^2. \]

Proof

The subspace \(L=\ker D\) is closed, hence Hilbert with the inherited inner product. The restriction \(B=C|_L\) is continuous, so its kernel is a closed subspace of \(L\). Under the inclusion into \(E\), this kernel is exactly \(M=L\cap\ker C\). Thus both projections used to define \(P\) exist.

For an input \(x\), write \(\ell=P_Lx\) and let \(Px\) be the projection of \(\ell\) onto \(\ker B\) inside \(L\). Then \(Px\in M\), \(u=x-\ell\in L^\perp\), and \(v=\ell-Px\in L\) is orthogonal to \(M\). Since \(M\subseteq L\), the vector \(u\) is also orthogonal to \(M\). Their sum \(x-Px=u+v\) is therefore orthogonal to \(M\). A vector in \(M\) with that error is the unique orthogonal projection of \(x\), so \(P=P_M\).

The two errors themselves are orthogonal because \(u\in L^\perp\) and \(v\in L\). Expanding the squared norm of their sum gives \({\left\lVert x-Px\right\rVert}^2={\left\lVert u\right\rVert}^2+{\left\lVert v\right\rVert}^2\). Finally \(\ker(D,C)=\ker D\cap\ker C=M\), so this is also the projection onto the kernel of the joint defect. The proof uses a second projection inside \(L\). Replacing it by the ambient projection onto \(\ker C\) would invalidate the membership step and need not preserve local exactness.

This identity does not require the local and overlap operators to commute. The second projection is taken in the already exact subspace, not in the whole raw space without restriction.

For a concrete failure of the unrestricted procedure, take \(L=\{(a,0)\}\) and \(\ker C=\{(a,a)\}\) in \({\mathbb R}^2\). Their intersection is zero. Starting from \((1,0)\), projection to \(L\) does nothing, while subsequent projection to \(\ker C\) gives \((1/2,1/2)\), which is no longer in \(L\). The restricted second stage instead gives the correct joint answer zero.

Local correction and overlap correction are orthogonal errors when the second problem is restricted to the locally exact subspace. Their composition is the projection onto the joint exact space. The overlap range inside that subspace is the additional stability obligation.
Figure 18. Local correction and overlap correction are orthogonal errors when the second problem is restricted to the locally exact subspace. Their composition is the projection onto the joint exact space. The overlap range inside that subspace is the additional stability obligation.

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20.2 A stable repair requires a stable matching problem

Suppose \({\operatorname{ran}} D\) and \({\operatorname{ran}} B\) are closed, with residual gains \(a,b\). Then

\[ {\left\lVert u\right\rVert}\le a{\left\lVert Dx\right\rVert},\qquad {\left\lVert v\right\rVert}\le b{\left\lVert CP_Lx\right\rVert} \le b({\left\lVert Cx\right\rVert}+{\left\lVert C\right\rVert}\,a{\left\lVert Dx\right\rVert}). \]

Therefore

\[ {\left\lVert x-Px\right\rVert}\le a(1+b{\left\lVert C\right\rVert}){\left\lVert Dx\right\rVert}+b{\left\lVert Cx\right\rVert}. \]
(20.1)

The Pythagorean identity gives the sharper estimate

\[ {\left\lVert x-Px\right\rVert}^2\le a^2{\left\lVert Dx\right\rVert}^2+b^2\bigl({\left\lVert Cx\right\rVert}+a{\left\lVert C\right\rVert}{\left\lVert Dx\right\rVert}\bigr)^2. \]

For the maximum norm on \(R\times Y\), two sufficient gains are therefore

\[ G_2=\sqrt{a^2+b^2(1+a{\left\lVert C\right\rVert})^2} \le G_1=a(1+b{\left\lVert C\right\rVert})+b. \]

The inequality follows from \(\sqrt{u^2+v^2}\le u+v\) for nonnegative \(u,v\). The formal interface supplies the sum-type gain \(G_1\), while its squared-error theorem also yields \(G_2\). Neither is claimed to be the least joint gain. In either bound, \({\left\lVert C\right\rVert}\) may be replaced by any certified bound on \(C\) restricted to \((\ker D)^\perp\).

Theorem 20.2: Closed range for the joint defect

Assume \({\operatorname{ran}} D\) is closed. Then

\[ {\operatorname{ran}}(D,C)\text{ is closed}\quad\Longleftrightarrow\quad {\operatorname{ran}}(C|_{\ker D})\text{ is closed}. \]

Under either condition, a finite joint residual-to-repair bound exists.

Proof

Suppose the range of the joint map is closed. To test closedness of \({\operatorname{ran}} B\), take a sequence \(Bk_n\to y\) with \(k_n\in\ker D\). The joint images are

\[ (Dk_n,Ck_n)=(0,Bk_n)\longrightarrow(0,y). \]

Closedness supplies \(x\in E\) with \((Dx,Cx)=(0,y)\). The first coordinate gives \(x\in\ker D\), and the second gives \(Bx=y\). Hence the matching range is closed. This direction did not require closedness of \({\operatorname{ran}} D\).

For the reverse direction, assume both \({\operatorname{ran}} D\) and \({\operatorname{ran}} B\) are closed, and take joint images converging to \((r,y)\). Thus \(Dx_n\to r\) and \(Cx_n\to y\). Decompose each input orthogonally as

\[ x_n=u_n+k_n,\quad u_n\in(\ker D)^\perp,\quad k_n\in\ker D. \]

Because \(r\in{\operatorname{ran}} D\) and the transverse inverse \(A\) of \(D\) is bounded by Theorem 18.2, the first components determine

\[ u_n=A(Dx_n)\longrightarrow A(r)=u, \qquad Du=r. \]

Continuity of \(C\) now gives

\[ Bk_n=Ck_n=Cx_n-Cu_n\longrightarrow y-Cu. \]

Closedness of \({\operatorname{ran}} B\) supplies \(k\in\ker D\) with \(Bk=y-Cu\). There is no need for the sequence \(k_n\) itself to converge. The single vector \(u+k\) satisfies

\[ D(u+k)=r, \qquad C(u+k)=Cu+Bk=y. \]

Thus the joint limit lies in the joint range, proving closedness. The target product is Banach under its maximum norm, so Theorem 18.2 applies to the joint map and gives a finite repair gain. The earlier two-stage estimate supplies an explicit, though not necessarily least, value.

This Hilbert model is a quantitative counterpart of gluing, but it is not a norm on an arbitrary categorical stack. It starts from a fixed raw candidate space, fixed norms, and actual local and overlap operators. Changing those choices requires its own comparison.

21 Controlled motion of exact spaces

21.1 A two-sided condition number theorem

Let \(D,D':E\to R\) be continuous linear maps from a real Hilbert space to the same normed target. Write \(q=P_{\ker D}\), \(q'=P_{\ker D'}\). Suppose

\[ {\left\lVert(I-q)x\right\rVert}\le C{\left\lVert Dx\right\rVert},\qquad {\left\lVert(I-q')x\right\rVert}\le C'{\left\lVert D'x\right\rVert},\qquad C,C'\ge0, \]

and \({\left\lVert D-D'\right\rVert}\le\varepsilon\).

Theorem 21.1: Motion of the exact projector

Without either kernel inclusion as a hypothesis,

\[ {\left\lVert q-q'\right\rVert}\le\max(C,C')\varepsilon. \]
(21.1)

In particular a uniform residual gain \(M\) makes \(D\mapsto P_{\ker D}\) \(M\)-Lipschitz on the class of operators carrying that gain.

Proof

For \(z\in\ker D'\), the old residual bound gives

\[ {\left\lVert(I-q)z\right\rVert}\le C{\left\lVert Dz\right\rVert} =C{\left\lVert(D-D')z\right\rVert}\le C\varepsilon{\left\lVert z\right\rVert}. \]

Interchanging the roles gives

\[ {\left\lVert(I-q')w\right\rVert}\le C'\varepsilon{\left\lVert w\right\rVert} \qquad(w\in\ker D). \tag{*} \]

We need a dual form of (*). For \(v\in(\ker D')^\perp\) and any \(y\in E\), self-adjointness of \(q\) and \(v=(I-q')v\) give

\[ |\langle qv,y\rangle| =|\langle v,qy\rangle| =|\langle v,(I-q')qy\rangle| \le C'\varepsilon{\left\lVert v\right\rVert}{\left\lVert qy\right\rVert} \le C'\varepsilon{\left\lVert v\right\rVert}{\left\lVert y\right\rVert}. \]

The Hilbert norm equals the supremum of these pairings on the unit ball, so \({\left\lVert qv\right\rVert}\le C'\varepsilon{\left\lVert v\right\rVert}\). This proves the precise restriction estimate needed on \((I-q')x\), not just a coarser bound in terms of \({\left\lVert x\right\rVert}\).

Now write

\[ (q-q')x=q(I-q')x-(I-q)q'x. \]

The two displayed terms lie in \(\ker D\) and \((\ker D)^\perp\), respectively, so they are orthogonal. The input components \((I-q')x\) and \(q'x\) are also orthogonal. Applying the dual estimate to the first and the original cross estimate to the second gives

\[ \begin{aligned} {\left\lVert(q-q')x\right\rVert}^2 &={\left\lVert q(I-q')x\right\rVert}^2+{\left\lVert(I-q)q'x\right\rVert}^2\\ &\le (C'\varepsilon)^2{\left\lVert(I-q')x\right\rVert}^2 +(C\varepsilon)^2{\left\lVert q'x\right\rVert}^2\\ &\le\varepsilon^2\max(C,C')^2 \bigl({\left\lVert(I-q')x\right\rVert}^2+{\left\lVert q'x\right\rVert}^2\bigr)\\ &=\varepsilon^2\max(C,C')^2{\left\lVert x\right\rVert}^2. \end{aligned} \]

The bound \({\left\lVert D-D'\right\rVert}\le\varepsilon\) implies \(\varepsilon\ge0\), so taking square roots yields the operator estimate. If the common gain is \(M\), substitute \(C=C'=M\) and \(\varepsilon={\left\lVert D-D'\right\rVert}\). This is exactly the Lipschitz inequality on the class carrying that gain. The use of two orthogonal decompositions explains the maximum coefficient instead of a sum.

There is no smallness threshold when both certificates are already supplied. The estimate can be uninformative when their gains are large. Knowing only the old certificate is a different situation.

For changing input as well as model, the same theorem gives

\[ {\left\lVert qx-q'y\right\rVert}\le{\left\lVert x-y\right\rVert}+\max(C,C')\varepsilon{\left\lVert y\right\rVert}. \]

It also bounds the change in distance to the exact space by \(\max(C,C')\varepsilon{\left\lVert x\right\rVert}\).

21.2 Constructing the new certificate

Assume the target \(R\) is Banach and \(A:R\to E\) is a continuous linear right inverse of \(D\), with \(DA=I\), \({\left\lVert A\right\rVert}\le a\), and \(a\varepsilon<1\). Set

\[ T=(D-D')A,\qquad Z=(I-T)^{-1},\qquad A'=AZ. \]

The inverse is supplied by the convergent Neumann series because \({\left\lVert T\right\rVert}\le a\varepsilon<1\).

Theorem 21.2: Stable surjectivity and derived repair

The perturbed map is surjective, with

\[ D'A'=I,\qquad {\left\lVert A'\right\rVert}\le\frac{a}{1-a\varepsilon}. \]

Its exact projection satisfies

\[ {\left\lVert x-q'x\right\rVert}\le\frac{a}{1-a\varepsilon}{\left\lVert D'x\right\rVert},\qquad {\left\lVert q-q'\right\rVert}\le\frac{a\varepsilon}{1-a\varepsilon}. \]

Proof

The map \(T=(D-D')A\) acts on the Banach target \(R\) and satisfies \({\left\lVert T\right\rVert}\le a\varepsilon<1\). The operator series

\[ Z=\sum_{n=0}^\infty T^n \]

converges in operator norm and obeys \({\left\lVert Z\right\rVert}\le(1-a\varepsilon)^{-1}\). Multiplying its finite partial sums on either side by \(I-T\) gives \(I-T^{N+1}\). Passing to the operator-norm limit proves \((I-T)Z=Z(I-T)=I\). Appendix E supplies the full series argument, including completeness of the operator space.

Since \(DA=I\), one has \(D'A=DA-(D-D')A=I-T\). Therefore \(A'=AZ\) satisfies

\[ D'A'=(I-T)Z=I,\qquad {\left\lVert A'\right\rVert}\le{\left\lVert A\right\rVert}{\left\lVert Z\right\rVert}\le\frac a{1-a\varepsilon}. \]

The first equation explicitly supplies a preimage of every target vector, proving surjectivity.

For any \(x\), put \(y=x-A'D'x\). Then \(D'y=D'x-D'A'D'x=0\), so \(y\) is a valid exact competitor for orthogonal projection. Its error gives

\[ {\left\lVert x-q'x\right\rVert}\le{\left\lVert x-y\right\rVert}={\left\lVert A'D'x\right\rVert} \le\frac a{1-a\varepsilon}{\left\lVert D'x\right\rVert}. \]

The same argument using \(A\) gives \({\left\lVert x-qx\right\rVert}\le a{\left\lVert Dx\right\rVert}\). Both coefficients are nonnegative and \(a/(1-a\varepsilon)\ge a\). Substitution into Theorem 21.1 yields

\[ {\left\lVert q-q'\right\rVert}\le\frac{a\varepsilon}{1-a\varepsilon}. \]

No assertion that \(I-A'D'\) is orthogonal was needed. It supplies an exact comparison vector, while best approximation supplies the orthogonal bound.

If a measured residual \(y\) satisfies \({\left\lVert D'x-y\right\rVert}\le\eta\), the distance to the new exact space is at most \(a({\left\lVert y\right\rVert}+\eta)/(1-a\varepsilon)\). The uncertainty radius remains a quantity to justify in the application. The theorem does not estimate it statistically.

For a surjective Hilbert-source operator, the right inverse need not be a separate unexplained input. The inverse of \(D:(\ker D)^\perp\to R\), followed by inclusion, constructs it. A known residual certificate bounds its norm. Surjectivity is still substantive, and cannot be assumed for a redundant residual map whose target contains unattainable directions.

21.3 An equivalence between the moving kernels

Theorem 21.3: Explicit kernel transport

Under the hypotheses of Theorem 21.2,

\[ J:\ker D\simeq_L\ker D',\qquad Jx=x-A'D'x, \]

with inverse \(y\mapsto y-ADy\). Moreover

\[ {\left\lVert Jx-x\right\rVert}\le\frac{a\varepsilon}{1-a\varepsilon}{\left\lVert x\right\rVert}. \]

Proof

Let \(R_0=I-AD\) and \(R_1=I-A'D'\). From \(DA=D'A'=I\) we obtain \(DR_0=0\) and \(D'R_1=0\). Each \(R_i\) fixes its corresponding kernel. Thus \(R_1\) restricts to a map from \(\ker D\) to \(\ker D'\), while \(R_0\) restricts in the other direction.

The inverse identities require two additional cancellations. First,

\[ R_0A'=(I-AD)AZ=(A-ADA)Z=0. \]

Second, using \(D'A=I-T\) and \(Z(I-T)=I\),

\[ R_1A=A-AZD'A=A-AZ(I-T)=0. \]

For \(x\in\ker D\), these identities give

\[ R_0R_1x=R_0(x-A'D'x)=R_0x=x. \]

For \(y\in\ker D'\), they give

\[ R_1R_0y=R_1(y-ADy)=R_1y=y. \]

Both restricted maps are bounded and linear as restrictions of bounded linear operators. They are therefore inverse continuous linear maps, establishing the asserted equivalence.

Finally, if \(Dx=0\), then \(D'x=(D'-D)x\). Hence

\[ {\left\lVert Jx-x\right\rVert}={\left\lVert A'D'x\right\rVert} \le{\left\lVert A'\right\rVert}\varepsilon{\left\lVert x\right\rVert} \le\frac{a\varepsilon}{1-a\varepsilon}{\left\lVert x\right\rVert}. \]

This derivation uses the selected right inverse \(A\) throughout. It proves a controlled transport of exact vectors, not a claim that the selected map is the nearest-point projection onto the new kernel.

The map \(J\) depends on the selected splitting. It is not generally the restriction of the orthogonal projection \(q'\). Equivalence of exact spaces and nearest-point repair answer different questions.

21.4 An all-real worked model

Let \(D_t(x,y)=x+ty\). Its kernel is the line \(\{(-tb,b):b\in{\mathbb R}\}\), and its orthogonal projector is

\[ q_t=\frac1{1+t^2} \begin{pmatrix}t^2&-t\\-t&1\end{pmatrix}. \]
(21.2)

The common right inverse \(r\mapsto(r,0)\) supplies gain at most one for every \(t\), and \({\left\lVert D_s-D_t\right\rVert}=|s-t|\). The general theorem gives \({\left\lVert q_s-q_t\right\rVert}\le|s-t|\).

Proposition 21.4: Exact motion of the line

For every real \(t\),

\[ {\left\lVert(q_t-q_0)x\right\rVert}^2=\frac{t^2}{1+t^2}{\left\lVert x\right\rVert}^2, \qquad {\left\lVert q_t-q_0\right\rVert}=\frac{|t|}{\sqrt{1+t^2}}. \]

In the small perturbation interface, kernel transport sends \((0,b)\) to \((-tb,b)\). Orthogonal projection instead sends it to \((-tb/(1+t^2),b/(1+t^2))\).

Proof

The vector \(v_t=(-t,1)\) spans \(\ker D_t\) and has squared norm \(1+t^2>0\). Projection onto this line is

\[ x\longmapsto\frac{\langle x,v_t\rangle}{1+t^2}v_t, \]

which gives the matrix in (21.2). In particular it is the orthogonal projector, not merely a map whose image is contained in the kernel.

Subtract \(q_0=\operatorname{diag}(0,1)\), obtaining the symmetric matrix

\[ B_t=q_t-q_0=\frac1{1+t^2} \begin{pmatrix}t^2&-t\\-t&-t^2\end{pmatrix}. \]

The two off-diagonal entries of its square are zero, since \(-t^3+t^3=0\). Both diagonal entries are \((t^4+t^2)/(1+t^2)^2=t^2/(1+t^2)\). Thus

\[ B_t^{\mathsf T}B_t=B_t^2=\frac{t^2}{1+t^2}I. \]

Pairing this identity with an arbitrary vector proves the all-vector norm formula. It bounds the operator norm above by \(|t|/\sqrt{1+t^2}\), and evaluating any unit vector gives equality. The argument includes \(t=0\), where both sides vanish.

For the common section \(A(r)=(r,0)\), the perturbation inverse leaves \(A\) unchanged because \(D_tA=I\). The constructed transport is therefore \(Jx=x-AD_tx\) on the old kernel. At \(x=(0,b)\), it gives \((-tb,b)\). Substitution into the projection formula gives instead \((-tb/(1+t^2),b/(1+t^2))\). The strict-radius theorem applies when \(|t|<1\), but these explicit line and projection calculations are valid for every real \(t\).

The exact space can move continuously without remaining equal to the original kernel. Transport along a chosen splitting preserves a coordinate, while orthogonal projection minimizes distance. In the line example these two maps have different formulas even though both land in the same exact space.
Figure 19. The exact space can move continuously without remaining equal to the original kernel. Transport along a chosen splitting preserves a coordinate, while orthogonal projection minimizes distance. In the line example these two maps have different formulas even though both land in the same exact space.

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21.5 What fails without the hypotheses

Take \(D_0=\operatorname{diag}(1,0)\) and \(D_t=\operatorname{diag}(1,t)\). The operator difference has norm \(|t|\). For every nonzero \(t\), however, the new kernel is zero, while the old kernel is the vertical axis. Their projections differ in norm by one. Operator closeness alone does not imply kernel continuity.

More generally, suppose a unit vector \(x\) is exact for the original operator but orthogonal to the new kernel. Every new residual gain \(C'\) obeys

\[ 1={\left\lVert x-q'x\right\rVert}\le C'{\left\lVert D'x\right\rVert}\le C'\varepsilon. \]

Losing an exact direction under a small operator change forces the new gain to grow. At the strict radius boundary, \(D=I\), \(A=I\), and \(D'=0\) have \(a=\varepsilon=1\), yet \(D'\) is not surjective. Thus the strict condition in Theorem 21.2 cannot be replaced universally by a non-strict one.

Two families can have the same small operator-change norm and very different exact-space motion. A moving line retains a uniform residual gain. The rank-changing diagonal family loses an exact direction for every nonzero parameter, so its projector gap remains one.
Figure 20. Two families can have the same small operator-change norm and very different exact-space motion. A moving line retains a uniform residual gain. The rank-changing diagonal family loses an exact direction for every nonzero parameter, so its projector gap remains one.

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21.6 Motion of the actual descent repair

Compare pairs \((D,C)\) and \((D',C')\) on the same raw Hilbert space. Suppose each pair has closed local range and closed overlap range on its own locally exact subspace. Let \(G,G'\) be the resulting joint residual gains. If

\[ {\left\lVert D-D'\right\rVert}\le\varepsilon_D,\qquad {\left\lVert C-C'\right\rVert}\le\varepsilon_C, \]

then the maximum norm on the target product gives

\[ {\left\lVert(D,C)-(D',C')\right\rVert}\le\max(\varepsilon_D,\varepsilon_C). \]

Applying Theorem 21.1 to the joint operators, and using the actual two-stage identity of Theorem 20.1, gives

\[ {\left\lVert P_{D,C}-P_{D',C'}\right\rVert} \le\max(G,G')\max(\varepsilon_D,\varepsilon_C). \]
(21.3)

This is a comparison of the original repair maps, not a replacement definition that happens to have a similar kernel. Both the local equations and overlap conditions can change. The raw space and its inner product remain fixed.

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