Blueprint for arXiv:2009.12982
Quantum Soundness of the Classical Low Individual Degree Test

4 Making measurements projective

Let \(\lvert \psi \rangle \) be a state in \(\mathcal H_{\mathrm A} \otimes \mathcal H_{\mathrm B}\). Let \(A = \{ A^x_a\} \) be a sub-measurement acting on \(\mathcal H_{\mathrm A}\) and \(B=\{ B^y_b\} \) be a sub-measurement acting on \(\mathcal H_{\mathrm B}\). Then there exist Hilbert spaces \(\mathcal H_{\mathrm A_{\mathsf{aux}}}\) and \(\mathcal H_{\mathrm B_{\mathsf{aux}}}\), a state \(\lvert \mathsf{aux} \rangle \in \mathcal H_{\mathrm A_{\mathsf{aux}}} \otimes \mathcal H_{\mathrm B_{\mathsf{aux}}}\), and projective sub-measurements \(\widehat{A} = \{ \widehat{A}^x_a\} \) and \(\widehat{B}=\{ \widehat{B}^y_b\} \) acting on \(\mathcal H_{\mathrm A} \otimes \mathcal H_{\mathrm A_{\mathsf{aux}}}\) and \(\mathcal H_{\mathrm B} \otimes \mathcal H_{\mathrm B_{\mathsf{aux}}}\), respectively, such that, if \(\lvert \widehat{\psi } \rangle = \lvert \psi \rangle \otimes \lvert \mathsf{aux} \rangle \), then for all \(x,y,a,b\),

\[ \langle \psi \rvert A^x_a \otimes B^y_b \lvert \psi \rangle = \langle \widehat{\psi } \rvert \widehat{A}^x_a \otimes \widehat{B}^y_b \lvert \widehat{\psi } \rangle . \]

In addition, \(\lvert \mathsf{aux} \rangle \) is a product state. The word “measurement” in the source statement is read here in the projective-submeasurement sense used by Lemma 4.7: for a general sub-measurement, the residual mass is carried by the additional \(\bot \) outcome in the auxiliary construction, so the original outcomes need not sum to the identity.

Proof

For each question \(x\), choose a local auxiliary state \(\lvert \mathsf{aux}_{\mathrm A,x} \rangle \) of dimension one larger than the number of outcomes of \(A^x\), and apply Lemma 4.7 to obtain a projective sub-measurement \(\widetilde A^x\). Do the same for each question \(y\) on Bob’s side, obtaining auxiliary states \(\lvert \mathsf{aux}_{\mathrm B,y} \rangle \) and projective sub-measurements \(\widetilde B^y\).

Let

\[ \lvert \mathsf{aux} \rangle = \Big(\bigotimes _x \lvert \mathsf{aux}_{\mathrm A,x} \rangle \Big) \otimes \Big(\bigotimes _y \lvert \mathsf{aux}_{\mathrm B,y} \rangle \Big), \qquad \lvert \widehat{\psi } \rangle = \lvert \psi \rangle \otimes \lvert \mathsf{aux} \rangle , \]

and let \(\widehat A^x_a\) and \(\widehat B^y_b\) be obtained by letting \(\widetilde A^x_a\) or \(\widetilde B^y_b\) act on the relevant auxiliary factor and the identity act on every other auxiliary factor. Because the auxiliary state is a product state and the two dilations act on disjoint tensor factors, the correlation for fixed \((x,y)\) reduces to the compression identity from Lemma 4.7 on the \(x\)- and \(y\)-registers. Hence

\[ \langle \widehat{\psi } \rvert \widehat A^x_a \otimes \widehat B^y_b \lvert \widehat{\psi } \rangle = \langle \psi \rvert A^x_a \otimes B^y_b \lvert \psi \rangle . \]
Remark 4.2 Lean questionwise Naimark interface
#

In addition to Theorem 4.1, Lean records the questionwise one-measurement interface obtained from Lemma 4.7. For every indexed family \(A^x\) and \(B^y\), it produces local dilation data for each question and proves the corresponding single-outcome marginal-preservation identities. This is a useful Lean-only auxiliary interface for downstream arguments, not a substitute for the full tensor-product correlation theorem, which is proved separately by naimarkTensorProductCorrelation.

Remark 4.3 Lean auxiliary declarations for Naimark
#

The checked Lean proof of Theorem 4.1 uses the standard one-measurement auxiliary register

\[ \mathrm{Option}(\mathcal A), \]

with the all-\(\bot \) vector as the initial auxiliary state. A separate Naimark unitary is chosen for each question, so the proof does not need a distinct auxiliary tensor factor for every question. This is equivalent for the theorem’s conclusion, since no commutation relation between different questions’ dilated measurements is required. The declaration OneMeasNaimarkData.twoSidedCorrelationPreservation proves the four-register trace identity which turns the two local compression identities into the bipartite correlation-preservation identity used by naimarkTensorProductCorrelation.

Let \(\lvert \psi \rangle \) be a permutation-invariant state, and let \(A = \{ A_a\} \) be a sub-measurement with strong self-consistency

\[ \sum _a \langle \psi \rvert A_a \otimes A_a \lvert \psi \rangle \geq \sum _a \langle \psi \rvert A_a \otimes I \lvert \psi \rangle - \zeta . \]

Then there exists a projective sub-measurement \(P = \{ P_a\} \) such that

\[ A_a \otimes I \approx _{100 \zeta ^{1/4}} P_a \otimes I. \]
Proof

Complete the sub-measurement by adding the missing outcome and use permutation invariance to convert strong self-consistency into the cross-consistency hypothesis of Lemma 4.9. Applying the locality-preserving projectivization repair gives the required projective sub-measurement with the paper constant \(100\zeta ^{1/4}\).

Remark 4.5 Lean right-register completion helpers
#

The inductive-step application of the orthogonalization lemma uses completion on both tensor factors. The formal development records the analytic completion statement on the left register; the shared preliminary helper compares right- and left-tensor placements at the level of the underlying state-dependent-distance form. Its submeasurement and indexed lemmas transport state-dependent distance to the right register under the permutation-invariance hypothesis on the state. The last linked declaration is a Lean-only construction from two already constructed orthonormalize-and-complete statements and a pre-projective consistency proof. It is not a source theorem and it is not an additional hypothesis of Theorem 2.14; it records only the tensor-factor bookkeeping needed to form the later line-156 projectivization transition.

Remark 4.6 Lean line-169 projectivization match-mass declarations
#

Lean exposes the quantitative obstruction at the projectivization transition used in the inductive step. The existing line-156 transition gives only the generic consequence of Proposition 3.20: from \(G^{\mathrm A}\simeq _{\zeta _1}G^{\mathrm B}\) and \(G^{\mathrm A}\approx _{\zeta _2}Q^{\mathrm A}\) one obtains \(Q^{\mathrm A}\simeq _{\zeta _1+\sqrt{\zeta _2}}G^{\mathrm B}\), and similarly on the other tensor factor. This direct square-root-loss route is an immediate specialization of the general Lean declarations MIPStarRE.LDT.Preliminaries.triangleSub and MIPStarRE.LDT.Preliminaries.triangleSub_right to the handoff fields, and is no longer maintained as separate named projectivization API.

Lean also proves a more local repaired transport that keeps the comparison at the pre-completion stage. If \(P^{\mathrm A}\) is the orthonormalized projective sub-measurement with \(G^{\mathrm A}\approx _{\epsilon }P^{\mathrm A}\), then Proposition 3.24 bounds the diagonal match-mass loss by \(\sqrt{\epsilon }\), and canonical completion can only add nonnegative diagonal match mass. Thus the declarations leftConsistency_of_completion_and_sdd and rightConsistency_of_completion_and_sdd prove \(Q^{\mathrm A}\simeq _{\zeta _1+\sqrt{\epsilon }}G^{\mathrm B}\) and its Bob-side mirror from the pre-projective \(\zeta _1\) consistency plus the pre-completion \(\approx _{\epsilon }\) comparison. In particular, substituting the checked orthonormalization error \(\epsilon =100\zeta _1^{1/4}\) yields the repaired line-169 bound \(\zeta _1+10\zeta _1^{1/8}\) recorded by leftConsistency_with_orthonormalization_loss and its mirror. This is much sharper than the direct completion-level \(\zeta _1+\sqrt{\zeta _2}\) route, but it is still not the paper’s exact \(\zeta _1\).

Lean also isolates the completion fact used inside this sharper repair: the canonical completion of a projective submeasurement can only increase its diagonal match mass against a fixed partner submeasurement. This is the formal declaration ProjectivizationMatchMassMonotonicity.completeAtOutcomeProj_left_matchMass_ge. The sharper route therefore pays its square-root loss before completion and then uses completion only in this monotone direction, with no additional match-mass penalty.

The older exact-\(\zeta _1\) construction-level monotonicity statement has been retired. The current Section 5 API proves the checked repaired transport above, and the active orthonormalization route now uses those repaired completion-transport estimates rather than a separate exact match-mass witness.

4.0.1 Naimark dilation

Let \(A = \{ A_a\} \) be a sub-measurement with \(k\) distinct outcomes \(a \in \mathcal A\), and let \(\lvert \mathsf{aux} \rangle \in \mathbb {C}^{k+1}\) be any state. Then there exists a projective sub-measurement \(\widehat{A} = \{ \widehat{A}_a\} \) such that for each outcome \(a\),

\[ (I \otimes \langle \mathsf{aux} \rvert ) \cdot \widehat{A}_a \cdot (I \otimes \lvert \mathsf{aux} \rangle ) = A_a. \]
Proof

Consider an orthonormal basis for \(\mathbb {C}^{k+1}\) consisting of vectors \(\lvert a \rangle \) for \(a \in \mathcal A\) and the vector \(\lvert \bot \rangle \). Let \(U\) be any unitary such that for each vector \(\lvert \phi \rangle \),

\[ U \cdot (\lvert \phi \rangle \otimes \lvert \mathsf{aux} \rangle ) = \sum _{a \in \mathcal A} ((A_a)^{1/2}\lvert \phi \rangle ) \otimes \lvert a \rangle + ((I-A)^{1/2}\lvert \phi \rangle ) \otimes \lvert \bot \rangle , \]

where \(A=\sum _a A_a\). Then

\[ U \cdot (I \otimes \lvert \mathsf{aux} \rangle ) = \sum _{a \in \mathcal A} (A_a)^{1/2} \otimes \lvert a \rangle + (I-A)^{1/2} \otimes \lvert \bot \rangle , \]

so for any \(a \in \mathcal A\),

\[ (I \otimes \langle a \rvert ) \cdot U \cdot (I \otimes \lvert \mathsf{aux} \rangle ) = (A_a)^{1/2}. \]

Define

\[ \widehat{A}_a = U^\dagger \cdot (I \otimes \lvert a \rangle \langle a \rvert ) \cdot U. \]

Each \(\widehat{A}_a\) is a projector, and

\begin{align*} (I \otimes \langle \mathsf{aux} \rvert ) \cdot \widehat{A}_a \cdot (I \otimes \lvert \mathsf{aux} \rangle ) & = (I \otimes \langle \mathsf{aux} \rvert ) \cdot U^\dagger \cdot (I \otimes \lvert a \rangle ) \cdot (I \otimes \langle a \rvert ) \cdot U \cdot (I \otimes \lvert \mathsf{aux} \rangle ) \\ & = (A_a)^{1/2} \cdot (A_a)^{1/2} = A_a. \end{align*}
Remark 4.8 Naimark dilation does not preserve \(\approx _\delta \)
#

Let \(\lvert \psi \rangle \) be any state in \(\mathbb {C}^d \otimes \mathbb {C}^d\), and consider the two-outcome measurements \(A = \{ A_0, A_1\} \) and \(B = \{ B_0, B_1\} \) with

\[ A_0 = A_1 = B_0 = B_1 = \tfrac {1}{2} I. \]

For each outcome \(a \in \{ 0,1\} \), the operators \(A_a \otimes I\) and \(I \otimes B_a\) are both equal to \(\tfrac {1}{2} I \otimes I\), so \(A_a \otimes I \approx _0 I \otimes B_a\) on the state \(\lvert \psi \rangle \).

Now apply the Naimark construction with a qubit auxiliary space on each side and auxiliary state \(\lvert + \rangle = \tfrac {1}{\sqrt2}(\lvert 0 \rangle +\lvert 1 \rangle )\). Since \(A\) and \(B\) are genuine measurements rather than sub-measurements, the extra \(\lvert \bot \rangle \) direction from 4.7 is unnecessary in this example. The unitary from 4.7 can then be taken to be the identity, so the dilated measurements are

\[ \widehat A_a = I \otimes \lvert a \rangle \langle a \rvert , \qquad \widehat B_a = I \otimes \lvert a \rangle \langle a \rvert . \]

If \(\lvert \widehat{\psi } \rangle = \lvert \psi \rangle \otimes \lvert + \rangle \otimes \lvert + \rangle \), then a direct calculation gives

\[ \sum _{a \in \{ 0,1\} } \bigl\lVert (\widehat A_a \otimes I - I \otimes \widehat B_a) \lvert \widehat{\psi } \rangle \bigr\rVert ^2 = 1. \]

Thus on the state \(\lvert \widehat{\psi } \rangle \) the dilated family satisfies \(\widehat A_a \otimes I \approx _\delta I \otimes \widehat B_a\) only for \(\delta \ge 1\), even though the original family satisfied the same relation with \(\delta = 0\). This is why we use Theorem 4.4 rather than simply applying Theorem 4.1: Naimark preserves the outcome probabilities, but it need not preserve the state-dependent \(\approx _\delta \) estimates needed later.

4.0.2 Orthogonalization lemma

Let \(\lvert \psi \rangle \) be a state, and let \(A = \{ A_a\} \) and \(B = \{ B_a\} \) be measurements such that

\[ A_a \otimes I \simeq _\zeta I \otimes B_a \]

on state \(\lvert \psi \rangle \). Here \(\lvert \psi \rangle \) is not assumed to be permutation-invariant. Then there exists a projective sub-measurement \(P = \{ P_a\} \) such that

\[ A_a \otimes I \approx _{84 \zeta ^{1/4}} P_a \otimes I. \]

This same-space corollary weakens Lemma 4.9 to the public orthonormalization envelope \(100\zeta ^{1/4}\). Thus, if \(A=\{ A_a\} \) and \(B=\{ B_a\} \) are measurements on the same finite-dimensional space satisfying

\[ A_a \otimes I \simeq _\zeta I \otimes B_a \]

on a normalized bipartite state \(\lvert \psi \rangle \), then there exists a projective sub-measurement \(P=\{ P_a\} \) such that

\[ A_a \otimes I \approx _{100\zeta ^{1/4}} P_a \otimes I . \]

This is the corrected Lean theorem proved from the Section 5 projectivization repair construction. The sharper heterogeneous source statement \(84\zeta ^{1/4}\) is now formalized as Lemma 4.9.

Proof

The consistency hypothesis first gives the source almost-projective estimate for \(A_a\otimes I\). The locality-preserving projectivization repair then produces a projective sub-measurement on the original space, and the scalar bounds convert the \(84\)-constant repair estimate into the public \(100\zeta ^{1/4}\) envelope.

Remark 4.11 Lean auxiliary declarations for the orthogonalization lemma
#

The Lean declaration MIPStarRE.LDT.MakingMeasurementsProjective.orthonormalizationMainLemma proves Lemma 4.9 without adding spectral-truncation or repair hypotheses. The proof first converts the cross-consistency hypothesis into the source almost-projective estimate for the measurement \(A_a \otimes I\), and then applies the locality-preserving \(Q/X/\widehat X/P\) construction in its heterogeneous left-register form. Lemma 4.10 remains as the same-space corollary with the weaker public \(100\zeta ^{1/4}\) envelope. The measurement-level declarations orthonormalizationMeasurement_of_consistency and orthonormalizationMeasurement are proved corollaries, not conditional wrappers: they derive the projective submeasurement from the displayed consistency or self-consistency hypotheses.

Paper origin: references/ldt-paper/orthonormalization.tex lines 534–860 (rank reduction and the \(Q\)-side setup, including 4.28 and 4.29) and 862–1194 (the \(X/\widehat X/P\) algebra: 4.30, 4.33, 4.34, 4.36, 4.37, 4.38, plus the final triangle-inequality calculation producing the \(84\zeta ^{1/4}\) bound). Together these are the late repair stage of the orthogonalization-lemma proof.

Given a normalized bipartite state \(\lvert \psi \rangle \), a measurement \(A = \{ A_a\} \), and the source almost-projective estimate for the left-lifted family \(\{ A_a \otimes I\} \), there exists a locality-preserving projective sub-measurement with error \(84\zeta ^{1/4}\).

More precisely, if \(\lvert \psi \rangle \) is a normalized bipartite state, if \(A = \{ A_a\} \) is a measurement, and if

\[ \sum _a \langle \psi \rvert \bigl((A_a \otimes I) - (A_a \otimes I)^2\bigr) \lvert \psi \rangle \le \zeta , \]

then there exists a projective sub-measurement \(P = \{ P_a\} \) on the underlying space such that

\[ A_a \otimes I \approx _{84\zeta ^{1/4}} P_a \otimes I. \]

The locality-preserving form – output \(P_a \otimes I\) rather than an arbitrary lifted family – is recorded in Remark 4.11 and is the form required by the unconditional orthonormalization theorem (4.4).

Proof

Pass to the left marginal state, apply the rank-reduction and \(Q/X/\widehat X/P\) construction there, and transport the resulting \(\approx _{84\zeta ^{1/4}}\) estimate back to left lifts via the left-marginal expectation formula.

Proposition 4.13 Measurement-level orthogonalization from consistency

This is the same-space measurement corollary recorded in Remark 4.11. Let \(\lvert \psi \rangle \) be a normalized bipartite state, let \(A=\{ A_a\} \) and \(B=\{ B_a\} \) be measurements on the same finite-dimensional space, and let \(0 \leq \zeta \). Assume the bipartite consistency estimate

\[ A_a \otimes I \simeq _{\zeta } I \otimes B_a . \]

Then there exists a projective sub-measurement \(P=\{ P_a\} \) such that

\[ A_a \otimes I \approx _{100\zeta ^{1/4}} P_a \otimes I . \]
Proof

The proof applies Lemma 4.9 and weakens the \(84\zeta ^{1/4}\) estimate to the public orthonormalization envelope. The spectral-truncation and locality-preserving repair steps are internal to that proof; they are not hypotheses of this declaration.

Proposition 4.14 Measurement-level orthogonalization from self-consistency

This is the self-consistency specialization of Proposition 4.13. Let \(\lvert \psi \rangle \) be a normalized bipartite state, let \(A=\{ A_a\} \) be a measurement, and let \(0\leq \zeta \). If \(A\) is bipartite strongly self-consistent with error \(\zeta \), then there exists a projective sub-measurement \(P=\{ P_a\} \) such that

\[ A_a \otimes I \approx _{100 \zeta ^{1/4}} P_a \otimes I. \]
Proof

Since \(A\) is complete, the self-consistency defect is the consistency defect of \(A\) with itself. The proof therefore applies the consistency corollary with \(B=A\). No spectral-truncation witness or repair witness is assumed at this interface.

The paper theorem 4.4 is proved in Lean with the \(100\zeta ^{1/4}\) constant. The declaration checked here is the completion-route theorem with the weaker bound \(120\zeta ^{1/4}\), recorded in orthonormalizationCompletionRouteError. See [ con26a ] .

Let \(\lvert \psi \rangle \) be a normalized permutation-invariant state, and let \(A=\{ A_a\} _{a\in \mathcal A}\) be a sub-measurement which is bipartite strongly self-consistent with error \(\zeta \). Then there exists a projective sub-measurement \(P=\{ P_a\} _{a\in \mathcal A}\) such that

\[ A_a \otimes I \approx _{120\zeta ^{1/4}} P_a \otimes I. \]
Proof

Write \(A=\sum _a A_a\). The strong self-consistency assumption implies

\[ \langle \psi \rvert A \otimes A \lvert \psi \rangle \geq \langle \psi \rvert A \otimes I \lvert \psi \rangle - \zeta , \]

so

\[ \langle \psi \rvert A \otimes (I-A) \lvert \psi \rangle \leq \zeta . \]

Rearranging once more gives

\[ \langle \psi \rvert (I-A) \otimes (I-A) \lvert \psi \rangle \geq \langle \psi \rvert (I-A) \otimes I \lvert \psi \rangle - \zeta . \]

Complete \(A\) to the measurement \(\widehat A=\{ \widehat A_a\} _{a \in \widehat{\mathcal A}}\) on \(\widehat{\mathcal A}=\mathcal A \cup \{ \bot \} \) by setting \(\widehat A_a=A_a\) for \(a \in \mathcal A\) and \(\widehat A_{\bot }=I-A\). Adding the two preceding inequalities shows that \(\widehat A\) is \(2\zeta \)-strongly self-consistent. By 3.35, this gives the source almost-projective estimate

\[ \sum _a \langle \psi \rvert \bigl((\widehat A_a\otimes I)-(\widehat A_a\otimes I)^2\bigr) \lvert \psi \rangle \le 4\zeta . \]

Apply 4.12 to obtain a projective sub-measurement \(\widehat P\) such that

\[ \widehat A_a \otimes I \approx _{84(4\zeta )^{1/4}} \widehat P_a \otimes I. \]

Discard the extra outcome and set \(P_a=\widehat P_a\) for \(a \in \mathcal A\). Then

\[ A_a \otimes I \approx _{84(4\zeta )^{1/4}} P_a \otimes I, \]

and \(84 \cdot 4^{1/4} \leq 120\), so the completion-route bound follows.

Proof of 4.9

The statement is trivial when \(\zeta {\gt} 1/4\), so assume

\begin{equation} \label{eq:assumption-on-zeta} \zeta \leq 1/4. \end{equation}
1

By 3.18,

\[ \sum _a \langle \psi \rvert A_a \otimes B_a \lvert \psi \rangle \geq 1-\zeta . \]

Apply Cauchy–Schwarz to

\[ \sum _a \langle \psi \rvert (A_a \otimes I)\cdot (I \otimes B_a)\lvert \psi \rangle \]

to obtain

\[ \sum _a \langle \psi \rvert (A_a)^2 \otimes I \lvert \psi \rangle \geq (1-\zeta )^2 \geq 1-2\zeta . \]

Because \(A\) is a measurement, this rewrites as

\begin{equation} \label{eq:A-looks-projective} \sum _a \langle \psi \rvert (A_a-(A_a)^2) \otimes I \lvert \psi \rangle \leq 2\zeta . \end{equation}
2

Lemma 4.16

For any \(x \in [0, 1]\),

\begin{equation*} (x - \mathsf{trunc}_\delta (x))^2 \leq \frac{1}{\delta } \cdot (x - x^2). \end{equation*}
Proof

If \(x \geq 1-\delta \), then \(\mathsf{trunc}_\delta (x)=1\). Since \(\delta \leq 1/2\) below, one also has \(x \geq \delta \), so

\[ (x-\mathsf{trunc}_\delta (x))^2 = (1-x)^2 \leq (1-x)\frac{x}{\delta } = \frac{1}{\delta }(x-x^2). \]

If \(x {\lt} 1-\delta \), then \(\mathsf{trunc}_\delta (x)=0\), and similarly

\[ (x-\mathsf{trunc}_\delta (x))^2 = x^2 \leq x\frac{1-x}{\delta } = \frac{1}{\delta }(x-x^2). \]

There exists a set of projective matrices \(\{ R_a\} \) such that

\begin{equation*} A_a \otimes I \approx _{2\sqrt{\zeta }} R_a \otimes I. \end{equation*}

and

\begin{equation*} R:= \sum _a R_a \leq (1+2\sqrt{\zeta }) \cdot I. \end{equation*}
Proof

Write the eigendecomposition of \(A_a\) as

\[ A_a = \sum _i \lambda _{a,i}\lvert u_{a,i} \rangle \langle u_{a,i} \rvert . \]

Choose

\begin{equation} \label{eq:bound-on-delta} 0 {\lt} \delta \leq 1/2, \end{equation}
3

define \(\mathsf{trunc}_\delta :[0,1] \to \{ 0,1\} \) by \(\mathsf{trunc}_\delta (x)=1\) when \(x \geq 1-\delta \) and \(0\) otherwise, and set

\[ R_a = \mathsf{trunc}_\delta (A_a) = \sum _i \mathsf{trunc}_\delta (\lambda _{a,i}) \lvert u_{a,i} \rangle \langle u_{a,i} \rvert . \]

By 4.16,

\[ (A_a-R_a)^2 \leq \frac{1}{\delta }(A_a-(A_a)^2). \]

Summing expectations and using 2 gives

\[ \sum _a \Vert (A_a-R_a)\otimes I \lvert \psi \rangle \Vert ^2 \leq \frac{2\zeta }{\delta }, \]

so \(A_a \otimes I \approx _{2\zeta /\delta } R_a \otimes I\).

For every \(x \in [0,1]\), one has \(\mathsf{trunc}_\delta (x) \leq x/(1-\delta )\), hence

\[ R_a \leq \frac{1}{1-\delta } A_a. \]

Summing over \(a\) and using that \(A\) is a measurement,

\[ R = \sum _a R_a \leq \frac{1}{1-\delta } I \leq (1+2\delta )I, \]

where the last estimate uses \(\delta \leq 1/2\). Setting \(\delta =\sqrt{\zeta }\) gives the claim, and 1 ensures \(\delta \leq 1/2\).

Remark 4.18 Lean auxiliary declarations for rounding to projectors
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The source-facing Lean declarations for Lemma 4.17 are the proposition projectiveNonMeasurement and the construction theorem projectiveNonMeasurement_of_sourceAlmostProjective_full. The declarations listed here are the endpoint and regime splits, the AlmostProjMeasStatement witness forms, and the spectral-truncation statement conversions used by later Section 5 arguments. They are not additional hypotheses in the paper statement of Lemma 4.17.

Let \(f : \alpha \to \mathbb {R}\) be a function on a finite index set \(\alpha \) with \(|\alpha | = r\), and let \(L \subseteq \alpha \) with \(|L| = d\) and \(d {\lt} r\). Write \(S = L^\complement \) and assume \(f(s) \leq f(l)\) for every \(s \in S\) and \(l \in L\). Then the pairwise double-counting inequality

\[ |L|\, \sum _{s \in S} f(s) \leq |S|\, \sum _{l \in L} f(l) \]

holds, and hence also

\[ r\, \sum _{s \in S} f(s) \leq |S|\, \sum _{x \in \alpha } f(x). \]

If in addition \(r \leq (1+2\sqrt{\zeta })\, d\), \(\sum _{x \in \alpha } f(x) \leq 1 + 2\sqrt{\zeta }\), and \(0 \leq \zeta \leq 1/4\), then

\[ \sum _{s \in S} f(s) \leq 4\sqrt{\zeta }. \]
Proof

Choose \(L\) to be a set of \(d\) indices on which the sum of \(f\) is maximal. If some \(s \in S\) and \(l \in L\) satisfied \(f(l) {\lt} f(s)\), replacing \(l\) by \(s\) would increase this sum, so every small index is bounded by every large index. Summing the inequalities \(f(s) \leq f(l)\) over all pairs \((s,l) \in S \times L\) gives

\[ |L|\sum _{s \in S} f(s) \leq |S|\sum _{l \in L} f(l). \]

Since \(\alpha \) is the disjoint union of \(L\) and \(S\), adding \(|S|\sum _{s \in S} f(s)\) to both sides yields

\[ r\sum _{s \in S} f(s) \leq |S|\sum _{x \in \alpha } f(x). \]

The hypotheses \(|L|=d\) and \(r \leq (1+2\sqrt{\zeta })d\) imply \(|S|/r \leq 2\sqrt{\zeta }\). Dividing by \(r\) and using \(\sum _{x \in \alpha } f(x) \leq 1+2\sqrt{\zeta }\) gives

\[ \sum _{s \in S} f(s) \leq 2\sqrt{\zeta }(1+2\sqrt{\zeta }). \]

Finally, \(\zeta \leq 1/4\) implies \(\sqrt{\zeta } \leq 1/2\), and hence \(2\sqrt{\zeta }(1+2\sqrt{\zeta }) \leq 4\sqrt{\zeta }\).

Lemma 4.20 Rank reduction

There exists a set of projection matrices \(\{ Q_a\} \) such that

\begin{equation*} A_a \otimes I \approx _{12\sqrt{\zeta }} Q_a \otimes I. \end{equation*}

and

\begin{equation*} Q:= \sum _a Q_a \leq (1+2\sqrt{\zeta }) \cdot I. \end{equation*}

Furthermore,

\begin{equation*} \sum _a \mathrm{rank}(Q_a) \leq d. \end{equation*}
Proof

Let \(\{ R_a\} \) be given by 4.17. Write \(r_a=\mathrm{rank}(R_a)\) and \(r=\sum _a r_a\). If \(r \leq d\), take \(Q_a=R_a\). Otherwise,

\begin{equation} \label{eq:bound-on-r} r = \sum _a r_a = \sum _a \operatorname{Tr}(R_a) = \operatorname{Tr}(R) \leq (1+2\sqrt{\zeta })d. \end{equation}
4

Let \(\lvert v_{a,1} \rangle ,\ldots ,\lvert v_{a,r_a} \rangle \) be an orthonormal basis for the range of \(R_a\), so

\[ R_a = \sum _{i=1}^{r_a} \lvert v_{a,i} \rangle \langle v_{a,i} \rvert . \]

Define the overlaps

\[ o_{a,i} = \langle \psi \rvert (\lvert v_{a,i} \rangle \langle v_{a,i} \rvert \otimes I)\lvert \psi \rangle . \]

Their total satisfies

\begin{equation} \label{eq:total-overlap} \sum _a \sum _{i=1}^{r_a} o_{a,i} = \langle \psi \rvert R \otimes I \lvert \psi \rangle \leq 1+2\sqrt{\zeta }. \end{equation}
5

Let \(\mathsf{Large}\) be the set of the \(d\) largest overlaps \(o_{a,i}\), breaking ties arbitrarily, and let \(\mathsf{Small}\) be the complement. Then

\begin{equation} \label{eq:size-of-small-is-small} |\mathsf{Small}| = r-d \leq 2\sqrt{\zeta }\, d \leq 2\sqrt{\zeta }\, r, \end{equation}
6

by 4. Averaging the overlaps over the \(r\) indices gives

\begin{equation} \label{eq:small-overlaps} \sum _{(a,i)\in \mathsf{Small}} o_{a,i} \leq \frac{|\mathsf{Small}|}{r}\sum _{a,i} o_{a,i} \leq 4\sqrt{\zeta }, \end{equation}
7

using 6, 5, and 1.

For each \(a\), let \(\mathsf{Large}_a=\{ i : (a,i)\in \mathsf{Large}\} \) and define

\[ Q_a = \sum _{i \in \mathsf{Large}_a} \lvert v_{a,i} \rangle \langle v_{a,i} \rvert . \]

Then \(\sum _a \mathrm{rank}(Q_a)=|\mathsf{Large}| \leq d\), and \(Q_a \leq R_a\) for every \(a\), so

\[ Q = \sum _a Q_a \leq \sum _a R_a = R \leq (1+2\sqrt{\zeta })I. \]

Also,

\[ R_a-Q_a = \sum _{i \in \mathsf{Small}_a} \lvert v_{a,i} \rangle \langle v_{a,i} \rvert \]

is a projector, hence

\[ \sum _a \Vert (R_a-Q_a)\otimes I \lvert \psi \rangle \Vert ^2 = \sum _{(a,i)\in \mathsf{Small}} o_{a,i} \leq 4\sqrt{\zeta } \]

by 7. Therefore \(R_a \otimes I \approx _{4\sqrt{\zeta }} Q_a \otimes I\). Combining this with 4.17 and the triangle inequality for \(\approx _\delta \) gives

\[ A_a \otimes I \approx _{12\sqrt{\zeta }} Q_a \otimes I. \]

Henceforth let \(Q=\{ Q_a\} \) be the family given by 4.20.

Lemma 4.21 Completeness of \(Q\)
\begin{equation*} \langle \psi \rvert Q \otimes I \lvert \psi \rangle \geq 1 - 11 \zeta ^{1/4}. \end{equation*}
Proof

Since each \(Q_a\) is projective,

\begin{equation} \label{eq:Q-for-an-A} \langle \psi \rvert Q \otimes I \lvert \psi \rangle = \sum _a \langle \psi \rvert (Q_a)^2 \otimes I \lvert \psi \rangle \approx _{5\zeta ^{1/4}} \sum _a \langle \psi \rvert (Q_a \cdot A_a)\otimes I \lvert \psi \rangle . \end{equation}
8

By Cauchy–Schwarz,

\[ \sum _a \langle \psi \rvert (Q_a)^2 \otimes I \lvert \psi \rangle \leq 1+2\sqrt{\zeta } \quad \text{and}\quad \sum _a \langle \psi \rvert (Q_a-A_a)^2 \otimes I \lvert \psi \rangle \leq 12\sqrt{\zeta } \]

from 4.20. A second Cauchy–Schwarz estimate yields

\begin{equation} \label{eq:another-Q-for-A} \sum _a \langle \psi \rvert (Q_a \cdot A_a)\otimes I \lvert \psi \rangle \approx _{4\zeta ^{1/4}} \sum _a \langle \psi \rvert (A_a)^2 \otimes I \lvert \psi \rangle . \end{equation}
9

Combining 8 and 9 with 2 gives

\[ \langle \psi \rvert Q \otimes I \lvert \psi \rangle \geq \sum _a \langle \psi \rvert A_a \otimes I \lvert \psi \rangle - 2\zeta - 9\zeta ^{1/4} = 1 - 11\zeta ^{1/4}, \]

since \(\zeta \leq \zeta ^{1/4}\) under 1.

Lemma 4.22 Completeness of \(\sqrt{Q}\)
\begin{equation*} \langle \psi \rvert \sqrt{Q} \otimes I \lvert \psi \rangle \geq 1 - 12 \zeta ^{1/4}. \end{equation*}
Proof

Diagonalize \(Q=\sum _i \nu _i \lvert u_i \rangle \langle u_i \rvert \). Because \(Q \leq (1+2\sqrt{\zeta })I\) by 4.20, each \(\nu _i\) is at most \(1+2\sqrt{\zeta }\). Therefore

\[ \sqrt{Q} = \sum _i \sqrt{\nu _i}\lvert u_i \rangle \langle u_i \rvert \geq \frac{1}{\sqrt{1+2\sqrt{\zeta }}} Q. \]

The scalar estimate

\[ \frac{1}{\sqrt{1+2\sqrt{\zeta }}} \geq 1-\sqrt{\zeta } \]

gives \(\sqrt{Q} \geq (1-\sqrt{\zeta })Q\). Hence 4.21 implies

\[ \langle \psi \rvert \sqrt{Q} \otimes I \lvert \psi \rangle \geq (1-\sqrt{\zeta })(1-11\zeta ^{1/4}) \geq 1-12\zeta ^{1/4}. \]
Lemma 4.23 \(Q\) is almost projective
\begin{equation*} \sum _a (Q_a \cdot Q \cdot Q_a - Q_a) \leq 4\sqrt{\zeta } \cdot I. \end{equation*}
Proof

Since \(Q \leq (1+2\sqrt{\zeta })I\) by 4.20,

\begin{align*} \sum _a Q_a \cdot Q \cdot Q_a - \sum _a Q_a & \leq (1+2\sqrt{\zeta }) \sum _a Q_a \cdot I \cdot Q_a - \sum _a Q_a \\ & = (1+2\sqrt{\zeta })Q - Q \\ & = 2\sqrt{\zeta }\, Q \\ & \leq 2\sqrt{\zeta }(1+2\sqrt{\zeta })I \\ & \leq 4\sqrt{\zeta }\, I, \end{align*}

using 1 in the last step.

For each \(a\), let

\[ m_a = \mathrm{rank}(Q_a), \]

and let \(\lvert v_{a,1} \rangle ,\ldots ,\lvert v_{a,m_a} \rangle \) be an orthonormal basis for the range of \(Q_a\), so that

\[ Q_a = \sum _{i=1}^{m_a} \lvert v_{a,i} \rangle \langle v_{a,i} \rvert . \]

Let

\[ m = \sum _a m_a, \]

and let \(\{ \lvert a,i \rangle \} \) be an orthonormal basis of \(\mathbb {C}^m\), indexed by all \(a\) and all \(1 \leq i \leq m_a\). For each \(a\), define

\[ X_a = \sum _{i=1}^{m_a} \lvert a,i \rangle \langle v_{a,i} \rvert , \qquad T_a = \sum _{i=1}^{m_a} \lvert a,i \rangle \langle a,i \rvert , \]

and define

\begin{equation} \label{eq:looks-like-singular-value-decomposition} X = \sum _a X_a = \sum _a \sum _{i=1}^{m_a} \lvert a,i \rangle \langle v_{a,i} \rvert . \end{equation}
10

Let \(T = \{ T_a\} \). Then \(T\) is a projective measurement on \(\mathbb {C}^m\).

Proof

Choose an orthonormal basis of the range of each projector \(Q_a\). The rank-one expansion gives the displayed decomposition, and the orthogonality of the labelled basis vectors makes the family \(T\) a projective measurement.

The paper presents this step by choosing a singular value decomposition

\[ X = U \cdot \Sigma _{m \times d} \cdot V^\dagger . \]

The formalization has two closely related auxiliary declarations. The reduced datum records the downstream consequences of the choice: the matrices \(X\) and \(\widehat X\), the identities \(X^\dagger X=Q\), \(\widehat X\widehat X^\dagger =I\), and \(X^\dagger \widehat X=\sqrt Q\), together with the \(Q_a=X^\dagger T_aX\) restatement. The rectangular-SVD lemmas take explicit matrices \(U,V,\Sigma ,I_{m\times d}\) and derive the two stored \(\widehat X\) identities from the matrix calculation below.

Proof

Apply the finite-dimensional singular value decomposition to \(X\) and record exactly the consequences used later: the identities for \(X^\dagger X\), \(\widehat X\widehat X^\dagger \), \(X^\dagger \widehat X\), and the restatement of the \(Q_a\)’s. The unitary-group constructors are the same rectangular-SVD calculation, with the square factors taken as elements of the relevant unitary groups rather than as matrices accompanied by separate unitarity equations. In the sigma-range specialization, the auxiliary row space is the lifted finite-enumeration carrier associated to the ranks of the \(Q_a\)’s, which is definitionally the carrier of the canonical sigma-range \(Q\)-layer.

Remark 4.26 Formalization support for orthogonal projector families
#

If the family \(\{ Q_a\} \) were a projective measurement, then the vectors \(\lvert v_{a,i} \rangle \), over all \(a\) and all \(1 \leq i \leq m_a\), would be orthonormal. Then 10 would already be a singular value decomposition of \(X\), with \(\Sigma = I_{m \times d}\). Equivalently,

\[ X = U \cdot I_{m \times d} \cdot V^\dagger . \]

This motivates replacing \(\Sigma \) by \(I\) in the definition of \(\widehat X\) and \(P\).

Definition 4.27 Definition of \(P\)

The paper defines

\[ \widehat{X} = U \cdot I_{m \times d} \cdot V^\dagger . \]

We take \(\widehat X\) to be the reduced matrix supplied by the stored datum. For each \(a\), define

\[ \widehat{X}_a = T_a \cdot \widehat{X}, \qquad P_a = \widehat{X}_a^\dagger \cdot \widehat{X}_a. \]
Proof

The definition is the formal \(Q/X/\widehat X/P\) construction: once \(\widehat X\) is chosen from the stored singular-value data, each \(P_a\) is defined as the positive operator \(\widehat X_a^\dagger \widehat X_a\).

Lemma 4.28

For each \(a\),

\[ X_a = T_a \cdot X. \]
Proof

Multiply the definition of \(X\) by \(T_a\) on the left and use that \(T_a\) selects exactly the basis vectors \(\lvert a,i \rangle \):

\[ T_a \cdot X = \Big(\sum _{i=1}^{m_a} \lvert a,i \rangle \langle a,i \rvert \Big) \Big(\sum _b \sum _{j=1}^{m_b} \lvert b,j \rangle \langle v_{b,j} \rvert \Big) = \sum _{i=1}^{m_a} \lvert a,i \rangle \langle v_{a,i} \rvert = X_a. \]

For each \(a\),

\begin{equation*} Q_a = X_a^\dagger \cdot X_a = X^\dagger \cdot T_a \cdot X = X_a^\dagger \cdot X. \end{equation*}
Proof

The identity \(X_a^\dagger X_a = Q_a\) follows by expanding the basis sums. The remaining equalities come from 4.28 and the projectivity of \(T\):

\[ X_a^\dagger \cdot X_a = (X^\dagger \cdot T_a)(T_a \cdot X) = X^\dagger \cdot T_a \cdot X = X_a^\dagger \cdot X. \]
Proof

Use that \(T\) is a measurement and then 4.29:

\[ X^\dagger \cdot X = \sum _a X^\dagger \cdot T_a \cdot X = \sum _a Q_a = Q. \]

The additional paper identities involving \(U,V,\Sigma \) are the usual SVD computations. The Lean development also records the spectral calculation which will identify the mixed positive-Gram-image product with \(\sqrt Q\): the positive eigenvalues give the nonzero columns, while the zero eigenspace has zero coefficient in the square-root expansion and is killed by \(X\). The conjugate right-eigenvector rows over the positive spectrum are also orthonormal. Equivalently, any row-space vector orthogonal to the positive Gram images is killed by \(X^\dagger \).

For each \(a\),

\begin{equation*} X_a^\dagger \cdot (X \cdot X^\dagger - I_{m \times m})^2 \cdot X_a = Q_a \cdot Q \cdot Q_a - Q_a. \end{equation*}
Proof

Expand the square and apply 4.30 and 4.29 term by term:

\[ X_a^\dagger (X \cdot X^\dagger \cdot X \cdot X^\dagger ) X_a = Q_a \cdot Q \cdot Q_a, \]

while

\[ X_a^\dagger (X \cdot X^\dagger ) X_a = (X_a^\dagger \cdot X)(X^\dagger \cdot X_a) = Q_a \cdot Q_a = Q_a, \]

and \(X_a^\dagger I_{m \times m} X_a = X_a^\dagger X_a = Q_a\). Substituting these identities into

\[ (X \cdot X^\dagger - I_{m \times m})^2 = X \cdot X^\dagger \cdot X \cdot X^\dagger - 2X \cdot X^\dagger + I_{m \times m} \]

gives the claim.

Lemma 4.32 \(P_a\) restated

For each \(a\),

\begin{equation*} P_a = \widehat{X}^\dagger \cdot T_a \cdot \widehat{X} = \widehat{X}_a^\dagger \cdot \widehat{X}. \end{equation*}
Proof

Since \(T\) is projective,

\[ P_a = \widehat{X}_a^\dagger \cdot \widehat{X}_a = (\widehat{X}^\dagger \cdot T_a)(T_a \cdot \widehat{X}) = \widehat{X}^\dagger \cdot T_a \cdot \widehat{X} = \widehat{X}_a^\dagger \cdot \widehat{X}. \]
Lemma 4.33 \(\widehat{X}\) squared
#
\begin{equation*} \widehat{X} \cdot \widehat{X}^\dagger = I_{m \times m}. \end{equation*}
Proof

The paper proves this by multiplying out \(\widehat{X}=U\cdot I_{m\times d}\cdot V^\dagger \) and using the unitarity of \(U\) and \(V\). In Lean, the dimension hypothesis \(m\leq d\) already gives a rectangular matrix with orthonormal rows on the sigma auxiliary space; the chosen matrix sigmaFinXHatCoisometry and its specification record this existence result as a hypothesis for the future construction. The formal lemma orthonormal_normalized_image_of_adjoint_comp_eigenvectors records the singular-vector normalization calculation, while normalized_matrix_image_rows_mul_conjTranspose combines the corresponding row-coisometry identity, and positive_gram_spectrum_image_rows_transpose_mixed records the adjoint action \(X^\dagger (\lambda ^{-1/2}Xv)=\lambda ^{1/2}v\) on the positive spectral part of the Gram operator. The formal lemma exists_unitaryGroup_with_positive_gram_spectrum_rows records the next finite-dimensional step: after choosing distinct row positions for the positive spectrum, these normalized image rows extend to a square unitary group element on the row space. The companion lemma exists_rectangular_coisometry_extending_orthonormal_rows records the analogous rectangular completion for prescribed right rows when the dimension bound permits it. The formal lemma unitaryGroup_mul_rectangular_coisometry and its right-multiplication companion rectangular_coisometry_mul_conjTranspose_unitaryGroup record the two unitary-preservation steps in the paper’s multiplication. The formal lemma rectangularSvd_xHat_coisometry_unitaryGroup applies these preservation steps to the rectangular-SVD expression. The unconditional positive-Gram route is exists_xHat_of_sigmaFinRangeEmbedding_positiveGram, which constructs \(\widehat X\) from the rank-reduction witness and proves \(\widehat X\widehat X^\dagger =I\) together with the mixed square-root identity below.

Lemma 4.34 \(X\) times \(\widehat{X}\)
#
\begin{equation*} X \cdot \widehat{X}^\dagger = U \cdot \Sigma _{m \times m} \cdot U^\dagger , \quad X^\dagger \cdot \widehat{X} = \sqrt{Q}. \end{equation*}
Proof

The paper obtains this from the SVD formula for \(X\) and the definition of \(\widehat X\). In Lean, the unconditional QXP data first proves that \(X\widehat X^\dagger \) is Hermitian and positive. The formal lemma x_mul_xHat_adjoint_spectral_theorem then applies Mathlib’s spectral theorem for Hermitian matrices, giving the displayed \(U\Sigma U^\dagger \) form with the Mathlib eigenvector unitary and the diagonal matrix of real eigenvalues. The auxiliary lemma rectangularSvd_x_mul_xHat_conjTranspose_raw records the same calculation under explicit rectangular-SVD data, where the middle factor \(S I_{m\times d}^\dagger \) is the formal square matrix \(\Sigma _{m\times m}\). The formal lemma rectangularSvd_xHat_mixed_of_sqrtQ_unitaryGroup records the second matrix calculation in the form whose square-root target is the operator \(Q\) supplied by the QXP construction. The formal lemma rectangularSvd_middle_eq_sqrt_of_square records the spectral step: a positive middle factor whose square is \(Q\) is the positive square root of \(Q\). The reduced datum then records this mixed-product identity as a primitive consequence, which is exactly the part needed in 4.36 and 4.38.

Remark 4.35 Lean status for the QXP algebra
#

The Lean declarations linked in Lemmas 4.30, 4.33, and 4.34 expose the corresponding matrix identities as construction theorems. These declarations prove the identities from the \(Q\)-layer, the sigma-range realization, and the positive-Gram spectral construction, with the rectangular-SVD calculation retained as an auxiliary comparison. Thus the local \(X/\widehat X/P\) algebra is formalized; the remaining chapter-level work is to compose this construction with the preceding orthonormalization step from the paper hypotheses.

Proof

The paper diagonalizes the positive operator \(X\widehat X^\dagger \) using the SVD notation. The formal proof avoids storing that SVD explicitly: set \(Y=X\widehat X^\dagger \). The primitive identities imply that \(Y\) is hermitian, nonnegative, and satisfies \(Y^2=XX^\dagger \). Hence \((X-\widehat X)(X-\widehat X)^\dagger =(Y-I)^2\), and positivity of \(Y\) gives \((Y-I)^2\leq (Y^2-I)^2=(XX^\dagger -I)^2\).

Proof

For outcomes \(a,b\),

\begin{align*} P_a \cdot P_b & = (\widehat{X}^\dagger \cdot T_a \cdot \widehat{X}) (\widehat{X}^\dagger \cdot T_b \cdot \widehat{X}) \\ & = \widehat{X}^\dagger \cdot T_a \cdot I_{m \times m} \cdot T_b \cdot \widehat{X} \\ & = \widehat{X}^\dagger \cdot T_a \cdot \widehat{X} \cdot \mathbf{1}\! \left[[\right]a=b] \\ & = P_a \cdot \mathbf{1}\! \left[[\right]a=b], \end{align*}

where the second line uses 4.33, the third uses that \(T\) is projective, and the last uses 4.32. Summing over \(a\) shows \(\sum _a P_a \leq I\), so \(P\) is a projective sub-measurement. The formalization also records the sharper identity

\[ \sum _a P_a=\widehat X^\dagger \widehat X, \]

and the resulting total-domination estimates used later in the monotone-total self-improvement route.

Proof

The formal proof follows this argument directly from the primitive \(X\), \(\widehat X\), and \(P\) identities; the \(30\zeta ^{1/4}\) estimate is derived here rather than stored as part of the reduced datum. The unitary-group rectangular-SVD lemma combines the same estimate with the positive-square identification of the middle factor from 4.34; the square unitary factors are again carried as elements of the relevant unitary groups. The positive-Gram sigma-space lemma also records the coisometry \(X X^\dagger =I\) for the original sigma embedding when the projective \(Q\)-family is subnormalized; this is the construction-level hypothesis later used to obtain the QXP-internal fresh-outcome comparison \(Q_{\mathrm{none}} \leq P_{\mathrm{none}}\). An additional source-to-\(Q\) comparison is still needed for source-facing residual domination. The quantity to bound is

\begin{equation} \label{eq:P-Q-thing-to-bound} \sum _a \langle \psi \rvert (Q_a-P_a)^2 \otimes I \lvert \psi \rangle = \langle \psi \rvert Q \otimes I \lvert \psi \rangle + \langle \psi \rvert P \otimes I \lvert \psi \rangle - \sum _a \langle \psi \rvert Q_aP_a \otimes I \lvert \psi \rangle - \sum _a \langle \psi \rvert P_aQ_a \otimes I \lvert \psi \rangle , \end{equation}
11

using the projectivity of \(Q\) and \(P\). The first term is at most \(1+2\sqrt{\zeta }\) by 4.20, and the second is at most \(1\) because \(P\) is a sub-measurement.

For the last two terms,

\begin{equation} \label{eq:complex-conjugates} \sum _a \langle \psi \rvert Q_aP_a \otimes I \lvert \psi \rangle + \sum _a \langle \psi \rvert P_aQ_a \otimes I \lvert \psi \rangle = 2 \cdot \mathfrak {R}\Big(\sum _a \langle \psi \rvert Q_aP_a \otimes I \lvert \psi \rangle \Big). \end{equation}
12

By 4.29,

\[ \sum _a \langle \psi \rvert Q_aP_a \otimes I \lvert \psi \rangle = \sum _a \langle \psi \rvert (X_a^\dagger \cdot X \cdot P_a) \otimes I \lvert \psi \rangle . \]

The main estimate is

\begin{equation} \label{eq:add-a-hat} \sum _a \langle \psi \rvert (X_a^\dagger \cdot X \cdot P_a)\otimes I \lvert \psi \rangle \approx _{2\zeta ^{1/4}} \sum _a \langle \psi \rvert (X_a^\dagger \cdot \widehat{X} \cdot P_a)\otimes I \lvert \psi \rangle . \end{equation}
13

This follows by Cauchy–Schwarz:

\[ \Big|\sum _a \langle \psi \rvert ((X_a^\dagger \cdot (X-\widehat X)) \otimes I)\cdot (P_a \otimes I)\lvert \psi \rangle \Big| \]

is bounded by the square root of

\[ \sum _a \langle \psi \rvert \big(X_a^\dagger \cdot (X-\widehat X)(X-\widehat X)^\dagger \cdot X_a\big)\otimes I \lvert \psi \rangle , \]

times the square root of \(\sum _a \langle \psi \rvert (P_a)^2 \otimes I \lvert \psi \rangle \leq 1\). The first factor is at most \(4\sqrt{\zeta }\) by 4.36, 4.31, and 4.23, so the total error is at most \(2\zeta ^{1/4}\).

The right-hand side of 13 is real, because

\[ \sum _a \langle \psi \rvert (X_a^\dagger \cdot \widehat{X} \cdot P_a)\otimes I \lvert \psi \rangle = \langle \psi \rvert (X^\dagger \cdot \widehat{X}) \otimes I \lvert \psi \rangle = \langle \psi \rvert \sqrt{Q} \otimes I \lvert \psi \rangle , \]

where the first equality uses 4.28, 4.32, and 4.33 and that \(T\) is a measurement, and the second uses 4.34. Hence 4.22 and 13 imply

\[ \mathfrak {R}\Big(\sum _a \langle \psi \rvert Q_aP_a \otimes I \lvert \psi \rangle \Big) \geq 1-14\zeta ^{1/4}. \]

Substituting this into 12 and then into 11 gives

\[ \sum _a \langle \psi \rvert (Q_a-P_a)^2 \otimes I \lvert \psi \rangle \leq (1+2\sqrt{\zeta }) + 1 - 2(1-14\zeta ^{1/4}) = 2\sqrt{\zeta } + 28\zeta ^{1/4} \leq 30\zeta ^{1/4}. \]

Finally, 4.20 gives

\[ A_a \otimes I \approx _{12\sqrt{\zeta }} Q_a \otimes I, \]

and 4.38 gives

\[ Q_a \otimes I \approx _{30\zeta ^{1/4}} P_a \otimes I. \]

The triangle inequality for \(\approx _\delta \) yields

\[ A_a \otimes I \approx _{84\zeta ^{1/4}} P_a \otimes I. \]