Balancing Kraus families and unitary couplings
Written by GPT-6.1 Sol (OpenAI), Ultra, October 2026. Self-checked by the writing AI. New original text: public domain (CC0).
A unital Kraus family has . To turn its reconstruction map into an approximate unitary intertwiner, we also need . We will average the second sum, scale down slightly, and fill both remaining defects exactly. The repaired map changes arbitrarily little on the matrix algebra being modeled.
The inputs are the trace-preserving finite models, the internal matrix Kraus formula, and canonical center-valued trace and projection comparison. The central trace cuts provide projections of arbitrary prescribed scalar trace in a factor. General tracial expectations retain the exact OA-MOD prerequisite used earlier. We prove the norm-averaging step here.
1. Filling two positive defects
Let be a finite von Neumann algebra with a faithful normal tracial state , and let be its canonical center-valued trace. Separability and factoriality are unnecessary in this section.
Lemma 1.1. If and , there is a finite or countable family such that
with strong convergence of the positive sums.
Proof. First suppose . Some nonzero spectral projection satisfies for . Put , its central support. Then , so . Choose a nonzero spectral projection with , . There are nonzero equivalent subprojections of and : otherwise , which would force to be orthogonal to the central support of . The polar decomposition of a nonzero element of gives a partial isometry with , . Thus
Take a maximal collection of nonzero operators for which every finite sum of their 's is at most , and every finite sum of their 's is at most . A chain has its union as an upper bound, so Zorn's lemma applies. This collection is countable: all , while the finite sums are bounded by . For each positive integer , only finitely many members can have trace at least , and these finite sets exhaust the collection.
The positive partial sums have strong limits , . Normality and traciality of give
If the first remainder is nonzero, (2) supplies an operator that can be appended. Multiplying it by a scalar in , if necessary, gives a new member distinct from every member of the countable collection, preserving both bounds. This contradicts maximality. Thus . Equation (3) and faithfulness of give . If initially, faithfulness also gives , and the empty family suffices.
2. Simultaneous averaging in operator norm
Lemma 2.1. Let be a factor with its normalized trace. For any finite list and , there is a finite convex combination of unitary conjugations
such that for every . No separable-predual hypothesis is needed.
Proof. First take one self-adjoint . Uniform spectral approximation gives , with a projection partition and . For a large integer , put
Cut of trace and split it into projections of trace . The residual projection has trace ; split it into such projections. Zero ranks require no projections. Together these give equivalent projections summing to , hence a full matrix system in . Its cyclic permutation unitary defines
The projection commutes with . Write . Since , positivity of gives . Its scalar trace has the same absolute bound. Consequently
First choose , then , to make this as small as desired.
For several self-adjoint elements, apply this one-element result successively to the current image of the next element. Every averaging map fixes scalars, preserves trace and is contractive; thus it preserves the error bounds already obtained. A finite composition of maps (4) is again a finite convex combination of unitary conjugations, by expanding the products of their unitaries and weights. For complex elements, include their real and imaginary parts with half the requested error. This proves the simultaneous assertion.
The residual projection in (5) records the dimension lost by rounding. Its cyclic average has norm , which is the reason this argument proves operator-norm approximation rather than only a trace-norm estimate.
A second proof by spectral contraction
There is a second proof that uses spectral contraction rather than rounding projection dimensions. It also works in every finite factor, including a matrix algebra. For a nonscalar self-adjoint , write , , and . Its spectral projection satisfies . Factor projection comparison puts either or below an equivalent subprojection of the other. First suppose . Choose with , , and set
The orthogonal initial and final projections show that is a self-adjoint unitary interchanging . Functional calculus gives . Conjugating this lower bound by and adding gives
The upper bound is . Thus
If , apply the same calculation to with lower projection , endpoints , and midpoint . The inequalities and give the same diameter bound. This uses the original complementary projection, so eigenvalues exactly at the midpoint cause no ambiguity.
Repeat the construction on the current averaged operator. After steps its spectral diameter is at most ; if an intermediate operator is scalar, stop. Each step preserves trace and is a convex average of two unitary conjugations. Their composite is a finite convex average of unitary conjugations. The number lies between the minimum and maximum of its spectrum, so
This proves the one-element assertion without choosing rational projection dimensions. For a finite list, average the current real and imaginary parts successively, using half the requested tolerance for each part. Trace preservation and contractivity keep every previous bound, and composition remains a finite convex average. This proves the same simultaneous conclusion as Lemma 2.1. The spectral-contraction method is developed in Anantharaman–Popa, Section 6.4.
3. Balanced reconstruction on a matrix subfactor
Theorem 3.1. Let be a factor, let be a unital copy of , and let be ucp with . For every , there is a finite or countable family such that
The sums of positive operators converge strongly. The family defines a normal trace-preserving ucp map on all of .
Proof. The internal Kraus lemma gives operators such that
Put . The trace-preserving expectation satisfies, for every ,
Nondegeneracy of the trace pairing on gives .
Matrix coordinates identify with , where is a factor. The product normalized trace is the ambient trace. Write , with . Equation (10) says . Lemma 2.1 gives one averaging map on bringing every coefficient within of its scalar trace. Its unitaries commute with . Replacing the family in (9) by
leaves unchanged and leaves the first positive sum equal to . Its second sum satisfies
Choose and then . Relabel the finite family as and put for . Its two sums are
The positive residuals
have equal scalar traces. In a factor this is equality of center-valued traces. Lemma 1.1 fills them with operators .
Let . For , its partial sums increase and are bounded by , so they converge strongly. Linear combinations of positive elements define the map for every ; the same argument at each matrix level gives complete positivity. Increasing positive nets can be interchanged with these positive sums in each normal positive functional, proving normality. Its norm is . On , the completed map is , so its distance from is at most .
The completed map on is ucp by its first sum. For , normality and traciality give . Thus it preserves trace by its second sum. This proves every assertion.
Factoriality is used in (14): scalar trace equality suffices there because the center is scalar. Lemma 1.1 itself retains the full nonfactor center-valued condition.
4. Approximation becomes a unitary coupling
Call two -tuples of unitaries , in a faithfully tracial finite algebra -related if a countable family satisfies
Proposition 4.1. For a family with the two balanced sums, put . Then
for any two unitaries .
Proof. Expand the squared norms of finite partial sums. The two positive terms tend to each, because , and the cross term converges to the displayed trace pairing. Strong convergence of the cp series and normality of justify that limit. Since , the middle expression equals . Cauchy–Schwarz gives its upper bound in (16).
Corollary 4.2. In an injective factor, every finite tuple is -related to a tuple of unitaries in some unital matrix subfactor, for every .
Proof. The preceding lesson gives a trace-preserving ucp reconstruction from with unitary input models. Projection cuts and comparison embed unitally as a subfactor , preserving its normalized trace. Choose its reconstruction errors below . Apply Theorem 3.1 with operator-norm map error below . On each unitary model the two errors add to less than in -norm. Equation (16) proves (15).
5. Problems with complete solutions
Exercise 1. Why is scalar trace equality insufficient for Lemma 1.1 off factors?
Solution. In with its equal-weight faithful trace, take and . They have the same scalar trace. However every has coordinate by coordinate, so the two sums in (1) must be identical. Here the center-valued trace is the identity and the necessary equality fails.
Exercise 2. Prove the countability assertion used in the maximal-family argument.
Solution. If each of distinct positive numbers is at least , their finite sum is at least . The bound by therefore limits their number to . Every positive number is at least for some positive integer . Thus the nonzero family is a countable union of finite sets.
Exercise 3. Compute the rounding loss in (5) for a projection partition of traces and .
Solution. Each , so . Each residual piece has trace ; their sum has trace . Split that sum into two projections of trace . These complete the eight equivalent diagonal projections, even though the individual residual traces are not multiples of .
Exercise 4. Why does later averaging preserve earlier scalar approximation errors?
Solution. Any convex combination of unitary conjugations fixes and is norm contractive. If , its image satisfies . Trace preservation ensures that the desired scalar for each next image is still the trace of the original element.
Exercise 5. Explain the direction of multiplication in (11).
Solution. The unitary multiplies on the left. Then for , because . The first sum is unchanged, while the second becomes , which is precisely the sum that needs averaging.
Exercise 6. Verify positivity and trace equality of the defects (14).
Solution. The bound implies . Also . Traciality and the first sum give . Hence .
Exercise 7. Why does the tail map in Theorem 3.1 have norm exactly ?
Solution. Its positive series is cp and sends to . For a cp map on a unital algebra, its operator norm is the norm of its value at , as proved in the finite CP preparation. Thus . The equality also follows by evaluating the norm at the unit, after the cp upper bound is established.
Exercise 8. Give a balanced family in defining the depolarizing map.
Solution. Take , for . Both and equal . Moreover . This checks both balance conventions and the reconstruction orientation.
Exercise 9. For that family, take . Compute the coupling energy.
Solution. The diagonal terms commute with and contribute zero. Each off-diagonal term has commutator , whose normalized squared -norm is . Their total energy is . Equation (16) gives the same result because , so .
Exercise 10. Show that the relation in (15) is symmetric.
Solution. Replace each by . The two balanced sums exchange roles. The adjoint of is . Multiplying this on the left by and on the right by gives . Unitary multiplication and adjoints preserve the tracial -norm, so every coupling energy is unchanged.
References and proof scope
Uffe Haagerup, A new proof of the equivalence of injectivity and hyperfiniteness for factors on a separable Hilbert space, Journal of Functional Analysis 62 (1985), 160–201. Lemma 5.1 and Proposition 5.2 give the defect-filling and balanced reconstruction method. The two-defect lemma here retains nonfactor center-valued traces and a faithful normal tracial state; scalar trace equality is used only in the factor application. The balanced reconstruction theorem and its injective application retain the factor hypothesis, without separability.
Claire Anantharaman and Sorin Popa, An introduction to II₁ factors, author draft, Theorem 6.4.1 and Corollary 6.4.2. Section 2 above supplies both a finite-cut averaging proof and a complete spectral-contraction proof of the required simultaneous operator-norm averaging. The next lesson turns small coupling energy into a single unitary conjugation.