Most accounts of the Kadison-Singer problem mention that it arose from considerations in the foundations of quantum mechanics. Specifically, a question about “extensions of pure states.” See, for instance, Gil’s blog. But trying to reconcile this question with my (limited) knowledge of QM proved frustrating. There is also an intuitive explanation posted at soulphysics, along with mathematical notes. But I couldn’t figure that one out either, because it only deals with “normal” quantum states (those corresponding to countably additive measures; see below). I think the KS problem for normal states is trivial. For the meat of KS, one has to think not only about infinite-dimensional spaces, but about “pathological” (non-constructible) measures. In particular, one has to think about “quantum states” that don’t have density matrices.

What follows are my notes on the matter, all of which are either well-known or wrong. Skip to the end for the very simple formulation with no mention of quantum states. Even better advice is to just Read Nick Harvey’s survey.

** How I understand quantum measurement **

A (mixed) quantum state on the space is an Hermatian matrix satisfying ( is positive semi-definite) and . Suppose we also have a resolution of the identity: A collection of PSD matrices with . Then when we perform the measurement , the probability of obtaining outcome is for .

A *pure state* is given by a density matrix of the form for some . Equivalently, a state is pure if and only if it cannot be written as a non-trivial convex combination of other states, i.e. if for , then . The pure states are the extreme points of the convex set of all states.

** Quantum logic **

There is another way to think about quantum measurement. Let be a (separable) Hilbert space and consider a projection onto some closed subspace. A *measure on projections* assigns to every such projection a value in . We say that is *-additive* if whenever and the projections are mutually orthogonal, we have . If this only holds for finite sums of projections, we say that is *finitely additive.* We should also have .

Note that we have allowed here the possibility that is infinite-dimensional. In the case where the measure is -additive, it is completely specified by its value at one-dimensional projections, i.e. the values where denotes projection onto . Now we can state Gleason’s theorem: Our two notions of quantum measurement coincide.

Theorem 1Let be a Hilbert space of dimension at least 3 and let be a -additive measure on projections. Then there exists a unique linear operator such that for any projection , we have .

In other words, every -additive measure on projections arises from a mixed state.

** Restricted purity **

Note that a measure on projections corresponds to a pure state if and only if it cannot be written as a non-trivial convex combination of measures on projections. In this way, we can also define purity with respect to a restricted family of projections.

Consider, for example, the Hilbert space of complex sequences, and let denote the standard basis. Suppose we consider only the projections onto each of the basis elements. Say that a *-measure* is a measure on all projections of the form for . Such a measure only gives us probabilities for measurements performed in the standard basis. (The algebra generated by is a canonical example of a “maximal abelian subalgebra,” i.e. MASA.) We can say that a -measure is *pure* if it cannot be written as a non-trivial convex combination of other -measures. What are the pure -measures? Well, the only -additive pure -measures are the point measures for some . If for , then by -additivity, we can split into a convex combination of two measures (one supported only on and the other supported off ).

But when -additivity is dropped, some tricky things can happen (see the next section). It turns out that, in this case, there are more pure states than just (in fact, the cardinality of the finitely-additive pure states is gigantic, ). Now we are in position to state the Kadison-Singer problem.

**Kadison-Singer Problem:** Is it the case that every pure, finitely-additive -measure has a unique extension to a finitely-additive measure on all the projections of ?

The answer is clearly positive for -additive measures (in which case the unique extension corresponds to ). The answer is also positive for finitely-additive -measures, as recently proved by Marcus, Spielman, and Srivistava.

In their original work, Kadison and Singer showed that the answer is false if one constructs the MASA using the continuous Hilbert space instead of . One can take the subalgebra of multiplication operators for . Here the corresponding family of projections are the maps for . Unlike in the case above, this subalgebra is not “discrete.” It turns out that every maximal abelian subalgebra of bounded operators on a separable Hilbert space is either finite-dimensional, the discrete one, the continuous one, or a direct sum of algebras isomorphic to these.

Note that states corresponding to finitely additive (but not -additive measures) do not have density matrices and are often considered to be “unphysical” because they would take an infinite amount of energy to prepare.

** A -world teeming with pure states **

In the above setting, we said there are finitely-additive pure -measures other than point measures. To see what one of these must look like, consider the following construction. Let denote the projection onto and define similarly. Define the measures and . Then we can write . This is a non-trivial convex combination unless either or .

Indeed, for every partition , a pure -measure can only put non-zero weight on projections involving coordinates of exactly one of or . Furthermore, if then . In other words, for every set of projections, the measure takes only values 0 or 1. Such finitely-additive measures are exactly given by ultrafilters on . The finitely-additive pure -measures are in one-to-one correspondence with such ultrafilters, the set of which can be identified with , the Stone-Cech compactification of the naturals. See Terry Tao’s notes on ultafilters and Stone-Cech compactification.

Take the Hilbert space with standard basis , and let denote the set of all its closed subspaces. Consider a map . We say that is a *finitely-additive measure* if and whenever is a finite collection of mutually orthogonal subspaces, we have . Say that such a measure is *pure* if it cannot be written as a non-trivial convex combination of two finitely-additive measures. A canonical example of a pure measure involves fixing a unit vector and setting where denotes the orthogonal projection onto .

Now let be the set of all the subspaces of of the form for some subset , i.e. all the coordinate subspaces. We can define “finitely-additive” and “pure” for measures on in the analogous way.

**Kadison-Singer problem:** Can every finitely-additive pure measure on be extended uniquely to a finitely-additive measure on ?

Note that the real question is about uniqueness of the extension. There always exists a pure extension; see the comments.

Am I missing something or is your canonical example of a pure measure never finitely additive? If we take two orthogonal vectors u and v such that x = u + v then mu(span(u)) = mu(span(v)) = 0 but mu(span(u, v)) = 1.

Yeah, you’re right. What I wrote didn’t make any sense at all. I changed the text to what I had intended.

I think a similar problem also breaks your canonical pure extension: Let u = e_1 + e_2 and v = e_1 – e_2. Then mu^(span(u)) = mu^(span(v)) = 0 because there are no basis vectors in there, but mu^(span(u, v)) = mu^(span(e_1, e_2)) = mu(span(e_1, e_2)) which is not necessarily zero.

Agreed. I think an attempt to do it correctly actually reveals the relationship to “paving conjectures.” Let be a pure measure on . Consider a subspace and and the associated orthogonal projection . Also take a partition of the interval . Let . Finally, define

.

By properties of ultrafilters, for every n, the sum inside the limit only has one non-zero term.

In other words, where is the ultrafilter defining .

Good article