Gluing two manifolds and
with a common boundary
yields a closed manifold
. Extending to formal
linear combinations yields
a sesquilinear pairing
with values in (formal linear combinations of) closed manifolds.
Topological quantum field theory (TQFT) represents this universal pairing
onto a finite dimensional
quotient pairing
with values in
which in physically motivated cases is positive definite. To see
if such a “unitary" TQFT can potentially detect any nontrivial
, we ask if
whenever
. If this is the case,
we call the pairing
positive. The question arises for each dimension
. We find
positive
for and
and not positive
for . We
conjecture that
is also positive. Similar questions may be phrased for (manifold, submanifold)
pairs and manifolds with other additional structure. The results in
dimension 4 imply that unitary TQFTs cannot distinguish homotopy
equivalent simply connected 4–manifolds, nor can they distinguish smoothly
–cobordant
4–manifolds. This may illuminate the difficulties that have been met
by several authors in their attempts to formulate unitary TQFTs for
.
There is a further physical implication of this paper. Whereas 3–dimensional
Chern–Simons theory appears to be well-encoded within 2–dimensional quantum
physics, e.g. in the fractional quantum Hall effect, Donaldson–Seiberg–Witten theory
cannot be captured by a 3–dimensional quantum system. The positivity of the
physical Hilbert spaces means they cannot see null vectors of the universal pairing;
such vectors must map to zero.