True. The Künneth theorem gives the Poincaré polynomial
so and . The proposed equality also gives . Even if compactness was not stated separately, these two numbers force the putative eight-manifold to be connected and compact: the top ordinary real cohomology of a connected noncompact manifold is zero.
The auxiliary Hard Lefschetz theorem on de Rham cohomology says that, on a compact Kähler manifold of complex dimension , is an isomorphism, where . Here , so is injective. If , then and therefore . Thus is injective, forcing . The inequality is impossible. Hence these Betti numbers cannot occur for a Kähler eight-manifold.
Here projection means Hermitian orthogonal projection: with , as indicated by the unitary conjugation in the question. These matrices represent the complex Grassmannian as orthogonal projections, a compact manifold of complex dimension . The constants are real. Let and use the given tangent directions . Cyclicity of the matrix trace gives
The commutator is skew-Hermitian. If this derivative vanishes for every skew-Hermitian , choose to obtain
so . Conversely makes every tangent derivative zero. Because the diagonal entries of are distinct, a commuting matrix is diagonal. Its idempotent entries are zero or one. Thus the critical projections are exactly
with critical points and values .
To compute the Hessian matrix, write and . A neighboring plane is the graph of a complex linear map . With , its orthogonal projection is . Writing for the diagonal blocks, we get
Expanding yields
Each complex coordinate has two real components, each with Hessian coefficient . Every coefficient is nonzero, proving that is a Morse function. Its negative directions correspond to . For there are complementary indices below , giving
This is the diagonal trace Morse function on a complex Grassmannian. Its critical values need not be distinct; ties between sums do not make its critical points degenerate.
All Morse indices are even. Choose a Morse-Smale gradient flow and form its integral Morse chain complex. The odd-degree chain groups vanish, so every differential vanishes. Equivalently the Morse handle-attachment theorem supplies only even-dimensional cells. The integral homology of complex Grassmannians is therefore
where counts the subsets with , and . In particular there is no torsion. The nondecreasing sequence lies between zero and , so reversing it identifies these subsets with partitions of an integer fitting in a by rectangle. The Poincaré polynomial is explicitly
For the permitted example , the subsets have indices . Thus
The general calculation above applies throughout ; it does not reduce to any of the excluded rank-one cases.
All cohomology below has rational coefficients. First describe the incidence space geometrically. The image of is , inside . For a line , choosing a plane containing is equivalent to choosing the line in . If is the tautological line bundle on , then
This is the projective bundle of a rank-three quotient bundle, with fibre . Local frames of the quotient bundle give local product charts. In particular is an oriented real six-dimensional manifold.
For , the intersection is exactly a line, so is a single point and the inverse map is . The intersection line varies continuously, indeed holomorphically, wherever its dimension is constant: in local Grassmannian charts it is the kernel of a matrix of constant rank, whose kernel bases can be chosen locally. Thus is an isomorphism over the open stratum. At the remaining point,
Set , a derived direct image of sheaves. The proper base change for sheaves theorem identifies its derived stalks with the cohomology complexes of the fibres. Consequently is the constant rational sheaf in degree zero on , and
The cohomology sheaves are therefore finite-rank local systems on the two strata, with no other nonzero degrees. This proves that is a constructible complex of sheaves and verifies normalization. The open stratum has real dimension six, so the isolated point has codimension six. Its middle perversity is , and the intersection-complex support and cosupport axioms require stalk vanishing in degrees above two. The fibre calculation verifies the support axiom, as well as vanishing in negative degrees.
For an oriented real six-dimensional manifold, Verdier duality gives . For a proper map, Verdier duality commutes with derived direct image. Applying these statements here yields
The duality identity converts this into
Here is the costalk, and dualization of rational complexes reverses degrees. Thus its only nonzero groups are in degrees four and six. In particular they vanish for , which is precisely the cosupport axiom at this isolated six-dimensional singularity. The uniqueness characterization by constructibility, normalization, support and cosupport now identifies with the unshifted intersection complex of . Taking hypercohomology, and using the composition of derived global sections with , gives
Finally apply the fibration result allowed in the question to . Its base is the simply connected complex projective line, its fibre is the Complex projective plane, and the projective-bundle charts above verify the fibration hypothesis. Hence, as graded rational vector spaces,
The resulting Betti numbers and Poincaré polynomial are
This uses with . No assertion that an arbitrary projective fibration has the product cohomology ring is needed.
The usual compact closed-manifold hypothesis is needed for the first assertion, or a proper bounded-below Morse exhaustion in an appropriate noncompact version. As literally printed without any such condition, on is a Morse function with no critical points, while . We prove the intended closed-manifold statement, which applies to the surface product later in the question.
By the Morse handle-attachment theorem, crossing an index- critical point attaches an -handle, and no topological change occurs between critical levels. Retraction to the core disks of handles gives a CW complex model with cells in dimension . Its cellular chain complex has . Tensor with , which computes the ranks of integral homology. Since homology is a quotient of a vector subspace of , . This argument has not used the Morse inequalities.
The strong Morse inequalities and top-dimensional equality are
Their weak form is . To see the algebra behind the strong form, put in the Morse chain complex, with . The kernel-image dimensions give , so the alternating difference at is exactly . Conversely, given the strong inequalities, denote those alternating differences by , with . Then , proving that they imply every weak inequality.
They are not equivalent as numerical restrictions. For the Betti numbers of , the formal counts satisfy all weak inequalities and the Euler equality, but at give . They therefore cannot be the counts of a Morse function on ; the strong inequalities detect that additional obstruction.
If all the strong inequalities are equalities, all vanish and . An integer boundary matrix with rational rank zero is the zero matrix. Thus the integral complex itself has zero differential, not merely its rationalization. Consequently
and higher homology vanishes. In particular there is no homology torsion. This is an integral consequence of a Perfect Morse function, rather than just an assertion about ranks.
For , the integral homology is free with Betti numbers . The Künneth theorem therefore has no torsion terms, and the product's Poincaré polynomial is
Summing the weak inequalities yields the lower bound
Choose a surface Morse function with one minimum, saddles and one maximum. It can be built from one closed disk, the standard one-handles, and a closing closed disk, using the local forms , , and at the handle centres. Regular collars interpolate between the handles without new critical points. Now set . Its critical points are the ordered pairs of those of , and its Hessian matrix is a block direct sum; the indices add. This product of Morse functions has exactly critical points and realizes every displayed Betti count. Small bumps constant near the critical pairs can separate their values without altering the Hessians or creating new critical points.
The same minimum does not apply to arbitrary smooth functions. Here is an explicit finite-critical-point counterexample, avoiding any assumption that degeneracy leaves the Morse lower bound intact. On , take
It is well defined because shifting either coordinate by reverses two of its factors. Its derivatives are and . If either or vanishes, both derivatives vanish only at . Otherwise and must be multiples of , giving exactly and in addition to the origin. At the first point the Hessian is , positive definite; at the second it is its negative. They are a minimum and maximum. The origin is an isolated degenerate monkey saddle, with leading term . Thus this three-critical-point function on a torus has exactly three critical points.
For , perform connected-sum gluing of functions between this torus and a perfect Morse surface of genus : delete a small neighbourhood of the torus maximum and of the other surface's minimum, and join their regular boundary circles by a monotone cylinder. Collar coordinates ensure nonzero differential throughout the neck, so precisely those two critical points are lost and none are added. The result on has critical points, retaining the degenerate point. For , simply use . Calling this smooth function and the earlier perfect Morse function , the smooth product has
critical points. This explicitly proves the negative answer to the unrestricted smooth-minimum question; it does not assert that this smaller illustrative count is sharp.
Figure 1.
The explicit three-critical-point torus function and the local merger of two Morse saddles into one degenerate saddle
. Details.