1 Introduction
In [Reference Goresky, Kottwitz and MacPhersonGKM98], Goresky, Kottwitz, and MacPherson introduced the notion of an equivariantly formal space. Let G be a compact, connected Lie group,
$T \subset G$
a maximal torus and R a commutative ring. A G-space M is called equivariantly formal over R if the Leray spectral sequence
degenerates. The main examples of equivariantly formal spaces (c.f. [Reference Goresky, Kottwitz and MacPhersonGKM98, §14.1]) arise from the following celebrated result of Atiyah–Bott–Kirwan ([Reference Atiyah and BottAB84, §7], [Reference KirwanKir84, §5]):
Theorem 1.1. Let
$(M,\omega )$
be a compact symplectic manifold equipped with a Hamiltonian G-action. Then M is equivariantly formal over any
$\mathbb {Q}$
-algebra R.
The proof of Theorem 1.1 easily reduces to the case
$G=T$
via taking Weyl invariants. In the torus-equivariant case, the idea is to argue that the moment map for a generic one-parameter subgroup of T is equivariantly perfect. Theorem 1.1 naturally leads one to ask what happens with integral coefficients. The proof of this claim in these classical references relies on the so-called Atiyah–Bott lemma ([Reference Atiyah and BottAB83, Proposition 13.4],[Reference KirwanKir84, Lemma 2.18]), whose proof may fail when
$R=\mathbb {Z}$
(or even
$R=\mathbb {F}_p)$
and the cohomology of the critical sets have torsion (see, e.g., [Reference Atiyah and BottAB83, §13], [Reference Harada and LandweberHL07, Remark 2.4], [Reference Tolman and WeitsmanTW99, §4]). The main result of this note is a somewhat surprising generalization of Theorem 1.1 to any complex-oriented cohomology theory
$\mathbb {E}^*$
, including integral cohomology as a special case. To state it, we setFootnote
1
:
Theorem 1.2. Let
$(M,\omega )$
be a compact symplectic manifold with Hamiltonian G-action.
-
(1) Suppose G is a product of unitary groups. For any complex oriented cohomology theory $\mathbb {E}^*$
, the Leray spectral sequence (1.2) $$ \begin{align} H^p(BG;\mathbb{E}^q(M))=> \mathbb{E}_G^{p+q}(M) \end{align} $$degenerates. Moreover, there is a splitting:
(1.3) $$ \begin{align} \mathbb{E}^*_G(M) \cong \mathbb{E}^*(M \times BG) \end{align} $$of $\mathbb {E}^*(BG)$
modules.
-
(2) For general G, suppose that $\mathbb {E}^*(pt)$
is an algebra over a field
$\mathbf {k}$
for which the natural map (1.4) $$ \begin{align} H^*(BG;\mathbf{k}) \to H^*(BT;\mathbf{k}) \end{align} $$is injective. Then the Leray spectral sequence (1.2) degenerates.
Specializing to the case of classical cohomology implies the following result, which already appears to be new:
Theorem 1.3. Let
$(M,\omega )$
be a compact symplectic manifold with Hamiltonian G-action.
-
(1) If G is a product of unitary groups, then M is equivariantly formal over any commutative ring R. In fact, there is a (noncanonical) isomorphism of $H^*(BG;R)$
-modules (1.5) $$ \begin{align} H_G^*(M;R) \cong H^*(M;R)\otimes_R H_G^*(pt;R). \end{align} $$
-
(2) For general G, let $\mathbf {k}$
be a field such that the natural map (1.4) is injective and let R be any
$\mathbf {k}$
-algebra. Then M is equivariantly formal over
$R.$
Remark 1.4. As far as the authors know, for
$R = \mathbb {Z}$
, the sharpest known results in the literature along the lines of Theorem 1.3 (1) for a general Hamiltonian G-manifold M were:
-
○ the short exact sequence (not proven to be split) for cohomology groups in degree $2$
(cf. [Reference Harada and LandweberHL07, Theorem A.3]) (1.6) $$ \begin{align} 0 \longrightarrow H^2_{G}(pt;\mathbb{Z}) \otimes_{\mathbb{Z}} H^0(M;\mathbb{Z}) \longrightarrow H^2_G(M;\mathbb{Z}) \longrightarrow H^2(M;\mathbb{Z}) \longrightarrow 0. \end{align} $$
-
○ for G a torus, equivariant formality over $\mathbb {Z}$
was known when all the isotropy groups are connected (cf. [Reference Franz and PuppeFP07, Theorem 5.1]).
Remark 1.5. When R is not a field, the splitting from (1.5) does not follow from equivariant formality; see [Reference Franz and PuppeFP07, Example 5.2] for a simple example of a space which is equivariantly formal but for which no splitting of this form exists.
Remark 1.6. For semi-simple Lie groups, Theorem 1.3 (2) is sharp in the following sense. The cohomology
$H^*(BT,\mathbf {k})$
is isomorphic to
$H_G^*(G/T,\mathbf {k})$
, where G acts by left-translation. This action is Hamiltonian for an appropriate symplectic form on the flag manifold
$G/T$
, and so if (1.4) is not injective,
$G/T$
is not equivariantly formal over
$\mathbf {k}.$
Remark 1.7. The map (1.4) can only fail to be injective in prime characteristics p where
$H^*(BG,\mathbb {Z})$
contains p-torsion. This set of ‘torsion primes’ has been completely determined for any compact Lie group by [Reference BorelBor61] (see [Reference TotaroTot05] for a concise summary of Borel’s result and [Reference TodaTod87, Theorem 2.1] for classical groups). For classical groups, we have that:
-
○ if $G=U(n),SU(n),$
or
$Sp(2n)$
, then Theorem 1.3 (2) holds over any field
$\mathbf {k}$
. -
○ If $G=SO(n)$
, then the result holds for any field
$\mathbf {k}$
with
$\mathrm {char}(\mathbf {k}) \neq 2.$
Theorem 1.3 may be unexpected as many of the other well-known consequences of the Atiyah–Bott lemma are known to fail with integral coefficients (or finite field coefficients).Footnote
2
For example, it is easy to construct examples of Hamiltonian T-manifolds M for which the restriction to the fixed point locus
$j^*: H_T^*(M,\mathbb {Z}) \to H_T^*(M^{T},\mathbb {Z})$
fails to be injective.
Instead, we deduce Theorem 1.2 from a more general result in symplectic topology. Recall that a locally trivial fiber bundle
$M \to P \to B$
with fiber a closed symplectic manifold
$(M,\omega )$
is said to be Hamiltonian if its structure group can be reduced to the group of Hamiltonian symplectomorphisms
$\mathrm {Ham}(M,\omega )$
. We prove the following cohomological splitting result for Hamiltonian fibrations:
Proposition 1.8. Let
$M \to P \to B$
be a Hamiltonian fibration over a base B which is a product of complex Grassmannians. Then there is a noncanonical isomorphism of
$\mathbb {E}^*(B)$
modules
The case where
$B=\mathbb {CP}^1$
is an important recent result of Abouzaid–McLean–Smith [Reference Abouzaid, McLean and SmithAMS21] (see also [Reference Bai and XuBX22] for a more direct argument in the case of integral cohomology, and [Reference Abouzaid and BaiAB24] for an alternative proof in the general case). Their argument is based on ‘hard’ pseudo-holomorphic curve methods first introduced by [Reference Lalonde, McDuff and PolterovichLMP99]. We are able to formally ‘bootstrap’ this result to prove Proposition 1.8 by sharpening the ‘soft’ topological approach to cohomological splitting of Hamiltonian fibrations by Lalonde–McDuff [Reference Lalonde and McDuffLM03].
Remark 1.9. In the introduction to their paper [Reference Abouzaid, McLean and SmithAMS21], the authors suggest that one could use the arguments of [Reference Lalonde and McDuffLM03] to prove Proposition 1.8 for B a product of projective spaces and cohomology with coefficients in any field. The goal of this note is to carry out and considerably generalize this idea (by establishing cohomological splitting for Hamiltonian fibrations over more general B and with coefficients in any complex-oriented cohomology theory) as well as to make the connection to classical concepts in equivariant symplectic geometry.
To finish this note, we include two applications of our equivariant formality result. Our applications both concern a class of cohomology theories studied by Hopkins–Kuhn–Ravenel in [Reference Hopkins, Kuhn and RavenelHKR00] (cf. Definition 3.1). For the first application, we establish an Atiyah–Bott style localization theorem (Lemma 3.6) for HKR theories which are furthermore integral and of finite Krull dimension in the sense of Definition 3.3. Combining this localization theorem with our equivariant formality result, we deduce the following:
Theorem 1.10. Let
$(M,\omega )$
be a compact symplectic manifold with Hamiltonian T-action. Let
$\mathbb {E}^*$
be an HKR cohomology theory which is integral and of finite Krull dimension. Suppose that
$\mathbb {E}^*(M)$
is free as a module over the ground ring
$\mathbb {E}_*$
. Then the restriction map on equivariant cohomology
is injective. In particular, if
$\mathbb {E}_*$
is a graded field,
$j^*$
is injective for any compact symplectic manifold M with Hamiltonian T-action.
This is in contrast to the aforementioned failure of injectivity of
$j^*$
for ordinary cohomology with finite field coefficients. The ingredients in the proof can further be used to prove the Atiyah–Bott ‘integration formula’ with
$\mathbb {E}^*$
-coefficients, which is completely analogous to the classical statement for the rational cohomology; see Theorem 3.7.
Remark 1.11. To provide some context for readers unfamiliar with homotopy theory, the HKR cohomology theories can be viewed as generalizations of complex K-theory, which include examples that detect the information of conjugacy classes of n-tuples of commuting elements of prime power order in G if evaluated at
$BG$
, where G is a compact Lie group. In particular, they include Morava K-theories, which can be thought of as building blocks of the complex cobordism theory.
The second application concerns one of the most interesting classes of HKR theories, the Morava K-theories
$K_{p}(n)$
. For
$\mathbb {E} = K_{p}(n)$
, we can prove the following Goresky–Kottwitz–MacPherson type theorem which calculates the (equivariant) Morava K-theories of GKM spaces.
Let
$(M,\omega )$
be a compact symplectic manifold with Hamiltonian torus action by
$T = (S^1)^m$
. It is said to satisfy the GKM conditions if T acts with only finitely many fixed points
$x_1, \dots , x_k$
, and the union of T-orbits of corank at most
$1$
is a union of invariant two-spheres
$\overline {E}_1, \dots , \overline {E}_l$
. Symplectic manifolds satisfying the GKM conditions come in abundance, including toric manifolds, hypertoric manifolds (cf. [Reference Harada and HolmHH05]), and certain homogeneous spaces (cf. [Reference Guillemin, Holm and ZaraGHZ06]).
Using the notations introduced in the previous paragraph, each
$\overline {E}_j$
is isomorphic to
$S^2 = \mathbb {C}^{\times } \cup \{x_{j_0}\} \cup \{x_{j_{\infty }}\} = E_{j} \cup \{x_{j_0}\} \cup \{x_{j_{\infty }}\}$
for some
$x_{j_0}, x_{j_{\infty }} \in \{x_1, \dots , x_k\}$
, and the action of T on
$E_j$
factors through a group homomorphism
$\Theta _j: T \to S^1$
where
$S^1$
rotates the sphere
$\overline {E}_j$
with fixed points
$x_{j_0}$
and
$x_{j_{\infty }}$
.
Theorem 1.12. Let
$(M,\omega )$
be a compact symplectic manifold with Hamiltonian torus action satisfying the GKM conditions and let
$\mathbb {E}^*=K_p(n)$
. The restriction to fixed points
is injective. Furthermore, the image is given by
where the restriction
$|_{\mathbb {E}^*_{\ker (\Theta _j)}}$
denotes the homomorphism
$\mathbb {E}^*_{T}(pt) \to \mathbb {E}^*_{\ker (\Theta _j)}(pt)$
induced by the inclusion
$\ker (\Theta _j) \hookrightarrow T$
of the kernel of
$\Theta _j$
.
This statement reduces the calculation of the cohomology rings
$\mathbb {E}^*(M)$
and
$\mathbb {E}^*_{T}(M)$
to the combinatorics of the T-invariant
$2$
-spheres. We leave the applications of this circle of ideas to topology and enumerative geometry for future investigations.
2 Complex-oriented splitting
2.1 Complex-oriented theories
Suppose
$\mathbb {E}^*$
is a complex-oriented cohomology theory with coefficient ring
$\mathbb {E}_*:=\mathbb {E}^*(pt)$
. Recall that this means that there exists a class
$u \in \mathbb {E}^2(BS^1)$
that restricts to a generator of the reduced cohomology,
$\tilde {\mathbb {E}}^*(\mathbb {CP}^1)$
(a free rank one
$\mathbb {E}_*$
-module). Such a class u is called a complex orientation of
$\mathbb {E}^*$
. The universal example of such a cohomology theory is complex cobordism
$MU^*$
. For a multiplicative cohomology theory
$\mathbb {E}^*$
, complex orientations are in bijective correspondence with multiplicative natural transformations to
$\mathbb {E}^*$
from complex cobordism
$MU^*$
. A choice of orientation
$u \in \mathbb {E}^2(BS^1)$
gives rise to isomorphisms
It follows from this that the complex orientation of
$\mathbb {E}^*$
has an associated formal group law. Let
$\mu : BS^1\times BS^1 \to BS^1$
denote the universal classifying map for tensor product of line bundles. The formal group law is by definition the pull-back of u under this classifying map:
From the formal group law, one can extract the
$\ell $
-series, which is given by:
We also record the following technical fact which will be used in the sequel:
Lemma 2.1. Let
$\mathbb {E}^*$
be a complex-oriented cohomology theory and let B be a finite-type CW complex (meaning B has finitely many cells in each degree) with only even cells. The Atiyah–Hirzebruch spectral sequence
degenerates.
Proof. Because the cohomology groups
$H^p(B,\mathbb {Z})$
are free, the
$E_2$
page of the spectral sequence can be identified with
The spectral sequence is linear over
$\mathbb {E}^q(pt)$
and it suffices to prove that
If
$\mathbb {E}^*=MU^*$
is complex cobordism the spectral sequence collapses because the
$E_2$
page is concentrated in even degrees. In general, the complex orientation of
$\mathbb {E}^*$
is induced by a natural transformation (of multiplicative cohomology theories)
$MU^* => \mathbb {E}^*$
and the Atiyah-Hirzebruch sequence is natural in the cohomology theory. The result therefore follows from the case of complex cobordism.
2.2 Splittings
Next, we discuss cohomological splittings with
$\mathbb {E}^*$
coefficients, where
$\mathbb {E}^*$
is a complex-oriented cohomology theory.
Definition 2.2. Suppose that we have a fibration
$M \xrightarrow {i} P \xrightarrow {\pi } B$
. A fibration is c-split if there exists a map of
$\mathbb {E}_*$
modules
$s:\mathbb {E}^*(M) \to \mathbb {E}^*(P)$
so that
$i^* \circ s=\mathrm {id}.$
We will refer to s as a c-splitting.
Definition 2.3. A smooth manifold B is called Hamiltonian c-split for
$\mathbb {E}^*$
if every Hamiltonian fibration
$M \xrightarrow {i} P \xrightarrow {\pi } B$
is c-split.
We suppress the cohomology theory
$\mathbb {E}$
when it is clear from the context. The key result for us is the following result of Abouzaid–McLean–Smith:
Theorem 2.4 [Reference Abouzaid, McLean and SmithAMS21]
The one-dimensional projective space,
$\mathbb {CP}^1$
, is Hamiltonian c-split.
Remark 2.5. When
$\mathbb {E}^*$
is ordinary cohomology with coefficients in a commutative ring R, the first author and Xu ([Reference Bai and XuBX22]) have given a more direct proof of Theorem 2.4 which avoids the chromatic homotopy theory arguments from [Reference Abouzaid, McLean and SmithAMS21].
The following two Lemmas are refinements of arguments in [Reference Lalonde and McDuffLM03] (cf. Corollary 4.2 and Lemma 4.3 of loc. cit.).
Lemma 2.6. Let
$\tau ^{B}:\tilde {B} \to B$
be a birational morphism of smooth projective varieties. If
$\tilde {B}$
is Hamiltonian c-split, then so is B.
Proof. Suppose that we have a Hamiltonian fibration
$M \xrightarrow {i} P \xrightarrow {\pi } B$
over B and let
$M \xrightarrow {\tilde {i}} \tilde {P} \xrightarrow {\tilde {\pi }} \tilde {B}$
be the pull-back Hamiltonian fibration, which admits a map
$\tau ^P:\tilde {P} \to P.$
We can factor
$\tau ^B$
as an inclusion followed by a projection
$\tilde {B} \to \mathbb {CP}^r \times B \to B$
and similarly for
$\tau ^P$
. This shows that the map
$\tau ^P$
is compatible with complex-orientations. Set
$U \subset B$
to be the locus over which
$\tau ^{B}$
is an isomorphism and let
$P_U$
denote the restriction of the bundle to this locus. Note that we can assume that our reference fiber
$M_b$
for both
$\tilde {P}$
and P lies over a point
$b \in U$
. We have a Cartesian diagram of complex-oriented manifolds/maps:

For such Cartesian squares, the Umkëhr maps on cohomology are compatible with pullback/restriction maps; see [Reference QuillenQui71, 1.7] for complex cobordism, [Reference Bressler and EvensBE90, E(iii)] in general, and [Reference Crabb and JamesCJ98, Proposition 12.9] for a statement at the level of spectra, which implies the statement for cohomology by taking homotopy groups. In the present case this means that:
Suppose we are given a splitting
$\tilde {s}:\mathbb {E}^*(M) \to \mathbb {E}^*(\tilde {P})$
such that
$(\tilde {i})^* \circ \tilde {s}= \mathrm {id}$
. Then it follows from (2.7) that
satisfies
$i^* \circ s=\mathrm {id}.$
Lemma 2.7. Suppose that we have a Hamiltonian fibration
$M \xrightarrow {i} P \xrightarrow {\pi } B$
with B simply connected. Suppose that M and B are Hamiltonian c-split. Then P is also Hamiltonian c-split.
Proof. Let
$F \to E \to P$
be a Hamiltonian bundle over P. After restricting to M we get a Hamiltonian bundle
$F \to W \to M$
which by assumption gives rise to a c-splitting:
By [Reference Lalonde and McDuffLM03, Lemma 3.9], the composite bundle
$ W \to E \to B$
is also Hamiltonian, thus gives rise to a c-splitting:
The desired c-splitting for
$F \to E \to P$
is the map
$s=s_B \circ s_M$
.
Lemma 2.8. Let B be a product of complex projective spaces. Then B is Hamiltonian c-split.
Proof. In view of Lemma 2.7, it suffices to consider the case where
$B=\mathbb {CP}^{k}$
is a single projective space. We proceed by induction on k. The base case where
$k=1$
is Theorem 2.4. Consider the blow-up
$\tilde {B}$
of
$\mathbb {CP}^{k}$
at a point. Then
$\tilde {B}$
can be identified with the
$\mathbb {CP}^1$
-bundle:
The inductive hypothesis together with Lemma 2.7 shows that
$\tilde {B}$
is Hamiltonian c-split. It then follows from Lemma 2.6 that
$\mathbb {CP}^{k}$
is c-split.
More generally, we have the following result:
Lemma 2.9. Let B be a product of Grassmannians. Then B is Hamiltonian c-split.
Proof. Again, it suffices to consider a single Grassmannian. Recall that the Schubert varieties of the complete flag variety
$GL(n,{\mathbb C})/B$
are indexed by elements w of the symmetric group
$S_n$
. If we consider the Schubert variety
$Z_w$
corresponding to the permutation
$w(i) = i+k (\mathrm {mod} n)$
, this maps birationally onto the complex Grassmannian
$\mathrm {Gr}(k,n)$
via the projection
$GL(n,{\mathbb C})/B \to \mathrm {Gr}(k,n)$
(see discussion above Example 1.2.3 in [Reference BrionBri05]). Now take the Bott–Samelson variety
$Z_{\underline {w}}$
associated to a reduced decomposition
$\underline {w}$
of w. By, for example, [Reference BrionBri05, Proposition 2.2.1 (iii), (iv)], this is an iterated fibration of Kähler manifolds
with fiber
$\mathbb {CP}^1$
, which maps birationally onto
$Z_w$
and hence onto
$\mathrm {Gr}(k,n)$
. The statement again follows from Lemma 2.6 and Lemma 2.7.
Remark 2.10. As explained to us by an anonymous referee, the same argument can be extended using [Reference Bernstein, Gelfand and GelandBGG73, Reference DemazureDem74] to show more generally that any partial flag variety
$B = G/P$
is Hamiltonian c-split. We only discuss the Grassmannian case in detail because it suffices for our desired application.
2.3 Proof of Theorems
We now turn to giving our main arguments. As in previous sections,
$\mathbb {E}^*$
will denote a complex-oriented cohomology theory. We will make use of the following technical variant of the Leray–Hirsch theorem:
Lemma 2.11. Suppose that we have a c-split fibration
$M \xrightarrow {i} P \xrightarrow {\pi } B$
, where B is a finite type CW-complex with only even dimensional cells. Then the following hold:
-
(1) If B is finite, the natural map $s \otimes \pi ^*$
induced by the splitting map s (cf. Definition 2.2) (2.13) $$ \begin{align} \phi: \mathbb{E}^*(M)\otimes_{\mathbb{E}_*} \mathbb{E}^*(B) \to \mathbb{E}^*(P) \end{align} $$is an isomorphism.
-
(2) For general B as above, the c-splitting induces an isomorphism
(2.14) $$ \begin{align} \mathbb{E}^*(M \times B)\cong \mathbb{E}^*(P). \end{align} $$of $\mathbb {E}^*(B)$
-modules.
Proof.
Part (1): We follow the proof of the Leray–Hirsch theorem in [Reference HatcherHat02, Theorem 4D.1]. We assume that B has dimension m and proceed by induction on m. We let
$B'$
be the subspace obtained by deleting a point
$x_\alpha $
from each m cell
$U_\alpha $
and let
$P'$
denote the restriction of the fibration to
$B'$
. Then
$M \to P' \to B'$
is also a c-split fibration. We let
$V_\alpha \subset U_\alpha $
be a small disc about
$x_\alpha $
over which the fibration is trivial.
We note that the cohomologies
$\mathbb {E}^*(B,B')$
,
$\mathbb {E}^*(B)$
,
$\mathbb {E}^*(B')$
are all free over
$\mathbb {E}_*$
. For
$\mathbb {E}^*(B)$
,
$\mathbb {E}^*(B')$
this follows from Lemma 2.1, together with the fact that
$B'$
retracts onto the
$m-2$
skeleton. For
$\mathbb {E}^*(B,B')$
, this follows from the excision isomorphism
$\mathbb {E}^*(B,B') \cong \mathbb {E}^*(V_\alpha ,V_\alpha -x_\alpha ).$
Lemma 2.1 implies that the maps
$\mathbb {E}^*(B) \to \mathbb {E}^*(B')$
are surjections as the assertion holds for the integral cohomology. It follows from the long exact sequence for the pair
$(B,B')$
that the connecting maps
This means that the long exact sequence gives rise to a short exact sequence:
Because all of these groups are finite free over
$\mathbb {E}_*$
, we learn that
is also exact. Let
$(\mathbb {E}^*(B,B')\otimes _{\mathbb {E}_{*}}\mathbb {E}^*(M))^{q}$
denote the degree q piece of the tensor product and similarly for the other groups. Then there is a commutative diagram:

The top row is exact by (2.17) and (2.15) and the commutativity of the diagram follows as in the proof of [Reference HatcherHat02, Theorem 4D.1]. It is then easy to establish that
$\phi : \mathbb {E}^*(B,B')\otimes _{\mathbb {E}_{*}}\mathbb {E}^*(M) \to \mathbb {E}^*(P,P')$
is an isomorphism by retracting everything on to
$V_\alpha .$
Because
$B'$
retracts onto the
$m-2$
skeleton, the induction hypothesis implies that the map
$\phi : \mathbb {E}^*(B')\otimes _{\mathbb {E}_{*}}\mathbb {E}^*(M) \to \mathbb {E}^*(P')$
is also an isomorphism. The claim now follows from the five-lemma.
Part (2): We let
$B^m$
denote the m-skeleton of B and let
$P^m \to B^m$
denote the restriction of P to
$B^m$
. Using the splitting s, we can identify
In particular, all of the restriction maps
$\mathbb {E}^*(P^{m+1}) \to \mathbb {E}^*(P^m)$
are surjective. Applying the Milnor exact sequence together with the Mittag-Leffler property, we obtain isomorphisms:
Finally, we note that the same argument shows that the inverse system
$\varprojlim _m \mathbb {E}^*(M)\otimes _{\mathbb {E}_*} \mathbb {E}^*(B^m)$
is canonically isomorphic to
$\mathbb {E}^*(M \times B)$
, proving the claim.
Remark 2.12. One can also use standard spectral sequence arguments to give a proof of Lemma 2.11.
Corollary 2.13 (= Proposition 1.8)
Suppose that we have a Hamiltonian fibration
$M \xrightarrow {i} P \xrightarrow {\pi } B$
, where B is a product of Grassmannians. Then there is a noncanonical isomorphism of
$\mathbb {E}^*(B)$
modules:
Lemma 2.14. Suppose that we have a c-split fibration
$M \xrightarrow {i} P \xrightarrow {\pi } B$
, where B is a finite type CW-complex with only even dimensional cells. Let
$i:B_0 \subset B$
be a subcomplex,
$P_0 \to B_0$
denote the restriction of the fibration to
$B_0$
, and
$\iota : P_0 \to P$
the inclusion. Given a fixed c-splitting
$s_{0}: \mathbb {E}^*(M) \to \mathbb {E}^*(P_{0})$
, we can find a c-splitting
$s: \mathbb {E}^*(M) \to \mathbb {E}^*(P)$
such that
Proof. Let
$\tilde {s}$
be the c-splitting over B. This gives rise to a commutative diagram:

where the horizontal arrows are isomorphisms. Thus, because
$\mathbb {E}^*(B)$
,
$\mathbb {E}^*(B_0)$
are free, we may choose a splitting of
$\mathbb {E}_*$
modules
$\mathbb {E}^*(B_0)\to \mathbb {E}^*(B)$
for
$i^*$
. This defines a splitting
$\tau : \mathbb {E}^*(P_{0})\hookrightarrow \mathbb {E}^*(P)$
of
$\mathbb {E}_*$
-modules for
$\iota ^*.$
We can thus split the cohomology
$\mathbb {E}^*(P)$
as
We then define a new splitting
$s:\mathbb {E}^*(M) \to \mathbb {E}^*(P)$
using
$s_{0}$
by letting
$s=(\tau \circ s_0,0)$
in this direct sum decomposition. By construction s satisfies (2.21).
Proof of Theorem 1.2
Part (1): Recall that there is a convenient model for the total space of the universal
$U(k)$
-bundle,
$EU(k)$
, given by taking the set of orthonormal k-frames in a complex Hilbert space
$\mathcal {H}.$
Topologically, this is the colimit of spaces of k-frames in
$\mathbb {C}^n$
as
$n \to \infty $
:
The group
$U(k)$
acts freely on this space and the quotient is the infinite Grassmannian of k-planes
$Gr_k(\mathcal {H}).$
Given a product of unitary groups
$G=\prod U(k_i)$
, we can similarly take
$EG:=\prod EU(k_i).$
The classifying space for G,
$BG$
, therefore admits finite dimensional approximations by spaces
$BG_n$
which are products of Grassmannians. We set
$M_G:=M\times _G EG$
and
$M_{G,n}:=M\times _G EG_n$
. In view of Lemma 2.9, we have c-splittings
$s_n: \mathbb {E}^*(M) \to \mathbb {E}^*(M_{G,n})$
which by Corollary 2.13 give rise to identifications:
The identifications from (2.23) imply that the restrictions
$\mathbb {E}^*(M_{G,n+1}) \to \mathbb {E}^*(M_{G,n})$
are surjective and we have that
By Lemma 2.14, we can arrange that the c-splittings
$s_n$
are compatible with restriction and thus give rise to a splitting:
Using Lemma 2.11 (2) (by construction the model for
$BG$
has only even-dimensional cells), we obtain that
It remains to prove that the Leray-spectral sequence
$\lbrace E_r^{p,q}(M_{G}) \rbrace $
for the fibration
$M_G \to BG$
degenerates. It follows easily from (2.23) that the Leray spectral sequences
$\lbrace E_r^{p,q}(M_{G,n}) \rbrace $
associated to the fibrations
$M_{G,n} \to BG_n$
degenerate. The
$E_2$
page
$E_2^{p,q}(M_{G})$
is an inverse limit of the
$E_2$
pages
$E_2^{p,q}(M_{G,n})$
, which implies that the differential vanishes on
$E_2^{p,q}(M_{G})$
. The same argument then implies that the differentials on the subsequent pages
$E_r^{p,q}(M_{G})$
are zero, which proves degeneration.
Part (2): We let
$EG$
be any CW-complex on which G (and hence
$T \subset G$
) acts freely. We again set
$M_T=M\times _T EG$
and
$M_G:=M\times _G EG$
and consider the diagram

We let
$\lbrace E_r^{p,q}(M_T) \rbrace $
and
$\lbrace E_r^{p,q}(M_G) \rbrace $
be the Leray spectral sequences associated to the fibrations over the respective Borel spaces
$BT$
and
$BG$
. By functoriality of the Leray spectral sequence, r induces maps
$r^*: E_r(M_G) \to E_r(M_T).$
We can identify the
$E_2$
pages of the spectral sequence with
$E_2(M_G)=\mathbb {E}^*(M)\otimes _{\mathbf {k}}H^*(BG,\mathbf {k})$
and
$E_2(M_T)=\mathbb {E}^*(M)\otimes _{\mathbf {k}}H^*(BT,\mathbf {k})$
respectively. By hypothesis
$r^*$
is injective on the
$E_2$
pages and hence there are no differentials on
$E_2(M_G).$
The same argument shows there are therefore no differentials on subsequent pages and thus the spectral sequence
$E_r^{p,q}(M_G)=>\mathbb {E}^*(M_G)$
degenerates at the second page as required.
Remark 2.15. We note that in the case of classical cohomology, the argument for Part (1) actually simplifies a little bit. This is because we can choose
$BG_n$
large enough so that the restriction map
By Lemma 2.9, we can produce a c-splitting
$\bar {s}: H^*(M) \to H^*(M_{G,n})$
for the fibration
$M_{G,n} \to BG_n.$
Then by composing with the inverse maps to (2.27), we get a c-splitting
$s: H^*(M) \to H^*(M_G)$
.
We have the following Corollary.
Corollary 2.16. Let
$T \cong (S^1)^m$
be a torus and M a symplectic manifold with Hamiltonian T-action. There is an isomorphism of
$\mathbb {E}^*(BT) \cong \mathbb {E}_*[\![u_1,\cdots ,u_m]\!]$
modules:
Proof. By equivariant formality,
$\mathbb {E}^*_T(M) \cong \mathbb {E}^*(M\times BT).$
We also have an identification
$\mathbb {E}^*(M\times BT) \cong \mathbb {E}^*(M)[\![u_1,\cdots ,u_m]\!]$
from which the result follows.
3 Localization and GKM
3.1 HKR theories
We next turn to discussing a particular class of complex-oriented cohomology theories. Throughout the discussion, we fix a prime number p. We let
$\mathbb {Z}_p$
denote the p-adic integers and let
$\mathbb {Z}_{(p)}=\mathbb {Z}_p \cap \mathbb {Q}.$
Suppose we have a complex-oriented cohomology theory
$\mathbb {E}^*$
where
$\mathbb {E}_*$
is a local ring with graded maximal ideal
$\mathfrak {m}$
such that
$p \in \mathfrak {m}$
. For such
$\mathbb {E}^*$
, the mod
$\mathfrak {m}$
reduction,
$L_{0}$
, of
$L_{\mathbb {E}}$
is a formal group over a graded field of characteristic
$p> 0$
. The height of such a cohomology theory is the height of the formal group law
$L_{0}$
, which we denote by n.
Definition 3.1. We say that a complex-oriented cohomology theory
$\mathbb {E}^*$
is of HKR-type if
$\mathbb {E}_*$
is a Noetherian, complete, local ring with (graded-) maximal ideal
$\mathfrak {m}$
such that
$p \in \mathfrak {m}$
and
$\mathbb {E}^*$
is of finite height
$n<\infty $
.
Cohomology theories of this kind were considered by Hopkins–Kuhn–Ravenel [Reference Hopkins, Kuhn and RavenelHKR00, §5]. Many interesting examples of such theories arise from Johnson–Wilson cohomology
$E(n)^*$
, which is a cohomology theory with coefficients:
where the periodic variable
$v_n$
plays a special role and has degree
$|v_n|= 2(p^n-1)$
. From
$E(n)^*$
, one can construct the following examples of HKR-type cohomology theories:
-
(1) The $I_n$
-adically complete version of
$E(n)_*$
,
$\hat {E}(n)_*$
, ([Reference Hopkins, Kuhn and RavenelHKR00, §1.3]) is a cohomology theory with coefficients the completion of
$E(n)_*$
at the ideal $$ \begin{align*}I_n=(p,v_1,\cdots,v_{n-1}).\end{align*} $$
-
(2) The integral lifts of Morava K-theory $\hat {K}(n)$
arise by taking the p-completion of the quotient
$E(n)/(v_1,\cdots ,v_{n-1}).$
See [Reference Greenlees and SadofskyGS96, §1.3] for more details. These theories have coefficients given by: (3.2) $$ \begin{align} \hat{K}(n)_* = \mathbb{Z}_p[v_n,v_n^{-1}]. \end{align} $$
-
(3) Finally the Morava K-theories $K(n)$
are the cohomology theories which arise by further quotienting by p. These cohomology theories have coefficients given by (3.3) $$ \begin{align} K(n)_{*} = \mathbb{F}_p[v_n,v_n^{-1}]. \end{align} $$
The key to the localization result is the following computation of the
$\mathbb {E}^*$
-theory for classifying spaces of finite abelian groups from [Reference Hopkins, Kuhn and RavenelHKR00, §5.2].
Lemma 3.2. Let
$\mathbb {E}^*$
be an HKR theory of height
$n<\infty $
. Let A be a finite cyclic group of order
$\ell $
. Write
$\ell =p^rs$
with
$(s,p^r)=1$
. Then
-
(1) $\mathbb {E}^*(BA)$
is free over
$\mathbb {E}_*$
of rank
$p^{rn}$
. -
(2) In the case $\mathbb {E}^*=K(n)$
is the Morava K-theory, we have: (3.4) $$ \begin{align} \mathbb{E}^*(BA) \cong \mathbb{E}_*[[u]]/(u^{p^{rn}}). \end{align} $$
Proof. Part (1) is established in [Reference Hopkins, Kuhn and RavenelHKR00, Cor. 5.8], so we focus on explaining Part (2). Note that by Part (1), we have that the pull-back map
is an isomorphism. Thus, it suffices to consider the case where
$\ell =p^r.$
View A as a finite subgroup
$A \subset S^1$
. Regard
$\mathbb {E}^*(BA)$
as a module over
$\mathbb {E}_*[\![u]\!]$
via the map
$BA \to BS^1$
. By [Reference Hopkins, Kuhn and RavenelHKR00, Lemma 5.7] we have that
The formal group law
$L_{\mathbb {E}}$
for Morava K-theory is essentially characterized by the fact that its p-series satisfies:
Iterating the formal group law, we obtain
for some integer
$d(r)>0$
. The result follows immediately from this.
3.2 Localization
Definition 3.3. An HKR theory
$\mathbb {E}^*$
is integral of finite Krull dimension if the coefficient ring
$\mathbb {E}_*$
is an integral domain of finite Krull dimension.
Remark 3.4. All of the examples
$\hat {E}(n)^*,E(n)^*, \hat {K}(n)^*, K(n)^* $
are integral of finite Krull dimension, see the coefficient rings listed after Definition 3.3.
Fix an HKR cohomology theory which is integral and of finite Krull dimension. The goal of this section is to extend the Atiyah–Bott localization theorem ([Reference Atiyah and BottAB84, Theorem 3.5]) to
$\mathbb {E}^*$
coefficients. Throughout this section we take our group to be a torus
$T \cong (S^1)^m$
. We have by [Sta24, Tag 0BNH] that
$\mathbb {E}^*(BT)$
is NoetherianFootnote
3
and it is also an integral domain. We may therefore set
$R=\mathrm {Frac}(\mathbb {E}^*(BT))$
to be the fraction field of
$\mathbb {E}^*(BT).$
We have the following version of the Atiyah-Bott support lemma (cf. [Reference Atiyah and BottAB84, Lemma 3.4]):
Lemma 3.5. Let
$X=T/K$
be an orbit of T, where K is a closed subgroup of T. Let
$\mathrm {supp}(\mathbb {E}^*_T(X)) \subset \mathrm {Spec}(\mathbb {E}^*(BT))$
denote the support of
$\mathbb {E}^*_T(X)$
as a module over
$\mathbb {E}^*(BT)).$
Then:
-
(1) $\mathrm {supp}(\mathbb {E}^*_T(X))$
is a closed subspace of codimension
$\mathrm {dim}(T)-\mathrm {dim}(K)$
. -
(2) In the case where $\mathbb {E}^*=K(n)^*$
is Morava K-theory,
$\mathrm {supp}(\mathbb {E}^*_T(T/K))=\mathrm {supp}(\mathbb {E}^*_T(T/K^0))$
, where
$K^0 \subset K$
is the connected component of K at the identity.
Proof. We have that
$\mathbb {E}_{T}^*(X) \cong \mathbb {E}^*(BK)$
and the induced
$\mathbb {E}^*(BT)$
module structure on this group is induced by the inclusion
$K \subset T$
. We first argue that the map
is surjective so that
$\mathrm {Spec}(\mathbb {E}^*(BK))$
is a closed subscheme of
$\mathrm {Spec}(\mathbb {E}^*(BT))$
. As above, we let
$K^0$
denote the connected component of K. After choosing a complementary torus H to
$K^0$
, we may write
$K=A \times K^0$
, where A is a finite abelian subgroup of H. Then by the Künneth isomorphism [Reference Hopkins, Kuhn and RavenelHKR00, Cor. 5.11], we have
Moreover, the Kunneth map fits into a diagram:

It therefore suffices to assume that
$K=A$
is a finite abelian group. Moreover, by Part (1) of Lemma 3.2 we can assume that
$A \cong \mathbb {Z}/p^{r_1} \times \mathbb {Z}/p^{r_2} \times \cdots \times \mathbb {Z}/p^{r_i}$
is a product of p-groups. It is easy to see that we may find:
-
○ a rank one subgroup $H' \cong S^1 \subset T$
so that
$\mathbb {Z}/p^{r_1} \subset H'$
-
○ a complementary torus $H"$
(for
$H'$
) together with a subgroup
$A' \subset H"$
so that
$A \cong \mathbb {Z}/p^{r_1} \times A'$
(the group
$A' \cong \mathbb {Z}/p^{r_2} \times \cdots \times \mathbb {Z}/p^{r_i}$
).
The surjectivity of the restriction
$\mathbb {E}^*(BT) \to \mathbb {E}^*(BA)$
follows from the Kunneth isomorphism together with induction on the number of factors in the product decomposition of A. To prove the claim on dimensions, we note that the claim is obvious for connected groups where
$K=K^0$
. In view of the Kunneth isomorphism and Part (1) of Lemma 3.2, we have that
$\mathbb {E}^*(BK)$
is finite over
$\mathbb {E}^*(BK^0)$
, which implies that they have equal dimensions [Sta24, Tag 01WG]. To prove Part (2) of the Lemma, we again write our group K as
$A\times K^0$
. Without loss of generality, we can assume
$A \cong \mathbb {Z}/p^{r_1} \times \mathbb {Z}/p^{r_2} \times \cdots \times \mathbb {Z}/p^{r_i}$
. Then Part (2) of Lemma 3.2 shows that
$K(n)^*(BA)$
is a tensor product of the algebras in (3.4). In particular,
$K(n)^*(BA)$
is a nilpotent extension of
$K(n)_*$
for any finite abelian group. The claim now follows from the Kunneth isomorphism (3.10).
For the rest of this section, unless otherwise specified, let M be a smooth compact manifold with T-action and denote by
$M^{T}$
the set of fixed points of the T-action. For the following statement, recall that
$R=\mathrm {Frac}(\mathbb {E}^*(BT))$
is the fraction field.
Lemma 3.6. Let
$j: M^T \to M$
denote the inclusion of
$M^T$
into M. Then the map:
is an isomorphism.
Proof. We stratify the complement of an equivariant tubular neighborhood U of
$M^T$
by finitely many open sets which equivariantly retract onto nonconstant orbits. Note that for a nonconstant orbit X, Lemma 3.5 implies in particular that
The result then follows from Lemma 3.2, Lemma 3.5, and the Mayer-Vietoris sequence.
Proof of Theorem 1.10
The assumption that
$\mathbb {E}_*$
is free implies by Corollary 2.16 that
Hence,
$\mathbb {E}_T^*(M)$
is free as a module over
$\mathbb {E}^*(BT).$
By Lemma 3.6, the kernel of
$j^*$
is a torsion module over
$\mathbb {E}^*_T(pt)$
. Because
$\mathbb {E}^*_{T}(M)$
is free, it follows that the kernel of
$j^*$
is trivial.
To end this subsection, we include an Atiyah–Bott localization formula for HKR theories.
Theorem 3.7. Suppose that M has an almost complex structure which is preserved under the T-action. Index the connected components of
$M^T$
by the set I, and for each
$i \in I$
, denote by
$\nu _i$
the normal bundle of the corresponding connected component. Then the pushforward on the localized cohomology
is an isomorphism with inverse
Proof. By the complex-orientation assumption and its compatibility with the T-action, we see that the pushforward in equivariant cohomology
$j_*$
and the Euler class of the normal bundle
$\nu _i$
are well-defined. For each
$i \in I$
, we have
$j_i^* j_* (1) = \mathit {eu}^{T}_{\mathbb {E}}(\nu _i)$
. Using the Mayer–Vietoris long exact sequence for the pair
$(M, M \setminus M^T)$
, as in Lemma 3.6, one can show that for the pushforward
$j_*$
, both
$\ker (j_*)$
and
$\mathrm {coker}(j_*)$
are torsion modules over
$\mathbb {E}^*(BT)$
. Combining with Lemma 3.6, it follows that
$j^* j_*$
is an isomorphism. This proves the invertibility of the Euler classes, so the statement follows accordingly.
Remark 3.8. Following [Reference Atiyah and BottAB84, Section 3], we can prove Theorem 3.7 in a slightly different way. For a connected component
$M^T_i$
, we can decompose its normal bundle into a direct sum of irreducible T-eigenbundles
such that for each
$1 \leq \alpha \leq k$
, the corresponding character
$\varphi _{\alpha }: T \to U(1)$
is nontrivial. If we write
$u_{\alpha } \in \mathbb {E}_{*}[\![ u_1, \dots , u_m ]\!]$
for the image of the generator of
$\mathbb {E}^*(BS^1)$
in
$\mathbb {E}^*(BT)$
induced by
$\varphi _{\alpha }$
, then
Here z lies in the kernel of the restriction map
$\mathbb {E}_{T}^*(M^T_i) \to \mathbb {E}_{T}^*(pt))$
corresponding to the inclusion of any point,
$pt \to M^T_i$
. A standard argument using the skeletal filtration on cohomology shows that any class in
$\mathrm {ker}(\mathbb {E}_{T}^*(M^T_i) \to \mathbb {E}_{T}^*(pt))$
is nilpotent (cf. [Reference Conner and FloydCF66, Corollary 7.2]). Accordingly, we see that
$\mathit {eu}^{T}_{\mathbb {E}}(\nu _i)$
is invertible after tensoring with the fraction field R.
3.3 GKM theorem
In this subsection, we specialize our discussion to the case where
$\mathbb {E}^*$
is a Morava K-theory
$K(n)$
. We show that the so-called Chang–Skjelbred lemma works verbatim for
$K(n)$
coefficients, and deduce the GKM calculation of equivariant cohomology as a corollary.
Let M be a compact smooth T-manifold. Denote by
$\mathcal {P}$
the set of closed subschemes
$\mathcal {Z}_K:=\mathrm {supp}(\mathbb {E}^*_T(T/K)) \subset \mathrm {Spec}(\mathbb {E}_*[\![ u_1, \dots , u_m ]\!])$
where K is a stabilizer of some point
$x \in M\setminus M^T$
(we give
$\mathcal {Z}_K$
the reduced-induced scheme structure). This is a partially ordered set, with partial order given by inclusion. Note that by Lemma 3.5 (2), the scheme
$\mathcal {Z}_K$
only depends on the connected component of the identity element
$K^0$
.
Let
$\delta '$
denote the connecting homomorphism of the
$\mathbb {E}^*_{T}$
-cohomology of the pair
$(M, M^T)$
. Given
$\xi \in \mathbb {E}^*_{T}(M^T)$
, write
$I(\xi )$
for the ideal of annihilators of
$\delta '(\xi )$
. On the other hand, for each
$\mathfrak {m} \in \mathcal {P}$
, we write
$M^{\mathfrak {m}}$
for the subset of M consisting of points
$x \in M$
whose stabilizer group
$K_x$
satisfies
$\mathfrak {m} \subset \mathcal {Z}_{K_x}$
. Denote the connecting homomorphism of
$\mathbb {E}^*_{T}$
-cohomology of the pair
$(M, M^{\mathfrak {m}})$
by
$\delta ^{\mathfrak {m}}$
. The following technical statement is proved in the same way as [Reference Chang and SkjelbredCS74, Lemma 2.3] and [Reference Goresky, Kottwitz and MacPhersonGKM98, Lemma 15.8].
Lemma 3.9. For
$\xi \in \mathbb {E}^*_{T}(M^T)$
, if
$\delta '(\xi ) \neq 0$
, then the variety defined by
$I(\xi )$
satisfies
in the scheme
$\mathrm {Spec}(\mathbb {E}_*[\![ u_1, \dots , u_m ]\!])$
.
Denote by
$M_1 \subset M$
the set of points consisting of the union of
$0$
and
$1$
-dimensional orbits of T. In particular,
$M^{T} \subset M_1$
.
Proposition 3.10. Let
$\mathbb {E}^*$
be a Morava K-theory. If the equivariant cohomology
$\mathbb {E}^*_T(M)$
is a free module over
$\mathbb {E}^*(BT)$
, then the sequence
is exact, where
$\mathbb {E}^{*+1}_T(M_1, M^T)$
denotes the relative equivariant cohomology of the pair
$(M_1, M^T)$
and
$\delta $
is the connecting homomorphism.
Proof. The fact that
$\ker (j)^*$
is trivial follows immediately from Theorem 1.10 because the coefficient ring is a graded field. Because the connecting homomorphism
$\delta $
factors as the composition
where recall that
$\delta '$
is the connecting homomorphism for the pair
$(M,M^T)$
, the long exact sequence implies that
$\delta \circ j^* = 0$
. To finish the proof, suppose
$\xi \in \mathbb {E}^*_{T}(M^T)$
satisfies
$\delta (\xi ) = 0$
. To show it lies in the image of
$j^*$
, we need to show that
$\delta '(\xi ) = 0$
.
Suppose this is not the case. We claim that the ideal
$I(\xi )$
is a principal ideal. We follow the proof of [Reference Chang and SkjelbredCS74, Lemma 2.2]. Indeed, let
$0 \neq a \in I(\xi )$
be an element which is not divisible by any other element and suppose
$b \in I(\xi )$
. Choosing a basis
$\{x_i\} \subset \mathbb {E}^*_T(M)$
, we can find
$a_i, b_i \in \mathbb {E}^*_{T}(pt)$
such that
$a\xi = j^*(\sum a_i x_i)$
and
$b \xi = j^*(\sum b_i x_i)$
using the long exact sequence for the pair
$(M, M^T)$
. Then we know that
$j^*(\sum b a_i x_i) = j^*(\sum a b_i x_i)$
, so
$\sum b a_i x_i = \sum a b_i x_i$
by the injectivity of
$j^*$
. This shows that for each i, we have
$b a_i = a b_i$
. As the
$a_i$
must have no common factor, we see that b is divisible by a, which proves the claim.
By Lemma 3.9, as
$I(\xi )$
is principal, there must be one
$\mathfrak {m}$
which has codimension
$1$
in T. Because of the inclusion
$M^{\mathfrak {m}} \subset M_1$
, the connecting homomorphism
$\delta ^K$
factors as
which tells us that
$\delta (\xi ) \neq 0$
, leading to a contradiction.
Proof of Theorem 1.12
This follows from the proof of [Reference Goresky, Kottwitz and MacPhersonGKM98, Theorem 7.2], which we reproduce for completeness. Because
$\mathbb {E}^*_T(M)$
is a free module over
$\mathbb {E}^*(BT)$
, using the exact sequence (3.19), it suffices to determine the kernel of
$\delta : \mathbb {E}^*_T(M^T) \to \mathbb {E}^{*+1}_T(M_1, M^T)$
. Given the complement of poles
$E_j$
, by definition, its stabilizer group is
$\ker (\Theta _j)$
. Therefore,
Choose a T-invariant open cover of
$\overline {E}_j = U_j \cup V_j$
where
$U_j = \overline {E}_j \setminus \{ x_{j_0} \}$
and
$V_j = \overline {E}_j \setminus \{ x_{j_{\infty }} \}$
. Then the corresponding Mayer–Vietoris long exact sequence splits into short exact sequences because all the cohomology groups concentrate in even degrees. Furthermore, we have a commutative diagram

which tells us that
$\delta $
agrees with the map
Ranging over all j, the theorem is proved.
Remark 3.11. In view of the calculation Lemma 3.2 (2), one can see that for an invariant
$2$
-sphere with orbit type
$T/K$
such that in the decomposition
$K = A \times K^0$
, the finite group component A has order greater than
$1$
, the formula in Theorem 1.12 depends on the height for the cohomology theory
$\mathbb {E}^*$
. We thank Ivan Smith for a related question.
Acknowledgments
We thank David Anderson, Yael Karshon, Allen Knutson, and Che Shen for sharing their expertise on Bott–Samelson resolutions. We also thank the anonymous referees for their careful reading.
Competing interest
The authors have no competing interest to declare.
Financial support
S.B. and D.P. were partially funded by NSF grants DMS-2404843 and DMS-2306204 respectively while working on this note.


