1. Introduction
Let
$\Sigma$
be a compact, connected, oriented surface with boundary. Its mapping class group
$\mathcal{M}\,:=\,\mathcal{M}(\Sigma)$
is the group of isotopy classes of orientation-preserving homeomorphisms of
$\Sigma$
that restrict to the identity on
$\partial \Sigma$
. Here, for simplicity, we assume that
$\Sigma$
has exactly one boundary component and genus
$g\geq 3$
. The subgroup
$\mathcal{I}\,:=\,\mathcal{I}(\Sigma)$
of
$\mathcal{M}$
that acts trivially on the homology
$H\,:=\, H_1(\Sigma;\mathbb{Z})$
of the surface is known as the Torelli group of
$\Sigma$
. It contains the subgroup
$\mathcal{K}\,:=\,\mathcal{K}(\Sigma)$
that is generated by Dehn twists along bounding simple closed curves, the latter being known as the Johnson subgroup of
$\Sigma$
.
Johnson fully determined in [
Reference Johnson18
] the abelianization
$\mathcal{I}_{\operatorname{ab}}\,:=\,\mathcal{I}/[\mathcal{I},\mathcal{I}]$
of the Torelli group. In particular, he proved that
$\mathcal{I}_{\operatorname{ab}}$
has non-trivial torsion (with only order-two elements), and that its torsion-free abelianization
$\mathcal{I}_{\operatorname{abf}}\,:=\, \mathcal{I}_{\operatorname{ab}} \big/ \hbox{Tors}(\mathcal{I}_{\operatorname{ab}} )$
is canonically isomorphic to
$\Lambda^3 H$
through the first Johnson homomorphism
which encodes the action of
$\mathcal{I}$
on the second nilpotent quotient of
$\pi_1(\Sigma)$
. Since the kernel of
$\tau_1$
coincides with the Johnson subgroup, we have
$\mathcal{I}_{\operatorname{abf}}=\mathcal{I}/\mathcal{K}$
or, equivalently,
$\hbox{Tors}(\mathcal{I}_{\operatorname{ab}} )\,=\,\mathcal{K}/[\mathcal{I},\mathcal{I}]$
.
Consider now the lower central series
$\Gamma_1\mathcal{I} \supset \Gamma_2\mathcal{I} \supset \Gamma_3\mathcal{I} \supset \cdots $
of the Torelli group, which is defined by
$\Gamma_1\mathcal{I}=\mathcal{I}$
,
$\Gamma_2 \mathcal{I} =[\mathcal{I},\mathcal{I}]$
,
$\Gamma_{3} \mathcal{I} = [\mathcal{I},[\mathcal{I},\mathcal{I}]]$
and so on. Its associated graded
is a graded Lie
$\mathbb{Z}$
-algebra, which is generated by its degree 1 part, namely by
$\mathcal{I}_{\operatorname{ab}}$
. As a general fact, the associated graded of the lower central series of a group is, with rational coefficients, the same as the associated graded of the natural filtration on the Malcev Lie algebra of the group. In the case of the Torelli group, much more is known: in the fundamental work [
Reference Hain13
], Hain proved that the degree-completion of
$\big(\!\operatorname{Gr}^{\Gamma} \mathcal{I}\big)\otimes \mathbb{Q}$
is (non-canonically) isomorphic to the Malcev Lie algebra of
$\mathcal{I}$
and, furthermore, he identified the latter graded Lie
$\mathbb{Q}$
-algebra in the following way.
Let
$H^\mathbb{Q}\,:=\,H\otimes \mathbb{Q}$
and consider the free Lie
$\mathbb{Q}$
-algebra
$\operatorname{Lie}(\Lambda^3 H^\mathbb{Q})$
generated by
$\Lambda^3 H^\mathbb{Q}$
. Clearly, the map
$J^\mathbb{Q}$
defined by the composition

is surjective, so that the determination of
$\big(\!\operatorname{Gr}^{\Gamma} \mathcal{I}\big)\otimes \mathbb{Q}$
resumes at the computation of the ideal of rational relations
$R^\mathbb{Q}\,:=\,\ker(J^\mathbb{Q})$
. Note that the conjugacy action of
$\mathcal{M}$
on
$\mathcal{I}$
induces an action of the symplectic group
$\operatorname{Sp}(H^\mathbb{Q})$
on
$\big(\!\operatorname{Gr}^{\Gamma} \mathcal{I}\big)\otimes \mathbb{Q}$
, such that
$J^\mathbb{Q}$
is
$\operatorname{Sp}(H^\mathbb{Q})$
-equivariant. Here the symplectic form
$\omega$
on
$H^\mathbb{Q}$
is given by the homology intersection pairing. Then, it turns out that the ideal
$R^\mathbb{Q}$
is generated by its degree 2 part
$R^\mathbb{Q}_2$
for
$g\geq 4$
[
Reference Hain13
, 14]. Furthermore, for
$g\geq 3$
, the subspace
$R_2^\mathbb{Q}$
can be described as the
$\operatorname{Sp}(H^\mathbb{Q})$
-submodule of
$\operatorname{Lie}_2\!(\Lambda^3 H^\mathbb{Q}) \simeq \Lambda^2(\Lambda^3 H^\mathbb{Q})$
generated by two explicit elements [9,
Reference Hain13
]. Thus, using Morita’s works on the Casson invariant and the second Johnson homomorphism [
Reference Morita22
,
Reference Morita23
], one obtains an explicit description of
Besides, the subspace
$R_2^\mathbb{Q}$
coincides with the kernel of a certain map B which is defined explicitly on
$\Lambda^2(\Lambda^3 H^\mathbb{Q})$
in terms of contractions with
$\omega$
: see equation (3·1) below for the exact definition. In the sequel, we shall refer to B as the diagrammatic bracket since it corresponds in [11] to a restriction of the Lie bracket of so-called “symplectic Jacobi diagrams”, and it gives rise there to a diagrammatic description of
$(\Gamma_2 \mathcal{I} / \Gamma_3 \mathcal{I})\otimes \mathbb{Q} $
.
In this paper, we are interested in the
$\mathbb{Z}$
-module structure of
$\operatorname{Gr}^{\Gamma} \mathcal{I}$
, which (beyond its rationalisation) seems to be largely unknown in degree greater than 1. A first step in this direction is the following.
Theorem A. Let
$g\geq 3$
. We have
$[\mathcal{I},[\mathcal{I}, \mathcal{I}]] =[\mathcal{I},\mathcal{K}]$
.
This is proved in Section 2 as follows. Firstly, by using Johnson’s descriptions [
Reference Johnson18
] of the group
$\mathcal{I}_{\operatorname{ab}}$
and its subgroup
$\mathcal{K}/[\mathcal{I},\mathcal{I}]$
, we observe that the triviality of the quotient
$[\mathcal{I},\mathcal{K}]/[\mathcal{I},[\mathcal{I}, \mathcal{I}]]$
follows from the nullity of two special elements (Lemma 2·3). This nullity is then ensured by using some appropriate “Push” maps for surfaces related to
$\Sigma$
.
Theorem A has the following two consequences. On the one hand, the torsion of
$\operatorname{Gr}^{\Gamma} _1\mathcal{I} =\mathcal{I}_{\operatorname{ab}}$
does not “propagate” to higher-degree torsion elements in
$\operatorname{Gr}^{\Gamma} \mathcal{I}$
. (However, note that
$\operatorname{Gr}^{\Gamma} \mathcal{I}$
does contain non-trivial torsion in any odd degree: see the forthcoming paper [
Reference Nozaki, Sato and Suzuki27
], which builds upon results of [
Reference Kupers and Randal-Williams19
,
Reference Nozaki, Sato and Suzuki26
].) On the other hand, the map (1·1) also exists with integral coefficients in degree greater than 1:

Consequently, we can consider the ideal of integral relations
$R\,:=\,\ker(J)$
, where J is the above map. Our next result, which is proved in Section 3, computes explicitly its degree 2 part
$R_2$
.
Theorem B. Let
$g\geq 3$
. We have
$R_2=\ker(B)\cap \Lambda^2 (\Lambda^3 H)$
.
Of course, the inclusion
$R_2 \subset \ker(B)\cap \Lambda^2 (\Lambda^3 H)$
follows from the above-mentioned identity
$R_2^\mathbb{Q}=\ker(B)$
[11]: alternatively, this inclusion is a direct consequence of the relationship between the homomorphism B and the pair (second Johnson homomorphism, Casson invariant) on
$[\mathcal{I},\mathcal{I}]$
, which will be specified in Proposition 3·2. The proof of the converse inclusion (i.e., the fact that any element of
$\Lambda^2 (\Lambda^3 H)$
with trivial diagrammatic bracket is a quadratic relation in the graded Lie ring
$\operatorname{Gr}^{\Gamma} \mathcal{I}$
) constitutes the most technical part of this paper. In contrast with the above-mentioned characterisations of
$R_2^\mathbb{Q}$
which use the representation theory of
$\operatorname{Sp}(H^\mathbb{Q})$
, our proof of Theorem B is rather pedestrian and proceeds in two steps. First, we fix a symplectic basis S of H, and we produce an explicit finite generating system of
$\ker(B)\cap \Lambda^2 (\Lambda^3 H)$
under the action of the subgroup of the integral symplectic group
$\operatorname{Sp}\!(H)$
that stabilises
$S\cup (-S)$
: see Theorem 3·6. Second, we check that each of these generators defines a quadratic relation for
$\operatorname{Gr}^{\Gamma} \mathcal{I}$
: one of the ingredients here is the “topological IHX relation” that has been identified by Gervais and Habegger in [
Reference Gervais and Habegger7
].
Being isomorphic to a lattice in the
$\mathbb{Q}$
-vector space
$\Lambda^2(\Lambda^3 H^\mathbb{Q})/ \ker(B)$
, the group
$\Gamma_2 \mathcal{I}/\Gamma_3 \mathcal{I}$
turns out to be torsion-free. Another output of (the proof of) Theorem B is an explicit description of the quadratic relations. Although it is known to be true with rational coefficients from the above-mentioned work of Hain [
Reference Hain13
], the graded Lie
$\mathbb{Z}$
-algebra
$\operatorname{Gr}^{\Gamma} \mathcal{I}$
may not be quadratically presented (even for g large enough). In this hypothesis, it would still be necessary to determine the relations in higher degrees.
In Section 4, we derive from Theorem A and Theorem B other consequences. (Actually, the reader only interested in these applications of Theorem A and Theorem B, may skip the detailed proofs of the latter, which are contained in Section 2·2–2·3 and Section 3·2–3·4 respectively, and jump directly to Section 4.) The exact structure of the groups
$\Gamma_2 \mathcal{I}/\Gamma_3 \mathcal{I}$
,
$\mathcal{K}/\Gamma_3 \mathcal{I}$
and
$\mathcal{I}/\Gamma_3 \mathcal{I}$
is obtained in Theorem 4·2 and Theorem 4·3. Note that we do not consider here the case of a closed surface. Nonetheless, it is very likely that one could derive from our study similar results for the same subquotients of the Torelli group of the surface
${\Sigma\kern-8.5pt\raise6pt\hbox{$\frown$}}$
that is obtained from
$\Sigma$
by gluing a closed disk along
$\partial \Sigma$
. We leave the study of the closed case, which is more technical, to future work.
Finally, there are two fundamental problems about the lower central series of
$\mathcal{I}$
in connection with other filtrations, to which we can provide (in low degrees) a few new pieces of answer. On the one hand, recall that the “Johnson filtration”
$\mathcal{M}=\mathcal{M}[0] \supset \mathcal{M}[1] \supset \mathcal{M}[2] \supset\,\cdots$
consists of the subgroups of the mapping class group acting trivially on the successive nilpotent quotients of
$\pi_1(\Sigma)$
. On the Torelli group
$\mathcal{M}[1]=\mathcal{I}$
, this filtration is larger than the lower central series, and the following questions arise.
Problem C. Determine the kernel and the image of the homomorphism
from the associated graded of the lower central series of
$\mathcal{I}$
to the associated graded of the Johnson filtration of
$\mathcal{M}$
.
Of course, the map (1·3) is very well understood in degree
$k=1$
thanks to [
Reference Johnson18
]. Subsequent works [
Reference Faes3
,
Reference Morita22
,
Reference Yokomizo30
] also give a nice description of its image in degree
$k=2$
. Besides, it follows from Hain’s results [
Reference Hain13
] that (1·3) is rationally surjective; see also [
Reference Kupers and Randal-Williams19
,
Reference Morita, Sakasai and Suzuki25
] for recent advances in the determination of the kernel of (1·3) with rational coefficients. Having ruled out the possibility of torsion in
$\Gamma_2 \mathcal{I}/\Gamma_3 \mathcal{I}$
, we determine the kernel of (1·3) for
$k=2$
(see Corollary 4·5). Moreover, using the main result of [
Reference Faes2
], we obtain that (1·3) is surjective for
$k=3$
(see Corollary 4·6).
On the other hand, let
$\mathcal{IC}\,:=\, \mathcal{IC}(\Sigma)$
be the monoid of homology cylinders over
$\Sigma$
. The study of
$\mathcal{IC}$
by means of surgery techniques and finite-type invariants has been initiated by Goussarov and Habiro in [
Reference Goussarov8
,
Reference Habiro10
]. Following this study, we are interested in the comparison between the lower central series of
$\mathcal{I}$
and the “Y-filtration”
$\mathcal{IC} = Y_1 \mathcal{IC} \supset Y_2 \mathcal{IC}\supset Y_3 \mathcal{IC} \supset \cdots $
Indeed,
$\mathcal{I}$
embeds into
$\mathcal{IC}$
via the “mapping cylinder” construction, which preserves those filtrations.
Problem D. Determine the kernel and the image of the homomorphism
from the associated graded of the lower central series of
$\mathcal{I}$
to the associated graded of the Y-filtration of
$\mathcal{IC}$
.
The case
$k=1$
is already known [
Reference Habiro10
,
Reference Massuyeau and Meilhan20
]. Besides, the question of the injectivity for arbitrary k, which has already been asked in [11], recently received a partial answer in [
Reference Kupers and Randal-Williams19
] for rational coefficients (in the stable range of the genus g, and up to central elements). Using some of the results of [
Reference Massuyeau and Meilhan21
], we solve Problem D in degree
$k=2$
(see Theorem 4·7).
Conventions.
Given a group G and a normal subgroup N of G, the class modulo N of an element
$x\in G$
is denoted by
$\{x\}_N\in G/N$
, or simply
$\{x\}$
(or even just x) if there is no risk of confusion. For any elements
$x,y\in G$
, we set
${}^xy=xyx^{-1}$
,
$y^x=x^{-1}yx$
and
$[x,y]=xyx^{-1}y^{-1}$
.
If not specified, the ground ring for linear algebra is
$\mathbb{Z}$
. (So, for instance, a “module” means a
$\mathbb{Z}$
-module, i.e., an abelian group.) For
$k\geq 1$
,
$\mathbb{Z}_k \,:=\, \mathbb{Z}/k\mathbb{Z}$
is the cyclic group of order k.
2. Proof of Theorem A
To prove Theorem A, we need to show that the abelian group
is trivial, and for this, we consider the bilinear map
defined by restricting the Lie bracket of
$\operatorname{Gr}^{\Gamma} \mathcal{I}$
to degrees
$1+1$
. Let
$(\gamma_+,\gamma_-)$
be a pair of simple closed curves cobounding a subsurface of genus 1 in
$\Sigma$
, and recall from [
Reference Johnson15
] that
$\mathcal{I}$
is normally generated in
$\mathcal{M}$
by the product
$p\,:=\,T_{\gamma_+} T_{\gamma_-}^{-1}$
of opposite Dehn twists: hence
$ \mathcal{I}_{\operatorname{ab}}$
is generated by
$\{p\}_{[\mathcal{I},\mathcal{I}]}$
as an
$\operatorname{Sp}\!(H)$
-module. Since
$\Upsilon$
is surjective and
$\operatorname{Sp}\!(H)$
-equivariant, the triviality of Q is equivalent to the nullity of the map
By Johnson’s work on the abelianized Torelli group [
Reference Johnson18
], the sources of the map
$\Upsilon$
and
$\upsilon$
are perfectly well understood. We now review his work very briefly.
2·1. The abelianization of the Torelli group
Recall that, by our assumption, the genus g of
$\Sigma$
is at least 3. Then, the main result of [
Reference Johnson18
] is an
$\operatorname{Sp}\!(H)$
-equivariant isomorphism

where
$\mathcal{Q}$
denotes the
$\mathbb{Z}_2$
-affine space of quadratic forms with polar form
$\omega \otimes \mathbb{Z}_2$
, the space
$B_{\leq k}(\mathcal{Q})$
consists of polynomial functions
$\mathcal{Q}\to \mathbb{Z}_2$
of degree at most k, the map
$\beta:\mathcal{I} \to B_{\leq 3}(\mathcal{Q})$
is the Birman–Craggs homomorphism, and the maps defining the above fibered product are as follows: the map
$\Lambda^3 H \to \Lambda^3 H \otimes \mathbb{Z}_2$
is the canonical homomorphism, and the map
$B_{\leq 3}(\mathcal{Q}) \to \Lambda^3 H \otimes \mathbb{Z}_2$
takes the third differential of cubic functions.
Recall that both
$\tau_1$
and
$\beta$
can be computed as follows on the product
$T_{\varepsilon}T_\delta^{-1}$
of opposite Dehn twists along a pair
$(\varepsilon,\delta)$
of disjoint and cobounding, simple closed curves:
\begin{equation} \tau_1\big(T_{\varepsilon}T_\delta^{-1}\big)=-\sum_{i=1}^h u_i \wedge v_i \wedge e\quad \hbox{and} \quad\beta\big(T_{\varepsilon}T_\delta^{-1}\big) =\sum_{i=1}^h \overline{u_i} \, \overline{v_i} \, (\overline{e}+ \overline{1}).\end{equation}
Here
$(u_1,\dots,u_h,v_1,\dots,v_h)$
is a symplectic basis of the subsurface cobounded by
$\varepsilon$
and
$\delta$
(with the orientation induced from
$\Sigma$
), and
$e\,:=\,\{\varepsilon\}$
is the homology class of
$\varepsilon$
and
$\delta$
(which have been oriented so that the oriented boundary of the previous subsurface is
$\varepsilon \cup (-\delta)$
). Furthermore, we use the following notations:
$\overline{1}\,:\,\mathcal{Q} \to \mathbb{Z}_2$
is the constant non-trivial function and, for any
$h\in H$
,
$\overline{h}\,:\,\mathcal{Q} \to \mathbb{Z}_2$
is the evaluation at h.
Remark 2·1. Note that
Besides, the canonical action of
$\operatorname{Sp}\!(H)$
on
$B_{\leq k}(\mathcal{Q})$
preserves the algebra structure, and is such that
$M\cdot \overline{h} = \overline{M(h)}$
for any
$M\in \operatorname{Sp}\!(H)$
and
$h\in H$
.
As a consequence of (2·1), we also have an
$\operatorname{Sp}\!(H)$
-equivariant isomorphism

which can be computed as follows: for any bounding simple closed curve
$\delta$
, we have
\begin{equation} \beta(T_\delta) =\sum_{i=1}^h \overline{u_i} \cdot \overline{v_i}\end{equation}
where
$(u_1,\dots,u_h,v_1,\dots,v_h)$
is a symplectic basis of the subsurface of
$\Sigma$
that is bounded by
$\delta$
.
2·2. Nullity of the map
$\upsilon$
Let
$(\alpha_1,\dots,\alpha_g,\beta_1,\dots,\beta_g)$
be a system of “meridians and parallels” in
$\Sigma$
as shown in Figure 1. These are oriented simple closed curves and, with the arcs to the basepoint shown on the same figure, they define a basis of the free group
$\pi\,:=\,\pi_1(\Sigma, \star)$
with
$\star \in \partial \Sigma$
. The corresponding basis of
$H=H_1(\Sigma;\mathbb{Z})$
is denoted by
In the sequel, we take
$\gamma_+$
and
$\gamma_-$
to be the curves shown in Figure 2.
A system of “meridians and parallels” in
$\Sigma$
.

The cobounding pair
$(\gamma_+,\gamma_-)$
, and the bounding simple closed curves
$c_1,c_2$
.

Let
$\mathcal{S}_p$
be the subgroup of
$\operatorname{Sp}\!(H)$
stabilising the class
$\{p\} \in \mathcal{I}_{\operatorname{ab}}$
of
$p=T_{\gamma_+} T_{\gamma_-}^{-1}$
.
Lemma 2·2. As an
$\mathcal{S}_p$
-module,
$B_{\leq 2}(\mathcal{Q})$
is generated by the following elements:
Proof. It follows from the isomorphism (2·1) and from formulas (2·2) that
$\mathcal{S}_p$
is the subgroup of
$\operatorname{Sp}\!(H)$
fixing both
$a_1 \wedge b_1 \wedge a_2 \in \Lambda^3 H$
and
$\overline{a_1}\, \overline{b_1}\, (\overline{1} + \overline{a_2}) \in B_{\leq 3}(\mathcal{Q})$
. Thus, using Remark 2·1, we easily check that the following elements of
$\operatorname{Sp}\!(H)$
belong to
$\mathcal{S}_p$
:
-
(1)
$C_1$
maps
$b_1$
to
$b_1+a_1$
and fixes all other elements of (2·6); -
(2) for
$i\neq g$
,
$D_i$
maps
$(b_i,b_{i+1})$
to
$(b_i+a_{i+1},b_{i+1}+a_i)$
and fixes all other elements of (2·6); -
(3) for
$i\neq 2$
,
$E_i$
maps
$(a_i,b_i)$
to
$(-b_i,a_i)$
and fixes all other elements of (2·6); -
(4) for
$i,j\geq 3$
,
$F_{ij}$
exchanges
$(a_i,b_i)$
with
$(a_j,b_j)$
and fixes all other elements of (2·6).
Let V be the
$\mathcal{S}_p$
-submodule of
$B_{\leq 2}(\mathcal{Q})$
generated by (2·7). As a
$\mathbb{Z}_2$
-vector space,
$B_{\leq 2}(\mathcal{Q})$
is generated by the following elements:
Hence, it suffices to check that the above elements belong to V:
-
(1) for
$i\geq 4$
, we have
$\overline{a_i}\overline{b_i}\in V$
since
$\overline{a_i}\overline{b_i}= F_{3i} \cdot \overline{a_3}\overline{b_3}$
, which gives the proof for (i); -
(2) we have
$D_2 \cdot \overline{a_2} \overline{b_2}= \overline{a_2} \overline{b_2} + \overline{a_2} \, \overline{a_3}$
, hence
$\overline{a_2} \,\overline{a_3}\in V$
which implies
$\overline{a_2} \,\overline{a_i} =F_{3i}\cdot \overline{a_2}\, \overline{a_3} \in V$
for all
$i\geq 3$
. Next,
$D_1 \cdot \overline{a_1} \overline{b_1}= \overline{a_1} \overline{b_1} + \overline{a_1}\, \overline{a_2}$
hence
$\overline{a_1}\, \overline{a_2}\in V$
. Moreover,
$D_2\cdot \overline{a_1} \overline{b_2}=\overline{a_1} \overline{b_2}+ \overline{a_1}\, \overline{a_3}$
so that
$\overline{a_1} \,\overline{a_3}\in V$
which implies
$\overline{a_1}\, \overline{a_i}=F_{3i}\cdot \overline{a_1}\, \overline{a_3} \in V$
for all
$i\geq 3$
. Finally,
$D_3 \cdot \overline{a_3} \overline{b_3} =\overline{a_3} \overline{b_3} + \overline{a_3}\, \overline{a_4}$
so that
$\overline{a_3}\, \overline{a_4} \in V$
, which implies
$\overline{a_i}\, \overline{a_j} \in V$
for all
$3 \leq i \lt j$
. This proves that elements of type (iii) belong to V; -
(3) for all
$i\geq 3$
, we have
$\overline{a_i} \overline{b_2} = R_{3i}\cdot \overline{a_3} \overline{b_2}\in V$
. Moreover, for all
$j \neq 2$
and
$i\neq j$
, we deduce from (iii) that
$\overline{a_i} \overline{b_j}= E_j \cdot \overline{a_i} \overline{a_j} \in V$
. Thus we have proved that elements of type (ii) belong to V; -
(4) for all
$i \neq 2$
and
$j\neq i$
, we deduce from (ii) that
$\overline{b_i} \overline{b_j}= E_i \cdot \overline{a_i} \overline{b_j} \in V$
, which proves (iv); -
(5) we have
$D_1\cdot \overline{a_1} \overline{b_2}=\overline{a_1} \overline{b_2} + \overline{a_1}$
which implies that
$\overline{a_1}\in V$
. We have
$D_1 \cdot \overline{b_1} \overline{a_2}= \overline{b_1} \overline{a_2} + \overline{a_2}$
and so, by (ii), we get
$\overline{a_2}\in V$
. Next, we have
$C_1 \cdot \overline{b_1} \overline{a_3} =\overline{a_1}\, \overline{a_3} + \overline{b_1} \overline{a_3}+ \overline{a_3}$
which, by (ii) and (iii), implies that
$\overline{a_3} \in V$
. It follows that
$\overline{a_i} = F_{3i} \cdot \overline{a_3}\in V$
for all
$i\geq 3$
, which concludes for (v); -
(6) we have
$C_1 \cdot \overline{b_1}\, \overline{b_2}=\overline{b_1}\, \overline{b_2} + \overline{a_1} \overline{b_2}+ \overline{b_2}$
so, using (ii) and (iv), we obtain
$\overline{b_2} \in V$
. Since
$\overline{b_i}=E_i \cdot \overline{a_i}$
for every
$i\neq 2$
, we then deduce case (vi) from case (v); -
(7) finally,
$C_1 \cdot \overline{b_1} = \overline{b_1}+ \overline{a_1} + \overline{1}$
, and case (vii) follows too.
Lemma 2·3. As an
$\mathcal{S}_p$
-module, the image of
$\upsilon\,:\,\mathcal{K}/[\mathcal{I},\mathcal{I}]\to Q$
is generated by
$\upsilon(T_{c_1})$
and
$\upsilon(T_{c_2})$
, where
$c_1$
and
$c_2$
are the simple closed curves shown in Figure 2.
Proof. Since the isomorphism (2·4) is
$\operatorname{Sp}\!(H)$
-equivariant, we deduce from Lemma 2·2 that the
$\mathcal{S}_p$
-module
$\mathcal{K}/[\mathcal{I},\mathcal{I}]$
is generated by the classes of any
$f_1,f_2,\dots, f_5 \in \mathcal{K}$
such that
Using (2·5) and considering the following bounding curves
$\gamma_1,\gamma_2,\gamma_3$
, we see that
$f_1\,:=\,T_{\gamma_1}$
,
$f_2\,:=\,T_{\gamma_1} T_{\gamma_2}$
and
$f_3\,:=\, T_{\gamma_2} T_{\gamma_3}$
suit our purposes:

Besides, (2·5) also gives
showing that we can take
$f_4 \,:=\, f_1 T_{c_1}$
and
$f_5 \,:=\, f_3 T_{c_2}$
.
Since the map
$\upsilon$
is
$\mathcal{S}_p$
-equivariant and since its source is
$\mathcal{S}_p$
-generated by
$\{\,f_1\},\dots,\{\,f_5\}$
, its image is
$\mathcal{S}_p$
-generated by
$\upsilon(\{\,f_1\}),\dots,\upsilon(\{\,f_5\})$
. Since the curve
$\gamma_i$
is disjoint from
$\gamma_+$
and
$\gamma_-$
for each
$i\in \{1,2,3\}$
, we obviously have
$\upsilon(\{T_{\gamma_i}\})=0$
. Hence, by definition of
$f_1,\dots,f_5$
, the image of
$\upsilon$
is
$\mathcal{S}_p$
-generated by
$\upsilon(\{T_{c_1}\})$
and
$\upsilon(\{T_{c_2}\})$
.
Assume now that both
$[p,T_{c_1}]$
and
$[p,T_{c_2}]$
belong to
$\Gamma_3 \mathcal{I}$
: this will follow from Example 2·5 and Example 2·6, respectively, in the next subsection. Then we have
$\upsilon(T_{c_1})=\upsilon(T_{c_2})=0$
, and Lemma 2·3 implies that the map
$\upsilon$
is zero. Therefore, the group
$Q={[\mathcal{I},\mathcal{K}]}/{[\mathcal{I},[\mathcal{I}, \mathcal{I}]]}$
is trivial, which proves Theorem A.
2·3. The “Push” map and its applications
To prove that
$[p,T_{c_i}] \in \Gamma_3 \mathcal{I}$
for
$i=1,2$
(see Examples 2·5 and 2·6 below), we use the “Push” map. So we start by reviewing this construction.
Let W be a compact, connected, oriented surface with
$b\in\{1,2\}$
boundary components, and fix a connected component
$\delta$
of
$\partial W$
. The surface obtained from W by gluing a closed disk D along
$\delta$
is denoted by
${W\kern-10pt\raise6pt\hbox{$\frown$}}$
. The unit tangent bundle of
${W\kern-10pt\raise6pt\hbox{$\frown$}}$
is denoted by
$UT({W\kern-10pt\raise6pt\hbox{$\frown$}})$
; we choose a base point
$\overrightarrow{\ast} \in UT({W\kern-10pt\raise6pt\hbox{$\frown$}})$
which projects to the center
$\ast \in D$
.
There is a homomorphism
$\mathcal{M}(W)\to \mathcal{M}({W\kern-10pt\raise6pt\hbox{$\frown$}})$
that maps any f to
${f\kern-6pt\raise6pt\hbox{$\frown$}}\,:=\, f\cup \operatorname{id}_D $
. Moreover, there is a anti-homomorphism
$\operatorname{Push}:\pi_1\big(UT({W\kern-10pt\raise6pt\hbox{$\frown$}}),\overrightarrow{\ast}\big) \to \mathcal{M}(W)$
given by
$\operatorname{Push}(\hbox{fiber}) = T_{\delta},$
and by
for any (smooth) oriented simple closed curve
$\gamma$
in
${W\kern-10pt\raise6pt\hbox{$\frown$}}$
, whose unit tangent vector field
$\overrightarrow{\gamma}$
passes through
$\overrightarrow{\ast}$
: here
$\gamma_+$
(resp
$.$
$\gamma_-$
) is the boundary component of a regular neighbourhood
$\hbox{N}(\gamma)$
of
$\gamma$
(containing D) where the orientation induced by
$\hbox{N}(\gamma)$
is the same as (resp. opposite to) the orientation parallel to
$\gamma$
. Then, the Birman’s exact sequence is

see [
Reference Farb and Margalit5
, section 4·2·5] or [
Reference Putman29
], for instance. Furthermore, the “Push” map is injective if
$\chi({W\kern-10pt\raise6pt\hbox{$\frown$}})\lt 0$
, but we shall not need this fact.
Let V be another (compact, connected, oriented) surface with
$c\in\{1,2\}$
boundary components, and assume that one connected component of
$\partial V$
is identified to
$\delta$
. Then, by gluing W and V along
$\delta$
, we get a new surface
$W^+=W \cup V$
, which has
$b+c-2$
boundary components.
There is a homomorphism
$\mathcal{M}(W)\to \mathcal{M}({W}^+)$
that maps any f to
${f}^+\,:=\, f\cup \operatorname{id}_V$
. In the sequel, we consider the following composition

Proposition 2·4. Assume that the curve
$\delta$
bounds in
$W^+$
(i.e.
$b=1$
or
$c=1$
), so that
$W^+$
has at most one boundary component. Then, we have the following:
-
(i)
$\operatorname{Push}^+$
takes values in
$\mathcal{I}(W^+)$
; -
(ii) for any
$u\in \pi_1\big(UT({W\kern-10pt\raise6pt\hbox{$\frown$}}),\overrightarrow{\ast}\big)$
and
$w\in \mathcal{M}(W)$
such that
${w\kern-8.2pt\raise3pt\hbox{$\frown$}}$
acts trivially on the quotient
$\pi_1({W\kern-10pt\raise6pt\hbox{$\frown$}},\ast)/\Gamma_{k} \pi_1({W\kern-10pt\raise6pt\hbox{$\frown$}},\ast)$
for some
$k\geq 2$
, the commutator
$\big[w^+,\operatorname{Push}^+(u)\big]$
in
$\mathcal{M}(W^+)$
belongs to
$\Gamma_{k} \mathcal{I}(W^+)$
.
Proof.
-
(i) By assumption,
$\operatorname{Push}^+(\!\operatorname{fiber}\!)=T_\delta \in \mathcal{M}(W^+)$
is the Dehn twist along a bounding simple closed curve and, so, belongs to
$\mathcal{I}(W^+$
). Thus, it remains to check that, for any simple closed curve
$\gamma \subset {W\kern-10pt\raise6pt\hbox{$\frown$}}$
as in (2·8), we have
$\operatorname{Push}(\overrightarrow{\gamma})\in \mathcal{I}(W^+)$
. Indeed, if
$c=1$
, then
$\gamma_+$
and
$\gamma_-$
cobound a subsurface in
$W^+$
(which contains V). Besides, if
$b=1$
, then (depending on whether
$\gamma$
is separating or not in
${W\kern-10pt\raise6pt\hbox{$\frown$}}$
) either each of
$\gamma_+$
and
$\gamma_-$
bounds a subsurface in
$W \subset W^+$
, or,
$\gamma_+$
and
$\gamma_-$
cobound a subsurface in
$W\subset W^+$
. -
(ii) For
$k=2$
, the statement follows from (i). Indeed it is easily checked with a Mayer–Vietoris argument that
$w^+\in \mathcal{I}(W^+)$
(by distinguishing the case
$b=1$
from the case
$c=1$
). Hence we assume in the sequel that
$k\geq 3$
. It easily follows from (2·8) that the
$\operatorname{Push}$
map is
$\mathcal{M}(W)$
-equivariant in the following sense: for any
$x\in \pi_1\big(UT({W\kern-10pt\raise6pt\hbox{$\frown$}}),\overrightarrow{\ast}\big)$
and
$f\in \mathcal{M}(W)$
, we have
$\operatorname{Push}\big(\overrightarrow{f}_*(x)\big)= f \operatorname{Push}(x)\ f^{-1},$
where
$\overrightarrow{f}:UT({W\kern-10pt\raise6pt\hbox{$\frown$}}) \to UT({W\kern-10pt\raise6pt\hbox{$\frown$}})$
is the fiber-bundle map induced by the diffeomorphism
${f\kern-6pt\raise6pt\hbox{$\frown$}}:{W\kern-10pt\raise6pt\hbox{$\frown$}} \to {W\kern-10pt\raise6pt\hbox{$\frown$}}$
. Hence we have (2·9)Next, we claim that
\begin{equation} \begin{aligned}\big[w^+,\operatorname{Push}^+(u)\big] &=\big(w\, \operatorname{Push}(u)\, w^{-1} \big)^+\, \big(\!\operatorname{Push}^+(u)\big)^{-1} \\&= \operatorname{Push}^+\big(\overrightarrow{w}_*(u)\big) \, \big(\!\operatorname{Push}^+(u)\big)^{-1}.\end{aligned}\end{equation}
$U\,:=\,u^{-1}\, \overrightarrow{w}_*(u)$
belongs to
$\Gamma_k \pi_1\big(UT({W\kern-10pt\raise6pt\hbox{$\frown$}}),\overrightarrow{\ast}\big)$
. Then, we conclude from (2·9) and statement (i) that
$\big[w^+,\operatorname{Push}^+(u)\big] = \operatorname{Push}^+\big(U)$
belongs to
$\Gamma_{k} \mathcal{I}(W^+)$
.
It now remains to prove the above claim. By the assumption on w, we know that
$u^{-1}\, \overrightarrow{w}_*(u) = \tilde{U} \cdot \hbox{fiber}^i$
for some
$\tilde U \in \Gamma_k \pi_1\big(UT({W\kern-10pt\raise6pt\hbox{$\frown$}}),\overrightarrow{\ast}\big)$
and
$i\in \mathbb{Z}$
(both depending on u). Projecting this identity onto
$H_1\big(UT({W\kern-10pt\raise6pt\hbox{$\frown$}});\mathbb{Z}\big)$
, we obtain that
$\overrightarrow{w}_*([u]) = [u] + i\cdot [\hbox{fiber}]$
. But, w acts trivially on
$H_1\big(UT({W\kern-10pt\raise6pt\hbox{$\frown$}});\mathbb{Z}\big)$
, which implies that
$i=0$
and proves the claim.The triviality of the action of
${w\kern-8.2pt\raise3pt\hbox{$\frown$}}$
on
$H_1\big(UT({W\kern-10pt\raise6pt\hbox{$\frown$}});\mathbb{Z}\big)$
can be justified as follows, by distinguishing the case
$b=2$
from
$b=1$
. Note that, in both cases, we have
${w\kern-8.2pt\raise3pt\hbox{$\frown$}} \in \mathcal{K}({W\kern-10pt\raise6pt\hbox{$\frown$}})$
by our assumption on
$k\geq 3$
. If
$b=2$
, then
${W\kern-10pt\raise6pt\hbox{$\frown$}}$
has one boundary component, so that we have a short exact sequence
which splits by choosing a non-singular vector field on
${W\kern-10pt\raise6pt\hbox{$\frown$}}$
; according to [
Reference Johnson16
], the Johnson subgroup
$\mathcal{K}({W\kern-10pt\raise6pt\hbox{$\frown$}})$
acts trivially on homotopy classes of non-singular vector fields; hence,
${w\kern-8.2pt\raise3pt\hbox{$\frown$}}$
preserves the above splitting so that the triviality of its action on
$ H_1({W\kern-10pt\raise6pt\hbox{$\frown$}};\mathbb{Z})$
implies the same on
$H_1\big(UT({W\kern-10pt\raise6pt\hbox{$\frown$}});\mathbb{Z}\big)$
. If
$b=1$
, then
${W\kern-10pt\raise6pt\hbox{$\frown$}}$
is closed and we can find
$w'\in \mathcal{K}(W)$
such that
${w'\kern-10.5pt\raise8pt\hbox{$\frown$}}={w\kern-8.2pt\raise3pt\hbox{$\frown$}}$
; by the same argument as in the previous case applied now to W, w
′ acts trivially on
$H_1\big(UT({W});\mathbb{Z}\big)$
and, since
$H_1\big(UT({W\kern-10pt\raise6pt\hbox{$\frown$}});\mathbb{Z}\big)$
is a quotient of
$H_1\big(UT({W});\mathbb{Z}\big)$
, we deduce that
${w\kern-8.2pt\raise3pt\hbox{$\frown$}}$
acts trivially on
$H_1\big(UT({W\kern-10pt\raise6pt\hbox{$\frown$}});\mathbb{Z}\big)$
.
We now apply Proposition 2·4 in the following two examples, where
$W^+$
is our reference surface
$\Sigma$
and we take
$k\,:=\,3$
.
Example 2·5. For the decomposition
$W \cup V$
of
$\Sigma$
shown below, take
$u\,:=\,\overrightarrow{\gamma}$
and
$w\,:=\,T_d$
. Then, we have
$\operatorname{Push}(u)=T_{\gamma_+} T_{\gamma_-}^{-1}$
and we deduce that
$\left[T_d,T_{\gamma_+} T_{\gamma_-}^{-1}\right]\in \Gamma_3 \mathcal{I}(\Sigma)$
.

Example 2·6. For the decomposition
$V \cup W$
of
$\Sigma$
shown below, take
$u\,:=\,\overrightarrow{\gamma}$
and
$w\,:=\,T_d$
. Then, we have
$\operatorname{Push}(u)=T_{\gamma_+} T_{\gamma_-}^{-1}$
and we deduce that
$\left[T_d,T_{\gamma_+} T_{\gamma_-}^{-1}\right]\in \Gamma_3 \mathcal{I}(\Sigma)$
.

3. Proof of Theorem B
In this section, we define the map B and we prove Theorem B.
3·1. The map B
We embed
$\Lambda^4 H^\mathbb{Q}$
into the space
$S^2(\Lambda^2 H^\mathbb{Q})$
, by sending any 4-vector
$a\wedge b \wedge c \wedge d$
to
$(a\wedge b) \cdot (c \wedge d) + (a\wedge c) \cdot (d \wedge b) +(a\wedge d) \cdot (b \wedge c)$
. (In the diagrammatic setting that is mentioned below in Remark 3·1, this embedding corresponds to the “IHX” relations.) Then we consider the
$\mathbb{Q}$
-linear map
defined by
and
\begin{equation} B^{(2)}\big((x_1\wedge x_2 \wedge x_3)\wedge (y_1\wedge y_2 \wedge y_3) \big)= -\frac{1}{4} \begin{vmatrix}\omega(x_1,y_1) & \omega(x_1,y_2) & \omega(x_1,y_3)\\\omega(x_2,y_1) & \omega(x_2,y_2) & \omega(x_2,y_3)\\\omega(x_3,y_1) & \omega(x_3,y_2) & \omega(x_3,y_3)\\\end{vmatrix}.\end{equation}
We refer to the map B as the diagrammatic bracket since, as specified in the next remark, it is also given by restricting the Lie bracket of the space of “symplectic Jacobi diagrams”.
Remark 3·1. There is a
$\mathbb{Q}$
-algebra of “symplectic Jacobi diagrams”, denoted by
$\mathcal{A}(H^\mathbb{Q})$
in [11], whose multiplication is a diagrammatic analogue of the Moyal–Weyl product. It is a graded Hopf
$\mathbb{Q}$
-algebra, whose primitive part
$\mathcal{A}^c(H^\mathbb{Q})$
consists of connected Jacobi diagrams. It turns out that, in degree
$1+1$
, its Lie bracket
is essentially the above map B: indeed, according to [15, lemma 5·4], the
$B^{(0)}$
component corresponds to 0-looped diagrams (i.e
$.$
trees) in the target, while the
$B^{(2)}$
component corresponds to 2-looped diagrams (i.e
$.$
multiples of the theta graph).
It is proved in [15, lemma 5·6 and (5·5)] that
$\ker(B)=R_2^\mathbb{Q}$
, i.e
$.$
the diagrammatic bracket B and the “topological” bracket
$J_2^\mathbb{Q}\,:\,\operatorname{Lie}_2(\Lambda^3 H^\mathbb{Q})\to (\Gamma_2\mathcal{I}/ \Gamma_3 \mathcal{I})\otimes \mathbb{Q}$
share the same kernel. In the sequel, we will just need the inclusion
$R_2^\mathbb{Q} \subset \ker(B)$
which follows also from Proposition 3·2 below.
To state this proposition, we need two ingredients. On the one hand, we consider the second Johnson homomorphism
$\tau_2:\mathcal{K} \to {S^2(\Lambda^2 H^\mathbb{Q})}/{\Lambda^4 H^\mathbb{Q}}$
. According to [
Reference Morita22
,
Reference Morita23
], it is determined by the fact that
for any bounding simple closed curve
$\gamma$
, where
$(u_1,\dots,u_h,v_1,\dots,v_h)$
is a symplectic basis of the subsurface of
$\Sigma$
bounded by
$\gamma$
.
On the other hand, we consider the second core of the Casson invariant
$d''\,:\,\mathcal{K} \to \mathbb{Q}$
, which appeared in Auclair’s thesis [
Reference Auclair1
, Theorem 4·4·6]. This is an alternative to Morita’s core of the Casson invariant
$d:\mathcal{K} \to \mathbb{Z}$
[
Reference Morita22
,
Reference Morita23
]. With the knowledge of
$\tau_2$
, these two homomorphisms are equivalent one to the other: specifically, we have
where
$d'\,:=\,-\overline{d'}\circ \tau_2$
and
$\overline{d'}\,:\,S^2(\Lambda^2 H^\mathbb{Q})/\Lambda^4 H^\mathbb{Q} \to \mathbb{Q}$
is defined by
Originally, both homomorphisms are defined from the Casson invariant and, a posteriori, they are determined by the formulae
for any bounding simple closed curve
$\gamma$
, where h denotes the genus of the subsurface of
$\Sigma$
bounded by
$\gamma$
. From our perspectives (see Remark 3·3 below), we find more natural to work here with d
$''$
rather than d.
Note that both
$\tau_2$
and d
$''$
can be restricted to
$\Gamma_2 \mathcal{I}=[\mathcal{I},\mathcal{I}]$
, and they both vanish on
$\Gamma_3 \mathcal{I}$
.
Proposition 3·2. We have
$(\tau_2,d'') \circ J_2^\mathbb{Q} = B$
.
Proof. That
$\tau_2 \circ J_2^\mathbb{Q}=B^{(0)}$
is well-known, and follows from the fact that the sequence of all Johnson homomorphisms
$\tau_k$
(
$k\geq 1$
) defines a Lie algebra map on the associated graded of the “Johnson filtration” [
Reference Morita24
]. That
$d'' \circ J_2^\mathbb{Q}=B^{(2)}$
is proved as follows. Let
$u,v\in \mathcal{I}$
and assume, without loss of generality, that we have
for some
$x_1,x_2,x_3,y_1,y_2,y_3 \in H$
. We wish to prove that
\begin{equation*}d''([u,v])= -\frac{1}{4} \begin{vmatrix}\omega(x_1,y_1) & \omega(x_1,y_2) & \omega(x_1,y_3)\\\omega(x_2,y_1) & \omega(x_2,y_2) & \omega(x_2,y_3)\\\omega(x_3,y_1) & \omega(x_3,y_2) & \omega(x_3,y_3)\\\end{vmatrix}.\end{equation*}
But this follows easily from (3·5), the above definition of d
$'$
and Morita’s formula [
Reference Morita22
, proposition 5·1] which, in our notations, states that
Remark 3·3. Alternatively, one can obtain Proposition 3·2 using the LMO homomorphism
$Z\,:\,\mathcal{I} \to \mathcal{A}(H^\mathbb{Q})$
that has been introduced in [11]. Indeed,
$\tau_2$
coincides with the tree part of the degree 2 part
$Z_2$
of Z [
Reference Massuyeau and Meilhan21
, lemma 4·3], while d
$''$
is exactly the coefficient of the theta graph in
$Z_2$
[
Reference Massuyeau and Meilhan21
, lemma 7·3]. Then, the proposition follows directly from [
Reference Massuyeau and Meilhan21
, (4·5)] and Remark 3·1.
3·2. Strategy for the proof of Theorem B
We are interested in the submodule
of
$\Lambda^2(\Lambda^3 H)$
. In the previous subsection, we have justified that K contains the kernel of
$J\,:\,\Lambda^2(\Lambda^3 H) \to \Gamma_2 \mathcal{I}/\Gamma_3 \mathcal{I}$
. To prove Theorem B, we now need to show that
$J(K)=0$
.
In the sequel, we use the following notation and terminology. We fix a symplectic basis
$S\,=\,\{a_1,\dots,a_g,b_1,\dots,b_g\}$
of H as in (2·6). An elementary trivector is an element
$s_1 \wedge s_2 \wedge s_3 \in \Lambda^3 H$
with
$s_1,s_2,s_3 \in S$
. The wedge of two elementary trivectors is denoted by
Remark 3·4. A basis of the free module
$\Lambda^2(\Lambda^3 H)$
can be extracted from the list
by deleting zeroes and fixing signs among repetitions, which means the following: if the element
$\mathsf{\bigwedge}\!\left({s_1},{s_2},{s_3}\,;\,{s'_1},{s'_2},{s'_3}\right)$
is zero, then it is deleted from the list; otherwise, among all the repetitions of
$\pm \mathsf{\bigwedge}\!\left({s_1},{s_2},{s_3}\,;\,{s'_1},{s'_2},{s'_3}\right)$
in the above list, we choose either
$\mathsf{\bigwedge}\!\left({s_1},{s_2},{s_3}\,;\,{s'_1},{s'_2},{s'_3}\right)$
or
$-\mathsf{\bigwedge}\!\left({s_1},{s_2},{s_3}\,;\,{s'_1},{s'_2},{s'_3}\right)$
. Thus, such a basis of
$\Lambda^2(\Lambda^3 H)$
is indexed by unordered pairs
$\{I,J\}$
of 3-element subsets I,J of S such that
$I\neq J$
(the corresponding element of the basis being equal to
$\pm \big({i_1}\wedge {i_2} \wedge {i_3}\big)\wedge \big( {j_1}\wedge {j_2} \wedge {j_3}\big)$
if I, J write
$\{i_1,i_2,i_3\}$
,
$\{\,j_1,j_2,j_3\}$
respectively), and any two choices of such bases differ by some sign changes.
We denote by
$\widetilde{\,\cdot\,}$
the involution of S that is defined by
$\widetilde{a_i}=b_i$
and
$\widetilde{b_i}=a_i$
. A self-contraction of an elementary trivector
$s_1 \wedge s_2 \wedge s_3$
is a pair
$\{s_i,s_j\}$
such that
$s_i= \widetilde{s_j}$
. A mixed contraction between two elementary trivectors
$s_1 \wedge s_2 \wedge s_3$
and
$s'_1 \wedge s'_2 \wedge s'_3$
is a pair
$\{s_i,s'_j\}$
such that
$s'_j = \widetilde{s_i}$
. There is the decomposition
where
$V_m$
denotes the submodule generated by the elements
$\mathsf{\bigwedge}\!\left({s_1},{s_2},{s_3}\,;\,{s'_1},{s'_2},{s'_3}\right)$
with m mixed contractions between the elementary trivectors
$s_1 \wedge s_2 \wedge s_3$
and
$s'_1 \wedge s'_2 \wedge s'_3$
. Furthermore,
$V_1$
decomposes itself as
where
$V_{1,n}$
is the submodule generated by the elements
$\mathsf{\bigwedge}\!\left({s_1},{s_2},{s_3}\,;\,{s'_1},{s'_2},{s'_3}\right)$
with a single mixed contraction between
$s_1 \wedge s_2 \wedge s_3$
and
$s'_1 \wedge s'_2 \wedge s'_3$
, and a total of n self-contractions which are disjoint from the mixed contraction. Therefore, we have
where
$U_0\,:=\,V_0$
,
$U_1\,:=\,V_{1,0}$
,
$U_2\,:=\, V_{1,1} \oplus V_2$
and
$U_3\,:=\, V_{1,2} \oplus V_3$
. We can extract bases of
$V_m$
and
$V_{1,n}$
from the above generating sets by deleting zeroes and fixing signs among repetitions, as explained in Remark 3·4.
Lemma 3·5. We have
$K = U_0 \oplus (K \cap U_1) \oplus(K \cap U_2) \oplus (K \cap U_3).$
Proof. We start by observing that
where
$W_r$
denotes the subspace generated by elements of the form
$(s_1 \wedge s_2)\cdot (s_3 \wedge s_4)$
showing exactly r pairs
$\{s_i,s_j\}$
of the form
$\{s,\widetilde{s}\}$
with
$s\in S$
. If
$r=2$
, we require that those two pairs are disjoint.
Note that, trivially,
$U_0 \subset K$
. Let
$k\in K$
. By (3·6), there exist
$k_0\in U_0,\dots,k_3\in U_3$
such that
$k=k_0+\cdots +k_3$
. Since
$B^{(0)}(U_i)$
is contained in
$W_{i-1}$
for
$i\geq 1$
, and since
each of
$B^{(0)}(k_1), B^{(0)}(k_2)$
and
$B^{(0)}(k_3)$
is trivial. Since
$B^{(2)}(k_1)=B^{(2)}(k_2)=0$
, it follows that
$k_i \in K \cap U_i$
for
$i=1,2$
. Finally, since
$0= B^{(2)}(k) = B^{(2)}(k_3),$
we have
$k_3 \in K \cap U_3$
as well.
In the sequel, we shall also consider the subgroup
of
$\operatorname{Sp}\!(H)$
that is generated by the transformations
$E_i$
and
$F_{ij}$
, where:
-
(i)
$E_i$
maps
$(a_i,b_i)$
to
$(-b_i,a_i)$
and fixes all other elements of S; -
(ii)
$F_{ij}$
exchanges
$(a_i,b_i)$
with
$(a_j,b_j)$
and fixes all other elements of S.
Observe that the G-action preserves the decomposition (3·6) of
$\Lambda^2(\Lambda^3 H)$
, as well as the resulting decomposition of K in Lemma 3·5. Then, the proof of Theorem B splits into two parts:
-
(i) in Section 3·3, we identify a G-generating system of K by finding a G-generating system of
$K\cap U_i$
for each
$i\in \{0,1,2,3\}$
; -
(ii) in Section 3·4, we show that J vanishes on this G-generating system of K.
3·3. A finite generating system of K
Set
$\varepsilon(s)\,:=\,\omega(s,\widetilde{s})$
for all
$s\in S$
. It is straightforward to check that the following elements of
$\Lambda^2(\Lambda^3 H)$
belong to
$K=\ker(B) \cap \Lambda^2(\Lambda^3 H) $
:

Theorem 3·6. As a G-submodule of
$\Lambda^2(\Lambda^3 H)$
, K is generated by the following 26 elements:
-
$(\mathcal{R}_0)$
$\mathsf{\bigwedge}\!\left({a_1},{a_2},{a_3}\,;\,{a_4},{a_5},{a_6}\right)$
,
$\mathsf{\bigwedge}\!\left({a_1},{b_1},{a_2}\,;\,{a_3},{a_4},{a_5}\right)$
,
$\mathsf{\bigwedge}\!\left({a_1},{b_1},{a_2}\,;\,{a_3},{b_3},{a_4}\right)$
,
$\mathsf{\bigwedge}\!\left({a_1},{a_2},{a_3}\,;\,{a_3},{a_4},{a_5}\right)$
,
$\mathsf{\bigwedge}\!\left({a_1},{b_1},{a_2}\,;\,{a_2},{a_3},{a_4}\right)$
,
$\mathsf{\bigwedge}\!\left({a_1},{b_1},{a_2}\,;\,{a_2},{a_3},{b_3}\right)$
,
$\mathsf{\bigwedge}\!\left({a_1},{a_2},{a_3}\,;\,{a_2},{a_3},{a_4}\right)$
; -
$(\mathcal{R}_1)$
$\mathsf{D}\!\left({a_{1}},{a_{2}}\,;\,{a_5},{a_{3}}\,;\,{a_{3}},{a_{4}}\right)$
,
$\mathsf{D}\!\left({a_{1}},{a_{2}}\,;\,{a_{3}},{a_{4}}\,;\,{a_{3}},{a_{4}}\right)$
,
$\mathsf{D}\!\left({a_{1}},{a_{2}}\,;\,{a_{3}},{b_{1}}\,;\,{a_{3}},{a_{4}}\right)$
,
$\mathsf{D}\!\left({a_{3}},{a_{1}}\,;\,{a_4},{a_{2}}\,;\,{a_{2}},{a_{3}}\right)$
,
$\mathsf{D}\!\left({a_{3}},{a_{1}}\,;\,{b_{1}},{a_{2}}\,;\,{a_{2}},{a_{3}}\right)$
,
$\mathsf{D}\!\left({a_1},{a_2}\,;\,{a_4},{a_3}\,;\,{a_2},{a_{1}}\right)$
,
$\mathsf{IHX}_1\!\left({a_{1}}\,;\,{a_{2}},{a_{3}},{a_{4}}\,;\,{b_{1}}\right)$
; -
$(\mathcal{R}_2)$
$\mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_4} & {a_5}\!\\{a_3} & {b_3}\! \end{array}\right)$
,
$\mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_4} & {b_4}\!\\{a_3} & {b_3}\! \end{array}\right)$
,
$\mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_2} & {b_1}\!\\{a_3} & {b_3}\! \end{array}\right)$
,
$\mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_2} & {a_4}\!\\{a_3} & {b_3}\! \end{array}\right)$
,
$\mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{b_1} & {a_4}\!\\{a_3} & {b_3}\! \end{array}\right)$
,
$\mathsf{T}\!\left({a_1}\,;\,{a_2} ,{a_3},{a_4}\right)$
,
$\mathsf{IHX}_2\!\left({a_1},{a_2}\,;\,{a_3}\,;\,{a_4}\right)$
,
$\mathsf{IHX}_2\!\left({a_1},{a_2}\,;\,{a_3}\,;\,{b_1}\right)$
; -
$(\mathcal{R}_3)$
$\mathsf{D}\!\left({a_1},{b_1}\,;\,{a_2},{b_2}\,;\,{a_3},{b_3}\right)$
,
$\mathsf{D}\!\left({a_1},{b_1}\,;\,{a_2},{a_3}\,;\,{a_4},{b_4}\right)$
,
$\mathsf{IHX}_3\!\left({a_1},{a_2}\,;\,{a_3}\right)$
,
$\mathsf{IHX}'_3\!\left({a_1},{a_2}\,;\,{a_3},{a_4}\right)$
.
In the above statement, it is understood that we only consider the elements making sense in the given genus: for instance, the element
$\mathsf{\bigwedge}\!\left({a_1},{a_2},{a_3}\,;\,{a_4},{a_5},{a_6}\right)$
in (
$\mathcal{R}_0)$
has to be removed in the cases
$g\lt 6$
. (Recall that our permanent assumption is that
$g\geq 3$
.)
The proof of Theorem 3·6, which is given below, consists in proving that the family (
$\mathcal{R}_i)$
is a G-generating system of
$K\cap U_i$
for each case
$i=0$
,
$i=1$
,
$i=2$
and
$i=3$
. Actually, as we shall see, the proofs are rather different in nature from one case to another.
3·3·1. A G-generating system of
$K \cap U_0$
By its very definition, the module
$K\cap U_0=U_0=V_0$
is generated by wedge of elementary trivectors without mixed contractions, i.e
$.$
the elements
Let
$N:S \to \{1,\dots,g\}$
be the map defined by
$N(a_i)=N(b_i)=i$
. We consider an element
$\Lambda\,:=\, \mathsf{\bigwedge}\!\left({s_1},{s_2},{s_3}\,;\,{s'_1},{s'_2},{s'_3}\right)$
of the form (3·8), and let
If
$n=0$
, then
$\pm \Lambda$
is in the G-orbit of
$\mathsf{\bigwedge}\!\left({a_1},{a_2},{a_3}\,;\,{a_4},{a_5},{a_6}\right)$
, or
$\mathsf{\bigwedge}\!\left({a_1},{b_1},{a_2}\,;\,{a_3},{a_4},{a_5}\right)$
, or
$\mathsf{\bigwedge}\!\left({a_1},{b_1},{a_2}\,;\,{a_3},{b_3},{a_4}\right)$
. If
$n=1$
, then
$\pm \Lambda$
is in the G-orbit of
$\mathsf{\bigwedge}\!\left({a_1},{a_2},{a_3}\,;\,{a_3},{a_4},{a_5}\right)$
or
$\mathsf{\bigwedge}\!\left({a_1},{b_1},{a_2}\,;\,{a_2},{a_3},{a_4}\right)$
, or
$\mathsf{\bigwedge}\!\left({a_1},{b_1},{a_2}\,;\,{a_2},{a_3},{b_3}\right)$
. If
$n=2$
, then
$\pm \Lambda$
is in the G-orbit of
$\mathsf{\bigwedge}\!\left({a_1},{a_2},{a_3}\,;\,{a_2},{a_3},{a_4}\right)$
. Thus,
$(\mathcal{R}_0)$
is a G-generating system of
$K \cap U_0$
.
3·3·2. A G-generating system of
$K \cap U_1$
As in the proof of Lemma 3·5, we consider here the subspace
$W_0$
of
$S^2(\Lambda^2 H^\mathbb{Q})/\Lambda^4 H^\mathbb{Q}$
generated by the elements
$(s_1\wedge s_2)\cdot (s_3\wedge s_4)$
showing no contraction. This decomposes as a direct sum
indexed by the unordered quadruplets
$\{s_1,s_2,s_3,s_4\}\in S^4/\mathfrak{S}_4$
showing no contraction and at most 2 repetitions, where
$W_{s_1,s_2,s_3,s_4}$
is the subspace generated by
$(s_{\sigma(1)}\wedge s_{\sigma(2)})\cdot (s_{\sigma(3)}\wedge s_{\sigma(4)})$
for
$\sigma \in \mathfrak{S}_4$
. Similarly, the submodule
$U_1=V_{1,0}$
of
$\Lambda^2(\Lambda^3 H)$
decomposes as a direct sum
indexed by the same quadruplets, where we denote by
$U_{s_1,s_2,s_3,s_4}$
the submodule generated by
$\mathsf{\bigwedge}\!\left({s_{\sigma(1)}},{s_{\sigma(2)}},{a_i}\,;\,{b_i},{s_{\sigma(3)}}, s_{\sigma(4)}\right)$
for
$i\in\{1,\dots,g\}$
and
$\sigma \in \mathfrak{S}_4$
. The map
$B^{(0)}\,:\,U_1\,\to\,W_0$
preserves the above decompositions, so that we have
Moreover, the map
$B^{(0)}$
is G-equivariant: so, a generating system of the G-module
$K\,\cap\,U_1$
is obtained by determining a generating system of the module
$K \cap U_{s_1,s_2,s_3,s_4}$
for a representative
$\{s_1,s_2,s_3,s_4\}$
in each G-orbit. But, an unordered quadruplet
$\{s_1,s_2,s_3,s_4\}$
with no contraction and at most 2 repetitions is G-equivalent to either
$\{a_1,a_2,a_3,a_4\}$
, or
$\{a_1,a_2,a_3,a_3\}$
, or
$\{a_1,a_1,a_2,a_2\}$
.
The following three lemmas deal with the above three subcases in this order and, all together, they prove that
$(\mathcal{R}_1)$
is a G-generating system of
$K \cap U_1$
.
Lemma 3·7. If
$g\geq 4$
, the module
$K\cap U_{a_1,a_2,a_3,a_4}$
is generated by:
-
(i)
$\mathsf{D}\!\left({a_{\sigma(1)}},{a_{\sigma(2)}}\,;\,{a_i},{a_{\sigma(3)}}\,;\,{}{a_{\sigma(3)} , {a_{\sigma(4)}}}\right)$
with
$i\geq 5$
,
$\sigma \in \mathfrak{S}_4$
; -
(ii)
$\mathsf{D}\!\left({a_{\sigma(1)}},{a_{\sigma(2)}}\,;\,{a_{\sigma(3)}},{{a_{\sigma(4)}}}\,;\,{a_{\sigma(3)}},{a_{\sigma(4)}}\right)$
with
$\sigma \in \mathfrak{S}_4$
; -
(iii)
$\mathsf{D}\!\left({a_{\sigma(1)}},{a_{\sigma(2)}}\,;\,{a_{\sigma(3)}},{{b_{\sigma(1)}}}\,;\,{a_{\sigma(3)}}, {a_{\sigma(4)}}\right)$
with
$\sigma \in \mathfrak{S}_4$
; -
(iv)
$\mathsf{IHX}_1\!\left({a_{\sigma(1)}}\,;\,{a_{\sigma(2)}},{a_{\sigma(3)}},{{a_{\sigma(4)}}}\,;\ {b_{\sigma(1)}}\right)$
with
$\sigma \in \mathfrak{S}_4$
.
Lemma 3·8. The module
$K \cap U_{a_1,a_2,a_3,a_3}$
is generated by:
-
(i)
$\mathsf{D}\!\left({a_{3}},{a_{\sigma(1)}}\,;\,{a_i},{a_{\sigma(2)}}\,;\,{{a_{3}}},{a_{\sigma(2)}}\right)$
with
$i\geq 4$
,
$\sigma \in \mathfrak{S}_2$
; -
(ii)
$\mathsf{D}\!\left({a_{3}},{a_{\sigma(1)}}\,;\,{b_{\sigma(1)}},{a_{\sigma(2)}}\,;\,{{a_{\sigma(2)}}},{a_{3}}\right)$
with
$\sigma \in \mathfrak{S}_2$
.
Lemma 3·9. The module
$K\cap U_{a_1,a_1,a_2,a_2}$
is generated by
$\mathsf{D}\!\left({a_1},{a_2}\,;\,{a_i},{a_3}\,;\,{a_2},{a_1}\right)$
with
$i\geq 4$
.
Proof of Lemma 3·7. The module
$U\,:=\,U_{a_1,a_2,a_3,a_4}$
is free, and a basis is obtained from the following list by deleting zeroes and fixing signs among repetitions, as explained in Remark 3·4:
We choose such a basis of U and we denote it by
$\{e_{J,i}\}_{J,i}$
, which is indexed by 2-element subsets
$J\subset \{1,2,3,4\}$
together with an element
$i \in \{1,\dots, g\}\setminus J$
; specifically, we have
$e_{J,i}= \pm\mathsf{\bigwedge}\!\left({a_{j}},{a_{j'}},{a_i}\,;\,{b_i},{a_{k}},{a_{k'}}\right)$
writing J and
$\overline{J}=\{1,2,3,4\}\setminus J$
as
$\{\,j,j'\}$
and
$\{k,k'\}$
, respectively. Let U
′ be the submodule of U (freely) generated by the previous elements
$e_{J,i}$
for
$i\leq 4$
(hence
$J\subset \{1,2,3,4\}$
is a 2-element subset and
$i\in \overline{J}$
). When viewed as a relation in U, any element of type (i) identifies a basis element
$e_{J,i}$
with
$\pm e_{J,k}$
for
$i\geq 5$
,
$J\subset \{1,2,3,4\}$
of cardinality 2 and some
$k\in \overline{J}$
. Similarly, for any
$J\subset \{1,2,3,4\}$
of cardinality 2, writing
$\overline{J}=\{i,k\}$
, the basis element
$e_{J,i}$
is identified with
$\pm e_{J,k}$
if an appropriate element of type (ii) is viewed as a relation in U. Therefore, the inclusion of U
′ in U induces an isomorphism
So, we can assume for the rest of the proof that
$g=4$
, and we need to show that the map
$B^{(0)}$
induces an injection from
$U/{\langle \, \hbox{(ii)}, \hbox{(iii)}, \hbox{(iv)} \, \rangle}$
to
${S^2(\Lambda^2 H^\mathbb{Q})}/{\Lambda^4 H^\mathbb{Q}}$
. By the above discussion, the module
$U/{\langle \, \hbox{(ii)} \, \rangle}$
is free of rank 6, with basis
$\{e_J\}_J$
indexed by 2-element subsets J of
$\{1,2,3,4\}$
where
$e_J = \pm\mathsf{\bigwedge}\!\left({a_{j}},{a_{j'}},{a_i}\,;\,{b_i},{a_{i}},{a_{k}}\right)$
writing
$J=\{\,j,j'\}$
and
$\overline{J}=\{i,k\}$
. When viewed as a relation in
$U/{\langle \, \hbox{(ii)} \, \rangle}$
, any element of type (iii) identifies a basis element
$e_J$
with
$\pm e_{\overline{J}}$
for a 2-element subset J of
$\{1,2,3,4\}$
. Consequently, the module
$U/{\langle \, \hbox{(ii)}, \hbox{(iii)}\, \rangle}$
is free of rank 3, with basis
$\{e_P\}_P$
indexed by partitions
$P=J \sqcup \overline{J}$
of
$\{1,2,3,4\}$
into two 2-element subsets.
On the other hand, the
$\mathbb{Q}$
-vector space
$W\,:=\,W_{a_1,a_2,a_3,a_4}$
is generated by
with the single relation
The map
$B^{(0)}:U/{\langle \, \hbox{(ii)}, \hbox{(iii)} \, \rangle} \to W$
sends the basis element
$e_{P}$
to
$\pm (a_{j} \wedge a_{j'})\cdot (a_{k} \wedge a_{k'})$
writing
$P=\{\,j,j'\}\sqcup \{k,k'\}$
. Finally, when viewed as a relation in
$U/{\langle \, \hbox{(ii)}, \hbox{(iii)} \, \rangle}$
, any element of type (iv) goes to (3·11). The conclusion follows.
Proof of Lemma 3·8. The module
$U\,:=\,U_{a_1,a_2,a_3,a_3}$
is free, and a basis is obtained from the following list by deleting zeroes and fixing signs among repetitions, as explained in Remark 3·4:
We choose such a basis of U and denote it by
$\{e_{j,i}\}_{j,i}$
, which is indexed by
$j\in \{1,2\}$
and
$i\not \in \{\,j,3\}$
; specifically, we have
$e_{j,i} = \pm \mathsf{\bigwedge}\!\left({a_3},{a_j},{a_i}\,;\,{b_i},{a_{\overline{j}}},{a_3}\right)$
, where
$\overline{j}$
is the element of
$\{1,2\}$
not equal to j. When viewed as a relation in U, any element of type (i) identifies a basis element
$e_{j,i}$
with
$\pm e_{j,\overline{j}}$
for
$i\geq 4$
and
$j\in \{1,2\}$
, and any element of type (ii) identifies
$e_{1,2}$
with
$\pm e_{2,1}$
. It follows that the module
$U/{\langle \, \hbox{(i)}, \hbox{(ii)} \, \rangle}$
is free of rank 1.
On the other hand, the
$\mathbb{Q}$
-vector space
$W\,:=\,W_{a_1,a_2,a_3,a_3}$
is 1-dimensional, generated by
$(a_1\wedge a_3) \cdot (a_2 \wedge a_3)$
. Since
$B^{(0)}$
maps
$e_{1,2}$
to
$\pm (a_1\wedge a_3) \cdot (a_2 \wedge a_3)$
, it induces an injection
$U/{\langle \, \hbox{(i)}, \hbox{(ii)} \, \rangle} \to W$
.
Proof of Lemma 3·9. The module
$U\,:=\,U_{a_1,a_1,a_2,a_2}$
is free, and a basis is obtained from the following list by deleting zeroes and fixing signs among repetitions, as explained in Remark 3·4:
We choose such a basis of U and denote it by
$\{e_i\}_{i\geq 3}$
, having
$e_i\,=\,\pm \mathsf{\bigwedge}\!\left({a_1},{a_2},{a_i}\,;\,{b_i},{a_2},{a_1}\right)$
. When viewed as a relation in U, any element of type (i) identifies a basis element
$e_i$
with
$\pm e_3$
for
$i\geq 3$
. It follows that the module
$U/{\langle \, \hbox{(i)} \, \rangle}$
is free of rank 1.
Besides, the
$\mathbb{Q}$
-vector space
$W\,:=\,W_{a_1,a_1,a_2,a_2}$
is 1-dimensional, generated by
$(a_1\,\wedge\,a_2)\,\cdot\,(a_1\,\wedge\,a_2)$
. Since
$B^{(0)}$
maps
$e_{3}$
to
$\pm (a_1\wedge a_2) \cdot (a_1 \wedge a_2)$
, it induces an injection
$U/{\langle \, \hbox{(i)} \, \rangle}\,\to\,W$
.
3·3·3. A G-generating system of
$K \cap U_2$
As in the proof of Lemma 3·5, we consider now the subspace
$W_1$
of
$S^2(\Lambda^2 H^\mathbb{Q})/\Lambda^4 H^\mathbb{Q}$
generated by the elements
$(s_1\wedge s_2)\cdot (s_3\wedge s_4)$
showing a single contraction. This decomposes as a direct sum
indexed by the unordered pairs
$\{s,s'\}\in S^2/\mathfrak{S}_2$
such that
$s'\neq \widetilde{s}$
, where
$W_{s,s'}$
denotes the subspace generated by the elements
$(s \wedge x)\cdot (s'\wedge \widetilde{x})$
for all
$x\in S$
. Similarly, the submodule
$U_2=V_{1,1} \oplus V_2$
decomposes as a direct sum
indexed by the same pairs, where
$U_{s,s'}$
denotes the submodule generated by the elements
$\mathsf{\bigwedge}\!\left({s},{x},{y}\,;\,{s'},{\widetilde{x}},{\widetilde{y}}\right)$
for all
$x,y\in S$
and
$\mathsf{\bigwedge}\!\left({s},{s'},{p}\,;\,{\widetilde{p}},{q},{\widetilde{q}}\right)$
for all
$p\in S,q \in S\setminus \{s,s',\widetilde{s},\widetilde{s'}\}$
. The map
$B^{(0)}:U_2 \to W_1$
preserves the above decompositions, so that we have
Since
$B^{(0)}$
is G-equivariant, a G-generating system of
$K\cap U_2$
is obtained by determining a generating system of
$K \cap U_{s,s'}$
for a representative
$\{s,s'\}$
in each G-orbit. Thus, we are reduced to determine a generating system of
$K\cap U_{a_1,a_2}$
and
$K\cap U_{a_1,a_1}$
. This is achieved by the following two lemmas which prove that
$(\mathcal{R}_2)$
is a G-generating system of
$K \cap U_2$
.
Lemma 3·10. The module
$K \cap U_{a_1,a_2}$
is generated by:
-
(i)
$\mathsf{S}\Big({a_{\sigma(1)}},{a_{\sigma(2)}}\,;\,\begin{array}{cc}{p} & {q}\!\\{r} & {\widetilde{r}}\! \end{array}\Big)$
with
$\sigma\in \mathfrak{S}_2$
,
$r\not\in \{p,\widetilde{p},q,\widetilde{q},a_1,a_2,b_1,b_2\}$
and
$p,q,a_{\sigma(1)},b_{\sigma(2)}$
pairwise different; -
(ii)
$\mathsf{IHX}_2\!\left({a_{\sigma(1)}},{a_{\sigma(2)}}\,;\,{p}\,;\,{q}\right)$
with
$\sigma\in \mathfrak{S}_2$
,
$p\not\in \{a_1,a_2,b_1,b_2\}$
and
$q \not\in \{ a_{1}, a_{2}, p, \widetilde{p}\}$
.
Lemma 3·11. The module
$K \cap U_{a_1,a_1}$
is generated by:
-
(*)
$\mathsf{T}\!\left({a_1}\,;\,{p} ,{q},{r}\right)$
with
$p,q,r \not\in \{a_1,b_1\}$
and
$p,\widetilde{p},q,\widetilde{q},r,\widetilde{r}$
pairwise different.
Proof of Lemma 3·10. The module
$U\,:=\,U_{a_1,a_2}$
is free of basis
$\{u(x,y)\}_{x,y} \sqcup \{u'(q,p)\}_{q,p}$
where
is indexed by 2-element subsets
$\{x,y\}$
of
$S\setminus \{a_1,b_2\}$
, and
is indexed by pairs (q, p) with
$q\in S\setminus\{a_1,a_2\}$
and
$p \in S\setminus\{a_1,a_2,b_1,b_2, q,\widetilde{q}\}$
. We claim that the quotient module
$U/{\langle \, \hbox{(i), (ii)} \, \rangle}$
is generated by
We start by observing that any element u
$'$
(q,p) of type (3·13) is, modulo (ii), equal to the element
$\pm u(p,\widetilde{p})$
of type (3·12). Indeed, we have
Thus, to prove the above claim, it is enough to show that the elements (3·12) not among the elements (3·14) can be written in terms of the latter using the relations (i). For any
$r\in S \setminus\{a_1,a_2,a_3,b_1,b_2,b_3\}$
, we have the following elements of type (i):
We deduce that, modulo (i),
$u(r,\widetilde{r})$
is a linear combination of (3·14) for
$r\in S \setminus\{a_1,a_2,b_1,b_2\}$
. Next, for any such r and
$p\in S \setminus \{a_1,a_2,b_2, r,\widetilde{r}\} $
, considering
shows that u(p, r) is also modulo (i) a linear combination of (3·14). This proves the above claim.
The
$\mathbb{Q}$
-vector space
$W\,:=\,W_{a_1,a_2}$
has a basis
$\{w(x)\}_x$
defined by
$w(x) \,:=\, (a_1\wedge x )\cdot (a_2\wedge \widetilde{x})$
for
$x\in S \setminus \{a_1,b_2\}$
. The map
$B^{(0)}\,:\,U/{\langle \, \hbox{(i)},\hbox{(ii)} \, \rangle} \to W$
sends u(x, y) to
$\varepsilon(x)\, w(y)+ \varepsilon(y)\, w(x)$
. Hence, the images of the generators (3·14) are
and they are easily checked to be
$\mathbb{Q}$
-linearly independent. It follows that the map
$B^{(0)}\,:\,U/{\langle \, \hbox{(i)}, \hbox{(ii)} \, \rangle} \to W$
is injective.
Proof of Lemma 3·11. The module
$U\,:=\,U_{a_1,a_1}$
is free, and a basis is obtained from the following list by deleting zeroes and fixing signs among repetitions:
Thus, we get a basis
$\{u(x,y)\}_{x,y}$
indexed by unordered pairs
$\{x,y\}\subset S\setminus\{a_1,b_1\}$
such that
$x\neq \widetilde{y}$
, up to the involution
$\{x,y\} \mapsto \{\widetilde{x},\widetilde{y}\}$
, and where
$u(x,y)= \pm \mathsf{\bigwedge}\!\left({a_1},{x},{y}\,;\,{a_1},{\widetilde{x}},{\widetilde{y}}\right)$
.
For any
$q,r\in \{a_3,\dots,a_g,b_3,\dots,b_g\}$
with
$q\neq \widetilde{r}$
, we have the following element of type
$(*)$
:
Hence,
$U/\langle \,(*)\, \rangle$
is generated by the elements u(x,y) such that the pair
$\{x,y\}$
contains
$a_2$
or
$b_2$
. Furthermore, for any
$r\in \{b_4,\dots,b_g\}$
, the elements
show that, modulo
$(*)$
,
$ u(a_2,r)$
is a linear combination of
Hence the quotient module
$U/\langle \,(*)\, \rangle$
is generated by (3·16).
The
$\mathbb{Q}$
-vector space
$W\,:=\,W_{a_1,a_1}$
has the basis
$\{w(x)\}_x$
defined by
$w(x) \,:=\, (a_1\wedge x )\cdot (a_1\wedge \widetilde{x})$
and indexed by the elements
$x\in S \setminus \{a_1,b_1\}$
, up to the involution
$x\mapsto \widetilde{x}$
. The map
$B^{(0)}\,:\,U/{\langle \, (*) \, \rangle} \to W$
sends u(x,y) to
$\pm \big(\varepsilon(x)\, w(y)+ \varepsilon(y)\, w(x)\big)$
. Hence, the images of the generators (3·16) are
Those vectors being linearly independent, the map
$B^{(0)}\,:\,U/{\langle \, (*) \, \rangle} \to W$
is injective.
3·3·4. A G-generating system of
$K \cap U_3$
As in the proof of Lemma 3·5, we finally consider the subspace
$W_2$
of
$S^2(\Lambda^2 H^\mathbb{Q})/\Lambda^4 H^\mathbb{Q}$
generated by the elements
$(s_1\wedge s_2)\cdot (s_3\wedge s_4)$
with
$s_i\in S$
, showing two (disjoint) contractions. We are interested in the kernel
$K \cap U_3$
of the map
defined on the module
$U_3 = V_{1,2} \oplus V_3$
. Note that, in contrast with the previous cases, the component
$B^{(2)}$
of B plays a role here, although minor.
The next lemma proves that
$(\mathcal{R}_3)$
is a G-generating system of
$K \cap U_3$
.
Lemma 3·12. The module
$K\cap U_3$
is generated by:
-
(i)
$\mathsf{D}\!\left({x},{\widetilde{x}}\,;\,{c},{\widetilde{c}}\,;\,{y},{\widetilde{y}}\right)$
with
$x,\widetilde{x},y,\widetilde{y},c,\widetilde{c}$
pairwise different; -
(ii)
$\mathsf{D}\!\left({x},{\widetilde{x}}\,;\,{c_1},{c_2}\,;\,{y},{\widetilde{y}}\right)$
with
$x,\widetilde{x},y,\widetilde{y},c_1,\widetilde{c_1},c_2,\widetilde{c_2}$
pairwise different; -
(iii)
$\mathsf{IHX}_3\!\left({p},{q}\,;\,{r}\right)$
with
$p,\widetilde{p},q,\widetilde{q},r,\widetilde{r}$
pairwise different; -
(iv)
$\mathsf{IHX}'_3\!\left({p},{q}\,;\,{r},{s}\right)$
with
$p,\widetilde{p},q,\widetilde{q},r,\widetilde{r},s,\widetilde{s}$
pairwise different.
Proof. We endow
$U\,:=\,U_3$
and
$W\,:=\,W_2$
with the following filtrations. First, observe that the map
$N:S \to \{1,\dots,g\}$
defined by
$N(a_i)=N(b_i)=i$
induces an increasing filtration
of the set S, where
$F_k S$
consists of the
$s\in S$
with
$N(s)\leq k$
. Thus, we get increasing filtrations
\begin{eqnarray*}&& \{0\} = F_0U \subset F_1 U\subset \cdots \subset F_{g-1} U \subset F_g U=U\\[6pt]&& \{0\} = F_0W \subset F_1 W\subset \cdots \subset F_{g-1} W \subset F_g W=W\end{eqnarray*}
of the module U and the
$\mathbb{Q}$
-vector space W, respectively. Specifically, for every
$k\in\{1,\dots,g\}$
, the module
$F_k U$
is generated by the elements
and
Similarly, for every
$k\in\{1,\dots,g\}$
, the
$\mathbb{Q}$
-vector space
$F_kW$
is generated by the elements
For future use, we compute the map
$B^{(0)}\,:\,U \to W$
in terms of those generators:
Since we have
$B^{(0)}(F_kU)\subset F_k W $
, there is a map
$\operatorname{Gr} B^{(0)}\,:\,\operatorname{Gr} U \to \operatorname{Gr} W$
on the associated graded, and we set
$L\,:=\, \ker \big(\!\operatorname{Gr} B^{(0)}\big)$
. The filtration on U induces a filtration on
$K\cap U$
, by setting
$F_k(K \cap U) \,:=\, K \cap (F_k U)$
. By definition of K, the inclusion of
$K\cap U$
in U induces an injective map
Let I be the submodule of U generated by the elements (i),(ii),(iii),(iv) of the statement, and endow I with the filtration defined by
$F_k I \,:=\, I \cap (F_k U)$
. The inclusion of I in
$K \cap U$
induces an injective map
We claim two things:
Claim (3·21) will imply that
$\iota_k$
is surjective for every
$k\geq 4$
, from which we will deduce that
$K\cap U=I + F_3(K\cap U)$
; then, with claim (3·22), we will conclude that
$K\cap U=I$
which will prove the lemma.
We first prove (3·21), fixing
$k\in \{4,\dots,g\}$
. Since the maps
$\iota$
and
$\kappa$
are injective, the quotient modules
$\operatorname{Gr}_k I=F_kI/F_{k-1} I$
and
$\operatorname{Gr}_k (K \cap U) = F_k(K\cap U)/F_{k-1} (K \cap U)$
can be viewed as submodules of
$\operatorname{Gr}_k U = F_k U/F_{k-1} U$
. Thus, claim (3·21) is equivalent to the injectivity of
The quotient module
$\operatorname{Gr}_k U$
is generated by the (classes of) elements
$u(q,t,\widetilde{t})$
, u(q, r, t),
$u'(t\,;\,q,r)$
,
$u'(r\,;\,q,t)$
with
$q,r,t \in S$
such that
$N(t)=k$
,
$N(q)\lt k$
,
$N(r)\lt k$
. This induces a generating system
of
$\operatorname{Gr}_k U/\operatorname{Gr}_k I$
, which we reduce as follows:
-
(1) for any
$t,q,r,s\in S$
such that
$N(t)=k$
,
$N(q)\lt k$
,
$N(r)\lt k$
,
$N(s)\lt k$
and N(q), N(r), N(s) are pairwise different, the elementis of type (ii), which shows that
\begin{equation*}\mathsf{D}\!\left({q},{\widetilde{q}}\,;\,{t},{s}\,;\,{r},{\widetilde{r}}\right)=\varepsilon(t)\, u'(t\,;\,q,r) - \varepsilon(s)\, u'(s\,;\,q,r)\end{equation*}
$\overline{u'}(t\,;\,q,r)=0$
. Thus, all the generators of
$\operatorname{Gr}_k U/\operatorname{Gr}_k I$
of type (3·27) are actually zero;
-
(2) for any
$t,q,r\in S$
such that
$N(t)=k$
,
$N(q)\lt k$
,
$N(r)\lt k$
and
$N(q)\neq N(r)$
, the element is of type (iii), which (using the previous item) implies that
\begin{equation*}\mathsf{IHX}_3\!\left({t},{q}\,;\,{r}\right) =\varepsilon(r)\, u'(q\,;\,t,r) + \varepsilon(q)\, u(r,\widetilde{r},t) - \varepsilon(r)\, u'(t\,;\,q,r) - \varepsilon(t)\, u(r,\widetilde{r},q)\end{equation*}
(3·29)Thus, all the generators of type (3·28) are repeated in (3·25), so that they can be removed;
\begin{equation} \overline{u'}(q\,;\,t,r)= -\varepsilon(q)\varepsilon(r) \, \overline{u}(r,\widetilde{r},t).\end{equation}
-
(3) for any
$t,p,q\in S$
such that
$N(t)=k$
,
$N(p)\lt k$
,
$N(q)\lt k$
and
$N(p)\neq N(q)$
, the elementis of type (iii), which (using (3·29)), implies that
\begin{equation*}\mathsf{IHX}_3\!\left({p},{q}\,;\,{t}\right)=\varepsilon(t)\,u'(q\,;\,p,t) + \varepsilon(q)\, u(t,\widetilde{t},p)-\varepsilon(t)\, u'(p\,;\,q,t)- \varepsilon(p)\, u(t,\widetilde{t},q)\end{equation*}
Thus, setting
\begin{equation*} \overline{u}(t,\widetilde{t},p)=\varepsilon(t)\varepsilon(p)\, \overline{u}(p,\widetilde{p},t)-\varepsilon(t)\varepsilon(p)\, \overline{u}(q,\widetilde{q},t)+ \varepsilon(p)\varepsilon(q)\, \overline{u}(t,\widetilde{t},q).\end{equation*}
$q\,:=\,a_1$
and
$t\,:=\,a_k$
in the above equation, we see that the submodule of
$\operatorname{Gr}_k U/\operatorname{Gr}_k I$
generated by (3·24) and (3·25) is actually generated by the single element
$u(a_1,a_k,b_k)$
of (3·24) and (3·25);
-
(4) for any
$t,q,r,s\in S$
such that
$N(t)=k$
,
$N(q)\lt k$
,
$N(r)\lt k$
,
$N(s)\lt k$
and N(q), N(r), N(s) are pairwise different, the element is of type (iv), which (using (3·29)) implies that
\begin{eqnarray*}\mathsf{IHX}'_3\!\left({t},{q}\,;\,{r},{s}\right)&= &\varepsilon(q)\, u(t,r,s)- \varepsilon(t)\, u(q,r,s) -\varepsilon(s)\, u(\widetilde{r},\widetilde{t},{q})\\&& - \varepsilon(r)\, u(s,\widetilde{t},q) - \varepsilon(r)\, u'(q\,;\,s,t) + \varepsilon(s)\, u'(t\,;\,q,r)\end{eqnarray*}
(3·30)Thus, setting
\begin{equation} \varepsilon(q)\ \overline{u}(t,r,s) +\varepsilon(s)\, \overline{u}({r},{t},\widetilde{q})+ \varepsilon(r)\, \overline{u}(\widetilde{s},t,\widetilde{q})+\varepsilon(r)\varepsilon(s)\varepsilon(q)\, \overline{u}(s,\widetilde{s},t) =0.\end{equation}
$(t,r)\,:=\,(a_k,a_1)$
in the above equation, we get and, setting
\begin{equation*}\overline{u}(\widetilde{s},\widetilde{q},a_k) = -\varepsilon(s)\, \overline{u}(\widetilde{q},a_1,a_k)- \varepsilon(q)\, \overline{u}(s,a_1,a_k)- \varepsilon(s)\varepsilon(q)\, \overline{u}(s,\widetilde{s},a_k),\end{equation*}
$(t,s)\,:=\,(a_k,a_1)$
in the same equation, we get The above two equations show that, in the presence of (3·24) and (3·25), the generators of type (3·26) can be reduced to those of the form
\begin{equation*} \overline{u}(\widetilde{q},b_1,a_k)= -\varepsilon(q)\, \overline{u}(b_1,a_1,a_k)- \varepsilon(r)\, \overline{u}({r},\widetilde{q},a_k)-\varepsilon(q)\varepsilon(r)\, \overline{u}(r,a_1,a_k).\end{equation*}
$\overline{u}(q,a_1,a_k)$
with
$q\in S$
such that
$1\lt N(q)\lt k$
. Furthermore, by setting
$(q,r,s,t)\,:=\,(a_j,a_1,a_2,a_k)$
in (3·30) for every
$j\in \{3,\dots,k-1\}$
, we obtain and, by setting
\begin{equation*}\overline{u}(b_j,a_1,a_k)=-\overline{u}(a_2,b_2,a_k) - \overline{u}(b_2,a_k,b_j)- \overline{u}(a_2,a_1,a_k)\end{equation*}
$(q,r,s,t)\,:=\,(a_2,a_1,a_j,a_k)$
in (3·30), we also get We deduce that, in the presence of (3·24) and (3·25), the generators of type (3·26) can be reduced to those of the form
\begin{equation*}\overline{u}(b_2,a_k,b_j) = -\overline{u}(a_j,a_1,a_k) - \overline{u}(b_2,a_1,a_k) - \, \overline{u}(a_j,b_j,a_k).\end{equation*}
$\overline{u}(b_2,a_1,a_k)$
and
$\overline{u}(a_j,a_1,a_k)$
with
$j\in \{2,\dots,k-1\}$
.
It follows from the above discussion that
$\operatorname{Gr}_k U/\operatorname{Gr}_k I$
is generated by the following elements:
For
$p,q\in S$
with
$N(p)\leq k, N(q)\leq k$
, let
$\overline{w}(p,q)$
be the class of w(p,q) in
$\operatorname{Gr}_k W$
. According to (3·19), the values of the map (3·23) on this generating set are as follows:
\begin{eqnarray*}\Phi\big( \overline{u}(a_1,a_k,b_k)\big)&=& \overline{w}(a_k,b_k) + \overline{w}(a_1,b_k)- \overline{w}(a_1,a_k),\\ \Phi\big( \overline{u}(a_i,b_i,a_k) \big)&=& \overline{w}(b_i,a_k) -\overline{w}(a_i,a_k), \\ \Phi\big( \overline{u}(b_2,a_1,a_k) \big) &=&-\overline{w}(a_1,a_k) + \overline{w}(b_2,a_k),\\ \Phi\big( \overline{u}(a_j,a_1,a_k) \big) &=&\overline{w}(a_1,a_k) + \overline{w}(a_j,a_k).\end{eqnarray*}
Using the fact that
$\big\{\overline{w}(a_i,a_k)\,\vert\, i\lt k\big\}\cup \big\{\overline{w}(b_i,a_k)\,\vert\, i\lt k\big\}\cup \big\{\overline{w}(a_k,b_k)\big\}$
is a basis of
$\operatorname{Gr}_k W$
, we easily check that the above values of
$\Phi$
are
$\mathbb{Q}$
-linearly independent. Claim (3·21) follows.
We now prove (3·22). The quotient
$Q\,:=\,F_3 U /F_3 I$
is generated by the classes
and the classes
of elements in
$F_3U$
of type (3·17) and (3·18), respectively. For any
$p,q,r \in F_3S$
such that N(p), N(q), N(r) are pairwise different, the element
is of type (i), so that we have
$\overline{u'}(q;\,p,r) = - \overline{u'}(\widetilde{q};\,p,r) \in Q$
. Thus, among the generators of Q of type (3·32), we can reduce ourselves to
$\overline{u'}(a_1;\,a_2,a_3)$
,
$\overline{u'}(a_2;\,a_1,a_3)$
,
$\overline{u'}(a_3;\,a_1,a_2)$
. Furthermore, for any
$p,q,r \in F_3S$
such that N(p), N(q), N(r) are pairwise different, the element
is of type (iii), so that
$\varepsilon(q)\, \overline{u}(r,\widetilde{r},p)= -\varepsilon(r)\,\overline{u'}(q;\,p,r)+\varepsilon(r)\, \overline{u'}(p;\,q,r)+ \varepsilon(p)\, \overline{u}(r,\widetilde{r},q)\in Q$
; hence, among the generators of Q of type (3·31), we can remove
$\overline{u}(a_1,b_1,a_2)$
,
$\overline{u}(a_2,b_2,a_3)$
and
$\overline{u}(a_3,b_3,a_1)$
. Consequently, the module Q is generated by the following 10 elements:
According to (3·19) and (3·20), the values of the map
$\overline{B}:Q \to F_3 W \oplus \mathbb{Q}$
(which is induced by
$B:F_3 U \to F_3 W \oplus \mathbb{Q}$
) on this generating set are as follows:
\begin{eqnarray*}\overline{B}\big(\overline{u}(a_1,a_2,a_3) \big) &=&\big(w(a_2,a_3)+ w(a_1,a_3)+w(a_1,a_2) \,,\, -1/4 \big) \\ \overline{B}\big(\overline{u}(b_1,a_2,a_3)\big) &=&\big(-w(a_2,a_3)+w(a_1,b_3)+w(a_1,b_2) \,,\, +1/4 \big) \\ \overline{B}\big(\overline{u}(a_1,b_2,a_3)\big) &=&\big(w(a_2,b_3)-w(a_1,a_3)+w(a_1,b_2) \,,\, +1/4 \big) \\ \overline{B}\big(\overline{u}(a_1,a_2,b_3)\big) &=&\big(w(a_2,b_3)+w(a_1,b_3)-w(a_1,a_2) \,,\, +1/4\big) \\ \overline{B}\big(\overline{u}(a_1,b_1,a_3)\big) &=&\big(w(a_1,b_3) -w(a_1,a_3)+w(a_1,b_1) \,,\, +1/4 \big) \\ \overline{B}\big(\overline{u}(a_2,b_2,a_1)\big) &=&\big(w(a_1,b_2)-w(a_1,a_2)+ w(a_2,b_2)\,,\, +1/4 \big) \\ \overline{B}\big(\overline{u}(a_3,b_3,a_2)\big) &=&\big(w(a_2,b_3) -w(a_2,a_3)+ w(a_3,b_3) \,,\, +1/4 \big) \\ \overline{B}\big(\overline{u'}(a_1\,;\,a_2,a_3)\big) &=&\big(w(a_2,a_3)-w(a_2,b_3) \,,\, 0\big) \\ \overline{B}\big(\overline{u'}(a_2\,;\,a_1,a_3)\big) &=&\big(w(a_1,a_3)-w(a_1,b_3) \,,\, 0\big) \\ \overline{B}\big(\overline{u'}(a_3\,;\,a_1,a_2)\big) &=&\big(w(a_1,a_2)-w(a_1,b_2) \,,\, 0\big).\end{eqnarray*}
Using that
$\big\{w(a_i,a_j)\,\vert\, 1 \leq i \lt j \leq 3 \big\}\cup \big\{w(a_i,b_i)\,\vert\, 1 \leq i \leq 3 \big\}\cup \big\{w(a_i,b_j)\,\vert\, 1 \leq i \lt j \leq 3 \big\}$
is a basis of the
$\mathbb{Q}$
-vector space
$F_3W$
, it is easily checked that the above vectors of
$F_3W\oplus \mathbb{Q}$
are
$\mathbb{Q}$
-linearly independent. Therefore, the map
$\overline{B}$
is injective.
3·4. Vanishing of J on K
We now prove that the map
$J:\Lambda^2 (\Lambda^3 H) \to \Gamma_2\mathcal{I}/\Gamma_3 \mathcal{I}$
vanishes on the elements of type (
$\mathcal{R}_i)$
with
$0\leq i \leq 3$
, which have been identified in Theorem 3·6. Again, we use the action of the subgroup
$G=G(S)$
of
$\operatorname{Sp}\!(H)$
defined at (3·7). Since the elements (
$\mathcal{R}_i)$
constitute a G-generating system of K and since J is G-equivariant, this will prove that
$J(K)=0$
and conclude the proof of Theorem B.
3·4·1. BP-maps and PB-maps
We start by fixing notations for some specific elements of the Torelli group
$\mathcal{I}$
, which we shall need in the sequel.
The first class of elements of
$\mathcal{I}$
, which we have already met in previous sections and are called BP-maps by Johnson, are opposite Dehn twists
$T_{\varepsilon}T_\delta^{-1}$
along a pair
$(\varepsilon,\delta)$
of disjoint and cobounding, simple closed curves. In fact, we shall only need such “B”ounding “P”airs
$(\varepsilon, \delta)$
that delimit a subsurface of genus 1 in
$\Sigma$
. The data of a BP-map
$T_{\varepsilon}T_\delta^{-1}$
of genus 1 is encoded by giving a chain of 3 circles in
$\Sigma$
, whose neighbourhood is a subsurface of genus 1 with 2 boundary components, as shown below:

(The value of
$\tau_1$
on
$T_{\varepsilon}T_\delta^{-1}$
is derived directly from (2·2).)
The second class of elements of
$\mathcal{I}$
are called PB-maps, since they arise from embeddings of the commutator subgroup of the “P”ure “B”raid group into
$\mathcal{I}$
[
Reference Oda28
]. Specifically, a PB-map in
$\mathcal{I}$
is encoded by a Y-shaped graph in the surface
$\Sigma$
, which gives a 2-holed disk in
$\Sigma$
and defines a commutator of two Dehn twists
$[T_{\varepsilon},T_\delta]$
, as shown below:

(The value of
$\tau_1$
on
$[T_{\varepsilon},T_\delta]$
can be derived, for instance, from the exact relationship between Milnor invariants and Johnson homomorphisms [
Reference Gervais and Habegger7
]; BP-maps also appear in [
Reference Putman29
] under the name “commutators of simply intersecting pairs”.)
Recall that
$N:S \to \{1,\dots,g\}$
is the map defined by
$N(a_i)=N(b_i)=i$
, and observe that any elementary trivector
$s_1\wedge s_2 \wedge s_3$
(with
$s_1,s_2,s_3\in S$
pairwise different) can be realised as the value of
$\tau_1$
on:
-
(1) a PB-map if
$N(s_1),N(s_2),N(s_3)$
are pairwise different; -
(2) a BP-map if
$N(s_i)=N(s_j)$
for some
$i\neq j$
.
Example 3·13. The elementary trivectors
$a_1 \wedge a_2 \wedge b_3$
and
$a_1 \wedge b_1 \wedge b_3$
are (up to signs) realised by the following PB-map and BP-map, respectively:

3·4·2. Vanishing of J on the elements (
$\mathcal{R}_0)$
All the elements of the family (
$\mathcal{R}_0)$
are of the form
$\mathsf{\bigwedge}\!\left({s_1},{s_2},{s_3}\,;\,{s'_1},{s'_2},{s'_3}\right)$
where the elementary trivectors
$s_1\wedge s_2 \wedge s_3$
and
$s_1'\wedge s_2' \wedge s_3'$
are realised by BP-maps or PB-maps with disjoint supports: specifically, realizations are shown (up to a sign) in Table 1. Therefore, all the elements of (
$\mathcal{R}_0)$
belong to
$\ker(J)$
.
Realizations of elementary trivectors with no contraction

Since
$(\mathcal{R}_0)$
is a G-generating system of
$K\cap U_0$
, we obtain the following more general result.
Lemma 3·14. The submodule
$K\cap U_0$
of
$\Lambda^2(\Lambda^3H)$
is contained in
$\ker(J)$
.
3·4·3. Vanishing of J on the elements
$(\mathcal{R}_1)$
We deduce from the following lemma that the first six elements of (
$\mathcal{R}_1)$
are in the kernel of J.
Lemma 3·15. Let
$x,y,c_1,c_2,u,v \in S$
be pairwise different, and assume that
$c_1\neq \widetilde{c_2}$
too. Then we have
$\mathsf{D}\!\left({x},{y}\,;\,{c_1},{c_2}\,;\,{\widetilde{u}},{\widetilde{v}}\right) \in \ker(J).$
Proof. Let
$\eta \,:=\, \varepsilon(c_1)\, \varepsilon(c_2)$
. We claim that
Since
$\mathsf{\bigwedge}\!\left({x},{y},{c_1}\,;\,{\widetilde{c_2}},{\widetilde{u}},{\widetilde{v}}\right)$
and
$\mathsf{\bigwedge}\!\left({x},{y},{c_2}\,;\,{\widetilde{c_1}},{\widetilde{u}},{\widetilde{v}}\right)$
belong to
$\ker(J)$
by Lemma 3·14, we deduce that
$-\eta\,\mathsf{\bigwedge}\!\left({x},{y},{c_1}\,;\,{\widetilde{c_1}},{\widetilde{u}},{\widetilde{v}}\right)+\mathsf{\bigwedge}\!\left({x},{y},{c_2}\,;\,{\widetilde{c_2}},{\widetilde{u}},{\widetilde{v}}\right)= -\varepsilon(c_2)\, \mathsf{D}\!\left({x},{y}\,;\,{c_1},{c_2}\,;\,{\widetilde{u}},{\widetilde{v}}\right)$
does too.
We now prove the above claim. If
${c_2} \notin \{\widetilde{x},\widetilde{y}\}$
and
$c_1\not\in \{\widetilde{u},\widetilde{v}\}$
, then we consider the symplectic transformation T that maps
$(c_1,\widetilde{c_1},c_2,\widetilde{c_2})$
to
$(c_1+c_2,\widetilde{c_1},c_2,-\eta\, \widetilde{c_1}+\widetilde{c_2})$
and fixes all other elements of S; then T maps
to C, so that
$C\in \ker(J)$
. If we have
${c_1} \notin \{\widetilde{x},\widetilde{y}\}$
and
$c_2\not\in \{\widetilde{u},\widetilde{v}\}$
, we can proceed similarly by exchanging the roles of
$c_1$
and
$c_2$
.
We now assume that none of the above two conditions occur, i.e
$.$
we have
$\{c_1,c_2\}=\{\widetilde{x},\widetilde{y}\}$
or (exclusively)
$\{c_1,c_2\}=\{\widetilde{u},\widetilde{v}\}$
. For instance, we assume that
$(c_1,c_2)=(\widetilde{x},\widetilde{y})$
, the other cases being treated similarly. Then
and we deduce from Lemma 3·15 that C belongs to
$\ker(J)$
in the present case too.
Besides, we have the following variant of Lemma 3·9 (which will be used later).
Lemma 3·16. Let
$x,y,c,u,v \in S$
be pairwise different, and assume that
$c\not\in \{\widetilde{x},\widetilde{y},\widetilde{u},\widetilde{v}\}$
. Then we have
$\mathsf{D}\!\left({x},{y}\,;\,{c},{\widetilde{c}}\,;\,{\widetilde{u}},{\widetilde{v}}\right) \in \ker(J).$
Proof. Let T be the symplectic transformation that maps c to
$c+\widetilde{c}$
and fixes all other elements of S. We have
\begin{align*} &T \cdot \mathsf{\bigwedge}\!\left({x},{y},{c}\,;\,{c},{\widetilde{u}},{\widetilde{v}}\right) -\mathsf{\bigwedge}\!\left({x},{y},{c}\,;\,{c},{\widetilde{u}},{\widetilde{v}}\right)-\mathsf{\bigwedge}\!\left({x},{y},{\widetilde{c}}\,;\,{\widetilde{c}},{\widetilde{u}},{\widetilde{v}}\right) \\&\quad = \varepsilon(c)\, \mathsf{D}\!\left({x},{y}\,;\,{c},{\widetilde{c}}\,;\,{\widetilde{u}},{\widetilde{v}}\right)\end{align*}
and we conclude with Lemma 3·14.
The next lemma deals with the seventh (and last) element of
$(\mathcal{R}_1)$
.
Lemma 3·17 (Gervais and Habegger). We have
$\mathsf{IHX}_1\!\left({a_{1}};{a_{2}},{a_{3}},{a_{4}}\,;\,{b_{1}}\right) \in \ker (J).$
Proof. This has been proved by Gervais and Habegger [
Reference Gervais and Habegger7
] but, for the sake of completeness, we repeat their arguments (with some variations). We focus on a subsurface of
$\Sigma$
of genus 4 which contains the based loops
$\alpha_1,\beta_1,\dots,\alpha_4,\beta_4$
of Figure 1. This subsurface (union a rectangle) is shown in Figure 3 as the cylinder
$D\times [0,1]$
over a 4-holed disk D: the curves X, Y, Z (shown in Figure 3) lie on
$D \times \{1\}$
and we denote by
$X_0,Y_0,Z_0$
the corresponding curves on
$D \times \{0\}$
(not shown in Figure 3).
The curves X,Y,Z and U,V,W on
$\partial(D\times [0,1])$
.

In the rest of this proof, the Dehn twist
$T_C$
along a simple closed curve C is simply denoted by C and, if C is oriented, the homology class
$\{C\}\in H$
is denoted by the lower case roman letter c. By the Hall–Witt identity, we know that
and, since the Dehn twists along
$X_0,Y_0,Z_0$
commute with those along X, Y, Z, we obtain that
Note that
$XX_0^{-1},YY_0^{-1},ZZ_0^{-1}$
are BP-maps (of genus 1) while [Y, Z], [X, Y], [Z, X] are PB-maps: hence the above identity gives a degree 2 relation in
$\operatorname{Gr}^{\Gamma} \mathcal{I}$
. (See [
Reference Putman29
] for a systematic use of Hall–Witt identities in presentations of the group
$\mathcal{I}$
.) Consequently, the sum
\begin{align*}&\big(Z_* \cdot \tau_1\big(XX_0^{-1}\big)\big) \wedge \tau_1([Y,Z])\\ &\quad+\big(Y_* \cdot \tau_1\big(ZZ_0^{-1}\big)\big) \wedge \tau_1([X,Y])\\&\quad+\big(X_* \cdot \tau_1\big(YY_0^{-1}\big)\big) \wedge \tau_1([Z,X])\end{align*}
belongs to
$\ker(J)$
. (Here
$X_*\in \operatorname{Sp}\!(H)$
denotes the action of the Dehn twist along X.) Using (3·33) and (3·34), we obtain
\begin{eqnarray*} Z_* \cdot \tau_1\big(XX_0^{-1}\big)&=& \varepsilon\, b_1 \wedge Z_*(u) \wedge b_4 \\& = & \varepsilon\, b_1 \wedge (u+z) \wedge b_4 \\& = & \varepsilon\, b_1 \wedge ((a_1-a_4)+(b_3+b_4)) \wedge b_4\ = \ \varepsilon\, b_1 \wedge ( a_1-a_4 +b_3 ) \wedge b_4\end{eqnarray*}
and
respectively. (Here
$\varepsilon$
and
$\eta$
are fixed signs, which we do not need to determine.) Next, it follows from Lemma 3·14 that
similarly, we obtain
and
Therefore the element
\begin{equation*}\underbrace{\mathsf{\bigwedge}\!\left({b_4},{b_1},{a_4}\,;\,{b_4},{b_3},{b_2}\right)+ \mathsf{\bigwedge}\!\left({b_4},{b_3},{a_4}\,;\,{b_4},{b_2},{b_1}\right)+ \mathsf{\bigwedge}\!\left({b_4},{b_2},{a_4}\,;\,{b_4},{b_1},{b_3}\right)}_{\mathsf{IHX}_1\!\left({b_4};{b_1},{b_3},{b_2}\,;\,{a_4}\right)}\end{equation*}
belongs to
$\ker(J)$
, and we conclude using the G-action.
Since
$(\mathcal{R}_1)$
is a G-generating system of
$K\cap U_1$
, we obtain the following.
Lemma 3·18 The submodule
$K\cap U_1$
of
$\Lambda^2(\Lambda^3H)$
is contained in
$\ker(J)$
.
3·4·4. Vanishing of J on the elements (
$\mathcal{R}_2)$
We now deal with the elements of the family (
$\mathcal{R}_2)$
through the next three lemmas.
Lemma 3·19. The elements
$\mathsf{IHX}_2\!\left({a_1},{a_2}\,;\,{a_3}\,;\,{b_1}\right)$
and
$\mathsf{IHX}_2\!\left({a_1},{a_2}\,;\,{a_3}\,;\,{a_4}\right)$
belong to
$\ker(J)$
.
Proof. For all
$h\in \{3,\dots, g\}$
, the element
$\sum_{i=1}^{h-1} \mathsf{\bigwedge}\!\left({a_1},{a_2},{b_2}\,;\,{a_h},{a_i},{b_i}\right)$
of
$\Lambda^2(\Lambda^3 H)$
belongs to
$\ker(J)$
, since
${a_1}\wedge{a_2}\wedge{b_2}$
and
$\sum_{i=1}^{h-1} {a_h}\wedge{a_i}\wedge{b_i}$
can be realised by BP maps (of genus 1 and
$h-1$
, respectively) whose supports are disjoint one from the other. Setting
$h\,:=\,3$
, we obtain that
belongs to
$\ker(J)$
. The element of
$G \simeq \mathbb{Z}_4^g \rtimes \mathfrak{S}_g$
corresponding to the transposition (23) maps W to
$\mathsf{IHX}_2\!\left({a_1},{a_2}\,;\,{a_3}\,;\,{b_1}\right)$
which, therefore, is in
$\ker(J)$
too.
Next, the element of G corresponding to the cycle (1423) transforms W to
which, therefore, belongs to
$\ker(J)$
. Let also T be the symplectic transformation that maps
$(a_4,b_2)$
to
$( a_4 + a_2 , b_2 - b_4)$
and leaves all other elements of S fixed. We have
Hence, using Lemma 3·14 and the G-action, we obtain that
Lemma 3·20 The following five elements belong to
$\ker(J)$
:
Proof. Consider the element
$W\in \ker(J)$
defined by (3·35), and let
$T_0$
be the symplectic transformation that maps
$(a_2,a_3)$
to
$(a_2+b_3,a_3+b_2)$
. We have
where
$W'\,:=\,\mathsf{\bigwedge}\!\left({a_1},{a_2},{b_2}\,;\,{a_3},{b_3},{b_2}\right)-\mathsf{\bigwedge}\!\left({a_1},{b_3},{a_3}\,;\,{b_2},{a_3},{b_3}\right)$
. But, an appropriate element of G transforms W
′ to W, and we deduce from Lemma 3·15 that
$\mathsf{S}\!\left({a_1},{b_2}\,;\begin{array}{cc}{b_2} & {b_1}\!\\{b_3} & {a_3}\! \end{array}\right)$
belongs to
$\ker(J)$
. Using again the G-action, we conclude that
$\mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_2} & {b_1}\!\\{a_3} & {b_3}\! \end{array}\right)$
is in
$\ker(J)$
too.
By Lemma 3·15,
$D\,:=\,\mathsf{D}\!\left({a_1},{a_3}\,;\,{a_2},{a_4}\,;\,{a_2},{a_4}\right)$
belongs to
$\ker(J)$
. For the symplectic transformation
$T_1$
that maps
$(a_3,a_4)$
to
$(a_3+b_4,a_4+b_3)$
and fixes all other elements of S, we have
where
\begin{eqnarray*}D_1 &\,:=\,&\mathsf{\bigwedge}\!\left({a_1},{a_3},{a_2}\,;\,{b_2},{a_2},{b_3}\right) + \mathsf{\bigwedge}\!\left({a_1},{b_4},{a_2}\,;\,{b_2},{a_2},{a_4}\right) \\&& \quad - \mathsf{\bigwedge}\!\left({a_1},{a_3},{a_4}\,;\,{b_4},{a_2},{b_3}\right) - \mathsf{\bigwedge}\!\left({a_1},{b_4},{a_4}\,;\,{b_4},{a_2},{a_4}\right)\ = \ -\mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_2} & {a_3}\!\\{b_4} & {a_4}\! \end{array}\right).\end{eqnarray*}
Hence, by Lemma 3·14 and Lemma 3·18,
$D_1$
belongs to
$\ker(J)$
. Using the G-action, we deduce that
$\mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_2} & {a_4}\!\\{a_3} & {b_3}\! \end{array}\right)$
does too.
Proceeding with the same strategy, we consider the symplectic transformation
$T_3$
mapping
$(a_2,b_5)$
to
$(a_2+a_5,b_5-b_2)$
and fixing all other elements of S. We have
\begin{eqnarray*}&& T_3\cdot \mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_2} & {a_4}\!\\{a_3} & {b_3}\! \end{array}\right)- \mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_2} & {a_4}\!\\{a_3} & {b_3}\! \end{array}\right) \\=&& D_3 + \mathsf{D}\!\left({a_1},{a_5}\,;\,{a_3},{a_4}\,;\,{a_2},{b_2}\right)+ \mathsf{D}\!\left({a_1},{a_5}\,;\,{a_3},{a_4}\,;\,{a_5},{b_2}\right),\end{eqnarray*}
where
\begin{eqnarray*}D_3 &\,:=\,& - \mathsf{\bigwedge}\!\left({a_1},{a_2},{a_4}\,;\,{a_5},{b_2},{b_4}\right)-\mathsf{\bigwedge}\!\left({a_1},{a_4},{b_3}\,;\,{a_5},{b_4},{a_3}\right)\\&& \quad + \mathsf{\bigwedge}\!\left({a_1},{a_3},{b_3}\,;\,{a_5},{b_3},{a_3}\right)+ \mathsf{\bigwedge}\!\left({a_1},{a_2},{a_3}\,;\,{a_5},{b_2},{b_3}\right)\ = \ \mathsf{S}\!\left({a_1},{a_5}\,;\begin{array}{cc}{a_2} & {a_4}\!\\{a_3} & {b_3}\! \end{array}\right).\end{eqnarray*}
Therefore, using the G-action, we deduce that
$\mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_4} & {a_5}\!\\{a_3} & {b_3}\! \end{array}\right)$
is in
$\ker(J)$
.
We continue with the symplectic transformation
$T_4$
mapping
$(a_2,b_4)$
to
$(a_2+a_4,b_4-b_2)$
and fixing all other elements of S. We have
\begin{eqnarray*}&& T_4\cdot \mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_2} & {b_1}\!\\{a_3} & {b_3}\! \end{array}\right)- \mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_2} & {b_1}\!\\{a_3} & {b_3}\! \end{array}\right) \\=&& D_4- \mathsf{D}\!\left({a_1},{a_4}\,;\,{a_3},{b_1}\,;\,{a_2},{b_2}\right)- \mathsf{D}\!\left({a_1},{a_4}\,;\,{a_3},{b_1}\,;\,{a_4},{b_2}\right),\end{eqnarray*}
where
\begin{eqnarray*}D_4 &\,:=\,& - \mathsf{\bigwedge}\!\left({a_1},{a_2},{b_1}\,;\,{a_4},{b_2},{a_1}\right)-\mathsf{\bigwedge}\!\left({a_1},{b_1},{b_3}\,;\,{a_4},{a_1},{a_3}\right)\\&& \quad - \mathsf{\bigwedge}\!\left({a_1},{a_3},{b_3}\,;\,{a_4},{b_3},{a_3}\right)- \mathsf{\bigwedge}\!\left({a_1},{a_2},{a_3}\,;\,{a_4},{b_2},{b_3}\right)\ = \ \mathsf{S}\!\left({a_1},{a_4}\,;\begin{array}{cc}{a_2} & {b_1}\!\\{a_3} & {b_3}\! \end{array}\right).\end{eqnarray*}
Therefore, using the G-action, we deduce that
$\mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{b_1} & {a_4}\!\\{a_3} & {b_3}\! \end{array}\right)$
is in
$\ker(J)$
.
Finally, using again the above transformation
$T_1$
, an elementary computation shows that the difference
$ T_1\cdot \mathsf{\bigwedge}\!\left({a_1},{a_3},{a_4}\,;\,{a_2},{a_3},{a_4}\right)- \mathsf{\bigwedge}\!\left({a_1},{a_3},{a_4}\,;\,{a_2},{a_3},{a_4}\right)$
decomposes as
\begin{align*} &\mathsf{\bigwedge}\!\left({a_1},{b_4},{b_3}\,;\,{a_2},{a_3},{a_4}\right)+\mathsf{\bigwedge}\!\left({a_1},{b_4},{a_4}\,;\,{a_2},{b_4},{a_4}\right)\\&\quad+\mathsf{\bigwedge}\!\left({a_1},{a_3},{b_3}\,;\,{a_2},{a_3},{b_3}\right)+\mathsf{\bigwedge}\!\left({a_1},{a_3},{a_4}\,;\,{a_2},{b_4},{b_3}\right)\end{align*}
plus a sum of 11 terms which belongs to
$K\cap U_0 + K\cap U_1$
. Using Lemma 3·14 and Lemma 3·18, we conclude that
$\mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_4} & {b_4}\!\\{a_3} & {b_3}\! \end{array}\right)$
belongs to
$\ker(J)$
.
Lemma 3·21. We have
$\mathsf{T}\!\left({a_1}\,;\,{a_2} ,{a_3},{a_4}\right) \in \ker(J)$
.
Proof. Let T be the symplectic transformation that maps
$(a_2,b_1)$
to
$(a_2 + a_1, b_1 - b_2)$
and leaves all other elements of S fixed. We have
\begin{eqnarray*}&&T \cdot \mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_2} & {a_4}\!\\{a_3} & {b_3}\! \end{array}\right) - \mathsf{S}\!\left({a_1},{a_2}\,;\begin{array}{cc}{a_2} & {a_4}\!\\{a_3} & {b_3}\! \end{array}\right)\\=&&\mathsf{\bigwedge}\!\left({a_1},{a_2},{a_3}\,;\,{a_1},{b_2},{b_3}\right)- \mathsf{\bigwedge}\!\left({a_1},{a_2},{a_4}\,;\,{a_1},{b_2},{b_4}\right)- \mathsf{\bigwedge}\!\left({a_1},{a_4},{b_3}\,;\,{a_1},{b_4},{a_3}\right),\end{eqnarray*}
which is
$-\mathsf{T}\!\left({a_1}\,;\,{a_2} ,{a_4},{a_3}\right)$
. Using the G-action, we obtain that
$\mathsf{T}\!\left({a_1}\,;\,{a_2} ,{a_3},{a_4}\right) \in \ker(J)$
.
Since
$(\mathcal{R}_2)$
is a G-generating system of
$K\cap U_2$
, we obtain the following.
Lemma 3·22. The submodule
$K\cap U_2$
of
$\Lambda^2(\Lambda^3H)$
is contained in
$\ker(J)$
.
3·4·5. Vanishing of J on the elements (
$\mathcal{R}_3)$
We deduce from Lemma 3·15 and Lemma 3·16 that the first two elements of (
$\mathcal{R}_3)$
belong to
$\ker(J)$
. The following deals with the last two elements of (
$\mathcal{R}_3)$
, and finishes the proof of Theorem B.
Lemma 3·23. The elements
$\mathsf{IHX}_3\!\left({a_1},{a_2}\,;\,{a_3}\right)$
and
$\mathsf{IHX}'_3\!\left({a_1},{a_2}\,;\,{a_3},{a_4}\right)$
belong to
$\ker(J)$
.
Proof. Let
$T_1$
be the symplectic transformation that maps
$(a_1,a_2)$
to
$( a_1 + b_2,a_2 +b_1)$
, and set
\begin{eqnarray*}E_1 &\,:=\,& \mathsf{\bigwedge}\!\left({b_2},{a_3},{b_3}\,;\,{b_1},{a_3},{b_3}\right)+ \mathsf{\bigwedge}\!\left({b_2},{a_2},{b_1}\,;\,{a_3},{b_3},{b_2}\right),\\F_1 &\,:=\,& \mathsf{\bigwedge}\!\left({a_1},{a_3},{b_3}\,;\,{b_1},{a_3},{b_3}\right)+ \mathsf{\bigwedge}\!\left({b_2},{a_3},{b_3}\,;\,{a_2},{a_3},{b_3}\right) \\&&+ \ \mathsf{\bigwedge}\!\left({a_1},{a_3},{b_3}\,;\,{b_1},{a_2},{b_2}\right) + \mathsf{\bigwedge}\!\left({b_2},{a_3},{b_3}\,;\,{a_1},{b_1},{a_2}\right).\end{eqnarray*}
We have
Since
$E_1$
belongs to
$K \cap(V_{1,1}+V_2)=K \cap U_2$
, it follows from Lemma 3·19 and Lemma 3·22 that
$F_1$
belongs to
$\ker\!(J)$
. Besides, we have
\begin{equation*}\mathsf{IHX}_3\!\left({a_1},{a_2}\,;\,{a_3}\right)= - F_1 +\underbrace{\mathsf{\bigwedge}\!\left({a_3},{b_3},{a_1}\,;\,{b_1},{a_2},{b_2}\right)+ \mathsf{\bigwedge}\!\left({a_3},{b_3},{b_1}\,;\,{a_1},{a_2},{b_2}\right)}_{\mathsf{D}\left({a_3},{b_3}\,;\,{a_1},{b_1}\,;\,{a_2},{b_2}\right)}.\end{equation*}
Thus, an application of Lemma 3·16 shows that J vanishes on
$\mathsf{IHX}_3\!\left({a_1},{a_2}\,;\,{a_3}\right)$
.
Finally, consider the symplectic transformation
$T_2$
that maps
$(a_2,a_3)$
to
$(a_2 + b_3,a_3 +b_2)$
and fixes all other elements of S. We have
where
\begin{eqnarray*}E_2& \,:=\, &-\mathsf{\bigwedge}\!\left({b_2},{a_2},{a_4}\,;\,{a_2},{b_2},{b_4}\right)-\mathsf{\bigwedge}\!\left({a_3},{b_3},{a_4}\,;\,{a_2},{b_2},{b_4}\right)-\mathsf{\bigwedge}\!\left({a_3},{a_2},{a_4}\,;\,{b_3},{b_2},{b_4}\right)\\&& + \mathsf{\bigwedge}\!\left({b_2},{a_2},{a_1}\,;\,{a_2},{b_2},{b_1}\right)+ \mathsf{\bigwedge}\!\left({a_3},{b_3},{a_1}\,;\,{a_2},{b_2},{b_1}\right)+ \mathsf{\bigwedge}\!\left({a_3},{a_2},{a_1}\,;\,{b_3},{b_2},{b_1}\right)\\&& -\mathsf{\bigwedge}\!\left({b_2},{a_4},{b_1}\,;\,{a_2},{b_4},{a_1}\right) - \mathsf{\bigwedge}\!\left({a_3},{a_4},{b_1}\,;\,{b_3},{b_4},{a_1}\right)\\&& +\mathsf{\bigwedge}\!\left({b_2},{a_1},{b_1}\,;\,{a_2},{b_1},{a_1}\right) + \mathsf{\bigwedge}\!\left({a_3},{a_1},{b_1}\,;\,{b_3},{b_1},{a_1}\right).\end{eqnarray*}
It follows from Lemma 3·18 and Lemma 3·22 that
$E_2$
is in
$\ker(J)$
. Next, we observe that:
\begin{eqnarray*}E_2&=& \mathsf{IHX}'_3\!\left({a_1},{a_4}\,;\,{a_2},{a_3}\right)+ \mathsf{\bigwedge}\!\left({a_3},{b_3},{a_4}\,;\,{b_4},{a_1},{b_1}\right) - \mathsf{\bigwedge}\!\left({a_4},{b_4},{a_1}\,;\,{b_1},{a_2},{b_2}\right)\\&& -\mathsf{\bigwedge}\!\left({b_2},{a_2},{a_4}\,;\,{a_2},{b_2},{b_4}\right)+ \mathsf{\bigwedge}\!\left({b_2},{a_2},{a_1}\,;\,{a_2},{b_2},{b_1}\right) \\&& +\mathsf{\bigwedge}\!\left({b_2},{a_1},{b_1}\,;\,{a_2},{b_1},{a_1}\right)+ \mathsf{\bigwedge}\!\left({a_3},{a_1},{b_1}\,;\,{b_3},{b_1},{a_1}\right) \\&& -\mathsf{\bigwedge}\!\left({a_3},{b_3},{a_4}\,;\,{a_2},{b_2},{b_4}\right)+ \mathsf{\bigwedge}\!\left({a_3},{b_3},{a_1}\,;\,{a_2},{b_2},{b_1}\right) \\&=& \mathsf{IHX}'_3\!\left({a_1},{a_4}\,;\,{a_2},{a_3}\right)+ \mathsf{\bigwedge}\!\left({a_3},{b_3},{a_4}\,;\,{b_4},{a_1},{b_1}\right) - \mathsf{\bigwedge}\!\left({a_4},{b_4},{a_1}\,;\,{b_1},{a_2},{b_2}\right)\\&& + \mathsf{IHX}_3\!\left({a_1},{a_4}\,;\,{a_2}\right) - \mathsf{\bigwedge}\!\left({a_1},{b_1},{a_4}\,;\,{b_4},{a_2},{b_2}\right)+ \mathsf{\bigwedge}\!\left({a_4},{b_4},{a_1}\,;\,{b_1},{a_2},{b_2}\right)\\&& -\mathsf{IHX}_3\!\left({a_2},{a_3}\,;\,{a_1}\right)+\mathsf{\bigwedge}\!\left({a_2},{b_2},{a_3}\,;\,{b_3},{a_1},{b_1}\right)-\mathsf{\bigwedge}\!\left({a_3},{b_3},{a_2}\,;\,{b_2},{a_1},{b_1}\right)\\&& -\mathsf{\bigwedge}\!\left({a_3},{b_3},{a_4}\,;\,{a_2},{b_2},{b_4}\right)+ \mathsf{\bigwedge}\!\left({a_3},{b_3},{a_1}\,;\,{a_2},{b_2},{b_1}\right) \\&=& \mathsf{IHX}'_3\!\left({a_1},{a_4}\,;\,{a_2},{a_3}\right)+ \mathsf{IHX}_3\!\left({a_1},{a_4}\,;\,{a_2}\right) -\mathsf{IHX}_3\!\left({a_2},{a_3}\,;\,{a_1}\right)\\&& + \mathsf{D}\!\left({a_3},{b_3}\,;\,{a_4},{a_2}\,;\,{a_1},{b_1}\right)+ \mathsf{D}\!\left({a_2},{b_2}\,;\,{a_3},{b_4}\,;\,{a_1},{b_1}\right)\\&&+\mathsf{D}\!\left({a_3},{b_3}\,;\,{a_1},{a_4}\,;\,{a_2},{b_2}\right).\end{eqnarray*}
From the previous paragraph, we know that
$\mathsf{IHX}_3\!\left({a_1},{a_2}\,;\,{a_3}\right)$
belongs to
$\ker(J)$
: so, by the G-action,
$\mathsf{IHX}_3\!\left({a_1},{a_4}\,;\,{a_2}\right)$
and
$\mathsf{IHX}_3\!\left({a_2},{a_3}\,;\,{a_1}\right)$
do too. Then, it follows from Lemma 3·15 and the above decomposition of
$E_2$
that
$\mathsf{IHX}'_3\!\left({a_1},{a_4}\,;\,{a_2},{a_3}\right)$
is in
$\ker(J)$
: using the G-action, so is
$\mathsf{IHX}'_3\!\left({a_1},{a_2}\,;\,{a_3},{a_4}\right)$
.
4. Structure of certain subquotients of the Torelli group
In this section, we derive from Theorem A and Theorem B some explicit descriptions of certain quotients of (subgroups of) the Torelli group
$\mathcal{I}$
.
4·1. The groups
$\Gamma_2 \mathcal{I}/\Gamma_3 \mathcal{I}$
,
$\mathcal{K}/\Gamma_3 \mathcal{I}$
and
$\mathcal{I}/\Gamma_3 \mathcal{I}$
Set
$\mathrm{D}'_2(H) \,:=\, S^2(\Lambda^2 H)/\Lambda^4 H$
, and view it as a lattice in
${S^2(\Lambda^2 H^\mathbb{Q})}/{\Lambda^4 H^\mathbb{Q}}\simeq \mathrm{D}'_2(H) \otimes \mathbb{Q}$
. Let also
$\mathrm{D}_2(H)$
be the submodule of
${S^2(\Lambda^2 H^\mathbb{Q})}/{\Lambda^4 H^\mathbb{Q}}$
generated by
$\mathrm{D}'_2(H)$
and the elements
$(1/2)(u\wedge v)\cdot(u\wedge v)$
for all
$u,v\in H$
. According to [
Reference Faes3
], the images
$\tau_2([\mathcal{I},\mathcal{I}])$
and
$\tau_2(\mathcal{K})$
of the second Johnson homomorphism are determined by the following commutative diagram with exact rows:

Here, the map
$S^2H \otimes \mathbb{Z}_2 \to \Lambda^2 H \otimes \mathbb{Z}_2$
is the canonical projection, and the “trace” maps are defined as follows:
Consider a basis
$S\,=\,\{a_1,\dots,a_g,b_1,\dots,b_g\}$
of H of the form (2·6), and let
$\langle -,-\rangle=\langle -,-\rangle_S\,:\,H \times H \to \mathbb{Z}$
be the symmetric bilinear form defined by
$\langle a_i,b_j\rangle = \delta_{i,j},\ \langle a_i,a_j\rangle =0,\ \langle b_i,b_j\rangle =0.$
Let also
$\Theta=\Theta_S\,:\,{S^2(\Lambda^2 H^\mathbb{Q})}/{\Lambda^4 H^\mathbb{Q}} \to \mathbb{Q}$
be the map defined by
Lemma 4·1. The restriction of
$\Theta$
(respectively,
$2\Theta$
) to
$\ker(\!\operatorname{Tr}^S\!)$
(respectively, to
$\ker(\!\operatorname{Tr}^\Lambda\!)$
) reduced modulo
$4\mathbb{Z}$
does not depend on the choice of the symplectic basis S.
Proof. Since
$\mathcal{K}/[\mathcal{I},\mathcal{I}]$
is 2-torsion, the abelian group
$\ker(\!\operatorname{Tr}^\Lambda\!)/\ker(\!\operatorname{Tr}^S\!)$
has to be also 2-torsion, so it suffices to prove the statement for the restriction of
$\Theta$
to
$\ker(\!\operatorname{Tr}^S\!)$
. Since
$\ker(\!\operatorname{Tr}^S\!)=\tau_2([\mathcal{I},\mathcal{I}])$
is the image of the map
$B^{(0)}:\Lambda^2 (\Lambda^3H) \to \mathrm{D}'_2(H)$
defined by (3·2), it suffices to check that the reduction of
modulo 4 is independent of the choice of S, for any
$x_1,x_2,x_3,y_1,y_2,y_3 \in H$
. Indeed, this integer
should be compared to the integer
\begin{eqnarray*}\widetilde{\theta} &\,:=\,& \sum_{i,j\in \mathbb{Z}_3}\omega(x_i,y_j) \, \big( \omega(x_{i+1}, y_{j+2}) \, \omega( x_{i+2} , y_{j+1})- \omega( x_{i+1}, y_{j+1})\, \omega( x_{i+2} , y_{j+2})\big) \\&=& -3 \begin{vmatrix}\omega(x_1,y_1) & \omega(x_1,y_2) & \omega(x_1,y_3)\\ \omega(x_2,y_1) & \omega(x_2,y_2) & \omega(x_2,y_3)\\ \omega(x_3,y_1) & \omega(x_3,y_2) & \omega(x_3,y_3)\\ \end{vmatrix}\end{eqnarray*}
which (obviously) does not depend on S. By decomposing every factor in
$\theta$
of the form
$\langle x,y \rangle$
as a sum
$\omega(x,y)+2\, z(x,y)$
where
$z(x,y) \in \mathbb{Z}$
, and distributing all the products, we easily observe that
$\theta-\widetilde{\theta}$
belongs to
$4\mathbb{Z}$
.
We can now give a complete description of the abelian groups
$\Gamma_2 \mathcal{I}/ \Gamma_3 \mathcal{I}$
and
$\mathcal{K}/ \Gamma_3 \mathcal{I}$
.
Theorem 4·2.
-
(i) The homomorphism
$(\tau_2,8d'')$
induces an isomorphism (4·2)onto the free abelian group
\begin{equation} \Gamma_2 \mathcal{I}/ \Gamma_3 \mathcal{I} \stackrel{\simeq}{\longrightarrow} \mathrm{U}'(H)\end{equation}
\begin{equation*}\mathrm{U}'(H)\,:=\,\big\{ (T,z) \in \mathrm{D}'_2(H) \oplus \mathbb{Z}\,:\,\operatorname{Tr}^S(T)=0, 2\Theta(T) \equiv -z\!\! \mod 8 \big\}.\end{equation*}
-
(ii) Similarly, the homomorphism
$(\tau_2,8d'')$
induces an isomorphism (4·3)onto the free abelian group
\begin{equation} \mathcal{K}/ \Gamma_3 \mathcal{I} \stackrel{\simeq}{\longrightarrow} \mathrm{U}(H)\end{equation}
\begin{equation*}\mathrm{U}(H) \,:=\, \big\{ (T,z) \in \mathrm{D}_2(H) \oplus \mathbb{Z}\,:\,\operatorname{Tr}^\Lambda(T)=0, 2\Theta(T) \equiv - z\!\! \mod 4 \big\}.\end{equation*}
Proof. According to Proposition 3.2, we have the commutative diagram

where, according to Theorem B, the map B is injective: it follows that
$(\tau_2,8d'')$
is injective.
To specify the image of
$(\tau_2,8d'')$
, we now review the way d
″ can be defined from
$\lambda$
, the Casson invariant of
$\mathbb{Z}$
-homology 3-spheres. Consider the Heegaard splitting
$S^3=A \cup B $
of genus g of the 3-sphere, and let
$j:\Sigma \hookrightarrow S^3$
be an embedding of our surface
$\Sigma$
such that
$j(\Sigma)$
is the Heegaard surface
$A\cap B=\partial A =-\partial B$
deprived of a small disk D. Then, consider the map
where
$S^3(\,f,j)$
is the homology 3-sphere
$A \cup_f B$
obtained by “cutting”
$S^3$
along its Heegaard surface and gluing back with
$(\,j \circ f \circ j^{-1})\cup \operatorname{id}_D\,:\,\partial B \to \partial A$
. Then, by [
Reference Massuyeau and Meilhan21
, lemma 7·2], we have
Here the basis S of H is chosen so that
$a_1,\dots,a_g$
(respectively,
$b_1,\dots,b_g$
) are the homology classes of a system of meridional curves
$\alpha_1,\dots,\alpha_g$
for the handlebody A (respectively, meridional curves
$\beta_1,\dots,\beta_g$
for the handlebody B).
Let
$f\in \Gamma_2 \mathcal{I}$
: then
$\lambda_j(\,f)$
is even as a consequence of [
Reference Morita23
, corollary. 4.4]. Thus, it follows from (4·4) that
$8d''(\,f)\equiv - 2\Theta(\tau_2(\,f))\!\! \mod 8$
; hence
$(\tau_2(\,f),8d''(\,f))$
belongs to
$\mathrm{U}'(H)$
. Conversely, let
$(T,z) \in \mathrm{U}'(H)$
: we claim that (T,z) is in the image of
$\Gamma_2\mathcal{I}$
by
$(\tau_2,8d'')$
. Indeed, by (4·1), there exists
$f\in \Gamma_2 \mathcal{I}$
such that
$\tau_2(\,f)=T$
. We know by [
Reference Morita22
, proposition 6·4] (see also [
Reference Massuyeau and Meilhan21
, proposition 6·3]) the existence of a
$\psi \in \ker\tau_2$
such that
$\lambda_j(\psi)=1$
: hence we have
$\psi^2 \in \Gamma_2 \mathcal{I} \cap \ker\tau_2$
and
$\lambda_j(\psi^2)=2$
. Therefore, for any
$\ell\in \mathbb{Z}$
, the element
$f_\ell \,:=\, f \psi^{2\ell}$
of
$\Gamma_2 \mathcal{I}$
satisfies
Thus, taking
$\ell\,:=\, d''(\,f)-z/8 \in \mathbb{Z}$
, we obtain that the value of
$f_\ell$
by
$(\tau_2,8d'')$
is (T,z). This achieves the proof of (i): the homomorphism (4·2) is bijective.
We now prove (ii). The surjectivity of (4·3) is proved similarly to the surjectivity of (4·2). Moreover, the injectivity of (4·2) implies the injectivity of (4·3) in the following way. Let
$k\in \mathcal{K}$
be such that
$\tau_2(k)=0$
and
$d''(k)=0$
. The fact that
$\tau_2(k)=0$
implies that the function
$\beta(k):\mathcal{Q} \to \mathbb{Z}_2$
(image of k by the Birman–Craggs homomorphism) is constant [
Reference Johnson17
, p
$.$
178], and the fact that
$d''(k)=0$
implies then that
$\beta(k)$
is null. We deduce from Johnson’s determination (2·1) of
$\mathcal{I}_{\operatorname{ab}}$
that
$k\in \Gamma_2 \mathcal{I}$
.
The following result, which describes the structure of the group
$\mathcal{I}/\Gamma_3 \mathcal{I}$
, is a refinement of Morita’s description [
Reference Morita23
, Theorem 3·1] of the group
$\mathcal{I}/\ker(\tau_2)$
.
Theorem 4·3. The extension of groups

is central, and its characteristic class viewed as an element of
maps any
$(x_1\wedge x_2 \wedge x_3) \wedge (y_1\wedge y_2 \wedge y_3)$
to
\begin{equation*}\Bigg( \sum_{i,j\in \mathbb{Z}_3}\omega(x_i,y_j) \, (x_{i+1} \wedge x_{i+2})\cdot (y_{j+1} \wedge y_{j+2}),- 2 \begin{vmatrix}\omega(x_1,y_1) & \omega(x_1,y_2) & \omega(x_1,y_3)\\ \omega(x_2,y_1) & \omega(x_2,y_2) & \omega(x_2,y_3)\\ \omega(x_3,y_1) & \omega(x_3,y_2) & \omega(x_3,y_3)\\ \end{vmatrix} \Bigg).\end{equation*}
Proof. The centrality of the extension is given by Theorem A. Let
$s\,:\,\Lambda^3 H \to \mathcal{I}/\Gamma_3 \mathcal{I}$
be a setwise section of
$\tau_1$
, and let
$c\,:\,\Lambda^3H \times \Lambda^3H \to \mathcal{K}/\Gamma_3\mathcal{I} $
be the corresponding 2-cocycle, i.e
$.$
$c(x\vert y)=s(x)\, s(y)\, s(xy)^{-1}$
. Then, as an element of
$\operatorname{Hom}(\Lambda^2(\Lambda^3 H), \mathcal{K}/\Gamma_3\mathcal{I})$
, the cohomology class C of c is given by
$C(x\wedge y) = c(x\vert y)\, c(y \vert x)^{-1}= [s(x),s(y)].$
Thus, we have a commutative diagram

where the composite
$[-,-] \circ (\tau_1 \times \tau_1)^{-1}$
is the map
$J_2$
. Then the conclusion comes from Proposition 3·2 and the definition of the map B.
We now give three applications of the previous theorems.
Corollary 4·4. The group
$\mathcal{I}/\Gamma_3 \mathcal{I}$
is torsion-free, and its center is
$\mathcal{K}/\Gamma_3\mathcal{I}$
.
Proof. The group
$\mathcal{I}/\Gamma_3 \mathcal{I}$
is torsion-free because (by Theorem 4·2 (ii)) it is an extension of a torsion-free abelian group by another one.
Let
$f\in \mathcal{I}$
with the property that
$[f,h]\in \Gamma_3 \mathcal{I}$
for all
$h\in \mathcal{I}$
. Then, we have
$d''([f,h])=0$
for all
$h\in \mathcal{I}$
and, by Proposition 3·2, we obtain that
$\tau_1(\,f) \in \Lambda^3H$
belongs to the kernel of the bilinear map
\begin{equation*}b\,:\,\Lambda^3 H \times \Lambda^3 H \longrightarrow \mathbb{Z}, (x_1\wedge x_2 \wedge x_3, y_1\wedge y_2 \wedge y_3) \longmapsto\begin{vmatrix}\omega(x_1,y_1) & \omega(x_1,y_2) & \omega(x_1,y_3)\\\omega(x_2,y_1) & \omega(x_2,y_2) & \omega(x_2,y_3)\\\omega(x_3,y_1) & \omega(x_3,y_2) & \omega(x_3,y_3)\\\end{vmatrix}.\end{equation*}
But, this form is non-singular since
$b(s_1 \wedge s_2 \wedge s_3, \widetilde{s_1} \wedge \widetilde{s_2} \wedge \widetilde{s_3}) = \pm 1$
for any pairwise-different
$s_1,s_2,s_3 \in S$
. Therefore, we have
$\tau_1(\,f)=0$
so that
$f\in \mathcal{K}$
. This proves that the center of
$\mathcal{I}/\Gamma_3 \mathcal{I}$
is contained in
$\mathcal{K}/\Gamma_3 \mathcal{I}$
. The converse inclusion is given by Theorem 4·3.
Denote by
$\mathcal{M}=\mathcal{M}[0] \supset \mathcal{M}[1] \supset \mathcal{M}[2] \supset \cdots$
the Johnson filtration of the mapping class group
$\mathcal{M}$
. Thus, for every
$k\geq 0$
,
$\mathcal{M}[k]$
is the subgroup of
$\mathcal{M}$
acting trivially on the kth nilpotent quotient
$\pi/\Gamma_{k+1} \pi$
of the fundamental group
$\pi=\pi_1(\Sigma, \star)$
. So far, we have encountered
$\mathcal{M}[1]=\mathcal{I}$
,
$\mathcal{M}[2]=\mathcal{K}=\ker \tau_1$
and
$\mathcal{M}[3]=\ker \tau_2$
. The inclusion
$\Gamma_k \mathcal{I} \subset \mathcal{M}[k]$
holds true for every
$k\geq 1$
, and determining the gap between the two filtrations is an important question: thus, the problem is to determine the kernel and the image of the induced homomorphism
In degree
$k=1$
, the kernel
$\mathcal{M}[2]/\Gamma_2 \mathcal{I}$
of (4·5) is isomorphic to the 2-torsion group
$B_{\leq 2}(\mathcal{Q})$
via the Birman–Craggs homomorphism
$\beta$
. The following, which identifies the kernel of (4·5) for
$k=2$
, is a direct consequence of Theorem 4·2 (i).
Corollary 4·5. We have
$(\Gamma_2\mathcal{I} \cap \mathcal{M}[3])/\Gamma_3 \mathcal{I} \simeq \mathbb{Z}$
via d
″.
By [
Reference Johnson16
], the map (4·5) is surjective in degree 1; but it is not in degree 2 since
$\beta$
induces an isomorphism between
$\mathcal{M}[2]/(\mathcal{M}[3] \cdot \Gamma_2 \mathcal{I})$
and
$B_{\leq 2}(\mathcal{Q})/B_{\leq 0}(\mathcal{Q})$
[
Reference Yokomizo30
, Prop
$.$
3.3]. The following gives the surjectivity of (4·5) in degree 3.
Corollary 4·6. We have
$\mathcal{M}[3] = \mathcal{M}[4] \cdot \Gamma_3 \mathcal{I}$
.
Proof. Let
$f \in \mathcal{M}[3]$
. By [
Reference Faes2
, Theorem A], there exists an element
$\psi \in \mathcal{M}[4]$
such that
$\lambda_j(\psi) = -1$
, which implies that
$2d''(\psi) = 1$
by (4·4). We also have that
$2d''(\mathcal{M}[3]) \subset \mathbb{Z}$
, hence setting
$k \,:=\, \psi^{2d''(\,f)} \in \mathcal{M}[4]$
, we obtain that
$fk^{-1} \in \mathcal{M}[3]$
and
$d''(\,fk^{-1}) = 0$
. It follows from Theorem 4·2 (ii) that
$fk^{-1}$
belongs to
$\Gamma_3 \mathcal{I}$
.
4·2. Relation to the monoid of homology cylinders
Let
$\mathcal{IC}\,:=\,\mathcal{IC}(\Sigma)$
be the monoid of homology cylinders over the surface
$\Sigma$
: its neutral element is the trivial cylinder
$\Sigma \times [-1,+1]$
, and its operation is the “stacking product”. The reader is referred to the survey paper [
Reference Habiro and Massuyeau12
] for the precise definition of
$\mathcal{IC}$
, and an overwiew of its relationship with the study of the Torelli group. Here, we simply recall a few facts and some notations about homology cylinders:
-
(1) the monoid
$\mathcal{IC}$
comes with a sequence of
$Y_k$
-equivalence relations (for
$k\geq 1$
), which are defined by surgery techniques; -
(2) the Y-filtration
$\mathcal{IC}= Y_1\mathcal{IC} \supset Y_2\mathcal{IC} \supset Y_3\mathcal{IC} \supset \cdots$
on the monoid
$\mathcal{IC}$
is defined by
$Y_k\mathcal{IC} \,:=\, \{ M \in \mathcal{IC}\,:\,M \textrm{ is $Y_k$-equivalent to } \Sigma \times [-1,+1] \}$
; -
(3) for every
$k\geq 1$
, the quotient monoid
$\mathcal{IC}/Y_k$
is actually a group; -
(4) the “mapping cylinder” construction defines a monoid homomorphism
$\textbf{c}:\mathcal{I} \to \mathcal{IC}$
, which is injective and maps the lower central series to the Y-filtration.
It is an important problem to compare the lower central series of
$\mathcal{I}$
with the pull-back by
$\textbf{c}$
of the Y-filtration. In the lowest (non-trivial) degree, it is known that the homomorphism
$\textbf{c}:\mathcal{I}/\Gamma_2\mathcal{I} \to \mathcal{IC}/Y_2$
induced by
$\textbf{c}$
is an isomorphism [
Reference Habiro10
,
Reference Massuyeau and Meilhan20
]. In the next degree, the group
$\mathcal{IC}/Y_3$
has been given a complete description in [
Reference Massuyeau and Meilhan21
, Theorem 5·8], in the same spirit of Theorem 4·3 and in terms of “symplectic Jacobi diagrams”; but the question of its comparison with the group
$\mathcal{I}/\Gamma_3 \mathcal{I}$
was left open. We can now answer this question.
Theorem 4·7. There is an exact sequence of groups

where
$\alpha$
denotes the “quadratic part” of the relative Alexander polynomial of homology cylinders, as defined in [
Reference Massuyeau and Meilhan21
, section 3·2].
Proof. Some of the homomorphisms that we considered in the previous subsections on (subgroups of)
$\mathcal{I}$
extend to (submonoids of)
$\mathcal{IC}$
. Specifically, we shall need the following:
-
(i) the first Johnson homomorphism extends to
$\tau_1\,:\,\mathcal{IC} \to \Lambda^3 H$
, and encodes the action of
$\mathcal{IC}$
on
$\pi/\Gamma_3 \pi$
; we denote its kernel by
$ \mathcal{KC}\,:=\, \mathcal{KC}(\Sigma)$
; -
(ii) the second Johnson homomorphism extends to
$\tau_2\,:\,\mathcal{KC} \to \mathrm{D}_2(H)$
, and encodes the action of
$\mathcal{KC}$
on
$\pi/\Gamma_4 \pi$
; -
(iii) the second core of the Casson invariant extends to
$d''\,:\,\mathcal{KC} \to \mathbb{Q}$
, and formula (4·4) generalises to(4·7)where
\begin{equation} d''= -\frac{\lambda_j}{2} - \frac{\check{\Theta}_S\circ \alpha}{4}- \frac{\Theta_S\circ \tau_2}{4},\end{equation}
$\lambda_j\,:\,\mathcal{IC} \to \mathbb{Z}$
measures the Casson invariant after the “insertion” of homology cylinders, and
$\check{\Theta}_S\,:\,S^2H \to \mathbb{Q}$
is a certain homomorphism depending on the choice of the basis S of H.
We prove the injectivity of
$\textbf{c}:\mathcal{I}/\Gamma_3\mathcal{I} \to \mathcal{IC}/Y_3$
. Let
$f\in \mathcal{I}$
whose mapping cylinder
$\textbf{c}(\,f)$
is
$Y_3$
-equivalent to the trivial cylinder. Since the action of
$\mathcal{IC}$
on
$\pi/\Gamma_4 \pi$
is preserved by
$Y_3$
-surgery, we have
$f\in \mathcal{K}$
and
$\tau_2(\,f)=0$
. Since the Casson invariant is preserved by
$Y_3$
-surgery, we also have
$d''(\,f)=0$
. It follows from the injectivity of (4·3) in Theorem 4·2 that f belongs to
$\Gamma_3 \mathcal{I}$
.
That the image of
$\textbf{c}:\mathcal{I}/\Gamma_3\mathcal{I} \to \mathcal{IC}/Y_3$
is contained in
$\ker \alpha$
is given by [
Reference Massuyeau and Meilhan21
, proposition 3·13]. To prove the converse inclusion, let
$M\in \mathcal{IC}$
satisfying
$\alpha(M)=0$
. Since
$\tau_1\,:\,\mathcal{I} \to \Lambda^3 H$
is surjective, we observe that
$\mathcal{IC}=\mathcal{KC} \cdot \mathbf{c}(\mathcal{I})$
: thus, there is an
$f\in \mathcal{I}$
such that
$M_0\,:=\, M \cdot \mathbf{c}(\,f^{-1})$
belongs to
$\mathcal{KC}$
. Next, according to [
Reference Faes4
, proposition 6·1], we have the commutative diagram

where the projection p maps
$h\cdot k$
to
$(h\wedge k \!\! \mod 2)$
for all
$h,k\in H$
. Therefore, the fact that
$\alpha(M_0)=\alpha(M)=0$
implies that
$\tau_2(M_0) \in \ker \mathrm{Tr}^\Lambda $
; besides, we deduce from (4·7) that
$8d''(M_0)\equiv -2 \Theta(\tau_2(M_0))\!\!\mod 4$
. Then, it follows from the surjectivity of (4·3) in Theorem 4·2 that there exists
$u \in \mathcal{K}$
such that
$d''(u)=d''(M_0)$
and
$\tau_2(u)=\tau_2(M_0)$
. As a consequence of [
Reference Massuyeau and Meilhan21
, Theorem A], we deduce that
$\mathbf{c}(u)$
is
$Y_3$
-equivalent to
$M_0$
. Hence we obtain that
belongs to the image of
$\mathbf{c}$
.
Finally, the sequence (4·6) is also exact at
$S^2 H$
for the following reasons. The identity
$\mathcal{IC}\,=\,\mathcal{KC} \cdot \mathbf{c}(\mathcal{I})$
implies that
$\alpha(\mathcal{IC})=\alpha(\mathcal{KC})$
. We know from [
Reference Garoufalidis and Levine6
, Theorem 3] that the map
$\tau_2$
in (4·8) is surjective, and we deduce from [
Reference Massuyeau and Meilhan21
, proposition 3·13] that
$\alpha(\mathcal{KC})$
contains
$\ker p\,=\,\langle h^2 \,\vert\, h\in H \rangle$
. Thus, we conclude that
\begin{eqnarray*}\alpha(\mathcal{KC})\ = \ \alpha(\mathcal{KC}) + \ker p&=& p^{-1}\big( \operatorname{Tr}^\Lambda(\mathrm{D}_2(H))\big)\\&\stackrel{(4.1)}{=}&p^{-1}\big( \ker \omega\,:\,\Lambda^2 H \otimes \mathbb{Z}_2 \to \mathbb{Z}_2\big)\ \\&=& \ \big( \ker (\omega\!\!\!\mod 2)\,:\,S^2 H \to \mathbb{Z}_2\big).\\[-37pt]\end{eqnarray*}
Acknowledgements
The first author was supported by Grant 200020_207374 of the Swiss National Science Foundation. The work of the second author was partly funded by the project “AlMaRe” (ANR-19-CE40-0001-01); the IMB receives support from the EIPHI Graduate School (ANR-17-EURE-0002). The work of the third author was partly supported by JSPS KAKENHI Grant Numbers JP18K03310 and JP22K03298.














