The approximation argument used to prove the decay of intersection multiplicities is flawed. In this correction, we give an alternative argument in a similar spirit, based on an explicit form of the approximation that we deduce from [Reference DisegniDis22]. This argument requires some bounds on the ramification so that the main theorem is weakened.
Referring to the paragraph The nonsplit case in § 1.1,Footnote
1
our general approximation result involved local arithmetic intersections, and so it does not imply the vanishing of global intersections with flat divisors in a proper local integral model. Instead, we revisit an idea of Perrin-Riou and apply an operator “
$U_{p}-1$
”. Since this acts as a difference operator on the Fourier coefficients of our generating series, we obtain the vanishing (up to multiples of
$p^{s}$
) once we prove, by inspection, that the relevant sequences of approximating vertical components are constant in the index s.
I would like to thank Wei Zhang for pointing out the mistake.
Corrected statement
We denote by
$S_{p,\mathrm {ns}}$
the set of places of F above p that are nonsplit in E. In Theorem B, the assumption that
$\chi _{p}$
is sufficiently ramified should be replaced by the following assumption:
$$ \begin{align} \textit{for each}\ v\in S_{p, \mathrm{ns}},\ v\ \textit{is inert and}\ \chi_{v}\ \textit{is unramified}. \end{align} $$
Remark 1. It should be possible to prove the theorem also (at least) in the case where at some nonsplit places
$v\vert p$
, the representation
$\pi _{v}$
is unramified and
$\chi _{v}$
is arbitrary. While in principle not more difficult than the case treated here, this case would require introducing a larger number of changes in the setup, making for a cumbersome text. We thus prefer to defer it to a future work under a different global approach.
The mistake
It occurs in Proposition 4.3.3, whose proof (with notation as in loc. cit.) correctly shows that
$$ \begin{align}\begin{aligned} (\overline{z}\cdot D) = c[\kappa(y):\kappa] q_{F,v}^{s}+ \rho (V\cdot D')_{y}.\end{aligned}\end{align} $$
The term
$(V\cdot D')_{y}$
is a local intersection multiplicity at y, and it is not necessarily equal to the global intersection
$(V\cdot D)$
on
$\mathscr {X}$
. Therefore, the corresponding terms in the formula displayed in the proof of Corollary 4.3.5 do not necessarily vanish, as the definition of flat extensions invoked in that proof only applies to global intersection pairings.
Correction
We explain the strategy to prove the statement under the hypothesis (1).
Setup
We discard Assumption 3.4.1 on
$\chi _{p}$
; as in the corrected statement, we assume instead that v is inert and
$\chi _{v}$
is unramified for all
$v\in S_{p, \mathrm {ns}}$
. We suppose that
$(\phi , U)$
satisfy the assumptions of [Reference DisegniDis17, § 6.1] as well as Assumption 3.4.2, and the following extra assumption. Let
$T_{\iota _{\mathfrak {p}}}(\sigma ^{\vee })$
be a spherical
$\sigma ^{\vee }$
-idempotent as in [Reference DisegniDis17, Proposition 2.4.4], which we may take to be of degree zero; by [Reference RamakrishnanRam], we may and do assume that
$T_{\iota _{\mathfrak {p}}}(\sigma ^{\vee })$
is supported at split places of F where all the data is unramified.
Assumption 2. We have
$$ \begin{align}\begin{aligned}\phi=T_{\iota_{\mathfrak{p}}}(\sigma^{\vee}) \phi^{\flat}\end{aligned}\end{align} $$
for some
$\phi^{\flat }$
satisfying the assumptions of [Reference DisegniDis17, § 6.1].
This assumption will have the same effect as Assumption 3.4.1; namely, it ensures that the geometric kernel can be written in terms of height pairings of degree-zero divisors.
Denote by
$\mathrm {T}(\sigma ^{\vee }) $
the Hecke correspondence on
$X_{U}$
attached to
$T_{\iota _{\mathfrak {p}}}(\sigma ^{\vee }) $
via [Reference DisegniDis17, Lemma 5.2.2]; it has degree zero. Then by the definitions and [Reference DisegniDis17, Lemma 5.2.2],
$$ \begin{align*}{}^{\mathbf{q}}\widetilde{Z}(\phi^{\infty}, \chi)_{U}=\langle {}^{\mathbf{q}}\widetilde{Z}_{*}(\phi^{\flat, \infty})1, \mathrm{T}(\sigma^{\vee}) t_{\chi}\rangle,\end{align*} $$
and in
$\overline {\mathbf {S}}{}'$
, we have the decomposition
$$ \begin{align*}{}^{\mathbf{q}} \widetilde{Z}( \phi^{\infty}, \chi) =\sum_{v} \widetilde{Z}( \phi^{\infty}, \chi)(v),\end{align*} $$
where
$$ \begin{align}\begin{aligned} \widetilde{Z}( \phi^{\infty}, \chi)(v)=\sum_{w\vert v} \langle {}^{\mathbf{q}} \widetilde{Z}_{*}(\phi^{\flat, \infty})1, \mathrm{T}(\sigma^{\vee})^{\mathrm{t}} t_{\chi}\rangle_{\ell,w}.\end{aligned}\end{align} $$
For
$w\nmid p$
, we may move the correspondence
$\mathrm {T}(\sigma ^{\vee })^{\mathrm {t}}$
back to the left entry by interpreting the resulting pairing similarly to [Reference Yuan, Zhang and ZhangYZZ12]. Namely, the local height pairing of two degree-zero divisors
$D_{1}$
,
$D_{2}$
on X is, up to a factor
$\ell (\varpi _{w})$
, the intersection multiplicity of flat extensions of
$D_{1}$
,
$D_{2}$
to an integral model (see [Reference DisegniDis17, Proposition 4.2.2]). In turn, this arithmetic intersection pairing extends to divisors of arbitrary degree with disjoint supports by considering
$\widehat {\xi }$
-admissible (rather than flat) extensions as in [Reference Yuan, Zhang and ZhangYZZ12, § 7.1]. As a result, the pairing
$$ \begin{align*}\langle {}^{\mathbf{q}}\widetilde{Z}_{*}(\phi^{ \infty})1, t_{\chi}\rangle_{\ell,w}\end{align*} $$
is well-defined and it equals the w-term in (4). The fact that
$t_{\chi }$
may not have degree zero introduces a term given by pairing with the Hodge class
$\widehat {\xi }$
, which however vanishes under our assumptions as in [Reference Yuan, Zhang and ZhangYZZ12, Proposition 7.3.3]. Thus, the expression of [Reference DisegniDis17, (8.2.1)] for
$\widetilde {Z}( \phi ^{\infty }, \chi )(v)$
is still valid, and Theorem 3.6.1 continues to hold under our assumptions.
Theorem B is therefore still reduced to Proposition 3.6.2. For each nonsplit
$v\vert p$
, fix
$m=m_{v}\geq r$
, which is a multiple of the order of
$\varpi _{v}$
in the set (7) below. Define an operator
$\mathscr {R}_{v}:= \mathrm {U}_{v, *}^{m_{v}}-1$
. We will prove the following.
Proposition 3. Let
$v\vert p$
. Under our running assumptions, the element
$$ \begin{align*}\mathscr{R}_{v}\widetilde{Z}(\phi^{\infty}, \chi)(v)\in \overline{\mathbf{S}}{}'\end{align*} $$
is v-critical in the sense of (3.1.7).
Since
$\ell _{\varphi ^{p},\alpha }\circ \mathscr {R}_{v}= (\alpha _{v}^{m}-1)\ell _{\varphi ^{p},\alpha }$
, and
$\alpha _{v}^{m}-1\neq 0$
by our assumptions, the proposition still implies Proposition 3.6.2
Decay of intersection multiplicities
We prove Proposition 3. We fix an inert place v of F, and denote by w its extension to E.
Given our assumption that
$\chi _{v}$
is unramified, we consider the action of
$\mathscr {O}_{E,w}^{\times }$
on CM points; for the set
$\Xi (\varpi _{v}^{r})_{a}$
of Lemma 4.1.3, we have
$$ \begin{align*}[\Xi(\varpi_{v}^{r})_{a}U_{F, v}^{\circ}]_{U}= \mathrm{rec}_{E_{w}}(\mathscr{O}_{E,w}^{\times}/ \mathscr{O}_{F,v}^{\times}(1+\varpi_{v}^{r+s}\mathscr{O}_{E,w})) [x(\overline{b}_{a})]_{U},\end{align*} $$
where the Galois action is faithful, and
$\overline {b}_{a}$
is any element of
$$ \begin{align}\begin{aligned} q_{v}^{-1}( 1-a(1+\varpi_{v}^{r}\mathscr{O}_{F,v})) / (1+\varpi_{v}^{r+s}\mathscr{O}_{E,w}) \end{aligned}\end{align} $$
In fact, let
$\sqrt {\ {} }$
be the principal square root defined in a neighbourhood of
$1\in \mathscr {O}_{F, v}$
. Then, if
$v(a)\geq 1$
(or
$v(a)\geq 2 $
if
$v\vert 2$
), we may and do fix
$\overline {b}_{a}$
to be the class of
$$ \begin{align*}{b}_{a}:=[\sqrt{1-a}].\end{align*} $$
Correspondingly, we define
$$ \begin{align*}H_{00}\end{align*} $$
to be the finite abelian extension of E with norm group
$U_{F}^{\circ } U_{T}^{v}\mathscr {O}_{E,v}^{\times }$
. It is contained in the extension
$H_{0}$
defined before Proposition 4.1.4, and it is unramified at w. The study of intersection multiplicities of § 4.3 then needs to take place in
$\mathscr {X}$
, the base change to
$H_{00, \overline {w}}$
of the integral model
$\mathscr {X}^{\natural }/\mathscr {O}_{F_{v}}$
of
$X_{U}$
defined by Carayol (we are renewing the notation: the model
$\mathscr {X}$
considered in § 4 is no longer in use). Note that under our assumption,
$H_{00, \overline {w}/F_{v}}$
is unramified, so that
$\mathscr {X}$
is still regular.
Consider Proposition 4.3.3. As noted above, its statement needs to be corrected by replacing (4.3.2) by
$$ \begin{align}\begin{aligned} (\overline{z}\cdot D) = c[\kappa(y):\kappa] q_{F,v}^{s}+ \rho (V\cdot D')_{\mathscr{X}_{y}}, \end{aligned}\end{align} $$
where
$V=V(z)$
,
$\rho =\rho (z)$
. (The proof goes through verbatim in our renewed setup.)
The following is the new ingredient needed.
Proposition 4. The sequence
$$ \begin{align*}(V_{s}, \rho_{s}):=\left((V,\rho)([x(\overline{b}_{a\varpi_{v}^{ms}})]_{U})\right)_{s\in \mathbf{N}}\end{align*} $$
is eventually constant.
Proof. We first consider
$V_{s}$
. By construction, it is the irreducible component of
$\mathscr {X}_{\kappa }$
maximising the intersection multiplicity with the closure of the image
$z_{s}\in X_{H_{00, \overline {w}}}$
of
$[x(\overline {b}_{a\varpi _{v}^{ms}})]_{U}$
. Here,
$\kappa $
is the residue field of
$H_{00, \overline {w}}$
. However, the irreducible components of
$\mathscr {X}_{\kappa }$
are already defined over the residue field
$\kappa ^{\natural }$
of
$F_{v}$
. Therefore,
$V_{s}$
is the base-change of the component
${V}_{s}^{\natural }\subset \mathscr {X}_{\kappa ^{\natural }}^{\natural }$
maximising the intersection multiplicity with the closure of the image
$z_{s}^{\natural }\in X_{F_{v}}$
of
$z_{s}$
.
We explicitly compute
$V_{s}^{\natural }$
in terms of the (equivalent) notions of geometric and algebraic basins of irreducible components introduced in [Reference DisegniDis22]. In fact,
$V_{s}^{\natural }$
is, essentially by definition, the component through y to whose (geometric) basin the point
$z_{s}^{\natural }$
belongs. First, recall from [Reference CarayolCar86, Reference DisegniDis22] that
-
– the supersingular points in
$\mathscr {X}_{\kappa }$
are parametrised by (7)
$$ \begin{align}\begin{aligned} B(v)^{\times}\backslash \mathbf{B}^{v\infty, \times}\times F_{v}^{\times}/(U^{v}\times q(U_{v}));\end{aligned}\end{align} $$
-
– the irreducible components of
$\mathscr {X}_{\kappa ^{\natural }}$
are parametrised by
$(\mathscr {O}_{F_{v}}/\varpi _{v}^{r}\mathscr {O}_{F_{v}})$
-lines
$L\subset (\varpi _{v}^{-r}\mathscr {O}_{F_{v}}/\mathscr {O}_{F_{v}})^{2}$
; -
– to a CM-by-E point
$z\in X_{F_{v}}$
with sufficiently large conductor is attached an
$F_{v}$
-isomorphism
$\tau \colon E_{w}\to F_{v}^{2}$
, normalised so that (8)and a corresponding line
$$ \begin{align}\begin{aligned}\mathscr{O}_{F,v}^{2}\subset \tau(\mathscr{O}_{E,w})\not\supset \varpi_{v}^{-1}\mathscr{O}_{F, v}^{2},\end{aligned}\end{align} $$
$L(\tau )= [\tau (\mathscr {O}_{E_{w}})]\subset (\varpi _{v}^{-r}\mathscr {O}_{F_{v}}/\mathscr {O}_{F_{v}})^{2}$
.
Then, in order to show the eventual constancy of
$V_{s}^{\natural }$
, we need to show that, for
$y_{s}$
the reduction of
$z_{s}$
and
$\tau _{s}$
the invariant attached to
$z_{s}^{\natural }$
, we have
$y_{s+1}=y_{s}$
and
$L(\tau _{s+1})=L(\tau _{s})$
(for any sufficiently large s).
We have
$[x(\overline {b}_{a\varpi _{v}^{m(s+1)}})]_{U}= [x(\overline {b}_{a\varpi _{v}^{ms}}) h)]_{U}$
where, setting
$b_{s}:= b_{a\varpi _{v}^{ms}}$
,
$$ \begin{align*}h= (1+\mathrm{j} b_{s})^{-1}(1+\mathrm{j} b_{s+1})= {1\over a\varpi_{v}^{ms}} {\left(\begin{array}{@{}cc@{}}{(1-b_{s})(1+b_{s})} & {[b_{s+1}(1-b_{s}) - b_{s}(1-b_{s+1})] \mathrm{T}} \\ {} & {(1+b_{s}) (1-b_{s+1})} \end{array}\right)} \end{align*} $$
in
$B_{v}^{\times }=\mathrm {GL}_{2}(F_{v}).$
The group
$B_{v}^{\times }$
acts on the supersingular points via the map to the group (7) induced by the reduced norm q. By construction,
$q(h)=\varpi _{v}^{m}$
has trivial image there; thus,
$y_{s+1}=y_{s}$
.
We have
$b_{s}=1-2^{-1}a\varpi _{v}^{ms} +O(\varpi _{v}^{ms})$
, so that
$$ \begin{align*}h \equiv {\left(\begin{array}{@{}cc@{}} 1 & {\mathrm{T}/2} \\ {} & {0} \end{array}\right)}\quad \pmod{ \varpi_{v}^{m}}.\end{align*} $$
By the construction in [Reference DisegniDis22, (1.2.1)], the group
$B_{v}^{\times }$
acts on the invariant
$F_{v}^{\times }\tau $
via left multiplication by
$h^{\mathrm {t}}$
. Recalling the normalisation (8), we then have
$$ \begin{align*}L(\tau_{s+1})= L\left( {\left(\begin{array}{@{}cc@{}} c & {} \\ {c\mathrm{T}/2} & {0} \end{array}\right)} \tau_{s}\right),\end{align*} $$
where
$c\in F_{v}^{\times }$
is such that the matrix is integral and not divisible by
$\varpi _{v}$
. But this line is just the one spanned by
${1 \choose 0}$
(note that
$\tau _{s}$
, as a surjective map to
$F_{v}^{2}$
, cannot be annihilated by a nonzero matrix over
$F_{v}$
). Thus,
$V_{s}$
is constant for
$s\geq 2$
.
We now show the eventual constancy of
$\rho _{s}$
. In fact, for large enough s, we have
$\rho _{s} = { (\overline {z}_{s}\cdot \Delta ) / (V_{s} \cdot \Delta )}$
for any divisor
$\Delta $
whose support does not contain
$V_{s}$
. We take
$\Delta =\mathrm {q}^{*}\Delta _{0}$
, where
$\mathscr {X}_{0}$
is as in the beginning of § 4.3,
$\mathrm {q}\colon \mathscr {X} \to \mathscr {X}_{0, \mathscr {O}_{H_{00}, \overline {w}}}$
is the projection, and
$\Delta _{0}$
is the Zariski closure of the canonical lift of
$y:=y_{s}=y_{s+1}$
. By the projection formula, and with the notation of the proof of Lemma 4.3.2, the intersection
$(\overline {z}_{s}\cdot \Delta )$
is a constant multiple of
$$ \begin{align}(\overline{\mathrm{q}(z_{s})}\cdot \Delta_{0})_{\mathscr{X}_{0, \mathscr{O}_{E, \overline{w}}^{\mathrm{un}}}, y}=\mathrm{dim}_{k} \mathscr{O}_{E, \overline{w}}^{\mathrm{un}}[[u]] / (\nu_{s}, u).\end{align} $$
Here, by [Reference GrossGro86], the local defining equation of the canonical lift
$ \Delta _{0}$
is
$u=0$
, and for the quasicanonical lift
$\overline {\mathrm {q}(z_{s})}$
, it is
$\nu _{s}(u)=0$
for an Eisenstein polynomial
$\nu _{s}$
. Thus, (9) equals
$1$
independently of s. This completes the proof.
The following replaces Corollary 4.3.5.
Corollary 5. If
$D\in \mathrm {Div}^{0}(X_{H_{0}})_{L}$
is any degree-zero divisor, then for all sufficiently large s and all a,
$$ \begin{align}\begin{aligned} m_{\overline{w}}( \widetilde{Z}_{a\varpi^{m(s+1)}}(\phi^{\infty}) [1]_{U}, D) - m_{\overline{w}}( \widetilde{Z}_{a\varpi^{ms}}(\phi^{\infty}) [1]_{U}, D) =O(q_{F,v}^{ms}) \end{aligned}\end{align} $$
in L, where the implied constant can be fixed independently of a and s.
Proof. Let
$\widehat {D}$
be a flat extension of D to a divisor on
$\mathscr {X}$
(with coefficients in L), and abbreviate
$Z_{a,s}:= \widetilde {Z}_{a\varpi ^{ms}}(\phi ^{\infty }) [1]_{U}$
. Then by the corrected Proposition 4.3.3,
$$ \begin{align}\begin{aligned} m_{\overline{w}}( Z_{a,s}, D)= (\overline{Z}_{a,s}\cdot \widehat{D}) = A_{s} q_{F,v}^{ms}+ \sum_{i} \lambda_{i,s}(V_{i,s} \cdot D^{\prime}_{s}) \end{aligned}\end{align} $$
for some vertical components
$V_{i,s}\subset \mathscr {X} $
and some
$A_{s}$
,
$\lambda _{i,s}\in L$
; here, we have written
$\widehat {D}=c_{s}\mathscr {X}_{\kappa }+ D^{\prime }_{s}$
, where
$D^{\prime }_{s} $
is a divisor whose support does not contain
$V_{s}$
. By Proposition 4 (transported by Hecke correspondences away from v), all terms indexed by s are, in fact, eventually independent of s; thus, the second term of (11) gives vanishing contribution to (10). As remarked in Corollary 4.3.5, the constant
$A=A_{s}$
is independent of a as well.
Then the argument of the proof of Proposition 3.6.3 at the very end of the paper goes through to prove Proposition 3, with the following modifications: we apply the operator
$(\mathscr {R}_{v}^{\mathrm {seq}}\star )_{s}:= \star _{m(s+1)}- \star _{ms}$
to (4.4.2) and (4.4.4) (each viewed as a sequence
$\star $
in s), and we use Corollary 5 instead of Corollary 4.3.5.
Erratum to [Reference DisegniDis17]
In Lemma 8.2.1 and in the Proof of Proposition 8.2.2, one should read ‘
$F^\times \mathbf{A}^{S_1 \infty, \times}$
’ in place of
$\mathbf{A}^{S_1 \infty, \times}$
.
I am grateful to Yangyu Fan for pointing this out.
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