Towards explicit description of ramification filtration in the 2-dimensional
casepar VICTOR ABRASHKIN
RÉSUMÉ. Le résultat
principal
de cet article est unedescription explicite
de la structure des sous-groupes de ramification du grou- pe de Galois d’un corps local de dimension 2 modulo son sous-groupe des commutateurs d’ordre ~ 3. Ce résultat joue un role clé dans la preuve par l’auteur d’un
analogue
de la conjecture de Grothendieck pour les corps de dimensionsupérieure,
cf. Proc.Steklov Math.
Institute,
vol. 241, 2003, pp. 2-34.ABSTRACT. The
principal
result of this paper is anexplicit
de- scription of the structure of ramificationsubgroups
of the Galoisgroup of 2-dimensional local field modulo its
subgroup
of commu-tators of order ~ 3. This result
plays
a clue role in the author’sproof
of ananalogue
of the GrothendieckConjecture
forhigher
dimensional local
fields,
cf. Proc. Steklov Math. Institute, vol.241, 2003, pp. 2-34.
0. Introduction
Let K be a 1-dimensional local
field,
i.e. K is acomplete
discrete valu- ation field with finite residue field. Let T =Gal(Ksep/ K)
be the absolute Galois group of K. The classical ramificationtheory,
cf.[8], provides
IFwith a
decreasing
filtrationby
ramificationsubgroups r(v),
where v > 0(the
first term of this filtrationr(O)
is the inertiasubgroup
ofT).
This ad-ditional structure on T carries as much information about the category of local 1-dimensional fields as one can
imagine:
thestudy
of such local fieldscan be
completely
reduced to thestudy
of their Galois groupstogether
withramification
filtration,
cf.[6, 3].
The Mochizuki method is a veryelegant application
of thetheory
ofHodge-Tate decompositions,
but his method worksonly
in the case of 1-dimensional local fields of characteristic 0 and it seems it cannot beapplied
to other local fields. The author’s method is based on anexplicit description
of ramification filtration for maximalp-extensions
of local 1-dimensional fields of characteristic p with Galois groups ofnilpotent
class 2(where
p is aprime
number >3).
This infor- mation is sufficient to establish the above strongproperty
of ramificationfiltration in the case of local fields of finite characteristic and can be
applied
to the characteristic 0 case via the field-of-norms functor.
Let now K be a 2-dimensional local
field,
i.e. K is acomplete
discretevaluation field with residue field
I~~1~,
which isagain
acomplete
discretevaluation field and has a finite residue field.
Recently
I.Zhukov[9]
pro-posed
an idea how to construct ahigher
ramificationtheory
of suchfields,
which
depends
on the choice of a subfield of "1-dimensional constants"Kc
in K
(i.e. Kc
is a 1-dimensional local field which is contained in K and isalgebraically
closed inI~) .
Weinterpret
this idea to obtain the ramifi- cation filtration of the group r =consisting
of ramificationsubgroups F(") ,
where v runs over the ordered set J =J1
UJ2
withNotice that the
orderings
onJ1
andJ2
areinduced, respectively, by
thenatural
ordering on Q
and thelexicographical ordering
onQ 2,
andby
definition any element from
Ji
is less than any element ofJ2.
We no-tice also that the
beginning
of the above filtration comes, infact,
from the classical "1-dimensional" ramification filtration of the groupIF,
= and its "2-dimensional"part gives
a filtra-tion of the group r = Notice also that the
beginning
of the
"J2-part"
of ourfiltration,
whichcorresponds
to the indices from theset ((0, v) v
EQ>o}
CJ2
comes, infact,
from the classical ramification filtration of the absolute Galois group of the first residue field of K.In this paper we
give
anexplicit description
of theimage
of the ramifica- tion filtration in the maximalquotient of F ,
which is a pro-p-group ofnilpotent
class2,
when K has a finite characteristic p. Our methodis,
infact,
ageneralisation
of methods from[1, 2],
where the ramification filtra- tion of the Galois group of the maximalp-extension
of 1-dimensional local field of characteristic p modulo itssubgroup
of commutators of order > pwas described.
Despite
of the fact that we consider hereonly
the case oflocal fields of dimension
2,
our method admits a directgeneralisation
tothe case of local fields of
arbitrary
dimension n > 2.In a
forthcoming
paper we shall prove that the additional structure on rgiven by
its ramification filtration with another additional struc- turegiven by
thespecial topology
on each abeliansub-quotient
of r(which
was introduced in
[5]
and[7])
does not reconstructcompletely (from
thepoint
of view of thetheory
ofcategories)
the field K butonly
itscomposite
with the maximal
inseparable
extension of Theexplanation
of thisphenomenon
can be found in the definition of the "2-dimensional"part
ofthe ramification filtration: this
part
isdefined,
infact,
over analgebraic
closure of the field of 1-dimensional constants.
The paper was written
during
the author’s visits of theUniversity
ofLimoges (LACO UPRESA)
in the autumn of 1999 and of the Universities ofNottingham
andCambridge
in thebeginning
of 2000 year. The author expresses hisgratitude
to theseorganisations
forhospitality and, especially,
to Professors
J.Coates,
F.Laubie and I.Fesenko for fruitful discussions.1. Preliminaries: Artin-Schreier
theory
for 2-dimensional local fields1.1. Basic
agreements.
Let K be a 2-dimensionalcomplete
discrete val-uation field of finite characteristic p > 0. In other
words, K
is acomplete
field with
respect
to a discrete valuation V1 and thecorresponding
residuefield
K~l~
iscomplete
withrespect
to a discrete valuation v2 with finite residue field k rrNo
E N. Fix a fieldembedding s :
-K,
whichis a section of the natural
projection
from the valuationring OK
ontoFix also a choice of
uniformising
elementsto E K and To
EK(l).
Then K = andK(l)
=k((fo)) (note
that 1~ iscanonically
identifiedwith subfields in
K(l)
andI~).
We assume also that analgebraic
closureKalg
of K ischosen,
denoteby Ksep
theseparable
closure of K inKalg,
setr =
Gal(Ksep /K),
and use the notation To =s(To).
1.2.
P-topology.
Consider the set P of collections where for some EZ,
one hasJi(w)
E ~ if i and -ooif i >
I(w).
For any wP,
consider the setA(w)
C Kconsisting
of elements written in the formEiEz
whereall bi
EK{l~,
for a
sufficiently
small i onehas b2
=0, and bi
E if -oo.The
family (A (w) w
E~~
when taken as a basis of zeroneighbourhoods
determines a
topology
of K. We shall denote thistopology by to)
because its definition
depends
on the choice of the section s and the uni- formiser to . In thistopology
- 0 for i - +oc,where {bi}
is anarbitrary
sequence inI~~1~. Besides,
for any a EZ,
we have0 0
2013~ 0 ifj
--~and, therefore, s
is a continuousembedding
of into .K(with
respect
to the valuationtopology
onK(l)
and thePK(s, to)-topology
onK) .
It isknown,
cf.[5],
if t 1 is another uniformiser and s 1 is an an-other section from to
K,
then thetopologies PK(s, to)
andPK(si, ti)
are
equivalent. Therefore,
we can use the notationPK
for any of thesetopologies.
Thefamily
oftopologies PE
for all extensions E of K in.Kalg
is
compatible,
cf.[7, 5].
Thisgives finally
thetopology
onKalg
and thistopology (as
well as its restriction to any subfield ofKalg)
can be denotedjust by
P.1.3. Artin-Schreier
theory.
Let a be the Frobeniusmorphism
of K.Denote
by rib
the maximal abelianquotient
of exponent p of h. Considerthe Artin-Schreier
pairing
This
pairing
is aperfect duality
oftopological Fp-modules,
whereid)K
isprovided
with discretetopology,
andrib
has thepro-finite
topology
ofprojective
limitrib
= whereE/K
runs over thefamily
of all finite extensions inKalg
with abelian Galois group ofexponent
P.
Consider the set
7~2
withlexicographical ordering,
where theadvantage
is
given
to the first coordinate. Setand
A U {(0, 0)}.
Consider
K/(Q - id)K
withtopology
inducedby
theP-topology
of K(in
this and another cases anytopology
inducedby
theP-topology
willbe also called the
P-topology).
Choose a basis rNo}
of theIFp-module k
and an elementao E k
such that ao = I. Then thesystem
of elementsgives
aP-topological
basis of theFp
moduleid)K.
Let Q be the set of collections w = where
I(w)
E7G>o
and
Ji(w)
E N for all 0 iI(c.~).
Setand n A =
A°(w) B f (0, 0) 1 (notice
that(0, 0)
EDenote
by U1(W)
theFp-submodule
ofK/(a-id)K generated by
theimages
of elements of the set
~ .. ,
where To =
s(fo).
This is a basis of thesystem
ofcompact Fp-submodules
in
id)K
withrespect
toP-topology.
Let
be the
system
of elements ofrib
dual to thesystem
of elements(1)
withrespect to the
pairing Ç1.
Forw E Q,
setDenote
by Nli (resp., A4 I (c,~))
theF -submodule
inrib generated by ele-
ments
of Gi (resp.,
Notice thatG1 (resp., G1(cv))
is anFp-basis
of.Mi (resp., A4 i(w)).
For any then
We shall use the identification of elements A with their
images
in :and
r 1 (w )ab
is identified with thecompletion
of in thetopology given by
thesystem
of zeroneibourghoods consisting
of allFp-submodules
of finite index. Denote
by A4pf
thecompletion
ofA4 (
in thetopology
given by
thesystem
of zeroneibourghoods consisting
ofFp-submodules,
which contain almost all elements of the set
G1(W).
ThenA4pf (cv)
is theset of all formal
Fp-linear
combinationsand we have natural
embeddings
AWe notice that
rib
is thecompletion
in thetopology given by
thebasis of zero
neibourghoods
of the where for some w EQ, Vi
is
generated by
elements with I rNo
and andFp-module V2
has a finite index inA4 ( (w).
Denoteby
thecompletion
of
A4 I
in thetopology given by
thesystem
ofneibourghoods consisting
ofsubmodules
containing
almost all elements of the setGi.
ThenMil
is theset of all
Fp-linear
combinations of elements fromGl,
and we have naturalembeddings Mf
Crib
CMil.
1.4. Witt
theory.
Choose ap-basis i E 11
of K. Then for any M E N‘ and a field E such that K C E CKsep,
one can construct alifting
of E modulo
pM,
that is afully
faithfulZ/pMZ-algebra OM(E)
such that
OM(E) 0ZjpMZ Fp
= E. Theseliftings
can begiven explicitly
inthe form
where =
(ai, 0, ... , 0)
E Theliftings OM(E) depend
functo-rially
on E and behavenaturally
withrespect
to the actions of the Galois group r and the Frobeniusmorphism
a.For any
M e N,
consider the continuous Wittpairing
modulopm
where
Fj
is the maximal abelianquotient
of F ofexponent pm
consideredwith its natural
topology,
and the first term of tensorproduct
isprovided
with discrete
topology.
Thesepairings
arecompatible
for different M and induce the continuouspairing
where
O(K)
=limOm(K) 4
andr(p)ab
is the maximal abelianquotient
ofthe Galois group
T(p)
of the maximalp-extension
of K inKsep.
Now we
specify
the abovearguments
for the local field K of dimension 2given
in the notation of n. 1.l.Clearly,
the elements to and Togive a p-basis
of
K,
i.e. the system of elementsis a basis of the KP-module K.
So,
for any and K c E C we can consider thesystem
ofliftings
modulopm
where t =
[to],
T =[70]
are the Teichmullerrepresentatives.
Choose a basis
{ar ~ 1
1 ~ r of theZp-module W(k)
and itselement ao with the absolute trace 1. We agree to use the same notation for residues modulo
pm
of the above elements ar, 0 rNo.
Then thesystem
of elementsgives
aP-topological
ofOM(K)/(Q - id)OM(K).
For w E
Q,
denoteby
theP-topological
closure of thesubmodule of
generated by
theimages
of elements of the setThis is a basis of the
system
ofcompact (with respect
to theP-topology)
submodules of
OM(K)/(Q - id)OM (K) (i.e.
any itscompact
submodule is contained in some Asearlier,
we introduce thesystem
of elementsof rM
° m
, , , ,
I I I I
which is dual to the
system (4)
withrespect
to thepairing ÇM. Similarly
to subsection 1.3 introduce the
Z/pMZ-modules Mfw, A4Pf
and for anyw E
Q,
the subsetGM(W)
C and theíZ/pMZ-submodules
Apply
thepairing Ç,M
to defines theP-topology
on11M. By definition,,
the basis of zeroneibourghoods
ofr~
consists of annihilators ofcompact
submodulesUM(w),
w E0,
withrespect
to thepairing ~m.
We note that
Finally,
we obtain theP-topology
on : and note thatthe
identity
map id :r(p )pb_top
-]p(p)ab
is continuous.Equivalently,
ifE/K
is a finite abelianextension,
then there is an M E N and an w E Q such that the canonicalprojection r(p)ab
--> factorsthrough
thecanonical
projection T(p)ab
-->rM(W)ab.
1.5.
Nilpotent
Artin-Schreiertheory.
For any Liealgebra
L overZp
of
nilpotent
class p, we agree to denoteby G(L)
the group of elements of L with the law ofcomposition given by
theCampbell-Hausdorff
formulaConsider the
system
ofliftings (3)
from n.1.4 and setO(E)
where K C E c
Ksep.
If L is a finite Liealgebra
ofnilpotent
class p setLE
=L 0zp O(E).
Then thenilpotent
Artin-Schreiertheory
from[1]
ispresented by
thefollowing
statements:a)
for any e EG(LK),
there is anf
EG(LKsep)
such thataf
=f
o e;b)
thecorrespondence
T H(T f )
o(- f ) gives
the continuous group homo- IFG (L);
c) if el
EG(LK)
andfl
EG(LKsep)
is such thata fi
=fl
o el, then the ho-momorphisms Of,e and of,,,,
areconjugated
if andonly
if e = c o ei o(-QC)
for some c E
G(LK);
d)
for any grouphomomorphism ’l/J :
F 2013G(L)
there are e eG(LK)
andf
EG(LKseP)
suchthat ’l/JI,e.
In order to
apply
the abovetheory
tostudy
T we need itspro-finite
version.
Identify T(p)ab
with theprojective
limit of Galois groups of finite abelianp-extensions E/K
inKsep.
With this notation denoteby G(E)
the maximalquotient
ofnilpotent
class p of the LieZp-algebra G(E) generated freely by
theZp-module rElK.
Then G = is atopological
free Liealgebra
overZp
withtopological
moduleof generators
r(p)ab
and L = is the maximalquotient
of E ofnilpotent
classp in the
category
oftopological
Liealgebras.
Define the
"diagonal
element" e EO(K)/(a -
asthe element
coming
from theidentity endomorphism
with respect to the identificationinduced
by
the Wittpairing (here O(K)
is considered with thep-adic topol-
ogy).
Denoteby s
theunique
section of the naturalprojection
fromO(K)
to
id)O(K)
with values in theP-topological
closed submodule ofO(K) generated by
elements of the set(4).
Use the section s to obtain the elementsuch that e ~ e
by
the naturalprojection
For any finite abelian
p-extension E/K
in denoteby
eE theprojection
of e to
LK(E)
=L(E) 0zp O(K),
and choose acompatible
on Esystem
offE
EG(E)Sep
=£(E) 00(Ksep)
such thatafE
=fE
o eE. Then thecorrespondences
T HT fE
o(- fE) give
acompatible system
of group ho-momorphisms T(p)
--->G(,C(E))
and the continuoushomomorphism
induces the
identity morphism
of thecorresponding
maximal abelian quo- tients.Therefore, 0 gives
identification of p-groupsr(p)modCp(r(p))
andG(G),
whereCp(r(p))
is the closure of the sub- group ofr(p) generated by
commutators of order > p. Of course, iff = lim fE E
thenaf
=f
o e and1jJ(9)
=(g f )
o(- f )
for any g E T.Clearly,
theconjugacy
class of theidentification 0 depends only
onthe choice of uniformisers to and To and the element ao E
W(k).
For w E S2 and
M E N,
denoteby
the maximalquotient
ofnilpotent
class p of the free LeeZ/pMZ-algebra GM(w)
withtopological
module of
generators
We use the naturalprojections r(p)ab
-to construct the
projections
of Liealgebras L
2013GM(w)
andinduced
morphisms
oftopological
groupsClearly,
thetopology
on the groupG(£ M (w) )
isgiven by
the basis ofneigh-
bourhoods of the neutral element
consisting
of allsubgroups
of finite index.Consider
ZjpMZ-modules
and from n.1.4. Denoteby
the maximal
quotient
ofnilpotent
class p of a free Liealgebra
overZ /pZ generated
andby GM(w)
the similarobject
constructed for thetopological Z/pMZ-module Clearly, Lpf (w)
is identifiedwith the
projective
limit of Liesub-algebras
ofLM(w) generated by
allfinite
subsystems
of itssystem
ofgenerators
Besides,
we have the natural inclusionswhere is identified with the
completion
ofGM(w)
in thetopology
defined
by
all its Liesub-algebras
of finite index. LetLemma 1.1. There exists
Proof.
Denoteby e~(w)
theimage
of e inThe residues
eomod(a - id)V
andeo mod(a - id)V
coincide because the both appear as theimages
of the"diagonal
element" for the Wittpairing.
But eo and
eo
are obtained from the above residuesby
the same sectionid)V
-V, therefore,
Because intersection of all open submodules
Uo
of.MM(w)
is0,
one haseM(w)
and we can take asfM(cv)
theimage
off
EG(£sep)
under the natural
projection G(GseP)
-~ The lemma isproved.
0By
the above lemma we have anexplicit
construction of all group mor-phisms qbM(w)
with M E N and w E SZ. Theirknowledge
isequivalent
tothe
knowledge
of theidentification ~ mod Cp(r(p)),
because of theequality
which is
implied by
thefollowing
lemma.Lemma 1.2. Let L be a
finite (discrete)
Liealgebra
overZp
andlet 0 : r(p)
->G(L) be a
continuous groupmorphisme.
Then there areM E N,
w E Q and a continuous group
morphism
such that
Proof.
Let e EG(LK)
andf
EG(Lsep)
be suchthat a f
=f o e
and for anyg E
r(p),
it holdsI , , , », , noB.
One can
easily
prove the existence of c EG(LK)
such that forei =
(-c)
o e o(ac),
one haswhere E
Lk
= L 0W(k)
andl(o,o),o
=aol(o,o)
for someL(o,o) E
L.If
f 1 - f
oc then a 11
=f 1
o e 1 and for any g Eh,
Let
hl, ... , hu
E L be such that for some mi EZ>o
with1 i u,
where all coefficients
a(a,b),i E W(k),
thenwhere all coefficients
with M =
1
1 iul. Clearly,
there exists cv E S2 such thata(a,b),i
= 0 for i u and(a,
Let
131, ... , /3No
be the dualW(Fp)-basis
ofW (k)
for the basis 01521, ... ,00Na from n.1.4. Consider themorphism
of Liealgebras 0’ m (w) : £ M (w)
- Luniquely
determinedby
thecorrespondences
for all
(a, b)
EA(cv)
and 1 ~ rNo.
Clearly, 0’ m (w)
is a continuousmorphism
of Liealgebras,
which trans-forms
eM(w)
to ei. Letf’
EG(Lsep)
be theimage
offM(w),
thenf’
o el.So,
thecomposition
is
given by
thecorrespondence 0’(g) = (g f’~
o(- f’)
forall g
Er(p).
fore,
for any g Er(p),
So,
we can take such that for any 1 ELM(w),
The lemma is
proved.
D2. 2-dimensional ramification
theory
In this section we assume that K is a 2-dimensional
complete
discretevaluation field of characteristic p
provided
with an additional structuregiven by
its subfield of 1-dimensional constantsI~~
andby
a double valu- ationt~ : ~ 2013~ Q2
UBy
definitionKc
iscomplete (with respect
to the first valuation of
K)
discrete valuation subfield ofK,
which has fi-nite residue field and is
algebraically
closed in I~. Asusually,
we assumethat an
algebraic
closureKalg
of K ischosen,
denoteby Esep
theseparable
closure of any subfield E of
Kalg
inKalg,
sethE - Gal(Esep /E)
and usethe
algebraic
closure ofKc
in E as its field of 1-dimensional constantsEc.
We shall use the same
symbol v(°)
for aunique
extension ofv(°)
to E. We notice thatE 2013~ Q
Ugives
the first valuation on E and is inducedby
the valuation of the first residue fieldE(l)
of E. The conditionv~°~ (E* ) - Z2 gives
a natural choice of one valuation in the set of allequivalent
valuations of the field E.2.1. 2-dimensional ramification filtration of
hE
Let E be a finite extension of K inKalg.
Consider a finite extension L of E inEsep
and set
rL/E
=Gal(L/ELc) (we
note thatLc = If limf LIE
:=rE
L
then we have the natural exact sequence of
pro-finite
groupsThe 2-dimensional ramification
theory
appears as adecreasing
sequence of normalsubgroups r(j) I
jEJ2o -
wheref
FE,
Here
Q 2is
considered withlexicographical ordering (where
theadvantage
isgiven
to the firstcoordinate),
inparticular, J2
=({0~
xQ>o) U (Q>o x ~).
Similarly
to the classical(1-dimensional)
case, one has to introduce thefiltration in lower
numbering
for any finite Galois extensionL/E. Apply
the process of"eliminating
wild ramification" from[4]
tochoose a finite extension
Ec
ofLc
inKe,alg
such that the extension L :=LE
over E :=
EEC
has relative ramification index 1. Then thecorresponding
extension of the
(first)
residue fields£(1) / E(l)
is atotally
ramified(usually, inseparable)
extension ofcomplete
discrete valuation fields ofdegree [L : E~.
if 0 is a
uniformising
element of£(1)
then =°E(1) [0].
Introducethe double valuation
rings 0 E
:=] v(°) (1) > (0, 0) } and Oz
:=for any
lifting 0
of 0 toOr.
Thisproperty provides
us with well-defined ramification filtration ofrLjE c RLIE in
lowernumbering
where j
runs over the setJ2.
One can
easily
see that the above definition does notdepend
on thechoices of and 9. The Herbrand function
(2) L/E
:J2
--J2
is definedsimilarly
to the classical case: for any(a, b) E J2
take apartition
such that the groups are of the same
order 9i
forall j
between(ai-1, bi-1)
and(ai,
where1 i C s,
and setLet E C
L1
C L be a tower of finite Galois extensions inEsep.
Then theabove defined Herbrand function satisfies the
composition property,
i.e. forany j
EJ~2~,
one hasThis
property
can beproved
as follows. Choose as earlier the finite extensionEe
ofLc,
then all fields in the towerwhere L =
L1 = L1Ee, E = EEe (note
thatLe = Ee),
have the same uniformiser
(with respect
to the firstvaluation).
If 0 is auniformiser of the first residue field of L and 0 E
C~L
is alifting of 0,
then
01
= and0- L
=C~L1 (8~ .
But we have also°L1 =
because
N
isuniformizing
element of Now one can relate the values of the Herbrand function in the formula(8) by
classical 1-dimensionalarguments
from[8].
Similarly
to classical case one can use thecomposition property (8)
toextend the definition of the Herbrand function to the class of all
(not
nec-essarily Galois)
finiteseparable extensions,
introduce the upper number- andapply
it to define the ramification filtration of thesubgroup rE C rE .
2.2. Ramification filtration of
rE.
The above definition of 2-dimen- sional ramification filtration worksformally
in the case of 1-dimensionalcomplete
discrete valuation fields K. Note that in this case there is acanonical choice of the field of 0-dimensional constants
Kc,
and we do notneed to
apply
the process ofeliminating
wild ramification. Thisgives
forany
complete
discrete valuation subfield E CKalg,
theof the inertia
subgroup rE C rE.
Note also that this filtrationdepends
onthe initial choice of the valuation
v~~~ : ~C 2013~ Q
U(oc)
and coincides withclassical ramification filtration if
v(°) (E*)
= Z.Consider the 2-dimensional ramification
filtration r(j) lj"2
L EJjeJ2
and theabove defined 1-dimensional ramification filtration for the
(first)
valuation
Kr - Q
U-
Let J =
Ji
UJ2,
whereJi
=~(v, c) v >
Introduce theordering
onJ
by
the use of naturalorderings
onJ1
andJ2,
andby setting j, j2
forany jl
EJl
andj2
EJ2.
Forany j
=(v, c)
EJi ,
set =pr-1
where pr :
rE
is the naturalprojection.
Thisgives
thecomplete
ramification
filtration ]P(i)l E jEJ
of the groupTE.
For any finite extensionL/E,
we denoteby
its Herbrand function
given by
thebijection p (2)E:
L/EJ2 J2
from n.2.1and its 1-dimensional
analogue
1Jl
2013Tl (which
coincides with L.lEr *the classical Herbrand function if
v° (E*) - 2).
We note also that the above filtration contains twopieces coming
from the 1-dimensionaltheory
and the both of them coincide with the classical filtration if
v(o) (E*) = Z2.
The first
piece
comes as the ramification filtration ofgiven by
thegroups Ec =
rw’) ,(o,o)
E E forall v >
- 0. The secondpiece
comes from theramification filtration of the first residue field
E(1)
of E. Here for any v >0,
2.3. n-dimensional filtration. The above
presentation
of the 2-dimen- sional aspect of ramificationtheory
can begeneralised directly
to the caseof n-dimensional local fields. If K is an n-dimensional
complete
discretevaluation
field,
then weprovide
it with an additional structureby
its(n-1 )-
dimensional subfield of "constants"
Kc
and an n-valuation) : 2013
~n
U For anycomplete
discrete valuation subfield E ofK,
the n-dimensional ramification filtration appears as the
filtration E L of
the group
rE
= Gal(Esep/Ec,sep)
with indexes from the set(where Ee
is thealgebraic
closure ofK,
inE) .
The process ofeliminating
wild ramification
gives
for any finite Galois extensionLj E
a finite extensionEc
ofLe
such that for thecorresponding
fields L =LEe
and E =EEe,
theramification index of each residue field of L with
respect
to the firstr n - 2 valuations over the similar residue field of E is
equal
to 1.Then one can use the
lifting
O of anyuniformising
element of the residue fieldL~n-1~
to the n-valuationring I v~°~ (l) > (o, ... , 0)
toobtain the
property
-- ,- - ..
This
property provides
us with a definition of ramification filtration offilE C rLIE in
lowernumbering. Clearly,
ifLi
is any field between E andL,
andL 1
= then one has theproperty
This
provides
us with thecomposition property
for Herbrandfunction,
andgives finally
the definition of the ramification filtration E .7 ofF E in
upper
numbering.
One can choose a subfield of
(n - 2)-dimensional
constantsKee
CK
and
apply
the abovearguments
to obtain the ramification filtration ofGal(Kc,sep/Kcc,sep).
Thisprocedure gives finally
the ramification filtra- tion of the whole groupFE,
whichdepends
on the choice of adecreasing
sequence of fields of constants of dimensions
n - 1, n - 2, ... ,
and 1.3.
Auxiliary
factsIn this section K is a 2-dimensional
complete
discrete valuation fieldgiven
in the notation of n.l.l. We assume that an additional structureon K is
given by
its subfield of 1-dimensional constantsKc
and a doublevaluation such that
Kc
andv ~°~ (K* ) _ Z2 (or, equivalently, (1, 0)
andv~°~ (T°) _ (0,1)).
As in n.1.4 we use the construction ofliftings
of K andKsep,
whichcorresponds
to thep-basis (to, To)
of K.We reserve the notation t and T for the Teichmuller
representatives
of to and To,respectively.
For any tower of field extensions K C E C L CKalg,
we set
where is the ramification
subgroup
ofrE
=Gal(Esep/E)
with theupper
index j
E J.Similarly
to the 1-dimensionalcase, j (L/E)
is thevalue of the Herbrand function of the extension
L/E
in its maximal "edge point" .
Then thecomposition property (8)
from n.2.1gives
forarbitrary
tower of finite extensions E C
L1
CL,
If a E
W(k),
then asusually
3.1. Artin-Schreier extensions. Let L =
K(X ),
wherewith ao E 1~* and
Proof.
The aboveexamples
can be found in[9].
Theproperty a)
is a well-known 1-dimensional fact. The
property b)
followsdirectly
fromdefinitions,
we
only
note that one must take the extensionMe
= =to,
tokill the ramification of
L/K
and to rewrite theequation (10)
in the formThe
proposition
isproved.
D3.2. The field
K(N*, j*).
Let N* EI~,
q andlet j*
=(a*, b*)
EJ2
be such that A* := E
N[I/p],
B*:= b* (q -1)
E ~ and(B*, p)
= 1.Set s*
maxf 0, -vp(a*)
and introduce t10, t20 EKalg
such thattqo =
tos
and
t20 -
Proposition
3.2. There exists an extensionKo
=K(N*, j*) of
K inKsep
such that
a) Ko,c
=Kc
and[Ko :
= q;b) for any j
EJ2,
one has(what implies
thatj(Ko/K)
=j*);
c) if K2
:=KO(t2O),
then itsfirst
residuefield K’(1) equals k((TIO)),
where(here tf;
:= and E is ananalogue of
the Artin-Hasseexponential from
thebeginning of
thissection).
Proof.
Weonly
sketch theproof,
which is similar to theproof
ofproposition
of n.1.5 in the
paper [2].
It is easy to see that
[Li : Ki] = q
and the "2-dimensionalcomponent"
ofthe Herbrand function L1/W i is
given by
theexpression
fromn.b)
of ourproposition.
Then one can check the existence of the field K’ such that KC K’ C L 1, ~K’ : K]
= q andLi
We notice thatK~
=Kc
andone can assume that K’ Now the
composition property
of theH b d fu t.. I. h /f (2) Herbrand er ran function nc Ion
implies
Imp les that t atcp2)
i i =(P (2)
=
To
verify
theproperty c)
of ourproposition
let us rewrite the aboveequation
for U in thefollowing
formwhere
U’
~* = U andt2
= t1(notice
thatt10).
. Thisim p lies
theexistence of T2 E
L1
such that =T2 - b* (q- 1)
i,e. the lastequation
can be written in the form
_ .. , ..n - ..n’ _... ,
One can take T2 in this
equality
such thatTi-1 = Tfo E
K’ and aftertaking
the - (I /b*)-th
power of the both sides of thatequality,
we obtainThis
gives
the relationwhere A E is such that
vO (A)
>(0, 0).
Then a suitable version of theHensel Lemma
gives
the existence of B EK’(t2o)
such that(0, 0)
and the
equality
ofn.c)
of ourproposition
holds with3.3. Relation between different
liftings. Choose j*
EJ2
and N* EN,
which
satisfy
thehypothesis
from thebeginning
of n.3.2 and consider thecorresponding
fieldKo - K(N*, j*).
Let K’ =KO(t,o),
then K’ is apurely inseparable
extension ofKo
ofdegree q
andClearly,
K’ =
K’~1~ ((t10)),
whereK’(1)
=Consider the field
isomorphism T/ : K -- K’,
which isuniquely
definedby
the conditionsT/lk
=a-N*, 77(to)
= 10 andq(To)
= Tlo. Denoteby
Tls,,pan extension
of q
to a fieldisomorphism
ofKsep
andKsep.
For M >
0,
denoteby OM+1 (K’)
andrespectively,
the lift-ings
modulo of K’ and with respect tothe p-basis
of K’.We reserve now the notation t1 and Tl for the Teichmuller
representatives
ofelements ~10 and Tlo,
respectively. Clearly, OM+1 (K’)
and=
· On the other
hand, by n.c)
ofProp. 3.2,
K2 : = K’ (t2o )
=Ko (t2o )
is aseparable
extension ofK2 : = K (t2o ) .
We notethat
KK2,sep = KsepK2
andK2,sep = K sepK2.
· Denoteby OM+1(K2)
andrespectively,
theliftings
modulopM of K2
andK2,sep
withrespect to the
p-basis ft20, To)
ofK2 (as earlier,
t2 and T are the Teichmullerrepresentatives
of elements t2o and ro,respectively) . Clearly,
one has the naturalembeddings
*
With respect to these
embeddings
we have t= t2ps .
Denoteby ~M+1 (K2)
and the
liftings
ofI~2
and with respect to thep-basis
{~20?
of~"2 (as usually,
t2 and T1 are the Teichmullerrepresentatives
ofelements t20 and T10,
respectively) . Clearly,
With
respect
to theseembeddings
we havet2s
= tl.The first group of the above
liftings
can be related to theliftings
of thesecond group
by
thefollowing
chain ofembeddings Similarly,
one has theembedding
above
embeddings correspond
to the relationwhich follows from the basic
equation given by n.c)
ofProp.
3.2.3.4. A criterion. Let L be a finite Lie
algebra
overZp
ofnilpotent
classp and let be such that
pM+1 L
= 0. Consider the group homomor-phism ~o :
r ---·G(L). By
thenilpotent
Artin-Schreiertheory
there existsan e E