Ramification groups
in Artin-Schreier-Witt extensions
par LARA THOMAS
RÉSUMÉ. Soit K un corps local de
caractéristique
p > 0.L’ob jec-
tif de cet article est de décrire les groupes de ramification des pro-p extensions abéliennes de K à travers la théorie d’Artin-Schreier- Witt. Dans le cadre usuel de la théorie du corps de classes
local,
cette étude est menée entièrement et conduit à un
accouplement non-dégénéré
que nous définissons endétail, généralisant
ainsi laformule de Schmid pour les vecteurs de Witt de
longueur
n. Aupassage, on retrouve un résultat de
Brylinski
avec des argumentsplus explicites
nécessitant moins d’outilstechniques.
La dernière partie aborde le casplus général
où le corps résiduel de K estparfait.
ABSTRACT. Let K be a local field of characteristic p > 0. The aim of this paper is to describe the ramification groups for the pro- p abelian extensions over K with
regards
to the Artin-Schreier- Witttheory.
We shall carry out this investigationentirely
in theusual framework of local class field
theory.
This leads to a certainnon-degenerate
pairing that we shall define in detail,generaliz-
ing in this way the Schmid formula to Witt vectors oflength
n.Along
the way, we recover a result ofBrylinski
but with a differentproof
which is moreexplicit
and requires less technicalmachinery.
A first attempt is
finally
made to extend these computations tothe case where the
perfect
field of K ismerely perfect.
1. Introduction
By
a local field we mean a discrete valuation field withperfect
residuefield. Let p be a
prime
number. This paper is concerned with the ramifi- cation groups for the Artin-Schreier-Witt extensions over a local field K ofcharacteristic p,
i.e. for its pro-p abelian extensions.We fix once and for all a
separable
closure Ksep of K. For each n >1,
let
Gpn
be the Galois group of the maximal abelian extension of expo- nentpn
over K and letGpoo
be the Galois group of the maximal pro-p11anuscrit reçu le 29 juillet 2005.
abelian extension over K. We also denote
by W(K)
the commutativering
of Witt vectors over K andby Wn (K)
thequotient ring
of truncated Witt vectors oflength
n. We shall consider the additive groupmorphism W,, (K) --+ Wn(K) given by ...) (xp 01 xp 11 ...)
X17...).
Itskernel is
Wn (Fp) =
The Artin-Schreier-Witt
theory [17] yields isomorphisms
oftopological
groups:
:
Gpn ~ Hpn
=Wn(JFp))
Q r-+
~a
+a
for sorne a E such that
p(a)
= a and where the action ofGpn
on
Wn(Ksep)
is definedcomponentwise. Here, Hpn
isprovided
with theproduct topology
inducedby
the discretetopology
onWn(Fp).
The
goal
of this paperis, given n > 1,
to describeexplicitly
how theramification groups of
Gpn
in the uppernumbering
behave under the Artin-Schreier-Wittisomorphism
asn.When the residue field of K is
finite,
theinterplay
between local class fieldtheory
and Artin-Schreier-Witttheory gives
rise to anon-degenerate pairing,
that we shall call the Artin-Schreier-Wittsymbol:
W (Fp)
(a
+b.K*pn)
H[a, b)
:=(b, L/K)(~) -
a, wherep(a)
= a, L =K(a)
and(b, L/K)
is the norm residuesymbol
of b inL/K.
We shallcompute
thissymbol explicitly
so as toget
the ramification groups ofGpn by Pontryagin duality
under the existence theorem.Our main result is then the
following:
Theorem 1.1. Let K be a local
field of
characteristic p withfinite
residuefield.
For everyinteger
u >0,
the Artin-Schreier- Wittisomorphism
a.5n inducesisomorphisms of topological
groups:,,(0) (0) i
Hpn
andif u
> 1.p 20132013 p aa p 20132013
pn
Here,
for eachinteger v > -1,
is thesubgroup
ofHpn given by:
:=
Hpn ~
+ =0
where we set:
(v .-
_ j j _ j V j
.. -vWn
.- (K
, PK
,PK
For the
Wn (K)
form anincreasing
sequence ofsubgroups
ofWn(K),
withW£(K)
=Wn(OK)
andW,~ 1(I~) _ (Pk,... ,
The groups form an exhaustive anddecreasing
filtration ofHpn
that theorem 1.1puts
inbijection
with the ramification groups ofGpn.
By taking
the inverse limit when n tends toinfinity,
weget
an Artin- Schreier-Wittisomorphim
for the Galois groupGpoo
of the maximal pro-p abelian extension over K:where
W(Fp) ri Zp
isprovided
with thep-adic topology. Then,
we may deduce from theorem 1.1 the ramification groups forGpoo:
Corollary
1.1. The Artin-Schreier- Wittisomorphism gives
rise toisomorphisms of topological
groups:Another consequence of theorem 1.1 is concerned with the
computation
of the Artin conductor for a
cyclic
extension ofdegree pn
over K(see corollary
5.1 of section5) .
In this manner, we refine Satz 3 of~12~ by writing explicitly
every crucialstep
of theproof
and inparticular by describing precisely
the Schmid-Witt residue formula for Witt vectors oflength
rt incharacteristic p. At the same
time,
we obtain a more direct and moreexplicit proof
forBrylinski’s
Theorem 1 of~2~ .
We may also mention[4]
and we thank Michel
Matignon
forpointing
out this reference.One
question
is then to tackle theproblem
when the residue field of K is assumed to bemerely perfect
and wepartially
solve it in two directions:we show that in this context theorem 1.1 is still valid for all ramification groups of
Gp
as well as for the inertia group of each 1.Indeed,
completing [7]
we first claim:Theorem 1.2. Let K be a local
field of
characteristic p withperfect
residuefield.
The Artin-Schreierisomorphism
asi inducesisomorphisms of topo-
logical
groups:G(o) __i_y H(o) G(u) Hp’-1 if
u > 1.p p p
As for the inertia group of every maximal abelian extension of exponent
pn
overK,
we shallfinally
state:Theorem 1.3. Let K be a local
field of
characteristic p withperfect
residuefield.
For each n >1,
the Artin-Schreier- Wittisomoqphism
induces onthe inertia group
of Gpn
theisomorphism of topological
groups:E I
O}.
p inverse
limit,
deooyields
anisomorphism of topological Passing
to the inverselimit,
as,,,,yields
anisomorphism of topological
groups:
G~~~ ~ lw
E =01-
where
OK
denotes the valuationring of
K.One may notice that this last theorem corroborates theorem 1.1 for u = 0 and for all n > 1 since
(p
EHpn :
=0 1
because
p(Wn(OK))
=Wn(OK) n p(Wn(K)). Moreover,
itsproof
will alsoshow that it corroborates
corollary
1.1 for u = 0.When K has finite residue
field,
thekey point
is that the Artin-Schreier- Wittsymbol
isnon-degenerate
and that it can beexpressed
as the trace ofan
explicit symbol,
the Schmid-Wittsymbol
which isactually
a "residue Witt vector" . Thisreciprocity
formula was first discoveredby
Schmid[10]
in 1936 for the local norm
symbol
ofcyclic
extensions ofdegree
p in charac- teristic p,following
up the work initiatedby
Schmidt(with
a"t" )
and thenHasse to establish class field
theory
for function fields.Then,
Witt~17~
gen-eralized Schmid’s formula to
cyclic
extensions ofdegree p’~.
The formula isnow
classical,
butunfortunately
not as well known as it deserves to be andWitt
actually proved
it in characteristic 0only.
For these reasons, in this paper, anattempt
is made todevelop
this norm residue formula for Witt vectors of anylength
over K verycarefully, sparing
none of the details.When the residue field of K is
perfect,
the crucialstep
isproposition
6.2which describes ramification groups for a
compositum.
Note that we broachthe
topic
from two differentapproaches:
when the residue field of K isfinite,
local class field
theory
allows us todirectly
get the ramification for maximalArtin-Schreier-Witt
extensions,
but when it ismerely perfect
we first needto compute the ramification groups for finite abelian extensions of exponent
dividing p’~
beforetaking
thecompositum.
This note is
organized
as follows. We start with apreliminary
sectionof brief reminders in ramification
theory
and local class fieldtheory
forthe convenience of the reader but also to define the
setup
for thesequel.
This section also
provides
someterminology
for Witt vectors. Then section 3 is the technical heart of the paper since it deals with the Schmid-Witt residue formula for Witt vectors oflength
n when K has finite residue field.Next section 4
develops
the notion of reduced Witt vectors; this is used tocompute
the Artin-Schreier-Wittsymbol
in section 5 and thus to describe the ramification groups for all maximal abelian extensions of exponentp’~
over
K, proving
theorem 1.1 this way.Finally,
section 6 is a firstapproach
to the
analogous problem
when the residue field of K isperfect
with adirect
proof
for theorems 1.2 and 1.3.Acknowledgments.
I would like to thank Hendrik W. Lenstra for manymotivating
and fruitful discussions and I am indebted to FarshidHajir
forhis
suggestions
in thewriting
of this paper. I am alsograteful
to the GTEMnetwork and in
particular
to the node of Bordeaux forhaving supported
me
during
my severalstays
at theUniversity
of Leiden.The
present
paper ismainly
issued from my Ph.D. thesis[16]
that Idid at the
University
of Toulouse II under the direction of Christian Maire(Toulouse)
and Bart de Smit(Leiden).
2. Preliminaries
This section collects some definitions and standard
properties
ofhigher
ramification groups as well as some
terminology
from local class fieldtheory.
For more
details,
we shall refer the reader to[13],
from which we borrow most of the notation in this paper. Inaddition,
we shall also describe the basicproblems
we are concerned with in this paper.Throughout,
we will use thefollowing
notations:OK
is the valuationring
of
K,
pK its maximalideal, UK
is the unit group of K and r, its residue field. Once we choose auniformizing
element T forK,
we mayidentify
Kwith the of formal power series over /’1;. When r, is
supposed
tobe
finite,
we will write K =Fq
for some power q of p.Recall that if is a finite abelian extension of Galois group
G,
theith ramification groups in the lower
numbering
are defined as:VX E OL, U(X) - X E
for all
integers
i > -1.They
form adecreasing
filtration of G:G~_1~
... D
G~",~
=0,
for some m > 0. is a realnumber,
we set
G(,)
= whereiv
is theonly integer
suchthat iv -
1 viv.
The
problem
is that these ramification groups are notadapted
toquotients
and thus
they
cannot be extended to infinite extensions.Now,
there existsa
homeomorphism 1/J : [- 1; ~-oo~~ ~-1; usually
called the Herbrandfunction,
such that if one sets:Vu 2: -1, U
E1f8, G (u)
:=the groups not
only
form adecreasing
filtration in Gagain:
G~-1~
= G DG(l) D
... DG(l)
=0,
0,
but alsothey
areadapted
toquotients
in the sense that for all normalsubgroups H
of G onegets:
-1, (GIH)(u)
=C(u)H/H.
This relation is often called the Herbrand theorem. We can thus define ramification groups in the upper
numbering
for an infinite abelian extensionby taking
the inverse limit over all finite subextensions.In the case of a finite Artin-Schreier-Witt
extension,
one has =G(°)
because
L/K
iswildly
ramified.Taking
the inverselimit,
this remains trueif
L/K
is infinite.Moreover,
it isonly
in thewildly
ramified case that non-trivial occur for u >
1,
hence our motivation toinvestigate higher
ramification groups in the Artin-Schreier-Witt extensions.
For a
cyclic
extension ofdegree
p overK, following [5]
it is well knownthat:
Proposition
2.1. Let K be a localfield of
characteristic p > 0 withperfect
residue
field.
LetL/K
be the extensiongiven by
theequation
XP - X = afor
some a E K and denoteby
G its Galois group. Then we have:(1) If vK(a)
> 0 orif vK(a)
= 0 and a Ep(K),
the extensionL/K
istrivial.
(2) If vK(a)
= 0 andif p(K),
the extensionL/K
iscyclic of degree
p and
unramified.
(3) If vK(a) _
-m 0 with m EZ>o
andif m is prime
to p, the exten- sionLIK is cyclic of degree
pagain
andtotally ramified. Moreover,
its
rami, fication
groups aregiven by:
G
= G~-1~ _
...= G~m~
and =1.This list is exhaustive.
Indeed,
ifvK(a)
0 andif p
dividesvK(a),
then modulo is
congruent
to some b EWn(K)
such thatvK(b)
>vK(a)
since the residue field of K isperfect.
The extension L is also definedby
= b andby
iteration we are reduced to one of theprevious
cases. When K isfinite,
this argument can begeneralised easily
toevery extension of exponent
pn
over K for which nojump
in the filtration of its ramification groups is divisibleby p’~ (see
section5).
To a
cyclic
extensionL/K
ofdegree p’~,
Artin-Schreier-Witttheory
attaches a Witt vector a E
Wn(K)
modulo such that L =where a =
(~0, ..., ~~_1)
EWn(Ksep)
andp(a) =
a.Thereby,
as acorollary
ofproposition 2.1,
wealready
have:Corollary
2.1. LetL/K
be acyclic
extensionof degree pn given by
someWitt vector a =
(ao, ..., an- 1)
inWn (K) . If
allcomponents of
a lie inOK,
then
L/K is unramified.
Proof.
Let a =(~o, ..., (xn-1)
EWn(Ksep)
be such thatp(a)
= a. For alli E
f 0, ...,
writeKi
=K(aa,
...,ai)
andK- I =
K. Thenby
iterationeach extension is
cyclic
ofdegree
p and it isgiven by
anequation
X
= Pi where P2
is apolynomial
in ao, ..., ai-I, ao, ..., ai that allbelong
to the valuationring
ofKi-l. Thus, according
toproposition 2.1,
is unramified and so is L = over K. D
We wish to
complete
these statementsby considering
allhigher
ramifica-tion groups for all Artin-Schreier-Witt extensions. Under the
assumption
that is finite we shall achieve this
goal.
Indeed,
in the usual framework of local class fieldtheory,
i.e. when Khas finite residue
field,
the existence theorem(e.g. [14], Chap.V, §4)
is es-sentially
the statement that the normcompletion
of K* and thecompletion
with respect to its open
subgroups
of finite index are the same. General-izing
thereciprocity
law for finite abelianextensions,
itgives
rise to anisomorphism
oftopological
groups between this lattercompletion
and themaximal abelian Galois group
GK over K,
that we shall denoteby
~~.Moreover,
for allintegers u > 0,
it inducesisomorphisms
oftopological
groups
---=-.
where thesubgroups uj;)
are defined to be 1 +p£
g p K K g p K
K
and form a basis of
neighbourhoods
of 1 inUK. Therefore,
in oursetup,
the existence theoremyields isomorphisms
oftopological
groups:and for 0:
o(u)
The idea is then to
apply Pontryagin duality
to the Artin-Schreier-Wittsymbol
so as to describe the filtration Kby orthogonal- ity,
and thus the ramification groups ofGpn.
Note thatWn(K)//(Wn(K))
is a discrete abelian group and is an abelian
profinite
group thatare both annihilated
by pn.
ThusPontryagin duality
coincides with theHom(-, Wn (Fp) ) duality
on both of these groups since is canoni-cally isomorphic
toMoreover,
it establishesisomorphisms
oftopo- logical
groups between each group and its bidual. For further information aboutPontryagin duality,
we shall refer the reader to([8], Chap.2, ~9) .
The crucial step is then to
give
anexplicit
formulation tocompute
the Artin-Schreier-Wittsymbol.
When n =1,
this wasalready
doneby
Schmid
[10] :
Proposition
2.2(Schmid Formula). I f a
E K and b EK*,
then:a, b)
=Tr r;./’Fp (Res( a-,; )).
dbHere,
the residue is defined as follows. Iff
is inK,
thenf dT
is adifferential form of K. The coefficient before
T-’
is called the residue off dT
and denotedby Res( f dT).
One may prove that it does notdepend
on the choice of the uniformizer.
We should stress the fact that the Schmid formula is
essentially
basedon the more
general identity ~a, b)
=[c,t)
where c = for n = 1.This remark will be of
great
use in thefollowing (see
lemma3.1).
In the beautiful treatement of Serre
([13], Chap. XIV, §6),
the Schmidformula is
originally
used to prove the existence theorem in characteristic p.Indeed,
when the universal norm groupDK
of K is trivial the existence theoremyields
a continuousinjection
from K* intoGK.
In characteristic p, this isproposition
16 of([13], Chap. XIV, §5) arising
from the Schmidformula:
Proposition
2.3. Let K be a localfield of
characteristic p withfinite
residues
field. If
an element b E K* is a normf rom
everycyclic
exten-sion
of
Kof degree
p, then b E K*P.Therefore, DK
is divisible and thusDK = nnK *n
= 1. Thisproposition
also proves that the kernel on the
right
in the Artin-Schreier-Wittsymbol
is
trivial,
whereas its kernel on the left wasalready clearly
trivial under the Artin-Schreier-Witttheory.
Now,
as anexplicit computation
for the Artin-Schreier-Wittsymbol
onK/p(K)
xK* I K*P,
the Schmid formula allows us to express the ramifi- cation groups for the maximal abelian extension of exponent p over K in terms ofsubgroups
ofHp
=Hom(K/p(K), However,
wedelay
the
proof
untillater,
since it will be included in the moregeneral proof
oftheorem 1.1 in section 5.
The consideration of the maximal abelian extensions of
exponent p’~
overK makes
appeal
to Witt vectorsaccording
to the classical Artin-Schreier- Witttheory.
As a set,W(K)
consists of infinite sequences(xo, ~l, ...)
withcomponents
in K. This set is thenfunctorially provided
with two laws ofoperation by
use ofghost components.
If(Xo, Xl, ...)
is a sequence of inde-terminates,
we define the sequence of itsghost components (X(O), X(’),...)
by:
l
X l
= + ...lxl.
X(l) =6PXi =Xo + ... + p
i=0
If R is an
arbitrary ring,
thisgives
rise to a map from toR~
that weshall call the
ghost
map and denoteby F R. Now,
the maindifficulty
stemsfrom the
following
observation. When R has characteristic0,
theghost
map is
injective
and it is moreoverbijective
if p is invertible in R. But in characteristic p, theghost
map is nolonger injective.
We thusprovide W(R)
with two laws ofoperation
that come from the usual laws ofRN
under
hR
when R has characteristic 0.According
to[17],
theseoperations
are
given by
apolynomial
formula that we then use to define sum andproduct
onW (K) .
We then define on
W(K)
ashifting operator
Vby :
v :=
(xo, ...)
H(0,
xo,xl, ...).
In
particular,
for every n >1,
thering Wn (K)
of truncated Witt vectors is thequotient ring
and one can pass fromW (K)
toWn(K)
via the truncation
map tn
defined as(~o, ...)
H(xo,
...,zn-i ) .
ThenW(K)
is the inverse limit of all
Wn (K)
withrespect
to the truncation maps andas such one can
provide
it with thep-adic topology.
Atlast,
let us mentionthe relation
V o F = F o V = p
where F is the additivemorphism (~o, ... )
H(xo, ...)
and where p is themultiplication by
p; thisimplies
inparticular that p
and V commute.Since
Wl (K)
is the additive group ofK,
we are led to define for Witt vectors of anylength
anexplicit
formulation of the Artin-Schreier-Wittsymbol
that extends the Schmid formula.3. The Schmid-Witt
symbol
For
arbitrary n > 1,
we shalldevelop
ageneral
formula tocompute
theArtin-Schreier-Witt
symbol
on x Witt[17]
did it
precisely
for ap-adic
field in thelanguage
of invariants ofalgebras.
Drawing
ourinspiration
from hisformula,
we shall prove itcarefully
incharacteristic p.
The Artin-Schreier-Witt
pairing
isgiven by
thetheory
of the same name:(a + b.K*pn )
~[a, b)
:=(b, L/K) (o) -
a,for some a =
(ao,
...,an_1)
EWn(Ksep)
such thatp(a)
= a and whereL =
K(ao, ..., an-i ) . Besides, (b, L/K)
is thereciprocity
law of b inL/K;
it is also
wK(b)
restricted to L.The notation
[.,.)n
would be more convenient but forsimplicity
we shallrather use the notation
~., . )
even if it does notspecify
the index n.Anyway,
we shall
always
fix anarbitrary integer n >
1 in what follows.Only
section 2dealt with the Artin-Schreier-Witt
symbol
for n =1,
that is also called the Artin-Schreiersymbol simply. Besides,
note that the square bracket[ stands
for the
additivity
of the group whereas thebracket )
isrelated to the
multiplicativity
ofK* /K*pn .
This Artin-Schreier-Witt
pairing
satisfies thefollowing:
Proposition
3.1.(i)
The Artin-Schreier- Wittsymbol
is bilinear.(ii)
For every a EK, [a, b)
= 0if
andonly if
b is a norm in the extensionwhere a = such that
p(a)
= a.(iii)
For all a E K and b EK*, [Va, b)
= where V is theshirting operator.
Moreover, according
to the existence theorem we claim:Proposition
3.2. The Artin-Schreier- Wittsymbol
isnon-degenerate.
Proof.
Let a E and suppose that a = 0 for all b’s in K* .By
the existencetheorem,
is dense inGK,
thusGK
fixes theextension
K(a)
definedby
a, so a EWn (K)
and a Ep(Wn(K)).
Now let b E K* . If = 0 for all a E
Wn (K)
then1JK (b)
fixesall
cyclic
extensions ofdegree dividing pn,
thus it fixes all finite abelian extensions of exponentpn by taking
the union and so it fixes the maximalabelian extension of
exponent pn
over K.Therefore,
theimage
of1JK(b)
is the
identity
inGpn
which means that b EK *pn
under the existencetheorem. The converse is trivial. D
The main idea of this section is to consider the Schmid formula in relation with the so-called
ghost components
of some Witt vector. For a EWn (K)
and b E
K*,
the idea is then to switchtemporarily
to characteristic 0by lifting
a and b to some elements A and B inWn(R((T)))
andR((T))*
respectively
where R is anycomplete
discrete valuationring
of character- istic 0 with residue field r, =IFq.
The main observation is that thering
R =
W (Fq)
satisfies thisproperty (see [13], Chap. II, §, Thm.7) .
We thendefine an
explicit pairing
onWn(R((T)))
xR((T))*
with value inWn(R):
given
A and B it returns a Witt vector(A, B)
ingiven by
itsghost components
that areexpressed
as the residues of some elements inR( (T ) ) generalizing
in this way the Schmid formula. This is the "Residuenvektor"of
[17].
Thispairing
is such that afterreducing
toWn (K)
x K* weget
apairing
that we shall call the Schmid-Wittsymbol
and thatcorresponds
tothe Artin-Schreier-Witt
symbol.
This isproposition
3.4. Inproposition
3.5we then
give
another formulation for the Schmid-Wittsymbol
that doesnot use the reduction to
Wn(K)
x K*. Thepresent
section is thus intended toprovide
athorough exposition
of the details of this process.Note that
Xo
=X(O). Therefore,
theghost
map isbijective
fromonto A whatever the characteristic of the
ring
A is. This is the reasonwhy
the Schmid formula for n =1 does not use any lift at
all, following
up ourreasoning.
Let a E write a =
(ai)i with ai
= EFq((T))
and 0. Let b E
I~q ( (T ) ) *,
we write b =bmT m
+ h.o.t. withbm
EF§
(the
abbreviation h. o.t, stands forhigher
orderterms).
We shall lift a and b to A E and B EW (Fq ) ( (T ) ) * respectively
as follows:A = E
with,
for all z E{O, ..., 7~ 2013 1}:
with
(Bl)o
=bi,
for all l m.In
particular,
if weprovide W(Fq)((T))
with the usualvaluation,
theneach
A2
has valuation and B has valuationvK (b) .
Under the identification K =
I~q((T)),
we then define apairing Wn(K)
xK* -
Wn(IFp) given by
the left vertical line in thefollowing
commutativediagram:
where the vertical and horizontal arrows are defined as follows:
Here,
the trace on is defined as follows:with
respect
to the Wittaddition,
where d is suchthat q
=pd.
Note that the Witt vector
(A, B)
definedby
itsghost
components should lie in apriori. However, according
to Satz 4 of[17],
eachcomponent
of(A, B)
is apolynomial
withinteger
coefficients in the inde- terminatesBl,
andAi,v
for m, i > 0 and v > vi.Moreover,
Bm’
lies inW(Fq)
since its first componentbm
is a unit inFq. Therefore,
the vector
(A, B)
doesbelong
to and thediagram
is well de-fined.
Furthermore,
eachcomponent
of(a, b)
is apolynomial
withinteger
coefficients evaluated in
bml, bl
and since the first component of thesum
(resp.
theproduct)
of two Witt vectors is the sum(resp.
theproduct)
of their first
components.
Therefore,
the Witt vector(a, b)
EWn(Fq)
is well defined and it does notdepend
on the choice of the lifts A and B. We call it the Schmid-Wittsymbol
of a and b.Clearly,
the Schmid-Wittsymbol
satisfies thefollowing:
Proposition
3.3.(i)
The Schmid-Wzttpairing
is bilinear.(ii) (Va, b)
In order to show that the Artin-Schreier-Witt
symbol
and the Schmid- Wittsymbol
areactually
the same on xK*IK *pn,
wefirst prove one crucial lemma:
Lemma 3.1. Let a E
Wn (K)
and b E K*.I f c
=(a, b)
EWn (Fq),
then:[a, b)
=[c, T),
where
(., .) : Wn(K)
x ~ 2013~Wn(Fp) is
the Artin-Schreier- Wittpairing.
Proof.
Theproof
ismainly
due to[17],
we shall rewrite it to show how thecomputation
of the Schmid-Wittsymbol
works. It is based on thefollowing
relation:
for all Witt vectors .c =
(zo, ..., zn-i)
inWn(K)
where each is theWitt vector
(xi, 0, ..., 0).
We first assume that b = T and we write ao =
EVEZ ao,vT v
so that:a =
+ {2:
+~>0 v>O
for some Witt vector S~a in Note that since the first component of
a sum is the sum of the first
components, (Qa)o
= 0 and there exists someWitt vector W =
(wo, ..., c~n-1 ) E Wn(K)
such that Qa =Besides, by bilinearity
of the Artin-Schreier-Wittsymbol,
onegets:
[a, T)
= +~f T) T)
+ Qa.~>0 ~>0
First,
sincelao,ol
lie in thenfao,ol
for if A is alift for in the way we defined the Schmid-Witt
symbol,
then A isin
Wn(W(JFq))
so that all itsghost components A(’)
are constant, thusRes( B A~2~ )
=A~2~
for eachi,
hence(A, T)
= A and soT)
=~ao,o }.
Thereby, T), T)
=T).
Next,
the Witt vector a>o =clearly belongs
to(pK, ...,
and then it is in(we
shall come back to thisproperty
in section 6 with
proposition
6.1 since it isactually
a moregeneral
state-ment when the residue field of K is
simply perfect).
Thus[a>o, T)
= 0.On the other
hand,
if A is a lift for a>o withregards
to the Schmid- Wittsymbol,
then allghost components
of A havestrictly positive
val-uation,
hence = 0 for each i and so(a>o, T)
= 0. Therefore~(a>o, T ), T ) _ (a>o, T ) again.
Then, according
to lemma 3.2 thatfollows,
each for v > 0 is such that = 0. We write ao forBesides,
when
computing
the Schmid-Wittsymbol (ao, T)
one can lift ao to someWitt vector A of the
type
withAo,-v E W(Fq)
so that allA~2~
are linear combinations of
strictly negative
powers of T and as suchsatisfy
= 0 thus
(ao, T)
= 0 and[(ao, T), T)
=[(ao, T).
Therefore, by bilinearity
of both the Artin-Schreier-Wittsymbol
and theSchmid-Witt
symbol
weget:
~(a~T)~T) - ~(~a~~’)~T) -
Since Qa = Ycv for some w E
Wn (K),
one may iterate the process and constructsuccessively
Witt vectorsf!ia
=with 1Ji
EWn (K)
suchthat:
0, [(a, T), T) - [a, T)
=L(~2a~ T ) ~ T ) - T).
In
particular,
for i = n weget
= = 0 and thus[(a, T), T) -
[a, T)
=0,
as was to be shown.Finally,
if b = ETm where e is a unit in K and m >0,
then T’ :=is a
uniformizing
element inK,
whence:[a, b)
=_ ( m _ 1 ) (a, T )
+~a, T’ )
= Cm -1)L(a?T)~T)
+and we conclude
by bilinearity
of the Schmid-Wittsymbol
from what pre-cedes, indeed :
~(a~ b) ~ T ) _ (m -1 ) L(a~ T ) ~ T ) + ~(a~ T’) ~ T )
_ (m -1 ) L(a~ T ) ~ T )
+f(a~ T’) ~ T’) - [(a, T’),
where bT-m is a unit in K. Now
(a, T’)
lies inWn (Fq)
thus inWn(OK)
andaccording
tocorollary
2.1 this means that thecorresponding
Artin-Schreier- Witt extension is unramified. Hence[(a, T’), bT -m)
= 0 since is aunit and so
[(a, b), T)
=[a, b)
as was to be shown. DIn the above
proof,
we made use of thefollowing
statement due toTeichmfller in
[15]:
Lemma 3.2. Let ao E K* and let a =
(ao) be a
Witt vectorof length
nsuch that ao =
aO,vT-v,
i. e, ao is the linear combinationof strictly negative
powersof
T. Then[a, T)
= 0.Generalizing
the Schmidformula,
wefinally get:
Proposition
3.4(Schmid-Witt Formula). If a
EWn(K)
andif
b EK*,
then:
[a, b)
Proo f . According
to lemma3.1,
one may take b = T and suppose that a isa constant, i.e. an element in
Wn (Fq)
whereI~q
= ~.Then, proposition
3.4amounts to the same as
saying:
[a, T)
=TrF, IF, (a),
since
(a, T)
= a when a is constant.So let a E be a root of the
equation p(a)
= a, and let be thecorresponding cyclic
extension ofdegree p~ pn
under Artin-Schreier- Witttheory.
We set K’ :=K’((T)):
it is an unramified extension of K.Thus, according
to([13], Chap. XIII, §4,
prop.13)
onegets:
Fq
whereFq
denotes the canonicalgenerator
ofGal(K’/K) -- Gal(~’/~)
defined
by
z - ~qwith q
=jrl. Therefore, writing q
=pi
and sinceFq
commutes with p, it comes:
for
Fq
iscyclic
of order 1 overFp.
DNote that Teichmuller’s lemma 3.2 is true when the residue field of K is
perfect
whereas the Schmid-Witt formula is validonly
when the residue field is finite. Itimplies
inparticular
that the Schmid-Wittsymbol
is non-degenerate
in the usual framework of local class fieldtheory.
We conclude this section with an
equivalent
construction for the Schmid- Wittsymbol corresponding
to the idea that the(n - I )th ghost
component of a Witt vector contains all the needed information. This will make itscomputation
easier:Proposition
3.5. For every a EWn(K)
and every b EK*, if
A and B areli f ts of
a and brespectively
withregards
to the Schmid- Wittsymbol,
then:(a b)
= inRes( dB
BA (n-1)
where tn : Wn(Fp)
is the truncation map.Proo f .
Theproof
is based on thefollowing
observation. If Y =(Yo, ...,
is a Witt vector in
then,
for everyinteger k
> 1 we have:lypk 0 I
+pk+l Z,
for some Witt vector Z E
Wn(Fq).
This isparticularly
due to the relationV o F = F o V = p.
So,
let X =(Xi)i
withXi
EW(Fq) denoting
the Witt vector(A, B)
andstand for
(a, b).
Recall that these are relatedby (Xi)o
= xifor all i. We are thus
going
to prove that =According
to theprevious remark,
there exist Witt vectorsZi
inWn(Fq)
such that:
Now,
since F is theidentity
map onWn(JFp), pi
=V 2
on andby linearity
of the trace weget:
Then,
once we observe thatTrjp /p (~wp~~)
=Try /y ( (w) )
for each w EJF q
and for all
integers k >
1 and that the trace commutes withV,
wefinally get:
n-1
=
V 2f (x2)o}
mod2=0
which means that =
TrFq lfpx
as was to be shown. DLikewise,
weget
a formula in characteristic p similar to that of Satz 18 in[17]
for Witt vectors oflength
n over ap-adic
field. Note that Schmid[12]
does not use this formula eventhough
it makes thecomputation
of theArtin-Schreier-Witt
symbol simpler.
4. The reduced form of a Witt vector
One way to make the
computation
of the Artin-Schreier-Wittsymbol
even easier is to prove that on the local field K every Witt vector of
length n
is
congruent
modulop(Wn(K))
to a Witt vector with suitablecomponents.
This reduction was
already
mentionedby
Schmid in[12]:
Proposition
4.1. Let a =(ao,
Witt vector inWn(K).
Thena is