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Multiplicative InvariantTheory
Workshop “Noncommutative Invariant Theory”U Washington, Seattle 05/27/2012
Jessie HammTemple University, Philadelphia
Special Thanks to Dr. Martin Lorenz
OverviewPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 2
■ Introductionto multiplicative invariants: definitions, examples, . . .
OverviewPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 2
■ Introductionto multiplicative invariants: definitions, examples, . . .
■ Regularity: reflection groups and semigroup algebras
OverviewPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 2
■ Introductionto multiplicative invariants: definitions, examples, . . .
■ Regularity: reflection groups and semigroup algebras
■ TheCohen-Macaulay property: reminders on CM rings, some resultson multiplicative invariants, and some problems
Part I: Introduction
Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative invariantsPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 4
■ Given: a groupG and aG-latticeL ∼= Z
n; so
G → GL(L) ∼= GLn(Z)
anintegral representationof G
k
k k k
k k
k k
Multiplicative invariantsPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 4
■ Given: a groupG and aG-latticeL ∼= Z
n; so
G → GL(L) ∼= GLn(Z)
■ Choose a base ringk and form thegroup algebra
k[L] =⊕
m∈L
kxm ∼= k[x±1
1 , . . . , x±1n ] , x
mxm′
= xm+m′
TheG-action onL extends uniquely to a“multiplicative” or“exponential”action on thek-algebrak[L]: g(xm) = x
g(m)
k k
Multiplicative invariantsPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 4
■ Given: a groupG and aG-latticeL ∼= Z
n; so
G → GL(L) ∼= GLn(Z)
■ Choose a base ringk and form thegroup algebra
k[L] =⊕
m∈L
kxm ∼= k[x±1
1 , . . . , x±1n ] , x
mxm′
= xm+m′
TheG-action onL extends uniquely to a“multiplicative” or“exponential”action on thek-algebrak[L]: g(xm) = x
g(m)
■Problem: k[L]G = {f ∈ k[L] | g(f) = f ∀g ∈ G} = ?
Example #1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 5
Multiplicative inversion in rank 2:(k = Z)
G = 〈g | g2 = 1〉L = Ze1 ⊕ Ze2action:g(ei) = −ei
Example #1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 5
Multiplicative inversion in rank 2:(k = Z)
G = 〈g | g2 = 1〉L = Ze1 ⊕ Ze2action:g(ei) = −ei
Puttingxi = xei we have: Z[L] = Z[x±1
1 , x±12 ] with g(xi) = x−1
i
Example #1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 5
Multiplicative inversion in rank 2:(k = Z)
G = 〈g | g2 = 1〉L = Ze1 ⊕ Ze2action:g(ei) = −ei
Puttingxi = xei we have: Z[L] = Z[x±1
1 , x±12 ] with g(xi) = x−1
i
Straightforward calculation
Z[L]G = Z[ξ1, ξ2]⊕ ηZ[ξ1, ξ2]
ξi = xi + x−1i
η = x1x2 + x−11 x−1
2
ηξ1ξ2 = η2 + ξ21 + ξ22 − 4
Example #1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 5
Multiplicative inversion in rank 2:(k = Z)
G = 〈g | g2 = 1〉L = Ze1 ⊕ Ze2action:g(ei) = −ei
Hence: Z[L]G ∼= Z[x, y, z]/(x2 + y2 + z2 − xyz − 4)
Example #1′: linear analogPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 6
Linear inversion in rank 2: G = 〈g | g2 = 1〉L = Ze1 ⊕ Ze2action:g(ei) = −ei
Example #1′: linear analogPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 6
Linear inversion in rank 2: G = 〈g | g2 = 1〉L = Ze1 ⊕ Ze2action:g(ei) = −ei
Now: S(L) = Z[x1, x2] with g(xi) = −xi
Example #1′: linear analogPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 6
Linear inversion in rank 2: G = 〈g | g2 = 1〉L = Ze1 ⊕ Ze2action:g(ei) = −ei
Now: S(L) = Z[x1, x2] with g(xi) = −xi
One obtains:
S(L)G = Z[ξ1, ξ2]⊕ ηZ[ξ1, ξ2]
ξi = x2i
η = x1x2
η2 = ξ1ξ2
Example #1′: linear analogPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 6
Linear inversion in rank 2: G = 〈g | g2 = 1〉L = Ze1 ⊕ Ze2action:g(ei) = −ei
Hence: Z[L]G ∼= Z[x, y, z]/(z2 − xy)
Some Special FeaturesPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 7
Back to general multiplicative actions:
L aG-lattice
k a commutative base ring
k[L] the group algebra
Some Special FeaturesPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 7
Multiplicative invariants have a Z-structure:
ak-basis ofk[L]G is given by the distinct orbit sums
orb(m) :=∑
m′∈G(m)
xm′
(m ∈ L)
⇓
k[L]G = k⊗
Z
Z[L]G
Some Special FeaturesPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 7
It suffices to considerfinite groups:
eachorb(m) is supported onLfin = {m ∈ L | [G : Gm] < ∞}
stabilizer ofm ∈ L
G acts onLfin through the finite quotientG = G/KerG(Lfin). Thus:
k[L]G = k[Lfin]G
Some Special FeaturesPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 7
In particular,k[L]G is always affine/k
(Hilbert # 14 ok).
Finite Linear GroupsPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 8
Jordan (1880):GLn(Z) has only finitely many finite subgroups up toconjugacy.
Finite Linear GroupsPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 8
Jordan (1880):GLn(Z) has only finitely many finite subgroups up toconjugacy.
there are onlyfinitely manymultiplicative invariant algebras
k[L]G (up to∼=) with rankL bounded
Finite Linear GroupsPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 8
n # fin. G ≤ GLn(Z) # max’l G(up to conj.) (up to conj.)
1 2 1
2 13 2
3 73 4
4 710 9
5 6079 17
6 85311 39
Pioneers of MITPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 9
■ Bourbaki : “Invariants exponentiels”(Chap. VI§ 3 of Groupes etalgebres de Lie, 1968)
R(g) ∼= Z[Λ]W ∼= Z[x1, . . . , xrank g]
whereR(g) = representation ring of a semisimple Lie algebrag, Λ =weight lattice ofg, andW = Weyl group.
Pioneers of MITPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 9
■ Bourbaki : “Invariants exponentiels”(Chap. VI§ 3 of Groupes etalgebres de Lie, 1968)
R(g) ∼= Z[Λ]W ∼= Z[x1, . . . , xrank g]
whereR(g) = representation ring of a semisimple Lie algebrag, Λ =weight lattice ofg, andW = Weyl group.
■ Steinberg, Richardson(1970s)
Pioneers of MITPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 9
■ Bourbaki : “Invariants exponentiels”(Chap. VI§ 3 of Groupes etalgebres de Lie, 1968)
R(g) ∼= Z[Λ]W ∼= Z[x1, . . . , xrank g]
whereR(g) = representation ring of a semisimple Lie algebrag, Λ =weight lattice ofg, andW = Weyl group.
■ Steinberg, Richardson(1970s)
■ “∆-methods” for group rings:Passman, Zalesskiı, Roseblade, DanFarkas “multiplicative invariants”
(mid 1980s)
Part II: Regularity
Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Regularity at 1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 11
Notations: G a finite groupL ∼= Z
n a faithfulG-lattice
k = k a field withchar k ∤ |G|
Will explain the following result . . .
Regularity at 1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 11
Theorem 1TFAE (1) k[L]G is regular atπ(1)(2) G acts as a reflection group onL(3)k[L]G = k[M ] is a semigroup
algebra withε(M) ⊆ k
∗
Regularity at 1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 11
Theorem 1TFAE (1) k[L]G is regular atπ(1)(2) G acts as a reflection group onL(3)k[L]G = k[M ] is a semigroup
algebra withε(M) ⊆ k
∗
Here,
X = Spec k[L]π
−→ X/G = Spec k[L]G
∈
1 = Ker ε
whereε : k[L] −→ k is the counit:ε(xm) = 1 for all m ∈ L
Regularity at 1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 11
Theorem 1TFAE (1) k[L]G is regular atπ(1)(2) G acts as a reflection group onL(3)k[L]G = k[M ] is a semigroup
algebra withε(M) ⊆ k
∗
(1)⇒ (2) useslinearization: PutE = Ker ε. Then
L
k
= L⊗ k
∼→ E/E2
m⊗ 1 7→ xm − 1 + E2
leads to S(L
k
)Gπ(0)
∼=
k[L]Gπ(1). Now use the S-T-C Theorem.
Regularity at 1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 11
Theorem 1TFAE (1) k[L]G is regular atπ(1)(2) G acts as a reflection group onL(3)k[L]G = k[M ] is a semigroup
algebra withε(M) ⊆ k
∗
(2)⇒ (3) usesroot systems: ∃ root systemΦ so that
ZΦ ⊆ L ⊆ Λ(Φ) with G = W(Φ)
UseBourbaki’s Thm: Z[Λ(Φ)]W(Φ) is a polynomial algebra.
Regularity at 1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 11
Theorem 1TFAE (1) k[L]G is regular atπ(1)(2) G acts as a reflection group onL(3)k[L]G = k[M ] is a semigroup
algebra withε(M) ⊆ k
∗
(3)⇒ (1) usestorus actions:
(3) ⇔X/G = Spec k[L]G is an affine toric variety so thatπ(1)belongs to the open torus orbit
This implies (1).
Example #1 RevisitedPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 12
Recall:multiplicative inversion(rank2)
G = 〈g | g2 = 1〉L = Ze1 ⊕ Ze2action:g(ei) = −ei
k[L]G ∼= k[x, y, z]/(x2 + y2 + z2 − xyz − 4)
k[L]G is not a semigroupalgebra:
Ex #2: Un and the root latticeAn−1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 13
Notation: Un =⊕n
1 Zei∼= Z
n
An−1 = {∑
i ziei ∈ Un |∑
i zi = 0} ∼= Z
n−1
Sn-action: σ(ei) = eσ(i) (σ ∈ Sn)
Ex #2: Un and the root latticeAn−1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 13
Notation: Un =⊕n
1 Zei∼= Z
n
An−1 = {∑
i ziei ∈ Un |∑
i zi = 0} ∼= Z
n−1
Sn-action: σ(ei) = eσ(i) (σ ∈ Sn)
Note: Sn acts as a reflection group;transpositions are reflections
Ex #2: Un and the root latticeAn−1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 13
Notation: Un =⊕n
1 Zei∼= Z
n
An−1 = {∑
i ziei ∈ Un |∑
i zi = 0} ∼= Z
n−1
Sn-action: σ(ei) = eσ(i) (σ ∈ Sn)
Putxi = xei ∈ k[Un]; soσ(xi) = xσ(i) for σ ∈ Sn. Then
k[Un] = k[x±11 , . . . , x±1
n ] = k[x1, . . . , xn][s−1n ] ,
wheresn =∏n
1 xi is thenth elementary symmetric polynomial.
Ex #2: Un and the root latticeAn−1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 13
Notation: Un =⊕n
1 Zei∼= Z
n
An−1 = {∑
i ziei ∈ Un |∑
i zi = 0} ∼= Z
n−1
Sn-action: σ(ei) = eσ(i) (σ ∈ Sn)
∴ k[Un]Sn = k[x1, . . . , xn][s
−1n ]Sn
= k[x1, . . . , xn]Sn [s−1
n ]
= k[s1, . . . , sn−1, s±1n ]
∼= k[Zn−1+ ⊕ Z]
elem. symmetric poly’s
Ex #2: Un and the root latticeAn−1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 13
Notation: Un =⊕n
1 Zei∼= Z
n
An−1 = {∑
i ziei ∈ Un |∑
i zi = 0} ∼= Z
n−1
Sn-action: σ(ei) = eσ(i) (σ ∈ Sn)
Now,
k[An−1] = k[Un]0 ,
the degree0-component for the (Sn-stable) “total degree” grading of
k[Un] = k[x±11 , . . . , x±1
n ].
Ex #2: Un and the root latticeAn−1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 13
Notation: Un =⊕n
1 Zei∼= Z
n
An−1 = {∑
i ziei ∈ Un |∑
i zi = 0} ∼= Z
n−1
Sn-action: σ(ei) = eσ(i) (σ ∈ Sn)
Get
k[An−1]Sn ∼= k[M ]
withM =
{
(t1, . . . , tn−1) ∈ Z
n−1+ |
∑
iti ∈ nZ
}
Ex #2: Un and the root latticeAn−1Part I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 13
Notation: Un =⊕n
1 Zei∼= Z
n
An−1 = {∑
i ziei ∈ Un |∑
i zi = 0} ∼= Z
n−1
Sn-action: σ(ei) = eσ(i) (σ ∈ Sn)
C[An−1]Sn is not regular:
(n > 2; picture forn = 3)
RegularityPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 14
Here is the global version of Theorem 1(same notations and hypotheses)
RegularityPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 14
Theorem 1′ TFAE (1) k[L]G is regular(2)G acts as a reflection group onL
andH1(G/D, LD) = 0(3) k[L]G ∼= k[Zr
+ ⊕ Z
s](4)∃ root systemΦ s.t.L/LG ∼= Λ(Φ)
andG = W(Φ)
Here,D is the subgroup ofG that is generated by the “diagonalizable”reflections, conjugate inGL(L) to
d =
(
−11
...1
)
RegularityPart I: Introduction Part II: Regularity Part III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 14
n
# finiteG ≤ GLn(Z)(up to conjugacy)
# reflection groupsG(up to conjugacy)
# cases withk[L]G regular
2 13 9 7
3 73 29 18
4 710 102 51
Part III: The Cohen-MacaulayProperty
Part I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Reminder: CM RingsPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 16
■ Hypotheses: R a comm. noetherian ringa an ideal ofR
Reminder: CM RingsPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 16
■ Hypotheses: R a comm. noetherian ringa an ideal ofR
■ Always:
height a ≥ depth a = inf{i | H ia(R) 6= 0}
Reminder: CM RingsPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 16
■ Hypotheses: R a comm. noetherian ringa an ideal ofR
■ Always:
height a ≥ depth a = inf{i | H ia(R) 6= 0}
(Zariski) topologydimension theory
(homological) algebra
Reminder: CM RingsPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 16
■ Hypotheses: R a comm. noetherian ringa an ideal ofR
■ Always:
height a ≥ depth a = inf{i | H ia(R) 6= 0}
(Zariski) topologydimension theory
(homological) algebra
■ Def: R is Cohen-Macaulayiff equality holds forall (maximal) idealsa
Some Examples of CM RingsPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 17
■ Standard example:R an affine domain/PIDk, finite / somepolynomial subalgebraP = k[x1, . . . , xn]. Then:
R CM ⇔ R is freeoverP
Some Examples of CM RingsPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 17
■ Standard example:R an affine domain/PIDk, finite / somepolynomial subalgebraP = k[x1, . . . , xn]. Then:
R CM ⇔ R is freeoverP
■ Hierarchy: catenary
regular +3 complete⋂ +3 Gorenstein +3 CM
KS
dim 0
6>✉✉✉✉✉✉✉✉✉
✉✉✉✉✉✉✉✉✉ dim 1reduced
KS
dim 2normal
^f❋❋❋❋❋❋❋❋
❋❋❋❋❋❋❋❋
Invariant RingsPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 18
Hypotheses: R a CM ringG a finite group acting onR
Invariant RingsPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 18
Hypotheses: R a CM ringG a finite group acting onR
If the trace mapR → RG , r 7→∑
Gg(r), is epi (“non-modular case”)
thenRG is CM; otherwiseusually not.
Invariant RingsPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 18
Hypotheses: R a CM ringG a finite group acting onR
If the trace mapR → RG , r 7→∑
Gg(r), is epi (“non-modular case”)
thenRG is CM; otherwiseusually not.
Here is anecessary condition. . .
Invariant RingsPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 18
Hypotheses: R a CM ringG a finite group acting onRRk = { k-reflectionsonR }AssumeR noetherian/RG
automorphisms belonging tothe inertia group of someprime of height≤ k
Proposition(L. - Pathak)
RG CM & H i(G, R) = 0 (0 < i < k)
⇒ res : Hk(G, R) →∏
H⊆Rk+1
Hk(H, R)
Invariant RingsPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 18
Hypotheses: R a CM ringG a finite group acting onRRk = {k-reflectionsonR }AssumeR noetherian/RG
Proposition(L. - Pathak)
RG CM & H i(G, R) = 0 (0 < i < k)
⇒ res : Hk(G, R) →∏
H⊆Rk+1
Hk(H, R)
Note: The (H i = 0)-condn
is vacuous fork = 1 bireflections.
Mult. Invariants: CM-propertyPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 19
Notations: G is a finite group6= 1L aG-lattice, WLOG faithful
Mult. Invariants: CM-propertyPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 19
Notations: G is a finite group6= 1L aG-lattice, WLOG faithful
SoG → GL(L), g 7→ gL. In this setting,
g ∈ G is ak-reflectiononk[L]
⇐⇒ rank(gL − IdL) ≤ k
”g is ak-reflection onL” — or onL⊗
Z
Q
Mult. Invariants: CM-propertyPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 19
Notations: G is a finite group6= 1L aG-lattice, WLOG faithful
Theorem 2(L, TAMS ’06)
If Z[L]G is CM then allGm/R2(Gm) for m ∈ L are
perfect groups, but notall Gm are.
subgroup gen. bybireflections onL
Mult. Invariants: CM-propertyPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 19
Notations: G is a finite group6= 1L aG-lattice, WLOG faithful
Theorem 2(L, TAMS ’06)
If Z[L]G is CM then allGm/R2(Gm) for m ∈ L are
perfect groups, but notall Gm are.
Corollary (“3-copies conjecture”) Z[L⊕r]G is never CMfor r ≥ 3.
Mult. Invariants: CM-propertyPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 19
Notations: G is a finite group6= 1L aG-lattice, WLOG faithful
Theorem 2(L, TAMS ’06)
If Z[L]G is CM then allGm/R2(Gm) for m ∈ L are
perfect groups, but notall Gm are.
Note that the conclusions of Theorem 2 only refer to therationaltype
of L. In fact . . .
Mult. Invariants: CM-propertyPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 19
Notations: G is a finite group6= 1L aG-lattice, WLOG faithful
Theorem 2(L, TAMS ’06)
If Z[L]G is CM then allGm/R2(Gm) for m ∈ L are
perfect groups, but notall Gm are.
Proposition If k[L]G is CM then so isk[L′]G for any G-latticeL′ so thatL′ ⊗ Q
∼= L⊗ Q.
Example: Sn-latticesPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 20
What are theSn-latticesL such thatZ[L]Sn is CM ?
Example: Sn-latticesPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 20
We know:
■ only the structure ofL
Q
= L⊗
Z
Q matters (Proposition)
■ Sn must act as a bireflection group onL (Theorem 2), and hence onall simple constituents ofL
Q
Example: Sn-latticesPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 20
Classification results of irreducible finite linear groups containing abireflection (Huffman and Wales, 70s) imply,for n ≥ 7:
L
Q
∼= Q
r ⊕ (Q−)s⊕ (An−1)
t
Q
(s+ t ≤ 2)
sign representation ofSn
Example: Sn-latticesPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 20
In all cases,Z[L]Sn is indeed CM, with the possibleexception of
L = A2n−1
This case reduces to
Problem(open forp ≤ n/2)
Are the “vector invariants”
Fp[x1, . . . , xn, y1, . . . , yn]Sn CM?
SummaryPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 21
LetL be aG-lattice, whereG is a finite group.
G is generated byreflectionsonL
Bourbaki, Farkas
L.
*2
Z[L]G is asemigroup algebra
?
jr
Hochster
��
G is generated bybireflectionsonL
Z[L]G isCohen-Macaulay+3
?
ks
ThanksPart I: Introduction Part II: RegularityPart III: The Cohen-Macaulay Property
Multiplicative Invariant Theory Seattle 05/27/2012 – slide 22
Thanks for your attention!