Multiplier Algebra of a Cβ-algebra #
Define the multiplier algebra of a Cβ-algebra as the algebra (over π
) of double centralizers,
for which we provide the localized notation π(π, A)
. A double centralizer is a pair of
continuous linear maps L R : A βL[π] A
satisfying the intertwining condition R x * y = x * L y
.
There is a natural embedding A β π(π, A)
which sends a : A
to the continuous linear maps
L R : A βL[π] A
given by left and right multiplication by a
, and we provide this map as a
coercion.
The multiplier algebra corresponds to a non-commutative StoneβΔech compactification in the sense
that when the algebra A
is commutative, it can be identified with Cβ(X, β)
for some locally
compact Hausdorff space X
, and in that case π(π, A)
can be identified with C(Ξ² X, β)
.
Implementation notes #
We make the hypotheses on π
as weak as possible so that, in particular, this construction works
for both π = β
and π = β
.
The reader familiar with Cβ-algebra theory may recognize that one
only needs L
and R
to be functions instead of continuous linear maps, at least when A
is a
Cβ-algebra. Our intention is simply to eventually provide a constructor for this situation.
We pull back the NormedAlgebra
structure (and everything contained therein) through the
ring (even algebra) homomorphism
DoubleCentralizer.toProdMulOppositeHom : π(π, A) β+* (A βL[π] A) Γ (A βL[π] A)α΅α΅α΅
which
sends a : π(π, A)
to (a.fst, MulOpposite.op a.snd)
. The star structure is provided
separately.
References #
TODO #
- Define a type synonym for
π(π, A)
which is equipped with the strict uniform space structure and show it is complete - Show that the image of
A
inπ(π, A)
is an essential ideal - Prove the universal property of
π(π, A)
- Construct a double centralizer from a pair of maps (not necessarily linear or continuous)
L : A β A
,R : A β A
satisfying the centrality conditionβ x y, R x * y = x * L y
. - Show that if
A
is unital, thenA βββ[π] π(π, A)
.
The type of double centralizers, also known as the multiplier algebra and denoted by
π(π, A)
, of a non-unital normed algebra.
If x : π(π, A)
, then x.fst
and x.snd
are what is usually referred to as $L$ and $R$.
The centrality condition that the maps linear maps intertwine one another.
Instances For
The type of double centralizers, also known as the multiplier algebra and denoted by
π(π, A)
, of a non-unital normed algebra.
If x : π(π, A)
, then x.fst
and x.snd
are what is usually referred to as $L$ and $R$.
Equations
- One or more equations did not get rendered due to their size.
Instances For
Algebraic structure #
Because the multiplier algebra is defined as the algebra of double centralizers, there is a natural
injection DoubleCentralizer.toProdMulOpposite : π(π, A) β (A βL[π] A) Γ (A βL[π] A)α΅α΅α΅
defined by fun a β¦ (a.fst, MulOpposite.op a.snd)
. We use this map to pull back the ring, module
and algebra structure from (A βL[π] A) Γ (A βL[π] A)α΅α΅α΅
to π(π, A)
.
Equations
- DoubleCentralizer.instAdd = { add := fun (a b : DoubleCentralizer π A) => { toProd := a.toProd + b.toProd, central := β― } }
Equations
- DoubleCentralizer.instZero = { zero := { toProd := 0, central := β― } }
Equations
- DoubleCentralizer.instNeg = { neg := fun (a : DoubleCentralizer π A) => { toProd := -a.toProd, central := β― } }
Equations
- DoubleCentralizer.instSub = { sub := fun (a b : DoubleCentralizer π A) => { toProd := a.toProd - b.toProd, central := β― } }
Equations
- DoubleCentralizer.instSMul = { smul := fun (s : S) (a : DoubleCentralizer π A) => { toProd := s β’ a.toProd, central := β― } }
Equations
- DoubleCentralizer.instOne = { one := { toProd := 1, central := β― } }
Equations
- DoubleCentralizer.instMul = { mul := fun (a b : DoubleCentralizer π A) => { toProd := (a.toProd.1.comp b.toProd.1, b.toProd.2.comp a.toProd.2), central := β― } }
Equations
- DoubleCentralizer.instPow = { pow := fun (a : DoubleCentralizer π A) (n : β) => { toProd := a.toProd ^ n, central := β― } }
Equations
- DoubleCentralizer.instInhabited = { default := 0 }
Alias of DoubleCentralizer.natCast_toProd
.
Alias of DoubleCentralizer.intCast_toProd
.
Alias of DoubleCentralizer.natCast_fst
.
Alias of DoubleCentralizer.natCast_snd
.
Alias of DoubleCentralizer.intCast_fst
.
Alias of DoubleCentralizer.intCast_snd
.
The natural injection from DoubleCentralizer.toProd
except the second coordinate inherits
MulOpposite.op
. The ring structure on π(π, A)
is the pullback under this map.
Equations
- a.toProdMulOpposite = (a.toProd.1, MulOpposite.op a.toProd.2)
Instances For
The ring structure is inherited as the pullback under the injective map
DoubleCentralizer.toProdMulOpposite : π(π, A) β (A βL[π] A) Γ (A βL[π] A)α΅α΅α΅
Equations
- DoubleCentralizer.instRing = Function.Injective.ring DoubleCentralizer.toProdMulOpposite β― β― β― β― β― β― β― β― β― β― β― β―
The canonical map DoubleCentralizer.toProd
as an additive group homomorphism.
Equations
- DoubleCentralizer.toProdHom = { toFun := DoubleCentralizer.toProd, map_zero' := β―, map_add' := β― }
Instances For
The canonical map DoubleCentralizer.toProdMulOpposite
as a ring homomorphism.
Equations
- DoubleCentralizer.toProdMulOppositeHom = { toFun := DoubleCentralizer.toProdMulOpposite, map_one' := β―, map_mul' := β―, map_zero' := β―, map_add' := β― }
Instances For
The module structure is inherited as the pullback under the additive group monomorphism
DoubleCentralizer.toProd : π(π, A) β+ (A βL[π] A) Γ (A βL[π] A)
Equations
- DoubleCentralizer.instModule = Function.Injective.module S DoubleCentralizer.toProdHom β― β―
Equations
- One or more equations did not get rendered due to their size.
Star structure #
The star operation on a : π(π, A)
is given by
(star a).toProd = (star β a.snd β star, star β a.fst β star)
.
Equations
- One or more equations did not get rendered due to their size.
Equations
- DoubleCentralizer.instStarAddMonoid = StarAddMonoid.mk β―
Equations
- DoubleCentralizer.instStarRing = StarRing.mk β―
Coercion from an algebra into its multiplier algebra #
The natural coercion of A
into π(π, A)
given by sending a : A
to the pair of linear
maps Lβ Rβ : A βL[π] A
given by left- and right-multiplication by a
, respectively.
Warning: if A = π
, then this is a coercion which is not definitionally equal to the
algebraMap π π(π, π)
coercion, but these are propositionally equal. See
DoubleCentralizer.coe_eq_algebraMap
below.
Equations
- βπ a = { toProd := ((ContinuousLinearMap.mul π A) a, (ContinuousLinearMap.mul π A).flip a), central := β― }
Instances For
The natural coercion of A
into π(π, A)
given by sending a : A
to the pair of linear
maps Lβ Rβ : A βL[π] A
given by left- and right-multiplication by a
, respectively.
Warning: if A = π
, then this is a coercion which is not definitionally equal to the
algebraMap π π(π, π)
coercion, but these are propositionally equal. See
DoubleCentralizer.coe_eq_algebraMap
below.
Equations
- DoubleCentralizer.instCoeTC = { coe := βπ }
The coercion of an algebra into its multiplier algebra as a non-unital star algebra homomorphism.
Equations
- DoubleCentralizer.coeHom = { toFun := fun (a : A) => βπ a, map_smul' := β―, map_zero' := β―, map_add' := β―, map_mul' := β―, map_star' := β― }
Instances For
Norm structures #
We define the norm structure on π(π, A)
as the pullback under
DoubleCentralizer.toProdMulOppositeHom : π(π, A) β+* (A βL[π] A) Γ (A βL[π] A)α΅α΅α΅
, which
provides a definitional isometric embedding. Consequently, completeness of π(π, A)
is obtained
by proving that the range of this map is closed.
In addition, we prove that π(π, A)
is a normed algebra, and, when A
is a Cβ-algebra, we show
that π(π, A)
is also a Cβ-algebra. Moreover, in this case, for a : π(π, A)
,
βaβ = βa.fstβ = βa.sndβ
.
The normed group structure is inherited as the pullback under the ring monomorphism
DoubleCentralizer.toProdMulOppositeHom : π(π, A) β+* (A βL[π] A) Γ (A βL[π] A)α΅α΅α΅
.
Equations
- DoubleCentralizer.instNormedRing = NormedRing.induced (DoubleCentralizer π A) ((A βL[π] A) Γ (A βL[π] A)α΅α΅α΅) DoubleCentralizer.toProdMulOppositeHom β―
Equations
- DoubleCentralizer.instNormedSpace = NormedSpace.mk β―
Equations
- DoubleCentralizer.instNormedAlgebra = NormedAlgebra.mk β―
Alias of DoubleCentralizer.isUniformEmbedding_toProdMulOpposite
.
For a : π(π, A)
, the norms of a.fst
and a.snd
coincide, and hence these
also coincide with βaβ
which is max (βa.fstβ) (βa.sndβ)
.
Equations
- DoubleCentralizer.instCStarAlgebraComplex = CStarAlgebra.mk