In mathematical branch of functional analysis is the maximum tensor product of C * -algebras a construction * -algebras with which one of two C and a new one gets designated C * algebra. It is a matter of completing the algebraic tensor product of and with a suitable norm . The construction presented below goes back to A. Guichardet .
A.
{\ displaystyle A}
B.
{\ displaystyle B}
A.
⊗
m
a
x
B.
{\ displaystyle A \ otimes _ {\ mathrm {max}} B}
A.
{\ displaystyle A}
B.
{\ displaystyle B}
construction
Let and two C * -algebras. A C * half-form on the algebraic tensor product is a half-norm such that
A.
{\ displaystyle A}
B.
{\ displaystyle B}
A.
⊙
B.
{\ displaystyle A \ odot B}
α
{\ displaystyle \ alpha}
α
(
s
t
)
≤
α
(
s
)
α
(
t
)
{\ displaystyle \ alpha (st) \ leq \ alpha (s) \ alpha (t)}
for all
s
,
t
∈
A.
⊙
B.
{\ displaystyle s, t \ in A \ odot B}
α
(
s
∗
s
)
=
α
(
s
)
2
{\ displaystyle \ alpha (s ^ {*} s) \, = \, \ alpha (s) ^ {2}}
for all
s
∈
A.
⊙
B.
{\ displaystyle s \ in A \ odot B}
One can show that for everyone and . For an element it therefore follows for every C * half-norm. Therefore , where it goes through all the C * half-norms is finite, and it is easy to confirm that a C * half-norm is and by construction the largest on . It is even a norm, because the C * half-norms include the spatial C * norm .
α
(
a
⊗
b
)
≤
‖
a
‖
‖
b
‖
{\ displaystyle \ alpha (a \ otimes b) \ leq \ | a \ | \ | b \ |}
a
∈
A.
{\ displaystyle a \ in A}
b
∈
B.
{\ displaystyle b \ in B}
s
=
∑
i
=
1
n
a
i
⊗
b
i
∈
A.
⊙
B.
{\ displaystyle s = \ sum _ {i = 1} ^ {n} a_ {i} \ otimes b_ {i} \ in A \ odot B}
α
(
s
)
≤
∑
i
=
1
n
‖
a
i
‖
‖
b
i
‖
{\ displaystyle \ alpha (s) \ leq \ sum _ {i = 1} ^ {n} \ | a_ {i} \ | \ | b_ {i} \ |}
μ
(
s
)
: =
sup
α
α
(
s
)
{\ displaystyle \ mu (s): = \ sup _ {\ alpha} \ alpha (s)}
α
{\ displaystyle \ alpha}
μ
{\ displaystyle \ mu}
A.
⊙
B.
{\ displaystyle A \ odot B}
The completion of with respect to this maximum C * -norm is called the maximum tensor product from and and is denoted by, other authors write for it .
A.
⊙
B.
{\ displaystyle A \ odot B}
A.
{\ displaystyle A}
B.
{\ displaystyle B}
A.
⊗
μ
B.
{\ displaystyle A \ otimes _ {\ mu} B}
A.
⊗
m
a
x
B.
{\ displaystyle A \ otimes _ {\ mathrm {max}} B}
properties
The maximum tensor product has the following useful property:
Let , and C * -algebras and as well as two * - homomorphisms with interchanging images, that is, for all and . Then there is exactly one * homomorphism with for all and .
A.
{\ displaystyle A}
B.
{\ displaystyle B}
C.
{\ displaystyle C}
φ
:
A.
→
C.
{\ displaystyle \ varphi: A \ rightarrow C}
ψ
:
B.
→
C.
{\ displaystyle \ psi: B \ rightarrow C}
φ
(
a
)
ψ
(
b
)
=
ψ
(
b
)
φ
(
a
)
{\ displaystyle \ varphi (a) \ psi (b) = \ psi (b) \ varphi (a)}
a
∈
A.
{\ displaystyle a \ in A}
b
∈
B.
{\ displaystyle b \ in B}
π
:
A.
⊗
m
a
x
B.
→
C.
{\ displaystyle \ pi: A \ otimes _ {\ mathrm {max}} B \ rightarrow C}
π
(
a
⊗
b
)
=
φ
(
a
)
ψ
(
b
)
{\ displaystyle \ pi (a \ otimes b) = \ varphi (a) \ psi (b)}
a
∈
A.
{\ displaystyle a \ in A}
b
∈
B.
{\ displaystyle b \ in B}
If and are C * -algebras, then a pair is called an exchanging pair of representations of , if and Hilbert space representations are on the same Hilbert space and for all and holds. With this concept formation the following formula can be set up for the maximum C * norm:
A.
{\ displaystyle A}
B.
{\ displaystyle B}
(
φ
,
ψ
)
{\ displaystyle (\ varphi, \ psi)}
(
A.
,
B.
)
{\ displaystyle (A, B)}
φ
:
A.
→
L.
(
H
)
{\ displaystyle \ varphi: A \ rightarrow L (H)}
ψ
:
B.
→
L.
(
H
)
{\ displaystyle \ psi: B \ rightarrow L (H)}
H
{\ displaystyle H}
φ
(
a
)
ψ
(
b
)
=
ψ
(
b
)
φ
(
a
)
{\ displaystyle \ varphi (a) \ psi (b) = \ psi (b) \ varphi (a)}
a
∈
A.
{\ displaystyle a \ in A}
b
∈
B.
{\ displaystyle b \ in B}
For two C * -algebras and and from the algebraic tensor product holds
A.
{\ displaystyle A}
B.
{\ displaystyle B}
s
=
∑
j
=
1
n
a
j
⊗
b
j
{\ displaystyle s = \ sum _ {j = 1} ^ {n} a_ {j} \ otimes b_ {j}}
A.
⊙
B.
{\ displaystyle A \ odot B}
μ
(
s
)
=
sup
{
‖
∑
j
=
1
n
φ
(
a
j
)
ψ
(
b
j
)
‖
;
(
φ
,
ψ
)
interchanging pair of representations of
(
A.
,
B.
)
}
.
{\ displaystyle \ mu (s) = \ sup \ {\ | \ sum _ {j = 1} ^ {n} \ varphi (a_ {j}) \ psi (b_ {j}) \ |; \, (\ varphi, \ psi) {\ mbox {interchanging pair of representations of}} (A, B) \}.}
See also
Individual evidence
^ A. Guichardet: Tensor products of C * -algebras , Aarhus University Lecture Notes, Volume 12 (1969)
^ RV Kadison , JR Ringrose : Fundamentals of the Theory of Operator Algebras II , 1983, ISBN 0-1239-3302-1 , §11.3
↑ Gerald. J. Murphy: C * -Algebras and Operator Theory , Academic Press Inc. (1990), ISBN 0-1251-1360-9 , chapter 6
↑ Gerald. J. Murphy: C * -Algebras and Operator Theory , Academic Press Inc. (1990), ISBN 0-1251-1360-9 , Theorem 6.3.7
^ RV Kadison, JR Ringrose: Fundamentals of the Theory of Operator Algebras II , 1983, ISBN 0-1239-3302-1 , Theorem 11.3.4
literature
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