In mathematical group theory, a quantum group is a specific type of Hopf algebras , namely quantizations (i.e. non-trivial deformations) of the enveloping Hopf algebras of semi-simple Lie algebras . Alternatively, one can consider quantum groups as deformations from the algebra of regular functions on algebraic groups .
The term was coined by the Ukrainian-US mathematician Vladimir Drinfeld at the International Congress of Mathematicians in 1986 in Berkeley . Independently of him, they were found around the same time by the Japanese mathematician Michio Jimbō .
example
The simplest quantum group is . This is the algebra of the variables , , and is produced and in which the relations
U
q
(
s
l
(
2
)
)
{\ displaystyle U_ {q} ({\ mathfrak {sl}} (2))}
K
{\ displaystyle K}
K
-
1
{\ displaystyle K ^ {- 1}}
E.
{\ displaystyle E}
F.
{\ displaystyle F}
K
K
-
1
=
K
-
1
K
=
1
{\ displaystyle KK ^ {- 1} = K ^ {- 1} K = 1}
,
K
E.
K
-
1
=
q
2
E.
{\ displaystyle KEK ^ {- 1} = q ^ {2} E}
,
K
F.
K
-
1
=
q
-
2
F.
{\ displaystyle KFK ^ {- 1} = q ^ {- 2} F}
,
[
E.
,
F.
]
=
K
-
K
-
1
q
-
q
-
1
{\ displaystyle [E, F] = {\ frac {KK ^ {- 1}} {qq ^ {- 1}}}}
be valid.
The Hopf algebra structure is given by
Δ
(
E.
)
=
1
⊗
E.
+
E.
⊗
K
{\ displaystyle \ Delta (E) = 1 \ otimes E + E \ otimes K}
,
Δ
(
F.
)
=
K
-
1
⊗
F.
+
F.
⊗
1
{\ displaystyle \ Delta (F) = K ^ {- 1} \ otimes F + F \ otimes 1}
,
Δ
(
K
)
=
K
⊗
K
{\ displaystyle \ Delta (K) = K \ otimes K}
,
Δ
(
K
-
1
)
=
K
-
1
⊗
K
-
1
{\ displaystyle \ Delta (K ^ {- 1}) = K ^ {- 1} \ otimes K ^ {- 1}}
,
ϵ
(
E.
)
=
ϵ
(
F.
)
=
0
{\ displaystyle \ epsilon (E) = \ epsilon (F) = 0}
,
ϵ
(
K
)
=
ϵ
(
K
-
1
)
=
1
{\ displaystyle \ epsilon (K) = \ epsilon (K ^ {- 1}) = 1}
,
S.
(
E.
)
=
-
E.
K
-
1
{\ displaystyle S (E) = - EK ^ {- 1}}
,
S.
(
F.
)
=
-
K
F.
{\ displaystyle S (F) = - KF}
,
S.
(
K
)
=
K
-
1
{\ displaystyle S (K) = K ^ {- 1}}
,
S.
(
K
-
1
)
=
K
{\ displaystyle S (K ^ {- 1}) = K}
.
E.
{\ displaystyle E}
and are therefore skew-primitive, and and are group-like.
F.
{\ displaystyle F}
K
{\ displaystyle K}
K
-
1
{\ displaystyle K ^ {- 1}}
Universal enveloping algebra
U
(
s
l
(
2
)
)
{\ displaystyle U ({\ mathfrak {sl}} (2))}
U
1
(
s
l
(
2
)
)
{\ displaystyle U_ {1} ({\ mathfrak {sl}} (2))}
is not defined in this form, as one would have to divide by 0. However, it is possible to use another variable to formulate the definition in such a way that this is possible.
L.
{\ displaystyle L}
K
K
-
1
=
K
-
1
K
=
1
{\ displaystyle KK ^ {- 1} = K ^ {- 1} K = 1}
,
K
E.
K
-
1
=
q
2
E.
{\ displaystyle KEK ^ {- 1} = q ^ {2} E}
,
K
F.
K
-
1
=
q
-
2
F.
{\ displaystyle KFK ^ {- 1} = q ^ {- 2} F}
,
[
E.
,
F.
]
=
L.
{\ displaystyle [E, F] = L}
(
q
-
q
-
1
)
L.
=
K
-
K
-
1
{\ displaystyle (qq ^ {- 1}) L = KK ^ {- 1}}
[
L.
,
E.
]
=
q
(
E.
K
+
K
-
1
E.
)
{\ displaystyle [L, E] = q (EK + K ^ {- 1} E)}
[
L.
,
F.
]
=
-
q
-
1
(
F.
K
+
K
-
1
F.
)
{\ displaystyle [L, F] = - q ^ {- 1} (FK + K ^ {- 1} F)}
In this form is well-defined and is closely related to universal enveloping algebra . It is true
U
1
(
s
l
(
2
)
)
{\ displaystyle U_ {1} ({\ mathfrak {sl}} (2))}
U
(
s
l
(
2
)
)
{\ displaystyle U ({\ mathfrak {sl}} (2))}
U
1
(
s
l
(
2
)
)
/
(
K
-
1
)
≅
U
(
s
l
(
2
)
)
{\ displaystyle U_ {1} ({\ mathfrak {sl}} (2)) / (K-1) \ cong U ({\ mathfrak {sl}} (2))}
,
where up , up and up is shown.
E.
{\ displaystyle E}
X
{\ displaystyle X}
F.
{\ displaystyle F}
Y
{\ displaystyle Y}
L.
{\ displaystyle L}
H
{\ displaystyle H}
literature
Christian Kassel: Quantum Groups (Graduate Texts in Mathematics). Springer-Verlag 1998, ISBN 0-387-94370-6 (English)
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