Primitive Elements: The Lie Algebra Hidden Inside a Hopf Algebra
A Hopf algebra carries both multiplication and comultiplication:
It is precisely the interaction between these two structures that allows both groups and Lie algebras to arise naturally inside a Hopf algebra.
We are already familiar with the group-like elements:
They form a group under multiplication.
In parallel, an element is called primitive if
We write
At first sight, this merely looks like a way of selecting a special class of elements from a Hopf algebra. In fact, the primitive elements automatically form a Lie algebra, and this construction defines a functor
More importantly, it is the right adjoint of the universal enveloping algebra functor:
In characteristic zero, this adjunction has a particularly strong property:
Thus, if we first pass from a Lie algebra to its universal enveloping algebra and then extract the primitive elements, no new primitive directions appear.
The goal of this article is to explain this functor and prove this statement.
Some Immediate Properties of Primitive Elements
Let . Starting from
apply . We obtain
and hence
Using the antipode identity
we similarly obtain
so that
Thus a primitive element satisfies
This should be compared with a group-like element:
The group-like condition is multiplicative, while the primitive condition is linear.
Primitive Elements Form a Lie Algebra
Every associative algebra becomes a Lie algebra under the commutator bracket
Now let . Since is an algebra homomorphism,
Substituting
we get
After expanding, the mixed terms cancel, leaving
Therefore
Hence is a Lie subalgebra of the commutator Lie algebra :
Notice that no cocommutativity assumption on is needed.
Primitive Elements Define a Functor
Let
be a morphism of Hopf algebras.
If , then
Therefore
Since is also an algebra homomorphism,
Thus restriction gives a Lie algebra homomorphism
Hence we obtain a functor
The Universal Enveloping Algebra Is Its Left Adjoint
Let be a Lie algebra. Its universal enveloping algebra carries a canonical Hopf algebra structure determined on by
and
Therefore the canonical map
actually lands in the primitive elements:
More importantly, there is a natural bijection
Thus
Let us see why.
Suppose we are given a Lie algebra homomorphism
Forgetting the coalgebra structure for the moment, the universal property of gives a unique algebra homomorphism
Since is primitive,
Hence for every ,
Both sides are algebra homomorphisms from to , and they agree on the generators . Therefore they agree everywhere.
The counit and antipode are handled similarly.
Thus is automatically a Hopf algebra morphism.
Equivalently:
The primitive condition is exactly the extra condition needed for a Lie algebra map to extend to a Hopf algebra map .
Representability and the Monoidal Origin of Group-Like and Primitive Elements
The group-like and primitive-element constructions admit another categorical interpretation. Both are representable, and both interact strongly with tensor products.
These two facts describe different aspects of the construction:
representability tells us that a group-like or primitive element can be regarded as a morphism from a universal probe;
strong monoidality explains how the multiplication of a Hopf algebra induces algebraic structure on the collection of such elements.
It is useful to examine these two ideas separately.
Group-Like Elements Are Representable
For a Hopf algebra , let
The elements of form a group under the multiplication of .
Consider the infinite cyclic group . For every group , choosing a group homomorphism
is equivalent to choosing the image of , hence to choosing an arbitrary element of . Therefore
Now use the adjunction
We obtain
Thus the underlying-set-valued group-like functor is represented by
In other words,
If denotes the canonical generator of , then
A Hopf algebra morphism
is completely determined by , and the Hopf compatibility forces to be group-like.
Thus is the universal Hopf algebra containing one group-like element.
Primitive Elements Are Representable
Now consider
Let be the one-dimensional abelian Lie algebra.
For every Lie algebra , a Lie algebra morphism
is completely determined by the image of , and this image may be any element of . Hence
Using the adjunction
we obtain
Since is one-dimensional and abelian,
with
Therefore
A Hopf algebra morphism
is determined by , and Hopf compatibility says precisely that
Thus is the universal Hopf algebra containing one primitive element.
We therefore obtain the parallel picture
The representing objects themselves reflect the two defining equations:
and
The first is multiplicative, while the second is its infinitesimal, additive analogue.
A General Principle Behind the Two Representations
Both calculations are instances of the same elementary categorical fact.
Suppose
is an adjunction, and suppose a Set-valued functor on is represented by an object :
Then
Thus representability is transported across the adjunction.
For group-like elements, the generic element of a group is represented by
and the left adjoint sends it to
For primitive elements, the generic element of a Lie algebra is represented by the one-dimensional abelian Lie algebra
and the left adjoint sends it to
Hence the representing Hopf algebras are not accidental. They are the images of the generic one-generator objects under the corresponding left adjoints.
Strong Monoidality and the Group-Like Multiplication
Representability tells us what an individual group-like element is. To understand why group-like elements form a group, it is useful to move one categorical level down and regard a Hopf algebra as a monoid object in coalgebras equipped with an antipode.
Let
be the group-like-element functor.
It is strong symmetric monoidal:
Under this isomorphism,
Indeed, if and are group-like, then
Now a bialgebra is precisely a monoid object in the monoidal category of coalgebras. Its multiplication and unit are coalgebra morphisms
A strong monoidal functor sends monoid objects to monoid objects. Therefore sends the multiplication of to
Explicitly,
Thus the multiplication on group-like elements is not an additional construction. It is the Hopf multiplication transported through the strong monoidal functor .
The strong monoidal argument first gives a monoid. When is a Hopf algebra, the antipode satisfies
for every group-like element , so this monoid is in fact a group.
Primitive Elements and the Additive Group
There is a completely parallel construction for primitive elements, but with an important change in the target monoidal structure.
For a coaugmented coalgebra , let
Then
is strong symmetric monoidal:
The comparison map is
Now take a Hopf algebra . Its multiplication
is a morphism of coaugmented coalgebras. Applying gives
Using strong monoidality, this becomes
What operation is this?
Starting with ,
and then applying multiplication gives
Therefore the multiplication transported through is
The unit becomes
and the antipode acts on primitive elements by
Thus the group structure produced on primitive elements is precisely their additive group structure:
If we further compose with the underlying-set functor
then
is again strong symmetric monoidal, and it sends a Hopf algebra to the ordinary additive group underlying its primitive vector space.
The Two Strong Monoidal Functors
We can now place the two constructions side by side:
with
and
with
For the same Hopf multiplication
the first functor produces
while the second produces
Thus
This is the categorical form of the passage from a group to its infinitesimal linearization.
There is, however, one further piece of structure on .
The additive group law on is explained entirely by the strong monoidality of . The Lie bracket
is additional information. It comes from the noncommutativity of the multiplication of , together with the fact that primitive elements are closed under commutators.
Hence the two structures on have conceptually different origins:
This distinction mirrors ordinary Lie theory. The differential of group multiplication at the identity is
and is simply
The Lie bracket is not this first derivative; it records a higher-order failure of commutativity.
In the Hopf-algebraic picture, group-like elements retain the multiplicative structure itself, while primitive elements retain its infinitesimal additive structure, with the commutator supplying the additional Lie bracket.