The Infinitesimal CommutatorWhy derivations of PROP-models form a Lie algebra1. PROP-models and automorphisms2. Derivations as tangent vectors3. Addition comes from first-order multiplication4. The infinitesimal square5. The two kernels6. The area layer is the tangent space again7. The commutator lands in the area layer
The Infinitesimal Commutator
Why derivations of PROP-models form a Lie algebra
The aim of this note is to prove the following fact in a way that avoids the usual calculation.
Let
Equivalently,
is a Lie subalgebra of
For associative algebras this is familiar. One checks directly that if
More precisely, derivations are tangent vectors to an automorphism group functor. Addition of derivations comes from first-order multiplication of infinitesimal automorphisms. The bracket of derivations comes from the group commutator of two infinitesimal automorphisms placed in two independent infinitesimal directions.
The proof is then almost formal.
1. PROP-models and automorphisms
Let
A model of
for every operation
in
Equivalently,
where
For every commutative
The structure maps extend
Define the automorphism functor of the PROP-model
Thus an element
is an
such that, for every operation
Therefore
is a group-valued functor.
No representability is assumed. The argument only uses the functor of points.
2. Derivations as tangent vectors
Consider the dual numbers
There is a quotient map
Applying
Define the tangent space at the identity by
An element of this kernel is an infinitesimal automorphism reducing to the identity modulo
Since
such an automorphism is necessarily of the form
for some
Its inverse is
because
Now impose the condition that
over
Expand
Since
where
For
Taking the coefficient of
This is the general Leibniz rule for a PROP-model.
So a derivation of
Equivalently,
Derivations are tangent vectors to the automorphism functor.
3. Addition comes from first-order multiplication
Before proving closure under commutators, one should first see why derivations are closed under addition.
Let
Then
are elements of
Since
But
Since
Therefore
Scalar closure is just as formal. For
sends
to
Hence
So
is a
At first order, group multiplication becomes addition.
4. The infinitesimal square
To see the bracket, one needs two independent infinitesimal directions.
Let
As a
The relations are
but
Thus
Now define
Equivalently,
There are quotient maps
The first quotient kills the area term
and the second quotient kills the two first-order directions
Geometrically, the arrows reverse:
The picture is:
The bracket lives in the difference between the square and its two axes.
5. The two kernels
Apply
We get group homomorphisms
Define
and
So
There is a natural homomorphism
The key point is that
Indeed, in
Thus every element of
with
The product is
because all products of first-order terms vanish in
Therefore
In particular,
Hence the homomorphism
factors through the abelianization of
Therefore every group commutator in
Equivalently,
But
This is the area layer.
6. The area layer is the tangent space again
The kernel
consists of automorphisms which become the identity after killing
Therefore every element of this kernel has the form
for some
Because
its inverse is
The condition that
preserves the PROP-structure is precisely the first-order condition saying that
Thus
Since
we may also write
This is the tangent space labelled by the area element.
7. The commutator lands in the area layer
Take
and put
inside
Their group commutator
also lies in
Now reduce modulo
the group
Thus
But this kernel is the area-labelled tangent space
Hence
Easy to see that
Since
This proves that derivations of a PROP-model are closed under commutators.
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