Locally nilpotent derivation explained

\partial

of a commutative ring

A

is called a locally nilpotent derivation (LND) if every element of

A

is annihilated by some power of

\partial

.

One motivation for the study of locally nilpotent derivations comes from the fact that some of the counterexamples to Hilbert's 14th problem are obtained as the kernels of a derivation on a polynomial ring.[1]

Over a field

k

of characteristic zero, to give a locally nilpotent derivation on the integral domain

A

, finitely generated over the field, is equivalent to giving an action of the additive group

(k,+)

to the affine variety

X=\operatorname{Spec}(A)

. Roughly speaking, an affine variety admitting "plenty" of actions of the additive group is considered similar to an affine space.[2]

Definition

Let

A

be a ring. Recall that a derivation of

A

is a map

\partial\colonA\toA

satisfying the Leibniz rule

\partial(ab)=(\partiala)b+a(\partialb)

for any

a,b\inA

. If

A

is an algebra over a field

k

, we additionally require

\partial

to be

k

-linear, so

k\subseteq\ker\partial

.

A derivation

\partial

is called a locally nilpotent derivation (LND) if for every

a\inA

, there exists a positive integer

n

such that

\partialn(a)=0

.

If

A

is graded, we say that a locally nilpotent derivation

\partial

is homogeneous (of degree

d

) if

\deg\partiala=\dega+d

for every

a\inA

.

The set of locally nilpotent derivations of a ring

A

is denoted by

\operatorname{LND}(A)

. Note that this set has no obvious structure: it is neither closed under addition (e.g. if

\partial1=y\tfrac{\partial}{\partialx}

,

\partial2=x\tfrac{\partial}{\partialy}

then

\partial1,\partial2\in\operatorname{LND}(k[x,y])

but

(\partial1+\partial2)2(x)=x

, so

\partial1+\partial2\not\in\operatorname{LND}(k[x,y])

) nor under multiplication by elements of

A

(e.g.

\tfrac{\partial}{\partialx}\in\operatorname{LND}(k[x])

, but

x\tfrac{\partial}{\partialx}\not\in\operatorname{LND}(k[x])

). However, if

[\partial1,\partial2]=0

then

\partial1,\partial2\in\operatorname{LND}(A)

implies

\partial1+\partial2\in\operatorname{LND}(A)

and if

\partial\in\operatorname{LND}(A)

,

h\in\ker\partial

then

h\partial\in\operatorname{LND}(A)

.

Relation to -actions

Let

A

be an algebra over a field

k

of characteristic zero (e.g.

k=C

). Then there is a one-to-one correspondence between the locally nilpotent

k

-derivations on

A

and the actions of the additive group

Ga

of

k

on the affine variety

\operatorname{Spec}A

, as follows.[3] A

Ga

-action on

\operatorname{Spec}A

corresponds to a

k

-algebra homomorphism

\rho\colonA\toA[t]

. Any such

\rho

determines a locally nilpotent derivation

\partial

of

A

by taking its derivative at zero, namely

\partial=\epsilon\circ\tfrac{d}{dt}\circ\rho,

where

\epsilon

denotes the evaluation at

t=0

. Conversely, any locally nilpotent derivation

\partial

determines a homomorphism

\rho\colonA\toA[t]

by

\rho=\exp

infty
(t\partial)=\sum
n=0
tn
n!

\partialn.

It is easy to see that the conjugate actions correspond to conjugate derivations, i.e. if

\alpha\in\operatorname{Aut}A

and

\partial\in\operatorname{LND}(A)

then

\alpha\circ\partial\circ\alpha-1\in\operatorname{LND}(A)

and

\exp(t\alpha\circ\partial\circ\alpha-1)=\alpha\circ\exp(t\partial)\circ\alpha-1

The kernel algorithm

The algebra

\ker\partial

consists of the invariants of the corresponding

Ga

-action. It is algebraically and factorially closed in

A

. A special case of Hilbert's 14th problem asks whether

\ker\partial

is finitely generated, or, if

A=k[X]

, whether the quotient

X//Ga

is affine. By Zariski's finiteness theorem,[4] it is true if

\dimX\leq3

. On the other hand, this question is highly nontrivial even for

X=Cn

,

n\geq4

. For

n\geq5

the answer, in general, is negative.[5] The case

n=4

is open.

However, in practice it often happens that

\ker\partial

is known to be finitely generated: notably, by the Maurer - Weitzenböck theorem,[6] it is the case for linear LND's of the polynomial algebra over a field of characteristic zero (by linear we mean homogeneous of degree zero with respect to the standard grading).

Assume

\ker\partial

is finitely generated. If

A=k[g1,...,gn]

is a finitely generated algebra over a field of characteristic zero, then

\ker\partial

can be computed using van den Essen's algorithm,[7] as follows. Choose a local slice, i.e. an element

r\in\ker\partial2\setminus\ker\partial

and put

f=\partialr\in\ker\partial

. Let

\pir\colonA\to(\ker\partial)f

be the Dixmier map given by

\pir

infty
(a)=\sum
n=0
(-1)n
n!

\partialn(a)

rn
fn
. Now for every

i=1,...,n

, chose a minimal integer

mi

such that

hi\colon=

mi
f

\pir(gi)\in\ker\partial

, put

B0=k[h1,...,hn,f]\subseteq\ker\partial

, and define inductively

Bi

to be the subring of

A

generated by

\{h\inA:fh\inBi-1\}

. By induction, one proves that

B0\subsetB1\subset...\subset\ker\partial

are finitely generated and if

Bi=Bi+1

then

Bi=\ker\partial

, so

BN=\ker\partial

for some

N

. Finding the generators of each

Bi

and checking whether

Bi=Bi+1

is a standard computation using Gröbner bases.

Slice theorem

Assume that

\partial\in\operatorname{LND}(A)

admits a slice, i.e.

s\inA

such that

\partials=1

. The slice theorem asserts that

A

is a polynomial algebra

(\ker\partial)[s]

and

\partial=\tfrac{d}{ds}

.

For any local slice

r\in\ker\partial\setminus\ker\partial2

we can apply the slice theorem to the localization

A\partial

, and thus obtain that

A

is locally a polynomial algebra with a standard derivation. In geometric terms, if a geometric quotient

\pi\colonX\toX//Ga

is affine (e.g. when

\dimX\leq3

by the Zariski theorem), then it has a Zariski-open subset

U

such that

\pi-1(U)

is isomorphic over

U

to

U x A1

, where

Ga

acts by translation on the second factor.

However, in general it is not true that

X\toX//Ga

is locally trivial. For example,[8] let

\partial=u\tfrac{\partial}{\partialx}+v\tfrac{\partial}{\partialy}+(1+uy2)\tfrac{\partial}{\partialz}\in\operatorname{LND}(C[x,y,z,u,v])

. Then

\ker\partial

is a coordinate ring of a singular variety, and the fibers of the quotient map over singular points are two-dimensional.

If

\dimX=3

then

\Gamma=X\setminusU

is a curve. To describe the

Ga

-action, it is important to understand the geometry

\Gamma

. Assume further that

k=C

and that

X

is smooth and contractible (in which case

S

is smooth and contractible as well[9]) and choose

\Gamma

to be minimal (with respect to inclusion). Then Kaliman proved that each irreducible component of

\Gamma

is a polynomial curve, i.e. its normalization is isomorphic to

C1

. The curve

\Gamma

for the action given by Freudenburg's (2,5)-derivation (see below) is a union of two lines in

C2

, so

\Gamma

may not be irreducible. However, it is conjectured that

\Gamma

is always contractible.[10]

Examples

Example 1

The standard coordinate derivations

\tfrac{\partial}{\partialxi}

of a polynomial algebra

k[x1,...,xn]

are locally nilpotent. The corresponding

Ga

-actions are translations:

txi=xi+t

,

txj=xj

for

ji

.

Example 2 (Freudenburg's (2,5)-homogeneous derivation[11])

Let

f1=x1x3-x

2
2
,

f2=x3f

2x
2f
5
1+x
, and let

\partial

be the Jacobian derivation \partial(f_)=\det \left[\tfrac{\partial f_{i}}{\partial x_{j}}\right]_. Then

\partial\in\operatorname{LND}(k[x1,x2,x3])

and

\operatorname{rank}\partial=3

(see below); that is,

\partial

annihilates no variable. The fixed point set of the corresponding

Ga

-action equals

\{x1=x2=0\}

.

Example 3

Consider

Sl2(k)=\{ad-bc=1\}\subseteqk4

. The locally nilpotent derivation

a\tfrac{\partial}{\partialb}+c\tfrac{\partial}{\partiald}

of its coordinate ring corresponds to a natural action of

Ga

on

Sl2(k)

via right multiplication of upper triangular matrices. This action gives a nontrivial

Ga

-bundle over

A2\setminus\{(0,0)\}

. However, if

k=C

then this bundle is trivial in the smooth category[12]

LND's of the polynomial algebra

Let

k

be a field of characteristic zero (using Kambayashi's theorem one can reduce most results to the case

k=C

[13]) and let

A=k[x1,...,xn]

be a polynomial algebra.

Triangular derivations

Let

f1,...,fn

be any system of variables of

A

; that is,

A=k[f1,...,fn]

. A derivation of

A

is called triangular with respect to this system of variables, if

\partialf1\ink

and

\partialfi\ink[f1,...,fi-1]

for

i=2,...,n

. A derivation is called triangulable if it is conjugate to a triangular one, or, equivalently, if it is triangular with respect to some system of variables. Every triangular derivation is locally nilpotent. The converse is true for

\leq2

by Rentschler's theorem above, but it is not true for

n\geq3

.
Bass's exampleThe derivation of

k[x1,x2,x3]

given by

x1\tfrac{\partial}{\partialx2}+2x2x1\tfrac{\partial}{\partialx3}

is not triangulable.[14] Indeed, the fixed-point set of the corresponding

Ga

-action is a quadric cone

x2x3=x

2
2
, while by the result of Popov,[15] a fixed point set of a triangulable

Ga

-action is isomorphic to

Z x A1

for some affine variety

Z

; and thus cannot have an isolated singularity.

Makar-Limanov invariant

The intersection of the kernels of all locally nilpotent derivations of the coordinate ring, or, equivalently, the ring of invariants of all

Ga

-actions, is called "Makar-Limanov invariant" and is an important algebraic invariant of an affine variety. For example, it is trivial for an affine space; but for the Koras–Russell cubic threefold, which is diffeomorphic to

C3

, it is not.[16]

Further reading

Notes and References

  1. Web site: Daigle . Daniel . Hilbert's Fourteenth Problem and Locally Nilpotent Derivations . . 11 September 2018.
  2. Arzhantsev. I.. Flenner. H.. Kaliman. S.. Kutzschebauch. F.. Zaidenberg. M.. Flexible varieties and automorphism groups. Duke Math. J.. 2013. 162. 4. 767–823. 10.1215/00127094-2080132. 1011.5375. 53412676 .
  3. Book: Freudenburg. G.. Algebraic theory of locally nilpotent derivations. 2006. Springer-Verlag. Berlin. 978-3-540-29521-1. 10.1.1.470.10.
  4. Zariski. O.. Interprétations algébrico-géométriques du quatorzième problème de Hilbert. Bull. Sci. Math. (2). 1954. 78. 155–168.
  5. Derksen. H. G. J.. The kernel of a derivation. J. Pure Appl. Algebra. 1993. 84. 1. 13–16. 10.1016/0022-4049(93)90159-Q. free.
  6. Seshadri. C.S.. On a theorem of Weitzenböck in invariant theory. J. Math. Kyoto Univ.. 1962. 1. 3. 403–409. 10.1215/kjm/1250525012. free.
  7. Book: van den Essen. A.. Polynomial automorphisms and the Jacobian conjecture. 2000. Birkhäuser Verlag. Basel. 978-3-7643-6350-5. 10.1007/978-3-0348-8440-2. 252433637 .
  8. Deveney. J.. Finston. D.. A proper

    Ga

    -action on

    C5

    which is not locally trivial. Proc. Amer. Math. Soc.. 1995. 123. 3. 651–655. 10.1090/S0002-9939-1995-1273487-0 . free. 2160782.
  9. Kaliman. S. Saveliev. N..

    C+

    -Actions on contractible threefolds
    . Michigan Math. J.. 2004. 52. 3. 619–625. 10.1307/mmj/1100623416. math/0209306. 15020160.
  10. Book: Kaliman. S.. Actions of

    C*

    and

    C+

    on affine algebraic varieties. 2009. Algebraic geometry-Seattle 2005. Part 2. 80. 629–654. 10.1090/pspum/080.2/2483949. http://www.math.miami.edu/~kaliman/library/seattle.paper.pdf. Proceedings of Symposia in Pure Mathematics. 9780821847039.
  11. Freudenburg. G.. Actions of

    Ga

    on

    A3

    defined by homogeneous derivations. Journal of Pure and Applied Algebra. 1998. 126. 1. 169–181. 10.1016/S0022-4049(96)00143-0. free.
  12. Dubouloz. A.. Finston. D.. On exotic affine 3-spheres. J. Algebraic Geom.. 2014. 23. 3. 445–469. 10.1090/S1056-3911-2014-00612-3. 1106.2900. 119651964 .
  13. Daigle. D.. Kaliman. S.. A note on locally nilpotent derivations and variables of

    k[X,Y,Z

    ]. Canad. Math. Bull.. 2009. 52. 4. 535–543. 10.4153/CMB-2009-054-5. free.
  14. Bass. H.. A non-triangular action of

    Ga

    on

    A3

    . Journal of Pure and Applied Algebra. 1984. 33. 1. 1–5. 10.1016/0022-4049(84)90019-7. free.
  15. Book: Popov. V. L.. Algebraic Groups Utrecht 1986 . On actions of

    Ga

    on

    An

    . 1271. 237–242. 10.1007/BFb0079241. Lecture Notes in Mathematics. 1987. 978-3-540-18234-4.
  16. Kaliman. S.. Makar-Limanov. L.. On the Russell-Koras contractible threefolds. J. Algebraic Geom.. 1997. 6. 2. 247–268.