nLab Fox derivative

Context

Algebra

Group Theory

Contents

Definitions

The original definition of Fox derivatives was on integer group rings of free groups:

This kind of definition naturally generalizes to any augmented algebra:

On free group rings

Let FF be a free group with basis X={x i} i∈IX = \{ x_i\}_{i\in I} and ℤF\mathbb{Z}F the integer group ring of FF.

Differentiation or derivation, DD, in this context is defined using a sort of nonsymmetric analogue of the Leibniz rule: it is an additive map D:ℤF→ℤFD:\mathbb{Z}F\to\mathbb{Z}F such that for all u,v∈Fu,v\in F,

D(uv)=D(u)+uD(v). D(u v) = D(u) + u D(v) \mathrlap{\,.}

The Fox partial derivatives ∂∂x i\frac{\partial}{\partial x_i} are defined by the rules

∂1∂x i=0 \frac{\partial 1}{\partial x_i} = 0
∂x i∂x i=1 \frac{\partial x_i}{\partial x_i} = 1

extended to the products u=y 1…y nu = y_1\ldots y_n where y i=x ky_i = x_k or y i=x k −1y_i=x_k^{-1} for some k=k(i)k = k(i) by the formula

∂u∂x i=∑ s=1 ny 1⋯y s−1∂y s∂x i. \frac{\partial u }{\partial x_i} \;=\; \sum_{s=1}^n y_1\cdots y_{s-1} \frac{\partial y_s }{\partial x_i} \mathrlap{\,.}

This then implies that

∂x i −1∂x i=−x i −1 \frac{\partial x_i^{-1}}{\partial x_i} = -x_i^{-1}
∂x j ±1∂x i=0,i≠j. \frac{\partial x_j^{\pm 1}}{\partial x_i} = 0,\;\;i\neq j \mathrlap{\,.}

Notice that the summands on the right-hand side are “of different length”.

The lemma given in derivation on a group allows the following alternative form of the above definition to be given:

Definition

For each x∈Xx \in X, let

∂∂x:F→ℤF\frac{\partial}{\partial x} : F \to \mathbb{Z}F

be defined by

  1. for y∈Xy \in X,

    ∂y∂x=1ifx=yand=0y≠x;.\frac{\partial y}{\partial x} = 1\,\,\, if\,\,\, x = y\,\,\, and \,\,\,= 0 \,\,\, y \neq x; .
  2. for any words, w 1,w 2∈Fw_1,w_2 \in F,

    ∂∂x(w 1w 2)=∂∂xw 1+w 1∂∂xw 2.\frac{\partial}{\partial x}(w_1w_2) = \frac{\partial}{\partial x}w_1 + w_1\frac{\partial}{\partial x}w_2.

Then these uniquely determine the Fox derivative of FF with respect to xx.

The Fox derivatives give a way of expanding any derivation (differentiation) defined on FF. For every differentiation

D(u)=∑ i∈I∂u∂x iD(x i). D(u) \;=\; \sum_{i\in I} \frac{\partial u }{\partial x_i} D(x_i) \mathrlap{\,.}

(This is a finite sum since uu will only involve finitely many of the generators.)

In particular if ϵ:ℤF→ℤ\epsilon:\mathbb{Z}F\to\mathbb{Z} is the augmentation map given by ϵ:x i↦1\epsilon:x_i\mapsto 1, then the differentiation u↦u−ϵ(u)1 Fu\mapsto u-\epsilon(u) 1_F satisfies

u−ϵ(u)1 F=∑ i∂u∂x i(x i−1), u - \epsilon(u) 1_F \;=\; \sum_i \frac{\partial u }{\partial x_i} (x_i -1) \mathrlap{\,,}

hence it belongs to the left ideal in ℤF\mathbb{Z}F which is generated by (x i−1)(x_i-1).

This construction is important in combinatorial group theory, particularly in the study of free products of groups and the study of metabelian groups.

Given any group GG with a presentation ⟨X;R⟩=F/N\langle X; R\rangle = F/N such that F=⟨X⟩F=\langle X\rangle is the free group on the set of letters XX and NN the normal closure of the set of relations RR, let G¯:=G/[G,G]\bar{G}:=G/[G,G], let ϕ:F→G\phi:F\to G, ϕ¯:F→G¯\bar\phi:F\to \bar{G} be the canonical projections; denote by the same letter their linearizations for group rings ϕ:ℤF→ℤG\phi:\mathbb{Z}F\to \mathbb{Z}G and ϕ¯:ℤF→ℤG¯\bar\phi:\mathbb{Z}F\to\mathbb{Z}\bar{G}. The Jacobi matrix of the presentation is the matrix

J=(ϕ(∂r i∂x j)) J \;=\; \big( \phi(\frac{\partial r_i}{\partial x_j}) \big)

and also the projected matrix J¯\bar{J} which is the image of JJ as a matrix over ℤG¯\mathbb{Z}\bar{G}. The determinant ideal D iD_i of order ii of the matrix J¯\bar{J} is the ideal of ℤG¯\mathbb{Z}\bar{G} generated by all minors (= determinants of submatrices) of size i×ii\times i in J¯\bar{J}. The sequence D 1,D 2,…D_1,D_2,\ldots is invariant (up to some technical details), that is does not depend on the presentation. In the case when G=π(S)G=\pi(S) where SS is the complement of a knot, G¯\bar{G} is an infinite cyclic group. Let tt be its generator; then the highest nonzero determinant ideal (of J¯\bar{J}) in ℤG¯\mathbb{Z}\bar{G} is a principal ideal, hence it has a normalized (in the sense that the heighest coefficient is 11) generator, which is a polynomial in tt. This polynomial is an invariant of the knot, the Alexander polynomial of the knot.

On augmented algebras

More generally, for RR a ground ring, an RR-linear map ∂:A→A\partial : A \to A on an augmented KK-algebra, A→augRA\xrightarrow{aug} R, is a left Fox derivative if for all a,b∈Aa, b \in A, we have

∂(ab)=∂(a)aug(b)+a∂(b) \partial(a b) \;=\; \partial(a) aug(b) + a\partial(b)

and a right Fox defivative if

∂(ab)=∂(a)b+aug(a)∂(b). \partial(a b) \;=\; \partial(a)b + aug(a)\partial(b) \,.

(cf. Massuyeau & Turaev 2013 §2.1)

References

The original articles include:

with textbook treatments in

and more recently

  • Valentino Zocca, Fox calculus, symplectic forms and moduli spaces, Trans. Amer. Math. Soc. 350, 4, (1998) 1429–1466, pdf

  • en.wikipedia:Fox derivative

Relation to double Poisson structures/brackets:

See also:

For a pro-ll-version of Fox calculus see

  • Pro-ll Fox free differential calculus, section 8.3 of Masanori Morishita, Knots and primes: an introduction to arithmetic topology, Springer 2012

Last revised on August 23, 2025 at 17:36:02. See the history of this page for a list of all contributions to it.