Normal basis

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In mathematics, specifically the algebraic theory of fields, a normal basis is a special kind of basis for Galois extensions of finite degree, characterised as forming a single orbit for the Galois group. The normal basis theorem states that any finite Galois extension of fields has a normal basis. In algebraic number theory, the study of the more refined question of the existence of a normal integral basis is part of Galois module theory.

Normal basis theorem

Let FK be a Galois extension with Galois group G. The classical normal basis theorem states that there is an element βK such that {g(β) for gG} forms a basis of K, considered as a vector space over F. That is, any element αK can be written uniquely as α=gGagg(β) for coefficients agF.

A normal basis contrasts with a primitive element basis of the form {1,β,β2,,βn1}, where βK is an element whose minimal polynomial has degree n=[K:F].

Case of finite fields

For finite fields this can be stated as follows:[1] Let F=GF(q)=𝔽q denote the field of q elements, where q = pm is a prime power, and let K=GF(qn)=𝔽qn denote its extension field of degree n ≥ 1. Here the Galois group is G=Gal(K/F)={1,Φ,Φ2,,Φn1} with Φn=1, a cyclic group generated by the relative Frobenius automorphism Φ(α)=αq,with Φn=1=IdK. Then there exists an element βK such that

{β,Φ(β),Φ2(β),,Φn1(β)} = {β,βq,βq2,,βqn1}

is a basis of K over F.

Proof for finite fields

In case the Galois group is cyclic as above, generated by Φ with Φn=1, the Normal Basis Theorem follows from two basic facts. The first is the linear independence of characters: a multiplicative character is a mapping χ from a group H to a field K satisfying χ(h1h2)=χ(h1)χ(h2); then any distinct characters χ1,χ2, are linearly independent in the K-vector space of mappings. We apply this to the Galois group automorphisms χi=Φi:KK, thought of as mappings from the multiplicative group H=K×. Now KFnas an F-vector space, so we may consider Φ:FnFn as an element of the matrix algebra Mn(F); since its powers 1,Φ,,Φn1 are linearly independent (over K and a fortiori over F), its minimal polynomial must have degree at least n, i.e. it must be Xn1. We conclude that the group algebra of G is F[G]F[X]/(Xn1), a quotient of the polynomial ring F[X], and the F-vector space K is a module (or representation) for this algebra.

The second basic fact is the classification of modules over a PID such as F[G]. These are just direct sums of cyclic modules of the form

F[X]/(f(x)),

where f(x) must be divisible by Xn 1. (Here G acts by

ΦXi=Xi+1.

) But since

dimFF[X]/(Xn1)=dimF(K)=n,

we can only have f(x) = Xn 1, and

K  F[X]/(Xn1)

as F[G]-modules, namely the regular representation of G. (Note this is not an isomorphism of rings or F-algebras!) Now the basis

{1,X,X2,,Xn1}

on the right side of this isomorphism corresponds to a normal basis

{β,Φ(β),Φ2(β),,Φm1(β)}

of K on the left.

Note that this proof would also apply in the case of a cyclic Kummer extension.

Example

Consider the field K=GF(23)=𝔽8 over F=GF(2)=𝔽2, with Frobenius automorphism Φ(α)=α2. The proof above clarifies the choice of normal bases in terms of the structure of K as a representation of G (or F[G]-module). The irreducible factorization

Xn1 = X31 = (X+1)(X2+X+1)  F[X]

means we have a direct sum of F[G]-modules (by the Chinese remainder theorem):

K  F[X](X31)  F[X](X+1)F[X](X2+X+1).

The first component is just FK, while the second is isomorphic as an F[G]-module to 𝔽22𝔽2[X]/(X2+X+1) under the action ΦXi=Xi+1. (Thus K𝔽2𝔽4 as F[G]-modules, but not as F-algebras.)

The elements βK which can be used for a normal basis are precisely those outside either of the submodules, so that (Φ+1)(β)0 and (Φ2+Φ+1)(β)0. In terms of the G-orbits of K, which correspond to the irreducible factors of:

t23t = t(t+1)(t3+t+1)(t3+t2+1)  F[t],

the elements of F=𝔽2 are the roots of t(t+1), the nonzero elements of the submodule 𝔽4 are the roots of t3+t+1, while the normal basis, which in this case is unique, is given by the roots of the remaining factor t3+t2+1.

By contrast, for the extension field L=GF(24)=𝔽16 in which n = 4 is divisible by p = 2, we have the F[G]-module isomorphism

L  𝔽2[X]/(X41) = 𝔽2[X]/(X+1)4.

Here the operator ΦX is not diagonalizable, the module L has nested submodules given by generalized eigenspaces of Φ, and the normal basis elements β are those outside the largest proper generalized eigenspace, the elements with (Φ+1)3(β)0.

Application to cryptography

The normal basis is frequently used in cryptographic applications based on the discrete logarithm problem, such as elliptic curve cryptography, since arithmetic using a normal basis is typically more computationally efficient than using other bases.

For example, in the field

K=GF(23)=𝔽8

above, we may represent elements as bit-strings:

α = (a2,a1,a0) = a2Φ2(β)+a1Φ(β)+a0β = a2β4+a1β2+a0β,

where the coefficients are bits

aiGF(2)={0,1}.

Now we can square elements by doing a left circular shift,

α2=Φ(a2,a1,a0)=(a1,a0,a2)

, since squaring β4 gives β8 = β. This makes the normal basis especially attractive for cryptosystems that utilize frequent squaring.

Primitive normal basis

A primitive normal basis of an extension of finite fields E/F is a normal basis for E/F that is generated by a primitive element of E, that is a generator of the multiplicative group K×. (Note that this is a more restrictive definition of primitive element than that mentioned above after the general Normal Basis Theorem: one requires powers of the element to produce every non-zero element of K, not merely a basis.) Lenstra and Schoof (1987) proved that every finite field extension possesses a primitive normal basis, the case when F is a prime field having been settled by Harold Davenport.

Free elements

If K/F is a Galois extension and x in E generates a normal basis over F, then x is free in K/F. If x has the property that for every subgroup H of the Galois group G, with fixed field KH, x is free for K/KH, then x is said to be completely free in K/F. Every Galois extension has a completely free element.[2]

See also

References

  1. Nader H. Bshouty; Gadiel Seroussi (1989), Generalizations of the normal basis theorem of finite fields, p. 1, https://hotcrp-vee2014.cs.technion.ac.il/users/wwwb/cgi-bin/tr-get.cgi/1989/CS/CS0578.pdf ; SIAM J. Discrete Math. 3 (1990), no. 3, 330–337.
  2. Dirk Hachenberger, Completely free elements, in Cohen & Niederreiter (1996) pp.97-107 Zbl 0864.11066