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Separable polynomial

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In mathematics, two slightly different notions of a separable polynomial are used (by different authors) for a polynomial P(X) is over a given field K; they coincide in case P(X) is irreducible over K, which is the case is used to define the notion of a separable extension of K. According to the first definition, P(X) is separable if all of its irreducible factors in K[X] have distinct roots in the splitting field of P(X), or equivalently in an algebraic closure of K.[1] The second definition requires P(X) itself to have distinct roots in such an extension of K.[2] This is a stronger condition (precisely) because it also forbids any irreducible factor to appear multiple times, in other word it requires P(X) to also be a square-free polynomial. If P(X) is separable according to the first definition, any multiple roots of P(X) are separated by the factorization of P(X) over K, in the sense that they can be attributed to different factors. On the other hand P(X) is separable according to the second definition if and only if it is coprime to its formal derivative P′(X).

Irreducible polynomials over perfect fields are separable, which includes in particular all fields of characteristic 0, and all finite fields. This criterion is of technical importance in Galois theory.

The criterion above leads to the quick conclusion that if P is irreducible and not separable, then K is non-perfect and

P′(X) = 0.

This is only possible as a characteristic p phenomenon: we must have

P(X) = Q(Xp)

for some polynomial Q over K, where the prime number p is the characteristic.

With this clue we can construct an example:

P(X) = XpT

with K the field of rational functions in the indeterminate T over the finite field with p elements. Here one can prove directly that P(X) is irreducible, and not separable. This is actually a typical example of why inseparability matters; in geometric terms P represents the mapping on the projective line over the finite field, taking co-ordinates to their pth power. Such mappings are fundamental to the algebraic geometry of finite fields. Put another way, there are coverings in that setting that cannot be 'seen' by Galois theory. (See radical morphism for a higher-level discussion.)

If L is the field extension

K(T1/p),

in other words the splitting field of P, then L/K is an example of a purely inseparable field extension. It is of degree p, but has no automorphism fixing K, other than the identity, because T1/p is the unique root of P. This shows directly that Galois theory must here break down. A field such that there are no such extensions is called perfect. That finite fields are perfect follows a posteriori from their known structure.

One can show that the tensor product of fields of L with itself over K for this example has nilpotent elements that are non-zero. This is another manifestation of inseparability: that is, the tensor product operation on fields need not produce a ring that is a product of fields (so, not a commutative semisimple ring).

If P(x) is separable, and its roots form a group (a subgroup of the field K), then P(x) is an additive polynomial.

See also

References

  1. ^ N. Jacobson, Basic Algebra I, p. 233
  2. ^ S. Lang, Algebra, p. 178
  • Pages 240-241 of Lang, Serge (1993), Algebra (Third ed.), Reading, Mass.: Addison-Wesley, ISBN 978-0-201-55540-0, Zbl 0848.13001