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Characterizing Splitting Fields Normal Extensions Size of the Galois Group Normal Field Extensions Bernd Schr oder logo1 Bernd Schr oder Louisiana Tech University, College of Engineering and Science Normal Field Extensions


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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Normal Field Extensions

Bernd Schr¨

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Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Introduction

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Introduction

  • 1. Ultimately, we want to compute Galois groups of splitting

fields.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Introduction

  • 1. Ultimately, we want to compute Galois groups of splitting

fields.

  • 2. To do so, we need some more properties of splitting fields

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Introduction

  • 1. Ultimately, we want to compute Galois groups of splitting

fields.

  • 2. To do so, we need some more properties of splitting fields,

and we are especially interested in properties that connect to Galois groups.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Introduction

  • 1. Ultimately, we want to compute Galois groups of splitting

fields.

  • 2. To do so, we need some more properties of splitting fields,

and we are especially interested in properties that connect to Galois groups.

  • 3. Demanding characteristic 0 will make some proofs a bit

easier.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Theorem.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a finite extension of F.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a finite extension of F. Then the following are equivalent.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a finite extension of F. Then the following are equivalent.

  • 1. E is the splitting field for a polynomial f of positive degree

in F[x].

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a finite extension of F. Then the following are equivalent.

  • 1. E is the splitting field for a polynomial f of positive degree

in F[x].

  • 2. Every irreducible polynomial p ∈ F[x] that has one zero in

E actually splits in E.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a finite extension of F. Then the following are equivalent.

  • 1. E is the splitting field for a polynomial f of positive degree

in F[x].

  • 2. Every irreducible polynomial p ∈ F[x] that has one zero in

E actually splits in E.

  • 3. F is the fixed field of G(E/F).

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a finite extension of F. Then the following are equivalent.

  • 1. E is the splitting field for a polynomial f of positive degree

in F[x].

  • 2. Every irreducible polynomial p ∈ F[x] that has one zero in

E actually splits in E.

  • 3. F is the fixed field of G(E/F).

Proof.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a finite extension of F. Then the following are equivalent.

  • 1. E is the splitting field for a polynomial f of positive degree

in F[x].

  • 2. Every irreducible polynomial p ∈ F[x] that has one zero in

E actually splits in E.

  • 3. F is the fixed field of G(E/F).
  • Proof. We will prove “1⇒2

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a finite extension of F. Then the following are equivalent.

  • 1. E is the splitting field for a polynomial f of positive degree

in F[x].

  • 2. Every irreducible polynomial p ∈ F[x] that has one zero in

E actually splits in E.

  • 3. F is the fixed field of G(E/F).
  • Proof. We will prove “1⇒2 ⇒3

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a finite extension of F. Then the following are equivalent.

  • 1. E is the splitting field for a polynomial f of positive degree

in F[x].

  • 2. Every irreducible polynomial p ∈ F[x] that has one zero in

E actually splits in E.

  • 3. F is the fixed field of G(E/F).
  • Proof. We will prove “1⇒2 ⇒3 ⇒1”.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“1⇒2”).

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F. Moreover, any field in which f splits must contain µ1,...,µn, so it must contain E = F(µ1,...,µn).

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F. Moreover, any field in which f splits must contain µ1,...,µn, so it must contain E = F(µ1,...,µn). Thus E = E(θ1) is the splitting field of f over F(θ1)

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F. Moreover, any field in which f splits must contain µ1,...,µn, so it must contain E = F(µ1,...,µn). Thus E = E(θ1) is the splitting field of f over F(θ1) (the splitting field must contain E and θ1)

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F. Moreover, any field in which f splits must contain µ1,...,µn, so it must contain E = F(µ1,...,µn). Thus E = E(θ1) is the splitting field of f over F(θ1) (the splitting field must contain E and θ1), and E(θ2) is the splitting field of f over F(θ2)

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F. Moreover, any field in which f splits must contain µ1,...,µn, so it must contain E = F(µ1,...,µn). Thus E = E(θ1) is the splitting field of f over F(θ1) (the splitting field must contain E and θ1), and E(θ2) is the splitting field of f over F(θ2) (the splitting field must contain E and θ2).

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F. Moreover, any field in which f splits must contain µ1,...,µn, so it must contain E = F(µ1,...,µn). Thus E = E(θ1) is the splitting field of f over F(θ1) (the splitting field must contain E and θ1), and E(θ2) is the splitting field of f over F(θ2) (the splitting field must contain E and θ2). There is an isomorphism Φ : E → E(θ2) that continues ϕ.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F. Moreover, any field in which f splits must contain µ1,...,µn, so it must contain E = F(µ1,...,µn). Thus E = E(θ1) is the splitting field of f over F(θ1) (the splitting field must contain E and θ1), and E(θ2) is the splitting field of f over F(θ2) (the splitting field must contain E and θ2). There is an isomorphism Φ : E → E(θ2) that continues ϕ. In particular, Φ fixes F.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F. Moreover, any field in which f splits must contain µ1,...,µn, so it must contain E = F(µ1,...,µn). Thus E = E(θ1) is the splitting field of f over F(θ1) (the splitting field must contain E and θ1), and E(θ2) is the splitting field of f over F(θ2) (the splitting field must contain E and θ2). There is an isomorphism Φ : E → E(θ2) that continues ϕ. In particular, Φ fixes F. But then [E : F] = [E(θ2) : F]

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F. Moreover, any field in which f splits must contain µ1,...,µn, so it must contain E = F(µ1,...,µn). Thus E = E(θ1) is the splitting field of f over F(θ1) (the splitting field must contain E and θ1), and E(θ2) is the splitting field of f over F(θ2) (the splitting field must contain E and θ2). There is an isomorphism Φ : E → E(θ2) that continues ϕ. In particular, Φ fixes F. But then [E : F] = [E(θ2) : F], which implies that E = E(θ2).

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F. Moreover, any field in which f splits must contain µ1,...,µn, so it must contain E = F(µ1,...,µn). Thus E = E(θ1) is the splitting field of f over F(θ1) (the splitting field must contain E and θ1), and E(θ2) is the splitting field of f over F(θ2) (the splitting field must contain E and θ2). There is an isomorphism Φ : E → E(θ2) that continues ϕ. In particular, Φ fixes F. But then [E : F] = [E(θ2) : F], which implies that E = E(θ2). Because θ2 was an arbitrary root of p, we conclude that all roots of p are in E

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“1⇒2”). Let E be the splitting field for a polynomial f ∈ F[x] of positive degree. Let µ1,...,µn ∈ E\F be the roots

  • f f that are not in F. Then E = F(µ1,...,µn).

Let p ∈ F[x] be an arbitrary irreducible polynomial with a root θ1 ∈ E. Let θ2 = θ1 be another arbitrary root of p. Then θ2 lies in some extension of F, but, at this stage, we do not know if it lies in E. There is an isomorphism ϕ : F(θ1) → F(θ2) so that ϕ(θ1) = θ2 and ϕ fixes F. Moreover, any field in which f splits must contain µ1,...,µn, so it must contain E = F(µ1,...,µn). Thus E = E(θ1) is the splitting field of f over F(θ1) (the splitting field must contain E and θ1), and E(θ2) is the splitting field of f over F(θ2) (the splitting field must contain E and θ2). There is an isomorphism Φ : E → E(θ2) that continues ϕ. In particular, Φ fixes F. But then [E : F] = [E(θ2) : F], which implies that E = E(θ2). Because θ2 was an arbitrary root of p, we conclude that all roots of p are in E, that is p splits in E.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“2⇒3”).

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“2⇒3”). In case E = F

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF}

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F. Every µk must be a zero of a polynomial in F[x], because otherwise

  • µj

k : j ∈ N0

  • would be an infinite F-linearly independent set in E.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F. Every µk must be a zero of a polynomial in F[x], because otherwise

  • µj

k : j ∈ N0

  • would be an infinite F-linearly independent set in E. There is a

θ ∈ E = F(µ1,...,µn) so that E = F(µ1,...,µn) = F(θ)

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F. Every µk must be a zero of a polynomial in F[x], because otherwise

  • µj

k : j ∈ N0

  • would be an infinite F-linearly independent set in E. There is a

θ ∈ E = F(µ1,...,µn) so that E = F(µ1,...,µn) = F(θ) and θ is a zero of an irreducible polynomial p ∈ F[x].

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F. Every µk must be a zero of a polynomial in F[x], because otherwise

  • µj

k : j ∈ N0

  • would be an infinite F-linearly independent set in E. There is a

θ ∈ E = F(µ1,...,µn) so that E = F(µ1,...,µn) = F(θ) and θ is a zero of an irreducible polynomial p ∈ F[x]. (We used that F has characteristic 0 here.)

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-47
SLIDE 47

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F. Every µk must be a zero of a polynomial in F[x], because otherwise

  • µj

k : j ∈ N0

  • would be an infinite F-linearly independent set in E. There is a

θ ∈ E = F(µ1,...,µn) so that E = F(µ1,...,µn) = F(θ) and θ is a zero of an irreducible polynomial p ∈ F[x]. (We used that F has characteristic 0 here.) Then

  • 1,θ,...,θ deg(p)−1

is a basis for E = F(θ) over F.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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SLIDE 48

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F. Every µk must be a zero of a polynomial in F[x], because otherwise

  • µj

k : j ∈ N0

  • would be an infinite F-linearly independent set in E. There is a

θ ∈ E = F(µ1,...,µn) so that E = F(µ1,...,µn) = F(θ) and θ is a zero of an irreducible polynomial p ∈ F[x]. (We used that F has characteristic 0 here.) Then

  • 1,θ,...,θ deg(p)−1

is a basis for E = F(θ) over F. Moreover deg(p) = [E : F] = n.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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SLIDE 49

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F. Every µk must be a zero of a polynomial in F[x], because otherwise

  • µj

k : j ∈ N0

  • would be an infinite F-linearly independent set in E. There is a

θ ∈ E = F(µ1,...,µn) so that E = F(µ1,...,µn) = F(θ) and θ is a zero of an irreducible polynomial p ∈ F[x]. (We used that F has characteristic 0 here.) Then

  • 1,θ,...,θ deg(p)−1

is a basis for E = F(θ) over F. Moreover deg(p) = [E : F] = n. By assumption, p splits in E.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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SLIDE 50

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F. Every µk must be a zero of a polynomial in F[x], because otherwise

  • µj

k : j ∈ N0

  • would be an infinite F-linearly independent set in E. There is a

θ ∈ E = F(µ1,...,µn) so that E = F(µ1,...,µn) = F(θ) and θ is a zero of an irreducible polynomial p ∈ F[x]. (We used that F has characteristic 0 here.) Then

  • 1,θ,...,θ deg(p)−1

is a basis for E = F(θ) over F. Moreover deg(p) = [E : F] = n. By assumption, p splits in E. Let θ1 := θ and let θ2,...,θn be the

  • ther zeros of p

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-51
SLIDE 51

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F. Every µk must be a zero of a polynomial in F[x], because otherwise

  • µj

k : j ∈ N0

  • would be an infinite F-linearly independent set in E. There is a

θ ∈ E = F(µ1,...,µn) so that E = F(µ1,...,µn) = F(θ) and θ is a zero of an irreducible polynomial p ∈ F[x]. (We used that F has characteristic 0 here.) Then

  • 1,θ,...,θ deg(p)−1

is a basis for E = F(θ) over F. Moreover deg(p) = [E : F] = n. By assumption, p splits in E. Let θ1 := θ and let θ2,...,θn be the

  • ther zeros of p (which must all be distinct).

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-52
SLIDE 52

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F. Every µk must be a zero of a polynomial in F[x], because otherwise

  • µj

k : j ∈ N0

  • would be an infinite F-linearly independent set in E. There is a

θ ∈ E = F(µ1,...,µn) so that E = F(µ1,...,µn) = F(θ) and θ is a zero of an irreducible polynomial p ∈ F[x]. (We used that F has characteristic 0 here.) Then

  • 1,θ,...,θ deg(p)−1

is a basis for E = F(θ) over F. Moreover deg(p) = [E : F] = n. By assumption, p splits in E. Let θ1 := θ and let θ2,...,θn be the

  • ther zeros of p (which must all be distinct).

Let j ∈ {2,...,n}.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-53
SLIDE 53

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3”). In case E = F, we have G(F/F) = {idF} and clearly E = F is the fixed field of G(F/F) = {idF}. So for the remainder of this part, we can assume that E = F. Let {µ1,...,µn} be a basis of E over F. Every µk must be a zero of a polynomial in F[x], because otherwise

  • µj

k : j ∈ N0

  • would be an infinite F-linearly independent set in E. There is a

θ ∈ E = F(µ1,...,µn) so that E = F(µ1,...,µn) = F(θ) and θ is a zero of an irreducible polynomial p ∈ F[x]. (We used that F has characteristic 0 here.) Then

  • 1,θ,...,θ deg(p)−1

is a basis for E = F(θ) over F. Moreover deg(p) = [E : F] = n. By assumption, p splits in E. Let θ1 := θ and let θ2,...,θn be the

  • ther zeros of p (which must all be distinct).

Let j ∈ {2,...,n}. There is an isomorphism ϕ : F(θ1) → F(θj) so that ϕ(θ1) = θj and ϕ fixes F.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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SLIDE 54

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.).

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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SLIDE 55

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-56
SLIDE 56

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-57
SLIDE 57

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F).

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-58
SLIDE 58

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-59
SLIDE 59

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-60
SLIDE 60

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e)

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-61
SLIDE 61

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e) = Φ

  • n−1

i=0

fiθ i

  • Bernd Schr¨
  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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SLIDE 62

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e) = Φ

  • n−1

i=0

fiθ i

  • =

n−1

i=0

fiΦ(θ)i

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-63
SLIDE 63

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e) = Φ

  • n−1

i=0

fiθ i

  • =

n−1

i=0

fiΦ(θ)i =

n−1

i=0

fiθ i

j .

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-64
SLIDE 64

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e) = Φ

  • n−1

i=0

fiθ i

  • =

n−1

i=0

fiΦ(θ)i =

n−1

i=0

fiθ i

j .

Let f(x) := −e+

n−1

i=0

fixi.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-65
SLIDE 65

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e) = Φ

  • n−1

i=0

fiθ i

  • =

n−1

i=0

fiΦ(θ)i =

n−1

i=0

fiθ i

j .

Let f(x) := −e+

n−1

i=0

  • fixi. Then f ∈ E[x] and deg(f) ≤ n−1.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-66
SLIDE 66

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e) = Φ

  • n−1

i=0

fiθ i

  • =

n−1

i=0

fiΦ(θ)i =

n−1

i=0

fiθ i

j .

Let f(x) := −e+

n−1

i=0

  • fixi. Then f ∈ E[x] and deg(f) ≤ n−1. But

the above shows that f has the n distinct zeros θ1,...,θn.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-67
SLIDE 67

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e) = Φ

  • n−1

i=0

fiθ i

  • =

n−1

i=0

fiΦ(θ)i =

n−1

i=0

fiθ i

j .

Let f(x) := −e+

n−1

i=0

  • fixi. Then f ∈ E[x] and deg(f) ≤ n−1. But

the above shows that f has the n distinct zeros θ1,...,θn. This is

  • nly possible if f = 0.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-68
SLIDE 68

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e) = Φ

  • n−1

i=0

fiθ i

  • =

n−1

i=0

fiΦ(θ)i =

n−1

i=0

fiθ i

j .

Let f(x) := −e+

n−1

i=0

  • fixi. Then f ∈ E[x] and deg(f) ≤ n−1. But

the above shows that f has the n distinct zeros θ1,...,θn. This is

  • nly possible if f = 0. But then −e+f0

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-69
SLIDE 69

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e) = Φ

  • n−1

i=0

fiθ i

  • =

n−1

i=0

fiΦ(θ)i =

n−1

i=0

fiθ i

j .

Let f(x) := −e+

n−1

i=0

  • fixi. Then f ∈ E[x] and deg(f) ≤ n−1. But

the above shows that f has the n distinct zeros θ1,...,θn. This is

  • nly possible if f = 0. But then −e+f0 = f(0)

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-70
SLIDE 70

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e) = Φ

  • n−1

i=0

fiθ i

  • =

n−1

i=0

fiΦ(θ)i =

n−1

i=0

fiθ i

j .

Let f(x) := −e+

n−1

i=0

  • fixi. Then f ∈ E[x] and deg(f) ≤ n−1. But

the above shows that f has the n distinct zeros θ1,...,θn. This is

  • nly possible if f = 0. But then −e+f0 = f(0) = 0

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-71
SLIDE 71

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“2⇒3” concl.). Moreover, (note that E = F(θ) is the splitting field of p) there is an isomorphism Φ : E → E that continues ϕ. In particular, Φ fixes F and Φ(θ1) = θj. Now let e ∈ E be fixed by G(E/F). Because E = F(θ) we have e =

n−1

i=0

fiθ i, and because there is a Φ ∈ G(E/F) with Φ(θ) = θj, we also have e = Φ(e) = Φ

  • n−1

i=0

fiθ i

  • =

n−1

i=0

fiΦ(θ)i =

n−1

i=0

fiθ i

j .

Let f(x) := −e+

n−1

i=0

  • fixi. Then f ∈ E[x] and deg(f) ≤ n−1. But

the above shows that f has the n distinct zeros θ1,...,θn. This is

  • nly possible if f = 0. But then −e+f0 = f(0) = 0, that is,

e = f0 ∈ F, which was to be proved.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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SLIDE 72

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1”).

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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SLIDE 73

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1”). In case E = F, E is the splitting field for f(x) = x over F.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-74
SLIDE 74

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1”). In case E = F, E is the splitting field for f(x) = x over F. So for the remainder of this part, we can assume that E = F.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-75
SLIDE 75

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1”). In case E = F, E is the splitting field for f(x) = x over F. So for the remainder of this part, we can assume that E = F. For each a ∈ E let a1,...,an be the elements of

  • σ(a) : σ ∈ G(E/F)
  • Bernd Schr¨
  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-76
SLIDE 76

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1”). In case E = F, E is the splitting field for f(x) = x over F. So for the remainder of this part, we can assume that E = F. For each a ∈ E let a1,...,an be the elements of

  • σ(a) : σ ∈ G(E/F)
  • and let

fa(x) :=

n

j=1

(x−aj)

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-77
SLIDE 77

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1”). In case E = F, E is the splitting field for f(x) = x over F. So for the remainder of this part, we can assume that E = F. For each a ∈ E let a1,...,an be the elements of

  • σ(a) : σ ∈ G(E/F)
  • and let

fa(x) :=

n

j=1

(x−aj) =

n

k=0

bkxk ∈ E[x].

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-78
SLIDE 78

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1”). In case E = F, E is the splitting field for f(x) = x over F. So for the remainder of this part, we can assume that E = F. For each a ∈ E let a1,...,an be the elements of

  • σ(a) : σ ∈ G(E/F)
  • and let

fa(x) :=

n

j=1

(x−aj) =

n

k=0

bkxk ∈ E[x]. Let σ ∈ G(E/F).

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-79
SLIDE 79

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1”). In case E = F, E is the splitting field for f(x) = x over F. So for the remainder of this part, we can assume that E = F. For each a ∈ E let a1,...,an be the elements of

  • σ(a) : σ ∈ G(E/F)
  • and let

fa(x) :=

n

j=1

(x−aj) =

n

k=0

bkxk ∈ E[x]. Let σ ∈ G(E/F). The function ˜ σ : E[x] → E[x] defined by ˜ σ

  • n

k=0

ckxk

  • :=

n

k=0

σ(ck)xk is an isomorphism

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-80
SLIDE 80

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1”). In case E = F, E is the splitting field for f(x) = x over F. So for the remainder of this part, we can assume that E = F. For each a ∈ E let a1,...,an be the elements of

  • σ(a) : σ ∈ G(E/F)
  • and let

fa(x) :=

n

j=1

(x−aj) =

n

k=0

bkxk ∈ E[x]. Let σ ∈ G(E/F). The function ˜ σ : E[x] → E[x] defined by ˜ σ

  • n

k=0

ckxk

  • :=

n

k=0

σ(ck)xk is an isomorphism (good exercise).

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1”). In case E = F, E is the splitting field for f(x) = x over F. So for the remainder of this part, we can assume that E = F. For each a ∈ E let a1,...,an be the elements of

  • σ(a) : σ ∈ G(E/F)
  • and let

fa(x) :=

n

j=1

(x−aj) =

n

k=0

bkxk ∈ E[x]. Let σ ∈ G(E/F). The function ˜ σ : E[x] → E[x] defined by ˜ σ

  • n

k=0

ckxk

  • :=

n

k=0

σ(ck)xk is an isomorphism (good exercise). Let a ∈ E.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1”). In case E = F, E is the splitting field for f(x) = x over F. So for the remainder of this part, we can assume that E = F. For each a ∈ E let a1,...,an be the elements of

  • σ(a) : σ ∈ G(E/F)
  • and let

fa(x) :=

n

j=1

(x−aj) =

n

k=0

bkxk ∈ E[x]. Let σ ∈ G(E/F). The function ˜ σ : E[x] → E[x] defined by ˜ σ

  • n

k=0

ckxk

  • :=

n

k=0

σ(ck)xk is an isomorphism (good exercise). Let a ∈ E. Because σ permutes the a1,...,an we infer

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa)

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • Bernd Schr¨
  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • Bernd Schr¨
  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj)

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk, so σ(bk) = bk for all k.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk, so σ(bk) = bk for all k. (We’re “sort of” using that F has characteristic 0 here.)

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk, so σ(bk) = bk for all k. (We’re “sort of” using that F has characteristic 0 here.) Because σ ∈ G(E/F) was arbitrary, all bk are in F, the fixed field of G(E/F).

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk, so σ(bk) = bk for all k. (We’re “sort of” using that F has characteristic 0 here.) Because σ ∈ G(E/F) was arbitrary, all bk are in F, the fixed field of G(E/F). By definition, fa splits in E

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk, so σ(bk) = bk for all k. (We’re “sort of” using that F has characteristic 0 here.) Because σ ∈ G(E/F) was arbitrary, all bk are in F, the fixed field of G(E/F). By definition, fa splits in E and, because a = id(a) ∈ {a1,...,an}, we have fa(a) = 0.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk, so σ(bk) = bk for all k. (We’re “sort of” using that F has characteristic 0 here.) Because σ ∈ G(E/F) was arbitrary, all bk are in F, the fixed field of G(E/F). By definition, fa splits in E and, because a = id(a) ∈ {a1,...,an}, we have fa(a) = 0. Let v1,...,vm be a basis of E over F.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk, so σ(bk) = bk for all k. (We’re “sort of” using that F has characteristic 0 here.) Because σ ∈ G(E/F) was arbitrary, all bk are in F, the fixed field of G(E/F). By definition, fa splits in E and, because a = id(a) ∈ {a1,...,an}, we have fa(a) = 0. Let v1,...,vm be a basis of E over F. Then f :=

m

j=1

fvk ∈ F[x] splits in E

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk, so σ(bk) = bk for all k. (We’re “sort of” using that F has characteristic 0 here.) Because σ ∈ G(E/F) was arbitrary, all bk are in F, the fixed field of G(E/F). By definition, fa splits in E and, because a = id(a) ∈ {a1,...,an}, we have fa(a) = 0. Let v1,...,vm be a basis of E over F. Then f :=

m

j=1

fvk ∈ F[x] splits in E and f(vk) = 0 for all k.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk, so σ(bk) = bk for all k. (We’re “sort of” using that F has characteristic 0 here.) Because σ ∈ G(E/F) was arbitrary, all bk are in F, the fixed field of G(E/F). By definition, fa splits in E and, because a = id(a) ∈ {a1,...,an}, we have fa(a) = 0. Let v1,...,vm be a basis of E over F. Then f :=

m

j=1

fvk ∈ F[x] splits in E and f(vk) = 0 for all k. Hence the splitting field of f must contain E.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk, so σ(bk) = bk for all k. (We’re “sort of” using that F has characteristic 0 here.) Because σ ∈ G(E/F) was arbitrary, all bk are in F, the fixed field of G(E/F). By definition, fa splits in E and, because a = id(a) ∈ {a1,...,an}, we have fa(a) = 0. Let v1,...,vm be a basis of E over F. Then f :=

m

j=1

fvk ∈ F[x] splits in E and f(vk) = 0 for all k. Hence the splitting field of f must contain E. So E is the splitting field of f.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (“3⇒1” concl.).

n

k=0

σ(bk)xk = ˜ σ(fa) = ˜ σ

  • n

j=1

(x−aj)

  • =

n

j=1

  • x− ˜

σ(aj)

  • =

n

j=1

(x−aj) = fa =

n

k=0

bkxk, so σ(bk) = bk for all k. (We’re “sort of” using that F has characteristic 0 here.) Because σ ∈ G(E/F) was arbitrary, all bk are in F, the fixed field of G(E/F). By definition, fa splits in E and, because a = id(a) ∈ {a1,...,an}, we have fa(a) = 0. Let v1,...,vm be a basis of E over F. Then f :=

m

j=1

fvk ∈ F[x] splits in E and f(vk) = 0 for all k. Hence the splitting field of f must contain E. So E is the splitting field of f.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Definition.

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Definition. Let (F,+,·) be a field and let E be a finite extension
  • f F.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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  • Definition. Let (F,+,·) be a field and let E be a finite extension
  • f F. Then E is called a normal extension of F iff every

irreducible polynomial p ∈ F[x] that has one zero in E actually splits in E.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Definition. Let (F,+,·) be a field and let E be a finite extension
  • f F. Then E is called a normal extension of F iff every

irreducible polynomial p ∈ F[x] that has one zero in E actually splits in E. Example.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Definition. Let (F,+,·) be a field and let E be a finite extension
  • f F. Then E is called a normal extension of F iff every

irreducible polynomial p ∈ F[x] that has one zero in E actually splits in E.

  • Example. R is not a normal extension of Q.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Definition. Let (F,+,·) be a field and let E be a finite extension
  • f F. Then E is called a normal extension of F iff every

irreducible polynomial p ∈ F[x] that has one zero in E actually splits in E.

  • Example. R is not a normal extension of Q.

The polynomial p(x) = x5 −3x4 −3x3 +3x2 +3x+3 from the Eisenstein presentation is irreducible in Q[x]

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Definition. Let (F,+,·) be a field and let E be a finite extension
  • f F. Then E is called a normal extension of F iff every

irreducible polynomial p ∈ F[x] that has one zero in E actually splits in E.

  • Example. R is not a normal extension of Q.

The polynomial p(x) = x5 −3x4 −3x3 +3x2 +3x+3 from the Eisenstein presentation is irreducible in Q[x], one of its zeros is real

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Definition. Let (F,+,·) be a field and let E be a finite extension
  • f F. Then E is called a normal extension of F iff every

irreducible polynomial p ∈ F[x] that has one zero in E actually splits in E.

  • Example. R is not a normal extension of Q.

The polynomial p(x) = x5 −3x4 −3x3 +3x2 +3x+3 from the Eisenstein presentation is irreducible in Q[x], one of its zeros is real (in fact, three of them are)

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Definition. Let (F,+,·) be a field and let E be a finite extension
  • f F. Then E is called a normal extension of F iff every

irreducible polynomial p ∈ F[x] that has one zero in E actually splits in E.

  • Example. R is not a normal extension of Q.

The polynomial p(x) = x5 −3x4 −3x3 +3x2 +3x+3 from the Eisenstein presentation is irreducible in Q[x], one of its zeros is real (in fact, three of them are), but not all of them are real.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Definition. Let (F,+,·) be a field and let E be a finite extension
  • f F. Then E is called a normal extension of F iff every

irreducible polynomial p ∈ F[x] that has one zero in E actually splits in E.

  • Example. R is not a normal extension of Q.

The polynomial p(x) = x5 −3x4 −3x3 +3x2 +3x+3 from the Eisenstein presentation is irreducible in Q[x], one of its zeros is real (in fact, three of them are), but not all of them are real.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Theorem.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a normal extension of F.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a normal extension of F. Then

  • G(E/F)
  • = [E : F].

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a normal extension of F. Then

  • G(E/F)
  • = [E : F].

Proof.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a normal extension of F. Then

  • G(E/F)
  • = [E : F].
  • Proof. Because E is a normal extension, it is the splitting field
  • f some polynomial f ∈ F[x].

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a normal extension of F. Then

  • G(E/F)
  • = [E : F].
  • Proof. Because E is a normal extension, it is the splitting field
  • f some polynomial f ∈ F[x]. Hence E = F(γ1,...,γm), where

γ1,...,γm are the zeros of f in E\F.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a normal extension of F. Then

  • G(E/F)
  • = [E : F].
  • Proof. Because E is a normal extension, it is the splitting field
  • f some polynomial f ∈ F[x]. Hence E = F(γ1,...,γm), where

γ1,...,γm are the zeros of f in E\F. There is a θ ∈ E so that E = F(γ1,...,γm) = F(θ) and θ is a zero of a polynomial in F[x].

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a normal extension of F. Then

  • G(E/F)
  • = [E : F].
  • Proof. Because E is a normal extension, it is the splitting field
  • f some polynomial f ∈ F[x]. Hence E = F(γ1,...,γm), where

γ1,...,γm are the zeros of f in E\F. There is a θ ∈ E so that E = F(γ1,...,γm) = F(θ) and θ is a zero of a polynomial in F[x]. (We’re using that F has characteristic 0 here.)

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a normal extension of F. Then

  • G(E/F)
  • = [E : F].
  • Proof. Because E is a normal extension, it is the splitting field
  • f some polynomial f ∈ F[x]. Hence E = F(γ1,...,γm), where

γ1,...,γm are the zeros of f in E\F. There is a θ ∈ E so that E = F(γ1,...,γm) = F(θ) and θ is a zero of a polynomial in F[x]. (We’re using that F has characteristic 0 here.) But then θ also is a zero of an irreducible polynomial of degree n in F[x].

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a normal extension of F. Then

  • G(E/F)
  • = [E : F].
  • Proof. Because E is a normal extension, it is the splitting field
  • f some polynomial f ∈ F[x]. Hence E = F(γ1,...,γm), where

γ1,...,γm are the zeros of f in E\F. There is a θ ∈ E so that E = F(γ1,...,γm) = F(θ) and θ is a zero of a polynomial in F[x]. (We’re using that F has characteristic 0 here.) But then θ also is a zero of an irreducible polynomial of degree n in F[x]. Hence the set

  • 1,θ,...,θ n−1

is a basis for E over F.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

  • Theorem. Let (F,+,·) be a field of characteristic 0 and let E

be a normal extension of F. Then

  • G(E/F)
  • = [E : F].
  • Proof. Because E is a normal extension, it is the splitting field
  • f some polynomial f ∈ F[x]. Hence E = F(γ1,...,γm), where

γ1,...,γm are the zeros of f in E\F. There is a θ ∈ E so that E = F(γ1,...,γm) = F(θ) and θ is a zero of a polynomial in F[x]. (We’re using that F has characteristic 0 here.) But then θ also is a zero of an irreducible polynomial of degree n in F[x]. Hence the set

  • 1,θ,...,θ n−1

is a basis for E over F. In particular, n = [E : F].

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (concl.).

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (concl.). Now

  • G(E/F)
  • =
  • G(F(θ)/F)
  • ≤ n.

Bernd Schr¨

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Louisiana Tech University, College of Engineering and Science Normal Field Extensions

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Proof (concl.). Now

  • G(E/F)
  • =
  • G(F(θ)/F)
  • ≤ n. Moreover,

p, being irreducible, has n distinct zeros θ1 = θ,θ2,...,θn.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-126
SLIDE 126

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (concl.). Now

  • G(E/F)
  • =
  • G(F(θ)/F)
  • ≤ n. Moreover,

p, being irreducible, has n distinct zeros θ1 = θ,θ2,...,θn. Because E is a normal extension of F, all zeros of p are in E.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-127
SLIDE 127

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (concl.). Now

  • G(E/F)
  • =
  • G(F(θ)/F)
  • ≤ n. Moreover,

p, being irreducible, has n distinct zeros θ1 = θ,θ2,...,θn. Because E is a normal extension of F, all zeros of p are in E. For every j ∈ {1,...,n} there is an automorphism of E that fixes F and that maps θ to θj.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-128
SLIDE 128

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (concl.). Now

  • G(E/F)
  • =
  • G(F(θ)/F)
  • ≤ n. Moreover,

p, being irreducible, has n distinct zeros θ1 = θ,θ2,...,θn. Because E is a normal extension of F, all zeros of p are in E. For every j ∈ {1,...,n} there is an automorphism of E that fixes F and that maps θ to θj. No two of these n automorphisms are equal to each other.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-129
SLIDE 129

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (concl.). Now

  • G(E/F)
  • =
  • G(F(θ)/F)
  • ≤ n. Moreover,

p, being irreducible, has n distinct zeros θ1 = θ,θ2,...,θn. Because E is a normal extension of F, all zeros of p are in E. For every j ∈ {1,...,n} there is an automorphism of E that fixes F and that maps θ to θj. No two of these n automorphisms are equal to each other. So

  • G(E/F)
  • ≥ n.

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-130
SLIDE 130

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (concl.). Now

  • G(E/F)
  • =
  • G(F(θ)/F)
  • ≤ n. Moreover,

p, being irreducible, has n distinct zeros θ1 = θ,θ2,...,θn. Because E is a normal extension of F, all zeros of p are in E. For every j ∈ {1,...,n} there is an automorphism of E that fixes F and that maps θ to θj. No two of these n automorphisms are equal to each other. So

  • G(E/F)
  • ≥ n. Hence
  • G(E/F)
  • = n = [E : F].

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions

slide-131
SLIDE 131

logo1 Characterizing Splitting Fields Normal Extensions Size of the Galois Group

Proof (concl.). Now

  • G(E/F)
  • =
  • G(F(θ)/F)
  • ≤ n. Moreover,

p, being irreducible, has n distinct zeros θ1 = θ,θ2,...,θn. Because E is a normal extension of F, all zeros of p are in E. For every j ∈ {1,...,n} there is an automorphism of E that fixes F and that maps θ to θj. No two of these n automorphisms are equal to each other. So

  • G(E/F)
  • ≥ n. Hence
  • G(E/F)
  • = n = [E : F].

Bernd Schr¨

  • der

Louisiana Tech University, College of Engineering and Science Normal Field Extensions