Choose a basis and let represent . Define the characteristic polynomial byUnder a change of basis with invertible change matrix , the new matrix is . HenceThus the polynomial is independent of the chosen coordinates. It is monic of degree .
To prove the sum is direct, suppose with . Fix and apply the polynomial in the linear operatorEvery with is killed by one factor. On , each factor is multiplication by , givingThe scalar coefficient is nonzero because the eigenvalues are distinct. Thus for every , provingIn particular, choosing a basis in each eigenspace yields a linearly independent combined list.
If , then , so is singular. By the rank-nullity theorem it has a nonzero kernel vector . ThusThis is exactly the definition of an eigenvalue. Here lies in the scalar field: for the stated real vector space it is real. A nonreal root instead gives an eigenvalue of the complexified operator, by the same argument over .
Expanding the determinant along the second column givesIf , there are three distinct real eigenvalues. Part (b)(ii) gives a nonzero eigenvector for each, and part (b)(i) makes them independent. They form a basis, so the matrix is diagonalisable.
When ,has rank one for every : the third row is nonzero, and the second row is times the third. Therefore the eigenspace for has dimension two. The eigenvalue provides at least one further independent eigenvector by part (b), so again there is an eigenbasis.
When ,Its rank is one if and two otherwise. Thus the eigenspace for has dimension two exactly when . For it has dimension one, while the eigenspace for also has dimension one, since then has rank two. There are no other eigenvalues by the characteristic polynomial. A diagonal matrix in an eigenbasis would need three independent eigenvectors, whereas these two eigenspaces supply only two; diagonalisation is impossible. Conversely, at their dimensions add to three and part (b) makes their sum direct. ThereforeThe argument uses only the determinant, rank-nullity, the established direct-sum result, and the definition of diagonalisation.
Use the convention that the inner product is linear in its first argument, as required by the displayed representation of a linear functional. Choose an orthonormal basis , for instance by Gram-Schmidt orthogonalization. DefineFor , conjugate linearity in the second argument givesThusThe representation is unique as well: if two vectors represent the same functional, their difference is orthogonal to every vector and therefore to itself, so it is zero.
The adjoint operator is characterized byFor each fixed , the map is a linear functional. Part (i) gives a representing vector, which we define to be . Hence such a map exists on every vector of . Part (b) proves that this constructed map is linear.
For scalars and vectors , use the adjoint identity and conjugate linearity in the second argument:The difference of the two second-argument vectors is orthogonal to every . Choosing to be that difference shows its squared norm is zero. ThereforeThe two conjugations are why the adjoint is a linear map, despite the conjugate-linear dependence of the representing functional on its second argument.
The finite-dimensional spectral theorem says that a self-adjoint operator on a complex inner-product space has an orthonormal basis of eigenvectors and all its eigenvalues are real. Equivalently, its matrix is unitarily diagonalisable with real diagonal entries.
For , the matrix is equal to its conjugate transpose:Thus it represents a self-adjoint operator for the standard inner product on . The theorem applies directly, proving
Set . Direct multiplication giveswith . If were diagonalisable, then subtracting the identity in the same basis would diagonalise . A diagonal matrix whose cube is zero has every diagonal entry zero and is itself zero. Similarity would then imply , a contradiction. HenceThis proves failure directly; merely observing that it is not self-adjoint would not suffice, because non-self-adjoint matrices can still be diagonalisable.
An ideal of a commutative ring is an additive subgroup such that for every and . A prime ideal is a proper ideal such that implies or .
If in the quotient ring, then . Primality implies or . Therefore there are no two nonzero cosets whose product is zero:Properness also ensures its identity coset is not zero, so this quotient is an integral domain.
To prove closure under addition, let . Expand by the binomial theorem. In every monomial , either or . Thus each term contains a factor or and belongs to . Hence , so . The additive subgroup and absorption properties are proved, givingThis ideal is the radical of an ideal. The finite exponent for a sum uses commutativity of the ring.
A coset is a nilpotent element of the quotient exactly when some positive power is zero:If , this forces every nilpotent coset to equal zero. Conversely, if there is no nonzero nilpotent coset, every has , hence . Since always, equality follows. ThereforeIn standard terms, an ideal is radical exactly when its quotient is a reduced ring.
Certainly , by taking exponent one. If , choose with . Primality applied to gives or . In the latter case repeat; induction reduces to . Thus as well, provingEvery prime ideal is therefore a radical ideal.
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