A holomorphic function on the open set is complex differentiable at every point of : the limit
exists independently of the direction of approach. Write . The Cauchy-Riemann equations are
To prove necessity, approach first with real , obtaining . Approach instead with for real , obtaining
Equality of real and imaginary parts yields the displayed Cauchy-Riemann equations.
A sufficient condition is that and have continuous first partial derivatives throughout and satisfy the Cauchy-Riemann equations there. Indeed, real differentiability gives, for ,
The Cauchy-Riemann equations imply , so this is . Dividing by proves complex differentiability and at every point. Merely having first partial derivatives and the equations at a point, without a suitable differentiability hypothesis, would not justify this argument.
Put . This is a closed set. First assume is nonempty. The Heine-Borel theorem makes the nonempty bounded closed set a compact set. By the preceding parts, is a continuous function and is strictly positive at every , because .
The extreme value theorem gives attaining its minimum. Therefore
The equality with the distance between two sets follows by taking the two infima successively. Crucially, compactness supplies a point attaining the minimum; positivity at each point alone would not make an arbitrary infimum positive. This is the principle that a compact subset of an open set has positive distance from its complement.
If , its complement is empty. With the usual extended-real convention , the stated inequality holds in that case too.
A subset is an open set if every admits a radius such that the open ball
is contained in . A subset is a closed set if its complement is an open set. Equivalently, contains the limit of every convergent sequence of its points.
Set to define a surjective ring homomorphism
Its kernel of a ring homomorphism is exactly : the constant coefficient in must vanish, so every remaining monomial is divisible by . The first isomorphism theorem for rings therefore gives
The polynomial ring is an integral domain, because the product of two nonzero polynomials has nonzero leading coefficient. It is not a field: has no polynomial multiplicative inverse, since a nonzero product has positive degree of a polynomial. Consequently is prime and is not maximal. Concretely, is a strict chain of ideals.
If the quotient ring is an integral domain, then , because an integral domain has . For ,
There are no nonzero zero divisors in an integral domain, so or . Thus or , proving is a prime ideal.
If is a field, again is proper. Let be an ideal properly containing , and choose . The nonzero element has a multiplicative inverse , so . Since , subtraction gives , hence . Therefore is a maximal ideal. These arguments establish the relevant prime ideal quotient criterion and maximal ideal quotient criterion.
A prime ideal is a proper ideal such that implies or . A maximal ideal is a proper ideal such that there is no ideal strictly between and .
Every ideal of the integers has the form for a unique nonnegative integer . Its prime ideals and maximal ideals are respectively
The zero ideal is a prime ideal because the integers form an integral domain. For a prime number , divisibility of by forces divisibility of one factor, so is a prime ideal. Also any ideal containing has , so it equals or ; thus is a maximal ideal.
If is composite, write with . Then while neither factor belongs to , so is not a prime ideal. A prime number gives , so is not a maximal ideal either. The zero ideal is not maximal since , and is not proper.
A diagonalizable matrix over the field admits an invertible matrix with entries in such that
Equivalently, the vector space has a basis of eigenvectors of . Indeed, says that each column of is an eigenvector with the corresponding diagonal entry as its eigenvalue. Requiring the basis and eigenvalues to lie in makes the choice of field essential.
For a linear functional , the definition of the dual map gives
Thus the kernel of a linear map is precisely the annihilator of a vector subspace
Write , and . The rank-nullity theorem, the dimension formula for an annihilator of a vector subspace, and give
Applying the same dimension formula in gives
Finally, if and , then . Therefore . These are finite-dimensional vector subspaces of equal dimension, so inclusion is equality:
This is the dual image and kernel annihilator identity.
The annihilator of a vector subspace consists of the linear functionals that vanish on every element of that vector subspace:
For the dimension identity, choose a basis of and use basis extension to obtain for . A linear functional is determined by its values on these basis vectors. Belonging to the annihilator of a vector subspace sets its first values to zero and leaves its last values arbitrary. Equivalently the last elements of the dual basis form a basis of .
The dual space consists of the linear functionals on the original vector space, with addition and scalar multiplication defined pointwise:
The dual map acts by function composition with :
For , its value is . The composite is a linear functional because both and are linear maps. Moreover , so the dual map is itself a linear map. Its direction is reversed because a measurement on the output of becomes a measurement on its input.
A pole of order at means
Equivalently the lowest nonzero power in its Laurent series is . In particular, tends to a finite nonzero limit.
An isolated singularity at means that the function is holomorphic on some punctured disc , while it is undefined or fails to be holomorphic at . The punctured neighbourhood contains no other singularities; this isolation is needed before applying the usual removable/pole/essential classification.
Away from zero, singularities occur exactly when , namely
For , differentiation at gives . Thus every is a simple pole, with residue .
As , these poles accumulate at zero. Therefore zero is a non-isolated singularity. Every punctured disc around it contains poles, so the function is not holomorphic on any punctured disc there. In particular zero cannot be classified as an isolated essential singularity; the isolated-singularity classification does not apply. The displayed poles and their accumulation point zero exhaust the finite singularities.

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