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Field extension

In , a field extension consists of a base field K and a larger field L such that K is a subfield of L, allowing L to be viewed as a over K. The dimension of this vector space, denoted [L:K], is called the of the extension and measures its "size" relative to K; extensions with finite degree are termed finite extensions. Elements \alpha \in L are classified as algebraic over K if they satisfy a nonzero equation with coefficients in K, or transcendental otherwise; an extension L/K is algebraic if every of L is algebraic over K, and transcendental if it contains at least one transcendental . All finite extensions are algebraic, but infinite algebraic extensions exist, such as the field of all algebraic numbers over \mathbb{Q}. Simple extensions, generated by adjoining a single \alpha to K to form K(\alpha), have equal to the degree of the minimal of \alpha over K when \alpha is algebraic. Field extensions underpin key results in , including the existence of splitting fields for —minimal extensions where a given factors completely into linear terms—and tower laws for degrees in chains of extensions, where [L:K] = [L:F] \cdot [F:K] for intermediate fields. They are central to , which studies the symmetries of extensions via Galois groups to determine solvability of by radicals, as in classical problems like or cube duplication. Examples include \mathbb{Q}(\sqrt{2})/\mathbb{Q} (degree 2, algebraic) and \mathbb{R}/\mathbb{Q} (infinite degree, transcendental elements like \pi).

Definitions and Basic Terminology

Field extensions

A field extension is formally defined as a pair of fields L and K, denoted L/K, where K is a subfield of L. In this setup, L contains an isomorphic copy of K via an injective field homomorphism, ensuring that the algebraic structure of K is preserved within L. Common notation for such extensions includes L \supseteq K or K \subseteq L, with the embedding \iota: K \to L typically taken as the identity map when K is literally a subset of L. This embedding guarantees that the addition and multiplication operations in L restrict exactly to those in K, maintaining compatibility between the fields. As a basic property, L forms a left vector space over K, where scalar multiplication is defined using the multiplication in L. The operations of and in L thus extend those of K naturally, allowing elements of K to act as scalars on elements of L. It is important to distinguish a extension from a mere set inclusion: not every superset of a qualifies as an extension unless equipped with an that aligns the field operations precisely. Without this embedding, the structure may fail to preserve the field axioms or compatibility. The concept of field extensions was introduced by in the 19th century, primarily in the context of , to study rings of algebraic integers within larger s.

Subfields

A subfield of a K is a subset F \subseteq K that forms a under the addition and multiplication operations induced from K. Equivalently, a subfield is a of K that is itself a , meaning it contains the multiplicative identity of K and every nonzero element of the subring has a within the subring. Subfields satisfy closure properties inherent to fields: they are closed under addition and multiplication, contain the additive identity 0 and the multiplicative identity 1 of K, and are closed under additive inverses. Additionally, for every nonzero element a \in F, the multiplicative inverse a^{-1} lies in F. These properties ensure that the subfield operations align perfectly with those of the ambient field K. The prime subfield of K is the smallest subfield of K, defined as the of all subfields of K. This prime subfield is unique and isomorphic to \mathbb{[Q](/page/Q)} when the characteristic of K is 0, or to the prime field \mathbb{F}_p when the characteristic of K is a prime p. Every subfield of K contains the prime subfield, and subfields of K correspond precisely to the subrings of K that are fields under the induced operations. Intermediate fields arise as subfields strictly between the prime subfield and K, forming chains such as P \subset [F_1](/page/Intermediate) \subset [F_2](/page/Intermediate) \subset \cdots \subset K, where P denotes the prime subfield. The collection of all subfields of K, ordered by inclusion, constitutes a with the prime subfield as the least element and K as the greatest.

Degree of a field extension

In field theory, given a field extension L/K where K is a subfield of L, the degree of the extension, denoted [L : K], is defined as the of L considered as a over K. This dimension measures the "size" of the extension in a linear algebraic sense. Every field extension L/K admits a Hamel basis, which is a linearly independent set over K that spans L as a K-; the existence of such a basis relies on the . The extension is finite if this basis has finite n, in which case [L : K] = n, a positive ; otherwise, the degree is infinite. Notably, [L : K] = 1 if and only if L = K. For infinite-degree extensions, the cardinality of a Hamel basis can vary; for instance, the extension \mathbb{Q}(x)/\mathbb{Q} of s has countably infinite degree, while \mathbb{R}/\mathbb{Q} requires an uncountable basis of equal to the . In transcendental extensions, the dimension is infinite, and the transcendence degree—defined as the of a maximal algebraically subset over K—provides a measure of the "transcendental part" of the extension, often aligning with the structure of purely transcendental cases like fields.

Properties of Field Extensions

Simple extensions

A field extension L/K is called a simple extension if there exists some \alpha \in L such that L = K(\alpha), meaning L is generated by adjoining a single element \alpha to K. This element \alpha is known as a element for the extension L/K. The elements of a simple extension K(\alpha) can be expressed as rational functions in \alpha with coefficients in K, specifically of the form p(\alpha)/q(\alpha), where p(x) and q(x) are in K and q(\alpha) \neq 0. If \alpha is algebraic over K, then the elements are precisely the linear combinations \sum_{i=0}^{n-1} c_i \alpha^i with c_i \in K, where n is the of the minimal polynomial of \alpha over K. The states that every finite L/K is , i.e., L = K(\alpha) for some \alpha \in L. The proof relies on the of certain conjugates of the generators, allowing the construction of a primitive element as a suitable that avoids finitely many "bad" values which would cause dependencies. In particular, all finite extensions in characteristic zero are , as separability holds automatically there. Not all finite extensions are simple; for instance, the extension \mathbb{F}_p(X,Y)/\mathbb{F}_p(X^p, Y^p) has degree p^2 but requires at least two generators and admits no primitive element. Infinite extensions can also be simple, such as the transcendental extension \mathbb{Q}(\pi)/\mathbb{Q}. For a simple finite extension L = K(\alpha), the degree [L:K] equals the degree of the minimal polynomial of \alpha over K. This follows from the fact that \{1, \alpha, \dots, \alpha^{n-1}\} forms a basis for L as a vector space over K, where n = [L:K].

Tower law for degrees

The tower law, also known as the multiplicativity of degrees, states that for a tower of field extensions K \subseteq M \subseteq L, the degree of the overall extension satisfies [L : K] = [L : M] \cdot [M : K], provided the individual degrees are finite. This relation extends multiplicatively to any finite tower of extensions by on the length of the chain. To sketch the proof for the finite case, suppose \{u_i \mid 1 \leq i \leq [M : K]\} is a basis for M as a vector space over K, and \{v_j \mid 1 \leq j \leq [L : M]\} is a basis for L as a vector space over M. Then the set \{u_i v_j\} forms a basis for L as a over K, establishing the dimension equality [L : K] = [L : M] \cdot [M : K]. This multiplicativity arises specifically because field extensions behave as vector spaces, where dimensions multiply in towers; it does not hold in general for extensions of rings, where modules may lack unique ranks. In the infinite case, if at least one of [L : M] or [M : K] is infinite, then [L : K] is also infinite, and the equality holds in the sense of cardinal multiplication of the dimensions as vector spaces. The tower law facilitates degree computations in composite extensions; for instance, adjoining square roots successively yields [\mathbb{Q}(\sqrt{2}) : \mathbb{Q}] = 2 and [\mathbb{Q}(\sqrt{2}, \sqrt{3}) : \mathbb{Q}(\sqrt{2})] = 2, so by the tower law, [\mathbb{Q}(\sqrt{2}, \sqrt{3}) : \mathbb{Q}] = 4.

Finite versus infinite extensions

A field extension L/K is finite if its degree [L : K] is a finite positive , meaning L is a finite-dimensional over the base field K. Every finite extension is algebraic, in the sense that every of L satisfies a with coefficients in K. This algebraicity follows from the fact that a basis of L over K allows any to be expressed as a , leading to a of bounded . An extension L/K is infinite if [L : K] = \infty, so L is not finite-dimensional over K. Infinite extensions may be algebraic, as in the case of the algebraic numbers \overline{\mathbb{Q}} over the rationals \mathbb{Q}, or transcendental, involving elements not satisfying any polynomial over K, such as \mathbb{R}/\mathbb{Q} which contains elements like \pi. Every field extension L/K possesses a transcendence basis, defined as a maximal of L that is algebraically independent over K; the of any such basis is the transcendence degree of the extension. The transcendence degree is zero the extension is algebraic, and the extension is finite the transcendence degree is zero and the resulting has finite degree. Infinite extensions thus allow for transcendence bases of positive , enabling the of L into a transcendental part followed by an . Finite extensions exhibit properties analogous to those of finite-dimensional vector spaces, such as the existence of bases, traces, norms, and determinants for K-linear maps from L to itself. These features do not hold for infinite extensions, where linear maps may lack such invariants. For example, the tower law states that degrees multiply in finite towers of extensions, but infinite degrees prevent similar multiplicative behavior. In certain contexts, such as number fields, finite extensions L/\mathbb{Q} ensure that the integral closure of \mathbb{Z} in L is finitely generated as a \mathbb{Z}-module.

Illustrative Examples

Rational to algebraic number fields

A fundamental example of a finite algebraic extension is \mathbb{Q}(\sqrt{2})/\mathbb{Q}, which has degree 2. The standard basis for this extension as a vector space over \mathbb{Q} is \{1, \sqrt{2}\}, and the minimal polynomial of \sqrt{2} over \mathbb{Q} is x^2 - 2. Every element in \mathbb{Q}(\sqrt{2}) can be uniquely expressed as a + b\sqrt{2} with a, b \in \mathbb{Q}. For extensions adjoining multiple square roots, consider \mathbb{Q}(\sqrt{2}, \sqrt{3})/\mathbb{Q}. This has degree 4, obtained via the tower \mathbb{Q} \subseteq \mathbb{Q}(\sqrt{2}) \subseteq \mathbb{Q}(\sqrt{2}, \sqrt{3}), where each step has degree 2. The extension is , generated by the primitive element \sqrt{2} + \sqrt{3}, whose minimal over \mathbb{Q} is x^4 - 10x^2 + 1. More generally, quadratic fields take the form \mathbb{Q}(\sqrt{d})/\mathbb{Q} for square-free integers d \neq 1, each of degree 2 over \mathbb{Q}. The discriminant of such a field is \Delta = d if d \equiv 1 \pmod{4} and \Delta = 4d otherwise, which measures the "ramification" in the extension. The ring of integers \mathcal{O}_K is \mathbb{Z}[\sqrt{d}] if d \equiv 2, 3 \pmod{4} and \mathbb{Z}\left[\frac{1 + \sqrt{d}}{2}\right] if d \equiv 1 \pmod{4}. All quadratic extensions are simple, as guaranteed by the for finite separable extensions. Quadratic fields play a key role in number theory, particularly for solving Diophantine equations such as Pell's equation x^2 - d y^2 = \pm 1, where solutions correspond to units in the ring of integers. In quadratic fields, the norm map N_{\mathbb{Q}(\sqrt{d})/\mathbb{Q}}(a + b\sqrt{d}) = a^2 - d b^2 and trace map \mathrm{Tr}_{\mathbb{Q}(\sqrt{d})/\mathbb{Q}}(a + b\sqrt{d}) = 2a provide multiplicative and additive invariants, previewing their generalization via field automorphisms in broader contexts.

Function fields and transcendental extensions

A classic example of a transcendental field extension is the rational function field \mathbb{C}(t) over the complex numbers \mathbb{C}, where t is an indeterminate, consisting of all quotients of polynomials in t with coefficients in \mathbb{C}. This extension has transcendence degree 1, meaning \{t\} forms a transcendence basis, and it is of infinite degree as a vector space over \mathbb{C}. Unlike algebraic extensions, t satisfies no minimal polynomial over \mathbb{C}, highlighting its transcendental nature. Elements of \mathbb{C}(t) are formal expressions f(t)/g(t), where f, g \in \mathbb{C} and g \neq 0, with defined by after clearing common factors. The extension admits no finite basis as a over \mathbb{C}, as powers of t and their inverses generate infinitely many linearly independent elements. A real analog is \mathbb{R}(x)/\mathbb{R}, the field of rational functions in x over the reals, which similarly exhibits transcendence degree 1 and models real rational functions on the line. Function fields like \mathbb{C}(t)/\mathbb{C} play a central role in , where they model the rational functions on algebraic , with the transcendence degree corresponding to the dimension of the (here, 1 for a ). In , such fields relate to meromorphic functions on Riemann surfaces, providing a field-theoretic framework for studying holomorphic forms and divisors on these surfaces. Transcendental extensions of this type are inherently non-algebraic, distinguishing them from finite extensions where every element satisfies a equation over the base .

Cyclotomic extensions

A cyclotomic extension is the field extension \mathbb{Q}(\zeta_n)/\mathbb{Q}, obtained by adjoining a primitive nth \zeta_n to the rational numbers \mathbb{Q}, where \zeta_n satisfies \zeta_n^n = 1 and no smaller positive exponent works. The degree of this extension is [\mathbb{Q}(\zeta_n) : \mathbb{Q}] = \phi(n), where \phi denotes , which counts the number of integers up to n that are coprime to n. The minimal polynomial of \zeta_n over \mathbb{Q} is the monic nth \Phi_n(x), defined as \Phi_n(x) = \prod (x - \zeta), where the product runs over all primitive nth roots of unity \zeta, and it has degree \phi(n). For example, when n=5, \phi(5) = 4, so [\mathbb{Q}(\zeta_5) : \mathbb{Q}] = 4, and the minimal is \Phi_5(x) = x^4 + x^3 + x^2 + x + 1. The extension \mathbb{Q}(\zeta_n)/\mathbb{Q} is Galois, hence and separable, with \mathrm{Gal}(\mathbb{Q}(\zeta_n)/\mathbb{Q}) isomorphic to the of units n, denoted (\mathbb{Z}/n\mathbb{Z})^\times, which is abelian. This abelian structure makes cyclotomic extensions fundamental in and . Cyclotomic fields have been instrumental in proofs of , especially in Kummer's approach using unique factorization failures in rings of cyclotomic integers and subsequent developments involving class numbers and units. The field \mathbb{Q}(\zeta_n) contains all mth roots of unity for m dividing n, as these are polynomials in \zeta_n. For a fixed prime p, the cyclotomic fields \mathbb{Q}(\zeta_{p^k}) for k = 1, 2, \dots form an infinite tower of extensions, each of degree p over the previous one, leading to the cyclotomic \mathbb{Z}_p-extension of \mathbb{Q}. An explicit power basis for \mathbb{Q}(\zeta_n) as a over \mathbb{Q} is \{1, \zeta_n, \zeta_n^2, \dots, \zeta_n^{\phi(n)-1}\}, reflecting the simplicity of the extension generated by a single .

Algebraic and Transcendental Extensions

Algebraic extensions

An element \alpha in an extension L of a K is said to be algebraic over K if there exists a non-zero f(x) \in K such that f(\alpha) = 0. The minimal of \alpha over K, denoted m_\alpha(x), is the monic in K of least degree that has \alpha as a . Thus, m_\alpha(\alpha) = 0, and every satisfies its minimal . A field extension L/K is algebraic if every element of L is algebraic over K. Such extensions include simple extensions obtained by adjoining a single algebraic element \alpha, where the degree [K(\alpha):K] equals the degree of the minimal polynomial \deg(m_\alpha). An algebraic extension L/K is finite if and only if [L:K] is finite, in which case L is generated by finitely many algebraic elements over K. The algebraic extensions of K are closed under finite unions, meaning the compositum of finitely many algebraic extensions of K is again algebraic over K. The algebraic closure of K, denoted \bar{K}, is a maximal algebraic extension of K that is algebraically closed, meaning every non-constant in \bar{K} has a in \bar{K}. Any two algebraic closures of K are isomorphic over K. For example, the algebraic closure \bar{\mathbb{Q}} of the rationals \mathbb{Q} consists precisely of the algebraic numbers, which form an algebraically closed field of infinite degree over \mathbb{Q}. In algebraic extensions, particularly over \mathbb{Q}, an element \alpha is integral over \mathbb{Z} (an ) if its minimal over \mathbb{Q} has integer coefficients and is monic. For a basis of a finite algebraic extension, the measures the "overlap" between basis elements and is defined as the of the trace form on the basis.

Transcendental extensions

In field theory, an \alpha in a field extension L/K is called transcendental over K if it is not algebraic over K, meaning there does not exist a nonzero f(x) \in K such that f(\alpha) = 0. A S \subseteq L is algebraically over K if no finite nonempty of S satisfies a nontrivial relation with coefficients in K, or equivalently, the evaluation K[x_s \mid s \in S] \to L sending each x_s to s is injective. A transcendence basis for L/K is a maximal algebraically B \subseteq L over K, and every such basis has the same , called the transcendence degree of L/K, denoted \operatorname{tr.deg}(L/K). A key property of field extensions is that every extension L/K admits a transcendence basis B, and moreover, L is algebraic over the purely transcendental extension K(B), where K(B) is the field generated by K and the elements of B. Thus, any field extension can be viewed as a tower consisting of a purely transcendental extension followed by an algebraic extension. For example, if u is transcendental over \mathbb{C}(t), then \operatorname{tr.deg}(\mathbb{C}(t,u)/\mathbb{C}) = 2, with \{t, u\} serving as a transcendence basis. Purely transcendental extensions of finite transcendence degree n are isomorphic to the rational function field K(x_1, \dots, x_n). The transcendence degree can be infinite, as in the case of \mathbb{R}/\mathbb{Q}, where \operatorname{tr.deg}(\mathbb{R}/\mathbb{Q}) equals the . In general, if \operatorname{tr.deg}(L/K) > 0, then the extension degree [L : K] is infinite, since even a purely of positive finite degree has infinite degree over K. Transcendence degrees play a crucial role in the study of function fields; for instance, Lüroth's theorem states that any subfield L with K \subsetneq L \subsetneq K(t) (where t is transcendental over K) has transcendence degree 1 over K and is itself a transcendental extension K(u) for some u \in L. This highlights the uniqueness of transcendence degree 1 extensions in the univariate case, with applications to the of curves.

Special Types of Extensions

Normal extensions

A field extension L/K is called if it is algebraic and every f \in K that has at least one in L splits completely into linear factors in L. This condition ensures that L contains all conjugates of any element over K, preserving the full structure of minimal polynomials. For finite extensions, L/K is normal if and only if L is the splitting field over K of some polynomial f \in K. In the general algebraic case, including infinite extensions, L/K is normal if and only if L is the splitting field over K of some family of polynomials in K. Normal extensions exhibit several key properties. The intersection of any finite collection of normal extensions of K contained in a common algebraic closure is again a normal extension of K. Moreover, if L/K is normal, then the Galois group \mathrm{Gal}(L/K) (defined as the group of K-automorphisms of L) acts transitively on the roots in L of any irreducible polynomial in K. Finite normal extensions are Galois precisely when they are also separable. For example, cyclotomic extensions \mathbb{Q}(\zeta_n)/\mathbb{Q}, where \zeta_n is a primitive nth root of unity, are normal because they are the splitting fields of the irreducible cyclotomic polynomials \Phi_n(x) \in \mathbb{Q}. In contrast, the extension \mathbb{Q}(\sqrt{{grok:render&&&type=render_inline_citation&&&citation_id=3&&&citation_type=wikipedia}}{2})/\mathbb{Q}, adjoining only the real cube root of 2, is not normal, as the minimal polynomial x^3 - 2 has one root in the extension but its other two complex roots are missing.

Separable extensions

A polynomial f \in K[X] over a field K is called separable if it has distinct roots in a over K, meaning no root has multiplicity greater than one; equivalently, f and its formal f' are coprime in K[X], so \gcd(f, f') = 1. An L/K is separable if every element \alpha \in L has a separable minimal over K; for finite extensions, this holds if and only if the number of distinct K-embeddings of L into an of K equals the degree [L:K]. In fields of characteristic zero, every is separable (since f' \neq 0), so every is separable. In characteristic p > 0, inseparable extensions exist; a basic example is the purely inseparable extension \mathbb{F}_p(t)/\mathbb{F}_p(t^p) of degree p, where t is transcendental over \mathbb{F}_p and the minimal of t over \mathbb{F}_p(t^p) is X^p - t^p = (X - t)^p, which has a multiple . The separable closure of a K exists as a inside an of K, consisting of all elements separable over K; it is the compositum of all finite separable extensions of K. Moreover, the compositum of any two separable extensions of K contained in a common extension is itself separable over K. Separable polynomials split into distinct linear factors in extensions, distinguishing separability from by focusing on multiplicity rather than completeness of splitting.

Galois extensions

A is a finite field extension L/K that is both and separable, meaning every over K with a root in L splits completely into linear factors in L, and the minimal polynomial of every element of L over K has distinct . Equivalently, L is the over K of a . The associated \mathrm{Gal}(L/K) is defined as the group \mathrm{Aut}_K(L) of all field automorphisms of L that fix K pointwise, and for a finite , the order of this group equals the degree of the extension: |\mathrm{Gal}(L/K)| = [L:K]. The establishes a bijective, order-reversing between the subfields of L containing K and the of \mathrm{Gal}(L/K). Specifically, each H \leq \mathrm{Gal}(L/K) corresponds to its fixed field L^H = \{ x \in L \mid \sigma(x) = x \ \forall \sigma \in H \}, and each intermediate field K \subseteq M \subseteq L corresponds to the \mathrm{Gal}(L/M); the [L:M] equals |H| where H = \mathrm{Gal}(L/M), and subgroups correspond to Galois subextensions. This lattice isomorphism provides a deep connection between the algebraic of the field extension and the group-theoretic of its . A field extension L/K is Galois if and only if it is finite, , and separable. For infinite Galois extensions, the theory extends by equipping the with the , making it a (an of finite groups), and the fundamental theorem holds for closed subgroups and their fixed fields. In such cases, the extension is the union of finite Galois subextensions, and the profinite structure captures the topology induced by open normal subgroups corresponding to finite quotients. Key properties of Galois extensions include the fact that the discriminant of a separable polynomial defining the extension (or more generally, of the extension itself via the different ideal) is nonzero, reflecting the separability condition. Galois theory plays a central role in determining solvability by radicals: a polynomial over a field of characteristic zero is solvable by radicals if and only if the Galois group of its splitting field is a solvable group. For example, the extension \mathbb{Q}(\sqrt{2})/\mathbb{Q} is Galois with \mathrm{Gal}(\mathbb{Q}(\sqrt{2})/\mathbb{Q}) \cong \mathbb{Z}/2\mathbb{Z}, generated by the automorphism sending \sqrt{2} to -\sqrt{2}.

Generalizations and Applications

Ring extensions

A ring extension consists of commutative rings A and B with a ring homomorphism \iota: A \to B such that B is an A-algebra via \iota, meaning B is also a module over A through the action induced by \iota. In this setup, B need not be a field even if A is, and elements of B are not necessarily invertible, unlike in field extensions where the codomain inherits the division ring structure. An integral extension is a special case where every element b \in B is integral over A, satisfying a monic polynomial f(x) = x^n + a_{n-1} x^{n-1} + \cdots + a_0 \in A with f(b) = 0. Key results include the going-up theorem, which states that for a prime ideal \mathfrak{p} \subset A, there exists a prime ideal \mathfrak{q} \subset B such that \mathfrak{q} \cap A = \mathfrak{p}, and chains of primes in A can be lifted to chains in B of the same length; the going-down theorem holds under additional conditions like normality of A. These theorems highlight how integral extensions preserve certain ideal-theoretic properties, such as lying-over (every prime in A contracts from some prime in B) and incomparability (corresponding primes have the same height). In the context of Dedekind domains, if A is a Dedekind domain and B is its integral closure in a finite extension of the fraction field of A, then B is also a Dedekind domain, preserving unique factorization of ideals into primes. This is crucial in number theory, where for extensions of number fields, ramification occurs when a prime ideal \mathfrak{p} \subset A factors in B with some prime powers having exponent greater than 1, measured by the ramification index e(\mathfrak{q}/\mathfrak{p}) for \mathfrak{q} \cap A = \mathfrak{p}. Notably, field extensions are integral precisely when they are algebraic, as every algebraic element satisfies a monic minimal polynomial over the base field. Unlike field extensions, where B is automatically a finite-dimensional vector space over A if algebraic, ring extensions generally lack such a structure; instead, one considers whether B is flat or projective as an A-, properties that ensure exactness of tensor products or lifting of projectives, but these do not hold universally without additional assumptions like freeness.

Extension of scalars

In the context of a field extension L/K, the extension of scalars provides a method to change the base field of a while preserving its structure. Given a V over K, the extended space V_L = V \otimes_K L is naturally an L-, where the L-action is defined by \ell \cdot (v \otimes \ell') = v \otimes (\ell \ell') for v \in V, \ell, \ell' \in L. This arises from viewing L as a K- via the inclusion and forming the , which endows V_L with the structure of an L-. Key properties of this extension include the preservation of for finite-dimensional spaces and conditions related to . If \dim_K V = n < \infty, then \dim_L V_L = n, with a basis for V_L given by \{1 \otimes b_i \mid b_i\} where \{b_i\} is a basis for V. Moreover, since any field extension L/K renders L as a K- (as it is a K- of equal to the if finite, or more generally a ), the V \mapsto V_L is exact, preserving exact sequences of K-vector spaces. This mechanism is foundational in algebraic geometry, where it facilitates the study of schemes over varying base fields by pulling back quasicoherent sheaves or vector bundles along base change morphisms, and plays a central role in descent theory for ensuring properties descend effectively under faithfully flat extensions. For instance, consider a \mathbb{Q}-vector space V; extending scalars to \mathbb{R} yields V_{\mathbb{R}} = V \otimes_{\mathbb{Q}} \mathbb{R}, which is an \mathbb{R}-vector space of the same dimension as V, effectively "complexifying" or realifying the structure while maintaining linear independence relations. Field extensions naturally induce scalar extensions on associated modules, transforming K-linear structures into L-linear ones compatibly with the extension map.

Applications in algebra and geometry

Field extensions play a crucial role in algebra, particularly in determining the solvability of polynomial equations by radicals, as established through Galois theory. In this framework, a polynomial is solvable by radicals if and only if its splitting field over the rationals has a solvable Galois group, a result originating from Galois's work on the quintic equation. This criterion not only resolves classical problems like the unsolvability of the general quintic but also extends to broader classes of equations, enabling the classification of solvable extensions via group-theoretic properties. In fields of p, Artin-Schreier theory provides an analogous tool for constructing cyclic extensions of degree p, where the extensions are generated by roots of equations of the form x^p - x = a for a in the base field not already in the image of the Artin-Schreier map. This construction is fundamental for understanding the structure of extensions in positive , paralleling in characteristic zero and facilitating the study of differential equations over such fields. In , field extensions underpin , which describes all abelian extensions of a number field as corresponding to ideals in its via the Artin map. This generalization of to infinite abelian groups connects algebraic structures to arithmetic, with applications to the distribution of primes in extensions. L-functions, such as Dirichlet L-functions for cyclotomic extensions, encode information about the arithmetic of these fields, including their zeta functions and regulator constants, which are central to the study of units and class numbers. Geometric applications arise in the study of algebraic curves, where the function of a curve over a captures its , with extensions corresponding to branched covers. The Riemann-Hurwitz formula quantifies the ramification in such covers, relating the of the extension to that of the via the degree and ramification indices: for a K/k of function fields of curves, 2g_K - 2 = [K:k](2g_k - 2) + \sum (e_P - 1), where g denotes and e_P the ramification index at place P. Modern developments highlight the role of p-adic extensions in local , where completions of global fields yield insights into global arithmetic via local-global principles. , as pursued in Grothendieck's program, posits that the algebraic of a , derived from étale extensions, recovers the variety's type, bridging field extensions to topological reconstruction. Étale cohomology further employs Galois extensions to define sheaf cohomology on algebraic stacks, providing tools for and arithmetic geometry beyond classical . Hilbert's 13th problem concerns the decomposability of algebraic functions into superpositions of functions of fewer variables, with resolutions involving towers of algebraic extensions showing that certain polynomials require towers of greater than 1, as measured by the resolvent degree. The Ax-Lindemann-Weierstrass theorem implies that if α is algebraic over , then e^{iα} is transcendental over ℚ(π) unless α/π is rational, linking algebraic and transcendental extensions in .

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