field (mathematics)

Informally, a field is a set, along with two operations defined on that set: an addition operation {{math|a + b}} and a multiplication operation {{math|a ⋅ b}}, both of which behave similarly as they do for rational numbers and real numbers. This includes the existence of an additive inverse {{math|−a}} for all elements {{mvar|a}} and of a multiplicative inverse {{math|b⁻¹}} for every nonzero element {{mvar|b}}. This allows the definition of the so-called inverse operations, subtraction {{math|a − b}} and division {{math|a / b}}, as {{math|1=a − b = a + (−b)}} and {{math|1=a / b = a ⋅ b⁻¹}}.

Often the product {{math|a ⋅ b}} is represented by juxtaposition, as {{mvar|ab}}.

Formally, a field is a set {{math|F}} together with two binary operations on {{mvar|F}} called addition and multiplication.{{harvp|Beachy|Blair|2006|loc=Definition 4.1.1, p. 181}} A binary operation on {{mvar|F}} is a mapping {{math|F × F → F}}, that is, a correspondence that associates with each ordered pair of elements of {{mvar|F}} a uniquely determined element of {{mvar|F}}.{{harvp|Fraleigh|1976|p=10}}{{harvp|McCoy|1968|p=16}} The result of the addition of {{math|a}} and {{math|b}} is called the sum of {{math|a}} and {{math|b}}, and is denoted {{math|a + b}}. Similarly, the result of the multiplication of {{math|a}} and {{math|b}} is called the product of {{math|a}} and {{math|b}}, and is denoted {{math|a ⋅ b}}. These operations are required to satisfy the following properties, referred to as field axioms.

These axioms are required to hold for all elements {{mvar|a}}, {{mvar|b}}, {{mvar|c}} of the field {{mvar|F}}:

• Associativity of addition and multiplication: {{math|1=a + (b + c) = (a + b) + c}}, and {{math|1=a ⋅ (b ⋅ c) = (a ⋅ b) ⋅ c}}.
• Commutativity of addition and multiplication: {{math|1=a + b = b + a}}, and {{math|1=a ⋅ b = b ⋅ a}}.
• Additive and multiplicative identity: there exist two distinct elements {{math|0}} and {{math|1}} in {{math|F}} such that {{math|1=a + 0 = a}} and {{math|1=a ⋅ 1 = a}}.
• Additive inverses: for every {{math|a}} in {{math|F}}, there exists an element in {{math|F}}, denoted {{math|−a}}, called the additive inverse of {{math|a}}, such that {{math|1=a + (−a) = 0}}.
• Multiplicative inverses: for every {{math|a ≠ 0}} in {{math|F}}, there exists an element in {{math|F}}, denoted by {{math|a⁻¹}} or {{math|1/a}}, called the multiplicative inverse of {{math|a}}, such that {{math|1=a ⋅ a⁻¹ = 1}}.
• Distributivity of multiplication over addition: {{math|1=a ⋅ (b + c) = (a ⋅ b) + (a ⋅ c)}}.

An equivalent, and more succinct, definition is: a field has two commutative operations, called addition and multiplication; it is a group under addition with {{math|0}} as the additive identity; the nonzero elements form a group under multiplication with {{math|1}} as the multiplicative identity; and multiplication distributes over addition.

Even more succinctly: a field is a commutative ring where {{math|0 ≠ 1}} and all nonzero elements are invertible under multiplication.

Fields can also be defined in different, but equivalent ways. One can alternatively define a field by four binary operations (addition, subtraction, multiplication, and division) and their required properties. Division by zero is, by definition, excluded.{{harvp|Clark|1984|loc=Chapter 3}} In order to avoid existential quantifiers, fields can be defined by two binary operations (addition and multiplication), two unary operations (yielding the additive and multiplicative inverses respectively), and two nullary operations (the constants {{math|0}} and {{math|1}}). These operations are then subject to the conditions above. Avoiding existential quantifiers is important in constructive mathematics and computing.{{harvp|Mines|Richman|Ruitenburg|1988|loc=§II.2}}. See also Heyting field. One may equivalently define a field by the same two binary operations, one unary operation (the multiplicative inverse), and two (not necessarily distinct) constants {{math|1}} and {{math|−1}}, since {{math|1=0 = 1 + (−1)}} and {{math|1=−a = (−1)a}}.{{efn|The a priori twofold use of the symbol "{{math|−}}" for denoting one part of a constant and for the additive inverses is justified by this latter condition.}}

{{Main|Rational number}}

Rational numbers have been widely used a long time before the elaboration of the concept of field.

They are numbers that can be written as fractions

{{math|a/b}}, where {{math|a}} and {{math|b}} are integers, and {{math|b ≠ 0}}. The additive inverse of such a fraction is {{math|−a/b}}, and the multiplicative inverse (provided that {{math|a ≠ 0}}) is {{math|b/a}}, which can be seen as follows:

: $\backslash frac\; b\; a\; \backslash cdot\; \backslash frac\; a\; b\; =\; \backslash frac\{ba\}\{ab\}\; =\; 1.$

The abstractly required field axioms reduce to standard properties of rational numbers. For example, the law of distributivity can be proven as follows:{{harvp|Beachy|Blair|2006|loc=p. 120, Ch. 3}}

: $$

\begin{align}

& \frac a b \cdot \left(\frac c d + \frac e f \right) \\[6pt]

= {} & \frac a b \cdot \left(\frac c d \cdot \frac f f + \frac e f \cdot \frac d d \right) \\[6pt]

= {} & \frac{a}{b} \cdot \left(\frac{cf}{df} + \frac{ed}{fd}\right) = \frac{a}{b} \cdot \frac{cf + ed}{df} \\[6pt]

= {} & \frac{a(cf + ed)}{bdf} = \frac{acf}{bdf} + \frac{aed}{bdf} = \frac{ac}{bd} + \frac{ae}{bf} \\[6pt]

= {} & \frac a b \cdot \frac c d + \frac a b \cdot \frac e f.

\end{align}

File:Complex multi.svg

{{main|Real number| Complex number}}

The real numbers {{math|R}}, with the usual operations of addition and multiplication, also form a field. The complex numbers {{math|C}} consist of expressions

: {{math|a + bi,}} with {{math|a, b}} real,

where {{math|i}} is the imaginary unit, i.e., a (non-real) number satisfying {{math|1=i² = −1}}.

Addition and multiplication of real numbers are defined in such a way that expressions of this type satisfy all field axioms and thus hold for {{math|C}}. For example, the distributive law enforces

: {{math|1=(a + bi)(c + di) = ac + bci + adi + bdi² = (ac − bd) + (bc + ad)i.}}

It is immediate that this is again an expression of the above type, and so the complex numbers form a field. Complex numbers can be geometrically represented as points in the plane, with Cartesian coordinates given by the real numbers of their describing expression, or as the arrows from the origin to these points, specified by their length and an angle enclosed with some distinct direction. Addition then corresponds to combining the arrows to the intuitive parallelogram (adding the Cartesian coordinates), and the multiplication is – less intuitively – combining rotating and scaling of the arrows (adding the angles and multiplying the lengths). The fields of real and complex numbers are used throughout mathematics, physics, engineering, statistics, and many other scientific disciplines.

File:Root_construction_geometric_mean5.svg asserts that {{math|1=h² = pq}}. Choosing {{math|1=q = 1}} allows construction of the square root of a given constructible number {{math|p}}.]]

{{main|Constructible numbers}}

In antiquity, several geometric problems concerned the (in)feasibility of constructing certain numbers with compass and straightedge. For example, it was unknown to the Greeks that it is, in general, impossible to trisect a given angle in this way. These problems can be settled using the field of constructible numbers.{{harvp|Artin|1991|loc=Chapter 13.4}} Real constructible numbers are, by definition, lengths of line segments that can be constructed from the points 0 and 1 in finitely many steps using only compass and straightedge. These numbers, endowed with the field operations of real numbers, restricted to the constructible numbers, form a field, which properly includes the field {{math|Q}} of rational numbers. The illustration shows the construction of square roots of constructible numbers, not necessarily contained within {{math|Q}}. Using the labeling in the illustration, construct the segments {{math|AB}}, {{math|BD}}, and a semicircle over {{math|AD}} (center at the midpoint {{math|C}}), which intersects the perpendicular line through {{math|B}} in a point {{math|F}}, at a distance of exactly $h=\backslash sqrt\; p$ from {{math|B}} when {{math|BD}} has length one.

Not all real numbers are constructible. It can be shown that $\backslash sqrt[3]\; 2$ is not a constructible number, which implies that it is impossible to construct with compass and straightedge the length of the side of a cube with volume 2, another problem posed by the ancient Greeks.

{{main|Finite field#Field with four elements}}

! scope="row" |

|}

In addition to familiar number systems such as the rationals, there are other, less immediate examples of fields. The following example is a field consisting of four elements called {{math|O}}, {{math|I}}, {{math|A}}, and {{math|B}}. The notation is chosen such that {{math|O}} plays the role of the additive identity element (denoted 0 in the axioms above), and {{math|I}} is the multiplicative identity (denoted {{math|1}} in the axioms above). The field axioms can be verified by using some more field theory, or by direct computation. For example,

: {{math|1=A ⋅ (B + A) = A ⋅ I = A}}, which equals {{nowrap|1={{math|1=A ⋅ B + A ⋅ A = I + B = A}}}}, as required by the distributivity.

This field is called a finite field or Galois field with four elements, and is denoted {{math|F₄}} or {{math|GF(4)}}.{{harvp|Lidl|Niederreiter|2008|loc=Example 1.62}} The subset consisting of {{math|O}} and {{math|I}} (highlighted in red in the tables at the right) is also a field, known as the binary field {{math|F₂}} or {{math|GF(2)}}.

In this section, {{math|F}} denotes an arbitrary field and {{math|a}} and {{math|b}} are arbitrary elements of {{math|F}}.

One has {{math|1=a ⋅ 0 = 0}} and {{math|1=−a = (−1) ⋅ a}}. In particular, one may deduce the additive inverse of every element as soon as one knows {{math|−1}}.{{harvp|Beachy|Blair|2006|loc=p. 120, Ch. 3}}

If {{math|1=ab = 0}} then {{math|1=a}} or {{math|b}} must be {{math|0}}, since, if {{math|a ≠ 0}}, then

{{math|1=b = (a⁻¹a)b = a⁻¹(ab) = a⁻¹ ⋅ 0 = 0}}. This means that every field is an integral domain.

In addition, the following properties are true for any elements {{math|a}} and {{math|b}}:

: {{math|1=−0 = 0}}

: {{math|1=1⁻¹ = 1}}

: {{math|1=(−(−a)) = a}}

: {{math|1=(−a) ⋅ b = a ⋅ (−b) = −(a ⋅ b)}}

: {{math|1=(a⁻¹)⁻¹ = a}} if {{math|a ≠ 0}}

The axioms of a field {{math|F}} imply that it is an abelian group under addition. This group is called the additive group of the field, and is sometimes denoted by {{math|(F, +)}} when denoting it simply as {{math|F}} could be confusing.

Similarly, the nonzero elements of {{math|F}} form an abelian group under multiplication, called the multiplicative group, and denoted by $(F\; \backslash smallsetminus\; \backslash \{0\backslash \},\; \backslash cdot)$ or just $F\; \backslash smallsetminus\; \backslash \{0\backslash \}$, or {{math|F^×}}.

A field may thus be defined as set {{math|F}} equipped with two operations denoted as an addition and a multiplication such that {{math|F}} is an abelian group under addition, $F\; \backslash smallsetminus\; \backslash \{0\backslash \}$ is an abelian group under multiplication (where 0 is the identity element of the addition), and multiplication is distributive over addition.{{efn|Equivalently, a field is an algebraic structure {{math|⟨F, +, ⋅, −, ⁻¹, 0, 1⟩}} of type {{math|{{angle bracket|2, 2, 1, 1, 0, 0}}}}, such that {{math|0⁻¹}} is not defined, {{math|{{angle bracket|F, +, −, 0}}}} and $\backslash left\backslash langle\; F\; \backslash smallsetminus\; \backslash \{0\backslash \},\; \backslash cdot,\; \{\}^\{-1\}\backslash right\backslash rangle$ are abelian groups, and {{math|⋅}} is distributive over {{math|+}}.{{harvp|Wallace|1998|loc=Th. 2}}}} Some elementary statements about fields can therefore be obtained by applying general facts of groups. For example, the additive and multiplicative inverses {{math|−a}} and {{math|a⁻¹}} are uniquely determined by {{math|a}}.

The requirement {{math|1 ≠ 0}} is imposed by convention to exclude the trivial ring, which consists of a single element; this guides any choice of the axioms that define fields.

Every finite subgroup of the multiplicative group of a field is cyclic (see {{slink|Root of unity|Cyclic groups}}).

In addition to the multiplication of two elements of {{math|F}}, it is possible to define the product {{math|n ⋅ a}} of an arbitrary element {{math|a}} of {{math|F}} by a positive integer {{math|n}} to be the {{math|n}}-fold sum

: {{math|a + a + ... + a}} (which is an element of {{math|F}}.)

If there is no positive integer such that

: {{math|1=n ⋅ 1 = 0}},

then {{math|F}} is said to have characteristic {{math|0}}.{{harvp|Adamson|2007|loc=§I.2, p. 10}} For example, the field of rational numbers {{math|Q}} has characteristic 0 since no positive integer {{math|n}} is zero. Otherwise, if there is a positive integer {{math|n}} satisfying this equation, the smallest such positive integer can be shown to be a prime number. It is usually denoted by {{math|p}} and the field is said to have characteristic {{math|p}} then.

For example, the field {{math|F₄}} has characteristic {{math|2}} since (in the notation of the above addition table) {{math|1=I + I = O }}.

If {{math|F}} has characteristic {{math|p}}, then {{math|1=p ⋅ a = 0}} for all {{math|a}} in {{math|F}}. This implies that

: {{math|1=(a + b)^p = {{itco|a}}^p + {{itco|b}}^p}},

since all other binomial coefficients appearing in the binomial formula are divisible by {{math|p}}. Here, {{math|1={{itco|a}}^p := a ⋅ a ⋅ ⋯ ⋅ a}} ({{math|p}} factors) is the {{math|p}}th power, i.e., the {{math|p}}-fold product of the element {{math|a}}. Therefore, the Frobenius map

: {{math|F → F : x ↦ {{itco|x}}^p}}

is compatible with the addition in {{math|F}} (and also with the multiplication), and is therefore a field homomorphism.{{harvp|Escofier|2012|loc=14.4.2}} The existence of this homomorphism makes fields in characteristic {{math|p}} quite different from fields of characteristic {{math|0}}.

A subfield {{math|E}} of a field {{math|F}} is a subset of {{math|F}} that is a field with respect to the field operations of {{math|F}}. Equivalently {{math|E}} is a subset of {{math|F}} that contains {{math|1}}, and is closed under addition, multiplication, additive inverse and multiplicative inverse of a nonzero element. This means that {{math|1 ∊ E}}, that for all {{math|a, b ∊ E}} both {{math|a + b}} and {{math|a ⋅ b}} are in {{math|E}}, and that for all {{math|a ≠ 0}} in {{math|E}}, both {{math|−a}} and {{math|1/a}} are in {{math|E}}.

Field homomorphisms are maps {{math|φ: E → F}} between two fields such that {{math|1=φ(e₁ + e₂) = φ(e₁) + φ(e₂)}}, {{math|1=φ(e₁e₂) = φ(e₁) φ(e₂)}}, and {{math|1=φ(1_E) = 1_F}}, where {{math|e₁}} and {{math|e₂}} are arbitrary elements of {{math|E}}. All field homomorphisms are injective.{{harvp|Adamson|2007|loc=§I.3}} If {{math|φ}} is also surjective, it is called an isomorphism (or the fields {{math|E}} and {{math|F}} are called isomorphic).

A field is called a prime field if it has no proper (i.e., strictly smaller) subfields. Any field {{math|F}} contains a prime field. If the characteristic of {{math|F}} is {{math|p}} (a prime number), the prime field is isomorphic to the finite field {{math|F_p}} introduced below. Otherwise the prime field is isomorphic to {{math|Q}}.{{harvp|Adamson|2007|loc=p. 12}}

{{Main|Finite field}}

Finite fields (also called Galois fields) are fields with finitely many elements, whose number is also referred to as the order of the field. The above introductory example {{math|F₄}} is a field with four elements. Its subfield {{math|F₂}} is the smallest field, because by definition a field has at least two distinct elements, {{math|0}} and {{math|1}}.

File:Clock group.svg

The simplest finite fields, with prime order, are most directly accessible using modular arithmetic. For a fixed positive integer {{math|n}}, arithmetic "modulo {{math|n}}" means to work with the numbers

: {{math|1=Z/nZ = {0, 1, ..., n − 1}.}}

The addition and multiplication on this set are done by performing the operation in question in the set {{math|Z}} of integers, dividing by {{math|n}} and taking the remainder as result. This construction yields a field precisely if {{math|n}} is a prime number. For example, taking the prime {{math|1=n = 2}} results in the above-mentioned field {{math|F₂}}. For {{math|1=n = 4}} and more generally, for any composite number (i.e., any number {{math|n}} which can be expressed as a product {{math|1=n = r ⋅ s}} of two strictly smaller natural numbers), {{math|1=Z/nZ}} is not a field: the product of two non-zero elements is zero since {{math|1=r ⋅ s = 0}} in {{math|Z/nZ}}, which, as was explained above, prevents {{math|Z/nZ}} from being a field. The field {{math|Z/pZ}} with {{math|p}} elements ({{math|p}} being prime) constructed in this way is usually denoted by {{math|F_p}}.

Every finite field {{math|F}} has {{math|1=q = pⁿ}} elements, where {{math|1=p}} is prime and {{math|n ≥ 1}}. This statement holds since {{math|F}} may be viewed as a vector space over its prime field. The dimension of this vector space is necessarily finite, say {{math|n}}, which implies the asserted statement.{{harvp|Lidl|Niederreiter|2008|loc=Lemma 2.1, Theorem 2.2}}

A field with {{math|1=q = pⁿ}} elements can be constructed as the splitting field of the polynomial

: {{math|1={{itco|f}}(x) = {{itco|x}}^q − x}}.

Such a splitting field is an extension of {{math|F_p}} in which the polynomial {{math|f}} has {{math|q}} zeros. This means {{math|f}} has as many zeros as possible since the degree of {{math|f}} is {{math|q}}. For {{math|1=q = 2² = 4}}, it can be checked case by case using the above multiplication table that all four elements of {{math|F₄}} satisfy the equation {{math|1=x⁴ = x}}, so they are zeros of {{math|f}}. By contrast, in {{math|F₂}}, {{math|f}} has only two zeros (namely {{math|0}} and {{math|1}}), so {{math|f}} does not split into linear factors in this smaller field. Elaborating further on basic field-theoretic notions, it can be shown that two finite fields with the same order are isomorphic.{{harvp|Lidl|Niederreiter|2008|loc=Theorem 1.2.5}} It is thus customary to speak of the finite field with {{math|q}} elements, denoted by {{math|F_q}} or {{math|GF(q)}}.

Historically, three algebraic disciplines led to the concept of a field: the question of solving polynomial equations, algebraic number theory, and algebraic geometry.{{harvp|Kleiner|2007|loc=p. 63}} A first step towards the notion of a field was made in 1770 by Joseph-Louis Lagrange, who observed that permuting the zeros {{math|x₁, x₂, x₃}} of a cubic polynomial in the expression

: {{math|(x₁ + ωx₂ + ω²x₃)³}}

(with {{math|ω}} being a third root of unity) only yields two values. This way, Lagrange conceptually explained the classical solution method of Scipione del Ferro and François Viète, which proceeds by reducing a cubic equation for an unknown {{math|x}} to a quadratic equation for {{math|x³}}.{{harvp|Kiernan|1971|loc=p. 50}} Together with a similar observation for equations of degree 4, Lagrange thus linked what eventually became the concept of fields and the concept of groups.{{harvp|Bourbaki|1994|loc=pp. 75–76}} Vandermonde, also in 1770, and to a fuller extent, Carl Friedrich Gauss, in his Disquisitiones Arithmeticae (1801), studied the equation

: {{math|1=x^p = 1}}

for a prime {{math|p}} and, again using modern language, the resulting cyclic Galois group. Gauss deduced that a regular polygon can be constructed if {{math|1=p = 2^2k + 1}}. Building on Lagrange's work, Paolo Ruffini claimed (1799) that quintic equations (polynomial equations of degree {{math|5}}) cannot be solved algebraically; however, his arguments were flawed. These gaps were filled by Niels Henrik Abel in 1824.{{harvp|Corry|2004|loc=p. 24}} Évariste Galois, in 1832, devised necessary and sufficient criteria for a polynomial equation to be algebraically solvable, thus establishing in effect what is known as Galois theory today. Both Abel and Galois worked with what is today called an algebraic number field, but conceived neither an explicit notion of a field, nor of a group.

In 1871 Richard Dedekind introduced, for a set of real or complex numbers that is closed under the four arithmetic operations, the German word Körper, which means "body" or "corpus" (to suggest an organically closed entity). The English term "field" was introduced by {{harvp|Moore|1893}}.{{cite web| url = http://jeff560.tripod.com/f.html| title = Earliest Known Uses of Some of the Words of Mathematics (F)}}

{{Blockquote|text=By a field we will mean every infinite system of real or complex numbers so closed in itself and perfect that addition, subtraction, multiplication, and division of any two of these numbers again yields a number of the system.

|author=Richard Dedekind, 1871{{harvp|Dirichlet|1871|loc=p. 42}}, translation by {{harvp|Kleiner|2007|loc=p. 66}}}}

In 1881 Leopold Kronecker defined what he called a domain of rationality, which is a field of rational fractions in modern terms. Kronecker's notion did not cover the field of all algebraic numbers (which is a field in Dedekind's sense), but on the other hand was more abstract than Dedekind's in that it made no specific assumption on the nature of the elements of a field. Kronecker interpreted a field such as {{math|Q(π)}} abstractly as the rational function field {{math|Q(X)}}. Prior to this, examples of transcendental numbers were known since Joseph Liouville's work in 1844, until Charles Hermite (1873) and Ferdinand von Lindemann (1882) proved the transcendence of {{math|e}} and {{math|π}}, respectively.{{harvp|Bourbaki|1994|loc=p. 81}}

The first clear definition of an abstract field is due to {{harvp|Weber|1893}}.{{harvp|Corry|2004|loc=p. 33}}. See also {{harvp|Fricke|Weber|1924}}. In particular, Heinrich Martin Weber's notion included the field {{math|F_p}}. Giuseppe Veronese (1891) studied the field of formal power series, which led {{harvp|Hensel|1904}} to introduce the field of {{math|p}}-adic numbers. {{harvp|Steinitz|1910}} synthesized the knowledge of abstract field theory accumulated so far. He axiomatically studied the properties of fields and defined many important field-theoretic concepts. The majority of the theorems mentioned in the sections Galois theory, Constructing fields and Elementary notions can be found in Steinitz's work. {{harvp|Artin|Schreier|1927}} linked the notion of orderings in a field, and thus the area of analysis, to purely algebraic properties.{{harvp|Bourbaki|1994|loc=p. 92}} Emil Artin redeveloped Galois theory from 1928 through 1942, eliminating the dependency on the primitive element theorem.

A commutative ring is a set that is equipped with an addition and multiplication operation and satisfies all the axioms of a field, except for the existence of multiplicative inverses {{math|a⁻¹}}.{{harvp|Lang|2002|loc=§II.1}} For example, the integers {{math|Z}} form a commutative ring, but not a field: the reciprocal of an integer {{math|n}} is not itself an integer, unless {{math|1=n = ±1}}.

In the hierarchy of algebraic structures fields can be characterized as the commutative rings {{math|R}} in which every nonzero element is a unit (which means every element is invertible). Similarly, fields are the commutative rings with precisely two distinct ideals, {{math|(0)}} and {{math|R}}. Fields are also precisely the commutative rings in which {{math|(0)}} is the only prime ideal.

Given a commutative ring {{math|R}}, there are two ways to construct a field related to {{math|R}}, i.e., two ways of modifying {{math|R}} such that all nonzero elements become invertible: forming the field of fractions, and forming residue fields. The field of fractions of {{math|Z}} is {{math|Q}}, the rationals, while the residue fields of {{math|Z}} are the finite fields {{math|F_p}}.

Given an integral domain {{math|R}}, its field of fractions {{math|Q(R)}} is built with the fractions of two elements of {{math|R}} exactly as Q is constructed from the integers. More precisely, the elements of {{math|Q(R)}} are the fractions {{math|a/b}} where {{math|a}} and {{math|b}} are in {{math|R}}, and {{math|b ≠ 0}}. Two fractions {{math|a/b}} and {{math|c/d}} are equal if and only if {{math|1=ad = bc}}. The operation on the fractions work exactly as for rational numbers. For example,

: $\backslash frac\{a\}\{b\}+\backslash frac\{c\}\{d\}\; =\; \backslash frac\{ad+bc\}\{bd\}.$

It is straightforward to show that, if the ring is an integral domain, the set of the fractions form a field.{{harvp|Artin|1991|loc=§10.6}}

The field {{math|F(x)}} of the rational fractions over a field (or an integral domain) {{math|F}} is the field of fractions of the polynomial ring {{math|F[x]}}. The field {{math|F((x))}} of Laurent series

: $\backslash sum\_\{i=k\}^\backslash infty\; a\_i\; x^i\; \backslash \; (k\; \backslash in\; \backslash Z,\; a\_i\; \backslash in\; F)$

over a field {{math|F}} is the field of fractions of the ring {{math|Fx}} of formal power series (in which {{math|k ≥ 0}}). Since any Laurent series is a fraction of a power series divided by a power of {{math|x}} (as opposed to an arbitrary power series), the representation of fractions is less important in this situation, though.

In addition to the field of fractions, which embeds {{math|R}} injectively into a field, a field can be obtained from a commutative ring {{math|R}} by means of a surjective map onto a field {{math|F}}. Any field obtained in this way is a quotient {{math|{{nowrap|R / m}}}}, where {{math|m}} is a maximal ideal of {{math|R}}. If {{math|R}} has only one maximal ideal {{math|m}}, this field is called the residue field of {{math|R}}.{{harvp|Eisenbud|1995|loc=p. 60}}

The ideal generated by a single polynomial {{math|f}} in the polynomial ring {{math|1=R = E[X]}} (over a field {{math|E}}) is maximal if and only if {{math|f}} is irreducible in {{math|E}}, i.e., if {{math|f}} cannot be expressed as the product of two polynomials in {{math|E[X]}} of smaller degree. This yields a field

: {{math|1=F = E[X] / ({{itco|f}}(X)).}}

This field {{math|F}} contains an element {{math|x}} (namely the residue class of {{math|X}}) which satisfies the equation

: {{math|1={{itco|f}}(x) = 0}}.

For example, {{math|C}} is obtained from {{math|R}} by adjoining the imaginary unit symbol {{mvar|i}}, which satisfies {{math|1={{itco|f}}(i) = 0}}, where {{math|1={{itco|f}}(X) = X² + 1}}. Moreover, {{math|f}} is irreducible over {{math|R}}, which implies that the map that sends a polynomial {{math|{{itco|f}}(X) ∊ R[X]}} to {{math|{{itco|f}}(i)}} yields an isomorphism

: $\backslash mathbf\; R[X]/\backslash left(X^2\; +\; 1\backslash right)\; \backslash \; \backslash stackrel\; \backslash cong\; \backslash longrightarrow\; \backslash \; \backslash mathbf\; C.$

Fields can be constructed inside a given bigger container field. Suppose given a field {{math|E}}, and a field {{math|F}} containing {{math|E}} as a subfield. For any element {{math|x}} of {{math|F}}, there is a smallest subfield of {{math|F}} containing {{math|E}} and {{math|x}}, called the subfield of F generated by {{math|x}} and denoted {{math|E(x)}}.{{harvp|Jacobson|2009|loc=p. 213}} The passage from {{math|E}} to {{math|E(x)}} is referred to by adjoining an element to {{math|E}}. More generally, for a subset {{math|S ⊂ F}}, there is a minimal subfield of {{math|F}} containing {{math|E}} and {{math|S}}, denoted by {{math|E(S)}}.

The compositum of two subfields {{math|E}} and {{math|E{{′}}}} of some field {{math|F}} is the smallest subfield of {{math|F}} containing both {{math|E}} and {{math|E{{′}}}}. The compositum can be used to construct the biggest subfield of {{math|F}} satisfying a certain property, for example the biggest subfield of {{math|F}}, which is, in the language introduced below, algebraic over {{math|E}}.{{efn|Further examples include the maximal unramified extension or the maximal abelian extension within {{math|F}}.}}

{{See|Glossary of field theory}}

The notion of a subfield {{math|E ⊂ F}} can also be regarded from the opposite point of view, by referring to {{math|F}} being a field extension (or just extension) of {{math|E}}, denoted by

: {{math|F / E}},

and read "{{math|F}} over {{math|E}}".

A basic datum of a field extension is its degree {{math|[F : E]}}, i.e., the dimension of {{math|F}} as an {{math|E}}-vector space. It satisfies the formula{{harvp|Artin|1991|loc=Theorem 13.3.4}}

: {{math|1=[G : E] = [G : F] [F : E]}}.

Extensions whose degree is finite are referred to as finite extensions. The extensions {{math|C / R}} and {{math|F₄ / F₂}} are of degree {{math|2}}, whereas {{math|R / Q}} is an infinite extension.

A pivotal notion in the study of field extensions {{math|F / E}} are algebraic elements. An element {{math|x ∈ F}} is algebraic over {{mvar|E}} if it is a root of a polynomial with coefficients in {{mvar|E}}, that is, if it satisfies a polynomial equation

: {{math|1=e_n xⁿ + e_n−1xⁿ⁻¹ + ⋯ + e₁x + e₀ = 0}},

with {{math|e_n, ..., e₀}} in {{mvar|E}}, and {{math|e_n ≠ 0}}.

For example, the imaginary unit {{math|i}} in {{math|C}} is algebraic over {{math|R}}, and even over {{math|Q}}, since it satisfies the equation

: {{math|1=i² + 1 = 0}}.

A field extension in which every element of {{math|F}} is algebraic over {{math|E}} is called an algebraic extension. Any finite extension is necessarily algebraic, as can be deduced from the above multiplicativity formula.{{harvp|Artin|1991|loc=Corollary 13.3.6}}

The subfield {{math|E(x)}} generated by an element {{math|x}}, as above, is an algebraic extension of {{math|E}} if and only if {{math|x}} is an algebraic element. That is to say, if {{math|x}} is algebraic, all other elements of {{math|E(x)}} are necessarily algebraic as well. Moreover, the degree of the extension {{math|E(x) / E}}, i.e., the dimension of {{math|E(x)}} as an {{math|E}}-vector space, equals the minimal degree {{math|n}} such that there is a polynomial equation involving {{math|x}}, as above. If this degree is {{math|n}}, then the elements of {{math|E(x)}} have the form

: $\backslash sum\_\{k=0\}^\{n-1\}\; a\_k\; x^k,\; \backslash \; \backslash \; a\_k\; \backslash in\; E.$

For example, the field {{math|Q(i)}} of Gaussian rationals is the subfield of {{math|C}} consisting of all numbers of the form {{math|a + bi}} where both {{math|a}} and {{math|b}} are rational numbers: summands of the form {{math|i²}} (and similarly for higher exponents) do not have to be considered here, since {{math|a + bi + ci²}} can be simplified to {{math|a − c + bi}}.

The above-mentioned field of rational fractions {{math|E(X)}}, where {{math|X}} is an indeterminate, is not an algebraic extension of {{math|E}} since there is no polynomial equation with coefficients in {{math|E}} whose zero is {{math|X}}. Elements, such as {{math|X}}, which are not algebraic are called transcendental. Informally speaking, the indeterminate {{math|X}} and its powers do not interact with elements of {{math|E}}. A similar construction can be carried out with a set of indeterminates, instead of just one.

Once again, the field extension {{math|E(x) / E}} discussed above is a key example: if {{math|x}} is not algebraic (i.e., {{math|x}} is not a root of a polynomial with coefficients in {{math|E}}), then {{math|E(x)}} is isomorphic to {{math|E(X)}}. This isomorphism is obtained by substituting {{math|x}} to {{math|X}} in rational fractions.

A subset {{math|S}} of a field {{math|F}} is a transcendence basis if it is algebraically independent (do not satisfy any polynomial relations) over {{math|E}} and if {{math|F}} is an algebraic extension of {{math|E(S)}}. Any field extension {{math|F / E}} has a transcendence basis.{{harvp|Bourbaki|1988|loc=Chapter V, §14, No. 2, Theorem 1}} Thus, field extensions can be split into ones of the form {{math|E(S) / E}} (purely transcendental extensions) and algebraic extensions.

A field is algebraically closed if it does not have any strictly bigger algebraic extensions or, equivalently, if any polynomial equation

: {{math|1=f_n xⁿ + f_n−1xⁿ⁻¹ + ⋯ + f₁x + f₀ = 0}}, with coefficients {{math|f_n, ..., f₀ ∈ F, n > 0}},

has a solution {{math|x ∊ F}}.{{harvp|Artin|1991|loc=§13.9}} By the fundamental theorem of algebra, {{math|C}} is algebraically closed, i.e., any polynomial equation with complex coefficients has a complex solution. The rational and the real numbers are not algebraically closed since the equation

: {{math|1=x² + 1 = 0}}

does not have any rational or real solution. A field containing {{math|F}} is called an algebraic closure of {{math|F}} if it is algebraic over {{math|F}} (roughly speaking, not too big compared to {{math|F}}) and is algebraically closed (big enough to contain solutions of all polynomial equations).

By the above, {{math|C}} is an algebraic closure of {{math|R}}. The situation that the algebraic closure is a finite extension of the field {{math|F}} is quite special: by the Artin–Schreier theorem, the degree of this extension is necessarily {{math|2}}, and {{math|F}} is elementarily equivalent to {{math|R}}. Such fields are also known as real closed fields.

Any field {{math|F}} has an algebraic closure, which is moreover unique up to (non-unique) isomorphism. It is commonly referred to as the algebraic closure and denoted {{math|{{overline|F}}}}. For example, the algebraic closure {{math|{{Overline|Q}}}} of {{math|Q}} is called the field of algebraic numbers. The field {{math|{{overline|F}}}} is usually rather implicit since its construction requires the ultrafilter lemma, a set-theoretic axiom that is weaker than the axiom of choice.{{harvp|Banaschewski|1992}}. [https://mathoverflow.net/questions/46566/is-the-statement-that-every-field-has-an-algebraic-closure-known-to-be-equivalent Mathoverflow post] In this regard, the algebraic closure of {{math|F_q}}, is exceptionally simple. It is the union of the finite fields containing {{math|F_q}} (the ones of order {{math|qⁿ}}). For any algebraically closed field {{math|F}} of characteristic {{math|0}}, the algebraic closure of the field {{math|F((t))}} of Laurent series is the field of Puiseux series, obtained by adjoining roots of {{math|t}}.{{harvp|Ribenboim|1999|loc=p. 186, §7.1}}

Since fields are ubiquitous in mathematics and beyond, several refinements of the concept have been adapted to the needs of particular mathematical areas.

{{Main|Ordered field}}

A field F is called an ordered field if any two elements can be compared, so that {{math|x + y ≥ 0}} and {{math|xy ≥ 0}} whenever {{math|x ≥ 0}} and {{math|y ≥ 0}}. For example, the real numbers form an ordered field, with the usual ordering {{math|≥}}. The Artin–Schreier theorem states that a field can be ordered if and only if it is a formally real field, which means that any quadratic equation

: $x\_1^2\; +\; x\_2^2\; +\; \backslash dots\; +\; x\_n^2\; =\; 0$

only has the solution {{math|1=x₁ = x₂ = ⋯ = x_n = 0}}.{{harvp|Bourbaki|1988|loc=Chapter VI, §2.3, Corollary 1}} The set of all possible orders on a fixed field {{math|F}} is isomorphic to the set of ring homomorphisms from the Witt ring {{math|W(F)}} of quadratic forms over {{math|F}}, to {{math|Z}}.{{harvp|Lorenz|2008|loc=§22, Theorem 1}}

An Archimedean field is an ordered field such that for each element there exists a finite expression

: {{math|1 + 1 + ⋯ + 1}}

whose value is greater than that element, that is, there are no infinite elements. Equivalently, the field contains no infinitesimals (elements smaller than all rational numbers); or, yet equivalent, the field is isomorphic to a subfield of {{math|R}}.

File:Illustration of supremum.svg

An ordered field is Dedekind-complete if all upper bounds, lower bounds (see Dedekind cut) and limits, which should exist, do exist. More formally, each bounded subset of {{math|F}} is required to have a least upper bound. Any complete field is necessarily Archimedean,{{harvp|Prestel|1984|loc=Proposition 1.22}} since in any non-Archimedean field there is neither a greatest infinitesimal nor a least positive rational, whence the sequence {{math|1/2, 1/3, 1/4, ...}}, every element of which is greater than every infinitesimal, has no limit.

Since every proper subfield of the reals also contains such gaps, {{math|R}} is the unique complete ordered field, up to isomorphism.{{harvp|Prestel|1984|loc=Theorem 1.23}} Several foundational results in calculus follow directly from this characterization of the reals.

The hyperreals {{math|R^*}} form an ordered field that is not Archimedean. It is an extension of the reals obtained by including infinite and infinitesimal numbers. These are larger, respectively smaller than any real number. The hyperreals form the foundational basis of non-standard analysis.

Another refinement of the notion of a field is a topological field, in which the set {{math|F}} is a topological space, such that all operations of the field (addition, multiplication, the maps {{math|a ↦ −a}} and {{math|a ↦ a⁻¹}}) are continuous maps with respect to the topology of the space.{{harvp|Warner|1989|loc=Chapter 14}}

The topology of all the fields discussed below is induced from a metric, i.e., a function

: {{math|d : F × F → R,}}

that measures a distance between any two elements of {{math|F}}.

The completion of {{math|F}} is another field in which, informally speaking, the "gaps" in the original field {{math|F}} are filled, if there are any. For example, any irrational number {{math|x}}, such as {{math|1=x = {{radic|2}}}}, is a "gap" in the rationals {{math|Q}} in the sense that it is a real number that can be approximated arbitrarily closely by rational numbers {{math|p/q}}, in the sense that distance of {{math|x}} and {{math|p/q}} given by the absolute value {{math|{{abs|x − p/q}}}} is as small as desired.

The following table lists some examples of this construction. The fourth column shows an example of a zero sequence, i.e., a sequence whose limit (for {{math|n → ∞}}) is zero.

The field {{math|Q_p}} is used in number theory and p-adic analysis. The algebraic closure {{math|{{overline|Q}}_p}} carries a unique norm extending the one on {{math|Q_p}}, but is not complete. The completion of this algebraic closure, however, is algebraically closed. Because of its rough analogy to the complex numbers, it is sometimes called the field of complex p-adic numbers and is denoted by {{math|C_p}}.{{harvp|Gouvêa|1997|loc=§5.7}}

The following topological fields are called local fields:{{harvp|Serre|1979}}{{efn|Some authors also consider the fields {{math|R}} and {{math|C}} to be local fields. On the other hand, these two fields, also called Archimedean local fields, share little similarity with the local fields considered here, to a point that {{harvtxt|Cassels|1986|loc=p. vi}} calls them "completely anomalous".}}

• finite extensions of {{math|Q_p}} (local fields of characteristic zero)
• finite extensions of {{math|F_p((t))}}, the field of Laurent series over {{math|F_p}} (local fields of characteristic {{math|p}}).

These two types of local fields share some fundamental similarities. In this relation, the elements {{math|p ∈ Q_p}} and {{math|t ∈ F_p((t))}} (referred to as uniformizer) correspond to each other. The first manifestation of this is at an elementary level: the elements of both fields can be expressed as power series in the uniformizer, with coefficients in {{math|F_p}}. (However, since the addition in {{math|Q_p}} is done using carrying, which is not the case in {{math|F_p((t))}}, these fields are not isomorphic.) The following facts show that this superficial similarity goes much deeper:

• Any first-order statement that is true for almost all {{math|Q_p}} is also true for almost all {{math|F_p((t))}}. An application of this is the Ax–Kochen theorem describing zeros of homogeneous polynomials in {{math|Q_p}}.
• Tamely ramified extensions of both fields are in bijection to one another.
• Adjoining arbitrary {{math|p}}-power roots of {{math|p}} (in {{math|Q_p}}), respectively of {{math|t}} (in {{math|F_p((t))}}), yields (infinite) extensions of these fields known as perfectoid fields. Strikingly, the Galois groups of these two fields are isomorphic, which is the first glimpse of a remarkable parallel between these two fields:{{harvp|Scholze|2014}} $$\backslash operatorname\; \{Gal\}\backslash left(\backslash mathbf\; Q\_p\; \backslash left(p^\{1/p^\backslash infty\}\; \backslash right)\; \backslash right)\; \backslash cong\; \backslash operatorname\; \{Gal\}\backslash left(\backslash mathbf\; F\_p((t))\backslash left(t^\{1/p^\backslash infty\}\backslash right)\backslash right).$$

Differential fields are fields equipped with a derivation, i.e., allow to take derivatives of elements in the field.{{harvp|van der Put|Singer|2003|loc=§1}} For example, the field {{math|R(X)}}, together with the standard derivative of polynomials forms a differential field. These fields are central to differential Galois theory, a variant of Galois theory dealing with linear differential equations.

{{Main|Galois theory}}

Galois theory studies algebraic extensions of a field by studying the symmetry in the arithmetic operations of addition and multiplication. An important notion in this area is that of finite Galois extensions {{math|F / E}}, which are, by definition, those that are separable and normal. The primitive element theorem shows that finite separable extensions are necessarily simple, i.e., of the form

: {{math|1=F = E[X] / {{itco|f}}(X)}},

where {{math|f}} is an irreducible polynomial (as above).{{harvp|Lang|2002|loc=Theorem V.4.6}} For such an extension, being normal and separable means that all zeros of {{math|f}} are contained in {{math|F}} and that {{math|f}} has only simple zeros. The latter condition is always satisfied if {{math|E}} has characteristic {{math|0}}.

For a finite Galois extension, the Galois group {{math|Gal(F/E)}} is the group of field automorphisms of {{math|F}} that are trivial on {{math|E}} (i.e., the bijections {{math|σ : F → F}} that preserve addition and multiplication and that send elements of {{math|E}} to themselves). The importance of this group stems from the fundamental theorem of Galois theory, which constructs an explicit one-to-one correspondence between the set of subgroups of {{math|Gal(F/E)}} and the set of intermediate extensions of the extension {{math|F/E}}.{{harvp|Lang|2002|loc=§VI.1}} By means of this correspondence, group-theoretic properties translate into facts about fields. For example, if the Galois group of a Galois extension as above is not solvable (cannot be built from abelian groups), then the zeros of {{math|f}} cannot be expressed in terms of addition, multiplication, and radicals, i.e., expressions involving $\backslash sqrt[n]\{~\}$. For example, the symmetric groups {{math|S_n}} is not solvable for {{math|n ≥ 5}}. Consequently, as can be shown, the zeros of the following polynomials are not expressible by sums, products, and radicals. For the latter polynomial, this fact is known as the Abel–Ruffini theorem:

: {{math|1=f(X) = X⁵ − 4X + 2}} (and {{math|1=E = Q}}),{{harvp|Lang|2002|loc=Example VI.2.6}}

: {{math|1=f(X) = {{itco|X}}ⁿ + a_n−1{{itco|X}}ⁿ⁻¹ + ⋯ + a₀}} (where {{math|f}} is regarded as a polynomial in {{math|E(a₀, ..., a_n−1)}}, for some indeterminates {{math|a_i}}, {{math|E}} is any field, and {{math|n ≥ 5}}).

The tensor product of fields is not usually a field. For example, a finite extension {{math|F / E}} of degree {{math|n}} is a Galois extension if and only if there is an isomorphism of {{math|F}}-algebras

: {{math|F ⊗_E F ≅ Fⁿ}}.

This fact is the beginning of Grothendieck's Galois theory, a far-reaching extension of Galois theory applicable to algebro-geometric objects.{{harvp|Borceux|Janelidze|2001}}. See also Étale fundamental group.

Basic invariants of a field {{math|F}} include the characteristic and the transcendence degree of {{math|F}} over its prime field. The latter is defined as the maximal number of elements in {{math|F}} that are algebraically independent over the prime field. Two algebraically closed fields {{math|E}} and {{math|F}} are isomorphic precisely if these two data agree.{{harvp|Gouvêa|2012|loc=Theorem 6.4.8}} This implies that any two uncountable algebraically closed fields of the same cardinality and the same characteristic are isomorphic. For example, {{math|{{overline|Q}}_p, C_p}} and {{math|C}} are isomorphic (but not isomorphic as topological fields).

In model theory, a branch of mathematical logic, two fields {{math|E}} and {{math|F}} are called elementarily equivalent if every mathematical statement that is true for {{math|E}} is also true for {{math|F}} and conversely. The mathematical statements in question are required to be first-order sentences (involving {{math|0}}, {{math|1}}, the addition and multiplication). A typical example, for {{math|n > 0}}, {{math|n}} an integer, is

: {{math|φ(E)}} = "any polynomial of degree {{math|n}} in {{math|E}} has a zero in {{math|E}}"

The set of such formulas for all {{math|n}} expresses that {{math|E}} is algebraically closed.

The Lefschetz principle states that {{math|C}} is elementarily equivalent to any algebraically closed field {{math|F}} of characteristic zero. Moreover, any fixed statement {{math|φ}} holds in {{math|C}} if and only if it holds in any algebraically closed field of sufficiently high characteristic.{{harvp|Marker|Messmer|Pillay|2006|loc=Corollary 1.2}}

If {{math|U}} is an ultrafilter on a set {{math|I}}, and {{math|F_i}} is a field for every {{math|i}} in {{math|I}}, the ultraproduct of the {{math|F_i}} with respect to {{math|U}} is a field.{{harvp|Schoutens|2002|loc=§2}} It is denoted by

: {{math|ulim_i→∞ F_i}},

since it behaves in several ways as a limit of the fields {{math|F_i}}: Łoś's theorem states that any first order statement that holds for all but finitely many {{math|F_i}}, also holds for the ultraproduct. Applied to the above sentence {{math|φ}}, this shows that there is an isomorphism{{efn|Both {{math|C}} and {{math|ulim_p {{overline|F}}_p}} are algebraically closed by Łoś's theorem. For the same reason, they both have characteristic zero. Finally, they are both uncountable, so that they are isomorphic.}}

: $\backslash operatorname\{ulim\}\_\{p\; \backslash to\; \backslash infty\}\; \backslash overline\; \backslash mathbf\; F\_p\; \backslash cong\; \backslash mathbf\; C.$

The Ax–Kochen theorem mentioned above also follows from this and an isomorphism of the ultraproducts (in both cases over all primes {{math|p}})

: {{math|ulim_p Q_p ≅ ulim_p F_p((t))}}.

In addition, model theory also studies the logical properties of various other types of fields, such as real closed fields or exponential fields (which are equipped with an exponential function {{math|exp : F → F^×}}).{{harvp|Kuhlmann|2000}}

For fields that are not algebraically closed (or not separably closed), the absolute Galois group {{math|Gal(F)}} is fundamentally important: extending the case of finite Galois extensions outlined above, this group governs all finite separable extensions of {{math|F}}. By elementary means, the group {{math|Gal(F_q)}} can be shown to be the Prüfer group, the profinite completion of {{math|Z}}. This statement subsumes the fact that the only algebraic extensions of {{math|Gal(F_q)}} are the fields {{math|Gal(F_qⁿ)}} for {{math|n > 0}}, and that the Galois groups of these finite extensions are given by

: {{math|1=Gal(F_qⁿ / F_q) = Z/nZ}}.

A description in terms of generators and relations is also known for the Galois groups of {{math|p}}-adic number fields (finite extensions of {{math|Q_p}}).{{harvp|Jannsen|Wingberg|1982}}

Representations of Galois groups and of related groups such as the Weil group are fundamental in many branches of arithmetic, such as the Langlands program. The cohomological study of such representations is done using Galois cohomology.{{harvp|Serre|2002}} For example, the Brauer group, which is classically defined as the group of central simple algebra, can be reinterpreted as a Galois cohomology group, namely

: {{math|1=Br(F) = H²(F, G_m)}}.

Milnor K-theory is defined as

: $K\_n^M(F)\; =\; F^\backslash times\; \backslash otimes\; \backslash cdots\; \backslash otimes\; F^\backslash times\; /\; \backslash left\backslash langle\; x\; \backslash otimes\; (1-x)\; \backslash mid\; x\; \backslash in\; F\; \backslash smallsetminus\; \backslash \{0,\; 1\backslash \}\; \backslash right\backslash rangle.$

The norm residue isomorphism theorem, proved around 2000 by Vladimir Voevodsky, relates this to Galois cohomology by means of an isomorphism

: $K\_n^M(F)\; /\; p\; =\; H^n(F,\; \backslash mu\_l^\{\backslash otimes\; n\}).$

Algebraic K-theory is related to the group of invertible matrices with coefficients the given field. For example, the process of taking the determinant of an invertible matrix leads to an isomorphism {{math|1=K₁(F) = F^×}}. Matsumoto's theorem shows that {{math|K₂(F)}} agrees with {{math|K₂^M(F)}}. In higher degrees, K-theory diverges from Milnor K-theory and remains hard to compute in general.

If {{math|a ≠ 0}}, then the equation

: {{math|1=ax = b}}

has a unique solution {{math|x}} in a field {{math|F}}, namely $x=a^\{-1\}b.$ This immediate consequence of the definition of a field is fundamental in linear algebra. For example, it is an essential ingredient of Gaussian elimination and of the proof that any vector space has a basis.{{harvp|Artin|1991|loc=§3.3}}

The theory of modules (the analogue of vector spaces over rings instead of fields) is much more complicated, because the above equation may have several or no solutions. In particular systems of linear equations over a ring are much more difficult to solve than in the case of fields, even in the specially simple case of the ring {{math|Z}} of the integers.

File:ECClines.svg

A widely applied cryptographic routine uses the fact that discrete exponentiation, i.e., computing

: {{math|1=aⁿ = a ⋅ a ⋅ ⋯ ⋅ a}} ({{math|n}} factors, for an integer {{math|n ≥ 1}})

in a (large) finite field {{math|F_q}} can be performed much more efficiently than the discrete logarithm, which is the inverse operation, i.e., determining the solution {{math|n}} to an equation

: {{math|1=aⁿ = b}}.

In elliptic curve cryptography, the multiplication in a finite field is replaced by the operation of adding points on an elliptic curve, i.e., the solutions of an equation of the form

: {{math|1=y² = x³ + ax + b}}.

Finite fields are also used in coding theory and combinatorics.

File:Double torus illustration.png two (two handles). The genus can be read off the field of meromorphic functions on the surface.]]

Functions on a suitable topological space {{math|X}} into a field {{mvar|F}} can be added and multiplied pointwise, e.g., the product of two functions is defined by the product of their values within the domain:

: {{math|1={{nowrap|1=(f ⋅ g)(x) = f(x) ⋅ g(x)}}}}.

This makes these functions a {{math|F}}-commutative algebra.

For having a field of functions, one must consider algebras of functions that are integral domains. In this case the ratios of two functions, i.e., expressions of the form

: $\backslash frac\{f(x)\}\{g(x)\},$

form a field, called field of functions.

This occurs in two main cases. When {{math|X}} is a complex manifold {{math|X}}. In this case, one considers the algebra of holomorphic functions, i.e., complex differentiable functions. Their ratios form the field of meromorphic functions on {{math|X}}.

The function field of an algebraic variety {{math|X}} (a geometric object defined as the common zeros of polynomial equations) consists of ratios of regular functions, i.e., ratios of polynomial functions on the variety. The function field of the {{math|n}}-dimensional space over a field {{math|F}} is {{math|F(x₁, ..., x_n)}}, i.e., the field consisting of ratios of polynomials in {{math|n}} indeterminates. The function field of {{math|X}} is the same as the one of any open dense subvariety. In other words, the function field is insensitive to replacing {{math|X}} by a (slightly) smaller subvariety.

The function field is invariant under isomorphism and birational equivalence of varieties. It is therefore an important tool for the study of abstract algebraic varieties and for the classification of algebraic varieties. For example, the dimension, which equals the transcendence degree of {{math|F(X)}}, is invariant under birational equivalence.{{harvp|Eisenbud|1995|loc=§13, Theorem A}} For curves (i.e., the dimension is one), the function field {{math|F(X)}} is very close to {{math|X}}: if {{math|X}} is smooth and proper (the analogue of being compact), {{math|X}} can be reconstructed, up to isomorphism, from its field of functions.{{efn|More precisely, there is an equivalence of categories between smooth proper algebraic curves over an algebraically closed field {{math|F}} and finite field extensions of {{math|F(T)}}.}} In higher dimension the function field remembers less, but still decisive information about {{math|X}}. The study of function fields and their geometric meaning in higher dimensions is referred to as birational geometry. The minimal model program attempts to identify the simplest (in a certain precise sense) algebraic varieties with a prescribed function field.

Global fields are in the limelight in algebraic number theory and arithmetic geometry.

They are, by definition, number fields (finite extensions of {{math|Q}}) or function fields over {{math|F_q}} (finite extensions of {{math|F_q(t)}}). As for local fields, these two types of fields share several similar features, even though they are of characteristic {{math|0}} and positive characteristic, respectively. This function field analogy can help to shape mathematical expectations, often first by understanding questions about function fields, and later treating the number field case. The latter is often more difficult. For example, the Riemann hypothesis concerning the zeros of the Riemann zeta function (open as of 2017) can be regarded as being parallel to the Weil conjectures (proven in 1974 by Pierre Deligne).

File:One5Root.svg.]]

Cyclotomic fields are among the most intensely studied number fields. They are of the form {{math|Q(ζ_n)}}, where {{math|ζ_n}} is a primitive {{math|n}}th root of unity, i.e., a complex number {{math|ζ}} that satisfies {{math|1={{itco|ζ}}ⁿ = 1}} and {{math|{{itco|ζ}}^m ≠ 1}} for all {{math|0 < m < n}}.{{harvp|Washington|1997}} For {{math|n}} being a regular prime, Kummer used cyclotomic fields to prove Fermat's Last Theorem, which asserts the non-existence of rational nonzero solutions to the equation

: {{math|1=xⁿ + yⁿ = zⁿ}}.

Local fields are completions of global fields. Ostrowski's theorem asserts that the only completions of {{math|Q}}, a global field, are the local fields {{math|Q_p}} and {{math|R}}. Studying arithmetic questions in global fields may sometimes be done by looking at the corresponding questions locally. This technique is called the local–global principle. For example, the Hasse–Minkowski theorem reduces the problem of finding rational solutions of quadratic equations to solving these equations in {{math|R}} and {{math|Q_p}}, whose solutions can easily be described.{{harvp|Serre|1996|loc=Chapter IV}}

Unlike for local fields, the Galois groups of global fields are not known. Inverse Galois theory studies the (unsolved) problem whether any finite group is the Galois group {{math|Gal(F/Q)}} for some number field {{math|F}}.{{harvp|Serre|1992}} Class field theory describes the abelian extensions, i.e., ones with abelian Galois group, or equivalently the abelianized Galois groups of global fields. A classical statement, the Kronecker–Weber theorem, describes the maximal abelian {{math|Q^ab}} extension of {{math|Q}}: it is the field

: {{math|Q(ζ_n, n ≥ 2)}}

obtained by adjoining all primitive {{math|n}}th roots of unity. Kronecker's Jugendtraum asks for a similarly explicit description of {{math|F^ab}} of general number fields {{math|F}}. For imaginary quadratic fields, $F=\backslash mathbf\; Q(\backslash sqrt\{-d\})$, {{math|d > 0}}, the theory of complex multiplication describes {{math|F^ab}} using elliptic curves. For general number fields, no such explicit description is known.

In addition to the additional structure that fields may enjoy, fields admit various other related notions. Since in any field {{math|0 ≠ 1}}, any field has at least two elements. Nonetheless, there is a concept of field with one element, which is suggested to be a limit of the finite fields {{math|F_p}}, as {{math|p}} tends to {{math|1}}.{{harvp|Tits|1957}} In addition to division rings, there are various other weaker algebraic structures related to fields such as quasifields, near-fields and semifields.

There are also proper classes with field structure, which are sometimes called Fields, with a capital 'F'. The surreal numbers form a Field containing the reals, and would be a field except for the fact that they are a proper class, not a set. The nimbers, a concept from game theory, form such a Field as well.{{harvp|Conway|1976}}

Dropping one or several axioms in the definition of a field leads to other algebraic structures. As was mentioned above, commutative rings satisfy all field axioms except for the existence of multiplicative inverses. Dropping instead commutativity of multiplication leads to the concept of a division ring or skew field;{{efn|Historically, division rings were sometimes referred to as fields, while fields were called commutative fields.}} sometimes associativity is weakened as well. The only division rings that are finite-dimensional {{math|R}}-vector spaces are {{math|R}} itself, {{math|C}} (which is a field), and the quaternions {{math|H}} (in which multiplication is non-commutative). This result is known as the Frobenius theorem. The octonions {{math|O}}, for which multiplication is neither commutative nor associative, is a normed alternative division algebra, but is not a division ring. This fact was proved using methods of algebraic topology in 1958 by Michel Kervaire, Raoul Bott, and John Milnor.{{harvp|Baez|2002}}

Wedderburn's little theorem states that all finite division rings are fields.

{{notelist}}

{{reflist|30em}}

{{refbegin|30em}}

• {{citation |title=Introduction to Field Theory| last=Adamson|first=I. T.|isbn=978-0-486-46266-0|year=2007|publisher=Dover Publications}}
• {{citation | last1=Allenby | first1=R. B. J. T. | title=Rings, Fields and Groups | publisher=Butterworth-Heinemann | isbn=978-0-340-54440-2 | year=1991}}
• {{citation | last1=Artin | first1=Michael | author1-link=Michael Artin | title=Algebra | publisher=Prentice Hall | isbn=978-0-13-004763-2 | year=1991}}, especially Chapter 13
• {{citation |last1=Artin|first1=Emil|last2=Schreier|first2=Otto|author1-link=Emil Artin|author2-link=Otto Schreier|title=Eine Kennzeichnung der reell abgeschlossenen Körper|journal=Abhandlungen aus dem Mathematischen Seminar der Universität Hamburg|issn=0025-5858| volume=5|pages=225–231|year=1927|language=de|doi=10.1007/BF02952522|jfm=53.0144.01|s2cid=121547404}}
• {{citation | last=Ax |first=James|author-link=James Ax|year=1968|title=The elementary theory of finite fields|journal=Ann. of Math. |series= 2|volume=88|issue=2|pages=239–271|doi=10.2307/1970573|jstor=1970573}}
• {{citation |last=Baez|first=John C.|author-link=John C. Baez|title=The octonions|journal=Bulletin of the American Mathematical Society |volume=39|issue=2|year=2002|pages=145–205|doi=10.1090/S0273-0979-01-00934-X|arxiv=math/0105155|s2cid=586512}}
• {{citation | last=Banaschewski|first=Bernhard|title=Algebraic closure without choice.|year=1992|journal=Z. Math. Logik Grundlagen Math.|volume=38|issue=4|pages=383–385|zbl=0739.03027|doi=10.1002/malq.19920380136}}
• {{citation |last1=Beachy|first1=John. A|last2=Blair|first2=William D.|title=Abstract Algebra|edition=3|publisher=Waveland Press|isbn=1-57766-443-4|year=2006}}
• {{citation | last1=Blyth | first1=T. S. | last2=Robertson | first2=E. F. |author2-link=Edmund F. Robertson| title=Groups, rings and fields: Algebra through practice| publisher=Cambridge University Press | year=1985}}. See especially Book 3 ({{ISBN|0-521-27288-2}}) and Book 6 ({{ISBN|0-521-27291-2}}).
• {{citation |last1=Borceux|first1=Francis|last2=Janelidze|first2=George|title=Galois theories|

isbn=0-521-80309-8|year=2001|publisher=Cambridge University Press|zbl=0978.12004}}

• {{citation |last1=Bourbaki|first1=Nicolas|author-link=Nicolas Bourbaki|title=Elements of the history of mathematics|publisher=Springer|year=1994|isbn=3-540-19376-6|mr=1290116|doi=10.1007/978-3-642-61693-8}}
• {{citation |title=Algebra II. Chapters 4–7|last=Bourbaki|first=Nicolas|author-link=Nicolas Bourbaki|isbn=0-387-19375-8|year=1988|publisher=Springer}}
• {{citation |last=Cassels|first=J. W. S.|author-link=J. W. S. Cassels|title=Local fields|series=London Mathematical Society Student Texts|volume=3|publisher=Cambridge University Press|year=1986|isbn=0-521-30484-9|mr=861410|doi=10.1017/CBO9781139171885}}
• {{citation |title=Elements of Abstract Algebra|last=Clark|first=A.|isbn=978-0-486-64725-8|series=Dover Books on Mathematics Series|year=1984|publisher=Dover |url=https://books.google.com/books?id=bj1kOY8gOfcC }}
• {{citation

|last1=Conway

|first1=John Horton

|year=1976

|author-link1=John Horton Conway

|title=On Numbers and Games

|publisher=Academic Press

|title-link=On Numbers and Games

}}

• {{citation |last=Corry|first=Leo|author-link=Leo Corry|title=Modern algebra and the rise of mathematical structures|edition=2nd|isbn=3-7643-7002-5|year=2004|publisher=Birkhäuser|zbl=1044.01008}}
• {{citation |last1=Dirichlet|first1=Peter Gustav Lejeune|author-link=Peter Gustav Lejeune Dirichlet|editor-last=Dedekind|editor-first=Richard|editor-link=Richard Dedekind|year=1871|edition=2nd|language=de|volume=1|location=Braunschweig, Germany|publisher=Friedrich Vieweg und Sohn|title=Vorlesungen über Zahlentheorie (Lectures on Number Theory)|url=https://books.google.com/books?id=SRJTAAAAcAAJ&pg=PA424}}
• {{citation | last=Eisenbud|first=David|author-link=David Eisenbud | title=Commutative algebra with a view toward algebraic geometry | location=New York | publisher=Springer-Verlag | series=Graduate Texts in Mathematics | volume=150 | year=1995 | mr=1322960 | isbn=0-387-94268-8 | doi=10.1007/978-1-4612-5350-1}}
• {{citation |last=Escofier|first=J. P.|isbn=978-1-4613-0191-2|title=Galois Theory|publisher=Springer|year=2012}}
• {{citation | last1 = Fraleigh | first1 = John B. | year = 1976 | isbn = 0-201-01984-1 | title = A First Course In Abstract Algebra | edition = 2nd | publisher = Addison-Wesley | location = Reading }}
• {{citation | last1= Fricke | first1= Robert|author1-link=Robert Fricke | last2= Weber | first2= Heinrich Martin | author2-link= Heinrich Martin Weber | title= Lehrbuch der Algebra | language=de|url= http://resolver.sub.uni-goettingen.de/purl?PPN234788267 | publisher= Vieweg | year= 1924 | jfm= 50.0042.03}}
• {{citation |title=p-adic numbers|

last=Gouvêa|first=Fernando Q.|author-link=Fernando Q. Gouvêa|edition=2nd|year=1997|publisher=Springer|series=Universitext}}

• {{citation |title=A Guide to Groups, Rings, and Fields|

last=Gouvêa|first=Fernando Q.|author-link=Fernando Q. Gouvêa|isbn=978-0-88385-355-9|year=2012|publisher=Mathematical Association of America}}

• {{springer|title=Field|id=p/f040090}}
• {{citation |last1=Hensel|first1=Kurt|author1-link=Kurt Hensel|title=Über eine neue Begründung der Theorie der algebraischen Zahlen|journal=Journal für die Reine und Angewandte Mathematik|

issn=0075-4102|volume=128|pages=1–32|year=1904|language=de|jfm=35.0227.01|url=https://eudml.org/doc/149187}}

• {{citation | last=Jacobson| first=Nathan| author-link=Nathan Jacobson| year=2009| title=Basic algebra| edition=2nd| volume = 1 | publisher=Dover| isbn = 978-0-486-47189-1}}
• {{citation |mr=0679774|first1=Uwe|last1=Jannsen|first2=Kay|last2=Wingberg|title=Die Struktur der absoluten Galoisgruppe 𝔭-adischer Zahlkörper. [The structure of the absolute Galois group of 𝔭-adic number fields]|journal=Invent. Math.|volume=70|year=1982|issue=1|pages=71–98|url=http://epub.uni-regensburg.de/26689/|doi=10.1007/bf01393199|bibcode=1982InMat..70...71J|s2cid=119378923}}
• {{citation |last=Kleiner|first=Israel|editor1-first=Israel|editor1-last=Kleiner|author-link=Israel Kleiner (mathematician)|title=A history of abstract algebra|publisher=Birkhäuser|year=2007|isbn=978-0-8176-4684-4|mr=2347309|doi=10.1007/978-0-8176-4685-1}}
• {{citation |last=Kiernan|first=B. Melvin|title=The development of Galois theory from Lagrange to Artin|journal=Archive for History of Exact Sciences

|volume=8|year=1971|number=1–2|pages=40–154|mr=1554154|doi=10.1007/BF00327219|s2cid=121442989}}

• {{citation |last1=Kuhlmann|first1=Salma|title=Ordered exponential fields|series=Fields Institute Monographs|volume=12|publisher=American Mathematical Society|year=2000|isbn=0-8218-0943-1|mr=1760173}}
• {{citation |first=Serge|last=Lang|author-link=Serge Lang|title=Algebra|series=Graduate Texts in Mathematics|volume=211|edition=3rd|publisher=Springer|year=2002|isbn=0-387-95385-X|doi=10.1007/978-1-4613-0041-0}}
• {{citation |first1=Rudolf|last1=Lidl|first2=Harald|last2=Niederreiter|author2-link=Harald Niederreiter|title=Finite fields| edition=2nd|year=2008|isbn=978-0-521-06567-2|publisher=Cambridge University Press|zbl=1139.11053}}
• {{citation |last=Lorenz|first=Falko|title=Algebra, Volume II: Fields with Structures, Algebras and Advanced Topics|year=2008|isbn=978-0-387-72487-4|publisher=Springer}}
• {{citation |last1=Marker|first1=David|last2=Messmer|first2=Margit|last3=Pillay|first3=Anand|title=Model theory of fields|series=Lecture Notes in Logic|volume=5|edition=2nd|publisher=Association for Symbolic Logic|year=2006|isbn=978-1-56881-282-3|mr=2215060|citeseerx=10.1.1.36.8448|url-access=registration|url=https://archive.org/details/modeltheoryoffie0000mark}}
• {{citation | last1 = McCoy | first1 = Neal H. | title = Introduction To Modern Algebra, Revised Edition | location = Boston | publisher = Allyn and Bacon | year = 1968 | lccn = 68015225 }}
• {{citation |last1=Mines|first1=Ray|last2=Richman|first2=Fred|last3=Ruitenburg|first3=Wim|title=A course in constructive algebra|series=Universitext|publisher=Springer|year=1988|isbn=0-387-96640-4|mr=919949|doi=10.1007/978-1-4419-8640-5}}
• {{citation

| last = Moore | first = E. Hastings | author-link = E. H. Moore

| year = 1893

| title = A doubly-infinite system of simple groups

| journal = Bulletin of the American Mathematical Society

| volume = 3

| issue = 3

| pages = 73–78

| mr = 1557275

| doi = 10.1090/S0002-9904-1893-00178-X

| doi-access = free

}}

• {{citation |last=Prestel|first=Alexander|title=Lectures on Formally Real Fields

|series=Lecture Notes in Mathematics |volume=1093|publisher=Springer|year=1984|isbn=3-540-13885-4|mr=769847|doi=10.1007/BFb0101548}}

• {{citation |last=Ribenboim|first=Paulo|author-link=Paulo Ribenboim|title=The theory of classical valuations|series=Springer Monographs in Mathematics|publisher=Springer|year=1999|isbn=0-387-98525-5|mr=1677964| doi=10.1007/978-1-4612-0551-7}}
• {{citation |last=Scholze|first=Peter|author-link=Peter Scholze|chapter=Perfectoid spaces and their Applications|year=2014|chapter-url=http://www.math.uni-bonn.de/people/scholze/ICM.pdf|title=Proceedings of the International Congress of Mathematicians 2014|publisher=Kyung Moon SA |url=http://www.icm2014.org/en/vod/proceedings.html|isbn=978-89-6105-804-9}}
• {{citation |last=Schoutens|first=Hans|isbn=978-3-642-13367-1|title=The Use of Ultraproducts in Commutative Algebra|year=2002|publisher=Springer|series=Lecture Notes in Mathematics|volume=1999}}
• {{citation |last=Serre|first=Jean-Pierre|author-link=Jean-Pierre Serre|title=A course in arithmetic. Translation of Cours d'arithmetique|edition=2nd|orig-year=1978|series=Graduate Text in Mathematics|volume=7|publisher=Springer|zbl=0432.10001|isbn=9780387900407|year=1996|url-access=registration|url=https://archive.org/details/courseinarithmet00serr}}
• {{citation|last=Serre|first=Jean-Pierre|author-link=Jean-Pierre Serre|title=Local fields|series=Graduate Texts in Mathematics |volume=67|publisher=Springer|year=1979|isbn=0-387-90424-7|mr=554237}}
• {{citation|first=Jean-Pierre|last=Serre|author-link=Jean-Pierre Serre|title=Topics in Galois theory|isbn=0-86720-210-6|year=1992|publisher=Jones and Bartlett Publishers|zbl=0746.12001}}
• {{citation | last1=Serre | first1=Jean-Pierre | author1-link= Jean-Pierre Serre | title=Galois cohomology | publisher=Springer-Verlag | location=Berlin, New York | series=Springer Monographs in Mathematics | isbn=978-3-540-42192-4 | mr=1867431 | year=2002 | zbl=1004.12003 | others=Translated from the French by Patrick Ion}}
• {{citation|last=Sharpe|first=David|title=Rings and factorization|isbn=0-521-33718-6|year=1987|publisher=Cambridge University Press|zbl=0674.13008|url-access=registration|url=https://archive.org/details/ringsfactorizati0000shar}}
• {{citation

| last1=Steinitz | first1=Ernst | author1-link=Ernst Steinitz

| year=1910

| title=Algebraische Theorie der Körper |trans-title=Algebraic Theory of Fields

| url=http://resolver.sub.uni-goettingen.de/purl?GDZPPN002167042

| journal=Journal für die reine und angewandte Mathematik

| volume=1910 | issue=137 | pages=167–309

| issn=0075-4102 | jfm=41.0445.03 | doi=10.1515/crll.1910.137.167

| s2cid=120807300

}}

• {{citation | last1 = Tits | first1 = Jacques | author-link=Jacques Tits | chapter = Sur les analogues algébriques des groupes semi-simples complexes | title = Colloque d'algèbre supérieure, tenu à Bruxelles du 19 au 22 décembre 1956, Centre Belge de Recherches Mathématiques Établissements Ceuterick, Louvain | publisher = Librairie Gauthier-Villars | place = Paris | year = 1957 | pages = 261–289 }}
• {{citation |title=Galois Theory of Linear Differential Equations|first1=M.|last1=van der Put|first2=M. F.|last2=Singer|year=2003|publisher=Springer|series=Grundlehren der mathematischen Wissenschaften|volume=328|url=http://www4.ncsu.edu/~singer/papers/dbook2.ps}}
• {{citation | last=von Staudt|first=Karl Georg Christian|author-link=Karl Georg Christian von Staudt |url=https://books.google.com/books?id=XwEHAAAAcAAJ&pg=PA127|title=Beiträge zur Geometrie der Lage (Contributions to the Geometry of Position)|volume=2|location=Nürnberg (Germany)|publisher=Bauer and Raspe|year=1857}}
• {{citation |last=Wallace|first=D. A. R.|year=1998|title=Groups, Rings, and Fields|series=SUMS|publisher=Springer|volume=151}}
• {{citation |first=Seth|last=Warner|title=Topological fields|isbn=0-444-87429-1|year=1989|publisher=North-Holland|zbl=0683.12014}}
• {{citation |first=Lawrence C.|last= Washington|author-link=Lawrence C. Washington|title=Introduction to Cyclotomic Fields|series=Graduate Texts in Mathematics|volume= 83|publisher=Springer-Verlag |year= 1997|edition=2nd |isbn=0-387-94762-0 |mr=1421575|doi=10.1007/978-1-4612-1934-7}}
• {{citation |last=Weber |first=Heinrich |author-link= Heinrich Martin Weber |title=Die allgemeinen Grundlagen der Galois'schen Gleichungstheorie |journal=Mathematische Annalen |issn=0025-5831 |volume=43 |issue=4 |pages=521–549 |year=1893 |language=de |doi=10.1007/BF01446451 |jfm=25.0137.01 |s2cid=120528969 |url=https://eudml.org/doc/157689 }}

{{refend}}

{{Wikibooks|Abstract algebra|Fields}}

{{DEFAULTSORT:Field (Mathematics)}}

Category:Algebraic structures

Category:Abstract algebra