In [[mathematics]], and more specifically in [[linear algebra]], a '''linear map''' (also called a '''linear mapping''', '''linear transformation''', '''vector space homomorphism''', or in some contexts '''linear function''') is a [[Map (mathematics)|mapping]] <math>V \to W</math> between two [[vector space]]s that preserves the operations of [[vector addition]] and [[scalar multiplication]]. The same names and the same definition are also used for the more general case of [[module (mathematics)|modules]] over a [[ring (mathematics)|ring]]; see [[Module homomorphism]].
In [[mathematics]], and more specifically in [[linear algebra]], a '''linear map''' (or '''linear mapping''') is a particular kind of [[function (mathematics)|function]] between [[vector space]]s, which respects the basic operations of [[vector addition]] and [[scalar multiplication]]. A standard example of a linear map is an <math>m\times n</math> matrix, which takes vectors in <math>n</math>-dimensions into vectors in <math>m</math>-dimensions in a way that is compatible with addition of vectors, and multiplication of vectors by [[Scalar (mathematics)|scalars]].
If a linear map is a [[bijection]] then it is called a '''{{visible anchor|Linear isomorphism|text=linear isomorphism}}'''. In the case where <math>V = W</math>, a linear map is called a '''linear endomorphism'''. Sometimes the term '''{{visible anchor|Linear operator|text=linear operator}}''' refers to this case,<ref>"Linear transformations of {{mvar|V}} into {{mvar|V}} are often called ''linear operators'' on {{mvar|V}}." {{harvnb|Rudin|1976|page=207}}</ref> but the term "linear operator" can have different meanings for different conventions: for example, it can be used to emphasize that <math>V</math> and <math>W</math> are [[Real number|real]] vector spaces (not necessarily with <math>V = W</math>),{{citation needed|date=November 2020}} or it can be used to emphasize that <math>V</math> is a [[function space]], which is a common convention in [[functional analysis]].<ref>Let {{mvar|V}} and {{mvar|W}} be two real vector spaces. A mapping a from {{mvar|V}} into {{mvar|W}} Is called a 'linear mapping' or 'linear transformation' or 'linear operator' [...] from {{mvar|V}} into {{mvar|W}}, if <br /> <math display="inline">a(\mathbf u + \mathbf v) = a \mathbf u + a \mathbf v</math> for all <math display="inline">\mathbf u,\mathbf v \in V</math>, <br /> <math display="inline"> a(\lambda \mathbf u) = \lambda a \mathbf u </math> for all <math>\mathbf u \in V</math> and all real {{mvar|λ}}. {{harvnb|Bronshtein|Semendyayev|2004|page=316}}</ref> Sometimes the term ''[[linear function]]'' has the same meaning as ''linear map'', while in [[mathematical analysis|analysis]] it does not.
A linear map is a [[homomorphism]] of vector spaces.<ref group="note">In the language of [[category theory]], linear maps are the [[morphism]]s of vector spaces. Restricted to the category of finite-dimensional vector spaces, they form a category [[equivalence of categories|equivalent]] to [[category of matrices|the one of matrices]].</ref> Thus, a linear map <math>T:V\to W</math> satisfies {{tmath|1= T(a x + b y) = a Tx + b Ty }}, where <math>a</math> and <math>b</math> are scalars, and <math>x</math> and <math>y</math> are vectors (elements of the vector space {{tmath|V}}). A linear mapping always maps the [[Origin (geometry)|origin]] of <math>V</math> to the origin of {{tmath|W}}, and [[linear subspace]]s of <math>V</math> onto linear subspaces in <math>W</math> (possibly of a lower [[Dimension (vector space)|dimension]]);<ref>{{harvnb|Rudin|1991|page=14}}<br />Here are some properties of linear mappings <math display="inline">\Lambda: X \to Y</math> whose proofs are so easy that we omit them; it is assumed that <math display="inline">A \subset X</math> and <math display="inline">B \subset Y</math>:
{{ordered list|<math display="inline">\Lambda 0 = 0.</math>|If {{mvar|A}} is a subspace (or a [[convex set]], or a [[balanced set]]) the same is true of <math display="inline">\Lambda(A)</math>|If {{mvar|B}} is a subspace (or a convex set, or a balanced set) the same is true of <math display="inline">\Lambda^{-1}(B)</math>|In particular, the set: <math display="block">\Lambda^{-1}(\{0\}) = \{\mathbf x \in X: \Lambda \mathbf x = 0\} = {N}(\Lambda)</math> is a subspace of {{mvar|X}}, called the ''null space'' of {{tmath|\Lambda}}|list-style-type=lower-alpha}}</ref> for example, it maps a [[Plane (geometry)|plane]] through the origin in <math>V</math> to either a plane through the origin in {{tmath|W}}, a [[Line (geometry)|line]] through the origin in {{tmath|W}}, or just the origin in {{tmath|W}}. Linear maps can often be represented as [[matrix (mathematics)|matrices]], and simple examples include [[Rotations and reflections in two dimensions|rotation and reflection linear transformations]].
A linear map from <math>V</math> to <math>W</math> always maps the origin of <math>V</math> to the origin of <math>W</math>. Moreover, it maps [[linear subspace]]s in <math>V</math> onto linear subspaces in <math>W</math> (possibly of a lower [[Dimension (vector space)|dimension]]);<ref>{{harvnb|Rudin|1991|page=14}}<br />Here are some properties of linear mappings <math display="inline">\Lambda: X \to Y</math> whose proofs are so easy that we omit them; it is assumed that <math display="inline">A \subset X</math> and <math display="inline">B \subset Y</math>:
== Definition and first consequences ==
{{ordered list|<math display="inline">\Lambda 0 = 0.</math>|If {{mvar|A}} is a subspace (or a [[convex set]], or a [[balanced set]]) the same is true of <math display="inline">\Lambda(A)</math>|If {{mvar|B}} is a subspace (or a convex set, or a balanced set) the same is true of <math display="inline">\Lambda^{-1}(B)</math>|In particular, the set: <math display="block">\Lambda^{-1}(\{0\}) = \{\mathbf x \in X: \Lambda \mathbf x = 0\} = {N}(\Lambda)</math> is a subspace of {{mvar|X}}, called the ''null space'' of <math display="inline">\Lambda</math>.|list-style-type=lower-alpha}}</ref> for example, it maps a [[Plane (geometry)|plane]] through the [[Origin (geometry)|origin]] in <math>V</math> to either a plane through the origin in <math>W</math>, a [[Line (geometry)|line]] through the origin in <math>W</math>, or just the origin in <math>W</math>. Linear maps can often be represented as [[matrix (mathematics)|matrices]], and simple examples include [[Rotations and reflections in two dimensions|rotation and reflection linear transformations]].
In the language of [[category theory]], linear maps are the [[morphism]]s of vector spaces, and they form a category [[equivalence of categories|equivalent]] to [[category of matrices|the one of matrices]].
Let <math>V</math> and <math>W</math> be vector spaces over the same [[Field (mathematics)|field]] {{tmath|K}}, such as the [[real number|real]] or [[complex numbers]].
==Definition and first consequences==
Let <math>V</math> and <math>W</math> be vector spaces over the same [[Field (mathematics)|field]] <math>K</math>.
A [[function (mathematics)|function]] <math>f: V \to W</math> is said to be a ''linear map'' if for any two vectors <math display="inline">\mathbf{u}, \mathbf{v} \in V</math> and any scalar <math>c \in K</math> the following two conditions are satisfied:
A [[function (mathematics)|function]] <math>f: V \to W</math> is said to be a ''linear map'' if for any two vectors <math display="inline">\mathbf{u}, \mathbf{v} \in V</math> and any scalar <math>c \in K</math> the following two conditions are satisfied:
* [[Additive map|Additivity]] / operation of addition<ref group="note">Although using the same symbol +, the operation defined in <math>V</math> and that defined in <math>W</math> are not necessarily same.</ref><math display="block">f(\mathbf{u} + \mathbf{v}) = f(\mathbf{u}) + f(\mathbf{v})</math>
* [[Homogeneous function|Homogeneity]] of degree 1 / operation of scalar multiplication <math display=block>f(c \mathbf{u}) = c f(\mathbf{u})</math>
* [[Homogeneous function|Homogeneity]] of degree 1 / operation of scalar multiplication <math display=block>f(c \mathbf{u}) = c f(\mathbf{u})</math>
Thus, a linear map is said to be ''operation preserving''. In other words, it does not matter whether the linear map is applied before (the right hand sides of the above examples) or after (the left hand sides of the examples) the operations of addition and scalar multiplication.
Thus, a linear map is said to be ''operation preserving''. In other words, it does not matter whether the linear map is applied before (the right sides of the above examples) or after (the left sides of the examples) the operations of addition and scalar multiplication.
By [[Addition#Associativity|the associativity of the addition operation]] denoted as +, for any vectors <math display="inline"> \mathbf{u}_1, \ldots, \mathbf{u}_n \in V</math> and scalars <math display="inline">c_1, \ldots, c_n \in K,</math> the following equality holds:<ref>{{harvnb|Rudin|1991|page=14}}. Suppose now that {{mvar|X}} and {{mvar|Y}} are vector spaces ''over the same scalar field''. A mapping <math display="inline">\Lambda: X \to Y</math> is said to be ''linear'' if <math display="inline"> \Lambda(\alpha \mathbf x + \beta \mathbf y) = \alpha \Lambda \mathbf x + \beta \Lambda \mathbf y</math> for all <math display="inline">\mathbf x, \mathbf y \in X</math> and all scalars <math display="inline">\alpha</math> and <math display="inline">\beta</math>. Note that one often writes <math display="inline">\Lambda \mathbf x</math>, rather than <math display="inline">\Lambda(\mathbf x)</math>, when <math display="inline"> \Lambda</math> is linear.</ref><ref>{{harvnb|Rudin|1976|page=206}}. A mapping {{mvar|A}} of a vector space {{mvar|X}} into a vector space {{mvar|Y}} is said to be a ''linear transformation'' if: <math display="inline">A\left(\mathbf{x}_1 + \mathbf{x}_2\right) = A\mathbf{x}_1 + A\mathbf{x}_2,\ A(c\mathbf{x}) = c A\mathbf{x}</math> for all <math display="inline">\mathbf{x}, \mathbf{x}_1, \mathbf{x}_2 \in X</math> and all scalars {{mvar|c}}. Note that one often writes <math display="inline">A\mathbf{x}</math> instead of <math display="inline">A(\mathbf {x})</math> if {{mvar|A}} is linear.</ref>
By [[Addition#Associativity|the associativity of the addition operation]] denoted as +, for any vectors <math display="inline"> \mathbf{u}_1, \ldots, \mathbf{u}_n \in V</math> and scalars {{tmath|c_1, \ldots, c_n \in K}}, the following equality holds:<ref>{{harvnb|Rudin|1991|page=14}}. Suppose now that {{mvar|X}} and {{mvar|Y}} are vector spaces ''over the same scalar field''. A mapping <math display="inline">\Lambda: X \to Y</math> is said to be ''linear'' if <math display="inline"> \Lambda(\alpha \mathbf x + \beta \mathbf y) = \alpha \Lambda \mathbf x + \beta \Lambda \mathbf y</math> for all <math display="inline">\mathbf x, \mathbf y \in X</math> and all scalars <math display="inline">\alpha</math> and {{tmath|\beta}}. Note that one often writes {{tmath|\Lambda \mathbf x}}, rather than {{tmath| \Lambda(\mathbf x) }}, when <math display="inline"> \Lambda</math> is linear.</ref><ref>{{harvnb|Rudin|1976|page=206}}. A mapping {{mvar|A}} of a vector space {{mvar|X}} into a vector space {{mvar|Y}} is said to be a ''linear transformation'' if: <math display="inline">A\left(\mathbf{x}_1 + \mathbf{x}_2\right) = A\mathbf{x}_1 + A\mathbf{x}_2,\ A(c\mathbf{x}) = c A\mathbf{x}</math> for all <math display="inline">\mathbf{x}, \mathbf{x}_1, \mathbf{x}_2 \in X</math> and all scalars {{mvar|c}}. Note that one often writes <math display="inline">A\mathbf{x}</math> instead of <math display="inline">A(\mathbf {x})</math> if {{mvar|A}} is linear.</ref>
<math display="block">f(c_1 \mathbf{u}_1 + \cdots + c_n \mathbf{u}_n) = c_1 f(\mathbf{u}_1) + \cdots + c_n f(\mathbf{u}_n).</math> Thus a linear map is one which preserves [[linear combination]]s.
<math display="block">f(c_1 \mathbf{u}_1 + \cdots + c_n \mathbf{u}_n) = c_1 f(\mathbf{u}_1) + \cdots + c_n f(\mathbf{u}_n).</math> Thus a linear map is one which preserves [[linear combination]]s.
Denoting the zero elements of the vector spaces <math>V</math> and <math>W</math> by <math display="inline">\mathbf{0}_V</math> and <math display="inline">\mathbf{0}_W</math> respectively, it follows that <math display="inline">f(\mathbf{0}_V) = \mathbf{0}_W.</math> Let <math>c = 0</math> and <math display="inline">\mathbf{v} \in V</math> in the equation for homogeneity of degree 1:
Denoting the zero elements of the vector spaces <math>V</math> and <math>W</math> by <math display="inline">\mathbf{0}_V</math> and <math display="inline">\mathbf{0}_W</math> respectively, it follows that {{tmath|1=f(\mathbf{0}_V) = \mathbf{0}_W}}. Let <math>c = 0</math> and <math display="inline">\mathbf{v} \in V</math> in the equation for homogeneity of degree 1:
These statements generalize to any left-module <math display="inline">{}_R M</math> over a ring <math>R</math> without modification, and to any right-module upon reversing of the scalar multiplication.
These statements generalize to any left-module <math display="inline">{}_R M</math> over a ring <math>R</math> without modification, and to any right-module upon reversing of the scalar multiplication.
==Examples==
== Examples ==
* The unique map of the form <math>T:\{\vec{0}\} \to \{\vec{0}\}</math> is linear.
* A prototypical example that gives linear maps their name is a function <math>f: \mathbb{R} \to \mathbb{R}: x \mapsto cx</math>, of which the [[graph of a function|graph]] is a line through the origin.<ref>{{Cite web|title=terminology - What does 'linear' mean in Linear Algebra?|url=https://math.stackexchange.com/questions/62789/what-does-linear-mean-in-linear-algebra|access-date=2021-02-17|website=Mathematics Stack Exchange}}</ref>
* A prototypical example that gives linear maps their name is a function {{tmath| f: \mathbb{R} \to \mathbb{R}: x \mapsto cx }}, of which the [[graph of a function|graph]] is a line through the origin.<ref>{{Cite web|title=terminology - What does 'linear' mean in Linear Algebra?|url=https://math.stackexchange.com/questions/62789/what-does-linear-mean-in-linear-algebra|access-date=2021-02-17|website=Mathematics Stack Exchange}}</ref>[[File:Linear_transformations_in_computer_graphics.svg|thumb|Examples of linear transformations used in computer graphics]]
* More generally, any [[homothety]] <math display="inline">\mathbf{v} \mapsto c\mathbf{v}</math> centered in the origin of a vector space is a linear map (here {{mvar|c}} is a scalar).
* More generally, any [[homothety]] <math display="inline">\mathbf{v} \mapsto c\mathbf{v}</math> centered in the origin of a vector space is a linear map (here {{mvar|c}} is a scalar).
* The zero map <math display="inline">\mathbf x \mapsto \mathbf 0</math> between two vector spaces (over the same [[field (mathematics)|field]]) is linear.
* The zero map <math display="inline">\mathbf x \mapsto \mathbf 0</math> between two vector spaces (over the same [[field (mathematics)|field]]) is linear.
* The [[identity function|identity map]] on any module is a linear operator.
* The [[identity map]] on any module is a linear operator.
* For real numbers, the map <math display="inline">x \mapsto x^2</math> is not linear.
* For real numbers, the map <math display="inline">x \mapsto x^2</math> is not linear.
* For real numbers, the map <math display="inline">x \mapsto x + 1</math> is not linear (but is an [[affine transformation]]).
* For real numbers, the map <math display="inline">x \mapsto x + 1</math> is not linear (but is an [[affine transformation]]).
* If <math>A</math> is a <math>m \times n</math> [[real matrix]], then <math>A</math> defines a linear map from <math>\R^n</math> to <math>\R^m</math> by sending a [[column vector]] <math>\mathbf x \in \R^n</math> to the column vector <math>A \mathbf x \in \R^m</math>. Conversely, any linear map between [[finite-dimensional]] vector spaces can be represented in this manner; see the {{slink||Matrices}}, below.
* If <math>A</math> is a <math>m \times n</math> [[real matrix]], then <math>A</math> defines a linear map from <math>\R^n</math> to <math>\R^m</math> by sending a [[column vector]] <math>\mathbf x \in \R^n</math> to the column vector {{tmath|A \mathbf x \in \R^m}}. Conversely, any linear map between [[finite-dimensional]] vector spaces can be represented in this manner; see ''{{slink|#Matrices}}'', below.
* If <math display="inline">f: V \to W</math> is an [[isometry]] between real [[normed space]]s such that <math display="inline"> f(0) = 0</math> then <math>f</math> is a linear map. This result is not necessarily true for complex normed space.{{sfn | Wilansky | 2013 | pp=21–26}}
* If <math display="inline">f: V \to W</math> is an [[isometry]] between real [[normed space]]s such that <math display="inline"> f(0) = 0</math> then <math>f</math> is a linear map. This result is not necessarily true for complex normed space.{{sfn | Wilansky | 2013 | pp=21–26}}
* [[Derivative|Differentiation]] defines a linear map from the space of all differentiable functions to the space of all functions. It also defines a [[linear operator]] on the space of all [[smooth function]]s (a linear operator is a [[linear endomorphism]], that is, a linear map with the same [[Domain of a function|domain]] and [[codomain]]). Indeed, <math display="block">\frac{d}{dx} \left( a f(x) + b g(x) \right) = a \frac{d f(x)}{dx} + b \frac{d g( x)}{dx}.</math>
* [[Derivative|Differentiation]] defines a linear map from the space of all differentiable functions to the space of all functions. It also defines a [[linear operator]] on the space of all [[smooth function]]s (a linear operator is a [[linear endomorphism]], that is, a linear map with the same [[Domain of a function|domain]] and [[codomain]]). Indeed, <math display="block">\frac{d}{dx} \left( a f(x) + b g(x) \right) = a \frac{d f(x)}{dx} + b \frac{d g( x)}{dx}.</math>
* A definite [[integral]] over some [[interval (mathematics)|interval]] {{mvar|I}} is a linear map from the space of all real-valued integrable functions on {{mvar|I}} to <math>\R</math>. Indeed, <math display="block">\int_u^v \left(af(x) + bg(x)\right) dx = a\int_u^v f(x) dx + b\int_u^v g(x) dx . </math>
* A definite [[integral]] over some [[interval (mathematics)|interval]] {{mvar|I}} is a linear map from the space of all real-valued integrable functions on {{mvar|I}} to {{tmath|\R}}. Indeed, <math display="block">\int_u^v \left(af(x) + bg(x)\right) dx = a\int_u^v f(x) dx + b\int_u^v g(x) dx . </math>
* An indefinite [[integral]] (or [[antiderivative]]) with a fixed integration starting point defines a linear map from the space of all real-valued integrable functions on <math>\R</math> to the space of all real-valued, differentiable functions on <math>\R</math>. Without a fixed starting point, the antiderivative maps to the [[quotient space (linear algebra)|quotient space]] of the differentiable functions by the linear space of constant functions.
* An indefinite [[integral]] (or [[antiderivative]]) with a fixed integration starting point defines a linear map from the space of all real-valued integrable functions on <math>\R</math> to the space of all real-valued, differentiable functions on {{tmath|\R}}. Without a fixed starting point, the antiderivative maps to the [[quotient space (linear algebra)|quotient space]] of the differentiable functions by the linear space of constant functions.
* If <math>V</math> and <math>W</math> are finite-dimensional vector spaces over a field {{mvar|F}}, of respective dimensions {{mvar|m}} and {{mvar|n}}, then the function that maps linear maps <math display="inline">f: V \to W</math> to {{math|''n'' × ''m''}} matrices in the way described in {{slink||Matrices}} (below) is a linear map, and even a [[linear isomorphism]].
* If <math>V</math> and <math>W</math> are finite-dimensional vector spaces over a field {{mvar|F}}, of respective dimensions {{mvar|m}} and {{mvar|n}}, then the function that maps linear maps <math display="inline">f: V \to W</math> to {{math|''n'' × ''m''}} matrices in the way described in ''{{slink|#Matrices}}'' (below) is a linear map, and even a [[linear isomorphism]].
* The [[expected value]] of a [[Random variable#Definition|random variable]] (which is in fact a function, and as such an element of a vector space) is linear, as for random variables <math>X</math> and <math>Y</math> we have <math>E[X + Y] = E[X] + E[Y]</math> and <math>E[aX] = aE[X]</math>, but the [[variance]] of a random variable is not linear.
* The [[expected value]] of a [[Random variable#Definition|random variable]] is a linear function of the random variable: for random variables <math>X</math> and <math>Y</math> we have <math>E[X + Y] = E[X] + E[Y]</math> and {{tmath|1= E[aX] = aE[X] }}. The [[conditional expectation]] is as well. But the [[variance]] of a random variable is not linear, because for instance {{tmath|1= \text{Var}(aX)=a^2\text{Var}(X) }}.
<gallery widths="180" heights="120">
<gallery widths="180" heights="120">
File:Streckung eines Vektors.gif|The function <math display="inline">f:\R^2 \to \R^2</math> with <math display="inline">f(x, y) = (2x, y)</math> is a linear map. This function scales the <math display="inline">x</math> component of a vector by the factor <math display="inline">2</math>.
File:Streckung eines Vektors.gif|The function <math display="inline">f:\R^2 \to \R^2</math> with <math display="inline">f(x, y) = (2x, y)</math> is a linear map. This function scales the <math display="inline">x</math> component of a vector by the factor {{tmath|2}}.
File:Streckung der Summe zweier Vektoren.gif|The function <math display="inline">f(x, y) = (2x, y)</math> is additive: It does not matter whether vectors are first added and then mapped or whether they are mapped and finally added: <math display="inline">f(\mathbf a + \mathbf b) = f(\mathbf a) + f(\mathbf b)</math>
File:Streckung der Summe zweier Vektoren.gif|The function <math display="inline">f(x, y) = (2x, y)</math> is additive: It does not matter whether vectors are first added and then mapped or whether they are mapped and finally added: <math display="inline">f(\mathbf a + \mathbf b) = f(\mathbf a) + f(\mathbf b)</math>
File:Streckung homogenitaet Version 3.gif|The function <math display="inline">f(x, y) = (2x, y)</math> is homogeneous: It does not matter whether a vector is first scaled and then mapped or first mapped and then scaled: <math display="inline">f(\lambda \mathbf a) = \lambda f(\mathbf a)</math>
File:Streckung homogenitaet Version 3.gif|The function <math display="inline">f(x, y) = (2x, y)</math> is homogeneous: It does not matter whether a vector is first scaled and then mapped or first mapped and then scaled: <math display="inline">f(\lambda \mathbf a) = \lambda f(\mathbf a)</math>
</gallery>
</gallery>
===Linear extensions===
=== Linear endomorphisms and isomorphisms ===
If a linear map is a [[bijection]] then it is called a '''{{visible anchor|Linear isomorphism|text=linear isomorphism}}'''. In the case where {{tmath|1= V = W }}, a linear map is called a '''linear endomorphism'''. Sometimes the term '''{{visible anchor|Linear operator|text=linear operator}}''' refers to this case,<ref>"Linear transformations of {{mvar|V}} into {{mvar|V}} are often called ''linear operators'' on {{mvar|V}}." {{harvnb|Rudin|1976|page=207}}</ref> but the term "linear operator" can have different meanings for different conventions.
=== Linear extensions ===
Often, a linear map is constructed by defining it on a subset of a vector space and then {{em|{{visible anchor|extending by linearity|extend by linearity}}}} to the [[linear span]] of the domain.
Often, a linear map is constructed by defining it on a subset of a vector space and then {{em|{{visible anchor|extending by linearity|extend by linearity}}}} to the [[linear span]] of the domain.
Suppose <math>X</math> and <math>Y</math> are vector spaces and <math>f : S \to Y</math> is a [[Function (mathematics)|function]] defined on some subset <math>S \subseteq X.</math>
Suppose <math>X</math> and <math>Y</math> are vector spaces and <math>f : S \to Y</math> is a [[Function (mathematics)|function]] defined on some subset {{tmath| S \subseteq X }}.
Then a ''{{visible anchor|linear extension|Linear extension}} of <math>f</math> to <math>X,</math>'' if it exists, is a linear map <math>F : X \to Y</math> defined on <math>X</math> that [[Extension of a function|extends]] <math>f</math><ref group=note>One map <math>F</math> is said to [[Extension of a function|{{em|extend}}]] another map <math>f</math> if when <math>f</math> is defined at a point <math>s,</math> then so is <math>F</math> and <math>F(s) = f(s).</math></ref> (meaning that <math>F(s) = f(s)</math> for all <math>s \in S</math>) and takes its values from the codomain of <math>f.</math>{{sfn|Kubrusly|2001|p=57}}
Then a ''{{visible anchor|linear extension|Linear extension}} of <math>f</math> to <math>X,</math>'' if it exists, is a linear map <math>F : X \to Y</math> defined on <math>X</math> that [[Extension of a function|extends]] <math>f</math><ref group=note>One map <math>F</math> is said to [[Extension of a function|{{em|extend}}]] another map <math>f</math> if when <math>f</math> is defined at a point {{tmath| s }}, then so is <math>F</math> and <math>F(s) = f(s).</math></ref> (meaning that <math>F(s) = f(s)</math> for all {{tmath| s \in S }}) and takes its values from the codomain of {{tmath| f }}.{{sfn|Kubrusly|2001|p=57}}
When the subset <math>S</math> is a vector subspace of <math>X</math> then a (<math>Y</math>-valued) linear extension of <math>f</math> to all of <math>X</math> is guaranteed to exist if (and only if) <math>f : S \to Y</math> is a linear map.{{sfn|Kubrusly|2001|p=57}} In particular, if <math>f</math> has a linear extension to <math>\operatorname{span} S,</math> then it has a linear extension to all of <math>X.</math>
When the subset <math>S</math> is a vector subspace of <math>X</math> then a ({{tmath|Y}}-valued) linear extension of <math>f</math> to all of <math>X</math> is guaranteed to exist if (and only if) <math>f : S \to Y</math> is a linear map.{{sfn|Kubrusly|2001|p=57}} In particular, if <math>f</math> has a linear extension to <math>\operatorname{span} S,</math> then it has a linear extension to all of {{tmath| X }}.
The map <math>f : S \to Y</math> can be extended to a linear map <math>F : \operatorname{span} S \to Y</math> if and only if whenever <math>n > 0</math> is an integer, <math>c_1, \ldots, c_n</math> are scalars, and <math>s_1, \ldots, s_n \in S</math> are vectors such that <math>0 = c_1 s_1 + \cdots + c_n s_n,</math> then necessarily <math>0 = c_1 f\left(s_1\right) + \cdots + c_n f\left(s_n\right).</math>{{sfn|Schechter|1996|pp=277–280}}
The map <math>f : S \to Y</math> can be extended to a linear map <math>F : \operatorname{span} S \to Y</math> if and only if whenever <math>n > 0</math> is an integer, <math>c_1, \ldots, c_n</math> are scalars, and <math>s_1, \ldots, s_n \in S</math> are vectors such that {{tmath|1= 0 = c_1 s_1 + \cdots + c_n s_n }}, then necessarily {{tmath|1= 0 = c_1 f\left(s_1\right) + \cdots + c_n f\left(s_n\right) }}.{{sfn|Schechter|1996|pp=277–280}}
If a linear extension of <math>f : S \to Y</math> exists then the linear extension <math>F : \operatorname{span} S \to Y</math> is unique and
If a linear extension of <math>f : S \to Y</math> exists then the linear extension <math>F : \operatorname{span} S \to Y</math> is unique and
holds for all <math>n, c_1, \ldots, c_n,</math> and <math>s_1, \ldots, s_n</math> as above.{{sfn|Schechter|1996|pp=277–280}}
holds for all {{tmath| n, c_1, \ldots, c_n }}, and <math>s_1, \ldots, s_n</math> as above.{{sfn|Schechter|1996|pp=277–280}}
If <math>S</math> is linearly independent then every function <math>f : S \to Y</math> into any vector space has a linear extension to a (linear) map <math>\;\operatorname{span} S \to Y</math> (the converse is also true).
If <math>S</math> is linearly independent then every function <math>f : S \to Y</math> into any vector space has a linear extension to a (linear) map <math>\operatorname{span} S \to Y</math> (the converse is also true).
For example, if <math>X = \R^2</math> and <math>Y = \R</math> then the assignment <math>(1, 0) \to -1</math> and <math>(0, 1) \to 2</math> can be linearly extended from the linearly independent set of vectors <math>S := \{(1,0), (0, 1)\}</math> to a linear map on <math>\operatorname{span}\{(1,0), (0, 1)\} = \R^2.</math> The unique linear extension <math>F : \R^2 \to \R</math> is the map that sends <math>(x, y) = x (1, 0) + y (0, 1) \in \R^2</math> to
For example, if <math>X = \R^2</math> and <math>Y = \R</math> then the assignment <math>(1, 0) \to -1</math> and <math>(0, 1) \to 2</math> can be linearly extended from the linearly independent set of vectors <math>S := \{(1,0), (0, 1)\}</math> to a linear map on {{tmath|1= \operatorname{span}\{(1,0), (0, 1)\} = \R^2 }}. The unique linear extension <math>F : \R^2 \to \R</math> is the map that sends <math>(x, y) = x (1, 0) + y (0, 1) \in \R^2</math> to
<math display=block>F(x, y) = x (-1) + y (2) = - x + 2 y.</math>
<math display=block>F(x, y) = x (-1) + y (2) = - x + 2 y.</math>
Every (scalar-valued) [[linear functional]] <math>f</math> defined on a [[vector subspace]] of a real or complex vector space <math>X</math> has a linear extension to all of <math>X.</math>
Every (scalar-valued) [[linear functional]] <math>f</math> defined on a [[vector subspace]] of a real or complex vector space <math>X</math> has a linear extension to all of {{tmath| X }}.
Indeed, the [[Hahn–Banach theorem|Hahn–Banach dominated extension theorem]] even guarantees that when this linear functional <math>f</math> is dominated by some given [[seminorm]] <math>p : X \to \R</math> (meaning that <math>|f(m)| \leq p(m)</math> holds for all <math>m</math> in the domain of <math>f</math>) then there exists a linear extension to <math>X</math> that is also dominated by <math>p.</math>
Indeed, the [[Hahn–Banach theorem|Hahn–Banach dominated extension theorem]] even guarantees that when this linear functional <math>f</math> is dominated by some given [[seminorm]] <math>p : X \to \R</math> (meaning that <math>|f(m)| \leq p(m)</math> holds for all <math>m</math> in the domain of {{tmath| f }}) then there exists a linear extension to <math>X</math> that is also dominated by {{tmath| p }}.
==Matrices==
{{Main|Transformation matrix}}
If <math>V</math> and <math>W</math> are [[finite-dimensional]] vector spaces and a [[basis of a vector space|basis]] is defined for each vector space, then every linear map from <math>V</math> to <math>W</math> can be represented by a [[matrix (mathematics)|matrix]].<ref>{{harvnb|Rudin|1976|page=210}}
Suppose <math display="inline">\left\{\mathbf{x}_1, \ldots, \mathbf{x}_n\right\}</math> and <math display="inline">\left\{\mathbf{y}_1, \ldots, \mathbf{y}_m\right\}</math> are bases of vector spaces {{mvar|X}} and {{mvar|Y}}, respectively. Then every <math display="inline">A \in L(X, Y)</math> determines a set of numbers <math display="inline">a_{i,j}</math> such that
It is convenient to represent these numbers in a rectangular array of {{mvar|m}} rows and {{mvar|n}} columns, called an {{mvar|m}} ''by'' {{mvar|n}} ''matrix'':
== Matrices ==
<math display="block">[A] = \begin{bmatrix}
{{main|Transformation matrix}}
a_{1,1} & a_{1,2} & \ldots & a_{1,n} \\
a_{2,1} & a_{2,2} & \ldots & a_{2,n} \\
\vdots & \vdots & \ddots & \vdots \\
a_{m,1} & a_{m,2} & \ldots & a_{m,n}
\end{bmatrix}</math>
Observe that the coordinates <math display="inline">a_{i,j}</math> of the vector <math display="inline">A\mathbf{x}_j</math> (with respect to the basis <math display="inline">\{\mathbf{y}_1, \ldots, \mathbf{y}_m\}</math>) appear in the ''j''<sup>th</sup> column of <math display="inline">[A]</math>. The vectors <math display="inline">A\mathbf{x}_j</math> are therefore sometimes called the ''column vectors'' of <math display="inline">[A]</math>. With this terminology, the ''range'' of {{mvar|A}} ''is spanned by the column vectors of <math display="inline">[A]</math>''.
If <math>V</math> and <math>W</math> are [[finite-dimensional]] vector spaces and a [[basis of a vector space|basis]] is defined for each vector space, then every linear map from <math>V</math> to <math>W</math> can be represented by a [[matrix (mathematics)|matrix]].<ref>{{harvnb|Rudin|1976|page=210}}</ref> This is useful because it allows concrete calculations. Matrices yield examples of linear maps: if <math>A</math> is a real <math>m \times n</math> matrix, then <math>f(\mathbf x) = A \mathbf x</math> describes a linear map <math>\R^n \to \R^m</math> (see [[Euclidean space]]).
</ref> This is useful because it allows concrete calculations. Matrices yield examples of linear maps: if <math>A</math> is a real <math>m \times n</math> matrix, then <math>f(\mathbf x) = A \mathbf x</math> describes a linear map <math>\R^n \to \R^m</math> (see [[Euclidean space]]).
Let <math>\{ \mathbf {v}_1, \ldots , \mathbf {v}_n \}</math> be a basis for <math>V</math>. Then every vector <math>\mathbf {v} \in V</math> is uniquely determined by the coefficients <math>c_1, \ldots , c_n</math> in the field <math>\R</math>:
Let <math>\{ \mathbf {v}_1, \ldots , \mathbf {v}_n \}</math> be a basis for {{tmath|V}}. Then every vector <math>\mathbf {v} \in V</math> is uniquely determined by the coefficients <math>c_1, \ldots , c_n</math> in the field {{tmath| \R }}:
which implies that the function ''f'' is entirely determined by the vectors <math>f(\mathbf {v}_1), \ldots , f(\mathbf {v}_n)</math>. Now let <math>\{ \mathbf {w}_1, \ldots , \mathbf {w}_m \}</math> be a basis for <math>W</math>. Then we can represent each vector <math>f(\mathbf {v}_j)</math> as
which implies that the function ''f'' is entirely determined by the vectors {{tmath| f(\mathbf {v}_1), \ldots , f(\mathbf {v}_n) }}. Now let <math>\{ \mathbf {w}_1, \ldots , \mathbf {w}_m \}</math> be a basis for {{tmath|W}}. Then we can represent each vector <math>f(\mathbf {v}_j)</math> as
Thus, the function <math>f</math> is entirely determined by the values of <math>a_{ij}</math>. If we put these values into an <math>m \times n</math> matrix <math>M</math>, then we can conveniently use it to compute the vector output of <math>f</math> for any vector in <math>V</math>. To get <math>M</math>, every column <math>j</math> of <math>M</math> is a vector
Thus, the function <math>f</math> is entirely determined by the values of {{tmath| a_{ij} }}. If we put these values into an <math>m \times n</math> matrix {{tmath|M}}, then we can conveniently use it to compute the vector output of <math>f</math> for any vector in {{tmath|V}}. To get {{tmath|M}}, every column <math>j</math> of <math>M</math> is a vector
corresponding to <math>f(\mathbf {v}_j)</math> as defined above. To define it more clearly, for some column <math>j</math> that corresponds to the mapping <math>f(\mathbf {v}_j)</math>,
corresponding to <math>f(\mathbf {v}_j)</math> as defined above. To define it more clearly, for some column <math>j</math> that corresponds to the mapping {{tmath| f(\mathbf {v}_j) }},
where <math>M</math> is the matrix of <math>f</math>. In other words, every column <math>j = 1, \ldots, n</math> has a corresponding vector <math>f(\mathbf {v}_j)</math> whose coordinates <math>a_{1j}, \cdots, a_{mj}</math> are the elements of column <math>j</math>. A single linear map may be represented by many matrices. This is because the values of the elements of a matrix depend on the bases chosen.
where <math>M</math> is the matrix of {{tmath| f }}. In other words, every column <math>j = 1, \ldots, n</math> has a corresponding vector <math>f(\mathbf {v}_j)</math> whose coordinates <math>a_{1j}, \cdots, a_{mj}</math> are the elements of column {{tmath| j }}. A single linear map may be represented by many matrices. This is because the values of the elements of a matrix depend on the bases chosen.
The matrices of a linear transformation can be represented visually:
The matrices of a linear transformation can be represented visually:
# Matrix for <math display="inline">T</math> relative to {{tmath| B }}: <math display="inline">A</math>
# Matrix for <math display="inline">T</math> relative to <math display="inline">B</math>: <math display="inline">A</math>
# Matrix for <math display="inline">T</math> relative to {{tmath| B' }}: <math display="inline">A'</math>
# Matrix for <math display="inline">T</math> relative to <math display="inline">B'</math>: <math display="inline">A'</math>
# Transition matrix from <math display="inline">B'</math> to {{tmath| B }}: <math display="inline">P</math>
# Transition matrix from <math display="inline">B'</math> to <math display="inline">B</math>: <math display="inline">P</math>
# Transition matrix from <math display="inline">B</math> to {{tmath| B' }}: <math display="inline">P^{-1}</math>
# Transition matrix from <math display="inline">B</math> to <math display="inline">B'</math>: <math display="inline">P^{-1}</math>
[[File:Linear_transformation_visualization.svg|frame|The relationship between matrices in a linear transformation|none]]
[[File:Linear_transformation_visualization.svg|frame|The relationship between matrices in a linear transformation|none]]
Such that starting in the bottom left corner <math display="inline">\left[\mathbf{v}\right]_{B'}</math> and looking for the bottom right corner <math display="inline">\left[T\left(\mathbf{v}\right)\right]_{B'}</math>, one would left-multiply—that is, <math display="inline">A'\left[\mathbf{v}\right]_{B'} = \left[T\left(\mathbf{v}\right)\right]_{B'}</math>. The equivalent method would be the "longer" method going clockwise from the same point such that <math display="inline">\left[\mathbf{v}\right]_{B'}</math> is left-multiplied with <math display="inline">P^{-1}AP</math>, or <math display="inline">P^{-1}AP\left[\mathbf{v}\right]_{B'} = \left[T\left(\mathbf{v}\right)\right]_{B'}</math>.
Such that starting in the bottom left corner <math display="inline">\left[\mathbf{v}\right]_{B'}</math> and looking for the bottom right corner {{tmath|\textstyle \left[T\left(\mathbf{v}\right)\right]_{B'} }}, one would left-multiply—that is, {{tmath|1=\textstyle A'\left[\mathbf{v}\right]_{B'} = \left[T\left(\mathbf{v}\right)\right]_{B'} }}. The equivalent method would be the "longer" method going clockwise from the same point such that <math display="inline">\left[\mathbf{v}\right]_{B'}</math> is left-multiplied with {{tmath|P^{-1}AP}}, or {{tmath|1=\textstyle P^{-1}AP\left[\mathbf{v}\right]_{B'} = \left[T\left(\mathbf{v}\right)\right]_{B'} }}.
===Examples in two dimensions===
=== Examples in two dimensions ===
In two-[[dimension]]al space '''R'''<sup>2</sup> linear maps are described by 2 × 2 [[matrix (mathematics)|matrices]]. These are some examples:
In two-[[dimension]]al space '''R'''<sup>2</sup> linear maps are described by 2 × 2 [[matrix (mathematics)|matrices]]. These are some examples:
If a linear map is only composed of rotation, reflection, and/or uniform scaling, then the linear map is a [[conformal linear transformation]].
If a linear map is only composed of rotation, reflection, and/or uniform scaling, then the linear map is a [[conformal linear transformation]].
==Vector space of linear maps==
== Vector space of linear maps ==
The composition of linear maps is linear: if <math>f: V \to W</math> and <math display="inline">g: W \to Z</math> are linear, then so is their [[Relation composition|composition]] <math display="inline">g \circ f: V \to Z</math>. It follows from this that the [[class (set theory)|class]] of all vector spaces over a given field ''K'', together with ''K''-linear maps as [[morphism]]s, forms a [[category (mathematics)|category]].
The composition of linear maps is linear: if <math>f: V \to W</math> and <math display="inline">g: W \to Z</math> are linear, then so is their [[Relation composition|composition]] {{tmath| g \circ f: V \to Z }}. It follows from this that the [[class (set theory)|class]] of all vector spaces over a given field ''K'', together with linear maps as [[morphism]]s, forms a [[category (mathematics)|category]].
The [[inverse function|inverse]] of a linear map, when defined, is again a linear map.
The [[inverse function|inverse]] of a linear map, when defined, is again a linear map.
If <math display="inline">f_1: V \to W</math> and <math display="inline">f_2: V \to W</math> are linear, then so is their [[pointwise]] sum <math>f_1 + f_2</math>, which is defined by <math>(f_1 + f_2)(\mathbf x) = f_1(\mathbf x) + f_2(\mathbf x)</math>.
If <math display="inline">f_1: V \to W</math> and <math display="inline">f_2: V \to W</math> are linear, then so is their [[pointwise]] sum {{tmath| f_1 + f_2 }}, which is defined by {{tmath|1= (f_1 + f_2)(\mathbf x) = f_1(\mathbf x) + f_2(\mathbf x) }}.
If <math display="inline">f: V \to W</math> is linear and <math display="inline">\alpha</math> is an element of the ground field <math display="inline">K</math>, then the map <math display="inline">\alpha f</math>, defined by <math display="inline">(\alpha f)(\mathbf x) = \alpha (f(\mathbf x))</math>, is also linear.
If <math display="inline">f: V \to W</math> is linear and <math display="inline">\alpha</math> is an element of the ground field {{tmath|K}}, then the map {{tmath| \alpha f }}, defined by {{tmath|1= (\alpha f)(\mathbf x) = \alpha (f(\mathbf x)) }}, is also linear.
Thus the set <math display="inline">\mathcal{L}(V, W)</math> of linear maps from <math display="inline">V</math> to <math display="inline">W</math> itself forms a vector space over <math display="inline">K</math>,<ref>{{Harvard citation text |Axler|2015}} p. 52, § 3.3</ref> sometimes denoted <math display="inline">\operatorname{Hom}(V, W)</math>.<ref>{{Harvard citation text|Tu|2011}}, p. 19, § 3.1</ref> Furthermore, in the case that <math display="inline">V = W</math>, this vector space, denoted <math display="inline"> \operatorname{End}(V)</math>, is an [[associative algebra]] under [[composition of maps]], since the composition of two linear maps is again a linear map, and the composition of maps is always associative. This case is discussed in more detail below.
Thus the set <math display="inline">\mathcal{L}(V, W)</math> of linear maps from <math display="inline">V</math> to <math display="inline">W</math> itself forms a vector space over {{tmath|K}},<ref>{{harvard citation text |Axler|2015}} p. 52, § 3.3</ref> sometimes denoted {{tmath| \operatorname{Hom}(V, W) }}.<ref>{{harvnb|Tu|2011|p=19|loc=§ 3.1}}</ref> Furthermore, in the case that {{tmath|1= V = W }}, this vector space, denoted {{tmath| \operatorname{End}(V) }}, is an [[associative algebra]] under [[composition of maps]], since the composition of two linear maps is again a linear map, and the composition of maps is always associative. This case is discussed in more detail below.
Given again the finite-dimensional case, if bases have been chosen, then the composition of linear maps corresponds to the [[matrix multiplication]], the addition of linear maps corresponds to the [[matrix addition]], and the multiplication of linear maps with scalars corresponds to the multiplication of matrices with scalars.
Given again the finite-dimensional case, if bases have been chosen, then the composition of linear maps corresponds to the [[matrix multiplication]], the addition of linear maps corresponds to the [[matrix addition]], and the multiplication of linear maps with scalars corresponds to the multiplication of matrices with scalars.
===Endomorphisms and automorphisms===
=== Endomorphisms and automorphisms ===
{{Main|Endomorphism|Automorphism}}
{{main|Endomorphism|Automorphism}}
A linear transformation <math display="inline">f : V \to V</math> is an [[endomorphism]] of <math display="inline">V</math>; the set of all such endomorphisms <math display="inline">\operatorname{End}(V)</math> together with addition, composition and scalar multiplication as defined above forms an [[associative algebra]] with identity element over the field <math display="inline">K</math> (and in particular a [[ring (algebra)|ring]]). The multiplicative identity element of this algebra is the [[identity function|identity map]] <math display="inline">\operatorname{id}: V \to V</math>.
A linear transformation <math display="inline">f : V \to V</math> is an [[endomorphism]] of <math display="inline">V</math>; the set of all such endomorphisms <math display="inline">\operatorname{End}(V)</math> together with addition, composition and scalar multiplication as defined above forms an [[associative algebra]] with identity element over the field <math display="inline">K</math> (and in particular a [[ring (algebra)|ring]]). The multiplicative identity element of this algebra is the [[identity map]] {{tmath| \operatorname{id}: V \to V }}.
An endomorphism of <math display="inline">V</math> that is also an [[isomorphism]] is called an [[automorphism]] of <math display="inline">V</math>. The composition of two automorphisms is again an automorphism, and the set of all automorphisms of <math display="inline">V</math> forms a [[group (math)|group]], the [[automorphism group]] of <math display="inline">V</math> which is denoted by <math display="inline">\operatorname{Aut}(V)</math> or <math display="inline">\operatorname{GL}(V)</math>. Since the automorphisms are precisely those [[endomorphisms]] which possess inverses under composition, <math display="inline">\operatorname{Aut}(V)</math> is the group of [[Unit (ring theory)|units]] in the ring <math display="inline">\operatorname{End}(V)</math>.
An endomorphism of <math display="inline">V</math> that is also an [[isomorphism]] is called an [[automorphism]] of {{tmath|V}}. The composition of two automorphisms is again an automorphism, and the set of all automorphisms of <math display="inline">V</math> forms a [[group (math)|group]], the [[automorphism group]] of <math display="inline">V</math> which is denoted by <math display="inline">\operatorname{Aut}(V)</math> or {{tmath| \operatorname{GL}(V) }}. Since the automorphisms are precisely those [[endomorphisms]] which possess inverses under composition, <math display="inline">\operatorname{Aut}(V)</math> is the group of [[Unit (ring theory)|units]] in the ring {{tmath| \operatorname{End}(V) }}.
If <math display="inline">V</math> has finite dimension <math display="inline">n</math>, then <math display="inline"> \operatorname{End}(V)</math> is [[isomorphism|isomorphic]] to the [[associative algebra]] of all <math display="inline">n \times n</math> matrices with entries in <math display="inline">K</math>. The automorphism group of <math display="inline">V</math> is [[group isomorphism|isomorphic]] to the [[general linear group]] <math display="inline">\operatorname{GL}(n, K)</math> of all <math display="inline">n \times n</math> invertible matrices with entries in <math display="inline">K</math>.
If <math display="inline">V</math> has finite dimension {{tmath|n}}, then <math display="inline"> \operatorname{End}(V)</math> is [[isomorphic]] to the [[associative algebra]] of all <math display="inline">n \times n</math> matrices with entries in {{tmath|K}}. The automorphism group of <math display="inline">V</math> is [[group isomorphism|isomorphic]] to the [[general linear group]] <math display="inline">\operatorname{GL}(n, K)</math> of all <math display="inline">n \times n</math> invertible matrices with entries in {{tmath|K}}.
==Kernel, image and the rank–nullity theorem==
== Kernel, image and the rank–nullity theorem ==
{{Main|Kernel (linear algebra)|Image (mathematics)|Rank of a matrix}}
{{main|Kernel (linear algebra)|Image (mathematics)|Rank of a matrix}}
If <math display="inline">f: V \to W</math> is linear, we define the [[kernel (linear operator)|kernel]] and the [[image (mathematics)|image]] or [[Range of a function|range]] of <math display="inline">f</math> by
If <math display="inline">f: V \to W</math> is linear, we define the [[kernel (linear operator)|kernel]] and the [[image (mathematics)|image]] or [[Range of a function|range]] of <math display="inline">f</math> by
<math display="block">\begin{align}
<math display="block">\begin{align}
Line 172:
Line 154:
\end{align}</math>
\end{align}</math>
<math display="inline">\ker(f)</math> is a [[Linear subspace|subspace]] of <math display="inline">V</math> and <math display="inline">\operatorname{im}(f)</math> is a subspace of <math display="inline">W</math>. The following [[dimension]] formula is known as the [[rank–nullity theorem]]:<ref>{{harvnb|Horn|Johnson|2013|loc=0.2.3 Vector spaces associated with a matrix or linear transformation, p. 6}}</ref>
<math display="inline">\ker(f)</math> is a [[Linear subspace|subspace]] of <math display="inline">V</math> and <math display="inline">\operatorname{im}(f)</math> is a subspace of {{tmath|W}}. The following [[dimension]] formula is known as the [[rank–nullity theorem]]:<ref>{{harvnb|Horn|Johnson|2013|loc=0.2.3 Vector spaces associated with a matrix or linear transformation, p. 6}}</ref>
<math display="block">\dim(\ker( f )) + \dim(\operatorname{im}( f )) = \dim( V ).</math>
<math display="block">\dim(\ker( f )) + \dim(\operatorname{im}( f )) = \dim( V ).</math>
The number <math display="inline">\dim(\operatorname{im}(f))</math> is also called the [[rank of a matrix|rank]] of <math display="inline">f</math> and written as <math display="inline">\operatorname{rank}(f)</math>, or sometimes, <math display="inline">\rho(f)</math>;<ref name=":0">{{Harvard citation text|Katznelson|Katznelson|2008}} p. 52, § 2.5.1</ref><ref name=":1">{{Harvard citation text|Halmos|1974}} p. 90, § 50</ref> the number <math display="inline">\dim(\ker(f))</math> is called the [[Kernel (matrix)#Subspace properties|nullity]] of <math display="inline">f</math> and written as <math display="inline">\operatorname{null}(f)</math> or <math display="inline">\nu(f)</math>.<ref name=":0" /><ref name=":1" /> If <math display="inline">V</math> and <math display="inline">W</math> are finite-dimensional, bases have been chosen and <math display="inline">f</math> is represented by the matrix <math display="inline">A</math>, then the rank and nullity of <math display="inline">f</math> are equal to the rank and nullity of the matrix <math display="inline">A</math>, respectively.
The number <math display="inline">\dim(\operatorname{im}(f))</math> is also called the [[rank of a matrix|rank]] of <math display="inline">f</math> and written as {{tmath| \operatorname{rank}(f) }}, or sometimes, {{tmath| \rho(f) }};<ref name=":0">{{Harvard citation text|Katznelson|Katznelson|2008}} p. 52, § 2.5.1</ref><ref name=":1">{{Harvard citation text|Halmos|1974}} p. 90, § 50</ref> the number <math display="inline">\dim(\ker(f))</math> is called the [[Kernel (matrix)#Subspace properties|nullity]] of <math display="inline">f</math> and written as <math display="inline">\operatorname{null}(f)</math> or {{tmath|\nu(f)}}.<ref name=":0" /><ref name=":1" /> If <math display="inline">V</math> and <math display="inline">W</math> are finite-dimensional, bases have been chosen and <math display="inline">f</math> is represented by the matrix {{tmath|A}}, then the rank and nullity of <math display="inline">f</math> are equal to the rank and nullity of the matrix {{tmath|A}}, respectively.
==Cokernel==
== Cokernel ==
{{Main|Cokernel}}
{{main|Cokernel}}
A subtler invariant of a linear transformation <math display="inline">f: V \to W</math> is the [[cokernel|''co''kernel]], which is defined as
A subtler invariant of a linear transformation <math display="inline">f : V \to W</math> is the [[cokernel|''co''kernel]], which is defined as
<math display="block">0 \to \ker(f) \to V \to W \to \operatorname{coker}(f) \to 0.</math>
<math display="block">0 \to \ker(f) \to V \to W \to \operatorname{coker}(f) \to 0.</math>
These can be interpreted thus: given a linear equation ''f''('''v''') = '''w''' to solve,
These can be interpreted thus: given a linear equation {{math|1=''f''('''v''') = '''w'''}} to solve,
* the kernel is the space of ''solutions'' to the ''homogeneous'' equation {{math|1=''f''('''v''') = 0}}, and its dimension is the number of [[degrees of freedom]] in the space of solutions, if it is not empty;
* the kernel is the space of ''solutions'' to the ''homogeneous'' equation ''f''('''v''') = 0, and its dimension is the number of [[degrees of freedom]] in the space of solutions, if it is not empty;
* the co-kernel is the space of [[wikt:constraint|constraints]] that the solutions must satisfy, and its dimension is the maximal number of independent constraints.
* the co-kernel is the space of [[wikt:constraint|constraints]] that the solutions must satisfy, and its dimension is the maximal number of independent constraints.
The dimension of the co-kernel and the dimension of the image (the rank) add up to the dimension of the target space. For finite dimensions, this means that the dimension of the quotient space ''W''/''f''(''V'') is the dimension of the target space minus the dimension of the image.
The dimension of the co-kernel and the dimension of the image (the rank) add up to the dimension of the target space. For finite dimensions, this means that the dimension of the quotient space {{math| ''W'' / ''f''(''V'')}} is the dimension of the target space minus the dimension of the image.
As a simple example, consider the map ''f'': '''R'''<sup>2</sup> → '''R'''<sup>2</sup>, given by ''f''(''x'', ''y'') = (0, ''y''). Then for an equation ''f''(''x'', ''y'') = (''a'', ''b'') to have a solution, we must have ''a'' = 0 (one constraint), and in that case the solution space is (''x'', ''b'') or equivalently stated, (0, ''b'') + (''x'', 0), (one degree of freedom). The kernel may be expressed as the subspace (''x'', 0) < ''V'': the value of ''x'' is the freedom in a solution – while the cokernel may be expressed via the map ''W'' → '''R''', <math display="inline"> (a, b) \mapsto (a)</math>: given a vector (''a'', ''b''), the value of ''a'' is the ''obstruction'' to there being a solution.
As a simple example, consider the map {{math|''f'' : '''R'''<sup>2</sup> → '''R'''<sup>2</sup>}}, given by {{math|1=''f''(''x'', ''y'') = (0, ''y'')}}. Then for an equation {{math|1=''f''(''x'', ''y'') = (''a'', ''b'')}} to have a solution, we must have {{math|1=''a'' = 0}} (one constraint), and in that case the solution space is {{math|(''x'', ''b'')}} or equivalently stated, {{math|
(0, ''b'') + (''x'', 0)}}, (one degree of freedom). The kernel may be expressed as the subspace {{math|(''x'', 0) < ''V''}}: the value of {{math|''x''}} is the freedom in a solution – while the cokernel may be expressed via the map {{math|''W'' → '''R'''}}, {{tmath| (a, b) \mapsto (a) }}: given a vector {{math|(''a'', ''b'')}}, the value of {{math|''a''}} is the ''obstruction'' to there being a solution.
An example illustrating the infinite-dimensional case is afforded by the map ''f'': '''R'''<sup>∞</sup> → '''R'''<sup>∞</sup>, <math display="inline">\left\{a_n\right\} \mapsto \left\{b_n\right\}</math> with ''b''<sub>1</sub> = 0 and ''b''<sub>''n'' + 1</sub> = ''a<sub>n</sub>'' for ''n'' > 0. Its image consists of all sequences with first element 0, and thus its cokernel consists of the classes of sequences with identical first element. Thus, whereas its kernel has dimension 0 (it maps only the zero sequence to the zero sequence), its co-kernel has dimension 1. Since the domain and the target space are the same, the rank and the dimension of the kernel add up to the same [[cardinal number#Cardinal addition|sum]] as the rank and the dimension of the co-kernel (<math display="inline">\aleph_0 + 0 = \aleph_0 + 1</math>), but in the infinite-dimensional case it cannot be inferred that the kernel and the co-kernel of an [[endomorphism]] have the same dimension (0 ≠ 1). The reverse situation obtains for the map ''h'': '''R'''<sup>∞</sup> → '''R'''<sup>∞</sup>, <math display="inline">\left\{a_n\right\} \mapsto \left\{c_n\right\}</math> with ''c<sub>n</sub>'' = ''a''<sub>''n'' + 1</sub>. Its image is the entire target space, and hence its co-kernel has dimension 0, but since it maps all sequences in which only the first element is non-zero to the zero sequence, its kernel has dimension 1.
An example illustrating the infinite-dimensional case is afforded by the map {{math|''f'' : '''R'''<sup>∞</sup> → '''R'''<sup>∞</sup>}}, <math display="inline">\left\{a_n\right\} \mapsto \left\{b_n\right\}</math> with {{math|1=''b''<sub>1</sub> = 0}} and {{math|1=''b''<sub>''n'' + 1</sub> = ''a<sub>n</sub>''}} for {{math|''n'' > 0}}. Its image consists of all sequences with first element {{math|0}}, and thus its cokernel consists of the classes of sequences with identical first element. Thus, whereas its kernel has dimension 0 (it maps only the zero sequence to the zero sequence), its co-kernel has dimension 1. Since the domain and the target space are the same, the rank and the dimension of the kernel add up to the same [[cardinal number#Cardinal addition|sum]] as the rank and the dimension of the co-kernel ({{tmath|1= \aleph_0 + 0 = \aleph_0 + 1 }}), but in the infinite-dimensional case it cannot be inferred that the kernel and the co-kernel of an [[endomorphism]] have the same dimension ({{math|0 ≠ 1}}). The reverse situation obtains for the map {{math|''h'' : '''R'''<sup>∞</sup> → '''R'''<sup>∞</sup>}}, <math display="inline">\left\{a_n\right\} \mapsto \left\{c_n\right\}</math> with {{math|1=''c<sub>n</sub>'' = ''a''<sub>''n'' + 1</sub>}}. Its image is the entire target space, and hence its co-kernel has dimension 0, but since it maps all sequences in which only the first element is non-zero to the zero sequence, its kernel has dimension 1.
===Index===
=== Index ===
For a linear operator with finite-dimensional kernel and co-kernel, one may define ''index'' as:
For a linear operator with finite-dimensional kernel and co-kernel, one may define ''index'' as:
For a transformation between finite-dimensional vector spaces, this is just the difference dim(''V'') − dim(''W''), by rank–nullity. This gives an indication of how many solutions or how many constraints one has: if mapping from a larger space to a smaller one, the map may be onto, and thus will have degrees of freedom even without constraints. Conversely, if mapping from a smaller space to a larger one, the map cannot be onto, and thus one will have constraints even without degrees of freedom.
For a transformation between finite-dimensional vector spaces, this is just the difference dim(''V'') − dim(''W''), by rank–nullity. This gives an indication of how many solutions or how many constraints one has: if mapping from a larger space to a smaller one, the map may be onto, and thus will have degrees of freedom even without constraints. Conversely, if mapping from a smaller space to a larger one, the map cannot be onto, and thus one will have constraints even without degrees of freedom.
The index of an operator is precisely the [[Euler characteristic]] of the 2-term complex 0 → ''V'' → ''W'' → 0. In [[operator theory]], the index of [[Fredholm operator]]s is an object of study, with a major result being the [[Atiyah–Singer index theorem]].<ref>{{SpringerEOM|title=Index theory|id=Index_theory&oldid=23864|first=Victor|last=Nistor}}: "The main question in index theory is to provide index formulas for classes of Fredholm operators ... Index theory has become a subject on its own only after M. F. Atiyah and I. Singer published their index theorems"</ref>
The index of an operator is precisely the [[Euler characteristic]] of the 2-term complex {{math|0 → ''V'' → ''W'' → 0}}. In [[operator theory]], the index of [[Fredholm operator]]s is an object of study, with a major result being the [[Atiyah–Singer index theorem]].<ref>{{SpringerEOM|title=Index theory|id=Index_theory&oldid=23864|first=Victor|last=Nistor}}: "The main question in index theory is to provide index formulas for classes of Fredholm operators ... Index theory has become a subject on its own only after M. F. Atiyah and I. Singer published their index theorems"</ref>
==Algebraic classifications of linear transformations==
== Algebraic classifications of linear transformations ==
No classification of linear maps could be exhaustive. The following incomplete list enumerates some important classifications that do not require any additional structure on the vector space.
No classification of linear maps could be exhaustive. The following incomplete list enumerates some important classifications that do not require any additional structure on the vector space.
Let {{mvar|V}} and {{mvar|W}} denote vector spaces over a field {{mvar|F}} and let {{math|''T'': ''V'' → ''W''}} be a linear map.
Let {{mvar|V}} and {{mvar|W}} denote vector spaces over a field {{mvar|F}} and let {{math|''T'' : ''V'' → ''W''}} be a linear map.
===Monomorphism===
=== Monomorphism ===
{{mvar|T}} is said to be ''[[injective]]'' or a ''[[monomorphism]]'' if any of the following equivalent conditions are true:
{{mvar|T}} is said to be ''[[injective]]'' or a ''[[monomorphism]]'' if any of the following equivalent conditions are true:
# {{mvar|T}} is [[injective|one-to-one]] as a map of [[set (mathematics)|sets]].
# {{mvar|T}} is [[injective|one-to-one]] as a map of [[set (mathematics)|sets]].
# {{math|1=ker ''T'' = {0<sub>''V''</sub>} }}
# {{math|1=ker ''T'' = {0<sub>''V''</sub>} }}
# {{math|1=dim(ker ''T'') = 0}}
# {{math|1=dim(ker ''T'') = 0}}
# {{mvar|T}} is [[monic morphism|monic]] or left-cancellable, which is to say, for any vector space {{mvar|U}} and any pair of linear maps {{math|''R'': ''U'' → ''V''}} and {{math|''S'': ''U'' → ''V''}}, the equation {{math|1=''TR'' = ''TS''}} implies {{math|1=''R'' = ''S''}}.
# {{mvar|T}} is [[monic morphism|monic]] or left-cancellable, which is to say, for any vector space {{mvar|U}} and any pair of linear maps {{math|''R'': ''U'' → ''V''}} and {{math|''S'' : ''U'' → ''V''}}, the equation {{math|1=''TR'' = ''TS''}} implies {{math|1=''R'' = ''S''}}.
# {{mvar|T}} is [[inverse (ring theory)|left-invertible]], which is to say there exists a linear map {{math|''S'': ''W'' → ''V''}} such that {{math|''ST''}} is the [[Identity function|identity map]] on {{mvar|V}}.
# {{mvar|T}} is [[inverse (ring theory)|left-invertible]], which is to say there exists a linear map {{math|''S'' : ''W'' → ''V''}} such that {{math|''ST''}} is the [[identity map]] on {{mvar|V}}.
===Epimorphism===
=== Epimorphism ===
{{mvar|T}} is said to be ''[[surjective]]'' or an ''[[epimorphism]]'' if any of the following equivalent conditions are true:
{{mvar|T}} is said to be ''[[surjective]]'' or an ''[[epimorphism]]'' if any of the following equivalent conditions are true:
# {{mvar|T}} is [[surjective|onto]] as a map of sets.
# {{mvar|T}} is [[epimorphism|epic]] or right-cancellable, which is to say, for any vector space {{mvar|U}} and any pair of linear maps {{math|''R'': ''W'' → ''U''}} and {{math|''S'': ''W'' → ''U''}}, the equation {{math|1=''RT'' = ''ST''}} implies {{math|1=''R'' = ''S''}}.
# {{mvar|T}} is [[epimorphism|epic]] or right-cancellable, which is to say, for any vector space {{mvar|U}} and any pair of linear maps {{math|''R'' : ''W'' → ''U''}} and {{math|''S'' : ''W'' → ''U''}}, the equation {{math|1=''RT'' = ''ST''}} implies {{math|1=''R'' = ''S''}}.
# {{mvar|T}} is [[inverse (ring theory)|right-invertible]], which is to say there exists a linear map {{math|''S'': ''W'' → ''V''}} such that {{math|''TS''}} is the [[Identity function|identity map]] on {{mvar|W}}.
# {{mvar|T}} is [[inverse (ring theory)|right-invertible]], which is to say there exists a linear map {{math|''S'' : ''W'' → ''V''}} such that {{math|''TS''}} is the [[identity map]] on {{mvar|W}}.
{{mvar|T}} is said to be an ''[[isomorphism]]'' if it is both left- and right-invertible. This is equivalent to {{mvar|T}} being both one-to-one and onto (a [[bijection]] of sets) or also to {{mvar|T}} being both epic and monic, and so being a [[bimorphism]].
{{mvar|T}} is said to be an ''[[isomorphism]]'' if it is both left- and right-invertible. This is equivalent to {{mvar|T}} being both one-to-one and onto (a [[bijection]] of sets) or also to {{mvar|T}} being both epic and monic, and so being a [[bimorphism]].
{{pb}}
{{pb}}
If {{math|''T'': ''V'' → ''V''}} is an endomorphism, then:
If {{math|''T'' : ''V'' → ''V''}} is an endomorphism, then:
* If, for some positive integer {{mvar|n}}, the {{mvar|n}}-th iterate of {{mvar|T}}, {{math|''T''<sup>''n''</sup>}}, is identically zero, then {{mvar|T}} is said to be [[nilpotent]].
* If, for some positive integer {{mvar|n}}, the {{mvar|n}}th iterate of {{mvar|T}}, {{math|''T''<sup>''n''</sup>}}, is identically zero, then {{mvar|T}} is said to be [[nilpotent]].
* If {{math|1=''T''<sup>2</sup> = ''T''}}, then {{mvar|T}} is said to be [[idempotent]]
* If {{math|1=''T''<sup>2</sup> = ''T''}}, then {{mvar|T}} is said to be [[idempotent]]
* If {{math|1=''T'' = ''kI''}}, where {{mvar|k}} is some scalar, then {{mvar|T}} is said to be a scaling transformation or scalar multiplication map; see [[scalar matrix]].
* If {{math|1=''T'' = ''kI''}}, where {{mvar|k}} is some scalar, then {{mvar|T}} is said to be a scaling transformation or scalar multiplication map; see [[scalar matrix]].
==Change of basis==
== Change of basis ==
{{Main|Basis (linear algebra)|Change of basis}}
{{main|Basis (linear algebra)|Change of basis}}
Given a linear map which is an [[endomorphism]] whose matrix is ''A'', in the basis ''B'' of the space it transforms vector coordinates [u] as [v] = ''A''[u]. As vectors change with the inverse of ''B'' (vectors coordinates are [[Covariance and contravariance of vectors|contravariant]]) its inverse transformation is [v] = ''B''[v'].
Given a linear map which is an [[endomorphism]] whose matrix is {{math|''A''}}, in the basis {{math|''B''}} of the space it transforms vector coordinates {{math|[''u'']}} as {{math|1=[''v''] = ''A''[''u'']}}. As vectors change with the inverse of {{math|''B''}} (vectors coordinates are [[Covariance and contravariance of vectors|contravariant]]) its inverse transformation is {{math|1=[''v''] = ''B''[''v''′]}}.
Therefore, the matrix in the new basis is ''A′'' = ''B''<sup>−1</sup>''AB'', being ''B'' the matrix of the given basis.
Therefore, the matrix in the new basis is {{math|1=''A''′ = ''B''<sup>−1</sup>''AB''}}, being {{math|''B''}} the matrix of the given basis.
Therefore, linear maps are said to be 1-co- 1-contra-[[covariance and contravariance of vectors|variant]] objects, or type (1, 1) [[tensor]]s.
Therefore, linear maps are said to be 1-co- 1-contra-[[covariance and contravariance of vectors|variant]] objects, or type (1, 1) [[tensor]]s.
==Continuity==
== Continuity ==
{{Main|Continuous linear operator|Discontinuous linear map}}
{{main|Continuous linear operator|Discontinuous linear map}}
A ''linear transformation'' between [[topological vector space]]s, for example [[normed space]]s, may be [[continuous function (topology)|continuous]]. If its domain and codomain are the same, it will then be a [[continuous linear operator]]. A linear operator on a normed linear space is continuous if and only if it is [[bounded operator|bounded]], for example, when the domain is finite-dimensional.<ref>{{harvnb|Rudin|1991|page=15}}
A ''linear transformation'' between [[topological vector space]]s, for example [[normed space]]s, may be [[continuous function (topology)|continuous]]. If its domain and codomain are the same, it will then be a [[continuous linear operator]]. A linear operator on a normed linear space is continuous if and only if it is [[bounded operator|bounded]], for example, when the domain is finite-dimensional.<ref>{{harvnb|Rudin|1991|page=15}}
'''1.18 Theorem''' ''Let <math display="inline">\Lambda</math> be a linear functional on a topological vector space {{mvar|X}}. Assume <math display="inline">\Lambda \mathbf x \neq 0</math> for some <math display="inline">\mathbf x \in X</math>. Then each of the following four properties implies the other three:''
'''1.18 Theorem''' ''Let <math display="inline">\Lambda</math> be a linear functional on a topological vector space {{mvar|X}}. Assume {{tmath| \Lambda \mathbf x \neq 0 }} for some {{tmath| \mathbf x \in X }}. Then each of the following four properties implies the other three'':
{{ordered list
{{ordered list
|list-style-type=lower-alpha
|list-style-type=lower-alpha
Line 259:
Line 241:
|The null space <math display="inline">N(\Lambda)</math> is closed.
|The null space <math display="inline">N(\Lambda)</math> is closed.
|<math display="inline">N(\Lambda)</math> is not dense in {{mvar|X}}.
|<math display="inline">N(\Lambda)</math> is not dense in {{mvar|X}}.
|<math display="inline">\Lambda</math> is bounded in some neighbourhood {{mvar|V}} of 0.}}</ref> An infinite-dimensional domain may have [[discontinuous linear operator]]s.
|<math display="inline">\Lambda</math> is bounded in some neighbourhood {{mvar|V}} of {{math|0}}.}}</ref> An infinite-dimensional domain may have [[discontinuous linear operator]]s.
An example of an unbounded, hence discontinuous, linear transformation is differentiation on the space of smooth functions equipped with the supremum norm (a function with small values can have a derivative with large values, while the derivative of 0 is 0). For a specific example, {{math|sin(''nx'')/''n''}} converges to 0, but its derivative {{math|cos(''nx'')}} does not, so differentiation is not continuous at 0 (and by a variation of this argument, it is not continuous anywhere).
An example of an unbounded, hence discontinuous, linear transformation is differentiation on the space of smooth functions equipped with the supremum norm (a function with small values can have a derivative with large values, while the derivative of {{math|0}} is {{math|0}}). For a specific example, {{math|sin(''nx'')/''n''}} converges to {{math|0}}, but its derivative {{math|cos(''nx'')}} does not, so differentiation is not continuous at {{math|0}} (and by a variation of this argument, it is not continuous anywhere).
==Applications==
== Applications ==
A specific application of linear maps is for [[geometric transformation]]s, such as those performed in [[computer graphics]], where the translation, rotation and scaling of 2D or 3D objects is performed by the use of a [[transformation matrix]]. Linear mappings also are used as a mechanism for describing change: for example in calculus correspond to derivatives; or in relativity, used as a device to keep track of the local transformations of reference frames.
A specific application of linear maps is for [[geometric transformation]]s, such as those performed in [[computer graphics]], where the translation, rotation and scaling of 2D or 3D objects is performed by the use of a [[transformation matrix]]. Linear mappings also are used as a mechanism for describing change: for example in calculus correspond to derivatives; or in relativity, used as a device to keep track of the local transformations of reference frames.
Another application of these transformations is in [[compiler optimizations]] of nested-loop code, and in [[parallelizing compiler]] techniques.
Another application of these transformations is in [[compiler optimizations]] of nested-loop code, and in [[parallelizing compiler]] techniques.
*{{cite book |last1=Bronshtein |first1= I. N. |last2= Semendyayev |first2= K. A. |year=2004 |title= [[Bronshtein and Semendyayev|Handbook of Mathematics]] |edition= 4th |location= New York |publisher= Springer-Verlag |isbn=3-540-43491-7}}
* {{cite book |last1=Bronshtein |first1= I. N. |last2= Semendyayev |first2= K. A. |year=2004 |title= [[Handbook of Mathematics]] |edition= 4th |location= New York |publisher= Springer-Verlag |isbn=3-540-43491-7}}
* {{Rudin Walter Functional Analysis|edition=1}} <!-- {{sfn|Rudin|1976|p=}} -->
* {{Rudin Walter Functional Analysis|edition=1}} <!-- {{sfn|Rudin|1976|p=}} -->
*{{cite book|last=Rudin|first=Walter|author-link=Walter Rudin|year=1976|edition=3rd|series=Walter Rudin Student Series in Advanced Mathematics|location=New York|url=https://archive.org/details/PrinciplesOfMathematicalAnalysis|title=Principles of Mathematical Analysis|publisher=McGraw–Hill|isbn=978-0-07-054235-8}}
* {{cite book|last=Rudin|first=Walter|author-link=Walter Rudin|year=1976|edition=3rd|series=Walter Rudin Student Series in Advanced Mathematics|location=New York|url=https://archive.org/details/PrinciplesOfMathematicalAnalysis|title=Principles of Mathematical Analysis|publisher=McGraw–Hill|isbn=978-0-07-054235-8}}
* {{Rudin Walter Functional Analysis|edition=2}} <!--{{sfn|Rudin|1991|p=}}-->
* {{Rudin Walter Functional Analysis|edition=2}} <!--{{sfn|Rudin|1991|p=}}-->
* {{Schechter Handbook of Analysis and Its Foundations}} <!--{{sfn|Schechter|1996|p=}}-->
* {{Schechter Handbook of Analysis and Its Foundations}} <!--{{sfn|Schechter|1996|p=}}-->
* {{Swartz An Introduction to Functional Analysis}} <!--{{sfn|Swartz|1992|p=}}-->
* {{Swartz An Introduction to Functional Analysis}} <!--{{sfn|Swartz|1992|p=}}-->
* {{Cite book|last=Tu|first=Loring W.|title=An Introduction to Manifolds|publisher=[[Springer Science+Business Media|Springer]]|year=2011|isbn=978-0-8218-4419-9|edition=2nd|author-link=Loring W. Tu}}
* {{cite book|last=Tu|first=Loring W.|title=An Introduction to Manifolds|title-link=An Introduction to Manifolds|publisher=[[Springer Science+Business Media|Springer]]|year=2011|isbn=978-0-8218-4419-9|edition=2nd|author-link=Loring W. Tu}}
* {{Wilansky Modern Methods in Topological Vector Spaces|edition=1}} <!--{{sfn|Wilansky|2013|p=}}-->
* {{Wilansky Modern Methods in Topological Vector Spaces|edition=1}} <!--{{sfn|Wilansky|2013|p=}}-->
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[[Category:Abstract algebra]]
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Latest revision as of 16:13, 28 June 2026
Template:Short descriptionScript error: No such module "redirect hatnote".Script error: No such module "redirect hatnote".Script error: No such module "Distinguish".Script error: No such module "Unsubst".
In mathematics, and more specifically in linear algebra, a linear map (or linear mapping) is a particular kind of function between vector spaces, which respects the basic operations of vector addition and scalar multiplication. A standard example of a linear map is an matrix, which takes vectors in -dimensions into vectors in -dimensions in a way that is compatible with addition of vectors, and multiplication of vectors by scalars.
Let and be vector spaces over the same fieldTemplate:Tmath, such as the real or complex numbers.
A function is said to be a linear map if for any two vectors and any scalar the following two conditions are satisfied:
Homogeneity of degree 1 / operation of scalar multiplication
Thus, a linear map is said to be operation preserving. In other words, it does not matter whether the linear map is applied before (the right sides of the above examples) or after (the left sides of the examples) the operations of addition and scalar multiplication.
Denoting the zero elements of the vector spaces and by and respectively, it follows that Template:Tmath. Let and in the equation for homogeneity of degree 1:
A linear map with viewed as a one-dimensional vector space over itself is called a linear functional.[4]
These statements generalize to any left-module over a ring without modification, and to any right-module upon reversing of the scalar multiplication.
If is an isometry between real normed spaces such that then is a linear map. This result is not necessarily true for complex normed space.Script error: No such module "Footnotes".Script error: No such module "Check for unknown parameters".
An indefinite integral (or antiderivative) with a fixed integration starting point defines a linear map from the space of all real-valued integrable functions on to the space of all real-valued, differentiable functions on Template:Tmath. Without a fixed starting point, the antiderivative maps to the quotient space of the differentiable functions by the linear space of constant functions.
If and are finite-dimensional vector spaces over a field Template:Mvar, of respective dimensions Template:Mvar and Template:Mvar, then the function that maps linear maps to n × mScript error: No such module "Check for unknown parameters". matrices in the way described in Template:Slink (below) is a linear map, and even a linear isomorphism.
The function is homogeneous: It does not matter whether a vector is first scaled and then mapped or first mapped and then scaled:
Linear endomorphisms and isomorphisms
If a linear map is a bijection then it is called a <templatestyles src="Template:Visible anchor/styles.css" />linear isomorphism. In the case where Template:Tmath, a linear map is called a linear endomorphism. Sometimes the term <templatestyles src="Template:Visible anchor/styles.css" />linear operator refers to this case,[6] but the term "linear operator" can have different meanings for different conventions.
Linear extensions
Often, a linear map is constructed by defining it on a subset of a vector space and then Template:Em to the linear span of the domain.
Suppose and are vector spaces and is a function defined on some subset Template:Tmath.
Then a <templatestyles src="Template:Visible anchor/styles.css" />linear extension of to if it exists, is a linear map defined on that extends[note 3] (meaning that for all Template:Tmath) and takes its values from the codomain of Template:Tmath.Script error: No such module "Footnotes".Script error: No such module "Check for unknown parameters".
When the subset is a vector subspace of then a (Template:Tmath-valued) linear extension of to all of is guaranteed to exist if (and only if) is a linear map.Script error: No such module "Footnotes".Script error: No such module "Check for unknown parameters". In particular, if has a linear extension to then it has a linear extension to all of Template:Tmath.
The map can be extended to a linear map if and only if whenever is an integer, are scalars, and are vectors such that Template:Tmath, then necessarily Template:Tmath.Script error: No such module "Footnotes".Script error: No such module "Check for unknown parameters".
If a linear extension of exists then the linear extension is unique and
holds for all Template:Tmath, and as above.Script error: No such module "Footnotes".Script error: No such module "Check for unknown parameters".
If is linearly independent then every function into any vector space has a linear extension to a (linear) map (the converse is also true).
For example, if and then the assignment and can be linearly extended from the linearly independent set of vectors to a linear map on Template:Tmath. The unique linear extension is the map that sends to
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If and are finite-dimensional vector spaces and a basis is defined for each vector space, then every linear map from to can be represented by a matrix.[7] This is useful because it allows concrete calculations. Matrices yield examples of linear maps: if is a real matrix, then describes a linear map (see Euclidean space).
Let be a basis for Template:Tmath. Then every vector is uniquely determined by the coefficients in the field Template:Tmath:
If is a linear map,
which implies that the function f is entirely determined by the vectors Template:Tmath. Now let be a basis for Template:Tmath. Then we can represent each vector as
Thus, the function is entirely determined by the values of Template:Tmath. If we put these values into an matrix Template:Tmath, then we can conveniently use it to compute the vector output of for any vector in Template:Tmath. To get Template:Tmath, every column of is a vector
corresponding to as defined above. To define it more clearly, for some column that corresponds to the mapping Template:Tmath,
where is the matrix of Template:Tmath. In other words, every column has a corresponding vector whose coordinates are the elements of column Template:Tmath. A single linear map may be represented by many matrices. This is because the values of the elements of a matrix depend on the bases chosen.
The matrices of a linear transformation can be represented visually:
Such that starting in the bottom left corner and looking for the bottom right corner Template:Tmath, one would left-multiply—that is, Template:Tmath. The equivalent method would be the "longer" method going clockwise from the same point such that is left-multiplied with Template:Tmath, or Template:Tmath.
Examples in two dimensions
In two-dimensional space R2 linear maps are described by 2 × 2 matrices. These are some examples:
If a linear map is only composed of rotation, reflection, and/or uniform scaling, then the linear map is a conformal linear transformation.
Vector space of linear maps
The composition of linear maps is linear: if and are linear, then so is their compositionTemplate:Tmath. It follows from this that the class of all vector spaces over a given field K, together with linear maps as morphisms, forms a category.
The inverse of a linear map, when defined, is again a linear map.
Thus the set of linear maps from to itself forms a vector space over Template:Tmath,[8] sometimes denoted Template:Tmath.[9] Furthermore, in the case that Template:Tmath, this vector space, denoted Template:Tmath, is an associative algebra under composition of maps, since the composition of two linear maps is again a linear map, and the composition of maps is always associative. This case is discussed in more detail below.
Given again the finite-dimensional case, if bases have been chosen, then the composition of linear maps corresponds to the matrix multiplication, the addition of linear maps corresponds to the matrix addition, and the multiplication of linear maps with scalars corresponds to the multiplication of matrices with scalars.
Endomorphisms and automorphisms
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A linear transformation is an endomorphism of ; the set of all such endomorphisms together with addition, composition and scalar multiplication as defined above forms an associative algebra with identity element over the field (and in particular a ring). The multiplicative identity element of this algebra is the identity mapTemplate:Tmath.
The number is also called the rank of and written as Template:Tmath, or sometimes, Template:Tmath;[11][12] the number is called the nullity of and written as or Template:Tmath.[11][12] If and are finite-dimensional, bases have been chosen and is represented by the matrix Template:Tmath, then the rank and nullity of are equal to the rank and nullity of the matrix Template:Tmath, respectively.
Cokernel
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A subtler invariant of a linear transformation is the cokernel, which is defined as
This is the dual notion to the kernel: just as the kernel is a subspace of the domain, the co-kernel is a quotient space of the target. Formally, one has the exact sequence
These can be interpreted thus: given a linear equation f(v) = wScript error: No such module "Check for unknown parameters". to solve,
the kernel is the space of solutions to the homogeneous equation f(v) = 0Script error: No such module "Check for unknown parameters"., and its dimension is the number of degrees of freedom in the space of solutions, if it is not empty;
the co-kernel is the space of constraints that the solutions must satisfy, and its dimension is the maximal number of independent constraints.
The dimension of the co-kernel and the dimension of the image (the rank) add up to the dimension of the target space. For finite dimensions, this means that the dimension of the quotient space W / f(V)Script error: No such module "Check for unknown parameters". is the dimension of the target space minus the dimension of the image.
As a simple example, consider the map f : R2 → R2Script error: No such module "Check for unknown parameters"., given by f(x, y) = (0, y)Script error: No such module "Check for unknown parameters".. Then for an equation f(x, y) = (a, b)Script error: No such module "Check for unknown parameters". to have a solution, we must have a = 0Script error: No such module "Check for unknown parameters". (one constraint), and in that case the solution space is (x, b)Script error: No such module "Check for unknown parameters". or equivalently stated,
(0, b) + (x, 0)Script error: No such module "Check for unknown parameters"., (one degree of freedom). The kernel may be expressed as the subspace (x, 0) < VScript error: No such module "Check for unknown parameters".: the value of xScript error: No such module "Check for unknown parameters". is the freedom in a solution – while the cokernel may be expressed via the map W → RScript error: No such module "Check for unknown parameters"., Template:Tmath: given a vector (a, b)Script error: No such module "Check for unknown parameters"., the value of aScript error: No such module "Check for unknown parameters". is the obstruction to there being a solution.
An example illustrating the infinite-dimensional case is afforded by the map f : R∞ → R∞Script error: No such module "Check for unknown parameters"., with b1 = 0Script error: No such module "Check for unknown parameters". and bn + 1 = anScript error: No such module "Check for unknown parameters". for n > 0Script error: No such module "Check for unknown parameters".. Its image consists of all sequences with first element 0Script error: No such module "Check for unknown parameters"., and thus its cokernel consists of the classes of sequences with identical first element. Thus, whereas its kernel has dimension 0 (it maps only the zero sequence to the zero sequence), its co-kernel has dimension 1. Since the domain and the target space are the same, the rank and the dimension of the kernel add up to the same sum as the rank and the dimension of the co-kernel (Template:Tmath), but in the infinite-dimensional case it cannot be inferred that the kernel and the co-kernel of an endomorphism have the same dimension (0 ≠ 1Script error: No such module "Check for unknown parameters".). The reverse situation obtains for the map h : R∞ → R∞Script error: No such module "Check for unknown parameters"., with cn = an + 1Script error: No such module "Check for unknown parameters".. Its image is the entire target space, and hence its co-kernel has dimension 0, but since it maps all sequences in which only the first element is non-zero to the zero sequence, its kernel has dimension 1.
Index
For a linear operator with finite-dimensional kernel and co-kernel, one may define index as:
namely the degrees of freedom minus the number of constraints.
For a transformation between finite-dimensional vector spaces, this is just the difference dim(V) − dim(W), by rank–nullity. This gives an indication of how many solutions or how many constraints one has: if mapping from a larger space to a smaller one, the map may be onto, and thus will have degrees of freedom even without constraints. Conversely, if mapping from a smaller space to a larger one, the map cannot be onto, and thus one will have constraints even without degrees of freedom.
Algebraic classifications of linear transformations
No classification of linear maps could be exhaustive. The following incomplete list enumerates some important classifications that do not require any additional structure on the vector space.
Let Template:Mvar and Template:Mvar denote vector spaces over a field Template:Mvar and let T : V → WScript error: No such module "Check for unknown parameters". be a linear map.
ker T = {0V}Script error: No such module "Check for unknown parameters".
dim(ker T) = 0Script error: No such module "Check for unknown parameters".
Template:Mvar is monic or left-cancellable, which is to say, for any vector space Template:Mvar and any pair of linear maps R: U → VScript error: No such module "Check for unknown parameters". and S : U → VScript error: No such module "Check for unknown parameters"., the equation TR = TSScript error: No such module "Check for unknown parameters". implies R = SScript error: No such module "Check for unknown parameters"..
Template:Mvar is left-invertible, which is to say there exists a linear map S : W → VScript error: No such module "Check for unknown parameters". such that STScript error: No such module "Check for unknown parameters". is the identity map on Template:Mvar.
cokerT = {0W}Script error: No such module "Check for unknown parameters".
Template:Mvar is epic or right-cancellable, which is to say, for any vector space Template:Mvar and any pair of linear maps R : W → UScript error: No such module "Check for unknown parameters". and S : W → UScript error: No such module "Check for unknown parameters"., the equation RT = STScript error: No such module "Check for unknown parameters". implies R = SScript error: No such module "Check for unknown parameters"..
Template:Mvar is right-invertible, which is to say there exists a linear map S : W → VScript error: No such module "Check for unknown parameters". such that TSScript error: No such module "Check for unknown parameters". is the identity map on Template:Mvar.
Isomorphism
Template:Mvar is said to be an isomorphism if it is both left- and right-invertible. This is equivalent to Template:Mvar being both one-to-one and onto (a bijection of sets) or also to Template:Mvar being both epic and monic, and so being a bimorphism.
Template:Pb
If T : V → VScript error: No such module "Check for unknown parameters". is an endomorphism, then:
If T2 = TScript error: No such module "Check for unknown parameters"., then Template:Mvar is said to be idempotent
If T = kIScript error: No such module "Check for unknown parameters"., where Template:Mvar is some scalar, then Template:Mvar is said to be a scaling transformation or scalar multiplication map; see scalar matrix.
Change of basis
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Given a linear map which is an endomorphism whose matrix is AScript error: No such module "Check for unknown parameters"., in the basis BScript error: No such module "Check for unknown parameters". of the space it transforms vector coordinates [u]Script error: No such module "Check for unknown parameters". as [v] = A[u]Script error: No such module "Check for unknown parameters".. As vectors change with the inverse of BScript error: No such module "Check for unknown parameters". (vectors coordinates are contravariant) its inverse transformation is [v] = B[v′]Script error: No such module "Check for unknown parameters"..
Substituting this in the first expression
hence
Therefore, the matrix in the new basis is A′ = B−1ABScript error: No such module "Check for unknown parameters"., being BScript error: No such module "Check for unknown parameters". the matrix of the given basis.
Therefore, linear maps are said to be 1-co- 1-contra-variant objects, or type (1, 1) tensors.
Continuity
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An example of an unbounded, hence discontinuous, linear transformation is differentiation on the space of smooth functions equipped with the supremum norm (a function with small values can have a derivative with large values, while the derivative of 0Script error: No such module "Check for unknown parameters". is 0Script error: No such module "Check for unknown parameters".). For a specific example, sin(nx)/nScript error: No such module "Check for unknown parameters". converges to 0Script error: No such module "Check for unknown parameters"., but its derivative cos(nx)Script error: No such module "Check for unknown parameters". does not, so differentiation is not continuous at 0Script error: No such module "Check for unknown parameters". (and by a variation of this argument, it is not continuous anywhere).
Applications
A specific application of linear maps is for geometric transformations, such as those performed in computer graphics, where the translation, rotation and scaling of 2D or 3D objects is performed by the use of a transformation matrix. Linear mappings also are used as a mechanism for describing change: for example in calculus correspond to derivatives; or in relativity, used as a device to keep track of the local transformations of reference frames.
↑Although using the same symbol +, the operation defined in and that defined in are not necessarily same.
↑One map is said to [[Extension of a function|Template:Em]] another map if when is defined at a point Template:Tmath, then so is and
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References
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↑Script error: No such module "Footnotes". Here are some properties of linear mappings whose proofs are so easy that we omit them; it is assumed that and :
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↑Script error: No such module "Footnotes".. Suppose now that Template:Mvar and Template:Mvar are vector spaces over the same scalar field. A mapping is said to be linear if for all and all scalars and Template:Tmath. Note that one often writes Template:Tmath, rather than Template:Tmath, when is linear.
↑Script error: No such module "Footnotes".. A mapping Template:Mvar of a vector space Template:Mvar into a vector space Template:Mvar is said to be a linear transformation if: for all and all scalars Template:Mvar. Note that one often writes instead of if Template:Mvar is linear.
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Linear mappings of Template:Mvar onto its scalar field are called linear functionals.
↑ abScript error: No such module "Footnotes". p. 52, § 2.5.1
↑ abScript error: No such module "Footnotes". p. 90, § 50
↑Script error: No such module "Template wrapper".: "The main question in index theory is to provide index formulas for classes of Fredholm operators ... Index theory has become a subject on its own only after M. F. Atiyah and I. Singer published their index theorems"
↑Script error: No such module "Footnotes".1.18 TheoremLet be a linear functional on a topological vector space Template:Mvar. Assume Template:Tmath for some Template:Tmath. Then each of the following four properties implies the other three:
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