Linear map
Template:Short description Template:Redirect Template:Redirect Template:Distinguish Template:More footnotes needed In mathematics, and more specifically in linear algebra, a linear map, linear mapping, or linear operator 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. When the two vector spaces are the same, a linear map is also called a linear transformation or linear endomorphism.
A linear map is a homomorphism of vector spaces. Thus, a linear map satisfies Template:Tmath, where and are scalars, and and are vectors (elements of the vector space Template:Tmath). A linear mapping always maps the origin of to the origin of Template:Tmath, and linear subspaces of onto linear subspaces in (possibly of a lower dimension);[1] for example, it maps a plane through the origin in to either a plane through the origin in Template:Tmath, a line through the origin in Template:Tmath, or just the origin in Template:Tmath. Linear maps can often be represented as matrices, and simple examples include rotation and reflection linear transformations.
Definition and first consequences
Let and be vector spaces over the same field Template: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:
- Additivity / operation of addition[note 1]
- 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.
By the associativity of the addition operation denoted as +, for any vectors and scalars Template:Tmath, the following equality holds:[2][3] Thus a linear map is one which preserves linear combinations.
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.
Examples
- The unique map of the form is linear.
- A prototypical example that gives linear maps their name is a function Template:Tmath, of which the graph is a line through the origin.[5]
Examples of linear transformations used in computer graphics - More generally, any homothety centered in the origin of a vector space is a linear map (here Template:Mvar is a scalar).
- The zero map between two vector spaces (over the same field) is linear.
- The identity map on any module is a linear operator.
- For real numbers, the map is not linear.
- For real numbers, the map is not linear (but is an affine transformation).
- If is a real matrix, then defines a linear map from to by sending a column vector to the column vector Template:Tmath. Conversely, any linear map between finite-dimensional vector spaces can be represented in this manner; see Template:Slink, below.
- 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.Template:Sfn
- 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 functions (a linear operator is a linear endomorphism, that is, a linear map with the same domain and codomain). Indeed,
- A definite integral over some interval Template:Mvar is a linear map from the space of all real-valued integrable functions on Template:Mvar to Template:Tmath. Indeed,
- 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 Template:Math matrices in the way described in Template:Slink (below) is a linear map, and even a linear isomorphism.
- The expected value of a random variable is a linear function of the random variable: for random variables and we have and Template:Tmath. The conditional expectation is as well. But the variance of a random variable is not linear, because for instance Template:Tmath.
-
The function with is a linear map. This function scales the component of a vector by the factor Template:Tmath.
-
The function is additive: It does not matter whether vectors are first added and then mapped or whether they are mapped and finally added:
-
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 Template:Visible anchor. In the case where Template:Tmath, a linear map is called a linear endomorphism. Sometimes the term Template:Visible anchor 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 Template:Visible anchor of to if it exists, is a linear map defined on that extends [note 2] (meaning that for all Template:Tmath) and takes its values from the codomain of Template:Tmath.Template:Sfn 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.Template:Sfn 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.Template:Sfn If a linear extension of exists then the linear extension is unique and holds for all Template:Tmath, and as above.Template:Sfn 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
Every (scalar-valued) linear functional defined on a vector subspace of a real or complex vector space has a linear extension to all of Template:Tmath. Indeed, the Hahn–Banach dominated extension theorem even guarantees that when this linear functional is dominated by some given seminorm (meaning that holds for all in the domain of Template:Tmath) then there exists a linear extension to that is also dominated by Template:Tmath.
Matrices
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:
- Matrix for relative to Template:Tmath:
- Matrix for relative to Template:Tmath:
- Transition matrix from to Template:Tmath:
- Transition matrix from to Template:Tmath:
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:
- rotation
- by 90 degrees counterclockwise:
- by an angle θ counterclockwise:
- reflection
- through the x axis:
- through the y axis:
- through a line making an angle θ with the origin:
- scaling by 2 in all directions:
- horizontal shear mapping:
- skew of the y axis by an angle θ:
- squeeze mapping:
- projection onto the y axis:
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 composition Template: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.
If and are linear, then so is their pointwise sum Template:Tmath, which is defined by Template:Tmath.
If is linear and is an element of the ground field Template:Tmath, then the map Template:Tmath, defined by Template:Tmath, is also linear.
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
Template:Main 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 map Template:Tmath.
An endomorphism of that is also an isomorphism is called an automorphism of Template:Tmath. The composition of two automorphisms is again an automorphism, and the set of all automorphisms of forms a group, the automorphism group of which is denoted by or Template:Tmath. Since the automorphisms are precisely those endomorphisms which possess inverses under composition, is the group of units in the ring Template:Tmath.
If has finite dimension Template:Tmath, then is isomorphic to the associative algebra of all matrices with entries in Template:Tmath. The automorphism group of is isomorphic to the general linear group of all invertible matrices with entries in Template:Tmath.
Kernel, image and the rank–nullity theorem
Template:Main If is linear, we define the kernel and the image or range of by
is a subspace of and is a subspace of Template:Tmath. The following dimension formula is known as the rank–nullity theorem:[10]
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
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 Template:Math to solve,
- the kernel is the space of solutions to the homogeneous equation Template:Math, 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 Template:Math is the dimension of the target space minus the dimension of the image.
As a simple example, consider the map Template:Math, given by Template:Math. Then for an equation Template:Math to have a solution, we must have Template:Math (one constraint), and in that case the solution space is Template:Math or equivalently stated, Template:Math, (one degree of freedom). The kernel may be expressed as the subspace Template:Math: the value of Template:Math is the freedom in a solution – while the cokernel may be expressed via the map Template:Math, Template:Tmath: given a vector Template:Math, the value of Template:Math is the obstruction to there being a solution.
An example illustrating the infinite-dimensional case is afforded by the map Template:Math, with Template:Math and Template:Math for Template:Math. Its image consists of all sequences with first element Template:Math, 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 (Template:Math). The reverse situation obtains for the map Template:Math, with Template:Math. 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.
The index of an operator is precisely the Euler characteristic of the 2-term complex Template:Math. In operator theory, the index of Fredholm operators is an object of study, with a major result being the Atiyah–Singer index theorem.[13]
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 Template:Math be a linear map.
Monomorphism
Template:Mvar is said to be injective or a monomorphism if any of the following equivalent conditions are true:
- Template:Mvar is one-to-one as a map of sets.
- Template:Math
- Template:Math
- Template:Mvar is monic or left-cancellable, which is to say, for any vector space Template:Mvar and any pair of linear maps Template:Math and Template:Math, the equation Template:Math implies Template:Math.
- Template:Mvar is left-invertible, which is to say there exists a linear map Template:Math such that Template:Math is the identity map on Template:Mvar.
Epimorphism
Template:Mvar is said to be surjective or an epimorphism if any of the following equivalent conditions are true:
- Template:Mvar is onto as a map of sets.
- Template:Math
- Template:Mvar is epic or right-cancellable, which is to say, for any vector space Template:Mvar and any pair of linear maps Template:Math and Template:Math, the equation Template:Math implies Template:Math.
- Template:Mvar is right-invertible, which is to say there exists a linear map Template:Math such that Template:Math 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 Template:Math is an endomorphism, then:
- If, for some positive integer Template:Mvar, the Template:Mvarth iterate of Template:Mvar, Template:Math, is identically zero, then Template:Mvar is said to be nilpotent.
- If Template:Math, then Template:Mvar is said to be idempotent
- If Template:Math, 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
Template:Main Given a linear map which is an endomorphism whose matrix is Template:Math, in the basis Template:Math of the space it transforms vector coordinates Template:Math as Template:Math. As vectors change with the inverse of Template:Math (vectors coordinates are contravariant) its inverse transformation is Template:Math.
Substituting this in the first expression hence
Therefore, the matrix in the new basis is Template:Math, being Template:Math 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
A linear transformation between topological vector spaces, for example normed spaces, may be 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, for example, when the domain is finite-dimensional.[14] An infinite-dimensional domain may have discontinuous linear operators.
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 Template:Math is Template:Math). For a specific example, Template:Math converges to Template:Math, but its derivative Template:Math does not, so differentiation is not continuous at Template:Math (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.
Another application of these transformations is in compiler optimizations of nested-loop code, and in parallelizing compiler techniques.
See also
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- Category of matrices
- Quasilinearization
Notes
References
Bibliography
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- Template:Rudin Walter Functional Analysis
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- Template:Rudin Walter Functional Analysis
- Template:Schaefer Wolff Topological Vector Spaces
- Template:Schechter Handbook of Analysis and Its Foundations
- Template:Swartz An Introduction to Functional Analysis
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- Template:Wilansky Modern Methods in Topological Vector Spaces
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- ↑ Template:Harvnb
Here are some properties of linear mappings whose proofs are so easy that we omit them; it is assumed that and : Template:Ordered list - ↑ Template:Harvnb. 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.
- ↑ Template:Harvnb. 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.
- ↑ Template:Harvnb. Linear mappings of Template:Mvar onto its scalar field are called linear functionals.
- ↑ Template:Cite web
- ↑ "Linear transformations of Template:Mvar into Template:Mvar are often called linear operators on Template:Mvar." Template:Harvnb
- ↑ Template:Harvnb
- ↑ Template:Harvard citation text p. 52, § 3.3
- ↑ Template:Harvnb
- ↑ Template:Harvnb
- ↑ 11.0 11.1 Template:Harvard citation text p. 52, § 2.5.1
- ↑ 12.0 12.1 Template:Harvard citation text p. 90, § 50
- ↑ Template:SpringerEOM: "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"
- ↑ Template:Harvnb 1.18 Theorem Let 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: Template:Ordered list
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