A linear map takes a real polynomial of degree at most one and returns a vector in . It has infinitely many possible inputs, yet six real numbers describe it completely, three for the image of and three for the image of . This lesson explains why basis images decide everything, and then treats the linear maps between two spaces as vectors in their own right. Adding and scaling maps one input at a time makes them a vector space, and when both spaces are finite-dimensional the matrix-unit maps give that space a basis, so its dimension is the product of the two dimensions.
Key terms
Linear extension from basis images
Definition Let and be vector spaces over the same field , where is or , and let be a basis of the finite-dimensional space . For any vectors in , chosen freely and not necessarily distinct or independent, there is exactly one linear map with for . It is given by
The formula is well defined because every vector of has unique coordinates in the basis. It is linear because the coordinates of are times those of plus times those of . Any linear map with these basis images agrees with the formula, since linearity forces . Both halves of the basis hypothesis matter. If the list spans but is dependent, prescribed images can contradict each other. If it is independent but does not span, such a map exists, and it is unique only when .
In plain words A linear map is completely decided by where it sends one basis, and those images can be anything at all. The output at any vector is the same combination of the chosen images as that vector is of the basis.
Example Work over with , the real polynomials of degree at most one including the zero polynomial, with basis , and with . Choose and . The theorem gives the single linear map
For instance . Each of the two images has three free coordinates, so six real numbers describe every linear map from to .
Space of linear maps
Definition Let and be vector spaces over the same field . The set of all linear maps from to is written . For and , pointwise addition and scaling are defined at every by
Both results are again linear. For the sum, linearity of each map and regrouping in give
and a similar computation works for . With these operations is a vector space over . Its zero vector is the zero map, which sends every input to , the negative of is the map , and every other axiom holds because it holds in at each input. Two maps are equal when they agree at every input. No finite-dimensional hypothesis is needed. Composition is a different operation. It applies one map after another, needs the output space of the first map to be the input space of the second, and is not the addition of .
In plain words Two maps with the same input and output spaces are added by feeding both the same input and adding the outputs. Maps then behave like vectors, so linear combinations, bases and dimension make sense for maps too.
Example On let and . Then and , and the standard matrices add and scale entry by entry. The composition is something else, since , which differs from .
Matrix-unit maps
Definition Let and be finite-dimensional vector spaces over with bases of and of . For and , the matrix-unit map is the unique linear map with
where is when and otherwise. So sends to and every other basis vector of to . On a vector with coordinates it gives
and its matrix has a single entry , in row and column , with zeros elsewhere. The maps depend on both chosen bases.
In plain words The map reads one input coordinate, the th, and writes it as the coefficient of one output basis vector, . Everything else is ignored.
Example Take with basis and with the standard basis . There are six matrix-unit maps. Three of them read the constant coefficient, for example , and three read the coefficient of , for example . The matrix of is
Dimension of the space of linear maps
Definition Let and be finite-dimensional vector spaces over with and . The matrix-unit maps built from bases of and of form a basis of , so
The coordinates of a map in this basis are the entries of its matrix. If for each , then
To see that the maps span, apply both sides to . Linearity gives , and the right side gives the same sum, so the two maps agree at every input. For independence, suppose is the zero map and evaluate it at . Every term with vanishes, leaving , and independence of the forces . Doing this for each shows that every coefficient is zero. If or , the only linear map is the zero map, and the formula correctly gives .
In plain words A linear map from an -dimensional space to an -dimensional space is fixed by basis images, each with free coordinates. That makes independent numbers, the entries of its matrix.
Example The map from to has matrix columns and , so
with coefficient on . At the input both sides give . The space has dimension , which accounts for the six numbers in the opening.
Rank-one map
Definition The rank of a linear map is the dimension of its image . A rank-one map is a linear map whose image is one-dimensional. Over , a linear map has rank one exactly when
for some nonzero vector and some linear map that is not the zero map. If the image is the line spanned by , each equals for exactly one scalar , and linearity of makes linear. Conversely, a nonzero takes every value in , so the image of such a map is the whole line spanned by . In coordinates, an matrix over has rank one exactly when it equals a nonzero column times a nonzero row . Each matrix-unit map has rank one, since its image is the line spanned by , and so does every nonzero multiple of it. Rank-one maps do not form a subspace, since the zero map has rank zero, and a sum can also raise the rank, as on has rank two.
In plain words A rank-one map measures its input with a single number and returns that number times one fixed vector. All of its outputs lie on one line through the origin.
Example Over , the matrix
defines the map from to . Both columns are multiples of , so the image is the line through that vector, and exactly when . At the output is .
Check yourself
- A linear map satisfies and . Find a formula for and explain why these two values determine .
Show the answer
The vectors and form a basis of , because the matrix with these columns has determinant . By linear extension exactly one linear map has the two given values. Every linear map from to has the form with and . The conditions read and . Adding gives , so and , and
- Is there a linear map with , and ? And if two linear maps from to agree at the single input , must they be equal?
Show the answer
No such map exists. The three vectors span but are dependent, since . Linearity forces , which contradicts the prescribed value . Images can be prescribed freely on an independent list. On a dependent list they must satisfy every linear relation among its vectors, and on a basis they also determine the map.
The second answer is also no. The zero map and the map both send to , yet they differ at , where the second gives . Agreement on a whole basis is what forces two linear maps to be equal.
- Find over , and write the derivative map in terms of the matrix-unit maps for the bases and .
Show the answer
The spaces have dimensions and , so . The basis images are , and . In the basis their coordinates are , and , which are the columns of
Hence . As a check, the map sends to , which is its derivative.