A linear map is a function between vector spaces that preserves the vector space structure—it respects both addition and scalar multiplication. This simple property underlies virtually all of linear algebra.
The concept of a linear map evolved alongside linear algebra itself. Arthur Cayley (1821–1895) introduced matrix algebra in 1858, implicitly using linear transformations. Giuseppe Peano (1858–1932) gave the first abstract definition of vector spaces and linear operations in 1888.
The modern "linear maps before matrices" approach emphasizes that linear maps are the fundamental objects and matrices are merely their representations with respect to chosen bases.
Linear maps appear throughout mathematics: differentiation and integration in calculus, expected value in probability, Fourier transforms in analysis. The linearity property underlies much of modern physics, from quantum mechanics to signal processing.
The concept of a linear map is central to all of linear algebra. A linear map is a function between vector spaces that respects the vector space structure—it preserves addition and scalar multiplication. This property makes linear maps remarkably well-behaved and leads to a rich theory.
Let and be vector spaces over the same field . A function is called a linear map (or linear transformation) if for all vectors and all scalars :
The linearity condition can be split into two separate properties:
These two conditions together are equivalent to the single condition in Definition 3.1. Having both conditions is sometimes more convenient for verification.
Let be a linear map. Then:
(1) Using homogeneity with :
(2) Using homogeneity with :
(3) Combining additivity and (2):
(4) Follows by induction on , using additivity and homogeneity repeatedly.
Here are fundamental examples that appear throughout mathematics:
Geometric transformations on provide intuitive examples:
Claim: The map defined by is linear.
Proof: Let and .
The following are NOT linear maps:
One of the beautiful features of linear algebra is that linear maps themselves form a vector space. This allows us to add linear maps and multiply them by scalars, creating new linear maps.
Let and be vector spaces over the same field . We denote by the set of all linear maps from to .
When , we write for , and call its elements linear operators on .
For and , we define:
With addition and scalar multiplication defined as above, is a vector space over . The zero vector is the zero map , and the additive inverse of is .
We verify that and are linear maps:
Sum is linear:
Scalar multiple is linear:
The vector space axioms follow from the corresponding properties in .
If and are finite, then:
A linear map is completely determined by its values on a basis of . If is a basis of , then can be any vector in . Each requires coordinates to specify, and there are basis vectors, giving degrees of freedom.
When we compose two linear maps, the result is again linear. This composition operation corresponds to matrix multiplication when we represent maps as matrices.
Let and . The composition is defined by:
If and , then .
For all and :
Composition of linear maps satisfies:
In general, ! This is one of the key differences from ordinary number multiplication. Even when both compositions are defined (e.g., for operators on ), they may produce different results.
Let be differentiation and be multiplication by .
For :
So .
One of the most powerful results about linear maps is that they are completely determined by their action on a basis. This is the foundation for representing linear maps as matrices.
Let be a basis of . If satisfy for all , then .
For any , we can write . Then:
Since this holds for all , we have .
Let be a basis of , and let be any vectors in . Then there exists a unique linear map such that for all .
Existence: Define by
This is well-defined since every has a unique representation as a linear combination of basis vectors. One can verify directly that is linear.
Uniqueness: Follows from Theorem 3.6.
Problem: Does there exist a linear map with and ?
Solution: Yes! Extend to a basis of by adding . Set (arbitrary choice). By Theorem 3.7, a unique linear map exists.
A proposed linear map fails to exist when:
Linear functionals are linear maps to the scalar field. They form the dual space and are fundamental in many areas of mathematics.
A linear functional (or linear form) on is a linear map , where is the scalar field of .
If , then .
Problem: Is defined by linear?
Solution: For and :
✓ T is linear.
Problem: Find .
Solution:
Therefore, .
Problem: Show is not linear.
Solution: Check homogeneity:
Since , T is NOT linear.
Problem: Let and . Find and .
Solution:
Note: .
Problem: Does there exist a linear map with
Solution: No! If were linear:
But the condition says . Contradiction!
Problem: Show that given by is a linear functional.
Solution: For matrices and scalar :
✓ Trace is a linear functional.
If , then is definitely NOT linear. This is a quick first check when testing linearity.
in general! Even for operators on the same space, composition order matters.
is NOT linear if . This is an affine map. Linear maps through the origin: .
Linear maps preserve dependence but not independence. If vectors are dependent, their images must be dependent. But independent vectors can map to dependent ones.
Both additivity AND homogeneity must hold. Some maps satisfy one but not the other (especially over certain fields).
for all vectors and scalars. Equivalently: additivity + homogeneity.
, , and linear maps preserve linear combinations and dependence.
is a vector space with . Composition is associative but not commutative.
A linear map is uniquely determined by its values on a basis. Given basis values, there exists a unique linear extension.
Linear maps are the central objects of study in linear algebra. They connect to every major topic in the subject and provide the framework for understanding matrices, determinants, eigenvalues, and more.
Every linear map between finite-dimensional spaces can be represented by a matrix once we choose bases for and . The matrix encodes the images of basis vectors as its columns.
Two fundamental subspaces associated with a linear map :
The Rank-Nullity Theorem relates these: .
A linear map is an isomorphism if it is bijective. For linear maps between spaces of the same dimension, the following are equivalent:
For a linear operator , an eigenvector is a nonzero vector such that for some scalar (the eigenvalue).
Eigenvalues reveal the intrinsic behavior of linear operators and are essential for diagonalization, solving differential equations, and many applications.
The dual space consists of all linear functionals on . Every linear map induces a dual map .
The dual perspective provides powerful tools for understanding linear algebra through row operations, transpose matrices, and annihilators.
Problem: Prove that the rotation by angle is linear.
Solution: The rotation is given by:
For any vectors and scalars :
Problem: Show that defined by is linear.
Solution: For differentiable functions and scalars :
This follows from the linearity of differentiation in calculus.
Problem: Show that expected value on a space of random variables is linear.
Solution: The fundamental property of expected value is:
This is exactly the linearity condition! Expected value is a linear functional.
Problem: Show that defined by is linear.
Solution: For matrices and scalars :
This uses the properties and .
Problem: On the space of sequences , define the right shift . Is this linear?
Solution: Yes! For sequences and scalars :
If is linear and is linearly dependent in , then is linearly dependent in .
Since is dependent, there exist scalars , not all zero, such that . Applying :
The same (non-all-zero) scalars show that is linearly dependent.
The converse is false! A linear map can take linearly independent vectors to linearly dependent vectors. For example, the projection maps the independent set to , which is dependent.
If is a basis of and is linear, then:
Any equals for some . Since :
Conversely, any element of the span is in the image since each .
For any linear map with :
Let be linear and be a subspace of . Then:
Problem 1
Let be defined by . Verify that is linear and find .
Problem 2
Prove or disprove: The map defined by is linear.
Problem 3
Find .
Problem 4
Let be linear operators. Prove that and are also linear operators on .
Problem 5
Does there exist a linear map such that and ? Justify your answer.
Problem 6
Let . Show that is a vector space and that the evaluation map defined by is a linear functional.
| Concept | Definition/Formula |
|---|---|
| Linear Map | |
| Zero Property | always |
| Space of Maps | , dim = |
| Sum of Maps | |
| Scalar Multiple | |
| Composition | , generally |
| Linear Functional | , where is the scalar field |
| Basis Determination | is uniquely determined by values on any basis |
Now that you understand what linear maps are, the next steps in our journey explore:
These concepts build directly on the definition of linear maps and reveal the deep structure underlying linear algebra.
These terms are often used interchangeably, but with slight distinctions: 'Linear map' is the most general term for any linear function T: V → W. 'Linear transformation' is synonymous, though some authors prefer it when V = W. 'Linear operator' typically refers to linear maps from a space to itself (T: V → V), also called endomorphisms. 'Linear functional' specifically means a linear map to the scalar field (T: V → F).
Linearity means the map respects the vector space structure—it preserves addition and scalar multiplication. This has profound consequences: (1) A linear map is completely determined by its action on a basis, (2) Linear maps can be represented by matrices, (3) Composition of linear maps is linear, (4) The set of linear maps forms a vector space itself, (5) Many important operations (differentiation, integration, expected value) are linear.
Method 1: Verify both properties separately: (a) T(u + v) = T(u) + T(v) for all u, v (additivity), and (b) T(αv) = αT(v) for all scalars α and vectors v (homogeneity). Method 2: Verify the combined condition: T(αu + βv) = αT(u) + βT(v) for all scalars α, β and vectors u, v. Quick check: If T(0) ≠ 0, then T is NOT linear.
Not in the usual finite sense. For infinite-dimensional spaces, you would need 'infinite matrices,' but these require careful handling of convergence. In functional analysis, continuous linear maps between Banach or Hilbert spaces are studied using operator theory, which generalizes the finite-dimensional theory.
Common non-linear maps include: (1) Translation: f(x) = x + c for c ≠ 0 (fails T(0) = 0), (2) Squaring: f(x) = x² (not homogeneous), (3) Absolute value: f(x) = |x| (not homogeneous), (4) Determinant: det(cA) = c^n det(A) ≠ c·det(A) for n > 1, (5) Any function with a constant term.
This follows from homogeneity: T(0) = T(0·v) = 0·T(v) = 0. This is a useful quick test: if T(0) ≠ 0, the map is definitely NOT linear.
A linear functional (or linear form) is a linear map from a vector space V to its scalar field F: f: V → F. Examples include evaluation at a point f(p) = p(a), integration f(g) = ∫g(x)dx, and trace tr(A). Linear functionals form the dual space V*.
A linear map T: V → W is completely determined by its values on a basis of V. If dim(V) = m and dim(W) = n, then T(vⱼ) can be any vector in W for each basis vector vⱼ. We need n scalars for each of m basis vectors, giving mn degrees of freedom total.
No! For S ∘ T to be defined, the codomain of T must equal the domain of S. If T: V → W and S: W → U, then S ∘ T: V → U is defined and linear. But if the spaces don't match, composition is undefined.
Yes! For example, T(x, y) = (x + y, x + y) takes the independent set {(1, 0), (0, 1)} to the dependent set {(1, 1), (1, 1)}. Linear maps preserve dependence but not necessarily independence.