# 2Linear Algebra Background

In this class we will mostly consider vector spaces over the reals, though it is sometimes necessary to also consider complex vector spaces. This overview of linear algebra will be incomprehensibly fast for those not already basically familiar with the concepts. Nonetheless, it is probably worth reading even if you have a strong linear algebra background, as some of the concepts we employ (such as the “quasi-matrix” perspective or our take on canonical forms) are not universally taught.

## 2.1 Vector spaces

Vectors are things that we can add together and scale in a way that is consistent with how we usually think about those words. More formally, a vector space $$\mathcal{V}$$ over a field $$\mathbb{F}$$ (which we will always take to be the real numbers $$\mathbb{R}$$ or the complex numbers $$\mathbb{C}$$) is a set together with a binary operation $$+ : \mathcal{V}\times \mathcal{V}\rightarrow \mathcal{V}$$ (addition) and $$\cdot : \mathbb{F}\times \mathcal{V}\rightarrow \mathcal{V}$$ (scalar multiplication) satisfying the following axioms:

• Commutativity: $$\forall u, v \in \mathcal{V}, u + v = v + u$$
• Associativity: $$\forall u, v \in \mathcal{V}, (u + v) + w = u + (v + w)$$
• Existence of additivity identity: $$\exists 0 \in \mathcal{V}$$ s.t. $$\forall u \in \mathcal{V}, u + 0 = u$$
• Existence of additive inverses: $$\forall u \in \mathcal{V}, \exists -u \in \mathcal{V}$$ s.t. $$u + -u = 0$$
• Scalar multiply compatibility: $$\forall \alpha, \beta \in \mathbb{F}, v \in \mathcal{V}$$, $$(\alpha \beta) v = \alpha (\beta v)$$
• Scaling by 1: If $$1 \in \mathbb{F}$$ is the multiplicative identity, then $$\forall v \in \mathcal{V}, 1 v = v$$
• Distributivity for scalar addition: $$\forall \alpha, \beta \in \mathbb{F}, u \in \mathcal{V}, (\alpha + \beta) u = \alpha u + \beta u$$
• Distributivity for vector addition: $$\forall \alpha \in \mathbb{F}, u, v \in \mathcal{V}, \alpha (u + v) = \alpha u + \alpha v$$

A subspace of a vector space is a set $$\mathcal{U}\subset \mathcal{V}$$ that is closed under addition and scaling, making $$\mathcal{U}$$ itself a vector space. The span of a set of vectors $$\mathcal{G}\subset \mathcal{V}$$ is the smallest subspace containing $$\mathcal{G}$$, i.e. everything that can be written as a linear combination of elements of $$\mathcal{G}$$, i.e. $\operatorname{span}(\mathcal{G}) = \{ u \in \mathcal{V}: u = \sum_{g \in \mathcal{G}} g c_g, c_g \in \mathbb{F}\}$ We say $$\mathcal{G}$$ is a spanning set for a subspace $$\mathcal{U}$$ if the span of $$\mathcal{G}$$ is $$\mathcal{U}$$.

Any subspace can be generated as the span of some generating set, but we place special emphasis on the case when every element $$\mathcal{U}$$ is a unique linear combination of $$\mathcal{G}$$. In this case, we say the elements of $$\mathcal{G}$$ are linearly independent. A necessary and sufficient condition for linear independence of $$\mathcal{G}\subset \mathcal{V}$$ is that the vector $$0 \in \mathcal{V}$$ has the unique representation as a linear combination $0 = \sum_{g \in \mathcal{G}} 0 g.$ If a spanning set is linear independent, it also has minimal cardinality.

If $$\mathcal{G}= \{ v_1, \ldots, v_k \}$$ is a spanning set of minimal cardinality, then any element $$u$$ in the generated set $$\mathcal{U}$$ has a unique representation $u = \sum_{j=1}^k v_j c_j$ for coefficients $$c_j \in \mathbb{F}$$. In this case, we say the set $$\mathcal{G}$$ is linearly independent.

A sum of two subspaces $$\mathcal{U}\subset \mathcal{V}$$ and $$\mathcal{W}\subset \mathcal{V}$$ is the set $$\mathcal{U}+ \mathcal{W}\equiv \{ u+w : u \in \mathcal{U}, w \in \mathcal{W}\}$$. We say $$\mathcal{U}+ \mathcal{W}$$ is a direct sum if there is a unique decomposition of each element $$v \in \mathcal{U}+ \mathcal{W}$$ as $$v = u + w$$ for $$u \in \mathcal{U}$$ and $$v \in \mathcal{V}$$. The sum $$\mathcal{U}+ \mathcal{W}$$ is a direct sum iff the unique decomposition of $$0$$ is as $$0 + 0$$. Alternately, we can say that if $$\mathcal{G}$$ and $$\mathcal{H}$$ are linearly independent on their own, then $$\operatorname{span}(\mathcal{G}) + \operatorname{span}(\mathcal{H})$$ is a direct sum iff $$\mathcal{G}\cup \mathcal{H}$$ is a linearly independent subset of $$\mathcal{V}$$. When we know a sum of subspaces is a direct sum, we often use the symbol $$\oplus$$ instead of $$+$$.

## 2.2 Examples

Some common examples of vector spaces include:

### Dual spaces

For every vector space $$\mathcal{V}$$ over a field $$\mathbb{F}$$, there is an associated dual space1 of all2 linear maps from $$\mathcal{V}$$ into $$\mathbb{F}$$ $\mathcal{V}^* = \{ w^* : \mathcal{V}\rightarrow \mathbb{F}\mbox{ s.t. } w^* \mbox{ is linear} \},$ i.e. a dual vector (also called a linear functional) $$w^* \in \mathcal{V}^*$$ represent a map such that $$w^* (\alpha v) = \alpha (w^* v)$$ and $$w^* (u+v) = w^* u + w^* v$$ for all scalars $$\alpha \in \mathbb{F}$$ and vectors $$u, v \in \mathcal{V}$$.

### Concrete spaces

Concrete vector spaces are just lists of elements of $$\mathbb{F}$$ (real or complex numbers for this class), which we conventionally arrange into a column3: $c = \begin{bmatrix} c_1 \\ \vdots \\ c_n \end{bmatrix}.$ The vector space $$\mathbb{F}^m$$ is useful both in its own right and because it is the main vector space we represent in the computer. Any finite-dimensional vector space of dimension $$n$$ can be represented as the image of $$\mathbb{F}^n$$ under a basis map.

A vector in Julia directly represents a vector in $$\mathbb{F}^n$$ as an array of floating point numbers laid out sequentially in memory. Entries in a vector in Julia are separated by semicolons or commas; if white space is used instead, the vector is interpreted as a row vector (an element of $$\mathbb{F}^{1 \times n}$$).

# Example (column) vector
[1.0; 0.0; 2.5]
3-element Vector{Float64}:
1.0
0.0
2.5
# Example row vector
[1.0  2.0  3.0]
1×3 Matrix{Float64}:
1.0  2.0  3.0

### Matrix spaces

A matrix $$A \in \mathbb{F}^{m \times n}$$ is a two-dimensional array of elements of $$a_{ij} \in \mathbb{F}$$ (real or complex) with row index $$i \in [m]$$ and column index $$j \in [n]$$4. While matrices can be seen as just a special type of concrete vector space where we use two integer indices rather than one, they are most usefully interpreted as representations of linear maps between vector spaces (or other types of maps discussed later in this chapter).

A matrix in Julia directly represents a vector in $$\mathbb{F}^{m \times n}$$ as an array of floating point numbers laid out column-by-column in memory. The same memory can be interpreted as a vector of length $$mn$$ where the entries are laid out in column-major order.

# Example of a 2-by-3 matrix
[1.0 3.0 5.0;
2.0 4.0 6.0]
2×3 Matrix{Float64}:
1.0  3.0  5.0
2.0  4.0  6.0
# Flatten a 2-by-3 matrix into a length 6 vector
let
A = [1.0 3.0 5.0;
2.0 4.0 6.0]
A[:]
end
6-element Vector{Float64}:
1.0
2.0
3.0
4.0
5.0
6.0

### Polynomial spaces

The polynomial space $$\mathcal{P}_d$$ consists of all univariate polynomials of degree at most $$d$$: $\mathcal{P}_d = \left\{ \sum_{j=0}^d c_j x^j : c_j \in \mathbb{F}\right\}.$ Polynomial spaces are very useful in applications, but they are also highly useful pedagogically as examples of familiar finite-dimensional vector spaces other than the concrete spaces $$\mathbb{F}^n$$.

Polynomials in Julia can be represented as objects from Polynomials.jl, a library that directly supports vector algebra with polynomials along with differentiation, integration, and root-finding.

let
p = Polynomial([1, 0, 2])  # Represent 1 + 2x^2
q = Polynomial([4, 5])     # Represent 4 + 5x
s = p + q                  # This should represent 5 + 5x + 2x^2
s, s(2)                    # Show s and evaluation at x = 2
end
(Polynomial(5 + 5*x + 2*x^2), 23)

Alternately, we may choose to write polynomials in Julia directly as functions. In this case, Julia does not know about addition and scalar multiplication, which must be implemented directly. So while we cannot write q = 2*p, for example, we are fine defining q(x) = 2*p(x).

let
p(x) = 1.0 + x^2/2
xs = range(-1.0, 1.0, length=100)
plot(xs, p.(xs))
end

### Linear maps

The space $$\mathcal{L}(\mathcal{U}, \mathcal{V})$$ is the space of all5 linear maps between vector spaces $$\mathcal{U}$$ and $$\mathcal{V}$$: $\mathcal{L}(\mathcal{U}, \mathcal{V}) = \{ L : \mathcal{U}\rightarrow \mathcal{V}\mbox{ s.t. } L \mbox{ is linear}\}.$ The dual space $$\mathcal{V}^* = \mathcal{L}(\mathcal{V}, \mathbb{F})$$ is an important special case.

### $$k$$-times differentiable functions

We will frequently care about the vector space of $$k$$-times continuously differentiable functions from a domain $$\Omega \subset \mathbb{F}^n$$ into $$\mathbb{F}$$. Unlike all our other examples, this is an infinite-dimensional vector space. Finite-dimensional vector spaces have a number of nice properties that infinite-dimensional vector spaces (like $$\mathcal{C}^k(\Omega, \mathbb{F})$$) often lack. The technical details of infinite-dimensional vector spaces are the topic of functional analysis courses. We will largely elide these details, but there are a few points later in the class where it will be necessary to deal with such annoyances.

## 2.3 Quasimatrices

A column-wise quasi-matrix is an ordered list of vectors $$v_1, \ldots, v_k \in \mathcal{V}$$ written as $V = \begin{bmatrix} v_1 & \ldots & v_k \end{bmatrix}.$ We refer to the vectors $$v_j$$ as the columns of the quasi-matrix. The primary use of quasi-matrices is to give us a compact notation for writing linear combinations of the columns; for a coefficient vector $$c \in \mathbb{F}^k$$, we write $Vc \equiv \sum_{j = 1}^k v_j c_j.$ Following this notation, we will use the symbol $$V$$ to refer either to the quasi-matrix or to the induced linear mapping from $$\mathbb{F}^n$$ to $$\mathcal{V}$$. The range space of $$V$$ is simply the span of the columns; we will refer to this space as either $$\mathcal{R}(V)$$ or as $$\operatorname{span}(V)$$.

In a row-wise quasi-matrix, we write a list of dual vectors $$w_1^*, \ldots, w_k^* \in \mathcal{V}^*$$ as $W^* = \begin{bmatrix} w_1^* \\ \vdots \\ w_k^* \end{bmatrix}$ A row-wise quasi-matrix gives us a compact notation for writing a concrete vector of linear functionals applied to a vector, i.e. $c = W^* v \mbox{ means } c_j = w_j^* v.$ As with column-wise quasi-matrices, we will refer interchangeably to a row-wise quasi-matrix $$W^*$$ and the induced linear map from $$\mathcal{V}\rightarrow \mathbb{F}^k$$.

A matrix $$A \in \mathbb{F}^{m \times n}$$ can be interpreted as either a column-wise quasi-matrix (where the columns of $$A$$ are viewed as vectors in $$\mathbb{F}^m$$) or as a row-wise quasi-matrix (where the rows of $$A$$ are viewed as row vectors in $$(\mathbb{F}^n)^*$$).

## 2.4 Bases

We deal with vectors from two perspectives:

• Abstract: A vector is an object that can be scaled or added to other vectors.
• Concrete: A vector is a column of numbers.

We map between the abstract and concrete pictures of (finite-dimensional) vector spaces using a basis.

A basis quasi-matrix6 for a vector space $$\mathcal{V}$$ is a quasi-matrix $$V$$ with linearly independent columns that spans $$\mathcal{V}$$ (the number of columns is the dimension of $$\mathcal{V}$$). The basis quasi-matrix represents an invertible linear map from $$\mathbb{F}^n$$ to $$\mathcal{V}$$. We write $$V^{-1}$$ to denote the inverse map, which we think of as a row-wise quasi-matrix. The rows in $$V^{-1}$$ form a basis for the dual space $$\mathcal{V}^*$$; this basis is called the dual basis to $$V$$. We note that the composition $$V^{-1} V$$ is an identity map on the concrete space $$\mathbb{F}^n$$, while $$V V^{-1}$$ is the identity map on the abstract space $$\mathcal{V}$$.

When $$W$$ and $$V$$ are two separate bases for the same space, the change of basis matrix $$A = W^{-1} V$$ tells us how to transform the coefficients in the $$V$$ basis into coefficients in the $$W$$ basis. That is, if we write $$v \in \mathcal{V}$$ as $$v = Vc = Wd$$, we have \begin{align} v &= Vc \\ d &= W^{-1} v \\ d &= W^{-1} V c = A c. \end{align} Using distributivity, we can interpret $$A$$ column-wise: the columns of $$A$$ represent the vectors $$v_1, \ldots, v_n$$ written in terms of the $$W$$ basis $d = W^{-1} v = W^{-1} \left( \sum_{j=1}^n v_j c_j \right) = \sum_{j=1}^n (W^{-1} v_j) c_j = Ac.$ The $$A$$ matrix must also be invertible, and the matrix $$A^{-1} = V^{-1} W$$ represents the linear mapping from the $$W$$ basis coefficients back to the $$V$$ basis coefficients, and the columns of $$A^{-1}$$ represent the vectors $$w_1, \ldots, w_n$$ written in terms of the $$V$$ basis.

### Example: Polynomial bases

For example, the power basis of the vector space $$\mathcal{P}_d$$ of polynomials of degree at most $$d$$ in one variable is the basis of $$d+1$$ monomials $$\begin{bmatrix} x^0 & x^1 & x^2 & \ldots & x^d \end{bmatrix}$$. Using this basis, we might concretely represent a polynomial $$p(x) = 1 + x^2/2 \in \mathcal{P}_2$$ as $p(x) = \begin{bmatrix} 1 & x & x^2 \end{bmatrix} \begin{bmatrix} 1 \\ 0 \\ 0.5 \end{bmatrix}.$ For numerical purposes, we often prefer the Chebyshev bases for $$\mathcal{P}_d$$, with basis vectors given by \begin{align} T_0(x) &= 1 \\ T_1(x) &= x \\ T_{k+1}(x) &= 2x T_k(x)-T_{k-1}(x), \mbox{ for } k \geq 1 \end{align} With respect to this basis, we might concretely represent $$p(x) = 1 + x^2/2 \in \mathcal{P}_2$$ as $p(x) = \begin{bmatrix} T_0(x) & T_1(x) & T_2(x) \end{bmatrix} \begin{bmatrix} 1.25 \\ 0 \\ 0.25 \end{bmatrix}.$

For a given degree $$d$$, let us denote the power basis and the Chebyshev bases as \begin{align} P &= \begin{bmatrix} x^0 & x^1 & \ldots & x^d \end{bmatrix} \\ T &= \begin{bmatrix} T_0(x) & T_1(X) & \ldots & T_d(x) \end{bmatrix} \end{align} The three-term recurrence relationship between the Chebyshev polynomials lets us write a simple computation for the matrix representing $$P^{-1} T$$ mapping from Chebyshev coefficients to coefficients in the power basis.

function cheb2power(d)
A = zeros(d+1, d+1)
A[1,1] = 1.0               # First column represents T_0 in power basis
if d > 1 A[2,2] = 1.0 end  # Second column represents T_1 in power basis
for j = 2:d
# Compute representation of T_{j+1} = 2*x*T_{j} - T_{j-1}
A[2:d+1,j+1] = 2*A[1:d,j]  # Multiplication by x shifts power basis coefficients
A[:,j+1] -= A[:,j-1]       # Subtract off the T_{j-1} coefficients
end
return UpperTriangular(A)
end
cheb2power (generic function with 1 method)

The 3-by-3 matrix representing the map from the Chebyshev coefficients to power coefficients can be computed by cheb2power(2).

cheb2power(2)
3×3 UpperTriangular{Float64, Matrix{Float64}}:
1.0  0.0  -1.0
⋅   1.0   0.0
⋅    ⋅    2.0

Hence, we have $T(x) = P(x) \begin{bmatrix} 1 & 0 & -1 \\ 0 & 1 & 0 \\ 0 & 0 & 2 \end{bmatrix}$ or, reading column-by-column, \begin{align} T_0(x) &= x^0 \\ T_1(x) &= x^1 \\ T_2(x) &= 2x^2 - x^0 \end{align} This matrix is upper triangular; that is, all entries below the main diagonal are zero. Intuitively, we expect this because $$T_j(x)$$ is a degree $$j$$ polynomial, so the maximum monomial involved is $$x^j$$.

To convert a vector of coefficients in the power basis into a vector of Chebyshev coefficients, we solve a linear system involving $$A = P^{-1} T$$. We prefer not to form the $$A^{-1}$$ explicitly; instead, we solve a linear system using the backslash operator.

let
A = cheb2power(2)  # Compute Chebyshev -> power basis coefficient mapping
A$1.0; 0.0; 0.5] # Solve for the Chebyshev coefficients for our example end 3-element Vector{Float64}: 1.25 0.0 0.25 ## 2.5 Norms A norm $$\|\cdot\|$$ provides a way to measure the lengths of vectors. Norms are characterized by three properties for any scalar $$\alpha$$ and vectors $$u, v$$: Positive definiteness $$\|v\| \geq 0$$; and $$\|v\| = 0$$ iff $$v = 0$$ Homogeneity $$\|\alpha v\| = |\alpha| \|v\|$$ Subadditivity (aka triangle inequality) $$\|u+v\| \leq \|u\| + \|v\|$$ All norms are equivalent on finite dimensional spaces7; that is, if $$\|\cdot\|$$ and $$\|\cdot\|_*$$ are two different norms on a finite-dimensional space $$\mathcal{V}$$, then there exist positive real constants $$c, C$$ such that for all $$v \in \mathcal{V}$$ \[ c \|v\| \leq \|v\|_* \leq C\|v\|.$ However, the constants may be rather large!

In normed infinite-dimensional spaces, we often insist that the space be complete with respect to the norm – that is, if we have a Cauchy sequence in the space, it must converge. Such spaces are called Banach spaces.

### Norms on concrete spaces

The three most common vector norms we work with for the spaces $$\mathbb{R}^n$$ and $$\mathbb{C}^n$$ are

Euclidean norm (aka 2-norm)
$$\|v\|_2 = \sqrt{\sum_{j=1}^n |v_j|^2}$$
Max norm (aka sup norm, $$\infty$$-norm)
$$\|v\|_\infty = \max_j |v_j|$$
1-norm
$$\|v\|_1 = \sum_{j=1}^n |v_j|$$

These norms are all implemented in the Julia LinearAlgebra package:

let
x = [3; 4]
norm(x,Inf), norm(x,2), norm(x,1)
end
(4.0, 5.0, 7.0)

Many other norms can be related to one of these three norms. For example, we can frequently connect these norms to other norms by scaling: for any norm $$\|\cdot\|$$ and any invertible matrix $$A$$, the function $$\|\cdot\|_*$$ given by $$\|v\|_* = \|Av\|$$ is also a norm.

### Norms on polynomials

We define similar norms for more general vector spaces. For example, for the polynomial spaces $$\mathcal{P}_d$$ on a finite interval (say $$[-1,1]$$), we have three common norms analogous to the norms on $$\mathbb{R}^n$$ and $$\mathbb{C}^n$$:

Euclidean norm (aka 2-norm)
$$\|p\|_2 = \sqrt{\int_{-1}^1 |p(x)|^2 \, dx}$$
Max norm (aka sup norm, $$\infty$$-norm)
$$\|p\|_\infty = \max_{-1 \leq x \leq 1} |p(x)|$$
1-norm
$$\|p\|_1 = \int_{-1}^1 |p(x)| \, dx$$

It is worth noting that these norms are not equivalent to applying the same norms to a vector of coefficients8! Unfortunately, the Polynomials.jl library does not implement these norms, though it is not so difficult to do so9.

### Consistency and induced norms

Suppose $$\mathcal{U}$$ and $$\mathcal{V}$$ are normed vector spaces. A norm on $$\mathcal{L}(\mathcal{U}, \mathcal{V})$$ is consistent with the norms on $$\mathcal{U}$$ and $$\mathcal{V}$$ (or submultiplicative) if for all $$u \in \mathcal{U}$$ and $$L \in \mathcal{L}(\mathcal{U}, \mathcal{V})$$, $\|Lu\|_{\mathcal V} \leq \|L\| \|u\|_{\mathcal{U}}.$ The induced norm on $$\mathcal{L}(\mathcal{U}, \mathcal{V})$$ is the tightest norm such that consistency holds $\|L\|_{\mathcal{L}(\mathcal{U},\mathcal{V})} = \sup_{0 \neq u \in \mathcal{U}} \frac{\|Lu\|_{\mathcal{V}}}{\|u\|_{\mathcal{U}}} = \sup_{u \in \mathcal{U}: \|u\|_{\mathcal{U}} = 1} \|Lu\|_{\mathcal{V}}.$ A particularly important special case is the induced norm on the dual space $$\mathcal{V}^* = \mathcal{L}(\mathcal{V}, \mathbb{F})$$ where $$\mathcal{V}$$ is a field over $$\mathbb{F}$$.

For matrices in $$\mathbb{R}^{m \times n}$$ and $$\mathbb{C}^{m \times n}$$, the induced 1-norm and max-norm are simple to compute: \begin{align} \|A\|_\infty &= \max_{i\in[m]} \sum_{j=1}^n |a_{ij}|; \\ \|A\|_1 &= \max_{j \in [n]} \sum_{i=1}^m |a_{ij}|. \end{align} The norm induced by the Euclidean norm on vector spaces (sometimes called the spectral norm) is rather more complicated to compute, and is given by the largest singular value of $$A$$. We describe this below. Fortunately, the Frobenius norm is simple to compute and is consistent with the Euclidean norm, even if it is not induced by it. The Frobenius norm is given by $\|A\|_F = \sqrt{\sum_{i,j} |a_{ij}|^2}.$

In Julia, the norm function computes a vector norm for a vector or for a matrix flattened into a vector. For example:

let
A = [1.0 3.0;
2.0 4.0]
# These are equivalent to computing norms of x = [1; 2; 3; 4]
norm(A,Inf), norm(A,2), norm(A,1)
end
(4.0, 5.477225575051661, 10.0)

These are all legitimate vector norms, but only norm(A,2) (which computes the Frobenius norm) even gives a consistent norm. To compute induced norms, we need the opnorm function

let
A = [1.0 3.0;
2.0 4.0]
# These are equivalent to computing norms of x = [1; 2; 3; 4]
opnorm(A,Inf), opnorm(A,2), opnorm(A,1)
end
(6.0, 5.464985704219042, 7.0)

## 2.6 Inner products

An inner product $$\langle \cdot, \cdot \rangle$$ is a function from two vectors into the real numbers (or complex numbers for complex vector space). It satisfies the following properties for all vectors $$u, v, w$$ and scalars $$\alpha$$

Positive definiteness
$$\langle v, v \rangle \geq 0$$ and $$\langle v, v \rangle = 0$$ iff $$v = 0$$
Linearity in the first slot
$$\langle u+v, w \rangle = \langle u, w \rangle + \langle v, w \rangle$$ and $$\langle \alpha u, w \rangle = \alpha \langle u, w \rangle$$
Symmetry (or Hermitian-ness)
$$\langle u, v \rangle = \overline{\langle v, u \rangle}$$

where the overbar in the last case corresponds to complex conjugation (for complex vector spaces). Every inner product defines a corresponding norm $\|v\| = \sqrt{\langle v, v \rangle}.$ The inner product and associated norm satisfy the Cauchy-Schwarz inequality $|\langle u, v \rangle| \leq \|u\| \|v\|.$ In the real case, we are also able to recover the inner product given the norm $\langle u, v \rangle = \frac{1}{2} (\|u+v\|^2 - \|u\|^2 - \|v\|^2).$ In the complex case, this formula only gives the real part of the inner product.

A Hilbert space is an inner-product space that is complete under the associated norm (i.e. all Cauchy sequences converge). All finite-dimensional inner-product spaces are Hilbert spaces, as are the infinite-dimensional inner-product spaces that we find most interesting. If $$\mathcal{V}$$ is a Hilbert space, the Riesz representation theorem tells us that every (continuous10) linear functional $$f \in \mathcal{V}^*$$ can be written in terms of an inner product with a unique $$w \in \mathcal{V}$$: $f(v) = \langle v, w \rangle.$ The map gives us a linear isomorphism (in the real case) or antilinear isomorphism (in the complex case) between $$\mathcal{V}$$ and $$\mathcal{V}^*$$.

Where norms give a notion of length, inner products also give a notion of angle. If $$u$$ and $$v$$ are nonzero vectors, the angle $$\theta$$ between them satisfies $\cos(\theta) = \frac{\langle u, v \rangle}{\|u\|\|v\|}.$ Apart from its geometric significance, this “cosine similarity” between vectors plays an important role in many data science and machine learning applications.

### Inner products on concrete spaces

The standard inner product on $$\mathbb{C}^n$$ (also called the dot product) is $\langle x, y \rangle = y^* x = \sum_{j=1}^n x_j \bar{y}_j.$ In this case, the Riesz map from the column vector $$y$$ to the functional (row vector) $$y^*$$ is just given by the conjugate transpose operation.

For the standard inner product, we have not only the Cauchy-Schwarz inequality, but also the very useful inequality11 $| \langle x, y \rangle | \leq \|x\|_1 \|y\|_\infty$ But the standard inner product is not the only inner product, just as the standard Euclidean norm is not the only Euclidean norm! In general, if $$M \in \mathbb{C}^{n \times n}$$ is Hermitian (or symmetric in the real case) and positive definite (i.e. $$x^* M x \geq 0$$ with equality iff $$x = 0$$), then $\langle x, y \rangle_M = y^* M x$ is an inner product. In fact, all possible inner products on $$\mathbb{C}^m$$ can be written in this way. Alternately, every symmetric positive definite matrix may be written in many ways as $$M = A^* A$$, giving us a representation in terms of the standard inner product composed with a linear transformation: $\langle x, y \rangle_M = (Ax) \cdot (Ay).$

### Inner products on polynomials

As before, it is useful to consider inner products on $$\mathcal{P}_d$$ as well as on $$\mathbb{R}^n$$ and $$\mathbb{C}^n$$. The standard inner product ($$L^2$$ inner product) on $$\mathcal{P}_d$$ over an interval $$[-1,1]$$, for example, is given by $\langle p, q \rangle = \int_{-1}^1 p(x) \overline{q(x)} \, dx.$

In an inner product space, two vectors are said to be orthogonal if their inner product is zero. A set of vectors are orthonormal if they are mutually orthogonal and each vector has unit length in the Euclidean norm. Orthonormal bases are particularly convenient. In $$\mathbb{R}^n$$ (or $$\mathbb{C}^n$$) with the standard inner product, the standard basis $$\begin{bmatrix} e_1 & e_2 & \ldots e_n \end{bmatrix}$$ (where $$e_k$$ is the vector of all zeros except for a one in the $$k$$th position) is orthonormal. In $$\mathcal{P}_d$$ with the $$L^2$$ inner product on $$[-1,1]$$, the Legendre polynomials form orthogonal bases; these are given by \begin{align} P_0(x) &= 1 \\ P_1(x) &= x \\ (n+1) P_{n+1}(x) &= (2n+1)x P_n(x) - n P_{n-1}(x). \end{align} The Legendre polynomials have Euclidean length of $\|P_n(x)\| = \sqrt{\frac{2}{2n+1}};$ the normalized Legendre polynomials are scaled to unit length, and so form an orthonormal basis $Q_n(x) = \sqrt{\frac{2n+1}{2}} P_n(x).$

### Gram-Schmidt

Let $$X$$ be a basis quasi-matrix for an $$n$$-dimensional space $$\mathcal{V}$$. The Gram-Schmidt orthonormalization process gives us a way of constructing an orthonormal basis $$Q$$ for $$\mathcal{V}$$ such that for all $$k \leq n$$ $\operatorname{span}(\{x_1, \ldots, x_k\}) = \operatorname{span}(\{q_1, \ldots, q_k\}).$ The classical construction is usually written as \begin{align} \tilde{q}_k &= x_k - \sum_{j=1}^{k-1} q_j \langle x_k, q_j \rangle \\ q_k &= \tilde{q}_k / \|\tilde{q}_k\|. \end{align} Let $$r_{jk} = \langle x_k, q_j \rangle$$ for $$j < k$$ and $$r_{kk} = \|\tilde{u}_k\|$$; then the Gram-Schimdt construction can be re-interpreted as a factorization of the quasi-matrix $$X$$: $X = Q R$ where $$R$$ is the upper triangular matrix with coefficients computed in the Gram-Schimdt construction. This factorization is sometimes called the QR factorization of the (quasi)matrix $$X$$.

For numerical comptuation, the classical Gram-Schmidt process is rarely used. However the QR factorization, computed using different algorithms, is broadly useful.

## 2.7 Maps and matrices

There are a variety of types of maps that are of interest in linear algebra, all of which have matrix representations under appropriate choices of bases. These include

• Linear maps between two different vector spaces $$\mathcal{U}$$ and $$\mathcal{V}$$.
• Linear operators mapping a vector space $$\mathcal{V}$$ to itself.
• Bilinear forms mapping $$\mathcal{U}\times \mathcal{V}\rightarrow \mathbb{F}$$, which are linear in each argument independently. These are most frequently used when $$\mathbb{F}= \mathbb{R}$$. An important special case is symmetric bilinear forms $$a : \mathcal{V}\times \mathcal{V}\rightarrow \mathbb{F}$$ such that $$a(u, v) = a(v, u)$$.
• Sesquilinear forms mapping $$\mathcal{U}\times \mathcal{V}\rightarrow \mathbb{C}$$ that are linear in the first argument and antilinear in the second argument. An important special case is Hermitian forms $$a : \mathcal{V}\times \mathcal{V}\rightarrow \mathbb{C}$$ such that $$a(u,v) = \overline{a(v,u)}$$.
• Quadratic forms mapping $$\mathcal{V}\rightarrow \mathbb{R}$$. These are homogeneous of degree 2, i.e. if $$\phi : \mathcal{V}\rightarrow \mathbb{R}$$ is a quadratic form, then $$\phi(\alpha v) = |\alpha|^2 \phi(v)$$.

Bilinear forms (over a real space) and sesquilinear forms (over an complex space) can be also be thought of as linear or antilinear maps into the dual space, i.e. $v \in \mathcal{V} \mapsto w^* \in \mathcal{U}^* \mbox{ via } w^* u = a(u, v).$ In an inner product space, we can define a linear map from $$\mathcal{V}$$ to $$\mathcal{U}^*$$ by composing this map with the map from $$\mathcal{U}^*$$ to $$\mathcal{U}$$ via the Riesz representation theorem.

Each of these types of linear algebraic objects can be represented as a matrix via a choice of basis. Suppose $$U$$ and $$V$$ are basis quasi-matrices for the vector spaces $$\mathcal{U}$$ and $$\mathcal{V}$$ with $$u = Uc$$ and $$v = Vd$$. Then we have the following matrix representations

• Linear maps: If $$L : \mathcal{U}\rightarrow \mathcal{V}$$ and $$v = Lu$$ then $$d = Ac$$ where $$A = V^{-1} L U$$.
• Linear operators: If $$L : \mathcal{V}\rightarrow \mathcal{V}$$, we have only a single basis, and the matrix representation is $$A = V^{-1} L V$$.
• Bilinear forms: If $$a : \mathcal{U}\times \mathcal{V}$$ is a bilinear form, then $$a(u,v) = d^T A c$$ where the matrix element $$a_{ij} = a(u_j, v_i)$$ is an evaluation of the form on a pair of basis vectors. For symmetric bilinear forms, the matrix representation is also symmetric (i.e. $$A = A^T$$).
• Sesquilinear forms: If $$a : \mathcal{U}\times \mathcal{V}$$ is a bilinear form, then $$a(u,v) = d^* A c$$ where the matrix element $$a_{ij} = a(u_j, v_i)$$ is an evaluation of the form on a pair of basis vectors. For Hermitian bilinear forms, the matrix representation is also Hermitian (i.e. $$A=A^*$$).
• Quadratic forms: If $$\phi : \mathcal{V}\rightarrow \mathbb{R}$$ is a quadratic form, then $$\phi(v) = d^* A d$$. The matrix $$A$$ is Hermitian. The real part of $$a_{jk}$$ is $$(\phi(v_j + v_k) - \phi(v_j) - \phi(v_k))/2$$ and the imaginary part is $$(\phi(v_j - i v_k) - \phi(v_j) - \phi(v_k))/2$$.

Matrix representations of the same linear operator with respect to different bases are said to be similar. Changing from the basis $$V$$ to a basis $$VX$$ (where $$X$$ is invertible) transforms the matrix representation $$A$$ to $$X^{-1} A X$$; this is called a similarity transformation. Similar matrices have the same eigenvalues, because the eigenvalues are a basis-independent property of linear operators.

Matrix representations of the same quadratic form (or Hermitian sesquilinear form) with respect to different bases are said to be congruent. Changing from the basis $$V$$ to a basis $$VX$$ (where $$X$$ again is invertible) transforms the matrix representation $$A$$ to $$X^* A X$$; this is called a congruence transformation. Congruent matrices share a property called Sylvester’s inertia, as this is a basis-independent property of quadratic forms. We will have more to say about this shortly in our discussion of canonical forms.

## 2.8 Block matrices

Now suppose that we are interested in a linear mapping $$L : \mathcal{U}\rightarrow \mathcal{V}$$ where the spaces have basis quasi-matrices $$U$$ and $$V$$, respectively. Now partition the $$U$$ and $$V$$ bases into disjoint sets of columns, written as \begin{align} U &= \begin{bmatrix} U_1 & U_2 & \ldots & U_q \end{bmatrix} \\ V &= \begin{bmatrix} V_1 & V_2 & \ldots & V_q \end{bmatrix}. \end{align} The partitioning of the bases corresponds to a partitioning of the two spaces as a direct sum of subspaces \begin{align} \mathcal{U}&= \mathcal{U}_1 \oplus \mathcal{U}_2 \oplus \ldots \oplus \mathcal{U}_q \\ \mathcal{V}&= \mathcal{V}_1 \oplus \mathcal{V}_2 \oplus \ldots \oplus \mathcal{V}_p \end{align}

If $$A = V^{-1} L U$$ is the matrix representing $$L$$ with respect to the $$U$$ and $$V$$ bases, then together with the partitioning of the bases comes a partitioning of $$A$$ into blocks: \begin{align} A = \begin{bmatrix} A_{11} & A_{12} & \ldots & A_{1q} \\ A_{21} & A_{22} & \ldots & A_{2q} \\ \vdots & \vdots & \ddots & \vdots \\ A_{p1} & A_{p2} & \ldots & A_{pq} \end{bmatrix} \end{align} where each submatrix $$A_{ij}$$ corresponds to the “piece” of the mapping $$L$$ from the $$\mathcal{U}_j$$ contribution to $$u$$ to the $$\mathcal{V}_i$$ contribution to $$Lu$$.

We can similarly partition matrices associated with other types of maps. In the case of operators and quadratic forms (or symmetric or Hermitian forms), sensible partitionings of the associated matrices generally yield diagonal blocks.

## 2.9 Schur complements

Suppose $$L : \mathcal{U}\rightarrow \mathcal{U}$$ is an operator on a vector space and $$\mathcal{U}= \mathcal{U}_1 \oplus \mathcal{U}_2$$ is a decomposition of $$\mathcal{U}$$ into a direct sum of subspaces. Then we have the block representation of the operator as $L = \begin{bmatrix} L_{11} & L_{12} \\ L_{21} & L_{22} \end{bmatrix}.$ If $$L$$ is invertible, we can similarly write the inverse in block form as $L^{-1} = \begin{bmatrix} M_{11} & M_{12} \\ M_{21} & M_{22} \end{bmatrix}$ Assuming $$L_{11}$$ is invertible, we can write the block factorization: $L = \begin{bmatrix} I & 0 \\ L_{21} L_{11}^{-1} & I \end{bmatrix} \begin{bmatrix} L_{11} & L_{12} \\ 0 & L_{22} - L_{21} L_{11}^{-1} L_{12} \end{bmatrix},$ and by forward and backward substitution we have that $$M_{22} = S^{-1}$$ where $S = L_{22} - L_{21} L_{11}^{-1} L_{12}$ is the Schur complement of $$L_{11}$$ in $$L$$.

Because they arise naturally in the process of algorithms like Gaussian elimination, Schur complements play an important role in numerical methods for solving linear systems. But Schur complements are also important in various non-numerical settings, such as in Bayesian statistics, where conditioning a multivariate Gaussian prior on linear measurements yields a multivariate Gaussian posterior distribution whose covariance is a Schur complement in the prior covariance.

## 2.10 The canonical forms

We start with abstract vector spaces and functions on them, but we compute with bases and matrices. The matrix associated with a linear algebra function always depends on the choice of basis, and so we ask: what basis would make the matrix as simple as possible? This simplest possible matrix representation is known as a canonical form. For computational purposes, we often want to restrict ourselves to orthonormal bases; therefore, for each type of function, we list two flavors of canonical forms – those associated with a general choice of basis and those associated with orthonormal bases. If we start with a matrix representation of some function on concrete vector spaces, we can also think of the canonical forms as matrix factorizations.

### Linear maps

Suppose $$L : \mathcal{V}\rightarrow \mathcal{U}$$ is a linear map between two different vector spaces with $$\operatorname{dim}(\mathcal{V}) = n$$ and $$\operatorname{dim}(\mathcal{U}) = m$$.

#### General bases

Suppose we decompose $$\mathcal{U}= \mathcal{U}_1 \oplus \mathcal{U}_2$$ where $$\mathcal{U}_1 = \operatorname{range}(L)$$, and we decompose $$\mathcal{V}= \mathcal{V}_1 \oplus \mathcal{V}_2$$ where $$\mathcal{V}_2 = \operatorname{null}(L)$$. Then for any associated choice of bases, we have a block matrix representation of the form $\begin{bmatrix} A_{11} & 0 \\ 0 & 0 \end{bmatrix}.$ where $$A_{11} \in \mathbb{C}^{r \times r}$$ is an invertible matrix. For appropriate choices of bases, we have the block matrix representation $\begin{bmatrix} I_{r \times r} & 0 \\ 0 & 0 \end{bmatrix}.$ That is, the canonical for a linear map between two different spaces can be described just by one number: the rank $$r$$ (from which we can also determine the null space dimension $$n-r$$). We can also write this as the (quasi)matrix factorization $L = \begin{bmatrix} U_1 & U_2 \end{bmatrix} \begin{bmatrix} I & 0 \\ 0 & 0 \end{bmatrix} \begin{bmatrix} V_1 & V_2 \end{bmatrix}^{-1}$

#### Orthonormal bases

If we restrict ourselves to orthonormal bases, we can still get the same general block form by decomposing $$U$$ into the range space and its orthogonal complement and decomposing $$V$$ into the null space and its orthogonal complement. However, we cannot get all the way to a representation of the leading block as an identity matrix – the best we can do is to get to a diagonal matrix with positive entries. Using the fact that the inverse of a unitary matrix is given by its conjugate transpose (or the Riesz map of the columns, in the more general case), we have the factorization $L = \begin{bmatrix} U_1 & U_2 \end{bmatrix} \begin{bmatrix} \Sigma_{11} & 0 \\ 0 & 0 \end{bmatrix} \begin{bmatrix} V_1 & V_2 \end{bmatrix}^* = U_1 \Sigma_{11} V_1^*,$ where the $$r$$-by-$$r$$ matrix $$\Sigma_{11}$$ has diagonal entries $$\sigma_1 \geq \sigma_2 \geq \ldots \geq \sigma_r > 0$$. The diagonals of the matrix are known as the singular values of the map, with associated bases of singular vectors.

### Linear operators

Now suppose $$L : \mathcal{V}\rightarrow \mathcal{V}$$. This case is different from the linear map because we only get to choose one basis, rather than two.

#### General bases

Over the complex numbers, we can choose a basis $$X$$ that usually renders the matrix for $$L$$ diagonal (and gives us something nearly diagonal otherwise): $L = X J X^{-1}, \quad J = \begin{bmatrix} J_{\lambda_1} & & & \\ & J_{\lambda_2} & & \\ & & J_{\lambda_3} & \\ & & & \ddots \end{bmatrix},$ where the submatrices $$J_{\lambda}$$ are Jordan blocks of the form $J_{\lambda} = \begin{bmatrix} \lambda & 1 & & & \\ & \lambda & 1 & & \\ & & \ddots & \ddots & \\ & & & \lambda & 1 \\ & & & & \lambda \end{bmatrix}.$ The columns of the basis $$X$$ are eigenvectors or generalized eigenvectors. This is known as the Jordan canonical form. Most matrices are diagonalizable, so that all the Jordan blocks are 1-by-1 and we have a complete basis of eigenvectors.

#### Orthonormal bases

Over the complex numbers, we can choose an orthonormal basis $$U$$ that gives us an upper triangular matrix $L = U T U^*,$ where the diagonal elements $$t_{jj}$$ are eigenvalues of $$L$$. This is known as the (complex) Schur canonical form of $$L$$. In this basis, the columns no longer correspond to eigenvectors. However, each prefix of columns $$u_1, \ldots u_k$$ spans an invariant subspace of $$L$$; that is $$L$$ maps this space into itself.

If we restrict ourselves to the reals, we have the real Schur form of $$L$$. This is close to the complex Schur form except that we insist on real basis vectors and $$T$$ is block upper triangular, with some 2-by-2 blocks corresponding to complex conjugate pairs of eigenvalues.

Now suppose $$\phi : \mathcal{V}\rightarrow \mathbb{R}$$ is a quadratic form.

#### General bases

For every quadratic form, there is a basis which we can write in partitioned form as $V = \begin{bmatrix} V_+ & V_- & V_0 \end{bmatrix}$ such that we have the block matrix representation $\phi(Vc) = \begin{bmatrix} c_+ \\ c_- \\ c_0 \end{bmatrix}^* \begin{bmatrix} I & & \\ & -I & \\ & & 0 \end{bmatrix} \begin{bmatrix} c_+ \\ c_- \\ c_0 \end{bmatrix}$ Let $$\nu_+$$, $$\nu_-$$, and $$\nu_0$$ be the number of columns in the three parts of the basis. The triple $$\nu = (\nu_+, \nu_-, \nu_0)$$ is called Sylvester’s inertia (or sometimes the metric signature) for the quadratic form, and characterizes the form in much the same way that the rank characterizes a linear map. Geometrically, Sylvester’s inertia describes the number of directions of positive curvature, negative curvature, and zero curvature for the bowl or saddle described by the quadratic form. A quadratic form is positive definite if $$\nu_+ = n$$, positive semi-definite if $$\nu_+ + \nu_0 = n$$, negative definite if $$\nu_- = n$$, and negative semi-definite if $$\nu- + \nu_0 = n$$. A quadratic form with both $$\nu_+$$ and $$\nu-$$ nonzero is strongly indefinite (also sometimes called a saddle).

If $$A$$ is the representation of $$\phi$$ under some arbitrary basis $$W$$ and $$W = VX$$, we have the factorization $A = X^* \begin{bmatrix} I & & \\ & -I & \\ & & 0 \end{bmatrix} X;$ in this case, we would say $$A$$ is congruent to the diagonal matrix described by the inertia.

#### Orthonormal bases

If we restrict our attention to orthonormal bases, the canonical form of the matrix representation is a simple real diagonal matrix: $\phi(Vc) = c^* \Lambda c, \quad \Lambda = \begin{bmatrix} \lambda_1 \\ & \lambda_2 \\ & & \ddots \\ & & & \lambda_n \end{bmatrix}$ where the eigenvalues $$\lambda_j$$ are typically listed in descending order. The number of positive, negative, and zero eigenvalues is given by Sylvester’s inertia.

If $$A$$ is the representation of $$\phi$$ under some orthonormal basis $$W$$ and $$W = V Q^*$$ (where $$Q$$ is a unitary matrix, i.e. $$Q^* Q = I$$), then we have the factorization $A = Q \Lambda Q^*;$ in this case, we would say $$A$$ is related to $$\Lambda$$ by a unitary congruence. A unitary congruence is also a similarity transform, hinting at a rich relation between the interpretation of the symmetric eigenvalue problem in terms of operators or in terms of quadratic forms.

### Other functions

What of bilinear and sesquilinear forms? For these functions, the appropriate canonical forms are essentially the same as those that we have already described. In the case of real symmetric bilinear or complex Hermitian sesquilinear forms, there is an associated quadratic form $$\phi(v) = a(v,v)$$, and the canonical form of the bilinear/sesquilinear form is the same as the canonical form for the quadratic form. In the case of bilinear or sesquilinear forms on two different spaces, the appropriate canonical form is the same as for a linear map.

## 2.11 Important invariants

The canonical forms of different maps that appear in linear algebra reveal important invariants of the maps that do not depend on the specific matrix representation. These include the rank of a linear map and the inertia of a quadratic form, but also the singular values and the eigenvalues (and their geometric and algebraic multiplicities). However, sometimes we want invariants that are simpler (and maybe easier to compute with than singular values and eigenvalues). We might also want invariants that are continuous under small changes to the map, which the rank, inertia, and eigenvalue multiplicities generally are not. In this section, we review a few additional invariants that see common use.

### Invariant norms

A matrix norm is said to be unitarily invariant if for any matrix $$A$$ and unitary matrices $$U$$ and $$V$$ of appropriate dimension, $$\|A\| = \|U^* A\| = \|AV\|$$. Such matrix norms characterize a linear mapping between inner product spaces, independent of the specific orthonormal basis chosen. Therefore, any unitarily invariant norm on a matrix space must depend only on the singular values of the matrix.

The Schatten $$p$$-norm on a matrix space is defined in terms of the $$p$$-norm on the vector of singular values, i.e. $\left( \sum_{i=1}^n \sigma_i^p \right)^{1/p}.$ The three most frequently used Schatten norms are:

• $$p = 2$$: The Frobenius norm $$\|A\|_F = \sqrt{\sum_{i=1}^n \sigma_i^2}$$. The Frobenius norm can also be written as the two-norm of the vector of coefficients, i.e. $$\|A\|_F = \sqrt{\sum_{i,j} |a_{ij}|^2}$$.
• $$p = \infty$$: The spectral norm $$\|A\|_2 = \sigma_1$$. This is the same as the operator norm induced by the vector 2-norm(s).
• $$p = 1$$: The nuclear norm $$\|A\|_* = \sum_{j=1}^n \sigma_j$$ (also sometimes called the trace norm). When $$A$$ is positive semi-definite, the nuclear norm is equal to $$\operatorname{tr}(A) = \sum_i a_{ii}$$.

We often use the Frobenius norm to measure the distance between data matrices and the spectral norm when considering the error in approximating a linear map. The nuclear norm appears somewhat less frequently, but plays an important role in methods for finding low-rank solutions to optimization problems over matrix spaces.

The Ky Fan $$k$$-norm on a matrix spaces is the sum of the largest $$k$$ singular values. The most frequent examples are $$k = 1$$ (the spectral norm) and $$k = n$$ (the nuclear norm).

### Stable rank

There are many times when we would like a low-rank approximate solution to some matrix equation or optimization problem. However, this is computationally awkward, as the rank is not a continuous function of the matrix entries! A useful continuous lower bound on the rank of a matrix is the stable rank: $\|A\|_F^2 / \|A_2\|^2 = \sum_{j=1}^n \left( \frac{\sigma_i}{\sigma_1} \right)^2.$ If the matrix $$A$$ has orthonormal columns (if tall and skinny) or rows (if short and fat), then the stable rank agrees with the rank. Many of the bounds on randomized algorithms for low-rank approximation of matrices are posed in terms of the stable rank.

### Spectral invariants

Unitarily invariant norms and the stable rank can all be phrased in terms of singular values, and so can be viewed as intrinsic properties of an underlying linear map between two inner product spaces. It is also useful to consider spectral invariants of an operator from a vector space to itself, which we can express in terms of the eigenvalues.

One invariant that occurs frequently is the spectral radius. If $$\Lambda(A)$$ denotes the spectrum of $$A$$, then $\rho(A) = \max_{\lambda \in \Lambda(A)} |\lambda|.$ Let $$v$$ be aany unit-length eigenvector associated with the largest modulus eigenvalue; then for any consistent matrix norm, $\|A\| \geq \|Av\| = \|\lambda v\| = |\lambda| = \rho(A).$ Therefore, the spectral radius is bounded from above by any consistent matrix norm. Conversely, at least in a finite-dimensional space, for any $$\epsilon > 0$$ there exists a vector space norm such that the associated operator norm satisfies $\rho(A) \leq \|A\| \leq \rho(A) + \epsilon.$ We can actually get equality if no maximal modulus eigenvalue is associated with a nontrivial Jordan block.

Many spectral invariants are expressed via the characteristic polynomial $p(z) = \prod_{i=1}^n (z-\lambda_i)$ where the $$\lambda_i$$ are the eigenvalues of the operator (with multiplicity). Written in the monomial basis, the characteristic polynomial is \begin{align} p(z) &= z^n - \left( \sum_i \lambda_i \right) z^{n-1} + \ldots + (-1)^n \prod_i \lambda_i \\ &= z^n - \operatorname{tr}(A) + \ldots + (-1)^n \det(A). \end{align} The coefficients of the characteristic polynomial are symmetric polynomials of the eigenvalues (i.e. polynomials of $$n$$ variables that are invariant under permutation of the inputs). By far the most important of these are the trace $$\operatorname{tr}(A)$$ and the determinant $$\det(A)$$. Because the eigenvalues of $$zI - A$$ are equal to $$z - \lambda_i$$, we can also write the characteristic polynomial in terms of the determinant, i.e. $$p(z) = \det(zI-A)$$.

The trace and the determinant have a variety of useful properties. The trace is a linear function of the entries of the matrix representation, and can be written as the diagonal sum, i.e. $\operatorname{tr}(A) = \sum_i a_{ii}.$ When the dimensions make sense, the trace is invariant under cyclic permutations of matrix products; that is, if $$A \in \mathbb{C}^{m \times n}, B \in \mathbb{C}^{n \times p}, C \in \mathbb{C}^{p \times m}$$, we have $\operatorname{tr}(ABC) = \sum_{i,j,k} a_{ij} b_{jk} c_{ki} = \sum_{i,j,k} c_{ki} a_{ij} b_{jk} = \operatorname{tr}(CAB)$ and similarly $$\operatorname{tr}(ABC) = \operatorname{tr}(BCA)$$. On the matrix space $$\mathbb{C}^{m \times n}$$, we can define Frobenius inner product (the analogue of the standard inner product) in terms of the trace: $\langle X, Y \rangle_F = \sum_{i,j} x_{ij} y_{ij}^* = \operatorname{tr}(Y^* X) = \operatorname{tr}(XY^*).$

The determinant is not linear, but it is a homomorphism from operators to the complex numbers, i.e. $$\det(AB) = \det(A) \det(B)$$ and $$\det(I) = 1$$. The determinant also satisfies $$\det(A^*) = \det(A)^*$$. Like the trace, the determinant can be written in terms of the entries of the matrix representation without direct reference to the eigenvalues. Perhaps the most common way that determinants are taught in introductory classes is with the Laplace formula (or cofactor expansion) $\det(A) = \sum_i (-1)^{i+1} a_{1i} m_{1i}$ where $$m_{1i}$$ is the determinant of the $$i$$th minor (the matrix with column 1 and row $$i$$ removed). Unfortunately, naively using the Laplace formula to compute derivatives yields an $$O(n!)$$ time algorithm, and alternate methods are usually used for $$n$$ larger than two or three.

Using the Laplace expansion, we find that the determinant of an upper triangular matrix $$U$$ (in which all subdiagonal elements are zero) is equal to the product of the diagonal entries, i.e. $$\det(U) = \prod_{j=1}^n u_{jj}$$. The determinant of a lower triangular matrix is similarly the product of the diagonal entries. Using these facts, we generally compute determinants12 by factoring the matrix as a product of triangular or unitary matrices. Geometrically, these factorizations correspond to using volume-preserving transformations (shear transforms or rotations) to transform a parallelipiped defined by the columns of $$A$$ into an axis-aligned parallelipiped where we can apply the generalization of “base times width times height” formulas from high school geometry.

1. When describing dual spaces, Prof. Kahan always used to look sternly over his glasses and pronounce: “Vector spaces are like potato chips; you can never have only one.”↩︎

2. We typically restrict our attention to continuous linear maps – or, in the case of a normed vector space, to maps that are bounded. However, this distinction only matters when we are dealing with infinite-dimensional spaces.↩︎

3. In statistics, concrete vectors are frequently arranged as rows by default; the column-oriented perspective we use is common in numerical computing.↩︎

4. We use $$[n]$$ for natural numbers $$n$$ to denote the index set $$\{1, 2, \ldots, n\}$$.↩︎

5. If $$\mathcal{U}$$ and $$\mathcal{V}$$ are normed vector spaces, we restrict our attention to all bounded linear maps. This is a distinction that only matters in the infinite dimensional setting, so if you only care about finite-dimensional spaces, you may promptly forget about this footnote.↩︎

6. In most linear algebra texts, we talk about a basis set of $$\mathcal{V}$$, i.e. a linearly independent spanning set (with no particular ordering). Using a quasi-matrix instead of a set just means we also pick an ordering, which we generally do in computation anyhow.↩︎

7. On infinite dimensional spaces, norms are not all equivalent.↩︎

8. There is a basis of polynomials (the normalized Legendre polynomials) for which applying the $$L^2$$ norm (the Euclidean norm described here) to a polynomial $$p \in \mathcal{P}_d$$ is equivalent to applying the $$L^2$$ norm to the vector of coefficients. But this is a special case.↩︎

9. This is a good exercise for the interested student!↩︎

10. All linear functionals are continuous in a finite-dimensional vector space; this makes a difference only in infinite-dimensional spaces.↩︎

11. This is a special case of the Hölder inequality, which states that $$|\langle x, y \rangle| \leq \|x\|_p \|y\|_q$$ for the so-called $$\ell^p$$ norms when $$1/p + 1/q = 1$$.↩︎

12. Determinants are used to represent (signed) volumes, and it is appropriate to compute them in settings like the change of variables formula for integration, or for transformation of probability distribution functions. Most other applications of determinants from linear algebra (Cramer’s rule for solving linear systems, computation of determinants to check for singularity, etc) are best avoided for numerical computation – they lead to algorithms that are inefficient, unstable, or both.↩︎