# LU factorization¶

Every first linear algebra course introduces Gaussian elimination for a general square system $$\mathbf{A}\mathbf{x}=\mathbf{b}$$. In Gaussian elimination one uses row operations on an augmented matrix $$[\mathbf{A}\; \mathbf{b}]$$ to reduce it to an equivalent triangular system (usually upper triangular).

## Review example¶

Rather than writing out the process in full generality, we use an example to refresh your memory while getting arithmetic support from Julia.

## The algebra of Gaussian elimination¶

In an earlier section we observed that row and column operations can be expressed as linear algebra using columns from the identity matrix. This connection allows us to express Gaussian elimination using matrices. We will ignore the augmentation step, set aside $$\mathbf{b}$$ for now, and consider only the square system matrix $$\mathbf{A}$$.

As the first step in the demo Gaussian elimination, we get the multiplier $$A_{21}/A_{11}=-2$$. The first row of $$\mathbf{A}$$ is extracted by $$\mathbf{e}_1^T\mathbf{A}$$. After $$-2$$ times this row is subtracted from row 2, with the other rows being left alone, we arrive at the matrix

$\begin{split} \begin{bmatrix} \mathbf{e}_1^T \\[2mm] \mathbf{e}_2^T + 2 \mathbf{e}_1^T \\[2mm] \mathbf{e}_3^T \\[2mm] \mathbf{e}_4^T \end{bmatrix}\mathbf{A}.\end{split}$

This expression can be manipulated into

$\begin{split}\mathbf{A} = \left(\mathbf{I} + \begin{bmatrix} 0 \mathbf{e}_1^T \\[2mm] 2 \mathbf{e}_1^T \\[2mm] 0 \mathbf{e}_1^T \\[2mm] 0 \mathbf{e}_1^T \end{bmatrix} \right) \mathbf{A} =\left(\mathbf{I} +2 \begin{bmatrix} 0 \\ 1 \\ 0 \\ 0 \end{bmatrix} \mathbf{e}_1^T \right) \mathbf{A} = (\mathbf{I} + 2 \mathbf{e}_2\mathbf{e}_1^T) \mathbf{A}.\end{split}$

In general, adding $$\alpha$$ times row $$j$$ of $$\mathbf{A}$$ to row $$i$$ in place is done via the expression

(28)$(\mathbf{I} + \alpha \, \mathbf{e}_i \mathbf{e}_j^T ) \mathbf{A}.$

Following many introductory texts on linear algebra, we refer to the matrix in parentheses above as an elementary matrix.

The elementary matrix factors found in Row operations, each in the form (28), have some important properties. First, in addition to being triangular, each has all ones on the diagonal, so we call each a unit triangular matrix. Triangular singularity implies that all unit triangular matrices are invertible, which is about to become important.

Let’s review. The Gaussian elimination procedure in Gaussian elimination did six row operations in order to introduce six zeros into the lower triangle of $$\mathbf{A}$$. Each row operation can be expressed using multiplication by an elementary matrix $$\mathbf{L}_{ij}$$. At the end we get an upper triangular matrix, $$\mathbf{U}$$:

(29)$\mathbf{U} = \mathbf{L}_{43}\mathbf{L}_{42}\mathbf{L}_{32}\mathbf{L}_{41}\mathbf{L}_{31}\mathbf{L}_{21} \mathbf{A}.$

Now we multiply both sides on the left by $$\mathbf{L}_{43}^{-1}$$. On the right-hand side, it can be grouped together with $$\mathbf{L}_{43}$$ to form an identity matrix. Then we multiply both sides on the left by $$\mathbf{L}_{42}^{-1}$$, which knocks out the next term on the right side, etc. Eventually we get

(30)$\mathbf{L}_{21}^{-1}\mathbf{L}_{31}^{-1}\mathbf{L}_{41}^{-1}\mathbf{L}_{32}^{-1}\mathbf{L}_{42}^{-1}\mathbf{L}_{43}^{-1} \mathbf{U} = \mathbf{A}.$

We come next to an interesting property of these elementary matrices. If $$i\ne j$$, then for any scalar $$\alpha$$ we can calculate that

$\begin{split}\begin{split} \bigl(\mathbf{I} + \alpha\, \mathbf{e}_i \mathbf{e}_j^T\bigr) \bigl(\mathbf{I} - \alpha \,\mathbf{e}_i \mathbf{e}_j^T\bigr) & = \mathbf{I} + \alpha \mathbf{e}_i \mathbf{e}_j^T - \alpha\, \mathbf{e}_i \mathbf{e}_j^T - \alpha^2\, \mathbf{e}_i \mathbf{e}_j^T \mathbf{e}_i \mathbf{e}_j^T \\ &= \mathbf{I} - \alpha^2\, \mathbf{e}_i \bigl(\mathbf{e}_j^T \mathbf{e}_i\bigr) \mathbf{e}_j^T = \mathbf{I}, \end{split}\end{split}$

since the inner product between any two different columns of $$\mathbf{I}$$ is zero. We have shown that

$\bigl(\mathbf{I} + \alpha \, \mathbf{e}_i \mathbf{e}_j^T\bigr)^{-1} = \mathbf{I} - \alpha\, \mathbf{e}_i \mathbf{e}_j^T.$

All that is needed to invert $$\mathbf{I} + \alpha\, \mathbf{e}_i \mathbf{e}_j^T$$ is to flip the sign of $$\alpha$$, the lone element in the lower triangle.

We need one more remarkably convenient property of the elementary matrices. Looking, for example, at the first two matrices on the left in (30), we calculate that

$(\mathbf{I} + \alpha \, \mathbf{e}_2\mathbf{e}_1^T) (\mathbf{I} + \beta\, \mathbf{e}_3\mathbf{e}_1^T) = \mathbf{I} + \alpha\, \mathbf{e}_2\mathbf{e}_1^T + \beta \,\mathbf{e}_3\mathbf{e}_1^T + \alpha\beta \,\mathbf{e}_2\mathbf{e}_1^T\mathbf{e}_3\mathbf{e}_1^T.$

We can use associativity in the last term to group together $$\mathbf{e}_{1}^T\mathbf{e}_{3}$$, which is another inner product that equals zero thanks to the structure of the identity matrix. In summary: the product of these elementary factors just combines the nonzero terms that each one has below the diagonal.

That reasoning carries across each of the new terms in the product on the left side of (30). The conclusion is that Gaussian elimination finds a unit lower triangular matrix $$\mathbf{L}$$ and an upper triangular matrix $$\mathbf{U}$$ such that

(31)$\mathbf{L} \mathbf{U} = \mathbf{A}.$

Furthermore, the lower triangular entries of $$\mathbf{L}$$ are the row multipliers we found as in Gaussian elimination, and the entries of $$\mathbf{U}$$ are those found at the end of the elimination process. Equation (31) is called an LU factorization of the matrix $$\mathbf{A}$$.

## An algorithm—for now¶

LU factorization reduces any linear system to two triangular ones. From this, solving $$\mathbf{A}\mathbf{x}=\mathbf{b}$$ follows immediately:

1. Factor $$\mathbf{L}\mathbf{U}=\mathbf{A}$$ using Gaussian elimination.

2. Solve $$\mathbf{L}\mathbf{z}=\mathbf{b}$$ for $$\mathbf{z}$$ using forward substitution.

3. Solve $$\mathbf{U}\mathbf{x}=\mathbf{z}$$ for $$\mathbf{x}$$ using backward substitution.

One of the important aspects of this algorithm is that the factorization step depends only on the matrix $$\mathbf{A}$$; the right-hand side $$\mathbf{b}$$ is not involved. Thus if one has to solve multiple systems with a single matrix $$\mathbf{A}$$, the factorization needs to be performed only once for all systems. As we show in \secref{opcount}, the factorization is by far the most computationally expensive step, so this note is of more than academic interest.

Based on the examples and discussion above, a code for LU factorization is given in lufact.

Function 14 (lufact)

LU factorization (not stable)

  1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 """ lufact(A) Compute the LU factorization of square matrix A, returning the factors. """ function lufact(A) n = size(A,1) L = Matrix(Diagonal(ones(n))) U = float(copy(A)) # Gaussian elimination for j = 1:n-1 for i = j+1:n L[i,j] = U[i,j] / U[j,j] # row multiplier U[i,j:n] -= L[i,j]*U[j,j:n] end end return L,triu(U) end 

Tip

Line 10 of lufact points out two subtle Julia issues. First, arrays, including vectors and matrices, are really just references to blocks of memory. This data is much more efficient to pass around than the complete contents of the array. However, it means that a statement such as U=A just clones the array reference into the variable U. Any changes made to entries of U would then also be made to entries of A, because they refer to the same contents. In the context of lufact we don’t want to change the original matrix, so we use copy here to create an independent clone of the array contents and a new reference to them.

The second issue is that even when A has all integer entries, the LU factors may not. So if by copying A we create U as a matrix of integers, the function will fail with an InexactError if we attempt to insert a noninteger result into U in line 16. To avoid this eventuality we convert U into a floating-point matrix with float.

The multipliers are stored in the lower triangle of $$\mathbf{L}$$ as they are found. When operations are done to put zeros in column $$j$$, they are carried out only in lower rows to create an upper triangular matrix. (Only columns $$j$$ through $$n$$ are accessed, since the other entries should already be zero.) At the end of the process the matrix $$\mathbf{A}$$ should be upper triangular, but since roundoff errors could create some small nonzeros the triu command is used to make them exactly zero.

Observe from lufact that the factorization can fail if $$A_{jj}=0$$ when it is put in the denominator in line~14. This does not necessarily mean there is a zero in the diagonal of the original $$\mathbf{A}$$, because $$\mathbf{A}$$ is changed during the computation. Moreover, there are perfectly good nonsingular matrices for which this type of failure occurs, such as

$\begin{split} \begin{bmatrix} 0 & 1\\1 & 0 \end{bmatrix}.\end{split}$

Fortunately, this defect can be repaired for all nonsingular matrices at minor cost, as we will see in the section on pivoting.

## Exercises¶

1. ✍ For each matrix, perform Gaussian elimination by hand to produce an LU factorization. Write out the $$\mathbf{L}$$ matrix using outer products of standard basis vectors.

(a) $$\displaystyle \begin{bmatrix} 2 & 3 & 4 \\ 4 & 5 & 10 \\ 4 & 8 & 2 \end{bmatrix}\qquad$$ (b) $$\displaystyle \begin{bmatrix} 6 & -2 & -4 & 4\\ 3 & -3 & -6 & 1 \\ -12 & 8 & 21 & -8 \\ -6 & 0 & -10 & 7 \end{bmatrix}$$

2. ⌨ The matrices

$\begin{split}\mathbf{T}(x,y) = \begin{bmatrix} 1 & 0 & 0 \\ 0 & 1 & 0 \\ x & y & 1 \end{bmatrix},\qquad \mathbf{R}(\theta) = \begin{bmatrix} \cos\theta & \sin \theta & 0 \\ -\sin\theta & \cos \theta & 0 \\ 0 & 0 & 1 \end{bmatrix}\end{split}$

are used to represent translations and rotations of plane points in computer graphics. For the following, let

$\begin{split}\mathbf{A} = \mathbf{T}(3,-1)\mathbf{R}(\pi/5)\mathbf{T}(-3,1), \qquad \mathbf{z} = \begin{bmatrix} 2 \\ 2 \\ 1 \end{bmatrix}.\end{split}$

(a) Find $$\mathbf{b} = \mathbf{A}\mathbf{z}$$.

(b) Find the LU factorization of $$\mathbf{A}$$.

(c) Use the factors with triangular substitutions in order to solve $$\mathbf{A}\mathbf{x}=\mathbf{b}$$, and find $$\mathbf{x}-\mathbf{z}$$.

3. ⌨ In Julia, define

$\begin{split}\mathbf{A}= \begin{bmatrix} 1 & 0 & 0 & 0 & 10^{12} \\ 1 & 1 & 0 & 0 & 0 \\ 0 & 1 & 1 & 0 & 0 \\ 0 & 0 & 1 & 1 & 0 \\ 0 & 0 & 0 & 1 & 0 \end{bmatrix}, \quad \hat{\mathbf{x}} = \begin{bmatrix} 0 \\ 1/3 \\ 2/3 \\ 1 \\ 4/3 \end{bmatrix}, \quad \mathbf{b} = \mathbf{A}\hat{\mathbf{x}}.\end{split}$

(a) Using lufact and triangular substitutions, solve the linear system $$\mathbf{A}\mathbf{x}=\mathbf{b}$$, showing the result. About how many (to the nearest integer) accurate digits are in the result? (The answer is much less than the default 16 of double precision).

(b) Repeat part (a) with $$10^{20}$$ as the corner element. (The result is even less accurate. We will study the causes of such low accuracy later in the chapter.)

4. not available

5. lufact factors $$\mathbf{A}=\mathbf{L}\mathbf{U}$$ in such a way that $$\mathbf{L}$$ is a unit lower triangular matrix—that is, has all ones on the diagonal. It is also possible to define the factorization so that $$\mathbf{U}$$ is a unit upper triangular matrix instead. Write a function lufact2 that uses lufact without modification to produce this version of the factorization. (Hint: Begin with the standard LU factorization of $$\mathbf{A}^T$$.) Demonstrate on a nontrivial $$4\times 4$$ example.

6. When computing the determinant of a matrix by hand, it’s common to use cofactor expansion and apply the definition recursively. But this is terribly inefficient as a function of the matrix size.

(a) ✍ Explain why, if $$\mathbf{A}=\mathbf{L}\mathbf{U}$$ is an LU factorization,

$\det(\mathbf{A}) = U_{11}U_{22}\cdots U_{nn}=\prod_{i=1}^n U_{ii}.$

(b) ⌨ Using the result of part (a), write a function determinant(A) that computes the determinant using lufact. Test your function on at least two nontriangular $$5\times 5$$ matrices, comparing your result to the result of det from the standard LinearAlgebra package.

7. not available