Gram–Schmidt process

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In mathematics and numerical analysis, the Gram–Schmidt process of linear algebra is a method of orthogonalizing a set of vectors in an inner product space, most commonly the Euclidean space Rn. Orthogonalization in this context means the following: we start with vectors v1,…, vk which are linearly independent and we want to find mutually orthogonal vectors u1, …, uk which generate the same subspace as the vectors v1, …, vk.

The method is named for Jørgen Pedersen Gram and Erhard Schmidt but it appeared earlier in the work of Laplace and Cauchy. In the theory of Lie group decompositions it is generalized by the Iwasawa decomposition.

The application of the Gram–Schmidt process to the column vectors of a full column rank matrix yields the QR decomposition (it is decomposed into an orthogonal and a triangular matrix).

Contents

The Gram–Schmidt process

We define the projection operator by

<math>\mathrm{proj}_{\mathbf{u}}\,\mathbf{v} = {\langle \mathbf{v}, \mathbf{u}\rangle\over\langle \mathbf{u}, \mathbf{u}\rangle}\mathbf{u}. </math>

It projects the vector v orthogonally onto the vector u.

The Gram–Schmidt process then works as follows: Image:Gram–Schmidt process.svg

<math>\mathbf{u}_1 = \mathbf{v}_1,</math> <math>\mathbf{e}_1 = {\mathbf{u}_1 \over \mathbf{u}_1}</math>
<math>\mathbf{u}_2 = \mathbf{v}_2-\mathrm{proj}_{\mathbf{u}_1}\,\mathbf{v}_2, </math> <math>\mathbf{e}_2 = {\mathbf{u}_2 \over \mathbf{u}_2}</math>
<math>\mathbf{u}_3 = \mathbf{v}_3-\mathrm{proj}_{\mathbf{u}_1}\,\mathbf{v}_3-\mathrm{proj}_{\mathbf{u}_2}\,\mathbf{v}_3, </math> <math>\mathbf{e}_3 = {\mathbf{u}_3 \over \mathbf{u}_3}</math>
<math>\vdots</math> <math>\vdots</math>
<math>\mathbf{u}_k = \mathbf{v}_k-\sum_{j=1}^{k-1}\mathrm{proj}_{\mathbf{u}_j}\,\mathbf{v}_k, </math> <math>\mathbf{e}_k = {\mathbf{u}_k\over\mathbf{u}_k}</math>

The sequence u1, …, uk is the required system of orthogonal vectors, and the normalized vectors e1, …, ek form an orthonormal system.

To check that these formulas yield an orthogonal sequence, first compute ⟨u1, u2⟩ by substituting the above formula for u2: you will get zero. Then use this to compute ⟨u1, u3⟩ again by substituting the formula for u3: you will get zero. The general proof proceeds by mathematical induction.

Geometrically, this method proceeds as follows: to compute ui, it projects vi orthogonally onto the subspace U generated by u1, …, ui−1, which is the same as the subspace generated by v1, …, vi−1. The vector ui is then defined to be the difference between vi and this projection, guaranteed to be orthogonal to all of the vectors in the subspace U.

The Gram–Schmidt process also applies to a linearly independent infinite sequence {vi}i. The result is an orthogonal (or orthonormal) sequence {ui}i such that for natural number n: the algebraic span of v1, …, vn is the same as that of u1, …, un.

Example

Consider the following set of vectors in R2 (with the conventional inner product)

<math>S = \left\lbrace\mathbf{v}_1=\begin{pmatrix} 3 \\ 1\end{pmatrix}, \mathbf{v}_2=\begin{pmatrix}2 \\2\end{pmatrix}\right\rbrace.</math>

Now, perform Gram–Schmidt, to obtain an orthogonal set of vectors:

<math>\mathbf{u}_1=\mathbf{v}_1=\begin{pmatrix}3\\1\end{pmatrix}</math>
<math> \mathbf{u}_2 = \mathbf{v}_2 - \mathrm{proj}_{\mathbf{u}_1} \, \mathbf{v}_2 = \begin{pmatrix}2\\2\end{pmatrix} - \mathrm{proj}_{({3 \atop 1})} \, {\begin{pmatrix}2\\2\end{pmatrix}} = \begin{pmatrix} -2/5 \\6/5 \end{pmatrix}. </math>

We check that the vectors u1 and u2 are indeed orthogonal:

<math>\langle\mathbf{u}_1,\mathbf{u}_2\rangle = \left\langle \begin{pmatrix}3\\1\end{pmatrix}, \begin{pmatrix}-2/5\\6/5\end{pmatrix} \right\rangle = -\frac65 + \frac65 = 0.</math>

We can then normalize the vectors by dividing out their sizes as shown above:

<math>\mathbf{e}_1 = {1 \over \sqrt {10}}\begin{pmatrix}3\\1\end{pmatrix}</math>
<math>\mathbf{e}_2 = {1 \over \sqrt{40 \over 25}} \begin{pmatrix}-2/5\\6/5\end{pmatrix}
= {1\over\sqrt{10}} \begin{pmatrix}-1\\3\end{pmatrix}. </math>

Numerical stability

When this process is implemented on a computer, then the vectors uk are not quite orthogonal because of rounding errors. For the Gram–Schmidt process as described above this loss of orthogonality is particularly bad; therefore, it is said that the (naive) Gram–Schmidt process is numerically unstable.

The Gram–Schmidt process can be stabilized by a small modification. Instead of computing the vector uk as

<math> \mathbf{u}_k = \mathbf{v}_k - \mathrm{proj}_{\mathbf{u}_1}\,\mathbf{v}_k - \mathrm{proj}_{\mathbf{u}_2}\,\mathbf{v}_k - \cdots - \mathrm{proj}_{\mathbf{u}_{k-1}}\,\mathbf{v}_k, </math>

it is computed as

<math> \mathbf{u}_k^{(1)} = \mathbf{v}_k - \mathrm{proj}_{\mathbf{u}_1}\,\mathbf{v}_k, </math>
<math> \mathbf{u}_k^{(2)} = \mathbf{u}_k^{(1)} - \mathrm{proj}_{\mathbf{u}_2} \, \mathbf{u}_k^{(1)}, </math>
<math> \vdots </math>
<math> \mathbf{u}_k^{(k-2)} = \mathbf{u}_k^{(k-3)} - \mathrm{proj}_{\mathbf{u}_{k-2}} \, \mathbf{u}_k^{(k-3)}, </math>
<math> \mathbf{u}_k = \mathbf{u}_k^{(k-2)} - \mathrm{proj}_{\mathbf{u}_{k-1}} \, \mathbf{u}_k^{(k-2)}. </math>

This series of computations gives the same result as the original formula in exact arithmetic, but it introduces smaller errors in finite-precision arithmetic.

Algorithm

The following algorithm implements the stabilized Gram–Schmidt process. The vectors v1, …, vk are replaced by orthonormal vectors which span the same subspace.

for j from 1 to k do
for i from 1 to j − 1 do
<math> \mathbf{v}_j \leftarrow \mathbf{v}_j - \langle \mathbf{v}_j, \mathbf{v}_i \rangle \mathbf{v}_i </math> (remove component in direction vi)
end for
<math> \mathbf{v}_j \leftarrow \frac{\mathbf{v}_j}{\|\mathbf{v}_j\|} </math> (normalize)
end for

The cost of this algorithm is asymptotically 2kn2 floating point operations, where n is the size of the vectors.

Alternatives

Other orthogonalization algorithms use Householder transformations or Givens rotations. The algorithms using Householder transformations is more stable than the (stabilized) Gram–Schmidt process. On the other hand, the Gram–Schmidt process produces the jth orthogonalized vector after the jth iteration, while orthogonalization using Householder reflections produces all the vectors only at the end. This makes only the Gram–Schmidt process applicable for iterative methods like the Arnoldi iteration

References

  • Lloyd N. Trefethen and David Bau, III, Numerical Linear Algebra, Society for Industrial and Applied Mathematics, 1997. ISBN 0-89871-361-7.

External links

es:Método de ortogonalización de Gram-Schmidt fr:Procédé de Gram-Schmidt it:Ortogonalizzazione di Gram - Schmidt he:תהליך גרם-שמידט nl:Gram-Schmidtmethode ja:グラム・シュミットの正規直交化法 pl:Ortogonalizacja Grama-Schmidta sr:Грам-Шмитов поступак zh:Gram-Schmidt正交化