Givens method

Primary authors of this description: A.V.Frolov, Vad.V.Voevodin (Section 2.2)

1 Properties and structure of the algorithm[edit]

1.1 General description of the algorithm

Givens' method (which is also called the rotation method in the Russian mathematical literature) is used to represent a matrix in the form $A = QR$, where $Q$ is a unitary and $R$ is an upper triangular matrix. The matrix $Q$ is not stored and used in its explicit form but rather as the product of rotations. Each (Givens) rotation can be specified by a pair of indices and a single parameter.

In a conventional implementation of Givens' method, this fact makes it possible to avoid using additional arrays by storing the results of decomposition in the array originally occupied by $A$. Various uses are possible for the $QR$ decomposition of $A$. It can be used for solving a SLAE (System of Linear Algebraic Equations) $Ax = b$ or as a step in the so-called $QR$ algorithm for finding the eigenvalues of a matrix.

At each step of Givens' method, two rows of the matrix under transformation are rotated. The parameter of this transformation is chosen so as to eliminate one of the entries in the current matrix. First, the entries in the first column are eliminated one after the other, then the same is done for the second column, etc., until the column $n-1$. The resulting matrix is $R$. The step of the method is split into two parts: the choice of the rotation parameter and the rotation itself performed over two rows of the current matrix. The entries of these rows located to the left of the pivot column are zero; thus, no modifications are needed there. The entries in the pivot column are rotated simultaneously with the choice of the rotation parameter. Hence, the second part of the step consists in rotating two-dimensional vectors formed of the entries of the rotated rows that are located to the right of the pivot column. In terms of operations, the update of a column is equivalent to multiplying two complex numbers (or to four multiplications, one addition and one subtraction for real numbers); one of these complex numbers is of modulus 1. The choice of the rotation parameter from the two entries of the pivot column is a more complicated procedure, which is explained, in particular, by the necessity of minimizing roundoff errors. The tangent [math]t[/math] of half the rotation angle is normally used to store information about the rotation matrix. The cosine [math]c[/math] and the sine [math]s[/math] of the rotation angle itself are related to [math]t[/math] via the simple formulas (the so-called combat formulas of trigonometry)

[math]c = (1 - t^2)/(1 + t^2), s = 2t/(1 + t^2)[/math]

It is the value [math]t[/math] that is usually stored in the corresponding array entry.

1.2 Mathematical description of the algorithm

In order to obtain the [math]QR[/math] decomposition of a square matrix [math]A[/math], this matrix is reduced to the upper triangular matrix [math]R[/math] (where [math]R[/math] means right) by successively multiplying [math]A[/math] on the left последовательностью умножений её слева на матрицы вращения [math]T_{1 2}, T_{1 3}, ..., T_{1 n}, T_{2 3}, T_{2 4}, ..., T_{2 n}, ... , T_{n-2 n}, T_{n-1 n}[/math].

Каждая из матриц [math]T_{i j}[/math] задаёт вращение в 2-мерном подпространстве, связанном с [math]i[/math]-й и [math]j[/math]-й компонентами столбцов, остальные компоненты не меняются. При этом вращение подбирается так, чтобы элемент новой матрицы в [math]j[/math]-й строке и [math]i[/math]-м столбце стал нулевым. Поскольку вращения и тождественные преобразования нулевых векторов оставляют их нулевыми, то последующие вращения сохраняют полученные ранее нули слева и сверху от текущего обнуляемого элемента.

В конце процесса имеем [math]R=T_{n-1 n}T_{n-2 n}T_{n-2 n-1}...T_{1 3}T_{1 2}A[/math].

Так как матрицы вращения унитарны, то естественно получается [math]Q=(T_{n-1 n}T_{n-2 n}T_{n-2 n-1}...T_{1 3}T_{1 2})^* =T_{1 2}^* T_{1 3}^* ...T_{1 n}^* T_{2 3}^* T_{2 4}^* ...T_{2 n}^* ...T_{n-2 n}^* T_{n-1 n}^*[/math] и [math]A=QR[/math].

В вещественном случае матрицы вращения ортогональны и [math]Q=(T_{n-1 n}T_{n-2 n}T_{n-2 n-1}...T_{1 3}T_{1 2})^T =T_{1 2}^T T_{1 3}^T ...T_{1 n}^T T_{2 3}^T T_{2 4}^T ...T_{2 n}^T ...T_{n-2 n}^T T_{n-1 n}^T[/math].

Для завершения математического описания остаётся записать вычисление матрицы вращения [math]T_{i j}[/math] и формулы её умножения на текущую промежуточную матрицу.