Determinants of Systems of Functions
[18/100%]We term the determinant
the Wronskian determinant of the system of functions .
If are constants, then we have
setting on the right-hand side.
If vanishes at every point and at no point of the interval , then there exist constants such that in the whole interval
If are linearly independent solutions of the homogeneous linear th order differential equation
then we have for an arbitrary function
(continued). Set
Then we have for an arbitrary function
This representation of the linear differential expression, in terms of independent solutions of the homogeneous differential equation, is analogous to the factorization of a polynomial of degree in terms of its zeros.
Let be continuous real functions, defined in the interval . The determinant
is never negative. It vanishes if and only if between the functions there exists a homogeneous linear relation with constant coefficients, not all .
(continued). The determinant
\begin{vmatrix} \displaystyle \int _{a}^{b} (f_{2}^{2}+f_{3}^{2}+\cdots +f_{n}^{2}) \, dx & -\displaystyle \int _{a}^{b} f_{1} f_{2} \, dx & \ldots & -\displaystyle \int _{a}^{b} f_{1} f_{n} \, dx \\ ]2ex] -\displaystyle \int _{a}^{b} f_{2} f_{1} \, dx & \displaystyle \int _{a}^{b} (f_{1}^{2}+f_{3}^{2}+\cdots +f_{n}^{2}) \, dx & \ldots & -\displaystyle \int _{a}^{b} f_{2} f_{n} \, dx \\[2ex] \multicolumn {4}{c}{\dotfill } \\ ]1ex] -\displaystyle \int _{a}^{b} f_{n} f_{1} \, dx & -\displaystyle \int _{a}^{b} f_{n} f_{2} \, dx & \ldots & \displaystyle \int _{a}^{b} (f_{1}^{2}+f_{2}^{2}+\cdots +f_{n-1}^{2}) \, dx \end{vmatrix} \[ is never negative. It vanishes if and only if the functions $f_{1}(x), f_{2}(x), \ldots , f_{n}(x)$ differ from one another only by constant factors, or, in other words, if they are all multiples of one of them. \](continued). The determinant
is never negative. It vanishes if and only if among the functions there are two identically equal.
A theorem mentioned in passing by Gauss in his Theoria combinationis observationum [Werke, Vol. 4, p. 12, cf. the last two lines of Art. 11] may be generalized as follows:
Let be defined for , non-increasing there, , but not identically . Moreover let the real numbers be distinct. Assuming the existence of all the integrals that occur, the determinant
is never negative. It is if and only if is a piecewise constant function with not more than jump discontinuities.
Let the function be properly integrable in the interval . Let its Fourier series (Section 4 of Part VI) be
The Hermite forms
formed from the constants , , , , are called the Toeplitz forms associated with . (Cf. Problem 43).
Form the Toeplitz forms that belong to the following functions:
If the function is positive in the interval , then all its associated Toeplitz forms are positive definite. More precisely: If lies between the bounds in the interval , then we have
provided that the variables satisfy the condition . The equality sign can hold here only if at every point of continuity of .
Calculate the determinant of the form for the functions in Problem 67 and show that, if is everywhere positive,
Let be a trigonometric polynomial of first order and let be a parameter. The determinant of the Toeplitz form associated with is a polynomial of degree in with only real zeros. Calculate these zeros.
(continued). The zeros of all lie between the minimum and the maximum of , that is , if in the interval . Moreover if denotes an arbitrary properly integrable function in the interval , then we have
Let the Hermitian form
be positive definite. Then all the zeros of the polynomial
lie in the interior of the unit circle.