Section 7.5

Determinants of Systems of Functions

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Problem 7.55

We term the determinant

∣f1(x)f1′(x)f1′′(x)…f1(n−1)(x)f2(x)f2′(x)f2′′(x)…f2(n−1)(x)f3(x)f3′(x)f3′′(x)…f3(n−1)(x)\multicolumn5c\dotfillfn(x)fn′(x)fn′′(x)…fn(n−1)(x)∣=W[f1(x),f2(x),…,fn(x)] \begin{vmatrix} f_{1}(x) & f_{1}'(x) & f_{1}''(x) & \ldots & f_{1}^{(n-1)}(x) \\ f_{2}(x) & f_{2}'(x) & f_{2}''(x) & \ldots & f_{2}^{(n-1)}(x) \\ f_{3}(x) & f_{3}'(x) & f_{3}''(x) & \ldots & f_{3}^{(n-1)}(x) \\ \multicolumn {5}{c}{\dotfill } \\ f_{n}(x) & f_{n}'(x) & f_{n}''(x) & \ldots & f_{n}^{(n-1)}(x) \end{vmatrix} = W[f_{1}(x), f_{2}(x), \ldots , f_{n}(x)]

the Wronskian determinant of the system of functions f1(x),f2(x),…,fn(x)f_{1}(x), f_{2}(x), \ldots , f_{n}(x).

If cλμc_{\lambda \mu } are constants, then we have

W(c11f1+c12f2+⋯+c1nfn,  c21f1+c22f2+⋯+c2nfn,  …,  cn1f1+cn2f2+⋯+cnnfn)=∣cλμ∣1n⋅W(f1,f2,…,fn). W(c_{11} f_{1} + c_{12} f_{2} + \cdots + c_{1n} f_{n}, \; c_{21} f_{1} + c_{22} f_{2} + \cdots + c_{2n} f_{n}, \; \ldots , \; c_{n1} f_{1} + c_{n2} f_{2} + \cdots + c_{nn} f_{n}) = \left|c_{\lambda \mu }\right|_{1}^{n} \cdot W(f_{1}, f_{2}, \ldots , f_{n}).
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Problem 7.56
W[f1(φ(x)),f2(φ(x)),…,fn(φ(x))]=φ′(x)n(n−1)2W[f1(y),f2(y),…,fn(y)], W[f_{1}(\varphi (x)), f_{2}(\varphi (x)), \ldots , f_{n}(\varphi (x))] = \varphi '(x)^{\frac{n(n-1)}{2}} W[f_{1}(y), f_{2}(y), \ldots , f_{n}(y)],

setting y=φ(x)y = \varphi (x) on the right-hand side.

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Problem 7.57
W(φf1,φf2,…,φfn)=φnW(f1,f2,…,fn). W(\varphi f_{1}, \varphi f_{2}, \ldots , \varphi f_{n}) = \varphi ^{n} W(f_{1}, f_{2}, \ldots , f_{n}).
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Problem 7.58
1f1nW(f1,f2,…,fn)=W[(f2f1)′,(f3f1)′,…,(fnf1)′]. \frac{1}{f_{1}^{n}} W(f_{1}, f_{2}, \ldots , f_{n}) = W\left[ \left( \frac{f_{2}}{f_{1}} \right)', \left( \frac{f_{3}}{f_{1}} \right)', \ldots , \left( \frac{f_{n}}{f_{1}} \right)' \right].
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Problem 7.59
ddxW(f1,…,fn−2,fn)W(f1,…,fn−2,fn−1)=W(f1,…,fn−2)W(f1,…,fn−2,fn−1,fn)[W(f1,…,fn−2,fn−1)]2. \frac{d}{dx} \frac{W(f_{1}, \ldots , f_{n-2}, f_{n})}{W(f_{1}, \ldots , f_{n-2}, f_{n-1})} = \frac{W(f_{1}, \ldots , f_{n-2}) W(f_{1}, \ldots , f_{n-2}, f_{n-1}, f_{n})}{[W(f_{1}, \ldots , f_{n-2}, f_{n-1})]^{2}}.
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Problem 7.60

If W(f1,f2,…,fn−1,fn)W(f_{1}, f_{2}, \ldots , f_{n-1}, f_{n}) vanishes at every point and W(f1,f2,…,fn−1)W(f_{1}, f_{2}, \ldots , f_{n-1}) at no point of the interval a,ba, b, then there exist n−1n-1 constants c1,c2,…,cn−1c_{1}, c_{2}, \ldots , c_{n-1} such that in the whole interval a,ba, b

fn(x)=c1f1(x)+c2f2(x)+⋯+cn−1fn−1(x). f_{n}(x) = c_{1} f_{1}(x) + c_{2} f_{2}(x) + \cdots + c_{n-1} f_{n-1}(x).
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Problem 7.61

If f1(x),f2(x),…,fn(x)f_{1}(x), f_{2}(x), \ldots , f_{n}(x) are nn linearly independent solutions of the homogeneous linear nnth order differential equation

y(n)+φ1(x)y(n−1)+φ2(x)y(n−2)+⋯+φn(x)y=0, y^{(n)} + \varphi _{1}(x) y^{(n-1)} + \varphi _{2}(x) y^{(n-2)} + \cdots + \varphi _{n}(x) y = 0,

then we have for an arbitrary function yy

y(n)+φ1(x)y(n−1)+φ2(x)y(n−2)+⋯+φn(x)y=W(f1,f2,…,fn,y)W(f1,f2,…,fn). y^{(n)} + \varphi _{1}(x) y^{(n-1)} + \varphi _{2}(x) y^{(n-2)} + \cdots + \varphi _{n}(x) y = \frac{W(f_{1}, f_{2}, \ldots , f_{n}, y)}{W(f_{1}, f_{2}, \ldots , f_{n})}.
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Problem 7.62

(continued). Set

1=W0,f1=W1,W(f1,f2)=W2,…,W(f1,f2,…,fn)=Wn. 1 = W_{0}, \qquad f_{1} = W_{1}, \qquad W(f_{1}, f_{2}) = W_{2}, \qquad \ldots , \qquad W(f_{1}, f_{2}, \ldots , f_{n}) = W_{n}.

Then we have for an arbitrary function yy

y(n)+φ1(x)y(n−1)+φ2(x)y(n−2)+⋯+φn(x)y y^{(n)} + \varphi _{1}(x) y^{(n-1)} + \varphi _{2}(x) y^{(n-2)} + \cdots + \varphi _{n}(x) y ≡WnWn−1⋅ddxWn−12Wn−2Wn⋯ddxW22W1W3⋅ddxW12W0W2⋅ddxyW1. \equiv \frac{W_{n}}{W_{n-1}} \cdot \frac{d}{dx} \frac{W_{n-1}^{2}}{W_{n-2} W_{n}} \cdots \frac{d}{dx} \frac{W_{2}^{2}}{W_{1} W_{3}} \cdot \frac{d}{dx} \frac{W_{1}^{2}}{W_{0} W_{2}} \cdot \frac{d}{dx} \frac{y}{W_{1}}.

This representation of the linear differential expression, in terms of nn independent solutions of the homogeneous differential equation, is analogous to the factorization of a polynomial of degree nn in terms of its nn zeros.

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Problem 7.63

Let f1(x),f2(x),…,fn(x)f_{1}(x), f_{2}(x), \ldots , f_{n}(x) be continuous real functions, defined in the interval a,ba, b. The determinant

∣∫abfλ(x)fμ(x) dx∣λ,μ=1,2,…,n \left|\int _{a}^{b} f_{\lambda }(x) f_{\mu }(x) \, dx\right|_{\lambda , \mu = 1, 2, \ldots , n}

is never negative. It vanishes if and only if between the functions f1(x),f2(x),…,fn(x)f_{1}(x), f_{2}(x), \ldots , f_{n}(x) there exists a homogeneous linear relation with constant coefficients, not all 00.

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Problem 7.64

(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} \[ is never negative. It vanishes if and only if the functions $f_{1}(x), f_{2}(x), \ldots , f_{n}(x)$ differ from one another only by constant factors, or, in other words, if they are all multiples of one of them. \]
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Problem 7.65

(continued). The determinant

∣e∫abfλ(x)fμ(x) dx∣λ,μ=1,2,…,n \left|e^{\int _{a}^{b} f_{\lambda }(x) f_{\mu }(x) \, dx}\right|_{\lambda , \mu = 1, 2, \ldots , n}

is never negative. It vanishes if and only if among the functions f1(x),f2(x),…,fn(x)f_{1}(x), f_{2}(x), \ldots , f_{n}(x) there are two identically equal.

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Problem 7.66

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 f(x)f(x) be defined for x>0x > 0, non-increasing there, f(x)≥0f(x) \geq 0, but not identically =0=0. Moreover let the real numbers a1,a2,…,ana_{1}, a_{2}, \ldots , a_{n} be distinct. Assuming the existence of all the integrals that occur, the determinant

∣(aλ+aμ+1)∫0∞xaλ+aμf(x) dx∣λ,μ=1,2,…,n \left|(a_{\lambda }+a_{\mu }+1) \int _{0}^{\infty } x^{a_{\lambda }+a_{\mu }} f(x) \, dx\right|_{\lambda , \mu = 1, 2, \ldots , n}

is never negative. It is =0=0 if and only if f(x)f(x) is a piecewise constant function with not more than n−1n-1 jump discontinuities.

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Problem 7.67

Let the function f(ϑ)f(\vartheta ) be properly integrable in the interval 0≤ϑ<2π0 \leq \vartheta < 2\pi. Let its Fourier series (Section 4 of Part VI) be

f(ϑ)∼a0+2∑n=1∞(ancos⁡nϑ+bnsin⁡nϑ). f(\vartheta ) \sim a_{0} + 2 \sum _{n=1}^{\infty } (a_{n} \cos n\vartheta + b_{n} \sin n\vartheta ).

The Hermite forms

Tn(f)=∑λ=0n∑μ=0ncμ−λxλxˉμ T_{n}(f) = \sum _{\lambda =0}^{n} \sum _{\mu =0}^{n} c_{\mu -\lambda } x_{\lambda } \bar{x}_{\mu }

formed from the constants c0=a0c_{0} = a_{0}, cn=an+ibnc_{n} = a_{n} + ib_{n}, c−n=cˉnc_{-n} = \bar{c}_{n}, n=1,2,3,…n = 1, 2, 3, \ldots, are called the Toeplitz forms associated with f(ϑ)f(\vartheta ). (Cf. Problem 43).

Form the Toeplitz forms that belong to the following functions:

f(ϑ)=c=const.,f(ϑ)=a0+2(a1cos⁡ϑ+b1sin⁡ϑ), f(\vartheta ) = c = \text{const.}, \qquad f(\vartheta ) = a_{0} + 2(a_{1} \cos \vartheta + b_{1} \sin \vartheta ), f(ϑ)=1−r21−2rcos⁡ϑ+r2,0<r<1. f(\vartheta ) = \frac{1-r^{2}}{1-2r\cos \vartheta +r^{2}}, \qquad 0 < r < 1.
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Problem 7.68

If the function f(ϑ)f(\vartheta ) is positive in the interval 0≤ϑ<2π0 \leq \vartheta < 2\pi, then all its associated Toeplitz forms are positive definite. More precisely: If f(ϑ)f(\vartheta ) lies between the bounds m≤f(ϑ)≤Mm \leq f(\vartheta ) \leq M in the interval 0≤ϑ<2π0 \leq \vartheta < 2\pi, then we have

m≤Tn(f)≤M, m \leq T_{n}(f) \leq M,

provided that the variables x0,x1,…,xnx_{0}, x_{1}, \ldots , x_{n} satisfy the condition Tn(1)=1T_{n}(1) = 1. The equality sign can hold here only if f(ϑ)=const.f(\vartheta ) = \text{const.} at every point of continuity of f(ϑ)f(\vartheta ).

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Problem 7.69

Calculate the determinant Dn(f)D_{n}(f) of the form Tn(f)T_{n}(f) for the functions in Problem 67 and show that, if f(ϑ)f(\vartheta ) is everywhere positive,

lim⁡n→∞Dn(f)n+1=e12π∫02πlog⁡f(ϑ) dϑ=G(f). \lim _{n \rightarrow \infty } \sqrt[n+1]{D_{n}(f)} = e^{\frac{1}{2\pi } \int _{0}^{2\pi } \log f(\vartheta ) \, d\vartheta } = \mathfrak {G}(f).
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Problem 7.70

Let f(ϑ)f(\vartheta ) be a trigonometric polynomial of first order and let hh be a parameter. The determinant Dn(f−h)D_{n}(f-h) of the Toeplitz form Tn(f−h)T_{n}(f-h) associated with f(ϑ)−hf(\vartheta )-h is a polynomial of degree n+1n+1 in hh with only real zeros. Calculate these zeros.

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Problem 7.71

(continued). The zeros h0n,h1n,…,hnnh_{0n}, h_{1n}, \ldots , h_{nn} of Dn(f−h)D_{n}(f-h) all lie between the minimum and the maximum of f(ϑ)f(\vartheta ), that is m≤hνn≤Mm \leq h_{\nu n} \leq M, if m≤f(ϑ)≤Mm \leq f(\vartheta ) \leq M in the interval 0,2π0, 2\pi. Moreover if F(h)F(h) denotes an arbitrary properly integrable function in the interval m≤h≤Mm \leq h \leq M, then we have

lim⁡n→∞F(h0n)+F(h1n)+⋯+F(hnn)n+1=12π∫02πF[f(ϑ)] dϑ. \lim _{n \rightarrow \infty } \frac{F(h_{0n})+F(h_{1n})+\cdots +F(h_{nn})}{n+1} = \frac{1}{2\pi } \int _{0}^{2\pi } F[f(\vartheta )] \, d\vartheta .
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Problem 7.72

Let the Hermitian form

∑λ=0n∑μ=0ncλ−μxλxˉμ,c−ν=cˉν, \sum _{\lambda =0}^{n} \sum _{\mu =0}^{n} c_{\lambda -\mu } x_{\lambda } \bar{x}_{\mu }, \qquad c_{-\nu } = \bar{c}_{\nu },

be positive definite. Then all the zeros of the polynomial

∣c0c1c2…cnc−1c0c1…cn−1c−2c−1c0…cn−2\multicolumn5c\dotfillc−n+1c−n+2c−n+3…c11zz2…zn∣ \begin{vmatrix} c_{0} & c_{1} & c_{2} & \ldots & c_{n} \\ c_{-1} & c_{0} & c_{1} & \ldots & c_{n-1} \\ c_{-2} & c_{-1} & c_{0} & \ldots & c_{n-2} \\ \multicolumn {5}{c}{\dotfill } \\ c_{-n+1} & c_{-n+2} & c_{-n+3} & \ldots & c_{1} \\ 1 & z & z^{2} & \ldots & z^{n} \end{vmatrix}

lie in the interior of the unit circle.

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