Section 7.1

Evaluation of Determinants. Solution of Linear Equations

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Problem 7.1

Let the nn vertices of a polyhedron be numbered in a definite order. Define a determinant of nnth order as follows:

If the λ\lambdath and the μ\muth vertices are the two end-points of an edge of the polyhedron, let aλμ=aμλ=1a_{\lambda \mu } = a_{\mu \lambda } = 1.

If the line joining the λ\lambdath and the μ\muth vertices is not an edge of the polyhedron, let aλμ=0a_{\lambda \mu } = 0. In particular aλλ=0a_{\lambda \lambda } = 0, λ=1,2,…,n\lambda = 1, 2, \ldots , n.

Show that the value of this determinant is independent of the manner of numbering the vertices. Form and calculate the determinants for the regular tetrahedron, hexahedron and octahedron.

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Problem 7.1.1

(continued). If exactly pp edges end in each vertex the determinant is divisible by pp.

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Problem 7.2

Calculate

∣111…1b1a1a1…a1b1b2a2…a2\multicolumn5c\dotfillb1b2b3…an∣ \begin{vmatrix} 1 & 1 & 1 & \ldots & 1 \\ b_{1} & a_{1} & a_{1} & \ldots & a_{1} \\ b_{1} & b_{2} & a_{2} & \ldots & a_{2} \\ \multicolumn {5}{c}{\dotfill } \\ b_{1} & b_{2} & b_{3} & \ldots & a_{n} \end{vmatrix}
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Problem 7.3

Prove the identity:

∣1aλ+bμ∣1n=∏j>k1,2,…,n(aj−ak)(bj−bk)∏λ,μ1,2,…,n(aλ+bμ). \left|\frac{1}{a_{\lambda } + b_{\mu }}\right|_{1}^{n} = \frac{\prod _{j > k}^{1, 2, \ldots , n} (a_{j} - a_{k})(b_{j} - b_{k})}{\prod _{\lambda , \mu }^{1, 2, \ldots , n} (a_{\lambda } + b_{\mu })}.
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Problem 7.4

Denoting the determinant of the quadratic form

∑λ=1n∑μ=1nxλxμλ+μ \sum _{\lambda =1}^{n} \sum _{\mu =1}^{n} \frac{x_{\lambda } x_{\mu }}{\lambda + \mu }

by DnD_{n}, we have

Dn=[1!2!…(n−1)!]3n!(n+1)!(n+2)!…(2n)!. D_{n} = \frac{[1! 2! \ldots (n-1)!]^{3} n!}{(n+1)! (n+2)! \ldots (2n)!}.

Also calculate the determinant Dn(α)D_{n}(\alpha ) of the quadratic form

∑λ=1n∑μ=1nxλxμλ+μ+α,α>−2. \sum _{\lambda =1}^{n} \sum _{\mu =1}^{n} \frac{x_{\lambda } x_{\mu }}{\lambda + \mu + \alpha }, \qquad \alpha > -2.
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Problem 7.5
∣(aλ−bμ)n−1∣1n=∏ν=1n−1(n−ν)n−2ν∏j>k1,2,…,n(aj−ak)(bj−bk). \left|(a_{\lambda } - b_{\mu })^{n-1}\right|_{1}^{n} = \prod _{\nu =1}^{n-1} (n-\nu )^{n-2\nu } \prod _{j > k}^{1, 2, \ldots , n} (a_{j} - a_{k})(b_{j} - b_{k}).
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Problem 7.6

Derive Theorem 86 of Part V from Theorem 48 of Part V by means of a transformation of the determinant ∣F(αλβμ)∣\left|F(\alpha_{\lambda } \beta_{\mu })\right|.

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Problem 7.7

Setting f(x)=(r1−x)(r2−x)…(rn−x)f(x) = (r_{1} - x)(r_{2} - x) \ldots (r_{n} - x), we have

∣r1aa…abr2a…abbr3…a\multicolumn5c\dotfillbbb…rn∣=af(b)−bf(a)a−b. \begin{vmatrix} r_{1} & a & a & \ldots & a \\ b & r_{2} & a & \ldots & a \\ b & b & r_{3} & \ldots & a \\ \multicolumn {5}{c}{\dotfill } \\ b & b & b & \ldots & r_{n} \end{vmatrix} = \frac{a f(b) - b f(a)}{a - b}.
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Remark.
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Add to all the n2n^{2} elements the variable xx. The determinant formed in this way is a linear function of xx and as such can be determined from two particular values.

Problem 7.8

Set Δ=ad−bc\Delta = ad - bc. Then the functional determinant

∂(aΔ,bΔ,cΔ,dΔ)∂(a,b,c,d)=3Δ4. \frac{\partial (a\Delta , b\Delta , c\Delta , d\Delta )}{\partial (a, b, c, d)} = 3\Delta ^{4}.
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Problem 7.9

Prove that ρ−2\rho - 2 is a divisor of the expression

∣ρlm+mlnl+ln]1ex]lm+mlρmn+nmnl+lnmn+nmρ∣,l≠0,  m≠0,  n≠0. \begin{vmatrix} \rho & \dfrac {l}{m} + \dfrac {m}{l} & \dfrac {n}{l} + \dfrac {l}{n} \\ ]1ex] \dfrac {l}{m} + \dfrac {m}{l} & \rho & \dfrac {m}{n} + \dfrac {n}{m} \\[1ex] \dfrac {n}{l} + \dfrac {l}{n} & \dfrac {m}{n} + \dfrac {n}{m} & \rho \end{vmatrix}, \qquad l \neq 0, \; m \neq 0, \; n \neq 0.

Determine the remaining factors.

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Problem 7.10

The determinant

∣1,  xν,  xν2,  …,  xνn−q−1,  xνn−q+1,  …,  xνn−1,  xνn∣,ν=1,2,…,n \left|1, \; x_{\nu }, \; x_{\nu }^{2}, \; \ldots , \; x_{\nu }^{n-q-1}, \; x_{\nu }^{n-q+1}, \; \ldots , \; x_{\nu }^{n-1}, \; x_{\nu }^{n}\right|, \qquad \nu = 1, 2, \ldots , n

is an alternating rational entire function of the nn numbers x1,x2,…,xnx_{1}, x_{2}, \ldots , x_{n} and thus divisible by the product of differences

∏j>k1,2,…,n(xj−xk). \prod _{j > k}^{1, 2, \ldots , n} (x_{j} - x_{k}).

Show that the quotient SqS_{q} is equal to the qqth elementary symmetric function of the nn numbers x1,x2,…,xnx_{1}, x_{2}, \ldots , x_{n}.

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Problem 7.11

Let the numbers a0,a1,a2,…,ana_{0}, a_{1}, a_{2}, \ldots , a_{n} be different from 00. Then we have identically in zz

a0∣z+a1a0a2a1a3a2…an−1an−2anan−1]1ex]−a1a0z0…000−a2a1z…00\multicolumn6c\dotfill000…−an−1an−2z∣=a0zn+a1zn−1+⋯+an. a_{0} \begin{vmatrix} z + \dfrac {a_{1}}{a_{0}} & \dfrac {a_{2}}{a_{1}} & \dfrac {a_{3}}{a_{2}} & \ldots & \dfrac {a_{n-1}}{a_{n-2}} & \dfrac {a_{n}}{a_{n-1}} \\ ]1ex] -\dfrac {a_{1}}{a_{0}} & z & 0 & \ldots & 0 & 0 \\[1ex] 0 & -\dfrac {a_{2}}{a_{1}} & z & \ldots & 0 & 0 \\ \multicolumn {6}{c}{\dotfill } \\ 0 & 0 & 0 & \ldots & -\dfrac {a_{n-1}}{a_{n-2}} & z \end{vmatrix} = a_{0} z^{n} + a_{1} z^{n-1} + \cdots + a_{n}.
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Problem 7.11.1

Let a0,a1,a2,…,b0,b1,b2,…a_{0}, a_{1}, a_{2}, \ldots , b_{0}, b_{1}, b_{2}, \ldots denote constants, zz a variable. Suppose that a0≠0a_{0} \neq 0 and that we have identically

(a0+a1z+a2z2+⋯ )(b0+b1z+b2z2+⋯ )=1. (a_{0} + a_{1} z + a_{2} z^{2} + \cdots )(b_{0} + b_{1} z + b_{2} z^{2} + \cdots ) = 1.

Then

a0n+1bn=(−1)n∣a1a000…0a2a1a00…0a3a2a1a0…0\multicolumn6c\dotfillanan−1an−2an−3…a1∣. a_{0}^{n+1} b_{n} = (-1)^{n} \begin{vmatrix} a_{1} & a_{0} & 0 & 0 & \ldots & 0 \\ a_{2} & a_{1} & a_{0} & 0 & \ldots & 0 \\ a_{3} & a_{2} & a_{1} & a_{0} & \ldots & 0 \\ \multicolumn {6}{c}{\dotfill } \\ a_{n} & a_{n-1} & a_{n-2} & a_{n-3} & \ldots & a_{1} \end{vmatrix}.

(This serves as a method of computing the reciprocal of a given power series. The supposed identity may be merely formal; no considerations of convergence are involved.)

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Problem 7.11.2

Compute the coefficient of znz^{n} in the expansion of [(1+z)a−xz]−1[(1+z)^{a} - xz]^{-1} first from Problem 11.1 then directly.

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Problem 7.11.3

Analogously to Problem 11.2, compute the coefficient of znz^{n} in the expansion of [ez−xz]−1[e^{z} - xz]^{-1}.

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Problem 7.12

Let a1,a2,a3,b1,b2,b3,ca_{1}, a_{2}, a_{3}, b_{1}, b_{2}, b_{3}, c be real numbers. The system

−a3x2+a2x3=b1,a3x1+a2x2−a1x3=b2,−a2x1+a1x2−a1x3=b3,a1x1+a2x2+a3x3=c \begin{aligned} -a_{3} x_{2} + a_{2} x_{3} & = b_{1}, \\ a_{3} x_{1} \phantom{{} + a_{2} x_{2}} - a_{1} x_{3} & = b_{2}, \\ -a_{2} x_{1} + a_{1} x_{2} \phantom{{} - a_{1} x_{3}} & = b_{3}, \\ a_{1} x_{1} + a_{2} x_{2} + a_{3} x_{3} & = c \end{aligned}

can be consistent in two different ways. In one case the unknowns x1,x2,x3x_{1}, x_{2}, x_{3} are completely undetermined, in the other case they are completely determined.

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Problem 7.13

Let the entire function

1+c1z+c2z2+c3z3+⋯ 1 + c_{1} z + c_{2} z^{2} + c_{3} z^{3} + \cdots

have all distinct zeros a1,a2,…,an,…,a_{1}, a_{2}, \ldots , a_{n}, \ldots ,

0<∣a1∣<∣a2∣<⋯<∣an∣<⋯ . 0 < \left|a_{1}\right| < \left|a_{2}\right| < \cdots < \left|a_{n}\right| < \cdots .

Consider the system of nn equations

1+a1u1(n)+a12u2(n)+⋯+a1nun(n)=0,1+a2u1(n)+a22u2(n)+⋯+a2nun(n)=0,\dotfill1+anu1(n)+an2u2(n)+⋯+annun(n)=0 \begin{aligned} 1 + a_{1} u_{1}^{(n)} + a_{1}^{2} u_{2}^{(n)} + \cdots + a_{1}^{n} u_{n}^{(n)} & = 0, \\ 1 + a_{2} u_{1}^{(n)} + a_{2}^{2} u_{2}^{(n)} + \cdots + a_{2}^{n} u_{n}^{(n)} & = 0, \\ & \dotfill \\ 1 + a_{n} u_{1}^{(n)} + a_{n}^{2} u_{2}^{(n)} + \cdots + a_{n}^{n} u_{n}^{(n)} & = 0 \end{aligned}

that completely determine the uk(n)u_{k}^{(n)}. If

1∣a1∣+1∣a2∣+⋯+1∣an∣+⋯ \frac{1}{\left|a_{1}\right|} + \frac{1}{\left|a_{2}\right|} + \cdots + \frac{1}{\left|a_{n}\right|} + \cdots

is convergent, then lim⁡n→∞uk(n)\lim_{n \rightarrow \infty } u_{k}^{(n)} exists, but it is not necessarily true that

lim⁡n→∞uk(n)=ck. \lim _{n \rightarrow \infty } u_{k}^{(n)} = c_{k}.
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Remark.
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One solution of the infinite system

1+aνu1+aν2u2+⋯=0,ν=1,2,3,… 1 + a_{\nu } u_{1} + a_{\nu }^{2} u_{2} + \cdots = 0, \qquad \nu = 1, 2, 3, \ldots

is: u1=c1,u2=c2,u3=c3,…u_{1} = c_{1}, u_{2} = c_{2}, u_{3} = c_{3}, \ldots.

Problem 7.14

In the equations

c11z1+c12z2+⋯+c1nzn=0,c21z1+c22z2+⋯+c2nzn=0,\dotfillcn1z1+cn2z2+⋯+cnnzn=0 \begin{aligned} c_{11} z_{1} + c_{12} z_{2} + \cdots + c_{1n} z_{n} & = 0, \\ c_{21} z_{1} + c_{22} z_{2} + \cdots + c_{2n} z_{n} & = 0, \\ & \dotfill \\ c_{n1} z_{1} + c_{n2} z_{2} + \cdots + c_{nn} z_{n} & = 0 \end{aligned}

let the coefficients and the unknowns be complex:

cλμ=aλμ+ibλμ,zμ=xμ+iyμ, c_{\lambda \mu } = a_{\lambda \mu } + i b_{\lambda \mu }, \qquad z_{\mu } = x_{\mu } + i y_{\mu },

aλμ,bλμ,xμ,yμa_{\lambda \mu }, b_{\lambda \mu }, x_{\mu }, y_{\mu } real. For the equations to admit not only the identically zero solution

z1=z2=⋯=zn=0,i.e.x1=x2=⋯=xn=y1=y2=⋯=yn=0, z_{1} = z_{2} = \cdots = z_{n} = 0, \qquad \text{i.e.} \quad x_{1} = x_{2} = \cdots = x_{n} = y_{1} = y_{2} = \cdots = y_{n} = 0,

it is necessary and sufficient that the determinant ∣cλμ∣1n\left|c_{\lambda \mu }\right|_{1}^{n} vanishes. This yields two equations in the 2n22n^{2} real numbers aλμ,bλμa_{\lambda \mu }, b_{\lambda \mu }. On the other hand the given equations may be written as 2n2n linear homogeneous equations for 2n2n real unknowns. The necessary and sufficient condition for the existence of a not identically vanishing solution now consists in the vanishing of a real determinant, i.e. in one equation in the aλμ,bλμa_{\lambda \mu }, b_{\lambda \mu }. How can this be correct?

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Problem 7.15

The six terms in the expansion of a third-order determinant cannot all be positive.

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Problem 7.16

The rule for the expansion of a determinant consists of two parts. The first part specifies what products are to be formed from the elements, while the second part determines the sign of these products.

The second part may be simplified in the case of second-order determinants in the following manner:

Associate with the elements

(a11a12a21a22) the signs (++−+) respectively. \begin{pmatrix} a_{11} & a_{12} \\ a_{21} & a_{22} \end{pmatrix} \text{ the signs } \begin{pmatrix} + & + \\ - & + \end{pmatrix} \text{ respectively.}

Then form the products prescribed in the first part from the elements, each with its fixed associated sign.

Now prove that a corresponding simplification is impossible in the case of a determinant of order higher than two, i.e. it is impossible to associate with the n2n^{2} elements n2n^{2} fixed signs in such a way that, if we form the products prescribed in the first part of the expansion rule from the elements each with its associated sign, we automatically obtain the correct sign in all the products.

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