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← 2013 Paper 1

UPSC Maths 2013 Paper 1 Q2b-i — Solution

8 marks · Section A

Question

Let A=[1111ω2ω1ωω2]A=\begin{bmatrix}1 & 1 & 1\\ 1 & \omega^{2} & \omega\\ 1 & \omega & \omega^{2}\end{bmatrix} where ω(1)\omega(\ne 1) is a cube root of unity. If λ1,λ2,λ3\lambda_1,\lambda_2,\lambda_3 denote the eigenvalues of A2A^{2}, show that λ1+λ2+λ39|\lambda_1|+|\lambda_2|+|\lambda_3|\le 9.

Technique

Compute AAA^{*}A; recognise the scalar-matrix outcome; use normality to convert singular values \to eigenvalue moduli.

Solution

Strategy. Compute AAA^{*}A and exploit that it turns out to be a scalar matrix. This makes AA (and hence A2A^{2}) a scalar multiple of a unitary matrix, so all eigenvalues lie on a circle.

Step 1 — Key facts about ω\omega

ω1\omega\ne 1 and ω3=1\omega^{3}=1, so 1+ω+ω2=01+\omega+\omega^{2}=0. Conjugation: ω=ω2\overline{\omega}=\omega^{2} and ω2=ω\overline{\omega^{2}}=\omega (the two non-real cube roots of unity are complex conjugates).

Also, AA is symmetric (AT=AA^{T}=A), so A=AT=AA^{*}=\overline{A^{T}}=\overline A.

Step 2 — Compute AAA^{*}A

A=[1111ωω21ω2ω]\overline A=\begin{bmatrix}1&1&1\\1&\omega&\omega^{2}\\1&\omega^{2}&\omega\end{bmatrix}. Compute (AA)ij=(AA)ij=kAkiAkj=kAikAkj(A^{*}A)_{ij}=(\overline A A)_{ij}=\sum_{k}\overline{A_{ki}}A_{kj}=\sum_{k}\overline{A_{ik}}A_{kj} (using symmetry Aki=AikA_{ki}=A_{ik}). Equivalently, dot the iith row of A\overline A with the jjth column of AA:

i\ji\backslash j123
11+1+1=31+1+1=31+ω2+ω=01+\omega^{2}+\omega=01+ω+ω2=01+\omega+\omega^{2}=0
21+ω+ω2=01+\omega+\omega^{2}=01+ω3+ω3=31+\omega^{3}+\omega^{3}=31+ω2+ω4=1+ω2+ω=01+\omega^{2}+\omega^{4}=1+\omega^{2}+\omega=0
31+ω2+ω=01+\omega^{2}+\omega=01+ω4+ω2=01+\omega^{4}+\omega^{2}=01+ω3+ω3=31+\omega^{3}+\omega^{3}=3

Therefore

  AA=3I3.  \boxed{\;A^{*}A=3\,I_{3}.\;}

So 13A\tfrac{1}{\sqrt 3}A is unitary; equivalently, the singular values of AA are all 3\sqrt 3.

Step 3 — A2A^{2} is also a scalar-times-unitary

(A2)(A2)=AAAA=A(AA)A=A(3I)A=3AA=9I(A^{2})^{*}(A^{2})=A^{*}A^{*}AA=A^{*}(A^{*}A)A=A^{*}(3I)A=3\,A^{*}A=9\,I.

So 13A2\tfrac{1}{3}A^{2} is unitary; equivalently, singular values of A2A^{2} are all 33.

Step 4 — A2A^{2} is normal; eigenvalues have modulus equal to singular values

A2A^{2} commutes with its adjoint: (A2)(A2)=9I=(A2)(A2)(A^{2})^{*}(A^{2})=9I=(A^{2})(A^{2})^{*} (the second equality is the same calculation applied to AAAA^{*}, which also equals 3I3I by an identical computation using symmetry of AA).

For a normal matrix BB, the absolute values of the eigenvalues equal the singular values (this is the spectral theorem — B=UDUB=U^{*}DU unitarily, so λi(B)=σi(B)|\lambda_i(B)|=\sigma_i(B)).

Therefore λi(A2)=σi(A2)=3|\lambda_i(A^{2})|=\sigma_i(A^{2})=3 for i=1,2,3i=1,2,3.

Step 5 — Sum up

λ1+λ2+λ3=3+3+3=9.|\lambda_1|+|\lambda_2|+|\lambda_3|=3+3+3=9.

In particular,

Answer

  λ1+λ2+λ39,  \boxed{\;|\lambda_1|+|\lambda_2|+|\lambda_3|\le 9,\;}

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