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Mathematical Methods for Physicists: A concise introduction - Site Map

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PROBLEMS<br />

5.10 Given the following three vectors from the vector space of real 2 2<br />

matrices:<br />

<br />

j1i ˆ 0 1 <br />

; j2i ˆ 1 1 2 1<br />

; j3i ˆ ;<br />

0 0<br />

0 1<br />

0 2<br />

determine whether they are linearly dependent or independent.<br />

5.11 If S ˆ fj1i; ji; 2 ...; jnig is a basis <strong>for</strong> a vector space V, show that every set<br />

with more than n vectors is linearly dependent.<br />

5.12 Show that any two bases <strong>for</strong> a ®nite-dimensional vector space have the same<br />

number of vectors.<br />

5.13 Consider the vector space E 3 with the Euclidean inner product. Apply the<br />

Gram±Schmidt process to trans<strong>for</strong>m the basis<br />

j1i ˆ…1; 1; 1†; j2i ˆ…0; 1; 1†; j3i ˆ…0; 0; 1†<br />

into an orthonormal basis.<br />

5.14 Consider the two linearly independent vectors of Example 5.10:<br />

jUi ˆ…3 4i†j1i‡…5 6i†j2i;<br />

jWi ˆ…1 i†j1i‡…2 3i†j2i;<br />

where j1i and j2i are an orthonormal basis. Apply the Gram±Schmidt process<br />

to trans<strong>for</strong>m the two vectors into an orthonormal basis.<br />

5.15 Show that the eigenvalue of the square of an operator is the square of the<br />

eigenvalue of the operator.<br />

1 1<br />

5.16 Show that if, <strong>for</strong> a given A , both operators A L and A R exist, then<br />

~ ~ ~<br />

A<br />

~<br />

1<br />

L<br />

ˆ A<br />

~<br />

1<br />

R A<br />

~ 1 :<br />

5.17 Show that if a unitary operator U can be written in the <strong>for</strong>m U ˆ 1 ‡ ie F ,<br />

~ ~ ~<br />

where e is a real in®nitesimally small number, then the operator F is<br />

~<br />

Hermitian.<br />

5.18 Show that the di€erential operator<br />

p ˆ p d<br />

~ i dx<br />

is linear and Hermitian in the space of all di€erentiable wave functions …x†<br />

that, say, vanish at both ends of an interval (a, b).<br />

5.19 The translation operator T…a† is de®ned to be such that T…a†…x† ˆ<br />

…x ‡ a†. Show that:<br />

(a) T…a† may be expressed in terms of the operator<br />

p ˆ p d<br />

~ i dx ;<br />

231

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