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Unformatted text preview: 14 CHAPTER 2. MATHEMATICAL PREREQUISITES (cos 45◦ , − sin 45◦ ). The dot product of (cos 45◦ , sin 45◦ ) and (cos 45◦ , − sin 45◦ ) is cos2 45◦ −
sin2 45◦ . That is zero, because cos 45◦ = sin 45◦ , so the two eigenvectors are orthogonal.
In linear algebra, you would write the relationship r2 = Ar out as:
x2
y2 2.6.3 x
y 11
11 = = x+y
x+y Solution hermc Question: Show that the operator 2 is a Hermitian operator, but i is not.
Answer: By deﬁnition, 2 corresponds to multiplying by 2, so 2g is simply the function 2g .
Now write the inner product f 2g and see whether it is the same as 2f g for any f and g :
f 2g = all x f ∗ 2g dx = all x (2f )∗ g dx = 2f g since the complex conjugate does not aﬀect a real number like 2. So 2 is indeed Hermitian.
On the other hand,
f ig = all x f ∗ ig dx = all x −(if )∗ g dx = − if g so i is not Hermitian. An operator like i that ﬂips over the sign of an inner product if it is
moved to the other side is called “skewHermitian”. An operator like 2 + i is neither Hermitian
nor skewHermitian. 2.6.4 Solution hermd Question: Generalize the previous question, by showing that any complex constant c comes
out of the right hand side of an inner product unchanged, but out of the left hand side as its
complex conjugate;
f cg = c f g
cf g = c∗ f g . As a result, a number c is only a Hermitian operator if it is real: if c is complex, the two
expressions above are not the same.
Answer: Since constants can be taken out of an integral:
f cg =
cf g = all x all x f ∗ cg dx = c (cf )∗ g dx = c∗ all x f ∗ g dx = c f g all x f ∗ g dx = c∗ f g . ...
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This note was uploaded on 01/06/2012 for the course PHY 3604 taught by Professor Dr.danielarenas during the Fall '11 term at UNF.
 Fall '11
 Dr.DanielArenas
 mechanics

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