(c)(d) The region beyond L/2 is classically forbidden and so the
probability of finding the particle in this region is very small,
although non-zero.
(e) The wavefunctions will become those for the simple harmonic
oscillator.11.22 (a)(b)(c)(d)F=−k(xn−xn− 1 ) +k(xn+ 1 −xn)(e)CHAPTER 12
12.1
12.2 (a) The ground state is n= 1(b) The first excited state is n= 212.3
12.4
2 0 2 1 058 10
00
−=r = =. ×−^10
aso ra mψ(^200) π 03 0
(^12)
4
1
2
=− 2 /^0
⎛
⎝
⎜
⎜
⎞
⎠
⎟
⎟
−
ar
aeraE
hcRh
=− =−.
3
2 15 eVE
hcRh
=− =−.
2
2 34 eVE
hcRh
=− =−.
1
2 13 6eVVre
r()=
−^2
4 πε 0−+−+−−+
Z^22
2 12
1
2
22 mxx
k
xx x x
nnnnnnd
dψ() [( ) ( )]]()ψψnnxEx= ()ψψ*d αdforthe
20
2
222
ÅÅxxx Nex x∞∞
−
∫∫() () =
/ gground state−+=
Z^22
22
22 μψψψd
dxxk
() xx Ex() ()μ ρρ()()
=
+
=
+
=
mm
mm(^12) mm
12
14 14
14 14
7
Δ
Δ
9
Z.
(.
==
×
×
−
2 −1 054 10
2 1 054 10
34
mx^34Js
kkg mms
)(. ).
05 10
11 10 10^111
×
− =× −
466 ANSWERS TO PROBLEMS
9781405124362_5_end.qxd 4/29/08 9:17 Page 466