you can do the integration using mathematica type the
TRANSCRIPT
Problem 1 Griffiths 1.5
Ξ¨ π₯, π‘ = π΄πβπ|π₯|πβπππ‘
(a) 1 = |Ξ¨|2ππ₯
β
ββ
= ΨΨβππ₯β
ββ
= π΄2 πβ2π|π₯|ππ₯β
ββ
= 2π΄2 πβ2ππ₯ππ₯β
0
= 2π΄2πβ2ππ₯
β2π β0
=π΄2
π β π΄ = π
(b) π₯ = π₯|Ξ¨|2ππ₯
β
ββ
= π΄2 π₯πβ2π π₯ ππ₯ = 0 β
ββ
(πππ πππ‘ππππππ)
π₯2 = π₯2|Ξ¨|2ππ₯β
ββ
= π΄2 π₯2πβ2π π₯ ππ₯ = β
ββ
2π΄2 π₯2πβ2ππ₯ππ₯β
0
You can do the integration using Mathematica if you donβt want to do it by hand. Type the following line in Mathematica then βShift + Enterβ:
Integrate[π₯^2 β Exp[β2 β π β π₯ , π₯, 0, Infinity
You will get 1/4π3
So π₯2 =
2π΄2
4π3 =2π
4π3 =1
2π2
(c) π2 = π₯2 β π₯ 2 =
1
2π2 β π π‘ππππππ πππ£πππ‘πππ π =
1
2π
3 2 1 1 2 3
0.2
0.4
0.6
0.8
1.0
|Ξ¨|2
π₯ π βπ
This figure plots |Ξ¨|2 as a function of x for
Ξ» = 1. The two vertical lines shows the
positions of Ο =1
2and βΟ.
Probability outside the range (βΟ, π):
πππ’π‘ = |Ξ¨|2ππ₯βπ
ββ
+ |Ξ¨|2ππ₯β
π
= 2π΄2 πβ2ππ₯ππ₯β
π
=2π΄2
β2ππβ2ππ₯
βπ
= πβ 2 = 0.2431
Problem 2
(a) π» =π2
2π+
1
2ππ2π₯2
(b) π0 π₯ = π΄ expβπππ₯2
2β
1 = |π0|2ππ₯β
ββ
= π΄2 expβπππ₯2
βππ₯
β
ββ
= π΄2πβ
ππ β π΄ =
ππ
πβ
1/4
(c) π1 π₯ = π΅ + πΆπ₯ expβπππ₯2
2β
Orthogonality condition:
0 = π0 π1 = π0βπ1ππ₯
β
ββ
= π΄(π΅ + πΆπ₯)expβπππ₯2
βππ₯
β
ββ
= π΄π΅ expβπππ₯2
βππ₯
β
ββ
+ π΄πΆ π₯expβπππ₯2
βππ₯
β
ββ
= 0
= π΄π΅πβ
ππ β π΅ = 0
Normalization condition:
1 = π1 π1 = |π1|2ππ₯β
ββ
= πΆ2 π₯2expβπππ₯2
βππ₯
β
ββ
= πΆ2π
2
β
ππ
3/2
β πΆ =ππ
πβ
1/4 2ππ
β
π2 π₯ = π· + πΈπ₯ + πΉπ₯2 expβπππ₯2
2β
Orthogonality conditions: π0 π2 = 0 & π1 π2 = 0
0 = π0 π2 = π0βπ2ππ₯
β
ββ
= π΄(π· + πΈπ₯ + πΉπ₯2)expβπππ₯2
βππ₯
β
ββ
= π΄π· expβπππ₯2
βππ₯
β
ββ
+ π΄πΈ π₯expβπππ₯2
βππ₯
β
ββ
+ π΄πΉ π₯2expβπππ₯2
βππ₯
β
ββ
= 0
= π΄π·πβ
ππ+ π΄πΉ
π
2
β
ππ
3/2
β πΉ = β2π·ππ
β
0 = π1 π2 = π1βπ2ππ₯
β
ββ
= πΆπ₯(π· + πΈπ₯ + πΉπ₯2)expβπππ₯2
βππ₯
β
ββ
= πΆπ· π₯expβπππ₯2
βππ₯
β
ββ
+ πΆπΈ π₯2expβπππ₯2
βππ₯
β
ββ
+ πΆπΉ π₯3expβπππ₯2
βππ₯
β
ββ
= 0 = 0
= πΆπΈπ
2
β
ππ
3/2
β πΈ = 0
Normalization condition:
1 = π2 π2 = |π2|2ππ₯β
ββ
= (π· + πΉπ₯2)2expβπππ₯2
βππ₯
β
ββ
= π·2 expβπππ₯2
βππ₯
β
ββ
+ 2π·πΉ π₯2expβπππ₯2
βππ₯
β
ββ
+ πΉ2 π₯4expβπππ₯2
βππ₯
β
ββ
= π·2πβ
ππ+ 2π·πΉ
π
2
β
ππ
3/2
+ πΉ23 π
4
β
ππ
5/2
π πππππ πΉ = β2π·ππ
β
= 2π·2πβ
ππ βΉ π· =
1
2
ππ
πβ
14 and πΉ = β
2
π1/4
ππ
β
5/4
(d) π1 π₯ = πΆπ₯expβπππ₯2
2β with πΆ =
ππ
πβ
1/4 2ππ
β
π» =π2
2π+
1
2ππ2π₯2 = β
β2
2π
π2
ππ₯2 +1
2ππ2π₯2
π»π1 π₯ = ββ2
2π
π2
ππ₯2 +1
2ππ2π₯2 πΆπ₯exp
βπππ₯2
2β
= ββ2
2π
π2
ππ₯2 πΆπ₯expβπππ₯2
2β+
1
2ππ2π₯2πΆπ₯exp
βπππ₯2
2β
= ββ2
2πβ
3ππ
βπ₯ +
π2π2
β2 π₯3 πΆexpβπππ₯2
2β
+1
2ππ2π₯3πΆexp
βπππ₯2
2β
=3βπ
2πΆπ₯exp
βπππ₯2
2β
=3βπ
2π1 π₯ βΉ πΈ1 =
3βπ
2
Problem 3
π+ =1
2βππ(βππ + πππ₯) πβ =
1
2βππ(+ππ + πππ₯)
πβ, π+ =1
2βππ[ππ + πππ₯, βππ + πππ₯ =
1
2βππ{πππ π, π₯ β πππ[π₯, π }
=1
2βππ{πππ(βπβ) β πππ(πβ)} = 1
βπ π+πβ +1
2= βπ
1
2βππβππ + πππ₯ ππ + πππ₯ +
1
2
=1
2ππ2 + ππππ₯π β πππππ₯ + π2π2π₯2 +
1
2βπ
=1
2ππ2 + πππ[π₯, π + π2π2π₯2 +
1
2βπ
=1
2ππ2 β βππ + π2π2π₯2 +
1
2βπ
=π2
2π+
1
2ππ2π₯2 = π»
π» π+ππ = βπ π+πβ +1
2π+ππ = βπ(π+πβπ+ + 1/2π+) ππ
= βππ+ πβπ+ +1
2ππ = βππ+ π+πβ + 1 +
1
2ππ
= π+ π» + βπ ππ = π+ πΈ + βπ ππ = πΈ + βπ π+ππ
Therefore π+ππ is an eigenstate of H with energy πΈ + βπ . But it may not be
normalized. It is related to the normalized eigenstate ππ+1 up to a coefficient:
π+ππ = πΆππ+1
1 = ππ+1 ππ+1 =1
|πΆ|2π+ππ π+ππ =
1
|πΆ|2ππ πβπ+ππ
=1
|πΆ|2ππ (π+πβ + 1)ππ =
1
|πΆ|2ππ (π»/βπ + 1/2)ππ =
1
πΆ 2 (π + 1)
βΉ πΆ = π + 1 and π+ππ = π + 1 ππ+1 Similarly πβππ = π ππβ1
π»ππ = βπ π+πβ +1
2ππ = βπ π+πβππ +
1
2ππ = βπ π+ π ππβ1 +
1
2ππ
= βπ π πππ +1
2ππ = βπ π +
1
2ππ
Problem 4
π0 π₯ = π΄ expβπππ₯2
2β Ground state: π΄ =
ππ
πβ
1/4
with
π₯ = π0β π₯ π₯π0 π₯ ππ₯
β
ββ
= π΄2 π₯expβπππ₯2
βππ₯
β
ββ
= 0
π₯2 = π0β π₯ π₯2π0 π₯ ππ₯ππ₯
β
ββ
= π΄2 π₯2expβπππ₯2
βππ₯
β
ββ
= π΄2π
2
β
ππ
3/2
=β
2ππ
ππ₯ = π₯2 β π₯ 2 =β
2ππ
π = π0β π₯ βπβ
π
ππ₯π0 π₯ ππ₯
β
ββ
= π΄2 expβπππ₯2
2βπππ π₯exp
βπππ₯2
2βππ₯
β
ββ
= ππππ΄2 π₯expβπππ₯2
βππ₯
β
ββ
= 0
π2 = π0β π₯ ββ2
π2
ππ₯2 π0 π₯ ππ₯β
ββ
= βπ΄2 β2 expβπππ₯2
2β
π2π2
β2 π₯2 βππ
βexp
βπππ₯2
2βππ₯
β
ββ
= βπ΄2 π2π2 π₯2expβπππ₯2
βππ₯
β
ββ
+ π΄2βππ expβπππ₯2
βππ₯
β
ββ
= βπ΄2 π2π2π
2
β
ππ
3/2
+ π΄2βπππβ
ππ=
1
2βππ
ππ = π2 β π 2 =1
2βππ
ππ₯ππ =β
2ππ
1
2βππ =
β
2 Minimum uncertainty
1st excited state:
π1 π₯ = πΆπ₯expβπππ₯2
2β with πΆ =
2
π1/4
ππ
β
3/4
π₯ = π1β π₯ π₯π1 π₯ ππ₯
β
ββ
= πΆ2 π₯3expβπππ₯2
βππ₯
β
ββ
= 0
π₯2 = π1β π₯ π₯2π1 π₯ ππ₯
β
ββ
= πΆ2 π₯4expβπππ₯2
βππ₯
β
ββ
= πΆ23 π
4
β
ππ
5/2
=3β
2ππ
ππ₯ = π₯2 β π₯ 2 =3β
2ππ
π = π1β π₯ βπβ
π
ππ₯π1 π₯ ππ₯
β
ββ
= βπβπΆ2 π₯ 1 βππ
βπ₯2 exp
βπππ₯2
βππ₯
β
ββ
= 0
π2 = π1β π₯ ββ2
π2
ππ₯2 π1 π₯ ππ₯β
ββ
= βπΆ2 β2 π2π2
β2 π₯4 β3ππ
βπ₯2 exp
βπππ₯2
βππ₯
β
ββ
= βπΆ2 π2π2 π₯4expβπππ₯2
βππ₯
β
ββ
+ 3πΆ2βππ π₯2expβπππ₯2
βππ₯
β
ββ
= β3
2βππ + 3βππ =
3
2βππ
ππ = π2 β π 2 =3
2βππ
ππ₯ππ =3β
2ππ
3
2βππ =
3β
2>
β
2
Problem 4: operator approach: MUCH simpler!
π₯ =β
2ππ(π+ + πβ) π = π
βππ
2(π+ β πβ)
π π₯ π =β
2πππ π+ + πβ π = 0
π π₯2 π =β
2πππ π+π+ + π+πβ + πβπ+ + πβπβ π =
β
πππ + 1/2
π π π = πβππ
2π π+ β πβ π = 0
π π2 π = ββππ
2π π+π+ β π+πβ β πβπ+ + πβπβ π = βππ π + 1/2
Ground state: ππ₯ππ =β
2ππ
1
2βππ =
β
2
ππ₯ππ =3β
2ππ
3
2βππ =
3β
2 1st excited state:
Problem 5
(a) Probability to be in the ground state =
| π1(π₯) ππ΄(π₯, π‘ = 0) |2 = π1(π₯)1
2π1 π₯ +
1
2π2 π₯
2
=1
2
(b) ππ΄ π₯, π‘ =
1
2π1 π₯ πβππΈ1π‘/β +
1
2π2 π₯ πβππΈ2π‘/β
For a 1D infinite square well πΈπ =π2π2β2
2ππ2 , πΈ1 =π2β2
2ππ2 , πΈ2 =2π2β2
ππ2 ,
ππ΄ π₯, π‘ =1
2π1 π₯ exp β
ππ2βπ‘
2ππ2 +1
2π2 π₯ exp β
π2π2βπ‘
ππ2
(c) Density distribution at π‘ = 0 is:
|ππ΄ π₯, π‘ = 0 |2 = ππ΄β π₯, π‘ = 0 ππ΄ π₯, π‘ = 0
=1
2π1
β π₯ +1
2π2
β π₯1
2π1 π₯ +
1
2π2 π₯
=1
2|π1|2 + |π2|2 + 2π1π2 since π1 & π2 are real
|ππ΄ π₯, π‘ |2 = ππ΄β π₯, π‘ ππ΄ π₯, π‘
=1
2π1
β π₯ πππΈ1π‘/β +1
2π2
β π₯ πππΈ2π‘/β1
2π1 π₯ πβππΈ1π‘/β +
1
2π2 π₯ πβππΈ2π‘/β
=1
2|π1|2 + |π2|2 + π1
βπ2πβπ(πΈ2βπΈ1)π‘/β+π1π2βππ(πΈ2βπΈ1)π‘/β
=1
2|π1|2 + |π2|2 + 2π1π2cos ((πΈ2βπΈ1)π‘/β)
Therefore |ππ΄ π₯, π‘ |2 = |ππ΄ π₯, π‘ = 0 |2 when cos ((πΈ2βπΈ1)π‘/β) = 1
Or (πΈ2βπΈ1)π‘/β = 2π, 4π, 6π, β¦
π‘ = 2ππβ/(πΈ2βπΈ1) = 2ππβ/2π2β2
ππ2 βπ2β2
2ππ2 =4πππ2
3πβ where π = 1,2,3, β¦
The smallest π‘1 =4ππ2
3πβ
(d)
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
2.5
3.0
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
2.5
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
2.5
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
2.5
3.0
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
2.5
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
2.5
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
2.5
3.0
t=0 t=0.1*t1 t=0.2*t1 t=0.3*t1
t=0.4*t1 t=0.5*t1 t=0.6*t1 t=0.7*t1
t=0.8*t1 t=0.9*t1 t=t1
(e)
ππ΅ π₯, π‘ =1
2π1 π₯ πβππΈ1π‘/β β
1
2π2 π₯ πβππΈ2π‘/β
Density distribution at π‘ = 0 is:
|ππ΅ π₯, π‘ = 0 |2 = ππ΅β π₯, π‘ = 0 ππ΅ π₯, π‘ = 0
=1
2π1
β π₯ β1
2π2
β π₯1
2π1 π₯ β
1
2π2 π₯
=1
2|π1|2 + |π2|2 β 2π1π2 since π1 & π2 are real
|ππ΅ π₯, π‘ |2 = ππ΅β π₯, π‘ ππ΅ π₯, π‘
=1
2π1
β π₯ πππΈ1π‘/β β1
2π2
β π₯ πππΈ2π‘/β1
2π1 π₯ πβππΈ1π‘/β β
1
2π2 π₯ πβππΈ2π‘/β
=1
2|π1|2 + |π2|2 β π1
βπ2πβπ(πΈ2βπΈ1)π‘/ββπ1π2βππ(πΈ2βπΈ1)π‘/β
=1
2|π1|2 + |π2|2 β 2π1π2cos ((πΈ2βπΈ1)π‘/β)
π‘1 ππ π‘βπ π πππ ππ π‘βπ ππππ£πππ’π πππ π
(f)
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
2.5
3.0
ππ΄
0.2 0.4 0.6 0.8 1.0
0.5
1.0
1.5
2.0
2.5
3.0
ππ΅
0 a a 0
0.3a 0.7a
The two initial states can be determined by measuring the position of the particle:
If the measured value of x is around 0.3a then the initial state is ππ΄;
If the measured value of x is around 0.7a then the initial state is ππ΅.