For the Gaussian wave packet (6.62). (pl(0)) is given by (6.68) and thus (x, t) is given by ¥ (x, t) = (x|\/(t)) = [dpe=ip²1/2mh (x\p)(p(0)) (6.75) If you are proficient at carrying out Gaussian integrals (see Appendix D), it is straightforward to show that 1 √(x,t) = e-x²/12a211+(iht/ma²)]} √√la+(iht/ma)] (6.76) Comparing *(x, t) (x, t) with its form (6.63) at r = 0, we see that the position uncertainty is given by 12,2 1/2 √(1+1)" Ax= 2 m2a4 (6.77) 6.4. (a) Show for a free particle of mass m initially in the state 1 v(x)=(x|y) √(x) = (xy) = -x²/2a² πα that 1 (x,t) = (x(t)) = e-x²/{2a² 11+ (iht/ma²] √√√[a+(iht/ma)] and therefore ht Ax 1+ √2 ma2 Page 254 (metric system) Problems 239 Suggestion: Start with (6.75) and take advantage of the Gaussian integral (D.7), but in momentum space instead of position space. (b) What is Ap, at time t? Suggestion: Use the momentum-space wave function to evaluate Ap

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do parts a and b, i gave 6.75

For the Gaussian wave packet (6.62). (pl(0)) is given by (6.68) and thus (x, t)
is given by
¥ (x, t) = (x|\/(t)) = [dpe=ip²1/2mh (x\p)(p(0))
(6.75)
If you are proficient at carrying out Gaussian integrals (see Appendix D), it is
straightforward to show that
1
√(x,t) =
e-x²/12a211+(iht/ma²)]}
√√la+(iht/ma)]
(6.76)
Comparing *(x, t) (x, t) with its form (6.63) at r = 0, we see that the position
uncertainty is given by
12,2 1/2
√(1+1)"
Ax=
2
m2a4
(6.77)
Transcribed Image Text:For the Gaussian wave packet (6.62). (pl(0)) is given by (6.68) and thus (x, t) is given by ¥ (x, t) = (x|\/(t)) = [dpe=ip²1/2mh (x\p)(p(0)) (6.75) If you are proficient at carrying out Gaussian integrals (see Appendix D), it is straightforward to show that 1 √(x,t) = e-x²/12a211+(iht/ma²)]} √√la+(iht/ma)] (6.76) Comparing *(x, t) (x, t) with its form (6.63) at r = 0, we see that the position uncertainty is given by 12,2 1/2 √(1+1)" Ax= 2 m2a4 (6.77)
6.4.
(a) Show for a free particle of mass m initially in the state
1
v(x)=(x|y)
√(x) = (xy) =
-x²/2a²
πα
that
1
(x,t) = (x(t)) =
e-x²/{2a² 11+ (iht/ma²]
√√√[a+(iht/ma)]
and therefore
ht
Ax
1+
√2
ma2
Page 254 (metric system)
Problems 239
Suggestion: Start with (6.75) and take advantage of the Gaussian integral
(D.7), but in momentum space instead of position space.
(b) What is Ap, at time t? Suggestion: Use the momentum-space wave function
to evaluate Ap
Transcribed Image Text:6.4. (a) Show for a free particle of mass m initially in the state 1 v(x)=(x|y) √(x) = (xy) = -x²/2a² πα that 1 (x,t) = (x(t)) = e-x²/{2a² 11+ (iht/ma²] √√√[a+(iht/ma)] and therefore ht Ax 1+ √2 ma2 Page 254 (metric system) Problems 239 Suggestion: Start with (6.75) and take advantage of the Gaussian integral (D.7), but in momentum space instead of position space. (b) What is Ap, at time t? Suggestion: Use the momentum-space wave function to evaluate Ap
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