Question 1.4: At time t = 0 a particle is represented by the wave function...

At time t = 0 a particle is represented by the wave function

Ψ (x,0) =\begin{cases} A(x,0) , & 0\leq x\leq a, \\ A(b-x)/(b-a) ,& a \leq x\leq b, \\ 0,& otherwise,\end{cases} .

where A, a, and b are (positive) constants.

(a) Normalize Ψ(that is, find A, in terms of a and b).

(b) Sketch Ψ(x,0) , as a function of x.

(c) Where is the particle most likely to be found, at t = 0?.

(d) What is the probability of finding the particle to the left of a? Check your result in the limiting cases b = a and b= 2a.

(e) What is the expectation value of x?.

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(a)

1 = \frac{\left|A\right|^2 }{a^2} \int_{0}^{a}{x^2}dx + \frac{\left|A\right|^2 }{(b-a)^2} \int_{0}^{b} {(b-a)^2}dx = \left|A\right|^2 \left\{\frac{1}{a^2}\Bigl(\frac{x^3}{3}\Bigr)\mid ^a_0 + \frac{1}{(b-a)^2 } \biggl(-\frac{(b-x)^3}{3}\biggr)\mid ^b_a \right\}

= \left|A\right|^2 \biggl[\frac{a}{3} + \frac{b-a}{3}\biggr] = \left|A\right|^2 \frac{b}{3}    ⇒ A = \sqrt{\frac{3}{b} }.

(b)

(c) At x = a.

(d)

P = \int_{0}^{a}{\left|Ψ\right|^2}dx = \frac{\left|A\right|^2 }{a^2} \int_{0}^{a}{x^2}dx  = \left|A\right|^2 \frac{a}{3} = \frac{a}{b} \begin{cases} P=1 & if b=a \\P=1/2 & if b=2a \end{cases} .

(e)

\left\langle x\right\rangle = \int{x \left|\Psi \right|^2 } dx = \left|A\right| ^2 \left\{\frac{1}{a^2}\int_{0}^{a}{x^3}dx + \frac{1}{(b-a)^2} \int_{a}^{b}{x(b-x)^2} dx \right\} .

= \frac{3}{b} \left\{\frac{1}{a^2}\Bigl(\frac{x^4}{4}\Bigr) \mid ^a_0 + \frac{1}{(b-a)^2}\biggl(b^2\frac{x^2}{2} -2 b \frac{x^3}{3} + \frac{x^4}{4} \biggr) \mid ^b_a\right\} .

= \frac{3}{4b(b – a)^2} [a^2(b – a)^2 + 2b^4 – 8b^4/3 + b^4 – 2a^2b^2 + 8a^3b/3 – a^4] .

= \frac{3}{4b(b – a)^2}  \biggl(\frac{b^4}{3} – a^2 b^2 + \frac{2}{3}a^3b \biggr) = \frac{1}{4(b – a)^2}(b^3 – 3a^2b + 2a^3) = \frac{2a + b}{4}      .

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