Answer on Question #61254-Physics-Quantum Mechanics
The quantum mechanical wave function for a particle is given by
ψ ( x ) = { A x 3 2 e − a x , x > 0 0 , x < 0 \psi \left(x\right) = \left\{ \begin{array}{c} A x ^ {\frac {3}{2}} e ^ {- a x}, x > 0 \\ 0, x < 0 \end{array} \right. ψ ( x ) = { A x 2 3 e − a x , x > 0 0 , x < 0
Determine (i) the normalization constant A and (ii) the most probable position.
Solution
(i)
1 = ∫ − ∞ ∞ ∣ ψ ( x ) ∣ 2 d x = ∫ 0 ∞ A 2 x 3 e − 2 a x d x = A 2 ∫ 0 ∞ x 3 e − 2 a x d x = ∣ y = 2 a x ∣ = A 2 ( 2 a ) 4 ∫ 0 ∞ y 3 e − y d y = A 2 ( 2 a ) 4 Γ ( 4 ) = A 2 ( 2 a ) 4 3 ! = 3 A 2 8 ( a ) 4 A = 2 2 3 a 2 \begin{array}{l} 1 = \int_{-\infty}^{\infty} |\psi(x)|^2 dx = \int_{0}^{\infty} A^2 x^3 \, e^{-2ax} dx = A^2 \int_{0}^{\infty} x^3 \, e^{-2ax} dx = |y = 2ax| = \frac{A^2}{(2a)^4} \int_{0}^{\infty} y^3 \, e^{-y} dy \\ = \frac{A^2}{(2a)^4} \Gamma(4) = \frac{A^2}{(2a)^4} 3! = \frac{3A^2}{8(a)^4} \\ A = 2 \sqrt{\frac{2}{3}} a^2 \\ \end{array} 1 = ∫ − ∞ ∞ ∣ ψ ( x ) ∣ 2 d x = ∫ 0 ∞ A 2 x 3 e − 2 a x d x = A 2 ∫ 0 ∞ x 3 e − 2 a x d x = ∣ y = 2 a x ∣ = ( 2 a ) 4 A 2 ∫ 0 ∞ y 3 e − y d y = ( 2 a ) 4 A 2 Γ ( 4 ) = ( 2 a ) 4 A 2 3 ! = 8 ( a ) 4 3 A 2 A = 2 3 2 a 2
(ii)
⟨ x ⟩ = ∫ − ∞ ∞ ψ ∗ ( x ) x ψ ( x ) d x = ∫ 0 ∞ A 2 x 4 e − 2 a x d x = ∫ 0 ∞ 8 a 4 3 x 4 e − 2 a x d x = ∣ y = 2 a x ∣ = 1 12 a ∫ 0 ∞ y 4 e − y d y = 1 12 a Γ ( 5 ) = 1 12 a 4 ! = 2 a . \begin{array}{l} \langle x \rangle = \int_{-\infty}^{\infty} \psi^{*}(x) x \psi(x) dx = \int_{0}^{\infty} A^2 x^4 \, e^{-2ax} dx = \int_{0}^{\infty} \frac{8a^4}{3} x^4 \, e^{-2ax} dx = |y = 2ax| = \frac{1}{12a} \int_{0}^{\infty} y^4 \, e^{-y} dy \\ = \frac{1}{12a} \Gamma(5) = \frac{1}{12a} 4! = \frac{2}{a}. \\ \end{array} ⟨ x ⟩ = ∫ − ∞ ∞ ψ ∗ ( x ) x ψ ( x ) d x = ∫ 0 ∞ A 2 x 4 e − 2 a x d x = ∫ 0 ∞ 3 8 a 4 x 4 e − 2 a x d x = ∣ y = 2 a x ∣ = 12 a 1 ∫ 0 ∞ y 4 e − y d y = 12 a 1 Γ ( 5 ) = 12 a 1 4 ! = a 2 .
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