String Waves and Matter Waves — Question 8

Section 39-1 · Physics pages 6426–6427

Question 8 Quadratic mode frequencies produce an exact full revival A particle in a hard-wall interval has eigenstates un with energies En = n2E1. An arbitrary finite superposition is Ψ(x, t) = ∑ n cnun(x)e−in2E1t/ℏ. n = 1 n = 2 n = 3 E En = n2E1 Schematic; labels, not drawing lengths, specify the data. (a) Find a positive time at which every component has its initial phase. (b) Compare that time with the classical round-trip period of a particle having momentum pn = nπℏ/L, using E1 = π2ℏ2/(2mL2).
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Question 8 - Solution Quadratic mode frequencies produce an exact full revival n = 1 n = 2 n = 3 E En = n2E1 (a) Method and calculation n2E1Trev/ℏ= 2πn2 ⇒Trev = 2πℏ/E1 . Ψ(x, Trev) = Ψ(x, 0) , Trev = 4mL2/(πℏ). (b) Interpretation and further calculation Tcl,n = 2L/(pn/m) = 2mL2/(nπℏ). Trev/Tcl,n = 2n . Physical check This is a common revival time for any finite superposition. A special choice of occupied modes can revive earlier, so it need not be the shortest recurrence for every state.

Question 8

Quadratic mode frequencies produce an exact full revival

A particle in a hard-wall interval has eigenstates unu_n with energies En=n2E1E_n=n^2E_1. An arbitrary finite superposition is Ψ(x,t)=∑ncnun(x)e−in2E1t/ℏ\Psi(x,t)=\sum_n c_nu_n(x)e^{-in^2E_1t/\hbar}.

Diagram shown in the original SVG worksheet.

  1. Find a positive time at which every component has its initial phase.

  2. Compare that time with the classical round-trip period of a particle having momentum pn=nπℏ/Lp_n=n\pi\hbar/L, using E1=π2ℏ2/(2mL2)E_1=\pi^2\hbar^2/(2mL^2).

Question 8 - Solution

Quadratic mode frequencies produce an exact full revival

Diagram shown in the original SVG worksheet.

(a) Method and calculation

n2E1Trev/ℏ=2πn2⇒Trev=2πℏ/E1.n^2E_1T_{\mathrm{rev}}/\hbar=2\pi n^2\Rightarrow\boxed{T_{\mathrm{rev}}=2\pi\hbar/E_1}.Ψ(x,Trev)=Ψ(x,0),Trev=4mL2/(πℏ).\boxed{\Psi(x,T_{\mathrm{rev}})=\Psi(x,0)},\qquad T_{\mathrm{rev}}=4mL^2/(\pi\hbar).

(b) Interpretation and further calculation

Tcl,n=2L/(pn/m)=2mL2/(nπℏ).T_{{\mathrm{cl}},n}=2L/(p_n/m)=2mL^2/(n\pi\hbar).Trev/Tcl,n=2n.\boxed{T_{\mathrm{rev}}/T_{{\mathrm{cl}},n}=2n}.

Physical check

This is a common revival time for any finite superposition. A special choice of occupied modes can revive earlier, so it need not be the shortest recurrence for every state.