String Waves and Matter Waves — Question 4

Section 39-1 · Physics pages 6418–6419

Question 4 The apparent zero-index solution of a hard-wall well is the zero function Inside 0 < x < L, a free stationary particle obeys −ℏ2ψ′′/(2m) = Eψ with ψ(0) = ψ(L) = 0. A proposed state has E = 0. x 0 L lowest nonzero mode Schematic; labels, not drawing lengths, specify the data. (a) Solve the differential equation at exactly zero energy. (b) Apply both boundaries and decide whether the result can represent a normalized state.
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Question 4 - Solution The apparent zero-index solution of a hard-wall well is the zero function x 0 L lowest nonzero mode (a) Method and calculation E = 0 ⇒ψ′′ = 0 ⇒ψ(x) = Ax + B. ψ(0) = 0 ⇒B = 0, ψ(L) = 0 ⇒AL = 0. (b) Interpretation and further calculation L > 0 ⇒A = B = 0, ψ ≡0 . ∫L 0 |ψ|2dx = 0̸ = 1 ⇒no normalized zero-energy state . Physical check The zero function solves the homogeneous equation but is not a physical state. This is why the hard-wall quantum number starts at one.

Question 4

The apparent zero-index solution of a hard-wall well is the zero function

Inside 0<x<L0<x<L, a free stationary particle obeys −ℏ2ψ′′/(2m)=Eψ-\hbar^2\psi\prime\prime/(2m)=E\psi with ψ(0)=ψ(L)=0\psi(0)=\psi(L)=0. A proposed state has E=0E=0.

Diagram shown in the original SVG worksheet.

  1. Solve the differential equation at exactly zero energy.

  2. Apply both boundaries and decide whether the result can represent a normalized state.

Question 4 - Solution

The apparent zero-index solution of a hard-wall well is the zero function

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E=0⇒ψ′′=0⇒ψ(x)=Ax+B.E=0\Rightarrow\psi\prime\prime=0\Rightarrow\psi(x)=Ax+B.ψ(0)=0⇒B=0,ψ(L)=0⇒AL=0.\psi(0)=0\Rightarrow B=0,\qquad\psi(L)=0\Rightarrow AL=0.

(b) Interpretation and further calculation

L>0⇒A=B=0,ψ≡0.L>0\Rightarrow\boxed{A=B=0,\quad\psi\equiv0}.∫0L|ψ|2dx=0≠1⇒no normalized zero-energy state.\int_0^L|\psi|^2dx=0\ne1\Rightarrow\boxed{\text{no normalized zero-energy state}}.

Physical check

The zero function solves the homogeneous equation but is not a physical state. This is why the hard-wall quantum number starts at one.