Chapter 5 wrote a state of the infinite well as with

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Quantum Mechanics · Wave mechanics in one dimension

Quantum Mechanics: From the Photon to the Hydrogen Atom, Ch Free particles, wave packets and tunnelling

Problem

Chapter 5 wrote a state of the infinite well as Ψ(x,0)=∑ncnψn(x)\Psi(x,0) = \sum_n c_n\psi_n(x) with cn=∫0aψn(x)Ψ(x,0) dxc_n = \int_0^a\psi_n(x)\Psi(x,0)\,dx. This chapter writes a free particle as Ψ(x,0)=(2π)−1/2∫ϕ(k)eikxdk\Psi(x,0) = (2\pi)^{-1/2}\int\phi(k)e^{ikx}dk with ϕ(k)=(2π)−1/2∫Ψ(x,0)e−ikxdx\phi(k) = (2\pi)^{-1/2}\int\Psi(x,0)e^{-ikx}dx. ((a)) Match each piece of the well's expansion to its counterpart in the packet's: what plays the role of ψn\psi_n? Of cnc_n? Of the sum over nn? ((b)) A packet is prepared with Ψ(x,0)=(2πs2)−1/4e−x2/4s2eik0x\Psi(x,0) = (2\pi s^2)^{-1/4}e^{-x^2/4s^2}e^{ik_0x}, s=0.20s = 0.20 nm and k0=15k_0 = 15 nm−1^{-1}. Using the Gaussian result from this chapter, evaluate ϕ(k)\phi(k) at k=k0k = k_0 and at k=k0+1/2sk = k_0 + 1/2s, and say what feature of ϕ\phi these two values mark out.

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