{[ promptMessage ]}

Bookmark it

{[ promptMessage ]}

hw_solutions_6 - Homework Solutions 6(Libo Ch 7 7.37 Use...

Info iconThis preview shows pages 1–2. Sign up to view the full content.

View Full Document Right Arrow Icon
Homework Solutions # 6 (Liboff Ch. 7) 7.37 Use the 1D form, ∂ρ/∂t + ∂J/∂x = 0, and go through the derivation in equations 7.102 to 7.105. You will get ∂ψ * ψ ∂t - i ¯ h 2 m ψ * 2 ψ ∂x 2 - ψ 2 ψ * ∂x 2 ! + i ¯ h ψ * ψ ( V - V * ) = 0 Since V 6 = V * , the last term does not vanish, and the continuity equation doesn’t work. The deeper reason it does not now work is not really given in Liboff, so it can be hard to figure out. It is that the density ρ and current density J must depend on ψ and ψ * only , and not on other functions such as V . More formally, J must be a functional, J [ ψ, ψ * ] only, and if the potential term does not vanish, it ends up depending on V . 7.40 The incoming wave is ψ inc = Ae ik 1 x , where the charge density is | A | 2 = 10 15 e/m, and ¯ h 2 k 2 1 / 2 m e = 100 eV. Use the electron mass m e = 0 . 511 MeV/ c 2 , and the current becomes J inc = ¯ hk 1 m e | A | 2 = 5 . 94 × 10 21 e/s = 950 A Use table 7.2 for the transmission coefficient, with V/E = 1 / 2, T = 4 q 1 - V/E [1 + q 1 - V/E ] 2 = 0 . 97 So J trans = 0 . 97 J inc = 5 . 77 × 10 21 e/s = 923 A J refl = 0 . 03 J inc = 1 . 78 × 10 20 e/s = 27 A Sending a beam of electrons through a slit into a large capacitor would work.
Background image of page 1

Info iconThis preview has intentionally blurred sections. Sign up to view the full version.

View Full Document Right Arrow Icon
Background image of page 2
This is the end of the preview. Sign up to access the rest of the document.

{[ snackBarMessage ]}