The p-n Junction — Question 9

Section 41-7 · Physics pages 6928–6929

Question 9 Band bending and electrostatic potential have opposite signs At equilibrium an abrupt homojunction has p material on the left and n material on the right. The electrostatic potential rises by Vbi = .700 V from p to n, and the electron band edge satisfies Ec = −eϕ + constant. The gap is spatially constant. Ec Ev EF p n Schematic; labels, not drawing lengths, specify the data. (a) Find the conduction- and valence-band energy changes from p to n in eV. (b) An electron moves from n to p without collisions. Find its electrostatic potential-energy increase and the minimum initial kinetic energy needed to surmount that barrier.
Show solutionHide solution
Question 9 - Solution Band bending and electrostatic potential have opposite signs Ec Ev EF p n (a) Method and calculation ∆Ec = Ec,n −Ec,p = −e(ϕn −ϕp) = −eVbi. ∆Ec = ∆Ev = −.700 eV . (b) Interpretation and further calculation ∆Un→p = −e(ϕp −ϕn) = +eVbi. Kmin = eVbi = .700 eV in the stated classical barrier picture. Physical check The flat equilibrium Fermi level coexists with bent band edges. A positive charge would experience the opposite electrostatic potential-energy change.

Question 9

Band bending and electrostatic potential have opposite signs

At equilibrium an abrupt homojunction has p material on the left and n material on the right. The electrostatic potential rises by Vbi=.700VV_{bi}=.700\,\mathrm V from p to n, and the electron band edge satisfies Ec=−eϕ+constantE_c=-e\phi+\text{constant}. The gap is spatially constant.

Diagram shown in the original SVG worksheet.

  1. Find the conduction- and valence-band energy changes from p to n in eV.

  2. An electron moves from n to p without collisions. Find its electrostatic potential-energy increase and the minimum initial kinetic energy needed to surmount that barrier.

Question 9 - Solution

Band bending and electrostatic potential have opposite signs

Diagram shown in the original SVG worksheet.

(a) Method and calculation

ΔEc=Ec,n−Ec,p=−e(ϕn−ϕp)=−eVbi.\Delta E_c=E_{c,n}-E_{c,p}=-e(\phi_n-\phi_p)=-eV_{bi}.ΔEc=ΔEv=−.700eV.\boxed{\Delta E_c=\Delta E_v=-.700\,\mathrm{eV}}.

(b) Interpretation and further calculation

ΔUn→p=−e(ϕp−ϕn)=+eVbi.\Delta U_{n\to p}=-e(\phi_p-\phi_n)=+eV_{bi}.Kmin=eVbi=.700eVin the stated classical barrier picture.\boxed{K_{\min}=eV_{bi}=.700\,\mathrm{eV}}\quad\text{in the stated classical barrier picture}.

Physical check

The flat equilibrium Fermi level coexists with bent band edges. A positive charge would experience the opposite electrostatic potential-energy change.