EmilyRuck
- 134
- 6
Hello!
The (potential) energy of an electron in a solid structure is always negative; also the E_c and E_v levels (conduction band and valence band limits) are negative, in the band diagram of a pn junction.
When the junction is built and thermal equilibrium is reached, the depletion region creates an electric field and a potential barrier \phi_i.
But I have some doubts about this.
1) First of all,
\phi_i = \displaystyle \frac{kT}{q} \log \left( \displaystyle \frac{N_D N_A}{n_i^2} \right)
where k is Boltzmann's constant, T is the absolute temperature and q is the absolute value of the electron charge. The energy step due to this built-in potential is q \phi_i, but why a positive q is used to calculate this step? Given a voltage difference \Delta V = \phi_i, the corresponding potential energy difference should be \Delta U = q \Delta V = - |q| \Delta V in the case of an electron.
2) Let's suppose anyway that q \phi_i > 0.
In the conduction band of the n-region, just the charge carriers with an energy E = E_c + q \phi_i can cross the junction and diffuse to the p-region. So, I would say that the p-region, with respect to the n-region, is at a higher potential.
In order to have a reference image, let's consider this document, page 11. Why in the last plot, which shows V as function of position, the n-side is at a higher potential and the p-side at V = 0? (Consider V_A = 0, that is the case of thermal equilibrium)
3) What about the vacuum level? It is never depicted in the band diagram of a pn junction; but how is it affected by the built-in voltage?
Thank you anyway for having read.
Emily
The (potential) energy of an electron in a solid structure is always negative; also the E_c and E_v levels (conduction band and valence band limits) are negative, in the band diagram of a pn junction.
When the junction is built and thermal equilibrium is reached, the depletion region creates an electric field and a potential barrier \phi_i.
But I have some doubts about this.
1) First of all,
\phi_i = \displaystyle \frac{kT}{q} \log \left( \displaystyle \frac{N_D N_A}{n_i^2} \right)
where k is Boltzmann's constant, T is the absolute temperature and q is the absolute value of the electron charge. The energy step due to this built-in potential is q \phi_i, but why a positive q is used to calculate this step? Given a voltage difference \Delta V = \phi_i, the corresponding potential energy difference should be \Delta U = q \Delta V = - |q| \Delta V in the case of an electron.
2) Let's suppose anyway that q \phi_i > 0.
In the conduction band of the n-region, just the charge carriers with an energy E = E_c + q \phi_i can cross the junction and diffuse to the p-region. So, I would say that the p-region, with respect to the n-region, is at a higher potential.
In order to have a reference image, let's consider this document, page 11. Why in the last plot, which shows V as function of position, the n-side is at a higher potential and the p-side at V = 0? (Consider V_A = 0, that is the case of thermal equilibrium)
3) What about the vacuum level? It is never depicted in the band diagram of a pn junction; but how is it affected by the built-in voltage?
Thank you anyway for having read.
Emily