P-N Junction Diodes How do they work? (postponing the math) Chap. 5.2
p-n Junction Diode p-n Junction p-Type Materialn-Type Material
p-n Junction Diode p-n Junction p-Type Material n-Type Material A p-n junction diode is made by forming a p-type region of material directly next to a n-type region. p-n Junction
p-Type Materialn-Type Material x N D - N A NDND NANA p-n Junction p-n Junction p-n Junction Diode
In regions far away from the “junction” the band diagram p-n Junction Diode p-Type Material n-Type Material ECEC EVEV EFEF EiEi ECEC EVEV EFEF EiEi
But when the device has no external applied forces, no current can flow. Thus, the Fermi-level must be flat! We can then fill in the junction region of the band diagram as: p-n Junction Diode p-Type Material n-Type Material ECEC EVEV EFEF EiEi ECEC EVEV EFEF EiEi
But when the device has no external applied forces, no current can flow. Thus, the Fermi-level must be flat! We can then fill in the junction region of the band diagram as: p-Type Material n-Type Material p-n Junction Diode ECEC EVEV EFEF EiEi ECEC EVEV EFEF EiEi
Built-in-potential p-n Junction Diode ECEC EVEV EFEF EiEi ECEC EVEV EFEF EiEi - q V BI p-Type Material n-Type Material x Electrostatic Potential Built-in-potential
Built-in-potential p-n Junction Diode x Electrostatic Potential Built-in-potential x Electric Field Electric Field
Charge Density (NOT Resistivity) Poisson’s Equation p-n Junction Diode in 1-dimension Electric Field Permittivity of free space Relative Permittivity of Semiconductor ( r )
x Electric Field Built-in-potential p-n Junction Diode Charge Density x qN D qN A Charge Density
p-n Junction Diode Energy Potential Electrical Field Charge Density
n no x x = 0 p no p po n po log(n), log(p) -eN a eN d M x E ( x ) B - h + p n M As + e – WpWp WnWn V o V(x) x PE(x) x –W p W n 0 eV o x –eV o Hole Potential Energy PE (x) o – E o E0E0 net M n i p-n Junction Principles Electron Potential Energy PE (x) Space charge region M -W p -W n Neutral n-regionNeutral p-region Metallurgical Junction