Working Principle of a Semiconductor Based Solar Cell Transport of Charge Carriers Week 2.3.3 Arno Smets
Diffusion Drift E-Field
Random movement = no net movement
J e = qD e dn/dx Diffusion density
Diffusion J e = qD e dn/dx density
Diffusion J e = qD e dn/dx density
Diffusion dn/dx=0 J=0 density
Drift Electron E-Field Hole
Drift Density Current density Charge Mobility Electric field J h = pq h E J e = nq e E
Drift Electron E-Field Hole
Diffusion Drift E-Field
Charge Carrier Recombination Recombination
Charge Carrier Recombination Radiative recombination
Charge Carrier Recombination Auger recombination
Charge Carrier Recombination Shockley-Read-Hall (SRH) recombination
Diffusion Length L h L e L = D t
Diffusion Length L h L e L = D t
Diffusion Length L h L e L = D t
Diffusion Length Transport by diffusion limited by minority carriers - - - - - - - - - - - - p-doped Diffusion length: L e = D e t e < L h
Diffusion Length Transport by diffusion limited by minority carriers - - - - + + + + - - - - + + + + - - - - + + + + p-doped n-doped Diffusion length: L e = D e t e < L h L D L h h h e
Diffusion Drift E-Field
Thank you for your attention!
Thank you for your attention!
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