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Working Principle of a Semiconductor Based Solar Cell Transport of - PowerPoint PPT Presentation

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


  1. Working Principle of a Semiconductor Based Solar Cell Transport of Charge Carriers Week 2.3.3 Arno Smets

  2. Diffusion Drift E-Field

  3. Random movement = no net movement

  4. J e = qD e dn/dx Diffusion density

  5. Diffusion J e = qD e dn/dx density

  6. Diffusion J e = qD e dn/dx density

  7. Diffusion dn/dx=0 J=0 density

  8. Drift Electron E-Field Hole

  9. Drift Density Current density Charge Mobility Electric field J h = pq h E J e = nq e E

  10. Drift Electron E-Field Hole

  11. Diffusion Drift E-Field

  12. Charge Carrier Recombination Recombination

  13. Charge Carrier Recombination Radiative recombination

  14. Charge Carrier Recombination Auger recombination

  15. Charge Carrier Recombination Shockley-Read-Hall (SRH) recombination

  16. Diffusion Length L h L e L = D t

  17. Diffusion Length L h L e L = D t

  18. Diffusion Length L h L e L = D t

  19. Diffusion Length Transport by diffusion limited by minority carriers - - - - - - - - - - - - p-doped Diffusion length: L e = D e t e < L h

  20. 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

  21. Diffusion Drift E-Field

  22. Thank you for your attention!

  23. Thank you for your attention!

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