1 / 19

EE 5340 Semiconductor Device Theory Lecture 8 - Fall 2010

EE 5340 Semiconductor Device Theory Lecture 8 - Fall 2010. Professor Ronald L. Carter ronc@uta.edu http://www.uta.edu/ronc. Test 1 – W 29Sep10. 11 AM Room 108 Nedderman Hall Covering Lectures 1 through 10 Open book - 1 legal text or ref., only. You may write notes in your book.

Télécharger la présentation

EE 5340 Semiconductor Device Theory Lecture 8 - Fall 2010

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. EE 5340Semiconductor Device TheoryLecture 8 - Fall 2010 Professor Ronald L. Carter ronc@uta.edu http://www.uta.edu/ronc

  2. Test 1 – W 29Sep10 • 11 AM Room 108 Nedderman Hall • Covering Lectures 1 through 10 • Open book - 1 legal text or ref., only. • You may write notes in your book. • Calculator allowed • A cover sheet will be included with full instructions. For examples see http://www.uta.edu/ronc/5340/tests/.

  3. Star Simulation of IC Resistor

  4. Star Simulation of IC Resistor Corner

  5. The equilibrium carrier concentration ahd the Fermi energy are related as The potential f = (Ef-Efi)/q If not in equilibrium, a quasi-Fermi level (imref) is used Fermi Energy

  6. Electron quasi-Fermi Energy (n = no + n)

  7. Hole quasi-Fermi Energy (p = po + p)

  8. Ex-field when Ef - Efi not constant • Since f = (Ef - Efi)/q = Vt ln(no/ni) • When Ef - Efi = is position dependent, • Ex = -df/dx = -[d(Ef-Efi)/dx] = - Vt d[ln(no/ni)]/dx • If non-equilibrium fn = (Efn-Efi)/q = Vt ln(n/ni), etc • Exn = -[dfn/dx] = -Vt d[ln(n/ni)]/dx

  9. Si and Al and model (approx. to scale) metal n-type s/c p-type s/c Eo Eo Eo qcsi~ 4.05eV qcsi~ 4.05eV qfm,Al ~ 4.1 eV qfs,n qfs,p Ec Ec EFm EFn EFi EFi EFp Ev Ev

  10. Eo Making contact be-tween metal & s/c • Equate the EF in the metal and s/c materials far from the junction • Eo(the free level), must be continuous across the jctn. N.B.: qc = 4.05 eV (Si), and qf = qc + Ec - EF qc(electron affinity) qf (work function) Ec EF EFi qfF Ev

  11. Equilibrium Boundary Conditions w/ contact • No discontinuity in the free level, Eo at the metal/semiconductor interface. • EF,metal = EF,semiconductor to bring the electron populations in the metal and semiconductor to thermal equilibrium. • Eo - EC = qcsemiconductor in all of the s/c. • Eo - EF,metal = qfmetal throughout metal.

  12. No disc in Eo Ex=0 in metal ==> Eoflat fBn=fm- cs = elec mtl to s/c barr fi=fBn-fn= fm-fs elect s/c to mtl barr Ideal metal to n-typebarrier diode (fm>fs,Va=0) metal n-type s/c Eo qcs qfm qfi qfs,n qfBn Ec EFm EFn EFi Depl reg Ev qf’n

  13. Metal to n-typenon-rect cont (fm<fs) n-type s/c No disc in Eo Ex=0 in metal ==> Eo flat fB,n=fm - cs = elec mtl to s/c barr fi= fBn-fn< 0 Accumulation region metal Eo qcs qfm qfs,n qfi qfB,n Ec EFm EFn EFi Ev qfn Acc reg

  14. Ideal metal to p-typebarrier diode (fm<fs) p-type s/c No disc in Eo Ex=0 in metal ==> Eoflat fBn= fm- cs = elec mtl to s/c barr fBp= fm- cs + Eg = hole m to s fi = fBp-fs,p = hole s/c to mtl barr metal Eo qcs qfm qfi qfs,p qfBn Ec EFi EFm EFp qfBp Ev qfi qfp<0 Depl reg

  15. Metal to p-typenon-rect cont (fm>fs) metal n-type s/c No disc in Eo Ex=0 in metal ==> Eo flat fB,n=fm- fs,n = elec mtl to s/c barr fBp= fm- cs + Eg = hole m to s Accumulation region Eo qcs qfm q(fi) qfs,n qfBn Ec EFm EFi EfP qfp Ev qfBp qfi Accum reg

  16. Metal/semiconductorsystem types n-type semiconductor • Schottky diode - blocking for fm > fs • contact - conducting for fm < fs p-type semiconductor • contact - conducting for fm > fs • Schottky diode - blocking for fm < fs

  17. Barrier transistion region, d Interface states above fo acc, p neutrl below fo dnr, n neutrl Ditd-> oo, qfBn=Eg- fo Fermi level “pinned” Ditd-> 0, qfBn=fm - c Goes to “ideal” case Real Schottkyband structure1

  18. Fig 8.41 (a) Image charge and electric field at a metal-dielectric interface (b) Distortion of potential barrier at E=0 and (c) E0

  19. References 1Device Electronics for Integrated Circuits, 2 ed., by Muller and Kamins, Wiley, New York, 1986. See Semiconductor Device Fundamentals, by Pierret, Addison-Wesley, 1996, for another treatment of the m model. 2Physics of Semiconductor Devices, by S. M. Sze, Wiley, New York, 1981. 3Semiconductor Physics & Devices, 2nd ed., by Neamen, Irwin, Chicago, 1997.

More Related