Presentation is loading. Please wait.

Presentation is loading. Please wait.

EE 5340 Semiconductor Device Theory Lecture 7 - Fall 2009

Similar presentations


Presentation on theme: "EE 5340 Semiconductor Device Theory Lecture 7 - Fall 2009"— Presentation transcript:

1 EE 5340 Semiconductor Device Theory Lecture 7 - Fall 2009
Professor Ronald L. Carter

2 Second Assignment Please print and bring to class a signed copy of the document appearing at L 07 Sept 15

3 Diffused or Implanted IC Resistor (Fig 2.451)
L 07 Sept 15

4 An IC Resistor with L = 8W (M&K)1
L 07 Sept 15

5 Typical IC doping profile (M&K Fig. 2.441)
L 07 Sept 15

6 Mobilities** L 07 Sept 15

7 IC Resistor Conductance
L 07 Sept 15

8 An IC Resistor with Ns = 8, R = 8Rs (M&K)1
L 07 Sept 15

9 The effect of lateral diffusion (M&K1)
L 07 Sept 15

10 A serpentine pattern IC Resistor (M&K1)
R = NSRS NCRS note: RC = 0.65RS L 07 Sept 15

11 Fermi Energy 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 L 07 Sept 16

12 Electron quasi-Fermi Energy (n = no + n)
L 07 Sept 16

13 Hole quasi-Fermi Energy (p = po + p)
L 07 Sept 16

14 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 L 07 Sept 16

15 Si and Al and model (approx. to scale)
metal n-type s/c p-type s/c Eo Eo Eo qcsi~ 4.05 eV qcsi~ 4.05 eV qfm,Al ~ 4.1 eV qfs,n qfs,p Ec Ec EFm EFn EFi EFi EFp Ev Ev L 07 Sept 16

16 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 Eo qc (electron affinity) qf (work function) Ec EF EFi qfF Ev L 07 Sept 15

17 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. L 07 Sept 16

18 Ideal metal to n-type barrier diode (fm>fs,Va=0)
n-type s/c 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 Eo qfm qcs qfi qfBn qfs,n Ec EFm EFn EFi Depl reg Ev qf’n L 07 Sept 16

19 References 1Device Electronics for Integrated Circuits, 2 ed., by Muller and Kamins, Wiley, New York, 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. L 07 Sept 15


Download ppt "EE 5340 Semiconductor Device Theory Lecture 7 - Fall 2009"

Similar presentations


Ads by Google