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MIT 3 23 - THE LAW OF MASS ACTION

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MIT OpenCourseWare http://ocw.mit.edu 3.23 Electrical, Optical, and Magnetic Properties of MaterialsFall 2007For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms.3.23 Fall 2007 – Lecture 13 THE LAW OF MASS ACTION 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) Last time 1. Band structure of oxides (perovskites), semiconductors (silicon and compared with lead) late (fcc) transition metals (silicon, and compared with lead), late (fcc) transition metals (same period, or same group), graphene and nanotubes 2. Independent electron gas: states, energy, density, DOS 3. DOS of massive and massless bands in 1, 2 and 3 dimensions 4. Statistics of classical and quantum particles, Fermi-Dirac distribution, chemical potential 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) 1•Study • Chap 6 SingletonChap 6 Singleton, or, much better, • Chap 28 (Homogeneous semiconductors) Ashcroft-Mermin (to be posted) 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) Sb-doped Germanium 3.23 Electronic, Optical and Mag -2 Courtesy of Elsevier, Inc., http://www.sciencedirect.com. Used with permission.Semiconductors 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) Valence+conduction bands in Si3 Image removed due to copyright restrictions.Please see: Fig. 6.1 in Singleton, John. Band Theory and Electronic Properties of Solids. Oxford, England: Oxford University Press, 2001.Image removed due to copyright restrictions. Please see any graph of semiconductor band gaps vs. lattice constants, such as http://www.tf.uni-kiel.de/matwis/amat/semi_en/kap_5/illustr/bandgap_misfit.gifBand structure of Si, Ge, GaAs 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) Conduction band minima (in 3d) 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) 4 Image removed due to copyright restrictions. Please see any image of Si, Ge, and GaAs energy bands, such as http://ecee.colorado.edu/~bart/book/book/chapter2/gif/fig2_3_6.gif.Image removed due to copyright restrictions. Please see Fig. 19.9 in Marder, Michael P. Condensed Matter Physics. New York, NY: Wiley-Interscience, 2000.Optical absorption in Ge 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) Impress your examiners (orals) 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) 5 Image removed due to copyright restrictions. Please see: Fig. 6.3 and 6.4 in Singleton, John. Band Theory and Electronic Properties of Solids. Oxford, England: Oxford University Press, 2001.Text removed due to copyright restrictions. Please see Table 19.1 in Marder, Michael P. Condensed Matter Physics. New York, NY: Wiley-Interscience, 2000.Number of carriers at thermal equilibrum 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) Conduction and valence DOS (non-degenerate sc, isotropic effective mass) 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) 6 Image removed due to copyright restrictions.Please see: Fig. 18 in Kittel, Charles. "Introduction to Solid State Physics." Chapter 8 in Semiconductor Crystals. New York, NY: John Wiley & Sons, 2004.Image removed due to copyright restrictions. Please see Fig. 2.16 in Pierret, Robert F. Semiconductor Device Fundamentals. Reading, MA: Addison-Wesley, 1996.Density of available states 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) Miracle ! Law of Mass Action ()= 2.5 ⎛⎛ mmc⎞⎞3/2 ⎛⎛ TT ⎞⎞ 3/2 10 19 / cm3 NTc ⎜⎝ m⎟⎠ ⎜⎝ 300 K⎟⎠ PT=2.5 10 / cmv() ⎜⎝⎛ mmv⎟⎠⎞3/2 ⎜⎝⎛ 300 TK⎟⎠⎞3/2 19 3 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) 7Intrinsic case pT ≡ nT )nTnTc(( ))= pT v (( ))≡ n((T) i 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) Intrinsic case 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) 8Extrinsic case nTnTc ( )− pT () ∆npT n() v ( )=∆ 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) Extrinsic case 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) 9n-type x x Al Asx x x x x Au x p-type deep level -+ -x Si x x Si Impurity levels • Adding impurities can lead to controlled domination of one carrier type – n-type is dominated by electrons – p-type is dominated by holes •• Adding other impurities can degrade electrical properties Adding other impurities can degrade electrical properties Impurities with close Impurities that create deep levels electronic structure to host EA Ev Ec Ev ED Ec Ev EDEEP 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) Ec Impurity states as “embedded” hydrogen atoms • Consider the weakly bound 5th electron in Phosphorus as a modified hydrogen atom • For hydrogenic donors or acceptors, we can think of the electron or hole, respectively, as an orbbiting ellectron aroundd a net ffixedd chharge • We can estimate the energy to free the carrier into the conduction band or valence band by using a modified expression for the energy of an electron in the H atom me4 13.6 En = 222 = − 28ε h n n (eV) o 2 =eme4 e 2 m * e4 1 13.6 m *1⎯ →En = 2 2 2 ⎯εr ⎯2 2 2 2 = − 2 28εh n 8εh n ε n m εo o r •Thus, for the ground state n=1, we can see already that since e is on the order of 10, the binding energy of the carrier to the impurity atom is <0.1eV •Expect that many carriers are then ionized at room T •B acceptor in Si: 0.046 eV •P donor in Si: 0.044 eV •As donor in Si: 0.049 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) 10Temperature dependence of majority carriers 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) (Inverse temperature plot) 3.23 Electronic, Optical and Magnetic Properties of Materials - Nicola Marzari (MIT, Fall 2007) 11 Image removed due to copyright restrictions. Please


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