Proceedings of the International School of Physics "Enrico Fermi.", Volume 22N. Zanichelli, 1963 - Nuclear physics |
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Page 199
... equation written in the form ( 2.3 ) Df + Dt ( f- fo ) T E - ( ) ( ) ( ) ( ) ( ) h E Of the two approaches the equation of motion gives a simpler pictorial ac- count of the motion and we will adopt this approach . It can simply be gene ...
... equation written in the form ( 2.3 ) Df + Dt ( f- fo ) T E - ( ) ( ) ( ) ( ) ( ) h E Of the two approaches the equation of motion gives a simpler pictorial ac- count of the motion and we will adopt this approach . It can simply be gene ...
Page 243
... equations of motion are more complicated and must be handled by means of a Boltzmann equation or by integrals which will be derived later . 21. Conductivity of holes and electrons . Since we are ultimately seeking an expression for the ...
... equations of motion are more complicated and must be handled by means of a Boltzmann equation or by integrals which will be derived later . 21. Conductivity of holes and electrons . Since we are ultimately seeking an expression for the ...
Page 480
... equation ( 2.1 ) where Hy = Ey , ( 2.2 ) H = p2 2m + V2 ( r ) , p 4 . i We have neglected any exchange interaction in this equation . This appears to be valid as the associated effects seem small [ 2 ] . Our equation has the well ...
... equation ( 2.1 ) where Hy = Ey , ( 2.2 ) H = p2 2m + V2 ( r ) , p 4 . i We have neglected any exchange interaction in this equation . This appears to be valid as the associated effects seem small [ 2 ] . Our equation has the well ...
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absorption acceptor approximation band edge band structure Brillouin zone calculated carrier Chem coefficient compound concentration conduction band constant corresponding crystal cyclotron resonance density diffusion direction donor doping effective mass electric field energy gap energy surfaces equation equilibrium example exciton experimental expression Faraday rotation foreign atoms free electron frequency germanium given hence holes imperfections impurity indium antimonide InSb interaction interband ionization ions Journ K,PM K₁ lattice levels linear liquid magnetic field matrix measurements melt mobility momentum N₁ obtained optical p-type phase phonon Phys potential pressure quantum range reciprocal lattice region Rendiconti S.I.F. samples scattering semiconductors shown in Fig solid spin-orbit structure elements symmetry temperature tensor theory thermodynamic potentials transition transverse valence band Voigt effect wave functions wave vector Zeeman effect zero zone