Titlebook: Semiconductor Physics; An Introduction Karlheinz Seeger Book 19822nd edition Springer-Verlag Berlin Heidelberg 1982 epitaxy.hydrogen.physic

Entangle

書目名稱Semiconductor Physics影響因子(影響力)




書目名稱Semiconductor Physics影響因子(影響力)學科排名




書目名稱Semiconductor Physics網(wǎng)絡(luò)公開度




書目名稱Semiconductor Physics網(wǎng)絡(luò)公開度學科排名




書目名稱Semiconductor Physics被引頻次




書目名稱Semiconductor Physics被引頻次學科排名




書目名稱Semiconductor Physics年度引用




書目名稱Semiconductor Physics年度引用學科排名




書目名稱Semiconductor Physics讀者反饋




書目名稱Semiconductor Physics讀者反饋學科排名

在駕駛

Energy Band Structure,uare of the momentum. The factor of proportionality is 1/2 .., where .. is the free electron mass. In the ., the same relationship between energy and momentum is assumed except that .. is replaced by an . This may be larger or smaller than ... Why this is so will be seen later in this chapter. Quite

MULTI

Semiconductor Statistics,ve seen in Fig. 2.8. A discussion of these levels can be confined to the first Brillouin zone. We saw in the last chapter that due to the crystal periodicity, the electron wave functions, which in one dimension are . = . exp (i ., also have to be periodic . Hence, from .and .we obtain .or .where a i

flutter

CHASE

閑聊

Scattering Processes in a Spherical One-Valley Model,nomagnetic, thermoelectric, thermomagnetic, etc., effects. We will now treat the important scattering mechanisms and find the energy dependence of τ. . For those cases where a power law is found, the magnitude of the exponent . will be determined.

Autobiography

Charge Transport and Scattering Processes in the Many-Valley Model,her 8 half-ellipsoids of 6 ellipsoids of revolution; these correspond to 4 and 6 energy valleys, respectively. In these and many other semiconductors the . of the energy bands has proved to be a fruitful concept for a description of the observed anisotropy of electrical and optical phenomena. Cyclot

烤架

Carrier Transport in the Warped-Sphere Model,s case are warped spheres which have already been discussed in Sect. 2.4 (Figs. 2.28 a-2.28 c) . In the zincblende lattice typical for III—V compounds, there is no center of inversion, in contrast to the diamond lattice.

GRIN

Quantum Effects in Transport Phenomena, only domain of quantum mechanics in semiconductivity. Although most transport phenomena can be explained by assuming a classical electron gas, there are some which can be understood only by quantum mechanical arguments. In Sect. 9.1 we will treat phenomena which rely on the quantum mechanical ., wh

separate

Impact Ionization and Avalanche Breakdown,uctors may serve as model substances for gaseous plasmas since their ionic charges are practically immobile and therefore the interpretation of experimental data is facilitated. Impact ionization has been achieved both in the bulk of homogeneously doped semiconductors at low temperatures and in p-n