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Interfaces with dielectrics and semiconductors

100 A of material, so that the sharpness of the interface also implies that there is little roughness of the interface. [Pg.341]

More precise measurements of the abruptness of the interface are obtained from Raman spectroscopy and X-ray scattering. Some Raman spectra of a-Si H and a-Ge H multilayers are shown in Fig. [Pg.341]

These measurements are not, however, the complete story. Electron [Pg.341]


There are several, relatively simple reasons for the dominance of silicon The band gap of 1.1 eV is just suitable for devices operating at temperatures encountered in the most applications (-40 to +50 °C). From the chemical point of view, silicon is the only semiconductor which forms a stable oxide with excellent dielectric properties. In spite of the incommensurability of their crystal lattices, an almost perfect interface with a low defect density of < 10 cm can be routinely prepared between silicon and... [Pg.821]


See other pages where Interfaces with dielectrics and semiconductors is mentioned: [Pg.340]    [Pg.341]    [Pg.343]    [Pg.345]    [Pg.347]    [Pg.340]    [Pg.341]    [Pg.343]    [Pg.345]    [Pg.347]    [Pg.468]    [Pg.139]    [Pg.8]    [Pg.120]    [Pg.326]    [Pg.96]    [Pg.217]    [Pg.218]    [Pg.219]    [Pg.225]    [Pg.230]    [Pg.42]    [Pg.43]    [Pg.48]    [Pg.133]    [Pg.140]    [Pg.158]    [Pg.409]    [Pg.517]    [Pg.517]    [Pg.106]    [Pg.36]    [Pg.57]    [Pg.105]    [Pg.114]    [Pg.115]    [Pg.245]    [Pg.247]    [Pg.247]    [Pg.1263]    [Pg.119]    [Pg.402]    [Pg.399]    [Pg.166]    [Pg.1340]    [Pg.1342]    [Pg.737]    [Pg.738]    [Pg.311]    [Pg.313]    [Pg.193]    [Pg.198]    [Pg.447]    [Pg.463]   


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