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Transient emission spectra recording

Fig. 48. DLTS measurement time constant t (inverse of rate window) versus the inverse temperature of the peak in the electron emission spectrum at that r for a typical sample. The activation energy of 0.94 eV is the slope of the raw data without the 2kT correction (see text). The circles are from DLTS spectra the triangles are calculated from directly recorded capacitance transients. Fig. 48. DLTS measurement time constant t (inverse of rate window) versus the inverse temperature of the peak in the electron emission spectrum at that r for a typical sample. The activation energy of 0.94 eV is the slope of the raw data without the 2kT correction (see text). The circles are from DLTS spectra the triangles are calculated from directly recorded capacitance transients.
See other pages where Transient emission spectra recording is mentioned: [Pg.297]    [Pg.4]    [Pg.54]    [Pg.216]    [Pg.310]    [Pg.74]    [Pg.63]    [Pg.239]    [Pg.198]    [Pg.24]    [Pg.149]    [Pg.445]    [Pg.155]    [Pg.155]    [Pg.198]    [Pg.20]    [Pg.64]   
See also in sourсe #XX -- [ Pg.184 ]



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