The extra electron is bound to an approximately singly charged donor through a dielectric-screened Coulomb attraction. In the isotropic hydrogenic donor state model, replace the vacuum electron mass by and the vacuum permittivity by :At low temperature, the donor is mainly in its state. Allowed electric-dipole transitions to states haveAssign the three printed lines to . Their independently inferred binding energies areThey are mutually close, giving . The hydrogenic impurity absorption series accumulates at the donor-ionization limit. Above about , absorption can place the electron in the conduction-band continuum, explaining the continuous spectrum.
Using the supplied and ,The corresponding effective radius isThese are the parameters inferred from the printed lines within the stipulated scalar model, rather than substituted tabulated material constants. Real impurity spectra can depart from a single hydrogenic ladder through anisotropy and short-distance impurity effects.[ref]
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