Deep-level transient spectroscopy was used to measure the activation energies of deep levels in n-type Si/Si1–x–yGexCy heterostructures grown by solid-source molecular-beam epitaxy. Four deep levels have been observed at various activation energies ranging from 231 to 405 meV below the conduction band. The largest deep-level concentration observed was in the deepest level and was found to be approximately 2 × 10^15 cm^–3. Although a large amount of nonsubstitutional C was present in the alloy layers (1–2 at. %), no deep levels were observed at any energy levels that, to the best of our knowledge, have been previously attributed to interstitial C
Molecular beam epitaxy of Si1−xGex alloys, using gaseous Si2H6 and solid Ge as sources, has been stu...
We study the passivation and recovery of shallow and deep levels in Si-doped AlGaAs exposed to CH4/H...
Deep centers in Si-doped n-GaN layers grown by reactive molecular beam epitaxy have been studied by ...
Deep-level transient spectroscopy was used to measure the activation energies of deep levels in n-ty...
We have used admittance spectroscopy and deep-level transient spectroscopy to characterize electroni...
We have used admittance spectroscopy to measure conduction-band and valence-band offsets in Si/Si1–x...
This paper reports on a Deep-Level Transient Spectroscopy (DLTS) study of the electrically active de...
Si1–x–yGexCy/Si superlattices were grown by solid-source molecular beam epitaxy using silicon carbid...
Deep level distributions have been investigated in B-doped Si/Si1-xGex/Si layers grown by molecular ...
Realization of group IV heterostructure devices requires the accurate measurement of the energy band...
The presence of deep levels in a silicon–oxygen (Si–O) superlattice (SL) deposited on p-type silicon...
This work reports on the deep levels observed in Pt/Al2O3/p-type Si metal-oxide-semiconductor capaci...
Changing the ratio of carbon to silicon during the epitaxial 4H–SiC growth is expected to alter the ...
The ability to determine structural and compositional information from the sub-surface region of a s...
Si/Si1-xGex strained layer heterostructures offer great promise for applications in field-effect and...
Molecular beam epitaxy of Si1−xGex alloys, using gaseous Si2H6 and solid Ge as sources, has been stu...
We study the passivation and recovery of shallow and deep levels in Si-doped AlGaAs exposed to CH4/H...
Deep centers in Si-doped n-GaN layers grown by reactive molecular beam epitaxy have been studied by ...
Deep-level transient spectroscopy was used to measure the activation energies of deep levels in n-ty...
We have used admittance spectroscopy and deep-level transient spectroscopy to characterize electroni...
We have used admittance spectroscopy to measure conduction-band and valence-band offsets in Si/Si1–x...
This paper reports on a Deep-Level Transient Spectroscopy (DLTS) study of the electrically active de...
Si1–x–yGexCy/Si superlattices were grown by solid-source molecular beam epitaxy using silicon carbid...
Deep level distributions have been investigated in B-doped Si/Si1-xGex/Si layers grown by molecular ...
Realization of group IV heterostructure devices requires the accurate measurement of the energy band...
The presence of deep levels in a silicon–oxygen (Si–O) superlattice (SL) deposited on p-type silicon...
This work reports on the deep levels observed in Pt/Al2O3/p-type Si metal-oxide-semiconductor capaci...
Changing the ratio of carbon to silicon during the epitaxial 4H–SiC growth is expected to alter the ...
The ability to determine structural and compositional information from the sub-surface region of a s...
Si/Si1-xGex strained layer heterostructures offer great promise for applications in field-effect and...
Molecular beam epitaxy of Si1−xGex alloys, using gaseous Si2H6 and solid Ge as sources, has been stu...
We study the passivation and recovery of shallow and deep levels in Si-doped AlGaAs exposed to CH4/H...
Deep centers in Si-doped n-GaN layers grown by reactive molecular beam epitaxy have been studied by ...