G. Landwehr

Band structure of semimagnetic Hg 1 − y Mn y Te quantum wells

The band structure of semimagnetic

Band structure of semimagnetic Hg1-yMnYTe quantum wells

{\mathrm{Hg}}_{1\ensuremath{-}y}{\mathrm{Mn}}_{y}\mathrm{Te}∕{\mathrm{Hg}}_{1\ensuremath{-}x}{\mathrm{Cd}}_{x}\mathrm{Te}

Band structure of semimagneticHg1−yMnyTequantum wells

type-III quantum wells (QWs) has been calculated using an eight-band

Rashba splitting in n-type modulation-doped HgTe quantum wells with an inverted band structure

\mathbit{k}∙\mathbit{p}

Band structure and its temperature dependence for type-III H g T e / H g 1 − x Cd x Te superlattices and their semimetal constituent

model in an envelope function approach. Details of the band structure calculations are given for the Mn-free case

Quantum transport in n-type and p-type modulation-doped mercury telluride quantum wells

(y=0)

Valence band structure ofHgTe/Hg1−xCdxTesingle quantum wells

. A mean-field approach is used to take the influence of the

Growth and studies of Hg1−xCdxTe based low dimensional structures

sp\text{\ensuremath{-}}d

MBE growth and characterization of Hg based compounds and heterostructures

exchange interaction on the band structure of QWs with low Mn concentrations into account. The calculated Landau level fan diagram and the density of states of a

Absence of magneto-intersubband scattering in n-type HgTe quantum wells

{\mathrm{Hg}}_{0.98}{\mathrm{Mn}}_{0.02}\mathrm{Te}∕{\mathrm{Hg}}_{0.3}{\mathrm{Cd}}_{0.7}\mathrm{Te}