Abstract
In this work we study the Zeeman splitting in induced ballistic 1D wires fabricated along two orthogonal crystallographic directions [ 2 ¯ 3 3 ] and [ 0 1 1 ¯ ] . Our data shows that the g-factor anisotropy for the high symmetry [ 0 1 1 ¯ ] direction can be explained by the 1D confinement only, whereas in the case of [ 2 ¯ 3 3 ] direction, the interaction between the 1D confinement and crystal anisotropy effects is evident.
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