1. Colloidal nanomaterials
Box 1 – History
Until the 1960s, low-dimensional objects remained the preserve
of theorists. In the 1970s, with advances in fabrication methods and
in particular molecular jet epitaxy, it became possible to design
samples whose size is smaller than the Bohr radius of the material
of which they are made. While silicon is the king of electronics,
its indirect gap makes it a poor candidate for optical applications.
In contrast, III-V semiconductors, and GaAs in particular, feature
a band structure with a direct band gap (i.e. the conduction band
maximum is located at the same pulse as the conduction band minimum),
so it's only natural that these materials should be used for optoelectronics.
In nanoscale semiconductor structures, the bandgap energy is modified
relative to bulk material by quantum confinement. Quantum confinement
has enabled a paradigm...
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Colloidal nanomaterials