In Situ Growth and Doping Studies of Topological Insulator Bismuth Selenide
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Abstract
The past decade has borne witness to the rapid development of a new field
of theoretical and experimental condensed matter physics commonly referred to
as "topological insulators". In a (experimentalist's) single sentence a topological
insulator can be thought of as material that behaves like an empty metal box:
the i-dimensional material (i = 2,3) is insulating, but conducting states exist at
the (i-1)-dimensional boundaries. These edge or surface states possess non-trivial
properties that have generated interest and excitement for their potential utility in
solving practical problems in spin electronics as well as the creation of condensed
matter systems for realizing and testing new physics. The most extensively studied
materials systems with these properties suffer a major drawback in that the interior
of the metal box is not "empty" (insulating) but instead filled with metal. The
goal of this work has been to understand why the box is full instead of empty, and
explore a particular pathway to making it empty.
To address these outstanding questions in the literature pertaining to the persistent n-doping of topological insulator Bi2Se3, a custom apparatus was developed
for combined epitaxial thin film growth with simultaneous, in situ measurement
of transport characteristics (resistivity, Hall carrier density and mobility). Bi2Se3
films are found to be n-doped before exposure to ambient conditions and this doping
appears to be interfacial in origin. This work and methodology was extended to
study the efficacy of an amorphous MoO3 capping layer. MoO3 acts as an electron
acceptor, p-doping the Bi2Se3 up to a |∆n| = 1x10^13 cm−2
change in carrier density.
Complimentary X-ray photoemission spectroscopy (XPS) on bulk crystals showed
that this was enough to put the Fermi level into the topological regime. Thin films
were too highly n-doped initially to reach the topological regime, but the same magnitude change in doping was observed via the Hall effect. Finally, a Bi2Se3 film with
a 100 nm capping layer of MoO3 was vented to ambient, and found to retain a stable
doping for days of ambient exposure, demonstrating the effectiveness of MoO3 for
passivation.