Reversible Electrochemistry of Mercury Chalcogenide Colloidal Quantum Dot Films.
The absolute positions of the energy levels of colloidal quantum dots of Hg(S, Se, Te), which are of interest as mid-infrared materials, are determined by electrochemistry. The bulk valence bands are at -5.85, -5.50, and -4.77 eV (±0.05 eV) for zinc-blend HgS, HgSe, HgTe, respectively, in the same order as the anions p-orbital energies. The conduction bands are conversely at -5.20, -5.50, and -4.77 eV. The stable ambient n-doping of Hg(S, Se) quantum dots compared to HgTe arises because the conduction band is sufficiently lower than the measured environment Fermi level of ∼ -4.7 eV to allow for n-doping for HgS and HgSe quantum dots even with significant electron confinement. The position of the Fermi level and the quantum dots states are reported for a specific surface treatment with ethanedithiol and electrolyte environment. The positions are however sensitive to different surface treatments, providing an avenue to control doping. Electrochemical gating is further used to determine the carrier mobility in the films of the three different systems as a function of CQD size. HgSe and HgS show increasing mobility with increasing particle sizes while HgTe shows a nonmonotonous behavior, which is attributed to some degree of aggregation of HgTe QDs.
James Franck Institute, The University of Chicago , 929 East 57th Street, Chicago, Illinois 60637, United States.
Menglu
0000-0003-0052-9310
M
Chen
James Franck Institute, The University of Chicago , 929 East 57th Street, Chicago, Illinois 60637, United States.
Philippe
0000-0003-0178-6255
P
Guyot-Sionnest
colloidal quantum dots; doping; electrochemistry; electronic structure; infrared; mobility