Band
alignments are essential for understanding the optical properties
and carrier transfer of core/shell QDs. As CdSe/CdS core/shell QDs
with increasing shell thickness represent red-shifted absorption and
luminescence spectra, weakened oscillator strength of the lowest electronic
transition, and elongated luminescence lifetime, they are assigned
to quasi-type II band alignment. However, femtosecond transient absorption
spectroscopy with state-selective excitation revealed a type I band
alignment of the CdSe/CdS QDs with a thin CdS shell, in which the
excited electron is localized in the CdSe core with core excitation
while delocalized in the whole QDs with shell excitation, even though
a quasi-type II carrier distribution was observed with steady-state
spectroscopy. In the type I core/shell QDs, the CdS shell acts as
an energy barrier in surface electron and hole-trapping processes.
The time constant of the hole-trapping process of the CdSe core (∼10
ps) was elongated 10 times owing to a tunnel effect through the high
energy barrier of the CdS shell, which was estimated from the decay
related to the biexcitonic induced spectral shift. The biexcitonic
spectral shift induced by a ∼100 ps hole-trapping process was
also observed at the 1S(e)–2S3/2(h) transition.
Our results from transient absorption spectroscopy with state-selective
excitation are useful to clarify band alignment and carrier distribution
of hetero-nanostructures, which could help to objectively extract
charge carriers in photovoltaic applications.