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Ultrafast and Nonlinear
Optical Studies of Reduced Dimensional and Quantum Confined Systems
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Our research focuses on interactions in reduced dimensional
and nanoscale systems, particularly the effects of confinement on the
interactions between different degrees of freedom (charge, spin, vibrational)
as manifested in electronic and vibrational dynamics. Confined systems of
interest include doped and heterostructured semiconductor nanocrystal quantum
dots (QDs) and colloidal graphene QDs. Our most recent work has focused on the
electronic properties of colloidal graphene QDs, nanoscale particles of sp2-hybridized
carbon with narrow size dispersion, in which confinement opens a large gap from
the otherwise gapless extended graphene band structure (Figure 1). We address these
problems via ultrafast nonlinear optical techniques.
Coherent
nonlinear optical processes are especially sensitive to the symmetries of a
system (e.g., the breaking of inversion symmetry at the surface of a system
with a centrosymmetric bulk structure), while optical techniques are among the
few ways to directly access dynamics on the picosecond and sub-picosecond
timescales that characterize many processes in condensed phases. Among problems
of interest to us is the vibrational dynamics at water surfaces, where the
hydrogen bond network is essential to numerous physical, chemical, and
biological phenomena and leads to unusual properties of water including
sub-picosecond vibrational relaxation (Figure 2).
Figure 1: Colloidal graphene quantum dot (A) of 132 conjugated carbon atoms
(blue) and ligands (black) that undergoes internal conversion (IC) and
intersystem crossing (ISC) (illustrated in the Jablonski diagram in B) after optical excitation. S0
represents the ground electronic state and Sn and Tn
(n>0) represent singlet and triplet excited states. Relaxation is followed
by fluorescence (Fl., panel C) and
phosphorescence (Phos., panel D).
(From Mueller et al., Nano Lett. 10, 2679 (2010).) Figure 2: OH-stretch vibrational dynamics at fused-silica/water
interface probed by infrared (IR)-visible sum-frequency generation (SFG) after
excitation by 100 fs, 3400 cm-1 pulse (illustrated schematically in
the inset on the right). The false-color diagram on the left shows the
normalized SFG signal as a function of probe IR frequency and delay. The pump
creates a broadband spectral hole (red), which decays on a ~300 fs timescale
(population relaxation) followed by thermal weakening of the hydrogen-bond
network in ~700 fs resulting in a blue shift of the spectrum reflected in a
long-lived spectral hole to the red and an increase of the signal to the blue.
The panel on the right is a fit. (Modified from J.A. McGuire and Y.R. Shen, Science 313, 1945 (2006).)
