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Excitonic coupling in SAMs of azobenzene-functionalized
alkanethiols
The functionalization of surfaces with molecular
switches is a rapidly growing field in today’s research. Molecules
can be used as repeatable building blocks for electronics and sensors
and thereby open the perspective to tailor devices on the nanoscale.
In this respect self-assembled monolayers (SAMs) have often been
considered as ideal platforms to order and align molecules at surfaces.
Optical properties and geometric structure of self-assembled monolayers
of azobenzenefunctionalized alkanethiols have been investigated
by UV/Visible and near edge X-ray absorption fine structure spectroscopy
in combination with density-functional theory. By attaching a trifluoro-methyl
endgroup to the chromophore both the molecular tilt and twist angle
of the azobenzene moiety are accessible. Based on this detailed
structural analysis the energetic shifts observed in optical reflection
spectroscopy can be qualitatively described within an extended dipole
model. This substantiates sizeable excitonic coupling among the
azobenzene chromophores as an important mechanism that hinders trans
to cis isomerization in denselypacked self-assembled monolayers.
J. Am. Chem. Soc., 2010 in press.
funded DFG through Sfb658,
Elementary Processes in Molecular Switches at Surfaces
Ultrafast demagnetisation of Gd
Gadolinium with its half-filled 4f core shell is a particular
prototype system to study magnetisation dynamics. The strongly localised
4f 7 electrons carry most of the magnetic moment
of 7.55 μB per atom. They spin-polarise the 5d
valence
electrons resulting in the extra contribution of 0.55 μB
per atom. This
intra-atomic 4f-5d exchange coupling in turn mediates magnetic order
within the 4f system below the Curie temperature of TC
= 293 K. This behaviour differs significantly from the itinerant
ferromagnets iron, cobalt, and nickel.
In a recent experiment we combined laser and synchrotron for pump-probe
experiments which allows us to directly measure the temporal evolution
of the 4f contribution to the magnetisation. Epitaxial
Gd(0001) films of 100 Å thickness, with the easy axis in plane,
have been grown on W(110). The Gd magnetisation is monitored by
magnetic linear dichroism (MLD) of the 4f photoemission
line. We established that the
temperature dependence of the MLD signal follows the spontaneous
magnetisation M/M(0) and assume that this likewise holds on a picosecond
time-scale. The transient magnetisation after laser excitation (hν
= 1.5 eV, fluence of 3.5 mJ/cm2) is shown in Fig. 1 as
a function of pump-probe delay Δt (open circles). A 20 % drop
is followed by a recovery within 1 ns. The drop in the MLD contrast
demonstrates that the 4f magnetic order is reduced upon
optical excitation of the 5d6s valence electrons.
One may argue that this is a pure thermal effect, since we probe
the 4f core-level with a 50 ps time-resolution and electron-lattice
equilibration takes 1.5 ps. From the transient lattice temperature
and the temperature-dependent magnetisation we calculated the transient
magnetisation under the assumption that thermal equilibrium is established
at all delays. This thermal scenario of M(Δt) is plotted in
Fig. 1 by the solid line which was convoluted with a Gaussian of
50 ps width to account for the synchrotron-radiation pulse-length.
80 ps after laser excitation the measured 4f MLD and the calculated
magnetisation agree nicely, which substantiates our modelling.
However, the measured drop of the magnetisation at earlier times
is by a factor of two smaller than expected, which is consistently
reproduced for different fluences. This striking deviation of the
data from the thermal estimate before 80 ps have elapsed shows directly
that equilibrium between the Gd spin system and lattice is not established
in this time regime. The 4f spin-lattice relaxation thus takes much
longer than the electron-lattice equilibration.
Fig. 1: Transient, relative change
of the magnetization: measured 4f dichroism (open circles), calculated
from lattice temperature and magnetization (dashed line), and convoluted
with a Gaussian of 50 ps FWHM (solid line).
Phys. Rev. Lett. 100 (2008) 107202.
funded by DFG through SPP1133 "Ultrafast Magnetization
Processes"
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