The spin state of [Fe(H2B(pz)2)2(bipy)] thin films is mediated by changes in the electric field at the interface of organic ferroelectric polyvinylidene fluoride with trifluoroethylene (PVDF-TrFE). Signatures of the molecular crossover transition are evident in changes in the unoccupied states and the related shift from diamagnetic to paramagnetic characteristics. This may point the way to the molecular magneto-electric effect on devices.
In this paper, we use atomic force microscopy (AFM) to nanostructure and image 1,10-decanedithiol (DDT)
and biphenyl 4,4‘-dithiol (BPDT) layers on Au(111) surfaces comparing them to those prepared by self-assembly. First, layers of dithiols are self-assembled from solution onto gold surfaces and are imaged in situ
with an AFM to examine the roughness of the layers. Second, 100 nm × 100 nm monolayer patches made
of dithiol molecules are nanografted into a self-assembled monolayer (SAM) inert matrix made of 1-decanethiol
(DT). Although nanografting of thiols routinely generates very compact layers with good height uniformity,
nanostructuring of dithiols using this method always yields multilayers that form through intermolecular S−S
bonds. We demonstrate in this paper two possible ways of tailoring, layer by layer, the structure of dithiols.
First, we form multilayers by nanografting, using then the AFM tip to gradually shave away the top layers.
In the second way, we add antioxidant to the solution while doing nanografting to suppress the oxidative
coupling of the −SH groups. We found that nanografting in the presence of excess amounts of antioxidant
can produce monolayers of dithiols. The so-produced DDT monolayer patches are lower than what can be
calculated by the 30° tilt model, while the height of nanografted patches of BPDT closely corresponds to a
vertical configuration. Finally, we use conductive-probe AFM to investigate the electron tunneling properties
through BPDT multilayers. The molecules in these layers turn out to behave as conductive molecular wires
and making these nanostructures good candidates for constructing molecular electronic devices.
Crystalline Langmuir–Blodgett copolymer films of vinylidene fluoride with trifluoroethylene (70%:30% and 80%:20%) absorb water. Water absorption is accompanied by film swelling, as indicated by an increase in lattice spacing, sometimes by as much as 5%. This water absorption, between 0 and 40 °C, is a result of intercalation or occupation of interstitial sites between the layers of the film, not just water molecules filling voids and defect sites alone. An increase in the film capacitance is observed, although the polymer chains retain all trans configuration of the ferroelectric phase.
Ferroelectric crystalline copolymer films of vinylidene fluoride with trifluoroethylene (70%:30%) strongly interact with the dipoles of adsorbed and absorbed water molecules. This interaction can be probed with laser-assisted thermal desorption techniques. The UV light enhancement of water desorption is strongly light polarization dependent. The electronic structure of the ferroelectric copolymer films of vinylidene fluoride with trifluoroethylene films is locally altered with incident UV radiation suggesting metastable excited states that may involve dipole reorientation.
Water adsorption and absorption on crystalline polyvinylidene fluoride with 30% trifluoroethylene, P(VDF-TrFE, 70:30), was examined by thermal desorption spectroscopy. Two distinctly different water adsorption sites are identified: one adsorbed species that resembles ice and another species that interacts more strongly with the polymer thin film. The existence of the latter species is consistent with X-ray diffraction studies of water absorbed into the bulk of copolymers of polyvinylidene fluoride with trifluoroethylene crystalline thin films. There are strong steric effects observed in the angle-resolved thermal desorption that may be a result of the large polymer thin film surface dipoles.
Two different polymers, with large local electric dipoles, are compared: copolymers
of polyvinylidene fluoride with trifluoroethylene [P(VDF-TrFE, 70%:30%)] and
polymethylvinylidenecyanide (PMVC). While the different local point group symmetries
play a key role, both crystalline polymers exhibit intra-molecular band structure, though
the Brillouin zone critical points differ.
For both water and heavy water adsorption and absorption on crystalline poly(vinylidene fluoride with trifluoroethylene (30%)), P(VDF-TrFE 70:30), two distinctly different adsorption sites have been identified by thermal desorption spectroscopy. One adsorbed water species resembles ice and there is also an absorbed water species that interacts more strongly with the polymer thin film, and in addition, there is a polymer surface (polymer to ice interface) water species. We find that there is H/D exchange between the water or heavy water molecules and the ferroelectric polymer (largely -(CH2-CF2)-), particularly at the polymer surface.
Atomic force microscopy (AFM) has been widely employed as a nanoscopic lithography technique. In this review, we summarize the current state of research in this field. We introduce the various forms of the technique, such as nanoshaving, nanografting and dip-pen nanolithography, which we classify according to the different interactions between the AFM probe and the substrate during the nanolithography fabrication process. Mechanical force, applied by the tip to the substrate, is the variable that can be controlled with good precision in AFM and it has been utilized in patterning self-assembled monolayers. In such applications, the AFM tip can break some relatively weak chemical bonds inside the monolayer. In general, the state of the art for AFM nanolithography demonstrates the power, resolution and versatility of the technique.
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