Energy level alignments at the organic donor–acceptor interface cannot be predicted from cyclic voltammetry. Onsets for joint density of states and charge generation, reveal cases of energy uphill and – newly observed – downhill charge generation.

We analyze the scattering of the surface plasmon incident at a planar interface between two dielectrics. By using the scattering matrix technique, developed by Oulton et al. [Phys. Rev. B 76, 035408 (2007)], we calculate the transmission, reflection coefficients and radiative losses for oblique incident angles. We found that the transmission of a surface wave through a single interface between two dielectrics may be accompanied with radiation losses of 10-40 per cent of the plasmon energy.

This paper deals with the electrochemically induced charge injection in the conductive polymer (CP), exemplified by well examined archetypal CP—poly(3-hexylthiophene-2,5-diyl). The polar solvent of acetonitrile with salt tetrabutylammonium hexafluorophosphate was used to transport electrons in the electrolyte. The decisive mechanism is the recombination current at the electrolyte/CP interface taking place at the Fermi energy of CP, whose energy position is determined by the externally applied voltage. The corresponding mechanism of the charge carrier transport in the polymer bulk is the space-charge limited current (SCLC) by holes or electrons (or more precisely positive and negative polarons) at the respective transport paths of HOMO and LUMO bands. The charge transport mechanisms and the occupation statistics are the basis of the energy-resolved electrochemical impedance spectroscopy for the mapping of the density of electronic states of conductive organic semiconductors [F. Schauer, V. Nádaždy, and K. Gmucová, J. Appl. Phys. 123, 161590 (2018)]. From the application point of view, the major message of the paper is that it is possible to pass high current densities of the order of 0.1 A cm−2 via electrochemical systems with the CP, induced by means of doping processes of both CP surface and its bulk, leading to the charge injection and SCLC in CP.

In this study, dendrimers have been purposed as an alternative approach for delivery of HIV peptides to dendritic cells. We have investigated the interaction of dendriplexes formed from polyanionic HIV peptide Nef and cationic carbosilane dendrimer (CBD) with model lipid membranes - large unilamellar vesicles (LUVs), Langmuir monolayers and supported lipid membranes (sBLMs) containing various molar ratio of zwitterionic 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) and 1,2-distearoyl-sn-glycero-3-phosphoethanolamine-N-[methoxy (polyethylene glycol)-2000] (DSPE-PEG). In our experiments, the lipid membranes represented the model of the plasma membrane of the cell. PEGylated lipids were used in order to model glycocalyx which constitutes the outer leaflet of cellular membranes. The presence of PEGylated lipids resulted in an increase of the phase transition temperature of the lipid bilayer of LUVs, in a decrease of specific volume and adiabatic compressibility. Fluorescence anisotropy study suggests that PEGylated LUVs possessed higher lipid order and decreased fluidity when compared to zwitterionic DMPC vesicles. The interaction of dendriplexes with monolayers was accompanied by the formation of the aggregates as revealed by BAM experiments. This conclusion has been confirmed also by AFM imaging of sBLMs. We have demonstrated that dendriplexes interact with lipid membranes for all types of lipid composition. Moreover, the stronger interaction of cationic dendrimer/peptide complexes with lipid monolayers, vesicles and sBLMs was observed for membranes composed of zwitterionic lipids than for PEGylated lipid membranes. Increased concentration of PEGylated lipids made this interaction weaker.

We study propagation of surface electromagnetic waves along a metallic surface covered by various layered dielectric struc− tures. We show that strong radiative losses, typical for scattering of a surface wave, can be considerably suppressed when a single dielectric step is substituted by gradient index or periodic layered structure.