Javascript must be enabled to continue!
C60 chain phases on ZnPc/Ag(111) surfaces: Supramolecular organization driven by competing interactions
View through CrossRef
Serpentine chain C60 phases were observed in scanning tunneling microscopy (STM) images of C60 layers on zinc phthalocyanine (ZnPc) or pentacene covered Ag(111) and Au(111) surfaces. This low-density, quasi-one-dimensional organization contrasts starkly with the close-packed hexagonal phases observed for C60 layers on bare metal substrates. STM was employed to perform a detailed investigation of these chain structures for C60/ZnPc/Ag(111) heterolayers. Motivated by the similarity of these chain phases, and the chain and stripe organization occurring in dipole-fluid systems, we investigated a model based on competing van der Waals attractions and electrostatic repulsions between C60 molecules as an explanation for the driving force behind these monolayer phases. Density functional theory (DFT) calculations revealed significant charge transfer to C60 from the Ag(111) substrate, through the intervening ZnPc layer, inducing electrostatic interactions between C60 molecules. Molecular dynamics simulations performed with attractive van der Waals interactions plus repulsive dipole-dipole interactions reproduced the C60 chain phases with dipole magnitudes consistent with DFT calculations.
Title: C60 chain phases on ZnPc/Ag(111) surfaces: Supramolecular organization driven by competing interactions
Description:
Serpentine chain C60 phases were observed in scanning tunneling microscopy (STM) images of C60 layers on zinc phthalocyanine (ZnPc) or pentacene covered Ag(111) and Au(111) surfaces.
This low-density, quasi-one-dimensional organization contrasts starkly with the close-packed hexagonal phases observed for C60 layers on bare metal substrates.
STM was employed to perform a detailed investigation of these chain structures for C60/ZnPc/Ag(111) heterolayers.
Motivated by the similarity of these chain phases, and the chain and stripe organization occurring in dipole-fluid systems, we investigated a model based on competing van der Waals attractions and electrostatic repulsions between C60 molecules as an explanation for the driving force behind these monolayer phases.
Density functional theory (DFT) calculations revealed significant charge transfer to C60 from the Ag(111) substrate, through the intervening ZnPc layer, inducing electrostatic interactions between C60 molecules.
Molecular dynamics simulations performed with attractive van der Waals interactions plus repulsive dipole-dipole interactions reproduced the C60 chain phases with dipole magnitudes consistent with DFT calculations.
Related Results
Photophysical Properties of Substituted Zinc Phthalocyanine‐Dextran Systems
Photophysical Properties of Substituted Zinc Phthalocyanine‐Dextran Systems
This study presents the synthesis of tetracarboxy ZnPc/dextran and octacarboxy ZnPc/dextran solutions and the investigation of their photophysical properties using UV–vis, transien...
Different Photoresponses for Positive and Negative Biases of CuPc/C60 Heterojunction Nanostructures
Different Photoresponses for Positive and Negative Biases of CuPc/C60 Heterojunction Nanostructures
Photoresponse characteristic from efficient exciton dissociated heterojunction based on copper phthalocyanine (CuPc) and fullerene (C60) layers was observed the different spectrum ...
Interaction of Molecules in Solutions of C60 in Polar Solvents
Interaction of Molecules in Solutions of C60 in Polar Solvents
The features of fullerene C60 in N-methyl-2-pyrrolidone (NMP) solutions and NMP/water solvents were studied using optical absorption spectroscopy, dynamic light scattering (DLS) an...
Fermi level determination in organic thin films by the Kelvin probe method
Fermi level determination in organic thin films by the Kelvin probe method
We show that the Kelvin probe method (KPM) is well suited for in situ measurements of the Fermi level of organic vapor-deposited dye layers. The method works well even for high res...
Effect of C60 as an electron buffer layer in polythiophene‐methanofullerene based bulk heterojunction solar cells
Effect of C60 as an electron buffer layer in polythiophene‐methanofullerene based bulk heterojunction solar cells
AbstractThe effect of C60 interlayer on charge transport and device performance in bulk heterojunction solar cells with active layer of poly3‐hexylthiophene (P3HT) and l‐3‐methoxyc...
Thermal stability of a star‐shaped poly(1,3‐cyclohexadiene)
Thermal stability of a star‐shaped poly(1,3‐cyclohexadiene)
AbstractA star‐shaped poly(1,3‐cyclohexadiene) (PCHD) with a fullerene‐C60 (C60) core (C60‐PCHD) was prepared to examine the thermal stability of the covalent bond between the C60 ...
Solution behavior of buckminsterfullerene (C60) in benzene
Solution behavior of buckminsterfullerene (C60) in benzene
Solution characterization of buckminsterfullerene C60 in benzene was carried out by laser light scattering. Static and dynamic light scattering (SLS and DLS) experiments were accom...
PHOTOPHYSICS OF Y2O3:ZnPc(COOH)4 ASSEMBLIES
PHOTOPHYSICS OF Y2O3:ZnPc(COOH)4 ASSEMBLIES
Yttrium oxide nanoparticles were conjugated separately to zinc
tetracarboxy phthalocyanine (ZnPc(COOH)₄) to form Y₂O₃:ZnPc(COOH)₄
assemblies. The triplet quantum yields and lifetim...

