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Prototypes of Molecular Gears with an Organometallic Piano-Stool Architecture

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Abstract

In the field of Molecular Machines, molecular gears have mainly been synthesized to be studied in solution. Then, the cogwheel subunits are restricted to be only arranged in an intramolecular manner. In the last years, the possibility to arrange a train of gears at the single molecular level and observe the propagation of a rotation motion from one molecule to its neighbor using Scanning Tunneling Microscopy (STM) opened new perspectives with the opportunity to have intermolecular arrangements on surfaces. In this chapter, we describe the research background of single molecular gears and our strategy using organometallic piano-stool complexes to anchor such gears on surfaces. Our molecules incorporate two subunits linked together through a ruthenium center acting as a ball bearing. The lower part is the anchoring tripodal ligand and the upper part the cogwheel. Various functionalities have been explored to behave as teeth, ranging from mono-dimensional phenyl rings to bi-dimensional porphyrin fragments.

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Empirical force-field calculations show that bis(9-triptycyl)methane has a C(s) ground state and that the securely meshed triptycyl groups undergo nearly unhindered cogwheel rotation through a C(2) transition state, with an activation energy of approximately 1.0 kcal mol(-1). These features lead to note-worthy stereochemical attributes in appropriately substituted derivatives and analogs. Bis(9-triptycyl)carbinol has been prepared as an example of a compound that is chemically achiral, even though all conformations are chiral under the constraint of gear meshing. It is shown that, under the same constraint, ring substitution of either compound (or analogous systems) may lead to residual stereoisomerism. A permutational analysis of chemical isomers and isomerizations for every possible type of substitution pattern gives an enumeration of residual stereoisomers under the operation of various gearing and nongearing modes and provides information essential for a choice among mechanistic alternatives for a given isomer count.
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Molecular machines, and in particular molecular motors with synthetic molecular structures and fuelled by external light, voltage or chemical conversions, have recently been reported. Most of these experiments are carried out in solution with a large ensemble of molecules and without access to one molecule at a time, a key point for future use of single molecular machines with an atomic scale precision. Therefore, to experiment on a single molecule-machine, this molecule has to be adsorbed on a surface, imaged and manipulated with the tip of a scanning tunnelling microscope (STM). A few experiments of this type have described molecular mechanisms in which a rotational movement of a single molecule is involved. However, until now, only uncontrolled rotations or indirect signatures of a rotation have been reported. In this work, we present a molecular rack-and-pinion device for which an STM tip drives a single pinion molecule at low temperature. The pinion is a 1.8-nm-diameter molecule functioning as a six-toothed wheel interlocked at the edge of a self-assembled molecular island acting as a rack. We monitor the rotation of the pinion molecule tooth by tooth along the rack by a chemical tag attached to one of its cogs.
Article
A combination of solid-state 13C CPMAS NMR, 2H NMR, X-ray-determined anisotropic displacement parameters (ADPs), and molecular mechanics calculations were used to analyze the rotational dynamics of 1,4-bis[3,3,3-tris(m-methoxyphenyl)propynyl]benzene (3A), a structure that emulates a gyroscope with a p-phenylene group acting as a rotator and two m-methoxy-substituted trityl groups acting as a stator. The line shape analysis of VT 13C CPMAS and broad-band 2H NMR data were in remarkable agreement with each other, with rotational barriers of 11.3 and 11.5 kcal/mol, respectively. The barriers obtained by analysis of ADPs obtained by single-crystal X-ray diffraction at 100 and 200 K, assuming a sinusoidal potential, were 10.3 and 10.1 kcal, respectively. A similar analysis of an X-ray structure solved from data acquired at 300 K suggested a barrier of only 8.0 kcal/mol. Finally, a rotational potential calculated with a finite cluster model using molecular mechanics revealed a symmetric but nonsinusoidal potential that accounts relatively well for the X-ray-derived values and the NMR experimental results. It is speculated that the discrepancy between the barriers derived from low and high-temperature X-ray data may be due to an increase in anharmonicity, or to disorder, at the higher temperature values.
World’s first nanocar race: a single molecule piloted per team
  • G Rapenne
  • C Joachim
STM Manipulation of boron-subphthalocyanine nano-wheel dimers on Au(111)
  • A Nickel
  • J Meyer
  • R Ohmann
  • H.-P Jacquot De Rouville
  • G Rapenne
  • C Joachim
  • G Cuniberti
  • F Moresco