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Review

From the Synthesis of Nanovehicles to Participation in the First Nanocar Race—View from the French Team

by
Henri-Pierre Jacquot de Rouville
1,
Claire Kammerer
1 and
Gwénaël Rapenne
1,2,*
1
CEMES, Université de Toulouse, CNRS, 31055 Toulouse, France
2
Graduate School of Materials Science, Nara Institute of Science and Technology, Takayama 8916-5, Ikoma, Nara, Japan
*
Author to whom correspondence should be addressed.
Molecules 2018, 23(3), 612; https://doi.org/10.3390/molecules23030612
Submission received: 29 January 2018 / Revised: 26 February 2018 / Accepted: 28 February 2018 / Published: 8 March 2018
(This article belongs to the Special Issue Interlocked Molecules, Molecular Machines, Motors and Muscles)
Browse Figures
Versions Notes

Abstract

:
This review article presents our accomplished work on the synthesis of molecular triptycene wheels and their introduction into nanovehicles such as wheelbarrows and nanocars, equipped with two and four wheels, respectively. The architecture of nanovehicles is based on polycyclic aromatic hydrocarbons, which provide a potential cargo zone. Our strategy allowed us to obtain planar or curved nanocars, exhibiting different mobilities on metallic surfaces. Our curved nanocar participated in the first nanocar race organized in Toulouse (France) on 28 and 29 April 2017.

Graphical Abstract

1. Introduction

In 2013, in a perspective article on “molecule concept nanocars” [1], Christian Joachim and Gwénaël Rapenne proposed “a yearly competition whereby all nanocar designers would meet together for a few days, similar to the microrobotics contests held around the world.” It took almost four years to find a way to organize such a race, find sponsors, leave the time necessary for competitors to design and synthesize their prototypes, and develop a four-tip scanning tunneling microscope (STM) suitable to host the race. In 2017, six competitors from Austria, Germany, Japan, Switzerland, the United States, and France finally met in Toulouse (France) to compare their designs and strategies to speed up the movement of a single nanocar on a metallic surface. On the 28 April 2017, the starting signal was sounded at exactly 11 a.m. by Dr. Jean-Pierre Launay, emeritus Professor at the University Paul Sabatier (Toulouse) and race commissioner.
The Nanocar Race [2] was seen as a major communication event by the general public. In this review, we will describe why it was a highly challenging scientific event, which was selected to be a part of “Research of the Year 2017” by Chemical Engineering News [3], the scientific journal of the American Chemical Society, as well as the leading French newspaper Le Monde [4]. The last 15 years of research in our group will be detailed, from the design and synthesis of the first molecular wheelbarrow (a platform with two wheels), to the different prototypes of nanocars developed for the nanocompetition.
Nanovehicles are molecular machines able to move efficiently and with some kind of control and directionality at the nanoscale. The first prototypes were technomimetic [5], with a chassis connected to wheels. As pioneers in the field, we proposed using triptycenes [6] to act as rolling elements [7] and synthesized the first nanovehicle with two wheels—a wheelbarrow [8]. Two years after us, Tour’s group reported a family of nanovehicles consisting of a molecular-scale chassis with four [60]-fullerene wheels [9]. Various nanocars were subsequently synthesized by the same group using carboranes [10], ruthenium organometallic complexes [11], and adamantanes [12] as alternative wheels. During that time, we also proposed another wheel candidate, subphthalocyanin [13], which gave very good STM images with direct information about the rolling motion on a metallic surface [14], but unfortunately too unstable to be incorporated in nanovehicles. In the technomimetic family, Feringa et al. proposed a nanovehicle with four motors as wheels [15] and Masson and Hla designed and synthesized the largest car of about 3.5 nm in length. Officially called the Bobcat Nano-Wagon, it had a pseudorotaxane H-shaped frame with four cucurbituril molecules as wheels [16]. It must be noted that in the last example, there was no covalent bond linking the wheels and the axle, but instead a supramolecular charge-transfer interaction.
Like physics, which follows different laws at the nanoscale (quantum physics) as compared to the macroscopic world (Newtonian physics), the design of nanovehicles will not follow the same rules developed for vehicles that surround us in our everyday life. In this way, a new kind of nanovehicle design evolved at the nanoscale. Some nanocars were developed without wheels or motors, and were able to transform an electronic excitation into a controlled movement. Indeed, the teams from Germany, Japan, and Switzerland competed during the Nanocar Race with such nanovehicles. The Japanese team synthesized a molecule similar to a butterfly, consisting of a bisbinaphthyldurene, with two binaphthyl groups (the wings) connected to a central durene spacer [17]. The German team and the Swiss team selected commercially available molecules: 4-acetylbiphenyl [18] and 4′-(p-tolyl)-2,2′:6′,2′′-terpyridine [19], respectively. It must be noted that the German nanocar (“the Nano-Windmill”) was composed of four 4-acetylbiphenyl units self-assembled on the surface and stabilized by hydrogen bonds.
We present here our contribution to the field, from the synthesis of a molecular wheelbarrow, the first direct proof of the rolling motion of the wheels and their introduction into four-wheel nanovehicles, to our participation in the first Nanocar Race.

2. The First Two-Wheeled and Two-Legged Vehicle: The Molecular Wheelbarrow

The Toulouse team published the design for the first molecule-vehicle in 2002 [7], and it was synthesized in 2003. It was equipped with a chassis, two wheels at the front, two legs, and two handles at the rear, structurally similar to a wheelbarrow [8]. In the case of a macroscopic wheelbarrow, pushing results in the rotation of the wheels. The purpose of this first vehicle was thus to observe the rotational movement of the two front wheels while pushing on the handles and keeping the rear part of its chassis far from the surface, thanks to the two rear molecular legs.

2.1. Design

Wheelbarrow 1 consists of two legs (3,5-di-tert-butylphenyl groups, shown in green in Figure 1) and two three-cogged wheels (triptycene groups, shown in red in Figure 1), which can freely rotate around the axle thanks to the presence of ethynyl spacers [20]. As shown in Figure 1, the skeleton consists of polycyclic aromatic hydrocarbons (PAHs), which due to their rigidity make manipulation by the STM tip easy. As anticipated, the two 3,5-di-tert-butylphenyl legs were shown to be held in a conformation in which the phenyl groups are nearly perpendicular to the main aromatic board. This was exploited to lift the chassis, and thus to minimize its interaction with the surface. Moreover, tert-butyl groups connected to PAHs are used to increase organic solubility and are easily observed by STM techniques, inducing good contrast in the image. The two 4-tert-butylphenyl groups (in blue) play the role of handles for subsequent manipulation using the tip of the microscope.

2.2. Synthesis

The synthesis of the molecular wheelbarrow 1 was achieved in twelve steps, with an overall yield of 2% [21]. As shown in Scheme 1, our strategy used the repetition of a “double Knœvenagel condensation—Diels–Alder reaction” sequence on an α-diketo fragment. The first sequence allowed the connection of the two 3,5-di-tert-butylphenyl legs (Step a) and the handles (Step b), while the second one provided the precursor for the connection of the wheels (Steps d and e). Thus, 1,3-di(4-iodophenyl)propan-2-one was selected as partner in this last double Knoevenagel reaction to introduce the iodine centers necessary for the final double Sonogashira coupling, which yielded the molecular wheelbarrow (Step f).
The starting cyclopentadienone 4 was obtained first via a double Knœvenagel reaction of 1,3-bis(3,5-di-tert-butylphenyl)propan-2-one 2 with diketopyracene 3 (Step a). The Diels–Alder reaction of cyclopentadienone 4 with di-(4-tert-butylphenyl)acetylene (Step b) provided the ethane-bridged precursor 5 in 97% yield. The 1H-NMR spectrum clearly showed the expected 2:1 ratio between the different types of tert-butyl groups, belonging to the legs and to the handles, respectively. Oxidation of the ethane bridge of the pyracene fragment with benzeneseleninic anhydride (Step c) yielded the α-diketo fragment 6 necessary for the connection of the second axle. This is the key step in our strategy. Aryl halides are introduced at this stage for subsequent cross-couplings, in order to connect the triptycene wheels. The double Knoevenagel condensation with 1,3-di(4-iodophenyl)propan-2-one (Step d) followed by another Diels–Alder reaction with di(4-tolyl)acetylene provided the diiodo intermediate 8 in 30% yield (Step e). The two wheels were then simultaneously covalently attached to the axle via a double coupling of 9-ethynyltriptycene under classical Sonogashira conditions (Step f), affording the molecular wheelbarrow 1 in 55% yield.

2.3. Single Molecule Scanning Tunneling Microscopy Images and Manipulation

Such a molecular-scale machine inevitably displays a high level of complexity due to the incorporation of several functionalities within the same molecule. This complexity was reflected in the relatively large molecular weight of the wheelbarrow (1802 g·mol−1), which can often lead to problems in the deposition due to the possibility of thermal fragmentations during the sublimation step [22]. In the present case, the required linear wheel axle included two thermally-sensitive triple bonds. However, a few intact molecular wheelbarrows were successfully imaged on a Cu(100) surface, as shown in Figure 2. It leads to a rather complicated STM image, dominated by three intense maxima separated by various weaker patterns, as expected for such a complex chemical structure. The characteristic dimensions, the equivalency of different molecules in the STM images, and comparison with images calculated by electron scattering quantum chemistry (ESQC) method [23] indicated that intact molecular wheelbarrows had been imaged. Manipulation with the STM tip at 5 K resulted in a conformational change in the molecule, which unambiguously confirmed the molecularity of the observed object: the spots obtained were not an assembly of fragments.
Unfortunately, lateral motion of the wheelbarrow could not be achieved. This could be explained by the fact that two wheels may not be enough to allow the motion on the surface of such a large molecule, due to strong coupling. Increasing the number of wheels was proposed to enhance the molecular mobility of nanovehicles, and as a result the design of nanovehicles with four wheels was envisioned.

3. The First Rotation of Wheels on a Surface

Wheels are of course one of the key mechanical elements of a vehicle, even on a molecular chassis. At the macroscopic scale, the molecular wheels move the frame slightly away from the supporting surface, in order to lower the lateral diffusion barrier of the molecule-vehicle by reducing the frame–surface electronic interactions. Such decoupling might be achieved using simple molecular legs, although the movement of the molecule on the surface would then cost more energy, as it would require a tilting movement of each molecular leg. As in the macroscopic world, rotation around an axis is thus more energetically favorable.
It was shown that the mechanical motion of a single molecule on a surface can be triggered by the tip apex of the STM [24]. Pushing a molecule with an STM tip was a convenient way to probe the triptycene fragment to act as a wheel at the nanoscale. For that purpose, a prototype composed of two wheels linked to an axle was designed.

3.1. Synthesis and Deposition of a Bis(ethynyltriptycene) as Prototype of a Wheel Dimer

Copper(II)-mediated Glaser homocoupling of 9-ethynyltriptycene fragments—the wheels already used in the molecular wheelbarrow—gave the corresponding dimer of wheels linked via a butadiyne spacer. The latter was a good candidate, since it allowed almost free rotation of the attached fragments [20] in combination with a linear geometry. The ethynyltriptycene dimer has subsequently been studied as a prototype wheel dimer.
Its deposition on a Cu(110) surface was achieved very cleanly by sublimation under high vacuum [25]. Figure 3 shows the image obtained; each bright lobe corresponds to one triptycene unit, and the observed pair of lobes constitutes the image of a dimer, as confirmed by calculations. No fragmentation or decomposition was observed.

3.2. Unidirectional Rotation of the Wheel

For the first time, it was possible to observe the rotation of a wheel on a surface, by working at 5 K under ultra-high vacuum. This was achieved by inducing the translation of the molecule upon pushing it with the STM tip [25]. In order to understand the motion of this molecule in detail, it was particularly important to study the manipulation signal (i.e., the tunneling current recorded at constant tip height during the motion), because the STM images before and after manipulation did not give information about the type of movement between measurements (translational or rotational).
The tip was moved across the molecular axle at a constant height, while the tunneling current was recorded. In most cases, it was possible to rotate one wheel, and in a few cases, the rolling of both wheels was observed (as shown in Figure 4). This behavior seems to depend on the precise shape of the tip apex, which in some cases allowed us to address both wheels during the manipulation. This triptycene dimer was the first molecule designed to yield a controlled rotation upon pushing the wheels using the STM tip. With this rolling motion proven, four triptycene units were then integrated into the next generation of nanovehicles, with the aim of increasing mobility on the surface.

4. A Planar Nanocar

For the preparation of nanovehicles containing four wheels (i.e., nanocars), it was necessary to develop the synthesis of a larger chassis based on a perylene unit. This was to sterically accommodate all the wheels on the same molecular structure [26], as the chassis used for molecular wheelbarrow 1 was too short. Therefore, as shown in Scheme 2, our strategy started with the synthesis of di(4-iodophenyl)cyclopentadienone 11 via a double Knœvenagel reaction between acenaphthenequinone 9 and 1,3-di(4-iodophenyl)propan-2-one 10 under basic conditions (Step a). Diels–Alder reaction with 1,2-di(3,5-di-tert-butylphenyl)ethyne gave—after aromatization—the half-chassis 12 along with evolution of carbon monoxide (Step b). The half-chassis 12 was subsequently dimerized by using a Scholl-type oxidative coupling with FeCl3 as oxidant (Step c). In the last step, the resulting planar chassis 13 was functionalized with four ethynyltriptycenyl wheels via Sonogashira cross-couplings to yield our first prototype nanocar 14 in 9% overall yield.
This nanovehicle was deposited on Au(111). However, due to its planarity and the resulting high interaction of the polyaromatic chassis with the surface, it was not possible to move the vehicle. Thus, we envisioned the design of an alternative molecule-car with a modified chassis, which would undergo less surface coupling.

5. A Curved Nanocar

To decrease the interaction of the polyaromatic chassis with the surface, a highly curved chassis was prepared. The synthetic strategy remained identical, but the 3,5-di-tert-butylphenyl fragments positioned at both ends were substituted with 4-tert-butylphenyl groups [26]. In this case, planarity of contiguous phenyl rings was more easily achieved and dimerization of the half-chassis 16 under Scholl oxidative conditions led to an overcyclized perylene platform bearing six additional C-C bonds, as shown in blue (highlighted in bold) in Scheme 3.
The last step consisted of connecting the four triptycene wheels via a quadruple Sonogashira coupling to give the corresponding nanovehicle 17 in 34% yield. Geometric optimization of this second-generation nanovehicle showed that this overcyclized chassis has a curved shape at both ends (Figure 5b). As with fullerenes, this geometry can be explained by the presence of alternating five- and six-membered rings in the polycyclic aromatic hydrocarbon platform. The two five-membered rings are shown in red in Scheme 3. This specificity is of great interest, since it provides an appropriate shape to act as an efficient cargo zone.
The planar and curved nanovehicles have very large differences in their solubilities and their spectroscopic properties. For instance, the color of the planar molecule is pink, while the curved one is dark green; hence, it was called “the green buggy”.

6. Participation in the First Nanocar Race: The View from the French Team

On 28 and 29 April 2017, six teams from three continents met in Toulouse to compete with their molecular racers. Both families of nanocars—the technomimetic models incorporating wheels (from Austria, France and the USA) and the smaller and lighter models lacking wheels (from Germany, Japan and Switzerland)—entered the competition [27]. Since the ultra-high-vacuum-low temperature (UHV-LT) STM instrument at Centre d’Elaboration de Matériaux et d'Etudes Structurales (CEMES-CNRS) in Toulouse employs only four tips, four nanocars competed using this microscope. Thus, the Ohio team and the Rice–Graz team were sitting in the same room as the other teams but were remotely piloting their own nanocar, deposited in the STM located at their home university. This presented a further challenge to control a nanocar at the atomic scale from half the world away.
Except for the Rice–Graz team who competed on a silver track, the other nanocars were on gold. The latter surface was originally designated as the common surface for the race, and this was why the official ranking contains two winners, one on gold and one on silver. Each track was 100 nm long and included at least two turns.

6.1. Deposition and Imaging of the French Nanocar

The French nanocar had the advantage of being very robust. It was deposited by sublimation, as with the other nanocars, and was identified on the surface as a long 3 nm molecule. As shown in Figure 6, the triptycene wheels appear as very bright spots when compared with the central polyaromatic core.

6.2. The Race and the Official Ranking

On 29 April at 5:00 p.m., after two days and one night of intense efforts, the first ever international nanocar race ended. As mentioned, two teams were ranked first: the Swiss team, racing on Au(111), as stated in the original rules [28] and the Rice–Graz team, racing on Ag(111), since their nanocar appeared to move uncontrollably fast on gold. On Au(111) with the lightest nanocar of the competition (only 42 atoms), the Swiss team arrived first, with a distance of 100 nm covered in six hours [29]. The US team (Ohio) arrived second, with a distance of 43 nm covered. Their nanocar—the Bobcat Nano-wagon—was the largest to participate, with about 650 atoms. Finally, the Nano-Windmill piloted by the German team (Dresden) covered a distance of 11 nm. On Ag(111), the dipolar racer (which consists of one axle with two wheels) was very fast, with a distance of 1000 nm covered in only 29 h [30] but without competitors, since the others competed on Au(111). The characteristics of each team are given in Table 1.
We targeted two strategies to move our nanocar directionally; first, we tried pulling the molecule on the surface, as pushing was forbidden in the rules. The second strategy was to find a way for an electronic excitation to induce the movement. Unfortunately, due to the limited time available both in training and during the race, this propulsion mode failed to drive our nanocar. Only our first strategy was effective, and pulling the molecule with the STM tip allowed us to cover an impressive distance of 25 nm in 3 s. However, we were disqualified from the race as the jury decided not to recognize movement by pulling. We are very satisfied to have participated in the first nanocar race; remembering the motto from the creator of the modern Olympic games, Pierre de Coubertin, which emphasizes that “the importance is to participate”. Moreover, for the first time, we were able to climb a step edge.
We received the “prize of elegance” due to the very smart STM images of our Green Buggy recorded during the race. The Japanese team was not ranked either, as their nanovehicle was unable to recover from a software crash, just one hour into the race. This team was awarded the “fair play” prize.

7. Conclusions and Perspectives

In summary, we have presented the design and synthesis of polyaromatic hydrocarbons conceived by analogy with macroscopic wheels, wheelbarrows, and nanocars. Concerning the nanocar race, we had confirmation that the smallest molecules completed the track distance first (the Swiss molecule-car had only 42 atoms and is commercially available). This is partly because smaller was better for easily and rapidly moving on the surface.
The first nanocar race was a real success, with a worldwide audience following the event on the internet, broadcasted live, night and day, with more than 100,000 viewers at peak times. We now have experience in organizing such an event, which may have a second edition around 2021. All the competitors went home with new ideas that will make them more competitive next time, and we can assume that new participants will enter. One could imagine organizing semi-finals, test selections to qualify for the final or to run the race at a higher temperature, in order to have a faster event. It has already been shown that control of motion is possible at higher temperatures on some semi-conductive surfaces, such as SmSi [31,32] or SiB [33]. Furthermore, the question of whether we need to create different categories will be addressed, in order to give everybody the same chance (e.g., dividing the nanovehicles by the number of atoms or by the molecular mass). We could also organize a different race, for example, moving the nanocar with cargo on its backbone. This would be similar to the “waiter’s race” (“course de garçons de café” in French) created in Paris (France), which tests the speed of a waiter carrying a loaded tray without tipping it over [34].

Acknowledgments

This work was supported by the CNRS, the Université Paul Sabatier (Toulouse), the European Union and the ANR (ACTION project n8 ANR 15-CE29-0005). All the official sponsors of the Nanocar race are also aknowledged, the full list appears on our website http://nanocar-race.cnrs.fr/. We are also grateful to the researchers who participated in all the work discussed here and whose names appear in the references, and in particular the talented Ph.D. and Post-doctoral students who achieved the synthesis of these systems: Romain Garbage, Agnès Sirven, and Gorka Jimenez-Bueno, as well as Francesca Moresco, Leonhard Grill, Sébastien Gauthier, Corentin Durand, Olivier Guillermet and We-Hyo Soe for STM studies, and Christian Joachim and Xavier Bouju for calculations. Colin Martin is also warmly aknowledged for his careful reading and improving of our manuscript.

Conflicts of Interest

The authors declare no conflict of interest. The founding sponsors had no role in the design of the study; in the collection, analyses, or interpretation of data; in the writing of the manuscript, and in the decision to publish the results.

References and Notes

  1. Joachim, C.; Rapenne, G. Molecule concept nanocars: Chassis, wheels and motors? ACS Nano 2013, 7, 11–14. [Google Scholar] [CrossRef] [PubMed]
  2. Nanocar Race Official Website. Available online: http://nanocar-race.cnrs.fr/indexEnglish.php (accessed on 7 January 2018).
  3. Research of the Year 2017. Chemical Engineering News. 18 December 2017. Available online: https://cen.acs.org/articles/95/i49/chemistry-research-of-the-year-2017.html (accessed on 7 January 2018).
  4. 2017, Une Année de Sciences en Images. Le Monde. Available online: http://www.lemonde.fr/sciences/portfolio/2017/12/26/2017-une-annee-de-sciences-en-images_5234475_1650684.html (accessed on 7 January 2018).
  5. Rapenne, G. Synthesis of technomimetic molecules: Towards rotation control in single molecular machines and motors. Org. Biomol. Chem. 2005, 3, 1165–1169. [Google Scholar] [CrossRef] [PubMed]
  6. Chen, C.F.; Ma, Y.X. Iptycenes Chemistry from Synthesis to Applications; Springer-Verlag: Berlin/Heidelberg, Germany, 2013. [Google Scholar] [CrossRef]
  7. Joachim, C.; Moresco, F.; Rapenne, G.; Meyer, G. The design of a nanoscale molecular barrow. Nanotechnology 2002, 13, 330–335. [Google Scholar] [CrossRef]
  8. Jimenez-Bueno, G.; Rapenne, G. Technomimetic molecules: Synthesis of a molecular wheelbarrow. Tetrahedron Lett. 2003, 44, 6261–6263. [Google Scholar] [CrossRef]
  9. Shirai, Y.; Osgood, A.J.; Zhao, Y.; Kelly, K.F.; Tour, J.M. Directional control in thermally driven single-molecule nanocars. Nano Lett. 2005, 5, 2330–2334. [Google Scholar] [CrossRef] [PubMed]
  10. Morin, J.-F.; Sasaki, T.; Shirai, Y.; Guerrero, J.M.; Tour, J.M. Synthetic Routes toward Carborane-Wheeled Nanocars. J. Org. Chem. 2007, 72, 9481–9490. [Google Scholar] [CrossRef] [PubMed]
  11. Vives, G.; Tour, J.M. Synthesis of a Nanocar with Organometallic Wheels. Tetrahedron Lett. 2009, 50, 1427–1430. [Google Scholar] [CrossRef]
  12. Chu, P.L.E.; Wang, L.Y.; Khatua, S.; Kolomeisky, A.B.; Link, S.; Tour, J.M. Synthesis and Single-Molecule Imaging of Highly Mobile Adamantane-Wheeled Nanocars. ACS Nano 2013, 7, 35–41. [Google Scholar] [CrossRef] [PubMed]
  13. Jacquot de Rouville, H.P.; Garbage, R.; Ample, F.; Nickel, A.; Meyer, J.; Moresco, F.; Joachim, C.; Rapenne, G. Synthesis and STM imaging of symmetric and dissymmetric ethynyl-bridged dimers of boron-subphthalocyanine bowl-shaped nano-wheels. Chem. Eur. J. 2012, 18, 8925–8928. [Google Scholar] [CrossRef] [PubMed]
  14. Nickel, A.; Meyer, J.; Ohmann, R.; Jacquot de Rouville, H.-P.; Rapenne, G.; Joachim, C.; Cuniberti, G.; Moresco, F. STM manipulation of boron-subphthalocyanine nano-wheel dimers on Au(111). J. Phys. Condens. Matter 2012, 24, 404001. [Google Scholar] [CrossRef] [PubMed]
  15. Kudernac, T.; Ruangsupapichat, N.; Parschau, M.; Maci, B.; Katsonis, N.; Harutyunyan, S.R.; Ernst, K.H.; Feringa, B.L. Electrically driven directional motion of a four-wheeled molecule on a metal surface. Nature 2011, 479, 208–211. [Google Scholar] [CrossRef] [PubMed]
  16. Kotturi, K.; Raeisi, M.; Latt, K.Z.; Zhang, Y.; Perumal, K.; Rabbani, R.; Sarkar, S.; Li, Y.; Hla, S.-W.; Masson, E. Anatomy of a Supramolecular Nanowagon. In preparation.
  17. Soe, W.H.; Shirai, Y.; Durand, C.; Yonamine, Y.; Minami, K.; Bouju, X.; Kolmer, M.; Ariga, K.; Joachim, C.; Nakanishi, W. Conformation Manipulation and Motion of a Double Paddle Molecule on an Au(111) Surface. ACS Nano 2017, 11, 10357–10365. [Google Scholar] [CrossRef] [PubMed]
  18. Durand, C.; Moresco, F.; Launay, J.P.; Joachim, C. Training for the 1st international nano-car race: The Dresden molecule-vehicle. Eur. Phys. J. Appl. Phys. 2016, 76, 10001. [Google Scholar] [CrossRef]
  19. Pawlak, R.; Meier, T.; Renaud, N.; Kisiel, M.; Hinaut, A.; Glatzel, T.; Sordes, D.; Durand, C.; Soe, W.H.; Baratoff, A.; et al. Design and Characterization of an Electrically Powered Single Molecule on Gold. ACS Nano 2017, 11, 9930–9940. [Google Scholar] [CrossRef] [PubMed]
  20. Toyota, S. Rotational isomerism involving acetylene carbon. Chem. Rev. 2010, 110, 5398–5424. [Google Scholar] [CrossRef] [PubMed]
  21. Rapenne, G.; Jimenez-Bueno, G. Molecular machines: Synthesis and characterization of two prototypes of molecular wheelbarrows. Tetrahedron 2007, 63, 7018–7026. [Google Scholar] [CrossRef]
  22. Rapenne, G.; Grill, L.; Zambelli, T.; Stojkovic, S.; Ample, F.; Moresco, F.; Joachim, C. Launching and landing single molecular wheelbarrows on a Cu (100) surface. Chem. Phys. Lett. 2006, 431, 219–222. [Google Scholar] [CrossRef]
  23. Grill, L.; Rieder, K.H.; Moresco, F.; Jimenez-Bueno, G.; Wang, C.; Rapenne, G.; Joachim, C. Imaging of a molecular wheelbarrow by scanning tunneling microscopy. Surf. Sci. 2005, 584, 153–158. [Google Scholar] [CrossRef]
  24. For early examples of mechanically-induced motions of molecules, see: Moresco, F.; Meyer, G.; Rieder, K.-H.; Tang, H.; Gourdon, A.; Joachim, A. Low temperature manipulation of big molecules in constant height mode. Appl. Phys. Lett. 2001, 78, 306–308. [Google Scholar], doi:10.1063/1.1339251 and the references cited.
  25. Grill, L.; Rieder, K.H.; Moresco, F.; Rapenne, G.; Stojkovic, S.; Bouju, X.; Joachim, C. Rolling a single molecular wheel at the atomic scale. Nat. Nanotechnol. 2007, 2, 95–98. [Google Scholar] [CrossRef] [PubMed]
  26. Jacquot de Rouville, H.P.; Garbage, R.; Cook, R.E.; Pujol, A.R.; Sirven, A.M.; Rapenne, G. Synthesis of polycyclic aromatic hydrocarbon-based nanovehicles equipped with triptycene wheels. Chem. Eur. J. 2012, 18, 3023–3031. [Google Scholar] [CrossRef] [PubMed]
  27. Rapenne, G.; Joachim, C. The first nanocar race. Nat. Rev. Mater. 2017, 2, 17040. [Google Scholar] [CrossRef]
  28. The rules of the Nanocar Race have been published in: Joachim, C.; Durand, C.; Launay, J.-P.; Rapenne, G.; Kammerer, C.; Jacquot de Rouville, H.-P.; Garbage, R.; Martrou, D.; Soe, W.-H.; Gauthier, S.; et al. The NanoCar Race: The First International Molecule-Cars Race. L’actualité Chimique. October 2016, n°411, Page V. It is mentioned that the race will take place on a small portion of Au (111) and that the nanocar must present a chemical structure of minimum 100 atoms.
  29. Pawlak, R.; Meier, T. Fast and curious. Nat. Nanotechnol. 2017, 12, 712. [Google Scholar] [CrossRef] [PubMed]
  30. Simpson, G.J.; García-López, V.; Petermeier, P.; Grill, L.; Tour, J.M. How to Build and Race a Fast Nanocar. Nat. Nanotechnol. 2017, 12, 604–606. [Google Scholar] [CrossRef] [PubMed]
  31. Makoudi, Y.; Duverger, E.; Arab, M.; Chérioux, F.; Ample, F.; Rapenne, G.; Bouju, X.; Palmino, F. Room temperature electronic template effect of the Sm/Si(111)-8x2 interface for self-alignment of organic molecules. Chem. Phys. Chem. 2008, 9, 1437–1441. [Google Scholar] [CrossRef] [PubMed] [Green Version]
  32. Bouju, X.; Chérioux, F.; Coget, S.; Rapenne, G.; Palmino, F. Directional molecular sliding at room temperature on a silicon runway. Nanoscale 2013, 5, 7005–7010. [Google Scholar] [CrossRef] [PubMed]
  33. Chérioux, F.; Palmino, F.; Galangau, O.; Rapenne, G. Controlled directional motions of molecular vehicles, rotors and motors: From metallic to silicon surfaces, a strategy to operate at higher temperature. Chem. Phys. Chem. 2016, 1742–1751. [Google Scholar] [CrossRef] [PubMed]
  34. “Course des Garçons de Café” (Waiter’s Race) Wikipedia Webpage. Available online: https://en.wikipedia.org/wiki/Waiters%27_Race (accessed on 7 January 2018).
Molecules 23 00612 g001 550
Figure 1. Macroscopic wheelbarrow (left), chemical structure of the molecular analogue 1 (center), and space-filling model showing its minimum energy conformation (right).
Figure 1. Macroscopic wheelbarrow (left), chemical structure of the molecular analogue 1 (center), and space-filling model showing its minimum energy conformation (right).
Molecules 23 00612 g001
Molecules 23 00612 sch001 550
Scheme 1. Synthesis of molecular wheelbarrow 1: reagents and conditions: (a) KOH, EtOH, 20 h, Ar, 20 °C; (b) di(4-tert-butylphenyl)acetylene, diphenylether, 16 h, Ar, reflux; (c) (C6H5SeO)2O, chlorobenzene, 62 h, Ar, reflux; (d) 1,3-bis(4-iodophenyl)propan-2-one, KOH, EtOH, Ar, reflux; (e) di(4-tolyl)acetylene, diphenylether, 16 h, Ar, reflux; (f) 9-ethynyltriptycene, Pd(PPh3)4 10 mol %, CuI 20 mol %, piperidine-THF (1:1), 24 h, Ar, 20 °C.
Scheme 1. Synthesis of molecular wheelbarrow 1: reagents and conditions: (a) KOH, EtOH, 20 h, Ar, 20 °C; (b) di(4-tert-butylphenyl)acetylene, diphenylether, 16 h, Ar, reflux; (c) (C6H5SeO)2O, chlorobenzene, 62 h, Ar, reflux; (d) 1,3-bis(4-iodophenyl)propan-2-one, KOH, EtOH, Ar, reflux; (e) di(4-tolyl)acetylene, diphenylether, 16 h, Ar, reflux; (f) 9-ethynyltriptycene, Pd(PPh3)4 10 mol %, CuI 20 mol %, piperidine-THF (1:1), 24 h, Ar, 20 °C.
Molecules 23 00612 sch001
Molecules 23 00612 g002 550
Figure 2. Experimental scanning tunneling microscope (STM) image (3 × 4 nm2, V = 0.5 V, I = 0.3 nA) on Cu(100) at 5 K (a) and the molecular conformation (c) corresponding to the electron scattering quantum chemistry (ESQC) calculated image (b).
Figure 2. Experimental scanning tunneling microscope (STM) image (3 × 4 nm2, V = 0.5 V, I = 0.3 nA) on Cu(100) at 5 K (a) and the molecular conformation (c) corresponding to the electron scattering quantum chemistry (ESQC) calculated image (b).
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Molecules 23 00612 g003 550
Figure 3. (a) Experimental STM image of a wheel dimer on a Cu(110) surface (30 × 30 Å2, V = 1 V, I = 0.2 nA) and (c) the molecular configuration corresponding to (b) the calculated STM image. Adapted from [22], copyright 2006, with permission from Elsevier.
Figure 3. (a) Experimental STM image of a wheel dimer on a Cu(110) surface (30 × 30 Å2, V = 1 V, I = 0.2 nA) and (c) the molecular configuration corresponding to (b) the calculated STM image. Adapted from [22], copyright 2006, with permission from Elsevier.
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Molecules 23 00612 g004 550
Figure 4. Rotational motion of triptycene wheels. Step 1: the STM tip approaches the molecule; Step 2: the rotation of the wheel starts; Step 3: the STM tip lies on the other side of the wheel after a 120° rotation. Adapted from [25], copyright 2007, with permission from Springer Nature.
Figure 4. Rotational motion of triptycene wheels. Step 1: the STM tip approaches the molecule; Step 2: the rotation of the wheel starts; Step 3: the STM tip lies on the other side of the wheel after a 120° rotation. Adapted from [25], copyright 2007, with permission from Springer Nature.
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Molecules 23 00612 sch002 550
Scheme 2. Synthesis of the planar nanocar 14. (a) KOH, MeOH, 2 h, Ar, room temperature (RT); (b) 1,2-bis(3,5-di-tert-butylphenyl)ethyne, diphenylether, 45 min, 250 °C, microwave (300 W); (c) FeCl3 25 eq, CH2Cl2–CH3NO2 (9:1), 15 min, Ar, RT; (d) 9-ethynyltriptycene 10 eq, Pd(PPh3)4 10 mol%, CuI 20 mol%, piperidine-THF (1:1), 6 h, Ar, 80 °C.
Scheme 2. Synthesis of the planar nanocar 14. (a) KOH, MeOH, 2 h, Ar, room temperature (RT); (b) 1,2-bis(3,5-di-tert-butylphenyl)ethyne, diphenylether, 45 min, 250 °C, microwave (300 W); (c) FeCl3 25 eq, CH2Cl2–CH3NO2 (9:1), 15 min, Ar, RT; (d) 9-ethynyltriptycene 10 eq, Pd(PPh3)4 10 mol%, CuI 20 mol%, piperidine-THF (1:1), 6 h, Ar, 80 °C.
Molecules 23 00612 sch002
Molecules 23 00612 sch003 550
Scheme 3. Synthesis of a new curved polyaromatic platform. (a) Diphenylether, 45 min, 260 °C, MW (300 W); (b) FeCl3 25 eq, CH2Cl2/CH3NO2 (9:1), 15 min, Ar, RT; (c) 9-ethynyltriptycene 8 eq, Pd(PPh3)4 10 mol %, CuI 20 mol %, piperidine/THF (1:1), 6 h, Ar, 80 °C. The additional carbon-carbon bonds obtained in the oxidative coupling are in blue and highlighted in bold, and the cyclopentadiene fragments inducing the curvature are shown in red.
Scheme 3. Synthesis of a new curved polyaromatic platform. (a) Diphenylether, 45 min, 260 °C, MW (300 W); (b) FeCl3 25 eq, CH2Cl2/CH3NO2 (9:1), 15 min, Ar, RT; (c) 9-ethynyltriptycene 8 eq, Pd(PPh3)4 10 mol %, CuI 20 mol %, piperidine/THF (1:1), 6 h, Ar, 80 °C. The additional carbon-carbon bonds obtained in the oxidative coupling are in blue and highlighted in bold, and the cyclopentadiene fragments inducing the curvature are shown in red.
Molecules 23 00612 sch003
Molecules 23 00612 g005 550
Figure 5. (a) CPK (Corey–Pauling–Koltun) model of the nanocar 14 with a planar chassis and (b) side view of the optimized geometry of the nanocar 17 with its highly-curved chassis.
Figure 5. (a) CPK (Corey–Pauling–Koltun) model of the nanocar 14 with a planar chassis and (b) side view of the optimized geometry of the nanocar 17 with its highly-curved chassis.
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Figure 6. Image of the curved nanocar 17 on Au(111). The four bright spots correspond to the four triptycene wheels (U = 1.1 V, I = 5 pA). Scale bar: 1 nm.
Figure 6. Image of the curved nanocar 17 on Au(111). The four bright spots correspond to the four triptycene wheels (U = 1.1 V, I = 5 pA). Scale bar: 1 nm.
Molecules 23 00612 g006
Table
Table 1. The six registered participants and their respective nanocars, with their characteristic parameters: country, team leader, landing surface, and number of atoms of their nanovehicle (with the corresponding chemical formula). In red, the parameters outside of the original rules [28] but accepted by the jury.
Table 1. The six registered participants and their respective nanocars, with their characteristic parameters: country, team leader, landing surface, and number of atoms of their nanovehicle (with the corresponding chemical formula). In red, the parameters outside of the original rules [28] but accepted by the jury.
Molecules 23 00612 i001 Molecules 23 00612 i002 Molecules 23 00612 i003 Molecules 23 00612 i004 Molecules 23 00612 i005 Molecules 23 00612 i006
MANA NIMSNano DragsterNano-WagonDipolar RacerNano-WindmillGreen Buggy
CountryJapanSwitzerlandUSAAustria & USAGermanyFrance
Team leaderWaka NakanichiRémy
Pawlack		Saw Wai Hla & Eric MassonLeonhard Grill & James TourFrancesca MorescoGwénaël Rapenne
SurfaceAu(111)Au(111)Au(111)Ag(111)Au(111)Au(111)
Number of atoms88 atoms
(C50H34O4)		42 atoms (C22H17N3)642 atoms
(C244H222N120056)		72 atoms (C32H36N2O2)108 atoms
(C56H48O4)		300 atoms
(C184H116)

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Jacquot de Rouville, H.-P.; Kammerer, C.; Rapenne, G. From the Synthesis of Nanovehicles to Participation in the First Nanocar Race—View from the French Team. Molecules 2018, 23, 612. https://doi.org/10.3390/molecules23030612

AMA Style

Jacquot de Rouville H-P, Kammerer C, Rapenne G. From the Synthesis of Nanovehicles to Participation in the First Nanocar Race—View from the French Team. Molecules. 2018; 23(3):612. https://doi.org/10.3390/molecules23030612

Chicago/Turabian Style

Jacquot de Rouville, Henri-Pierre, Claire Kammerer, and Gwénaël Rapenne. 2018. "From the Synthesis of Nanovehicles to Participation in the First Nanocar Race—View from the French Team" Molecules 23, no. 3: 612. https://doi.org/10.3390/molecules23030612

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