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(a–d) The STM images of four types of melem hexamers which have been observed within the porous nanostructure, where the brighter ones are indicated by the green dashed ellipses. (e–h) The STM images (a)–(d) and their corresponding DFT-optimized structural models are superimposed. (i–l) The charge density difference maps of the corresponding STM images, where red and blue isosurfaces indicate charge accumulation and depletion, respectively (an isosurface value of 0.016 e Å À3 ). 

(a–d) The STM images of four types of melem hexamers which have been observed within the porous nanostructure, where the brighter ones are indicated by the green dashed ellipses. (e–h) The STM images (a)–(d) and their corresponding DFT-optimized structural models are superimposed. (i–l) The charge density difference maps of the corresponding STM images, where red and blue isosurfaces indicate charge accumulation and depletion, respectively (an isosurface value of 0.016 e Å À3 ). 

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We studied the self-assembly of melem on the Au(111) and Ag(111) surface. By scanning tunneling microscopy imaging, we have observed two different STM appearances of the melem molecule within the self-assembled nanostructure on Au(111), which are resulted from the different intermolecular bonding configurations. Moreover, further DFT details includ...

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... calculations of the two motifs on the Au(111) surface (Fig. S1, ESI †), and the two models stand out as shown in Fig. 1c and d. Both of the melem molecules in the two motifs adopt a flat-lying geometry with a similar height in Fig. 1e and f. In addition, we have not reproduced the different contrasts from their Tersoff-Hamann STM simulations in Fig. S2 (ESI †), where the top figure shows experimental data and the bottom figure (showing no difference in contrast) shows simulated data. Their flat geometries imply that hydrogen-bonded inter- molecular interaction among melem molecules determines the formation of the observed melem network, whereas the surface serves primarily as a ...
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... addition, we could divide the porous structure into hexamers which consist of six melem molecules to further analyze the porous structure. As shown in the STM images of Fig. 2, we find four different hexamer structures. One is formed exclusively by the dim melem, i.e., Motif-1 ( Fig. 2a and e). One is composed of four dim molecules and a pair of bright dimers (Fig. 2b and f). One is composed of two dim molecules and two pairs of bright dimers at the opposite position ( Fig. 2c and g). And the other is ...
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... addition, we could divide the porous structure into hexamers which consist of six melem molecules to further analyze the porous structure. As shown in the STM images of Fig. 2, we find four different hexamer structures. One is formed exclusively by the dim melem, i.e., Motif-1 ( Fig. 2a and e). One is composed of four dim molecules and a pair of bright dimers (Fig. 2b and f). One is composed of two dim molecules and two pairs of bright dimers at the opposite position ( Fig. 2c and g). And the other is composed of two dim molecules and two pairs of bright dimers at the neighboring position ( Fig. 2d and h). In the last case, ...
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... could divide the porous structure into hexamers which consist of six melem molecules to further analyze the porous structure. As shown in the STM images of Fig. 2, we find four different hexamer structures. One is formed exclusively by the dim melem, i.e., Motif-1 ( Fig. 2a and e). One is composed of four dim molecules and a pair of bright dimers (Fig. 2b and f). One is composed of two dim molecules and two pairs of bright dimers at the opposite position ( Fig. 2c and g). And the other is composed of two dim molecules and two pairs of bright dimers at the neighboring position ( Fig. 2d and h). In the last case, the interaction between two Motif-2 units is in a staggered form as that of ...
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... structure. As shown in the STM images of Fig. 2, we find four different hexamer structures. One is formed exclusively by the dim melem, i.e., Motif-1 ( Fig. 2a and e). One is composed of four dim molecules and a pair of bright dimers (Fig. 2b and f). One is composed of two dim molecules and two pairs of bright dimers at the opposite position ( Fig. 2c and g). And the other is composed of two dim molecules and two pairs of bright dimers at the neighboring position ( Fig. 2d and h). In the last case, the interaction between two Motif-2 units is in a staggered form as that of Motif-1. Based on these STM images, we performed the corresponding DFT calculations for the four hexamer structures ...
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... the dim melem, i.e., Motif-1 ( Fig. 2a and e). One is composed of four dim molecules and a pair of bright dimers (Fig. 2b and f). One is composed of two dim molecules and two pairs of bright dimers at the opposite position ( Fig. 2c and g). And the other is composed of two dim molecules and two pairs of bright dimers at the neighboring position ( Fig. 2d and h). In the last case, the interaction between two Motif-2 units is in a staggered form as that of Motif-1. Based on these STM images, we performed the corresponding DFT calculations for the four hexamer structures in the gas phase. The optimized structural models are superimposed on the relative STM images in Fig. 2e-h, and a good ...
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... neighboring position ( Fig. 2d and h). In the last case, the interaction between two Motif-2 units is in a staggered form as that of Motif-1. Based on these STM images, we performed the corresponding DFT calculations for the four hexamer structures in the gas phase. The optimized structural models are superimposed on the relative STM images in Fig. 2e-h, and a good agreement is achieved in all cases. Moreover, we also performed DFT calculations of the charge density difference maps of the four hexamer structures in the gas phase as shown in Fig. 2i-l, which clearly illustrate the cyclic double hydrogen bonds between the amino groups and heptazine ...
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... DFT calculations for the four hexamer structures in the gas phase. The optimized structural models are superimposed on the relative STM images in Fig. 2e-h, and a good agreement is achieved in all cases. Moreover, we also performed DFT calculations of the charge density difference maps of the four hexamer structures in the gas phase as shown in Fig. 2i-l, which clearly illustrate the cyclic double hydrogen bonds between the amino groups and heptazine ...

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... Unsupported H-Bonded Networks. As shown in previous STM studies, [20][21][22]39 melem molecules adsorb planar on surfaces like Au(111) and Ag(111) forming a variety of different, mostly coexisting, hydrogen-bonded networks. All structures feature two basic intermolecular H-bond patterns, which are usually denoted as side-by-side (SS) and head-to-tail (HT) (see Figure 1 panels a and b, respectively). ...
... It means that the molecules can assemble to well-organized structures spontaneously without the assistance of external forces. The internal driving force between the molecules to form self-assembly structures derives mainly from intermolecular interactions, such as van der Waals interactions[156][157][158][159] , hydrogen bonding[160][161][162] , halogen bonding[163][164][165] , π-π staking 166,167 , dipole-dipole interactions168,169 , or coordination bonding170,171 . In addition, external stimuli such as heat172,173 , light174,175 , electric fields156,176,177 and even the molecule-substrate interactions[178][179][180] play pivotal roles in switching the self-assembly structures from one type to another, providing practical approaches towards designing and tuning functional molecular structures. ...
Thesis
Metal oxides hold promise for the development of future organic electronics and low-cost, high-efficient heterogeneous catalysts due to their wide range of crystallographic, electronic and magnetic structures. As the size of today’s electronic devices reaches the nanometer scale, and as interest has grown in establishing the catalytic mechanisms of metal oxide catalysts, the interface interactions between metal oxides and adsorbates are at the focus of current research. Likewise, functionalization of surfaces by organic molecules has been an important topic during the last two decades. Especially the potential arising from new macromolecular structures on surfaces created by self-assembly has triggered a lot of research. While this area of research is relatively mature when it comes to adsorption and self-assembly on metal surfaces, studies on oxide surfaces are still rare. This thesis aims at performing fundamental, comparative studies of the adsorption of large organic molecules on cobalt oxides and copper by using scanning tunneling microscopy (STM), in order to gain a fundamental understanding of the adsorption behavior, such as the adsorption geometry of the molecules, the interactions between the molecules and the substrate surfaces, and possible on-surface reactions. By this, the similarities of and differences between the adsorption of molecules on metal and metal oxide surfaces are revealed. The results will open a door towards designing and fabricating functional molecular nanostructures on metal oxide surfaces. Therefore, an important aspect of this thesis is to study the adsorption properties of porphyrin molecules on the Cu(111) surface to set the appropriate basis for a comparison. The adsorption geometry of free-base and cobalt metalated 5,15-diphenylporphyrin (2H-DPP and Co-DPP) are studied by scanning tunneling microscopy and density functional theory. The self-assembly structures as a function of molecular coverage are subsequently explored. Both the 2H- and Co-DPP exhibit chirality on the surface that derives from the saddle shape distortion of the molecules. It is shown that and how such a molecular chirality transfers to self-assembly structures. The self-assembly structures of 2H-DPP are independent of the molecular coverage. Conversely, the Co-DPP is more mobile on the copper surface, which allows structural phase transitions as function of molecular coverage. The molecule-molecule and the molecule-substrate interactions play important roles in the transition of Co-DPP self-assembly structures from chirally separated, enantiopure to racemic networks as the molecular coverage increases. On-surface reactions of DPP molecules on a metal substrate is another important aspect that is discussed in this thesis. By using unfunctionalized 2H-DPP molecules, the possible mechanism of their intramolecular dehydrogenative coupling is revealed. The reaction products further act as precursors for the subsequent intermolecular organometallic and dehydrogenative coupling. The competition between these two on-surface reactions is studied as a function of sample temperature, annealing time, molecular coverage and molecular geometries. The last aspect in this thesis is to study the adsorption of 2H-DPP and Co-DPP molecules on rock salt and spinel type cobalt oxide films, which are epitaxially grown on Ir(100). On rock salt type cobalt oxide films of ~2.6nm (~11BL) thickness, both 2H-DPP and Co-DPP are weakly adsorbed due to the π-anion interactions. The metalation of 2H-DPP with Co ions from the cobalt oxide film is observed and studied by STM and x-ray photoelectron spectroscopy. The adsorption of Co-DPP is affected by the cobalt oxide film thickness. When the film is thicker than 0.26nm (1BL), the Co-DPP is found to rotate at 80K on the rock salt type cobalt oxide film. The time average of this rotation imaged by STM reveals the potential landscape of the molecule-molecule and molecule-substrate interactions. At approximately 470K, the molecules start to react with the substrate and eventually decompose. On spinel type cobalt oxides, the interaction between the DPP molecules and the film surface is much stronger. As a consequence, the metalation by cobalt ions from the oxide and the (partial) decomposition appear at almost the same temperature.
... As with melamine, melem is stable in two different forms on the surface as well as forming chiral rings on the surface. 34 The structure of the three stable forms are shown in ...
Article
Self-assembly of ordered molecular structures on surfaces is of great interest in the formation of devices with novel properties. By utilising molecules that form ordered structures, structures can form spontaneously without the need for lithographic processes. The de-halogenation and polymerisation of 1,3,5-tris-(4-iodophenyl)benzene on the hBN surface was investigated with AFM, XPS and SIMS. The molecules were deposited both from solution and in vacuum in minor variations of the previously reported sine-wave structure. Above 100°C, polymerisation was observed with AFM and confirmed with SIMS, which revealed that, after polymerisation, additional iodine was still present suggesting that dehalogenation had not fully taken place prior to polymerisation occurring as suggested by the XPS results. Using a vacuum deposition method, the structures formed by melamine on the hBN surface were investigated with AFM. Thick film triangular islands suggested an alignment of the molecular structure with the hBN substrate. Two main structures were seen: a rhombic lattice 0.87 ± 0.01 nm by 0.89 ± 0.01 nm and a square lattice 2.22 ± 0.03 nm by 2.10 ± 0.10 nm. An additional structure was seen on the top of the thick islands of 2.02 ± 0.06 nm by 0.77 ± 0.03 nm which was deemed to be a variant of the rhombic structure with out-of-plane rows due to the transition into the bulk structure. The rhombic structure was also deemed to be the structure forming an observed moiré pattern with a period of 3.19 ± 0.03 nm. The polymerisation of porphyrin monomers with varying numbers of reactive ethynyl groups on Ag(111) was investigated in vacuum using a novel indirect deposition method and STM. The 2R porphyrin was found to form chains when annealed to 120°C for 15 min with an intra-chain porphyrin separation of 1.33 ± 0.05 nm and an inter-chain distance of 1.90 ± 0.10 nm. The 4R porphyrin was also observed to form a lattice of 1.53 ± 0.04 nm by 1.69 ± 0.02 nm which was rationalised to be partially reacted into chains containing Ag atoms in one direction after heating to 120°C for a 15 min. The 3R porphyrin was observed to form short chains without heating when imaged with a low temperature STM. The 4R porphyrin was also deposited onto HOPG using a solution deposition method and formed lines separated by 1.70 ± 0.20 nm. Finally, mechanical transfer of hBN supported C60 islands was carried out. The C60 islands were found to be undamaged by soft deposit mechanical transfer process from a PPC/PDMS stamp. The transfer process using PPC/PDMS stamps was also used to form hBN/ C60 /hBN heterostructures and to transfer these to silicon nitride TEM grids for imaging although this step involved delaminating the PPC material at high temperature and subsequent cleaning.
... The formation of self-assembled monolayers (SAMs) on metal surfaces has aroused significant interest of scientists and resulted in development of many crucial technologies, such as protective coatings [1,2], chemical [3] and biological [4] sensors, biocompatible materials [5,6], stabilization of clusters [7], molecular electronics [8], nanofabrication [9], friction and lubrication control [10], read/write/ erase memory [11], and magnetism [12]. Controlling the molecule-substrate and molecule-molecule interactions, primarily by tuning hydrogen bonding and van der Waals interactions through designing different macrocycles having different linkers, plays a critical role in the development of noble metal-based SAM devices [13][14][15][16]. In this respect, there has been considerable literature on the investigation of SAM structures of large macrocyles adsorbed on inert metal surfaces [17,18]. ...
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Investigations of interactions between macrocyclic molecules and metal surfaces are crucial for emerging technologies, such as chemical and biological sensors, molecular electronics, read/write/erase memory, and magnetism. Thus, understanding the organic molecule and metal interface gains considerable importance. In this respect, we investigate a relatively unexplored porphyrin-related macrocycle, named as Pyrphyrin (Pyr), on Ag(111) surface by means of density functional theory. Our results show that main contribution to the adsorption energy is the dispersive contribution arising due to the interactions between the molecules and the surface. Optimal coordination of two cyano Ns and Co atoms (for CoPyr) to the surface Ag atoms determine preferred adsorption sites. Cyano ends of the Pyr molecule act as anchoring groups and enhances the stability of the complex by bending towards the Ag(111) surface. Cobalt incorporation into the Pyr core, on the other hand, further increases the adsorption strength by contribution of the attractive interactions between Co and Ag atoms. Selected molecular orbital representations of the complexes reveal the extension of orbitals located on Co and/or on two cyano N towards surface Ag atoms, thus, hybridization between molecular and surface states upon adsorption are confirmed.
... [10][11][12][13] By contrast, H-bonded structures formed by melaminea nd/or melem on different kinds of surfaces have been the subject of extensive STM and theoretical investigations. [14][15][16][17][18][19][20] Both compoundsc an be sublimed under ultrahigh vacuum to grow highly pure and defect-free epitaxial films. In the monolayerr egime, surfaces such as Au(111)a nd Ag(111)p romote flat adsorption and the formationo fp eculiar honeycombs tructures, in which the nitrogen functional groups are involved in intermolecular H-bonds that are very similart ot hose existing in the crystalline structures of melon and PHI. ...
... An amendatory way is to introduce more proper anchoring sites into the molecular building blocks which has considerable binding strength with these Au adatoms. Therefore in this work, we have considered the trimerization product of melamine, melem (triamino-s-heptazine), which can also form similar honeycomb self-assembly structure but with larger pores concomitantly decorated with heterocyclic N (h-N) atoms at the sides [35][36][37][38][39] . Our scanning tunneling microscopy (STM) experiments clearly show that exposing the melem film to CO atmosphere can efficiently generate quite a number of Au adatoms inside the nanopores of melem, whose concentration and stability are greatly enhanced in comparison with those on melamine films. ...
... It possesses three amino endgroups (denoted as D) and six on-side heterocyclic nitrogen atoms (denoted as A), through which the intermolecular hydrogen bonding (HB) pairs can be formed and the corresponding assembly structures can be constructed on inert surfaces. Honestly, all the predictable HB patterns (Scheme 1b-d) have been observed in the assemblies of melem 35,39 . We want to point out that in the cases of Scheme 1c, As already addressed in our previous report, a nearly pure phase of honeycomb structure of melem (termed as H-melem) can be achieved by controlling the melem coverage during deposition in combination with subsequent thermal annealing 35 . ...
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The controllability of metal adatoms has been attracting ever-growing attention because the metal species in particular single-atom metals can play an important role in various surface processes, including heterogeneous catalytic reactions. On the other hand, organic self-assembly films have been regarded as an efficient and versatile bottom-up method to fabricate surface nanostructures, whose functionality and periodicity can be highly designable. In this work, we have developed a novel strategy to steer the generation and distribution of metal adatoms by combining the surface self-assemblies with exposure to small inorganic gaseous molecules. More specifically, we have prepared a honeycomb structure of melem (triamino-s-heptazine) on the Au(111) surface based on a well-structured hydrogen bonding network. The achieved melem self-assembly contains periodic hexagonal pores having diameters as large as around 1 nm. More importantly, the peripheries of the nanopores are decorated with heterocyclic N atoms that can probably form strong interactions with the metal species. Upon exposing the melem self-assembly to a CO atmosphere at room temperature, a fair number of Au adatoms were produced and trapped inside the nanopores encircled by the melem molecules. Single or clustered Au vacancies were concomitantly formed that were also trapped by the melem pores and stabilized by the surrounding molecules, as confirmed by high-resolution scanning tunneling microscopy (STM) images. Both types of added species showed positive correlations with the CO exposure and saturated at around 0.01 monolayer. In addition, owing to the large pore size, as well as the presence of multiple docking sites inside the nanopores, more than one Au adatom can reside in a melem nanopore; they can be distributed in a variety of configurations for bi-Au (two Au adatoms) and tri-Au (three Au adatoms) species, whose population can be manipulated with the CO exposure. Moreover, control experiments demonstrated that these CO-induced Au species, including the adatoms and vacancies, can survive annealing treatments up to the temperature at which the melem molecules start to desorb, indicating a substantial thermal stability. The formed Au species may hold great potential for serving as active sites for surface reactions. More interestingly, the bi-Au and tri-Au species have moderate Au-Au intervals, and can be potentially active for certain structurally sensitive bimolecular reactions. Considering all these aspects, we believe that this work presents a fresh approach to utilizing organic self-assembly films and has demonstrated a rather novel strategy for preparing various single-atom metal species on substrate surfaces.
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