Abstract:We
present molecular beam epitaxial growth of blue phosphorene
(BlueP), a new allotrope of black phosphorene, on Au(111) and its
surface functionalization with fullerene (C60) molecules
by low-temperature scanning tunneling microscopy and scanning tunneling
spectroscopy (STS). In contrast to the well-ordered aggregation on
conventional surfaces, C60 molecules favor to adsorb at
the domain boundaries of BlueP and create defects and a disordered
phase nearby. STS reveals a shift of the conduction band minimum of… Show more
“…Increasing the coverage to 0.8 ML, BlueP on Au(111) still preserves its honeycomb structure, while several holes are filled with P atoms (circles in Figure a,b). The dark‐colored lines in Figure a are domain boundaries between unidirectionally aligned BlueP islands, including dislocation lines, defective chains, and big holes . In the case of Sb, high coverage generates a new phase along with the disappearance of dispersed bright dots, as shown in Figure c.…”
Section: Group Va Elements On Noble Metal Surfaces Buckled Phosphorementioning
“…Increasing the coverage to 0.8 ML, BlueP on Au(111) still preserves its honeycomb structure, while several holes are filled with P atoms (circles in Figure a,b). The dark‐colored lines in Figure a are domain boundaries between unidirectionally aligned BlueP islands, including dislocation lines, defective chains, and big holes . In the case of Sb, high coverage generates a new phase along with the disappearance of dispersed bright dots, as shown in Figure c.…”
Section: Group Va Elements On Noble Metal Surfaces Buckled Phosphorementioning
“…Stable in‐situ substitutional doping during the synthesis of 2D phosphorus (e.g., nitrogen doping of BlueP 79 ) represents a promising approach to extend their application in multifunctional devices, but is rarely investigated. It is also important to explore other nondestructive doping strategies, for example, combining with other organic 89,90 and inorganic quantum materials 91,92 to construct 2D phosphorus‐based heterojunctions.…”
Phosphorus is an important non‐metal element with many allotropes and tunable electronic properties. As one of the most important allotropes of phosphorus, two‐dimensional (2D) black phosphorus (BP) possesses many extraordinary properties, such as high charge carrier mobility with high on/off ratio, thickness‐dependent direct bandgap varying from 0.3 to 2 eV, and anisotropic electrical, optical and thermal properties. Inspiring by the success of 2D BP, other 2D phosphorus allotropes with intriguing properties for next‐generation electronic and optoelectronic devices have also attracted much attention. However, large‐scale growth of high‐quality 2D single/few‐layer phosphorus remains a great challenge. In this review, we highlight recent progress achieved on 2D phosphorus, with special focus on the epitaxial growth of 2D BP films, blue phosphorus (BlueP) monolayers as well as phosphorus‐metal porous networks. The remaining challenges and future perspectives on the development of monolayer phosphorus or phosphorus‐metal alloys are also provided.
“…Compared to our results, periodic vdW-KBM calculations and molecular dynamics simulations have reported non-covalent Phos−C60 complexes with Eads values of 0.7 and −1.0 eV, respectively 19,23 ; then, our results agree with previous reports. Additionally, UV-VIS-NIR absorbance, temperature scanning tunneling microscopy, and scanning tunneling spectroscopy measurements indicate that C60 molecules physically adsorb on phosphorene, where desorption occurs with annealing 400 K [20][21] . As can be seen, Eads=0.9 eV for Phos−C60 complexes agrees with the experimental favorable non-covalent adsorption of fullerenes on phosphorene-based materials.…”
Section: Structure and Stabilitymentioning
confidence: 99%
“…Mechanochemical reactions in a high energy mechanical milling process have been used as a strategy to form phosphorus-carbon (P−C) bonds between phosphorene and carbon materials, including C60, graphite, and graphite oxide 16 ; in this way, the content of the P−C bond in the phosphorene-C60 hybrids is only 0.8%, denoting C60 is not preferably bonded to phosphorene via covalent interactions until breaking the sp 2 C=C/C−C bonds to form defects 16 . In addition, low-temperature scanning tunneling microscopy, X-ray, ultraviolet photoelectron, and scanning tunneling spectroscopy measurements also show that C60 molecules are mainly physisorbed at room temperature on the honeycomb lattice of blue and black phosphorene synthesized by epitaxial growth, where an interfacial charge transfer is evidenced upon interaction with C60 [21][22] .…”
Hybrid materials formed by carbon fullerenes and layered materials have emerged due to their advantages for several technological applications, and phosphorene arises as a promising two-dimensional semiconductor for C60 adsorption. However, the properties of phosphorenefullerene hybrids remain mainly unexplored. In this work, we employed density functional theory to obtain structures, adsorption energies, electronic/optical properties, binding (AIM, NBO), and energy decomposition analyses (ALMO-EDA) of nanostructures formed by phosphorene and fullerenes (C24 to C70). We find fullerenes form covalent and non-covalent complexes with phosphorene depending on the molecular size, showing remarkable stability even in solution. Two classes of covalent complexes arise by cycloaddition-like reactions: the first class, where short-range effects (charge-transfer and polarization) determines the stability; and the second one, where short-range effects decay to avoid steric repulsion, and balanced longrange forces (electrostatics and dispersion) favors the stability. Otherwise, high-size fullerenes (C50 to C70) only form non-covalent complexes due to strong repulsion at shorter intermolecular distances and lack of dissociation barriers. In terms of electronic properties, fullerenes act as mild p-dopants for phosphorene, increasing its polar character and ability to acquire induced dipole moments (polarizability). Also, small energy-bandgap fullerenes (<0.8 eV) largely increase the phosphorene metallic character. We also note fullerenes retain their donor/acceptor properties upon adsorption, acting as active sites for orbital-controlled interactions and maximizing the phosphorene light absorbance at the UV-Vis region. Finally, we strongly believe our study will inspire future experimental/theoretical studies focused on phosphorene-fullerene uses for storage, anode materials, sensing, phosphorene bandgap engineering, and optoelectronics.<br>
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