2017
DOI: 10.1021/acs.jpclett.7b01965
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Pair Correlation Function of a 2D Molecular Gas Directly Visualized by Scanning Tunneling Microscopy

Abstract: The state of matter in fluid phases, determined by the interactions between particles, can be characterized by a pair correlation function (PCF). At the nanoscale, the PCF has been so far obtained experimentally only by means of reciprocal-space techniques. We use scanning tunneling microscopy (STM) at room temperature in combination with lattice-gas kinetic Monte Carlo (KMC) simulations to study a two-dimensional gas of highly mobile molecules of fluorinated copper phthalocyanine on a Si(111)/Tl-(1×1) surface… Show more

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Cited by 10 publications
(12 citation statements)
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“…In fact, the 2D gas plays an indispensable role in the phase transformations, mediating mass transport between the individual islands. The presence of the 2D molecular gas is visible in our room-temperature STM images as characteristic noise caused by molecules passing below the scanning tip and rapid changes at the edges of the molecular islands. , …”
Section: Resultsmentioning
confidence: 84%
See 1 more Smart Citation
“…In fact, the 2D gas plays an indispensable role in the phase transformations, mediating mass transport between the individual islands. The presence of the 2D molecular gas is visible in our room-temperature STM images as characteristic noise caused by molecules passing below the scanning tip and rapid changes at the edges of the molecular islands. , …”
Section: Resultsmentioning
confidence: 84%
“…The presence of the 2D molecular gas is visible in our room-temperature STM images as characteristic noise caused by molecules passing below the scanning tip and rapid changes at the edges of the molecular islands. 31,32 The sample temperature was slowly increased at a rate of 3 K•min −1 from room temperature; at 341 K we observed the formation of β phase islands simultaneously at different locations within the LEEM view field (see Figures 4 and S5 and Supporting Videos SV1 and SV3). Altogether we make the following observations: (I) As the temperature is increased, before nucleation of the β phase islands, we observe a reduction in the area of the α phase islands (see Supporting Information, Section 5) as well as Ostwald ripening of the α phase (the small islands disappear and the larger ones grow).…”
Section: Resultsmentioning
confidence: 86%
“…This is probably caused by a narrow temperature interval between formation of the 1×1 structure and Tl desorption 34 . We note that other less frequent types of defects coexisting with the ring-shaped ones can be observed occasionally 32 .
Figure 1( a ) STM image of the Tl/Si(111)1×1 surface at sample voltage U S = +1 V showing ring-shaped defects. ( b ) Top and side views of the relaxed structure of the multi-vacancy defect on the Tl/Si(111)1×1 surface induced by the presence of an extra Si atom at the topmost atomic layer and missing Tl atoms.
…”
Section: Resultsmentioning
confidence: 99%
“…Furthermore, we demonstrated the metallicity of the observed layers in contrast to predictions from density functional theory (DFT) calculations and discussed a possible doping effect of the defects. The defects also play an important role in the interaction with other adsorbates on the surface 32,33 . In the second important work, Sakamoto et al .…”
Section: Introductionmentioning
confidence: 99%
“…In our previous works we studied room-temperature behavior of F 0 CuPC and F 16 CuPC molecules deposited on the Si(111)-Tl 1 × 1 surface. We found that the F 0 CuPC molecules form ordered structures at full ML coverage.…”
Section: Introductionmentioning
confidence: 99%