“…The charge distribution in the surface (ET) 2 layer is analyzed with the wavefunction analysis described in the previous section [1]. Figures 8 and 9 show the observed STM images in the ab plane, where the higher the probe tip, the brighter the topography appears.…”
Section: Site Assignmentmentioning
confidence: 99%
“…The parentheses show uncertainty in the last digit (reused from Ref. [1]). Figure 9B shows the STM image with the structure determined by X-ray analysis [23], where the position and direction of the bright areas agree with the 3p orbitals of the sulfur atoms without recognizable reconstructions.…”
Section: Site Assignmentmentioning
confidence: 99%
“…However, since STM images are constructed with the electron tunneling probability between the wavefunctions of an STM probe tip and those of a sample surface, it is required for us to analyze the wavefunctions of the atoms and the molecules in the surface layer to extract structural information. In this chapter, some examples of the wavefunction analysis [1] are demonstrated in the organic charge transfer salts composed of electron donor and electron acceptor molecules, in which the van der Waals interaction and the π electron transfer integrals between like molecules, and the Coulomb attractive interaction between unlike molecules govern the formation of the crystals. Since the van der Waals interaction between the like molecules is relatively weak, the analysis of atomic π orbitals of sulfur, oxygen, and carbon atoms of the donor molecules would be a good approximation for the wavefunction analysis of STM images.…”
Section: Introductionmentioning
confidence: 99%
“…Thus, we are possible to continuously control the structure of the π electron networks from 1D to 2D, the filling of the π electron bands and electron-electron correlation of π bands, resulting in not only non-BCS superconductor, but also metals with variety of ground states like antiferromagnetic (AF), charge density wave (CDW), spin density wave (SDW), spin Peierls (SP), charge ordering (CO) states, and their combinations with exotic magnetic structures, for example, magnetic-field induced superconductivity [7]. Then, STM investigation of these organic systems is useful to collect local information of the π electron systems of the crystal surface layer [1,[8][9][10][11][12][13][14][15][16][17][18].…”
Section: Introductionmentioning
confidence: 99%
“…On the second point, the partner anion layer of the double layer generally forms a flat sheet and generates approximately uniform electric field normal to the anion layer [1]. The uniform electric field attracts uniformly the cation layer sheet, in which the cation molecules are tightly bound each other by the cohesive interaction with the other cation molecules, forming a π band, under constraint of the steric hindrance with the cation molecules and the partner anion molecules in the double layer.…”
In this chapter, the wavefunction analysis is demonstrated, applied to the organic charge transfer salts composed of electron donor and electron acceptor molecules. Scanning tunneling microscopy (STM) images of the surface donor layers in the three charge transfer salts, α-(BEDT-TTF) 2 I 3 , β-(BEDT-TTF) 2 I 3 , and (EDO-TTF) 2 PF 6 , are analyzed with the atomic π electron orbitals of sulfur, oxygen, and carbon atoms. We have deduced three different kinds of surface molecular reconstructions as follows: (1) charge redistribution in α-(BEDT-TTF) 2 I 3 , (2) translational reconstruction up to 0.1 nm in β-(BEDT-TTF) 2 I 3 , and (3) rotational reconstruction transforming the 1D axis from the a axis to the b axis in (EDO-TTF) 2 PF 6 . Finally, it is concluded that the surface reconstruction is ascribed to the additional gain of the cohesive energy of the π electron system, provoked by the reduced steric hindrance with the anions of the missing outside double layer. The investigations of the surface states provide not only interesting behaviors of the surface cation layer, but also important insights into the electronic states of a lot of similar charge transfer crystals, as demonstrated in α-(BEDT-TTF) 2 I 3 .
“…The charge distribution in the surface (ET) 2 layer is analyzed with the wavefunction analysis described in the previous section [1]. Figures 8 and 9 show the observed STM images in the ab plane, where the higher the probe tip, the brighter the topography appears.…”
Section: Site Assignmentmentioning
confidence: 99%
“…The parentheses show uncertainty in the last digit (reused from Ref. [1]). Figure 9B shows the STM image with the structure determined by X-ray analysis [23], where the position and direction of the bright areas agree with the 3p orbitals of the sulfur atoms without recognizable reconstructions.…”
Section: Site Assignmentmentioning
confidence: 99%
“…However, since STM images are constructed with the electron tunneling probability between the wavefunctions of an STM probe tip and those of a sample surface, it is required for us to analyze the wavefunctions of the atoms and the molecules in the surface layer to extract structural information. In this chapter, some examples of the wavefunction analysis [1] are demonstrated in the organic charge transfer salts composed of electron donor and electron acceptor molecules, in which the van der Waals interaction and the π electron transfer integrals between like molecules, and the Coulomb attractive interaction between unlike molecules govern the formation of the crystals. Since the van der Waals interaction between the like molecules is relatively weak, the analysis of atomic π orbitals of sulfur, oxygen, and carbon atoms of the donor molecules would be a good approximation for the wavefunction analysis of STM images.…”
Section: Introductionmentioning
confidence: 99%
“…Thus, we are possible to continuously control the structure of the π electron networks from 1D to 2D, the filling of the π electron bands and electron-electron correlation of π bands, resulting in not only non-BCS superconductor, but also metals with variety of ground states like antiferromagnetic (AF), charge density wave (CDW), spin density wave (SDW), spin Peierls (SP), charge ordering (CO) states, and their combinations with exotic magnetic structures, for example, magnetic-field induced superconductivity [7]. Then, STM investigation of these organic systems is useful to collect local information of the π electron systems of the crystal surface layer [1,[8][9][10][11][12][13][14][15][16][17][18].…”
Section: Introductionmentioning
confidence: 99%
“…On the second point, the partner anion layer of the double layer generally forms a flat sheet and generates approximately uniform electric field normal to the anion layer [1]. The uniform electric field attracts uniformly the cation layer sheet, in which the cation molecules are tightly bound each other by the cohesive interaction with the other cation molecules, forming a π band, under constraint of the steric hindrance with the cation molecules and the partner anion molecules in the double layer.…”
In this chapter, the wavefunction analysis is demonstrated, applied to the organic charge transfer salts composed of electron donor and electron acceptor molecules. Scanning tunneling microscopy (STM) images of the surface donor layers in the three charge transfer salts, α-(BEDT-TTF) 2 I 3 , β-(BEDT-TTF) 2 I 3 , and (EDO-TTF) 2 PF 6 , are analyzed with the atomic π electron orbitals of sulfur, oxygen, and carbon atoms. We have deduced three different kinds of surface molecular reconstructions as follows: (1) charge redistribution in α-(BEDT-TTF) 2 I 3 , (2) translational reconstruction up to 0.1 nm in β-(BEDT-TTF) 2 I 3 , and (3) rotational reconstruction transforming the 1D axis from the a axis to the b axis in (EDO-TTF) 2 PF 6 . Finally, it is concluded that the surface reconstruction is ascribed to the additional gain of the cohesive energy of the π electron system, provoked by the reduced steric hindrance with the anions of the missing outside double layer. The investigations of the surface states provide not only interesting behaviors of the surface cation layer, but also important insights into the electronic states of a lot of similar charge transfer crystals, as demonstrated in α-(BEDT-TTF) 2 I 3 .
Charge density waves have been intensely
studied in inorganic materials
such as transition metal dichalcogenides; however their counterpart
in organic materials has yet to be explored in detail. Here we report
the finding of robust two-dimensional charge density waves in molecular
layers formed by α-(BEDT-TTF)2–I3 on a Ag(111) surface. Low-temperature scanning tunneling microscopy
images of a multilayer thick α-(BEDT-TTF)2–I3 on a Ag(111) substrate reveal the coexistence of 5a
0 × 5a
0 and
R9° charge density
wave patterns commensurate with the underlying molecular lattice at
80 K. Both charge density wave patterns remain in nanosize molecular
islands with just a single constituent molecular-layer thickness at
80 and 5 K. Local tunneling spectroscopy measurements reveal the variation
of the gap from 244 to 288 meV between the maximum and minimum charge
density wave locations. Density functional theory calculations further
confirm a vertical positioning of BEDT-TTF molecules in the molecular
layer. While the observed charge density wave patterns are stable
for the defect sites, they can be reversibly switched for one molecular
lattice site by means of inelastic tunneling electron energy transfer
with the electron energies exceeding 400 meV using a scanning tunneling
microscope manipulation scheme.
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