Publication Cover
Molecular Physics
An International Journal at the Interface Between Chemistry and Physics
Volume 121, 2023 - Issue 11-12: Special Issue of Molecular Physics in Honour of Péter Szalay
1,504
Views
2
CrossRef citations to date
0
Altmetric
Péter G. Szalay Special Issue of Molecular Physics

Spin-density calculation via the graphical unitary group approach

ORCID Icon, , ORCID Icon, ORCID Icon, ORCID Icon, ORCID Icon & ORCID Icon show all
Article: e2091049 | Received 27 Apr 2022, Accepted 07 Jun 2022, Published online: 23 Jun 2022

Figures & data

Figure 1. Phenalenyl valence bond structure with the indication for the carbon positions. Doping is considered in positions 2 and 12. The blue positions can present the open radical in ressonant structures.

Figure 1. Phenalenyl valence bond structure with the indication for the carbon positions. Doping is considered in positions 2 and 12. The blue positions can present the open radical in ressonant structures.

Figure 2. Spin-density distributions ρ[;1/2](r) for the pristine phenalenyl computed for the doublet ground state obtained from (a) MCSCF, (b) UHF, (c) ROHF, (d) PBE50, (e) PBE0, (f) PBE, (g) TPSS calculations and (h) 2D structure with Mulliken populations (e) from the MCSCF calculation. Blue denotes positive spin-density and red denotes negative values. The isovalue is ±0.001eÅ3 for positive and negative values, respectively.

Figure 2. Spin-density distributions ρ[−;1/2](r) for the pristine phenalenyl computed for the doublet ground state obtained from (a) MCSCF, (b) UHF, (c) ROHF, (d) PBE50, (e) PBE0, (f) PBE, (g) TPSS calculations and (h) 2D structure with Mulliken populations (e) from the MCSCF calculation. Blue denotes positive spin-density and red denotes negative values. The isovalue is ±0.001e⋅Å−3 for positive and negative values, respectively.

Figure 3. ρ±[;1/2](r) spin-promotion distributions and the natural spin-density orbitals (NSDOs) with their eigenvalues (μp(1/2)) for the pristine phenalenyl computed for the 2A2(2A1) ground state obtained from the MCSCF calculation. The isovalue is ±0.001eÅ3 for ρ±[;1/2](r) and ±0.05Å3/2 for the NSDOs. Blue and red represent positive and negative values, respectively.

Figure 3. ρ±[−;1/2](r) spin-promotion distributions and the natural spin-density orbitals (NSDOs) with their eigenvalues (μp(1/2)) for the pristine phenalenyl computed for the 2A2(2A1′′) ground state obtained from the MCSCF calculation. The isovalue is ±0.001e⋅Å−3 for ρ±[−;1/2](r) and ±0.05Å−3/2 for the NSDOs. Blue and red represent positive and negative values, respectively.

Figure 4. Spin-density distributions ρ[;1/2](r) for the N-didoped phenalenyl computed for the doublet ground state obtained from (a) MCSCF, (b) TPSS calculations and (c) 2D structure with Mulliken populations (e) from the MCSCF calculation. Blue denotes positive spin density and red denotes negative values. The isovalue is ±0.001eÅ3 for positive and negative values, respectively.

Figure 4. Spin-density distributions ρ[−;1/2](r) for the N-didoped phenalenyl computed for the doublet ground state obtained from (a) MCSCF, (b) TPSS calculations and (c) 2D structure with Mulliken populations (e) from the MCSCF calculation. Blue denotes positive spin density and red denotes negative values. The isovalue is ±0.001e⋅Å−3 for positive and negative values, respectively.

Figure 5. Spin-density distributions ρ[;1/2](r) for the N-monodoped phenalenyl computed for the doublet ground state obtained from (a) MCSCF, (b) TPSS calculations and (c) 2D structure with Mulliken populations (e) from the MCSCF calculation. Blue denotes positive spin density and red denotes negative values. The isovalue is ±0.001eÅ3 for positive and negative values, respectively.

Figure 5. Spin-density distributions ρ[−;1/2](r) for the N-monodoped phenalenyl computed for the doublet ground state obtained from (a) MCSCF, (b) TPSS calculations and (c) 2D structure with Mulliken populations (e) from the MCSCF calculation. Blue denotes positive spin density and red denotes negative values. The isovalue is ±0.001e⋅Å−3 for positive and negative values, respectively.

Figure 6. Spin-density distributions ρ[;1/2](r) for the NH-didoped phenalenyl computed for the doublet ground state obtained from (a) MCSCF, (b) TPSS calculations and (c) 2D structure with Mulliken populations (e) from the MCSCF calculation. Blue denotes positive spin density and red denotes negative values. The isovalue is ±0.001eÅ3 for positive and negative values, respectively.

Figure 6. Spin-density distributions ρ[−;1/2](r) for the NH-didoped phenalenyl computed for the doublet ground state obtained from (a) MCSCF, (b) TPSS calculations and (c) 2D structure with Mulliken populations (e) from the MCSCF calculation. Blue denotes positive spin density and red denotes negative values. The isovalue is ±0.001e⋅Å−3 for positive and negative values, respectively.
Supplemental material

Supplementary Material

Download MS Word (8.2 MB)