| Title: | anion_triplet_point4 |
| Browse item: | https://iochem-bd.bsc.es:443/browse/handle/100/314795 |
| Program: | Molcas 23.02 - 251-g879886393 |
| Author: | Vlaisavljevich, Bess |
| Formula: | C12H30B3U |
| Calculation type: | Single point |
| Method: | CASSCF CASPT2 |
Character Table for C1
| Charge | -1.000 |
| Multiplicity | 3 |
| Multipole Moment integrals up to order 2 |
| Kinetic Energy integrals |
| Nuclear Attraction integrals (point charge) |
| One-Electron Hamiltonian integrals |
| Velocity integrals |
| Relativistic Douglas-Kroll-Hess integrals: |
| - Parametrization : EXP |
| - DKH order of Hamiltonian: 2 |
| - DKH order of Properties : 0 |
| - multipole moment operators |
| - electric potential operators |
| - contact operators |
| Orbital angular momentum around (-0.8836 0.0747 -0.0051 ) |
| Velocity quadrupole around (-0.8836 0.0747 -0.0051 ) |
| Atomic mean-field integrals |
| Cholesky decomposed two-electron repulsion integrals |
| - CD Threshold: 0.10E-03 |
| Atom1 | Atom2 | Distance |
|---|---|---|
| U1 | C3 | 2.633774 |
| U1 | C6 | 2.628450 |
| U1 | B16 | 2.581156 |
| U1 | B14 | 2.569190 |
| U1 | B15 | 2.568530 |
| C2 | C8 | 1.501508 |
| C2 | C3 | 1.445411 |
| C2 | C7 | 1.385574 |
| C3 | C9 | 1.503649 |
| C3 | C4 | 1.444491 |
| C4 | C10 | 1.500811 |
| C4 | C5 | 1.385386 |
| C5 | C11 | 1.499541 |
| C5 | C6 | 1.443006 |
| C6 | C12 | 1.504123 |
| C6 | C7 | 1.447098 |
| C7 | C13 | 1.500634 |
| C8 | H17 | 1.092956 |
| C8 | H18 | 1.092860 |
| C8 | H19 | 1.086739 |
| C9 | H32 | 1.102327 |
| C9 | H33 | 1.089751 |
| C9 | H34 | 1.089429 |
| C10 | H31 | 1.076386 |
| C10 | H30 | 1.072809 |
| C10 | H29 | 1.072546 |
| C11 | H27 | 1.073643 |
| C11 | H26 | 1.065115 |
| C11 | H28 | 1.056591 |
| C12 | H23 | 1.049875 |
| C12 | H24 | 1.042025 |
| C12 | H25 | 1.036972 |
| C13 | H22 | 1.069300 |
| C13 | H20 | 1.063733 |
| C13 | H21 | 1.055475 |
| B14 | H41 | 1.244732 |
| B14 | H39 | 1.243948 |
| B14 | H40 | 1.238205 |
| B14 | H42 | 1.203134 |
| B15 | H35 | 1.244707 |
| B15 | H38 | 1.243443 |
| B15 | H36 | 1.237482 |
| B15 | H37 | 1.203062 |
| B16 | H43 | 1.244700 |
| B16 | H46 | 1.242598 |
| B16 | H45 | 1.237812 |
| B16 | H44 | 1.202941 |
| Number of closed shell electrons | 200 |
| Number of electrons in active shells | 10 |
| Max number of holes in RAS1 space | 0 |
| Max nr of electrons in RAS3 space | 0 |
| Number of inactive orbitals | 100 |
| Number of active orbitals | 18 |
| Number of secondary orbitals | 386 |
| Spin quantum number | 1.0 |
| State symmetry | 1 |
| Total molecular charge | -1.00 |
| Symmetry species | 1 |
| a | |
| Frozen orbitals | 0 |
| Inactive orbitals | 100 |
| Active orbitals | 18 |
| RAS1 orbitals | 0 |
| RAS2 orbitals | 18 |
| RAS3 orbitals | 0 |
| Secondary orbitals | 386 |
| Deleted orbitals | 0 |
| Number of basis functions | 504 |
| Number of determinants | 56805840 | ||
| Number of root(s) required | 1 | ||
| CI roots used / Weights |
|
||
| Highest root included in the CI | 1 | ||
| Root passed to geometry opt. | 1 |
| Root | Total energy (au) | ∆E (eV) | ∆E (cm-1) |
| 1 | -28496.129717 | 0.00 | 0 |
| Conf | 111111111111111111 | 1 |
|---|
| Symmetry 1 | 1 |
|---|---|
| 101a | 1.959621 |
| 102a | 1.931126 |
| 103a | 1.943542 |
| 104a | 0.992788 |
| 105a | 0.989507 |
| 106a | 1.717492 |
| 107a | 0.264818 |
| 108a | 0.071287 |
| 109a | 0.023635 |
| 110a | 0.013064 |
| -1.000 |
| 1 |
|---|
| 1 |
|---|
| Number of closed shell electrons | 92 |
| Number of electrons in active shells | 10 |
| Max number of holes in RAS1 space | 0 |
| Max nr of electrons in RAS3 space | 0 |
| Number of inactive orbitals | 46 |
| Number of active orbitals | 18 |
| Number of secondary orbitals | 386 |
| Spin quantum number | 1.0 |
| State symmetry | 1 |
| Total molecular charge | -1.00 |
| Symmetry species | 1 |
| a | |
| Frozen orbitals | 54 |
| Inactive orbitals | 46 |
| Active orbitals | 18 |
| Secondary orbitals | 386 |
| Deleted orbitals | 0 |
| Number of basis functions | 504 |
| Root | Total energy (au) | ∆E (eV) | ∆E (cm-1) | Ref. Weight |
|---|---|---|---|---|
| 1 | -28498.6216692147 | 0.00 | 0 | 0.54213 |