Table 2 Configurations making significant contributions to the ground state (11Ag) wave functions of RGM-n (n = 28–72), computed using the MRSDCI approach, and the standard (Std) and screened (Scr) parameters in the PPP-model Hamiltonian.
System | Scr | Std |
---|---|---|
RGM-28 | |HF〉 (0.7899) | |HF〉 (0.8315) |
|H → L; H → L〉 (0.2264) | |H → L; H → L〉 (0.2362) | |
RGM-30 | |HF〉 (0.8143) | |HF〉 (0.8574) |
|H → L; H → L〉 (0.1685) | |H → L; H → L〉 (0.1415) | |
RGM-36 | |HF〉 (0.7269) | |HF〉 (0.7572) |
|H → L; H → L〉 (0.3468) | |H → L; H → L〉 (0.3399) | |
RGM-40 | |HF〉 (0.7946) | |HF〉 (0.8401) |
|H → L; H → L〉 (0.1796) | |H → L; H → L〉 (0.1534) | |
RGM-42 | |HF〉 (0.7247) | |HF〉 (0.7530) |
|H → L; H → L〉 (0.3508) | |H → L; H → L〉 (0.3342) | |
RGM-50 | |HF〉 (0.8044) | |HF〉 (0.8434) |
|H → L; H → L〉 (0.2064) | |H → L; H → L〉 (0.1586) | |
RGM-54 | |HF〉 (0.6504) | |HF〉 (0.6400) |
|H → L; H → L〉 (0.4866) | |H → L; H → L〉 (0.4975) | |
RGM-56 | |HF〉 (0.6798) | |HF〉 (0.6724) |
|H → L; H → L〉 (0.4541) | |H → L; H → L〉 (0.4469) | |
RGM-72 | |HF〉 (0.6164) | |HF〉 (0.5958) |
|H → L; H → L〉 (0.5562) | |H → L; H → L〉 (0.5666) |