C2H+ potentials
Ab initio points
fit.sci
Information on grid:
pot = [struct] with 8 fields:
thetas: [9x1 constant (1)] # Θ = [100:10:180] deg
CCs: [9x1 constant (1)] # r_CC = [2.2:0.1:3.2] a₀
CHs: [11x1 constant (1)] # r_CH = [1.6:0.1:2.0 2.05 2.1 2.2 2.3 2.4 2.6] a₀
zs: [9x1 constant (1)] # zs(i) = cos(Θᵢ), i=1:nz
nz: 9
ntheta: 9
nCC: 9
nCH: 11
The MRCI ab initio points:
qmV = |itheta(9), iCC(10), iCH(12)>A(1080;3)<V(3)| # All points
qmPi = |itheta(9), iCC(9), iCH(11)>A(891;2)<V(2)| # A'' and A', correlating with ³Π
qmSig = |itheta(9), iCC(9), iCH(11)>A(891;1)<V(1)| # 2A'', correlating with ³Σ⁻
qmPi0 = |iCC(9), iCH(11)>A(99;1)<V(1)| # ³Π, linear geometry
qmSig0 = |iCC(9), iCH(11)>A(99;1)<V(1)| # ³Σ⁻, linear geometry
Two-dimensional fits, product of Hermite polynomials
\[\begin{split}V_\mathrm{2d}(r_\mathrm{CC}, r_\mathrm{CH}) = \sum_{i=0}^{N_x} \sum_{\substack{j=0\\ i+j \leq N_{xy}}}^{N_y} H_i[f_x (r_\mathrm{CC}-r_x)]
H_j[f_y (r_\mathrm{CC}-r_y)] c_{i,j}\end{split}\]
Parameters for ³Π state:
parPi0 = [struct] with 11 fields:
fx: 5.30392
rx: 2.7
fy: 5.30392
ry: 2.1
Nx: 6
Ny: 6
Nxy: 6
c0: |nCC(7), nCH(7)>A(28;1)<V(1)|
Hxy: |iCC(9), iCH(11)>A(99;28)<nCC(7), nCH(7)|
namX: CC
namY: CH
Parameters for ³Σ⁻ state:
parSig0 = [struct] with 11 fields:
fx: 5.30392
rx: 2.7
fy: 5.30392
ry: 2.1
Nx: 6
Ny: 6
Nxy: 6
c0: |nCC(7), nCH(7)>A(28;1)<V(1)|
Hxy: |iCC(9), iCH(11)>A(99;28)<nCC(7), nCH(7)|
namX: CC
namY: CH
Three-dimensional fits:
\[\begin{split}V_\mathrm{3d}(r_\mathrm{CC}, r_\mathrm{CH}, \theta) = \sum_{i=0}^{N_x}
\sum_{\substack{j=0\\ i+j \leq N_{xy}}}^{N_y} H_i[f_x (r_\mathrm{CC}-r_x)]
H_j[f_y (r_\mathrm{CC}-r_y)]
\sum_{L=0}^{L_\mathrm{max}} P_L(\cos\theta)c_{ijL}\end{split}\]
Parameters for \(V_2=V_\mathrm{1A'}\)
parV2 = [struct] with 12 fields:
fx: 5.30392
rx: 2.7
fy: 5.30392
ry: 2.1
Nx: 6
Ny: 6
Nxy: 6
Hxy: |iCC(9), iCH(11)>A(99;28)<nCC(7), nCH(7)|
namX: CC
namY: CH
LS: |itheta(9)>A(9;5)<L(5)|
c: |nCC(7), nCH(7), L(5)>A(140;1)<V(1)|