Comparing the above P’s with Eqs.5.136we see that convergence to within our one
part in 1,000 criterion has not occurred: the largest change in the density matrix is |
(0.1996#0.1885)/0.1885|¼0.059, which is above 0.001, so the SCF procedure is
repeated.
Three more SCF cycles were carried out; the results of the “zeroth cycle” (the
initial guess) and the five cycles are summarized in Table5.1. Only with the fifth
cycle has convergence been achieved, i.e. have the changes in all the density
matrix elements fallen below one part in 1,000 (the largest change is inP 11 ,
|(0.2020#0.2019)/0.2019|¼0.0005<0.001). In actual practice, a convergence
criterion of from about one part in 10^4 to 1 in 10^8 is used, depending on the program
and the particular kind of calculation. The coefficients and the density matrix
elements change smoothly, although the energy levels andEtotalHF show some oscil-
lation. To reduce the number of steps needed to achieve convergence, programs
sometimes extrapolate the density matrix, i.e. estimate the finalPvalues and use
these estimates to initiate the final few SCF cycles.
Often the main result from a Hartree–Fock (i.e. an SCF) calculation is the energy
of the molecule (the calculation of energy may be subsumed into a geometry
optimization, which is really the task of finding the minimum-energy geometry).
The STO-1G energy of HHeþwith an internuclear distance of 0.800 A ̊ may be
calculated from our results:
The electronic energy is
EHF¼
Xn
i¼ 1
eiþ
1
2
Xm
r¼ 1
Xm
s¼ 1
PrsHcorers ð 5 : 147 ¼ 5 : 90 Þ
The internuclear repulsion energy is
VNN¼
X
allm;v
ZmZv
rmv
ð 5 : 148 ¼ 5 : 92 Þ
and the total internal energy of the molecule at 0 K (except for zero point energy –
Section 5.2.3.6.4) is
Table 5.1 Results of initial guess and SCF cycles on HHeþat bond length 0.800 A ̊using the
STO-1G basis set. Energies (e 1 ,e 2 , andEtotalHF) are in hartrees
Initial guess
(zeroth
cycle)
First cycle Second cycle Third cycle Fourth cycle Fifth cycle
e 1 ,e 2 ,– #1.4027,
#0.0756
#1.4447,
#0.1062
#1.4466,
#0.1054
#1.4473,
#0.1056
#1.4470,
#0.1051
c 11 ,c 21 0.249,
0.867
0.3070,
0.8100
0.3159,
0.8034
0.3175,
0.8022
0.3177,
0.8021
0.3178,
0.8020
c 12 ,c 22 – 1.1145,
#0.8247
1.1120,
#0.8319
1.1115,
#0.8323
1.1115,
#0.8325
1.1114,
#0.8325
P 11 0.1240 0.1885 0.1996 0.2010 0.2019 0.2020
P 12 0.4318 0.4973 0.5076 0.5094 0.5097 0.5097
P 22 1.5034 1.3122 1.2909 1.2870 1.2867 1.2864
EtotalHF – #2.3992 #2.4419 #2.4428 #2.4443 #2.4438
228 5 Ab initio Calculations