Jump to
S1C2
S1C3
Energy calculated at HSEh1PBE/6-31+G**
| hartrees |
Energy at 0K | -581.066459 |
Energy at 298.15K | |
HF Energy | -581.066459 |
Nuclear repulsion energy | 78.797325 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HSEh1PBE/6-31+G**
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
Ag |
2279 |
2176 |
0.00 |
421.27 |
0.19 |
0.32 |
2 |
Ag |
943 |
900 |
0.00 |
22.47 |
0.23 |
0.37 |
3 |
Ag |
596 |
569 |
0.00 |
106.43 |
0.20 |
0.33 |
4 |
Au |
545 |
521 |
0.00 |
0.00 |
0.00 |
0.00 |
5 |
B1u |
2273 |
2170 |
76.40 |
0.00 |
0.00 |
0.00 |
6 |
B1u |
861 |
822 |
106.80 |
0.00 |
0.00 |
0.00 |
7 |
B2g |
220i |
210i |
0.00 |
44.12 |
0.75 |
0.86 |
8 |
B2u |
2309 |
2205 |
138.91 |
0.00 |
0.00 |
0.00 |
9 |
B2u |
352 |
336 |
16.47 |
0.00 |
0.00 |
0.00 |
10 |
B3g |
2300 |
2196 |
0.00 |
227.61 |
0.75 |
0.86 |
11 |
B3g |
598 |
571 |
0.00 |
7.00 |
0.75 |
0.86 |
12 |
B3u |
520 |
496 |
0.50 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 6678.0 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 6376.2 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at HSEh1PBE/6-31+G**
Point Group is D2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Si1 |
0.000 |
0.000 |
1.069 |
Si2 |
0.000 |
0.000 |
-1.069 |
H3 |
0.000 |
1.255 |
1.854 |
H4 |
0.000 |
-1.255 |
1.854 |
H5 |
0.000 |
1.255 |
-1.854 |
H6 |
0.000 |
-1.255 |
-1.854 |
Atom - Atom Distances (Å)
|
Si1 |
Si2 |
H3 |
H4 |
H5 |
H6 |
Si1 | | 2.1377 | 1.4802 | 1.4802 | 3.1811 | 3.1811 |
Si2 | 2.1377 | | 3.1811 | 3.1811 | 1.4802 | 1.4802 | H3 | 1.4802 | 3.1811 | | 2.5093 | 3.7087 | 4.4778 | H4 | 1.4802 | 3.1811 | 2.5093 | | 4.4778 | 3.7087 | H5 | 3.1811 | 1.4802 | 3.7087 | 4.4778 | | 2.5093 | H6 | 3.1811 | 1.4802 | 4.4778 | 3.7087 | 2.5093 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Si1 |
Si2 |
H5 |
122.050 |
|
Si1 |
Si2 |
H6 |
122.050 |
Si2 |
Si1 |
H3 |
122.050 |
|
Si2 |
Si1 |
H4 |
122.050 |
H3 |
Si1 |
H4 |
115.900 |
|
H5 |
Si2 |
H6 |
115.900 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Si |
0.087 |
|
|
|
2 |
Si |
0.087 |
|
|
|
3 |
H |
-0.044 |
|
|
|
4 |
H |
-0.044 |
|
|
|
5 |
H |
-0.044 |
|
|
|
6 |
H |
-0.044 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
0.000 |
0.000 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.943 |
0.000 |
0.000 |
y |
0.000 |
-29.039 |
0.000 |
z |
0.000 |
0.000 |
-27.590 |
|
Traceless |
| x | y | z |
x |
-3.628 |
0.000 |
0.000 |
y |
0.000 |
0.727 |
0.000 |
z |
0.000 |
0.000 |
2.901 |
|
Polar |
3z2-r2 | 5.802 |
x2-y2 | -2.904 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.161 |
0.000 |
0.000 |
y |
0.000 |
6.782 |
0.000 |
z |
0.000 |
0.000 |
14.790 |
<r2> (average value of r
2) Å
2
<r2> |
70.480 |
(<r2>)1/2 |
8.395 |
Jump to
S1C1
S1C3
Energy calculated at HSEh1PBE/6-31+G**
| hartrees |
Energy at 0K | -581.067288 |
Energy at 298.15K | |
HF Energy | -581.067288 |
Nuclear repulsion energy | 78.223377 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HSEh1PBE/6-31+G**
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
Ag |
2256 |
2154 |
0.00 |
432.18 |
0.19 |
0.32 |
2 |
Ag |
947 |
905 |
0.00 |
35.65 |
0.25 |
0.40 |
3 |
Ag |
575 |
549 |
0.00 |
82.87 |
0.25 |
0.40 |
4 |
Ag |
296 |
283 |
0.00 |
32.60 |
0.38 |
0.55 |
5 |
Au |
2285 |
2182 |
167.45 |
0.00 |
0.00 |
0.00 |
6 |
Au |
532 |
508 |
0.28 |
0.00 |
0.00 |
0.00 |
7 |
Au |
343 |
328 |
16.84 |
0.00 |
0.00 |
0.00 |
8 |
Bg |
2274 |
2171 |
0.00 |
261.86 |
0.75 |
0.86 |
9 |
Bg |
611 |
583 |
0.00 |
8.89 |
0.75 |
0.86 |
10 |
Bu |
2251 |
2149 |
119.92 |
0.00 |
0.00 |
0.00 |
11 |
Bu |
904 |
863 |
161.06 |
0.00 |
0.00 |
0.00 |
12 |
Bu |
455 |
435 |
27.10 |
0.00 |
0.00 |
0.00 |
Unscaled Zero Point Vibrational Energy (zpe) 6864.2 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 6553.9 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at HSEh1PBE/6-31+G**
Point Group is C2h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Si1 |
0.000 |
1.081 |
0.000 |
Si2 |
0.000 |
-1.081 |
0.000 |
H3 |
0.389 |
1.806 |
1.237 |
H4 |
0.389 |
1.806 |
-1.237 |
H5 |
-0.389 |
-1.806 |
1.237 |
H6 |
-0.389 |
-1.806 |
-1.237 |
Atom - Atom Distances (Å)
|
Si1 |
Si2 |
H3 |
H4 |
H5 |
H6 |
Si1 | | 2.1629 | 1.4851 | 1.4851 | 3.1650 | 3.1650 |
Si2 | 2.1629 | | 3.1650 | 3.1650 | 1.4851 | 1.4851 | H3 | 1.4851 | 3.1650 | | 2.4734 | 3.6945 | 4.4461 | H4 | 1.4851 | 3.1650 | 2.4734 | | 4.4461 | 3.6945 | H5 | 3.1650 | 1.4851 | 3.6945 | 4.4461 | | 2.4734 | H6 | 3.1650 | 1.4851 | 4.4461 | 3.6945 | 2.4734 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Si1 |
Si2 |
H5 |
119.194 |
|
Si1 |
Si2 |
H6 |
119.194 |
Si2 |
Si1 |
H3 |
119.194 |
|
Si2 |
Si1 |
H4 |
119.194 |
H3 |
Si1 |
H4 |
112.761 |
|
H5 |
Si2 |
H6 |
112.761 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Si |
0.098 |
|
|
|
2 |
Si |
0.098 |
|
|
|
3 |
H |
-0.049 |
|
|
|
4 |
H |
-0.049 |
|
|
|
5 |
H |
-0.049 |
|
|
|
6 |
H |
-0.049 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
0.000 |
0.000 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-31.740 |
-0.252 |
0.000 |
y |
-0.252 |
-27.739 |
0.000 |
z |
0.000 |
0.000 |
-29.317 |
|
Traceless |
| x | y | z |
x |
-3.212 |
-0.252 |
0.000 |
y |
-0.252 |
2.790 |
0.000 |
z |
0.000 |
0.000 |
0.422 |
|
Polar |
3z2-r2 | 0.844 |
x2-y2 | -4.001 |
xy | -0.252 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
7.151 |
-0.621 |
0.000 |
y |
-0.621 |
15.017 |
0.000 |
z |
0.000 |
0.000 |
7.224 |
<r2> (average value of r
2) Å
2
<r2> |
71.000 |
(<r2>)1/2 |
8.426 |
Jump to
S1C1
S1C2
Energy calculated at HSEh1PBE/6-31+G**
| hartrees |
Energy at 0K | -581.028538 |
Energy at 298.15K | |
HF Energy | -581.028538 |
Nuclear repulsion energy | 73.109254 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HSEh1PBE/6-31+G**
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A1 |
2109 |
2014 |
417.90 |
296.53 |
0.40 |
0.57 |
2 |
A1 |
1665 |
1589 |
0.06 |
73.15 |
0.12 |
0.21 |
3 |
A1 |
887 |
847 |
39.59 |
118.84 |
0.33 |
0.50 |
4 |
A1 |
408 |
390 |
1.37 |
65.27 |
0.41 |
0.58 |
5 |
A1 |
379 |
362 |
0.57 |
5.18 |
0.11 |
0.19 |
6 |
A2 |
1416 |
1352 |
0.00 |
0.13 |
0.75 |
0.86 |
7 |
A2 |
638 |
610 |
0.00 |
0.36 |
0.75 |
0.86 |
8 |
B1 |
1337 |
1276 |
41.15 |
0.05 |
0.75 |
0.86 |
9 |
B1 |
841 |
803 |
12.93 |
23.64 |
0.75 |
0.86 |
10 |
B2 |
2081 |
1987 |
12.82 |
18.85 |
0.75 |
0.86 |
11 |
B2 |
1387 |
1324 |
1145.09 |
22.40 |
0.75 |
0.86 |
12 |
B2 |
729 |
696 |
79.11 |
15.59 |
0.75 |
0.86 |
Unscaled Zero Point Vibrational Energy (zpe) 6938.6 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 6625.0 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Geometric Data calculated at HSEh1PBE/6-31+G**
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Si1 |
0.000 |
1.315 |
-0.089 |
Si2 |
0.000 |
-1.315 |
-0.089 |
H3 |
-1.034 |
0.000 |
-0.182 |
H4 |
1.034 |
0.000 |
-0.182 |
H5 |
0.000 |
1.322 |
1.430 |
H6 |
0.000 |
-1.322 |
1.430 |
Atom - Atom Distances (Å)
|
Si1 |
Si2 |
H3 |
H4 |
H5 |
H6 |
Si1 | | 2.6302 | 1.6752 | 1.6752 | 1.5195 | 3.0433 |
Si2 | 2.6302 | | 1.6752 | 1.6752 | 3.0433 | 1.5195 | H3 | 1.6752 | 1.6752 | | 2.0671 | 2.3268 | 2.3268 | H4 | 1.6752 | 1.6752 | 2.0671 | | 2.3268 | 2.3268 | H5 | 1.5195 | 3.0433 | 2.3268 | 2.3268 | | 2.6435 | H6 | 3.0433 | 1.5195 | 2.3268 | 2.3268 | 2.6435 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
Si1 |
Si2 |
H5 |
29.953 |
|
Si1 |
Si2 |
H6 |
90.250 |
Si2 |
Si1 |
H3 |
38.276 |
|
Si2 |
Si1 |
H4 |
38.276 |
H3 |
Si1 |
H4 |
76.192 |
|
H5 |
Si2 |
H6 |
60.297 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-31+G**
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Si |
0.223 |
|
|
|
2 |
Si |
0.223 |
|
|
|
3 |
H |
-0.144 |
|
|
|
4 |
H |
-0.144 |
|
|
|
5 |
H |
-0.079 |
|
|
|
6 |
H |
-0.079 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
0.000 |
0.000 |
0.847 |
0.847 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-27.265 |
0.000 |
0.000 |
y |
0.000 |
-32.881 |
0.000 |
z |
0.000 |
0.000 |
-33.587 |
|
Traceless |
| x | y | z |
x |
5.970 |
0.000 |
0.000 |
y |
0.000 |
-2.456 |
0.000 |
z |
0.000 |
0.000 |
-3.514 |
|
Polar |
3z2-r2 | -7.028 |
x2-y2 | 5.617 |
xy | 0.000 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
6.344 |
0.000 |
0.000 |
y |
0.000 |
13.252 |
0.000 |
z |
0.000 |
0.000 |
8.246 |
<r2> (average value of r
2) Å
2
<r2> |
77.951 |
(<r2>)1/2 |
8.829 |