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S1C2
S1C3
Energy calculated at LSDA/6-31G
| | hartrees |
| Energy at 0K | -165.604469 |
| Energy at 298.15K | |
| HF Energy | -165.604469 |
| Nuclear repulsion energy | 49.305191 |
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 LSDA/6-31G
Geometric Data calculated at LSDA/6-31G
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
S1C3
Energy calculated at LSDA/6-31G
| | hartrees |
| Energy at 0K | -165.605568 |
| Energy at 298.15K | |
| HF Energy | -165.605568 |
| Nuclear repulsion energy | 49.612036 |
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 LSDA/6-31G
Geometric Data calculated at LSDA/6-31G
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S1C2
Energy calculated at LSDA/6-31G
| | hartrees |
| Energy at 0K | -165.605572 |
| Energy at 298.15K | -165.606408 |
| HF Energy | -165.605572 |
| Nuclear repulsion energy | 49.583776 |
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 LSDA/6-31G
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σg |
4011 |
3930 |
0.00 |
|
|
|
| 2 |
Σg |
796 |
779 |
0.00 |
|
|
|
| 3 |
Σu |
4009 |
3927 |
402.98 |
|
|
|
| 4 |
Σu |
1716 |
1681 |
383.20 |
|
|
|
| 5 |
Πg |
199 |
195 |
0.00 |
|
|
|
| 5 |
Πg |
199 |
195 |
0.00 |
|
|
|
| 6 |
Πu |
409 |
401 |
117.37 |
|
|
|
| 6 |
Πu |
409 |
401 |
117.37 |
|
|
|
| 7 |
Πu |
209 |
205 |
438.41 |
|
|
|
| 7 |
Πu |
209 |
205 |
438.41 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6082.7 cm
-1
Scaled (by 0.9797) Zero Point Vibrational Energy (zpe) 5959.2 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 LSDA/6-31G
Point Group is D∞h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Be1 |
0.000 |
0.000 |
0.000 |
| O2 |
0.000 |
0.000 |
1.390 |
| O3 |
0.000 |
0.000 |
-1.390 |
| H4 |
0.000 |
0.000 |
2.346 |
| H5 |
0.000 |
0.000 |
-2.346 |
Atom - Atom Distances (Å)
| |
Be1 |
O2 |
O3 |
H4 |
H5 |
| Be1 | | 1.3902 | 1.3902 | 2.3461 | 2.3461 |
O2 | 1.3902 | | 2.7803 | 0.9559 | 3.7363 | O3 | 1.3902 | 2.7803 | | 3.7363 | 0.9559 | H4 | 2.3461 | 0.9559 | 3.7363 | | 4.6922 | H5 | 2.3461 | 3.7363 | 0.9559 | 4.6922 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| Be1 |
O2 |
H4 |
180.000 |
|
Be1 |
O3 |
H5 |
180.000 |
| O2 |
Be1 |
O3 |
180.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/6-31G
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Be |
0.498 |
|
|
|
| 2 |
O |
-0.649 |
|
|
|
| 3 |
O |
-0.649 |
|
|
|
| 4 |
H |
0.400 |
|
|
|
| 5 |
H |
0.400 |
|
|
|
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 |
-16.585 |
0.000 |
0.000 |
| y |
0.000 |
-16.585 |
0.000 |
| z |
0.000 |
0.000 |
-6.058 |
|
| Traceless |
| | x | y | z |
| x |
-5.263 |
0.000 |
0.000 |
| y |
0.000 |
-5.263 |
0.000 |
| z |
0.000 |
0.000 |
10.527 |
|
| Polar |
| 3z2-r2 | 21.054 |
| x2-y2 | 0.000 |
| 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 |
1.353 |
0.000 |
0.000 |
| y |
0.000 |
1.353 |
0.000 |
| z |
0.000 |
0.000 |
3.896 |
<r2> (average value of r
2) Å
2
| <r2> |
50.096 |
| (<r2>)1/2 |
7.078 |