Jump to
S1C2
Energy calculated at wB97X-D/TZVP
| | hartrees |
| Energy at 0K | -2627.128823 |
| Energy at 298.15K | -2627.128569 |
| HF Energy | -2627.128823 |
| Nuclear repulsion energy | 308.604349 |
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 wB97X-D/TZVP
| 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' |
936 |
894 |
0.00 |
|
|
|
| 2 |
A2" |
285 |
273 |
31.36 |
|
|
|
| 3 |
E' |
1042 |
995 |
107.56 |
|
|
|
| 3 |
E' |
1042 |
995 |
107.52 |
|
|
|
| 4 |
E' |
345 |
329 |
32.75 |
|
|
|
| 4 |
E' |
345 |
329 |
32.75 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1997.1 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 1907.3 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 wB97X-D/TZVP
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Se1 |
0.000 |
0.000 |
0.000 |
| O2 |
0.000 |
1.589 |
0.000 |
| O3 |
1.376 |
-0.795 |
0.000 |
| O4 |
-1.376 |
-0.795 |
0.000 |
Atom - Atom Distances (Å)
| |
Se1 |
O2 |
O3 |
O4 |
| Se1 | | 1.5893 | 1.5893 | 1.5893 |
O2 | 1.5893 | | 2.7528 | 2.7528 | O3 | 1.5893 | 2.7528 | | 2.7528 | O4 | 1.5893 | 2.7528 | 2.7528 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
Se1 |
O3 |
120.000 |
|
O2 |
Se1 |
O4 |
120.000 |
| O3 |
Se1 |
O4 |
120.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Se |
1.181 |
|
|
|
| 2 |
O |
-0.394 |
|
|
|
| 3 |
O |
-0.394 |
|
|
|
| 4 |
O |
-0.394 |
|
|
|
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 |
-38.368 |
0.000 |
0.000 |
| y |
0.000 |
-38.368 |
0.000 |
| z |
0.000 |
0.000 |
-29.997 |
|
| Traceless |
| | x | y | z |
| x |
-4.185 |
0.000 |
0.000 |
| y |
0.000 |
-4.185 |
0.000 |
| z |
0.000 |
0.000 |
8.371 |
|
| Polar |
| 3z2-r2 | 16.742 |
| 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 |
5.467 |
0.000 |
0.000 |
| y |
0.000 |
5.465 |
0.000 |
| z |
0.000 |
0.000 |
2.507 |
<r2> (average value of r
2) Å
2
| <r2> |
82.843 |
| (<r2>)1/2 |
9.102 |
Jump to
S1C1
Energy calculated at wB97X-D/TZVP
| | hartrees |
| Energy at 0K | -2627.128820 |
| Energy at 298.15K | -2627.128566 |
| HF Energy | -2627.128820 |
| Nuclear repulsion energy | 308.599985 |
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 wB97X-D/TZVP
| 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 |
1041 |
994 |
107.40 |
|
|
|
| 2 |
A1 |
936 |
894 |
0.00 |
|
|
|
| 3 |
A1 |
345 |
329 |
32.78 |
|
|
|
| 4 |
B1 |
285 |
272 |
31.36 |
|
|
|
| 5 |
B2 |
1042 |
995 |
107.57 |
|
|
|
| 6 |
B2 |
345 |
329 |
32.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1996.8 cm
-1
Scaled (by 0.955) Zero Point Vibrational Energy (zpe) 1907.0 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 wB97X-D/TZVP
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Se1 |
0.000 |
0.000 |
0.012 |
| O2 |
0.000 |
0.000 |
-1.971 |
| O3 |
0.000 |
1.336 |
0.959 |
| O4 |
0.000 |
-1.336 |
0.959 |
Atom - Atom Distances (Å)
| |
Se1 |
O2 |
O3 |
O4 |
| Se1 | | 1.9831 | 1.6380 | 1.6380 |
O2 | 1.9831 | | 3.2206 | 3.2206 | O3 | 1.6380 | 3.2206 | | 2.6727 | O4 | 1.6380 | 3.2206 | 2.6727 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
Se1 |
O3 |
125.327 |
|
O2 |
Se1 |
O4 |
125.327 |
| O3 |
Se1 |
O4 |
109.346 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at wB97X-D/TZVP
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Se |
1.181 |
|
|
|
| 2 |
O |
-0.394 |
|
|
|
| 3 |
O |
-0.394 |
|
|
|
| 4 |
O |
-0.394 |
|
|
|
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 |
-0.002 |
0.002 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-29.997 |
0.000 |
0.000 |
| y |
0.000 |
-38.364 |
0.000 |
| z |
0.000 |
0.000 |
-38.371 |
|
| Traceless |
| | x | y | z |
| x |
8.370 |
0.000 |
0.000 |
| y |
0.000 |
-4.180 |
0.000 |
| z |
0.000 |
0.000 |
-4.190 |
|
| Polar |
| 3z2-r2 | -8.381 |
| x2-y2 | 8.367 |
| 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 |
2.507 |
0.000 |
0.000 |
| y |
0.000 |
5.464 |
0.000 |
| z |
0.000 |
0.000 |
5.469 |
<r2> (average value of r
2) Å
2
| <r2> |
82.844 |
| (<r2>)1/2 |
9.102 |