Jump to
S1C2
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -2628.253900 |
| Energy at 298.15K | -2628.253538 |
| HF Energy | -2628.253900 |
| Nuclear repulsion energy | 304.071009 |
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 B97D3/6-311+G(3df,2p)
| 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' |
864 |
853 |
0.00 |
|
|
|
| 2 |
A2" |
251 |
248 |
21.04 |
|
|
|
| 3 |
E' |
973 |
960 |
80.63 |
|
|
|
| 3 |
E' |
973 |
960 |
80.64 |
|
|
|
| 4 |
E' |
335 |
331 |
19.63 |
|
|
|
| 4 |
E' |
335 |
331 |
19.63 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1866.1 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 1841.9 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 B97D3/6-311+G(3df,2p)
Point Group is D3h
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Se1 |
0.000 |
0.000 |
0.000 |
| O2 |
0.000 |
1.613 |
0.000 |
| O3 |
1.397 |
-0.807 |
0.000 |
| O4 |
-1.397 |
-0.807 |
0.000 |
Atom - Atom Distances (Å)
| |
Se1 |
O2 |
O3 |
O4 |
| Se1 | | 1.6130 | 1.6130 | 1.6130 |
O2 | 1.6130 | | 2.7938 | 2.7938 | O3 | 1.6130 | 2.7938 | | 2.7938 | O4 | 1.6130 | 2.7938 | 2.7938 | |
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 B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Se |
1.333 |
|
|
|
| 2 |
O |
-0.444 |
|
|
|
| 3 |
O |
-0.444 |
|
|
|
| 4 |
O |
-0.444 |
|
|
|
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 |
-37.466 |
0.000 |
0.000 |
| y |
0.000 |
-37.466 |
0.000 |
| z |
0.000 |
0.000 |
-30.394 |
|
| Traceless |
| | x | y | z |
| x |
-3.536 |
0.000 |
0.000 |
| y |
0.000 |
-3.536 |
0.000 |
| z |
0.000 |
0.000 |
7.072 |
|
| Polar |
| 3z2-r2 | 14.145 |
| 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 |
6.539 |
0.000 |
0.000 |
| y |
0.000 |
6.539 |
0.000 |
| z |
0.000 |
0.000 |
3.646 |
<r2> (average value of r
2) Å
2
| <r2> |
84.371 |
| (<r2>)1/2 |
9.185 |
Jump to
S1C1
Energy calculated at B97D3/6-311+G(3df,2p)
| | hartrees |
| Energy at 0K | -2628.253916 |
| Energy at 298.15K | -2628.253556 |
| HF Energy | -2628.253916 |
| Nuclear repulsion energy | 304.075174 |
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 B97D3/6-311+G(3df,2p)
| 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 |
974 |
961 |
80.71 |
|
|
|
| 2 |
A1 |
865 |
853 |
0.00 |
|
|
|
| 3 |
A1 |
336 |
332 |
19.58 |
|
|
|
| 4 |
B1 |
251 |
248 |
21.04 |
|
|
|
| 5 |
B2 |
973 |
960 |
80.57 |
|
|
|
| 6 |
B2 |
336 |
332 |
19.70 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1867.1 cm
-1
Scaled (by 0.987) Zero Point Vibrational Energy (zpe) 1842.9 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 B97D3/6-311+G(3df,2p)
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| Se1 |
0.000 |
0.000 |
-0.000 |
| O2 |
0.000 |
0.000 |
-1.613 |
| O3 |
0.000 |
1.397 |
0.807 |
| O4 |
0.000 |
-1.397 |
0.807 |
Atom - Atom Distances (Å)
| |
Se1 |
O2 |
O3 |
O4 |
| Se1 | | 1.6130 | 1.6130 | 1.6130 |
O2 | 1.6130 | | 2.7938 | 2.7938 | O3 | 1.6130 | 2.7938 | | 2.7937 | O4 | 1.6130 | 2.7938 | 2.7937 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
Se1 |
O3 |
125.257 |
|
O2 |
Se1 |
O4 |
125.257 |
| O3 |
Se1 |
O4 |
109.486 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B97D3/6-311+G(3df,2p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Se |
1.333 |
|
|
|
| 2 |
O |
-0.444 |
|
|
|
| 3 |
O |
-0.444 |
|
|
|
| 4 |
O |
-0.444 |
|
|
|
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 |
-30.393 |
0.000 |
0.000 |
| y |
0.000 |
-37.466 |
0.000 |
| z |
0.000 |
0.000 |
-37.466 |
|
| Traceless |
| | x | y | z |
| x |
7.072 |
0.000 |
0.000 |
| y |
0.000 |
-3.536 |
0.000 |
| z |
0.000 |
0.000 |
-3.536 |
|
| Polar |
| 3z2-r2 | -7.073 |
| x2-y2 | 7.072 |
| 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 |
3.646 |
0.000 |
0.000 |
| y |
0.000 |
6.538 |
0.000 |
| z |
0.000 |
0.000 |
6.539 |
<r2> (average value of r
2) Å
2
| <r2> |
84.369 |
| (<r2>)1/2 |
9.185 |