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S1C2
Vibrational Frequencies calculated at B1B95/cc-pVTZ
Geometric Data calculated at B1B95/cc-pVTZ
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
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S1C1
Energy calculated at B1B95/cc-pVTZ
| | hartrees |
| Energy at 0K | -280.255683 |
| Energy at 298.15K | -280.257362 |
| Nuclear repulsion energy | 120.566781 |
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 B1B95/cc-pVTZ
| 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 |
1375 |
1316 |
42.25 |
|
|
|
| 2 |
A1 |
1138 |
1089 |
1.59 |
|
|
|
| 3 |
A1 |
171 |
164 |
2.10 |
|
|
|
| 4 |
B1 |
821 |
785 |
13.87 |
|
|
|
| 5 |
B2 |
1036 |
991 |
10.39 |
|
|
|
| 6 |
B2 |
413 |
395 |
24.20 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 2476.4 cm
-1
Scaled (by 0.9571) Zero Point Vibrational Energy (zpe) 2370.1 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 B1B95/cc-pVTZ
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| N1 |
0.000 |
0.000 |
0.033 |
| O2 |
0.000 |
0.000 |
1.237 |
| O3 |
0.000 |
1.040 |
-0.633 |
| O4 |
0.000 |
-1.040 |
-0.633 |
Atom - Atom Distances (Å)
| |
N1 |
O2 |
O3 |
O4 |
| N1 | | 1.2033 | 1.2350 | 1.2350 |
O2 | 1.2033 | | 2.1392 | 2.1392 | O3 | 1.2350 | 2.1392 | | 2.0797 | O4 | 1.2350 | 2.1392 | 2.0797 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| O2 |
N1 |
O3 |
122.647 |
|
O2 |
N1 |
O4 |
122.647 |
| O3 |
N1 |
O4 |
114.706 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.469 |
|
|
|
| 2 |
O |
-0.179 |
|
|
|
| 3 |
O |
-0.145 |
|
|
|
| 4 |
O |
-0.145 |
|
|
|
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 |
-0.105 |
0.105 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.738 |
0.000 |
0.000 |
| y |
0.000 |
-22.066 |
0.000 |
| z |
0.000 |
0.000 |
-22.567 |
|
| Traceless |
| | x | y | z |
| x |
2.579 |
0.000 |
0.000 |
| y |
0.000 |
-0.914 |
0.000 |
| z |
0.000 |
0.000 |
-1.665 |
|
| Polar |
| 3z2-r2 | -3.330 |
| x2-y2 | 2.328 |
| 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 |
1.517 |
0.000 |
0.000 |
| y |
0.000 |
4.647 |
0.000 |
| z |
0.000 |
0.000 |
4.133 |
<r2> (average value of r
2) Å
2
| <r2> |
49.353 |
| (<r2>)1/2 |
7.025 |