Vibrational Frequencies calculated at LSDA/aug-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 |
A |
3586 |
3552 |
64.13 |
|
|
|
| 2 |
A |
3313 |
3282 |
1.94 |
|
|
|
| 3 |
A |
1577 |
1562 |
158.64 |
|
|
|
| 4 |
A |
1498 |
1484 |
120.99 |
|
|
|
| 5 |
A |
1201 |
1190 |
107.54 |
|
|
|
| 6 |
A |
1109 |
1099 |
29.20 |
|
|
|
| 7 |
A |
728 |
721 |
3.80 |
|
|
|
| 8 |
A |
611 |
605 |
1.47 |
|
|
|
| 9 |
A |
343 |
340 |
177.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6982.4 cm
-1
Scaled (by 0.9906) Zero Point Vibrational Energy (zpe) 6916.7 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.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at LSDA/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
O |
-0.391 |
|
|
|
| 2 |
N |
0.041 |
|
|
|
| 3 |
N |
0.106 |
|
|
|
| 4 |
H |
0.111 |
|
|
|
| 5 |
H |
0.134 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
3.720 |
0.805 |
-0.003 |
3.807 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-15.485 |
0.412 |
-0.006 |
| y |
0.412 |
-17.365 |
-0.001 |
| z |
-0.006 |
-0.001 |
-18.018 |
|
| Traceless |
| | x | y | z |
| x |
2.206 |
0.412 |
-0.006 |
| y |
0.412 |
-0.613 |
-0.001 |
| z |
-0.006 |
-0.001 |
-1.593 |
|
| Polar |
| 3z2-r2 | -3.186 |
| x2-y2 | 1.880 |
| xy | 0.412 |
| xz | -0.006 |
| yz | -0.001 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
5.577 |
0.075 |
0.000 |
| y |
0.075 |
3.989 |
-0.000 |
| z |
0.000 |
-0.000 |
2.733 |
<r2> (average value of r
2) Å
2
| <r2> |
35.975 |
| (<r2>)1/2 |
5.998 |