Vibrational Frequencies calculated at B1B95/cc-pVDZ
| 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 |
3122 |
3001 |
165.91 |
|
|
|
| 2 |
A1 |
1578 |
1517 |
0.51 |
|
|
|
| 3 |
A1 |
1027 |
987 |
113.65 |
|
|
|
| 4 |
E |
3081 |
2961 |
42.95 |
|
|
|
| 4 |
E |
3081 |
2961 |
42.97 |
|
|
|
| 5 |
E |
1633 |
1570 |
2.03 |
|
|
|
| 5 |
E |
1633 |
1570 |
2.03 |
|
|
|
| 6 |
E |
1194 |
1148 |
26.16 |
|
|
|
| 6 |
E |
1194 |
1148 |
26.15 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8771.2 cm
-1
Scaled (by 0.9612) Zero Point Vibrational Energy (zpe) 8430.9 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.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B1B95/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
0.268 |
|
|
|
| 2 |
O |
-0.584 |
|
|
|
| 3 |
H |
0.105 |
|
|
|
| 4 |
H |
0.105 |
|
|
|
| 5 |
H |
0.105 |
|
|
|
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 |
-4.997 |
4.997 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.176 |
0.000 |
0.000 |
| y |
0.000 |
-11.176 |
0.000 |
| z |
0.000 |
0.000 |
-12.267 |
|
| Traceless |
| | x | y | z |
| x |
0.545 |
0.000 |
0.000 |
| y |
0.000 |
0.545 |
0.000 |
| z |
0.000 |
0.000 |
-1.091 |
|
| Polar |
| 3z2-r2 | -2.181 |
| 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 |
1.653 |
0.000 |
0.000 |
| y |
0.000 |
1.653 |
0.000 |
| z |
0.000 |
0.000 |
2.916 |
<r2> (average value of r
2) Å
2
| <r2> |
19.740 |
| (<r2>)1/2 |
4.443 |