Vibrational Frequencies calculated at B1B95/6-31+G**
| 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 |
3267 |
3125 |
86.98 |
|
|
|
| 2 |
A1 |
1566 |
1498 |
0.73 |
|
|
|
| 3 |
A1 |
1004 |
960 |
60.39 |
|
|
|
| 4 |
E |
3307 |
3163 |
0.40 |
|
|
|
| 4 |
E |
3307 |
3163 |
0.40 |
|
|
|
| 5 |
E |
1668 |
1595 |
11.56 |
|
|
|
| 5 |
E |
1668 |
1595 |
11.56 |
|
|
|
| 6 |
E |
1175 |
1124 |
32.37 |
|
|
|
| 6 |
E |
1175 |
1124 |
32.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 9067.4 cm
-1
Scaled (by 0.9566) Zero Point Vibrational Energy (zpe) 8673.9 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 B1B95/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
N |
-0.485 |
|
|
|
| 2 |
O |
-0.522 |
|
|
|
| 3 |
H |
0.336 |
|
|
|
| 4 |
H |
0.336 |
|
|
|
| 5 |
H |
0.336 |
|
|
|
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 |
-5.726 |
5.726 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.783 |
0.000 |
0.000 |
| y |
0.000 |
-11.783 |
0.000 |
| z |
0.000 |
0.000 |
-13.158 |
|
| Traceless |
| | x | y | z |
| x |
0.687 |
0.000 |
0.000 |
| y |
0.000 |
0.687 |
0.000 |
| z |
0.000 |
0.000 |
-1.375 |
|
| Polar |
| 3z2-r2 | -2.750 |
| 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 |
2.043 |
0.000 |
0.000 |
| y |
0.000 |
2.043 |
0.000 |
| z |
0.000 |
0.000 |
3.161 |
<r2> (average value of r
2) Å
2
| <r2> |
20.361 |
| (<r2>)1/2 |
4.512 |