Vibrational Frequencies calculated at B3PW91/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 |
3200 |
3088 |
17.04 |
|
|
|
| 2 |
A1 |
2251 |
2172 |
351.77 |
|
|
|
| 3 |
A1 |
1415 |
1366 |
33.52 |
|
|
|
| 4 |
A1 |
1226 |
1183 |
0.82 |
|
|
|
| 5 |
B1 |
583 |
563 |
1.38 |
|
|
|
| 6 |
B1 |
398 |
384 |
142.84 |
|
|
|
| 7 |
B2 |
3337 |
3220 |
5.01 |
|
|
|
| 8 |
B2 |
1095 |
1057 |
1.26 |
|
|
|
| 9 |
B2 |
423 |
408 |
0.55 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 6964.2 cm
-1
Scaled (by 0.965) Zero Point Vibrational Energy (zpe) 6720.4 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 B3PW91/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.150 |
|
|
|
| 2 |
N |
0.144 |
|
|
|
| 3 |
N |
-0.154 |
|
|
|
| 4 |
H |
0.080 |
|
|
|
| 5 |
H |
0.080 |
|
|
|
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 |
-1.537 |
1.537 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.682 |
0.000 |
0.000 |
| y |
0.000 |
-15.190 |
0.000 |
| z |
0.000 |
0.000 |
-18.430 |
|
| Traceless |
| | x | y | z |
| x |
-1.873 |
0.000 |
0.000 |
| y |
0.000 |
3.366 |
0.000 |
| z |
0.000 |
0.000 |
-1.493 |
|
| Polar |
| 3z2-r2 | -2.987 |
| x2-y2 | -3.492 |
| 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 |
1.688 |
0.000 |
0.000 |
| y |
0.000 |
2.282 |
0.000 |
| z |
0.000 |
0.000 |
6.502 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |