Vibrational Frequencies calculated at HF/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 |
3338 |
3038 |
10.56 |
|
|
|
| 2 |
A1 |
2302 |
2095 |
871.11 |
|
|
|
| 3 |
A1 |
1561 |
1421 |
79.39 |
|
|
|
| 4 |
A1 |
1283 |
1168 |
38.18 |
|
|
|
| 5 |
B1 |
668 |
608 |
4.02 |
|
|
|
| 6 |
B1 |
553 |
503 |
166.50 |
|
|
|
| 7 |
B2 |
3473 |
3160 |
0.23 |
|
|
|
| 8 |
B2 |
1236 |
1125 |
4.25 |
|
|
|
| 9 |
B2 |
466 |
424 |
0.81 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7439.4 cm
-1
Scaled (by 0.9101) Zero Point Vibrational Energy (zpe) 6770.6 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 HF/cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.374 |
|
|
|
| 2 |
N |
0.202 |
|
|
|
| 3 |
N |
-0.104 |
|
|
|
| 4 |
H |
0.138 |
|
|
|
| 5 |
H |
0.138 |
|
|
|
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 |
-1.277 |
1.277 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.327 |
0.000 |
0.000 |
| y |
0.000 |
-15.570 |
0.000 |
| z |
0.000 |
0.000 |
-18.824 |
|
| Traceless |
| | x | y | z |
| x |
-2.129 |
0.000 |
0.000 |
| y |
0.000 |
3.505 |
0.000 |
| z |
0.000 |
0.000 |
-1.376 |
|
| Polar |
| 3z2-r2 | -2.752 |
| x2-y2 | -3.756 |
| 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 |
2.323 |
0.000 |
0.000 |
| y |
0.000 |
2.515 |
0.000 |
| z |
0.000 |
0.000 |
7.000 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |