Vibrational Frequencies calculated at HSEh1PBE/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 |
A' |
3495 |
3337 |
0.75 |
|
|
|
| 2 |
A' |
3168 |
3025 |
30.20 |
|
|
|
| 3 |
A' |
3055 |
2917 |
48.97 |
|
|
|
| 4 |
A' |
1744 |
1665 |
27.77 |
|
|
|
| 5 |
A' |
1502 |
1434 |
4.99 |
|
|
|
| 6 |
A' |
1367 |
1306 |
32.59 |
|
|
|
| 7 |
A' |
1069 |
1021 |
37.83 |
|
|
|
| 8 |
A" |
1169 |
1116 |
56.40 |
|
|
|
| 9 |
A" |
1104 |
1054 |
17.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8836.1 cm
-1
Scaled (by 0.9548) Zero Point Vibrational Energy (zpe) 8436.7 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 HSEh1PBE/6-31+G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.190 |
|
|
|
| 2 |
N |
-0.359 |
|
|
|
| 3 |
H |
0.134 |
|
|
|
| 4 |
H |
0.154 |
|
|
|
| 5 |
H |
0.261 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.570 |
1.574 |
0.000 |
2.223 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.724 |
2.239 |
0.000 |
| y |
2.239 |
-12.895 |
0.000 |
| z |
0.000 |
0.000 |
-13.802 |
|
| Traceless |
| | x | y | z |
| x |
1.625 |
2.239 |
0.000 |
| y |
2.239 |
-0.132 |
0.000 |
| z |
0.000 |
0.000 |
-1.493 |
|
| Polar |
| 3z2-r2 | -2.986 |
| x2-y2 | 1.171 |
| xy | 2.239 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.782 |
0.106 |
0.000 |
| y |
0.106 |
4.153 |
0.000 |
| z |
0.000 |
0.000 |
1.897 |
<r2> (average value of r
2) Å
2
| <r2> |
19.708 |
| (<r2>)1/2 |
4.439 |