Vibrational Frequencies calculated at HSEh1PBE/aug-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 |
A' |
3471 |
3340 |
1.00 |
|
|
|
| 2 |
A' |
3152 |
3033 |
28.47 |
|
|
|
| 3 |
A' |
3044 |
2929 |
47.38 |
|
|
|
| 4 |
A' |
1729 |
1664 |
23.50 |
|
|
|
| 5 |
A' |
1479 |
1423 |
6.70 |
|
|
|
| 6 |
A' |
1364 |
1312 |
40.59 |
|
|
|
| 7 |
A' |
1068 |
1027 |
33.11 |
|
|
|
| 8 |
A" |
1162 |
1118 |
47.35 |
|
|
|
| 9 |
A" |
1101 |
1059 |
15.97 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 8784.5 cm
-1
Scaled (by 0.9622) Zero Point Vibrational Energy (zpe) 8452.5 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/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.634 |
|
|
|
| 2 |
N |
-0.249 |
|
|
|
| 3 |
H |
-0.163 |
|
|
|
| 4 |
H |
-0.234 |
|
|
|
| 5 |
H |
0.012 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.366 |
1.502 |
0.000 |
2.030 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-11.759 |
2.066 |
0.000 |
| y |
2.066 |
-12.853 |
0.000 |
| z |
0.000 |
0.000 |
-13.755 |
|
| Traceless |
| | x | y | z |
| x |
1.546 |
2.066 |
0.000 |
| y |
2.066 |
-0.096 |
0.000 |
| z |
0.000 |
0.000 |
-1.450 |
|
| Polar |
| 3z2-r2 | -2.899 |
| x2-y2 | 1.095 |
| xy | 2.066 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.260 |
0.110 |
0.000 |
| y |
0.110 |
4.357 |
0.000 |
| z |
0.000 |
0.000 |
2.499 |
<r2> (average value of r
2) Å
2
| <r2> |
19.726 |
| (<r2>)1/2 |
4.441 |