Vibrational Frequencies calculated at HSEh1PBE/daug-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 |
A |
3632 |
3632 |
26.19 |
|
|
|
| 2 |
A |
1305 |
1305 |
0.00 |
|
|
|
| 3 |
A |
914 |
914 |
13.17 |
|
|
|
| 4 |
A |
720 |
720 |
90.60 |
|
|
|
| 5 |
A |
550 |
550 |
0.59 |
|
|
|
| 6 |
B |
3629 |
3629 |
160.03 |
|
|
|
| 7 |
B |
2249 |
2249 |
712.15 |
|
|
|
| 8 |
B |
913 |
913 |
428.94 |
|
|
|
| 9 |
B |
554 |
554 |
81.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7232.4 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 7232.4 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 HSEh1PBE/daug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.104 |
|
|
|
| 2 |
N |
-0.563 |
|
|
|
| 3 |
N |
-0.563 |
|
|
|
| 4 |
H |
0.510 |
|
|
|
| 5 |
H |
0.510 |
|
|
|
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 |
1.952 |
1.952 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.997 |
4.108 |
0.000 |
| y |
4.108 |
-16.309 |
0.000 |
| z |
0.000 |
0.000 |
-17.508 |
|
| Traceless |
| | x | y | z |
| x |
-0.089 |
4.108 |
0.000 |
| y |
4.108 |
0.944 |
0.000 |
| z |
0.000 |
0.000 |
-0.855 |
|
| Polar |
| 3z2-r2 | -1.710 |
| x2-y2 | -0.688 |
| xy | 4.108 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.129 |
0.242 |
0.000 |
| y |
0.242 |
6.755 |
0.000 |
| z |
0.000 |
0.000 |
3.102 |
<r2> (average value of r
2) Å
2
| <r2> |
38.728 |
| (<r2>)1/2 |
6.223 |