Vibrational Frequencies calculated at HSEh1PBE/3-21G*
| 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' |
1539 |
1477 |
145.94 |
|
|
|
| 2 |
A' |
1158 |
1111 |
250.72 |
|
|
|
| 3 |
A' |
800 |
768 |
133.49 |
|
|
|
| 4 |
A' |
786 |
754 |
7.96 |
|
|
|
| 5 |
A' |
602 |
577 |
5.30 |
|
|
|
| 6 |
A' |
425 |
408 |
1.14 |
|
|
|
| 7 |
A' |
238 |
229 |
0.01 |
|
|
|
| 8 |
A" |
647 |
621 |
12.11 |
|
|
|
| 9 |
A" |
123 |
118 |
0.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3158.5 cm
-1
Scaled (by 0.9599) Zero Point Vibrational Energy (zpe) 3031.8 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/3-21G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
Cl |
0.188 |
|
|
|
| 2 |
O |
-0.270 |
|
|
|
| 3 |
N |
0.554 |
|
|
|
| 4 |
O |
-0.242 |
|
|
|
| 5 |
O |
-0.231 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.753 |
-0.258 |
0.000 |
0.796 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-32.785 |
-0.568 |
0.000 |
| y |
-0.568 |
-35.571 |
0.000 |
| z |
0.000 |
0.000 |
-32.405 |
|
| Traceless |
| | x | y | z |
| x |
1.203 |
-0.568 |
0.000 |
| y |
-0.568 |
-2.976 |
0.000 |
| z |
0.000 |
0.000 |
1.773 |
|
| Polar |
| 3z2-r2 | 3.546 |
| x2-y2 | 2.786 |
| xy | -0.568 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
7.285 |
-0.173 |
0.000 |
| y |
-0.173 |
3.776 |
0.000 |
| z |
0.000 |
0.000 |
1.414 |
<r2> (average value of r
2) Å
2
| <r2> |
136.915 |
| (<r2>)1/2 |
11.701 |