Vibrational Frequencies calculated at BLYP/aug-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 |
3060 |
3050 |
12.21 |
|
|
|
| 2 |
A1 |
2791 |
2781 |
18.60 |
|
|
|
| 3 |
A1 |
1472 |
1467 |
53.75 |
|
|
|
| 4 |
A1 |
1247 |
1243 |
8.17 |
|
|
|
| 5 |
B1 |
706 |
704 |
75.81 |
|
|
|
| 6 |
B1 |
609 |
607 |
1.48 |
|
|
|
| 7 |
B2 |
3111 |
3101 |
1.47 |
|
|
|
| 8 |
B2 |
903 |
900 |
32.95 |
|
|
|
| 9 |
B2 |
410 |
408 |
1.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7154.7 cm
-1
Scaled (by 0.9966) Zero Point Vibrational Energy (zpe) 7130.4 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 BLYP/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.604 |
|
|
|
| 2 |
B |
-0.145 |
|
|
|
| 3 |
H |
0.358 |
|
|
|
| 4 |
H |
0.358 |
|
|
|
| 5 |
H |
0.032 |
|
|
|
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 |
-0.504 |
0.504 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.394 |
0.000 |
0.000 |
| y |
0.000 |
-12.011 |
0.000 |
| z |
0.000 |
0.000 |
-11.937 |
|
| Traceless |
| | x | y | z |
| x |
-4.420 |
0.000 |
0.000 |
| y |
0.000 |
2.155 |
0.000 |
| z |
0.000 |
0.000 |
2.266 |
|
| Polar |
| 3z2-r2 | 4.531 |
| x2-y2 | -4.383 |
| 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 |
4.512 |
0.000 |
0.000 |
| y |
0.000 |
3.844 |
0.000 |
| z |
0.000 |
0.000 |
6.126 |
<r2> (average value of r
2) Å
2
| <r2> |
21.938 |
| (<r2>)1/2 |
4.684 |