Vibrational Frequencies calculated at HF/LANL2DZ
| 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 |
3436 |
3092 |
1.75 |
|
|
|
| 2 |
A1 |
3419 |
3076 |
29.29 |
|
|
|
| 3 |
A1 |
3392 |
3053 |
0.21 |
|
|
|
| 4 |
A1 |
1791 |
1612 |
46.91 |
|
|
|
| 5 |
A1 |
1654 |
1488 |
78.97 |
|
|
|
| 6 |
A1 |
1327 |
1194 |
64.25 |
|
|
|
| 7 |
A1 |
1289 |
1160 |
20.61 |
|
|
|
| 8 |
A1 |
1124 |
1011 |
8.24 |
|
|
|
| 9 |
A1 |
1092 |
983 |
1.28 |
|
|
|
| 10 |
A1 |
863 |
777 |
31.56 |
|
|
|
| 11 |
A1 |
560 |
504 |
6.86 |
|
|
|
| 12 |
A2 |
1122 |
1010 |
0.00 |
|
|
|
| 13 |
A2 |
962 |
866 |
0.00 |
|
|
|
| 14 |
A2 |
469 |
422 |
0.00 |
|
|
|
| 15 |
B1 |
1150 |
1035 |
0.91 |
|
|
|
| 16 |
B1 |
1053 |
947 |
14.68 |
|
|
|
| 17 |
B1 |
877 |
789 |
132.13 |
|
|
|
| 18 |
B1 |
779 |
701 |
33.13 |
|
|
|
| 19 |
B1 |
558 |
502 |
12.83 |
|
|
|
| 20 |
B1 |
264 |
237 |
0.40 |
|
|
|
| 21 |
B2 |
3432 |
3088 |
14.91 |
|
|
|
| 22 |
B2 |
3406 |
3065 |
15.48 |
|
|
|
| 23 |
B2 |
1793 |
1614 |
12.76 |
|
|
|
| 24 |
B2 |
1611 |
1450 |
3.86 |
|
|
|
| 25 |
B2 |
1470 |
1323 |
0.82 |
|
|
|
| 26 |
B2 |
1369 |
1232 |
0.35 |
|
|
|
| 27 |
B2 |
1273 |
1145 |
0.05 |
|
|
|
| 28 |
B2 |
1178 |
1060 |
8.87 |
|
|
|
| 29 |
B2 |
683 |
615 |
0.20 |
|
|
|
| 30 |
B2 |
417 |
375 |
4.71 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 21905.8 cm
-1
Scaled (by 0.8999) Zero Point Vibrational Energy (zpe) 19713.0 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 HF/LANL2DZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
F |
-0.361 |
|
|
|
| 2 |
C |
0.429 |
|
|
|
| 3 |
C |
-0.335 |
|
|
|
| 4 |
C |
-0.335 |
|
|
|
| 5 |
C |
-0.164 |
|
|
|
| 6 |
C |
-0.164 |
|
|
|
| 7 |
C |
-0.229 |
|
|
|
| 8 |
H |
0.250 |
|
|
|
| 9 |
H |
0.250 |
|
|
|
| 10 |
H |
0.219 |
|
|
|
| 11 |
H |
0.219 |
|
|
|
| 12 |
H |
0.221 |
|
|
|
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 |
-2.619 |
2.619 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-44.689 |
0.000 |
0.000 |
| y |
0.000 |
-34.025 |
0.000 |
| z |
0.000 |
0.000 |
-43.414 |
|
| Traceless |
| | x | y | z |
| x |
-5.970 |
0.000 |
0.000 |
| y |
0.000 |
10.027 |
0.000 |
| z |
0.000 |
0.000 |
-4.057 |
|
| Polar |
| 3z2-r2 | -8.114 |
| x2-y2 | -10.665 |
| 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 |
3.636 |
0.000 |
0.000 |
| y |
0.000 |
9.928 |
0.000 |
| z |
0.000 |
0.000 |
10.135 |
<r2> (average value of r
2) Å
2
| <r2> |
0.000 |
| (<r2>)1/2 |
0.000 |