Vibrational Frequencies calculated at BLYP/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' |
3136 |
3141 |
2.49 |
|
|
|
| 2 |
A' |
3043 |
3048 |
6.88 |
|
|
|
| 3 |
A' |
2218 |
2222 |
110.83 |
|
|
|
| 4 |
A' |
1381 |
1384 |
0.52 |
|
|
|
| 5 |
A' |
998 |
999 |
21.02 |
|
|
|
| 6 |
A' |
953 |
954 |
0.92 |
|
|
|
| 7 |
A' |
724 |
725 |
0.01 |
|
|
|
| 8 |
A" |
865 |
866 |
24.94 |
|
|
|
| 9 |
A" |
817 |
818 |
30.86 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7066.8 cm
-1
Scaled (by 1.0016) Zero Point Vibrational Energy (zpe) 7078.1 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/cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.129 |
|
|
|
| 2 |
P |
0.073 |
|
|
|
| 3 |
H |
0.041 |
|
|
|
| 4 |
H |
0.044 |
|
|
|
| 5 |
H |
-0.030 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.388 |
0.773 |
0.000 |
0.865 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-19.806 |
0.863 |
0.000 |
| y |
0.863 |
-19.401 |
0.000 |
| z |
0.000 |
0.000 |
-21.285 |
|
| Traceless |
| | x | y | z |
| x |
0.536 |
0.863 |
0.000 |
| y |
0.863 |
1.145 |
0.000 |
| z |
0.000 |
0.000 |
-1.681 |
|
| Polar |
| 3z2-r2 | -3.362 |
| x2-y2 | -0.406 |
| xy | 0.863 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
4.852 |
0.420 |
-0.000 |
| y |
0.420 |
6.888 |
0.002 |
| z |
-0.000 |
0.002 |
2.697 |
<r2> (average value of r
2) Å
2
| <r2> |
35.206 |
| (<r2>)1/2 |
5.933 |