Jump to
S1C2
Energy calculated at HSEh1PBE/aug-cc-pVDZ
| hartrees |
Energy at 0K | -759.130920 |
Energy at 298.15K | |
HF Energy | -759.130920 |
Nuclear repulsion energy | 180.572786 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HSEh1PBE/aug-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 |
A1' |
574 |
552 |
0.00 |
|
|
|
2 |
A2" |
411 |
396 |
22.93 |
|
|
|
3 |
E' |
105i |
101i |
2.55 |
|
|
|
3 |
E' |
105i |
101i |
2.55 |
|
|
|
4 |
E' |
598 |
576 |
287.33 |
|
|
|
4 |
E' |
598 |
576 |
287.32 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 986.0 cm
-1
Scaled (by 0.9622) Zero Point Vibrational Energy (zpe) 948.7 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.
Geometric Data calculated at HSEh1PBE/aug-cc-pVDZ
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.000 |
F2 |
0.000 |
1.756 |
0.000 |
F3 |
1.521 |
-0.878 |
0.000 |
F4 |
-1.521 |
-0.878 |
0.000 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.7563 | 1.7563 | 1.7563 |
F2 | 1.7563 | | 3.0419 | 3.0419 | F3 | 1.7563 | 3.0419 | | 3.0419 | F4 | 1.7563 | 3.0419 | 3.0419 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
120.000 |
|
F2 |
Cl1 |
F4 |
120.000 |
F3 |
Cl1 |
F4 |
120.000 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.188 |
|
|
|
2 |
F |
-0.396 |
|
|
|
3 |
F |
-0.396 |
|
|
|
4 |
F |
-0.396 |
|
|
|
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 |
0.000 |
0.000 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-30.164 |
0.000 |
0.000 |
y |
0.000 |
-30.164 |
0.000 |
z |
0.000 |
0.000 |
-26.778 |
|
Traceless |
| x | y | z |
x |
-1.693 |
0.000 |
0.000 |
y |
0.000 |
-1.693 |
0.000 |
z |
0.000 |
0.000 |
3.386 |
|
Polar |
3z2-r2 | 6.772 |
x2-y2 | 0.000 |
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 |
5.844 |
0.000 |
0.000 |
y |
0.000 |
5.844 |
0.000 |
z |
0.000 |
0.000 |
2.526 |
<r2> (average value of r
2) Å
2
<r2> |
101.416 |
(<r2>)1/2 |
10.071 |
Jump to
S1C1
Energy calculated at HSEh1PBE/aug-cc-pVDZ
| hartrees |
Energy at 0K | -759.159814 |
Energy at 298.15K | -759.161132 |
HF Energy | -759.159814 |
Nuclear repulsion energy | 191.838108 |
The energy at 298.15K was derived from the energy at 0K
and an integrated heat capacity that used the calculated vibrational frequencies.
Vibrational Frequencies calculated at HSEh1PBE/aug-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 |
A1 |
774 |
745 |
45.77 |
|
|
|
2 |
A1 |
546 |
525 |
3.64 |
|
|
|
3 |
A1 |
302 |
290 |
12.90 |
|
|
|
4 |
B1 |
319 |
307 |
16.86 |
|
|
|
5 |
B2 |
730 |
702 |
505.22 |
|
|
|
6 |
B2 |
401 |
386 |
0.36 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1535.0 cm
-1
Scaled (by 0.9622) Zero Point Vibrational Energy (zpe) 1477.0 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.
Geometric Data calculated at HSEh1PBE/aug-cc-pVDZ
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.367 |
F2 |
0.000 |
0.000 |
-1.270 |
F3 |
0.000 |
1.735 |
0.289 |
F4 |
0.000 |
-1.735 |
0.289 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.6369 | 1.7363 | 1.7363 |
F2 | 1.6369 | | 2.3319 | 2.3319 | F3 | 1.7363 | 2.3319 | | 3.4692 | F4 | 1.7363 | 2.3319 | 3.4692 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
87.415 |
|
F2 |
Cl1 |
F4 |
87.415 |
F3 |
Cl1 |
F4 |
174.830 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/aug-cc-pVDZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.224 |
|
|
|
2 |
F |
-0.340 |
|
|
|
3 |
F |
-0.442 |
|
|
|
4 |
F |
-0.442 |
|
|
|
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 |
0.686 |
0.686 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-26.534 |
0.000 |
0.000 |
y |
0.000 |
-33.407 |
0.000 |
z |
0.000 |
0.000 |
-25.651 |
|
Traceless |
| x | y | z |
x |
2.996 |
0.000 |
0.000 |
y |
0.000 |
-7.315 |
0.000 |
z |
0.000 |
0.000 |
4.319 |
|
Polar |
3z2-r2 | 8.638 |
x2-y2 | 6.874 |
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 |
2.510 |
0.000 |
0.000 |
y |
0.000 |
6.198 |
0.000 |
z |
0.000 |
0.000 |
3.660 |
<r2> (average value of r
2) Å
2
<r2> |
90.281 |
(<r2>)1/2 |
9.502 |