Jump to
S1C2
Energy calculated at HSEh1PBE/aug-cc-pVTZ
| hartrees |
Energy at 0K | -759.231820 |
Energy at 298.15K | |
HF Energy | -759.231820 |
Nuclear repulsion energy | 183.191078 |
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-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' |
578 |
556 |
0.00 |
|
|
|
2 |
A2" |
435 |
418 |
23.03 |
|
|
|
3 |
E' |
126i |
121i |
3.81 |
|
|
|
3 |
E' |
126i |
121i |
3.81 |
|
|
|
4 |
E' |
584 |
562 |
307.64 |
|
|
|
4 |
E' |
584 |
562 |
307.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 964.0 cm
-1
Scaled (by 0.9618) Zero Point Vibrational Energy (zpe) 927.2 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-pVTZ
Point Group is D3h
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.000 |
F2 |
0.000 |
1.731 |
0.000 |
F3 |
1.499 |
-0.866 |
0.000 |
F4 |
-1.499 |
-0.866 |
0.000 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.7312 | 1.7312 | 1.7312 |
F2 | 1.7312 | | 2.9985 | 2.9985 | F3 | 1.7312 | 2.9985 | | 2.9985 | F4 | 1.7312 | 2.9985 | 2.9985 | |
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-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.117 |
|
|
|
2 |
F |
-0.372 |
|
|
|
3 |
F |
-0.372 |
|
|
|
4 |
F |
-0.372 |
|
|
|
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 |
-29.947 |
0.000 |
0.000 |
y |
0.000 |
-29.947 |
0.000 |
z |
0.000 |
0.000 |
-26.614 |
|
Traceless |
| x | y | z |
x |
-1.666 |
0.000 |
0.000 |
y |
0.000 |
-1.666 |
0.000 |
z |
0.000 |
0.000 |
3.333 |
|
Polar |
3z2-r2 | 6.665 |
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 |
5.746 |
0.000 |
0.000 |
y |
0.000 |
5.746 |
0.000 |
z |
0.000 |
0.000 |
2.685 |
<r2> (average value of r
2) Å
2
<r2> |
98.928 |
(<r2>)1/2 |
9.946 |
Jump to
S1C1
Energy calculated at HSEh1PBE/aug-cc-pVTZ
| hartrees |
Energy at 0K | -759.265688 |
Energy at 298.15K | -759.267078 |
HF Energy | -759.265688 |
Nuclear repulsion energy | 195.075102 |
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-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 |
788 |
757 |
50.26 |
|
|
|
2 |
A1 |
548 |
527 |
3.80 |
|
|
|
3 |
A1 |
324 |
311 |
12.77 |
|
|
|
4 |
B1 |
334 |
321 |
16.08 |
|
|
|
5 |
B2 |
715 |
688 |
522.95 |
|
|
|
6 |
B2 |
431 |
414 |
0.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 1569.6 cm
-1
Scaled (by 0.9618) Zero Point Vibrational Energy (zpe) 1509.6 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-pVTZ
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
Cl1 |
0.000 |
0.000 |
0.359 |
F2 |
0.000 |
0.000 |
-1.246 |
F3 |
0.000 |
1.708 |
0.284 |
F4 |
0.000 |
-1.708 |
0.284 |
Atom - Atom Distances (Å)
|
Cl1 |
F2 |
F3 |
F4 |
Cl1 | | 1.6057 | 1.7096 | 1.7096 |
F2 | 1.6057 | | 2.2930 | 2.2930 | F3 | 1.7096 | 2.2930 | | 3.4159 | F4 | 1.7096 | 2.2930 | 3.4159 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
F2 |
Cl1 |
F3 |
87.460 |
|
F2 |
Cl1 |
F4 |
87.460 |
F3 |
Cl1 |
F4 |
174.920 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/aug-cc-pVTZ
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
Cl |
1.084 |
|
|
|
2 |
F |
-0.274 |
|
|
|
3 |
F |
-0.405 |
|
|
|
4 |
F |
-0.405 |
|
|
|
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 |
0.603 |
0.603 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-26.356 |
0.000 |
0.000 |
y |
0.000 |
-33.020 |
0.000 |
z |
0.000 |
0.000 |
-25.609 |
|
Traceless |
| x | y | z |
x |
2.958 |
0.000 |
0.000 |
y |
0.000 |
-7.038 |
0.000 |
z |
0.000 |
0.000 |
4.079 |
|
Polar |
3z2-r2 | 8.158 |
x2-y2 | 6.664 |
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 |
2.644 |
0.000 |
0.000 |
y |
0.000 |
5.937 |
0.000 |
z |
0.000 |
0.000 |
3.668 |
<r2> (average value of r
2) Å
2
<r2> |
87.823 |
(<r2>)1/2 |
9.371 |