Jump to
S1C2
S2C1
S2C2
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -131.307622 |
| Energy at 298.15K | -131.306897 |
| HF Energy | -131.307622 |
| Nuclear repulsion energy | 47.500789 |
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/6-311G**
| 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' |
3405 |
3270 |
42.41 |
|
|
|
| 2 |
A' |
1803 |
1732 |
38.79 |
|
|
|
| 3 |
A' |
1241 |
1192 |
8.05 |
|
|
|
| 4 |
A' |
466 |
448 |
10.15 |
|
|
|
| 5 |
A' |
346 |
332 |
37.63 |
|
|
|
| 6 |
A" |
455 |
437 |
1.21 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3858.1 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 3705.3 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/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.056 |
-1.215 |
0.000 |
| C2 |
0.000 |
0.087 |
0.000 |
| N3 |
-0.127 |
1.276 |
0.000 |
| H4 |
0.556 |
-2.160 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3036 | 2.4979 | 1.0691 |
C2 | 1.3036 | | 1.1955 | 2.3150 | N3 | 2.4979 | 1.1955 | | 3.5032 | H4 | 1.0691 | 2.3150 | 3.5032 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.344 |
|
C2 |
C1 |
H4 |
154.554 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -131.307281 |
| Energy at 298.15K | |
| HF Energy | -131.307281 |
| Nuclear repulsion energy | 47.553660 |
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/6-311G**
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
Σ |
3456 |
3319 |
69.54 |
|
|
|
| 2 |
Σ |
1745 |
1676 |
42.06 |
|
|
|
| 3 |
Σ |
1276 |
1225 |
5.87 |
|
|
|
| 4 |
Π |
455 |
437 |
0.42 |
|
|
|
| 4 |
Π |
455 |
437 |
0.42 |
|
|
|
| 5 |
Π |
231i |
222i |
48.24 |
|
|
|
| 5 |
Π |
231i |
222i |
48.24 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3462.7 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 3325.6 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/6-311G**
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.205 |
| C2 |
0.000 |
0.000 |
0.083 |
| N3 |
0.000 |
0.000 |
1.286 |
| H4 |
0.000 |
0.000 |
-2.270 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2884 | 2.4914 | 1.0648 |
C2 | 1.2884 | | 1.2031 | 2.3532 | N3 | 2.4914 | 1.2031 | | 3.5563 | H4 | 1.0648 | 2.3532 | 3.5563 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
180.000 |
|
C2 |
C1 |
H4 |
180.000 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.051 |
|
|
|
| 2 |
C |
0.028 |
|
|
|
| 3 |
N |
-0.249 |
|
|
|
| 4 |
H |
0.170 |
|
|
|
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 |
-3.258 |
3.258 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.206 |
0.000 |
0.000 |
| y |
0.000 |
-17.206 |
0.000 |
| z |
0.000 |
0.000 |
-15.383 |
|
| Traceless |
| | x | y | z |
| x |
-0.911 |
0.000 |
0.000 |
| y |
0.000 |
-0.911 |
0.000 |
| z |
0.000 |
0.000 |
1.822 |
|
| Polar |
| 3z2-r2 | 3.644 |
| 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 |
1.915 |
0.000 |
0.000 |
| y |
0.000 |
1.915 |
0.000 |
| z |
0.000 |
0.000 |
6.339 |
<r2> (average value of r
2) Å
2
| <r2> |
35.857 |
| (<r2>)1/2 |
5.988 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -131.275356 |
| Energy at 298.15K | -131.274822 |
| HF Energy | -131.275356 |
| Nuclear repulsion energy | 47.182294 |
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/6-311G**
| 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' |
3090 |
2967 |
6.01 |
|
|
|
| 2 |
A' |
2123 |
2039 |
22.02 |
|
|
|
| 3 |
A' |
1100 |
1056 |
34.83 |
|
|
|
| 4 |
A' |
937 |
900 |
48.13 |
|
|
|
| 5 |
A' |
462 |
443 |
25.20 |
|
|
|
| 6 |
A" |
324 |
311 |
10.80 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4017.2 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 3858.2 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/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.054 |
-1.278 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.202 |
1.249 |
0.000 |
| H4 |
1.095 |
-1.631 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3707 | 2.5398 | 1.0997 |
C2 | 1.3707 | | 1.1748 | 2.0418 | N3 | 2.5398 | 1.1748 | | 3.1593 | H4 | 1.0997 | 2.0418 | 3.1593 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.035 |
|
|
|
| 2 |
C |
0.091 |
|
|
|
| 3 |
N |
-0.226 |
|
|
|
| 4 |
H |
0.171 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.771 |
-1.415 |
0.000 |
2.267 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.980 |
-2.536 |
0.000 |
| y |
-2.536 |
-20.937 |
0.000 |
| z |
0.000 |
0.000 |
-15.825 |
|
| Traceless |
| | x | y | z |
| x |
1.401 |
-2.536 |
0.000 |
| y |
-2.536 |
-4.534 |
0.000 |
| z |
0.000 |
0.000 |
3.134 |
|
| Polar |
| 3z2-r2 | 6.267 |
| x2-y2 | 3.957 |
| xy | -2.536 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.581 |
-0.617 |
0.000 |
| y |
-0.617 |
6.325 |
0.000 |
| z |
0.000 |
0.000 |
2.434 |
<r2> (average value of r
2) Å
2
| <r2> |
36.122 |
| (<r2>)1/2 |
6.010 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -131.275356 |
| Energy at 298.15K | -131.274822 |
| HF Energy | -131.275356 |
| Nuclear repulsion energy | 47.182294 |
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/6-311G**
Geometric Data calculated at HSEh1PBE/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability