Jump to
S1C2
S2C1
S2C2
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -130.724682 |
| Energy at 298.15K | -130.724073 |
| HF Energy | -130.724682 |
| Nuclear repulsion energy | 47.487199 |
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 HF/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 |
A' |
3469 |
3159 |
19.62 |
|
|
|
| 2 |
A' |
1653 |
1505 |
147.27 |
|
|
|
| 3 |
A' |
1202 |
1095 |
5.09 |
|
|
|
| 4 |
A' |
624 |
568 |
18.47 |
|
|
|
| 5 |
A' |
389 |
354 |
0.42 |
|
|
|
| 6 |
A" |
417 |
379 |
0.08 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3877.0 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 3529.7 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 HF/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.216 |
-1.208 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.323 |
1.237 |
0.000 |
| H4 |
0.965 |
-1.961 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3184 | 2.5034 | 1.0619 |
C2 | 1.3184 | | 1.1888 | 2.2686 | N3 | 2.5034 | 1.1888 | | 3.4469 | H4 | 1.0619 | 2.2686 | 3.4469 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
173.662 |
|
C2 |
C1 |
H4 |
144.533 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -130.722653 |
| Energy at 298.15K | |
| HF Energy | -130.722653 |
| Nuclear repulsion energy | 47.579449 |
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 HF/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 |
Σ |
3542 |
3225 |
58.39 |
|
|
|
| 2 |
Σ |
1564 |
1424 |
136.18 |
|
|
|
| 3 |
Σ |
1255 |
1142 |
0.00 |
|
|
|
| 4 |
Π |
413 |
376 |
0.21 |
|
|
|
| 4 |
Π |
413 |
376 |
0.21 |
|
|
|
| 5 |
Π |
421i |
383i |
43.39 |
|
|
|
| 5 |
Π |
421i |
383i |
43.39 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3172.7 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 2888.5 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 HF/aug-cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.204 |
| C2 |
0.000 |
0.000 |
0.079 |
| N3 |
0.000 |
0.000 |
1.287 |
| H4 |
0.000 |
0.000 |
-2.260 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2835 | 2.4910 | 1.0557 |
C2 | 1.2835 | | 1.2076 | 2.3392 | N3 | 2.4910 | 1.2076 | | 3.5468 | H4 | 1.0557 | 2.3392 | 3.5468 | |
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 HF/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.856 |
|
|
|
| 2 |
C |
0.790 |
|
|
|
| 3 |
N |
-0.516 |
|
|
|
| 4 |
H |
0.581 |
|
|
|
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 |
-3.210 |
3.210 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.461 |
0.000 |
0.000 |
| y |
0.000 |
-17.461 |
0.000 |
| z |
0.000 |
0.000 |
-15.697 |
|
| Traceless |
| | x | y | z |
| x |
-0.882 |
0.000 |
0.000 |
| y |
0.000 |
-0.882 |
0.000 |
| z |
0.000 |
0.000 |
1.765 |
|
| Polar |
| 3z2-r2 | 3.529 |
| 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 |
2.976 |
0.000 |
0.000 |
| y |
0.000 |
2.976 |
0.000 |
| z |
0.000 |
0.000 |
6.295 |
<r2> (average value of r
2) Å
2
| <r2> |
35.976 |
| (<r2>)1/2 |
5.998 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -130.666424 |
| Energy at 298.15K | -130.665968 |
| HF Energy | -130.666424 |
| Nuclear repulsion energy | 47.525840 |
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 HF/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 |
A' |
3224 |
2935 |
3.78 |
|
|
|
| 2 |
A' |
2339 |
2129 |
37.86 |
|
|
|
| 3 |
A' |
1135 |
1033 |
71.24 |
|
|
|
| 4 |
A' |
1016 |
925 |
19.83 |
|
|
|
| 5 |
A' |
489 |
445 |
27.56 |
|
|
|
| 6 |
A" |
355 |
323 |
16.82 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4279.1 cm
-1
Scaled (by 0.9104) Zero Point Vibrational Energy (zpe) 3895.7 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 HF/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.253 |
-1.266 |
0.000 |
| C2 |
0.000 |
0.112 |
0.000 |
| N3 |
0.118 |
1.246 |
0.000 |
| H4 |
0.693 |
-1.801 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.4012 | 2.5391 | 1.0864 |
C2 | 1.4012 | | 1.1398 | 2.0349 | N3 | 2.5391 | 1.1398 | | 3.1009 | H4 | 1.0864 | 2.0349 | 3.1009 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HF/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.535 |
|
|
|
| 2 |
C |
0.328 |
|
|
|
| 3 |
N |
-0.235 |
|
|
|
| 4 |
H |
0.441 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.357 |
-2.174 |
0.000 |
2.563 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-18.663 |
-3.419 |
0.000 |
| y |
-3.419 |
-20.225 |
0.000 |
| z |
0.000 |
0.000 |
-16.193 |
|
| Traceless |
| | x | y | z |
| x |
-0.453 |
-3.419 |
0.000 |
| y |
-3.419 |
-2.797 |
0.000 |
| z |
0.000 |
0.000 |
3.251 |
|
| Polar |
| 3z2-r2 | 6.501 |
| x2-y2 | 1.563 |
| xy | -3.419 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.231 |
0.306 |
0.000 |
| y |
0.306 |
6.199 |
0.000 |
| z |
0.000 |
0.000 |
3.347 |
<r2> (average value of r
2) Å
2
| <r2> |
36.230 |
| (<r2>)1/2 |
6.019 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at HF/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -130.666424 |
| Energy at 298.15K | -130.665968 |
| HF Energy | -130.666424 |
| Nuclear repulsion energy | 47.525840 |
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 HF/aug-cc-pVTZ
Geometric Data calculated at HF/aug-cc-pVTZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability