Jump to
S1C2
S2C1
S2C2
Energy calculated at PBE1PBE/6-311G*
| | hartrees |
| Energy at 0K | -131.292250 |
| Energy at 298.15K | -131.291579 |
| HF Energy | -131.292250 |
| Nuclear repulsion energy | 47.475531 |
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 PBE1PBE/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' |
3395 |
3254 |
29.54 |
|
|
|
| 2 |
A' |
1818 |
1743 |
38.61 |
|
|
|
| 3 |
A' |
1233 |
1182 |
8.69 |
|
|
|
| 4 |
A' |
489 |
469 |
23.47 |
|
|
|
| 5 |
A' |
386 |
370 |
24.92 |
|
|
|
| 6 |
A" |
454 |
436 |
1.30 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3887.8 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 3726.4 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 PBE1PBE/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.053 |
-1.219 |
0.000 |
| C2 |
0.000 |
0.088 |
0.000 |
| N3 |
-0.131 |
1.275 |
0.000 |
| H4 |
0.603 |
-2.137 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3077 | 2.5002 | 1.0706 |
C2 | 1.3077 | | 1.1940 | 2.3053 | N3 | 2.5002 | 1.1940 | | 3.4899 | H4 | 1.0706 | 2.3053 | 3.4899 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.995 |
|
C2 |
C1 |
H4 |
151.380 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at PBE1PBE/6-311G*
| | hartrees |
| Energy at 0K | -131.291601 |
| Energy at 298.15K | |
| HF Energy | -131.291601 |
| Nuclear repulsion energy | 47.538464 |
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 PBE1PBE/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 |
3457 |
3314 |
57.00 |
|
|
|
| 2 |
Σ |
1747 |
1675 |
42.08 |
|
|
|
| 3 |
Σ |
1276 |
1223 |
6.18 |
|
|
|
| 4 |
Π |
455 |
436 |
0.38 |
|
|
|
| 4 |
Π |
455 |
436 |
0.38 |
|
|
|
| 5 |
Π |
286i |
274i |
51.62 |
|
|
|
| 5 |
Π |
286i |
274i |
51.62 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3408.6 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 3267.2 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 PBE1PBE/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.206 |
| C2 |
0.000 |
0.000 |
0.083 |
| N3 |
0.000 |
0.000 |
1.286 |
| H4 |
0.000 |
0.000 |
-2.271 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2892 | 2.4922 | 1.0656 |
C2 | 1.2892 | | 1.2030 | 2.3549 | N3 | 2.4922 | 1.2030 | | 3.5579 | H4 | 1.0656 | 2.3549 | 3.5579 | |
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 PBE1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.063 |
|
|
|
| 2 |
C |
0.027 |
|
|
|
| 3 |
N |
-0.255 |
|
|
|
| 4 |
H |
0.291 |
|
|
|
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 |
-3.288 |
3.288 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.240 |
0.000 |
0.000 |
| y |
0.000 |
-17.240 |
0.000 |
| z |
0.000 |
0.000 |
-15.275 |
|
| Traceless |
| | x | y | z |
| x |
-0.983 |
0.000 |
0.000 |
| y |
0.000 |
-0.983 |
0.000 |
| z |
0.000 |
0.000 |
1.966 |
|
| Polar |
| 3z2-r2 | 3.931 |
| 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 |
1.899 |
0.000 |
0.000 |
| y |
0.000 |
1.899 |
0.000 |
| z |
0.000 |
0.000 |
6.300 |
<r2> (average value of r
2) Å
2
| <r2> |
35.868 |
| (<r2>)1/2 |
5.989 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at PBE1PBE/6-311G*
| | hartrees |
| Energy at 0K | -131.260587 |
| Energy at 298.15K | -131.260049 |
| HF Energy | -131.260587 |
| Nuclear repulsion energy | 47.162220 |
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 PBE1PBE/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' |
3096 |
2967 |
9.48 |
|
|
|
| 2 |
A' |
2126 |
2038 |
21.96 |
|
|
|
| 3 |
A' |
1098 |
1053 |
37.95 |
|
|
|
| 4 |
A' |
950 |
910 |
47.49 |
|
|
|
| 5 |
A' |
461 |
442 |
25.26 |
|
|
|
| 6 |
A" |
322 |
309 |
10.43 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4026.5 cm
-1
Scaled (by 0.9585) Zero Point Vibrational Energy (zpe) 3859.4 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 PBE1PBE/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.069 |
-1.278 |
0.000 |
| C2 |
0.000 |
0.093 |
0.000 |
| N3 |
-0.218 |
1.247 |
0.000 |
| H4 |
1.115 |
-1.618 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3720 | 2.5410 | 1.0999 |
C2 | 1.3720 | | 1.1749 | 2.0421 | N3 | 2.5410 | 1.1749 | | 3.1603 | H4 | 1.0999 | 2.0421 | 3.1603 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBE1PBE/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.139 |
|
|
|
| 2 |
C |
0.115 |
|
|
|
| 3 |
N |
-0.231 |
|
|
|
| 4 |
H |
0.256 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.815 |
-1.375 |
0.000 |
2.277 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.909 |
-2.530 |
0.000 |
| y |
-2.530 |
-21.050 |
0.000 |
| z |
0.000 |
0.000 |
-15.851 |
|
| Traceless |
| | x | y | z |
| x |
1.542 |
-2.530 |
0.000 |
| y |
-2.530 |
-4.670 |
0.000 |
| z |
0.000 |
0.000 |
3.128 |
|
| Polar |
| 3z2-r2 | 6.257 |
| x2-y2 | 4.142 |
| xy | -2.530 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.580 |
-0.665 |
0.000 |
| y |
-0.665 |
6.305 |
0.000 |
| z |
0.000 |
0.000 |
2.408 |
<r2> (average value of r
2) Å
2
| <r2> |
36.159 |
| (<r2>)1/2 |
6.013 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at PBE1PBE/6-311G*
| | hartrees |
| Energy at 0K | -131.260587 |
| Energy at 298.15K | -131.260049 |
| HF Energy | -131.260587 |
| Nuclear repulsion energy | 47.162220 |
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 PBE1PBE/6-311G*
Geometric Data calculated at PBE1PBE/6-311G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability