Jump to
S1C2
S2C1
S2C2
Energy calculated at mPW1PW91/6-311G**
| | hartrees |
| Energy at 0K | -131.415900 |
| Energy at 298.15K | -131.415191 |
| HF Energy | -131.415900 |
| Nuclear repulsion energy | 47.517817 |
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 mPW1PW91/6-311G**
| 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' |
3406 |
3258 |
39.95 |
|
|
|
| 2 |
A' |
1803 |
1725 |
39.40 |
|
|
|
| 3 |
A' |
1237 |
1184 |
8.66 |
|
|
|
| 4 |
A' |
471 |
450 |
12.46 |
|
|
|
| 5 |
A' |
358 |
343 |
33.67 |
|
|
|
| 6 |
A" |
455 |
435 |
1.23 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3864.6 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 3697.2 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 mPW1PW91/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.057 |
-1.216 |
0.000 |
| C2 |
0.000 |
0.087 |
0.000 |
| N3 |
-0.130 |
1.275 |
0.000 |
| H4 |
0.572 |
-2.152 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3045 | 2.4974 | 1.0683 |
C2 | 1.3045 | | 1.1943 | 2.3110 | N3 | 2.4974 | 1.1943 | | 3.4975 | H4 | 1.0683 | 2.3110 | 3.4975 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.226 |
|
C2 |
C1 |
H4 |
153.652 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at mPW1PW91/6-311G**
| | hartrees |
| Energy at 0K | -131.415511 |
| Energy at 298.15K | |
| HF Energy | -131.415511 |
| Nuclear repulsion energy | 47.575167 |
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 mPW1PW91/6-311G**
| 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 |
3462 |
3312 |
68.50 |
|
|
|
| 2 |
Σ |
1739 |
1664 |
42.46 |
|
|
|
| 3 |
Σ |
1275 |
1220 |
6.09 |
|
|
|
| 4 |
Π |
455 |
435 |
0.41 |
|
|
|
| 4 |
Π |
455 |
435 |
0.41 |
|
|
|
| 5 |
Π |
237i |
227i |
48.05 |
|
|
|
| 5 |
Π |
237i |
227i |
48.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3455.8 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 3306.1 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 mPW1PW91/6-311G**
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 |
-2.269 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2880 | 2.4905 | 1.0638 |
C2 | 1.2880 | | 1.2024 | 2.3518 | N3 | 2.4905 | 1.2024 | | 3.5543 | H4 | 1.0638 | 2.3518 | 3.5543 | |
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 mPW1PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.056 |
|
|
|
| 2 |
C |
0.037 |
|
|
|
| 3 |
N |
-0.259 |
|
|
|
| 4 |
H |
0.166 |
|
|
|
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 |
-3.263 |
3.263 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.166 |
0.000 |
0.000 |
| y |
0.000 |
-17.166 |
0.000 |
| z |
0.000 |
0.000 |
-15.371 |
|
| Traceless |
| | x | y | z |
| x |
-0.898 |
0.000 |
0.000 |
| y |
0.000 |
-0.898 |
0.000 |
| z |
0.000 |
0.000 |
1.796 |
|
| Polar |
| 3z2-r2 | 3.592 |
| 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 |
1.912 |
0.000 |
0.000 |
| y |
0.000 |
1.912 |
0.000 |
| z |
0.000 |
0.000 |
6.333 |
<r2> (average value of r
2) Å
2
| <r2> |
35.816 |
| (<r2>)1/2 |
5.985 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at mPW1PW91/6-311G**
| | hartrees |
| Energy at 0K | -131.383753 |
| Energy at 298.15K | -131.383220 |
| HF Energy | -131.383753 |
| Nuclear repulsion energy | 47.204202 |
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 mPW1PW91/6-311G**
| 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' |
3095 |
2961 |
6.34 |
|
|
|
| 2 |
A' |
2126 |
2034 |
22.22 |
|
|
|
| 3 |
A' |
1098 |
1050 |
37.20 |
|
|
|
| 4 |
A' |
943 |
902 |
45.30 |
|
|
|
| 5 |
A' |
461 |
441 |
25.13 |
|
|
|
| 6 |
A" |
324 |
310 |
10.72 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4023.5 cm
-1
Scaled (by 0.9567) Zero Point Vibrational Energy (zpe) 3849.3 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 mPW1PW91/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.050 |
-1.278 |
0.000 |
| C2 |
0.000 |
0.092 |
0.000 |
| N3 |
-0.198 |
1.249 |
0.000 |
| H4 |
1.090 |
-1.631 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3711 | 2.5392 | 1.0986 |
C2 | 1.3711 | | 1.1737 | 2.0394 | N3 | 2.5392 | 1.1737 | | 3.1556 | H4 | 1.0986 | 2.0394 | 3.1556 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at mPW1PW91/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.031 |
|
|
|
| 2 |
C |
0.098 |
|
|
|
| 3 |
N |
-0.236 |
|
|
|
| 4 |
H |
0.169 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.768 |
-1.426 |
0.000 |
2.271 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.955 |
-2.542 |
0.000 |
| y |
-2.542 |
-20.903 |
0.000 |
| z |
0.000 |
0.000 |
-15.788 |
|
| Traceless |
| | x | y | z |
| x |
1.390 |
-2.542 |
0.000 |
| y |
-2.542 |
-4.531 |
0.000 |
| z |
0.000 |
0.000 |
3.141 |
|
| Polar |
| 3z2-r2 | 6.282 |
| x2-y2 | 3.947 |
| xy | -2.542 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.574 |
-0.604 |
0.000 |
| y |
-0.604 |
6.319 |
0.000 |
| z |
0.000 |
0.000 |
2.430 |
<r2> (average value of r
2) Å
2
| <r2> |
36.080 |
| (<r2>)1/2 |
6.007 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at mPW1PW91/6-311G**
| | hartrees |
| Energy at 0K | -131.383753 |
| Energy at 298.15K | -131.383220 |
| HF Energy | -131.383753 |
| Nuclear repulsion energy | 47.204202 |
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 mPW1PW91/6-311G**
Geometric Data calculated at mPW1PW91/6-311G**
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability