Jump to
S1C2
S2C1
S2C2
Energy calculated at PBEPBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -131.308360 |
| Energy at 298.15K | -131.307577 |
| HF Energy | -131.308360 |
| Nuclear repulsion energy | 47.220098 |
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 PBEPBE/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' |
3324 |
3303 |
43.19 |
|
|
|
| 2 |
A' |
1785 |
1773 |
24.02 |
|
|
|
| 3 |
A' |
1221 |
1213 |
3.65 |
|
|
|
| 4 |
A' |
438 |
435 |
7.50 |
|
|
|
| 5 |
A' |
335 |
333 |
39.49 |
|
|
|
| 6 |
A" |
428 |
426 |
0.44 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3765.9 cm
-1
Scaled (by 0.9935) Zero Point Vibrational Energy (zpe) 3741.4 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 PBEPBE/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.086 |
-1.217 |
0.000 |
| C2 |
0.000 |
0.084 |
0.000 |
| N3 |
-0.156 |
1.282 |
0.000 |
| H4 |
0.573 |
-2.174 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3039 | 2.5111 | 1.0742 |
C2 | 1.3039 | | 1.2084 | 2.3300 | N3 | 2.5111 | 1.2084 | | 3.5327 | H4 | 1.0742 | 2.3300 | 3.5327 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
176.382 |
|
C2 |
C1 |
H4 |
156.799 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at PBEPBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -131.308067 |
| Energy at 298.15K | |
| HF Energy | -131.308067 |
| Nuclear repulsion energy | 47.257224 |
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 PBEPBE/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 |
3367 |
3345 |
65.85 |
|
|
|
| 2 |
Σ |
1757 |
1746 |
23.00 |
|
|
|
| 3 |
Σ |
1243 |
1235 |
2.69 |
|
|
|
| 4 |
Π |
427 |
424 |
0.07 |
|
|
|
| 4 |
Π |
427 |
424 |
0.07 |
|
|
|
| 5 |
Π |
246i |
244i |
44.20 |
|
|
|
| 5 |
Π |
246i |
244i |
44.20 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3365.1 cm
-1
Scaled (by 0.9935) Zero Point Vibrational Energy (zpe) 3343.2 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 PBEPBE/aug-cc-pVTZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.212 |
| C2 |
0.000 |
0.000 |
0.081 |
| N3 |
0.000 |
0.000 |
1.295 |
| H4 |
0.000 |
0.000 |
-2.282 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2930 | 2.5066 | 1.0708 |
C2 | 1.2930 | | 1.2136 | 2.3638 | N3 | 2.5066 | 1.2136 | | 3.5774 | H4 | 1.0708 | 2.3638 | 3.5774 | |
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 PBEPBE/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.688 |
|
|
|
| 2 |
C |
0.624 |
|
|
|
| 3 |
N |
-0.446 |
|
|
|
| 4 |
H |
0.509 |
|
|
|
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 |
-3.240 |
3.240 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.511 |
0.000 |
0.000 |
| y |
0.000 |
-17.511 |
0.000 |
| z |
0.000 |
0.000 |
-15.852 |
|
| Traceless |
| | x | y | z |
| x |
-0.829 |
0.000 |
0.000 |
| y |
0.000 |
-0.829 |
0.000 |
| z |
0.000 |
0.000 |
1.659 |
|
| Polar |
| 3z2-r2 | 3.318 |
| 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 |
3.214 |
0.000 |
0.000 |
| y |
0.000 |
3.214 |
0.000 |
| z |
0.000 |
0.000 |
7.384 |
<r2> (average value of r
2) Å
2
| <r2> |
36.388 |
| (<r2>)1/2 |
6.032 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at PBEPBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -131.282459 |
| Energy at 298.15K | -131.281870 |
| HF Energy | -131.282459 |
| Nuclear repulsion energy | 46.866029 |
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 PBEPBE/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' |
2997 |
2978 |
3.86 |
|
|
|
| 2 |
A' |
2010 |
1997 |
16.04 |
|
|
|
| 3 |
A' |
1090 |
1083 |
21.48 |
|
|
|
| 4 |
A' |
898 |
892 |
63.09 |
|
|
|
| 5 |
A' |
450 |
447 |
22.33 |
|
|
|
| 6 |
A" |
293 |
291 |
9.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3868.7 cm
-1
Scaled (by 0.9935) Zero Point Vibrational Energy (zpe) 3843.5 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 PBEPBE/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.226 |
-1.259 |
0.000 |
| C2 |
0.000 |
0.089 |
0.000 |
| N3 |
-0.380 |
1.219 |
0.000 |
| H4 |
1.303 |
-1.509 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3668 | 2.5507 | 1.1055 |
C2 | 1.3668 | | 1.1919 | 2.0622 | N3 | 2.5507 | 1.1919 | | 3.2055 | H4 | 1.1055 | 2.0622 | 3.2055 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at PBEPBE/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.359 |
|
|
|
| 2 |
C |
0.291 |
|
|
|
| 3 |
N |
-0.231 |
|
|
|
| 4 |
H |
0.299 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.799 |
-1.182 |
0.000 |
2.153 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.814 |
-1.852 |
0.000 |
| y |
-1.852 |
-21.512 |
0.000 |
| z |
0.000 |
0.000 |
-16.193 |
|
| Traceless |
| | x | y | z |
| x |
2.038 |
-1.852 |
0.000 |
| y |
-1.852 |
-5.009 |
0.000 |
| z |
0.000 |
0.000 |
2.971 |
|
| Polar |
| 3z2-r2 | 5.941 |
| x2-y2 | 4.698 |
| xy | -1.852 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.854 |
-0.951 |
0.000 |
| y |
-0.951 |
7.224 |
-0.001 |
| z |
0.000 |
-0.001 |
3.436 |
<r2> (average value of r
2) Å
2
| <r2> |
36.598 |
| (<r2>)1/2 |
6.050 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at PBEPBE/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -131.282459 |
| Energy at 298.15K | -131.281870 |
| HF Energy | -131.282459 |
| Nuclear repulsion energy | 46.866029 |
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 PBEPBE/aug-cc-pVTZ
Geometric Data calculated at PBEPBE/aug-cc-pVTZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability