Jump to
S1C2
S2C1
S2C2
Energy calculated at M06-2X/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -131.383235 |
| Energy at 298.15K | -131.382663 |
| HF Energy | -131.383235 |
| Nuclear repulsion energy | 47.168009 |
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 M06-2X/aug-cc-pVDZ
| 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' |
3420 |
3420 |
32.51 |
|
|
|
| 2 |
A' |
1934 |
1934 |
22.34 |
|
|
|
| 3 |
A' |
1165 |
1165 |
13.69 |
|
|
|
| 4 |
A' |
615 |
615 |
26.33 |
|
|
|
| 5 |
A' |
413 |
413 |
3.58 |
|
|
|
| 6 |
A" |
437 |
437 |
0.92 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3992.0 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3992.0 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 M06-2X/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.015 |
-1.241 |
0.000 |
| C2 |
0.000 |
0.100 |
0.000 |
| N3 |
-0.105 |
1.280 |
0.000 |
| H4 |
0.646 |
-2.115 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3406 | 2.5232 | 1.0783 |
C2 | 1.3406 | | 1.1845 | 2.3075 | N3 | 2.5232 | 1.1845 | | 3.4773 | H4 | 1.0783 | 2.3075 | 3.4773 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.552 |
|
C2 |
C1 |
H4 |
144.878 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at M06-2X/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -131.381367 |
| Energy at 298.15K | |
| HF Energy | -131.381367 |
| Nuclear repulsion energy | 47.303528 |
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 M06-2X/aug-cc-pVDZ
| 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 |
3440 |
3440 |
81.23 |
|
|
|
| 2 |
Σ |
1743 |
1743 |
41.92 |
|
|
|
| 3 |
Σ |
1246 |
1246 |
14.95 |
|
|
|
| 4 |
Π |
443 |
443 |
0.09 |
|
|
|
| 4 |
Π |
443 |
443 |
0.09 |
|
|
|
| 5 |
Π |
412i |
412i |
41.93 |
|
|
|
| 5 |
Π |
412i |
412i |
41.93 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3244.6 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3244.6 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 M06-2X/aug-cc-pVDZ
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.216 |
| C2 |
0.000 |
0.000 |
0.092 |
| N3 |
0.000 |
0.000 |
1.291 |
| H4 |
0.000 |
0.000 |
-2.288 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3075 | 2.5066 | 1.0718 |
C2 | 1.3075 | | 1.1991 | 2.3793 | N3 | 2.5066 | 1.1991 | | 3.5784 | H4 | 1.0718 | 2.3793 | 3.5784 | |
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 M06-2X/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.788 |
|
|
|
| 2 |
C |
-0.046 |
|
|
|
| 3 |
N |
-0.301 |
|
|
|
| 4 |
H |
-0.442 |
|
|
|
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 |
-3.535 |
3.535 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.601 |
0.000 |
0.000 |
| y |
0.000 |
-17.601 |
0.000 |
| z |
0.000 |
0.000 |
-15.547 |
|
| Traceless |
| | x | y | z |
| x |
-1.027 |
0.000 |
0.000 |
| y |
0.000 |
-1.027 |
0.000 |
| z |
0.000 |
0.000 |
2.054 |
|
| Polar |
| 3z2-r2 | 4.108 |
| 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 |
2.990 |
0.000 |
0.000 |
| y |
0.000 |
2.990 |
0.000 |
| z |
0.000 |
0.000 |
7.123 |
<r2> (average value of r
2) Å
2
| <r2> |
36.382 |
| (<r2>)1/2 |
6.032 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at M06-2X/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -131.359649 |
| Energy at 298.15K | -131.359101 |
| HF Energy | -131.359649 |
| Nuclear repulsion energy | 46.854182 |
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 M06-2X/aug-cc-pVDZ
| 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' |
3118 |
3118 |
3.83 |
|
|
|
| 2 |
A' |
2177 |
2177 |
28.14 |
|
|
|
| 3 |
A' |
1069 |
1069 |
68.31 |
|
|
|
| 4 |
A' |
991 |
991 |
12.79 |
|
|
|
| 5 |
A' |
445 |
445 |
21.69 |
|
|
|
| 6 |
A" |
316 |
316 |
9.14 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4057.9 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4057.9 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 M06-2X/aug-cc-pVDZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.016 |
-1.297 |
0.000 |
| C2 |
0.000 |
0.099 |
0.000 |
| N3 |
-0.133 |
1.265 |
0.000 |
| H4 |
1.026 |
-1.667 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3962 | 2.5646 | 1.1057 |
C2 | 1.3962 | | 1.1733 | 2.0424 | N3 | 2.5646 | 1.1733 | | 3.1525 | H4 | 1.1057 | 2.0424 | 3.1525 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/aug-cc-pVDZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.140 |
|
|
|
| 2 |
C |
0.200 |
|
|
|
| 3 |
N |
-0.210 |
|
|
|
| 4 |
H |
-0.130 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.635 |
-1.639 |
0.000 |
2.316 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.539 |
-2.721 |
0.000 |
| y |
-2.721 |
-20.934 |
0.000 |
| z |
0.000 |
0.000 |
-16.228 |
|
| Traceless |
| | x | y | z |
| x |
1.042 |
-2.721 |
0.000 |
| y |
-2.721 |
-4.051 |
0.000 |
| z |
0.000 |
0.000 |
3.008 |
|
| Polar |
| 3z2-r2 | 6.017 |
| x2-y2 | 3.395 |
| xy | -2.721 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
3.348 |
-0.291 |
0.000 |
| y |
-0.291 |
6.820 |
0.000 |
| z |
0.000 |
0.000 |
3.242 |
<r2> (average value of r
2) Å
2
| <r2> |
36.697 |
| (<r2>)1/2 |
6.058 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at M06-2X/aug-cc-pVDZ
| | hartrees |
| Energy at 0K | -131.359649 |
| Energy at 298.15K | -131.359101 |
| HF Energy | -131.359649 |
| Nuclear repulsion energy | 46.854182 |
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 M06-2X/aug-cc-pVDZ
Geometric Data calculated at M06-2X/aug-cc-pVDZ
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability