Jump to
S1C2
S2C1
S2C2
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -131.394300 |
| Energy at 298.15K | -131.393746 |
| HF Energy | -131.394300 |
| Nuclear repulsion energy | 47.441375 |
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/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' |
3412 |
3412 |
21.33 |
|
|
|
| 2 |
A' |
1937 |
1937 |
20.22 |
|
|
|
| 3 |
A' |
1158 |
1158 |
13.29 |
|
|
|
| 4 |
A' |
624 |
624 |
32.17 |
|
|
|
| 5 |
A' |
418 |
418 |
6.63 |
|
|
|
| 6 |
A" |
457 |
457 |
1.76 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4003.1 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4003.1 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 M06-2X/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.029 |
-1.234 |
0.000 |
| C2 |
0.000 |
0.100 |
0.000 |
| N3 |
-0.058 |
1.275 |
0.000 |
| H4 |
0.581 |
-2.116 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3342 | 2.5095 | 1.0722 |
C2 | 1.3342 | | 1.1768 | 2.2902 | N3 | 2.5095 | 1.1768 | | 3.4504 | H4 | 1.0722 | 2.2902 | 3.4504 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.921 |
|
C2 |
C1 |
H4 |
144.020 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -131.392436 |
| Energy at 298.15K | |
| HF Energy | -131.392436 |
| Nuclear repulsion energy | 47.578576 |
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/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 |
3450 |
3450 |
59.34 |
|
|
|
| 2 |
Σ |
1732 |
1732 |
39.33 |
|
|
|
| 3 |
Σ |
1242 |
1242 |
16.10 |
|
|
|
| 4 |
Π |
459 |
459 |
0.46 |
|
|
|
| 4 |
Π |
459 |
459 |
0.46 |
|
|
|
| 5 |
Π |
396i |
396i |
48.05 |
|
|
|
| 5 |
Π |
396i |
396i |
48.05 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3275.3 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 3275.3 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 M06-2X/6-311G*
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.209 |
| C2 |
0.000 |
0.000 |
0.091 |
| N3 |
0.000 |
0.000 |
1.283 |
| H4 |
0.000 |
0.000 |
-2.275 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3004 | 2.4922 | 1.0656 |
C2 | 1.3004 | | 1.1918 | 2.3660 | N3 | 2.4922 | 1.1918 | | 3.5578 | H4 | 1.0656 | 2.3660 | 3.5578 | |
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/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.100 |
|
|
|
| 2 |
C |
0.043 |
|
|
|
| 3 |
N |
-0.253 |
|
|
|
| 4 |
H |
0.310 |
|
|
|
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 |
-3.481 |
3.481 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.378 |
0.000 |
0.000 |
| y |
0.000 |
-17.378 |
0.000 |
| z |
0.000 |
0.000 |
-15.366 |
|
| Traceless |
| | x | y | z |
| x |
-1.006 |
0.000 |
0.000 |
| y |
0.000 |
-1.006 |
0.000 |
| z |
0.000 |
0.000 |
2.012 |
|
| Polar |
| 3z2-r2 | 4.024 |
| 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 |
1.884 |
0.000 |
0.000 |
| y |
0.000 |
1.884 |
0.000 |
| z |
0.000 |
0.000 |
6.326 |
<r2> (average value of r
2) Å
2
| <r2> |
35.956 |
| (<r2>)1/2 |
5.996 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -131.368948 |
| Energy at 298.15K | -131.368420 |
| HF Energy | -131.368948 |
| Nuclear repulsion energy | 47.120596 |
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/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' |
3113 |
3113 |
8.11 |
|
|
|
| 2 |
A' |
2183 |
2183 |
25.93 |
|
|
|
| 3 |
A' |
1072 |
1072 |
66.88 |
|
|
|
| 4 |
A' |
984 |
984 |
14.07 |
|
|
|
| 5 |
A' |
453 |
453 |
23.18 |
|
|
|
| 6 |
A" |
335 |
335 |
9.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4069.5 cm
-1
Scaled (by 1) Zero Point Vibrational Energy (zpe) 4069.5 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 M06-2X/6-311G*
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.015 |
-1.290 |
0.000 |
| C2 |
0.000 |
0.100 |
0.000 |
| N3 |
-0.132 |
1.258 |
0.000 |
| H4 |
1.019 |
-1.662 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3896 | 2.5504 | 1.0987 |
C2 | 1.3896 | | 1.1657 | 2.0348 | N3 | 2.5504 | 1.1657 | | 3.1384 | H4 | 1.0987 | 2.0348 | 3.1384 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-311G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.123 |
|
|
|
| 2 |
C |
0.101 |
|
|
|
| 3 |
N |
-0.232 |
|
|
|
| 4 |
H |
0.254 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.738 |
-1.568 |
0.000 |
2.341 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.307 |
-2.797 |
0.000 |
| y |
-2.797 |
-20.930 |
0.000 |
| z |
0.000 |
0.000 |
-15.960 |
|
| Traceless |
| | x | y | z |
| x |
1.138 |
-2.797 |
0.000 |
| y |
-2.797 |
-4.297 |
0.000 |
| z |
0.000 |
0.000 |
3.159 |
|
| Polar |
| 3z2-r2 | 6.318 |
| x2-y2 | 3.623 |
| xy | -2.797 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.485 |
-0.415 |
0.000 |
| y |
-0.415 |
6.150 |
0.000 |
| z |
0.000 |
0.000 |
2.373 |
<r2> (average value of r
2) Å
2
| <r2> |
36.324 |
| (<r2>)1/2 |
6.027 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at M06-2X/6-311G*
| | hartrees |
| Energy at 0K | -131.368948 |
| Energy at 298.15K | -131.368420 |
| HF Energy | -131.368948 |
| Nuclear repulsion energy | 47.120596 |
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/6-311G*
Geometric Data calculated at M06-2X/6-311G*
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability