Jump to
S1C2
S2C1
S2C2
Energy calculated at M06-2X/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.369222 |
| Energy at 298.15K | |
| HF Energy | -131.369222 |
| Nuclear repulsion energy | 47.437750 |
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/6-31G(2df,p)
Geometric Data calculated at M06-2X/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.029 |
-1.232 |
0.000 |
| C2 |
0.000 |
0.098 |
0.000 |
| N3 |
-0.118 |
1.272 |
0.000 |
| H4 |
0.649 |
-2.105 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3299 | 2.5081 | 1.0707 |
C2 | 1.3299 | | 1.1801 | 2.2965 | N3 | 2.5081 | 1.1801 | | 3.4631 | H4 | 1.0707 | 2.2965 | 3.4631 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
175.535 |
|
C2 |
C1 |
H4 |
145.937 |
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Jump to
S1C1
S2C1
S2C2
Energy calculated at M06-2X/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.368011 |
| Energy at 298.15K | |
| HF Energy | -131.368011 |
| Nuclear repulsion energy | 47.575557 |
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/6-31G(2df,p)
| 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 |
3473 |
3307 |
73.49 |
|
|
|
| 2 |
Σ |
1724 |
1642 |
54.77 |
|
|
|
| 3 |
Σ |
1257 |
1197 |
17.98 |
|
|
|
| 4 |
Π |
468 |
445 |
0.66 |
|
|
|
| 4 |
Π |
468 |
445 |
0.66 |
|
|
|
| 5 |
Π |
337i |
321i |
43.17 |
|
|
|
| 5 |
Π |
337i |
321i |
43.17 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 3356.8 cm
-1
Scaled (by 0.9524) Zero Point Vibrational Energy (zpe) 3197.1 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/6-31G(2df,p)
Point Group is C∞v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
-1.208 |
| C2 |
0.000 |
0.000 |
0.088 |
| N3 |
0.000 |
0.000 |
1.284 |
| H4 |
0.000 |
0.000 |
-2.272 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.2964 | 2.4919 | 1.0638 |
C2 | 1.2964 | | 1.1956 | 2.3602 | N3 | 2.4919 | 1.1956 | | 3.5558 | H4 | 1.0638 | 2.3602 | 3.5558 | |
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/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.238 |
|
|
|
| 2 |
C |
0.262 |
|
|
|
| 3 |
N |
-0.295 |
|
|
|
| 4 |
H |
0.271 |
|
|
|
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 |
-3.443 |
3.443 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.948 |
0.000 |
0.000 |
| y |
0.000 |
-16.948 |
0.000 |
| z |
0.000 |
0.000 |
-14.955 |
|
| Traceless |
| | x | y | z |
| x |
-0.997 |
0.000 |
0.000 |
| y |
0.000 |
-0.997 |
0.000 |
| z |
0.000 |
0.000 |
1.993 |
|
| Polar |
| 3z2-r2 | 3.986 |
| 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 |
1.997 |
0.000 |
0.000 |
| y |
0.000 |
1.997 |
0.000 |
| z |
0.000 |
0.000 |
6.215 |
<r2> (average value of r
2) Å
2
| <r2> |
35.674 |
| (<r2>)1/2 |
5.973 |
Jump to
S1C1
S1C2
S2C2
Energy calculated at M06-2X/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.344522 |
| Energy at 298.15K | -131.344016 |
| HF Energy | -131.344522 |
| Nuclear repulsion energy | 47.089645 |
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/6-31G(2df,p)
| 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' |
3116 |
2968 |
7.15 |
|
|
|
| 2 |
A' |
2188 |
2084 |
26.59 |
|
|
|
| 3 |
A' |
1076 |
1025 |
64.09 |
|
|
|
| 4 |
A' |
980 |
934 |
13.99 |
|
|
|
| 5 |
A' |
465 |
443 |
21.36 |
|
|
|
| 6 |
A" |
344 |
327 |
11.60 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 4084.9 cm
-1
Scaled (by 0.9524) Zero Point Vibrational Energy (zpe) 3890.5 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/6-31G(2df,p)
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-0.060 |
-1.289 |
0.000 |
| C2 |
0.000 |
0.098 |
0.000 |
| N3 |
-0.087 |
1.263 |
0.000 |
| H4 |
0.964 |
-1.693 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
H4 |
| C1 | | 1.3881 | 2.5517 | 1.1008 |
C2 | 1.3881 | | 1.1679 | 2.0342 | N3 | 2.5517 | 1.1679 | | 3.1371 | H4 | 1.1008 | 2.0342 | 3.1371 | |
More geometry information
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at M06-2X/6-31G(2df,p)
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.225 |
|
|
|
| 2 |
C |
0.258 |
|
|
|
| 3 |
N |
-0.236 |
|
|
|
| 4 |
H |
0.204 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
1.520 |
-1.607 |
0.000 |
2.212 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-17.084 |
-2.621 |
0.000 |
| y |
-2.621 |
-20.192 |
0.000 |
| z |
0.000 |
0.000 |
-15.693 |
|
| Traceless |
| | x | y | z |
| x |
0.859 |
-2.621 |
0.000 |
| y |
-2.621 |
-3.803 |
0.000 |
| z |
0.000 |
0.000 |
2.944 |
|
| Polar |
| 3z2-r2 | 5.889 |
| x2-y2 | 3.108 |
| xy | -2.621 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.526 |
-0.350 |
0.000 |
| y |
-0.350 |
5.991 |
0.000 |
| z |
0.000 |
0.000 |
2.415 |
<r2> (average value of r
2) Å
2
| <r2> |
36.083 |
| (<r2>)1/2 |
6.007 |
Jump to
S1C1
S1C2
S2C1
Energy calculated at M06-2X/6-31G(2df,p)
| | hartrees |
| Energy at 0K | -131.344522 |
| Energy at 298.15K | -131.344016 |
| HF Energy | -131.344522 |
| Nuclear repulsion energy | 47.089645 |
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/6-31G(2df,p)
Geometric Data calculated at M06-2X/6-31G(2df,p)
Point Group is Cs
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability