Jump to
S1C2
S1C3
Energy calculated at HSEh1PBE/3-21G*
| hartrees |
Energy at 0K | -223.788064 |
Energy at 298.15K | -223.793895 |
HF Energy | -223.788064 |
Nuclear repulsion energy | 123.160312 |
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 HSEh1PBE/3-21G*
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 |
3734 |
3584 |
36.01 |
|
|
|
2 |
A |
3605 |
3460 |
5.79 |
|
|
|
3 |
A |
1801 |
1729 |
329.43 |
|
|
|
4 |
A |
1695 |
1627 |
3.20 |
|
|
|
5 |
A |
1174 |
1127 |
0.44 |
|
|
|
6 |
A |
973 |
934 |
5.23 |
|
|
|
7 |
A |
492 |
472 |
3.34 |
|
|
|
8 |
A |
487 |
468 |
0.04 |
|
|
|
9 |
A |
138 |
133 |
0.00 |
|
|
|
10 |
B |
3730 |
3581 |
39.77 |
|
|
|
11 |
B |
3595 |
3451 |
47.74 |
|
|
|
12 |
B |
1666 |
1599 |
196.59 |
|
|
|
13 |
B |
1450 |
1392 |
286.74 |
|
|
|
14 |
B |
1017 |
976 |
12.87 |
|
|
|
15 |
B |
814 |
782 |
140.46 |
|
|
|
16 |
B |
586 |
563 |
85.02 |
|
|
|
17 |
B |
562 |
540 |
13.80 |
|
|
|
18 |
B |
472 |
453 |
607.13 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13995.1 cm
-1
Scaled (by 0.9599) Zero Point Vibrational Energy (zpe) 13433.9 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 HSEh1PBE/3-21G*
Point Group is C2
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.144 |
O2 |
0.000 |
0.000 |
1.381 |
N3 |
0.000 |
1.154 |
-0.606 |
N4 |
0.000 |
-1.154 |
-0.606 |
H5 |
0.003 |
2.027 |
-0.101 |
H6 |
-0.001 |
1.172 |
-1.614 |
H7 |
-0.003 |
-2.027 |
-0.101 |
H8 |
0.001 |
-1.172 |
-1.614 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2371 | 1.3761 | 1.3761 | 2.0418 | 2.1132 | 2.0418 | 2.1132 |
O2 | 1.2371 | | 2.2975 | 2.2975 | 2.5108 | 3.2165 | 2.5108 | 3.2165 | N3 | 1.3761 | 2.2975 | | 2.3080 | 1.0088 | 1.0086 | 3.2210 | 2.5357 | N4 | 1.3761 | 2.2975 | 2.3080 | | 3.2210 | 2.5357 | 1.0088 | 1.0086 | H5 | 2.0418 | 2.5108 | 1.0088 | 3.2210 | | 1.7383 | 4.0543 | 3.5396 | H6 | 2.1132 | 3.2165 | 1.0086 | 2.5357 | 1.7383 | | 3.5396 | 2.3450 | H7 | 2.0418 | 2.5108 | 3.2210 | 1.0088 | 4.0543 | 3.5396 | | 1.7383 | H8 | 2.1132 | 3.2165 | 2.5357 | 1.0086 | 3.5396 | 2.3450 | 1.7383 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
116.940 |
|
C1 |
N3 |
H6 |
124.056 |
C1 |
N4 |
H7 |
116.940 |
|
C1 |
N4 |
H8 |
124.056 |
O2 |
C1 |
N3 |
123.005 |
|
O2 |
C1 |
N4 |
123.005 |
N3 |
C1 |
N4 |
113.990 |
|
H5 |
N3 |
H6 |
119.004 |
H7 |
N4 |
H8 |
119.004 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.882 |
|
|
|
2 |
O |
-0.549 |
|
|
|
3 |
N |
-0.821 |
|
|
|
4 |
N |
-0.821 |
|
|
|
5 |
H |
0.340 |
|
|
|
6 |
H |
0.315 |
|
|
|
7 |
H |
0.340 |
|
|
|
8 |
H |
0.315 |
|
|
|
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 |
-4.331 |
4.331 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.088 |
0.019 |
0.000 |
y |
0.019 |
-15.884 |
0.000 |
z |
0.000 |
0.000 |
-23.265 |
|
Traceless |
| x | y | z |
x |
-5.514 |
0.019 |
0.000 |
y |
0.019 |
8.293 |
0.000 |
z |
0.000 |
0.000 |
-2.779 |
|
Polar |
3z2-r2 | -5.558 |
x2-y2 | -9.204 |
xy | 0.019 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.074 |
0.003 |
0.000 |
y |
0.003 |
4.046 |
0.000 |
z |
0.000 |
0.000 |
4.299 |
<r2> (average value of r
2) Å
2
<r2> |
68.735 |
(<r2>)1/2 |
8.291 |
Jump to
S1C1
S1C3
Energy calculated at HSEh1PBE/3-21G*
| hartrees |
Energy at 0K | -223.788064 |
Energy at 298.15K | -223.793898 |
HF Energy | -223.788064 |
Nuclear repulsion energy | 123.162318 |
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 HSEh1PBE/3-21G*
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' |
3734 |
3584 |
35.94 |
|
|
|
2 |
A' |
3605 |
3460 |
5.86 |
|
|
|
3 |
A' |
1801 |
1729 |
329.52 |
|
|
|
4 |
A' |
1695 |
1627 |
3.16 |
|
|
|
5 |
A' |
1174 |
1127 |
0.45 |
|
|
|
6 |
A' |
973 |
934 |
5.21 |
|
|
|
7 |
A' |
814 |
782 |
140.50 |
|
|
|
8 |
A' |
586 |
563 |
83.69 |
|
|
|
9 |
A' |
492 |
472 |
3.38 |
|
|
|
10 |
A' |
472 |
453 |
608.39 |
|
|
|
11 |
A" |
3730 |
3581 |
39.97 |
|
|
|
12 |
A" |
3594 |
3450 |
47.52 |
|
|
|
13 |
A" |
1666 |
1599 |
196.79 |
|
|
|
14 |
A" |
1450 |
1392 |
286.45 |
|
|
|
15 |
A" |
1017 |
976 |
12.86 |
|
|
|
16 |
A" |
562 |
540 |
13.78 |
|
|
|
17 |
A" |
487 |
468 |
0.00 |
|
|
|
18 |
A" |
140 |
134 |
0.00 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13996.1 cm
-1
Scaled (by 0.9599) Zero Point Vibrational Energy (zpe) 13434.9 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 HSEh1PBE/3-21G*
Point Group is Cs
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.144 |
0.000 |
O2 |
0.000 |
1.381 |
0.000 |
N3 |
0.000 |
-0.606 |
1.154 |
N4 |
0.000 |
-0.606 |
-1.154 |
H5 |
-0.001 |
-0.101 |
2.027 |
H6 |
-0.001 |
-1.614 |
1.172 |
H7 |
-0.001 |
-0.101 |
-2.027 |
H8 |
-0.001 |
-1.614 |
-1.172 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2372 | 1.3760 | 1.3760 | 2.0417 | 2.1131 | 2.0417 | 2.1131 |
O2 | 1.2372 | | 2.2977 | 2.2977 | 2.5109 | 3.2166 | 2.5109 | 3.2166 | N3 | 1.3760 | 2.2977 | | 2.3076 | 1.0088 | 1.0087 | 3.2206 | 2.5350 | N4 | 1.3760 | 2.2977 | 2.3076 | | 3.2206 | 2.5350 | 1.0088 | 1.0087 | H5 | 2.0417 | 2.5109 | 1.0088 | 3.2206 | | 1.7384 | 4.0540 | 3.5389 | H6 | 2.1131 | 3.2166 | 1.0087 | 2.5350 | 1.7384 | | 3.5389 | 2.3439 | H7 | 2.0417 | 2.5109 | 3.2206 | 1.0088 | 4.0540 | 3.5389 | | 1.7384 | H8 | 2.1131 | 3.2166 | 2.5350 | 1.0087 | 3.5389 | 2.3439 | 1.7384 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
116.937 |
|
C1 |
N3 |
H6 |
124.048 |
C1 |
N4 |
H7 |
116.937 |
|
C1 |
N4 |
H8 |
124.048 |
O2 |
C1 |
N3 |
123.017 |
|
O2 |
C1 |
N4 |
123.017 |
N3 |
C1 |
N4 |
113.966 |
|
H5 |
N3 |
H6 |
119.015 |
H7 |
N4 |
H8 |
119.015 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.882 |
|
|
|
2 |
O |
-0.549 |
|
|
|
3 |
N |
-0.821 |
|
|
|
4 |
N |
-0.821 |
|
|
|
5 |
H |
0.340 |
|
|
|
6 |
H |
0.315 |
|
|
|
7 |
H |
0.340 |
|
|
|
8 |
H |
0.315 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
|
x |
y |
z |
Total |
|
-0.009 |
-4.332 |
0.000 |
4.332 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.089 |
0.007 |
0.000 |
y |
0.007 |
-23.265 |
0.000 |
z |
0.000 |
0.000 |
-15.887 |
|
Traceless |
| x | y | z |
x |
-5.512 |
0.007 |
0.000 |
y |
0.007 |
-2.778 |
0.000 |
z |
0.000 |
0.000 |
8.290 |
|
Polar |
3z2-r2 | 16.580 |
x2-y2 | -1.823 |
xy | 0.007 |
xz | 0.000 |
yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
|
x |
y |
z |
x |
1.074 |
0.000 |
0.000 |
y |
0.000 |
4.299 |
0.000 |
z |
0.000 |
0.000 |
4.045 |
<r2> (average value of r
2) Å
2
<r2> |
68.731 |
(<r2>)1/2 |
8.290 |
Jump to
S1C1
S1C2
Energy calculated at HSEh1PBE/3-21G*
| hartrees |
Energy at 0K | -223.788064 |
Energy at 298.15K | -223.793894 |
HF Energy | -223.788064 |
Nuclear repulsion energy | 123.157254 |
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 HSEh1PBE/3-21G*
Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
1 |
A1 |
3734 |
3584 |
35.97 |
|
|
|
2 |
A1 |
3605 |
3460 |
5.83 |
|
|
|
3 |
A1 |
1802 |
1730 |
329.46 |
|
|
|
4 |
A1 |
1695 |
1627 |
3.41 |
|
|
|
5 |
A1 |
1174 |
1127 |
0.43 |
|
|
|
6 |
A1 |
972 |
933 |
5.25 |
|
|
|
7 |
A1 |
492 |
472 |
3.38 |
|
|
|
8 |
A2 |
487 |
467 |
0.00 |
|
|
|
9 |
A2 |
138 |
133 |
0.00 |
|
|
|
10 |
B1 |
814 |
782 |
140.31 |
|
|
|
11 |
B1 |
586 |
563 |
83.42 |
|
|
|
12 |
B1 |
471 |
453 |
609.00 |
|
|
|
13 |
B2 |
3730 |
3581 |
39.90 |
|
|
|
14 |
B2 |
3595 |
3451 |
47.61 |
|
|
|
15 |
B2 |
1666 |
1599 |
196.20 |
|
|
|
16 |
B2 |
1449 |
1391 |
286.85 |
|
|
|
17 |
B2 |
1017 |
976 |
12.98 |
|
|
|
18 |
B2 |
562 |
539 |
13.78 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13994.2 cm
-1
Scaled (by 0.9599) Zero Point Vibrational Energy (zpe) 13433.0 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 HSEh1PBE/3-21G*
Point Group is C2v
Cartesians (Å)
Atom |
x (Å) |
y (Å) |
z (Å) |
C1 |
0.000 |
0.000 |
0.144 |
O2 |
0.000 |
0.000 |
1.381 |
N3 |
0.000 |
1.154 |
-0.606 |
N4 |
0.000 |
-1.154 |
-0.606 |
H5 |
0.000 |
2.027 |
-0.101 |
H6 |
0.000 |
1.172 |
-1.614 |
H7 |
0.000 |
-2.027 |
-0.101 |
H8 |
0.000 |
-1.172 |
-1.614 |
Atom - Atom Distances (Å)
|
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
C1 | | 1.2370 | 1.3762 | 1.3762 | 2.0420 | 2.1131 | 2.0420 | 2.1131 |
O2 | 1.2370 | | 2.2977 | 2.2977 | 2.5111 | 3.2164 | 2.5111 | 3.2164 | N3 | 1.3762 | 2.2977 | | 2.3080 | 1.0088 | 1.0087 | 3.2211 | 2.5352 | N4 | 1.3762 | 2.2977 | 2.3080 | | 3.2211 | 2.5352 | 1.0088 | 1.0087 | H5 | 2.0420 | 2.5111 | 1.0088 | 3.2211 | | 1.7385 | 4.0545 | 3.5391 | H6 | 2.1131 | 3.2164 | 1.0087 | 2.5352 | 1.7385 | | 3.5391 | 2.3438 | H7 | 2.0420 | 2.5111 | 3.2211 | 1.0088 | 4.0545 | 3.5391 | | 1.7385 | H8 | 2.1131 | 3.2164 | 2.5352 | 1.0087 | 3.5391 | 2.3438 | 1.7385 | |
More geometry information
Calculated Bond Angles
atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
C1 |
N3 |
H5 |
116.945 |
|
C1 |
N3 |
H6 |
124.033 |
C1 |
N4 |
H7 |
116.945 |
|
C1 |
N4 |
H8 |
124.033 |
O2 |
C1 |
N3 |
123.016 |
|
O2 |
C1 |
N4 |
123.016 |
N3 |
C1 |
N4 |
113.968 |
|
H5 |
N3 |
H6 |
119.022 |
H7 |
N4 |
H8 |
119.022 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/3-21G*
Charges (e)
Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
1 |
C |
0.882 |
|
|
|
2 |
O |
-0.549 |
|
|
|
3 |
N |
-0.821 |
|
|
|
4 |
N |
-0.821 |
|
|
|
5 |
H |
0.340 |
|
|
|
6 |
H |
0.315 |
|
|
|
7 |
H |
0.340 |
|
|
|
8 |
H |
0.315 |
|
|
|
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 |
-4.330 |
4.330 |
CHELPG |
|
|
|
|
AIM |
|
|
|
|
ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
Primitive |
| x | y | z |
x |
-25.089 |
0.000 |
0.000 |
y |
0.000 |
-15.887 |
0.000 |
z |
0.000 |
0.000 |
-23.265 |
|
Traceless |
| x | y | z |
x |
-5.513 |
0.000 |
0.000 |
y |
0.000 |
8.290 |
0.000 |
z |
0.000 |
0.000 |
-2.777 |
|
Polar |
3z2-r2 | -5.553 |
x2-y2 | -9.202 |
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 |
1.074 |
0.000 |
0.000 |
y |
0.000 |
4.046 |
0.000 |
z |
0.000 |
0.000 |
4.299 |
<r2> (average value of r
2) Å
2
<r2> |
68.738 |
(<r2>)1/2 |
8.291 |