Jump to
S1C2
S1C3
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -225.105172 |
| Energy at 298.15K | -225.111369 |
| HF Energy | -225.105172 |
| Nuclear repulsion energy | 124.093029 |
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/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 |
3728 |
3580 |
34.79 |
|
|
|
| 2 |
A |
3613 |
3470 |
3.24 |
|
|
|
| 3 |
A |
1850 |
1777 |
419.08 |
|
|
|
| 4 |
A |
1635 |
1570 |
0.58 |
|
|
|
| 5 |
A |
1188 |
1141 |
3.22 |
|
|
|
| 6 |
A |
971 |
933 |
8.07 |
|
|
|
| 7 |
A |
580 |
557 |
74.98 |
|
|
|
| 8 |
A |
476 |
457 |
2.59 |
|
|
|
| 9 |
A |
385 |
369 |
73.49 |
|
|
|
| 10 |
B |
3727 |
3580 |
29.11 |
|
|
|
| 11 |
B |
3609 |
3466 |
45.63 |
|
|
|
| 12 |
B |
1641 |
1576 |
226.62 |
|
|
|
| 13 |
B |
1436 |
1380 |
196.39 |
|
|
|
| 14 |
B |
1055 |
1013 |
22.07 |
|
|
|
| 15 |
B |
798 |
766 |
77.58 |
|
|
|
| 16 |
B |
585 |
562 |
83.71 |
|
|
|
| 17 |
B |
546 |
525 |
174.64 |
|
|
|
| 18 |
B |
449 |
431 |
150.38 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 14135.4 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 13575.6 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 HSEh1PBE/6-311G**
Point Group is C2
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.145 |
| O2 |
0.000 |
0.000 |
1.356 |
| N3 |
0.000 |
1.156 |
-0.611 |
| N4 |
0.000 |
-1.156 |
-0.611 |
| H5 |
0.206 |
1.978 |
-0.068 |
| H6 |
0.446 |
1.126 |
-1.513 |
| H7 |
-0.206 |
-1.978 |
-0.068 |
| H8 |
-0.446 |
-1.126 |
-1.513 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2110 | 1.3810 | 1.3810 | 2.0005 | 2.0535 | 2.0005 | 2.0535 |
O2 | 1.2110 | | 2.2810 | 2.2810 | 2.4459 | 3.1143 | 2.4459 | 3.1143 | N3 | 1.3810 | 2.2810 | | 2.3121 | 1.0069 | 1.0074 | 3.1879 | 2.4945 | N4 | 1.3810 | 2.2810 | 2.3121 | | 3.1879 | 2.4945 | 1.0069 | 1.0074 | H5 | 2.0005 | 2.4459 | 1.0069 | 3.1879 | | 1.6953 | 3.9783 | 3.4864 | H6 | 2.0535 | 3.1143 | 1.0074 | 2.4945 | 1.6953 | | 3.4864 | 2.4228 | H7 | 2.0005 | 2.4459 | 3.1879 | 1.0069 | 3.9783 | 3.4864 | | 1.6953 | H8 | 2.0535 | 3.1143 | 2.4945 | 1.0074 | 3.4864 | 2.4228 | 1.6953 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
112.870 |
|
C1 |
N3 |
H6 |
117.735 |
| C1 |
N4 |
H7 |
112.870 |
|
C1 |
N4 |
H8 |
117.735 |
| O2 |
C1 |
N3 |
123.161 |
|
O2 |
C1 |
N4 |
123.161 |
| N3 |
C1 |
N4 |
113.677 |
|
H5 |
N3 |
H6 |
114.626 |
| H7 |
N4 |
H8 |
114.626 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.436 |
|
|
|
| 2 |
O |
-0.391 |
|
|
|
| 3 |
N |
-0.478 |
|
|
|
| 4 |
N |
-0.478 |
|
|
|
| 5 |
H |
0.236 |
|
|
|
| 6 |
H |
0.219 |
|
|
|
| 7 |
H |
0.236 |
|
|
|
| 8 |
H |
0.219 |
|
|
|
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 |
-3.665 |
3.665 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-24.561 |
3.266 |
0.000 |
| y |
3.266 |
-17.599 |
0.000 |
| z |
0.000 |
0.000 |
-24.776 |
|
| Traceless |
| | x | y | z |
| x |
-3.373 |
3.266 |
0.000 |
| y |
3.266 |
7.070 |
0.000 |
| z |
0.000 |
0.000 |
-3.696 |
|
| Polar |
| 3z2-r2 | -7.392 |
| x2-y2 | -6.962 |
| xy | 3.266 |
| 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 |
0.169 |
0.000 |
| y |
0.169 |
4.801 |
0.000 |
| z |
0.000 |
0.000 |
4.941 |
<r2> (average value of r
2) Å
2
| <r2> |
68.134 |
| (<r2>)1/2 |
8.254 |
Jump to
S1C1
S1C3
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -225.103475 |
| Energy at 298.15K | -225.109016 |
| HF Energy | -225.103475 |
| Nuclear repulsion energy | 124.135416 |
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/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' |
3760 |
3611 |
39.26 |
|
|
|
| 2 |
A' |
3639 |
3494 |
9.20 |
|
|
|
| 3 |
A' |
1841 |
1768 |
445.55 |
|
|
|
| 4 |
A' |
1642 |
1577 |
13.26 |
|
|
|
| 5 |
A' |
1178 |
1132 |
2.74 |
|
|
|
| 6 |
A' |
978 |
940 |
9.12 |
|
|
|
| 7 |
A' |
785 |
754 |
26.24 |
|
|
|
| 8 |
A' |
553 |
531 |
31.98 |
|
|
|
| 9 |
A' |
482 |
462 |
11.41 |
|
|
|
| 10 |
A' |
372 |
357 |
393.92 |
|
|
|
| 11 |
A" |
3757 |
3609 |
35.02 |
|
|
|
| 12 |
A" |
3629 |
3486 |
47.00 |
|
|
|
| 13 |
A" |
1633 |
1569 |
256.88 |
|
|
|
| 14 |
A" |
1439 |
1382 |
195.22 |
|
|
|
| 15 |
A" |
1018 |
978 |
17.95 |
|
|
|
| 16 |
A" |
576 |
553 |
22.14 |
|
|
|
| 17 |
A" |
408 |
392 |
49.90 |
|
|
|
| 18 |
A" |
71 |
68 |
43.26 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13880.2 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 13330.5 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 HSEh1PBE/6-311G**
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.008 |
0.142 |
0.000 |
| O2 |
0.034 |
1.354 |
0.000 |
| N3 |
0.034 |
-0.601 |
1.158 |
| N4 |
0.034 |
-0.601 |
-1.158 |
| H5 |
-0.147 |
-0.073 |
1.994 |
| H6 |
-0.251 |
-1.564 |
1.165 |
| H7 |
-0.147 |
-0.073 |
-1.994 |
| H8 |
-0.251 |
-1.564 |
-1.165 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2124 | 1.3760 | 1.3760 | 2.0117 | 2.0820 | 2.0117 | 2.0820 |
O2 | 1.2124 | | 2.2719 | 2.2719 | 2.4586 | 3.1550 | 2.4586 | 3.1550 | N3 | 1.3760 | 2.2719 | | 2.3166 | 1.0051 | 1.0050 | 3.2015 | 2.5314 | N4 | 1.3760 | 2.2719 | 2.3166 | | 3.2015 | 2.5314 | 1.0051 | 1.0050 | H5 | 2.0117 | 2.4586 | 1.0051 | 3.2015 | | 1.7097 | 3.9884 | 3.4953 | H6 | 2.0820 | 3.1550 | 1.0050 | 2.5314 | 1.7097 | | 3.4953 | 2.3302 | H7 | 2.0117 | 2.4586 | 3.2015 | 1.0051 | 3.9884 | 3.4953 | | 1.7097 | H8 | 2.0820 | 3.1550 | 2.5314 | 1.0050 | 3.4953 | 2.3302 | 1.7097 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
114.418 |
|
C1 |
N3 |
H6 |
121.173 |
| C1 |
N4 |
H7 |
114.418 |
|
C1 |
N4 |
H8 |
121.173 |
| O2 |
C1 |
N3 |
122.610 |
|
O2 |
C1 |
N4 |
122.610 |
| N3 |
C1 |
N4 |
114.663 |
|
H5 |
N3 |
H6 |
116.548 |
| H7 |
N4 |
H8 |
116.548 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.458 |
|
|
|
| 2 |
O |
-0.401 |
|
|
|
| 3 |
N |
-0.480 |
|
|
|
| 4 |
N |
-0.480 |
|
|
|
| 5 |
H |
0.240 |
|
|
|
| 6 |
H |
0.211 |
|
|
|
| 7 |
H |
0.240 |
|
|
|
| 8 |
H |
0.211 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-1.514 |
-4.035 |
0.000 |
4.310 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.183 |
1.583 |
0.000 |
| y |
1.583 |
-24.097 |
0.000 |
| z |
0.000 |
0.000 |
-16.984 |
|
| Traceless |
| | x | y | z |
| x |
-4.642 |
1.583 |
0.000 |
| y |
1.583 |
-3.014 |
0.000 |
| z |
0.000 |
0.000 |
7.656 |
|
| Polar |
| 3z2-r2 | 15.312 |
| x2-y2 | -1.086 |
| xy | 1.583 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
2.445 |
0.119 |
0.000 |
| y |
0.119 |
4.925 |
0.000 |
| z |
0.000 |
0.000 |
4.815 |
<r2> (average value of r
2) Å
2
| <r2> |
68.180 |
| (<r2>)1/2 |
8.257 |
Jump to
S1C1
S1C2
Energy calculated at HSEh1PBE/6-311G**
| | hartrees |
| Energy at 0K | -225.103021 |
| Energy at 298.15K | |
| HF Energy | -225.103021 |
| Nuclear repulsion energy | 124.239948 |
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/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 |
A1 |
3796 |
3646 |
54.13 |
|
|
|
| 2 |
A1 |
3664 |
3519 |
6.59 |
|
|
|
| 3 |
A1 |
1835 |
1762 |
478.52 |
|
|
|
| 4 |
A1 |
1630 |
1566 |
2.95 |
|
|
|
| 5 |
A1 |
1154 |
1108 |
0.28 |
|
|
|
| 6 |
A1 |
986 |
947 |
7.99 |
|
|
|
| 7 |
A1 |
480 |
461 |
3.07 |
|
|
|
| 8 |
A2 |
372 |
357 |
0.00 |
|
|
|
| 9 |
A2 |
394i |
378i |
0.00 |
|
|
|
| 10 |
B1 |
785 |
754 |
8.45 |
|
|
|
| 11 |
B1 |
570 |
547 |
10.06 |
|
|
|
| 12 |
B1 |
266i |
256i |
478.67 |
|
|
|
| 13 |
B2 |
3794 |
3644 |
43.24 |
|
|
|
| 14 |
B2 |
3655 |
3510 |
65.50 |
|
|
|
| 15 |
B2 |
1629 |
1564 |
321.66 |
|
|
|
| 16 |
B2 |
1443 |
1386 |
195.84 |
|
|
|
| 17 |
B2 |
993 |
953 |
11.07 |
|
|
|
| 18 |
B2 |
569 |
546 |
15.12 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 13346.5 cm
-1
Scaled (by 0.9604) Zero Point Vibrational Energy (zpe) 12818.0 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/6-311G**
Point Group is C2v
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
0.000 |
0.000 |
0.142 |
| O2 |
0.000 |
0.000 |
1.356 |
| N3 |
0.000 |
1.154 |
-0.596 |
| N4 |
0.000 |
-1.154 |
-0.596 |
| H5 |
0.000 |
2.016 |
-0.084 |
| H6 |
0.000 |
1.181 |
-1.598 |
| H7 |
0.000 |
-2.016 |
-0.084 |
| H8 |
0.000 |
-1.181 |
-1.598 |
Atom - Atom Distances (Å)
| |
C1 |
O2 |
N3 |
N4 |
H5 |
H6 |
H7 |
H8 |
| C1 | | 1.2140 | 1.3698 | 1.3698 | 2.0290 | 2.1028 | 2.0290 | 2.1028 |
O2 | 1.2140 | | 2.2675 | 2.2675 | 2.4777 | 3.1812 | 2.4777 | 3.1812 | N3 | 1.3698 | 2.2675 | | 2.3082 | 1.0028 | 1.0025 | 3.2116 | 2.5409 | N4 | 1.3698 | 2.2675 | 2.3082 | | 3.2116 | 2.5409 | 1.0028 | 1.0025 | H5 | 2.0290 | 2.4777 | 1.0028 | 3.2116 | | 1.7293 | 4.0328 | 3.5376 | H6 | 2.1028 | 3.1812 | 1.0025 | 2.5409 | 1.7293 | | 3.5376 | 2.3616 | H7 | 2.0290 | 2.4777 | 3.2116 | 1.0028 | 4.0328 | 3.5376 | | 1.7293 | H8 | 2.1028 | 3.1812 | 2.5409 | 1.0025 | 3.5376 | 2.3616 | 1.7293 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
N3 |
H5 |
116.714 |
|
C1 |
N3 |
H6 |
124.115 |
| C1 |
N4 |
H7 |
116.714 |
|
C1 |
N4 |
H8 |
124.115 |
| O2 |
C1 |
N3 |
122.590 |
|
O2 |
C1 |
N4 |
122.590 |
| N3 |
C1 |
N4 |
114.821 |
|
H5 |
N3 |
H6 |
119.171 |
| H7 |
N4 |
H8 |
119.171 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at HSEh1PBE/6-311G**
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.496 |
|
|
|
| 2 |
O |
-0.411 |
|
|
|
| 3 |
N |
-0.509 |
|
|
|
| 4 |
N |
-0.509 |
|
|
|
| 5 |
H |
0.248 |
|
|
|
| 6 |
H |
0.219 |
|
|
|
| 7 |
H |
0.248 |
|
|
|
| 8 |
H |
0.219 |
|
|
|
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 |
-4.337 |
4.337 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.524 |
0.000 |
0.000 |
| y |
0.000 |
-16.311 |
0.000 |
| z |
0.000 |
0.000 |
-23.630 |
|
| Traceless |
| | x | y | z |
| x |
-5.554 |
0.000 |
0.000 |
| y |
0.000 |
8.266 |
0.000 |
| z |
0.000 |
0.000 |
-2.712 |
|
| Polar |
| 3z2-r2 | -5.425 |
| x2-y2 | -9.213 |
| 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 |
2.372 |
0.000 |
0.000 |
| y |
0.000 |
4.791 |
0.000 |
| z |
0.000 |
0.000 |
4.871 |
<r2> (average value of r
2) Å
2
| <r2> |
68.119 |
| (<r2>)1/2 |
8.253 |