Jump to
S1C2
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -209.078610 |
| Energy at 298.15K | |
| HF Energy | -208.797275 |
| Nuclear repulsion energy | 117.430987 |
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 B2PLYP=FULLultrafine/aug-cc-pVTZ
| 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' |
3833 |
3676 |
93.04 |
|
|
|
| 2 |
A' |
3152 |
3024 |
10.73 |
|
|
|
| 3 |
A' |
3118 |
2991 |
10.27 |
|
|
|
| 4 |
A' |
3053 |
2928 |
16.78 |
|
|
|
| 5 |
A' |
1720 |
1649 |
0.72 |
|
|
|
| 6 |
A' |
1498 |
1437 |
10.40 |
|
|
|
| 7 |
A' |
1446 |
1387 |
3.26 |
|
|
|
| 8 |
A' |
1410 |
1353 |
19.68 |
|
|
|
| 9 |
A' |
1288 |
1235 |
52.34 |
|
|
|
| 10 |
A' |
1161 |
1114 |
3.87 |
|
|
|
| 11 |
A' |
1001 |
960 |
119.38 |
|
|
|
| 12 |
A' |
903 |
866 |
33.53 |
|
|
|
| 13 |
A' |
567 |
544 |
15.30 |
|
|
|
| 14 |
A' |
327 |
313 |
2.92 |
|
|
|
| 15 |
A" |
3104 |
2977 |
11.82 |
|
|
|
| 16 |
A" |
1496 |
1435 |
8.26 |
|
|
|
| 17 |
A" |
1092 |
1047 |
1.33 |
|
|
|
| 18 |
A" |
920 |
882 |
8.98 |
|
|
|
| 19 |
A" |
401 |
384 |
126.18 |
|
|
|
| 20 |
A" |
288 |
276 |
0.76 |
|
|
|
| 21 |
A" |
202 |
194 |
0.11 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15989.8 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 15335.8 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 B2PLYP=FULLultrafine/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.287 |
1.309 |
0.000 |
| C2 |
0.000 |
0.563 |
0.000 |
| N3 |
-0.004 |
-0.707 |
0.000 |
| O4 |
1.310 |
-1.218 |
0.000 |
| H5 |
1.164 |
-2.168 |
0.000 |
| H6 |
-2.126 |
0.619 |
0.000 |
| H7 |
-1.355 |
1.953 |
0.877 |
| H8 |
-1.355 |
1.953 |
-0.877 |
| H9 |
0.943 |
1.103 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4879 | 2.3902 | 3.6236 | 4.2546 | 1.0861 | 1.0900 | 1.0900 | 2.2395 |
C2 | 1.4879 | | 1.2699 | 2.2105 | 2.9687 | 2.1265 | 2.1302 | 2.1302 | 1.0870 | N3 | 2.3902 | 1.2699 | | 1.4093 | 1.8704 | 2.5025 | 3.1096 | 3.1096 | 2.0432 | O4 | 3.6236 | 2.2105 | 1.4093 | | 0.9615 | 3.8959 | 4.2336 | 4.2336 | 2.3502 | H5 | 4.2546 | 2.9687 | 1.8704 | 0.9615 | | 4.3119 | 4.9088 | 4.9088 | 3.2792 | H6 | 1.0861 | 2.1265 | 2.5025 | 3.8959 | 4.3119 | | 1.7723 | 1.7723 | 3.1067 | H7 | 1.0900 | 2.1302 | 3.1096 | 4.2336 | 4.9088 | 1.7723 | | 1.7548 | 2.6023 | H8 | 1.0900 | 2.1302 | 3.1096 | 4.2336 | 4.9088 | 1.7723 | 1.7548 | | 2.6023 | H9 | 2.2395 | 1.0870 | 2.0432 | 2.3502 | 3.2792 | 3.1067 | 2.6023 | 2.6023 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
119.948 |
|
C1 |
C2 |
H9 |
120.055 |
| C2 |
C1 |
H6 |
110.436 |
|
C2 |
C1 |
H7 |
110.494 |
| C2 |
C1 |
H8 |
110.494 |
|
C2 |
N3 |
O4 |
111.079 |
| N3 |
C2 |
H9 |
119.997 |
|
N3 |
O4 |
H5 |
102.526 |
| H6 |
C1 |
H7 |
109.064 |
|
H6 |
C1 |
H8 |
109.064 |
| H7 |
C1 |
H8 |
107.212 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/aug-cc-pVTZ
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
-0.545 |
|
|
|
| 2 |
C |
-0.248 |
|
|
|
| 3 |
N |
-0.292 |
|
|
|
| 4 |
O |
-0.310 |
|
|
|
| 5 |
H |
0.167 |
|
|
|
| 6 |
H |
0.279 |
|
|
|
| 7 |
H |
0.231 |
|
|
|
| 8 |
H |
0.231 |
|
|
|
| 9 |
H |
0.487 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
-0.441 |
0.798 |
0.000 |
0.912 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-25.906 |
-1.968 |
0.009 |
| y |
-1.968 |
-19.354 |
-0.011 |
| z |
0.009 |
-0.011 |
-25.592 |
|
| Traceless |
| | x | y | z |
| x |
-3.433 |
-1.968 |
0.009 |
| y |
-1.968 |
6.395 |
-0.011 |
| z |
0.009 |
-0.011 |
-2.962 |
|
| Polar |
| 3z2-r2 | -5.924 |
| x2-y2 | -6.552 |
| xy | -1.968 |
| xz | 0.009 |
| yz | -0.011 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
6.441 |
-1.406 |
-0.000 |
| y |
-1.406 |
7.682 |
0.001 |
| z |
-0.000 |
0.001 |
4.524 |
<r2> (average value of r
2) Å
2
| <r2> |
91.870 |
| (<r2>)1/2 |
9.585 |
Jump to
S1C1
Energy calculated at B2PLYP=FULLultrafine/aug-cc-pVTZ
| | hartrees |
| Energy at 0K | -209.077843 |
| Energy at 298.15K | |
| HF Energy | -208.796043 |
| Nuclear repulsion energy | 119.923515 |
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 B2PLYP=FULLultrafine/aug-cc-pVTZ
| 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' |
3835 |
3678 |
93.74 |
|
|
|
| 2 |
A' |
3185 |
3055 |
8.39 |
|
|
|
| 3 |
A' |
3172 |
3042 |
1.07 |
|
|
|
| 4 |
A' |
3059 |
2934 |
11.91 |
|
|
|
| 5 |
A' |
1724 |
1653 |
7.39 |
|
|
|
| 6 |
A' |
1494 |
1433 |
14.36 |
|
|
|
| 7 |
A' |
1417 |
1359 |
12.76 |
|
|
|
| 8 |
A' |
1379 |
1323 |
22.31 |
|
|
|
| 9 |
A' |
1340 |
1286 |
49.43 |
|
|
|
| 10 |
A' |
1153 |
1105 |
9.78 |
|
|
|
| 11 |
A' |
929 |
891 |
59.01 |
|
|
|
| 12 |
A' |
902 |
865 |
80.59 |
|
|
|
| 13 |
A' |
674 |
646 |
13.15 |
|
|
|
| 14 |
A' |
314 |
302 |
1.48 |
|
|
|
| 15 |
A" |
3107 |
2980 |
9.86 |
|
|
|
| 16 |
A" |
1504 |
1443 |
8.59 |
|
|
|
| 17 |
A" |
1075 |
1031 |
0.71 |
|
|
|
| 18 |
A" |
872 |
837 |
13.50 |
|
|
|
| 19 |
A" |
501 |
481 |
34.61 |
|
|
|
| 20 |
A" |
395 |
378 |
80.38 |
|
|
|
| 21 |
A" |
38i |
36i |
0.01 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 15996.1 cm
-1
Scaled (by 0.9591) Zero Point Vibrational Energy (zpe) 15341.9 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 B2PLYP=FULLultrafine/aug-cc-pVTZ
Point Group is Cs
Cartesians (Å)
| Atom |
x (Å) |
y (Å) |
z (Å) |
| C1 |
-1.443 |
0.488 |
0.000 |
| C2 |
0.000 |
0.861 |
0.000 |
| N3 |
1.014 |
0.091 |
0.000 |
| O4 |
0.653 |
-1.272 |
0.000 |
| H5 |
1.511 |
-1.705 |
0.000 |
| H6 |
-1.579 |
-0.587 |
0.000 |
| H7 |
-1.934 |
0.911 |
0.876 |
| H8 |
-1.934 |
0.911 |
-0.876 |
| H9 |
0.271 |
1.909 |
0.000 |
Atom - Atom Distances (Å)
| |
C1 |
C2 |
N3 |
O4 |
H5 |
H6 |
H7 |
H8 |
H9 |
| C1 | | 1.4908 | 2.4897 | 2.7374 | 3.6797 | 1.0834 | 1.0899 | 1.0899 | 2.2263 |
C2 | 1.4908 | | 1.2733 | 2.2305 | 2.9780 | 2.1424 | 2.1243 | 2.1243 | 1.0822 | N3 | 2.4897 | 1.2733 | | 1.4101 | 1.8639 | 2.6809 | 3.1836 | 3.1836 | 1.9637 | O4 | 2.7374 | 2.2305 | 1.4101 | | 0.9612 | 2.3354 | 3.4969 | 3.4969 | 3.2034 | H5 | 3.6797 | 2.9780 | 1.8639 | 0.9612 | | 3.2867 | 4.4141 | 4.4141 | 3.8208 | H6 | 1.0834 | 2.1424 | 2.6809 | 2.3354 | 3.2867 | | 1.7712 | 1.7712 | 3.1064 | H7 | 1.0899 | 2.1243 | 3.1836 | 3.4969 | 4.4141 | 1.7712 | | 1.7528 | 2.5741 | H8 | 1.0899 | 2.1243 | 3.1836 | 3.4969 | 4.4141 | 1.7712 | 1.7528 | | 2.5741 | H9 | 2.2263 | 1.0822 | 1.9637 | 3.2034 | 3.8208 | 3.1064 | 2.5741 | 2.5741 | |
More geometry information
Calculated Bond Angles
| atom1 |
atom2 |
atom3 |
angle |
|
atom1 |
atom2 |
atom3 |
angle |
| C1 |
C2 |
N3 |
128.330 |
|
C1 |
C2 |
H9 |
118.969 |
| C2 |
C1 |
H6 |
111.689 |
|
C2 |
C1 |
H7 |
109.824 |
| C2 |
C1 |
H8 |
109.824 |
|
C2 |
N3 |
O4 |
112.348 |
| N3 |
C2 |
H9 |
112.701 |
|
N3 |
O4 |
H5 |
101.963 |
| H6 |
C1 |
H7 |
109.171 |
|
H6 |
C1 |
H8 |
109.171 |
| H7 |
C1 |
H8 |
107.046 |
|
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability