GENERAL INFO
Title:
tskcn9attack_nrs
Browse item:
https://iochem-bd.iciq.es:443/browse/handle/100/92777
Program:
Gaussian 09 EM64L-G09RevD.01
Author:
García-Padilla, Eduardo
Formula:
C69N9K9
Calculation type:
Geometry optimization Minimum
Method(s):
RB3LYP - Grimme-D3
Temperature
298.150 K
Pressure
1.00000 atm
ATOM INFO
Atomic coordinates [Å]
(optimized)
MOLECULAR INFO
Charge / Multiplicity:
0 1
Frozen section
Polarizable Continuum Model (PCM)
Model:
PCM (using non-symmetric T matrix)
Atomic radii
UFF
Solvent
C60
Eps= 4.080000
Eps(inf)= 3.830000
JOB
|
Energies
Energy
Value
Units
SCF Done:
-8521.81903237
Eh
Mulliken charges
Dipole moment (Debye)
Dipole moment
X
Y
Z
Total
5.1161
9.3997
8.3264
13.5594
Quadrupole moment
XX
YY
ZZ
XY
XZ
YZ
-528.6637
-554.1260
-526.6243
-4.0800
13.5678
49.2839
JOB
|
Energies
Energy
Value
Units
SCF Done:
-8521.81904603
Eh
Mulliken charges
Dipole moment (Debye)
Dipole moment
X
Y
Z
Total
5.1424
9.4109
8.4422
13.6484
Quadrupole moment
XX
YY
ZZ
XY
XZ
YZ
-528.5352
-554.2836
-526.8428
-4.1095
13.7595
49.2348
JOB
|
Energies
Energy
Value
Units
SCF Done:
-8521.81904603
Eh
Zero-point correction
0.435185
Eh
Thermal correction to Energy
0.508254
Eh
Thermal correction to Enthalpy
0.509198
Eh
Thermal correction to Gibbs Free Energy
0.312999
Eh
Sum of electronic and zero-point Energies
-8521.383861
Eh
Sum of electronic and thermal Energies
-8521.310792
Eh
Sum of electronic and thermal Enthalpies
-8521.309848
Eh
Sum of electronic and thermal Free Energies
-8521.506047
Eh
IR spectrum
Selected frequency:
.... select ....
Base
-406.0819
9.2406
11.4054
15.1387
17.8956
22.5940
29.9450
31.1377
35.1224
38.7498
40.2175
43.0462
43.9870
46.1426
48.7011
52.8265
55.0021
57.0706
58.2649
59.8416
61.5237
63.8631
64.7290
67.5268
71.2672
72.9816
74.0610
76.6989
80.9042
82.2213
85.1159
85.8696
89.2908
91.4359
94.6791
95.4350
97.2620
99.5879
103.0378
104.9152
105.5131
107.7440
109.2957
112.3218
115.5443
119.2659
119.5983
122.1767
125.4405
127.1925
128.9315
129.6759
134.8414
135.0784
137.9516
138.6236
142.4464
146.3904
147.8349
150.7224
157.7070
162.7793
172.4478
178.8959
181.7145
184.2103
194.2182
199.7778
204.6813
206.9401
234.0242
253.0114
263.2692
263.5264
267.2718
269.1531
273.9789
337.2463
343.8295
344.3781
352.9778
353.6556
358.0854
360.8629
405.0531
407.1096
409.6673
411.9209
413.1514
427.7659
433.3198
434.1802
438.8287
440.6198
479.2190
483.7034
486.5033
488.9330
498.9039
521.5543
532.3615
533.2549
534.5975
535.9681
536.8666
538.4200
540.8416
564.2095
564.9586
565.5701
565.9639
568.2624
573.4370
575.3223
580.4796
582.0301
583.4010
585.1929
596.8735
597.3176
675.2559
678.0342
678.5506
679.6739
682.3136
702.1439
711.8525
713.5376
717.8077
718.1728
720.0484
721.6096
722.7209
730.4557
734.9152
736.2877
738.2844
739.0581
741.7239
743.1620
744.0724
749.8176
750.2970
751.1251
753.3855
753.9871
754.0941
755.6205
760.0148
767.8229
768.5731
769.0583
770.0664
780.6509
789.6863
791.2705
793.5762
795.0570
808.3510
808.8997
809.4134
840.3117
841.3865
842.3181
967.2487
971.8302
973.9341
982.5089
984.0395
984.4545
986.9770
989.2695
1091.6513
1096.1614
1098.0998
1100.7021
1118.3562
1125.5142
1127.7063
1130.9956
1131.9355
1193.8010
1198.0059
1203.6846
1210.6933
1211.8429
1216.2953
1230.6066
1232.6797
1242.0088
1243.0504
1246.0912
1267.6584
1268.2712
1274.1049
1276.2327
1280.6823
1299.5231
1300.5218
1306.1127
1324.4896
1327.6444
1333.3981
1333.9931
1336.6430
1337.5052
1338.8164
1346.9027
1362.9365
1364.7895
1369.2560
1370.6036
1371.6258
1373.9320
1375.3033
1377.5707
1425.6562
1437.6134
1444.7496
1448.0843
1450.7246
1455.6018
1457.4642
1459.7567
1461.1938
1463.4092
1465.1875
1467.6496
1497.2865
1520.7512
1532.8096
1536.1405
1542.0079
1557.8477
1564.9081
1568.2635
1586.9539
1600.6652
1604.0333
1605.6252
1608.0407
1612.0256
1613.7008
1614.8099
1615.9514
1616.1992
2150.0935
2153.0086
2159.0262
2160.0527
2164.7518
2165.3030
2166.7323
2167.9251
2169.3547
Mulliken charges
Dipole moment (Debye)
Dipole moment
X
Y
Z
Total
5.1422
9.4107
8.4423
13.6483
Quadrupole moment
XX
YY
ZZ
XY
XZ
YZ
-528.5358
-554.2838
-526.8428
-4.1096
13.7601
49.2350
Report data
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