GENERAL INFO
Title:
/Copper ITS2
Browse item:
https://iochem-bd.iciq.es:443/browse/handle/100/941
Program:
Gaussian 09 EM64L-G09RevD.01
Author:
Besora, Maria
Formula:
C 36 H 50 Cu 1 N 2 O 4
Calculation type:
Geometry optimization TS
Method(s):
RB97D - Grimme-D2
Temperature
298.150 K
Pressure
1.00000 atm
ATOM INFO
Atomic coordinates [Å]
(optimized)
MOLECULAR INFO
Charge / Multiplicity:
1 1
Full point group
Full point group
C1
NOp
1
Polarizable Continuum Model (PCM)
Model:
PCM (using non-symmetric T matrix)
Atomic radii
SMD-Coulomb.
Solvent
Benzene
Eps= 2.270600
Eps(inf)= 2.253301
JOB
|
Energies
Energy
Value
Units
SCF Done:
-2007.63984854
Eh
Dipole moment (Debye)
Dipole moment
X
Y
Z
Total
3.3417
-0.3930
-1.9550
3.8914
Quadrupole moment
XX
YY
ZZ
XY
XZ
YZ
-175.4371
-229.0435
-224.4944
-4.0898
-13.0071
1.5646
JOB
|
Energies
Energy
Value
Units
SCF Done:
-2007.63984854
Eh
Zero-point correction
0.774127
Eh
Thermal correction to Energy
0.821539
Eh
Thermal correction to Enthalpy
0.822484
Eh
Thermal correction to Gibbs Free Energy
0.692931
Eh
Sum of electronic and zero-point Energies
-2006.865722
Eh
Sum of electronic and thermal Energies
-2006.818309
Eh
Sum of electronic and thermal Enthalpies
-2006.817365
Eh
Sum of electronic and thermal Free Energies
-2006.946917
Eh
IR spectrum
Selected frequency:
.... select ....
Base
-706.0750
17.5349
26.1606
31.2452
32.8986
35.4663
46.0152
48.8420
52.3609
54.0724
57.5562
60.1029
66.8963
69.2945
72.3568
73.9649
82.4223
90.0994
95.0576
96.5511
102.6562
110.4673
129.4593
132.6370
134.1780
137.6542
142.1425
150.0645
157.2018
167.0086
171.4298
183.7119
186.3478
213.1682
236.8025
241.4243
246.5703
253.5836
257.3118
262.3155
266.5636
269.0015
271.8288
280.7236
284.3165
286.7785
293.4978
298.5142
303.5376
308.3726
310.0538
313.2962
315.0688
320.4288
330.4615
331.5497
356.4236
392.3385
396.4660
402.9944
421.6097
425.3767
430.7517
437.5774
439.7046
442.8342
473.9406
480.0685
518.2386
519.9714
521.1196
536.9669
544.1824
568.3706
568.8472
577.0589
582.5791
600.1241
607.9242
611.1903
624.6242
629.8295
631.3145
643.2487
654.0661
684.5663
694.0820
703.6578
721.2305
724.8719
735.0582
738.7340
744.1060
748.5131
750.6196
758.2247
794.3236
795.0550
798.4468
798.6723
799.3027
823.1234
840.8381
862.3245
873.8497
874.5457
881.4119
895.6654
898.2897
911.5205
912.5040
921.1431
923.5348
924.7343
928.8507
932.5424
939.3980
942.4046
945.6246
946.8027
948.7633
951.7627
958.0543
961.8574
963.3467
975.5383
976.5664
1015.4460
1036.1593
1040.2761
1042.1320
1044.4060
1063.0767
1065.9575
1073.9497
1074.7360
1079.2810
1095.5255
1096.8826
1099.4401
1101.3724
1106.2975
1124.0517
1132.3214
1136.8559
1143.2122
1152.2251
1157.4229
1165.4009
1168.2875
1169.2386
1181.5415
1181.9743
1189.5651
1195.6057
1208.8878
1210.9971
1234.1316
1243.9873
1252.7655
1260.3141
1261.4317
1299.0816
1304.6278
1309.3346
1309.8072
1312.3441
1316.2881
1319.2391
1319.7764
1323.5529
1342.0791
1343.7017
1348.7771
1378.2778
1379.6346
1381.1933
1383.0074
1385.1038
1386.3673
1390.2512
1405.2394
1405.5099
1406.0211
1408.1522
1414.3725
1417.9270
1442.0601
1459.2231
1459.8153
1460.5895
1465.8258
1466.1853
1468.6097
1470.1974
1470.7170
1472.0237
1472.9529
1474.2066
1475.3571
1475.8761
1479.0822
1480.3772
1482.5254
1484.3779
1487.0288
1488.6146
1489.6340
1490.8924
1492.4165
1495.1330
1497.8949
1503.7134
1547.4650
1550.0991
1561.0131
1591.4776
1598.0811
1598.8377
1599.7629
1600.6649
1607.1727
1690.6158
1804.5357
2072.7292
2207.7564
2949.6803
2957.2415
2957.8585
2960.4297
2961.9138
2962.3744
2963.7886
2967.1033
2983.5302
2996.3298
3005.8347
3011.0833
3013.0156
3037.7955
3040.5928
3043.1148
3045.1865
3045.7675
3047.5481
3048.0524
3049.9498
3051.6831
3052.1525
3052.2677
3052.5216
3054.3043
3056.1264
3063.6579
3065.8334
3075.7325
3104.0314
3106.2629
3124.5233
3124.9586
3130.5576
3134.6650
3139.6394
3140.2852
3141.2939
3149.7027
3157.7133
3158.6170
3187.2929
3234.3342
3253.7994
3627.6861
3630.9243
Dipole moment (Debye)
Dipole moment
X
Y
Z
Total
3.3461
-0.3953
-1.9578
3.8969
Quadrupole moment
XX
YY
ZZ
XY
XZ
YZ
-175.4470
-229.0582
-224.4666
-4.0932
-13.0246
1.5600
Report data
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