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All results from a given calculation for C6H4F2 (1,4-difluorobenzene)

using model chemistry: MP2=FULL/cc-pVTZ

19 10 17 12 22

States and conformations

State Conformation minimum conformation conformer description state description
1 1 yes D2H 1Ag
Energy calculated at MP2=FULL/cc-pVTZ
 hartrees
Energy at 0K-430.105651
Energy at 298.15K 
HF Energy-428.558005
Nuclear repulsion energy343.129096
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 MP2=FULL/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 Ag 3274 3108 0.00 267.25 0.17 0.28
2 Ag 1678 1593 0.00 5.22 0.61 0.76
3 Ag 1307 1241 0.00 20.82 0.11 0.20
4 Ag 1173 1113 0.00 6.70 0.64 0.78
5 Ag 876 832 0.00 33.27 0.08 0.14
6 Ag 456 433 0.00 4.60 0.43 0.60
7 Au 979 929 0.00 0.00 0.00 0.00
8 Au 442 420 0.00 0.00 0.00 0.00
9 B1g 831 789 0.00 0.15 0.75 0.86
10 B1u 3252 3088 2.18 0.00 0.31 0.47
11 B1u 1562 1483 261.69 0.00 0.26 0.00
12 B1u 1253 1190 158.52 0.00 0.40 0.00
13 B1u 1038 985 1.42 0.00 0.00 0.00
14 B1u 763 724 54.09 0.00 0.00 0.00
15 B2g 957 909 0.00 0.29 0.75 0.86
16 B2g 722 685 0.00 0.57 0.75 0.86
17 B2g 389 369 0.00 3.31 0.75 0.86
18 B2u 3273 3107 0.08 0.00 0.40 0.57
19 B2u 1488 1412 0.97 0.00 0.51 0.68
20 B2u 1440 1367 0.02 0.00 0.51 0.68
21 B2u 1116 1060 12.89 0.00 0.50 0.67
22 B2u 351 333 4.04 0.00 0.00 0.00
23 B3g 3256 3091 0.00 109.30 0.75 0.86
24 B3g 1671 1586 0.00 5.71 0.75 0.86
25 B3g 1299 1233 0.00 1.75 0.75 0.86
26 B3g 646 613 0.00 6.52 0.75 0.86
27 B3g 445 422 0.00 0.04 0.75 0.86
28 B3u 875 831 80.11 0.00 0.00 0.00
29 B3u 528 502 17.31 0.00 0.00 0.00
30 B3u 163 155 1.51 0.00 0.00 0.00

Unscaled Zero Point Vibrational Energy (zpe) 18751.0 cm-1
Scaled (by 0.9494) Zero Point Vibrational Energy (zpe) 17802.2 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.
Rotational Constants (cm-1) from geometry optimized at MP2=FULL/cc-pVTZ
ABC
0.19112 0.04792 0.03831

See section I.F.4 to change rotational constant units
Geometric Data calculated at MP2=FULL/cc-pVTZ

Point Group is D2h

Cartesians (Å)
Atom x (Å) y (Å) z (Å)
C1 0.000 0.000 1.362
C2 0.000 0.000 -1.362
C3 0.000 1.208 0.693
C4 0.000 -1.208 0.693
C5 0.000 -1.208 -0.693
C6 0.000 1.208 -0.693
F7 0.000 0.000 2.704
F8 0.000 0.000 -2.704
H9 0.000 2.125 1.253
H10 0.000 -2.125 1.253
H11 0.000 -2.125 -1.253
H12 0.000 2.125 -1.253

Atom - Atom Distances (Å)
  C1 C2 C3 C4 C5 C6 F7 F8 H9 H10 H11 H12
C12.72451.38051.38052.38402.38401.34194.06642.12782.12783.36963.3696
C22.72452.38402.38401.38051.38054.06641.34193.36963.36962.12782.1278
C31.38052.38402.41522.78491.38662.34563.60571.07463.37933.85922.1515
C41.38052.38402.41521.38662.78492.34563.60573.37931.07462.15153.8592
C52.38401.38052.78491.38662.41523.60572.34563.85922.15151.07463.3793
C62.38401.38051.38662.78492.41523.60572.34562.15153.85923.37931.0746
F71.34194.06642.34562.34563.60573.60575.40832.57332.57334.49154.4915
F84.06641.34193.60573.60572.34562.34565.40834.49154.49152.57332.5733
H92.12783.36961.07463.37933.85922.15152.57334.49154.25004.93372.5058
H102.12783.36963.37931.07462.15153.85922.57334.49154.25002.50584.9337
H113.36962.12783.85922.15151.07463.37934.49152.57334.93372.50584.2500
H123.36962.12782.15153.85923.37931.07464.49152.57332.50584.93374.2500

picture of 1,4-difluorobenzene state 1 conformation 1
More geometry information
Calculated Bond Angles
atom1 atom2 atom3 angle atom1 atom2 atom3 angle
C1 C3 C6 118.985 C1 C3 H9 119.632
C1 C4 C5 118.985 C1 C4 H10 119.632
C2 C5 C4 118.985 C2 C5 H11 119.632
C2 C6 C3 118.985 C2 C6 H12 119.632
C3 C1 C4 122.031 C3 C1 F7 118.985
C3 C6 H12 121.383 C4 C1 F7 118.985
C4 C5 H11 121.383 C5 C2 C6 122.031
C5 C2 F8 118.985 C5 C4 H10 121.383
C6 C2 F8 118.985 C6 C3 H9 121.383
Electronic energy levels
Charges, Dipole, Quadrupole and Polarizability